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REFRIGERATION CYCLE
REFRIGERATORS AND HEAT PUMPS The objective of a refrigerator is to remove heat ( Q L ) from the cold medium; the objective of a heat pump is to supply heat ( Q H ) to a warm medium. The transfer of heat from a low-temperature region to a high-temperature one requires special devices called  refrigerators . Refrigerators and heat pumps are essentially the same devices; they differ in their objectives only. for fixed values of  Q L  and  Q H
THE IDEAL VAPOR-COMPRESSION REFRIGERATION CYCLE The  vapor-compression refrigeration cycle  is the ideal model for refrigeration systems.  Unlike the reversed Carnot cycle, the refrigerant is vaporized completely before it is compressed and the turbine is replaced with a throttling device.  Schematic and  T - s  diagram for the ideal vapor-compression refrigeration cycle. This is the most widely used cycle for refrigerators, A-C systems, and heat pumps.
The  P - h  diagram of an ideal vapor-compression refrigeration cycle. The ideal vapor-compression refrigeration cycle involves an irreversible (throttling) process to make it a more realistic model for the actual systems.  Replacing the expansion valve by a turbine is not practical since the added benefits cannot justify the added cost and complexity. Steady-flow energy balance
ACTUAL VAPOR-COMPRESSION REFRIGERATION CYCLE Schematic and  T - s  diagram for the actual vapor-compression refrigeration cycle. An actual vapor-compression refrigeration cycle differs from the ideal one in several ways, owing mostly to the irreversibilities that occur in various components, mainly due to  fluid friction  (causes pressure drops) and  heat transfer to or from the surroundings .  The COP decreases as a result of irreversibilities. DIFFERENCES Non-isentropic compression Superheated vapor at evaporator exit Subcooled liquid at condenser exit Pressure drops in condenser and evaporator
SELECTING THE RIGHT REFRIGERANT ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
HEAT PUMP SYSTEMS A heat pump can be used to heat a space in winter and to cool it in summer. The most common energy source for heat pumps is atmospheric air (air-to- air systems).  Water-source systems usually use well water and ground-source (geothermal) heat pumps use earth as the energy source. They typically have higher COPs but are more complex and more expensive to install. Both the capacity and the efficiency of a heat pump fall significantly at low temperatures. Therefore, most air-source heat pumps require a supplementary heating system such as electric resistance heaters or a gas furnace. Heat pumps are most competitive in areas that have a large cooling load during the cooling season and a relatively small heating load during the heating season. In these areas, the heat pump can meet the entire cooling and heating needs.

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Refrigeration cycle

  • 2. REFRIGERATORS AND HEAT PUMPS The objective of a refrigerator is to remove heat ( Q L ) from the cold medium; the objective of a heat pump is to supply heat ( Q H ) to a warm medium. The transfer of heat from a low-temperature region to a high-temperature one requires special devices called refrigerators . Refrigerators and heat pumps are essentially the same devices; they differ in their objectives only. for fixed values of Q L and Q H
  • 3. THE IDEAL VAPOR-COMPRESSION REFRIGERATION CYCLE The vapor-compression refrigeration cycle is the ideal model for refrigeration systems. Unlike the reversed Carnot cycle, the refrigerant is vaporized completely before it is compressed and the turbine is replaced with a throttling device. Schematic and T - s diagram for the ideal vapor-compression refrigeration cycle. This is the most widely used cycle for refrigerators, A-C systems, and heat pumps.
  • 4. The P - h diagram of an ideal vapor-compression refrigeration cycle. The ideal vapor-compression refrigeration cycle involves an irreversible (throttling) process to make it a more realistic model for the actual systems. Replacing the expansion valve by a turbine is not practical since the added benefits cannot justify the added cost and complexity. Steady-flow energy balance
  • 5. ACTUAL VAPOR-COMPRESSION REFRIGERATION CYCLE Schematic and T - s diagram for the actual vapor-compression refrigeration cycle. An actual vapor-compression refrigeration cycle differs from the ideal one in several ways, owing mostly to the irreversibilities that occur in various components, mainly due to fluid friction (causes pressure drops) and heat transfer to or from the surroundings . The COP decreases as a result of irreversibilities. DIFFERENCES Non-isentropic compression Superheated vapor at evaporator exit Subcooled liquid at condenser exit Pressure drops in condenser and evaporator
  • 6.
  • 7. HEAT PUMP SYSTEMS A heat pump can be used to heat a space in winter and to cool it in summer. The most common energy source for heat pumps is atmospheric air (air-to- air systems). Water-source systems usually use well water and ground-source (geothermal) heat pumps use earth as the energy source. They typically have higher COPs but are more complex and more expensive to install. Both the capacity and the efficiency of a heat pump fall significantly at low temperatures. Therefore, most air-source heat pumps require a supplementary heating system such as electric resistance heaters or a gas furnace. Heat pumps are most competitive in areas that have a large cooling load during the cooling season and a relatively small heating load during the heating season. In these areas, the heat pump can meet the entire cooling and heating needs.