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JP2733991B2 - Steel continuous casting method - Google Patents

Steel continuous casting method

Info

Publication number
JP2733991B2
JP2733991B2 JP22491988A JP22491988A JP2733991B2 JP 2733991 B2 JP2733991 B2 JP 2733991B2 JP 22491988 A JP22491988 A JP 22491988A JP 22491988 A JP22491988 A JP 22491988A JP 2733991 B2 JP2733991 B2 JP 2733991B2
Authority
JP
Japan
Prior art keywords
mold
magnetic field
immersion nozzle
molten steel
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.)
Expired - Fee Related
Application number
JP22491988A
Other languages
Japanese (ja)
Other versions
JPH0275456A (en
Inventor
幹雄 鈴木
融 北川
忍 宮原
章生 長棟
義行 金尾
範夫 青
裕則 山本
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.)
JFE Engineering Corp
Original Assignee
Nippon Kokan 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 Nippon Kokan Ltd filed Critical Nippon Kokan Ltd
Priority to JP22491988A priority Critical patent/JP2733991B2/en
Publication of JPH0275456A publication Critical patent/JPH0275456A/en
Application granted granted Critical
Publication of JP2733991B2 publication Critical patent/JP2733991B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B22CASTING; POWDER METALLURGY
    • B22DCASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
    • B22D11/00Continuous casting of metals, i.e. casting in indefinite lengths
    • B22D11/10Supplying or treating molten metal
    • B22D11/11Treating the molten metal
    • B22D11/114Treating the molten metal by using agitating or vibrating means
    • B22D11/115Treating the molten metal by using agitating or vibrating means by using magnetic fields

Landscapes

  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Continuous Casting (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] この発明は鋳型内浸漬ノズルからの吐出流の流速を減
衰すると同時に、片流れを抑制して、鋳型内湯面波動高
さを制御すると共に良好な表面性状を有する製品を製造
する鋼の連続鋳造方法に関する。
The present invention attenuates the flow velocity of the discharge flow from a submerged nozzle in a mold, suppresses one-sided flow, controls the wave height of the molten metal in the mold, and improves the quality. The present invention relates to a method for continuously casting steel for producing a product having a surface property.

