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Question: A rod of length l and cross section area A has a variable thermal conductivity given by K = a T, whe...

A rod of length l and cross section area A has a variable thermal conductivity given by K = a T, where a is a positive constant and T is temperature in Kelvin. Two ends of the rod are maintained at temperatures T1 and T2 (T1> T2). Heat current flowing through the rod will be –

A

Aα(T12T22)3l\frac{A\alpha(T_{1}^{2} - T_{2}^{2})}{3\mathcal{l}}

B

Aα(T12+T22)l\frac{A\alpha(T_{1}^{2} + T_{2}^{2})}{\mathcal{l}}

C

Aα(T12+T22)3l\frac{A\alpha(T_{1}^{2} + T_{2}^{2})}{3\mathcal{l}}

D

Aα(T12T22)2l\frac{A\alpha(T_{1}^{2} - T_{2}^{2})}{2\mathcal{l}}

Answer

Aα(T12T22)2l\frac{A\alpha(T_{1}^{2} - T_{2}^{2})}{2\mathcal{l}}

Explanation

Solution

Heat current i = – KA dTdX\frac{dT}{dX}

idX = – KA dT

i0ldX=AαT1T2TdTi\int_{0}^{\mathcal{l}}{dX = - A\alpha\int_{T_{1}}^{T_{2}}{TdT}}

̃ il = – A a(T22T12)2\frac{(T_{2}^{2} - T_{1}^{2})}{2}

̃ i = A a (T12T22)2l\frac{(T_{1}^{2} - T_{2}^{2})}{2\mathcal{l}}