JP2000052006A - Equipment and method for continuous casting of metallic pieces - Google Patents

Equipment and method for continuous casting of metallic pieces

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Publication number
JP2000052006A
JP2000052006A JP10228910A JP22891098A JP2000052006A JP 2000052006 A JP2000052006 A JP 2000052006A JP 10228910 A JP10228910 A JP 10228910A JP 22891098 A JP22891098 A JP 22891098A JP 2000052006 A JP2000052006 A JP 2000052006A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic pole
molten steel
continuous casting
casting
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.)
Withdrawn
Application number
JP10228910A
Other languages
Japanese (ja)
Inventor
Katsuaki Morita
克明 森田
Ichiro Yamashita
一郎 山下
Yoichiro Tsumura
陽一郎 津村
Koichi Hirata
耕一 平田
Masahiro Kasai
正弘 葛西
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.)
Mitsubishi Heavy Industries Ltd
Original Assignee
Mitsubishi Heavy Industries Ltd
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 Mitsubishi Heavy Industries Ltd filed Critical Mitsubishi Heavy Industries Ltd
Priority to JP10228910A priority Critical patent/JP2000052006A/en
Publication of JP2000052006A publication Critical patent/JP2000052006A/en
Withdrawn legal-status Critical Current

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  • Continuous Casting (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a continuous casting equipment to cast metallic pieces under the application of rotating magnetic field with large magnetomotive force obtained at the same current density and high saturated flux density. SOLUTION: This continuous casting equipment is composed of a cylindrical mold 1 with both ends opened, a nozzle 2 to supply a molten steel 3 from one open end of the mold 1, a cooler 4 to cool the molten steel 3, an electromagnet to apply a rotating magnetic field to the molten steel 3 in the mold 1, and rotating rolls 10 to pull out a solidified shell 9 made as the molten steel 3 grows and a billet 11 made as the solidified shell 9 grows. A magnetic pole 7 is formed narrow in the tip portion and wide in the bottom portion, and an exciting coil 6 is wound so as to meet its shape and cover its surrounding. As a result, the distance between adjacent magnetic pole tip corners is prolonged and the exciting coil 6 can be wound across almost total length of the magnetic pole 7, thus making it possible to reduce leakage flux and at the same time to increase the magnetomotive force by increasing the molten steel penetration flux.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、金属片の連続鋳造
装置及び連続鋳造方法に係り、特に、電磁石による回転
磁界の印加の下で鋳造する金属片の連続鋳造装置及び連
続鋳造方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a continuous casting apparatus and a continuous casting method for metal pieces, and more particularly to a continuous casting apparatus and a continuous casting method for metal pieces cast under the application of a rotating magnetic field by an electromagnet.

【0002】[0002]

【従来の技術】従来、金属片を連続鋳造する場合に、電
磁石を用いて鋳片の送出の方向を軸とする回転磁界を溶
融金属に印加することにより、良質の鋳片を得る連続鋳
造装置が知られている。特開平9−29403号公報に
このような連続鋳造装置の代表例が記載されている。
2. Description of the Related Art Conventionally, in continuous casting of metal slabs, a continuous casting apparatus for obtaining high quality slabs by applying a rotating magnetic field to the molten metal using an electromagnet as an axis in the direction of the slab delivery. It has been known. Japanese Patent Application Laid-Open No. 9-29403 describes a typical example of such a continuous casting apparatus.

【0003】図5〜図7は、従来における金属片の連続
鋳造装置の構成例を示したもので、図5は外観構成を示
す斜視図、図6は水平断面図、図7は垂直断面図であ
る。金属片の連続鋳造装置は、モールド1、ノズル2、
冷却装置4、ヨーク5に設けられた磁極7′及び励磁コ
イル6′からなる電磁石を具備し、ノズル2を介してモ
ールド1内に供給された溶鋼3は冷却装置4で冷却さ
れ、モールド1との接触面に凝固シェル9が生成され
る。この凝固シェル9が成長しながら2基の回転ロール
10によって下方向へ導伴され、鋼片11となって連続
的に送り出される。
FIGS. 5 to 7 show an example of the configuration of a conventional continuous casting apparatus for metal pieces. FIG. 5 is a perspective view showing the external configuration, FIG. 6 is a horizontal sectional view, and FIG. 7 is a vertical sectional view. It is. The continuous casting apparatus for metal pieces includes a mold 1, a nozzle 2,
The cooling device 4 includes an electromagnet including a magnetic pole 7 ′ and an exciting coil 6 ′ provided on the yoke 5. The molten steel 3 supplied into the mold 1 via the nozzle 2 is cooled by the cooling device 4, and A solidified shell 9 is generated on the contact surface of the solid. The solidified shell 9 is guided downward by the two rotating rolls 10 while growing, and is continuously sent out as a billet 11.

【0004】上記電磁石は、モールド1の外周に設けら
れた枠状のヨーク5と、このヨーク5の内側に配置され
た4つの磁極7′と、この磁極7′の外周に巻かれた4
つの励磁コイル6′とからなり、この4つの励磁コイル
6′に2つの交流電源8が接続される。この交流電源8
によって励磁コイル6′に交流電流が供給されると、向
かい合う磁極間に溶鋼貫通磁束12が発生し、これによ
って溶鋼3内に、鋼片11の送出の方向を軸とする均一
な回転磁界が発生する。
The electromagnet includes a frame-shaped yoke 5 provided on the outer periphery of the mold 1, four magnetic poles 7 ′ disposed inside the yoke 5, and a coil 4 wound around the outer periphery of the magnetic pole 7 ′.
And two AC power supplies 8 are connected to the four exciting coils 6 '. This AC power supply 8
When an alternating current is supplied to the exciting coil 6 ′, a flux penetrating the molten steel 12 is generated between the magnetic poles facing each other, whereby a uniform rotating magnetic field is generated in the molten steel 3 with the direction of delivery of the steel slab 11 as an axis. I do.

【0005】この回転磁界によって生じるローレンツ力
が鋼片11の送出方向に対し垂直に作用し、鋼片11の
送出方向の流れである注入時の下方流、またその循環流
として発生する上方流の流速を低下させることが出来
る。このため、下方流によって生じていた凝固シェル9
の不均一な成長が防止されると共に、上方流によって生
じていた溶鋼3中の介在物の巻き込みが抑制される。以
下、この効果を電磁ブレーキ作用と呼ぶ。
The Lorentz force generated by the rotating magnetic field acts perpendicularly to the direction in which the steel slab 11 is sent out, so that the downward flow during injection, which is the flow in the direction in which the steel slab 11 is sent out, and the upward flow generated as a circulating flow. The flow rate can be reduced. Therefore, the solidified shell 9 caused by the downward flow
Is prevented, and inclusion of inclusions in the molten steel 3 caused by the upward flow is suppressed. Hereinafter, this effect is called an electromagnetic braking action.

