Step 1: Identify the Process:
The expansion is at constant pressure, so it is an Isobaric Process.
Heat supplied at constant pressure is given by:
\[ Q_p = n C_p \Delta T \]
Using ideal gas equation $PV = nRT$, for isobaric process $P \Delta V = nR \Delta T \Rightarrow n \Delta T = \frac{P \Delta V}{R}$.
Substitute into heat equation:
\[ Q_p = C_p \left( \frac{P \Delta V}{R} \right) = \frac{C_p}{R} P \Delta V \]
Step 2: Specific Heat for Diatomic Gas:
For a diatomic gas, molar heat capacity at constant pressure is:
\[ C_p = \frac{7}{2} R \]
So,
\[ Q_p = \frac{\frac{7}{2} R}{R} P \Delta V = \frac{7}{2} P \Delta V \]
Step 3: Substitution and Calculation:
Pressure $P = 2$ atm $= 2 \times 10^5$ Pa.
Change in Volume $\Delta V = V_2 - V_1 = (37 - 18) \times 10^{-3} m^3 = 19 \times 10^{-3} m^3$.
\[ Q_p = \frac{7}{2} \times (2 \times 10^5) \times (19 \times 10^{-3}) \]
\[ Q_p = 7 \times 10^5 \times 19 \times 10^{-3} \]
\[ Q_p = 7 \times 19 \times 10^2 \]
\[ Q_p = 133 \times 100 = 13300 \, \text{J} \]
Step 4: Final Answer:
The heat supplied is 13300 J.