JPS6135655B2 - - Google Patents
Info
- Publication number
- JPS6135655B2 JPS6135655B2 JP9246381A JP9246381A JPS6135655B2 JP S6135655 B2 JPS6135655 B2 JP S6135655B2 JP 9246381 A JP9246381 A JP 9246381A JP 9246381 A JP9246381 A JP 9246381A JP S6135655 B2 JPS6135655 B2 JP S6135655B2
- Authority
- JP
- Japan
- Prior art keywords
- counting device
- energy
- radiation
- spherical shell
- tube
- 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
Links
- 230000005855 radiation Effects 0.000 claims description 14
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 claims description 6
- 239000000463 material Substances 0.000 claims description 2
- 239000011257 shell material Substances 0.000 claims 3
- 230000035945 sensitivity Effects 0.000 description 11
- 238000010586 diagram Methods 0.000 description 3
- 239000007789 gas Substances 0.000 description 3
- 239000002184 metal Substances 0.000 description 3
- 238000002834 transmittance Methods 0.000 description 3
- 239000005028 tinplate Substances 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 229910052736 halogen Inorganic materials 0.000 description 1
- 150000002367 halogens Chemical class 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 1
- 229910052754 neon Inorganic materials 0.000 description 1
- GKAOGPIIYCISHV-UHFFFAOYSA-N neon atom Chemical compound [Ne] GKAOGPIIYCISHV-UHFFFAOYSA-N 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J47/00—Tubes for determining the presence, intensity, density or energy of radiation or particles
- H01J47/08—Geiger-Müller counter tubes
Landscapes
- Measurement Of Radiation (AREA)
Description
【発明の詳細な説明】
本発明は、放射線量の検出等に用いられるガイ
ガ・ミユラー計数装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a Geiga-Muller counting device used for detecting radiation doses and the like.
金属小筒内に金属芯を挿入し、内部にヘリウム
とネオンガスおよびイオン消去用のハロゲンガス
を充填し、プラトー領域において、放射線を検出
するガイガ・ミユラー計数管(以下GM管とい
う)がガイガ・ミユラー計数装置(以下GM計数
装置という)に広く用いられている。 Gaiga-Muller counter tubes (hereinafter referred to as GM tubes) detect radiation in the plateau region by inserting a metal core into a small metal cylinder and filling the inside with helium, neon gas, and halogen gas for ion erasure. Widely used in counting devices (hereinafter referred to as GM counting devices).
そのようなGM管の感度は、封入ガスの吸収効
率に依存して200KeV以上の高エネルギ領域では
感度が低く、かつ一定であるが200KeV以下の低
エネルギ領域では感度が高く、感度が放射線のエ
ネルギにより変化するという問題がある。 The sensitivity of such a GM tube depends on the absorption efficiency of the filled gas, and is low and constant in the high energy region of 200 KeV or more, but is high in the low energy region of 200 KeV or less, and the sensitivity increases depending on the energy of the radiation. There is a problem that it changes depending on the situation.
第1図に枚射線のエネルギー(KeV)を横軸に
してGM管の感度(カウント/レントゲン)を縦
軸にして前記GM管のエネルギー特性を曲線aで
示してある。 In FIG. 1, the energy characteristic of the GM tube is shown by curve a, with the horizontal axis representing the energy of the radiation (KeV) and the vertical axis representing the sensitivity (counts/roentgen) of the GM tube.
この問題を解決するために、GM管の外周をエ
ネルギの低い領域の放射線を吸収する金属筒で囲
み、200KeV以下の感度を降下させるようにした
GM計数装置がある。第2図はそのような対策を
施した従来例を示す図である。 To solve this problem, we surrounded the outer periphery of the GM tube with a metal tube that absorbs radiation in the low-energy region, reducing the sensitivity below 200 KeV.
There is a GM counting device. FIG. 2 is a diagram showing a conventional example in which such a countermeasure is taken.
