Skip to main content
. 2023 Mar 29;9(4):e15007. doi: 10.1016/j.heliyon.2023.e15007

Table 1.

Energy and exergy balance equations for the components of the ORC configurations.

Components Energy Balance Exergy Balance
Basic ORC
Pump W˙p=m˙wf(h2h1) Ex1˙+Wp˙=Ex2˙+EDp˙
Evaporator Q˙ev=m˙wf(h3h2) Ex2˙+Ex5˙=Ex3˙+Ex6˙+EDev˙
Expander W˙exp=m˙wf(h3h4) Ex˙3=Ex˙4+W˙exp+ED˙exp
Condenser Q˙c=m˙wf(h4h1) Ex˙4+Ex˙7=Ex˙1+Ex˙8+ED˙c
IHE-ORC
IHE Q˙IHE=m˙wf(h2h3)=m˙wf(h6h5)
Q˙IHE=εIHECmin(T2T5)
Ex˙2+Ex˙5=Ex˙3+Ex˙6+ED˙IHE
Pump W˙p=m˙wf(h2h1) Ex˙1+W˙p=Ex˙2+ED˙p
Evaporator Q˙ev=m˙wf(h4h3) Ex3˙+Ex7˙=Ex4˙+Ex8˙+EDev˙
Expander W˙exp=m˙wf(h4h5) Ex˙4=Ex˙5+W˙exp+ED˙exp
Condenser Q˙c=m˙wf(h6h1) Ex˙6+Ex˙9=Ex˙1+Ex˙10+ED˙c
FFH-ORC
FFH m˙wfXh6+m˙wf(1X)h2=m˙wfh3 Ex2˙+Ex6˙=Ex3˙+ED˙FFH
Pump-I W˙pI=m˙wf(1X)(h2h1) Ex1˙+W˙pI=Ex2˙+ED˙pI
Pump-II W˙pII=m˙wf(h4h3) Ex3˙+W˙pII=Ex4˙+ED˙pII
Evaporator Q˙b=m˙wf(h5h4) Ex4˙+Ex8˙=Ex5˙+Ex9˙+ED˙ev
Expander W˙t=m˙wfX(h5h6)+m˙wf(1X)(h5h7) Ex˙5=Ex˙6+Ex˙7+W˙t+ED˙exp
Condenser Q˙y=m˙wf(1X)(h1h7) Ex˙7+Ex˙10=Ex˙1+Ex˙11+ED˙c
IHE–FFH–ORC
Pump-I W˙pI=m˙lpe(h2h1) Ex˙1+W˙p1=Ex˙2+EY˙pI
IHE Q˙IHE=m˙lpe(h3h2)=m˙lpe(h10h11)
Q˙IHE=εIHECmin(T2T10)
Ex˙2+Ex˙10=Ex˙3+Ex˙11+ED˙IHE
FFH Q˙FFH=m˙wfh4=m˙lpeh9+m˙lpeh3 Ex˙3+Ex˙9=Ex˙4+ED˙FFH
Pump-II W˙pII=m˙ORÇ(h5h4) Ex˙4+W˙p2=Ex˙5+ED˙pII
Evaporator Q˙b=m˙wf(h6h5)=m˙12(h12h13) Ex˙5+Ex˙12=Ex˙6+Ex˙13+ED˙ev
High-pressure expander W˙hpe=m˙wf(h6h7) Ex˙6=Ex˙7+W˙hpe+ED˙hpe
Low-pressure expander W˙lpe=m˙lpe(h8h10) Ex˙8=Ex˙10+W˙lpe+ED˙lpe
Condenser Q˙c=m˙lpe(h11h1)=m˙14(h15h14) Ex˙11+Ex˙14=Ex˙1+Ex˙15+ED˙c