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Heat and Thermodynamics question

2025 · 22 Jan · Shift 1 · Q72
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Heat and Thermodynamics question

2025 · 22 Jan · Shift 1 · Q72

JEE MainPhysicsHeat and ThermodynamicsNumerical+4 / −1
Three conductors of same length having thermal conductivity k1,k2k_1, k_2k1​,k2​ and k3k_3k3​ are connected as shown in figure. JEE Main 2025 (Online) 22nd January Morning Shift Physics - Heat and Thermodynamics Question 42 English Area of cross sections of 1st 1^{\text {st }}1st  and 2nd 2^{\text {nd }}2nd  conductor are same and for 3rd 3^{\text {rd }}3rd  conductor it is double of the 1st 1^{\text {st }}1st  conductor. The temperatures are given in the figure. In steady state condition, the value of θ\thetaθ is ‾\underline{\hspace{2cm}}​∘C{ }^{\circ} \mathrm{C}∘C. (Given : k1=60Js−1 m−1 K−1,k2=120Js−1 m−1 K−1,k3=135Js−1 m−1 K−1\mathrm{k}_1=60 \mathrm{Js}^{-1} \mathrm{~m}^{-1} \mathrm{~K}^{-1}, \mathrm{k}_2=120 \mathrm{Js}^{-1} \mathrm{~m}^{-1} \mathrm{~K}^{-1}, \mathrm{k}_3=135 \mathrm{Js}^{-1} \mathrm{~m}^{-1} \mathrm{~K}^{-1}k1​=60Js−1 m−1 K−1,k2​=120Js−1 m−1 K−1,k3​=135Js−1 m−1 K−1 )
Numerical answer
View written solutionFree

Correct answer: 40

Let the common length of each conductor be LLL.

Take area of cross-section of conductor 1 and 2 as AAA. Then for conductor 3, area is 2A2A2A.

In the shown arrangement, conductor 1 and 2 are connected between the same two temperature points, so they are in parallel, and conductor 3 is connected in series with this parallel combination.

We are to find the junction temperature θ\thetaθ in steady state.


1. Thermal conductance of each rod

Thermal conductance is G=kALG=\frac{kA}{L}G=LkA​

So,

  • For conductor 1: G1=k1AL=60ALG_1=\frac{k_1A}{L}=\frac{60A}{L}G1​=Lk1​A​=L60A​

  • For conductor 2: G2=k2AL=120ALG_2=\frac{k_2A}{L}=\frac{120A}{L}G2​=Lk2​A​=L120A​

  • For conductor 3: G3=k3(2A)L=135⋅2AL=270ALG_3=\frac{k_3(2A)}{L}=\frac{135\cdot 2A}{L}=\frac{270A}{L}G3​=Lk3​(2A)​=L135⋅2A​=L270A​


2. Equivalent conductance of conductors 1 and 2 in parallel

For parallel combination, G12=G1+G2=60AL+120AL=180ALG_{12}=G_1+G_2=\frac{60A}{L}+\frac{120A}{L}=\frac{180A}{L}G12​=G1​+G2​=L60A​+L120A​=L180A​


3. Apply steady-state heat current condition

From the figure, the parallel combination is between 100∘C100^\circ \mathrm{C}100∘C and θ\thetaθ, and conductor 3 is between θ\thetaθ and 0∘C0^\circ \mathrm{C}0∘C.

Hence,

  • Heat current through the parallel part: Q˙12=G12(100−θ)=180AL(100−θ)\dot Q_{12}=G_{12}(100-\theta)=\frac{180A}{L}(100-\theta)Q˙​12​=G12​(100−θ)=L180A​(100−θ)

  • Heat current through conductor 3: Q˙3=G3(θ−0)=270ALθ\dot Q_3=G_3(\theta-0)=\frac{270A}{L}\thetaQ˙​3​=G3​(θ−0)=L270A​θ

In steady state, these must be equal: 180AL(100−θ)=270ALθ\frac{180A}{L}(100-\theta)=\frac{270A}{L}\thetaL180A​(100−θ)=L270A​θ

Cancel AL\frac{A}{L}LA​: 180(100−θ)=270θ180(100-\theta)=270\theta180(100−θ)=270θ

18000−180θ=270θ18000-180\theta=270\theta18000−180θ=270θ

18000=450θ18000=450\theta18000=450θ

θ=40∘C\theta=40^\circ \mathrm{C}θ=40∘C


4. Final answer

40\boxed{40}40​

The derived answer matches the stored correct answer.

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