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Heat & Mass Transfer - acharya ng ranga agricultural university

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temperature differential T i - T o and determine what the heat flow will be. For a<br />

cylinder with length very large compared to diameter, it may be assumed that<br />

the heat flows only in a radial direction, so that the only space coordinate<br />

needed to specify the system is r. Again, Fourier's law is used by inserting the<br />

proper area relation. The area for heat flow in the cylindrical system is<br />

A =2πrL<br />

so that Fourier's law is written<br />

with the boundary conditions<br />

q<br />

r<br />

dT<br />

= −k<br />

Ar<br />

or<br />

dr<br />

q r<br />

=−2πk rL<br />

T = T i at r = r i ,<br />

dT<br />

dr<br />

T = T o at r = r o<br />

The solution to equation<br />

q<br />

r<br />

dT<br />

= −k<br />

Ar<br />

is<br />

dr<br />

q=<br />

k<br />

2πL<br />

ln( r<br />

2<br />

/ r1<br />

)<br />

( T −T<br />

)<br />

1<br />

2<br />

and the thermal resistance in this case is<br />

R<br />

th<br />

ln( ro<br />

/ ri<br />

)<br />

=<br />

2πkL<br />

The thermal-resistance concept may be used for multiple-layer<br />

cylindrical walls just as it was used for plane walls. For the three-layer system<br />

shown in Figure the solution is<br />

2π<br />

L ( T1<br />

−T4<br />

)<br />

q =<br />

ln( r2<br />

/ r1<br />

) ln( r3<br />

/ r2<br />

) ln( r4<br />

/ r2<br />

)<br />

+ +<br />

K K K<br />

a<br />

The thermal circuit is also shown in Figure.<br />

B<br />

B

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