Free Hemispherical Shell with a Circular Pole Hole Subjected to Two Orthogonal Pairs of Mutually Balanced Radial Tensile and Compressive Forces Applied at the Equator

Objective: Check of the obtained values of the transverse displacements of a free hemispherical shell with a circular pole hole in the direction of action of two orthogonal pairs of mutually balanced radial tensile and compressive forces applied at the equator.

 

Initial data files:

File name

Description

Quadrant_of_a_spherical_shell_42_Mesh_2x2.spr
Quadrant_of_a_spherical_shell_42_Mesh_4x4.spr
Quadrant_of_a_spherical_shell_42_Mesh_8x8.spr
Quadrant_of_a_spherical_shell_42_Mesh_16x16.spr
Quadrant_of_a_spherical_shell_42_Mesh_32x32.spr

Design model with the elements of type 42 for meshes 2x2, 4x4, 8x8, 16x16, 32x32

Quadrant_of_a_spherical_shell_44_Mesh_2x2.spr
Quadrant_of_a_spherical_shell_44_Mesh_4x4.spr
Quadrant_of_a_spherical_shell_44_Mesh_8x8.spr
Quadrant_of_a_spherical_shell_44_Mesh_16x16.spr
Quadrant_of_a_spherical_shell_44_Mesh_32x32.spr

Design model with the elements of type 44 for meshes 2x2, 4x4, 8x8, 16x16, 32x32

 Quadrant_of_a_spherical_shell_45_Mesh_2x2.spr
Quadrant_of_a_spherical_shell_45_Mesh_4x4.spr
Quadrant_of_a_spherical_shell_45_Mesh_8x8.spr
Quadrant_of_a_spherical_shell_45_Mesh_16x16.spr
Quadrant_of_a_spherical_shell_45_Mesh_32x32.spr

Design model with the elements of type 45 for meshes 2x2, 4x4, 8x8, 16x16, 32x32

Quadrant_of_a_spherical_shell_50_Mesh_2x2.spr
Quadrant_of_a_spherical_shell_50_Mesh_4x4.spr
Quadrant_of_a_spherical_shell_50_Mesh_8x8.spr
Quadrant_of_a_spherical_shell_50_Mesh_16x16.spr
Quadrant_of_a_spherical_shell_50_Mesh_32x32.spr

Design model with the elements of type 50 for meshes 2x2, 4x4, 8x8, 16x16, 32x32

Quadrant_of_a_spherical_solid_36_Mesh_2x2.spr
Quadrant_of_a_spherical_solid_36_Mesh_4x4.spr
Quadrant_of_a_spherical_solid_36_Mesh_8x8.spr
Quadrant_of_a_spherical_solid_36_Mesh_16x16.spr
Quadrant_of_a_spherical_solid_36_Mesh_32x32.spr
Quadrant_of_a_spherical_solid_36_Mesh_64x64.spr
Quadrant_of_a_spherical_solid_36_Mesh_128x128.spr
Quadrant_of_a_spherical_solid_36_Mesh_256x256.spr
Quadrant_of_a_spherical_solid_36_Mesh_512x512.spr

Design model with the elements of type 36 for meshes 2x2, 4x4, 8x8, 16x16, 32x32, 64x64, 128x128, 256x256, 512x512

Quadrant_of_a_spherical_solid_37_Mesh_2x2.spr
Quadrant_of_a_spherical_solid_37_Mesh_4x4.spr
Quadrant_of_a_spherical_solid_37_Mesh_8x8.spr
Quadrant_of_a_spherical_solid_37_Mesh_16x16.spr
Quadrant_of_a_spherical_solid_37_Mesh_32x32.spr
Quadrant_of_a_spherical_solid_37_Mesh_64x64.spr
Quadrant_of_a_spherical_solid_37_Mesh_128x128.spr

Design model with the elements of type 37 for meshes 2x2, 4x4, 8x8, 16x16, 32x32, 64x64, 128x128

 

Problem formulation: The free hemispherical shell with a circular pole hole is subjected to two orthogonal pairs of mutually balanced radial tensile and compressive forces F applied at the equator. Check the obtained values of the transverse displacements of the free hemispherical shell wFX and wFY in the direction of the action of forces applied at the equator.

