Research ArticleThe Experimental and Simulation Study of Selective CatalyticReduction System in a Single Cylinder Diesel Engine Using NH3as a Reducing Agent
Manoj Kumar Athrashalil Phaily Sreekumar Jayachandra Sreekalaand Padmanabha MohananDepartment of Mechanical Engineering NITK Surathkal Karnataka Mangalore 575025 India
Correspondence should be addressed to Manoj Kumar Athrashalil Phaily manu666240gmailcom
Received 21 November 2013 Revised 13 March 2014 Accepted 14 March 2014 Published 15 April 2014
Academic Editor Alırio Rodrigues
Copyright copy 2014 Manoj Kumar Athrashalil Phaily et al This is an open access article distributed under the Creative CommonsAttribution License which permits unrestricted use distribution and reproduction in any medium provided the original work isproperly cited
Selective catalytic reduction (SCR) technology has been widely used in automotive applications in order to meet the stringentlimits on emission standards The maximum NO119909 conversion efficiency of an SCR depends on temperature and mass flow rate ofan exhaust gas In order to assess the suitability of CordieritePt catalyst for low temperature application an experimental workis carried out using single cylinder diesel engine for different load conditions by varying ammonia induction rate from 02 kghrto 08 kghr The simulation is carried out using AVL FIRE for the validation of experimental results From the study it has beenfound that for 06 kghr ammonia induction rate themaximum conversion is achieved whereas for 08 kghr conversion is reduceddue to desorption of ammonia Also it has been found that at 75 of load for all mass flow rates of ammonia the conversion wasdrastically reduced due to higher exhaust gas temperature and higher emission of unburnt hydrocarbons More than 55 of NO119909conversion was achieved using CordieritePt catalyst at a temperature of 320∘C
1 Introduction
In NH3SCR system NH
3is inducted to the exhaust gas
coming out from the engine exhaust which will undergovarious reactions to convert NO119909 into free nitrogen (N
2)
The most important reactions are
4NH3+ 4NO +O
2997888rarr 4N
2+ 6H2O (1)
4NH3+ 2NO + 2NO
2997888rarr 4N
2+ 6H2O (2)
Two most commonly used SCR reductants are anhydrous(dry) ammonia and aqueous ammonia or urea Pure anhy-drous ammonia is extremely toxic and difficult to store safelybut does not require further conversion to operate withinan SCR It is typically favoured by large industrial SCRoperators Aqueous ammonia must be hydrolyzed in order touse but it is substantially safer to store and transport thananhydrous ammonia Urea is the safest to store but requires
conversion to ammonia through thermal decomposition inorder to be used as an effective reductant The temperature-programmed activity of a series of oxide-supported (TiO
2
Al2O3and SiO
2) Cu catalysts formed from two different Cu
precursors (Cu(NO3)2and CuSO
4) for the selective catalytic
reduction of NO119909 using solutions of urea as a reductant [1]These activities are compared to those found using NH
3as a
reducing agent over the same catalysts in the presence of H2O
and it is found that catalysts that are active for the selectivereduction of NO119909 with NH
3are inactive for its reduction
using solutions of urea However catalyst plays a major rolein the conversion of NO119909 V
2O5Al2O3catalysts can be used
for operating temperature higher than 250∘C but restrictedto sulphur free application due to deactivation of the cat-alyst from alumina reaction with SO
3forming Al
2(SO4)3
The nonsulphating TiO2carrier was recommended for the
V2O5 Studies that have been carried out with V
2O5catalyst
Hindawi Publishing CorporationInternational Journal of Chemical EngineeringVolume 2014 Article ID 350185 8 pageshttpdxdoiorg1011552014350185
2 International Journal of Chemical Engineering
Figure 1 Experimental test rig
supported on TiO2and WO
3used for Heavy Duty diesel
Engines in Europe with numerous highway studies [2]The studies highlighted that problems with vanadium
catalyst are quickly deactivated at high temperatures above500∘C and concluded that recommended temperature win-dow for vanadium is from 300 to 450∘C [3] Zeolite catalystsare developed to cover a wider range of temperature windowsover platinum- and vanadium-based catalysts Zeolite cata-lysts are developed to extend the operating temperature above350∘Cover platinum and vanadiumbased catalysts Howevertwo types of zeolite catalysts were developed to cover highand low temperature windows The high temperature zeolitecovers temperature windows from 350 to 600∘C Automotivecatalytic converters constantly heat up and cool down as theengine starts and stops This requires some special materialwith the greatest possible resistance to change temperatureand a low heat expansion coefficient There are studiesconducted on the effect of HC emission on the retardedactivity of SCR catalysts [4] They considered CuZSM5FeZSM5 andV
2O5TiO2catalysts and compared the effect of
HC emission on the DeNO119909 efficiency of SCR catalyst Theyconcluded that the primary cause for the inhibition is thecompetitive adsorption of NH
3and C
3H6onto the catalyst
surface and the useless consumption of NH3by the side
reaction including the NH3oxidation and ammoxidation
reactions during the course of NH3SCR reaction with C
3H6
Another study was conducted on the effect of unburnthydrocarbons in the activity of automobile catalysts [5] Thestudy reveals that the NO119909 conversion efficiency of SCRcatalyst will reduce when there is an HC in exhaust gasWhen HCs are added to the flow some C-species depositforms on the surface This result is consistent with a poreblocking effect which will slightly affect the NO119909 removal atthe highest reaction temperature They also found that themost important effect of HC presence on the SCR activity isdue to the competitive adsorption between hydrocarbons andammoniawhich limits theNO119909 conversion efficiency of SCR
In the current work CordieritePt ceramic honeycombstructured catalyst has been used to assess the suitability ofthis material for the medium and light duty diesel vehiclesas it gives resistance to temperature changes and a low heatexpansion coefficient
Ball valve
Exhaust pipeAmmonia injection line
SCR catalyst
Figure 2 SCR setup
Table 1 SCR catalyst properties
Catalyst material CordieritePtCatalyst type Circular honeycomb structureSize of the catalyst 1184mm times 127mm (119863 times 119871)Specific heat 146 kJkgKCell density 400 1in2
Volume of catalyst 12 LWall thickness 0114mmDensity 00215 kgm3
Thermal conductivity 3WmK
2 Experimental Work
Whole set of experiments were conducted at the designedinjection timing of 27 deg bTDC speed of 1500 rpm and 175compression ratio on test rig as shown in Figure 1
Airflow measurement was done by the conventionalmethodU-tubemanometer as well as by air intake DP unit inthe control panel Engine speedmeasurement was sensed andinducted by inductive pickup sensor in conjunctionwith digi-tal RPM indicator which is a part of eddy current dynamome-ter controlling unit The dynamometer shaft rotates close toinductive pickup sensor as an arrangement to send voltagepulse whose frequency is converted into RPM and displayedby digital indicator in the control panel To measure the loadon the engine an eddy current dynamometer is attachedto the crankshaft of the engine An AVL-made exhaust gasanalyzer was used tomeasure the exhaust gas emissionsWiththe analyzer NO119909 (ppm) CO (vol) UBHC (ppm) andCO2(vol) emissions were measured A rotameter specially
calibrated for ammonia was used to measure the flow rate ofammonia The experiments were conducted at no load 25of full load 50 of full load and 75 of full load conditionwith diesel fuel
The experiment is conducted on two conditions firstlywithout using SCR at the exhaust pipe and secondly fitting
International Journal of Chemical Engineering 3
Diesel without SCRDiesel experimental with SCR 02 kghrDiesel simulation with SCR 02 kghr
0 25 50 75
0
100
200
300
400
500
600
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(a)
0 25 50 75
0
100
200
300
400
500
600
Diesel without SCR
Diesel experimental with SCR 06 kghrDiesel simulation with SCR 06 kghr
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(b)
Diesel without SCRDiesel experimental with SCR 04 kghrDiesel simulation with SCR 04 kghr
0 25 50 75
0
100
200
300
400
500
600
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(c)
Diesel without SCRDiesel experimental with SCR 08 kghrDiesel simulation with SCR 08 kghr
0 25 50 75
0
100
200
300
400
500
600
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(d)
Figure 3 Concentration of NO119909 versus percentage of load
SCR catalyst at the exhaust pipe Both the readings will betabulated and can find the DeNO119909 efficiency of SCR
3 SCR Setup
In this experimental setup a circular shaped honeycombtype of SCR catalyst (CordieritePt 12 L) is fitted to theexhaust pipe with flange supports as shown in Figure 2 Seal-ing gaskets were placed in between two flange connectionsThe gasket used was a high temperature resistance type toprevent gas leakage from the exhaust system Some minoradjustment was necessary in the final SCR exhaust assemblybecause of the restricted space within the cell A half inch
barrel nipple of length of 3 inches is coupled to the exhaustpipe through which ammonia gas is passed
A hose pipe from the ammonia cylinder is connected toammonia rotameter where the ammonia flow rate can becontrolled by turning the regulating knob
4 Simulation Work
The simulation has been carried out using CFD code AVLFIRE The governing equations and reactions used in AVLFIRE are listed in [5]Theproperties of thematerial are shownin Table 1
4 International Journal of Chemical Engineering
0 25 50 75
150
200
250
300
350
400
450
500
Exha
ust g
as te
mpe
ratu
re (∘
C)
Load ( kg)
Figure 4 Variation of exhaust gas temperature versus percentage ofload
Themass flow rate of exhaust gas is calculated for differentload conditions It was found that as the load increasesthe mass flow rate of exhaust gas decreases This is due tochange in density of gas When load increases exhaust gastemperature also increases which results in lower density ofa gas The boundary conditions considered in the simulationare given in Table 2 The normalized residual values forthe convergence criteria were taken as 1e-4 for continuitymomentum and energy equations It took 60 iterations toreach the convergenceThemaximum iterationwas limited to60 since the solution arrived at was close to the exact solution(experimental values) within these convergence criteria
The mass fractions of different species including NO119909CO CO
2 H2 and HC are considered from experimental
values measured by AVL Five gas analyzer The outletpressure was assumed to be 1 bar The mass flow rate andtemperature of exhaust gas are also given as input whichis measured by experimental work The SCR catalyst wasmodeled using the abovementioned dimensions and meshedin AVL Workflow manager The simulation is carried out fordifferent load conditions by varying ammonia flow rate from02 kghr to 08 kghr
5 Results and Discussion
Theexperiment was carried out for diesel fuel by varying loadconditions It reveals that as the load increases the exhaustgas temperature increases The flow rate of ammonia is alsovaried from 02 kghr to 08 kghr The three major factorswhich have got significant effect in the conversion of NO119909are exhaust gas temperature exhaust gas mass flow rate andammonia flow rate
The SCR catalyst used in the experiment can withstandtemperature range up to 500∘CTherefore the load conditionapplied was limited to 75 of full load where exhaust gastemperature was found to be 486∘C At 100 of load thetemperature will go beyond 520∘C which will damage the
