JPS59155906A - Demagnetizing circuit of dc exciting electromagnetic coil - Google Patents
Demagnetizing circuit of dc exciting electromagnetic coilInfo
- Publication number
- JPS59155906A JPS59155906A JP2691584A JP2691584A JPS59155906A JP S59155906 A JPS59155906 A JP S59155906A JP 2691584 A JP2691584 A JP 2691584A JP 2691584 A JP2691584 A JP 2691584A JP S59155906 A JPS59155906 A JP S59155906A
- Authority
- JP
- Japan
- Prior art keywords
- circuit
- electromagnetic coil
- resistor
- switch
- coil
- 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
Links
Landscapes
- Video Image Reproduction Devices For Color Tv Systems (AREA)
- Magnetic Treatment Devices (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔発明の属する技術分野〕
この発明は、直流励磁電磁コイル特に電磁開閉器の電磁
コイルをこのコイルに接続した消磁分路により消磁する
た′めの回路であって、励磁電圧に依存して開閉する電
子式スイッチがこの電磁コイルに直列に接続されかつこ
のスイッチに非1直線抵抗が並列に接続された消磁回路
にか/J)わる。[Detailed description of the invention] [Technical field to which the invention pertains] The present invention provides a circuit for demagnetizing a DC-excited electromagnetic coil, particularly an electromagnetic coil of an electromagnetic switch, by a demagnetizing shunt connected to the coil, An electronic switch that opens and closes depending on the excitation voltage is connected in series with this electromagnetic coil, and a degaussing circuit is connected in parallel with this switch.
かかる消磁回路lこ関する従来技術としては、本件出願
人の出願にかかるドイツ連邦共和国特許出願第3232
217.8−.33号(昭和関部8月別日に日本国出願
2発明の名称「直流励磁の電磁コイルの消磁用回路装置
」、以下前出願という)がある。As a prior art related to such a degaussing circuit, Patent Application No. 3232 of the Federal Republic of Germany filed by the present applicant is known.
217.8-. There is No. 33 (named ``Circuit device for degaussing a DC-excited electromagnetic coil'' filed in Japan on a separate date in August of 1920, hereinafter referred to as the previous application).
この従来技術においては、電磁コイルへの励磁電圧の値
に依存して開閉する電子式開閉器が電磁コイルに直列に
接続され、また電磁コイルに並列に非直線抵抗が接続さ
れろ。これにより電磁コイルによって操作される開閉器
類の開路遅延時間をわずかな費用で短縮することが可能
となったが、使用目的によりかかる開路遅延時間を自由
に調整しないしは選択する必要が生じたときには、かか
る従来技術の手段のみでは開路遅延時間の肖整や選択が
必ずしも容易でない。In this prior art, an electronic switch that opens and closes depending on the value of the excitation voltage applied to the electromagnetic coil is connected in series to the electromagnetic coil, and a nonlinear resistor is connected in parallel to the electromagnetic coil. This made it possible to shorten the opening delay time of switches operated by electromagnetic coils at a small cost, but it became necessary to freely adjust or select the opening delay time depending on the purpose of use. Sometimes, it is not always easy to adjust and select the opening delay time using only such prior art means.
この発明は、電磁υ11閉器の開極遅延時間を必要lこ
応じてその最小値から”I FA整に延長しつるように
頭韻の回路を改良することを目的とする。The object of this invention is to improve the alliteration circuit so that the opening delay time of the electromagnetic υ11 switch can be extended from its minimum value to "IFA adjustment" as necessary.
r発明の要旨〕
この目的は□、電子式スイッチと非直線抵抗との並列回
路にさらに別の抵抗を並列に接続することにより達成さ
れる。また、この抵抗lこよりFAl1次的4こ非直線
抵抗a)エネルギ負不IJか減少する。この抵抗が可調
整であわ、ば、開極遅延時間は抵抗を交換する必要なく
現地において望ましい状態に適合させることができる。rSummary of the Invention This object is achieved by further connecting another resistor in parallel to the parallel circuit of the electronic switch and the non-linear resistor. Also, from this resistance l, the FAl primary nonlinear resistance a) energy negative IJ decreases. If this resistor is adjustable, the opening delay time can be adapted to desired conditions in the field without the need to replace the resistor.
