JPS6255942B2 - - Google Patents
Info
- Publication number
- JPS6255942B2 JPS6255942B2 JP55042356A JP4235680A JPS6255942B2 JP S6255942 B2 JPS6255942 B2 JP S6255942B2 JP 55042356 A JP55042356 A JP 55042356A JP 4235680 A JP4235680 A JP 4235680A JP S6255942 B2 JPS6255942 B2 JP S6255942B2
- Authority
- JP
- Japan
- Prior art keywords
- wall
- electromagnetic
- molten steel
- convex magnetic
- magnetic poles
- 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.)
- Expired
Links
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B22—CASTING; POWDER METALLURGY
- B22D—CASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
- B22D11/00—Continuous casting of metals, i.e. casting in indefinite lengths
- B22D11/10—Supplying or treating molten metal
- B22D11/11—Treating the molten metal
- B22D11/114—Treating the molten metal by using agitating or vibrating means
- B22D11/115—Treating the molten metal by using agitating or vibrating means by using magnetic fields
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- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Continuous Casting (AREA)
- Mixers With Rotating Receptacles And Mixers With Vibration Mechanisms (AREA)
Description
【発明の詳細な説明】
本発明は、断面長方形の鋼片を製造するために
使用される連続鋳造設備において、水平断面長方
形状鋳型銅壁又は該鋳型銅壁から引き抜かれる鋼
片に適用する電磁撹拌装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention is directed to an electromagnetic system applied to a mold copper wall having a rectangular horizontal cross section or a steel billet drawn from the mold copper wall in continuous casting equipment used for producing steel billets with a rectangular cross section. Regarding a stirring device.
近年、高級鋼種を対象とする連続鋳造設備にお
いては、鋼片内溶鋼に水平回転運動を与えて、等
軸晶率の向上と介在物の浮上を図る電磁撹拌装置
が提供されている。 In recent years, in continuous casting equipment for high-grade steel grades, electromagnetic stirring devices have been provided that apply horizontal rotational motion to molten steel within a billet to improve equiaxed crystallinity and float inclusions.
この電磁撹拌装置は、誘導電動機の原理を応用
したものであつて、鋼片に、回転磁界を生じしめ
る固定子を配置し、該回転磁界によつて鋼片内の
溶鋼に水平回転運動を与えるようにしたものであ
る。 This electromagnetic stirring device applies the principle of an induction motor, and a stator that generates a rotating magnetic field is placed in a steel billet, and the rotating magnetic field gives horizontal rotational motion to the molten steel inside the steel billet. This is how it was done.
上記のように、電磁撹拌装置を用いれば、等軸
晶率の向上や介在物の浮上を図れるのであるが、
従来の円筒鉄心形電磁撹拌装置においては、鋳型
銅壁が水平断面長方形又は正方形等の角形である
場合、鋳型銅壁や鋼片のコーナー部に乱流が発生
しやすく、この乱流が原因で鋳型内溶鋼液面上の
フラツクスが溶鋼中に巻き込まれたりあるいは製
造された鋼片の撹拌該当位置に発生する負偏析量
が顕著になる等の不具合がある。 As mentioned above, using an electromagnetic stirring device can improve the equiaxed crystallinity and float inclusions.
In conventional cylindrical core electromagnetic stirrers, when the copper mold wall has a rectangular or square horizontal cross section, turbulence tends to occur at the corners of the copper mold wall and the steel billet. There are problems such as the flux on the liquid surface of the molten steel in the mold getting caught up in the molten steel, or the amount of negative segregation occurring at the stirring position of the manufactured steel bill becoming noticeable.
特に、鋳型銅壁が水平断面長方形である場合、
鋼片の長側面に沿つて流れる回転速度が短側面に
沿つて流れる回転速度より速くなる関係で、溶鋼
回転方向に見て長側面から短側面に至る2つのコ
ーナ部における乱流が激しく、鋼片内溶鋼の円滑
な水平回転運動が得られないという不具合があつ
た。 In particular, if the molded copper wall has a rectangular horizontal cross section,
Because the rotational speed of the flow along the long side of the steel piece is faster than the rotational speed of the flow along the short side of the piece, the turbulence at the two corners from the long side to the short side when viewed in the direction of rotation of the molten steel is intense, and the steel There was a problem that smooth horizontal rotation of the molten steel within the piece could not be achieved.
