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Research Article Research on Multiobjective Topology Optimization of Diesel Engine Cylinder Block Based on Analytic Hierarchy Process Fenghe Wu , 1,2 Zhaohua Wang , 1,2 Jinxu Han , 1,2 and Guobin Pei 1,2 1 College of Mechanical Engineering, Yanshan University, Qinhuangdao 066004, China 2 Hebei Province Heavy Intelligent Manufacturing Equipment Technology Innovation Center, Qinhuangdao 066004, China Correspondence should be addressed to Fenghe Wu; [email protected] Received 25 December 2018; Revised 1 February 2019; Accepted 17 February 2019; Published 10 March 2019 Guest Editor: Love Ekenberg Copyright © 2019 Fenghe Wu et al. is is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. ere are alternating impact loads for the diesel engine cylinder block. e topology optimization of the extreme single-working condition cannot guarantee its overall mechanical performance, and the traditional multiworking condition optimization has the problem that the weight coefficients are difficult to determine. us, a multiobjective topology optimization method based on analytic hierarchy process is proposed. Firstly, the static, dynamic characteristics and structure efficiency are calculated by the finite element analysis which indicates the direction of topology optimization for the cylinder block. e hierarchical structure model of topology optimization, including 12 weighting coefficients, is constructed considering static multiworking condition stiffness and dynamic multiorder natural frequency. e comprehensive evaluation function for the cylinder block is established by the compromise programming method and the weight coefficients are determined based on analytic hierarchy process. e optimization mathematical model is established and the multiobjective topology optimization of the cylinder block is carried out. e optimization results show that the proposed method can take into account structural multiworking condition performance, which has obvious advantages over the single objective topology optimization. e simulation results show that the static and dynamic characteristics are improved to some extent and the overall mechanical performance of the new model is more uniform with a 5.22% reduction in weight. It shows that the topology structure of the cylinder block is more reasonable. 1. Introduction With the rapid and sustained development of automobile manufacturing industry all over the world, automobile own- ership has increased greatly and the energy and environ- ment issues are becoming more and more prominent. e energy conservation and emission reduction have become an inevitable trend in the development of automobile industry. e diesel engine, as one of the core components in engi- neering vehicles, is developing towards high-power-density, high-speed, and lightweight [1]. e cylinder block is the main structure and the heaviest part of the diesel engine; it must have sufficient stiffness and strength to support a variety of loads. At present, the design and optimization for the cylinder block mainly adopt traditional method combining finite element analysis (FEA) with engineering experience to check its strength and stiffness [2, 3]. e method is heavy and cumbersome, and it is difficult to effectively play structural bearing capacity [4]. e topology optimization method can provide lightweight and efficient structure form in the conceptual design stage, which has been widely concerned [5–7]. e single objective topology optimization for a V-type twelve-cylinder diesel cylinder block is carried out in [8] and the structural performance is improved. Jia et al. [9] get the optimal topology structure of a single cylinder block in the extreme working condition by using the topology and shape optimization. To achieve a low vibration design for a four-cylinder block, Du et al. [10] obtained the layout of the inner ribs by the topology optimization. us, the application of topology optimization for the cylinder block has made some progress and the research mainly focuses on the extreme working condition [11, 12]. However, there are alternating impact loads in the working process Hindawi Mathematical Problems in Engineering Volume 2019, Article ID 6194634, 16 pages https://doi.org/10.1155/2019/6194634
Transcript
Page 1: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

Research ArticleResearch on Multiobjective Topology Optimization of DieselEngine Cylinder Block Based on Analytic Hierarchy Process

FengheWu 12 ZhaohuaWang 12 Jinxu Han 12 and Guobin Pei 12

1College of Mechanical Engineering Yanshan University Qinhuangdao 066004 China2Hebei Province Heavy Intelligent Manufacturing Equipment Technology Innovation Center Qinhuangdao 066004 China

Correspondence should be addressed to Fenghe Wu risingwuysueducn

Received 25 December 2018 Revised 1 February 2019 Accepted 17 February 2019 Published 10 March 2019

Guest Editor Love Ekenberg

Copyright copy 2019 Fenghe Wu et al This is an open access article distributed under the Creative Commons Attribution Licensewhich permits unrestricted use distribution and reproduction in any medium provided the original work is properly cited

There are alternating impact loads for the diesel engine cylinder block The topology optimization of the extreme single-workingcondition cannot guarantee its overall mechanical performance and the traditional multiworking condition optimization has theproblem that the weight coefficients are difficult to determine Thus a multiobjective topology optimization method based onanalytic hierarchy process is proposed Firstly the static dynamic characteristics and structure efficiency are calculated by thefinite element analysis which indicates the direction of topology optimization for the cylinder block The hierarchical structuremodel of topology optimization including 12 weighting coefficients is constructed considering static multiworking conditionstiffness and dynamic multiorder natural frequency The comprehensive evaluation function for the cylinder block is establishedby the compromise programming method and the weight coefficients are determined based on analytic hierarchy process Theoptimization mathematical model is established and the multiobjective topology optimization of the cylinder block is carried outThe optimization results show that the proposed method can take into account structural multiworking condition performancewhich has obvious advantages over the single objective topology optimization The simulation results show that the static anddynamic characteristics are improved to some extent and the overall mechanical performance of the new model is more uniformwith a 522 reduction in weight It shows that the topology structure of the cylinder block is more reasonable

1 Introduction

With the rapid and sustained development of automobilemanufacturing industry all over the world automobile own-ership has increased greatly and the energy and environ-ment issues are becoming more and more prominent Theenergy conservation and emission reduction have become aninevitable trend in the development of automobile industryThe diesel engine as one of the core components in engi-neering vehicles is developing towards high-power-densityhigh-speed and lightweight [1] The cylinder block is themain structure and the heaviest part of the diesel engine itmust have sufficient stiffness and strength to support a varietyof loads At present the design and optimization for thecylinder block mainly adopt traditional method combiningfinite element analysis (FEA) with engineering experience tocheck its strength and stiffness [2 3]Themethod is heavy and

cumbersome and it is difficult to effectively play structuralbearing capacity [4]

The topology optimization method can providelightweight and efficient structure form in the conceptualdesign stage which has been widely concerned [5ndash7]The single objective topology optimization for a V-typetwelve-cylinder diesel cylinder block is carried out in [8]and the structural performance is improved Jia et al [9] getthe optimal topology structure of a single cylinder blockin the extreme working condition by using the topologyand shape optimization To achieve a low vibration designfor a four-cylinder block Du et al [10] obtained the layoutof the inner ribs by the topology optimization Thusthe application of topology optimization for the cylinderblock has made some progress and the research mainlyfocuses on the extreme working condition [11 12] Howeverthere are alternating impact loads in the working process

HindawiMathematical Problems in EngineeringVolume 2019 Article ID 6194634 16 pageshttpsdoiorg10115520196194634

2 Mathematical Problems in Engineering

Multi-Objective Topology Optimization of the Cylinder Block

Geometric modelof cylinder block

Working-condition feature

Structuralfeature

The analysis of topologyoptimization space

The mathematical modelof topology optimization

Finite element model

modal analysis

Analyzing structure efficiency

static characteristic analysis

Hierarchical structure model

Establishing evaluation function

Determining weight coefficient

Mathematical model

Multi-working condition topology optimization

Verifying topology optimization results

Objective

Researchobject

Method

Results

Figure 1 The block diagram of multiobjective topology optimization

of diesel engine If the explosion of each cylinder for amulticylinder block is regarded as an extreme conditionthe topology optimization of the cylinder block belongs tothe typical multiworking condition problem The traditionalsingle objective optimization usually only ensures that themechanical properties are optimal in a certain workingcondition while the overall mechanical property may bereduced to a lower value in other working conditions thatis to say the topology optimization result for the cylinderblock will oscillate between different working conditions andthe overall mechanical property cannot be guaranteed Inaddition the dynamic characteristics of the cylinder blockalso need to be considered in the process of optimization

The multiobjective topology optimization can considersimultaneously several objective functions in the designprocess [13ndash15] and the optimal solution can be obtainedfor each objective function The intelligent algorithms areused to solve directly to avoid decision of multiobjectiveweight coefficients [16ndash18] However the calculation forcomplex structures will cost a lot of time and high economiccosts because of numerical instability during the process oftopology optimization [19 20] Therefore it is necessary toestablish a comprehensive evaluation function to considerseveral objectives as a whole But if the weight coefficientof each working condition is decided by the engineeringexperience the function will not reflect the overall structuralperformance in optimization So the method of determiningweight coefficients is the key of the multiobjective topol-ogy optimization and whose essence is the multicriteriondecision-making problem

The analytic hierarchy process (AHP) proposed by Saaty[21 22] is a systematic analysis method for determining

qualitatively and quantitatively the relative importance of aset of activities in a multicriteria decision-making problemThe method can effectively analyze the nonsequential rela-tionship between multiobjective criterion systems by com-bining mathematical processing with subjective judgmentwhich has been widely used in the field of resource systemanalysis economic management education managementsocial science and so on [23 24] The AHP is applied todeterminate the weight coefficients of the external economicevaluation model to ensure that the wind power engineeringproject is constructed and developed in a scientific manner[25] A multiobjective evolutionary structure optimizationmethod is proposed by combining the AHP and evolutionarystructural optimization which improves the optimizationeffect [26]Therefore it has obvious advantages to bring AHPinto the decision of weight coefficients for the multiobjectivetopology optimization

Under the above background this paper presents amultiobjective topology optimization method based on AHPwhich is applied to a certain four-cylinder diesel enginecylinder block

2 Multiobjective TopologyOptimization Method

The multiobjective topology optimization method of dieselengine cylinder block based on AHP in this paper is mainlydivided into four steps as shown in Figure 1 The firstis to introduce the structural geometry characteristic andworking condition of the cylinder block in Section 3 Sec-ondly the topology optimization space is determined on

Mathematical Problems in Engineering 3

Table 1 The mechanical property of HT300

Material Elastic modulus GPa Poissons ratio Density kg∙mminus3 Tensile strength MPaHT300 143 027 7300 300

z

y

x

1 2 3 4

(a) Front

z

y

x

(b) Back

Figure 2 The cylinder block structure

the basis of analyzing the static characteristics vibrationmode and structure efficiency of each working conditionin Section 4 Then in Section 5 the hierarchical structuremodel of topology optimization is constructed consideringthe static multiworking condition stiffness and dynamicmultiorder natural frequency The comprehensive evaluationfunction is established by the compromise programmingmethod which can more accurately evaluate the structuraloverall performance The weight coefficients are determinedby AHP and the mathematical model is established Finallymultiobjective topology optimization of cylinder block iscarried out and the optimization effect is verified in Section 6

3 Structure Analysis

31 Structure Feature The four-cylinder diesel engine cylin-der block as shown in Figure 2 is a box-type structureobtained by casting and machining and widely used inthe heavy engineering vehicle In order to achieve thelightweight the topology structure of the cylinder block hasbeen modified many times through finite element analysisand manual experience but the structure is still too cumber-some and unsatisfactory Its dimensions are 5267mm long3261mm wide and 3878mm high with a weight of 8897 kgThe material is gray cast iron HT300 and the mechanicalproperty is shown in Table 1

As the main structure of the diesel engine it is coveredwith various stiffening ribs convex plates bearing holes oilchannel holes water-cooled jacket and so on So its mechan-ical property is directly related to the working efficiency ofthe diesel engine and it has to possess sufficient strength andstiffness to support a variety of loads

32 Working Condition For the diesel engine cylinder blockits working condition is a cyclic process including four pro-cesses of intake compression power and exhaust The firingorder of cylinder block is 1-3-4-2 and the rotation speed ofcrank is 3000rpm Therefore there are alternating and high-speed impact loads for the cylinder block and the loads are

very complicated including the explosion pressure the wallpressure from crank-link mechanism the bolt pretighteningforce between cylinder block and cylinder head the reactionforce of bearing block and thermal load etc It is consideredthat the heat generated at the moment of gas explosion is firsttransmitted to the cylinder liner and then to the cylinderwallthe cylinder liner and the water-cooled jacket bear a largeamount of heat during the heat transfer process In order tosimplify calculation in this paper the thermal load on thecylinder wall is ignored So the main loads considered areshown in Figure 3

And the freedom constraints are applied to the six contactfaces ( a-f ) at the bottom of the cylinder block as shown inTable 2 where 119879x 119879y and 119879z mean that the displacementsof x y and z direction are limited 119877x 119877y and 119877z meanthat the rotation angles of x y and z direction are limitedAccording to the basic parameters of the cylinder block thecorresponding extreme load values at the moment of eachcylinder explosion are calculated as shown in Table 3 Thebolt pretightening force is different in different position of thebolt hole and the number of bolt holes is a great many onlythe maximum bolt pretightening force is listed

4 Optimization Space Analysis

41 Static Characteristics Analysis In order to obtain thetopology optimization space the static and dynamic char-acteristics of the cylinder block during the working processare obtained by the FEA The first is to carry out thestatic characteristics analysis at the moment of each cylinderexplosion

The geometry model is imported into the finite ele-ment software and the bolt hole chamfer and oil pipelineare simplified According to the working condition of thecylinder block in Section 32 the finite element modelconsisting of the tetrahedral andhexahedralmixing elementsis established as shown in Figure 4 The displacement andstress distribution are calculated and the results are shownin Table 4 It can be seen that the first working condition is

4 Mathematical Problems in Engineering

Table 2 The constraints of the cylinder block

Constraint face a b c d e fDisplacement freedoms 119879y 119879z 119879y 119879x 119879y 119879z 119879x 119879yRotation freedoms 119877x 119877y 119877z

Table 3 The extreme load value of each cylinder at the time of explosion

The extreme Loads No of explosion1 2 3 4

Bolt pre-tightening force N 69007 67586 69474 75693Reaction force of bearing blockN 63750 63336 47300 63752The wall pressure N 17695 17695 17695 17695The explosion pressure MPa 17 17 17 17

Explosion pressure

A

A A-Aa(f)

Wall pressure

Reaction force of bearing block

Bolt pre-tightening

force

1 2 3 4

b(e)z

y

x

c

d

(def) (abc)

Figure 3 The loads and boundary conditions of cylinder block

Figure 4 The finite element model

the worst and corresponding displacement and stress distri-bution cloud charts are shown in Figure 5 The maximumstress is 2179MPa located at the bolt hole while most of therest region is about 80 MPa which is much smaller than thematerial ultimate strength (300 MPa) It indicates that thecylinder block has optimization space in the worst condition

42 Modal Analysis The static analysis can only reflect struc-tural stiffness and strength and cannot reflect its vibrationperformance Modal analysis is the basis for the dynamicdesign analysis and optimization in modern mechanicalproducts The structural natural frequencies and vibrationmodes can be obtained by the modal analysis to evaluate itsvibration characteristics

Table 4 Results of FEA for the cylinder block

No ofexplosions

Maxstress(MPa)

Maxdisplacement

(mm)1 2179 02542 1688 02233 1684 02144 1992 0246

The constrained modal of the cylinder block is analyzedby the FEA and the top 6-order natural frequencies andcorresponding vibration modes are shown in Figure 6 and

Mathematical Problems in Engineering 5

Table 5 The top 6-order natural frequencies and vibration modes

Orders Frequency Vibration mode1 264Hz First-order torsional vibration around the X axis2 493 Hz First-order bending vibration around the Z axis3 531 Hz Second-order torsional vibration around the X axis4 562 Hz The skirt vibrates with torsion along the X direction5 778 Hz Whole bending torsional vibration6 1038 Hz Whole torsional vibrating around the X axis

(a) Displacement distribution (b) Stress distribution

Figure 5 Results of FEA under extreme working condition

Table 5 It can be seen from Figure 6 that the cylinder blockfirstly appears whole torsional vibration while the wholebending vibration appears in the higher frequency rangewhich show that the torsional stiffness is less than the bendingstiffness for the cylinder block In addition the relativedisplacement near the four corners is large and it is necessaryto improve the freedom constraints to lower the extent of thevibration

To further evaluate its dynamic performance theworkingfrequency is calculated by (1) The cylinder block studied inthis paper is a four-stroke reciprocating piston engine thecrankshaft turns twice and the cylinder body completes aworking cycle including four times vibration of intake com-pression power and exhaust So the corresponding workingfrequency f is 100Hz calculated which is much smaller thanthe first-order natural frequency for the cylinder block Itindicates that the resonance will not occur in working

119891 = 2 sdot 11989960 (1)

where n is the rotation speed of crank n=3000rpm

43 Structure Efficiency Analysis Structure efficiency [27]refers to the structural comprehensive characterization of thestrength and stiffness per unit weight in the case of meetingthe load-bearing property It is commonly used to evaluatethe structural overall performance The greater structural

efficiency the higher the material utilization while thesmaller the structural efficiency the larger the optimizationspace

In this paper the structure efficiency of the cylinder blockis calculated under four extreme working conditions Thecalculation formula of the structure efficiency index 120578119894 isshown in (2) In terms of the multiworking condition topol-ogy optimization its physical meaning is as follows the valueis greater indicating that thematerial utilization is higher andthe working condition is worse On the contrary it shows thatthe working condition is safer and the optimization space islarger

120578119894 = 120590119894max sdot 119889119894max119898 times 100 (2)

where 120578119894 is the structure efficiency index under the ith work-ing condition 120590119894max and 119889119894max are the maximum stress andmaximum displacement under the ith working conditionandm is the structural weight

Substituting the analysis results of Table 4 into (2) thestructure efficiency of the cylinder block is calculated asshown in Figure 7 It can be seen that the cylinder block hasthe highest structure efficiency at the moment of the firstcylinder explosion and followed by the fourth cylinder thesecond cylinder and the third cylinder It shows that the firstcylinder explosion is the worst working condition and thethird cylinder explosion is the safest condition

6 Mathematical Problems in Engineering

Contour Plot

4181E+003717E+003252E+002788E+002324E+001859E+001395E+00

Max = 4181E+00

Min = 1802E-03Grids 4612

Grids 32494

9306E-014662E-011802E-03

No result

Eigen Mode(Mag)Analysis system

(a) The first-order mode

Contour Plot

5090E+004600E+004111E+003621E+003131E+002641E+002152E+00

Max = 5090E+00

Min = 6824E-01Grids 7120

Grids 33177

1662E+001172E+006824E-01

No result

Eigen Mode(Mag)Analysis system

(b) The second-order mode

Contour Plot

5616E+004998E+004379E+003761E+003143E+002524E+001906E+00

Max = 5616E+00

Min = 5048E-02Grids 629

Grids 90051

1287E+00

5048E-026689E-01

No result

Eigen Mode(Mag)Analysis system

(c) The third-order mode

Contour Plot

9348E+008314E+007281E+006248E+005214E+004181E+003148E+00

Max = 9348E+00

Min = 4777E-02Grids 31763

Grids 19024

2114E+001081E+004777E-02

No result

Eigen Mode(Mag)Analysis system

(d) The fourth-order mode

Contour Plot

4681E+004258E+003835E+003412E+002989E+002566E+002143E+00

Max = 4681E+00

Min = 8739E-01Grids 98310

Grids 762

1720E+001297E+008739E-01

No result

Eigen Mode(Mag)Analysis system

(e) The fifth-order mode

Contour Plot

8861E+007876E+006892E+005907E+004923E+003938E+002954E+00

Max = 8861E+00

Min = 1354E-05Grids 4690

Grids 263900

1969E+00

1354E-059845E-01

No result

Eigen Mode(Mag)Analysis system

(f) The sixth-order mode

Figure 6 Results of modal analysis

0

20

40

60

80

1 2 3 4

struc

ture

effici

ency

the number of working conditions

Figure 7 The structure efficiency of each cylinder

Based on the analysis mentioned in Figures 5ndash7 thecylinder block studied in this paper can meet the stiffnessand strength requirements under the worst working con-dition The overall stress value (80 MPa) is much lower

than material ultimate strength (300 MPa) which indicatesthat the cylinder block has surplus material and topologyoptimization space Its working frequency (100 Hz) is muchlower than the first-order natural frequency (264 Hz) andthe resonance does not occur In addition the importancefor four working conditions is sorted the first cylinder thefourth cylinder the second cylinder and the third cylinderTherefore the first cylinder and the fourth cylinder shouldbe focused when determining the weighting coefficientsin multiobjective topology optimization And the materialnear the second cylinder and the third cylinder should beconsidered when improving the topology structure

5 Topology Optimization MathematicalModel Based on AHP

51 The Hierarchical Structure Model The topology opti-mization for the diesel engine cylinder block belongs to thetypical multiworking condition problem It is necessary to

