JPH08197196A - Molten metal flow control device - Google Patents
Molten metal flow control deviceInfo
- Publication number
- JPH08197196A JPH08197196A JP1067295A JP1067295A JPH08197196A JP H08197196 A JPH08197196 A JP H08197196A JP 1067295 A JP1067295 A JP 1067295A JP 1067295 A JP1067295 A JP 1067295A JP H08197196 A JPH08197196 A JP H08197196A
- Authority
- JP
- Japan
- Prior art keywords
- mold
- molten metal
- slots
- electromagnet core
- electric coils
- 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.)
- Granted
Links
Landscapes
- Continuous Casting (AREA)
Abstract
(57)【要約】
【目的】 連続鋳造モ−ルドの鋳型片直近の溶融金属上
層部を効果的に流動駆動する。
【構成】 複数個のx方向に延びy方向に分布するスロ
ットを有し、スロット間の歯の先端が鋳型内の溶融金属
上面に対向しかつ鋳型開口内にある電磁石コア(10);ス
ロットに挿入され、電磁石コア(10)の各スロットの基底
部(10b)を周回する胴巻きで電磁石コア(10)に装着さ
れ、一部分が鋳型上端面の上方に位置する、複数個の電
気コイル(1Aa〜2Ca);および、スロットの配列方向yに
沿う推力を溶融金属に与えるための位相差がある交流電
圧を電気コイルのそれぞれに印加する通電手段(20F1);
を備える。
(57) [Summary] [Purpose] To effectively drive the molten metal upper layer near the mold piece of continuous casting mold. An electromagnet core (10) having a plurality of slots extending in the x direction and distributed in the y direction, the tips of the teeth between the slots facing the upper surface of the molten metal in the mold and within the mold opening; A plurality of electric coils (1Aa ~), which are inserted and attached to the electromagnet core (10) with a body winding that circulates the base portion (10b) of each slot of the electromagnet core (10), and a part of which is located above the upper end surface of the mold. 2Ca); and an energizing means (20F1) for applying an alternating voltage having a phase difference for applying a thrust force along the slot arrangement direction y to the molten metal to each of the electric coils;
Is provided.
Description
【0001】[0001]
【産業上の利用分野】本発明は、鋳型内溶融金属の流動
速度を調節する流動制御装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a flow control device for adjusting the flow rate of molten metal in a mold.
【0002】[0002]
【従来技術】例えば連続鋳造では、タンデイッシュより
鋳型に溶鋼が注入され、鋳型において溶鋼は鋳型壁面か
ら次第に冷却されつつ引き抜かれる。同一高さの鋳型壁
面における温度が不均一であると、表面割れやシェル破
断を生じ易い。これを改善するために、従来は、リニア
モ−タを用いて、鋳型内で溶鋼を鋳型壁面に沿って流動
駆動する(例えば特開平1−228645号公報)。2. Description of the Related Art For example, in continuous casting, molten steel is poured into a mold from a tundish, and in the mold, the molten steel is drawn out while gradually cooling from the wall surface of the mold. If the temperatures on the wall surfaces of the mold having the same height are not uniform, surface cracks and shell breakages are likely to occur. In order to improve this, conventionally, a linear motor is used to drive the molten steel to flow along the wall surface of the mold in the mold (for example, JP-A 1-228645).
【0003】図8の(a)に鋳型の垂直断面図を示し、
図8の(b)には鋳型の上方から鋳型内溶鋼の上面(メ
ニスカス)を見おろした平面を示す。ノズル30から鋳
型内には(a)に実線矢印で示すように溶鋼が流れ込
み、鋳型短片方向およびやや下方向に溶鋼流,を生
じ、これが鋳型短片に当って一部は上方に他は下方に流
れる。上方に流れる溶鋼流,が、メニスカスでは図
8の(b)に実線矢印で示すように、ノズル30に向か
う表層流を生ずる。この表層流はメニスカス上のパウダ
を巻き込み易い。一方、溶鋼が固体に変わるときにCO
などの気体(気泡)が発生する。加えて、鋳型内面の一
部に溶鋼が滞留するとパウダが溶鋼に残留し易くしかも
ブレ−クアウトの原因となる焼付きとなり易い。これら
を防止するため、表層に図8の(b)に2点鎖線矢印で
示すような、安定した整流を形成させるのが良い。FIG. 8 (a) shows a vertical sectional view of the mold.
FIG. 8B shows a plane looking down on the upper surface (meniscus) of the molten steel in the mold from above the mold. Molten steel flows from the nozzle 30 into the mold as shown by the solid arrow in (a), and a molten steel flow is generated in the direction of the mold short piece and slightly downward, which hits the mold short piece and part of it is upward and the other is downward. Flowing. In the meniscus, the molten steel flow that flows upward generates a superficial flow toward the nozzle 30, as indicated by a solid arrow in FIG. This superficial flow easily entrains powder on the meniscus. On the other hand, when molten steel changes to solid, CO
Such as gas (air bubbles) is generated. In addition, if the molten steel stays on a part of the inner surface of the mold, the powder is likely to remain on the molten steel, and further seizure that causes breakout is likely to occur. In order to prevent these, it is preferable to form stable rectification on the surface layer as shown by the double-dotted chain line arrow in FIG.
【0004】溶鋼流,の起こす表層流に対して、図
10の(b)に示すように、鋳型長片に沿ったリニアモ
−タ3RFおよび3RLで点線矢印で示す方向の電磁駆
動力を溶鋼に与えて、図10の(c)に実線矢印で示す
ような、鋳型内壁1に沿う循環流を溶鋼の表層に生起で
きれば、この循環流は、表層部に図10の(b)に2点
鎖線矢印で示すような循環流を定速度で安定して発生さ
せることになり、これにより、気泡の浮上が促進され、
溶鋼中へのパウダ巻き込みがなくなり、表層付近の鋳型
内面がきれいにぬぐわれて溶鋼の滞留がなくなる。With respect to the surface flow caused by the molten steel flow, as shown in FIG. 10 (b), the electromagnetic driving force in the direction indicated by the dotted arrow is applied to the molten steel in the linear motors 3RF and 3RL along the mold long piece. Given that a circulating flow along the mold inner wall 1 as shown by the solid arrow in FIG. 10 (c) can be generated in the surface layer of the molten steel, this circulating flow is indicated by a two-dot chain line in FIG. 10 (b) in the surface layer portion. A circulating flow indicated by an arrow will be stably generated at a constant speed, which promotes the floating of bubbles,
The powder is not entrained in the molten steel, the inner surface of the mold near the surface layer is wiped clean, and the molten steel does not stay.
【0005】ところで、リニアモータの電磁石として従
来より一般的に使用されているものでは、電磁石コアに
切られた各スロットに亀の子状(6角形)の電気コイル
の一辺を挿入したコイルエンド方式がある。すなわち、
例えば3相リニアモ−タの場合では、スロットにその配
列順にNo.1,2,3,・・・と番号を付け、スロッ
トNo.1と2の間の歯にNo.2と番号を付けるとする
と、第1番の亀の子状の電気コイルの相対向する1対の
長辺の一方をスロットNo.1に他方をスロットNo.
3に挿入してスロット間の歯(No.2,3)2個を周回させ、
第2番の電気コイルの相対向する1対の長辺の一方をス
ロットNo.2に他方をスロットNo.4に挿入してス
ロット間の歯(No.3,4)2個を周回させ、第3番の電気コ
イルの相対向する1対の長辺の一方をスロットNo.3
に他方をスロットNo.5に挿入してスロット間の歯(N
o.4,5)2個を周回させるという具合に、各電気コイルを
電磁石コアに装着するものである。このようなコイルエ
ンド方式は、力率が大であり、高周波の電源を使用する
ことが可能であるので電源容量を小さくすることができ
る。つまり、設備費が低い。By the way, a coil end type in which one side of a tortoise-shaped (hexagonal) electric coil is inserted into each slot cut in the electromagnet core has been commonly used as an electromagnet of a linear motor. There is. That is,
For example, in the case of a three-phase linear motor, No. The slot numbers are numbered 1, 2, 3 ,. If the teeth between Nos. 1 and 2 are numbered No. 2, one of the pair of long sides of the No. 1 tortoise-shaped electric coil facing each other is slot No. 2. 1 to the other slot No.
Insert into 3 and orbit two teeth (No.2,3) between slots,
One of the pair of long sides facing each other of the second electric coil is slot No. 2 to the other slot No. No. 3, 4 teeth inserted between the slots, and one of the pair of long sides of the No. 3 electric coil facing each other is inserted into the slot No. 4. Three
To the other slot No. 5 and insert the teeth between the slots (N
o.4,5) Each electric coil is attached to the electromagnet core in such a manner that two coils are wound. Such a coil end system has a large power factor and can use a high-frequency power source, so that the power source capacity can be reduced. That is, the equipment cost is low.