本発明は、水平断面が長方形である鋳型銅壁又
は該鋳型銅壁から引抜かれる鋼片に適用する電磁
撹拌装置の改良を目的とするものであつて、溶鋼
回転方向に見て鋼片の長側面から短側面に至る2
つのコーナ部における溶鋼流れ方向を制御するこ
とによつて、溶鋼の上記コーナ部における乱流を
緩和し、円滑な水平回転運動を行なわしめ、以つ
て、スラツクスの巻き込みによる鋼質劣化の防止
をホワイトバンドの改善を図ろうとするものであ
る。 The purpose of the present invention is to improve an electromagnetic stirring device that is applied to a copper mold wall having a rectangular horizontal cross section or a steel billet drawn from the copper wall. From the side to the short side 2
By controlling the flow direction of the molten steel at the two corners, the turbulence of the molten steel at the corners is alleviated and smooth horizontal rotational movement is achieved, thereby preventing steel quality deterioration due to slacks getting caught. This is an attempt to improve the band.
本発明に係る電磁撹拌装置は、鉄心が水平断面
長方形状であつてかつ各側壁の内面に1つの凸形
磁極を有し、各長壁の凸形磁極が中立位置より鋳
型銅壁内溶鋼又は鋼片内溶鋼の回転方向寄りに偏
在する一方各短壁の凸形磁極が中立位置又は上記
溶鋼の回転方向と反対の方向寄りに偏在し、上記
各長壁の凸形磁極に1つの電磁コイルが巻回され
る一方上記各短壁の凸形磁極に今1つの電磁コイ
ルが巻回されてなり略電気角π/2の位相差を有
する2相の交流を、その一方を各長壁の凸形磁極
の電磁コイルにまたその他方を各短壁の凸形磁極
の電磁コイルに夫々流して溶鋼に水平回転運動を
与えるようにしたことを特徴としている。 The electromagnetic stirring device according to the present invention has an iron core having a rectangular horizontal cross section and one convex magnetic pole on the inner surface of each side wall, and the convex magnetic pole of each long wall is connected to the molten steel or steel in the mold copper wall from a neutral position. One electromagnetic coil is wound around the convex magnetic pole of each long wall, while the convex magnetic poles of each short wall are unevenly distributed in the neutral position or in the direction opposite to the rotational direction of the molten steel. On the other hand, an electromagnetic coil is wound around the convex magnetic poles of each of the short walls, and a two-phase alternating current having a phase difference of approximately electrical angle π/2 is transmitted, one of which is connected to the convex magnetic poles of each long wall. The molten steel is characterized in that the molten steel is given horizontal rotational motion by flowing the current into one electromagnetic coil and the other into an electromagnetic coil having convex magnetic poles on each short wall.
この電磁撹拌装置によれば、上記2つのコーナ
部において、中心からコーナ部方向への磁界が強
くなり、その結果、強い電磁力が磁界の方向に対
して直角方向、つまり上記コーナ部を逸れる方向
に作用するので、溶鋼の上記コーナ部における巻
き込みが緩和され、溶鋼の全体的回転運動が円滑
となる。したがつて、鋳型銅壁の上記コーナ部の
摩耗の軽減や、ホワイトバンドの防止を図ること
ができる。 According to this electromagnetic stirring device, the magnetic field from the center to the corner becomes stronger at the two corners, and as a result, the strong electromagnetic force is directed in a direction perpendicular to the direction of the magnetic field, that is, in a direction that deviates from the corner. Therefore, the entrainment of the molten steel at the corner portions is alleviated, and the overall rotational movement of the molten steel becomes smooth. Therefore, it is possible to reduce wear on the corner portions of the mold copper wall and to prevent white bands.
