JPS5979861A - Static electricity detector - Google Patents

Static electricity detector

Info

Publication number
JPS5979861A
JPS5979861A JP18909082A JP18909082A JPS5979861A JP S5979861 A JPS5979861 A JP S5979861A JP 18909082 A JP18909082 A JP 18909082A JP 18909082 A JP18909082 A JP 18909082A JP S5979861 A JPS5979861 A JP S5979861A
Authority
JP
Japan
Prior art keywords
hollow body
current collector
conductive hollow
static electricity
resistance
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
Application number
JP18909082A
Other languages
Japanese (ja)
Other versions
JPS6365907B2 (en
Inventor
Shinji Yagi
八木 新治
Toshio Nakada
中田 敏男
Taiji Nakamura
泰治 中村
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.)
Tokyo Gas Co Ltd
Kasuga Denki Inc
Original Assignee
Tokyo Gas Co Ltd
Kasuga Denki Inc
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 Tokyo Gas Co Ltd, Kasuga Denki Inc filed Critical Tokyo Gas Co Ltd
Priority to JP18909082A priority Critical patent/JPS5979861A/en
Publication of JPS5979861A publication Critical patent/JPS5979861A/en
Publication of JPS6365907B2 publication Critical patent/JPS6365907B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R29/00Arrangements for measuring or indicating electric quantities not covered by groups G01R19/00 - G01R27/00
    • G01R29/24Arrangements for measuring quantities of charge

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Radiation (AREA)

Abstract

PURPOSE:To prevent the deterioration of detection preciseness caused by applying insulating coating to a conductive hollow body, by mounting a means for regulating the resistance of an electric circuit formed in the space between a current collector and the conductive hollow body in said body. CONSTITUTION:A static electricity detection probe 7 is constituted from such a mechanism that a current collector 14 is supported by an insulating support 13 in a metal cylindrical case 12 and an output circuit is further connected to the current collector 14 through a connector resistance 16 while the current collector 14 is connected to the case 12 through high resistance 17. alpha-Rays radiated from the current collector 14 irradiates the bottom surface 11 of a liquid-tight space 10 which is, in turn, ionized to form an electric circuit. The resistance R2 of this circuit is proportional to the distance between the current collector 14 and the bottom surface 11. Therefore, the position to be inserted and mounted of the cylindrical case 12 is adjusted up and down to enable the adjustment of R2. As mentioned above, by properly selecting the position to be inserted and mounted for the case 12, the deterioration of detection preciseness of a conductive hollow body having insulating coating applied thereto can be prevented.

Description

【発明の詳細な説明】 本発明は、帯電している液体、気体、粉体等の流体の静
箪気を框出する静電気検出器に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a static electricity detector that detects static air from a fluid such as a charged liquid, gas, or powder.

不出願人らは、この種の静市7気検出器であって、特に
石油類の帯′#I.電位を検出することを意図レたもの
として、記l図に示すように、放射性物体を有する集電
器及び出力回路を内蔵した集電式静電気検出ブローブ1
を、外周ih+に薄い絶縁被シ2を施した金属球3内に
固定配置(動かないように固着)し、この金属球3に誘
導された静寛気を放射線%離イ1用によって集雷,器゛
煽集可し、その電位に応じた亀9,信号を出力回路より
出力するようにして在るものを既シて提案(特公昭57
−1791号公報で公知)している。
The applicants proposed a static air detector of this type, especially for petroleum products. As shown in Figure 1, a current collecting type static electricity detection probe 1 with a built-in current collector having a radioactive substance and an output circuit is intended to detect electric potential.
is fixedly placed (fixed so as not to move) inside a metal ball 3 whose outer periphery is covered with a thin insulating sheath 2, and the static air induced in this metal ball 3 is collected by radiation % separation A1. , a device has already been proposed in which a signal can be collected from the output circuit according to the electric potential of the turtle 9 (Special Publication Publication No. 57).
-1791)).