【0006】[0006]
【発明が解決しようとする課題】しかし、上述のコイル
エンド方式においては電磁石コアより突出するコイルエ
ンドが大きく、スロットが延びる方向xの突出長が長
く、しかもスロットが分布する方向yのコア外の長さ
(2短辺長の和)が長い。加えて、例えば上述の例で
は、スロットNo.3の側端外方(x方向)に、第1,
第2および第3の電気コイルの短辺(コイルエンド)が
重なって張り出すなど、大量のコイルエンドが電磁石コ
アの側端外方に存在して、リニアモ−タ全体の幅を非常
に大きくしている。However, in the above-mentioned coil end system, the coil end protruding from the electromagnet core is large, the protruding length in the direction x in which the slots extend is long, and the outside of the core in the direction y in which the slots are distributed is large. The length (sum of two short sides) is long. In addition, for example, in the above example, the slot number. To the outside (x direction) of the side edge of 3
A large amount of coil ends exist outside the side ends of the electromagnet core, such that the short sides (coil ends) of the second and third electric coils overlap and project, which greatly increases the overall width of the linear motor. ing.
【0007】ところが鋳型(モ−ルド)の幅(短辺長)
は比較的に狭く、鋳型に溶鋼を注入するノズルが鋳型開
口の実質上中心位置に存在し、しかもノズル上方のタン
ディッシュとモ−ルド上端の間の空間が挟く限られてい
るので、コイルエンド方式のリニアモ−タをモ−ルド開
口上方に配設しにくいという問題がある。リニアモ−タ
を小型にすると溶融金属に与える推力が小さくなる。大
きな推力を与えるためには、モールドを改造しなければ
ならず設備費が大となる。However, the width of the mold (short side length)
Is relatively narrow, the nozzle for injecting molten steel into the mold is located substantially at the center of the mold opening, and the space between the tundish above the nozzle and the top of the mold is limited so that the coil There is a problem that it is difficult to dispose the end type linear motor above the mold opening. When the linear motor is downsized, the thrust applied to the molten metal becomes small. In order to give a large thrust, the mold must be modified and the equipment cost becomes large.
【0008】本発明は、モ−ルド内溶融金属にモ−ルド
開口側から効果的に推力を与えることを目的とする。An object of the present invention is to effectively apply a thrust to the molten metal in the mold from the side of the opening of the mold.
【0009】[0009]
【課題を解決するための手段】本発明の溶融金属の流動
制御装置は、複数個のx方向に延びy方向に分布するス
ロットを有し、スロット間の歯の先端が鋳型内の溶融金
属上面に対向しかつ鋳型開口内にある電磁石コア(10);
スロットに挿入され、電磁石コア(10)の各スロットの基
底部(10b)を周回する胴巻きで電磁石コア(10)に装着さ
れ、一部分が鋳型上端面の上方に位置する、複数個の電
気コイル(1Aa〜2Ca);および、スロットの配列方向yに
沿う推力を溶融金属に与えるための位相差がある交流電
圧を電気コイルのそれぞれに印加する通電手段(20F1);
を備える。なお、カッコ内には、理解を容易にするた
め、図面に示し後述する実施例の対応要素の記号を、参
考までに付記した。The molten metal flow control apparatus of the present invention has a plurality of slots extending in the x direction and distributed in the y direction, and the tips of the teeth between the slots are the upper surface of the molten metal in the mold. An electromagnet core (10) opposite to and in the mold opening;
A plurality of electric coils, each of which is inserted into the slot and attached to the electromagnet core (10) by a body winding that circulates around the base portion (10b) of each slot of the electromagnet core (10), a part of which is located above the upper end surface of the mold ( 1Aa to 2Ca); and an energizing means (20F1) for applying an AC voltage having a phase difference for applying thrust to the molten metal along the slot arrangement direction y to each of the electric coils;
Is provided. In addition, in order to facilitate understanding, symbols in the parentheses that correspond to the elements shown in the drawings and described later are added for reference.
【0010】本発明の好ましい実施例は、y方向に延び
相対向する1対の長辺(5F,5L)とx方向に延び相対向す
る1対の短辺(3R,3L)を含む鋳型の、1対の長辺の一方
(5F)に沿って分布しx方向に延びる複数個の第1組のス
ロットを有し、スロット間の歯の先端が、1対の短辺の
一方(3R)に近い位置の鋳型内溶融金属上面に対向しかつ
鋳型開口内にある、第1電磁石コア(10);第1組のスロ
ットに挿入され、第1電磁石コア(10)の各スロットの基
底部(10b)を周回する胴巻きで第1電磁石コア(10)に装
着され、一部分が前記一方の長辺(5F)の上端面の上方に
位置する、複数個の第1組の電気コイル(1Aa〜2Ca);第
1組のスロットの配列方向yに沿う推力を溶融金属に与
えるための位相差がある交流電圧を第1組の電気コイル
(1Aa〜2Ca)のそれぞれに印加する第1通電手段(20F1);
1対の長辺の他方(5L)に沿って分布しx方向に延びる複
数個の第2組のスロットを有し、スロット間の歯の先端
が、1対の短辺の他方(3L)に近い位置の鋳型内溶融金属
上面に対向しかつ鋳型開口内にある、第2電磁石コア(2
0);第2組のスロットに挿入され、第2電磁石コア(20)
の各スロットの基底部(20b)を周回する胴巻きで第2電
磁石コア(20)に装着され、一部分が前記他方の長辺(5L)
の上端面の上方に位置する、複数個の第2組の電気コイ
ル(4Ab〜5Cb);および、第2組のスロットの配列方向y
に沿う推力を溶融金属に与えるための位相差がある交流
電圧を第2組の電気コイル(4Ab〜5Cb)のそれぞれに印加
する第2通電手段(20L2);を備える。A preferred embodiment of the present invention is a mold comprising a pair of long sides (5F, 5L) extending in the y direction and facing each other and a pair of short sides (3R, 3L) extending in the x direction and facing each other. One of a pair of long sides
Molten metal in a mold having a plurality of first sets of slots distributed along (5F) and extending in the x direction, and the tips of the teeth between the slots being close to one of the pair of short sides (3R) A first electromagnet core (10) facing the upper surface and within the mold opening; inserted in the first set of slots and wrapped around the base (10b) of each slot of the first electromagnet core (10) with a body winding 1. A plurality of first sets of electric coils (1Aa to 2Ca) mounted on the electromagnet core (10) and partially located above the upper end surface of the one long side (5F); An AC voltage having a phase difference for applying a thrust force along the arrangement direction y to the molten metal, the first set of electric coils
First energizing means (20F1) applied to each of (1Aa to 2Ca);
It has a plurality of second sets of slots distributed along the other (5L) of the pair of long sides and extending in the x direction, and the tips of the teeth between the slots are on the other (3L) of the pair of short sides. A second electromagnet core (2 facing the upper surface of the molten metal in the mold at a close position and located in the mold opening)
0); inserted in the second set of slots, the second electromagnet core (20)
It is attached to the second electromagnet core (20) by a body winding that circulates around the base portion (20b) of each slot, and a part of the other long side (5L)
A plurality of second sets of electric coils (4Ab to 5Cb) located above the upper end surface of the second set, and the array direction y of the second set of slots.
A second energizing means (20L2) for applying an AC voltage having a phase difference for applying a thrust force along the wire to the molten metal to each of the second set of electric coils (4Ab to 5Cb).
【0011】[0011]
【作用】電磁石コア(10)に対して複数個の電気コイル(1
Aa〜2Ca)が胴巻きであるので、複数個の電気コイル(1Aa
〜2Ca)は、同一y軸を周回する形でy方向に分布し、各
電気コイルは1つのスロットのみに挿入されy方向に延
びるコイルエンドを実質上有しない。これにより、スロ
ット間の歯の側端面より外方(x方向)へのコイル突出
長はきわめて小さく、リニアモ−タの全体幅が小さい。
電磁石コア(10)のスロット間の歯の先端をモ−ルド(鋳
型)開口内に挿入して鋳型内壁面近くの溶融金属表面に
近づけることができ、溶融金属に効果的に推力を与える
ことができる。これを、格別な改善を施すことなく、既
存のモ−ルドに実施することができる。[Operation] A plurality of electric coils (1
(Aa ~ 2Ca) is a body winding, so multiple electric coils (1Aa
.About.2Ca) are distributed in the y-direction so as to go around the same y-axis, and each electric coil is inserted into only one slot and has substantially no coil end extending in the y-direction. As a result, the coil protrusion length outward (x direction) from the side end surface of the tooth between the slots is extremely small, and the overall width of the linear motor is small.
