JPS6384944A - Static recording head - Google Patents

Static recording head

Info

Publication number
JPS6384944A
JPS6384944A JP22980086A JP22980086A JPS6384944A JP S6384944 A JPS6384944 A JP S6384944A JP 22980086 A JP22980086 A JP 22980086A JP 22980086 A JP22980086 A JP 22980086A JP S6384944 A JPS6384944 A JP S6384944A
Authority
JP
Japan
Prior art keywords
ion
ion flow
flow control
ions
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.)
Granted
Application number
JP22980086A
Other languages
Japanese (ja)
Other versions
JPH0630908B2 (en
Inventor
Daisuke Tsuda
大介 津田
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 JP22980086A priority Critical patent/JPH0630908B2/en
Publication of JPS6384944A publication Critical patent/JPS6384944A/en
Publication of JPH0630908B2 publication Critical patent/JPH0630908B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B41PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
    • B41JTYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
    • B41J2/00Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
    • B41J2/385Typewriters 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
    • B41J2/41Typewriters 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
    • B41J2/415Typewriters 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

  • Dot-Matrix Printers And Others (AREA)
  • Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)

Abstract

PURPOSE:To improve ion derivation efficiency by providing a head in which an ion flow course is formed between opposed insulation members, an ion generation part in which a high frequency high voltage is applied between both discharging electrodes and an ion flow control which controls the passage and interruption of generated ions. CONSTITUTION:A static recording head is composed of a head 10 in which an ion flow course 13 is formed between flat insulation members 11, 14, an ion generation part 20 provided at an outlet of the ion flow course 13 and an ion flow control 30. If a high frequency high voltage 23 is applied to each discharging electrode 21, 22 of the ion generation part 20, a differently oriented electric field is alternately formed in the range of an overlapping part. At that time, air breaks down dielectrically near the edge 22a of an upper discharging electrode 22, and positive and negative ions generate alternately from the edge 22a. Then generated ion groups 40 are gradually trapped and proliferated following the high-speed change of polarity of an applied voltage. Immediately these ions reach the ion flow control 30 provided at almost the same position as the ion generation part 20. Thus it is possible to eliminate an ion loss on the way to the ion flow control.

Description

【発明の詳細な説明】 [産業上の利用分野] この発明は、静電記録ヘッドに係り、特に、イオン発生
部として、一対の放電電極を絶縁層を介して重合配置し
てなるものが用いられる静電記録ヘッドの改良に関する
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to an electrostatic recording head, and particularly to an electrostatic recording head in which a pair of discharge electrodes are arranged in a polymerized manner with an insulating layer interposed therebetween as an ion generating section. This invention relates to improvements in electrostatic recording heads.

[従来の技術] 従来の静電記録ヘッドとしては、例えば特開昭59−1
64154号、同59−190854号の各公報所載の
ものがある。これは、第4図に示すように、放電ワイヤ
1及びこの放電ワイヤ1を取囲むシールド2でイオン発
生器を構成し、上記シールド2にはイオン排出路3を開
設すると共に、圧縮空気導入用の空気導入路4を開設す
る一方、上記イオン排出路3には画素密度に応じた制御
電極5を適宜数配置したものである。
[Prior Art] As a conventional electrostatic recording head, for example, Japanese Patent Application Laid-Open No. 59-1
There are those published in the publications No. 64154 and No. 59-190854. As shown in Fig. 4, an ion generator is constructed of a discharge wire 1 and a shield 2 surrounding the discharge wire 1, and an ion discharge path 3 is provided in the shield 2, and an ion discharge path 3 is provided for introducing compressed air. An air introduction path 4 is opened, and an appropriate number of control electrodes 5 are arranged in the ion exhaust path 3 in accordance with the pixel density.

