JPH0722719B2 - Particle classification method and apparatus - Google Patents
Particle classification method and apparatusInfo
- Publication number
- JPH0722719B2 JPH0722719B2 JP19356285A JP19356285A JPH0722719B2 JP H0722719 B2 JPH0722719 B2 JP H0722719B2 JP 19356285 A JP19356285 A JP 19356285A JP 19356285 A JP19356285 A JP 19356285A JP H0722719 B2 JPH0722719 B2 JP H0722719B2
- Authority
- JP
- Japan
- Prior art keywords
- electric field
- particle
- field matrix
- linear electrodes
- particles
- 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
Links
- 239000002245 particle Substances 0.000 title claims description 63
- 238000000034 method Methods 0.000 title claims description 14
- 230000005684 electric field Effects 0.000 claims description 39
- 239000011159 matrix material Substances 0.000 claims description 33
- 230000005520 electrodynamics Effects 0.000 description 5
- 239000011148 porous material Substances 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 230000005484 gravity Effects 0.000 description 3
- 239000000843 powder Substances 0.000 description 3
- 239000002994 raw material Substances 0.000 description 3
- 230000000903 blocking effect Effects 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 2
- 239000000428 dust Substances 0.000 description 2
- 239000004698 Polyethylene Substances 0.000 description 1
- 239000004809 Teflon Substances 0.000 description 1
- 229920006362 Teflon® Polymers 0.000 description 1
- 239000004568 cement Substances 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 239000006185 dispersion Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000012717 electrostatic precipitator Substances 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000000819 phase cycle Methods 0.000 description 1
- -1 polyethylene Polymers 0.000 description 1
- 229920000573 polyethylene Polymers 0.000 description 1
- 238000007873 sieving Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Landscapes
- Electrostatic Separation (AREA)
Description
【発明の詳細な説明】 産業上の利用分野 この発明はセメント工業,薬品工業,セラミックス工業
等の粉体工業全般において用いられる粒子分級方法及び
装置に関するものである。TECHNICAL FIELD The present invention relates to a particle classification method and apparatus used in the powder industry in general, such as cement industry, chemical industry, and ceramic industry.
従来の技術 従来、一般にこの種の方法と装置は、重力,風力,遠心
力等の二種以上の力を、空間に浮遊する粒子に、一定方
向及びこれと直角方向等に作用させ、その結果、粒子の
空間軌跡に生ずる差異を利用して分級するのが普通であ
る。2. Description of the Related Art Conventionally, in general, this type of method and apparatus applies two or more types of forces such as gravity, wind force, and centrifugal force to particles suspended in a space in a fixed direction and a direction perpendicular thereto, and as a result, , It is usual to classify by utilizing the difference generated in the spatial trajectory of particles.
発明が解決しようとする問題点 ところが上記従来の方法と装置は次のような問題点を有
している。即ち風力は気流分布の不均一、及び気流変動
にもとづく粒子の軌道擾乱が避けられず、そのため必然
的に分級精度に限界を生じる。Problems to be Solved by the Invention However, the above-mentioned conventional method and apparatus have the following problems. That is, the wind force inevitably causes non-uniform air flow distribution and orbital disturbance of particles due to air flow fluctuations, which inevitably limits the classification accuracy.
又、分級精度の誤差はたとえば遠心力等の作用力に較べ
て風力(空気粘性)のきき方が強くなる微粉領域では特
に大きくなり、そのため分級粒径(限界粒径)にも越え
がたい下限を生じる。この下限は現在の最高性能の装置
でも5μm前後である。In addition, the error of classification accuracy becomes particularly large in the fine powder region where the wind force (air viscosity) is stronger than the acting force such as centrifugal force, and therefore the lower limit that cannot be exceeded in the classification particle size (limit particle size). Cause This lower limit is around 5 μm even with the current highest performance devices.
この発明はこのような問題を解決するためになされたも
ので、その目的は上記従来のような粒子分級方法よりも
一層高精度な粒子分級方法と装置を提供することであ
る。The present invention has been made to solve such a problem, and an object thereof is to provide a particle classification method and apparatus with higher accuracy than the conventional particle classification methods described above.
