Prog.EnergyCombust.Sci.,Vol. 2,
pp.129-141,1976.PergamonPress.Printed in GreatBritain FLARI NGI
NTHEENERGYI NDUSTRY T . A . B R Z U ST O WSK ITh erma l
EngineeringGroup,Dep a rtmentofMech a nica l Engineering,Univ
ersityof Waterloo, Waterl oo,Ontario,CanadaN 2 L 3
GIAbstraet--Flaring is thecombustion processused for the
safedisposal of largequantities of flammable gasesand vapoursin
thepetroleum industry. This paperisacriticalreviewof thetechnology
of flaring and of the state of knowledge on whichdesign information
canbe based.Discussion includes the length and shapeof
theflameonanelevatedflare,itsradiationfield,aswellasnoiseandairpollution
from flares. NOTATIONSreleasedtotheflare,andvariouskindsofnoi se--
CL =leanlimitconcentrationofflaregasinair,volumeparticularly
thenoiseofsteam j etsandlow-frequency fractionvibrations ofthe
flare system. d=diameterAthoroughunderst andi ngofallthesephenomena
F=fraction of heat releaseradiated by the flameis now required
forthe design of modernflare systems, which are generally larger
and, at the same time, subject F r-~ gd~U~\ P ~ - P f / ( Pl
tdensityFrudenumber foraflame of constanttomuchstricterregulationst
hantheirforerunners. L=flame length measured from the nozzle along
the flameThe design guidelines which have evolved over the years
axisfromexperiencewithsmallerflaresmustbeputona M=- pu 2 momentum
fluxfirmbasis,andreliablemethodsforextrapolationin =molecular
weightbot hsize and performance mustbe developed. ~h=mass flow
p=densityThepurposeof thispaperistoassistthisdevelop- R= - M J M ~
ment intwoways.Itiswrittenbothtoacquaint s=curvilinear coordinate
along flameaxisfromtheflarecombust i on specialists
withtheparticularcombust i on
tipproblemsencounteredinflaring,andtointroduce S=- s/ ( d j
R~)engineers whospecify anddesignflaresystemstothe u=velocity
x=horizontal coordinate downwind from the
flaretipresearchresultswhichbearonthesecombust i on X=mole
fractionproblems. A critical descriptionof anumber of generic X=- x
/ ( d~R )andproprietarydesignsofflareswhichareavailable
z=verticalcoordinate upward from the flare
tipfromtheprincipalsuppliersintheworldmarketis Z=z / ( d j
R~)presentedforthebenefit ofbothgroupsof readers. Subscripts
f=flame i=i' th component of flare gas mixture2.THENEED FORFLARING
j=flaretip dischargeconditions L=lean limitThe flaring of gases in
the petroleum industry occurs =ambient
airinthreeways.First,thereisarequirementforsafe
I.INTRODUCTIONdisposal of f lammable gases in connection with
produc- ingoilfields, inthosecaseswherenoprovisionexists Flaring is
the combust i on processwhich has been thefor collecting and
processing the gas.Therewasatime
traditionalmethodforthesafedisposaloflargewhenalmostallgasreleasedinthiswaywasflared,
quantities of unwant ed f lammable gases and vapours inbut the
great value now placed on nat uralgas has made
theoilindustry.Withtheadventofairqualitygasrecoveryeconomicalinmanyfields.Nevertheless,
standards,flaringhasalsotakenonanaddedif
thegasoccursinquantitieswhicharetoosmallfor
importanceasamethodofindustrialenvi ronment al economical
processing or if it is so sour thatprocessing
control,sincemostgaseswhichcouldpreviouslybeit wouldbe very
expensive, itmaystillbeflared.Such ventedtotheatmospheremust
nowbeburnedinaflaring is usually called product i on flaring.
