JPH1125817A - Electromagnetic repulsion mechanism for switch - Google Patents

Electromagnetic repulsion mechanism for switch

Info

Publication number
JPH1125817A
JPH1125817A JP17966597A JP17966597A JPH1125817A JP H1125817 A JPH1125817 A JP H1125817A JP 17966597 A JP17966597 A JP 17966597A JP 17966597 A JP17966597 A JP 17966597A JP H1125817 A JPH1125817 A JP H1125817A
Authority
JP
Japan
Prior art keywords
repulsion
coil
plate
electromagnetic
switch
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.)
Pending
Application number
JP17966597A
Other languages
Japanese (ja)
Inventor
Yuichi Yamaji
祐一 山地
Toshimasa Maruyama
稔正 丸山
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP17966597A priority Critical patent/JPH1125817A/en
Publication of JPH1125817A publication Critical patent/JPH1125817A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01HELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
    • H01H33/00High-tension or heavy-current switches with arc-extinguishing or arc-preventing means
    • H01H33/02Details
    • H01H33/28Power arrangements internal to the switch for operating the driving mechanism
    • H01H33/285Power arrangements internal to the switch for operating the driving mechanism using electro-dynamic repulsion
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01HELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
    • H01H33/00High-tension or heavy-current switches with arc-extinguishing or arc-preventing means
    • H01H33/60Switches wherein the means for extinguishing or preventing the arc do not include separate means for obtaining or increasing flow of arc-extinguishing fluid
    • H01H33/66Vacuum switches
    • H01H33/666Operating arrangements

Landscapes

  • Driving Mechanisms And Operating Circuits Of Arc-Extinguishing High-Tension Switches (AREA)

Abstract

PROBLEM TO BE SOLVED: To obtain larger repulsion with a smaller, lighter repulsive plate without making a power supply larger by composing this electromagnetic repulsion mechanism out of a repulsive coil and a thin repulsive plate fixed on a movable rod opposite to the coil surface and by setting the resonance frequency of a resonant circuit which is composed of an inductance of the coil and the capacitance of a capacitor with in a specific range. SOLUTION: This electromagnetic repulsion mechanism 48 is produced so as to comprise a switch frame 50, a switch movable rod 1A and a repulsive coil 22 fixed on the frame 50, and the repulsive coil 22 is so formed as to have an inductance having a resonance frequency set by the aid of a capacitor in a power supply in the range of 500 Hz or gher to 2000 Hz or lower. A thin repulsive plate 23 made of a thin copper plate is fixed on the movable rod 1A opposite to the coil surface of the repulsive coil 22 and has a thickness ranging from 2 to 6 mm, so as to have the same thickness as the effective depth of eddy current corresponding to frequencies from 500 to 2000 Hz. A reinforcing plate 13 is made of a light non-magnetic material and reinforces the thin repulsive plate 23.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】この発明は開閉器の接点を駆
動する機構に関するもので、特に、開極速度の向上に関
するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a mechanism for driving a contact of a switch, and more particularly to an improvement in an opening speed.

【0002】[0002]

【従来の技術】開閉器として、ここでは真空遮断器を用
いて説明を行う。一般に開閉器はその接点を開くときに
は、出来るだけ素速く開くことが要求される。そうする
ことがアークによる接点の損耗を減らし、開閉器として
の性能の向上につながるからである。接点を素早く開く
ための駆動源としては、古くからスプリングが用いられ
てきたが、最近ではスプリングに加えていわゆる電磁反
発機構が併用されたものがある。図12は特公平7−6
0624号公報に示されたものと類似の電磁反発機構を
装備した開閉器の全体概要図である。
2. Description of the Related Art Here, a description will be given using a vacuum circuit breaker as a switch. In general, a switch is required to open its contacts as quickly as possible. This is because doing so reduces the wear of the contacts due to the arc and leads to an improvement in the performance as a switch. As a driving source for quickly opening the contact, a spring has been used for a long time. Recently, however, a so-called electromagnetic repulsion mechanism has been used in addition to the spring. Figure 12 shows Tokuhei 7-6
FIG. 1 is an overall schematic view of a switch equipped with an electromagnetic repulsion mechanism similar to that shown in Japanese Patent No. 0624.

【0003】図12において50はこの開閉器のフレー
ムである。1は接離可能な主接点(可動接点)を有する
真空バルブ、1Aは真空バルブ1の主接点(図示しな
い)を駆動する可動ロッド、2はフレーム50に固定さ
れた反発コイル、3は可動ロッド1Aに固着され前記反
発コイル2に接近して設けられている反発板、4は主接
点に接触圧を与える投入(接圧)ばね、5は可動ロッド
1Aを駆動するための駆動機構である。駆動機構5は図
示しない開極保持機構、投入機構等で構成されている
が、この発明の説明上詳しい説明は必要ないので詳細な
説明は省略する。
In FIG. 12, reference numeral 50 denotes a frame of the switch. Reference numeral 1 denotes a vacuum valve having a detachable main contact (movable contact), 1A denotes a movable rod for driving a main contact (not shown) of the vacuum valve 1, 2 denotes a repulsion coil fixed to a frame 50, and 3 denotes a movable rod. A repulsion plate fixed to 1A and provided close to the repulsion coil 2 is a closing (contact pressure) spring for applying a contact pressure to the main contact, and a driving mechanism 5 for driving the movable rod 1A. The drive mechanism 5 includes an opening holding mechanism, a closing mechanism, and the like (not shown). However, detailed description is not necessary for the description of the present invention, and thus detailed description is omitted.

