JPH03105265A - Measuring apparatus of amount of electrification of toner - Google Patents

Measuring apparatus of amount of electrification of toner

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Publication number
JPH03105265A
JPH03105265A JP24179289A JP24179289A JPH03105265A JP H03105265 A JPH03105265 A JP H03105265A JP 24179289 A JP24179289 A JP 24179289A JP 24179289 A JP24179289 A JP 24179289A JP H03105265 A JPH03105265 A JP H03105265A
Authority
JP
Japan
Prior art keywords
toner
faraday cage
pressure gas
gas
charge
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
JP24179289A
Other languages
Japanese (ja)
Inventor
Hideaki Iwasaki
岩崎 秀昭
Masahiro Wano
和納 正弘
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP24179289A priority Critical patent/JPH03105265A/en
Publication of JPH03105265A publication Critical patent/JPH03105265A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To measure the amount of electrification of toner quickly and accurately by producing a gas flow from a gas producing means so as to prevent the toner from sticking to a Faraday cage when a prescribed amount of binary developer is put in the cage and discharged together with a high-pressure gas. CONSTITUTION:A gas producing means 16 is provided so as to prevent toner T from sticking to a Faraday cage 10 when the toner T is discharged from the cage 10 together with a high-pressure gas. The means 16 is constructed of an air gun 16a, and a pipe 16b for supply, which is connected to a high- pressure nitrogen gas source not shown in the figure, is connected thereto. When the toner T is discharged from the cage 10 together with the high-pressure gas, a high-pressure gas jet wave B is generated in the direction perpendicular substantially to the direction of discharge of the toner T so that it comes into contact with the annular lower surface of a fixation fitting 10c, and thereby the toner T sticking on the annular lower surface is removed. According to this constitution, the development, design, maintenance and control of an electrophotographic recording apparatus are facilitated very much.

Description

【発明の詳細な説明】 〔概 要〕 電子写真記録装置等の現像プロセスで用いられる二或分
現像剤、すなわち磁性体キャリヤとトナーとからなる二
或分現像剤のうちの現像剤成分を威すトナーの帯電量を
測定するトナー帯電量測定装置に関し、 ブローオフ法を導入したトナー帯電量測定装置であって
、ファラデーケージへのトナー付着を阻止して測定を正
確かつ迅速に達或し得るトナー帯電量測定装置を提供す
ることを目的とし、ファラデーケージに所定量の二成分
現像剤を導入し、ファラデーケージに高圧をガスを吹き
込んで二成分現像剤のうちのトナーをファラデーケージ
から高圧ガスと共に排出させ、ファラデーケージ内に残
された二或分現像剤のうちの磁性体キャリヤの電荷をフ
ァラデーケージを介して抽出して測定するトナー帯電量
測定装置において、ファラデーケージから高圧ガスと共
にトナーを排出させる際にファラデーケージへのトナー
の付着を阻止するように気体流を発生させる気体流発生
手段が設けられることを特徴とするトナー帯電量測定装
置を構或する。
[Detailed Description of the Invention] [Summary] A two-part developer used in the development process of electrophotographic recording devices, that is, a developer component of a two-part developer consisting of a magnetic carrier and a toner. The present invention relates to a toner charge amount measuring device that measures the amount of charge on a toner, and is a toner charge amount measuring device that incorporates a blow-off method, which can prevent toner from adhering to a Faraday cage and achieve accurate and quick measurement. The purpose of this device is to introduce a predetermined amount of two-component developer into a Faraday cage, blow high-pressure gas into the Faraday cage, and remove toner from the two-component developer from the Faraday cage together with the high-pressure gas. In a toner charge measurement device that extracts and measures the charge of the magnetic carrier of the two-part developer left in the Faraday cage through the Faraday cage, the toner is discharged from the Faraday cage along with high-pressure gas. A toner charge amount measuring device is provided with a gas flow generating means for generating a gas flow so as to prevent toner from adhering to a Faraday cage when the toner is charged.

〔産業上の利用分野) 本発明は電子写真記録装置等の現像プロセスで用いられ
る二成分現像剤、すなわち磁性体キャリヤとトナーとか
らなる二成分現像剤のうちの現像剤或分を威すトナーの
帯電量を測定するトナー帯電量測定装置に関する。
[Industrial Application Field] The present invention relates to a two-component developer used in the development process of an electrophotographic recording device, that is, a toner that uses a certain amount of the developer in the two-component developer consisting of a magnetic carrier and a toner. The present invention relates to a toner charge amount measuring device that measures the amount of charge on a toner.