flare.Flaring alsotakesplaceinpetrochemicalplants,oil
Flaringhasonlyrecentlyattractedtheat t ent i
onofrefineriesandgasprocessingplantswheretheflare combust i
onscientists.Itisnowrecognizedthatcorn-systemisoneof
thes0-called"offsite"facilities.Pro- bust i oninthec
ommonelevatedflareoccursinacessflaringandemergencyflaringcanoccurinthis
turbulent diffusion flame in across-wind.Suchaflamesetting. I n
processflaring, the gaswhich leakspastthe presentsanumberof
fascinatingandchallengingsafetyvalvesprotectingthevariousprocessunitsis
phenomena for study, including:the effect ofcross-windbrought to
the flare and burned. This gas feeds the small on its shape an d
length, its radi at i on field, the f ormationflames which burn
almost continuously on refinery flare anddispersionof
smokeandgaseouspollutants,thestacks.Processflaring atmuch
greaterratescanoccur act i on of steam in suppressing the f
ormationof smoke,when processunitsareevacuatedduri ngashutdown
thecompletenessofcombust i onofanytoxicgasesor when
off-specification productsare produced duri ng 129
130T.A.BRZUSTOWSKI tFxG. 1.Principalelementsof a' steam-ring'
smokelessflare
tip:(1)high-temperaturealloytip,(2)refractorylining,Steam
(3)pilotlight,(4)nozzleliporperforated' flame-holder' ,I nl
et(5)centre-steamnozzle,(6)steam-ringheader,(7)steam-Fl~.2a.Principalelementsofthe
Flaregas FS Antipollutant ringnozzle,flaretip. start-up.Emergency
flaring occurs whenlargevolumesorderof
magnitude.Ontheotherhand,processflaring ofvolatileliquidsorf
lammablegaseshavetoberatesareusuallynomorethanafewpercentof the
disposedof safely in an emergency suchas afire,
poweremergencyflaring rates.
failure,coolingwaterloss,compressorfailure,over-Agoodintroductiontothesystemsavailablefor
pressureinaprocessvessel, etc.processandemergencyflaringisgiven
byJones. Underemergency conditions, the flaring ratethrough asingle
refinery flare mightbeof theorderof 105 kg/
h,3.THETECHNOLOGYOFFLARING withaheatreleaserateof theorderof1000
MWfor afew minutes.ThelargestflareinstallationscanreachThemostc
ommontypesoftipsforelevatedflares
flaringrateswhichareevenhigher,perhapsbyanare shown in
Figs.1-5andare describedin TableI. The Air ~ AirSteam and ai r
mixture / N'ji FIG. 2b.Detail of theCoandanozzle which induces air
intothe conicalmixing section. Flaring in the energy industry131 i
FXG. 3.PrincipalelementsoftheIndairSmokelessFlare:"1[II (1) conical
nozzle inside contoured burner tip, (2) adjustable annular
nozzleforh.p.gas,(3)h.p.gasnozzleadjustment
mechanism,(4)annularh.p.gasduct,(5)l.p.gasduct,FIG. 5.Principal
elementsoftheZink Series SA Field Flare (6) pilot
lightassembly,tip:(1)ejectortubescarryingsteamandinducedairinto the
flame, (2) ejectorentrance nozzle,(3) steam-ring header
firstfigureandtablerefertothreegenericdesignsofandnozzles,(4)
centre-steam nozzle,(5)acousticalshroud.
flares:the"utility"flare,the"centre-steam"flareand
the"steam-ring"flare.Figures2,3,4and5andseveralofthefiguresarebasedondetaileddrawings
Table1-Dreferstofourproprietaryflaredesigns.Thepresentedinthesalesliteratureof
someofthemanu- tablescont ai nself-explanatorycommentsabout
thefacturers;therestaretheauthor' srendition basedon
constructionandtheparticularadvantagesanddis-thefarlessdetaileddat
areleasedbytheother advantagesofalltheflares.Flaretipsof
thesedesignsmanufacturers. are generally available forflare
stacksvarying betweenFigure6andTable. 2refertogroundflares.Other
0.4and1.2mindiameter,but
someflarestacksofgroundflares,inparticularthe"Multij et"flare 1.8
mhavealsobeenbuilt.Itshouldbenotedthatdeveloped by the ( now)
ExxonResearchandEngineer- ingCompany, aredescribedindetailbyJones.