The tips of the teeth between the slots of the electromagnet core (10) can be inserted into the mold (mold) opening to bring them closer to the surface of the molten metal near the inner wall surface of the mold, which effectively gives thrust to the molten metal. it can. This can be done in existing modes without any particular improvement.
【0012】加えて、電気コイルの一部分が鋳型上端面
の上方に位置するように鋳型片に近づけてリニアモ−タ
(10+1Aa〜2Ca)を設置するので、鋳型内壁面に沿う推
力が積極的に溶融金属に与えられ、これによる溶融金属
の流動が、溶融金属中の気泡の浮上を促進し、溶融金属
中へのパウダ巻き込みがなくなり、表層付近の鋳型内面
をきれいにぬぐい溶融金属の滞留をなくする。なお、溶
融金属が鋳型内面に滞留すると、鋳型の冷却効果が強く
作用し滞留部の固化が急速に進んで凝固金属が鋳型内面
に固着してブレ−クアウトの原因となることがある。In addition, a part of the electric coil is brought close to the mold piece so that a part of the electric coil is located above the upper end surface of the mold, and the linear motor is moved.
Since (10 + 1Aa ~ 2Ca) is installed, the thrust along the inner wall surface of the mold is positively given to the molten metal, and the flow of the molten metal by this promotes the floating of bubbles in the molten metal, Eliminates powder entrainment, wipes the inner surface of the mold near the surface cleanly, and eliminates retention of molten metal. When the molten metal stays on the inner surface of the mold, the cooling effect of the mold strongly acts, the solidification of the staying portion rapidly progresses, and the solidified metal may adhere to the inner surface of the mold, causing breakout.
【0013】本発明の上述の好ましい実施例は2組のリ
ニアモ−タ(10+1Aa〜2Ca/20+4Ab〜5Cb)を、モ−ル
ド開口(4辺形)の対角位置にそれぞれ鋳型長辺に沿っ
て、しかもそれらの電気コイルの一部が長辺上端面の上
方にあるように長辺に極く近付けて設置するので、溶融
金属表面の表層流を効果的に整えることができる。例え
ば、注入ノズル(30)の突出流により現われる溶融金属表
層流と逆方向の推力(図1に破線矢印で示す)を溶融金属
に与えることができ、その場合には、図10の(c)に
示すような、比較的に整った表層流が形成し、結果とし
て図8の(b)に2点鎖線矢印で示すような比較的に定
速度で安定した循環流が得られる。これにより、気泡の
浮上が促進され、溶融金属中へのパウダ巻き込みがなく
なり、表層付近の鋳型内面がきれいにぬぐわれて溶融金
属の滞留がなくなる。リニアモ−タ(10+1Aa〜2Ca/20
+4Ab〜5Cb)は1対のみであって4角形の空間の2つの
対角方向の1つのみに存在するので、溶融金属上方の空
き空間が多く、他の機器又はセンサの配置が容易であ
る。通電回路も1対で済むので消費電力も少く通電制御
も簡単となる。したがって設備コストおよび維持コスト
が低減する。The above-described preferred embodiment of the present invention includes two sets of linear motors (10 + 1Aa-2Ca / 20 + 4Ab-5Cb) at diagonal positions of the mold opening (quadrilateral) along the long side of the mold. Moreover, since some of these electric coils are installed very close to the long side so that they are above the upper end face of the long side, the surface layer flow on the surface of the molten metal can be effectively arranged. For example, a thrust force (indicated by a broken line arrow in FIG. 1) in a direction opposite to the surface flow of the molten metal generated by the protruding flow of the injection nozzle (30) can be applied to the molten metal, in which case (c) of FIG. As a result, a relatively regular surface layer flow is formed, and as a result, a stable circulating flow at a relatively constant velocity is obtained as indicated by the two-dot chain line arrow in FIG. As a result, the floating of bubbles is promoted, the powder is not caught in the molten metal, the inner surface of the mold near the surface layer is wiped clean, and the molten metal does not stay. Linear motor (10 + 1Aa to 2Ca / 20
Since there is only one pair of + 4Ab to 5Cb) and it exists only in one of the two diagonal directions of the quadrangular space, there is a lot of empty space above the molten metal and other devices or sensors can be easily arranged. . Since only one pair of energizing circuits is required, power consumption is small and energization control is simple. Therefore, equipment costs and maintenance costs are reduced.
【0014】本発明の他の目的および特徴は、図面を参
照した以下の実施例の説明より明らかになろう。Other objects and features of the present invention will become apparent from the following description of embodiments with reference to the drawings.
【0015】[0015]
【実施例】図1に、本発明の一実施例の、リニアモ−タ
の配置を示す。図中5Fおよび5Lは、連続鋳造鋳型の
第1および第2長片、6Rおよび6Lは第1および第2
短片であり、これらが囲む空間に、注入ノズル30を通
して溶鋼が、図1紙面の表側から裏側に向けて(垂直方
向zで上方から下方に)、注入される。各辺(5F,5
L,6R,6L)は銅板1F,1L,3R,3Lに、非
磁性ステンレス板2F,2L,4R,4Lを裏当てした
ものである。なお、鋳型各辺の上端面には図3に示すよ
うに、ステンレスカバ−板が乗っているが、図1および
図2においてはその図示は省略した。DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 shows the arrangement of linear motors according to an embodiment of the present invention. In the figure, 5F and 5L are the first and second long pieces of the continuous casting mold, and 6R and 6L are the first and second long pieces.
Molten steel is injected into the space surrounded by these through the injection nozzle 30 from the front side to the back side of the paper surface of FIG. 1 (from the upper side to the lower side in the vertical direction z). Each side (5F, 5
L, 6R, 6L) is a copper plate 1F, 1L, 3R, 3L backed by a non-magnetic stainless steel plate 2F, 2L, 4R, 4L. A stainless cover plate is placed on the upper end surface of each side of the mold as shown in FIG. 3, but the illustration is omitted in FIGS. 1 and 2.
【0016】この実施例では、鋳型(5F,5L,6
R,6L)内の溶鋼を、3相リニアモ−タ型で長片5L
に沿って右から左に(+yから−yの方向に)駆動する
ために、連続鋳造鋳型(5F,5L,6R,6L)内の
溶鋼の上表面に対向して第1および第2の電磁石コア1
0および20が、注入ノズル30を中心として対角線上
に配置されている。In this embodiment, the molds (5F, 5L, 6
R, 6L) molten steel in 3 phase linear motor type 5L long piece
First and second electromagnets facing the upper surface of the molten steel in a continuous casting mold (5F, 5L, 6R, 6L) for driving right to left along the direction (from + y to -y direction). Core 1
0 and 20 are arranged diagonally around the injection nozzle 30.
【0017】図2の(a)には、第1電磁石コア10の
拡大縦断面(図1の2A−2A線拡大断面)を示すとと
もに、図3には電磁石コア10の拡大横断面(図1の3
A−3A線拡大断面)を示す。これらの図面において寸
法引出線(一点鎖線)間の小形の数字は寸法値(mm)
を示す。なお、第1電磁石コア10を含む第1リニアモ
−タと第2電磁石コア20を含む第2リニアモ−タとは
同一寸法および同一電気定格のものであり、鋳型開口の
中心位置にあるノズル30に対して軸対称に配置されて
いる。2A shows an enlarged vertical section of the first electromagnet core 10 (enlarged section 2A-2A in FIG. 1), and FIG. 3 shows an enlarged transverse section of the electromagnet core 10 (FIG. 1). Of 3
A-3A line enlarged cross section) is shown. In these drawings, the small numbers between the dimension leader lines (chain lines) are the dimension values (mm).
Indicates. The first linear motor including the first electromagnet core 10 and the second linear motor including the second electromagnet core 20 have the same size and the same electric rating, and the nozzle 30 at the center position of the mold opening is They are arranged symmetrically with respect to each other.