References: R. H. Macneal, R. L. Harder, A proposed standard set of problems to test finite element accuracy, North-Holland, Finite elements in analysis and design, 1, 1985, p. 3-20.

L. S. D. Morley, A. J. Morris, Conflict between finite elements and shell theory, London, Royal aircraft establishment report, 1978.

Initial data:

E = 6.825·107 kPa - elastic modulus of the material of the hemispherical shell;
ν = 0.30 - Poisson’s ratio;
R = 10.00 m - radius of the midsurface of the hemispherical shell;
2·θ = 2·18° - central angle of the surface of the circular hole of the hemispherical shell;
h = 0.04 m - thickness of the hemispherical shell;
FX = + 2.0 kN - values of the concentrated radial tensile forces applied at the equator of the hemispherical shell;
FY = – 2.0 кН - values of the concentrated radial compressive forces applied at the equator of the hemispherical shell.

 

Finite element model: Design model – general type system. Six design models of a quarter of the hemispherical shell according to the symmetry conditions are considered:

Model 1 – 8, 32, 128, 512, 2048 three-node shell elements of type 42 with a regular mesh 2x2, 4x4, 8x8, 16x16, 32x32. Boundary conditions and the dimensional stability are provided by imposing constraints according to the symmetry conditions. Number of nodes in the model – 9, 25, 81, 289, 1089.

Model 2 – 4, 16, 64, 256, 1024 four-node shell elements of type 44 with a regular mesh 2x2, 4x4, 8x8, 16x16, 32x32. Boundary conditions and the dimensional stability are provided by imposing constraints according to the symmetry conditions. Number of nodes in the model – 9, 25, 81, 289,1089.

Model 3 – 8, 32, 128, 512, 2048 six-node shell elements of type 45 with a regular mesh 2x2, 4x4, 8x8, 16x16, 32x32. Boundary conditions and the dimensional stability are provided by imposing constraints according to the symmetry conditions. Number of nodes in the model – 25, 81, 289, 1089, 4225.

Model 4 – 4, 16, 64, 256, 1024 eight- node shell elements of type 50 with a regular mesh 2x2, 4x4, 8x8, 16x16, 32x32. Boundary conditions and the dimensional stability are provided by imposing constraints according to the symmetry conditions. Number of nodes in the model – 21, 65, 225, 833, 3201.

Model 5 – 4, 16, 64, 256, 1024, 4096, 16384, 65536, 262144 eight-node isoparametric solid elements of type 36 with a regular mesh 2x2x1, 4x4x1, 8x8x1, 16x16x1, 32x32x1, 64x64x1, 128x128x1, 256x256x1, 512x512x1. Boundary conditions and the dimensional stability are provided by imposing constraints according to the symmetry conditions. Number of nodes in the model – 18, 50, 162, 578, 2178, 8450, 33282, 132149, 526338.

Model 6 – 4, 16, 64, 256, 1024, 4096, 16384 twenty-node isoparametric solid elements of type 37 with a regular mesh 2x2x1, 4x4x1, 8x8x1, 16x16x1, 32x32x1, 64x64x1, 128x128x1. Boundary conditions and the dimensional stability are provided by imposing constraints according to the symmetry conditions. Number of nodes in the model – 51, 155, 531, 1955, 7491, 29315, 115971.