問題点を解決するための手段 この発明を実施例を示す図面について述べると、まず装
置については第1図及び7図において、平行に設けられ
た複数の線状電極1から成る電極群2の、少くとも二組
を重合させ、各線状電極1を互に絶縁して交叉させ、該
電極群2間に交流電源3を接続し、電界マトリクス4を
形成して成る粒子分級装置である。又粒子分級方法とし
ては上記電界マトリクスに被分級粒子を供給するもので
ある。Means for Solving the Problems With reference to the drawings showing an embodiment of the present invention, first, regarding the apparatus in FIGS. 1 and 7, an electrode group 2 composed of a plurality of linear electrodes 1 arranged in parallel, This is a particle classifying apparatus in which at least two sets are polymerized, the linear electrodes 1 are insulated from each other and crossed, an AC power source 3 is connected between the electrode groups 2, and an electric field matrix 4 is formed. As a particle classification method, particles to be classified are supplied to the electric field matrix.
そして前記交流電源3は第1図に示すように単相交流電
源でもよく、又は第5図あるいは第7図に示すように三
相交流電源でもよく、図示は省略するが、三相交流電源
を含む多相交流電源でもよい。又前記線状電極1の交叉
は第6図に示すように単に重合したものでもよく、又は
第1図に示すように他の電極群2の線状電極1と上下方
向において交互に位置を替えてなされていてもよい。即
ち織り合わされていてもよい。又、好ましくは第12図、
第14図に示すように前記電界マトリクス4に連通する供
給粒子の通路5に、粒子に電荷を与える荷電装置6が設
けられるが、これは後述のようになくても差支えはな
い。又前記電界マトリクス4は大気よりも高い気圧の中
に設けられていてもよく、又空気以外のガス、又は同ガ
スと空気の混合気体中に設けられていてもよい。The AC power supply 3 may be a single-phase AC power supply as shown in FIG. 1 or a three-phase AC power supply as shown in FIG. 5 or FIG. It may be a multi-phase AC power source including. Further, the crossovers of the linear electrodes 1 may be simply polymerized as shown in FIG. 6, or as shown in FIG. 1, the positions of the linear electrodes 1 of another electrode group 2 may be alternately changed in the vertical direction. May be done. That is, it may be woven. Also, preferably, FIG.
As shown in FIG. 14, a path 5 for supplying particles communicating with the electric field matrix 4 is provided with a charging device 6 for giving an electric charge to the particles, but this may be omitted as will be described later. Further, the electric field matrix 4 may be provided in a pressure higher than the atmosphere, or may be provided in a gas other than air or a mixed gas of the same gas and air.
作 用 被分級粒子をそのまま、又は粒子荷電装置6により荷電
させて、これを風力、又は重力等により前記電界マトリ
クス4に供給する。被分級粒子は電界マトリクス4に接
近し、接触帯電により、又は荷電装置6により予め荷電
させられており、一方電界マトリクス4は前記のように
電界を形成しており、第3図及び第4図に示すような電
気力線7を発生させている。そしてこの電気力線7は交
番的にその方向を変化させている。このため前記供給さ
れた粒子のうち、ある粒径以上の粒径をもつ粒子8は、
その荷電により第3図に示すように弧状の電気力線7上
において、電気力線7に沿って振動し、その結果矢印A8
方向の遠心力を受け、このため第3図においては電界マ
トリクス4上に浮遊させられている。一方、上記粒子8
よりも小径の粒子9はその表面積が小さいため荷電量が
粒子8よりも小さく、このため電界マトリクス4の、上
記のような電気力学的な阻止力を受けることが少く、従
って電界の弱い電気力学的細孔10を通過する。こうして
分級が行われる。又第5図に示すように交流電源3とし
て三相交流電源を用いたものは電界マトリクス4にいわ
ゆる進行波型電界カーテンを形成でき、例えば前記のよ
うにして電界マトリクス4上に浮遊した粒子8をその相
順の方向に移動させることができるようになっている。
このようにすれば、通過を阻止された粒子の集収を早め
ることができよう。The particles to be classified are charged as they are or charged by the particle charging device 6, and are supplied to the electric field matrix 4 by wind force, gravity or the like. The particles to be classified approach the electric field matrix 4 and have been precharged by contact charging or by the charging device 6, while the electric field matrix 4 forms the electric field as described above, and FIGS. The lines of electric force 7 as shown in are generated. The lines of electric force 7 are alternating in direction. Therefore, among the supplied particles, the particles 8 having a particle size larger than a certain particle size are
As a result of the charging, as shown in FIG. 3, the electric field line 7 has an arcuate shape and vibrates along the electric field line 7, resulting in arrow A8.
