For an ideal gas, the heat energy required to raise the temperature can be expressed using the equation:
\[
Q = n C_V \Delta T
\]
Where:
- \( n \) is the number of moles,
- \( C_V \) is the specific heat at constant volume,
- \( \Delta T \) is the change in temperature.
For a monatomic gas:
\[
Q_{\text{monatomic}} = n C_V \Delta T
\]
For a diatomic gas, the specific heat at constant volume \( C_V \) is higher. For monatomic gas \( C_V = \frac{3}{2} R \) and for diatomic gas \( C_V = \frac{5}{2} R \).
The heat energy required for 2 moles of a monatomic gas to go from 30°C to 40°C is \( Q \), so:
\[
Q = 2 \times \frac{3}{2} R \times 10 = 30 R
\]
For 4 moles of a diatomic gas, the temperature change is from 28°C to 33°C, so:
\[
Q_{\text{diatomic}} = 4 \times \frac{5}{2} R \times 5 = 50 R
\]
Since the heat energy for the monatomic gas was \( 30 R \), we find that:
\[
Q_{\text{diatomic}} = \frac{5Q}{3}
\]
Thus, the correct answer is \( \frac{5Q}{3} \).