JPH02147963A - Method for measuring electric field intensity distribution of development area in magnetic brush developing method - Google Patents

Method for measuring electric field intensity distribution of development area in magnetic brush developing method

Info

Publication number
JPH02147963A
JPH02147963A JP30086188A JP30086188A JPH02147963A JP H02147963 A JPH02147963 A JP H02147963A JP 30086188 A JP30086188 A JP 30086188A JP 30086188 A JP30086188 A JP 30086188A JP H02147963 A JPH02147963 A JP H02147963A
Authority
JP
Japan
Prior art keywords
electrode
electric field
sleeve
developer
capacitance
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
JP30086188A
Other languages
Japanese (ja)
Inventor
Masashi Kagami
鏡 昌司
Tsutomu Uezono
勉 上薗
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.)
Kyocera Mita Industrial Co Ltd
Original Assignee
Mita Industrial 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 Mita Industrial Co Ltd filed Critical Mita Industrial Co Ltd
Priority to JP30086188A priority Critical patent/JPH02147963A/en
Publication of JPH02147963A publication Critical patent/JPH02147963A/en
Pending legal-status Critical Current

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  • Magnetic Brush Developing In Electrophotography (AREA)

Abstract

PURPOSE:To obtain good images by a method wherein capacitance of each measurement electrode is calculated from respective waveforms of applied voltage from ac power source and current flowing to electrode to be measured, and electric field intensity in development width is obtained from this capacitance distribution. CONSTITUTION:AC voltage is applied between an electrode 3 to be measured and a sleeve 1, and while developer is carried with the sleeve 1 rotated, a waveform of applied voltage from ac power source and a waveform of current flowing into the electrode 3 to be measured are obtained for each position of the electrode 3 to be measured by an oscilloscope 5. Then, capacitance C of the developer is calculated by equation I. Dielectric constant epsilons is calculated from this capacitance C with an equation II, and electric field intensity E is further calculated with an equation III. This enables measurement of electric field intensity distribution in a developing area and good images to be obtained.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、電子写真法において採用される磁気ブラシ現
像法において、現像域における電界強度分布の測定方法
に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a method for measuring electric field intensity distribution in a developing area in a magnetic brush developing method employed in electrophotography.

(従来技術) 複写器等の静電写真装置においては、感光体ドラム上に
形成された原稿画像の静電潜像を現像するための手段と
して、磁気ブラシ現像法が一般的に採用されている。
(Prior Art) In electrostatic photographic devices such as copiers, a magnetic brush development method is generally employed as a means for developing an electrostatic latent image of an original image formed on a photoreceptor drum. .

この磁気ブラシ現像法は、−成分系或いは二成分系の磁
性現像剤を使用して現像剤搬送用スリーブ上に現像剤の
磁気ブラシを形成させ、この磁気ブラシを感光体ドラム
と摺擦せしめて静電引力によって前記静電潜像にトナー
を付着させることによって行なわれるものである。
This magnetic brush development method uses a one-component or two-component magnetic developer to form a developer magnetic brush on a developer conveying sleeve, and causes this magnetic brush to rub against a photoreceptor drum. This is done by attaching toner to the electrostatic latent image using electrostatic attraction.

従って、磁気ブラシが感光体ドラムと接触する域、即ち
現像域における電界強度分布を測定することは、得られ
る画像を解析する上で極めて重要な意義を有するが、こ
の様な電界強度分布の測定法は未だ知られていない。
Therefore, measuring the electric field strength distribution in the area where the magnetic brush contacts the photoreceptor drum, that is, the developing area, has extremely important significance in analyzing the obtained image. The law is still unknown.

従って本発明は、現像域における電界強度分布の測定法
を提供することを目的とする。
It is therefore an object of the present invention to provide a method for measuring the electric field strength distribution in the development zone.

