JP2820973B2 - Corrugated line - Google Patents
Corrugated lineInfo
- Publication number
- JP2820973B2 JP2820973B2 JP23429189A JP23429189A JP2820973B2 JP 2820973 B2 JP2820973 B2 JP 2820973B2 JP 23429189 A JP23429189 A JP 23429189A JP 23429189 A JP23429189 A JP 23429189A JP 2820973 B2 JP2820973 B2 JP 2820973B2
- Authority
- JP
- Japan
- Prior art keywords
- waveform shaping
- line
- pulse
- outer electrode
- waveform
- 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.)
- Expired - Fee Related
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/09—Processes or apparatus for excitation, e.g. pumping
- H01S3/097—Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
Description
【発明の詳細な説明】 産業上の利用分野 本発明は、パルス回路に使用されるパルス波形成形線
路の改良に関するもので、粒子ビームや自由電子レーザ
ー等の発生用電源部のパルス回路に用いられる。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an improvement of a pulse waveform shaping line used for a pulse circuit, and is used for a pulse circuit of a power supply unit for generating a particle beam, a free electron laser, or the like. .
従来の技術 これらのパルス回路に用いられる波形成形線路は、例
えばインピーダンス1〜50Ω、電圧0.1〜10MV、パルス
幅10〜100nsというきわめて急峻な矩形波を形成するた
めに用いられる。2. Description of the Related Art Waveform shaping lines used in these pulse circuits are used to form a very steep rectangular wave having, for example, an impedance of 1 to 50Ω, a voltage of 0.1 to 10 MV, and a pulse width of 10 to 100 ns.
このような波形は、通常同軸円筒や平行平板による波
形成形線路を用いて、いわゆる進行波理論によるところ
の矩形波をえている。これらを用いた波形成形線路の実
施例を第3図に示す。Such a waveform is usually a rectangular wave according to the so-called traveling wave theory using a waveform shaping line made of a coaxial cylinder or a parallel plate. FIG. 3 shows an embodiment of a waveform shaping line using these.
高電圧のパルス電源2は第1のスイッチ3を閉じるこ
とによって、波形成形線路1にパルス的に電荷を供給す
る電源部である。波形成形線路1は同軸円筒状の低圧側
外電極4と高圧側内電極5からなり、その間に誘電体6
が充填されて、等価回路的にサージインピーダンスZ1を
なす。絶縁物7を介して、内電極5と第1の端子8また
は、8aは電気的に接続されかつ図示しない方法で気密に
保持されている。同様に絶縁物7を介して、外電極4と
第2の端子9または9aまたは電気的に接続されかつ図示
しない方法で気密に保持されている。The high-voltage pulse power supply 2 is a power supply unit that supplies electric charges to the waveform shaping line 1 in a pulsed manner by closing the first switch 3. The corrugated line 1 comprises a coaxial cylindrical low voltage side outer electrode 4 and a high voltage side inner electrode 5, between which a dielectric 6
There is filled, the equivalent circuit to form a surge impedance Z 1. The inner electrode 5 and the first terminal 8 or 8a are electrically connected via the insulator 7 and are kept airtight by a method (not shown). Similarly, the external electrode 4 is electrically connected to the second terminal 9 or 9a or via an insulator 7 and is kept airtight by a method (not shown).
第1の端子8と第2の端子9とは第1のスイッチ3と
パルス電源2とで閉回路を構成する。第1の端子8aと第
2の端子9aとは、第2のスイッチ10と回路に既成するイ
ンダクタンス11ならびにインピーダンスZ2である負荷12
とで閉回路を構成する。The first terminal 8 and the second terminal 9 form a closed circuit with the first switch 3 and the pulse power supply 2. The first terminal 8a and the second terminal 9a, the load is the inductance 11 and the impedance Z 2 is established to the second switch 10 and the circuit 12
And constitute a closed circuit.
さて、動作について説明すると、第1のスイッチ3を
閉じて、パルス電源2よりサージインピーダンスZ1の波
形成形線路1にパルス的に電荷を供給し、外電極4と内
電極5の間の空間に誘電体6を充電してなるコンデンサ
を充電し、電圧が最大値付近に達した時点で、第2のス
イッチ10を閉じてインダクタンス11を介し、インピーダ
ンスZ2の負荷12へ電荷を供給する。Now, to describe the operation, close the first switch 3, the pulse to supply the charge from the pulse power source 2 to the waveform shaping line 1 of the surge impedance Z 1, the space between the inner electrode 5 and outer electrode 4 It charges the capacitor formed by charging the dielectric 6, when the voltage reaches the vicinity of the maximum value, via an inductance 11 closes the second switch 10 and supplies the charge to the load 12 of impedance Z 2.
