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JPH0565116B2 - - Google Patents
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JPH0565116B2 - - Google Patents

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Publication number
JPH0565116B2
JPH0565116B2 JP26196787A JP26196787A JPH0565116B2 JP H0565116 B2 JPH0565116 B2 JP H0565116B2 JP 26196787 A JP26196787 A JP 26196787A JP 26196787 A JP26196787 A JP 26196787A JP H0565116 B2 JPH0565116 B2 JP H0565116B2
Authority
JP
Japan
Prior art keywords
dose
radiation
rubber
amino acid
dosimeter
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
Application number
JP26196787A
Other languages
Japanese (ja)
Other versions
JPH01102388A (en
Inventor
Takuji Kojima
Yosuke Morita
Ryuichi Tanaka
Tadao Seguchi
Shigeru Kashiwazaki
Hideki Yagyu
Shigeki Matsuyama
Jiro Ogura
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.)
Hitachi Cable Ltd
Japan Atomic Energy Agency
Original Assignee
Hitachi Cable Ltd
Japan Atomic Energy Research Institute
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 Hitachi Cable Ltd, Japan Atomic Energy Research Institute filed Critical Hitachi Cable Ltd
Priority to JP26196787A priority Critical patent/JPH01102388A/en
Publication of JPH01102388A publication Critical patent/JPH01102388A/en
Publication of JPH0565116B2 publication Critical patent/JPH0565116B2/ja
Granted legal-status Critical Current

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  • Measurement Of Radiation (AREA)
  • Manufacture Of Macromolecular Shaped Articles (AREA)
  • Compositions Of Macromolecular Compounds (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、γ線、X線、電子線、重荷電粒子線
および中性子線などの電離性放射線による吸収線
量を正確に、かつ簡便に測定するための薄膜放射
線線量計素子に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention is a method for accurately and easily measuring the absorbed dose due to ionizing radiation such as gamma rays, X-rays, electron beams, heavily charged particle beams, and neutron beams. The present invention relates to a thin film radiation dosimeter element for use in radiation dosimetry.

[従来の技術] 近年、原子力発電所、放射性廃棄物処理施設な
どの放射性物質を取扱う大型施設や粒子線、γ線
などの各種の照射利用施設等が普及してきた。こ
れらの施設では、通常の環境下はもちろん、高温
度や高湿度といつたような環境下で広い線量範囲
にわたつて正確かつ簡便に放射線の線量を評価す
ることが求められている。
[Background Art] In recent years, large-scale facilities that handle radioactive materials, such as nuclear power plants and radioactive waste treatment facilities, and facilities that utilize various types of irradiation, such as particle beams and gamma rays, have become widespread. These facilities are required to accurately and easily evaluate radiation doses over a wide dose range, not only under normal environments but also under environments such as high temperature and high humidity.

従来の10Gyから100kGyの中、高レベルの線量
測定を目的とした固体の放射線量計としては、熱
ルミネツセンス線量計、ライオルミネツセンス線
量計、ポリメチルメタクリレート線量計、ラジア
クロミツクダイフイルム線量計、コバルトガラス
線量計等が知られている。これらはいずれも放射
線を固体素子に照射後、固体素子から発光量や特
定波長の光の吸収を測定して、線量を求めるもの
であるが、線量応答のばらつきが大きい、線量応
答の経時変化が大きい、有効線量測定範囲が狭
い、といつた問題を有している。
Conventional solid-state radiation dosimeters aimed at high-level dose measurements between 10Gy and 100kGy include thermoluminescence dosimeters, liyoluminescence dosimeters, polymethyl methacrylate dosimeters, and radial chromic di-film dosimeters. , cobalt glass dosimeters, etc. are known. In both of these methods, the dose is determined by irradiating a solid-state element with radiation and then measuring the amount of light emitted from the solid-state element and the absorption of light at a specific wavelength. It has problems such as large size and narrow effective dose measurement range.

アミノ酸の一種であるアラニンは、結晶状態で
放射線を照射すると、その線量に比例して安定な
固有のラジカル(遊離基)を生じるため、単位重
量あたりの生成ラジカル濃度を電子スピン共鳴
(ESR)装置で求めることにより線量を測定する
ことが可能である。この方法によれば、10Gyか
ら100kGyの広範囲の線量を測定でき、しかもラ
ジカル数の変化(減衰)は2年間で約2%と極め
て少ないことから、線量応答の経時変化は上記の
線量計に比べケタ違いに少ない。
When alanine, a type of amino acid, is irradiated with radiation in a crystalline state, it generates unique radicals (free radicals) that are stable in proportion to the dose, so the concentration of generated radicals per unit weight can be measured using an electron spin resonance (ESR) device It is possible to measure the dose by calculating According to this method, it is possible to measure a wide range of doses from 10 Gy to 100 kGy, and the change (attenuation) in the number of radicals is extremely small at about 2% over two years, so the change in dose response over time is smaller than that of the above dosimeters. There are far fewer.

