JPH01157280A - Saturable reactor for high-voltage pulse generating device - Google Patents

Saturable reactor for high-voltage pulse generating device

Info

Publication number
JPH01157280A
JPH01157280A JP62313644A JP31364487A JPH01157280A JP H01157280 A JPH01157280 A JP H01157280A JP 62313644 A JP62313644 A JP 62313644A JP 31364487 A JP31364487 A JP 31364487A JP H01157280 A JPH01157280 A JP H01157280A
Authority
JP
Japan
Prior art keywords
voltage pulse
saturable reactor
pulse generator
saturable
high voltage
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
JP62313644A
Other languages
Japanese (ja)
Inventor
Susumu Nakajima
晋 中島
Kiyotaka Yamauchi
山内 清隆
Hideaki Shimizu
英明 清水
Akira Yamataka
山高 晶
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.)
Proterial Ltd
Original Assignee
Hitachi Metals 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 Hitachi Metals Ltd filed Critical Hitachi Metals Ltd
Priority to JP62313644A priority Critical patent/JPH01157280A/en
Publication of JPH01157280A publication Critical patent/JPH01157280A/en
Pending legal-status Critical Current

Links

Landscapes

  • Generation Of Surge Voltage And Current (AREA)

Abstract

PURPOSE:To improve cooling efficiency, by a method wherein a plurality of tape wound cores, employing an amorphous magnetic thin belt or the like, being applied with an insulating tape or the like between layers and having different sizes, is arranged concentrically and a saturable magnetic core having gaps is employed. CONSTITUTION:A saturable reactor for high-voltage pulse generating device is composed of input and output terminals 1, 3, a coaxial cylindrical conductor 2, an oil inlet port 4, an oil outlet port 5, tape-wound magnetic cores 6, an insulating body guide 8, an insulating body 9 and the like. In this case, an amorphous magnetic thin belt is employed for the tape-wound core 6 while an insulating tape or an insulating coating is applied between layers. Gaps 7 are provided in order to increase the cooling efficiency of the tape-wound core 6 while cooling oil is made to flow from the oil inlet port 4 through a route shown by arrow signs in a diagram to cool the edge faces of respective magnetic cores uniformly, is discharged from the oil outlet port 5 and is circulated by a pump. According to this method, said gaps 7 are formed in the saturable magnetic core by three pieces of tape-wound magnetic cores 6-1-6-3, which are arranged concentrically and provided with different configurations.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、エキシマレーザ、銅蒸気レーザ等の放電励起
レーザや加速監等に用いられる高電圧パルス発生回路に
使用される磁気スイッチ用可飽和リアクトルに関するも
のである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention is directed to a saturable magnetic switch used in a discharge excitation laser such as an excimer laser or a copper vapor laser, or a high voltage pulse generation circuit used in acceleration monitoring, etc. It is related to reactors.

〔従来の技術〕[Conventional technology]

放電励起レーザの1つであるエキシマレーザ用筒電圧パ
ルス発生回路の1例を図6に示す。図6の回路は磁気圧
縮回路と呼はれるものであり、入力端31−32閾には
図示の極性で、直流電圧Viが印加されており、サイ2
トロン64がオフの期間に王コンデンサ66は図示の極
性に通常数十KVlitの電圧Viが印加されている。
FIG. 6 shows an example of a tube voltage pulse generation circuit for an excimer laser, which is one type of discharge excitation laser. The circuit in FIG. 6 is called a magnetic compression circuit, and a DC voltage Vi is applied to the input terminals 31-32 thresholds with the polarities shown in the figure, and the size is 2.
While the TRON 64 is off, a voltage Vi of several tens of KVlit is normally applied to the capacitor 66 with the polarity shown.

本回路における可飽和リアクトル68は、サイラトロン
64がターンオンした後にコンデンサ67両端に印加さ
れる66と37のキャパシタンス、及びインダクタンス
35の時定数で定まるパルス幅の電圧ガを、エキシマレ
ーザの発振に必要な100n+s程度のパルス幅の電圧
ちに圧縮するために使用されるもので、この意味から磁
気スイッチとも呼はれる0なお同図において、33.4
2は主コンデンサ66の充電用インダクタンス、37.
39はピーキングコンデンサ、40は配線により生ずる
浮遊インダクタンス、41はエキシマレーザ主放電々極
である。
The saturable reactor 68 in this circuit generates a voltage with a pulse width determined by the capacitances 66 and 37 applied across the capacitor 67 after the thyratron 64 is turned on, and the time constant of the inductance 35, which is necessary for the oscillation of the excimer laser. It is used to compress a voltage with a pulse width of about 100n+s, and for this reason it is also called a magnetic switch.
2 is the charging inductance of the main capacitor 66, 37.
39 is a peaking capacitor, 40 is a floating inductance caused by wiring, and 41 is an excimer laser main discharge pole.

