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JP3259022B2 - Method and apparatus for measuring charge amount of charged powder particles - Google Patents
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JP3259022B2 - Method and apparatus for measuring charge amount of charged powder particles - Google Patents

Method and apparatus for measuring charge amount of charged powder particles

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Publication number
JP3259022B2
JP3259022B2 JP13033490A JP13033490A JP3259022B2 JP 3259022 B2 JP3259022 B2 JP 3259022B2 JP 13033490 A JP13033490 A JP 13033490A JP 13033490 A JP13033490 A JP 13033490A JP 3259022 B2 JP3259022 B2 JP 3259022B2
Authority
JP
Japan
Prior art keywords
charged powder
image
image information
powder particle
flow
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 - Fee Related
Application number
JP13033490A
Other languages
Japanese (ja)
Other versions
JPH0425772A (en
Inventor
幸夫 田端
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
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Filing date
Publication date
Application filed by Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP13033490A priority Critical patent/JP3259022B2/en
Publication of JPH0425772A publication Critical patent/JPH0425772A/en
Application granted granted Critical
Publication of JP3259022B2 publication Critical patent/JP3259022B2/en
Anticipated expiration legal-status Critical
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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はたとえば電子写真用現像剤に用いられるトナ
ー等の荷電粉体粒子の帯電量を測定する方法及び装置に
関する。
Description: TECHNICAL FIELD The present invention relates to a method and an apparatus for measuring a charge amount of charged powder particles such as a toner used for an electrophotographic developer, for example.

〔従来の技術〕[Conventional technology]

一般に、工学的に応用されている荷電粉体粒子として
は電子写真用トナーが知られている。
Generally, an electrophotographic toner is known as a charged powder particle that is applied in engineering.

このトナーの比電荷(帯電量)を測定する方法は最近
開発され始められているが、その主な方法としては、つ
ぎの二つの方法が広く採用されている。
A method for measuring the specific charge (charge amount) of the toner has recently been developed, and the following two methods are widely used as main methods.

(1)一様流中の1ケ所にトナー群を集中的に導入して
電界下で偏位させ、落下したトナーの位置座標を読みと
ってトナーの比電荷(帯電量)を測定する方法。
(1) A method of intensively introducing a group of toners into one place in a uniform flow, displacing the group under an electric field, reading the position coordinates of the dropped toner, and measuring the specific charge (charge amount) of the toner.

(2)トナー群の流れを散在的に作成し、この流れにレ
ーザー光を照射してその反射光によりトナーの流速を求
め、この値から比電荷(帯電量)を測定する方法。
(2) A method of scatteredly creating a flow of a toner group, irradiating the flow with a laser beam, determining the flow velocity of the toner based on the reflected light, and measuring the specific charge (charge amount) from this value.

〔発明が解決しようとする課題〕[Problems to be solved by the invention]

しかしながら、(1)の方法は、精度に問題があり、
また(2)の方法はトナーの流速を算出するため(1)
の方法に比べ精度が高くなる可能性を秘めてはいるが、
測定結果の校正が難かしく、またレーザー光を用いるた
め高度の技術と複雑な装置を必要としそのメインテナン
スが高価となる欠点があった。
However, the method (1) has a problem in accuracy,
The method (2) calculates the flow velocity of the toner (1).
Although there is a possibility that the accuracy will be higher than the method of
Calibration of the measurement results is difficult, and the use of laser light requires a high level of technology and complicated equipment, and has the disadvantage of high maintenance.

本発明は安価かつ簡易なメインテナンスによって荷電
粉体粒子の帯電量を簡便かつ高精度で測定し得る方法及
び装置を提供することを目的とする。
SUMMARY OF THE INVENTION An object of the present invention is to provide a method and an apparatus which can measure the charge amount of charged powder particles simply and with high accuracy by inexpensive and simple maintenance.

〔課題を解決するための手段〕[Means for solving the problem]

上記目的を達成するため、本発明における荷電粉体粒
子の帯電量測定方法は、一様流速の空気流中に荷電粉体
粒子を導き、荷電粉体粒子流を作り、その流れ方向に垂
直な方向に平行電界を印加し、該電界下で変位する荷電
粉体粒子群を拡大光学系により拡大し、該拡大映像を光
電換素子によって光電変換し画情報となし、該画情報を
加工処理することによって荷電粉体粒子の変位情報と粒
径を求め、もって荷電粉体粒子の比電荷を算出するもの
である。
In order to achieve the above object, the method for measuring the charged amount of charged powder particles in the present invention is to guide the charged powder particles into an air stream having a uniform flow rate, to create a charged powder particle flow, and to make the flow perpendicular to the flow direction. A parallel electric field is applied in the direction, the charged powder particle group displaced under the electric field is enlarged by an enlargement optical system, the enlarged image is photoelectrically converted by a photoelectric conversion element into image information, and the image information is processed. Thus, the displacement information and the particle size of the charged powder particles are obtained, and the specific charge of the charged powder particles is thereby calculated.