【0004】図13は反発コイル2に接続する電磁反発
用電源49の回路図である。電磁反発用電源49はフレ
ーム50内に収納されている場合もあれば、外部に設置
されている場合もあるが、どちらにしてもこの発明の説
明上収納位置は関係がない。反発コイル2と反発板3と
電磁反発用電源49は電磁反発機構6を構成している。
電磁反発用電源49は充電用交流電源7、この交流電源
7に直列に接続された充電抵抗8、更に直列に接続され
たダイオード9、ダイオード9の出力側で電源7に並列
に接続されたコンデンサ10、ダイオード9に直列に接
続されたスイッチ11で構成されており、充電用交流電
源7によりコンデンサ10に直流を充電し、スイッチ1
1がONすることで反発コイル2にコンデンサ10から
電流を放電する。
FIG. 13 is a circuit diagram of a power supply 49 for electromagnetic repulsion connected to the repulsion coil 2. The power supply 49 for electromagnetic repulsion may be housed in the frame 50 or may be installed outside, but in any case, the housing position is irrelevant for the description of the present invention. The repulsion coil 2, the repulsion plate 3, and the power supply 49 for electromagnetic repulsion constitute an electromagnetic repulsion mechanism 6.
The power supply 49 for electromagnetic repulsion includes an AC power supply 7 for charging, a charging resistor 8 connected in series to the AC power supply 7, a diode 9 connected in series, and a capacitor connected in parallel to the power supply 7 on the output side of the diode 9. 10, a switch 11 connected in series with a diode 9. The DC power is supplied to the capacitor 10 by the charging AC power supply 7, and the switch 1
When 1 is turned on, current is discharged from the capacitor 10 to the repulsion coil 2.

【0005】次に電磁反発機構49を装備した開閉器の
開閉動作について説明する。図13の電源回路図におい
て、コンデンサ10は充電用交流電源7により一定電圧
に充電されている。開極動作の場合、外部から指令され
る開極信号により、スイッチ11がONとなり、コンデ
ンサ10から反発コイル2にパルス的なコイル電流が流
れる。この時のコイル電流波形の一例を図14に示す。
スイッチ11が閉じるとコンデンサ10と反発コイル2
とで並列共振回路が構成されるので、電流は図示のよう
に振動的になるが、その周波数fはコンデンサ10の容
量Cと、反発コイル2のインダクタンスL及びその直流
抵抗Rとから f=1/〔2π{(R/2L)2−(1/LC)}1/2〕 となることは周知である。
Next, the opening / closing operation of the switch equipped with the electromagnetic repulsion mechanism 49 will be described. In the power supply circuit diagram of FIG. 13, the capacitor 10 is charged to a constant voltage by the charging AC power supply 7. In the case of the opening operation, the switch 11 is turned on by an opening signal instructed from the outside, and a pulse-like coil current flows from the capacitor 10 to the repulsion coil 2. FIG. 14 shows an example of the coil current waveform at this time.
When the switch 11 is closed, the capacitor 10 and the repulsion coil 2
, The current becomes oscillating as shown in the figure, but its frequency f is determined by the capacitance C of the capacitor 10, the inductance L of the repulsion coil 2 and its DC resistance R, f = 1 / [2π {(R / 2L) 2- (1 / LC)} 1/2 ].

【0006】この振動電流によって高周波磁界が発生
し、その高周波磁界によって反発板3には渦電流が誘起
される。この高周波磁界と渦電流との相互作用により反
発コイル2と反発板3の間に、電磁反発力が発生する。
この電磁反発力によって反発板3が図12の下方に押下
げられ、接点が瞬時に開極する。なお、開極位置に達す
ると接点11が開くと共に図示しない開極保持機構によ
って、真空バルブ1の接点は開極状態を保持する。
A high-frequency magnetic field is generated by the oscillating current, and an eddy current is induced in the repulsion plate 3 by the high-frequency magnetic field. Due to the interaction between the high-frequency magnetic field and the eddy current, an electromagnetic repulsion is generated between the repulsion coil 2 and the repulsion plate 3.
The repulsion plate 3 is pushed down in FIG. 12 by this electromagnetic repulsion, and the contacts are instantaneously opened. When the contact position is reached, the contact 11 is opened and the contact of the vacuum valve 1 is kept in the open state by an opening holding mechanism (not shown).

【0007】閉極動作の場合、図示しない投入機構によ
り開極保持を外し、開極時に圧縮している投入(接圧)
ばね4により反発板3とともに可動ロッド1Aは閉極方
向(図12の上方)に動作し、可動ロッド1Aに接続し
ている真空バルブ1が閉極する。
In the closing operation, the opening is not held by an opening mechanism (not shown), and the opening (contact pressure) is compressed during opening.
The movable rod 1A moves together with the repulsion plate 3 in the closing direction (upward in FIG. 12) by the spring 4, and the vacuum valve 1 connected to the movable rod 1A is closed.

【0008】[0008]