【0006】また、上記回転磁界によって周方向に溶鋼
3の流れが発生する。このためモールド内壁との接触部
から成長する溶鋼凝固シェルが等結晶化され、更に、溶
鋼3内部に含まれるガス成分が均一に拡散するので、生
成する鋼片11の表面の小孔数が減少する。以下、この
効果を電磁攪拌作用と呼ぶ。
The flow of the molten steel 3 is generated in the circumferential direction by the rotating magnetic field. As a result, the solidified shell of molten steel growing from the contact portion with the inner wall of the mold is crystallized equally, and the gas component contained in the molten steel 3 is diffused uniformly, so that the number of small holes on the surface of the steel slab 11 to be generated is reduced. I do. Hereinafter, this effect is called an electromagnetic stirring effect.

【0007】これらの電磁ブレーキ作用、電磁攪拌作用
は溶鋼貫通磁束12が多いほど、大きな効果を得ること
が出来る。
[0007] The greater the amount of magnetic flux penetrating the molten steel 12, the greater the effect of these electromagnetic braking and electromagnetic stirring functions.

【0008】一方、前記電磁石では、溶鋼貫通磁束12
が発生すると同時に、隣り合う2つの磁極間を磁路とす
る漏れ磁束13が発生する。これに関連して、このよう
な従来の連続鋳造装置では、次の点のような課題があ
る。
On the other hand, in the electromagnet, the flux penetrating the molten steel 12
Is generated, a leakage flux 13 having a magnetic path between two adjacent magnetic poles is generated. In connection with this, such a conventional continuous casting apparatus has the following problems.

【0009】従来の回転磁界の印加の下で鋳造する連続
鋳造装置において、回転磁界を得るための電磁石の構造
は、水平断面を見たときの磁極の幅が(以下、磁極の幅
とは、水平断面を見たときの磁極の幅のことを指す)、
根元部分(図6で、ヨーク5寄りの端)から先端部分
(図6で、モールド1寄りの端)まで均一である。ま
た、隣り合う磁極に巻かれる励磁コイル6′どうしが接
触しないように励磁コイル6′は磁極根元部分に集中し
て巻かれている。このため次のような問題がある。
In a conventional continuous casting apparatus that performs casting under the application of a rotating magnetic field, the structure of an electromagnet for obtaining a rotating magnetic field is such that the width of a magnetic pole when viewed in a horizontal section (hereinafter, the width of a magnetic pole is Refers to the width of the magnetic pole when looking at the horizontal section),
It is uniform from the root portion (the end near the yoke 5 in FIG. 6) to the tip portion (the end near the mold 1 in FIG. 6). The exciting coil 6 'is wound around the magnetic pole base so that the exciting coils 6' wound on adjacent magnetic poles do not come into contact with each other. Therefore, there are the following problems.

【0010】(1)隣り合う磁極7′の磁極先端角どう
しを結ぶ距離が短く、この部分の磁路に磁束が集中して
漏れ磁束13となり、溶鋼貫通磁束12が少ない。
(1) The distance connecting the magnetic pole tip angles of the adjacent magnetic poles 7 'is short, and the magnetic flux concentrates on the magnetic path in this portion to become the leakage magnetic flux 13 and the molten steel penetration magnetic flux 12 is small.

【0011】(2)交流電源8により供給する電流値を
大きくすると、磁極根元部分の磁束密度が上限値(飽和
磁束密度)に達しやすく、溶鋼3に作用させることの出
来る磁束密度の上限値が小さい。
(2) When the value of the current supplied by the AC power supply 8 is increased, the magnetic flux density at the base of the magnetic pole tends to reach the upper limit value (saturated magnetic flux density), and the upper limit value of the magnetic flux density that can act on the molten steel 3 is increased. small.

【0012】(3)励磁コイル6′に覆われていない磁
極先端部分からの漏れ磁束13が多く、溶鋼貫通磁束1
2が少なく、また、励磁コイル6′を巻く領域(コイル
断面積)が狭く、大きな起磁力を得られない。
(3) A large amount of leakage flux 13 from the tip of the magnetic pole not covered by the exciting coil 6 ′
2 and the area (coil cross-sectional area) around which the exciting coil 6 'is wound is narrow, and a large magnetomotive force cannot be obtained.

【0013】[0013]

【発明が解決しようとする課題】上記のように、従来の
電磁石による回転磁界の印加の下で金属片の鋳造を行な
う連続鋳造装置は、漏れ磁束があることと、得られる磁
束密度に飽和磁束密度という上限値があることから、得
られる起磁力に上限があり、従って、鋳造片に作用させ
ることの出来る電磁攪拌作用、電磁ブレーキ作用の効果
にも上限があった。
As described above, the conventional continuous casting apparatus for casting a metal piece under the application of a rotating magnetic field by an electromagnet has a leakage flux and a saturated magnetic flux density. Due to the upper limit of the density, there is an upper limit to the magnetomotive force that can be obtained, and therefore, there is also an upper limit to the effects of electromagnetic stirring and electromagnetic braking that can act on the cast piece.

【0014】本発明は上記の課題を解決するためになさ
れたもので、同じ電流密度で得られる起磁力が大きく、
また、飽和磁束密度が高い、回転磁界の印加の下で金属
片の鋳造を行なう連続鋳造装置および連続鋳造方法を提
供することを目的とする。
The present invention has been made to solve the above-mentioned problems, and the magnetomotive force obtained at the same current density is large.
It is another object of the present invention to provide a continuous casting apparatus and a continuous casting method for casting a metal piece under application of a rotating magnetic field having a high saturation magnetic flux density.

【0015】[0015]

【課題を解決するための手段】本発明の請求項1に対応
する金属片の連続鋳造装置は、電磁石による回転磁界の
印加の下で金属片の鋳造を行なう連続鋳造装置におい
て、鋳造対象を垂直方向に流す過程で凝固させるための
モールドと、4つの磁極が、鋳造対象を取り囲むよう
に、隣り合う磁極の軸が一つの水平面上で90度の角度
をなす位置に配置され、向かい合う磁極間に鋳造対象を
貫通する磁束が水平方向に発生する、前記回転磁界を印
加するための電磁石とを具備し、前記4つの磁極は根本
部分の幅より先端部分の幅を狭く形成したことを特徴と
する。
According to the present invention, there is provided a continuous casting apparatus for casting metal pieces under the application of a rotating magnetic field by an electromagnet. The mold for solidification in the process of flowing in the direction and the four magnetic poles are arranged at positions where the axes of adjacent magnetic poles make an angle of 90 degrees on one horizontal plane so as to surround the casting object, between the facing magnetic poles An electromagnet for applying the rotating magnetic field, in which a magnetic flux penetrating the casting object is generated in a horizontal direction, wherein the four magnetic poles are formed so that the width of the tip portion is smaller than the width of the root portion. .

