JPH04118565A - Measuring device for charge quantity distribution - Google Patents
Measuring device for charge quantity distributionInfo
- Publication number
- JPH04118565A JPH04118565A JP23694090A JP23694090A JPH04118565A JP H04118565 A JPH04118565 A JP H04118565A JP 23694090 A JP23694090 A JP 23694090A JP 23694090 A JP23694090 A JP 23694090A JP H04118565 A JPH04118565 A JP H04118565A
- Authority
- JP
- Japan
- Prior art keywords
- toner particles
- toner
- charge amount
- electric field
- measuring
- 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
Links
- 239000002245 particle Substances 0.000 claims abstract description 147
- 230000001105 regulatory effect Effects 0.000 claims description 12
- 230000001276 controlling effect Effects 0.000 claims 1
- 230000005684 electric field Effects 0.000 abstract description 25
- 238000000034 method Methods 0.000 description 37
- 239000010410 layer Substances 0.000 description 9
- 238000010586 diagram Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- 239000011247 coating layer Substances 0.000 description 2
- 238000000926 separation method Methods 0.000 description 2
- 206010024229 Leprosy Diseases 0.000 description 1
- BGPVFRJUHWVFKM-UHFFFAOYSA-N N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] Chemical compound N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] BGPVFRJUHWVFKM-UHFFFAOYSA-N 0.000 description 1
- 238000003869 coulometry Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
Landscapes
- Other Investigation Or Analysis Of Materials By Electrical Means (AREA)
- Developing Agents For Electrophotography (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は1成分系トナー粒子の帯電量分布の測定装置に
関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a device for measuring the charge amount distribution of monocomponent toner particles.
[従来の技術]
近年、粒子写真、静電記録、静電印刷等の画像形成装置
の普及に伴って、その用途も広範囲にわたり、画像への
品質要求は厳しくなっぎている。[Prior Art] In recent years, with the spread of image forming apparatuses such as particle photography, electrostatic recording, and electrostatic printing, their uses have become widespread, and quality requirements for images have become increasingly strict.
個々で用いられるトナー粒子の特性、特に帯電量や粒径
は最終的な複写画像の画像濃度、鮮明度、かぶり等に大
きく影響する為に粒子写真特性として重要な因子となつ
いる。The characteristics of the individual toner particles used, especially the charge amount and particle size, are important factors in particle photographic characteristics because they greatly affect the image density, sharpness, fog, etc. of the final copied image.
従来、18:電量の測定はブローオフ法がよく知られて
いるが、これだけでは粒子写真特性の情報量としては不
十分である。つまりトナー粒子1個の個々の帯電量がど
のようになっているかが粒子写真特性としては重要であ
る。このようなトナーの帯電量分布を測定する方法とし
ていくつかの提案が為されている。Conventionally, the blow-off method is well known for measuring 18:coulometric capacity, but this method alone is not sufficient to provide information on particle photographic characteristics. In other words, the amount of charge of each toner particle is important for particle photographic characteristics. Several proposals have been made as methods for measuring the charge amount distribution of toner.
例えば、特開昭57−79958号公報に定速気流中の
トナー粒子を電界により偏向させ、一定時間後の偏向量
からトナーの帯電量分布を測定する方法が提案されてい
る。しかしながら、トナー粒子は場合によっては広い粒
径分布を有しており、粒径との対応がわからなければ有
効な帯電量分布とは言えない。For example, Japanese Patent Application Laid-open No. 57-79958 proposes a method in which toner particles in a constant velocity airflow are deflected by an electric field and the toner charge distribution is measured from the amount of deflection after a certain period of time. However, toner particles have a wide particle size distribution depending on the case, and if the correspondence with the particle size is not known, it cannot be said that the charge amount distribution is effective.
このような問題を解決する方法として、特開昭61−2
77071号公報が提案されている。これは、定速気流
、電界および振動波中のトナー粒子の偏向度、振動位相
より、トナー粒子の粒径に対応した帯電量分布を求める
ものである。これは、非常に有効な方法であるが、これ
らの測定法の最も重要な点は、現像系に近い形で帯電さ
れているか、更にそれらのトナーのすべてを測定してい
るかどうかである。As a method to solve such problems, Japanese Patent Application Laid-Open No. 61-2
No. 77071 has been proposed. This method determines the charge amount distribution corresponding to the particle size of toner particles from the degree of deflection and vibration phase of toner particles in a constant velocity airflow, electric field, and vibration waves. This is a very effective method, but the most important point in these measurement methods is whether all of the toner is being charged in a manner close to the development system and whether all of the toner is being measured.
