JPH0247581A - Neutron detector - Google Patents
Neutron detectorInfo
- Publication number
- JPH0247581A JPH0247581A JP19872488A JP19872488A JPH0247581A JP H0247581 A JPH0247581 A JP H0247581A JP 19872488 A JP19872488 A JP 19872488A JP 19872488 A JP19872488 A JP 19872488A JP H0247581 A JPH0247581 A JP H0247581A
- Authority
- JP
- Japan
- Prior art keywords
- dose equivalent
- container
- proportional counter
- neutron detector
- signal
- 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
Links
- -1 hydrogen compound Chemical class 0.000 claims abstract description 22
- 239000004698 Polyethylene Substances 0.000 claims abstract description 10
- 229920000573 polyethylene Polymers 0.000 claims abstract description 10
- 239000011248 coating agent Substances 0.000 claims abstract 2
- 238000000576 coating method Methods 0.000 claims abstract 2
- WTEOIRVLGSZEPR-UHFFFAOYSA-N boron trifluoride Chemical compound FB(F)F WTEOIRVLGSZEPR-UHFFFAOYSA-N 0.000 claims description 4
- 239000012528 membrane Substances 0.000 claims description 3
- 229910015900 BF3 Inorganic materials 0.000 claims description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 claims description 2
- 229910052796 boron Inorganic materials 0.000 claims description 2
- 150000002483 hydrogen compounds Chemical class 0.000 claims description 2
- 239000001257 hydrogen Substances 0.000 abstract description 10
- 229910052739 hydrogen Inorganic materials 0.000 abstract description 10
- 239000002245 particle Substances 0.000 abstract description 10
- 239000007789 gas Substances 0.000 abstract description 6
- 239000004020 conductor Substances 0.000 abstract description 2
- 238000010586 diagram Methods 0.000 description 6
- 238000012545 processing Methods 0.000 description 5
- 230000005855 radiation Effects 0.000 description 5
- 238000005259 measurement Methods 0.000 description 3
- 239000003758 nuclear fuel Substances 0.000 description 3
- 238000001514 detection method Methods 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 1
- 231100000987 absorbed dose Toxicity 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 231100000673 dose–response relationship Toxicity 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
Landscapes
- Measurement Of Radiation (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は粒子加速器取扱施設、核燃料施設、原子炉施設
等における放射線計測、放射線管理に用いることのでき
る中性子検出器に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a neutron detector that can be used for radiation measurement and radiation management in particle accelerator handling facilities, nuclear fuel facilities, nuclear reactor facilities, and the like.
[従来の技術]
一般に、生体に対する放射線の効果を評価する場合、線
量当量という概念が用いられ、吸収線量と線質係数の積
で与えられる。線質係数は、粒子の飛跡に沿った生体分
子に対する局所的なエネルギーの付加率、即ち線エネル
ギー付与と共に増加し、高速電子線、ベータ線、X線、
ガンマ線等では1であり、α粒子、中性子等では大きな
値となる。また線量当量は、実効線量当量や組織線量当
量に分類され、線量当量率は線量当量の単位時間当たり
の値として定義される。[Prior Art] Generally, when evaluating the effects of radiation on a living body, the concept of dose equivalent is used, and is given as the product of absorbed dose and radiation quality coefficient. The radiation quality factor is the local energy addition rate to biomolecules along the trajectory of the particle, that is, it increases with the addition of linear energy.
It is 1 for gamma rays, etc., and becomes a large value for α particles, neutrons, etc. Further, dose equivalent is classified into effective dose equivalent and tissue dose equivalent, and dose equivalent rate is defined as the value of dose equivalent per unit time.
従来、中性子線量当量率の測定は、中性子をポリエチレ
ン等の中性子減速材で減速させ、3フツカ硼素(BFi
を封入したアルミ、或いはステンレス等からなる容器中
に入射させて(n、 α)反応を起こさせ、このとき
出るα粒子(α)でガスをイオン化して、これを電気信
号パルスとして出力端子より取り出すようにしていた。Conventionally, the measurement of neutron dose equivalent rate involves moderating neutrons with a neutron moderator such as polyethylene,
The (n, α) reaction is caused by injecting the gas into a container made of aluminum or stainless steel, etc., and the α particles (α) released at this time ionize the gas, which is then sent as an electrical signal pulse from the output terminal. I was about to take it out.
