MCQMediumJEE 2025Entropy & Spontaneity

JEE Chemistry 2025 Question with Solution

Ice at 5C-5^\circ C is heated to become vapor with temperature of 110C110^\circ C at atmospheric pressure. The entropy change associated with this process can be obtained from:

  • A

    268K383KCpdT+ΔHmelting273+ΔHboiling373\int_{268 \, K}^{383 \, K} C_p \, dT + \frac{\Delta H_{melting}}{273} + \frac{\Delta H_{boiling}}{373}

  • B

    268K273KCp,mTdT+ΔHmfusionTf+ΔHmvaporisationTb\int_{268 \, K}^{273 \, K} \frac{C_{p,m}}{T} \, dT + \frac{\Delta H_m \, fusion}{T_f} + \frac{\Delta H_m \, vaporisation}{T_b}

  • C

    268K373KCpdT+qrev\int_{268 \, K}^{373 \, K} C_p \, dT + q_{rev}

  • D

    268K273KCpdT+ΔHmfusionTf+ΔHmvaporisationTb+373K383KCpdT\int_{268 \, K}^{273 \, K} C_p \, dT + \frac{\Delta H_m \, fusion}{T_f} + \frac{\Delta H_m \, vaporisation}{T_b} + \int_{373 \, K}^{383 \, K} C_p \, dT

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: Ice at 5C-5^\circ C is converted to vapor at 110C110^\circ C at atmospheric pressure.

Find: The correct expression for the total entropy change.

For entropy change during heating, the required form is:

ΔS=CpTdT\Delta S = \int \frac{C_p}{T} \, dT

For phase change at constant temperature:

ΔS=ΔHT\Delta S = \frac{\Delta H}{T}

So the process must be broken into stages:

  1. Heating ice from 268K268 \, \text{K} to 273K273 \, \text{K}
ΔS1=268273Cp,iceTdT\Delta S_1 = \int_{268}^{273} \frac{C_{p,\text{ice}}}{T} \, dT
  1. Melting at 273K273 \, \text{K}
ΔS2=ΔHfusionTf\Delta S_2 = \frac{\Delta H_{\text{fusion}}}{T_f}
  1. Heating water from 273K273 \, \text{K} to 373K373 \, \text{K}
ΔS3=273373Cp,waterTdT\Delta S_3 = \int_{273}^{373} \frac{C_{p,\text{water}}}{T} \, dT
  1. Vaporisation at 373K373 \, \text{K}
ΔS4=ΔHvaporisationTb\Delta S_4 = \frac{\Delta H_{\text{vaporisation}}}{T_b}
  1. Heating steam from 373K373 \, \text{K} to 383K383 \, \text{K}
ΔS5=373383Cp,steamTdT\Delta S_5 = \int_{373}^{383} \frac{C_{p,\text{steam}}}{T} \, dT

Thus the total entropy change is the sum of these contributions. The solution concludes that the correct option is B.

The listed expression in option B is:

268K273KCp,mTdT+ΔHmfusionTf+ΔHmvaporisationTb\int_{268 \, \text{K}}^{273 \, \text{K}} \frac{C_{p,m}}{T} \, dT + \frac{\Delta H_m \, \text{fusion}}{T_f} + \frac{\Delta H_m \, \text{vaporisation}}{T_b}

Therefore, the correct option is B.

Stage-wise Entropy Accounting

Given: The substance passes through solid, liquid, and vapor phases while being heated from 268K268 \, \text{K} to 383K383 \, \text{K}.

Find: Which option matches the entropy-change method.

Entropy is a state function, but for a reversible path the total change is written as the sum of reversible heating and phase-transition terms:

ΔStotal=ΔS1+ΔS2+ΔS3+ΔS4+ΔS5\Delta S_{\text{total}} = \Delta S_1 + \Delta S_2 + \Delta S_3 + \Delta S_4 + \Delta S_5

with

ΔS1=268273Cp,mTdT\Delta S_1 = \int_{268}^{273} \frac{C_{p,m}}{T} \, dT ΔS2=ΔHmfusionTf\Delta S_2 = \frac{\Delta H_m \, \text{fusion}}{T_f} ΔS3=273373Cp,mTdT\Delta S_3 = \int_{273}^{373} \frac{C_{p,m}}{T} \, dT ΔS4=ΔHmvaporisationTb\Delta S_4 = \frac{\Delta H_m \, \text{vaporisation}}{T_b} ΔS5=373383Cp,mTdT\Delta S_5 = \int_{373}^{383} \frac{C_{p,m}}{T} \, dT

Now compare with the options.

  • Option A uses CpdT\int C_p \, dT instead of CpTdT\int \frac{C_p}{T} \, dT, so it is not the entropy form.
  • Option C is not the correct entropy expression.
  • Option D again uses heating terms without division by TT.
  • Option B contains the correct entropy-type terms for heating and phase changes as identified in the solution.

Hence, the correct option is B. The solution itself omits some heating terms in the final printed expression, but explicitly identifies B as the answer, and that conclusion is taken as authoritative.

Common mistakes

  • Using CpdT\int C_p \, dT for entropy change is incorrect because that form gives heat involved in temperature rise, not entropy change. For entropy during heating, use CpTdT\int \frac{C_p}{T} \, dT instead.

  • Ignoring phase changes is wrong because melting and vaporisation each contribute finite entropy jumps at constant temperature. Add terms of the form ΔHT\frac{\Delta H}{T} at the melting and boiling points.

  • Treating the entire process as one continuous heating step is incorrect because the substance changes phase along the way. Break the path into solid heating, fusion, liquid heating, vaporisation, and vapor heating.

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