つぎζこ前出願にもとづく回路とこの発明にもとづく回
路とを示す図面によりこの発明の詳細な説明する。The present invention will now be described in detail with reference to drawings showing a circuit based on the previous application and a circuit based on the present invention.
前出1fjflにもとづく回路をポす第1図において、
ダイオード4+ 5+6+7からなろ全波整流回路が開
閉器3を介して胤諒漏子1,21こ接続されている。全
波整流回路の直流′tシ圧出力端は端子8,9を介して
ダイオード10.抵抗11及びツェナーダイオード12
とキャパシタ15と抵抗16との並列回路から成る直列
回路に接続されている。電界効果トランジスタ13のド
レン、ソース口出線間には非IK線抵抗17が並列に接
続され、ここではこの抵抗はバリスタである。電界効果
トランジスタ13のドレン。In Figure 1, which shows a circuit based on the above-mentioned 1fjfl,
A full-wave rectifier circuit consisting of diodes 4+5+6+7 is connected to the diodes 1 and 21 via the switch 3. The DC voltage output end of the full-wave rectifier circuit is connected to a diode 10 through terminals 8 and 9. Resistor 11 and Zener diode 12
is connected to a series circuit consisting of a parallel circuit of a capacitor 15 and a resistor 16. A non-IK line resistor 17 is connected in parallel between the drain and source lead lines of the field effect transistor 13, and here this resistor is a varistor. Drain of field effect transistor 13.
ソース口出線とバリスタ17との並列回路は、その一つ
の結合点を端子9にまた他の結合点を′電磁コイ7+/
1.4の一つの口出緋に接続され、韮た電磁コイルの他
の口出線はψ′11i子8に接続、されている。The parallel circuit between the source lead wire and the varistor 17 has one connection point connected to the terminal 9 and the other connection point connected to the electromagnetic coil 7+/
1.4 is connected to one lead wire, and the other lead wire of the small electromagnetic coil is connected to ψ'11i wire 8.
開閉器3が閉じられると、全波整流された脈動直流電圧
が端子8.9に加わる。端子8は正極であり、端子9は
負極である。端子8と9との間の電圧がツェナーダイオ
ード12のツェナー′成圧とダイオード10のしきい′
?匡圧との相を上回ねっている限り、ダイオード10.
抵抗11及びツェナーダイオード12を経て補助電流が
流れ、この補助電流がツェナーダイオード12にツェナ
ー電圧降下を生ぜしめる。ツェナーダイオード12)こ
おりるこの電圧降下により無電力で制御可能な電界効果
トライリスク13は導通状態となるので、電磁コイル1
4は励磁される。キャパシタ15と抵抗16とから成る
回路σ)時定数は、端子8と9との間に加わる直流電圧
σ)fifr期的な落ち込み期間中でもルL界効果トラ
ンジスタ】3が導通状態に維持されろように選ばれろ。When the switch 3 is closed, a full-wave rectified pulsating DC voltage is applied to the terminal 8.9. Terminal 8 is a positive electrode, and terminal 9 is a negative electrode. The voltage between terminals 8 and 9 is the Zener voltage of Zener diode 12 and the threshold of diode 10.
? As long as the voltage exceeds the phase with the diode 10.
An auxiliary current flows through the resistor 11 and the Zener diode 12, and this auxiliary current causes a Zener voltage drop across the Zener diode 12. Zener diode 12) Due to this voltage drop, the field effect trial risk 13, which can be controlled without power, becomes conductive, so the electromagnetic coil 1
4 is excited. The circuit σ) consisting of a capacitor 15 and a resistor 16 has a time constant such that the field effect transistor 3 remains conductive even during periods of periodic dips in the DC voltage σ) applied between terminals 8 and 9. Be selected.
開閉器3が開かれると、端子8,9間θ)電圧シま急激
にダイオード4ないし7の順方向電圧降下σ)2倍の値
に低ドする。キャンぐシタ15はツェナーダイオード1
2のツエ、ナー直圧にプd電されているσ)で、クーイ
オード10は阻止されで、ツェナーダイオ−)”12゜
キャパシタ15及び抵抗16は端子8から切り離さ′I
]7る。そしてキャン(シタ15は抵抗16を介して放
電し、電界効果トランジスタ13は阻止状態にされる。When the switch 3 is opened, the voltage strip between the terminals 8 and 9 suddenly drops to a value twice the forward voltage drop σ) of the diodes 4 to 7. Camping point 15 is Zener diode 1
2, the Zener diode 10 is blocked by σ), which is connected to the direct voltage, and the Zener diode 12. Capacitor 15 and resistor 16 are separated from terminal 8.
