JPH08172018A - Pulse power source - Google Patents
Pulse power sourceInfo
- Publication number
- JPH08172018A JPH08172018A JP31390194A JP31390194A JPH08172018A JP H08172018 A JPH08172018 A JP H08172018A JP 31390194 A JP31390194 A JP 31390194A JP 31390194 A JP31390194 A JP 31390194A JP H08172018 A JPH08172018 A JP H08172018A
- Authority
- JP
- Japan
- Prior art keywords
- pulse
- winding
- current
- core
- transformer
- 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
- Coils Of Transformers For General Uses (AREA)
- Coils Or Transformers For Communication (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、高電圧・大電流の短パ
ルスを発生するパルス電源に係り、特にパルストランス
に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a pulse power source for generating short pulses of high voltage and large current, and more particularly to a pulse transformer.
【0002】[0002]
【従来の技術】パルスレーザ励起やパルスプラズマ発
生,パルス脱硝装置等のパルス電源には、サイラトロン
スイッチやトリガトロンスイッチ等の放電スイッチを用
いて直接に高電圧・大電流をスイッチングすることでパ
ルスを発生するものと、半導体スイッチと磁気スイッチ
になる可飽和リアクトルを組合せたものがある。2. Description of the Related Art For a pulse power source such as pulse laser excitation, pulse plasma generation, pulse denitration equipment, etc., a discharge switch such as a thyratron switch or a triggertron switch is used to directly switch a high voltage and a large current to generate a pulse. There is a combination of the generated one and a saturable reactor that becomes a semiconductor switch and a magnetic switch.
【0003】図3は、半導体スイッチと可飽和トラン
ス、可飽和リアクトルを組み合わせ、LC反転回路によ
り高圧・大電流を得るパルス電源の例を示す。FIG. 3 shows an example of a pulse power supply that combines a semiconductor switch, a saturable transformer, and a saturable reactor to obtain a high voltage and a large current by an LC inverting circuit.
【0004】半導体スイッチSWは1つの半導体スイッ
チング素子とそのゲート制御回路,スナバ回路を有して
構成された初段スイッチにされる。The semiconductor switch SW is a first-stage switch having one semiconductor switching element, its gate control circuit, and a snubber circuit.
【0005】パルストランスPTと初段エネルギー蓄積
用コンデンサC0及び高圧直流電源HDCに半導体スイ
ッチSWを組み合わせた初段パルス発生回路により、矢
印で示すパルス電流I0を発生する。A pulse current I 0 indicated by an arrow is generated by a first stage pulse generation circuit in which a pulse transformer PT, a first stage energy storage capacitor C 0 and a high voltage DC power supply HDC are combined with a semiconductor switch SW.
【0006】パルストランスPTの二次巻線には昇圧と
磁気パルス圧縮を行う可飽和トランスSTが接続され
る。可飽和トランスSTの二次巻線にはコンデンサ
C1、C2とリアクトルLからなる倍電圧発生回路が設け
られる。A saturable transformer ST that performs boosting and magnetic pulse compression is connected to the secondary winding of the pulse transformer PT. The secondary winding of the saturable transformer ST is provided with a voltage doubler generation circuit composed of capacitors C 1 and C 2 and a reactor L.
【0007】さらに、倍電圧発生回路の出力端になるリ
アクトルLの両端には可飽和リアクトルSI2とピーキ
ング・コンデンサCPの直列回路が並列接続される。ま
た、コンデンサCPには負荷としてのレーザ発振器LH
が並列接続される。Further, a series circuit of a saturable reactor SI 2 and a peaking capacitor C P is connected in parallel to both ends of a reactor L which is an output terminal of the voltage doubler generation circuit. Further, the capacitor C P has a laser oscillator LH as a load.
Are connected in parallel.
【0008】パルス発生の開始には、コンデンサC0は
高圧直流電源HDCによって高圧充電しておく。この充
電後、半導体スイッチSWをオンさせることにより、コ
ンデンサC0→パルストランスPTの一次巻線→半導体
スイッチSWの経路で一次電流I0を流す。At the start of pulse generation, the capacitor C 0 is charged to a high voltage by the high voltage DC power supply HDC. After this charging, by turning on the semiconductor switch SW, the primary current I 0 flows through the path of the capacitor C 0 → the primary winding of the pulse transformer PT → the semiconductor switch SW.