【0016】本発明の請求項2に対応する金属片の連続
鋳造装置は、電磁石による回転磁界の印加の下で金属片
の鋳造を行なう連続鋳造装置において、鋳造対象を垂直
方向に流す過程で凝固させるためのモールドと、4つの
磁極が、鋳造対象を取り囲むように、隣り合う磁極の軸
が一つの水平面上で90度の角度をなす位置に配置さ
れ、向かい合う磁極間に鋳造対象を貫通する磁束が水平
方向に発生する、前記回転磁界を印加するための電磁石
とを具備し、前記4つの磁極は、根本部分に均一な幅の
領域を形成すると共に、この均一幅の領域より先端部分
の幅を狭く形成したことを特徴とする。
According to a second aspect of the present invention, there is provided a continuous casting apparatus for casting a metal piece under the application of a rotating magnetic field by an electromagnet. And a magnetic flux penetrating the casting object between the facing magnetic poles so that the axes of the adjacent magnetic poles form an angle of 90 degrees on one horizontal plane so that the four magnetic poles surround the casting object. And an electromagnet for applying the rotating magnetic field, which is generated in the horizontal direction. The four magnetic poles form a region having a uniform width at a root portion, and a width of a tip portion from the region having the uniform width. Is formed narrow.

【0017】本発明の請求項3に対応する金属片の連続
鋳造装置は、請求項1又は2に対応する金属片の連続鋳
造装置において、前記電磁石のコイルが、磁極形状に合
わせて磁極全体を覆うように巻かれていることを特徴と
する。
According to a third aspect of the present invention, there is provided a continuous casting apparatus for a metal piece according to the first or second aspect, wherein the coil of the electromagnet has a whole magnetic pole adapted to the shape of the magnetic pole. It is characterized by being wound to cover.

【0018】本発明の請求項4に対応する金属片の連続
鋳造方法は、前記請求項3に対応する金属片の連続鋳造
装置を用いて、炭素鋼を鋳造する連続鋳造方法におい
て、鋳造速度が1.6〜5m/minで、前記電磁石に
よって発生する磁界のモールド中央磁極中心部の磁束密
度が0.2〜0.3T、前記回転磁界を発生させるため
の交流電流の周波数が0.3〜1Hzの条件にて鋳造す
ることを特徴とする。
According to a fourth aspect of the present invention, there is provided a continuous casting method for casting carbon steel using the continuous casting apparatus for a metal piece according to the third aspect. 1.6 to 5 m / min, the magnetic flux density of the magnetic field generated by the electromagnet at the center of the mold center magnetic pole is 0.2 to 0.3 T, and the frequency of the alternating current for generating the rotating magnetic field is 0.3 to 0.3 T It is characterized by casting under the condition of 1 Hz.

【0019】本発明の電磁石による回転磁界の印加の下
で鋳造を行なう金属片の連続鋳造装置および連続鋳造方
法は、漏れ磁束を減らすと同時に溶鋼貫通磁束を増加さ
せることが出来、同じ電流密度で得られる起磁力を大き
くすることが出来る。
The continuous casting apparatus and the continuous casting method of a metal piece which performs casting under the application of a rotating magnetic field by the electromagnet of the present invention can reduce the leakage flux and at the same time increase the molten steel penetration flux, and at the same current density The resulting magnetomotive force can be increased.

【0020】[0020]

【発明の実施の形態】以下、図面を参照して本発明の実
施形態を説明する。
Embodiments of the present invention will be described below with reference to the drawings.

【0021】[第1実施形態]図1は本発明の第1実施
形態に係る金属片の連続鋳造装置の外観構成を示す斜視
図、図2は同水平断面図ある。
[First Embodiment] FIG. 1 is a perspective view showing an external configuration of a continuous casting apparatus for metal pieces according to a first embodiment of the present invention, and FIG. 2 is a horizontal sectional view of the same.

【0022】この第1実施形態に係る金属片の連続鋳造
装置は、両端が開口した筒状のモールド1と、モールド
1の開口端の片側よりモールド1に溶鋼3を供給するノ
ズル2と、モールド1の一部を覆うように設置された、
モールド1内の溶鋼3を冷却するための冷却装置4と、
この冷却装置4の一部を覆うように設置され、モールド
1内の溶鋼3に回転磁界を印加するためのヨーク5に設
けられた磁極7及び励磁コイル6からなる電磁石と、溶
鋼3が成長して作られる凝固シェル9およびこの凝固シ
ェル9が成長して作られる鋼片11を、モールド1の溶
鋼3が供給される反対側の開口端から引き抜くための2
基の回転ロール10を具備している。
The apparatus for continuously casting metal pieces according to the first embodiment includes a cylindrical mold 1 having both ends opened, a nozzle 2 for supplying molten steel 3 to the mold 1 from one side of the open end of the mold 1, 1 was installed to cover a part of
A cooling device 4 for cooling the molten steel 3 in the mold 1;
An electromagnet including a magnetic pole 7 and an exciting coil 6 provided on a yoke 5 for applying a rotating magnetic field to the molten steel 3 in the mold 1 is installed so as to cover a part of the cooling device 4, and the molten steel 3 grows. 2 for withdrawing a solidified shell 9 formed by the process and a billet 11 formed by growing the solidified shell 9 from the opposite open end of the mold 1 to which the molten steel 3 is supplied.
A base rotating roll 10 is provided.

【0023】上記ノズル2を介してモールド1内に供給
された溶鋼3は冷却装置4で冷却され、モールド1との
接触面に凝固シェル9が生成される。この凝固シェル9
が成長しながら回転ロール10により下方向へ導伴さ
れ、鋼片11となって連続的に送り出される。すなわ
ち、溶鋼3は、前記従来装置の図7に示したように鋼片
11の送出の方向に対して垂直な方向について、外縁部
から中心に向かって成長していき、また、その成長は、
鋼片11の送出の方向について、ノズル2から離れるほ
ど進んでいる。
The molten steel 3 supplied into the mold 1 via the nozzle 2 is cooled by a cooling device 4, and a solidified shell 9 is formed on a contact surface with the mold 1. This solidified shell 9
Is grown downward by the rotating roll 10 and continuously sent out as a billet 11. That is, the molten steel 3 grows from the outer edge toward the center in a direction perpendicular to the direction of delivery of the steel slab 11, as shown in FIG.
With respect to the direction in which the billet 11 is delivered, the farther from the nozzle 2 the farther the nozzle 11 is advanced.