【0018】図1〜図3を参照すると、この実施例で
は、電磁石コア10は、y方向に長く、この長手方向y
にスロット用の6個の切欠を等ピッチで形成した、平板
面が櫛形の薄鋼板を積層したものであり、6個のスロッ
トがあり、スロットのそれぞれに電気コイル1Aa〜2
Caが挿入されている。なお、電磁石コア10および電
気コイル1Aa〜2Caは冷却されかつ耐熱カバ−で被
覆されているが、冷却構造およびカバ−は図示を省略し
ている。電磁石コア10は、下面にx方向に延びるスロ
ットがある櫛形であり、各スロットに電気コイルが挿入
され、スロット間の歯が磁極でありその下端面が、連続
鋳造鋳型(5F,5L,6R,6L)内の溶鋼の上表面
に対向している。電気コイル1Aa〜2Caの、電磁石
コア10よりx方向に突出したコイルエンドは、銅板1
F上部(+z方向)の空間において略90度上に向きを
変え、電磁石コア10の上平面を通過している。すなわ
ち電気コイル1Aa〜2Caは、電磁石コア10に「胴
巻き」されている。With reference to FIGS. 1 to 3, in this embodiment, the electromagnet core 10 is long in the y direction, and the longitudinal direction y
Is a stack of thin steel plates with flat plate surfaces in which six notches for slots are formed at equal pitches, and there are six slots, and each of the slots has an electric coil 1Aa-2.
Ca is inserted. Although the electromagnet core 10 and the electric coils 1Aa to 2Ca are cooled and covered with a heat-resistant cover, the cooling structure and the cover are not shown. The electromagnet core 10 has a comb shape having slots extending in the x direction on the lower surface, electric coils are inserted in the respective slots, teeth between the slots are magnetic poles, and lower end surfaces thereof are continuous casting molds (5F, 5L, 6R, 6L) facing the upper surface of the molten steel. The coil ends of the electric coils 1Aa to 2Ca protruding from the electromagnet core 10 in the x direction are the copper plates 1.
In the space in the upper part of F (+ z direction), the direction is turned upward by about 90 degrees, and it passes through the upper plane of the electromagnet core 10. That is, the electric coils 1Aa to 2Ca are “wound around” the electromagnet core 10.
【0019】この実施例では、電気コイル1Aa〜2C
aの内空間に高さ(z)が150mmの電磁石コア10
を通した後、電気コイル1Aa〜2Caの一辺を各スロ
ットに押し込むため、電気コイル1Aa〜2Caの内空
間の高さ方向zの幅は、この実施例では150mmであ
り、スロットの深さ(z)が75mmであるので、電気
コイルをスロットに押し込んだ後は、電気コイルの上辺
とコア10の背面(上面)との間に75mmの空隙を生
ずる。この空隙に、長方形の薄鋼板を積層した補助コア
10aが挿入されている。電磁石コア10および補助コ
ア10aの両者にも、冷却用の流体流路がありこれに冷
媒管が接続されているが、これらの図示は省略した。In this embodiment, the electric coils 1Aa to 2C are used.
An electromagnet core 10 having a height (z) of 150 mm in the inner space of a
After passing through the electric coils 1Aa to 2Ca, one side of the electric coils 1Aa to 2Ca is pushed into each slot. Therefore, the width of the inner space of the electric coils 1Aa to 2Ca in the height direction z is 150 mm in this embodiment, and the slot depth (z ) Is 75 mm, a 75 mm gap is created between the upper side of the electric coil and the back surface (top surface) of the core 10 after the electric coil is pushed into the slot. The auxiliary core 10a in which rectangular thin steel plates are laminated is inserted into this void. Both the electromagnet core 10 and the auxiliary core 10a also have a cooling fluid flow path, to which a refrigerant pipe is connected, but they are not shown.
【0020】電気コイル1Aa〜2Caが、電磁石コア
10に対して胴巻きであるので、各電気コイルは、y方
向にはy方向スロット幅分のみ分布し、従来のコイルエ
ンド方式のリニアモ−タのように、1つの電気コイルが
数スロット分y方向に延びることはなく、これにより電
磁石コア10の外方(x方向)の突出長が短く、リニア
モ−タ(10+1Aa〜2Ca)のx方向幅が狭い。こ
れにより、図3に示すように、電磁石コア10のスロッ
ト間の歯の先端をモ−ルド開口内に挿入しかつ電気コイ
ルの一部を鋳型壁5Fの上方に置く形で、電磁石コア1
0を鋳型辺5Fに極く近付けて配置しうる。つまり、リ
ニアモ−タのx方向幅が狭いので、短辺幅が狭いモ−ル
ドにもリニアモ−タを配設することが可能であり、更に
は、鋳型辺内面直近の溶鋼に効果的に推力を与えるよう
に、電磁石コア10を鋳型辺の直近に配置しうる。Since the electric coils 1Aa to 2Ca are wound around the electromagnet core 10, each electric coil is distributed in the y direction only by the width of the slot in the y direction, which is similar to that of a conventional coil end type linear motor. In addition, one electric coil does not extend in the y direction for several slots, so that the protruding length of the outer side (x direction) of the electromagnet core 10 is short and the width of the linear motor (10 + 1Aa to 2Ca) in the x direction is narrow. . As a result, as shown in FIG. 3, by inserting the tips of the teeth between the slots of the electromagnet core 10 into the mold opening and placing a part of the electric coil above the mold wall 5F, the electromagnet core 1
0 can be placed very close to the mold side 5F. That is, since the width of the linear motor in the x direction is narrow, it is possible to dispose the linear motor even in a mold having a narrow short side width, and further, it is possible to effectively thrust the molten steel near the inner surface of the mold side. The electromagnet core 10 can be placed in the immediate vicinity of the mold side to provide
【0021】図2の(b)に、第2電磁石コア20の拡
大縦断面(図1の2B−2B線拡大断面)を示す。電磁
石コア20も、10と同様な構造であり、長辺5Fおよ
び短辺6Rに対する第1電磁石コア10の配置位置関係
と同じく、長辺5Lおよび短辺6Lに対して位置決めさ
れている。FIG. 2B shows an enlarged vertical section of the second electromagnet core 20 (enlarged section 2B-2B in FIG. 1). The electromagnet core 20 also has a structure similar to that of 10, and is positioned with respect to the long side 5L and the short side 6L, similar to the positional relationship of the first electromagnet core 10 with respect to the long side 5F and the short side 6R.
【0022】図4に、図2の(a),(b)に示す電気
コイル1Aa〜2Caと4Ab〜5Cbの結線および電
源回路との接続態様を示す。この結線は2極(N=2)
のものであり、電気コイルに3相交流(M=3)を通電
する。例えば、電気コイル1Aa〜2Caは、図4では
この順に、u,V,w,U,v,Wと表わしている。そ
して「U」は3相交流のU相の正相通電(そのままの通
電)を、「u」はU相の逆相通電(U相より180度の
位相づれ通電)を表わし、電気コイル「U」にはその巻
始め端にU相が印加されるのに対し、電気コイル「u」
にはその巻終り端にU相が印加されることを意味する。
同様に、「V」は3相交流のV相の正相通電を、「v」
はV相の逆相通電を、「W」は3相交流のW相の正相通
電を、「w」はW相の逆相通電を表わす。図4に示す端
子U11,V11およびW11は、電気コイル1Aa〜
2Caの電源接続端子であり、端子U12,V12およ
びW12は、電気コイル4Ab〜5Cbの電源接続端子
である。FIG. 4 shows the connection between the electric coils 1Aa to 2Ca and 4Ab to 5Cb shown in FIGS. 2A and 2B and the connection with the power supply circuit. This connection has 2 poles (N = 2)
The electric coil is energized with a three-phase alternating current (M = 3). For example, the electric coils 1Aa to 2Ca are represented by u, V, w, U, v, W in this order in FIG. The "U" represents the U-phase positive phase energization of the three-phase alternating current (the energization as it is), and the "u" represents the U-phase reverse phase energization (the phase is energized by 180 degrees from the U phase). , The U-phase is applied to the winding start end, while the electric coil "u"
Means that the U phase is applied to the end of the winding.
Similarly, “V” is the positive phase current of the V phase of the three-phase alternating current,
Indicates V-phase reverse-phase conduction, "W" indicates W-phase positive-phase conduction of three-phase AC, and "w" indicates W-phase reverse-phase conduction. Terminals U11, V11 and W11 shown in FIG.
2Ca is a power supply connection terminal, and terminals U12, V12, and W12 are power supply connection terminals for the electric coils 4Ab to 5Cb.