【発明が解決しようとする課題】真空バルブの接点の開
く速さを早くするためには、反発コイルと反発板との間
に働く反発力は出来るだけ大きくしたい。発生する電磁
反発力は電源電圧に大きく依存している。電源電圧を高
くすれば電磁反発力は大きくすることができるが、電源
電圧を高くするためには、コンデンサ10が大きくな
り、電源装置全体の寸法も大きくなる。また、反発コイ
ルや反発板の形状をある程度大きくすることも有効だ
が、大きさは装置の形状により制約される。実際真に必
要なのは力ではなく接点の加速度であるから、電源電圧
や反発板の寸法を大きくすることなしに、出来るだけ小
さな反発板でより大きい反発力を得る方法で加速度を大
きくしたいというのが課題である。また,反発コイルに
流れるコイル電流は振動し、それに伴って電磁反発力も
振動して山、谷が繰返し現れるので、開極時間の長さに
丁度電磁反発力の谷が当るような場合には、電磁反発力
を効率よく利用することができない。
In order to increase the speed at which the contacts of the vacuum valve open, it is desirable to increase the repulsive force acting between the repulsion coil and the repulsion plate as much as possible. The generated electromagnetic repulsion greatly depends on the power supply voltage. The electromagnetic repulsion can be increased by increasing the power supply voltage. However, in order to increase the power supply voltage, the size of the capacitor 10 is increased, and the size of the entire power supply device is also increased. It is also effective to increase the shape of the repulsion coil and the repulsion plate to some extent, but the size is limited by the shape of the device. In fact, what is really needed is not the force but the acceleration of the contacts.Therefore, without increasing the power supply voltage or the size of the repulsion plate, it is desirable to increase the acceleration by using a smaller repulsion plate to obtain a larger repulsion force. It is an issue. In addition, the coil current flowing through the repulsion coil oscillates, and the electromagnetic repulsion also oscillates, and peaks and valleys appear repeatedly. Therefore, when the valley of the electromagnetic repulsion just hits the length of the opening time, Electromagnetic repulsion cannot be used efficiently.

【0009】この発明は上記のような問題点を解決する
ためになされたもので、電源を大型化することなく、よ
り小さく軽い反発板でより大きい反発力を得ることが出
来る電磁反発機構を得ようとするものである。また、コ
イル電流の振動つまり電磁反発力の振動を抑え、電磁反
発力を効率よく利用できる電磁反発機構を得ようとする
ものである。
SUMMARY OF THE INVENTION The present invention has been made to solve the above-mentioned problems, and an electromagnetic repulsion mechanism capable of obtaining a larger repulsion force with a smaller and lighter repulsion plate without increasing the size of a power supply. It is to try. Another object of the present invention is to provide an electromagnetic repulsion mechanism that suppresses the vibration of the coil current, that is, the vibration of the electromagnetic repulsion, and can efficiently use the electromagnetic repulsion.

【0010】[0010]

【課題を解決するための手段】この発明による電磁反発
機構は、フレームに固定され接離可能な可動接点を有す
る真空バルブと、前記可動接点に接続された可動ロッド
とを有する開閉器に用いられ、前記可動ロッドを駆動す
る電磁反発機構であって、前記可動ロッドの周囲で前記
フレームに固定された反発コイルと、前記反発コイルの
コイル面に対応して前記可動ロッドに固着された薄板反
発板と、直流電圧を保持するコンデンサを有する電源と
を含み、前記コイルのインダクタンスと前記コンデンサ
の容量とで構成される共振回路の共振周波数が500H
Z以上2KHZ以下としたものである。共振周波数を高
くすることは、表皮効果によって渦電流が反発コイルに
近い表面に集中して発生するので、反発コイルと渦電流
との距離が近くなり、反発力が大きくなると言う作用を
生む。
An electromagnetic repulsion mechanism according to the present invention is used in a switch having a vacuum valve having a movable contact fixed to and detachable from a frame and a movable rod connected to the movable contact. An electromagnetic repulsion mechanism for driving the movable rod, a repulsion coil fixed to the frame around the movable rod, and a thin plate repulsion plate fixed to the movable rod corresponding to a coil surface of the repulsion coil And a power supply having a capacitor for holding a DC voltage, wherein the resonance frequency of the resonance circuit formed by the inductance of the coil and the capacitance of the capacitor is 500H.
It is Z or more and 2 KHZ or less. Increasing the resonance frequency produces an effect that the eddy current is concentrated on the surface near the repulsion coil due to the skin effect, so that the distance between the repulsion coil and the eddy current is short and the repulsion force is increased.

【0011】また、この発明による電磁反発機構は、薄
板反発板が2〜6mmの厚みの銅板と、この銅板を支え
るプラスティック又は非磁性金属からなる補強板とで構
成されているものである。周波数を高くしたことによる
表皮効果によって、渦電流が表面に集中して流れる結
果、反発板を薄くしても渦電流の値は小さくならず、そ
の分軽量化されるので、加速度が大きくなると言う作用
を生む。
The electromagnetic repulsion mechanism according to the present invention is such that the thin plate repulsion plate is composed of a copper plate having a thickness of 2 to 6 mm and a reinforcing plate made of a plastic or non-magnetic metal for supporting the copper plate. According to the skin effect caused by the higher frequency, the eddy current flows intensively on the surface.As a result, the value of the eddy current does not decrease even if the rebound plate is thinned, and the weight is reduced accordingly, so the acceleration increases. Produce action.

【0012】また、この発明による電磁反発機構は、補
強板がその外周に近い部分の厚みが内周に近い部分の厚
みより薄いテーパ構造を有するものである。テーパ状と
した補強板は軽量化され加速度を高くすると言う作用を
生む。
Further, in the electromagnetic repulsion mechanism according to the present invention, the reinforcing plate has a tapered structure in which the thickness of the portion near the outer periphery is smaller than the thickness of the portion near the inner periphery. The tapered reinforcing plate has the effect of reducing weight and increasing acceleration.

【0013】また、反発コイルは逆並列に接続されたダ
イオードを有するものである。ダイオードは並列共振回
路の振動電流を直流電流に変え、電磁反発力が効率よく
利用されるようにするという作用を生む。
The repulsion coil has a diode connected in anti-parallel. The diode produces an effect of converting the oscillating current of the parallel resonance circuit into a direct current, so that the electromagnetic repulsion is used efficiently.