電子写真記録装置では、現像プロセスは記録画像の画質
に大きな影響を与える重要なプロセスのlつであり、こ
の現像プロセスにおいて、トナーの帯電量は記録画像の
画質を左右する最も基本的なパラメータである。このた
め電子写真記録装置の開発、設計およびその維持管理に
おいては、トナーの帯電量を正確に把握することが必要
であり、トナーの帯電量を正確かつ迅速に測定すること
が求められている。
In electrophotographic recording devices, the development process is one of the important processes that greatly affects the quality of recorded images.In this development process, the amount of charge on the toner is the most fundamental parameter that affects the quality of recorded images. be. Therefore, in the development, design, and maintenance of electrophotographic recording devices, it is necessary to accurately grasp the amount of charge on the toner, and there is a need to accurately and quickly measure the amount of charge on the toner.

〔従来の技術〕[Conventional technology]

従来のトナー帯電量測定法の1つとして、ブローオフ法
が知られており、このブローオフ法では、所定量の二成
分現像剤に高圧ガス(例えば窒素ガス)を吹き付けて、
そこから粒径の小さなしかも軽量なトナーを吹き飛ばし
、次いでトナーと等価でしかも逆極性の電荷を持つ磁性
体キャリヤの帯電量を測定し、続いて磁性体キャリヤの
全質量を測定する。当初の二成分現像剤の全質量は既知
であるから、そこから磁性体キャリヤの全質量を差し引
くことによって、吹き飛ばされたトナーの全質量を知る
ことができる。したがって、磁性体キャリヤの帯電量を
トナーの全質量で割ることによって、単位質量当たりの
トナーの帯電量が測定されることになる。
The blow-off method is known as one of the conventional toner charge amount measurement methods. In this blow-off method, high pressure gas (for example, nitrogen gas) is blown onto a predetermined amount of two-component developer.
The toner, which is small in size and lightweight, is blown away, and then the amount of charge on the magnetic carrier, which has a charge equivalent to that of the toner and opposite in polarity, is measured, and then the total mass of the magnetic carrier is measured. Since the total mass of the original two-component developer is known, the total mass of blown toner can be determined by subtracting the total mass of the magnetic carrier from it. Therefore, by dividing the amount of charge on the magnetic carrier by the total mass of the toner, the amount of charge on the toner per unit mass is measured.

第5図を参照すると、上述のブローオフ法を導入した従
来のトナー帯電量測定装置が概略的に示され、このトナ
ー帯電量測定装置はファラデーケージ10を具備する。
Referring to FIG. 5, a conventional toner charge amount measuring device incorporating the above-described blow-off method is schematically shown, and this toner charge amount measuring device is equipped with a Faraday cage 10. As shown in FIG.

ファラデーケージ10は逆漏斗状の形態を持つ金属製ケ
ーシング10aと、この金属製ケーシング10aの下側
開口部に適用された金属製メッシュ10bと、この金属
製メッシュ10bの固定具10cとからなる。また、ト
ナー帯電量測定装置は予め既知の容量を持つコンデンサ
12を具備し、このコンデンサl2の一端側はファラデ
ーケージ10の金属製ケーシング12aに接続され、そ
の他端側は接地される。更に、トナー帯電量測定装置は
電位差計l4を具備し、この電位差計14はコンデンサ
12の両端側に接続されてその間の電位を測定し得るよ
うになっている。
The Faraday cage 10 includes a metal casing 10a having an inverted funnel shape, a metal mesh 10b applied to the lower opening of the metal casing 10a, and a fixture 10c for the metal mesh 10b. Further, the toner charge amount measuring device includes a capacitor 12 having a previously known capacity, one end of the capacitor l2 is connected to the metal casing 12a of the Faraday cage 10, and the other end is grounded. Furthermore, the toner charge amount measuring device is equipped with a potentiometer 14, which is connected to both ends of the capacitor 12 so as to be able to measure the potential therebetween.

