This node defines a boundary semitransparent to radiation. If no radiation is transmitted through the surface, use the
Opaque Surface (Radiation in Participating Media and Radiation in Absorbing-Scattering Media Interfaces) node instead.
When the Radiation discretization method is
Discrete ordinates method, the net radiative heat flux is defined as the difference between the incoming and outgoing radiative heat fluxes, and the incoming and outgoing radiative heat fluxes are defined from the weighted sums of the incident intensities. See
Semitransparent Surface for more details.
When the Radiation discretization method is
P1 approximation, the net radiative heat flux is defined from the incident radiation
G. See
Semitransparent Surface for more details.
At the internal boundaries, the net radiative heat fluxes, qr,net,d and
qr,net,u on each side of the surface are defined. Specific radiative properties of the surface can be defined on each side of the boundary.
If this node is selected from the Pairs menu, choose the pair to apply this condition to. A pair must be created first. See
Identity and Contact Pairs in the
COMSOL Multiphysics Reference Manual for more details.
There is one standard model input — the Temperature T, which is used in the expression of the blackbody radiative intensity.
This section is available when the Wavelength dependence of radiative properties is defined as
Solar and ambient or
Multiple spectral bands in the Radiation in Participating Media interface (see
Participating Media Settings).
When the Fractional emissive power is
Blackbody/Graybody, the fractional emissive power
FEPk is automatically calculated for each spectral band as a function of the band endpoints and temperature.
When the Fractional emissive power is
User defined for each band, define the
Fractional emissive power,
FEPk for each spectral band in the table displayed below. All fractional emissive powers are expected to be in [0,1] and their sum must equal 1. Select the
Define fractional emissive power on each side check box to set specific
Upside and
Downside values in the table.
If the Wavelength dependence of radiative properties is
Constant:
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By default, the Emissivity ε (dimensionless), Diffuse transmissivity τd (dimensionless), and Specular transmissivity τs (dimensionless) use values From material. These are properties of the material surface that depend both on the material itself and the structure of the surface. Make sure a material is defined at the boundary level (by default materials are defined at the domain level).
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For User defined, set values or expressions. You can define temperature-dependent emissivity and transmissivities using the variable rad.T.
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Select the Define properties on each side check box to set specific values for each side. Select the
Boundary material, upside and
Boundary material, downside to have different material properties on each side. The boundary material specified is used only when
Emissivity, upside,
Emissivity, downside,
Diffuse transmissivity, upside,
Diffuse transmissivity, downside,
Specular transmissivity, upside, and
Specular transmissivity, downside are
From material.
If the Wavelength dependence of radiative properties is
Solar and ambient or
Multiple spectral bands:
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By default, Emissivity ε (dimensionless), Diffuse transmissivity τd (dimensionless), and Specular transmissivity τs (dimensionless) use values From material.
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When Emissivity is User defined, enter a value or expression for the Emissivity ε. The wavelength is accessible through the rad.lambda variable. Any expression set for the emissivity is then averaged on each spectral band to obtain a piecewise constant emissivity. If the average value of the emissivity on each band is known, you can use instead the User defined for each band option to avoid the evaluation of the average.
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When Diffuse transmissivity is User defined, enter a value or expression for the Diffuse transmissivity τd. The wavelength is accessible through the rad.lambda variable. Any expression set for the transmissivity is then averaged on each spectral band to obtain a piecewise constant transmissivity. If the average value of the transmissivity on each band is known, you can use instead the User defined for each band option to avoid the evaluation of the average.
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When Specular transmissivity is User defined, enter a value or expression for the Specular transmissivity τs. The wavelength is accessible through the rad.lambda variable. Any expression set for the specular transmissivity is then averaged on each spectral band to obtain a piecewise constant specular transmissivity. If the average value of the specular transmissivity on each band is known, you can use instead the User defined for each band option to avoid the evaluation of the average.
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When Emissivity is User defined for each band, enter a value for the Emissivity for each spectral band. Within a spectral band, each value is assumed to be independent of wavelength. By default, the same emissivity is defined on both sides. Select the Define properties on each side check box and fill the Upside and Downside columns of the table for a specific definition on each side.
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When Diffuse transmissivity is User defined for each band, enter a value for the Diffuse transmissivity for each spectral band. Within a spectral band, each value is assumed to be independent of wavelength. By default, the same transmissivity is defined on both sides. Select the Define properties on each side check box and fill the Upside and Downside columns of the table for a specific definition on each side.
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When Specular transmissivity is User defined for each band, enter a value for the Specular transmissivity for each spectral band. Within a spectral band, each value is assumed to be independent of wavelength. By default, the same transmissivity is defined on both sides. Select the Define properties on each side check box and fill the Upside and Downside columns of the table for a specific definition on each side.
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Set the surface emissivity to a number between
0 and
1, where
0 represents a diffuse mirror and
1 is suitable for a perfect blackbody. The appropriate value for a physical material is somewhere in between and can be found in tables or measurements.
Set the surface diffuse transmissivity to a number between
0 and
1, where
0 applies to an opaque surface and
1 is appropriate for a fully transparent surface.
Set the surface specular transmissivity to a number between
0 and
1, where
0 applies to a perfect diffuse surface and
1 is appropriate when transmissivity is only specular.
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The Specular transmissivity is only needed when Discrete ordinates method is selected.
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When the Wavelength dependence of radiative properties is set to
Constant, two options are available to define the external radiation intensity. Set
External radiation intensity to
User defined to define
Iext (SI unit: W/m
²/sr) directly. Alternatively, select
Blackbody radiation to define
Iext as
Ib(Text) and set the
External temperature Text (SI unit: K, default value 293.15 K) or select an
Ambient temperature to specify the temperature at which the blackbody radiation intensity
Ib is evaluated.
When the Wavelength dependence of radiative properties is set to
Solar and ambient or to
Multiple spectral bands, the external radiation intensity,
Iext,k is defined for each spectral band.
Set External radiation intensity to
Blackbody radiation and set the
External temperature Text (SI unit: K, default value 293.15 K) or select an
Ambient temperature to define
Iext,k from the blackbody intensity
Ib(Text), the
External temperature Text, and the fractional emissive power for each spectral band at external temperature
FEPk(Text).
Set the External radiation intensity to
User defined for each band, to define
Iext,k from user defined expression for each spectral band in the table displayed underneath.
Set the External radiation intensity to
User defined distribution, and define an expression for
Iλ,ext(SI unit: W/m
3/sr) to define
Iext,k from a spectral distribution. In this case
Iext,k is automatically computed per spectral band as the integral of the distribution over each spectral band. If this integral over each band is known, you can use instead the
User defined for each band option to avoid the numerical overhead due to the evaluation of the average.
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When Discrete ordinates method is selected, the components of each discrete ordinate vector can be used in this expression. The syntax is name.sx, name.sy, and name.sz, where name is the name of the physics interface node. By default, the Radiation in Participating Media interface is rpm so rpm.sx, rpm.sy, and rpm.sz correspond to the components of discrete ordinate vectors.
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Physics tab with Radiation in Participating Media or
Radiation in Absorbing-Scattering Media selected: