JPS63221278A - Irradiation dose detector - Google Patents
Irradiation dose detectorInfo
- Publication number
- JPS63221278A JPS63221278A JP5404587A JP5404587A JPS63221278A JP S63221278 A JPS63221278 A JP S63221278A JP 5404587 A JP5404587 A JP 5404587A JP 5404587 A JP5404587 A JP 5404587A JP S63221278 A JPS63221278 A JP S63221278A
- Authority
- JP
- Japan
- Prior art keywords
- irradiation
- dose
- irradiation dose
- radiation
- irradiated
- 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.)
- Pending
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/02—Dosimeters
- G01T1/04—Chemical dosimeters
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)
- Measurement Of Radiation (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は電離放線照射線量感応検知器に係り、特に、γ
線照射物の照射線量制御用センサに好適な照射線量検知
器に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to an ionizing radiation radiation dose-sensitive detector, and in particular,
The present invention relates to an irradiation dose detector suitable for use as a sensor for controlling irradiation dose of a radiation irradiated object.
従来、γ線照射装置で照射する場合は、あらかじめ照射
場の線量率を測定しておいて、あとは時間によって反応
に必要な線量率を推定していた。Conventionally, when irradiating with a gamma ray irradiation device, the dose rate of the irradiation field was measured in advance, and then the dose rate required for the reaction was estimated based on the time.
この場合、測定に用いた線量計は、例えば、放射線化学
関連の文献に記載されている(放射線化学(70ナ社、
昭55年)P76〜93)ような化学線量計が一般的で
ある。最も普及した測定方法は、フリツケ線量計と言わ
れる二価の鉄イオン(Fe”+)が水溶液中で水の放射
線分解で生成した過酸化水素(H2,□ Z )によっ
て酸化を受は二価の鉄イオン(Fe3+)になる。この
ときFez+→Fe3+になる割合は吸収線量に比例す
るので、吸収線量を照射時間の商で表わせば線量率が求
まる。In this case, the dosimeter used for measurement is described in, for example, radiation chemistry-related literature (Radiation Chemistry (70Nasha,
Chemical dosimeters such as P76-93) (1980) are common. The most popular measurement method is the Fritzke dosimeter, in which divalent iron ions (Fe"+) are oxidized by hydrogen peroxide (H2, □ Z ) produced by radiolysis of water in an aqueous solution. becomes iron ion (Fe3+).At this time, the ratio of Fez+→Fe3+ is proportional to the absorbed dose, so the dose rate can be found by expressing the absorbed dose as the quotient of the irradiation time.
この他、固体線量計ではガラス線量計が知られている。In addition, glass dosimeters are known as solid-state dosimeters.
これらの線量計で測定できる線量の範囲は10”〜10
’G:yの範囲である。The dose range that can be measured with these dosimeters is 10” to 10
'G: y range.
これに対して、照射に必要な線量は、物質及び用途によ
って異るが、高分子材の重合反応には103〜3−0’
G y、食品、医療具等の殺菌や滅菌には同じく108
〜10’G yが必要とされている。On the other hand, the dose required for irradiation varies depending on the substance and application, but for polymerization reactions of polymeric materials, the dose required for irradiation is 103 to 3-0'.
108 for sterilization and sterilization of Gy, food, medical equipment, etc.
~10'Gy is required.
この線量計で照射場の線量率を正確に測定しておけば、
必要な照射線量は、照射時間を制御することによって得
ることができる。If you accurately measure the dose rate of the irradiation field with this dosimeter,
The required irradiation dose can be obtained by controlling the irradiation time.
