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About combustion in Kiln
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Burners - Influence of flame and flame shape on the refractoryliningAlain Czaplinski
WHAT IS COMBUSTION ?
A CHEMICAL REACTION BETWEEN TWO CHEMICAL COMPONENTS WHICH CREATES HEAT
TYPICALLY ONE OF THE COMPONENT IS AIR ( OXYDISING REACTION ), THE SECOND IS CALLED FUEL
GEORG ERNST STAHL ( 1660 1734 ) :
COMBUSTION WAS DUE TO THE PHLOGISTIC COMPONENT IN COAL IN ORDER TO CALCINATE METAL
COAL ( INCLUDING PHLOGISTIC ) => COAL + PHLOGISTIC => FIREMETAL + PHLOGISTIC => CALCINED METAL
IN 1760, BLACK IDENTIFIED FIXED AIR WHICH IS CO2IN 1766, CAVENDISH IDENTIFIED INFLAMMABLE AIR WHICH IS H2
PRIESTLEY IDENTIFIED PHLOGISTIC AIR WHICH IS N2
IN NOVEMBER 1772, LAVOISIER ESTABLISHED THE MASS CONSERVATION PRINCIPLE DURING TIN CALCINATION BY WEIGHTING THE AIR BEFORE AND AFTER THE REACTION
COMBUSTION IS NOT
CALCINATION :
CaCO3 + HEAT ( 1800kJ/kg ) => Ca0 + CO2
BY EXTENSION, CALCINATION MEANS TO BURN AT HIGH TEMPERATURE A MATERIAL IN ORDER TO GET A NEW ONE
PYROLYSIS :
CHEMICAL DECOMPOSITION DUE TO HEAT
COMBUSTION REACTIONS
C + 0 => CO + 111 kJ/mol
CO + 0 => CO2 + 283 kJ/mol
C + 02 => CO2 + 394 kJ/mol
H2 + 0 => H20 + 242 kJ/mol
S + 02 => S02 + 71 kJ/mol
CH4 + 202 => CO2 + 2H20 + 820 kJ/mol
CALORIFIC HEAT VALUE
HEATING VALUE : MEANS THE HEAT QUANTITY OBTAINED WHEN BURNING ONE UNIT OF FUEL
IT IS THE HEAT POTENTIAL OF A FUEL WHICH CAN BE COMPARED WITH OTHERS
HIGH HEATING VALUE ( HHV ) : WATER IS CONSIDERED AS LIQUID (CONDENSATE )
LOW HEATING VALUE ( LHV ) : WATER IS CONSIDERED AS VAPOR
HHV and LHV are expressed in kJ/kg
HHV = LHV + WATER VAPORISATION HEAT
IN PRACTICE, IN ATMOSPHERIC CONDITIONS, WE NEED TO CONSIDER THE LHV AS FLUE GAS TEMPERATURE IS HIGHER THAN 100c
RELATION BETWEEN HHV AND LHV
HHV = LHV + WATER LATENT VAPORISATION HEAT
HHV = LHV + ( %H20 ) x 25 + ( % H ) x 226
% PERCENTAGES IN WEIGHT
IE : HEAVY FUEL OIL LHV = 40100kJ/kg , H20 = 0,95% , H = 11%
HHV = 40100 + (0,95)x25 + ( 11)x226 = 40100 + 24 +2486 = 42610 kJ/kg
6% difference
IE : NATURAL GASLHV = 36500 kJ/Nm3 , H20 = 0% , H = 18%
HHV = 36500 + (0)x25 + ( 18)x226 = 36500 + 4068 = 40568 kJ/Nm3
11% difference
MAIN NOBLE FUEL CLASSIFICATION PER LHV
NATURAL GAZ : 34 000 to 45 000 kJ/Nm3 ( depends on N2 content )
HEAVY FUEL OIL : 40 000 kJ/kg
DIESEL OIL : 43 000 kJ/kg
COAL : ANTHRACITE ( raw basis ) : up to 39 000 kJ/kg STEAM COAL ( raw basis ) : 24 000 kJ/kg to 27 000 kJ/kgLIGNITE ( raw basis ) : 15 000 kJ/kg to 19 000 kJ/kg
PETCOKE ( raw basis ) 33 000 kJ/kg to 36 500 kJ/kg
* Contaminated water negative
* Blast furnace gaz 2 700 kJ/kg
* Dried sewage 8 000 to 15 000 kJ/kg
* Paper, cardboard 13 000 to 17 000 kJ/kg
* tyres 25 000 to 31 000 kJ/kg
* solvents 29 000 to 37 000 kJ/kg
* waste oils 27 000 to 40 000 kJ/kg
* Waste plastics 18 000 to 42 000 kJ/kg
ALTERNATIVE FUELS : TYPICAL LHV VALUES
ALTERNATIVE FUELS : WHY IN A CEMENT PLANT ?
