JPS595983A - Proportional counter - Google Patents

Proportional counter

Info

Publication number
JPS595983A
JPS595983A JP11595582A JP11595582A JPS595983A JP S595983 A JPS595983 A JP S595983A JP 11595582 A JP11595582 A JP 11595582A JP 11595582 A JP11595582 A JP 11595582A JP S595983 A JPS595983 A JP S595983A
Authority
JP
Japan
Prior art keywords
voltage
anode
cathode
proportional counter
case
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
JP11595582A
Other languages
Japanese (ja)
Other versions
JPH0248074B2 (en
Inventor
Toshimasa Tomota
友田 利正
Shinji Fukakusa
深草 伸二
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP11595582A priority Critical patent/JPH0248074B2/en
Publication of JPS595983A publication Critical patent/JPS595983A/en
Publication of JPH0248074B2 publication Critical patent/JPH0248074B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/18Measuring radiation intensity with counting-tube arrangements, e.g. with Geiger counters

Abstract

PURPOSE:To widen a usable temp. range, by a method wherein two coaxial cables are attached and the central conductor of one cable is connected to an anode while the central conductor of the other one is connected to a cathode and voltage is applied to the cathode and the anode in an allotted state. CONSTITUTION:When voltage required in operating a proportional counter is set to VO and voltage with +VO/2 and voltage of -VO/2 are supplied by two DC high voltage power sources 105a, 105b, because voltage VO is applied between the cathode 1 and the anode 2 of the proportional counter, this proportional counter is normally operated while an electric pulse signal generated in the proportional counter is amplified by an amplifier. When the amplified pulse signal is counted by a counting circuit, the counting of radioactive rays can be carried out. On the other hand, because voltages +VO/2 applied to coaxial cables 6a, 6b may be the half of the operation voltage VO of the proportional counter, the possibility of the generation of a minute discharge pulse in the cable becomes extremely small and said counter can be sufficiently used even at a temp. higher than a conventional limit environmental temp.

Description

【発明の詳細な説明】 この発明は、放射線を計測する比例計数管、特に高温で
使用され得る比例計数管に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a proportional counter for measuring radiation, particularly to a proportional counter that can be used at high temperatures.

従来この種の装置として第1図に示すものがあった。図
において、(1)I/ま線状の陽極、(2)は陽極(1
)と同軸状に、陽極<1)からは電気的に絶縁されて配
設された円筒状の陰極、(3)は陰陽極の間の空間に封
入された電離用ガス、(4)Iま陰・陽極から電気的に
絶縁されながらこれらを収容する気密ケース、(6)は
気密ケースの一端に取付けられた二重シールドの同軸ケ
ーブルであり、その中心導体(7)は陽極に、内部シー
ルド導体(8)は陰極に、外部シールド導体(9)は気
密ケースに電気的に接続されている。
A conventional device of this type is shown in FIG. In the figure, (1) I/line-shaped anode, (2) an anode (1
) coaxially with a cylindrical cathode electrically insulated from the anode <1), (3) an ionizing gas sealed in the space between the cathode and the anode, and (4) I or The airtight case (6) that houses the cathode and anode while being electrically insulated from them is a double-shielded coaxial cable attached to one end of the airtight case, with the center conductor (7) connected to the anode and the inner shield. The conductor (8) is electrically connected to the cathode and the outer shield conductor (9) to the airtight case.

図中”(101)は前置増幅器であシ、その内部で増幅
回路(t02)と抵抗器(108)コンデン?−(10
4)が図のように接続されている。(105)は直流高
圧電源であり、図のように前置増幅器(101)と直流
高圧電源(105)を接続させて放射線の計測を行う。
In the figure, "(101)" is a preamplifier, inside which is an amplifier circuit (t02), a resistor (108) and a capacitor (10
4) are connected as shown in the figure. (105) is a DC high voltage power supply, and as shown in the figure, the preamplifier (101) and DC high voltage power supply (105) are connected to measure radiation.

