Verified Solution • 2025–26 Session moderate

QJEEM24Ph0c83: JEE Main 2024 Physics - Class 12 JEEM24Ph0c83 Solution: Two conductors have the same resistances at but their…

Two conductors have the same resistances at 0∘C0^{\circ} \mathrm{C} but their temperature coefficients of resistance are α1\alpha_1 and α2\alpha_2 . The respective temperature coefficients for their series and parallel combinations are :

Multiple Choice Options

  • A α1+α2,α1α2α1+α2\alpha_1+\alpha_2, \frac{\alpha_1 \alpha_2}{\alpha_1+\alpha_2}
  • B α1+α22,α1+α22\frac{\alpha_1+\alpha_2}{2}, \frac{\alpha_1+\alpha_2}{2}
  • C α1+α2,α1+α22\alpha_1+\alpha_2, \frac{\alpha_1+\alpha_2}{2}
  • D α1+α22,α1+α2\frac{\alpha_1+\alpha_2}{2}, \alpha_1+\alpha_2

Step-by-Step Verified Solution

Series :

amp;Req=R1+R2amp;2R(1+αeqΔθ)=R(1+α1Δθ)+R(1+α2Δθ)amp;2R(1+αeqΔθ)=2R+(α1+α2)RΔθamp;αeq=α1+α22\begin{aligned}& \mathrm{R}_{\mathrm{eq}}=\mathrm{R}_1+\mathrm{R}_2 \\& 2 \mathrm{R}\left(1+\alpha_{\mathrm{eq}} \Delta \theta\right)=\mathrm{R}\left(1+\alpha_1 \Delta \theta\right)+\mathrm{R}\left(1+\alpha_2 \Delta \theta\right) \\& 2 \mathrm{R}\left(1+\alpha_{\mathrm{eq}} \Delta \theta\right)=2 \mathrm{R}+\left(\alpha_1+\alpha_2\right) \mathrm{R} \Delta \theta \\& \alpha_{\mathrm{eq}}=\frac{\alpha_1+\alpha_2}{2}\end{aligned}

Parallel :

amp;1Req =1R1+1R2amp;1R2(1+αeq Δθ)=1R(1+α1Δθ)+1R(1+α2Δθ)\begin{aligned}& \frac{1}{R_{\text {eq }}}=\frac{1}{R_1}+\frac{1}{R_2} \\& \frac{1}{\frac{R}{2}\left(1+\alpha_{\text {eq }} \Delta \theta\right)}=\frac{1}{R\left(1+\alpha_1 \Delta \theta\right)}+\frac{1}{\mathrm{R}\left(1+\alpha_2 \Delta \theta\right)}\end{aligned}

amp;21+αeqΔθ=11+α1Δθ+11+α2Δθamp;21+αeqΔθ=1+α2Δθ+1+α1Δθ(1+α1Δθ)(1+α2Δθ)amp;2[(1+α1Δθ)(1+α2Δθ)]amp;=[2+(α1+α2)Δθ][1+αeqΔθ]amp;2[1+α1Δθ+α2Δθ+α1α2Δθ]\begin{aligned}& \frac{2}{1+\alpha_{\mathrm{eq}} \Delta \theta}=\frac{1}{1+\alpha_1 \Delta \theta}+\frac{1}{1+\alpha_2 \Delta \theta} \\& \frac{2}{1+\alpha_{\mathrm{eq}} \Delta \theta}=\frac{1+\alpha_2 \Delta \theta+1+\alpha_1 \Delta \theta}{\left(1+\alpha_1 \Delta \theta\right)\left(1+\alpha_2 \Delta \theta\right)} \\& 2\left[\left(1+\alpha_1 \Delta \theta\right)\left(1+\alpha_2 \Delta \theta\right)\right] \\& =\left[2+\left(\alpha_1+\alpha_2\right) \Delta \theta\right]\left[1+\alpha_{\mathrm{eq}} \Delta \theta\right] \\& 2\left[1+\alpha_1 \Delta \theta+\alpha_2 \Delta \theta+\alpha_1 \alpha_2 \Delta \theta\right]\end{aligned}

amp;=amp;2+2αeqΔθ+(α1+α2)Δθ+αeq(α1+α2)Δθ2\begin{aligned}& = \\& 2+2 \alpha_{\mathrm{eq}} \Delta \theta+\left(\alpha_1+\alpha_2\right) \Delta \theta+\alpha_{\mathrm{eq}}\left(\alpha_1+\alpha_2\right) \Delta \theta^2\end{aligned}

Neglecting small terms

amp;2+2(α1+α2)Δθ=2+2αeqΔθ+(α1+α2)Δθamp;(α1+α2)Δθ=2αeqΔθamp;αeq=α1+α22\begin{aligned}& 2+2\left(\alpha_1+\alpha_2\right) \Delta \theta=2+2 \alpha_{\mathrm{eq}} \Delta \theta+\left(\alpha_1+\alpha_2\right) \Delta \theta \\& \left(\alpha_1+\alpha_2\right) \Delta \theta=2 \alpha_{\mathrm{eq}} \Delta \theta \\& \alpha_{\mathrm{eq}}=\frac{\alpha_1+\alpha_2}{2}\end{aligned}

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