第6図を参照すると、磁性体キャリヤCとトナーTとが
二或分現像剤中に存在する状態で示されている。すなわ
ち、、磁性体キャリヤCとトナーTとは二或分現像剤中
で互いに摩擦して逆極性の電荷を帯び、しかも磁性体キ
ャリヤCの粒径はトナーTの粒径よりも遥かに大きいの
で、トナーTは磁性体キャリヤCの周囲に静電的に付着
した状態となっている。このとき磁性体キャリヤCの全
体が持つ電荷量とトナーTの全体が持つ電荷量とは互い
に等価で逆極性となっている。なお、第6図の例では、
磁性体キャリヤCが正の電荷に、またトナーTが負の電
荷に帯電されているが、磁性体キャリヤCが負の電荷に
、またトナーTが正の電荷に帯電される逆の場合もある
Referring to FIG. 6, a magnetic carrier C and a toner T are shown in two parts in a developer. That is, the magnetic carrier C and the toner T rub against each other in the developer and are charged with opposite polarities, and the particle size of the magnetic carrier C is much larger than that of the toner T. , the toner T is electrostatically attached around the magnetic carrier C. At this time, the amount of charge held by the entire magnetic carrier C and the amount of charge held by the entire toner T are equivalent to each other and have opposite polarities. In addition, in the example of Fig. 6,
Although the magnetic carrier C is charged with a positive charge and the toner T is charged with a negative charge, there is also the opposite case where the magnetic carrier C is charged with a negative charge and the toner T is charged with a positive charge. .

第5図に示した従来のトナー帯電量測定装置の作動につ
いて述べると、先ず、磁性体キャリヤCとトナーTとが
第6図に示すような状態にある二成分現像剤の所定量を
ファラデーケージ10の金属製ケーシング10a内にそ
の上側開口部から導入し、次いで,金属製ケーシング1
0aの上側開口部から高圧ガス(例えば、窒素ガス)を
該金属ケーシング10a内に吹き込む。このような高圧
ガスの吹込みによって、磁性体キャリヤCとトナーTと
が互いに作用する静電的吸着力に抗して分離されると、
トナーTは吹込み高圧ガスに同伴されて金属製メッシュ
10bを通して金属製ケーシング10aの外部に排出さ
れ、一方粒径の大きな磁性体キャリヤCは金属製ケーシ
ング10a内に残される。なお、金属製メッシュ10b
の目がトナーTの粒径よりも十分に大きく、しかも磁性
体キャリヤCの粒径よりも十分に小さいことは言うまで
もない。
To describe the operation of the conventional toner charge amount measuring device shown in FIG. 5, first, a predetermined amount of the two-component developer in which the magnetic carrier C and the toner T are in the state shown in FIG. 6 is placed in a Faraday cage. 10 into the metal casing 10a from its upper opening, and then the metal casing 1
High pressure gas (for example, nitrogen gas) is blown into the metal casing 10a from the upper opening of the metal casing 10a. When the magnetic carrier C and the toner T are separated by the blowing of such high-pressure gas against the electrostatic adsorption force acting on each other,
The toner T is entrained by the blown high-pressure gas and discharged to the outside of the metal casing 10a through the metal mesh 10b, while the magnetic carrier C having a large particle size remains inside the metal casing 10a. In addition, the metal mesh 10b
Needless to say, the diameter of the particles is sufficiently larger than the particle size of the toner T and also sufficiently smaller than the particle size of the magnetic carrier C.

磁性体キャリヤC自体は導電性であるので、金属製ケー
シング10a内に残された磁性体キャリヤCの電荷は金
属製メッシュ10bおよび金属製ケーシング10aを経
て、更に金属製ケーシング10aとコンデンサ12との
間の導電路を経てコンデンサ12に蓄えられる。コンデ
ンサ12への蓄電が飽和した時点で電位差計14の計測
値が読み取られ、これにより金属製ケーシングlOa内
に残された磁性体キャリヤCの全電荷量が測定され、こ
の全電荷量は金属製ケーシング10aから排出されたト
ナーTが持っていた逆極性の全電荷量と等価である。な
お、コンデンサ12の容量は上述したように既知である
Since the magnetic carrier C itself is conductive, the electric charge of the magnetic carrier C left in the metal casing 10a passes through the metal mesh 10b and the metal casing 10a, and is further transferred between the metal casing 10a and the capacitor 12. It is stored in the capacitor 12 via the conductive path between them. When the charge in the capacitor 12 is saturated, the measured value of the potentiometer 14 is read, and the total amount of charge on the magnetic carrier C left in the metal casing lOa is measured. This is equivalent to the total amount of charge of the opposite polarity that the toner T discharged from the casing 10a had. Note that the capacitance of the capacitor 12 is known as described above.

