JP3347940B2 - Powder triboelectric charge measuring device - Google Patents
Powder triboelectric charge measuring deviceInfo
- Publication number
- JP3347940B2 JP3347940B2 JP14548496A JP14548496A JP3347940B2 JP 3347940 B2 JP3347940 B2 JP 3347940B2 JP 14548496 A JP14548496 A JP 14548496A JP 14548496 A JP14548496 A JP 14548496A JP 3347940 B2 JP3347940 B2 JP 3347940B2
- Authority
- JP
- Japan
- Prior art keywords
- powder
- faraday cage
- charge amount
- sample powder
- wire mesh
- 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
Links
- 239000000843 powder Substances 0.000 title claims description 90
- 238000007664 blowing Methods 0.000 claims description 17
- 125000006850 spacer group Chemical group 0.000 claims description 17
- 239000002184 metal Substances 0.000 claims description 3
- 238000005259 measurement Methods 0.000 description 13
- 239000002245 particle Substances 0.000 description 11
- 238000000034 method Methods 0.000 description 6
- 238000000926 separation method Methods 0.000 description 6
- 239000003990 capacitor Substances 0.000 description 3
- 239000000203 mixture Substances 0.000 description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 238000005299 abrasion Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005294 ferromagnetic effect Effects 0.000 description 2
- 239000000654 additive Substances 0.000 description 1
- 230000000996 additive effect Effects 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000013011 mating Effects 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229920000728 polyester Polymers 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 238000003908 quality control method Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 229920001909 styrene-acrylic polymer Polymers 0.000 description 1
- 230000004580 weight loss Effects 0.000 description 1
Landscapes
- Other Investigation Or Analysis Of Materials By Electrical Means (AREA)
- Developing Agents For Electrophotography (AREA)
Description
【0001】[0001]
【発明の属する技術分野】本発明は、試料粉体と接触相
手粉体との間の摩擦帯電量を精度よく、かつ迅速・簡便
に測定することのできる接触帯電量測定装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a contact charge amount measuring device capable of measuring the triboelectric charge amount between a sample powder and a contact partner powder accurately, quickly and easily.
【0002】[0002]
【従来の技術】一般に、試料粉体の摩擦帯電特性を測定
する手段は、試料粉体に帯電を付与する接触相手粉体と
混合し、風力,遠心力,機械力,衝撃力,静電気力,振
動などを加えて摩擦帯電された両者を分離して、一方の
粉体に残留している(残った)電荷量の測定で行ってい
る。すなわち、試料粉体および接触相手粉体に粒径の差
がある場合、たとえば金網を用いて分離すると、金網の
目開きを通して小粒径粉体のみを選択的に除去できるた
め、残存・残留した比較的粒径の大きい粉体に残った帯
電量を測定することができる。また、試料粉体および接
触相手粉末のいずれか一方が強磁性体である場合には、
両者の分離に磁石を用いて強磁性体粉体のみを選択的に
固定することにより、強磁性体粉体の帯電量を容易に測
定できる。摩擦帯電された試料粉体および接触相手粉体
の分離に風力を用い、金網を用いて大粒径粉体を捕集し
てその帯電量を測定する方法は、ブローオフ法と呼ば
れ、最も一般的に使用されている。このブローオフ法で
は、少なくとも一端に金網を張設した金属円筒(以下フ
ァラデーケージ本体と称する)内に、予め混合して十分
な摩擦帯電をもった試料粉体および接触相手粉体の混合
物を収容し、一端から他端の金網面に向けて圧縮空気を
吹き付けて両者を分離することを骨子としている。2. Description of the Related Art In general, a means for measuring the triboelectric charging characteristics of a sample powder is prepared by mixing a powder with a contact partner powder which imparts a charge to the sample powder and applying a wind force, centrifugal force, mechanical force, impact force, electrostatic force, or the like. Vibration or the like is applied to separate the triboelectrically charged two, and the amount of charge remaining (remaining) on one of the powders is measured. That is, when there is a difference in the particle diameter between the sample powder and the contact partner powder, for example, when separated using a wire mesh, only the small particle size powder can be selectively removed through the openings of the wire mesh. The amount of charge remaining on the powder having a relatively large particle size can be measured. Further, when one of the sample powder and the contact partner powder is a ferromagnetic material,
By selectively fixing only the ferromagnetic powder using a magnet to separate them, the charge amount of the ferromagnetic powder can be easily measured. The method of using a wind force to separate the triboelectrically charged sample powder and the contact partner powder, collecting large-diameter powder using a wire mesh, and measuring the charge amount is called a blow-off method. Is used regularly. In this blow-off method, a mixture of a sample powder and a contact partner powder which have been mixed in advance and have a sufficient triboelectric charge are accommodated in a metal cylinder (hereinafter referred to as a Faraday cage body) having a wire mesh stretched at least at one end. The main point is that compressed air is blown from one end to the wire mesh surface at the other end to separate them.