GM管1はプラスチツクの窓3を有する錫の管
状の外套2および4の内側に挿入されており、比
較的エネルギに低い放射線の相当部分を錫の管状
の外套2および4で吸収することによりエネルギ
特性を改善したものである。第1図に放射線のエ
ネルギー(KeV)に対する厚さ2mmの錫の透過率
(%)を縦軸にして、曲線cで示してある。図か
ら100KeV近辺以下での透過率は極めて小さく、
60KeV近辺では実質的に透過しないということが
理解できる。 The GM tube 1 is inserted inside a tin tubular jacket 2 and 4 with a plastic window 3 and absorbs a significant portion of the relatively low-energy radiation in the tin tubular jacket 2 and 4, thereby generating energy. It has improved characteristics. In FIG. 1, the transmittance (%) of a 2 mm thick tin with respect to radiation energy (KeV) is plotted as a curve c on the vertical axis. From the figure, the transmittance is extremely small below around 100KeV.
It can be understood that there is virtually no transmission around 60KeV.
すなわち従来のGM計数装置におけるプラスチ
ツク窓3は、これを設けてないと60KeV近辺の放
射線は全部遮断されるので、そのような放射線を
一部透過させる目的で設けたものである。 That is, the plastic window 3 in the conventional GM counting device is provided for the purpose of allowing some of the radiation to pass through, since if it were not provided, all radiation around 60 KeV would be blocked.
このような構成によれば、エネルギ特性を全体
として改善することができるプラスチツク窓3に
対向する方向に低エネルギのX線に対して鋭い指
向性が現れるので好ましくない。 Such a configuration is undesirable because a sharp directivity appears for low-energy X-rays in the direction facing the plastic window 3, which can improve the energy characteristics as a whole.
本発明の目的は、前述した問題を解決した無指
向性GM計数装置を提供することにある。 An object of the present invention is to provide an omnidirectional GM counting device that solves the above-mentioned problems.
前記目的を達成するために本発明による無指向
性GM計数装置は、管状のGM管を比較的低エネ
ルギの放射線を遮断する材料の球殻内に固定し、
その球殻に多数の透孔を均一に分布させて構成し
てある。 In order to achieve the above object, the omnidirectional GM counting device according to the present invention fixes a tubular GM tube within a spherical shell of a material that blocks relatively low-energy radiation;
The spherical shell has a large number of holes evenly distributed in it.
前記構成によれば、エネルギ特性の良好な無指
向性GM計数装置が実現でき本発明の目的は完全
に達成できる。 According to the above configuration, an omnidirectional GM counting device with good energy characteristics can be realized, and the object of the present invention can be completely achieved.
以下図面等を参照して、本発明によるGM計数
装置をさらに詳しく説明する。 The GM counting device according to the present invention will be explained in more detail below with reference to the drawings and the like.
第3図は、本発明によるGM計数装置の実施例
を示す図であり、内部構造を示すために一部破断
して示してある。GM管1の外周壁からの引出線
1b、中心に張られている心線1aは一方向にま
とめて引き出される。錫の厚さ2mmの板よりなる
球殻5には透孔6が球殻中心に向けて多数設けら
れている。 FIG. 3 is a diagram showing an embodiment of the GM counting device according to the present invention, and is partially cut away to show the internal structure. The lead wire 1b from the outer circumferential wall of the GM tube 1 and the core wire 1a stretched at the center are pulled out in one direction all at once. A spherical shell 5 made of a tin plate with a thickness of 2 mm is provided with a large number of through holes 6 toward the center of the spherical shell.
この透孔6は全表面に均一に分布するように
し、この実施例では直径40mmの球殻に直径2mmの
透孔6を24個設けている。 The holes 6 are uniformly distributed over the entire surface, and in this embodiment, 24 holes 6 with a diameter of 2 mm are provided in a spherical shell with a diameter of 40 mm.
上記構成のGM計数装置のエネルギー感度特性
は第1図のbに示すとおりきわめて平担な特性が
得られている。感度の単位は(カウント/レント
ゲン)である。 The energy sensitivity characteristics of the GM counting device having the above configuration are extremely flat, as shown in b in FIG. The unit of sensitivity is (counts/roentgen).
先に説明した曲線aは第3図に示す構成で球殻
5をとり除いたGM管1だけの特性に相当する。 The curve a described above corresponds to the characteristics of only the GM tube 1 with the configuration shown in FIG. 3 from which the spherical shell 5 is removed.
第4図は第2図に示した従来の装置と前記実施
例装置の指向性の比較をして示してある。 FIG. 4 shows a comparison of the directivity of the conventional device shown in FIG. 2 and the device of the embodiment.