このものにおいて、金h4球3に絶縁被留2を施したの
け、その金属球3と外部の帯笛,物との間のコロナ放電
あるいは火花放市,を防止するためであるが、このよう
に絶縁被供を施すと、それを施していないものよりも検
出精度が炒くなる憂いがある。
In this product, the metal H4 ball 3 is coated with an insulating coating 2 in order to prevent corona discharge or spark emission between the metal ball 3 and external strings or objects. There is a concern that if an insulating coating is applied, the detection accuracy will be worse than one without it.

これtt′izのような理由による。This is due to reasons such as tt'iz.

すなわち、絶縁被覆2を施すとそれに静寛容量か生じる
もので、この静電容魁をC,、静亀気検出ブローブ1の
アースされている円筒ケース(接地外筒)と金属球3と
の間のいわゆる浮遊容景をC,、金属球3とアース間の
漏洩抵抗をR,、放射紳N離作用によって集ml器と金
属球3との間の空間中に形成される電気回路の抵抗をR
2、集tIf.器人力抵抗を一定に保つだめの抵抗をR
3とすると、帯■物と集電器との間には第2図に示すよ
うな熔価回路が成立する。なお%V’Id:入力嘗位(
帯電電位)、Vol;i出力電位(集電器検出電位)で
ある。
That is, when the insulating coating 2 is applied, a static capacitance is generated, and this capacitance is C, between the grounded cylindrical case (grounded outer cylinder) of the static glide detection probe 1 and the metal ball 3. Let the so-called floating appearance of R
2, Collection tIf. R is the resistance that keeps the resistance constant.
3, a melting circuit as shown in FIG. 2 is established between the band and the current collector. Note that %V'Id: Input position (
charging potential), Vol; i output potential (current collector detection potential).

この等価回路から明らかなように、絶縁被p2Kよって
静電容量CIが生じると、回路の時定数が変り、vOの
出力特性が変化、すなわち帯電電位に対する集L{.器
の応答性が恕〈なる。
As is clear from this equivalent circuit, when the capacitance CI is generated by the insulation p2K, the time constant of the circuit changes, and the output characteristics of vO change, that is, the concentration L{. The responsiveness of the instrument becomes worse.

本発印j者らは、これを改善すべく種々の試験研究を重
ね、次のような実験結果から、絶縁被發2を施してあっ
てもそれを施さないものと同様の出力特性を生じさせる
ことが可能であることをつきとめ、このことから、絶縁
被留を施したことによる上記のような不利を簡単K補償
できる本発明を案出したものである。
In order to improve this, the authors have conducted various tests and research, and based on the following experimental results, they have found that even with insulation sheathing 2, the same output characteristics as those without it are produced. Based on this finding, the present invention has been devised to easily compensate for the disadvantages described above due to the use of insulating sheathing.

すなわち、本発明者らは、絶縁被覆2を施した第1図の
栴造のもの(以下には絶縁被覆球という)と、これを施
さないことが第1図のものと相違するのみでその他につ
いてはそれと実質的に同じ構成のもの(以下には裸球と
いう)とをつくり、絶縁被粗球には、その金屈球3に、
第3図のキt価回路に示すように抵抗値の高い接地され
た抵抗(接地抵抗)RCを積極的に接続し”’Cソノ値
ヲ10”Q+10”Q,10”Qと変え、他方外球には
これを接続しないでそのままにして、これら画球を同じ
所定の電位まで帯軍1させたのち、両者の静電気検出グ
ローブの出力をそれぞれ測定した。
In other words, the present inventors have developed the SEIZO bulb shown in FIG. 1 which is coated with insulation coating 2 (hereinafter referred to as the insulation coating bulb), and the one shown in FIG. 1 which is different from the one shown in FIG. For this, we made a ball with substantially the same configuration as that (hereinafter referred to as a bare ball), and for the insulated ball, we added the following:
As shown in the circuit of Figure 3, a grounded resistor (earthed resistance) RC with a high resistance value is actively connected, and the value is changed to 10Q+10Q, 10Q, and the other The outer sphere was left unconnected and these spheres were charged to the same predetermined potential, and then the outputs of both static electricity detection gloves were measured.

