Assume diffuse, grey surfaces with uniform radiosity.
The heat transferred by radiation from surface1 to surface 2 is:
q12=sigma*(T1^4-T2^4)/((1-e1)/e1/A1+1/A1/F12+(1-e2)/e2/A2)
Question 1.
Surface 1 is the bottom surface of a finite rectangular area sitting above (and parallel to) an infinite plane (surface 2). The view factor, F12, is
1.0 in this case. The problem I see here is that A2 is infinite. This doesn't cause any real mathematical problems in the equation above, but it does seem to mean that the emissivity of the infinite plane is no longer relevant--it is as if the infinite plane has emissivity of 1.0, regardless of its actual emissivity. This doesn't "feel" right to me. Does it make sense? Does having infinite space to absorb heat mean that all heat will be absorbed, even when the emissivity is less than 1.0?Question 2.
There are two rectangular areas in parallel planes. The directions of the rectangles are aligned with each other. One rectangle is not necessarily directly above the other. Is there a general expression for the view factor between the two rectangles? I cannot make any simplifying assumptions. (i.e. I cannot say that one area is very small; I cannot say that the vertical spacing is very large or very small relative to anything, etc.) I know there is a simple solution if the two areas are very small relative to the distance between them. I have also found (in
Thanks,
-Paul