JPH0762779B2 - Development method - Google Patents
Development methodInfo
- Publication number
- JPH0762779B2 JPH0762779B2 JP62060454A JP6045487A JPH0762779B2 JP H0762779 B2 JPH0762779 B2 JP H0762779B2 JP 62060454 A JP62060454 A JP 62060454A JP 6045487 A JP6045487 A JP 6045487A JP H0762779 B2 JPH0762779 B2 JP H0762779B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- toner
- developing
- particles
- sleeve
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 238000000034 method Methods 0.000 title claims description 26
- 238000011161 development Methods 0.000 title description 23
- 239000006249 magnetic particle Substances 0.000 claims description 133
- 239000002245 particle Substances 0.000 claims description 50
- 230000005684 electric field Effects 0.000 claims description 35
- 108091008695 photoreceptors Proteins 0.000 claims description 3
- 230000000694 effects Effects 0.000 description 27
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- 239000011248 coating agent Substances 0.000 description 11
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- 210000005069 ears Anatomy 0.000 description 7
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- 229910000859 α-Fe Inorganic materials 0.000 description 6
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- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 4
- 239000000696 magnetic material Substances 0.000 description 4
- 239000000463 material Substances 0.000 description 4
- 230000002093 peripheral effect Effects 0.000 description 4
- 241000519995 Stachys sylvatica Species 0.000 description 3
- 230000009471 action Effects 0.000 description 3
- 229910052782 aluminium Inorganic materials 0.000 description 3
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 3
- 238000002474 experimental method Methods 0.000 description 3
- 230000006872 improvement Effects 0.000 description 3
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- 238000011084 recovery Methods 0.000 description 3
- 238000007789 sealing Methods 0.000 description 3
- 238000005245 sintering Methods 0.000 description 3
- 238000012546 transfer Methods 0.000 description 3
- QPLDLSVMHZLSFG-UHFFFAOYSA-N Copper oxide Chemical compound [Cu]=O QPLDLSVMHZLSFG-UHFFFAOYSA-N 0.000 description 2
- YCKRFDGAMUMZLT-UHFFFAOYSA-N Fluorine atom Chemical compound [F] YCKRFDGAMUMZLT-UHFFFAOYSA-N 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- NIXOWILDQLNWCW-UHFFFAOYSA-N acrylic acid group Chemical group C(C=C)(=O)O NIXOWILDQLNWCW-UHFFFAOYSA-N 0.000 description 2
- 239000000969 carrier Substances 0.000 description 2
- 239000004020 conductor Substances 0.000 description 2
- 230000001419 dependent effect Effects 0.000 description 2
- 230000006866 deterioration Effects 0.000 description 2
- 230000001747 exhibiting effect Effects 0.000 description 2
- 239000010419 fine particle Substances 0.000 description 2
- 239000011737 fluorine Substances 0.000 description 2
- 229910052731 fluorine Inorganic materials 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 229920002050 silicone resin Polymers 0.000 description 2
- 230000006641 stabilisation Effects 0.000 description 2
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- 229910052725 zinc Inorganic materials 0.000 description 2
- 239000011701 zinc Substances 0.000 description 2
- PCTMTFRHKVHKIS-BMFZQQSSSA-N (1s,3r,4e,6e,8e,10e,12e,14e,16e,18s,19r,20r,21s,25r,27r,30r,31r,33s,35r,37s,38r)-3-[(2r,3s,4s,5s,6r)-4-amino-3,5-dihydroxy-6-methyloxan-2-yl]oxy-19,25,27,30,31,33,35,37-octahydroxy-18,20,21-trimethyl-23-oxo-22,39-dioxabicyclo[33.3.1]nonatriaconta-4,6,8,10 Chemical compound C1C=C2C[C@@H](OS(O)(=O)=O)CC[C@]2(C)[C@@H]2[C@@H]1[C@@H]1CC[C@H]([C@H](C)CCCC(C)C)[C@@]1(C)CC2.O[C@H]1[C@@H](N)[C@H](O)[C@@H](C)O[C@H]1O[C@H]1/C=C/C=C/C=C/C=C/C=C/C=C/C=C/[C@H](C)[C@@H](O)[C@@H](C)[C@H](C)OC(=O)C[C@H](O)C[C@H](O)CC[C@@H](O)[C@H](O)C[C@H](O)C[C@](O)(C[C@H](O)[C@H]2C(O)=O)O[C@H]2C1 PCTMTFRHKVHKIS-BMFZQQSSSA-N 0.000 description 1
- 241000490494 Arabis Species 0.000 description 1
- 229910001369 Brass Inorganic materials 0.000 description 1
- 239000005751 Copper oxide Substances 0.000 description 1
- HCHKCACWOHOZIP-UHFFFAOYSA-N Zinc Chemical compound [Zn] HCHKCACWOHOZIP-UHFFFAOYSA-N 0.000 description 1
- 239000006061 abrasive grain Substances 0.000 description 1
- 238000013019 agitation Methods 0.000 description 1
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 229910021417 amorphous silicon Inorganic materials 0.000 description 1
- 238000005452 bending Methods 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000010951 brass Substances 0.000 description 1
- 229910052793 cadmium Inorganic materials 0.000 description 1
- 239000011247 coating layer Substances 0.000 description 1
- 239000008119 colloidal silica Substances 0.000 description 1
- 230000001276 controlling effect Effects 0.000 description 1
- 239000012050 conventional carrier Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
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- 230000007547 defect Effects 0.000 description 1
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- 238000005516 engineering process Methods 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 238000007667 floating Methods 0.000 description 1
- RBTKNAXYKSUFRK-UHFFFAOYSA-N heliogen blue Chemical compound [Cu].[N-]1C2=C(C=CC=C3)C3=C1N=C([N-]1)C3=CC=CC=C3C1=NC([N-]1)=C(C=CC=C3)C3=C1N=C([N-]1)C3=CC=CC=C3C1=N2 RBTKNAXYKSUFRK-UHFFFAOYSA-N 0.000 description 1
- 230000001771 impaired effect Effects 0.000 description 1
- 238000010348 incorporation Methods 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 230000009545 invasion Effects 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 229910052745 lead Inorganic materials 0.000 description 1
- 229910052749 magnesium Inorganic materials 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 229910052748 manganese Inorganic materials 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 229910044991 metal oxide Inorganic materials 0.000 description 1
- 150000004706 metal oxides Chemical class 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- 239000000049 pigment Substances 0.000 description 1
- 238000007747 plating Methods 0.000 description 1
- 238000005498 polishing Methods 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
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- 238000005488 sandblasting Methods 0.000 description 1
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- 229920003048 styrene butadiene rubber Polymers 0.000 description 1
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Landscapes
- Magnetic Brush Developing In Electrophotography (AREA)
- Dry Development In Electrophotography (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、交番電界中において磁性キヤリア粒子とトナ
ー粒子とを用いて現像を行う2成分現像方式の現像方法
及び装置に関する。Description: TECHNICAL FIELD The present invention relates to a two-component development type developing method and apparatus for performing development using magnetic carrier particles and toner particles in an alternating electric field.
本発明は画像記録形成用の表示装置、プリンター、フア
クシミリ電子写真装置の種々に適用可能な現像方法及び
装置である。The present invention is a developing method and apparatus applicable to various kinds of display devices for image recording formation, printers, and facsimile electrophotographic devices.
本願出願人は、先に、従来2成分現像方式とは異なり、
現像容器内は2成分で、現像部へは1成分トナーのみを
供給して交番電界中で現像を行う方法及び装置を提供し
た(特開昭58-143360,同59-101680各公報)。The applicant of the present application, unlike the conventional two-component developing method,
There is provided a method and apparatus for developing in an alternating electric field by supplying only one-component toner to a developing section with two-component toner in the developing container (JP-A-58-143360 and 59-101680).
このように現像容器内にのみ磁性粒子とトナー粒子を混
在させている現像方法では、トナーが磁性材料を含有す
ることによる欠点を解消したので有用であった。しか
し、画像のエツジ効果が強く、ベタ部の濃度が低く、負
性特性(画像濃度が潜像電位の上昇とともに低下するこ
と)を示す場合があり現像特性の欠点を有していた。As described above, the developing method in which the magnetic particles and the toner particles are mixed only in the developing container is useful because the drawbacks due to the toner containing the magnetic material are eliminated. However, the edge effect of the image is strong, the density of the solid portion is low, and the negative property (the image density decreases with the increase of the latent image potential) may be exhibited, which has a drawback of the developing property.
そこで出願人は多くの実験によって、これらの不都合を
も解決でき、積極的に現像部に磁性キヤリア粒子を供給
する2成分現像装置において多大なる効果を生む現像装
置を特願昭60-204605号(昭和60年9月17日出願)等に
提案している。又、近年各方面で2成分現像剤を用いて
交番電界中で現像する方法も各種提案されている。Therefore, the applicant has been able to solve these inconveniences through many experiments, and has developed a developing device which produces a great effect in a two-component developing device which positively supplies the magnetic carrier particles to the developing portion, in Japanese Patent Application No. 60-204605 ( (September 17, 1985 application) etc. Further, in recent years, various methods of developing in various fields using a two-component developer in an alternating electric field have been proposed.
一方、2成分現像装置に対して、交番電界を印加する技
術は、基本的に特開昭55-32060号公報に記載されてい
る。これはキヤリア粒子を現像電極として用い、カブリ
防止効果を得ることを開示した優れた発明である。On the other hand, the technique of applying an alternating electric field to a two-component developing device is basically described in JP-A-55-32060. This is an excellent invention which discloses that carrier particles are used as a developing electrode to obtain an antifoggant effect.
又、一般の2成分現像装置に用いられるキヤリア粒子
は、導電キヤリアやフエライト単体の中抵抗キヤリアで
あり、トナー粒子付着による劣化を生じ易く耐久性,ト
ナーへの帯電付与能力の低下といった問題がある。Further, the carrier particles used in a general two-component developing device are conductive carriers or medium resistance carriers of ferrite alone, and are liable to be deteriorated due to adhesion of toner particles, resulting in problems such as deterioration of durability and ability to impart charge to toner. .
この耐久性や帯電付与能力向上のために、樹脂被覆キヤ
リア粒子を用いることもかなり以前から知られたことで
ある。従来の樹脂被覆キヤリア粒子は、かなりの絶縁性
を示すもので帯電付与能力は増し、表面性も良好である
ので耐久性の意味では実用上好ましい。It has been known for a long time that resin-coated carrier particles are used to improve the durability and the charge imparting ability. Conventional resin-coated carrier particles exhibit a considerable insulating property, have an increased charge imparting ability, and have a good surface property, and are therefore practically preferable in terms of durability.
