Modeling Ohmic Heating
Simcenter STAR-CCM+ allows you to calculate the heat that is generated by electric currents flowing in resistive materials. You can use the Ohmic Heating model in combination with an energy model.
- Prepare the electromagnetic analysis following the guidelines outlined in the previous sections, Modeling Electric Currents and Modeling Magnetic Fields. In the physics continua associated with electrically conducting regions, activate the required potential models.
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Complete the electromagnetic analysis set up, by specifying appropriate boundary, interface, and region settings. For guidelines, see
Modeling Electric Currents and
Modeling Magnetic Fields.
If you define an electric resistance at a boundary or interface, Simcenter STAR-CCM+ also accounts for the energy dissipation due to the specified resistance (see Eqn. (4360)).
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Optionally, you can activate an energy model and specify settings for thermal
analysis. All energy models, including the Finite Element Solid
Energy model for solids, are compatible with the
Ohmic Heating model.
When the continuum contains an energy model, Simcenter STAR-CCM+ accounts for the heat source calculated by the Ohmic Heating model in the energy equation. In thermal analyses of electrically conducting materials, you generally account for Ohmic heating when the Ohmic heat source is significant compared to all other source terms in the energy equation. For more information, see Joule Heating.
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Activate the
Ohmic Heating model in the physics continua that are assigned to the electrically conducting regions.
For more information on the model dependencies and associated field functions, see Ohmic Heating Model Reference.
- To model Ohmic heating in porous media, follow the additional steps in Modeling Ohmic Heating in Porous Media.
- In all physics continua that use the Ohmic Heating model, expand the relevant node.
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Select the
Electrical Conductivity node and specify the electrical conductivity of the material using an appropriate method.
In thermal analyses, the electrical conductivity of a material is generally a function of temperature and, therefore, it has a high impact on the accuracy of the heat calculation. When the temperature change is relatively small, you can neglect the dependency of the material electrical conductivity on temperature. When the temperature change is significant, define the electrical conductivity as a function of temperature using one of the following methods:
Option Steps To define as a polynomial function of temperature - Select Polynomial in T.
- Define the polynomial function using the Using Polynomial in T. node. See
To define using a table of values - Select Table (T).
- Define the input table using the Using Table(T). node. See
To define using a user-defined function of temperature - Select Field Function.
- Under the Creating a User Field Function). node, create an appropriate temperature-dependent field function (see
- Finally, select the node and set Scalar Function to the user field function that you created.
To define an anisotropic - Select Anisotropic.
- In the relevant regions, select the Anisotropic Electrical Conductivity node and define the components of the second-order tensor as a function of temperature. See Tensor Quantities.
- Prepare the required scenes and plots for post-processing and run the simulation.
The specific Ohmic heat source (Eqn. (4357)) can be significantly large at the beginning of the solution process, causing the energy solution to diverge.
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If the energy solution is diverging during initial iterations, you can:
- Examine the critical areas where the ohmic heat source term is large, using the Specific Ohmic Heat Source field function. Evaluate whether the mesh quality can be improved in these areas.
- In the relevant physics continuum Reference Values, reduce the maximum allowable temperature. This option is not available for the Finite Element Solid Energy model.
- In thermal analyses, decouple the thermal and the electromagnetic solutions. That is, freeze the energy solver and get a converged solution for the potentials then activate the energy solver to continue with the thermal analysis.