【0023】図5に、電気コイル1Aa〜2Caに3相
交流を流す電源回路20F1を示す。3相交流電源(3
相電力線)21には直流整流用のサイリスタブリッジ2
2A1が接続されており、その出力(脈流)はインダク
タ25A1およびコンデンサ26A1で平滑化される。平
滑化された直流電圧は3相交流形成用のパワ−トランジ
スタブリッジ27A1に印加され、これが出力する3相
交流のU相が図4に示す電源接続端子U11に、V相が
電源接続端子V11に、またW相が電源接続端子W11
に印加される。FIG. 5 shows a power supply circuit 20F1 for supplying a three-phase alternating current to the electric coils 1Aa to 2Ca. 3-phase AC power supply (3
Phase power line) 21 is a thyristor bridge 2 for DC rectification
2A1 is connected, and its output (pulsating current) is smoothed by the inductor 25A1 and the capacitor 26A1. The smoothed DC voltage is applied to the power transistor bridge 27A1 for forming a three-phase AC, and the U-phase of the three-phase AC output from the power-transistor bridge 27A1 is supplied to the power connection terminal U11 shown in FIG. , And W phase is the power supply connection terminal W11
Is applied to
【0024】電気コイル1Aa〜2Caが、図10の
(b)に点線矢印で示す推力を発生するコイル電圧指令
値VdcA1が位相角α算出器24A1に与えられ、位相
角α算出器24A1が、指令値VdcA1に対応する導通
位相角α(サイリスタトリガ−位相角)を算出し、これ
を表わす信号をゲ−トドライバ23A1に与える。ゲ−
トドライバ23A1は、各相のサイリスタを、各相のゼ
ロクロス点から位相カウントを開始して位相角αで導通
トリガ−する。これにより、トランジスタブリッジ27
A1には、指令値VdcA1が示す直流電圧が印加され
る。For the electric coils 1Aa to 2Ca, the coil voltage command value VdcA1 for generating the thrust indicated by the dotted arrow in FIG. 10B is given to the phase angle α calculator 24A1, and the phase angle α calculator 24A1 commands The conduction phase angle α (thyristor trigger-phase angle) corresponding to the value VdcA1 is calculated, and a signal representing this is given to the gate driver 23A1. Gee
The driver 23A1 starts phase counting of the thyristor of each phase from the zero-cross point of each phase and triggers conduction at the phase angle α. As a result, the transistor bridge 27
A direct current voltage indicated by the command value VdcA1 is applied to A1.
【0025】一方、3相信号発生器31A1は、周波数
指令値Fdcで指定された周波数(この実施例では50H
z)の、定電圧3相交流信号を発生して、比較器29A
1に与える。比較器29A1にはまた、三角波発生器3
0A1が3KHzの、定電圧三角波を与える。比較器2
9A1は、U相信号が正レベルのときには、それが三角
波発生器30A1が与える三角波のレベル以上のとき高
レベルH(トランジスタオン)で、三角波のレベル未満
のとき低レベルL(トランジスタオフ)の信号を、U相
の正区間宛て(U相正電圧出力用トランジスタ宛て)に
ゲ−トドライバ28A1に出力し、U相信号が負レベル
のときには、それが三角波発生器30A1が与える三角
波のレベル以下のとき高レベルHで、三角波のレベルを
越えるとき低レベルLの信号を、U相の負区間宛て(U
相負電圧出力用トランジスタ宛て)にゲ−トドライバ2
8A1に出力する。V相信号およびW相信号に関しても
同様である。ゲ−トドライバ28A1は、これら各相,
正,負区間宛ての信号に対応してトランジスタブリッジ
27A1の各トランジスタをオン,オフ付勢する。これ
により、電源接続端子U11には、3相交流のU相電圧
が出力され、電源接続端子V11に同様なV相電圧が出
力され、また電源接続端子W11に同様なW相電圧が出
力され、これらの電圧の上ピ−ク/下ピ−ク間レベルは
コイル電圧指令値VdcA1で定まる。この3相電圧の周
波数はこの実施例では周波数指令値Fdcにより50Hz
である。すなわち、コイル電圧指令値VdcA1で指定さ
れたピ−ク電圧値(推力)の50Hzの3相交流電圧
が、図2及び図4に示す電気コイル1Aa〜2Caに印
加される。On the other hand, the three-phase signal generator 31A1 has a frequency designated by the frequency command value Fdc (50H in this embodiment).
z), a constant voltage three-phase AC signal is generated, and the comparator 29A
Give to one. The comparator 29A1 also includes a triangular wave generator 3
0A1 gives a constant voltage triangular wave of 3 KHz. Comparator 2
9A1 is a high level H (transistor on) when the U-phase signal has a positive level and is higher than the level of the triangular wave provided by the triangular wave generator 30A1, and a low level L (transistor off) when it is less than the level of the triangular wave. Is output to the gate driver 28A1 to the positive section of the U-phase (to the U-phase positive voltage output transistor), and when the U-phase signal is at a negative level, it is below the level of the triangular wave provided by the triangular wave generator 30A1. When the level is high level H, and when the level of the triangular wave is exceeded, a low level L signal is sent to the negative section of the U phase (U
Gate driver 2 to the phase negative voltage output transistor)
Output to 8A1. The same applies to the V-phase signal and the W-phase signal. The gate driver 28A1 is provided for each of these phases,
Each transistor of the transistor bridge 27A1 is turned on and off in response to a signal addressed to the positive and negative sections. As a result, a U-phase voltage of three-phase AC is output to the power supply connection terminal U11, a similar V-phase voltage is output to the power supply connection terminal V11, and a similar W-phase voltage is output to the power supply connection terminal W11. The level between the upper peak and the lower peak of these voltages is determined by the coil voltage command value VdcA1. In this embodiment, the frequency of the three-phase voltage is 50 Hz according to the frequency command value Fdc.
Is. That is, a three-phase AC voltage of 50 Hz having a peak voltage value (thrust) designated by the coil voltage command value VdcA1 is applied to the electric coils 1Aa to 2Ca shown in FIGS.
【0026】図6に、電気コイル4Ab〜5Cbに3相
交流を流す電源回路20L2を示す。この電源回路20
L2の構成は、上述の20F1と同一であるが、コイル
電圧指令値(VdcB2)が異なる。FIG. 6 shows a power supply circuit 20L2 for supplying a three-phase alternating current to the electric coils 4Ab to 5Cb. This power circuit 20
The configuration of L2 is the same as that of 20F1 described above, but the coil voltage command value (VdcB2) is different.
【0027】すなわち、電気コイル4Ab〜5Cbが図
10の(b)に点線矢印で示す推力を発生するコイル電
圧指令値VdcB2が、位相角α算出器24B2に与えら
れる。これらのコイル電圧指令値VdcA1(図5)およ
びコイル電圧指令値VdcB2(図6)は、図7に示すコ
ンピュ−タ43が、各電源回路20F1および20L2
に与えるものである。That is, the coil voltage command value VdcB2 that causes the electric coils 4Ab to 5Cb to generate the thrust indicated by the dotted arrow in FIG. 10B is given to the phase angle α calculator 24B2. The coil voltage command value VdcA1 (FIG. 5) and the coil voltage command value VdcB2 (FIG. 6) are supplied to the power supply circuits 20F1 and 20L2 by the computer 43 shown in FIG.
To give to.
【0028】図7に、図2に示す鋳型短片6Lおよび6
Rの背部を示す。これらの短片6L,6Rには、熱電対
S31〜S3nおよびS41〜S4nが、それぞれ鋳片
引抜き方向(高さ方向z;上下方向)に各一列で等間隔
に配列され、それぞれの熱電対は、裏当てステンレス板
を貫通し銅板のやや内部の(溶鋼に接する表面部の)温
度を検出する。信号処理回路41A及び41Bが熱電対
が検出する温度を表わすアナログ信号(検出信号)を発
生してアナログゲ−ト42に与える。FIG. 7 shows the mold short pieces 6L and 6 shown in FIG.
The back of R is shown. In these short pieces 6L, 6R, thermocouples S31 to S3n and S41 to S4n are arranged at equal intervals in one row in the slab drawing direction (height direction z; vertical direction), and each thermocouple is The temperature of the inside of the copper plate (on the surface that contacts molten steel) is detected by penetrating the backing stainless steel plate. The signal processing circuits 41A and 41B generate an analog signal (detection signal) representing the temperature detected by the thermocouple and apply it to the analog gate 42.
【0029】コンピュ−タ43は、アナログゲ−ト42
を制御して、熱電対S31〜S3nおよびS41〜S4
nの検出信号を順次に選択してA/D変換して読込み、
高温値抽出処理44により、熱電対S31〜S3nの検
出温度の中の最高温度値Tm1L1および次に高い温度
値Tm2L1を抽出し、かつ、熱電対S41〜S4nの
検出温度の中の最高温度値Tm1R1および次に高い温
度値Tm2R1を抽出する。そして、短片6Lの代表温
度 (Tm1L1−Tm2L1)×0.7+TM2L1 を算出し、短片6Rの代表温度 (Tm1R1−Tm2R1)×0.7+TM2R1 を算出して、両者の差すなわち短片6L,6R間の代表
温度差 (Tm1L1-Tm2L1)×0.7+TM2L1−(Tm1R1-Tm2R1)×0.7−T
M2R1 を算出して、それが正値(0以上)である(短片6Rの
方が温度が高い)ときには、VdcA1=代表温度差×
A(Aは係数)を算出し、かつ、VdcB2=B−VdcA
1を算出する。代表温度差が負値である(短片15Lの
方が温度が高い)ときには、VdcB2=−代表温度差×
Aを算出し、かつVdcA1=B−VdcB2を算出する。The computer 43 is an analog gate 42.