交番電界を印加した2成分現像方式も当然耐久性を必要
とするため従来の高抵抗樹脂被覆キヤリア粒子を用いる
ことは当然の設計事項であるが、新たな問題をもたら
す。この高抵抗キヤリア粒子には、樹脂被覆以外に磁性
微粒子樹脂結着型キヤリア粒子もあるが、極めて高い電
気抵抗を示すものである。キヤリア粒子の電気抵抗が高
く絶縁性に近いもの程、現像部での電気的リーク防止に
なり、高い潜像電位及び交番電界を設定することがで
き、交番電界による現像特性を期待できるためである。
しかし、例えば1014Ωcm以上の絶縁抵抗のキヤリアで
は、トナーと逆極性に帯電し、非画線ベタ白部にキヤリ
ア引きが生じやすく、又キヤリアを用いているにもかか
わらずエツジ効果が強くでてしまう欠点がある。Since the two-component developing method in which an alternating electric field is applied naturally needs durability, it is a matter of course to use the conventional high-resistivity resin-coated carrier particles, but it causes a new problem. In addition to resin coating, there are magnetic fine particle resin-bonded type carrier particles as the high resistance carrier particles, but they exhibit extremely high electric resistance. This is because the higher the electrical resistance of the carrier particles and the closer they are to the insulating property, the more the electrical leakage is prevented in the developing section, the higher the latent image potential and the alternating electric field can be set, and the developing characteristics due to the alternating electric field can be expected. .
However, for example, a carrier with an insulation resistance of 10 14 Ωcm or more is charged in the opposite polarity to the toner, and it is easy for the carrier to be drawn in the non-printed solid white area, and even though the carrier is used, the edge effect is strong. There is a drawback that
従って、2成分現像方式では、耐久性のあるキヤリア粒
子を用いた場合の画像再現性の改善がさらに要求されて
いる。Therefore, in the two-component developing method, there is a further demand for improvement in image reproducibility when using durable carrier particles.
本発明は、交番電界を印加した際の樹脂被覆キヤリア粒
子がもたらす新たな問題を解決することを目的とする。It is an object of the present invention to solve a new problem caused by resin-coated carrier particles when an alternating electric field is applied.
本発明は、樹脂被覆キヤリア粒子の条件を交番電界印加
現像における現像効果を一層高め、良質の画像を形成で
きる現像方法の提供を目的とする。It is an object of the present invention to provide a developing method capable of forming a high-quality image by further improving the developing effect in the alternating electric field application development under the conditions of resin-coated carrier particles.
本発明は、樹脂被覆キヤリア粒子の絶縁性に着目し、従
来のキヤリア粒子とは異なる特性を求めた結果なされた
もので、耐久性はむろんのこと、トナー粒子に与える帯
電特性や電極効果を維持して良質の画像を得るものであ
る。The present invention has been made as a result of focusing on the insulating property of resin-coated carrier particles and seeking properties different from those of conventional carrier particles. The durability is of course, and the charging property and electrode effect given to toner particles are maintained. To obtain good quality images.
即ち、本発明は、樹脂被覆キヤリア粒子の電気抵抗に着
目したもので、従来では認識されていなかった電界依存
性のキヤリア粒子の抵抗値変化状態が再現画像性に大き
く影響するという事実に基いたものである。That is, the present invention focuses on the electric resistance of the resin-coated carrier particles, and is based on the fact that the electric field-dependent change in the resistance value of the carrier particles, which has hitherto been unrecognized, greatly affects the reproducibility. It is a thing.
この本発明は、磁性粒子とトナー粒子を有する現像剤を
用いて、感光体と現像剤担持体との間に交番電界が印加
されている状態で磁性粒子の穂を感光体に接触させてト
ナー像を形成する現像方法において、上記感光体はOPC
であり、上記磁性粒子は0.2×103V/cmの電界における抵
抗値が108以上1011Ωcm以下、または2×103V/cmの電界
における抵抗値が2×107以上3×109Ωcm以下であるこ
とを特徴とするものである。According to the present invention, a developer having magnetic particles and toner particles is used, and the magnetic particles are brought into contact with the photoconductor in the state where an alternating electric field is applied between the photoconductor and the developer carrying member, thereby toner In the developing method for forming an image, the photoreceptor is an OPC.
The magnetic particles have a resistance value of 10 8 or more and 10 11 Ωcm or less in an electric field of 0.2 × 10 3 V / cm, or a resistance value of 2 × 10 7 or more and 3 × 10 7 in an electric field of 2 × 10 3 V / cm. It is characterized by being 9 Ωcm or less.
本発明によれば磁性粒子を絶縁性とはせず、ある程度電
流が流れる抵抗値とすることで、磁性粒子の穂が現像電
極の役割を果し、現像部で非常に高いトナーの振動効果
が得られるため現像特性は非常に優れたものとなる。According to the present invention, the magnetic particles are not made to be insulative, but have a resistance value through which an electric current flows to some extent, so that the ears of the magnetic particles serve as a developing electrode, and a very high toner vibration effect is obtained in the developing section. Since it is obtained, the developing property becomes very excellent.
しかし、このように磁性粒子の抵抗を107〜1011Ωcmと
した場合、表面性に優れた感光体は問題はないがピンホ
ールが多いa-Siや傷が発生し易いSe等ではピンホールや
傷に現像バイアスがリークする。However, when the resistance of the magnetic particles is set to 10 7 to 10 11 Ωcm in this way, there is no problem with a photoreceptor having excellent surface properties, but there are many pinholes such as a-Si and Se which easily scratches. The development bias leaks to scratches and scratches.
この現像を防止するため磁性粒子の抵抗値を高くする
と、前述した磁性粒子の現像電極効果が損なわれる。If the resistance value of the magnetic particles is increased in order to prevent the development, the developing electrode effect of the magnetic particles described above is impaired.
そこで本願発明は感光体としてOPCを用いている。OPCは
非常にピンホール、傷が発生しにくく、このため、磁性
粒子の穂の現像電極効果を得つつ、現像バイアスのリー
クを防止できる。Therefore, the present invention uses OPC as the photoconductor. OPC is extremely unlikely to cause pinholes and scratches. Therefore, leakage of the developing bias can be prevented while obtaining the developing electrode effect of the spikes of magnetic particles.
第2図は本発明が適用できる現像装置の断面図である。
潜像担持体1はOPC(Organic Photoconductor)からな
る光導電絶縁物質層を持つ感光ドラムもしくは感光ベル
トである。潜像担持体1は図示しない駆動装置によって
矢印a方向に回転される。22は潜像担持体1に近接もし
くは接触されている現像スリーブであり、例えばアルミ
ニウム、SUS316等の非磁性材料で構成されている。現像
スリーブ22は現像容器36の左下方壁に容器長手方向に形
成した横長開口に右略半周面を容器36内へ突入させ、左
略半周面を容器外へ露出させて回転自在に軸受けさせて
横設してあり、矢印b方向に回転駆動される。FIG. 2 is a sectional view of a developing device to which the present invention can be applied.
The latent image carrier 1 is a photosensitive drum or photosensitive belt having a photoconductive insulating material layer made of OPC (Organic Photoconductor). The latent image carrier 1 is rotated in the direction of arrow a by a driving device (not shown). Reference numeral 22 denotes a developing sleeve which is in proximity to or in contact with the latent image carrier 1, and is made of a non-magnetic material such as aluminum or SUS316. The developing sleeve 22 has a laterally long opening formed in the lower left wall of the developing container 36 in a longitudinal direction of the container so that a substantially right half peripheral surface projects into the container 36, and a substantially left half peripheral surface is exposed outside the container and rotatably supported. It is installed horizontally and is driven to rotate in the direction of arrow b.
23は現像スリーブ22内に挿入し図示の位置姿勢に位置決
め保持した固定磁界発生手段としての固定の永久磁石
(マグネット)であり、現像スリーブ22が回転駆動され
てもこの磁石23は図示の位置・姿勢にそのまま固定保持
される。この磁石23はN極の磁極23a,S極の磁極23b,N極
の磁極23c,S極の磁極23dの4磁極を有する。磁石23は永
久磁石に代えて電磁石を配設してもよい。Reference numeral 23 is a fixed permanent magnet (magnet) as fixed magnetic field generating means which is inserted into the developing sleeve 22 and positioned and held in the position and orientation shown in the drawing. Even if the developing sleeve 22 is driven to rotate, the magnet 23 is at the position shown in the drawing. It is fixedly held as it is. The magnet 23 has four magnetic poles, an N-pole magnetic pole 23a, an S-pole magnetic pole 23b, an N-pole magnetic pole 23c, and an S-pole magnetic pole 23d. The magnet 23 may be an electromagnet instead of the permanent magnet.
24は現像スリーブ2を配設した現像剤供給器開口の上縁
側に、基部を容器側壁に固定し、先端側は開口上縁位置
よりも容器36の外側へ突出させて開口上縁長手に沿って
配設した現像剤規制部材としての非磁性ブレードで、例
えばSuS316を横断面路への字形に曲げ加工したものであ
る。The reference numeral 24 is fixed to the side wall of the container on the upper edge side of the developer supply device in which the developing sleeve 2 is arranged, and the tip side is projected to the outside of the container 36 from the position of the upper edge of the opening to extend along the length of the upper edge of the opening. A non-magnetic blade serving as a developer regulating member that is arranged as described above, for example, is obtained by bending SuS316 into a letter shape in a cross-section path.
26は非磁性ブレード24の下面側に上面を接触させ前端面
を現像剤案内面261とした磁性粒子限定部材である。Reference numeral 26 is a magnetic particle limiting member whose upper surface is in contact with the lower surface side of the non-magnetic blade 24 and whose front end surface is the developer guide surface 261.
27は磁性粒子であり粒径が20〜100μm、好ましくは30
〜80μmの見掛密度約2.4〜2.8g/ccフエライト粒子(最
大直60〜70emu/g)へ樹脂コーテイングしたものが用い
られ得る。27 is a magnetic particle having a particle size of 20 to 100 μm, preferably 30
Resin coated to an apparent density of about 2.4 to 2.8 g / cc ferrite particles (up to 60 to 70 emu / g maximum) of -80 μm can be used.
20μよりも小さいと、現像スリーブ上の穂立ちが悪く、
ムラの発生した画像となる傾向がある。又100μよりも
大きいと、トナーへのトリボ賦与能力が低下し感光板へ
の傷も生じやすい。If it is less than 20μ, the spikes on the developing sleeve will be poor,
The image tends to be uneven. On the other hand, if it is larger than 100 μm, the ability to impart tribo to the toner is lowered and the photosensitive plate is apt to be damaged.
