All property dialogs for Thermal entities have only one tab to define their properties as shown in the table below.
Figure 15.8: Thermal Entities property dialogs
Type | Parameters | Connector | Special |
Temperature | O | X | X |
Heat Flow | O | X | X |
Heat Flux | O | X | X |
Heat Generation | O | X | X |
Convection | O | X | X |
Thermal Contact | O | X | X |
The parameters in the property dialog are used to calculate a magnitude of each heat source or loss. The formulation and modification pages of each thermal entity show the usage and definition of each parameter. All thermal entities can be defined by using a function expression or user subroutine as shown in the table below.
Note: In extreme cases, such as with rapid temperature changes or large thermal strains, convergence issues may arise. During the Newton-Raphson (NR) process, the thermal-mechanical coupling is not fully bidirectional. Specifically, temperature changes affect deformation, but deformation does not affect temperature within an iteration. This sequential update of thermal and mechanical responses may lead to convergence issues, particularly under extreme conditions. For example, when thermal entities are related to state variables such as position, velocity, acceleration, force, variable, and differential equation, significant temperature changes can occur. If these large temperature changes result in significant volume changes, integration and NR failures will occur. To mitigate such failures, you should reduce the error tolerance for the NR convergence or the step size.
Figure 15.9: Main parameters of thermal entities
Type | Main parameters | |||
Prescribed method | Spline | Function expression | User subroutine | |
Temperature | X | X | O | O |
Heat Flow | X | X | O | O |
Heat Flux | X | X | O | O |
Heat Generation | X | X | O | O |
Convection | X | X | O | O |
Thermal Contact | X | X | O | O |