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JPS635873B2 - - Google Patents
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JPS635873B2 - - Google Patents

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Publication number
JPS635873B2
JPS635873B2 JP6911883A JP6911883A JPS635873B2 JP S635873 B2 JPS635873 B2 JP S635873B2 JP 6911883 A JP6911883 A JP 6911883A JP 6911883 A JP6911883 A JP 6911883A JP S635873 B2 JPS635873 B2 JP S635873B2
Authority
JP
Japan
Prior art keywords
side edge
blank
heating coil
magnetic
heating
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
Application number
JP6911883A
Other languages
Japanese (ja)
Other versions
JPS59196590A (en
Inventor
Hideo Kurashima
Kazuhisa Ishibashi
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.)
Toyo Seikan Group Holdings Ltd
Original Assignee
Toyo Seikan Kaisha 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 Toyo Seikan Kaisha Ltd filed Critical Toyo Seikan Kaisha Ltd
Priority to JP6911883A priority Critical patent/JPS59196590A/en
Publication of JPS59196590A publication Critical patent/JPS59196590A/en
Publication of JPS635873B2 publication Critical patent/JPS635873B2/ja
Granted legal-status Critical Current

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  • General Induction Heating (AREA)

Description

【発明の詳細な説明】 本発明は非磁性金属薄板の加熱方法に関し、さ
らに詳しくは、例えば側面接着部を有する缶胴体
を製造するために、非磁性金属薄板の、ノツチを
形成された側縁部を、高周波誘導加熱する方法に
関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for heating a sheet of non-magnetic metal, and more particularly to a heating method for heating a sheet of non-magnetic metal, and more particularly, for heating a notched side edge of a sheet of non-magnetic metal, for example for producing a can body with a side adhesive. The present invention relates to a method for high-frequency induction heating of parts.

非磁性金属薄板、例えばアルミニウム薄板の側
縁部を長さ方向に沿い比較的均一に加熱する方法
として、本発明等の一人は特公昭55−39606号公
報において、浸透の深さ以上の厚さを持つ短冊状
の非磁性金属薄板を所定の平面状通路を通して移
動せしめ、この薄板の側縁を、前記通路面に、前
記薄板がない状態において実質的に垂直な磁界を
持つ高周波誘導加熱コイルで加熱するにあたり、
前記金属薄板を前記通路を通して間歇的に送るこ
と、および前記金属薄板の間歇運動における停止
位置の一つと、前記高周波誘導加熱コイルの設置
位置とを対応せしめかつ前記加熱コイルによる実
質的に垂直な磁界が実質的に存在する領域の前記
薄板側縁に沿つた長さが、前記金属薄板の側縁の
長さよりも実質的に短かいこと、および前記金属
薄板の側縁の前端が前記領域の前端よりも実質的
に進行方向前方に、かつ前記側縁の後端が前記領
域の後端よりも実質的に進行方向後方にある期間
に、加熱コイルへの入力電圧を強めることを特徴
とする高周波誘導加熱方法を提案した。
In Japanese Patent Publication No. 55-39606, one of the authors of the present invention proposed a method for heating the side edges of a non-magnetic metal thin plate, such as an aluminum thin plate, relatively uniformly along the length direction. A rectangular non-magnetic metal thin plate having a shape is moved through a predetermined planar passage, and the side edge of this thin plate is heated by a high-frequency induction heating coil having a magnetic field substantially perpendicular to the plane of the passage when the thin plate is not present. When heating,
feeding the thin metal sheet intermittently through the passageway; one of the stop positions in the intermittent movement of the thin metal sheet corresponds to an installation position of the high frequency induction heating coil; and a substantially perpendicular magnetic field by the heating coil; The length along the side edge of the thin metal plate of the area where substantially exists is substantially shorter than the length of the side edge of the thin metal plate, and the front end of the side edge of the thin metal plate is the front edge of the area. and during a period in which the rear end of the side edge is substantially rearward in the traveling direction than the rear end of the region, the input voltage to the heating coil is increased. An induction heating method was proposed.

この方法によれば、側縁部の前後端が過熱によ
り溶融することなく、その前端から後端まで実質
的に均一に加熱することができる。
According to this method, the front and rear ends of the side edge portions do not melt due to overheating, and can be heated substantially uniformly from the front end to the rear end.