【0003】すなわち、試料粉体もしくは接触相手粉体
のいずれか一方は、金網の目開きより大きい粒径とし、
また他方は金網の目開きより小さい粒径となるようにす
る。その結果、分離した一方の粉体は金網の目開きを通
してファラデーケージ本体外に吹き飛ばされる。ファラ
デーケージ本体内に残った大粒径粉体の表面には、ファ
ラデーケージ本体外に吹き飛ばされた小粒径粉体がもち
去ったと等量で、かつ逆の電荷が残っているため、この
電荷量を測定することによって両者の摩擦帯電量を知る
ことができる。なお、圧縮空気を吹き付ける代わりに、
ファラデーケージ本体内および金網面を通して気体を吸
引する方式を採っても同様に、両者の摩擦帯電量を測定
できる。That is, either the sample powder or the contact partner powder has a particle size larger than the mesh of the wire mesh,
The other has a particle size smaller than the mesh of the wire mesh. As a result, one of the separated powders is blown out of the Faraday cage body through the openings of the wire mesh. On the surface of the large particle size powder remaining in the Faraday cage body, an equal amount of the opposite charge remains when the small particle size powder blown out of the Faraday cage body is removed, and the opposite charge remains. By measuring the amount, the triboelectric charge amount of both can be known. In addition, instead of blowing compressed air,
Even if a method of sucking gas through the inside of the Faraday cage main body and the wire mesh surface is used, the triboelectric charge amount of both can be measured similarly.
【0004】[0004]
【発明が解決しようとする課題】上記、ブローオフ手段
は、構造,操作が簡便で、試料粉体および接触相手粉体
の摩擦帯電特性を迅速、かつ高精度に知ることができる
ので、一般的な手法として広く実用されている。しかし
ながら、従来のブローオフ帯電量測定では、次のような
問題があり、その解決・解消が望まれている。The above blow-off means has a simple structure and operation, and can quickly and accurately know the triboelectric charging characteristics of the sample powder and the contact partner powder. It is widely used as a method. However, the conventional blow-off charge amount measurement has the following problems, and it is desired to solve and eliminate them.
【0005】(1)ファラデーケージ本体内で分離した試
料粉体と接触相手粉体とが、静電的に引き合って再び合
体し、接触と分離を繰り返す傾向がある。つまり、ファ
ラデーケージ本体が1種の摩擦帯電器として作用し、帯
電測定値の一定化までに時間がかかり、迅速な帯電量の
測定が困難である。(1) The sample powder separated in the Faraday cage main body and the contact partner powder tend to be electrostatically attracted to unite again and repeat contact and separation. That is, the Faraday cage body acts as one kind of friction charger, and it takes time to stabilize the measured charge value, and it is difficult to quickly measure the charge amount.
【0006】(2)ブローオフ操作で、試料粉体とファラ
デーケージ本体内壁面との摩擦帯電、試料粉体と金網と
の摩擦帯電も生じるので、精度の高い帯電量測定が困難
である。(2) The blow-off operation also causes frictional charging between the sample powder and the inner wall surface of the Faraday cage body and frictional charging between the sample powder and the wire mesh, making it difficult to measure the charge amount with high accuracy.
【0007】(3)ファラデーケージ本体内壁面や金網の
一部に分離粉体が付着し易いため、測定帯電量に誤差が
生じ易い。(3) Since the separated powder easily adheres to the inner wall surface of the Faraday cage main body and a part of the wire net, an error easily occurs in the measured charge amount.
【0008】(4)金網面で大粒径粉体もしくは金網の磨
耗が発生し、この磨耗によって帯電起きるため、測定帯
電量に誤差を生ずる恐れがある。(4) The large-diameter powder or the wire mesh is worn on the wire mesh surface, and the wear is caused by the wear, which may cause an error in the measured charge amount.
【0009】(5)試料粉体と接触相手粉体との間の摩擦
帯電量が大きくなるに伴って、分離に時間がかかるだけ
でなく、ときには分離できない場合もあり、迅速な測定
や適切な測定が困難である。(5) As the amount of triboelectric charge between the sample powder and the contact partner powder increases, not only does the separation take time, but sometimes the separation cannot be performed. Difficult to measure.
【0010】本発明は、上記事情に対処して成されたも
ので、試料粉体の摩擦帯電量を精度よく、かつ迅速に測
定できる粉体の摩擦帯電量測定装置の提供を目的とす
る。SUMMARY OF THE INVENTION The present invention has been made in view of the above circumstances, and an object of the present invention is to provide a device for measuring a triboelectric charge amount of a powder capable of accurately and quickly measuring the triboelectric charge amount of a sample powder.
