JPH0321074B2 - - Google Patents

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Publication number
JPH0321074B2
JPH0321074B2 JP58117431A JP11743183A JPH0321074B2 JP H0321074 B2 JPH0321074 B2 JP H0321074B2 JP 58117431 A JP58117431 A JP 58117431A JP 11743183 A JP11743183 A JP 11743183A JP H0321074 B2 JPH0321074 B2 JP H0321074B2
Authority
JP
Japan
Prior art keywords
toner particles
electric field
filter
electrode
side wall
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP58117431A
Other languages
Japanese (ja)
Other versions
JPS608759A (en
Inventor
Seiichiro Hiratsuka
Satoru Haneda
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.)
Konica Minolta Inc
Original Assignee
Konica Minolta Inc
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 Konica Minolta Inc filed Critical Konica Minolta Inc
Priority to JP58117431A priority Critical patent/JPS608759A/en
Publication of JPS608759A publication Critical patent/JPS608759A/en
Publication of JPH0321074B2 publication Critical patent/JPH0321074B2/ja
Granted legal-status Critical Current

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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、略一様強度の電界及び該電界中を流
れる略一様速度の空気流をハウジングの内部室内
に生じさせると共に、該内部室にトナー粒子を導
入し該トナー粒子の荷電分布を測定するトナー粒
子の荷電分布測定装置に関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) The present invention produces an electric field of substantially uniform strength and an air flow of substantially uniform velocity flowing through the electric field in an internal chamber of a housing, and The present invention relates to a toner particle charge distribution measuring device for introducing toner particles into a toner particle and measuring the charge distribution of the toner particles.

(従来技術) 第1図はこの種の装置の主要部を示す構成図で
ある。図中、1は吸込管で、中間部が絞られたガ
ラス管でなり、且つその内面は酸化錫で被覆さ
れ、該酸化錫は接地されている。この吸込管1の
開口部の周辺には、環状のエアフイルター材2が
配設され、空気が吸込管1に周囲から流入可能と
なつている。該エアフイルター材2は吸込管1に
矢印方向に入つてくるトナー粒子(サンプル)を
同軸的に取巻く空気層を形成するためのもので、
圧縮空気流入路15からの空気に対し適度な空気
抵抗を示すと共に、ゴミ等を除去する多孔性で、
しかも孔の周囲は導電性でなる部材である。3は
主空気流をハウジング4の内部室5内に導入する
ためのナイロンフイルターで、この主空気流は、
その後、ナイロンのメツシユスクリーン6、蜂の
巣形直線気流形成器7、ナイロンフイルター8及
び9を通過し、略平坦な流速分布で且つ吸込管1
からの流出空気と略同一の流速となつて第1図の
下方に流れる。10は偏向用の側壁電極で、ハウ
ジング4のガラス壁面に被覆された多数の略長方
形状酸化錫でなる。該側壁電極10には、ハウジ
ング4の内部室5内に一様な電界が形成されるよ
うに、相異なる電圧が与えられている。11は略
等間隔の電線とこれに直角方向の略等間隔のナイ
ロン系とから構成された通気性を有する格子状の
底部電極で、フイルター12の下流側に配設さ
れ、フイルター12に補集されたそこに付着した
粒子パターンを歪ませないように、滑らかな電位
傾斜を形成するものである。該底部電極11に対
する抵抗は、格子の1端縁をコロイド状グラフア
イトと二硫化モリブデンとのスラリで被覆して、
端から端までの抵抗値が例えば20MΩの塗布抵抗
を作ることによつて形成される。この底部電極1
1は、台部13に取付けられたガラスフリツトフ
イルター14によつて支持されている。
(Prior Art) FIG. 1 is a block diagram showing the main parts of this type of device. In the figure, reference numeral 1 denotes a suction pipe, which is a glass tube with a constricted middle portion, and whose inner surface is coated with tin oxide, which is grounded. An annular air filter material 2 is disposed around the opening of the suction pipe 1 so that air can flow into the suction pipe 1 from the surrounding area. The air filter material 2 is for forming an air layer coaxially surrounding the toner particles (sample) entering the suction pipe 1 in the direction of the arrow.
It exhibits appropriate air resistance against the air from the compressed air inflow path 15, and is porous to remove dust and the like.
Moreover, the area around the hole is a conductive member. 3 is a nylon filter for introducing the main air flow into the internal chamber 5 of the housing 4;
After that, it passes through a nylon mesh screen 6, a honeycomb-shaped straight air flow generator 7, and nylon filters 8 and 9, with a substantially flat flow velocity distribution and a suction pipe 1.
The air flows downward in FIG. 1 at approximately the same flow velocity as the air flowing out from the air. Reference numeral 10 denotes a side wall electrode for deflection, which is made of a large number of approximately rectangular tin oxide coated on the glass wall surface of the housing 4. Different voltages are applied to the side wall electrodes 10 so that a uniform electric field is formed within the interior chamber 5 of the housing 4. Reference numeral 11 denotes a grid-like bottom electrode having air permeability, which is composed of electrical wires arranged at approximately equal intervals and nylon wires arranged at approximately equal intervals in a direction perpendicular to the electrical wires. This creates a smooth potential gradient so as not to distort the particle pattern attached thereto. The resistance to the bottom electrode 11 is provided by coating one edge of the grid with a slurry of colloidal graphite and molybdenum disulfide.
It is formed by creating a coated resistor with an end-to-end resistance value of, for example, 20 MΩ. This bottom electrode 1
1 is supported by a glass frit filter 14 attached to a base 13.