To control thermocouples S31 to S3n and S41 to S4.
n detection signals are sequentially selected, A / D converted and read,
By the high temperature value extraction process 44, the highest temperature value Tm1L1 and the next highest temperature value Tm2L1 among the detection temperatures of the thermocouples S31 to S3n are extracted, and the highest temperature value Tm1R1 of the detection temperatures of the thermocouples S41 to S4n. And the next highest temperature value Tm2R1. Then, the representative temperature (Tm1L1-Tm2L1) × 0.7 + TM2L1 of the short piece 6L is calculated, the representative temperature (Tm1R1-Tm2R1) × 0.7 + TM2R1 of the short piece 6R is calculated, and the difference between them, that is, the representative between the short pieces 6L and 6R. Temperature difference (Tm1L1-Tm2L1) × 0.7 + TM2L1-(Tm1R1-Tm2R1) × 0.7-T
When M2R1 is calculated and is a positive value (0 or more) (the temperature of the short piece 6R is higher), VdcA1 = representative temperature difference ×
A (A is a coefficient) is calculated, and VdcB2 = B-VdcA
Calculate 1. When the representative temperature difference is a negative value (the temperature of the short piece 15L is higher), VdcB2 = −representative temperature difference ×
A is calculated, and VdcA1 = B−VdcB2 is calculated.
【0030】VdcA1は、短片6R側の電気コイル1A
a〜2Ca(図4)に対する電流レベル(推力)指令値
であり、VdcB2は短片6L側の電気コイル4Ab〜5
Cb(図4)に対する電流レベル(推力)である。これ
らの指令値は、代表温度差が正値(短片6Rの方が温度
が高い;突出流により図11のbに示す不平衡表層流が
推定される)ときには電気コイル1Aa〜2Caの電気
コイルに流す3相交流電流レベルを大きくして強い推力
(図1,図9のbの点線矢印)をかけ、電気コイル4A
b〜5Cbに流す相交流電流レベルを小さくして推力を
弱くし、逆に、代表温度差が負値(短片6Lの方が温度
が高い)ときには、電気コイル4Ab〜5Cbに流す3
相交流電流レベルを大きくして強い推力をかけ、電気コ
イル1Aa〜2Ca流す3相交流電流レベルを小さくし
て推力を弱くすることを意味する。VdcA1 is an electric coil 1A on the short piece 6R side.
a to 2Ca (FIG. 4) is a current level (thrust) command value, and VdcB2 is an electric coil 4Ab to 5B on the short piece 6L side.
It is a current level (thrust) with respect to Cb (FIG. 4). These command values are applied to the electric coils of the electric coils 1Aa to 2Ca when the representative temperature difference is a positive value (the temperature of the short piece 6R is higher; the unbalanced surface layer flow shown in b of FIG. 11 is estimated by the protruding flow). By increasing the level of the three-phase alternating current to be applied and applying a strong thrust (dotted line arrow in FIG. 1 and FIG. 9), the electric coil 4A
When the representative temperature difference is a negative value (the temperature of the short piece 6L is higher), the phase AC current level flowing in b to 5Cb is made smaller, and conversely, when the representative temperature difference is negative (the temperature of the short piece 6L is higher), the electric current is supplied to the electric coils 4Ab to 5Cb
This means increasing the phase AC current level to apply a strong thrust, and decreasing the level of the three-phase AC current flowing through the electric coils 1Aa to 2Ca to weaken the thrust.
【0031】ノズル30から鋳型に流れ込む溶鋼流(図
8のaに示す突出流,)がノズル30に関して実質
上対称であると、短片6Rと6Lの温度は実質上同じと
なり、表層流が図8の(b)および図9の(a)に実線
矢印,で示すようにノズル30に関して対称とな
り、この場合には、VdcA1=VdcB2となって、短片
6R側の電気コイル1Aa〜2Caと短片6L側の電気
コイル4Ab〜5Cbの通電レベルが実質上等しく、第
1電磁石コア10と第2電磁石コア20は、図1および
図8の(b)に点線矢印で示すように、実質上等しい強
さの、方向が逆の推力を溶鋼に与える。これにより、溶
鋼の実際の表層流は、図10の(c)の実線矢印を逆方
向に変えた形となり、図8の(b)に2点鎖線矢印で示
す循環流をもたらす。これにより、気泡の浮上が促進さ
れ、溶鋼中へのパウダ巻き込みがなくなり、表層付近の
鋳型内面がきれいにぬぐわれて溶鋼の滞留がなくなる。
鋳型内溶鋼の温度分布が均一化する。When the molten steel flow (protruding flow shown in FIG. 8a) flowing from the nozzle 30 into the mold is substantially symmetrical with respect to the nozzle 30, the temperatures of the short pieces 6R and 6L are substantially the same, and the surface layer flow is shown in FIG. 9B and FIG. 9A, the nozzles 30 are symmetrical with respect to the nozzle 30, as shown by the solid line arrow. In this case, VdcA1 = VdcB2, and the electric coils 1Aa to 2Ca on the short piece 6R side and the short piece 6L side. The electric current levels of the electric coils 4Ab to 5Cb are substantially equal to each other, and the first electromagnet core 10 and the second electromagnet core 20 have substantially equal strengths, as shown by dotted arrows in FIGS. 1 and 8B. , Thrust is applied in the opposite direction to molten steel. As a result, the actual surface layer flow of the molten steel has a shape in which the solid line arrow in (c) of FIG. 10 is changed in the opposite direction, and the circulating flow shown by the two-dot chain line arrow in (b) of FIG. 8 is provided. As a result, the floating of the bubbles is promoted, the powder is not caught in the molten steel, the inner surface of the mold near the surface layer is wiped clean, and the molten steel does not stay.
Uniform temperature distribution of molten steel in the mold.
【0032】図11の(a)に示すように、短片6Rに
向かう突出流が強く、短片6Lに向かう突出流が弱
くなると、短片6Rの温度が上昇し短片6Lの温度が低
下し、表層流は図11の(b)に実線矢印,で示す
ようにノズル30と短片6Rの間の表層流が強く、ノ
ズル30と短片6Lの間の表層流が弱くなり、この場
合には、VdcA1>VdcB2となって、短片6R側の電
気コイル1Aa〜2Caの通電レベルが高く、短片6L
側の電気コイル4Ab〜5Cbの通電レベルが低くな
り、第1電磁石コア10は強い推力を、第2電磁石コア
20は弱い推力を溶鋼に与える。これにより、図9の
(b)に点線矢印で示すように、第1電磁石コア10は
強い推力を、第2電磁石コア20は弱い推力を溶鋼に与
える。これにより、図8の(b)に2点鎖線矢印で示す
循環流をもたらす。この場合には、この循環流は高温の
短片6R側で高速、低温の短片6L側で低速であるが、
ル−プを描く循環流であるので渦流を生じない。短片6
R側の高温溶鋼を低温の短片6L側に搬送し、温度差を
低減する。この循環流により、気泡の浮上が促進され、
溶鋼中へのパウダ巻き込みがなくなり、表層付近の鋳型
内面がきれいにぬぐわれて溶鋼の滞留がなくなる。鋳型
内溶鋼の温度分布が均一化する。As shown in FIG. 11A, when the protruding flow toward the short piece 6R is strong and the protruding flow toward the short piece 6L is weak, the temperature of the short piece 6R rises and the temperature of the short piece 6L decreases, and the surface layer flow 11B, the superficial flow between the nozzle 30 and the short piece 6R is strong and the superficial flow between the nozzle 30 and the short piece 6L is weak, as indicated by the solid arrow in FIG. 11B. In this case, VdcA1> VdcB2 Therefore, the energization level of the electric coils 1Aa to 2Ca on the short piece 6R side is high, and the short piece 6L is
The energization level of the side electric coils 4Ab to 5Cb becomes low, and the first electromagnet core 10 gives a strong thrust and the second electromagnet core 20 gives a weak thrust to the molten steel. As a result, the first electromagnet core 10 gives a strong thrust to the molten steel, and the second electromagnet core 20 gives a weak thrust to the molten steel, as shown by a dotted arrow in FIG. 9B. As a result, a circulating flow indicated by a two-dot chain line arrow in FIG. In this case, the circulating flow is high speed on the high temperature short piece 6R side and low speed on the low temperature short piece 6L side,
Since it is a circulation flow that draws a loop, no eddy current is generated. Short piece 6
The high temperature molten steel on the R side is conveyed to the low temperature short piece 6L side to reduce the temperature difference. This circulation flow promotes the floating of bubbles,
The powder is not entrained in the molten steel, the inner surface of the mold near the surface layer is wiped clean, and the molten steel does not stay. Uniform temperature distribution of molten steel in the mold.
