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JPS5824903B2 - Multilayer electrode type ionization chamber - Google Patents
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JPS5824903B2 - Multilayer electrode type ionization chamber - Google Patents

Multilayer electrode type ionization chamber

Info

Publication number
JPS5824903B2
JPS5824903B2 JP1930377A JP1930377A JPS5824903B2 JP S5824903 B2 JPS5824903 B2 JP S5824903B2 JP 1930377 A JP1930377 A JP 1930377A JP 1930377 A JP1930377 A JP 1930377A JP S5824903 B2 JPS5824903 B2 JP S5824903B2
Authority
JP
Japan
Prior art keywords
ionization chamber
electrode type
window
multilayer electrode
electrodes
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
Application number
JP1930377A
Other languages
Japanese (ja)
Other versions
JPS53105280A (en
Inventor
関英治
斎藤貞勝
小長井主税
白山新平
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
Tokyo Shibaura Electric Co Ltd
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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP1930377A priority Critical patent/JPS5824903B2/en
Publication of JPS53105280A publication Critical patent/JPS53105280A/en
Publication of JPS5824903B2 publication Critical patent/JPS5824903B2/en
Expired 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

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

Description

【発明の詳細な説明】 この発明は感度および応答性を向上させた多層電極形電
離箱に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a multilayer electrode type ionization chamber with improved sensitivity and responsiveness.

たとえば厚み計などに使用される放射線電離箱は第1図
に示したように筒状陽極1の中央に集電極(陰極)2を
絶縁体3を介して設け、筒形陽極1の1端をなす放射線
入射窓4にステンレス鋼などの薄膜を貼着しかつ他端の
端板5を設け、内部に有感ガスを封入してなるものであ
る。
For example, in a radiation ionization chamber used for a thickness gauge, as shown in FIG. A thin film of stainless steel or the like is adhered to the radiation entrance window 4, an end plate 5 is provided at the other end, and a sensitive gas is sealed inside.

そして窓4を図示してない線源に対向させ、線源と窓4
の中間に試料を挿入し両電極1,2に高電圧を印刀口し
て有感ガスの電離電流を測定して試料の厚みを測定する
Then, the window 4 is made to face a radiation source (not shown), and the radiation source and the window 4 are
A sample is inserted between the electrodes 1 and 2, a high voltage is applied to both electrodes 1 and 2, and the ionization current of the sensitive gas is measured to measure the thickness of the sample.

なお、図中6,7はリード線、8は放射線入射方向を示
す。
In addition, in the figure, 6 and 7 indicate lead wires, and 8 indicates the radiation incident direction.

ところで、線源たとえばX線、r線のエネルギが低い場
合には窓4での吸収が非常に多く出力が小さくなり、そ
のため出力を増大させるには電離箱を大きくするかまた
は線源の強度を大きくする必要がある。
By the way, when the energy of the radiation source, such as X-rays or r-rays, is low, the absorption in the window 4 is very large and the output decreases. Therefore, in order to increase the output, the ionization chamber must be made larger or the intensity of the radiation source must be increased. It needs to be bigger.

しかし、電離箱の応答速度を考慮すると印加電圧を大き
くするか有感ガスの圧力を小さくしなければならず、し
たがって感度が低下する原因にもなっている。
However, in consideration of the response speed of the ionization chamber, it is necessary to increase the applied voltage or decrease the pressure of the sensitive gas, which is also a cause of a decrease in sensitivity.

電離箱の感度は線源が等しい場合、厚み測定の精度に直
接関係があって高い方が望ましい。
The sensitivity of the ionization chamber is directly related to the accuracy of thickness measurement when the radiation sources are the same, and the higher the sensitivity, the better.

また応答速度はたとえば鉄板の圧延工程などに厚み計を
使用するような場合には厚さを測定してから制御するま
でが速いほど好ましい。
Furthermore, when the thickness gauge is used in the rolling process of iron plates, the response speed is preferably as fast as possible from measuring the thickness to controlling the thickness.

したがって感度および応答性のすぐれた電離箱が要望さ
れる。
Therefore, an ionization chamber with excellent sensitivity and responsiveness is desired.