しかし、上記従来の照射方法では線源の強さが不変で、
かつ、被照射物が点状で内部吸収を無視できることが前
提である。線源の強さが変化したときは、その都度、こ
の方法で照射場の線量率を測定する必要がある。この化
学的線量計測法は、信頼性の高い計測法であるが、溶液
を取扱うため、化学分析の基礎的技術を必要とし、一般
の利用者にとっては手軽な汎用法とは言い難い。また、
試料溶液も一定量以上を必要とし、飛散等の恐れもあっ
て取扱い性が良いとは言えず、被照射物と同時に照射し
ようとしたときには不便である。さらに、最大の問題は
測定結果を照射中に積算線量を知ることが難しいことに
ある。However, in the conventional irradiation method described above, the strength of the radiation source remains unchanged,
It is also assumed that the object to be irradiated is point-like and that internal absorption can be ignored. Whenever the intensity of the radiation source changes, it is necessary to measure the dose rate of the irradiation field using this method. This chemical dosimetry method is a highly reliable measurement method, but since it deals with solutions, it requires basic chemical analysis techniques, and it cannot be said to be an easy and versatile method for general users. Also,
The sample solution also requires a certain amount or more, and there is a risk of scattering, so it cannot be said that it is easy to handle, and it is inconvenient when trying to irradiate the object at the same time. Furthermore, the biggest problem is that it is difficult to know the cumulative dose while irradiating the measurement results.
本発明の目的は照射線量に係る計測情報をその場で電気
信号として取り出し、この信号に基づいて照射完了後の
被照射物の移送や線源格納などの操作を迅速に行い照射
制御の精度を高め自動化を可能にする簡便なセンサ材を
提供することにある。The purpose of the present invention is to extract measurement information related to irradiation dose as an electrical signal on the spot, and based on this signal, quickly perform operations such as transferring the irradiated object and storing the source after irradiation is completed, thereby improving the accuracy of irradiation control. The objective is to provide a simple sensor material that enables high automation.
上記目的を達成するために注目したのが導電性高分子材
を放射線重合反応によって製造し、一定線量を照射して
重合反応が完了した時に導電信号を得て、照射の完了又
は完了後の操作表示を行う。In order to achieve the above objective, we focused on manufacturing conductive polymer materials by radiation polymerization reaction, irradiating a certain amount of radiation, obtaining a conductive signal when the polymerization reaction is completed, and performing operations after the irradiation is completed or after completion. Perform display.
電導性高分子材は、アセチレン(CHCH)の重合体ポ
リアセチレン(P、A)、又は、ジアセチレン(R−C
C−CC−R’)の重合体ポリジアセチレン(PDA)
が知られている。(化学の領域、35巻3号(1980
年)記載)このうちPDAは同相の状態で重合反応する
ため、固体粉末を塗布しておくだけで熱や光、又は、放
射線によって重合する。γ線によって重合するPDAは
pTs(置換基:パラトルコンスルホネイト・−CHy
、−〇−802−CaHa−CHa)や3BCMU(置
換基:ブトキシ・カルボニル・メチルウレタン:
(CHz)s−OCO−NH−CHz−COO(CHz
)a−CHa)が知られている。これらの固相重合高分
子結晶の電導度は製造条件によって異なるが、単体では
絶縁体(10−”S/cm以下)であるものが、重合後
には10−’S/a!1からl5Z1の導電率を示すに
至る。従って、電極間にジアセチレンの単分子粉末を層
状に置き、これに104Gyから10δay のγ線
を照射すると重合反応が進行して導電率を測定すればそ
の立ち上がり曲線を計測することができる。すなわち、
照射線量と重合反応率の関係をあらかじめ求めておけば
、一定の照射線量に至ったことを検知し、電気信号に変
換することができる。これをセンサ化しておけば、多点
を測定してa量率分布を求めたり、信号を用いて照射装
置の制御に応用できるなどの利点がある。The conductive polymer material is a polymer of acetylene (CHCH), polyacetylene (P, A), or diacetylene (R-C
C-CC-R') polymer polydiacetylene (PDA)
It has been known. (Region of Chemistry, Vol. 35, No. 3 (1980)
(2013) Description) Of these, PDA polymerizes in the same phase, so it can be polymerized by heat, light, or radiation just by applying a solid powder. PDA that is polymerized by γ-rays is pTs (substituent: paratorconesulfonate・-CHy
, -0-802-CaHa-CHa) and 3BCMU (substituent: butoxy carbonyl methylurethane:
(CHz)s-OCO-NH-CHz-COO(CHz
)a-CHa) is known. The conductivity of these solid phase polymerized polymer crystals varies depending on the manufacturing conditions, but when used alone they are insulators (10-'S/cm or less), but after polymerization they range from 10-'S/a!1 to 15Z1. Therefore, when monomolecular powder of diacetylene is placed in a layer between the electrodes and γ-rays of 104 Gy to 10 δay are irradiated, the polymerization reaction proceeds and the rise curve can be seen by measuring the conductivity. can be measured, i.e.