しかしながら第1図に示すような、ノツチ2を
有する非磁性金属薄板よりなるブランク1の側縁
部1aを加熱する場合には、第3図に示すような
誘導電流3が側縁部1aを流れて、ノツチ2の近
傍部2aにおける電流密度が他の部分よりも過大
となるため、近傍部2aが過熱されて、近傍部2
a表面の有機塗膜が焦げたり、極端な場合には近
傍部2aの金属が溶融するという問題を生じ易
い。
However, when heating the side edge 1a of a blank 1 made of a non-magnetic metal thin plate having a notch 2 as shown in FIG. 1, an induced current 3 as shown in FIG. 3 flows through the side edge 1a. As a result, the current density in the vicinity part 2a of the notch 2 becomes excessively large compared to other parts, so that the vicinity part 2a is overheated and the vicinity part 2a is
Problems such as burning of the organic coating film on the surface a or, in extreme cases, melting of the metal in the vicinity part 2a, are likely to occur.

本発明は以上に述べた従来技術の問題点の解消
を図ることを目的とする。
It is an object of the present invention to solve the problems of the prior art described above.

上記目的を達成するため、本発明は非磁性金属
薄板の、ノツチを形成された側縁部を、高周波誘
導加熱コイルに沿う所定の平面状通路を通つて間
欠的に移動せしめて高周波誘導加熱する方法であ
つて、該加熱コイルは、該通路に該側縁部がない
状態において該通路に対し実質的に垂直な磁束を
形成し、該通路に該側縁部が停止している状態に
おいて、該ノツチに対応する該コイルの部分と該
側縁部間の電磁結合が弱くなるようになつてお
り、かつ上記の該側縁部が停止している状態にお
いて、該加熱コイルへの入力電力を高めることを
特徴とする非磁性金属薄板の側縁部の加熱方法を
提供するものである。
To achieve the above object, the present invention performs high-frequency induction heating by intermittently moving the notched side edge of a non-magnetic metal thin plate through a predetermined planar path along a high-frequency induction heating coil. The heating coil generates a magnetic flux substantially perpendicular to the passageway when the passageway is free of the side edges, and when the side edges are stationary in the passageway. When the electromagnetic coupling between the part of the coil corresponding to the notch and the side edge is weakened, and the side edge is stopped, input power to the heating coil is reduced. The present invention provides a method for heating the side edge of a non-magnetic metal thin plate, which is characterized by heating the side edge of a non-magnetic thin metal plate.

以下図面を参照しながら本発明について説明す
る。
The present invention will be described below with reference to the drawings.

第1図のブランク1は、本発明に適用される非
磁性金属薄板の例を示したものであつて、両面に
焼付塗膜(例えばエポキシフエノール系塗膜)を
有するアルミニウム合金薄板より形成されてい
る。ブランク1の両側縁部1a,1bの中央には
V字状のノツチ2が形成されており、また両ノツ
チ2の頂点を通つて、両面に、第2図に示すよう
な断面V字状のスコア部4が形成されている。ま
た側縁部1a,1bの両端には隅切り部5が形成
されている。さらに側縁部1a,1bには、熱接
着テープ6が熱融着されている。
Blank 1 in FIG. 1 shows an example of a non-magnetic metal thin plate to which the present invention is applied, and is made of an aluminum alloy thin plate having baked coatings (for example, epoxyphenol coatings) on both sides. There is. A V-shaped notch 2 is formed in the center of both side edges 1a and 1b of the blank 1, and a V-shaped cross section as shown in FIG. A score section 4 is formed. Further, corner cut portions 5 are formed at both ends of the side edge portions 1a and 1b. Further, a thermal adhesive tape 6 is heat-sealed to the side edges 1a and 1b.

このようなブランク1は例えば次のようにして
形成される。
Such a blank 1 is formed, for example, as follows.