第4図はその出力特性(所定電位帯電後の電荷の移動に
よる減衰推移)を示すもので、X印のついた曲線か絶縁
被覆球の出力、○印のついた曲紳が裸球の出力をそれぞ
れ示している。
Figure 4 shows the output characteristics (attenuation transition due to charge movement after charging at a given potential). are shown respectively.

この図から分かるように、絶縁被1&球の出力特性は接
地抵抗R《の抵抗値によって変化し、接地抵抗R′lが
101jQの場合に裸球の出力特性とほP1等しくなっ
ている。
As can be seen from this figure, the output characteristics of the insulating sheath 1 and the bulb change depending on the resistance value of the grounding resistance R<<, and when the grounding resistance R'l is 101jQ, the output characteristics of the bare bulb are almost equal to P1.

このことは、接地抵抗Bl,の値を適当に選び、回路の
時定数を、静電容鍛C,かないもの(裸球)と同じにす
れば、裸球と同じ出力特性がえられることを照明してい
る。
This clearly shows that if the value of the grounding resistance Bl is chosen appropriately and the time constant of the circuit is made the same as that of a bare bulb (bare bulb), the same output characteristics as a bare bulb can be obtained. are doing.

従って、第1図の絶縁被投球において、その金属球3に
接地抵抗R′8を接続してその値を訓整するようにすれ
ば、該絶縁被拉球の検出精度を裸球と同等にすることが
できることになる。
Therefore, in the case of the insulated hit ball shown in Fig. 1, if the ground resistance R'8 is connected to the metal ball 3 and its value is adjusted, the detection accuracy of the insulated hit ball can be made equal to that of a bare ball. You will be able to do so.

しかし、その接地抵抗は、上記から明らかなように、1
012〜1011Ωという高い値でないと出力特性を調
整できないもので、その値を加減して同じ検出精度のも
のを大斌生産することは現実には非常に難しい。
However, as is clear from the above, the ground resistance is 1
The output characteristics cannot be adjusted unless the value is as high as 012 to 1011 ohms, and it is actually very difficult to adjust this value and produce products with the same detection accuracy.

しかして、本発明者らは、第2図の等価回路において、
抵抗R,(放射線電離作用によって形成される電気回路
の抵抗)によってもその回路の時定数の調整を行うこと
かできる、ということを実験で確め、この抵抗R,を調
整することができる手段を、導電中空体(第1図におい
ては金属球3がこれに相当)内に備えることにより、裸
球と同じ検出精度のものを簡単につくることがてきる本
発明を案出したものである。
Therefore, in the equivalent circuit shown in FIG.
It was confirmed through experiments that the time constant of the circuit can also be adjusted by the resistance R (resistance of an electric circuit formed by the action of radiation ionization), and a means for adjusting this resistance R. The present invention has been devised in which it is possible to easily create the same detection accuracy as a bare bulb by providing a conductive hollow body (corresponding to the metal ball 3 in Fig. 1). .

以下には本発明を第5図に示す実施例について詳細に説
明する。
The present invention will be described in detail below with reference to the embodiment shown in FIG.

本静電気検出器は、椀状の金属製、例えばアルミニウム
製導電中空体4の外周面(半球向)に、薄い(厚さ0.
5〜0.8m)絶緑被橢5を施すとともに、その導電中
空休4の上面開口を肉厚円盤状の絶縁支持台6にて閉塞
し、この絶縁支持台6に集箪式静電気検出プローブ7を
支持している。
This static electricity detector has a thin (thickness of 0.5 mm) on the outer peripheral surface (in the hemisphere direction) of a bowl-shaped conductive hollow body 4 made of metal, for example, aluminum.
5 to 0.8 m) A green cover 5 is applied, and the top opening of the conductive hollow hole 4 is closed with a thick disc-shaped insulating support 6, and a collection type static electricity detection probe is attached to this insulating support 6. 7 is supported.

絶縁被覆5及ひ絶緑支持台6には、高給縁でしかも耐油
性のよい合成梱脂を用いるとよい。
For the insulation coating 5 and the green support base 6, it is preferable to use synthetic bale lubricant that has high coverage and good oil resistance.

