JPH0342810A - Pulse transformer - Google Patents

Pulse transformer

Info

Publication number
JPH0342810A
JPH0342810A JP1177103A JP17710389A JPH0342810A JP H0342810 A JPH0342810 A JP H0342810A JP 1177103 A JP1177103 A JP 1177103A JP 17710389 A JP17710389 A JP 17710389A JP H0342810 A JPH0342810 A JP H0342810A
Authority
JP
Japan
Prior art keywords
winding
pulse
pulse transformer
transformer
coaxial cable
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
JP1177103A
Other languages
Japanese (ja)
Inventor
Katsuya Okamura
勝也 岡村
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP1177103A priority Critical patent/JPH0342810A/en
Publication of JPH0342810A publication Critical patent/JPH0342810A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/28Coils; Windings; Conductive connections
    • H01F27/2823Wires
    • H01F2027/2833Wires using coaxial cable as wire

Landscapes

  • Coils Of Transformers For General Uses (AREA)

Abstract

PURPOSE:To obtain a pulse transformer for achieving a compact and high-frequency pulse by constituting the winding of the transformer using a coaxial cable and by dividing the outer side conductor of this coaxial cable equally and connecting in parallel for forming a primary winding. CONSTITUTION:A coaxial cable 30 where an outer-side conductor 31 and a central conductor 32 are insulated by polyethylene vinyl is wound around a core 20 and the outer-side conductor 31 is cut off at 1/2 the total winding. This cut-off outer-side conductor 31 is connected in parallel, a winding-start side and winding-end side are set to a (u) and (v) terminals, respectively, which are connected to a pulse power supply 40. If current flowing from this pulse power supply 40 to the terminals (u) and (v) is set to I1, current which flows to the outer-side conductor 31 becomes I1/2 so that apparent primary winding becomes the same as a secondary winding but the actual ratio of winding becomes 1:2, which is a boost-type transformer.

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は、パルス変圧器に関する。[Detailed description of the invention] [Purpose of the invention] (Industrial application field) The present invention relates to pulse transformers.

(従来の技術) 従来からパルス状の大電流を得るために、高電圧に充電
されたコンデンサの回路を開閉する方法が用いられ、こ
の開閉素子には低圧の水素ガスを封入したサイラトロン
やガスギャップなどが使われてきた。しかし、このサイ
ラトロンやガスギャップは、放電時の発弧で電極が消耗
して寿命が短いので、代りに半導体素子が使われている
が、こ半導体素子はサイラトロンやガスギャップなどに
比べて耐電圧値が低いので、高電圧のパルス変圧器で昇
圧する必要がある。
(Prior art) Conventionally, in order to obtain a large pulse-like current, a method has been used to open and close the circuit of a capacitor charged to a high voltage. etc. have been used. However, these thyratrons and gas gaps have short lifespans because their electrodes wear out due to arcing during discharge, so semiconductor devices are used instead, but these semiconductor devices have a higher withstand voltage than thyratrons and gas gaps. Since the value is low, it is necessary to step up the voltage with a high voltage pulse transformer.

第3図は、半導体素子を使ったパルススイッチング回路
の一例を示す図で、半導体スイッチlOがオフ状態でコ
ンデンサ1に直流電源4で充電された後、半導体スイッ
チ1Gがオンされてコンデンサ1の電荷が放電され、こ
のパルス電流でパルス変圧器3の二次側に流れたパルス
電流でコンデンサ2は充電される。そしてこの電荷は、
例えばガスレーザ装置のレーザガスの励起やパルス磁場
の成虫に使われる。
FIG. 3 is a diagram showing an example of a pulse switching circuit using a semiconductor element. After the capacitor 1 is charged by the DC power supply 4 with the semiconductor switch 1O in the off state, the semiconductor switch 1G is turned on and the charge on the capacitor 1 is is discharged, and the capacitor 2 is charged by the pulse current flowing to the secondary side of the pulse transformer 3. And this charge is
For example, it is used to excite laser gas in gas laser equipment or to imitate pulsed magnetic fields.

ところで、このようにして出力されるパルスでは、コン
デンサ2に充電されるパルスの周波数の高さが要求され
、第3図ではこの周波数f。は、但し、 となるが、 Ls :パルストランス3の二次側からみたパルストラ
ンス3の洩れイ ンダクタンス C1:コンデンサ1のパルストランス 3の二次側に換算したキャパタ シタンス C2:コンデンサ2のキャパタシ タンス 通常はC,=C2に設定されるので、 となる。
By the way, the pulse output in this manner requires a high frequency of the pulse that charges the capacitor 2, and in FIG. 3, this frequency is f. However, Ls: Leakage inductance of the pulse transformer 3 seen from the secondary side of the pulse transformer 3 C1: Capacitance of the capacitor 1 converted to the secondary side of the pulse transformer 3 C2: Capacitance of the capacitor 2 Since the resistance is normally set to C,=C2, it becomes as follows.

