Over View of Super Critcal
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Over view of Super Critical
SUPERCRTICAL TECHNOLOGY OVER VIEW
Presentation ByAJAY SHUKLADGM PMI
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Drivers For Ultra MegaPower Projects LARGE CAPACITY ADDITION PLANNED OVER
NEXT DECADE IN 11TH PLAN BEYOND PACE OF THERMAL CAPACITY ADDITION TO
INCREASE FROM ~ 5000 MW/Yr TO ~ 10,000 MW/Yr
ADVANCED PROVEN TECHNOLOGY WITH HIGHEFFICIENCY FOR
OPTIMAL USE OF RESOURCES HIGHER
EFFICIENCY
ECOFRIENDLY POWER GENERATION ECONOMY OF SCALE
OPERATIONAL FLEXIBILITY( Faster Start Up, Load
Cycling)
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CONTENTS Importance of Efficiency
What is Thermal cycle Efficiency
How to Increase Cycle efficiency
What is Super critical Boiler
Advantages & Disadvantages of Super critical Boiler
The SG 3 x 660 MW Boiler package
Comparison with 500 MW SG package
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IMPORTANCE OF EFFICIENCY
The cost of operating the Plant of 3 x 660 MW, one percentagepoint below the design point, will incur additional fuel cost ofRs. 20 Crores in a year.
The indirect costs for Maintenance, APC, Ash Dyke land etc.
will give additional burden of Rs. 2 Crores in a year. The environment will suffer on account of GHGs.
The life time loss is Rs. 660 Crores for efficiency lower by onepercentage point .
At Sipat, we gain an efficiency of 2.5 percentage point byadopting super critical technology in 1980 MW station, thussaving Rs. 1650 Crores in its life time.
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Trend in unit sizes & Cycle parameters
2008568/596256800 MW
2008568/596256660 MW
1985540/568179500 MW
1991540/540156250 MW1972(37.5%)540/540137 / 156200 / 210 MW
1966(35.7%)540/540139110 / 120 MW
1965(30.5%)5409660 / 70 MW
Year ofIntroduction
SHO/RHOTemperature
(Deg.C)
SHO Pressure(kg/cm2(a))
Unit Size
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QUEST FOR EFFICIENCY IMPROVEMENT
Since the time thermal power stations have been engineered,
there is a quest for efficiency improvement.
And supercritical parameters (Press. above 225Kg/cm2 andtemperature above 374.15 C) is an effort in that direction.
The selected supercritical parameters for Sipat Boiler are :
Pressure : 256 kg/cm2
Temperature : 540 C SH and 568C RH
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UNDERSTANDING THE THERMAL CYCLE
EFFICIENCY
Let us refresh our knowledge of thermodynamics laws
First Law states that the total energy of a system in all its formsremain constant.
Second Law states that it is impossible to construct an enginewhose sole purpose is to convert all the heat supplied to it intoequivalent amount of work. In other words, it is impossible toconvert all heat energy supplied to a system to work.
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EFFICIENCY & CARNOTS ENGINE
= work output from a system
heat input to the system
Because of 2nd Law of Thermodynamics # 100%
Hence, for some heat, which is not converted to work, heat sink
is necessary.
Thus = Q1 Q2Q1
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CARNOT ENGINE (FRENCH ENGINEER SODI CARNOT 1824)
1-2 - Isothermal Expansion at T1K
2-3 - Adiabatic Expansion upto T2K
3-4 - Isothermal Compression at T2K 4-1 - Adiabatic Expansion upto T1K
For Carnot Cycle = 1 - T2
T1T1 = Temp. of heat source
whereT2 = Temp. of heat sink
Carnot Cycle gives maximum possible thermal efficiency which
can be obtained between any two given temperature limits.
