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Question: The entropy change in the isothermal reversible expansion of 2 moles of an ideal gas from 10L to 100...

The entropy change in the isothermal reversible expansion of 2 moles of an ideal gas from 10L to 100L at 300K is:
(A) 42.3 JK142.3{\text{ J}}{{\text{K}}^{ - 1}}
(B) 35.8 JK1{\text{35}}{\text{.8 J}}{{\text{K}}^{ - 1}}
(C) 38.3 JK1{\text{38}}{\text{.3 J}}{{\text{K}}^{ - 1}}
(D) 32.3 JK1{\text{32}}{\text{.3 J}}{{\text{K}}^{ - 1}}

Explanation

Solution

Hint: In an isothermal process, temperature remains constant i.e. ΔT = 0\Delta {\text{T = 0}}. Joule's law states that if q=0 then there is no change in the internal energy U and hence, change in entropy entirely depends on change in volume of the gas.

Complete step by step answer:
Change in entropy in an isothermal irreversible process is given by
ΔS = 2.303 nR logVfinalVinitial\Delta {\text{S = 2}}{\text{.303 nR log}}\dfrac{{{{\text{V}}_{{\text{final}}}}}}{{{{\text{V}}_{{\text{initial}}}}}}
We have Vinitial = 10 dm3{{\text{V}}_{{\text{initial}}}}{\text{ = 10 d}}{{\text{m}}^3} and Vfinal = 100 dm3{{\text{V}}_{{\text{final}}}}{\text{ = 100 d}}{{\text{m}}^3}
Substituting these values in the given equation we get,
ΔS = 2.303 × 2 × 8.314 × log 10010\Delta {\text{S = 2}}{\text{.303 }} \times {\text{ 2 }} \times {\text{ 8}}{\text{.314 }} \times {\text{ log }}\dfrac{{100}}{{10}}
Since, log 10010 = log 10 = 1{\text{log }}\dfrac{{100}}{{10}}{\text{ = log 10 = 1}}
ΔS = 2.303 × 2 × 8.314 \Delta {\text{S = 2}}{\text{.303 }} \times {\text{ 2 }} \times {\text{ 8}}{\text{.314 }}
 = 38.29{\text{ = 38}}{\text{.29}}
 38.3 KJ1\approx {\text{ 38}}{\text{.3 K}}{{\text{J}}^{ - 1}}
So, the change in entropy is 38.3 JK1{\text{38}}{\text{.3 J}}{{\text{K}}^{ - 1}} i.e. option C is correct.

Additional information:
Whether the process is reversible or irreversible, in case of free expansion of a gas, the amount of work done is always 0.
We know that internal energy of a system is given by the formula: q + ( - W){\text{q + ( - W)}}
Where, ΔU\Delta {\text{U}}= change in internal energy of a system, q= heat supplied and W= Amount of work done on the system.
However, this equation changes as the type of process changes.
When an ideal gas is subjected to isothermal expansion i.e. ΔT = 0\Delta {\text{T = 0}} in vacuum the work done W = 0 as pex = 0{{\text{p}}_{{\text{ex}}}}{\text{ = 0}}. As determined by Joule experimentally q =0, thus Δ=0\Delta {\text{U }} = 0.

Note: The process after which the system as well as the surroundings return to their original states is called a reversible process. Whereas the process in which on completion, permanent changes occur in the system as well as the surrounding is called an irreversible process.