そして、測定精度をより一層高めるためには、荷電粉
体粒子群と拡大光学系との間に回転可能もしくは移動可
能な反射鏡を設け、該反射鏡を荷電粉体粒子群の流れ方
向の移動に応じて回転もしくは移動させることにより、
光電変換素子上に前記流れ方向に関しては静止している
荷電粉体粒子群の拡大映像を与えるようにするのが好ま
しい。
In order to further improve the measurement accuracy, a rotatable or movable reflecting mirror is provided between the charged powder particle group and the magnifying optical system, and the reflecting mirror is moved in the flow direction of the charged powder particle group. By rotating or moving according to
It is preferable to provide an enlarged image of the charged powder particle group that is stationary in the flow direction on the photoelectric conversion element.

また、光電変換素子で変換した画情報を一旦画像記録
装置で記録体に記録した後、これを再生しながら上記画
情報の処理を行なうようにしてもよい。この画像記録装
置には、ビデオテープレコーダが用いられる。
Further, the image information converted by the photoelectric conversion element may be temporarily recorded on a recording medium by an image recording device, and then the image information may be processed while reproducing the image information. This image recording device uses a video tape recorder.

また、光電変換素子で映像を撮影しながら、変換され
た画情報を記憶し該情報を加工、処理し、結果を画情報
として記憶するようにしてもよい。
Alternatively, the converted image information may be stored, the information may be processed and processed, and the result may be stored as image information while the video is captured by the photoelectric conversion element.

さらに、上記目的を達成するため、本発明の荷電粉体
粒子の帯電量測定装置は、一様流速の空気流中に荷電粉
体粒子を導き、荷電粉体粒子流を作成する装置、該荷粉
体粒子流の流れ方向に垂直な方向に平行電界を印加する
装置、該電界下で変位する荷電粉体粒子群の像を拡大光
学系により拡大し、該拡大映像を光電変換し画情報を得
る装置、及び該画情報を加工処理し荷電粉体粒子の変位
情報と粒径を求め、これらの値に基づいて荷電粉体粒子
の比電荷を算出する装置を具備して構成される。
Further, in order to achieve the above object, a charged amount measuring apparatus for charged powder particles according to the present invention is an apparatus for guiding a charged powder particle into an air stream having a uniform flow rate to create a charged powder particle flow, A device for applying a parallel electric field in a direction perpendicular to the flow direction of the powder particle flow, an image of a group of charged powder particles displaced under the electric field is enlarged by an enlargement optical system, and the enlarged image is photoelectrically converted to obtain image information. And a device for processing the image information to obtain displacement information and the particle size of the charged powder particles, and calculating the specific charge of the charged powder particles based on these values.

そして、測定精度をより一層高めるためには、荷電粉
体粒子群と拡大光学系との間に、光電変換素子上に荷電
粉体粒子流の流れ方向に関しては静止している荷電粉体
粒子群の拡大映像を与えるように荷電粉体粒子群の流れ
方向に応じて回転可能もしくは移動可能な反射鏡を設け
るのが好ましい。
In order to further improve the measurement accuracy, the charged powder particle group which is stationary with respect to the flow direction of the charged powder particle flow on the photoelectric conversion element between the charged powder particle group and the magnifying optical system It is preferable to provide a reflecting mirror that is rotatable or movable in accordance with the flow direction of the charged powder particle group so as to give an enlarged image.

〔作用〕[Action]

本発明の荷電粉体粒子の帯電量測定方法及び装置によ
れば、荷電粉体粒子流に電界を印加したときに変位する
荷電粉体粒子群の画情報を得、この情報を加工処理して
変位情報と粒径を求め、これらデータに基づいて演算を
行うことにより、高度の技術と複雑な装置を必要としな
いで、高精度に所望の荷電粉体粒子の比電荷が得られる
ようになる。
According to the method and apparatus for measuring the charged amount of charged powder particles of the present invention, image information of a group of charged powder particles that are displaced when an electric field is applied to a charged powder particle stream is obtained, and this information is processed. By calculating the displacement information and the particle size and performing calculations based on these data, it becomes possible to obtain the specific charge of the desired charged powder particles with high accuracy without requiring advanced technology and complicated equipment. .

また、反射鏡を用いた場合には、この反射鏡が流れ方
向に関して静止している荷電粉体粒子群の拡大映像を与
えるように働くので、拡大光学系の倍率を上げることが
できより一層の高精度化が可能となる。
In addition, when a reflecting mirror is used, the reflecting mirror works so as to give an enlarged image of the charged powder particle group which is stationary in the flow direction, so that the magnification of the magnifying optical system can be increased, and furthermore, Higher accuracy is possible.

〔実施例〕〔Example〕

第1図は荷電粉体粒子としてトナーを対象とした本発
明の第1の実施例に係る帯電量測定装置の機能構成図で
あり、以下詳細に説明する。
FIG. 1 is a functional configuration diagram of a charge amount measuring apparatus according to a first embodiment of the present invention, which targets toner as charged powder particles, and will be described in detail below.

先ず、本実施例におけるトナーの帯電量の測定原理に
ついて説明する。
First, the principle of measuring the charge amount of the toner in this embodiment will be described.

