JPS58117553A - Developing device - Google Patents

Developing device

Info

Publication number
JPS58117553A
JPS58117553A JP56212660A JP21266081A JPS58117553A JP S58117553 A JPS58117553 A JP S58117553A JP 56212660 A JP56212660 A JP 56212660A JP 21266081 A JP21266081 A JP 21266081A JP S58117553 A JPS58117553 A JP S58117553A
Authority
JP
Japan
Prior art keywords
toner particles
developer
particle size
image
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.)
Pending
Application number
JP56212660A
Other languages
Japanese (ja)
Inventor
Toshio Kaneko
利雄 金子
Koji Sakamoto
康治 坂本
Fuchio Sugano
菅野 布千雄
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP56212660A priority Critical patent/JPS58117553A/en
Publication of JPS58117553A publication Critical patent/JPS58117553A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G9/00Developers
    • G03G9/08Developers with toner particles
    • G03G9/0819Developers with toner particles characterised by the dimensions of the particles

Abstract

PURPOSE:To suppress unevenness of inclination, picture drift, and texture staining and to increase picture density by using a developer which contains <=2wt% toner particles of 5-10mum in volumetric mean particle size and >=15mum in particle size. CONSTITUTION:The developer 4 charged by friction is conveyed on a sleeve 2 in a layer 4a to reach a developing area D. At this time, the developer on the sleeve, i.e. toner particles stick to an electrostatic latent image formed on a photoreceptor 9 to make the latent image visible. As the volumetric mean particle size of the toner particles increases more and more, the amount of friction charging of the toner particles decreases more and more. When the developer has <=10mum volumetric mean particle size, the visible image is sharp and has such picture density that (unevenness of inclination) and (picture drift) are eliminated or less. Further, the visible image has high quality when the developer contains <=2wt% toner particles having 5-10mum volumetric mean particle size and >=15mum particle size based upon the whole of the developer.

Description

【発明の詳細な説明】[Detailed description of the invention]

