JPS5814073A - Self-output type radiation detector - Google Patents
Self-output type radiation detectorInfo
- Publication number
- JPS5814073A JPS5814073A JP11270681A JP11270681A JPS5814073A JP S5814073 A JPS5814073 A JP S5814073A JP 11270681 A JP11270681 A JP 11270681A JP 11270681 A JP11270681 A JP 11270681A JP S5814073 A JPS5814073 A JP S5814073A
- Authority
- JP
- Japan
- Prior art keywords
- emitter
- radiation detector
- lead wire
- collector
- outer diameter
- 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
- G01T3/00—Measuring neutron radiation
- G01T3/006—Measuring neutron radiation using self-powered detectors (for neutrons as well as for Y- or X-rays), e.g. using Compton-effect (Compton diodes) or photo-emission or a (n,B) nuclear reaction
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
Description
【発明の詳細な説明】
この発明は、中性子やγ線を検出する自己出力型放射線
検出器に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a self-powering radiation detector that detects neutrons and gamma rays.
第1図は従来の自己出力型放射線検出器の構成を示す断
面図である。この第1図において、lは円筒シース状の
コレクタであり、2はコレクタ1の内部に同軸状に配設
された円柱状のエミッタである。このエミッタ2の一端
にリード線8が電気的に接続されている。このリード線
8はコレクタ1の内部において同軸状に配設され、信号
引き出し用として使用されている。FIG. 1 is a sectional view showing the configuration of a conventional self-output type radiation detector. In FIG. 1, 1 is a cylindrical sheath-like collector, and 2 is a cylindrical emitter disposed coaxially inside the collector 1. In FIG. A lead wire 8 is electrically connected to one end of the emitter 2. This lead wire 8 is disposed coaxially inside the collector 1 and is used for extracting signals.
コレクタlとエミッタ20間の空隙には、絶縁物4が充
填されている。この絶縁物4のために、コレクタ1およ
びエミッタはリード線8から電気的に絶縁されている。The gap between the collector l and the emitter 20 is filled with an insulator 4. Due to this insulator 4, collector 1 and emitter are electrically isolated from lead wire 8.
絶縁物4として、通常A1*OsまたはMgOが用いら
れている。As the insulator 4, A1*Os or MgO is usually used.
中性子用の検出管においては、エミッタは中性子を吸収
断面積の大きい物質、たとえば、ロジウムやバナジウム
でできており、中性子が入射すると、エミッタは中性子
を吸収して放射能を帯び、β崩壊する。In a neutron detection tube, the emitter is made of a material with a large neutron absorption cross section, such as rhodium or vanadium, and when a neutron is incident, the emitter absorbs the neutron, becomes radioactive, and undergoes β decay.
この際、放出されたβ線の一部は絶縁物4を貫いてコレ
クタlに到達する。コレクタ1も同様に放射能を帯び、
β線を放出するが、コレクタlには中性子の吸収断面積
の小さい物質を選んであるので、β線の正味の流れはエ
ミッタ2からコレクタ1に向かう。At this time, a part of the emitted β rays penetrates the insulator 4 and reaches the collector l. Collector 1 is also radioactive,
β-rays are emitted, but since a material with a small neutron absorption cross section is selected for the collector l, the net flow of β-rays is directed from the emitter 2 to the collector 1.
このβ線の流れは、周囲の中性子束に比例するので、エ
ミッタとコレクタ間に流れる電流を測定すれば、中性子
束に比例した信号が得られる。The flow of β-rays is proportional to the surrounding neutron flux, so if the current flowing between the emitter and collector is measured, a signal proportional to the neutron flux can be obtained.
また、γ線用の検出器には、エミッタ2にβ線吸収断面
積の大きい物が使用され、コレクタlにはβ線の吸収断
面積の小さい物質を用いており、T線により放出された
電子の正味の流れはエミッタ2からコレクタ1に向かい
、・この電流の大きさがβ線束に比例するので、この電
流を測定すれば、T線束に比例した信号が得られる。In addition, in the gamma ray detector, a material with a large beta ray absorption cross section is used for the emitter 2, and a material with a small beta ray absorption cross section is used for the collector l. The net flow of electrons is from the emitter 2 to the collector 1, and since the magnitude of this current is proportional to the β-ray flux, measuring this current yields a signal proportional to the T-ray flux.
さて、自己出力型検出器の代表的な製法は仕上り外径よ
シはるかに大きい外径をもつコレクタパイプ、エミッタ
棒、リード線およびビーズ状絶縁物を用いて、第2図に
示すように組み立てを行う。Now, the typical manufacturing method for a self-output type detector is to use a collector pipe with an outer diameter much larger than the finished outer diameter, an emitter rod, a lead wire, and a bead-shaped insulator, and assemble it as shown in Figure 2. I do.