そこで、2成分系トナーのキャリア粒子からトナー粒子
を分離する方法として特開昭57−79958号公報、
特開昭63−263475号公報等では、圧縮空気によ
りキャリア粒子からトナー粒子を分離する方法が提案さ
れている。しかし、これらはキャリア粒子のかげとなり
圧縮空気が有効に効かないトナー粒子が存在する為キャ
リア粒子からすべてのトナー粒子を分離することが難し
く、すべてのトナー粒子の帯電量分布を測定することは
困難である。また、特開昭60−8758号公報では、
現像容器の下方にメツシュを用いることによりトナー粒
子をキャリア粒子から分離する方法が提案されているが
、この方法ではキャリア粒子を捕集する為にメツシュが
細かくなっており、トナー粒子はメツシュを通り抜ける
際にメツシュとの摩擦により再帯電を生じ、正確な帯電
量分布の測定が困難となる場合がある。Therefore, as a method for separating toner particles from carrier particles of a two-component toner, Japanese Patent Application Laid-Open No. 57-79958 discloses
Japanese Unexamined Patent Publication No. 63-263475 proposes a method of separating toner particles from carrier particles using compressed air. However, it is difficult to separate all the toner particles from the carrier particles because some toner particles are hidden by the carrier particles and cannot be effectively affected by compressed air, making it difficult to measure the charge distribution of all toner particles. It is. Also, in Japanese Patent Application Laid-Open No. 60-8758,
A method has been proposed in which toner particles are separated from carrier particles by using a mesh below the developer container, but in this method, the mesh is fine to collect the carrier particles, and the toner particles pass through the mesh. In some cases, friction with the mesh may cause recharging, making it difficult to accurately measure the charge amount distribution.
このような問題を解決する方法として特開昭64−80
969号公報が提案されている。これは、電界によりト
ナー粒子とキャリア粒子間のクーロン力を弱め、この状
態で空気流を吹き付けることでトナー粒子をキャリア粒
子から分離するものである。しかし、この方法は最終的
なトナー粒子の分離を空気流に頼る為、すべてのトナー
粒子を分離することが難しく、よって、正しくトナー粒
子の帯電量分布を測定することが困難な場合が生じる。As a method to solve such problems, JP-A-64-80
No. 969 has been proposed. This method uses an electric field to weaken the Coulomb force between toner particles and carrier particles, and in this state, blows an air stream to separate the toner particles from the carrier particles. However, since this method relies on airflow for final separation of toner particles, it is difficult to separate all toner particles, and therefore it may be difficult to accurately measure the charge amount distribution of toner particles.
以上のように、帯電量分布の測定方法は、いまだ十分と
は言えない。As described above, the method for measuring the charge amount distribution is still not sufficient.
さらに近年、2成分現像方法に変わって1成分現像方法
が多く使われるようになってきた。1成分現像方法は現
像機が非常に小さくできる為特に小型の機械に適してい
るが、現像機の改良などにより毎分80枚(らいの高速
機械にも使われるようになってきている。しかしながら
、1成分トナーの帯電量、特に帯電量分布はいまだ十分
は解析できておらず、これらを解析することによりさら
なるレベルアップが可能だと考えられる。特に絶縁性1
成分現像方法は、トナーが、トナー粒子担持部材表面に
薄(コートされるためさらにトナー粒子の分離が難しく
なっている。すなわち、例えば分離する手段として、空
気流を用いた場合、薄層コートされたトナー眉はトナー
粒子担持部材上で吹き寄せられるため、トナー粒子担持
部材表面と再帯電を生じる、あるいは不均一なトナーコ
ート層となり帯電量分布が変化してしまうなどの不都合
が生じる。さらにトナー粒子が、トナー粒子担持部材上
で滑ってしまい測定部にトナー粒子がうまく搬送されな
い場合がある。Furthermore, in recent years, one-component developing method has been increasingly used instead of two-component developing method. The one-component developing method is particularly suitable for small machines because the developing machine can be made very small, but due to improvements in the developing machine, it is now possible to process 80 sheets per minute (also used in high-speed machines for leprosy). , the charge amount of single-component toner, especially the charge amount distribution, has not yet been fully analyzed, and it is thought that further improvements can be made by analyzing these.In particular, the insulation property 1
In the component development method, the toner particles are coated in a thin layer on the surface of the toner particle supporting member, making it even more difficult to separate the toner particles.For example, when an air stream is used as a means of separation, the toner particles are coated in a thin layer. Since the toner particles are blown onto the toner particle carrying member, problems arise such as recharging with the surface of the toner particle carrying member, or creating an uneven toner coating layer and changing the charge amount distribution.Furthermore, toner particles However, the toner particles may slip on the toner particle supporting member and the toner particles may not be properly conveyed to the measuring section.