1A somewhatsimilardesignisalsoofferedbyAlphons
CustodisK.G.ofDiisseldorf.Typicaldesignheat
releaseratesforgroundflaresofthetypeshownin
Fig.6lieintherangefromlessthan1 MWtomore than100MW,
withaflareheightoftheorderof 10-20 m. FIG. 4.Principal
elementsoftheSmoke-BanModelSVLFIG. 6.Principal elements of atypical
ground flare: (1) ex- flare tip: (1) shroud, (2) steam-ring
header,(3) hollow spokesterior frame, (2) refractory lining, (3)
flare gas header,(4) flare carrying gas from the central duct
totheradialslit nozzles,gas burners, (5) pilot lightswith an
independent gassupply, (4) pilot light.(6) louvred enclosure. J PEC
S Vol . 2,No. 3 - - B 1 3 2 T . A . BRZUSTOWSKITABLE 1.Tipsfor
elevatedflaresditionsmayproducebot hj etnoiseand low-frequency
noise (chugging) A."Utility" flare
tipssteamringandnozzlesaresusceptibleto damagebyflameintheabsenceof
steam ConstructiontipasinFig.1butwithoutcentresteamflow nozzle5,
steamring6orsteamnozzles7Availability- - f r omseveralsuppliers - -
may havewindscreens surroundingtipof e.g.NationalAiroilNRC
flareSamiasmokeless flare Advantages--c heap,quiet,requires no
utilities except forZinkseries STF-S ignitionsystem andgasforpilots
- -mi ni mumofpartsexposedtothe flameD.Proprietaryandspecial
purposeflaretips Disadvantages - -no provision for smoke
suppression, can be usedforflaringH2,CH4,H2SandCOFLAREGASSERIES
FSANTIPOLLUTANT FLARE TIP butevensmallproport i onsof
heavyorConstructiontipasinFig.2a.Principalfeatureisa
unsaturatedhydrocarbonscausesmokingperf
oratedconicalmixingsectioninto Availabilityf
rommostsupplierswhichairisentrainedbysteam-driven e. g. --Flaregas
series FNCoanda j etejectors (detailinFig.2b) --Nat i onal
AiroilNCGAdvantagesconfinedmixingof hydrocarbonwith --Sami ast
andardflaresteam and induced air leads to very efficient --Zi
nkseriesSTF-Usteamuse - - st eamwall j etsintheCoandaejectorsare
muchquieterthansonicsteamj etsfrom B."Centresteam" flaretipsnozzles
intypicalsteam-ring designs Disadvantages - -expensive construction
Constructiontip as in Fig.1 butwithoutsteamring6or--openi
ngsinmixingsectionmaycause steamnozzles 7problems with flame
stability atlow flaring - - may havewindscreens surroundingtipof
ratesinastrong wind flare Advantages--c
heapestprovisionforsmokesuppressionINDAIRSMOKELESSFLARE (
GKNBirwelco) forinstallationsinwhichonlysmall Construction- - t i p
as inFig.3.Principalfeatureisatulip- quantitiesof
heavysaturatesandany unsaturatesareflaredshapednozzle with
low-pressure gasflow- - h y dr oc ar b ons andsteamarewellmixedingt
hroughitandhigh-pressuregas atlow flaring rateseven
inastrongwindflowingoverit.Theh.p.gasremainsina - - st eamnozzlenot
susceptibletoflamewallj etandfollowsthecurvatureof the nozzlewall(
Coandaeffect) whileentrain- damageintheabsence ofsteamflow
ingair.The1.p. gasburnswithinh.p.gas Disadvantages - - st eam is
not usedtoentrainairintoflame,flame as a result a greater proport i
on ofsteamto Advantages--speci al purposeflareforproduci ng fields,
hydrocarbonisrequiredforsmokesup- pression t haninothersmokeless
flaresoff-shore rigs, etc.,whereh.p.gasisavail- -steam noise is
possible at peaksteam flows,able depending on location anddesign
ofsteam--ent rai nment of airintoh.p.wallj etis
nozzlerelativelysilentandefficient,smokeis suppressed,
flameluminosity islow Availability- - f r omseveralsupplierswall j
etofh.p.gascoolsnozzlewall,high e. g. --Flaregas
seriesFCtemperaturematerialsareunnecessary --Nat i onal AiroilNCS-
- maybe operated vertically orhorizontally, - - Zi
nk(notadesignatedmodel)withsignificant liquid carry-over
Disadvantagescannotbeusedunless h.p.gasisavailable --devel opment
toreplaceh.p.gasbysteam C."Steamring"