[従来の技術] 第6図はスラブの連続鋳造機における鋳型内の溶鋼の
状態を示す図である。この図を参照して従来の技術を説
明する。鋳型1内の溶鋼8の表面には、溶鋼8の酸化防
止と保温、凝固シェル9と鋳型1との間の潤滑、非金属
介在物の吸着等の役目を持つモールドパウダー5があ
る。このモールドパウダー5の湯面側は溶鋼8の熱で溶
融して溶融パウダー6になっており、このモールドパウ
ダー5の大気側は粉状パウダー7となって溶鋼8の表面
を覆っている。溶融パウダー6は凝固シェル9と鋳型1
との間に流入して潤滑剤の役目を果たす。従って溶融パ
ウダー6は消耗するので一定厚のモールドパウダー5を
維持するため、前記溶融パウダー6の消耗量を見合うだ
け補給される。第6図に示すように鋳型1中央に鉛直に
設けられた浸漬ノズル2の先端に設けられた吐出孔3
は、鋳型1短辺に対向して開口している。溶鋼はこの吐
出孔3から鋳型内に吐出される。溶鋼の吐出流4は鋳型
内で鋳型短辺面に向かって斜め下方に注入される。この
溶鋼の吐出流4が、短辺に衝突して上下の2つの流れ、
反転流11と侵入流12に分かれ、短辺面の凝固シェル9に
沿って上昇する反転流11は鋳型1の上部短辺面付近の湯
面波動の原因となる。第7図は湯面波動の概略図であ
る。この湯面波動とは、第7図に示すように浸漬ノズル
2の吐出孔3からの吐出流は反転流11と侵入流12に分か
れるが、反転流11は溶湯表面に到達し、鋳型内の溶湯表
面を波立たせる。この湯面波動を渦流距離計15により測
定し、その電圧値をフィルターを通して高周波数成分
(ここでは10Hz以上の周波数成分)を除去後、ミリボル
ト計で測定した。この渦流距離計15の設置位置は第7図
に示すように、短辺面から50mm、湯面から50mmである。
第8図は約1分間の湯面レベルの経時変化を示す図であ
る。1分間の最大波動レベルを測定し、この最大値を最
大湯面波動高さhとしてデータ処理を行った。上矢印は
上昇方向を意味し、下矢印は下降方向を示す。特に溶鋼
の吐出量が3ton/min以上の高速鋳造においては、浸漬ノ
ズル2の吐出孔3の吐出流速が大きいため、凝固シェル
9に衝突後の反転流11も大きく、大きな湯面波動が発生
する。第9図は最大湯面波動高さと熱延板表面欠陥指数
の関係を示すグラフ図である。この図から明らかなよう
に最大湯面波動高さが4mm〜8mmの範囲で熱延板の表面欠
陥の発生率が少なく最大湯面波動高さに最適範囲があ
る。この湯面波動が大きい場合溶融パウダー6が、溶湯
波動により溶鋼側に巻き込まれ懸濁する。溶鋼中に巻き
込まれた溶融パウダー6は、溶鋼と溶融パウダー6の比
重差により浮上してしまうが、一部凝固シェル9に捕捉
される。一方湯面波動が小さい場合には、溶鋼表面への
新しい溶鋼の供給が少ないので、モールドパウダー5の
溶融性も悪い。従って溶融パウダー6への溶鋼中の介在
物の溶解吸着性が悪くなり、介在物は凝固シェル9に捕
捉され鋳片の内質欠陥となると考えられる。ここで示し
た最大湯面波動高さの適正範囲は4mm〜8mmという値は連
続鋳造操業の経験によって得られた値であり、この範囲
に入るように浸漬ノズル2の形状、浸漬ノズル2の吐出
角度、浸漬ノズル2の吐出孔3の面積、鋳型1の幅等を
規制していた。
[Prior Art] FIG. 6 is a view showing a state of molten steel in a mold in a continuous slab casting machine. The prior art will be described with reference to FIG. On the surface of the molten steel 8 in the mold 1, there is a mold powder 5 having a role of preventing oxidation of the molten steel 8 and keeping it warm, lubricating between the solidified shell 9 and the mold 1, adsorbing nonmetallic inclusions, and the like. The molten metal surface of the mold powder 5 is melted by the heat of the molten steel 8 to form a molten powder 6, and the air side of the mold powder 5 becomes a powdery powder 7 and covers the surface of the molten steel 8. The molten powder 6 comprises a solidified shell 9 and a mold 1
And flows in between to serve as a lubricant. Therefore, since the molten powder 6 is consumed, the mold powder 5 having a constant thickness is maintained, so that the molten powder 6 is replenished in proportion to the consumed amount of the molten powder 6. As shown in FIG. 6, a discharge hole 3 provided at the tip of an immersion nozzle 2 provided vertically in the center of the mold 1
Are open facing the short side of the mold 1. Molten steel is discharged from the discharge holes 3 into the mold. The molten steel discharge stream 4 is injected obliquely downward in the mold toward the short side of the mold. The discharge flow 4 of the molten steel collides with the short side, and the upper and lower two flows,
The reversing flow 11, which is divided into the reversing flow 11 and the inflowing flow 12 and rises along the solidified shell 9 on the short side surface, causes the surface wave near the upper short side surface of the mold 1. FIG. 7 is a schematic view of the surface wave motion. This molten surface wave means that the discharge flow from the discharge hole 3 of the immersion nozzle 2 is divided into a reverse flow 11 and an inflow flow 12 as shown in FIG. 7, but the reverse flow 11 reaches the surface of the molten metal and Make the surface of the melt ruffled. This level wave was measured by an eddy current distance meter 15, and its voltage value was measured by a millivolt meter after removing a high frequency component (here, a frequency component of 10 Hz or more) through a filter. As shown in FIG. 7, the installation position of the eddy current distance meter 15 is 50 mm from the short side surface and 50 mm from the molten metal surface.
FIG. 8 is a diagram showing the change over time of the level of the molten metal for about 1 minute. The maximum wave level for one minute was measured, and the maximum value was used as the maximum wave height h to perform data processing. The upward arrow indicates the upward direction, and the downward arrow indicates the downward direction. In particular, in high-speed casting in which the discharge rate of molten steel is 3 ton / min or more, since the discharge flow velocity of the discharge hole 3 of the immersion nozzle 2 is large, the reversal flow 11 after collision with the solidified shell 9 is large, and a large surface wave is generated. . FIG. 9 is a graph showing the relationship between the maximum surface wave height and the surface defect index of the hot-rolled sheet. As is clear from this figure, when the maximum level wave height is in the range of 4 mm to 8 mm, the incidence of surface defects on the hot-rolled sheet is small, and there is an optimum range for the maximum level wave height. When the level wave of the molten metal is large, the molten powder 6 is caught and suspended in the molten steel by the wave of the molten metal. The molten powder 6 entrained in the molten steel floats due to a difference in specific gravity between the molten steel and the molten powder 6, but is partially captured by the solidified shell 9. On the other hand, when the surface wave is small, the supply of new molten steel to the molten steel surface is small, so that the melting property of the mold powder 5 is poor. Therefore, it is considered that the inclusion and dissolution of inclusions in the molten steel to the molten powder 6 is poor, and the inclusions are trapped by the solidified shell 9 and become internal defects of the slab. The appropriate range of the maximum surface wave height shown here is a value of 4 mm to 8 mm obtained from the experience of the continuous casting operation, and the shape of the immersion nozzle 2 and the discharge of the immersion nozzle 2 fall within this range. The angle, the area of the discharge hole 3 of the immersion nozzle 2, the width of the mold 1, and the like were regulated.

しかしながら、最近の連続鋳造機の生産性の向上のた
め、 (1)一つのタンディッシュ及び浸漬ノズルで数チャー
ジ連続して連続鋳造を行う多連続鋳造技術、 (2)鋳造中の鋳型幅の変更、 (3)鋳造速度が低速から高速に変わる 等で、操業条件が変わってきた。この結果、最初の操業
条件に適した浸漬ノズルの吐出孔の形状や吐出角度では
満足できない操業条件が発生するようになり、湯面波動
高さを最適範囲に制御できなくなった。湯面波動高さを
コントロールする技術として、 (1)直流磁場により吐出流にブレーキを掛ける方法
(*1:以下従来方法1という)で、鋳型長辺面の冷却箱
内に2対の直流磁石を設置し、浸漬ノズルからの吐出流
に対して直流磁場を作用させ、流動する溶鋼内に発生す
る誘導電流と直流磁場とにより、溶鋼の流動とは逆方向
に発生する電磁力により溶鋼の流動を制御するものであ
る。
However, in order to improve the productivity of recent continuous casting machines, (1) a multi-continuous casting technique in which a single tundish and an immersion nozzle perform continuous casting for several charges continuously, and (2) a change in mold width during casting. (3) Operating conditions have changed, for example, the casting speed has changed from low to high. As a result, operating conditions that cannot be satisfied with the shape and the discharge angle of the immersion nozzle of the immersion nozzle suitable for the initial operating conditions are generated, and the level of the surface wave cannot be controlled to the optimum range. As a technology to control the wave height of the molten metal surface, (1) a method of applying a brake to the discharge flow by a DC magnetic field (* 1: hereinafter referred to as conventional method 1), and two pairs of DC magnets in a cooling box on the long side of the mold A DC magnetic field acts on the discharge flow from the immersion nozzle, and the induced current and the DC magnetic field generated in the flowing molten steel cause the flow of the molten steel by the electromagnetic force generated in the opposite direction to the flow of the molten steel. Is controlled.