木例においては、絶縁被嬉5の利賀がエポキシ系熱硬化
性樹脂、絶縁支持台6の材質がガラス繊維入りエポキシ
樹脂CF.R.P.)になっている。
In the wooden example, the material of the insulation support 5 is epoxy thermosetting resin, and the material of the insulation support 6 is glass fiber-containing epoxy resin CF. R. P. )It has become.

絶縁支持台6は、その雄ねじ8を導電中空体4の雌ねじ
9に螺合することにより導電中空体4の上面開口を液密
に閉塞している。従って、導電中空体4内は液密空間1
0になっている。
The insulating support base 6 liquid-tightly closes the upper opening of the conductive hollow body 4 by screwing its male screw 8 into the female screw 9 of the conductive hollow body 4 . Therefore, the inside of the conductive hollow body 4 is a liquid-tight space 1.
It is 0.

導電中空体4の内面であって液密空間10の底面11は
、尖鋭部分のない水平な平面になつている。液密空間1
0の他の面も尖鋭部分のない平滑面になっている。
The bottom surface 11 of the liquid-tight space 10, which is the inner surface of the conductive hollow body 4, is a horizontal plane without sharp parts. Liquid-tight space 1
The other surface of 0 is also a smooth surface with no sharp parts.

静電気検出プローブ7は、金属製の円筒ケース(接地外
筒)12内において、絶縁支持体13に集電器14を支
持するとともに回路基板15に出力回路を実装し、さら
にこの出力回路を結合抵抗16を介し集電器14に接続
するとともに、集電器l4を高抵抗17を介し円筒ケー
ス12に接続したものである。集電器l4には、放射性
物質であるアメリシウムAm241(8.8μCt)が
内蔵されている。集電器14によってえもれた検出信号
は、出力回路によって増幅及びインピーダンス変換され
たのち、この出力回路に接続したケーブルl8によって
外部出力される。
The static electricity detection probe 7 has a current collector 14 supported on an insulating support 13 and an output circuit mounted on a circuit board 15 in a metal cylindrical case (grounded outer cylinder) 12, and furthermore, this output circuit is connected to a coupling resistor 16. The current collector l4 is connected to the cylindrical case 12 via a high resistance 17. The current collector l4 contains americium Am241 (8.8 μCt), which is a radioactive substance. The detection signal leaked by the current collector 14 is amplified and impedance-converted by the output circuit, and then outputted to the outside via a cable 18 connected to this output circuit.

かかる朽造の静電気検出プロープ7は、その円筒ケース
12を絶縁支持台6の中央の取付孔19に上下摺動可能
に下向きに挿着してあり、アメリシウムよりの放射線(
α線)が液密空間10の底面11に真直ぐ照射されるよ
うになつているとともに、取付孔19に対する円筒ケー
ス12の挿着位置を上下調整することにより、集電器1
4と底面11との間の距離を調整できるようになってい
る。取付孔19に対する円筒ケース12の上下摺動は、
取付孔19の上端開口経に形成10四部20に嵌めたパ
ッキン21によって規制されている。
This dilapidated static electricity detection probe 7 has its cylindrical case 12 inserted downward into the mounting hole 19 at the center of the insulating support base 6 so as to be able to slide up and down.
The current collector 1
4 and the bottom surface 11 can be adjusted. The vertical sliding of the cylindrical case 12 with respect to the mounting hole 19 is as follows:
It is regulated by a packing 21 fitted into the four parts 20 formed at the upper end opening of the mounting hole 19 .

