JPH0630907B2 - Electrostatic recording method - Google Patents
Electrostatic recording methodInfo
- Publication number
- JPH0630907B2 JPH0630907B2 JP60025852A JP2585285A JPH0630907B2 JP H0630907 B2 JPH0630907 B2 JP H0630907B2 JP 60025852 A JP60025852 A JP 60025852A JP 2585285 A JP2585285 A JP 2585285A JP H0630907 B2 JPH0630907 B2 JP H0630907B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- ions
- dielectric
- electrodes
- alternating 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 - Lifetime
Links
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03G—ELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
- G03G15/00—Apparatus for electrographic processes using a charge pattern
- G03G15/22—Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20
- G03G15/32—Apparatus 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
- G03G15/321—Apparatus 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
- G03G15/323—Apparatus 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
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B41—PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
- B41J—TYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
- B41J2/00—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
- B41J2/385—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective supply of electric current or selective application of magnetism to a printing or impression-transfer material
- B41J2/41—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective supply of electric current or selective application of magnetism to a printing or impression-transfer material for electrostatic printing
- B41J2/415—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective supply of electric current or selective application of magnetism to a printing or impression-transfer material for electrostatic printing by passing charged particles through a hole or a slit
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)
- Electrophotography Using Other Than Carlson'S Method (AREA)
- Dot-Matrix Printers And Others (AREA)
Description
【発明の詳細な説明】 技術分野 本発明は、静電記録方法に関する。TECHNICAL FIELD The present invention relates to an electrostatic recording method.
背景技術 静電印刷などにおいて、高電流密度のイオンを発生さ
せ、これを抽出して選択的に被帯電部材に付与して、該
部材を画像状に帯電させることが、例えば、米国特許第
4155093 号公報などで知られている。この装置に用いら
れるイオン発生装置では、誘電体と該誘電体の一方の側
に固着され第1の方向に延びる複数の第1電極と、該誘
電体の他方の側に固着され該第1の方向と交差する方向
に延びる複数の第2電極とを有し、複数の第1電極と複
数の第2電極とでマトリックスを構成する。このマトリ
ックスの選択された部分に対応する第1電極と第2電極
との間に交互電圧を印加することにより、その部分に対
応する第2電極の近傍に正・負イオンが発生する。この
発生したイオンを選択的に抽出して被帯電部材を帯電す
ることができる。したがって、マトリックス構造の電極
を選択的に駆動することによって、ドットによる静電記
録を行なうことがができる。BACKGROUND ART In electrostatic printing and the like, it is possible to generate ions with a high current density, extract the ions, and selectively apply the ions to a member to be charged to charge the member in an image-like manner.
It is known from the publication No. 4155093. In the ion generator used in this device, a dielectric, a plurality of first electrodes fixed to one side of the dielectric and extending in a first direction, and a first electrode fixed to the other side of the dielectric are provided. A plurality of second electrodes extending in a direction intersecting the direction, and the plurality of first electrodes and the plurality of second electrodes form a matrix. By applying an alternating voltage between the first electrode and the second electrode corresponding to the selected portion of this matrix, positive and negative ions are generated in the vicinity of the second electrode corresponding to that portion. The generated ions can be selectively extracted to charge the member to be charged. Therefore, it is possible to perform electrostatic recording by dots by selectively driving the electrodes having the matrix structure.
この方法による静電記録は有用と考えられるが、現在知
られているものでは記録の1ドットの大きさが一定せ
ず、ばらつくという欠点があり、この為均一な潜像を形
成出来ないという問題がある。Although electrostatic recording by this method is considered to be useful, there is a drawback that the size of one dot of recording is not constant and varies with the currently known ones, so that a uniform latent image cannot be formed. There is.
発明の目的 したがって、本発明は上述の形式の静電記録方法におい
て、ドットサイズのばらつきが生ずる原因を解明し、こ
れを解消することによってサイズの均一なドットの形成
を可能ならしめ、均一な潜像を形成できる静電記録方法
を提供することを目的とする。SUMMARY OF THE INVENTION Therefore, the present invention has clarified the cause of dot size variation in the electrostatic recording method of the above-described type, and by eliminating this, it is possible to form dots of a uniform size, and a uniform latent image is formed. An object is to provide an electrostatic recording method capable of forming an image.