【0011】[0011]
【課題を解決するための手段】請求項1の発明は、一端
に圧縮気体の吹き込み口を備え、前記一端から他端側に
向かって内径が広大化した筒状の導電金属製のファラデ
ーケージ本体と、前記ファラデーケージ本体の他端に取
り付け具によって着脱自在に架張・装着され、前記ファ
ラデーケージ本体内に収容された試料粉体および接触相
手粉体のうち試料粉体を前記圧縮気体の吹き込みで通過
させる金網と、前記取り付け具に、スペーサーを介して
密着的に配置・装着された吸引部と、前記ファラデーケ
ージ本体内に残存する接触相手粉体の帯電量測定手段と
を備え、前記スペーサー又は前記取り付け具もしくは前
記吸引部の前記スペーサーと当接する端面には、前記吸
引部における試料粉体の吸引路の外周方向に渦流を生じ
させる気体流入溝が形成されている粉体の摩擦帯電量測
定装置である。According to a first aspect of the present invention, there is provided a cylindrical Faraday cage body made of a conductive metal having a compressed gas blowing port at one end and having an inner diameter that increases from one end to the other end. If, taken to the other end of the Faraday cage body
Ri attached tool detachably be stretched, attached by a wire mesh passing a sample powder of the file <br/> Radekeji sample powder and the contact partner powder housed in the body by blowing the compressed gas , To the fixture via a spacer
A contact arranged-loaded suction unit, and a contact mating powder charge amount measuring means for remaining in the Faraday cage body, the spacer or the fitting or pre
An end surface of the suction portion that contacts the spacer is provided with the suction member.
A vortex is generated in the direction of the outer circumference of the sample powder suction path in the drawing section
This is a device for measuring the amount of triboelectric charge of powder having a gas inflow groove to be formed .
【0012】[0012]
【0013】[0013]
【0014】本発明は、少なくとも一端に金網が架帳
(架設)されたファラデーゲージ本体内に、摩擦帯電さ
せた試料粉体および接触相手粉体を収容し、これに圧縮
気体を吹き込んで金網を通して一方の粉体を選択的に吹
き飛ばとともに、ファラデーゲージ本体内に残った粉体
の帯電量を測定する装置の改良である。すなわち、ブロ
ーフロー方式の摩擦帯電量測定装置において、目開きを
通して粉体を吹き飛ばす金網面に沿わせて水平の方向に
渦流気体を発生させる気体供給手段を付設した点で特徴
付けられる。According to the present invention, a frictionally charged sample powder and a contact partner powder are accommodated in a Faraday gauge body having a wire mesh at least at one end, and compressed gas is blown into the powder to pass through the wire mesh. It is an improvement of a device for selectively blowing off one powder and measuring the charge amount of the powder remaining in the Faraday gauge body. That is, in the blow flow type triboelectric charge amount measuring apparatus, it is characterized in that gas supply means for generating a swirling gas in a horizontal direction along a wire mesh surface that blows powder through an aperture is additionally provided.
【0015】そして、この発明は、次のような知見に基
づいてなされたものである。すなわち、本発明者らは、
上記問題点の解決・解消に対応して鋭意研究・検討を重
ねた結果、ファラデーケージ本体内およびその外側を含
めた気体の流れを適正に制御した場合、 (a)試料粉体お
よび接触相手粉体の分離効率が向上すること、また、
(b)分離した試料粉体が効率よく吹き飛ばし除去される
こと、 (c)前記の (a)および (b)に伴って従来見られな
かったレベルの高い精度の測定が可能になることを見出
して、本発明に係る粉体の摩擦帯電量測定装置を提供す
るに至ったものである。[0015] The present invention has been made based on the following findings. That is, the present inventors,
As a result of intensive research and examination in response to the resolution and resolution of the above problems, when the flow of gas including the inside and outside of the Faraday cage body was properly controlled, (a) sample powder and contact partner powder Improved body separation efficiency,
(b) It has been found that the separated sample powder is efficiently blown off and removed, and (c) it is possible to measure at a high level of accuracy that has not been seen conventionally with (a) and (b). Thus, the present invention provides a powder triboelectric charge measuring device according to the present invention.
【0016】本発明において、ファラデーゲージ本体
は、一般的に、圧縮気体の吹き込み口を備えた一端側か
ら金網を装着した他端側にその内径が広大化る構成を採
った筒状体を成している。そして、この筒状体は、たと
えば軸方向に分割された複数個の筒状体片を係合・組み
合わせた構成としてもよい。また、金網の装着は、前記
筒状体の他端側に配置し、この他端側に係合可能な取り
付け具を装着することによって行ってもよいし、あるい
は前記筒状体の他端側を縮径した形とて、その内側面に
配置する着脱可能な構成としてもよい。In the present invention, the Faraday gauge body is generally a cylindrical body having a configuration in which the inside diameter is widened from one end provided with a compressed gas blowing port to the other end provided with a wire mesh. are doing. The tubular body may have a configuration in which, for example, a plurality of tubular body pieces divided in the axial direction are engaged and combined. The wire mesh may be mounted on the other end of the tubular body by attaching a fitting that can be engaged with the other end, or the other end of the tubular body. May have a reduced diameter, and may be configured to be removable on the inner surface thereof.
