JPS6033075A - Plastic scintillator - Google Patents

Plastic scintillator

Info

Publication number
JPS6033075A
JPS6033075A JP14058083A JP14058083A JPS6033075A JP S6033075 A JPS6033075 A JP S6033075A JP 14058083 A JP14058083 A JP 14058083A JP 14058083 A JP14058083 A JP 14058083A JP S6033075 A JPS6033075 A JP S6033075A
Authority
JP
Japan
Prior art keywords
residual monomer
plastic scintillator
plastic
scintillator
period
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
JP14058083A
Other languages
Japanese (ja)
Other versions
JPH0472872B2 (en
Inventor
Tatsu Hiraga
平賀 龍
Shigeo Sato
茂雄 佐藤
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 JP14058083A priority Critical patent/JPS6033075A/en
Publication of JPS6033075A publication Critical patent/JPS6033075A/en
Publication of JPH0472872B2 publication Critical patent/JPH0472872B2/ja
Granted 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
    • G01T1/20Measuring radiation intensity with scintillation detectors
    • G01T1/203Measuring radiation intensity with scintillation detectors the detector being made of plastics

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Molecular Biology (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Length-Measuring Devices Using Wave Or Particle Radiation (AREA)
  • Measurement Of Radiation (AREA)
  • Luminescent Compositions (AREA)

Abstract

PURPOSE:To volatilize speedily an internal residual monomer, and to shorten considerably a keeping period after manufacture and to improve a responding speed by boring holes which communicate with the outside in the internal core part of a plastic scintillator formed into a block in a desired shape. CONSTITUTION:For example, four communication holes 16 which communication with the outside are bored in the inner center part at the circumference of the center of the main columnar body 15a of the plastic scintillator 15 used as a radiation thickness measurement type from the bottom surface in parallel to the axial line of the main body 15a. In another method, one large-diameter hole 16 or horizontal hole 16 is formed in the center part. It takes conventionally about one year to remove the residual monomer after the injection and polymerization of plastic, to shorter a period about two months; and the product is required to left as it is for stabilization for a long period because a decrease in light output due to the residual monomer is slow, but the period is shortened considerably to obtain the scintillator having quick response.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、放射線検出に用いるプラスチックシンチレー
タに関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a plastic scintillator used for radiation detection.

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

第1図はプラスチックシンチレータが用いられている放
射線厚み計測定系のブロック図である。
FIG. 1 is a block diagram of a radiation thickness meter measurement system using a plastic scintillator.

線源容器(1)内の放射線源(2)から放射される放射
線(3)は、板状の被測定物(4)を透過してプラスチ
ックシンチレータ(5)に入る。放射線(3)が入射す
るとプラスチックシンチレータ(5)は発光し、この発
光な光電子増倍管(6)で電流に変換し増幅する。この
電流をプリアンプ(力で電圧に変換し信号処理部(8)
に入力する。信号処理部(8)で種々の演算をして被測
定物(4)の厚みをめ、プロコン(10)からの設定値
との差、すなわち偏差信号を記録計(9)およびプロコ
ンa0へ出力する。
Radiation (3) emitted from a radiation source (2) within a radiation source container (1) passes through a plate-shaped object to be measured (4) and enters a plastic scintillator (5). When radiation (3) is incident, the plastic scintillator (5) emits light, which is converted into an electric current and amplified by a photomultiplier tube (6). This current is converted into voltage by the preamplifier (signal processing unit (8)
Enter. The signal processing section (8) performs various calculations to determine the thickness of the object to be measured (4), and outputs the difference from the set value from the program controller (10), that is, a deviation signal, to the recorder (9) and program controller a0. do.

