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ME354

Thermodynamics 2 Name:

Quiz #3 - T02: ID #:

Problem: A commercial refrigerator with refrigerant- 134a as the working fluid is used to keep the
refrigerated space at −30 ◦ C by rejecting its waste heat to cooling water that enters the condenser at
18 ◦ C at a rate of 0.25 kg/s and leaves at 26 ◦ C. The refrigerant enters the condenser at 1.2 M P a
and 65 ◦ C and leaves at 42 ◦ C. The inlet state of the compressor is 60 kP a and −34 ◦ C and the
compressor is estimated to gain a net heat of 450 W from the surroundings.

Determine:
(a) the quality of the refrigerant at the
evaporator inlet,
(b) the refrigeration load, [kW ]
(c) the COP of the refrigerator,

Assumptions

1. SS − SF
2. KE = P E → 0
3. properties are constant

Part a)

state T P h s comment
(◦ C) (kP a) (kJ/kg) (kJ/kg · K)

1 -34 60 230.05
2 65 1200 295.13 Table A-13 1 mark
3 42 1200 111.37
4 60 111.37 h4 = h3

State 1
We first notice from Table A-12, our temperature at 1 is above the saturation temperature at 60 kP a,
therefore state point 1 is in the superheated region. From Table A-13 at P1 = 0.06 M P a we need to
interpolate.
1 mark
h1 = 0.826(227.79) + 0.174(240.76) = 230.05 kJ/kg
State 3
We notice from Table A-12, our temperature at 3 is below the saturation temperature 1200 kP a, there-
fore state point 3 is in the sub cooled region. From Table A-11 we can determine

h3 = hf (T ) + vf (T )[P − Psat (T )] = 111.26 + 0.0008786(1200 − 1072.8) = 111.37 kJ/kg


1 mark

State 4
State point 4 is under the dome with pressure and entropy known, therefore from Table A-12
111.37 − 3.841 1 mark
x4 = = 0.4802 ⇐
227.79 − 3.841

Part b)
The mass flow rate of the refrigerant can be determined by applying a 1st law energy balance across the
condenser.
The water properties can be obtained by using a saturated liquid at the given temperature

hw1 = hf @18 ◦ C = 75.54 kJ/kg


1 mark
hw2 = hf @26 ◦ C = 109.01 kJ/kg

ṁR (h2 − h3 ) = ṁw (hw2 − hw1 )

ṁR (295.13 − 111.37) kJ/kg = (0.25 kg/s)(109.01 − 75.54) kJ/kg


2 marks
ṁR = 0.0455 kg/s

The refrigeration load is given as


1 mark
Q̇L = ṁR (h1 − h4 ) = (0.0455 kg/s)(230.03 − 111.37) kJ/kg = 5.39 kW ⇐

Note: Cengel calculates the refrigeration load as Q̇H − Ẇin. This includes the Qin of the compressor
in addition to the enthalpy of the evaporator and provides a Q̇L = 5.85 kW . While not technically the
cooling load, I will accept this answer.

Part c)
The specific work into the compressor can be determined as

Q̇in 0.450 kJ/s


win = (h2 − h1 ) − = (295.13 − 230.03) kJ/kg − = 55.21 kJ/kg
ṁR 0.0455 kg/s
1 mark
The COP is determined as
q̇L h1 − h4 (230.03 − 111.37) kJ/kg
COP = = = = 2.14 ⇐ 1 mark
ẇin win 55.21 kJ/kg
Note: I have calculated qL as the actual heat gain across the evaporator. Cengel calculates qL =
qH − win. Since win is biased by the heat gain at the compressor this leads to a COP = 2.33. I will
accept this as a valid solution although, the COP should only be based on the actual energy gain which is
h1 − h4 .

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