この第2図において、第1図と同一部分には同一符号が
付されており、また、4a〜41はそれぞれビーズ状絶
縁物を示す。In FIG. 2, the same parts as in FIG. 1 are given the same reference numerals, and 4a to 41 indicate bead-shaped insulators, respectively.
第2図に示すようにして組み立てた組み立て物にドウロ
ーイングあるいはスウエージングを繰9返し加え、ビー
ズ状絶縁物の充填率を増加させながら、所定の仕上り寸
法まで減少させるものである。Drawing or swaging is applied nine times to the assembly assembled as shown in FIG. 2, thereby increasing the filling rate of the bead-shaped insulators and reducing them to a predetermined finished size.
ところが、従来の自己出力型放射線検出器は棒状のエミ
ッタ2とこれよシ小径のリード線8を外径が異なったま
ま溶接などの方法によ多接合しているので、上記減寸プ
ロセスの際に、この接合部に大きな力がかかり、製作途
中において断線を起こすことが多かった。However, in the conventional self-output type radiation detector, the rod-shaped emitter 2 and the lead wire 8 with a smaller diameter are joined together by welding or other methods with different outer diameters. In addition, a large force was applied to this joint, which often caused the wire to break during manufacturing.
この発明は、上記従来の欠点を除去するためになされた
もので、エミッタとリード線の接続を一方または両方の
外径をゆるやかに変化させるか、両者の間に円錐台状の
金属片を介在させることにより、エミッタとリード線と
の接合面での両者の外径を等しくさせ、製作時の減寸プ
ロセスにおける断線の発生を少なくできる自己出力型放
射線検出器を提供することを目的とする。This invention was made to eliminate the above-mentioned conventional drawbacks, and the emitter and lead wire are connected by either gently changing the outer diameter of one or both, or by interposing a truncated cone-shaped metal piece between the two. It is an object of the present invention to provide a self-output type radiation detector that can make the outer diameters of the emitter and lead wire equal at their joint surfaces and reduce the occurrence of wire breakage during the reduction process during manufacturing.
以下、この発明の自己出力型放射線検出器の実施例につ
いて図面に基づき説明する。第8図はその一実施例の構
成を示す断面図である。この第8図において、第1図お
よび第2図と同一部分には同一符号を付して述べること
にする。Embodiments of the self-output type radiation detector of the present invention will be described below with reference to the drawings. FIG. 8 is a sectional view showing the configuration of one embodiment. In FIG. 8, the same parts as in FIGS. 1 and 2 will be described with the same reference numerals.
コレクタl内にエミッタ2が同軸状に挿入されており、
エミッタ2の一端にリード線8が接続されているが、エ
ミッタ2との接合端部分はテーパ状に太くなっており、
接合面において、エミッタ2とリード線8と外径寸法が
等しくなっている。Emitter 2 is coaxially inserted into collector l,
A lead wire 8 is connected to one end of the emitter 2, and the end where it connects to the emitter 2 is tapered and thick.
At the joint surface, the emitter 2 and the lead wire 8 have the same outer diameter.
この場合、放射線の検出性能に関しては、従来の自己出
力型放射線検出器と比べて実質的な変化はないが、製作
時の減寸プロセスにおいて加わる引張力に対して強い抵
抗力を示し、従来の欠点であった製作途上での断線トラ
ブルを減少させることができる。In this case, there is no substantial change in radiation detection performance compared to conventional self-powering radiation detectors, but it shows strong resistance to the tensile force applied during the manufacturing process and It is possible to reduce the problem of wire breakage during manufacturing, which was a drawback.
同じ効果は、エミッタの外径をその端部で漸減させるこ
とによっても得られることは明らかである。It is clear that the same effect can also be obtained by tapering the outer diameter of the emitter at its ends.
第4図はこの発明の自己出力型放射線検出器の他の実施
例の構成を示す断面図である。この第4図では、リード
線8またはエミッタ2の外径をその接合端部分において
変化せる代わりに、円錐台状の金属片5を介在させるこ
とにより、2個所ある接合面での両側の部分の外径を等
しくしている。FIG. 4 is a sectional view showing the structure of another embodiment of the self-output type radiation detector of the present invention. In FIG. 4, instead of changing the outer diameter of the lead wire 8 or the emitter 2 at the joint end portion, a truncated cone-shaped metal piece 5 is interposed to change the outer diameter of the lead wire 8 or the emitter 2 on both sides of the two joint surfaces. The outer diameters are the same.
