b
(b)
At constant pressure heat absorbed $=\Delta Q=n C_P \Delta T \quad \dots (1)$
At constant volume heat absorbed $=\Delta U=n C_v \Delta T \quad \dots (2)$
Dividing $(1)$ by $(2)$,
$\frac{\Delta Q}{\Delta U}=\frac{C_P}{C_V}=\gamma=1.4 \Rightarrow \frac{105}{\Delta U}=1.4$
$\therefore \Delta U_V=75 \,cal$