JPH0131428B2 - - Google Patents
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- Publication number
- JPH0131428B2 JPH0131428B2 JP8745484A JP8745484A JPH0131428B2 JP H0131428 B2 JPH0131428 B2 JP H0131428B2 JP 8745484 A JP8745484 A JP 8745484A JP 8745484 A JP8745484 A JP 8745484A JP H0131428 B2 JPH0131428 B2 JP H0131428B2
- Authority
- JP
- Japan
- Prior art keywords
- classification
- solid
- collection
- flow
- electrostatic
- 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
Links
- 239000002245 particle Substances 0.000 claims description 88
- 239000011882 ultra-fine particle Substances 0.000 claims description 47
- 239000000843 powder Substances 0.000 claims description 40
- 238000000034 method Methods 0.000 claims description 14
- 230000007246 mechanism Effects 0.000 claims description 12
- 238000009423 ventilation Methods 0.000 claims 3
- 238000011084 recovery Methods 0.000 description 27
- 239000000428 dust Substances 0.000 description 13
- 150000002500 ions Chemical class 0.000 description 11
- 239000000463 material Substances 0.000 description 10
- 238000005516 engineering process Methods 0.000 description 8
- 230000002776 aggregation Effects 0.000 description 6
- 238000004220 aggregation Methods 0.000 description 6
- 230000009471 action Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 5
- 239000012717 electrostatic precipitator Substances 0.000 description 5
- 230000008569 process Effects 0.000 description 4
- 230000008901 benefit Effects 0.000 description 3
- 230000006399 behavior Effects 0.000 description 2
- 239000012212 insulator Substances 0.000 description 2
- 239000006247 magnetic powder Substances 0.000 description 2
- 229910021332 silicide Inorganic materials 0.000 description 2
- FVBUAEGBCNSCDD-UHFFFAOYSA-N silicide(4-) Chemical compound [Si-4] FVBUAEGBCNSCDD-UHFFFAOYSA-N 0.000 description 2
- 208000011231 Crohn disease Diseases 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 230000001680 brushing effect Effects 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000007599 discharging Methods 0.000 description 1
- 238000010292 electrical insulation Methods 0.000 description 1
- 238000009297 electrocoagulation Methods 0.000 description 1
- 238000005265 energy consumption Methods 0.000 description 1
- 238000003912 environmental pollution Methods 0.000 description 1
- 238000007667 floating Methods 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 230000001771 impaired effect Effects 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 229920003023 plastic Polymers 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 230000002250 progressing effect Effects 0.000 description 1
- 238000007789 sealing Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 238000011144 upstream manufacturing Methods 0.000 description 1
- 230000004304 visual acuity Effects 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)
この発明は粉体粒子の静電分級方法と装置に関
するものであり、更に詳しくはフアインセラミツ
クスに用いられるケイ素化物粉や磁気記憶媒体に
用いられる磁性粉などのように所謂先端技術の分
野で用いるものであつて、粒度の点で、非常に高
度な均質性を要求される超微粒子料を高いい精度
で単相あるいは複相に粒度分級する新技術の開発
に関するものである。[Detailed Description of the Invention] (Industrial Application Field) This invention relates to a method and apparatus for electrostatic classification of powder particles, and more specifically to silicide powder used in fine ceramics and magnetic storage media. Ultra-fine particle materials, such as magnetic powder used in so-called cutting-edge technology fields, which require extremely high degree of homogeneity in terms of particle size, can be classified into single-phase or multi-phase particles with high precision. This is related to the development of new technology.
(従来技術)
以下の記載において「超微粒子」とは粒度が
1μm.以下の粒子を指して言う。また「粉体粒
子群」とは1μm.単位の粒径のものを含めてあ
る粒度範囲に亘つて分布する超微粒子を含む粒子
によつて構成される群を指して言うう。更に「粉
体粒子小群」とはそのような粉体粒子群中にあつ
てそれより狭い粒度範囲に亘つて分布する超微粒
子を含む粒子によつて構成される小群を指して言
う。例えばある粉体粒子群が0.9〜0.1μm.の粒
度範囲に亘つて分布する超微粒子によつて構成さ
れているとすると、0.7〜0.5μm.の粒度範囲に
亘つて分布する超微粒子によつて構成される小群
は、その粉体粒子群のひとつの粉体粒子小群であ
る。(Prior art) In the following description, "ultrafine particles" refer to
1μm. Point to the following particles. In addition, "powder particle group" is 1 μm. It refers to a group consisting of particles including ultrafine particles distributed over a certain particle size range, including those with a unit particle size. Furthermore, the term "powder particle small group" refers to a small group comprised of particles including ultrafine particles distributed over a narrower particle size range within such a powder particle group. For example, a certain powder particle group has a diameter of 0.9 to 0.1 μm. If it is composed of ultrafine particles distributed over a particle size range of 0.7 to 0.5 μm. A small group composed of ultrafine particles distributed over a particle size range of is one of the powder particle groups.