ところで、プラスチックシンチレータの製造は、約14
0℃の液体中でスチレン」−化合物(または、ビニール
トルエン士化合物)を重合させてポリスチレン(または
、ポリビニールトルエン)を製造するが、このとき重合
しないスチレン(または、ビニールトルエン)が発生す
る。これを残留モノマという。この残留モノマは、放射
線が入射した際に生ずる光の減衰時間が長い、すなわち
応答が遅いという欠点の要因となる。
By the way, the production of plastic scintillators takes about 14
Polystyrene (or polyvinyl toluene) is produced by polymerizing a styrene compound (or vinyl toluene compound) in a liquid at 0° C. At this time, unpolymerized styrene (or vinyl toluene) is generated. This is called residual monomer. This residual monomer causes a drawback that the decay time of light that occurs when radiation is incident is long, that is, the response is slow.

残留モノマは除々(二揮発して行くが、放射線厚み計の
検出器としてのプラスチックシンチレータは、精度上重
要な誤差要因である一統計ノイズを減少させるには成程
度の体積が必要であり、かなり大きなものとなる。この
場合、プラスチックンンチレータの中心部の残留モノマ
が抜は切るには長時間を要する。
The residual monomer gradually evaporates (2), but the plastic scintillator used as a detector in a radiation thickness meter requires a large volume to reduce statistical noise, which is an important error factor for accuracy, and is quite large. In this case, it takes a long time to remove the residual monomer from the center of the plastic enticillator.

従来のプラスチックシンチレータを第2図に示す。プラ
スチックシンチレータ(5)は、中実の円柱状の本体(
5a)の上面に、光電子増倍管への結合部突・ をなすライトパイプ(5b)が峰設された形状をしてお
り、本体(5;l)の中心部の残留モノマの揮発が遅く
、そのため製造後長期間(例えば1年間程度)放置して
おかないと使用できなかった。残留モノマが抜は切って
いないプラスチックシンチレータを第1図に示した放射
線厚み計に用いた場合のプラスチックシンチレータ(5
)の立上り特性を示したのが第3図で、縦軸は時間、横
軸はプラスチックシンチレータの光出力を示す。図に示
す直線(4)は、第1図における被測定物(4)が線源
(2)からの放射線(3)の経路に挿入されていないと
きのプラスチックシンチレータ(5)の光出力を示し、
被測定物(4)による減衰を受けない放射線が入射する
ので光出力が大である。図示のB点で被測定物が挿入さ
れると、プラスチックシンチレータへ入射する放射線が
被測定物によって減衰されるため、プラスチックシンチ
レータの光出力は直ちに低下する筈であるが、残留モノ
マにより発光の減衰時間が長いため(二図示の曲線(C
)のように光出力が除々に低下して、減衰された放射線
の入射時に相当する光出力に落ち付く応答を示す。ずな
わち、残留モノマがあるために時刻1.からt2までの
応答遅れ時間があることがわかる。
A conventional plastic scintillator is shown in FIG. The plastic scintillator (5) has a solid cylindrical body (
The top surface of 5a) is shaped like a light pipe (5b) that forms a connecting part to the photomultiplier tube, and the residual monomer in the center of the main body (5; l) is slow to volatilize. Therefore, it could not be used unless it was left for a long period of time (for example, about one year) after manufacture. The plastic scintillator (5) when a plastic scintillator with no residual monomer removed is used in the radiation thickness meter shown in Figure 1.
) is shown in FIG. 3, where the vertical axis shows time and the horizontal axis shows the optical output of the plastic scintillator. The straight line (4) shown in the figure indicates the optical output of the plastic scintillator (5) when the object to be measured (4) in Figure 1 is not inserted into the path of the radiation (3) from the radiation source (2). ,
Since radiation that is not attenuated by the object to be measured (4) enters, the optical output is large. When the object to be measured is inserted at point B in the figure, the radiation incident on the plastic scintillator is attenuated by the object to be measured, so the optical output of the plastic scintillator should immediately decrease, but the residual monomer causes attenuation of the light emission. Because the time is long (the curve shown in the second figure (C)
) shows a response in which the optical output gradually decreases and settles down to the optical output corresponding to the incidence of attenuated radiation. That is, due to the residual monomer, time 1. It can be seen that there is a response delay time from t2 to t2.