円筒ケース12の上輝部は、取何孔19の上端開口より
突出しているものであるが、該上端部は、絶縁支持台6
の上面にパッキン22を介してねじ止めした絶縁材製の
保護リング23と、この保護リング23の上面にねじ止
めしたゴム等の弾性材質の蓋板24によって液密に覆わ
れている。保設リング23は本例の場合絶縁支持台6と
同じ材質である。
The upper bright part of the cylindrical case 12 protrudes from the upper end opening of the mounting hole 19, and the upper end part is connected to the insulating support base 6.
It is liquid-tightly covered by a protective ring 23 made of an insulating material screwed onto the upper surface of the protective ring 23 via a packing 22, and a lid plate 24 made of an elastic material such as rubber screwed onto the upper surface of the protective ring 23. In this example, the retaining ring 23 is made of the same material as the insulating support base 6.

絶縁支持台6の下面には、取付孔19に続く円錐台形の
放射口部25が形成され、円筒ケース12の先端開口(
下端開口)ねこの放射口部25の上端に位置している。
A truncated cone-shaped radiation opening 25 is formed on the lower surface of the insulating support base 6 and continues to the mounting hole 19.
(Lower end opening) Located at the upper end of the cat's radiation mouth portion 25.

この放射口部25内には、絶縁支持台6に比ベ絶縁性が
幾分劣る絶縁材質の漏斗状絶縁部材26を嵌め込んであ
る。本例の場合、この絶縁部拐26の材質はフェノール
樹脂になっており、ガラス繊維入りエポキシ樹脂製の絶
縁支持台6の抵抗率が10”Qanであるのに対し、絶
縁部拐26のそれは10”〜10I2QQ%になつてい
る。
A funnel-shaped insulating member 26 made of an insulating material whose insulating properties are somewhat inferior to that of the insulating support base 6 is fitted into the radiation opening 25 . In the case of this example, the material of the insulating part 26 is phenolic resin, and while the resistivity of the insulating support base 6 made of glass fiber-containing epoxy resin is 10"Qan, that of the insulating part 26 is 10” to 10I2QQ%.

円筒ケース12の下端開口部には、その開口面積を実質
的に小さくする金属製の絞り板27が着脱自在に螺着さ
れている。この紋り板27はその中央に絞り孔28を開
設している。
A metal diaphragm plate 27 is removably screwed onto the lower end opening of the cylindrical case 12 to substantially reduce the opening area. This crest plate 27 has an aperture hole 28 in its center.

しかして、集電器14内のアメリシウムより放射された
α線は液密空間10の底面11に照射され、これら集電
器14と底面11との間の空間が電離されてそれらの間
に電気回路が形成される。この電気回路の抵抗RS(本
静電気検出器の等価回路を第6図に示す)は、集電器1
4と底面11との間の距離tによって左右され、tが大
きくなるとR!も大きくなり、tが小さくなるとR,も
小さくなる。従って、取付孔19に対する円筒ケース1
2の挿着位置を上下調整することによりI6を調整でき
、従ってまた等価回路の時定数を調整できるもので、円
筒ケース120挿着位置を適当に選ぶことにより、絶縁
被宥5を施さないものと同じような出力特性にすること
ができる。また、上記電離作用は、絞り板27によって
弱められ、その弱められた分だけ第6図の哨価回路中の
抵抗R,が高くなる。その弱められる度合は、絞り孔2
8の大きさと関係しており、これが小さければ小さいほ
ど弱められる度合が強くなる。従って、絞り孔28の大
きさの異なる絞り板27を複数枚用意しておいて交換使
用するようにすれば、抵抗R,を調整でき、従ってまた
測定電位の範囲を調整(いわゆるレンジ切候)できる。
Therefore, the α rays emitted from the americium in the current collector 14 are irradiated onto the bottom surface 11 of the liquid-tight space 10, and the space between the current collector 14 and the bottom surface 11 is ionized, and an electric circuit is formed between them. It is formed. The resistance RS of this electric circuit (the equivalent circuit of this static electricity detector is shown in Fig. 6) is the current collector 1.
4 and the bottom surface 11, and as t increases, R! also becomes larger, and as t becomes smaller, R also becomes smaller. Therefore, the cylindrical case 1 for the mounting hole 19
By vertically adjusting the insertion position of the cylindrical case 120, I6 can be adjusted, and therefore the time constant of the equivalent circuit can also be adjusted.By appropriately selecting the insertion position of the cylindrical case 120, the insulation cover 5 is not applied. It is possible to achieve output characteristics similar to Further, the ionization effect is weakened by the aperture plate 27, and the resistance R in the circuit of FIG. 6 increases by the weakened amount. The degree of weakening is determined by the aperture hole 2
8, and the smaller the value, the stronger the degree of weakening. Therefore, by preparing a plurality of aperture plates 27 with different sizes of aperture holes 28 and using them interchangeably, the resistance R can be adjusted, and therefore the range of measurement potential can also be adjusted (so-called range adjustment). can.