12
3
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S
T244
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CARNOT ENGINE (CARNOT ENGINE (FRENCH ENGINEER SODI CARNOTFRENCH ENGINEER SODI CARNOT
1824)1824)
1-2 - Isothermal Expansion at T1K
2-3 - Adiabatic Expansion upto T2K
3-4 - Isothermal Compression at T2K
4-1 - Adiabatic Expansion upto T1K
For Carnot Cycle = 1 - T2T1T1 = Temp. of heat source
whereT2 = Temp. of heat sink
Carnot Cycle gives maximum possible thermalefficiency which can be obtained between any two
given temperature limits.
12
3
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T244
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CONCLUSION ON CARNOTS CYCLE EFFICIENCY
No engine working on cyclic process is more efficient than
Carnots engine when working between same limits oftemperature.
All efforts should be made to come closer to Carnots cycle as
far as possible to achieve maximum efficiency out of any
thermal cycle.
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eff=(1-T2/T1)
T1
T2
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THERMAL EFFICIENCY OF RANKINE CYCLE
Q1-Q2 W Useful work = ------- = --- = ----------------
Q1 Q Heat suppliedRejected Heat
= 1 - --------------------Useful Heat
T1 - T2 T2 Carnot = -------- = 1 - ---
T1 T1
To achieve more efficiency T2 should be as low as possible and T1
should be as high as possible
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METHODS OF INCREASING RANKINE CYCLE
EFFICIENCY
Raising supply temperature by super heating.
Increasing the inlet temperature will raise the heat supply tothe cycle more than the heat rejection.
Raising inlet pressure of steam :
Increasing the pressure will mean increase in saturationtemperature at which steam evaporates thus increasing theaverage inlet temperature (T1)
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(Contd..)
Dropping the final pressure (or temperature) at which heat is
rejected.
Regenerative Heating : Heating the feed water pumped toBoiler by bleeding steam from turbine.
Reheat Cycle : Reheating of steam in boiler after it has already
expanded in HP Turbine will avoid moisture formation in LTTurbine. Also, more heat content of steam before IP Turbine,
will improve efficiency.
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WHY SUPERCRITICAL PRESSURE
The purpose of having high inlet steam pressure for turbine
has already been discussed in this presentation.
A Boiler operating at a pressure above critical point is
called SUPERCRITICAL BOILER
A point where boiling water and dry saturated lines meet sothat associated latent heat is zero, this point is called Critical
Point and occurs at 225 kg/cm2 (abs) 374.15 C
temperature.
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CRITICAL CONDITION
Definition
CRITICAL is a thermodynamic expressiondescribing the state of a substance beyond whichthere is no clear distinction between the liquid andgaseous phase.
The critical pressure & temperature for water are Pressure = 225.56 Kg / cm2
Temperature = 374.15 C
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WHAT IS SUPER CRITICAL
T
S
P1
Pcr
P2
Cycle of Super critical boiler
operating above critical pressure
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SC Steam generator
Boiler Steam Pressure
above the critical point Critical Point
221 bar, 374c
S
T
1
2
3
4
Entropy
Temperature
1-2 Feed Water Pumping Process2-
3 Heat addition in the Feed
Water Heaters & Boiler
3-4 Expansion in HP Turbine4-5 Reheating in Boiler5-
6
Expansion in IP & LP Turbine
6-1 Heat rejection in Condenser
5
6
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256K
g/cm
2
0
100
200
300
400
500
600
SUPER CRITICAL
BOILER CYCLE
WITH SH, RH &
Regenerationof SIPAT 3 x 660 MW
540C 568C
Steam flow :2225 T/Hr
Steam temp : 540 c
Steam Pres : 256 kg/cm2RH pre : 51.6 Kg/cm2
RH Temp : 568c
Feed water Temp : 291c
ENTROPY
TEMP
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SUPERCRITICAL BOILER
Supercritical pressure boiler has no drum and heat absorbing
surface being, in effect, one continuous tube, hence called once
through Supercritical pressure boilers.
The water in boiler is pressurized by Boiler Feed Pump, sensible
heat is added in feed heaters, economizer and furnace tubes, until
water attains saturation temperature and flashes instantaneouslyto dry saturated steam and super heating commences.