負荷12に印加される電圧は、通常Z2=Z1となるようイ
ンピーダンス整合がとられているため、波形成形線路1
に充電される電圧の1/2の電圧の矩形波が負荷12に与え
られ、その矩形波のパルス幅は波形成形線路の長さに比
例したτとなる。式で表すと、下記の通りとなる。Since the voltage applied to the load 12 is normally impedance-matched so that Z 2 = Z 1 , the waveform shaping line 1
Is applied to the load 12, and the pulse width of the rectangular wave becomes τ proportional to the length of the waveform shaping line. This is represented by the following equation.
ε5:誘電体の比誘電率 c:光速 l:波形成形線路の長さ r1 :内電極の半径 r2 :外電極の半径 従って、パルス幅の長い矩形波を必要とする場合は、
比誘電率の大きい誘電体6を選んだりまたは波形成形線
路1の長さを長くする方法をとり、インピーダンスの設
定には、誘電体6の選定に加えて、外電極4と内電極5
の半径の比を適当に選ぶ等して設計していた。 ε 5 : dielectric constant of dielectric c: speed of light l: length of waveform forming line r 1 : radius of inner electrode r 2 : radius of outer electrode Therefore, when a rectangular wave with a long pulse width is required,
A method of selecting the dielectric 6 having a large relative dielectric constant or increasing the length of the waveform-shaped line 1 is adopted. In addition to the selection of the dielectric 6, the impedance of the outer electrode 4 and the inner electrode 5 is set.
The design was made by appropriately selecting the ratio of the radii.
発明が解決しようとする問題点 前述の通り従来の波形成形線路の考え方によるとイン
ピーダンスが高くて、かつパルス幅の長い矩形波を得よ
うとすると実現は困難なものとなった。例えば、波形成
形線路1の使用電圧が1MVインピーダンスZ1=50Ω、パ
ルス幅τ=300nsの矩形波を得たいとしたとき、耐電圧
特性の優れた誘電体6に比誘電率の小さい絶縁油(ε5
=2.2)と逆に大きい純水(ε5=80)を用いた場合の
波形成形線路1の設計寸法を第1表に示す。Problems to be Solved by the Invention As described above, it is difficult to realize a rectangular wave having a high impedance and a long pulse width according to the concept of the conventional waveform shaping line. For example, when it is desired to obtain a rectangular wave having a voltage of 1 MV impedance Z 1 = 50Ω and a pulse width τ = 300 ns in the waveform forming line 1, an insulating oil having a small relative dielectric constant is added to the dielectric 6 having excellent withstand voltage characteristics ( ε 5
Table 2.2 shows the design dimensions of the corrugated line 1 when large pure water (ε 5 = 80) is used.
なお、内電極5の表面最大電位傾度を150kV/cmとし
た。The surface maximum potential gradient of the inner electrode 5 was set to 150 kV / cm.
この表からも解るように絶縁油の場合は、あまりにも
長すぎ、また純水の場合は直径があまりにも大きすぎ
て、非現実的な形状になる欠点があった。 As can be seen from this table, in the case of insulating oil, the length was too long, and in the case of pure water, the diameter was too large, resulting in an unrealistic shape.
問題点を解決するための手段 本発明は、波形成形線路を分割して集中定数としての
複数のコンデンサに置き替え、その各々の間をコイルで
結合した複数段のパルス・フォーミング・ネットワーク
回路(以下PFN回路という)を構成させ、そのコンデン
サとコイルのインダクタンス値を適切な値に選定する事
によって、インピーダンス、パルス幅を決める方法を採
用すれば、現実的な波形成形線路を形成する事ができ
る。Means for Solving the Problems The present invention provides a multi-stage pulse forming network circuit (hereinafter, referred to as a multi-stage circuit) in which a waveform shaping line is divided and replaced with a plurality of capacitors as lumped constants, and each of them is connected by a coil. A PFN circuit) is formed, and by selecting the inductance values of the capacitor and the coil to appropriate values, a method of determining the impedance and the pulse width can be used to form a realistic waveform-shaped line.
