JPH0613031A - Electrode of discharge tube having passing hole of high speed charged particle - Google Patents
Electrode of discharge tube having passing hole of high speed charged particleInfo
- Publication number
- JPH0613031A JPH0613031A JP19290292A JP19290292A JPH0613031A JP H0613031 A JPH0613031 A JP H0613031A JP 19290292 A JP19290292 A JP 19290292A JP 19290292 A JP19290292 A JP 19290292A JP H0613031 A JPH0613031 A JP H0613031A
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- negative electrode
- cations
- cathode
- discharge
- 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
- Discharge Lamp (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】高電圧大容量の放電管の電極に利
用するもので、特に高電圧・大容量間欠の直流放電のス
トロボ管の電極に使用した場合、電極が加熱されにく
く、放電管としての寿命が長時間化する。[Industrial field of application] It is used for electrodes of high-voltage and large-capacity discharge tubes, especially when used for electrodes of high-voltage, large-capacity intermittent DC discharge strobe tubes, the electrodes are less likely to be heated As a long life.
【0002】[0002]
【従来の技術】従来の放電管内の電極は、高速度の荷電
粒子が通過してゆく孔を設けられていないため、多くの
高速度荷電粒子が電極と衝突し、電極で多量の熱が発生
している。2. Description of the Related Art Since the conventional electrodes in a discharge tube are not provided with holes through which high-velocity charged particles pass, many high-velocity charged particles collide with the electrodes and a large amount of heat is generated at the electrodes. is doing.
【0003】[0003]
【発明が解決しようとする課題】高速荷電粒子が通過し
てゆく孔を設けていない従来の電極を使用した放電管で
は、高電圧で大容量の間欠放電を長時間繰り返し行った
場合、電極は多数の高速荷電粒子の衝突により発生した
大量の熱により、電極が溶融したり、電極の一部が飛散
し、放電管のガラスの内側部分に附着しガラス管黒化の
一因となっている。また電極とガラスの熱膨張の違いか
らガラス管が破損したり、高温に加熱された電極からの
熱や荷電粒子の衝突を受けた透明ガラスの一部は、組織
変化を起こして白濁することもある。これらのため長時
間、高電圧・大容量間欠放電を繰り返すことができる放
電管が得られなかった。DISCLOSURE OF INVENTION Problems to be Solved by the Invention In a discharge tube using a conventional electrode which is not provided with a hole through which fast charged particles pass, when a large-capacity intermittent discharge is repeatedly performed at a high voltage for a long time, the electrode is Due to the large amount of heat generated by the collision of many fast charged particles, the electrode melts or a part of the electrode scatters and adheres to the inner part of the glass of the discharge tube, contributing to blackening of the glass tube. . In addition, the glass tube may be damaged due to the difference in thermal expansion between the electrode and the glass, or part of the transparent glass that has received heat from the electrode heated to high temperature or collision of charged particles may change its structure and become cloudy. is there. For these reasons, a discharge tube capable of repeating high voltage, large capacity intermittent discharge for a long time could not be obtained.
【0004】[0004]
【課題を解決するための手段】多数の高速荷電粒子が電
極に衝突し、大量の熱が発生する電極を使用している放
電管では、長時間の高電圧・大容量の間欠放電を繰り返
すことはできない。したがって高速荷電粒子の大部分が
電極と衝突せずに通過してゆく孔を、電極の一部に設け
た電極を使用すればよい。In a discharge tube using an electrode in which a large number of fast charged particles collide with the electrode and a large amount of heat is generated, a high voltage / large capacity intermittent discharge is repeated for a long time. I can't. Therefore, it is sufficient to use an electrode provided with a part of the electrode through which most of the fast charged particles pass without colliding with the electrode.
【0005】[0005]
【作用】高電圧で加速された荷電粒子は、高速になるに
つれて直進性の運動の慣性を強くもつようになる。その
ため中央部に大きな孔を設けた電極に、多数の高速度の
荷電粒子が向った場合、大多数の高速の荷電粒子は電極
中央部の孔を通過するため、電極に衝突する荷電粒子は
減少し、電極での発熱も減少するのである。The charged particles accelerated by a high voltage have a strong inertia of rectilinear motion with increasing speed. Therefore, when a large number of high-speed charged particles face the electrode with a large hole in the center, the majority of high-speed charged particles pass through the hole in the center of the electrode, reducing the number of charged particles that collide with the electrode. However, heat generation at the electrodes is also reduced.