系現像剤を用いて静電潜像を可視像化する現像装置に関
する。 電子複写機、静電記録装置又はその他の各種記録装置?
こて用いられ.る上記形式の現像装置は従来より周知で
あり、この種現僧装置においては、磁性体を含むトナー
粒子又は磁性体を実質的に含まないトナー粒子力)ら成
る現像剤等の各種形式の現像剤が用いられている。この
場合、いずれの形式の現像剤を用いたときも、トナー粒
子の粒径によって、可視像の画質が変化することは従来
より知られでおり、この点に着目して成る特定の粒径以
下のトナー粒子を含めないか、或いはその含有量を抑え
た現像剤を用い、こねによって、可曲像の地肌部(画像
の形成さねない部分)にトナー粒子が付着する、所謂地
肌汚れを防止しようとする構成が提案されている。この
ように、小径なトナー粒子を含まない、或いはその含有
量の少ない現像剤を用いようとする考えは従来より知ら
れているが、その反面、粒径の大きなトナー粒子につい
ての考慮はあまり払われてぃなかった。ところが、本発
明者の検討したところによると、粒径の大きなトナー粒
子から成る現像剤を用いると、こねにより現像された可
視像のきめがあらくなるだけでなく、次の如を不都合を
生ずることが明らかとなった。即ち; ■ 比較的体積固有抵抗率の高いトナーから成る一成分
系現像剤を用いた場合、これを現像に用いるに先立ち、
該現像剤を強制的に所定の極性に帯電する必要があるが
、大粒径なトナー粒子は、その帯電量がどうしても少な
くなり、こイ1に基いて可ネp像の品質が低下する。 この不都合は回転磁界を生せしめる磁石によってffJ
、像剤を駒込する形式のJ’lj像装置において都(こ
顕著に現わわる。 0 イ・φり性トナー粒子から成る現像剤を用い、この
4t、、 (”ar剤を、磁石による磁気力で搬送して
fl’7((,4+を行う形式の現像装置においては、
粒径の大きなトナー粒子は比較的大きな力で磁石にp7
?・引さね、l¥i電β・像に付着する確率が低下する
ため、大径なトナー粒子を多量に含む現像剤を用いると
、可視像の濃度が低くならざるを得ない。 本を囮は上記h1夕識に基去なされたφ)のであり、従
来の考えとはむしろ逆に、大粒径のトナー粒子の含有量
を所つ量以下に抑オた現像剤を用いることlこよって、
上述した欠点を除去しようとするものである。 エソ下、本発明を適用可能な現像装置を図面に従に則し
てより一層明らかにし、併せて本発明の有利な実施例を
説明する。 第1図は、本発明を適用可能な観像装W1を、電子複写
機に用いた場合の構成例を示す。ここに示した現像装置
lは、現像スリーブ2として構成された現像剤相持体と
、この現像スリーブ2に内設されたローラ状の磁石3と
、トナー粒子から成る一成分系現像剤4を収容する。た
ぬのタンク5とを有している。本例では、工押像剤4を
構成するトナー粒子々して、その少なくとも一部が磁性
体がら成る高抵抗トナー粒子が用いられている。磁石3
の各磁極S、Nは、スリーブ2の周方向に沿って交互に
逆極性となっている。図示した現像装置においては、磁
石3が時計方向に回転駆動さね、現像スリーブ2が反時
計方向に回転駆動されるようになっている。6は現像ス
リーブ2に対して押圧された磁性ならし板、7はスリー
ブ2から所定の間隙をあけて配置されたドクター、そし
て8はスリーブ2上の現像剤を掻き取る掻き取り板であ
る。一方、現像スリーブ2に対向した位置には、ドラム
状の感光体9として構成された潜像相持体が位置し、こ
の感光体9は時計方向に回転駆動ざ狽、る。 複写動作が開始でれると、感光体9″1ま上述の如く時
計方向に回転駆動てれ、その際、図示していない竹像形
成手段によって感光体表面に静電潜像が形成され、この
潜像は現像スリーブ2と感光体9、!0:の間の現像領
域りへと移動するOf+l像装置1においては、その現
像スリーブ2と41゛ム石3とが既述の方向にそれぞれ
回転され、これC′こよってタンク5内の現像剤4の一
部が現像スリーブ2に担持坏れて、反時計方向に搬送さ
れる。 この場合、現像剤がドクター7とスリーブ2との間を通
過するとき、該現像剤はドクター7によって+4き取り
作用を受け、搬送だれる現像剤の量をおお1かに規制さ
れる。次いで現像剤が磁性ならし板6とスリーブ2との
間の微小な隙間を通過するとき、スリーブ2−ヒの現像
剤はならし板6により押圧;れてその厚さを規制てれる
と共に、所定の極性(例えば既述の静電潜像を形成する
電荷の極性と逆極性)に帯電てれる。この場合、本例で
はならし板6が磁性体A・ら成す、シカ・も磁石3が回
転して回転磁界が生ぜしめられて0るので、磁性ならし
板6は磁石3によって吸引てれつつ振動し、スリーブ2
とならし板6との間の微小な間隔が周期的変化し、よっ
て、ここを通過する現像剤はその厚さを極く薄く規制で
れつつ摩擦力を受け、これによって所定の極性に摩擦帯
電σれる。このように現像剤は薄層化されて摩擦帯電こ
れるので、現像剤層の厚σ方向全体に亘って比較的均一
に帯電きれる。 上述の如く帯電でれ大現像剤は、層4aをなしてスリー
ブ2士を搬送され既述の現像領域りへ至り、このとき、
スリーブ上の現像剤、即ちトナー粒子が感光体9に形成
された静電潜像に付着し、該潜像が可視像化でれる。こ
の場什、トナー粒子は既述の如く予め強制的に摩擦帯電
されているので、該トナー粒子は静電潜像に静電的に付
着することができる(尚、予め強′制的に帯電する必要
のあるJi像削は、通常、その体積固有抵抗率がlol
。 Ω−m以七、特に1013乃至】014Ω−m以上であ
る)。 感が皿体9に付着しなかつにトナー粒子は、引き続きス
リーブ2上を搬送プれてタンク5内に戻これ、掻き取り
板8vCよってスリーブ2から掻き取られる。尚、第1
図に示す現像装置においては、スリーブ2と感光体9と
の間のギャップは、例えば100μ程度、層厚規制後の
スリーブ−ヒの現像剤層の厚づは20乃至30μ程度に
することができる。 第1図に示す構成及びその作用は大略以上の通りである
。この場合、第1図に示す装置のように磁石3によって
回転磁界を生せしめて磁性現像剤を搬送するようにする
と、現像スリーブ2土の現像剤のブラシを比較約款くて
き、よって、形成されlc or視像の11.1像均−
性を比較的高めることが可11巨で、5イ)。ところが
現像剤、即ちトナー粒子を予め帯電する際に、各トナー
粒子に与える電荷量が不充分であると、潜像に静電的に
付着したトナー粒子き、該潜像とに作用するクーロン力
が弱いだめ、磁石3の回転動に伴って、潜像に付着しに
トナー粒子が潜像上を移動し、このkめ、可バ」像の濃
度が部分的に高するものの他の部分の濃度は著しく低下
し、所謂「傾斜むら」を生じ可視像の濃度むらを起す恐
れがある。そしてこの現象が著しくなるさ、潜像のエツ
ジ部、即ち地肌部に近接した潜像部分に多量のトナー粒
子が付着し、場合によって・4まトナー粒子がこのエツ
ジ部をはみ出て地肌部[までトナー粒子が流れ串る所謂
「画像流れ」を起すこともめる。 第1図に示す現像装置においては、トナー粒子の帯電量
が不足しに場合、可視像の品質低下を招く恐れのあるこ
とは、上の説明からよく判る。この場合、トナー粒子の
帯電量は、トナー粒子の粒径に大きな影響を受け、トナ
ー粒子の粒径が大きい程、帯電量lま少なくなる。これ
を、第1図に示しに現像装置を用いて行った実験経過を
説明することによって明らかにする。 スチレン・アクリル樹脂48重量部、磁性粉さしてのマ
グネタイト50重量部、帯電極性制御剤2重量部を練り
、次いでこれを粉砕して得たトナー粒−トを現像剤とし
て用い女。そしてトナー粒子の71、積モ均粒径が鴇な
る4種の現像剤を用意しに0トナ一粒子の体積固有抵抗
率は約10′4Ω−(7)でろ−)/ζ。次(lこ第1
図に示す現像装置の磁石3の回転数f 150flrp
m 、現像スリーブ20回転数ヲ1000r p nI
K設定し、厚−gtが0.2mmのSK’(81から成
る/1′並性ならし板6を用いて、既述の各現像剤につ
(1てそれぞれ現像動作を行い、トナ毒粒子の体積平均
粒径と、その摩擦帯電量さの関係を調べ友ところ、第2
図r(示す結果が得られた。尚、帯電量はブローオフ法
によって測定しkO 第2図から明らかなように、トナー粒子の体積平均粒径
が太pくなる程、トナー粒子の摩擦帯電にが低下してい
る。次にこのトナー粒子の粒径と、可視像の画質とを出
校検討しkところ、体積平均粒径が10μ以下の現像剤
を用いると、先に説明し左画像濃度の「傾斜むら」及び
「画像流れ」の無い又は少ないシャープな可視像が得ら
れ、逆に体積平均粒径がこれより大きい現像剤を用いる
と、傾斜よrら及び画像流れの発生が著しくなつToそ
を不するトナー粒子を現像剤全体V・り対して、2重量
%以下さしたときに、高品質な可視像の得られることを
明らかにすることができko・不へ発明は、このような
現像剤の構成をその特徴とするものでるる。 ところで第1図に示す装置において既述の「傾斜むら」
及び「画像流れ」の現象が発生するのは、現像剤が磁石
3に強く引かれることに起因しているので、これら現象
が発生するか否かは、トナー粒子の帯電量の外、トナー
粒子に含1れに磁性体の量によっても左右され、トナー
粒子中の磁性体の含有量が多い程、トナー粒子は磁石3
に強く引かれ、よって傾斜むら及び画像流れが起りやす
くなる。この場合、トナー粒子中の磁性体の含有量は、
各トナー粒子中の磁性体の占める割付の外、各トナー粒
子の全体積、換言すれば七〇粒径によっても左右される
。トナー粒子の径が犬キ<、その体積が太きければ、そ
れに含1れる全磁性体の(11−も増大するからである
。このようにトナー粒子中の磁性体の含イ;−喰によっ
て、可視像の品質に影響が与えられるが、各トナー粒子
中の両性体育有料(重−量%)が、通常の割付の範囲内
にあり、必要以上の特に高い割付でトナー粒子に磁性体
を含有ζゼな(σれば5、上述しπ小粒径のトナー粒子
から成る現像剤、即ち体積平均粒径5μ乃至10μであ
って、151t以上の粒径のトナー粒子を2重量係以下
とした現像剤を用いることに1って、傾斜むら及び画像
流れを効果的に抑えることができる。 寸1ζ、このようにトナー粒子の粒径を比較的小ζくす
れば、一般に各トナー粒子に含寸れる磁性体の絶対晴を
少なくて衾、これによっても、画像流れ等の現象を抑え
ることができると言える。 更に上述しに粒径のトナー粒子から成る工1.1像剤・
シ用いると、次の如き利点も得られる。 ■ 体積平均粒径が5μ乃至10μ、15μ以上の粒径
のトナー粒子が2重t%以丁である現像剤は、従来用い
られている通常の現像剤のトナー粒径よりも小径であり
、このような小径のトナー粒子を用いるさ、可視像のき
めを細かくすることかでな、シかもその7ヤープ性を高
めることができる。のみならず、トナー粒子が小径でる
るので、これが少々地肌部に付着してもめ1つ目立にず
、実質的に地肌汚れを低減することが可能である。 ■ トナー粒子が小だければ、先にも説明したように各
トナー粒子中に含捷れる全磁性体量も比較的少なくなり
、よってトナー粒子が磁石に引かれる力が比較的小ざく
なるkめ、トナー粒子が層像に付着する確率が高1つ、
可視像の濃度が高まる。 ■ 第1図に示す装置のように、高抵抗現像剤を用いる
ときには、これを均一に帯電すべく、現像剤を薄くする
・〆゛要がめるが、粒径の小なるトナー粒子から成る現
像剤は、これを比較的簡単に薄層化でき、よって、現像
剤の均一帯電、ひいては地肌汚れの低減を達成すること
ができる。まに粒径が小セいと、比較的簡単に現像剤を
薄層化できるのでならし板6の負担を低減できる。この
よI″IfXIfX効果図に示す手段以外の手段によっ
て現像剤を薄層化し、帯電する場合にも言えることであ
る。 以上、第1図に示す構成に則して不発明に係る構lJ1
例と、その効果について説明したが、不発明は第1図以
外の各種形態の現像装置に対しても適Illできる。例
えば第3図に示すように、感光体109が2つのローラ
10.11 K巻き掛けられた無端ベルト状vc杉成さ
れている複写機用の現像装置1にも・14噸用で・檜、
その場合、現像スリーブ2に対問する方のローラ10の
少なくとも表面をゴム等の弾性体て構成し、現像スリー
ブ2と感光体10qとのギャップをほぼ零に設定するこ
ともできる。第3図における他の構成は第1図の場合と
実質的に同様で、ラリ、がかる現像装置における現像剤
4として既述の粒径含有するトナー粒子を用いることに
よって、先に説明した効果と同様の効果が得られる。 第4図においては、ベルト状の感光体109が3−)の
ローラ10,11,12 に巻き掛けられ、2つのロー
ラ10,11間の感光体部分に現像スリーブ2が位し、
ドクター7(第1図)が省略でれてお11 、他の構成
は実質的に第1図の場ひと同様である。ヤして、第4図
に示す現像装置IKも不発明を先に説明した実施例と同
様Vこ適用できる。 第5図においては、感光体】09が4つのローラ10乃