まず前工程において、ブランク1が12枚ほど切
り取れる長さのストリツプ状薄板の両側縁部(1
a,1bにあたる部分)を高周波誘導加熱(例え
ば、200℃〜300℃に)した後、側縁部(1aにあ
たる部分)の片面(第1図における)および側縁
部(1bにあたる部分)の両面に接着剤テープ6
(例えばナイロン12のフイルムよりなる)を熱
融着し、その後ブランク1の長さにスリツトし、
同時にスコア部4を形成する。次いでブランク1
を缶胴成形機に運び、ノツチ2および隅切り部5
を形成して、ブランク1を形成する。
First, in the pre-process, both edges (1
After high-frequency induction heating (for example, to 200°C to 300°C) of the side edges (portions corresponding to a and 1b), one side of the side edge (portion corresponding to 1a) (in Fig. 1) and both sides of the side edge (portion corresponding to 1b) adhesive tape 6
(for example, made of a nylon 12 film) is heat-sealed, and then slit to the length of the blank 1,
At the same time, the score section 4 is formed. Then blank 1
is carried to the can body forming machine, and the notch 2 and corner cut portion 5 are
to form blank 1.

次にブランク1を印刷面が外面にくるようにし
て缶胴状に丸め、後記のような高周波誘導加熱法
により側縁部1a,1bの接着剤テープ6を溶融
し、側縁部1a,1bが重なるように重ね合わせ
て押圧を加えながら、側縁部1a,1bを接着剤
テープ6を介して熱融着し、短時間に冷却して側
面接着部を有する缶胴成形体(図示されない)を
形成する。
Next, the blank 1 is rolled into a can body shape with the printed surface facing the outside, and the adhesive tape 6 on the side edges 1a, 1b is melted by a high frequency induction heating method as described later. The side edges 1a and 1b are heat-sealed via the adhesive tape 6 while applying pressure so that they overlap, and are cooled in a short time to form a can body molded body (not shown) having a side surface adhesive part. form.

この缶胴成形体をスコア部4に沿つて切断する
ことによつて側面接着部を有する缶胴体(図示さ
れない)を製造することができる。缶胴体はその
後両開口端部にフランジ部を形成された後、フラ
ンジ部に底部材と蓋部材を2重巻締されて密封缶
となる。
By cutting this molded can body along the score portion 4, a can body (not shown) having a side adhesive portion can be manufactured. After that, flanges are formed on both open ends of the can body, and a bottom member and a lid member are double-sealed to the flanges to form a sealed can.

以上のようにして同一工程で2ケの缶胴体を製
造することができる。なおノツチ2および隅切り
部5は、上記缶胴体のフランジ部の側面接着部に
対応する部分が他の部分より厚くなつて、2重巻
締後の密封性が損われるのを防止するため形成さ
れたものである。
As described above, two can bodies can be manufactured in the same process. Note that the notch 2 and the corner cut portion 5 are formed to prevent the part corresponding to the side adhesive part of the flange part of the can body from becoming thicker than other parts, which would impair the sealing performance after double seaming. It is what was done.

第4図、第5図、第6図は、ブランク1の側縁
部1aを加熱するのに用いられる、高周波誘導加
熱コイル装置7(以上コイル装置と略称する)を
示したものであつて、コイル装置7は、高周波誘
導加熱コイル8(本明細書においては加熱コイル
とよぶ)、および加熱コイル8を包囲する断面コ
字状の高透磁率材料(例えばフエライト)よりな
る、ポケツト部9dを有する磁芯9を備えてい
る。
FIG. 4, FIG. 5, and FIG. 6 show a high-frequency induction heating coil device 7 (hereinafter abbreviated as the coil device) used to heat the side edge 1a of the blank 1. The coil device 7 has a high-frequency induction heating coil 8 (referred to as a heating coil in this specification) and a pocket portion 9d that surrounds the heating coil 8 and is made of a high magnetic permeability material (for example, ferrite) and has a U-shaped cross section. It has a magnetic core 9.

加熱コイル8は、第5図に示すように、流れる
電流の方向が同じである上下方向に対向して配設
された導体8a,8b、および流れる電流の方向
が導体8a,8bの夫々と反対であり、かつ夫々
導体8aおよび8bに近接して、上下方向に対向
して配設された導体8cおよび8dを備えてい
る。
As shown in FIG. 5, the heating coil 8 has conductors 8a and 8b disposed facing each other in the vertical direction, in which the current flows in the same direction, and conductors 8a and 8b in which the direction of the current flows is opposite to that of the conductors 8a and 8b, respectively. The conductors 8c and 8d are disposed close to the conductors 8a and 8b, respectively, and facing each other in the vertical direction.