この装置において、トナー粒子は、トナー粒子
の導入手段によつて吸込管1を通つてハウジング
4の内部室5内に導かれ、降下しながら電極10
及び11によつて吸込管1の中心軸と直角の方向
(電界の方向)に偏向され、トナー付着検出用の
フイルター12上に付着する。この偏向方向の変
位量は、トナー粒子の大きさ及び電荷の関数にな
つている。
In this device, toner particles are introduced into an internal chamber 5 of a housing 4 through a suction pipe 1 by a toner particle introducing means, and while falling, the toner particles are introduced into an electrode 10.
and 11 in a direction perpendicular to the central axis of the suction pipe 1 (the direction of the electric field), and is deposited on a filter 12 for detecting toner adhesion. The amount of displacement in the deflection direction is a function of the size and charge of the toner particles.

ところで、上述の如く一様電界を形成するのに
側壁電極及び底部電極を用いた従来装置において
は、底部電極の構造が複雑であり製作が面倒であ
ると共に高価な材料を必要とするため、装置のコ
ストが高くなるという問題がある。又、格子構造
といえども、現実には上流側のフイルターの空気
流を乱すという問題がある。
By the way, in the conventional device using the side wall electrode and the bottom electrode to form a uniform electric field as described above, the bottom electrode has a complicated structure, is troublesome to manufacture, and requires expensive materials. The problem is that the cost is high. Furthermore, even with a lattice structure, there is a problem in that it actually disturbs the airflow of the upstream filter.

(発明の目的) 本発明は、このような問題に鑑みてなされたも
ので、その目的は、一様な強度の電界を形成する
電極を簡単な構造で且つ空気流を乱さない電極配
置で得ることにある。
(Objective of the Invention) The present invention was made in view of the above problems, and its object is to obtain an electrode that forms an electric field of uniform strength with a simple structure and an electrode arrangement that does not disturb airflow. There is a particular thing.

(発明の構成) この目的を達成する本発明は、略一様強度の電
界及び該電界中を流れる略一様速度の空気流をハ
ウジングの内部室内に生じさせると共に、該内部
室にトナー粒子を導入し該トナー粒子の荷電分布
を測定するトナー粒子の荷電分布測定装置におい
て、前記略一様強度の電界を形成する側壁電極
を、トナー粒子を補集するフイルターの上流側だ
けでなく下流側にも配設したことを特徴とするも
のである。
SUMMARY OF THE INVENTION The present invention achieves this object by creating an electric field of substantially uniform strength and an air flow of substantially uniform velocity flowing through the electric field in an internal chamber of a housing, and disposing toner particles in the internal chamber. In a toner particle charge distribution measuring device that measures the charge distribution of toner particles, the side wall electrode that forms the electric field of substantially uniform strength is provided not only on the upstream side but also on the downstream side of the filter that collects the toner particles. It is also characterized by the fact that it is also provided with.

(実施例) 以下、図面を用いて本発明を詳細に説明する。(Example) Hereinafter, the present invention will be explained in detail using the drawings.

第2図は本発明の一実施例の要部を示す構成図
である。この図において第1図と同一部分には同
一符号を付した。図中、20はフイルター12の
下流側の管部内壁に設けられた側壁電極で、フイ
ルター12の上流側の側壁電極10をフイルター
12の下流側に延長したような形で配設され、側
壁電極10と同様、ガラス管部壁面に被覆された
略長方形状の酸化錫の膜で構成され且つ同様の電
圧が印加される。この側壁電極20の長さ(管軸
方向)は、管径の1/2以上に選ぶことが好ましい。
FIG. 2 is a configuration diagram showing a main part of an embodiment of the present invention. In this figure, the same parts as in FIG. 1 are given the same reference numerals. In the figure, 20 is a side wall electrode provided on the inner wall of the tube on the downstream side of the filter 12. The side wall electrode 20 is arranged in such a manner that the side wall electrode 10 on the upstream side of the filter 12 is extended to the downstream side of the filter 12. Like No. 10, it is composed of a substantially rectangular tin oxide film coated on the wall surface of the glass tube part, and the same voltage is applied. The length of this side wall electrode 20 (in the tube axis direction) is preferably selected to be 1/2 or more of the tube diameter.

