One way coupling of hydrostatic stress and effective plastic strain on a kernel #31400
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Hello
Hydrostatic stress, coming from solid mechanics? If so it's likely a material property (not a coupled variable, displacements are the variables), likely a tensor.
That's for postprocessing right?
That kernel being fairly complicated, I think the way forward is to examine the related kernels in solid mechanics |
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Hydrogen.Embrittlement.2.pdf To output hydrostatic stress, I guess we can maybe use the stress tensor, compute its trace and divide it by 3. I am having trouble computing the gradient of hydrostatic stress for the kernel. |
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I want to implement the kernel for the weak form given below,
$-\int_\Omega \nabla \phi . \left( \frac{D \bar{V_H}}{R T} C_L \nabla \sigma_H \right) d\Omega$ $N_T$ as given below,
$N_T = 10^{(23.6 - 2.33 \exp{(- 5.5 \epsilon^P)})}$ $\nabla \sigma_H$ (Gradient of Hydrostatic stress) and $\epsilon^P$ (Effective plastic strain) are to be passed using one way coupling from solid mechanics. Also $C_L$ is the degree of freedom.
with material model for calculating
Where,
Can somebody help me to find information about how to compute gradient of hydrostatic stress as a coupled variable?
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