SCR catalyst which in turn affects the exhaust gas analyserThe experiment has been carried out for two conditions Inthe first case SCR catalyst was not fitted at the downstreamexhaust pipe Engine was run for different load conditionsand the concentration ofNO119909wasmeasured directly byAVL-made Five gas analyser In the second case the SCR catalysthas been fitted at the exhaust pipe The ammonia gas wasinducted to the exhaust pipe just before SCR setup The flowrate has been varied from 02 kghr to 08 kghr Again theengine can run in varying load conditionsThe concentrationof NO119909 can again be measured by exhaust gas analyzerFigure 3 explains the concentration of NO119909 measured forboth the conditions explained above
From Figure 3 it is clear that as the load increases theconcentration of NO119909 also increases because of higher com-bustion temperature The higher combustion temperatureresults in higher exhaust gas temperature
Figure 4 explains the variation of exhaust gas temperaturewith respect to varying load conditions It shows that asthe percentage load increases the exhaust gas temperaturealso increases At no load condition 180∘C temperature wasobserved whereas at 25 of full load at 50 of full load andat 75of full load 260∘C 378∘C and 486∘C temperatures havebeen observed From the graph it can be clearly observed thatat 50 of full load for all the ammonia flow rates maximumconversion has been observed where NO119909 concentrationwas reduced from 378 ppm to 169 ppm This is because thecatalyst exhibited themaximum selectivity at the temperatureof 378∘CTheminimum conversion is observed at 75 of fullload where NO119909 concentration was reduced from 615 ppmto 526 ppmTheNO119909 conversionwith respect to varying loadcondition is explained in Figure 5
It was found that up to 50 load NO119909 conversion keepson increasing whereas at 75 load DeNO119909 efficiency isdrastically reduced Similar pattern of graph is observed forall the ammonia mass flow rate conditions It was foundthat the experimental values are in close agreement withsimulation results The increase in NO119909 conversion is due toincrease in exhaust gas temperature At 50 load maximumconversion is obtained since the exhaust gas temperatureis 320∘C where the catalyst exhibits maximum selectivitydue to which fast SCR reaction takes place which in turnconverts NO119909 into free nitrogen (N
2) It was found that for
02 kghr of ammonia induction at no load condition up to25 of NO119909 conversion is achieved Similarly for 04 kghr06 kghr and 08 kghr of ammonia induction rate 2629 and 27 of NO119909 conversion are achieved as shownin Figure 5 Similarly at 25 load for 02 kghr 04 kghr06 kghr and 08 kghr ammonia induction rate 31 3336 and 34 of NO119909 conversion are achieved A slightincrement in NO119909 conversion is achieved at 25 loadbecause of increased exhaust gas temperature and lowermassflow rate of exhaust gas At 50 load maximum conversionis obtained for all the mass flow rates It was found thatat 02 kghr ammonia induction 55 of NO119909 conversionis obtained Similarly for 04 kghr 06 kghr and 08 kghrammonia induction 55 55 and 54 of NO119909 conversion
International Journal of Chemical Engineering 5
Table 2 Boundary conditions used in the simulation work
Solver control discretizationCalculation of boundaryconditions extrapolate
Calculation of derivativesleast square fit Iteration method simple Decoupled domains no Realizability constraints
noEquation control
Momentum and continuityyes Turbulence K-epsilon Energy yes Viscous heating yes Pressure work yes
Differencing schemeMomentum centraldifferencing
Continuity centraldifferencing Turbulence upwind Energy upwind Scalar upwind
Convergence criteria per time stepMaximum number of iterations 60 Minimum number of iterations 10
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 02 kghrDiesel simulation 02 kghr
NOx
conv
ersio
n (
)
(a)
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 04 kghrDiesel simulation 04 kghr
NOx
conv
ersio
n (
)
(b)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 06 kghrDiesel simulation 06 kghr
NOx
conv
ersio
n (
)
(c)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 08 kghrDiesel simulation 08 kghr
NOx
conv
ersio
n (
)
(d)
Figure 5 NO119909 conversion versus percentage of load
6 International Journal of Chemical Engineering
are obtained The conversion is more here due to higherexhaust gas temperature and higher reaction rate
But at 75 load the NO119909 conversion is reduced dras-tically due to increased exhaust gas temperature At veryhigh temperature (gt450∘C) the catalyst selectivity goes ondecreasing due to sintering effect of the catalyst [6] anddesorption of ammonia [7] through the walls of monolithAnother reason for the lower NO119909 conversion at 75 loadis the increased emission of hydrocarbons as explained inthe Introduction part Figure 6 explains the concentration ofunburnt hydrocarbons for different load conditions
At 75 load 34 ppm of HC can be liberated whencompared with no load where just 13 ppm of HC emissionis found When there is more emission of HC at highertemperature the carbon particles deposit at the pores of thecatalyst which results in lower NO119909 conversion
The NH3conversion is another parameter which will
greatly influence NO119909 conversion The concentration ofammonia can be calculated in different ammonia flow rateFour samples of 1 NHCL acid had been taken in beakersAmmonia gas was passed through these samples for differentammonia flow rates varying from 02 kghr to 08 kghr Thetitration was carried out against 1 NNaOH Also a blanktitration was carried out for 1 NHCL acid without ammoniagas passing through it against 1 NNaOH The readings weretabulated and the concentration is calculated by subtractingboth the readings It has been found that as the ammonia flowrate increases the concentration of ammonia also increasesFrom Figure 7 it can be noted that for 02 kghr ammoniaflow rate 400 ppm ammonia concentration is obtained Simi-larly for 04 kghr 06 kghr and 08 kghr ammonia flow rate450 ppm 550 ppm and 600 ppm ammonia concentrationsare obtained
Ammonia slip is the major disadvantage in SCR systemwhich will harm the environment and cause health problemsHence NH
3conversion is the major focus of study in the
current work Figure 8 explains the NH3conversion with
respect to varying load conditionsFrom Figure 5 it was found that there is no much
difference in NO119909 conversion by varying ammonia flow ratefrom 02 kghr to 08 kghr Hence the study is focused onto find out the optimum ammonia inlet concentration whichwill result in the maximum NH
3conversion From Figure 8
it has been found that using 02 kghr ammonia flow ratethe maximum conversion of 24 of NH
3conversion was
achieved Since the ammonia flow meter used in the exper-iment can measure a minimum of 02 kghr ammonia flowrate where ammonia concentrationwas found to be 400 ppmthe simulation work has been extended by again minimizingthe ammonia inlet concentration to find out the maximumNH3conversion efficiency
The ammonia inlet concentration was varied from100 ppm to 400 ppm to find out the maximum NH
3con-
version It has been observed that below 100 ppm ammoniainlet concentration the NO119909 conversion as well as NH
3
conversion is drastically reduced Hence ammonia inletconcentration was limited to 100 ppm Figure 9 explains the
0 25 50 75
5
10
15
20
25
30
35
HC
(ppm
)
Load ( kg)
Figure 6 Hydrocarbon emission versus percentage of load
02 03 04 05 06 07 08
400
450
500
550
600A
mm
onia
conc
entr
atio
n (p
pm)
Ammonia concentration
Ammonia flow rate (kghr)
Figure 7 Variation of NH3
concentration with respect to inletammonia flow rate
NH3conversion rate with respect to varying ammonia inlet
concentrationIt was found that as the ammonia inlet concentration
reduces the NH3conversion rate increases At 50 of full
load and 100 ppm ammonia inlet concentration 98 of NH3
conversion was achieved Similarly for 100 ppm ammoniainlet concentration at no load condition at 25 of full loadand at 75 of full load 13 36 and 41 of NH
3conversion
were achieved This reveals that 100 ppm ammonia inletconcentration is the optimum concentration which willresult in the maximum NH
3conversion The corresponding
NO119909 conversion is also given in Figure 10 It has been foundthat there is slight increment at 50 of load where 58 ofNO119909 conversion was achieved Hence it can be concludedthat the CordieritePt catalyst will give a maximum of 58 ofNO119909 conversion at 100 ppm of ammonia inlet concentration
International Journal of Chemical Engineering 7
0 25 50 75
0
5
10
15
20
25
NH
3co
nver
sion
()
Diesel 02 kghrDiesel 04 kghr
Diesel 06 kghrDiesel 08 kghr
Load ( kg)
Figure 8 NH3
conversion versus percentage of load
100 150 200 250 300 350 400
0
20
40
60
80
100
Ammonia inlet concentration (ppm)
NH
3co
nver
sion
()
No load25 load
50 load75 load
Figure 9 NH3
conversion versus ammonia inlet concentration
6 Conclusions
(1) It has been found that up to 06 kghr ammoniainduction the NO119909 conversion goes on increasingwhereas at 08 kghr NO119909 conversion is slightlyreduced due to desorption of ammonia and blockageof pores in a catalyst
(2) At 50 load and for all the ammonia flow rate con-ditions gt50 of NO119909 conversion has been achieveddue to higher exhaust gas temperature where catalystshows better selectivity which results in conversion ofNO119909 into free nitrogen (N
2)
(3) At 75 load and for all ammonia flow rate conditionsthe NO119909 conversion has been reduced drastically
100 150 200 250 300 350 400
15
20
25
30
35
40
45
50
55
60
Ammonia inlet concentration (ppm)
No load25 load
50 load75 load
NOx
conv
ersio
n (
)
Figure 10 NO119909 conversion versus ammonia inlet concentration
because of ammonia desorption and increased emis-sion of unburnt hydrocarbons
(4) It was found that as the ammonia inlet concentrationreduces the NH
3conversion goes on increasing
where a slight increment in NO119909 conversion is onlyobserved It concludes that CordieritePt catalyst willgive a maximum of 58 of NO119909 conversion at100 ppm of ammonia inlet concentration
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors greatly acknowledge AVL-AST for providingsoftware AVL FIRE for conducting the simulation work
References
[1] A J Sullivan and A J Doherty ldquoNH3
and Urea in the selectivecatalytic reduction of NOx over oxide-supported copper cata-lystsrdquoApplied Catalysis B Environmental vol 55 no 3 pp 185ndash194 2005
[2] L Lietti I Nova E Tronconi and P Forzatti ldquoTransient kineticstudy of the SCR-DeNOx reactionrdquo Catalysis Today vol 45 no1ndash4 pp 85ndash92 1998
[3] J Gieshoff A Schafer-Sindlinger P C Spurk and J A Avan den Tillaart ldquoImproved SCR systems for heavy dutyapplicationsrdquo SAE Technical Paper 2000-01-0189 2000
[4] I Malpartida O Marie P Bazin M Daturi and X JeandelldquoAn operando IR study of the unburnt HC effect on the activityof a commercial automotive catalyst for NH
3
-SCRrdquo AppliedCatalysis B Environmental vol 102 no 1-2 pp 190ndash200 2011
8 International Journal of Chemical Engineering
[5] I Heo Y Lee I-S Nam JW Choung J-H Lee and H-J KimldquoEffect of hydrocarbon slip onNO removal activity of CuZSM5FeZSM5 and V
2
O5
TiO2
catalysts by NH3
rdquo Microporous andMesoporous Materials vol 141 no 1ndash3 pp 8ndash15 2011
[6] S Pritchard ldquoOptimizing SCR catalyst design and performancefor coal-fired boilersrdquo in Proceedings of the EPAEPRI Sympo-sium on Stationary Combination NOx Control 1995
[7] I Nova L Lietti E Tronconi and P Forzatti ldquoDynamics of SCRreaction over a TiO
3