【0014】また、反発コイルを取付けたフレームは、
前記反発コイルの巻き線に直交するスリットを有するも
のである。フレーム側のスリットは、フレーム側の無駄
な渦電流を減少させ反発板に生じる渦電流が大きくな
り、反発力が強くなると言う作用を生む。
The frame on which the repulsion coil is mounted is
It has a slit orthogonal to the winding of the repulsion coil. The slit on the frame side produces an effect that wasteful eddy current on the frame side is reduced, the eddy current generated in the repulsion plate is increased, and the repulsion force is increased.

【0015】[0015]

【発明の実施の形態】BEST MODE FOR CARRYING OUT THE INVENTION

実施の形態1.図1はこの発明の実施の形態1による電
磁反発機構48をしめすものである。この発明の電磁反
発機構48を装備した開閉器の電磁反発機構48以外の
部分の構成は従来のものと同じなので詳細な説明は省略
する。図1において、50は開閉器のフレーム、1Aは
開閉器の可動ロッド、22はフレーム50に固定された
反発コイルで後述する電源(図6に示す)のコンデンサ
20との共振周波数が500HZ以上2000HZ以下
になるようなインダクタンスを持つように製作されてい
る。23は薄い銅板で製作された薄板反発板で、前記反
発コイル22のコイル面に対応して可動ロッド1Aに固
着され、上記500〜2000HZの渦電流の有効深さ
の厚みを有するように、例えば6〜2mmの厚みになっ
ている。13は薄板反発板23に掛る反発力を可動ロッ
ドに伝達するための補強板であり非磁性材で製作され、
かつ、出来るだけ軽量化された形状になっている。電磁
反発機構48は反発コイル22と薄板反発板23と後述
する電磁反発用電源47(以下電源という場合もある)
で構成されている。
Embodiment 1 FIG. FIG. 1 shows an electromagnetic repulsion mechanism 48 according to Embodiment 1 of the present invention. Since the configuration of the portion of the switch equipped with the electromagnetic repulsion mechanism 48 of the present invention other than the electromagnetic repulsion mechanism 48 is the same as that of the conventional one, detailed description will be omitted. In FIG. 1, reference numeral 50 denotes a frame of a switch, 1A denotes a movable rod of the switch, 22 denotes a repulsion coil fixed to the frame 50, and has a resonance frequency with a capacitor 20 of a power source (shown in FIG. It is manufactured to have the following inductance. Reference numeral 23 denotes a thin sheet repulsion plate made of a thin copper plate, which is fixed to the movable rod 1A corresponding to the coil surface of the repulsion coil 22 so as to have a thickness of the effective depth of the eddy current of 500 to 2000 HZ, for example. The thickness is 6 to 2 mm. Reference numeral 13 denotes a reinforcing plate for transmitting a repulsive force applied to the thin plate repulsion plate 23 to the movable rod, and is made of a non-magnetic material.
In addition, the shape is as light as possible. The electromagnetic repulsion mechanism 48 includes a repulsion coil 22, a thin plate repulsion plate 23, and a power supply 47 for electromagnetic repulsion described below (hereinafter, also referred to as a power supply).
It is composed of

【0016】図2は同一の構造寸法を有する電磁反発機
構48において、振動電流の周波数と発生する反発力と
の関係を示すものである。この図は各周波数でのコイル
電流のピーク値が、周波数が60Hzのときのコイル電
流のピーク値と同じになるようにして、そのコイル電流
により発生する電磁反発力を周波数60Hzの時を1と
して比例的に縦軸に示している。周波数を高くすればす
るほど、表皮効果により薄板反発板23に誘起される渦
電流は反発コイル22に対向する薄板反発板23の表面
付近に分布し、相対的に反発コイル22と渦電流との距
離が近づくため、電磁反発力は周波数60Hzの場合よ
りも大きくなる。
FIG. 2 shows the relationship between the frequency of the oscillating current and the generated repulsive force in the electromagnetic repulsion mechanism 48 having the same structural dimensions. In this figure, the peak value of the coil current at each frequency is set to be the same as the peak value of the coil current when the frequency is 60 Hz, and the electromagnetic repulsion generated by the coil current is set to 1 when the frequency is 60 Hz. The vertical axis is proportionally shown. As the frequency is increased, the eddy current induced in the thin plate repulsion plate 23 due to the skin effect is distributed near the surface of the thin plate repulsion plate 23 facing the repulsion coil 22, and the eddy current between the repulsion coil 22 and the eddy current is relatively increased. Since the distance is reduced, the electromagnetic repulsion becomes larger than when the frequency is 60 Hz.

【0017】これを図3に示す。図3は縦軸が薄板反発
板23の厚み方向の距離を示し、上部がコイル22に近
い側、図の下方がコイル22の反対側である。横軸は薄
板反発板23の内部を流れる電流の密度を比例的に示す
ものである。薄板反発板23の厚みは表皮効果によって
表面付近に集中した電流の厚みさえあれば十分であるか
ら、低い周波数の時よりも高い周波数のときの方が、相
対的に薄くすることが出来る。
This is shown in FIG. In FIG. 3, the vertical axis indicates the distance in the thickness direction of the thin plate repulsion plate 23, the upper side is the side closer to the coil 22, and the lower side of the figure is the opposite side to the coil 22. The horizontal axis indicates the density of the current flowing inside the thin plate repulsion plate 23 in proportion. The thickness of the thin repulsion plate 23 is sufficient if the thickness of the current concentrated near the surface due to the skin effect is sufficient, so that it can be made relatively thinner at higher frequencies than at lower frequencies.