Mathematical Problems in Engineering 7

The top 6-order natural

Topologyoptimizationof cylinder

block

Static topology

dynamic topology

target

criterionThe cylinder No1

The cylinder No2

The cylinder No3

The cylinder No4

index

optimization 2

optimization 1

of explosion w4

of explosion w3

of explosion w2

of explosion w1

frequencies w5 sim w10

Figure 8 The hierarchical structure model of topology optimization

take into account the structural performance requirementsincluding static and dynamic characteristics For the staticcharacteristics structural stiffness has to be considered atthe moment of each cylinder explosion And the top 6-order natural frequencies need to be concerned for dynamiccharacteristicsTherefore the hierarchical structure model oftopology optimization for the cylinder block is establishedbased on staticmultiworking condition stiffness and dynamicmultiorder natural frequency as shown in Figure 8 It canbe seen from the figure that the multiobjective topologyoptimization of the cylinder block includes 12 weightingcoefficients that are static and dynamic topology optimization1205721 1205722 in the criterion layer static multiworking conditionstiffness1199081 sim 1199084 and dynamic multiorder natural frequency1199085 sim 1199081052 Comprehensive Evaluation of the Cylinder Block Thelinear weighting method is usually used to transform themultiobjective problem into a single-objective problem forthe traditional multiobjective topology optimization How-ever the linear weighting method is to calculate weightaverage value for all functions and it cannot reflect the promi-nent influence from some certain functions which doesnot guarantee that all functions obtain the relative optimalsolutionThe compromise programmingmethod [28] can geta group of better relative optimal solutions by calculating thesensitivity of all functions to design variables and adjustingeach objective to balance each other From the hierarchicalstructuremodel shown in Figure 8 the topology optimizationfor the cylinder block includes ten optimization objectivesand the static and dynamic multiobjective optimizationproblem is converted into the single-objective optimizationproblem by the compromise programming method

521 Static Multiworking Condition Stiffness The topologyoptimization oriented by stiffnessmaximization is to research

material distribution form in the design domain to maxi-mize the structural stiffness In this paper the static stiff-ness of the cylinder block under four extreme conditionsis studied which belongs to the multiworking conditionstiffness problem In this paper the objective function ofstatic multiworking condition stiffness is obtained by thecompromise programming method as shown in (3) 119862(120588)is the comprehensive evaluation value of the static stiffnessand the smaller the value the larger the structural overallstiffness

min120588119862 (120588) = 119898sum

119894=1

119908119902119894 [119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]1199021119902 (3)

where 120588 is the relative density in the variable density topologyoptimization and m is the total number of working condi-tions m=4 119908119894 is the weight coefficient of the ith workingcondition while q is the penalty coefficient (qge2) 119862119894(120588) is thestructural compliance of the ith working condition119862max

119894 and119862min119894 are the maximum and minimum compliance of the ith

working condition respectively

522 Dynamic Multiorder Natural Frequency The topologyoptimization of dynamic multiorder natural frequency isusually targeted at maximizing the low-order natural fre-quency and the material remove ratio is taken as boundaryHowever if only one low-order natural frequency is used asthe optimization objective the eigenvalues of other adjacenthigher order natural frequency may be reduced because ofthe gradual material remove in the structure It will result inthe interchange of the low-order natural frequencies and theconvergence of topology optimization will be influencedTheaverage frequency method [29] can consider simultaneouslythemultiorder natural frequency by defining a smooth objec-tive function and improve the convergence which is widelyused in dynamic topology optimization In this paper the

8 Mathematical Problems in Engineering

objective function of dynamic multiorder natural frequencyis defined by the average frequency method as shown in (4)Λ(120588) is the comprehensive evaluation value of the top feworder natural frequency and the larger the value the largerthe top few order natural frequency

maxΛ (120588) = 1205820 + 119904( 119899sum119895=1

119908119895120582119895 minus 1205820)minus1

(4)

where 120588 is the relative density in the variable density topologyoptimization 120582119895 is the jth order natural frequency 1205820 ands as given parameters are used to adjust the function valueusually 1205820=0 s=1 119908119895 is the weight coefficient of the jth ordernatural frequency while n is the order of low-order naturalfrequency that need to be optimized n=6

In addition the low-order natural frequency is usuallypaid to attention during the optimization process and thelower the order the higher the degree of attention Accordingto this principle aiming at reducing the complexity of theweighting coefficients determined by the analytic hierarchyprocess the weight coefficients 1199085 sim 11990810 of the top 6natural frequencies are taken as 03 02 02 01 01 and 01respectively So the 12 unknown weighting coefficients in thehierarchical structure model are reduced to six

523 Comprehensive Evaluation Function The comprehen-sive evaluation function of multiobjective topology opti-mization considering both the staticmultiworking conditionstiffness and the dynamic multiorder natural frequency isestablished by the compromise programming method asshown in (5) By adjusting the position of 119862119894(120588) and Λ 120588 inthe function the comprehensive evaluation function can uni-formly guide the convergence direction of the optimizationAnd the smaller the value the better the overall performanceof the cylinder block

min119865 (120588) = 12057221 [ 119898sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2

+ 12057222 [Λmax minus Λ (120588)Λmax minus Λmin ]212

(5)

where 119865(120588) is the objective function value and Λmin andΛmax representminimum andmaximumnatural frequenciesrespectively Other variables have the same meaning as (3)and (4)

53 The Weighting Coefficients The comprehensive evalua-tion function ofmultiobjective topology optimization shownin (5) has six unknown weighting coefficients including1205721 1205722 1199081 sim 1199084 These unknown weighting coefficientsare calculated based on the analytic hierarchy process inthis paper The concrete calculating flow chart is shownin Figure 9 The subjective judgment is scaled based onthe measure theory and the judgment matrix is established

Begin

Analyzing hierarchical structure model

Determining static anddynamic weight coefficients

Sort by the importance of working condition

Comparing the importancebetween two working conditions

Calculating the judgment matrix

Calculating the weight coefficientsof every working condition

consistency check

Conformity

All weight coefficients of multi-objectivetopology optimization is obtained

End

Criterionlayer

Index layerYes

No

Figure 9 The calculating flow chart of the weight coefficients

Then the all weighting coefficients are calculated through theconsistency check

531 Criteria Layer Decision There are static stiffness topol-ogy optimization and dynamic natural frequency topologyoptimization in the criterion layer and the correspondingweighting factors are respectively 1205721 1205722 The cylinder blocksuffers from the alternating impact loads when differentcylinder explodes and its stiffness performance directlyaffects the working reliability But for the vibration charac-teristics it can be seen from Section 42 that the maximumworking frequency is 100 Hz which is much smaller than thefirst-order natural frequency of 264 Hz Therefore the staticmultiworking condition stiffness is more important in thetopology optimization for the cylinder block So the weightcoefficients 1205721 1205722 are defined as 06 and 04 respectively

532 Index Layer Decision Firstly it is necessary to deter-mine the importance of four working conditions Accordingto the structure efficiency shown in Figure 7 the importanceis sorted the first cylinder the fourth cylinder the secondcylinder and the third cylinder So the weight coefficients areranked as shown in

1199081 gt 1199084 gt 1199082 gt 1199083 (6)

Mathematical Problems in Engineering 9

Table 6 Meanings of relative scale

Relative scale Meanings1 Two elements have equal importance3 The former is slightly important than the latter between two elements

5 The former is obviously important than the latter between twoelements

7 The former is strongly important than the latter between two elements

9 The former is extremely important than the latter between twoelements

2 4 6 8 Indicating the intermediate value above judgment

Reciprocal If the important ratio between the elements 119894 and 119895 is 119909 the importantratio between the elements 119895 and i is 1119909

Then according to the standard meaning table of relativescale in the AHP shown in Table 6 the relative importanceratio of four working conditions is determined and thejudgment matrix119882 is constructed as shown in

119882 =

[[[[[[[[[[[[[[[

11990811199081 1199081119908119894

1199081119908119899 1199081198951199081 119908119895119908119894

119908119895119908119899 1199081198991199081 119908119899119908119894

119908119899119908119899

]]]]]]]]]]]]]]]

=[[[[[[[[[[[

11990811 1199081119894 1199081119899 1199081198951 119908119895119894 119908119895119899 1199081198991 119908119899119894 119908119899119899

]]]]]]]]]]]

(7)

where n is the number of the weight coefficients 119908119894 and119908119895 (119894 119895 = 1 2 6) represent the weight coefficients and119908119895119894 = 119908119895119908119894 denotes the relative importance of 119908119895 to 119908119894According to the results in Section 4 the first cylinder

explosion is the worst condition and it is obviously moreimportant than the third working condition and slightlymore important than the fourth working condition so theweight coefficients 11990813 11990814 are determined as 5 and 2respectivelyThe importance of the secondworking conditionis between the third working condition and the fourthworking condition so the weight coefficient 11990812 is defined as4 In the same way the relative importance ratio of the fourworking conditions is obtained and the judgment matrix isconstructed

119882 =[[[[[[[[[[

1 4 5 214 1 2 1315 12 1 1412 3 4 1

]]]]]]]]]] (8)

The judgment matrix W is right multiplied by a vector120596 = (1199081 1199082 1199083 1199084)Τ consisting of all the weight coefficientsas shown in

119882120596 = 120582120596 997904rArr(119882 minus 120582119868)120596 = 0 (9)

Substituting the judgment matrix 119882 into (9) themaximum eigenvalue 120582max = 40484 is calculatedand the corresponding eigenvector normalized is 120596 =(049 012 008 031)Τ So all weight coefficients areobtained for multiobjective topology optimization of thecylinder block

In order to ensure the accuracy and reliability of thejudgment matrix and avoid influence of individual subjectivefactor the consistency test of the judgment matrix is carriedout in terms of (10) The consistency ratio CR of thejudgment matrixW calculated by (10) is 00179 which is lessthan 01 Therefore it is considered that the judgment matrixhas a satisfactory consistency and the four weight coefficientscan well reflect the importance of each working condition

119862119877 = 119862119868119877119868 (10)

where 119862119868 is the consistency index 119862119868 = (120582max minus119899)(119899 minus 1)119877119868 is the mean random consistency index whose value canbe obtained directly by referring to the standard randomconsistency index 119877119868-119899 table in the analytic hierarchyprocess as shown in Table 7 119862119877 is the random consistencyratio and the inconsistency is acceptable when 119862119877 lt 01

In addition the computing platform of weight coefficientfor multiworking condition topology optimization (TOWC)is built inMatlab to improve the computational efficiency ofthe method as shown in Figure 10 According to the numberof working conditions and the importance of each working

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

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Page 2: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

2 Mathematical Problems in Engineering

Multi-Objective Topology Optimization of the Cylinder Block

Geometric modelof cylinder block

Working-condition feature

Structuralfeature

The analysis of topologyoptimization space

The mathematical modelof topology optimization

Finite element model

modal analysis

Analyzing structure efficiency

static characteristic analysis

Hierarchical structure model

Establishing evaluation function

Determining weight coefficient

Mathematical model

Multi-working condition topology optimization

Verifying topology optimization results

Objective

Researchobject

Method

Results

Figure 1 The block diagram of multiobjective topology optimization

of diesel engine If the explosion of each cylinder for amulticylinder block is regarded as an extreme conditionthe topology optimization of the cylinder block belongs tothe typical multiworking condition problem The traditionalsingle objective optimization usually only ensures that themechanical properties are optimal in a certain workingcondition while the overall mechanical property may bereduced to a lower value in other working conditions thatis to say the topology optimization result for the cylinderblock will oscillate between different working conditions andthe overall mechanical property cannot be guaranteed Inaddition the dynamic characteristics of the cylinder blockalso need to be considered in the process of optimization

The multiobjective topology optimization can considersimultaneously several objective functions in the designprocess [13ndash15] and the optimal solution can be obtainedfor each objective function The intelligent algorithms areused to solve directly to avoid decision of multiobjectiveweight coefficients [16ndash18] However the calculation forcomplex structures will cost a lot of time and high economiccosts because of numerical instability during the process oftopology optimization [19 20] Therefore it is necessary toestablish a comprehensive evaluation function to considerseveral objectives as a whole But if the weight coefficientof each working condition is decided by the engineeringexperience the function will not reflect the overall structuralperformance in optimization So the method of determiningweight coefficients is the key of the multiobjective topol-ogy optimization and whose essence is the multicriteriondecision-making problem

The analytic hierarchy process (AHP) proposed by Saaty[21 22] is a systematic analysis method for determining

qualitatively and quantitatively the relative importance of aset of activities in a multicriteria decision-making problemThe method can effectively analyze the nonsequential rela-tionship between multiobjective criterion systems by com-bining mathematical processing with subjective judgmentwhich has been widely used in the field of resource systemanalysis economic management education managementsocial science and so on [23 24] The AHP is applied todeterminate the weight coefficients of the external economicevaluation model to ensure that the wind power engineeringproject is constructed and developed in a scientific manner[25] A multiobjective evolutionary structure optimizationmethod is proposed by combining the AHP and evolutionarystructural optimization which improves the optimizationeffect [26]Therefore it has obvious advantages to bring AHPinto the decision of weight coefficients for the multiobjectivetopology optimization

Under the above background this paper presents amultiobjective topology optimization method based on AHPwhich is applied to a certain four-cylinder diesel enginecylinder block

2 Multiobjective TopologyOptimization Method

The multiobjective topology optimization method of dieselengine cylinder block based on AHP in this paper is mainlydivided into four steps as shown in Figure 1 The firstis to introduce the structural geometry characteristic andworking condition of the cylinder block in Section 3 Sec-ondly the topology optimization space is determined on

Mathematical Problems in Engineering 3

Table 1 The mechanical property of HT300

Material Elastic modulus GPa Poissons ratio Density kg∙mminus3 Tensile strength MPaHT300 143 027 7300 300

z

y

x

1 2 3 4

(a) Front

z

y

x

(b) Back

Figure 2 The cylinder block structure

the basis of analyzing the static characteristics vibrationmode and structure efficiency of each working conditionin Section 4 Then in Section 5 the hierarchical structuremodel of topology optimization is constructed consideringthe static multiworking condition stiffness and dynamicmultiorder natural frequency The comprehensive evaluationfunction is established by the compromise programmingmethod which can more accurately evaluate the structuraloverall performance The weight coefficients are determinedby AHP and the mathematical model is established Finallymultiobjective topology optimization of cylinder block iscarried out and the optimization effect is verified in Section 6

3 Structure Analysis

31 Structure Feature The four-cylinder diesel engine cylin-der block as shown in Figure 2 is a box-type structureobtained by casting and machining and widely used inthe heavy engineering vehicle In order to achieve thelightweight the topology structure of the cylinder block hasbeen modified many times through finite element analysisand manual experience but the structure is still too cumber-some and unsatisfactory Its dimensions are 5267mm long3261mm wide and 3878mm high with a weight of 8897 kgThe material is gray cast iron HT300 and the mechanicalproperty is shown in Table 1

As the main structure of the diesel engine it is coveredwith various stiffening ribs convex plates bearing holes oilchannel holes water-cooled jacket and so on So its mechan-ical property is directly related to the working efficiency ofthe diesel engine and it has to possess sufficient strength andstiffness to support a variety of loads

32 Working Condition For the diesel engine cylinder blockits working condition is a cyclic process including four pro-cesses of intake compression power and exhaust The firingorder of cylinder block is 1-3-4-2 and the rotation speed ofcrank is 3000rpm Therefore there are alternating and high-speed impact loads for the cylinder block and the loads are

very complicated including the explosion pressure the wallpressure from crank-link mechanism the bolt pretighteningforce between cylinder block and cylinder head the reactionforce of bearing block and thermal load etc It is consideredthat the heat generated at the moment of gas explosion is firsttransmitted to the cylinder liner and then to the cylinderwallthe cylinder liner and the water-cooled jacket bear a largeamount of heat during the heat transfer process In order tosimplify calculation in this paper the thermal load on thecylinder wall is ignored So the main loads considered areshown in Figure 3

And the freedom constraints are applied to the six contactfaces ( a-f ) at the bottom of the cylinder block as shown inTable 2 where 119879x 119879y and 119879z mean that the displacementsof x y and z direction are limited 119877x 119877y and 119877z meanthat the rotation angles of x y and z direction are limitedAccording to the basic parameters of the cylinder block thecorresponding extreme load values at the moment of eachcylinder explosion are calculated as shown in Table 3 Thebolt pretightening force is different in different position of thebolt hole and the number of bolt holes is a great many onlythe maximum bolt pretightening force is listed

4 Optimization Space Analysis

41 Static Characteristics Analysis In order to obtain thetopology optimization space the static and dynamic char-acteristics of the cylinder block during the working processare obtained by the FEA The first is to carry out thestatic characteristics analysis at the moment of each cylinderexplosion

The geometry model is imported into the finite ele-ment software and the bolt hole chamfer and oil pipelineare simplified According to the working condition of thecylinder block in Section 32 the finite element modelconsisting of the tetrahedral andhexahedralmixing elementsis established as shown in Figure 4 The displacement andstress distribution are calculated and the results are shownin Table 4 It can be seen that the first working condition is

4 Mathematical Problems in Engineering

Table 2 The constraints of the cylinder block

Constraint face a b c d e fDisplacement freedoms 119879y 119879z 119879y 119879x 119879y 119879z 119879x 119879yRotation freedoms 119877x 119877y 119877z

Table 3 The extreme load value of each cylinder at the time of explosion

The extreme Loads No of explosion1 2 3 4

Bolt pre-tightening force N 69007 67586 69474 75693Reaction force of bearing blockN 63750 63336 47300 63752The wall pressure N 17695 17695 17695 17695The explosion pressure MPa 17 17 17 17

Explosion pressure

A

A A-Aa(f)

Wall pressure

Reaction force of bearing block

Bolt pre-tightening

force

1 2 3 4

b(e)z

y

x

c

d

(def) (abc)

Figure 3 The loads and boundary conditions of cylinder block

Figure 4 The finite element model

the worst and corresponding displacement and stress distri-bution cloud charts are shown in Figure 5 The maximumstress is 2179MPa located at the bolt hole while most of therest region is about 80 MPa which is much smaller than thematerial ultimate strength (300 MPa) It indicates that thecylinder block has optimization space in the worst condition

42 Modal Analysis The static analysis can only reflect struc-tural stiffness and strength and cannot reflect its vibrationperformance Modal analysis is the basis for the dynamicdesign analysis and optimization in modern mechanicalproducts The structural natural frequencies and vibrationmodes can be obtained by the modal analysis to evaluate itsvibration characteristics

Table 4 Results of FEA for the cylinder block

No ofexplosions

Maxstress(MPa)

Maxdisplacement

(mm)1 2179 02542 1688 02233 1684 02144 1992 0246

The constrained modal of the cylinder block is analyzedby the FEA and the top 6-order natural frequencies andcorresponding vibration modes are shown in Figure 6 and

Mathematical Problems in Engineering 5

Table 5 The top 6-order natural frequencies and vibration modes

Orders Frequency Vibration mode1 264Hz First-order torsional vibration around the X axis2 493 Hz First-order bending vibration around the Z axis3 531 Hz Second-order torsional vibration around the X axis4 562 Hz The skirt vibrates with torsion along the X direction5 778 Hz Whole bending torsional vibration6 1038 Hz Whole torsional vibrating around the X axis

(a) Displacement distribution (b) Stress distribution

Figure 5 Results of FEA under extreme working condition

Table 5 It can be seen from Figure 6 that the cylinder blockfirstly appears whole torsional vibration while the wholebending vibration appears in the higher frequency rangewhich show that the torsional stiffness is less than the bendingstiffness for the cylinder block In addition the relativedisplacement near the four corners is large and it is necessaryto improve the freedom constraints to lower the extent of thevibration

To further evaluate its dynamic performance theworkingfrequency is calculated by (1) The cylinder block studied inthis paper is a four-stroke reciprocating piston engine thecrankshaft turns twice and the cylinder body completes aworking cycle including four times vibration of intake com-pression power and exhaust So the corresponding workingfrequency f is 100Hz calculated which is much smaller thanthe first-order natural frequency for the cylinder block Itindicates that the resonance will not occur in working

119891 = 2 sdot 11989960 (1)

where n is the rotation speed of crank n=3000rpm

43 Structure Efficiency Analysis Structure efficiency [27]refers to the structural comprehensive characterization of thestrength and stiffness per unit weight in the case of meetingthe load-bearing property It is commonly used to evaluatethe structural overall performance The greater structural

efficiency the higher the material utilization while thesmaller the structural efficiency the larger the optimizationspace

