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JP3112904B2 - Apparatus and method for measuring triboelectric charge of powder - Google Patents
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JP3112904B2 - Apparatus and method for measuring triboelectric charge of powder - Google Patents

Apparatus and method for measuring triboelectric charge of powder

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Publication number
JP3112904B2
JP3112904B2 JP11219024A JP21902499A JP3112904B2 JP 3112904 B2 JP3112904 B2 JP 3112904B2 JP 11219024 A JP11219024 A JP 11219024A JP 21902499 A JP21902499 A JP 21902499A JP 3112904 B2 JP3112904 B2 JP 3112904B2
Authority
JP
Japan
Prior art keywords
powder
gas
wire mesh
conductive container
friction partner
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
JP11219024A
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Japanese (ja)
Other versions
JP2000105260A (en
Inventor
寿彦 小口
富夫 星
Original Assignee
東芝ケミカル株式会社
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Application filed by 東芝ケミカル株式会社 filed Critical 東芝ケミカル株式会社
Priority to JP11219024A priority Critical patent/JP3112904B2/en
Publication of JP2000105260A publication Critical patent/JP2000105260A/en
Application granted granted Critical
Publication of JP3112904B2 publication Critical patent/JP3112904B2/en
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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、試料粉体と摩擦相
手粉体との間に生じた摩擦帯電量を精度よく迅速かつ簡
便に測定するための帯電量測定装置及びその測定方法に
関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a charge amount measuring apparatus and method for measuring the amount of triboelectric charge generated between a sample powder and a friction partner powder accurately, quickly and simply.

【0002】[0002]

【従来の技術】試料粉体の摩擦帯電特性を測定するため
に、従来から一般に試料粉体と帯電を付与する摩擦相手
粉体とを混合して予め充分に摩擦帯電させた後、風力、
遠心力、機械力、衝撃力、静電気力、振動などによって
両者間を分離し、分離した一方の粉体に残った電荷量を
測定する方法が採られている。この試料粉体と摩擦相手
粉体との分離は、試料粉体と摩擦相手粉体相互間に粒径
の差がある場合には金網の目を通して粒径を振るい分
け、また試料粉体と摩擦相手粉体のいずれか一方が強磁
性体である場合には、磁石にて吸着分離させることがで
きる。
2. Description of the Related Art In order to measure the triboelectric charging characteristics of a sample powder, conventionally, a sample powder and a friction partner powder to be charged are mixed and sufficiently friction-charged in advance, and then the wind power,
A method has been adopted in which the two are separated by centrifugal force, mechanical force, impact force, electrostatic force, vibration, or the like, and the amount of charge remaining on one of the separated powders is measured. This separation of the sample powder and the friction partner powder is performed by separating the particle size through a wire mesh when there is a difference in particle size between the sample powder and the friction partner powder. When one of the partner powders is a ferromagnetic material, it can be adsorbed and separated by a magnet.

【0003】前記したように、金網の目を通すことによ
り小粒径粉体を除去して大粒径粉体のみを捕集する方法
はブローオフ法と呼ばれ、最も一般的に用いられてい
る。この方法は、気流の流入側及び排出側に開口した少
なくとも一方の開口端に金網を張設した金属製の導電性
容器中に、試料粉体と摩擦相手粉体とを混合して予め充
分に摩擦帯電させてから入れた後、気体流入側から排出
側の金網面に向けて圧縮空気を吹きつけることにより、
小粒径粉体を金網の目を通して吹き飛ばして除去し、導
電性容器内に残った大粒径粉体を捕集するものである。
このようにして導電性容器内に残った大粒径粉体の表面
には、除去された小径粉体が持ち去ったと等量の電荷が
残留しいることから、この電荷量を測定することにより
摩擦帯電量を知ることが可能となる。
[0003] As described above, a method of removing a small particle size powder by passing through a wire mesh and collecting only a large particle size powder is called a blow-off method and is most commonly used. . In this method, a sample powder and a friction partner powder are mixed sufficiently in advance in a metal conductive container having a wire mesh stretched over at least one opening end opened on the inflow side and the discharge side of the airflow. After charging after friction charging, by blowing compressed air from the gas inflow side to the discharge side wire mesh surface,
The powder having a small particle diameter is blown off through a wire mesh and removed, and the powder having a large particle diameter remaining in the conductive container is collected.
When the removed small-diameter powder is taken away, an equivalent amount of charge remains on the surface of the large-diameter powder remaining in the conductive container in this manner. It becomes possible to know the charge amount.

【0004】なお、前記した導電性容器の気体流入側か
ら圧縮空気を吹き込むことに替えて、気体排出側から吸
引しても同様な効果が得られる。
A similar effect can be obtained by sucking from the gas discharge side instead of blowing the compressed air from the gas inlet side of the conductive container.

【0005】[0005]

【発明が解決しようとする課題】しかしながら、前記従
来のブローオフ法による装置は、簡便で迅速かつ高精度
に摩擦帯電特性を知ることができるものの、帯電量の測
定において次のような問題がある。
However, although the apparatus using the conventional blow-off method can easily and quickly and accurately know the triboelectric charging characteristics, it has the following problems in measuring the amount of charge.

