JPH059020B2 - - Google Patents

Info

Publication number
JPH059020B2
JPH059020B2 JP29136786A JP29136786A JPH059020B2 JP H059020 B2 JPH059020 B2 JP H059020B2 JP 29136786 A JP29136786 A JP 29136786A JP 29136786 A JP29136786 A JP 29136786A JP H059020 B2 JPH059020 B2 JP H059020B2
Authority
JP
Japan
Prior art keywords
electrostatic
recording
dielectric layer
charge
electrostatic recording
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
JP29136786A
Other languages
Japanese (ja)
Other versions
JPS63143554A (en
Inventor
Hirosuke Hamada
So Matsubayashi
Isamu Nakano
Hisanori Yagi
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.)
Kanzaki Paper Manufacturing Co Ltd
Original Assignee
Kanzaki Paper Manufacturing 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 Kanzaki Paper Manufacturing Co Ltd filed Critical Kanzaki Paper Manufacturing Co Ltd
Priority to JP29136786A priority Critical patent/JPS63143554A/en
Priority to EP87117599A priority patent/EP0270032B1/en
Priority to DE3751221T priority patent/DE3751221T2/en
Publication of JPS63143554A publication Critical patent/JPS63143554A/en
Priority to US07/399,441 priority patent/US4944959A/en
Publication of JPH059020B2 publication Critical patent/JPH059020B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G5/00Recording members for original recording by exposure, e.g. to light, to heat, to electrons; Manufacture thereof; Selection of materials therefor
    • G03G5/02Charge-receiving layers
    • G03G5/0202Dielectric layers for electrography

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Electrophotography Using Other Than Carlson'S Method (AREA)
  • Photoreceptors In Electrophotography (AREA)

Description

【発明の詳細な説明】 本発明は、静電記録体の改良に、特に、400ド
ツト/インチなどの高密度記録用静電フアクシミ
リや静電プロツター等に適する静電記録体に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in electrostatic recording media, and particularly to electrostatic recording media suitable for high-density recording such as 400 dots/inch, electrostatic facsimiles, electrostatic plotters, and the like.

(従来技術) 近年、通信技術の進歩に付随して高速度の記録
と高画像品位を同時に満たす記録方法として静電
記録方式に関する技術要求が高まつている。特に
光通信やコンピユーターの端末用機器としてのフ
アクシミリ、プリンター、更にはコンピユーター
を用いる設計技術であるCAD、これらの記録出
力としても静電プリンターが好んで用いられてい
る。
(Prior Art) In recent years, along with advances in communication technology, there has been an increasing technical demand for electrostatic recording as a recording method that simultaneously satisfies high-speed recording and high image quality. In particular, electrostatic printers are preferred for use in optical communications, facsimiles as computer terminal equipment, printers, and CAD, which is a design technology using computers, and for recording and outputting these.

これらの静電記録方式において最も多用されて
いる多針電極型記録方法は、片面制御型と両面制
御型があるが、いずれも静電記録体とは一定の間
隙を保ちながら記録針と記録体の表面が相対する
必要がある。従来の200ドツト/インチの記録密
度の記録では記録針の面積が充分あるためか、そ
の放電の発生そのものには特に問題がなかつた。
ところが400ドツト/インチのような高密度記録
を行うと、細線抜けが生じたり異常放電が発生す
る難点がある。
The multi-needle electrode recording method, which is most commonly used in these electrostatic recording methods, includes single-sided control type and double-sided control type. The surfaces of the two must be facing each other. In the conventional recording with a recording density of 200 dots/inch, there was no particular problem in the occurrence of the discharge itself, probably because the area of the recording needle was sufficient.
However, when performing high-density recording such as 400 dots/inch, there are drawbacks such as missing thin lines and abnormal discharge.

本発明者等は、誘電体層表面の平滑性と画像品
位との関係に注目し、記録針と誘電体層表面の距
離を正確に適切な範囲に収めるため、誘電体層を
形成する樹脂および支持体の導電性も考慮に入れ
ながら、誘電体層表面の表面粗さや凸凹の個数な
どを適度にコントロールする改良を試みてきた
が、細線を描いた場合に正常な放電が起こらず、
細線抜け現象が発生したり、逆に場所によつては
放電が記録針の面積の10倍以上にも達し、画像品
位が低下するいわゆる異常放電発生の問題が依然
として解決されないままでいるのが現状である。
The present inventors focused on the relationship between the smoothness of the surface of the dielectric layer and image quality, and in order to accurately keep the distance between the recording needle and the surface of the dielectric layer within an appropriate range, the inventors of the present invention We have tried to improve the surface roughness of the dielectric layer and the number of irregularities while taking into account the conductivity of the support, but when drawing a thin line, normal discharge did not occur.
The current situation is that the problem of so-called abnormal discharges, which can cause thin line omissions or, in some places, discharges that can reach more than 10 times the area of the recording stylus, degrading image quality, remains unsolved. It is.

