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Current Electricity question

2010 · Shift 0 · Q66
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Current Electricity question

2010 · Shift 0 · Q66

JEE MainPhysicsCurrent ElectricityMCQ+4 / −1
Two conductors have the same resistance at 0∘C{0^ \circ }C0∘C but their temperature coefficients of resistance are α1{\alpha _1}α1​ and α2.{\alpha _2}.α2​. The respective temperature coefficients of their series and parallel combinations are nearly
  1. A
    α1+α22, α1+α2{{{\alpha _1} + {\alpha _2}} \over 2},\,{\alpha _1} + {\alpha _2}2α1​+α2​​,α1​+α2​
  2. B
    α1+α2, α1+α22{\alpha _1} + {\alpha _2},\,{{{\alpha _1} + {\alpha _2}} \over 2}α1​+α2​,2α1​+α2​​
  3. C
    α1+α2, α1α2α1+α2{\alpha _1} + {\alpha _2},\,{{{\alpha _1}{\alpha _2}} \over {{\alpha _1} + {\alpha _2}}}α1​+α2​,α1​+α2​α1​α2​​
  4. D
    α1+α22, α1+α22{{{\alpha _1} + {\alpha _2}} \over 2},\,{{{\alpha _1} + {\alpha _2}} \over 2}2α1​+α2​​,2α1​+α2​​
View written solutionFree

Correct answer: D

  1. Write resistance of each conductor at temperature ttt

Since both have the same resistance at 0∘C0^\circ C0∘C, let that resistance be RRR.

Then at temperature ttt, R1=R(1+α1t),R2=R(1+α2t)R_1 = R(1+\alpha_1 t), \qquad R_2 = R(1+\alpha_2 t)R1​=R(1+α1​t),R2​=R(1+α2​t)

For temperature coefficient of a combination, we compare the total resistance with its value at 0∘C0^\circ C0∘C.


  1. Series combination

In series, Rs=R1+R2=R(1+α1t)+R(1+α2t)R_s = R_1 + R_2 = R(1+\alpha_1 t)+R(1+\alpha_2 t)Rs​=R1​+R2​=R(1+α1​t)+R(1+α2​t) Rs=2R+R(α1+α2)tR_s = 2R + R(\alpha_1+\alpha_2)tRs​=2R+R(α1​+α2​)t

At 0∘C0^\circ C0∘C, series resistance is Rs0=2RR_{s0}=2RRs0​=2R

Let the temperature coefficient of the series combination be αs\alpha_sαs​. Then Rs=Rs0(1+αst)=2R(1+αst)R_s = R_{s0}(1+\alpha_s t)=2R(1+\alpha_s t)Rs​=Rs0​(1+αs​t)=2R(1+αs​t)

Comparing with Rs=2R+R(α1+α2)tR_s = 2R + R(\alpha_1+\alpha_2)tRs​=2R+R(α1​+α2​)t we get 2Rαst=R(α1+α2)t2R\alpha_s t = R(\alpha_1+\alpha_2)t2Rαs​t=R(α1​+α2​)t αs=α1+α22\alpha_s = \frac{\alpha_1+\alpha_2}{2}αs​=2α1​+α2​​


  1. Parallel combination

In parallel, Rp=R1R2R1+R2R_p = \frac{R_1R_2}{R_1+R_2}Rp​=R1​+R2​R1​R2​​

Substitute: Rp=R(1+α1t) R(1+α2t)R(1+α1t)+R(1+α2t)R_p = \frac{R(1+\alpha_1 t)\,R(1+\alpha_2 t)}{R(1+\alpha_1 t)+R(1+\alpha_2 t)}Rp​=R(1+α1​t)+R(1+α2​t)R(1+α1​t)R(1+α2​t)​ Rp=R (1+α1t)(1+α2t)2+(α1+α2)tR_p = R\,\frac{(1+\alpha_1 t)(1+\alpha_2 t)}{2+(\alpha_1+\alpha_2)t}Rp​=R2+(α1​+α2​)t(1+α1​t)(1+α2​t)​

Since the question says nearly, we neglect second-order term α1α2t2\alpha_1\alpha_2 t^2α1​α2​t2: (1+α1t)(1+α2t)≈1+(α1+α2)t(1+\alpha_1 t)(1+\alpha_2 t) \approx 1+(\alpha_1+\alpha_2)t(1+α1​t)(1+α2​t)≈1+(α1​+α2​)t

So, Rp≈R1+(α1+α2)t2+(α1+α2)tR_p \approx R\frac{1+(\alpha_1+\alpha_2)t}{2+(\alpha_1+\alpha_2)t}Rp​≈R2+(α1​+α2​)t1+(α1​+α2​)t​

Now use 1+xt2+xt=12⋅1+xt1+xt2\frac{1+xt}{2+xt} = \frac{1}{2}\cdot \frac{1+xt}{1+\frac{xt}{2}}2+xt1+xt​=21​⋅1+2xt​1+xt​ where x=α1+α2x=\alpha_1+\alpha_2x=α1​+α2​.

For small xtxtxt, 11+xt2≈1−xt2\frac{1}{1+\frac{xt}{2}} \approx 1-\frac{xt}{2}1+2xt​1​≈1−2xt​

Thus, Rp≈R2(1+xt)(1−xt2)R_p \approx \frac{R}{2}(1+xt)\left(1-\frac{xt}{2}\right)Rp​≈2R​(1+xt)(1−2xt​) Neglecting higher-order terms, Rp≈R2(1+xt2)R_p \approx \frac{R}{2}\left(1+\frac{xt}{2}\right)Rp​≈2R​(1+2xt​)

So, Rp≈R2(1+α1+α22t)R_p \approx \frac{R}{2}\left(1+\frac{\alpha_1+\alpha_2}{2}t\right)Rp​≈2R​(1+2α1​+α2​​t)

At 0∘C0^\circ C0∘C, parallel resistance is Rp0=R⋅RR+R=R2R_{p0} = \frac{R\cdot R}{R+R}=\frac{R}{2}Rp0​=R+RR⋅R​=2R​

Hence temperature coefficient of parallel combination is αp=α1+α22\alpha_p = \frac{\alpha_1+\alpha_2}{2}αp​=2α1​+α2​​


  1. Final result

Therefore, the temperature coefficients of:

  • series combination =α1+α22= \dfrac{\alpha_1+\alpha_2}{2}=2α1​+α2​​
  • parallel combination =α1+α22= \dfrac{\alpha_1+\alpha_2}{2}=2α1​+α2​​

So the correct option is: D\boxed{\text{D}}D​


  1. Comparison with stored answer

Stored correct answer: D

Derived answer: D

They agree.

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