【0018】図2中に点線で示すように、コイル電流の
周波数が500Hz付近以上では効果が飽和してくるこ
とと、薄板反発板23がある程度より薄くなつても製作
する上でメリットがなく、また、あまり高くしすぎると
見かけ上、渦電流の流れる部分の抵抗が高くなって渦電
流が減少するので、500〜2000HZの周波数を選
択するのがよい。500HZでも、薄板反発板23の厚
みを6mm以下とすることができ、コイル電流により誘
起される渦電流を十分に利用でき、接点の開極時間をた
とえば1ms以下にもすることができる。薄板反発板2
3は薄く、機械的強度が低いのでそのままでは渦電流に
よる反発力を可動ロッド1Aに伝えることが出来ない。
そこでその下に取り付けた補強板13で電磁反発力に対
する強度を持たせている。図4に補強板13の裏面斜視
図を示す。この補強板13は磁界に影響のないようにプ
ラスティック又は非磁性材料を用い、かつ軽量化するた
めに図に示すような適当なスチフナ(梁)を設ける。
As shown by the dotted line in FIG. 2, the effect becomes saturated when the frequency of the coil current is around 500 Hz or higher, and there is no merit in manufacturing even if the thin plate repulsion plate 23 becomes thinner to some extent. On the other hand, if it is too high, apparently the resistance of the portion where the eddy current flows increases and the eddy current decreases, so that a frequency of 500 to 2000 Hz is preferably selected. Even at 500 Hz, the thickness of the thin plate repulsion plate 23 can be made 6 mm or less, the eddy current induced by the coil current can be sufficiently utilized, and the contact opening time can be made 1 ms or less, for example. Thin rebound board 2
Since 3 is thin and has low mechanical strength, the repulsive force due to the eddy current cannot be transmitted to the movable rod 1A as it is.
Therefore, the reinforcing plate 13 attached thereunder has strength against electromagnetic repulsion. FIG. 4 shows a back perspective view of the reinforcing plate 13. The reinforcing plate 13 is made of a plastic or non-magnetic material so as not to affect the magnetic field, and is provided with a suitable stiffener (beam) as shown in the figure to reduce the weight.

【0019】図1の電磁反発機構48を用いた開閉器を
従来のものと比較するため図5に構成図を示す。図5に
おいて開閉器はフレーム50、真空バルブ1、駆動ロッ
ド1A、インダクタンスがL1で抵抗がR1の反発コイ
ル22、銅の薄い板で構成された薄板反発板23、薄板
反発板23を補強する非磁性材で作られた補強板13、
投入(接圧)ばね4、駆動機構5で構成されている。ま
た、図6は共振周波数が500HZ以上になるように設
計された電磁反発用電源47であり、充電用交流電源
7、充電抵抗8、ダイオード9、容量C1のコンデンサ
20、スイッチ11で構成されている。スイッチ11を
閉じたときに反発コイル22に流れる振動電流の周波数
は f=1/〔{2π(R1/2L1)2−(1/L1C
1)}1/2〕 である。
FIG. 5 shows a configuration diagram of a switch using the electromagnetic repulsion mechanism 48 of FIG. 1 in comparison with a conventional switch. In FIG. 5, the switch includes a frame 50, a vacuum valve 1, a driving rod 1A, a repulsion coil 22 having an inductance L1 and a resistance R1, a thin repulsion plate 23 made of a thin copper plate, and a non-reinforcing plate for reinforcing the thin repulsion plate 23. Reinforcing plate 13 made of magnetic material,
It comprises a closing (contact pressure) spring 4 and a drive mechanism 5. FIG. 6 shows an electromagnetic repulsion power supply 47 designed to have a resonance frequency of 500 HZ or more, and includes a charging AC power supply 7, a charging resistor 8, a diode 9, a capacitor 20 having a capacitance C1, and a switch 11. I have. The frequency of the oscillating current flowing through the repulsion coil 22 when the switch 11 is closed is f = 1 / [{2π (R1 / 2L1) 2 − (1 / L1C
1)} 1/2 ].

【0020】電磁反発機構として必要な電磁反発力は、
電源電圧一定の場合、反発コイル22とコンデンサ20
に依存している。反発コイル22の外形寸法は開閉器の
大きさによりある程度制約を受けるが、その制約の範囲
内で、コイルに使用する電線の太さとターン数の組合せ
を選ぶことにより、ある範囲内のインダクタンスを選択
することが出来る。また、コンデンサ22の容量も同じ
く外形的制約の範囲内で選択することが出来る。つま
り、周波数が高い時コンデンサ容量は小さく、周波数が
低い時コンデンサ容量は大きい。
The electromagnetic repulsion required as an electromagnetic repulsion mechanism is:
When the power supply voltage is constant, the repulsion coil 22 and the capacitor 20
Depends on. The external dimensions of the repulsion coil 22 are limited to some extent by the size of the switch, but within that limit, an inductance within a certain range is selected by selecting a combination of the wire thickness and the number of turns used for the coil. You can do it. Further, the capacity of the capacitor 22 can also be selected within the range of the external restrictions. That is, when the frequency is high, the capacitance is small, and when the frequency is low, the capacitance is large.

【0021】反発コイル22とコンデンサ20との組合
せにより、コイル電流の周波数を500Hz以上に設定
すると、コンデンサ容量を小さくできるとともに、薄板
反発板23に誘起される渦電流が表皮効果により反発コ
イル22に対向する反発板23の表面付近に分布し、相
対的に反発コイル22と反発板23との距離が近づくこ
とになるため、周波数60Hzの時の電磁反発力よりも
大きな電磁反発力を得る事ができる。さらに薄板反発板
23が薄く(軽く)できるため可動部分全体の質量が小
さくなり、加速度(接点の開く速度)が早くなる。
When the frequency of the coil current is set to 500 Hz or more by the combination of the repulsion coil 22 and the capacitor 20, the capacitance of the capacitor can be reduced, and the eddy current induced in the thin repulsion plate 23 is applied to the repulsion coil 22 by the skin effect. Since it is distributed near the surface of the opposing repulsion plate 23 and the distance between the repulsion coil 22 and the repulsion plate 23 becomes relatively small, it is possible to obtain an electromagnetic repulsion force larger than the electromagnetic repulsion force at the frequency of 60 Hz. it can. Further, since the thin plate repulsion plate 23 can be made thin (light), the mass of the entire movable part becomes small, and the acceleration (the speed at which the contacts open) increases.