発明の概要 本件発明者は、第1の方向に延びる複数の第1電極と、
第1の方向と異なる第2の方向に延びて該第1電極とと
もにマトリックスを構成する第2電極と、該第2電極に
対し、前記第1電極とは反対側に設けられ前記マトリッ
クスに対応した開口を有する第3電極と、第1電極と第
2電極との間の第1誘電体と、前記第2電極と第3電極
との間の第2誘電体とを有し、該第2誘電体はマトリッ
クスに対応した開口部を有し、前記第1電極と第2電極
間に交互電圧を印加し、前記第2電極と第1誘電体表面
との放電によってイオンを発生させ、該イオンを前記第
2電極と第3電極との電位差によって前記第3電極の開
口部から引出し、該イオンによって記録体面に電荷ドッ
トによる電荷パターンを形成する静電記録方法におい
て、ドットサイズに不均一が生ずる原因を解明し、1個
の電荷ドットを形成するさいの有効イオン発生回数を1
0以上とすることによって、ドットサイズを均一とし、
したがって、均一な潜像の形成を可能にした。SUMMARY OF THE INVENTION The present inventor has a plurality of first electrodes extending in a first direction,
A second electrode extending in a second direction different from the first direction and forming a matrix with the first electrode; and a second electrode provided on the side opposite to the first electrode with respect to the second electrode and corresponding to the matrix. A third electrode having an opening, a first dielectric between the first electrode and the second electrode, and a second dielectric between the second electrode and the third electrode. The body has openings corresponding to the matrix, and an alternating voltage is applied between the first electrode and the second electrode to generate ions by the discharge between the second electrode and the first dielectric surface. Cause of non-uniformity in dot size in an electrostatic recording method in which a potential difference between the second electrode and the third electrode causes extraction from the opening of the third electrode to form a charge pattern of charge dots on the surface of the recording medium by the ions To form a single charge dot The effective ionic number of occurrences of Rusai 1
By setting it to 0 or more, the dot size becomes uniform,
Therefore, it is possible to form a uniform latent image.
実施例 第1図は本発明の静電記録方法に用いる静電記録ヘッド
の断面図、第2図は同斜視図である。EXAMPLE FIG. 1 is a sectional view of an electrostatic recording head used in the electrostatic recording method of the present invention, and FIG. 2 is a perspective view of the same.
この静電記録ヘッド1は第1図の横方向(第1の方向)
に延びる誘導電極である第1電極11と第1の方向と異
なる第2の方向に延びる放電電極である第2電極12
(フィンガー電極)とを有し、第1図上方から見た場合
にこれらの電極はマトリックスをを構成する。第2電極
12の第1電極11と反対側には第3電極13があり、
これはマトリックスに対応した複数の開口を有する。第
1電極11と第2電極12とそれらの間に第1誘電体1
4を挟持する。すなわち第1電極11と第2電極12と
は第1誘電体14の夫々の面に固着されている。第2電
極12と第3電極13もそれらの間に第2誘電体15を
挟持する。第2誘電体15は第3電極13の複数開口に
対応した開口16を有する。この構成のイオン発生装置
の複数の第1電極11と第2電極12との間に選択的に
交互電圧を印加することにより、マトリックスの選択さ
れた部分に対応する第2電極12の近傍に正・負イオン
が発生する。第2電極12と第3電極13との間にはバ
イアス電圧が印加され、その極性によって決まる極性の
イオンのみが前記正・負イオンから抽出され、このイオ
ンは開口16および開口17を通過して開口17に対向
して設けられる不図示の記録材である被帯電部材を帯電
する。このようにして、複数の第1電極11と第2電極
12の選択的駆動によって記録材上にドット潜像を形成
することができる。This electrostatic recording head 1 is shown in the lateral direction of FIG. 1 (first direction).