-supported vanadia-tungsta commercialcatalystrdquo Catalysis Today vol 60 no 1 pp 73ndash82 2000
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International Journal of
2 International Journal of Chemical Engineering
Figure 1 Experimental test rig
supported on TiO2and WO
3used for Heavy Duty diesel
Engines in Europe with numerous highway studies [2]The studies highlighted that problems with vanadium
catalyst are quickly deactivated at high temperatures above500∘C and concluded that recommended temperature win-dow for vanadium is from 300 to 450∘C [3] Zeolite catalystsare developed to cover a wider range of temperature windowsover platinum- and vanadium-based catalysts Zeolite cata-lysts are developed to extend the operating temperature above350∘Cover platinum and vanadiumbased catalysts Howevertwo types of zeolite catalysts were developed to cover highand low temperature windows The high temperature zeolitecovers temperature windows from 350 to 600∘C Automotivecatalytic converters constantly heat up and cool down as theengine starts and stops This requires some special materialwith the greatest possible resistance to change temperatureand a low heat expansion coefficient There are studiesconducted on the effect of HC emission on the retardedactivity of SCR catalysts [4] They considered CuZSM5FeZSM5 andV
2O5TiO2catalysts and compared the effect of
HC emission on the DeNO119909 efficiency of SCR catalyst Theyconcluded that the primary cause for the inhibition is thecompetitive adsorption of NH
3and C
3H6onto the catalyst
surface and the useless consumption of NH3by the side
reaction including the NH3oxidation and ammoxidation
reactions during the course of NH3SCR reaction with C
3H6
Another study was conducted on the effect of unburnthydrocarbons in the activity of automobile catalysts [5] Thestudy reveals that the NO119909 conversion efficiency of SCRcatalyst will reduce when there is an HC in exhaust gasWhen HCs are added to the flow some C-species depositforms on the surface This result is consistent with a poreblocking effect which will slightly affect the NO119909 removal atthe highest reaction temperature They also found that themost important effect of HC presence on the SCR activity isdue to the competitive adsorption between hydrocarbons andammoniawhich limits theNO119909 conversion efficiency of SCR
In the current work CordieritePt ceramic honeycombstructured catalyst has been used to assess the suitability ofthis material for the medium and light duty diesel vehiclesas it gives resistance to temperature changes and a low heatexpansion coefficient
Ball valve
Exhaust pipeAmmonia injection line
SCR catalyst
Figure 2 SCR setup
Table 1 SCR catalyst properties
Catalyst material CordieritePtCatalyst type Circular honeycomb structureSize of the catalyst 1184mm times 127mm (119863 times 119871)Specific heat 146 kJkgKCell density 400 1in2
Volume of catalyst 12 LWall thickness 0114mmDensity 00215 kgm3
Thermal conductivity 3WmK
2 Experimental Work
Whole set of experiments were conducted at the designedinjection timing of 27 deg bTDC speed of 1500 rpm and 175compression ratio on test rig as shown in Figure 1
Airflow measurement was done by the conventionalmethodU-tubemanometer as well as by air intake DP unit inthe control panel Engine speedmeasurement was sensed andinducted by inductive pickup sensor in conjunctionwith digi-tal RPM indicator which is a part of eddy current dynamome-ter controlling unit The dynamometer shaft rotates close toinductive pickup sensor as an arrangement to send voltagepulse whose frequency is converted into RPM and displayedby digital indicator in the control panel To measure the loadon the engine an eddy current dynamometer is attachedto the crankshaft of the engine An AVL-made exhaust gasanalyzer was used tomeasure the exhaust gas emissionsWiththe analyzer NO119909 (ppm) CO (vol) UBHC (ppm) andCO2(vol) emissions were measured A rotameter specially
calibrated for ammonia was used to measure the flow rate ofammonia The experiments were conducted at no load 25of full load 50 of full load and 75 of full load conditionwith diesel fuel
The experiment is conducted on two conditions firstlywithout using SCR at the exhaust pipe and secondly fitting
International Journal of Chemical Engineering 3
Diesel without SCRDiesel experimental with SCR 02 kghrDiesel simulation with SCR 02 kghr
0 25 50 75
0
100
200
300
400
500
600
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(a)
0 25 50 75
0
100
200
300
400
500
600
Diesel without SCR
Diesel experimental with SCR 06 kghrDiesel simulation with SCR 06 kghr
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(b)
Diesel without SCRDiesel experimental with SCR 04 kghrDiesel simulation with SCR 04 kghr
0 25 50 75
0
100
200
300
400
500
600
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(c)
Diesel without SCRDiesel experimental with SCR 08 kghrDiesel simulation with SCR 08 kghr
0 25 50 75
0
100
200
300
400
500
600
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(d)
Figure 3 Concentration of NO119909 versus percentage of load
SCR catalyst at the exhaust pipe Both the readings will betabulated and can find the DeNO119909 efficiency of SCR
3 SCR Setup
In this experimental setup a circular shaped honeycombtype of SCR catalyst (CordieritePt 12 L) is fitted to theexhaust pipe with flange supports as shown in Figure 2 Seal-ing gaskets were placed in between two flange connectionsThe gasket used was a high temperature resistance type toprevent gas leakage from the exhaust system Some minoradjustment was necessary in the final SCR exhaust assemblybecause of the restricted space within the cell A half inch
barrel nipple of length of 3 inches is coupled to the exhaustpipe through which ammonia gas is passed
A hose pipe from the ammonia cylinder is connected toammonia rotameter where the ammonia flow rate can becontrolled by turning the regulating knob
4 Simulation Work
The simulation has been carried out using CFD code AVLFIRE The governing equations and reactions used in AVLFIRE are listed in [5]Theproperties of thematerial are shownin Table 1
4 International Journal of Chemical Engineering
0 25 50 75
150
200
250
300
350
400
450
500
Exha
ust g
as te
mpe
ratu
re (∘
C)
Load ( kg)
Figure 4 Variation of exhaust gas temperature versus percentage ofload
Themass flow rate of exhaust gas is calculated for differentload conditions It was found that as the load increasesthe mass flow rate of exhaust gas decreases This is due tochange in density of gas When load increases exhaust gastemperature also increases which results in lower density ofa gas The boundary conditions considered in the simulationare given in Table 2 The normalized residual values forthe convergence criteria were taken as 1e-4 for continuitymomentum and energy equations It took 60 iterations toreach the convergenceThemaximum iterationwas limited to60 since the solution arrived at was close to the exact solution(experimental values) within these convergence criteria
The mass fractions of different species including NO119909CO CO
2 H2 and HC are considered from experimental
values measured by AVL Five gas analyzer The outletpressure was assumed to be 1 bar The mass flow rate andtemperature of exhaust gas are also given as input whichis measured by experimental work The SCR catalyst wasmodeled using the abovementioned dimensions and meshedin AVL Workflow manager The simulation is carried out fordifferent load conditions by varying ammonia flow rate from02 kghr to 08 kghr
5 Results and Discussion
Theexperiment was carried out for diesel fuel by varying loadconditions It reveals that as the load increases the exhaustgas temperature increases The flow rate of ammonia is alsovaried from 02 kghr to 08 kghr The three major factorswhich have got significant effect in the conversion of NO119909are exhaust gas temperature exhaust gas mass flow rate andammonia flow rate
The SCR catalyst used in the experiment can withstandtemperature range up to 500∘CTherefore the load conditionapplied was limited to 75 of full load where exhaust gastemperature was found to be 486∘C At 100 of load thetemperature will go beyond 520∘C which will damage the
SCR catalyst which in turn affects the exhaust gas analyserThe experiment has been carried out for two conditions Inthe first case SCR catalyst was not fitted at the downstreamexhaust pipe Engine was run for different load conditionsand the concentration ofNO119909wasmeasured directly byAVL-made Five gas analyser In the second case the SCR catalysthas been fitted at the exhaust pipe The ammonia gas wasinducted to the exhaust pipe just before SCR setup The flowrate has been varied from 02 kghr to 08 kghr Again theengine can run in varying load conditionsThe concentrationof NO119909 can again be measured by exhaust gas analyzerFigure 3 explains the concentration of NO119909 measured forboth the conditions explained above
From Figure 3 it is clear that as the load increases theconcentration of NO119909 also increases because of higher com-bustion temperature The higher combustion temperatureresults in higher exhaust gas temperature
Figure 4 explains the variation of exhaust gas temperaturewith respect to varying load conditions It shows that asthe percentage load increases the exhaust gas temperaturealso increases At no load condition 180∘C temperature wasobserved whereas at 25 of full load at 50 of full load andat 75of full load 260∘C 378∘C and 486∘C temperatures havebeen observed From the graph it can be clearly observed thatat 50 of full load for all the ammonia flow rates maximumconversion has been observed where NO119909 concentrationwas reduced from 378 ppm to 169 ppm This is because thecatalyst exhibited themaximum selectivity at the temperatureof 378∘CTheminimum conversion is observed at 75 of fullload where NO119909 concentration was reduced from 615 ppmto 526 ppmTheNO119909 conversionwith respect to varying loadcondition is explained in Figure 5
It was found that up to 50 load NO119909 conversion keepson increasing whereas at 75 load DeNO119909 efficiency isdrastically reduced Similar pattern of graph is observed forall the ammonia mass flow rate conditions It was foundthat the experimental values are in close agreement withsimulation results The increase in NO119909 conversion is due toincrease in exhaust gas temperature At 50 load maximumconversion is obtained since the exhaust gas temperatureis 320∘C where the catalyst exhibits maximum selectivitydue to which fast SCR reaction takes place which in turnconverts NO119909 into free nitrogen (N
2) It was found that for
02 kghr of ammonia induction at no load condition up to25 of NO119909 conversion is achieved Similarly for 04 kghr06 kghr and 08 kghr of ammonia induction rate 2629 and 27 of NO119909 conversion are achieved as shownin Figure 5 Similarly at 25 load for 02 kghr 04 kghr06 kghr and 08 kghr ammonia induction rate 31 3336 and 34 of NO119909 conversion are achieved A slightincrement in NO119909 conversion is achieved at 25 loadbecause of increased exhaust gas temperature and lowermassflow rate of exhaust gas At 50 load maximum conversionis obtained for all the mass flow rates It was found thatat 02 kghr ammonia induction 55 of NO119909 conversionis obtained Similarly for 04 kghr 06 kghr and 08 kghrammonia induction 55 55 and 54 of NO119909 conversion
International Journal of Chemical Engineering 5
Table 2 Boundary conditions used in the simulation work
Solver control discretizationCalculation of boundaryconditions extrapolate
Calculation of derivativesleast square fit Iteration method simple Decoupled domains no Realizability constraints
noEquation control
Momentum and continuityyes Turbulence K-epsilon Energy yes Viscous heating yes Pressure work yes