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SH
DRUM
ECOHTRBFP
W/WALL
DOWN COMER
RISERS
Natural CirculationBoiler
W/WALL
BF
P
HTR ECO
SH
SEPERATOR
ONCE THROUGH SYSTEM
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SH
DRUM
ECOHTRBFP
W/WALL
DOWN COMER
RISERS
Natural CirculationBoiler
W/WALL
BF
P
HTR ECO
SH
SEPERATOR
ONCE THROUGH SYSTEM
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Types of boilers
Drum type
Once-through type
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Division of heating surfaces
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Drum type boiler
Steam generation takes place in furnace water walls
Fixed evaporation end point - the drum
Steam -water separation takes place in the drum
Separated water mixed with incoming feed water
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Drum type boiler
Natural Circulation Boiler Circulation thru water walls by
thermo-siphon effect
Controlled Circulation Boiler
At higher operating pressures
just below critical pressure levels,
thermo-siphon effect supplemented
by pumps
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500 MW Boiler Typical Arrangement
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540C, 255 Ksc
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HPT
IPTLPTC
O
N
D
E
N
S
E
R
FEED WATER
FRS
S
T
O
R
A
G
E
T
A
N
K
SEPARATOR
BWRP
Spiralwa
terwall
s
MS LINEHRH LINE
VERTICAL WW
ECO I/L
ECO
JUNCTIONHDR
ECO HGR O/LHDR
FUR LOWER HDR
FUR ROOF I/L
HDR
DIV PANELS SH PLATEN SH
FINAL RH
FINAL SH
LTRH
ECONOMISER
290C, 302 KSC
411C,
277Ksc411C,
275 Ksc
492C, 260 Ksc
540 C, 255 Ksc
305C,
49K
sc
457C, 49 Ksc
568C, 47
Ksc
G LPT
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Steam generation process
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Boiler-Cycle Thermodynamics
3208
2865
1800
Pres s
ure
Ps
ia
Enthalpy BTU/lb
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Over view of Super CriticalWell suited for < 2100 psi cycles
Natural Circulation System
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Over view of Super CriticalOptimum solution for reliable high pressure subcritical operation
Controlled Circulation System
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CONTROLLED CIRCULATION (Vs) ONCETHRU
CC OT
B il i h E
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Boiler with Evaporator system
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Once-thru BoilerMajor differences from Drum type boiler :
Evaporator system
Low load circulation system
Separator
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Once -thru Boiler
Evaporator system :
Formed by a number of parallel tubes
Tubes spirally wound around the furnace to reduce
number of tubes and to increase the mass flow rate
thru the tubes
Small tube diameter
Arrangement ensures high mass velocity thru thetubes
mp e ra n
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mp e ra n
Discharge System
To Condenser
WW
ECO
HPH
BFP
DeaeratorC
WL
C
HWL
SH
Separator
Flash
Tank
S U S i h R i l i
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Start-Up System with Recirculation
Added Cost vs.
Simplified Drain
System
Reduced Heat andWater Loss During
Start-Up
HPH
BFP
Deaerator
C
C
WW
ECO
To Condenser
C
HWL
SH
Start-Up SystemRecirculation Pump in Main Bypass Line
Separa
tor
Flash
Tank
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ADVANTAGES
OF
SUPER CRITICAL BOILER
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SUPERCRITICALTHERMAL CYCLE ADVANTAGES
(1)
Improvements in plant efficiency by more than
2 % Decrease in Coal Consumption
Reduction in Green House gases.
Overall reduction in Auxiliary Power
consumption.
Reduction in requirement of Ash dyke Land &Consumptive water.
SUPERCRITICAL ADVANTAGES (2)
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( )
Sliding pressure operation because of Once through
system . Even distribution of heat due to spiral wall
arrangement leading to less Boiler tube failure,
thereby improving system continuity and availability
of the station.
Low thermal stress in Turbine . The startup time is less for boiler.
