JPH0398297A - Static electricity removing device - Google Patents

Static electricity removing device

Info

Publication number
JPH0398297A
JPH0398297A JP23606089A JP23606089A JPH0398297A JP H0398297 A JPH0398297 A JP H0398297A JP 23606089 A JP23606089 A JP 23606089A JP 23606089 A JP23606089 A JP 23606089A JP H0398297 A JPH0398297 A JP H0398297A
Authority
JP
Japan
Prior art keywords
static electricity
capacitor
energy
contact
contact terminals
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
Application number
JP23606089A
Other languages
Japanese (ja)
Inventor
Yasuo Murakami
村上 易男
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP23606089A priority Critical patent/JPH0398297A/en
Publication of JPH0398297A publication Critical patent/JPH0398297A/en
Pending legal-status Critical Current

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  • Elimination Of Static Electricity (AREA)

Abstract

PURPOSE:To eliminate a static electricity including positive charge and negative charge by providing a rectifying element directing the voltage application to a capacitor in a fixed direction in a device in which the static electricity generated between contact terminals in contact with a target material charged with static electricity is accumulated by the capacitor and released as an electric energy. CONSTITUTION:A capacitor C for accumulating and holding a voltage by the static electricity generated between contact terminals A, B in contact with a charged target material and an energy releasing means D for releasing the electric energy accumulated in the capacitor C are connected in parallel to each other through wirings 3, 4 between the contact terminals. A bridge circuit E having a rectifying element combined therewith is connected to a circuit leading a Zener diode 4a and the capacitor O. Even if the polarity of the static electricity is changed, the energy releasing action is never stopped by the inversion of the polarity, and the circuit of the capacitor C and energy releasing means D regularly repeats releasing, and the static electricity can most efficiently be eliminated.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、食品、化粧容器等の加工、充填工程、紙、フ
イルム、シート類の巻取、裁断工程、半導体の製造組み
立て工程、及び複写機、レコー1・盤等に生じる静電気
を除去する為の新規な静電気除去装置に関する。
Detailed Description of the Invention (Industrial Field of Application) The present invention is applicable to processing and filling of food and cosmetic containers, winding and cutting of paper, films, and sheets, manufacturing and assembly of semiconductors, and copying. This invention relates to a new static electricity removal device for removing static electricity generated on machines, records, discs, etc.

(従来の技術) 従来、静電気除去手段として、a)コロナ放電により正
負の両イオンを発生させ、そのイオン風を静電気を帯び
た対象物に送風し、その逆性のイオンを結合させること
で静電気を中和消滅させる方法、b)圧電性強誘導体を
基盤とする静電型交圧器の一次電極板を交流電源たる高
周波発信器に接続し、対向する二つの二次側電極板をそ
れ自体放電電極となして両電極間において放電を行なわ
せる方法、C)電導マットやアース線による方法等が実
効的手段として知られている。
(Prior art) Conventionally, as a means for removing static electricity, a) both positive and negative ions are generated by corona discharge, the ion wind is blown onto an object charged with static electricity, and the ions of the opposite polarity are combined to eliminate static electricity. b) Connect the primary electrode plate of an electrostatic AC converter based on a piezoelectric ferroconductor to a high-frequency oscillator that is an AC power source, and discharge the two opposing secondary electrode plates by themselves. Effective means include a method in which discharge is caused between both electrodes, and C) a method in which a conductive mat or a ground wire is used.

しかし、(a)の方法は、比較的高い電圧を印加するた
めイオン空気の外にオゾンや酸化窒素を併発し易く、又
、装置が大型となる欠点を有し、(b)の方法は、高周
波コロナ放電が極めて微弱であり、正負イオンの密度が
小さいため除電効果が劣り、且つ、圧電性強誘導体が高
価であるという欠点を夫々有している。そして、(a)
  (b)に共通ずる重大な欠点は、対象物に帯電した
正負の静電気に対し、送風するイオン風の正負の逆性イ
オンの量的組合せが必ずしも一致せず、どちらかに過不
足が生じ、中和されない静電気が一部に残留すると共に
、余ったイオンがその電磁気的極性のために新に対象物
に静電気を起こさせてしまうという問題が残る点である
。又、電導マット及びアース線は簡易的ではあるが、除
電が不充分である。
However, method (a) has the disadvantage that ozone and nitrogen oxides are likely to be generated in addition to ionized air because a relatively high voltage is applied, and the device becomes large. Each of these has disadvantages in that the high-frequency corona discharge is extremely weak, the density of positive and negative ions is low, so the static elimination effect is poor, and the piezoelectric ferroelectric material is expensive. and (a)
A serious drawback common to (b) is that the quantitative combination of positive and negative ions in the blown ion wind does not necessarily match the positive and negative static electricity charged on the object, resulting in excess or deficiency in one or the other. The remaining problem is that unneutralized static electricity remains in some parts, and the remaining ions cause new static electricity on the object due to their electromagnetic polarity. Further, although the conductive mat and the ground wire are simple, they are insufficient in eliminating static electricity.