]7ru. Then, the capacitor 15 is discharged through the resistor 16, and the field effect transistor 13 is placed in a blocking state.
7電磁コイルのIA留雷電流)くリスク17に転流さ1
1.る力5、パリス、り17はこれに生じる′P!圧が
電界効果トランジスタのドレーン、ソース間の最高許容
電圧を一゛ド回わろように設定されている。3Fつて°
醒磁コイルJ4に蓄えられたエネルギは急速かつ損傷を
生じろことノIく消滅される。7 IA current of electromagnetic coil) Risk of commutation 17
1. The force 5, Paris, ri 17 arises from this 'P! The voltage is set so as to exceed the maximum allowable voltage between the drain and source of the field effect transistor by one degree. 3F
The energy stored in the energizing coil J4 is dissipated rapidly and without causing damage.
前出願(こもとづく回路の第20)回路例を示す第2図
においては、ダイオード4と端子8との間ζこ電磁開閉
器の遅延常閉接点18が挿入接続されてし)る。常閉接
点18が開放することにより全波整流回路は半波整流回
路に切り換えられろ。消磁分路1ま二つのダイオード5
.7から成り、半波整流回路はダイオード5と6とから
盛る。遅延常閉接点19゛が開くと電磁コイル14の手
前に抵抗額が挿入される。こうして電磁コイルの保持電
力は著しく減少される。In FIG. 2 showing an example of the circuit of the previous application (No. 20 of the Komototsu circuit), a delay normally closed contact 18 of an electromagnetic switch is inserted and connected between the diode 4 and the terminal 8. By opening the normally closed contact 18, the full-wave rectifier circuit is switched to a half-wave rectifier circuit. Demagnetizing shunt 1 or two diodes 5
.. The half-wave rectifier circuit consists of diodes 5 and 6. When the delayed normally closed contact 19' opens, a resistor is inserted in front of the electromagnetic coil 14. The holding power of the electromagnetic coil is thus significantly reduced.
半波整流のためlこ端子8,9間の電圧は半波ごとに欠
落するので、電界効果トランジスタ】:3力≦この電圧
欠落期間中導通状態を保つようにRC回路15、lf’
iの時定数は第1図に示す回路に較べて大きく選ばれる
。しかしながらこのために電磁開閉器(の開極遅延時間
は第1図に示す回路に較べて増加することになる。この
理由にもとづ(、>て夕゛イメー一゛ ド4と6との
結合点22にダイオ−)” 21 (7)アノードが接
続される。ダイオード21Q)カソード(ま夕゛イオー
ド10と抵抗J1との結合点乙に接続される。これによ
り補助電流の欠落した半波は補Aつれる。こQ〕ときダ
イオード10は阻止状態にあるO)で、半波整l′1i
12回路への切り換えが無効となることは避けられろ。Due to half-wave rectification, the voltage between the terminals 8 and 9 is lost every half wave, so the field effect transistor is connected to the RC circuit 15, lf' so as to remain conductive during this voltage drop period.
The time constant of i is chosen to be large compared to the circuit shown in FIG. However, for this reason, the opening delay time of the electromagnetic switch will increase compared to the circuit shown in Figure 1. Based on this reason, (7) The anode of the diode 21 is connected to the connection point 22. The cathode of the diode 21Q is connected to the connection point B between the diode 10 and the resistor J1. This causes the missing half-wave of the auxiliary current. is complemented by A. At this time, the diode 10 is in the blocking state O), and the half-wave rectifier l'1i
Avoid switching to 12 circuits from becoming invalid.
かかる回路によりRC回路の時定数を増す必要がなくな
る。Such a circuit eliminates the need to increase the time constant of the RC circuit.