flaretipsseemspossible,butitmaycompromise combustionperf ormance
since the1.p. gas Construction- - t i p as in Fig.1, some designs
do not includej etwillnotbe surroundedbyaflame the
centresteamnozzle5 Advantages--c heapest
provisionforsmokesuppressionSMOKE-BANMODEL SVL
forinstallationsinwhichlargeflowsofheavysaturatesandunsaturatesmaybeConstruction-
- t i pasinFig.4.Principalfeatureisa flaredconverging-diverging
conicalshroud.The - - steamisusedtoentrainairintotheflame,flared
gas flows from the stackintoacentre lowering the proport i on
ofsteam to hydro-bodyfrom whichitemergesthroughslots carbon
forsuppression ofsmokeinradialspokes.Steamnozzlesmount ed - - wh en
fitted with a centre steamnozzle,
canonasteamringundertheshroudinduce be usedover
widerangeofflaringratesanairflowoverthespokesinsidetile - - t h i s
is the smokeless flare most widely usedshroud
inrefineriesandpetrochemicalplants,Advantageslarge area for mixing
the hydrocarbon with provendesignsavailablefromseveralairandsteam
vendors- - st eamusedeffectivelytoinduceairflow Di s adv ant ages
-steam ringmaybenoisy (jet noise) athighinside shroud smokeless
flaring rates- - sh r ou dprovidessomeacousticalshielding - - st
eamringaloneisnotveryeffectiveforfor thesteamnozzles
lowflaringrates,particularlyinastrong--l argecapacityfor smokeless
flaring wind,excessivesteamuseatthesecon-Di sadvant ages--expensi
ve construction Flaring inthe energy industry133 TABLE
1.Continuedof water sealswhichdivert gastotheelevated flare when
the ZTOF is operating at capacity.The system ZINK
SERIESSASMOKELESSFIELDFLAREoffersunobtrusiveburningatcapacitylevels
sufficientforroutineplant-wideflaring,withthe Construction--t i
pasinFig.5.Principalfeatureisthe location of the
steamringunderashroudstand-by capacity of an elevated flare for
emergency near the bottom of the flare tip. The steamflaring.The
one drawbackof thissystemisitshigh cost.
nozzlesaredirectedintoejectortubes
whichcarrytheinducedairflowthrough the tip up to its exit plane,
where the steam- airflowmixeswiththehydrocarbon.ATABLE 3.Suppliers
of flare equipment centre-steamnozzle is providedbelow the
steamringFlaregasEngineeringLimited,BentinckHouse,Bentinck
Road,WestDrayton,Middlesex, EnglandUB7 7SJ Advantages--large area
for mixing the hydrocarbon
withGKNBirwelcoLimited,MucklowHouse,MucklowHill, airandsteam
--steamusedeffectivelyin air ejectorsHalesowen,
WestMidlands,EnglandB628DG --shroudprovides some acoustical
shieldingNationalAiroil BurnerCompany,1284 EastSedgleyAve., for the
steamnozzlesPhiladelphia,Pa.19134, USA
--largemaximumcapacityfor'smokelessSamia,S.p.A., 20145Milano-Via
Guerrazzi,27, Italy flaringSmoke-Ban Manufacturing, Inc., 711 E.
Curtis St., Pasadena, --centre-steamnozzlegivesgoodper-Texas,77502,
USA formance atlow flaring ratesJohnZinkCompany,P.O.Box7388,
Tulsa,Oklahoma, Disadvantages -- expensive construction74105, USA
TABLE 2.Groundlevel flaresTable3isalisting
oftheprincipalsuppliersof flare equipment.Anumberof
othercompaniesalsobuild Construction- a s
inFig.6.Theprincipalfeatureisaflares,
buttheygenerallyusetheflaretipsandcontrol
refractory-linedelevatedductstanding
insidealouvredenclosure.Anumberofsystemsprovidedbytheprincipalsuppliers.
small burnersismountedonheadersandFlares are also used in other
types ofchemical process
providedwithpilotburnersusinganin-plants,e.g.heavywaterplantsusingtheH2Scycle.
dependentgas supplyTheyarealsof oundinsteelmillswhereoff gasfrom
Advantages-- cheap and unobtrusive, small ground flaresthe basic
oxygen furnace andother gases mighthaveto may be built among
process units and closebeflared.I
nwhatfollows,however,theemphasiswill to property lines because the
flames are notbeonflaring inthepetroleumindustry.