37は非磁性現像剤トナーである。37 is a non-magnetic developer toner.
31は現像スリーブ22を配設した現像容器36下部からの磁
性粒子27ないしは非磁性トナー粒子37の漏出を防止する
ために現像容器下部内面に現像スリーブ22に対向して配
設された磁性体であり、例えば鉄板にメツキを施したも
のである。磁性体31とS極性の磁極23dとの間の磁界で
は磁性粒子27の回収と漏れ防止を達成するシール効果が
得られる。Reference numeral 31 is a magnetic material disposed on the inner surface of the lower portion of the developing container so as to face the developing sleeve 22 in order to prevent leakage of the magnetic particles 27 or the non-magnetic toner particles 37 from the lower portion of the developing container 36 in which the developing sleeve 22 is disposed. There is, for example, an iron plate to which plating is applied. In the magnetic field between the magnetic body 31 and the S-polarized magnetic pole 23d, a sealing effect for achieving recovery of the magnetic particles 27 and leakage prevention can be obtained.
39は現像スリーブ22内の固定磁極23により形成された磁
性粒子のブラシ部分へトナーを供給するトナー供給部材
であり回転自在に軸受した板金にゴムシートを貼り付け
現像容器下面を掃くが如くトナーを搬送する。トナー供
給部材39には、不図示のトナー貯蔵容器38中のトナー搬
送部材によってトナー供給される。Reference numeral 39 denotes a toner supply member for supplying toner to the brush portion of magnetic particles formed by the fixed magnetic pole 23 in the developing sleeve 22, and a rubber sheet is attached to a sheet metal rotatably bearing to sweep the toner as if sweeping the lower surface of the developing container. Transport. Toner is supplied to the toner supply member 39 by a toner conveying member in a toner storage container 38 (not shown).
38,35はそれぞれトナー貯蔵容器、磁性粒子貯蔵容器で
ある。38 and 35 are a toner storage container and a magnetic particle storage container, respectively.
40は現像容器36下部部分に溜るトナーを封止するシール
部材で弾性を有しスリーブ22の回転方向に向って曲がっ
ており、スリーブ22表面側を弾性的に押圧している。こ
のシール部材40は、現像剤の容器内部側への進入を許可
するように、スリーブとの接触域でスリーブ回転方向下
流側に端部を有している。Reference numeral 40 denotes a seal member for sealing the toner accumulated in the lower portion of the developing container 36, which has elasticity and is bent in the rotation direction of the sleeve 22, and elastically presses the surface side of the sleeve 22. The seal member 40 has an end portion on the downstream side in the sleeve rotation direction in the contact area with the sleeve so as to allow the developer to enter the inside of the container.
30は現像工程で発生した浮遊現像剤を現像剤と同極性の
電圧を印加して感光体側に付着させ飛散を防止する飛散
防止電極板である。Reference numeral 30 denotes a scattering prevention electrode plate for preventing the scattering by floating voltage generated in the developing process by applying a voltage having the same polarity as that of the developer to adhere to the photosensitive member side.
又、S磁極23dは、磁性部材31との間に一方から他方に
磁界を形成するための磁性シール用磁界発生手段であ
り、磁性部材31に対して1部が対向する。Further, the S magnetic pole 23d is a magnetic field for magnetic sealing for forming a magnetic field from one side to the other with the magnetic member 31, and one part faces the magnetic member 31.
磁性部材31は、現像剤容器の現像剤収納部の実質的な端
部で現像装置の下方に位置し、この容器内周辺では回収
された磁性キヤリア粒子の移動によって、スリーブ表面
の現像剤中に容器内下方に位置するトナー粒子を取り込
む。従って、磁性粒子の安定した回収は、現像能力を安
定化する効果がある。The magnetic member 31 is located below the developing device at a substantial end of the developer storage portion of the developer container, and the magnetic carrier particles collected around the inside of the container cause the magnetic member 31 to move into the developer on the sleeve surface. Intake toner particles located in the lower part of the container. Therefore, the stable recovery of magnetic particles has the effect of stabilizing the developing ability.
磁極23dを前記のごとく配置することによって、磁極23a
との関係で別の好ましい効果が得られる。すなわち、容
器21の収容部底部と磁極23dとの上記関係によって、磁
気ブラシが21内で(単に停滞している状態に比較して)
粗の状態で形成されないので、磁性粒子中へのトナー粒
子の取込み量が過剰になることがない。過剰取込みはト
ナーの帯電不足を招き、かぶり発生の原因となる。By arranging the magnetic pole 23d as described above, the magnetic pole 23a
Another preferable effect is obtained in relation to. That is, due to the above-described relationship between the bottom of the container of the container 21 and the magnetic pole 23d, the magnetic brush is inside the 21 (compared to a stagnant state).
Since it is not formed in a rough state, the amount of toner particles taken into the magnetic particles does not become excessive. Excessive incorporation leads to insufficient charging of the toner and causes fogging.
なおこの構成は現像剤容器内に磁性粒子と非磁性あるい
は弱磁性のトナーが混在している場合にも有効である。This configuration is also effective when magnetic particles and non-magnetic or weakly magnetic toner are mixed in the developer container.
非磁性ブレード24の端部241と現像スリーブ22面との前
記距離d2は50〜800μm、好ましくは150〜500μmであ
る。この距離が50μmより小さいと後述する磁性粒子が
この間に詰まり現像剤層にムラを生じやすいと共に良好
な現像を行うのに必要な現像剤を塗布することが出来ず
濃度の薄いムラの多い現像画像しか得られない欠点があ
る。また800μmより大きいと現像スリーブ22上へ塗布
される現像剤量が増加し所定の現像剤厚の規制が行え
ず、潜像担持体への磁性粒子付着が多くなると共に後述
する現像剤の循環、現像剤限定部材26による現像規制が
弱まりトナーとトリボが不足しカブリやすくなる欠点が
ある。The distance d 2 between the end 241 of the non-magnetic blade 24 and the surface of the developing sleeve 22 is 50 to 800 μm, preferably 150 to 500 μm. If this distance is less than 50 μm, the magnetic particles to be described later become clogged between them and the developer layer is likely to have unevenness, and the developer necessary for good development cannot be applied, resulting in a thin developed image with a large unevenness. There is a drawback that can only be obtained. On the other hand, if it is larger than 800 μm, the amount of the developer applied onto the developing sleeve 22 increases and the predetermined developer thickness cannot be regulated, the magnetic particles adhere to the latent image carrier more, and the circulation of the developer described later, There is a drawback that the regulation of development by the developer limiting member 26 is weakened, toner and tribo are insufficient, and fogging is likely to occur.
次に現像剤塗布量規制部材である非磁性ブレード24の近
傍及び限定部材26の近傍部の磁性粒子層について説明す
る。限定部材は現像剤規制部への補給トナーの不要な進
入を機械的に防ぐだけではない。前述したように、上記
部材26をスリーブに囲まれた規制領域においては磁極23
aのN極によってスリーブの回転とともに搬送された磁
性粒子が限定部材26の案内面261に沿って詰め込まれて
密度がたかくなる。この領域では、搬送されて進入して
くる磁性粒子とブレードから流出していく磁性粒子との
入れ替わりが動的に発生しているため磁性粒子同士がお
互いに衝突してかくらん状態になっているものの実質的
なパツキング状態になっている。このため磁性粒子ない
しはスリーブ上からトナーへのトリボ賦与が行われ、又
磁性粒子ないしはスリーブ上に弱い力で付着して搬送さ
れてきたトリボ賦与の小さいトナーは磁性粒子ないしは
スリーブ上から離脱する。つまり、トナーの選別や、帯
電改良が行われる。従ってトリボ賦与が十分与えられた
トナーを現像に供することができる。又、磁性粒子の搬
送時の不均一状態も該空間において均平化され、磁性粒
子層の塗布の均一化・安定化も達成される。従って限定
部材26は上記案内面261が必須であり、該斜面の傾き及
び空間の容積は該空間での磁性粒子のパツキング状態に
大きな影響を与える。Next, the magnetic particle layer in the vicinity of the non-magnetic blade 24, which is the developer application amount controlling member, and in the vicinity of the limiting member 26 will be described. The limiting member not only mechanically prevents unnecessary invasion of the replenishment toner into the developer regulating portion. As described above, the magnetic pole 23 in the restriction region surrounded by the member 26 is
The magnetic particles conveyed by the rotation of the sleeve by the N pole of a are packed along the guide surface 261 of the limiting member 26, and the density increases. In this area, the magnetic particles that are conveyed and enter and the magnetic particles that flow out from the blade are exchanged dynamically, so that the magnetic particles collide with each other and are in a blunt state. It is in a practical packing state. Therefore, tribo is imparted to the toner from the magnetic particles or the sleeve, and the toner having a small tribo imparted to the magnetic particles or the sleeve by a weak force and conveyed is separated from the magnetic particles or the sleeve. That is, toner selection and charging improvement are performed. Therefore, the toner to which tribo is sufficiently imparted can be used for development. Further, the non-uniform state during the transportation of the magnetic particles is leveled in the space, and the coating of the magnetic particle layer is made uniform and stable. Therefore, the guide surface 261 is essential for the limiting member 26, and the inclination of the slope and the volume of the space have a great influence on the packing state of the magnetic particles in the space.
これに対して、この領域に対して固定配置された磁極23
aは、上記パツキング状態の磁性粒子を磁力線に沿って
再配置する。該空間でのパツキング状態はトリボ賦与に
対しては不安定なところがあり、安定化させるためには
常に一定のパツキング状態を必要とする。これはスリー
ブ上をほぼ接線方向に搬送されてきた磁性粒子を該方向
と直向する力で磁気ブラシを形成するため、磁性粒子へ
の撹拌効果はもちろんのこと、ほぐし効果も働き、上記
トナーへのトリボ賦与及び磁性粒子層の塗布の均一化・
安定化がさらに促進される。この時、周辺の構成によっ
て集中せしめられた現像剤が多大な圧力を受けたままで
あると現像剤がつまり過ぎる問題があるが、磁極23aの
最大磁力を発生する部分が案内面261に対向することに
よって、規制領域中における過大な圧力集中を防止し、
現像剤の集中と安定した高密度の磁性粒子存在割合を維
持できるものと考えられる。On the other hand, the magnetic pole 23 fixedly arranged in this area
In a, the magnetic particles in the packing state are rearranged along the lines of magnetic force. The packing state in the space is unstable with respect to the tribo application, and a constant packing state is always required for stabilization. This forms a magnetic brush with the force of directing the magnetic particles conveyed almost tangentially on the sleeve to the direction, so that not only the stirring effect on the magnetic particles but also the loosening effect works, and Tribo and uniform coating of magnetic particle layer
Stabilization is further promoted. At this time, if the concentrated developer due to the peripheral configuration is still under a great pressure, there is a problem that the developer gets too clogged, but the portion of the magnetic pole 23a that generates the maximum magnetic force faces the guide surface 261. Prevents excessive pressure concentration in the regulated area,
It is considered that the concentration of the developer and the stable high-density magnetic particle existence ratio can be maintained.