次いで、金属製ケーシング10aから磁性体キャリヤC
が取り出されて、その全質量が測定され、これにより金
属製ケーシング10aから排出されたトナーTの全質量
が計算されて、単位質量当たりの1・ナー帯電量が求め
られる。
Next, the magnetic carrier C is removed from the metal casing 10a.
is taken out, its total mass is measured, the total mass of the toner T discharged from the metal casing 10a is calculated, and the 1·toner charge amount per unit mass is determined.

〔発明が解決しようとする課題] ところで、第5図に示したような従来のトナー帯電!J
:/fl!J定装置においては、金属製メッシュ10b
を通して排出されたトナーTは軽量でしかも微細である
ために飛散し、その一部はファラデーケージ10に、特
にその固定具10cの環状下面に付着し得ることになる
。このような付着トナーTの幾分かは高圧ガスの吹込み
によって除去される得るが、固定具10cの環状下面に
付着したトナーTの大部分は金属製メッシュ10bを通
して吹き出される高圧ガスの影響を受けることはなく、
このため付着トナーTが固定具10cの環状下面から除
去され得ることはない, このようにファラデーケージ10にトナーTが付着する
と、上述したような磁性体キャリヤCの電荷量の迅速な
測定が阻害されるだけでなく、その測定結果の信頼性も
損なわれることになる。というのは、付着トナーTの幾
分かが除去されつつあるときには、コンデンサl2への
蓄電が終了しておらず、このためコンデンサ12が完全
に蓄電されるまでの時間が長く、このため迅速な測定の
妨げになるからであり、また除去不可能な付着トナーT
が存在する場合にはその電荷の影響を受けて測定が不完
全なものとなるからである。なお、ファラデーケージ1
0に付着したトナーTを刷毛あるいは布等で払拭して除
去することは可能ではあるが、その場合には刷毛あるい
は布等での払拭時に摩擦帯電が生じ、測定に重大な影響
を及ぼすことになるので、付着トナーTの除去のために
刷毛あるいは布等を用いることはできない。
[Problems to be Solved by the Invention] By the way, the conventional toner charging as shown in FIG. 5! J
:/fl! In the J constant device, the metal mesh 10b
Since the toner T discharged through the toner T is lightweight and fine, it scatters, and a portion of it may adhere to the Faraday cage 10, particularly to the annular lower surface of the fixture 10c. Although some of the adhered toner T can be removed by blowing high-pressure gas, most of the toner T adhered to the annular lower surface of the fixture 10c is removed by the influence of the high-pressure gas blown out through the metal mesh 10b. without receiving
Therefore, the adhered toner T cannot be removed from the annular lower surface of the fixture 10c. If the toner T adheres to the Faraday cage 10 in this way, the rapid measurement of the charge amount of the magnetic carrier C as described above is hindered. Not only that, but the reliability of the measurement results is also impaired. This is because when some of the adhered toner T is being removed, the capacitor 12 has not yet been charged with electricity, and therefore it takes a long time until the capacitor 12 is completely charged. This is because the attached toner T interferes with measurement and cannot be removed.
This is because if there is a charge, the measurement will be incomplete due to the influence of the charge. Furthermore, Faraday cage 1
Although it is possible to remove the toner T adhering to the toner by wiping it with a brush or cloth, in that case, frictional charging will occur when wiping with a brush or cloth, which will seriously affect the measurement. Therefore, it is not possible to use a brush or cloth to remove the adhered toner T.

したがって、本発明の目的はブローオフ法を導入したト
ナー帯電量測定装置であって、ファラデーケージへのト
ナー付着を阻止して測定を正確かつ迅速に達威し得るト
ナー帯電量測定装置を提供することである。
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a toner charge amount measuring device incorporating the blow-off method, which can prevent toner from adhering to a Faraday cage and achieve measurement accurately and quickly. It is.

