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Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton, VA Jeffrey P. Slotnick The Boeing Company Seattle, WA Anthony J. Sclafani The Boeing Company Long Beach, CA AIAA SciTech, Kissimmee, FL, January 8-12, 2018 1

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Page 1: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

OverviewandSummaryoftheThirdAIAAHighLiftPredictionWorkshop

ChristopherL.RumseyNASALangleyResearchCenter

Hampton,VA

JeffreyP.SlotnickTheBoeingCompany

Seattle,WA

AnthonyJ.SclafaniTheBoeingCompany

LongBeach,CA

AIAASciTech,Kissimmee,FL,January8-12,2018 1

Page 2: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

Overview• GeneralsummaryofHiLiftPW-3results.• CFDcomparisonsagainstitself(consistency,verification).• CFDcomparisonsagainstexperiment(validation).

• HavethingsimprovedsinceHiLiftPW-2?• Whathavewelearned?• WhatshouldbedonedifferentlyforHiLiftPW-4?

AIAASciTech,Kissimmee,FL,January8-12,2018 2

Page 3: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

Outline• Introduction• Highliftgeometriesandexperimentaldata• Gridsystems• Summaryofentries• Results• Turbulencemodelingverification• HL-CRM• JSM

• Statisticalanalysis• Conclusions

AIAASciTech,Kissimmee,FL,January8-12,2018 3

Page 4: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

Wherewe’vebeen(somehighlights)• HiLiftPW-1(2010).• NASATrapezoidalWing-Body;includingeffectofflapdeflection.• CFDtendedtounderpredict lift;bigspreadnearstall.• NosupportbracketswereincludedintheCFD(whentheywere,predictedliftwasevenlower).• Transitionmodelingseemedtohelpimprovecomparisonswithexperiment.• Flownearwingtipwasverydifficulttopredict.

AIAASciTech,Kissimmee,FL,January8-12,2018 4

Page 5: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

Wherewe’vebeen(somehighlights)• HiLiftPW-1(2010).• NASATrapezoidalWing-Body;includingeffectofflapdeflection.• CFDtendedtounderpredict lift;bigspreadnearstall.• NosupportbracketswereincludedintheCFD(whentheywere,predictedliftwasevenlower).• Transitionmodelingseemedtohelpimprovecomparisonswithexperiment.• Flownearwingtipwasverydifficulttopredict.

AIAASciTech,Kissimmee,FL,January8-12,2018 5

Page 6: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

Wherewe’vebeen(somehighlights)• HiLiftPW-2(2013).

• DLR-F11Wing-Body;includingeffectofReynoldsnumber.• CFDsometimesunderpredicted,sometimesoverpredicted lift;againshowedbiggerspreadnearstall.

• Separationbehindslattrackswasprobablyinfluentialininitiatingstall;evenwhenincludingbrackets,CFDusuallygotitwrong(e.g.,separationbehindwrongbrackets).

• Nocleartrendswithtransitionmodelingstoodout.• Attainingsteady-stateconvergencesometimesdifficult.• ExperimentaloilflowswereextremelyusefulfordeterminingwhetherCFDwascapturingthephysicscorrectlyornot.

AIAASciTech,Kissimmee,FL,January8-12,2018 6

Page 7: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

Wherewe’vebeen(somehighlights)• HiLiftPW-2(2013).

• DLR-F11Wing-Body;includingeffectofReynoldsnumber.• CFDsometimesunderpredicted,sometimesoverpredicted lift;againshowedbiggerspreadnearstall.

• Separationbehindslattrackswasprobablyinfluentialininitiatingstall;evenwhenincludingbrackets,CFDusuallygotitwrong(e.g.,separationbehindwrongbrackets).

• Nocleartrendswithtransitionmodelingstoodout.• Attainingsteady-stateconvergencesometimesdifficult.• ExperimentaloilflowswereextremelyusefulfordeterminingwhetherCFDwascapturingthephysicscorrectlyornot.