このような、空気流によるトナー粒子の分離方法にだい
し、電界のみでトナー粒子を分離する方法が特開昭62
−58175号公報に提案されている。この方法は絶縁
体からなるスリーブの内部に埋め込められた2電極間に
交番電界を印加し、この交番電界により絶縁スリーブ表
面に担持される2成分系トナーからトナー粒子を分離し
、測定部へ自由落下させトナー粒子の帯電量分布を測定
するものである。In contrast to this method of separating toner particles using air flow, a method of separating toner particles using only an electric field was developed in Japanese Patent Application Laid-Open No. 1983-1999.
This method is proposed in Japanese Patent No. -58175. In this method, an alternating electric field is applied between two electrodes embedded inside a sleeve made of an insulator, and the toner particles are separated from the two-component toner supported on the surface of the insulating sleeve by this alternating electric field. This method measures the charge amount distribution of toner particles that are dropped.
しかし、この方法に使用するスリーブは特殊なものであ
り、実際に現像に寄与するトナー粒子の帯電量分布をは
かっているとは言えない。However, the sleeve used in this method is special, and it cannot be said that it measures the charge amount distribution of toner particles that actually contribute to development.
以上のように、絶縁性1成分現像法におけるトナー粒子
の帯電量分布の測定装置は、いまだ確立されていない。As described above, an apparatus for measuring the charge amount distribution of toner particles in the insulating one-component development method has not yet been established.
[発明が解決しようとする課題]
本発明は上述のごとき問題点を解決するものである。す
なわち、実際の粒子写真システム等の画像形成装置にお
ける現像系に近い形で、帯電した1成分系トナー粒子の
IF電量分布を測定することである。また、トナー粒子
担持部材上の薄層かつ均一なトナーコート層を保ちつつ
、トナー粒子の再帯電を防止し、トナー粒子担持部材上
のすべてのトナー粒子のIF電量分布を測定することで
ある。更に、磁性トナー粒子の帯電量分布を現像系に近
い形で正しく測定することである。[Problems to be Solved by the Invention] The present invention solves the above-mentioned problems. That is, the purpose is to measure the IF charge amount distribution of charged one-component toner particles in a form similar to the developing system in an image forming apparatus such as an actual particle photography system. Another object of the present invention is to prevent recharging of toner particles while maintaining a thin and uniform toner coating layer on the toner particle carrying member, and to measure the IF charge distribution of all toner particles on the toner particle carrying member. Furthermore, it is necessary to accurately measure the charge amount distribution of magnetic toner particles in a form close to that of the developing system.