【0006】第1に、導電性容器内にて分離した試料粉
体と摩擦相手粉体とが静電気的に引き合って再び合体
し、複数回の接触と分離を繰り返すため、一種の摩擦帯
電器として働く。これにより帯電測定値の一定化までに
時間がかかり、迅速な測定が困難になる。
First, the sample powder and the friction partner powder separated in the conductive container are electrostatically attracted to each other to unite again and repeat contact and separation a plurality of times. work. As a result, it takes time to stabilize the measured charge value, and it is difficult to perform quick measurement.

【0007】第2に、ブローオフ操作にて、試料粉体や
摩擦相手粉体が導電性容器の壁面や金網との間で摩擦帯
電することにより、両粉体間の摩擦にて生じる摩擦帯電
量とは異なる値となる。
Second, when the sample powder and the friction partner powder are frictionally charged between the wall surface and the wire mesh of the conductive container by the blow-off operation, the frictional charge generated by the friction between the two powders Will be different.

【0008】第3に、導電性容器の内壁あるいは金網の
一部に、分離した粉体が付着しやすいため測定帯電量に
誤差が生じる。
Third, since the separated powder easily adheres to the inner wall of the conductive container or a part of the wire net, an error occurs in the measured charge amount.

【0009】第4に、金網面に大粒径粉体が摩擦して磨
耗することにより生じる帯電にて測定帯電量に誤差が生
じる。
Fourth, an error occurs in the measured charge amount due to the charging caused by the friction of the large particle size powder on the surface of the wire mesh.

【0010】第5に、試料粉体と摩擦相手粉体との間の
摩擦帯電量が大きくなるに従って、分離に時間がかかる
ばかりでなく、場合によっては分離できないこともあ
る。
Fifth, as the amount of triboelectric charge between the sample powder and the friction partner powder increases, not only does it take time to separate, but in some cases, separation is not possible.

【0011】よって本発明は前記問題点に鑑みてなされ
たものであり、導電性容器の気体流入側から排出側に至
る気体の流れを制御することにより、試料粉体と摩擦相
手粉体との分離効果を高めることを目的とする。
Accordingly, the present invention has been made in view of the above-mentioned problems, and controls the flow of gas from the gas inflow side to the discharge side of the conductive container so that the sample powder and the friction partner powder can be separated. The purpose is to increase the separation effect.

【0012】[0012]

【課題を解決するための手段】上記目的を達成するた
め、請求項1の摩擦帯電量測定装置は、金網を張設した
導電性容器中に、摩擦帯電した試料粉体と摩擦相手粉体
との混合粉体を入れ、該混合粉体を気流にて、前記試料
粉体と前記摩擦相手粉体とに分離すると共に前記混合粉
体のうち小粒径の試料粉体のみを前記金網を通して排出
し、該金網内に残った大径粒の摩擦相手粉体の帯電量を
測定する粉体の摩擦帯電量測定装置において、上端部に
圧縮気体を吹き込む気体噴出口と該気体噴出口周辺に気
体を導入する気体流入口とを設けると共に、下端部に前
記圧縮気体を吸引する気体吸引口を開口された筒状の導
電性容器と、該導電性容器の前記気体流入口と前記気体
吸引口の間に架張され、かつ前記導電性容器内に収容さ
れた試料粉体および摩擦相手粉体のうち試料粉体を前記
圧縮気体の吹込みと吸引で選択通過させる金網と、該金
網の下面外周部に水平方向に気体を流入する開口部を
し、該開口部から気体を前記金網面に向け流入して渦
流を発生させる渦流発生手段と、前記導電性容器の上端
部の吹込口から噴出される圧縮気体を前記金網の下部で
吸引する気体吸引手段と、前記導電性容器内に残存する
摩擦相手粉体の帯電量を測定する帯電量測定手段とを具
備していることを特徴とする。
In order to achieve the above object, an apparatus for measuring the amount of triboelectric charge according to claim 1 is provided in which a triboelectrically charged sample powder and a friction partner powder are placed in a conductive container having a wire mesh stretched. And the mixed powder is separated into the sample powder and the friction partner powder by an air current, and only the sample powder having a small particle diameter of the mixed powder is discharged through the wire mesh. In a powder triboelectric charge measuring device for measuring the charge of a large-diameter particle friction partner powder remaining in the wire netting, a gas outlet for blowing a compressed gas into an upper end portion and a gas around the gas outlet are provided. provided with a gas inlet for introducing a cylindrical conductive container having an opening to the gas suction port for sucking the compressed gas to the lower portion, and the gas inlet of the conductive container of the gas suction port It is stretched between, and the sample powder accommodated in the conductive container and Shape and wire mesh for selectively passing the sample powder with suction and blowing of the compressed gas out of the friction partners powder, an opening for flowing gas in a horizontal direction on the lower surface outer peripheral portion of the gold network
Adult City, sucks the vortex generating means for the gas from the opening and flows toward the wire mesh surface to generate a vortex, the compressed gas ejected from the blowing port of the upper end of the conductive container at the bottom of the wire mesh Gas suction means, remaining in the conductive container
And a charge amount measuring means for measuring a charge amount of the friction partner powder .