このタイプにおいて、上記放電ワイヤ1に直流高電圧7
を印加すると、この放電ワイヤ1とシールド2との間で
放電が生じ、放電ワイヤ1周囲から多量のイオンが発生
して、導入された圧縮空気と共にイオン排出路3側へと
導かれる。このとき、上記制御電極5に適宜の画像制御
信号8を印加すると、各制御電極5部分での電界の有無
に応じてイオン流が通過若しくは遮断され、これによっ
て、記録体6上に画像制tlI11!圧に応じた静W1
潜像が形成されるのである。
In this type, a DC high voltage 7 is applied to the discharge wire 1.
When this is applied, a discharge occurs between the discharge wire 1 and the shield 2, and a large amount of ions are generated around the discharge wire 1 and guided to the ion exhaust path 3 side together with the introduced compressed air. At this time, when an appropriate image control signal 8 is applied to the control electrode 5, the ion flow passes or is blocked depending on the presence or absence of an electric field at each control electrode 5 portion. ! Static W1 according to pressure
A latent image is formed.

[発明が解決しようとする問題点] しかしながら、このような従来の静電記録ヘッドにあっ
ては、放電ワイヤ1の周囲で発生したイオンはシールド
2側へ放射状に向かうようになっており、その一部が圧
縮空気と共にイオン排出路3側へ取出されるに過ぎない
ので、イオンの絶対量を充分には確保することができず
、高速記録には向かないという問題がある。
[Problems to be Solved by the Invention] However, in such a conventional electrostatic recording head, ions generated around the discharge wire 1 are directed radially toward the shield 2, and Since only a portion is taken out to the ion exhaust path 3 side together with the compressed air, there is a problem that a sufficient absolute amount of ions cannot be secured, making it unsuitable for high-speed recording.

このような問題を解決するだめの手段としては例えば第
5図に示すようなものが考えられる。これは、平板状の
絶縁部材11と半円柱状の凹部を有する絶縁部材12ど
の間にイオン流通路13が形成されるヘッド本体10と
、イオン流通路13に面した平板状の絶縁部材11の一
部に設けられ且つ高周波高電圧24が印加される一対の
放′RM極21.22を絶縁層23を介して重合配置し
てなるイオン発生部20と、上記イオン流通路13の出
口付近に位置する再給縁部材11.12間に画素密度に
応じた制御電極31及びこれに対向する対向制御電極3
2が設けられ且つ両制御電極31.32間に画像制御信
号33が適宜印加されてイオン発生部20で発生したイ
オン流を通過、遮断制御するイオン流制御部30とから
なる。尚、符号35はヘッド本体1Gの出口部分と記録
体6との間に所定の電界を与えて例えば正のイオンのみ
を記録体6側へ導く直流バイアス電源である。
As a means to solve this problem, for example, the one shown in FIG. 5 can be considered. This includes a head body 10 in which an ion flow path 13 is formed between a flat insulating member 11 and an insulating member 12 having a semi-cylindrical recess, and a flat insulating member 11 facing the ion flow path 13. The ion generating section 20 includes a pair of radiation RM poles 21 and 22 which are provided in a part and to which a high frequency high voltage 24 is applied and which are arranged in a superimposed manner with an insulating layer 23 interposed therebetween, and an ion generating section 20 in the vicinity of the exit of the ion flow path 13. A control electrode 31 corresponding to the pixel density and a counter control electrode 3 opposite thereto are located between the resupply edge members 11 and 12.
2, and an ion flow control section 30 which controls passage and interruption of the ion flow generated in the ion generation section 20 by appropriately applying an image control signal 33 between both control electrodes 31 and 32. Incidentally, reference numeral 35 is a DC bias power supply that applies a predetermined electric field between the exit portion of the head body 1G and the recording medium 6 to guide, for example, only positive ions toward the recording medium 6 side.