IN EUROPEAN COMMUNITY, CITY WASTES NEEDS FOR INCINERATION :
A RESIDENCE TIME SUPERIOR TO 2 SECOND AT 850c
IN A ROTARY KILN : RESIDENCE TIME IS SEVERAL SECONDS BETWEEN 900c AND 1300 c
A ROTARY KILN IS A PERFECT INCINERATOR WHEREASHES ARE REUSED
DEFINITIONS ABOUT AIR
STOECHIOMETRIC AIR : EXACT AIR QUANTITY REQUIRED TO BURN ONE UNIT OF FUEL ( kg of air/ kg of fuel )
EXCESS AIR LAMBDA : AVAILABLE AIR QUANTITY / STOECHIOMETRIC AIR
LAMBDA > 1 : REAL AIR EXCESS TO ALLOW A COMPLETE COMBUSTION
LAMBDA
OTHER DEFINITIONS :
SPEED OF FLAME : SPEED OF THE FRONT OF FLAME IN THE DIRECTION OF THE MIXING AIR AND FUEL TO BE BURNT NEXT
DEFLAGRATION : IF THE FLAME CAN SPREAD IN A AUTONOMOUS AND SUBSONIC WAY
DETONATION : IN CASE OF DEFLAGRATION, FLAME PROPAGATION AND GAZ DILATATION CAN CREATE A CHOCK WAVE AHEAD OF THE FRONT OF FLAME.THEN COMBUSTION IS CREATED BY PRESSURE INCREASE ( SO TEMPERATURE INCREASE ) AHEAD OF THE FRONT OF FLAME. IT HAPPENS AT ULTRASONIC SPEED GENERATING OVERPRESSURE OF SEVERAL MPa.
DEFINITION OF FLAME LENGTH
THERE ARE SEVERAL DEFINITIONS OF A FLAME LENGTH
DEFINITION 1 : DISTANCE BETWEEN THE BURNER OUTLET TO THE POINT WHERE THE COMBUSTION RATE IS , BY EXAMPLE, 99%
DEFINITION 2 : DISTANCE BETWEEN THE BURNER OUTLET TO THE FURNACE POSITION WHERE THE FLUE GAS TEMPERATURE IS, BY EXAMPLE, 1000c
DEFINITION 3 : DISTANCE BETWEEN THE BURNER OUTLET TO THE POINT WHERE THE FLAME BECOMES UNVISIBLE BY EYE
OTHERS
IN CEMENT INDUSTRY, WE SHOULD USE THE THIRD DEFINITIONAS WE ARE MAINLY INTERESTED IN HEAT EXCHANGE BY RADIATION
BUT WE CANT MEASURE IT
INFLAMMABILITY LIMITS
MAXIMUM AND MINIMUM GAZ FUEL CONCENTRATIONS IN AIR WHERE STABLE COMBUSTION MAY OCCUR
FOR NATURAL GAZ : Lmin is around 5% , Lmax is around 15%FOR ACETYLENE ( C2H2 ) : Lmin is 2,2% , Lmax is 85%( in volume )
MINIMUM INFLAMATION TEMPERATURE : MINIMUM TEMPERATURE AT WHICH SPONTANEOUS COMBUSTION WITH AIR STARTS ( under atmospheric pressure)
FOR METHANE : 580cFOR BUTANE : 420c
FOR COALS : depends on fineness to allow volatile matter inflammation
WHAT IS FLAME TEMPERATURE ?
WE NEED TO SPEAK ABOUT ADIABATIC FLAME TEMPERATURE IN STOECHIOMETRIC CONDITIONS
A COMBUSTION IS ALWAYS CREATING A TEMPERATURE INCREASE ( T ), SO WE NEED TO FIX A REFERENCE TEMPERATURE ( IE AMBIANT AIR )
ADIABATIC MEANS THAT THE SYSTEM IS ISOLATED, ALL THE HEAT CREATED BY COMBUSTION IS TRANSFERRED TO THE STOECHIOMETRIC FLUE GAS
STOCHIOMETRIC CONDITIONS ARE REQUIRED :IN LACK OF AIR, WE CANT REACH THE MAXIMUM FLAME TEMPERATURE.IN EXCESS OF AIR, FLUE GAS ARE IN EXCESS TO ABSORB THE HEAT, THE FLAME
TEMPERATURE IS DECREASING
% OF STOECHIOMETRIC AIR
PEAK OF FLAME TEMPERATURE UNDER STOECHIOMETRIC CONDITIONS
1,0
UNDERSTOECHIMETRIC CONDITIONS :NOT ENOUGH AIR TO BURN THE FUEL
EXCESS AIR CONDITIONS :UNBURNT AIR IS COOLING THE FLAME
ADIABATIC FLAME TEMPERATURE : TYPICAL CURVE PROFILE