しかしながら、従来の中性子検出器では線量応答特性が
広いエネルギー領域で一定となるようにポリエチレン等
の中性子減速材を多く使用しているため、装置が大型化
しかつ重くなりがちで、そのため検出器の小型軽量化を
図る上で障害になっていた。また、この方式の線量当量
率計では実効線量当量や組織線量当量等の異なった線量
当量を一つの検出器で測定することが不可能であると共
に、中性子の平均エネルギー等のエネルギー情報を得る
ことができなかった。However, conventional neutron detectors use a large amount of neutron moderating material such as polyethylene so that the dose response characteristics remain constant over a wide energy range, which tends to make the equipment large and heavy. This was an obstacle in efforts to reduce weight. In addition, with this type of dose equivalent rate meter, it is impossible to measure different dose equivalents such as effective dose equivalent and tissue dose equivalent with one detector, and it is also difficult to obtain energy information such as the average energy of neutrons. I couldn't do it.
本発明は上記問題点を解決するためのもので、中性子の
実効線量当量や組織線量当量等、エネルギーにより応答
特性が異なる線量当量を同時に測定でき、かつ中性子の
平均エネルギーも求めることができ、中性子サーベイメ
ータまたはモニタの小型軽量化を図ることの可能な中性
子検出器を提供することを目的とする。The present invention is intended to solve the above-mentioned problems.It is possible to simultaneously measure dose equivalents whose response characteristics differ depending on energy, such as neutron effective dose equivalent and tissue dose equivalent, and also to determine the average energy of neutrons. An object of the present invention is to provide a neutron detector that can reduce the size and weight of a survey meter or monitor.
そのために本発明の中性子検出器は、3フッ化ほう素を
充填し、ほう素の(n、 α)反応を利用したBP、比
例計数管を用いた中性子検出器において、比例計数管の
容器の内面にポリエチレン等の水素化合物の膜をコーテ
ィングしたこと、比例計数管の出力を波高または波形弁
別回路により弁別し、2種類以上の電気信号を取り出す
ようにし、また波高または波形弁別回路により弁別され
た2種類基−ヒの電気信号を各々計数し、各計数値の比
から線量当量、平均エネルギーを求めるようしたことを
特徴とする。To this end, the neutron detector of the present invention is filled with boron trifluoride and utilizes the (n, α) reaction of boron, and is a neutron detector using a proportional counter. The inner surface is coated with a film of hydrogen compound such as polyethylene, the output of the proportional counter is discriminated by a wave height or waveform discrimination circuit, and two or more types of electrical signals are extracted. It is characterized in that two types of electrical signals are counted, and the dose equivalent and average energy are determined from the ratio of each counted value.
本発明の中性子検出器はBF、比例計数管の容器の内面
にポリエチレン等の水素化合物の膜をコーティングし、
低速中性子においては(n、 α)反応により、高速中
性子においては(n、p)反応によりそれぞれ電気信号
を取り出し、(nα)反応、(n、 ρ)反応により
波高または波形が異なることを利用し、それぞれ分離し
て計数し、その計数比と線量当量、平均エネルギーとの
間に所定の函数関係があることを利用して線量当量や平
均エネルギー等も求めることができるため、1つの検出
器で実効線量当量や組織線量当量の測定を同時に行うこ
とができ、またポリエチレン等の水素化合物が高速中性
子に反応するため多量の減速材を必要とせず、装置の小
型軽量化を図ることができる。The neutron detector of the present invention coats the inner surface of the container of the BF and proportional counter tube with a film of a hydrogen compound such as polyethylene,
Electrical signals are extracted by the (n, α) reaction for slow neutrons and by the (n, p) reaction for fast neutrons, and take advantage of the fact that the wave height or waveform differs depending on the (nα) reaction and (n, ρ) reaction. , are counted separately, and by using the fact that there is a predetermined functional relationship between the counting ratio and the dose equivalent and average energy, it is possible to calculate the dose equivalent and average energy, etc., using a single detector. Effective dose equivalent and tissue dose equivalent can be measured simultaneously, and since hydrogen compounds such as polyethylene react with fast neutrons, a large amount of moderator is not required, making the device smaller and lighter.
