Solid Temperature Model¶
Introduction¶
The solid temperature model describes how temperature changes in a solid. It uses thermal conduction with internal heat sources. It also supports heat exchange at the solid boundaries through convection and radiation. The governing transient heat equation is $$ \begin{align} \rho c_p \frac{\partial T}{\partial t} - \nabla \cdot (\kappa \nabla T) = Q. \end{align} $$
- \(T\) - temperature [K]
- \(\rho\) - material density [kg/m\(^3\)]
- \(c_p\) - specific heat capacity [J/(kg K)]
- \(\kappa\) - thermal conductivity [W/(m K)]
- \(Q\) - volumetric heat power density [W/m\(^3\)]
You typically use the model for:
- Thermal-management studies in electric machines and transformers.
- Induction-heating workpieces.
- Electronics cooling.
- Welding and casting simulations.
- Any solid-conduction problem with convective, radiative, or prescribed-flux boundaries.
Model¶
You create the model and add it to the simulation with
solid_thermal_model = SolidTemperatureModel(
marker=["Plate"] @ Vol,
order=1,
)
sim.get_model_manager().add_model(solid_thermal_model)
where
- marker specifies the domain on which the model is solved
- order is the polynomial order of the discretization
Materials¶
In general, the material parameters \(\rho\), \(c_p\), and \(\kappa\) in the governing equation can vary in space. They can also be direction-dependent or depend on other physical quantities. You can define these dependencies with material functions. You give them as analytical expressions, tabulated data, or numerical models. Details are provided in Solid Temperature Material.
![]() Example of a silicon plate. |
Silicon The silicon plate has the following properties: $$ \begin{alignat*}{2} \kappa &= 111 \quad &\left[ \mathrm{W} / (\mathrm{m} \cdot \mathrm{K}) \right] \\ c_p &= 668 &\left[ \mathrm{J} / (\mathrm{kg} \cdot \mathrm{K}) \right] \\ \rho &= 2330 &\left[ \mathrm{kg} / \mathrm{m}^3 \right] \end{alignat*} $$ We can create the material using:
|
After you create the materials, add them to the model:
Conditions¶
| Name | Supported Entities | Description |
|---|---|---|
| Adiabatic | Boundary | Enforces zero normal heat flux (perfect thermal insulation, no heat transfer). |
| Convection | Boundary | Models heat exchange with a surrounding fluid using Newton’s cooling law. |
| Heat Flux | Boundary | Prescribes the normal heat flux across the boundary (including zero-flux case). |
| Radiation | Boundary | Models radiative heat transfer between the surface and its surroundings. |
| Temperature | Volume, Boundary | Prescribes a fixed temperature within a volume or on a boundary (Dirichlet condition). |
| Volumetric Heat Source | Volume | Defines internal heat generation within the material domain. |
| Mushy Zone | Volume | Linear latent-heat storage term over a solidus / liquidus temperature range — phase-change problems (casting, welding, thermal storage). |
| Matching Interface | Boundary pair | Stitches the temperature DOFs of two geometrically coincident boundaries on separately-meshed bodies, giving a continuous temperature across the interface. |
Coefficients¶
The following functions are available in the solid temperature model for visualization or querying:
| Name | Field Type | Description |
|---|---|---|
| Temperature | Scalar | Temperature: $T$ [K] |
| Density | Scalar | Material density: $\rho$ [kg/m$^3$] |
| Specific Heat Capacity | Scalar | Specific heat capacity: $c_p$ [J/(kg K)] |
| Thermal Conductivity | Scalar | Thermal conductivity: $\kappa$ [W/(m K)] |
Solver¶
The model exposes a solver instance that configures convergence and damping.
You get and configure the solver with
See Solver for more details.