【0013】請求項1の粉体の摩擦帯電量測定装置によ
れば、前記摩擦帯電量測定装置内の気流が、前記摩擦帯
電量測定装置下部からの前記気体吸引手段による吸引
と、該吸引によって派生する前記渦流発生手段の開口部
から金網の下面側に沿って水平方向に流入する気体、前
記導電性容器の気体流入口から流入する気体と、前記摩
擦帯電量測定装置上部の気体噴出口からの圧縮気体の吹
き込みによる気流との合成気流からなるまた、帯電量
測定に際して、予め前記気体吸引手段にて前記導電性容
器の気体流入口及び渦流発生手段の開口部から気体を流
入させ、その状態を保ちつつ前記気体噴出口から前記圧
縮気体を吹き込むことになる。
According to the apparatus for measuring the amount of triboelectric charge of a powder according to the present invention, the air flow in the apparatus for measuring triboelectric charge is controlled by the friction band.
Suction from the lower part of the coulometer by the gas suction means
And an opening of the vortex generating means derived by the suction
Gas flowing horizontally along the underside of the wire mesh from the front
The gas flowing from the gas inlet of the conductive container and the friction
Blowing of compressed gas from the gas outlet on the top
It is composed of a combined airflow with the airflow caused by the intrusion . Also, the charge amount
At the time of measurement, the conductive volume is previously measured by the gas suction means.
Gas from the gas inlet of the vessel and the opening of the vortex generator.
Into the gas outlet while maintaining the state.
The compressed gas will be blown.

【0014】請求項2の粉体の摩擦帯電量測定方法は、
上端部に圧縮気体を吹き込む気体噴出口と該気体噴出口
周囲に気体を導入する気体流入口とを設け、下端部に前
記圧縮気体を吸引する気体吸引口を設けるとともに前記
気体流入口と前記気体吸引口の間に金網を架張してなる
筒状の導電性容器の下部に、前記導電性容器の水平方向
に気体を流入する開口部を有する渦流発生手段を配置
し、前記導電性容器中に摩擦帯電した前記金網を通過し
得る小粒径の試料粉体と前記試料粉体より大粒径の摩擦
相手粉体との混合粉体を収容し、前記導電性容器の気体
吸引口から吸引して前記導電性容器の気体流入口及び渦
流発生手段の開口部から流入した気体流により前記金網
下部に気体の渦流を形成させて前記混合粉体を前記金網
面に均一に分布させ、次いで前記導電性容器の気体噴出
口から圧縮気体を吹き込むことにより前記試料粉体と前
記摩擦相手粉体とを分離しつつ試料粉体のみを前記金網
を通して排出させ、しかる後該金網内に残った摩擦相手
粉体の帯電量を測定する
According to a second aspect of the present invention, there is provided a method for measuring a triboelectric charge amount of a powder.
Gas outlet for injecting compressed gas into upper end and gas outlet
A gas inlet for introducing gas is provided around the
Providing a gas suction port for sucking the compressed gas and
A wire mesh is stretched between the gas inlet and the gas suction port
At the bottom of the cylindrical conductive container, the horizontal direction of the conductive container
Vortex generator with an opening for gas flow
And passing through the wire net frictionally charged in the conductive container.
Sample powder of small particle size obtained and friction of larger particle size than said sample powder
The mixed powder with the counterpart powder is stored, and the gas in the conductive container is
Suction from the suction port and gas inlet and vortex of the conductive container
The wire mesh is caused by the gas flow flowing from the opening of the flow generating means.
A gas swirl is formed in the lower part to mix the powder mixture with the wire mesh.
Uniformly distributed on the surface, and then gas ejection from the conductive container
By blowing compressed gas through the mouth,
The metal mesh is used to separate only the sample powder while separating the friction partner powder.
Through the wire mesh, and then the friction partner left in the wire mesh
The charge amount of the powder is measured .

【0015】請求項2の粉体の摩擦帯電量測定方法によ
れば、前記導電性容器中に、予め気体吸引手段にて導電
性容器の気体流入口及び渦流発生手段の開口部から気体
を流入させ、その状態を保ちつつ気体吸引手段にて気体
吸引口と渦流発生手段の開口部から気体を吸引させつ
つ、導電性容器内に気体を流入させ、気体噴出口から圧
縮気体を金網に向けて吹き込むことにより、金網下部に
渦流を発生させて、試料粉体と摩擦相手粉体とに分離
し、混合粉体のうち小粒径の試料粉体のみを金網を通し
て排出させ、該金網内に残った大径粒の摩擦相手粉体の
帯電量が測定できる。
According to a second aspect of the present invention, there is provided a method for measuring a triboelectric charge amount of a powder.
If it is, conductive in the conductive container by gas suction means in advance
Gas from the gas inlet and the opening of the vortex generator
While maintaining the state,
The gas is sucked from the suction port and the opening of the vortex generator.
First, gas is introduced into the conductive container, and pressure is
By blowing compressed gas toward the wire mesh,
Generates vortex and separates into sample powder and friction partner powder
Only the sample powder with a small particle size out of the mixed powder is passed through a wire mesh.
To remove the large-diameter grain friction partner powder remaining in the wire mesh.
The charge amount can be measured.

【0016】 削除[0016] Delete

【0017】 削除[0017] Delete

【0018】 削除[0018] Delete

【0019】[0019]

【発明の実施の形態】以下、本発明の実施の形態を図面
に基づいて説明する。
Embodiments of the present invention will be described below with reference to the drawings.