第4図に示すように、磁芯9内を水平に延びる
上部導体8a,8cは、磁芯9の上壁部9aの両
側端部9a1,9a2を出ると直ちに立上り、一方磁
芯9内を水平に延びる下部導体8b,8dは、磁
芯9の下壁部9bの両側端部9b1,9b2を出ると
直ちに立下つている。そして第6図に示すよう
に、磁芯9の長さl1は、側縁部1aの両側端1
a2,1a3の過熱防止のため、加熱されるべき側縁
部1aの長さl2よりも僅かに小さく(通常6〜10
mm程度小さく)定められている。また磁芯の上壁
部9aおよび下壁部9bの、長手方向中央には夫
夫、側壁部9cまで延びる凹部10および11が
形成されていて、凹部10,11に対応する部分
にはポケツト部9dは存在しない。
As shown in FIG. 4, the upper conductors 8a and 8c extending horizontally within the magnetic core 9 rise immediately after exiting both ends 9a 1 and 9a 2 of the upper wall 9a of the magnetic core 9; The lower conductors 8b and 8d extending horizontally inside the magnetic core 9 fall immediately after exiting both ends 9b 1 and 9b 2 of the lower wall 9b of the magnetic core 9. As shown in FIG. 6, the length l 1 of the magnetic core 9 is equal to
To prevent overheating of a 2 and 1a 3 , the length l 2 of the side edge 1a to be heated is slightly smaller (usually 6 to 10
mm) is determined. Further, recesses 10 and 11 are formed in the longitudinal center of the upper wall portion 9a and the lower wall portion 9b of the magnetic core, and extend to the side wall portion 9c. 9d does not exist.

ブランク1は、第5図b、第6図に示されるよ
うに、磁芯9のポケツト部9d内を、側縁部1a
が上部導体8a,8cおよび下部導体8b,8d
の間の、高さ方向中央位置に沿つて水平方向に、
すなわち平面状通路14(第5図a)に沿つて移
動するようにして、間欠的に図示されない移送装
置によつて移送される。
As shown in FIG. 5b and FIG.
are upper conductors 8a, 8c and lower conductors 8b, 8d
horizontally along the height center position between
That is, it is intermittently transferred by a transfer device (not shown) so as to move along the planar path 14 (FIG. 5a).

第5図aはポケツト部9dにブランク1がない
場合に、導体8a,8bによつて形成される磁束
12および導体8c,8dによつて形成される磁
束13を示したものであつて、対向する導体8a
および8bを流れる電流の方向が同じであるの
で、磁束12は、ブランク1の通路14に対し実
質的に垂直に形成される。同様にして磁束13も
通路14に対し実質的に垂直に形成される。
FIG. 5a shows the magnetic flux 12 formed by the conductors 8a and 8b and the magnetic flux 13 formed by the conductors 8c and 8d when there is no blank 1 in the pocket part 9d. conductor 8a
Since the direction of the current flowing through and 8b is the same, the magnetic flux 12 is formed substantially perpendicular to the path 14 of the blank 1. Similarly, the magnetic flux 13 is also formed substantially perpendicular to the passage 14.

なお、ブランク1の通路14に対し、実質的に
垂直な磁束を形成する加熱コイル装置の他の例と
して、特願昭56−33926に提案されている加熱コ
イル装置があげられるが、本例の加熱コイル装置
の方が好ましい。
Note that another example of a heating coil device that forms magnetic flux substantially perpendicular to the passage 14 of the blank 1 is the heating coil device proposed in Japanese Patent Application No. 56-33926. A heating coil device is preferred.