上記鋳型銅壁における他の1対のコーナ部、つ
まり溶鋼の回転方向に見て鋼片の短側面から長側
面に至るコーナ部では、溶鋼の流れは加速されに
くいので、乱流は生じにくい。 In the other pair of corners of the copper mold wall, that is, the corners extending from the short side to the long side of the billet when viewed in the direction of rotation of the molten steel, the flow of the molten steel is less likely to be accelerated, so turbulence is less likely to occur.
以下に、本発明を図示の実施例について具体的
に説明する。尚、この実施例は、電磁撹拌装置を
鋳型銅壁に適用した例であるが、鋳型銅壁より引
き抜かれる鋼片にも適用できるものである。 The present invention will be specifically described below with reference to illustrated embodiments. Although this embodiment is an example in which the electromagnetic stirring device is applied to a copper mold wall, it can also be applied to a steel piece drawn from a copper mold wall.
第1図に電磁撹拌装置1を、第3図に電磁撹拌
装置1を鋳型銅壁5の外周に嵌め込んだ状態を示
している。電磁撹拌装置1は鋳型銅壁5と相似形
であつて、両者共水平断面長方形状である。 FIG. 1 shows the electromagnetic stirring device 1, and FIG. 3 shows the state in which the electromagnetic stirring device 1 is fitted into the outer periphery of the mold copper wall 5. The electromagnetic stirring device 1 has a similar shape to the mold copper wall 5, and both have a rectangular horizontal cross section.
固定子1は珪素鋼板の成層鉄心よりなり、その
各壁2a,2a′;2b,2b′はその内面に、凸形
磁極3a,3a′;3b,3b′を有している。ま
た、上記各凸形磁極3a,3a′;3b,3b′は各
壁2a,2a′;2b,2b′の中立位置(中心線
0,0′上)より一方向に偏在している。すなわ
ち、第3図に示す如く、鋳型銅壁5内の溶鋼の回
転方向を矢印×方向とすれば、各長壁2a,2
a′の凸形磁極3a,3a′は中立位置より回転方向
寄りに偏在する一方、各短壁2b,2b′の凸形磁
極3b,3b′は中立位置より反回転寄りに偏在し
ている。尚、上記凸形磁極3b,3b′は中立位置
にあつてもよい。 The stator 1 is made of a laminated core of silicon steel plates, and each of its walls 2a, 2a'; 2b, 2b' has convex magnetic poles 3a, 3a'; 3b, 3b' on its inner surface. Further, each of the convex magnetic poles 3a, 3a'; 3b, 3b' is unevenly distributed in one direction from the neutral position (on the center line 0, 0') of each wall 2a, 2a'; 2b, 2b'. That is, as shown in FIG. 3, if the rotation direction of the molten steel in the mold copper wall 5 is the arrow
The convex magnetic poles 3a, 3a' of a' are unevenly distributed in the direction of rotation from the neutral position, while the convex magnetic poles 3b, 3b' of each short wall 2b, 2b' are unevenly distributed in the anti-rotation direction from the neutral position. Incidentally, the convex magnetic poles 3b, 3b' may be in neutral positions.
上記長壁2a,2a′の対向凸形磁極3a,3
a′には1つの電磁コイル4aを同方向に巻回し、
また、短壁2b,2b′の対向凸形磁極3b,3
b′には今1つの電磁コイル4bを同方向に巻回し
ている。尚、これらの電磁コイル4a,4bは自
己冷却形であつて、第2図に示すように、本体4
cの中心が中空になつていて、該中空部4d内に
冷却水を流すようにしている。本体4cの外周に
は絶縁層4eを形成している。 Opposing convex magnetic poles 3a, 3 of the long walls 2a, 2a'
One electromagnetic coil 4a is wound in the same direction on a',
Moreover, the opposing convex magnetic poles 3b, 3 of the short walls 2b, 2b'
Another electromagnetic coil 4b is wound around b' in the same direction. Note that these electromagnetic coils 4a and 4b are of a self-cooling type, and as shown in FIG.
The center of c is hollow, and cooling water is allowed to flow into the hollow part 4d. An insulating layer 4e is formed on the outer periphery of the main body 4c.
