Components of a heat pump for supplying heated air to a dwelling are shown in the schematic below. At steady state, Refrigerant 134a enters the compressor at 6 °C, 3.2 bar and is compressed adiabatically to 75 °C, 14 bar. From the compressor, the refrigerant passes through the condenser, where it condenses to liquid at 28 °C, 14 bar. The refrigerant then expands through a throttling valve to 3.2 bar. The states of the refrigerant are shown on the accompanying T-s diagram. Return air from the dwelling enters the condenser at 20 °C, 1 bar with a volumetric flow rate of 0.42 m³/s and exits at 50 °C with a negligible change in pressure. Using the ideal gas model for the air and neglecting kinetic and potential energy effects. (a) determine the rates of entropy production, in kW/K, for control volumes enclosing the condenser, compressor, and expansion valve, respectively. (b) Discuss the sources of irreversibility in the components considered in part (a).

Elements Of Electromagnetics
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Components of a heat pump for supplying heated air to a dwelling are shown in the
schematic below. At steady state, Refrigerant 134a enters the compressor at 6 °C,
3.2 bar and is compressed adiabatically to 75 °C, 14 bar. From the compressor,
the refrigerant passes through the condenser, where it condenses to liquid at 28 °C,
14 bar. The refrigerant then expands through a throttling valve to 3.2 bar. The
states of the refrigerant are shown on the accompanying T-s diagram. Return air
from the dwelling enters the condenser at 20 °C, 1 bar with a volumetric flow rate
of 0.42 m³/s and exits at 50 °C with a negligible change in pressure. Using the
ideal gas model for the air and neglecting kinetic and potential energy effects, (a)
determine the rates of entropy production, in kW/K, for control volumes enclosing
the condenser, compressor, and expansion valve, respectively. (b) Discuss the
sources of irreversibility in the components considered in part (a).
Indoor return air
T5 = 20°C
P₁ = 1 bar
(AV)s = 0.42 m³/s
3
T3 = 28°C
P3= 14 bar
Expansion
4 Valve
P₁ = 3.2 bar
Condenser
www
wwwwwww
Evaporator
Supply air
To = 50°C
P6 = 1 bar
T₂ = 75°C
P₂ = 14 bar
-2
Outdoor air
1
T₁ = 6°C
P₁ = 3.2 bar
T
14 bar
*28°C
4
3.2 bar
75°C
6 °C
Transcribed Image Text:Components of a heat pump for supplying heated air to a dwelling are shown in the schematic below. At steady state, Refrigerant 134a enters the compressor at 6 °C, 3.2 bar and is compressed adiabatically to 75 °C, 14 bar. From the compressor, the refrigerant passes through the condenser, where it condenses to liquid at 28 °C, 14 bar. The refrigerant then expands through a throttling valve to 3.2 bar. The states of the refrigerant are shown on the accompanying T-s diagram. Return air from the dwelling enters the condenser at 20 °C, 1 bar with a volumetric flow rate of 0.42 m³/s and exits at 50 °C with a negligible change in pressure. Using the ideal gas model for the air and neglecting kinetic and potential energy effects, (a) determine the rates of entropy production, in kW/K, for control volumes enclosing the condenser, compressor, and expansion valve, respectively. (b) Discuss the sources of irreversibility in the components considered in part (a). Indoor return air T5 = 20°C P₁ = 1 bar (AV)s = 0.42 m³/s 3 T3 = 28°C P3= 14 bar Expansion 4 Valve P₁ = 3.2 bar Condenser www wwwwwww Evaporator Supply air To = 50°C P6 = 1 bar T₂ = 75°C P₂ = 14 bar -2 Outdoor air 1 T₁ = 6°C P₁ = 3.2 bar T 14 bar *28°C 4 3.2 bar 75°C 6 °C
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