JPH02162288A - Neutron counter - Google Patents
Neutron counterInfo
- Publication number
- JPH02162288A JPH02162288A JP31652488A JP31652488A JPH02162288A JP H02162288 A JPH02162288 A JP H02162288A JP 31652488 A JP31652488 A JP 31652488A JP 31652488 A JP31652488 A JP 31652488A JP H02162288 A JPH02162288 A JP H02162288A
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- neutron
- radiation source
- particle
- live zero
- 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
- 230000005855 radiation Effects 0.000 claims abstract description 10
- 239000011248 coating agent Substances 0.000 claims abstract description 4
- 238000000576 coating method Methods 0.000 claims abstract description 4
- WTEOIRVLGSZEPR-UHFFFAOYSA-N boron trifluoride Chemical compound FB(F)F WTEOIRVLGSZEPR-UHFFFAOYSA-N 0.000 abstract description 21
- 229910015900 BF3 Inorganic materials 0.000 abstract description 12
- 239000002245 particle Substances 0.000 abstract description 10
- 238000006243 chemical reaction Methods 0.000 abstract description 5
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical group [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 abstract description 4
- LBDSXVIYZYSRII-IGMARMGPSA-N alpha-particle Chemical compound [4He+2] LBDSXVIYZYSRII-IGMARMGPSA-N 0.000 abstract description 3
- 150000002500 ions Chemical class 0.000 abstract description 3
- 238000005259 measurement Methods 0.000 abstract description 2
- 230000005684 electric field Effects 0.000 description 1
- 230000005281 excited state Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は中性子の検出に用いられる中性子計数管に関
するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] This invention relates to a neutron counter used for detecting neutrons.
第2図は例えば特公昭61−35657号公報に示され
た従来の中性子計数管を示す縦断面図であり、以下の説
明では3フッ化ホウ素比例計数管を例として説明する。FIG. 2 is a longitudinal cross-sectional view showing a conventional neutron counter disclosed, for example, in Japanese Patent Publication No. 61-35657, and the following description will be made using a boron trifluoride proportional counter as an example.
第2図において、lは外筒電極である円筒状陰極(以下
、陰極という)、2a、2bは陰極lの両端に気密的に
取付けられた端板、3a、3bはこの端板2a、2bの
ほぼ中央に取付けられた絶縁端子、4はこの絶縁端子3
a、3b間の陰極1の中心軸上に張設された芯線径が2
5〜1100uのタングステン線よりなる中心電極であ
る陽極、5は3フツ化ホウ素(BF。In FIG. 2, l is a cylindrical cathode (hereinafter referred to as a cathode) which is an outer cylinder electrode, 2a and 2b are end plates airtightly attached to both ends of the cathode l, and 3a and 3b are end plates 2a and 2b. The insulated terminal 4 is installed approximately in the center of the insulated terminal 3.
The diameter of the core wire stretched on the central axis of the cathode 1 between a and 3b is 2
The anode is a center electrode made of a tungsten wire of 5 to 1100 u, and 5 is boron trifluoride (BF).
ガス)である。gas).
次に動作について説明する。3フッ化ホウ素比例計数管
は、熱中性子(エネルギーが0.025 eV程度の中
性子)を検出する中性子検出器である。Next, the operation will be explained. A boron trifluoride proportional counter is a neutron detector that detects thermal neutrons (neutrons with an energy of about 0.025 eV).
中性子はそれ自身電荷をもたないので、次のような核反
応を起こさせ、電離能力をもった荷電粒子を発生させる
。Since neutrons themselves have no electric charge, they cause the following nuclear reactions to generate charged particles that have the ability to ionize.
凰’B +n (中性子)→フLi” +α+2.3
MeV’Li” −* ’Ll+0.48MeV(r)
’Li”:励起状態
核反応で生じたα粒子とLi核とがBF、ガス中を通過
する時、各々の核はBF、ガスを電離しながらそのエネ
ルぎ−を失っていく。一方、陰極lの中央には陽極4が
張架され高電圧が印加され強い電場が形成されており、
その電荷によって電子はガス増幅を起こしパルス信号を
作り出す。凰'B +n (neutron) → FuLi” +α+2.3
MeV'Li'' −* 'Ll+0.48MeV(r)
'Li': When α particles and Li nuclei generated in an excited state nuclear reaction pass through BF and gas, each nucleus loses its energy while ionizing BF and gas. An anode 4 is stretched across the center of the l, and a high voltage is applied to form a strong electric field.
This charge causes the electrons to amplify the gas and create a pulse signal.