しかし、アラニン粉末そのものは、水に可溶で
あるため水中あるいは空気中で水や湿度の影響を
受ける。また、粉末が微細ですぐに静電気を帯び
るため、正確な秤量や容器への充填も困難であ
り、取扱いに極めて不便である。このため、ポリ
マをバインダとしてアラニン粉末を成形加工した
実用的な線量計素子が提案されている(小島、他
3名;第46回応物講演会予稿集(1985.秋)、小
島、他3名;放射線プロセスシンポジウム講演要
旨集P9(1985.11.18))。
However, since alanine powder itself is soluble in water, it is affected by water and humidity in water or in the air. Furthermore, since the powder is fine and easily charged with static electricity, it is difficult to accurately weigh it and fill it into a container, making it extremely inconvenient to handle. For this reason, a practical dosimeter element has been proposed in which alanine powder is molded using a polymer as a binder (Kojima and 3 others; Proceedings of the 46th Applied Physics Conference (Autumn 1985), Kojima and 3 others). ; Radiation Process Symposium Abstracts P9 (1985.11.18)).

かかる線量計素子は、5mmφ(外径)×10mm(長
さ)、3mmφ(外径)×30mm(長さ)といつた円筒
形状のものである。
The dosimeter element has a cylindrical shape with dimensions of 5 mmφ (outer diameter) x 10 mm (length) and 3 mmφ (outer diameter) x 30 mm (length).

[発明が解決しようとする問題点] しかし、低エネルギーの放射線あるいは透過力
の弱い放射線種の線量測定においては、物質中の
深さによつて線量が異なるため、厚さのある円筒
形状の線量計素子を用いると、放射線の飛程以上
の厚さに対する線量の平均値しか測定できず、正
確な線量評価ができないことが指摘されるに至つ
た。また、パイプ接続部のパツキン等のように狭
小部分に置かれた部品の線量は測定できないとい
う状況にある。
[Problems to be solved by the invention] However, when measuring the dose of low-energy radiation or radiation species with weak penetrating power, the dose differs depending on the depth in the material, so the dose of a thick cylindrical shape is It has been pointed out that when measuring elements are used, only the average value of the dose can be measured for a thickness greater than the range of the radiation, making accurate dose evaluation impossible. Furthermore, it is not possible to measure the dose of parts placed in narrow areas, such as gaskets at pipe connections.

本発明は上記に基づいてなされたものであり、
物質中の深さによつて線量が異なつても、その違
いを誤差少なく明確に評価できることから線量測
定値の信頼性が向上され、また狭小部分での線量
測定を可能とする薄膜放射線線量計素子の提供を
目的とするものである。
The present invention has been made based on the above,
Even if the dose differs depending on the depth in the material, the reliability of the dose measurement value is improved because the difference can be clearly evaluated with less error, and the thin film radiation dosimeter element also makes it possible to measure the dose in narrow areas. The purpose is to provide the following.

[問題点を解決するための手段] 本発明の放射線量計素子は、バインダにアミノ
酸結晶粉末を含有せしめてなる組成物を厚さ1mm
以下線のシートまたはフイルム状の薄膜に成形し
てなることを特徴とするものである。
[Means for Solving the Problems] The radiation dosimeter element of the present invention has a composition in which a binder contains amino acid crystal powder, and a composition having a thickness of 1 mm.
It is characterized by being formed into a sheet or film-like thin film as shown below.

バインダとしては、天然ゴム、合成ゴムあるい
は合成樹脂があげられ、特に、放射線によるラジ
カル生産量が少ないもの、あるいは生成ラジカル
が急速に減衰するものが好ましい。
As the binder, natural rubber, synthetic rubber, or synthetic resin can be used, and it is particularly preferable to use a binder that produces a small amount of radicals due to radiation, or a binder that rapidly attenuates the generated radicals.

合成ゴムとしては、エチレンプロピレン(−ジ
エン)共重合体、エチレン−酢酸ビニル共重合
体、クロロプレンゴム、ニトリルゴム、ブチルゴ
ム、合成イソプレンゴム、スチレンブタジエン共
重合体、スチレン−ブタジエン−アクリロニトリ
ル共重合体、ブタジエンゴム、アクリルゴム、ウ
レタンゴム、シリコーンゴム、クロロスルホン化
ポリエチレン、ポリイソブチレン、ポリエステル
ゴム、エピクロルヒドリンゴム、四ふつ化エチレ
ン−プロピレン交互共重合体などがあげられる。
Examples of synthetic rubber include ethylene propylene (-diene) copolymer, ethylene-vinyl acetate copolymer, chloroprene rubber, nitrile rubber, butyl rubber, synthetic isoprene rubber, styrene-butadiene copolymer, styrene-butadiene-acrylonitrile copolymer, Examples include butadiene rubber, acrylic rubber, urethane rubber, silicone rubber, chlorosulfonated polyethylene, polyisobutylene, polyester rubber, epichlorohydrin rubber, tetrafluoroethylene-propylene alternating copolymer, and the like.