今、第1図に示すように、一様流速の空気流中にトナ
ー群を導き、その流れ方向に対して垂直な方向に平行電
界を印加したとする。ここでトナーは球形と近似し、空
気流の流れ方向をz方向、電界の印加方向をx方向、ト
ナーのz方向の速度をVz、トナーのx方向の速度をVx、
トナー粒子1個の電荷量をq、トナー粒子の半径をrと
すると、粘性流体内における物体の受ける抵抗を与える
法則(ストークスの定理)により次の関係式が得られ
る。
Now, as shown in FIG. 1, it is assumed that the toner group is guided into an air flow having a uniform flow velocity, and a parallel electric field is applied in a direction perpendicular to the flow direction. Here, the toner is approximated as a sphere, the flow direction of the air flow is the z direction, the direction of application of the electric field is the x direction, the speed of the toner in the z direction is Vz, the speed of the toner in the x direction is Vx,
Assuming that the charge amount of one toner particle is q and the radius of the toner particle is r, the following relational expression is obtained by the law (Stokes' theorem) that gives the resistance of the object in the viscous fluid.

したがって、Vxを求めることにより、q/2rが求まる。
ここでトナーの半径rは測定より得られ、トナー密度も
既知であるから比電荷を算出する。比電荷の値は、トナ
ー粒子1個の質量を算出し、トナー粒子1個の質量
(m)当たりの既に得られている電荷量(q)の値よ
り、q/mを算出することより、計算される。
Therefore, q / 2r is obtained by obtaining Vx.
Here, since the radius r of the toner is obtained from the measurement and the toner density is also known, the specific charge is calculated. The value of the specific charge is calculated by calculating the mass of one toner particle and calculating q / m from the value of the already obtained charge amount (q) per mass (m) of one toner particle. Is calculated.

次に、装置構成について説明する。 Next, the device configuration will be described.

第1の実施例の装置は、第1図に示すように、一様流
作成装置1、電界付与装置2、照明3、拡大光学系4、
光電変換素子5、物理量測定装置6及び情報処理装置7
から構成される。物理量測定装置6は画情報を取り込み
ながら変位の情報及び粒径の物理量を計算する装置で、
これにより、実時間の測定が可能となる。
As shown in FIG. 1, the apparatus of the first embodiment includes a uniform flow creating device 1, an electric field applying device 2, an illumination 3, an enlargement optical system 4,
Photoelectric conversion element 5, physical quantity measuring device 6, and information processing device 7
Consists of The physical quantity measuring device 6 is a device that calculates displacement information and physical quantity of particle size while taking in image information.
This allows real-time measurement.

また、第1図の構成で物理量測定装置6の代りに録画
再生装置及び画情報記憶装置で置き換えることもでき
る。このような置き換えをしたものを本発明の第2の実
施例とし、その機能構成を第2図に、一部模式化した外
観構成を第3図にそれぞれ示す。
Further, in the configuration of FIG. 1, a recording / reproducing device and an image information storage device can be substituted for the physical quantity measuring device 6. FIG. 2 shows a second embodiment of the present invention in which such replacement is performed, and FIG. 3 shows a functional configuration thereof, and FIG. 3 shows a partially schematic external configuration thereof.

以下、第2の実施例につき第2図及び第3図を参照し
て詳細に説明する。なお、図中Pはトナー粒子を代表し
て示す。一様流作成装置1は一様流速の空気流を形成
し、その中にトナー粒子群を導き、トナー流を形成す
る。電界付与装置2は一様流作成装置1が形成したトナ
ー流にその流れ方向に対して垂直な方向に平行電界を付
与する。照明3はトナー粒子の像を生じさせるためのも
ので、連続照射光でもよく、録画再生装置8と同期した
ストロボ光でもよい。また照明3は図示の如く透過光を
撮像できるようにトナーに対して撮像側と反対に設ける
方がコントラストを高くとれるので好ましいが、撮像側
と同側とし反射光を撮像するようにしてもよい。拡大光
学系4はたとえば顕微鏡からなり、変位するトナー群の
像を拡大して撮像側に与える。光電変換素子5はたとえ
ばCCDからなり、トナー粒子の像を表わす光信号を映像
信号に変換して出力する。録画再生装置8はたとえばビ
デオテープレコーダーからなり、トナー粒子群の移動映
像を録画、再生する機能を有するとともに、光電変換素
子5を制御する機能(カメラコントローラー)を有す
る。画情報記憶装置9は録画再生装置8が再生したトナ
ー粒子群の移動映像を電子情報として格納する。情報処
理装置7はコンピューターで構成でき、画情報記憶装置
9から画情報を取り込み、その画情報を加工処理し、変
位情報と粒径の物理量を計算しこれから比電荷を算出し
集計する。なお、第3図には各装置を連結するケーブル
と、その中を通る信号の向きが示されている。
Hereinafter, the second embodiment will be described in detail with reference to FIG. 2 and FIG. In the drawing, P represents a toner particle as a representative. The uniform flow creating device 1 forms an air flow having a uniform flow velocity, guides a group of toner particles therein, and forms a toner flow. The electric field applying device 2 applies a parallel electric field to the toner flow formed by the uniform flow creating device 1 in a direction perpendicular to the flow direction. The illumination 3 is for generating an image of toner particles, and may be continuous irradiation light or strobe light synchronized with the recording / reproducing device 8. It is preferable to provide the illumination 3 opposite to the image pickup side with respect to the toner so that the transmitted light can be picked up as shown in the figure, since the contrast can be increased. However, the illumination 3 may be provided on the same side as the image pickup side to pick up the reflected light. . The magnifying optical system 4 includes, for example, a microscope, and magnifies the image of the displaced toner group and provides the magnified image to the imaging side. The photoelectric conversion element 5 is formed of, for example, a CCD, and converts an optical signal representing an image of a toner particle into a video signal and outputs the video signal. The recording / reproducing device 8 is composed of, for example, a video tape recorder, and has a function of recording and reproducing a moving image of the toner particle group and a function of controlling the photoelectric conversion element 5 (camera controller). The image information storage device 9 stores the moving image of the toner particle group reproduced by the recording and reproducing device 8 as electronic information. The information processing device 7 can be constituted by a computer, fetches image information from the image information storage device 9, processes the image information, calculates displacement information and physical quantities of particle diameters, and then calculates and totals specific charges. FIG. 3 shows the cables connecting the devices and the directions of the signals passing through the cables.

