Carnot Vapour compression Refrigeration cycle

(a) Schematic representation (b) T-s diagram

(a) Schematic representation (b) T-s diagram
Processes: -
1-2: Isentropic compression from state 1 (wet vapour) to state 2 (saturated vapour)
2-3: Heat rejection (QH) in the condenser
3-4: Isentropic expansion from state 3 (saturated liquid)
4-1: Heat absorption ( QL) in the evaporator
The COP of the refrigerator,
1-2: Isentropic compression from state 1 (wet vapour) to state 2 (saturated vapour)
2-3: Heat rejection (QH) in the condenser
3-4: Isentropic expansion from state 3 (saturated liquid)
4-1: Heat absorption ( QL) in the evaporator
The COP of the refrigerator,
Practical Vapour compression refrigeration cycle

(Ws)compressor=h2-h1
QH=h2-h3
h3=h4
and QL=h1-h4
The COP of the refrigerator is given by,

In some cases the refrigerant leaves the evaporator as either saturated vapour or superheated vapour.

Gas refrigeration cycle

(a) Schematic diagram (b) T-s diagram
The simplest gas refrigeration cycle is the reversed Brayton cycle
Processes: -
1-2: isentropic compression for state 1 (atmospheric air) to state 2
2-3: energy exchange with the surrounding, air is cooled
3-4: isentropic expansion to state 4
Work obtained during the expansion process can be used to run the compressor
Work done on the compressor,
Processes: -
1-2: isentropic compression for state 1 (atmospheric air) to state 2
2-3: energy exchange with the surrounding, air is cooled
3-4: isentropic expansion to state 4
Work obtained during the expansion process can be used to run the compressor
Work done on the compressor,


The COP of this refrigeration system is given by,

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