合成樹脂としては、パラフイン、ポリスチレ
ン、アクリロニトリル−スチレン樹脂、硬質アク
リロニトリル−ブタジエン−スチレン樹脂、ポリ
ウチレンテレフタレート樹脂、ポリエチレンテレ
フタレート樹脂、ポリアーボネート樹脂、ポリエ
チレン、ポリプロピレン、ポリエステル樹脂、ナ
イロン12などがあげられる。
Examples of synthetic resins include paraffin, polystyrene, acrylonitrile-styrene resin, hard acrylonitrile-butadiene-styrene resin, polyethylene terephthalate resin, polyethylene terephthalate resin, polyarbonate resin, polyethylene, polypropylene, polyester resin, and nylon 12. .

アミノ酸結晶粉末としては、モノアミノモノカ
ルボン酸であるグリシン、バリン、ロイシン、オ
キシアミノ酸であるセリン、イオウを含むアミノ
酸であるシステイン、シスチン、モノアミノジカ
ルボン酸であるリシン、アルギニン、芳香族環を
もつアミノ環であるフエニルアラニン、アントラ
ニル酸などの比較的低分子量で結晶性の高いもの
が有効である。
Amino acid crystal powder includes monoamino monocarboxylic acids glycine, valine, and leucine, oxyamino acids serine, sulfur-containing amino acids cysteine and cystine, monoamino dicarboxylic acids lysine, arginine, and aromatic ring-containing amino acids. Those with relatively low molecular weight and high crystallinity, such as amino ring phenylalanine and anthranilic acid, are effective.

バインダとアミノ酸結晶粉末との配合割合は特
に規定しないが、上限は、形成加工性および成形
体を扱うに際して実用的な機械的特性を保持して
いるか否かにより、下限は、線量計素子として有
効なアミノ酸量を含んでいるか否かにより定めら
れ、バイダ100重量部に体してアミノ酸結晶粉末
10〜1000重量部、好ましくは100〜600重量部の範
囲から選定するのが適切である。
The blending ratio of the binder and the amino acid crystal powder is not particularly specified, but the upper limit depends on the forming processability and whether practical mechanical properties are maintained when handling the molded product, and the lower limit is the value that is effective as a dosimeter element. Amino acid crystal powder containing 100 parts by weight of Vyda
It is appropriate to select from the range of 10 to 1000 parts by weight, preferably 100 to 600 parts by weight.

本発明においては、上記成分以外に酸化防止
剤、滑剤を適宜含有させてもよい。酸化防止剤、
滑剤の添加により、混練、成形時なプレドーズ
(照射前に素子中に存在するラジカル)が増加す
るのを抑制でき、測定制度を向上できる。
In the present invention, an antioxidant and a lubricant may be appropriately contained in addition to the above-mentioned components. Antioxidant,
Addition of a lubricant can suppress an increase in predose (radicals present in the element before irradiation) during kneading and molding, and can improve measurement accuracy.

[発明の実施例] ポリエチレン(宇部興産(株)製、UBEC−400)
400gおよびDL−α−アラニン(和光純薬(株)製、
特級)600gを140℃の6インチテストロールで混
練し、次いでプレス成形により厚さ1.0mmおよび
0.3mmのフイルム状線量計素子(5mm×30mm)を
製造した。
[Embodiments of the invention] Polyethylene (manufactured by Ube Industries, Ltd., UBEC-400)
400g and DL-α-alanine (manufactured by Wako Pure Chemical Industries, Ltd.)
600g of special grade) was kneaded with a 6-inch test roll at 140℃, and then press-molded into 1.0mm thick and
A 0.3 mm film dosimeter element (5 mm x 30 mm) was manufactured.

電子線加速器を用い、上記の各線量計素子数枚
を重ねてエネルギーの異なる電子線(0.5MeV、
1.0MeV、1.5MeV、2.0MeV)により104Gy相当
の線量を照射した(照射条件は予めカロリメータ
により調整)。照射したせ量計素子の吸収線量は
ESRを用いて測定した。
Using an electron beam accelerator, several of the above dosimeter elements are stacked to generate electron beams with different energies (0.5 MeV,
1.0MeV, 1.5MeV, 2.0MeV) at a dose equivalent to 10 4 Gy (irradiation conditions were adjusted in advance using a calorimeter). The absorbed dose of the irradiated dosimeter element is
Measured using ESR.

