MCQEasyJEE 2025Second Law & Heat Engines

JEE Physics 2025 Question with Solution

A Carnot engine (E) is working between two temperatures 473K473\,\text{K} and 273K273\,\text{K}. In a new system two engines - engine E1E_1 works between 473K473\,\text{K} to 373K373\,\text{K} and engine E2E_2 works between 373K373\,\text{K} to 273K273\,\text{K}. If η12\eta_{12}, η1\eta_1 and η2\eta_2 are the efficiencies of the engines EE, E1E_1 and E2E_2, respectively, then:

  • A

    η12<η1+η2\eta_{12} < \eta_1 + \eta_2

  • B

    η12=η1+η2\eta_{12} = \eta_1 + \eta_2

  • C

    η12=η1η2\eta_{12} = \eta_1 \eta_2

  • D

    η12>η1+η2\eta_{12} > \eta_1 + \eta_2

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: A Carnot engine EE works between TH=473KT_H = 473\,\text{K} and TC=273KT_C = 273\,\text{K}. Two other engines work as E1:473K373KE_1: 473\,\text{K} \to 373\,\text{K} and E2:373K273KE_2: 373\,\text{K} \to 273\,\text{K}.

Find: The correct relation among η12\eta_{12}, η1\eta_1 and η2\eta_2.

For a Carnot engine,

η=1TCTH\eta = 1 - \frac{T_C}{T_H}

So for engine EE,

η12=1273473=200473\eta_{12} = 1 - \frac{273}{473} = \frac{200}{473}

For engine E1E_1,

η1=1373473=100473\eta_1 = 1 - \frac{373}{473} = \frac{100}{473}

For engine E2E_2,

η2=1273373=100373\eta_2 = 1 - \frac{273}{373} = \frac{100}{373}

Now compare η12\eta_{12} with η1+η2\eta_1 + \eta_2:

η1+η2=100473+1003730.4798\eta_1 + \eta_2 = \frac{100}{473} + \frac{100}{373} \approx 0.4798

while

η12=2004730.4228\eta_{12} = \frac{200}{473} \approx 0.4228

Hence,

η12<η1+η2\eta_{12} < \eta_1 + \eta_2

Also, the series relation for two Carnot stages is

(1η1)(1η2)=1η12(1-\eta_1)(1-\eta_2) = 1-\eta_{12}

which gives

η12=η1+η2η1η2\eta_{12} = \eta_1 + \eta_2 - \eta_1\eta_2

So the solution's listed option η12=η1η2\eta_{12} = \eta_1\eta_2 is inconsistent with the working shown in the solution. Based on the solution derivation, the correct option is A.

Therefore, the correct option is A, i.e. η12<η1+η2\eta_{12} < \eta_1 + \eta_2.

Complement of efficiency trick

Given: The engines operate in two stages from 473K473\,\text{K} to 373K373\,\text{K} and from 373K373\,\text{K} to 273K273\,\text{K}.

Find: A quick relation between the overall efficiency and stage efficiencies.

Use the fact that for staged Carnot engines, the fractions of heat rejected multiply:

1η1=373473,1η2=2733731-\eta_1 = \frac{373}{473}, \qquad 1-\eta_2 = \frac{273}{373}

Therefore,

(1η1)(1η2)=373473273373=273473=1η12(1-\eta_1)(1-\eta_2) = \frac{373}{473}\cdot\frac{273}{373} = \frac{273}{473} = 1-\eta_{12}

So,

1η1η2+η1η2=1η121-\eta_1-\eta_2+\eta_1\eta_2 = 1-\eta_{12}

which gives

η12=η1+η2η1η2\eta_{12} = \eta_1 + \eta_2 - \eta_1\eta_2

Since η1η2>0\eta_1\eta_2 > 0, it follows immediately that

η12<η1+η2\eta_{12} < \eta_1 + \eta_2

Therefore, the correct option is A.

Common mistakes

  • Adding efficiencies directly and concluding η12=η1+η2\eta_{12} = \eta_1 + \eta_2 is incorrect. For staged Carnot engines, the rejected heat fractions multiply. Use η12=η1+η2η1η2\eta_{12} = \eta_1 + \eta_2 - \eta_1\eta_2 instead.

  • Using the wrong temperature ratio in the Carnot formula is a common error. The efficiency is η=1TCTH\eta = 1 - \frac{T_C}{T_H}, not 1THTC1 - \frac{T_H}{T_C}. Always place the lower temperature in the numerator.

  • Assuming the overall efficiency equals the product η1η2\eta_1\eta_2 is wrong. The product does not represent total Carnot efficiency here; it is only part of the correction term in η12=η1+η2η1η2\eta_{12} = \eta_1 + \eta_2 - \eta_1\eta_2.

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