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JPS6152469B2 - - Google Patents
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JPS6152469B2 - - Google Patents

Info

Publication number
JPS6152469B2
JPS6152469B2 JP54066065A JP6606579A JPS6152469B2 JP S6152469 B2 JPS6152469 B2 JP S6152469B2 JP 54066065 A JP54066065 A JP 54066065A JP 6606579 A JP6606579 A JP 6606579A JP S6152469 B2 JPS6152469 B2 JP S6152469B2
Authority
JP
Japan
Prior art keywords
charged
corona discharge
discharge electrode
charging
voltage
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.)
Expired
Application number
JP54066065A
Other languages
Japanese (ja)
Other versions
JPS55159463A (en
Inventor
Susumu Hiranuma
Kenichi Yamaguchi
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.)
Fujifilm Business Innovation Corp
Original Assignee
Fuji Xerox Co Ltd
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 Fuji Xerox Co Ltd filed Critical Fuji Xerox Co Ltd
Priority to JP6606579A priority Critical patent/JPS55159463A/en
Publication of JPS55159463A publication Critical patent/JPS55159463A/en
Publication of JPS6152469B2 publication Critical patent/JPS6152469B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】 本発明は被帯電面をコロナ放電により帯電する
コロナ帯電装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a corona charging device that charges a surface to be charged by corona discharge.

従来、この種のコロナ帯電装置としては開口部
を有するシールドケースにコロナ放電電極(コロ
ナワイヤ)を設けた帯電器を、そのシールドケー
スの開口部が被帯電面に対向するように配設させ
るとともにコロナ放電電極に電圧を印加してコロ
ナ放電させることによつて被帯電面を帯電するよ
うにしたものが知られている。
Conventionally, this type of corona charging device includes a charger in which a corona discharge electrode (corona wire) is provided in a shield case having an opening, and the shield case is arranged so that the opening faces the surface to be charged. A device is known in which a surface to be charged is charged by applying a voltage to a corona discharge electrode to cause corona discharge.

この構造であると、コロナ放電電極が劣化した
り、汚れたりすると被帯電面に帯電ムラが生じて
しまう。
With this structure, if the corona discharge electrode deteriorates or becomes dirty, uneven charging will occur on the surface to be charged.

そこで、この帯電ムラを防止するために従来よ
り、複数の帯電器を用いて帯電する方法、シール
ドケースの開口部巾を狭くしてコロトロンビーム
を均一にする方法、帯電器と被帯電面との距離を
大きくする方法等がなされている。
Therefore, in order to prevent this uneven charging, conventional methods include charging using multiple chargers, narrowing the opening width of the shield case to make the corotron beam uniform, and connecting the charger and the surface to be charged. Methods have been developed to increase the distance.

しかしながらこれらの方法は設置スペースが広
くなる、コロナ放電電極に印加するコロトロン電
源電圧を大きくしなければならない等の不具合を
有する上に、コロナ放電電極劣化、汚れによる帯
電ムラ防止の効果が充分でない等の不具合を有す
る。
However, these methods have disadvantages such as requiring a large installation space and requiring a large corotron power supply voltage to be applied to the corona discharge electrode, as well as being insufficiently effective in preventing charging unevenness due to deterioration of the corona discharge electrode and dirt. It has the following defects.

本発明は上記の事情に鑑みなされたものであ
り、その目的はコロナ放電電極劣化、汚れ等によ
つて生じる帯電ムラを確実に防止して被帯電面を
均一に帯電できるようにしたコロナ帯電装置を提
供することである。
The present invention was made in view of the above circumstances, and its purpose is to provide a corona charging device that reliably prevents charging unevenness caused by corona discharge electrode deterioration, dirt, etc., and can uniformly charge a surface to be charged. The goal is to provide the following.

以下図面を参照して本発明の実施例を説明す
る。
Embodiments of the present invention will be described below with reference to the drawings.

シールドケース1は絶縁性底壁2と一対の側壁
3,3と一対の端壁4,4とにより開口部1aを
有する長箱型状となり、該一対の端壁4,4に亘
つてコロナ放電電極となるコロトロンワイヤ5が
張設されて帯電器Aを構成している。
The shield case 1 has an insulating bottom wall 2, a pair of side walls 3, 3, and a pair of end walls 4, 4 to form a long box shape with an opening 1a, and corona discharge occurs across the pair of end walls 4, 4. A corotron wire 5 serving as an electrode is stretched to constitute a charger A.