(問題点を解決するための手段) 本発明によれば、現像剤搬送用スリーブ近傍に、幅広の
アース電極に囲まれた線状の測定電極を周面に備えた回
転可能なドラムを配置し、該スリーブと測定電極との間
に交流電圧を印加し、該スリーブ上に現像剤を供給して
磁気ブラシを形成させ、該磁気ブラシが前記ドラム表面
に摺擦する様に現像剤の搬送を行なうとともに、交流電
源からの印加電圧及び測定電極に流れる電流の各波形か
ら測定電極の位置毎の静電容量を算出し、この静電容量
の分布から現像幅内での電解強度を求めることを特徴と
する方法が提供される。
(Means for Solving the Problems) According to the present invention, a rotatable drum having a linear measuring electrode surrounded by a wide ground electrode on its circumferential surface is disposed near the developer conveying sleeve. , applying an alternating current voltage between the sleeve and the measurement electrode, supplying developer onto the sleeve to form a magnetic brush, and transporting the developer so that the magnetic brush rubs against the drum surface. At the same time, the capacitance at each position of the measurement electrode is calculated from the applied voltage from the AC power supply and the waveform of the current flowing through the measurement electrode, and the electrolytic strength within the development width is determined from the distribution of this capacitance. A method of characterizing is provided.

(作 用) 本発明の測定方法を好適に実施するために用いる測定装
置の装置の電気回路図を示す第1図から明らかな通り、
本発明は、現像に際して感光体ドラム表面と現像剤搬送
用スリーブとの間に介在する現像剤Fl(磁気ブラシ層
)が、抵抗RとコンデンサCとの並列回路と電気的に等
価であることを前提条件とし、その静電容量変化から電
界強度分布を算出するものである。
(Function) As is clear from FIG. 1 showing the electric circuit diagram of the measuring device used to suitably carry out the measuring method of the present invention,
The present invention recognizes that the developer Fl (magnetic brush layer) interposed between the photoreceptor drum surface and the developer conveying sleeve during development is electrically equivalent to a parallel circuit of a resistor R and a capacitor C. As a precondition, the electric field strength distribution is calculated from the change in capacitance.

この静電器官量の変化は、交流電源からの印加電圧及び
測定電極に流れる電流の各波形から算出される。
This change in the electrostatic organ quantity is calculated from each waveform of the applied voltage from the AC power source and the current flowing through the measurement electrode.

(発明の好適態様) 1友1 本発明の測定方法を好適に実施するための装置の全体の
構造を簡単に示す第2図において、この装置は大まかに
言って、現像剤撤送用スリーブ1の近傍に配置される絶
縁性筒体2から成る。
(Preferred Embodiment of the Invention) In FIG. 2, which briefly shows the overall structure of an apparatus for suitably carrying out the measuring method of the present invention, this apparatus generally consists of a developer withdrawal sleeve 1. It consists of an insulating cylindrical body 2 placed near the.

絶縁性筒体2は、感光体ドラムに対応するものであり、
その周面軸方向に延びている測定電極3を備えている。
The insulating cylindrical body 2 corresponds to the photosensitive drum,
It is provided with a measuring electrode 3 extending in the axial direction of its circumferential surface.

また、この筒体2の斜視図を示す第3図から明らかな通
り、測定電8i3は、幅広のアース電極4.4の間にサ
ンドイッチされる様にして設けられている。
Further, as is clear from FIG. 3, which is a perspective view of this cylinder 2, the measuring electrode 8i3 is provided so as to be sandwiched between the wide ground electrodes 4.4.

即ち、測定電極3には、該電極3に最近接位置にあるス
リーブ1の面上からのみ電流が流ね込む様になっており
、周辺部分からの電流は全てアース電極4.4に流れ込
む。これによって電界強度の分布を正確に測定し得る。
That is, current flows into the measurement electrode 3 only from the surface of the sleeve 1 that is closest to the electrode 3, and all current from the surrounding area flows into the ground electrode 4.4. This makes it possible to accurately measure the distribution of electric field strength.