第5図bは、ポケツト部9dにブランク1の側
縁部1aがある場合の、導体8a,8bによつて
形成される磁束12′、および導体8c,8dに
よつて形成される磁束13′を示したものである。
ブランク1は非磁性体よりなるので、磁束13′
は側縁部1a内に入り込むことなく、側縁部1a
の端縁1a1を回り込むようにして、磁芯の側壁部
9cを通つて形成される。また磁束12′は側縁
部1aの上方と下方に分れて、導体8aおよび8
bの周りに、夫々磁芯の上壁部9aおよび下壁部
9bを通つて形成される。
FIG. 5b shows the magnetic flux 12' formed by the conductors 8a, 8b and the magnetic flux 13' formed by the conductors 8c, 8d when the side edge 1a of the blank 1 is in the pocket part 9d. This is what is shown.
Since the blank 1 is made of non-magnetic material, the magnetic flux 13'
without entering the side edge 1a.
It is formed through the side wall portion 9c of the magnetic core so as to go around the edge 1a1 of the magnetic core. Further, the magnetic flux 12' is divided into upper and lower parts of the side edge 1a, and conductors 8a and 8
b, respectively, through the upper wall portion 9a and lower wall portion 9b of the magnetic core.

以上のように、磁束12′,13′は高透磁率材
料よりなる磁芯を通つて形成されるので、ポケツ
ト部9dがない凹部10,11の導体8の部分に
形成される磁束(図示されない)よりも、高い磁
束密度を有する。このような場合、一般に単位時
間当りの金属板の温度上昇は、磁束密度のほぼ2
乗に比例するとみなされるから、かりに側縁部1
aの状態が長手方向に一様の場合(例えばノツチ
2がない場合)は、ポケツト部9dに停止して位
置する側縁部1aの部分よりも、凹部10,11
に対向して位置する側縁部1aの部分の加熱温度
は低くなる。
As described above, since the magnetic fluxes 12' and 13' are formed through the magnetic core made of a high magnetic permeability material, the magnetic fluxes (not shown) formed in the portions of the conductor 8 in the recesses 10 and 11 where the pocket portion 9d is not present. ) has a higher magnetic flux density. In such cases, the temperature rise of the metal plate per unit time is generally approximately 2 times the magnetic flux density.
Since it is considered to be proportional to the power of
When the condition of a is uniform in the longitudinal direction (for example, when there is no notch 2), the recesses 10, 11
The heating temperature of the portion of the side edge portion 1a located opposite to is lower.

以上のコイル装置7によつてブランク1の側縁
部1aは次のようにして誘導加熱される。
The side edge portion 1a of the blank 1 is induction heated by the coil device 7 described above in the following manner.

加熱コイル8の入力電力を0、又は比較的小さ
くした状態において、通路14に沿つてブランク
の側縁部1aをコイル装置7のポケツト部9d内
を矢印方向(第6図)に移行させ、第6図に示す
ように、ノツチ2が凹部10,11の長手方向
(磁芯9の)中央に位置したとき、停止させ、直
ちに加熱コイル8に比較的大きな電力を入力す
る。
With the input power of the heating coil 8 set to 0 or relatively small, the side edge 1a of the blank is moved along the passage 14 into the pocket 9d of the coil device 7 in the direction of the arrow (FIG. 6). As shown in FIG. 6, when the notch 2 is located at the center of the recesses 10 and 11 in the longitudinal direction (of the magnetic core 9), the operation is stopped and a relatively large electric power is immediately input to the heating coil 8.

このさい側縁部1aに第7図に示されるような
誘導電流15,16が、凹部10,11のためノ
ツチ近傍部2aに過度に集中することなく誘起さ
れる。すなわち凹部10,11の寸法、特に長手
方向間隔dを、ノツチ2の底辺幅wと高さh等と
の関連において、実験的に適当に定めることによ
り、ノツチ近傍部2aを過熱することなく、側縁
部1aを、その長手方向に沿い比較的均一に所望
温度範囲内に誘導加熱することができる。上記所
望温度範囲内に達した後、直ち加熱コイル8の入
力電力を、ポケツト部9dに送入前と同様に0又
は比較的小さくして、再びブランク1を矢印方向
に移行させて、コイル装置7から送出する。
At this time, induced currents 15 and 16 as shown in FIG. 7 are induced in the side edges 1a because of the recesses 10 and 11 without being excessively concentrated in the notch vicinity 2a. That is, by appropriately determining the dimensions of the recesses 10 and 11, especially the longitudinal distance d, in relation to the base width w and height h of the notch 2, etc., it is possible to avoid overheating the notch vicinity 2a. The side edge portion 1a can be induction heated relatively uniformly along its longitudinal direction within a desired temperature range. Immediately after reaching the above desired temperature range, the input power of the heating coil 8 is reduced to 0 or relatively small as before feeding into the pocket portion 9d, and the blank 1 is moved again in the direction of the arrow, and the coil It is sent from the device 7.

