In a thermodynamic process on an ideal monatomic gas, the infinitesimal heat absorbed by the gas is given by T Δ X \Delta X Δ X , where T is temperature of the system and Δ X \Delta X Δ X is the infinitesimal change in a thermodynamic quantity X of the system. For a mole of monatomic ideal gas X= 3 2 \frac32 2 3 R ln [ T T A ] \ln\left\lbrack\frac{T}{T_{A}}\right\rbrack ln [ T A T ] + [ V V A ] \left\lbrack\frac{V}{V_{A}}\right\rbrack [ V A V ] R ln \ln ln RIn. Here, R is gas constant, V is volume of gas, Ta and Va are constants.Match the quantities in List-I with the expressions in List-II.
Physics · Thermodynamics
In a thermodynamic process on an ideal monatomic gas, the infinitesimal heat absorbed by the gas is given by TΔX, where T is temperature of the system and ΔX is the infinitesimal change in a thermodynamic quantity X of the system. For a mole of monatomic ideal gas X=23Rln[TAT]+[VAV]Rln
RIn. Here, R is gas constant, V is volume of gas, Ta and Va are constants.Match the quantities in List-I with the expressions in List-II.

List 1
I. Work done in 1→2→3
II. Change in internal energy in 1→2→3
III. Heat absorbed in 1→2→3
IV. Heat absorbed in 1→2
V.
VI.
List 2
(P) (RT₀/3)ln 2
(Q) RT₀/3
(R) RT₀
(S) 4RT₀/3
(T) (RT₀/3)(3+ln 2)
(U) 5RT₀/6
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