(2)湯面位置に直流磁場を印加する方法(*2:以下従
来方法2という)で、湯面位置に直流磁場を配置し、湯
面に水平に直流磁場を印加することにより、磁場内の湯
面波動高さを制御するものである。
(2) In the method of applying a DC magnetic field to the molten metal surface position (* 2: hereinafter referred to as conventional method 2), the DC magnetic field is arranged at the molten metal surface position and the DC magnetic field is applied horizontally to the molten metal surface, so that the inside of the magnetic field is reduced. To control the wave height of the molten metal surface.

例(*1)永井ら:68,鉄と鋼(1982),S270 鈴木ら:68,鉄と鋼(1982),S92 (*2)小塚ら:72,鉄と鋼(1986),S718 [発明が解決しようとする課題] 鋳型内の湯面波動の発生は、浸漬ノズルから吐出され
た吐出流が凝固シェルに衝突し、上向きの反転流と下向
きの侵入流に分かれる。このうち、上向きの反転流の持
つ運動エネルギーが湯面を振動させるため湯面波動が発
生する。
Example (* 1) Nagai et al .: 68, Iron and Steel (1982), S270 Suzuki et al .: 68, Iron and Steel (1982), S92 (* 2) Kozuka et al .: 72, Iron and Steel (1986), S718 [Invention Problems to be Solved] When the surface wave in the mold is generated, the discharge flow discharged from the immersion nozzle collides with the solidification shell and is divided into an upward reverse flow and a downward inflow flow. Among them, the kinetic energy of the upward reversal flow causes the surface of the metal to vibrate, so that a surface wave of the surface of the metal occurs.

しかしながら従来方法1では、浸漬ノズルと短辺面と
の途中の吐出流に直角に直流磁場を印加して流体にブレ
ーキを掛ける方法であるが、浸漬ノズルから吐出された
後の吐出流は拡散して行くため、広い範囲に直流磁場を
印加する必要がある。このため設備が大型になりコスト
が高くなる。又この方法では、吐出流と印加した直流磁
場との相互作用によって発生する渦電流の回路が溶鋼内
にできるため、電流密度を大きくできない。従って大き
なブレーキ力を発生させるためには磁束密度を大きくす
る必要があり、このことによって設備コストが高くなる
という問題がある。
However, the conventional method 1 is a method in which a DC magnetic field is applied at right angles to the discharge flow on the way between the immersion nozzle and the short side surface to brake the fluid, but the discharge flow discharged from the immersion nozzle diffuses. Therefore, it is necessary to apply a DC magnetic field to a wide range. For this reason, the equipment becomes large and the cost increases. Further, in this method, an eddy current circuit generated by the interaction between the discharge flow and the applied DC magnetic field can be formed in the molten steel, so that the current density cannot be increased. Therefore, in order to generate a large braking force, it is necessary to increase the magnetic flux density, which causes a problem that the equipment cost increases.

従来方法2では、湯面波動に直接直流磁場を印加する
ため、波動の制御は最もやりやすいが、湯面波動の最も
激しい位置は鋳型短辺面から100mmの範囲である。従っ
て、この位置に直流磁場を印加すれば良く、そのため磁
場発生装置は鋳型長辺銅板の裏面で鋳型長辺銅板の上端
から約100mm付近に設置する必要がある。この場合に
は、冷却水箱の大掛かりな改造が必要であり、かつ鋳型
銅板の冷却溝の方向も横方向にする必要があり、鋳型長
辺銅板の冷却が不十分となる。
In the conventional method 2, since the direct current magnetic field is applied directly to the level wave, the control of the level wave is easiest, but the position where the level wave is most intense is within a range of 100 mm from the short side surface of the mold. Therefore, it is sufficient to apply a DC magnetic field to this position. Therefore, it is necessary to install the magnetic field generating device on the back surface of the copper plate on the long side of the mold and about 100 mm from the upper end of the copper plate on the long side of the mold. In this case, a large-scale modification of the cooling water box is necessary, and the direction of the cooling groove of the mold copper plate also needs to be horizontal, so that the cooling of the mold long side copper plate becomes insufficient.

この発明は、係る事情に鑑みてなされたものであっ
て、鋳型内の湯面波動を小さくしパウダーの巻き込みを
防止することと介在物の侵入深さを浅くすることによっ
て、介在物の浮上を図り、良好な表面性状を有する製品
を製造する鋼の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 in view of the above circumstances, and reduces the wave motion of the molten metal in the mold to prevent the entrainment of the powder and the shallow penetration depth of the inclusion, thereby reducing the floating of the inclusion. It is an object of the present invention to provide a continuous casting method of steel for producing a product having good surface properties.

