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Order Isothermal Processes by Magnitude of Work Involved

Arrange the following isothermal processes in order of the magnitude of the work (pV)(p - V) involved between states 1 and 2.

A. Expansion in single stage wAw_A
B. Expansion in multi stages wBw_B
C. Compression in single stage wCw_C
D. Compression in multi stages wDw_D

Choose the correct option :

Options

A

wB>wA>wC>wD|w_B| > |w_A| > |w_C| > |w_D|

B

wC>wD>wA>wB|w_C| > |w_D| > |w_A| > |w_B|

C

wC>wD>wB>wA|w_C| > |w_D| > |w_B| > |w_A|

Correct
D

wB>wA>wD>wC|w_B| > |w_A| > |w_D| > |w_C|

Topics & Concepts

Step-by-Step Solution

To find the correct order of the magnitude of work involved in the given isothermal processes, let us consider two states: State 1 with (P1,V1)(P_1, V_1) and State 2 with (P2,V2)(P_2, V_2).

1. Expansion Process (from State 1 to State 2, where V2>V1V_2 > V_1 and P1>P2P_1 > P_2):

  • Single-stage expansion (wAw_A): The gas expands in one step against a constant external pressure Pext=P2P_{\text{ext}} = P_2. Magnitude of work: wA=P2(V2V1)\text{Magnitude of work: } |w_A| = P_2(V_2 - V_1)

  • Multi-stage expansion (wBw_B): The expansion occurs in multiple intermediate steps. As the number of stages increases, the area under the PVP-V curve increases toward the reversible path. Magnitude of work: wB>wA\text{Magnitude of work: } |w_B| > |w_A|

  • Reversible expansion (wrevw_{\text{rev}}): Represented by the area directly under the isothermal PVP-V curve, serving as the upper bound for expansion work: wrev=nRTln(V2V1)|w_{\text{rev}}| = nRT \ln\left(\frac{V_2}{V_1}\right) Thus, for expansion: wrev>wB>wA|w_{\text{rev}}| > |w_B| > |w_A|


2. Compression Process (from State 2 to State 1, where V1<V2V_1 < V_2 and P1>P2P_1 > P_2):

  • Single-stage compression (wCw_C): The gas is compressed in one step against a constant external pressure Pext=P1P_{\text{ext}} = P_1. Magnitude of work: wC=P1(V2V1)\text{Magnitude of work: } |w_C| = P_1(V_2 - V_1)

  • Multi-stage compression (wDw_D): The gas is compressed in multiple intermediate steps. As the number of stages increases, the work required to compress the gas decreases toward the reversible work magnitude. Magnitude of work: wC>wD\text{Magnitude of work: } |w_C| > |w_D|

  • Reversible compression (wrevw_{\text{rev}}): Serves as the lower bound for compression work: wC>wD>wrev|w_C| > |w_D| > |w_{\text{rev}}|


3. Comparison of all magnitudes:

Since P1>P2P_1 > P_2, the area of the rectangle corresponding to single-stage compression (P1ΔVP_1 \Delta V) is larger than the area under the reversible curve, which in turn is larger than the area corresponding to single-stage expansion (P2ΔVP_2 \Delta V).

Combining all the inequalities: wC>wD>wrev>wB>wA|w_C| > |w_D| > |w_{\text{rev}}| > |w_B| > |w_A|

Thus, the order of magnitude of work is: wC>wD>wB>wA|w_C| > |w_D| > |w_B| > |w_A|

This corresponds to Option C.

Order Isothermal Processes by Magnitude of Work Involved | Chemistry PYQ Solution - JEE Challenger