【0006】[0006]
【実施例】図1は、本発明の電極を陰極に用いたキセノ
ンガス入りのストロボ放電管の平面図で、図2は中央縦
断側面図である。1a,1bは放電管の透明なガラス部
分で、2は本発明のリング状の陰極で、3a,3bは陽
極である。4,5,5a,5bはリード線で、電圧10
00〔V〕の直流電源で充電されているコンデンサーの
陰極、陽極に接続されている。6a,6bはトリーガー
電極で7はそのリード線である。そしてこの放電管内の
電界は、陽極3a,3bからガラス管中を陰極2に向っ
て形成されている。陰極2とトリーガー電極6に接続さ
れているリード線7を通して、約6000〔V〕の放電
刺激を与えるとこの放電管中にキセノンガスの陽イオン
が生じ、その陽イオンは陽極3a,3bと陰極2との間
に形成されている電界の力を受けて、陰極2に向って加
速進行してゆき高速度になってゆく。このトリーガーの
刺激放電によりコンデンサーに充電されていた電荷も、
キセノンガスを媒介にして瞬時に放電されてゆく。その
ため非常に多くのキセノンの陽イオンが一挙に陰極2に
向って加速進行し高速化してゆく。もし陰極2が図のよ
うなリング状でなく円板状の場合、陰極板は非常に多く
の高速度のキセノンガスの衝突を受けて発熱してゆく。
比較的点滅回数の少ない60〔Hz〕のストロボ発光の
ときでも、これを長時間繰り返した場合、ストロボ管全
体の外部への放熱より発生熱が多い場合には陰極板が溶
融することも起る。図のようなリング状の陰極2の場合
には、陰極2の中央部に向ったキセノンの陽イオンは陰
極2と衝突することなく孔を通過し、陰極の反対側の進
行方向と逆向きの電界中に突入し、電界の力を受けて急
激に減速してゆく。この電極2はキセノンガスの衝突を
多く受けないため、発熱が少なくなり、長時間・高電圧
の大容量間欠放電が可能になるのである。EXAMPLE FIG. 1 is a plan view of a strobe discharge tube containing xenon gas using the electrode of the present invention as a cathode, and FIG. 2 is a central longitudinal side view. 1a and 1b are transparent glass parts of the discharge tube, 2 is a ring-shaped cathode of the present invention, and 3a and 3b are anodes. 4,5, 5a, 5b are lead wires, voltage 10
It is connected to the cathode and anode of a capacitor charged by a DC power source of 00 [V]. 6a and 6b are Triger electrodes, and 7 is a lead wire thereof. The electric field in the discharge tube is formed from the anodes 3a and 3b toward the cathode 2 in the glass tube. When a discharge stimulus of about 6000 [V] is applied through the lead wire 7 connected to the cathode 2 and the Triger electrode 6, cations of xenon gas are generated in this discharge tube, and the cations are the anodes 3a and 3b and the cathode. Under the influence of the electric field formed between the cathode and the cathode 2, the cathode 2 accelerates and accelerates to a high speed. The electric charge that was charged in the capacitor by the stimulation discharge of this Triger,
It is instantly discharged through xenon gas. Therefore, a large number of xenon cations are accelerated toward the cathode 2 all at once, and the speed is increased. If the cathode 2 has a disk shape instead of the ring shape as shown in the figure, the cathode plate will generate heat due to collision of a large amount of high-speed xenon gas.
Even when flashing at 60 [Hz], which has a relatively small number of blinks, if this is repeated for a long time and the heat generated is larger than the heat radiated to the outside of the entire flash tube, the cathode plate may melt. . In the case of the ring-shaped cathode 2 as shown in the figure, the xenon cations directed to the central portion of the cathode 2 pass through the hole without colliding with the cathode 2 and are directed in the opposite direction to the traveling direction on the opposite side of the cathode. It rushes into the electric field, and receives the force of the electric field to rapidly decelerate. Since the electrode 2 does not receive many collisions of xenon gas, heat generation is reduced and a large-capacity intermittent discharge of high voltage for a long time becomes possible.
【0007】[0007]
【発明の効果】事実円板状の陰極2に比較して、本発明
のリング状の陰極2を用いた場合、非常に発熱が少な
く、長時間・大容量の間欠放電を繰り返すことができる
ようになった。As compared with the disk-shaped cathode 2, the ring-shaped cathode 2 of the present invention produces very little heat and can be intermittently discharged for a long time and with a large capacity. Became.
【図1】本発明の陰極を備えた放電管の平面図である。FIG. 1 is a plan view of a discharge tube including a cathode of the present invention.
【図2】同じく中央縦断側面図である。FIG. 2 is likewise a side view of the central longitudinal section.