従来の中性子計数管は以上のように構成されているので
、熱中性子を精度よく計測するには定期的に校正を行っ
ているが、通常その校正は標準線源である中性子を持っ
ていなければならず、また長期にわたって未使用の3フ
ッ化ホウ素比例計数管は電荷をパルス的に計数して中性
子を正しく計測するという健全性の確保が容易にできな
いという問題点があった。Conventional neutron counter tubes are configured as described above, so they must be calibrated periodically to accurately measure thermal neutrons, but normally this calibration is only possible if you have a standard source of neutrons. In addition, there was a problem in that it was not easy to ensure the integrity of the boron trifluoride proportional counter tube, which had not been used for a long time, by counting charges in pulses and accurately measuring neutrons.
この発明は上記のような問題点を解消するためになされ
たもので、標準中性子源を持たずして健全性が確認でき
るようにした中性子計数管を得ることを目的とする。This invention was made to solve the above-mentioned problems, and its purpose is to obtain a neutron counter whose health can be confirmed without having a standard neutron source.
(課題を解決するための手段)
この発明に係る中性子計数管は、内部が気密保持された
外筒電極の中心に設けられた芯線に半減期の長いライブ
ゼロ線源をコーティングして中心電極を形成したもので
ある。(Means for Solving the Problem) A neutron counter according to the present invention has a core wire provided at the center of an outer cylindrical electrode whose interior is kept airtight, and a live zero radiation source with a long half-life is coated to form a center electrode. It was formed.
この発明における中性子計数管は、中性子がなくても芯
線に半減期の長いライブゼロ線源をコーティングした中
心電極を用いたために、ライブゼロ線源からのα粒子で
常に一定の信号パルスが発生することになり、健全性の
確認が容易に行える。The neutron counter in this invention uses a center electrode whose core wire is coated with a live zero source with a long half-life, so that alpha particles from the live zero source always generate a constant signal pulse. Therefore, the soundness can be easily confirmed.
以下、この発明の一実施例を図について説明する。第1
図はこの発明の一実施例を示す縦断面図で、第1図にお
いて第2図と同一または均等部分には同一符号を付して
重複説明を省略する0図において、6はタングステン芯
線に例えば”’Amのライブゼロ線源をコーティングし
た陽極で、この陽極6のライブゼロ線源からは約5.4
MeVのα粒子が半減期433年で放出されている。An embodiment of the present invention will be described below with reference to the drawings. 1st
The figure is a longitudinal cross-sectional view showing one embodiment of the present invention. In Figure 1, the same or equivalent parts as in Figure 2 are denoted by the same reference numerals and redundant explanation is omitted. In Figure 0, 6 is a tungsten core wire, for example. "'Am's live zero radiation source is coated on the anode, and from this anode 6 live zero radiation source, approximately 5.4
MeV alpha particles are emitted with a half-life of 433 years.
しかして、陰極1となる外筒の両端に気密的に端板2a
、2bを取付けることにより気密容器が形成され、この
気密容器と絶縁された絶縁端子3bを貫通して外部へ信
号線が取出される。Thus, the end plates 2a are airtightly attached to both ends of the outer cylinder which becomes the cathode 1.
, 2b are attached to form an airtight container, and a signal line is taken out to the outside through an insulated terminal 3b that is insulated from this airtight container.
また、動作についての説明は従来例と同様であるので省
略するが、外筒電極に対してはタングステン芯線に”A
mのライブゼロ線源をコーティングした中心電極を用い
たので、高電圧を印加すると、下記反応によりイオン対
を生成し、各極性の電橋ヘイオン、電子の流れが起こり
信号パルスとなる。In addition, the explanation of the operation is omitted as it is the same as the conventional example, but for the outer cylinder electrode, the tungsten core wire is
Since a center electrode coated with a live zero radiation source of m is used, when a high voltage is applied, ion pairs are generated by the reaction described below, and a flow of electric bridge heyons and electrons of each polarity occurs, resulting in a signal pulse.