この測定電極3とアース電極4との間隔は0.1乃至1
ma+の範囲に設定される。
The distance between the measurement electrode 3 and the earth electrode 4 is 0.1 to 1
It is set in the range of ma+.

測定電極3の輻d(1,1乃至0.5 tmmの範囲に
あることが望ましく、アース電極4の幅は、それぞれ5
mm以上であることが好適である。
The width d of the measuring electrode 3 is preferably in the range of 1.1 to 0.5 tmm, and the width of the ground electrode 4 is 5 tmm.
It is preferable that the thickness is not less than mm.

絶縁性筒体2とスリーブ1との間1sIは、通常の複写
器と同様、約1乃至2mm程度に設定されている。
The distance 1sI between the insulating cylindrical body 2 and the sleeve 1 is set to about 1 to 2 mm, as in a normal copying machine.

本発明において、測定電極3は、前記スリーブ1の近傍
位置(現像域)に位置固定されているとともに、オシロ
スコープ5を介して交流電源7に結線され、該電極3と
スリーブ1との間に交流電圧が加えられる様になってい
る。
In the present invention, the measuring electrode 3 is fixed in position near the sleeve 1 (development area), and is connected to an AC power source 7 via an oscilloscope 5, so that an AC power source 7 is connected between the electrode 3 and the sleeve 1. Voltage can be applied.

現像剤搬送用スリーブ1は、通常の電子写真装置におい
て使用されるものと全く同様の構造を有する9例えば、
内部にマグネット(図示せず)を内蔵しており、スリー
ブ回転によって、該スリーブ1上に供給される現像剤を
筒体2との間隙部10(即ち現像域)に搬送するもので
ある。
The developer conveying sleeve 1 has a structure 9 that is exactly the same as that used in ordinary electrophotographic devices, for example,
A magnet (not shown) is built inside, and as the sleeve rotates, the developer supplied onto the sleeve 1 is conveyed to the gap 10 between the sleeve 2 and the cylindrical body 2 (ie, the developing area).

静電容量分布の算出 本発明によれば、上記の測定装置を使用し、測定電極3
とスリーブ1との間に交流電圧を印加し、スリーブ1を
回転させて現像剤の搬送を行ないながら、オシロスコー
プ5により、測定電極3の位置毎に、交流電源からの印
加電圧の波形と、測定電極3に流れ込む電流の波形とが
得られる。
Calculation of capacitance distribution According to the present invention, the above measurement device is used, and the measurement electrode 3 is
While rotating the sleeve 1 and transporting the developer, the oscilloscope 5 measures the waveform of the voltage applied from the AC power supply and the measurement at each position of the measurement electrode 3. The waveform of the current flowing into the electrode 3 is obtained.

この波形の一例を第4図に示す。An example of this waveform is shown in FIG.

第4図から明らかな通り、印加電圧をX及び測定電流を
yとすると、次式が与えられる。
As is clear from FIG. 4, when the applied voltage is X and the measured current is y, the following equation is given.

X x V QCosωt  ■1+1+e1++18
■y=I6cos(ct+t+ψ) + E/R−−−
−−−−■式中、Eは現像剤の摩擦等で発生すると考え
られる直流起電力であり、 ωは、角周波数であり、 Rは、現像剤の抵抗値である。
X x V QCosωt ■1+1+e1++18
■y=I6cos(ct+t+ψ) + E/R---
----■ In the formula, E is a DC electromotive force that is thought to be generated due to friction of the developer, ω is the angular frequency, and R is the resistance value of the developer.

ここで、現像剤の静電容量C(第1図のコンデンサーに
相当)は、次式で表わされる。
Here, the electrostatic capacitance C of the developer (corresponding to the capacitor in FIG. 1) is expressed by the following equation.

式中、V、は印加電圧、 ω は角周波数、 11は電圧V=Oのときの電流値(直 流分を除く)、 第4図の部分拡大図を示す第5図参 照。In the formula, V is the applied voltage, ω is the angular frequency, 11 is the current value (direct) when voltage V=O (excluding flow), See Figure 5, which shows a partially enlarged view of Figure 4. Light.