【0017】さらに、金網面に沿わせて水平の方向に渦
流気体を発生させる気体供給手段は、たとえば取り付け
具,筒状体の縮径部,専用スペーサーもしくは気体吸引
筒の端面部に、孔や溝ないし段差を接線方向に設置する
ことにより容易に付設できる。そして、この渦流気体を
発生させる気体供給手段は、ファラデーゲージ本体から
のブローフロー量などによっても異なるが、ブローフロ
ーの口径が20〜60mm程度の場合、たとえば取り付け具
面,筒状体の縮径部端面,専用スペーサー面もしくは気
体吸引筒の端面に 0.3〜 2.0mm程度のギャップができる
ような段差をほぼ等間隔に設定すればよい。Further, the gas supply means for generating swirling gas in the horizontal direction along the surface of the wire mesh includes, for example, a hole, a hole or a hole in the end face of the fitting, the reduced diameter portion of the cylindrical body, the dedicated spacer or the gas suction cylinder. The grooves or steps can be easily provided by tangentially installing them . Their to, gas supply means for generating the vortex gas, etc. but blow flow amount from the Faraday cage body, the diameter of the blow flow when about 20 to 60 mm, for example fitting surface, of the cylindrical body Steps may be set at substantially equal intervals so that a gap of about 0.3 to 2.0 mm is formed on the end face of the reduced diameter portion, the dedicated spacer face, or the end face of the gas suction cylinder.
【0018】[0018]
【発明の実施の形態】以下図1〜図4を参照して実施例
を説明する。The reference to examples below FIGS PREFERRED EMBODIMENTS be described.
【0019】図1は、本発明の一実施例に係る粉体の摩
擦帯電量測定装置の要部構成を示す断面図である。この
実施例では、試料粉体5のブローオフ側に吸引部10を密
着的に取り付けた構成を採っている。すなわち、導電性
材料製の、一端から他端側に向かって内径が広大化した
筒状のファラデーケージ本体1の一端(内径の小さい
側)に圧縮気体ノズル2が装着され、また、金網3が、
前記ファラデーケージ本体1の他端(内径の大きい側)
に取り付け具4によって着脱可能に架張・装着された構
成を採っている。そして、前記取り付け具4に対して、
気体吹き込み溝(ギャップ)7を備えたスペーサー11を
介して吸引部10の一端を密着的に配置・装着したもので
ある。ここで、スペーサー11の気体吹き込み溝(ギャッ
プ)7は、取り付け具4下端面との間に、 0.2〜 2.0mm
程度の段差でほぼ等間隔に接線方向のギャップを形成す
る形で設けられている。FIG. 1 is a cross-sectional view showing the configuration of a main part of a device for measuring the triboelectric charge amount of a powder according to one embodiment of the present invention. In this embodiment, a configuration is adopted in which the suction unit 10 is closely attached to the blow-off side of the sample powder 5. That is, the compressed gas nozzle 2 is attached to one end (the smaller inner diameter side) of a cylindrical Faraday cage body 1 made of a conductive material and having an inner diameter that increases from one end to the other end side. ,
The other end of the Faraday cage body 1 (the side with the larger inner diameter)
A configuration is adopted in which it is stretched and attached detachably by the attachment 4. And, for the mounting fixture 4,
One end of the suction unit 10 is closely arranged and mounted via a spacer 11 having a gas blowing groove (gap) 7. Here, the gas blowing groove (gap) 7 of the spacer 11 is between 0.2 mm and 2.0 mm
It is provided in such a manner that tangential gaps are formed at substantially equal intervals with a level difference.
【0020】すなわち、専用スペーサー11は、図2に平
面的に示すごとく、試料粉体5の吸引路12の外周方向に
吸引・ブローオフ流の渦流13を生ずるような、深さ 0.2
〜 2.0mm程度の気体流入(気体吸い込み)溝7が形設さ
れている。そして、試料粉体5の摩擦帯電量測定時にお
いては、ファラデーケージ本体1に装着した取り付け具
4と吸引部10の一端とをスペーサー11を介して密着させ
た状態とし、圧縮気体のブローおよび吸引を同時に行う
と、金網3の目開きを通して吹き飛ばされた試料粉体
(たとえばトナー粒子)5は、スペーサー11から吸い込
まれる(吹き込む)気流によって発生した渦流13によっ
て即座に除去される。That is, as shown in plan view in FIG. 2, the dedicated spacer 11 has a depth of 0.2 so as to generate a vortex 13 of a suction / blow-off flow in the outer peripheral direction of the suction path 12 for the sample powder 5.