It is subjected to a directional centrifugal force and is therefore suspended above the electric field matrix 4 in FIG. On the other hand, the particles 8
Since the surface area of the particle 9 is smaller than that of the particle 8, the amount of electric charge is smaller than that of the particle 8. Therefore, the electromotive force of the electric field matrix 4 as described above is less likely to occur, and therefore the electrodynamics of the electric field is weaker. Through the target pore 10. In this way, classification is performed. Further, as shown in FIG. 5, the one using a three-phase AC power source as the AC power source 3 can form a so-called traveling wave type electric field curtain in the electric field matrix 4, and for example, particles 8 suspended on the electric field matrix 4 as described above. Can be moved in the direction of the phase sequence.
This would speed up the collection of particles that were blocked from passing.
実施例 第8図、第9図に示すものはあや織とした電界マトリク
スを、第10図、第11図に示すものは朱子織とした電界マ
トリクス4を示す。又これらは定在波型電界マトリクス
を示している。又前記線状電極1は一例としてテフロ
ン、ポリエチレン等の絶縁体で被覆された電線が用いら
れた。Example FIGS. 8 and 9 show a twill weave electric field matrix, and FIGS. 10 and 11 show a satin weave electric field matrix 4. These also show standing wave type electric field matrices. As the linear electrode 1, for example, an electric wire coated with an insulator such as Teflon or polyethylene is used.
第12図に示すものは定在波型の電界マトリクス4を円筒
状に形成し、上部に荷電装置6としてコロナ放電極6aと
対向電極6bを設けた分級装置である。原料は口部11から
入り荷電装置6で荷電され、そのうちある粒径以下の粒
子9は電界マトリクス4の電気力学的細孔10を通過し、
出口12から製品として回収される。一方電界マトリクス
4の阻止力を強く受ける、粒子9よりも大きい粒子8は
重力により降下し、排出口13から排出されるようになっ
ている。なおこの分級は電界マトリクス4に印加する交
番電圧、及び周波数を変えることにより粒子の篩分け
(いわゆる分級点)の調節ができる。なお電界マトリク
ス4は交流電圧に直流電圧を重畳して与えてもよい。What is shown in FIG. 12 is a classifying device in which a standing wave type electric field matrix 4 is formed in a cylindrical shape and a corona discharge electrode 6a and a counter electrode 6b are provided as a charging device 6 on the upper part. The raw material enters through the mouth portion 11 and is charged by the charging device 6, of which particles 9 having a particle size smaller than a certain size pass through the electrodynamic pores 10 of the electric field matrix 4,
Collected as a product from the outlet 12. On the other hand, the particles 8 larger than the particles 9 which are strongly affected by the blocking force of the electric field matrix 4 descend by gravity and are discharged from the discharge port 13. In this classification, the sieving of particles (so-called classification point) can be adjusted by changing the alternating voltage and frequency applied to the electric field matrix 4. The electric field matrix 4 may be applied by superimposing a DC voltage on an AC voltage.
