JPH0362504A - Magnetic levitation apparatus for magnetic plate - Google Patents

Magnetic levitation apparatus for magnetic plate

Info

Publication number
JPH0362504A
JPH0362504A JP19691789A JP19691789A JPH0362504A JP H0362504 A JPH0362504 A JP H0362504A JP 19691789 A JP19691789 A JP 19691789A JP 19691789 A JP19691789 A JP 19691789A JP H0362504 A JPH0362504 A JP H0362504A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic plate
plate
horizontal
magnet
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
Application number
JP19691789A
Other languages
Japanese (ja)
Other versions
JPH0529285B2 (en
Inventor
Hirokazu Saito
斉藤 宏和
Kunihiko Ushio
邦彦 牛尾
Yuzuru Taguchi
譲 田口
Kazuma Watabe
渡部 数馬
Yoshitaka Machida
町田 義孝
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.)
Nippon Steel Corp
Sumitomo Heavy Industries Ltd
Original Assignee
Sumitomo Heavy Industries Ltd
Sumitomo Metal Industries 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 Sumitomo Heavy Industries Ltd, Sumitomo Metal Industries Ltd filed Critical Sumitomo Heavy Industries Ltd
Priority to JP19691789A priority Critical patent/JPH0362504A/en
Publication of JPH0362504A publication Critical patent/JPH0362504A/en
Publication of JPH0529285B2 publication Critical patent/JPH0529285B2/ja
Granted legal-status Critical Current

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Abstract

PURPOSE:To support a magnetic plate approximately horizontally against the gravity and prevent said magnetic plate from warping by installing magnets with specific intervals above and in the horizontal side of the ends of said magnetic plate arranged so that the plane thereof may be approximately horizontal. CONSTITUTION:A magnetic plate 1 is arranged so that the plane 1a thereof may be approximately horizontal. Upper magnets 2 are arranged above both ends 1b of the plate 1 with specific intervals. Horizontal-side magnets 3 are arranged in the horizontal side of both the ends 1b of the plate 1 with specific intervals. The cores 3a of the magnets 3 are connected to the cores 2a of the magnets 2. When currents are passed through the coils 2b and 3b, magnetic circuits each consisting of the core 2a, the gap between the core 2a and the plate 1, the plate 1, the gap between the plate 1 and the core 3a, and the core 3a are formed. Thereby the plate 1 is supported approximately horizontally and the ends 1b thereof are attracted to prevent the plate 1 from warping.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、磁性板材をこれに接触しないで磁気吸引力に
より浮上させる磁性板材用磁気浮上装置に関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magnetic levitation device for magnetic plates that levitates magnetic plates by magnetic attraction without contacting them.

〔従来の技術] この種の磁性板材用磁気浮上装置は、磁性板材の移送時
にこれに接触しないで支持する場合および鋼板塗装ライ
ンにおいて鋼板の先端をこれに接触しないで保持する場
合などに用いられる。
[Prior Art] This type of magnetic levitation device for magnetic plates is used to support magnetic plates without touching them during transport, and to hold the tip of a steel plate without touching it in a steel plate painting line. .

従来の磁性板材用磁気浮上装置は、例えば、第5図に示
すように、磁性板材1の平面の上側にギャップG3をお
いて配置された吸引用電磁石11と、ギャップG3を検
出する距離センサー12と吸引用電磁石11のコア11
aを巻回するコイル11bに励磁電流を流すための制御
電源13とを具備し、距離センサー12からの出力信号
に基づいてギャップG、を所定の値に維持するようにコ
イル11bへの励磁電流を制御して、磁性板材1を水平
にこれに接触しないで定位置に支持するものである。
A conventional magnetic levitation device for a magnetic plate, for example, as shown in FIG. 5, includes an attraction electromagnet 11 placed above the plane of the magnetic plate 1 with a gap G3 therebetween, and a distance sensor 12 that detects the gap G3. and the core 11 of the attraction electromagnet 11
A control power source 13 is provided for passing an excitation current through a coil 11b around which the coil 11b is wound. The magnetic plate 1 is supported horizontally in a fixed position without contacting the magnetic plate 1.