 

Results in SCAD




Model 1. Design model

 



Model 1. Deformed model

 










Model 1. Values of the displacements in the direction of the pairs of tensile forces and the pairs of compressive forces along the X and Y axes of the global coordinate system respectively wFX  and wFY (m, m)

 



ScreenShot1685

Model 2. Design model

 



Model 2. Deformed model

 










Model 2. Values of the displacements in the direction of the pairs of tensile forces and the pairs of compressive forces along the X and Y axes of the global coordinate system respectively wFX and wFY (m, m)

 



Model 3. Design model

 



Model 3. Deformed model

 










Model 3. Values of the displacements in the direction of the pairs of tensile forces and the pairs of compressive forces along the X and Y axes of the global coordinate system respectively wFX  and wFY (m, m)

 



Model 4. Design model

 



Model 4. Deformed model

 










Model 4. Values of the displacements in the direction of the pairs of tensile forces and the pairs of compressive forces along the X and Y axes of the global coordinate system respectively wFX  and wFY (m, m)

 





Model 5. Design model

 





Model 5. Deformed model

 
















Model 5. Values of the displacements in the direction of the pairs of tensile forces and the pairs of compressive forces along the X and Y axes of the global coordinate system respectively wFX  and wFY (m, m)

 




Model 6. Design model

 




Model 6. Deformed model

 














Model 6. Values of the displacements in the direction of the pairs of tensile forces and the pairs of compressive forces along the X and Y axes of the global coordinate system respectively wFX  and wFY (m, m)

 

Comparison of solutions:

Displacements in the direction of the pairs of radial tensile forces and the pairs of radial compressive forces FX and FY along the X and Y axes of the global coordinate system respectively wFX  and wFY (m, m)

 

Model

Finite element mesh

Theory

SCAD

Deviation, %

1

(Member type 42)

2x2

+0.0940

–0.0940

+0.0828

–0.0862

11.91

8.30

4x4

+0.0902

–0.0919

4.04

2.23

8x8

+0.0917

–0.0922

2.45

1.91

16x16

+0.0920

–0.0922

2.13

1.91

32x32

+0.0927

–0.0928

1.38

1.28

2

(Member type 44)

2x2

+0.0940

–0.0940

+0.0924

–0.0924

1.70

1.70

4x4

+0.0938

–0.0938

0.21

0.21

8x8

+0.0930

–0.0930

1.06

1.06

16x16

+0.0928

–0.0928

1.28

1.28

32x32

+0.0932

–0.0932

0.85

0.85

3

(Member type 45)

2x2

+0.0940

–0.0940

+0.0506

–0.0510

46.17

45.74

4x4

+0.0389

–0.0395

58.62

57.98

8x8

+0.0484

–0.0489

48.51

47.98

16x16

+0.0834

–0.0835

11.28

11.17

32x32

+0.0927

–0.0927

1.38

1.38

4

(Member type 50)

2x2

+0.0940

–0.0940

+0.0526

–0.0526

44.04

44.04

4x4

+0.0459

–0.0459

51.17

51.17

8x8

+0.0651

–0.0651

30.74

30.74

16x16

+0.0899

–0.0899

4.36

4.36

32x32

+0.0932

–0.0932

0.85

0.85

5

(Member type 36)

2x2

+0.0940

–0.0940

+0.0000

–0.0000

100.00

100.00

4x4

+0.0001

–0.0001

99.89

99.89

8x8

+0.0003

–0.0003

99.68

99.68

16x16

+0.0010

–0.0010

98.94

98.94

32x32

+0.0036

–0.0036

96.17

96.17

64x64

+0.0126

–0.0126

86.60

86.60

128x128

+0.0350

–0.0350

62.77

62.77

256x256

+0.0654

–0.0654

30.43

30.43

512x512

+0.0842

–0.0842

10.43

10.43

6

(Member type 37)

2x2

+0.0940

–0.0940

+0.0014

–0.0014

98.51

98.51

4x4

+0.0100

–0.0100

89.36

89.36

8x8

+0.0589

–0.0590

37.34

37.23

16x16

+0.0900

–0.0900

4.26

4.26

32x32

+0.0933

–0.0933

0.74

0.74

64x64

+0.0936

–0.0936

0.43

0.43

128x128

+0.0937

–0.0937

0.32

0.32