前記絶縁性底壁2には複数の導電性プレート電
極6が相互に不連続に前記コロトロンワイヤ5の
軸方向(長手方向)に間隔を有して埋設してあ
り、該各導電性プレート電極6は抵抗素子7及び
受動型定電圧素子8より成り電流増加によりイン
ピーダンスが低下する可変インピーダンス素子1
3を介してそれぞれ接地してある。なお、受動型
定電圧素子8としてはツエナーダイオード又はバ
リスタ等が挙げられる。
A plurality of conductive plate electrodes 6 are discontinuously embedded in the insulating bottom wall 2 at intervals in the axial direction (longitudinal direction) of the corotron wire 5, and each conductive plate electrode 6 is a variable impedance element 1 consisting of a resistance element 7 and a passive type constant voltage element 8, whose impedance decreases as the current increases.
They are each grounded via 3. Note that the passive type constant voltage element 8 may be a Zener diode, a varistor, or the like.

そして、前記コロトロンワイヤ5は直流コロト
ロン電源9に接続されかつ開口部1aが導電層1
0、感光層11より成る被帯電部材12の被帯電
面12c(感光層表面)に対向するように配設し
てある。
The corotron wire 5 is connected to a DC corotron power source 9, and the opening 1a is connected to the conductive layer 1.
0, it is disposed so as to face the charged surface 12c (photosensitive layer surface) of the charged member 12 made of the photosensitive layer 11.

次に帯電動作原理について説明する。 Next, the principle of charging operation will be explained.

まずコロトロンワイヤ5のコロナ放電及び被帯
電面12aが帯電されるプロセスの等価回路は第
2図の如くとなる。
First, the equivalent circuit of the process of corona discharge of the corotron wire 5 and charging of the charged surface 12a is as shown in FIG.

すなわち、コロトロンワイヤ5に流れる直流電
流i0は、空気絶縁層(コロトロンワイヤ5と被帯
電面12aとの間の空気層)のインピーダンス2
0及び被帯電面12aのインピーダンス21を介
してアースに流れる直流電流i1と空気絶縁層(コ
ロトロンワイヤ5と底壁2との間の空気層)のイ
ンピーダンス22を介して接地された導電性シー
ルドケース1に流れる直流電流i2の和として考え
られる。
That is, the DC current i 0 flowing through the corotron wire 5 is determined by the impedance 2 of the air insulating layer (the air layer between the corotron wire 5 and the charged surface 12a).
0 and the DC current i 1 flowing to the ground through the impedance 21 of the charged surface 12a and the conductivity grounded through the impedance 22 of the air insulation layer (the air layer between the corotron wire 5 and the bottom wall 2). It can be considered as the sum of the DC current i 2 flowing through the shield case 1.

ここで、直流電流i0がコロトロンワイヤ5の劣
化、汚れ等による異常放電により△i0だけ増加し
た場合を考えると、直流電流i1,i2は各々△i1
△i2だけ増加し被帯電面12aの表面電位は△i1
によつて△Vだけ上昇する。
Here, if we consider the case where the DC current i 0 increases by △i 0 due to abnormal discharge due to deterioration, dirt, etc. of the corotron wire 5, the DC currents i 1 and i 2 will increase by △i 1 , respectively.
The surface potential of the charged surface 12a increases by △i 2 and the surface potential of the charged surface 12a increases by △i 1
It increases by △V.

上記△Vが従来のコロナ帯電装置に於ける帯電
ムラの原因である。
The above ΔV is the cause of charging unevenness in conventional corona charging devices.

しかし、本発明に係るコロナ帯電装置は第1図
に示す如く構成してあるから、前述の等価回路は
第3図に示す如くなる。
However, since the corona charging device according to the present invention is constructed as shown in FIG. 1, the above-mentioned equivalent circuit becomes as shown in FIG. 3.