至13に巻A掛けられ、現像スリーブ2か感光体109
に対して大きな面積に亘って、[[!像剤を介して接触
している。1にスリーブ2に内股これに1複数の磁石1
03が不動に固定されている。他の構成は第4図と同様
である。このように磁石が固定σれていると、これが回
転する場合に比べて、既述の傾斜むら、画像流れは元々
発生しにくいが、この現像装置に不発明を適用すること
によって、第2図に示しに状態と同様なトナー粒子への
帯電量関係が得られ、きめの細かいシャープ性に富んだ
、しかも地肌汚れの少ない可視像が得られる。 まに1第5図に示す現像装置
The present invention relates to a developing device that visualizes an electrostatic latent image using a developer. Electronic copying machine, electrostatic recording device or other various recording devices?
A trowel is used. Developing devices of the above-mentioned type have been well known in the past, and in this type of developing device, various types of developing devices can be used, such as developers made of toner particles containing magnetic material or toner particles substantially free of magnetic material. agent is used. In this case, it has been known that the image quality of the visible image changes depending on the particle size of the toner particles when any type of developer is used. By using a developer that does not contain the following toner particles or has a reduced content, it is possible to remove so-called background stains in which toner particles adhere to the background part of the flexible image (the part where no image will be formed) by kneading. Configurations have been proposed to try to prevent this. As described above, the idea of using a developer that does not contain small-sized toner particles or contains only a small amount of small-sized toner particles has been known for a long time, but on the other hand, little consideration has been given to large-sized toner particles. It wasn't worth it. However, according to studies conducted by the present inventors, when a developer consisting of toner particles with a large particle size is used, not only the texture of the visible image developed by kneading becomes rough, but also the following disadvantages occur. It became clear that That is, when using a one-component developer consisting of a toner with a relatively high specific volume resistivity, before using it for development,
Although it is necessary to forcibly charge the developer to a predetermined polarity, large-sized toner particles inevitably have a small amount of charge, and the quality of the neppy image deteriorates based on this phenomenon. This disadvantage is caused by the magnet that generates the rotating magnetic field.
, in the J'lj image device of the type in which the developer is embedded, this phenomenon appears conspicuously. In a developing device that performs fl'7((,4+) by conveying it by magnetic force,
Toner particles with a large particle size are attracted to the magnet by a relatively large force (p7).
? - If a developer containing a large amount of large-diameter toner particles is used, the density of the visible image will inevitably be lowered because the probability of the toner adhering to the image decreases. The decoy is φ) based on the above h1 knowledge, and contrary to the conventional idea, it is necessary to use a developer that suppresses the content of large toner particles to a certain amount or less. Because of this,
It is an attempt to eliminate the above-mentioned drawbacks. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A developing device to which the present invention can be applied will be further clarified with reference to the drawings, and advantageous embodiments of the present invention will also be explained. FIG. 1 shows an example of a configuration in which a viewing device W1 to which the present invention is applicable is used in an electronic copying machine. The developing device 1 shown here accommodates a developer carrier configured as a developing sleeve 2, a roller-shaped magnet 3 disposed inside the developing sleeve 2, and a one-component developer 4 made of toner particles. do. It has a raccoon tank 5. In this example, high-resistance toner particles, at least a portion of which are made of a magnetic material, are used as the toner particles constituting the printing press material 4. magnet 3
The magnetic poles S and N have opposite polarity alternately along the circumferential direction of the sleeve 2. In the illustrated developing device, the magnet 3 is rotated clockwise and the developing sleeve 2 is rotated counterclockwise. 6 is a magnetic leveling plate pressed against the developing sleeve 2; 7 is a doctor disposed at a predetermined gap from the sleeve 2; and 8 is a scraping plate for scraping off the developer on the sleeve 2. On the other hand, at a position facing the developing sleeve 2, a latent image carrier configured as a drum-shaped photoreceptor 9 is located, and this photoreceptor 9 is rotated clockwise. When the copying operation starts, the photoreceptor 9''1 is rotated clockwise as described above, and at this time, an electrostatic latent image is formed on the surface of the photoreceptor by bamboo image forming means (not shown). In the Of+l image device 1 in which the latent image moves to the developing area between the developing sleeve 2 and the photoreceptor 9, !0:, the developing sleeve 2 and the 41-degree stone 3 are rotated in the aforementioned directions. As a result, a part of the developer 4 in the tank 5 is carried by the developing sleeve 2 and transported in the counterclockwise direction. When passing, the developer is subjected to a +4 scraping action by the doctor 7, and the amount of the developer carried and dripping is regulated to approximately 1.Then, the developer passes between the magnetic leveling plate 6 and the sleeve 2. When passing through a minute gap, the developer in the sleeve 2-1 is pressed by the leveling plate 6 to regulate its thickness, and also to maintain a predetermined polarity (for example, the electric charge forming the electrostatic latent image mentioned above). In this case, in this example, the leveling plate 6 is made of the magnetic material A, and since the magnet 3 rotates and a rotating magnetic field is generated, the magnetic The leveling plate 6 vibrates while being attracted by the magnet 3, and the sleeve 2