即ち、直流高圧電源により比例計数管の陰陽極間に直流
高電圧を印加し、放射線により陰陽極間のガス中に生じ
た電離電荷をガス増幅をさせながら電極に収集し、生じ
た電気的パルス信号を、増幅回路(102)で増幅した
後、図示していない計数回路で計数し放射線の計測を行
う。
That is, a high DC voltage is applied between the cathode and anode of a proportional counter tube using a DC high voltage power supply, and the ionized charges generated in the gas between the cathode and anode due to radiation are collected on the electrodes while amplifying the gas, resulting in an electrical pulse. After the signal is amplified by an amplifier circuit (102), it is counted by a counting circuit (not shown) to measure radiation.

ところで、比例計数管が強い放射線や高温の環境で使用
されるときには、同軸グープルの絶縁材料として通常よ
く使用される有機絶縁物をよ耐放射線性、耐熱性が悪い
ため使用できずアルミナやマグネシア等の無機絶縁物が
使用される。ところがこの無機絶縁ケーブルの耐電圧特
性があまりよくなく、印加電圧が高くなるとグープル内
で微小なパルス性放電を起す。このケーブル内での微小
放電パルスは、比例計数管で生じた信号、(ルスと同様
に増幅器で増幅され計数回路で計数されるので、信号パ
ルスと区別がつかず、放射線計測上の妨害となっていた
By the way, when proportional counter tubes are used in environments with strong radiation or high temperatures, organic insulators that are commonly used as insulating materials for coaxial groups cannot be used because of their poor radiation resistance and heat resistance, so alumina, magnesia, etc. of inorganic insulators are used. However, the withstand voltage characteristics of this inorganic insulated cable are not very good, and when the applied voltage increases, minute pulsed discharges occur within the group. The minute discharge pulses within this cable are the signals generated by the proportional counter tube (similar to the Luss, they are amplified by an amplifier and counted by a counting circuit, so they are indistinguishable from signal pulses and can cause interference in radiation measurement. was.

なお、ケーブル内での微小放電パルスの発生頻度は、第
2図に示すように、印加電圧が高くなると大きくなり、
また環境温度が高くなると、微小放電パルス開始電圧が
低下しまた微小放電、<ルス発生頗度も増える。そのた
め、室温では満足に使用できるものも、高温環境では微
小放電/<パルスの発生のため使用できないなどの欠点
があった。
Furthermore, as shown in Figure 2, the frequency of occurrence of minute discharge pulses within the cable increases as the applied voltage increases.
Furthermore, as the environmental temperature rises, the microdischarge pulse starting voltage decreases, and the frequency of microdischarge and <Russ generation also increases. For this reason, even though they can be used satisfactorily at room temperature, they have drawbacks such as being unable to be used in high-temperature environments due to the generation of minute discharges/pulses.

この発明は、上記のような従来のものの欠点を除去する
ため釦なされたもので、2本の同軸グープルを取り付け
、一方の中心導体は陽極に、他方の中心導体は陰極に接
続し、陰陽極に電圧を分担して印加することKより、使
用できる温度範囲の広い比例計数管を提供することを目
的としている。
This invention was made in order to eliminate the drawbacks of the conventional ones as described above.Two coaxial groups are attached, one center conductor is connected to the anode, the other center conductor is connected to the cathode, and the cathode and anode are connected. The purpose of the present invention is to provide a proportional counter that can be used over a wide temperature range by applying voltage in a divided manner.

以下、この発明の一実施例について、説明する。An embodiment of the present invention will be described below.