【0024】上記電磁石は、ヨーク5に設けられた4つ
の磁極7と、この磁極7の外周に巻かれて交流電源8に
接続される4つの励磁コイル6とを有している。磁極7
は、モールド1の外側において、隣り合う磁極の軸が一
つの水平面上で90度の角度をなす位置に配置される。
前記電磁石において、向かい合う2つの磁極7に巻かれ
た励磁コイル6は、相互の磁束を強め合う方向に巻かれ
ており、同じ交流電源8に接続し、向かい合う2つの磁
極7の作る磁束の位相差を0度とする。また、隣り合う
2つの磁極7に巻かれた励磁コイル6は、別々の交流電
源8に接続し、位相差を90度ずらした交流電流を供給
し、隣り合う2つの磁極7の作る磁束の位相差を90度
とする。
The electromagnet has four magnetic poles 7 provided on the yoke 5 and four exciting coils 6 wound around the magnetic poles 7 and connected to an AC power supply 8. Magnetic pole 7
Is arranged at a position where the axes of adjacent magnetic poles form an angle of 90 degrees on one horizontal plane outside the mold 1.
In the electromagnet, the exciting coil 6 wound around the two facing magnetic poles 7 is wound in a direction to reinforce each other's magnetic flux, is connected to the same AC power supply 8, and has a phase difference of the magnetic flux created by the two facing magnetic poles 7. Is 0 degrees. The exciting coil 6 wound around the two adjacent magnetic poles 7 is connected to a separate AC power supply 8 to supply an alternating current with a phase difference of 90 degrees, and the position of the magnetic flux generated by the two adjacent magnetic poles 7 is changed. The phase difference is 90 degrees.

【0025】交流電源8によって励磁コイル6に交流電
流が流れると、強磁性体である磁極7及びヨーク5を介
して、向かい合う磁極7間に溶鋼貫通磁束12が発生す
る。このとき、向かい合う2つの磁極7の間を磁路とす
る2組の溶鋼貫通磁束12の位相差は90度となり、相
互に作用して溶鋼3内には、鋼片11の送出の方向を軸
とする均一な回転磁界が発生する。
When an AC current flows through the exciting coil 6 by the AC power supply 8, a molten steel penetrating magnetic flux 12 is generated between the magnetic poles 7 facing each other via the magnetic poles 7 and the yoke 5, which are ferromagnetic substances. At this time, the phase difference between the two sets of molten steel penetrating magnetic fluxes 12 having a magnetic path between the two magnetic poles 7 facing each other is 90 degrees, and they interact with each other so that the direction in which the steel slab 11 is fed out into the molten steel 3. A uniform rotating magnetic field is generated.

【0026】本実施形態で重要なのは、電磁石の磁極7
及び励磁コイル6の形状であり、磁極先端部分の幅は狭
く、磁極根元部分の幅は広く、励磁コイル6は磁極7の
形状に合わせてその周囲を覆うように巻かれている。
What is important in the present embodiment is that the magnetic pole 7 of the electromagnet is used.
The width of the magnetic pole tip is narrow, the width of the magnetic pole root is wide, and the excitation coil 6 is wound so as to cover the periphery of the magnetic pole 7 in accordance with the shape of the magnetic pole 7.

【0027】磁極7の先端部の幅を狭くすることによ
り、隣り合う磁極先端角どうしの距離が長くなり、漏れ
磁束13を減らすと同時に溶鋼貫通磁束12を増加させ
ることが出来る。これは以下のことから説明される。溶
鋼中心の磁束密度Bg(T)は、磁極7内の磁束密度B
c(T)に比例し、次式で表される。
By reducing the width of the tip of the magnetic pole 7, the distance between the adjacent magnetic pole tip angles becomes longer, and the leakage flux 13 can be reduced and the molten steel penetration flux 12 can be increased. This is explained from the following. The magnetic flux density Bg (T) at the center of the molten steel is the magnetic flux density Bg in the magnetic pole 7.
It is proportional to c (T) and is expressed by the following equation.

【0028】 Bg=(P0/(P0+P1))・Bc ・・・(1) 但し、P0:溶鋼貫通磁束12の通る磁路のパーミアン
ス(H) P1:漏れ磁束13の通る磁路のパーミアンス(H) 上記(1)式において、パーミアンスP1を小さくする
と磁束密度Bcの係数が大きくなり、溶鋼中心の磁束密
度Bgも大きくなるので、磁束が通過する断面積が一定
とすると、向かい合う磁極間の距離を一定に保ったま
ま、溶鋼貫通磁束12を増加させることが出来る。一般
に、2つの磁極間のパーミアンスP(H)は次式で表さ
れ、 P=μS/L ・・・(2) 但し、μ:透磁率(H/m) S:磁路の断面積(m2) L:磁路の長さ(m) 上記(2)式より、パーミアンスPを小さくするには、
磁路Lを長くすれば良いことが分かる。図2に示すよう
に、磁極先端幅を狭くし、漏れ磁束13の磁路を長くす
ることにより、パーミアンスP1は小さくなり溶鋼貫通
磁束12を増加させることが出来る。
Bg = (P0 / (P0 + P1)) · Bc (1) where P0: Permeance of magnetic path through which molten steel penetration magnetic flux 12 passes (H) P1: Permeance of magnetic path through which leakage magnetic flux 13 passes (H) In the above equation (1), when the permeance P1 is reduced, the coefficient of the magnetic flux density Bc increases, and the magnetic flux density Bg at the center of the molten steel also increases. Therefore, if the cross-sectional area through which the magnetic flux passes is constant, the distance between the facing magnetic poles is reduced. The molten steel penetration magnetic flux 12 can be increased while being kept constant. In general, the permeance P (H) between two magnetic poles is represented by the following equation: P = μS / L (2) where μ: magnetic permeability (H / m) S: cross-sectional area of magnetic path (m 2 ) L: Length of magnetic path (m) From equation (2), to reduce permeance P,
It can be seen that the magnetic path L should be lengthened. As shown in FIG. 2, by reducing the width of the magnetic pole tip and lengthening the magnetic path of the leakage magnetic flux 13, the permeance P <b> 1 decreases and the molten steel penetration magnetic flux 12 can be increased.

【0029】また、磁極7の根元部分の幅を広くするこ
とにより、磁極根元部分の磁束密度が上限値(飽和磁束
密度)に達し難くすることが出来る。これは以下のこと
から説明される。
Further, by increasing the width of the root portion of the magnetic pole 7, the magnetic flux density at the root portion of the magnetic pole can be made hard to reach the upper limit value (saturated magnetic flux density). This is explained from the following.

