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JPH0410430B2 - - Google Patents
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JPH0410430B2 - - Google Patents

Info

Publication number
JPH0410430B2
JPH0410430B2 JP57119171A JP11917182A JPH0410430B2 JP H0410430 B2 JPH0410430 B2 JP H0410430B2 JP 57119171 A JP57119171 A JP 57119171A JP 11917182 A JP11917182 A JP 11917182A JP H0410430 B2 JPH0410430 B2 JP H0410430B2
Authority
JP
Japan
Prior art keywords
electrode
hole
ion flow
aperture
aperture electrode
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 - Lifetime
Application number
JP57119171A
Other languages
Japanese (ja)
Other versions
JPS5911258A (en
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 filed Critical
Priority to JP11917182A priority Critical patent/JPS5911258A/en
Publication of JPS5911258A publication Critical patent/JPS5911258A/en
Publication of JPH0410430B2 publication Critical patent/JPH0410430B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G15/00Apparatus for electrographic processes using a charge pattern
    • G03G15/22Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20
    • G03G15/32Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20 in which the charge pattern is formed dotwise, e.g. by a thermal head
    • G03G15/321Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20 in which the charge pattern is formed dotwise, e.g. by a thermal head by charge transfer onto the recording material in accordance with the image
    • G03G15/323Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20 in which the charge pattern is formed dotwise, e.g. by a thermal head by charge transfer onto the recording material in accordance with the image by modulating charged particles through holes or a slit

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Dot-Matrix Printers And Others (AREA)
  • Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)
  • Electrophotography Using Other Than Carlson'S Method (AREA)

Description

【発明の詳細な説明】 この発明は、記録の制御電圧は低く、中間調記
録が可能であり、かつ記録速度の速い静電記録用
静電潜像書きこみ装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electrostatic latent image writing device for electrostatic recording that uses a low recording control voltage, is capable of halftone recording, and has a high recording speed.

第1図は従来この種の静電記録用静電潜像書き
こみ装置の説明図であつて、1はコロナイオン発
生のためのワイヤ、2はイオン流を制御するため
のアパーチヤ電極、3はイオン流を制御するため
の電圧発生回路、4はイオン流、5はコロナ荷電
器である。アパーチヤ電極2の構成は、絶縁板2
1に穴22をあけ、一方の面に電極23、他方の
面に電極24が設けられ、両電極23,24とも
穴22に一致する穴が形成されている。そして電
極23,24間に電圧発生回路3の電圧が印加さ
れる。なお、穴22はワイヤ1の長さ方向に沿つ
て多数形成されており、電極23は1枚の導電板
に穴22に合わせて穴を形成したものを用い、電
極24の方は各穴22の周囲を囲むようにして、
互に独立して設けられ、それぞれの電極23,2
4に電圧発生回路3の電圧が印加される。
FIG. 1 is an explanatory diagram of a conventional electrostatic latent image writing device for electrostatic recording of this type, in which 1 is a wire for generating corona ions, 2 is an aperture electrode for controlling the ion flow, and 3 is an aperture electrode for controlling the ion flow. A voltage generating circuit for controlling the ion flow, 4 is an ion flow, and 5 is a corona charger. The structure of the aperture electrode 2 is as follows:
A hole 22 is made in 1, an electrode 23 is provided on one surface, and an electrode 24 is provided on the other surface, and both electrodes 23 and 24 have holes that correspond to the holes 22. Then, the voltage of the voltage generating circuit 3 is applied between the electrodes 23 and 24. Note that a large number of holes 22 are formed along the length direction of the wire 1, and the electrode 23 is formed by forming holes in a single conductive plate to match the holes 22, and the electrode 24 is formed in each hole 22. so as to surround it,
Each electrode 23, 2 is provided independently from the other.
The voltage of the voltage generating circuit 3 is applied to the voltage generating circuit 4.

上記従来の装置は、このようにイオン流4のア
パーチヤ電極2で制御し、そのイオン流4により
静電潜像を形成し記録を行つていたので、コロナ
により発生するイオン流4は密度が少ないため、
記録速度が遅いという欠点があつた。
In the conventional device described above, the ion flow 4 is controlled by the aperture electrode 2, and an electrostatic latent image is formed and recorded by the ion flow 4, so the ion flow 4 generated by the corona has a low density. Because there are few
The drawback was that the recording speed was slow.

