JPH088050A - Induction heating method for rolled material - Google Patents
Induction heating method for rolled materialInfo
- Publication number
- JPH088050A JPH088050A JP16275794A JP16275794A JPH088050A JP H088050 A JPH088050 A JP H088050A JP 16275794 A JP16275794 A JP 16275794A JP 16275794 A JP16275794 A JP 16275794A JP H088050 A JPH088050 A JP H088050A
- Authority
- JP
- Japan
- Prior art keywords
- rolled material
- amount
- heating
- induction heating
- lapping
- 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
- General Induction Heating (AREA)
Abstract
(57)【要約】
【目的】 圧延材を効率よく加熱し、エッジヒーター本
体の漏れ磁束による過熱を防止して必要温度昇温カーブ
が得られ、加熱効率の優れた圧延材の誘導加熱方法を提
供するものである。
【構成】 圧延ラインを連続的に走行させて圧延材5の
両端側をエッジヒーター1で加熱する圧延材の誘導加熱
方法において、エッジヒーター1の端部から両側に突出
した圧延材5の幅をラップ量Lとして、ラップ量Lが0
以上の範囲で圧延材5の必要昇温温度を得る場合にはラ
ップ量Lを調整するラップ制御を行なって加熱し、ラッ
プ量Lが0未満で必要昇温温度を得る場合には、ラップ
量Lを0として周波数fを可変コンデンサ11で調整する
周波数制御で加熱することを特徴とするものである。
(57) [Abstract] [Purpose] A method for induction heating of rolled material with excellent heating efficiency that efficiently heats rolled material and prevents overheating due to leakage flux of the edge heater body to obtain the required temperature rise curve. It is provided. In the induction heating method for a rolled material, in which both ends of the rolled material 5 are heated by the edge heaters 1 by continuously running the rolling line, the width of the rolled material 5 protruding from the end portion of the edge heater 1 to both sides is set. As the lap amount L, the lap amount L is 0
When the required temperature rising temperature of the rolled material 5 is obtained in the above range, the lapping amount L is adjusted to perform heating, and when the necessary temperature rising temperature is obtained when the lapping amount L is less than 0, the lapping amount is adjusted. It is characterized in that heating is performed by frequency control in which L is 0 and the frequency f is adjusted by the variable capacitor 11.
Description
【0001】[0001]
【産業上の利用分野】本発明は連続的に搬送される圧延
材の端部をエッジヒーターで加熱する圧延材の誘導加熱
方法に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an induction heating method for a rolled material which is continuously conveyed by heating an end portion of the rolled material with an edge heater.
【0002】[0002]
【従来の技術】一般に、鉄鋼圧延ラインなど圧延材を連
続的に走行させて複数の圧延ローラに通して順次圧延し
て所定の厚さの圧延材を製造している。しかしながら圧
延材は薄いので、両端側は中央部分に比べて放熱量が多
くなり図3に示すように温度降下が大きい。このため圧
延機に入る直前で、板幅方向の温度分布を均一にしてか
ら圧延しないと割れが発生したり、所定の板厚に圧延で
きなくなる問題がある。このため圧延機に入る直前で、
温度降下部分を補償するように図3に一点鎖線で示すよ
うに昇温させて板幅方向の温度分布を均一にしてから圧
延している。2. Description of the Related Art Generally, a rolled material such as an iron and steel rolling line is continuously run, passed through a plurality of rolling rollers, and sequentially rolled to produce a rolled material having a predetermined thickness. However, since the rolled material is thin, the amount of heat radiation on both ends is larger than that on the central part, and the temperature drop is large as shown in FIG. Therefore, immediately before entering the rolling mill, if the temperature distribution in the width direction of the plate is made uniform and then rolling occurs, there is a problem that cracks occur or it becomes impossible to roll to a predetermined plate thickness. Therefore, just before entering the rolling mill,
In order to compensate for the temperature drop portion, the temperature is raised as indicated by the alternate long and short dash line in FIG. 3 to make the temperature distribution in the strip width direction uniform before rolling.