本回路においては、可飽和リアクトル38を用いること
でパルス圧縮が可能なため、サイラトロン34のターン
オン時に生ずるピーク損失、アフタカレント、及び反転
電流による損失を抑制することができ、エキシマレーザ
の高く少返し化、高出力化及び長寿命化が可能どなる。
In this circuit, since pulse compression is possible by using the saturable reactor 38, it is possible to suppress the peak loss, aftercurrent, and loss due to reversal current that occur when the thyratron 34 is turned on, and the excimer laser has a high return rate and a small amount. This makes it possible to achieve higher power output, higher output, and longer life.

図7はエキシマレーザ用高電圧パルス発生回路の別の例
であり、本回路は磁気アシスト回路と呼はれるものであ
る。本回路における可か和リアクトル38の役割は、図
示電流 の立上りを遅らせることにより、サイラトロン
64のターンオン時に生ずるスイッチング損失を低減さ
せることにあり、図6の回路と同様にエキシマレーザの
高くり返し化、高出力化及び長寿命化が可能となる。
FIG. 7 shows another example of a high voltage pulse generation circuit for excimer laser, and this circuit is called a magnetic assist circuit. The role of the reactive reactor 38 in this circuit is to reduce the switching loss that occurs when the thyratron 64 is turned on by delaying the rise of the indicated current. Higher output and longer life are possible.

上記用途における可#和磁心としては、非晶質磁性薄帯
を用い、絶縁耐圧を数十KV1度以上とするとともに渦
電流損を抑制するため層間に絶縁テープ、もしくは絶縁
コーティングを施した巻磁心、あるいはフェライト磁心
が用いられている。
The magnetic core for the above applications uses an amorphous magnetic ribbon, and has a dielectric strength of several tens of KV1 degree or more, and a wound core with an insulating tape or insulating coating applied between the layers to suppress eddy current loss. , or a ferrite magnetic core is used.

特に数百Hz以上の高くシ返し用途で用いる場合には、
図5のように油冷の可能な構造とすることが行なわれる
。同図において、21は入力端あるいは出力端、22は
同軸円筒導体、23は出力端あるいは入力端、24は油
入口、25は油出口、26は可飽和磁心、27は可飽和
磁心(支)走用絶縁リンク、28は入出力端の絶縁と油
をシールするための絶縁体である。この可飽和リアクト
ルでは、油をポンプにより循環することで磁心の冷却を
図っている。
Especially when used for high frequency applications of several hundred Hz or more,
As shown in FIG. 5, a structure capable of oil cooling is used. In the figure, 21 is an input end or an output end, 22 is a coaxial cylindrical conductor, 23 is an output end or an input end, 24 is an oil inlet, 25 is an oil outlet, 26 is a saturable magnetic core, and 27 is a saturable magnetic core (support). The running insulating link 28 is an insulator for insulating the input and output ends and sealing oil. In this saturable reactor, the magnetic core is cooled by circulating oil using a pump.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