(発明の解決しようとする課題) そこで、本発明者が実験を繰り返したところ、静電気は
対象物上に正の電荷と負の電荷とが局所的に混在してい
ることが多いという知見を得、この混在化した静電気を
過不足なく消滅させることが大切であり、本発明はこれ
を満足させる装置を開発せんとするものである。
(Problem to be Solved by the Invention) Therefore, the inventor of the present invention repeatedly conducted experiments and found that static electricity often consists of a local mixture of positive and negative charges on an object. It is important to eliminate just the right amount of mixed static electricity, and the present invention aims to develop a device that satisfies this requirement.

(課題を解決するための手段) 本発明静電気除去装置は、静電気を帯電した対象物と接
触する接触端子A,Bを配し、その接触端子間に生した
静電気による電圧を蓄狽保持するコンデン4J−Cと、
該コンデンサーCに帯植された電気エネルギーを放出す
るエネルキー放出手段Dとを並列に接続し、該コンデン
サー〇への電圧印加を一定方向にする整流素子を組み合
わせたブリッジ回路Eを端子間に接続したことを特徴と
して構成される。
(Means for Solving the Problems) The static electricity removing device of the present invention has contact terminals A and B that come into contact with an object charged with static electricity, and a capacitor that stores and retains the voltage due to the static electricity generated between the contact terminals. 4J-C and
An energy key release means D that releases the electric energy implanted in the capacitor C is connected in parallel, and a bridge circuit E is connected between the terminals, which is a combination of a rectifying element that applies voltage to the capacitor 〇 in a fixed direction. It is composed of the following characteristics.

(作用) 対象物に発生した静電気は、接触端子A,Bを通してコ
ンデンサーCに流れて蓄積保持され、これが一定電圧以
上になると放電し、並列に接続されたエネルギー放出手
段Dを作動させ、この結果、電気エネルギーの消耗によ
り静電気が消滅する。
(Function) The static electricity generated on the object flows through the contact terminals A and B to the capacitor C, where it is accumulated and held, and when it reaches a certain voltage or higher, it is discharged and activates the energy release means D connected in parallel. , static electricity disappears due to consumption of electrical energy.

そして、接触端子A,Bに負荷される電気極性が逆転し
たとき、整流素子を組み合わせたブリッジ回路Eが働き
、逆極性の電気も交差した通路から前と同一方向にコン
デンサー〇の回路に入り、コンデンサー〇を一定方向か
ら印加するように働き、コンデンサーC及びエネルキー
放出手段Dを最大効率で作用させる。
Then, when the polarity of the electricity loaded on the contact terminals A and B is reversed, the bridge circuit E, which is a combination of rectifying elements, is activated, and the electricity of the opposite polarity also enters the circuit of capacitor 〇 from the crossed path in the same direction as before. The capacitor 〇 works to apply voltage from a certain direction, and the capacitor C and the energy release means D work at maximum efficiency.

(実施例) 本発明の実施例を示した第1図に基づいて説明すれば、
A及びBが帯電した対象物に接触する接触端子で、その
対象物とは、プラスチック製品、印刷物、複写機、電子
部品絹み立てライン等の静電気除去が必要とされる凡ゆ
る対象物を指す。
(Example) An explanation will be given based on FIG. 1 showing an example of the present invention.
A and B are contact terminals that come into contact with a charged object, and the object refers to any object that requires static electricity removal, such as plastic products, printed matter, copying machines, electronic parts sewing lines, etc. .

