WO2009018810A1 - Verfahren und eintrichtung zum elektromagnetischen rühren von elektrisch leitenden flüssigkeiten - Google Patents

Verfahren und eintrichtung zum elektromagnetischen rühren von elektrisch leitenden flüssigkeiten Download PDF

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Publication number
WO2009018810A1
WO2009018810A1 PCT/DE2008/001261 DE2008001261W WO2009018810A1 WO 2009018810 A1 WO2009018810 A1 WO 2009018810A1 DE 2008001261 W DE2008001261 W DE 2008001261W WO 2009018810 A1 WO2009018810 A1 WO 2009018810A1
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WO
WIPO (PCT)
Prior art keywords
rmf
wmf
magnetic field
container
rotating
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
PCT/DE2008/001261
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German (de)
English (en)
French (fr)
Inventor
Petr A. Nikrityuk
Sven Eckert
Dirk RÄBIGER
Bernd Willers
Kerstin Eckert
Roger Grundmann
Gunter Gerbeth
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Technische Universitaet Dresden
Helmholtz Zentrum Dresden Rossendorf eV
Original Assignee
Technische Universitaet Dresden
Helmholtz Zentrum Dresden Rossendorf eV
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Technische Universitaet Dresden, Helmholtz Zentrum Dresden Rossendorf eV filed Critical Technische Universitaet Dresden
Priority to JP2010518495A priority Critical patent/JP2010535106A/ja
Priority to US12/672,046 priority patent/US20100163207A1/en
Priority to EP08801099A priority patent/EP2178661A1/de
Publication of WO2009018810A1 publication Critical patent/WO2009018810A1/de
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

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Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B22CASTING; POWDER METALLURGY
    • B22DCASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
    • B22D27/00Treating the metal in the mould while it is molten or ductile ; Pressure or vacuum casting
    • B22D27/02Use of electric or magnetic effects
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B01PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
    • B01FMIXING, e.g. DISSOLVING, EMULSIFYING OR DISPERSING
    • B01F33/00Other mixers; Mixing plants; Combinations of mixers
    • B01F33/45Magnetic mixers; Mixers with magnetically driven stirrers
    • B01F33/451Magnetic mixers; Mixers with magnetically driven stirrers wherein the mixture is directly exposed to an electromagnetic field without use of a stirrer, e.g. for material comprising ferromagnetic particles or for molten metal
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B22CASTING; POWDER METALLURGY
    • B22DCASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
    • B22D11/00Continuous casting of metals, i.e. casting in indefinite lengths
    • B22D11/10Supplying or treating molten metal
    • B22D11/11Treating the molten metal
    • B22D11/114Treating the molten metal by using agitating or vibrating means
    • B22D11/115Treating the molten metal by using agitating or vibrating means by using magnetic fields

