3. Modeling A#
A modeling is a case of pure mechanics in 3D transverse isotropy (modeling already validated elsewhere) followed by the same in HM modeling (elastic saturated modeling).
3.1. Characteristics of modeling#
3D_SI modeling then 3D modelling_ HMS
3.2. Characteristics of the mesh#
Number of meshes: |
\(5\mathrm{\times }5\mathrm{\times }5\) type HEXA20et 150 QUAD8 |
3.3. Tested sizes and results#
We will observe the movements \(\mathit{DX}\) and \(\mathit{DZ}\) at the coordinate point \((\mathrm{1,1}\mathrm{,1})\), i.e. \(\mathit{N7}\) and the movement in \(\mathit{DY}\) at the coordinate point \((0.8\mathrm{,0}.2\mathrm{,0}.8)\) or \(\mathit{N216}\)
We check that the results in HM are the same as in pure mechanics, which is used as a reference:
Node |
Instant |
Size |
Reference |
Aster |
\(\mathit{N7}\) |
1 |
|
Pure Mechanical Modeling |
—5.98E-3 |
\(\mathit{N7}\) |
1 |
|
Pure Mechanical Modeling |
—3.569E-3 |
\(\mathit{N216}\) |
1 |
|
Pure Mechanical Modeling |
—1.965E-3 |