tendon material¶
Module: solid
Category: material
Type string: "tendon material"
Parameters¶
| Name | Description | Default | Units |
|---|---|---|---|
density |
density | 1 | [M/L^3] |
k |
bulk modulus | 0 | [P] |
pressure_model |
pressure_model | 0 | [] |
g1 |
g1 | 0 | [P] |
g2 |
g2 | 0 | [P] |
l1 |
l1 | 0 | [P] |
l2 |
l2 | 0 | [] |
lam_max |
lam_max | 0 | [] |
fiber |
[] |
Description¶
The material type for the tendon material is tendon material. The tendon material is similar to the muscle material 1 (also see muscle material). The only difference is the fiber function. For tendon material this is defined as:
\[
\lambda\frac{\partial F_{t}}{\partial\lambda}=\sigma\left(\lambda\right),
\]
where
\[
\sigma\left(\lambda\right)=\begin{cases}
0 & \lambda\leqslant1\\
L_{1}\left(e^{L_{2}\left(\lambda-1\right)}-1\right) & 1<\lambda<\lambda^{\ast}\\
L_{3}\lambda+L_{4} & \lambda\geqslant\lambda^{\ast}
\end{cases}\,.
\]
The parameters \(L_{3}\) and \(L_{4}\) are determined by requiring \(C^{0}\) and \(C^{1}\) continuity at \(\lambda^{\ast}\).
The tendon fiber direction is specified similarly to the transversely isotropic Mooney-Rivlin model.
Example:
<material id="1" type="tendon material">
<g1>5e4</g1>
<g2>5e4</g2>
<l1>2.7e6/l1>
<l2>46.4</l2>
<lambda>1.03</lambda>
<k>1e7</k>
<fiber type="vector">1,0,0</fiber>
</material>
-
Blemker, SS, 3D Modeling of Complex Muscle Architecture and Geometry (2004). ↩