このタイプによれば、放ll111!極21.22間に
高周波高電圧24を印加すると、放’RM極21.22
間に向きの異なる電界が交互に形成される。このとき、
第6図に示すように、上記電界によってイオン流通路1
3に面した放電電極22のエツジ部分22a付近の空気
が絶縁破壊し、このエツジ部分22aから正負のイオン
が交互に生成されることになるが、放電電極21.22
への印加電圧の極性が高速で変化するため、イオン群が
次第にトラップされて増殖され、このイオン群がイオン
流通路13中へ導入された圧縮空気と共に記録体6側へ
直ちに運び去られる。このため、記録体6に到達するイ
オンの絶対量は第4図に示されるタイプに比べて多く設
定される。
According to this type, releasell111! When the high frequency high voltage 24 is applied between the poles 21 and 22, the radiating RM pole 21 and 22
Electric fields with different directions are alternately formed between them. At this time,
As shown in FIG. 6, the ion flow path 1 is
The air near the edge portion 22a of the discharge electrode 22 facing 3 undergoes dielectric breakdown, and positive and negative ions are alternately generated from this edge portion 22a.
Since the polarity of the applied voltage changes rapidly, the ion group is gradually trapped and multiplied, and the ion group is immediately carried away to the recording medium 6 side together with the compressed air introduced into the ion flow path 13. Therefore, the absolute amount of ions reaching the recording medium 6 is set to be larger than that of the type shown in FIG.

ところが、このタイプにあっては、イオン発生部20で
イオンを発生させた後、発生イオンをイオン流制御部3
0で制御するという観点から両者を機能的に分離した構
成になっているため、必然的に、イオン発生部20とイ
オン流制御部30とはイオン流通路13に沿っである程
度の距離!をもって離間配置されることになる。この場
合、イオン発生部20で発生したイオンの一部は、イオ
ン流制御部30に到達するまでのイオン流通路13中に
おいて壁面等に衝合して中和されてしまうため、イオン
流制御部30に到達するまでのイオンの損失分だけ実質
的に取出されるイオンの絶対量が少なくなり、その分、
高速記録を図る上での障害になっていた。
However, in this type, after the ions are generated in the ion generator 20, the generated ions are transferred to the ion flow controller 3.
Since the configuration is such that the two are functionally separated from each other from the viewpoint of controlling at 0, the ion generation section 20 and the ion flow control section 30 are necessarily separated by a certain distance along the ion flow path 13! They will be spaced apart from each other. In this case, some of the ions generated in the ion generation section 20 collide with the wall surface etc. in the ion flow path 13 until reaching the ion flow control section 30 and are neutralized. The absolute amount of ions actually taken out decreases by the loss of ions until reaching 30, and by that amount,
This was an obstacle to achieving high-speed records.

[発明が解決しようとする問題点] この発明は、以上の問題点に着目して為されたものであ
って、構成の簡略化を図りながら、イオンの取出し効率
をより向上させることができる静電記録ヘッドを提供す
るものである。
[Problems to be Solved by the Invention] The present invention has been made by focusing on the above-mentioned problems. The present invention provides an electro-recording head.

すなわち、この発明は、相対向する絶縁部材間にイオン
流通路が形成されるヘッド本体と、一方の絶縁部材上に
一対の放電電極が絶縁層を介して重合配置されると共に
両放MWi極間に高周波高電圧が印加されるイオン発生
部と、このイオン発生部に対向する他方の絶縁部材上に
制御電極が画素密度に応じて配列され且つ各制御電極と
上記一方の放電電極を兼用してなる対向制御電極との間
に画像制御信号が印加されてイオン発生部で発生したイ
オン流を通過、遮断制御するイオン流制御部とを備えた
ものである。
That is, the present invention has a head main body in which an ion flow path is formed between opposing insulating members, a pair of discharge electrodes on one insulating member, which are arranged overlapping each other with an insulating layer interposed therebetween, and a discharge electrode between the two discharge MWi electrodes. An ion generating section to which a high frequency and high voltage is applied, and control electrodes are arranged on the other insulating member facing the ion generating section according to the pixel density, and each control electrode also serves as one of the discharge electrodes. and an ion flow control section to which an image control signal is applied between the counter electrode and the ion flow control section to control passage or interruption of the ion flow generated in the ion generation section.