第8図において、(1)は線状の陽極、(2)は陽極(
1)と同軸状に、陽極(1)からは電気的に絶縁されて
配設された円筒状の陰極、(3)は陰陽極の間の空間に
封入された電離用ガス、(4)は陰・陽極から電気的に
絶縁されながら、これらを収容する気密ケース、(6a
)(6b)は気密ケースの一端に取付けられた同軸ケー
ブルであり、それぞれの中心導体(7a)および(7b
)tよ、それぞれ陽極および陰極に電気的に接続されて
おり、外部シールド導体(9a)および(9b)tま気
密ケースに電気的に接続されている。(101)は11
置増幅器であり、その内部で、増幅回路(102)と抵
抗器(108a)(108b)、コンデンサ(104)
が図のように接続されている。(105a ) (10
5b )は極性の異る直流高圧電源であり、図のように
抵抗器(108a)(108b)を介して中心導体(7
a)(7b)に接続されている。
In Figure 8, (1) is a linear anode, (2) is an anode (
A cylindrical cathode is arranged coaxially with 1) and electrically insulated from the anode (1), (3) is an ionizing gas sealed in the space between the cathode and anode, and (4) is a cylindrical cathode arranged coaxially with the anode (1). An airtight case (6a) that houses the negative and anodes while being electrically insulated from them
) (6b) is a coaxial cable attached to one end of the airtight case, with its respective center conductor (7a) and (7b)
) are electrically connected to the anode and cathode, respectively, and the outer shield conductors (9a) and (9b) are electrically connected to the airtight case. (101) is 11
It is a stationary amplifier, and inside it, an amplifier circuit (102), resistors (108a) (108b), and a capacitor (104) are installed.
are connected as shown in the figure. (105a) (10
5b) is a DC high voltage power supply with different polarity, and as shown in the figure, it is connected to the center conductor (7
a) Connected to (7b).

さて、比例計数管を動作させるに必餅な電圧をVoとす
ると2台の直流高圧電源により+vO/2および−VO
/2の電圧を供給してやれば、比例計数管の陰陽極間に
はvOの電圧が印加されるので、比例計数管は正常に動
作し比例計数管内で生じた電気、<ルス信号を増幅器で
増幅し、その後、計数回路で計数すれば放射線の計測が
できる。一方、同軸グープルに印加される電圧tよ、比
例計数管の動作電圧の半分でよいので、グープル内での
微小放電ノfルス発生の可能性tよ、はるかに小さくな
り、従来の限界環境温度よりも高い湿度でも、十分使用
できることになる。これを第2図を用いて説明する。
Now, if the voltage required to operate the proportional counter tube is Vo, then +vO/2 and -VO are generated by two DC high-voltage power supplies.
If a voltage of /2 is supplied, a voltage of vO will be applied between the cathode and anode of the proportional counter, so the proportional counter will operate normally and the electricity generated within the proportional counter, the pulse signal, will be amplified by the amplifier. After that, radiation can be measured by counting with a counting circuit. On the other hand, since the voltage t applied to the coaxial goople can be half of the operating voltage of the proportional counter, the possibility of minute discharge nozzles occurring within the goople is much smaller, and the conventional limit environmental temperature This means that it can be used satisfactorily even at higher humidity. This will be explained using FIG.

図はある温度T。での微小放電パルス発生頻度である。The figure shows a certain temperature T. This is the frequency of micro discharge pulses occurring at

図からケーブルにvOの電圧が印加されると、微小放電
パルスが発生し、印加電圧がVO/2であれば微小放電
パルスは発生しないことがわかる。従って、従来のよう
に一本のクープルで、比例計数管の動作に必要な電圧V
oを供給していた場合、ケーブル内で発生する微小放電
パレスが妨害となって、正確な放射線の計測が行えない
が、本考案のように2木のグープルで+VO/2、−V
O/2を供給することにより比例計数管の動作に必要な
電圧■0を与えると、ケーブル内で微小放電パルスは発
生せず正確な放射線の計測が行えるっ なお上記においては、2本のケーブルに1極性をかえて
動作電圧の半分の電圧を印加するようにしたが、動作電
圧の配分は、例えば+2Vo/a *−Vo/sとして
も、相当の改善効果があり、必ずしも半分づつに配分す
る必要はない。
It can be seen from the figure that when a voltage of vO is applied to the cable, a minute discharge pulse is generated, and when the applied voltage is VO/2, no minute discharge pulse is generated. Therefore, unlike the conventional method, with one couple, the voltage V required for the operation of the proportional counter tube is
If 0 is supplied, the minute discharge pulses generated within the cable will cause interference, making it impossible to measure the radiation accurately.
By supplying O/2, the voltage necessary for the operation of the proportional counter tube■ If 0 is applied, no minute discharge pulses are generated within the cable, allowing accurate radiation measurement.In the above example, two cables However, even if the operating voltage distribution is +2Vo/a *-Vo/s, for example, there is a considerable improvement effect, and it is not necessary to distribute it in half. do not have to.