The minute gap between the flattening plate 6 and the leveling plate 6 changes periodically, so that the developer passing through this plate is subjected to frictional force while keeping its thickness extremely thin. Charged. Since the developer is triboelectrically charged in a thin layer in this way, the developer layer can be charged relatively uniformly over the entire thickness σ direction. As mentioned above, the charged and large developer is conveyed through the two sleeves in the layer 4a and reaches the development area mentioned above, and at this time,
The developer, or toner particles, on the sleeve adheres to the electrostatic latent image formed on the photoreceptor 9, and the latent image becomes visible. In this case, since the toner particles are forcibly charged by friction in advance as described above, the toner particles can electrostatically adhere to the electrostatic latent image. Ji image removal that needs to be done usually has a specific volume resistivity of lol
. Ω-m or more, especially 1013 to 014 Ω-m or more). Before the toner particles adhere to the plate 9, the toner particles continue to be transported on the sleeve 2 and returned to the tank 5, where they are scraped off from the sleeve 2 by the scraping plate 8vC. Furthermore, the first
In the developing device shown in the figure, the gap between the sleeve 2 and the photoreceptor 9 can be, for example, about 100 μm, and the thickness of the developer layer on the sleeve after controlling the layer thickness can be about 20 to 30 μm. . The structure shown in FIG. 1 and its operation are roughly as described above. In this case, if the magnetic developer is conveyed by generating a rotating magnetic field using the magnet 3 as in the device shown in FIG. 11.1 image average of lc or visual image
It is possible to relatively increase the sex level (11 and 5). However, when pre-charging the developer, i.e., toner particles, if the amount of charge given to each toner particle is insufficient, toner particles electrostatically adhere to the latent image, causing Coulomb force to act on the latent image. However, as the magnet 3 rotates, the toner particles adhere to the latent image and move over it. The density decreases significantly, and there is a possibility that so-called "tilt unevenness" may occur, causing density unevenness in the visible image. This phenomenon becomes more noticeable when a large amount of toner particles adhere to the edge portion of the latent image, that is, the latent image portion close to the background area, and in some cases, toner particles protrude from this edge area and reach the background area. This can also cause so-called "image bleeding" in which toner particles run off. It is clear from the above description that in the developing device shown in FIG. 1, if the amount of charge on the toner particles is insufficient, the quality of the visible image may deteriorate. In this case, the amount of charge of the toner particles is greatly influenced by the particle size of the toner particles, and the larger the particle size of the toner particles, the smaller the amount of charge l becomes. This will be made clear by explaining the progress of an experiment conducted using the developing device shown in FIG. 48 parts by weight of styrene/acrylic resin, 50 parts by weight of magnetite as a magnetic powder, and 2 parts by weight of a charge polarity control agent were kneaded and then ground to obtain toner particles, which were used as a developer. By preparing four kinds of developers having toner particles of 71 and a total average particle diameter of 0, the volume specific resistivity of one toner particle was approximately 10'4 Ω-(7)/ζ. Next (1st
The rotation speed f of the magnet 3 of the developing device shown in the figure is 150flrp
m, developing sleeve 20 revolutions wo 1000 r p nI
SK'(81/1') with a thickness -gt of 0.2 mm. We investigated the relationship between the volume average particle diameter of particles and their triboelectric charge, and found that the second
The results shown in Figure R were obtained.The amount of charge was measured using the blow-off method, and as is clear from Figure 2, the larger the volume average particle diameter of the toner particles, the more the frictional electrification of the toner particles increases. Next, we examined the particle size of the toner particles and the image quality of the visible image, and found that if a developer with a volume average particle size of 10 μm or less was used, the image on the left as explained earlier A sharp visible image with no or little density unevenness and image blurring can be obtained; conversely, if a developer with a larger volume average particle diameter is used, tilting unevenness and image blurring will occur. It has been revealed that high-quality visible images can be obtained when toner particles that do not deteriorate significantly are added in an amount of 2% by weight or less based on the entire developer. The structure of the developer is characterized by the above-mentioned structure.By the way, in the apparatus shown in FIG.
