Analysis of magnetohydrodynamics GTAW arc behavior

Analysis of magnetohydrodynamics GTAW arc behavior

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时间:2019-09-19

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1、FrédéricRogerAnalysisofmagnetohydrodynamicsGTAWarcbehaviorAbstractArgonplasmabehavioringastungsten2Mathematicalmodelarcwelding(GTAW)isdirectlylinkedtotheweldquality.Indeed,thearcistheheatsourcewhichThemodeldescribesthefluidflowandthedrivestheweldshape.Solutionofaninduction-electromagneticfie

2、ldinthespacebetweenthediffusionequationunderaxialsymmetryconditionstungstencathodeandtheanodeworkpiece.WehasbeendeveloppedusingthermalconductionandconsideranaxialsymmetrictwodimensionalconvectionmoduleofFemlab3.1©.Wepredictdescription.currentdistributioninelectricarc,inducedmagneticfieldandt

3、henresultingelectromagneticforces.The2DaxialsymmetricstationaryNavierStokesThelatterisintroducedinincompressibleaxialincompressibleequationsareusedinFemlab3.1fluidsymmetricNavier-Stokesequations.BothPdesaredynamicsmodule.Fortheconvectioninductionstronglycoupled.Indeed,Plasmavelocityfieldequa

4、tion,weusetheconductiveandconvectiveintroducesasourcetermintheinductiondiffusionstationaryheattransfermodel.TemperatureTisthenequation.replacedbytheazimuthalmagneticfieldBBθ.KeywordsArcwelding–magnetohydrodynamics-plasma2.1Governingsequations1IntroductionWeconsiderthemagneticfieldBastheprinc

5、ipalelectromagneticquantity.AlltheotherquantitiesThefirstworkaboutelectromagneticarcplasma(E,J,q)canbededucedusingMaxwell’sequationsbehaviorisfiftyyearsold[1]withtheMaecker’sandOhm’sLaw.FromOhm’slaw,AmpereanddescriptionoftheconvectionintheplasmawhichisFaraday’sequationswecandeducethestationa

6、ryassumedtobeinlocalthermodynamicequilibriuminductionconvectionequation:(LTE)withthesamelocaltemperatureforionsandelectrons.1curl()uB∧+Δ=B0(1)Convection,withhighplasmavelocity(aboutμσ100m/s),drivesheattransferwiththeweldpooland-1withutheplasmavelocity(m.s),μthethentheshapeandthethermomechani

7、csbehaviorof-1permeabilityofmatter(orvacuum,H.m)andσthetheweld.-1-1electricalconductivity(Ω.m).FemlaballowstoconsiderthewholesetofnonInthe2Daxialsymmetricconfiguration,equationlinearphysicsequations(nonlinearcouplingPDE’s)(1)becomes:todescribetheve

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