In this paper the structure efficiency of the cylinder blockis calculated under four extreme working conditions Thecalculation formula of the structure efficiency index 120578119894 isshown in (2) In terms of the multiworking condition topol-ogy optimization its physical meaning is as follows the valueis greater indicating that thematerial utilization is higher andthe working condition is worse On the contrary it shows thatthe working condition is safer and the optimization space islarger

120578119894 = 120590119894max sdot 119889119894max119898 times 100 (2)

where 120578119894 is the structure efficiency index under the ith work-ing condition 120590119894max and 119889119894max are the maximum stress andmaximum displacement under the ith working conditionandm is the structural weight

Substituting the analysis results of Table 4 into (2) thestructure efficiency of the cylinder block is calculated asshown in Figure 7 It can be seen that the cylinder block hasthe highest structure efficiency at the moment of the firstcylinder explosion and followed by the fourth cylinder thesecond cylinder and the third cylinder It shows that the firstcylinder explosion is the worst working condition and thethird cylinder explosion is the safest condition

6 Mathematical Problems in Engineering

Contour Plot

4181E+003717E+003252E+002788E+002324E+001859E+001395E+00

Max = 4181E+00

Min = 1802E-03Grids 4612

Grids 32494

9306E-014662E-011802E-03

No result

Eigen Mode(Mag)Analysis system

(a) The first-order mode

Contour Plot

5090E+004600E+004111E+003621E+003131E+002641E+002152E+00

Max = 5090E+00

Min = 6824E-01Grids 7120

Grids 33177

1662E+001172E+006824E-01

No result

Eigen Mode(Mag)Analysis system

(b) The second-order mode

Contour Plot

5616E+004998E+004379E+003761E+003143E+002524E+001906E+00

Max = 5616E+00

Min = 5048E-02Grids 629

Grids 90051

1287E+00

5048E-026689E-01

No result

Eigen Mode(Mag)Analysis system

(c) The third-order mode

Contour Plot

9348E+008314E+007281E+006248E+005214E+004181E+003148E+00

Max = 9348E+00

Min = 4777E-02Grids 31763

Grids 19024

2114E+001081E+004777E-02

No result

Eigen Mode(Mag)Analysis system

(d) The fourth-order mode

Contour Plot

4681E+004258E+003835E+003412E+002989E+002566E+002143E+00

Max = 4681E+00

Min = 8739E-01Grids 98310

Grids 762

1720E+001297E+008739E-01

No result

Eigen Mode(Mag)Analysis system

(e) The fifth-order mode

Contour Plot

8861E+007876E+006892E+005907E+004923E+003938E+002954E+00

Max = 8861E+00

Min = 1354E-05Grids 4690

Grids 263900

1969E+00

1354E-059845E-01

No result

Eigen Mode(Mag)Analysis system

(f) The sixth-order mode

Figure 6 Results of modal analysis

0

20

40

60

80

1 2 3 4

struc

ture

effici

ency

the number of working conditions

Figure 7 The structure efficiency of each cylinder

Based on the analysis mentioned in Figures 5ndash7 thecylinder block studied in this paper can meet the stiffnessand strength requirements under the worst working con-dition The overall stress value (80 MPa) is much lower

than material ultimate strength (300 MPa) which indicatesthat the cylinder block has surplus material and topologyoptimization space Its working frequency (100 Hz) is muchlower than the first-order natural frequency (264 Hz) andthe resonance does not occur In addition the importancefor four working conditions is sorted the first cylinder thefourth cylinder the second cylinder and the third cylinderTherefore the first cylinder and the fourth cylinder shouldbe focused when determining the weighting coefficientsin multiobjective topology optimization And the materialnear the second cylinder and the third cylinder should beconsidered when improving the topology structure

5 Topology Optimization MathematicalModel Based on AHP

51 The Hierarchical Structure Model The topology opti-mization for the diesel engine cylinder block belongs to thetypical multiworking condition problem It is necessary to

Mathematical Problems in Engineering 7

The top 6-order natural

Topologyoptimizationof cylinder

block

Static topology

dynamic topology

target

criterionThe cylinder No1

The cylinder No2

The cylinder No3

The cylinder No4

index

optimization 2

optimization 1

of explosion w4

of explosion w3

of explosion w2

of explosion w1

frequencies w5 sim w10

Figure 8 The hierarchical structure model of topology optimization

take into account the structural performance requirementsincluding static and dynamic characteristics For the staticcharacteristics structural stiffness has to be considered atthe moment of each cylinder explosion And the top 6-order natural frequencies need to be concerned for dynamiccharacteristicsTherefore the hierarchical structure model oftopology optimization for the cylinder block is establishedbased on staticmultiworking condition stiffness and dynamicmultiorder natural frequency as shown in Figure 8 It canbe seen from the figure that the multiobjective topologyoptimization of the cylinder block includes 12 weightingcoefficients that are static and dynamic topology optimization1205721 1205722 in the criterion layer static multiworking conditionstiffness1199081 sim 1199084 and dynamic multiorder natural frequency1199085 sim 1199081052 Comprehensive Evaluation of the Cylinder Block Thelinear weighting method is usually used to transform themultiobjective problem into a single-objective problem forthe traditional multiobjective topology optimization How-ever the linear weighting method is to calculate weightaverage value for all functions and it cannot reflect the promi-nent influence from some certain functions which doesnot guarantee that all functions obtain the relative optimalsolutionThe compromise programmingmethod [28] can geta group of better relative optimal solutions by calculating thesensitivity of all functions to design variables and adjustingeach objective to balance each other From the hierarchicalstructuremodel shown in Figure 8 the topology optimizationfor the cylinder block includes ten optimization objectivesand the static and dynamic multiobjective optimizationproblem is converted into the single-objective optimizationproblem by the compromise programming method

521 Static Multiworking Condition Stiffness The topologyoptimization oriented by stiffnessmaximization is to research

material distribution form in the design domain to maxi-mize the structural stiffness In this paper the static stiff-ness of the cylinder block under four extreme conditionsis studied which belongs to the multiworking conditionstiffness problem In this paper the objective function ofstatic multiworking condition stiffness is obtained by thecompromise programming method as shown in (3) 119862(120588)is the comprehensive evaluation value of the static stiffnessand the smaller the value the larger the structural overallstiffness

min120588119862 (120588) = 119898sum

119894=1

119908119902119894 [119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]1199021119902 (3)

where 120588 is the relative density in the variable density topologyoptimization and m is the total number of working condi-tions m=4 119908119894 is the weight coefficient of the ith workingcondition while q is the penalty coefficient (qge2) 119862119894(120588) is thestructural compliance of the ith working condition119862max

119894 and119862min119894 are the maximum and minimum compliance of the ith

working condition respectively

522 Dynamic Multiorder Natural Frequency The topologyoptimization of dynamic multiorder natural frequency isusually targeted at maximizing the low-order natural fre-quency and the material remove ratio is taken as boundaryHowever if only one low-order natural frequency is used asthe optimization objective the eigenvalues of other adjacenthigher order natural frequency may be reduced because ofthe gradual material remove in the structure It will result inthe interchange of the low-order natural frequencies and theconvergence of topology optimization will be influencedTheaverage frequency method [29] can consider simultaneouslythemultiorder natural frequency by defining a smooth objec-tive function and improve the convergence which is widelyused in dynamic topology optimization In this paper the

8 Mathematical Problems in Engineering

objective function of dynamic multiorder natural frequencyis defined by the average frequency method as shown in (4)Λ(120588) is the comprehensive evaluation value of the top feworder natural frequency and the larger the value the largerthe top few order natural frequency

maxΛ (120588) = 1205820 + 119904( 119899sum119895=1

119908119895120582119895 minus 1205820)minus1

(4)

where 120588 is the relative density in the variable density topologyoptimization 120582119895 is the jth order natural frequency 1205820 ands as given parameters are used to adjust the function valueusually 1205820=0 s=1 119908119895 is the weight coefficient of the jth ordernatural frequency while n is the order of low-order naturalfrequency that need to be optimized n=6

In addition the low-order natural frequency is usuallypaid to attention during the optimization process and thelower the order the higher the degree of attention Accordingto this principle aiming at reducing the complexity of theweighting coefficients determined by the analytic hierarchyprocess the weight coefficients 1199085 sim 11990810 of the top 6natural frequencies are taken as 03 02 02 01 01 and 01respectively So the 12 unknown weighting coefficients in thehierarchical structure model are reduced to six

523 Comprehensive Evaluation Function The comprehen-sive evaluation function of multiobjective topology opti-mization considering both the staticmultiworking conditionstiffness and the dynamic multiorder natural frequency isestablished by the compromise programming method asshown in (5) By adjusting the position of 119862119894(120588) and Λ 120588 inthe function the comprehensive evaluation function can uni-formly guide the convergence direction of the optimizationAnd the smaller the value the better the overall performanceof the cylinder block

min119865 (120588) = 12057221 [ 119898sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2

+ 12057222 [Λmax minus Λ (120588)Λmax minus Λmin ]212

(5)

where 119865(120588) is the objective function value and Λmin andΛmax representminimum andmaximumnatural frequenciesrespectively Other variables have the same meaning as (3)and (4)

53 The Weighting Coefficients The comprehensive evalua-tion function ofmultiobjective topology optimization shownin (5) has six unknown weighting coefficients including1205721 1205722 1199081 sim 1199084 These unknown weighting coefficientsare calculated based on the analytic hierarchy process inthis paper The concrete calculating flow chart is shownin Figure 9 The subjective judgment is scaled based onthe measure theory and the judgment matrix is established

Begin

Analyzing hierarchical structure model

Determining static anddynamic weight coefficients

Sort by the importance of working condition

Comparing the importancebetween two working conditions

Calculating the judgment matrix

Calculating the weight coefficientsof every working condition

consistency check

Conformity

All weight coefficients of multi-objectivetopology optimization is obtained

End

Criterionlayer

Index layerYes

No

Figure 9 The calculating flow chart of the weight coefficients

Then the all weighting coefficients are calculated through theconsistency check

531 Criteria Layer Decision There are static stiffness topol-ogy optimization and dynamic natural frequency topologyoptimization in the criterion layer and the correspondingweighting factors are respectively 1205721 1205722 The cylinder blocksuffers from the alternating impact loads when differentcylinder explodes and its stiffness performance directlyaffects the working reliability But for the vibration charac-teristics it can be seen from Section 42 that the maximumworking frequency is 100 Hz which is much smaller than thefirst-order natural frequency of 264 Hz Therefore the staticmultiworking condition stiffness is more important in thetopology optimization for the cylinder block So the weightcoefficients 1205721 1205722 are defined as 06 and 04 respectively

532 Index Layer Decision Firstly it is necessary to deter-mine the importance of four working conditions Accordingto the structure efficiency shown in Figure 7 the importanceis sorted the first cylinder the fourth cylinder the secondcylinder and the third cylinder So the weight coefficients areranked as shown in

1199081 gt 1199084 gt 1199082 gt 1199083 (6)

Mathematical Problems in Engineering 9

Table 6 Meanings of relative scale

Relative scale Meanings1 Two elements have equal importance3 The former is slightly important than the latter between two elements

5 The former is obviously important than the latter between twoelements

7 The former is strongly important than the latter between two elements

9 The former is extremely important than the latter between twoelements

2 4 6 8 Indicating the intermediate value above judgment

Reciprocal If the important ratio between the elements 119894 and 119895 is 119909 the importantratio between the elements 119895 and i is 1119909

Then according to the standard meaning table of relativescale in the AHP shown in Table 6 the relative importanceratio of four working conditions is determined and thejudgment matrix119882 is constructed as shown in

119882 =

[[[[[[[[[[[[[[[

11990811199081 1199081119908119894

1199081119908119899 1199081198951199081 119908119895119908119894

119908119895119908119899 1199081198991199081 119908119899119908119894

119908119899119908119899

]]]]]]]]]]]]]]]

=[[[[[[[[[[[

11990811 1199081119894 1199081119899 1199081198951 119908119895119894 119908119895119899 1199081198991 119908119899119894 119908119899119899

]]]]]]]]]]]

(7)

where n is the number of the weight coefficients 119908119894 and119908119895 (119894 119895 = 1 2 6) represent the weight coefficients and119908119895119894 = 119908119895119908119894 denotes the relative importance of 119908119895 to 119908119894According to the results in Section 4 the first cylinder

explosion is the worst condition and it is obviously moreimportant than the third working condition and slightlymore important than the fourth working condition so theweight coefficients 11990813 11990814 are determined as 5 and 2respectivelyThe importance of the secondworking conditionis between the third working condition and the fourthworking condition so the weight coefficient 11990812 is defined as4 In the same way the relative importance ratio of the fourworking conditions is obtained and the judgment matrix isconstructed

119882 =[[[[[[[[[[

1 4 5 214 1 2 1315 12 1 1412 3 4 1

]]]]]]]]]] (8)

The judgment matrix W is right multiplied by a vector120596 = (1199081 1199082 1199083 1199084)Τ consisting of all the weight coefficientsas shown in

119882120596 = 120582120596 997904rArr(119882 minus 120582119868)120596 = 0 (9)

Substituting the judgment matrix 119882 into (9) themaximum eigenvalue 120582max = 40484 is calculatedand the corresponding eigenvector normalized is 120596 =(049 012 008 031)Τ So all weight coefficients areobtained for multiobjective topology optimization of thecylinder block

In order to ensure the accuracy and reliability of thejudgment matrix and avoid influence of individual subjectivefactor the consistency test of the judgment matrix is carriedout in terms of (10) The consistency ratio CR of thejudgment matrixW calculated by (10) is 00179 which is lessthan 01 Therefore it is considered that the judgment matrixhas a satisfactory consistency and the four weight coefficientscan well reflect the importance of each working condition

119862119877 = 119862119868119877119868 (10)

where 119862119868 is the consistency index 119862119868 = (120582max minus119899)(119899 minus 1)119877119868 is the mean random consistency index whose value canbe obtained directly by referring to the standard randomconsistency index 119877119868-119899 table in the analytic hierarchyprocess as shown in Table 7 119862119877 is the random consistencyratio and the inconsistency is acceptable when 119862119877 lt 01

In addition the computing platform of weight coefficientfor multiworking condition topology optimization (TOWC)is built inMatlab to improve the computational efficiency ofthe method as shown in Figure 10 According to the numberof working conditions and the importance of each working

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

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Page 3: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

Mathematical Problems in Engineering 3

Table 1 The mechanical property of HT300

Material Elastic modulus GPa Poissons ratio Density kg∙mminus3 Tensile strength MPaHT300 143 027 7300 300

z

y

x

1 2 3 4

(a) Front

z

y

x

(b) Back

Figure 2 The cylinder block structure

the basis of analyzing the static characteristics vibrationmode and structure efficiency of each working conditionin Section 4 Then in Section 5 the hierarchical structuremodel of topology optimization is constructed consideringthe static multiworking condition stiffness and dynamicmultiorder natural frequency The comprehensive evaluationfunction is established by the compromise programmingmethod which can more accurately evaluate the structuraloverall performance The weight coefficients are determinedby AHP and the mathematical model is established Finallymultiobjective topology optimization of cylinder block iscarried out and the optimization effect is verified in Section 6

3 Structure Analysis

31 Structure Feature The four-cylinder diesel engine cylin-der block as shown in Figure 2 is a box-type structureobtained by casting and machining and widely used inthe heavy engineering vehicle In order to achieve thelightweight the topology structure of the cylinder block hasbeen modified many times through finite element analysisand manual experience but the structure is still too cumber-some and unsatisfactory Its dimensions are 5267mm long3261mm wide and 3878mm high with a weight of 8897 kgThe material is gray cast iron HT300 and the mechanicalproperty is shown in Table 1

As the main structure of the diesel engine it is coveredwith various stiffening ribs convex plates bearing holes oilchannel holes water-cooled jacket and so on So its mechan-ical property is directly related to the working efficiency ofthe diesel engine and it has to possess sufficient strength andstiffness to support a variety of loads

32 Working Condition For the diesel engine cylinder blockits working condition is a cyclic process including four pro-cesses of intake compression power and exhaust The firingorder of cylinder block is 1-3-4-2 and the rotation speed ofcrank is 3000rpm Therefore there are alternating and high-speed impact loads for the cylinder block and the loads are

very complicated including the explosion pressure the wallpressure from crank-link mechanism the bolt pretighteningforce between cylinder block and cylinder head the reactionforce of bearing block and thermal load etc It is consideredthat the heat generated at the moment of gas explosion is firsttransmitted to the cylinder liner and then to the cylinderwallthe cylinder liner and the water-cooled jacket bear a largeamount of heat during the heat transfer process In order tosimplify calculation in this paper the thermal load on thecylinder wall is ignored So the main loads considered areshown in Figure 3

And the freedom constraints are applied to the six contactfaces ( a-f ) at the bottom of the cylinder block as shown inTable 2 where 119879x 119879y and 119879z mean that the displacementsof x y and z direction are limited 119877x 119877y and 119877z meanthat the rotation angles of x y and z direction are limitedAccording to the basic parameters of the cylinder block thecorresponding extreme load values at the moment of eachcylinder explosion are calculated as shown in Table 3 Thebolt pretightening force is different in different position of thebolt hole and the number of bolt holes is a great many onlythe maximum bolt pretightening force is listed

4 Optimization Space Analysis

41 Static Characteristics Analysis In order to obtain thetopology optimization space the static and dynamic char-acteristics of the cylinder block during the working processare obtained by the FEA The first is to carry out thestatic characteristics analysis at the moment of each cylinderexplosion

The geometry model is imported into the finite ele-ment software and the bolt hole chamfer and oil pipelineare simplified According to the working condition of thecylinder block in Section 32 the finite element modelconsisting of the tetrahedral andhexahedralmixing elementsis established as shown in Figure 4 The displacement andstress distribution are calculated and the results are shownin Table 4 It can be seen that the first working condition is

4 Mathematical Problems in Engineering

Table 2 The constraints of the cylinder block

Constraint face a b c d e fDisplacement freedoms 119879y 119879z 119879y 119879x 119879y 119879z 119879x 119879yRotation freedoms 119877x 119877y 119877z

Table 3 The extreme load value of each cylinder at the time of explosion

The extreme Loads No of explosion1 2 3 4

Bolt pre-tightening force N 69007 67586 69474 75693Reaction force of bearing blockN 63750 63336 47300 63752The wall pressure N 17695 17695 17695 17695The explosion pressure MPa 17 17 17 17

Explosion pressure

A

A A-Aa(f)

Wall pressure

Reaction force of bearing block

Bolt pre-tightening

force

1 2 3 4

b(e)z

y

x

c

d

(def) (abc)

Figure 3 The loads and boundary conditions of cylinder block

Figure 4 The finite element model

the worst and corresponding displacement and stress distri-bution cloud charts are shown in Figure 5 The maximumstress is 2179MPa located at the bolt hole while most of therest region is about 80 MPa which is much smaller than thematerial ultimate strength (300 MPa) It indicates that thecylinder block has optimization space in the worst condition

42 Modal Analysis The static analysis can only reflect struc-tural stiffness and strength and cannot reflect its vibrationperformance Modal analysis is the basis for the dynamicdesign analysis and optimization in modern mechanicalproducts The structural natural frequencies and vibrationmodes can be obtained by the modal analysis to evaluate itsvibration characteristics

Table 4 Results of FEA for the cylinder block

No ofexplosions

Maxstress(MPa)

Maxdisplacement

(mm)1 2179 02542 1688 02233 1684 02144 1992 0246

The constrained modal of the cylinder block is analyzedby the FEA and the top 6-order natural frequencies andcorresponding vibration modes are shown in Figure 6 and

Mathematical Problems in Engineering 5

Table 5 The top 6-order natural frequencies and vibration modes

Orders Frequency Vibration mode1 264Hz First-order torsional vibration around the X axis2 493 Hz First-order bending vibration around the Z axis3 531 Hz Second-order torsional vibration around the X axis4 562 Hz The skirt vibrates with torsion along the X direction5 778 Hz Whole bending torsional vibration6 1038 Hz Whole torsional vibrating around the X axis

(a) Displacement distribution (b) Stress distribution

Figure 5 Results of FEA under extreme working condition

Table 5 It can be seen from Figure 6 that the cylinder blockfirstly appears whole torsional vibration while the wholebending vibration appears in the higher frequency rangewhich show that the torsional stiffness is less than the bendingstiffness for the cylinder block In addition the relativedisplacement near the four corners is large and it is necessaryto improve the freedom constraints to lower the extent of thevibration