上記従来技術による油冷式昼電圧パルス発生装置用可飽
和リアクトルにおいては、くり返し周波数を高めた場合
(例えばIKHz程度以上)、可飽和磁心に磁心損失に
よるヒートスポットが発生し、可飽和リアクトルとして
の特性が、稼動開始後、短時間で劣化するとともに、極
端な場合にはヒートスポット発生ケ所の磁気特性が大幅
に劣化してしまい、動作停止後、再稼動させた際に初期
の特性を発揮し得ないという問題がある。このヒートス
ポットの発生による磁気特性の劣化は、特に非晶質磁性
薄帯を用いた場合に顕著なことはよく知られている。
In the saturable reactor for an oil-cooled daytime voltage pulse generator according to the above-mentioned conventional technology, when the repetition frequency is increased (for example, about IKHz or more), a heat spot is generated in the saturable magnetic core due to core loss, and the saturable reactor cannot be used as a saturable reactor. The characteristics deteriorate in a short period of time after the start of operation, and in extreme cases, the magnetic characteristics at the location where the heat spot occurs will deteriorate significantly, and the initial characteristics will not be exhibited when restarted after the operation has stopped. The problem is that you can't get it. It is well known that the deterioration of magnetic properties due to the generation of heat spots is particularly noticeable when an amorphous magnetic ribbon is used.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は、非晶質磁性薄帯等を用い絶縁耐圧を数十KV
程度以上とするため層間に絶縁テープもしくは絶縁コー
ティングを施した寸法の異なる複数の巻磁心を同心円状
に配置するとともに、各巻磁心間に冷却のだめの空隙を
有する構造とした可飽和磁心を用いることによυ磁心の
冷却効率を著しく向上させた高電圧パルス発生装置用可
飽和リアクトルを提供するものである。
The present invention uses an amorphous magnetic ribbon or the like to increase the dielectric strength to several tens of kilovolts.
In order to achieve this, we decided to use a saturable magnetic core with a structure in which multiple wound magnetic cores of different dimensions with insulating tape or insulating coating applied between the layers are arranged concentrically, and a cooling reservoir gap is provided between each wound magnetic core. The present invention provides a saturable reactor for a high-voltage pulse generator that significantly improves the cooling efficiency of a υ magnetic core.

〔実施例〕〔Example〕

以下、本発明を実施例によシ説明する。 The present invention will be explained below using examples.

図1は、本発明による高電圧パルス発生装置用可飽和リ
アクトルの一実施例断面図である。図中、1は入力端も
しくは出力端、2は同軸円筒導体、6は出力端もしくは
入力端、4は油入口、5は油出口、6は非晶質磁性薄帯
を用い層間に絶縁テープもしくは絶縁コーティングを施
した巻磁心、7は巻磁心6の冷却効率を高めるために設
けられた空隙、8は巻磁心と同軸円筒導体が接触しない
ようにするとともに巻磁心の端面を均一に油冷し得るよ
うにするための絶縁体カイトであり、9は入出力端の絶
縁と油をシールする機能を有する絶縁体である。また、
図中、冷却油は油入口4から図示矢印のような経路を流
れ、各磁心の端面を均一に冷却し、油出口5を出てポン
プにip循環される。なお、本実施例では冷却油として
、粘度5−/Sのシリコン油を用いた。
FIG. 1 is a sectional view of an embodiment of a saturable reactor for a high voltage pulse generator according to the present invention. In the figure, 1 is an input end or an output end, 2 is a coaxial cylindrical conductor, 6 is an output end or an input end, 4 is an oil inlet, 5 is an oil outlet, 6 is an amorphous magnetic ribbon, and insulating tape or The wound magnetic core is coated with an insulating coating, 7 is a gap provided to improve the cooling efficiency of the wound magnetic core 6, and 8 is a space provided to prevent the wound magnetic core and the coaxial cylindrical conductor from coming into contact with each other, and the end face of the wound magnetic core is evenly cooled with oil. 9 is an insulator having the function of insulating the input and output terminals and sealing oil. Also,
In the figure, cooling oil flows from an oil inlet 4 along a path shown by an arrow in the figure, cools the end face of each magnetic core uniformly, exits an oil outlet 5, and is circulated by IP to a pump. In this example, silicone oil with a viscosity of 5-/S was used as the cooling oil.

図2Fi、図1で用いた可飽和磁心の極数を示したもの
であり、本例では同心円状に配置された形状の共なる6
ケの巻磁心6−1 、6−2 、6−3により、冷却の
ための環状”l隙7−1及び7−2が設けられ、隣り合
う巻磁心は前記冷却のための環状空隙間に絶縁体スペー
サを挿入することにより固定されている。
Figure 2Fi shows the number of poles of the saturable magnetic core used in Figure 1, and in this example, the number of poles of the saturable magnetic core used in Figure 1 is 6.
An annular gap 7-1 and 7-2 for cooling is provided by the wound magnetic cores 6-1, 6-2, and 6-3, and adjacent wound magnetic cores are placed in the annular gap for cooling. It is fixed by inserting an insulating spacer.