このような技術的手段において、上記ヘッド本体を構成
する絶縁部材の形状や大きさについては適宜選択して差
支えないが、設計上、イオン発生部及びイオン流制御部
を略同一箇所に設けることができるため、イオン流通路
をそれほど長く確保する必要はない。また、イオン発生
部についても、絶縁層を挟んで配置した放電電極間に高
周波高電圧を印加する方式のものであれば、放電電極の
大きさや配II係については必要とする発生イオン社に
応じて適宜設計変更して差支えないが、イオンの生成率
をより向上させるには、イオン流通路に面した側の放i
!電極に多数の切込み凹部を設けることにより、実質的
にイオンの生成部として機能するエツジ部面積を拡大す
るように設計することが望ましい。更に、イオン1t4
t!11部としては、少なくとも、イオン発生部に対向
する絶縁部材上に設けられた11111電極側に画像制
御信号を印加し、放電電極のうち接地電位に保たれるも
のを対向制御1ffi極として選択するようにすればよ
い。更にまた、発生したイオンを記録体側へ移行させる
方法としては、イオン流通路に圧縮空気を導入したり、
ヘッドと記録体との間にイオンを導く電界を予め形成し
ておく等適宜選択して差支えない。
In such technical means, the shape and size of the insulating member constituting the head body may be selected as appropriate, but the ion generation section and the ion flow control section may be provided at approximately the same location due to design. Therefore, it is not necessary to ensure a very long ion flow path. In addition, regarding the ion generation section, if it is of a type that applies high frequency and high voltage between discharge electrodes arranged with an insulating layer in between, the size of the discharge electrodes and the arrangement II will depend on the required generation ion company. However, in order to further improve the ion generation rate, it is necessary to change the design on the side facing the ion flow path.
! It is desirable to design the electrode so as to expand the area of the edge portion that essentially functions as an ion generation portion by providing a large number of notch recesses in the electrode. Furthermore, ion 1t4
T! As part 11, an image control signal is applied at least to the 11111 electrode side provided on the insulating member facing the ion generating part, and one of the discharge electrodes that is maintained at the ground potential is selected as the opposing control 1ffi pole. Just do it like this. Furthermore, as a method for transferring the generated ions to the recording medium side, compressed air is introduced into the ion flow path,
An electric field for guiding ions may be formed in advance between the head and the recording medium, or the like may be selected as appropriate.

[作用] 上述したような技術的手段によれば、イオン発生部の一
対の放1!電極間に高周波高電圧を印加すると、イオン
流通路に面した側の放電電極のエツジ部分で空気の絶縁
破壊が起り、この部分から多量のイオンが発生する。そ
して、発生した多くのイオンは、このイオン発生部と略
同一部位に設けられたイオン流制御部で直ちに通過、遮
断l11111され、通過したイオンが記録体側へ移動
していき、所定の静電潜像を形成する。
[Operation] According to the technical means as described above, a pair of ion generators 1! When a high frequency and high voltage is applied between the electrodes, air dielectric breakdown occurs at the edge portion of the discharge electrode facing the ion flow path, and a large amount of ions are generated from this portion. Many of the generated ions immediately pass through and are blocked by the ion flow control unit installed at approximately the same location as the ion generation unit, and the passed ions move toward the recording medium to maintain a predetermined electrostatic potential. form an image.

[実施例] 以下、添附図面に示す実施例に基づいてこの発明の詳細
な説明する。
[Embodiments] Hereinafter, the present invention will be described in detail based on embodiments shown in the accompanying drawings.

第1図ないし第3図において、静電記録ヘッドの基本的
構成は、平板状の絶縁部材11.14間にイオン流通路
13が形成されるヘッド本体10と、イオン流通路13
の出口部分に設けられるイオン発生部20と、同じくイ
オン流通路13の出口部分に設けられるイオン流制御部
30とか°らなる。
1 to 3, the basic structure of the electrostatic recording head is: a head body 10 in which an ion flow path 13 is formed between flat insulating members 11 and 14;
The ion generating section 20 is provided at the exit of the ion flow path 13, and the ion flow control section 30 is also provided at the exit of the ion flow path 13.

