JPS58208772A - Method for inverse development - Google Patents

Method for inverse development

Info

Publication number
JPS58208772A
JPS58208772A JP9130682A JP9130682A JPS58208772A JP S58208772 A JPS58208772 A JP S58208772A JP 9130682 A JP9130682 A JP 9130682A JP 9130682 A JP9130682 A JP 9130682A JP S58208772 A JPS58208772 A JP S58208772A
Authority
JP
Japan
Prior art keywords
toner
magnetic
image
photoreceptor
latent image
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.)
Pending
Application number
JP9130682A
Other languages
Japanese (ja)
Inventor
Eiichi Kato
栄一 加藤
Yasuaki Yuyama
湯山 泰明
Shuichi Otsuka
秀一 大塚
Keiichi Yamana
山名 啓一
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 Holdings Corp
Original Assignee
Fuji Photo Film 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 Photo Film Co Ltd filed Critical Fuji Photo Film Co Ltd
Priority to JP9130682A priority Critical patent/JPS58208772A/en
Publication of JPS58208772A publication Critical patent/JPS58208772A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G13/00Electrographic processes using a charge pattern
    • G03G13/06Developing
    • G03G13/08Developing using a solid developer, e.g. powder developer
    • G03G13/09Developing using a solid developer, e.g. powder developer using magnetic brush

Abstract

PURPOSE:To obtain many fine copies without the generation of fog and the change of density by using magnetic toner consisting of one component which is agitated in a magnetic field in the method to inversely develop an electrostatic latent image into a toner image by magnetic brush method. CONSTITUTION:After forming an electrostatic latent image on an electrophotographic receptor 4 obtained by forming a photoconductive layer 1 (e.g. a layer obtained by dispersing zinc oxide into a bonding agent) on a conductive supporting element 2, the latent image is developed into a toner image by magnetic toner 7 through a non-magnetic sleeve 8 (to which bias voltage having the same polarity as the surface potential of the photoreceptor 1 is applied) to be rotated relatively to a magnetic roll 10. For said toner, toner obtained by agitating (by using an insulated case 5 and an agitator 6) unmagnetized toner 3 (about <=35wt% of <=15mu grain size and about <=3wt% of <=10mu grain size) consisting of an adhering agent and magnetic powder for 5min-10hr at about 5-60 deg.C under about <=700 gausses of magnetic field generated by a coil 11 is used.

Description

【発明の詳細な説明】 本発明は電子写真における一成分磁性トナーを用いた磁
気プツシ現像法による反転現像方法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a reversal development method using a magnetic push development method using a one-component magnetic toner in electrophotography.

従来、露光中に光を受けた部分にトナー粒子を耐着させ
可視像化する反転現像方法では、マグネットローラを用
いた磁気ブラシ現像方法が一般的に知られており、特公
昭56.−2705号、特開昭53−112740号、
特開昭53−115299号、特開昭54−98,24
8号及び特開昭52−146243号公報等に開示され
ている。即ち、第1図に示すように、例えばシリンダー
形状の導電性の非磁性体スリーブ8を有し、非磁性体ス
リーブ8は内部に配置されたマグネットロー210と相
対的に回転可能に支持され、非磁性体スIJ−プ8は潜
像の形成された感光体4上の光導電層10表表面位と同
一極性で同じオーダの電位を有し、そして比較的高抵抗
のトナー(107〜1014Ω・cIIL)を非磁性体
スリーブ80表面に搬送させ、現像に供される感光体面
と接触させて現像する。
Conventionally, in the reversal development method in which toner particles are made to adhere to the areas that received light during exposure and are visualized, a magnetic brush development method using a magnet roller is generally known, and was published in Japanese Patent Publication No. 1983. -2705, JP-A-53-112740,
JP-A-53-115299, JP-A-54-98, 24
No. 8 and Japanese Unexamined Patent Publication No. 146243/1983. That is, as shown in FIG. 1, it has, for example, a cylinder-shaped conductive non-magnetic sleeve 8, and the non-magnetic sleeve 8 is rotatably supported relative to a magnet row 210 disposed inside. The non-magnetic strip 8 has the same polarity and potential on the same order as the surface of the photoconductive layer 10 on the photoreceptor 4 on which the latent image is formed, and has a relatively high resistance toner (107 to 1014 Ω). cIIL) is conveyed to the surface of the non-magnetic sleeve 80, brought into contact with the surface of the photoreceptor to be developed, and developed.