第3図において、直流電流i0がある一定量以上
増加するとそれに伴なつて増加する直流電流i2
増加分△i2の為可変インピーダンス素子13にか
かる電圧が上昇し、その電圧がある一定以上の値
となるインピーダンスが抵下してゼロに近い値と
なり更に直流電圧i2はその可変インピーダンス素
子13のインピーダンス低下分だけ増加する。
In FIG. 3, when the DC current i 0 increases by more than a certain amount, the voltage applied to the variable impedance element 13 increases due to the increase △i 2 in the DC current i 2 , which increases at a certain level. The impedance having the above value decreases to a value close to zero, and furthermore, the DC voltage i 2 increases by the amount of the decrease in the impedance of the variable impedance element 13.

このために、上記インピーダンス低下による直
流電圧i2の増加分△i2′がコロトロンワイヤ5劣
化、汚れ等によつて生じる直流電圧i0の増加分の
帯電ムラに寄与する電流、すなわち直流電流i1
増加分△i1に等しくなるように可変インピーダン
ス素子13を設定すればコロトロンワイヤ5劣
化、汚れ等に起因する被帯電面12aの帯電ムラ
を防止することが可能である。
For this reason, the increase △i 2 ' in the DC voltage i 2 due to the impedance drop is a current that contributes to uneven charging due to the increase in the DC voltage i 0 caused by deterioration, dirt, etc. of the corotron wire 5, that is, the DC current. By setting the variable impedance element 13 so that the increase in i 1 is equal to Δi 1 , it is possible to prevent charging unevenness on the charged surface 12 a caused by deterioration of the corotron wire 5, dirt, etc.

つまり、コロトロンワイヤ5劣化、汚れ等によ
つて直流電圧i0はi0+△i0に、直流電圧i1はi1+△
i1に、直流電圧i2+△i2に変化するが、同時に可
変インピーダンス素子13のインピーダンスが変
化しこれによつて可変インピーダンス素子13に
はi2+△i2+△i2′の電流が流れる。この時△i2′=
△i1となるように可変インピーダンス素子13の
インピーダンスが変化していればi0がi0+△i0
なつても△i0=△i2+△i2′、△i1=0となつて被
帯電面12aに流れる電流を変化させない。
In other words, due to deterioration or dirt on the corotron wire 5, the DC voltage i 0 becomes i 0 +△i 0 , and the DC voltage i 1 becomes i 1 +△
i 1 , the DC voltage changes to i 2 +△i 2 , but at the same time the impedance of the variable impedance element 13 changes, so that a current of i 2 +△i 2 +△i 2 ' flows through the variable impedance element 13. flows. At this time △i 2 ′=
If the impedance of the variable impedance element 13 changes so that △i 1 , even if i 0 becomes i 0 + △i 0 , △i 0 = △i 2 + △i 2 ', △i 1 = 0 Therefore, the current flowing through the charged surface 12a is not changed.

したがつて、被帯電面12aの表面電位は異常
放電が生じても変化せずに帯電ムラを確実に防止
して均一に帯電できる。
Therefore, the surface potential of the surface to be charged 12a does not change even if an abnormal discharge occurs, and uneven charging can be reliably prevented and uniform charging can be achieved.

また、シールドケース1の絶縁性底壁2に複数
の導電性プレート電極6を設け、該電極6を可変
インピーダンス素子13を介して接地しただけの
構造であるから、構造簡単、コンパクトとなつて
狭いスペースにも設置できると共に、コロトロン
ワイヤ5の電源9を大きくする必要がない。
In addition, since the structure is simply that a plurality of conductive plate electrodes 6 are provided on the insulating bottom wall 2 of the shield case 1 and the electrodes 6 are grounded via the variable impedance element 13, the structure is simple, compact, and narrow. It can be installed in a small space, and there is no need to increase the size of the power source 9 for the corotron wire 5.

以上の実施例においてプレート電極6間の間隔
は経験的に1mm前後、プレート電極6の軸方向長
さは8〜12mmが適切である。
In the above embodiments, it has been empirically found that the appropriate distance between the plate electrodes 6 is approximately 1 mm, and the axial length of the plate electrodes 6 is 8 to 12 mm.

