- For an ideal Brayton cycle, the thermal efficiency \( \eta \) is given by:
\[
\eta = 1 - \left( \frac{T_1}{T_2} \right)^{\gamma - 1}
\]
where \( T_1 \) is the temperature at the compressor inlet, and \( T_2 \) is the temperature at the turbine inlet.
- Given that \( \eta = 50% = 0.5 \), \( T_1 = 300 \, \text{K} \), and \( \gamma = 1.4 \), we can solve for \( T_2 \):
\[
0.5 = 1 - \left( \frac{300}{T_2} \right)^{1.4 - 1}
\]
\[
0.5 = 1 - \left( \frac{300}{T_2} \right)^{0.4}
\]
\[
\left( \frac{300}{T_2} \right)^{0.4} = 0.5
\]
Taking the reciprocal and raising both sides to the power of \( 2.5 \), we find:
\[
T_2 = 1595.00 \, \text{K} \text{ to } 1605.00 \, \text{K}
\]