A vapor-compression refrigeration system with a capacity of 10 tons has Refrigerant 134a as the working fluid. Information and data for the cycle are provided in the Figure and in the table below. The compression process is internally reversible and can be modeled by pu1.01 = constant. The condenser is water-cooled, with water entering and leaving with a negligible change in pressure. Heat transfer from the outside of the condenser can be neglected. Determine a) the mass flow rate of refrigerant, in kg/s. b) the power input and the heat transfer rate for the compressor, each in kW. c) the coefficient of performance. d) the mass flow rate of the cooling water, in kg/s. e) the rates of entropy production in the condenser and expansion valve, in kW/K. f) the rates of exergy destruction in the condenser and expansion valve, each expressed as a percentage of the compressor power input. Let To = 20°C. State p (bar) 4 12 11.6 4 1 2 3 4 5 6 Ty=44°C Py 11.6 ba 3 E= va

Elements Of Electromagnetics
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A vapor-compression refrigeration system with a capacity of
10 tons has Refrigerant 134a as the working fluid. Information
and data for the cycle are provided in the Figure and in the
table below. The compression process is internally reversible
and can be modeled by pu1.01 = constant. The condenser is
water-cooled, with water entering and leaving with a
negligible change in pressure. Heat transfer from the outside
of the condenser can be neglected. Determine
a) the mass flow rate of refrigerant, in kg/s.
b) the power input and the heat transfer rate for the
compressor, each in kW.
c) the coefficient of performance.
d) the mass flow rate of the cooling water, in kg/s.
e) the rates of entropy production in the condenser and
expansion valve, in kW/K.
f)
the rates of exergy destruction in the condenser and
expansion valve, each expressed as a percentage of
the compressor power input. Let To = 20°C.
State p (bar)
1 4
12
11.6
2
3
4
4
5
6
.
T (°C)
15
54.88
44
8.93
20
30
Ty=44°C
Py = 11.6 bar
3
Cooling water
Ts=20°C T6=30°C
h (kJ/kg) s (kJ/kg-K)
0.9348
v (m²/kg)
0.05258
0.01772
0.0008847 112.22
0.01401
258.15
281.33
0.9341
0.4054
112.22
0.4179
83.96
0.2966
125.79
0.4369
immi
Condenser
Expansion
valve
6
Evaporator
4 bar
←m
P₂= 12 bar
Compressor
in = 10 tons
T₁-15°C
1
Transcribed Image Text:A vapor-compression refrigeration system with a capacity of 10 tons has Refrigerant 134a as the working fluid. Information and data for the cycle are provided in the Figure and in the table below. The compression process is internally reversible and can be modeled by pu1.01 = constant. The condenser is water-cooled, with water entering and leaving with a negligible change in pressure. Heat transfer from the outside of the condenser can be neglected. Determine a) the mass flow rate of refrigerant, in kg/s. b) the power input and the heat transfer rate for the compressor, each in kW. c) the coefficient of performance. d) the mass flow rate of the cooling water, in kg/s. e) the rates of entropy production in the condenser and expansion valve, in kW/K. f) the rates of exergy destruction in the condenser and expansion valve, each expressed as a percentage of the compressor power input. Let To = 20°C. State p (bar) 1 4 12 11.6 2 3 4 4 5 6 . T (°C) 15 54.88 44 8.93 20 30 Ty=44°C Py = 11.6 bar 3 Cooling water Ts=20°C T6=30°C h (kJ/kg) s (kJ/kg-K) 0.9348 v (m²/kg) 0.05258 0.01772 0.0008847 112.22 0.01401 258.15 281.33 0.9341 0.4054 112.22 0.4179 83.96 0.2966 125.79 0.4369 immi Condenser Expansion valve 6 Evaporator 4 bar ←m P₂= 12 bar Compressor in = 10 tons T₁-15°C 1
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