Gas flow of about ~ 2.0 mm (suction gas form) groove 7 is Katachi設. At the time of measuring the triboelectric charge amount of the sample powder 5, the fitting 4 attached to the Faraday cage body 1 and one end of the suction unit 10 are brought into close contact with each other via the spacer 11, and blow and suction of the compressed gas are performed. Is performed simultaneously, the sample powder (for example, toner particles) 5 blown off through the openings of the wire netting 3 is immediately removed by the vortex 13 generated by the air flow sucked (blown) from the spacer 11.
【0021】さらに、8はコンデンサー(容量C)、9
はエレクトロメーターであり、前記ファラデーケージ本
体1外に吹き飛ばされた後、ファラデーケージ本体1側
に残っている電荷による充電電圧から試料粉体5の帯電
量を測定するものである。すなわち、試料粉体5がファ
ラデーケージ本体1外に持ち去ったと当量で、かつ逆の
電荷が接触相手粉体6に残っている。したがって、この
電荷がファラデーケージ本体1に接続したコンデンサー
8を充電するので、コンデンサー8両端の電圧(V)を
エレクトロメーター9で測定し、試料粉体5の帯電量|
Q|を、|Q|=CVとして求める構成となっている。Further, 8 is a capacitor (capacity C), 9
Is an electrometer for measuring the charge amount of the sample powder 5 from the charge voltage due to the charge remaining on the Faraday cage body 1 after being blown out of the Faraday cage body 1. That is, when the sample powder 5 is taken out of the Faraday cage main body 1, an equivalent amount of an opposite charge remains on the contact partner powder 6. Therefore, since this charge charges the capacitor 8 connected to the Faraday cage body 1, the voltage (V) across the capacitor 8 is measured by the electrometer 9, and the charge amount of the sample powder 5 |
Q | is obtained as | Q | = CV.
【0022】なお、この実施例では、スペーサー11に気
体吸い込み溝7を形設した構成を示したが、取り付け具
4もしくは吸引部10の一端面にほぼ等間隔、かつ接線方
向に段差をつけ、スペーサ11面との間にギャップを設け
て気体吸い込み溝7とする構成を採ってもよいし、ま
た、気体吸い込み溝7の代りに、細孔を設けこの細孔か
ら吸引気体が吸い込まれる(流入する)ようにしてもよ
い。いずれにしても、吸引気体の吹き出し路12の外周方
向に、吸引気体による渦流13を生ずるように設置する
と、試料粉体5の除去効率が最も高いことが確認され
た。また、この実施例の場合は、気体吸い込み溝7から
吸引(流入)される気体の圧力がポイントとなり、試料
粉体5をより効率よく除去するためには 300〜3000mmAq
程度の範囲が望ましい。In this embodiment, the structure in which the gas suction groove 7 is formed in the spacer 11 is shown. However, a step is provided at substantially equal intervals and tangentially on one end surface of the attachment 4 or the suction portion 10. The gas suction groove 7 may be formed by providing a gap between the spacer 11 and the surface of the spacer 11. Alternatively, a fine hole may be provided instead of the gas suction groove 7, and the suction gas may be sucked from the fine hole. Do). In any case, it was confirmed that the sample powder 5 was most efficiently removed when it was installed in the outer circumferential direction of the suction gas blowing path 12 so as to generate the vortex 13 due to the suction gas. Further, in the case of this embodiment, the pressure of the gas sucked (inflow) from the gas suction groove 7 is a point, and in order to remove the sample powder 5 more efficiently, 300 to 3000 mmAq
A range of degrees is desirable.
【0023】次に、この実施例に係る摩擦帯電量測定装
置による電子写真用トナーの摩擦帯電量測定例を説明す
る。Next, an example of measuring the triboelectric charge of the electrophotographic toner by the triboelectric charge measuring apparatus according to this embodiment will be described.
【0024】図1に図示した摩擦帯電量測定装置の構成
において、金網3として目開き40μm のステンレス鋼製
の金網を張設したファラデーケージ本体1中に、電子写
真用のトナー・キャリア混合体を収容した。その後、口
径 3mmの圧縮気体吹き込み口2から 0.4Kg/cm2 の圧縮
空気を吹き付けると同時に、吸引部11を2000mmAqの圧力
で吸引し、金網3の目開きを通してトナー粉体(トナー
粒子)を吸引部10側にブローフローさせた。In the configuration of the apparatus for measuring the amount of triboelectric charge shown in FIG . 1 , a toner-carrier mixture for electrophotography is placed in a Faraday cage body 1 in which a stainless steel wire mesh having an aperture of 40 μm is stretched as a wire mesh 3. Housed. Then, at the same time as blowing compressed air of 0.4 kg / cm2 from the compressed gas blowing port 2 having a diameter of 3 mm, the suction part 11 is sucked at a pressure of 2000 mmAq, and the toner powder (toner particles) is sucked through the opening of the wire mesh 3. Blow flow to 10 side.