次に動作について述べる。 Next, the operation will be described.

先ず、一様流作成装置1において一様流の空気流が形
成され、その中にトナー粒子群が導かれ、トナー流とな
る。このトナー流は電界付与装置2が付与する流れ方向
と垂直な平行電界により第3図に示すように途中で変位
する。このとき、撮像側とは反対側に設けられた照明3
によりトナー流に照光が行われ、その透過光によってト
ナー粒子の像が得られる。この像は拡大光学系4により
拡大され、光電変換素子5の素子面上に結像する。光電
変換素子5は録画再生装置8の制御の下に、トナー粒子
の像の光信号を光電変換して映像信号として録画再生装
置8に出力する。このとき、手動で録画再生装置8を録
画モードに設定し、トナー粒子群の移動映像を録画す
る。録画が終了するとテープを巻戻し、情報処理装置7
による自動制御に切り換える。すると情報処理装置7は
録画再生装置8を制御し、通常、スローあるいはスチル
(静止)モードの再生を使い分けて行わせ、録画再生装
置8が再生した画面の情報を画情報記憶装置9に取り込
ませる。そして情報処理装置7は画情報記憶装置9が格
納している画情報を加工、処理し、トナーの比電荷の値
を算出するために必要な原始データを計算し、その結果
を記憶する。1つの画面の画情報の処理が終わると、所
定時間経過した次の画面の画情報を同様に処理し、以下
同様にして全部の画面の画情報の処理を行う。原始デー
タが得られると、これらに基づいて比電荷q/mを算出し
これらを集計する。
First, a uniform flow of air is formed in the uniform flow creating device 1, and a group of toner particles is guided into the air to form a toner flow. This toner flow is displaced on the way as shown in FIG. 3 by a parallel electric field perpendicular to the flow direction applied by the electric field applying device 2. At this time, the illumination 3 provided on the side opposite to the imaging side
Illuminates the toner flow, and an image of toner particles is obtained by the transmitted light. This image is enlarged by the enlargement optical system 4 and forms an image on the element surface of the photoelectric conversion element 5. The photoelectric conversion element 5 photoelectrically converts the optical signal of the image of the toner particles under the control of the recording / reproducing device 8 and outputs it to the recording / reproducing device 8 as a video signal. At this time, the recording / reproducing device 8 is manually set to the recording mode, and the moving image of the toner particle group is recorded. When the recording is completed, the tape is rewound and the information processing device 7
Switch to automatic control by. Then, the information processing device 7 controls the recording / reproducing device 8 to perform the normal or slow (still) mode reproduction properly, and causes the image information storage device 9 to capture the information of the screen reproduced by the recording / reproducing device 8. . Then, the information processing device 7 processes and processes the image information stored in the image information storage device 9, calculates source data necessary for calculating the value of the specific charge of the toner, and stores the result. When the processing of the image information of one screen is completed, the image information of the next screen after a lapse of a predetermined time is similarly processed, and the processing of the image information of all the screens is performed in the same manner. When the primitive data is obtained, the specific charge q / m is calculated based on these, and these are totaled.

次に第4図のフローチャートを用いて情報処理装置7
が原始データを得る手順について詳細に説明する。
Next, the information processing apparatus 7 will be described with reference to the flowchart of FIG.
The procedure for obtaining source data will be described in detail.

先ず、情報処理装置7は画情報記憶装置9から最初の
画面の画情報を取り込み(ステップS1)、これに対し2
値化処理、ノイズ除去等の前処理を施す(ステップS2,S
3)。これらの処理を施した後、トナー粒子1個の粒径
dを求め、これから半径rを得る(ステップS4)。次に
トナー粒子の中心座標、速度Vx、Vzの導出を行い(ステ
ップS5,S6)、その結果を格納する(ステップS7)。以
上の処理が終わると、画情報記憶装置9から次の画面の
画情報を取り込み、上記と同様のルーチンを、全部の画
面の画情報に対し行う。そして原始データの蓄積が終了
すると、これらのデータを基に前述の関係式にしたがっ
て演算を行い、比電荷q/mを得、集計し結果を得る。
First, the information processing device 7 fetches the image information of the first screen from the image information storage device 9 (step S1).
Perform pre-processing such as binarization processing and noise removal (steps S2, S
3). After performing these processes, the particle diameter d of one toner particle is obtained, and the radius r is obtained therefrom (step S4). Next, the central coordinates and velocities Vx and Vz of the toner particles are derived (steps S5 and S6), and the results are stored (step S7). When the above processing is completed, the image information of the next screen is fetched from the image information storage device 9, and the same routine as described above is performed on the image information of all the screens. When the accumulation of the primitive data is completed, an operation is performed on the basis of these data in accordance with the above-mentioned relational expression, a specific charge q / m is obtained, and a total result is obtained.