(発明が解決しようとする問題点) 本発明は400ドツト/インチのような高密度静
電記録方式に用いる静電記録体で、細線抜けや異
常放電の起こらない鮮明画像が得られる静電記録
体の製造方法を提供することを目的とするもので
ある。
(Problems to be Solved by the Invention) The present invention is an electrostatic recording medium used in high-density electrostatic recording methods such as 400 dots/inch, and is capable of producing clear images without thin lines or abnormal discharge. The purpose of this invention is to provide a method for manufacturing a body.

(問題を解決するための手段) 本発明者等は、前記の問題点は記録体の構成面
からの検討では改良程度に限界があることから、
誘電体層表面への放電、帯電状況について更に研
究を行つた。因に従来から静電記録体の誘電体層
表面は記録画像用の静電荷を印加するまでは静電
荷の存在しない誘電体層表面でなければならない
というのが、技術常識であつた。従つて何等かの
理由によつて誘電体層表面に静電荷が発生した場
合には、これを除去する必要があるというのが従
来の考え方であつた。本発明は一見、このような
技術常識に対して逆行する発想であるが、本発明
者等は記録画像形成のための静電荷を印加する前
に予め印加電荷とは反対極性の静電荷を所望の分
布状態に帯電させておくと、細線抜けや異常放電
の解消になりはしないかとの考えの下に検討を進
めてきたところ、これまで全く予期できなかつた
効果が得られることが発見された。そこで更に検
討を進めたところ、予め誘電体層表面に帯電させ
る静電荷が島状に均一又は不均一に分布させる場
合は、各々の静電荷の径が1μ〜300μの範囲内が
効果的であることが確認された。因みに該静電荷
の長径が1μ以下では効果が乏しく、また300μ以
上になると異常放電が発生し始め、画像品位を低
下させることになる。そこで本発明者等は、予め
誘電体層表面に島状に形成させる静電荷の最大長
径を前記の適正範囲内にコントロールした状態に
形成する手段について検討を進めてきた。その結
果、以下の構成から成る発明に到達した。
(Means for Solving the Problem) The present inventors believe that there is a limit to the degree of improvement in the above-mentioned problem when considering the structure of the recording medium.
Further research was conducted on the discharge and charging conditions on the surface of the dielectric layer. Incidentally, it has conventionally been common general knowledge that the surface of the dielectric layer of an electrostatic recording medium must be free of static charge until an electrostatic charge for a recorded image is applied. Therefore, the conventional thinking has been that if static charges are generated on the surface of the dielectric layer for some reason, it is necessary to remove them. At first glance, the present invention is an idea that goes against such common technical knowledge, but the inventors of the present invention have previously determined that, before applying electrostatic charges for forming a recorded image, they desire electrostatic charges with the opposite polarity to the applied charges. As a result of our research, we have been working on the idea that if the wires are charged to a distribution state of , it might be possible to eliminate thin wire dropouts and abnormal electrical discharges, and it was discovered that a totally unexpected effect could be obtained. . After further investigation, we found that if the static charges that are pre-charged on the surface of the dielectric layer are uniformly or non-uniformly distributed in the form of islands, it is effective if the diameter of each static charge is within the range of 1μ to 300μ. This was confirmed. Incidentally, if the major axis of the electrostatic charge is less than 1μ, the effect is poor, and if it is more than 300μ, abnormal discharge begins to occur, degrading the image quality. Therefore, the inventors of the present invention have conducted studies on a means for controlling the maximum major axis of the electrostatic charges to be formed in the island shape on the surface of the dielectric layer within the above-mentioned appropriate range. As a result, we have arrived at an invention consisting of the following configuration.

即ち、本発明は、導電性支持体上に誘電体層を
有する、記録画像形成のための静電荷を多針電極
からの放電で印加する静電記録方式用の静電記録
体の製造方法であり、誘電体層表面を絶縁性物質
及び導電性物質とで摩擦することにより該誘電体
層表面に予め記録画像用の印加電荷とは反対極性
の静電荷を形成することを特徴とする静電記録体
の製造方法である。
That is, the present invention is a method for manufacturing an electrostatic recording medium for an electrostatic recording method, which has a dielectric layer on a conductive support and applies electrostatic charge for forming a recorded image by discharging from a multi-needle electrode. Electrostatic charge is characterized in that an electrostatic charge of the opposite polarity to the charge applied for recording images is previously formed on the surface of the dielectric layer by rubbing the surface of the dielectric layer with an insulating substance and a conductive substance. This is a method for manufacturing a recording medium.

