JPS5992373A - ionization chamber - Google Patents

ionization chamber

Info

Publication number
JPS5992373A
JPS5992373A JP20204782A JP20204782A JPS5992373A JP S5992373 A JPS5992373 A JP S5992373A JP 20204782 A JP20204782 A JP 20204782A JP 20204782 A JP20204782 A JP 20204782A JP S5992373 A JPS5992373 A JP S5992373A
Authority
JP
Japan
Prior art keywords
case
flange
ionization chamber
airtightly
radiation
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.)
Granted
Application number
JP20204782A
Other languages
Japanese (ja)
Other versions
JPH0358136B2 (en
Inventor
Takaaki Okino
沖野 孝昭
Kiyoshi Ishida
石田 喜代志
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 JP20204782A priority Critical patent/JPS5992373A/en
Publication of JPS5992373A publication Critical patent/JPS5992373A/en
Publication of JPH0358136B2 publication Critical patent/JPH0358136B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J47/00Tubes for determining the presence, intensity, density or energy of radiation or particles
    • H01J47/02Ionisation chambers

Landscapes

  • Measurement Of Radiation (AREA)
  • Electron Tubes For Measurement (AREA)

Abstract

PURPOSE:To improve the yield of an ionization chamber by forming the surface of a radiation incidence flange which faces the inside of a case into a recessed spherical surface, and connecting it with a cylindrical edge part which is jointed with the lower end of the case by a curved surface with a large radius of curvature. CONSTITUTION:An upper flange 12 made of aluminum is welded airtightly to the upper end of the cylindrical case 11 made of aluminum for closure. Further, the lower end of the case 11 has the recessed spherical surface 13a which faces the inside of the case, and the circumferential edge part 16b is formed into a cylindrical surface connecting with the spherical surface by the curved surface 13c with the large radius of curvature. This radiation incidence flange 13 made of the aluminum plate is welded airtightly to the lower end part of the case 11. A terminal 14 made of an insulator of ceramics, etc., is fitted airtightly in the center of the upper flange 12 while piercing the flange airtightly, and a signal electrode 15 made of a conductive material is arranged concentrically with the center axial line of the case 11. The case 11 is evacuated through a discharge cylinder 16, pressurized ionized gas 7 is charged, and the case 11 is sealed airtightly.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、電離箱に関する。[Detailed description of the invention] [Technical field of invention] The present invention relates to an ionization chamber.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

一般的な電離箱の断面を第1図に示す。第1図において
、(1)は端子で、絶縁体で作られ、導電性金属調の上
部フラン> (41の中心部忙貫通配置され気密に接′
合されている。(2)は信号電極で、端子(1)の中心
を貫通して気密に接合されている。(5)は円筒状のケ
ースで、導電性金属で作られ、その上端に上部フランジ
(4)が気密に接合されている。(6)は放射線入射フ
ラン:)で、導電性金属で作られ、ケース(5)の下端
に気密に接合されている。これらの(41、(51、+
61は高圧電極を構成する。(3)は排気筒で、上部7
ランジ(4)に接合され、その端末は、ケース(5)内
を排気し電離気体を充填した後チップされて気密に閉塞
されている。ケース(5)内の電離気体(刀は数気圧に
加圧されて封入されている。
Figure 1 shows a cross section of a typical ionization chamber. In Fig. 1, (1) is a terminal made of an insulator, which is made of a conductive metal-like upper flange (41) and is arranged through the center of the terminal in airtight contact.
are combined. (2) is a signal electrode that passes through the center of the terminal (1) and is airtightly joined to the terminal (1). (5) is a cylindrical case made of conductive metal, and has an upper flange (4) hermetically joined to its upper end. (6) is a radiation entrance flan: ) made of conductive metal and hermetically joined to the lower end of the case (5). These (41, (51, +
61 constitutes a high voltage electrode. (3) is the exhaust pipe, and the upper part 7
It is joined to the flange (4), and its terminal end is sealed airtightly after the inside of the case (5) is evacuated and filled with ionized gas. The case (5) is filled with ionized gas (the sword is pressurized to several atmospheres).