以下、実施例を図面を参照して説明する。 Examples will be described below with reference to the drawings.
第1図は本発明の中性子検出器の構造を示す図で、図中
、lOは比例計数管、11は計数管容器、12は中心電
極用芯線、13は出力端子、14は水素化合物の膜、1
5は外側電極である。FIG. 1 is a diagram showing the structure of the neutron detector of the present invention, in which lO is a proportional counter, 11 is a counter container, 12 is a core wire for the center electrode, 13 is an output terminal, and 14 is a hydrogen compound membrane. ,1
5 is an outer electrode.
図において、比例計数管10は容器11の内面にポリエ
チレン等の水素化合物の膜14がコーティングされ、そ
の膜の表面に導電体を塗布して外側電極15を形成し、
中心電極用芯線12との間に高電圧が印加されており、
内部にはBF、ガスが封入されている。In the figure, a proportional counter 10 has a container 11 whose inner surface is coated with a film 14 of a hydrogen compound such as polyethylene, and a conductor is applied to the surface of the film to form an outer electrode 15.
A high voltage is applied between the center electrode core wire 12,
BF and gas are sealed inside.
そしてエネルギーの低い低速中性子が入射すると(n、
α)反応が起こり、比例計数管内にα粒子が放出さ
れる。このα粒子によりガスがイオン化され、イオン化
粒子が円筒形または球形の外側電極15と、中心電極で
ある芯線12の間の高電圧により加速されて両電極間に
電流が流れて増幅され、出力端子13より電気信号パル
スとして出力される。また、高速中性子が入射した場合
には、比例計数管10の容器11の内側にコーティング
したポリエチレン等の水素化合物の膜の14中の水素と
、(n、P)反応を起こし、この反跳陽子(p)が比例
計数管内に放出される。この反跳陽子がα粒子の場合と
同様にガスをイオン化させ、電気信号パルスとして出力
端子より取り出される。When a slow neutron with low energy enters (n,
α) A reaction occurs and α particles are released into the proportional counter. The gas is ionized by these α particles, and the ionized particles are accelerated by the high voltage between the cylindrical or spherical outer electrode 15 and the core wire 12, which is the center electrode, and a current flows between the two electrodes and is amplified. 13, it is output as an electrical signal pulse. In addition, when fast neutrons are incident, a (n, p) reaction occurs with the hydrogen in the film 14 of a hydrogen compound such as polyethylene coated on the inside of the container 11 of the proportional counter 10, and the recoil protons (p) is released into the proportional counter. These recoil protons ionize the gas in the same way as α particles, and are extracted from the output terminal as electrical signal pulses.
そして、低速中性子と高速中性子が入射した場合の出力
信号は電圧レヘルや波形が異なるため、信号弁別回路で
弁別可能で、それぞれ別々に計数することができる。Since the output signals when slow neutrons and fast neutrons are incident have different voltage levels and waveforms, they can be discriminated by a signal discrimination circuit and each can be counted separately.
第2図はこのような弁別回路を有する本発明の検出回路
構成を示す図で、図中、21は高電圧回路、22は増幅
器、23は信号弁別回路、24゜25は31数回路、2
6は演算処理回路、27は表承部である。FIG. 2 is a diagram showing the configuration of a detection circuit according to the present invention having such a discrimination circuit.
6 is an arithmetic processing circuit, and 27 is a representation section.