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

本発明によるトナー帯電量測定装置では、従来の場合と
同様に、ファラデーケージに所定量の二或分現像剤を導
入し、咳ファラデーケージに高圧をガスを吹き込んで二
或分現像剤のうちのトナーを該ファラデーケージから高
圧ガスと共に排出させ、該ファラデーケージ内に残され
た二或分現像剤のうちの磁性体キャリヤの電荷を該ファ
ラデーケージを介して抽出して測定する。しかし、本発
明によるトナー帯電量測定装置においては、ファラデー
ケージから高圧ガスと共にトナーを排出させる際に該フ
ァラデーケージへの該トナーの付着を阻止するように気
体流を発生させる気体流発生手段が設けられる点が特徴
とされる。
In the toner charge amount measuring device according to the present invention, as in the conventional case, a predetermined amount of two-part developer is introduced into the Faraday cage, and gas is blown into the Faraday cage under high pressure to remove the part of the two-part developer. The toner is discharged from the Faraday cage with a high pressure gas, and the charge on the magnetic carrier of the two-part developer remaining in the Faraday cage is extracted through the Faraday cage and measured. However, in the toner charge amount measuring device according to the present invention, a gas flow generating means is provided for generating a gas flow so as to prevent the toner from adhering to the Faraday cage when the toner is discharged from the Faraday cage together with the high-pressure gas. It is characterized by the fact that

〔作 用〕[For production]

本発明によるトナー帯電量測定装置にあっては、気体流
発生手段から気体流が発生させられ、この気体流によっ
て、ファラデーケージから高圧ガスと共にトナーを排出
させる際に該ファラデーケージへの該トナーの付着が阻
止されることになる。
In the toner charge amount measuring device according to the present invention, a gas flow is generated from the gas flow generating means, and when the toner is discharged from the Faraday cage together with the high pressure gas, the toner is transferred to the Faraday cage. Adhesion will be prevented.

〔実施例〕〔Example〕

次に、添付図面の第1図ないし第4図を参照して、本発
明によるトナー帯電量測定装置の実施例について説明す
る。
Next, an embodiment of the toner charge amount measuring device according to the present invention will be described with reference to FIGS. 1 to 4 of the accompanying drawings.

先ず、第1図を参照すると、本発明によるトナー帯電量
測定装置の一実施例が示され、その構成要素の多くは第
5図に示したものと実質的に同じものである。したがっ
て、第1図では、第5図に示したトナー帯電量測定装置
の構或要素と同様な構成要素については同じ参照番号お
よび参照記号が用いられ、それら構或要素の説明につい
ては第5図の説明を援用することにする。
First, referring to FIG. 1, one embodiment of a toner charge amount measuring device according to the present invention is shown, and many of its components are substantially the same as those shown in FIG. Therefore, in FIG. 1, the same reference numerals and symbols are used for the same components as those of the toner charge amount measuring device shown in FIG. I will refer to the explanation of

第1図に示すトナー帯電量測定装置には、ファラデーケ
ージlOから高圧ガスと共にトナーTを排出させた際に
該ファラデーケージIOへのトナーTの付着を阻止する
ための気体流発生手段l6が設けられる。本実施例では
、気体流発生手段16はエアガン16aからなり、この
エアガン16aからは高圧ガス給送用バイブ16bが延
びて適当な高圧ガス源(図示されない)に接続される。
The toner charge amount measuring device shown in FIG. 1 is provided with a gas flow generating means 16 for preventing the toner T from adhering to the Faraday cage IO when the toner T is discharged from the Faraday cage IO together with high-pressure gas. It will be done. In this embodiment, the gas flow generating means 16 comprises an air gun 16a, and a high-pressure gas supplying vibrator 16b extends from the air gun 16a and is connected to a suitable high-pressure gas source (not shown).

