Thick Circular Slab Clamped along the Side Surface Subjected to a Load Uniformly Distributed over the Upper Face

Objective: Determination of the stress-strain state of a thick circular slab clamped along the side surface subjected to a load uniformly distributed over the upper face in accordance with the spatial problem of the theory of elasticity.

SCAD version used: 21.1

Initial data files:

File name

Description

4.37_4m.SPR

Design model for the slab thickness of 4 m

4.37_6m.SPR

Design model for the slab thickness of 6 m

 

Problem formulation: The thick circular slab is clamped along the side surface and subjected to a load q uniformly distributed over the upper face. Determine:

  • distribution of the radial σr and vertical σz normal stresses across the slab thickness in its center (r = 0);
  • distribution of the vertical displacements w across the slab thickness in its center (r = 0).

 

References: Solyanik-Krassa K.V. Axisymmetric Problem of the Theory of Elasticity. – M.: Stroyizdat. 1987.
p. 336.

Initial data:

E = 1.0·107 kPa - elastic modulus;
μ = 0.25 - Poisson’s ratio;
2∙a = 20.0 m - diameter of the slab;
2∙h = 4.0 m; 6.0 m - thickness of the slab;
q = 10 kPa - load uniformly distributed over the upper face.

 

Finite element model

The spacing of the finite element mesh of the slab in plan in the radial direction is 0.5 m and there are 16 layers of finite elements along the thickness (models 1х1).

Elements of the design model:

  • 4384 solid twenty-node isoparametric elements of type 37 (parallelepiped);
  • 400 solid fifteen-node isoparametric elements of type 35 (triangular prism).

Number of nodes in the design model – 20866.

The calculation was performed taking into account the symmetry planes. The constraints were imposed:

  • on the side surface in the directions of all the linear degrees of freedom;
  • on the YOZ plane – along the x axis;
  • on the XOZ plane – along the y axis.


Design models of 4.0 m and 6.0 m thick slabs

 

Results in SCAD


Values of vertical displacements w (mm) in 4.0 m and 6.0 m thick slabs

 

Comparison of solutions:

Thickness

Value

Point

Approximate theory

SCAD

Deviation (%)

4m

w(mm)

(0,0,2)

-0.0436

-0.04538

4.08

(0,0,0)

-0.0424

-0.0454

7.08

(0,0,-2)

-0.0411

-0.04364

6.18

σrθ

(kPa)

(0,0,2)

-34.51

-33.78

2.12

(0,0,0)

-1.6667

-1.5547

6.72

(0,0,-2)

31.1719

30.62

1.76

σz

(kPa)

(0,0,2)

-10

-10.16

0.16

(0,0,0)

-5

-5.07

0.14

(0,0,-2)

0

-0.05

6m

w

(0,0,3)

-0.02097

-0.02112

0.72

(0,0,0)

-0.01916

-0.01994

4.07

(0,0,-3)

-0.01722

-0.01851

7.49

σrθ

(kPa)

(0,0,3)

-18.2292

-18.51

1.54

(0,0,0)

-1.6667

-1.5149

9.12

(0,0,-3)

14.896

14.4884

2.74

σz

(kPa)

(0,0,3)

-10

-9.797

2.03

(0,0,0)

-5

-5.0569

1.14

(0,0,-3)

0

0.043

 

Note 1: The approximate analytical values were calculated according to the formulas given on pages 124-125 of “Solyanik-Krassa K.V. Axisymmetric Problem of the Theory of Elasticity. – M.: Stroyizdat. 1987.”

Note 2: The calculations were performed for meshes refined by a factor of 2 and 4 (4x4 models) to study the convergence of the method. The symmetry planes were taken into account. The maximum design model contained:

  • 280576 solid twenty-node isoparametric elements of type 37 (parallelepiped);
  • 25600 solid fifteen-node isoparametric elements of type 35 (triangular prism).

Number of nodes in the design model – 1222501.

Comparison of solutions:

Thickness

Value

Point

SCAD

Deviation (%)

4х4

1х1

4m

w(mm)

(0,0,2)

-0.04534

-0.04538

0.09

(0,0,0)

-0.0454

-0.0454

(0,0,-2)

-0.04374

-0.04364

0.23

σrθ

(kPa)

(0,0,2)

-33.6603

-33.78

0.36

(0,0,0)

-1.5683

-1.5547

0.87

(0,0,-2)

30.527

30.62

0.30

σz

(kPa)

(0,0,2)

-10.0062

-10.16

1.36

(0,0,0)

-5.0037

-5.0742

1.41

(0,0,-2)

0.00326

-0.05

6m

w

(0,0,3)

-0.02108

-0.02112

0.19

(0,0,0)

-0.01995

-0.01994

0.05

(0,0,-3)

-0.01852

-0.01851

0.05

σrθ

(kPa)

(0,0,3)

-17.373

-17.557

1.06

(0,0,0)

-1.5213

-1.5149

0.42

(0,0,-3)

14.3485

14.4884

0.98

σz

(kPa)

(0,0,3)

-10.0006

-9.797

2.03

(0,0,0)

-5.0367

-5.0694

0.65

(0,0,-3)

0.0028

0.0434