To further evaluate its dynamic performance theworkingfrequency is calculated by (1) The cylinder block studied inthis paper is a four-stroke reciprocating piston engine thecrankshaft turns twice and the cylinder body completes aworking cycle including four times vibration of intake com-pression power and exhaust So the corresponding workingfrequency f is 100Hz calculated which is much smaller thanthe first-order natural frequency for the cylinder block Itindicates that the resonance will not occur in working

119891 = 2 sdot 11989960 (1)

where n is the rotation speed of crank n=3000rpm

43 Structure Efficiency Analysis Structure efficiency [27]refers to the structural comprehensive characterization of thestrength and stiffness per unit weight in the case of meetingthe load-bearing property It is commonly used to evaluatethe structural overall performance The greater structural

efficiency the higher the material utilization while thesmaller the structural efficiency the larger the optimizationspace

In this paper the structure efficiency of the cylinder blockis calculated under four extreme working conditions Thecalculation formula of the structure efficiency index 120578119894 isshown in (2) In terms of the multiworking condition topol-ogy optimization its physical meaning is as follows the valueis greater indicating that thematerial utilization is higher andthe working condition is worse On the contrary it shows thatthe working condition is safer and the optimization space islarger

120578119894 = 120590119894max sdot 119889119894max119898 times 100 (2)

where 120578119894 is the structure efficiency index under the ith work-ing condition 120590119894max and 119889119894max are the maximum stress andmaximum displacement under the ith working conditionandm is the structural weight

Substituting the analysis results of Table 4 into (2) thestructure efficiency of the cylinder block is calculated asshown in Figure 7 It can be seen that the cylinder block hasthe highest structure efficiency at the moment of the firstcylinder explosion and followed by the fourth cylinder thesecond cylinder and the third cylinder It shows that the firstcylinder explosion is the worst working condition and thethird cylinder explosion is the safest condition

6 Mathematical Problems in Engineering

Contour Plot

4181E+003717E+003252E+002788E+002324E+001859E+001395E+00

Max = 4181E+00

Min = 1802E-03Grids 4612

Grids 32494

9306E-014662E-011802E-03

No result

Eigen Mode(Mag)Analysis system

(a) The first-order mode

Contour Plot

5090E+004600E+004111E+003621E+003131E+002641E+002152E+00

Max = 5090E+00

Min = 6824E-01Grids 7120

Grids 33177

1662E+001172E+006824E-01

No result

Eigen Mode(Mag)Analysis system

(b) The second-order mode

Contour Plot

5616E+004998E+004379E+003761E+003143E+002524E+001906E+00

Max = 5616E+00

Min = 5048E-02Grids 629

Grids 90051

1287E+00

5048E-026689E-01

No result

Eigen Mode(Mag)Analysis system

(c) The third-order mode

Contour Plot

9348E+008314E+007281E+006248E+005214E+004181E+003148E+00

Max = 9348E+00

Min = 4777E-02Grids 31763

Grids 19024

2114E+001081E+004777E-02

No result

Eigen Mode(Mag)Analysis system

(d) The fourth-order mode

Contour Plot

4681E+004258E+003835E+003412E+002989E+002566E+002143E+00

Max = 4681E+00

Min = 8739E-01Grids 98310

Grids 762

1720E+001297E+008739E-01

No result

Eigen Mode(Mag)Analysis system

(e) The fifth-order mode

Contour Plot

8861E+007876E+006892E+005907E+004923E+003938E+002954E+00

Max = 8861E+00

Min = 1354E-05Grids 4690

Grids 263900

1969E+00

1354E-059845E-01

No result

Eigen Mode(Mag)Analysis system

(f) The sixth-order mode

Figure 6 Results of modal analysis

0

20

40

60

80

1 2 3 4

struc

ture

effici

ency

the number of working conditions

Figure 7 The structure efficiency of each cylinder

Based on the analysis mentioned in Figures 5ndash7 thecylinder block studied in this paper can meet the stiffnessand strength requirements under the worst working con-dition The overall stress value (80 MPa) is much lower

than material ultimate strength (300 MPa) which indicatesthat the cylinder block has surplus material and topologyoptimization space Its working frequency (100 Hz) is muchlower than the first-order natural frequency (264 Hz) andthe resonance does not occur In addition the importancefor four working conditions is sorted the first cylinder thefourth cylinder the second cylinder and the third cylinderTherefore the first cylinder and the fourth cylinder shouldbe focused when determining the weighting coefficientsin multiobjective topology optimization And the materialnear the second cylinder and the third cylinder should beconsidered when improving the topology structure

5 Topology Optimization MathematicalModel Based on AHP

51 The Hierarchical Structure Model The topology opti-mization for the diesel engine cylinder block belongs to thetypical multiworking condition problem It is necessary to

Mathematical Problems in Engineering 7

The top 6-order natural

Topologyoptimizationof cylinder

block

Static topology

dynamic topology

target

criterionThe cylinder No1

The cylinder No2

The cylinder No3

The cylinder No4

index

optimization 2

optimization 1

of explosion w4

of explosion w3

of explosion w2

of explosion w1

frequencies w5 sim w10

Figure 8 The hierarchical structure model of topology optimization

take into account the structural performance requirementsincluding static and dynamic characteristics For the staticcharacteristics structural stiffness has to be considered atthe moment of each cylinder explosion And the top 6-order natural frequencies need to be concerned for dynamiccharacteristicsTherefore the hierarchical structure model oftopology optimization for the cylinder block is establishedbased on staticmultiworking condition stiffness and dynamicmultiorder natural frequency as shown in Figure 8 It canbe seen from the figure that the multiobjective topologyoptimization of the cylinder block includes 12 weightingcoefficients that are static and dynamic topology optimization1205721 1205722 in the criterion layer static multiworking conditionstiffness1199081 sim 1199084 and dynamic multiorder natural frequency1199085 sim 1199081052 Comprehensive Evaluation of the Cylinder Block Thelinear weighting method is usually used to transform themultiobjective problem into a single-objective problem forthe traditional multiobjective topology optimization How-ever the linear weighting method is to calculate weightaverage value for all functions and it cannot reflect the promi-nent influence from some certain functions which doesnot guarantee that all functions obtain the relative optimalsolutionThe compromise programmingmethod [28] can geta group of better relative optimal solutions by calculating thesensitivity of all functions to design variables and adjustingeach objective to balance each other From the hierarchicalstructuremodel shown in Figure 8 the topology optimizationfor the cylinder block includes ten optimization objectivesand the static and dynamic multiobjective optimizationproblem is converted into the single-objective optimizationproblem by the compromise programming method

521 Static Multiworking Condition Stiffness The topologyoptimization oriented by stiffnessmaximization is to research

material distribution form in the design domain to maxi-mize the structural stiffness In this paper the static stiff-ness of the cylinder block under four extreme conditionsis studied which belongs to the multiworking conditionstiffness problem In this paper the objective function ofstatic multiworking condition stiffness is obtained by thecompromise programming method as shown in (3) 119862(120588)is the comprehensive evaluation value of the static stiffnessand the smaller the value the larger the structural overallstiffness

min120588119862 (120588) = 119898sum

119894=1

119908119902119894 [119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]1199021119902 (3)

where 120588 is the relative density in the variable density topologyoptimization and m is the total number of working condi-tions m=4 119908119894 is the weight coefficient of the ith workingcondition while q is the penalty coefficient (qge2) 119862119894(120588) is thestructural compliance of the ith working condition119862max

119894 and119862min119894 are the maximum and minimum compliance of the ith

working condition respectively

522 Dynamic Multiorder Natural Frequency The topologyoptimization of dynamic multiorder natural frequency isusually targeted at maximizing the low-order natural fre-quency and the material remove ratio is taken as boundaryHowever if only one low-order natural frequency is used asthe optimization objective the eigenvalues of other adjacenthigher order natural frequency may be reduced because ofthe gradual material remove in the structure It will result inthe interchange of the low-order natural frequencies and theconvergence of topology optimization will be influencedTheaverage frequency method [29] can consider simultaneouslythemultiorder natural frequency by defining a smooth objec-tive function and improve the convergence which is widelyused in dynamic topology optimization In this paper the

8 Mathematical Problems in Engineering

objective function of dynamic multiorder natural frequencyis defined by the average frequency method as shown in (4)Λ(120588) is the comprehensive evaluation value of the top feworder natural frequency and the larger the value the largerthe top few order natural frequency

maxΛ (120588) = 1205820 + 119904( 119899sum119895=1

119908119895120582119895 minus 1205820)minus1

(4)

where 120588 is the relative density in the variable density topologyoptimization 120582119895 is the jth order natural frequency 1205820 ands as given parameters are used to adjust the function valueusually 1205820=0 s=1 119908119895 is the weight coefficient of the jth ordernatural frequency while n is the order of low-order naturalfrequency that need to be optimized n=6

In addition the low-order natural frequency is usuallypaid to attention during the optimization process and thelower the order the higher the degree of attention Accordingto this principle aiming at reducing the complexity of theweighting coefficients determined by the analytic hierarchyprocess the weight coefficients 1199085 sim 11990810 of the top 6natural frequencies are taken as 03 02 02 01 01 and 01respectively So the 12 unknown weighting coefficients in thehierarchical structure model are reduced to six

523 Comprehensive Evaluation Function The comprehen-sive evaluation function of multiobjective topology opti-mization considering both the staticmultiworking conditionstiffness and the dynamic multiorder natural frequency isestablished by the compromise programming method asshown in (5) By adjusting the position of 119862119894(120588) and Λ 120588 inthe function the comprehensive evaluation function can uni-formly guide the convergence direction of the optimizationAnd the smaller the value the better the overall performanceof the cylinder block

min119865 (120588) = 12057221 [ 119898sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2

+ 12057222 [Λmax minus Λ (120588)Λmax minus Λmin ]212

(5)

where 119865(120588) is the objective function value and Λmin andΛmax representminimum andmaximumnatural frequenciesrespectively Other variables have the same meaning as (3)and (4)

53 The Weighting Coefficients The comprehensive evalua-tion function ofmultiobjective topology optimization shownin (5) has six unknown weighting coefficients including1205721 1205722 1199081 sim 1199084 These unknown weighting coefficientsare calculated based on the analytic hierarchy process inthis paper The concrete calculating flow chart is shownin Figure 9 The subjective judgment is scaled based onthe measure theory and the judgment matrix is established

Begin

Analyzing hierarchical structure model

Determining static anddynamic weight coefficients

Sort by the importance of working condition

Comparing the importancebetween two working conditions

Calculating the judgment matrix

Calculating the weight coefficientsof every working condition

consistency check

Conformity

All weight coefficients of multi-objectivetopology optimization is obtained

End

Criterionlayer

Index layerYes

No

Figure 9 The calculating flow chart of the weight coefficients

Then the all weighting coefficients are calculated through theconsistency check

531 Criteria Layer Decision There are static stiffness topol-ogy optimization and dynamic natural frequency topologyoptimization in the criterion layer and the correspondingweighting factors are respectively 1205721 1205722 The cylinder blocksuffers from the alternating impact loads when differentcylinder explodes and its stiffness performance directlyaffects the working reliability But for the vibration charac-teristics it can be seen from Section 42 that the maximumworking frequency is 100 Hz which is much smaller than thefirst-order natural frequency of 264 Hz Therefore the staticmultiworking condition stiffness is more important in thetopology optimization for the cylinder block So the weightcoefficients 1205721 1205722 are defined as 06 and 04 respectively

532 Index Layer Decision Firstly it is necessary to deter-mine the importance of four working conditions Accordingto the structure efficiency shown in Figure 7 the importanceis sorted the first cylinder the fourth cylinder the secondcylinder and the third cylinder So the weight coefficients areranked as shown in

1199081 gt 1199084 gt 1199082 gt 1199083 (6)

Mathematical Problems in Engineering 9

Table 6 Meanings of relative scale

Relative scale Meanings1 Two elements have equal importance3 The former is slightly important than the latter between two elements

5 The former is obviously important than the latter between twoelements

7 The former is strongly important than the latter between two elements

9 The former is extremely important than the latter between twoelements

2 4 6 8 Indicating the intermediate value above judgment

Reciprocal If the important ratio between the elements 119894 and 119895 is 119909 the importantratio between the elements 119895 and i is 1119909

Then according to the standard meaning table of relativescale in the AHP shown in Table 6 the relative importanceratio of four working conditions is determined and thejudgment matrix119882 is constructed as shown in

119882 =

[[[[[[[[[[[[[[[

11990811199081 1199081119908119894

1199081119908119899 1199081198951199081 119908119895119908119894

119908119895119908119899 1199081198991199081 119908119899119908119894

119908119899119908119899

]]]]]]]]]]]]]]]

=[[[[[[[[[[[

11990811 1199081119894 1199081119899 1199081198951 119908119895119894 119908119895119899 1199081198991 119908119899119894 119908119899119899

]]]]]]]]]]]

(7)

where n is the number of the weight coefficients 119908119894 and119908119895 (119894 119895 = 1 2 6) represent the weight coefficients and119908119895119894 = 119908119895119908119894 denotes the relative importance of 119908119895 to 119908119894According to the results in Section 4 the first cylinder

explosion is the worst condition and it is obviously moreimportant than the third working condition and slightlymore important than the fourth working condition so theweight coefficients 11990813 11990814 are determined as 5 and 2respectivelyThe importance of the secondworking conditionis between the third working condition and the fourthworking condition so the weight coefficient 11990812 is defined as4 In the same way the relative importance ratio of the fourworking conditions is obtained and the judgment matrix isconstructed

119882 =[[[[[[[[[[

1 4 5 214 1 2 1315 12 1 1412 3 4 1

]]]]]]]]]] (8)

The judgment matrix W is right multiplied by a vector120596 = (1199081 1199082 1199083 1199084)Τ consisting of all the weight coefficientsas shown in

119882120596 = 120582120596 997904rArr(119882 minus 120582119868)120596 = 0 (9)

Substituting the judgment matrix 119882 into (9) themaximum eigenvalue 120582max = 40484 is calculatedand the corresponding eigenvector normalized is 120596 =(049 012 008 031)Τ So all weight coefficients areobtained for multiobjective topology optimization of thecylinder block

In order to ensure the accuracy and reliability of thejudgment matrix and avoid influence of individual subjectivefactor the consistency test of the judgment matrix is carriedout in terms of (10) The consistency ratio CR of thejudgment matrixW calculated by (10) is 00179 which is lessthan 01 Therefore it is considered that the judgment matrixhas a satisfactory consistency and the four weight coefficientscan well reflect the importance of each working condition

119862119877 = 119862119868119877119868 (10)

where 119862119868 is the consistency index 119862119868 = (120582max minus119899)(119899 minus 1)119877119868 is the mean random consistency index whose value canbe obtained directly by referring to the standard randomconsistency index 119877119868-119899 table in the analytic hierarchyprocess as shown in Table 7 119862119877 is the random consistencyratio and the inconsistency is acceptable when 119862119877 lt 01

In addition the computing platform of weight coefficientfor multiworking condition topology optimization (TOWC)is built inMatlab to improve the computational efficiency ofthe method as shown in Figure 10 According to the numberof working conditions and the importance of each working

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

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Page 4: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

4 Mathematical Problems in Engineering

Table 2 The constraints of the cylinder block

Constraint face a b c d e fDisplacement freedoms 119879y 119879z 119879y 119879x 119879y 119879z 119879x 119879yRotation freedoms 119877x 119877y 119877z

Table 3 The extreme load value of each cylinder at the time of explosion

The extreme Loads No of explosion1 2 3 4

Bolt pre-tightening force N 69007 67586 69474 75693Reaction force of bearing blockN 63750 63336 47300 63752The wall pressure N 17695 17695 17695 17695The explosion pressure MPa 17 17 17 17

Explosion pressure

A

A A-Aa(f)

Wall pressure

Reaction force of bearing block

Bolt pre-tightening

force

1 2 3 4

b(e)z

y

x

c

d

(def) (abc)

Figure 3 The loads and boundary conditions of cylinder block

Figure 4 The finite element model

the worst and corresponding displacement and stress distri-bution cloud charts are shown in Figure 5 The maximumstress is 2179MPa located at the bolt hole while most of therest region is about 80 MPa which is much smaller than thematerial ultimate strength (300 MPa) It indicates that thecylinder block has optimization space in the worst condition

42 Modal Analysis The static analysis can only reflect struc-tural stiffness and strength and cannot reflect its vibrationperformance Modal analysis is the basis for the dynamicdesign analysis and optimization in modern mechanicalproducts The structural natural frequencies and vibrationmodes can be obtained by the modal analysis to evaluate itsvibration characteristics

Table 4 Results of FEA for the cylinder block

No ofexplosions

Maxstress(MPa)

Maxdisplacement

(mm)1 2179 02542 1688 02233 1684 02144 1992 0246

The constrained modal of the cylinder block is analyzedby the FEA and the top 6-order natural frequencies andcorresponding vibration modes are shown in Figure 6 and

Mathematical Problems in Engineering 5

Table 5 The top 6-order natural frequencies and vibration modes

Orders Frequency Vibration mode1 264Hz First-order torsional vibration around the X axis2 493 Hz First-order bending vibration around the Z axis3 531 Hz Second-order torsional vibration around the X axis4 562 Hz The skirt vibrates with torsion along the X direction5 778 Hz Whole bending torsional vibration6 1038 Hz Whole torsional vibrating around the X axis

(a) Displacement distribution (b) Stress distribution

Figure 5 Results of FEA under extreme working condition

Table 5 It can be seen from Figure 6 that the cylinder blockfirstly appears whole torsional vibration while the wholebending vibration appears in the higher frequency rangewhich show that the torsional stiffness is less than the bendingstiffness for the cylinder block In addition the relativedisplacement near the four corners is large and it is necessaryto improve the freedom constraints to lower the extent of thevibration

To further evaluate its dynamic performance theworkingfrequency is calculated by (1) The cylinder block studied inthis paper is a four-stroke reciprocating piston engine thecrankshaft turns twice and the cylinder body completes aworking cycle including four times vibration of intake com-pression power and exhaust So the corresponding workingfrequency f is 100Hz calculated which is much smaller thanthe first-order natural frequency for the cylinder block Itindicates that the resonance will not occur in working

119891 = 2 sdot 11989960 (1)

where n is the rotation speed of crank n=3000rpm

43 Structure Efficiency Analysis Structure efficiency [27]refers to the structural comprehensive characterization of thestrength and stiffness per unit weight in the case of meetingthe load-bearing property It is commonly used to evaluatethe structural overall performance The greater structural

efficiency the higher the material utilization while thesmaller the structural efficiency the larger the optimizationspace

In this paper the structure efficiency of the cylinder blockis calculated under four extreme working conditions Thecalculation formula of the structure efficiency index 120578119894 isshown in (2) In terms of the multiworking condition topol-ogy optimization its physical meaning is as follows the valueis greater indicating that thematerial utilization is higher andthe working condition is worse On the contrary it shows thatthe working condition is safer and the optimization space islarger

120578119894 = 120590119894max sdot 119889119894max119898 times 100 (2)

where 120578119894 is the structure efficiency index under the ith work-ing condition 120590119894max and 119889119894max are the maximum stress andmaximum displacement under the ith working conditionandm is the structural weight

Substituting the analysis results of Table 4 into (2) thestructure efficiency of the cylinder block is calculated asshown in Figure 7 It can be seen that the cylinder block hasthe highest structure efficiency at the moment of the firstcylinder explosion and followed by the fourth cylinder thesecond cylinder and the third cylinder It shows that the firstcylinder explosion is the worst working condition and thethird cylinder explosion is the safest condition