【0025】この過程において、ファラデーケージ本体
1に接続されたエレクトロメーター9で測定された帯電
量は、圧縮気体吹き込み口2からの圧縮気体吹き付けと
ともに増加し、 3秒後にはファラデーケージ本体1内の
トナー粉体5の全てが吹き飛ばされて測定帯電量が飽和
した。試料(トナー・キャリア混合体)を充填した状態
でのファラデーケージの重量を、前記摩擦帯電量を測定
する前後で測定したところ、ブロー時間 3秒後の重量差
は試料粉体5の重量に相当する値を示し、試料中のトナ
ー粉体5がほぼ完全に吹き飛ばされていることが確認さ
れた。また、前記摩擦帯電量測定後のファラデーケージ
本体1下端部および金網3の下面には全くトナーが付着
しておらず試料粉体5の除去効果が非常にすぐれている
ことが分かった。In this process, the charge amount measured by the electrometer 9 connected to the Faraday cage body 1 increases with the blowing of the compressed gas from the compressed gas blowing port 2, and after 3 seconds, the charge inside the Faraday cage body 1 is increased. All of the toner powder 5 was blown off and the measured charge amount was saturated. When the weight of the Faraday cage with the sample (toner / carrier mixture) filled was measured before and after the measurement of the triboelectric charge, the difference in weight after 3 seconds of blowing time was equivalent to the weight of the sample powder 5. It was confirmed that the toner powder 5 in the sample was almost completely blown off. Further, no toner adhered to the lower end of the Faraday cage main body 1 and the lower surface of the wire mesh 3 after the measurement of the triboelectric charge amount, and it was found that the effect of removing the sample powder 5 was excellent.
【0026】一方、比較のため、従来の摩擦帯電量測定
装置(金網の下面に沿って渦流れを発生させる機構を備
えていない)によって、前記と同じ条件で摩擦帯電量の
測定を行った。この場合は、帯電量が飽和に達するまで
に、20秒以上を必要としただけでなく、飽和帯電量も実
施例の場合に比べて約 1.5倍の値になった。この帯電量
の差は、ファラデーケージ本体内の全トナーが、金網の
目開きを通してファラデーケージ本体外に吹き飛ばされ
るまでに、キャリアとの分離接触を複数回繰り返したこ
とによる摩擦帯電分に起因するものであるといえる。On the other hand, for comparison, the triboelectric charge amount was measured under the same conditions as above using a conventional triboelectric charge amount measuring device (not provided with a mechanism for generating a vortex flow along the lower surface of the wire mesh). In this case, it took not less than 20 seconds for the charge amount to reach saturation, and the saturation charge amount was also about 1.5 times the value in the example. This difference in the amount of charge is due to the frictional charge due to the repeated contact and separation with the carrier several times before all the toner in the Faraday cage body is blown out of the Faraday cage body through the mesh of the wire mesh. You can say that.
【0027】図3および図4は、上記図1に図示した摩
擦帯電量測定装置および従来の摩擦帯電量測定装置によ
る測定例を比較して示したものである。図3は、正帯電
系トナー(スチレンアクリル系高硬度トナー)を試料粉
末として摩擦帯電量を測定したときの測定時間と測定値
の関係で、曲線Aは実施例の測定装置による場合を、曲
線aは従来の測定装置による場合をそれぞれ示す。ま
た、図4は負帯電系トナー(シリカ系外添剤を含むポリ
エステル系トナー)を試料粉末として摩擦帯電量を測定
したときの測定時間と測定値の関係で、曲線Bは実施例
の測定装置による場合を、曲線bは従来の測定装置によ
る場合をそれぞれ示す。 FIGS. 3 and 4 show a comparison between measurement examples using the frictional charge measuring device shown in FIG. 1 and a conventional frictional charge measuring device. FIG. 3 shows the relationship between the measurement time and the measured value when the triboelectric charge amount was measured using a positively charged toner (styrene-acrylic high-hardness toner) as a sample powder. a shows the case of the conventional measuring device. FIG. 4 shows the relationship between the measurement time and the measured value when the triboelectric charge amount was measured using a negatively charged toner (a polyester-based toner containing a silica-based external additive) as a sample powder. And the curve b shows the case of the conventional measuring device.
