87
Burners - Influence of flame and flame shape on the refractory lining Alain Czaplinski

Burners Czaplinski 2006

Embed Size (px)

DESCRIPTION

About combustion in Kiln

Citation preview

  • 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

  • 1 2 43

    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

    1 2 43

    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