JPS6067867A - Electric field forming apparatus - Google Patents

Electric field forming apparatus

Info

Publication number
JPS6067867A
JPS6067867A JP17671583A JP17671583A JPS6067867A JP S6067867 A JPS6067867 A JP S6067867A JP 17671583 A JP17671583 A JP 17671583A JP 17671583 A JP17671583 A JP 17671583A JP S6067867 A JPS6067867 A JP S6067867A
Authority
JP
Japan
Prior art keywords
cylindrical tube
electric field
range
electrode plate
center
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
JP17671583A
Other languages
Japanese (ja)
Inventor
Seiichiro Hiratsuka
平塚 誠一郎
Satoru Haneda
羽根田 哲
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Konica Minolta Inc
Original Assignee
Konica Minolta Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Konica Minolta Inc filed Critical Konica Minolta Inc
Priority to JP17671583A priority Critical patent/JPS6067867A/en
Publication of JPS6067867A publication Critical patent/JPS6067867A/en
Pending legal-status Critical Current

Links

Landscapes

  • Plasma Technology (AREA)

Abstract

PURPOSE:To generate a uniform electric field over a considerable range in a cylindrical tube, by arranging a pair of electrode plates, to which positive and negative voltages are applied, to the inner wall of the cylindrical tube at positions synmetric around the center of said tube so as to have a circular arc cross- sectional area shape. CONSTITUTION:In an experiment conducted by changing the string length of an electrode plate to 0.4D, 0.5D and 0.6D, at the time of 0.5D, the electric field in a cylindrical tube is most stable. It is experimentally cleared that the electrode plate, which can obtain a uniform electric field within a difference range of about 5% or less with respect to a range of + or -0.05D in left and right X-directions and + or -0.3D in before and behind Y-directions around the center axis 10A of the cylindrical tube 10, has pref. a string of which the length is present in a range of 0.45D<X<0.55D. By using the electrode plate having this range, a considerably stable electric field is obtained in the vicinity of the center axis 10A of the cylindrical tube 10.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、例えば静電記録装置に用いられるトナー粒子
の荷電分布を測定する際等において必要とする、円筒内
部に一様な電界を発生させる電界形成装置の改良に関す
るものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention is directed to generating a uniform electric field inside a cylinder, which is necessary when measuring the charge distribution of toner particles used in an electrostatic recording device, for example. This invention relates to an improvement of an electric field forming device that generates electric fields.

〔従来技術〕[Prior art]

例えば特開昭57−79958号公報による提案は、静
電記録装置に用いられるトナー粒子の荷電分布を測定す
る方法及び装置に関する提案で、チャンバ内に実質的に
一様な電界を形成し、一様な速度の空気層流を発生せし
めて、トナー粒子をチャンバ内に導入し、トナー粒子の
荷電分布を測定するものである。このようなチャンバ内
に一様な電界を発生させるには、従来大型の電界形成装
置を必要としていた。
For example, Japanese Patent Laid-Open No. 57-79958 proposes a method and apparatus for measuring the charge distribution of toner particles used in an electrostatic recording device. Toner particles are introduced into a chamber by generating a laminar flow of air at various speeds, and the charge distribution of the toner particles is measured. Generating a uniform electric field within such a chamber has conventionally required a large electric field generating device.

第1図は之を示したもので、円筒管1の内部に一様な電
界を発生させる電極板の構造としては、得たい一様電界
の領域よりも十分に広い1対の平行極板2A、2B中に
円筒管lを配置したうえ、前記平行極板2A、2Bに電
圧を印加することがなされてきた。
Figure 1 shows this, and the structure of the electrode plates that generate a uniform electric field inside the cylindrical tube 1 consists of a pair of parallel electrode plates 2A that are sufficiently wider than the desired uniform electric field area. , 2B, and a voltage is applied to the parallel polar plates 2A, 2B.

このような電界形成装置にあっては、次の欠点を有して
いた。
Such an electric field forming device has the following drawbacks.

(1) 非常・に広い平行電極板2A、2Bを使用する
ので、広い空間を使用してしまう。
(1) Since the parallel electrode plates 2A and 2B are very wide, a large space is used.

(2)平行電極板2A、2Bは円筒管1の外にあるので
、平行電極板2A、2Bに高電圧をかけている場合、危
険性がある。
(2) Since the parallel electrode plates 2A and 2B are located outside the cylindrical tube 1, there is a danger if a high voltage is applied to the parallel electrode plates 2A and 2B.

