For an adiabatic process, $T V^{\gamma - 1} = {constant}$, where $\gamma$ is the ratio of specific heats ($C_p/C_v$).
Given $T \propto \frac{1}{\sqrt{V}}$, rewrite as $T = k V^{-1/2}$.
So, $T V^{1/2} = {constant}$. Comparing with $T V^{\gamma - 1} = {constant}$, we get $\gamma - 1 = \frac{1}{2}$.
Thus, $\gamma = 1 + \frac{1}{2} = 1.5$.