【0003】このように温度降下した圧延材の端部側を
局部的に加熱する誘導加熱装置のエッジヒーターは、従
来例えば図4に示すように構成されている。この誘導加
熱装置のエッジヒーター1は、複数の溝部2を形成した
積層鉄心3の前記溝部2…に、水冷銅管を巻回して加熱
コイル4を形成したもので、このエッジヒーター1は、
圧延材5の両端側を上下から挟むように夫々設置され、
走行する圧延材5を誘導加熱して温度降下の大きい両端
部を局部的に加熱するようになっている。The edge heater of the induction heating device for locally heating the end portion side of the rolled material whose temperature has dropped in this way is conventionally constructed as shown in FIG. 4, for example. An edge heater 1 of this induction heating device is one in which a water-cooled copper pipe is wound around the groove portions 2 of a laminated iron core 3 having a plurality of groove portions 2 to form a heating coil 4, and the edge heater 1 is
Installed so that both ends of the rolled material 5 are sandwiched from above and below,
The rolling material 5 which is running is induction-heated to locally heat both ends having a large temperature drop.
【0004】この場合、圧延材5の温度降下は板厚によ
り変化すると考えられ、板厚に応じたエッジヒーター1
の昇温比率を変えるため、従来はエッジヒーター1と圧
延材5の相対位置、すなわちエッジヒーター1の端部か
ら両側に突出した圧延材5の幅をラップ量Lとして、こ
のラップ量Lを変えて、目的の昇温カーブを得ていた。
通常エッジヒーターの昇温カーブ特性は図5に示すよう
になり、この関係は次式で表される。但し式中、△Tは
昇温値、Aは定数、EXPは指数関数、Kはラップ量L
により定まる変数、xは圧延材5の端面からの距離であ
る。In this case, it is considered that the temperature drop of the rolled material 5 changes depending on the plate thickness, and the edge heater 1 according to the plate thickness.
In order to change the temperature rising ratio of the rolled material 5, the relative position between the edge heater 1 and the rolled material 5, that is, the width of the rolled material 5 protruding from the end of the edge heater 1 to both sides is set as the lapping amount L, and the lapping amount L is changed. Then, the desired temperature rising curve was obtained.
The temperature rising curve characteristic of the normal edge heater is as shown in FIG. 5, and this relationship is expressed by the following equation. Where ΔT is the temperature rise value, A is a constant, EXP is an exponential function, and K is the lap amount L.
X is a distance from the end surface of the rolled material 5.
【0005】[0005]
【数1】△T=A・EXP(−Kx)[Equation 1] ΔT = A · EXP (-Kx)
【0006】このように従来は図6及び図7に示すよう
にラップ量Lを変化させることによりKの値を変えて、
温度降下した圧延材5の端部側を目的の昇温カーブで加
熱していた。この場合、端部の昇温比率を急激に増加さ
せるには、圧延材5のラップ量Lを少なくしてKの値を
大きくする必要がある。しかし図7に示すようにラップ
量LをマイナスにするとKの値は大きくなるが、漏れ磁
束6が増えて圧延材5と鎖交する有効な磁束が減少する
と共に、水冷銅管を巻回した加熱コイル4の温度が上昇
して過熱され、全体としてエッジヒーター1の加熱効率
が図8に示すように低下してくる問題がある。As described above, conventionally, the value of K is changed by changing the lap amount L as shown in FIG. 6 and FIG.
The end portion side of the rolled material 5 having the temperature lowered was heated by the intended temperature rising curve. In this case, in order to rapidly increase the temperature rising ratio of the end portion, it is necessary to decrease the lapping amount L of the rolled material 5 and increase the value of K. However, as shown in FIG. 7, when the lap amount L is set to a negative value, the value of K increases, but the leakage magnetic flux 6 increases and the effective magnetic flux interlinking with the rolled material 5 decreases, and the water-cooled copper pipe is wound. There is a problem that the temperature of the heating coil 4 rises and is overheated, and the heating efficiency of the edge heater 1 as a whole decreases as shown in FIG.
【0007】[0007]
【発明が解決しようとする課題】本発明は上記欠点を除
去し、圧延材を効率よく加熱し、エッジヒーター本体の
漏れ磁束による過熱を防止して必要温度昇温カーブが得
られ、加熱効率の優れた圧延材の誘導加熱方法を提供す
るものである。DISCLOSURE OF THE INVENTION The present invention eliminates the above-mentioned drawbacks, efficiently heats a rolled material, prevents overheating due to leakage flux of the edge heater main body, and obtains a required temperature rising curve, thereby improving heating efficiency. An excellent method for induction heating of rolled material is provided.