〔発明の目的〕[Purpose of the invention]

安全でかつ簡便な電極配置により、円筒管内に可成りの
範囲に亘って一様な電界を発生させる電界形成装置を提
供することを目的とする。
It is an object of the present invention to provide an electric field forming device that generates a uniform electric field over a considerable range within a cylindrical tube by safe and simple electrode arrangement.

〔発明の構成〕[Structure of the invention]

本発明は上記目的を達成しようとするもので、円筒管の
内壁、又は内壁に近接して円筒管中心を中心とした1対
の電極板を設けて、円筒管内に中心部を含む可成りの範
囲に亘って一様な電界を得るようにしたもので、それは 1対の正負に電圧印加する極板が、円筒管の中心を中心
とした対称の位置で、該円筒管の内壁あるいは内壁に近
接して円弧状の断面形状で配置されており、該極板の弦
の長さXが 0.45D< X (0,55D の範囲内にある電界形成装置により達成される。
The present invention aims to achieve the above object, and includes a pair of electrode plates centered on the center of the cylindrical tube on or near the inner wall of the cylindrical tube. A uniform electric field is obtained over a range, and a pair of polar plates that apply positive and negative voltages are placed at symmetrical positions around the center of the cylindrical tube, and are applied to the inner wall or inner wall of the cylindrical tube. This is achieved by an electric field forming device which is arranged closely in an arcuate cross-sectional shape and whose chord length X of the plates is in the range 0.45D<X (0.55D).

ここでDは円筒管の内径とする。Here, D is the inner diameter of the cylindrical tube.

〔実施例〕〔Example〕

第2図は絶縁性の円筒管1oの内壁に沿って、円筒管中
心10Aを中心として設けた1対の円弧状の電極板を、
その電極の大ぎさく円弧の大きさ)を変針で実験を行な
った実験結果を示す。
FIG. 2 shows a pair of arc-shaped electrode plates placed along the inner wall of an insulating cylindrical tube 1o, with the cylindrical tube center 10A as the center.
The results of an experiment were conducted by changing the direction (the size of the large circular arc of the electrode).

円筒管工0の内径をDQするとぎ、第2図(a)の1対
の電極21A、 、 21Bはその電極の弦の長さは0
.4Dとしたもので、第2図(b)の1対の電極22A
 、 22Bはその電極の弦の長さは0.5Dとしたも
ので、第2図(e)の1対の電極23A 、 23Bは
その電極の弦の長さは0.6Dとしたものである。
When the inner diameter of the cylindrical pipework 0 is DQ, the chord length of the pair of electrodes 21A, 21B in Fig. 2(a) is 0.
.. 4D, a pair of electrodes 22A in FIG. 2(b)
, 22B have electrodes with a string length of 0.5D, and the pair of electrodes 23A and 23B in FIG. 2(e) have electrodes with a chord length of 0.6D. .

ここで電極板に印加した電圧■は±500vで、円筒管
lOの内径りは50フ五で実験を行なった。
Here, the experiment was conducted with the voltage (2) applied to the electrode plate at ±500 V, and the inner diameter of the cylindrical tube (10) was 50 mm.

第2図(a)〜(c)の右側のグラフはそれぞれの電極
板を用いたときの円筒管10の中心部10Aと、中心1
10Aから左右方向に0.05D (2,5mm)離れ
た紗上での前後(7)方向の電界強度をそれぞれ実線と
破綜とで示した。
The graphs on the right side of FIGS. 2(a) to (c) show the center 10A of the cylindrical tube 10 and the center 1
The electric field strength in the front-rear (7) direction on the gauze spaced 0.05D (2.5 mm) from 10A in the left-right direction is shown by a solid line and a broken line, respectively.

1対の正極板と負極板によって形成される円筒管10内
の電界は、電極板の弦の長さにより可成り変って(るこ
とが分かる。電極板の弦の長さを0.4D 、 0.5
D 、 0.6Dと変えた第2図に示した実験では、電
極板の弦の長さが0,5Dのとき円筒管10内の電界が
最も安定している。
It can be seen that the electric field within the cylindrical tube 10 formed by a pair of positive and negative electrode plates varies considerably depending on the length of the chord of the electrode plate.If the chord length of the electrode plate is 0.4D, 0.5
In the experiment shown in FIG. 2 where D and 0.6D were changed, the electric field within the cylindrical tube 10 was most stable when the chord length of the electrode plate was 0.5D.