比例計数管10には高電圧回路21により外側電極と中
心電極間に高電圧が印加されており、前述したように中
性子が入射すると出力端子より電気信号パルスが取り出
され、この出力パルスを増幅器22で増幅し、信号弁別
回路23でエネルギーレヘル或いは波形によって、α信
号(α粒子により生した信号)、或いはp信号(反跳陽
子により生した信号)に弁別し、それぞれ計数回路24
゜25により計数する。A high voltage is applied to the proportional counter tube 10 between the outer electrode and the center electrode by the high voltage circuit 21, and as described above, when a neutron is incident, an electric signal pulse is extracted from the output terminal, and this output pulse is sent to the amplifier 22. The signal is amplified by a signal discrimination circuit 23 and discriminated into an α signal (a signal generated by α particles) or a p signal (a signal generated by recoil protons) depending on the energy level or waveform, and a counting circuit 24 respectively.
Count by ゜25.
ところで、中性子エネルギーに対する(nρ)反応、(
n、 α)反応の感度は第3図のような特性を示し、
各反応は中性子のエネルギーによりそれぞれ異なり、所
定の確率で生じている。そこで、第2図の計数回路24
における計数値を02、計数回路25における計数値を
CIとし、単一エネルギー中性子による照射実験や中性
子輸送計算による感度解析を行うことにより、計数比C
2/CIと線量当i1D、又は平均エネルギー巳、V。By the way, the (nρ) reaction to neutron energy, (
n, α) The sensitivity of the reaction shows the characteristics as shown in Figure 3,
Each reaction differs depending on the energy of the neutron, and occurs with a predetermined probability. Therefore, the counting circuit 24 in FIG.
By setting the count value in 02 and the count value in the counting circuit 25 as CI, the count ratio C
2/CI and i1D per dose, or mean energy, V.
との間に、例えば第4図に示すような函数曲線が求める
られる。なお、図の函数曲線は計数値CIで除して規格
化している。この函数をプログラム化し、演算処理回路
26に記憶させておき、任意の中性子エネルギー分布を
持つ場所で測定することにより、計数(l¥CIおよび
C2から第4図の函数関係を利用し、演算処理回路26
により線量当〒や平均エネルギーを算出することができ
る。For example, a functional curve as shown in FIG. 4 is obtained between . Note that the function curve in the figure is normalized by dividing by the count value CI. By programming this function, storing it in the arithmetic processing circuit 26, and measuring it at a location with an arbitrary neutron energy distribution, it is possible to perform arithmetic processing using the functional relationship shown in Figure 4 from l\CI and C2. circuit 26
The dose equivalent and average energy can be calculated by
こうして演算処理回路22で線量当量や平均エネルギー
が算出され、その値が表示部27に表示される。In this way, the arithmetic processing circuit 22 calculates the dose equivalent and the average energy, and the values are displayed on the display section 27.
〔発明の効果]
以上のように本発明によれば、1つの検出器で実効線量
当量や&[I織線量当量の測定を同時に行うことが可能
となり、また測定場所の平均エネルギー等のエネルギー
情報を得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 simultaneously measure the effective dose equivalent and the &[I-weave dose equivalent] with one detector, and it is also possible to measure energy information such as the average energy of the measurement location. It becomes possible to obtain.
そしてポリエチレン等の水素化合物が高速中性子に反応
するため、従来のように多量の減速材を必要としないた
め、中性子検出器の小型軽量化を図ることができる。Since a hydrogen compound such as polyethylene reacts with fast neutrons, a large amount of moderator is not required as in the conventional method, so the neutron detector can be made smaller and lighter.
第1図は本発明の中性子検出器の構造を示す図、第2図
は本発明の中性子検出回路の構成を示す図、第3図は中
性子エネルギーに対する反応の感度特性を示す図、第4
図は計数比C2/C1と線量当ID、tたは平均エネル
ギーE @ V 1+との関係を示す図である。
10・・・比例計数管、II・・・計数管容器、12・
・・中心fi17ji用芯線、13・・・出力端子、1
4・・・水素化合物の膜、15・・・外側電極、21・
・・高電圧回路、22・・・増幅器、23・・・信号弁
別回路、24.25・・・計数回路、26・・・演算処
理回路、27・・・表示部。
出 願 人 動力炉・核燃料開発事業団代理人弁理
士 蛭 川 昌 信(外4名)第4図
讐土&ぶヒ(C2/C1)FIG. 1 is a diagram showing the structure of the neutron detector of the present invention, FIG. 2 is a diagram showing the configuration of the neutron detection circuit of the present invention, FIG. 3 is a diagram showing the sensitivity characteristics of the reaction to neutron energy, and FIG.