Differencing schemeMomentum centraldifferencing
Continuity centraldifferencing Turbulence upwind Energy upwind Scalar upwind
Convergence criteria per time stepMaximum number of iterations 60 Minimum number of iterations 10
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 02 kghrDiesel simulation 02 kghr
NOx
conv
ersio
n (
)
(a)
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 04 kghrDiesel simulation 04 kghr
NOx
conv
ersio
n (
)
(b)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 06 kghrDiesel simulation 06 kghr
NOx
conv
ersio
n (
)
(c)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 08 kghrDiesel simulation 08 kghr
NOx
conv
ersio
n (
)
(d)
Figure 5 NO119909 conversion versus percentage of load
6 International Journal of Chemical Engineering
are obtained The conversion is more here due to higherexhaust gas temperature and higher reaction rate
But at 75 load the NO119909 conversion is reduced dras-tically due to increased exhaust gas temperature At veryhigh temperature (gt450∘C) the catalyst selectivity goes ondecreasing due to sintering effect of the catalyst [6] anddesorption of ammonia [7] through the walls of monolithAnother reason for the lower NO119909 conversion at 75 loadis the increased emission of hydrocarbons as explained inthe Introduction part Figure 6 explains the concentration ofunburnt hydrocarbons for different load conditions
At 75 load 34 ppm of HC can be liberated whencompared with no load where just 13 ppm of HC emissionis found When there is more emission of HC at highertemperature the carbon particles deposit at the pores of thecatalyst which results in lower NO119909 conversion
The NH3conversion is another parameter which will
greatly influence NO119909 conversion The concentration ofammonia can be calculated in different ammonia flow rateFour samples of 1 NHCL acid had been taken in beakersAmmonia gas was passed through these samples for differentammonia flow rates varying from 02 kghr to 08 kghr Thetitration was carried out against 1 NNaOH Also a blanktitration was carried out for 1 NHCL acid without ammoniagas passing through it against 1 NNaOH The readings weretabulated and the concentration is calculated by subtractingboth the readings It has been found that as the ammonia flowrate increases the concentration of ammonia also increasesFrom Figure 7 it can be noted that for 02 kghr ammoniaflow rate 400 ppm ammonia concentration is obtained Simi-larly for 04 kghr 06 kghr and 08 kghr ammonia flow rate450 ppm 550 ppm and 600 ppm ammonia concentrationsare obtained
Ammonia slip is the major disadvantage in SCR systemwhich will harm the environment and cause health problemsHence NH
3conversion is the major focus of study in the
current work Figure 8 explains the NH3conversion with
respect to varying load conditionsFrom Figure 5 it was found that there is no much
difference in NO119909 conversion by varying ammonia flow ratefrom 02 kghr to 08 kghr Hence the study is focused onto find out the optimum ammonia inlet concentration whichwill result in the maximum NH
3conversion From Figure 8
it has been found that using 02 kghr ammonia flow ratethe maximum conversion of 24 of NH
3conversion was
achieved Since the ammonia flow meter used in the exper-iment can measure a minimum of 02 kghr ammonia flowrate where ammonia concentrationwas found to be 400 ppmthe simulation work has been extended by again minimizingthe ammonia inlet concentration to find out the maximumNH3conversion efficiency
The ammonia inlet concentration was varied from100 ppm to 400 ppm to find out the maximum NH
3con-
version It has been observed that below 100 ppm ammoniainlet concentration the NO119909 conversion as well as NH
3
conversion is drastically reduced Hence ammonia inletconcentration was limited to 100 ppm Figure 9 explains the
0 25 50 75
5
10
15
20
25
30
35
HC
(ppm
)
Load ( kg)
Figure 6 Hydrocarbon emission versus percentage of load
02 03 04 05 06 07 08
400
450
500
550
600A
mm
onia
conc
entr
atio
n (p
pm)
Ammonia concentration
Ammonia flow rate (kghr)
Figure 7 Variation of NH3
concentration with respect to inletammonia flow rate
NH3conversion rate with respect to varying ammonia inlet
concentrationIt was found that as the ammonia inlet concentration
reduces the NH3conversion rate increases At 50 of full
load and 100 ppm ammonia inlet concentration 98 of NH3
conversion was achieved Similarly for 100 ppm ammoniainlet concentration at no load condition at 25 of full loadand at 75 of full load 13 36 and 41 of NH
3conversion
were achieved This reveals that 100 ppm ammonia inletconcentration is the optimum concentration which willresult in the maximum NH
3conversion The corresponding
NO119909 conversion is also given in Figure 10 It has been foundthat there is slight increment at 50 of load where 58 ofNO119909 conversion was achieved Hence it can be concludedthat the CordieritePt catalyst will give a maximum of 58 ofNO119909 conversion at 100 ppm of ammonia inlet concentration
International Journal of Chemical Engineering 7
0 25 50 75
0
5
10
15
20
25
NH
3co
nver
sion
()
Diesel 02 kghrDiesel 04 kghr
Diesel 06 kghrDiesel 08 kghr
Load ( kg)
Figure 8 NH3
conversion versus percentage of load
100 150 200 250 300 350 400
0
20
40
60
80
100
Ammonia inlet concentration (ppm)
NH
3co
nver
sion
()
No load25 load
50 load75 load
Figure 9 NH3
conversion versus ammonia inlet concentration
6 Conclusions
(1) It has been found that up to 06 kghr ammoniainduction the NO119909 conversion goes on increasingwhereas at 08 kghr NO119909 conversion is slightlyreduced due to desorption of ammonia and blockageof pores in a catalyst
(2) At 50 load and for all the ammonia flow rate con-ditions gt50 of NO119909 conversion has been achieveddue to higher exhaust gas temperature where catalystshows better selectivity which results in conversion ofNO119909 into free nitrogen (N
2)
(3) At 75 load and for all ammonia flow rate conditionsthe NO119909 conversion has been reduced drastically
100 150 200 250 300 350 400
15
20
25
30
35
40
45
50
55
60
Ammonia inlet concentration (ppm)
No load25 load
50 load75 load
NOx
conv
ersio
n (
)
Figure 10 NO119909 conversion versus ammonia inlet concentration
because of ammonia desorption and increased emis-sion of unburnt hydrocarbons
(4) It was found that as the ammonia inlet concentrationreduces the NH
3conversion goes on increasing
where a slight increment in NO119909 conversion is onlyobserved It concludes that CordieritePt catalyst willgive a maximum of 58 of NO119909 conversion at100 ppm of ammonia inlet concentration
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors greatly acknowledge AVL-AST for providingsoftware AVL FIRE for conducting the simulation work
References
[1] A J Sullivan and A J Doherty ldquoNH3
and Urea in the selectivecatalytic reduction of NOx over oxide-supported copper cata-lystsrdquoApplied Catalysis B Environmental vol 55 no 3 pp 185ndash194 2005
[2] L Lietti I Nova E Tronconi and P Forzatti ldquoTransient kineticstudy of the SCR-DeNOx reactionrdquo Catalysis Today vol 45 no1ndash4 pp 85ndash92 1998
[3] J Gieshoff A Schafer-Sindlinger P C Spurk and J A Avan den Tillaart ldquoImproved SCR systems for heavy dutyapplicationsrdquo SAE Technical Paper 2000-01-0189 2000
[4] I Malpartida O Marie P Bazin M Daturi and X JeandelldquoAn operando IR study of the unburnt HC effect on the activityof a commercial automotive catalyst for NH
3
-SCRrdquo AppliedCatalysis B Environmental vol 102 no 1-2 pp 190ndash200 2011
8 International Journal of Chemical Engineering
[5] I Heo Y Lee I-S Nam JW Choung J-H Lee and H-J KimldquoEffect of hydrocarbon slip onNO removal activity of CuZSM5FeZSM5 and V
2
O5
TiO2
catalysts by NH3
rdquo Microporous andMesoporous Materials vol 141 no 1ndash3 pp 8ndash15 2011
[6] S Pritchard ldquoOptimizing SCR catalyst design and performancefor coal-fired boilersrdquo in Proceedings of the EPAEPRI Sympo-sium on Stationary Combination NOx Control 1995
[7] I Nova L Lietti E Tronconi and P Forzatti ldquoDynamics of SCRreaction over a TiO
3
-supported vanadia-tungsta commercialcatalystrdquo Catalysis Today vol 60 no 1 pp 73ndash82 2000
International Journal of
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International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
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Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
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Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
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The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
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Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
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Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
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Navigation and Observation
International Journal of
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DistributedSensor Networks
International Journal of
International Journal of Chemical Engineering 3
Diesel without SCRDiesel experimental with SCR 02 kghrDiesel simulation with SCR 02 kghr
0 25 50 75
0
100
200
300
400
500
600
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(a)
0 25 50 75
0
100
200
300
400
500
600
Diesel without SCR
Diesel experimental with SCR 06 kghrDiesel simulation with SCR 06 kghr
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(b)
Diesel without SCRDiesel experimental with SCR 04 kghrDiesel simulation with SCR 04 kghr
0 25 50 75
0
100
200
300
400
500
600
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(c)
Diesel without SCRDiesel experimental with SCR 08 kghrDiesel simulation with SCR 08 kghr
0 25 50 75
0
100
200
300
400
500
600
Load ( kg)
NOx
conc
entr
atio
n (p
pm)
(d)
Figure 3 Concentration of NO119909 versus percentage of load
SCR catalyst at the exhaust pipe Both the readings will betabulated and can find the DeNO119909 efficiency of SCR
3 SCR Setup
In this experimental setup a circular shaped honeycombtype of SCR catalyst (CordieritePt 12 L) is fitted to theexhaust pipe with flange supports as shown in Figure 2 Seal-ing gaskets were placed in between two flange connectionsThe gasket used was a high temperature resistance type toprevent gas leakage from the exhaust system Some minoradjustment was necessary in the final SCR exhaust assemblybecause of the restricted space within the cell A half inch
barrel nipple of length of 3 inches is coupled to the exhaustpipe through which ammonia gas is passed
A hose pipe from the ammonia cylinder is connected toammonia rotameter where the ammonia flow rate can becontrolled by turning the regulating knob
4 Simulation Work
The simulation has been carried out using CFD code AVLFIRE The governing equations and reactions used in AVLFIRE are listed in [5]Theproperties of thematerial are shownin Table 1
4 International Journal of Chemical Engineering
0 25 50 75
150
200
250
300
350
400
450
500
Exha
ust g
as te
mpe
ratu
re (∘
C)
Load ( kg)
Figure 4 Variation of exhaust gas temperature versus percentage ofload
Themass flow rate of exhaust gas is calculated for differentload conditions It was found that as the load increasesthe mass flow rate of exhaust gas decreases This is due tochange in density of gas When load increases exhaust gastemperature also increases which results in lower density ofa gas The boundary conditions considered in the simulationare given in Table 2 The normalized residual values forthe convergence criteria were taken as 1e-4 for continuitymomentum and energy equations It took 60 iterations toreach the convergenceThemaximum iterationwas limited to60 since the solution arrived at was close to the exact solution(experimental values) within these convergence criteria