(作用) 上記の構成で、誘電体層表面に予め記録画像用
の印加電荷とは反対極性の静電荷を付与するため
用いる絶縁性物質としては高分子化合物、例えば
ポリエチレン、ポリプロピレン、ポリスチレン、
ブチラール、ポリ酢酸ビニル、ポリエステル、ポ
リ塩化ビニル、ポリアクリレート、ポリエーテ
ル、又はこれらの共重合体等の熱可塑性樹脂、メ
ラミン−ホルマリン樹脂、尿素−ホルマリン樹
脂、フエノール−ホルマリン樹脂、エポキシ樹脂
等の熱硬化性樹脂等が使用でき、また導電性物質
としては高分子電解質、アニオン、ノニオン、カ
チオンあるいは両性イオン等の界面活性剤、金属
半導体粉末等が使用できる。スチレンとアクリル
酸エステル第4級アンモニウム塩の共重合体など
のように、一分子内に絶縁性と導電性の両セグメ
ントを有するものであつてもよい。
(Function) In the above configuration, the insulating substance used to previously apply an electrostatic charge of opposite polarity to the charge applied for recording images to the surface of the dielectric layer is a polymer compound such as polyethylene, polypropylene, polystyrene,
Thermoplastic resins such as butyral, polyvinyl acetate, polyester, polyvinyl chloride, polyacrylate, polyether, or copolymers thereof, melamine-formalin resin, urea-formalin resin, phenol-formalin resin, epoxy resin, etc. A curable resin or the like can be used, and as the conductive substance, a polymer electrolyte, a surfactant such as anion, nonion, cation or amphoteric ion, metal semiconductor powder, etc. can be used. The material may have both insulating and conductive segments in one molecule, such as a copolymer of styrene and acrylic acid ester quaternary ammonium salt.

而して、本発明の構成で絶縁性物質及び導電性
物質というのは、各々別のものであつてもよい
し、また一体物に構成したものであつてもよいと
いう意味である。例えば絶縁性物質と導電性物質
の各々の単独を棒状又はロール状に成形したも
の、あるいは導電性物質を絶縁性物質に混練して
棒状又はロール状に成形したもの、更には、これ
らの物質をシート状物に塗布又は含浸させ、それ
を棒状体又はロール状体に巻きつけた形態のもの
にして使用してもよい。
Thus, in the structure of the present invention, the insulating substance and the conductive substance may be separate substances, or may be formed into an integrated substance. For example, an insulating substance and a conductive substance individually formed into a rod or a roll, or a conductive substance mixed with an insulating substance and formed into a rod or a roll, and furthermore, It may also be used by coating or impregnating a sheet material and winding it around a rod or roll.

上記、絶縁性物質と導電性物質で誘電体層表面
を摩擦する場合、それぞれが別々に構成されたも
のである場合には、その摩擦順序は絶縁性物質で
先づ摩擦し、次いで導電性物質で摩擦するのが効
果的である。そして絶縁性物質と導電性物質とを
混在させ、一体物として成形したものを使用する
場合は、それをそのまま誘電体層表面に摩擦させ
るだけでよい。
When rubbing the surface of a dielectric layer with an insulating material and a conductive material as described above, if each is configured separately, the order of friction is that the insulating material is rubbed first, then the conductive material is rubbed. It is effective to rub it with If an insulating material and a conductive material are mixed and molded into an integral product, it is sufficient to simply rub the material as it is against the surface of the dielectric layer.

因みに、絶縁性物質のみで誘電体層表面を摩擦
し、静電荷を形成せしめた際には、各々の静電荷
は大小さまざまなものが発生し、最大が300μを
こえるものが多数存在することになる。そこで
300μ以上の巨大な静電荷については、導電性物
質との摩擦によつて1〜300μの範囲内となるよ
うに調節されることになる。なお、この調節は、
導電性物質が絶縁性物質とは別に構成されている
ものである場合は、導電性物質との摩擦によつて
行われ、また、導電性物質と絶縁性物質とが一体
物に成形されたもの、あるいは導電性セグメント
と絶縁性セグメントとを1分子内に含む物質であ
る場合には、その成形物で摩擦した際に静電荷の
発生と同時に1〜300μの範囲内に調節されるこ
とになる。なお、静電荷は1〜300μの範囲が望
ましいわけであるが、記録像の解像性の面からし
て、より望ましくは各々のピン電極の最大径より
も小さい範囲内に調節するのがよい。
By the way, when the surface of a dielectric layer is rubbed with only an insulating material and static charges are formed, each static charge is generated in a variety of sizes, and there are many with a maximum of over 300μ. Become. Therefore
A huge electrostatic charge of 300μ or more will be adjusted to within the range of 1 to 300μ by friction with a conductive material. Note that this adjustment is
If the conductive material is composed separately from the insulating material, this is done by friction with the conductive material, or if the conductive material and the insulating material are formed into one piece. , or in the case of a substance containing a conductive segment and an insulating segment in one molecule, when it is rubbed with a molded product, an electrostatic charge is generated and the charge is adjusted within the range of 1 to 300μ. . The electrostatic charge is preferably in the range of 1 to 300μ, but in terms of the resolution of the recorded image, it is more desirable to adjust it within a range smaller than the maximum diameter of each pin electrode. .