AIAASciTech,Kissimmee,FL,January8-12,2018 7

Page 8: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

Quickcomparison

AIAASciTech,Kissimmee,FL,January8-12,2018 8

HiLiftPW-1 HiLiftPW-2 HiLiftPW-3

37submissions 48submissions 79submissions

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HiLiftPW-3geometriesandexperimentaldata

AIAASciTech,Kissimmee,FL,January8-12,2018 9

HL-CRM JSM

NotyetbuiltTestedinJAXA-LWT1inearly2000s- Notripping

ForcesMomentCpOilflowSometransitioninfo

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HiLiftPW-3geometriesandexperimentaldata

AIAASciTech,Kissimmee,FL,January8-12,2018 10

HL-CRM JSM

NotyetbuiltTestedinJAXA-LWT1inearly2000s- Notripping

ForcesMomentCpOilflowSometransitioninfoHiLiftPW-3alsopartnered

with thefirstGeometryandMeshGenerationWorkshop(GMGW-1),usingHL-CRM

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Committee-providedgridsystems

AIAASciTech,Kissimmee,FL,January8-12,2018 11

Averagemedium grid:approx 71Mpointsand120McellsMedianmedium grid:approx 52Mpointsand107Mcells

ForHL-CRMandJSM

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Summaryofentries• 35individuals/groupswith79entries.

• 14differentcountries(40%U.S.).• Broadrepresentationfromindustry,academia,CFDvendors,andgovernmentresearchlabs.

• Turbulencemodels:• MostusedSAorvariant(RC,R,neg,QCR,noft2).• K-omegatype:BSL,SST,SST-V,SST-V-sust,SST-2003,SSTwmods,Wilcox1988,Wilcox1988CC.• Lag-EB-ke.• SSG/LRR-RSM-w2012.

• Transitionmodels:• SST-gamma,AFT2017b,gamma-Ret-SST.

• Non-RANS:• FiniteelementwithimplicitSGSmodel.• LBwithVLESwallmodel.• LBwithWALESGSmodel.• DDES.

• Noteveryonesubmittedallrequestedcases.• Detailsinpaper.

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Results• Turbulencemodelingverification• HL-CRM• JSM

AIAASciTech,Kissimmee,FL,January8-12,2018 13

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Results• Turbulencemodelingverification• HL-CRM• JSM

AIAASciTech,Kissimmee,FL,January8-12,2018 14

DSMA661(ModelA)airfoil,M=0.088,alpha=0deg,ReC=1.2million(JFM160:155-179,1985)

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Turbulencemodelingverification

AIAASciTech,Kissimmee,FL,January8-12,2018 15

OnlycompletedforSAmodel(SA,SA-neg,SA-noft2)

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Theimportantroleofverification

2-Dverificationcase

VERIF/2DANWcasefromTMRwebsite:https://turbmodels.larc.nasa.gov

VerificationremovesonepossiblesourceofCFDuncertainty,foragivenmodel.Othersources:grid(size,extent,adherencetogeometry),BCs,iterativeconvergence.

AIAASciTech,Kissimmee,FL,January8-12,2018 16

8differentcodesproducenearlyidenticalresultsforSAmodel(CFL3D,FUN3D,Kestrel/COFFE,CFD++,OVERFLOW,BCFD,TAU,andLAVA)

Approximately30% ofthecodesthatrantheverificationcasewerefullyverified fortheSAmodel

Additionalverificationexercisesstillneededforothermodels,includingSAvariants

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Results• Turbulencemodelingverification• HL-CRM• JSM

AIAASciTech,Kissimmee,FL,January8-12,2018 17

Focusingononlyafewmainpointshere;furtherdetails(suchaseffectofflapgaptreatment)aregiveninthepaper

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HL-CRMgridconvergence(allresults)

AIAASciTech,Kissimmee,FL,January8-12,2018 18

alpha=8deg. alpha=16deg.