A first electrode 11 which is an induction electrode extending in the first direction and a second electrode 12 which is a discharge electrode extending in a second direction different from the first direction
(Finger electrodes), and these electrodes form a matrix when viewed from above in FIG. There is a third electrode 13 on the opposite side of the second electrode 12 from the first electrode 11,
It has a plurality of openings corresponding to the matrix. The first electrode 11 and the second electrode 12 and the first dielectric 1 between them
Hold 4 That is, the first electrode 11 and the second electrode 12 are fixed to the respective surfaces of the first dielectric body 14. The second electrode 12 and the third electrode 13 also sandwich the second dielectric 15 between them. The second dielectric 15 has openings 16 corresponding to the plurality of openings of the third electrode 13. By selectively applying an alternating voltage between the plurality of first electrodes 11 and the second electrodes 12 of the ion generating device of this configuration, a positive electrode is provided in the vicinity of the second electrode 12 corresponding to the selected portion of the matrix.・ Negative ions are generated. A bias voltage is applied between the second electrode 12 and the third electrode 13, and only ions having a polarity determined by the polarity are extracted from the positive and negative ions, and these ions pass through the openings 16 and 17. A member to be charged, which is a recording material (not shown) provided facing the opening 17 is charged. In this way, a dot latent image can be formed on the recording material by selectively driving the plurality of first electrodes 11 and the second electrodes 12.
この記録ヘッドを使用した本発明の静電記録方法を説明
する前に、本件発明者が解明したドットサイズのばらつ
きの原因について詳細に説明する。第3図は第1電極1
1と第2電極12との間を流れる電流の時間的変化を示
したものである。1周期の間に複数回(典型的には2
回)生じる鋭いスパイク状の電流は前記の正・負イオン
を発生させる放電によるものである。この放電は強い電
界のある場所で放射線などが引金となって、起こるもの
と考えられ、放電発生時点はランダムで一定していな
い。放電電流波形を何回にもわたってかさねると、第3
図のようになり、放電発生の時点が大きくばらついてい
ることが理解される。Before explaining the electrostatic recording method of the present invention using this recording head, the cause of the variation in dot size which the present inventors have clarified will be described in detail. FIG. 3 shows the first electrode 1
1 shows a temporal change in a current flowing between the first electrode and the second electrode 12. Multiple times (typically 2
The sharp spike-shaped current that occurs is due to the discharge that generates the positive and negative ions. It is considered that this discharge is triggered by radiation or the like in a place where there is a strong electric field, and the time of discharge occurrence is random and not constant. If you repeat the discharge current waveform over and over,
As shown in the figure, it is understood that the time of occurrence of discharge varies greatly.
発明者はこのように放電発生時点が1周期ごとに異なる
ので、放電電圧が異なり、したがって、抽出されて開口
17を通過するイオン量が毎回異なることになると考
え、これが不均一なドット潜像を得るための障害になる
と考えた。そしてこの不均一性を解消するために大きな
放電1回でドットを作るのでなく、1回の放電量を小さ
くし、1ドット当り複数回にわたってイオンを発生させ
ることが考えられる。発明者はこの放電を小さくして回
数を増加させることについて実験を繰返したところ、放
電回数を10回以上とすることで、ドット径のばらつき
がめだって小さくなることを見出した。The inventor thinks that the discharge generation time differs for each cycle in this way, and therefore the discharge voltage is different, and therefore the amount of ions extracted and passing through the opening 17 is different every time, which results in a non-uniform dot latent image. I thought it would be an obstacle to getting. Then, in order to eliminate this non-uniformity, it is conceivable to reduce the amount of discharge at one time and generate ions a plurality of times per dot, instead of making dots at one large discharge. The inventor repeated an experiment to reduce the discharge and increase the number of times, and found that the number of discharges was 10 or more, the dot diameter variation was extremely small.
以下本発明の静電記録方法について説明する。The electrostatic recording method of the present invention will be described below.