すなわち、パルス電源より電荷の供給を受けて矩形波
を生成する波形成形線路に於いて、円筒、角形等の筒状
の外電極と、該外電極の内部に外電極と適正な距離を隔
てて、沿わせるよう長手方向に配置した複数個の内電極
との間に誘電体を充満させて、コンデンサを形成し、か
つその各々の内電極間をコイルで結合して、パルス・フ
ォーミング・ネットワーク回路を構成したことを特長と
する波形成形線路である。That is, in a waveform shaping line that receives a supply of electric charge from a pulse power supply and generates a rectangular wave, a cylindrical outer electrode such as a cylinder or a square, and an appropriate distance from the outer electrode inside the outer electrode. A pulse forming network circuit is formed by filling a dielectric between a plurality of inner electrodes arranged in the longitudinal direction so as to be aligned with each other, forming a capacitor, and coupling the respective inner electrodes with a coil. This is a waveform shaping line characterized by having the above configuration.
実施例 第1図(a)に、実施例を示す。上述の従来の第3図
と同一機能のものについては、同一符号を付してあるた
め、その説明を省略する。図示しない方法で固定された
内電極5aとコイル13は要求される矩形波の形状によっ
て、必要個数に分割して第3の端子14と14a間に直列に
電気的に接続されてn段のPFN回路を構成する。Embodiment FIG. 1A shows an embodiment. Components having the same functions as those of the above-described conventional FIG. 3 are denoted by the same reference numerals, and the description thereof will be omitted. The inner electrode 5a and the coil 13 fixed by a method not shown are divided into a required number according to a required rectangular wave shape, and are electrically connected in series between the third terminals 14 and 14a. Configure the circuit.
また、第1の端子8と第3の端子14と絶縁物7並びに
第1の端子8aと第3の端子14aと絶縁物7とが図示しな
い方法で、気密に保持されて第1の端子8と第3の端子
14とがまた、第1の端子8aと第3の端子14aとが電気的
に接続されている。Further, the first terminal 8, the third terminal 14, and the insulator 7 and the first terminal 8a, the third terminal 14a, and the insulator 7 are hermetically held by a method (not shown) so that the first terminal 8 And the third terminal
14 is also electrically connected to the first terminal 8a and the third terminal 14a.
さて、負荷12のインピーダンスZ2にマッチングをとっ
たPFN回路のインピーダンスZ1を構成するには、次の式
を満足させる必要がある。Now, to configure the impedance Z 1 of the PFN circuit took matching the impedance Z 2 of the load 12, it is necessary to satisfy the following equation.
L :波形成形線路の合成インダクタンス C :波形成形線路の内電極と外電極間で構成されるコン
デンサの合成静電容量 また、パルス巾τは次式で表わされる。 L: Synthetic inductance of waveform shaping line C: Synthetic capacitance of capacitor formed between inner electrode and outer electrode of waveform shaping line Further, pulse width τ is expressed by the following equation.
さて、要求矩形波の形状によって、このL、Cの値を
n段に分割するが、その各々の単位インダクタンスΔ
L、並びに単位コンデンサの静電容量ΔCは次式で表わ
される。 Now, the values of L and C are divided into n stages according to the shape of the required rectangular wave.
L and the capacitance ΔC of the unit capacitor are represented by the following equations.
次に動作を説明する。 Next, the operation will be described.
第1のスイッチ3を閉じて、パルス電源2よりインピ
ーダンスZ1の波形成形線路1にパルス的に電荷を供給
し、外電極4と複数の内電極5aの間の空間に誘電体6を
充填して成る複数の単位コンデンサをそれぞれ充電し、
電圧が最大値付近に達した時点で、第2のスイッチ10を
閉じてインダクタンス11を介し、負荷12へ電荷を供給す
る。第1図(b)には第1図(a)の波形成形線路の等
価回路を示す。この回路から判るように一般の矩形波を
生成するPFN回路である。従って、負荷12に印加される
電圧は通常Z2=Z1に定められるため、波形成形線路1に
充電された電圧の1/2が負荷12に与えられ、その矩形波
のパルス幅τは、 で与えられる。Closing the first switch 3, a pulsed manner to supply charge to the waveform shaping line 1 of the impedance Z 1 from the pulse power supply 2, the dielectric 6 was filled in a space between the outer electrode 4 and a plurality of inner electrodes 5a Each of the unit capacitors consisting of
When the voltage reaches the vicinity of the maximum value, the second switch 10 is closed to supply the charge to the load 12 via the inductance 11. FIG. 1 (b) shows an equivalent circuit of the waveform shaping line of FIG. 1 (a). As can be seen from this circuit, this is a PFN circuit that generates a general rectangular wave. Therefore, since the voltage applied to the load 12 is usually determined to be Z 2 = Z 1 , half of the voltage charged in the waveform shaping line 1 is given to the load 12, and the pulse width τ of the rectangular wave is Given by
さて、前述の例に従って同一条件、即ち波形成形線路
1の使用電圧が1MV、インピーダンスZ1=50Ω、パルス
幅τ=300nsとした時(内電極5aの表面最大電位傾度を1
50kV/cmとする)の各部の定数を示す。Now, under the same conditions according to the above-described example, that is, when the operating voltage of the waveform forming line 1 is 1 MV, the impedance Z 1 = 50Ω, and the pulse width τ = 300 ns (the surface maximum potential gradient of the inner electrode 5a is 1
50kV / cm) is shown for each part.