誘電体層表面に上記した径の静電荷を形成する
には、静電記録体の製造工程において、その最終
工程でシートにかかる弾力を利用して摩擦し付与
しておくのもよいし、また、例えば記録装置に画
像形成用のための印加装置とは別に上記静電荷の
付与装置を内蔵させておき、記録直前に付与する
方式を採つてもよい。
In order to form an electrostatic charge having the diameter described above on the surface of the dielectric layer, it is possible to apply it by friction using the elasticity applied to the sheet in the final step of the manufacturing process of the electrostatic recording medium, or For example, a method may be adopted in which the recording apparatus has a built-in device for applying the electrostatic charge, separate from the application device for image formation, and applies the electrostatic charge immediately before recording.

誘電体層表面に予め付与する静電荷の極性は記
録方式により正極性でも負極性のいずれを選択し
てもよいわけであるが、現在の静電記録方式が負
極性の放電が正極性に比べ放電効率が良いことか
ら負極性を利用するケースが多く、そのため予め
付与する静電荷の極性は正極性を付与するのが望
ましい。以下に印加される記録画像用電荷とは反
対極性の静電荷を形成する場合を説明する。
The polarity of the electrostatic charge applied in advance to the surface of the dielectric layer can be either positive or negative depending on the recording method, but current electrostatic recording methods have a negative polarity discharge compared to a positive polarity discharge. Negative polarity is often used because of its good discharge efficiency, and therefore it is desirable that the electrostatic charge applied in advance be of positive polarity. A case in which electrostatic charges having a polarity opposite to the charges for a recorded image to be applied are formed will be described below.

静電記録装置で印加される記録画像用電荷が負
極性では、先づ誘電体層を正極性に帯電させ物質
で摩擦処理する。この工程で形成される静電荷は
電子顕微鏡による観察によると、大きさが不規則
であり島状に分布しているか、全体に網目状に分
布している。このような分布状態のまま静電記録
装置で細線の記録をとると、細線抜けは改良され
るものの、異常放電は増加しており良好な記録は
得られない。しかし導電性物質でさらに摩擦処理
すると島状に分布する各正極性の電荷の広がりが
ほぼ1〜300μに揃い、その結果細線、特に1ド
ツト記録時の細線抜けを全く無くすのみならず、
1ドツト記録時に特に多く発生する異常放電の数
を極めて少なくすることが出来る。本発明による
特定の摩擦処理により得られる改良効果は処理1
年後においても認められる。
If the charge for recording images applied by the electrostatic recording device is of negative polarity, the dielectric layer is first charged to positive polarity and subjected to friction treatment with a substance. According to observation using an electron microscope, the electrostatic charges formed in this process are irregular in size and distributed in islands or in a mesh pattern throughout. If thin lines are recorded with an electrostatic recording device in such a distribution state, thin line omissions will be improved, but abnormal discharge will increase and good recording will not be obtained. However, when subjected to further friction treatment with a conductive material, the spread of each positive polarity charge distributed in an island shape becomes approximately equal to 1 to 300μ, and as a result, not only does it completely eliminate thin lines, especially when recording single dots, but also
The number of abnormal discharges that occur particularly frequently during one-dot recording can be extremely reduced. The improvement effect obtained by the specific friction treatment according to the present invention is treatment 1.
It will be recognized even after 2000 years.