第14図に示すものは電界マトリクス4を平面状に形成
し、傾斜させられており、電気力学的阻止力を強く受け
た粒子8は電界マトリクス4上を降下し、ホッパ14に入
り、それよりも小さい粒子9は電気力学的細孔10を通過
して製品ホッパ15に入り分級される。第15図に示すもの
は原料ホッパ16から供給機17を通して予備荷電部18に入
り、荷電部19に入る前にその濃度を粉塵濃度計20で検出
し、その出力を供給機17へフイードバックし、荷電部19
への粉塵負荷を一定にする。荷電部19で帯電された粒子
は電界マトリクス4を設けた分級室21に入り、電気力学
的細孔10を通過した微粒子は電気集塵機22で回収され
る。補集されなかった粒子は再び供給機17へ送る。そし
てこの装置は閉回路方式であるので高気圧環境とするこ
とができ、充分に高い電圧で、電界マトリクス4を運転
することができるようになっている。このため第19図に
示すような高気圧空気の環境下での分級特性を期待する
ことができる。In the structure shown in FIG. 14, the electric field matrix 4 is formed in a flat shape and is inclined, and the particles 8 which are strongly subjected to the electrodynamic blocking force descend on the electric field matrix 4 and enter the hopper 14, The smaller particles 9 pass through the electrodynamic pores 10 and enter the product hopper 15 for classification. The one shown in FIG. 15 enters the preliminary charging section 18 from the raw material hopper 16 through the feeder 17 and detects its concentration with the dust densitometer 20 before entering the charging section 19, and feed back its output to the feeder 17. Charged part 19
To keep the dust load on the surface constant. The particles charged by the charging unit 19 enter the classification chamber 21 provided with the electric field matrix 4, and the particles passing through the electrodynamic pores 10 are collected by the electrostatic precipitator 22. The particles not collected are sent again to the feeder 17. Since this device is a closed circuit system, it can be set in a high pressure environment, and the electric field matrix 4 can be operated at a sufficiently high voltage. Therefore, it is possible to expect classification characteristics under the environment of high-pressure air as shown in FIG.
第16図〜第18図に示すものは、第15図における予備荷電
部18の説明図であり、第18図に示すように、電圧が印加
された被覆電極の表面は、正又は負の電位を持ってお
り、無電荷の粒子が何組かこのような荷電層を接触通過
することにより帯電粒子となる。そこで第17図に示すよ
うに電界マトリクス4を何層にもロール状に形成したも
のを作り、かつ第16図に示すケーシング23内に設け、入
口11から進入した無電荷粒子が出口12を出る迄にある程
度電荷をもった粒子になる。これは粒子の予備荷電と、
分級精度を向上させるための、原料粉の分散を良好にす
ることができるようになっている。FIG. 16 to FIG. 18 are explanatory views of the preliminary charging unit 18 in FIG. 15, and as shown in FIG. 18, the surface of the coated electrode to which a voltage is applied has a positive or negative potential. And several sets of uncharged particles come into contact with such a charged layer to become charged particles. Therefore, as shown in FIG. 17, the electric field matrix 4 is formed in a roll shape in many layers, and is provided in the casing 23 shown in FIG. 16 so that the uncharged particles entering from the inlet 11 exit from the outlet 12. By the time it becomes a particle with a certain amount of charge. This is the precharge of the particles,
It has become possible to improve the dispersion of the raw material powder in order to improve the classification accuracy.
発明の効果 この発明は前記のように構成されたことにより前記従来
の方法より一層分級精度の高い分級方法と装置を提供す
ることができる。EFFECTS OF THE INVENTION Since the present invention is configured as described above, it is possible to provide a classification method and apparatus having higher classification accuracy than the conventional method.