なお、かかる高圧ガス源は例えば高圧窒素ガス源であっ
てよい。第1図に示すように、エアガン16aはファラ
デーケージ10から高圧ガスと共にトナーTを排出させ
る際のトナーTの排出方向に対してほぼ直角方向に高圧
ガス噴射流Bを発生させるように配置され、このとき高
圧ガス噴射流Bが固定具10cの環状下面に接触するよ
うにされ、これにより固定具10cの環状下面に付着し
たトナーTは第1図に示すように除去され得ることにな
る。
Note that such a high-pressure gas source may be, for example, a high-pressure nitrogen gas source. As shown in FIG. 1, the air gun 16a is arranged to generate a high-pressure gas jet flow B in a direction substantially perpendicular to the direction in which the toner T is discharged from the Faraday cage 10 together with the high-pressure gas; At this time, the high-pressure gas jet stream B is brought into contact with the annular lower surface of the fixture 10c, so that the toner T adhering to the annular lower surface of the fixture 10c can be removed as shown in FIG.

固定具10cの環状下面の直径はほぼ30m+程度であ
り、そのような寸法の環状下面から一気にトナーTを除
去するためにエアガン16aの高圧ジェット噴射口を3
0[111以上の幅広とすることが好ましい。しかしな
がら、エアガン16aの高圧ジェット噴射口を小さくし
てビーム状の高圧ジェット噴射流を形或するようにして
もよく、この場合には、エアガン16aを固定具10c
の環状周囲壁に対して接線方向に移動し得るようにする
か、あるいはエアガン16aを垂直軸線の回りで回動さ
せ得るようにすれば、かかるビーム状の高圧ジェット噴
射流によっても固定具10cの環状下面の全面からトナ
ーTを除去することが可能である。
The diameter of the annular lower surface of the fixture 10c is approximately 30 m+, and in order to remove the toner T at once from the annular lower surface of such size, the high-pressure jet nozzle of the air gun 16a is
It is preferable that the width is 0[111 or more. However, the high-pressure jet nozzle of the air gun 16a may be made smaller to form a beam-like high-pressure jet flow, and in this case, the air gun 16a may be attached to the fixture 10c.
If the air gun 16a can be moved tangentially with respect to the annular surrounding wall of the fixture 10c, or the air gun 16a can be rotated about a vertical axis, such a beam-shaped high-pressure jet stream can also cause the fixture 10c to It is possible to remove the toner T from the entire surface of the annular lower surface.

第1図に示したようなトナー帯電量測定装置において、
二或分現像剤のトナー帯電量についての測定が以下に示
すような条件下で実際に行われた。
In the toner charge amount measuring device as shown in Fig. 1,
Measurements of the toner charge amount of the two-part developer were actually carried out under the conditions shown below.

(1)  試料     :0.8g(キャリヤの平均
粒径iooμ鋼、トナーの平均粒径10μ)(2)金属
製メッシュ:500メッシュ(3)吹込み高圧ガス: 
0.8 kg/cd(4)  ジェット噴射流: 1.
5 kg/cd試料(二成分現像剤)0.8gをファラ
デーケージの金属製ケーシング10a内に導入して、約
40秒に亘っての高圧ガス(0 . 8 kg / a
ll )を金属製ケーシング10a内に吹き込み、その
間エアガンl6aからジェット噴射流(1.5kg/c
4)を噴出させた。
(1) Sample: 0.8 g (carrier average particle size iooμ steel, toner average particle size 10μ) (2) Metal mesh: 500 mesh (3) Blowing high pressure gas:
0.8 kg/cd (4) Jet flow: 1.
0.8 g of a 5 kg/cd sample (two-component developer) was introduced into the metal casing 10a of the Faraday cage, and high pressure gas (0.8 kg/a) was applied for about 40 seconds.
ll) into the metal casing 10a, while a jet stream (1.5 kg/c
4) was ejected.

比較のために、エアガン16aを作動させない点を除い
てその他は同一条件で同様な測定を行った。
For comparison, similar measurements were conducted under the same conditions except that the air gun 16a was not activated.