而して、誘電体層表面に予め記録画像を形成す
るための印加電荷とは反対極性の静電荷を形成さ
せることが400ドツト/インチなどの高密度記録
用静電フアクシミリや静電プロツタ等に適し、殊
に細線を描く場合に細線抜け防止に顕著な効果が
得られる理由は、正確なことについては必ずしも
明らかではないが、誘電体層表面に予め例えば正
極性の静電荷を形成しておき、記録する場合は、
予め正極性の静電荷を形成しないで記録する場合
に比べて放電開始電圧の低下があるためか、より
確実な放電が発生するのではないかと考えられ
る。
Therefore, it is possible to form an electrostatic charge of the opposite polarity to the charge applied to previously form a recorded image on the surface of the dielectric layer in electrostatic facsimile machines and electrostatic plotters for high-density recording such as 400 dots/inch. The exact reason why a remarkable effect is obtained in preventing thin lines from falling out, especially when drawing thin lines, is not necessarily clear, but the reason why a positive electrostatic charge is formed in advance on the surface of the dielectric layer is , if you want to record,
It is thought that more reliable discharge occurs, probably because the discharge starting voltage is lower than when recording is performed without forming positive electrostatic charges in advance.

次に、静電記録体を構成するための導電性支持
体としては、塩化ナトリウムのような無機塩、ポ
リビニルベンジルトリメチルアンモニウムクロラ
イドなどのカチオンあるいはアニオンの高分子電
解質、界面活性剤、あるいは酸化亜鉛、導電性処
理した酸化亜鉛等の金属酸化物半導体を含浸ない
しは塗布し、表面抵抗105〜1011Ωとなした紙、プ
ラスチツクフイルム、布等が使用される。静電記
録体を構成する誘電体層としては、樹脂として、
ブチラール樹脂、ポリアクリレート、ポリスチレ
ン、ポリ酢酸ビニル、ポリエステルなどの誘導体
や共重合体である絶縁性樹脂を単体又は混合体で
使用し、これに含有させるスペーサー用顔料とし
ては炭酸カルシウム、酸化チタン、無定形シリ
カ、クレー等の無機顔料やポリエチレンや、ポリ
スチレン等を成分とするプラスチツク顔料等を使
用することになる。以下、本発明の実施例を記載
するが、本発明がこれらの実施例に限定されるも
のでないことは勿論である。
Next, as the conductive support for forming the electrostatic recording material, inorganic salts such as sodium chloride, cationic or anionic polymer electrolytes such as polyvinylbenzyltrimethylammonium chloride, surfactants, or zinc oxide, Paper, plastic film, cloth, etc. impregnated or coated with a conductive-treated metal oxide semiconductor such as zinc oxide to have a surface resistance of 10 5 to 10 11 Ω are used. As the dielectric layer constituting the electrostatic recording medium, as a resin,
Insulating resins, which are derivatives or copolymers of butyral resin, polyacrylate, polystyrene, polyvinyl acetate, polyester, etc., are used singly or as a mixture, and the spacer pigments to be contained in these resins include calcium carbonate, titanium oxide, and insulating resins. Inorganic pigments such as regular silica and clay, and plastic pigments containing polyethylene, polystyrene, etc., are used. Examples of the present invention will be described below, but it goes without saying that the present invention is not limited to these Examples.

〔静電記録体の調製〕[Preparation of electrostatic recording medium]

メチルメタアクリレートとエチルアクリレート
の1:1共重合体樹脂と炭酸カルシウムを1:1
の重量比で混合して調製した誘電体層形成用の塗
料を導電性支持体上に乾燥重量で5g/m2となる
ように塗布し静電記録体を用意した。
1:1 copolymer resin of methyl methacrylate and ethyl acrylate and 1:1 calcium carbonate
An electrostatic recording medium was prepared by coating a coating material for forming a dielectric layer prepared by mixing at a weight ratio of 5 g/m 2 on a conductive support so as to have a dry weight of 5 g/m 2 .

実施例 1 メチルエチルケトン200重量部、ポリスチレン
80重量部、カチオン系界面活性剤(商品名「カチ
オンBB」日本油脂(株)製)20重量部とを混合して
調製した樹脂液を上質紙に乾燥重量で10g/m2
なるように塗布乾燥した後、直径150mmのポリス
チレン棒に塗布面が外側となるように巻きつけ
た。かかる物質で予め用意した前記の静電記録体
の誘電体層表面を常温、常湿下で押え圧260g/
cm2、スピード10m/分で摩擦し本発明にかかる静
電記録体とした。
Example 1 200 parts by weight of methyl ethyl ketone, polystyrene
A resin liquid prepared by mixing 80 parts by weight of a cationic surfactant (product name: "Cation BB" manufactured by NOF Corporation) with 20 parts by weight was applied to high-quality paper so that the dry weight was 10 g/ m2 . After the coating was dried, it was wrapped around a polystyrene rod with a diameter of 150 mm with the coated side facing outward. The surface of the dielectric layer of the electrostatic recording material prepared in advance using such a substance was pressed at room temperature and humidity with a pressure of 260 g/
cm 2 at a speed of 10 m/min to obtain an electrostatic recording material according to the present invention.