このような現像装置に一成分磁性トナーを用いる事は複
写機全体の小型化及びメンテナンスフリー、更にトナー
濃にのコントロールが不要なことなどで優れている。本
発明者等が酸化亜鉛粒子を結着剤中に分散した光導電層
を導電性支持体上に有した感光体を用いて反転現像を行
なった処、著しくカプリの多いコントラストの小さい画
像しか得られないことが判った。
The use of one-component magnetic toner in such a developing device is advantageous in that the entire copying machine can be made smaller, maintenance-free, and there is no need to control toner density. When the present inventors performed reversal development using a photoreceptor having a photoconductive layer on a conductive support in which zinc oxide particles were dispersed in a binder, only images with a significantly large amount of capri and low contrast were obtained. It turned out that I couldn't do it.

一成分磁性トナーを用いた磁気ノラシ現像法を用いて反
転現像を行なって、カプリがなく、コントラストの良好
な画像を得る方法が特開昭55−134864号公報に
開示されている。この方法は上記−成分磁性トナーを用
いた磁気ブラシ現像法を用いて反転現像を行なう際に、
感光体の帯電しはルを飽和帯電電位(感光体の帯電しう
る最大の表面電位)よりも極めて低い、例えば該飽和帯
電電位の60%程度の電位に抑えて帯電しく非飽和帯電
)、更に現像に際してこの表面電位と同極性でしかもほ
ぼ同等かあるいはこれより若干高い電位を一成分磁性ト
ナーに付与して現像する方法である。
JP-A-55-134864 discloses a method for obtaining an image with no capri and good contrast by performing reversal development using a magnetic nozzle development method using a one-component magnetic toner. In this method, when performing reversal development using the magnetic brush development method using the above-mentioned -component magnetic toner,
The photoreceptor is charged by suppressing the charging potential to a potential that is extremely lower than the saturation charging potential (the maximum chargeable surface potential of the photoreceptor), for example, about 60% of the saturation charging potential (non-saturated charging), and This is a method of developing by applying a potential to the one-component magnetic toner that has the same polarity as this surface potential and is approximately equal to or slightly higher than this surface potential.

この方法によれば、−成分磁性トナーを用いた磁気プラ
ン現像法を用いて正現像を行なって得た画像と同等にカ
プリがなく、コントラストの良好な画像を反転現像によ
って得ることが可能となるが、同時に次の如き欠点を併
せ持つこととなる。
According to this method, it is possible to obtain an image by reversal development that is free from capri and has good contrast, equivalent to an image obtained by normal development using a magnetic plan development method using -component magnetic toner. However, it also has the following drawbacks:

即ち、この方法では感光体表面の帯電電位を正確に制御
することが必要であり、その実現のためにコロナワイヤ
用の電源と該コロナワイヤからの電荷の量を制御するグ
リッド用の電源とを必要とする所謂スコロトロンを用い
る必要があるので得られる装置がコスト高となるを得ず
又装置自体も大型化してしまう。又、スコロトロンを用
いて良好な現像を行ないうる一定値以上の帯電電位とな
るまで帯電を行なう場合にはコロトロンを用いる場合に
比して著しく帯電に時間がかかり、高速化に難点がある
3、又この高速化を行なうためにスコロトロンとコロト
ロンを併用する考案が特開昭55−144260号公報
に開示されているが、これによっても依然として前者の
欠点は残シ、更にスコロトロン単独を用いるよりも更に
装置が複雑化、大型化及び、装置の使用コスト高化にな
らざるを得ない。
That is, in this method, it is necessary to accurately control the charging potential on the surface of the photoreceptor, and in order to achieve this, a power source for the corona wire and a power source for the grid that controls the amount of charge from the corona wire are required. Since it is necessary to use a so-called scorotron, the cost of the resulting device is inevitably high, and the device itself becomes large. Furthermore, when charging is performed using a scorotron until the charging potential reaches a certain value or higher that allows good development, it takes much longer to charge than when using a corotron, making it difficult to increase the speed 3. In addition, in order to increase the speed, a method of using a scorotron and a corotron in combination is disclosed in Japanese Patent Application Laid-Open No. 144260/1982, but even with this, the drawbacks of the former still remain, and furthermore, it is even more difficult than using a scorotron alone. This inevitably increases the complexity and size of the device, and increases the cost of using the device.

本発明者らは先に、特願昭56−196627号にてこ
れら問題を解決するために、−成分磁性トナーの電気抵
抗値及びその抗磁力を特定領域に設定することにより、
カプリのないコントラストの良好な画像が得られること
を提案した。
The present inventors previously proposed in Japanese Patent Application No. 56-196627 that in order to solve these problems, by setting the electric resistance value of the -component magnetic toner and its coercive force in a specific range,
It was proposed that images with good contrast without capri can be obtained.