The mass fractions of different species including NO119909CO CO
2 H2 and HC are considered from experimental
values measured by AVL Five gas analyzer The outletpressure was assumed to be 1 bar The mass flow rate andtemperature of exhaust gas are also given as input whichis measured by experimental work The SCR catalyst wasmodeled using the abovementioned dimensions and meshedin AVL Workflow manager The simulation is carried out fordifferent load conditions by varying ammonia flow rate from02 kghr to 08 kghr
5 Results and Discussion
Theexperiment was carried out for diesel fuel by varying loadconditions It reveals that as the load increases the exhaustgas temperature increases The flow rate of ammonia is alsovaried from 02 kghr to 08 kghr The three major factorswhich have got significant effect in the conversion of NO119909are exhaust gas temperature exhaust gas mass flow rate andammonia flow rate
The SCR catalyst used in the experiment can withstandtemperature range up to 500∘CTherefore the load conditionapplied was limited to 75 of full load where exhaust gastemperature was found to be 486∘C At 100 of load thetemperature will go beyond 520∘C which will damage the
SCR catalyst which in turn affects the exhaust gas analyserThe experiment has been carried out for two conditions Inthe first case SCR catalyst was not fitted at the downstreamexhaust pipe Engine was run for different load conditionsand the concentration ofNO119909wasmeasured directly byAVL-made Five gas analyser In the second case the SCR catalysthas been fitted at the exhaust pipe The ammonia gas wasinducted to the exhaust pipe just before SCR setup The flowrate has been varied from 02 kghr to 08 kghr Again theengine can run in varying load conditionsThe concentrationof NO119909 can again be measured by exhaust gas analyzerFigure 3 explains the concentration of NO119909 measured forboth the conditions explained above
From Figure 3 it is clear that as the load increases theconcentration of NO119909 also increases because of higher com-bustion temperature The higher combustion temperatureresults in higher exhaust gas temperature
Figure 4 explains the variation of exhaust gas temperaturewith respect to varying load conditions It shows that asthe percentage load increases the exhaust gas temperaturealso increases At no load condition 180∘C temperature wasobserved whereas at 25 of full load at 50 of full load andat 75of full load 260∘C 378∘C and 486∘C temperatures havebeen observed From the graph it can be clearly observed thatat 50 of full load for all the ammonia flow rates maximumconversion has been observed where NO119909 concentrationwas reduced from 378 ppm to 169 ppm This is because thecatalyst exhibited themaximum selectivity at the temperatureof 378∘CTheminimum conversion is observed at 75 of fullload where NO119909 concentration was reduced from 615 ppmto 526 ppmTheNO119909 conversionwith respect to varying loadcondition is explained in Figure 5
It was found that up to 50 load NO119909 conversion keepson increasing whereas at 75 load DeNO119909 efficiency isdrastically reduced Similar pattern of graph is observed forall the ammonia mass flow rate conditions It was foundthat the experimental values are in close agreement withsimulation results The increase in NO119909 conversion is due toincrease in exhaust gas temperature At 50 load maximumconversion is obtained since the exhaust gas temperatureis 320∘C where the catalyst exhibits maximum selectivitydue to which fast SCR reaction takes place which in turnconverts NO119909 into free nitrogen (N
2) It was found that for
02 kghr of ammonia induction at no load condition up to25 of NO119909 conversion is achieved Similarly for 04 kghr06 kghr and 08 kghr of ammonia induction rate 2629 and 27 of NO119909 conversion are achieved as shownin Figure 5 Similarly at 25 load for 02 kghr 04 kghr06 kghr and 08 kghr ammonia induction rate 31 3336 and 34 of NO119909 conversion are achieved A slightincrement in NO119909 conversion is achieved at 25 loadbecause of increased exhaust gas temperature and lowermassflow rate of exhaust gas At 50 load maximum conversionis obtained for all the mass flow rates It was found thatat 02 kghr ammonia induction 55 of NO119909 conversionis obtained Similarly for 04 kghr 06 kghr and 08 kghrammonia induction 55 55 and 54 of NO119909 conversion
International Journal of Chemical Engineering 5
Table 2 Boundary conditions used in the simulation work
Solver control discretizationCalculation of boundaryconditions extrapolate
Calculation of derivativesleast square fit Iteration method simple Decoupled domains no Realizability constraints
noEquation control
Momentum and continuityyes Turbulence K-epsilon Energy yes Viscous heating yes Pressure work yes
Differencing schemeMomentum centraldifferencing
Continuity centraldifferencing Turbulence upwind Energy upwind Scalar upwind
Convergence criteria per time stepMaximum number of iterations 60 Minimum number of iterations 10
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 02 kghrDiesel simulation 02 kghr
NOx
conv
ersio
n (
)
(a)
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 04 kghrDiesel simulation 04 kghr
NOx
conv
ersio
n (
)
(b)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 06 kghrDiesel simulation 06 kghr
NOx
conv
ersio
n (
)
(c)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 08 kghrDiesel simulation 08 kghr
NOx
conv
ersio
n (
)
(d)
Figure 5 NO119909 conversion versus percentage of load
6 International Journal of Chemical Engineering
are obtained The conversion is more here due to higherexhaust gas temperature and higher reaction rate
But at 75 load the NO119909 conversion is reduced dras-tically due to increased exhaust gas temperature At veryhigh temperature (gt450∘C) the catalyst selectivity goes ondecreasing due to sintering effect of the catalyst [6] anddesorption of ammonia [7] through the walls of monolithAnother reason for the lower NO119909 conversion at 75 loadis the increased emission of hydrocarbons as explained inthe Introduction part Figure 6 explains the concentration ofunburnt hydrocarbons for different load conditions
At 75 load 34 ppm of HC can be liberated whencompared with no load where just 13 ppm of HC emissionis found When there is more emission of HC at highertemperature the carbon particles deposit at the pores of thecatalyst which results in lower NO119909 conversion
The NH3conversion is another parameter which will
greatly influence NO119909 conversion The concentration ofammonia can be calculated in different ammonia flow rateFour samples of 1 NHCL acid had been taken in beakersAmmonia gas was passed through these samples for differentammonia flow rates varying from 02 kghr to 08 kghr Thetitration was carried out against 1 NNaOH Also a blanktitration was carried out for 1 NHCL acid without ammoniagas passing through it against 1 NNaOH The readings weretabulated and the concentration is calculated by subtractingboth the readings It has been found that as the ammonia flowrate increases the concentration of ammonia also increasesFrom Figure 7 it can be noted that for 02 kghr ammoniaflow rate 400 ppm ammonia concentration is obtained Simi-larly for 04 kghr 06 kghr and 08 kghr ammonia flow rate450 ppm 550 ppm and 600 ppm ammonia concentrationsare obtained
Ammonia slip is the major disadvantage in SCR systemwhich will harm the environment and cause health problemsHence NH
3conversion is the major focus of study in the
current work Figure 8 explains the NH3conversion with
respect to varying load conditionsFrom Figure 5 it was found that there is no much
difference in NO119909 conversion by varying ammonia flow ratefrom 02 kghr to 08 kghr Hence the study is focused onto find out the optimum ammonia inlet concentration whichwill result in the maximum NH
3conversion From Figure 8
it has been found that using 02 kghr ammonia flow ratethe maximum conversion of 24 of NH
3conversion was
achieved Since the ammonia flow meter used in the exper-iment can measure a minimum of 02 kghr ammonia flowrate where ammonia concentrationwas found to be 400 ppmthe simulation work has been extended by again minimizingthe ammonia inlet concentration to find out the maximumNH3conversion efficiency
The ammonia inlet concentration was varied from100 ppm to 400 ppm to find out the maximum NH
3con-
version It has been observed that below 100 ppm ammoniainlet concentration the NO119909 conversion as well as NH
3
conversion is drastically reduced Hence ammonia inletconcentration was limited to 100 ppm Figure 9 explains the
0 25 50 75
5
10
15
20
25
30
35
HC
(ppm
)
Load ( kg)
Figure 6 Hydrocarbon emission versus percentage of load
02 03 04 05 06 07 08
400
450
500
550
600A
mm
onia
conc
entr
atio
n (p
pm)
Ammonia concentration
Ammonia flow rate (kghr)
Figure 7 Variation of NH3
concentration with respect to inletammonia flow rate
NH3conversion rate with respect to varying ammonia inlet
concentrationIt was found that as the ammonia inlet concentration
reduces the NH3conversion rate increases At 50 of full
load and 100 ppm ammonia inlet concentration 98 of NH3
conversion was achieved Similarly for 100 ppm ammoniainlet concentration at no load condition at 25 of full loadand at 75 of full load 13 36 and 41 of NH
3conversion
were achieved This reveals that 100 ppm ammonia inletconcentration is the optimum concentration which willresult in the maximum NH
3conversion The corresponding
NO119909 conversion is also given in Figure 10 It has been foundthat there is slight increment at 50 of load where 58 ofNO119909 conversion was achieved Hence it can be concludedthat the CordieritePt catalyst will give a maximum of 58 ofNO119909 conversion at 100 ppm of ammonia inlet concentration
International Journal of Chemical Engineering 7
0 25 50 75
0
5
10
15
20
25
NH
3co
nver
sion
()
Diesel 02 kghrDiesel 04 kghr
Diesel 06 kghrDiesel 08 kghr
Load ( kg)
Figure 8 NH3
conversion versus percentage of load
100 150 200 250 300 350 400
0
20
40
60
80
100
Ammonia inlet concentration (ppm)
NH
3co
nver
sion
()
No load25 load
50 load75 load
Figure 9 NH3
conversion versus ammonia inlet concentration
6 Conclusions
(1) It has been found that up to 06 kghr ammoniainduction the NO119909 conversion goes on increasingwhereas at 08 kghr NO119909 conversion is slightlyreduced due to desorption of ammonia and blockageof pores in a catalyst
(2) At 50 load and for all the ammonia flow rate con-ditions gt50 of NO119909 conversion has been achieveddue to higher exhaust gas temperature where catalystshows better selectivity which results in conversion ofNO119909 into free nitrogen (N
2)
(3) At 75 load and for all ammonia flow rate conditionsthe NO119909 conversion has been reduced drastically
100 150 200 250 300 350 400
15
20
25
30
35
40
45
50
55
60
Ammonia inlet concentration (ppm)
No load25 load
50 load75 load
NOx
conv
ersio
n (
)
Figure 10 NO119909 conversion versus ammonia inlet concentration
because of ammonia desorption and increased emis-sion of unburnt hydrocarbons
(4) It was found that as the ammonia inlet concentrationreduces the NH
3conversion goes on increasing
where a slight increment in NO119909 conversion is onlyobserved It concludes that CordieritePt catalyst willgive a maximum of 58 of NO119909 conversion at100 ppm of ammonia inlet concentration
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors greatly acknowledge AVL-AST for providingsoftware AVL FIRE for conducting the simulation work
References
[1] A J Sullivan and A J Doherty ldquoNH3
and Urea in the selectivecatalytic reduction of NOx over oxide-supported copper cata-lystsrdquoApplied Catalysis B Environmental vol 55 no 3 pp 185ndash194 2005