また、上記各凸形磁極3a,3a′;3b,3
b′は、磁気抵抗を小さくするため、鋳型銅壁5の
各壁6a,6a′;6b,6b′に対するエヤーギヤ
ツプを小ならしめる。 In addition, each of the above convex magnetic poles 3a, 3a'; 3b, 3
b' reduces the air gap for each wall 6a, 6a'; 6b, 6b' of the mold copper wall 5 in order to reduce the magnetic resistance.
上記各凸形磁極の各電磁コイル4a,4bには
第5図に示した電気角π/2の位相差をもつて
2相の交流u,vを流すようになつている。すな
わち長壁2a,2a′の磁極3a,3a′の電磁コイ
ル4aにはu相の交流を流す一方、短壁2b,2
b′の磁極3b,3b′の電磁コイル4bにはv相の
交流を流すようにしている。 Two-phase alternating currents u and v are passed through the electromagnetic coils 4a and 4b of each convex magnetic pole with a phase difference of electrical angle π/2 as shown in FIG. That is, U-phase alternating current is passed through the electromagnetic coils 4a of the magnetic poles 3a, 3a' of the long walls 2a, 2a', while the short walls 2b, 2a'
V-phase alternating current is applied to the magnetic pole 3b of b' and the electromagnetic coil 4b of 3b'.
今、各相の交流の電磁コイル内の流れ方向が例
えば第4図に示す方向(図中印は紙面奥方向へ
の流れを示し、○・印は紙面手前方向への流れを示
す)であるとすれば、u相の交流の流れによつ
て、φuの磁界が生じ、またv相の交流の流れに
よつて、φvの磁界が生じる。つまり、鋳型銅壁
5内における、電磁コイル4aに基づく磁界φu
の方向は凸形磁極3a′から3aへの斜め方向であ
り、また、電磁コイル4bに基づく磁界φvの方
向は凸形磁極3bから3b′への斜め方向である。
各相の交流の電磁コイル内の流れ方向が逆方向に
なれば磁界の方向も逆方向となる。尤も何れの場
合も一定の漏れ磁束は生じる。 Now, the flow direction of each phase of alternating current in the electromagnetic coil is, for example, the direction shown in Figure 4 (the marks in the figure indicate the flow toward the back of the page, and the ○ marks indicate the flow toward the front of the page). Then, the u-phase alternating current flow produces a magnetic field φu, and the v-phase alternating current flow produces a magnetic field φv. In other words, the magnetic field φu based on the electromagnetic coil 4a within the mold copper wall 5
The direction is an oblique direction from the convex magnetic poles 3a' to 3a, and the direction of the magnetic field φv based on the electromagnetic coil 4b is an oblique direction from the convex magnetic poles 3b to 3b'.
If the flow direction of each phase of alternating current in the electromagnetic coil is reversed, the direction of the magnetic field is also reversed. However, in either case, a certain amount of leakage flux occurs.
u相の電流Iu,v相の電流Ivは夫々次式で表わ
される(但しIm:最大電流)
Iu=Im sinωt
Iv=Im sin(ωt―π/2)
磁界φu,φvの強さは夫々電流Iu,Ivに対応
するが、各電気角π/4,π……における磁界並
びに該磁界に基づく電磁力を第5図,イ〜チに
示している。尚、図中一線矢印は磁界分布を、ま
た二線矢印は電磁力をベクトル表示したもであ
る。 The u-phase current Iu and the v-phase current Iv are respectively expressed by the following formulas (where Im: maximum current) Iu = Im sinωt Iv = Im sin (ωt-π/2) The strengths of the magnetic fields φu and φv are respectively expressed by the current Corresponding to Iu, Iv, the magnetic field at each electrical angle π/4, π... and the electromagnetic force based on the magnetic field are shown in FIG. In the figure, the single-line arrow represents the magnetic field distribution, and the double-line arrow represents the electromagnetic force as a vector.
今、電気角ωtが0の場合について考えると、
u相の電流は0であり、v相はマイナスの電流―
Imである。したがつて、磁界φvのみがイに示
す方向、つまり、凸形磁極3bから3b′への方向
に作用し、電磁力F1は磁界φvに対する直交方
向つまり鋳型銅壁5の短壁6b′(又は鋼片の短側
面)沿いに該短壁6b′と長壁6a(又は鋼片の長
側面)のコーナ部Aに向つて作用する。 Now, considering the case where the electrical angle ωt is 0,
The current in the u phase is 0, and the current in the v phase is negative.