上記実施例では、画情報記憶装置9と情報処理装置7
とが別個に設けてあるが、両装置を一体化して一台のコ
ンピューターで画情報記憶・情報処理装置としてもよ
い。この場合、上記実施例の画情報記憶装置9の機能は
コンピューター内部に組込まれる。
In the above embodiment, the image information storage device 9 and the information processing device 7
Are provided separately, but the image information storage / information processing apparatus may be integrated with a single computer by integrating the two apparatuses. In this case, the functions of the image information storage device 9 of the above embodiment are incorporated in the computer.

上記実施例では、録画再生装置8における録画までを
手動で行っているが、勿論、これについても情報処理装
置7による自動制御とすることが可能である。
In the above embodiment, up to the recording in the recording / reproducing device 8 is manually performed. However, it is needless to say that automatic control by the information processing device 7 is also possible.

また、録画再生装置8の録画速度が不十分な場合は、
フロートナー像を録画する録画装置と、該録画装置で録
画されたテープを情報処理装置7で制御し再生するため
の録画再生装置の2台を用いてもよい。この場合は、録
画装置におけるテープへの録画及び該テープを録画再生
装置に装填するところは手動となる。
If the recording speed of the recording / playback device 8 is insufficient,
A recording device for recording the flow toner image and a recording and reproducing device for controlling and reproducing the tape recorded by the recording device with the information processing device 7 may be used. In this case, recording on the tape in the recording device and loading the tape into the recording / reproducing device are performed manually.

次に、本発明による第3の実施例について説明する。 Next, a third embodiment according to the present invention will be described.

本発明の第3の実施例に係る帯電量測定装置の機能構
成を第5図に示す。同図において第1図と同様な要素に
は同一符号が付してある。図中、10は誘導管、11はスリ
ット、12は回転可能な反射鏡であり、また一様流作成装
置及び電界付与装置は図示を省略してある。反射鏡12は
誘導管10中のトナー流の流速と、該反射鏡12による光像
の移動速度が等しくなるように回転するようになってい
る。
FIG. 5 shows a functional configuration of the charge amount measuring device according to the third embodiment of the present invention. In this figure, the same elements as those in FIG. 1 are denoted by the same reference numerals. In the figure, 10 is a guide tube, 11 is a slit, 12 is a rotatable reflecting mirror, and a uniform flow creating device and an electric field applying device are not shown. The reflecting mirror 12 rotates so that the flow velocity of the toner flow in the guide tube 10 and the moving speed of the optical image by the reflecting mirror 12 become equal.

動作について説明すると、先ず、一様流作成装置(図
示せず)において一様流の空気流が形成され、その中に
トナー粒子群が導かれ、トナー流れとなり、誘導管10に
導入される。トナー流が誘導管10を通過する際、電界付
与装置(図示せず)の一対の電極が付与する電界により
各トナー粒子は変位する。このとき、照明3からの照射
光により生じるトナー粒子の像はスリット11を経て反射
鏡12に当たる。この反射鏡12は図示しない駆動手段によ
り、トナー流の流速と、該反射鏡12による像の移動速度
が等しくなるように回転している。このため、着目して
いるトナー粒子を広い範囲で把えることができ、また光
電変換素子5上に映ったトナー粒子の像は流れ方向に関
しては静止したものとなる。すなわち、光電変換素子5
上言い換えるとモニター画面上でのトナー粒子の像の動
きは第6図に示すように水平方向(x方向)における移
動のみとなる。第6図にはn番目の画面と(n+1)番
目の画面を同時に示してある。更に、この場合、トナー
粒子の像が流れ方向に関して相対的に静止するので、ボ
ケがなくなり、鮮明度の高い画像が得られるというメリ
ットもある。したがって、高速のトナー流れであって
も、画面上で多数のトナー粒子の移動がとらえられるこ
とになる。
In operation, first, a uniform flow of air is formed in a uniform flow creating device (not shown), and a group of toner particles is guided into the air flow, becomes a toner flow, and is introduced into the guide tube 10. When the toner flow passes through the guide tube 10, each toner particle is displaced by an electric field applied by a pair of electrodes of an electric field applying device (not shown). At this time, the image of the toner particles generated by the irradiation light from the illumination 3 strikes the reflecting mirror 12 via the slit 11. The reflecting mirror 12 is rotated by a driving unit (not shown) so that the flow velocity of the toner flow and the moving speed of the image by the reflecting mirror 12 become equal. Therefore, the toner particles of interest can be grasped in a wide range, and the image of the toner particles reflected on the photoelectric conversion element 5 becomes stationary in the flow direction. That is, the photoelectric conversion element 5
In other words, the movement of the image of the toner particles on the monitor screen is only a movement in the horizontal direction (x direction) as shown in FIG. FIG. 6 shows the n-th screen and the (n + 1) -th screen at the same time. Furthermore, in this case, since the image of the toner particles is relatively stationary in the flow direction, there is an advantage that blur is eliminated and an image with high definition can be obtained. Therefore, even with a high-speed toner flow, movement of a large number of toner particles on the screen can be captured.