【0008】[0008]
【課題を解決するための手段】本発明は、圧延ラインを
連続的に走行させて圧延材の両端側をエッジヒーターで
加熱する圧延材の誘導加熱方法において、エッジヒータ
ーの端部から両側に突出した圧延材の幅をラップ量とし
て、ラップ量が0以上の範囲で圧延材の必要昇温温度を
得る場合にはラップ量を調整するラップ制御を行なって
加熱し、ラップ量が0未満で必要昇温温度を得る場合に
は、ラップ量を0として周波数を調整する周波数制御で
加熱することを特徴とするものである。DISCLOSURE OF THE INVENTION The present invention is an induction heating method for a rolled material, in which both ends of the rolled material are heated by edge heaters by continuously running a rolling line. The width of the rolled material is used as the lap amount, and when the required temperature rise temperature of the rolled material is obtained in the range where the lap amount is 0 or more, lap control is performed to adjust the lap amount and heating is performed. In order to obtain the temperature rise temperature, heating is performed by frequency control in which the lap amount is set to 0 and the frequency is adjusted.
【0009】[0009]
【作用】本発明の圧延材の誘導加熱方法は、数1に△T
=A・EXP(−Kx)で表される関係式で必要昇温温
度が得られるラップ量Lが0以上の範囲ではラップ制御
を行なうと効率よく加熱することができる。また数1に
△T=A・EXP(−Kx)で表される関係式で必要昇
温温度が得られるラップ量Lが0未満となる場合には、
エッジヒーターの端部と圧延材の端部を揃えてラップ量
Lを0とし、可変コンデンサのコンデンサ容量を調整し
て、周波数fを変化させる周波数制御を行なうことによ
り、加熱効率を低下させずに必要昇温温度カーブで加熱
することができる。The method of induction heating of rolled material according to the present invention is based on the equation
= A · EXP (−Kx), the lapping amount L that provides the required temperature rise can be efficiently heated by performing the lapping control. In addition, in the relational expression represented by ΔT = A · EXP (−Kx) in Equation 1, when the lapping amount L at which the required temperature rise is obtained is less than 0,
By aligning the end portion of the edge heater and the end portion of the rolled material to set the wrap amount L to 0, adjusting the condenser capacity of the variable condenser, and performing frequency control to change the frequency f, the heating efficiency is not reduced. It can be heated with the required temperature rise temperature curve.
【0010】[0010]
【実施例】以下本発明の一実施例を詳細に説明する。図
1は本発明の圧延材の誘導加熱装置の回路を示すもの
で、高周波電源7から整合変圧器8を介して力率改善用
コンデンサ9が接続され、更にエッジヒーター1の加熱
コイル4との間に、開閉器10を介して可変コンデンサ11
が接続されている。また周波数と昇温特性との関係は実
験の結果、次式の関係を有することが見い出された。但
し式中、A、B、C、Dは定数、EXPは指数関数、f
は周波数、Lはラップ量、xは圧延材の端面からの距離
である。DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described below in detail. FIG. 1 shows a circuit of an induction heating apparatus for rolled material according to the present invention, in which a power factor improving capacitor 9 is connected from a high frequency power source 7 through a matching transformer 8 and further to a heating coil 4 of an edge heater 1. In the meantime, via the switch 10 the variable capacitor 11
Is connected. As a result of an experiment, it was found that the relationship between the frequency and the temperature rising characteristic has the following relationship. However, in the formula, A, B, C, and D are constants, EXP is an exponential function, and f
Is the frequency, L is the lapping amount, and x is the distance from the end face of the rolled material.