したがって、出力パルスの周波数f0を上げるためには
、LmかC,、C2を小さくしなければならないが、後
者のC1、C2を小さくすると出力が減るので、前者の
L3を減らす必要がある。
Therefore, in order to increase the frequency f0 of the output pulse, it is necessary to reduce Lm or C, C2, but since reducing the latter C1 and C2 reduces the output, it is necessary to reduce the former L3.

第4図に従来のパルス変圧器の巻線の部分断面図を示す
FIG. 4 shows a partial sectional view of a winding of a conventional pulse transformer.

同図では、低圧巻線21と高圧巻線22はそれぞれ直径
の異なる絶縁筒23A、 23Bに巻き付けられて鉄心
20に挿着されている。
In the figure, a low-voltage winding 21 and a high-voltage winding 22 are wound around insulating tubes 23A and 23B having different diameters, respectively, and are inserted into the iron core 20.

(発明が解決しようとする課題) ところがこのような構成のパルス変圧器3においては、
パルス変圧器3の洩れインダクタンスL3は、巻線の積
圧、直径9巻回数とともに高・低圧の巻線21.22間
の間隔dに大きく影響する。
(Problem to be solved by the invention) However, in the pulse transformer 3 having such a configuration,
The leakage inductance L3 of the pulse transformer 3 greatly influences the stacked pressure of the windings, the number of turns (9 turns in diameter), and the distance d between the high and low voltage windings 21 and 22.

しかるに従来のパルス変圧器3では、間隔dは巻線21
.22間の絶縁耐力に制約されて限度がある。
However, in the conventional pulse transformer 3, the spacing d is
.. There is a limit due to the dielectric strength between the two.

そのため、もし、変圧器を複数個並列に接続すると、外
形が大きくなる。
Therefore, if multiple transformers are connected in parallel, the external size will increase.

そこで、本発明の目的は、小形で高周波のパルスを得る
ことのできるパルス変圧器を得ることである。
SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a pulse transformer that is small and can generate high-frequency pulses.

[発明の構成] (課題を解決するための手段と作用) 本発明は、−次側に印加されたパルス電圧を昇圧するパ
ルス変圧器において、変圧器の巻線を同軸ケーブルで構
威し、この同軸ケーブルの外側導体を複数に等分割して
並列に接続して一次巻線として、洩れインダクタンスを
減らして、小形で周波数の高いパルスを出力することの
できるパルス変圧器である。
[Structure of the Invention] (Means and Effects for Solving the Problems) The present invention provides a pulse transformer that boosts a pulse voltage applied to the negative side, in which the winding of the transformer is configured with a coaxial cable, The outer conductor of this coaxial cable is divided into a plurality of equal parts and connected in parallel to form a primary winding, thereby reducing leakage inductance and producing a compact pulse transformer that can output high-frequency pulses.

(実施例) 以下、本発明のパルス変圧器の一実施例を図面を参照し
て説明する。
(Embodiment) Hereinafter, one embodiment of the pulse transformer of the present invention will be described with reference to the drawings.

第1図は、パルス変圧器の鉄心20に一次と二次のコイ
ルの巻数比が1対2に巻線が巻かれた斜視図である。
FIG. 1 is a perspective view of a pulse transformer in which windings are wound around an iron core 20 with a turns ratio of 1:2 between primary and secondary coils.

すなわち、第1図において、鉄心20には外側導体31
と中心導体32がポリエチレンビニールで絶縁された同
軸ケーブル30が巻き付けられ、全巻数の2分の1のと
ころで外側導体31は切断され、この切断された外側導
体31は並列に接続され、巻き始め側は低圧側のU端子
、巻き終り側は同じくv端子として図示しないパルス電
源にそれぞれ接続されている。そして、中心導体32は
、巻き始め側のU端子と巻き終り側のV端子が図示しな
い二次側のコンデンサに接続されている。
That is, in FIG. 1, the iron core 20 has an outer conductor 31.
A coaxial cable 30 with a center conductor 32 insulated with polyethylene vinyl is wound, and the outer conductor 31 is cut at one-half of the total number of turns.The cut outer conductors 31 are connected in parallel, and the winding start side is connected to a pulse power source (not shown) as a U terminal on the low voltage side, and as a V terminal on the winding end side. The center conductor 32 has a U terminal on the winding start side and a V terminal on the winding end side connected to a secondary side capacitor (not shown).

第2図は第1図の接続図を示す。FIG. 2 shows the connection diagram of FIG.

第2図において、パルス電源40から端子u、  vに
流れる電源を11とすれば、外側導体31に分流した電
流は11/2となるので、見かけ上の一次巻線は二次巻
線と同巻数であるが、実際には巻数比が1:2の昇圧変
圧器となっている。
In Figure 2, if the power flowing from the pulse power source 40 to the terminals u and v is 11, the current shunted to the outer conductor 31 is 11/2, so the apparent primary winding is the same as the secondary winding. In reality, it is a step-up transformer with a turns ratio of 1:2.