Definitions

  • the invention relates to a method and a device for the electromagnetic stirring of electrically conductive liquids using a magnetic field rotating in a horizontal plane and a magnetic field traveling in the vertical direction. Due to their contactless interaction with electrically conductive liquids, time-dependent electromagnetic fields provide an attractive possibility for stirring hot molten metals or semiconductor melts. Using the parameters magnetic field amplitude and magnetic field frequency, the electromagnetic force field can be controlled directly and accurately in a simple manner.
  • the electromagnetic stirring is used on an industrial scale i.a. used in the directional solidification of metallic alloys or semiconductor melts.
  • a significant problem is that flows in the immediate vicinity of a progressing solidification front can lead to segregation in the solidified material, which deteriorate the mechanical properties of the resulting solid significantly.
  • Due to the different solubility of individual components in the liquid or solid phase a concentration boundary layer is formed on the solidification front. Due to the convective transport of the enriched melt away from the solidification front, a flow counteracts the build-up of an extended concentration boundary layer. If the melt flows exclusively in one direction, segregation zones occur in other volume areas.
  • Rotating or migrating magnetic fields are already used in metallurgical processes, such as the continuous casting of steel.
  • metallurgical processes such as the continuous casting of steel.
  • an arrangement of a polyphase electromagnetic winding for generating a traveling field perpendicular to the casting direction at a continuous casting plant in the publication DE AS 1 962 341 is described.
  • JP2003220323 An apparatus and a method for intensively stirring a melt contained in a cylindrical container in which a rotating magnetic field and a traveling magnetic field are simultaneously used are described in JP2003220323.
  • the rotating magnetic field is from a radial coil surrounding the container, the turns of which are annular, generates the traveling magnetic field by a longitudinal coil, the turns of which extend in an axial direction in a jacketed section and annularly surround the container shell, wherein the longitudinal coil between the container shell and the radial coil arranged is.
  • the radial coil generates a rotational movement and the longitudinal coil generates an axial movement of the liquid melt in the container.
  • the invention has for its object to provide a method and a device for electromagnetic stirring of electrically conductive liquids, which are designed so suitable 'that asymmetrical flow structures are avoided in containers filled with melts, especially at the beginning and during the course of solidification.
  • an effective mixing of the liquid and / or a controlled solidification of metallic alloys while avoiding the formation of segregation zones in the solidification structure should be achieved.
  • both the rotating magnetic field RMF and the traveling magnetic field WMF discontinuous Form of time-limited and adjustable periods Tp 1RMF and Tp 1WMF and alternately connected in chronological succession.
  • the duration Tp 1 RM F of the periods of the rotating magnetic field RMF and the duration Tp 1 WMF of the periods of the traveling magnetic field WMF can be determined in a time interval
  • In the container can be filled as electrically conductive liquid metallic or semiconductor melt.
  • the amplitude Bo RMF of the rotating magnetic field RMF is to be increased so that at least the maximum of the two values
  • Bi RMF and B 2 RMF are the lower limits of the amplitudes of the rotating magnetic field, which can change in the course of solidification depending on the parameters v, Vsoi and Ho.
  • the amplitude B 0 WMF of the traveling magnetic field WMF can be set to be as large or up to four times greater than the amplitude Bo RMF of the rotating magnetic field RMF, ie
  • the course and the maximum value of the magnetic field RMF or WMF are set so that for the different pulse forms an identical energy input results.
  • the amplitudes B 0 RMF , B 0 WMF of the magnetic fields RMF or WMF can be adjusted continuously during the stirring in accordance with the requirements derived from the process to be considered.
  • the individual periods T PI RMF and T P , W MF, in which one of the magnetic fields RMF or WMF is switched on, can be interrupted by a pause duration Tp ause , in which neither of the two magnetic fields RMF or WMF acts on the liquid, wherein Tp aU se ⁇ O.5-TP, RMF or T PaU se ⁇ O.5-TP, WMF can be set.
  • the direction of the rotating magnetic field RMF and / or WMF can be inverted between two pulses.
  • the device for electromagnetic stirring of electrically conductive liquids contains at least
  • the container with the liquid or liquid melt can be arranged concentrically within the induction coils.
  • the container may be provided with a heating device and / or cooling device.
  • the bottom plate of the container can be in direct contact with a solid metal body, which is flowed through by a cooling medium in the interior.
  • the side walls of the container may be thermally insulated.
  • the heat sink can communicate with a thermostat.
  • Between the heat sink and the container may be a liquid metal film to achieve a stable heat transfer with low contact resistance.
  • the liquid metal film may be made of a gallium alloy.
  • At least one temperature sensor may be positioned in the form of a thermocouple, which provides information about the time of onset of solidification and with the control unit connected to the temperature control of the liquid.