【0020】図1から図5は本発明の実施の形態を示
し、図1は粉体の摩擦帯電量測定装置の断面図、図2は
金網ホルダー及び渦流発生ノズルを示す断面図、図3は
渦流発生手段の開口部の正面図、図4は導電性容器(以
下ファラデーケージという)に金網ホルダーを組み込ん
だ状態を示す斜視図、図5は電荷量の時間的変化を示す
線図である。
FIGS. 1 to 5 show an embodiment of the present invention. FIG. 1 is a sectional view of a device for measuring the amount of triboelectricity of powder, FIG. 2 is a sectional view showing a wire mesh holder and a vortex generating nozzle, and FIG. FIG. 4 is a front view of the opening of the eddy current generating means, FIG. 4 is a perspective view showing a state where a wire mesh holder is incorporated in a conductive container (hereinafter referred to as a Faraday cage), and FIG.

【0021】本発明の粉体の摩擦帯電量測定装置は、図
1に示すように、略中央にファラデーケージ1が配設さ
れ、このファラデーケージ1は導電性材料(一般的には
ステンレススチール、銅、真鍮、アルミニウム、鉄等、
あるいはプラスチックにて形成してその内面に酸化に対
して安定なニッケル、クロム、金、白金等のメッキを施
したものであってもよい)からなり、上部に取付台15
を形設し、気体流入側に開口部16を設けた筒状に形成
される容器である。
As shown in FIG. 1, the apparatus for measuring the amount of triboelectric charge of a powder according to the present invention has a Faraday cage 1 disposed substantially at the center thereof. The Faraday cage 1 is made of a conductive material (generally, stainless steel, Copper, brass, aluminum, iron, etc.
Alternatively, it may be formed of plastic and the inner surface thereof is plated with nickel, chromium, gold, platinum or the like which is stable against oxidation.
And a cylindrical container provided with an opening 16 on the gas inflow side.

【0022】その下面、即ち、気体排出側には金網ホル
ダー3が設けられ、金網ホルダー3には、図2に示すよ
うに、ファラデーケージ1の外径が嵌合する嵌合部3a
と中央にファラデーケージ1の排出側開口部内径1aと
同一径の開口部3bが形成され、嵌合部3aの底部3c
には金網2(例えばステンレススチール製のもの)を挿
入してファラデーケージ1を嵌合することにより金網2
をファラデーケージ1にて押さえ込んで固定することが
できるようになっている。
A wire mesh holder 3 is provided on the lower surface, that is, on the gas discharge side. The wire mesh holder 3 has a fitting portion 3a into which the outer diameter of the Faraday cage 1 is fitted as shown in FIG.
An opening 3b having the same diameter as the inner diameter 1a of the discharge side opening of the Faraday cage 1 is formed at the center, and a bottom 3c of the fitting portion 3a is formed.
The wire mesh 2 (for example, made of stainless steel) is inserted into the
Can be held down and fixed by the Faraday cage 1.

【0023】一方、図2及び図3に示すように、金網ホ
ルダー3の下面には、渦流発生手段として渦流発生用開
口部13が形成されている。この渦流発生用開口部13
は、略円弧状あるいは三角形状にて、高さHが1mmの
気流ガイド部14が3箇所ないし6箇所、等配に形成さ
れたものである。この気流ガイド部14によってファラ
デーケージ1の外周側の3箇所ないし6箇所から、気体
を旋回させつつ金網2の下面に沿って流入させ又は吸引
することによって渦流を生じさせることができる。
On the other hand, as shown in FIGS. 2 and 3, on the lower surface of the wire mesh holder 3, an eddy current generating opening 13 is formed as eddy current generating means. This vortex generation opening 13
Is an approximately arc-shaped or triangular-shaped air flow guide section 14 having a height H of 1 mm, which is formed at three or six places at equal intervals. The gas flow guide portion 14 can generate a vortex by flowing or sucking the gas from the three or six locations on the outer peripheral side of the Faraday cage 1 along the lower surface of the wire mesh 2 while rotating the gas.

【0024】なお、前記気流ガイド部14の形状は、略
円弧状あるいは三角形状に限らず直線状その他の形状で
あってもよく、要は金網2の面に渦流が発生しうる形状
であればよい。また配置は3箇所に限らず3箇所以上の
複数箇所であってもよい。
The shape of the air flow guide portion 14 is not limited to a substantially arc shape or a triangular shape, but may be a straight line shape or any other shape. Good. The arrangement is not limited to three places, but may be three or more places.

【0025】また、金網ホルダー3の下方には絶縁体の
筒体であるテフロン台7が配設されている。テフロン台
7の内径は、ファラデーケージ1の排出側内径1a及び
金網ホルダー3の内径3bと同一径であり、テフロン台
7の上面に対して金網ホルダ3を挿着したファラデーケ
ージ1を載置した際にファラデーケージ1と金網ホルダ
3とテフロン台7それぞれの内径が同一径にて連通する
ことができるようになっている。さらにテフロン台7の
下方には吸引系11が連結されており、吸引系11の端
末には吸引手段として図示しない吸引装置が連結されて
いる。
Below the wire mesh holder 3, a Teflon base 7, which is a cylindrical body of an insulator, is provided. The inner diameter of the Teflon stand 7 is the same as the inner diameter 1a on the discharge side of the Faraday cage 1 and the inner diameter 3b of the wire mesh holder 3, and the Faraday cage 1 in which the wire mesh holder 3 is inserted on the upper surface of the Teflon stand 7 is placed. In this case, the inner diameters of the Faraday cage 1, the wire mesh holder 3, and the Teflon table 7 can be communicated with the same diameter. Further, a suction system 11 is connected below the Teflon base 7, and a suction device (not shown) is connected to a terminal of the suction system 11 as suction means.

