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CFD-ACE+ has a unique Boundary Condition feature
called "Thin Walls". This feature can be used to
model very thin entities such as baffles, plates, and
thermal resistances. Since the entity is very thin,
you can actually ignore the volume it displaces, but
not from a momentum, heat transfer, and/or scalar
transport standpoint. For the flow field, a thin-wall
acts simply as a wall boundary, i.e it
appears as a blockage to flow. In simulations where
the users want to assign an internal BC as Wall, you
can assign it as a Thin Wall. For the thermal
field, it may be used to model:
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Contact resistance, which is brought about
by poor contact at a material interface
(solid-solid, or fluid-solid interface)
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Lead, which is a thin layer of metal with
much higher values of conductivity than the
materials on either side of it. For the scalar
field, it is used to model only the contact
resistance.
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Thermal resistance, where two conductive
metals are connected to each other by a layer of
material with low thermal conductivity (e.g. a
ceramic)
In addition to the above applications, the Thin Wall
boundary condition also provides for high fidelity
contact resistance calculation through the thermal
gap model. The thermal gap model is used
to calculate the heat transfer between solid bodies
separated by a gap. The thermal gap model
accounts for a) the gaseous conduction within the
gap, b) the effects of direct-contact conduction
(solid-solid conduction), and c) radiation heat
transfer across the gap. Applications of the thin
wall boundary condition are often found in the
semi-conductor and the electronics / thermal
packaging industries.
Activating Thin Wall's in
CFD-ACE-GUI
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Go to the BC tab and change the Boundary Condition
Setting Mode to Thin-Wall.

Figure 1. Change the BC Setting Mode to Thin
Wall
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Pick a domain-domain interface boundary condition
from either the Viewer Window or the BC Explorer.
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Press the Set button to convert the Interface to a
Thin-Wall boundary condition. (Press the Unset
button to revert the boundary condition back to an
Interface.)

Figure 2. Use 'Set' and 'Unset' to create the
Thin Walls
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Once you have hit the 'Set' button, you may enter
the thickness of the material and the thermal
conductivity to use for the material.
Thermal Resistance Modeling in
CFD-ACE+
This user tip will demonstrate how thin walls can be
used to study the effect of a thermally resistive
material, which connects two thermally conductive
metal solids, without having to grid the thermal
resistance layer. Two Cases are studied, one with the
thermal resistance layer as a separate volume and one
with the Thin Wall BC, to compare the resulting
temperature field.
Case 1: Heat Transfer Between Two Solids
Using a Thermal Resistance Layer

Figure 3. Thermal resistance layer is a separate
volume
Case 2: Heat Transfer Between Two Solids
Using Thin Wall BC's to Model the Thermal Resistance
Layer

Figure 4. The thermal resistance layer is not a
separate volume, but is represented as a 'Thin Wall'
The Thin Wall BC has two inputs, the thickness of the
layer and its thermal conductivity. This is used to
calculate the effective thermal conductivity with the
assumption that the heat flux across the thin wall is
continuous. To read more on how the effective thermal
conductivity is calculated, please refer to the
theory section of the Thin Walls Chapter.
For this case, the thickness of the thermal
resistance layer is 0.00254m (0.1") The thermal
conductivity is set to the value of the thermal
resistance layer, which is 10W/m-K is this case.
Metal Solid 1 and Solid2 are given the properties of
1020 Stainless Steel.

Figure 5. Inputs required for the Thin Wall option
Results
Case 1 and Case 2 are solved using the Heat Transfer
module in CFD-ACE+. Figure 6 (a) and (b) shows a plot
of the temperature fields for Case 1 and Case 2
respectively. In Figure 6 (b), you can see that there
is a temperature jump across the Thin Wall. Figure 7
(a) and (b) shows the temperature field in Metal
Solid 2 for Case 1 and Case 2. It can be seen that
the temperature values match well between the two
cases, which indicates that Thin Wall BC's can be
used effectively to model thermal resistance layers
without the need to grid the layer.
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Figure 6. (a) Temperature profile using the Thin
Wall option (b) Temperature profile using the
thermal resistance layer
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Figure 7. (a) Temperature profile using the Thin
Wall option (b) Temperature profile using the
thermal resistance layer
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Caveats with Thin Walls:
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A Thin Wall can only be assigned at a
Domain-Domain interface, which must be taken
into account during the grid generation
process.
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Thin Wall's cannot be used with parallel
processing.
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The domains on each side of the Thin Wall
must be more than one cell thick.
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The Thin Wall feature is not compatible with
the following modules/features:
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Magnetic Module
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Electroplating Feature
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Electrochemistry
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If you would like to have the files used in this tip,
please click
here to download them. Once you download the files, you can
look in the Heat Transfer Summary located in the output file
and verify that the heat flux is the same for both Case 1 and
Case 2, 1.7419E+04W/m, across the "Thermal Resistance" (whether it
be a Thin Wall or separate volume).
If you have any questions about this feature or would
like us to discuss some other topic in the future,
please let us know.
Amit Saxena
Applications Engineer
ESI CFD Customer Support
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