  • a use of the device for electro-magnetic stirring of electrically conductive liquids according to claims 10 to 18 can in the form of metallic melts in metallurgical processes or in the form of semiconductor melts in the crystal growth, for the purification of molten metal, in continuous casting or in the process of solidification of metallic materials of the method according to claim 1 to 9 take place.
  • both the rotating and the vertically migrating magnetic field RMF and WMF are switched on discontinuously in the form of pulses of limited duration, wherein both magnetic fields RMF and WMF are switched on alternately and in succession.
  • the induction coil pairs fed with a three-phase alternating current are thus controlled such that a magnetic field RMF or WMF acts on the melt at any time.
  • the period T P is WMF of the traveling magnetic field
  • the amplitude B P> WMF of the vertically traveling magnetic field WMF can be at least as great as the amplitude B pjmr of the rotating magnetic field RMF 1, preferably it is a multiple (maximum 4 times) larger.
  • Fig. 3a2 is a snapshot of the meridional velocity as a vector diagram when the rotating magnetic field
  • 3b1 is a snapshot of the azimuthal flow when the traveling magnetic field WMF is turned on and at the same time the rotating magnetic field RMF is turned off,
  • FIG. 3b2 shows a snapshot of the meridional velocity as a vector diagram, when the traveling magnetic field WMF is switched on and, at the same time, the rotating magnetic field RMF is switched off
  • Fig. 4a1 is a snapshot of the azimuthal flow, when the rotating magnetic field RMF is turned on and at the same time the wandering magnetic field WMF is turned off
  • Fig. 4a2 is a snapshot of the meridional velocity as a vector diagram when the rotating magnetic field RMF is turned on and at the same time the wandering
  • 4b1 is a snapshot of the azimuthal flow when the traveling magnetic field WMF is turned on and at the same time the rotating magnetic field RMF is turned off,
  • FIG. 4b2 shows a snapshot of the meridional velocity as a vector diagram, when the traveling magnetic field WMF is switched on and at the same time the rotating magnetic field RMF is switched off, FIG.
  • FIG. 5 a shows a macrostructure under the influence of a continuously acting traveling magnetic field WMF at 6 mT
  • FIG. 5 b shows a macrostructure under the influence of a continuously acting rotating magnetic field RMF at 6.5 mT
  • FIG. 5 a shows a macrostructure under the influence of a continuously acting traveling magnetic field WMF at 6 mT
  • FIG. 5 b shows a macrostructure under the influence of a continuously acting rotating magnetic field RMF at 6.5 mT
  • FIG. 5 a shows a macrostructure under the influence of a continuously acting traveling magnetic field WMF at 6 mT
  • FIG. 5 b shows a macrostructure under the influence of a continuously acting rotating magnetic field RMF at 6.5 mT
  • FIG. 5 a shows a macrostructure under the influence of a continuously acting traveling magnetic field WMF at 6 mT
  • FIG. 5 b shows a macrostructure under the influence of a continuously acting rotating magnetic field RMF at 6.5 mT
  • FIG. 5 a shows a macrostructure
  • 5c shows a macrostructure under the influence of the discontinuously and alternately acting magnetic fields RMF and WMF, each with 6mT. demonstrate.
  • FIG. 1 shows, in a schematic representation, a device 1 for the electromagnetic stirring of electrically conductive liquids 2, which contains at least
  • the power supply unit 9 is connected to the respectively associated induction coils 31, 32, 33; 41, 42, 43, 44, 45, 46 with the control unit 10, a current supply to the induction coils 31, 32, 33; 41, 42, 43, 44, 45, 46 with the given conditions
  • the container 14 is located centrally symmetrically in the middle of an arrangement 3 of pairs 31, 32, 33 of induction coils for generating a rotating magnetic field RMF 34 and an arrangement 4 of induction coils 41, 42, 43, 44, 45, 46 of a traveling magnetic field WMF 47
  • Induction coil pairs 31, 32, 33 and the induction coils 41, 42, 43, 44, 46 stacked coaxially with respect to the axis of symmetry 15 are each connected to the power supply unit 9 and are supplied from there with a current I 0 fed in the form of a 3-PhasenwechseIstroms and generate a rotating about the symmetry axis 15 of the device 1, horizontally oriented magnetic field RMF 34 and a along the axis of symmetry 15 aligned, in the vertical direction migrating magnetic field WMF 47.
  • the power supply unit 9 is connected to the electronic control / Control unit 10 connected, which causes at predetermined intervals, a connection and disconnection of the 3-phase alternating current ID.
  • the switching on and off of the magnetic fields RMF 34 and WMF 47 is controlled in the control / regulating unit 10 so that at most a maximum of only one magnetic field RMF 34 or WMF 47 acts on the melt 2.
  • the device 1 of the filled with the electrically conductive melt 2 cylindrical container 14 may be supplemented with a cooling device 11 for the solidification of metallic melts 2.
  • the cooling device 11 contains a metal block 5, in the interior of which cooling channels 6 are present.
  • the container 14 is with its bottom plate 12 on the metal block 5.
  • the located inside the metal block 5 cooling channels 6 are flowed through during the solidification process of a coolant.
  • the cooling device 11 of the melt 2 By means of the cooling device 11 of the melt 2, the heat is withdrawn down.
  • a thermal insulation 7 of the container 14 prevents heat losses in the radial direction.
  • On the bottom plate 12 and / or in / on the side walls 13 of the container 14 at least one temperature sensor 8, for example in the form of a thermocouple for temperature control is mounted.
