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Match Isothermal Thermodynamic Processes with Expression

Match List - I with List - II. Given V1\text{V}_1 and V2\text{V}_2 are initial and final volumes respectively.

List - IList - II(Isothermal process)(Expression)A. Reversible expansionI. q=0B. Free expansionII. q=nRTlnV2V1C. Irreversible CompressionIII. w=Pext(V1V2)D. Cyclic reversibleIV. qrevT=0\begin{array}{ll} \text{List - I} & \text{List - II} \\ \text{(Isothermal process)} & \text{(Expression)} \\ \text{A. Reversible expansion} & \text{I. } q = 0 \\ \text{B. Free expansion} & \text{II. } q = nRT \ln \frac{V_2}{V_1} \\ \text{C. Irreversible Compression} & \text{III. } w = -P_{\text{ext}} (V_1 - V_2) \\ \text{D. Cyclic reversible} & \text{IV. } \frac{q_{\text{rev}}}{T} = 0 \end{array}

Choose the correct answer from the options given below :

Options

A

A-II, B-III, C-I, D-IV

B

A-II, B-I, C-IV, D-III

C

A-II, B-I, C-III, D-IV

Correct
D

A-I, B-II, C-III, D-IV

Topics & Concepts

Step-by-Step Solution

To solve this matching question, let us analyze each process in List - I and find its corresponding mathematical expression in List - II:

  1. A. Reversible expansion (Isothermal): For an isothermal process involving an ideal gas, the internal energy change is zero (ΔU=0\Delta U = 0). By the First Law of Thermodynamics: ΔU=q+w=0    q=w\Delta U = q + w = 0 \implies q = -w The work done in a reversible isothermal expansion from volume V1V_1 to V2V_2 is given by: w=nRTln(V2V1)w = -nRT \ln \left(\frac{V_2}{V_1}\right) Therefore, the heat absorbed is: q=nRTln(V2V1)q = nRT \ln \left(\frac{V_2}{V_1}\right) Thus, A matches with II.

  2. B. Free expansion (Isothermal): In a free expansion, the gas expands against zero external pressure (Pext=0P_{\text{ext}} = 0), so the work done is w=0w = 0. Since the process is also isothermal, ΔU=0\Delta U = 0. From the First Law of Thermodynamics (ΔU=q+w\Delta U = q + w): 0=q+0    q=00 = q + 0 \implies q = 0 Thus, B matches with I.

  3. C. Irreversible Compression: Work done during an irreversible process against a constant external pressure PextP_{\text{ext}} is expressed as: w=PextΔV=Pext(V2V1)=Pext(V1V2)w = -P_{\text{ext}} \Delta V = -P_{\text{ext}} (V_2 - V_1) = -P_{\text{ext}} (V_1 - V_2) Thus, C matches with III.

  4. D. Cyclic reversible: Entropy SS is a state function, so for any cyclic process, the total change in entropy is zero: ΔS=dqrevT=0    qrevT=0\Delta S = \oint \frac{dq_{\text{rev}}}{T} = 0 \implies \frac{q_{\text{rev}}}{T} = 0 Thus, D matches with IV.

Combining these matches gives: A-II, B-I, C-III, D-IV\text{A-II, B-I, C-III, D-IV}

This corresponds to Option C.

Match Isothermal Thermodynamic Processes with Expression | Chemistry PYQ Solution - JEE Challenger