An Ideal Gas Refrigeration Cycle is a Brayton Cycle run in reverse as shown in the schematic below. In this system, the Compressor Ratio (P2/P1) is 3, and air enters the compressor at −23°C (Stream 1) and leaves Heat Exchanger 1 at 25°C (Stream 3). Solve this problem by assuming that air behaves as an ideal gas with constant heat capacity as given below): a) Draw the cycle on P-V and T-S diagrams. Also show for which process QH, Qc, Win, and Wout cross the system boundary. You do not need to give numerical values for the pressures and temperatures, but show relative changes correctly. b) Find the maximum temperature of the cycle in °C. c) Find the Coefficient of Performance (COPRef) for the cycle. Data of air: Cp = 1.005 kJ/kg R = 0.287 kJ/kg∙K Cycle Steps: 1-2: Isentropic Compression 2-3: Constant Pressure Heat Rejection 3-4: Isentropic Expansion 4-1: Constant Pressure Heat Addition
An Ideal Gas Refrigeration Cycle is a Brayton Cycle run in reverse as shown in the
schematic below. In this system, the Compressor Ratio (P2/P1) is 3, and air enters the compressor at
−23°C (Stream 1) and leaves Heat Exchanger 1 at 25°C (Stream 3). Solve this problem by assuming
that air behaves as an ideal gas with constant heat capacity as given below):
a) Draw the cycle on P-V and T-S diagrams. Also show for which process QH, Qc, Win, and Wout cross the
system boundary. You do not need to give numerical values for the pressures and temperatures, but
show relative changes correctly.
b) Find the maximum temperature of the cycle in °C.
c) Find the Coefficient of Performance (COPRef) for the cycle.
Data of air:
Cp = 1.005 kJ/kg
R = 0.287 kJ/kg∙K
Cycle Steps:
1-2: Isentropic Compression
2-3: Constant Pressure Heat Rejection
3-4: Isentropic Expansion
4-1: Constant Pressure Heat Addition
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