[課題を解決するための手段及び作用]本発明により講
じられた手段は、1成分系トナー粒子の帯電量分布測定
方法において、導電部材を有するトナー粒子担持部材上
に該トナー粒子を薄層にコートする規制部材と、該トナ
ー粒子担持部材および該トナー粒子担持部材と対向して
設置された対向t8i!との間に電圧を印加する電源と
、該トナー粒子の少なくとも帯電量に関する値を測定で
きる測定装置と、空気流発生装置と、該トナー粒子担持
部材と該対向電極の距離を制御する装置とを備えた帯電
量分布測定装置とするものであり、または、該規制部材
が磁性ブレートで構成されていることを特徴とする帯電
量分布測定装置、または、該規制部材が弾性ゴムブレー
ドで構成されていることを特徴とする帯電量分布測定装
置とするものである。[Means and effects for solving the problem] The means taken by the present invention is to form a thin layer of toner particles on a toner particle supporting member having a conductive member in a method for measuring the charge amount distribution of one-component toner particles. The regulating member to be coated, the toner particle carrying member, and the opposing t8i! installed opposite to the toner particle carrying member. a power supply that applies a voltage between the toner particles, a measuring device that can measure at least a value related to the amount of charge of the toner particles, an air flow generating device, and a device that controls the distance between the toner particle carrying member and the opposing electrode. The charge amount distribution measuring device is characterized in that the regulating member is composed of a magnetic plate, or the regulating member is composed of an elastic rubber blade. This is a charge amount distribution measuring device characterized by:
また、本発明の1成分系トナーの帯電量分布測定装置に
おいては以下のような作用がある。トナー粒子担持部材
上に現像系に近い形で薄層コートされたトナー粒子を、
距離を制御されたトナー粒子担持部材と対向電極との間
に電圧を印加し、該電圧により生じる電界によって、ト
ナー粒子を該トナー粒子担持部材から剥離せしめ、さら
に該電界と空気流により、トナー粒子を測定部に搬送す
ることにより、殆どすべてのトナー粒子をトナー粒子担
持部材から分離し測定することができる。このとき、空
気流の方向は電界の方向と同一がよく、少なくとも電界
と±30°でなければならない。それ以上角度が大きい
と該トナー粒子担持部材上のトナー粒子をすべて測定部
へ搬送することができない。また、空気流が強すぎると
該トナー粒子担持部材上に電界と直角の空気流が生じ、
正確に帯電量分布をはかることができない。Furthermore, the device for measuring the charge amount distribution of one-component toner according to the present invention has the following effects. Toner particles are coated in a thin layer on a toner particle carrying member in a form similar to that of a developing system.
A voltage is applied between the toner particle carrying member and the counter electrode with a controlled distance, and the electric field generated by the voltage causes the toner particles to be peeled off from the toner particle carrying member, and the toner particles are further separated by the electric field and air flow. By conveying the toner particles to the measuring section, almost all of the toner particles can be separated from the toner particle carrying member and measured. At this time, the direction of the air flow may be the same as the direction of the electric field, and must be at least ±30° with respect to the electric field. If the angle is larger than that, all the toner particles on the toner particle carrying member cannot be conveyed to the measuring section. Furthermore, if the air flow is too strong, an air flow perpendicular to the electric field will occur on the toner particle supporting member.
It is not possible to accurately measure the charge amount distribution.
特に、1成分磁性トナーはトナー粒子担持部材上で磁力
により拘束されているため、磁気的に凝集している割合
が多く、本発明の方法では凝集をほぐした状態で測定す
ることができ非常に有効である。また、近年高画質化の
方向へ技術が進み、トナー粒径がどんどん小さくなって
きているため、トナー粒子の粉体凝集力が増加し、トナ
ー粒子の帯電量分布測定が難しくなってきている。この
点でも本発明の方法は非常に有効である。In particular, since single-component magnetic toner is restrained by magnetic force on the toner particle supporting member, there is a large proportion of magnetically aggregated toner, and the method of the present invention allows measurement in a state in which the aggregates are loosened, which is very effective. It is valid. Furthermore, in recent years, technology has progressed toward higher image quality, and toner particle diameters have become smaller and smaller. This has increased the powder cohesive force of toner particles, making it difficult to measure the charge amount distribution of toner particles. The method of the present invention is also very effective in this respect.
[実施例]
以下、本発明に係わる一実施例を図面に基づいて説明す
る。[Example] Hereinafter, an example according to the present invention will be described based on the drawings.
実施例1
第1図は本発明に係わる帯電量分布測定装置の概略断面
模式図である。図中Aはトナー粒子1をトナー粒子担持
部材2より電界により剥離し、剥離したトナー粒子1を
測定部Bに搬送する為の剥離・搬送部、図中Bはトナー
粒子1の粒径と帯電量を測定する帯電量分布測定部であ
る。Example 1 FIG. 1 is a schematic cross-sectional view of a charge amount distribution measuring device according to the present invention. In the figure, A is a peeling/conveying section for peeling toner particles 1 from the toner particle carrying member 2 using an electric field and transporting the peeled toner particles 1 to measurement section B. In the figure, B is the particle size and charging of toner particles 1. This is a charge amount distribution measuring section that measures the amount of charge.