この実施例において、上記イオン発生部20は、イオン
流通路13に面した一方の絶縁部材11上に下側放電電
極21を設けると共に、この下側放電電極21上には絶
縁1123を介して上側放電電極22を設け、両放電電
極21.22間に高周波高電圧24を印加するようにし
たものである。より具体的に述べると、上記下側放電電
極21は、略矩形状に形成されるもので、上記絶縁部材
11上に金ペーストによってスクリーン印刷焼付けを行
い、しかる後、フォトリソグラフ工程によって所定形状
に画成するものである。また、上記絶縁層23は、上記
下側放電電極21を覆う範囲に設けられ、例えばガラス
ペーストによってスクリーン印刷焼付けして構成される
ものである。更に、上記上側数i!電極22は、上記絶
縁層23上に金ペーストによってスクリーン印刷焼付け
を行い、しかる後、フォトリソグラフ工程を経て所定形
状に画成されるものである。
In this embodiment, the ion generating section 20 is provided with a lower discharge electrode 21 on one insulating member 11 facing the ion flow path 13, and an upper A discharge electrode 22 is provided, and a high frequency high voltage 24 is applied between both discharge electrodes 21 and 22. More specifically, the lower discharge electrode 21 is formed into a substantially rectangular shape, and is screen-printed with gold paste on the insulating member 11, and then shaped into a predetermined shape by a photolithography process. It is something that defines. Further, the insulating layer 23 is provided in a range that covers the lower discharge electrode 21, and is formed by screen printing and baking with glass paste, for example. Furthermore, the above upper number i! The electrode 22 is formed by screen-printing a gold paste onto the insulating layer 23 and then defining it into a predetermined shape through a photolithography process.

そして、この実施例において、上記上側数′11?!!
極22は、下側放電電極21の一側縁を除く全領域に重
合配置されるもので、上側放1[極22の一側縁は下側
放電電極21の他側縁から僅かに突出配置されている。
In this embodiment, the upper number '11? ! !
The poles 22 are arranged so as to overlap the entire area of the lower discharge electrode 21 except for one side edge, and the upper discharge electrode 22 is arranged so as to overlap the entire area except for one side edge of the lower discharge electrode 21. has been done.

そして、上側数WIW極22は、下側放電電極21と集
合した範囲において多数の切込み四部25を有しており
、この切込み凹部25群は櫛状に形成されている。そし
て更に、各切込み凹部25は例えば4個/m程度の密度
で構成されており、各切込み凹部25と切込み凹部25
間に形成される各枝部26との幅寸法は略等しいものと
して設定されている。
The upper few WIW poles 22 have a large number of four notches 25 in the range where they are combined with the lower discharge electrode 21, and the group of the notches 25 is formed in a comb shape. Furthermore, each cut recess 25 is configured with a density of, for example, about 4 pieces/m, and each cut recess 25 and the cut recess 25
The width dimensions of the respective branch portions 26 formed therebetween are set to be approximately equal.

また、上記イオン流制御部30は、上記上側放電電極2
2の基幹部27に対向した絶縁部材14面に画素帯r!
1(例えば12本/m)に応じて分割配置される制am
極31と、上記上側放電電極22の基幹部2γを兼用し
且つ接地電位に保たれる対向制m+電極34とからなり
、上記各制御211′R極31に画像パターンに応じた
画像制御信号33を印加するようにしたものである。尚
、符号35は従来例と同様な直流バイアス電源である。
The ion flow control section 30 also controls the upper discharge electrode 2.
A pixel band r!
1 (for example, 12 lines/m)
It consists of a pole 31 and an opposing control m+ electrode 34 which also serves as the base portion 2γ of the upper discharge electrode 22 and is kept at ground potential, and each control 211'R pole 31 receives an image control signal 33 according to the image pattern. is applied. Incidentally, reference numeral 35 is a DC bias power supply similar to the conventional example.

