JPH0513472B2 - - Google Patents
Info
- Publication number
- JPH0513472B2 JPH0513472B2 JP29210185A JP29210185A JPH0513472B2 JP H0513472 B2 JPH0513472 B2 JP H0513472B2 JP 29210185 A JP29210185 A JP 29210185A JP 29210185 A JP29210185 A JP 29210185A JP H0513472 B2 JPH0513472 B2 JP H0513472B2
- Authority
- JP
- Japan
- Prior art keywords
- sample
- vacuum container
- radiation
- vacuum
- radioactive contamination
- 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 - Lifetime
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- Measurement Of Radiation (AREA)
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は放射能汚染検出装置、特に試料表面の
微弱な放射能を検出する装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a radioactive contamination detection device, and particularly to a device for detecting weak radioactivity on the surface of a sample.
原子力産業分野あるいは放射性物質を取り扱う
分野において、放射能汚染の防止には細心の注意
が払われている。例えば、放射性物質の加工、成
形や取扱いに用いた装置や物品を外部に持ち出し
又は廃棄する場合においては、この装置や物品の
表面からの放射線放出による弊害を防止するため
に、これら装置や物品表面の放射能濃度が「放射
性同位元素等による放射線障害の防止に関する法
律」に基づいて定めた管理基準以下であることを
確認する必要がある。 In the nuclear industry or in fields that handle radioactive materials, great care is taken to prevent radioactive contamination. For example, when equipment or items used for processing, molding, or handling radioactive materials are to be taken outside or disposed of, the surfaces of these equipment or items should be It is necessary to confirm that the radioactive concentration of the substance is below the management standards established based on the ``Act on Prevention of Radiation Hazards Due to Radioactive Isotopes, etc.''
[従来の技術]
第1図には、従来の放射能汚染検出装置の概略
構成が示され、試料10に対向させてα線サーベ
イメータ検出器12が配置され、試料表面の放射
能濃度、第1図装置においては、α線サーベイメ
ータ検出器12によつてα線濃度が検出される。[Prior Art] FIG. 1 shows a schematic configuration of a conventional radioactive contamination detection device, in which an α-ray survey meter detector 12 is arranged facing a sample 10, and the radioactive concentration on the sample surface, the first In the apparatus shown in the figure, the α-ray concentration is detected by the α-ray survey meter detector 12.
前記α線サーベイメータ検出器12には、第2
図に示すように、放射線の入射面に外光を遮蔽す
る遮光膜14が設けられており、この遮光膜14
の近傍位置にはシンチレータ板16が配設されて
いる。そして、シンチレータ板16の後方位置に
は光電子増倍管18が設けられており、放射線強
度が光電子増倍管18によつて電気信号に変換さ
れ、更にブリーダ回路20により所望の信号処理
が行われ、図示されていない放射線計測部にて放
射能濃度の表示が行われる。 The α-ray survey meter detector 12 includes a second
As shown in the figure, a light shielding film 14 for shielding external light is provided on the radiation incident surface, and this light shielding film 14
A scintillator plate 16 is disposed near the. A photomultiplier tube 18 is provided at the rear of the scintillator plate 16, and the radiation intensity is converted into an electrical signal by the photomultiplier tube 18, and further the desired signal processing is performed by the bleeder circuit 20. , the radioactivity concentration is displayed in a radiation measuring section (not shown).
しかしながら、この種の装置においては、試料
10からの微弱放射線を高精度にて検出できない
という欠点があつた。 However, this type of device has a drawback in that it cannot detect the weak radiation from the sample 10 with high precision.
すなわち、試料10の形状が図示のごとく凹凸
形状をしている場合には、凹部から放出される放
射線を確実に検出できないという問題がある。 That is, when the sample 10 has an uneven shape as shown in the figure, there is a problem that radiation emitted from the recesses cannot be reliably detected.
すなわち、α線の飛程は3〜4cmであり、この
ため、試料10の凹面からα線サーベイメータ検
出器12のシンチレータ面までの距離を前記放射
線の飛程範囲内に設定することは極めて困難であ
り、従つて試料10の凸面からの放射線を検出す
ることは可能であるが、試料10の凹面からの放
射線検出が困難となり、このため、試料10の全
表面から放出する放射線量を高精度にて検出する
ことができないという欠点があつた。 That is, the range of α-rays is 3 to 4 cm, and therefore it is extremely difficult to set the distance from the concave surface of the sample 10 to the scintillator surface of the α-ray survey meter detector 12 within the range of the radiation. Therefore, although it is possible to detect radiation from the convex surface of the sample 10, it is difficult to detect radiation from the concave surface of the sample 10. Therefore, it is difficult to accurately measure the amount of radiation emitted from the entire surface of the sample 10. The disadvantage was that it could not be detected.
発明の目的
本発明は前記従来の課題に鑑みなされたもので
あり、その目的は、凸凹形状の試料においてもこ
の試料表面から放射される放射線を高精度にて検
出することができる放射能汚染検出装置を提供す
ることにある。Purpose of the Invention The present invention has been made in view of the above-mentioned conventional problems, and its purpose is to detect radioactive contamination that can detect radiation emitted from the surface of a sample with high accuracy even in an uneven sample. The goal is to provide equipment.