【0009】この電流I0に対し、パルストランスPT
と可飽和トランスSTによる2段の昇圧がなされ、倍電
圧発生回路等を通して負荷に高電圧・大電流の超短パル
スを供給する。For this current I 0 , the pulse transformer PT
Then, the voltage is boosted in two steps by the saturable transformer ST, and an ultrashort pulse of high voltage and large current is supplied to the load through the voltage doubler generation circuit and the like.
【0010】ここで、パルストランスPTは、商用周波
数(50、60HZ)のトランスに比べて高周波電流に
トランス作用を得るのに、鉄心等を用いたトランスでは
渦電流損が増加するため、一般的には低損失のコア材を
使用するか、又は空心トランスにされる。[0010] Here, the pulse transformer PT is to obtain a trans-acting high frequency current than the transformer of the commercial frequency (50,60H Z), since the eddy current loss increases in transformer using the core or the like, generally Typically, a low-loss core material is used, or an air-core transformer is used.
【0011】[0011]
【発明が解決しようとする課題】従来のパルス電源にお
いて、パルストランスは、高電圧・短パルスで使用さ
れ、高耐電圧絶縁した巻線は線径が大きくなるため、一
次巻線及び二次巻線共に巻数を多くできない。このた
め、昇圧トランスでは高い昇圧比を得ようとすると一次
巻線が1ターンに制約されることが多い。In the conventional pulse power supply, the pulse transformer is used for high voltage / short pulse, and the wire diameter of the winding insulated with high withstand voltage is large. Therefore, the primary winding and the secondary winding are You cannot increase the number of turns for both wires. For this reason, in the step-up transformer, the primary winding is often limited to one turn in order to obtain a high step-up ratio.
【0012】一方、トランスの電圧時間積は磁心断面積
と巻数に比例するため、巻数を多く取れないパルス電源
用トランスでは磁心が大きくなる。On the other hand, the voltage-time product of the transformer is proportional to the cross-sectional area of the magnetic core and the number of turns. Therefore, the transformer for a pulse power supply that cannot take many turns has a large magnetic core.
【0013】結果的に、昇圧比が制約され、しかもトラ
ンス自体の大型化を招く。As a result, the step-up ratio is restricted and the size of the transformer itself is increased.
【0014】本発明の目的は、パルストランスを小型化
し、装置全体の小型化を可能にするパルス電源を提供す
ることにある。It is an object of the present invention to provide a pulse power supply which can downsize the pulse transformer and downsize the entire apparatus.
【0015】[0015]
【課題を解決するための手段】本発明は、前記課題の解
決を図るため、単方向のパルス電流が供給されるパルス
トランスを有して高電圧・大電流のパルスを得るパルス
電源において、前記パルストランスはコアに一次巻線と
二次巻線の他に第3の巻線を設け、前記パルストランス
の第3の巻線には一次巻線に流れるパルス電流で発生す
る磁束方向とは逆方向の極性になる直流定電流を供給す
る直流バイアス手段を設けたことを特徴とする。In order to solve the above-mentioned problems, the present invention provides a pulse power supply having a pulse transformer to which a unidirectional pulse current is supplied to obtain a high-voltage / high-current pulse. In the pulse transformer, a third winding is provided on the core in addition to the primary winding and the secondary winding, and the third winding of the pulse transformer has a magnetic flux direction opposite to that generated by the pulse current flowing through the primary winding. It is characterized in that a DC bias means for supplying a DC constant current having a directional polarity is provided.
【0016】[0016]
【作用】第3の巻線に逆方向の直流バイアス電流を流す
ことにより、パルストランスの実行動作磁束密度量ΔB
を大きくする。この実行動作磁束密度量ΔBは、コアの
電圧時間積に比例することからトランスのコア断面積を
小さくでき、これに伴いコア容積を小さくし、パルスト
ランスの小型化を得る。By applying a reverse DC bias current to the third winding, the magnetic flux density amount ΔB of the execution operation of the pulse transformer is increased.