測定結果は第2図に示す通りである。同図において、特
性曲線aは本発明による場合、特性曲線bは比較例(従
来)の場合である。特性曲線aから明らかなように、本
発明によれば、高圧ガス吹込み開始時から約14秒後に
はコンデンサl2への蓄電は終了するが、比較例の場合
(特性曲線b)にはコンデンサ12への蓄電が終了する
まで、高圧ガス吹込み開始時から約40秒程掛かる。こ
れは明らかにファラデーケージ10に付着したトナーに
よる影響である。コンデンサl2への蓄電の完了時での
特性曲線aと特性曲線bとの間の差は比較例の場合の測
定の不正確さを示している。
The measurement results are shown in FIG. In the figure, characteristic curve a is the case according to the present invention, and characteristic curve b is the case according to the comparative example (conventional). As is clear from the characteristic curve a, according to the present invention, the storage of electricity in the capacitor 12 ends approximately 14 seconds after the start of high-pressure gas injection, but in the case of the comparative example (characteristic curve b), the storage of electricity in the capacitor 12 ends. It takes about 40 seconds from the start of high pressure gas injection until the electricity storage is completed. This is clearly an effect of toner adhering to the Faraday cage 10. The difference between characteristic curve a and characteristic curve b at the end of charging capacitor l2 shows the inaccuracy of the measurement in the case of the comparative example.

第3図を参照すると、この実施例では、気体流発生手段
16として吸引器16cが用いられ、この吸引器16c
は漏斗状の形態を有する。第3図から明らかなように、
吸引器16cの開口部はファラデーケージ10の下側面
よりも大きく、その下側面を受け入れるように配置され
る。吸引器16cは適当な真空装置例えば吸引ポンプ(
図示されない)に接続され、これによりファラデーケー
ジ10から高圧ガスと共にトナーTを排出させる際のト
ナーTの排出方向とほぼ同じ方向に沿う吸引気体流が発
生させられる。したがって、ファラデーケージ10から
排出される高圧ガスおよびトナーTは吸引器16c内に
引き込まれ、その結果ファラデーケージlOへのトナー
Tの付着が阻止されることになる。
Referring to FIG. 3, in this embodiment, a suction device 16c is used as the gas flow generating means 16, and this suction device 16c
has a funnel-shaped morphology. As is clear from Figure 3,
The opening of the suction device 16c is larger than the lower surface of the Faraday cage 10 and is arranged to receive the lower surface. The suction device 16c is a suitable vacuum device such as a suction pump (
(not shown), thereby generating a suction gas flow along substantially the same direction as the discharge direction of the toner T when the toner T is discharged from the Faraday cage 10 together with the high-pressure gas. Therefore, the high pressure gas and toner T discharged from the Faraday cage 10 are drawn into the suction device 16c, and as a result, the toner T is prevented from adhering to the Faraday cage IO.

第4図を参照すると、第3図に示した実施例の変形例が
示され、ここで用いられる吸引器160′は第3図に示
されるものよりも小型にされ、その開口部の直径は固定
具10cの半径方向幅よりも幾分大きい程度される。吸
引器160′も第3図の場合と同様に適当な真空装置例
えば吸引ポンプ(図示されない)に接続され、これによ
りファラデーケージ10から高圧ガスと共にトナーTを
排出させる際のトナーTの排出方向とほぼ同じ方向に沿
う吸引気体流が発生させられる。吸引器160′は第3
図の場合とは異なって固定具10cの環状下面に沿って
移動され、これにより該環状下面から付着トナーTを真
空掃除機と同様な態様で除去することになる。
Referring to FIG. 4, a variation of the embodiment shown in FIG. 3 is shown in which the aspirator 160' used is smaller than that shown in FIG. The width is somewhat larger than the radial width of the fixture 10c. The suction device 160' is also connected to a suitable vacuum device, such as a suction pump (not shown), as in the case of FIG. A suction gas flow is generated along approximately the same direction. The suction device 160' is the third
Unlike the case shown, it is moved along the annular lower surface of the fixture 10c, thereby removing the adhered toner T from the annular lower surface in a manner similar to a vacuum cleaner.

なお、上述の実施例では、ファラデーケージ内に残され
た磁性体キャリヤの電荷を測定するためにコンデンサお
よび電位差計が用いられたが、該電荷を検流計等でも測
定し得ることは言うまでもない。
In the above embodiment, a capacitor and a potentiometer were used to measure the charge of the magnetic carrier left in the Faraday cage, but it goes without saying that the charge can also be measured with a galvanometer, etc. .

〔発明の効果] 以上の記載から明らかなように、本発明によるトナー帯
電量測定装置においては、ファラデーケージへのトナー
の付着が阻止されるので、トナー帯電量の測定を迅速か
つ正確に行うことが可能となり、その結果電子写真記録
装置の開発、設計およびその維持管理に寄与し得る。
[Effects of the Invention] As is clear from the above description, in the toner charge amount measuring device according to the present invention, since toner is prevented from adhering to the Faraday cage, the toner charge amount can be measured quickly and accurately. This makes it possible to contribute to the development, design, and maintenance of electrophotographic recording devices.