第1図に各エネルギーの場合の物質中の厚さに
体する線量分布(計算値)を示す。第2図および
第3図に1.0MeVの電子線を使用した場合につい
て、厚さ1.0mmおよび0.3mmの本線量計素子を用い
て測定した結果を一例として示す。厚さ1.0mm
(1.6g/cm2)の素子では3段階の分解能である
が、0.3mm素子用いれば9段階の分解能で分布測
定が可能である。外径3mmφのロツド状素子を用
いた場合などは、このような分解能が期待でき
ず、図のような分布の平均値もしくは放射線の飛
程以上の厚さについての平均値しか測定できな
い。
Figure 1 shows the dose distribution (calculated values) to the thickness of the material for each energy. Figures 2 and 3 show, as an example, the results of measurements using the present dosimeter elements with thicknesses of 1.0 mm and 0.3 mm when using a 1.0 MeV electron beam. Thickness 1.0mm
(1.6 g/cm 2 ) element has three levels of resolution, but if a 0.3 mm element is used, distribution measurement can be performed with nine levels of resolution. When a rod-shaped element with an outer diameter of 3 mmφ is used, such resolution cannot be expected, and only the average value of the distribution as shown in the figure or the average value of the thickness beyond the range of the radiation can be measured.

このことこら、厚さの薄い素子ほど、精密に物
質中の深さ方向の線量分布が測定でき、正確な線
量評価が可能となることが明らかである。
From this point of view, it is clear that the thinner the element, the more precisely the dose distribution in the depth direction in the substance can be measured, and the more accurate the dose evaluation becomes.

また、本発明のようにシートまたはフイルム状
の薄い線量計素子であれば、例えば、スチレンス
パイプの接続部分のような狭い場所にも取付ける
ことができ、γ線にさらされる接続部分に用いら
れるゴムパツキンの線量測定も可能となる。
Furthermore, if the dosimeter element is thin in the form of a sheet or film as in the present invention, it can be installed in a narrow place, such as a connection part of a styrene pipe, and it can be used in a connection part exposed to gamma rays. It also becomes possible to measure the dose of rubber gaskets.

[発明の効果] 以上説明してきた通り、本発明によれば物質深
さによつて異なる線量評価の誤差を減少できるこ
とから信頼性を向上でき、また、狭小な場所での
線量測定を行なうことが可能となる。
[Effects of the Invention] As explained above, according to the present invention, reliability can be improved because errors in dose evaluation that vary depending on material depth can be reduced, and dose measurement can be performed in a narrow place. It becomes possible.

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

第1図は線量分布曲線の計算値のグラフ、第2
図は厚さ1mm素子で測定した線量分布を示すグラ
フ、第3図は厚さ0.3mm素子で測定した線量分布
を示すグラフである。
Figure 1 is a graph of calculated values of the dose distribution curve, Figure 2 is a graph of calculated values of the dose distribution curve.
The figure is a graph showing the dose distribution measured with a 1 mm thick element, and Figure 3 is a graph showing the dose distribution measured with a 0.3 mm thick element.

Claims (1)

【特許請求の範囲】 1 バインダにアミノ酸結晶粉末を含有せしめて
なる組成物を厚さ1mm以下のシートまたはフイル
ム状に成形してなることを特徴とする薄膜放射線
線量計素子。 2 アミノ酸がアラニンである特許請求の範囲第
1項記載の薄膜放射線線量計素子。
[Scope of Claims] 1. A thin film radiation dosimeter element, characterized in that it is formed by forming a composition in which a binder contains amino acid crystal powder into a sheet or film having a thickness of 1 mm or less. 2. The thin film radiation dosimeter element according to claim 1, wherein the amino acid is alanine.
JP26196787A 1987-10-16 1987-10-16 Thin film radiation dosimeter element Granted JPH01102388A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26196787A JPH01102388A (en) 1987-10-16 1987-10-16 Thin film radiation dosimeter element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26196787A JPH01102388A (en) 1987-10-16 1987-10-16 Thin film radiation dosimeter element

Publications (2)

Publication Number Publication Date
JPH01102388A JPH01102388A (en) 1989-04-20
JPH0565116B2 true JPH0565116B2 (en) 1993-09-17

Family

ID=17369144

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26196787A Granted JPH01102388A (en) 1987-10-16 1987-10-16 Thin film radiation dosimeter element

Country Status (1)

Country Link
JP (1) JPH01102388A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03197534A (en) * 1989-12-26 1991-08-28 Ain Kk Aggregate for molding resin
US6892948B2 (en) 2001-11-27 2005-05-17 Eastman Kodak Company Method of measuring dose of local radiation
US6787107B2 (en) 2001-11-27 2004-09-07 Eastman Kodak Company Element with coated dosimeter

Also Published As

Publication number Publication date
JPH01102388A (en) 1989-04-20

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