停止のさい、側縁部1aの両側端部1a2,1a3
は、磁芯9の両側端部9a1,9b1および9a2,9
b2よりも外側に出ているので、磁束の側端部1
a2,1a3への回り込みは殆んどなく、ブランク1
を移動のさいの加熱コイル8の入力電力を、実験
にもとづいて適当に定めることにより、側端部1
a2,1a3の加熱温度も、側縁部1aの他の部分の
夫とほぼ等しくすることができる。
When stopping, both ends 1a 2 and 1a 3 of the side edge 1a
are the opposite ends 9a 1 , 9b 1 and 9a 2 , 9 of the magnetic core 9
b 2 , so the side edge 1 of the magnetic flux
There is almost no wraparound to a 2 , 1a 3 , and blank 1
By appropriately determining the input power of the heating coil 8 when moving the side end 1 based on experiments,
The heating temperature of a 2 and 1a 3 can also be made approximately equal to that of the other portions of the side edge portion 1a.

第9図は以上に説明したような構造の高周波誘
導加熱コイル装置7を用いて、側縁部1aと側縁
部1bの間が開いた状態で缶胴状に丸められたブ
ランク1の側縁部1a,1b(熱接着テープ6が
前工程で熱融着されている)を、熱接着テープ6
の融点または軟化点以上に加熱する場合の例を示
したものであつて、20は缶胴状ブランク1を案
内するマンドレルである。
FIG. 9 shows the side edge of the blank 1 which is rolled up into a can body shape with the side edge 1a and side edge 1b open using the high frequency induction heating coil device 7 having the structure as explained above. The parts 1a and 1b (thermal adhesive tape 6 has been heat-sealed in the previous step) are connected to the thermal adhesive tape 6.
The figure shows an example of heating above the melting point or softening point of can body blank 1, and 20 is a mandrel that guides can body-shaped blank 1.

本発明は以上の例によつて制限されるものでな
く、例えば凹部10,11に対応する部分の加熱
コイル8の内面側を、電気良導性の金属板(図示
されない、例えば銅板)で遮蔽することによつ
て、さらに確実にノツチ近傍部2aの過熱を防止
することができる。
The present invention is not limited to the above examples, and for example, the inner surface of the heating coil 8 in the portion corresponding to the recesses 10 and 11 is shielded with a metal plate (not shown, for example, a copper plate) having good electrical conductivity. By doing so, overheating of the notch vicinity portion 2a can be more reliably prevented.

またノツチ2は側縁部に沿い複数個形成されて
いてもよい。この場合はブランクが停止した状態
において、ノツチに対応する位置に凹部が形成さ
れた、もしくは前述の遮蔽板がさらに設けられた
コイル装置を用いて、誘導加熱を行なう。またノ
ツチも任意の形状のものであつてよい。
Further, a plurality of notches 2 may be formed along the side edges. In this case, while the blank is stopped, induction heating is performed using a coil device in which a recess is formed at a position corresponding to the notch, or in which the above-mentioned shielding plate is further provided. Further, the notch may also be of any shape.

本発明によれば、非磁性金属薄板のノツチの形
成された側縁部を、ノツチ近傍部において過熱を
生ずることなく、すなわち塗膜の焦げや、金属の
溶融等のトラブルを生ずることなく、長手方向に
沿い比較的均一に加熱できるという効果を奏す
る。
According to the present invention, the notched side edge of a non-magnetic thin metal plate can be extended in the longitudinal direction without overheating in the vicinity of the notch, that is, without causing troubles such as burning of the paint film or melting of the metal. This has the effect of being able to heat relatively uniformly along the direction.

以下実施例について説明する。 Examples will be described below.

