$T{V^{\gamma - 1}}=constant$ or ${T_1}{V_1}^{\gamma - 1} = {T_2}{V_2}^{\gamma - 1}$
For monoatomic gas $\gamma = \frac{5}{3}$
$\left( {300} \right){V^{2/3}} = {T_2}{\left( {2V} \right)^{2/3}} \Rightarrow {T_2} = \frac{{300}}{{{{\left( 2 \right)}^{2/3}}}}$
${T_2} = 189\,K\,\left( {final\,temperature} \right)$
Change in internal energy $\Delta U = n\frac{f}{2}R\,\Delta T$
$ = 2\left( {\frac{3}{2}} \right)\left( {\frac{{25}}{3}} \right)\left( { - 111} \right) = - 2.7\,kJ$




