|
|
![]() |
|
|
|

Rule of summation: F11 + F12 + F13 = 1
Surface 1 is perfectly flat F11 = 0
By symmetry F12 = F13
\ F12 = 0.5
Rule of reciprocity: A1F12 = A2F21
Surfaces are of length "L" perpendicular to page:
(b) Assume that no radiation escapes from the ends of the enclosure. All radiation from 1 goes to 2, as 1 is flat and 2 is the only available destination for it. Surfaces are of length "L" perpendicular to page:

Surface 1 is perfectly flat F11 = 0
\ F12 = 1
Rule of reciprocity:

Rule of reciprocity: A1F12 = A2F21
Rule of summation: F31 + F32 + F33
= 1
Bottom is perfectly flat F31 = F33 = 0
\ F32 = 1.0
Rule of reciprocity: A3F32 = A2F23

Rule of reciprocity:

where, remembering that the graph can give figures for F12,
F1a2, F12a, F1a2a
A1 = A1a + A1b = 2A1a
A1F12b = A1aF1a2b + A1bF1b2b
A1aF1a2 = A1aF1a2a + A1aF1a2b
Substituting back into first expression
2A1aF12 = 2A1aF12a + (A1aF1a2
- A1aF1a2a)+ A1bF1b2b
F1b2b = 2F12 - 2F12a + F1a2a
- F1a2
®
from formula, F12a = 0.101543970
®
from formula, F1a2 = 0.213712346
®
from formula, F1a2a = 0.179622642
F1b2b = 2(0.132581156) - 2(0.101543970) + 0.179622642 -
0.213712346 = 0.027984668
By reciprocity, the other view factor can be found:

where, remembering that the formulae can give figures for F12,
F1a2, F12a, F1a2a
A1 = A1a + A1b
A1F12b = A1aF1a2b + A1bF1b2b
A1aF1a2 = A1aF1a2a + A1aF1a2b
Substituting back into first expression
A1F12 = A1F12a + A1a(F1a2
- F1a2a) + (A1 - A1a)F1b2b
(A1 - A1a)F1b2b = A1F12
- A1F12a - A1a(F1a2 - F1a2a)
For large discs (1 and 2):
For small discs (1a and 2a):
® A1a = p
´ 0.12 = 0.01p
m2
® A1 = p
´ 0.22 = 0.04p
m2