光電変換素子5で電気的情報に変換された画像情報は
物理量測定装置6に入り、ここでトナーのx方向すなわ
ち電界印加方向の速度Vxが計算される。速度Vxは、ある
画面から次の画面に移る時間tOと、時間tO中の移動距離
lとを求めた後、次式に従って算出される。
The image information converted into electrical information by the photoelectric conversion element 5 enters the physical quantity measuring device 6, where the velocity Vx of the toner in the x direction, that is, the electric field application direction is calculated. The speed Vx is calculated according to the following equation after obtaining a time t O at which one screen is changed to the next screen and a moving distance 1 during the time t O.

Vxの計算結果は直ちに情報処理装置7に送られ、ここ
でトナー流速Vxを用いて前記理論式に従って、q,d,q/m
が計算され集計されていき、一工程が終れば一測定が完
了し、最終計算結果が得られる。
The calculation result of Vx is immediately sent to the information processing device 7, where the q, d, q / m
Are calculated and totaled. When one process is completed, one measurement is completed, and a final calculation result is obtained.

第7図は第3の実施例(第5図)の物理量測定装置8
を録画再生装置8と画情報記憶装置9に置き換えた実施
例(第4の実施例)であり、両装置の動作は第2の実施
例のものと同様で、一旦録画し、これを再生しながら物
理量を求め集計していくことになる。
FIG. 7 shows a physical quantity measuring device 8 of the third embodiment (FIG. 5).
Is an embodiment (fourth embodiment) in which the recording and playback device 8 and the image information storage device 9 are replaced. The operation of both devices is the same as that of the second embodiment, and once the video is recorded and reproduced. In the meantime, physical quantities are determined and tabulated.

第8図は第7図に示す第4の実施例の具体的構成図で
あり、ここでは第3図に示した第2の実施例の装置構成
と異なる所について述べる。左側のボックスで示す装置
と右側のボックスで示す装置により誘導管10中に一様流
が形成されており、左側のボックスで示す装置からトナ
ーが導かれている。誘導管10の上下には平行電界を付与
するための一対の電極13が設けられている。そして、ト
ナー流れに対して垂直に照明3からの照射光が当てられ
ている。この照射光は前述と同様、連続光でもストロボ
光でもよい。照射光がトナー群に当たってシルエットを
担った光像はスリット11を会して反射鏡12に当たり、光
電変換素子5へと導かれる。誘導管10において光像が通
過する部分はフラット面14になっている。また反射鏡12
は前述したように光電変換素子5上即ちモニター画面上
でのトナー粒子の流れ方向の動きが静止するようモータ
ー15により所定の回転速度で回転するようになってい
る。光電変換素子5より後段の装置構成は第2の実施例
と同様である。
FIG. 8 is a specific configuration diagram of the fourth embodiment shown in FIG. 7, and here, a point different from the device configuration of the second embodiment shown in FIG. 3 will be described. A uniform flow is formed in the guide tube 10 by the device shown in the left box and the device shown in the right box, and toner is guided from the device shown in the left box. A pair of electrodes 13 for applying a parallel electric field are provided above and below the guide tube 10. Irradiation light from the illumination 3 is applied perpendicular to the toner flow. This irradiation light may be continuous light or strobe light as described above. The light image, which is illuminated and shines on the toner group and bears a silhouette, meets the slit 11, hits the reflecting mirror 12, and is guided to the photoelectric conversion element 5. A portion of the guide tube 10 through which the light image passes is a flat surface 14. Also reflector 12
As described above, the motor 15 is rotated at a predetermined rotation speed by the motor 15 so that the movement in the flow direction of the toner particles on the photoelectric conversion element 5, that is, on the monitor screen is stopped. The device configuration downstream of the photoelectric conversion element 5 is the same as that of the second embodiment.

以上述べた第3及び第4の実施例では、回転式反射鏡
を用いたが、トナー流の方向と平行に移動するタイプの
平行移動型反射鏡であっても勿論よい。
In the third and fourth embodiments described above, the rotary reflecting mirror is used. However, it is needless to say that a parallel moving reflecting mirror of a type that moves in parallel with the direction of toner flow may be used.

また、反射鏡の形状は、第9図(a)に示すように両
面がミラー面になったものでも、同図(b),(c)に
示すように多面体外面がミラー面になったものでもよ
い。なお図中斜線部がミラー面を示す。
Further, the shape of the reflecting mirror may be a mirror having a mirror surface on both sides as shown in FIG. 9 (a), or a mirror having an outer surface of a polyhedron as shown in FIGS. 9 (b) and 9 (c). May be. Note that the hatched portion in the figure indicates the mirror surface.

以上述べた第3及び第4の実施例によれば、第1及び
第2の実施例による効果に加えて、次のような効果が得
られる。
According to the third and fourth embodiments described above, the following effects can be obtained in addition to the effects of the first and second embodiments.