上記の規制領域によって、現像スリーブ表面には、安定
した量の磁性粒子と十分に帯電したトナー粒子とが現像
剤薄層として形成できる。従って現像領域102での現像
効果は安定したものとなる。そして前述した現像部に搬
送された現像剤の内少なくとも前記現像担持部材表面に
担持されたトナー粒子を静電潜像担持体に転移させる交
番電界を前記現像部に形成する交互電界形成手段を有
し、前記現像部において、前記静電潜像担持体と前記現
像剤担持部材とで画成される空間の容積に対して、該現
像部に搬送された現像剤の磁性粒子が占める体積比率が
1.5%乃至30%である現像方法及び装置に対して多大な
効果を与えることが確認できた。Due to the above-mentioned restriction region, a stable amount of magnetic particles and sufficiently charged toner particles can be formed as a thin developer layer on the surface of the developing sleeve. Therefore, the developing effect in the developing area 102 becomes stable. An alternating electric field forming means is provided for forming in the developing section an alternating electric field for transferring at least the toner particles carried on the surface of the developing carrying member among the developers conveyed to the developing section to the electrostatic latent image carrier. In the developing section, the volume ratio of the magnetic particles of the developer transported to the developing section to the volume of the space defined by the electrostatic latent image carrier and the developer carrying member is
It has been confirmed that a great effect is exerted on the developing method and apparatus which are 1.5% to 30%.
第2図は現像剤限定部材26の非磁性ブレード側に磁性体
50を設置した場合を示してある。この場合磁性体50は磁
極23aに対向する位置に設けるのは好ましくない。なぜ
ならば対向していると、磁極23aとの間に強い集中磁界
が発生し、上記磁極23aによる磁性粒子のかくはん及び
ほぐし効果が低減するからである。しかし、規制部に磁
性体を設けスリーブ内部磁石23との間で磁性粒子の磁気
的規制を行うことは規制部材のスリーブとの間隙公差の
拡大になり、有効的である。又、磁性粒子ないしはスリ
ーブ上に付着したトナーを比較すると、スリーブ上に付
着したトナーの帯電電荷量は磁性粒子に付着したものよ
りも小さい、この理由はスリーブの移動と供に、磁性粒
子も搬送されるためスリーブ上のトナーが磁性粒子によ
って摺擦される機会が少なくなっているためである。こ
のスリーブ上のトナーを所定の値にまで持ち上げるため
には、スリーブ上のトナーを積極的に摺擦してやる必要
がある。即ち、スリーブ表面近傍でスリーブの移動に反
して相対速度のずれを生じさせる磁性粒子の存在が必要
となる。FIG. 2 shows a magnetic material on the non-magnetic blade side of the developer limiting member 26.
The case where 50 is installed is shown. In this case, it is not preferable to provide the magnetic body 50 at a position facing the magnetic pole 23a. This is because when they face each other, a strong concentrated magnetic field is generated between the magnetic pole 23a and the magnetic particle agitation and loosening effect of the magnetic pole 23a is reduced. However, it is effective to provide a magnetic body in the restricting portion to magnetically restrict the magnetic particles between the restricting portion and the magnet 23 inside the sleeve, because the gap tolerance between the restricting member and the sleeve is increased. Also, when comparing the magnetic particles or the toner adhered on the sleeve, the amount of electrified charge of the toner adhered on the sleeve is smaller than that on the magnetic particles because the movement of the sleeve also carries the magnetic particles. This is because the toner on the sleeve is less likely to be rubbed by the magnetic particles. In order to raise the toner on the sleeve to a predetermined value, it is necessary to positively rub the toner on the sleeve. That is, it is necessary to have magnetic particles in the vicinity of the sleeve surface that cause a relative velocity shift against the movement of the sleeve.
しかし、単純に磁性粒子の搬送性を低下させることは前
述のトナーの取り込み作用を考慮すると、不可能であ
る。又、規制部で上述の様にスリーブ内磁極23aに対向
して磁性体を配置し、集中磁界を発生させ磁界粒子のス
リーブ上への摺擦力を向上することも上述の如く、現像
剤循環規制部材26のつくる空間に磁極の最大磁力発生部
を配置する効果を低減させる。However, simply lowering the transportability of the magnetic particles is impossible in view of the above-mentioned toner intake action. Further, as described above, it is also possible to arrange a magnetic body in the restricting portion so as to face the in-sleeve magnetic pole 23a and generate a concentrated magnetic field to improve the rubbing force of magnetic field particles on the sleeve, as described above. The effect of arranging the maximum magnetic force generating portion of the magnetic pole in the space formed by the regulating member 26 is reduced.
そこで本実施例においては磁極23aよりもスリーブ回転
方向に関して下流側に該磁性体50を設け、磁極23aのブ
レード側の磁力線がほぼスリーブ表面の接線方向に集中
する如く構成した。これによりスリーブ表面近傍のみの
磁性粒子がスリーブ表面に沿って、磁気ブラシを形成
し、スリーブ上のトナーを摺擦し、スリーブ上のトナー
のトリボ賦与を高めることができた。Therefore, in this embodiment, the magnetic body 50 is provided on the downstream side of the magnetic pole 23a in the sleeve rotation direction so that the magnetic lines of force on the blade side of the magnetic pole 23a are substantially concentrated in the tangential direction of the sleeve surface. As a result, the magnetic particles only near the surface of the sleeve formed a magnetic brush along the surface of the sleeve and rubbed the toner on the sleeve to enhance tribo-impartment of the toner on the sleeve.
上記装置構成において、磁性粒子27を、測定条件が測定
電極面積4cm2,電極間間隙0.4cmのサントイツチタイプの
セルを用い、片方の電極に1kg重量の加圧下で、両電極
間の印加電圧E(V/cm)を印加して回路に流れた電流か
ら磁性粒子の抵抗値を得るというもの(以下の磁性粒子
27の抵抗はこの測定条件下の値である)で、E=0.2×1
03で3.1×109Ωcmの抵抗値、E=2×103で4.0×108Ωc
mの抵抗値を示す中抵抗樹脂被覆キヤリア粒子として、
交番電界下で現像を行ったところ、画像部においてキヤ
リア付着がなく、画像部のベタ黒内に白点のような現像
不良を生じることなく、良質の画像が得られた。In the above device configuration, the magnetic particles 27, the measurement condition is a measurement electrode area 4cm 2 , using a gap between the electrodes 0.4cm, using a sun-touch type cell, under pressure of 1kg weight to one electrode, the applied voltage between both electrodes Applying E (V / cm) to obtain the resistance value of magnetic particles from the current flowing in the circuit (the following magnetic particles
The resistance of 27 is the value under this measurement condition), and E = 0.2 × 1
A resistance value of 3.1 × 10 9 Ωcm at 0 3 and 4.0 × 10 8 Ωc at E = 2 × 10 3
As medium resistance resin coated carrier particles showing a resistance value of m,
When the image was developed under an alternating electric field, a good quality image was obtained without carrier adhesion in the image area and without developing defects such as white spots in solid black in the image area.
このように磁性粒子を絶縁性とはせず、若干の電流が流
れる抵抗値とすることで磁性粒子の穂が現像電極の役割
を果たし現像部で非常に高いトナーの振動効果が得られ
るため、かぶり防止効果が高く、高濃度、且つ、中間調
の再現性に優れている。In this way, the magnetic particles do not have an insulating property and the resistance of a slight amount of current is used so that the spikes of the magnetic particles serve as a developing electrode and a very high toner vibration effect is obtained in the developing section. High fog prevention effect, high density, and excellent halftone reproducibility.
この磁性粒子の抵抗値条件が上記のE=0.2×103,E=2
×103との範囲内に対するもので規定しているのは、電
界依存性の電気抵抗変化が、この範囲内で大きく変化
し、これより大の電界ではなだらかな抵抗減少があるた
め、この範囲内の抵抗変化は交互電界中の電界変化に対
応するものと認識できるためである。The resistance value condition of this magnetic particle is the above E = 0.2 × 10 3 , E = 2
Specified within the range of × 10 3 is that the electric field-dependent electric resistance change greatly changes within this range, and there is a gradual decrease in resistance at higher electric fields. This is because it can be recognized that the change in resistance inside corresponds to the change in electric field during the alternating electric field.
本発明者は、数多くの実験から、この範囲内の抵抗変化
が現像性に大きく影響することをつきとめ、市販の絶縁
性キヤリアに改良を数多く加えて到達したものが以下の
条件である。The present inventors have found from a number of experiments that the resistance change within this range has a large effect on the developability, and the following conditions have been reached by making many improvements to the commercially available insulating carrier.
即ち、磁性キヤリア粒子の抵抗をR(Ωcm)とすると、
測定電圧E(V/cm)が0.2×103(V/cm)以上2×103(V
/cm)以下の範囲内で、 で画成される領域内を少なくとも1点以上通過する抵抗
特性を示す樹脂被覆磁性キヤリア粒子であれば、交番電
界中において、画像を乱すことなく、しかも耐久性があ
りキヤリア損失も少なく安定した画像を達成する。樹脂
被覆のため、湿度変化に対して特性が変化せず、流動性
が高く実用上の利点が覆いことはいうまでもない。That is, if the resistance of the magnetic carrier particles is R (Ωcm),
Measurement voltage E (V / cm) is 0.2 × 10 3 (V / cm) or more 2 × 10 3 (V
/ cm) within the following range, If the resin-coated magnetic carrier particles exhibit resistance characteristics of passing at least one point in the area defined by, the image will not be disturbed in an alternating electric field, and the image will be durable and stable with little carrier loss. To achieve. Needless to say, because of the resin coating, the characteristics do not change in response to changes in humidity, the fluidity is high and the practical advantage is covered.
本実施例に用いる磁性粒子は公知の焼結フエライトであ
り、Zn,Fe,Cd,Cu,Pb,Ni,Mg,Mn,などの1種あるい2種以
上の組成の焼結からつくられる。特に本発明に適する組
成はCuO,ZnO,Fe2O3を主成分とする金属酸化物である。The magnetic particles used in this example are known sintered ferrites, and are made by sintering one or more compositions of Zn, Fe, Cd, Cu, Pb, Ni, Mg, Mn. A composition particularly suitable for the present invention is a metal oxide containing CuO, ZnO and Fe 2 O 3 as main components.