visible,combustionissmokelessand radiantheating is minimum
--manywellseparatedsmallflamesare
inherentlycleanerthanasinglelarge4.CURRENTPROBLEMS INFLARING
diffusionflame --good design of
theindividualburnerscanThreekindsofproblemsareassociatedwithflaring:leadtosmokelessburningoverawideturn-economi
cproblems,environmentalproblemsand downratio
--turn-downratiocanbeincreasedbysafetyproblems. staging the gas
flow to headersOneeconomi c probl em is simply the lossofvaluable
--utilitiessuchassteamoraircanbeusedmaterials.Itis
generallythou~ghtthatprocessflaring to burndifficultmaterials
cleanlyleadstoalossof anaverageof about
0.15-0.5~oofDisadvantages--small capacity, compared to elevated
flares,feedstockinrefineriesandpetrochemicalplants.I na
Groundflaresoflargecapacitycoverarefineryof200,000bpd(barrelsperday)capacityand
large landarea
--requireextremereliabilityofflame-outwithcrudeoilat$11perbarrel,thiscouldmeana
protectionwhenburningtoxicgasesordailylossofasmuchas$11,000.
gasesheavier thanairsince
dispersionbyTheenvironmentalproblemsassociatedwithflaring
windatthetopof astackis notavailableareprincipallythoseof
airpollutionandnoise.Air in the event of flame-out --i nmany
designsthe burnersare setupforpollutionisprimarilyinthef ormof
visiblesmoke. cleancombustionof specificgases,there-However,
unburnedhydrocarbons, SO2,andNOxare
foretheflarecanbeusedforroutinepossiblepollutantswhoseappearanceisfarlesscon-
flaring associated with given process units,spicuous.I nthecaseof
H2Sflares,thedispersionof butnot for plant-wide emergency
flaringthistoxicgasastheresultof anyincompletenessofAvailability--
from mostsupplierscombust i on may be a problem. The potentially
far more e.g.--Flaregas GroundFlaresseriousprobl emof f
lame-outonanH2Sflareisvery --NationalAiroil NPAC --ZinkZTOF (see
note)unlikely to arise because the pilot light systems usedon
flareshavebeendevelopedtoaveryhighlevelofN ore- - The
ZinkZTOFisagroundflare of large capacityreliability.For
example,ithasbeenshownthatpilot
intheformofatallcylindricalstackoflargelights on ahydrogenflare
haveprovidedignitionupto
diameterstandingongrade.Withfourstagedwindspeedsof134km/ h. 2
Oncetheflame wasignited, burnersmountedatthe base, the ZTOFisinmany
ways similar to an induced-draft furnace.The ZTOFwindsupto176 km/
handsimulatedrainof 114 mm/ h is integrated with an elevated flare
througha systemfailedtoextinguishit. 134T.A. BRZUSTOWSKI To
suppress smoke formation in processflaring,it
isprecisebutactuallyinvolveunprovenformulaefor customary toinject
steamintotheflared gas.Variousbasic quantities suchasflame length,
flamedeflection waysof doing this weredescribed in the Tables
above,in awind, etc.Someof theseformulae arereasonable Theamountof
steamperunitmassofhydrocarbonguessesbasedonexperience,butsomeothersare
depends both on the type of hydrocarbon (least for
lightquestionableAsummarydesignguideforflaresys-
saturatedhydrocarbons,increasingwithmolecularterns,contained
intheAmericanPetroleumInstitute weight and degreeofunsaturation,
most for aromatics)GuideRP521, 8 acceptsmanyoftheserecommenda-
andonthedesignoftheflaretips.Inpractice,thesetions uncritically
Theaccuracy of thisdocument itself
ratiosrangefromsome0.2kgsteamper1 kghydro-is questioned by
Heitner.9 carbontoover1 kgsteamperkghydrocarbon.This
processofsteamadditionistheprincipalsourceof5.1.Ch oi ceo f T i p D
i a m e t e rnoise in processflaring. Steam injection may produce
noise in two ways.TheThe choice of the flaretip diameter depends on
many first is jet noise associated with the high-velocity
steamfactors,includingthe performance of the pilot lights and
jets.(Someoftheflaretipsdescribedinthepreviousthe flame-holding
characteristics of the tip selected,the
sectionhavebeendesignedtominimizethiseffect)composition of
thegastobe flared,theavailability of The second is a more indirect
effect of the steam injectorpurge gastokeepair from entering
theflarewhen the processontheacousticsoftheentireflaresystem,flowof
flaregasisveryloworintermittent,1'11 and includingthe stack, the
liquid-seal drum in its base,
andtheturndownratiorequiredoftheflare.Ofthese
theflareheaders.Itismanifestinasub-audibleconsiderations,
theturndown ratioappearsnowtobe
vibrationatlowflaringratesandhighsteamflows,the most important
factor.Modern flaretipsandpilot which becomes an environmental
noise problem whenlights appearcapableofstabilizing flamesatgasdis-
it rattles windows in aneighbouring community Thischarge
velocitiesover100 m/s. Gas seals, such as Zink' s appearstobe j
ustoneof severallow-frequency noise"Molecular
Seal"andNationalAiroil's "Fluidic Seal" phenomena associated with
flares,havereducedtherequiredflowsofpurgegastovery
Combustionnoiseisnotgenerallyaprobleminlow values. 12
processflaring.However,atemergencyflaringcon-It is generally easier
topredict the maximum flaring ditions
whenthegasdischargesatsome100m/stherateatemergency
conditionsunderwhichparticular flame could be noisy. Itshould
benoted, though,thatprocessvesselshavetobedepressurized,thanitisto
in suchcircumstances themostseriousconcern isthepredict the minimum
rate of process flaring likely to be
safetyproblemcausedbythermalradiationfromtheencountered.