この発明は、これらの欠点を解決するため、ア
パーチヤ電極とコロナイオン発生源の間に、アパ
ーチヤ電極に対応して穴のあいた電極を配置し、
イオン流がアパーチヤー電極に収束するような電
位を印加したものであり。以下、図面についてこ
の発明を説明する。
In order to solve these drawbacks, this invention arranges an electrode with a hole corresponding to the aperture electrode between the aperture electrode and the corona ion generation source,
A potential is applied that causes the ion flow to converge on the aperture electrode. The invention will now be explained with reference to the drawings.

第2図はこの発明の一実施例であつて、6はイ
オン流収束用電源、7は前記イオン流の収束用電
極あり、中央には穴71が形成されている。この
穴71の数は穴22の数と同じで、中心を合わせ
てあり、穴22の直径φaに対し、穴71の直径
φbは大略2倍位にとつてある。その他は第1図
と同じである。
FIG. 2 shows an embodiment of the present invention, in which reference numeral 6 denotes a power source for converging the ion flow, 7 an electrode for converging the ion flow, and a hole 71 formed in the center. The number of holes 71 is the same as the number of holes 22, and their centers are aligned, and the diameter φ b of the holes 71 is approximately twice as large as the diameter φ a of the holes 22. Other details are the same as in Figure 1.

これを動作するには、ワイヤ1の高電圧を印加
し、イオン流4を生じさせる。流れ出してきたイ
オン流4を収束用電極7により収束させイオン密
度を高め、イオン制御のアパーチヤ電極2に導
く。
To operate it, a high voltage on the wire 1 is applied, causing an ion flow 4. The flowing ion stream 4 is focused by a focusing electrode 7 to increase ion density, and is guided to an aperture electrode 2 for ion control.

アパーチヤ電極2においては、制御信号により
イオン通過順方向電界が電極23と24により穴
22内に形成されている場合はイオン流4か通過
でき、また、逆に制御信号によりイオン通過逆方
向電界が形成されている場合はイオン流4が阻止
される。
In the aperture electrode 2, if a forward electric field for passing ions is formed in the hole 22 by the electrodes 23 and 24, the ion stream 4 can pass, and conversely, a reverse electric field for passing ions is established by the control signal. If so, the ion flow 4 is blocked.

上記に説明したように、イオン流4を収束用電
極7により収束してアパーチヤ電極2に導き、こ
のアパーチヤ電極2によりイオン流4の通過を制
御しているので、イオン流4中のイオン密度が増
大し、記録速度を速くすることができる。また、
イオン流制御法の利点である制御電圧が低くてよ
い点及び電極と被書きこみ部の距離の精度が厳し
くない点はそのまま保持されている。
As explained above, since the ion flow 4 is focused by the focusing electrode 7 and guided to the aperture electrode 2, and the passage of the ion flow 4 is controlled by the aperture electrode 2, the ion density in the ion flow 4 is This increases the recording speed. Also,
The advantages of the ion flow control method, such as the fact that the control voltage can be low and the accuracy of the distance between the electrode and the part to be written is not strict, are maintained.

さらに、収束用電極7は、ステンレス等の薄い
板にエツチング等により穴をあけることにより容
易に作成することができ、構造が簡単であるとい
う利点がある。
Further, the converging electrode 7 can be easily made by etching a hole in a thin plate made of stainless steel or the like, and has the advantage of having a simple structure.