ところで、吸引用電磁石11の吸引力の′:A整におい
ては、吸引用電磁石11により磁性板材1が吸引されて
、ギャップG3が小さくなればなるほど、吸引力Fcが
強くなり、そのままでは、吸引用電磁石11に磁性板材
1が接触してしまうことになるので、これを防止するた
め、ギャップG3に対応した吸引力の制御を必要とする
By the way, when the attraction force of the attraction electromagnet 11 is adjusted to ':A, the magnetic plate material 1 is attracted by the attraction electromagnet 11 and the smaller the gap G3, the stronger the attraction force Fc becomes. Since the magnetic plate material 1 will come into contact with the electromagnet 11, in order to prevent this, it is necessary to control the attraction force corresponding to the gap G3.

[発明が解決しようとする課題] しかし、従来の磁性板材用磁気浮上装置は、ギャップG
、の変化に対する吸引用電磁石11の吸引力F、の変化
が非常に大きく、磁気飽和および磁気漏洩を無視すれば
、一定の励磁化では、ギャップG3の2乗に反比例して
変化するので、ギャップG3の変化に追随させて吸引力
Fcを制御することが面倒であるという欠点がある。
[Problem to be solved by the invention] However, the conventional magnetic levitation device for magnetic plate material has a gap G
The change in the attraction force F of the attraction electromagnet 11 with respect to the change in , is very large, and if magnetic saturation and magnetic leakage are ignored, with constant excitation, it changes in inverse proportion to the square of the gap G3. There is a drawback that it is troublesome to control the suction force Fc to follow the change in G3.

また、従来の磁性板材用磁気浮上装置は、磁性板材が薄
い場合または広い場合には、その弾力性のため自重によ
りたわむという欠点がある。
Furthermore, conventional magnetic levitation devices for magnetic plates have the disadvantage that when the magnetic plates are thin or wide, they bend due to their own weight due to their elasticity.

本発明の目的は、磁性板材に対する磁石の吸引力の制御
を必要とせず、かつ、磁性板材のたわみを防止すること
ができる磁性板材用磁気浮上装置を提供することにある
SUMMARY OF THE INVENTION An object of the present invention is to provide a magnetic levitation device for a magnetic plate that does not require control of the attractive force of a magnet to the magnetic plate and can prevent the magnetic plate from deflecting.

[課題を解決するための手段] 本発明は、平面がほぼ水平になるように配置された磁性
板材の端部の上側に所定間隔をおいて配置された上側磁
石と、前記磁性板材の端部の水平方向側に所定間隔をお
いて配置された水平方向側磁石とを具備する。
[Means for Solving the Problems] The present invention provides an upper magnet disposed at a predetermined interval above an end of a magnetic plate arranged so that its plane is substantially horizontal; horizontal direction side magnets arranged at predetermined intervals on the horizontal direction side.

[作用] 本発明は、上側磁石が磁性板材を重力に抗して平面がほ
ぼ水平になるように支持し、かつ水平方向側磁石が磁性
板材のたわみを防止する。
[Function] According to the present invention, the upper magnet supports the magnetic plate material against gravity so that the plane becomes substantially horizontal, and the horizontal magnet prevents the magnetic plate material from deflecting.

[実施例] 次に本発明の一実施例を図面に基づいて詳細に説明する
[Example] Next, an example of the present invention will be described in detail based on the drawings.

第1図において、符号1は磁性板材を示している。この
磁性板材1はその平面1aがほぼ水平になるように配置
される。この磁性板材1の両側の端部1b、lbの上側
には、それぞれ所定のギャップG、をおいて上側磁石2
,2が配置されている。これらの上側磁石2,2は1図
示した実施例においては、コア2aとコイル2bからな
る電磁石で構成されている。
In FIG. 1, reference numeral 1 indicates a magnetic plate material. This magnetic plate 1 is arranged so that its plane 1a is substantially horizontal. A predetermined gap G is provided above the ends 1b and lb on both sides of the magnetic plate 1, and the upper magnet 2
, 2 are arranged. In the embodiment shown in FIG. 1, these upper magnets 2, 2 are constituted by electromagnets consisting of a core 2a and a coil 2b.

