Radiation Heat Transfer between Surfaces
rate of radiation heat transfer between two surfaces in this case is expressed as
)( 4
2
4
1121TTFAQ
where A1 is the
surface area, F12 is the view factor, and T1 and T2 are the temperatures of two surfaces.
radiation energy as well as reflected energy. Radiosity and emitted energy are equal for blackbodies since a blackbody does
not reflect any radiation.
radiation. It is zero for black surfaces. The space resistance is the radiation resistance between two surfaces and is expressed
as
back sides of these surfaces are well insulated and net heat transfer through these surfaces is zero. When the convection
effects on the front (heat transfer) side of such a surface is negligible and steady-state conditions are reached, the surface
must lose as much radiation energy as it receives. Such a surface is called reradiating surface. In radiation analysis, the
surface resistance of a reradiating surface is taken to be zero since there is no heat transfer through it.
and 21-35 give N linear algebraic equations for the determination of the N unknown radiosities for an N -surface enclosure.
Once the radiosities are available, the unknown surface temperatures and heat transfer rates can be determined from these
equations respectively. This method involves the use of matrices especially when there are a large number of surfaces.
Therefore this method requires some knowledge of linear algebra.
The network method involves drawing a surface resistance associated with each surface of an enclosure and
connecting them with space resistances. Then the radiation problem is solved by treating it as an electrical network problem
where the radiation heat transfer replaces the current and the radiosity replaces the potential. The network method is not
practical for enclosures with more than three or four surfaces due to the increased complexity of the network.