M+i出Bt4 Hこもとづく回路の第3の回路例を示
す第3図においでは、開閉器2・1が電磁コイル14の
励磁lE+3路0)直流源側に股りられでいる。ここで
もまた電磁コイル1.1に蓄えられたエネルギの消滅を
確実にずイ〕ため、D:12子8 、911!lにダイ
メート5が接続さ才ノ、ており、このダーfメート17
仁↑紅伺浸コイル14の消磁’y)路をバリスタエフを
介して閉じろ。このダイオード’IHO)挿入により制
御開閉器2・1の焼損が減少するという長lヅ「が副次
的に生じる。In FIG. 3 showing a third circuit example of a circuit based on M+i output Bt4H, the switch 2.1 is straddled on the side of the DC source for exciting the electromagnetic coil 14. Again, in order to ensure that the energy stored in the electromagnetic coil 1.1 disappears, D: 12 8, 911! Dimate 5 is connected to l, and this damate 17
Close the demagnetizing coil 14 through Ballistaev. The insertion of this diode (IHO) has the additional effect of reducing burnout of the control switches 2 and 1.
第・1ないし6図には、第1ないし3図に示す回路にI
S目しit界効果トランジリスJ30)ドレン、ソース
回路と1ト直へ抵抗17とに並列に可変抵抗かを接続し
たこの発明による回路が示されている。この可変抵抗に
より電磁開閉器の開極遅延時間がその最小値を越えて延
長される。抵抗値を無限大にすると開極遅延時間は最小
に調整される。抵抗値をセr1iこ一4′ろと、前出願
にもとづく回路を使用しなかった場合に設定される本来
の開極遅延時間に調整される。さらにこの可変抵抗によ
り非直線抵抗のエネルギ負荷が減少する。Figures 1 to 6 show that the circuits shown in Figures 1 to 3 are
A circuit according to the invention is shown in which a variable resistor is connected in parallel to the drain-source circuit and the resistor 17 in parallel to the drain-source circuit. This variable resistance extends the opening delay time of the electromagnetic switch beyond its minimum value. When the resistance value is set to infinity, the opening delay time is adjusted to the minimum value. When the resistance value is set by the circuit r1i4', it is adjusted to the original opening delay time that would have been set if the circuit based on the previous application was not used. Additionally, the variable resistance reduces the energy load of non-linear resistances.
この発明lこもとづき直流励磁電磁コイル特に電磁開閉
器の電磁コイルをこのコイルに接続した消磁分路により
消磁するための回路であって、励磁電圧に依存して開閉
する電子式スイッチがこの電磁フィルに1負列に接続さ
れかつこのスイッチに非直線抵抗が並列に接続された前
出願にもとづく回路tこおいて、前記の電子式スイッチ
と非直線抵抗との一1■列回路にさらに別の抵抗が並列
に接続されろ。This invention is a circuit for demagnetizing a DC excitation electromagnetic coil, especially an electromagnetic coil of an electromagnetic switch, by a demagnetizing shunt connected to this coil, and an electronic switch that opens and closes depending on the excitation voltage is connected to the electromagnetic filter. In the circuit based on the previous application in which the electronic switch and the non-linear resistor are connected in one negative column and a non-linear resistor is connected in parallel with this switch, there is a Connect the resistors in parallel.
かかる構成により、電源側の開閉器が開放され電界効果
トランジスタが阻止状態となったときに、電磁コイルの
残留電流が電界効果トランジスタから非直線抵抗及び別
の抵抗に転流されて消磁分路を流れ、電磁コイルに蓄え
られたエネルギはこれら抵抗の中で熱エネルギとして急
速に消費され、電磁開閉器の開極遅延時間が短縮される
。別の抵抗の抵抗値を無限大からゼロに向って変化する
と、開極遅延時間は最小値から可調整に延長しつる。With this configuration, when the switch on the power supply side is opened and the field effect transistor is in a blocking state, the residual current of the electromagnetic coil is commutated from the field effect transistor to the nonlinear resistor and another resistor, thereby creating a demagnetizing shunt. The energy stored in the electromagnetic coil is rapidly dissipated as thermal energy in these resistors, shortening the opening delay time of the electromagnetic switch. As the resistance of another resistor is varied from infinity to zero, the opening delay time is adjustable from a minimum value.
またこの別の抵抗により副次的に非直線抵抗のエネルギ
負荷が減少する。This additional resistance also reduces the energy load of the non-linear resistance.
施した回路図、である。This is the circuit diagram.
図面において、13は電子式スイッチ(電界効果トラン
ジスタ)、14は電磁コイル、17は非直線抵抗、26
は別の抵抗、である。In the drawing, 13 is an electronic switch (field effect transistor), 14 is an electromagnetic coil, 17 is a nonlinear resistor, and 26
is another resistance.