SOME ADIABATIC FLAME TEMPERATURES
BLAST OVEN GAS = > +/- 1200c
H2 => 1430c
CH4 = > 1957c
C2H4 => 1560c
C3H8 = > 1980c
C4H10 = > 1970c
STEAM COAL = > +/- 2000c
COAL ANALYSIS
% PROXIMATE ANALYSIS ULTIMATE ANALYSIS
MOISTURE 7.0 C 68.00ASH 18.0 H 2.20VOLATILE MATTER 10.0 S 0.80FIXED CARBON 65.0 N 1.00
O 3.00H20 7.0
ASH 18.0
TOTAL 100.0 100,0
Moisture : difference in weight after drying at 105/110c
Volatile matter : difference in weight after pyrolysis at 900c ( ISO ) or 950c ( ASTM )
Ashes : remaining weight after complete combustion
Fixed carbon : calculated by difference
COAL ANALYSIS
PROXIMATE ANALYSIS ON DIFFERENT BASIS
raw basis as dried dry ash and moisture freeMoisture 7.0 1,0 0.0 0,0 Ash 18.0 19,16 19,36 0,0Volatile Matter 10.0 10,65 10,75 13,33Fixed Carbon 65.0 69,19 69,89 86,67
HHV ( Kj/Kg ) 26,0 27,68 27,96 34,61
Total 100.0 100,0 100,0 100,0
% in weight
HHV is proportional to H20 and ashes, LHV to be calculated from HHV, H20 and H
FOR SOLID FUEL, BASIS OF HEATING VALUE SHOULD BE ALWAYS MENTIONED
KEY POINT : IGNITION OF COAL
IGNITION MECHANISM OF COAL RELIES ON VOLATILE MATTER :
PYROLYSIS AND COMBUSTION OF VOLATILE MATTER => HEATING UP OF AIR AND SOLID FUEL AT BURNER OUTLET
QUANTITY AND QUALITY OF VOLATILE MATTERS ARE THE KEY FACTORS FOR IGNITION
SIMPLE CRITERIA :IGNITION BASED ON VOLATILE MATTER CONTENT
MORE INTERESTING CRITERIAIGNITION BASED ON QUALITY OF VOLATILE MATTER
HHV COAL = HHV FIXED CARBON + HHV VOLATILE MATTER
Calculations made on moisture and ash free basis
IN CEMENT, WE INTRODUCED COAL WHEN TEMPERATURE IS AROUND 800c , WE AVOID THE IGNITION PROBLEMS
COAL REACTIVITY : % VOLATILE MATTER RELEASED VS TEMPERATURE
COAL REACTIVITY : COMBUSTION RATE OF CHAR ( AT 700c + AIR )
IGNITION OF ANTHRACITE COMPARED TO STEAM COAL
0
500
1000
1500
T
e
m
p
e
r
a
t
u
r
e
(
C
)
0
500
1000
1500
0,00 1,00 2,00 3,00 4,00 5,00 6,00 7,00
STEAM COALANTHRACITE OF VIET NAM
COAL CLASSIFICATION (ASTM D388)
8890 7780 7220 6110 5280 4610 kCal/kg
Anthracite
Low vol.Bit.
Mediumvol. bit.
High vol.A bit.
Highvol.
B bit.
Highvol.
C bit.or
Subbit A
SubbitB
SubbitC Lignite
VM/MAF FC/MAF%
HHV WITH INHERENT MOISTURE WITHOUT MINERAL MATTER
40
69
78
86
9298
100
31
22
14
820
60
LOW REACTIVITY
HIGH REACTIVITY
SPECIFICITIES OF COMBUSTION IN CEMENT KILNS
ONE SINGLE BURNERONE VERY LONG AND NARROW FURNACE ( L/D : 10 to 40 )
DIRECT HEAT EXCHANGE WITH CLINKER ( RADIATIONS, CONVECTION )FUELS ASHES ARE INCORPORATED IN CLINKER
ONLY 10% OF COMBUSTION AIR THOUGH THE BURNEREXTREMELY HOT SECONDARY AIR ( 700 TO 1200c ) COMBUSTION EFFICIENCY IS USELY NOT A CRITERIA
STABLE LOADLARGE MIXING OF FUELS
SPECIFICITIES OF COMBUSTION IN CEMENT KILNS
ONE SINGLE BURNER
ONE VERY LONG AND NARROW FURNACE ( L/D : 10 to 40 )
BURNER OUTPUT : UP TO 250 MW ( 5000 tpd, 4,2MJ/kg )=> equivalent to 21tph of Heavy Fuel oil