The phenomenon of "image deletion" occurs because the developer is strongly attracted to the magnet 3, so whether or not these phenomena occur depends on the amount of charge on the toner particles as well as the amount of charge on the toner particles. It also depends on the amount of magnetic material contained in the toner particles, and the higher the content of magnetic material in the toner particles, the more the toner particles become
Therefore, uneven tilting and image deletion are likely to occur. In this case, the content of magnetic material in the toner particles is
In addition to the allocation of the magnetic material in each toner particle, it also depends on the total volume of each toner particle, in other words, the particle diameter. This is because if the diameter of the toner particle is small and the volume is large, the total magnetic material contained in the toner particle (11-) also increases. , the quality of the visible image is affected, but the ampholytic content (weight %) in each toner particle is within the range of normal allocations, and magnetic material is added to toner particles at particularly high allocations than necessary. A developer consisting of toner particles with a small particle size, i.e., a volume average particle size of 5 μ to 10 μ, and a particle size of 151 tons or more, with a weight coefficient of 2 or less. By using a developer having a diameter of 1, it is possible to effectively suppress tilt unevenness and image deletion.If the particle size of the toner particles is made relatively small in this way, generally each toner particle is It can be said that phenomena such as image blurring can be suppressed by reducing the absolute fineness of the magnetic material contained in the toner.
The following advantages can also be obtained by using (2) A developer having a volume average particle size of 5 μ to 10 μ and 2% or more of toner particles with a particle size of 15 μ or more is smaller in diameter than the toner particle size of conventionally used normal developers; By using such small-diameter toner particles, it is possible to improve the printability by making the visible image finer. In addition, since the toner particles have a small diameter, even if they adhere to the skin a little, they do not make any noticeable stains, and it is possible to substantially reduce skin stains. ■ As explained earlier, if the toner particles are small, the total amount of magnetic material contained in each toner particle will be relatively small, and therefore the force that attracts the toner particles to the magnet will be relatively small. Therefore, the probability that toner particles will adhere to the layer image is high.
The density of the visible image increases. ■ When using a high-resistance developer, as in the device shown in Figure 1, the developer must be made thin in order to charge it uniformly. This can be relatively easily made into a thin layer, thereby achieving uniform charging of the developer and, by extension, reduction of background stains. If the particle size is small, the developer can be made into a thin layer relatively easily, and the burden on the leveling plate 6 can be reduced. This also applies to the case where the developer is made into a thin layer and charged by means other than the means shown in the I''IfXIfX effect diagram.The above is the structure according to the invention according to the structure shown in FIG.
Although examples and their effects have been described, the invention can also be applied to various types of developing devices other than those shown in FIG. For example, as shown in FIG. 3, there is also a developing device 1 for a copying machine in which the photoreceptor 109 is formed of an endless belt-like VC cedar wrapped around two rollers 10 and 11.
In that case, at least the surface of the roller 10 facing the developing sleeve 2 may be made of an elastic material such as rubber, and the gap between the developing sleeve 2 and the photoreceptor 10q may be set to approximately zero. The other configuration in FIG. 3 is substantially the same as that in FIG. 1, and by using toner particles having the above-mentioned particle size as the developer 4 in the developing device, the effect described above can be achieved. A similar effect can be obtained. In FIG. 4, a belt-shaped photoreceptor 109 is wound around the rollers 10, 11, 12 of 3-), and the developing sleeve 2 is placed in the photoreceptor portion between the two rollers 10, 11.
The doctor 7 (FIG. 1) is omitted, but the other constructions are substantially the same as in FIG. 1. Therefore, the present invention can also be applied to the developing device IK shown in FIG. 4 in the same way as the embodiment described above. In FIG. 5, the photoreceptor 109 is wrapped around the four rollers 10 to 13, and the developing sleeve 2 or the photoreceptor 109
[[! Contact is made through the image agent. 1, sleeve 2, inner thigh, 1, multiple magnets 1
03 is fixed immovably. The other configurations are the same as in FIG. 4. When the magnet is fixed and tilted in this way, the above-mentioned tilt unevenness and image deletion are less likely to occur than when it rotates, but by applying the invention to this developing device, A similar charge amount relationship to the toner particles as shown in Fig. 1 is obtained, and a visible image with fine grain and rich sharpness and less background staining is obtained. Mani 1 Developing device shown in Figure 5