そして、第2図に示すように、放射線源(8)からの放
射線ビーム(9)が電離箱tllK入射すると、電離気
体に衝突した放射線によシス体が電離されてイオン電子
(放射線量にほぼ比例する)が生成され、電流として信
号電極(2)から出力される。
As shown in Fig. 2, when the radiation beam (9) from the radiation source (8) enters the ionization chamber tllK, the cis-isomer is ionized by the radiation that collides with the ionized gas, and the ion electrons (approximately the radiation dose (proportional) is generated and output as a current from the signal electrode (2).

放射線厚さ計に用いる電離箱は、厚さ計の性能向上のた
めに高感度が要求される。そのだめ、電離箱の検出感度
を上げるために各種の工夫がなされているが、基本的に
は、できるだけ多くの放射線を電離箱内に入射させるこ
と、入射した放射線を効率よく電離電流に変換すること
の二つがあげられる。前者については放射線入射フラン
ジ(6)を放射線吸収の少ない物質で作ること。後者に
ついては電離気体(力(電離分子)の密度を高め、放射
線の捕捉率を上けることと、電離したイオンを速やかに
収集できるような内部構造とすることである。すなわち
、前者については原子番号の小さい物質を極力薄くして
作ればよく、後者については電離気体の圧力を上げて信
号電極と高圧電極の構造を工夫すればよい。
Ionization chambers used in radiation thickness gauges are required to have high sensitivity in order to improve the performance of the thickness gauge. To avoid this, various efforts have been made to increase the detection sensitivity of the ionization chamber, but basically, it is necessary to allow as much radiation as possible to enter the ionization chamber, and to efficiently convert the incident radiation into ionizing current. Two things can be mentioned. For the former, the radiation entrance flange (6) should be made of a material that absorbs little radiation. For the latter, we need to increase the density of ionized gas (force (ionized molecules)) to increase the radiation capture rate, and to create an internal structure that can quickly collect ionized ions. The material with the lowest number can be made as thin as possible, and the latter can be made by increasing the pressure of the ionized gas and devising the structure of the signal electrode and high-voltage electrode.

ところが、電離気体の圧力を上げると、放射線入射フラ
ンジ(6)もこの圧力に耐える強度を要するため厚くし
なければならず、厚さ計の使用環境や製品としての余裕
を考慮した場合、両者を同時に満足させることはなかな
か難しい。
However, when the pressure of the ionized gas is increased, the radiation entrance flange (6) also needs to be strong enough to withstand this pressure, so it must be made thicker. It is difficult to satisfy both at the same time.

そこで、従来技術としては、放射線入射フランジ(6)
に放射線吸収の最も少ない金属であるべIJ IJウム
板を用い、電離気体の圧力を上げて所要の感度を得てい
るものがあるが、ぺIJ IJウムは加工性が悪く有害
金属である上に、溶接技術が確立されていないため、製
品として歩留りが悪く、高価であるという欠点があった
Therefore, as a conventional technology, the radiation entrance flange (6)
In some cases, the required sensitivity is obtained by increasing the pressure of ionized gas using a metal plate with the least amount of radiation absorption, but metal plate has poor workability and is a toxic metal. In addition, because the welding technology has not been established, the product has a low yield and is expensive.

〔発明のll的〕[Invention's purpose]

本発明ケ↓、上記の欠点を解消した電離箱を提供するこ
とを目的とする。
An object of the present invention is to provide an ionization chamber that eliminates the above-mentioned drawbacks.

〔発明の概要〕[Summary of the invention]

本発明は、上端を上部フランジで気密に閉塞された導電
性材料製の円筒状のケースの下端に、このケース内部に
向いた面が凹の球面状をなし周縁端部が前記球面に曲面
でつながる円筒面に形成されたアルミニウム製の放射線
入射フランジが気密に接合されている高圧電極とs −
mll上上7ランジの中央に気密に取着された絶縁材料
製の端子と、この端子を気密に貫通し前記ケースの中心
軸線と同心に配置され前記放射線入射7ランジの内面近
傍まで延在した導電性材料製の信号電極とを具え、前記
ケース内に所要圧に加圧した電離気体を封入してなる電
離箱を実現して所期の目的を達成した。
The present invention provides a lower end of a cylindrical case made of a conductive material whose upper end is hermetically closed with an upper flange, the surface facing inside the case has a concave spherical shape, and the peripheral edge has a curved surface on the spherical surface. An aluminum radiation entrance flange formed on a connected cylindrical surface is hermetically connected to a high-voltage electrode and s-
A terminal made of an insulating material is airtightly attached to the center of the upper 7 langes on the mll, and a terminal made of an insulating material is airtightly passed through the terminals and is arranged concentrically with the central axis of the case and extends to the vicinity of the inner surface of the radiation entrance 7 langes. The desired objective was achieved by realizing an ionization chamber which is equipped with a signal electrode made of a conductive material and in which ionized gas pressurized to a required pressure is sealed in the case.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明の実施例を図面を参照して説明する。 Embodiments of the present invention will be described below with reference to the drawings.