実施例 磁芯の長さl1が62.5mm、凹部10,11の間隔
dが7.5mm、ポケツト部9dの奥行14mm、側壁部
9cの高さ23.5mm、断面楕円状の導体8a,8
b,8c,8dの高さ5.5mm、最大幅2.3mm、導体
8aと8c間、および8bと8d間の中心間隔が
何れも6mm、上部導体8a,8cと下部導体8
b,8d間の間隔(高さ方向の)が7mm、導体8
c,8dの中心より側壁部9c内面の延長面まで
の距離が6mmである第5図、第6図に示すタイプ
のコイル装置7を用意した。
Example The length l1 of the magnetic core is 62.5 mm, the distance d between the recesses 10 and 11 is 7.5 mm, the depth of the pocket portion 9d is 14 mm, the height of the side wall portion 9c is 23.5 mm, and the conductors 8a and 8 have an elliptical cross section.
The height of b, 8c, and 8d is 5.5 mm, the maximum width is 2.3 mm, the center distance between conductors 8a and 8c, and between 8b and 8d is all 6 mm, and the upper conductor 8a, 8c and the lower conductor 8
The distance between b and 8d (in the height direction) is 7 mm, conductor 8
A coil device 7 of the type shown in FIGS. 5 and 6 was prepared in which the distance from the center of the coils c and 8d to the extended surface of the inner surface of the side wall portion 9c was 6 mm.

一方側縁部1aの長さl2が70.6mm、厚さ0.23mm、
ノツチ2の底辺幅wが2mm、高さhが3.5mmの第
1図に示す形状のアルミニウム合金薄板(5052
材)よりなるブランク1を、側縁部1aのポケツ
ト部9dへの突込み深さm(第6図)が12mmとな
るようにして、コイル装置7に通路14を通つ
て、毎分200個の速度で送入した。ブランク1の
コイル装置7における停止時間は0.16秒であり、
停止時にはノツチ2が凹部10,11の長手方向
中央に位置するようにした。
On the other hand, the length l 2 of the side edge 1a is 70.6 mm, the thickness is 0.23 mm,
An aluminum alloy thin plate (5052
A blank 1 made of material) is passed through a passage 14 into a coil device 7 so that the plunge depth m (Fig. 6) of the side edge portion 1a into the pocket portion 9d is 12 mm, and the blank 1 is heated at a rate of 200 coils per minute. Delivered at speed. The stopping time in the coil device 7 of blank 1 is 0.16 seconds,
When stopped, the notch 2 is positioned at the center in the longitudinal direction of the recesses 10, 11.

加熱コイル8に供給される高周波電流の周波数
は400kHzで、真空管式の発振器を用いた。ブラ
ンク1が移行中の加熱コイル8への入力電力は
0、停止中の入力電力は5kWとし、高周波電流
のON時間は0.15秒となるように制御した。
The frequency of the high-frequency current supplied to the heating coil 8 was 400kHz, and a vacuum tube type oscillator was used. The input power to the heating coil 8 when the blank 1 was in transition was 0, the input power when it was stopped was 5 kW, and the ON time of the high frequency current was controlled to be 0.15 seconds.

以上のようにして加熱された側縁部1a近傍
の、示温塗料によつて測定された温度パターンを
第8図に示す。図中e,fおよびgは夫々、温度
が232℃、270℃および300℃の領域を示す。
FIG. 8 shows a temperature pattern measured by the temperature-indicating paint near the side edge 1a heated as described above. In the figure, e, f, and g indicate temperature regions of 232°C, 270°C, and 300°C, respectively.

