(d) During adiabatic expansion
$TV^{\gamma - 1} =$ constant of $T_{2}V_{2}^{\gamma - 1} = T_{1}V_{1}^{\gamma - 1}$
$\frac{T_{1}}{T_{2}} = \left( \frac{V_{2}}{V_{1}} \right)^{\gamma - 1}$
For monoatomic gas, $\gamma = 5/3$
$\frac{T_{1}}{T_{2}} = \left( \frac{AL_{2}}{AL_{1}} \right)^{5/3 - 1} = \left( \frac{L_{2}}{L_{1}} \right)^{2/3}$