Claims (1)
をこのコイルに接続した消磁分路により消磁するための
回路であって、励磁電圧に依存して開閉する電子式スイ
ッチがこ。の電磁コイルに直列に接続されかつこのスイ
ッチに非直線抵抗が並列に接続された消磁回路において
、前記の電子式スイッチと非i線抵抗との並列回路にさ
らに別の抵抗が並列に接続されることを特徴とする直流
励磁電磁コイルの消磁回路。 2、特許請求の範囲第1項に記載の回路において、前記
抵抗が可調整であることを特徴とする直流励磁t(i8
コイルの消磁回路。[Claims] 1) A circuit for demagnetizing a DC excitation coil, particularly an electromagnetic coil of an electromagnetic switch, by a demagnetizing shunt connected to this coil, which is an electronic type that opens and closes depending on the excitation voltage. Here's the switch. In a degaussing circuit that is connected in series to the electromagnetic coil and a non-linear resistor is connected in parallel to this switch, another resistor is connected in parallel to the parallel circuit of the electronic switch and the non-i-line resistor. A degaussing circuit for a DC-excited electromagnetic coil, characterized in that: 2. The circuit according to claim 1, characterized in that the resistance is adjustable.
Coil demagnetization circuit.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE33056749 | 1983-02-18 | ||
DE19833305674 DE3305674A1 (en) | 1982-08-30 | 1983-02-18 | Circuit arrangement for deenergising DC-energised magnet coils |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59155906A true JPS59155906A (en) | 1984-09-05 |
Family
ID=6191217
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2691584A Pending JPS59155906A (en) | 1983-02-18 | 1984-02-15 | Demagnetizing circuit of dc exciting electromagnetic coil |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59155906A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04111293U (en) * | 1991-03-18 | 1992-09-28 | 日本サーボ株式会社 | Brake drive circuit |
JP2010103262A (en) * | 2008-10-22 | 2010-05-06 | Mitsubishi Heavy Ind Ltd | Inductor drive circuit |
JP2013021853A (en) * | 2011-07-13 | 2013-01-31 | Toyooki Kogyo Co Ltd | Solenoid driving circuit |
-
1984
- 1984-02-15 JP JP2691584A patent/JPS59155906A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04111293U (en) * | 1991-03-18 | 1992-09-28 | 日本サーボ株式会社 | Brake drive circuit |
JP2010103262A (en) * | 2008-10-22 | 2010-05-06 | Mitsubishi Heavy Ind Ltd | Inductor drive circuit |
US8508201B2 (en) | 2008-10-22 | 2013-08-13 | Mitsubishi Heavy Industries, Ltd. | Inductor driving circuit |
JP2013021853A (en) * | 2011-07-13 | 2013-01-31 | Toyooki Kogyo Co Ltd | Solenoid driving circuit |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US4464585A (en) | Gate circuit of gate turn-off thyristor | |
JPH0691747B2 (en) | Switch mode power supply device | |
JPH0866037A (en) | Power supply | |
JPS59155906A (en) | Demagnetizing circuit of dc exciting electromagnetic coil | |
JPH04368469A (en) | Switching power source | |
JP2000341848A (en) | Reverse-polarity input protective device | |
JP3251192B2 (en) | Overcurrent protection circuit | |
JP3175205B2 (en) | Inrush current suppression circuit for switching power supply | |
EP0580237B1 (en) | Power factor correction circuit | |
JPS6361859B2 (en) | ||
JP2861246B2 (en) | Switching power supply | |
JPS5960838A (en) | Demagnetizing circuit device for dc exciting electromagneticcoil | |
KR20030005785A (en) | Snubber circuit | |
JP2816672B2 (en) | DC power supply | |
JP4236459B2 (en) | Rectifier circuit and switching power supply provided with the rectifier circuit | |
JP3375188B2 (en) | Switching regulator overcurrent protection circuit | |
JP3425107B2 (en) | Overcurrent protection circuit | |
JP2884855B2 (en) | Temperature control circuit | |
JPS5812571A (en) | Thyristor control circuit in rush current limiting circuit | |
KR810000442B1 (en) | Degaussing circuit in a color television receiver | |
JPS5914296A (en) | Device for firing discharge lamp | |
JPS63107458A (en) | Switcing power source | |
JP3469510B2 (en) | Self-excited switching power supply circuit | |
KR950003488Y1 (en) | Power circuit for inrush current | |
JP2002142461A (en) | High voltage generator |