・波形成形線路の合成静電容量 C=3nF ・波形成形線路の合成インダクタンス L=7.5μH PFN回路の段数をn=5とした時 ・単位コンデンサの静電容量 ΔC=600pF ・単位インダクタンス ΔL=1.5μH 誘電体6に純水を用いた時の波形成形線路1の具体的
寸法は次の通りとなる。-Synthetic capacitance of the waveform shaping line C = 3nF-Synthetic inductance of the waveform shaping line L = 7.5μH When the number of stages of the PFN circuit is n = 5-Capacitance of the unit capacitor ΔC = 600pF-Unit inductance ΔL = 1.5 The specific dimensions of the wave-shaped line 1 when pure water is used for the μH dielectric 6 are as follows.
・内電極の外径 10.8cm ・外電極の内径 37.1cm ・内電極1ヶの長さ 16.7cm したがって、n=5段のため、内電極が5ヶ必要でか
つΔL=1.5μHの単位コイルが5ヶ必要となるが、こ
れらの寸法をすべて合わせても波形成形線路の全長は1.
5m以下とする事ができる。・ The outer diameter of the inner electrode is 10.8cm ・ The inner diameter of the outer electrode is 37.1cm ・ The length of one inner electrode is 16.7cm Therefore, since n = 5 stages, five inner electrodes are required and ΔL = 1.5μH unit coil Five are required, but the total length of the corrugated line is 1.
It can be less than 5m.
すなわち、第1表と比較すると明らかなように波形成
形線路1の寸法、直径方向は絶縁油を使用した場合と同
じだが、その長さは非常に短くてすむ実用的な高インピ
ーダンス、長パルス幅の波形成形線路を作ることができ
る。That is, as apparent from comparison with Table 1, the dimensions and the diameter direction of the corrugated line 1 are the same as those in the case where the insulating oil is used, but the length is very short. Can be made.
さて、第1図(a)は同軸円筒形形状で示したが、第
2図に他の実施例を示す。Now, FIG. 1A shows a coaxial cylindrical shape, but FIG. 2 shows another embodiment.
第2図は角形タンク形状を念頭において考えたもので
ある。同一機能のものについて、同一符号を付してお
り、その動作も同じであるので説明を省略する。FIG. 2 is based on a rectangular tank shape. The components having the same function are denoted by the same reference numerals, and the operation is the same, so that the description is omitted.
次に本発明の別の応用例を述べる。これまでは、PFN
回路の複数のコンデンサとインダクタンスの値は、平坦
な矩形波を成形するためにそれぞれ全て同じ値にしてい
たが、各コンデンサと各インダクタンスの値のどちらか
一方または両方をそれぞれ適当に場所毎に異なる値にな
る様にしておけば、矩形波の波尾を上げたり、あるいは
下げたりする事が意図的に出来るため、任意の波形を成
形することが容易となる。例えば、第1図(b)に於い
て複数の単位コンデンサΔCの値を全て同じにして、複
数の単位インダクタンスΔLの値を電源に近い方は低く
して、負荷に近づくにつれて段階的に高くしていけば、
負荷に発生する矩形波の波尾を持ち上げることができ
る。コンデンサの値の変更に比べてインダクタンスの値
の変更は一般的に容易であるので、この方法は出力波形
の調整に際しては有効な方法となる。Next, another application example of the present invention will be described. Until now, PFN
The values of multiple capacitors and the inductance of the circuit were all the same in order to form a flat rectangular wave, but one or both of the values of each of the capacitors and each of the inductances differed appropriately from place to place If the value is set to a value, the tail of the rectangular wave can be intentionally raised or lowered, so that an arbitrary waveform can be easily formed. For example, in FIG. 1 (b), the values of the plurality of unit capacitors ΔC are all the same, and the values of the plurality of unit inductances ΔL are decreased near the power supply and gradually increased as the load approaches. If you go,
The tail of the rectangular wave generated in the load can be lifted. Since the change of the inductance value is generally easier than the change of the capacitor value, this method is an effective method for adjusting the output waveform.
