JPH0559182B2 - - Google Patents
Info
- Publication number
- JPH0559182B2 JPH0559182B2 JP19257289A JP19257289A JPH0559182B2 JP H0559182 B2 JPH0559182 B2 JP H0559182B2 JP 19257289 A JP19257289 A JP 19257289A JP 19257289 A JP19257289 A JP 19257289A JP H0559182 B2 JPH0559182 B2 JP H0559182B2
- Authority
- JP
- Japan
- Prior art keywords
- transformer
- heating
- winding
- primary winding
- taps
- 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 - Lifetime
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Landscapes
- Heat Treatment Of Strip Materials And Filament Materials (AREA)
Description
(産業上の利用分野)
本発明は走行する帯材を各種目的で所定温度ま
で通電加熱する装置における帯材通電加熱用リン
グトランス、詳しくは各種寸法や各種材質の帯材
に対応して巾方向均一加熱可能、ないし不均一加
熱可能な汎用性のある帯材通電加熱用リングトラ
ンスに関する。
(従来の技術)
本願共同出願人中の一方出願人は、新規技術思
想に立脚した走行材の通電加熱装置を創出し、線
材を対象とする発明は特願昭61−272798号(特開
昭63−128125号)をもつて、また帯材を対象とす
る発明は特願昭62−300127号をもつて出願してい
る。両出願発明は、例えば帯材を対象する装置を
示す第1図aおよびbに従つて説明すれば、送り
通路Lが環状鉄心11の環内を貫通するトランス
10、当該トランス10の両端に近接配置されて
送り通路上の帯材Wに接触する例えば対ロール
a,bからなるロール電極21,22、および当
該両ロール電極21,22間を例えば摺動子Sを
介して電気的に接続する導電材3,3から構成さ
れ、両ロール電極21,22間にある走行中の被
加熱帯材Wの抵抗R1と導電材3,3の抵抗R2
との関係をR1>>R2に設定し、トランス10
の一次巻線12への給電により上記両ロール電極
21,22間を走行中の帯材Wに導電材3,3を
帰線とする二次電流を誘起させて加熱することを
要旨とする通電加熱装置である。
(従来技術に存する問題点)
ところで、当該通電加熱装置100は、線材を
加熱対象とする場合には何等問題を生じないが、
帯材を加熱対象とする場合には実施にあたり、巾
方向を如何に均一加熱するかの問題が浮かび上が
つてきた。また、たとえ均一加熱が得られる所定
構成としても、均一加熱が得られる帯材の寸法範
囲は限定され、かつ帯材の材質が異なると、たと
え寸法が同じであつても均一加熱が得られず、従
つて異なる材質、寸法の帯材にそれぞれ対応した
多数のトランスを準備する必要があり、設備費が
嵩むという問題点が指摘された。さらには、装置
が帯材を均一加熱可能構成にしてあると、必要に
応じて、例えばエツジ部を中央部よりやや高温に
加熱したい等、能動的に巾方向の偏熱を望む場合
には、全く対応し難いなどの問題点を内蔵してい
ることも判明し、対策が希求されるところとなつ
た。
(発明の目的)
本発明は特願昭62−300127号出願発明である帯
材通電加熱装置発明が抱える上述の問題点を解消
するためになされたもので、各種寸法や各種材質
の帯材に対応して巾方向均一加熱可能、ないし所
望する不均一加熱を得ることが可能な汎用性のあ
る帯材通電加熱用リングトランスを提供すること
を目的とする。
(発明の構成)
本発明の要旨は、トランスの一次巻線を鉄心の
間口巾方向ほぼ全長にわたり多巻回するととも
に、当該巻線の所定複数位置にタツプを設け、当
該タツプを介して一次巻線への給電範囲を加熱帯
材の材質、巾および板厚に応じて制御可能に構成
してなることを特徴とする帯材通電加熱用リング
トランスにある。
(実施例)
本発明を第2図に従つて以下に詳述する。
トランス10の鉄心11には、図示の如く間口
巾方向ほぼ全長にわたり一次巻線12が多巻回さ
れている。当該一次巻線12には、Tとして示す
タツプが例えばa〜nの如く、所定複数位置の巻
線に設けられている。従つて、例えばタツプTg
およびThを閉、その他を開状態とし、Eとして
示す電源から一次巻線12へ給電すれば、給電電
流はタツプTg・Th間に位置する巻線に限定され
て流れ、タツプTeおよびTiを閉、その他を開状
態として給電すれば、給電電流はタツプTe・Ti
間に位置する巻線に限定されて流れ、さらにタツ
プTaおよびTnを閉、その他を開状態として給電
すれば、給電電流は一次巻線12の全長を流れる
こととなる。このように本発明トランス構成は、
一次巻線12への給電電流を所定範囲に限定給電
したり、あるいは全長にわたる給電とする等、一
次巻線12への給電範囲を制御可能である。
(発明の作用)
本発明は、材質や巾および板厚が異なる各種の
帯材それぞれに対応して一次巻線への給電範囲を
所定に制御することにより、それぞれの帯材を巾
方向均一加熱、ないし所望する不均一加熱可能と
する作用がある。
(発明完成に至るまでの経過)
本発明は、通電加熱時の電流密度解析、熱伝導
解析ならびに実機を用いた実験を経て完成され
た。
(1) 通電加熱時の電流密度解析:
通電加熱時のトランス10により被加熱帯材W