【0028】図3および図4の特性比較から分かるよう
に、本発明の摩擦帯電量測定装置の場合は、速やかに、
かつ精度よく摩擦帯電量を測定できる。As can be seen from the comparison of the characteristics shown in FIGS. 3 and 4 , in the case of the triboelectric charge measuring device of the present invention,
In addition, the amount of triboelectric charge can be accurately measured.
【0029】また、この摩擦帯電量測定においては、測
定前後の試料の重量減少が試料粉体の量より大きく、ブ
ロー操作によって、金網面でキャリア表面が磨耗を生じ
ていることを示す。さらに、測定後ファラデーケージ本
体下端部に僅かのトナーが再付着しており、試料粉体を
完全に除去することが困難であることも確認された。な
お、本発明は、上記実施例に限定されるものでなく、発
明の趣旨を逸脱しない範囲でいろいろの変形を採ること
ができる。たとえば、金網面に沿って渦流を発生させる
ため流入もしくは供給する気体流入路は溝型(隙間)の
他、孔もしくはノズル型などとしてもよい。Further, in the measurement of the amount of triboelectric charging, the weight loss of the sample before and after the measurement is larger than the amount of the sample powder, which indicates that the carrier surface is worn on the wire mesh surface by the blowing operation. Furthermore, after the measurement, a small amount of toner was reattached to the lower end of the Faraday cage body, and it was confirmed that it was difficult to completely remove the sample powder. It should be noted that the present invention is not limited to the above embodiment, and various modifications can be made without departing from the spirit of the invention. For example, the gas inflow path for inflow or supply to generate a vortex along the surface of the wire mesh may be a hole type or a nozzle type in addition to a groove type (gap).
【0030】[0030]
【発明の効果】本発明の粉体帯電量測定装置によれば、
次のような作用・効果が容易に得られ、たとえば高品質
な電子写真画像を再現性よく現像・形成するためのトナ
ーの品質管理を始め、各種の材料の帯電特性の評価など
が容易になる。According to the powder charge measuring device of the present invention,
The following functions and effects can be easily obtained. For example, quality control of toner for developing and forming a high-quality electrophotographic image with good reproducibility and evaluation of charging characteristics of various materials can be easily performed. .
【0031】(1)ファラデーケージ本体内で分離した試
料粉体と接触相手粉体とが静電的に引き合って再び合体
して接触と分離を繰り返す、いわゆるファラデーケージ
本体が1種の摩擦帯電器して働くという作用がなくなる
ので、迅速に、また、正確な摩擦帯電量を測定すること
ができる。(1) The sample powder separated in the Faraday cage body and the contact partner powder electrostatically attract each other and unite again to repeat contact and separation. A so-called Faraday cage body is a kind of friction charger. The triboelectric charge can be measured quickly and accurately.
【0032】(2)試料粉体の選択的な除去効率が高く、
また、ブローオフ操作でも試料粉体とファラデーケージ
本体内壁との摩擦帯電や試料粉体と金網との摩擦帯電を
極少量に抑制できるため、正確な摩擦帯電量を測定する
ことができる。(2) Selective removal efficiency of sample powder is high,
Further, even in the blow-off operation, the frictional charge between the sample powder and the inner wall of the Faraday cage body and the frictional charge between the sample powder and the wire mesh can be suppressed to a very small amount, so that an accurate amount of frictional charge can be measured.
【0033】(3)ファラデーケージ本体内壁や金網の一
部に、分離した試料粉体の付着が回避されるため、測定
帯電量に誤差を生じるおそれもない。(3) Since the separated sample powder is prevented from adhering to the inner wall of the Faraday cage body or a part of the wire net, there is no possibility that an error occurs in the measured charge amount.
【0034】(4)金網面において、接触相手方粉体もし
くは金網の磨耗発生や、磨耗による帯電量の発生で、測
定帯電量に誤差が生ずることもないので、正確な摩擦帯
電量を測定することができる。(4) There is no error in the measured charge amount due to the occurrence of abrasion of the contact partner powder or the wire mesh on the wire mesh surface or the generation of the charge amount due to the abrasion. Can be.
【図1】実施例の摩擦帯電量測定装置の要部構成を示す
断面図。FIG. 1 is a cross-sectional view illustrating a configuration of a main part of a triboelectric charge amount measuring device according to an embodiment.
【図2】図1の摩擦帯電量測定装置における気体流入手
段の配設状態を示す平面図。FIG. 2 is a plan view showing an arrangement state of gas inflow means in the frictional charge amount measuring device of FIG. 1;
【図3】 実施例の摩擦帯電量測定装置による正帯電系ト
ナーの摩擦帯電量の測定特性を従来の摩擦帯電量測定装
置による場合と比較して示す特性図。 FIG. 3 is a characteristic diagram showing a measurement characteristic of a triboelectric charge amount of a positively charged toner by the triboelectric charge amount measuring device of the embodiment in comparison with a case of using a conventional triboelectric charge amount measuring device.
