For an adiabatic process,
\[
\boxed{Q=0}
\]
and
\[
\boxed{W=-\Delta U.}
\]
For a monoatomic ideal gas,
\[
\boxed{C_V=\frac{3R}{2}}
\]
Hence,
\[
\boxed{W=-\frac32nR\Delta T.}
\]
Always calculate the temperature difference in Kelvin. Since temperature intervals are the same in Celsius and Kelvin,
\[
\boxed{\Delta T(^\circ C)=\Delta T(K).}
\]