Nevertheless,the flare should be designed
flame.Theremayalsobemassive smoking, sinceitisin
suchawaythatthedischargevelocityof theflare
entirelyimpracticaltomaintainastandbysteamgasisaslargeaspossibleunderallconditions.
The capacityofsome105 kg/hwhichcanbeinstantlyreason for this
requirement is aerodynamic. diverted tothe flareduring an
emergency.Theparameterwhichgovernsthebehaviourofthe The principal
problem in emergency flaring is one
offlaregasjetinthecross-windintheregionnearthe
safety.PersonnelandsensitivestructuresmustbeflaretipisR-~M j / M ~
=p j uZ / p ~ u2 ~ , theratioofthe protectedfrom the intense
radiation emitted by alongmomentum flux in the jettothemomentum
flux of the bent-overflame(flamelengthsoftheorderof100mwind. At
sufficiently high values of R,the jetpenetrates
havebeenreported,byeyewitnesses,butnotrelatively
farintothecross-wind beforeitbends over. documented, in anumber of
emergencies atrefineriesAt the same time, the entrainment of air
into the jet near and petrochemical plants. Grumer et a l . 3 have
reportedthetipisveryrapid.Atlowvaluesof R,ontheother aflame90
mlongonaflare0.75 mindiameterdis-hand, the jet is shearedoff
atthedischargeorificeand charging hydrogen at 720 m/s). One way of
doing this isissuckedintothewakeofthetipwhereentrainment
to"sterilize"anareasurroundingtheflare.Atthisof air is very slowand
a lazy smoky flame is produced. point, the safety problem leads to
an economic problem.This effectof Risshown inFigs.7and8reproduced
The sterilizedspace can be very expensive,particularlyfrom
Reference13. 2forafixednozzle,flaregas,if it lies within a plant
which is surrounded by built-upSinceRvariesasmj areas and which is
being expanded to increase capacity,and wind, a turndown ratio of
1000 between the design emergencyflaringrateandtheminimumexpected
5.CURRENT STATE OFKNOWLEDGEprocess flaring rate through the same
tip means that the flamewillbehavesomewhatasinFig.8ratherthan
ThisdescriptionofthecurrentstateofknowledgeFig. 7 much of the
time.Smoke suppression under such on flaring iswritten
withreferencetotheneedsof theconditions
isaproblemwithatleastthesteam-ring "offsite"designer
whomustselectthediameterof theflaretip(see
Tablel-C).Ontheotherhand,Ralso
flaretip,andthendecideontheheightofthestack,variesas1/
d4atconstantvhj andgasandwindcon- and on the extent of the
restricted area around it.ditions.Thismeansthatiftwotipswereusedin
Severalarticlesonthedesignof flaresystems4"5'6'7conjunction, one of
themhaving dj fourtimes smaller appeared in the technical
literature in the1960s. All ofthan the other, a turndown in flaring
rate of 1000 could them suffer to some degreefrom the same
shortcoming,beaccomplishedatadecreaseofRofonlyabouta namely,
presenting calculations which appear to be veryfactor of four,
provided that only the small tip was used Flaring inthe energy
industry135 FIG. 7.Theturbulentdiffusionflame in a cross-wind: a
detachedflame athighratioRof jetmomentum fluxto
cross-windmomentumflux. Exposure for the flame
failstoshowthemodelflare whichislocated
attherightendofthexintervalmarkedunderthephotographs.Flamecross-sectionsarelong-time
averageshapesobtainedbyimmersingpaintedscreensintheflameforseveralminutes.Temperature
increasesfromthegraycolouroutsidethecontour,throughtheblackoutline,intothewhiteoxidized
region within.(FromReference13.)