第1及び第2の実施例において、粒径等の精度をより
一層高めようとすると拡大光学系の倍率を上げなければ
ならず、倍率を上げると撮像システムの時間応答が追い
つかなくなる場合が生じる。即ち、1つの荷電粉体粒子
を複数のフレーム上で把えることができなくなり、直ぐ
に画面外に出てしまうといった事態となる。これに対
し、第3及び第4の実施例では、反射鏡を用いることに
より拡大光学系の倍率を上げた場合でもすぐに画面外に
出てしまうことがなくなり、より一層精度の高い測定が
可能となる。さらに、トナー粒子の像が流れ方向に関し
て静止したものになることより、トナー粒子を長い移動
距離にわたって捉えることができ、よって多数の粒子を
鮮明に捉えることができる等のメリットがある。
In the first and second embodiments, the magnification of the magnifying optical system must be increased in order to further increase the accuracy of the particle diameter and the like. If the magnification is increased, the time response of the imaging system may not be able to keep up. That is, one charged powder particle cannot be grasped on a plurality of frames, and immediately comes out of the screen. On the other hand, in the third and fourth embodiments, even when the magnification of the magnifying optical system is increased by using the reflecting mirror, the mirror does not immediately go out of the screen, and more accurate measurement is possible. Becomes Further, since the image of the toner particles becomes stationary in the flow direction, there is an advantage that the toner particles can be captured over a long moving distance, and thus a large number of particles can be captured clearly.

〔発明の効果〕 以上詳細に説明したように、本発明によれば、荷電粉
体粒子流に電界を印加したときに変位する荷電粉体粒子
群の画情報を得、この情報に基づいて荷電粉体粒子の比
電荷を得るようにしたので、荷電粉体粒子の帯電量(比
電荷)を簡便かつ高精度に測定できる利点がある。また
レーザー光を用いる場合のような高度な技術と複雑な装
置が必要ないので、安価にかつ簡易なメインテナンスで
所望の帯電量測定が可能となる。
[Effects of the Invention] As described above in detail, according to the present invention, image information of a group of charged powder particles that is displaced when an electric field is applied to a charged powder particle flow is obtained, and charging is performed based on this information. Since the specific charge of the powder particles is obtained, there is an advantage that the charge amount (specific charge) of the charged powder particles can be measured easily and with high accuracy. In addition, since a sophisticated technique and a complicated apparatus such as those using laser light are not required, a desired charge amount can be measured at low cost and with simple maintenance.

更に、荷電粉体粒子群と拡大光学系との間に回転可能
もしくは移動可能な反射鏡を設け、該反射鏡により荷電
粉体粒子群の拡大映像をその流れ方向には静止している
如く与えるようにすることにより上述の利点に加えて、
さらに一層高精度の測定が可能になるという利点があ
る。
Further, a rotatable or movable reflecting mirror is provided between the charged powder particle group and the magnifying optical system, and an enlarged image of the charged powder particle group is given by the reflecting mirror so as to be stationary in the flow direction. By doing so, in addition to the advantages described above,
There is an advantage that measurement with even higher accuracy is possible.

【図面の簡単な説明】 第1図は本発明の第1の実施例に係る帯電量測定装置の
機能構成図、第2図は本発明の第2の実施例に係る帯電
量測定装置の機能構成図、第3図は第2図の装置の外観
構成を示す斜視図、第4図は情報処理装置における原始
データを得る手順を示すフローチャート、第5図は本発
明の第3の実施例に係る帯電量測定装置の機能構成図、
第6図はモニター画面上のトナー粒子像を示す図、第7
図は本発明の第4の実施例に係る帯電量測定装置の機能
構成図、第8図は第7図の装置の外観構成を示す斜視
図、第9図は反射鏡の例を示す図である。 1……一様流作成装置、2……電界付与装置 3……照明、4……拡大光学系 5……光電変換素子、6……物理量測定装置 7……情報処理装置、8……録画再生装置 9……画情報記憶装置、12……反射鏡
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a functional configuration diagram of a charge amount measuring device according to a first embodiment of the present invention, and FIG. 2 is a function of a charge amount measuring device according to a second embodiment of the present invention. FIG. 3 is a perspective view showing an external configuration of the apparatus shown in FIG. 2, FIG. 4 is a flowchart showing a procedure for obtaining source data in an information processing apparatus, and FIG. 5 is a view showing a third embodiment of the present invention. Functional configuration diagram of such a charge amount measurement device,
FIG. 6 is a diagram showing a toner particle image on a monitor screen, FIG.
FIG. 8 is a functional configuration diagram of a charge amount measuring device according to a fourth embodiment of the present invention, FIG. 8 is a perspective view showing an external configuration of the device of FIG. 7, and FIG. 9 is a diagram showing an example of a reflecting mirror. is there. DESCRIPTION OF SYMBOLS 1 ... Uniform flow creation apparatus, 2 ... Electric field application apparatus 3 ... Illumination, 4 ... Magnification optical system 5 ... Photoelectric conversion element, 6 ... Physical quantity measuring apparatus 7 ... Information processing apparatus, 8 ... Recording Reproduction device 9: Image information storage device, 12: Reflecting mirror

