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8/10/2019 Chpt09SG.vapour Power Cycle
1/24
Chapter 9-1
Chapter 9: Vapor and Combined Power Cycles
We consider power cycles where the working fluid undergoes a phase
change. The best example of this cycle is the steam power cycle where
water (steam) is the working fluid.
Carnot Vapor Cycle
The heat engine may be composed of the following components.
Steam Power Cycle
Turbine
2
Pump
Condenser
Wturb
1
3
QI n
Qout
4
Boiler
Wp
Heat source
TH> TL
QH
QL
Heat Sink
TL
Heat
engineWnet
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Chapter 9-2
The working fluid, steam (water), undergoes a thermodynamic cycle from
1-2-3-4-1. The cycle is shown on the following T-sdiagram.
The thermal efficiency of this cycle is given as
th Carnotnet
in
out
in
L
H
W
Q
Q
Q
T
T
, = =
=
1
1
Note the effect of THand TLon th, Carnot.
The larger the THthe larger the th, Carnot The smaller the TLthe larger the th, Carnot
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
0
100
200
300
400
500
600
700700
s [kJ/kg-K]
T
[C]
6000 kPa
100 kPa
Carnot Vapor Cycle Using Steam
1
2 3
4
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Chapter 9-3
To increase the thermal efficiency in any power cycle, we try to increase the
maximum temperature at which heat is added.
Reasons why the Carnot cycle is not used:
Pumping process 1-2 requires the pumping of a mixture of saturatedliquid and saturated vapor at state 1 and the delivery of a saturated liquid
at state 2.
To superheat the steam to take advantage of a higher temperature,
elaborate controls are required to keep THconstant while the steam
expands and does work.
To resolve the difficulties associated with the Carnot cycle, the Rankine
cycle was devised.
Rankine Cycle
The simple Rankine cycle has the same component layout as the Carnot
cycle shown above. The simple Rankine cycle continues the condensation
process 4-1 until the saturated liquid line is reached.
Ideal Rankine Cycle Processes
Process Description1-2 Isentropic compression in pump
2-3 Constant pressure heat addition in boiler
3-4 Isentropic expansion in turbine
4-1 Constant pressure heat rejection in condenser
The T-sdiagram for the Rankine cycle is given below. Locate the processes
for heat transfer and work on the diagram.
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Chapter 9-4
Example 9-1
Compute the thermal efficiency of an ideal Rankine cycle for which steam
leaves the boiler as superheated vapor at 6 MPa, 350oC, and is condensed at
10 kPa.
We use the power system and T-sdiagram shown above.
P2=P3= 6 MPa = 6000 kPa
T3= 350oC
P1=P4= 10 kPa
Pump
The pump work is obtained from the conservation of mass and energy for
steady-flow but neglecting potential and kinetic energy changes and
assuming the pump is adiabatic and reversible.
( )
m m m
m h W m h
W m h h
pump
pump
1 2
1 1 2 2
2 1
= =
+ =
=
0 2 4 6 8 10 1212
0
100
200
300
400
500
s [kJ/kg-K]
T[C]
6000 kPa
10 kPa
Rankine Vapor Power Cycle
1
2
3
4
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8/10/2019 Chpt09SG.vapour Power Cycle
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Chapter 9-6
w v P P
m
kg kPa
kJ
m kPa
kJ
kg
pump =
=
=
1 2 1
3
30 00101 6000 10
6 05
( )
. ( )
.
Now, h2is found from
h w h
kJ
kg
kJ
kg
kJ
kg
pump2 1
6 05 19183
197 88
= +
= +
=
. .
.
Boiler
To find the heat supplied in the boiler, we apply the steady-flow
conservation of mass and energy to the boiler. If we neglect the potentialand kinetic energies, and note that no work is done on the steam in the boiler,
then
( )
m m m
m h Q m h
Q m h h
in
in
2 3
2 2 3 3
3 2
= =
+ =
=
We find the properties at state 3 from the superheated tables as
P kPa
T C
h kJ
kg
s kJ
kg K
o
3
3
3
3
6000
350
30430
6335
=
=
UVW
=
=
R
S||
T||
.
.
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Chapter 9-7
The heat transfer per unit mass is
q
Q
m h h
kJ
kg
kJ
kg
in
in
= =
=
=
( . . )
.
3 2
30403 19788
28452
Turbine
The turbine work is obtained from the application of the conservation of
mass and energy for steady flow. We assume the process is adiabatic and
reversible and neglect changes in kinetic and potential energies.
( )
m m m
m h W m h
W m h h
turb
turb
3 4
3 3 4 4
3 4
= =
= +
=
We find the properties at state 4 from the steam tables by notings4=s3and
asking three questions.
at P kPa s kJ
kg Ks
kJ
kg K
is s s
is s s s
is s s
f g
f
f g
g
4
4
4
4
10 0 6483 81502= =
=