図6は、図2で用いた巻磁心(5−1,6−2゜6−6
の構造を示したものであり、本例では非晶質磁性薄帯の
層間をポリエステルフィルムテープで絶縁するようにし
て栃成された巻磁心11が変形しないようにステンレス
製リンク12及び16で、各々巻磁心11の内周、及び
外周を固定している。
Figure 6 shows the wound magnetic core (5-1, 6-2゜6-6
In this example, stainless steel links 12 and 16 are used to prevent the wound core 11, which is formed by insulating the layers of amorphous magnetic ribbon with polyester film tape, from being deformed. The inner circumference and outer circumference of each wound magnetic core 11 are fixed.

図4は、図1で用いた巻磁心と同軸円筒導体が接触しな
いようにするとともに巻磁心の端面を均一に油冷し得る
ようにするための絶縁体ガイド8の構造を示したもので
ある。本例において14及び15は巻磁心と同軸円筒導
体が接触しないようにするためのスペーサ部であシ、1
6は冷却油の流れる方向を定めるための空隙でロシ、巻
磁心の端面を均一に冷却し得るような位置に多数設けで
ある。
FIG. 4 shows the structure of the insulator guide 8 used in FIG. 1 to prevent contact between the wound magnetic core and the coaxial cylindrical conductor and to uniformly cool the end face of the wound magnetic core with oil. . In this example, 14 and 15 are spacer parts to prevent the wound magnetic core and the coaxial cylindrical conductor from coming into contact with each other.
Numeral 6 denotes air gaps for determining the flow direction of the cooling oil, which are provided in large numbers at positions where the end faces of the wound magnetic core can be uniformly cooled.

以上の栃成とすることにより可飽和磁心の表面積を大き
くすることができ動作時の磁心損失による発熱に対する
冷却効率の向上が期待できる。また、巻磁心、特に本実
施例のように層間絶縁した巻磁心の場合、磁心の径方向
への熱伝導率は磁心の径方向と垂直な方向への熱伝導率
に比べて大幅に悪いため、冷麹効率を高める上では本実
於例のように磁心の端面を均一に冷却し得る衛成とする
ことが有効と考えられる。
By adopting the above structure, the surface area of the saturable magnetic core can be increased, and an improvement in cooling efficiency against heat generated by core loss during operation can be expected. In addition, in the case of a wound magnetic core, especially in the case of a wound magnetic core with interlayer insulation as in this example, the thermal conductivity in the radial direction of the magnetic core is significantly lower than that in the direction perpendicular to the radial direction of the magnetic core. In order to increase the cold koji efficiency, it is considered effective to use a structure that can uniformly cool the end face of the magnetic core, as in this example.

表1は、本実施例における高電圧パルス発生装置用可飽
和リアクトルと図5に示す従来例を図6のKtFエキシ
マレーザ装置に使用したときの圧縮比(図6において、
サイラトロン64がターンオン後に生じるコンデンサ3
7の端子電圧−のパルス幅をコンデンサ69の端子電圧
1のパルス幅で割った値。)の時間変化を比軟したもの
である。
Table 1 shows the compression ratio (in FIG. 6) when the saturable reactor for the high voltage pulse generator according to this embodiment and the conventional example shown in FIG.
Capacitor 3 generated after thyratron 64 turns on
The value obtained by dividing the pulse width of the terminal voltage 7 of - by the pulse width of the terminal voltage 1 of the capacitor 69. ) is a comparative example of the change over time.

本発明では圧縮比の時間変化が極めて小さく実用上十分
な特性を有するのに対し、従来例では主に磁心内部で発
生したヒートスポットの影響により可飽和磁心の飽和磁
束密度低下によシ圧縮比の大幅な低下が生じていること
がわかる。
In the present invention, the time change in the compression ratio is extremely small and has sufficient characteristics for practical use, whereas in the conventional example, the compression ratio is reduced due to a decrease in the saturation magnetic flux density of the saturable magnetic core mainly due to the influence of heat spots generated inside the magnetic core. It can be seen that a significant decrease has occurred.

表2は、表1と同一の装置、同−条件下で5分間動作後
、可飽和磁心の冷却に十分な時間をおいた後に栴度動作
させる試験を行なったときの動作再開時の圧縮比の動作
回数による特性変化を示したものである。本発明の場合
における圧縮比は動作回数に依存しないのに対し、従来
例では動作時のヒートスポットによる可飽和磁心磁気特
性劣化が生じていることがわかる。
Table 2 shows the compression ratio at the time of resumption of operation when the same equipment as in Table 1 was operated for 5 minutes under the same conditions, and after sufficient time had elapsed for the saturable magnetic core to cool down, it was operated at low temperature. This shows the change in characteristics depending on the number of operations. It can be seen that the compression ratio in the case of the present invention does not depend on the number of operations, whereas in the conventional example, the saturable core magnetic characteristics deteriorate due to heat spots during operation.