6 Mathematical Problems in Engineering

Contour Plot

4181E+003717E+003252E+002788E+002324E+001859E+001395E+00

Max = 4181E+00

Min = 1802E-03Grids 4612

Grids 32494

9306E-014662E-011802E-03

No result

Eigen Mode(Mag)Analysis system

(a) The first-order mode

Contour Plot

5090E+004600E+004111E+003621E+003131E+002641E+002152E+00

Max = 5090E+00

Min = 6824E-01Grids 7120

Grids 33177

1662E+001172E+006824E-01

No result

Eigen Mode(Mag)Analysis system

(b) The second-order mode

Contour Plot

5616E+004998E+004379E+003761E+003143E+002524E+001906E+00

Max = 5616E+00

Min = 5048E-02Grids 629

Grids 90051

1287E+00

5048E-026689E-01

No result

Eigen Mode(Mag)Analysis system

(c) The third-order mode

Contour Plot

9348E+008314E+007281E+006248E+005214E+004181E+003148E+00

Max = 9348E+00

Min = 4777E-02Grids 31763

Grids 19024

2114E+001081E+004777E-02

No result

Eigen Mode(Mag)Analysis system

(d) The fourth-order mode

Contour Plot

4681E+004258E+003835E+003412E+002989E+002566E+002143E+00

Max = 4681E+00

Min = 8739E-01Grids 98310

Grids 762

1720E+001297E+008739E-01

No result

Eigen Mode(Mag)Analysis system

(e) The fifth-order mode

Contour Plot

8861E+007876E+006892E+005907E+004923E+003938E+002954E+00

Max = 8861E+00

Min = 1354E-05Grids 4690

Grids 263900

1969E+00

1354E-059845E-01

No result

Eigen Mode(Mag)Analysis system

(f) The sixth-order mode

Figure 6 Results of modal analysis

0

20

40

60

80

1 2 3 4

struc

ture

effici

ency

the number of working conditions

Figure 7 The structure efficiency of each cylinder

Based on the analysis mentioned in Figures 5ndash7 thecylinder block studied in this paper can meet the stiffnessand strength requirements under the worst working con-dition The overall stress value (80 MPa) is much lower

than material ultimate strength (300 MPa) which indicatesthat the cylinder block has surplus material and topologyoptimization space Its working frequency (100 Hz) is muchlower than the first-order natural frequency (264 Hz) andthe resonance does not occur In addition the importancefor four working conditions is sorted the first cylinder thefourth cylinder the second cylinder and the third cylinderTherefore the first cylinder and the fourth cylinder shouldbe focused when determining the weighting coefficientsin multiobjective topology optimization And the materialnear the second cylinder and the third cylinder should beconsidered when improving the topology structure

5 Topology Optimization MathematicalModel Based on AHP

51 The Hierarchical Structure Model The topology opti-mization for the diesel engine cylinder block belongs to thetypical multiworking condition problem It is necessary to

Mathematical Problems in Engineering 7

The top 6-order natural

Topologyoptimizationof cylinder

block

Static topology

dynamic topology

target

criterionThe cylinder No1

The cylinder No2

The cylinder No3

The cylinder No4

index

optimization 2

optimization 1

of explosion w4

of explosion w3

of explosion w2

of explosion w1

frequencies w5 sim w10

Figure 8 The hierarchical structure model of topology optimization

take into account the structural performance requirementsincluding static and dynamic characteristics For the staticcharacteristics structural stiffness has to be considered atthe moment of each cylinder explosion And the top 6-order natural frequencies need to be concerned for dynamiccharacteristicsTherefore the hierarchical structure model oftopology optimization for the cylinder block is establishedbased on staticmultiworking condition stiffness and dynamicmultiorder natural frequency as shown in Figure 8 It canbe seen from the figure that the multiobjective topologyoptimization of the cylinder block includes 12 weightingcoefficients that are static and dynamic topology optimization1205721 1205722 in the criterion layer static multiworking conditionstiffness1199081 sim 1199084 and dynamic multiorder natural frequency1199085 sim 1199081052 Comprehensive Evaluation of the Cylinder Block Thelinear weighting method is usually used to transform themultiobjective problem into a single-objective problem forthe traditional multiobjective topology optimization How-ever the linear weighting method is to calculate weightaverage value for all functions and it cannot reflect the promi-nent influence from some certain functions which doesnot guarantee that all functions obtain the relative optimalsolutionThe compromise programmingmethod [28] can geta group of better relative optimal solutions by calculating thesensitivity of all functions to design variables and adjustingeach objective to balance each other From the hierarchicalstructuremodel shown in Figure 8 the topology optimizationfor the cylinder block includes ten optimization objectivesand the static and dynamic multiobjective optimizationproblem is converted into the single-objective optimizationproblem by the compromise programming method

521 Static Multiworking Condition Stiffness The topologyoptimization oriented by stiffnessmaximization is to research

material distribution form in the design domain to maxi-mize the structural stiffness In this paper the static stiff-ness of the cylinder block under four extreme conditionsis studied which belongs to the multiworking conditionstiffness problem In this paper the objective function ofstatic multiworking condition stiffness is obtained by thecompromise programming method as shown in (3) 119862(120588)is the comprehensive evaluation value of the static stiffnessand the smaller the value the larger the structural overallstiffness

min120588119862 (120588) = 119898sum

119894=1

119908119902119894 [119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]1199021119902 (3)

where 120588 is the relative density in the variable density topologyoptimization and m is the total number of working condi-tions m=4 119908119894 is the weight coefficient of the ith workingcondition while q is the penalty coefficient (qge2) 119862119894(120588) is thestructural compliance of the ith working condition119862max

119894 and119862min119894 are the maximum and minimum compliance of the ith

working condition respectively

522 Dynamic Multiorder Natural Frequency The topologyoptimization of dynamic multiorder natural frequency isusually targeted at maximizing the low-order natural fre-quency and the material remove ratio is taken as boundaryHowever if only one low-order natural frequency is used asthe optimization objective the eigenvalues of other adjacenthigher order natural frequency may be reduced because ofthe gradual material remove in the structure It will result inthe interchange of the low-order natural frequencies and theconvergence of topology optimization will be influencedTheaverage frequency method [29] can consider simultaneouslythemultiorder natural frequency by defining a smooth objec-tive function and improve the convergence which is widelyused in dynamic topology optimization In this paper the

8 Mathematical Problems in Engineering

objective function of dynamic multiorder natural frequencyis defined by the average frequency method as shown in (4)Λ(120588) is the comprehensive evaluation value of the top feworder natural frequency and the larger the value the largerthe top few order natural frequency

maxΛ (120588) = 1205820 + 119904( 119899sum119895=1

119908119895120582119895 minus 1205820)minus1

(4)

where 120588 is the relative density in the variable density topologyoptimization 120582119895 is the jth order natural frequency 1205820 ands as given parameters are used to adjust the function valueusually 1205820=0 s=1 119908119895 is the weight coefficient of the jth ordernatural frequency while n is the order of low-order naturalfrequency that need to be optimized n=6

In addition the low-order natural frequency is usuallypaid to attention during the optimization process and thelower the order the higher the degree of attention Accordingto this principle aiming at reducing the complexity of theweighting coefficients determined by the analytic hierarchyprocess the weight coefficients 1199085 sim 11990810 of the top 6natural frequencies are taken as 03 02 02 01 01 and 01respectively So the 12 unknown weighting coefficients in thehierarchical structure model are reduced to six

523 Comprehensive Evaluation Function The comprehen-sive evaluation function of multiobjective topology opti-mization considering both the staticmultiworking conditionstiffness and the dynamic multiorder natural frequency isestablished by the compromise programming method asshown in (5) By adjusting the position of 119862119894(120588) and Λ 120588 inthe function the comprehensive evaluation function can uni-formly guide the convergence direction of the optimizationAnd the smaller the value the better the overall performanceof the cylinder block

min119865 (120588) = 12057221 [ 119898sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2

+ 12057222 [Λmax minus Λ (120588)Λmax minus Λmin ]212

(5)

where 119865(120588) is the objective function value and Λmin andΛmax representminimum andmaximumnatural frequenciesrespectively Other variables have the same meaning as (3)and (4)

53 The Weighting Coefficients The comprehensive evalua-tion function ofmultiobjective topology optimization shownin (5) has six unknown weighting coefficients including1205721 1205722 1199081 sim 1199084 These unknown weighting coefficientsare calculated based on the analytic hierarchy process inthis paper The concrete calculating flow chart is shownin Figure 9 The subjective judgment is scaled based onthe measure theory and the judgment matrix is established

Begin

Analyzing hierarchical structure model

Determining static anddynamic weight coefficients

Sort by the importance of working condition

Comparing the importancebetween two working conditions

Calculating the judgment matrix

Calculating the weight coefficientsof every working condition

consistency check

Conformity

All weight coefficients of multi-objectivetopology optimization is obtained

End

Criterionlayer

Index layerYes

No

Figure 9 The calculating flow chart of the weight coefficients

Then the all weighting coefficients are calculated through theconsistency check

531 Criteria Layer Decision There are static stiffness topol-ogy optimization and dynamic natural frequency topologyoptimization in the criterion layer and the correspondingweighting factors are respectively 1205721 1205722 The cylinder blocksuffers from the alternating impact loads when differentcylinder explodes and its stiffness performance directlyaffects the working reliability But for the vibration charac-teristics it can be seen from Section 42 that the maximumworking frequency is 100 Hz which is much smaller than thefirst-order natural frequency of 264 Hz Therefore the staticmultiworking condition stiffness is more important in thetopology optimization for the cylinder block So the weightcoefficients 1205721 1205722 are defined as 06 and 04 respectively

532 Index Layer Decision Firstly it is necessary to deter-mine the importance of four working conditions Accordingto the structure efficiency shown in Figure 7 the importanceis sorted the first cylinder the fourth cylinder the secondcylinder and the third cylinder So the weight coefficients areranked as shown in

1199081 gt 1199084 gt 1199082 gt 1199083 (6)

Mathematical Problems in Engineering 9

Table 6 Meanings of relative scale

Relative scale Meanings1 Two elements have equal importance3 The former is slightly important than the latter between two elements

5 The former is obviously important than the latter between twoelements

7 The former is strongly important than the latter between two elements

9 The former is extremely important than the latter between twoelements

2 4 6 8 Indicating the intermediate value above judgment

Reciprocal If the important ratio between the elements 119894 and 119895 is 119909 the importantratio between the elements 119895 and i is 1119909

Then according to the standard meaning table of relativescale in the AHP shown in Table 6 the relative importanceratio of four working conditions is determined and thejudgment matrix119882 is constructed as shown in

119882 =

[[[[[[[[[[[[[[[

11990811199081 1199081119908119894

1199081119908119899 1199081198951199081 119908119895119908119894

119908119895119908119899 1199081198991199081 119908119899119908119894

119908119899119908119899

]]]]]]]]]]]]]]]

=[[[[[[[[[[[

11990811 1199081119894 1199081119899 1199081198951 119908119895119894 119908119895119899 1199081198991 119908119899119894 119908119899119899

]]]]]]]]]]]

(7)

where n is the number of the weight coefficients 119908119894 and119908119895 (119894 119895 = 1 2 6) represent the weight coefficients and119908119895119894 = 119908119895119908119894 denotes the relative importance of 119908119895 to 119908119894According to the results in Section 4 the first cylinder

explosion is the worst condition and it is obviously moreimportant than the third working condition and slightlymore important than the fourth working condition so theweight coefficients 11990813 11990814 are determined as 5 and 2respectivelyThe importance of the secondworking conditionis between the third working condition and the fourthworking condition so the weight coefficient 11990812 is defined as4 In the same way the relative importance ratio of the fourworking conditions is obtained and the judgment matrix isconstructed

119882 =[[[[[[[[[[

1 4 5 214 1 2 1315 12 1 1412 3 4 1

]]]]]]]]]] (8)

The judgment matrix W is right multiplied by a vector120596 = (1199081 1199082 1199083 1199084)Τ consisting of all the weight coefficientsas shown in

119882120596 = 120582120596 997904rArr(119882 minus 120582119868)120596 = 0 (9)

Substituting the judgment matrix 119882 into (9) themaximum eigenvalue 120582max = 40484 is calculatedand the corresponding eigenvector normalized is 120596 =(049 012 008 031)Τ So all weight coefficients areobtained for multiobjective topology optimization of thecylinder block

In order to ensure the accuracy and reliability of thejudgment matrix and avoid influence of individual subjectivefactor the consistency test of the judgment matrix is carriedout in terms of (10) The consistency ratio CR of thejudgment matrixW calculated by (10) is 00179 which is lessthan 01 Therefore it is considered that the judgment matrixhas a satisfactory consistency and the four weight coefficientscan well reflect the importance of each working condition

119862119877 = 119862119868119877119868 (10)

where 119862119868 is the consistency index 119862119868 = (120582max minus119899)(119899 minus 1)119877119868 is the mean random consistency index whose value canbe obtained directly by referring to the standard randomconsistency index 119877119868-119899 table in the analytic hierarchyprocess as shown in Table 7 119862119877 is the random consistencyratio and the inconsistency is acceptable when 119862119877 lt 01

In addition the computing platform of weight coefficientfor multiworking condition topology optimization (TOWC)is built inMatlab to improve the computational efficiency ofthe method as shown in Figure 10 According to the numberof working conditions and the importance of each working

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

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Page 5: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

Mathematical Problems in Engineering 5

Table 5 The top 6-order natural frequencies and vibration modes

Orders Frequency Vibration mode1 264Hz First-order torsional vibration around the X axis2 493 Hz First-order bending vibration around the Z axis3 531 Hz Second-order torsional vibration around the X axis4 562 Hz The skirt vibrates with torsion along the X direction5 778 Hz Whole bending torsional vibration6 1038 Hz Whole torsional vibrating around the X axis

(a) Displacement distribution (b) Stress distribution

Figure 5 Results of FEA under extreme working condition

Table 5 It can be seen from Figure 6 that the cylinder blockfirstly appears whole torsional vibration while the wholebending vibration appears in the higher frequency rangewhich show that the torsional stiffness is less than the bendingstiffness for the cylinder block In addition the relativedisplacement near the four corners is large and it is necessaryto improve the freedom constraints to lower the extent of thevibration

To further evaluate its dynamic performance theworkingfrequency is calculated by (1) The cylinder block studied inthis paper is a four-stroke reciprocating piston engine thecrankshaft turns twice and the cylinder body completes aworking cycle including four times vibration of intake com-pression power and exhaust So the corresponding workingfrequency f is 100Hz calculated which is much smaller thanthe first-order natural frequency for the cylinder block Itindicates that the resonance will not occur in working

119891 = 2 sdot 11989960 (1)

where n is the rotation speed of crank n=3000rpm

43 Structure Efficiency Analysis Structure efficiency [27]refers to the structural comprehensive characterization of thestrength and stiffness per unit weight in the case of meetingthe load-bearing property It is commonly used to evaluatethe structural overall performance The greater structural

efficiency the higher the material utilization while thesmaller the structural efficiency the larger the optimizationspace

In this paper the structure efficiency of the cylinder blockis calculated under four extreme working conditions Thecalculation formula of the structure efficiency index 120578119894 isshown in (2) In terms of the multiworking condition topol-ogy optimization its physical meaning is as follows the valueis greater indicating that thematerial utilization is higher andthe working condition is worse On the contrary it shows thatthe working condition is safer and the optimization space islarger

120578119894 = 120590119894max sdot 119889119894max119898 times 100 (2)

where 120578119894 is the structure efficiency index under the ith work-ing condition 120590119894max and 119889119894max are the maximum stress andmaximum displacement under the ith working conditionandm is the structural weight

Substituting the analysis results of Table 4 into (2) thestructure efficiency of the cylinder block is calculated asshown in Figure 7 It can be seen that the cylinder block hasthe highest structure efficiency at the moment of the firstcylinder explosion and followed by the fourth cylinder thesecond cylinder and the third cylinder It shows that the firstcylinder explosion is the worst working condition and thethird cylinder explosion is the safest condition

6 Mathematical Problems in Engineering

Contour Plot

4181E+003717E+003252E+002788E+002324E+001859E+001395E+00

Max = 4181E+00

Min = 1802E-03Grids 4612

Grids 32494

9306E-014662E-011802E-03

No result

Eigen Mode(Mag)Analysis system

(a) The first-order mode

Contour Plot

5090E+004600E+004111E+003621E+003131E+002641E+002152E+00

Max = 5090E+00

Min = 6824E-01Grids 7120

Grids 33177

1662E+001172E+006824E-01

No result

Eigen Mode(Mag)Analysis system

(b) The second-order mode

Contour Plot

5616E+004998E+004379E+003761E+003143E+002524E+001906E+00

Max = 5616E+00

Min = 5048E-02Grids 629

Grids 90051

1287E+00

5048E-026689E-01

No result

Eigen Mode(Mag)Analysis system

(c) The third-order mode

Contour Plot

9348E+008314E+007281E+006248E+005214E+004181E+003148E+00

Max = 9348E+00

Min = 4777E-02Grids 31763

Grids 19024

2114E+001081E+004777E-02

No result

Eigen Mode(Mag)Analysis system

(d) The fourth-order mode

Contour Plot

4681E+004258E+003835E+003412E+002989E+002566E+002143E+00

Max = 4681E+00

Min = 8739E-01Grids 98310

Grids 762

1720E+001297E+008739E-01

No result

Eigen Mode(Mag)Analysis system

(e) The fifth-order mode

Contour Plot

8861E+007876E+006892E+005907E+004923E+003938E+002954E+00

Max = 8861E+00

Min = 1354E-05Grids 4690

Grids 263900

1969E+00

1354E-059845E-01

No result

Eigen Mode(Mag)Analysis system

(f) The sixth-order mode

Figure 6 Results of modal analysis

0

20

40

60

80

1 2 3 4

struc

ture

effici

ency

the number of working conditions

Figure 7 The structure efficiency of each cylinder

Based on the analysis mentioned in Figures 5ndash7 thecylinder block studied in this paper can meet the stiffnessand strength requirements under the worst working con-dition The overall stress value (80 MPa) is much lower

than material ultimate strength (300 MPa) which indicatesthat the cylinder block has surplus material and topologyoptimization space Its working frequency (100 Hz) is muchlower than the first-order natural frequency (264 Hz) andthe resonance does not occur In addition the importancefor four working conditions is sorted the first cylinder thefourth cylinder the second cylinder and the third cylinderTherefore the first cylinder and the fourth cylinder shouldbe focused when determining the weighting coefficientsin multiobjective topology optimization And the materialnear the second cylinder and the third cylinder should beconsidered when improving the topology structure

5 Topology Optimization MathematicalModel Based on AHP

51 The Hierarchical Structure Model The topology opti-mization for the diesel engine cylinder block belongs to thetypical multiworking condition problem It is necessary to

Mathematical Problems in Engineering 7

The top 6-order natural

Topologyoptimizationof cylinder

block

Static topology

dynamic topology

target

criterionThe cylinder No1

The cylinder No2

The cylinder No3

The cylinder No4

index

optimization 2

optimization 1

of explosion w4

of explosion w3

of explosion w2

of explosion w1

frequencies w5 sim w10

Figure 8 The hierarchical structure model of topology optimization

take into account the structural performance requirementsincluding static and dynamic characteristics For the staticcharacteristics structural stiffness has to be considered atthe moment of each cylinder explosion And the top 6-order natural frequencies need to be concerned for dynamiccharacteristicsTherefore the hierarchical structure model oftopology optimization for the cylinder block is establishedbased on staticmultiworking condition stiffness and dynamicmultiorder natural frequency as shown in Figure 8 It canbe seen from the figure that the multiobjective topologyoptimization of the cylinder block includes 12 weightingcoefficients that are static and dynamic topology optimization1205721 1205722 in the criterion layer static multiworking conditionstiffness1199081 sim 1199084 and dynamic multiorder natural frequency1199085 sim 1199081052 Comprehensive Evaluation of the Cylinder Block Thelinear weighting method is usually used to transform themultiobjective problem into a single-objective problem forthe traditional multiobjective topology optimization How-ever the linear weighting method is to calculate weightaverage value for all functions and it cannot reflect the promi-nent influence from some certain functions which doesnot guarantee that all functions obtain the relative optimalsolutionThe compromise programmingmethod [28] can geta group of better relative optimal solutions by calculating thesensitivity of all functions to design variables and adjustingeach objective to balance each other From the hierarchicalstructuremodel shown in Figure 8 the topology optimizationfor the cylinder block includes ten optimization objectivesand the static and dynamic multiobjective optimizationproblem is converted into the single-objective optimizationproblem by the compromise programming method

521 Static Multiworking Condition Stiffness The topologyoptimization oriented by stiffnessmaximization is to research

material distribution form in the design domain to maxi-mize the structural stiffness In this paper the static stiff-ness of the cylinder block under four extreme conditionsis studied which belongs to the multiworking conditionstiffness problem In this paper the objective function ofstatic multiworking condition stiffness is obtained by thecompromise programming method as shown in (3) 119862(120588)is the comprehensive evaluation value of the static stiffnessand the smaller the value the larger the structural overallstiffness

min120588119862 (120588) = 119898sum

119894=1

119908119902119894 [119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]1199021119902 (3)

where 120588 is the relative density in the variable density topologyoptimization and m is the total number of working condi-tions m=4 119908119894 is the weight coefficient of the ith workingcondition while q is the penalty coefficient (qge2) 119862119894(120588) is thestructural compliance of the ith working condition119862max