【0022】実施の形態2.図7はこの発明の実施の他
の形態を示すものである。図に於いてRaは反発コイル
22のコイル巻き線の中心の平均半径(以下半径とい
う)を示している。Fは軸中心から距離rの位置に発生
する反発力を示している。図8は軸心からの距離rと電
磁反発力Fとの関係である。この図で電磁反発力Fは最
大値を1として比例的に表し、横軸は軸心からの距離r
とコイル平均半径との比で表わしている。この電磁反発
力Fの最大値はコイル半径の位置で発生し、このコイル
半径より外側に離れても内側に離れても、離れるほど電
磁反発力は小さくなる。薄板反発板23に掛る全ての力
は可動ロッド1Aと接続している部分に掛るので,薄板
反発板23の中心部には最も大きい曲げ応力が発生す
る。そのため反発板中心部には補強が必要である。一
方,コイル半径より外側では,電磁反発力は小さいため
補強板13の強度を小さく、即ち、厚さを薄くすること
ができる。従って,この電磁反発力に対して外周に近い
外側を補強板13aのようにテーパ状に薄くした構造と
することにより、可動部重量の軽量化を図ることがで
き,同じ電磁反発力でも更に加速度を高めることができ
る。
Embodiment 2 FIG. FIG. 7 shows another embodiment of the present invention. In the drawing, Ra indicates an average radius of the center of the coil winding of the repulsion coil 22 (hereinafter referred to as radius). F indicates a repulsive force generated at a distance r from the axis center. FIG. 8 shows the relationship between the distance r from the axis and the electromagnetic repulsion F. In this figure, the electromagnetic repulsion force F is proportionally represented with the maximum value as 1, and the horizontal axis is the distance r from the axis.
And the average radius of the coil. The maximum value of the electromagnetic repulsive force F occurs at the position of the coil radius, and the electromagnetic repulsive force decreases as the distance from the coil radius increases or decreases. Since all the force applied to the thin plate repulsion plate 23 is applied to the portion connected to the movable rod 1A, the largest bending stress is generated at the center of the thin plate repulsion plate 23. Therefore, reinforcement is required at the center of the repulsion plate. On the other hand, outside the coil radius, since the electromagnetic repulsion is small, the strength of the reinforcing plate 13 can be reduced, that is, the thickness can be reduced. Therefore, the weight of the movable portion can be reduced by forming a structure in which the outer portion close to the outer periphery is tapered and thin like the reinforcing plate 13a with respect to the electromagnetic repulsive force. Can be increased.

【0023】実施の形態3.図9はこの発明の他の実施
の形態を示す電磁反発用電源の回路図であり、反発コイ
ル22と逆並列にダイオード12を接続している。図2
の電磁反発用電源では振動しながら減衰するコイル電流
が流れる(図10の破線)。この場合、コイル電流が振
動することで電磁反発力も振動し、高速開極に必要なエ
ネルギーを得る事ができなかった。図9では、反発コイ
ル22と逆並列にダイオード12を接続することで、図
10の実線に示すようなコイル電流が流れる。このよう
なコイル電流を流すことにより,同じ充電電圧、同じコ
ンデンサ容量に対して、高速開極に必要なエネルギーを
より早く利用することできる。このような電流波形とし
た場合でも、電流の最初の立上がり時の周波数成分は前
述の式に示す高周波数となり、渦電流が表皮効果により
薄板反発板23の表面付近に集中すると言うことには変
りがない。
Embodiment 3 FIG. FIG. 9 is a circuit diagram of a power supply for electromagnetic repulsion according to another embodiment of the present invention, in which a diode 12 is connected in antiparallel with a repulsion coil 22. FIG.
In the power supply for electromagnetic repulsion, a coil current that attenuates while vibrating flows (broken line in FIG. 10). In this case, the coil current oscillates and the electromagnetic repulsion also oscillates, making it impossible to obtain the energy required for high-speed opening. In FIG. 9, by connecting the diode 12 in antiparallel with the repulsion coil 22, a coil current flows as shown by the solid line in FIG. By supplying such a coil current, the energy required for high-speed opening can be used more quickly for the same charging voltage and the same capacitor capacity. Even in the case of such a current waveform, the frequency component at the first rise of the current becomes the high frequency shown in the above-mentioned equation, and it can be said that the eddy current is concentrated near the surface of the thin repulsion plate 23 by the skin effect. There is no.

【0024】実施の形態4.図1において反発コイル2
2の電磁力は図の上方にも及ぶから、反発コイル22を
取付けているフレーム50の反発コイル22と接してい
る部分には渦電流が生じる。これは1ターンの短絡コイ
ルとして作用するから、反発コイル22の電磁力を弱め
るように作用してしまう。そこで、反発コイル22を取
付けてあるフレーム50の板を抵抗の高いステンレス板
にするとか、反発コイル22とフレーム50との間に絶
縁性のスペーサ(図示しない)を入れて反発コイル22
とフレーム50との距離を離すなどの方法を採っても良
いが、いずれも経済的でないので、図11に示す方法を
採るのがよい。
Embodiment 4 In FIG. 1, the repulsion coil 2
Since the electromagnetic force of No. 2 extends to the upper part of the drawing, an eddy current is generated in a portion of the frame 50 on which the repulsion coil 22 is mounted, in contact with the repulsion coil 22. Since this acts as a one-turn short-circuit coil, it acts to weaken the electromagnetic force of the repulsion coil 22. Therefore, the plate of the frame 50 to which the repulsion coil 22 is attached may be made of a high-resistance stainless steel plate, or an insulating spacer (not shown) may be inserted between the repulsion coil 22 and the frame 50 to make the repulsion coil 22
A method such as increasing the distance between the frame and the frame 50 may be used, but since none of them is economical, the method shown in FIG. 11 is preferably used.

