Step 1: Enthalpy of an ideal gas.
For an ideal gas the enthalpy depends only on temperature, so pressure does not enter.
\[ \Delta H = \int_{T_1}^{T_2} C_p \, dT \]
Step 2: Set the temperatures.
\[ T_1 = 300 \text{ K}, \quad T_2 = 600 \text{ K} \]
Step 3: Integrate $C_p = a + bT$ and put in values.
\[ \Delta H = a(T_2-T_1) + \frac{b}{2}(T_2^2 - T_1^2) = 6270 + 5670 = 11940 \text{ J} \]
Step 4: Answer.
\[ \boxed{11.94 \, \text{kJ}} \]