第1図において第1電極11と第2電極12との間には
周波数3MHzの交互電圧が印加され、この記録ヘッド
の下方には記録体である被帯電部材(不図示)が第3電
極13に対向して設置されている。この被帯電部材は12
インチ/秒で移動する。第1電極11は16本の細長電極
であり、前記の交互電圧は時分割で順次各第1電極11
に印加される。本実施例はドット潜像密度を300ドット
/in.としたので、1ドットの書込に要する時間は、
1/(300×12×16)=17.4μsである。In FIG. 1, an alternating voltage having a frequency of 3 MHz is applied between the first electrode 11 and the second electrode 12, and a charged member (not shown), which is a recording medium, is provided below the recording head with the third electrode 13. It is installed opposite to. This charged member is 12
Move in inches / second. The first electrodes 11 are 16 elongated electrodes, and the alternating voltage is time-divisionally sequentially applied to each of the first electrodes 11.
Applied to. In this embodiment, the dot latent image density is 300 dots / in. Therefore, the time required to write 1 dot is
1 / (300 × 12 × 16) = 17.4 μs.
一方、第1電極11と第2電極12との間に交互電圧信
号が印加されると同時に放電可能電圧に到達するのでは
なく、第5図に示すように立上りに所定時間Trを要
し、同様に立下りについてもTfを要する。この立上り
時間Trは約2μs、立下り時間Tfは約8μsであ
る。したがって、有効放電の生ずる時間間隔は17.4−2
−8=7.4μsとなる。交互電圧の周波数は前記のごと
く3MHzであるので、この7.4μs中に交互電圧のピ
ークは正・負を含めれば、3×7.4×2=44回発生す
る。しかし、1周期内の2個のピークのうち第1電極1
1が第3電極13に対して正電圧である時の放電は潜像
形成には寄与しない。第6図および第7図はその様子を
示したもので第1電極11が第3電極13に対して+10
00Vの時(第6図)と−1000Vの時(第7図)の電気力
線を示したものである。第6図の場合放電発生部分で発
生した負イオンはすべて第1誘電体14の表面に吸収さ
れ下方にはでないことが理解される。したがって、1つ
のドット潜像を得るために利用できる放電の回数は44/
2=22回である。このように1ドット潜像を形成するた
めに10回以上の放電を利用することによってサイズばら
つきの少ないドット潜像を得ることができる。On the other hand, when the alternating voltage signal is applied between the first electrode 11 and the second electrode 12 and the dischargeable voltage is not reached at the same time, it takes a predetermined time Tr to rise as shown in FIG. Similarly, the fall also requires Tf. The rising time Tr is about 2 μs and the falling time Tf is about 8 μs. Therefore, the effective discharge time interval is 17.4-2.
-8 = 7.4 μs. Since the frequency of the alternating voltage is 3 MHz as described above, the peak of the alternating voltage in this 7.4 μs occurs 3 × 7.4 × 2 = 44 times if positive and negative are included. However, of the two peaks in one cycle, the first electrode 1
Discharge when 1 is a positive voltage with respect to the third electrode 13 does not contribute to latent image formation. FIG. 6 and FIG. 7 show the situation, in which the first electrode 11 is +10 with respect to the third electrode 13.
The electric lines of force at 00V (Fig. 6) and -1000V (Fig. 7) are shown. In the case of FIG. 6, it is understood that all the negative ions generated in the discharge generation portion are absorbed by the surface of the first dielectric substance 14 and are not in the downward direction. Therefore, the number of discharges that can be used to obtain one dot latent image is 44 /
2 = 22 times. In this way, by utilizing the discharge 10 times or more to form a 1-dot latent image, it is possible to obtain a dot-latent image with little size variation.
イオン発生回数を1ドット当り10回以上にするためには
周波数fは、記録体の相対移動速度をVp、時分割数を
n、記録体の単位長さ当りに形成されるドット数をp、
交互電圧の振巾が印加されてから有効イオンが発生する
までの時間をTr、有効イオンの発生が停止してから交
互電圧の振巾が0になるまでの時間をTfとしたとき、 10/[1/(Vp×n×p)−Tr−Tf]≦f を満足することになる。In order to make the number of ions generated 10 times or more per dot, the frequency f is Vp, the relative moving speed of the recording medium, n is the number of time divisions, and p is the number of dots formed per unit length of the recording medium.