[2] L Lietti I Nova E Tronconi and P Forzatti ldquoTransient kineticstudy of the SCR-DeNOx reactionrdquo Catalysis Today vol 45 no1ndash4 pp 85ndash92 1998
[3] J Gieshoff A Schafer-Sindlinger P C Spurk and J A Avan den Tillaart ldquoImproved SCR systems for heavy dutyapplicationsrdquo SAE Technical Paper 2000-01-0189 2000
[4] I Malpartida O Marie P Bazin M Daturi and X JeandelldquoAn operando IR study of the unburnt HC effect on the activityof a commercial automotive catalyst for NH
3
-SCRrdquo AppliedCatalysis B Environmental vol 102 no 1-2 pp 190ndash200 2011
8 International Journal of Chemical Engineering
[5] I Heo Y Lee I-S Nam JW Choung J-H Lee and H-J KimldquoEffect of hydrocarbon slip onNO removal activity of CuZSM5FeZSM5 and V
2
O5
TiO2
catalysts by NH3
rdquo Microporous andMesoporous Materials vol 141 no 1ndash3 pp 8ndash15 2011
[6] S Pritchard ldquoOptimizing SCR catalyst design and performancefor coal-fired boilersrdquo in Proceedings of the EPAEPRI Sympo-sium on Stationary Combination NOx Control 1995
[7] I Nova L Lietti E Tronconi and P Forzatti ldquoDynamics of SCRreaction over a TiO
3
-supported vanadia-tungsta commercialcatalystrdquo Catalysis Today vol 60 no 1 pp 73ndash82 2000
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
4 International Journal of Chemical Engineering
0 25 50 75
150
200
250
300
350
400
450
500
Exha
ust g
as te
mpe
ratu
re (∘
C)
Load ( kg)
Figure 4 Variation of exhaust gas temperature versus percentage ofload
Themass flow rate of exhaust gas is calculated for differentload conditions It was found that as the load increasesthe mass flow rate of exhaust gas decreases This is due tochange in density of gas When load increases exhaust gastemperature also increases which results in lower density ofa gas The boundary conditions considered in the simulationare given in Table 2 The normalized residual values forthe convergence criteria were taken as 1e-4 for continuitymomentum and energy equations It took 60 iterations toreach the convergenceThemaximum iterationwas limited to60 since the solution arrived at was close to the exact solution(experimental values) within these convergence criteria
The mass fractions of different species including NO119909CO CO
2 H2 and HC are considered from experimental
values measured by AVL Five gas analyzer The outletpressure was assumed to be 1 bar The mass flow rate andtemperature of exhaust gas are also given as input whichis measured by experimental work The SCR catalyst wasmodeled using the abovementioned dimensions and meshedin AVL Workflow manager The simulation is carried out fordifferent load conditions by varying ammonia flow rate from02 kghr to 08 kghr
5 Results and Discussion
Theexperiment was carried out for diesel fuel by varying loadconditions It reveals that as the load increases the exhaustgas temperature increases The flow rate of ammonia is alsovaried from 02 kghr to 08 kghr The three major factorswhich have got significant effect in the conversion of NO119909are exhaust gas temperature exhaust gas mass flow rate andammonia flow rate
The SCR catalyst used in the experiment can withstandtemperature range up to 500∘CTherefore the load conditionapplied was limited to 75 of full load where exhaust gastemperature was found to be 486∘C At 100 of load thetemperature will go beyond 520∘C which will damage the
SCR catalyst which in turn affects the exhaust gas analyserThe experiment has been carried out for two conditions Inthe first case SCR catalyst was not fitted at the downstreamexhaust pipe Engine was run for different load conditionsand the concentration ofNO119909wasmeasured directly byAVL-made Five gas analyser In the second case the SCR catalysthas been fitted at the exhaust pipe The ammonia gas wasinducted to the exhaust pipe just before SCR setup The flowrate has been varied from 02 kghr to 08 kghr Again theengine can run in varying load conditionsThe concentrationof NO119909 can again be measured by exhaust gas analyzerFigure 3 explains the concentration of NO119909 measured forboth the conditions explained above
From Figure 3 it is clear that as the load increases theconcentration of NO119909 also increases because of higher com-bustion temperature The higher combustion temperatureresults in higher exhaust gas temperature
Figure 4 explains the variation of exhaust gas temperaturewith respect to varying load conditions It shows that asthe percentage load increases the exhaust gas temperaturealso increases At no load condition 180∘C temperature wasobserved whereas at 25 of full load at 50 of full load andat 75of full load 260∘C 378∘C and 486∘C temperatures havebeen observed From the graph it can be clearly observed thatat 50 of full load for all the ammonia flow rates maximumconversion has been observed where NO119909 concentrationwas reduced from 378 ppm to 169 ppm This is because thecatalyst exhibited themaximum selectivity at the temperatureof 378∘CTheminimum conversion is observed at 75 of fullload where NO119909 concentration was reduced from 615 ppmto 526 ppmTheNO119909 conversionwith respect to varying loadcondition is explained in Figure 5
It was found that up to 50 load NO119909 conversion keepson increasing whereas at 75 load DeNO119909 efficiency isdrastically reduced Similar pattern of graph is observed forall the ammonia mass flow rate conditions It was foundthat the experimental values are in close agreement withsimulation results The increase in NO119909 conversion is due toincrease in exhaust gas temperature At 50 load maximumconversion is obtained since the exhaust gas temperatureis 320∘C where the catalyst exhibits maximum selectivitydue to which fast SCR reaction takes place which in turnconverts NO119909 into free nitrogen (N
2) It was found that for
02 kghr of ammonia induction at no load condition up to25 of NO119909 conversion is achieved Similarly for 04 kghr06 kghr and 08 kghr of ammonia induction rate 2629 and 27 of NO119909 conversion are achieved as shownin Figure 5 Similarly at 25 load for 02 kghr 04 kghr06 kghr and 08 kghr ammonia induction rate 31 3336 and 34 of NO119909 conversion are achieved A slightincrement in NO119909 conversion is achieved at 25 loadbecause of increased exhaust gas temperature and lowermassflow rate of exhaust gas At 50 load maximum conversionis obtained for all the mass flow rates It was found thatat 02 kghr ammonia induction 55 of NO119909 conversionis obtained Similarly for 04 kghr 06 kghr and 08 kghrammonia induction 55 55 and 54 of NO119909 conversion
International Journal of Chemical Engineering 5
Table 2 Boundary conditions used in the simulation work
Solver control discretizationCalculation of boundaryconditions extrapolate
Calculation of derivativesleast square fit Iteration method simple Decoupled domains no Realizability constraints
noEquation control
Momentum and continuityyes Turbulence K-epsilon Energy yes Viscous heating yes Pressure work yes
Differencing schemeMomentum centraldifferencing
Continuity centraldifferencing Turbulence upwind Energy upwind Scalar upwind
Convergence criteria per time stepMaximum number of iterations 60 Minimum number of iterations 10
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 02 kghrDiesel simulation 02 kghr
NOx
conv
ersio
n (
)
(a)
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 04 kghrDiesel simulation 04 kghr
NOx
conv
ersio
n (
)
(b)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 06 kghrDiesel simulation 06 kghr
NOx
conv
ersio
n (
)
(c)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 08 kghrDiesel simulation 08 kghr
NOx
conv
ersio
n (
)
(d)
Figure 5 NO119909 conversion versus percentage of load
6 International Journal of Chemical Engineering
are obtained The conversion is more here due to higherexhaust gas temperature and higher reaction rate
But at 75 load the NO119909 conversion is reduced dras-tically due to increased exhaust gas temperature At veryhigh temperature (gt450∘C) the catalyst selectivity goes ondecreasing due to sintering effect of the catalyst [6] anddesorption of ammonia [7] through the walls of monolithAnother reason for the lower NO119909 conversion at 75 loadis the increased emission of hydrocarbons as explained inthe Introduction part Figure 6 explains the concentration ofunburnt hydrocarbons for different load conditions
At 75 load 34 ppm of HC can be liberated whencompared with no load where just 13 ppm of HC emissionis found When there is more emission of HC at highertemperature the carbon particles deposit at the pores of thecatalyst which results in lower NO119909 conversion
The NH3conversion is another parameter which will
greatly influence NO119909 conversion The concentration ofammonia can be calculated in different ammonia flow rateFour samples of 1 NHCL acid had been taken in beakersAmmonia gas was passed through these samples for differentammonia flow rates varying from 02 kghr to 08 kghr Thetitration was carried out against 1 NNaOH Also a blanktitration was carried out for 1 NHCL acid without ammoniagas passing through it against 1 NNaOH The readings weretabulated and the concentration is calculated by subtractingboth the readings It has been found that as the ammonia flowrate increases the concentration of ammonia also increasesFrom Figure 7 it can be noted that for 02 kghr ammoniaflow rate 400 ppm ammonia concentration is obtained Simi-larly for 04 kghr 06 kghr and 08 kghr ammonia flow rate450 ppm 550 ppm and 600 ppm ammonia concentrationsare obtained
Ammonia slip is the major disadvantage in SCR systemwhich will harm the environment and cause health problemsHence NH
3conversion is the major focus of study in the
current work Figure 8 explains the NH3conversion with
respect to varying load conditionsFrom Figure 5 it was found that there is no much
difference in NO119909 conversion by varying ammonia flow ratefrom 02 kghr to 08 kghr Hence the study is focused onto find out the optimum ammonia inlet concentration whichwill result in the maximum NH
3conversion From Figure 8
it has been found that using 02 kghr ammonia flow ratethe maximum conversion of 24 of NH
3conversion was
achieved Since the ammonia flow meter used in the exper-iment can measure a minimum of 02 kghr ammonia flowrate where ammonia concentrationwas found to be 400 ppmthe simulation work has been extended by again minimizingthe ammonia inlet concentration to find out the maximumNH3conversion efficiency
The ammonia inlet concentration was varied from100 ppm to 400 ppm to find out the maximum NH
3con-
version It has been observed that below 100 ppm ammoniainlet concentration the NO119909 conversion as well as NH
3
conversion is drastically reduced Hence ammonia inletconcentration was limited to 100 ppm Figure 9 explains the
0 25 50 75
5
10
15
20
25
30
35
HC
(ppm
)
Load ( kg)
Figure 6 Hydrocarbon emission versus percentage of load
02 03 04 05 06 07 08
400
450
500
550
600A
mm
onia
conc
entr
atio
n (p
pm)
Ammonia concentration
Ammonia flow rate (kghr)
Figure 7 Variation of NH3
concentration with respect to inletammonia flow rate
NH3conversion rate with respect to varying ammonia inlet
concentrationIt was found that as the ammonia inlet concentration
reduces the NH3conversion rate increases At 50 of full
load and 100 ppm ammonia inlet concentration 98 of NH3
conversion was achieved Similarly for 100 ppm ammoniainlet concentration at no load condition at 25 of full loadand at 75 of full load 13 36 and 41 of NH
3conversion
were achieved This reveals that 100 ppm ammonia inletconcentration is the optimum concentration which willresult in the maximum NH
3conversion The corresponding