本発明一実施例の電離箱を第3図に示す。第3図におい
て、円筒状のケース1ll)はアルミニウムで作られ、
その下端近傍の外周面にケースの中心軸線と直角な面を
下方に向けた段部(tta)を有する。
An ionization chamber according to one embodiment of the present invention is shown in FIG. In Figure 3, the cylindrical case 1ll) is made of aluminum;
It has a stepped portion (tta) on its outer circumferential surface near its lower end, with a surface perpendicular to the central axis of the case facing downward.

ケース(11)の上端はアルミニウム製の上部フランジ
(13が溶接によシ気密に接合されて閉塞されている。
The upper end of the case (11) is closed by an aluminum upper flange (13) hermetically joined by welding.

さらに、ケースaυの下端はけ、ケース内に向いた面が
凹の球面(13a)をなし、周縁端部(13b)が前記
球面に曲率半径の大きい曲面(13(りでつながる円筒
面に形成されたアルミニウム板製の放射線入射フランジ
(13が周縁端部(13b)をケース60下端部に溶接
によシ気密に接合されている。ケースαυ、上部フラン
ジ0邊、放射線入射ノランジ(13は高圧電極を構成し
ている。
Furthermore, the lower end of the case aυ has a concave spherical surface (13a) facing inward, and the peripheral edge (13b) is formed into a cylindrical surface connected to the spherical surface by a curved surface (13) with a large radius of curvature. The radiation entrance flange (13) is made of aluminum plate and its peripheral edge (13b) is hermetically joined to the lower end of the case 60 by welding. It constitutes an electrode.

上部7ランジ仕邊の中央にはセラミックなどの絶縁材料
製の端子Iが気密に取着されている2、この端子Iを気
密に貫通しケース01)の中心軸線と同心に導電性材料
製の信号電極(【5)が配置され、放射線、入射フーノ
ンジ0漕の内面近傍まで延在している。そして、上部フ
ランジ(14に設けられた排気筒<[eにょシ、ケース
0υ内を排気した上、所要の圧力に加圧した電離気体(
7)を充填し、排気筒−の端末をチップしてケース(1
υを気密に封止している。
A terminal I made of an insulating material such as ceramic is airtightly attached to the center of the upper 7 flange fitting. A signal electrode (5) is arranged and extends to the vicinity of the inner surface of the radiation and incident sensor. Then, after exhausting the inside of the case 0υ, an ionized gas (
7), tip the end of the exhaust pipe and attach the case (1).
υ is hermetically sealed.

上記のように構成された本発明一実施例の電離箱は、高
圧電極と信号電極間に所定の電圧を印加(1、第2図と
同様に、放射線入射フランジ(E騰に放射線を入射させ
ると、電離気体(7)に衝突した放射線により気体が電
離されてイオン電子が生成され、放射線量にtυ丁比例
した電流として信号電極(lから出力される。よって、
この電流を測定することによシ単位時間当りの入射線量
を知ることができる。
The ionization chamber of the embodiment of the present invention configured as described above applies a predetermined voltage between the high voltage electrode and the signal electrode (1, as in Figure 2, allows radiation to enter the radiation entrance flange (E)) Then, the gas is ionized by the radiation colliding with the ionized gas (7) and ion electrons are generated, which are output from the signal electrode (l) as a current proportional to the radiation dose.
By measuring this current, the incident dose per unit time can be determined.