If the relationship between the irradiation dose and the polymerization reaction rate is determined in advance, it is possible to detect when a certain irradiation dose has been reached and convert it into an electrical signal. If this is made into a sensor, there are advantages such as being able to measure multiple points to obtain the a mass rate distribution, and applying the signal to control the irradiation device.
以下、本発明の一実施例を第1図、第2図及び第3図に
より説明する。第1図はジアセチレン単分子の粉末1を
一対の電極2の間に挟み、両端は絶縁材3で支持された
状態を示す。これにコバルト(6°Co)のようにγ線
線源5から、例えば、PTSの場合は室温で6X10’
Gy の放射線量を照射すると、ジアセチレン単体の粉
末は重合反応を起こし高分子結晶6になる。その状態を
第2図に示す。従って、この照射の間、電流計4で監視
を続ければ、反応の完了点、すなわち、照射線量がわか
る。An embodiment of the present invention will be described below with reference to FIGS. 1, 2, and 3. FIG. 1 shows a state in which a monomolecular diacetylene powder 1 is sandwiched between a pair of electrodes 2, and both ends are supported by an insulating material 3. In addition, from the gamma ray source 5 such as cobalt (6°Co), for example, in the case of PTS, 6X10' at room temperature.
When irradiated with a radiation dose of Gy, the powder of diacetylene alone undergoes a polymerization reaction and becomes a polymer crystal 6. The state is shown in FIG. Therefore, if monitoring is continued with the ammeter 4 during this irradiation, the completion point of the reaction, that is, the irradiation dose can be determined.
重合反応はγ線のみならず紫外線や熱によっても進行す
るので照射前の品質管理は計画的にする必要がある。し
かし、この性質を逆に利用してあらかじめ熱や光照射処
理を行って重合反応を進行させておけば、少ないγ線照
射量で重合反応を完了させることができる。これらの前
処理で感度調整済みのジアセチレン粉末を用いて任意の
線量とこれに対応した電気信号を得ることができる。Since the polymerization reaction proceeds not only with gamma rays but also with ultraviolet rays and heat, quality control before irradiation must be planned. However, if this property is used to advance the polymerization reaction by applying heat or light irradiation in advance, the polymerization reaction can be completed with a small amount of γ-ray irradiation. By using diacetylene powder whose sensitivity has been adjusted through these pretreatments, it is possible to obtain any dose and the corresponding electrical signal.
次に、第2図に示した照射線量検知器を装置に適用した
実施例以下第3図に従って説明する。第3図は重合や架
橋反応を行う高分子材料や殺菌や滅菌を目的とした医療
器具や食品などを箱や籠に納めて順次バッチ方式で照射
する例を示す。箱に被照射物を納め、この内部に上記の
ジアセチレン粉末を電極間に挾んだ照射線量検知器11
を挿入しておく。前照射物12をクレーン16で中央の
照射場へ移動する。被照射物13を所定の場所に設置し
、例えば、80Coからなる線源15から発生するγ線
に曝露する。本例では、6 X 10’G yの照射線
量を受けたときジアセチレン粉末の固相重合が完了する
。導電性を滞びると、両極間に一定レベル以上の電流が
流れるので、これを検知回路17で検知し、制御及び表
示器19で信号処理を行い、クレーン駆動装置18を作
動させる。これによって被照射物13はクレーンによっ
て生体遮へい壁20の外側に照射済み体14として移送
される。本実施例はクレーンによって移送するバッチ方
式であるが、移送手段はベルトコンベアでもよい。また
、照射後の操作は、照射物の移動ばかりでなく線源を貯
蔵孔に自動格納することも含める。Next, an example in which the irradiation dose detector shown in FIG. 2 is applied to an apparatus will be described with reference to FIG. 3. Figure 3 shows an example in which polymeric materials that undergo polymerization and crosslinking reactions, medical instruments and foods for sterilization and sterilization are placed in boxes or baskets, and irradiated sequentially in a batch manner. The object to be irradiated is placed in a box, and the irradiation dose detector 11 has the above-mentioned diacetylene powder sandwiched between electrodes inside the box.
