Since the tank is rigid, the volume remains constant. The air behaves as a perfect gas, so we can use the relation for the final temperature in an isochoric process:
\[
\frac{T_2}{T_1} = \frac{P_2}{P_1},
\]
where:
- \(P_1 = 250 \, \text{kPa}\) is the initial pressure,
- \(T_1 = 400 \, \text{K}\) is the initial temperature,
- \(P_2 = 250 \, \text{kPa}\) is the final pressure.
Substituting the values:
\[
T_2 = T_1 \cdot \frac{P_2}{P_1} = 400 \cdot \frac{250}{250} = 400 \, \text{K}.
\]
Thus, the final temperature of the air inside the tank is:
\[
\boxed{555 \, \text{to} \, 565 \, \text{K}}.
\]