この発明は上記要望を満たすためになされたもので、電
離箱の感度を高め、かつ応答測度を速くして測定精度を
向上させ、併せてたとえば製造ラインの工程管理を容易
にできる多層電極形電離箱を提供することにある。
This invention was made to meet the above-mentioned needs, and it is a multilayer electrode type ionization chamber that can increase the sensitivity of the ionization chamber, speed up the response measurement, improve measurement accuracy, and facilitate the process control of a manufacturing line, for example. The purpose is to provide the box.

すなわち、この発明は放射線入射窓にアルミニウム部材
が使用され、かつ放射線入射方向に沿って信号取出し用
電極と高電圧印刀日用電極とが交互に複層同心円状に配
列され、しかも有感ガスが封入されてなることを特徴と
する多層電極形電離箱にある。
That is, in this invention, an aluminum member is used for the radiation entrance window, and signal extraction electrodes and high voltage impression electrodes are arranged alternately in multi-layer concentric circles along the radiation entrance direction, and the sensitive gas A multilayer electrode type ionization chamber is characterized in that it is encapsulated with:

以下、第1図と同一部分は同一符号をもって示す第2図
を参照しながら、この発明に係る電離箱の1実施例を説
明する。
Hereinafter, one embodiment of the ionization chamber according to the present invention will be described with reference to FIG. 2, in which the same parts as in FIG. 1 are designated by the same reference numerals.

この発明が従来例と異なる点をま■放射線入射窓にアル
ミニウム部材板4aを使用して窓面での吸収を小さくし
、6凍電電極を同心円的に複数の円筒2a、2b、2c
に分割して各円筒2a + 2 b +2cを円板2d
に固定し、円板2dを絶縁体3を介してリード線6に接
続し、■高電圧印加用電極をアルミニウム製窓4aに同
心円状に円筒9a。
This invention differs from the conventional example in that an aluminum member plate 4a is used for the radiation entrance window to reduce absorption on the window surface, and 6 freezing electrodes are arranged concentrically in a plurality of cylinders 2a, 2b, 2c.
Divide each cylinder 2a + 2b + 2c into a disk 2d
The disk 2d is connected to the lead wire 6 via the insulator 3, and the high voltage application electrode is placed concentrically around the aluminum window 4a in the cylinder 9a.

9bを取着し、各円筒9a、9bは前記円筒2b。9b is attached, and each cylinder 9a, 9b is the cylinder 2b.

2b、2c間に挿入された構造になっていることである
It has a structure inserted between 2b and 2c.

しかして、放射線8が窓4aを通過して電極2a 、2
b 、2cおよび9a 、9b間に到達すると有感ガス
たとえばキセノンガスは電離される。
Therefore, the radiation 8 passes through the window 4a and the electrodes 2a, 2
When reaching between b, 2c and 9a, 9b, a sensitive gas such as xenon gas is ionized.

電極2a、2b、2cおよび9a、9bにバイアス電圧
を印加して果状し電流出力とする。
A bias voltage is applied to the electrodes 2a, 2b, 2c and 9a, 9b to produce a current output.

なお、窓4aにアルミニウムを使用した場合、たとえば
ステンレス鋼(SUS304)の窓厚を0.5mmにお
いてアルミニウム(A5084)では窓厚は0.93m
mに相当する。
Note that when aluminum is used for the window 4a, for example, when the window thickness of stainless steel (SUS304) is 0.5 mm, the window thickness of aluminum (A5084) is 0.93 m.
Corresponds to m.

ステンレス鋼0.5 mmでの60 Keyのr線の透
過率は64%で、アルミニウム0.93mmでの透過率
は93係となって透過率が非常に良好になり、1.46
倍の感度が得られる。
The transmittance of 60 Key r-rays with stainless steel 0.5 mm is 64%, and the transmittance with aluminum 0.93 mm is 93, which is a very good transmittance of 1.46.
Double the sensitivity.

(ただし、放射線の線質とエネルギで吸収系数が異なる
ので、ここではAm””からのr線60Kevについて
述べたものである。
(However, since the absorption coefficient differs depending on the quality and energy of the radiation, here we will discuss r-rays of 60Kev from Am"".

)また、応答速度については各電極を同心円状円筒体を
相互に挾み込むようにして電極間隔を挾めティるので、
第2図に示したような構成においては電極間隔が115
になる。
) Also, regarding the response speed, the electrode spacing is determined by sandwiching the concentric cylinders between each electrode.
In the configuration shown in Figure 2, the electrode spacing is 115
become.