119894 and119862min119894 are the maximum and minimum compliance of the ith

working condition respectively

522 Dynamic Multiorder Natural Frequency The topologyoptimization of dynamic multiorder natural frequency isusually targeted at maximizing the low-order natural fre-quency and the material remove ratio is taken as boundaryHowever if only one low-order natural frequency is used asthe optimization objective the eigenvalues of other adjacenthigher order natural frequency may be reduced because ofthe gradual material remove in the structure It will result inthe interchange of the low-order natural frequencies and theconvergence of topology optimization will be influencedTheaverage frequency method [29] can consider simultaneouslythemultiorder natural frequency by defining a smooth objec-tive function and improve the convergence which is widelyused in dynamic topology optimization In this paper the

8 Mathematical Problems in Engineering

objective function of dynamic multiorder natural frequencyis defined by the average frequency method as shown in (4)Λ(120588) is the comprehensive evaluation value of the top feworder natural frequency and the larger the value the largerthe top few order natural frequency

maxΛ (120588) = 1205820 + 119904( 119899sum119895=1

119908119895120582119895 minus 1205820)minus1

(4)

where 120588 is the relative density in the variable density topologyoptimization 120582119895 is the jth order natural frequency 1205820 ands as given parameters are used to adjust the function valueusually 1205820=0 s=1 119908119895 is the weight coefficient of the jth ordernatural frequency while n is the order of low-order naturalfrequency that need to be optimized n=6

In addition the low-order natural frequency is usuallypaid to attention during the optimization process and thelower the order the higher the degree of attention Accordingto this principle aiming at reducing the complexity of theweighting coefficients determined by the analytic hierarchyprocess the weight coefficients 1199085 sim 11990810 of the top 6natural frequencies are taken as 03 02 02 01 01 and 01respectively So the 12 unknown weighting coefficients in thehierarchical structure model are reduced to six

523 Comprehensive Evaluation Function The comprehen-sive evaluation function of multiobjective topology opti-mization considering both the staticmultiworking conditionstiffness and the dynamic multiorder natural frequency isestablished by the compromise programming method asshown in (5) By adjusting the position of 119862119894(120588) and Λ 120588 inthe function the comprehensive evaluation function can uni-formly guide the convergence direction of the optimizationAnd the smaller the value the better the overall performanceof the cylinder block

min119865 (120588) = 12057221 [ 119898sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2

+ 12057222 [Λmax minus Λ (120588)Λmax minus Λmin ]212

(5)

where 119865(120588) is the objective function value and Λmin andΛmax representminimum andmaximumnatural frequenciesrespectively Other variables have the same meaning as (3)and (4)

53 The Weighting Coefficients The comprehensive evalua-tion function ofmultiobjective topology optimization shownin (5) has six unknown weighting coefficients including1205721 1205722 1199081 sim 1199084 These unknown weighting coefficientsare calculated based on the analytic hierarchy process inthis paper The concrete calculating flow chart is shownin Figure 9 The subjective judgment is scaled based onthe measure theory and the judgment matrix is established

Begin

Analyzing hierarchical structure model

Determining static anddynamic weight coefficients

Sort by the importance of working condition

Comparing the importancebetween two working conditions

Calculating the judgment matrix

Calculating the weight coefficientsof every working condition

consistency check

Conformity

All weight coefficients of multi-objectivetopology optimization is obtained

End

Criterionlayer

Index layerYes

No

Figure 9 The calculating flow chart of the weight coefficients

Then the all weighting coefficients are calculated through theconsistency check

531 Criteria Layer Decision There are static stiffness topol-ogy optimization and dynamic natural frequency topologyoptimization in the criterion layer and the correspondingweighting factors are respectively 1205721 1205722 The cylinder blocksuffers from the alternating impact loads when differentcylinder explodes and its stiffness performance directlyaffects the working reliability But for the vibration charac-teristics it can be seen from Section 42 that the maximumworking frequency is 100 Hz which is much smaller than thefirst-order natural frequency of 264 Hz Therefore the staticmultiworking condition stiffness is more important in thetopology optimization for the cylinder block So the weightcoefficients 1205721 1205722 are defined as 06 and 04 respectively

532 Index Layer Decision Firstly it is necessary to deter-mine the importance of four working conditions Accordingto the structure efficiency shown in Figure 7 the importanceis sorted the first cylinder the fourth cylinder the secondcylinder and the third cylinder So the weight coefficients areranked as shown in

1199081 gt 1199084 gt 1199082 gt 1199083 (6)

Mathematical Problems in Engineering 9

Table 6 Meanings of relative scale

Relative scale Meanings1 Two elements have equal importance3 The former is slightly important than the latter between two elements

5 The former is obviously important than the latter between twoelements

7 The former is strongly important than the latter between two elements

9 The former is extremely important than the latter between twoelements

2 4 6 8 Indicating the intermediate value above judgment

Reciprocal If the important ratio between the elements 119894 and 119895 is 119909 the importantratio between the elements 119895 and i is 1119909

Then according to the standard meaning table of relativescale in the AHP shown in Table 6 the relative importanceratio of four working conditions is determined and thejudgment matrix119882 is constructed as shown in

119882 =

[[[[[[[[[[[[[[[

11990811199081 1199081119908119894

1199081119908119899 1199081198951199081 119908119895119908119894

119908119895119908119899 1199081198991199081 119908119899119908119894

119908119899119908119899

]]]]]]]]]]]]]]]

=[[[[[[[[[[[

11990811 1199081119894 1199081119899 1199081198951 119908119895119894 119908119895119899 1199081198991 119908119899119894 119908119899119899

]]]]]]]]]]]

(7)

where n is the number of the weight coefficients 119908119894 and119908119895 (119894 119895 = 1 2 6) represent the weight coefficients and119908119895119894 = 119908119895119908119894 denotes the relative importance of 119908119895 to 119908119894According to the results in Section 4 the first cylinder

explosion is the worst condition and it is obviously moreimportant than the third working condition and slightlymore important than the fourth working condition so theweight coefficients 11990813 11990814 are determined as 5 and 2respectivelyThe importance of the secondworking conditionis between the third working condition and the fourthworking condition so the weight coefficient 11990812 is defined as4 In the same way the relative importance ratio of the fourworking conditions is obtained and the judgment matrix isconstructed

119882 =[[[[[[[[[[

1 4 5 214 1 2 1315 12 1 1412 3 4 1

]]]]]]]]]] (8)

The judgment matrix W is right multiplied by a vector120596 = (1199081 1199082 1199083 1199084)Τ consisting of all the weight coefficientsas shown in

119882120596 = 120582120596 997904rArr(119882 minus 120582119868)120596 = 0 (9)

Substituting the judgment matrix 119882 into (9) themaximum eigenvalue 120582max = 40484 is calculatedand the corresponding eigenvector normalized is 120596 =(049 012 008 031)Τ So all weight coefficients areobtained for multiobjective topology optimization of thecylinder block

In order to ensure the accuracy and reliability of thejudgment matrix and avoid influence of individual subjectivefactor the consistency test of the judgment matrix is carriedout in terms of (10) The consistency ratio CR of thejudgment matrixW calculated by (10) is 00179 which is lessthan 01 Therefore it is considered that the judgment matrixhas a satisfactory consistency and the four weight coefficientscan well reflect the importance of each working condition

119862119877 = 119862119868119877119868 (10)

where 119862119868 is the consistency index 119862119868 = (120582max minus119899)(119899 minus 1)119877119868 is the mean random consistency index whose value canbe obtained directly by referring to the standard randomconsistency index 119877119868-119899 table in the analytic hierarchyprocess as shown in Table 7 119862119877 is the random consistencyratio and the inconsistency is acceptable when 119862119877 lt 01

In addition the computing platform of weight coefficientfor multiworking condition topology optimization (TOWC)is built inMatlab to improve the computational efficiency ofthe method as shown in Figure 10 According to the numberof working conditions and the importance of each working

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

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Page 6: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

6 Mathematical Problems in Engineering

Contour Plot

4181E+003717E+003252E+002788E+002324E+001859E+001395E+00

Max = 4181E+00

Min = 1802E-03Grids 4612

Grids 32494

9306E-014662E-011802E-03

No result

Eigen Mode(Mag)Analysis system

(a) The first-order mode

Contour Plot

5090E+004600E+004111E+003621E+003131E+002641E+002152E+00

Max = 5090E+00

Min = 6824E-01Grids 7120

Grids 33177

1662E+001172E+006824E-01

No result

Eigen Mode(Mag)Analysis system

(b) The second-order mode

Contour Plot

5616E+004998E+004379E+003761E+003143E+002524E+001906E+00

Max = 5616E+00

Min = 5048E-02Grids 629

Grids 90051

1287E+00

5048E-026689E-01

No result

Eigen Mode(Mag)Analysis system

(c) The third-order mode

Contour Plot

9348E+008314E+007281E+006248E+005214E+004181E+003148E+00

Max = 9348E+00

Min = 4777E-02Grids 31763

Grids 19024

2114E+001081E+004777E-02

No result

Eigen Mode(Mag)Analysis system

(d) The fourth-order mode

Contour Plot

4681E+004258E+003835E+003412E+002989E+002566E+002143E+00

Max = 4681E+00

Min = 8739E-01Grids 98310

Grids 762

1720E+001297E+008739E-01

No result

Eigen Mode(Mag)Analysis system

(e) The fifth-order mode

Contour Plot

8861E+007876E+006892E+005907E+004923E+003938E+002954E+00

Max = 8861E+00

Min = 1354E-05Grids 4690

Grids 263900

1969E+00

1354E-059845E-01

No result

Eigen Mode(Mag)Analysis system

(f) The sixth-order mode

Figure 6 Results of modal analysis

0

20

40

60

80

1 2 3 4

struc

ture

effici

ency

the number of working conditions

Figure 7 The structure efficiency of each cylinder

Based on the analysis mentioned in Figures 5ndash7 thecylinder block studied in this paper can meet the stiffnessand strength requirements under the worst working con-dition The overall stress value (80 MPa) is much lower

than material ultimate strength (300 MPa) which indicatesthat the cylinder block has surplus material and topologyoptimization space Its working frequency (100 Hz) is muchlower than the first-order natural frequency (264 Hz) andthe resonance does not occur In addition the importancefor four working conditions is sorted the first cylinder thefourth cylinder the second cylinder and the third cylinderTherefore the first cylinder and the fourth cylinder shouldbe focused when determining the weighting coefficientsin multiobjective topology optimization And the materialnear the second cylinder and the third cylinder should beconsidered when improving the topology structure

5 Topology Optimization MathematicalModel Based on AHP

51 The Hierarchical Structure Model The topology opti-mization for the diesel engine cylinder block belongs to thetypical multiworking condition problem It is necessary to

Mathematical Problems in Engineering 7

The top 6-order natural

Topologyoptimizationof cylinder

block

Static topology

dynamic topology

target

criterionThe cylinder No1

The cylinder No2

The cylinder No3

The cylinder No4

index

optimization 2

optimization 1

of explosion w4

of explosion w3

of explosion w2

of explosion w1

frequencies w5 sim w10

Figure 8 The hierarchical structure model of topology optimization

take into account the structural performance requirementsincluding static and dynamic characteristics For the staticcharacteristics structural stiffness has to be considered atthe moment of each cylinder explosion And the top 6-order natural frequencies need to be concerned for dynamiccharacteristicsTherefore the hierarchical structure model oftopology optimization for the cylinder block is establishedbased on staticmultiworking condition stiffness and dynamicmultiorder natural frequency as shown in Figure 8 It canbe seen from the figure that the multiobjective topologyoptimization of the cylinder block includes 12 weightingcoefficients that are static and dynamic topology optimization1205721 1205722 in the criterion layer static multiworking conditionstiffness1199081 sim 1199084 and dynamic multiorder natural frequency1199085 sim 1199081052 Comprehensive Evaluation of the Cylinder Block Thelinear weighting method is usually used to transform themultiobjective problem into a single-objective problem forthe traditional multiobjective topology optimization How-ever the linear weighting method is to calculate weightaverage value for all functions and it cannot reflect the promi-nent influence from some certain functions which doesnot guarantee that all functions obtain the relative optimalsolutionThe compromise programmingmethod [28] can geta group of better relative optimal solutions by calculating thesensitivity of all functions to design variables and adjustingeach objective to balance each other From the hierarchicalstructuremodel shown in Figure 8 the topology optimizationfor the cylinder block includes ten optimization objectivesand the static and dynamic multiobjective optimizationproblem is converted into the single-objective optimizationproblem by the compromise programming method

521 Static Multiworking Condition Stiffness The topologyoptimization oriented by stiffnessmaximization is to research

material distribution form in the design domain to maxi-mize the structural stiffness In this paper the static stiff-ness of the cylinder block under four extreme conditionsis studied which belongs to the multiworking conditionstiffness problem In this paper the objective function ofstatic multiworking condition stiffness is obtained by thecompromise programming method as shown in (3) 119862(120588)is the comprehensive evaluation value of the static stiffnessand the smaller the value the larger the structural overallstiffness

min120588119862 (120588) = 119898sum

119894=1

119908119902119894 [119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]1199021119902 (3)

where 120588 is the relative density in the variable density topologyoptimization and m is the total number of working condi-tions m=4 119908119894 is the weight coefficient of the ith workingcondition while q is the penalty coefficient (qge2) 119862119894(120588) is thestructural compliance of the ith working condition119862max

119894 and119862min119894 are the maximum and minimum compliance of the ith

working condition respectively

522 Dynamic Multiorder Natural Frequency The topologyoptimization of dynamic multiorder natural frequency isusually targeted at maximizing the low-order natural fre-quency and the material remove ratio is taken as boundaryHowever if only one low-order natural frequency is used asthe optimization objective the eigenvalues of other adjacenthigher order natural frequency may be reduced because ofthe gradual material remove in the structure It will result inthe interchange of the low-order natural frequencies and theconvergence of topology optimization will be influencedTheaverage frequency method [29] can consider simultaneouslythemultiorder natural frequency by defining a smooth objec-tive function and improve the convergence which is widelyused in dynamic topology optimization In this paper the

8 Mathematical Problems in Engineering

objective function of dynamic multiorder natural frequencyis defined by the average frequency method as shown in (4)Λ(120588) is the comprehensive evaluation value of the top feworder natural frequency and the larger the value the largerthe top few order natural frequency

maxΛ (120588) = 1205820 + 119904( 119899sum119895=1

119908119895120582119895 minus 1205820)minus1

(4)

where 120588 is the relative density in the variable density topologyoptimization 120582119895 is the jth order natural frequency 1205820 ands as given parameters are used to adjust the function valueusually 1205820=0 s=1 119908119895 is the weight coefficient of the jth ordernatural frequency while n is the order of low-order naturalfrequency that need to be optimized n=6

In addition the low-order natural frequency is usuallypaid to attention during the optimization process and thelower the order the higher the degree of attention Accordingto this principle aiming at reducing the complexity of theweighting coefficients determined by the analytic hierarchyprocess the weight coefficients 1199085 sim 11990810 of the top 6natural frequencies are taken as 03 02 02 01 01 and 01respectively So the 12 unknown weighting coefficients in thehierarchical structure model are reduced to six

523 Comprehensive Evaluation Function The comprehen-sive evaluation function of multiobjective topology opti-mization considering both the staticmultiworking conditionstiffness and the dynamic multiorder natural frequency isestablished by the compromise programming method asshown in (5) By adjusting the position of 119862119894(120588) and Λ 120588 inthe function the comprehensive evaluation function can uni-formly guide the convergence direction of the optimizationAnd the smaller the value the better the overall performanceof the cylinder block

min119865 (120588) = 12057221 [ 119898sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2

+ 12057222 [Λmax minus Λ (120588)Λmax minus Λmin ]212

(5)

where 119865(120588) is the objective function value and Λmin andΛmax representminimum andmaximumnatural frequenciesrespectively Other variables have the same meaning as (3)and (4)

53 The Weighting Coefficients The comprehensive evalua-tion function ofmultiobjective topology optimization shownin (5) has six unknown weighting coefficients including1205721 1205722 1199081 sim 1199084 These unknown weighting coefficientsare calculated based on the analytic hierarchy process inthis paper The concrete calculating flow chart is shownin Figure 9 The subjective judgment is scaled based onthe measure theory and the judgment matrix is established

Begin

Analyzing hierarchical structure model

Determining static anddynamic weight coefficients

Sort by the importance of working condition

Comparing the importancebetween two working conditions

Calculating the judgment matrix

Calculating the weight coefficientsof every working condition

consistency check

Conformity

All weight coefficients of multi-objectivetopology optimization is obtained

End

Criterionlayer

Index layerYes

No

Figure 9 The calculating flow chart of the weight coefficients

Then the all weighting coefficients are calculated through theconsistency check

531 Criteria Layer Decision There are static stiffness topol-ogy optimization and dynamic natural frequency topologyoptimization in the criterion layer and the correspondingweighting factors are respectively 1205721 1205722 The cylinder blocksuffers from the alternating impact loads when differentcylinder explodes and its stiffness performance directlyaffects the working reliability But for the vibration charac-teristics it can be seen from Section 42 that the maximumworking frequency is 100 Hz which is much smaller than thefirst-order natural frequency of 264 Hz Therefore the staticmultiworking condition stiffness is more important in thetopology optimization for the cylinder block So the weightcoefficients 1205721 1205722 are defined as 06 and 04 respectively

532 Index Layer Decision Firstly it is necessary to deter-mine the importance of four working conditions Accordingto the structure efficiency shown in Figure 7 the importanceis sorted the first cylinder the fourth cylinder the secondcylinder and the third cylinder So the weight coefficients areranked as shown in

1199081 gt 1199084 gt 1199082 gt 1199083 (6)

Mathematical Problems in Engineering 9

Table 6 Meanings of relative scale

Relative scale Meanings1 Two elements have equal importance3 The former is slightly important than the latter between two elements

5 The former is obviously important than the latter between twoelements

7 The former is strongly important than the latter between two elements

9 The former is extremely important than the latter between twoelements

2 4 6 8 Indicating the intermediate value above judgment

Reciprocal If the important ratio between the elements 119894 and 119895 is 119909 the importantratio between the elements 119895 and i is 1119909

Then according to the standard meaning table of relativescale in the AHP shown in Table 6 the relative importanceratio of four working conditions is determined and thejudgment matrix119882 is constructed as shown in

119882 =

[[[[[[[[[[[[[[[

11990811199081 1199081119908119894

1199081119908119899 1199081198951199081 119908119895119908119894

119908119895119908119899 1199081198991199081 119908119899119908119894

119908119899119908119899

]]]]]]]]]]]]]]]

=[[[[[[[[[[[

11990811 1199081119894 1199081119899 1199081198951 119908119895119894 119908119895119899 1199081198991 119908119899119894 119908119899119899

]]]]]]]]]]]

(7)

where n is the number of the weight coefficients 119908119894 and119908119895 (119894 119895 = 1 2 6) represent the weight coefficients and119908119895119894 = 119908119895119908119894 denotes the relative importance of 119908119895 to 119908119894According to the results in Section 4 the first cylinder

explosion is the worst condition and it is obviously moreimportant than the third working condition and slightlymore important than the fourth working condition so theweight coefficients 11990813 11990814 are determined as 5 and 2respectivelyThe importance of the secondworking conditionis between the third working condition and the fourthworking condition so the weight coefficient 11990812 is defined as4 In the same way the relative importance ratio of the fourworking conditions is obtained and the judgment matrix isconstructed

119882 =[[[[[[[[[[

1 4 5 214 1 2 1315 12 1 1412 3 4 1

]]]]]]]]]] (8)

The judgment matrix W is right multiplied by a vector120596 = (1199081 1199082 1199083 1199084)Τ consisting of all the weight coefficientsas shown in

119882120596 = 120582120596 997904rArr(119882 minus 120582119868)120596 = 0 (9)

Substituting the judgment matrix 119882 into (9) themaximum eigenvalue 120582max = 40484 is calculatedand the corresponding eigenvector normalized is 120596 =(049 012 008 031)Τ So all weight coefficients areobtained for multiobjective topology optimization of thecylinder block

In order to ensure the accuracy and reliability of thejudgment matrix and avoid influence of individual subjectivefactor the consistency test of the judgment matrix is carriedout in terms of (10) The consistency ratio CR of thejudgment matrixW calculated by (10) is 00179 which is lessthan 01 Therefore it is considered that the judgment matrixhas a satisfactory consistency and the four weight coefficientscan well reflect the importance of each working condition