図中、線A,B,Cは従来のGM計数装置の
60KeV,122KeVおよび660KeVの放射線について
の指向特性、線D,E,Fは本発明の実施例の
GM計数装置の60KeV,122KeVおよび660KeVの
放射線についての指向性を示すものである。各
GM計数装置の中心軸方向を0゜とし、放射線の
放射方向を0゜,30゜,45゜,60゜,90゜として
照射し、90゜における感度をそれぞれ100として
一致させ比較している。 In the figure, lines A, B, and C represent the conventional GM counting device.
Directional characteristics for 60KeV, 122KeV and 660KeV radiation, lines D, E and F are of the embodiment of the present invention.
This shows the directivity of the GM counter for 60KeV, 122KeV, and 660KeV radiation. each
The direction of the central axis of the GM counter is set at 0°, and the radiation directions are irradiated at 0°, 30°, 45°, 60°, and 90°, and the sensitivity at 90° is set as 100 for each, and the comparison is made.
第2図に示した従来のGM計数装置は線A,B
およびCが示すように90゜(プラスチツク窓3の
方向)0゜方向に感度を持ち、45゜の感度は著る
しく低下している。これに対して本発明による前
記実施例GM計数装置は線D,EおよびFが示す
ように0゜と90゜方向の感度が一致し、30゜,45
゜,60゜の点において感度がわずかに大きくなる
だけで、概ね変化しないと言うことができる。 The conventional GM counting device shown in Figure 2 shows lines A and B.
As shown in FIGS. and C, the sensitivity is in the 90° (direction of the plastic window 3) 0° direction, and the sensitivity at 45° is significantly reduced. On the other hand, the GM counting device according to the embodiment of the present invention has the same sensitivity in the 0° and 90° directions, as shown by lines D, E, and F;
It can be said that the sensitivity increases only slightly at the angles of 60° and 60°, but remains essentially unchanged.
以上詳しく説明したように本発明によれば、エ
ネルギ特性の秀れた無指向性のGM計数装置が実
現できる。 As described above in detail, according to the present invention, it is possible to realize an omnidirectional GM counting device with excellent energy characteristics.
第1図はGM管およびGM計数装置のエネルギ
特性a,bと錫板の透過率特性cを示すグラフ、
第2図は従来のGM計数装置の構成例を示す図、
第3図は本発明によるGM計数装置の実施例を一
部破断して示した図、第4図は実施例装置の指向
性を従来装置と比較して示したグラフである。
1……GM管、2,4……錫外套、3……プラ
スチツク窓、5……錫球殻、6……透孔。
Figure 1 is a graph showing the energy characteristics a and b of the GM tube and GM counting device and the transmittance characteristic c of the tin plate.
Figure 2 is a diagram showing an example of the configuration of a conventional GM counting device.
FIG. 3 is a partially cutaway view of an embodiment of the GM counting device according to the present invention, and FIG. 4 is a graph showing the directivity of the embodiment device in comparison with a conventional device. 1... GM pipe, 2, 4... tin mantle, 3... plastic window, 5... tin spherical shell, 6... through hole.
Claims (1)
線を遮断する材料の球殻内に固定し、その球殻に
多数の透孔を均一に分布させて構成した無指向性
GM計数装置。 2 前記球殻材料は錫である特許請求の範囲第1
項記載の無指向性GM計数装置。[Claims] 1. An omnidirectional system in which a tubular GM tube is fixed within a spherical shell made of a material that blocks relatively low-energy radiation, and a large number of through holes are uniformly distributed in the spherical shell.
GM counting device. 2. Claim 1, wherein the spherical shell material is tin.
Omnidirectional GM counting device as described in section.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9246381A JPS57208053A (en) | 1981-06-16 | 1981-06-16 | Non-directional gm counter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9246381A JPS57208053A (en) | 1981-06-16 | 1981-06-16 | Non-directional gm counter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57208053A JPS57208053A (en) | 1982-12-21 |
| JPS6135655B2 true JPS6135655B2 (en) | 1986-08-14 |
Family
ID=14055041
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9246381A Granted JPS57208053A (en) | 1981-06-16 | 1981-06-16 | Non-directional gm counter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57208053A (en) |
-
1981
- 1981-06-16 JP JP9246381A patent/JPS57208053A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57208053A (en) | 1982-12-21 |
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