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Question: The specific heat of an ideal gas depends on the temperature as \(A)\text{ }\dfrac{1}{T}\) \(B...

The specific heat of an ideal gas depends on the temperature as
A) 1TA)\text{ }\dfrac{1}{T}
B) TB)\text{ }T
C) TC)\text{ }\sqrt{T}
D) Does not depend on temperature

Explanation

Solution

The specific heat at constant volume is the ratio of the change in internal energy of a gas with change in its temperature and the specific heat at constant pressure can be related to the specific heat at constant volume. By using the formula for the internal energy of a gas and finding its variation with temperature we can solve this problem.

Formula used:
U=n2RTU=\dfrac{n}{2}RT
CV=dUdT{{C}_{V}}=\dfrac{dU}{dT}
Cp=CV+R{{C}_{p}}={{C}_{V}}+R

Complete step-by-step answer:
We will use the direct formula for the internal energy of a gas to find out its variation with temperature which will give us the value of the specific heat of the gas at constant volume.
The internal energy UU of one mole of a gas with nn degrees of freedom and at temperature TT is given by
U=n2RTU=\dfrac{n}{2}RT --(1)
Where R=8.314J.mol1K1R=8.314J.mo{{l}^{-1}}{{K}^{-1}} is the universal gas constant.
Now, the specific heat constant at constant volume CV{{C}_{V}} of an ideal gas is the ratio of the change in its internal energy UU to the change in temperature TT
CV=dUdT{{C}_{V}}=\dfrac{dU}{dT} --(2)
Now, putting (1) in (2), we get
CV=d(n2RT)dT=n2R{{C}_{V}}=\dfrac{d\left( \dfrac{n}{2}RT \right)}{dT}=\dfrac{n}{2}R --(3)
Also, the specific heat at constant pressure CP{{C}_{P}} of an ideal gas is related to the specific heat at constant volume CV{{C}_{V}} by
CP=CV+R{{C}_{P}}={{C}_{V}}+R --(4)
Now, putting (3) in (4), we get
CP=n2R+R=(n2+1)R{{C}_{P}}=\dfrac{n}{2}R+R=\left( \dfrac{n}{2}+1 \right)R --(5)
From (3) and (5), we can see that both CV{{C}_{V}} and CP{{C}_{P}} have no relation with the temperature TT of the gas and are not dependent on it.

So, the correct answer is “Option D”.

Note: The specific heat of an ideal gas at constant pressure is actually the ratio of the change in the enthalpy of the gas with the change in its temperature. Similar to the internal energy, the enthalpy of a gas also depends directly upon its temperature and therefore, similar to the process of finding out CV{{C}_{V}}, the term TT vanishes when we differentiate the enthalpy with the temperature. This is the exhaustive method of proving that none of the specific constants depends upon the temperature of the gas.