Yeoh
Regularized Yeoh Material For Compressible Rubbers
The following strain energy density is used.
\[
W=\sum_{i=1}^nC_{i0}(J_1-3)^i+\sum_{i=1}^nC_{i1}(J_3-1)^{2i}.
\]
where \(C_{i0}\) and \(C_{i1}\) are material constants. \(J_1\) and \(J_3\) are reduced invariants of the right Cauchy-Green deformation tensor.
Syntax
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Remarks
- The above command takes input list of arbitrary length (\(\ge2\), excluding tag).
- If the number of double inputs is odd, the last one is interpreted as density.
- If the number of double inputs is even, the density is assumed to be zero.
- The first half of double inputs is read as \(C_{i0}\) and the second half \(C_{i1}\).
Examples
For \(i=1\), let \(C_{10}=20\) and \(C_{11}=4000\), the strain energy density is
\[
W=20(J_1-3)+4000(J_3-1)^2.
\]
The following command shall be used.
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If density is nonzero, say for example \(\rho=10^{-4}\), then the following command shall be used.
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For \(i=3\), let \(C_{10}=20\), \(C_{20}=30\), \(C_{30}=40\), \(C_{11}=2000\),\(C_{21}=3000\) and \(C_{31}=4000\), the strain energy density is
\[
W=20(J_1-3)+30(J_1-3)^2+40(J_1-3)^3+2000(J_3-1)^2+3000(J_3-1)^4+4000(J_3-1)^6.
\]
The following command shall be used.
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