即ち、該発明の電子写真現像方法は飽和電位まで帯電さ
れ、画像露光によって静電潜像が形成された電子写真感
光体に、バイアス電位印加手段によって前記感光体の帯
電電位と同極性の電位が印加された一成分磁性トナーに
よって磁気ブラシ法により反転現像を行なう電子写真現
像方法において、−成分磁性トナーが107Ω・錦以上
でかつ電荷交換が行なわれる範囲の電気抵抗を有し、1
50工ルステツド以上の抗磁力を有するものを用いるこ
とを特徴とするもので、従来の問題点も解決でき正現像
と同様に反転現像においてもカプリのないコントラスト
の安定した画像を得ることが出来だ。しかしながら、本
発明者らは更に研究を■ねたところ、前記トナーでは、
反転現像法により反転現像を得る場合所定の各印加電圧
において現像開始直後と多数枚コピーした後とでは濃度
の変化及びカプリの発生程度の変化が大きく、従って、
コピ一枚数による時間変化を含めた中で、濃度が充分満
足されかつカプリがない印加電位の範囲が狭くなるとい
う問題のあることが判った。ここで−成分磁性トナーを
用いて正現像(ポジ原稿からポジ画像を形成し、しかる
後これを他の記録媒体に転写する)方法において、コピ
一枚数の増加に従って画質が変化する(即ちコピ一枚数
が増えるに従って地が太る現象や濃度が大きくなる現象
が見られ更に文字の周りのチリ尾側現象が発生し易くな
る。)ことを防ぐために、従来のトナーの粒度分布より
も小径粒子(10μm以下の粒子)を増加させる事が特
開昭55−106466号公報によって知られている。
That is, in the electrophotographic developing method of the present invention, an electrophotographic photoreceptor that has been charged to a saturation potential and on which an electrostatic latent image has been formed by image exposure is applied with a potential of the same polarity as the charged potential of the photoreceptor by a bias potential applying means. In an electrophotographic development method in which reversal development is performed by a magnetic brush method using an applied one-component magnetic toner, the -component magnetic toner has an electrical resistance of 107Ω or more and in a range where charge exchange is performed, and 1
It is characterized by the use of a material with a coercive force of 50 millimeters or more, which solves the problems of conventional methods, and makes it possible to obtain images with stable contrast without capri during reverse development as well as normal development. . However, after further research, the present inventors found that the toner has the following properties:
When obtaining reversal development by the reversal development method, there are large changes in density and the degree of capri generation between immediately after the start of development and after copying a large number of sheets at each predetermined applied voltage.
It has been found that there is a problem in that the range of applied potentials in which the density is sufficiently satisfied and there is no capillarity becomes narrow, including the change over time due to the number of copies. Here, in a positive development method (forming a positive image from a positive original and then transferring it to another recording medium) using -component magnetic toner, the image quality changes as the number of copies increases (i.e., the number of copies increases). In order to prevent this phenomenon (as the number of sheets increases, the phenomenon that the background becomes thicker and the density increases, and the dust tail phenomenon around the letters becomes more likely to occur), the particle size distribution of the conventional toner is smaller than the particle size distribution (10 μm). It is known from Japanese Unexamined Patent Publication No. 106466/1983 that the following particles) can be increased.

この方法はトナーの流動性の改良という点から上記の構
成が採用されたものであるが、かかるトナーを反転現像
に用いたところネガ像の現像では、コピ一枚数の増加に
おいて濃度変化は多少小さくなることは確認されたが、
カプリの発止が非常に起こり易く、良好な画質を得るこ
とができなかった。そこで本発明者らは種々の検討を行
なった結果、磁場の存在下で攪拌したトナーを用いるこ
とにより前記の欠点がなく良好な結果がイnられること
を見出し本発明に到達した。即ち本発明の主目的は従来
の磁性トナーの欠点を排除して、反転現像における接写
枚数の増加による濃度変化もなくしかもカプリも生じな
い高濃度にして鮮明な画像が得られ、更に印加するバイ
アス電圧の範囲を非常に広く設定できる反転現仕方法を
提供することにある。
The above structure was adopted in this method from the point of view of improving the fluidity of the toner, but when such toner was used for reversal development, when developing a negative image, the density change was somewhat small as the number of copies increased. Although it was confirmed that
Capri was very likely to stop, making it impossible to obtain good image quality. As a result of various studies, the inventors of the present invention have discovered that by using a toner stirred in the presence of a magnetic field, the above-mentioned drawbacks can be avoided and good results can be obtained, and the present invention has been achieved. That is, the main purpose of the present invention is to eliminate the drawbacks of conventional magnetic toners, to obtain high-density and clear images that do not cause density changes due to an increase in the number of close-up images in reversal development, and that do not cause capri. The object of the present invention is to provide an inversion method that can set a very wide voltage range.