なお、この絞り板27によっても抵抗R,は少しく変化
する。
Note that the resistance R changes slightly depending on the diaphragm plate 27 as well.

液蕾空間lOの全内周面は尖鋭部分のない平滑面になっ
ているので、このなかにおいてコロナ放電あるいは火花
放電が生ずることはなく、またその底面11は平面にな
っているので、α線を平均に照射することができ、導電
中空体4に誘導された静電気を集電器14に正確に集電
できる。
Since the entire inner circumferential surface of the liquid bud space IO is a smooth surface with no sharp parts, no corona discharge or spark discharge will occur therein, and since the bottom surface 11 is flat, alpha rays will not be generated. can be irradiated evenly, and the static electricity induced in the conductive hollow body 4 can be accurately collected in the current collector 14.

さらに、静電気検出プロープ7の放射口の外周部、すな
わち絶縁支持台6の放射口部25の周りには、その絶縁
支持台6よりも抵抗率が低くて帯電しにくい材質の絶縁
部材26を設定してあるので、ここにおいて絶縁支持台
6が帯電して検出精度が悪くなるということはない。
Further, an insulating member 26 made of a material that has a lower resistivity than the insulating support 6 and is less likely to be charged is set around the outer periphery of the radiation port of the static electricity detection probe 7, that is, around the radiation port 25 of the insulating support 6. Therefore, there is no possibility that the insulating support base 6 is charged and the detection accuracy is deteriorated.

なお、上記実施例においては、絞り孔28の大きさが異
なる紋り板27を複数枚用意しておいて交換使用するこ
とにより抵抗R,を調整することができるようにしたが
、絞り孔の大きさを変えることができる可変式紋り板を
用いて調整するようにしてもよい。また、メッシュの5
1る報数枚の金網を交換使用(円筒ケース12の下端開
口に着脱自在に取り刊ける)して調整してもよい。
In the above embodiment, the resistance R can be adjusted by preparing a plurality of embossed plates 27 with different sizes of aperture holes 28 and using them interchangeably. Adjustment may be made using a variable crest plate whose size can be changed. Also, mesh 5
Adjustments may be made by replacing the number of pieces of wire mesh (detachably attached to the opening at the lower end of the cylindrical case 12).

叙上のように本発明静電気検出器は、放射線iI離作用
によって集電器と導電中空体との間の空間中に形成され
る電気回路の抵抗を調整することができる手段を、導電
中空体内に備えだので、絶縁被覆を施したことによる検
出精度上の不利を簡単に補償できる。
As described above, the electrostatic detector of the present invention includes a means in the conductive hollow body that can adjust the resistance of the electric circuit formed in the space between the current collector and the conductive hollow body by the radiation iI separating action. Since the sensor is equipped with an insulating coating, it is possible to easily compensate for the disadvantage in detection accuracy caused by applying an insulating coating.

また、特許請求の範囲第3項の実施態様のように、導電
中空体の内面であって放射紳を照射される部分を平面に
すれば、放射線を平均に照射することができ、sm.中
空体に誘導された静電気を隼亀器に正僅に集箪できる。
Further, as in the embodiment of claim 3, if the inner surface of the conductive hollow body and the portion that is irradiated with radiation is made flat, the radiation can be irradiated evenly, and the sm. The static electricity induced in the hollow body can be collected into the Hayabusa device.

