Orthotropic Conductivity 2D¶
Bases: IsotropicConductivity2D
Orthotropic heat conductivity material in 2D.
Parameters:
-
kappa_1(Tensor | float) –Conductivity along local axis 1.
-
kappa_2(Tensor | float) –Conductivity along local axis 2.
-
rho(Tensor | float, default:1.0) –Mass density. Default is
1.0.
Notes
- No internal state variables (
n_state = 0). - Supports batched/vectorized material parameters.
- Supports rotation of the material coordinate system via
rotate().
Orthotropic plane conductivity tensor
The two principal in-plane conductivities are aligned with the material
axes, so the conductivity tensor is diagonal in the material frame
$$
\pmb{\kappa} =
\begin{bmatrix}
\kappa_1 & 0 \cr
0 & \kappa_2
\end{bmatrix}
= \sum_{i=1}^{2} \kappa_i \, \mathbf{e}_i \otimes \mathbf{e}_i
$$
with the material axes \(\mathbf{e}_i\). rotate() maps it into the global
frame as \(\kappa_{ij} \mapsto R_{ik} R_{jl} \kappa_{kl}\).
vectorize(n_elem)
¶
Returns the material batched over n_elem elements.
Parameters:
-
n_elem(int) –Number of elements to vectorize the material for.
Returns:
-
Material(T) –A material of the same type carrying one entry per element, or itself if it is vectorized already.
step(grad_inc, grad, flux, state, cl, iter)
¶
Performs an incremental step in the isotropic heat conduction model.
Fourier's law, \(\Delta \mathbf{q} = -\pmb{\kappa} \cdot \Delta \nabla T\), with a constant conductivity.
Parameters:
-
grad_inc(Tensor) –Incremental temperature gradient. Shape:
(..., 1, 3), where...represents batch dimensions. -
grad(Tensor) –Current temperature gradient. Unused. Shape:
(..., 1, 3), same asgrad_inc. -
flux(Tensor) –Current heat flux. Shape:
(..., 1, 3). -
state(Tensor) –Internal state variables (unused in heat conductivity). Shape: Arbitrary, remains unchanged.
-
cl(Tensor) –Characteristic lengths. Shape:
(...). -
iter(int) –Current iteration number.
Returns:
-
flux_new(Tensor) –Updated heat flux. Shape:
(..., 1, 3). -
state_new(Tensor) –Updated internal state (unchanged). Shape: same as
state. -
dqdg(Tensor) –Algorithmic tangent conductivity. Shape:
(..., 3, 3).
rotate(R)
¶
Returns a copy with its conductivity tensor rotated by R.