【0030】磁極7内の磁束密度Bcは磁極の材質によ
り上限値(飽和磁束密度)を持つため、溶鋼中心の磁束
密度Bgも上限値を持つ。磁極7内の磁束数Φ(Wb)
は、次式で表される。
Since the magnetic flux density Bc in the magnetic pole 7 has an upper limit (saturated magnetic flux density) depending on the material of the magnetic pole, the magnetic flux density Bg at the center of the molten steel also has an upper limit. Magnetic flux number Φ (Wb) in magnetic pole 7
Is represented by the following equation.

【0031】Φ=Bc・Sc ・・・(3) 但し、Sc:磁極断面積(m2) 図2に示したように、磁極根元部分の幅を大きくし磁極
断面積Scを大きくすることにより、磁束数Φの上限値
を増やすことが出来る。磁極7内の磁束数Φの増加に伴
い、溶鋼部への作用磁束数も増加させることが出来るの
で、溶鋼中心の磁束密度の上限値を大きくすることが出
来る。溶鋼中心の磁束密度の増加に伴い、電磁攪拌、電
磁ブレーキ効果は大きくなるので、溶鋼に作用させるこ
との出来る電磁攪拌、電磁ブレーキ効果の上限を大きく
とることが出来る。
Φ = Bc · Sc (3) where Sc: magnetic pole cross-sectional area (m 2 ) As shown in FIG. 2, by increasing the width of the magnetic pole root portion and enlarging the magnetic pole cross-sectional area Sc. , The upper limit of the number of magnetic fluxes Φ can be increased. As the number of magnetic fluxes Φ in the magnetic pole 7 increases, the number of magnetic fluxes acting on the molten steel portion can also be increased, so that the upper limit of the magnetic flux density at the center of the molten steel can be increased. As the magnetic flux density at the center of the molten steel increases, the electromagnetic stirring and the electromagnetic braking effect increase, so that the upper limit of the electromagnetic stirring and the electromagnetic braking effect that can act on the molten steel can be increased.

【0032】更に、本発明では、磁極7の先端部分の幅
を狭く根元部分の幅を広くすることによって、磁極全体
を覆うように励磁コイル6を巻くことが可能となり、磁
極7の形状に合わせ、磁極全体を覆うように励磁コイル
6を巻くことによって、(a)磁極側面からの漏れ磁束
の磁路を励磁コイル6で遮断することが出来、溶鋼貫通
磁束12を増加させることが出来る。例えば、図2に示
すように、励磁コイル6が磁極7全体を覆う構造とする
と、漏れ磁束13の磁路の断面積が狭くなる。磁路の断
面積Sを小さくすると、(2)式から分かるようにパー
ミアンスP1が小さくなるため、溶鋼貫通磁束12を増
加させることが出来る。
Further, according to the present invention, by narrowing the width of the tip portion of the magnetic pole 7 and widening the width of the root portion, the exciting coil 6 can be wound so as to cover the entire magnetic pole. By winding the exciting coil 6 so as to cover the entire magnetic pole, (a) the magnetic path of the leakage magnetic flux from the side surface of the magnetic pole can be cut off by the exciting coil 6, and the molten steel penetration magnetic flux 12 can be increased. For example, as shown in FIG. 2, when the exciting coil 6 covers the entire magnetic pole 7, the cross-sectional area of the magnetic path of the leakage magnetic flux 13 is reduced. When the cross-sectional area S of the magnetic path is reduced, the permeance P1 is reduced as can be seen from the equation (2), so that the molten steel penetration magnetic flux 12 can be increased.

【0033】(b)また、隣り合う磁極に巻かれるコイ
ルどうしが接触することなく、従来装置に比べコイル断
面積を広くとることが出来、大きな起磁力を得ることが
出来る。
(B) Further, the coils wound around the adjacent magnetic poles do not come into contact with each other, so that the coil cross-sectional area can be made wider than that of the conventional device, and a large magnetomotive force can be obtained.

【0034】本実施形態における具体例として、図4の
実線aに、ヨーク外寸法720(mm)×720(mm)、
向かい合う磁極間距離270(mm)、モールド内寸法1
69(mm)×169(mm)、磁極先端幅70(mm)、磁
極根元幅170(mm)とした場合の磁極内磁束密度Bc
に対する溶鋼中心磁束密度Bgの計算値を示す。合わせ
て、ヨーク外寸法760(mm)×760(mm)、向かい
合う磁極間距離210(mm)、モールド内寸法150
(mm)×150(mm)、磁極幅は先端と根元で等しく1
30(mm)である従来装置の計算値も点線cとして示
す。なお、このとき励磁コイル6を流れている電流の周
波数は5(Hz)である。
As a specific example of the present embodiment, the solid line a in FIG. 4 indicates the yoke outer dimensions 720 (mm) × 720 (mm),
Distance between facing magnetic poles 270 (mm), mold size 1
Magnetic flux density Bc in the magnetic pole when 69 (mm) x 169 (mm), magnetic pole tip width 70 (mm), and magnetic pole base width 170 (mm)
Shows the calculated value of the molten steel center magnetic flux density Bg with respect to. Together, the outer dimensions of the yoke are 760 (mm) x 760 (mm), the distance between the facing magnetic poles is 210 (mm), and the dimension in the mold is 150
(Mm) x 150 (mm), magnetic pole width is equal at tip and root
The calculated value of the conventional device of 30 (mm) is also shown as a dotted line c. At this time, the frequency of the current flowing through the exciting coil 6 is 5 (Hz).

【0035】図4の直線の傾きは(1)式における磁極
内磁束密度Bcの係数を示す。図4より、(1)式にお
ける磁極内磁束密度Bcの係数が、従来装置では約0.
12であったものが、本発明に基づく装置では、約0.
21まで大きくなったことが分かる。また、磁極7の飽
和磁束密度によって決まる溶鋼中心磁束密度Bgの上限
値が約0.18(T)から約0.32(T)まで大きく
なったことも分かる。
The slope of the straight line in FIG. 4 indicates the coefficient of the magnetic flux density Bc in the magnetic pole in the equation (1). As shown in FIG. 4, the coefficient of the magnetic flux density Bc in the magnetic pole in the equation (1) is about 0.
From about 12 to about 0.1 in the device according to the invention.
It can be seen that the size has increased to 21. It can also be seen that the upper limit value of the molten steel center magnetic flux density Bg determined by the saturation magnetic flux density of the magnetic pole 7 has increased from about 0.18 (T) to about 0.32 (T).