NO119909 conversion is also given in Figure 10 It has been foundthat there is slight increment at 50 of load where 58 ofNO119909 conversion was achieved Hence it can be concludedthat the CordieritePt catalyst will give a maximum of 58 ofNO119909 conversion at 100 ppm of ammonia inlet concentration
International Journal of Chemical Engineering 7
0 25 50 75
0
5
10
15
20
25
NH
3co
nver
sion
()
Diesel 02 kghrDiesel 04 kghr
Diesel 06 kghrDiesel 08 kghr
Load ( kg)
Figure 8 NH3
conversion versus percentage of load
100 150 200 250 300 350 400
0
20
40
60
80
100
Ammonia inlet concentration (ppm)
NH
3co
nver
sion
()
No load25 load
50 load75 load
Figure 9 NH3
conversion versus ammonia inlet concentration
6 Conclusions
(1) It has been found that up to 06 kghr ammoniainduction the NO119909 conversion goes on increasingwhereas at 08 kghr NO119909 conversion is slightlyreduced due to desorption of ammonia and blockageof pores in a catalyst
(2) At 50 load and for all the ammonia flow rate con-ditions gt50 of NO119909 conversion has been achieveddue to higher exhaust gas temperature where catalystshows better selectivity which results in conversion ofNO119909 into free nitrogen (N
2)
(3) At 75 load and for all ammonia flow rate conditionsthe NO119909 conversion has been reduced drastically
100 150 200 250 300 350 400
15
20
25
30
35
40
45
50
55
60
Ammonia inlet concentration (ppm)
No load25 load
50 load75 load
NOx
conv
ersio
n (
)
Figure 10 NO119909 conversion versus ammonia inlet concentration
because of ammonia desorption and increased emis-sion of unburnt hydrocarbons
(4) It was found that as the ammonia inlet concentrationreduces the NH
3conversion goes on increasing
where a slight increment in NO119909 conversion is onlyobserved It concludes that CordieritePt catalyst willgive a maximum of 58 of NO119909 conversion at100 ppm of ammonia inlet concentration
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors greatly acknowledge AVL-AST for providingsoftware AVL FIRE for conducting the simulation work
References
[1] A J Sullivan and A J Doherty ldquoNH3
and Urea in the selectivecatalytic reduction of NOx over oxide-supported copper cata-lystsrdquoApplied Catalysis B Environmental vol 55 no 3 pp 185ndash194 2005
[2] L Lietti I Nova E Tronconi and P Forzatti ldquoTransient kineticstudy of the SCR-DeNOx reactionrdquo Catalysis Today vol 45 no1ndash4 pp 85ndash92 1998
[3] J Gieshoff A Schafer-Sindlinger P C Spurk and J A Avan den Tillaart ldquoImproved SCR systems for heavy dutyapplicationsrdquo SAE Technical Paper 2000-01-0189 2000
[4] I Malpartida O Marie P Bazin M Daturi and X JeandelldquoAn operando IR study of the unburnt HC effect on the activityof a commercial automotive catalyst for NH
3
-SCRrdquo AppliedCatalysis B Environmental vol 102 no 1-2 pp 190ndash200 2011
8 International Journal of Chemical Engineering
[5] I Heo Y Lee I-S Nam JW Choung J-H Lee and H-J KimldquoEffect of hydrocarbon slip onNO removal activity of CuZSM5FeZSM5 and V
2
O5
TiO2
catalysts by NH3
rdquo Microporous andMesoporous Materials vol 141 no 1ndash3 pp 8ndash15 2011
[6] S Pritchard ldquoOptimizing SCR catalyst design and performancefor coal-fired boilersrdquo in Proceedings of the EPAEPRI Sympo-sium on Stationary Combination NOx Control 1995
[7] I Nova L Lietti E Tronconi and P Forzatti ldquoDynamics of SCRreaction over a TiO
3
-supported vanadia-tungsta commercialcatalystrdquo Catalysis Today vol 60 no 1 pp 73ndash82 2000
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
International Journal of Chemical Engineering 5
Table 2 Boundary conditions used in the simulation work
Solver control discretizationCalculation of boundaryconditions extrapolate
Calculation of derivativesleast square fit Iteration method simple Decoupled domains no Realizability constraints
noEquation control
Momentum and continuityyes Turbulence K-epsilon Energy yes Viscous heating yes Pressure work yes
Differencing schemeMomentum centraldifferencing
Continuity centraldifferencing Turbulence upwind Energy upwind Scalar upwind
Convergence criteria per time stepMaximum number of iterations 60 Minimum number of iterations 10
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 02 kghrDiesel simulation 02 kghr
NOx
conv
ersio
n (
)
(a)
0 25 50 75
10
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 04 kghrDiesel simulation 04 kghr
NOx
conv
ersio
n (
)
(b)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 06 kghrDiesel simulation 06 kghr
NOx
conv
ersio
n (
)
(c)
0 25 50 75
15
20
25
30
35
40
45
50
55
60
Load ( kg)
Diesel experimental 08 kghrDiesel simulation 08 kghr
NOx
conv
ersio
n (
)
(d)
Figure 5 NO119909 conversion versus percentage of load
6 International Journal of Chemical Engineering
are obtained The conversion is more here due to higherexhaust gas temperature and higher reaction rate
But at 75 load the NO119909 conversion is reduced dras-tically due to increased exhaust gas temperature At veryhigh temperature (gt450∘C) the catalyst selectivity goes ondecreasing due to sintering effect of the catalyst [6] anddesorption of ammonia [7] through the walls of monolithAnother reason for the lower NO119909 conversion at 75 loadis the increased emission of hydrocarbons as explained inthe Introduction part Figure 6 explains the concentration ofunburnt hydrocarbons for different load conditions
At 75 load 34 ppm of HC can be liberated whencompared with no load where just 13 ppm of HC emissionis found When there is more emission of HC at highertemperature the carbon particles deposit at the pores of thecatalyst which results in lower NO119909 conversion
The NH3conversion is another parameter which will
greatly influence NO119909 conversion The concentration ofammonia can be calculated in different ammonia flow rateFour samples of 1 NHCL acid had been taken in beakersAmmonia gas was passed through these samples for differentammonia flow rates varying from 02 kghr to 08 kghr Thetitration was carried out against 1 NNaOH Also a blanktitration was carried out for 1 NHCL acid without ammoniagas passing through it against 1 NNaOH The readings weretabulated and the concentration is calculated by subtractingboth the readings It has been found that as the ammonia flowrate increases the concentration of ammonia also increasesFrom Figure 7 it can be noted that for 02 kghr ammoniaflow rate 400 ppm ammonia concentration is obtained Simi-larly for 04 kghr 06 kghr and 08 kghr ammonia flow rate450 ppm 550 ppm and 600 ppm ammonia concentrationsare obtained
Ammonia slip is the major disadvantage in SCR systemwhich will harm the environment and cause health problemsHence NH
3conversion is the major focus of study in the
current work Figure 8 explains the NH3conversion with
respect to varying load conditionsFrom Figure 5 it was found that there is no much
difference in NO119909 conversion by varying ammonia flow ratefrom 02 kghr to 08 kghr Hence the study is focused onto find out the optimum ammonia inlet concentration whichwill result in the maximum NH
3conversion From Figure 8
it has been found that using 02 kghr ammonia flow ratethe maximum conversion of 24 of NH
3conversion was
achieved Since the ammonia flow meter used in the exper-iment can measure a minimum of 02 kghr ammonia flowrate where ammonia concentrationwas found to be 400 ppmthe simulation work has been extended by again minimizingthe ammonia inlet concentration to find out the maximumNH3conversion efficiency
The ammonia inlet concentration was varied from100 ppm to 400 ppm to find out the maximum NH
3con-
version It has been observed that below 100 ppm ammoniainlet concentration the NO119909 conversion as well as NH
3
conversion is drastically reduced Hence ammonia inletconcentration was limited to 100 ppm Figure 9 explains the
0 25 50 75
5
10
15
20
25
30
35
HC
(ppm
)
Load ( kg)
Figure 6 Hydrocarbon emission versus percentage of load
02 03 04 05 06 07 08
400
450
500
550
600A
mm
onia
conc
entr
atio
n (p
pm)
Ammonia concentration
Ammonia flow rate (kghr)
Figure 7 Variation of NH3
concentration with respect to inletammonia flow rate
NH3conversion rate with respect to varying ammonia inlet
concentrationIt was found that as the ammonia inlet concentration
reduces the NH3conversion rate increases At 50 of full
load and 100 ppm ammonia inlet concentration 98 of NH3
conversion was achieved Similarly for 100 ppm ammoniainlet concentration at no load condition at 25 of full loadand at 75 of full load 13 36 and 41 of NH
3conversion
were achieved This reveals that 100 ppm ammonia inletconcentration is the optimum concentration which willresult in the maximum NH
3conversion The corresponding
NO119909 conversion is also given in Figure 10 It has been foundthat there is slight increment at 50 of load where 58 ofNO119909 conversion was achieved Hence it can be concludedthat the CordieritePt catalyst will give a maximum of 58 ofNO119909 conversion at 100 ppm of ammonia inlet concentration
International Journal of Chemical Engineering 7
0 25 50 75
0
5
10
15
20
25
NH
3co
nver
sion
()
Diesel 02 kghrDiesel 04 kghr
Diesel 06 kghrDiesel 08 kghr
Load ( kg)
Figure 8 NH3
conversion versus percentage of load
100 150 200 250 300 350 400
0
20
40
60
80
100
Ammonia inlet concentration (ppm)
NH
3co
nver
sion
()
No load25 load
50 load75 load
Figure 9 NH3
conversion versus ammonia inlet concentration
6 Conclusions
(1) It has been found that up to 06 kghr ammoniainduction the NO119909 conversion goes on increasingwhereas at 08 kghr NO119909 conversion is slightlyreduced due to desorption of ammonia and blockageof pores in a catalyst
(2) At 50 load and for all the ammonia flow rate con-ditions gt50 of NO119909 conversion has been achieveddue to higher exhaust gas temperature where catalystshows better selectivity which results in conversion ofNO119909 into free nitrogen (N
2)
(3) At 75 load and for all ammonia flow rate conditionsthe NO119909 conversion has been reduced drastically
100 150 200 250 300 350 400
15
20
25
30
35
40
45
50
55
60
Ammonia inlet concentration (ppm)
No load25 load
50 load75 load
NOx
conv
ersio
n (
)
Figure 10 NO119909 conversion versus ammonia inlet concentration
because of ammonia desorption and increased emis-sion of unburnt hydrocarbons
(4) It was found that as the ammonia inlet concentrationreduces the NH
3conversion goes on increasing
where a slight increment in NO119909 conversion is onlyobserved It concludes that CordieritePt catalyst willgive a maximum of 58 of NO119909 conversion at100 ppm of ammonia inlet concentration
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors greatly acknowledge AVL-AST for providingsoftware AVL FIRE for conducting the simulation work
References
[1] A J Sullivan and A J Doherty ldquoNH3
and Urea in the selectivecatalytic reduction of NOx over oxide-supported copper cata-lystsrdquoApplied Catalysis B Environmental vol 55 no 3 pp 185ndash194 2005
[2] L Lietti I Nova E Tronconi and P Forzatti ldquoTransient kineticstudy of the SCR-DeNOx reactionrdquo Catalysis Today vol 45 no1ndash4 pp 85ndash92 1998
[3] J Gieshoff A Schafer-Sindlinger P C Spurk and J A Avan den Tillaart ldquoImproved SCR systems for heavy dutyapplicationsrdquo SAE Technical Paper 2000-01-0189 2000
[4] I Malpartida O Marie P Bazin M Daturi and X JeandelldquoAn operando IR study of the unburnt HC effect on the activityof a commercial automotive catalyst for NH
3
-SCRrdquo AppliedCatalysis B Environmental vol 102 no 1-2 pp 190ndash200 2011
8 International Journal of Chemical Engineering
[5] I Heo Y Lee I-S Nam JW Choung J-H Lee and H-J KimldquoEffect of hydrocarbon slip onNO removal activity of CuZSM5FeZSM5 and V
2
O5
TiO2
catalysts by NH3
rdquo Microporous andMesoporous Materials vol 141 no 1ndash3 pp 8ndash15 2011