[発明の構成]
上記目的を達成するために、本発明は、内部に
試料載置台が設けられた真空容器と、真空容器の
壁面に固定配置された光電子増倍管と、光電子増
倍管と試料間に配置され真空容器に固定されたシ
ンチレータ板とを含み、試料表面の放射能汚染が
真空雰囲気中で検出されることを特徴とする。[Structure of the Invention] In order to achieve the above object, the present invention provides a vacuum container in which a sample mounting stage is provided, a photomultiplier tube fixedly arranged on the wall of the vacuum container, and a photomultiplier tube. It is characterized in that it includes a scintillator plate placed between samples and fixed to a vacuum container, and radioactive contamination on the sample surface is detected in a vacuum atmosphere.
[実施例]
第3図には、本発明に係る放射能汚染検出装置
の構成が示され、従来装置と同一部材には同一符
号を付し、その説明を省略する。本発明において
特徴的なことは、試料表面からの放射線強度を真
空雰囲気中において検出する構成としたことであ
る。[Example] FIG. 3 shows the configuration of a radioactive contamination detection device according to the present invention, and the same members as those in the conventional device are denoted by the same reference numerals, and the explanation thereof will be omitted. A feature of the present invention is that the radiation intensity from the sample surface is detected in a vacuum atmosphere.
すなわち、本発明においては、第4図に示すよ
うに、試料表面からの放射線の飛程が真空度を高
めることにより大きくなることに着目し、従つて
前述のごとく本発明は試料を真空雰囲気中に置い
て、その放射能汚染量を検出する構成とされる。 That is, the present invention focuses on the fact that the range of radiation from the sample surface increases as the degree of vacuum increases, as shown in FIG. The system is configured to detect the amount of radioactive contamination at the site.
例えば、第4図において、5Me Vのα線にあ
つては、大気中で約3.5cmの飛程であるが、真空
度を約26mmHgとすることにより飛程が100cmに増
大される。従つて、このように真空度を高めるこ
とによつて放射線の飛程を大きくでき、試料表面
から放出される放射線を確実に捕えることが可能
となる。 For example, in FIG. 4, the range of 5 Me V alpha rays is about 3.5 cm in the atmosphere, but by setting the degree of vacuum to about 26 mmHg, the range is increased to 100 cm. Therefore, by increasing the degree of vacuum in this manner, the range of the radiation can be increased, and it becomes possible to reliably capture the radiation emitted from the sample surface.
本実施例において、真空容器21の壁面には複
数個の光電子増倍管18が点在配置される。そし
て、真空容器21の内部には試料載置台22が設
けられており、この試料載置台22に試料10が
載置される。そして、試料10と光電子増倍管1
8間にはシンチレータ板16が配設される。一
方、真空容器21には排気管23が設けられてお
り、真空ポンプ24を駆動することにより真空容
器内を真空雰囲気とすることが可能となる。 In this embodiment, a plurality of photomultiplier tubes 18 are arranged on the wall surface of the vacuum container 21 in a dotted manner. A sample mounting table 22 is provided inside the vacuum container 21, and the sample 10 is placed on this sample mounting table 22. Then, sample 10 and photomultiplier tube 1
A scintillator plate 16 is disposed between 8 and 8. On the other hand, the vacuum container 21 is provided with an exhaust pipe 23, and by driving the vacuum pump 24, it is possible to create a vacuum atmosphere inside the vacuum container.
このように本実施例において、真空容器21内
を真空雰囲気とすることにより、試料10からの
放射線の飛程を大きくすることが可能となり、こ
のため、試料10の凹部からの放射線放出線をも
高精度にて検出することが可能となる。 In this example, by creating a vacuum atmosphere inside the vacuum container 21, it is possible to increase the range of the radiation from the sample 10, and therefore, the radiation emitted from the recessed portion of the sample 10 can be reduced. It becomes possible to detect with high precision.
また、本実施例においては、真空容器21内を
真空雰囲気状態にして試料10の微に弱放射線を
検出するため、真空容器内のラドン量を減少する
ことができるので、測定際してのバツクグラウン
ドを減少することが可能であり、この結果、検出
感度が改善できるという利点がある。 In addition, in this embodiment, the very weak radiation of the sample 10 is detected with the inside of the vacuum container 21 in a vacuum atmosphere, so the amount of radon in the vacuum container can be reduced, so there is no back-up during measurement. This has the advantage that the ground can be reduced and, as a result, detection sensitivity can be improved.
更に、本実施例においては、前述したように真
空容器21の壁面のほぼ全周にわたり光電子増倍
管18を複数個点在配置する結果、試料10の凸
凹状面の向きをどちらの方向に向けても試料10
の微弱放射線を高精度にて検出することができ
る。そして、また試料のいわゆる4π測定が可能
となる。 Furthermore, in this embodiment, as described above, as a result of disposing a plurality of photomultiplier tubes 18 over almost the entire circumference of the wall surface of the vacuum container 21, it is possible to direct the uneven surface of the sample 10 in either direction. Even sample 10
It is possible to detect weak radiation with high precision. Also, so-called 4π measurement of the sample becomes possible.