円筒管10の中心軸10Aを中心とした、左右方向±0
.05D、前後(イ)方向±0.3Dの範囲について約
5%以内を差異範囲として一様な電界の得られる電極板
は、電極板の弦の長さXが次の範囲にあることが好まし
いことを実験的に明らかとした。
±0 in the left and right direction around the central axis 10A of the cylindrical tube 10
.. 05D, for an electrode plate that can obtain a uniform electric field with a difference range of within about 5% in the range of ±0.3D in the longitudinal (A) direction, it is preferable that the chord length X of the electrode plate is in the following range. This was experimentally clarified.

0.45D < X (0,55D この範囲の電極板を用いれば、円筒管10内の中心aI
IIOA付近では可成り安定した電界が得られる。
0.45D <
A fairly stable electric field can be obtained near IIOA.

第3図は、本発明の電界形成装置を、トナー粒子の荷電
分布を測定するのに適用した適用例を示したもので、チ
ャンバは円筒状をなした内径りの円筒管10で、この内
壁に0.5Dの弦をなした1対の弧状をした電極板22
A 、 22Bを設けてEV/、Lの電場を形成し、筺
た円筒管10の上端面にはハニカム状のフィルタ33を
通って空気Aは円筒管10内に導入され、流速V&の平
行な層流があるようにしたもので、l゛個宛粒子状態に
分離したトナーTは円筒管10の中心軸10Aの上端の
導入管31から自然に吸入され、落下する。ここでトナ
ー粒子の帯電量をqとすると、 Fe”qE のクーロン力が働ろく。
FIG. 3 shows an example in which the electric field generating device of the present invention is applied to measuring the charge distribution of toner particles. A pair of arc-shaped electrode plates 22 forming a chord of 0.5D.
A and 22B are provided to form an electric field of EV/, L, and air A is introduced into the cylindrical tube 10 through a honeycomb-shaped filter 33 on the upper end surface of the enclosed cylindrical tube 10, and the air A is introduced into the cylindrical tube 10 at a parallel flow rate of V&. Since there is a laminar flow, the toner T separated into 1 particles is naturally sucked in from the introduction tube 31 at the upper end of the central axis 10A of the cylindrical tube 10 and falls. Here, if the amount of charge on the toner particles is q, then the Coulomb force of Fe''qE acts.

また空気の粘性係数をη、トナー粒子半径なr、横方向
速度をVとすれば Fr=6πηrV のストークスの式が成立し、トナーTが長さeだけ落下
し、フィルタ32上に中心軸10Aからd離れた位【に
落下したとすると、 V:Va=d:d j Fr=Fe の関係があるので  6E となる。
Furthermore, if the viscosity coefficient of air is η, the toner particle radius is r, and the lateral velocity is V, then the Stokes equation Fr = 6πηrV holds true, and the toner T falls by a length e and falls onto the filter 32 with the center axis 10A. Assuming that it falls at a distance d from , the relationship is V: Va = d: d j Fr = Fe, so it becomes 6E.

よってフィルタ32上に収集されたトナーは装置外に取
出されて電像解析装置により解析される。
Therefore, the toner collected on the filter 32 is taken out of the apparatus and analyzed by an electromagnetic analyzer.

第4図は上記の解析結果の1例を示すトナーチャージス
ペクトログラムである。
FIG. 4 is a toner charge spectrogram showing an example of the above analysis results.

〔発明の効果〕〔Effect of the invention〕

上記説明で明らかなように、本発明により安全でかつ簡
便な電極配置により、円筒管内に広範囲に亘って一様な
電界を発生させることが可能と1、[った。
As is clear from the above description, the present invention makes it possible to generate a uniform electric field over a wide range within a cylindrical tube by using a safe and simple electrode arrangement.