  • the temperature measurements enable a monitoring of the liquid state, the beginning and the course of the state of solidification and allow a timely adjustment of the magnetic field parameters, eg B 0 RMF , B 0 WMF and the period T P , controlled by the control unit 10 Power supply unit 9 to the individual stages of the solidification process.
  • the container 14 with the melt 2 is arranged concentrically within the induction coils 31, 32, 33, 41, 42, 43, 44, 45, 46.
  • the container 14 may be provided with a heater and / or cooling device 11.
  • the bottom plate 12 is in direct contact with a solid metal body 5, which is traversed in the interior of a cooling medium.
  • the side walls 13 of the container 14 are thermally insulated by an insulating jacket 7.
  • the heat sink 5 is connected to a thermostat (not shown) in connection.
  • the liquid metal film may be made of a gallium alloy.
  • a temperature sensor 8 is positioned in the form of a thermocouple, which provides information about the time of onset of solidification and with the control - / control unit 10 is connected.
  • the time sequence of RMF and WMF is shown in each case, wherein the amplitude of the traveling magnetic field B 0 WMF is three times the amplitude of the rotating magnetic field B 0 RMF and the same period ends T P
  • both the rotating magnetic field RMF 34 and FIG the wandering magnetic field WMF 47 dis- continuously in the form of time-limited and adjustable periods Tp 1 RMF and Tp 1WMF and alternately generated in chronological succession.
  • the duration TP.RMF of the periods of rotating magnetic field RMF 34 and the duration TP, WMF of the periods of traveling magnetic field WMF 47 may be in a time interval
  • the amplitude B 0 RMF of the rotating magnetic field RMF 34 is to be increased so that at least the maximum of the two values
  • the amplitude Bo WMF of the traveling magnetic field WMF 47 can be set to be equal to or up to four times greater than the amplitude B 0 RMF of the rotating magnetic field RMF 34, ie
  • the amplitudes B 0 RMF , B 0 WMF of the magnetic fields RMF 34 and WMF 47 can be continuously adjusted during the stirring in accordance with the requirements derived from the process to be considered.
  • the individual period durations TP.RMF and TP, WMF, in which one of the magnetic fields RMF 34 or WMF 47 is switched on, can be interrupted by a pause duration Tpausei in which neither of the two magnetic fields acts on the liquid 2, where Tp out ⁇ 0.5TP, RMF or TpoutU ⁇ O.5-TP, WMF.
  • the direction of the rotating magnetic field RMF 34 and / or the traveling magnetic field WMF 47 can be inverted between two pulses.
  • 3a is a snapshot of the azimuthal flow when the rotating magnetic field RMF 34 is turned on and at the same time the traveling magnetic field WMF 47 is turned off,
  • 3a2 shows a snapshot of the meridional velocity as a vector diagram, when the rotating magnetic field RMF 34 is switched on and at the same time the traveling magnetic field WMF 47 is switched off,
  • Fig. 3b1 is a snapshot of the azimuthal flow when the wandering magnetic field WMF 47 is turned on and at the same time the rotating magnetic field RMF 34 is turned off and Fig. 3b2 is a snapshot of the meridional velocity as a vector diagram when the traveling magnetic field WMF 47 is turned on and the rotating magnetic field RMF 34 is turned off.
  • FIG. 4 a shows a snapshot of the azimuthal flow when the rotating magnetic field RMF 34 is switched on and at the same time the traveling magnetic field WMF 47 is switched off.
  • FIG. 4 a shows a snapshot of the meridional velocity as a vector diagram when the rotating magnetic field RMF 34 is switched on and simultaneously
  • Fig. 4b1 is a snapshot of the azimuthal flow when the traveling magnetic field WMF 47 is turned on and at the same time the rotating magnetic field RMF 34 is turned off
  • Fig. 4b2 is a snapshot of the meridional velocity as a vector diagram when the traveling magnetic field WMF 47 is turned on and at the same time the rotating magnetic field RMF 34 is turned off, show.
  • FIG. 5 shows a plurality of schematic representations of the solidification of an Al-Si alloy under the influence of magnetic fields in the form of the macrostructure in vertical section, in which:
  • 5b shows a microstructure under the influence of a continuously acting rotating magnetic field RMF 34 at 6.5 mT and
  • FIG. 5c shows a microstructure under the influence of the discontinuously and alternately acting magnetic fields RMF 34 and WMF 47 with 6mT each.
  • the corresponding magnetic fields RMF 34 and WMF 47 are each switched on 30 seconds after the start of solidification at the container bottom.
  • a coarse columnar structure grows parallel to the symmetry axis of the container.
  • the wandering magnetic field WMF 47 in FIG. 5a a very coarse microstructure can be recognized.
  • the columnar grains continue to grow almost unchanged until the transition from columnar to equiaxial growth occurs approximately in the middle of the sample.
  • a modified columnar structure initially forms, ie the columnar grains become finer and grow inclined to the side.
  • a morphology transition from columnar to equiaxial grain growth can be observed.
  • the secondary flow transports Si-rich melt towards the symmetry axis 15. This leads to typical segregation patterns, which have a depletion of eutectic phase in the edge zones and a concentration in the region of the axis of symmetry 15. If the rotating magnetic field RMF 34 and the traveling magnetic field WMF 47, as shown in Fig. 5c, applied discontinuously one after the other, a transition from coarse-grained columnar to fine-grained equiaxial growth is observed immediately with activation of the electromagnetic stirring. Dismissals are undetectable.

