TC nonlinear orthotropic¶
Module: solid
Category: material
Type string: "TC nonlinear orthotropic"
Parameters¶
| Name | Description | Default | Units |
|---|---|---|---|
density |
density | 1 | [M/L^3] |
k |
bulk modulus | 0 | [P] |
pressure_model |
pressure_model | 0 | [] |
c1 |
c1 | 0 | [] |
c2 |
c2 | 0 | [] |
beta |
beta | [] | |
ksi |
ksi | [] | |
mat_axis |
[] |
Description¶
The material type for the tension-compression nonlinear orthotropic material is TC nonlinear orthotropic.
This material is based on the following uncoupled hyperelastic strain energy function 1:
The isotropic strain energy \(\tilde{\Psi}_{iso}\) and the dilatational energy \(U\) are the same as for the Mooney-Rivlin material. The tension-compression term is defined as follows:
The \(\tilde{\lambda}_{i}\) parameters are the deviatoric fiber stretches of the local material fibers:
The local material fibers are defined (in the reference frame) as an orthonormal set of vectors \(\mathbf{a}_{i}^{0}\). As with all uncoupled materials, this material uses the three-field element formulation.
A complete example for this material follows.
<material id="7" name="cartilage" type="TC nonlinear orthotropic">
<c1>1.0</c1>
<c2>0.0</c2>
<k>100</k>
<beta>4.3,4.3,4.3</beta>
<ksi>4525, 4525, 4525</ksi>
<mat_axis type="local">0,0,0</mat_axis>
</material>
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Ateshian, Gerard A, Ellis, Benjamin J, and Weiss, Jeffrey A, "Equivalence between short-time biphasic and incompressible elastic material responses", J Biomech Eng 129, 3 (2007), pp. 405-12. ↩