【図4】 実施例の摩擦帯電量測定装置による負帯電系ト
ナーの摩擦帯電量の測定特性を従来の摩擦帯電量測定装
置による場合と比較して示す特性図。 FIG. 4 is a characteristic diagram showing measurement characteristics of a triboelectric charge amount of a negatively charged toner by the triboelectric charge amount measurement device of the embodiment, in comparison with a case of using a conventional triboelectric charge amount measurement device.
1……ファラデーケージ本体 2……圧縮気体吹き込み口(ノズル) 3……金網 4……取り付け具 5……試料粉体(粒径小) 6……接触相手方粉体(粒径大) 7……気体流入手段 8……コンデンサー 9……エレクトロメーター 10……吸引部 11……スペーサー 12……吸引路 13……渦流 DESCRIPTION OF SYMBOLS 1 ... Faraday cage main body 2 ... Compressed gas blowing port (nozzle) 3 ... Wire mesh 4 ... Attachment 5 ... Sample powder (small particle size) 6 ... Contact partner powder (large particle size) 7 ... ... Gas inflow means 8 ... Condenser 9 ... Electometer 10 ... Suction unit 11 ... Spacer 12 ... Suction path 13 ... Swirl
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平7−214454(JP,A) 特開 平3−105265(JP,A) 特開 昭52−84779(JP,A) 実開 平3−68048(JP,U) (58)調査した分野(Int.Cl.7,DB名) G01N 27/60 G01R 29/24 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-7-214454 (JP, A) JP-A-3-105265 (JP, A) JP-A-52-84779 (JP, A) 68048 (JP, U) (58) Field surveyed (Int. Cl. 7 , DB name) G01N 27/60 G01R 29/24
Claims (1)
記一端から他端側に向かって内径が広大化した筒状の導
電金属製のファラデーケージ本体と、 前記ファラデーケージ本体の他端に取り付け具によって
着脱自在に架張・装着され、前記ファラデーケージ本体
内に収容された試料粉体および接触相手粉体のうち試料
粉体を前記圧縮気体の吹き込みで通過させる金網と、前記取り付け具に、スペーサーを介して密着的に配置・
装着された吸引部と、 前記ファラデーケージ本体内に残存する接触相手粉体の
帯電量測定手段とを備え、 前記スペーサー又は前記取り付け具もしくは前記吸引部
の前記スペーサーと当接する端面には、前記吸引部にお
ける試料粉体の吸引路の外周方向に渦流を生じさせる気
体流入溝が形成されている ことを特徴とする粉体の摩擦
帯電量測定装置。1. A cylindrical Faraday cage body made of a conductive metal, having a compressed gas blowing port at one end, and having an inner diameter increasing from the one end to the other end side, and attached to the other end of the Faraday cage body. Depending on the tool
Removably be stretched-mounted, and a wire mesh passing the sample powder in blowing the compressed gas out of the Faraday cage sample powder and the contact partner powder housed in the body, the fixture, the spacer Through close contact
A suction unit mounted thereon ; and a charge amount measuring unit for a contact partner powder remaining in the Faraday cage body , wherein the spacer or the attachment or the suction unit is provided.
The end face that comes into contact with the spacer of
To create a vortex in the outer circumferential direction of the suction path of the sample powder
An apparatus for measuring a triboelectric charge amount of a powder, wherein a body inflow groove is formed .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14548496A JP3347940B2 (en) | 1996-06-07 | 1996-06-07 | Powder triboelectric charge measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14548496A JP3347940B2 (en) | 1996-06-07 | 1996-06-07 | Powder triboelectric charge measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH09329583A JPH09329583A (en) | 1997-12-22 |
| JP3347940B2 true JP3347940B2 (en) | 2002-11-20 |
Family
ID=15386335
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14548496A Expired - Fee Related JP3347940B2 (en) | 1996-06-07 | 1996-06-07 | Powder triboelectric charge measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3347940B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5836004A (en) * | 1997-01-07 | 1998-11-10 | Industrial Technology Research Institute | Differential mode time to digital converter |
| US6686743B2 (en) * | 2000-10-24 | 2004-02-03 | Univation Technologies, Llc | Apparatus for measuring the static charge of flowable solids |
| CZ303324B6 (en) * | 2009-03-05 | 2012-08-01 | Vysoká škola bánská - Technická univerzita Ostrava | Shear cell for measuring dependence of particulate matter internal friction angle on boundary conditions |
| CZ303325B6 (en) * | 2009-03-05 | 2012-08-01 | Vysoká škola bánská - Technická univerzita Ostrava | Measuring cell for measuring friction parameters of particulate matter on boundary conditions |
-
1996
- 1996-06-07 JP JP14548496A patent/JP3347940B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH09329583A (en) | 1997-12-22 |
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