【0026】一方、ファラデーケージ1の上方には、圧
縮気体を吹込む圧力ホース12に連結された圧縮気体噴
出口である上部ノズル10が取り付け台15を介して配
置されており、取り付け台15はその側面が開口されて
いて気体吸引手段の作動によりこの開口部16からファ
ラデーケージ1内に気体が自由に吸引されるとともに、
上部ノズル10からの圧縮気体が吹き込まれるようにな
っている。
On the other hand, above the Faraday cage 1, an upper nozzle 10 which is a compressed gas jet port connected to a pressure hose 12 for blowing compressed gas is disposed via a mounting table 15, and the mounting table 15 is The side is opened, and the gas is freely sucked into the Faraday cage 1 from the opening 16 by the operation of the gas suction means.
Compressed gas is blown from the upper nozzle 10.

【0027】また、上記構成の装置にて摩擦帯電量を測
定する粉体は、試料粉体4あるいは摩擦相手粉体6のい
ずれか一方が金網2の目より大きいか又は小さい粒径の
組み合わせにする。例えば、電子写真のトナーとキャリ
ヤの組み合わせにおいて、試料粉体に相当するトナーは
1〜30μm程度の粒径であり、摩擦相手粉体に相当す
るキャリヤ粉は30〜500μm程度の粒径である。な
お金網2の目開きは、使用する摩擦相手粉体の最小径よ
り小さいものが選択される。
The powder for which the amount of triboelectric charge is measured by the apparatus having the above-mentioned configuration is a combination of one of the sample powder 4 and the friction partner powder 6 having a particle size larger or smaller than the mesh of the wire mesh 2. I do. For example, in a combination of an electrophotographic toner and a carrier, the toner corresponding to the sample powder has a particle size of about 1 to 30 μm, and the carrier powder corresponding to the friction partner powder has a particle size of about 30 to 500 μm. The mesh of the wire mesh 2 is selected to be smaller than the minimum diameter of the friction partner powder to be used.

【0028】次に本発明の装置の作動について説明す
る。
Next, the operation of the apparatus of the present invention will be described.

【0029】まず、金網ホルダー3とファラデーケージ
1との間に金網2を取りつける。この場合、図1に示す
ように、金網ホルダー3の嵌合部3aの底部3cに金網
2を挿入して嵌合部3aにファラデーケージ1の下端外
径を嵌合する。ここに用いる金網2はステンレススチー
ル製で、目の大きさが400メッシュのものである。こ
の後、ファラデーケージ1の上部より粒径10μmの試
料粉体4と、粒径50〜80μmの摩擦相手粉体6との
混合粉体5(混合重量比5:95)を入れ、金網側を下
方に向けてテフロン台7に乗せる。
First, the wire mesh 2 is attached between the wire mesh holder 3 and the Faraday cage 1. In this case, as shown in FIG. 1, the wire mesh 2 is inserted into the bottom 3c of the fitting portion 3a of the wire mesh holder 3, and the outer diameter of the lower end of the Faraday cage 1 is fitted into the fitting portion 3a. The wire mesh 2 used here is made of stainless steel and has a mesh size of 400 mesh. Thereafter, a mixed powder 5 (mixing weight ratio of 5:95) of a sample powder 4 having a particle size of 10 μm and a friction partner powder 6 having a particle size of 50 to 80 μm is placed from above the Faraday cage 1, and the wire mesh side is placed. Place it on the Teflon table 7 downward.

【0030】次いで、取付台15の上部、すなわちファ
ラデーケージ1の上端部に、圧力ホース12を連結した
圧縮気体吹き込み用のノズル10を配置する。これによ
り摩擦帯電量測定装置内の流路が、気体流入側Aから気
体排出側Bに至るまで、一直線で連結された状態とな
る。
Next, a nozzle 10 for blowing a compressed gas to which a pressure hose 12 is connected is disposed above the mounting base 15, that is, at the upper end of the Faraday cage 1. As a result, the flow paths in the frictional charge measuring device are connected in a straight line from the gas inlet side A to the gas outlet side B.

【0031】この状態にて、吸引系11の端末に接続さ
れた図示しない吸引装置を駆動して吸引を開始する。こ
れにより、渦流発生用開口部13から気体が導電性容器
内に吸入され、金網2の下面に渦流が生じると同時に、
ファラデーケージ1上方の上部ノズル取り付け台15の
開口部16からも気体が吸入され、これらの気流により
混合粉体5が金網の面に均一に分布される。
In this state, a suction device (not shown) connected to the terminal of the suction system 11 is driven to start suction. As a result, gas is sucked into the conductive container from the vortex generation opening 13, and a vortex is generated on the lower surface of the wire mesh 2.
Gas is also sucked from the opening 16 of the upper nozzle mounting base 15 above the Faraday cage 1, and the mixed powder 5 is evenly distributed on the surface of the wire mesh by these airflows.

【0032】このようにして混合粉体5が予め金網2の
面に均一に分布された状態を保ちつつ、上部ノズル10
から圧力ホース12を介して圧縮気体を吹き込み、試料
粉体4を金網2の目を通して除去する。
While maintaining the state in which the mixed powder 5 is uniformly distributed on the surface of the wire mesh 2 in this manner, the upper nozzle 10
Then, compressed gas is blown through the pressure hose 12 to remove the sample powder 4 through the wire mesh 2.