【0036】また、上記本発明による装置では、励磁コ
イル6は磁極7全体を覆うように幅75mmで巻かれてお
り、コイル領域の断面積は9.0E−3(mm2)である
のに対し、上記従来装置では励磁コイル6は磁極7の根
元から70(mm)部分までの部分に幅80(mm)で集中
して巻かれており、コイル領域の断面積は、5.6E−
3(mm2)である。すなわち、本発明に基づく装置の方
が、同じ電流密度で得られる起磁力を従来装置より約
1.6倍大きくすることが出来る。例えば、本実施形態
に基づく磁石装置(磁極高さ400mm)を用いて、モー
ルド中心部の磁束密度0.2〜0.3T、電源周波数
0.3〜1Hzの条件にて、炭素鋼を鋳造速度1.6〜
5m/minにて鋳造した結果、 (1)電磁ブレーキ作用と相関のあるモールド内のシェ
ルの厚さの分布を見たとき、シェル厚さの平均値からの
偏差で、本装置がない場合±37%であったものが、本
装置を設置する事により±19.6%にする事が出来
た。 (2)また、電磁攪拌効果と相関のある鋳造片横断面の
等軸晶率は、本装置がない場合は9.8%であったもの
が、本装置を設置する事により45〜50%に等結晶化
する事が出来た。
In the device according to the present invention, the exciting coil 6 is wound with a width of 75 mm so as to cover the entire magnetic pole 7, and the sectional area of the coil region is 9.0E-3 (mm 2 ). On the other hand, in the conventional device described above, the exciting coil 6 is concentratedly wound with a width of 80 (mm) around a portion from the base of the magnetic pole 7 to 70 (mm), and the cross-sectional area of the coil region is 5.6E-
3 (mm 2 ). That is, the device according to the present invention can increase the magnetomotive force obtained at the same current density by about 1.6 times as compared with the conventional device. For example, using a magnet device (magnetic pole height 400 mm) according to the present embodiment, the carbon steel casting speed is set at a magnetic flux density of 0.2 to 0.3 T at the center of the mold and a power supply frequency of 0.3 to 1 Hz. 1.6-
As a result of casting at 5 m / min, (1) When the distribution of the shell thickness in the mold, which is correlated with the electromagnetic braking action, is seen, the deviation from the average value of the shell thickness. What was 37% could be reduced to ± 19.6% by installing this device. (2) In addition, the equiaxed crystal ratio of the cross section of the cast piece, which has a correlation with the electromagnetic stirring effect, was 9.8% in the absence of the present apparatus, but is 45 to 50% by installing the present apparatus. It was able to be crystallized uniformly.

【0037】[第2実施形態]図3に、本発明に係る第
2実施形態の水平断面図を示す。
[Second Embodiment] FIG. 3 shows a horizontal sectional view of a second embodiment according to the present invention.

【0038】この第2実施形態の連続鋳造装置は、第1
実施形態と同様に、モールド1、ノズル2、冷却装置
4、および電磁石を具備し、ノズル2を介してモールド
1内に供給された溶鋼3は冷却装置4で冷却され、モー
ルド1との接触面に凝固シェル9が生成される。この凝
固シェル9が成長しながら図示されていない回転ロール
によって下方向へ導伴され、鋼片11となり連続的に送
り出される。
The continuous casting apparatus according to the second embodiment comprises a first
Similarly to the embodiment, a mold 1, a nozzle 2, a cooling device 4, and an electromagnet are provided, and molten steel 3 supplied into the mold 1 via the nozzle 2 is cooled by the cooling device 4, and a contact surface with the mold 1 is provided. A solidified shell 9 is generated. As the solidified shell 9 grows, it is guided downward by a rotating roll (not shown) to form a billet 11 and is continuously fed.

【0039】前記電磁石は、第1実施形態と同様に、ヨ
ーク5と4つの磁極7を有しており、励磁コイル6には
2つの交流電源8が供給される。このとき向かい合う磁
極間に溶鋼貫通磁束12が発生し、溶鋼3内には、鋼片
11の送出の方向を軸とする均一な回転磁界が発生す
る。また、同時に、隣り合う2つの磁極間を磁路とする
漏れ磁束13が発生する。
The electromagnet has a yoke 5 and four magnetic poles 7 as in the first embodiment, and two AC power supplies 8 are supplied to the exciting coil 6. At this time, a molten steel penetrating magnetic flux 12 is generated between the magnetic poles facing each other, and a uniform rotating magnetic field is generated in the molten steel 3 with the sending direction of the billet 11 as an axis. At the same time, a leakage flux 13 having a magnetic path between two adjacent magnetic poles is generated.

【0040】本実施形態で重要なのは、電磁石の磁極7
及び励磁コイル6の形状であり、磁極先端部分の幅は狭
く、磁極根元部分の幅は広く、磁極根元付近には磁極幅
が均一な部分がある。そして、励磁コイル6は磁極形状
に合わせてその周囲を覆うように巻く。磁極7の先端部
の幅を狭くすることにより、隣り合う磁極先端角どうし
の距離が長くなり、漏れ磁束13を減らすと同時に溶鋼
貫通磁束12を増加させることが出来る。これは以下の
ことから説明される。
What is important in the present embodiment is that the magnetic pole 7 of the electromagnet is used.
And the shape of the exciting coil 6, the width of the tip of the magnetic pole is narrow, the width of the base of the magnetic pole is wide, and there is a portion near the base of the magnetic pole where the magnetic pole width is uniform. Then, the exciting coil 6 is wound so as to cover the periphery thereof in accordance with the shape of the magnetic pole. By reducing the width of the tip of the magnetic pole 7, the distance between adjacent magnetic pole tip angles becomes longer, and the leakage flux 13 can be reduced while the molten steel penetration flux 12 can be increased. This is explained from the following.

【0041】第1実施形態のように、磁極7の先端部分
の幅を狭く、根元部分を広くするのに加えて、磁極7の
根元部分付近に幅が均一な部分を設けることにより、コ
イル断面積を広くとることが出来、第1実施形態よりも
更に、大きな起磁力を得ることが出来る。
As in the first embodiment, in addition to making the width of the tip of the magnetic pole 7 narrow and widening the root, a coil having a uniform width near the root of the magnetic pole 7 is provided. The area can be widened, and a larger magnetomotive force can be obtained than in the first embodiment.

【0042】本実施形態の具体例として、図4の破線b
に、ヨーク外寸法870(mm)×870(mm)、向かい
合う磁極間距離270(mm)、モールド内寸法169
(mm)×169(mm)、磁極先端幅70(mm)、磁極根
元幅170(mm)、磁極幅均一部長さ75(mm)に設定
した場合の磁極内磁束密度Bcに対する溶鋼中心磁束密
度Bgの計算値を示す。なお、このとき励磁コイル6を
流れている電流の周波数は5(Hz)である。図4に示
す破線bより、(1)式における磁極内磁束密度Bcの
係数は、約0.18であることが分かり、第1実施形態
と同様、従来装置に比べ大きくなったことが分かる。
As a specific example of this embodiment, a broken line b in FIG.
The outer dimensions of the yoke are 870 (mm) x 870 (mm), the distance between facing magnetic poles is 270 (mm), and the dimension in the mold is 169.
(Mm) x 169 (mm), magnetic pole tip width 70 (mm), magnetic pole root width 170 (mm), magnetic pole magnetic flux density Bc relative to magnetic flux density Bc in the magnetic pole when the magnetic pole width uniform length is set to 75 (mm) Shows the calculated value of. At this time, the frequency of the current flowing through the exciting coil 6 is 5 (Hz). From the broken line b shown in FIG. 4, it can be seen that the coefficient of the magnetic flux density Bc in the magnetic pole in the equation (1) is about 0.18, and it is understood that the coefficient is larger than that of the conventional device as in the first embodiment.