〔発明の目的〕[Purpose of the invention]

本発明は、残留モノマが抜は切るのに要する期間が大幅
に短縮されたプラスチックシンチレータを提供すること
を目的とする。
An object of the present invention is to provide a plastic scintillator in which the period required for removal of residual monomer is significantly shortened.

〔発明の概要〕[Summary of the invention]

本発明は、所望の形状をしたブロック(=形成されたプ
ラスチックシンチレータの内芯部に、外気に連通ずる少
なくとも1個の連通穴を穿設することにより、残留モノ
マの揮発を早めるようにして所期の目的を達成した。
The present invention provides a method of accelerating the volatilization of residual monomer by drilling at least one communication hole communicating with the outside air in the inner core of a plastic scintillator having a desired shape. Achieved the purpose of the term.

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

以下、本発明の実施例を図面?参照して説明する。 Below are drawings of embodiments of the present invention? Refer to and explain.

本発明一実施例のプラスチックシンチレータを第4図に
示す。本発明一実施例のプラスチックシンチレータ(■
5)は円柱状の本体(15a)の上面に、光電子j角倍
管への結合部をなすライトパイプ(15b)が突設され
た形状をしており、本体(15a)の中心されている。
A plastic scintillator according to an embodiment of the present invention is shown in FIG. A plastic scintillator according to an embodiment of the present invention (■
5) has a cylindrical main body (15a) with a light pipe (15b) protruding from the upper surface thereof, which forms a connection part to a photoelectron J-angle multiplier, and the light pipe (15b) is located at the center of the main body (15a). .

上記構成の本発明一実施例のプラスチックシンチレータ
(1■においては、連通穴(Ifi)を穿設したことに
占り、その部分の残留モノマが収り除かれるだけでなく
、連通穴が無い場合には本体(15a)の外面からだけ
しか残留モノ67が揮発できなかったのに対して、連通
穴(IGIへも揮発できるようになり、それだけ短期間
で残留モノマが抜は切るようになる7、同じような形状
寸法のもので、残留モノマが抜は切るための所要期間は
従来のものに比べて1/6以下になる。
The plastic scintillator according to the embodiment of the present invention having the above structure (1) is determined by the fact that a communicating hole (Ifi) is formed, and the residual monomer in that part is not only contained and removed, but also when there is no communicating hole. In contrast to the case where the residual monomer 67 could only be volatilized from the outer surface of the main body (15a), it is now possible to volatilize also to the communication hole (IGI), and the residual monomer can be removed in a short period of time. , the time required to remove the residual monomer is 1/6 or less compared to conventional products with similar shapes and dimensions.

したがって、従来、放射線厚み計の検出器として使用す
るのに製造後約1年もねかぜでおかなければならなかっ
たのが、2ケ月以下で使用できることになり、実用上の
利点が大きい。第5図は、製造後約2ケ月ねかした後の
本発明によるプラスチックシンチレータ(15)を放射
線厚みf?lに用いた場合のプラスチックシンチレータ
θ5)の光出力の立−1−り特性を示すもので、被測定
物が無いときの光出力囚が被測定物が挿入されたB点か
ら急速に但1丁し、被測定物により減衰された放射線の
入射時に相当する光出力に落ち付くことを示しており、
時刻t、からt2までの応答遅れ時間が極めて短かくな
っていて、残留モノマが抜は切っていることがわかる。
Therefore, while conventionally it was necessary to leave the product in a cold environment for about one year after manufacture to use it as a detector of a radiation thickness meter, it can now be used for less than two months, which is a great practical advantage. FIG. 5 shows the radiation thickness f? of the plastic scintillator (15) according to the present invention after being aged for about two months after manufacture. This figure shows the vertical characteristic of the optical output of the plastic scintillator θ5) when used at point 1, where the optical output when there is no object to be measured rapidly increases by 1 from point B where the object to be measured is inserted. However, it shows that the optical output settles down to the level corresponding to when the radiation is attenuated by the object to be measured.
It can be seen that the response delay time from time t to time t2 is extremely short, and the residual monomer is completely removed.