上記条件がいかに有効であるかを第1図の領域(ABCD)
とデータをもって説明する。Figure 1 area (ABCD) shows how effective the above conditions are.
And explain with data.
第1図のk,l,m,n,o,p,g,r,s,tの記号で示す磁性粒子は
前記酸化銅及び亜鉛を用いて焼結条件又は/且つ焼結フ
エライト粒子に樹脂コートする条件を変化させた場合の
横軸に測定用電界Eを縦軸に磁性粒子の抵抗値Rを示す
グラフにおける磁性粒子の電気抵抗特性曲線である。例
えばn磁性粒子はコート樹脂量をp磁性粒子よりも2倍
にしてある。測定は常温,常湿で行った。なお、樹脂コ
ート材は従来から用いられていた。2成分現像剤のキヤ
リアコート材、例えば、アクリルフツ素系樹脂やシリコ
ーン系樹脂等でよいが、第1図例ではシリコーンの樹脂
を用いた。最大磁性64emu/gで、粘度分布70〜50μ(250
/350メツシユ)のフエライトを用いた。The magnetic particles indicated by the symbols k, l, m, n, o, p, g, r, s, and t in FIG. 1 are the sintering conditions using the copper oxide and zinc, and / or the resin is used as the sintered ferrite particles. 6 is an electric resistance characteristic curve of magnetic particles in a graph showing the electric field for measurement E on the horizontal axis and the resistance value R of the magnetic particles on the vertical axis when the coating conditions are changed. For example, the amount of coating resin for n magnetic particles is twice that of p magnetic particles. The measurement was performed at normal temperature and normal humidity. The resin coating material has been used conventionally. A carrier coating material for a two-component developer, such as an acrylic fluorine resin or a silicone resin, may be used, but in the example of FIG. 1, a silicone resin is used. Maximum magnetic 64emu / g, viscosity distribution 70-50μ (250
/ 350 mesh) ferrite was used.
下表にk〜tまでの特性をもった磁性粒子の画像評価を
示す。粒子kからtに向って樹脂被覆量は小さく、粒子
oとpは、焼結条件を変えたものである。The table below shows the image evaluation of magnetic particles having characteristics of k to t. The amount of resin coating is small from the particles k to t, and the particles o and p are obtained by changing the sintering conditions.
×:画像悪 △:画像やや良 ○:画像良 ◎:画像最良 尚、市販の絶縁キヤリア粒子は、かなりの高抵抗を示
し、第3図のグラフ中に記載できるものではなく、これ
を用いた画像像は、白ヌケやキヤリア粒子の付着が見ら
れ、満足のいくものではなかった。×: Image is bad △: Image is slightly good ○: Image is good ◎: Image is best In addition, the commercially available insulating carrier particles showed a considerably high resistance and could not be described in the graph of FIG. 3, and the image image using this image shows satisfactory whiteness and adhesion of the carrier particles. It didn't go.
第1図の線CDよりも低い電気抵抗を示す磁性粒子tは画
像上現像剤のブラシ跡が生じやすく、又ベタ画像部に画
像が抜けた白点が発生しやすい。これらは磁性粒子を通
じて発生する潜像電荷のリークによるものである。又ベ
タ黒画像部に磁性粒子が付着しやすい。本発明によれば
磁性粒子の抵抗を線分ABを超えることでこれらの発生を
有効に防止できる。The magnetic particles t having an electric resistance lower than that of the line CD in FIG. 1 are likely to cause a brush mark of the developer on the image, and easily generate a white spot where an image is missing in a solid image portion. These are due to leakage of latent image charges generated through the magnetic particles. In addition, magnetic particles tend to adhere to the solid black image area. According to the present invention, the generation of these can be effectively prevented by making the resistance of the magnetic particles exceed the line segment AB.
第1図の線分ABよりも高い電気抵抗を示す磁性粒子は磁
性粒子自身の帯電性が強くなりトナー粒子と強固に付着
するため現像領域で潜像電荷へ飛翔しにくくなる。この
ため画像濃度が低下する。又、磁性粒子が現像電極とし
て働く効果も低下し、濃度低下を引き起こす。又、トナ
ーの電荷極性と逆極性に磁性粒子が帯電しやすいため非
画像部ベタ白部にキヤリアが付着しやすくなる。特に本
発明を適用した実施例の現像装置においては、容器内の
磁性粒子層の循環作用によって必要な補給トナーを磁性
粒子層へ取り込む構成となっているため磁性粒子の帯電
性が強すぎると、磁性粒子層へのトナーの取り込みの不
安定化を引き起こし、これにより画像上スジ,ムラを発
生しやすくなるが、本発明の適用によって、この不都合
も解決できる。これは装置の問題を解決するので重要な
技術である。The magnetic particles having an electric resistance higher than that of the line segment AB in FIG. 1 have a stronger charging property of the magnetic particles themselves and firmly adhere to the toner particles, so that they are less likely to fly to the latent image charge in the developing area. Therefore, the image density is reduced. In addition, the effect of the magnetic particles acting as a developing electrode also decreases, causing a decrease in density. Further, since the magnetic particles are likely to be charged with the polarity opposite to the charge polarity of the toner, the carrier is likely to be attached to the solid white portion in the non-image area. In particular, in the developing device of the embodiment to which the present invention is applied, when the replenishment toner required by the circulating action of the magnetic particle layer in the container is incorporated into the magnetic particle layer, the chargeability of the magnetic particles is too strong, This causes instability of the toner taken into the magnetic particle layer, which easily causes streaks and unevenness on the image. However, application of the present invention can solve this problem. This is an important technique as it solves the device problem.
上記実施例の樹脂をアクリルフツ素系の樹脂に変えて実
験を行ったところ同様の結果が得られた。又、磁性粒子
の径を変化させたところ画像上の変化はみられず、上記
抵抗特性が交番電界印加の現像方法に極めて有効である
こともたしかめられた。The same result was obtained when an experiment was conducted by changing the resin of the above-mentioned example to an acrylic fluorine resin. Further, when the diameter of the magnetic particles was changed, no change was observed on the image, and it was confirmed that the above resistance characteristics are extremely effective for the developing method in which an alternating electric field is applied.
上記実施例から理解できるように、測定電界0.2×103〜
2×103(V/cm)で、磁性粒子が示す抵抗値が上記領域
内にすべて含まれていることは、より好ましい画像を形
成できる。これは、交番電界が強度変化するものである
ために、この領域内での抵抗変化のみを示すことによっ
て常に安定した挙動を示すためであると考えられる。特
に注目すべきことは、磁性粒子が電界0.2×103(V/cm)
で108Ωcm以上1011Ωcm以下,2×103(V/cm)で2×107
Ωcm以上3×109Ωcm以下の抵抗値を示すことで上記の
挙動を得られることになることである。As can be understood from the above example, the measured electric field 0.2 × 10 3 ~
A more preferable image can be formed when the resistance value of the magnetic particles is 2 × 10 3 (V / cm) and is entirely within the above range. It is considered that this is because the alternating electric field changes in intensity, and therefore exhibits stable behavior by showing only the resistance change in this region. Of particular note is that magnetic particles have an electric field of 0.2 × 10 3 (V / cm).
At 10 8 Ωcm or more and at 10 11 Ωcm or less, 2 × 10 3 (V / cm) at 2 × 10 7
The above behavior can be obtained by exhibiting a resistance value of Ωcm or more and 3 × 10 9 Ωcm or less.
さらに重要なことは、E(0.2×103,2×1010),F(2×
103,109),H(2×103,5×107),G(0.2×103,2×108)
の4点を互いに結んだ領域Z(斜線部)内に磁性粒子の
抵抗変化がすべて入るものについては、極めて好ましい
結果が得られた。これは、上記領域の中間領域を示すも
である。More importantly, E (0.2 × 10 3 , 2 × 10 10 ), F (2 ×
10 3 , 10 9 ), H (2 × 10 3 , 5 × 10 7 ), G (0.2 × 10 3 , 2 × 10 8 )
Very preferable results were obtained for those in which the resistance change of the magnetic particles was entirely within the region Z (hatched portion) in which the four points were connected to each other. This is also an intermediate area of the above area.
これは、図の曲線を延長し、実際の交番電界の最大強度
下での印加電圧を測定値に変更して想定して見ると、磁
性粒子が、最大交番電界の現像下で5×107Ωcm以上
(少なくとも2×107Ωcm以上)109Ωcm以下の高抵抗を
安定した範囲内で示すと供に、低電界下でも安定した領
域Zの高抵抗を安定領域Zの高抵抗を示すこになるから
であると考えられる。This is because, assuming that the curve in the figure is extended and the applied voltage under the maximum strength of the actual alternating electric field is changed to the measured value, the magnetic particles are 5 × 10 7 under the development of the maximum alternating electric field. In addition to showing a high resistance of Ωcm or more (at least 2 × 10 7 Ωcm or more) of 10 9 Ωcm or less within a stable range, a high resistance of a stable area Z even under a low electric field should be a high resistance of a stable area Z. It is thought to be because.
いずれにしても線文ABを越えず、線分CDを下回らない電
気抵抗特性をもつ磁性粒子を用いることで、従来の樹脂
被覆絶縁キヤリア粒子の欠点を効果的に防止できる。In any case, by using magnetic particles having electric resistance characteristics that do not exceed the line sentence AB and do not fall below the line segment CD, the drawbacks of the conventional resin-coated insulating carrier particles can be effectively prevented.
以上のように第1図の4つの線分で囲まれた領域が、現
像される画像の品質に関して極めて臨界的なものである
ことは、この領域から、はずれた設定条件下で著しい画
質の低下が認められるという実験事実から明白なものと
考える。As described above, the area surrounded by the four line segments in FIG. 1 is extremely critical with respect to the quality of the image to be developed. I think it is obvious from the experimental fact that
尚、磁極23aの磁束密度は600G以上、好ましくは700G以
上が好ましい。これは磁性粒子層のトナーコンテンツ変
化に対して現像剤の塗布状態がカツト磁極の磁束密度が
高い程安定する傾向にあるからである。特にトナーコン
テンツ維持のために自動トナー補給装置を持たない本発
明の現像装置に於いては800G以上の磁束密度であること
が好ましい。The magnetic flux density of the magnetic pole 23a is 600 G or higher, preferably 700 G or higher. This is because the applied state of the developer tends to be more stable as the magnetic flux density of the cut magnetic pole is higher, against changes in the toner content of the magnetic particle layer. Particularly, in the developing device of the present invention which does not have an automatic toner replenishing device for maintaining the toner content, it is preferable that the magnetic flux density is 800 G or more.