また、二つの接合端部分の接合面の間の円錐台状金属片
5の外径はゆるやかに変わっている。これによシ、放射
性の検出性能の実質的な変化をもたらすことなく、第8
図の場合と同様に製作過程における断線トラブルを減少
させることができる。Further, the outer diameter of the truncated conical metal piece 5 between the joint surfaces of the two joint end portions changes gradually. This allows the eighth
As in the case shown in the figure, disconnection troubles during the manufacturing process can be reduced.
なお、第8図および第4図における4は従来と同様の絶
縁物である。Note that 4 in FIGS. 8 and 4 is an insulator similar to the conventional one.
以上のように、この発明の自己出力型放射線検出器によ
れば、エミッタに接続するリード線の端部をエミッタと
同じ外径寸法にして漸減させるか、あるいはエミッタと
リード線との間に円錐台状の金属片を介在させ、この円
錐台状金属片のエミッタ側をエミッタの外径と同寸法に
、リード線に向かって漸減するようにしたので、放射線
検出性能を低下することなく、製作時の断線トラブルを
減少させることができる。As described above, according to the self-output type radiation detector of the present invention, the end of the lead wire connected to the emitter is made to have the same outer diameter as the emitter and gradually decreases, or a cone is formed between the emitter and the lead wire. A truncated metal piece is interposed, and the emitter side of this truncated conical metal piece has the same dimensions as the emitter's outer diameter and gradually decreases toward the lead wire, so it can be manufactured easily without degrading radiation detection performance. It is possible to reduce disconnection troubles at times.
第1図は従来の自己出力型放射線検出器の断面図、第2
図は従来の自己出力型放射線検出器における初期組み立
て段階の断面図、第8図はこの発明の自己出力型放射検
出器の一実施例の構成を示す断面図、第4図はこの発明
の自己出力型放射線検出器の他の実施例の構成を示す断
面図である。
1・・・・・ コレクタ、2・・・・・ エミッタ、8
・・・・リード線、4・・・・・絶縁物、5・・・・・
円錐台状の金属片。
なお、図中同一符号は同一または相当部分を示す。
代理人 葛 野 信 −
管1図
/
2 l づFigure 1 is a cross-sectional view of a conventional self-output type radiation detector;
The figure is a cross-sectional view of the initial assembly stage of a conventional self-output type radiation detector, FIG. 8 is a cross-sectional view showing the configuration of an embodiment of the self-output type radiation detector of the present invention, and FIG. 7 is a cross-sectional view showing the configuration of another example of the output type radiation detector. 1... Collector, 2... Emitter, 8
...Lead wire, 4...Insulator, 5...
A truncated cone-shaped metal piece. Note that the same reference numerals in the figures indicate the same or corresponding parts. Agent Makoto Kuzuno - Figure 1/2
Claims (2)
的に絶縁されて同心状に配設された柱状のエミッタ、こ
のエミッタの一端に電気的に接続されて信号を取シ出す
とともに、エミッタとの接合端部分においてエミッタと
同一外径寸法を′なしかつエミッタとは反対方向に向か
って外径寸法が漸減したリード線を備えてなる自己出力
型放射線検出器。(1) A cylindrical sheath-like collector, a columnar emitter electrically insulated and concentrically arranged within this collector, electrically connected to one end of this emitter to output signals, and A self-output type radiation detector comprising a lead wire having the same outer diameter as the emitter at the joint end portion thereof and whose outer diameter gradually decreases in the direction opposite to the emitter.
錐台状の金属片を介在させてエミッタに接合されこの金
属片のエミッタ側の接合端分の外径はエミッタと同寸法
となしリード線側に向かって漸減することを特徴とする
特許請求の範囲第1項記載の放射線検出器。(2) The lead wire is joined to the emitter with a truncated cone-shaped metal piece interposed at the end where it connects to the emitter, and the outer diameter of the joined end of this metal piece on the emitter side is the same size as the emitter. 2. The radiation detector according to claim 1, wherein the radiation detector gradually decreases toward the sides.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11270681A JPS5814073A (en) | 1981-07-17 | 1981-07-17 | Self-output type radiation detector |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11270681A JPS5814073A (en) | 1981-07-17 | 1981-07-17 | Self-output type radiation detector |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5814073A true JPS5814073A (en) | 1983-01-26 |
Family
ID=14593451
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11270681A Pending JPS5814073A (en) | 1981-07-17 | 1981-07-17 | Self-output type radiation detector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5814073A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6316462U (en) * | 1986-07-16 | 1988-02-03 |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS55125468A (en) * | 1979-03-14 | 1980-09-27 | Westinghouse Electric Corp | Wideerange radiation detector |
-
1981
- 1981-07-17 JP JP11270681A patent/JPS5814073A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS55125468A (en) * | 1979-03-14 | 1980-09-27 | Westinghouse Electric Corp | Wideerange radiation detector |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6316462U (en) * | 1986-07-16 | 1988-02-03 |
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