なお、本発明は第4図に示した実施例に限らず、下記の
ように変形して実施することができる。
Note that the present invention is not limited to the embodiment shown in FIG. 4, and can be implemented with modifications as described below.

(a) 形状は円柱に限らず、第6図(、)乃至第6図
(g)に示すように種々な形状でよく、また、ライトパ
イプ(15b)は有っても無くてもよい。さらに、間 寸法の大小も侮わない。
(a) The shape is not limited to a cylinder, but may be various shapes as shown in FIGS. 6(a) to 6(g), and the light pipe (15b) may or may not be included. Furthermore, don't underestimate the size of the space.

(b) 連通穴〇〇は、第4図のような小径の穴複数個
所の代りに、$7図(a)に示すような同等の大径の穴
1個所でもよい。また、連通穴(16)は上下方向に限
らず第7図(b)に示すように水平方向でもよい。
(b) The communicating hole 〇〇 may be a single large-diameter hole as shown in Figure 7 (a) instead of multiple small-diameter holes as shown in Figure 4. Further, the communication hole (16) is not limited to the vertical direction, but may be formed horizontally as shown in FIG. 7(b).

さらに、連フリ穴(1G)は下部からあけても上部から
あけてもよい。また、加より■能ならば貫通していても
よい。
Furthermore, the continuous free holes (1G) may be made from the bottom or the top. Also, if it is more than ka, it may be penetrating.

〔発明の効果〕〔Effect of the invention〕

以上詳述1−だように本発明によれば、プラスチックシ
ンチレータの製造時に発生し内部に含まれる残留モノマ
の揮発を促進するために、プラスチックシンチレータの
内芯部を外部に連通させる連通穴を穿設するようにした
ことにより、その部分の残留モノマが取り除かれるだけ
でなく、連通穴が無い場合にはプラスブ〜ンクシンチレ
ータの外面だけしか揮発できなかったのに対して連通穴
へも揮発可fh2となり、それだけ短期間で残留モノマ
が抜は切るようになる。その結果、同じような形状寸法
のもので残留モノマが抜切るための所要期間が従来のも
のに比べて1/6以下に短縮される。したがって、放射
線厚み計等の検出器として使用できる応答速度が得られ
るまで(=、従来のものでは製造後約1年もねかぜでお
かなければならなかったものが、簡単な追加工により2
り月以下で使用できるようになり、実用上の利点が大き
い。さらに、プラスチックシンチレータ全体としての形
状は変らないので、容器、ホルダ等は従来のまま使用で
きる利点もある。
As described above in detail 1-1, according to the present invention, in order to promote the volatilization of the residual monomer generated during the manufacturing of the plastic scintillator and contained inside, a communication hole is formed to communicate the inner core of the plastic scintillator with the outside. This not only removes the residual monomer from that area, but also allows it to volatilize into the communication hole, whereas in the case where there was no communication hole, the monomer could only volatilize on the outer surface of the positive blank scintillator. Therefore, the residual monomer will be completely removed in a short period of time. As a result, the time required for cutting out residual monomer with similar shapes and dimensions is shortened to 1/6 or less compared to conventional products. Therefore, until a response speed that can be used as a detector such as a radiation thickness meter is obtained (=, conventional products had to be kept in a dry environment for about a year after manufacture, but with simple additional work, it takes about 20 days
It can be used in less than a month, and has great practical advantages. Furthermore, since the shape of the plastic scintillator as a whole does not change, there is an advantage that the container, holder, etc. can be used as is.

