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---------------------------------------------- ------------------------------------- Dresden, October 16-19, 2005 2 nd Sino-German Workshop on Electromagnetic Processing of Materials FREE SURFACE INSTABILITIES PRODUCED BY HIGH-FREQUENCY MAGNETIC FIELDS Christian Karcher Technische Universität Ilmenau • Motivation • Model Experiments, Analytical Model • Results • Conculsions • Proposals for Collaboration within Common Project

FREE SURFACE INSTABILITIES PRODUCED BY HIGH-FREQUENCY MAGNETIC FIELDS

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FREE SURFACE INSTABILITIES PRODUCED BY HIGH-FREQUENCY MAGNETIC FIELDS. Christian Karcher Technische Universität Ilmenau. Motivation Model Experiments, Analytical Model Results Conculsions Proposals for Collaboration within Common Project. Motivation: Electromagnetic Shaping. - PowerPoint PPT Presentation

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  • Experimental setup

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    Karcher, Mohring in MHD (2003), Mohring, Karcher, Schulze in Phys. Rev. E (2005)

  • Digital image processing 1

    Liquid metal

    sodium hydroxide

    mirror (upper surface)

    free surface

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    Small surface waves 1

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    Dynamics of the free surface 1Spectrum of different wavelengths (gravity, capillary)Amplitudes increase upon increasing I0a = 3 mm, H = 24 mm, L = 17 mm, f = 21.9 kHz, I = 120 A

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    Static surface deformation 1

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    Dynamics of the free surface 2a = 3 mm, H = 24 mm, L = 17 mm, f = 21.9 kHz, I = 127 AWavelength corresponding to skin depth: 1 ~ 2p d

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    Pinch

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    a = 3 mm, H = 24 mm, L = 17 mm, f = 47.2 kHz, I = 123 A Pinch development

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    Magnetohydrodynamics 2003Theoretical ModelHele Shaw approximationSkin depth approximationKarcher, MohringCartesian geometry2dLiquid metalr,u,sHLxy,vh(y,t)zI coswtnz,wpa, pMI coswtpgLorentz force:j, B from vector potentials Ai, Aamagnetic pressure:

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    governing equationsboundary conditions

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    evolution equationMost dangerous modeNeutral instability HPhysical interpretationConclusionsLinear stabilty analysis for basic state

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    Measurement vs. theorya = 3 mm, H = 30 mm