【0011】[0011]
【数2】 [Equation 2]
【0012】従って、圧延ラインを連続的に走行させて
圧延材5の両端側をエッジヒーター1、1で加熱する場
合、前記数1に△T=A・EXP(−Kx)で表される
関係式で必要昇温温度が得られるラップ量Lが、図6に
示すように0以上の範囲ではラップ制御を行なう。これ
は図8に示すようにラップ量Lが0以上の場合には、効
率よく加熱することができるからである。Therefore, in the case where both ends of the rolled material 5 are heated by the edge heaters 1 and 1 while the rolling line is continuously run, the relation expressed by ΔT = A · EXP (−Kx) in the above mathematical expression 1 As shown in FIG. 6, the lap control is performed when the lap amount L at which the required temperature rise is obtained by the equation is 0 or more. This is because heating can be performed efficiently when the lap amount L is 0 or more as shown in FIG.
【0013】また数1に△T=A・EXP(−Kx)で
表される関係式で必要昇温温度が得られるラップ量Lが
図7に示すように0未満となるマイナスの場合には、図
2に示すようにエッジヒーター1の端部と圧延材5の端
部を揃えてラップ量Lを0とした状態に設定し、数2で
示す関係式に基づいて、可変コンデンサ11のコンデンサ
容量を調整して、開閉器10を入れることにより周波数f
を調整する周波数制御で加熱を行なう。この場合ラップ
量Lが0となるので、周波数と昇温特性との関係は、次
式の関係となる。Further, in the case where the lap amount L for obtaining the required temperature rise is less than 0 as shown in FIG. 7 in the relational expression represented by ΔT = A · EXP (−Kx) in the equation 1, it is negative. As shown in FIG. 2, the end portion of the edge heater 1 and the end portion of the rolled material 5 are aligned to set the lap amount L to 0, and the condenser of the variable condenser 11 is set based on the relational expression shown in Formula 2. Frequency f by adjusting the capacity and inserting switch 10.
Heating is performed by controlling the frequency. In this case, since the lap amount L is 0, the relationship between the frequency and the temperature rising characteristic is the following expression.
【0014】[0014]
【数3】 (Equation 3)
【0015】従って、数1の関係式でラップ量Lが0未
満となる範囲ではラップ量Lを0として、漏れ磁束6を
少なくして圧延材5と鎖交する有効な磁束を多くすると
共に、加熱コイル4の過熱を防止して、全体として図8
に示すように効率良く加熱することができる。また圧延
材5の端部側の必要温度昇温カーブは周波数fを調整す
ることにより容易に得ることができる。Therefore, in the range where the lapping amount L is less than 0 in the relational expression of Equation 1, the lapping amount L is set to 0 to reduce the leakage magnetic flux 6 to increase the effective magnetic flux interlinking with the rolled material 5, and As a whole, the heating coil 4 is prevented from being overheated, and the heating coil 4 shown in FIG.
As shown in, the heating can be performed efficiently. Further, the required temperature rising curve on the end side of the rolled material 5 can be easily obtained by adjusting the frequency f.
【0016】[0016]
【発明の効果】以上説明した如く本発明に係る圧延材の
誘導加熱方法によれば、加熱効率の良いラップ量Lが0
以上の範囲ではラップ量Lを調整するラップ制御を行な
い、ラップ量が0未満となる場合には、ラップ量を0と
して周波数を調整する周波数制御の2段階に切替えて加
熱することにより、圧延材を効率よく必要温度昇温カー
ブで加熱できると共に、漏洩磁束による加熱コイルの過
熱を防止してコイル寿命を長くすることができる。As described above, according to the induction heating method for rolled material according to the present invention, the lapping amount L with good heating efficiency is 0.
In the above range, lap control for adjusting the lap amount L is performed, and when the lap amount is less than 0, the rolled material is heated by switching to two stages of frequency control in which the lap amount is 0 and the frequency is adjusted. It is possible to efficiently heat the heating coil with the required temperature rising curve, and prevent the heating coil from overheating due to the leakage magnetic flux, thereby extending the life of the coil.
【図1】本発明の一実施例による圧延材の誘導加熱回路
を示す単線回路図である。FIG. 1 is a single-line circuit diagram showing an induction heating circuit for rolled material according to an embodiment of the present invention.
【図2】圧延材の端部をエッジヒーターの端部に合わせ
て誘導加熱している状態を示す断面図である。FIG. 2 is a cross-sectional view showing a state in which the end of the rolled material is aligned with the end of an edge heater and induction heating is performed.