前記磁性板材1の両側の端部1b、lbの水平方向側に
は、それぞれ所定のギャップG2をおいて水平方向側磁
石3.3が配置されている。これらの水平方向側磁石3
,3は2図示した実施例においてはコア3aとコイル3
bからなる電磁石で構成されている。これらの水平方向
側磁石3,3のコア3a、3aは、前記上側磁石2,2
のコア2a、2aと連設されている。前記コイル2b。
Horizontal magnets 3.3 are arranged on the horizontal sides of both end portions 1b, 1b of the magnetic plate 1, with a predetermined gap G2 therebetween. These horizontal side magnets 3
, 3 is 2 In the illustrated embodiment, the core 3a and the coil 3
It consists of an electromagnet consisting of b. The cores 3a, 3a of these horizontal side magnets 3, 3 are connected to the upper side magnets 2, 2.
The cores 2a, 2a are connected to each other. The coil 2b.

3bに電流が供給されると、磁束がコア2aから出てギ
ャップG1を通って磁性板材1に入り1次にギャップG
2を通ってコア3aに入り1次にコア2aへ戻る磁気回
路が構成される。
When a current is supplied to 3b, magnetic flux exits the core 2a, passes through the gap G1, enters the magnetic plate 1, and enters the primary gap G.
A magnetic circuit is constructed which enters the core 3a through the core 2 and then returns to the core 2a.

この磁気回路が構成されると、前記上側磁石2゜2は、
磁性板材1を垂直方向へ吸引力F、で上へ吸引して磁性
板材1を所定範囲内に平面1aがほぼ水平になるように
磁性板材1に接触しないで重力に抗して支持し、かつ、
前記水平方向側磁石3゜3は、磁性板材1の端部1b、
lbを吸引力F。
When this magnetic circuit is configured, the upper magnet 2゜2
Attract the magnetic plate 1 upward in the vertical direction with an attractive force F, and support the magnetic plate 1 within a predetermined range against gravity without contacting the magnetic plate 1 so that the plane 1a is almost horizontal, and ,
The horizontal side magnet 3°3 is located at the end 1b of the magnetic plate 1,
lb is the suction force F.

で吸引して磁性板材1のたわみを防止する。to prevent the magnetic plate material 1 from deflecting.

前記ギャップG1は、上側磁石2.2による磁性板材1
の上下方向への位置変化を許容する範囲に設定される。
The gap G1 is formed by the magnetic plate 1 formed by the upper magnet 2.2.
It is set within a range that allows vertical position changes.

また、前記ギャップG2を介して磁性板材1の端部1b
、lbの端面に臨む水平方向側磁石3,3のコア3a、
3aの端面は、磁性板材1の厚みに対応した対向面積に
絞られており。
Also, the end portion 1b of the magnetic plate material 1 is inserted through the gap G2.
, the core 3a of the horizontal side magnets 3, 3 facing the end face of lb,
The end faces of 3a are narrowed down to a facing area corresponding to the thickness of the magnetic plate 1.

これにより、ギャップG2における磁束密度を高くして
、磁性板材1に対する水平方向側磁石3゜3の吸引力F
、の増大を図っている。
As a result, the magnetic flux density in the gap G2 is increased, and the attractive force F of the horizontal magnet 3°3 to the magnetic plate 1 is increased.
We are trying to increase the number of people.

前記磁性板材1のたわみを防止することができる理由を
詳細に説明する。
The reason why the deflection of the magnetic plate 1 can be prevented will be explained in detail.

前記磁性板材1の端面の中心が水方向側磁石3゜3のコ
ア3a、3aの端面(磁極)の中心と同一レベルにある
場合(磁性板材1のレベルが0である場合)には磁性板
材1に対して水平方向側磁石3.3の吸引力F、は水平
方向へ作用するので。
When the center of the end surface of the magnetic plate 1 is on the same level as the center of the end surface (magnetic pole) of the cores 3a, 3a of the water direction magnet 3°3 (when the level of the magnetic plate 1 is 0), the magnetic plate 1, the attraction force F of the horizontal side magnet 3.3 acts in the horizontal direction.