収束用電極7の穴71の直径φbが、アパーチ
ヤ電極2の穴22の直径φaより大きいため、な
るべく穴22の間隔を離しておかないと穴71が
対応して形成できなくなるため穴22の配置を工
夫する必要が生ずる。ここでは、一例を第3図
a,bに示す。第3図aに示すように電極23に
は穴22が斜めに配置されている。また、第3図
bに示すように、電極24は各穴22の周りを取
り囲んでそれぞれ独立に設けられ、かつリード線
25がそれぞれ取り付けれている。アパーチヤ極
電2の穴22の配置に対応して、収束用電極7の
穴71の配置も第4図に示すように斜めになり、
したがつて隣接するものが接触しないで形成で
き、収束効果を持つた収束用電極7が可能とな
る。収束用電極7の収束効果の実験例を示すと次
のようである。
Since the diameter φ b of the hole 71 of the converging electrode 7 is larger than the diameter φ a of the hole 22 of the aperture electrode 2, the holes 71 cannot be formed correspondingly unless the holes 22 are spaced apart as much as possible. It becomes necessary to devise the arrangement of the Here, an example is shown in FIGS. 3a and 3b. As shown in FIG. 3a, holes 22 are arranged diagonally in the electrode 23. Further, as shown in FIG. 3B, electrodes 24 are provided independently surrounding each hole 22, and lead wires 25 are attached to each electrode. Corresponding to the arrangement of the holes 22 of the aperture electrode 2, the arrangement of the holes 71 of the converging electrode 7 is also oblique as shown in FIG.
Therefore, adjacent electrodes can be formed without contacting each other, and a focusing electrode 7 with a focusing effect can be obtained. An experimental example of the focusing effect of the focusing electrode 7 is as follows.

アパーチヤ電極2の穴22の直径φaが100〜
400μmで、この直径φaと等距離に、2倍の直径
φbを持つ穴71を有する収束用電極7を配置し、
収束用電極7とアパーチヤ電極2の間に5×
105V/mの電界を加えたところ、収束用電極7
がないときに比べ約9倍の収束効果があつた。
The diameter φ a of the hole 22 of the aperture electrode 2 is 100~
400 μm, and a focusing electrode 7 having a hole 71 with twice the diameter φ b is placed equidistant from this diameter φ a ,
5× between convergence electrode 7 and aperture electrode 2
When an electric field of 10 5 V/m was applied, the focusing electrode 7
The convergence effect was about 9 times greater than when it was not used.

第5図はアパーチヤ電極2の他の実施例を示す
もので、第3図bに対応するものである。この実
施例では穴22を斜めの2本の直線上に配置する
ようにしている。すなわち、第3図bでは穴22
が斜め1本の直線上にあるが、これを1つ置きに
下方に下げて他の斜めの直線上に配置したもので
ある。この実施例によると穴22相互間の距離が
さらに大きくとれ、したがつて、収束用電極7の
穴71の直径を大きくとつても支障がないように
なる。
FIG. 5 shows another embodiment of the aperture electrode 2, and corresponds to FIG. 3b. In this embodiment, the holes 22 are arranged on two diagonal straight lines. That is, in FIG. 3b, hole 22
is on one diagonal straight line, but every other one is lowered and placed on the other diagonal straight line. According to this embodiment, the distance between the holes 22 can be further increased, so that there is no problem even if the diameter of the hole 71 of the focusing electrode 7 is increased.

なお、上記実験は、ワイヤ1に+6KVの電圧
を印加し、アパーチヤ電極2を通過した電流をエ
レクトロメータで測定することにより行つた。さ
らに、収束用電極7の穴径とそこに加える電圧を
増大すれば、さらに収束することも可能である。
The above experiment was conducted by applying a voltage of +6 KV to the wire 1 and measuring the current passing through the aperture electrode 2 with an electrometer. Further, by increasing the hole diameter of the focusing electrode 7 and the voltage applied thereto, further focusing is possible.

以上説明したように、この発明は、イオン流制
御用のアパーチヤ電極とコロナワイヤの間に収束
用電極を配置し、イオン流を収束させるようにし
たので、記録の制御電圧が低くてすみ、また、中
間調記録が可能で、かつ記録速度の速い静電記録
用静電潜像書きこみ装置を簡単な機構で実現でき
る。そして、収束用電極はアパーチヤ電極とは独
立されているので、アパーチヤ電極の電位の変動
によつて収束効果に変動を来さないばかりでな
く、高いイオン収束効率が得られる利点がある。
As explained above, in this invention, the focusing electrode is arranged between the aperture electrode for controlling the ion flow and the corona wire to focus the ion flow, so the control voltage for recording can be kept low. , an electrostatic latent image writing device for electrostatic recording that is capable of halftone recording and has a high recording speed can be realized with a simple mechanism. Since the focusing electrode is independent from the aperture electrode, there is an advantage that not only the focusing effect does not change due to fluctuations in the potential of the aperture electrode, but also high ion focusing efficiency can be obtained.