【Cおいては、磁石]03
が固定されているので、各磁石1031/(:対向して
位置する現像剤の穂立ちが大きくなり、よって現像剤に
充分な帯電量を与えるには、なrケし板6と磁石】0:
3との間のE11気力を強める必要があり、この上うV
こすると一般にならし板に作用する力が大きくなり、々
らし板等に傷が付きやすくなるが、不発明Vこ係る小径
トナー粒子の現像剤を用いれば、既述の如く、ならし板
の負担を軽減でき、ならし叛及び現像スリーブに傷を付
ける可能性を低減できる。 更に第4図及び第5図、並びに第6図に示すように、現
像スリーブ2を、4上体支持体】4と、そのと而に設け
た誘電体層J5と、これに支持でれπρ数の微小電極J
6とから構成し、これら微小電極16を導電性支持体1
4に対して電気的に絶縁するさjl、に、微小電極同志
をも実質的に絶縁状態にすると、(p電潜像のライン画
像(課状の潜像)を−濃度Vこ可1児像化でき、原稿に
おける比較的濃度の低い細線画像からも高濃度な可視像
を得られるが、このようh現像スリーブを有する現像装
置に対しても不発明を支障々く適用できる。 μ上、現像剤として母性現像剤を用い、しかも現像スリ
ーブの表面を剛体から構成した装置に不発明を適用し、
1?:具体例を説明したが、第7図C・こ)rミすよう
に、少なくさもその表面がゴム等の弾性体から[配る現
像スリーブ2に、非磁性トナー粒子から成る現像剤4を
埠持し、摩擦帯電部材IOi[よってこの現像剤を薄層
化しつつ帯電し、こゎを感光体9に擦り付けることによ
って現像を行う現像装置にも本発明を適用できる。この
場合、既述の効果のうち、磁性現像を用いることによっ
てのみ得られる効果は、第7図に示す装置では得られな
いが、他の効果はそのまま得ることができる。ま1ζ、
第7図に示すスリーブ2の表面には、通常微小な凹凸が
形成されているが、その際、この凹凸が太きいと、現像
剤を薄層化することが困難さなり、逆に凹凸が小はすぎ
ると、粒径の大きなトナー粒子が摩擦帯電部材106と
スリーブ2との間を通過できなくなる0さころが不発明
では、トナー粒子の粒径が小ζいので、現像剤の層厚を
薄くすべく、凹凸を小さくしても、トナー粒子が摩擦帯
電部材とスリーブとの間を通過し得ないという不都付を
低減することができる。 才女、第4図、第5図、第7図に示す装置のよ’+ (
/こ、スリーブ2上の現像剤を感光体に接触ζせ一6現
像をjj f) 噂触現像1でおいては、スリーブ上の
現像剤が、八・2九体の地肌部に付着したトナー粒子を
取り去る所謂スキャベンジング効果が充分に得られるの
で、曵肌汚れを特に効果的に抑えることかてさ、よって
、小径なトナー粒子を用いるこさくノコ起因する地肌汚
れ発生を41効に抑制することができる。 次に、不発明と直接関係し々いのであるが、先に簡単に
説明しに1各トナ一粒子中の磁性体の含41+と、可視
像の画質との関係を参考1でに説明しても・く。先ず第
1図に関連して先に説明し爬笑験例1Cて用いたトナー
粒子の樹脂(!:磁性粉との配合比を各種変えて得に平
均粒径12μのトナー粒子から成る現像剤を用意し、第
1図に示す現像装置しくて、これら現像剤を用いて現像
動作を行りに0その結果、磁性体含有率の少ないトナー
粒子を用(するみ、両像流れ、傾斜むらの発生を少なく
留めることができるが、逆に磁性体量の多いトナー粒子
では、これら現象が顕著に現われることが判っに0これ
は、各トナー粒子中の磁性体の含有率が低ければ逆に樹
脂の割合が高まる結果、トナー粒子の摩擦帯電量が増大
すること、及びトナー粒子が磁石3に引かれる力が低下
することに起因している(第8f図は、各トナー粒子中
の磁性粉の含有割合(重量%)と、その摩擦帯電量との
関係を示すグラフである)。このことがら、磁石を回転
きせる形式の現像装置では、スリーブ2上の現像剤を搬
送するのに必要な最小の磁気力をトナー粒子に及ぼすよ
うにし、且つトナー粒子の帯電電荷を大キくするように
すれば、高品質な可視像を得られることが判る。そして
、このようにするには、トナー粒子の磁性体量を考慮す
る外、磁石の磁気力を考慮する必要もあり、同じ現像剤
を用いて、700ガウス吉、12ooガウスの磁石で現
像動作を行ってみたところ、700ガウスの方が傾斜む
ら等の現象は少なかつ7i’oFナ一粒子中の磁性体含
有率の多少という問題は不発明に直接関係する事項では
ないが、上に説明した高品質な可視像を得る穴lこの条
件は、不発明によっても達放し得”ることでちる。 1す、士、本発明を各種形態の現像装置に適用しに′μ
弛例を説明したが、不発明は更に池の形式の現像装置l
/こも適用でき、例、えば、Fす傷創を電荷注入1η1
3J4による電荷注入によって帯*c/* リ、或いは
現像スリーブとトナー粒子との摩擦りこよりてこれを摩
擦帯電し1でり、又はコロナ放電器によって現像剤を帯
電する形式の現像装置や、永久磁石の代す9こ電磁石を
用いる現像装置、或いはま−IC史像スリーブが不動に
同定された現像装置にも適用できる。更に、現像剤担持
体がスリーブではなくベルト状に形成された装置や、静
電記録装置における現像装−1或いは、層像担持体を最
終コピーとする直写式vt録装置の現像装置VCも適用
可能である。 −f* 3M 傷創として低抵抗トナー粒子から成るも
のを用(1女ときにも、不発明を適用することによって
、きめの細かな可硬像を形成できるとする不発明の効果
を得ることができる。 以上の説明からも判るよう・に不発明によれば簡単な構
成によって、その所期の目的を達成できる0
[For C, magnet] 03
is fixed, so each magnet 1031/(: The spikes of the developer located opposite to each other become large, and therefore, in order to give a sufficient amount of charge to the developer, the rake plate 6 and the magnet]0 :
It is necessary to strengthen E11's energy between 3 and V.
Rubbing generally increases the force acting on the leveling plate, making it more likely to be damaged, but if a developer with small-diameter toner particles is used, as described above, the leveling plate can be easily damaged. It is possible to reduce the burden and reduce the possibility of damaging the break-in and developing sleeve. Further, as shown in FIGS. 4, 5, and 6, the developing sleeve 2 is supported by the upper body supporter 4 and the dielectric layer J5 provided therebetween. number of microelectrodes J
6, and these microelectrodes 16 are connected to the conductive support 1.
In addition to electrically insulating the microelectrodes from each other, if the microelectrodes are also substantially insulated from each other, the line image of the p-electrode latent image (the latent image) becomes -density V. Although it is possible to obtain a high-density visible image even from a relatively low-density thin line image on an original, the invention can be applied to a developing device having such an h-developing sleeve without difficulty. , by applying the invention to a device that uses a mother developer as the developer and in which the surface of the developing sleeve is made of a rigid body,
1? Although a specific example has been explained, as shown in FIG. The present invention can also be applied to a developing device which carries out development by holding a triboelectric charging member IOi (Thus, this developer is charged while being made into a thin layer, and is rubbed against the photoreceptor 9. In this case, among the effects described above, the effects that can only be obtained by using magnetic development cannot be obtained with the apparatus shown in FIG. 7, but the other effects can be obtained as they are. Ma1ζ,
The surface of the sleeve 2 shown in FIG. 7 is normally formed with minute irregularities, but if these irregularities are thick, it becomes difficult to thin the developer, and conversely, the irregularities If the size is too small, toner particles with a large particle size will not be able to pass between the triboelectric charging member 106 and the sleeve 2.If the size is too small, the toner particle size will be small, so the layer thickness of the developer will be reduced. Even if the unevenness is made smaller in order to reduce the thickness of the sleeve, it is possible to reduce the inconvenience that toner particles cannot pass between the frictional charging member and the sleeve. Thank you, for the equipment shown in Figures 4, 5, and 7.
/Here, the developer on the sleeve 2 was brought into contact with the photoreceptor. Since the so-called scavenging effect of removing toner particles can be sufficiently obtained, it is possible to particularly effectively suppress skin stains.Therefore, it has a 41-effective effect on the occurrence of skin stains caused by scraping using small-diameter toner particles. Can be suppressed. Next, although it is directly related to non-invention, I will briefly explain the relationship between the content of magnetic material in each toner particle and the image quality of the visible image in Reference 1. Even if it is. First of all, a developer consisting of toner particles having an average particle size of 12μ was prepared by changing the blending ratio of the toner particles with the resin (!: magnetic powder), which was explained earlier in connection with FIG. 1 and used in Example 1C. The developing device shown in Fig. 1 is used to perform a developing operation using these developers. On the other hand, it has been found that in toner particles with a large amount of magnetic material, these phenomena appear conspicuously. As a result of increasing the ratio of resin, the amount of frictional electrification of the toner particles increases and the force with which the toner particles are attracted to the magnet 3 decreases (Figure 8f shows the magnetic powder in each toner particle). (This is a graph showing the relationship between the content ratio (weight %) and the amount of frictional electrification).For this reason, in a developing device that uses a rotating magnet, the amount of water required to transport the developer on the sleeve 2 is It can be seen that a high quality visible image can be obtained by applying a minimum magnetic force to the toner particles and by increasing the electrostatic charge on the toner particles. In addition to considering the amount of magnetic material in the toner particles, it is also necessary to consider the magnetic force of the magnet. Using the same developer, we performed development with a magnet of 700 gauss and 120 gauss, and the result was 700 gauss. However, phenomena such as tilt unevenness are small, and the problem of the amount of magnetic material content in a single particle of 7i'oF is not directly related to non-invention, but This condition can be achieved even by non-invention. 1. To apply the present invention to various types of developing devices
Although the simple example has been explained, the non-inventive one is also a pond-type developing device l.
/ can also be applied, for example, when F
3J4 charges are injected into the band*c/*, or friction between the developing sleeve and toner particles is used to frictionally charge the developer, or a corona discharger is used to charge the developer. The present invention can also be applied to a developing device using nine electromagnets instead of a magnet, or a developing device in which a magnetic IC historical image sleeve is immovably identified. Furthermore, there are also devices in which the developer carrier is formed in the form of a belt rather than a sleeve, the developing device 1 in an electrostatic recording device, or the developing device VC in a direct copy type VT recording device in which the layered image carrier is used as the final copy. Applicable. -f* 3M Using something made of low-resistance toner particles as a wound (also by applying the invention, we can obtain the effect of the invention that a fine-grained hardenable image can be formed) As can be seen from the above explanation, according to non-invention, the intended purpose can be achieved with a simple configuration.