Im. Therefore, only the magnetic field φv acts in the direction shown in A, that is, in the direction from the convex magnetic poles 3b to 3b', and the electromagnetic force F1 acts in the direction orthogonal to the magnetic field φv, that is, in the short wall 6b' of the mold copper wall 5 ( or the short side of the steel piece) toward the corner A of the short wall 6b' and the long wall 6a (or the long side of the steel piece).
電気角ωtがπ/4になると、 ,u相の電流
はプラスの電流となる一方v相の電流はマイナス
の電流になる。したがつて、磁界φuとφvの両
者が生じ、その合成磁界φuvは、ロに示すよう
に、磁界φuとφvとをベクトル合成したものと
なる。この合成磁界φuvに基づく電磁力F2は、
イにおいて電磁力F1によつてコーナ部Aに向け
て移動せしめられた鋳型銅壁内溶鋼を方向転換せ
しめ長壁6aに沿つて移動せしめる方向に作用す
る。 When the electrical angle ωt becomes π/4, the current in the u phase becomes a positive current, while the current in the v phase becomes a negative current. Therefore, both the magnetic fields φu and φv are generated, and the resultant magnetic field φuv is a vector combination of the magnetic fields φu and φv, as shown in FIG. The electromagnetic force F 2 based on this composite magnetic field φuv is
In A, the electromagnetic force F1 acts in a direction to change the direction of the molten steel inside the mold copper wall, which has been moved toward the corner A, and to move it along the long wall 6a.
電気角ωtがπ/2になると、u相の電流はプ
ラスの電流となり、一方v相の電流は0になる。
そうすれば、ハに示すように、磁界はφuのみが
生じ、電磁力F3は大略長壁6a沿いに、詳しく
は、長壁6aから短壁6bに向つてかつ該長壁6
aから離れる方向に作用する。したがつて、鋳型
銅壁内溶鋼は該磁力F3によつて、長壁6aと短
壁6b間のコーナ部Bから幾分反れる方向に移動
せしめられる。 When the electrical angle ωt becomes π/2, the u-phase current becomes a positive current, while the v-phase current becomes 0.
Then, as shown in FIG .
Acts in the direction away from a. Therefore, the molten steel inside the mold copper wall is moved in a direction slightly warped from the corner B between the long wall 6a and the short wall 6b by the magnetic force F3 .
電気角ωtが3π/4になると、u相およびv
相いずれの電流もプラスの電流となる。そうすれ
ば、ハと同方向の磁界φuとロと反対方向の磁界
φvが生じ、その合成磁界φuvはニに示すよう
に非常に強いものとなる。この合成磁界φuvは
中心からコーナ部Bの方向に作用し、これに基づ
く電磁力F4も強くなるとともに鋳型内溶鋼をコ
ーナ部Bから逸れるように大略コーナCの方向に
移動せしめる。したがつてコーナ部Bにおける巻
き込みや乱流は生じにくい。 When the electrical angle ωt becomes 3π/4, the u phase and v
The current in either phase is a positive current. Then, a magnetic field φu in the same direction as C and a magnetic field φv in the opposite direction to B are generated, and the resultant magnetic field φuv becomes extremely strong as shown in D. This composite magnetic field φuv acts from the center in the direction of the corner B, and the electromagnetic force F4 based on this also becomes stronger and moves the molten steel in the mold roughly in the direction of the corner C so as to deviate from the corner B. Therefore, entrainment and turbulence at the corner portion B are less likely to occur.
ホ,ヘ,ト,チは夫々、電気角ωtがπ,5
π/4,3/2・π,7π/4になつた場合の合
成磁界並びに電磁力F5,F6,F7,F8を示してい
る。これらの電磁力F5,F6,F7,F8は夫々イ,
ロ,ハ,ニにおける電磁力F1,F2,F3,F4と同
一大きさでかつ逆方向に作用する。したがつてチ
においても、ニの場合と同様に、鋳型銅壁内溶鋼
がコーナ部Dから逸れるように移動せしめられ、
その結果、溶鋼の巻き込みや乱流は生じにくい。 Ho, He, To, and Chi have electrical angles ωt of π and 5, respectively.