表      1 人カニVi=DC30KV コンデンを容t:コンデンサ36 、37 、39いず
れも15nF 可能’ML I)アクドル(本発明、従来例とも以下同
一)コバルト基アモルファス 有効断面積 1.2X10−を4ケ使用平均磁路長 3
80X10  m くり返し周波数  I KHz 表      2 人カニVi−DC30KV コンデンサ容量:コンデンサ!+6 、37 、39い
ずれも15nF 可飽和リアクトル(本発明、従来例とも以下同一)コバ
ルト基アモルファス 有効断面積 1.2X10 −を4ケ使用平均磁路長 
380 X 10  m 〈シ返し周波数  IKHz 1回の動作時間  5分間 〔発明の効果〕 以上紗明したように本発明によれば、磁心を効果的に冷
却することができるため巻磁心を用いて構成した油冷式
高電圧パルス発生装置用可飽和リアクトルにおいて問題
であったヒートスポットの発生を防止することが可能と
なる。
Table 1 Capacity of capacitor Vi=DC30KV Capacitor t: Capacitors 36, 37, and 39 are all 15 nF Possible' ML Average magnetic path length used 3
80X10 m Repetition frequency I KHz Table 2 Human crab Vi-DC30KV Capacity: Capacitor! +6, 37, 39 are all 15nF Saturable reactor (same as below for both the present invention and conventional example) Cobalt-based amorphous effective cross-sectional area 1.2X10 - 4 pieces used Average magnetic path length
380 x 10 m <Return frequency IKHz Single operation time 5 minutes [Effects of the invention] As explained above, according to the present invention, since the magnetic core can be effectively cooled, a wound magnetic core is used. It becomes possible to prevent the occurrence of heat spots, which was a problem in the saturable reactor for an oil-cooled high-voltage pulse generator.

特に磁心として非晶質磁性薄帯のようにヒートショック
による特性変化が不可逆的な材質を用いた場合には、ヒ
ートスポットの発生による磁心の極部的な結晶化あるい
は変質による特性劣化を防止できる等の効果もある。
In particular, when a material such as an amorphous magnetic ribbon is used for the magnetic core, whose characteristics change irreversibly due to heat shock, it is possible to prevent characteristic deterioration due to crystallization or alteration in the poles of the magnetic core due to the generation of heat spots. There are also other effects.

また、高く9返し化による特性劣化が少ないため従来用
いられていなかった高<シ返し動作の必要な用途での利
用も可能である。
Furthermore, since there is little characteristic deterioration due to high nine-turn operation, it can be used in applications requiring high < nine-turn operation, which have not been used in the past.

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

第1図は本発明による高電圧パルス発生装置用可飽和リ
アクトルの一実施例を示す構成断面図、第2図は本発明
における寸法の異なる巻磁心を用いて構成した可飽和磁
心の構造図、第6図は本発明による可飽和磁心を構成す
る巻磁心の構造図、第4図は本発明による可飽和磁心と
同軸円筒導体の接触を防止するとともに冷却油のガイド
を兼ねる絶縁体の構造図、第5図は従来方式の高電圧パ
ルス発生装置用可飽和リアクトルの構成断面図、第6図
は磁気圧縮型高電圧パルス発生回路を有するエキシマレ
ーザの回路構成図、第7図は磁気アシスト型高電圧パル
ス発生回路を有するエキシマレーザ回路構成図である。
FIG. 1 is a structural sectional view showing an embodiment of a saturable reactor for a high voltage pulse generator according to the present invention, and FIG. 2 is a structural diagram of a saturable magnetic core constructed using wound cores of different dimensions in the present invention. Fig. 6 is a structural diagram of a wound magnetic core that constitutes a saturable magnetic core according to the present invention, and Fig. 4 is a structural diagram of an insulator that prevents contact between the saturable magnetic core and a coaxial cylindrical conductor according to the present invention and also serves as a guide for cooling oil. , Fig. 5 is a cross-sectional view of the structure of a saturable reactor for a conventional high-voltage pulse generator, Fig. 6 is a circuit block diagram of an excimer laser having a magnetic compression type high-voltage pulse generation circuit, and Fig. 7 is a magnetically assisted type excimer laser. FIG. 2 is a configuration diagram of an excimer laser circuit having a high voltage pulse generation circuit.