【0033】逆に、短片6Rに向かう突出流が弱く、
短片6Lに向かう突出流が強くなると、短片6Rの温
度が低下し短片6Lの温度が上昇し、表層流はノズル3
0と短片6Rの間の表層流が弱く、ノズル30と短片
6Lの間の表層流が強くなり、この場合には、VdcA
1<VdcB2となって、短片6R側の電気コイル1Aa
〜2Caの通電レベルが低く、短片6L側の電気コイル
4Ab〜5Cbの通電レベルが高くなり、第1電磁石コ
ア10は弱い推力を、第2電磁石コア20は強い推力を
溶鋼に与える。これにより、図9の(c)に点線矢印で
示すように、第1電磁石コア10は弱い推力を、第2電
磁石コア20は強い推力を溶鋼に与える。これにより、
図8の(b)に2点鎖線矢印で示す循環流をもたらす。
この場合には、この循環流は低温の短片6R側で低速、
高温の短片6L側で高速であるが、ル−プを描く循環流
であるので渦流を生じない。短片6L側の高温溶鋼を低
温の短片6R側に搬送し、温度差を低減する。この循環
流により、気泡の浮上が促進され、溶鋼中へのパウダ巻
き込みがなくなり、表層付近の鋳型内面がきれいにぬぐ
われて溶鋼の滞留がなくなる。鋳型内溶鋼の温度分布が
均一化する。On the contrary, the protruding flow toward the short piece 6R is weak,
When the projecting flow toward the short piece 6L becomes strong, the temperature of the short piece 6R decreases and the temperature of the short piece 6L rises, and the surface layer flow causes the nozzle 3 to flow.
The surface flow between 0 and the short piece 6R is weak, and the surface flow between the nozzle 30 and the short piece 6L is strong. In this case, VdcA
1 <VdcB2, and the electric coil 1Aa on the short piece 6R side
The energization level of ~ 2Ca is low, the energization level of the electric coils 4Ab-5Cb on the short piece 6L side is high, and the first electromagnet core 10 gives a weak thrust and the second electromagnet core 20 gives a strong thrust to the molten steel. As a result, the first electromagnet core 10 gives a weak thrust to the molten steel and the second electromagnet core 20 gives a strong thrust to the molten steel, as shown by a dotted arrow in (c) of FIG. 9. This allows
The circulating flow indicated by the two-dot chain line arrow in FIG.
In this case, this circulation flow is low speed on the side of the low temperature short piece 6R,
Although it is high speed on the side of the high temperature short piece 6L, it does not generate a vortex because it is a circulating flow that draws a loop. The high temperature molten steel on the short piece 6L side is conveyed to the low temperature short piece 6R side to reduce the temperature difference. By this circulating flow, the floating of bubbles is promoted, the powder is not entrained in the molten steel, the inner surface of the mold near the surface layer is wiped clean, and the molten steel does not stay. Uniform temperature distribution of molten steel in the mold.
【0034】上述の実施例では、短片6R,6Lの温度
を熱電対で検出して注入ノズル30からの鋳型内への突
出流の強さ対応の表層流の強さ(流速)を検出し、これ
に対応して安定した循環流(図8のbの2点鎖線矢印)
を生成するための電磁推力を、第1および第2電磁石コ
ア10,20で溶鋼に与えるようにしているが、例え
ば、流速センサで図1のVspaの位置の表層流の速度Vs
aおよびVspbの位置の表層流の速度Vsbを検出して、電
流レベル指示値VdcA1およびVdcB2を、それぞれV
saおよびVsbに反比例する値とするようにしてもよい。
本発明では1対の電磁石のみを鋳型空間の上方に対角方
向に配置しているので、位置Vspa,Vspbの流速を検出
するように流速センサを配設するか、あるいは、位置V
spa,Vspbに対して昇降させることが容易である。In the above-mentioned embodiment, the temperature of the short pieces 6R, 6L is detected by the thermocouple to detect the strength of the surface layer flow (flow velocity) corresponding to the strength of the protruding flow from the injection nozzle 30 into the mold. Correspondingly stable circulation flow (two-dot chain line arrow in Fig. 8b)
Although the electromagnetic thrust for generating is applied to the molten steel by the first and second electromagnet cores 10 and 20, for example, the velocity Vs of the surface layer flow at the position of Vspa in FIG.
The velocity Vsb of the surface flow at the positions of a and Vspb is detected, and the current level instruction values VdcA1 and VdcB2 are respectively set to V
The value may be inversely proportional to sa and Vsb.
In the present invention, since only one pair of electromagnets are diagonally arranged above the mold space, the flow velocity sensor is arranged to detect the flow velocity at the positions Vspa and Vspb, or the position V
It is easy to move up and down with respect to spa and Vspb.
【図1】 本発明の一実施例の、連続鋳造鋳型の溶鋼表
面の上方の、磁極および電気コイルの配列を示す平面図
である。FIG. 1 is a plan view showing an arrangement of magnetic poles and electric coils above the surface of molten steel of a continuous casting mold according to an embodiment of the present invention.
【図2】 図1に示す電磁石コア10および20の拡大
縦断面図である。FIG. 2 is an enlarged vertical sectional view of electromagnet cores 10 and 20 shown in FIG.
【図3】 図1に示す電磁石コア10および20の拡大
横断面図である。3 is an enlarged cross-sectional view of electromagnet cores 10 and 20 shown in FIG.
【図4】 図2に示す電気コイルの結線及び電源回路と
の接続態様を示す電気回路図である。4 is an electric circuit diagram showing a connection mode of the electric coil shown in FIG. 2 and a connection with a power supply circuit.
【図5】 図3に示す電気コイル1Aa〜2Caに3相
交流電圧を印加する電源回路を示す電気回路図である。5 is an electric circuit diagram showing a power supply circuit for applying a three-phase AC voltage to the electric coils 1Aa to 2Ca shown in FIG.
【図6】 図3に示す電気コイル4Ab〜5Cbに3相
交流を印加する電源回路を示す電気回路図である。6 is an electric circuit diagram showing a power supply circuit for applying a three-phase alternating current to the electric coils 4Ab to 5Cb shown in FIG.
【図7】 図1に示す鋳造鋳型の短片6L,6Rの背部
とそれらに備わった熱電対に接続された電気回路を示す
ブロック図である。7 is a block diagram showing the electric circuits connected to the backs of the short pieces 6L and 6R of the casting mold shown in FIG. 1 and the thermocouples provided therein.
【図8】 (a)は図1に示す鋳型(5F,5L,6
F,6R)の垂直断面図、(b)は水平断面図である。FIG. 8 (a) is a template (5F, 5L, 6 shown in FIG.
(F, 6R) is a vertical sectional view, and (b) is a horizontal sectional view.
【図9】 (a)は鋳型内溶鋼の上面を示す平面図、
(b)および(c)は電磁石コウ10,20により鋳型
内溶鋼のメニスカスに誘起される表層流(点線矢印)を
示す平面図である。9 (a) is a plan view showing the upper surface of the molten steel in the mold, FIG.
(B) And (c) is a top view which shows the surface layer flow (dotted line arrow) induced in the meniscus of molten steel in a mold by electromagnet ko, 10.
【図10】 (a)は、鋳型内溶鋼のメニスカスにおけ
る、注入ノズルからの溶鋼注入により生ずる表層流を示
す平面図、(b)は従来の2個のリニアモ−タで生起し
ようとする表層流を点線矢印で示す平面図、(c)は注
入ノズルからの溶鋼注入により生ずる表層流と2個のリ
ニアモ−タの推力により生ずる表層流とのベクトル和を
実線矢印で示す平面図である。FIG. 10 (a) is a plan view showing a superficial flow caused by molten steel injection from an injection nozzle in a meniscus of molten steel in a mold, and FIG. 10 (b) is a superficial flow intended to occur by two conventional linear motors. Is a plan view indicated by a dotted arrow, and (c) is a plan view showing a vector sum of the surface layer flow generated by the molten steel injection from the injection nozzle and the surface layer flow generated by the thrusts of the two linear motors by a solid arrow.