即ち本発明は、電子4負感光体を飽和電位に帯電し、画
像露光によって静電M像を形成した後、該trI\光体
の帯電電位と同極性のバイアス電圧を印加しつつ磁気ブ
ラシ現像方法によって該靜′Fkt潜像をトナー現像す
ることがら々る反転現像方法において、トナーとして少
なくも結着剤と磁性粉とからなシ磁場の存在下で撹拌処
理された一成分磁性トナーを用いることを特徴とする反
転現像方法である。
That is, in the present invention, after charging an electron 4 negative photoreceptor to a saturation potential and forming an electrostatic M image by image exposure, magnetic brush development is performed while applying a bias voltage of the same polarity as the charging potential of the trI\photoreceptor. In the reversal development method in which the silent Fkt latent image is often developed with toner, a one-component magnetic toner containing at least a binder and magnetic powder and stirred in the presence of a magnetic field is used as the toner. This is a reversal development method characterized by the following.

以下図面を参照して本発明を更に説明する。The present invention will be further explained below with reference to the drawings.

第2図は、本発明による一成分磁性トナーを用いて第1
図の如き磁気ブラシ現像装置による反転現像の様子を説
明する拡大断面図である。結着剤中に酸化亜鉛゛まだは
硫化カド9ミウム等の無機光尋電体を分散した光導電層
1が、導電性支持体2上に塗布されて感光体4を形成し
ている。との感光体4は例えばコロナ帯電装置等により
飽和帯電後、像露光され靜′[lf、?a像が形成され
る。光導電層1の電荷を有する部分は非露光部、電荷の
ない部分は画像露光された部分である。非磁性体スリー
ブ8に帯電と同極性のバイアス電圧を供給するため直流
電源9が(本図ではマイナス側に)接続されている。こ
の非磁性体スリーブ8け固ii>2され、内部に多極の
回転可能に配置された一7グイ・ットロ=う10を有し
、トナー粉7を非磁性体スリーブ8表面に搬送させ、感
光体4面と接触させ感光体面の露光部にトナーを付着さ
せ反転現像を行なう。このような装置で柚々の一成分磁
性トナーを用い反転現像を行なった実験結果を第1表に
示す。
FIG.
FIG. 3 is an enlarged cross-sectional view illustrating the state of reversal development using the magnetic brush developing device shown in the figure. A photoconductive layer 1 in which an inorganic photoconductor such as zinc oxide, cadmium sulfide or the like is dispersed in a binder is coated on a conductive support 2 to form a photoreceptor 4. After the photoreceptor 4 is charged to saturation using, for example, a corona charging device, it is imagewise exposed to a blank state. an image is formed. The charged portion of the photoconductive layer 1 is a non-exposed portion, and the uncharged portion is an imagewise exposed portion. A DC power supply 9 is connected (to the negative side in this figure) to supply a bias voltage of the same polarity as the charging to the non-magnetic sleeve 8. This non-magnetic sleeve 8 is hardened and has a multi-polar rotatably arranged 17 girder 10 inside, and the toner powder 7 is conveyed to the surface of the non-magnetic sleeve 8, It is brought into contact with the 4th surface of the photoreceptor, toner is attached to the exposed portion of the photoreceptor surface, and reversal development is performed. Table 1 shows the results of an experiment in which reversal development was carried out using a one-component magnetic toner of Yuzu in such an apparatus.

即ち第1表の実験結果は経時におけるバイアス電圧と画
像反射濃度およびカズリに関するものである。
That is, the experimental results shown in Table 1 relate to bias voltage, image reflection density, and fogging over time.