When the time from the application of the amplitude of the alternating voltage to the generation of the effective ions is Tr and the time from the stop of the generation of the effective ions to the amplitude of the alternating voltage is Tf, 10 / [1 / (Vp × n × p) −Tr−Tf] ≦ f is satisfied.
本実施例ではVp=12in./s、n=16、p=300
ドット/in.Tr=2μs、Tf=8μsであるか
ら、周波数fはf≧1.4MHzを満足することになる。
一方,発生したイオンがイオン発生部から第3電極13
の開口17に到達するまでには一定の時間がかかり、こ
れより速い周波数の交互電圧を印加するとイオンが開口
17に到達しないことが判明した。この理由は第6図と
第7図の間の電界の切替りが早すぎて、イオンが下方に
加速されないためであると考えられる。したがって、周
波数はf≦1/T、(Tは第2電極12の近傍に発生し
たイオンが開口17に達するのに要する時間)を満足す
ることがこのましい。時間Tは実験によると約0.2μs
である。したがって本実施例においては周波数は5MH
z以下であることが好ましい。In this embodiment, Vp = 12 in. / S, n = 16, p = 300
Dot / in. Since Tr = 2 μs and Tf = 8 μs, the frequency f satisfies f ≧ 1.4 MHz.
On the other hand, the generated ions are transferred from the ion generator to the third electrode 13
It took a certain amount of time to reach the opening 17, and it was found that the ions did not reach the opening 17 when an alternating voltage having a faster frequency was applied. It is considered that this is because the switching of the electric field between FIG. 6 and FIG. 7 is too early and the ions are not accelerated downward. Therefore, it is preferable that the frequency satisfies f ≦ 1 / T, where T is the time required for the ions generated near the second electrode 12 to reach the opening 17. Time T is about 0.2μs according to the experiment
Is. Therefore, in this embodiment, the frequency is 5 MH.
It is preferably z or less.
本実施例では周波数を3MHzに設定したので、均一な
ドット潜像が形成され高精細な画像が形成された。In this embodiment, since the frequency was set to 3 MHz, a uniform dot latent image was formed and a high-definition image was formed.
発明の効果 以上説明のごとく本発明によれば、ドット径のばらつき
をなくし均一かつ高精細な潜像形成が可能となった。EFFECTS OF THE INVENTION As described above, according to the present invention, it is possible to form a uniform and high-definition latent image without variations in dot diameter.
第1図は本発明の静電記録方法に用いる静電気録ヘッド
の断面図、 第2図は第1図の静電記録ヘッドの分解斜視図、 第3図は第1電極と第2電極との間を流れる電流を示す
図、 第4図は第1電極と第2電極との間の電流を時間的に重
ねたもの、 第5図は第1電極と第2電極との間に生ずる交互電圧の
時間的変化を示す図、 第6図および第7図は第1図の装置における異った状態
での電気力線の様子を示す図である。 符号の説明 11:第1電極 12:第2電極 13:第3電極 14:第1誘電体FIG. 1 is a sectional view of an electrostatic recording head used in the electrostatic recording method of the present invention, FIG. 2 is an exploded perspective view of the electrostatic recording head of FIG. 1, and FIG. 3 shows a first electrode and a second electrode. FIG. 4 is a diagram showing a current flowing between the electrodes, FIG. 4 is a diagram in which currents between the first electrode and the second electrode are temporally overlapped, and FIG. 5 is an alternating voltage generated between the first electrode and the second electrode. FIG. 6 and FIG. 7 are diagrams showing the state of electric lines of force in different states in the apparatus of FIG. DESCRIPTION OF SYMBOLS 11: 1st electrode 12: 2nd electrode 13: 3rd electrode 14: 1st dielectric
───────────────────────────────────────────────────── フロントページの続き (72)発明者 竹内 達夫 東京都大田区下丸子3丁目30番2号 キヤ ノン株式会社内 (72)発明者 江上 秀己 東京都大田区下丸子3丁目30番2号 キヤ ノン株式会社内 (72)発明者 保坂 昭仁 東京都大田区下丸子3丁目30番2号 キヤ ノン株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Tatsuo Takeuchi 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc. (72) Hideki Egami 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Incorporated (72) Inventor Akito Hosaka 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc.
