NVAMediumJEE 2025Heat Transfer (Conduction, Convection, Radiation)

JEE Physics 2025 Question with Solution

Two cylindrical rods A and B made of different materials, are joined in a straight line. The ratio of lengths, radii and thermal conductivities of these rods are : LALB=12\frac{L_A}{L_B} = \frac{1}{2}, rArB=2\frac{r_A}{r_B} = 2, and KAKB=12\frac{K_A}{K_B} = \frac{1}{2}. The free ends of rods A and B are maintained at 400K400 \, \text{K}, 200K200 \, \text{K}, respectively. The temperature of rods interface is _____ K\text{K}, when equilibrium is established.

Answer

Correct answer:360

Step-by-step solution

Thermal resistance method

Given:

  • Temperature at the free end of rod A is 400K400 \, \text{K}.
  • Temperature at the free end of rod B is 200K200 \, \text{K}.
  • LALB=12\frac{L_A}{L_B} = \frac{1}{2}
  • rArB=2\frac{r_A}{r_B} = 2
  • KAKB=12\frac{K_A}{K_B} = \frac{1}{2}

Find: The interface temperature TT.

For a cylindrical rod, thermal resistance is

Rth=LKA=LKπr2R_{th} = \frac{L}{KA} = \frac{L}{K\pi r^2}

So,

Rth,A=LAKAπrA2,Rth,B=LBKBπrB2R_{th,A} = \frac{L_A}{K_A \pi r_A^2}, \qquad R_{th,B} = \frac{L_B}{K_B \pi r_B^2}

Now,

Rth,ARth,B=LALBKBKA(rBrA)2\frac{R_{th,A}}{R_{th,B}} = \frac{L_A}{L_B} \cdot \frac{K_B}{K_A} \cdot \left(\frac{r_B}{r_A}\right)^2

Substituting the given ratios,

Rth,ARth,B=(12)2(12)2=14\frac{R_{th,A}}{R_{th,B}} = \left(\frac{1}{2}\right) \cdot 2 \cdot \left(\frac{1}{2}\right)^2 = \frac{1}{4}

Hence,

Rth,B=4Rth,AR_{th,B} = 4R_{th,A}

At equilibrium, the heat current through both rods is the same. If the interface temperature is TT, then

400TRth,A=T200Rth,B\frac{400 - T}{R_{th,A}} = \frac{T - 200}{R_{th,B}}

Using Rth,B=4Rth,AR_{th,B} = 4R_{th,A},

400TRth,A=T2004Rth,A\frac{400 - T}{R_{th,A}} = \frac{T - 200}{4R_{th,A}}

So,

4(400T)=T2004(400 - T) = T - 200 16004T=T2001600 - 4T = T - 200 1800=5T1800 = 5T T=360KT = 360 \, \text{K}

Therefore, the temperature of the rods interface is 360K360 \, \text{K}.

Resolving the discrepancy in Approach 1

Given: The same ratios and end temperatures as above.

Find: The correct interface temperature.

The first approach on the page writes the conduction equation correctly as

KAπrA2(400T)LA=KBπrB2(T200)LB\frac{K_A \pi r_A^2 (400 - T)}{L_A} = \frac{K_B \pi r_B^2 (T - 200)}{L_B}

but simplifies the ratio incorrectly.

Using

KAKB=12,rArB=2,LALB=12\frac{K_A}{K_B} = \frac{1}{2}, \qquad \frac{r_A}{r_B} = 2, \qquad \frac{L_A}{L_B} = \frac{1}{2}

we get

KArA2/LAKBrB2/LB=KAKB(rArB)2LBLA\frac{K_A r_A^2 / L_A}{K_B r_B^2 / L_B} = \frac{K_A}{K_B} \cdot \left(\frac{r_A}{r_B}\right)^2 \cdot \frac{L_B}{L_A} =(12)42=4= \left(\frac{1}{2}\right) \cdot 4 \cdot 2 = 4

Therefore,

4(400T)=T2004(400 - T) = T - 200

and not

2(400T)=T2002(400 - T) = T - 200

Now solve:

16004T=T2001600 - 4T = T - 200 1800=5T1800 = 5T T=360KT = 360 \, \text{K}

So the value 333.33K333.33 \, \text{K} shown in Approach 1 comes from an algebraic simplification error. The correct interface temperature is 360K360 \, \text{K}.

Common mistakes

  • Using the same heat-flow equation but simplifying the ratio incorrectly. This gives a wrong factor on the left-hand side and leads to T=333.33KT = 333.33 \, \text{K}. Instead, carefully substitute KAKB\frac{K_A}{K_B}, rArB\frac{r_A}{r_B} and LBLA\frac{L_B}{L_A} with the correct powers and orientation.

  • Forgetting that cross-sectional area of a rod is proportional to r2r^2, not rr. If you use radius directly instead of area, the thermal resistance ratio becomes wrong. Always use A=πr2A = \pi r^2 in conduction problems.

  • Treating the rods as if the temperature drop is the same across both parts. In series conduction, the heat current is the same, not the temperature drop. Use equal heat current or thermal resistance division to find the interface temperature.

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