第2図に於いて磁極23cは現像磁極であるが、この現像
磁極は、ほぼ現像部に位置し、磁性粒子の潜像への付着
を防止するため、800G以上の磁束密度であるとよい。In FIG. 2, the magnetic pole 23c is a developing magnetic pole. The developing magnetic pole is located almost at the developing portion and preferably has a magnetic flux density of 800 G or more in order to prevent magnetic particles from adhering to the latent image.
本発明は、上述した各構成の任意の組合せを含むことは
言うまでもない。It goes without saying that the present invention includes any combination of the above-described configurations.
いずれにしても本発明は、従来現像方法、装置では得ら
れなかった高画質を提供できるものであり、現像装置を
使い捨てタイプの小型なものにできたという優れた効果
を奏するものである。In any case, the present invention can provide a high image quality which has not been obtained by the conventional developing method and apparatus, and has an excellent effect that the developing apparatus can be a disposable type small-sized apparatus.
トナー供給部材は現像容器36内にあって磁性粒子層に近
接或いは接触して矢印d方向に回転駆動してトナー37を
磁性粒子層へ供給する。The toner supply member is in the developing container 36 and is close to or in contact with the magnetic particle layer to rotate and drive in the direction of arrow d to supply the toner 37 to the magnetic particle layer.
現像容器36の概略水平方向に隣接してトナーを貯蔵して
おくトナー貯蔵容器38を配設し、該トナー貯蔵容器内に
は現像容器36内へトナーを送るトナー搬送部材(不図
示)が設けられている。A toner storage container 38 for storing toner is arranged adjacent to the developing container 36 in a substantially horizontal direction, and a toner conveying member (not shown) for feeding the toner into the developing container 36 is provided in the toner storage container. Has been.
S磁極23bはカツト磁極23aと現像磁極23cの間隔が離れ
ているために非磁性ブレード24部で均一に塗布された現
像剤層が乱れるのを防止するために設けられた搬送磁極
である。S磁極23bは現像剤層を乱さぬために磁極の強
さとしては概略現像磁極23cと同等かやや低目が良い。
現像スリーブとして20φのものを用いた場合、カツト磁
極と現像磁極の間隔がスリーブ中心角で100°以内であ
ればスリーブ上の現像剤層の乱れは少ないが100°を越
えた場合、現像剤層の乱れれが大きく中間に搬送極を設
けた方が好ましい。The S magnetic pole 23b is a carrier magnetic pole provided to prevent the developer layer applied uniformly on the nonmagnetic blade 24 from being disturbed because the cut magnetic pole 23a and the developing magnetic pole 23c are separated from each other. Since the S magnetic pole 23b does not disturb the developer layer, the strength of the magnetic pole is approximately equal to or slightly lower than that of the developing magnetic pole 23c.
When using a developing sleeve with a diameter of 20φ, if the distance between the cutting magnetic pole and the developing magnetic pole is within 100 ° at the sleeve center angle, the developer layer on the sleeve is less disturbed, but if it exceeds 100 °, the developer layer It is preferable that a carrier electrode be provided in the middle because the carrier is greatly disturbed.
S磁極23dは現像後の現像剤を回収する回収磁極であ
り、磁性シール先端部よりも現像スリーブ移動方向上流
側に配置される。磁極23dが磁性シール先端部より下流
側に配置された場合、現像容器下部のトナー取り込み口
付近に磁極23dによる磁性粒子の穂立ち部分が生じ、ト
ナーを極めて取り込み易くなり摩擦帯電が十分に行われ
ずカブリ等の原因になりやすい。The S magnetic pole 23d is a recovery magnetic pole for recovering the developer after development, and is arranged on the upstream side in the moving direction of the developing sleeve with respect to the tip of the magnetic seal. If the magnetic pole 23d is located downstream of the tip of the magnetic seal, the magnetic particles 23d will have a spiked portion near the toner intake port at the bottom of the developing container, and it will be extremely easy to take in toner, resulting in insufficient triboelectrification. It is easy to cause fog.
ここで、現像部における磁性粒子の体積比率について説
明する。「現像部」とはスリーブ22から感光ドラム1へ
のトナーが転移あるいは供給される部分である。「体積
比率」とはこの現像部の容積に対するその中に存在する
磁性粒子の占める体積の百分率である。上記現像装置に
おいてはこの体積比率が重要な影響を有すること、およ
びこれを1.5〜30%、特に2.6〜26%とすることが極めて
好ましい。Here, the volume ratio of the magnetic particles in the developing section will be described. The “developing portion” is a portion where the toner is transferred or supplied from the sleeve 22 to the photosensitive drum 1. "Volume ratio" is the percentage of the volume occupied by the magnetic particles present therein to the volume of this developing zone. In the above-mentioned developing device, it is extremely preferable that this volume ratio has an important influence, and that it is 1.5 to 30%, particularly 2.6 to 26%.
1.5%未満では、現像像濃度の低下が認められること、
スリーブゴーストが発生すること、穂51が存在する部分
としない部分との間で顕著な濃度差が発生すること、ス
リーブ22表面上に形成される現像剤像の厚さが全体的に
不均一となること、などの点で好ましくない。If it is less than 1.5%, a reduction in developed image density is observed,
A sleeve ghost occurs, a remarkable density difference occurs between a portion where the spikes 51 are present and a portion where the spikes 51 are not present, and the thickness of the developer image formed on the surface of the sleeve 22 is generally uneven. It is not preferable in that it becomes.
30%を超えると、スリーブ面を閉鎖する度合が増大し、
かぶりが発生すること、などの点で好ましくない。When it exceeds 30%, the degree of closing the sleeve surface increases,
It is not preferable in terms of fogging.
特に、本発明にとって、好ましい現像方法として挙げた
上記条件は体積比率の増加あるいは減少にしたがって画
質が単調に劣化または増加するのではなく、1.5〜30%
の範囲で十分な画像濃度が得られ、1.5%未満でも30%
を超えても、画質低下が発生し、しかもこの画質が十分
な上記数値の範囲ではスリーブゴーストもかぶりも発生
しないという事実に基づくものである。前者の画質低下
は負性特性によるものと思われ、後者は磁性粒子の存在
量が大きくなってスリーブ22表面を開放できなくなりス
リーブ22表面からのトナー供給量が大幅に減少すること
から生ずると考えられる。In particular, for the present invention, the above-mentioned conditions listed as the preferred developing method do not cause the image quality to monotonically deteriorate or increase as the volume ratio increases or decreases, but 1.5 to 30%.
A sufficient image density can be obtained in the range of, and 30% even if it is less than 1.5%.
This is based on the fact that the image quality is deteriorated even if the value exceeds the above range, and neither the sleeve ghost nor the fog occurs in the range of the above numerical value where the image quality is sufficient. It is considered that the former image quality deterioration is due to the negative characteristic, and the latter is because the amount of magnetic particles present becomes large and the surface of the sleeve 22 cannot be opened, and the toner supply amount from the surface of the sleeve 22 is significantly reduced. To be
又、1.5%未満では、線画像の再現性に劣り、画質濃度
の低下が顕著である。逆に30%えを超えた場合は磁性粒
子が感光ドラム面を傷つける問題、画質の一部として付
着して行くために生じる転写、定着の問題がある。On the other hand, if it is less than 1.5%, the reproducibility of the line image is inferior, and the image quality density is significantly lowered. On the other hand, if it exceeds 30%, there are problems that the magnetic particles damage the surface of the photosensitive drum, and transfer and fixing problems that occur because they adhere as part of the image quality.
そして、磁性粒子の存在が1.5%に近い場合は、大面積
の一様高濃度画像(ベタ黒)の再現時に、「あらび」と
称せられる部分的現像ムラが発生する場合(特別環境下
等)があるので、これらが発生しにくい体積比率とする
ことが好ましい。この数値は現像部に対して磁性粒子の
体積比率が2.6%以上であることで、この範囲はより好
ましい範囲となる、又、磁性粒子の存在が30%に近い場
合は、磁性粒子の穂が接する部分の周辺にスリーブ面か
らのトナー補給が遅れる場合(現像速度大の時等)があ
り、ベタ黒再現時にうろこ状の濃度ムラを生じる可能性
がある。これを防止する確実な範囲としては、磁性粒子
の上記体積比率が26%以下がより好ましいものとなる。When the presence of magnetic particles is close to 1.5%, partial development unevenness called "arabi" occurs when reproducing a large area uniform high-density image (solid black) (e.g. under special environment). Therefore, it is preferable that the volume ratio is such that these are less likely to occur. This value is because the volume ratio of the magnetic particles to the developing portion is 2.6% or more, this range becomes a more preferable range, and when the presence of the magnetic particles is close to 30%, the spikes of the magnetic particles are There is a case where toner supply from the sleeve surface is delayed around the contacting portion (when the developing speed is high, etc.), and scaly density unevenness may occur during solid black reproduction. As a certain range for preventing this, the volume ratio of the magnetic particles is more preferably 26% or less.
体積比率が1.5%〜30%の範囲であれば(実施例では4
%に設定した)、第3図に示すようにスリーブ22表面上
に穂51が好ましい程度に疎らな状態で形成され。スリー
ブ22および穂上の両方のトナーが感光ドラム1に対して
十分に開放され、スリーブ上のトナー100も交番電界で
飛翔転移するので、ほとんどすべてのトナーが現像に消
費可能な状態となることから高い現像効率(現像部に存
在するトナーのうち現像に消費され得るトナーの割合)
および高画像濃度が得られる。好ましくは、微小なしか
し激しい穂の振動を生じさせ、これによって磁性粒子お
よびスリーブ22に付着しているトナー100がほぐされ
る。いずれにせよ磁気ブラシの場合などのような掃目む
らやゴースト像の発生を防止できる。さらに、穂の振動
によって、磁性粒子27とトナー28との摩擦接触が活発に
なるのでトナー28への摩擦帯電を向上させ、かぶり発生
を防止できる。なお、現像効率が高いことが現像装置の
小型化に適する。第3図の現像磁極はS極23bとして第
2図の現像極23cと変えているが、本例としてはどちら
でも良い。If the volume ratio is in the range of 1.5% to 30% (4 in the embodiment)
%), And the ears 51 are formed on the surface of the sleeve 22 in a sparse state to a desired degree as shown in FIG. Both the toner on the sleeve 22 and the ears are sufficiently opened to the photosensitive drum 1, and the toner 100 on the sleeve also fly-transfers due to the alternating electric field, so that almost all of the toner is ready for consumption for development. High development efficiency (ratio of toner that can be consumed for development among the toner existing in the development area)
And high image density is obtained. Preferably, a slight but severe spike vibration is produced, which loosens the magnetic particles and the toner 100 adhering to the sleeve 22. In any case, it is possible to prevent the generation of uneven sweep and ghost image as in the case of a magnetic brush. Further, the friction of the magnetic particles 27 and the toner 28 is activated by the vibration of the ears, so that the triboelectric charge on the toner 28 can be improved and the occurrence of fogging can be prevented. High development efficiency is suitable for downsizing of the developing device. The developing magnetic pole in FIG. 3 is the S pole 23b, which is different from the developing pole 23c in FIG. 2, but either one may be used in this example.