さらに1特許請求の範囲第4項の発明のように、導電中
空体の内面と集電器との間に1孔を設けた金棒製の紋り
板あるいは金網を配置すれば、測定電位の範囲を簡単に
調整できる。
Furthermore, as in the invention of claim 4 of the first patent, by arranging a metal rod plate or wire mesh with one hole between the inner surface of the conductive hollow body and the current collector, the range of the measured potential can be widened. Easy to adjust.

さらにまた、特詐請求の範囲第5項の発明のように、絶
縁支持台の先端開口部の周辺に、該絶縁支持台よりも抵
抗率が低い絶縁部拐を付設すれは、上記周辺における帯
電を防止でき、検出精度を一層向上させることができる
Furthermore, as in the invention of Claim 5, if an insulating part having a lower resistivity than that of the insulating support is attached around the opening at the tip of the insulating support, the charge in the periphery can be reduced. can be prevented, and detection accuracy can be further improved.

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

図面第1図は従来例の断面図、第2図はその等価回路図
、第3図はその金属球に接地抵抗を接続した場合の等価
回路図、第4図は上記接地抵抗を接糺した従来例とそれ
における絶縁被覆を施さないお・±造のものとの出力特
性を比較するための実験測定データを示すグラフ、第5
図は本発明の一実施例を示す断面図、第6図はその等価
回路図である。 14・・・集電器、7・・・静電気検出プローブ、4・
・・導電中空体、27・・・紋り板、6・・・絶縁支持
台、26・・・絶縁部材。
Figure 1 is a sectional view of the conventional example, Figure 2 is its equivalent circuit diagram, Figure 3 is an equivalent circuit diagram when a grounding resistor is connected to the metal ball, and Figure 4 is a diagram when the above grounding resistor is connected. Graph 5 showing experimental measurement data for comparing the output characteristics of the conventional example and the manufactured one without insulation coating.
The figure is a sectional view showing an embodiment of the present invention, and FIG. 6 is an equivalent circuit diagram thereof. 14... Current collector, 7... Static electricity detection probe, 4.
... Conductive hollow body, 27... Crest plate, 6... Insulating support base, 26... Insulating member.

Claims (5)

