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HEAT TRANSFER: solutions to radiation tutorial problems (view factors)

  • (a) Add an imaginary third surface to complete the (isosceles) triangle and assume that no radiation escapes from the ends of the enclosure:
  • 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:

    Rule of summation: F11 + F12 = 1

    Surface 1 is perfectly flat F11 = 0
    \ F12 = 1

    Rule of reciprocity:


  • Let the disc be surface 1, the inside top and sides of the box be 2 and the remainder of the bottom inner surface 3.
  • Rule of summation: F11 + F12 + F13 = 1
    Bottom is perfectly flat F11 = F13 = 0
    \ F12 = 1.0

    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


  • Use the charts for view factors between two surfaces at right angles:

  • ® from formula in module pack, F12 = 0.132581156

    Rule of reciprocity:

    Here, we need to find F1b2b
    A1F12 = A1F12a + A1F12b

    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:


  • Use the formulae for view factors between two parallel discs, and treat cut-out areas as discs themselves:
  • Here, we need to find F1b2b
    A1F12 = A1F12a + A1F12b

    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