このように構成すれば、側壁電極10及び20
の協働により、フイルター12部分においても一
様な電界が生じるので、従来装置における底部電
極が不要になり、フイルター12付近での空気流
の乱れが無くなる。このため、高積層の測定が可
能になる。又、底部電極が不要になることで、そ
の材料及び製作工程が不要になり、装置の低コス
ト化を図れる。
With this configuration, the side wall electrodes 10 and 20
As a result of the cooperation of the above, a uniform electric field is generated even in the filter 12 portion, so the bottom electrode in the conventional device is not required, and the air flow in the vicinity of the filter 12 is no longer disturbed. This makes it possible to measure highly stacked layers. Further, since the bottom electrode is not required, the material and manufacturing process thereof are also eliminated, and the cost of the device can be reduced.

尚、上記実施例においては、側壁電極10,2
0を酸化錫膜で形成したものを示したが、他の導
電性金属膜を使用してもよいし、金属板を空気流
の流れを乱さないように貼付けてもよい。又、第
2図に示した発明部分以外の構成は、第1図と同
様であるが、必ずしもそれに限定するものではな
い。
Incidentally, in the above embodiment, the side wall electrodes 10, 2
Although 0 is shown as being formed of a tin oxide film, other conductive metal films may be used, or a metal plate may be attached so as not to disturb the air flow. Further, the configuration other than the inventive portion shown in FIG. 2 is the same as that in FIG. 1, but is not necessarily limited thereto.

(発明の効果) 以上説明したように、本発明によれば、一様強
度の電界を簡単な電極構造で得ることができる。
又、この電極によればトナー粒子を補集するフイ
ルター部分の空気流が乱れることもない。
(Effects of the Invention) As explained above, according to the present invention, an electric field of uniform strength can be obtained with a simple electrode structure.
Furthermore, with this electrode, the air flow in the filter portion that collects toner particles is not disturbed.

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

第1図は従来のトナー粒子の荷電分布測定装置
を示す構成図、第2図は本発明の一実施例の要部
を示す構成図である。 1……吸込管、2……エアフイルター材、4…
…ハウジング、5……内部室、10……上流側の
側壁電極、12……フイルター、15……圧縮空
気流入路、20……下流側の側壁電極。
FIG. 1 is a block diagram showing a conventional toner particle charge distribution measuring device, and FIG. 2 is a block diagram showing a main part of an embodiment of the present invention. 1...Suction pipe, 2...Air filter material, 4...
... Housing, 5 ... Internal chamber, 10 ... Upstream side wall electrode, 12 ... Filter, 15 ... Compressed air inlet path, 20 ... Downstream side wall electrode.

Claims (1)

【特許請求の範囲】[Claims] 1 略一様強度の電界及び該電界中を流れる略一
様速度の空気流をハウジングの内部室内に生じさ
せると共に、該内部室にトナー粒子を導入し該ト
ナー粒子の荷電分布を測定するトナー粒子の荷電
分布測定装置において、前記略一様強度の電界を
形成する側壁電極を、トナー粒子を補集するフイ
ルターの上流側だけでなく下流側にも配設したこ
とを特徴とするトナー粒子の荷電分布測定装置。
1. Toner particles that generate an electric field of substantially uniform strength and an air flow of substantially uniform velocity flowing through the electric field in the internal chamber of the housing, introduce toner particles into the internal chamber, and measure the charge distribution of the toner particles. charge distribution measuring device, characterized in that the side wall electrode that forms the electric field of substantially uniform strength is disposed not only on the upstream side of the filter that collects the toner particles but also on the downstream side of the filter. Distribution measuring device.
JP58117431A 1983-06-29 1983-06-29 Measuring device of electric charge distribution of toner particle Granted JPS608759A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58117431A JPS608759A (en) 1983-06-29 1983-06-29 Measuring device of electric charge distribution of toner particle

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58117431A JPS608759A (en) 1983-06-29 1983-06-29 Measuring device of electric charge distribution of toner particle

Publications (2)

Publication Number Publication Date
JPS608759A JPS608759A (en) 1985-01-17
JPH0321074B2 true JPH0321074B2 (en) 1991-03-20

Family

ID=14711473

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58117431A Granted JPS608759A (en) 1983-06-29 1983-06-29 Measuring device of electric charge distribution of toner particle

Country Status (1)

Country Link
JP (1) JPS608759A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61281975A (en) * 1985-06-07 1986-12-12 Fujitsu Ltd Measuring instrument for distribution of toner electric charge quantity
JPS63175689A (en) * 1987-01-12 1988-07-20 Nippon Denki Kankyo Eng Kk Treatment method for wastewater containing amine compounds

Also Published As

Publication number Publication date
JPS608759A (en) 1985-01-17

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