従って、この実施例に係る静電記録ヘッドによれば、今
、イオン発生部20の各放電電極21.22に高周波a
i!圧24を印加すると、各放電電極21.22の重合
部分範囲に向きの異なる電界が交互に形成される。この
とき、イオン流通路13に面した側の上側放電電極22
のエツジ部分22a付近で空気が絶縁破壊し、このエツ
ジ部分22aから正負のイオン40が交互に生成される
と共に、印加電圧の極性の高速変化に伴って発生イオン
40群が次第にトラップされて増殖される。特に、この
実施例においては、第一に、上記エツジ部分22aは切
込み凹部25の内側縁及び枝部26の突出端縁で構成さ
れているので、エツジ部分22aの面積、言い換えれば
イオン40の生成領域が充分に広く確保され、その分、
イオン40の生成量を増加させることができ、第二に、
放電電極21.22間の実質的重合面積は、切込み凹部
25の存在分だけ減少したものになっているため、放電
電極21.22間の静電容量が小さく設定されることに
なり、これに伴って、絶縁1[23に充放電するための
電流は比較的小さいものに抑えられ、放電電極21.2
2間での消費される電力を低減することができる。
Therefore, according to the electrostatic recording head according to this embodiment, the high frequency a is applied to each discharge electrode 21 and 22 of the ion generating section 20.
i! When the pressure 24 is applied, electric fields with different directions are created alternately in the overlapping area of each discharge electrode 21,22. At this time, the upper discharge electrode 22 facing the ion flow path 13
Dielectric breakdown occurs in the air near the edge portion 22a, and positive and negative ions 40 are alternately generated from this edge portion 22a, and as the polarity of the applied voltage changes rapidly, the generated ion 40 group is gradually trapped and multiplied. Ru. Particularly, in this embodiment, firstly, since the edge portion 22a is composed of the inner edge of the cut recess 25 and the protruding edge of the branch portion 26, the area of the edge portion 22a, in other words, the generation of ions 40. The area is sufficiently wide, and
The amount of ions 40 produced can be increased, and secondly,
Since the substantial overlapping area between the discharge electrodes 21 and 22 is reduced by the presence of the notch recess 25, the capacitance between the discharge electrodes 21 and 22 is set to be small. Accordingly, the current for charging and discharging the insulation 1[23] is suppressed to a relatively small value, and the discharge electrode 21.2
The power consumed between the two can be reduced.

そして、上記イオン発生部20で生成されたイオン40
は、直ちにイオン発生部20と略同一箇所に設けられた
イオン流1i1j御部30に到達する。このとき、上記
制御電極31に適宜の画像制御信号33が印加されると
、画像制御信号33が印加された制御電極31と対向制
御電極34との間にイオン流通路13と直交する方向に
電界が形成されることになる。すると、対応するイオン
40部分は上記電界によって制611電極31.34側
へ移動し、その部分で中和されて消滅するため、電界形
成部においてイオン流は遮断される一方、電界非形成部
においてはイオン40はイオン流通路13に導かれた圧
縮空気と共に記録体6側へ向かって通過し、記録体6上
にはイオン流に基づく静電潜像が形成されることになる
。このとき、イオン発生部20とイオン流制御部30と
の間の距離は略零に設定されることから、発生したイオ
ン40がイオン流制御部30に至る途中においてイオン
40が損失するという事態は有効に回避される。
The ions 40 generated by the ion generating section 20 are
immediately reaches the ion flow control section 30 provided at approximately the same location as the ion generation section 20. At this time, when an appropriate image control signal 33 is applied to the control electrode 31, an electric field is generated between the control electrode 31 to which the image control signal 33 is applied and the counter control electrode 34 in a direction perpendicular to the ion flow path 13. will be formed. Then, the corresponding ion 40 portion moves toward the control 611 electrode 31, 34 side by the electric field, and is neutralized and disappears at that portion, so that the ion flow is blocked in the electric field forming portion, while the ion flow is blocked in the electric field non-forming portion. The ions 40 pass toward the recording medium 6 together with the compressed air guided into the ion flow path 13, and an electrostatic latent image is formed on the recording medium 6 based on the ion flow. At this time, since the distance between the ion generation section 20 and the ion flow control section 30 is set to approximately zero, there is no possibility that the generated ions 40 are lost on the way to the ion flow control section 30. effectively avoided.