1a,1b 放電管のガラス部分 2 本発明の陰極 3a,3b 陽極 4 陰極用のリード線 5,5a,5b 陽極用のリード線 6a,6b トリーガー電極 7 トリーガー電極用リード線 1a, 1b Glass part of discharge tube 2 Cathode 3a, 3b Anode of the present invention 4 Lead wire for cathode 5, 5a, 5b Lead wire for anode 6a, 6b Triger electrode 7 Lead wire for Triger electrode
─────────────────────────────────────────────────────
─────────────────────────────────────────────────── ───
【手続補正書】[Procedure amendment]
【提出日】平成4年8月20日[Submission date] August 20, 1992
【手続補正1】[Procedure Amendment 1]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】0006[Correction target item name] 0006
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【0006】[0006]
【実施例】図1は、本発明の電極を陰極に用いたキセノ
ンガス入りのストロボ放電管の平面図で、図2は中央縦
断側面図である。1a,1bは放電管の透明なガラス部
分で、2は本発明のリング状の陰極で、3a,3bは陽
極である。4,5,5a,5bはリード線で、電圧10
00〔V〕の直流電源で充電されているコンデンサーの
陰極、陽極に接続されている。6a,6bはトリーガー
電極で7はそのリード線である。そしてこの放電管内の
電界は、陽極3a,3bからガラス管中を陰極2に向っ
て形成されている。陰極2とトリーガー電極6に接続さ
れているリード線7を通して、約6000〔V〕の放電
刺激を与えるとこの放電管中にキセノンガスの陽イオン
が生じ、その陽イオンは陽極3a,3bと陰極2との間
に形成されている電界の力を受けて、陰極2に向って加
速進行してゆき高速度になってゆく。このトリーガーの
刺激放電によりコンデンサーに充電されていた電荷も、
キセノンガスを媒介にして瞬時に放電されてゆく。その
ため非常に多くのキセノンの陽イオンが一挙に陰極2に
向って加速進行し高速化してゆく。もし陰極2が図のよ
うなリング状でなく円板状の場合、陰極板は非常に多く
の高速度のキセノンガスの衝突を受けて発熱してゆく。
比較的点滅回数の少ない60〔Hz〕のストロボ発光の
ときでも、これを長時間繰り返した場合、ストロボ管全
体の外部への放熱より発生熱が多い場合には陰極板が溶
融することも起る。図のようなリング状の陰極2の場合
には、陰極2の中央部に向ったキセノンの陽イオンは陰
極2と衝突することなく孔を通過し、陰極の反対側の進
行方向と逆向きの電界中に突入し、電界の力を受けて急
激に減速してゆく。この電極2はキセノンガスの衝突を
多く受けないため、発熱が少なくなり、長時間・高電圧
の大容量間欠放電が可能になるのである。EXAMPLE FIG. 1 is a plan view of a strobe discharge tube containing xenon gas using the electrode of the present invention as a cathode, and FIG. 2 is a central longitudinal side view. 1a and 1b are transparent glass parts of the discharge tube, 2 is a ring-shaped cathode of the present invention, and 3a and 3b are anodes. 4,5, 5a, 5b are lead wires, voltage 10
It is connected to the cathode and anode of a capacitor charged by a DC power source of 00 [V]. 6a and 6b are Triger electrodes, and 7 is a lead wire thereof. The electric field in the discharge tube is formed from the anodes 3a and 3b toward the cathode 2 in the glass tube. When a discharge stimulus of about 6000 [V] is applied through the lead wire 7 connected to the cathode 2 and the Triger electrode 6, cations of xenon gas are generated in this discharge tube, and the cations are the anodes 3a and 3b and the cathode. Under the influence of the electric field formed between the cathode and the cathode 2, the cathode 2 accelerates and accelerates to a high speed. The electric charge that was charged in the capacitor by the stimulation discharge of this Triger,
It is instantly discharged through xenon gas. Therefore, a large number of xenon cations are accelerated toward the cathode 2 all at once, and the speed is increased. If the cathode 2 has a disk shape instead of the ring shape as shown in the figure, the cathode plate will generate heat due to collision of a large amount of high-speed xenon gas.
Even when flashing at 60 [Hz], which has a relatively small number of blinks, if this is repeated for a long time and the heat generated is larger than the heat radiated to the outside of the entire flash tube, the cathode plate may melt. . In the case of the ring-shaped cathode 2 as shown in the figure, the xenon cations directed to the central portion of the cathode 2 pass through the hole without colliding with the cathode 2 and are directed in the opposite direction to the traveling direction on the opposite side of the cathode. It rushes into the electric field, and receives the force of the electric field to rapidly decelerate. Since the electrode 2 does not receive many collisions of xenon gas, heat generation is reduced and a large-capacity intermittent discharge of high voltage for a long time becomes possible.
Claims (1)
衝突することなく、通過できる孔を設けた電極の構造。1. A structure of an electrode provided with a hole through which fast charged particles can pass without colliding with the electrode in a discharge tube.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19290292A JPH0613031A (en) | 1992-06-26 | 1992-06-26 | Electrode of discharge tube having passing hole of high speed charged particle |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19290292A JPH0613031A (en) | 1992-06-26 | 1992-06-26 | Electrode of discharge tube having passing hole of high speed charged particle |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0613031A true JPH0613031A (en) | 1994-01-21 |
Family
ID=16298884
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19290292A Pending JPH0613031A (en) | 1992-06-26 | 1992-06-26 | Electrode of discharge tube having passing hole of high speed charged particle |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0613031A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06225880A (en) * | 1993-07-07 | 1994-08-16 | Toshiba Corp | Ultrasonic bloodstream imaging device |
-
1992
- 1992-06-26 JP JP19290292A patent/JPH0613031A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06225880A (en) * | 1993-07-07 | 1994-08-16 | Toshiba Corp | Ultrasonic bloodstream imaging device |
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