この端子の配線1,2間に、生じた静電気による電圧を
蓄積保持するコンデンサーCと、該コンデンサーCに蓄
積された電気エネルギーを放出するエネルギー放出手段
Dとを配線3,4で並列に接続する。該コンデンサーC
は比較的容量が大であれば1個でも良いが、コンデンサ
ーの耐電圧を引き上げるため、3a,3b,3c,3d
と4直列に連結した。又、エネルギー放出手段Dは、前
記コンデンサーCに蓄積された電気エネルギーを放出さ
せるものであれば手段を問わないが、ツェナダイオード
4aによる他の電気エネルギーへの変換、ネオン管によ
る光エネルギーへの変換、抵抗による熱エネルギーへの
変換等がある。この中で、ツエナダイオート4aは、電
圧を一定として一5一 電流を変化させうるため、帯電量が変化する場合でもそ
の変化に合わせて通電量を適合できる点て優れる。又、
ネオン管によればエネルギー放出が視覚的に確認できる
Between the wirings 1 and 2 of this terminal, a capacitor C that stores and holds the voltage due to the generated static electricity, and an energy release means D that releases the electrical energy stored in the capacitor C are connected in parallel by wires 3 and 4. . The capacitor C
3a, 3b, 3c, 3d may be enough if the capacitance is relatively large, but in order to increase the withstand voltage of the capacitor, 3a, 3b, 3c, 3d
4 were connected in series. The energy release means D may be any means as long as it releases the electrical energy stored in the capacitor C, but may include conversion into other electrical energy by a Zener diode 4a, conversion into light energy by a neon tube, etc. , conversion into thermal energy through resistance, etc. Among these, the Zener die auto 4a is superior in that it can keep the voltage constant and vary the current, so even if the amount of charge changes, the amount of current can be adjusted in accordance with the change. or,
Neon tubes allow visual confirmation of energy release.

そして、このツエナダイオード4a及びコンデンサーC
に至る回路に、整流素子を組み合わせたブリッジ回路E
を接続するが、その詳細は、配線1,2間に分枝した配
線5及ひ6を交差させて結線し、配線1に順方向のダイ
オードla,lbを連結し、分校の配線5に逆方向のダ
イオード5a,5bを連結して、A端子から入力した静
電気を配線1を経て結線1x側から正に印加させるよう
する。そして、配線2に逆方向のダイオード2a,2b
を連結し、分校配線6に順方向の6a,6bを連結して
、B端子から入力した静電気を、逆方向のダイオード2
a,2bにより分枝した配線6側に流してA端子側の結
線1xから入力させ、逆方向に端子B側から入力した場
合にも前記と同様に結線IX側から正に印加させるよう
に構成する。
And this Zener diode 4a and capacitor C
Bridge circuit E that combines a rectifying element with the circuit leading to
The details are as follows: connect the branched wires 5 and 6 between wires 1 and 2, connect the forward direction diodes la and lb to the wire 1, and connect the reverse direction to the branch wire 5. The diodes 5a and 5b in the direction are connected so that the static electricity input from the A terminal is positively applied from the wiring 1x side via the wiring 1. Then, diodes 2a and 2b in the opposite direction are connected to the wiring 2.
6a and 6b in the forward direction are connected to the branch wiring 6, and the static electricity input from the B terminal is transferred to the diode 2 in the reverse direction.
It is configured so that it flows into the wiring 6 side branched by a and 2b and is input from the connection 1x on the A terminal side, and when it is input in the opposite direction from the terminal B side, it is applied positively from the connection IX side in the same way as above. do.

そして、配線1,2及び4に破壊電圧の入力を一6一 規制して整流素子等を保護するための抵抗1r,2r及
び4rを夫々直列に接続する。
Resistors 1r, 2r and 4r are connected in series to the wirings 1, 2 and 4, respectively, for regulating the input of breakdown voltage and protecting the rectifying elements and the like.

さて、上記のような構成において、対象物に静電気が帯
電した場合には、その接触端子A,Bを通じて本回路内
に静電気が入力し、比較的電圧が高い場合には、そのま
まツエナダイオーF’ 4 aに印加し、ツエナ電圧で
すダレ効果が惹起されて通電し、即ち静電気エネルギー
が他の電気エナルギー等に変換されて消滅する。又、ネ
オン管の場合は放電により紫外線および可視光線に変換
されて、抵抗の場合は熱に変換されて、静電気エネルギ
が消滅する。
Now, in the above configuration, if the object is charged with static electricity, the static electricity will be input into this circuit through the contact terminals A and B, and if the voltage is relatively high, it will be directly connected to the Zener diode F'4. When applied to a, the Zener voltage causes a sagging effect and conducts electricity, that is, the electrostatic energy is converted into other electrical energy and disappears. Further, in the case of a neon tube, the electrostatic energy is converted into ultraviolet rays and visible light by discharge, and in the case of a resistor, it is converted into heat, and the electrostatic energy is extinguished.