また、イオン40の損失が抑えられることに伴って、イ
オン流速を不必要に速く設定する必要がなくなり、その
分、圧縮空気流を少なくすることができ、圧縮空気発生
装置の小型化を図ることもできる。
In addition, as the loss of ions 40 is suppressed, it is no longer necessary to set the ion flow rate unnecessarily high, and the compressed air flow can be reduced accordingly, making it possible to downsize the compressed air generator. You can also do it.

尚、上記実施例において、上側放T1電極22の切込み
凹部25の形成密度を画素密度より細がいものとして設
定すれば、上側放電電極22からのイオン量生成分布が
ある程度ばらついているとしても、そのばらつきは有効
に吸収され、イオン流制御部3Gの各画素対応部の通過
イオンmを略均−なものにすることが可能になる。この
とき、静電潜像ドツトの電位を略均−に保つことができ
、その分、現像されたトナー像の濃度むらを確実に回避
することができる。また、上記実施例において、下側放
電電極21にも上側放%fffi極22と同様な切込み
凹部を形成し、両放電電極21.22の実質的重合面積
を極力減少させるようにすれば、放電電極21.22間
の静電容量を更に低減させて、放電電極21.22間で
の消費電力をより低減させることができる。
In the above embodiment, if the formation density of the notch recesses 25 of the upper discharge T1 electrode 22 is set to be thinner than the pixel density, even if the distribution of the amount of ions produced from the upper discharge electrode 22 varies to some extent, the Variations are effectively absorbed, and it becomes possible to make the ions m passing through each pixel corresponding portion of the ion flow control section 3G approximately equal. At this time, the potential of the electrostatic latent image dots can be kept approximately uniform, and density unevenness in the developed toner image can thereby be reliably avoided. Further, in the above embodiment, if the lower discharge electrode 21 is also formed with a notched recess similar to the upper discharge electrode 22, and the substantial overlapping area of both discharge electrodes 21 and 22 is reduced as much as possible, the discharge can be improved. By further reducing the capacitance between the electrodes 21 and 22, the power consumption between the discharge electrodes 21 and 22 can be further reduced.

[発明の効果] 以上説明してきたように、この発明に係る静電記録ヘッ
ドによれば、イオンの生成効率の良いイオン発生部を有
し、しかも、イオン流通路中の略同一箇所にイオン発生
部とイオン流制御部とを設けるようにしたので、イオン
発生部からイオン流制御部へ至る途中でのイオンの損失
をな(すことが可能になり、イオン発生部で多聞に生成
されたイオンを直ちにイオン流制御部に導いて、記録体
側へ送出することができる。このため、イオンの絶対量
を充分に確保することが可能になり、その分、より高速
記録を実現することができる。
[Effects of the Invention] As explained above, the electrostatic recording head according to the present invention has an ion generating section with high ion generation efficiency, and moreover, ions are generated at approximately the same location in the ion flow path. Since the ion flow control section is provided with a section and an ion flow control section, it is possible to eliminate the loss of ions on the way from the ion generation section to the ion flow control section. can be immediately guided to the ion flow control section and sent to the recording medium.Therefore, it is possible to ensure a sufficient absolute amount of ions, and accordingly higher speed recording can be realized.

また、この発明によれば、イオン発生部の構成部材であ
る一方の放電電極をイオン流III御部の一構成部材と
して兼用したので、ヘッド構成の簡略化を図ることもで
きる。
Further, according to the present invention, one of the discharge electrodes, which is a component of the ion generation section, is also used as a component of the ion flow III control section, so that the head configuration can be simplified.