[6] S Pritchard ldquoOptimizing SCR catalyst design and performancefor coal-fired boilersrdquo in Proceedings of the EPAEPRI Sympo-sium on Stationary Combination NOx Control 1995
[7] I Nova L Lietti E Tronconi and P Forzatti ldquoDynamics of SCRreaction over a TiO
3
-supported vanadia-tungsta commercialcatalystrdquo Catalysis Today vol 60 no 1 pp 73ndash82 2000
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
6 International Journal of Chemical Engineering
are obtained The conversion is more here due to higherexhaust gas temperature and higher reaction rate
But at 75 load the NO119909 conversion is reduced dras-tically due to increased exhaust gas temperature At veryhigh temperature (gt450∘C) the catalyst selectivity goes ondecreasing due to sintering effect of the catalyst [6] anddesorption of ammonia [7] through the walls of monolithAnother reason for the lower NO119909 conversion at 75 loadis the increased emission of hydrocarbons as explained inthe Introduction part Figure 6 explains the concentration ofunburnt hydrocarbons for different load conditions
At 75 load 34 ppm of HC can be liberated whencompared with no load where just 13 ppm of HC emissionis found When there is more emission of HC at highertemperature the carbon particles deposit at the pores of thecatalyst which results in lower NO119909 conversion
The NH3conversion is another parameter which will
greatly influence NO119909 conversion The concentration ofammonia can be calculated in different ammonia flow rateFour samples of 1 NHCL acid had been taken in beakersAmmonia gas was passed through these samples for differentammonia flow rates varying from 02 kghr to 08 kghr Thetitration was carried out against 1 NNaOH Also a blanktitration was carried out for 1 NHCL acid without ammoniagas passing through it against 1 NNaOH The readings weretabulated and the concentration is calculated by subtractingboth the readings It has been found that as the ammonia flowrate increases the concentration of ammonia also increasesFrom Figure 7 it can be noted that for 02 kghr ammoniaflow rate 400 ppm ammonia concentration is obtained Simi-larly for 04 kghr 06 kghr and 08 kghr ammonia flow rate450 ppm 550 ppm and 600 ppm ammonia concentrationsare obtained
Ammonia slip is the major disadvantage in SCR systemwhich will harm the environment and cause health problemsHence NH
3conversion is the major focus of study in the
current work Figure 8 explains the NH3conversion with
respect to varying load conditionsFrom Figure 5 it was found that there is no much
difference in NO119909 conversion by varying ammonia flow ratefrom 02 kghr to 08 kghr Hence the study is focused onto find out the optimum ammonia inlet concentration whichwill result in the maximum NH
3conversion From Figure 8
it has been found that using 02 kghr ammonia flow ratethe maximum conversion of 24 of NH
3conversion was
achieved Since the ammonia flow meter used in the exper-iment can measure a minimum of 02 kghr ammonia flowrate where ammonia concentrationwas found to be 400 ppmthe simulation work has been extended by again minimizingthe ammonia inlet concentration to find out the maximumNH3conversion efficiency
The ammonia inlet concentration was varied from100 ppm to 400 ppm to find out the maximum NH
3con-
version It has been observed that below 100 ppm ammoniainlet concentration the NO119909 conversion as well as NH
3
conversion is drastically reduced Hence ammonia inletconcentration was limited to 100 ppm Figure 9 explains the
0 25 50 75
5
10
15
20
25
30
35
HC
(ppm
)
Load ( kg)
Figure 6 Hydrocarbon emission versus percentage of load
02 03 04 05 06 07 08
400
450
500
550
600A
mm
onia
conc
entr
atio
n (p
pm)
Ammonia concentration
Ammonia flow rate (kghr)
Figure 7 Variation of NH3
concentration with respect to inletammonia flow rate
NH3conversion rate with respect to varying ammonia inlet
concentrationIt was found that as the ammonia inlet concentration
reduces the NH3conversion rate increases At 50 of full
load and 100 ppm ammonia inlet concentration 98 of NH3
conversion was achieved Similarly for 100 ppm ammoniainlet concentration at no load condition at 25 of full loadand at 75 of full load 13 36 and 41 of NH
3conversion
were achieved This reveals that 100 ppm ammonia inletconcentration is the optimum concentration which willresult in the maximum NH
3conversion The corresponding
NO119909 conversion is also given in Figure 10 It has been foundthat there is slight increment at 50 of load where 58 ofNO119909 conversion was achieved Hence it can be concludedthat the CordieritePt catalyst will give a maximum of 58 ofNO119909 conversion at 100 ppm of ammonia inlet concentration
International Journal of Chemical Engineering 7
0 25 50 75
0
5
10
15
20
25
NH
3co
nver
sion
()
Diesel 02 kghrDiesel 04 kghr
Diesel 06 kghrDiesel 08 kghr
Load ( kg)
Figure 8 NH3
conversion versus percentage of load
100 150 200 250 300 350 400
0
20
40
60
80
100
Ammonia inlet concentration (ppm)
NH
3co
nver
sion
()
No load25 load
50 load75 load
Figure 9 NH3
conversion versus ammonia inlet concentration
6 Conclusions
(1) It has been found that up to 06 kghr ammoniainduction the NO119909 conversion goes on increasingwhereas at 08 kghr NO119909 conversion is slightlyreduced due to desorption of ammonia and blockageof pores in a catalyst
(2) At 50 load and for all the ammonia flow rate con-ditions gt50 of NO119909 conversion has been achieveddue to higher exhaust gas temperature where catalystshows better selectivity which results in conversion ofNO119909 into free nitrogen (N
2)
(3) At 75 load and for all ammonia flow rate conditionsthe NO119909 conversion has been reduced drastically
100 150 200 250 300 350 400
15
20
25
30
35
40
45
50
55
60
Ammonia inlet concentration (ppm)
No load25 load
50 load75 load
NOx
conv
ersio
n (
)
Figure 10 NO119909 conversion versus ammonia inlet concentration
because of ammonia desorption and increased emis-sion of unburnt hydrocarbons
(4) It was found that as the ammonia inlet concentrationreduces the NH
3conversion goes on increasing
where a slight increment in NO119909 conversion is onlyobserved It concludes that CordieritePt catalyst willgive a maximum of 58 of NO119909 conversion at100 ppm of ammonia inlet concentration
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors greatly acknowledge AVL-AST for providingsoftware AVL FIRE for conducting the simulation work
References
[1] A J Sullivan and A J Doherty ldquoNH3
and Urea in the selectivecatalytic reduction of NOx over oxide-supported copper cata-lystsrdquoApplied Catalysis B Environmental vol 55 no 3 pp 185ndash194 2005
[2] L Lietti I Nova E Tronconi and P Forzatti ldquoTransient kineticstudy of the SCR-DeNOx reactionrdquo Catalysis Today vol 45 no1ndash4 pp 85ndash92 1998
[3] J Gieshoff A Schafer-Sindlinger P C Spurk and J A Avan den Tillaart ldquoImproved SCR systems for heavy dutyapplicationsrdquo SAE Technical Paper 2000-01-0189 2000
[4] I Malpartida O Marie P Bazin M Daturi and X JeandelldquoAn operando IR study of the unburnt HC effect on the activityof a commercial automotive catalyst for NH
3
-SCRrdquo AppliedCatalysis B Environmental vol 102 no 1-2 pp 190ndash200 2011
8 International Journal of Chemical Engineering
[5] I Heo Y Lee I-S Nam JW Choung J-H Lee and H-J KimldquoEffect of hydrocarbon slip onNO removal activity of CuZSM5FeZSM5 and V
2
O5
TiO2
catalysts by NH3
rdquo Microporous andMesoporous Materials vol 141 no 1ndash3 pp 8ndash15 2011
[6] S Pritchard ldquoOptimizing SCR catalyst design and performancefor coal-fired boilersrdquo in Proceedings of the EPAEPRI Sympo-sium on Stationary Combination NOx Control 1995
[7] I Nova L Lietti E Tronconi and P Forzatti ldquoDynamics of SCRreaction over a TiO
3
-supported vanadia-tungsta commercialcatalystrdquo Catalysis Today vol 60 no 1 pp 73ndash82 2000
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
International Journal of Chemical Engineering 7
0 25 50 75
0
5
10
15
20
25
NH
3co
nver
sion
()
Diesel 02 kghrDiesel 04 kghr
Diesel 06 kghrDiesel 08 kghr
Load ( kg)
Figure 8 NH3
conversion versus percentage of load
100 150 200 250 300 350 400
0
20
40
60
80
100
Ammonia inlet concentration (ppm)
NH
3co
nver
sion
()
No load25 load
50 load75 load
Figure 9 NH3
conversion versus ammonia inlet concentration
6 Conclusions
(1) It has been found that up to 06 kghr ammoniainduction the NO119909 conversion goes on increasingwhereas at 08 kghr NO119909 conversion is slightlyreduced due to desorption of ammonia and blockageof pores in a catalyst
(2) At 50 load and for all the ammonia flow rate con-ditions gt50 of NO119909 conversion has been achieveddue to higher exhaust gas temperature where catalystshows better selectivity which results in conversion ofNO119909 into free nitrogen (N
2)
(3) At 75 load and for all ammonia flow rate conditionsthe NO119909 conversion has been reduced drastically
100 150 200 250 300 350 400
15
20
25
30
35
40
45
50
55
60
Ammonia inlet concentration (ppm)
No load25 load
50 load75 load
NOx
conv
ersio
n (
)
Figure 10 NO119909 conversion versus ammonia inlet concentration
because of ammonia desorption and increased emis-sion of unburnt hydrocarbons
(4) It was found that as the ammonia inlet concentrationreduces the NH
3conversion goes on increasing
where a slight increment in NO119909 conversion is onlyobserved It concludes that CordieritePt catalyst willgive a maximum of 58 of NO119909 conversion at100 ppm of ammonia inlet concentration
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors greatly acknowledge AVL-AST for providingsoftware AVL FIRE for conducting the simulation work
References
[1] A J Sullivan and A J Doherty ldquoNH3
and Urea in the selectivecatalytic reduction of NOx over oxide-supported copper cata-lystsrdquoApplied Catalysis B Environmental vol 55 no 3 pp 185ndash194 2005
[2] L Lietti I Nova E Tronconi and P Forzatti ldquoTransient kineticstudy of the SCR-DeNOx reactionrdquo Catalysis Today vol 45 no1ndash4 pp 85ndash92 1998
[3] J Gieshoff A Schafer-Sindlinger P C Spurk and J A Avan den Tillaart ldquoImproved SCR systems for heavy dutyapplicationsrdquo SAE Technical Paper 2000-01-0189 2000
[4] I Malpartida O Marie P Bazin M Daturi and X JeandelldquoAn operando IR study of the unburnt HC effect on the activityof a commercial automotive catalyst for NH
3
-SCRrdquo AppliedCatalysis B Environmental vol 102 no 1-2 pp 190ndash200 2011
8 International Journal of Chemical Engineering
[5] I Heo Y Lee I-S Nam JW Choung J-H Lee and H-J KimldquoEffect of hydrocarbon slip onNO removal activity of CuZSM5FeZSM5 and V
2
O5
TiO2
catalysts by NH3
rdquo Microporous andMesoporous Materials vol 141 no 1ndash3 pp 8ndash15 2011
[6] S Pritchard ldquoOptimizing SCR catalyst design and performancefor coal-fired boilersrdquo in Proceedings of the EPAEPRI Sympo-sium on Stationary Combination NOx Control 1995
[7] I Nova L Lietti E Tronconi and P Forzatti ldquoDynamics of SCRreaction over a TiO
3
-supported vanadia-tungsta commercialcatalystrdquo Catalysis Today vol 60 no 1 pp 73ndash82 2000
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
8 International Journal of Chemical Engineering
[5] I Heo Y Lee I-S Nam JW Choung J-H Lee and H-J KimldquoEffect of hydrocarbon slip onNO removal activity of CuZSM5FeZSM5 and V
2
O5
TiO2
catalysts by NH3
rdquo Microporous andMesoporous Materials vol 141 no 1ndash3 pp 8ndash15 2011
[6] S Pritchard ldquoOptimizing SCR catalyst design and performancefor coal-fired boilersrdquo in Proceedings of the EPAEPRI Sympo-sium on Stationary Combination NOx Control 1995
[7] I Nova L Lietti E Tronconi and P Forzatti ldquoDynamics of SCRreaction over a TiO
3
-supported vanadia-tungsta commercialcatalystrdquo Catalysis Today vol 60 no 1 pp 73ndash82 2000
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of