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

、第1図は円筒管内に一様1よ電界を発生させる従来の
電界形成装誼。第2図(a) 、 (b) 、 (c)
は円筒管内に設けた電極形状を変えたときの円筒管断面
とこの電界強度分布を示すグラフ。第3図は本発明のト
ナー粒子の荷電分布測定装置への適用例。第4図は第3
図による解析結果の1例を示すトナーチャージスペクト
ログラム。 10・・・円筒管 10A−°°中心軸(21A、21
B)、 (22A、 22B)、 (23A、21)・
・・対をなす電極板 D・・・円筒管内径 代理人 桑原義美
, FIG. 1 shows a conventional electric field forming device that generates a uniform electric field within a cylindrical tube. Figure 2 (a), (b), (c)
is a graph showing the cross section of a cylindrical tube and its electric field strength distribution when the shape of the electrode provided inside the cylindrical tube is changed. FIG. 3 is an example of application of the present invention to a toner particle charge distribution measuring device. Figure 4 is the third
A toner charge spectrogram showing an example of graphical analysis results. 10... Cylindrical tube 10A-°° central axis (21A, 21
B), (22A, 22B), (23A, 21)・
...Paired electrode plate D...Cylindrical tube inner diameter agent Yoshimi Kuwahara

Claims (1)

【特許請求の範囲】 1対の正負に電圧印加する極板が、円筒管の中心を中心
とした対称の位置で、該円筒管の内壁あるいは内壁に近
接して円弧状の断面形状で配置されており、該極板の弦
の長さXが 0.45D < x (0,55D の範囲内にある電界形成装置。 ここでDは円筒管の内径とする。
[Scope of Claims] A pair of positive and negative electrode plates for applying voltages are disposed at symmetrical positions about the center of the cylindrical tube and have an arcuate cross-sectional shape on or near the inner wall of the cylindrical tube. and the chord length X of the electrode plate is within the range of 0.45D < x (0.55D), where D is the inner diameter of the cylindrical tube.
JP17671583A 1983-09-22 1983-09-22 Electric field forming apparatus Pending JPS6067867A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17671583A JPS6067867A (en) 1983-09-22 1983-09-22 Electric field forming apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17671583A JPS6067867A (en) 1983-09-22 1983-09-22 Electric field forming apparatus

Publications (1)

Publication Number Publication Date
JPS6067867A true JPS6067867A (en) 1985-04-18

Family

ID=16018491

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17671583A Pending JPS6067867A (en) 1983-09-22 1983-09-22 Electric field forming apparatus

Country Status (1)

Country Link
JP (1) JPS6067867A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61281975A (en) * 1985-06-07 1986-12-12 Fujitsu Ltd Measuring instrument for distribution of toner electric charge quantity

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57202630A (en) * 1981-06-08 1982-12-11 Rikagaku Kenkyusho Electrostatic deflector

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57202630A (en) * 1981-06-08 1982-12-11 Rikagaku Kenkyusho Electrostatic deflector

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61281975A (en) * 1985-06-07 1986-12-12 Fujitsu Ltd Measuring instrument for distribution of toner electric charge quantity

Similar Documents

Publication Publication Date Title
Adachi et al. Unipolar and bipolar diffusion charging of ultrafine aerosol particles
Surugau et al. Electrophoretic methods for separation of nanoparticles
US6004375A (en) Process and apparatus to treat gasborne particles
Intra et al. An overview of unipolar charger developments for nanoparticle charging
JPH05505463A (en) Enhanced capillary zone electrophoresis method and its implementation device
JP6282036B2 (en) Method and control apparatus for controlling movement speed of substance
US3413545A (en) Apparatus and method for determining aerosol particle concentration and particle size distribution
JPH08173841A (en) Electrostatic settling device and method of collecting carbon particle
JP2003337087A (en) Apparatus for collecting suspended particle
US7361212B2 (en) Electrostatic precipitator
US3673463A (en) Methods and apparatus for electrogasdynamic coating
JPS6067867A (en) Electric field forming apparatus
KR20080072928A (en) Aerosol charge neutralizing device
Yazbeck et al. Characterization and manipulation of single nanoparticles using a nanopore-based electrokinetic tweezer
KR101322689B1 (en) Method and system for separating fibrous particles
JP2000046720A (en) Differential electrical-mobility measuring apparatus
WO2017195723A1 (en) Particle charging device
US3518488A (en) Corona discharge charging of particles wherein a porous insulator is disposed between the corona electrodes
CN205317609U (en) Fine particles adsorption equipment
Yen et al. A planar electric curtain used as a device for the control and removal of particulate materials
WO2004103568A1 (en) Particle separation apparatus and method
Stepkina et al. Application of Electrostatic Effect for Cleansing Finely Divided Aerosol from Air
SU748192A1 (en) Method of determining volumetric concentration of aerosol dispersed phase
Belhadj et al. An experimental measurement of corona discharge using laser Doppler velocimetry
Fjeld et al. Electrically enhanced deposition of a confined aerosol in the presence of ionizing radiation