【0033】以上の操作は実際面において、例えば、先
ず最初に気体吸引装置の作動により開口部16及び渦流
発生開口部13から気体を流入させ、これにより発生し
た渦流にて金網の面に混合粉体5を均一に分布させる。
このように、気体吸引装置を作動させてから、圧力ホー
ス12を経て上部ノズル10から0.5kg/cm2 の圧縮
窒素ガスを吹き込む。
In the above operation, for example, first, gas is caused to flow from the opening 16 and the vortex generation opening 13 by the operation of the gas suction device, and the mixed powder is generated on the surface of the wire mesh by the vortex generated thereby. The body 5 is evenly distributed.
After operating the gas suction device in this way, 0.5 kg / cm 2 of compressed nitrogen gas is blown from the upper nozzle 10 through the pressure hose 12.

【0034】これにより混合粉5は試料粉体4と摩擦相
手粉体6とに分離され、分離された試料粉体4は、金網
2の面に発生した渦流と吸引系11側からの吸引気流と
により金網2の目を効率よく通って吸引系11側に排除
される。これにより金網2の上流側の面には摩擦相手粉
体6が残る。
Thus, the mixed powder 5 is separated into the sample powder 4 and the friction partner powder 6, and the separated sample powder 4 is swirled on the surface of the wire mesh 2 and the suction airflow from the suction system 11 side. Thus, the wire is efficiently passed through the mesh of the wire mesh 2 and is removed to the suction system 11 side. As a result, the friction partner powder 6 remains on the upstream surface of the wire mesh 2.

【0035】この時、摩擦相手粉体6は、金網2の面に
生じた渦流及びファラデーケージ1の上方から流入する
気体とにより金網2の面に均一に分布した層を形成させ
るとともにその層を固定させることにより、摩擦相手粉
体6がファラデーケージ1の内壁に衝突したり金網2の
面に摩擦したりすることがない。一方、ブロウされた試
料粉体4は効率よく金網2の目から通過して下流側に吸
引されるので、通過した試料粉体4(トナー)が摩擦相
手粉体6に再付着することがなくなる。
At this time, the friction partner powder 6 forms a layer uniformly distributed on the surface of the wire mesh 2 by the eddy current generated on the surface of the wire mesh 2 and the gas flowing from above the Faraday cage 1 and forms the layer. By fixing, the friction partner powder 6 does not collide with the inner wall of the Faraday cage 1 or rub against the surface of the wire mesh 2. On the other hand, the blown sample powder 4 efficiently passes through the wire mesh 2 and is sucked downstream, so that the passed sample powder 4 (toner) does not adhere to the friction partner powder 6 again. .

【0036】このようにして金網2の面に残った摩擦相
手粉体6には試料粉体4が持ち去ったと等量かつ逆の帯
電量が残っており、この場合の電荷量Qはファラデーケ
ージ1に接続されたコンデンサ8(静電容量C)を充電
させる。従って、その両端の電圧9を測定することによ
り、Q=CVとして測定値を得ることが可能となる。図
5は電荷量の時間的変化を記録した線図である。この線
図によれば、初期吸引開始後の1秒以内にて電荷量が飽
和状態となり、試料中の試料粉体4が完全に除去された
ことが判る。また上記モードにて全測定時間を1秒にセ
ットし、化学天秤を用いて測定前後におけるファラデー
ケージ1の重量を測定したところ、測定後の重量減はフ
ァラデーケージ1中に秤り込んだ重量に一致した。
The friction partner powder 6 remaining on the surface of the wire mesh 2 has an equal and opposite charge amount when the sample powder 4 is removed, and the charge amount Q in this case is the Faraday cage 1 To charge the capacitor 8 (capacitance C) connected to. Therefore, by measuring the voltage 9 at both ends, it becomes possible to obtain a measured value as Q = CV. FIG. 5 is a diagram in which the change over time of the charge amount is recorded. According to this diagram, it can be seen that the charge amount became saturated within one second after the start of the initial suction, and the sample powder 4 in the sample was completely removed. When the total measurement time was set to 1 second in the above mode and the weight of the Faraday cage 1 before and after the measurement was measured using an analytical balance, the weight loss after the measurement was reduced to the weight measured in the Faraday cage 1 Matched.

【0037】このことは試料粉体の摩擦相手粉体からの
分離と、ファラデーケージ1外への除去が極めて速やか
に終了したことを示す。
This indicates that the separation of the sample powder from the friction partner powder and the removal of the sample powder from the Faraday cage 1 were completed very quickly.

【0038】測定後のファラデーケージ1の内側面、下
端及び金網2にはトナーは全く付着しておらず、ファラ
デーケージ1内に残った摩擦相手粉体6は金網2の上に
均一な層を形成して付着していた。
After the measurement, no toner adheres to the inner surface, the lower end, and the wire mesh 2 of the Faraday cage 1, and the friction partner powder 6 remaining in the Faraday cage 1 forms a uniform layer on the wire mesh 2. Formed and adhered.

