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Modal Analysis of a Rectangular Plate - PDF

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MAE 501: PROJECT 02 Modal Analysis of Rectangular Plate Project Report Sasi Bhushan Beera Person# 35763829
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Page 1: Modal Analysis of  a Rectangular Plate - PDF

MAE 501: PROJECT 02

Modal Analysis of Rectangular Plate

Project Report

Sasi Bhushan Beera Person# 35763829

Page 2: Modal Analysis of  a Rectangular Plate - PDF

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Table of Contents

Problem Details: ...................................................................................................................................... 4

Problem statement: .............................................................................................................................. 4

Geometry of the plate: ......................................................................................................................... 4

Material Properties of the plate: ........................................................................................................... 4

Boundary Conditions: .......................................................................................................................... 4

Element Details: .................................................................................................................................. 4

Modal Analysis using SOLID45: ............................................................................................................. 5

Meshing: ............................................................................................................................................. 5

Solver used for Modal Analysis: .......................................................................................................... 5

Applying boundary conditions: ............................................................................................................ 5

Convergence Criteria: .......................................................................................................................... 5

Results: ............................................................................................................................................... 5

Observations: ...................................................................................................................................... 8

Modal Analysis using SHELL 63: ........................................................................................................... 9

Meshing: ............................................................................................................................................. 9

Solver used for the analysis: .............................................................................................................. 10

Applying boundary conditions: .......................................................................................................... 10

Convergence Criteria: ........................................................................................................................ 10

Results: ............................................................................................................................................. 10

Observations: .................................................................................................................................... 12

Comparison of modal analysis using SOLID45 and SHELL63:.............................................................. 13

Case 1 i.e. h = 2.5mm: ....................................................................................................................... 13

Case 2 i.e. h = 0.625mm: ................................................................................................................... 14

Case3 i.e. h = 0.15625mm: ................................................................................................................ 15

Modal Shapes: ....................................................................................................................................... 17

Mode Shape for the 1st Natural Frequency: ........................................................................................ 17

Mode Shape for the 2nd

Natural Frequency: ........................................................................................ 17

Mode Shape for the 3rd

Natural Frequency: ........................................................................................ 18

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Mode Shape for 4th Natural Frequency: ............................................................................................. 18

Mode Shape for 5th Natural Frequency: ............................................................................................ 189

Conclusion: ........................................................................................................................................... 19

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Problem Details:

Problem statement:

- To determine the lowest six non-zero frequencies and associated mode shapes for a

rectangular plate for three different thickness of the plate.

Geometry of the plate:

- Rectangular Plate with length 2a, width 2b and thickness h.

- γ = a/b=2

- ξ = h/b = 1/4, 1/16, 1/64

- a = 20 mm, b = 10 mm, h = 2.5mm, 0.625mm, 0.15625mm

- Thus, the dimensions of the plate are as follows:

o Length of the plate = 40mm

o Width of the plate = 20mm

o Thickness of the plate = 2.5mm, 0.625mm, 0.15625mm

Material Properties of the plate:

- ν = Poisson’s ratio = 0.05

- Material of the plate : Cast Iron

- E = Modulus of Elasticity = 139.7GPa

- ρ = Density = 7300 kg/m3

Boundary Conditions:

- The two adjacent edges of the rectangular plate are fixed while the other two are free.

Element Details:

- The modal analysis is performed using two types of elements i.e. solid and shell.

Now, we will go through the details of the modal analysis of the plate in case of the different thickness

values as obtained on running the problem using ANSYS 12.

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Modal Analysis using SOLID45:

Meshing:

- A 3-D model of the plate was created and the plate was meshed using SOLID45 element.

- Properties of SOLID45:

o SOLID45 is used for the 3-D modeling of solid structures. The element is defined by

eight nodes having three degrees of freedom at each node: translations in the nodal x,

y, and z directions.

o The element has plasticity, creep, swelling, stress stiffening, large deflection, and

large strain capabilities.

- The mesh was refined per iteration using manual size control. Thus, the mesh was refined

along all the three dimensions of the plate.

Solver used for Modal Analysis:

- The modal analysis was performed using the PCG Lanczos solver.

Applying boundary conditions:

- The two adjacent sides of the plate are fixed in x and y directions and all the four sides are

constrained in z direction.