Claims (6)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】一様流速の空気流中に荷電粉体粒子を導
き、荷電粉体粒子流を作り、その流れ方向に垂直な方向
に平行電界を印加し、該電界下で変位する荷電粉体粒子
群を拡大光学系により拡大し、該拡大映像を光電変換素
子によって光電変換し画情報となし、該画情報を加工処
理することによって荷電粉体粒子の変位情報と粒径を求
め、もって荷電粉体粒子の比電荷を算出することを特徴
とする荷電粉体粒子の帯電量測定方法。
A charged powder particle is introduced into an air flow having a uniform flow velocity to form a charged powder particle flow, a parallel electric field is applied in a direction perpendicular to the flow direction, and the charged powder is displaced under the electric field. The body particle group is enlarged by an enlargement optical system, the enlarged image is photoelectrically converted by a photoelectric conversion element into image information, and the image information is processed to obtain displacement information and particle size of the charged powder particles. A method for measuring a charge amount of a charged powder particle, comprising calculating a specific charge of the charged powder particle.
【請求項2】荷電粉体粒子群と拡大光学系との間に回転
可能もしくは移動可能な反射鏡を設け、該反射鏡を荷電
粉体粒子群の流れ方向の移動に応じて回転もしくは移動
させることにより、光電変換素子上に前記流れ方向に関
しては静止している荷電粉体粒子群の拡大映像を与える
ことを特徴とする請求項1記載の方法。
2. A rotatable or movable reflecting mirror is provided between the charged powder particle group and the magnifying optical system, and the reflecting mirror is rotated or moved in accordance with the movement of the charged powder particle group in the flow direction. The method according to claim 1, wherein an enlarged image of the charged powder particle group that is stationary in the flow direction is provided on the photoelectric conversion element.
【請求項3】光電変換素子で変換した画情報を一旦画像
記録装置で記録体に記録した後、これを再生しながら上
記画情報の処理を行なうことを特徴とする請求項1又は
2記載の方法。
3. The image information according to claim 1, wherein the image information converted by the photoelectric conversion element is once recorded on a recording medium by an image recording device, and the image information is processed while reproducing the image information. Method.
【請求項4】光電変換素子で映像を撮影しながら、変換
された画情報を記憶し該情報を加工、処理し、結果を電
子情報として記憶することを特徴とする請求項1又は2
記載の方法。
4. The method according to claim 1, wherein the converted image information is stored, processed and processed, and the result is stored as electronic information while the video is captured by the photoelectric conversion element.
The described method.
【請求項5】(a)一様流速の空気流中に荷電粉体粒子
を導き、荷電粉体粒子流を作成する装置、 (b)該荷電粉体粒子流の流れ方向に垂直な方向に平行
電界を印加する装置、 (c)該電界下で偏位する荷電粉体粒子群の像を光学拡
大系により拡大し、該拡大映像を光電変換し画情報を得
る装置、 及び(d)該画情報を加工処理し荷電粉体粒子の変位情
報と粒径を求め、これらの値に基づいて荷電粉体粒子の
比電荷を算出する装置 からなることを特徴とする荷電粉体粒子の帯電量測定装
置。
5. An apparatus for producing a charged powder particle stream by introducing charged powder particles into an air stream having a uniform flow rate, and (b) in a direction perpendicular to the flow direction of the charged powder particle stream. A device for applying a parallel electric field, (c) a device for enlarging an image of a group of charged powder particles displaced under the electric field by an optical magnifying system, and photoelectrically converting the magnified image to obtain image information; A device for processing the image information to obtain displacement information and a particle size of the charged powder particles, and calculating a specific charge of the charged powder particles based on these values. measuring device.
【請求項6】荷電粉体粒子群と拡大光学系との間に、光
電変換素子上に荷電粉体粒子流の流れ方向に関しては静
止している荷電粉体粒子群の拡大映像を与えるように荷
電粉体粒子群の流れ方向の移動に応じて回転可能もしく
は移動可能な反射鏡を設けたことを特徴とする請求項5
記載の装置。
6. An enlarged image of a charged powder particle group which is stationary with respect to the flow direction of the charged powder particle flow on the photoelectric conversion element is provided between the charged powder particle group and the magnifying optical system. 6. A reflecting mirror which is rotatable or movable in accordance with the movement of the charged powder particle group in the flow direction.
The described device.
JP13033490A 1990-05-22 1990-05-22 Method and apparatus for measuring charge amount of charged powder particles Expired - Fee Related JP3259022B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13033490A JP3259022B2 (en) 1990-05-22 1990-05-22 Method and apparatus for measuring charge amount of charged powder particles

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13033490A JP3259022B2 (en) 1990-05-22 1990-05-22 Method and apparatus for measuring charge amount of charged powder particles

Publications (2)

Publication Number Publication Date
JPH0425772A JPH0425772A (en) 1992-01-29
JP3259022B2 true JP3259022B2 (en) 2002-02-18

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Country Link
JP (1) JP3259022B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2938327B2 (en) * 1993-12-06 1999-08-23 シャープ株式会社 Measuring device for toner charge
CN105130855B (en) 2009-12-07 2018-05-25 约翰斯霍普金斯大学 Succinylated hydroxy amine derivatives and application thereof
JP5650609B2 (en) * 2011-08-15 2015-01-07 大成建設株式会社 Charge amount identification device for charged particles
CN109946531B (en) * 2019-04-19 2024-02-23 温州大学 A measuring device and method for measuring remaining power after λ-DNA neutralization
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