上記現像部に存在する磁性粒子27の体積比率は(M/h)
×(1/ρ)×[(C/(T+C)]で求めることができ
る。ここでMはスリーブの単位面積当りの現像剤(混合
物・・・・非穂立時)の塗布量(g/cm2)、hは現像部
空間の高さ(cm)、ρは磁性粒子の真密度g/cm3、C/
(T+C)はスリーブ上の現像剤中の磁性粒子の重量割
合である。The volume ratio of the magnetic particles 27 existing in the developing section is (M / h)
It can be calculated by × (1 / ρ) × [(C / (T + C)], where M is the coating amount (g / cm) of the developer (mixture ... in the non-peaking) per unit area of the sleeve. 2 ), h is the height of the developing space (cm), ρ is the true density of magnetic particles g / cm 3 , C /
(T + C) is the weight ratio of magnetic particles in the developer on the sleeve.
なお、上記定義の現像部において磁性粒子に対するトナ
ーの割合は4〜40重量%が好ましい。上記実施例のよう
に交番電界が強い(変化率が大きいかまたはVppが大き
い)場合、穂がスリーブ22からあるいはその基部から離
脱し、離脱した磁性粒子27はスリーブ22と感光ドラム1
との間の空間を往復運動する。この往復運動のエネルギ
ーは大きいので、上述の振動による効果がさらに促進さ
れる。The ratio of the toner to the magnetic particles in the developing section defined above is preferably 4 to 40% by weight. When the alternating electric field is strong (the rate of change is large or Vpp is large) as in the above-mentioned embodiment, the ears separate from the sleeve 22 or the base thereof, and the separated magnetic particles 27 are separated from the sleeve 22 and the photosensitive drum 1.
Reciprocates in the space between. Since the energy of this reciprocating motion is large, the effect of the above-mentioned vibration is further promoted.
以上の挙動は高速度カメラ(日立製作所製)で8000コマ
/秒の撮影を行って確認された。感光ドラム1表面とス
リーブ22表面との間隙を小さくして、感光ドラム1と穂
との接触圧力を高め、振動を小さくした場合でも、現像
部の入口側および出口側では空隙は大きいので、十分な
振動が起り、上述の効果が奏される・ 逆に、感光ドラム1とスリーブ22との間隙を大きくし
て、磁界を印加しない状態で穂は感光ドラム1に接触し
ないが、印加した場合は接触するような距離とすること
が好ましい。The above behavior was confirmed by shooting 8000 frames / sec with a high-speed camera (manufactured by Hitachi, Ltd.). Even when the gap between the surface of the photosensitive drum 1 and the surface of the sleeve 22 is made small to increase the contact pressure between the photosensitive drum 1 and the ears and the vibration is made small, the gap is large on the inlet side and the outlet side of the developing section, so it is sufficient. However, when the magnetic field is not applied, the ears do not come into contact with the photosensitive drum 1 when the magnetic field is not applied. It is preferable that the distance is such that they come into contact with each other.
第2図において、スリーブ22として直径20mmのアルミス
リーブの表面を、アランダム砥粒により不定型サンドブ
ラスト処理したものを用い、磁石23として4極着磁でN
極、S極が交互に第2図で示されるようなものを用い
た。磁石23による表面磁束密度の最大値は約900ガウス
であった。In FIG. 2, a sleeve 22 is made of an aluminum sleeve having a diameter of 20 mm, the surface of which is subjected to irregular sandblasting with alundum abrasive grains.
A pole and a south pole were used alternately as shown in FIG. The maximum value of the surface magnetic flux density by the magnet 23 was about 900 gauss.
ブレード24としては1.2mm厚の非磁性ステンレスを用
い、上記角度θを15°とした。磁性粒子としては、上記
領域の範囲内の抵抗特性を示す粒子0で表面にシリコン
樹脂コートした粒径70〜50μ(250/350メツシユ)のフ
エライト(最大磁化64emu/g)を用いた。電気抵抗は第
1図のn,o,p,q曲線のものを用いて良結果を得た。As the blade 24, 1.2 mm thick non-magnetic stainless steel was used, and the angle θ was set to 15 °. Ferrite (maximum magnetization 64 emu / g) having a particle size of 70 to 50 μ (250/350 mesh) having a surface coated with a particle 0 exhibiting resistance characteristics within the above range was used as the magnetic particles. Good results were obtained by using the n, o, p, q curves of FIG. 1 for the electric resistance.
第1図の実施例のようにスリーブ上の磁性粒子層の循環
によってトナーの取り込み制御を行う系においては磁性
粒子の抵抗はたかくないことが好ましい。これは磁性粒
子自身の帯電を少なくした方がトナー取り込み安定化に
なるためである。磁性粒子の帯電性が強いと、トナーが
磁性粒子上に強固に付着しているためトナーを磁性粒子
層に新らたに取り込む場合、前回に付着していたトナー
と新らたに取り込むトナーとの入り替りが発生しにく
い。このため前回付着したトナーが長時間スリーブ上に
存在し、このトナー自身帯電過剰を引きおこす。好まし
くは第1図E,F,G,Hの各4点を結ぶ線分によって囲まれ
る領域と電気抵抗特性曲線とが交わることが必要であ
る。さらに好ましくはEG,FHに線分と交わることが必要
である。In the system in which the toner intake is controlled by circulating the magnetic particle layer on the sleeve as in the embodiment of FIG. 1, it is preferable that the resistance of the magnetic particles is not high. This is because the toner intake is stabilized when the magnetic particles themselves are less charged. If the magnetic particles have a strong charging property, the toner adheres strongly to the magnetic particles, so when newly incorporating the toner into the magnetic particle layer, the toner that was previously attached and the toner that is newly incorporated. It is difficult for the replacement of. For this reason, the toner that was previously attached remains on the sleeve for a long time, and the toner itself causes excessive charging. Preferably, it is necessary that the region surrounded by the line segment connecting each of the four points of E, F, G, and H in FIG. 1 intersects with the electric resistance characteristic curve. More preferably, it is necessary that EG and FH intersect with the line segment.
非磁性トナーとしては、スチレン/ブタジエン共重合体
系樹脂100部に銅フタロシアニン系顔料5部から成る平
均粒径10μのトナー粉体にコロイダルシリカ0.6%を外
添したブルートナーを用いたところ、スリーブ22表面上
にコーテイング厚約10〜30μmのトナー塗布層を得、さ
らにその上層として200〜300μの磁性粒子層を得た。各
磁性粒子の表面上には上記トナーが付着している。As the non-magnetic toner, a blue toner obtained by externally adding 0.6% of colloidal silica to a toner powder having an average particle size of 10 μm, which is composed of 100 parts of styrene / butadiene copolymer resin and 5 parts of copper phthalocyanine pigment, is used. A toner coating layer having a coating thickness of about 10 to 30 μm was obtained on the surface, and a magnetic particle layer having a thickness of 200 to 300 μ was obtained as an upper layer. The toner adheres to the surface of each magnetic particle.
このときのスリーブ22上の磁性粒子と全トナーとの合計
重量は約2.43×10-2g/cm2であった。At this time, the total weight of the magnetic particles on the sleeve 22 and all the toner was about 2.43 × 10 -2 g / cm 2 .
このときの磁性粒子付着トナーとスリーブ付着トナーの
重量比は約2:1であった。At this time, the weight ratio of the toner attached to the magnetic particles and the toner attached to the sleeve was about 2: 1.
磁性粒子は現像部およびその近傍でスリーブ22内の磁極
23bにより磁界によって穂立ちして、最大長約1.2mm程の
穂立ちブラシを形成していた。The magnetic particles are magnetic poles inside the sleeve 22 at and near the developing unit.
By 23b, the spikes were erected by a magnetic field to form a shaving brush with a maximum length of about 1.2 mm.
帯電量をブローオフ法で測定したところスリーブ上及び
磁性粒子上のトナーのトリボ電荷量が+12μC/gであっ
た。When the charge amount was measured by the blow-off method, the triboelectric charge amount of the toner on the sleeve and the magnetic particles was +12 μC / g.
この現像装置をキヤノン(株)製PC-10型複写機に組み
込み、感光ドラム3(有機感光材料製)とスリーブ22の
表面との間隔を350μmとしたこの条件で体積比率を求
めると、約10%であった。(h=350μm、M=2.43×1
0-2g/cm2、ρ=5.5g/cm3、T/(T+C)=20.4%)。バ
イアス電源4として周波数1600Hz,ピーク対ピーク値130
0Vの交流電圧に−300Vの直流電圧を重畳させたものを用
いて現像を行ったところ、良好なブルー色の画像を得
た。When this developing device was installed in a PC-10 type copying machine manufactured by Canon Inc. and the distance between the photosensitive drum 3 (made of an organic photosensitive material) and the surface of the sleeve 22 was 350 μm, the volume ratio was calculated to be about 10 %Met. (H = 350 μm, M = 2.43 × 1
0 -2 g / cm 2 , ρ = 5.5 g / cm 3 , T / (T + C) = 20.4%). Frequency 1600Hz, peak-to-peak value 130 as bias power supply 4
When development was carried out using an alternating voltage of 0 V and a DC voltage of −300 V superimposed, a good blue image was obtained.
また、ベタ黒画像について現像し、現像後のスリーブ面
を観察したところ、磁性粒子に付着したトナー及びスリ
ーブ上のトナーはほとんど消費され100%近い現像効率
で現像が行われていた。Further, when the solid black image was developed and the sleeve surface after the development was observed, the toner adhering to the magnetic particles and the toner on the sleeve were almost consumed, and the development was performed at a developing efficiency close to 100%.
現像特性についてもカブリが無く、キヤリア付着がなく
良好現像特性を得ることができた。Regarding the developing characteristics, there was no fogging and no carrier adhesion, and good developing characteristics could be obtained.