44 第1表で、トナーAは本発明に用いる一成分磁性トナー
である。即ち、ワックス40重量部とマグネタイト60
重景部の割合から成る磁性トナーを直流磁界のもとて攪
拌処理を施した抗磁力は270エルステッド、固有抵抗
は1.2X1012Ω・備を有するものである。トナー
Bは、トナーAと同一の出発原料の磁性トナーであり、
またトナーCは、トナーBを無磁界中で攪拌処理のみ行
なったものである。このようなトナーを用いて、8極の
非磁性導電スリーブ上に700ガウスの磁場を生じるマ
グネットローラを有する24,5φの現像器を用いて、
スリーブを固定して、マグネットローラを1000 r
pmで回転させた状態において、帯電後露光をした酸化
亜鉛感光体をスリーブにノよイアスミ圧を印加して反転
現像を行なった。この際酸化亜鉛感光体は75cIn/
secの移動速度で現像装置下を通過させた。その後、
マグネットローラをそのまま20分間空運転後、再び同
様の方法で画像を得た。第1表の結果よシ明らかな通り
、本発明による磁性トナーAは、経時による画像反射濃
度の変化も少なく、またカプリを生じないバイアス電圧
の領域中も変化しない安定した画像が得られた。トナー
Bはカプリを生じないバイアス電圧領域は広いが、初期
の画像反射a度が著しく低くなり、濃度及びカプリ発生
程度を共に満足するノζイアス電圧領域巾が非常に狭く
なっている。またトナーCにおいては、濃度変化は小さ
くなり好ましいが、カプリが発生し易く、バイアス電圧
の領域が広くなって実用に供し得なかった。このような
結果において本発明に用いるトナーが優れていることが
分ったが、この効果を生じる原因として、先にも述べた
様に攪拌によシトナー表簡の均一化が企られ、且つトナ
ーが弱く着磁されているので、その流動性も改良された
ことに起因するものと推定できた。本発明は磁場の存在
下でトナー粒子を所定時間、所定温度のもとて攪拌処理
したものを用いて磁気ブラシ現像法により反転現像を行
なうものであり、その結果、飽和帯電された感光体で連
続複写を行なっても正現像と同様に優れた画像が得られ
る。その具体的手段において、例えばトナー粒子の接触
する所で700ガウス以下の磁場のもと、所定時間5分
〜10時間、好ましくは5分〜2時間及び所定温度50
〜60C1好ましくFi20r〜4DCのもとてトナー
粒子を攪拌処理することにより達成される。磁性トナー
を磁化させる方法は、直流磁界、交番磁界減衰交流磁界
等を印加する方法もしくはこれらの磁場中を通過させる
方法等がある。
44 In Table 1, Toner A is a one-component magnetic toner used in the present invention. That is, 40 parts by weight of wax and 60 parts by weight of magnetite.
The magnetic toner consisting of the heavy image area is agitated under a direct current magnetic field and has a coercive force of 270 oersteds and a specific resistance of 1.2×10 12 Ω·. Toner B is a magnetic toner made of the same starting material as Toner A,
Toner C is obtained by subjecting toner B only to stirring treatment in the absence of a magnetic field. Using such toner, a 24.5φ developing device with a magnetic roller that generates a 700 Gauss magnetic field on an 8-pole non-magnetic conductive sleeve,
Fix the sleeve and rotate the magnetic roller to 1000 r.
While the photoreceptor was being rotated at pm, the charged and exposed zinc oxide photoreceptor was subjected to reversal development by applying an insulating pressure to the sleeve. At this time, the zinc oxide photoreceptor was 75cIn/
The film was passed under the developing device at a moving speed of sec. after that,
After the magnetic roller was operated for 20 minutes, an image was obtained again in the same manner. As is clear from the results in Table 1, magnetic toner A according to the present invention showed little change in image reflection density over time, and stable images were obtained that did not change even in the bias voltage range where capriion did not occur. Toner B has a wide bias voltage range in which no capillary occurs, but the initial image reflection degree is extremely low, and the width of the bias voltage range in which both the density and the degree of capillary occurrence are satisfied is extremely narrow. Further, in Toner C, the density change is small, which is preferable, but capri is likely to occur, and the bias voltage range becomes wide, so that it cannot be put to practical use. These results show that the toner used in the present invention is superior, but the reason for this effect is that, as mentioned earlier, the toner surface is made uniform by stirring, and the toner is Since it was weakly magnetized, it was assumed that this was due to its improved fluidity. The present invention performs reversal development using a magnetic brush development method using toner particles stirred at a predetermined temperature for a predetermined time in the presence of a magnetic field. Even if continuous copying is performed, excellent images can be obtained as in normal development. In the specific means, for example, under a magnetic field of 700 Gauss or less at a place where the toner particles come into contact, for a predetermined time of 5 minutes to 10 hours, preferably 5 minutes to 2 hours, and a predetermined temperature of 50
This is achieved by stirring toner particles of ~60C1, preferably Fi20r~4DC. The method of magnetizing the magnetic toner includes a method of applying a direct current magnetic field, a method of applying an attenuated alternating current magnetic field, a method of passing the magnetic toner through these magnetic fields, and the like.

次に本発明の好ましい1つの態様は、磁性トナーの粒度
分布において粒径15μm以下の粒子が約65重■%以
下で且つ粒径10μm以下の粒子が約6重月−%以下で
あるものを用いることで更に好ましい効果を得られる。
Next, in a preferred embodiment of the present invention, in the particle size distribution of the magnetic toner, particles with a particle size of 15 μm or less account for about 65% by weight or less, and particles with a particle size of 10 μm or less account for about 6% by weight or less. By using it, more favorable effects can be obtained.

本発明者らは、更に前述と同様の装置を用いて同様の方
法により異なる粒度分布を有するトナーを用いた実験を
行なったところ第2表の結果を得た。
The present inventors further conducted experiments using toners having different particle size distributions using the same apparatus and method as described above, and obtained the results shown in Table 2.