電極間隔が115になることは電離されたイオンの陽極
から陰極までの移動時間が1/25となるから電荷集成
時間は1/25に短縮できる。
When the electrode spacing is 115, the time taken for ionized ions to travel from the anode to the cathode becomes 1/25, so the charge accumulation time can be shortened to 1/25.

このことは電離箱の応答時間が速くなるので当然測定系
全体の応答時間も速くなる。
This speeds up the response time of the ionization chamber, which naturally speeds up the response time of the entire measurement system.

したがって、この発明によれば感度および応答性が向上
し、かつ窓にアルミニウムを使用シティることにより軽
量化され取扱い易い電離箱を提供することができる。
Therefore, according to the present invention, it is possible to provide an ionization chamber that has improved sensitivity and responsiveness, and is lightweight and easy to handle by using aluminum for the window.

なお、電極に使用される円筒は数が多いほど年別電圧な
らびに有感ガス圧を小さくできる利点がある。
It should be noted that the larger the number of cylinders used for the electrodes, the more advantageous it is that the annual voltage and sensitive gas pressure can be reduced.

また、有感ガスとしてはキセノンガスのほかにアルコン
、クリプトンなどの希ガスや炭酸ガス、窒素ガスなども
使用することができる。
In addition to xenon gas, rare gases such as alcone and krypton, carbon dioxide gas, and nitrogen gas can also be used as sensitive gases.

さらにこの発明では電離箱の用途例として厚み計につい
て説明したが、これに限ることなく他にも適用できる。
Further, in this invention, a thickness gauge has been described as an example of the application of the ionization chamber, but the invention is not limited to this and can be applied to other applications.

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

第1図は従来の電離箱を示す縦断面図、第2図はこの発
明に係る電離箱の1実施例を示す縦断面図である。 1・・・筒形陽極、2・・・集電極、計・・絶縁体、4
・・・窓、5・・・端板、6・7・・・リード線、8・
・・放射線入射方向。
FIG. 1 is a longitudinal sectional view showing a conventional ionization chamber, and FIG. 2 is a longitudinal sectional view showing one embodiment of the ionization chamber according to the present invention. 1... Cylindrical anode, 2... Collector electrode, Meter... Insulator, 4
...Window, 5...End plate, 6.7...Lead wire, 8.
...Radiation incident direction.

Claims (1)

【特許請求の範囲】[Claims] 1 放射線入射窓にアルミニウム部材が使用され、かつ
放射線入射方向に沿って信号取出し用電極と電圧年別用
電極とが交互に複層同心円状に配列され、しかも有感ガ
スが封入されてなることを特徴とする多層電極形電離箱
1. An aluminum member is used for the radiation entrance window, and signal extraction electrodes and voltage year electrodes are arranged alternately in a multilayer concentric circle along the radiation entrance direction, and a sensitive gas is sealed. A multilayer electrode type ionization chamber featuring:
JP1930377A 1977-02-25 1977-02-25 Multilayer electrode type ionization chamber Expired JPS5824903B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1930377A JPS5824903B2 (en) 1977-02-25 1977-02-25 Multilayer electrode type ionization chamber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1930377A JPS5824903B2 (en) 1977-02-25 1977-02-25 Multilayer electrode type ionization chamber

Publications (2)

Publication Number Publication Date
JPS53105280A JPS53105280A (en) 1978-09-13
JPS5824903B2 true JPS5824903B2 (en) 1983-05-24

Family

ID=11995643

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1930377A Expired JPS5824903B2 (en) 1977-02-25 1977-02-25 Multilayer electrode type ionization chamber

Country Status (1)

Country Link
JP (1) JPS5824903B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11442382B2 (en) 2019-07-22 2022-09-13 Hewlett-Packard Development Company, L.P. Imaging system with gloss treatment device

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01172256U (en) * 1988-05-25 1989-12-06
JP2009098095A (en) * 2007-10-19 2009-05-07 Yasuto Ioka Ionization chamber type x-ray foreign matter detector and cylindrical ionization chamber

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11442382B2 (en) 2019-07-22 2022-09-13 Hewlett-Packard Development Company, L.P. Imaging system with gloss treatment device

Also Published As

Publication number Publication date
JPS53105280A (en) 1978-09-13

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