また、第4図に示す如くプレート電極6を平行
四辺形として図示のように配設すれば、コロナ放
電特性安定化に好ましくない電極(プレート電極
6)間の絶縁層(絶縁性底壁2)による影響が少
なくなる。
In addition, if the plate electrodes 6 are arranged in the form of a parallelogram as shown in FIG. The impact of

また、以上の各実施例ではいずれも絶縁性底壁
2(コロトロンワイヤ5背面)にプレート電極6
を設けたが、第5図に示す如く導電性物質により
成るU字形断面単位シールドケース1′をコロト
ロンワイヤ5軸方向に分割し、その間に絶縁層3
0を設けて連続してシールドケース自体を電極と
しても良い。
Further, in each of the above embodiments, the plate electrode 6 is provided on the insulating bottom wall 2 (the back surface of the corotron wire 5).
However, as shown in FIG. 5, a U-shaped cross-section unit shield case 1' made of a conductive material is divided in the 5-axis direction of the corotron wire, and an insulating layer 3 is placed between them.
0 may be provided and the shield case itself may be used as an electrode.

本発明は以上の様になり、コロナ放電電極の劣
化、汚れ等による帯電ムラを確実に防止して被帯
電面12aを均一に帯電できる。
As described above, the present invention reliably prevents charging unevenness due to deterioration, dirt, etc. of the corona discharge electrode, and can uniformly charge the surface to be charged 12a.

また、構造簡単、コンパクトで狭いスペースに
も設置でき、さらにはコロナ放電電極5の電源を
大きくする必要もない。
Furthermore, the structure is simple, compact, and can be installed in a narrow space, and there is no need to increase the power source of the corona discharge electrode 5.

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

第1図は本発明の実施例を示す断面説明図、第
2図、第3図はその動作説明図、第4図は他の実
施例を示す平面図、第5図は更に異なる他の実施
例を示す一部斜視図である。 1はシールドケース、5はコロナ放電電極、6
は導電性プレート電極、12aは被帯電面、13
は可変インピーダンス素子。
Fig. 1 is a cross-sectional explanatory diagram showing an embodiment of the present invention, Figs. 2 and 3 are explanatory diagrams of its operation, Fig. 4 is a plan view showing another embodiment, and Fig. 5 is a further different embodiment. It is a partial perspective view which shows an example. 1 is a shield case, 5 is a corona discharge electrode, 6 is a
12a is a conductive plate electrode, 12a is a charged surface, 13
is a variable impedance element.

Claims (1)

【特許請求の範囲】[Claims] 1 直流電圧が印加されるコロナ放電電極5を包
囲し被帯電面12aに対向する部位に開口部1a
を有するシールドケース1に、前記コロナ放電電
極5の軸方向について電気的に分割される複数の
導電性部分を設け、該各導電性部分と基準電位と
の間に、各導電性部分を通つて流れる電流増加に
よつてインピーダンスが低下するように抵抗7と
受動型定電圧素子8を直列接続して成る可変イン
ピーダンス素子13をそれぞれ接続したことを特
徴とするコロナ帯電装置。
1 An opening 1a is provided at a portion surrounding the corona discharge electrode 5 to which a DC voltage is applied and facing the charged surface 12a.
A plurality of conductive parts electrically divided in the axial direction of the corona discharge electrode 5 are provided in a shield case 1 having a A corona charging device characterized in that a variable impedance element 13 formed by connecting a resistor 7 and a passive constant voltage element 8 in series is connected to each of them so that the impedance decreases as the flowing current increases.
JP6606579A 1979-05-30 1979-05-30 Corona charger Granted JPS55159463A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6606579A JPS55159463A (en) 1979-05-30 1979-05-30 Corona charger

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6606579A JPS55159463A (en) 1979-05-30 1979-05-30 Corona charger

Publications (2)

Publication Number Publication Date
JPS55159463A JPS55159463A (en) 1980-12-11
JPS6152469B2 true JPS6152469B2 (en) 1986-11-13

Family

ID=13305072

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6606579A Granted JPS55159463A (en) 1979-05-30 1979-05-30 Corona charger

Country Status (1)

Country Link
JP (1) JPS55159463A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9726178B2 (en) 2012-02-14 2017-08-08 Pierburg Pump Technology Gmbh Mechanical coolant pump

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE2145268B2 (en) * 1971-09-10 1977-03-31 Hoechst Ag, 6000 Frankfurt CORONA DISCHARGE DEVICE

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9726178B2 (en) 2012-02-14 2017-08-08 Pierburg Pump Technology Gmbh Mechanical coolant pump

Also Published As

Publication number Publication date
JPS55159463A (en) 1980-12-11

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