To increase. Since this execution operation magnetic flux density amount ΔB is proportional to the voltage-time product of the core, the core cross-sectional area of the transformer can be reduced, and accordingly, the core volume can be reduced and the pulse transformer can be miniaturized.
【0017】[0017]
【実施例】図1は本発明の一実施例を示す回路図であ
り、図3のパルストランスPTの部分を示す。1 is a circuit diagram showing an embodiment of the present invention, showing a portion of the pulse transformer PT of FIG.
【0018】パルストランスは、一次巻線11と二次巻
線12とが所定の巻数比でコア13に巻かれる他に、直流
バイアス電流を流すための第3の巻線14がコア13に巻
かれる。In the pulse transformer, the primary winding 1 1 and the secondary winding 1 2 are wound around the core 1 3 at a predetermined turn ratio, and the third winding 1 4 for passing a DC bias current is provided. wound on the core 1 3.
【0019】巻線14には、定電流電源2からチョーク
コイル3を通して定電流が供給される。このチョークコ
イル3は、一次巻線11に流れるパルス電流に対して高
いインピーダンスを呈するものにされ、該パルス電流が
巻線14側へ流れる(エネルギーが漏れる)のを抑制す
る。[0019] winding 1 4, a constant current is supplied through the choke coil 3 from the constant current source 2. The choke coil 3 is the one that exhibits a high impedance to a pulse current flowing through the primary winding 1 1 suppresses the pulse current flows into the winding 1 4 side of (energy leakage).
【0020】巻線14に流す直流電流極性は、一次巻線
11に供給されるパルス電流により発生する磁束方向
(矢印で示す)とは逆方向にされる。The polarity of the direct current flowing through the winding 1 4 is opposite to the direction of the magnetic flux (indicated by the arrow) generated by the pulse current supplied to the primary winding 1 1 .
【0021】また、電流の大きさは、コア13の保持力
以上の磁束を発生するものにされる。例えば、保持力1
(A/m)、最外周1(m)のトロイダル形コアには貫
通型巻線(1ターン)にした巻線14に1(A)以上の
直流バイアス電流を流す。The magnitude of the current is such that a magnetic flux larger than the coercive force of the core 1 3 is generated. For example, holding power 1
(A / m), passing a DC bias current of 1 (A) or the winding 1 4 that the through-type windings to toroidal core (1 turn) the outermost 1 (m).
【0022】コア13の形状は、トロイダル形やレース
トラック形、さらにはソレノイド形の何れかにされる。
また、コア13の材質は、低損失・高透磁率の磁心にさ
れ、例えば鉄系アモルファス、コバルト系アモルファ
ス、鉄系超微結晶質にされる。The core 1 3 shape, a toroidal shape or a racetrack shape, further is in either of solenoids.
The material of the core 1 3 is the core of low loss and high magnetic permeability, is for example, iron-based amorphous, cobalt-based amorphous, iron-based ultracrystallite.
【0023】本実施例の構成において、一次巻線11に
は単方向のパルス電流が流れる。このパルス電流に対し
て、巻線14に逆方向の直流バイアス電流を流す。これ
により、図2の(a)に示すように、実行動作磁束密度
量ΔBが(b)に示す直流バイアスを行わない従来構成
の場合よりも大きくなる。[0023] In the structure of this embodiment, pulse current unidirectional flows through the primary winding 1 1. For this pulse current, flowing a reverse DC bias current to the winding 1 4. As a result, as shown in FIG. 2A, the execution operation magnetic flux density amount ΔB becomes larger than that in the case of the conventional configuration shown in FIG.
【0024】ここで、実行動作磁束密度量ΔBは、コア
13の電圧時間積に比例するため、トランスのコア断面
積を小さくでき、結果的にコア容積を小さくすることが
できる。[0024] Here, execution operation magnetic flux density amount ΔB is proportional to the voltage time product of the core 1 3, it is possible to reduce the core area of the transformer, can be reduced resulting in the core volume.
【0025】また、角形比(Br/Bs)の良い(≒
1)コアであるときは直流バイアス電流により約2倍の
ΔB(=Br+Bs)を得ることができる。Also, the squareness ratio (Br / Bs) is good (≈
1) When it is a core, it is possible to obtain about twice as much ΔB (= Br + Bs) by the DC bias current.