[課題を解決するための手段] この発明による鋼の連続鋳造方法は、浸漬ノズルを挟
んで鋳型長辺銅板の背面に、少なくとも一対の直流磁石
を設置し、前記直流磁石の一方の磁極を鋳型長辺銅板の
上端の直上に、他方の磁極を浸漬ノズルの吐出孔より下
方の鋳型長辺銅板の背面に配置し、浸漬ノズルを挟んで
相対する磁極の特性を同一にして、直流磁界を発生さ
せ、浸漬ノズルからの溶鋼の吐出流に鉛直に直流磁界を
印加しながら鋳造することを特徴とする。
[Means for Solving the Problems] In the continuous casting method for steel according to the present invention, at least one pair of DC magnets is installed on the back of a copper plate on the long side of a mold with an immersion nozzle interposed therebetween, and one magnetic pole of the DC magnet is used as a mold. Directly above the upper end of the long side copper plate, the other magnetic pole is placed on the back side of the long side copper plate of the mold below the discharge hole of the immersion nozzle, and the characteristics of the magnetic poles facing each other across the immersion nozzle are made identical to generate a DC magnetic field The casting is performed while a DC magnetic field is applied vertically to the molten steel discharge flow from the immersion nozzle.

[作用] この発明は連続鋳造鋳型内の浸漬ノズル吐出孔からの
溶鋼吐出流に対し、鉛直方向に直流磁場を印加しながら
鋳造する。導電性流体である溶鋼が磁場中を流動すると
フレミングの右手の法則により流体内に起電力が発生
し、渦電流が流れる。この渦電流と印加磁場との相互作
用により、流体方向とは逆方向に電磁力(フレミングの
左手の法則)が働くため、流体の運動は妨げられる。こ
の結果吐出流は減速する。吐出流が減速すると、短辺面
シェルに衝突後の反転流の流速も小さくなり、湯面波動
は起こりにくくなる。又、片流れ現象が発生した場合、
吐出流速の大きい方には発生する電磁力がより大きくな
る。この結果、片流れ現象は抑制される。直流磁場を鉛
直方向に印加すると渦電流のパスは第5図に示すように
浸漬ノズルの周りに回路を描く。この時、渦電流の回路
の一部として電気抵抗の小さい鋳型銅板(銅の電気抵抗
率2.5×10-8Ω・m)を電流が流れるため、回路の電気
抵抗が小さくなり電流密度が大きくなる。この結果、発
生する電磁力は大きくなり効率的に電磁力を発生させる
ことができる。直流磁場を水平方向(スラブ厚み方向と
同じ)に印加した場合には、発生する渦電流は鋳型銅板
と平行な面で電気抵抗の大きい溶後(溶後の電気抵抗率
150×10-8Ω・m)内に回路を作るため、回路の電気抵
抗が大きくなり渦電流密度が小さくなる。そのため、直
流磁場を鉛直方向に印加できるように直流磁場の一方の
磁極を鋳型長片銅板の上端の直上と他方の磁極を浸漬ノ
ズル吐出孔より下方の鋳型長辺銅板の背面に配置した。
又、一方の磁極を鋳型長辺銅板の直上に置くことで、こ
の磁極と浸漬ノズル吐出孔の下方に設けた磁極とを結ぶ
磁束の多くは、鋳型長辺銅板中を通らずに溶鋼中を通る
ので、溶鋼中に効率良く電磁力を発生させることができ
る。
[Operation] The present invention performs casting while applying a DC magnetic field in the vertical direction to the molten steel discharge flow from the immersion nozzle discharge hole in the continuous casting mold. When molten steel, which is a conductive fluid, flows in a magnetic field, an electromotive force is generated in the fluid by Fleming's right-hand rule, and an eddy current flows. Due to the interaction between the eddy current and the applied magnetic field, an electromagnetic force (Fleming's left-hand rule) acts in a direction opposite to the fluid direction, so that the fluid is prevented from moving. As a result, the discharge flow is decelerated. When the discharge flow is decelerated, the flow velocity of the reversal flow after colliding with the short-side surface shell also decreases, and the surface wave wave is less likely to occur. Also, when the one-sided flow phenomenon occurs,
The higher the discharge flow rate, the greater the generated electromagnetic force. As a result, the one-sided flow phenomenon is suppressed. When a DC magnetic field is applied vertically, the path of the eddy current draws a circuit around the immersion nozzle as shown in FIG. At this time, as a part of the eddy current circuit, a current flows through a mold copper plate having a small electric resistance (copper electric resistivity of 2.5 × 10 −8 Ω · m), so that the electric resistance of the circuit decreases and the current density increases. . As a result, the generated electromagnetic force increases, and the electromagnetic force can be generated efficiently. When a DC magnetic field is applied in the horizontal direction (same as the slab thickness direction), the generated eddy current is generated after melting with high electric resistance on the surface parallel to the mold copper plate (electrical resistivity after melting).
Since a circuit is formed within 150 × 10 −8 Ω · m), the electrical resistance of the circuit increases and the eddy current density decreases. Therefore, one magnetic pole of the DC magnetic field was disposed immediately above the upper end of the long copper piece of the mold and the other magnetic pole was disposed on the back of the long side copper sheet of the mold below the discharge hole of the immersion nozzle so that the DC magnetic field could be applied in the vertical direction.
In addition, by placing one magnetic pole directly above the copper plate on the long side of the mold, most of the magnetic flux connecting this magnetic pole and the magnetic pole provided below the discharge port of the immersion nozzle passes through the molten steel without passing through the copper plate on the long side of the mold. As a result, the electromagnetic force can be efficiently generated in the molten steel.