第2表の実験結果はトナーの粒度分布におけるバイアス
電圧と画故反射a度およびカプリに関するものである。
The experimental results in Table 2 relate to the bias voltage, image error reflection a degree, and capri in the particle size distribution of the toner.

第2表でトナーDは、゛その粒度分布の測定結果を第6
図に示す通り、粒径15μm以下の粒子が約35重ht
OI)以下で且つ粒径10μnL以下の粒子が約3重量
%以下存在し、磁場の存在下で攪拌処理しである。トナ
ーEは、トナーDと同一組成により同一の電気特性およ
び磁場の存在下で攪拌処理も施しであるが、粒度分布が
第4図に示す通り小径粒子(10pm以下)をより多く
含んでいるものである。なお、第6図および第4図で破
線はS+′、積粒度分布を表わす。第2表の結果より、
トナーDとトナーEを比較するとトナーDは一定のノミ
イアスミ圧において現像初期と経時後でも画像反射濃度
の差がトナーEに比べ少ない。特にカプリにおいてカプ
リを生じないバイアス電位の範囲が常にほぼ一定であり
、且つ一定濃度以上でカプリを発生しないバイアス電位
の範囲が広く設定できることが分る。このような比較的
大径の粒子を多く含む粒度分布を有することが本発明の
効果として何故生じるか、必ずしも明確ではないが、次
の様に推定される。即ち比較的小径のものを用いると、
トナーの重量当りのトナー表面積が大きくなるために現
像時のマグネットローラの磁気釣人吸引力に比べ、感光
層の帯電電位とトナー供給される電位間に作用する電気
的吸引力の方が支配的となり、その結果生じるカプリを
比較的大径の粒子を用いることによって磁気的吸引力を
大きくすることでカプリが除去されると考えられる。次
に本発明に用いる磁性トナーの具体的な製造方法の一例
を記述する。751定の粒度分布を崩する未着磁;・ナ
ーを第4図に示すような装置を用いて直流磁界中で攪拌
処理することにより得られる。即ち第4図に示す装置に
前記のようにして生成された磁化前のトナー8を絶縁性
容器9に入れ、コイル10により直流磁界1,000工
ルステツド以上の磁場の存在下で磁化させると共に、菟
温のもと攪拌機11により1時間攪拌して得る。丑だ、
他の製造例として磁化前のトナーを、第1図に示したよ
うなマグネットローラを用い、スリーブ表1用磁束密度
700ガウスのマグネットローラ上を一ングネット回転
数80 Or、pomで30分間回転させて得ることも
できる。このようにして得られる磁性トナーの好ましい
態様として、107Ω・い以上の固有抵抗を有し、且つ
150工ルステツド以上の高抗磁力を有すること、特に
反転現像では150工ルステツド以上の高抗磁力を有す
ることがかぶシを生じない画像を得るのに重要であるこ
とを特願昭56−196627号で提案した事を先に述
べた。
In Table 2, toner D is
As shown in the figure, particles with a particle size of 15 μm or less weigh approximately 35 ht.
About 3% by weight or less of particles having a particle size of 10 μnL or less and having a particle diameter of 10 μnL or less are present, and the agitation treatment is performed in the presence of a magnetic field. Toner E has the same composition as Toner D, has the same electrical properties, and has been subjected to stirring treatment in the presence of a magnetic field, but has a particle size distribution that contains more small-diameter particles (10 pm or less) as shown in Figure 4. It is. In addition, the broken line in FIGS. 6 and 4 represents S+', the grain size distribution. From the results in Table 2,
Comparing Toner D and Toner E, Toner D has a smaller difference in image reflection density than Toner E even at the initial stage of development and after development at a constant ink pressure. In particular, it can be seen that the range of bias potentials in which capri does not occur is always approximately constant, and that the range of bias potentials in which capri does not occur above a certain concentration can be set wide. Although it is not necessarily clear why such a particle size distribution containing many relatively large particles occurs as an effect of the present invention, it is presumed as follows. In other words, if a relatively small diameter one is used,
As the toner surface area per toner weight becomes larger, the electric attraction force acting between the charged potential of the photosensitive layer and the potential supplied to the toner becomes more dominant than the magnetic attraction force of the magnetic roller during development. It is thought that the resulting capri is removed by increasing the magnetic attraction force by using particles with a relatively large diameter. Next, a specific example of a method for manufacturing the magnetic toner used in the present invention will be described. 751 is obtained by stirring an unmagnetized toner that disrupts the constant particle size distribution in a direct current magnetic field using an apparatus as shown in FIG. That is, the unmagnetized toner 8 produced as described above is placed in an insulating container 9 in the apparatus shown in FIG. The mixture is stirred for 1 hour using a stirrer 11 at room temperature. It's ox.
As another manufacturing example, unmagnetized toner is rotated for 30 minutes on a magnetic roller with a magnetic flux density of 700 Gauss for sleeve table 1 at a net rotation speed of 80 Or, using a magnetic roller as shown in Fig. 1. You can also get it. A preferred embodiment of the magnetic toner obtained in this way is that it has a specific resistance of 107 ohms or more and a high coercive force of 150 or more, particularly in reversal development, a high coercive force of 150 or more. It was mentioned earlier that it was proposed in Japanese Patent Application No. 196627-1983 that it is important to have images without fogging.