Convergence Criteria:

- Natural Frequency: For the problem to converge, the variation of all the six natural

frequencies between two iterations should be less that 1%.

Results:

- Case 1 i.e. h = 2.5 mm:

o It was observed that the frequency values go on decreasing as the mesh size is

refined, thus, converging to the lowest frequency values.

o The problem was converged in six iterations and their details of are as follows:

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It.

No

Mesh-

Size(

mm)

Freq-1

(Hz)

%E-

Freq

Freq-2

(Hz)

%E-

Freq

Freq-3

(Hz)

%E-

Freq

Freq-4

(Hz)

%E-

Freq

Freq-5

(Hz)

%E-

Freq

Freq-6

(Hz)

%E-

Freq

1 2.5 21.687

30.076

39.952

45.057

56.733

63.824

2 2.25 21.51

-

0.816

16 29.777

-

0.994

15 38.48

-

3.684

42 44.431

-

1.389

35 53.049

-

6.493

58 62.317

-

2.361

18

3 2 21.41

-

0.464

9 29.633

-

0.483

59 38.417

-

0.163

72 44.125

-

0.688

71 52.995

-

0.101

79 61.48

-

1.343

13

4 1.75 21.279

-

0.611

86 29.453

-

0.607

43 38.327

-

0.234

27 43.774

-

0.795

47 52.918

-

0.145

3 60.396

-

1.763

18

5 1.5 21.194

-

0.399

45 29.322

-

0.444

78 38.25

-

0.200

9 43.495

-

0.637

36 52.857

-

0.115

27 59.728

-

1.106

03

6 1.25 21.134

-

0.283

1 29.224

-

0.334

22 38.184

-

0.172

55 43.278

-

0.498

91 52.808

-

0.092

7 59.275

-

0.758

44

- Case 2 i.e. h = 0.625mm:

o This problem converged in six iterations and their details are as follows:

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It.

No

Mesh-

Size(

mm)

Freq-1

(Hz)

%E-

Freq

Freq-2

(Hz)

%E-

Freq

Freq-3

(Hz)

%E-

Freq

Freq-4

(Hz)

%E-

Freq

Freq-5

(Hz)

%E-

Freq

Freq-6

(Hz)

%E-

Freq

1 2.5 5.7937

8.3503

12.901

18.249

19.684

21.133

2 2.25 5.7322

-

1.061

5 8.2041

-

1.750

84 12.583

-

2.464

93 17.777

-

2.586

44 19.039

-

3.276

77 20.407

-

3.435

39

3 2 5.6923

-

0.696

07 8.1141

-

1.097

01 12.387

-

1.557

66 17.462

-

1.771

95 18.634

-

2.127

21 19.948

-

2.249

23

4 1.75 5.6468

-

0.799

33 8.0226

-

1.127

67 12.195

-

1.550

01 17.083

-

2.170

43 18.241

-

2.109

05 19.442

-

2.536

6

5 1.5 5.6203

-

0.469

29 7.9683

-

0.676

84 12.073

-

1.000

41 16.864

-

1.281

98 17.974

-

1.463

74 19.155

-

1.476

19

6 1.25 5.6037

-

0.295

36 7.9347

-

0.421

67 11.994

-

0.654

35 16.727

-

0.812

38 17.796

-

0.990

32 18.981

-

0.908

38

- Case 3 i.e. h = 0.15625mm:

o Initially, the model is meshed with a much finer mesh of 1.25 mm.

o Thus, the problem converged in five iterations and their details are as follows:

Page 8: Modal Analysis of  a Rectangular Plate - PDF

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It.

No

Mesh-

Size(

mm)

Freq-1

(Hz)

%E-

Freq

Freq-2

(Hz)

%E-

Freq

Freq-3

(Hz)

%E-

Freq

Freq-4

(Hz)

%E-

Freq

Freq-5

(Hz)

%E-

Freq

Freq-6

(Hz)

%E-

Freq

1 1.25 1.4241

2.0588

3.149

4.269

4.7007

4.9974

2 1.125 1.4153

-

0.617

93 2.0313

-

1.335

73 3.0922

-

1.803

75 4.2264

-

0.997

89 4.6007

-

2.127

34 4.895

-

2.049

07

3 1 1.4099

-

0.381

54 2.0152

-

0.792

6 3.0585

-

1.089

84 4.1991

-

0.645

94 4.5408

-

1.301

98 4.8333

-

1.260

47

4 0.875 1.4052

-

0.333

36 2.0015

-

0.679

83 3.0298

-

0.938

37 4.1735

-

0.609

65 4.4889

-

1.142

97 4.7794

-

1.115

18

5 0.75 1.4019

-

0.234

84 1.9923

-

0.459

66 3.0106

-

0.633

71 4.154

-

0.467

23 4.4533

-

0.793

07 4.7419

-

0.784

62

Observations:

- As the thickness of the plate decreases the frequency values go on decreasing as the mass and

the dimensions of the plate are decreased.