The resultant magnetic field and electromagnetic forces F 5 , F 6 , F 7 , and F 8 are shown in the case of π/4, 3/2·π, and 7π /4. These electromagnetic forces F 5 , F 6 , F 7 , F 8 are respectively a and
It has the same magnitude as the electromagnetic forces F 1 , F 2 , F 3 , and F 4 in B, C, and D, and acts in the opposite direction. Therefore, in case 1, as in case d, the molten steel in the mold copper wall is moved away from the corner D,
As a result, entrainment and turbulence of molten steel are less likely to occur.
上記したように、コーナ部AやCにおいては、
電磁力F1,F5は鋳型内溶鋼を該コーナ部A,C
に巻き込む方向に作用するが、短壁6b,6b′沿
いの流れ距離は短かいので流速は余り大きくな
い。したがつて、該コーナ部A,Cにおける乱流
は余り生じない。 As mentioned above, at corner parts A and C,
Electromagnetic forces F 1 and F 5 move the molten steel in the mold to the corners A and C.
However, since the flow distance along the short walls 6b and 6b' is short, the flow velocity is not very high. Therefore, little turbulence occurs in the corner portions A and C.
以上の磁界制御によつて鋳型銅壁内溶鋼は全体
的に円滑な回転運動をする。 By controlling the magnetic field as described above, the molten steel within the copper mold wall rotates smoothly as a whole.
尚、u相およびv相の交流は2Hz〜12Hz程度の
低周波が好ましい。 Note that the u-phase and v-phase alternating currents preferably have a low frequency of about 2 Hz to 12 Hz.
上記実施例では、2相の交流u,vは電気角
π/2の位相差を有するが、本発明はこれに限定
されるものではなく、この2相の交流u,vの位
相差はπ/2より多少は外れていても上記と略同
様の作用・効果を生ずる。 In the above embodiment, the two-phase alternating currents u and v have a phase difference of π/2 in electrical angle, but the present invention is not limited to this, and the phase difference between the two-phase alternating currents u and v is π Even if it deviates from /2 to some extent, substantially the same action and effect as above will be produced.
上に説明したように、本発明に係る電磁撹拌装
置によれば、2対の凸形磁極の位置を中立位置よ
り所定の方向に偏位させるという簡単な構造によ
つて、鋼片内溶鋼のコーナ部における流動を制御
でき、所期の目的を達成できるものである。 As explained above, the electromagnetic stirring device according to the present invention has a simple structure in which the positions of the two pairs of convex magnetic poles are deviated from the neutral position in a predetermined direction, thereby stirring the molten steel in the billet. The flow in the corners can be controlled and the intended purpose can be achieved.
図面は本発明の実施例を示し、第1図は鉄心に
電磁コイルを巻回した電磁撹拌装置を示す斜視
図、第2図は電磁コイルの断面図、第3図は鋳型
銅壁の外周に固定子を嵌め込んだ状態を示す平面
図、第4図は電磁コイルに一方向の電流が流れた
場合の磁界を示す説明図、第5図は電磁コイル
に流す2相の電流の波形図、第5図,イ〜チは
第5図の各電気角における磁界および電磁力を
示す説明図である。
1……電磁撹拌装置、2a,2a′……電磁撹拌
装置1の長壁、2b,2b′……電磁撹拌装置1の
短壁、3a,3a′;3b,3b′……凸形磁極、4
a,4b……電磁コイル、5……鋳型銅壁、6
a,6a′……鋳型銅壁5の長壁、6b,6b′……
鋳型銅壁5の短壁、A,B,C,D……鋳型銅壁
5のコーナ部。
The drawings show embodiments of the present invention, and FIG. 1 is a perspective view showing an electromagnetic stirring device in which an electromagnetic coil is wound around an iron core, FIG. A plan view showing the state in which the stator is fitted, Fig. 4 is an explanatory diagram showing the magnetic field when a unidirectional current flows through the electromagnetic coil, Fig. 5 is a waveform diagram of two-phase current flowing through the electromagnetic coil, 5, 1 to 1 are explanatory diagrams showing the magnetic field and electromagnetic force at each electrical angle in FIG. 5. 1... Electromagnetic stirring device, 2a, 2a'... Long wall of electromagnetic stirring device 1, 2b, 2b'... Short wall of electromagnetic stirring device 1, 3a, 3a'; 3b, 3b'... Convex magnetic pole, 4
a, 4b...Electromagnetic coil, 5...Mold copper wall, 6
a, 6a'...Long wall of mold copper wall 5, 6b, 6b'...