Insert. The pre-irradiation object 12 is moved to the central irradiation field by a crane 16. An irradiated object 13 is placed at a predetermined location and exposed to gamma rays generated from a radiation source 15 made of, for example, 80Co. In this example, the solid state polymerization of the diacetylene powder is completed upon receiving an irradiation dose of 6 X 10'G y. When conductivity is interrupted, a current of a certain level or higher flows between the two electrodes, so this is detected by the detection circuit 17, signal processing is performed by the control and display unit 19, and the crane driving device 18 is operated. As a result, the irradiated object 13 is transferred by the crane to the outside of the biological shielding wall 20 as an irradiated object 14. Although this embodiment uses a batch method in which the materials are transferred by a crane, the transfer means may also be a belt conveyor. Further, operations after irradiation include not only moving the irradiation object but also automatically storing the radiation source in the storage hole.
照射物の移送操作を連続方式にするときは、クレーン、
又は、ベルトコンベアの速度制御をするため、所定の線
量が得られる時間を測定しつつ最適化演算を行う。When transferring the irradiated object in a continuous manner, use a crane,
Alternatively, in order to control the speed of the belt conveyor, optimization calculations are performed while measuring the time required to obtain a predetermined dose.
なお、ポリジアセチレン材料(N換基の種類)を変えた
り、熱処理や紫外線や紫外線照射による前処理を行うこ
とによって重合に必要な線量を調節しておけば線量分布
、線量率の測定も可能である。Note that it is also possible to measure the dose distribution and dose rate by adjusting the dose required for polymerization by changing the polydiacetylene material (type of N substituent), heat treatment, or pretreatment with ultraviolet light or ultraviolet irradiation. be.
本発明によれば、照射線量検出器を被照射物の箱の片隅
に納まる程度に小型化でき、これを被照射物中に埋め込
むことにより、形状が同じで内容物の異なる被照射物内
部での吸収に影響されることなく、実際の照射量を電気
的に検知でき、しかも、照射と同時に線量に係わる情報
が得られるので照射装置の自動化も容易になる。According to the present invention, the irradiation dose detector can be miniaturized to the extent that it fits in one corner of the box of the irradiated object, and by embedding it in the irradiated object, it can be used inside the irradiated object with the same shape but different contents. The actual irradiation dose can be electrically detected without being affected by the absorption of radiation, and information related to the dose can be obtained at the same time as the irradiation, making it easier to automate the irradiation equipment.
Claims (1)
を一対の電極間に層状に付着、あるいは、充填配置した
構造からなり、所定量照射を受けて重合し、導電性高分
子結晶を形成したとき前記電極間に規定値以上の導電性
を得て照射線量を検知することを特徴とする照射線量検
知器。1. Consists of a structure in which a monomolecular compound that solid-phase polymerizes when irradiated with ionizing radiation is attached or packed in a layer between a pair of electrodes, and polymerizes when exposed to a predetermined amount of irradiation to form a conductive polymer crystal. An irradiation dose detector characterized in that when the irradiation dose is detected, the irradiation dose is detected by obtaining conductivity between the electrodes that exceeds a specified value.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5404587A JPS63221278A (en) | 1987-03-11 | 1987-03-11 | Irradiation dose detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5404587A JPS63221278A (en) | 1987-03-11 | 1987-03-11 | Irradiation dose detector |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS63221278A true JPS63221278A (en) | 1988-09-14 |
Family
ID=12959630
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5404587A Pending JPS63221278A (en) | 1987-03-11 | 1987-03-11 | Irradiation dose detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS63221278A (en) |
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2002009775A3 (en) * | 2000-08-02 | 2002-05-30 | Sicel Technologies Inc | Evaluation of irradiated foods or other items with telemetric dosimeters and associated methods |
