A monoatomic gas of $n$-moles is heated from temperature $T_1$ to $T_2$ under two different conditions. (i)…
The change in internal energy of the gas is
- More when heated at constant volume
- More when heated at constant pressure
- Same in both the cases
- Zero in both the cases
Solution
At constant volume, $(\Delta \mathrm{U})_1=\frac{\mathrm{nfR} \Delta \mathrm{~T}}{2}=\frac{3 \mathrm{nR}\left(\mathrm{~T}_2-\mathrm{T}_1\right)}{2}$
At constant pressure, $\begin{aligned} & (\Delta \mathrm{U})_2=\frac{\mathrm{nfR} \Delta \mathrm{~T}}{2}=\frac{3 \mathrm{nR}\left(\mathrm{~T}_2-\mathrm{T}_1\right)}{2} \\ & \therefore \quad(\Delta \mathrm{U})_1=(\Delta \mathrm{U})_2 \end{aligned}$
Asked in: AP EAMCET 2024 (21 May Shift 1)