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  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Continuous Casting (AREA)
  • Waste-Gas Treatment And Other Accessory Devices For Furnaces (AREA)
PCT/DE2008/001261 2007-08-03 2008-08-01 Verfahren und eintrichtung zum elektromagnetischen rühren von elektrisch leitenden flüssigkeiten Ceased WO2009018810A1 (de)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP2010518495A JP2010535106A (ja) 2007-08-03 2008-08-01 導電性流体を電磁撹拌するための方法およびデバイス
US12/672,046 US20100163207A1 (en) 2007-08-03 2008-08-01 Method and device for the electromagnetic stirring of electrically conductive fluids
EP08801099A EP2178661A1 (de) 2007-08-03 2008-08-01 Verfahren und eintrichtung zum elektromagnetischen rühren von elektrisch leitenden flüssigkeiten

Applications Claiming Priority (2)

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DE102007038281A DE102007038281B4 (de) 2007-08-03 2007-08-03 Verfahren und Einrichtung zum elektromagnetischen Rühren von elektrisch leitenden Flüssigkeiten
DE102007038281.4 2007-08-03

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WO2009018810A1 true WO2009018810A1 (de) 2009-02-12

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US (1) US20100163207A1 (enExample)
EP (1) EP2178661A1 (enExample)
JP (1) JP2010535106A (enExample)
DE (1) DE102007038281B4 (enExample)
WO (1) WO2009018810A1 (enExample)

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US8870446B2 (en) * 2006-06-21 2014-10-28 Spinomix S.A. Device and method for manipulating and mixing magnetic particles in a liquid medium
DE102007037340B4 (de) 2007-08-03 2010-02-25 Forschungszentrum Dresden - Rossendorf E.V. Verfahren und Einrichtung zum elektromagnetischen Rühren von elektrisch leitenden Flüssigkeiten
US8608370B1 (en) * 2009-04-02 2013-12-17 Inductotherm Corp. Combination holding furnace and electromagnetic stirring vessel for high temperature and electrically conductive fluid materials
DE102010041061B4 (de) 2010-09-20 2013-10-24 Forschungsverbund Berlin E.V. Kristallisationsanlage und Kristallisationsverfahren zur Herstellung eines Blocks aus einem Material, dessen Schmelze elektrisch leitend ist
CA2859739C (en) 2011-12-22 2016-03-22 Abb Ab Arrangement and method for flow control of molten metal in a continuous casting process
WO2013158200A1 (en) * 2012-04-20 2013-10-24 Fs Precision Tech Single piece casting of reactive alloys
CN102980415A (zh) * 2012-11-20 2013-03-20 中国科学院研究生院 基于通电线圈螺旋磁场驱动金属熔体周期性流动的方法
EP3354367B1 (de) * 2017-01-30 2019-07-17 Hydro Aluminium Rolled Products GmbH Vorrichtung und verfahren zur reinigung einer elektrisch leitenden flüssigkeit von nichtleitenden verunreinigungen
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TWI834515B (zh) * 2023-03-08 2024-03-01 鑫科材料科技股份有限公司 金屬鑄件之鑄造方法
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Publication number Priority date Publication date Assignee Title
FR3051698A1 (fr) * 2016-05-30 2017-12-01 Constellium Issoire Procede de fabrication de lingots de laminage par coulee verticale d'un alliage d'aluminium
WO2017207886A1 (fr) * 2016-05-30 2017-12-07 Constellium Issoire Procede de fabrication de lingots de laminage par coulee verticale d'un alliage d'aluminium
CN109311081A (zh) * 2016-05-30 2019-02-05 伊苏瓦尔肯联铝业 通过立式铸造铝合金生产板铸锭的方法

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DE102007038281A1 (de) 2009-02-19
US20100163207A1 (en) 2010-07-01
EP2178661A1 (de) 2010-04-28
DE102007038281B4 (de) 2009-06-18

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