The Label is the default physics interface name.
The Name is used primarily as a scope prefix for variables defined by the physics interface. Refer to such physics interface variables in expressions using the pattern
<name>.<variable_name>. In order to distinguish between variables belonging to different physics interfaces, the
name string must be unique. Only letters, numbers, and underscores (_) are permitted in the
Name field. The first character must be a letter.
The default Name (for the first physics interface in the model) is
htlsh.
By default, all boundaries are available for the application of the Heat Transfer in Shells interface. Select the Restrict to layered boundaries checkbox to make the interface applicable only if a layered material is defined on the boundary. If a layered material (
Material with
Layer thickness specified,
Single Layer Material,
Layered Material Link, or
Layered Material Stack) is available, its name is then displayed beside the boundary index (for example,
slmat1), otherwise the boundary is marked as not applicable.
By default, the Shell type is
Layered shell, and the thickness of the layered material should be set as follows, depending on the type of material:
|
•
|
In a Material node, the Layer thickness can be in the table found under the Material Contents section of the material Settings window. This automatically adds a Shell subnode under the Material node, transforming it as a layered material.
|
|
•
|
For a general Layered Material, added through a Layered Material Link or a Layered Material Stack, the Thickness is set in the Layer Definition section of the Settings window. Several layers may be defined in the table, and the Thickness should be defined for each of them. The total thickness of the layered material is the sum of all the layers thicknesses.
|
Note that the Layered shell option should be used whenever a layered material is applied on the boundaries, because the thickness is part of the material settings.
In the Solid,
Fluid, and
Porous Medium nodes, the same layered material is used, and this choice is not editable. And both the
Thermally thin approximation and
General options are available as
Layer type in these nodes.
Clear the Use all layers checkbox to apply the Heat Transfer in Shells interface on some layers only. Select a
Layered material from the list (the interface is then applicable only on the boundaries where this latter material is defined), and clear the checkboxes corresponding to layers where the interface should not be applied in the
Selection table.
If the Restrict to layered boundaries checkbox is not selected in the
Boundary Selection section, a nonlayered material may be defined on the selected boundaries, and the
Thickness Lth can be set as a user defined value or expression. This value overrides the values set in the material nodes.
In the Solid,
Fluid, and
Porous Medium nodes, the
Thickness is set by default to
From physics interface, and is editable only in a manually added node. Only the
Thermally thin approximation option is available as
Layer type in these nodes.
|
|
|
•
|
The layer thickness variable, htlsh.ds, used in the weak equations, is the product of the thickness set in the Shell Properties section, htlsh.lth, and the scale factor htlsh.lsc, which is equal to 1 by default, and can be overridden by a user defined value in a single layer material.
|
|
|
|
When the Heat Transfer in Shells interface is coupled to a Surface-to-Surface Radiation interface through a Heat Transfer with Surface-to-Surface Radiation multiphysics coupling, these inputs are automatically defined from the multiphysics coupling. These variables are set to unit length of the component unit system. This corresponds to the assumption that the geometry is infinite in the out-of-plane direction and that the equations are defined per unit length. This assumption is required as it corresponds to the view factor computation in these dimensions.
|
Set the Reference temperature Tref. It is used in the definition of the reference enthalpy
Href which is set to 0 J/kg at
pref (1 atm) and
Tref. The corresponding interface variable is
htlsh.Tref.
This section is available by clicking the Show More Options button (

) and selecting
Stabilization in the
Show More Options dialog.
The Streamline diffusion checkbox is selected by default and should remain selected for optimal performance for heat transfer in fluids or other applications that include a convective or translational term.
Crosswind diffusion provides extra diffusion in regions with sharp gradients. The added diffusion is orthogonal to the streamlines, so streamline diffusion and crosswind diffusion can be used simultaneously. The
Crosswind diffusion checkbox is also selected by default and is only available when the
Streamline diffusion checkbox is selected.
The Use dynamic subgrid time scale checkbox is selected by default. When selected, it estimates the influence of temporal variations in the temperature field instead of using the solver time step as a time scale in the consistent stabilization terms.
This section is available by clicking the Show More Options button (

) and selecting
Stabilization in the
Show More Options dialog.
The Isotropic diffusion option (not selected by default) adds an additional term to the diffusion coefficient to dampen spurious oscillations caused by convective terms. Increasing the
Tuning parameter δid amplifies the effect of the isotropic diffusion. As a rule of thumb, the tuning parameter should be large enough to ensure convergence, while remaining as small as possible as it reduces the accuracy of the original problem.
To display all settings available in this section, click the Show More Options button (

) and select
Advanced Physics Options in the
Show More Options dialog. You can choose the type and order of the shape functions used for the variables solved by the Heat Transfer in Shells interfaces.
For the temperature, you can choose not only the order of the discretization, but also the type of shape functions: Lagrange or
serendipity. For highly distorted elements, Lagrange shape functions provide better accuracy than serendipity shape functions of the same order. The serendipity shape functions will however give significant reductions of the model size for a given mesh containing hexahedral, prism, or quadrilateral elements.
The shape functions used for the temperature are Quadratic Lagrange for the modeling of heat transfer in shells, and
Linear for the modeling of heat transfer in films and heat transfer in fractures.
The Heat Transfer in Shells interfaces have the dependent variable Temperature T. The dependent variable names can be changed. Editing the name of a scalar dependent variable changes both its field name and the dependent variable name. If a new field name coincides with the name of another field of the same type, the fields share degrees of freedom and dependent variable names. A new field name must not coincide with the name of a field of another type or with a component name belonging to some other field.