119862119877 = 119862119868119877119868 (10)

where 119862119868 is the consistency index 119862119868 = (120582max minus119899)(119899 minus 1)119877119868 is the mean random consistency index whose value canbe obtained directly by referring to the standard randomconsistency index 119877119868-119899 table in the analytic hierarchyprocess as shown in Table 7 119862119877 is the random consistencyratio and the inconsistency is acceptable when 119862119877 lt 01

In addition the computing platform of weight coefficientfor multiworking condition topology optimization (TOWC)is built inMatlab to improve the computational efficiency ofthe method as shown in Figure 10 According to the numberof working conditions and the importance of each working

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

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Page 7: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

Mathematical Problems in Engineering 7

The top 6-order natural

Topologyoptimizationof cylinder

block

Static topology

dynamic topology

target

criterionThe cylinder No1

The cylinder No2

The cylinder No3

The cylinder No4

index

optimization 2

optimization 1

of explosion w4

of explosion w3

of explosion w2

of explosion w1

frequencies w5 sim w10

Figure 8 The hierarchical structure model of topology optimization

take into account the structural performance requirementsincluding static and dynamic characteristics For the staticcharacteristics structural stiffness has to be considered atthe moment of each cylinder explosion And the top 6-order natural frequencies need to be concerned for dynamiccharacteristicsTherefore the hierarchical structure model oftopology optimization for the cylinder block is establishedbased on staticmultiworking condition stiffness and dynamicmultiorder natural frequency as shown in Figure 8 It canbe seen from the figure that the multiobjective topologyoptimization of the cylinder block includes 12 weightingcoefficients that are static and dynamic topology optimization1205721 1205722 in the criterion layer static multiworking conditionstiffness1199081 sim 1199084 and dynamic multiorder natural frequency1199085 sim 1199081052 Comprehensive Evaluation of the Cylinder Block Thelinear weighting method is usually used to transform themultiobjective problem into a single-objective problem forthe traditional multiobjective topology optimization How-ever the linear weighting method is to calculate weightaverage value for all functions and it cannot reflect the promi-nent influence from some certain functions which doesnot guarantee that all functions obtain the relative optimalsolutionThe compromise programmingmethod [28] can geta group of better relative optimal solutions by calculating thesensitivity of all functions to design variables and adjustingeach objective to balance each other From the hierarchicalstructuremodel shown in Figure 8 the topology optimizationfor the cylinder block includes ten optimization objectivesand the static and dynamic multiobjective optimizationproblem is converted into the single-objective optimizationproblem by the compromise programming method

521 Static Multiworking Condition Stiffness The topologyoptimization oriented by stiffnessmaximization is to research

material distribution form in the design domain to maxi-mize the structural stiffness In this paper the static stiff-ness of the cylinder block under four extreme conditionsis studied which belongs to the multiworking conditionstiffness problem In this paper the objective function ofstatic multiworking condition stiffness is obtained by thecompromise programming method as shown in (3) 119862(120588)is the comprehensive evaluation value of the static stiffnessand the smaller the value the larger the structural overallstiffness

min120588119862 (120588) = 119898sum

119894=1

119908119902119894 [119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]1199021119902 (3)

where 120588 is the relative density in the variable density topologyoptimization and m is the total number of working condi-tions m=4 119908119894 is the weight coefficient of the ith workingcondition while q is the penalty coefficient (qge2) 119862119894(120588) is thestructural compliance of the ith working condition119862max

119894 and119862min119894 are the maximum and minimum compliance of the ith

working condition respectively

522 Dynamic Multiorder Natural Frequency The topologyoptimization of dynamic multiorder natural frequency isusually targeted at maximizing the low-order natural fre-quency and the material remove ratio is taken as boundaryHowever if only one low-order natural frequency is used asthe optimization objective the eigenvalues of other adjacenthigher order natural frequency may be reduced because ofthe gradual material remove in the structure It will result inthe interchange of the low-order natural frequencies and theconvergence of topology optimization will be influencedTheaverage frequency method [29] can consider simultaneouslythemultiorder natural frequency by defining a smooth objec-tive function and improve the convergence which is widelyused in dynamic topology optimization In this paper the

8 Mathematical Problems in Engineering

objective function of dynamic multiorder natural frequencyis defined by the average frequency method as shown in (4)Λ(120588) is the comprehensive evaluation value of the top feworder natural frequency and the larger the value the largerthe top few order natural frequency

maxΛ (120588) = 1205820 + 119904( 119899sum119895=1

119908119895120582119895 minus 1205820)minus1

(4)

where 120588 is the relative density in the variable density topologyoptimization 120582119895 is the jth order natural frequency 1205820 ands as given parameters are used to adjust the function valueusually 1205820=0 s=1 119908119895 is the weight coefficient of the jth ordernatural frequency while n is the order of low-order naturalfrequency that need to be optimized n=6

In addition the low-order natural frequency is usuallypaid to attention during the optimization process and thelower the order the higher the degree of attention Accordingto this principle aiming at reducing the complexity of theweighting coefficients determined by the analytic hierarchyprocess the weight coefficients 1199085 sim 11990810 of the top 6natural frequencies are taken as 03 02 02 01 01 and 01respectively So the 12 unknown weighting coefficients in thehierarchical structure model are reduced to six

523 Comprehensive Evaluation Function The comprehen-sive evaluation function of multiobjective topology opti-mization considering both the staticmultiworking conditionstiffness and the dynamic multiorder natural frequency isestablished by the compromise programming method asshown in (5) By adjusting the position of 119862119894(120588) and Λ 120588 inthe function the comprehensive evaluation function can uni-formly guide the convergence direction of the optimizationAnd the smaller the value the better the overall performanceof the cylinder block

min119865 (120588) = 12057221 [ 119898sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2

+ 12057222 [Λmax minus Λ (120588)Λmax minus Λmin ]212

(5)

where 119865(120588) is the objective function value and Λmin andΛmax representminimum andmaximumnatural frequenciesrespectively Other variables have the same meaning as (3)and (4)

53 The Weighting Coefficients The comprehensive evalua-tion function ofmultiobjective topology optimization shownin (5) has six unknown weighting coefficients including1205721 1205722 1199081 sim 1199084 These unknown weighting coefficientsare calculated based on the analytic hierarchy process inthis paper The concrete calculating flow chart is shownin Figure 9 The subjective judgment is scaled based onthe measure theory and the judgment matrix is established

Begin

Analyzing hierarchical structure model

Determining static anddynamic weight coefficients

Sort by the importance of working condition

Comparing the importancebetween two working conditions

Calculating the judgment matrix

Calculating the weight coefficientsof every working condition

consistency check

Conformity

All weight coefficients of multi-objectivetopology optimization is obtained

End

Criterionlayer

Index layerYes

No

Figure 9 The calculating flow chart of the weight coefficients

Then the all weighting coefficients are calculated through theconsistency check

531 Criteria Layer Decision There are static stiffness topol-ogy optimization and dynamic natural frequency topologyoptimization in the criterion layer and the correspondingweighting factors are respectively 1205721 1205722 The cylinder blocksuffers from the alternating impact loads when differentcylinder explodes and its stiffness performance directlyaffects the working reliability But for the vibration charac-teristics it can be seen from Section 42 that the maximumworking frequency is 100 Hz which is much smaller than thefirst-order natural frequency of 264 Hz Therefore the staticmultiworking condition stiffness is more important in thetopology optimization for the cylinder block So the weightcoefficients 1205721 1205722 are defined as 06 and 04 respectively

532 Index Layer Decision Firstly it is necessary to deter-mine the importance of four working conditions Accordingto the structure efficiency shown in Figure 7 the importanceis sorted the first cylinder the fourth cylinder the secondcylinder and the third cylinder So the weight coefficients areranked as shown in

1199081 gt 1199084 gt 1199082 gt 1199083 (6)

Mathematical Problems in Engineering 9

Table 6 Meanings of relative scale

Relative scale Meanings1 Two elements have equal importance3 The former is slightly important than the latter between two elements

5 The former is obviously important than the latter between twoelements

7 The former is strongly important than the latter between two elements

9 The former is extremely important than the latter between twoelements

2 4 6 8 Indicating the intermediate value above judgment

Reciprocal If the important ratio between the elements 119894 and 119895 is 119909 the importantratio between the elements 119895 and i is 1119909

Then according to the standard meaning table of relativescale in the AHP shown in Table 6 the relative importanceratio of four working conditions is determined and thejudgment matrix119882 is constructed as shown in

119882 =

[[[[[[[[[[[[[[[

11990811199081 1199081119908119894

1199081119908119899 1199081198951199081 119908119895119908119894

119908119895119908119899 1199081198991199081 119908119899119908119894

119908119899119908119899

]]]]]]]]]]]]]]]

=[[[[[[[[[[[

11990811 1199081119894 1199081119899 1199081198951 119908119895119894 119908119895119899 1199081198991 119908119899119894 119908119899119899

]]]]]]]]]]]

(7)

where n is the number of the weight coefficients 119908119894 and119908119895 (119894 119895 = 1 2 6) represent the weight coefficients and119908119895119894 = 119908119895119908119894 denotes the relative importance of 119908119895 to 119908119894According to the results in Section 4 the first cylinder

explosion is the worst condition and it is obviously moreimportant than the third working condition and slightlymore important than the fourth working condition so theweight coefficients 11990813 11990814 are determined as 5 and 2respectivelyThe importance of the secondworking conditionis between the third working condition and the fourthworking condition so the weight coefficient 11990812 is defined as4 In the same way the relative importance ratio of the fourworking conditions is obtained and the judgment matrix isconstructed

119882 =[[[[[[[[[[

1 4 5 214 1 2 1315 12 1 1412 3 4 1

]]]]]]]]]] (8)

The judgment matrix W is right multiplied by a vector120596 = (1199081 1199082 1199083 1199084)Τ consisting of all the weight coefficientsas shown in

119882120596 = 120582120596 997904rArr(119882 minus 120582119868)120596 = 0 (9)

Substituting the judgment matrix 119882 into (9) themaximum eigenvalue 120582max = 40484 is calculatedand the corresponding eigenvector normalized is 120596 =(049 012 008 031)Τ So all weight coefficients areobtained for multiobjective topology optimization of thecylinder block

In order to ensure the accuracy and reliability of thejudgment matrix and avoid influence of individual subjectivefactor the consistency test of the judgment matrix is carriedout in terms of (10) The consistency ratio CR of thejudgment matrixW calculated by (10) is 00179 which is lessthan 01 Therefore it is considered that the judgment matrixhas a satisfactory consistency and the four weight coefficientscan well reflect the importance of each working condition

119862119877 = 119862119868119877119868 (10)

where 119862119868 is the consistency index 119862119868 = (120582max minus119899)(119899 minus 1)119877119868 is the mean random consistency index whose value canbe obtained directly by referring to the standard randomconsistency index 119877119868-119899 table in the analytic hierarchyprocess as shown in Table 7 119862119877 is the random consistencyratio and the inconsistency is acceptable when 119862119877 lt 01

In addition the computing platform of weight coefficientfor multiworking condition topology optimization (TOWC)is built inMatlab to improve the computational efficiency ofthe method as shown in Figure 10 According to the numberof working conditions and the importance of each working

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

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Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

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Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 8: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

8 Mathematical Problems in Engineering

objective function of dynamic multiorder natural frequencyis defined by the average frequency method as shown in (4)Λ(120588) is the comprehensive evaluation value of the top feworder natural frequency and the larger the value the largerthe top few order natural frequency

maxΛ (120588) = 1205820 + 119904( 119899sum119895=1

119908119895120582119895 minus 1205820)minus1

(4)

where 120588 is the relative density in the variable density topologyoptimization 120582119895 is the jth order natural frequency 1205820 ands as given parameters are used to adjust the function valueusually 1205820=0 s=1 119908119895 is the weight coefficient of the jth ordernatural frequency while n is the order of low-order naturalfrequency that need to be optimized n=6

In addition the low-order natural frequency is usuallypaid to attention during the optimization process and thelower the order the higher the degree of attention Accordingto this principle aiming at reducing the complexity of theweighting coefficients determined by the analytic hierarchyprocess the weight coefficients 1199085 sim 11990810 of the top 6natural frequencies are taken as 03 02 02 01 01 and 01respectively So the 12 unknown weighting coefficients in thehierarchical structure model are reduced to six

523 Comprehensive Evaluation Function The comprehen-sive evaluation function of multiobjective topology opti-mization considering both the staticmultiworking conditionstiffness and the dynamic multiorder natural frequency isestablished by the compromise programming method asshown in (5) By adjusting the position of 119862119894(120588) and Λ 120588 inthe function the comprehensive evaluation function can uni-formly guide the convergence direction of the optimizationAnd the smaller the value the better the overall performanceof the cylinder block

min119865 (120588) = 12057221 [ 119898sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2

+ 12057222 [Λmax minus Λ (120588)Λmax minus Λmin ]212

(5)

where 119865(120588) is the objective function value and Λmin andΛmax representminimum andmaximumnatural frequenciesrespectively Other variables have the same meaning as (3)and (4)

53 The Weighting Coefficients The comprehensive evalua-tion function ofmultiobjective topology optimization shownin (5) has six unknown weighting coefficients including1205721 1205722 1199081 sim 1199084 These unknown weighting coefficientsare calculated based on the analytic hierarchy process inthis paper The concrete calculating flow chart is shownin Figure 9 The subjective judgment is scaled based onthe measure theory and the judgment matrix is established

Begin

Analyzing hierarchical structure model

Determining static anddynamic weight coefficients

Sort by the importance of working condition

Comparing the importancebetween two working conditions

Calculating the judgment matrix

Calculating the weight coefficientsof every working condition

consistency check

Conformity

All weight coefficients of multi-objectivetopology optimization is obtained

End

Criterionlayer

Index layerYes

No

Figure 9 The calculating flow chart of the weight coefficients

Then the all weighting coefficients are calculated through theconsistency check

531 Criteria Layer Decision There are static stiffness topol-ogy optimization and dynamic natural frequency topologyoptimization in the criterion layer and the correspondingweighting factors are respectively 1205721 1205722 The cylinder blocksuffers from the alternating impact loads when differentcylinder explodes and its stiffness performance directlyaffects the working reliability But for the vibration charac-teristics it can be seen from Section 42 that the maximumworking frequency is 100 Hz which is much smaller than thefirst-order natural frequency of 264 Hz Therefore the staticmultiworking condition stiffness is more important in thetopology optimization for the cylinder block So the weightcoefficients 1205721 1205722 are defined as 06 and 04 respectively

532 Index Layer Decision Firstly it is necessary to deter-mine the importance of four working conditions Accordingto the structure efficiency shown in Figure 7 the importanceis sorted the first cylinder the fourth cylinder the secondcylinder and the third cylinder So the weight coefficients areranked as shown in

1199081 gt 1199084 gt 1199082 gt 1199083 (6)

Mathematical Problems in Engineering 9

Table 6 Meanings of relative scale

Relative scale Meanings1 Two elements have equal importance3 The former is slightly important than the latter between two elements

5 The former is obviously important than the latter between twoelements

7 The former is strongly important than the latter between two elements

9 The former is extremely important than the latter between twoelements

2 4 6 8 Indicating the intermediate value above judgment

Reciprocal If the important ratio between the elements 119894 and 119895 is 119909 the importantratio between the elements 119895 and i is 1119909

Then according to the standard meaning table of relativescale in the AHP shown in Table 6 the relative importanceratio of four working conditions is determined and thejudgment matrix119882 is constructed as shown in

119882 =

[[[[[[[[[[[[[[[

11990811199081 1199081119908119894

1199081119908119899 1199081198951199081 119908119895119908119894

119908119895119908119899 1199081198991199081 119908119899119908119894

119908119899119908119899

]]]]]]]]]]]]]]]

=[[[[[[[[[[[

11990811 1199081119894 1199081119899 1199081198951 119908119895119894 119908119895119899 1199081198991 119908119899119894 119908119899119899

]]]]]]]]]]]

(7)

where n is the number of the weight coefficients 119908119894 and119908119895 (119894 119895 = 1 2 6) represent the weight coefficients and119908119895119894 = 119908119895119908119894 denotes the relative importance of 119908119895 to 119908119894According to the results in Section 4 the first cylinder

explosion is the worst condition and it is obviously moreimportant than the third working condition and slightlymore important than the fourth working condition so theweight coefficients 11990813 11990814 are determined as 5 and 2respectivelyThe importance of the secondworking conditionis between the third working condition and the fourthworking condition so the weight coefficient 11990812 is defined as4 In the same way the relative importance ratio of the fourworking conditions is obtained and the judgment matrix isconstructed

119882 =[[[[[[[[[[

1 4 5 214 1 2 1315 12 1 1412 3 4 1

]]]]]]]]]] (8)

The judgment matrix W is right multiplied by a vector120596 = (1199081 1199082 1199083 1199084)Τ consisting of all the weight coefficientsas shown in

119882120596 = 120582120596 997904rArr(119882 minus 120582119868)120596 = 0 (9)

Substituting the judgment matrix 119882 into (9) themaximum eigenvalue 120582max = 40484 is calculatedand the corresponding eigenvector normalized is 120596 =(049 012 008 031)Τ So all weight coefficients areobtained for multiobjective topology optimization of thecylinder block

In order to ensure the accuracy and reliability of thejudgment matrix and avoid influence of individual subjectivefactor the consistency test of the judgment matrix is carriedout in terms of (10) The consistency ratio CR of thejudgment matrixW calculated by (10) is 00179 which is lessthan 01 Therefore it is considered that the judgment matrixhas a satisfactory consistency and the four weight coefficientscan well reflect the importance of each working condition

119862119877 = 119862119868119877119868 (10)

where 119862119868 is the consistency index 119862119868 = (120582max minus119899)(119899 minus 1)119877119868 is the mean random consistency index whose value canbe obtained directly by referring to the standard randomconsistency index 119877119868-119899 table in the analytic hierarchyprocess as shown in Table 7 119862119877 is the random consistencyratio and the inconsistency is acceptable when 119862119877 lt 01

In addition the computing platform of weight coefficientfor multiworking condition topology optimization (TOWC)is built inMatlab to improve the computational efficiency ofthe method as shown in Figure 10 According to the numberof working conditions and the importance of each working

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom

Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 9: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

Mathematical Problems in Engineering 9

Table 6 Meanings of relative scale

Relative scale Meanings1 Two elements have equal importance3 The former is slightly important than the latter between two elements

5 The former is obviously important than the latter between twoelements

7 The former is strongly important than the latter between two elements

9 The former is extremely important than the latter between twoelements

2 4 6 8 Indicating the intermediate value above judgment

Reciprocal If the important ratio between the elements 119894 and 119895 is 119909 the importantratio between the elements 119895 and i is 1119909

Then according to the standard meaning table of relativescale in the AHP shown in Table 6 the relative importanceratio of four working conditions is determined and thejudgment matrix119882 is constructed as shown in

119882 =

[[[[[[[[[[[[[[[

11990811199081 1199081119908119894

1199081119908119899 1199081198951199081 119908119895119908119894

119908119895119908119899 1199081198991199081 119908119899119908119894

119908119899119908119899

]]]]]]]]]]]]]]]

=[[[[[[[[[[[

11990811 1199081119894 1199081119899 1199081198951 119908119895119894 119908119895119899 1199081198991 119908119899119894 119908119899119899

]]]]]]]]]]]

(7)

where n is the number of the weight coefficients 119908119894 and119908119895 (119894 119895 = 1 2 6) represent the weight coefficients and119908119895119894 = 119908119895119908119894 denotes the relative importance of 119908119895 to 119908119894According to the results in Section 4 the first cylinder

explosion is the worst condition and it is obviously moreimportant than the third working condition and slightlymore important than the fourth working condition so theweight coefficients 11990813 11990814 are determined as 5 and 2respectivelyThe importance of the secondworking conditionis between the third working condition and the fourthworking condition so the weight coefficient 11990812 is defined as4 In the same way the relative importance ratio of the fourworking conditions is obtained and the judgment matrix isconstructed

119882 =[[[[[[[[[[

1 4 5 214 1 2 1315 12 1 1412 3 4 1

]]]]]]]]]] (8)

The judgment matrix W is right multiplied by a vector120596 = (1199081 1199082 1199083 1199084)Τ consisting of all the weight coefficientsas shown in

119882120596 = 120582120596 997904rArr(119882 minus 120582119868)120596 = 0 (9)

Substituting the judgment matrix 119882 into (9) themaximum eigenvalue 120582max = 40484 is calculatedand the corresponding eigenvector normalized is 120596 =(049 012 008 031)Τ So all weight coefficients areobtained for multiobjective topology optimization of thecylinder block

