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A gas-turbine power plant operates on a simple Brayton cycle with air as the working fluid. The air enters the turbine at 800 kPa800 \mathrm{~kPa} and 1100 K1100 \mathrm{~K} and leaves at 100 kPa100 \mathrm{~kPa} and 670 K670 \mathrm{~K}. Heat is rejected to the surroundings at a rate of 6700 kW6700 \mathrm{~kW}, and air flows through the cycle at a rate of 18 kg/s18 \mathrm{~kg} / \mathrm{s}. For what compressor efficiency will the gas-turbine power plant produce zero net work?

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Zero net work is produced when the difference between the rate work between the inlet and outlet energies is zero.

W˙net, out =W˙C, in W˙T,out0=W˙C, in W˙T,outW˙C, in =W˙T,out\begin{gather*} \dot{W}_{\mathrm{net}, \text { out }}= \dot{W}_{\mathrm{C}, \text { in }}-\dot{W}_{\mathrm{T}, \mathrm{out}} \\ 0 = \dot{W}_{\mathrm{C}, \text { in }}-\dot{W}_{\mathrm{T}, \mathrm{out}}\\ \dot{W}_{\mathrm{C}, \text { in }} = \dot{W}_{\mathrm{T}, \mathrm{out}} \end{gather*}

Where W˙C, in \dot{W}_{\mathrm{C}, \text { in }} is

W˙C,in=m˙(h2sh1)/ηC\dot{W}_{\mathrm{C}, \mathrm{in}}=\dot{m}\left(h_{2 s}-h_{1}\right) / \eta_{C}

and W˙T,out\dot{W}_{\mathrm{T}, \mathrm{out}} is

W˙T,out=m˙(h3h4)\dot{W}_{\mathrm{T}, \mathrm{out}}= \dot{m}\left(h_{3}-h_{4}\right)

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