Hyperelastic bulk active term. Stress
,
where
is the activation in
.
| Definition : |
|---|

| Call signature: |
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| dw_tl_bulk_active | (material, virtual, state) |
| Arguments : |
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Hyperelastic bulk penalty term. Stress
.
| Definition : |
|---|

| Call signature: |
|---|
| dw_tl_bulk_penalty | (material, virtual, state) |
| Arguments : |
|
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Hyperelastic bulk pressure term. Stress
.
| Definition : |
|---|

| Call signature: |
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| dw_tl_bulk_pressure | (virtual, state, state_p) |
| Arguments : |
|
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Diffusion term in the total Lagrangian formulation with
linearized deformation-dependent permeability
,
where
relates to the previous time step
and
expresses the dependence on volume compression/expansion.
| Definition : |
|---|

| Call signature: |
|---|
| dw_tl_diffusion | (material_1, material_2, virtual, state, parameter) |
| Arguments : |
|
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Base class for all hyperelastic terms in TL formulation family.
The subclasses should have the following static method attributes: - stress_function() (the stress) - tan_mod_function() (the tangent modulus)
The common (family) data are cached in the evaluate cache of state variable.
Hyperelastic Mooney-Rivlin term. Effective stress
.
| Definition : |
|---|

| Call signature: |
|---|
| dw_tl_he_mooney_rivlin | (material, virtual, state) |
| Arguments : |
|
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Hyperelastic neo-Hookean term. Effective stress
.
| Definition : |
|---|

| Call signature: |
|---|
| dw_tl_he_neohook | (material, virtual, state) |
| Arguments : |
|
|---|
Surface traction term in the total Lagrangian formulation, expressed
using
, the outward unit normal vector w.r.t. the
undeformed surface,
, the deformation gradient,
, and
a given traction,
often equal to a given pressure, i.e.
.
| Definition : |
|---|

| Call signature: |
|---|
| dw_tl_surface_traction | (material, virtual, state) |
| Arguments : |
|
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Volume term (weak form) in the total Lagrangian formulation.
| Definition : |
|---|

| Call signature: |
|---|
| dw_tl_volume | (virtual, state) |
| Arguments : |
|
|---|