摩擦後、該誘電体層表面の表面電位を測定する
と+2Vを示していた。そしてこの静電荷の大き
さは、電子顕微鏡(日本電子JSM−T−300)で
加速電圧2キロボルトにて2次電子像を観察(正
極性の静電荷は黒く表現され、負極性の静電荷は
白く表現される。)すると300μ以上のものは殆ど
見られなかつた。この摩擦後の静電記録体に針電
極に負の電圧を印加する松下電送(株)製の静電プロ
ツターEP−101で1ドツト記録を行うと第1図の
如く、細線抜け及び異常放電も少なく、良好な記
録適性を示した。
After the friction, the surface potential of the dielectric layer surface was measured and found to be +2V. The magnitude of this electrostatic charge can be determined by observing a secondary electron image using an electron microscope (JEOL JSM-T-300) at an accelerating voltage of 2 kilovolts (positive electrostatic charges are expressed in black, negative electrostatic charges are (It is expressed as white.) Then, there were almost no objects larger than 300μ. When a single dot is recorded using an electrostatic plotter EP-101 manufactured by Matsushita Densen Co., Ltd., which applies a negative voltage to the needle electrode on the electrostatic recording medium after friction, as shown in Figure 1, thin lines and abnormal discharges occur. It showed good recording aptitude.

実施例 2 メチルエチルケトン200重量部中に、ポリスチ
レン樹脂20重量部を溶解し、更に、導電性酸化亜
鉛粉末の10重量部を混合して調製した樹脂液を上
質紙に乾燥重量で10g/m2となるように塗布乾燥
した後、スーパーキヤレンダー掛けして塗布面を
平滑化した後、直径150mmのポリスチレン棒に塗
布面が外側となるように巻きつけた。かかる物質
で予め用意した前記の静電記録体の誘電体層表面
を常温、常湿下で押え圧260g/cm2、スピード10
m/分で摩擦し本発明にかかる静電記録体とし
た。
Example 2 A resin solution prepared by dissolving 20 parts by weight of polystyrene resin in 200 parts by weight of methyl ethyl ketone and further mixing 10 parts by weight of conductive zinc oxide powder was spread on high-quality paper at a dry weight of 10 g/ m2 . After coating and drying, the coated surface was smoothed using a supercalender, and then wrapped around a polystyrene rod with a diameter of 150 mm with the coated surface facing outward. The surface of the dielectric layer of the electrostatic recording material previously prepared using such a substance was pressed at room temperature and humidity with a pressure of 260 g/cm 2 and a speed of 10.
The electrostatic recording material according to the present invention was obtained by rubbing at a speed of m/min.

摩擦後、該誘電体層表面の表面電位を測定する
と+1.5Vを示していた。そしてこの静電荷の大
きさは、実施例1に記載と同じ電子顕微鏡で観測
すると300μ以上のものは殆ど見られなかつた。
この摩擦後の静電記録体に針電極に負の電圧を印
加する松下電送(株)製の静電プロツターEP−101で
1ドツト記録を行うと第2図の如く細線抜け及び
異常放電は少なく、良好な記録適性を示した。
After the friction, the surface potential of the dielectric layer surface was measured and found to be +1.5V. When the electrostatic charge was observed using the same electron microscope as described in Example 1, almost no electrostatic charge larger than 300 μm was observed.
When one-dot recording is performed using an electrostatic plotter EP-101 manufactured by Matsushita Densen Co., Ltd., which applies a negative voltage to the needle electrode on the electrostatic recording medium after friction, there are few thin line omissions and abnormal discharges as shown in Figure 2. , showed good recording aptitude.

実施例 3 直径150mmのポリスチレン棒で予め用意した前
記の静電記録体の誘電体層表面を常温、常湿下で
押え圧260g/cm2、スピード10m/分で摩擦した。
この誘電体層表面を更に両性界面活性剤(商品名
「アンヒトール24B」花王(株)製)を上質紙に乾燥
重量で5g/m2となるように塗布乾燥し、その塗
布面が外側になるように巻きつけた直径150mmの
ポリスチレン棒で押え圧100g/cm2、スピード10
m/分で摩擦し本発明にかかる静電記録体とし
た。
Example 3 A polystyrene rod with a diameter of 150 mm was rubbed against the surface of the dielectric layer of the electrostatic recording material prepared in advance at room temperature and humidity at a pressing pressure of 260 g/cm 2 and a speed of 10 m/min.
On the surface of this dielectric layer, an amphoteric surfactant (trade name "Anhitor 24B" manufactured by Kao Corporation) is further coated on high-quality paper to a dry weight of 5 g/m 2 and dried, with the coated surface facing outward. Using a polystyrene rod with a diameter of 150 mm wrapped around the
The electrostatic recording material according to the present invention was obtained by rubbing at a speed of m/min.

