(b) Let $V_{0},\ V_{t} =$ Volume of the metal ball at $0℃$ and $t℃$ respectively, $\rho_{0},\ p_{t} =$ density of alcohol at $0℃$ and $t℃$ respecitvely. Then
$W_{1} = W_{0} - V_{0}\rho_{0}g$
$W_{2} = W_{t} - V_{t}\rho_{t}g$
Where $V_{t} = V_{0}(1 + \gamma_{m}t)$ and $\rho_{t} = \frac{\rho_{0}}{(1 + \gamma_{a}t)}g = V_{0}\rho_{0}\frac{(1 + \gamma_{m}l)}{(1 + \gamma_{a}l)}$
As $\gamma_{m} < \gamma_{a}$, hence upthrust at $t℃$ is less than at $0℃$. It means upthrust has been decreased with increase in temperature. Due to which the $W_{2} > W_{1}$