また、上記実施例でtよ、気密容器に取付ける同軸ケー
ブルのしゃへい導体は一重としたが、電磁誘導障害を軽
減するために、二重にすることもできる。この場合、第
4図に示すように、気密容器と陰極との間に、両者から
電気的に絶縁してシールド筒(5)を配設し、同軸ケー
ブルの内部シールド導体(8a)(8b)と電気的に接
続すれば一層効果的である。
Further, in the above embodiment, the shielding conductor of the coaxial cable attached to the airtight container is single layered, but it may be double layered in order to reduce electromagnetic induction interference. In this case, as shown in Fig. 4, a shield tube (5) is provided between the airtight container and the cathode so as to be electrically insulated from both, and the inner shield conductor (8a) (8b) of the coaxial cable is It will be even more effective if it is electrically connected to the

以上のようにこの発明は、陰陽極を収納し、上記陰陽極
から電気的に絶縁したケース、及びこのケースに収付け
た2木の同軸ケーブルを有し、上記同軸グープルの一方
の中心導体は上記陽極に、他方の中心導体t:+ニー1
z記陰極に電気的に接続し、上記2本の同軸ケーブルの
外部シールド導体は上記ケースに電気的に接続し、上記
陽極には上記ケースに対してプラス側の電圧を印加し、
」1記陰極には上記ケースに対してマイナス側の電圧を
印加するようにしたので、比例計数管の動作に必要な電
圧を2本のグープルで分担して供給することができ、ケ
ーブルには、動作電圧より低い電圧を印加すればよくな
るので、ケーブル内で発生する微小放電パルスの問題が
軽減され、高温環境下でも使用できるものが容易に得ら
れる効果がある。
As described above, the present invention includes a case that houses a cathode and anode and is electrically insulated from the cathode and anode, and two coaxial cables that are housed in this case, and the center conductor of one of the coaxial groups is To the above anode, the other center conductor t: + knee 1
z electrically connected to the cathode, external shield conductors of the two coaxial cables are electrically connected to the case, and a positive voltage is applied to the anode with respect to the case,
1) Since the negative voltage is applied to the cathode of the above case, the voltage necessary for the operation of the proportional counter tube can be shared between the two groups, and the cable is Since it is only necessary to apply a voltage lower than the operating voltage, the problem of minute discharge pulses occurring within the cable is alleviated, and it is possible to easily obtain a device that can be used even in a high-temperature environment.

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

第1図は従来の比例計数管を示す模式図、第2図は、ケ
ーブル内で発生する微小放電パルスの頻度と印加電圧の
関係を示す特性図、第8図は、この発明の一実施例によ
る比例計数管を示す模式図第4図t±、この発明の他の
実施例による比例計数管を示す模式図である。 図において、(1) 11陽極、(2)Iま陰極、(3
)は電離用ガス、(4)はケース、(6aX6b)は同
軸ケーブル、(7a)(7b)tお(柑キ導体、(9a
)(9b)は外部シールド導体である。 なお図中同一符号は同−又は相当部分を示す。 代理人 葛野信− 第1図 第2図 第3図 oyb 第4図 手続補正書(自発) 1.事件の表示    特願昭6!−115965号2
、発明の名称   比例計数管 3、補正をする者 事件との関係   特許出願人 住 所     東京都千代田区丸の内二丁目2番3号
名 称(601)   三菱電機株式会社代表者片山仁
八部 4、代理人 住 所     東京都千代田区丸の自重丁目2番3号
5、補正の対象 明細書の発明の詳細な説明の欄 6、補正の内容 (1)明細書の第6頁第2行の「放電パレス」を「放電
パルス」と訂正する。 以  上
Fig. 1 is a schematic diagram showing a conventional proportional counter tube, Fig. 2 is a characteristic diagram showing the relationship between the frequency of minute discharge pulses generated in the cable and the applied voltage, and Fig. 8 is an embodiment of the present invention. Figure 4 t± is a schematic diagram showing a proportional counter according to another embodiment of the present invention. In the figure, (1) 11 anodes, (2) I cathodes, (3
) is the ionizing gas, (4) is the case, (6aX6b) is the coaxial cable, (7a) (7b) (conductor), (9a
) (9b) is an outer shield conductor. Note that the same reference numerals in the figures indicate the same or equivalent parts. Agent Makoto Kuzuno - Figure 1 Figure 2 Figure 3 oyb Figure 4 Procedural amendment (voluntary) 1. Display of the incident Special request in 1973! -115965 No. 2
, Title of the invention Proportional counter 3, Relationship to the case of the person making the amendment Patent applicant address 2-2-3 Marunouchi, Chiyoda-ku, Tokyo Name (601) Mitsubishi Electric Corporation Representative Hitachi Katayama 4; Agent Address: 2-3-5, Maruno-Jiju-chome, Chiyoda-ku, Tokyo, Column 6 of Detailed Description of the Invention in the Specification Subject to Amendment, Contents of Amendment (1) " Correct "discharge pulse" to "discharge pulse". that's all