摩擦後、該誘電体層表面の表面電位を測定する
と+2Vを示していた。そしてその静電荷の大き
さは、実施例1に記載と同じ電子顕微鏡で観測す
ると300μ以上のものは殆ど見られなかつた。こ
の摩擦後の静電記録体に針電極に負の電圧を印加
する松下電送(株)製の静電プロツターEP−101で1
ドツト記録を行うと第3図の如く細線抜け及び異
常放電は少なく、良好な記録適性を示した。
After the friction, the surface potential of the dielectric layer surface was measured and found to be +2V. When the electrostatic charge was observed using the same electron microscope as described in Example 1, almost no electrostatic charge larger than 300 μm was observed. After this friction, an electrostatic plotter EP-101 manufactured by Matsushita Densen Co., Ltd. is used to apply a negative voltage to the needle electrode on the electrostatic recording medium.
When dot recording was performed, as shown in FIG. 3, there were few thin line omissions and abnormal discharges, indicating good recording suitability.

比較例 1 予め用意した前記の静電記録体をそのまま松下
電送(株)製の静電プロツターEP−101で1ドツト記
録を行つた。その結果、第4図の如く細線抜けが
多く、本発明に係る静電記録体と比較すると記録
適性は、はるかに劣つていた。
Comparative Example 1 One-dot recording was performed on the electrostatic recording medium prepared in advance using an electrostatic plotter EP-101 manufactured by Matsushita Densen Co., Ltd. As a result, as shown in FIG. 4, there were many thin lines missing, and the recording suitability was far inferior to that of the electrostatic recording material according to the present invention.

比較例 2 直径150mmのポリスチレン棒で、予め用意した
前記の静電記録体の誘電体層表面を常温、常湿下
で、押え圧260g/cm2、スピード10m/分で摩擦
した。
Comparative Example 2 A polystyrene rod with a diameter of 150 mm was rubbed against the surface of the dielectric layer of the electrostatic recording material previously prepared at room temperature and humidity at a presser pressure of 260 g/cm 2 and a speed of 10 m/min.

摩擦後、該誘電体層表面の表面電位を測定する
と+2Vを示していた。そしてその静電荷の大き
さは実施例1に記載と同じ電子顕微鏡で観測する
と300μ以上のものが多数(5cm×5cmの枠内に
200個)存在しているのが確認された。この摩擦
後の静電記録体に針電極に負の電圧を印加する松
下電送(株)製の静電プロツターEP−101で1ドツト
記録を行うと第5図の如く、細線抜けは比較例1
の場合に比較しても格段に向上しているものの、
異常放電が多く発生し、本発明に係る静電記録体
と比較する記録適性は、はるかに劣つていた。
After the friction, the surface potential of the dielectric layer surface was measured and found to be +2V. When observed with the same electron microscope as described in Example 1, many of the electrostatic charges were larger than 300μ (within a frame of 5cm x 5cm).
200 pieces) were confirmed to exist. When a single dot was recorded on the electrostatic recording medium after friction using an electrostatic plotter EP-101 manufactured by Matsushita Electric Transmission Co., Ltd., which applied a negative voltage to the needle electrode, as shown in Figure 5, there were no thin lines missing in Comparative Example 1.
Although this is a significant improvement compared to the case of
Many abnormal discharges occurred, and the recording suitability was far inferior to that of the electrostatic recording medium according to the present invention.

比較例 3 スチレンとメチルメタアクリレートが3:1の
割合から成る共重合体と、両性界面活性剤(商品
名「アンヒトール24B」花王(株)製)を80重量部対
20重量部の割合で混合し、上質紙に乾燥重量て10
g/m2となるように塗布乾燥し、その塗布面が外
側になるように巻きつけた直径150mmのポリスチ
レン棒で、押え圧260g/cm2、スピード10m/分
で摩擦した。
Comparative Example 3 80 parts by weight of a copolymer consisting of styrene and methyl methacrylate in a ratio of 3:1 and an amphoteric surfactant (trade name "Amhitol 24B" manufactured by Kao Corporation)
Mix at a ratio of 20 parts by weight and dry weight 10 on high-quality paper.
g/m 2 and dried, and rubbed with a 150 mm diameter polystyrene rod wound around the coated surface at a presser pressure of 260 g/cm 2 and a speed of 10 m/min.

