Since the container is perfectly insulated and rigid, the process is:
- Adiabatic (\(Q = 0\))
- Constant volume (\(V = \text{constant}\))
The first law for a closed system gives:
\[
\Delta U = Q + W = 0 + 225\ \text{kJ} = 225\ \text{kJ}
\]
For an ideal gas, the change in internal energy is:
\[
\Delta U = m c_v \Delta T
\]
Given:
\[
m = 1\ \text{kg}, \qquad c_v = 750\ \text{J/kg·K} = 0.75\ \text{kJ/kg·K}
\]
So,
\[
225 = 1 \times 0.75 \times \Delta T
\]
\[
\Delta T = \frac{225}{0.75} = 300\ \text{K}
\]
Initial temperature:
\[
T_1 = 300\ \text{K}
\]
Final temperature:
\[
T_2 = T_1 + \Delta T = 300 + 300 = 600\ \text{K}
\]
Since volume is constant, pressure is proportional to temperature:
\[
\frac{P_2}{P_1} = \frac{T_2}{T_1}
\]
\[
P_2 = 1\ \text{bar} \times \frac{600}{300} = 2\ \text{bar}
\]
Thus, the final pressure of the gas is \(2\) bar.