【0025】図11は図1の上方から下方を見た平面図
で、24は可動ロッド1Aが貫通する穴、25は貫通穴
24の周囲に反発コイル22のコイル巻き線に直交する
ように設けたスリットである。スリット25によりフレ
ーム50の反発コイル22と接する部分に生じる渦電流
は僅かとなり、フレーム50が1巻の短絡コイルとして
作用すると言うことがなくなる。その結果反発コイル2
2の電磁力が強くなり反発板23に生じる反発力も大き
くなる。なお、図11では スリット25は穴24の周
囲に4本示しているが、1本でも設けられて居れば効果
が生じる。
FIG. 11 is a plan view of FIG. 1 as viewed from above, in which 24 is a hole through which the movable rod 1A penetrates, and 25 is provided around the through hole 24 so as to be orthogonal to the coil winding of the repulsion coil 22. It is a slit. The eddy current generated in the portion of the frame 50 in contact with the repulsion coil 22 by the slit 25 becomes small, and the frame 50 does not function as a single-turn short-circuit coil. As a result, the repulsion coil 2
2, the repulsive force generated on the repulsion plate 23 also increases. Although four slits 25 are shown around the hole 24 in FIG. 11, an effect is obtained if at least one slit 25 is provided.

【0026】[0026]

【発明の効果】この発明による電磁反発機構は、コイル
に流れる電流のピーク値を一定として、コンデンサの容
量を変化させて、コイル電流の周波数を500〜200
0HZとすることで、周波数の低い場合に発生する電磁
反発力よりも大きな電磁反発力を利用することができ、
可動部重量の軽量化、更には電磁反発用電源の最適化が
図れる。
According to the electromagnetic repulsion mechanism of the present invention, the peak value of the current flowing through the coil is kept constant, the capacitance of the capacitor is changed, and the frequency of the coil current is increased from 500 to 200.
By setting the frequency to 0HZ, it is possible to use an electromagnetic repulsive force larger than the electromagnetic repulsive force generated when the frequency is low,
The weight of the movable part can be reduced, and the power source for electromagnetic repulsion can be optimized.

【0027】また、この発明による電磁反発機構は、薄
板反発板が2〜6mmの厚みの銅板と、この銅板を支え
るプラスティック又は非磁性金属からなる補強板とで構
成されているので、その分軽量化されるので、加速度が
大きくなると言う効果が得られる。
In the electromagnetic repulsion mechanism according to the present invention, the thin repulsion plate is composed of a copper plate having a thickness of 2 to 6 mm and a reinforcing plate made of a plastic or a non-magnetic metal for supporting the copper plate. Therefore, the effect of increasing the acceleration can be obtained.

【0028】また、この発明による電磁反発機構は、補
強板がその外周に近い部分の厚みが内周に近い部分の厚
みより薄いテーパ構造を有するので、テーパ状とした補
強板は軽量化され加速度を高くすると言う効果が得られ
る。
In the electromagnetic repulsion mechanism according to the present invention, the reinforcing plate has a tapered structure in which the thickness of the portion near the outer periphery is thinner than the thickness of the portion near the inner periphery. To increase the effect.

【0029】また、反発コイルは逆並列に接続されたダ
イオードを有するので、並列共振回路の振動電流を直流
電流に変え、電磁反発力が効率よく利用されると言う効
果が得られる。
Further, since the repulsion coil has a diode connected in anti-parallel, the oscillation current of the parallel resonance circuit is converted into a DC current, and the effect that the electromagnetic repulsion is used efficiently can be obtained.

【0030】また、反発コイルを取付けたフレームは、
前記コイルの巻き線に直交するスリットを有するので、
フレーム側の無駄な渦電流を減少し、反発板に生じる渦
電流が大きくなり反発力が強くなると言う効果が得られ
る。
The frame on which the repulsion coil is mounted is
Since it has a slit orthogonal to the winding of the coil,
The effect of reducing unnecessary eddy current on the frame side, increasing the eddy current generated in the repulsion plate, and increasing the repulsion force can be obtained.

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

【図1】 この発明の実施の形態1による電磁反発機構
部である。
FIG. 1 shows an electromagnetic repulsion mechanism according to Embodiment 1 of the present invention.

【図2】 図1の電磁反発機構の周波数と反発力の関係
図である。
FIG. 2 is a relationship diagram between a frequency and a repulsive force of the electromagnetic repulsion mechanism of FIG.

【図3】 図1の電磁反発機構の反発板の板厚方向の電
流密度特性を示す図である。
FIG. 3 is a diagram showing a current density characteristic in a thickness direction of a repulsion plate of the electromagnetic repulsion mechanism of FIG. 1;

【図4】 図1の電磁反発機構の補強板の外形図であ
る。
FIG. 4 is an external view of a reinforcing plate of the electromagnetic repulsion mechanism of FIG. 1;

【図5】 図1の電磁反発機構を用いた装備した開閉器
の図である。
FIG. 5 is a view of a switch equipped with the electromagnetic repulsion mechanism of FIG. 1;

【図6】 図1の電磁反発機構用電源の回路図である。FIG. 6 is a circuit diagram of the power supply for the electromagnetic repulsion mechanism of FIG. 1;

【図7】 実施の形態2の電磁反発機構の機構部を説明
する図である。
FIG. 7 is a diagram illustrating a mechanism of an electromagnetic repulsion mechanism according to a second embodiment.