- The lower frequencies converge quickly as compared to the higher frequencies.

- The convergence details of each case are plotted graphically below:

- Case 1 i.e. h =2.5mm:

Page 9: Modal Analysis of  a Rectangular Plate - PDF

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- Case 2 i.e. h = 0.625mm:

- Case 3 i.e. h = 0.15625mm:

Modal Analysis using SHELL 63:

Meshing:

- A 2D-model of the plate was created and the plate was meshed using SHELL63 element.

- The thickness of the plate was entered as a real constant of the SHELL63 element.

- Properties of SHELL63:

o SHELL63 has both bending and membrane capabilities.

o Both in-plane and normal loads are permitted.

Page 10: Modal Analysis of  a Rectangular Plate - PDF

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o The element has six degrees of freedom at each node: translations in the nodal x, y,

and z directions and rotations about the nodal x, y, and z-axes. Stress stiffening and

large deflection capabilities are included.

- The mesh was refined per iteration using the manual size control. The mesh size was refined

along the two dimensions of the plate

Solver used for the analysis:

- The PCG Lanczos solver was used to perform the modal analysis.

Applying boundary conditions:

- The fixed boundary conditions are applied to the two adjacent edges and all the edges are

constrained in z direction.

Convergence Criteria:

- It was observed that SHELL63 gave much better convergence that SOLID45. Thus, a lower

convergence criterion was decided for SHELL63 element.

- Natural Frequency: For the problem to converge, the variation of all the six natural

frequencies between two iterations should be less that 0.03%.

Results:

- Case 1 i.e. h = 2.5mm:

As the mesh size is refined, the frequency values increased.

o The problem converged in five iterations and their details are as follows:

It.

No

No of

divisi

ons

Freq-1

(Hz)

%E-

Freq

Freq-2

(Hz)

%E-

Freq

Freq-3

(Hz)

%E-

Freq

Freq-4

(Hz)

%E-

Freq

Freq-5

(Hz)

%E-

Freq

Freq-6

(Hz)

%E-

Freq

1 2.5 15.456

24.593

39.838

39.975

52.277

56.704

2 2.25 15.501

0.291

149 24.766

0.703

452 39.908

0.175

712 40.207

0.580

363 52.628

0.671

423 56.637

-

0.118

16

3 2 15.51

0.058

061 24.799

0.133

247 39.894

-

0.035

08 40.282

0.186

535 52.699

0.134

909 56.624

-

0.022

95

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4 1.75 15.513

0.019

342 24.811

0.048

389 39.899

0.012

533 40.309

0.067

027 52.724

0.047

439 56.62

-

0.007

06

5 1.5 15.514

0.006

446 24.817

0.024

183 39.899 0 40.321

0.029

77 52.736

0.022

76 56.618

-

0.003

53

- Case 2 i.e. h = 0.625mm:

o The problem converged in five iterations and their details are as follows:

It.

No

No of

divisi

ons

Freq-1

(Hz)

%E-

Freq

Freq-2

(Hz)

%E-

Freq

Freq-3

(Hz)

%E-

Freq

Freq-4

(Hz)

%E-

Freq

Freq-5

(Hz)

%E-

Freq

Freq-6

(Hz)

%E-

Freq

1 2.5 3.864

6.1483

9.9596

13.069

15.303

15.354

2 2.25 3.8753

0.292

443 6.1914

0.701

007 10.052

0.927

748 13.157

0.673

349 15.456

0.999

804 15.468

0.742

478

3 1.75 3.8774

0.054

189 6.1998

0.135

672 10.071

0.189

017 13.175

0.136

809 15.489

0.213

509 15.494

0.168

089

4 1.5 3.8782

0.020

632 6.2028

0.048

389 10.077

0.059

577 13.181

0.045

541 15.501

0.077

474 15.504

0.064

541

5 1.25 3.8785

0.007

736 6.2042

0.022

57 10.08

0.029

771 13.184

0.022

76 15.505

0.025

805 15.508

0.025

8

- Case3 i.e. h = 0.15625mm:

o The problem converged in six iterations and their details are as follows:

It.