    Tabelle1

    a in mmH in mmL in mmf in HzIkrit in AIkritneu

    1241721500100

    124172410097

    124172770093

    124173360088

    124174620084

    1242221200112

    1242223600110

    1242227100106

    1242233000102

    124224540095

    3241721900130

    3241724400129

    3241728100128

    3241734100125

    3241747200123

    3301222552108.32

    3301225160104.3

    3301228933103.38

    3301235093101.81

    330124829099.71

    33014.522182115.85

    33014.524750113.81

    33014.528416113.25

    33014.534503110.73

    33014.547490107.94

    3301721870125.44

    3301724405122.93

    3301728045121.08

    3301734043118.34

    3301746877115.44

    33019.521594136.11

    33019.524084132.48

    33019.527696130.17

    33019.533598128.17

    33019.546258125.46

    3302221370146.04

    3302223859141.51

    3302227418139.91

    3302233273137.18

    3302245826133.67

    3202221423152

    3202223893149

    3202227480146

    3202233359143

    3202245943140

    322.52221418149.35

    322.52223893146.78

    322.52227468144

    322.52233325142.27

    322.52245884138.76

    3252221380147.6

    3252223851145.93

    3252227419143.74

    3252233291140.58

    3252245800138.74

    327.52221405143.53

    327.52223885140.45

    327.52227421138.72

    327.52233313136.05

    327.52245878133.3

    3302221387142.68

    3302223875140.36

    3302227410139.41

    3302233289136.23

    3302245830133.39

    332.52221336142.76

    332.52223807140.66

    332.52227362139.87

    332.52233194136.5

    332.52245721133.3

    6241722000186

    6241724500184

    6241728200181

    6241734200178

    6241747000175

    6242221500213214.6500155328262.2034508866

    6242223900204209.987056653255.1029058274

    6242227500200204.1277414349246.2364185535

    6242233400194196.3210729988234.521896047

    6242246000183.997302295216.266408157

    10241722400240

    10241725000227

    10241728800220

    10241735000210

    10241748400200

    I(f) Par. a

    100130186240

    97129184227

    93128181220

    88125178210

    84123175200

    Frequenz in Hz

    Strom in A

    Pincheffekt: Induktorstrom in Abhngigkeit der Frequenz f. a = 3 mm. Parameter: Flssigkeitshhe H, Koppelspalt L

    I(f) Par. H

    152149.35147.6143.53142.68142.76

    149146.78145.93140.45140.36140.66

    146144143.74138.72139.41139.87

    143142.27140.58136.05136.23136.5

    140138.76138.74133.3133.39133.3

    I(f) Par. L

    108.32115.85125.44136.11146.04

    104.3113.81122.93132.48141.51

    103.38113.25121.08130.17139.91

    101.81110.73118.34128.17137.18

    99.71107.94115.44125.46133.67

    Tabelle2

    L in mmH in mmmf in Hza in mmI in A

    172425000195.8239905885

    1724250003128.7296656531

    1724250006183.4241656549

    17242500010229.3763818669

    172430000191.8502726113

    1724300003126.9790664132

    1724300006180.7385482068

    17243000010220.1491846731

    172435000188.6193806341

    1724350003125.517541966

    1724350006178.4985917706

    17243500010212.6378950077

    172440000185.9126630435

    1724400003124.2651162876

    1724400006176.5807046988

    17244000010206.3387892624

    172445000183.593873595

    1724450003123.1707755926

    1724450006174.906120326

    17244500010200.9376551059

    I(a) Par. f

    95.823990588591.850272611388.619380634185.912663043583.593873595

    128.7296656531126.9790664132125.517541966124.2651162876123.1707755926

    183.4241656549180.7385482068178.4985917706176.5807046988174.906120326

    229.3763818669220.1491846731212.6378950077206.3387892624200.9376551059

    f = 25000 Hz

    f = 30000 Hz

    f = 35000 Hz

    f = 40000 Hz

    f = 45000 Hz

    Spaltbreite a in mm

    Induktorstrom in A

    Pincheffekt: Induktorstrom in Abhngigkeit der Spaltbreite. H = 24 mm, L = 17 mm.Parameter: Frequenz f

