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Question: Two wires of resistance R<sub>1</sub> and R<sub>2</sub> have temperature co-efficient of resistance ...

Two wires of resistance R1 and R2 have temperature co-efficient of resistance α1 and α2 respectively. These are joined in series. The effective temperature co-efficient of resistance is

A

α1+α22\frac{\alpha_{1} + \alpha_{2}}{2}

B

α1α2\sqrt{\alpha_{1}\alpha_{2}}

C

α1R1+α2R2R1+R2\frac{\alpha_{1}R_{1} + \alpha_{2}R_{2}}{R_{1} + R_{2}}

D

R1R2α1α2R12+R22\frac{\sqrt{R_{1}R_{2}\alpha_{1}\alpha_{2}}}{\sqrt{R_{1}^{2} + R_{2}^{2}}}

Answer

α1R1+α2R2R1+R2\frac{\alpha_{1}R_{1} + \alpha_{2}R_{2}}{R_{1} + R_{2}}

Explanation

Solution

Suppose at toC resistances of the two wires becomes R1tR_{1t} and R2tR_{2t} respectively and equivalent resistance becomes Rt. In series grouping Rt = R1t + R2t, also R1t = R1(1 + α1t) and R2t = R2(1 + α2t)

Rt = R1(1 + α1t) + R2(1 + α2t) = (R1 + R2) + (R1α1 + R2α2) t = (R1+R2)[1+R1α1+R2α2R1+R2t](R_{1} + R_{2})\left\lbrack 1 + \frac{R_{1}\alpha_{1} + R_{2}\alpha_{2}}{R_{1} + R_{2}}t \right\rbrack.

Hence effective temperature co-efficient is R1α1+R2α2R1+R2\frac{R_{1}\alpha_{1} + R_{2}\alpha_{2}}{R_{1} + R_{2}}.