【0043】本実施形態では、従来装置に比較して同じ
電流密度で得られる起磁力を約2.7倍大きくすること
が出来、また、第1実施形態と比較しても起磁力を約
1.7倍大きくすることが出来る。また、溶鋼中心磁束
密度Bcの上限値は約0.27Tである。上記実施形態
に基づく装置では、励磁コイル6は磁極7全体を覆うよ
うに幅75mmで巻かれており、コイル領域の断面積は1
5E−3(mm2)である。
In the present embodiment, the magnetomotive force obtained at the same current density can be increased by about 2.7 times as compared with the conventional device, and the magnetomotive force can be increased by about 1 times compared with the first embodiment. 0.7 times larger. The upper limit of the molten steel center magnetic flux density Bc is about 0.27T. In the device according to the above embodiment, the exciting coil 6 is wound with a width of 75 mm so as to cover the entire magnetic pole 7, and the sectional area of the coil region is 1 mm.
5E-3 (mm 2 ).

【0044】[0044]

【発明の効果】以上説明したように、本発明による金属
片の連続鋳造装置では、鋳造対象を取り囲むように、隣
り合う磁極の軸が90度の角度をなして電磁石内に配置
された4つの磁極について、先端部分の幅は狭く、根元
部分の幅は広くするようにしたので、隣り合う磁極先端
角どうしの距離が長くなり、また、磁極形状に合わせて
磁極のほぼ全長にわたって巻くことが出来るため、漏れ
磁束を減らすと同時に溶鋼貫通磁束を増加させることが
出来、同じ電流密度で得られる起磁力を大きくすること
が出来る。また、磁極の先端部分の幅は狭く、根元部分
の幅は広くするのに加えて、磁極の根元部分付近に磁極
幅が均一な部分を設けることにより、更に大きな起磁力
を得ることが出来る。
As described above, in the continuous casting apparatus for a metal piece according to the present invention, four magnetic poles are arranged in the electromagnet such that the axes of adjacent magnetic poles form an angle of 90 degrees so as to surround the casting object. As for the magnetic pole, the width of the tip part is narrow and the width of the root part is wide, so the distance between adjacent magnetic pole tip angles becomes longer, and it is possible to wind almost the entire length of the magnetic pole according to the magnetic pole shape Therefore, it is possible to reduce the leakage magnetic flux and at the same time increase the molten steel penetration magnetic flux, and it is possible to increase the magnetomotive force obtained at the same current density. Further, in addition to the width of the tip portion of the magnetic pole being narrow and the width of the root portion being widened, a greater magnetomotive force can be obtained by providing a portion having a uniform magnetic pole width near the root portion of the magnetic pole.

【0045】また、根元部分の幅を広くすることで、根
元部分の磁束密度が飽和磁束密度に達しにくくなる。
Further, by increasing the width of the root portion, the magnetic flux density of the root portion does not easily reach the saturation magnetic flux density.

【0046】以上のように、同じ電流密度で得られる電
磁石の起磁力が大きくなることで、同じ電流密度で得ら
れる電磁ブレーキ作用および電磁攪拌作用の効果を上げ
ることが出来る。また、同じ電流密度で得られる電磁石
の起磁力が大きくなることと、磁束密度の上限が高くな
ることから、電磁ブレーキ作用および電磁攪拌作用の効
果の上限が高くなる。
As described above, by increasing the magnetomotive force of the electromagnet obtained at the same current density, the effects of the electromagnetic braking action and the electromagnetic stirring action obtained at the same current density can be improved. Further, since the magnetomotive force of the electromagnet obtained at the same current density increases and the upper limit of the magnetic flux density increases, the upper limits of the effects of the electromagnetic braking action and the electromagnetic stirring action increase.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明の第1実施形態に係る金属片の連続鋳造
装置の外観構成を示す斜視図。
FIG. 1 is a perspective view showing an external configuration of a continuous casting apparatus for metal pieces according to a first embodiment of the present invention.

【図2】同実施形態における水平断面図。FIG. 2 is a horizontal sectional view in the embodiment.

【図3】本発明の第2実施形態における水平断面図。FIG. 3 is a horizontal sectional view according to a second embodiment of the present invention.

【図4】本発明装置及び従来装置の磁極内磁束密度に対
する溶鋼中心磁束密度の関係を示す図。
FIG. 4 is a diagram showing the relationship between the magnetic flux density in the magnetic pole and the magnetic flux density at the center of molten steel in the apparatus of the present invention and the conventional apparatus.

【図5】従来における金属片の連続鋳造装置の外観構成
を示す斜視図。
FIG. 5 is a perspective view showing the appearance of a conventional continuous casting apparatus for metal pieces.

【図6】従来の金属片の連続鋳造装置の水平断面図。FIG. 6 is a horizontal sectional view of a conventional continuous casting apparatus for metal pieces.

【図7】従来の金属片の連続鋳造装置の垂直断面図。FIG. 7 is a vertical sectional view of a conventional continuous casting apparatus for metal pieces.

【符号の説明】[Explanation of symbols]

1 モールド 2 ノズル 3 溶鋼 4 冷却装置 5 ヨーク 6 励磁コイル 7 磁極 8 交流電源 9 凝固シェル 10 回転ロール 11 鋼片 DESCRIPTION OF SYMBOLS 1 Mold 2 Nozzle 3 Molten steel 4 Cooling device 5 Yoke 6 Exciting coil 7 Magnetic pole 8 AC power supply 9 Solidification shell 10 Rotating roll 11 Steel bill