また、感光体としては非常にピンホール、傷が発生しに
くいOPCを用いているため107〜1011Ωcmの電流が流れ現
像電極効果の得られる磁性粒子を用いても現像バイアス
の集中的リークが発生しない。In addition, because OPC is used as a photoconductor, which is extremely resistant to pinholes and scratches, a current of 10 7 to 10 11 Ωcm flows, and even if magnetic particles that produce the developing electrode effect are used, a concentrated leak of the developing bias occurs. Does not occur.
さらに、磁性部材31の効果についても、良好な磁性粒子
の進入、漏出防止および良好な循環が行われることが確
認された。Further, regarding the effect of the magnetic member 31, it was confirmed that good intrusion and leakage of magnetic particles and good circulation can be performed.
以上の説明のごとく、本実施例によれば、高画像濃度、
高現像効率で、かぶり、ゴースト像、掃目むら、負性特
性のない現像を行うことができる。As described above, according to this embodiment, high image density,
It is possible to perform development without fog, ghost image, unevenness of sweep, and negative characteristics with high development efficiency.
スリーブ22の材料としてはアルミニウムのほか真ちゅう
やステンレス鋼などの導電体、紙筒や合成樹脂の円筒を
使用可能である。また、これら円筒の表面を導電処理す
るか、導電体で構成すると現像電極として機能させるこ
ともできる。さらに、芯ロールを用いてその周面に導電
性の弾性体、例えば導電性スポンジを巻装して構成して
もよい。As the material of the sleeve 22, a conductor such as brass or stainless steel, a paper cylinder or a cylinder of synthetic resin can be used in addition to aluminum. Further, the surface of these cylinders can be made to function as a developing electrode if they are subjected to a conductive treatment or are made of a conductor. Further, a core roll may be used to wind a conductive elastic body, for example, a conductive sponge, around the peripheral surface of the core roll.
現像部の磁極23bについては、実施例では現像部の中央
に磁極を配置したが、中央からずらした位置としてもよ
く、また磁極間に現像部を配置するようにしてもよい。Regarding the magnetic pole 23b of the developing unit, the magnetic pole is arranged at the center of the developing unit in the embodiment, but it may be displaced from the center, or the developing unit may be arranged between the magnetic poles.
トナーには、流動性を高めるためにシリカ粒子や、例え
ば転写方式画像形成方法に於いて潜像保持部材たる感光
ドラム3の表面の研磨のために研磨材粒子等を外添して
もよい。トナー中に少量の磁性粒子を加えたものを用い
てもよい。すなわち、磁性粒子に比べ著しく弱い磁性で
あり、トリボ帯電可能であれば磁性トナーも用いること
ができる。To the toner, silica particles may be externally added to improve the fluidity, and abrasive particles or the like may be externally added for polishing the surface of the photosensitive drum 3, which is a latent image holding member in the transfer type image forming method. You may use what added a small amount of magnetic particles to the toner. That is, the magnetic toner is remarkably weaker than the magnetic particles, and a magnetic toner can be used as long as the toner can be tribocharged.
ゴースト像現像を防止するために、容器21内へ戻り回動
したスリーブ22面から現像に供されずにスリーブ22上に
残った現像剤層を、一旦スクレーバ手段(不図示)でか
き落し、そのかき落しされたスリーブ面を磁性粒子層に
接触させて現像剤の再コーテイングを行わせるようにし
てもよい。In order to prevent ghost image development, the developer layer remaining on the sleeve 22 that has not been used for development from the surface of the sleeve 22 that has returned to the inside of the container 21 and has been rotated is scraped off once by a scraper means (not shown). The scraped sleeve surface may be brought into contact with the magnetic particle layer to recoat the developer.
磁性粒子とトナーとの濃度を検出して、この出力に応じ
て自動的にトナーを補給する機構を設けてもよい。A mechanism may be provided for detecting the concentrations of the magnetic particles and the toner and automatically replenishing the toner according to the output.
本発明の現像装置は容器21、スリーブ22およびブレード
24などを一体化した使いすてタイプの現像器としても、
画像形成装置に固定された通常現像器としても使用可能
である。The developing device of the present invention includes a container 21, a sleeve 22 and a blade.
Even as a used type developing device that integrates 24 etc.,
It can also be used as a normal developing device fixed to the image forming apparatus.
又、本発明の磁性キヤリアを用いることで粒径10μ以下
の微粒子トナーの使用も可能である。Further, by using the magnetic carrier of the present invention, it is possible to use a fine particle toner having a particle diameter of 10 μ or less.
本発明は、交番電界印加の現像方法として説明している
が、上記磁性粒子は、現像バイアスとして直流成分のみ
を加える2成分現像方式の磁性粒子と使用した場合、キ
ヤリア付着という問題を解決できるため、新たな発明と
して認定されるべきものである。Although the present invention has been described as a developing method by applying an alternating electric field, the magnetic particles can solve the problem of carrier adhesion when used with the two-component developing type magnetic particles in which only a DC component is added as a developing bias. , Should be certified as a new invention.
本発明は、画像上、磁性粒子の付着がなく、ベタ黒の白
点発生を防止し、良好な画像を得ることができる。According to the present invention, magnetic particles are not adhered on an image, white spots of solid black are prevented from occurring, and a good image can be obtained.
本発明によればスリーブやベルト等の現像剤担持体上で
磁性粒子とトナーとをかくはん・混合して用いる簡易2
成分現像器のトナー濃度維持を安定して達成できる。即
ち、特定の現像条件を悪化させることがないので磁性粒
子の作用を安定させ信頼性の高い現像装置を提供でき
た。According to the present invention, the magnetic particles and the toner are agitated and mixed on a developer carrier such as a sleeve or a belt, and used simply.
It is possible to stably maintain the toner density of the component developing device. That is, since the specific developing conditions are not deteriorated, the action of the magnetic particles can be stabilized and a highly reliable developing device can be provided.
又、上記構成の現像器の現像ローラーの小径スリーブ化
によって、スリーブ上の磁性粒子量が低下する場合も、
本発明の適用によりトナーの磁性粒子層へ取り込みが安
定するので有効である。In addition, when the developing roller of the developing device having the above-mentioned configuration has a smaller diameter sleeve, the amount of magnetic particles on the sleeve may decrease.
The application of the present invention is effective because the toner is stably incorporated into the magnetic particle layer.
第1図は現像方法の磁性キヤリア粒子の抵抗特性を説明
するグラフ、第2図は本発明を実施した好ましい現像構
成の説明図、第3図は第2図の現像部現像説明図であ
る。 23a〜23dは磁極、31は磁性部材、27は磁性粒子。FIG. 1 is a graph for explaining the resistance characteristics of magnetic carrier particles in the developing method, FIG. 2 is an explanatory view of a preferred developing constitution in which the present invention is carried out, and FIG. 3 is an explanatory view of developing in the developing section of FIG. 23a to 23d are magnetic poles, 31 is a magnetic member, and 27 is magnetic particles.
フロントページの続き (72)発明者 星加 令久 東京都大田区下丸子3丁目30番2号 キヤ ノン株式会社内 (72)発明者 田鹿 博司 東京都大田区下丸子3丁目30番2号 キヤ ノン株式会社内 (72)発明者 木下 正英 東京都大田区下丸子3丁目30番2号 キヤ ノン株式会社内 (56)参考文献 特開 昭58−184158(JP,A) 特開 昭59−121077(JP,A) 特開 昭60−123859(JP,A)Front Page Continuation (72) Inventor Hoshika Reikyu 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc. (72) Inventor Hiroshi Taka 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc. (72) Inventor Masahide Kinoshita 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc. (56) Reference JP-A-58-184158 (JP, A) JP-A-59-121077 (JP, A) ) JP-A-60-123859 (JP, A)
Claims (3)
いて、感光体と現像剤担持体との間に交番電界が印加さ
れている状態で磁性粒子の穂を感光体に接触させてトナ
ー像を形成する現像方法において、 上記感光体はOPCであり、上記磁性粒子は0.2×103V/cm
の電界における抵抗値が108以上1011Ωcm以下、または
2×103V/cmの電界における抵抗値が2×107以上3×10
9Ωcm以下であることを特徴とする現像方法。1. A toner comprising a magnetic particle and a toner particle, wherein the magnetic particles are brought into contact with the photoconductor while an alternating electric field is applied between the photoconductor and the developer carrier. In the developing method for forming an image, the photoreceptor is OPC, and the magnetic particles are 0.2 × 10 3 V / cm.
Resistance value in the electric field of 10 8 to 10 11 Ωcm or less, or resistance value in the electric field of 2 × 10 3 V / cm is 2 × 10 7 to 3 × 10
A developing method characterized by being 9 Ωcm or less.
は1.5%以上30%以下であることを特徴とする特許請求
の範囲第1項記載の現像方法。2. The developing method according to claim 1, wherein the volume ratio of the magnetic particles in the developing portion is 1.5% or more and 30% or less.
り、現像部において磁性粒子に対して4以上40重量%以
下の比率であることを特徴とする特許請求の範囲第2項
記載の現像方法。3. The developing method according to claim 2, wherein the toner particles are non-magnetic toner particles and have a ratio of 4 to 40% by weight with respect to the magnetic particles in the developing section. .
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62060454A JPH0762779B2 (en) | 1987-03-16 | 1987-03-16 | Development method |
US07/168,434 US4873551A (en) | 1987-03-16 | 1988-03-15 | Developing apparatus using magnetic carrier under AC field |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62060454A JPH0762779B2 (en) | 1987-03-16 | 1987-03-16 | Development method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS63225262A JPS63225262A (en) | 1988-09-20 |
JPH0762779B2 true JPH0762779B2 (en) | 1995-07-05 |
Family
ID=13142729
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62060454A Expired - Lifetime JPH0762779B2 (en) | 1987-03-16 | 1987-03-16 | Development method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0762779B2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006091425A (en) | 2004-09-24 | 2006-04-06 | Ricoh Printing Systems Ltd | Developing device and electrophotographic apparatus using the same |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58184158A (en) * | 1982-04-21 | 1983-10-27 | Konishiroku Photo Ind Co Ltd | Developing method of electrostatic image |
JPS59121077A (en) * | 1982-12-28 | 1984-07-12 | Toshiba Corp | Electrostatic latent image developing device |
JPS60123859A (en) * | 1983-12-09 | 1985-07-02 | Konishiroku Photo Ind Co Ltd | Developing method |
-
1987
- 1987-03-16 JP JP62060454A patent/JPH0762779B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPS63225262A (en) | 1988-09-20 |
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