Claims (9)

【特許請求の範囲】[Claims] (1)高電圧パルス発生装置用可飽和リアクトルにおい
て、可飽和磁心として、同心円状に配置した際に各磁心
間に冷却のための空隙が生じるような寸法とした寸法の
異なる複数の巻磁心を同心円状に配置して構成された可
飽和磁心を用いることを特徴とする高電圧パルス発生装
置用可飽和リアクトル。
(1) In a saturable reactor for a high-voltage pulse generator, a plurality of wound magnetic cores with different dimensions are used as the saturable magnetic core, and the dimensions are such that when arranged concentrically, air gaps are created between each magnetic core for cooling. A saturable reactor for a high voltage pulse generator, characterized by using a saturable magnetic core arranged concentrically.
(2)特許請求の範囲第1項記載の高電圧パルス発生装
置用可飽和リアクトルにおいて、前記寸法の異なる複数
の巻磁心を同心円状に配置して構成された可飽和磁心を
複数個組み合わせて用いることを特徴とする高電圧パル
ス発生装置用可飽和リアクトル。
(2) In the saturable reactor for a high-voltage pulse generator according to claim 1, a plurality of saturable magnetic cores configured by concentrically arranging a plurality of wound magnetic cores having different dimensions is used in combination. A saturable reactor for a high voltage pulse generator, characterized by:
(3)特許請求の範囲第1項、又は第2項記載の高電圧
パルス発生装置用可飽和リアクトルにおいて、前記巻磁
心の端面を均一に冷却する構成を設け、動作時の磁心損
失による磁心のヒートスポットの発生を防止したことを
特徴とする高電圧パルス発生装置用可飽和リアクトル。
(3) In the saturable reactor for a high voltage pulse generator according to claim 1 or 2, a configuration is provided to uniformly cool the end face of the wound core, and the core loss due to the core loss during operation is provided. A saturable reactor for a high voltage pulse generator characterized by preventing the generation of heat spots.
(4)特許請求の範囲第1項から第3項に記載の高電圧
パルス発生装置用可飽和リアクトルにおいて、前記巻磁
心の端面の方向に前記巻磁心を均一に冷却するための絶
縁体で構成されたガイドを設けたことを特徴とする高電
圧発生装置用可飽和リアクトル。
(4) In the saturable reactor for a high voltage pulse generator according to claims 1 to 3, the saturable reactor is composed of an insulator for uniformly cooling the wound core in the direction of the end face of the wound magnetic core. A saturable reactor for a high voltage generator, characterized in that it is provided with a guided guide.
(5)特許請求の範囲第1項から第4項に記載の高電圧
パルス発生装置用可飽和リアクトルにおいて、前記同心
円状に配置された寸法の異なる複数の巻磁心は、いずれ
も内周と外周に変形を防止するための固定リンクが設け
られていることを特徴とする高電圧パルス発生装置用可
飽和リアクトル。
(5) In the saturable reactor for a high voltage pulse generator according to claims 1 to 4, each of the plurality of wound magnetic cores having different dimensions arranged concentrically has an inner periphery and an outer periphery. A saturable reactor for a high voltage pulse generator, characterized in that a fixed link is provided to prevent deformation of the reactor.
(6)特許請求の範囲第1項から第5項に記載の高電圧
パルス発生装置用可飽和リアクトルにおいて、前記同心
円状に配置された寸法の異なる複数の巻磁心は、隣り合
う巻磁心間に生ずる冷却のための空隙部に設けられたス
ペーサにより固定されることを特徴とする高電圧パルス
発生装置用可飽和リアクトル。
(6) In the saturable reactor for a high voltage pulse generator according to claims 1 to 5, the plurality of wound cores having different dimensions arranged concentrically are arranged between adjacent wound cores. A saturable reactor for a high voltage pulse generator, characterized in that the reactor is fixed by a spacer provided in a gap for cooling.
(7)特許請求の範囲第1項から第6項記載の高電圧パ
ルス発生装置用可飽和リアクトルにおいて、前記可飽和
磁心として磁性薄帯の層間に絶縁テープ、又は絶縁コー
ティングを施して構成した巻磁心を用いることを特徴と
する高電圧パルス発生装置用可飽和リアクトル。
(7) In the saturable reactor for a high voltage pulse generator according to claims 1 to 6, the saturable magnetic core is a winding formed by applying an insulating tape or an insulating coating between layers of magnetic ribbon. A saturable reactor for a high voltage pulse generator characterized by using a magnetic core.
(8)特許請求の範囲第1項から第7項記載の高電圧パ
ルス発生装置用可飽和リアクトルにおいて、前記可飽和
リアクトルとして非晶質磁性薄帯を用いることを特徴と
した高電圧パルス発生装置用可飽和リアクトル。
(8) A saturable reactor for a high voltage pulse generator according to claims 1 to 7, characterized in that an amorphous magnetic ribbon is used as the saturable reactor. Saturation reactor available for use.
(9)特許請求の範囲第18から第8項記載の高電圧パ
ルス発生装置用可飽和リアクトルにおいて 変圧器油、
あるいはシリコン油等の絶縁油を用いて前記可飽和磁心
を冷却することを特徴とする高電圧パルス発生装置用可
飽和リアクトル。
(9) In the saturable reactor for a high voltage pulse generator according to claims 18 to 8, transformer oil;
Alternatively, a saturable reactor for a high voltage pulse generator, characterized in that the saturable magnetic core is cooled using insulating oil such as silicone oil.
JP62313644A 1987-12-11 1987-12-11 Saturable reactor for high-voltage pulse generating device Pending JPH01157280A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62313644A JPH01157280A (en) 1987-12-11 1987-12-11 Saturable reactor for high-voltage pulse generating device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62313644A JPH01157280A (en) 1987-12-11 1987-12-11 Saturable reactor for high-voltage pulse generating device