PRECALCINER KILN : 12 000 tph, 40%/60%, 3MJ/kg clinker=> main burner output is 166MW => precalciner output is 250 MW
POWER GENERATION : TANGENTIAL FIRING
FIRING SYSTEMTANGENTIAL WINDBOW BURNERS
DOUBLE ARCH FIRING CALLED W FLAME
TYPICAL ARCH COAL BURNER
BURNER ARRANGEMENT ON THE ARCH
SPECIFICITIES OF COMBUSTION IN CEMENT KILNS
ONE SINGLE BURNER
BURNER OUTPUT : UP TO 250 MW ( 5000 tpd, 4,2MJ/kg )=> equivalent to 21tph of Heavy Fuel oil
PRECALCINER KILN : 12 000 tph, 40%/60%, 3MJ/kg clinker=> main burner output is 166MW => precalciner output is 250 MW
A KILN BURNER IS SINGLE : RELIABILITY IS A KEY FACTOR
VERY FEW BURNER MANUFACTURERS ON THE WORLD MARKET
SPECIFICITIES OF COMBUSTION IN CEMENT KILNS
ONE VERY LONG AND NARROW FURNACE ( L/D : 10 to 40 )
THE FLAME SHAPE IS A KEY ISSUE TO FIT INSIDE THE NARROW TUNNEL
THE TEMPERATURE PROFILE IS THE MOST IMPORTANT PARAMETER FOR A CEMENT OR LIME PRODUCER
PREMIUM CRITERIA IS : FLAME SHAPE FLEXIBILITY
MULTICHANNELS BURNERS ARE USED IN ROTARY KILNS
MULTI CHANNEL BURNERS : PRINCIPLES
THE THREE CHANNEL BURNER TYPE :
A
AXIAL AIR (ANNULUS)
COAL STREAM
AXIAL AIRSWIRL AIR
Unitherm Cemcon Firing Systems
TEMPERATURE PROFILE (CFD Modelling)
p.a. nozzle setting fully axial controlled long flame
p.a. nozzle setting 35 angle short, hot flame
TEMPERATURE PROFIL :
T"long" flame"short" flame
FOR CEMENT PRODUCERS :BURNER EFFICIENCY IS TO CONTROL THE FLAME TEMPERATURE ALONG THE KILN
FLAME TEMPERATURE : FLAME WITH LIGNITE AND WASTES
FLAME TEMPERATURE : LIGNITE AND WASTES FIRING
MAIN MULTICHANNEL BURNER MANUFACTURERS
COMBUSTION COMPANIES :
PILLARD : THREE CHANNELS BURNER, ROTAFLAM
UNITHERM : UNIGO, UNIGRESS, UNIGAS, MAS
GRECO ENFIL
CEMENT ENGINEERING COMPANIES :
FLS : SWIRLAX, CENTRAX AND DUOFLEX
KHD : PYROJET
UNITHERM MAS BURNER
ONE STABILISER IN THE CENTER
ONE SINGLE AIR CHANNEL
ADJUSTABLE AIR ANGLE DEVICE
ONE 250mbar PA FAN
SOLID and WASTES IN THE CENTER
SWIRL SETTING DEVICE FOR PRIMARY AIR
Unitherm Cemcon Firing Systems
PILLARD ROTAFLAM BURNER
ONE STABILISER IN THE CENTER
TWO AIR CHANNELS
ADJUSTABLE AIR CROSS SECTIONS
ONE 250mbar PA FAN
SOLID and WASTES IN THE CENTER
PILLARD ROTAFLAM : ADJUSTMENT OF AIR CROSS SECTIONS
FLS DUOFLEX BURNER
ONE STABILISER IN THE CENTER
TWO AIR CHANNELS MIXED BEFORE BURNER OUTLET
ADJUSTABLE AIR CROSS SECTIONS
ONE 250mbar PA FAN
SOLID and WASTES IN THE CENTER
FLS DUOFLEX BURNER : AIR CROSS SECTIONS ADJUSTMENTS
KHD : PYROJET BURNERS
NO STABILISER IN THE CENTER
COAL CHANNEL BETWEEN TWO AIR CHANNELS
FIXED CROSS SECTIONS
ONE BLOWER FOR AXIAL AIR 450mbar
ONE FAN FOR RADIAL AIR
Jet Air Nozzle Ring
GRECO ENFIL BURNERS
NO FIXED CONCEPT, NO BRAND NAME
CASE BY CASE STUDY
FIXED CROSS SECTIONS
COAL CHANNEL BETWEEN TWOAIR CHANNELS
ONE ROOT BLOWER FOR AIR AT 450mbar
WASTES IN THE CENTER
SPECIFICITIES OF COMBUSTION IN CEMENT KILNS
DIRECT HEAT EXCHANGE WITH CLINKER ( RADIATIONS..)