本発明の磁性トナーに使用されるバインダは合成樹脂或
いは天然樹脂の倒れでもよい。このうち合成樹脂として
、例えばポリスチレン樹脂、ポリエチレン樹脂、ポリエ
ステル樹脂、エポキシ樹脂、アクリル樹脂またはそれら
の共重合体、クマロン“樹脂、インデン樹脂、フタル酢
樹脂、およびワックス類等を単独あるいは複合で用いる
ことができる。
The binder used in the magnetic toner of the present invention may be a synthetic resin or a natural resin. Among these, as synthetic resins, for example, polystyrene resin, polyethylene resin, polyester resin, epoxy resin, acrylic resin or copolymers thereof, coumaron resin, indene resin, phthalate resin, waxes, etc. may be used alone or in combination. I can do it.

また磁性粉としては、フェライト、マグネタイト、欽、
コバルト、ニッケルなどの強磁性を示す元素を含む合金
あるいは化合物、すの他aX理号何らかの処理を施すこ
とによって強磁性を示す様な棟々の合金等を用いればよ
い。具体例としては、マグネタイト(Faao4)  
Co 添加マネタイト スピネル屋フェライト マグネ
ットプランノ2イト型フェライトなどがあげられる。
In addition, magnetic powders include ferrite, magnetite,
An alloy or compound containing an element exhibiting ferromagnetism such as cobalt or nickel, or an alloy that exhibits ferromagnetism by undergoing some kind of aX-physical treatment may be used. A specific example is magnetite (Faao4)
Examples include Co-added manetite, spinel ferrite, and magnetoplano 2ite type ferrite.

なお本発明の如くトナーの電気抵抗を任意の値に設定す
る手段として、トナーに添加するカーボンブラック、錫
、ニッケル、アルミニウム等の導電化剤の世を加減する
ことによシ達成できる。
As a means of setting the electrical resistance of the toner to an arbitrary value as in the present invention, this can be achieved by adjusting the amount of conductive agent added to the toner, such as carbon black, tin, nickel, aluminum, or the like.

また本発明の他の態様として、結合剤中に酸化亜鉛を分
散させてなる感光層を有する電子写真感光体を用いた反
転現像方法である。i像濃度においてコントラストがあ
る画像を得ることができるトナー抵抗は、107Ω・α
以上必要であり、特に反転現像であることを先の特願昭
56−196627号でも述べだが、一方、画像濃度は
感光体とトナーとの電荷交換の容易性、即ちトナーから
感光体表面への電荷注入の容易性に相関があると思われ
る。感光体が酸化亜鉛感光体の場合、酸化亜鉛の電子伝
導体のエネルギーレベルが比較的低いため(Photo
chem、Photobiol−16219〜241(
1972)参照)トナーからマイナス電荷が注入し易い
が、比較的高抵抗トナーを用いるためコントラストのあ
る画像が得られるのである。
Another embodiment of the present invention is a reversal development method using an electrophotographic photoreceptor having a photosensitive layer formed by dispersing zinc oxide in a binder. The toner resistance that can obtain an image with contrast at i image density is 107Ω・α
As stated in the previous Japanese Patent Application No. 196627/1986, the above is necessary, especially reversal development. On the other hand, image density is determined by the ease of charge exchange between the photoreceptor and toner, that is, the ease of charge exchange from the toner to the photoreceptor surface. This seems to be related to the ease of charge injection. When the photoreceptor is a zinc oxide photoreceptor, the energy level of the zinc oxide electron conductor is relatively low (Photo
chem, Photobiol-16219-241 (
(1972))) Although negative charges are easily injected from the toner, images with contrast can be obtained because a relatively high resistance toner is used.

以上詳細に説明した通シ、本発明による磁性トナーを用
いることによシ飽和帯電されて像形成された記録媒体で
しかも連続複写に適用しても、濃度差の少ない且つカプ
リを生じない画像の得られる反転現像法である。
As described in detail above, by using the magnetic toner according to the present invention, images with small density differences and no capillary formation can be produced even when applied to continuous copying on a recording medium that is saturated and has an image formed thereon. This is a reversal development method.