Claims (2)
1の方向と異なる第2の方向に延びて該第1電極ととも
にマトリックスを構成する第2電極と、該第2電極に対
し、前記第1電極とは反対側に設けられ前記マトリック
スに対応した開口を有する第3電極と、第1電極と第2
電極との間の第1誘電体と、前記第2電極と第3電極と
の間の第2誘電体とを有し、該第2誘電体はマトリック
スに対応した開口部を有し、前記第1電極と第2電極間
に交互電圧を印加し、前記第2電極と第1誘電体表面と
の放電によってイオンを発生させ、該イオンを前記第2
電極と第3電極との電位差によって前記第3電極の開口
部から引出し、該イオンによって記録体面に電荷ドット
による電荷パターンを形成する静電記録方法であって、
1個の電荷ドットを形成するさいの有効イオン発生回数
を10以上とすることを特徴とする静電記録方法。1. A plurality of first electrodes extending in a first direction, a second electrode extending in a second direction different from the first direction and forming a matrix with the first electrode, and a second electrode. On the other hand, a third electrode provided on the opposite side of the first electrode and having an opening corresponding to the matrix, the first electrode and the second electrode.
A first dielectric between the electrodes and a second dielectric between the second and third electrodes, the second dielectric having openings corresponding to the matrix, Alternating voltage is applied between the first electrode and the second electrode, ions are generated by the discharge between the second electrode and the first dielectric surface, and the ions are generated by the second electrode.
An electrostatic recording method of forming a charge pattern of charge dots on a surface of a recording medium by extracting the ions from an opening of the third electrode by a potential difference between the electrode and the third electrode,
An electrostatic recording method characterized in that the number of generation of effective ions when forming one charge dot is 10 or more.
において、記録体の相対移動速度をVp、時分割数を
n、記録体の単位長さ当りに形成されるドット数をp、
交互電圧の振巾が印加されてから有効イオンが発生する
までの時間をTr、有効イオンの発生が停止してから交
互電圧の振巾が0になるまでの時間をTfとしたとき、
交互電圧の周波数を10/[1/(Vp×n×p)−
Tr−Tf]以上としたことを特徴とする静電記録方
法。2. The electrostatic recording method according to claim 1, wherein the relative moving speed of the recording medium is Vp, the number of time divisions is n, and the number of dots formed per unit length of the recording medium is p. ,
Let Tr be the time from the application of the amplitude of the alternating voltage to the generation of the effective ions, and Tf be the time from the stop of the generation of the effective ions to the amplitude of the alternating voltage being 0.
The frequency of the alternating voltage is 10 / [1 / (Vp × n × p) −
Tr-Tf] or more.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60025852A JPH0630907B2 (en) | 1985-02-13 | 1985-02-13 | Electrostatic recording method |
| US06/827,431 US4697196A (en) | 1985-02-13 | 1986-02-10 | Electrostatic recording method and apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60025852A JPH0630907B2 (en) | 1985-02-13 | 1985-02-13 | Electrostatic recording method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61185456A JPS61185456A (en) | 1986-08-19 |
| JPH0630907B2 true JPH0630907B2 (en) | 1994-04-27 |
Family
ID=12177361
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60025852A Expired - Lifetime JPH0630907B2 (en) | 1985-02-13 | 1985-02-13 | Electrostatic recording method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0630907B2 (en) |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4155093A (en) * | 1977-08-12 | 1979-05-15 | Dennison Manufacturing Company | Method and apparatus for generating charged particles |
| NZ198031A (en) * | 1980-08-21 | 1988-11-29 | Dennison Mfg Co | Electrostatic printer: charged particles extracted from glow discharge |
| JPS59140459A (en) * | 1983-02-01 | 1984-08-11 | Minolta Camera Co Ltd | Electrostatic image forming method |
-
1985
- 1985-02-13 JP JP60025852A patent/JPH0630907B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61185456A (en) | 1986-08-19 |
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