THE FLAME NEEDS TO BE RADIANT TO IMPROVE THE HEAT EXCHANGE EFFICIENCY
RADIATIONS : HEAT EXCHANGE VIA ELECTROMAGNETIC WAVES ( PHOTONS )
RADIANT HEAT FLUX IS PROPORTIONAL TO : T 4
THE FLAME NEEDS HIGH TEMPERATURE AND HIGH INTERNAL MIXING( NATURAL GAS IS LESS EFFICIENT )
SPECIFICITIES OF COMBUSTION IN CEMENT KILNS
FUELS ASHES ARE INCORPORATED IN CLINKER
IN POWER GENERATION, FLY AND BOTTOM ASHES ARE RECOVERED,BUT REUSING IS VERY DIFFICULT
IN CEMENT KILNS, REUSING IS EASY AS IT IS A PART OF THE FINAL PRODUCT WHICI IS REAL SPECIFIC TO THIS INDUSTRY
IT MAY CREATE LIMITATIONS ( P2O5 , Cl etc ) WHEN FIRING WASTES
SPECIFICITIES OF COMBUSTION IN CEMENT KILNS
PRIMARY AIR IS AMBIANT ( LOW TEMPERATURE ): HIGH %PA = LOW EFFICIENCY
LOW PRIMARY AIR REDUCES ALSO NOx EMISSIONS
LOW PA BURNERS WERE CALLED HIGH EFFICIENCY BURNERS
ONLY 10% OF COMBUSTION AIR THOUGH THE BURNEREXTREMELY HOT SECONDARY AIR ( 700 TO 1200c )
HIGH SPEED PRIMARY AIR IS MIXED WITH LOW SPEED SECONDARY AIRMIXING IS SOMETIMES DIFFICULT,
POSITION OF THE BURNER INSIDE THE KILN SHOULD BE ADJUSTABLE
SECONDARY AIR INJECTION AT BURNER TIP
Secondary Air Mixing Flow pattern velocity in [m/s]
(velocities above 25 m/s are displayed in red)Unitherm Cemcon Firing Systems
SPECIFICITIES OF COMBUSTION IN CEMENT KILNS
USUALLY WITH A RIGHT EXCESS AIR AT KILN OUTLET ( 2% O2 )IS ENOUGH FOR A COMPLETE COMBUSTION
AS RESIDENCE TIME IS LONG ENOUGH
COMBUSTION EFFICIENCY IS USELY NOT A CRITERIA
WITH WASTE FUELS ( SOLID ) ,IT MIGHT BE NECESSARY TO INCREASE THE EXCESS AIR
FOR BURNERS MANUFACTURERS : BURNER EFFICIENCY IS THE COMBUSTION RATE
RELATIONS BETWEEN BRICKS AND BURNER
AFTER 7 DAYS OF OPERATION
RELATIONS BETWEEN BRICKS AND BURNER
AFTER 7 DAYS OF OPERATION
NOTHING TO DO WITH THE BRICKS NOTHING TO DO WITH BURNER DESIGN
BUT A MISTAKE IN BURNER OPERATION
USUAL IGNITION PROCESS :
1) GAZ IGNITOR WITH ELECTRODES
2) LIQUID OR GAZ LANCE
3) SOLID FUEL INJECTION WHEN TEMPERATURE IS OK
4) CHANGE OF ROTATION SPEED
5) MEAL INJECTION
HEATING UP : RISK WITH POOR FUEL OIL PULVERISATION (1)
HEATING UP OF THE KILN WITH HEAVY FUEL OIL (2)
HEATING UP OF THE KILN WITH HEAVY FUEL OIL (3)
NEW LINING AFTER 8 HOURS HEATING UP TO 1000c
RELATION BETWEEN FLAME INTENSITY AND CLINKER
INFLUENCING FACTORS :
CEMENT PRODUCERS ARE FOCUSING ON :CLINKER PARAMETERS:
BURNABILITY INDEXSILICA RATIO
FREE LIMEGRINDABILITY
S02 , ALKALI RECIRCULATIONS etc..
BURNER MANUFACTURERS ARE FOCUSING ON :DIAMETER AND LENGTH OF KILN
TYPE OF PROCESSFUELS TO BE BURNT
KILN THERMAL LOAD IN BURNING ZONE
KILN THERMAL LOAD IN BURNING ZONE
Q2 /S : HEAT INPUT THROUGH MAIN BURNER DIVIDED BY THE KILN SECTION ( INSIDE BRICKS ) :
CALCULATED WITH : SPECIFIC HEAT CONSUMPTION IN kcal/kg KILN OUTPUTKILN DIAMETER
Example : KILN : 2300 TPD, Diameter 4,6m , precalciner kiln
SPECIFIC HEAT CONSUMPTION : 880 kcal/kg with 65% through the main burner
bricks : B620/B320
Q2 /S = 0,65*(( 2300/24)*880*4)/ ( (4,6-0,44)2* )
Q2 /S = 4033 Gcal/hm2
KILN THERMAL LOAD IMPACT ON LOWER TRANSITION ZONE BRICKS
ONE TENTATIVE OF APPROACH BY CALCULATIONS :
FLS KILN, 5000 TPD, PRECALCINER, DIAMETER 4,75M
FIRST OPERATION KILN 1 : AT 5000 TPD : Q2 / S = 3,8 Gcal/hm2
LTZ : AG 85 0,4 TO 9M , STABLE COATING FROM 12 to 19M=> LIFETIME : 14 MONTHS
SECOND OPERATION KILN 1 : RUNNING AT 6000 TPD, Q2 / S = 4,5 Gcal/hm2
LTZ : AG 85 BETWEEN 0,4 TO 9M, STABLE COATING FROM 9 to 19M=> LIFETIME : 14 MONTHS ( still running )
CONCLUSION : Q2 / S < 4,5 Gcal/hm2
=> NO REAL IMPACT ON BRICK LIFETIME ( in this case )