| US7491942B2 (en) | 2001-11-30 | 2009-02-17 | Sicel Technologies, Inc. | Single-use internal dosimeters for detecting radiation in fluoroscopy and other medical procedures/therapies |
| WO2011044221A3 (en) * | 2009-10-06 | 2012-04-26 | Massachusetts Institute Of Technology | Method and apparatus for determining radiation |
| US8456073B2 (en) | 2009-05-29 | 2013-06-04 | Massachusetts Institute Of Technology | Field emission devices including nanotubes or other nanoscale articles |
| US8476510B2 (en) | 2010-11-03 | 2013-07-02 | Massachusetts Institute Of Technology | Compositions comprising and methods for forming functionalized carbon-based nanostructures |
| US8735313B2 (en) | 2008-12-12 | 2014-05-27 | Massachusetts Institute Of Technology | High charge density structures, including carbon-based nanostructures and applications thereof |
| US8951473B2 (en) | 2008-03-04 | 2015-02-10 | Massachusetts Institute Of Technology | Devices and methods for determination of species including chemical warfare agents |
| US11505467B2 (en) | 2017-11-06 | 2022-11-22 | Massachusetts Institute Of Technology | High functionalization density graphene |
-
1987
- 1987-03-11 JP JP5404587A patent/JPS63221278A/en active Pending
Cited By (16)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6717154B2 (en) | 2000-08-02 | 2004-04-06 | Sicel Technologies, Inc. | Evaluation of irradiated foods and other items with telemetric dosimeters and associated methods |
| WO2002009775A3 (en) * | 2000-08-02 | 2002-05-30 | Sicel Technologies Inc | Evaluation of irradiated foods or other items with telemetric dosimeters and associated methods |
| US7491942B2 (en) | 2001-11-30 | 2009-02-17 | Sicel Technologies, Inc. | Single-use internal dosimeters for detecting radiation in fluoroscopy and other medical procedures/therapies |
| US7495224B2 (en) | 2001-11-30 | 2009-02-24 | Sicel Technologies, Inc. | Single-use external dosimeters for use in radiation therapies and related methods and systems |
| US7557353B2 (en) | 2001-11-30 | 2009-07-07 | Sicel Technologies, Inc. | Single-use external dosimeters for use in radiation therapies |
| US8951473B2 (en) | 2008-03-04 | 2015-02-10 | Massachusetts Institute Of Technology | Devices and methods for determination of species including chemical warfare agents |
| US9267908B2 (en) | 2008-03-04 | 2016-02-23 | Massachusetts Institute Of Technology | Devices and methods for determination of species including chemical warfare agents |
| US9114377B2 (en) | 2008-12-12 | 2015-08-25 | Massachusetts Institute Of Technology | High charge density structures, including carbon-based nanostructures and applications thereof |
| US8735313B2 (en) | 2008-12-12 | 2014-05-27 | Massachusetts Institute Of Technology | High charge density structures, including carbon-based nanostructures and applications thereof |
| US8456073B2 (en) | 2009-05-29 | 2013-06-04 | Massachusetts Institute Of Technology | Field emission devices including nanotubes or other nanoscale articles |
| US8426208B2 (en) | 2009-10-06 | 2013-04-23 | Massachusetts Institute Of Technology | Method and apparatus for determining radiation |
| US8187887B2 (en) | 2009-10-06 | 2012-05-29 | Massachusetts Institute Of Technology | Method and apparatus for determining radiation |
| WO2011044221A3 (en) * | 2009-10-06 | 2012-04-26 | Massachusetts Institute Of Technology | Method and apparatus for determining radiation |
| US8476510B2 (en) | 2010-11-03 | 2013-07-02 | Massachusetts Institute Of Technology | Compositions comprising and methods for forming functionalized carbon-based nanostructures |
| US9770709B2 (en) | 2010-11-03 | 2017-09-26 | Massachusetts Institute Of Technology | Compositions comprising functionalized carbon-based nanostructures and related methods |
| US11505467B2 (en) | 2017-11-06 | 2022-11-22 | Massachusetts Institute Of Technology | High functionalization density graphene |
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