【図3】圧延材の端部側の板幅方向の温度分布を示すグ
ラフである。FIG. 3 is a graph showing a temperature distribution in the plate width direction on the end side of the rolled material.
【図4】エッジヒーターの間に圧延材の端部を通過させ
て端部を誘導加熱している状態を示す斜視図である。FIG. 4 is a perspective view showing a state in which an end portion of the rolled material is passed between the edge heaters and the end portion is induction-heated.
【図5】圧延材端面からの距離による昇温値の変化を示
すグラフである。FIG. 5 is a graph showing a change in a temperature rise value depending on a distance from an end surface of a rolled material.
【図6】圧延材の端部をエッジヒーターの端部から突出
させてラップ量Lが0を越えた範囲で誘導加熱している
状態を示す断面図である。FIG. 6 is a cross-sectional view showing a state in which an end portion of a rolled material is projected from an end portion of an edge heater and induction heating is performed in a range where a lapping amount L exceeds 0.
【図7】圧延材の端部をエッジヒーターの端部より内側
に走行させてラップ量Lが0未満の範囲で誘導加熱して
いる状態を示す断面図である。FIG. 7 is a cross-sectional view showing a state in which an end portion of a rolled material is made to travel inward from an end portion of an edge heater and induction heating is performed in a range where a lapping amount L is less than 0.
【図8】ラップ量Lと加熱効率の関係を示すグラフであ
る。FIG. 8 is a graph showing a relationship between a lapping amount L and heating efficiency.
1 エッジヒーター 2 溝部 3 積層鉄心 4 加熱コイル 5 圧延材 6 磁束 7 高周波電源 8 整合変圧器 9 力率改善用コンデンサ 10 開閉器 11 可変コンデンサ 1 Edge Heater 2 Groove 3 Laminated Iron Core 4 Heating Coil 5 Rolled Material 6 Magnetic Flux 7 High Frequency Power Supply 8 Matching Transformer 9 Power Factor Improvement Capacitor 10 Switch 11 Variable Capacitor
Claims (1)
の両端側をエッジヒーターで加熱する圧延材の誘導加熱
方法において、エッジヒーターの端部から両側に突出し
た圧延材の幅をラップ量として、ラップ量が0以上の範
囲で圧延材の必要昇温温度を得る場合にはラップ量を調
整するラップ制御を行なって加熱し、ラップ量が0未満
で必要昇温温度を得る場合には、ラップ量を0として周
波数を調整する周波数制御で加熱することを特徴とする
圧延材の誘導加熱方法。1. In an induction heating method for a rolled material, in which both ends of the rolled material are heated by edge heaters by continuously running on a rolling line, the width of the rolled material protruding from the end of the edge heater to both sides is wrapped. When the required temperature rising temperature of the rolled material is obtained in the range where the lapping amount is 0 or more, heating is performed by performing the lapping control for adjusting the lapping amount, and when the necessary heating temperature is obtained when the lapping amount is less than 0, The method for induction heating of a rolled material is characterized in that heating is performed by frequency control in which the lap amount is set to 0 and the frequency is adjusted.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP06162757A JP3112617B2 (en) | 1994-06-21 | 1994-06-21 | Induction heating method for rolled material |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP06162757A JP3112617B2 (en) | 1994-06-21 | 1994-06-21 | Induction heating method for rolled material |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH088050A true JPH088050A (en) | 1996-01-12 |
| JP3112617B2 JP3112617B2 (en) | 2000-11-27 |
Family
ID=15760668
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP06162757A Expired - Fee Related JP3112617B2 (en) | 1994-06-21 | 1994-06-21 | Induction heating method for rolled material |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3112617B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100838092B1 (en) * | 2000-04-19 | 2008-06-13 | 엘렉뜨리시뜨 드 프랑스 | Transverse flux induction heating device with magnetic circuit of variable width |
-
1994
- 1994-06-21 JP JP06162757A patent/JP3112617B2/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100838092B1 (en) * | 2000-04-19 | 2008-06-13 | 엘렉뜨리시뜨 드 프랑스 | Transverse flux induction heating device with magnetic circuit of variable width |
Also Published As
| Publication number | Publication date |
|---|---|
| JP3112617B2 (en) | 2000-11-27 |
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