比較のため凹部10,11が形成されない点
は、上記と同様なコイル装置を用い、ブランク1
を用いて同一条件で加熱を行なつたが、ノツチ2
の近傍部2aの金属が溶融して、満足な加熱ブラ
ンクを得ることができなかつた。
For comparison, blank 1 was prepared using the same coil device as above, except that recesses 10 and 11 were not formed.
Heating was carried out under the same conditions using
The metal in the vicinity of the portion 2a melted, making it impossible to obtain a satisfactory heated blank.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明が適用される非磁性金属薄板の
例の平面図、第2図は第1図の―線に沿う縦
断面図、第3図は従来の方法で第1図の金属薄板
の側縁部を高周波誘導加熱した場合に誘起される
誘導電流を示す要部平面図、第4図は本発明に適
用される高周波誘導加熱コイル装置の例の斜視
図、第5図は第4図の―線に沿う縦断面図で
あつて、第5図aおよびbは、夫々金属薄板が装
入されていない場合、および装入されている場合
の磁束の状態を示す図面、第6図は第4図の―
線に沿う横断面図、第7図は本発明の方法で誘
導加熱された、第1図の金属薄板の側縁部に誘起
され誘導電流を示す要部平面図、第8図は本発明
の方法で誘導加熱された第1図の金属薄板の側縁
部の温度パターンの例を示す要部平面図、第9図
は第4図の加熱コイル装置を缶胴成形機に取付け
て、加熱している状態の例を示す縦断面図であ
る。 1…ブランク(非磁性金属薄板)、1a…側縁
部、2…ノツチ、8…高周波誘導加熱コイル、1
2,13…磁束、14…平面状通路。
FIG. 1 is a plan view of an example of a non-magnetic thin metal plate to which the present invention is applied, FIG. 2 is a longitudinal sectional view taken along the line - in FIG. FIG. 4 is a perspective view of an example of a high-frequency induction heating coil device applied to the present invention, and FIG. FIGS. 5a and 5b are longitudinal cross-sectional views taken along the line - in the figure, and FIGS. is shown in Figure 4.
7 is a cross-sectional view taken along the line, FIG. 7 is a plan view of the main part showing the induced current induced in the side edge of the thin metal plate of FIG. 1 which has been induction heated by the method of the present invention, and FIG. FIG. 9 is a plan view of the main part showing an example of the temperature pattern of the side edge of the thin metal plate shown in FIG. FIG. 1... Blank (non-magnetic metal thin plate), 1a... Side edge, 2... Notch, 8... High frequency induction heating coil, 1
2, 13...Magnetic flux, 14...Planar path.

Claims (1)

【特許請求の範囲】[Claims] 1 非磁性金属薄板の、ノツチを形成された側縁
部を、高周波誘導加熱コイルに沿う所定の平面状
通路を通つて間欠的に移動せしめて高周波誘導加
熱する方法であつて、該加熱コイルは、該通路に
該側縁部がない状態において該通路に対し実質的
に垂直な磁束を形成し、該通路に該側縁部が停止
している状態において、該ノツチに対応する該コ
イルの部分と該側縁部間の電磁結合が弱くなるよ
うになつており、かつ上記の該側縁部が停止して
いる状態において、該加熱コイルへの入力電力を
高めることを特徴とする非磁性金属薄板の側縁部
の加熱方法。
1. A method of performing high frequency induction heating by intermittently moving the notched side edge of a non-magnetic metal thin plate through a predetermined planar path along a high frequency induction heating coil, the heating coil comprising: , forming a magnetic flux substantially perpendicular to the passageway when the side edge is absent from the passageway, and a portion of the coil corresponding to the notch when the side edge is stopped in the passageway; A non-magnetic metal characterized in that the electromagnetic coupling between the side edge portion and the side edge portion is weakened, and the input power to the heating coil is increased when the side edge portion is stopped. Method of heating the side edges of thin plates.
JP6911883A 1983-04-21 1983-04-21 Heating method for non-magnetic metal thin plate Granted JPS59196590A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6911883A JPS59196590A (en) 1983-04-21 1983-04-21 Heating method for non-magnetic metal thin plate

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6911883A JPS59196590A (en) 1983-04-21 1983-04-21 Heating method for non-magnetic metal thin plate

Publications (2)

Publication Number Publication Date
JPS59196590A JPS59196590A (en) 1984-11-07
JPS635873B2 true JPS635873B2 (en) 1988-02-05

Family

ID=13393403

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6911883A Granted JPS59196590A (en) 1983-04-21 1983-04-21 Heating method for non-magnetic metal thin plate

Country Status (1)

Country Link
JP (1) JPS59196590A (en)

Also Published As

Publication number Publication date
JPS59196590A (en) 1984-11-07

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