垂直方向への分力はOである。The component force in the vertical direction is O.

前記磁性板材1が第2図の実線で示すように水平方向側
磁石3と同一レベルより距離りだけ下がった場合(磁性
板材1のレベルが−Lである場合)には、磁性板材1に
対して水平方向側磁石3の吸引力F、は水平線とθの角
度をなす上方斜め方向へ作用するため、第3図に示すよ
うな上方向分力F、(Fv−F、X5lnθ)が発生す
る。
When the magnetic plate 1 is lowered by a distance from the same level as the horizontal magnet 3 (when the level of the magnetic plate 1 is −L), as shown by the solid line in FIG. Since the attractive force F of the horizontal side magnet 3 acts in an upward diagonal direction forming an angle θ with the horizontal line, an upward component force F, (Fv-F, X5lnθ) as shown in Fig. 3 is generated. .

反対に、第2図小−点鎖線で示す゛うに、磁性板材1の
レベルが水平方向側磁石3のレベルより距離りだけ上が
った場合(磁性板材1のレベルが+Lである場合)には
、第3図に示すように下方向分力Fv  (F、−−F
a xsinθ)が発生する。
On the other hand, as shown by the small-dotted chain line in FIG. 2, when the level of the magnetic plate 1 is higher than the level of the horizontal magnet 3 by a distance (when the level of the magnetic plate 1 is +L), As shown in Fig. 3, downward component force Fv (F, -F
a xsinθ) occurs.

前記上側磁石2の磁性板材1に対する吸引力F、は常に
上方へのみ作用する。
The attractive force F of the upper magnet 2 against the magnetic plate 1 always acts only upward.

今、磁気飽和や磁気漏洩を無視し、磁性板材1を通って
上側磁石2および水平方向側磁石3を通る有効磁束数を
Φとし、かつ、水平方向側磁石3および上側磁石2の有
効対向面積をそれぞれAg1.Ag2とすると。
Now, ignoring magnetic saturation and magnetic leakage, let Φ be the effective number of magnetic flux passing through the magnetic plate 1 and passing through the upper magnet 2 and the horizontal magnet 3, and the effective opposing area of the horizontal magnet 3 and the upper magnet 2. respectively Ag1. If it is Ag2.

となり、F、、F、はΦの2乗に比例し、かつ。So, F,, F, is proportional to the square of Φ, and.

Ag+、Ag2に反比例する。It is inversely proportional to Ag+ and Ag2.

前記(1)および(2〉式の関係から、第3図に示すよ
うにF、が上方向へ作用する場合のθを+とし、かつ、
F、が下方向へ作用する場合のθを−とすると、磁性板
材1の一端部に作用する合計支持力Fは1次の式で表わ
れる。
From the relationship of equations (1) and (2> above, as shown in FIG. 3, when F acts upward, θ is +, and
If θ is - when F acts downward, the total supporting force F acting on one end of the magnetic plate 1 is expressed by the following equation.

したがって1合計支持力FはAg+、Ag2の値を選ぶ
ことにより、第4図の曲線A、Bで囲む範囲内(斜線で
示す範囲内)の曲線で示す値とすることができるから、
磁性板材1の端部1b、1bが水平方向側磁石3の中心
と対応したレベルに配置されるように、すなわち、磁性
板材1がたわむのを防止するように、水平方向側磁石3
は磁性板材1に復元力を作用させる。
Therefore, by selecting the values of Ag+ and Ag2, the total supporting force F can be set to the value shown by the curve within the range surrounded by curves A and B in Fig. 4 (within the shaded range).
The horizontal side magnet 3 is arranged so that the ends 1b, 1b of the magnetic plate 1 are arranged at a level corresponding to the center of the horizontal side magnet 3, that is, so as to prevent the magnetic plate 1 from bending.
causes a restoring force to act on the magnetic plate 1.