即ち、第4図に示される波形から、0式を用いて静電容
量Cが算出される。
That is, from the waveform shown in FIG. 4, the capacitance C is calculated using equation 0.

1L里度立血旦1遇 本発明においては、上記の如くして算出された静電容量
Cから比話電率ε3を求め、これから電界強度Eを算出
する。
In the present invention, the specific electrostatic rate ε3 is determined from the capacitance C calculated as described above, and the electric field strength E is calculated from this.

即ち、 C;ε。ε3−  ・・・・・・・・・・・・・・・・
■式中、ε0は真空誘電率(8,85x 10−”F/
m)、S は測定電極の面積(@2)、 d は測定電極とスリーブとの実効距 離(第2図参照)を示す、 で表わされるから、これから65が計算され、更に下記
式、 より電界強度が算出される。
That is, C;ε. ε3− ・・・・・・・・・・・・・・・
■In the formula, ε0 is the vacuum permittivity (8,85x 10-”F/
m), S is the area of the measuring electrode (@2), and d is the effective distance between the measuring electrode and the sleeve (see Figure 2). From this, 65 is calculated, and further, from the following formula, the electric field is The intensity is calculated.

尚、実効距lidは、第2図から明らかな通り、ドラム
−スリーブ間圧@D、ドラム半径R1及びスリーブ半径
rとすると、下記式、 (R+D+r−Rcosθ)2” (R51nθ)2=
(d+r)”  ・・・・・・・・・・・・・・■が成
立するので、該0式より実効距離dは求まる。
As is clear from Fig. 2, the effective distance lid is calculated by the following formula, (R+D+r-Rcosθ)2" (R51nθ)2=
(d+r)” .....■ holds true, so the effective distance d can be found from the formula 0.

かくして本発明によれば、測定電極の位置(第2図にお
いてθで表わされる)毎で、オシロ波形を測定すること
により、前記各式から電界強度を求めることにより電界
強度分布が得られる。
Thus, according to the present invention, the electric field intensity distribution can be obtained by measuring the oscilloscope waveform at each measurement electrode position (represented by θ in FIG. 2) and determining the electric field intensity from each of the above equations.

(発明の効果) 本発明によれば、現像域における電界強度分布を測定す
ることができ、良好な画像を得るための現像条件を設定
する上で極めて重要な意義を有する。
(Effects of the Invention) According to the present invention, it is possible to measure the electric field strength distribution in the development area, which has extremely important significance in setting development conditions for obtaining a good image.

(実施例) 三田工業社複写機(DC−112C)を用い、現像幅内
(−10’≦θ≦+10” )での静電容量分布の測定
を行なフた。
(Example) Using a Sanda Kogyo copying machine (DC-112C), the capacitance distribution within the development width (-10'≦θ≦+10'') was measured.

汲血ゑ豆 穂切:  1.Omm ドラム−スリーブ間圧1!1:  1.1mo+スリー
ブ: 主極位置 +3.5゛ 主極度 800ガウス φ     38++ui スリーブ周速 400mm/sec 現像剤: 二成分系現像剤 フェライトキャリヤ、中心粒径 80μm抵抗10’Ω
cm トナー、負帯電用の平均粒径11μmのトナー トナー濃度は、キャリヤとトナーの比表面積比が1=1
となる様に設定した。
Dumped blood Ezu beans cut: 1. Omm Drum-sleeve pressure 1!1: 1.1mo+sleeve: Main pole position +3.5゛Main pole 800 Gauss φ 38++ui Sleeve peripheral speed 400mm/sec Developer: Two-component developer ferrite carrier, center particle diameter 80μm resistance 10'Ω
cm Toner, negatively charged toner with an average particle diameter of 11 μm The toner concentration is such that the specific surface area ratio of carrier and toner is 1=1
It was set so that

測定電極、  長さ28mm   幅0.5m+nアー
ス電極、 長さ28ma+   幅10 mmアース電
極と測定電極との間隔 0.5ff1mこの静電容量分
布から前述した各式から比話電率(ε8)及び電界強度
(E)の分布を算出した。
Measuring electrode, length 28 mm Width 0.5 m + n Earth electrode, length 28 ma + width 10 mm Distance between earth electrode and measuring electrode 0.5 ff 1 m From this capacitance distribution, the specific electric rate (ε8) and the electric field are calculated from the above formulas. The distribution of intensity (E) was calculated.