に誘起される電流密度分布が帯材Wの巾(Ww)、
板厚tおよび一次巻線12の巻巾(Cw)との関
係で如何なる変化を示すかを有限要素法を使用し
たコンピユータにより解析した。その一部を以下
に開示する。
電磁方程式の基本式
rot(1/μrot〓)=〓o−σ∂〓/〓t−σgradφ…
…(1)
上記式(1)において、x−y2次元場では等方性
であるとし、また〓が正弦波的に変化するものと
すれば、式(1)は次のようになる。
1/μ(∂2Az/∂x2+∂2Az/∂y2)=−Jo+jωσAz
+σgradφ
……(2)
ただし、
〓:磁気ベクトルポテンシヤル (wb/m)
Az:磁気ベクトルポテンシヤルのZ方向成分
(wb/m)
〓o:強制電流密度 (A/m2)
Joz:強制電流密度のZ方向成分 (A/m2)
μ:透磁率 (H/m)
σ:導電率 (υ/m)
ω:角周波数 (rad/s)
φ:電位 (V)
A 上記式(2)を用い、共通解析条件ならびに物性
値を下記の通りとし、例えば一般的な加熱対象
材である鋼帯を取り上げ、板厚t2mmの帯材を対
象として、帯巾(Ww)と一次巻線の巻巾
(Cw)とが(Ww=Cw)の関係にある場合の
帯材導電率σsの変化と帯材の巾方向表面電流密
度J分布の変化との相関関係を求めた。
f=60(Hz)
μc=6000(鉄心の比透磁率)
μw=1(一次巻線の比透磁率)
μs=30(帯材の比透磁率)
σs=(帯材導電率);20℃……7.7×106
200℃……4.0×106
750℃……1.0×106
ただし、一次巻線・帯材間のギヤツプ
g=150(mm)
また、一次巻線電流Jozは帯材の平均電流密
度が1.5×106(A/m2)になるように設定した。
第3図は(Ww=Cw)の関係にある場合の
解析結果であり、aは磁束シミユレーシヨン
図、またbは帯材導電率σsの上記変化に対応し
た帯材の電流密度J分布図で、図における線イ
は7.7×106の、線ロは4.0×106の、また線ハは
1.0×106の場合であつて、温度上昇とともに電
流密度Jが均一分布となることを示す。
また、各条件における電流密度偏差(edge
−center/center)をまとめて第1表として示
す。
(Industrial Application Field) The present invention relates to a ring transformer for energizing and heating a running band in a device that energizes and heats a running band to a predetermined temperature for various purposes. The present invention relates to a versatile ring transformer for electrically heating a band material that can be heated uniformly or unevenly. (Prior art) One of the joint applicants of this application created an electrical heating device for running materials based on a new technical concept, and the invention directed to wire rods was published in Japanese Patent Application No. 61-272798 (Japanese Unexamined Patent Publication No. 272798). No. 63-128125), and the invention directed to the band material was filed in Japanese Patent Application No. 62-300127. The inventions of both applications will be described with reference to FIGS. 1a and 1b showing a device for handling a strip material, for example, a transformer 10 in which the feed passage L passes through the inside of the ring of the annular iron core 11, and a transformer 10 that is close to both ends of the transformer 10. Roll electrodes 21 and 22 made up of, for example, a pair of rolls a and b are placed and in contact with the strip material W on the feed path, and the two roll electrodes 21 and 22 are electrically connected via, for example, a slider S. The resistance R1 of the running heated belt material W, which is composed of the conductive materials 3 and 3 and is between the roll electrodes 21 and 22, and the resistance R2 of the conductive materials 3 and 3.
