1. Reference problem#
1.1. Geometry#

Radius of sphere |
\(R=500\mathrm{mm}\) |
Imposed displacement |
\(100\mathrm{mm}\) |
1.2. Material properties#
Two different models to represent the rigid sphere:
Material stiffness: \(E=\mathrm{2,1E9}\mathrm{Mpa}\) and \(\nu =\mathrm{0,3}\)
Stiffening by kinematic conditions
Block: Steel, perfect elasto‑plastic behavior law.
Module Young |
\(E=210000\mathrm{MPa}\) |
Poisson’s Ratio |
\(\nu =\mathrm{0,3}\) |
Work hardening module |
\(\mathrm{Et}=0\) |
Elastic limit |
\({\sigma }_{y}=50\mathrm{MPa}\) |
1.3. Boundary conditions and loads#
The deformations are axisymmetric and the block forming the plane is assumed to be embedded on its base.
An imposed displacement is applied:
Loading from 0 to \(–100\mathrm{mm}\) on the upper part of the sphere in models A and D
Loading from 0 to \(–100\mathrm{mm}\) on the contact surface of the sphere in models B and C