また粒度についての「高位」あるいは「低位」
とは比較上の表現であつて、例えば上記した粉体
粒子群の場合なら0.9〜0.7μm.の粒度は「高位」
であり、0.5〜0.3μm.の粒度は「低位」である
と言う。 Also, “high” or “low” regarding particle size.
is a comparative expression; for example, in the case of the above powder particle group, it is 0.9 to 0.7 μm. The grain size of is "high"
and 0.5 to 0.3 μm. The grain size of is said to be "low".
前記したような先端技術分野において用いられ
る超微粒子材料は極めて均質であること、即ち粒
度が揃つていることが強く要求される。例えばレ
ンズなどに用いる極薄透明プラスチツクス場合に
は、その材料として用いられるケイ素化物の粉末
の均質性いかんによつて、得られるレンズの電気
絶縁性や解像力が大きく左右される。また磁気テ
ープや磁気デイスクなどのような計算機に用いら
れる記憶媒体にあつては、その材料として用いら
れる磁性粉の均質性によつては、得られる媒体に
記憶密度やノイズ発生などが大きく左右される。 Ultrafine particle materials used in the above-mentioned cutting-edge technology fields are strongly required to be extremely homogeneous, that is, to have uniform particle sizes. For example, in the case of ultra-thin transparent plastics used for lenses, the electrical insulation properties and resolving power of the resulting lenses are greatly influenced by the homogeneity of the silicide powder used as the material. Furthermore, in the case of storage media used in computers, such as magnetic tapes and magnetic disks, the homogeneity of the magnetic powder used as the material greatly affects the storage density and noise generation of the resulting media. Ru.
上記したような先端技術用材料としての超微粒
子の利用分野の進歩のためには、その粉砕、分級
および搬送などの取扱技術の開発が不可欠であ
り、なかでも製品機能の点からして分級技術の開
発が重要である。 In order to advance the field of application of ultrafine particles as materials for advanced technology as described above, it is essential to develop handling technologies such as crushing, classification, and transportation. development is important.
粉体粒子の分級技術としては遠心力を利用した
もの、ジエツト噴流を利用したもの、および流体
素子を利用したものなどが知られている。しかし
これら公知の技術おける分級の限界は精々ミクロ
ン単位迄にとどまるものであり、到底サブミクロ
ン単位の超微粒子には及ぶものではない。一部に
理論的なレベルでの提案もない訳ではないが、い
ずれも実務的な処理能力や消費エネルギーの面な
どで多々問題を含んでおり、工業的な規模で採用
される迄には至つていない。 Known techniques for classifying powder particles include those that utilize centrifugal force, jet jets, and fluid elements. However, the limits of classification in these known techniques are limited to micron units at most, and do not extend to ultrafine particles in submicron units. Although some proposals have been made on a theoretical level, they all have many problems in terms of practical processing capacity and energy consumption, and have not been adopted on an industrial scale. It's not working.
また後に詳述するように、この発明は超微粒子
をコロナ放電場において荷電させた場合に静電引
力と空気同伴イオン流との作用により超微粒子が
静電放電の方向に偏向移動する現象を基礎として
いるが、このような粒子の静電荷電を利用した技
術としては電気集塵機が知られている。従来の電
気集塵機の一般的構成としては縦型の構造を有し
ており、放電極と集塵極板とを間隙を置いて対設
させ、放電下に含塵気流をして該間隙内を通過せ
しめ、荷電された塵埃粒子を集塵極板上に堆積さ
せ、この堆積塵埃粒子を一定の周期で払い落して
除去し、除塵された気流を系外に送り出すもので
ある。なるほどこの方法によれば含塵気流中にサ
ブミクロン単位の超微粒子が含まれている場合に
も、これをミクロン単位の塵埃と共に一括して荷
電捕捉することはできる。勿論集塵、即ち含塵気
流からの除塵という目的からすればこれで充分で
ある。しかし従来の電気集塵機の機能はそこでと
どまるのであつて、それを越えて捕捉した超微粒
子あるいはミクロン単位の塵埃をその粒度に応じ
て分級するというようなことは一切期待し得ない
のである。 As will be detailed later, this invention is based on the phenomenon that when ultrafine particles are charged in a corona discharge field, the ultrafine particles are deflected and moved in the direction of electrostatic discharge due to the action of electrostatic attraction and air-entrained ion flow. However, electrostatic precipitators are known as a technology that utilizes the electrostatic charge of particles. Conventional electrostatic precipitators generally have a vertical structure, in which a discharge electrode and a dust-collecting plate are placed opposite each other with a gap between them, and a dust-containing airflow is generated during discharge to fill the gap. The charged dust particles are deposited on the dust collection electrode plate, and the accumulated dust particles are removed by being brushed off at regular intervals, and the dust-removed airflow is sent out of the system. Indeed, according to this method, even when submicron-sized ultrafine particles are included in the dust-containing airflow, they can be charged and captured together with micron-sized dust. Of course, this is sufficient for the purpose of collecting dust, that is, removing dust from a dust-containing airflow. However, the function of conventional electrostatic precipitators is limited to this, and it cannot be expected to go beyond that and classify captured ultrafine particles or dust on the micron scale according to their particle size.
