A refrigerator operates on the reversed Carnot cycle and uses water as the working
fluid. At the beginning of the isothermal expansion, the steam has an absolute
pressure of 1kPa and a quality of 7%; at the end of the isothermal expansion, the
steam is dry and saturated. At the end of heat rejection process the water is saturated
liquid. Firstly: Sketch the T‐s and P‐v diagrams for the cycle, and secondly: for one kg
of water, calculate: a) The steam pressure at beginning of the heat rejection process,
b) the net work per cycle, c) the COP of the cycle in two conditions: 1‐refrigeration
and 2‐heat pump
The performance of refrigerators and heat pumps is expressed in terms of coefficient of performance (COP):
"COP_R = \\frac{Q_L}{W_{in}}"
"COP_{HP} = \\frac{Q_H}{W_{in}}"
Reversed Carnot Cycle:
An internally, reversible, constant pressure heat rejection
"Q_H = h_2 \u2212 h_3" ..."h_3 =h4"
An internally, reversible, constant pressure heat interaction
"Q_L = h_1\u2212 h_4"
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