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VAPOUR POWER
CYCLES
RANKINE CYCLE
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
1
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
2
THEOROTICAL CYCLE ON WHICH STEAM
TURBINE WORKS
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
3
SCHEMATIC DIAGRAM
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
4
PROCESSES
Process 1-2 : Reversible adiabatic expansion in the turbine (or steam engine).
Process 2-3 : Constant-pressure transfer of heat in the condenser.
Process 3-4 : Reversible adiabatic pumping process in the feed pump.
Process 4-1 : Constant-pressure transfer of heat in the boiler.
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
5
4-1 BOILER
STATE OF FLUID
4-WATER
1-STEAM
4
4
1
1
1
1
f
f
h
h
Q
h
Q
h
boiler
for
SFEE




III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
6
1-2 TURBINE
STATE OF FLUID
1-STEAM
2-STEAM
Dryness
reduces
during
expansion
2
1
2
1
h
h
W
W
h
h
Turbine
for
SFEE
T
T




III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
7
2-3 CONDENSOR
STATE OF FLUID
2-STEAM
3-WATER
3
3
2
2
2
2
f
f
h
h
Q
h
Q
h
Condensor
for
SFEE




III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
8
3-4 PUMP
STATE OF FLUID
3-WATER
4-WATER
3
4
4
3
f
f
P
P
f
f
h
h
W
W
h
h
Pump
for
SFEE




III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
9
EFFICIENCY
1
1 Q
W
W
Q
W
cycle
Rankine
of
Efficiency
P
T
NET
RANKINE




)
(
)
(
)
(
4
3
4
1
2
1
1 f
f
f
NET
RANKINE
h
h
h
h
h
h
Q
W
cycle
Rankine
of
Efficiency







)
(
)
(
)
( 3
4
3
4 2
1 f
f
f
f h
h
h
h
as
h
h
Neglect 



)
(
)
(
4
1
2
1
1 f
NET
RANKINE
h
h
h
h
Q
W
cycle
Rankine
of
Efficiency





III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
10
METHODS OF IMPROVING RANKINE EFFICIENCY
Increasing
boiler
pressure
•. It has been
observed that by
increasing the boiler
pressure (other
factors remaining the
same) the cycle
tends to rise and
reaches a maximum
value at a boiler
pressure of about
166 bar
Superheatin
g
•. All other factors
remaining the same,
if the steam is
superheated before
allowing it to expand
the Rankine cycle
efficiency may be
increased. The use of
superheated steam
also ensures longer
turbine blade life
because of the
absence of erosion
from high velocity
water particles that
are suspended in wet
vapour.
Reducing
condenser
pressure.
•The thermal
efficiency of the
cycle can be amply
improved by
reducing the
condenser pressure
(hence by reducing
the temperature at
which heat is
rejected), especially
in high vacuums. But
the increase in
efficiency is obtained
at the increased cost
of condensation
apparatus.
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
11
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
12
SCHEMATIC DIAGRAM
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
13
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
14
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
15
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
16
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
17
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
18
SCHEMATIC DIAGRAM
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
19
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
20
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
21
III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER
CYCLEES/DR.R.SUDHAKARAN
22

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17.pptx

  • 1. VAPOUR POWER CYCLES RANKINE CYCLE III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 1
  • 2. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 2 THEOROTICAL CYCLE ON WHICH STEAM TURBINE WORKS
  • 3. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 3 SCHEMATIC DIAGRAM
  • 4. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 4 PROCESSES Process 1-2 : Reversible adiabatic expansion in the turbine (or steam engine). Process 2-3 : Constant-pressure transfer of heat in the condenser. Process 3-4 : Reversible adiabatic pumping process in the feed pump. Process 4-1 : Constant-pressure transfer of heat in the boiler.
  • 5. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 5 4-1 BOILER STATE OF FLUID 4-WATER 1-STEAM 4 4 1 1 1 1 f f h h Q h Q h boiler for SFEE    
  • 6. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 6 1-2 TURBINE STATE OF FLUID 1-STEAM 2-STEAM Dryness reduces during expansion 2 1 2 1 h h W W h h Turbine for SFEE T T    
  • 7. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 7 2-3 CONDENSOR STATE OF FLUID 2-STEAM 3-WATER 3 3 2 2 2 2 f f h h Q h Q h Condensor for SFEE    
  • 8. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 8 3-4 PUMP STATE OF FLUID 3-WATER 4-WATER 3 4 4 3 f f P P f f h h W W h h Pump for SFEE    
  • 9. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 9 EFFICIENCY 1 1 Q W W Q W cycle Rankine of Efficiency P T NET RANKINE     ) ( ) ( ) ( 4 3 4 1 2 1 1 f f f NET RANKINE h h h h h h Q W cycle Rankine of Efficiency        ) ( ) ( ) ( 3 4 3 4 2 1 f f f f h h h h as h h Neglect     ) ( ) ( 4 1 2 1 1 f NET RANKINE h h h h Q W cycle Rankine of Efficiency     
  • 10. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 10 METHODS OF IMPROVING RANKINE EFFICIENCY Increasing boiler pressure •. It has been observed that by increasing the boiler pressure (other factors remaining the same) the cycle tends to rise and reaches a maximum value at a boiler pressure of about 166 bar Superheatin g •. All other factors remaining the same, if the steam is superheated before allowing it to expand the Rankine cycle efficiency may be increased. The use of superheated steam also ensures longer turbine blade life because of the absence of erosion from high velocity water particles that are suspended in wet vapour. Reducing condenser pressure. •The thermal efficiency of the cycle can be amply improved by reducing the condenser pressure (hence by reducing the temperature at which heat is rejected), especially in high vacuums. But the increase in efficiency is obtained at the increased cost of condensation apparatus.
  • 11. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 11
  • 12. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 12 SCHEMATIC DIAGRAM
  • 13. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 13
  • 14. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 14
  • 15. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 15
  • 16. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 16
  • 17. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 17
  • 18. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 18 SCHEMATIC DIAGRAM
  • 19. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 19
  • 20. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 20
  • 21. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 21
  • 22. III SEM- ENGINEERING THERMODYNAMICS-UNIT IV VAPOUR POWER CYCLEES/DR.R.SUDHAKARAN 22