【図8】 軸心からの距離と電磁反発力との関係を説明
する図である。
FIG. 8 is a diagram illustrating a relationship between a distance from an axis and an electromagnetic repulsion.

【図9】 実施の形態3で用いる電磁反発用電源の回路
図である。
FIG. 9 is a circuit diagram of a power supply for electromagnetic repulsion used in the third embodiment.

【図10】 図9の回路に流れる電流の説明図である。FIG. 10 is an explanatory diagram of a current flowing in the circuit of FIG. 9;

【図11】 実施の形態4によるフレームの構造を示す
図である。
FIG. 11 is a diagram showing a structure of a frame according to a fourth embodiment.

【図12】 従来の電磁反発機構を装備した開閉器の図
である。
FIG. 12 is a diagram of a switch equipped with a conventional electromagnetic repulsion mechanism.

【図13】 従来の電磁反発用電源の回路図である。FIG. 13 is a circuit diagram of a conventional power supply for electromagnetic repulsion.

【図14】 図12の回路に流れるコイル電流を示す図
である。
FIG. 14 is a diagram showing a coil current flowing in the circuit of FIG.

【符号の説明】[Explanation of symbols]

1 真空バルブ 1A 可動ロ
ッド 2、22 反発コイル 3 反発板 5 駆動機構 6 電磁反発
機構 7 充電用交流電源 9 ダイオー
ド 10 コンデンサ 11 スイッ
チ 12 ダイオード 13、13a
補強板 22 反発コイル 23 薄板
反発板 20 コンデンサ 24 可動ロ
ッド貫通穴 25 スリット 47 電磁反発用電源 48 電磁反発機構 49 電磁反発用電源 50 フレーム r 軸心からの距離 Ra 反発コイルのコイル半径
DESCRIPTION OF SYMBOLS 1 Vacuum valve 1A Movable rod 2, 22 Repulsion coil 3 Repulsion plate 5 Driving mechanism 6 Electromagnetic repulsion mechanism 7 AC power supply for charging 9 Diode 10 Capacitor 11 Switch 12 Diode 13, 13a
Reinforcement plate 22 Repulsion coil 23 Thin repulsion plate 20 Capacitor 24 Movable rod through hole 25 Slit 47 Electromagnetic repulsion power supply 48 Electromagnetic repulsion mechanism 49 Electromagnetic repulsion power supply 50 Frame r Distance from axis Ra Radius of coil of repulsion coil

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 フレームに固定され接離可能な可動接点
を有する真空バルブと、前記可動接点に接続された可動
ロッドとを有する開閉器に用いられ、前記可動ロッドを
駆動する開閉器の電磁反発機構であって、 前記可動ロッドの周囲で前記フレームに固定された反発
コイルと、前記反発コイルのコイル面に対応して前記可
動ロッドに固着された薄板反発板と、直流電圧を保持す
るコンデンサを有する電源とを含み、前記コイルのイン
ダクタンスと前記コンデンサの容量とで構成される共振
回路の共振周波数が500HZ以上2KHZ以下である
ことを特徴とする開閉器の電磁反発機構。
An electromagnetic repulsion of a switch used for a switch having a movable valve fixed to a frame and having a movable contact that can be separated from and moved and a movable rod connected to the movable contact, the switch driving the movable rod. A repulsion coil fixed to the frame around the movable rod, a thin plate repulsion plate fixed to the movable rod corresponding to a coil surface of the repulsion coil, and a capacitor for holding a DC voltage. An electromagnetic repulsion mechanism for a switch, comprising: a power supply having a resonance frequency of 500 Hz or more and 2 KHZ or less, the resonance circuit including a coil inductance and a capacitance of the capacitor.
【請求項2】 薄板反発板は2〜6mmの厚みの銅板
と、この銅板を支えるプラスティック又は非磁性金属か
らなる補強板とで構成されていることを特徴とする請求
項1に記載の開閉器の電磁反発機構。
2. The switch according to claim 1, wherein the thin plate repulsion plate comprises a copper plate having a thickness of 2 to 6 mm and a reinforcing plate made of a plastic or a non-magnetic metal for supporting the copper plate. Electromagnetic repulsion mechanism.
【請求項3】 補強板は外周に近い部分の厚みが内周に
近い部分の厚みより薄いテーパ構造を有するものである
ことを特徴とする請求項2に記載の開閉器の電磁反発機
構。
3. The electromagnetic repulsion mechanism of a switch according to claim 2, wherein the reinforcing plate has a tapered structure in which a thickness of a portion near an outer periphery is thinner than a thickness of a portion near an inner periphery.
【請求項4】 反発コイルは逆並列に接続されたダイオ
ードを有することを特徴とする請求項2に記載の開閉器
の電磁反発機構。
4. The electromagnetic repulsion mechanism of a switch according to claim 2, wherein the repulsion coil has a diode connected in anti-parallel.
【請求項5】 反発コイルを取付けたフレームは、前記
反発コイルの巻き線に直交するスリットを有するもので
あることを特徴とする請求項1に記載の開閉器の電磁反
発機構。
5. The electromagnetic repulsion mechanism for a switch according to claim 1, wherein the frame on which the repulsion coil is mounted has a slit orthogonal to the winding of the repulsion coil.
JP17966597A 1997-07-04 1997-07-04 Electromagnetic repulsion mechanism for switch Pending JPH1125817A (en)

Priority Applications (1)

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