Set the relationship between R1>>R2 and transformer 10
The purpose of energization is to heat the belt material W running between the two roll electrodes 21 and 22 by inducing a secondary current with the conductive materials 3 and 3 as return wires by supplying power to the primary winding 12. It is a heating device. (Problems existing in the prior art) By the way, the current heating device 100 does not cause any problems when heating a wire rod.
When heating a strip material, the problem of how to uniformly heat it in the width direction has arisen. Furthermore, even if a certain configuration is used to obtain uniform heating, the size range of the strip material that provides uniform heating is limited, and if the material of the strip material is different, even if the dimensions are the same, uniform heating may not be obtained. Therefore, it has been pointed out that it is necessary to prepare a large number of transformers corresponding to strips of different materials and sizes, leading to an increase in equipment costs. Furthermore, if the device is configured to uniformly heat the strip material, if necessary, for example, if you want to heat the edge portion to a slightly higher temperature than the center portion, or actively want to heat unevenly in the width direction, It was also discovered that there were some built-in problems that were difficult to deal with, and countermeasures were sought. (Purpose of the Invention) The present invention has been made to solve the above-mentioned problems of the invention of the device for energizing heating of strip material, which is the invention of Japanese Patent Application No. 62-300127. Accordingly, it is an object of the present invention to provide a versatile ring transformer for electrically heating a band material, which can uniformly heat the width direction or obtain desired non-uniform heating. (Structure of the Invention) The gist of the present invention is to wind the primary winding of the transformer multiple times over almost the entire length in the width direction of the iron core, provide taps at a plurality of predetermined positions on the winding, and wind the primary winding through the taps. A ring transformer for energizing a heating band is characterized in that the range of power feeding to the wire can be controlled in accordance with the material, width and thickness of the heating band. (Example) The present invention will be described in detail below with reference to FIG. As shown in the figure, a primary winding 12 is wound around the core 11 of the transformer 10 in multiple turns over almost the entire length in the width direction. In the primary winding 12, taps indicated as T are provided at a plurality of predetermined positions of the winding, such as a to n. Therefore, for example, tap Tg
and Th are closed, and the others are open, and if power is supplied to the primary winding 12 from the power supply shown as E, the power supply current flows only to the winding located between taps Tg and Th, and taps Te and Ti are closed. , and other open states, the power supply current will be the same as the tap Te/Ti.