まず磁石5を内包したトナー粒子担持部材2が回転し、
磁性ブレードの規制部材4により規制されたトナー粒子
1が該トナー粒子担持部材2上に薄層にコートされる。First, the toner particle carrying member 2 containing the magnet 5 rotates,
The toner particles 1 regulated by the regulating member 4, which is a magnetic blade, are coated in a thin layer on the toner particle carrying member 2.
トナー粒子担持部材2と該対向電極3との間に、電源1
0により印加された電圧により電界を生じせしめる。こ
のとき任意の電圧の場合、該トナー粒子担持部材2は車
輪6によりレール7上を該対向電極3に対して前後に動
き、電界の力により該トナー粒子1が剥離する距離まで
移動し、固定される。そのときの電界強度はパッシェン
の法則による、放電限界以下である。A power source 1 is connected between the toner particle supporting member 2 and the counter electrode 3.
The voltage applied by 0 causes an electric field to be generated. At this time, in the case of an arbitrary voltage, the toner particle carrying member 2 moves back and forth on the rail 7 with the wheels 6 with respect to the counter electrode 3, moves to a distance where the toner particles 1 are separated by the force of the electric field, and is fixed. be done. The electric field strength at that time is below the discharge limit according to Paschen's law.
したがって該トナー粒子担持部材2上に担持されたトナ
ー粒子1には、電界と同方向の力が働(。したがって、
該トナー粒子1を該トナー粒子担持部材2より剥離する
ことが可能となる。Therefore, a force in the same direction as the electric field acts on the toner particles 1 supported on the toner particle supporting member 2.
The toner particles 1 can be peeled off from the toner particle supporting member 2.
上記の剥離されたトナー粒子1は、上記電界による力に
より該対向電極3方向に飛翔する。該対向電極3の近傍
では空気流発生装置31により、3000cm’/wi
nに設定された均一な空気流が矢印の方向へ通じている
。したがって、上記対向電極3近傍に飛翔してきたトナ
ー粒子1は上記空気流により帯電量分布測定部Bの導入
部へと搬送される。The peeled off toner particles 1 fly in the direction of the counter electrode 3 due to the force caused by the electric field. In the vicinity of the counter electrode 3, an air flow generator 31 generates an air flow of 3000 cm'/wi.
A uniform air flow set at n leads in the direction of the arrow. Therefore, the toner particles 1 flying near the counter electrode 3 are conveyed to the introduction section of the charge amount distribution measuring section B by the air flow.
本発明においては規制部材4によりトナー粒子担持部材
2上に薄層コートされたトナー粒子1は、電界の力によ
り剥離、飛翔し、さらに測定装置を通した空気流発生装
置31により吸引することで均一な空気流を形成させ、
帯電量分布測定部Bまで搬送することができる。In the present invention, the toner particles 1 coated in a thin layer on the toner particle carrying member 2 by the regulating member 4 are peeled off and flown by the force of an electric field, and are further sucked by the air flow generator 31 passing through the measuring device. Creates a uniform airflow,
It can be transported to the charge amount distribution measuring section B.
帯電量分布測定部Bまで搬送されたトナー粒子1は、測
定装置21により所定の物理量が測定され、演算部22
により該物理量が、帯電量と粒径に変換される。The toner particles 1 conveyed to the charge amount distribution measuring section B have a predetermined physical quantity measured by the measuring device 21, and are transferred to the calculating section 22.
The physical quantities are converted into charge amount and particle size.
したがって、複数個のトナー粒子1を上記過程により、
測定することにより、粒径に対する帯電量分布を得るこ
とができる。Therefore, by the above process, a plurality of toner particles 1 are
By measuring, it is possible to obtain the charge amount distribution with respect to the particle size.