摩擦後、該誘電体層表面の表面電位を測定する
と−1Vを示していた。そしてこの静電荷の大き
さは、実施例1に記載と同じ電子顕微鏡で観測す
ると300μ以上のものは殆ど見られなかつた。こ
の摩擦後の静電記録体に針電極に負の電圧を印加
する松下電送(株)製の静電プロツターEP−101で1
ドツト記録を行うと第6図の如く細線抜けが多
く、本発明に係る静電記録体と比較すると記録適
性ははるかに劣つていた。
After the friction, the surface potential of the dielectric layer surface was measured and found to be -1V. When the electrostatic charge was observed using the same electron microscope as described in Example 1, almost no electrostatic charge larger than 300 μm was observed. After this friction, an electrostatic plotter EP-101 manufactured by Matsushita Densen Co., Ltd. is used to apply a negative voltage to the needle electrode on the electrostatic recording medium.
When dot recording was performed, there were many thin lines missing as shown in FIG. 6, and the recording suitability was far inferior to that of the electrostatic recording material according to the present invention.

(効果) 本発明にかかる静電記録体は、400ドツト/イ
ンチのような高密度静電記録方式に用いた場合で
も、細線抜けや異常放電の起こらない鮮明な記録
画像を得ることができる。
(Effects) Even when the electrostatic recording medium according to the present invention is used in a high-density electrostatic recording system such as 400 dots/inch, it is possible to obtain clear recorded images without thin line omissions or abnormal discharge.

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

第1図から第3図は実施例1〜3に於いて記載
した本発明にかかる静電記録体に、針電極に負の
電圧を印加する静電プロツターで1ドツト記録を
行つたときの記録適性を示した見本であり、第4
図から第6図は、比較例1〜3に於いて記載した
静電記録体に針電極に負の電圧を印加する静電プ
ロツターで1ドツト記録を行つたときの記録適性
を示した見本である。
Figures 1 to 3 show records when one dot recording was performed on the electrostatic recorder according to the present invention described in Examples 1 to 3 using an electrostatic plotter that applied a negative voltage to the needle electrode. It is a sample of aptitude, and the fourth
Figures 6 to 6 are samples showing the recording suitability when one dot recording is performed on the electrostatic recording medium described in Comparative Examples 1 to 3 using an electrostatic plotter that applies a negative voltage to the needle electrode. be.

Claims (1)

【特許請求の範囲】[Claims] 1 導電性支持体上に誘電体層を有する、記録画
像形成のための静電荷を多針電極からの放電で印
加する静電記録方式用の静電記録体の製造方法で
あり、誘電体層表面を絶縁性物質及び導電性物質
とで摩擦することにより該誘電体層表面に予め記
録画像用の印加電荷とは反対極性の静電荷を形成
することを特徴とする静電記録体の製造方法。
1 A method for producing an electrostatic recording medium for an electrostatic recording method, which has a dielectric layer on a conductive support and applies electrostatic charge for forming a recorded image by discharge from a multi-needle electrode, and the dielectric layer A method for producing an electrostatic recording material, characterized in that an electrostatic charge having a polarity opposite to that applied for a recorded image is previously formed on the surface of the dielectric layer by rubbing the surface with an insulating material and a conductive material. .
JP29136786A 1986-11-29 1986-12-05 Electrostatic recording body Granted JPS63143554A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP29136786A JPS63143554A (en) 1986-12-05 1986-12-05 Electrostatic recording body
EP87117599A EP0270032B1 (en) 1986-11-29 1987-11-27 Electrostatic recording method
DE3751221T DE3751221T2 (en) 1986-11-29 1987-11-27 Electrostatic recording method.
US07/399,441 US4944959A (en) 1986-11-29 1989-08-28 Process for electrostatic recording comprising charging dielectric sheet to polarity opposite of imaging charge

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29136786A JPS63143554A (en) 1986-12-05 1986-12-05 Electrostatic recording body

Publications (2)

Publication Number Publication Date
JPS63143554A JPS63143554A (en) 1988-06-15
JPH059020B2 true JPH059020B2 (en) 1993-02-03

Family

ID=17767999

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29136786A Granted JPS63143554A (en) 1986-11-29 1986-12-05 Electrostatic recording body

Country Status (1)

Country Link
JP (1) JPS63143554A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0365957A (en) * 1989-08-04 1991-03-20 Tomoegawa Paper Co Ltd Electrostatic recording body
JPH061383B2 (en) * 1990-03-23 1994-01-05 株式会社巴川製紙所 Electrostatic recording body

Also Published As

Publication number Publication date
JPS63143554A (en) 1988-06-15

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