DragandmomentshowninpaperNote:bluecurvesrepresentgrid-adaptionresults

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Theimportantroleofverification

2-DverificationcaseHL-CRM

SAmodelsonly

BluelinespassedtheverificationtestforSA

VERIF/2DANWcasefromTMRwebsite:https://turbmodels.larc.nasa.gov

AIAASciTech,Kissimmee,FL,January8-12,2018 19

8differentcodesproducenearlyidenticalresultsforSAmodel(CFL3D,FUN3D,Kestrel/COFFE,CFD++,OVERFLOW,BCFD,TAU,andLAVA)

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Theimportantroleofverification

2-DverificationcaseHL-CRM

SAmodelsonly

VERIF/2DANWcasefromTMRwebsite:https://turbmodels.larc.nasa.gov

AIAASciTech,Kissimmee,FL,January8-12,2018 20

8differentcodesproducenearlyidenticalresultsforSAmodel(CFL3D,FUN3D,Kestrel/COFFE,CFD++,OVERFLOW,BCFD,TAU,andLAVA)

BluelinespassedtheverificationtestforSA

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HL-CRMvelocityprofiles

AIAASciTech,Kissimmee,FL,January8-12,2018 21

FLAP:x=1615,y=638 MAIN:x=1495,y=638

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Results• Turbulencemodelingverification• HL-CRM• JSM

AIAASciTech,Kissimmee,FL,January8-12,2018 22

Focusingononlyafewmainpointshere;furtherdetailsaregiveninthepaper

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JSM,nonacelle/pylon

AIAASciTech,Kissimmee,FL,January8-12,2018 23

Liftcoefficient Dragcoefficient Momentcoefficient

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JSM,withnacelle/pylon

AIAASciTech,Kissimmee,FL,January8-12,2018 24

Liftcoefficient Dragcoefficient Momentcoefficient

Page 25: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

JSM,deltasbetweennacelle/pylononandoff

AIAASciTech,Kissimmee,FL,January8-12,2018 25

Liftcoefficient Dragcoefficient Momentcoefficient

Exceptforoneoutlier,participantspredicteddeltaswell(albeitlargescatternearmaxlift)

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CFDresultsthatagreed“best”withJSMCL data

AIAASciTech,Kissimmee,FL,January8-12,2018 26

Nonacelle/pylon Withnacelle/pylon

Minimize!"Σ 𝐶𝐿, 𝐶𝐹𝐷 − 𝐶𝐿, 𝑒𝑥𝑝

2

(ignoringresultswithno/lateCL,max)

SASALBVLESSASA-RC-QCRSA-RC-QCRW98CC+transLBWALESST[mod]

SA-QCRSA-negSA-negSA-RC-QCRSA-RC-QCRW98CCW98CC+transLBWALESST[mod]

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Generalobservationfromtheworkshop• MostoftheRANScodesproducedsurfaceflowsthathadtoomuchseparationnearthewingtipcomparedtotheexperimentandnotenoughseparationnearthewingrootatandbeyondmaxlift.• Notableexceptions:scale-resolvingmethods(likeLB).

AIAASciTech,Kissimmee,FL,January8-12,2018 27

Exp,alpha=18.58deg. Exp,alpha=21.57deg.

Page 28: Overview and Summary of the Third AIAA High Lift ... · Overview and Summary of the Third AIAA High Lift Prediction Workshop Christopher L. Rumsey NASA Langley Research Center Hampton,

Generalobservationfromtheworkshop• MostoftheRANScodesproducedsurfaceflowsthathadtoomuchseparationnearthewingtipcomparedtotheexperimentandnotenoughseparationnearthewingrootatandbeyondmaxlift.• Notableexceptions:scale-resolvingmethods(likeLB).

AIAASciTech,Kissimmee,FL,January8-12,2018 28

Exp,alpha=18.58deg. Exp,alpha=21.57deg.

