For an adiabatic flow of an ideal gas, the stagnation temperature is given by:
\[
T_0 = T + \frac{V^2}{2c_p},
\]
where:
- \(T = 330 \, \text{K}\) is the temperature,
- \(V = 300 \, \text{m/s}\) is the velocity,
- \(c_p = 1.005 \, \text{kJ/kg.K} = 1005 \, \text{J/kg.K}\) is the specific heat.
Substituting the values:
\[
T_0 = 330 + \frac{300^2}{2 \times 1005} = 330 + \frac{90000}{2010} \approx 330 + 44.8 = 374.8 \, \text{K}.
\]
Thus, the stagnation temperature is:
\[
\boxed{373.00 \, \text{to} \, 377.00 \, \text{K}}.
\]