【0026】なお、本実施例のパルストランスは、図3
に示す構成のパルス電源に限らず、パルストランスを使
用する他の多くのパルス電源に適用して同等の作用効果
を奏する。The pulse transformer of this embodiment is shown in FIG.
Not only the pulse power source having the configuration shown in (1) but also other pulse power sources using a pulse transformer, the same operational effect can be obtained.
【0027】[0027]
【発明の効果】以上のとおり、本発明によれば、パルス
トランスにはコアに一次巻線と二次巻線の他に第3の巻
線を設け、この第3の巻線には一次巻線に流れるパルス
電流で発生する磁束方向とは逆方向の極性になる直流定
電流を供給する構成としたため、パルストランスの実行
動作磁束密度量ΔBを大きくすることができ、トランス
のコア断面積を小さくしてコア容積を小さくし、パルス
トランスの小型化を得ることができる。ひいては、パル
ス電源の小型化を図ることができる。As described above, according to the present invention, in the pulse transformer, the core is provided with the third winding in addition to the primary winding and the secondary winding, and the third winding is provided with the primary winding. Since the configuration is such that a DC constant current whose polarity is opposite to the direction of the magnetic flux generated by the pulse current flowing through the line is supplied, the magnetic flux density amount ΔB of the operation of the pulse transformer can be increased and the core cross-sectional area of the transformer can be increased. The size of the pulse transformer can be reduced by reducing the size of the core and the core volume. As a result, the pulse power supply can be downsized.
【図1】本発明の一実施例を示す回路図。FIG. 1 is a circuit diagram showing an embodiment of the present invention.
【図2】直流バイアスを与える場合(a)と従来の場合
(b)の磁化特性図。FIG. 2 is a magnetization characteristic diagram in the case of applying a DC bias (a) and the conventional case (b).
【図3】パルス電源の回路例。FIG. 3 is a circuit example of a pulse power supply.
SW…半導体スイッチ ST…可飽和トランス PT…パルストランス 11…一次巻線 12…二次巻線 13…コア 14…第3の巻線 2…定電流電源 3…チョークコイルSW ... Semiconductor switch ST ... Saturable transformer PT ... Pulse transformer 1 1 ... Primary winding 1 2 ... Secondary winding 1 3 ... Core 1 4 ... Third winding 2 ... Constant current power supply 3 ... Choke coil
───────────────────────────────────────────────────── フロントページの続き (72)発明者 原 喜芳 東京都品川区大崎2丁目1番17号 株式会 社明電舎内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Yoshiyoshi Hara 2-17 Osaki, Shinagawa-ku, Tokyo Incorporated company Meidensha
Claims (1)
トランスを有して高電圧・大電流のパルスを得るパルス
電源において、 前記パルストランスはコアに一次巻線と二次巻線の他に
第3の巻線を設け、前記パルストランスの第3の巻線に
は一次巻線に流れるパルス電流で発生する磁束方向とは
逆方向の極性になる直流定電流を供給する直流バイアス
手段を設けたことを特徴とするパルス電源。1. A pulse power supply for obtaining a high-voltage / large-current pulse by having a pulse transformer to which a unidirectional pulse current is supplied, wherein the pulse transformer has a core, in addition to a primary winding and a secondary winding. A third winding is provided, and the third winding of the pulse transformer is provided with DC bias means for supplying a DC constant current having a polarity opposite to the direction of the magnetic flux generated by the pulse current flowing in the primary winding. A pulse power supply characterized by that.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP31390194A JPH08172018A (en) | 1994-12-19 | 1994-12-19 | Pulse power source |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP31390194A JPH08172018A (en) | 1994-12-19 | 1994-12-19 | Pulse power source |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH08172018A true JPH08172018A (en) | 1996-07-02 |
Family
ID=18046887
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP31390194A Pending JPH08172018A (en) | 1994-12-19 | 1994-12-19 | Pulse power source |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH08172018A (en) |
-
1994
- 1994-12-19 JP JP31390194A patent/JPH08172018A/en active Pending
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