そして、静電気の帯電電圧がツエナダイオート゛4aの
ツエナ電圧より低い場合には、先ず、静電気はコンデン
サーC内に徐々に蓄積保持され、それが一定電圧以上に
なった場合に放電し、前記と同様ツエナダイオード4a
の通電で他の電気エネルギーに変換され消滅する。
When the charged voltage of static electricity is lower than the zener voltage of the zener die auto 4a, first, the static electricity is gradually accumulated and held in the capacitor C, and when it exceeds a certain voltage, it is discharged, and the zener die is discharged as described above. diode 4a
When energized, it is converted into other electrical energy and disappears.

このとき、ツエナダイオーF’ 4. aのツエナ電圧
におけるナダレ効果による通電量は、生した静電気の帯
電量に応して変化するので、帯電量が大の場合には多量
に小の場合には少量にと、通電量が自動的に調整され、
帯電量が一定しない対象物の場合にも静電気をきれいに
消滅させ得る。
At this time, Zena Daioh F' 4. The amount of energization due to the Nadare effect at the Zener voltage of a changes depending on the amount of static electricity generated, so the amount of energization is automatically changed to a large amount when the amount of static electricity is large and a small amount when the amount of electrification is small. adjusted to
Static electricity can be completely eliminated even when the amount of charge on an object is not constant.

ところで、通常上記作用で静電気問題は解消されると理
解されるが、本発明者が実験したところによると、静電
気は発生する対象物の面々で正負の極性が必ずしも一定
でなく、面上において正負の極性が局所的に混在してい
るため、一方だけの極性を除去しようとしたのでは、逆
極性になった場合その間エネルギー放出作用が停止し、
不完全なことが判明した。
By the way, it is generally understood that the static electricity problem is solved by the above action, but according to experiments conducted by the present inventor, the positive and negative polarity of static electricity is not necessarily constant on each surface of the object in which it is generated, and that the positive and negative polarities are different on the surface. Since the polarities of are mixed locally, if you try to remove only one polarity, if the polarity becomes reversed, the energy release action will stop during that time.
It turned out to be incomplete.

そこで、整流素子を組み合わせたブリッジ回路Eを接続
すると、例えばA端子側から正の電荷が加わっている場
合はそのまま結線1a側から印加されるが、これが一旦
B端子側に逆転した場合に本来反対側に移るものが、該
ブリッジ回路EによりB端子に人力した電流が逆方向の
ダイオー1・2a,2bに規制されて分枝した配線6に
流れ、順方向のダイオード6a,6bを経て反対側に至
り、前と同様の結線1x側からコンデンサーC等に印加
される。従って、・極性が変化した場合でも、その極性
の逆転によってエネルキー放出作用が停止する虞がなく
、コンデンサーC及ひエネルギー放出手段Dの回路は常
時放出を繰り返し、静電気を最も効率良く消滅させるこ
とができる。
Therefore, when connecting a bridge circuit E that combines rectifying elements, for example, if a positive charge is applied from the A terminal side, it will be applied as it is from the connection 1a side, but if it is reversed to the B terminal side, the opposite will originally be applied. The current applied to the B terminal by the bridge circuit E is regulated by the diodes 1, 2a and 2b in the opposite direction, flows to the branched wiring 6, and passes through the diodes 6a and 6b in the forward direction to the opposite side. , and is applied to capacitor C etc. from the 1x side of the same connection as before. Therefore, even if the polarity changes, there is no risk that the energy release action will stop due to the reversal of the polarity, and the circuit of the capacitor C and the energy release means D constantly repeats the release, making it possible to eliminate static electricity most efficiently. can.

(発明の効果) 以上のように、本発明によれば、静電気の帯電した対象
物に接触端子を接触させれば、コンデンサーとエネルギ
ー放出手段との絹み合わせて静電気のエネルギーを放散
させて消滅させることができ、且つ、正負の逆極性の静
電気が混在している場合でもブリッジ回路の連結でコン
デンサーとエネルギー放出手段に必ず一定方向に電圧を
印加させ、この効率を最大限に引き出すことができ、静
電気を完全に消滅させるという優れた効果がある。
(Effects of the Invention) As described above, according to the present invention, when a contact terminal is brought into contact with an object charged with static electricity, the electrostatic energy is dissipated and disappears due to the combination of the capacitor and the energy emitting means. Furthermore, even when static electricity of opposite polarity (positive and negative) coexists, by connecting the bridge circuit, the voltage can always be applied to the capacitor and the energy release means in a fixed direction, and this efficiency can be maximized. It has the excellent effect of completely eliminating static electricity.