更に超微粒子の分級に当つては、超微粒子が非
常に空気中に舞い上り易いという点も考慮しなけ
ればならない。即ち折角粉体粒子群をいくつかの
粉体粒子小群に分級しても、その後の処理を誤る
と超微粒子が空気中に舞い上る結果、一旦分級さ
れた粉体粒子小群がたとえ部分的にしても再び混
り合つてしまうのである。特に上記した電気集塵
機のように、集塵極板上の堆積したものを払い落
すような取扱い方は、超微粒子の激しい舞上りを
招くから、分級を目的とする場合には絶対避けな
ければならない。加えて空気中への超微粒子の舞
上りは環境汚染という公害上の問題にもつながる
のである。 Furthermore, when classifying ultrafine particles, consideration must be given to the fact that ultrafine particles are very likely to fly up into the air. In other words, even if a group of powder particles is classified into several small groups of powder particles, if the subsequent processing is incorrect, the ultrafine particles will fly up into the air, and even if the small groups of powder particles once classified are However, they are mixed together again. In particular, as with the electrostatic precipitator mentioned above, handling that involves brushing off the accumulated material on the dust collecting electrode plate will cause a violent upheaval of ultrafine particles, so this must be avoided at all costs when the purpose is classification. . In addition, the rise of ultrafine particles into the air can lead to environmental pollution problems.
(発明の目的)
この発明の目的は、先端技術用材料として適し
た非常に高度な均質性を有した超微粒子を、工業
的規模で提供することにある。(Objective of the Invention) The object of the present invention is to provide ultrafine particles on an industrial scale that have a very high degree of homogeneity and are suitable as materials for advanced technology.
この発明の他の目的は、非常に少ない消費動力
でかつ、連続的に超微粒子からなる粉体粒子群を
高精度でかつ高度に、整然と分級することにあ
る。 Another object of the present invention is to continuously classify powder particles consisting of ultrafine particles in a highly accurate, highly orderly manner while consuming very little power.
この発明の更に他の目的は、超微粒子からなる
粒体粒子群の分級を、作業、公害環境を汚染する
ことなくしかも材料の散失によるロスを生じるこ
となく、遂行することにある。 Still another object of the present invention is to carry out the classification of granular particles consisting of ultrafine particles without contaminating the working environment and without causing loss due to scattering of materials.
(発明の基本的構成)
この発明によれば、搬送気流中に広い粒度範囲
に亘る超微粒子を含む粉体粒子群を混入し、プツ
シユ・プル式整流機構によつて進行方向と直交す
る平面方向に亘つて均一な速度分布を有する固気
混相流を形成し、密閉状の分級室内に対面立設さ
れた1個以上の静電高電圧放電極板と2個以上の
上下に並設された回収要素間の間隙(分級域)に
この固気混相流を導いて進行させ、放電下に高位
の粒度範囲を有する粉体粒子小群から順次に進行
中の固気混相流から分離し、それぞれの回収要素
により個別に吸引捕捉回収するものである。(Basic Structure of the Invention) According to the present invention, a group of powder particles including ultrafine particles over a wide particle size range is mixed into a conveying air flow, and a push-pull type rectification mechanism is used to disperse powder particles in a plane direction perpendicular to the traveling direction. A solid-gas multiphase flow with a uniform velocity distribution is formed over the air, and two or more electrostatic high voltage discharge electrode plates are installed vertically in parallel with one or more electrostatic high voltage discharge electrodes that are vertically placed facing each other in a closed classification chamber. This solid-gas multiphase flow is guided into the gap between the collection elements (classification zone) and allowed to proceed, and under electrical discharge, small groups of powder particles having a high particle size range are sequentially separated from the ongoing solid-gas multiphase flow, and each The collection elements are used to individually suction, capture and collect.
