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. 2022 Dec 7;148(3):1149–1162. doi: 10.1007/s10973-022-11721-w

Table 1.

Equations for exergy and exergy analysis [45]

Component Energy balance Exergy balance
com.

W˙com.=m˙1h2-h1

=m˙1h2,is-h1/ηcom.

χ˙D,com.=m˙1T0(s2-s1)
con. Q˙con.=m˙1(h2-h3) χ˙D,con.=m˙1T0s3-s2+Q˙con(1-T0/T3)
EV1 h3=h4 χ˙D,EV1=m˙5T0(s4-s3)
EV2 h5=h6 χ˙D,EV2=m˙5T0(s6-s5)
EV3 h9=h10 χ˙D,EV3=m˙9T0(s10-s9)
EV4 h12=h13 χ˙D,EV4=m˙12T0(s13-s12)
CE1

Q˙CE1=m˙7h7-h8

=m˙1h1-h17

χ˙D,CE1=m˙7h7-h8-T0s7-s8+m˙1[h17-h1-T0s17-s1]
CE2

Q˙CE2=m˙11h11-h12

=m˙16h16-h15

χ˙D,CE2=m˙11h11-h12-T0s11-s12+m˙15h15-h16-T0s15-s16
eva. Q˙eva.=m˙13h14-h13 χ˙D,eva.=T0[m˙s14-s13-Q˙eva.Tave+ΔT]

where Tave is the mathematic average temperature of the refrigerant at the inlet and outlet of the evaporator (K), and ΔT represents the temperature difference between the refrigerant and the cooled space, which is assumed to be 10 K