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

第1図は従来の静電記録用静電潜像書きこみ装
置の構成略図、第2図はこの発明の一実施例を示
す構成略図、第3図a,bはこの発明のアパーチ
ヤ電極の一例を示す表面図および裏面図、第4図
は同じく収束用電極の平面図、第5図はアパーチ
ヤ電極の他の例を示す裏面図である。 図中、1はワイヤ、2はアパーチヤ電極、3は
電圧発生回路、4はイオン流、5はコロナ荷電
器、6はイオン流収束用電源、7は収束用電極、
21は絶縁板、22は穴、23,24は電極、2
5はリード線、71は穴である。
FIG. 1 is a schematic diagram of the configuration of a conventional electrostatic latent image writing device for electrostatic recording, FIG. 2 is a schematic diagram of the configuration of an embodiment of the present invention, and FIGS. 3 a and b are examples of the aperture electrode of the present invention. FIG. 4 is a plan view of the focusing electrode, and FIG. 5 is a back view of another example of the aperture electrode. In the figure, 1 is a wire, 2 is an aperture electrode, 3 is a voltage generation circuit, 4 is an ion flow, 5 is a corona charger, 6 is a power source for converging the ion flow, 7 is a convergence electrode,
21 is an insulating plate, 22 is a hole, 23 and 24 are electrodes, 2
5 is a lead wire, and 71 is a hole.

Claims (1)

【特許請求の範囲】[Claims] 1 コロナイオン発生源とコロナイオン流を電気
的に制御するアパーチヤ電極との間に、前記アパ
ーチヤ電極の個々の穴の位置に対応して、その穴
径より大きい穴径からなる個々の孔を有する収束
用電極を設け、該収束用電極側の前記アパーチヤ
電極と該収束用電極との間に一定の電圧を加える
定電圧源を配置し、前記コロナイオン流を前記ア
パーチヤ電極の穴に収束させることを特徴とする
静電記録用静電潜像書きこみ装置。
1. Between the corona ion generation source and the aperture electrode that electrically controls the corona ion flow, each hole has a diameter larger than the hole diameter corresponding to the position of each hole of the aperture electrode. A focusing electrode is provided, and a constant voltage source is arranged to apply a constant voltage between the aperture electrode on the focusing electrode side and the focusing electrode, and the corona ion flow is focused into the hole of the aperture electrode. An electrostatic latent image writing device for electrostatic recording, characterized by:
JP11917182A 1982-07-10 1982-07-10 Electrostatic latent image writing apparatus for electrostatic recording Granted JPS5911258A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11917182A JPS5911258A (en) 1982-07-10 1982-07-10 Electrostatic latent image writing apparatus for electrostatic recording

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11917182A JPS5911258A (en) 1982-07-10 1982-07-10 Electrostatic latent image writing apparatus for electrostatic recording

Publications (2)

Publication Number Publication Date
JPS5911258A JPS5911258A (en) 1984-01-20
JPH0410430B2 true JPH0410430B2 (en) 1992-02-25

Family

ID=14754664

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11917182A Granted JPS5911258A (en) 1982-07-10 1982-07-10 Electrostatic latent image writing apparatus for electrostatic recording

Country Status (1)

Country Link
JP (1) JPS5911258A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0679858B2 (en) * 1984-03-30 1994-10-12 株式会社東芝 Ion flow modulator

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5087330A (en) * 1973-12-05 1975-07-14
JPS5697358A (en) * 1979-12-29 1981-08-06 Sony Corp Ion current controlling electrostatic recorder
JPS58129439A (en) * 1982-01-27 1983-08-02 Konishiroku Photo Ind Co Ltd Electrostatic recording device

Also Published As

Publication number Publication date
JPS5911258A (en) 1984-01-20

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