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

第1図は不発明を適用可能な現像装置を示す断面図、第
2図はトナー粒子の体積平均粒径さ摩擦帯電置きの関係
を示すグラフ、第3図乃至第5図は第1図とは異なる現
像装置を、示・す断面図、第6図は第4図、第5図に示
した現像スリーブの拡大模式断面図、第7図は更に他の
現像装置を示す断−面図、第8図はトナー粒子中の磁性
体の含有率と摩擦帯電量との関係を示すグラフである。 1・・・現像装置 4・・・現像剤 1111の浄鼻(内容に変更なし) 第1図 第2[ヌ1 第4図 第5図 第8図 L+−1k +ΦfIJ轟ff1ξシ1−11イ→F手
  続  補  正  書  (方式)%式% 2発明の名称 現像装置 :(補正をする者 を件との関係  特許出願人 住所 東京都太田区中馬込1丁目3番6号名称 (67
4)株式会社リコー 、1代  理  人   〒105 住所 東京都港区西新橋1丁目9番9号中銀第5ヒル3
階Ta (501)4887番昭和57年4月9日 発送日  昭和57年4月27シ 6補正の対象 図面 7補正の内容
Fig. 1 is a cross-sectional view showing a developing device to which the invention can be applied, Fig. 2 is a graph showing the relationship between the volume average particle diameter of toner particles and the frictional electrification setting, and Figs. 3 to 5 are the same as Fig. 1. is a sectional view showing a different developing device, FIG. 6 is an enlarged schematic sectional view of the developing sleeve shown in FIGS. 4 and 5, and FIG. 7 is a sectional view showing another developing device. FIG. 8 is a graph showing the relationship between the content of magnetic material in toner particles and the amount of triboelectric charge. 1... Developing device 4... Purifying the developer 1111 (no change in content) Fig. 1 Fig. 2 [nu 1 Fig. 4 Fig. 5 Fig. 8 →F Procedure Amendment (Method) % Formula % 2 Name of the invention Developing device: (Relationship to the person making the amendment Patent applicant address 1-3-6 Nakamagome, Ota-ku, Tokyo Name (67)
4) Ricoh Co., Ltd., Managing Director 1st Address: 3, Chugin 5th Hill, 1-9-9 Nishi-Shinbashi, Minato-ku, Tokyo 105
Floor Ta (501) No. 4887 April 9, 1980 Shipment date April 27, 1982 Subject to amendment 6 Contents of amendment 7

