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Mean Configuration Factor: Infinite Strips

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Publisher’s version / Version de l'éditeur:

Technical Note (National Research Council of Canada. Division of Building Research), 1962-05-01

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For the publisher’s version, please access the DOI link below./ Pour consulter la version de l’éditeur, utilisez le lien DOI ci-dessous.

https://doi.org/10.4224/20359164

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Mean Configuration Factor: Infinite Strips McGuire, J. H.

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DIVISION OF BUILDING RESEARCH

NATIONAL RESEARCH COUNCIL OF CANADA

.iJ

'Jr

E

C

JH[

N II CAlL

NOTlE

セQ

NOT FOR PUBLICATION

PREPARED BY J. H. McGuire

PREPARED FOR Record Purposes

CHECKED BY GWS

FOR INTERNAL USE

APPROyED By NBH

Rlll.. May 1962

SUBJECT MEAN CONFIGURATION FACTOR: INFINITE STRIPS

An important factor in the transfer of heat by radiation from one surface to another is the geometrical イ・ャ。エゥッョウィセー of the radiating and receiving surfaces. Its effect is discussed in tenns of the "configuration factortt which may be defined as the ratio of the radiant intensity, at a small receiving element, to the radiant intensity near the radiator. The range of values which a configuration factor can assume is thus zero to unity.

When a receiver, with finite dimensions, is being considered, the configuration factor may vary over the surface and a value of the mean configuration factor over the surface may be required. In this note, the mean configuration factor over an infinite strip receiver is evaluated,' the radiator being a second infinite strip and the axes of the two strips being parallel.

In Fig. 1, where AB and OC represent strips which are infinite in the dimension perpendicular to the plane of the drawing, the configuration factor of AB at a point D

is (1):

l(J . == セH」ッウッH + cos;/3)

(X2 - x) (x - Xl)

= +

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2

-The mean configuration factor セ over OC will be given by X 3 X3 - 1

f

1

I

(X2 - x)dx 'P =

X3

'Pdx = 2X 3

j

(X _ x) 2 .. Y

1 ..

o 0 2 " 2

Changing the variables to a

=

(X2 - x) and b

=

(x - Xl)

(X2 - X 3) (X3 -Xl) \p - -1

f

a. da 1

r

b. db

-

ja

2

+ Y 2 + 2X3

J j

セ「R

+ Y 2 X2 2 -Xl 1 = 2i 3

[j

x/ ..

Y2 2 ..

j

(X 3 - Xl) 2 .. YI 2 -

Jx/

.. y

l 2

-JX2-

X 3)2 .. Y2 2 ] 1 = 20C (OB + AC - OA - BC) •

This last expression has been referred to as the "crossed string rule." It is a very convenient geometric

method of evaluating the mean configuration factor (Fig. 2) in this particular case. It is not likely that any such simple construction will" apply for other geometrical relationships of a radiator and a receiver for which the expression for the mean configuration factor is often quite complex. Reference

1. McGuire, J. H. Heat transfer by radiation. Fire Research Special Report No.2, HMSO 1953.

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./ , IY I I I I I I I -- I 0' I I I FIGURE

aセradiator

I , I , B I " ...,

"

"...

,

,

' , , , " , I ' ... " I I ... , I . . . " I I ... " I I , I ,',.,-"

"

'

o

H )I

e

REeE I VER FIGURE 2 BR.2GII

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