According to the first law of thermodynamics for a process at constant pressure, the work done ($W$) is:
$$W = P\Delta V = nR\Delta T$$
The heat supplied at constant volume ($Q_v$) for the exact same temperature rise ($\Delta T$) is equal to the change in internal energy:
$$Q_v = nC_v\Delta T$$
For an ideal monoatomic gas, the molar heat capacity at constant volume is $C_v = \frac{3}{2}R$. Substituting this into the internal energy equation:
$$Q_v = n\left(\frac{3}{2}R\right)\Delta T = \frac{3}{2}(nR\Delta T)$$
Since $W = nR\Delta T$, we substitute it directly into our expression:
$$Q_v = \frac{3W}{2}$$
Final Answer:
The heat supplied at constant volume is $\frac{3W}{2}$, which corresponds to option (D).