───────────────────────────────────────────────────── フロントページの続き (72)発明者 津村 陽一郎 広島県広島市西区観音新町四丁目6番22号 三菱重工業株式会社広島研究所内 (72)発明者 平田 耕一 広島県広島市西区観音新町四丁目6番22号 三菱重工業株式会社広島研究所内 (72)発明者 葛西 正弘 広島県広島市西区観音新町四丁目6番22号 三菱重工業株式会社広島製作所内 Fターム(参考) 4E004 AA09  ──────────────────────────────────────────────────続 き Continuing from the front page (72) Inventor Yoichiro Tsumura 4-22, Kannonshinmachi, Nishi-ku, Hiroshima City, Hiroshima Prefecture Inside the Hiroshima Research Laboratory, Mitsubishi Heavy Industries, Ltd. (72) Koichi Hirata 4-chome Kannonshinmachi, Nishi-ku, Hiroshima City, Hiroshima Prefecture No. 6-22 Mitsubishi Heavy Industries, Ltd. Hiroshima Laboratory (72) Inventor Masahiro Kasai 4-22 Kanon Shinmachi, Nishi-ku, Hiroshima City, Hiroshima Prefecture Mitsubishi Heavy Industries, Ltd. Hiroshima Works F-term (reference) 4E004 AA09

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 電磁石による回転磁界の印加の下で金属
片の鋳造を行なう連続鋳造装置において、 鋳造対象を垂直方向に流す過程で凝固させるためのモー
ルドと、 4つの磁極が、鋳造対象を取り囲むように、隣り合う磁
極の軸が一つの水平面上で90度の角度をなす位置に配
置され、向かい合う磁極間に鋳造対象を貫通する磁束が
水平方向に発生する、前記回転磁界を印加するための電
磁石とを具備し、 前記4つの磁極は根本部分の幅より先端部分の幅を狭く
形成したことを特徴とする金属片の連続鋳造装置。
In a continuous casting apparatus for casting a metal piece under the application of a rotating magnetic field by an electromagnet, a mold for solidifying a casting object in a process of flowing the casting object in a vertical direction, and four magnetic poles surround the casting object. As described above, the axes of adjacent magnetic poles are arranged at a position forming an angle of 90 degrees on one horizontal plane, and a magnetic flux penetrating the casting object between the opposite magnetic poles is generated in the horizontal direction, for applying the rotating magnetic field. An electromagnet, wherein the four magnetic poles are formed so that the width of the tip portion is smaller than the width of the root portion.
【請求項2】 電磁石による回転磁界の印加の下で金属
片の鋳造を行なう連続鋳造装置において、 鋳造対象を垂直方向に流す過程で凝固させるためのモー
ルドと、 4つの磁極が、鋳造対象を取り囲むように、隣り合う磁
極の軸が一つの水平面上で90度の角度をなす位置に配
置され、向かい合う磁極間に鋳造対象を貫通する磁束が
水平方向に発生する、前記回転磁界を印加するための電
磁石とを具備し、 前記4つの磁極は、根本部分に均一な幅の領域を形成す
ると共に、この均一幅の領域より先端部分の幅を狭く形
成したことを特徴とする金属片の連続鋳造装置。
2. A continuous casting apparatus for casting a metal piece under the application of a rotating magnetic field by an electromagnet, wherein a mold for solidifying a casting object in a process of flowing the casting object in a vertical direction, and four magnetic poles surround the casting object. As described above, the axes of adjacent magnetic poles are arranged at a position forming an angle of 90 degrees on one horizontal plane, and a magnetic flux penetrating the casting object between the opposite magnetic poles is generated in the horizontal direction, for applying the rotating magnetic field. An electromagnet; wherein the four magnetic poles form a region having a uniform width in a root portion and a width of a tip portion is formed to be narrower than the region having a uniform width. .
【請求項3】 請求項1又は2に記載の金属片の連続鋳
造装置において、 前記電磁石のコイルが、磁極形状に合わせて磁極全体を
覆うように巻かれていることを特徴とする金属片の連続
鋳造装置。
3. The continuous casting apparatus of a metal piece according to claim 1, wherein the coil of the electromagnet is wound so as to cover the entire magnetic pole according to the shape of the magnetic pole. Continuous casting equipment.
【請求項4】 請求項3に記載の金属片の連続鋳造装置
を用いて炭素鋼を鋳造する連続鋳造方法において、 鋳造速度が1.6〜5m/minで、前記電磁石によっ
て発生する磁界のモールド中央磁極中心部の磁束密度が
0.2〜0.3T、前記回転磁界を発生させるための交
流電流の周波数が0.3〜1Hzの条件にて鋳造するこ
とを特徴とする金属片の連続鋳造方法。
4. A continuous casting method for casting carbon steel using the continuous casting apparatus for metal pieces according to claim 3, wherein a casting speed is 1.6 to 5 m / min and a magnetic field generated by the electromagnet is molded. Continuous casting of a metal piece, wherein the magnetic flux density at the center of the central magnetic pole is 0.2 to 0.3 T, and the frequency of the alternating current for generating the rotating magnetic field is 0.3 to 1 Hz. Method.
JP10228910A 1998-08-13 1998-08-13 Equipment and method for continuous casting of metallic pieces Withdrawn JP2000052006A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10228910A JP2000052006A (en) 1998-08-13 1998-08-13 Equipment and method for continuous casting of metallic pieces

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10228910A JP2000052006A (en) 1998-08-13 1998-08-13 Equipment and method for continuous casting of metallic pieces

Publications (1)

Publication Number Publication Date
JP2000052006A true JP2000052006A (en) 2000-02-22

Family

ID=16883777

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10228910A Withdrawn JP2000052006A (en) 1998-08-13 1998-08-13 Equipment and method for continuous casting of metallic pieces

Country Status (1)

Country Link
JP (1) JP2000052006A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN100406165C (en) * 2003-06-17 2008-07-30 Usinor公司 A continuous casting device that electromagnetically rotates the molten metal moving in the nozzle
JP2020006420A (en) * 2018-07-10 2020-01-16 日本製鉄株式会社 Electromagnetic brake device
CN112074359A (en) * 2018-05-08 2020-12-11 日本制铁株式会社 Electromagnetic stirring device
CN112974749A (en) * 2021-02-09 2021-06-18 东北大学 Electromagnetic stirring device and method for improving feeding capacity and center quality of casting blank liquid core
CN115415507A (en) * 2022-08-12 2022-12-02 中国兵器装备集团西南技术工程研究所 Device for intervening solidification process of aluminum alloy melt through magnetic field

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN100406165C (en) * 2003-06-17 2008-07-30 Usinor公司 A continuous casting device that electromagnetically rotates the molten metal moving in the nozzle
CN112074359A (en) * 2018-05-08 2020-12-11 日本制铁株式会社 Electromagnetic stirring device
JP2020006420A (en) * 2018-07-10 2020-01-16 日本製鉄株式会社 Electromagnetic brake device
CN112974749A (en) * 2021-02-09 2021-06-18 东北大学 Electromagnetic stirring device and method for improving feeding capacity and center quality of casting blank liquid core
CN115415507A (en) * 2022-08-12 2022-12-02 中国兵器装备集团西南技术工程研究所 Device for intervening solidification process of aluminum alloy melt through magnetic field

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