If power is supplied with the taps Ta and Tn closed and the others open, the supplied current will flow through the entire length of the primary winding 12. In this way, the transformer configuration of the present invention is
It is possible to control the range of power supply to the primary winding 12, such as by limiting the power supply current to the primary winding 12 to a predetermined range, or by supplying power over the entire length. (Function of the Invention) The present invention heats each strip material uniformly in the width direction by controlling the power supply range to the primary winding in a predetermined manner corresponding to each of various strip materials having different materials, widths, and plate thicknesses. , or has the effect of enabling desired non-uniform heating. (Progress until completion of the invention) The present invention was completed through current density analysis during electrical heating, heat conduction analysis, and experiments using an actual machine. (1) Current density analysis during current heating: The belt material W to be heated by the transformer 10 during current heating
The current density distribution induced by the width of the strip W (Ww),
A computer using the finite element method was used to analyze changes in relation to the plate thickness t and the winding width (Cw) of the primary winding 12. Some of them are disclosed below. Basic formula of electromagnetic equation rot(1/μrot〓)=〓o−σ∂〓/〓t−σgradφ…
...(1) In the above equation (1), if it is assumed that the x-y two-dimensional field is isotropic and that 〓 changes sinusoidally, then equation (1) becomes as follows. 1/μ(∂ 2 Az/∂x 2 +∂ 2 Az/∂y 2 )=−Jo+jωσAz
+σgradφ ...(2) However, 〓: Magnetic vector potential (wb/m) Az: Z-direction component of magnetic vector potential
(wb/m) 〓o: Forced current density (A/m 2 ) Joz: Z-direction component of forced current density (A/m 2 ) μ: Magnetic permeability (H/m) σ: Electrical conductivity (υ/m) ω: Angular frequency (rad/s) φ: Potential (V) A Using the above formula (2), the common analysis conditions and physical property values are as follows, and for example, taking a steel strip that is a common material to be heated, Changes in the conductivity σs of the strip material and the width of the strip material when the strip width (Ww) and the winding width of the primary winding (Cw) are in the relationship (Ww=Cw) for a strip material with a plate thickness of 2 mm. The correlation between the change in the directional surface current density J distribution was determined. f = 60 (Hz) μc = 6000 (relative magnetic permeability of iron core) μw = 1 (relative magnetic permeability of primary winding) μs = 30 (relative magnetic permeability of strip material) σs = (conductivity of strip material); 20℃ ……7.7×10 6 200℃……4.0×10 6 750℃……1.0×10 6 However, the gap between the primary winding and the strip g = 150 (mm) Also, the primary winding current Joz is The average current density was set to 1.5×10 6 (A/m 2 ). Figure 3 shows the analysis results when there is a relationship of (Ww = Cw), a is a magnetic flux simulation diagram, and b is a current density J distribution diagram of the strip material corresponding to the above change in the strip material conductivity σs, Line A in the figure is 7.7×10 6 , line B is 4.0×10 6 , and line C is
In the case of 1.0×10 6 , it shows that the current density J becomes uniformly distributed as the temperature rises. In addition, the current density deviation (edge
-center/center) are summarized in Table 1.
【表】【table】
Claims (1)
ス、当該トランス両端に近接してそれぞれ配置さ
れて送り通路上の帯材と接触するロール電極、お
よび当該両ロール電極間を電気的に接続する導電
材からなり、上記トランスの一次巻線への給電に
より上記両ロール電極間を走行中の帯材に上記導
電材を帰線とする二次電流を誘起させて加熱する
加熱装置のトランスにおいて、一次巻線を鉄心の
間口巾方向ほぼ全長にわたり多巻回するととも
に、当該巻線の所定複数位置にタツプを設け、当
該タツプを介して一次巻線への給電範囲を加熱帯
材の材質、巾および板厚に応じて制御可能に構成
してなることを特徴とする帯材通電加熱用リング
トランス。1. A transformer in which a feed passage passes through the ring of the annular iron core, roll electrodes arranged close to both ends of the transformer and in contact with the strip material on the feed passage, and a conductor that electrically connects the two roll electrodes. In the transformer of the heating device, the primary The winding is wound multiple times over almost the entire length in the width direction of the iron core, and taps are provided at a plurality of predetermined positions on the winding, and the power supply range to the primary winding through the taps is determined by the material of the heating band material, the width, and the like. A ring transformer for energizing heating of a band material, characterized by being configured to be controllable according to the thickness of the plate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19257289A JPH0361336A (en) | 1989-07-27 | 1989-07-27 | Ring transformer for electrical heating of strip |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19257289A JPH0361336A (en) | 1989-07-27 | 1989-07-27 | Ring transformer for electrical heating of strip |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0361336A JPH0361336A (en) | 1991-03-18 |
| JPH0559182B2 true JPH0559182B2 (en) | 1993-08-30 |
Family
ID=16293513
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19257289A Granted JPH0361336A (en) | 1989-07-27 | 1989-07-27 | Ring transformer for electrical heating of strip |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0361336A (en) |
-
1989
- 1989-07-27 JP JP19257289A patent/JPH0361336A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0361336A (en) | 1991-03-18 |
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