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

M1図は、本発明に用いられ磁気ブラシ現像装置の1例
を示す斜視図、第2図はその反転現像の様子を説明する
拡大断面図、第6図は本発明に用いる磁性トナーの粒度
分布を示す図、第4図は比較トナーの粒度分布を示す図
、第5図は本発明に用いる磁性トナーの製造例を示す図
である。 1・・・光導電層 2・・・導電性支持体 3・・・未着磁トナー 4・・・電子写真感光体 5・・・絶縁性容器 6・・・攪拌機 7・・・磁性トナー 8・・・非磁性体スリーブ 9・・・直流電源 10・・・マノネットローシ 11・・・コイル (はか6名) 手続補正書 昭和57年 9月、2Z日 昭和57年特許願第 91606  月2、発明の名称 反転現像方法 3、補正をする者 事件との関係:特許出願人 名称 (520)  富士写真フィルム株式会社霞が関
ビル内郵便局 私書箱第49月 7、補正の対象 r(Fe=o、 )7 、CoJと補正する。 453−
Figure M1 is a perspective view showing an example of a magnetic brush developing device used in the present invention, Figure 2 is an enlarged sectional view illustrating the state of reversal development, and Figure 6 is a particle size distribution of the magnetic toner used in the present invention. FIG. 4 is a diagram showing the particle size distribution of a comparative toner, and FIG. 5 is a diagram showing an example of manufacturing a magnetic toner used in the present invention. 1... Photoconductive layer 2... Conductive support 3... Unmagnetized toner 4... Electrophotographic photoreceptor 5... Insulating container 6... Stirrer 7... Magnetic toner 8 ...Non-magnetic sleeve 9...DC power supply 10...Manonet Roshe 11...Coil (6 people) Procedural amendment September 1982, 2Z-1982 Patent Application No. 91606 2. Name of the invention Reversal development method 3. Person making the amendment Relationship with the case: Name of the patent applicant (520) Fuji Photo Film Co., Ltd. Kasumigaseki Building Post Office P.O. Box 49/7 Subject of amendment r (Fe=o , )7, corrected as CoJ. 453-

Claims (4)

【特許請求の範囲】[Claims] (1)  電子写真感光体を飽和電位に帯電し、画像露
光によって静電潜像を形成した後、該感光体の帯電電位
と同極性のバイアス電圧を印加しつつ磁気ブラシ現像方
法によって該静電潜像をトナー現像することからなる反
転現像方法において、トナーとして少なくも結着剤と磁
性粉とからなシ磁場の存在下で攪拌処理された一成分磁
性トナーを用いることを特徴とする反転現像方法。
(1) After charging an electrophotographic photoreceptor to a saturation potential and forming an electrostatic latent image by image exposure, the electrostatic latent image is removed by a magnetic brush development method while applying a bias voltage of the same polarity as the charged potential of the photoreceptor. A reversal development method comprising toner development of a latent image, characterized in that a one-component magnetic toner comprising at least a binder and magnetic powder and stirred in the presence of a magnetic field is used as the toner. Method.
(2)前記トナーが粒径15μm以下の粒子が約35重
量係以下で且つ粒径10μm以下の粒−7!塑約6重甘
係以下であることを特徴とする特許請求の範囲第1項記
載の反転現像方法。
(2) The toner has particles with a particle size of 15 μm or less in a weight ratio of about 35 μm or less, and particles with a particle size of 10 μm or less - 7! 2. The reversal developing method according to claim 1, wherein the reversal development method has a plasticity of less than about 6 times.
(3)前記トナーが10Ω・儒以上の体積固有抵抗値を
有し、且つ150工ルステツド以上の抗磁力を有するこ
とを特徴とする特許請求の範囲第1項記載の反転現像方
法。
(3) The reversal developing method according to claim 1, wherein the toner has a volume resistivity of 10 Ω·F or more and a coercive force of 150 or more.
(4)前記電子写真感光体が結合剤中に酸化亜鉛を分散
させてなる感光層を有することを特徴とする特許請求の
範囲M1項記載の反転現像方法。
(4) The reversal developing method according to claim M1, wherein the electrophotographic photoreceptor has a photosensitive layer formed by dispersing zinc oxide in a binder.
JP9130682A 1982-05-31 1982-05-31 Method for inverse development Pending JPS58208772A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9130682A JPS58208772A (en) 1982-05-31 1982-05-31 Method for inverse development

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9130682A JPS58208772A (en) 1982-05-31 1982-05-31 Method for inverse development

Publications (1)

Publication Number Publication Date
JPS58208772A true JPS58208772A (en) 1983-12-05

Family

ID=14022775

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9130682A Pending JPS58208772A (en) 1982-05-31 1982-05-31 Method for inverse development

Country Status (1)

Country Link
JP (1) JPS58208772A (en)

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