JPS61226628A - Vacuum gage - Google Patents
Vacuum gageInfo
- Publication number
- JPS61226628A JPS61226628A JP6644385A JP6644385A JPS61226628A JP S61226628 A JPS61226628 A JP S61226628A JP 6644385 A JP6644385 A JP 6644385A JP 6644385 A JP6644385 A JP 6644385A JP S61226628 A JPS61226628 A JP S61226628A
- Authority
- JP
- Japan
- Prior art keywords
- filament
- discharge
- vacuum
- electric discharge
- cathode
- 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
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L21/00—Vacuum gauges
- G01L21/30—Vacuum gauges by making use of ionisation effects
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Fluid Pressure (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は、放電電流により圧力を計測する放電型の真空
計測に係9、特に高真空側でも放電の開始を容易にする
真空計に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a discharge-type vacuum measurement that measures pressure using a discharge current, and particularly to a vacuum gauge that facilitates the initiation of discharge even on the high vacuum side.
従来の磁界?用いた放電型電離真空計として、「真空の
物理と応用(1981)J (熊谷・富永、他2名)
の図6−30に示されるような構造のものが矧られてい
る。次にその真空計の計測法について第10から第3図
を用いて説明する。dXx図は真空計、及び計測のため
の心気回路の概略を示す。真空容器4内に、絶縁物5を
介して設置された2個の対向する陰極1,2があυ、こ
れに直角方向に磁界Bがかけられている。さらに、絶縁
物6を介して、磁界已に平行な円筒状の陽極3が設けら
れている。陰極1,2と陽極3との間には、高圧fjL
源7によって高電圧がかけられている。この時上記電圧
によって、陰極1.2から放出されfcW!l子は、磁
界のためにつる巻き運動上しながら、陰極1,2間を何
度も往復する。これにLす、電子は気体分子全多数分離
し、陰極、陽極の間にはイオンが発生し、このイオンは
陰極へ流れ込む。Conventional magnetic field? The discharge type ionization vacuum gauge used was published in ``Physics and Applications of Vacuum (1981) J (Kumagai, Tominaga, and 2 others).
The structure shown in FIG. 6-30 is widely used. Next, a measurement method using the vacuum gauge will be explained using FIGS. 10 to 3. The dXx diagram schematically shows the vacuum gauge and the inspiratory circuit for measurement. Two opposing cathodes 1 and 2 are placed in a vacuum container 4 with an insulator 5 in between, and a magnetic field B is applied to them in a perpendicular direction. Further, a cylindrical anode 3 parallel to the magnetic field is provided with an insulator 6 interposed therebetween. There is a high pressure fjL between the cathodes 1 and 2 and the anode 3.
A high voltage is applied by source 7. At this time, due to the above voltage, fcW! is emitted from the cathode 1.2. The lion moves back and forth between the cathodes 1 and 2 many times while performing a spiral motion due to the magnetic field. In response to this, the electrons are separated from all gas molecules, and ions are generated between the cathode and anode, and these ions flow into the cathode.
この結果、電子の方が多くな力、磁界Bと直角方向に電
界が現れ、電子は陽極3へ向かって流れて放電が起こる
。この放wL亀流を電流計8によって測定し圧力を知る
ことができる。第2図は圧力と放電直流の関係を示して
いる。しかし、前述の放電型ICM真空計は、第3図に
示すよう罠、圧力の低い領域では、電圧を印加してから
放電するまで長時間を要したシ、あるいは放電が起こら
ないという問題があった。As a result, an electric field appears in a direction perpendicular to the magnetic field B, which has a greater force on the electrons, and the electrons flow toward the anode 3, causing a discharge. The pressure can be determined by measuring this discharged L current with an ammeter 8. Figure 2 shows the relationship between pressure and discharge DC. However, as shown in Figure 3, the above-mentioned discharge-type ICM vacuum gauge has the problem that in low-pressure areas, it takes a long time to discharge after voltage is applied, or that discharge does not occur. Ta.