No

No of

divisi

ons

Freq-1

(Hz)

%E-

Freq

Freq-2

(Hz)

%E-

Freq

Freq-3

(Hz)

%E-

Freq

Freq-4

(Hz)

%E-

Freq

Freq-5

(Hz)

%E-

Freq

Freq-6

(Hz)

%E-

Freq

1 2.5 0.966

1.5371

2.4899

3.2673

3.8257

3.8384

2 2.25

0.9688

2

0.291

925 1.5479

0.702

622 2.513

0.927

748 3.2892

0.670

278 3.864

1.001

124 3.867

0.745

102

3 2.00

0.9693

6

0.055

738 1.55

0.135

668 2.5176

0.183

048 3.2937

0.136

811 3.8723

0.214

803 3.8736

0.170

675

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4 1.75

0.9695

5

0.019

601 1.5507

0.045

161 2.5193

0.067

525 3.2952

0.045

541 3.8753

0.077

473 3.876

0.061

958

5 1.5

0.9696

4

0.009

283 1.5511

0.025

795 2.5201

0.031

755 3.296

0.024

278 3.8767

0.036

126 3.8771

0.028

38

6 1.25

0.9696

8

0.004

125 1.5512

0.006

447 2.5205

0.015

872 3.2964

0.012

136 3.8774

0.018

057 3.8777

0.015

475

Observations:

- As the thickness of the plate decreases the frequency values go on decreasing.

- Lower frequencies converge quickly as compared to higher frequencies.

- The convergence details of each case are plotted graphically below:

- Case 1 i.e. h = 2.5mm:

Page 13: Modal Analysis of  a Rectangular Plate - PDF

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- Case 2 i.e. h = 0.625mm:

- Case 3 i.e. h = 0.15625mm:

Comparison of modal analysis using SOLID45 and SHELL63:

Case 1 i.e. h = 02.5 mm:

- The converged frequency values obtained using SOLID45 and SHELL63 are plotted in the

graph below:

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- It can be observed that the natural frequencies values obtained using SOLID45 are higher

than those obtained using SHELL63.

Case 2 i.e. h = 0.625mm:

- The converged frequency values obtained using SOLID45 and SHELL63 are plotted in the

graph below:

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- The difference in the frequency values of SOLID45 and SHELL63 obtained in Case 2 is

lower as compared to Case 1.

Case3 i.e. h = 0.15625mm:

- The converged frequency values obtained using SOLID45 and SHELL63 are plotted in the

graph below:

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- It can be observed that the natural frequency values obtained from SHELL63 and SOLID45

are almost the same.

- Thus, it can be concluded that, the shell elements show better performance for lower shell

thickness.

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Modal Shapes:

The mode shapes obtained for Case 3 (i.e. h = 0.15625m) for both SHELL63 and SOLID45 are given

below:

Mode Shape for the 1st Natural Frequency:

Solid Elements: Shell Elements:

- The mode shape obtained here is the same for both SOLID45 and SHELL63.

Mode Shape for the 2nd

Natural Frequency:

Solid Elements: Shell Elements:

- The mode shape for both the elements is same.

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Mode Shape for the 3rd

Natural Frequency:

Solid Elements: Shell Elements:

- The mode shape in both the cases is the same.

Mode Shape for 4th Natural Frequency:

Solid Elements: Shell Elements

- Same mode shape is obtained in both the cases with deformations in different directions.

Mode Shape for 5th

Natural Frequency:

Solid Elements: Shell Elements:

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- Different mode shapes are obtained.

Mode shape for 6th

Natural Frequency:

Solid Elements: Shell Elements:

- Different mode shapes are obtained.

Conclusion:

- The natural frequency values of any structure depend on its dimensions and boundary

conditions. In this case, the frequency values decrease with decrease in thickness of the plate.

- Meshing with SHELL elements is easier as compared to SOLID mesh in case of complex

structures.

- SHELL elements give better performance as the shell thickness go on decreasing.

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