第1図はこの発明の実施例を示し、粒子分級装置の概略
を示す図、第2図は第1図のII−II線矢視図、第3図は
この発明の原理的説明図、第4図は同じくこの発明の原
理的説明図、第5図はこの発明の第2の実施例を示し第
2図に相当する図、第6図は同第3の実施例を示し粒子
分級装置の部分の斜視図、第7図は同第4の実施例を示
し第1図に相当する図、第8図は同第5の実施例を示
し、第1図に相当する図、第9図は第8図のIX−IX線矢
視図、第10図はこの発明の第6の実施例を示し、第1図
に相当する図、第11図は第10図のXI−XI線矢視図、第12
図はこの発明の第7の実施例を示し粒子分級装置の断面
図、第13図は第12図のXIII−XIII線部断面図、第14図は
この発明の第8の実施例を示し、第12図に相当する図、
第15図は同第9の実施例を示し粒子分級装置の概略を示
す図、第16図は第15図に示す装置の予備荷電部18の詳細
断面図、第17図は第16図のXVII−XVII線部断面図、第18
図は第17図に示す装置の作用の説明図、第19図は第15図
に示す装置を運転した際の期待される分級特性の1例を
示すグラフである。 1……線状電極 2……電極群 3……交流電源 4……電界マトリクスFIG. 1 shows an embodiment of the present invention, showing an outline of a particle classifier, FIG. 2 is a view taken along the line II-II of FIG. 1, and FIG. 3 is a principle explanatory view of the present invention. FIG. 4 is a diagram for explaining the principle of the present invention, FIG. 5 is a diagram showing a second embodiment of the present invention and corresponding to FIG. 2, and FIG. 6 is a diagram showing the third embodiment of the present invention. FIG. 7 is a perspective view of a part, FIG. 7 is a view corresponding to FIG. 1 showing the fourth embodiment, FIG. 8 is a view showing the fifth embodiment, a view corresponding to FIG. 1, and FIG. 8 is a view taken along the line IX-IX of FIG. 8, FIG. 10 shows a sixth embodiment of the present invention, and is a view corresponding to FIG. 1, and FIG. 11 is a view taken along the line XI-XI of FIG. , 12th
FIG. 7 is a sectional view of a particle classifier showing a seventh embodiment of the present invention, FIG. 13 is a sectional view taken along line XIII-XIII of FIG. 12, and FIG. 14 is an eighth embodiment of the present invention. Figure corresponding to Figure 12,
FIG. 15 is a view showing the outline of a particle classifying apparatus according to the ninth embodiment, FIG. 16 is a detailed sectional view of a preliminary charging section 18 of the apparatus shown in FIG. 15, and FIG. 17 is a XVII of FIG. -XVII line sectional view, 18th
17 is an explanatory view of the operation of the device shown in FIG. 17, and FIG. 19 is a graph showing an example of expected classification characteristics when the device shown in FIG. 15 is operated. 1 ... Linear electrode 2 ... Electrode group 3 ... AC power supply 4 ... Electric field matrix
Claims (14)
電極群の、少なくとも二組を重合させ、各組の線状電極
を互いに絶縁して交叉させ、該電極群間に交流電圧を印
加して電界マトリクスを形成し、該電界マトリクスに被
分級粒子を供給することを特徴とする粒子分級方法。1. An electrode group consisting of a plurality of linear electrodes arranged in parallel, at least two sets of which are superposed, and the linear electrodes of each set are insulated and crossed from each other, and an AC voltage is applied between the electrode groups. A particle classification method, which comprises applying an electric field matrix to supply particles to be classified to the electric field matrix.
と上下方向において交互に位置を替えてなされている特
許請求の範囲第1項記載の粒子分級方法。2. The method for classifying particles according to claim 1, wherein the crossing of the linear electrodes is performed by alternating the positions of the linear electrodes of other electrode groups in the vertical direction.
とを特徴とする特許請求の範囲第1項又は第2項いずれ
か1項記載の粒子分級方法。3. The particle classification method according to claim 1, wherein the particles to be classified to be supplied are charged.
たは双方を可変できる単相交流電圧であることを特徴と
する特許請求の範囲第1項乃至第3項いずれか1項記載
の粒子分級方法。4. The particle classification method according to claim 1, wherein the AC voltage is a single-phase AC voltage whose frequency and / or applied voltage can be varied. .
たは双方を可変できる多相交流電圧であることを特徴と
する特許請求の範囲第1項乃至第3項いずれか1項記載
の粒子分級方法。5. The particle classification method according to claim 1, wherein the AC voltage is a polyphase AC voltage capable of varying one or both of frequency and applied voltage. .