本発明の目的は、圧力の低い領域においても、放Wtを
容易ならしめる、放f11m電離真空計を提供すること
Kある。An object of the present invention is to provide a discharge f11m ionization vacuum gauge that facilitates discharge Wt even in a low pressure region.
放電の起きKくい圧力領域でも、一度放電が起こると、
放電は持続する。そこで、放電のトリガとなる、電子と
イオンに着目し、外的にこれらを発生させようとしたの
が本発明であシ、そのために、Jic空計空部内部ィラ
メントを設置し、フィラメントよシ発生する、熱電子と
ガスを放電のトリガとしたものである。Even in the pressure range where discharge occurs, once discharge occurs,
The discharge continues. Therefore, the present invention focuses on electrons and ions, which are the triggers of discharge, and attempts to generate them externally.For this purpose, a filament is installed inside the JIC empty space, and the filament and ions are generated externally. The generated thermoelectrons and gas are used as a trigger for discharge.
以下、本発明の実施例を図を用いて説明する。 Embodiments of the present invention will be described below with reference to the drawings.
第4図は、本発明による真空計全示すもので真空計断面
図及び、回路の概略図である。図において、4は真空容
器を示し、この真空容器4内には、絶縁物5を介して設
置された2個の対向する陰極1゜2が再シ、これに直角
方向に磁界Bがかけられている。さらに、絶縁物6を介
して、磁界日に平行な陽極3が設けられ°ている。陰極
1,2と陽極3との間には、高圧IK#7によって^電
圧がかけられる。また、真空容器4内には、絶縁物11
゜12t−介し、陰極2に開けられた孔、あるいは絶縁
物1(1通って、電極内部に、フィラメント9が設けら
れている。FIG. 4 shows the entire vacuum gauge according to the present invention, including a sectional view of the vacuum gauge and a schematic diagram of the circuit. In the figure, 4 indicates a vacuum container, and within this vacuum container 4, two opposing cathodes 1°2 are installed with an insulator 5 in between, and a magnetic field B is applied to them in the perpendicular direction. ing. Further, an anode 3 parallel to the magnetic field is provided with an insulator 6 interposed therebetween. A voltage is applied between the cathodes 1 and 2 and the anode 3 by high voltage IK#7. Furthermore, inside the vacuum container 4, an insulator 11 is provided.
A filament 9 is provided inside the electrode through a hole drilled in the cathode 2 or through the insulator 1 (1).
本発明は、前述の如き構成としたので、放電型電離真空
計の測定範囲でありながら、接点13を閉じ、電源7に
より、電極に高電圧を印加しても放電が起きない場合に
は、接点15r閉じ、フィラメント9iC通電して、熱
電子及び、フィラメントに吸着していたガスを放出させ
ることにょシ、両者がトリガとなって放N!t−起こさ
せ、圧力計測が可能となる。真空計の計測範囲内で一度
放電を起こせば、その後の計測は可能となる。Since the present invention has the above-described configuration, if no discharge occurs even if the contact 13 is closed and a high voltage is applied to the electrode by the power source 7 within the measurement range of the discharge type ionization vacuum gauge, The contact 15r is closed and the filament 9iC is energized to release the thermoelectrons and the gas adsorbed on the filament. Both act as a trigger and release N! t- wake up and pressure measurement becomes possible. Once a discharge occurs within the measurement range of the vacuum gauge, subsequent measurements are possible.
第4図ではフィラメントを、陰極、陽極内部に設置した
が、第5図に示したように、電極の外にフィラメント9
があっても本発明の効果は得られる。また、制御回路1
6を設け、放電が起こらず、電流計8に訃いて放flL
遡流が零の場合、電源13の接点を自動的に閉じ、放送
磁流が流れたら、電源13を開にするような、放電トリ
ガ回路を設けることも可能でめる。In Fig. 4, the filaments are installed inside the cathode and anode, but as shown in Fig. 5, the filaments 9 are placed outside the electrodes.
Even if there is, the effect of the present invention can be obtained. In addition, the control circuit 1
6 was installed, no discharge occurred, and the current meter 8 was set, and the discharge flL
It is also possible to provide a discharge trigger circuit that automatically closes the contacts of the power source 13 when the backward flow is zero, and opens the power source 13 when the broadcast magnetic current flows.