Claims (1)

【特許請求の範囲】[Claims] (1)線状の陽極、この陽極から電気的に絶縁し、陽極
を内包するよう配設した陰極、・上記陰陽極間の空間に
封入した電離用ガス、上記陰陽極を収納し、上記陰陽極
から電気的に絶縁したケース、及びこのケースに取付け
た2本の同軸ケーブルを有し、上記同軸グープルの一方
の中心導体は上記陽極に、他方の中心導体は上記陰極に
電気的に接続し、上記2木の同軸ケーブルの外部シール
ド導体は上記ケースに電気的に接続し、上記陽極には上
記ケースに対してプラス側の電圧を印加し、上記陰極に
は上記ケースに対してマイナス側の電圧を印加するよう
にした比例計数管。
(1) A linear anode, a cathode that is electrically insulated from the anode and arranged to contain the anode, an ionizing gas sealed in the space between the cathode and the anode, and a cathode that houses the cathode and the anode. It has a case electrically insulated from the pole, and two coaxial cables attached to the case, one center conductor of the coaxial group is electrically connected to the anode, and the other center conductor is electrically connected to the cathode. , the outer shield conductors of the two coaxial cables are electrically connected to the case, a voltage on the positive side with respect to the case is applied to the anode, and a voltage on the negative side with respect to the case is applied to the cathode. A proportional counter to which voltage is applied.
JP11595582A 1982-07-02 1982-07-02 HIREIKEISUKAN Expired - Lifetime JPH0248074B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11595582A JPH0248074B2 (en) 1982-07-02 1982-07-02 HIREIKEISUKAN

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11595582A JPH0248074B2 (en) 1982-07-02 1982-07-02 HIREIKEISUKAN

Publications (2)

Publication Number Publication Date
JPS595983A true JPS595983A (en) 1984-01-12
JPH0248074B2 JPH0248074B2 (en) 1990-10-23

Family

ID=14675276

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11595582A Expired - Lifetime JPH0248074B2 (en) 1982-07-02 1982-07-02 HIREIKEISUKAN

Country Status (1)

Country Link
JP (1) JPH0248074B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011080862A (en) * 2009-10-07 2011-04-21 Mitsubishi Electric Corp Radiation monitor
US9190250B2 (en) 2013-07-03 2015-11-17 Nihon Dempa Kogyo Co., Ltd Radiation measurement apparatus
US9378935B2 (en) 2013-12-04 2016-06-28 Nihon Dempa Kogyo Co., Ltd. Geiger-Muller counter tube and radiation measurement apparatus

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011080862A (en) * 2009-10-07 2011-04-21 Mitsubishi Electric Corp Radiation monitor
US9190250B2 (en) 2013-07-03 2015-11-17 Nihon Dempa Kogyo Co., Ltd Radiation measurement apparatus
US9378935B2 (en) 2013-12-04 2016-06-28 Nihon Dempa Kogyo Co., Ltd. Geiger-Muller counter tube and radiation measurement apparatus

Also Published As

Publication number Publication date
JPH0248074B2 (en) 1990-10-23

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