【図11】 (a)は鋳型内溶鋼の断面図、(b)は鋳
型内溶鋼のメニスカスにおける表層流を示す平面図であ
る。11A is a cross-sectional view of the molten steel in the mold, and FIG. 11B is a plan view showing a superficial flow in the meniscus of the molten steel in the mold.
1:鋳型の内壁 1F,1L,3R,3
L:銅板 2F,2L,4R,4L:非磁性ステンレス板 5F,5L:長片 6R,6L:短片 10,20:電磁石コア 10a,20a:補助
コア 10b,20b:基底部 19:流出口 30:注入ノズル 20F1,20L2:
電源回路 PW:パウダ 1Aa,1Ba,1Ca,2Aa,2Ba,2Ca :電気コイル 4Ab,4Bb,4Cb,5Ab,5Bb,5Cb :電気コイル U11,V11,W11/U12,V12,W12:電源接続端子1: Inner wall of mold 1F, 1L, 3R, 3
L: Copper plate 2F, 2L, 4R, 4L: Non-magnetic stainless plate 5F, 5L: Long piece 6R, 6L: Short piece 10, 20: Electromagnetic core 10a, 20a: Auxiliary core 10b, 20b: Base portion 19: Outlet port 30: Injection nozzle 20F1, 20L2:
Power supply circuit PW: Powder 1Aa, 1Ba, 1Ca, 2Aa, 2Ba, 2Ca: Electric coil 4Ab, 4Bb, 4Cb, 5Ab, 5Bb, 5Cb: Electric coil U11, V11, W11 / U12, V12, W12: Power supply connection terminal
Claims (3)
ロットを有し、スロット間の歯の先端が鋳型内の溶融金
属上面に対向しかつ鋳型開口内にある電磁石コア;スロ
ットに挿入され、電磁石コアの各スロットの基底部を周
回する胴巻きで電磁石コアに装着され、一部分が鋳型上
端面の上方に位置する、複数個の電気コイル;および、 スロットの配列方向yに沿う推力を溶融金属に与えるた
めの位相差がある交流電圧を電気コイルのそれぞれに印
加する通電手段;を備える溶融金属の流動制御装置。1. An electromagnet core having a plurality of slots extending in the x-direction and distributed in the y-direction, the tips of the teeth between the slots facing the upper surface of the molten metal in the mold and within the mold opening; A plurality of electric coils, which are attached to the electromagnet core by a body winding that circulates around the base of each slot of the electromagnet core, and a part of which is located above the upper end surface of the mold; and the thrust force along the slot arrangement direction y. A molten metal flow control device, comprising: energizing means for applying an AC voltage having a phase difference to the metal to each of the electric coils.
向に延び相対向する1対の短辺を含む鋳型の、長辺に沿
って分布しx方向に延びる複数個のスロットを有し、ス
ロット間の歯の先端が、鋳型内溶融金属上面に対向しか
つ鋳型開口内にある、電磁石コア;スロットに挿入さ
れ、電磁石コアの各スロットの基底部を周回する胴巻き
で電磁石コアに装着され、一部分が鋳型長辺の上端面の
上方に位置する、複数個の電気コイル;および、 スロットの配列方向yに沿う推力を溶融金属に与えるた
めの位相差がある交流電圧を電気コイルのそれぞれに印
加する通電手段;を備える溶融金属の流動制御装置。2. A plurality of slots distributed along the long side and extending in the x direction of a mold including a pair of long sides extending in the y direction and facing each other and a pair of short sides extending in the x direction and facing each other. An electromagnet core having tips of teeth between slots facing the upper surface of the molten metal in the mold and within the mold opening; the electromagnet core being inserted into the slot and wound around the base of each slot of the electromagnet core. A plurality of electric coils mounted on the upper part of the long side of the mold, and an AC voltage having a phase difference for applying thrust to the molten metal along the slot arrangement direction y. A molten metal flow control device comprising: an energizing means for applying to each of the.
向に延び相対向する1対の短辺を含む鋳型の、1対の長
辺の一方に沿って分布しx方向に延びる複数個の第1組
のスロットを有し、スロット間の歯の先端が、1対の短
辺の一方に近い位置の鋳型内溶融金属上面に対向しかつ
鋳型開口内にある、第1電磁石コア;第1組のスロット
に挿入され、第1電磁石コアの各スロットの基底部を周
回する胴巻きで第1電磁石コアに装着され、一部分が前
記一方の長辺の上端面の上方に位置する、複数個の第1
組の電気コイル;第1組のスロットの配列方向yに沿う
推力を溶融金属に与えるための位相差がある交流電圧を
第1組の電気コイルのそれぞれに印加する第1通電手
段;1対の長辺の他方に沿って分布しx方向に延びる複
数個の第2組のスロットを有し、スロット間の歯の先端
が、1対の短辺の他方に近い位置の鋳型内溶融金属上面
に対向しかつ鋳型開口内にある、第2電磁石コア;第2
組のスロットに挿入され、第2電磁石コアの各スロット
の基底部を周回する胴巻きで第2電磁石コアに装着さ
れ、一部分が前記他方の長辺の上端面の上方に位置す
る、複数個の第2組の電気コイル;および、 第2組のスロットの配列方向yに沿う推力を溶融金属に
与えるための位相差がある交流電圧を第2組の電気コイ
ルのそれぞれに印加する第2通電手段;を備える溶融金
属の流動制御装置。3. A mold having a pair of long sides extending in the y direction and facing each other and a pair of short sides extending in the x direction and facing each other, and distributed along one of the pair of long sides in the x direction. A first electromagnet having a plurality of first sets of slots extending therein, the tips of teeth between the slots facing the upper surface of the molten metal in the mold at a position close to one of the pair of short sides and within the mold opening. Core; inserted in the first set of slots and attached to the first electromagnet core by a body winding that circulates around the base of each slot of the first electromagnet core, and a part thereof is located above the upper end surface of the one long side, A plurality of first
A pair of electric coils; a first energizing means for applying an AC voltage having a phase difference for applying a thrust force along the arrangement direction y of the slots of the first set to the molten metal to each of the electric coils of the first set; It has a plurality of second sets of slots distributed along the other of the long sides and extending in the x direction, and the tips of the teeth between the slots are on the upper surface of the molten metal in the mold at a position near the other of the pair of short sides. A second electromagnet core opposite and within the mold opening; a second
A plurality of first electromagnet cores, each of which is inserted into a set of slots and is wound around the base of each slot of the second electromagnet core, and is attached to the second electromagnet core by a part of which is located above the upper end surface of the other long side. Two sets of electric coils; and a second energizing means for applying an alternating voltage having a phase difference for applying thrust to the molten metal along the array direction y of the second set of slots to each of the second sets of electric coils; A molten metal flow control device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP07010672A JP3089176B2 (en) | 1995-01-26 | 1995-01-26 | Flow controller for molten metal |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP07010672A JP3089176B2 (en) | 1995-01-26 | 1995-01-26 | Flow controller for molten metal |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH08197196A true JPH08197196A (en) | 1996-08-06 |
| JP3089176B2 JP3089176B2 (en) | 2000-09-18 |
Family
ID=11756752
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP07010672A Expired - Lifetime JP3089176B2 (en) | 1995-01-26 | 1995-01-26 | Flow controller for molten metal |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3089176B2 (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100672775B1 (en) * | 2005-12-05 | 2007-01-22 | 김상건 | Coating material for lubricity sheet, preparation method thereof and lubricity sheet |
| JP2008246534A (en) * | 2007-03-30 | 2008-10-16 | Jfe Steel Kk | Steel continuous casting method |
| CN112105469A (en) * | 2018-07-17 | 2020-12-18 | 日本制铁株式会社 | Mold apparatus and continuous casting method |
-
1995
- 1995-01-26 JP JP07010672A patent/JP3089176B2/en not_active Expired - Lifetime
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100672775B1 (en) * | 2005-12-05 | 2007-01-22 | 김상건 | Coating material for lubricity sheet, preparation method thereof and lubricity sheet |
| JP2008246534A (en) * | 2007-03-30 | 2008-10-16 | Jfe Steel Kk | Steel continuous casting method |
| CN112105469A (en) * | 2018-07-17 | 2020-12-18 | 日本制铁株式会社 | Mold apparatus and continuous casting method |
| CN112105469B (en) * | 2018-07-17 | 2022-04-15 | 日本制铁株式会社 | Mold apparatus and continuous casting method |
Also Published As
| Publication number | Publication date |
|---|---|
| JP3089176B2 (en) | 2000-09-18 |
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