【0039】この結果は、圧縮気体の吹き込みや気体排
出側からの吸引による粉体の動きが、吸引穴及び排出穴
を通して流れる気流と金網2の面に沿って吸い込まれる
渦流発生開口部13からの圧縮気体の気流とのバランス
のとれた合成気流によって、摩擦相手粉体が金網2の近
傍にてほぼ固定された状態を保ちつつ分離除去が行われ
ていることを示している。
The result is that the movement of the powder due to the blowing of the compressed gas and the suction from the gas discharge side is caused by the airflow flowing through the suction hole and the discharge hole and the vortex generation opening 13 sucked along the surface of the wire mesh 2. This indicates that the separated air is being separated and removed while keeping the friction partner powder substantially fixed in the vicinity of the wire mesh 2 by the synthetic airflow balanced with the compressed gas airflow.

【0040】以上による摩擦帯電量の測定は1秒以下の
短時間に終了した。
The measurement of the triboelectric charge amount was completed in a short time of 1 second or less.

【0041】[0041]

【発明の効果】本発明によれば、導電性容器の気体流入
側に気体が自由に流入しうる開口部を、また導電性容器
の気体排出側に金網の面に渦流を発生させる渦流発生手
段を設けたことにより、操作開始時点で試料粉体と摩擦
相手粉体との混合粉体を予め金網の面に均一に分布させ
ることが可能となり、この均一な分布状態を保ちつつ上
部ノズルから圧縮気体を吹き込むことにより、混合粉体
は試料粉体と摩擦相手粉体とに効率的に分離され金網上
に摩擦相手粉体の均一な層を形成しかつ固定することが
可能となるとともに試料粉体は金網の目を通してファラ
デーケージ外に効率的に除去される。
According to the present invention, an opening through which gas can freely flow into the gas inflow side of the conductive container and a vortex generating means for generating a vortex in the surface of the wire mesh on the gas discharge side of the conductive container. At the start of the operation, the mixed powder of the sample powder and the friction partner powder can be uniformly distributed in advance on the surface of the wire mesh, and compressed from the upper nozzle while maintaining this uniform distribution state. By blowing the gas, the mixed powder is efficiently separated into the sample powder and the friction partner powder, so that a uniform layer of the friction partner powder can be formed and fixed on a wire mesh and the sample powder can be fixed. The body is effectively removed through the wire mesh and out of the Faraday cage.

【0042】これによりファラデーケージ内で分離され
た試料粉体と摩擦相手粉体とが静電気的に引き合って結
合・分離を繰り返すことがなく殆ど完全に分離すること
が可能になるとともに、ブロウによって摩擦相手粉体が
飛散することが全くないので摩擦相手粉体の磨耗が減少
し、摩擦相手粉体のロスが少なくなる。
As a result, the sample powder separated in the Faraday cage and the friction partner powder electrostatically attract each other, so that the powder can be almost completely separated without repeating bonding and separation. Since the opponent powder is not scattered at all, wear of the opponent powder is reduced, and loss of the opponent powder is reduced.

【0043】さらに分離された粉体がファラデーケージ
の内壁や下端に再付着することが非常に少なくなり、帯
電量の測定精度が向上するとともに測定の再現性が著し
く向上する。
Further, the separated powder is very unlikely to reattach to the inner wall or lower end of the Faraday cage, so that the measurement accuracy of the charge amount is improved and the reproducibility of the measurement is significantly improved.

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

【図1】本発明の実施の形態に係る粉体の摩擦帯電量測
定装置の断面図。
FIG. 1 is a sectional view of a device for measuring the amount of triboelectric charge of a powder according to an embodiment of the present invention.

【図2】金網ホルダー及び渦流発生開口部を示す断面
図。
FIG. 2 is a cross-sectional view showing a wire mesh holder and a vortex generation opening.

【図3】渦流発生開口部の正面図。FIG. 3 is a front view of a vortex generation opening.

【図4】ファラデーケージに金網ホルダー組み込んだ状
態を示す斜視図。
FIG. 4 is a perspective view showing a state in which a wire mesh holder is incorporated in a Faraday cage.

【図5】電荷量の時間的変化を示す線図。FIG. 5 is a diagram showing a temporal change of a charge amount.

【符号の説明】[Explanation of symbols]

1…ファラデーケージ 2…金網 3…金網ホルダ 4…試料粉体 5…混合粉 6…摩擦相手粉体 7…テフロン台 8…コンデンサ 9…電圧 10…上部ノズル 11…吸引系 12…圧力ホース 13…渦流発生開口部 14…気流ガイド部 15…取付台 16…開口部 DESCRIPTION OF SYMBOLS 1 ... Faraday cage 2 ... Wire mesh 3 ... Wire mesh holder 4 ... Sample powder 5 ... Mixed powder 6 ... Friction partner powder 7 ... Teflon stand 8 ... Condenser 9 ... Voltage 10 ... Top nozzle 11 ... Suction system 12 ... Pressure hose 13 ... Eddy current generating opening 14: Air flow guide 15: Mounting base 16: Opening

フロントページの続き (58)調査した分野(Int.Cl.7,DB名) G01R 29/24 G01N 27/60 Continuation of front page (58) Field surveyed (Int. Cl. 7 , DB name) G01R 29/24 G01N 27/60