The figure is a diagram showing the relationship between the count ratio C2/C1 and the ID per dose, t, or the average energy E @ V 1+. 10... Proportional counter tube, II... Counter tube container, 12.
... Core wire for center fi17ji, 13 ... Output terminal, 1
4... Hydrogen compound membrane, 15... Outer electrode, 21.
...High voltage circuit, 22...Amplifier, 23...Signal discrimination circuit, 24.25...Counting circuit, 26...Arithmetic processing circuit, 27...Display unit. Applicant Patent attorney representing the Power Reactor and Nuclear Fuel Development Corporation Masanobu Hirukawa (4 others) Figure 4 Hokuto & Buhi (C2/C1)
Claims (3)
応を利用したBF_3比例計数管を用いた中性子検出器
において、比例計数管の容器の内面にポリエチレン等の
水素化合物の膜をコーティングしたことを特徴とする中
性子検出器。(1) In a neutron detector using a BF_3 proportional counter filled with boron trifluoride and utilizing the (n, α) reaction of boron, hydrogen compounds such as polyethylene are added to the inner surface of the proportional counter container. A neutron detector characterized by a membrane coating.
り弁別し、2種類以上の電気信号を取り出すようにした
請求項1記載の中性子検出器。(2) The neutron detector according to claim 1, wherein the output of the proportional counter tube is discriminated by a wave height or waveform discrimination circuit to extract two or more types of electrical signals.
以上の電気信号を各々計数し、各計数値の比から線量当
量、平均エネルギーを求めるようにした請求項2記載の
中性子検出器。(3) The neutron detector according to claim 2, wherein the two or more types of electrical signals discriminated by the wave height or waveform discrimination circuit are each counted, and the dose equivalent and average energy are determined from the ratio of each counted value.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19872488A JPH0247581A (en) | 1988-08-09 | 1988-08-09 | Neutron detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19872488A JPH0247581A (en) | 1988-08-09 | 1988-08-09 | Neutron detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0247581A true JPH0247581A (en) | 1990-02-16 |
| JPH0525313B2 JPH0525313B2 (en) | 1993-04-12 |
Family
ID=16395938
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19872488A Granted JPH0247581A (en) | 1988-08-09 | 1988-08-09 | Neutron detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0247581A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009097967A (en) * | 2007-10-16 | 2009-05-07 | High Energy Accelerator Research Organization | Gas detector for neutron measurement |
| JP2010223632A (en) * | 2009-03-19 | 2010-10-07 | National Institute Of Advanced Industrial Science & Technology | Neutron energy measuring instrument |
| US20130284926A1 (en) * | 2012-04-26 | 2013-10-31 | Mitsubishi Electric Corporation | Dose rate measuring apparatus |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP3407032B2 (en) * | 2000-03-13 | 2003-05-19 | 核融合科学研究所長 | Radiation detector |
-
1988
- 1988-08-09 JP JP19872488A patent/JPH0247581A/en active Granted
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009097967A (en) * | 2007-10-16 | 2009-05-07 | High Energy Accelerator Research Organization | Gas detector for neutron measurement |
| JP2010223632A (en) * | 2009-03-19 | 2010-10-07 | National Institute Of Advanced Industrial Science & Technology | Neutron energy measuring instrument |
| US20130284926A1 (en) * | 2012-04-26 | 2013-10-31 | Mitsubishi Electric Corporation | Dose rate measuring apparatus |
| US9029769B2 (en) * | 2012-04-26 | 2015-05-12 | Mitsubishi Electric Corporation | Dose rate measuring apparatus |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0525313B2 (en) | 1993-04-12 |
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