そのとき、静電気が局部的に残ることや、逆に新たな静
電気の発生原因を併発させてしまうという虞もなく、過
不足なくこれを一掃できる。
At that time, there is no risk that static electricity will remain locally or that new causes of static electricity will occur, and it can be wiped out in just the right amount.

又、接触端子に上記回路を組み込めば良いから、装置が
コンパクトで、装着に当たってもアースのような埋設の
手間が要らず簡便であるというイ」股上の効果もある。
Furthermore, since the above-mentioned circuit can be incorporated into the contact terminal, the device is compact, and there is also the added advantage that installation is simple and does not require the trouble of burying the device, such as grounding.

更に、エネルギー放出手段にツエナダイオートを用いれ
ば、対象物の静電気帯電量が経時的に変化する場合にも
柔軟に対応できる点て優れる。
Furthermore, if a Zener diode is used as the energy emitting means, it is advantageous in that it can flexibly respond to changes in the amount of electrostatic charge on the object over time.

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

図面は本発明の一実施例を示す回路図である。 A,B・・・接触端子  C・・・コンデンサD・・・
エネルギー変換手段  E・・・ブリッジ回路
The drawing is a circuit diagram showing an embodiment of the present invention. A, B...Contact terminal C...Capacitor D...
Energy conversion means E...Bridge circuit

Claims (1)

【特許請求の範囲】 1)静電気を帯びた対象物と接触する接触端子A、Bを
配し、 その接触端子間に生じた静電気による電圧を蓄積保持す
るコンデンサーCと、該コンデンサーCに蓄積された電
気エネルギーを放出するエネルギー放出手段Dとを並列
に接続し、 該コンデンサーCへの電圧印加を一定方向にする整流素
子を組み合わせたブリッジ回路Eを端子間に接続したこ
とを特徴とする静電気除去装置。 2)エネルギー放出手段Dが、ツェナダイオードである
特許請求の範囲第1項記載の静電気除去装置。
[Claims] 1) Contact terminals A and B that come into contact with an object charged with static electricity are arranged, and a capacitor C that stores and holds the voltage due to the static electricity generated between the contact terminals, and a capacitor C that stores and holds the voltage due to the static electricity generated between the contact terminals, and A bridge circuit E, which is connected in parallel with an energy emitting means D that emits electrical energy, and a bridge circuit E that combines a rectifying element that applies voltage to the capacitor C in a fixed direction, is connected between the terminals. Device. 2) The static electricity eliminator according to claim 1, wherein the energy emitting means D is a Zener diode.
JP23606089A 1989-09-12 1989-09-12 Static electricity removing device Pending JPH0398297A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23606089A JPH0398297A (en) 1989-09-12 1989-09-12 Static electricity removing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23606089A JPH0398297A (en) 1989-09-12 1989-09-12 Static electricity removing device

Publications (1)

Publication Number Publication Date
JPH0398297A true JPH0398297A (en) 1991-04-23

Family

ID=16995140

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23606089A Pending JPH0398297A (en) 1989-09-12 1989-09-12 Static electricity removing device

Country Status (1)

Country Link
JP (1) JPH0398297A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
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JP2015197942A (en) * 2014-03-31 2015-11-09 日本電産サンキョー株式会社 Electronic equipment device
JP2023097362A (en) * 2021-12-27 2023-07-07 一般社団法人日本アーシング協会 Human body static electricity removal system with situational response function
JP2023126133A (en) * 2022-02-28 2023-09-07 一般社団法人日本アーシング協会 Static electricity elimination system

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015197942A (en) * 2014-03-31 2015-11-09 日本電産サンキョー株式会社 Electronic equipment device
JP2023097362A (en) * 2021-12-27 2023-07-07 一般社団法人日本アーシング協会 Human body static electricity removal system with situational response function
JP2023126133A (en) * 2022-02-28 2023-09-07 一般社団法人日本アーシング協会 Static electricity elimination system

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