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Heat & Mass Transfer - acharya ng ranga agricultural university
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