In order to ensure the accuracy and reliability of thejudgment matrix and avoid influence of individual subjectivefactor the consistency test of the judgment matrix is carriedout in terms of (10) The consistency ratio CR of thejudgment matrixW calculated by (10) is 00179 which is lessthan 01 Therefore it is considered that the judgment matrixhas a satisfactory consistency and the four weight coefficientscan well reflect the importance of each working condition

119862119877 = 119862119868119877119868 (10)

where 119862119868 is the consistency index 119862119868 = (120582max minus119899)(119899 minus 1)119877119868 is the mean random consistency index whose value canbe obtained directly by referring to the standard randomconsistency index 119877119868-119899 table in the analytic hierarchyprocess as shown in Table 7 119862119877 is the random consistencyratio and the inconsistency is acceptable when 119862119877 lt 01

In addition the computing platform of weight coefficientfor multiworking condition topology optimization (TOWC)is built inMatlab to improve the computational efficiency ofthe method as shown in Figure 10 According to the numberof working conditions and the importance of each working

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

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Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

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Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

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Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

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Dierential EquationsInternational Journal of

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Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 10: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

10 Mathematical Problems in Engineering

Table 7 The standard random consistency index RI-n

n 1 2 3 4 5 6 7 8 9 10RI 0 0 058 09 112 124 132 141 145 149

Figure 10 The computing platform of weight coefficient

condition the platform can automatically construct thejudgment matrix output the weight coefficients and verifyits consistency Taking the cylinder block as an example theoperation steps are as follows

Step 1 Enter the number of working conditions n=4

Step 2 Rank the importance of each working condition[1 4 2 3]Step 3 Refer to Table 6 and enter the relative importancebetween two working conditions expressed in vector formBefore entering the vector you can click the prompt button toget the number of elements you need to input The elementsin the vector are expressed in sequence as the importanceof the first working condition to other working conditionsand the importance of the second working condition to otherworking conditions and so on In this paper six elementsneed to be input for four working conditions of cylinderblock Based on above analysis the corresponding vector is[4 5 2 2 13 14]Step 4 Click the control button ldquocalculating the JudgmentMatrixrdquo and the button ldquocalculating the Weight Coefficientsrdquoin turn the judgment matrix and weight coefficients arecalculated and the consistency is checked If it is satisfied theweight coefficients are output or else the relative importancebetween two working conditions needs to be modified inStep 3 Finally for multiobjective topology optimization ofthe cylinder block the weight coefficients (049 012 008031) are output

54 Mathematical Model

(1) Objective The main objective for the cylinder block is toimprove the static and dynamic characteristics in the actual

A

A A-A

Cylinder wall

Bearing blockOther regions

Figure 11 Optimized region and non-optimized region

working processThe comprehensive evaluation function canconsider both the static multiworking condition stiffness andthe dynamic multiorder natural frequency Therefore thecomprehensive evaluation function shown in (5) is taken asthe optimization objective in this paper

(2) Design Variable The classical variable density topologyoptimization is applied for the cylinder block and the designvariable is set to the relative density of each element in theoptimized area Since the cylinder wall is to cooperate withthe cylinder liner and the cylinder head it is regarded asa nonoptimized area In addition the other area connectedwith the fuel injection pump supercharger radiator bearingblock etc is also set as nonoptimized area In Figure 11the red region represents the nonoptimized region while thegreen region represents the optimized region

(3) Constraint Condition In the process of topology opti-mization it is necessary to ensure that the structure satis-fies the equilibrium equation with the continuous materialremoval in local area And the relative density of each elementis controlled between 0 and 1 In addition the maximummaterial remove rate of the cylinder block is set at 10

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom

Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 11: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

Mathematical Problems in Engineering 11

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(a) Front

Contour Plot

1000E+00

Max = 1000E+00

Min = 1000E-023D 723907

3D 614091

8900E-017800E-016700E-015600E-014500E-013400E-012300E-011200E-011000E-02

No result

Element Densities(Density)

(b) Back

Figure 12 Result of the multiobjective topology optimization

Thus themathematical model of multiobjective topologyoptimization is established as shown in

Find 120588 = (1205881 sdot sdot sdot 120588119899)min 119865 (120588) = 06

2 sdot [ 4sum119894=1

119908119894119862119894 (120588) minus 119862min119894119862max

119894 minus 119862min119894

]2 + 042 (Λmax minus Λ (120588)Λmax minus Λmin)212

Subject to K (120588) u = P

119881 (120588) le 09 sdot 11988100 lt 120588min le 120588119894 le 1

(11)

where 119865(120588) is the comprehensive evaluation function valueK(120588) is the stiffnessmatrix of finite elementmodel and it is thefunction of relative density120588u is the displacement vector andP is the force vector 119881(120588) is the objective volume value and1198810 is the initial volume value 120588min represents the minimumrelative density in all elements and 120588119894 is the relative density ofith element Other variables have the same meaning as (3)sim(5)

6 Results and Discussion

61 Topology Optimization Result The finite element modelof the cylinder block is imported into the topology optimiza-tion software and the load and boundary condition are thesame as those in Section 32 The multiobjective topologyoptimization mathematical model established by (11) is usedfor the cylinder block and the result is shown in Figure 12where the areas from blue to red mean that materials becomemore and more important According to the result the areaswhere materials can be removed are mainly concentrated on

stiffening ribs convex plates the side edges and the innersupport plates of cylinder block Refer to the result of stressanalysis and modal analysis in Section 4 the new model isobtained as shown in Figure 13 where the partial area isremoved the thickness and height of the ribs are changed insome areas and the lightening holes are added in the innersupport plate Its weight has been reduced from 8897 kg to8433 kg accounting for about 522

62 Comparing with Single Objective Topology OptimizationIn order to verify the effectiveness of the multiobjectivetopology optimization proposed in this paper the singleobjective topology optimization of four extreme workingconditions for the cylinder block is studied respectivelyFor the mathematical model only the objective is replacedwith the minimum structural compliance and other variablesremain unchanged as shown in

min 119888 (120588) = u119879Ku = 119899sum119890=1

(120588119890)119901 u119879119890K119890u119890 (12)

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom

Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 12: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

12 Mathematical Problems in Engineering

A

A A-A

removing material changing dimension lightening hole

Figure 13 New model of the cylinder block

where 119888(120588) is structural compliance p is penalty factor 119901 gt1 u119890K119890 are the displacement vector and the element stiffnessmatrix corresponding to the eth element Other variableshave the same meaning as (11)

The results are shown in Figure 14 It shows that thematerial is removed in the vicinity of the fourth cylinderwhen the first cylinder explodes as shown in Figure 14(a)Similarly the material is removed in the vicinity of the firstcylinder when the fourth cylinder explodes as shown inFigure 14(b) So it is very clear that the optimization result isdifferent when different working condition is selectedThat isto say the topology optimization of single working conditionusually only ensures that structural mechanical propertyreaches to optimal in the selected working condition whilethe mechanical property of other working conditions may bereduced to a lower level

By comparing with the results it is necessary to com-prehensively consider all working conditions in topologyoptimization for the cylinder block If the optimization resultof single working condition in a certain working conditionis accepted the structural overall mechanical property maydecrease sharply Therefore it shows that the method pro-posed in this paper has obvious advantages comparing withthe single objective topology optimization

63 Mechanical Properties Analysis of New Model The finiteelement analysis for the new model is used to obtain its staticand dynamic characteristics to verify the optimization effectThe calculation process is the same as Section 4 and thedisplacement and stress distribution are shown inTable 8 andthe top 6-order nature frequencies are shown in Table 9

According to Tables 4 and 8 the comparison of mechani-cal performance including displacement and stress is respec-tively shown in Figures 15 and 16 From the comparison theoverall stress and displacement of four working conditionskeep the same level and the maximum displacement andmaximum stress are slightly reduced in the first and the

Table 8 Results of FEA for the new model

No ofexplosions

Max stress(MPa)

Maxdisplacement

(mm)1 2104 02512 1772 02023 1783 02194 1855 0245

fourth working condition and others are slightly raised Thefirst working condition is still the worst and its displacementand stress distribution are shown in Figure 17 The distri-bution trend of displacement and stress is the same as theoriginal model and the stress is about 80 MPa in most ofregion which ismuch smaller thanmaterial ultimate strength(300 MPa) It indicates that the stiffness and strength of thecylinder block can meet working requirements ComparingTable 5 with Table 9 the 1st natural frequency of newcylinder model is increased by 4 Hz and other order naturalfrequencies remain basically unchanged which indicates thatthe vibration characteristics of the new model meet workingrequirements

To reflect intuitively the comprehensive performance ofthe new model in the explosion of each cylinder structureefficiency is calculated and the results are shown in Table 10It can be seen from the table that the structure efficiency isincreased in the first second and third working conditionindicating that the material utilization rate becomes higherThe structure efficiency of the fourth working condition isdecreased which indicates that the safety becomes higherIn addition the variance of the original model and thenew model are calculated which are 00108 and 00079respectively It denotes that the mechanical performance ofthe new model is more uniform In general the topologystructure of the cylinder block becomes more reasonable bythe multiobjective topology optimization

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom

Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 13: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

Mathematical Problems in Engineering 13

Table 9 The top 6-order modal analysis results for the new model

Orders 1 2 3 4 5 6FrequencyHz 268 495 534 575 785 1018

Contour Plot

1000E+00

Max = 1000E+00

Min = 1500E-013D 723907

3D 739240

9056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

No result

Element Densities(Density)

(a) First cylinder explosion

Max = 1000E+00

Min = 2507E-013D 731946

3D 559134

1000E+009167E-018335E-017502E-016670E-015837E-015005E-014172E-013340E-012507E-01

Contour PlotElement Densities(Density)

No result

(b) Second cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 566290

Contour PlotElement Densities(Density)

No result1500E-012444E-013389E-014333E-015278E-016222E-017167E-018111E-019056E-011000E+00

(c) Third cylinder explosion

Max = 1000E+00

Min = 1500E-013D 577900

3D 581038

1000E+009056E-018111E-017167E-016222E-015278E-014333E-013389E-012444E-011500E-01

Contour PlotElement Densities(Density)

No result

(d) Fourth cylinder explosion

Figure 14 Results of single working topology optimization

original model new model

0

01

02

03

max

disp

lace

men

t (m

m)

2 3 41the number of working conditions

Figure 15 Comparison of the displacement

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom

Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 14: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

14 Mathematical Problems in Engineering

Table 10 Comparison of structure efficiency (MPa∙mm∙kgminus1)Structure efficiency No of explosions

1 2 3 4Original model 6221 4231 4051 5508New model 6262 4245 4630 5389Variation +041 +014 +579 -119

original model new model

0

50

100

150

200

250

max

stre

ss (M

Pa)

2 3 41the number of working conditions

Figure 16 Comparison of the stress

(a) Displacement distribution (b) Stress distribution

Figure 17 Results of FEA for the new model under extreme working condition

7 Conclusion

This paper proposes a multiobjective topology optimizationmethod based on AHP The comprehensive evaluation func-tion for the cylinder block is established by the compromiseprogramming method and the weight coefficients are deter-mined based on AHP The method is applied to the dieselengine cylinder block and several important conclusions areas follows(1)There are alternating impact loads for the diesel enginecylinder block The traditional single-working conditiontopology optimization cannot guarantee its overall mechan-ical performance The comprehensive evaluation functionfor the cylinder block is established by the compromise

programming method which can more accurately evaluatethe structural performance(2) By constructing the hierarchical structure model oftopology optimization including 12 weighting coefficientsthe establishing process of the comprehensive evaluationfunction for cylinder block becomes more hierarchical andthe determination of the weight coefficients has a theoreticalguidance The method is equally suitable for other multiob-jective optimization(3) According to the simulation results the overall struc-tural performance of the cylinder block is improved witha 522 reduction in weight Comparing the structure effi-ciency variances of the original model and the new model itcan be seen that the mechanical performance becomes more

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom

Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 15: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

Mathematical Problems in Engineering 15

uniform under different conditions which shows that thetopology structure of the cylinder block is more reasonable

Data Availability

The [DATA TYPE] data used to support the findings ofthis study are available from the corresponding author uponrequest

Conflicts of Interest

The authors declare that they have no financial and personalrelationships with other people or organizations that caninappropriately influence their work and there is no profes-sional or other personal interest of any nature or kind in anyproduct service andor company that could be construed asinfluencing the position presented in this manuscript

Acknowledgments

The authors would like to acknowledge the supports by theChinese National Key Research and Development Program(Grant No 2016YFC0802900) and the Natural Science Foun-dation of Hebei Province (E2017203372)

References

[1] W Schoffmann H Sorger F Zieher et al ldquoFriction reductionand lightweight design-efficiency improvement at the passengercar base enginerdquo Internationaler Motorenkongress 2015 MitNutzfahrzeugmotorenndashSpezial pp 303ndash330 2015

[2] B Zheng Q L Yong R X Liu and J Meng ldquoFinite elementanalysis and structural improvement of diesel engine connect-ing rodrdquo Advanced Materials Research vol 291-294 pp 2413ndash2416 2011

[3] A Ghasemi ldquoCAE simulations for cylinder block bore distor-tionrdquo SAE Technical Paper vol 2012 no 1 pp 1320ndash1327 2012

[4] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoBlock design of diesel engine for low vibration level basedon topology and shape optimizationrdquo Journal of MechanicalEngineering vol 48 no 9 pp 117ndash122 2012

[5] O Sigmund and K Maute ldquoTopology optimizationapproachesrdquo Structural and Multidisciplinary Optimizationvol 48 no 6 pp 1031ndash1055 2013

[6] Q Zhao X Chen Z-D Ma and Y Lin ldquoReliability-based topology optimization using stochastic response surfacemethod with sparse grid designrdquo Mathematical Problems inEngineering vol 2015 Article ID 487686 13 pages 2015

[7] A Boonpan and S Bureerat ldquoMulti-stage design of an automo-tive componentrdquo International Journal of Vehicle Design vol 60no 1-2 pp 84ndash99 2012

[8] H-S Lee Y-S Lee J-H Kim J-T Jun J-O Lee and C-G Kim ldquoA structural analysis and topology optimization oncylinder block of heavy duty diesel enginrdquo International Journalof Modern Physics B vol 24 no 15 pp 2670ndash2675 2010

[9] W-X Jia Z-Y Hao and H-M Xu ldquoLight-weight design ofsingle cylinder block based on structure optimizationrdquo Journalof Zhejiang University Engineering Science vol 42 no 2 pp224ndash228 2008

[10] X F Du Z J Li F R Bi J H Zhang X Wang and K ShaoldquoLow vibration design of diesel engine body based on topologyand shape optimizationrdquo Journal ofMechanical Engineering vol48 no 9 pp 117ndash122 2012

[11] Z-Y Hao W-X Jia and L Guo ldquoApplication of topologyoptimization to light-weight design of single cylinder enginerdquoJournal of Jiangsu University (Natural Science Edition) vol 27no 4 pp 306ndash309 2006

[12] Y C Kang X M Liu and Y S Jiao ldquoResearch on lightweightquantification of six-cylinder engine cylinder based on topol-ogy optimizationrdquoAutomobile Parts vol 3 no 6 pp 80-81 2011

[13] DGuirguis KHamzaMAlyHHegazi andK Saitou ldquoMulti-objective topology optimization of multi-component contin-uum structures via a Kriging-interpolated level set approachrdquoStructural and Multidisciplinary Optimization vol 51 no 3 pp733ndash748 2014

[14] H Li L Gao and P Li ldquoTopology optimization of structuresunder multiple loading cases with a new compliance-volumeproductrdquo Engineering Optimization vol 46 no 6 pp 725ndash7442014

[15] S Sleesongsom and S Bureerat ldquoNew conceptual design ofaeroelastic wing structures by multi-objective optimizationrdquoEngineering Optimization vol 45 no 1 pp 107ndash122 2013

[16] R Balamurugan C V Ramakrishnan and N SwaminathanldquoA two phase approach based on skeleton convergence andgeometric variables for topology optimization using geneticalgorithmrdquo Structural and Multidisciplinary Optimization vol43 no 3 pp 381ndash404 2011

[17] G-C Luh C-Y Lin and Y-S Lin ldquoA binary particle swarmoptimization for continuum structural topology optimizationrdquoApplied Soft Computing vol 11 no 2 pp 2833ndash2844 2011

[18] T Kunakote and S Bureerat ldquoMulti-objective topology opti-mization using evolutionary algorithmsrdquo Engineering Opti-mization vol 43 no 5 pp 541ndash557 2011

[19] O Sigmund and J Petersson ldquoNumerical instabilities intopology optimization a survey on procedures dealing withcheckerboards mesh-dependencies and local minimardquo Journalof Structural Optimization vol 16 no 1 pp 68ndash75 1998

[20] O Sigmund ldquoOn the usefulness of non-gradient approachesin topology optimizationrdquo Structural and MultidisciplinaryOptimization vol 43 no 5 pp 589ndash596 2011

[21] T L Saaty ldquoAnalytic hierarchy processrdquo inMathematicalModelsfor Decision Support pp 109ndash121 1980

[22] A Darko A P C Chan E E Ameyaw E K Owusu EParn and D J Edwards ldquoReview of application of analytichierarchy process (AHP) in constructionrdquo International Journalof Construction Management pp 1ndash17 2018

[23] C-C Shih R S Horng and S-K Lee ldquoInvestigation of labfire prevention management system of combining root causeanalysis and analytic hierarchy process with event tree analysisrdquoMathematical Problems in Engineering vol 2016 Article ID3161823 12 pages 2016

[24] L Chai and T Sun ldquoThe design of LQG controller for activesuspension based on analytic hierarchy processrdquoMathematicalProblems in Engineering vol 2010 Article ID 701951 19 pages2010

[25] H-Z Li and S Guo ldquoExternal economies evaluation of windpower engineering project based on analytic hierarchy processand matter-element extension modelrdquo Mathematical Problemsin Engineering vol 2013 Article ID 848901 11 pages 2013

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom

Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 16: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

16 Mathematical Problems in Engineering

[26] W S Fernandes M Greco and V S Almeida ldquoApplication ofthe smooth evolutionary structural optimization method com-bined with a multi-criteria decision procedurerdquo EngineeringStructures vol 143 pp 40ndash51 2017

[27] H T Cen Structure Bionics Theory Structure Bionics Design ofLightweight Parts and RP Process Validation BeiHang Univer-sity Beijing China 2004

[28] E Ballestero ldquoUtility functions a compromise programmingapproach to specification and optimizationrdquo Journal of Multi-Criteria Decision Analysis vol 6 no 1 pp 11ndash16 2015

[29] Z DMa N Kikuchi andH-C Cheng ldquoTopological design forvibrating structuresrdquo Computer Methods in Applied Mechanicsand Engineering vol 121 no 1ndash4 pp 259ndash280 1995

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom

Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom

Page 17: Research on Multiobjective Topology Optimization of Diesel ...downloads.hindawi.com/journals/mpe/2019/6194634.pdf · Eigen Mode(Mag) Analysis system (b) esecond-ordermode Contour

Hindawiwwwhindawicom Volume 2018

MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Mathematical Problems in Engineering

Applied MathematicsJournal of

Hindawiwwwhindawicom Volume 2018

Probability and StatisticsHindawiwwwhindawicom Volume 2018

Journal of

Hindawiwwwhindawicom Volume 2018

Mathematical PhysicsAdvances in

Complex AnalysisJournal of

Hindawiwwwhindawicom Volume 2018

OptimizationJournal of

Hindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom Volume 2018

Engineering Mathematics

International Journal of

Hindawiwwwhindawicom Volume 2018

Operations ResearchAdvances in

Journal of

Hindawiwwwhindawicom Volume 2018

Function SpacesAbstract and Applied AnalysisHindawiwwwhindawicom Volume 2018

International Journal of Mathematics and Mathematical Sciences

Hindawiwwwhindawicom Volume 2018

Hindawi Publishing Corporation httpwwwhindawicom Volume 2013Hindawiwwwhindawicom

The Scientific World Journal

Volume 2018

Hindawiwwwhindawicom Volume 2018Volume 2018

Numerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisNumerical AnalysisAdvances inAdvances in Discrete Dynamics in

Nature and SocietyHindawiwwwhindawicom Volume 2018

Hindawiwwwhindawicom

Dierential EquationsInternational Journal of

Volume 2018

Hindawiwwwhindawicom Volume 2018

Decision SciencesAdvances in

Hindawiwwwhindawicom Volume 2018

AnalysisInternational Journal of

Hindawiwwwhindawicom Volume 2018

Stochastic AnalysisInternational Journal of

Submit your manuscripts atwwwhindawicom


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