第2図は、上記測定装置の一例を示したものである。第
2図(a)は、レーザードツプラー法を用いた、帯電量
と粒径を測定する方法である。図中の211a、 21
1bは、振!lJ電極板であり、212は、振動発生装
置である。よく知られているように、−足振動している
空気基に存在する微小粒体は、空気振動に追従して振動
する。このとき、粒体の慣性のため、大きな粒体はど基
準の振動から遅れて振動する。また、上記振!I]電極
板211a、 211bに電圧を加えると、粒体は、そ
の粒径と帯電量と印加された電圧による電界とにより、
電界方向に偏移する。したがって、粒体の空気振動に対
する振動の位相遅れと、電界による偏移度を測定すると
、粒体の粒径と帯電量が求められる。FIG. 2 shows an example of the above measuring device. FIG. 2(a) shows a method of measuring the amount of charge and particle size using the laser Doppler method. 211a, 21 in the figure
1b is shaking! 1J electrode plate, and 212 is a vibration generator. As is well known, minute particles existing in an air base that vibrates follow the air vibrations. At this time, due to the inertia of the grains, the large grains vibrate with a delay from the standard vibration. Also, the above shake! I] When a voltage is applied to the electrode plates 211a and 211b, the particles change due to their particle size, amount of charge, and electric field due to the applied voltage.
Shifts in the direction of the electric field. Therefore, by measuring the phase delay of the vibration of the particles relative to the air vibration and the degree of deviation due to the electric field, the particle size and charge amount of the particles can be determined.
本発明においてはレーザー発生部213とレーザー受光
部214 とを配し、レーザードツプラー法を用いるこ
とにより、トナー粒子1の空気振動に対する位相遅れと
、電界による偏移速度を測定し、この測定量を第1図中
の演算部22で演算することにより、トナー粒子1の粒
径と帯電量を得ている。In the present invention, a laser generating section 213 and a laser receiving section 214 are arranged, and by using the laser Doppler method, the phase delay of the toner particles 1 with respect to air vibration and the shift speed due to the electric field are measured, and the measured quantity is The particle size and charge amount of the toner particles 1 are obtained by calculating them in the calculating section 22 in FIG.
また、測定方法は第2図(a)の如くには限らず、例え
ば第2図(b)の如くでもよい。Further, the measuring method is not limited to that shown in FIG. 2(a), but may be, for example, as shown in FIG. 2(b).
すなわち、レーザー発生部213から、レーザーを発生
し、発生レーザーを窓217を通してレーザー受光部2
14に入れ、トナー粒子1の空気流方向の速度を、レー
ザードツプラー法により測定する。よく知られているよ
うに、空気流中を落下している微小粒体の空気流に対す
る相対落下速度を測定することにより、粒体の径を求め
ることができる。したがフて、上記レーザードツプラー
法により、トナー粒子1の相対落下速度を求め、演算装
置22(a)により演算することにより、トナー粒子1
の粒径を得ることができる。That is, the laser generator 213 generates a laser, and the generated laser passes through the window 217 to the laser receiver 2.
14, and the velocity of the toner particles 1 in the air flow direction is measured by the laser Doppler method. As is well known, the diameter of a particle can be determined by measuring the relative falling speed of a minute particle falling in an air stream with respect to the air stream. Therefore, the relative falling speed of the toner particles 1 is determined by the laser Doppler method and calculated by the arithmetic unit 22(a).
particle size can be obtained.
また、よく知られているように、検出電極218にトナ
ー粒子1により誘起される電荷を、電荷測定装置22(
b)で測定することにより、トナー粒子1の帯電量を測
定することができる。In addition, as is well known, the charge measurement device 22 (
By measuring in b), the amount of charge on the toner particles 1 can be measured.
実施例2
本発明は上記実施例に限るものではなく、例えば第3図
の模式図に示すように、規制部材4が非磁性ブレートに
より薄層にする構成にしても良い。Embodiment 2 The present invention is not limited to the above-mentioned embodiment. For example, as shown in the schematic diagram of FIG. 3, the regulating member 4 may be formed into a thin layer using a non-magnetic plate.
実施例3
また、第4図に示すように、規制部材4が弾性ゴムブレ
ードで薄層にする構成をとっても良い。Embodiment 3 Furthermore, as shown in FIG. 4, the regulating member 4 may be made of a thin layer of elastic rubber blade.