    Tabelle3

    a in mmL in mmf in HzH in mmH/deltaI in A

    32225000209.629356884148.4168833694

    3222500022.510.8330264945146.3569290731

    322250002512.036696105145.2163247187

    3222500027.513.2403657155140.4148326931

    322250003014.444035326140.2074435116

    3222500032.515.6477049365140.5460537647

    322300002010.5484319593145.5867220948

    3223000022.511.8669859542143.9067300537

    322300002513.1855399491143.0275314831

    3223000027.514.504093944138.0590775177

    322300003015.822647939138.0010218505

    3223000032.517.1412019339138.2763065617

    322350002011.3936087172143.2360008352

    3223500022.512.8178098068141.8671460989

    322350002514.2420108965141.2026917062

    3223500027.515.6662119861136.0981761032

    322350003017.0904130758136.1626300748

    3223500032.518.5146141654136.3858838389

    322400002012.1802800625141.2304156784

    3224000022.513.7028150703140.1237585626

    322400002515.2253500781139.6407737069

    3224000027.516.7478850859134.4220927526

    322400003018.2704200937134.5899501068

    3224000032.519.7929551015134.7692283084

    322450002012.9191379434139.4846866035

    3224500022.514.5340301863138.6037735744

    322450002516.1489224292138.2774115642

    3224500027.517.7638146721132.960824137

    322450003019.3787069151133.2178323222

    3224500032.520.993599158133.3591507993

    I(H) Par. f

    148.4168833694145.5867220948143.2360008352141.2304156784139.4846866035

    146.3569290731143.9067300537141.8671460989140.1237585626138.6037735744

    145.2163247187143.0275314831141.2026917062139.6407737069138.2774115642

    140.4148326931138.0590775177136.0981761032134.4220927526132.960824137

    140.2074435116138.0010218505136.1626300748134.5899501068133.2178323222

    140.5460537647138.2763065617136.3858838389134.7692283084133.3591507993

    f = 25000 Hz

    f = 30000 Hz

    f = 35000 Hz

    f = 40000 Hz

    f = 45000 Hz

    Flssigkeitshhe H in mm

    Induktorstrom in A

    Pincheffekt: Induktorstrom in Abhngigkeit der Flssigkeitshhe H. a = 3 mm, L = 22 mm.Parameter: Frequenz f

    I(H_delta)

    148.4168833694

    146.3569290731

    145.2163247187

    140.4148326931

    140.2074435116

    140.5460537647

    145.5867220948

    143.9067300537

    143.0275314831

    138.0590775177

    138.0010218505

    138.2763065617

    143.2360008352

    141.8671460989

    141.2026917062

    136.0981761032

    136.1626300748

    136.3858838389

    141.2304156784

    140.1237585626

    139.6407737069

    134.4220927526

    134.5899501068

    134.7692283084

    139.4846866035

    138.6037735744

    138.2774115642

    132.960824137

    133.2178323222

    133.3591507993

    Tabelle4

    a in mmH in mmf in HzL in mmI in A

    3302500012105.5304466597

    3302500014.5114.2432493064

    3302500017122.8851406254

    3302500019.5132.5457788487

    3302500022141.947091978

    3303000012103.7032131772

    3303000014.5112.3798371489

    3303000017120.5220660896

    3303000019.5130.1558261248

    3303000022139.2022285868

    3303500012102.1830144608

    3303500014.5110.8280770567

    3303500017118.5596026222

    3303500019.5128.1688015575

    3303500022136.922930977

    3304000012100.884183164

    3304000014.5109.5012115563

    3304000017116.8854875377

    3304000019.5126.4720992182

    3304000022134.9787026406

    330450001299.7522430979

    3304500014.5108.3440252948

    3304500017115.4284460458

    3304500019.5124.9941551417

    3304500022133.2866996526

    I(L) Par. f

    105.5304466597103.7032131772102.1830144608100.88418316499.7522430979

    114.2432493064112.3798371489110.8280770567109.5012115563108.3440252948

    122.8851406254120.5220660896118.5596026222116.8854875377115.4284460458

    132.5457788487130.1558261248128.1688015575126.4720992182124.9941551417

    141.947091978139.2022285868136.922930977134.9787026406133.2866996526

    f = 25000 Hz

    f = 30000 Hz

    f = 35000 Hz

    f = 40000 Hz

    f = 45000 Hz

    Coupling gap in mm

    Inductor current in A

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    ConclusionsElectromagnetic shaping with high-frequency magnetic fields Squeezing of drops up to 15% possible Onset of drop instabilities; critical parameters depending on drop volume and inductor current frequeny3 Types of surface instabilities: small surface waves, large-amplitude static deformation, electromagnetic pinch First instability well-predicted by simple model based on Hele Shaw and skin depth approximation High-frequency fields not suited for sealing purposesAcknoledgementsDFG: Research Group MagnetofluiddynamicsDAAD: PROCOPE program with EPM Grenoble (Professor Yves Fautrelle)

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    Proposal for Collaboration ILorentz force velocimetry (Thess, Kolesnikov, Karcher: Patent 2005) BMBF project; start 01.07.2006Measurement of mass flow in liquid aluminum, steel, glass, semiconductor melts

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    Proposal for Collaboration II