発明の効果 本発明によれば、従来の高電圧矩形波発生装置におい
て、その波形成形線路技術の概念をあまり変えることな
く、高インピーダンス、長パルス幅の矩形波を成形する
ことが可能である。そして構造的寸法のみならず、充填
する誘電体としてガス、油、純水、その他の絶縁体を適
正に選択することが可能である。また、コイルについて
は線、棒、パイプや板等によって、任意の形状および巻
数に作る事ができるので、コイルのインダクタンスとコ
ンデンサの静電容量を適正に選定することによって、イ
ンピーダンス数百Ω、パルス幅数μsに至る実用的な小
形の波形成形線路を作ることが可能となり、実用的価値
は大きい。According to the present invention, it is possible to form a high-impedance, long-pulse-width rectangular wave in a conventional high-voltage rectangular-wave generator without changing the concept of the waveform shaping line technology so much. In addition to the structural dimensions, it is possible to appropriately select gas, oil, pure water, and other insulators as the dielectric to be filled. Also, the coil can be made into any shape and number of turns using wires, rods, pipes, plates, etc., so by properly selecting the inductance of the coil and the capacitance of the capacitor, the impedance can be several hundred Ω, pulse It is possible to produce a practical small-sized waveform-shaped line having a width of several μs, which is of great practical value.
該1図は本発明の波形成形線路の一実施例で(a)は説
明図、(b)は等価回路図、第2図は本発明の波形成形
線路の他の実施例の要部切断斜視図、第3図は従来の波
形成形線路の説明図である 1:波形成形線路、2:パルス電源 4:外電極、5、5a:内電極、6:誘電体 13:コイルFIG. 1 is an embodiment of a waveform-shaped line according to the present invention, in which (a) is an explanatory diagram, (b) is an equivalent circuit diagram, and FIG. 2 is a perspective cut-away view of another embodiment of the waveform-shaped line according to the present invention. FIGS. 3A and 3B are explanatory diagrams of a conventional waveform shaping line. 1: Waveform shaping line, 2: Pulse power supply 4: Outer electrode, 5, 5a: Inner electrode, 6: Dielectric 13: Coil
───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.6,DB名) H03K 3/53 H03K 3/543 H03K 3/55 H03K 3/57 5H790 KK01──────────────────────────────────────────────────続 き Continued on the front page (58) Field surveyed (Int.Cl. 6 , DB name) H03K 3/53 H03K 3/543 H03K 3/55 H03K 3/57 5H790 KK01
Claims (1)
を生成する波形成形線路に於いて、円筒、角形等の筒状
の外電極と、該外電極の内部に外電極と適正な距離を隔
てて、沿わせるよう長手方向に配置した複数個の内電極
との間に誘電体を充満させて、コンデンサを形成し、か
つその各々の内電極間をコイルで結合して、パルス・フ
ォーミング・ネットワーク回路を構成したことを特徴と
する波形成形線路。1. A waveform shaping line which receives a charge from a pulse power supply to generate a rectangular wave, and has a cylindrical outer electrode having a proper distance from the outer electrode inside the outer electrode. A dielectric is filled between a plurality of inner electrodes arranged in a longitudinal direction so as to be separated from each other to form a capacitor, and each of the inner electrodes is connected with a coil to form pulse forming. -A waveform shaping line characterized by comprising a network circuit.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23429189A JP2820973B2 (en) | 1989-09-08 | 1989-09-08 | Corrugated line |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23429189A JP2820973B2 (en) | 1989-09-08 | 1989-09-08 | Corrugated line |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0396109A JPH0396109A (en) | 1991-04-22 |
| JP2820973B2 true JP2820973B2 (en) | 1998-11-05 |
Family
ID=16968686
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP23429189A Expired - Fee Related JP2820973B2 (en) | 1989-09-08 | 1989-09-08 | Corrugated line |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2820973B2 (en) |
-
1989
- 1989-09-08 JP JP23429189A patent/JP2820973B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0396109A (en) | 1991-04-22 |
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