KILN THERMAL LOAD IN BURNING ZONE
POLYSIUS KILN WITH PREHEATER , 1800 TPD, DIAMETER 4,6M
FIRST TYPE OF CLINKER : Q2 / S = 4,9 Gcal/hm2
SECOND TYPE OF CLINKER, Q2 / S = 5,4 Gcal/hm2
AG AF BETWEEN 7 TO 16M, stable coating starting from 12/14M
LTZ LIFE TIME : 6 months with relative stable coating
LIFE TIME : 3 months with 2 weeks operation without coating
CONCLUSION : Q2 / S > 5,3 Gcal/hm2
BECOMES CRITICAL WITHOUT COATING
KILN THERMAL LOAD IN BURNING ZONE
COMPARISON BETWEEN THE KILNS IN Gcal/hm2 :
Q2 / S < 4 : LOW TO NORMAL THERMAL LOAD
4 < Q2 / S < 4, 5 : NORMAL THERMAL LOAD
4,5 < Q2 / S < 5,3 : HIGH THERMAL LOAD
Q2 / S > 5,3 : HIGH TO EXTREME HIGH THERMAL LOAD
1950 1960 1970 1980 1990
3
4
5
1000
2000
3000
5000
6000
7000
8000
4000
hmGcal
2
tpd
specific heat average load in the sintering zone
kiln efficiency
kiln efficiency with precalciner
KILN THERMAL LOAD EVOLUTION
KILN THERMAL LOAD IN BURNING ZONE
IN BELGIUM :
1640tpd, POLYSIUS PREHEATER KILN , Q2 / S = 3,8 Gcal/hm2
4600tpd, POLYSIUS PRECALCINER, Q2 / S = 4,3 Gcal/hm2
Same fuels , bricks B322/B622 on both kilns
According to the production manager: the flame is stronger on kiln 3 than on kiln 4
Life time of bricks in LTZ : Kiln 3 : RG 85/ RG AF = 9 months hot spotsKiln 4 : AG AF = 12 months ( remaining thickness 150 to 200mm )
THERMAL LOAD IS ONE CALCULATED PARAMETER,BUT FLAME CONTROL IS A NON QUANTIFIED PARAMETER
WHICH IS MORE CRITICAL
GAZ FLAME : WITHOUT CONTROL
)()()/()/()/()/()()()( smskgsmskgNNN
VrQmrVaQmaGxrGxaGx +=+=
)()()/()/()/()/()()()( smskgsmskgNNN
VxrQmrVaQmaGxrGxaGx +=+=
)/()()/(/
hrGcalNGcalNS PGxI =)/()()/(
/hrGcalNGcalN
S PGxI =SPECIFIC FLAME MOMENTUM
BURNER IMPULSE , FLAME MOMENTUM , FLAME INTENSITY :IMAGE OF FLAME HARDNESS
BE CAREFUL, THERE ARE DIFFERENT WAYS OF CALCULATION (with or without fuels streams ) :
FORMULA USED BY LAFARGE, PILLARD ETC..
AXIAL FLAME MOMENTUM : IT IS THE FORCE OF THE AIR STREAMS IN THE KILN AXIS
SPECIFIC FLAME MOMENTUM WITH THE SAME WAY OF CALCULATIONSMUST BE USED FOR COMPARISONS
)/()()/(/
hrGcalNGcalNS PGxI =
)(3)(2
33
33
rirerirerg
=
SWIRL NUMBER : ROTATION INSIDE THE FLAME
BE CAREFUL, THERE ARE DIFFERENT WAYS OF CALCULATION :FORMULA USED BY LAFARGE, PILLARD ETC..
tgGxrGtNN=
)()(Radial air momentum : taking into account the radial air angle
)(3)(2
33
33
rirerirerg
=
)()(2
GxmQmrQmaDe
+=
GxDergGtSN
=
De is the orifice diameter through which can pass a gaseous flow Qv with a momentum of GX
rg : gyration radius of swirl channel
TYPICAL VALUES
LOW NOx GENERATION BURNERS : LOW PRIMARY AIR BURNERS
SPECIFIC AXIAL AIR MOMENTUM : 3 to 5 N / MWSWIRL : 0,4 to 0,5PRIMARY AIR PERCENTAGE : 4 to 8%
HIGH IMPULSE BURNER : SHORT FLAME BURNERS
SPECIFIC AXIAL AIR MOMENTUM : 8 to 12 N / MWSWIRL : 0,1 to 0,2PRIMARY AIR PERCENTAGE : 8 to 12%
)()()/()/()/()/()()()( smskgsmskgNNN
VrQmrVaQmaGxrGxaGx +=+=
PROBLEMS WITH HIGH IMPULSE BURNERS FOR BRICKS
WITH HIGH IMPULSE LOW OR IMPULSE BURNERS : THE THEORITICAL THERMAL LOAD IN THE BURNING SECTION ( Q2 / S ) REMAINS THE SAME
)()()/()/()/()/()()()( smskgsmskgNNN
VrQmrVaQmaGxrGxaGx +=+=
BUT THE HEAT TRANSFER PROCESS IS DIFFERENTIE THE TEMPERATURE PROFIL IS DIFFERENT
THE PROBLEM FOR BURNER MANUFACTURERS WAS TO COMPACT THE FLAME VOLUME :IN THE PAST, THE FLAME WAS LONG AND SHARP
OR SHORT AND LARGE
BURNER MANUFACTURERS HAD TO WORK ON NEW DETAILED DESIGNS( BY KEEPING OPERATING PRINCIPLES )
FOR FIRING PETCOKE AND ALTERNATIVE FUELS THEY SHOULD CALLED THEM MAS AF, PYROJET AF, ROTAFLAM AF etc..