[実施例] 先ず、溶鋼に電磁力を作用させた場合の溶鋼の流動に
ついての考え方を説明する。第5図は鋳型内の溶鋼に電
磁力を作用させた場合の溶鋼の流動を示す図で、(a)
は鋳型内の縦断面図で、(b)は(a)図のA−A平面
断面図である。21は鋳型長辺銅板、22は浸漬ノズル、23
は電磁石、24は直流磁石、25は直流磁石コイル、26は磁
界(印又は点線の矢印)、27は吐出流(黒矢印)、28
は渦電流(実線矢印)、29は制動力(白矢印)30は溶
鋼、31は直流磁場の一方の磁極、32は直流磁石の他方の
磁極、33は浸漬ノズルの吐出孔である。溶鋼30をタンデ
ィッシュから浸漬ノズル22を通して鋳型に注入する連続
鋳造方法において、浸漬ノズル22を挟んで、相対する少
なくとも一対以上の電磁石23(直流磁石24と直流磁石コ
イル25から構成されている)を設置し、前記直流磁石24
の一方の磁極31(N極あるいはS極)を鋳型長辺銅板21
の上端直上に、直流磁石の他方の磁極32(S極あるいは
N極)を浸漬ノズルの吐出孔33より下方の鋳型長辺面21
の背面に配置し、浸漬ノズル22を挟んで、相対する磁極
(31又は32)の極性を同一にして、浸漬ノズル22からの
吐出流27に対し、磁界26を鉛直に印加しながら、鋳造す
ることによって、吐出流27内に運動方向とは逆向きの制
動力29を発生させることによって吐出流27を減衰させる
ことができる。
[Example] First, the concept of the flow of molten steel when an electromagnetic force is applied to the molten steel will be described. FIG. 5 is a diagram showing the flow of molten steel when an electromagnetic force is applied to the molten steel in the mold.
FIG. 2 is a longitudinal sectional view in the mold, and FIG. 2B is a sectional view taken along the line AA in FIG. 21 is the long side copper plate of the mold, 22 is the immersion nozzle, 23
Is an electromagnet, 24 is a DC magnet, 25 is a DC magnet coil, 26 is a magnetic field (marked or dotted arrow), 27 is a discharge flow (black arrow), 28
Is the eddy current (solid arrow), 29 is the braking force (white arrow) 30, molten steel 30, 31 is one magnetic pole of the DC magnetic field, 32 is the other magnetic pole of the DC magnet, and 33 is the discharge hole of the immersion nozzle. In a continuous casting method in which molten steel 30 is poured from a tundish into a mold through an immersion nozzle 22, at least one pair or more of opposed electromagnets 23 (consisting of a DC magnet 24 and a DC magnet coil 25) are sandwiched by the immersion nozzle 22. Install the DC magnet 24
One of the magnetic poles 31 (N pole or S pole)
The other magnetic pole 32 (S-pole or N-pole) of the DC magnet is directly above the upper end of
The casting is performed while applying the magnetic field 26 vertically to the discharge flow 27 from the immersion nozzle 22 with the same polarity of the magnetic poles (31 or 32) facing each other with the immersion nozzle 22 interposed therebetween. Thus, the discharge flow 27 can be attenuated by generating a braking force 29 in the discharge flow 27 in a direction opposite to the direction of movement.

流動している溶鋼30に直流磁場を印加すると、下式に
より起電力が発生する。
When a DC magnetic field is applied to the flowing molten steel 30, an electromotive force is generated by the following equation.

E=×=VY・BZ ……(1) : 溶鋼の速度(m/sec) : 磁束密度 VY : 溶鋼の速度の鋳型幅方向の成分(m/sec) BZ : 磁束密度の鉛直方向成分 この起電力により溶鋼内に渦電流が流れ渦電流
と磁束密度との相互作用により溶鋼の運動方向と逆方
向に制動力が働く。
E = × = V Y · B Z …… (1): Speed of molten steel (m / sec): Magnetic flux density V Y : Component of velocity of molten steel in mold width direction (m / sec) B Z : Vertical of magnetic flux density Directional component Due to this electromotive force, eddy current flows in the molten steel and a braking force acts in a direction opposite to the direction of movement of the molten steel due to the interaction between the eddy current and the magnetic flux density.

=−×=−σVY・BZ 2 ……(2) σ: 流体の電気抵抗率(Ω・m) (2)式により、制動力の大きさはVYとBZ 2に依存す
る。
= - × = -σV Y · B Z 2 ...... (2) σ: the electrical resistivity of the fluid (Ω · m) (2) equation, the magnitude of the braking force is dependent on V Y and B Z 2.

溶鋼の連続鋳造においては、低速鋳造の場合はVYが小
さいため、溶鋼に働く制動力は小さいが、高速鋳造に
なる程、VYが大きくなるので制動力は大きくなる。
In continuous casting of molten steel, for the case of low-speed casting V Y is small, although the braking force acting on the molten steel is small, enough to be faster casting, the braking force since V Y increases increases.