そして、放射線入射7ランジ0を平板状でなく、ケース
内部に向いた面が凹な球1ni(13a)に形成し、且
つケース(11)の下端部に接合される円筒面状の周縁
端部(13b)と球面(13a)とを曲率半径の大きい
曲面(13c)でつないだ形状にしたので、板厚を薄く
しても充分な強度が得られ放射線吸収を小さくすること
ができる。このためベリリウムを使用しなくて済むし、
電離気体の封入圧力を高くすることが可能となる。これ
らにより、検出感度を高めることができる。ベリリウム
を使用しないので毒性の心配がなく、アルミニウムを使
用したことにより加工性が良く、溶接上の難点もないの
で製品の歩留りが格段に向上し、価格も安くなる。
The radiation incidence 7 flange 0 is not shaped like a flat plate, but is formed into a sphere 1ni (13a) with a concave surface facing inside the case, and a cylindrical peripheral edge portion is joined to the lower end of the case (11). (13b) and the spherical surface (13a) are connected by a curved surface (13c) with a large radius of curvature, so even if the plate thickness is reduced, sufficient strength can be obtained and radiation absorption can be reduced. This eliminates the need to use beryllium,
It becomes possible to increase the sealing pressure of ionized gas. With these, detection sensitivity can be increased. Since it does not use beryllium, there is no need to worry about toxicity, and because it uses aluminum, it has good workability and there are no welding difficulties, so the product yield is significantly improved and the price is lower.

また、ケース圓に直角面を下方に向けた段部(lla)
i設けたことにより、この段部(lla)を座面として
用いて電離箱を安定に固定することができる。なお、段
部(lla)を設ける代シに、上部フランジ員をケース
01)の外周面より外方へ鍔状に突出した形状に作り、
この鍔状の突出面を座面として電離箱を固定するよりに
してもよい。
In addition, there is a stepped part (lla) with the surface perpendicular to the case circle facing downward.
By providing the stepped portion (lla), the ionization chamber can be stably fixed using the stepped portion (lla) as a seating surface. In addition, instead of providing the step (lla), the upper flange member is made in a shape that protrudes outward from the outer peripheral surface of the case 01) in the shape of a flange.
The ionization chamber may be fixed using this brim-shaped protruding surface as a seat surface.

〔発明の効果〕〔Effect of the invention〕

以上詳述したように本発明によれば、放射線入射フラン
ジをケース内部に向いた面が凹な球面に形成し、且つケ
ースの下端部に接合される円筒面状の周縁端部と前記球
面と4曲率半径の大きい曲面でつないだ形状にしたので
、板厚を薄くしても充分な強度を得ることができる。そ
の結果、下記のような効果が得られる。
As detailed above, according to the present invention, the radiation entrance flange is formed into a spherical surface with a concave surface facing the inside of the case, and the cylindrical peripheral edge joined to the lower end of the case and the spherical surface are connected to each other. 4 Since the shape is connected by curved surfaces with a large radius of curvature, sufficient strength can be obtained even if the plate thickness is reduced. As a result, the following effects can be obtained.

〔1〕放射紳入射フランジがアルミニウムを用いて板厚
を薄く作ることが可能で、放射線吸収を小さくすること
ができ、(7かも強度が高い構造のため電離気体の個人
圧を高めることができ、検出感度が向上する。
[1] The radiation entrance flange can be made thin using aluminum, which can reduce radiation absorption, and (7) The structure has high strength, so the personal pressure of ionized gas can be increased. , the detection sensitivity is improved.

〔2〕有害金属のベリリウムを使わなくて済むので、加
工性、溶接の問題が解消し、製品の歩留りが向上し価格
も安くなる。
[2] Since there is no need to use beryllium, a toxic metal, problems with workability and welding are solved, and product yields are improved and prices are reduced.

〔3〕ケースの外周面に直角面を下方に向けた段部分設
けるか、またtよ上部フランジをケースの外周面より外
方へ鍔状に突出させたことにより、これらを座面として
電離箱を安定に固定することができる。
[3] By providing a stepped section on the outer circumferential surface of the case with the right-angled surface facing downward, or by making the upper flange protrude outward from the outer circumferential surface of the case in a flange shape, these can be used as seating surfaces for the ionization chamber. can be stably fixed.