Short walls of the molded copper wall 5, A, B, C, D...corner parts of the molded copper wall 5.
Claims (1)
銅壁又は該鋳型銅壁から引き抜かれる鋼片の周囲
に配置して使用される電磁撹拌装置であつて、 鉄心が水平断面長方形状であつてかつ各側壁の
内面に1つの凸形磁極を有し、各長壁の凸形磁極
が中立位置より鋳型銅壁内溶鋼又は鋼片内溶鋼の
回転方向寄りに偏在する一方各短壁の凸形磁極が
中立位置又は上記溶鋼の回転方向と反対の方向寄
りに偏在し、上記各長壁の凸形磁極に1つの電磁
コイルが巻回される一方上記各短壁の凸形磁極に
今1つの電磁コイルが巻回されてなり、 略電気角π/2の位相差を有する2相の交流
を、その一方を各長壁の凸形磁極の電磁コイルに
またその他方を各短壁の凸形磁極の電磁コイルに
夫々流して溶鋼に水平回転運動を与えるようにし
たことを特徴とする電磁撹拌装置。[Scope of Claims] 1. An electromagnetic stirring device used by being placed around a mold copper wall having a rectangular horizontal cross section in continuous casting equipment or around a steel piece drawn from the mold copper wall, the iron core having a rectangular horizontal cross section. and has one convex magnetic pole on the inner surface of each side wall, and the convex magnetic pole of each long wall is unevenly distributed in the direction of rotation of the molten steel in the mold copper wall or the molten steel in the billet from the neutral position, while the convex magnetic pole of each short wall is The convex magnetic poles are unevenly distributed in a neutral position or in a direction opposite to the rotational direction of the molten steel, and one electromagnetic coil is wound around the convex magnetic poles on each of the long walls, while one electromagnetic coil is wound around the convex magnetic poles on each of the short walls. Two electromagnetic coils are wound, and one of the two-phase alternating current having a phase difference of approximately electrical angle π/2 is sent to the electromagnetic coil of the convex magnetic pole of each long wall, and the other is connected to the convex magnetic pole of each short wall. An electromagnetic stirring device characterized in that a horizontal rotational motion is imparted to molten steel by flowing through the electromagnetic coils of magnetic poles.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4235680A JPS56139262A (en) | 1980-03-31 | 1980-03-31 | Electromagnetic stirrer in continuous casting plant |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4235680A JPS56139262A (en) | 1980-03-31 | 1980-03-31 | Electromagnetic stirrer in continuous casting plant |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56139262A JPS56139262A (en) | 1981-10-30 |
| JPS6255942B2 true JPS6255942B2 (en) | 1987-11-24 |
Family
ID=12633747
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4235680A Granted JPS56139262A (en) | 1980-03-31 | 1980-03-31 | Electromagnetic stirrer in continuous casting plant |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56139262A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2502996A1 (en) * | 1981-04-03 | 1982-10-08 | Rotelec Sa | ROTATING FIELD ELECTROMAGNETIC INDUCTOR AND CONTINUOUS CASTING LINGOTIERE EQUIPMENT FOR METALS THEREOF |
| JP5428780B2 (en) * | 2009-11-11 | 2014-02-26 | 新日鐵住金株式会社 | Steel continuous casting method |
-
1980
- 1980-03-31 JP JP4235680A patent/JPS56139262A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56139262A (en) | 1981-10-30 |
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