以上説明したように、本発明によれば、放電が起こらな
かった時、熱電子とガスによってトリガをかけることが
でき、放電が可能となって、正常な真空計測を図れると
いう効果がある。As explained above, according to the present invention, when no discharge occurs, it is possible to apply a trigger using thermionic electrons and gas, enabling the discharge to occur and achieving normal vacuum measurement.
第1図は従来の真空計の断面図と回路の概略図、第2図
、第3図は従来の真空計の特性を説明する図、第4図、
第5図は本発明による真空計の断面図と回路の概略図で
ある。
1、 2・・・陰極、3・・・陽極、4・・・真空容器
、9・・・フィラメント、10・・・空孔又は絶縁物。
■ 1 口
1g
冨Z 図
Eカ(lσ1p)
l仁/7(zりr)
冨 4 n
B
冨 5 図Figure 1 is a cross-sectional view and circuit diagram of a conventional vacuum gauge, Figures 2 and 3 are diagrams explaining the characteristics of a conventional vacuum gauge, Figure 4,
FIG. 5 is a sectional view and a schematic diagram of a circuit of a vacuum gauge according to the present invention. DESCRIPTION OF SYMBOLS 1, 2... Cathode, 3... Anode, 4... Vacuum container, 9... Filament, 10... Hole or insulator. ■ 1 Mouth 1g Tomi Z Diagram Eka (lσ1p) l nin/7 (zuri r) Fuji 4 n B Fuji 5 Diagram
Claims (1)
に直角方向の磁界をかけ、該磁界と平行に設けた陽極と
、これら陰極、陽極を収納する真空容器とを備え、上記
電極を絶縁物を介してフランジ上に支持せしめ、陰極と
陽極の間に高電圧を印加することにより、陰極から放出
された電子によつて放電が起こり、該放電電流を検出し
て圧力指示値を得る真空計において、前記真空容器内に
フィラメントを設置したことを特徴とする真空計。 2、電極に電圧を印加しても放電が発生しない場合、フ
ィラメント通電を自動的に行い、放電後フィラメント通
電を止めることを特徴とする特許請求の範囲第1項記載
の真空計。[Claims] 1. Two or more cathodes facing each other, an anode that applies a magnetic field perpendicular to the cathode surface and is provided parallel to the magnetic field, and a vacuum container that houses these cathodes and anodes. The electrode is supported on the flange via an insulator, and by applying a high voltage between the cathode and the anode, a discharge occurs due to electrons emitted from the cathode, and the discharge current is detected. A vacuum gauge for obtaining a pressure indication value, characterized in that a filament is installed in the vacuum container. 2. The vacuum gauge according to claim 1, wherein the filament is automatically energized when no discharge occurs even when a voltage is applied to the electrodes, and the filament energization is stopped after discharge.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6644385A JPS61226628A (en) | 1985-04-01 | 1985-04-01 | Vacuum gage |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6644385A JPS61226628A (en) | 1985-04-01 | 1985-04-01 | Vacuum gage |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61226628A true JPS61226628A (en) | 1986-10-08 |
Family
ID=13315920
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP6644385A Pending JPS61226628A (en) | 1985-04-01 | 1985-04-01 | Vacuum gage |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61226628A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2009128276A (en) * | 2007-11-27 | 2009-06-11 | Shinku Jikkenshitsu:Kk | Ionization vacuum device |
US8456167B2 (en) | 2007-11-12 | 2013-06-04 | Edwards Limited | Ionisation vacuum gauges and gauge heads |
-
1985
- 1985-04-01 JP JP6644385A patent/JPS61226628A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US8456167B2 (en) | 2007-11-12 | 2013-06-04 | Edwards Limited | Ionisation vacuum gauges and gauge heads |
JP2009128276A (en) * | 2007-11-27 | 2009-06-11 | Shinku Jikkenshitsu:Kk | Ionization vacuum device |
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