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

第1図は従来の一般的な電離箱を示す断面図、第2図は
放射線源から放射線がIM、酸相に入射する状態を示す
説明図、第3図は本発明一実施例の電離箱を示す断面図
である。 7  電離気体    11   ケースi1a  段
部      12  上部フランジ13   放射線
入射フランジ 13a  球面13’b  周縁端部 
   t3C曲面714  ・端子      15 
 信号電極16  排気筒 代理人 弁理士  井 上 −男
Fig. 1 is a sectional view showing a conventional general ionization chamber, Fig. 2 is an explanatory view showing a state in which radiation enters the IM and acid phase from a radiation source, and Fig. 3 is an ionization chamber of an embodiment of the present invention. FIG. 7 Ionized gas 11 Case i1a Step part 12 Upper flange 13 Radiation incidence flange 13a Spherical surface 13'b Peripheral end
t3C curved surface 714 ・Terminal 15
Signal electrode 16 Exhaust stack agent Patent attorney Inoue - Male

Claims (1)

【特許請求の範囲】 (1)  上端を上部フランジで気密に閉塞された導電
性材料製の円筒状のケースの下端に、このケース内部に
向いた面が凹の球面状をなし周縁端部が前記球面に曲面
でつながる円筒面に形成されたアルミニウム製の放射線
入射フランジが気密に接合されてなる高圧電極と、前記
上部フランジの中央に気密に取着された絶縁材料製の端
子と、この端子を気密に貫通し前記ケースの中心軸線と
同心に配置され前記放射線入射フランジの内面近傍まで
延在した導電性材料性の信号電極とを具え、前記ケース
内に所要圧に加圧した電離気体を封入してなる電離箱5
1(2)  ケースの外周面にケースの中心軸線と直角
な面を下方に向けた段部を有することを特徴とする特許
請求の範囲第1項記載の電離箱。 (3)上部フランジがケースの外周面より外方へ鍔状に
突出した形状に形成されたことを特徴とする特許請求の
範囲第1項記載の電離箱。
[Scope of Claims] (1) A cylindrical case made of a conductive material whose upper end is hermetically closed with an upper flange has a spherical shape with a concave surface facing the inside of the case, and a peripheral edge thereof. a high-voltage electrode formed by an aluminum radiation incidence flange formed on a cylindrical surface connected to the spherical surface by a curved surface and hermetically joined; a terminal made of an insulating material airtightly attached to the center of the upper flange; and this terminal. a signal electrode made of a conductive material that airtightly penetrates the case, is arranged concentrically with the central axis of the case, and extends to the vicinity of the inner surface of the radiation entrance flange; Enclosed ionization chamber 5
1(2) The ionization chamber according to claim 1, wherein the ionization chamber has a stepped portion on the outer peripheral surface of the case, with a surface perpendicular to the central axis of the case facing downward. (3) The ionization chamber according to claim 1, wherein the upper flange is formed in a shape that projects outward from the outer circumferential surface of the case in the shape of a brim.
JP20204782A 1982-11-19 1982-11-19 ionization chamber Granted JPS5992373A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20204782A JPS5992373A (en) 1982-11-19 1982-11-19 ionization chamber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20204782A JPS5992373A (en) 1982-11-19 1982-11-19 ionization chamber

Publications (2)

Publication Number Publication Date
JPS5992373A true JPS5992373A (en) 1984-05-28
JPH0358136B2 JPH0358136B2 (en) 1991-09-04

Family

ID=16451044

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20204782A Granted JPS5992373A (en) 1982-11-19 1982-11-19 ionization chamber

Country Status (1)

Country Link
JP (1) JPS5992373A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2013047634A (en) * 2011-08-29 2013-03-07 Fuji Electric Co Ltd Ionization chamber type radiation detector

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56154685A (en) * 1980-04-04 1981-11-30 Gen Electric Gas-sealed x rays detector with improved window

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56154685A (en) * 1980-04-04 1981-11-30 Gen Electric Gas-sealed x rays detector with improved window

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2013047634A (en) * 2011-08-29 2013-03-07 Fuji Electric Co Ltd Ionization chamber type radiation detector

Also Published As

Publication number Publication date
JPH0358136B2 (en) 1991-09-04

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