この試料10の放射線強度は、光電子増倍管1
8からの電気信号を処理することにより図示され
ていない表示部に表示することが可能となる。本
実施例においては、図示のごとく真空容器21の
各壁面に配置された光電子増倍管な各群ごとにブ
ロツク区分され(A〜D)、各ブロツクの光電子
増倍管18からの電気信号が第5図に示すよう
に、信号処理回路26に導かれ、この信号処理回
路26により所望の信号演算が行われる。例え
ば、この信号処理回路26から各ブロツクごとの
検出信号を取り出すことができるとともに、一方
のブロツクと他方のブロツクとの信号和を取り出
すことも可能である。また、場合によつては各ブ
ロツクを構成する光電子増倍管ごとに信号取出し
を行うことも可能である。従つて、このような信
号演算により試料表面からの放射線放射強度を高
精度にて検出できる。 The radiation intensity of this sample 10 is
By processing the electrical signals from 8, it becomes possible to display them on a display section (not shown). In this embodiment, as shown in the figure, blocks are divided into groups (A to D) of photomultiplier tubes arranged on each wall of the vacuum vessel 21, and the electric signals from the photomultiplier tubes 18 of each block are divided into blocks. As shown in FIG. 5, the signal is guided to a signal processing circuit 26, and a desired signal operation is performed by this signal processing circuit 26. For example, it is possible to extract a detection signal for each block from the signal processing circuit 26, and it is also possible to extract the signal sum of one block and the other block. In some cases, it is also possible to extract signals from each photomultiplier tube constituting each block. Therefore, by such signal calculation, the radiation intensity from the sample surface can be detected with high precision.
[発明の効果]
以上説明したように、本発明によれば、凸凹形
状の試料にあつても、この試料表面から放出され
る放射線強度を高精度にて検出することが可能と
なる。[Effects of the Invention] As described above, according to the present invention, it is possible to detect the radiation intensity emitted from the surface of the sample with high accuracy even when the sample has an uneven shape.
第1図は従来の放射能汚染検出装置を示す概略
構成図、第2図は第1図装置のα線サーベイメー
タ検出器の断面図、第3図は本発明に係る放射能
汚染検出装置を示す構成図、第4図は放射線の各
真空度に対する飛程を示す特性図、第5図は本発
明装置の信号処理を示すブロツク図である。
10……試料、16……シンチレータ板、18
……光電子増倍管、21……真空容器、22……
試料載置台。
Fig. 1 is a schematic configuration diagram showing a conventional radioactive contamination detection device, Fig. 2 is a cross-sectional view of the α-ray survey meter detector of the device shown in Fig. 1, and Fig. 3 shows a radioactive contamination detection device according to the present invention. FIG. 4 is a characteristic diagram showing the range of radiation for each degree of vacuum, and FIG. 5 is a block diagram showing signal processing of the apparatus of the present invention. 10...Sample, 16...Scintillator plate, 18
...Photomultiplier tube, 21...Vacuum container, 22...
Sample mounting table.
Claims (1)
真空容器の壁面に固定配置された光電子増倍管
と、光電子増倍管と試料間に配置され真空容器に
固定されたシンチレータ板とを含み、試料表面の
放射能汚染が真空雰囲気中で検出されることを特
徴とする放射能汚染検出装置。 2 特許請求の範囲1記載の装置において、光電
子増倍管は、真空容器のほぼ全周壁にわたつて複
数個点在配置されることを特徴とする放射能汚染
検出装置。[Claims] 1. A vacuum container having a sample mounting stage provided therein;
It includes a photomultiplier tube fixedly placed on the wall of the vacuum container and a scintillator plate placed between the photomultiplier tube and the sample and fixed to the vacuum container, and radioactive contamination on the sample surface is detected in a vacuum atmosphere. A radioactive contamination detection device characterized by: 2. The radioactive contamination detection device according to claim 1, wherein a plurality of photomultiplier tubes are scattered over substantially the entire circumferential wall of the vacuum container.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP29210185A JPS62151780A (en) | 1985-12-26 | 1985-12-26 | Radiation contamination detecting device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP29210185A JPS62151780A (en) | 1985-12-26 | 1985-12-26 | Radiation contamination detecting device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62151780A JPS62151780A (en) | 1987-07-06 |
| JPH0513472B2 true JPH0513472B2 (en) | 1993-02-22 |
Family
ID=17777558
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP29210185A Granted JPS62151780A (en) | 1985-12-26 | 1985-12-26 | Radiation contamination detecting device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62151780A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03261887A (en) * | 1990-03-12 | 1991-11-21 | Ngk Insulators Ltd | Instrument for measuring radiation of radioactive waste |
| JP2001147271A (en) * | 1999-11-22 | 2001-05-29 | Aloka Co Ltd | Radiation measuring device |
| US7267015B2 (en) | 2004-09-20 | 2007-09-11 | Quantum Corporation | System and method for testing media device doors |
-
1985
- 1985-12-26 JP JP29210185A patent/JPS62151780A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62151780A (en) | 1987-07-06 |
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