[発明の効果]
以上説明したように本発明によれば、現像系に近い形で
薄層コートされ帯電した1成分系トナー粒子のIF電量
分布が、より精度よく測定できる。[Effects of the Invention] As described above, according to the present invention, the IF charge distribution of charged monocomponent toner particles coated in a thin layer in a manner similar to that of a developing system can be measured with higher accuracy.
特に、トナー粒子担持部材上のトナー粒子のほとんどを
トナー粒子担持部材上から剥離できるため、再現性も向
上する。In particular, since most of the toner particles on the toner particle carrying member can be peeled off from the toner particle carrying member, reproducibility is also improved.
また、トナー粒子担持部材上から剥離したトナー粒子の
ほとんどを測定できるため、効率も良い。Furthermore, since most of the toner particles peeled off from the toner particle supporting member can be measured, efficiency is also high.
第1図は本発明の概略模式断面図、
第2図は本発明に用いた測定部の概略図、第4図は本発
明の別実施例の概略棋式
第3図。
図である。
1:トナー粒子
3:対向電極
5:磁石
7:レール
21:測定装置
22(a):演算装置
31・空気流発生装置
212:振動発生装置
214:レーザー受光部
218:検出電極
B:帯電量分布測定部
2:トナー粒子担持部材
4、規制部材
6、車輪
10、電圧可変電源
22:演算部
22 (b) :電荷測定装置
211a、 211b :振動電極板
213:レーザー発生部
217:窓
A:剥離・搬送部FIG. 1 is a schematic sectional view of the present invention, FIG. 2 is a schematic diagram of a measuring section used in the present invention, and FIG. 4 is a third schematic diagram of a chess game system of another embodiment of the present invention. It is a diagram. 1: Toner particles 3: Opposing electrode 5: Magnet 7: Rail 21: Measuring device 22 (a): Arithmetic device 31/air flow generator 212: Vibration generator 214: Laser receiver 218: Detection electrode B: Charge amount distribution Measuring section 2: toner particle carrying member 4, regulating member 6, wheel 10, variable voltage power source 22: calculating section 22 (b): charge measuring device 211a, 211b: vibrating electrode plate 213: laser generating section 217: window A: peeling・Transportation section
Claims (3)
導電部材を有するトナー粒子担持部材上に該トナー粒子
を薄層にコートする規制部材と、該トナー粒子担持部材
および該トナー粒子担持部材と対向して設置された対向
電極との間に電圧を印加する電源と、該トナー粒子の少
なくとも帯電量に関する値を測定できる測定装置と、空
気流発生装置と、該トナー粒子担持部材と該対向電極の
距離を制御する装置とを備えた帯電量分布測定装置。(1) In measuring the charge amount distribution of one-component toner particles,
Applying a voltage between a regulating member that coats a thin layer of toner particles on a toner particle carrying member having a conductive member, and a counter electrode disposed opposite to the toner particle carrying member and the toner particle carrying member. A charge amount distribution measuring device comprising: a power supply for measuring at least a value related to the charge amount of the toner particles; a measuring device capable of measuring at least a value related to the charge amount of the toner particles; an air flow generating device; and a device controlling the distance between the toner particle carrying member and the counter electrode. .
、規制部材が磁性ブレードで構成されていることを特徴
とする帯電量分布測定装置。(2) The charge amount distribution measuring device according to claim (1), wherein the regulating member is constituted by a magnetic blade.
、規制部材が弾性ゴムブレードで構成されていることを
特徴とする帯電量分布測定装置。(3) The charge amount distribution measuring device according to claim (1), wherein the regulating member is constituted by an elastic rubber blade.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP23694090A JPH04118565A (en) | 1990-09-10 | 1990-09-10 | Measuring device for charge quantity distribution |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP23694090A JPH04118565A (en) | 1990-09-10 | 1990-09-10 | Measuring device for charge quantity distribution |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04118565A true JPH04118565A (en) | 1992-04-20 |
Family
ID=17008006
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP23694090A Pending JPH04118565A (en) | 1990-09-10 | 1990-09-10 | Measuring device for charge quantity distribution |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04118565A (en) |
-
1990
- 1990-09-10 JP JP23694090A patent/JPH04118565A/en active Pending
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