その結果を第1表に示す。The results are shown in Table 1.

第1表Table 1

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

第1図は、本発明の測定方法を好適に実施するために用
いる測定装置の電気回路図、 第2図は、本発明において用いる測定装置の全体の構造
を簡単に示す図、 第3図は、第2図の測定装置に用いる測定ドラムを示す
図、 第4図は、オシロ波形を示す図、 第5図は、第4図のすシロ波形の部分拡大図を示す図で
ある。
FIG. 1 is an electric circuit diagram of a measuring device used to suitably implement the measuring method of the present invention, FIG. 2 is a diagram briefly showing the overall structure of the measuring device used in the present invention, and FIG. , FIG. 4 is a diagram showing an oscilloscope waveform, and FIG. 5 is a partially enlarged view of the oscilloscope waveform in FIG. 4.

Claims (1)

【特許請求の範囲】[Claims] (1)現像剤搬送用スリーブ近傍に、幅広のアース電極
に囲まれた線状の測定電極を周面に備えた回転可能なド
ラムを配置し、該スリーブと測定電極との間に交流電圧
を印加し、該スリーブ上に現像剤を供給して磁気ブラシ
を形成させ、該磁気ブラシが前記ドラム表面に摺擦する
様に現像剤の搬送を行なうとともに、交流電源からの印
加電圧及び測定電極に流れる電流の各波形から測定電極
の位置毎の静電容量を算出し、この静電容量の分布から
現像幅内での電解強度を求めることを特徴とする方法。
(1) A rotatable drum equipped with a linear measuring electrode surrounded by a wide ground electrode on its circumferential surface is placed near the developer conveying sleeve, and an AC voltage is applied between the sleeve and the measuring electrode. The developer is supplied onto the sleeve to form a magnetic brush, and the developer is transported so that the magnetic brush rubs against the drum surface. A method characterized by calculating the capacitance for each position of the measuring electrode from each waveform of the flowing current, and determining the electrolytic strength within the development width from the distribution of this capacitance.
JP30086188A 1988-11-30 1988-11-30 Method for measuring electric field intensity distribution of development area in magnetic brush developing method Pending JPH02147963A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30086188A JPH02147963A (en) 1988-11-30 1988-11-30 Method for measuring electric field intensity distribution of development area in magnetic brush developing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30086188A JPH02147963A (en) 1988-11-30 1988-11-30 Method for measuring electric field intensity distribution of development area in magnetic brush developing method

Publications (1)

Publication Number Publication Date
JPH02147963A true JPH02147963A (en) 1990-06-06

Family

ID=17890001

Family Applications (1)

Application Number Title Priority Date Filing Date
JP30086188A Pending JPH02147963A (en) 1988-11-30 1988-11-30 Method for measuring electric field intensity distribution of development area in magnetic brush developing method

Country Status (1)

Country Link
JP (1) JPH02147963A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7715744B2 (en) * 2007-04-20 2010-05-11 Canon Kabushiki Kaisha Image forming apparatus using peak AC potentials to move toner toward an image bearing member and a developer carrying member, respectively

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7715744B2 (en) * 2007-04-20 2010-05-11 Canon Kabushiki Kaisha Image forming apparatus using peak AC potentials to move toner toward an image bearing member and a developer carrying member, respectively
US7826758B2 (en) 2007-04-20 2010-11-02 Canon Kabushiki Kaisha Image forming apparatus

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