浸漬ノズル22から吐出された吐出流27は直流磁場が無
い場合には、片方の吐出孔33から優先的に流出する片流
れ現象が起こりやすく、直流磁場を鉛直方向に印加する
ことによって、吐出流速の速い方には、(2)式に従っ
てより大きな制動力が働くため、吐出流は均一化され、
片流れ現象は緩和される。こうすることによって最大湯
面波動高さが、一定の範囲に制御することができる。
When there is no DC magnetic field, the discharge flow 27 discharged from the immersion nozzle 22 tends to cause a one-flow phenomenon that preferentially flows out of one of the discharge holes 33.By applying a DC magnetic field in the vertical direction, the discharge flow rate is reduced. In the faster one, a larger braking force acts according to the equation (2), so that the discharge flow is made uniform,
The one-sided flow phenomenon is mitigated. By doing so, the maximum level wave height can be controlled within a certain range.

以下、添付図面を参照してこの発明の一実施例につい
て具体的に説明する。
Hereinafter, an embodiment of the present invention will be specifically described with reference to the accompanying drawings.

第1図はこの本発明の一実施例の連続鋳造鋳型の断面
図で、(a)は側断面図で、(b)は第1図の(a)の
線A−A断面図で、(c)は第1図の(a)におけるB
−B側面の斜視図である。21は鋳型長辺銅板、22は浸漬
ノズル、23は電磁石、24は直流磁石、25は直流磁石コイ
ル、30は溶鋼、31は直流磁石の一方の磁極、32は直流磁
石の他方の磁極、33は浸漬ノズルの吐出孔である。
FIG. 1 is a sectional view of a continuous casting mold according to one embodiment of the present invention, in which (a) is a side sectional view, (b) is a sectional view taken along line AA of (a) of FIG. c) is B in FIG. 1 (a).
It is a perspective view of -B side. 21 is a copper plate on the long side of the mold, 22 is an immersion nozzle, 23 is an electromagnet, 24 is a DC magnet, 25 is a DC magnet coil, 30 is molten steel, 31 is one magnetic pole of the DC magnet, 32 is the other magnetic pole of the DC magnet, 33 Is a discharge hole of the immersion nozzle.

図示しないタンディッシュの下部に取り付けられた浸
漬ノズル22を挟んで前、後面の鋳型長辺銅板21の背後に
相対する一対の電磁石23(直流磁石24と直流磁石コイル
25から構成されている)が配置されている。直流磁石の
一方の磁極31は鋳型長辺銅板21の上端の直上に、直流磁
石の他方の磁極32は浸漬ノズルの吐出孔33の下250mm位
置に配置した。直流磁石24の断面寸法は100(H)×600
(W)mmである。直流磁石24の磁極(31又は32)の極性
は、浸漬ノズル22を挟んで、同極対向になるように選ん
だ。こうすることにより磁界方向を鉛直方向、すなわち
浸漬ノズル22と平行にすることができる。
A pair of electromagnets 23 (a DC magnet 24 and a DC magnet coil) facing each other behind a long side copper plate 21 on the front and rear sides of a dipping nozzle 22 attached to the lower part of a tundish (not shown)
Consists of 25). One magnetic pole 31 of the DC magnet was disposed immediately above the upper end of the copper plate 21 on the long side of the mold, and the other magnetic pole 32 of the DC magnet was disposed 250 mm below the discharge hole 33 of the immersion nozzle. The cross-sectional dimension of DC magnet 24 is 100 (H) x 600
(W) mm. The polarity of the magnetic pole (31 or 32) of the DC magnet 24 was selected so as to be of the same polarity across the immersion nozzle 22. By doing so, the direction of the magnetic field can be made vertical, that is, parallel to the immersion nozzle 22.

(実施例1) 第1図で示した相対する一対の電磁石23を設置した連
続鋳造鋳型を用いて、鋳造した鋳型短辺銅板34近傍の湯
面波動高さの測定結果を以下に示す。220mm厚み、1200m
m幅の断面寸法のスラブを引抜速度0.7〜2.7m/minの範囲
で変更した鋳造を実施した。この時の鋳造速度は、1.4
〜5.0ton/minの間で変化した。第2図は直流磁場を印加
した場合としない場合の鋳型短辺銅板近傍の最大湯面波
動高さと引抜速度又は鋳造速度との関係を示すグラフ図
である。この図の横軸に引抜速度と鋳造速度との関係を
示す。○は磁場無しで、●は磁場有りである。直流磁場
の磁束密度は2000〜2500ガウスの範囲で調整した。磁場
を印加した場合の最大湯面波動高さは、磁場を印加しな
い場合の最大湯面波動高さに比べかなり小さくなってい
る。2.5ton/min以下の鋳造速度では、最大湯面波動高さ
は抑制されたが、一方、2.5ton/min以上の鋳造速度でも
最大湯面波動高さは、8mm以下に抑制することができ
る。
(Example 1) Using a continuous casting mold in which a pair of opposed electromagnets 23 shown in FIG. 1 are installed, a measurement result of the level wave height in the vicinity of the short side copper plate 34 of the casting mold is shown below. 220mm thickness, 1200m
Casting was performed with a slab having a cross-sectional dimension of m width changed at a drawing speed of 0.7 to 2.7 m / min. The casting speed at this time is 1.4
It varied between ~ 5.0ton / min. FIG. 2 is a graph showing the relationship between the maximum wave height in the vicinity of the copper plate on the short side of the mold and the drawing speed or the casting speed when a DC magnetic field is not applied. The horizontal axis in this figure shows the relationship between the drawing speed and the casting speed. ○ indicates no magnetic field, and ● indicates a magnetic field. The magnetic flux density of the DC magnetic field was adjusted in the range of 2000 to 2500 Gauss. The maximum level wave height when a magnetic field is applied is considerably smaller than the maximum level wave height when a magnetic field is not applied. At a casting speed of 2.5 ton / min or less, the maximum level wave height was suppressed. On the other hand, at a casting speed of 2.5 ton / min or more, the maximum level wave height could be suppressed to 8 mm or less.