SINTERING ZONE, FLAME SHAPE WITH LOW IMPULSE BURNER
WITH HIGH IMPULSE BURNER
~16 m Flame !!
~23 m Flame
!/!
HOLCIM IN SWITZERLAND : CHANGE OF FLAME LENGTH
HIGH IMPULSE BURNER : IMPACT ON SINTERING ZONES BRICKSSTABLE COATING IS THE BEST PROTECTION OF THE BRICKS IN SINTERING ZONE
WITH HIGH IMPULSE BURNERS, THE SINTERING ZONE IS SHORTENED WHICH MAY CREATE PROBLEMS IN THE SELECTION OF BRICKS IN THIS ZONE
SINCE COMMISSSIONING, STABLE COATING ENDS AT 19/20M
LIFE TIME OF RG 85 BETWEEN 19 TO 29M : 7 TO 9 MONTHS
REPLACED WITH ALMAG 85 : LIFE TIME 1 YEAR ( running at 6000 tpd )
5000 TPD ( 4,75 * 74,2m ), FLS PRECALCINER KILNS WITH HIGH IMPULSE DUOFLEX BURNER
AT THE DESIGN STAGE THE FOLLOWING SELECTION WAS MADE WITH FLS :
0 to 0,4M : KRONEX 850,4 to 9M : ALMAG 85
9 to 29M : REFRAMAG 8529 to 41M : ALMAG 85
LAVA LIKE COATING : OVERHEATING
PROBLEM OF RAW MATERIAL PREPARATION ( IRON ORE ..)
PROBLEM OF BURNER ADJUSTMENT :LOCAL WEAR : ORIENTATION OF BURNERFOR SOME METERS : HEAT INPUT IS TOO HIGH
COMBUSTION : IMPACT ON UPPER TRANSITION ZONE AND UPSTREAM BRICKS
MAIN IMPACT, AS THE SINTERING MAY BE SHORTENED,THE POSITION OF THE UTZ IS CHANGED
SELECTION ON THE BRICKS HAS TO FOLLOW THIS NEW POSITION
IF THE COMBUSTION OF SOLID FUELS IS NOT MASTERED IN THE FLAME ( INSUFFICIENT MIXING, TOO COARSE etc.. )
SOLID FUELS CAN FINISH BURNING ON THE BRICKS
LOCAL REDOX CONDITIONS ON THE BRICKS
PROBLEMS WITH HIGH IMPULSE BURNERS FOR BRICKS
)()()/()/()/()/()()()( smskgsmskgNNN
VrQmrVaQmaGxrGxaGx +=+=
BURNER MANUFACTURERS HAD TO WORK ON NEW DETAILED DESIGNS
( BUT THEY KEPT THE BASIC PRINCIPLES OF OPERATION )
FOR FIRING PETCOKE AND ALTERNATIVE FUELS
WE COULD CALLED THEM MAS AR, PYROJET AR, ROTAFLAM AR etc..
HOLCIM UNTERVARZ CEMENT PLANTVision of a new mega burner
Household waste
Coal
Paper
Carboard
Wood
Waste oil
Contaminated water
Tetra pack
Plastic waste
Liquid waste
Heavy fuel oil Low calorific gas
Distilation residues
ROTAFLAM 125 MW for CEMENTOS APASCO / HOLCIM / Mexico
Axial air channel
Radial air channel
Petcoke channel: 14.000 kg / h
Solid waste: 9.000 kg / h
Natural gas: 6.240 Nm/ h
Heavy fuel oil: 11.300 kg / h
Waste oil: 9.170 kg / h
WASTE FUEL FIRING : REAR PART OF A UNITHERM MAS BURNER
MIXING OF ALTERNATIVE FUEL IN BURNER CENTER
ROTAFLAM FLAME ADJUSMENT WITH A TEST TEST BURNER
ROTAFLAMROTAFLAM SMALL SCALE TESTSMALL SCALE TEST
ROTAFLAM CFD SIMULATION WITH CFD SIMULATIONQ AIR RADIAL = 840 Nm3/h Q AIR RADIAL = 5700 Nm3/hQ AIR AXIAL = 7000 Nm3/h Q AIR AXIAL = 2700 Nm3/h
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Previous Design:1) Long axial excess at burner tip2) Divergent axial air outlet3) 45 Divergence of swirl air4) 40 Swirl angle for swirl airPrimary air pressure: 160200 mbarPrimary air amount: 6-8%Split Axial / Swirl: 40 / 60 Axial impulse: 2,8-3,8 N/MWSwirl number: 0,4-0,5