Publications (1)

Publication Number Publication Date
JPH01157280A true JPH01157280A (en) 1989-06-20

Family

ID=18043792

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62313644A Pending JPH01157280A (en) 1987-12-11 1987-12-11 Saturable reactor for high-voltage pulse generating device

Country Status (1)

Country Link
JP (1) JPH01157280A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112383240A (en) * 2020-10-15 2021-02-19 中国人民解放军空军工程大学 Multi-pulse discharging device and method based on magnetic switch

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63314820A (en) * 1987-06-18 1988-12-22 Toshiba Corp Saturable reactor

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63314820A (en) * 1987-06-18 1988-12-22 Toshiba Corp Saturable reactor

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112383240A (en) * 2020-10-15 2021-02-19 中国人民解放军空军工程大学 Multi-pulse discharging device and method based on magnetic switch

Similar Documents

Publication Publication Date Title
JPH0258811A (en) Magnetic component for high voltage pulse generator
US5448580A (en) Air and water cooled modulator
JP3752978B2 (en) Winding device and high voltage pulse generation circuit using winding device
CA2261316C (en) Ignition device for a discharge lamp and method for igniting a discharge lamp
JPH01157280A (en) Saturable reactor for high-voltage pulse generating device
JPH0198206A (en) Magnetic component for high-voltage pulse generator
JP2645459B2 (en) Saturable reactor for high voltage pulse generator
JPH03159218A (en) High tension pulse generating magnetic part
JP2703631B2 (en) Iron core cooling method
CA1293539C (en) Magnetic device for high-voltage pulse generating apparatuses
JPH03240212A (en) High voltage pulse generating magnetic part and high voltage pulse generator using the same
JP3132251B2 (en) Magnetic switch for pulse power supply
JPH03212908A (en) Magnetic core part for generation high voltage pulse
JP2778708B2 (en) Magnetic components for high-voltage pulse generation
US5177762A (en) Saturable reactor
JPH0716057B2 (en) Magnetic parts for high voltage pulse generation
EP0674803A1 (en) Air-cooled magnetic cores
JP3438825B2 (en) Wound core, method of manufacturing wound core, high-voltage pulse generator, and laser device
JPH0437007A (en) Gas laser oscillator
JPH04283908A (en) Saturable reactor for generating high-voltage pulse
JPH0547967B2 (en)
SU1121717A1 (en) High-voltage electronic device
JP3535308B2 (en) Pulse generation circuit
JPH0529123B2 (en)
JPH07111441A (en) Pulse power supply circuit