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

第1図はこの発明に係る静電記録ヘッドの一実施例を示
す斜視図、第2図は第1図中n−m線断面図、第3図は
第1図中n−向から見た矢視図、第4図は従来の静電記
録ヘッドの一例を示寸断面説明図、第5図は従来におけ
る静電記録ヘッドの他の例を示す断面説明図、第6図は
第5図中■方向から見た矢視図である。 [符号の説明] (10)・・・ヘッド本体 (20)・・・イオン発生部 (21,22)・・・放電電極 (23)・・・絶縁層 (25)・・・切込み凹部 (30)・・・イオン流制御部 (31)・・・制御電極 (34)・・・対向制tlllli極 特許出願人  富士ゼロックス株式会社代 理 人  
弁理士 中村 凹溝(外2名)第2図 第3図 第4図 フ 第5図 第6図
FIG. 1 is a perspective view showing an embodiment of an electrostatic recording head according to the present invention, FIG. 2 is a cross-sectional view taken along line nm in FIG. 1, and FIG. 3 is a view taken from the n-direction in FIG. 4 is a cross-sectional explanatory diagram showing an example of a conventional electrostatic recording head, FIG. 5 is a cross-sectional explanatory diagram showing another example of a conventional electrostatic recording head, and FIG. It is an arrow view seen from the middle ■ direction. [Explanation of symbols] (10)...Head body (20)...Ion generating portion (21, 22)...Discharge electrode (23)...Insulating layer (25)...Notch recess (30) )...Ion flow control section (31)...Control electrode (34)...Opposed control tlllli electrode Patent applicant Fuji Xerox Co., Ltd. Agent
Patent Attorney Nakamura Konamizo (2 others) Figure 2 Figure 3 Figure 4 Figure 5 Figure 6

Claims (1)

【特許請求の範囲】 1)相対向する絶縁部材間にイオン流通路が形成される
ヘッド本体と、一方の絶縁部材上に一対の放電電極が絶
縁層を介して重合配置されると共に両放電電極間に高周
波高電圧が印加されるイオン発生部と、このイオン発生
部に対向する他方の絶縁部材上に制御電極が画素密度に
応じて配列され且つ各制御電極と上記一方の放電電極を
兼用してなる対向制御電極との間に画像制御信号が印加
されてイオン発生部で発生したイオン流を通過、遮断制
御するイオン流制御部とを備えた静電記録ヘッド。 2)イオン流通路に面した側の放電電極は多数の切込み
凹部を有していることを特徴とする特許請求の範囲第1
項記載の静電記録ヘッド。
[Scope of Claims] 1) A head main body in which an ion flow path is formed between opposing insulating members, and a pair of discharge electrodes on one insulating member are arranged overlappingly with each other with an insulating layer interposed therebetween, and both discharge electrodes are provided. An ion generating section between which a high frequency and high voltage is applied, and control electrodes are arranged on the other insulating member facing the ion generating section according to the pixel density, and each control electrode also serves as one of the discharge electrodes. An electrostatic recording head comprising: an ion flow control section to which an image control signal is applied between a counter control electrode formed of a ion generator and an ion flow control section that controls passage or interruption of an ion flow generated in an ion generation section. 2) Claim 1, characterized in that the discharge electrode on the side facing the ion flow path has a large number of notch recesses.
The electrostatic recording head described in Section 1.
JP22980086A 1986-09-30 1986-09-30 Electrostatic recording head Expired - Lifetime JPH0630908B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22980086A JPH0630908B2 (en) 1986-09-30 1986-09-30 Electrostatic recording head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22980086A JPH0630908B2 (en) 1986-09-30 1986-09-30 Electrostatic recording head

Publications (2)

Publication Number Publication Date
JPS6384944A true JPS6384944A (en) 1988-04-15
JPH0630908B2 JPH0630908B2 (en) 1994-04-27

Family

ID=16897866

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22980086A Expired - Lifetime JPH0630908B2 (en) 1986-09-30 1986-09-30 Electrostatic recording head

Country Status (1)

Country Link
JP (1) JPH0630908B2 (en)

Also Published As

Publication number Publication date
JPH0630908B2 (en) 1994-04-27

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