【特許請求の範囲】[Claims] 1.放射性物体を有する集電器及び出力回路を備えた集
電式静電気検出プローブを、外面K薄い絶縁計8妃を施
した導電中空体に内蔵し、この導市、中空科に読導さJ
1た静電気を放射糾■?離作用によって集電器に集寛し
、その電位に応じた電気伯号を出力回路より出力するよ
うにしたWDm気検出器において、土配放射網・市離作
用Kよって上記集電器と上記導箪中空体との間の空間中
に形成される電気回路の抵抗をp多することができる手
段を、上記導電中空体内に備えてなることを特徴とする
静電気検出器。
1. A current-collecting electrostatic detection probe equipped with a current collector and an output circuit containing a radioactive object is built into a conductive hollow body with a thin insulation meter on the outer surface, and the probe is equipped with a conductive hollow body with a thin insulation meter on the outside.
1. Does it radiate static electricity? In a WDm air detector in which a current is collected in a collector by a separation action and an electric voltage corresponding to the potential is output from an output circuit, the current collector and the conductor are connected by a distribution radiation network and a separation action. A static electricity detector characterized in that the conductive hollow body is provided with means capable of increasing the resistance of the electric circuit formed in the space between the hollow body and the conductive hollow body.
2.抵抗を訓弊することができる手段が、静電気検出プ
ローブをその軸線方向K前後動可能に支持する部材であ
る特許精求の範囲第1項に記載のe和気哲・出器。
2. The device according to item 1 of the scope of the patent application, wherein the means capable of reducing resistance is a member that supports the static electricity detection probe so that it can move back and forth in the axial direction K.
3.導甫1中空体の内面であって放射紳を照射される部
分を平面にしてなることを特徴とする特許請求の範囲第
1項に記載の静電気検出器。
3. 2. The electrostatic detector according to claim 1, wherein the inner surface of the hollow body of the electrostatic conductor 1, which is irradiated with the radiation, is made flat.
4.放射性物体を有する集電器及び出力回路を備えた集
電式静電気検出プローブを、外面に薄い絶縁被橢を施し
た導瞥,中空体に内蔵し、この導電中空体に誘導された
静電気を放射#電離作用Kよって集Wi1器に集電し、
その電位に応じた電気信号を出力回路より出力するよう
にした静電,気検出器において、上記放射紳電離作用に
よって上記集iIi器と上記導電中空付との間の空間中
に形成される電気回路の抵抗を訃1整ずることができる
手段を、上記導電中空体内に備えるとともK1この導軍
,中空体の内1h1と土記集電器との間に、孔を設けた
金属製の絞り板あるいは金網を配置してなることを特徴
とする静電気検出器。
4. A current-collecting static electricity detection probe equipped with a current collector and an output circuit containing a radioactive object is built into a conductive hollow body with a thin insulating coating on the outer surface, and the static electricity induced in this conductive hollow body is radiated. Current is collected in the collector Wi1 by the ionization effect K,
In an electrostatic detector configured to output an electrical signal according to the potential from an output circuit, electricity is generated in the space between the collector IIIi and the conductive hollow due to the radiation ionization action. A means capable of adjusting the resistance of the circuit is provided in the conductive hollow body, and a metal aperture with a hole is provided between the conducting force, 1h1 of the hollow body, and the current collector. A static electricity detector characterized by being formed by arranging plates or wire mesh.
5.放射性物体を有する集電,器及ひ出力回路を備えた
集電式静N1気検出プローブを、外面に薄い絶縁被覆を
施した導電中空体に内蔵し、この導電中空体に誘導され
たー静電気を放射線電離作用によって集電器K集電し、
その電位に応じた電気信号を出力回路より出力するよう
にした静電気検出器において、上記放射糾電離作用によ
って上記集電器と上記導亀中空体との間の空間中に形成
される電気(ロ)路の抵抗を訓整することができる手段
を、上記導電中空体内に備えるとともに、上JC,静電
気枦出プローブを、絶縁支持台によって導電中空体に支
持し、この絶縁支持台の内側面であってtp亀気検出プ
ローブの先端開口部の周辺に、該絶縁支持台よりも抵抗
率が低い絶縁部材を付設してなることを特徴とする静電
気検出器。
5. A current-collecting static N1 gas detection probe equipped with a current collector, a device, and an output circuit containing a radioactive object is built into a conductive hollow body with a thin insulation coating on the outer surface, and the static electricity induced in this conductive hollow body is is collected by the current collector K by the action of radiation ionization,
In a static electricity detector configured to output an electrical signal from an output circuit according to the electric potential, electricity (b) is formed in the space between the current collector and the conducting turtle hollow body by the radiation ionization effect. The conductive hollow body is provided with means for adjusting the resistance of the conductive conductor, and the upper JC and the electrostatic discharge probe are supported on the conductive hollow body by an insulating support, and the inner surface of the insulating support is An electrostatic detector characterized in that an insulating member having a lower resistivity than the insulating support base is attached around the tip opening of the tp glans detection probe.
JP18909082A 1982-10-29 1982-10-29 Static electricity detector Granted JPS5979861A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18909082A JPS5979861A (en) 1982-10-29 1982-10-29 Static electricity detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18909082A JPS5979861A (en) 1982-10-29 1982-10-29 Static electricity detector

Publications (2)

Publication Number Publication Date
JPS5979861A true JPS5979861A (en) 1984-05-09
JPS6365907B2 JPS6365907B2 (en) 1988-12-19

Family

ID=16235157

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18909082A Granted JPS5979861A (en) 1982-10-29 1982-10-29 Static electricity detector

Country Status (1)

Country Link
JP (1) JPS5979861A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006126285A1 (en) * 2005-05-27 2006-11-30 Hugle Electronics Inc. Ion control sensor

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01161518U (en) * 1988-06-27 1989-11-09

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006126285A1 (en) * 2005-05-27 2006-11-30 Hugle Electronics Inc. Ion control sensor

Also Published As

Publication number Publication date
JPS6365907B2 (en) 1988-12-19

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