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SUPERCRITICAL DISADVANTAGES
Higher power consumption of BFP
Higher feed water quality required.
More complex supporting and framing in Boiler
due to Spiral Wall tubes.
Slight higher capital cost.
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HISTORY & EVOLUTION
HISTORY
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HISTORY
.
DEVELOPED IN USA IN -1950S
INTRODUCED IN JAPAN IN -1960S
MORE THAN 110 UNITS IN OPERATION IN
JAPAN
SLIDING PRESSURE INTRODUCED IN JAPAN-
1980S
INITIAL PROBLEMS
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INITIAL PROBLEMS
SLAGGING PROBLEMS DUE TO INADEQUATE
FURNACE SIZE.
FAILURE OF FURNACE TUBES DUE TO
INAPPROPRIATE FLOW CIRCUITS. BYPASS OPERATION DURING STARTUP
STARTUP VALVES FAILURE / EROSION DUE TO LARGE
PRESSURE DIFFERENCE.
COMPARISION OF THERMAL CYCLE
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COMPARISION OF THERMAL CYCLE
EFFICIENCIES.
OPEN CYCLE EFFICIENCY - 14.68 %
WITH CONDENSER - 26.2 %
WITH SUPER HEAT 30.75 TO 34.15 %
WITH REHEAT - 34.2 TO 36.6 %
WITH SUPER CRITICAL PARAMETERS-
36.0 TO 39.15 %
INCREASE IN PLANT EFFICIENCY by SUPER
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INCREASE IN PLANT EFFICIENCY by SUPER
CRITICAL PARAMETERS
1.5
0.90.6
3.2
167 bar
538/538c250 bar
538/538250 bar
540/560c
250 bar
580/600c
250bar
566/566
c
1
2
3
4
5
6
.
Efficiency Increase
REQUIREMENTS OF SUPERCRITICAL
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REQUIREMENTS OF SUPERCRITICAL
TECHNOLOGY
REQUIREMENT OF HIGH STRENGTH MATERIALS.
OXYGENATED FEED WATER TREATMENT (OWT)
ADVANCED DIGITAL BASED CONTROL SYSTEMS
HIGHLY AUTOMATED OPERATION.
LOW LOAD CIRCULATION SYSTEM
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Boiler load %
40
100
W WFlow
%
40
LOW LOAD CIRCULATION SYSTEM
60 80100
LOW LOAD CIRCULATION SYSTEM
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Boiler load %
40
100
W WFlow
%
40
LOW LOAD CIRCULATION SYSTEM
60 80100
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BOILER PARAMETERS
STEAM PARAMETERS UNDER BMCR CONDITION
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291.9FEED WATER TEMP AT ECONOMISER INLET8
565STEAM TEMP AT IP TURBINE INLET DEGC7
568STEAM TEMP AT REHEATER OUTLET DEG C
306.3STEAM TEMP AT HP TURBINE EXHAUST DEG C6
51.6STEAM PRESSURE AT HP TURBINE EXHAUST KG/CM25
1754STEAM FLOW TO REHEATER ( T/HR)8
1742.6STEAM FLOW TO REHEATER T/HR7
540TEMPERATURE AT SUPERHEATER OUTLET (DEG C)5
247PRESSURE AT HP TURBINE INLET KG/CM2 (ABS)4
256PRESSURE AT SUPER HEATER OUTLET KG/CM2 (ABS)3
2225STEAM FLOW AT SUPER HEATER OUTLET (T/HR)1
DESCRIPTIONSL
COMPARISION OF 660 MW Vs 500 MW BOILER
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255.2291.40CFEED WATER TEMP
46.151.17KG/CM2RH STEAM PRESS INLET
5405680CRH STEAM TEMP OUTLET
338.5303.70CRH STEAM TEMP INLET
1397.41742T/HRRH STEAM FLOW
5405400CSH STEAM TEMP
179256KG/CM2SH STEAM PR
16252225T/HRS/H STEAM FLOW
500660unitDescription
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