New Design:1) Minimum axial excess at burner tip2) Axial air outlet axis parallel 3) Reduced divergence of swirl air4) Reduced swirl angle of swirl airPrimary air pressure: 250 mbarPrimary air amount: 8-12%Split Axial / Swirl: 65 / 35 Axial impulse: 8-12 N/MWSwirl number: 0,1-0,2
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ROTAFLAM TIPS DESIGN MODIFICATIONS
ISFAHAN CEMENT : GAZ BURNER WITHOUT CONTROL ( VERY LOW IMPULSE )
ISFAHAN : MULTICHANNEL GAZ BURNER( LOW IMPULSE )
ISFAHAN : HIGH IMPULSE BURNER
COMPARISON OF TWO FLAMES WITH MULTICHANNELS BURNERS
LOW IMPULSE WITHOUT CONTROL HIGH IMPULSE UNDER CONTROL
Burners - Influence of flame and flame shape on the refractoryliningWHAT IS COMBUSTION ?COMBUSTION IS NOT COMBUSTION REACTIONSCALORIFIC HEAT VALUERELATION BETWEEN HHV AND LHVMAIN NOBLE FUEL CLASSIFICATION PER LHVALTERNATIVE FUELS : WHY IN A CEMENT PLANT ?DEFINITIONS ABOUT AIR OTHER DEFINITIONS :DEFINITION OF FLAME LENGTHINFLAMMABILITY LIMITSWHAT IS FLAME TEMPERATURE ?SOME ADIABATIC FLAME TEMPERATURESCOAL ANALYSISCOAL ANALYSISIGNITION OF ANTHRACITE COMPARED TO STEAM COALSPECIFICITIES OF COMBUSTION IN CEMENT KILNSSPECIFICITIES OF COMBUSTION IN CEMENT KILNSSPECIFICITIES OF COMBUSTION IN CEMENT KILNSSPECIFICITIES OF COMBUSTION IN CEMENT KILNSTEMPERATURE PROFIL :FLAME TEMPERATURE : FLAME WITH LIGNITE AND WASTESFLAME TEMPERATURE : LIGNITE AND WASTES FIRINGMAIN MULTICHANNEL BURNER MANUFACTURERS UNITHERM MAS BURNERSWIRL SETTING DEVICE FOR PRIMARY AIRPILLARD ROTAFLAM BURNERPILLARD ROTAFLAM : ADJUSTMENT OF AIR CROSS SECTIONSFLS DUOFLEX BURNERFLS DUOFLEX BURNER : AIR CROSS SECTIONS ADJUSTMENTSKHD : PYROJET BURNERSGRECO ENFIL BURNERS SPECIFICITIES OF COMBUSTION IN CEMENT KILNSSPECIFICITIES OF COMBUSTION IN CEMENT KILNSSPECIFICITIES OF COMBUSTION IN CEMENT KILNSSECONDARY AIR INJECTION AT BURNER TIPSPECIFICITIES OF COMBUSTION IN CEMENT KILNSRELATIONS BETWEEN BRICKS AND BURNERRELATIONS BETWEEN BRICKS AND BURNERHEATING UP : RISK WITH POOR FUEL OIL PULVERISATION (1)HEATING UP OF THE KILN WITH HEAVY FUEL OIL (2)NEW LINING AFTER 8 HOURS HEATING UP TO 1000cRELATION BETWEEN FLAME INTENSITY AND CLINKERKILN THERMAL LOAD IN BURNING ZONEKILN THERMAL LOAD IMPACT ON LOWER TRANSITION ZONE BRICKSKILN THERMAL LOAD IN BURNING ZONEKILN THERMAL LOAD IN BURNING ZONEKILN THERMAL LOAD IN BURNING ZONEGAZ FLAME : WITHOUT CONTROLTYPICAL VALUESPROBLEMS WITH HIGH IMPULSE BURNERS FOR BRICKSHIGH IMPULSE BURNER : IMPACT ON SINTERING ZONES BRICKSCOMBUSTION : IMPACT ON UPPER TRANSITION ZONE AND UPSTREAM BRICKSPROBLEMS WITH HIGH IMPULSE BURNERS FOR BRICKSWASTE FUEL FIRING : REAR PART OF A UNITHERM MAS BURNERMIXING OF ALTERNATIVE FUEL IN BURNER CENTERROTAFLAM FLAME ADJUSMENT WITH A TEST TEST BURNERROTAFLAM CFD SIMULATION WITH CFD SIMULATIONQ AIR RADIAL = 840 Nm3/h Q AIR RADIAL = 5700 Nm3/hISFAHAN CEMENT : GAZ BURNER WITHOUT CONTROL ( VERY LOW IMPULSE )ISFAHAN : MULTICHANNEL GAZ BURNER ( LOW IMPULSE )ISFAHAN : HIGH IMPULSE BURNERCOMPARISON OF TWO FLAMES WITH MULTICHANNELS BURNERS