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】金網を張設した導電性容器中に、摩擦帯電
した試料粉体と摩擦相手粉体との混合粉体を入れ、該混
合粉体を気流にて、前記試料粉体と前記摩擦相手粉体と
に分離すると共に前記混合粉体のうち小粒径の試料粉体
のみを前記金網を通して排出し、該金網内に残った大径
粒の摩擦相手粉体の帯電量を測定する粉体の摩擦帯電量
測定装置において、 上端部に圧縮気体を吹き込む気体噴出口と該気体噴出口
周辺に気体を導入する気体流入口とを設けると共に、下
端部に前記圧縮気体を吸引する気体吸引口を開口された
筒状の導電性容器と、 該導電性容器の前記気体流入口と前記気体吸引口の間に
架張され、かつ前記導電性容器内に収容された試料粉体
および摩擦相手粉体のうち試料粉体を前記圧縮気体の吹
込みと吸引で選択通過させる金網と、 該金網の下面外周部に水平方向に気体を流入する開口部
形成し、該開口部から気体を前記金網面に向け流入し
て渦流を発生させる渦流発生手段と、 前記導電性容器の上端部の吹込口から噴出される圧縮気
体を前記金網の下部で吸引する気体吸引手段と、 前記導電性容器内に残存する摩擦相手粉体の帯電量を測
定する帯電量測定手段とを具備していることを特徴とす
る粉体の摩擦帯電量測定装置。
1. A mixed powder of a triboelectrically charged sample powder and a friction partner powder is placed in a conductive container having a wire mesh stretched thereon, and the mixed powder is mixed with the sample powder by an air current. At the same time as separating into the friction partner powder, only the sample powder having a small particle diameter of the mixed powder is discharged through the wire mesh, and the charge amount of the large-diameter friction partner powder remaining in the wire mesh is measured. In an apparatus for measuring the amount of triboelectric charge of a powder, a gas outlet for blowing compressed gas at an upper end and a gas inlet for introducing gas around the gas outlet are provided , and a gas suction for sucking the compressed gas at a lower end. A cylindrical conductive container having an open mouth; a sample powder and a friction partner which are stretched between the gas inlet and the gas suction port of the conductive container and accommodated in the conductive container; samples powder is selected passage with suction and blowing of the compressed gas out of the powder Network and an opening for flowing gas is formed in the horizontal direction on the lower surface outer peripheral portion of the gold network, a vortex generating means for generating a vortex flow of the gas from the opening and flows toward the wire mesh surface, the conductive container A gas suction means for sucking compressed gas ejected from a blowing port at an upper end of the wire mesh at a lower portion of the wire mesh; and a charge amount measuring means for measuring a charge amount of a friction partner powder remaining in the conductive container. An apparatus for measuring the amount of triboelectric charge of powder.
【請求項2】 上端部に圧縮気体を吹き込む気体噴出口
と該気体噴出口周囲に気体を導入する気体流入口とを設
け、下端部に前記圧縮気体を吸引する気体吸引口を設け
るとともに前記気体流入口と前記気体吸引口の間に金網
を架張してなる筒状の導電性容器の下部に、前記導電性
容器の水平方向に気体を流入する開口部を有する渦流発
生手段を配置し、 前記導電性容器中に摩擦帯電した前記金網を通過し得る
小粒径の試料粉体と前記試料粉体より大粒径の摩擦相手
粉体との混合粉体を収容し、前記導電性容器の気体吸引
口から吸引して前記導電性容器の気体流入口及び渦流発
生手段の開口部 から流入した気体流により前記金網下部
に気体の渦流を形成させて前記混合粉体を前記金網面に
均一に分布させ、次いで前記導電性容器の気体噴出口か
ら圧縮気体を吹き込むことにより前記試料粉体と前記摩
擦相手粉体とを分離しつつ試料粉体のみを前記金網を通
して排出させ、しかる後該金網内に残った摩擦相手粉体
の帯電量を測定する 粉体の摩擦帯電量測定方法。
2. A gas outlet for blowing compressed gas into the upper end.
And a gas inlet for introducing gas around the gas outlet.
A gas suction port for sucking the compressed gas at the lower end.
And a wire mesh between the gas inlet and the gas suction port.
The conductive material is placed at the bottom of a cylindrical conductive container
Vortex flow with an opening for gas flow in the horizontal direction of the container
A raw means can be arranged to pass through the wire mesh triboelectrically charged in the conductive container.
Sample powder with small particle size and friction partner with larger particle size than the sample powder
Containing the mixed powder with the powder, and gas suction of the conductive container.
Suction from the gas inlet and vortex of the conductive container
The lower part of the wire mesh by the gas flow flowing from the opening of the raw means
To form a swirl of gas on the wire mesh surface
Distribute evenly, and then remove the gas from the conductive container
By blowing compressed gas from the
Pass only the sample powder through the wire mesh while separating
And then discharged, and then the friction partner powder remaining in the wire mesh
A method for measuring the triboelectric charge of a powder for measuring the charge of a powder.
JP11219024A 1998-07-31 1999-08-02 Apparatus and method for measuring triboelectric charge of powder Expired - Lifetime JP3112904B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11219024A JP3112904B2 (en) 1998-07-31 1999-08-02 Apparatus and method for measuring triboelectric charge of powder

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP21750798 1998-07-31
JP10-217507 1998-07-31
JP11219024A JP3112904B2 (en) 1998-07-31 1999-08-02 Apparatus and method for measuring triboelectric charge of powder

Publications (2)

Publication Number Publication Date
JP2000105260A JP2000105260A (en) 2000-04-11
JP3112904B2 true JP3112904B2 (en) 2000-11-27

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Country Link
JP (1) JP3112904B2 (en)

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