(実施例2) 第1図で示した相対する一対の電磁石23を設置した連
続鋳造鋳型を用いて、浸漬ノズルの吐出流に直流磁場を
印加しながら鋳造を実施した。直流磁場の印加条件は実
施例1に示した結果より判断した。即ち、3.0ton/min以
上の鋳造速度の鋳造条件で直流磁場の磁束密度は一律20
00ガウスに設定した。220mm厚み、1200mm幅の断面寸法
のスラブを鋳造した。第3図は鋳造時間と引抜速度、及
び、鋳造時間と直流磁場の有無における最大湯面波動高
さとの経時変化を示すグラフ図である。鋳造開始直後に
ついては最大湯面波動高さを測定するための渦流距離計
のセッテングと調節が必要なため測定はできなかった
が、測定できる状態になってから直流磁場を印加する
と、最大湯面波動高さの値は、ほぼ全鋳造領域にわたっ
て適正な範囲に制御ができる。
(Example 2) Using a continuous casting mold provided with a pair of opposing electromagnets 23 shown in Fig. 1, casting was performed while applying a DC magnetic field to the discharge flow of the immersion nozzle. The conditions for applying the DC magnetic field were determined from the results shown in Example 1. That is, the magnetic flux density of the DC magnetic field is uniformly 20 at the casting condition of the casting speed of 3.0 ton / min or more.
Set to 00 Gauss. A slab with a cross-sectional dimension of 220 mm thickness and 1200 mm width was cast. FIG. 3 is a graph showing a change with time of the casting time and the drawing speed, and the casting time and the maximum surface wave height in the presence or absence of a DC magnetic field. Immediately after the start of casting, measurement was not possible because the setting and adjustment of the eddy current distance meter for measuring the maximum height of the surface wave were not possible. The value of the wave height can be controlled in an appropriate range over almost the entire casting area.

なお、鍋交換の時には、吐出流速が遅いため湯面波動
は静かであり、直流磁場を印加して吐出流に制動力を作
用させる必要がない。
In addition, when the pot is replaced, the discharge flow speed is low, so that the surface wave is quiet, and there is no need to apply a DC magnetic field to apply a braking force to the discharge flow.

第4図は直流磁場の有無による熱延板表面欠陥指数と
鋳造速度との関係を示すグラフ図である。○は磁場無し
で、●は磁場有りである。なお、直流磁場を掛けたの
は、鋳造速度を3.0ton/min以上の時である。表面欠陥指
数とはヘゲ個数を観察面積で割った値を指数化したもの
である。この図から明らかなように直流磁場を印加する
ことにより、高速鋳造において熱延板表面欠陥指数が著
しく減少している。
FIG. 4 is a graph showing the relationship between the hot-rolled sheet surface defect index and the casting speed depending on the presence or absence of a DC magnetic field. ○ indicates no magnetic field, and ● indicates a magnetic field. The DC magnetic field was applied when the casting speed was 3.0 ton / min or more. The surface defect index is an index obtained by dividing the number of scabs by the observation area. As is apparent from this figure, by applying a DC magnetic field, the hot-rolled sheet surface defect index is significantly reduced in high-speed casting.

[発明の効果] 以上説明したように、本発明による鋼の連続鋳造方法
は、浸漬ノズルを挟んで、少なくとも1対の直流磁石を
設置し、一方の磁極を鋳型長辺銅板の上端の上側に、他
方の磁極を浸漬ノズルの吐出孔より下方の鋳型長辺銅板
の背面に配置し、鋳型挟んで相対する磁極の極静を同一
にして、直流磁界を発生させ、浸漬ノズルからの溶鋼の
吐出流に鉛直に直流磁界を印加しながら鋳造するため、
吐出流速の速い方には大きな制動力が働くため、吐出流
は均一化されるので、湯面波動高さが一定の範囲に制御
できるので、良好な表面性状を有する熱延板を得ること
ができる。
[Effects of the Invention] As described above, in the continuous casting method of steel according to the present invention, at least one pair of DC magnets is installed with the immersion nozzle interposed therebetween, and one magnetic pole is placed above the upper end of the copper plate on the long side of the mold. The other magnetic pole is placed on the back side of the copper plate on the long side of the mold below the discharge hole of the immersion nozzle, and the poles of the magnetic poles facing each other are sandwiched between the molds to generate the DC magnetic field, thereby discharging the molten steel from the immersion nozzle. Casting while applying a DC magnetic field vertically to the flow,
Since a large braking force acts on the one with a higher discharge flow velocity, the discharge flow is made uniform, so that the surface wave height can be controlled within a certain range, so that a hot rolled sheet having good surface properties can be obtained. it can.