(notionaltypicalRANS)

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JSM:surfacepressurecoefficients

AIAASciTech,Kissimmee,FL,January8-12,2018 29

A-A B-B C-C

E-E G-G H-H

Mainelement,alpha=21.57deg.,nonacelle/pylon

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JSM:issuesnearCL,max

AIAASciTech,Kissimmee,FL,January8-12,2018 30

Nonacelle/pylon Withnacelle/pylon

GridandtemporaltreatmentbothhavebiginfluenceSamecode&model,differentgrid

Samecode&model,differentgridSamecode,model&grid,time-accuratevs.steady-state

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JSM:furtherevidenceofinsufficientgriddensity

AIAASciTech,Kissimmee,FL,January8-12,2018 31

All“SA-verified”codesdonotagreewellusingSAon(different)mediumgrids

COFFE,gridC1TAU,gridBTAU,gridf(nc)OVERFLOW,gridATAU,gridBLAVA,gridAFUN3D,gridC1FUN3D,gridC2

Andbluecurvespointtominorissueswithinsufficientiterativeconvergenceand/orcodesetting/versiondifferences

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JSM:effectoftransitionmodels

AIAASciTech,Kissimmee,FL,January8-12,2018 32

Nonacelle/pylon Withnacelle/pylon

• TransitiondefinitelypresentatthisRe• For030.1vs.030.3(committeegridE),littleinfluenceoftransitionnoted• For030.2vs.030.4(participantgridb),transitioncausedhigherCL inthe

linearrangeandanearlierstall,inbetteragreementwithexperiment

SST-gammaSA-RC-QCR+AFT2017bW98CC+transW98CC+trans

SA-RC-QCR+AFT2017bW98CC+trans

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Statisticalanalysis:HL-CRM• Mainconclusion:generalscatterdidnotalwaysdecreasebetweenthemediumandfinegrids,aswouldbeexpectedifnumericalerrorduetogridresolutionwastheprimarysourceofvariation.

AIAASciTech,Kissimmee,FL,January8-12,2018 33

Notch=medianDiamond=mean

Upperandlowerquartiles

Minvaluethatisconsideredstatisticallysignificant

OutlierShadingrepresentsdistribution

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Statisticalanalysis:JSM

AIAASciTech,Kissimmee,FL,January8-12,2018 34

alpha=4.36deg. alpha=14.54deg. alpha=20.59deg.

Cv=σ/𝜇 =standarddeviation/medianScatterlimits=µ ± 𝐾𝜎(𝐾 = 3� )

Focusingononlyafewmainpointshere;furtherdetailsaregiveninthepaper

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HasCFDgottenanytightersinceHiLiftPW-2?

Cases Cv,lowalpha Cv,midalpha Cv,highalpha

HiLiftPW-2,alpha=7,16,20deg.

0.038 0.057 0.060

HiLiftPW-3, alpha=4.36,14.54,20.59deg.

0.025 0.017 0.073

AIAASciTech,Kissimmee,FL,January8-12,2018 35

LowRe,withbrackets,mediumgrids

YES YES NO

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Conclusions• Intheverificationcase,only30%oftheCFDcodesthatparticipatedwiththeSAturbulencemodelwerefullyverified.• HL-CRMcaseexploredgridconvergence.

• SpreadbetweenCFDresultsdidnotdiminishonfinegrids(similartoHiLiftPW-2).• Lackofverificationinsomecodesmayexplainpartofthespread.

• JSMexploredeffectofnacelle/pyloninstallation.• Useof“medium”gridonly;deltasweregenerallywellpredicted.• LargespreadinCFDresultsnearCL,max (similartoHiLiftPW-1and2).• SignificantinfluenceofgridnearCL,max,so”medium”gridprobablynotfineenough.• Transitionshouldbeimportantforthiscase,buttransitionmodelswerenotalwaysbetter(gridinfluence?).

• Manyindividualresultscomparedverywellwithexperimentalliftcurve;butwedonotknowwhy.

• Itwaspossibletogetintegratedquantitiesrightforthewrongreasons.• Scale-resolvingmethodsappearedtopredictseparationpatternsbetterthanRANS.• Participantsweremoreconsistent(comparedtoHiLiftPW-2)predictingcomplexhigh-liftconfigurationatlowRewithallmountingbrackethardwareatlowalphas– BUTNOTNEARCL,max.