なお、第4図の曲線Cは第5図に示す従来の磁性板材用
磁気浮上装置における磁性板材1に作用する合計支持力
Fを示すものであり、従来の磁性板材用浮上装置は磁性
板材1を基準レベルに復元する力が得られないことが曲
線Cにより示されている。
Note that the curve C in FIG. 4 indicates the total supporting force F acting on the magnetic plate 1 in the conventional magnetic levitation device for magnetic plates shown in FIG. Curve C shows that no force is available to restore the voltage to the reference level.

第3図に示すように前記水平方向側磁石3の磁性板材1
に対する吸引力F、は常に水平方向分力F、を有し、こ
の水平方向分力F、も磁性板材1のたわみを防止する。
As shown in FIG. 3, the magnetic plate 1 of the horizontal side magnet 3
The attractive force F on the magnetic plate always has a horizontal component F, and this horizontal component F also prevents the magnetic plate 1 from deflecting.

なお、前記上側磁石2のコイル2aおよび水平方向側磁
石3のコイル3aへ供給する電流の大きさを制御して、
磁性板材1に対する吸引力の制御を必要としない。した
がって、上側磁石2のコア2aと水平方向側磁石3のコ
ア3bとを連設しなくてもよく、かつ、上側磁石2およ
び水平方向側磁石3は永久磁石で構成することもできる
Note that by controlling the magnitude of the current supplied to the coil 2a of the upper magnet 2 and the coil 3a of the horizontal magnet 3,
There is no need to control the attraction force to the magnetic plate 1. Therefore, it is not necessary to connect the core 2a of the upper magnet 2 and the core 3b of the horizontal magnet 3, and the upper magnet 2 and the horizontal magnet 3 may be made of permanent magnets.

[発明の効果コ 本発明は、磁性板材に対する磁石の吸引力の制御を必要
とせず、かつ、磁性板材のたわみを防止することができ
る。
[Effects of the Invention] The present invention does not require control of the attraction force of the magnet to the magnetic plate, and can prevent the magnetic plate from deflecting.

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

第1図は本発明の一実施例を示す概略図、第2めの図並
びに第5図は従来の磁性板材用磁気浮上装置を示す概略
図である。 ・・・磁性板材。 2・・・上側磁石。 3・・・水平方向側 磁石。 第2図 2 第 図 第4図 中L 磁性板材のレベル L 第 図 3
FIG. 1 is a schematic diagram showing an embodiment of the present invention, and the second diagram and FIG. 5 are schematic diagrams showing a conventional magnetic levitation device for magnetic plate material. ...Magnetic plate material. 2... Upper magnet. 3...Horizontal side magnet. Figure 2 2 L in Figure 4 Level of magnetic plate L Figure 3

Claims (1)

【特許請求の範囲】[Claims] (1)平面がほぼ水平になるように配置された磁性板材
の端部の上側に所定間隔をおいて配置された上側磁石と
,前記磁性板材の端部の水平方向側に所定間隔をおいて
配置された水平方向側磁石とを具備することを特徴とす
る磁性板材用磁気浮上装置。
(1) An upper magnet placed at a predetermined interval above the end of a magnetic plate arranged so that its plane is almost horizontal, and an upper magnet placed at a predetermined interval above the end of the magnetic plate in the horizontal direction. What is claimed is: 1. A magnetic levitation device for magnetic plate material, comprising: a horizontal side magnet arranged therein.
JP19691789A 1989-07-31 1989-07-31 Magnetic levitation apparatus for magnetic plate Granted JPH0362504A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19691789A JPH0362504A (en) 1989-07-31 1989-07-31 Magnetic levitation apparatus for magnetic plate

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19691789A JPH0362504A (en) 1989-07-31 1989-07-31 Magnetic levitation apparatus for magnetic plate

Publications (2)

Publication Number Publication Date
JPH0362504A true JPH0362504A (en) 1991-03-18
JPH0529285B2 JPH0529285B2 (en) 1993-04-30

Family

ID=16365814

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19691789A Granted JPH0362504A (en) 1989-07-31 1989-07-31 Magnetic levitation apparatus for magnetic plate

Country Status (1)

Country Link
JP (1) JPH0362504A (en)

Also Published As

Publication number Publication date
JPH0529285B2 (en) 1993-04-30

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