Claims (1)

【特許請求の範囲】 トナー粒子を含む一成分系現像剤を用いて静電潜像を町
+pr像化する現像装置において、15μ以」二の粒径
を有するトナー粒子を、現像剤全体に対して、2重量%
以下とし、且つトナー粒。 子の体積平均粒径を5μ乃至10μとしたことを特徴と
する前記現像装置。
[Scope of Claims] In a developing device that converts an electrostatic latent image into a PR image using a one-component developer containing toner particles, toner particles having a particle size of 15 μm or more are added to the entire developer. 2% by weight
The following and toner particles. The above-described developing device is characterized in that the particles have a volume average particle diameter of 5 μ to 10 μ.
JP56212660A 1981-12-31 1981-12-31 Developing device Pending JPS58117553A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56212660A JPS58117553A (en) 1981-12-31 1981-12-31 Developing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56212660A JPS58117553A (en) 1981-12-31 1981-12-31 Developing device

Publications (1)

Publication Number Publication Date
JPS58117553A true JPS58117553A (en) 1983-07-13

Family

ID=16626289

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56212660A Pending JPS58117553A (en) 1981-12-31 1981-12-31 Developing device

Country Status (1)

Country Link
JP (1) JPS58117553A (en)

Cited By (17)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60131553A (en) * 1983-12-20 1985-07-13 Konishiroku Photo Ind Co Ltd Developing method
JPS6227360U (en) * 1985-08-05 1987-02-19
JPS62172374A (en) * 1986-01-24 1987-07-29 Konishiroku Photo Ind Co Ltd Method for forming multiple color image
JPS62279375A (en) * 1986-05-29 1987-12-04 Fuji Xerox Co Ltd Electrophotographic developing device
JPS62279373A (en) * 1986-05-29 1987-12-04 Fuji Xerox Co Ltd Electrophotographic developing device
JPS632084A (en) * 1986-06-12 1988-01-07 Konica Corp Developing device
JPS6381427A (en) * 1986-09-26 1988-04-12 Mita Ind Co Ltd Preparation of original for heat sensitive screen printing
JPS63237082A (en) * 1987-03-26 1988-10-03 Fuji Xerox Co Ltd One-component developing device
JPS642258U (en) * 1987-06-24 1989-01-09
JPH01112253A (en) * 1987-10-26 1989-04-28 Canon Inc Magnetic toner
JPH01219760A (en) * 1988-02-29 1989-09-01 Canon Inc Developer for electrostatic charge image
JPH01219757A (en) * 1988-02-29 1989-09-01 Canon Inc Electrostatic charge image developing magnetic toner
JPH02160250A (en) * 1988-12-14 1990-06-20 Canon Inc Heat fixing method and toner for same
JPH02173661A (en) * 1988-12-27 1990-07-05 Canon Inc Image forming method with electrophotographic device utilizing improved nonsingle crystal silicon type photoreceptive member
JPH02173657A (en) * 1988-12-27 1990-07-05 Canon Inc Image forming method with electrophotographic device utilizing improved nonsingle crystal silicon type photoreceptive member
JPH02287365A (en) * 1989-04-28 1990-11-27 Canon Inc Image forming method
JPH02287366A (en) * 1989-04-28 1990-11-27 Canon Inc Image forming method

Cited By (19)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0414793B2 (en) * 1983-12-20 1992-03-13 Konishiroku Photo Ind
JPS60131553A (en) * 1983-12-20 1985-07-13 Konishiroku Photo Ind Co Ltd Developing method
JPS6227360U (en) * 1985-08-05 1987-02-19
JPH0540525Y2 (en) * 1985-08-05 1993-10-14
JPS62172374A (en) * 1986-01-24 1987-07-29 Konishiroku Photo Ind Co Ltd Method for forming multiple color image
JPS62279375A (en) * 1986-05-29 1987-12-04 Fuji Xerox Co Ltd Electrophotographic developing device
JPS62279373A (en) * 1986-05-29 1987-12-04 Fuji Xerox Co Ltd Electrophotographic developing device
JPS632084A (en) * 1986-06-12 1988-01-07 Konica Corp Developing device
JPS6381427A (en) * 1986-09-26 1988-04-12 Mita Ind Co Ltd Preparation of original for heat sensitive screen printing
JPS63237082A (en) * 1987-03-26 1988-10-03 Fuji Xerox Co Ltd One-component developing device
JPS642258U (en) * 1987-06-24 1989-01-09
JPH01112253A (en) * 1987-10-26 1989-04-28 Canon Inc Magnetic toner
JPH01219757A (en) * 1988-02-29 1989-09-01 Canon Inc Electrostatic charge image developing magnetic toner
JPH01219760A (en) * 1988-02-29 1989-09-01 Canon Inc Developer for electrostatic charge image
JPH02160250A (en) * 1988-12-14 1990-06-20 Canon Inc Heat fixing method and toner for same
JPH02173661A (en) * 1988-12-27 1990-07-05 Canon Inc Image forming method with electrophotographic device utilizing improved nonsingle crystal silicon type photoreceptive member
JPH02173657A (en) * 1988-12-27 1990-07-05 Canon Inc Image forming method with electrophotographic device utilizing improved nonsingle crystal silicon type photoreceptive member
JPH02287365A (en) * 1989-04-28 1990-11-27 Canon Inc Image forming method
JPH02287366A (en) * 1989-04-28 1990-11-27 Canon Inc Image forming method

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