atlowflaringrates.Itiseasytoseethatifbothtipswouldrequirethelargeflare.Bothflarescould,ofhadthesamedesigndischargevelocity,thesmalltipcourse,be
mount edononetowerorerectedasasingle couldhandleupto1/16of
designemergencyflaringstack,as
hasoftenbeendonewithso-called"sour-gas"
rate.Athigherflaringrates,theexcessflowcouldbeflaresalongsideregularflares.
directedtothelargerflarebyasystemof suitable
waterseals.Suchsystemsexistandarenotexpensive.5.2.Len#th and Shape
ofthe Flame If twotipswereusedinthisway,theratiooftheir
diameterswouldbechosensuchthatall ofthenormalTheheightof
theflarestackandtheextentofany
processflaringcouldbehandledbythesmallflarerestrictedareaarounditdependsonthelengthand
andonlyashutdownoremergencydepressurizationshapeof
theflameandtheradiationf romitunder d j =5m muj = 2 , ~ mls. . ~T=|
Se T=I / I 000sec dj3~2 8 4 3FIG. 8.The turbulentdiffusionflame in
a cross-wind: an attached flame at alow ratio Rof jetmomentum
fluxto cross-windmomentumflux. (FromReference 13.)
136T.A.BRZUSTOWSK! emergency flaringconditions.At themoment ,
thereisTABLE 4.Calculation of flame shapeandlength 16
nocompletelyreliable met hodofpredictingthelength
andshapeofafull-scaleturbulentdiffusionflameinaThemethodisbasedonthecold-flowcorrelationsof
cross-wind.AnalyticalmodelsbyEscudier 14andcncentratininwind'
blwnhydrcarbnj etslS Brzustowski 15basedonbent -overcircularj
etswith1.Requiredinformation: 54~, pj,uj, dj,CL, uo~, p~ , /
~top-hatprofileshaveyieldedsomeinsightintothe problem, but
muchmoreneedstobedonebeforea2.Calculatedimensionlesslean-limitconcentrationof
fuel reliable predictive procedureemergesf romthiswork.CL =Cd u/ u~
) ( ~ l / I 9 1)For themoment , theonlydesignprocedurewhich
3.Calculatethedimensionlessco-ordinateSLofthecon-
takesintoaccountthedeflectionoftheflamebywindcentrationCL on the
axisof the jet andfrom it the down-
inevenapproximatelyrealisticfashionisthemodelwindco-ordinateXL.
Thisco-ordinateisidentifiedwith proposedbyBrzustowski
16andelaboratedbythe location of the flame tip Brzustowskiand
Sommer.17The calculation procedure(i)if C'L 0. 5: SL=2. 51(
CL)-'62~ combinesthemeasuredcold-flowcorrelationsforif SL >2.35
,~L =SL- 1.65 hydrocarbonj etsincross-flow iswiththesuggestionif SL
~< 2.35 SL ~- 1.04 , ~ +2.05 .~o.2s t.oIn this case XL
asafunctionof SL isshowninFig.9 4.Calculate the dimensionless rise
ZL of the flame tip above the flare tipZL =2.05 .~o.2s
5.CalculatetheratioRof the jetmomentumfluxtothe
cross-windmomentumflux U22 R=( p j j ) / ( p ~ u ~
)046.Calculatethedimensionalco-ordinatesof theflametip relative ro
the flare tip zL=Z L d j R aleXL=X L d ; R1/2 i [ j ^N ot es :
(i)This procedureshouldnot be usedfor uj / u~ >llO (ii)For a
mixture of flammable gases,the leanlimit canoften be approximatedby
0.011/ CL=~(XI/CL,~) i components This equation is only an
approximation.CL = forinertcomponents.Steamisnotstrictlyan
inertandtheuseof thissimplemixingrulefor
hydrocarbon-steammixturesmaynotbeac- curate. o.12oiiLI 0 0 ' 5 I '
0 ~ L 1'5~=2 . 0 2 5afactorof two. 2I nthecaseof propane, theflame
FIG. 9.TherelationbetweenSL andXL for SL