Step 1: Relation for enthalpy change.
For an ideal gas, enthalpy depends only on temperature
\[
\Delta H = \int_{T_1}^{T_2} C_p \, dT
\]
Step 2: Substitute given heat capacity expression.
\[
C_p = a + bT
\]
Thus,
\[
\Delta H = \int_{T_1}^{T_2} (a + bT)\, dT
\]
Step 3: Perform integration.
\[
\Delta H = a(T_2 - T_1) + \frac{b}{2}(T_2^2 - T_1^2)
\]
Step 4: Convert temperatures to Kelvin.
\[
T_1 = 27 + 273 = 300 \, K, \quad T_2 = 327 + 273 = 600 \, K
\]
Step 5: Substitute values.
\[
\Delta H = 20.9(600 - 300) + \frac{0.042}{2}(600^2 - 300^2)
\]
\[
= 20.9 \times 300 + 0.021 (360000 - 90000)
\]
\[
= 6270 + 0.021 \times 270000
\]
\[
= 6270 + 5670 = 11940 \, J
\]
Step 6: Convert to kJ.
\[
\Delta H = 11.94 \, \text{kJ}
\]
Step 7: Conclusion.
\[
\boxed{11.94 \, \text{kJ}}
\]