体中に設けられていることを特徴とする特許請求の範囲
第1項乃至第5項いずれか1項記載の粒子分級方法。6. The particle classification method according to any one of claims 1 to 5, wherein the electric field matrix is provided in a gas having a pressure higher than atmospheric pressure.
ガスと空気の混合した大気中に設けられていることを特
徴とする特許請求の範囲第1項乃至第6項いずれか1項
記載の粒子分級方法。7. The electric field matrix according to claim 1, wherein the electric field matrix is provided in a gas other than air, or in the atmosphere in which the gas and air are mixed. Particle classification method.
電極群の、少なくとも二組を重合させ、各組の線状電極
を互いに絶縁して交叉させ、該電極群間に交流電源を接
続し、電界マトリクスを形成することを特徴とする粒子
分級装置。8. An electrode group consisting of a plurality of linear electrodes arranged in parallel is overlapped with at least two sets, and the linear electrodes of each set are insulated and crossed from each other, and an AC power supply is provided between the electrode groups. A particle classifier, which is connected to form an electric field matrix.
と上下方向において交互に位置を替えてなされている特
許請求の範囲第8項記載の粒子分級装置。9. The particle classifying apparatus according to claim 8, wherein the crossing of the linear electrodes is made to alternate with the linear electrodes of another electrode group in the vertical direction.
した粒子の供給通路を有している特許請求の範囲第8項
又は第9項いずれか1項記載の粒子分級装置。10. The particle classification device according to claim 8, wherein the electric field matrix has a particle supply passage communicating with the particle charging device.
または双方を可変できる単相交流電源であることを特徴
とする特許請求の範囲第8項乃至第10項いずれか1項記
載の粒子分級装置。11. The particle classifying apparatus according to claim 8, wherein the AC power supply is a single-phase AC power supply capable of varying one or both of frequency and applied voltage. .
または双方を可変できる多相交流電源であることを特徴
とする特許請求の範囲第8項乃至第10項いずれか1項記
載の粒子分級装置。12. The particle classification device according to claim 8, wherein the AC power supply is a multi-phase AC power supply capable of varying one or both of frequency and applied voltage. .
気体中に設けられていることを特徴とする特許請求の範
囲第8項乃至第12項いずれか1項記載の粒子分級装置。13. The particle classifying apparatus according to claim 8, wherein the electric field matrix is provided in a gas having a pressure higher than atmospheric pressure.
同ガスと空気との混合気体の中に設けられていることを
特徴とする特許請求の範囲第8項乃至第13項いずれか1
項記載の粒子分級装置。14. The electric field matrix is provided in a gas other than air or in a mixed gas of the same gas and air, according to claim 8.
Item particle classifier.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19356285A JPH0722719B2 (en) | 1985-09-02 | 1985-09-02 | Particle classification method and apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19356285A JPH0722719B2 (en) | 1985-09-02 | 1985-09-02 | Particle classification method and apparatus |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6253753A JPS6253753A (en) | 1987-03-09 |
| JPH0722719B2 true JPH0722719B2 (en) | 1995-03-15 |
Family
ID=16310095
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19356285A Expired - Lifetime JPH0722719B2 (en) | 1985-09-02 | 1985-09-02 | Particle classification method and apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0722719B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6438152A (en) * | 1987-08-05 | 1989-02-08 | Ishikawajima Harima Heavy Ind | Classifier for particles by high frequency power source |
| JP2008018340A (en) * | 2006-07-13 | 2008-01-31 | Trinc:Kk | Apparatus for collecting floating material and apparatus for repelling floating material |
| EP3195935B1 (en) * | 2014-08-08 | 2019-04-10 | Shimadzu Corporation | Particle charger |
| JP2017051919A (en) * | 2015-09-10 | 2017-03-16 | 株式会社東芝 | Dust collector |
-
1985
- 1985-09-02 JP JP19356285A patent/JPH0722719B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6253753A (en) | 1987-03-09 |
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