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

第1図はプラスチックシンチレータが用いられている放
射線厚みH1測定系を示すブロック医1、第2図は従来
のプラスナックシンチレータの一例を示す斜視図、第3
図は残留モノマが抜は切っていないプラスチックシンチ
レータをm 1図の放射線厚み計に用いた場合のプラス
ブーンクシンチレータの光出力の立上り特性を示すグラ
フ、第4図は本発明一実施例のプラスチックシンチレー
タを示す斜視図、第5図は製造後約2ケ月ねかぜだ後の
第4図のプラスチックシンチレータを第1図の放射線厚
みi+に用いた場合のプラスナックシンチレータの光出
力の立上り特性を示すグラフ、第6図(a)乃至第6図
(glは本発明の実施可能なプラスチックシンチレータ
の月1々な形状を示す斜視図、第7図(a) 、 (b
)はそれぞれ本発明の異なる新形例のプラスチックシン
チレータを示す窄1視図である。 15・・・プラスチックシンチレータ 15a・木 休 15b〜・・ライトパイプ16 ・・
・ノ21巳i、nr 穴 代理入 ヨf「埋土 井 上 −男 第 1 図 第2図 第3図 第 4 図 第 5 図 (OL) (i CC> (d) 第 7 図
Fig. 1 is a block doctor 1 showing a radiation thickness H1 measuring system using a plastic scintillator, Fig. 2 is a perspective view showing an example of a conventional plastic scintillator, and Fig. 3 is a perspective view showing an example of a conventional plastic scintillator.
Figure 4 is a graph showing the rise characteristics of the optical output of the Plus Boonck scintillator when a plastic scintillator with no residual monomer removed is used in the radiation thickness meter shown in Figure 1. A perspective view showing a scintillator, and Fig. 5 shows the rise characteristics of the optical output of the plastic scintillator when the plastic scintillator of Fig. 4 is used with the radiation thickness i+ of Fig. 1 after being heated for about two months after manufacture. Graphs, FIGS. 6(a) to 6(gl are perspective views showing different shapes of plastic scintillators that can be implemented according to the present invention, FIGS. 7(a) and (b)
) are close-up views showing different new types of plastic scintillators of the present invention. 15...Plastic scintillator 15a/Thu closed 15b~...Light pipe 16...
・ノ21巳i,nr Hole substitution Yof ``Filled soil Inoue - Male 1st Figure 2 Figure 3 Figure 4 Figure 5 (OL) (i CC> (d) Figure 7

Claims (1)

【特許請求の範囲】[Claims] 所望の形状をしたブロックに形成され放射線の入射によ
り光を発するプラスチックシンチレータにおいて、その
内芯部に、外気に連通ずる少なくとも1個の連通穴が穿
設されたことを特徴とするプラスチックシンチレータ。
A plastic scintillator that is formed into a block having a desired shape and emits light upon incidence of radiation, characterized in that the inner core of the plastic scintillator is provided with at least one communication hole that communicates with the outside air.
JP14058083A 1983-08-02 1983-08-02 Plastic scintillator Granted JPS6033075A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14058083A JPS6033075A (en) 1983-08-02 1983-08-02 Plastic scintillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14058083A JPS6033075A (en) 1983-08-02 1983-08-02 Plastic scintillator

Publications (2)

Publication Number Publication Date
JPS6033075A true JPS6033075A (en) 1985-02-20
JPH0472872B2 JPH0472872B2 (en) 1992-11-19

Family

ID=15271994

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14058083A Granted JPS6033075A (en) 1983-08-02 1983-08-02 Plastic scintillator

Country Status (1)

Country Link
JP (1) JPS6033075A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5571967A (en) * 1978-11-25 1980-05-30 Mitsubishi Electric Corp Radiation measuring instrument

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5571967A (en) * 1978-11-25 1980-05-30 Mitsubishi Electric Corp Radiation measuring instrument

Also Published As

Publication number Publication date
JPH0472872B2 (en) 1992-11-19

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