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

第1図はこの本発明の一実施例の連続鋳造鋳型の断面
図、第2図は直流磁場を印加した場合としない場合の鋳
型短辺銅板近傍の最大湯面波動高さと引抜速度又は鋳造
速度との関係を示すグラフ図、第3図は鋳造時間と引抜
速度、及び、鋳造時間と直流磁場濃有無における最大湯
面波動高さとの経時変化を示すグラフ図、第4図は直流
磁場の有無による熱延板表面欠陥指数と鋳造速度との関
係を示すグラフ図、第5図は鋳型内の溶鋼に電磁力を作
用させた場合の溶鋼の流動を示す図、第6図はスラブの
連続鋳造機の鋳型内の溶鋼状態を示す図、第7図は湯面
波動の概略図、第8図は約1分間の湯面レベルの経時変
化を示す図、第9図は最大湯面波動高さと熱延板表面欠
陥指数の関係を示すグラフ図である。 21……鋳型長辺銅板、22……浸漬ノズル、23……電磁
石、24……直流磁石、25……直流磁石コイル、30……溶
鋼、31……直流磁石の一方の磁極、32……直流磁石の他
方の磁極、33……浸漬ノズルの吐出孔。
FIG. 1 is a cross-sectional view of a continuous casting mold according to one embodiment of the present invention, and FIG. 2 is a diagram showing the maximum wave height and drawing speed or casting speed near the copper plate on the short side of the mold with and without applying a DC magnetic field. FIG. 3 is a graph showing the relationship between the casting time and the drawing speed, and FIG. 3 is a graph showing the change over time between the casting time and the maximum surface wave height in the presence or absence of the DC magnetic field, and FIG. 4 is the presence or absence of the DC magnetic field. FIG. 5 is a graph showing the relationship between the surface defect index of a hot-rolled sheet and the casting speed, FIG. 5 is a view showing the flow of molten steel when an electromagnetic force is applied to molten steel in a mold, and FIG. 6 is continuous casting of a slab. Figure 7 shows the molten steel state in the mold of the machine, FIG. 7 is a schematic view of the level wave, FIG. 8 is a view showing the change of the level of the level for about 1 minute, and FIG. 9 is the maximum level wave height. It is a graph which shows the relationship of a hot-rolled sheet surface defect index. 21 ... Mold long side copper plate, 22 ... Immersion nozzle, 23 ... Electromagnet, 24 ... DC magnet, 25 ... DC magnet coil, 30 ... Metal steel, 31 ... One magnetic pole of DC magnet, 32 ... The other magnetic pole of the DC magnet, 33 ... the discharge hole of the immersion nozzle.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 金尾 義行 東京都千代田区丸の内1丁目1番2号 日本鋼管株式会社内 (72)発明者 青 範夫 東京都千代田区丸の内1丁目1番2号 日本鋼管株式会社内 (72)発明者 山本 裕則 東京都千代田区丸の内1丁目1番2号 日本鋼管株式会社内 審査官 天野 斉 ──────────────────────────────────────────────────続 き Continuing on the front page (72) Yoshiyuki Kanao, Inventor 1-1-2 Marunouchi, Chiyoda-ku, Tokyo Nippon Kokan Co., Ltd. (72) Inventor Norio Blue 1-2-1, Marunouchi, Chiyoda-ku, Tokyo Japan (72) Inventor Hironori Yamamoto 1-1-2 Marunouchi, Chiyoda-ku, Tokyo Nippon Kokan Co., Ltd.Examiner Hitoshi Amano

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】タンディッシュから浸漬ノズルを通して溶
鋼を鋳型内に鋳造する鋼の連続鋳造方法において、浸漬
ノズルを挟んで鋳型長辺銅板の背面に、少なくとも一対
の直流磁石を設置し、前記直流磁石の一方の磁極を鋳型
長辺銅板の上端の直上に、他方の磁極を浸漬ノズルの吐
出孔より下方の鋳型長辺銅板の背面に配置し、浸漬ノズ
ルを挟んで相対する磁極の特性を同一にして直流磁界を
発生させ、浸漬ノズルからの溶鋼の吐出流に鉛直に直流
磁界を印加しながら鋳造することを特徴とする鋼の連続
鋳造方法。
1. A continuous casting method of steel in which molten steel is cast into a mold from a tundish through an immersion nozzle. One magnetic pole is placed just above the upper end of the copper plate on the long side of the mold, and the other magnetic pole is placed on the back side of the copper plate on the long side of the mold below the discharge hole of the immersion nozzle, and the characteristics of the magnetic poles facing each other across the immersion nozzle are made the same. A continuous casting method for steel, comprising: generating a direct-current magnetic field by applying a direct-current magnetic field to a discharge flow of molten steel from an immersion nozzle.
JP22491988A 1988-09-08 1988-09-08 Steel continuous casting method Expired - Fee Related JP2733991B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22491988A JP2733991B2 (en) 1988-09-08 1988-09-08 Steel continuous casting method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22491988A JP2733991B2 (en) 1988-09-08 1988-09-08 Steel continuous casting method

Publications (2)

Publication Number Publication Date
JPH0275456A JPH0275456A (en) 1990-03-15
JP2733991B2 true JP2733991B2 (en) 1998-03-30

Family

ID=16821223

Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP2733991B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2773154B2 (en) * 1988-09-30 1998-07-09 日本鋼管株式会社 Steel continuous casting method
CN117333558B (en) 2023-09-28 2024-04-05 北方工业大学 Method and system for analyzing global average grayscale changes in tundish ink tracing experiments
CN117250158B (en) * 2023-09-28 2024-04-12 北京科技大学 Tundish evaluation method and system based on ink staining test area change

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