To ensure incompressibility (Mach number \( M \leq 0.3 \)), we use the relation between area and Mach number in an isothermal flow:
\[
\frac{A}{A^*} = \frac{1}{M} \left( \frac{2}{\gamma + 1} \left( 1 + \frac{\gamma - 1}{2} M^2 \right) \right)^{\frac{\gamma + 1}{2(\gamma - 1)}}.
\]
where
- \( \gamma = 1.4 \) (ratio of specific heats),
- \( M = 0.3 \),
- \( A = 1 \, \text{m}^2 \) (at section P).
From the equation for incompressible flow:
\[
M = \frac{v}{a}, \quad a = \sqrt{\gamma R T}.
\]
We calculate the necessary values and find the required area at section Q:
\[
A_Q \approx 0.14 \, \text{m}^2.
\]
Thus, the minimum area required at section Q is approximately \( 0.14 \, \text{m}^2 \).