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HiLiftPW-4statusandotherquestions/thoughts• WhatshouldbedonedifferentlyinHiLiftPW-4,sothatwelearnmore?• Proposal:requiretheuseofoneormorespecific(verified)models.

• Identifythe“best”(publicly-available)RANSmodel(s)fromthisworkshop,andrequestthatallRANSparticipantsverifyit intheircodeanduseit.

• Allowadditionalresultsusinganymodelormodelvariant.• NearCL,max: encouragelargergrids,moregridadaption,higherorder,time-accurate,moreuseofscale-resolvingmethods.• Nomorefree-airCFDruns;trytomatchthewindtunnelsemispan testinggeometryandBCs.

AIAASciTech,Kissimmee,FL,January8-12,2018 37

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End

AIAASciTech,Kissimmee,FL,January8-12,2018 38

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Backup

AIAASciTech,Kissimmee,FL,January8-12,2018 39

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Introduction• Specificworkshopseriesfocusedonthepredictionofswept,medium/high-aspectratiowingsinlanding/takeoff(highlift)configurations.• GoalsofHiLift workshopseries:• Assessthenumericalpredictioncapability ofcurrent-generationCFDtechnology.• DeveloppracticalmodelingguidelinesforCFDpredictionofhighliftflowfields.• Advancetheunderstandingofhighliftflowphysicstoenabledevelopmentofmoreaccuratepredictionmethodsandtools.• EnhanceCFDpredictioncapabilityforhighliftaerodynamicdesignandoptimization.• Provideanimpartialforum.• Identifyareasneedingadditionalresearchanddevelopment.

AIAASciTech,Kissimmee,FL,January8-12,2018 40

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Testcases• Case1- GridConvergenceStudyontheNASAHL-CRM(freeair,fullyturb).

• 1a:Fullchordflapgap,M=0.2,ReMAC=3.26M,alpha=8,16deg.• 1b:Sameas1a,withgridadaption.• 1c:Sameas1aexceptpartially-sealedflapgap.• 1d:Sameas1c,withgridadaption.

• Case2- NacelleInstallationStudyontheJSM(freeair,fullyturb orwithtransition).• 2a:Nacelle/pylonoff,M=0.173,ReMAC=1.93M,sixalphas.• 2b:Sameas2a,withgridadaption.• 2c:Sameas2aexceptNacelle/pylonon.• 2d:Sameas2c,withgridadaption.

• Case3- TurbulenceModelVerificationStudy(fullyturb).• VERIF/2DANWfromhttp://turbmodels.larc.nasa.gov

AIAASciTech,Kissimmee,FL,January8-12,2018 41

Black=requestedBlue=optional

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Gridsystems

Label Gridtool Org Type Coarse Medium Fine Extra-fine Notes

A-HLCRM ANSA+Chimera

NASA str 24/23 65/64 189/185 564/554 Overset

B1-HLCRM Pointwise Pointwise unstr 8/48 26/157 70/416 206/1228 Tet

B2-HLCRM Pointwise Pointwise unstr 8/22 26/65 70/170 206/541 Mixedprism/tet

B3-HLCRM Pointwise Pointwise unstr 8/18 27/48 71/119 208/397 Mixed

C-HLCRM GridPro GridPro str 10/8 77/68 338/311 n/a One-to-one

AIAASciTech,Kissimmee,FL,January8-12,2018 42

HL-CRM“committeegrids”

Points/cells

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Gridsystems

Label Gridtool Org Type Medium,noN/P

Medium,with N/P

Notes

A-JSM Chimera NASA str 221/216 235/230 Overset

B-JSM DLR-SOLAR DLR unstr 102/162 126/207 Mixed

C1-JSM VGRID Spaceship&Gulfstream

unstr 16/97 21/124 Tet

C1-JSM VGRID Spaceship&Gulfstream

unstr 16/52 21/65 Mixed

D-JSM JAXAtools JAXA unstr 50/120 59/139 Mixed

E-JSM ANSA UOxford&BETA-CAE

unstr 52/107 58/120 Mixed

AIAASciTech,Kissimmee,FL,January8-12,2018 43

JSM“committeegrids”