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

第l図は本発明によるトナー帯電量測定装置の一実施例
を示す概略断面図、第2図は第1図に示したようなトナ
ー帯電量測定装置によってトナー帯電量の測定を行った
際の測定結果を示すグラフ、第3図は本発明によるトナ
ー帯電量測定装置の別の実施例を示す概略断面図、第4
図は第3図の実施例の変形例を示す概略断面図、第5図
は従来のトナー帯電量測定装置の概略断面図、第6図は
二成分現像剤中に存在する磁性体キャリヤとトナーとと
の状態を示す図式図である。 10・・・ファラデーケージ、10a・・・金属製ケー
シング、10b・・・金属製メッシュ、10c・・・固
定具、12・・・コンデンサ、l4・・・電位差針、1
6・・・気体流発生手段、16a・・・エアガン、16
c・160′・・・吸引器。
FIG. 1 is a schematic cross-sectional view showing an embodiment of the toner charge amount measuring device according to the present invention, and FIG. Graph showing measurement results; FIG. 3 is a schematic sectional view showing another embodiment of the toner charge amount measuring device according to the present invention; FIG.
The figure is a schematic sectional view showing a modification of the embodiment shown in FIG. 3, FIG. 5 is a schematic sectional view of a conventional toner charge amount measuring device, and FIG. 6 shows the magnetic carrier and toner present in the two-component developer It is a schematic diagram showing the state of and. DESCRIPTION OF SYMBOLS 10... Faraday cage, 10a... Metal casing, 10b... Metal mesh, 10c... Fixture, 12... Capacitor, l4... Potentiometric needle, 1
6... Gas flow generating means, 16a... Air gun, 16
c・160'...Suction device.

Claims (1)

【特許請求の範囲】 1、ファラデーケージ(10)に所定量の二成分現像剤
を導入し、該ファラデーケージに高圧をガスを吹き込ん
で二成分現像剤のうちのトナー(T)を該ファラデーケ
ージから高圧ガス(A)と共に排出させ、該ファラデー
ケージ内に残された二成分現像剤のうちの磁性体キャリ
ヤ(C)の電荷を該ファラデーケージを介して抽出して
測定するトナー帯電量測定装置において、 前記ファラデーケージから高圧ガスと共にトナーを排出
させた際に該ファラデーケージへの該トナーの付着を阻
止するように気体流を発生させる気体流発生手段(16
)が設けられることを特徴とするトナー帯電量測定装置
[Claims] 1. A predetermined amount of two-component developer is introduced into a Faraday cage (10), and a high pressure gas is blown into the Faraday cage to transfer the toner (T) of the two-component developer to the Faraday cage. A toner charge amount measuring device that extracts and measures the electric charge of a magnetic carrier (C) of the two-component developer left in the Faraday cage through the Faraday cage. , a gas flow generating means (16) for generating a gas flow so as to prevent the toner from adhering to the Faraday cage when the toner is discharged from the Faraday cage together with the high-pressure gas;
) A toner charge amount measuring device.
JP24179289A 1989-09-20 1989-09-20 Measuring apparatus of amount of electrification of toner Pending JPH03105265A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24179289A JPH03105265A (en) 1989-09-20 1989-09-20 Measuring apparatus of amount of electrification of toner

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24179289A JPH03105265A (en) 1989-09-20 1989-09-20 Measuring apparatus of amount of electrification of toner

Publications (1)

Publication Number Publication Date
JPH03105265A true JPH03105265A (en) 1991-05-02

Family

ID=17079586

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24179289A Pending JPH03105265A (en) 1989-09-20 1989-09-20 Measuring apparatus of amount of electrification of toner

Country Status (1)

Country Link
JP (1) JPH03105265A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005300831A (en) * 2004-04-09 2005-10-27 Bridgestone Corp Image display panel, particle group combination determination method used therefor, and image display device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005300831A (en) * 2004-04-09 2005-10-27 Bridgestone Corp Image display panel, particle group combination determination method used therefor, and image display device

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