そして、このパルス変圧器では、同軸ケーブル30の中
心導体32と外側導体31には同一大きさの電流が流れ
るために、磁束は完全に打ち消され、その結果洩れ磁束
は減るので、洩れインダクタンスは極めて小さくなる。
In this pulse transformer, since the same magnitude of current flows through the center conductor 32 and outer conductor 31 of the coaxial cable 30, the magnetic flux is completely canceled out, and as a result, the leakage magnetic flux is reduced, so the leakage inductance is extremely low. becomes smaller.

そして、従来のような絶縁筒が要らないので、小形で高
周波のパルスを得ることのできるパルス変圧器とするこ
とができる。
Further, since an insulating tube as in the conventional case is not required, a pulse transformer that is small and can obtain high-frequency pulses can be provided.

なお、上記実施例では、昇圧比が1:2の例で説明した
が、外側導体31の並列数を増やすことでさらに昇圧比
を増やすことができ、絶縁筒が不要で、同軸ケーブル3
0を巻き付けるだけでよいので、部品数が減り製造容易
で信頼性のあるパルス変圧器を得ることができる。
In the above embodiment, the step-up ratio is 1:2, but the step-up ratio can be further increased by increasing the number of parallel outer conductors 31.
Since it is only necessary to wind 0, it is possible to obtain a reliable pulse transformer that is easy to manufacture and has a reduced number of parts.

又、上記実施例において、二次電圧が高いときには、同
軸ケーブル30を巻き付けた後に例えば工ボキシ樹脂で
真空含浸してもよい。
Further, in the above embodiment, when the secondary voltage is high, the coaxial cable 30 may be vacuum impregnated with, for example, a synthetic boxy resin after being wound.

[発明の効果] 以上、本発明によれば、−次側に印加されたパルス電圧
を昇圧するパルス変圧器において、変圧器の鉄心に同軸
ケーブルを巻き付け、外側導体を複数に分割して複数の
並列−次巻線としたので、洩れインダクタンスが小さく
、小形で高周波のパルスを出力することのできるパルス
変圧器を得ることができる。
[Effects of the Invention] As described above, according to the present invention, in a pulse transformer that boosts the pulse voltage applied to the negative side, a coaxial cable is wound around the iron core of the transformer, and the outer conductor is divided into a plurality of parts. Since the parallel windings are used, a pulse transformer with small leakage inductance and capable of outputting high-frequency pulses can be obtained.

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

第1図は本発明のパルス変圧器の一実施例を示す斜視図
、第2図は本発明のパルス変圧器の作用を示す接続図、
第3図は従来のパルス変圧器を示す接続図、第4図は従
来のパルス変圧器の作用を示す部分詳細図である。
FIG. 1 is a perspective view showing an embodiment of the pulse transformer of the present invention, FIG. 2 is a connection diagram showing the operation of the pulse transformer of the present invention,
FIG. 3 is a connection diagram showing a conventional pulse transformer, and FIG. 4 is a partially detailed diagram showing the operation of the conventional pulse transformer.

Claims (1)

【特許請求の範囲】 一次側に印加されたパルス電圧を昇圧するパルス変圧器
において、 このパルス変圧器の巻線を同軸ケーブルで構成し、この
同軸ケーブルの外側導体を複数に等分割して並列に接続
して一次巻線としたことを特徴とするパルス変圧器。
[Claims] In a pulse transformer that boosts the pulse voltage applied to the primary side, the winding of the pulse transformer is composed of a coaxial cable, and the outer conductor of the coaxial cable is divided into a plurality of equal parts and paralleled. A pulse transformer characterized in that it is connected to a primary winding.
JP1177103A 1989-07-11 1989-07-11 Pulse transformer Pending JPH0342810A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1177103A JPH0342810A (en) 1989-07-11 1989-07-11 Pulse transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1177103A JPH0342810A (en) 1989-07-11 1989-07-11 Pulse transformer

Publications (1)

Publication Number Publication Date
JPH0342810A true JPH0342810A (en) 1991-02-25

Family

ID=16025201

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1177103A Pending JPH0342810A (en) 1989-07-11 1989-07-11 Pulse transformer

Country Status (1)

Country Link
JP (1) JPH0342810A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20020007098A (en) * 2000-07-15 2002-01-26 박선순 A high frequency power apparatus using a complete coupling transformer
KR20030071091A (en) * 2002-02-27 2003-09-03 유영일 Ionizing apparatus
KR100435253B1 (en) * 2001-10-26 2004-06-11 실버레이 주식회사 Manufacture apparatus for silver solvent
KR20050105909A (en) * 2004-05-03 2005-11-08 이선희 A bathtub water convert to colloidal silver water apparatus

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20020007098A (en) * 2000-07-15 2002-01-26 박선순 A high frequency power apparatus using a complete coupling transformer
KR100435253B1 (en) * 2001-10-26 2004-06-11 실버레이 주식회사 Manufacture apparatus for silver solvent
KR20030071091A (en) * 2002-02-27 2003-09-03 유영일 Ionizing apparatus
KR20050105909A (en) * 2004-05-03 2005-11-08 이선희 A bathtub water convert to colloidal silver water apparatus

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