BF2−+ BF3”+e−(w値は約35eV)また
、この”’Amのライブゼロ線源からでるα粒子のエネ
ルギーは約5.4MeVであり、3フッ化ホウ素比例計
数管として中性子と3フツ化ホウ素との核反応によって
生ずる荷電粒子のもつエネルギーは約3MeVであり、
入射粒子1個当たり(中性子あるいはライブゼロ線源か
らのα粒子)のパルスは同程度のものであり、計測条件
(印加電圧、ディスクリ設定電圧)を変えずに両パルス
共に計測できる。そこで中性子モニターとして計測しな
い場合(長期保管している場合)にも上記α粒子による
パルスを定期的に計測することで37フ化ホウ素計数管
の健全性が確認できる。BF2-+ BF3"+e- (w value is about 35 eV) Also, the energy of the α particles emitted from this "'Am live zero radiation source is about 5.4 MeV, and as a boron trifluoride proportional counter, it can be used as a neutron and 3 The energy of the charged particles produced by the nuclear reaction with boron fluoride is approximately 3 MeV,
The pulse per incident particle (neutron or α particle from a live zero radiation source) is of the same magnitude, and both pulses can be measured without changing the measurement conditions (applied voltage, discret setting voltage). Therefore, even when not being measured as a neutron monitor (when stored for a long period of time), the health of the 37 boron fluoride counter can be confirmed by periodically measuring the pulses caused by the α particles.
なお、上記実施例では、外筒電極を陰極で、中心電極を
陽極で説明したが、これは外筒電橋を陽極にし、中心電
極を陰極としても上記実施例と同様の効果を奏する。In the above embodiment, the outer tube electrode is used as a cathode and the center electrode is used as an anode. However, even if the outer tube bridge is used as an anode and the center electrode is used as a cathode, the same effect as in the above embodiment can be obtained.
以上のように、この発明によれば、中性子計数管の芯線
に半減期の長いライブゼロ線源(t41Am)をコーテ
ィングして中心電極を形成したものであるため、標準中
性子源がなくても健全性の確認をいつでも、どこでもで
きるという効果がある。As described above, according to the present invention, since the center electrode is formed by coating the core wire of the neutron counter tube with a live zero source (t41Am) having a long half-life, it can be operated without a standard neutron source. It has the effect of allowing you to confirm your gender anytime, anywhere.
【図面の簡単な説明】
第1図はこの発明の一実施例による中性子計数管を示す
縦断面図、第2図は従来の中性子計数管の一例を示す縦
断面図である。
1は外筒電極、6は中心電極である。
なお、図中、同一符号は同一、または相当部分を示す。BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a longitudinal sectional view showing a neutron counter according to an embodiment of the present invention, and FIG. 2 is a longitudinal sectional view showing an example of a conventional neutron counter. 1 is an outer cylinder electrode, and 6 is a center electrode. In addition, in the figures, the same reference numerals indicate the same or equivalent parts.
Claims (1)
上記外筒電極と中心電極との間に高電圧を印加すること
により生ずる信号パルスを計数して熱中性子を計測する
中性子計数管において、上記中心電極を芯線に半減期の
長いライブゼロ線源をコーティングして形成したことを
特徴とする中性子計数管。A center electrode is provided at the center of an outer cylinder electrode whose interior is kept airtight.
In a neutron counter tube that measures thermal neutrons by counting signal pulses generated by applying a high voltage between the outer cylindrical electrode and the center electrode, a live zero radiation source with a long half-life is connected to the center electrode as a core wire. A neutron counter tube characterized by being formed by coating.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP31652488A JPH02162288A (en) | 1988-12-16 | 1988-12-16 | Neutron counter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP31652488A JPH02162288A (en) | 1988-12-16 | 1988-12-16 | Neutron counter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02162288A true JPH02162288A (en) | 1990-06-21 |
Family
ID=18078065
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP31652488A Pending JPH02162288A (en) | 1988-12-16 | 1988-12-16 | Neutron counter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02162288A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008014947A (en) * | 2006-07-06 | 2008-01-24 | General Electric Co <Ge> | Helium-3 neutron proportional counter equipped with internal gas leak detection, and related method |
KR100866888B1 (en) * | 2006-10-04 | 2008-11-04 | 한국원자력연구원 | Radiation Sensor And Method For Measuring Steel-Sheet Thickness With Improving Sensitivity By Using Wire Electrode And Pressurized Mixed-Gas |
JP2015197332A (en) * | 2014-03-31 | 2015-11-09 | 株式会社東芝 | radiation measuring device |
-
1988
- 1988-12-16 JP JP31652488A patent/JPH02162288A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008014947A (en) * | 2006-07-06 | 2008-01-24 | General Electric Co <Ge> | Helium-3 neutron proportional counter equipped with internal gas leak detection, and related method |
KR100866888B1 (en) * | 2006-10-04 | 2008-11-04 | 한국원자력연구원 | Radiation Sensor And Method For Measuring Steel-Sheet Thickness With Improving Sensitivity By Using Wire Electrode And Pressurized Mixed-Gas |
JP2015197332A (en) * | 2014-03-31 | 2015-11-09 | 株式会社東芝 | radiation measuring device |
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