(発明の実施態様)
第1図に示すのはこの発明の静電分級装置の一
例であつて、縦長の構造を有しており、その主要
部はフレームと壁体(図中これらを省略する)と
によつて画定形成される実質的に密閉状の分級室
内に収容配置されている。(Embodiment of the invention) Fig. 1 shows an example of an electrostatic classifier of the present invention, which has a vertically elongated structure, the main parts of which are a frame and a wall (these are omitted in the figure). ) is housed in a substantially closed classification chamber defined by and.
この分級装置は、分級されるべき粉体粒子群を
混入させた搬送気流を進行方向と直交する平面方
向に亘つて均一な速度分布を有した固気混相流と
して積極的に送り出す供給部1と、その上方に設
けられてかつこの固気混相流から所定の粒度範囲
別に粉体粒子小群を分離する分級部2と、更にそ
の上方に設けられて分級、分離済みの搬送気流を
積極的に引取る収容部3とから、成るものであ
る。 This classification device includes a supply section 1 that actively sends out a conveying airflow mixed with powder particles to be classified as a solid-gas mixed phase flow having a uniform velocity distribution in a plane direction perpendicular to the direction of travel. , a classification section 2 is provided above the solid-gas multiphase flow to separate small groups of powder particles according to a predetermined particle size range, and a classification section 2 is provided above the classification section 2 that separates small groups of powder particles according to a predetermined particle size range from the solid-gas mixed phase flow. It consists of a storage section 3 to be taken over.
もつともこれは固気混相流を上昇させながら分
級を行なう場合の配置であつて、この逆に固気混
相流を下降させながら分級を行なつてもよい、こ
の場合には、供給部1の分級部2の上方に、また
収容部3は分級部2の下方に位置することにな
る。但し以下の記載では、固気混相流を上昇させ
ながら分級を行なう場合を例にとつて説明する。 Of course, this is an arrangement for performing classification while raising the solid-gas mixed phase flow; conversely, classification may be performed while lowering the solid-gas mixed phase flow. In this case, the classification in the supply section 1 The storage section 3 is located above the classification section 2 and the storage section 3 is located below the classification section 2. However, in the following description, an example will be explained in which classification is performed while raising the solid-gas multiphase flow.
前記した三者の内少なくとも分級部2は密閉分
級室内に配置されている。また供給部1と収容部
3とは、その気流の積極的送出しと積極的引取り
とにより、所謂プツシユ・プル方式による気流を
形成するものである。 At least the classification section 2 of the three parts described above is arranged in a closed classification chamber. Furthermore, the supply section 1 and the storage section 3 form a so-called push-pull type airflow by actively sending out and actively taking in the airflow.
供給部1は整流吐出機構11と搬送気流供給ダ
クト13と両者と連結する混合ダクト12とを有
しており、混合ダクト12の天井には広い粒度範
囲に亘る粉体粒子群を収容するホツパー14の底
部が開口している。ホツパー14内の粉体粒子群
は、例えば公知のロータリーフイーダーなどの働
きにより、単位時間当り所定量が混合ダクト12
内に落下供給され、供給ダクト13からの搬送気
流と混合されて固気混相流を形成する。 The supply unit 1 has a rectifying discharge mechanism 11, a conveying air flow supply duct 13, and a mixing duct 12 connected to both. On the ceiling of the mixing duct 12, there is a hopper 14 that accommodates a group of powder particles covering a wide particle size range. The bottom is open. The powder particles in the hopper 14 are transferred to the mixing duct 12 in a predetermined amount per unit time by the action of, for example, a known rotary feeder.
The solid-gas mixed phase flow is mixed with the conveying air flow from the supply duct 13 to form a solid-gas multiphase flow.
整流吐出機構11としては例えば特許第
1027787号あるいは特許第1175637号などに開示さ
れたダクト吐出口における流速均一化装置などを
用いる。前記のように混合ダクト12内で形成さ
れた固気混相流は、ここで進行方向と直交する平
面方向に亘つて均一な速度分布を有するようにな
つた後で、上方に吐出されてゆく。 As the rectifying discharge mechanism 11, for example, Patent No.
A flow velocity equalizing device at a duct discharge port, etc. disclosed in Japanese Patent No. 1027787 or Patent No. 1175637 is used. The solid-gas multiphase flow formed in the mixing duct 12 as described above has a uniform velocity distribution in a plane direction perpendicular to the direction of movement, and then is discharged upward.
分級部2は、上下に延在する放電極板21と、
間隙(分級域)Sを間に置いてこれに対面して上
下に隣接してフレームに固定配置された複数個
(図示の例では4個)の回収要素の主体を構成す
る回収板22a〜22dを有している。ここで分
級域Sは固気混相流の流路となる。放電極板21
は絶縁体からなる(あるいは絶縁体によつて被覆
された)アーム23によつてフレームに固定さ
れ、かつ適宜公知の方法により直流高電圧電源
(図示せず)に電気的に接続されている。また第
2図に示すように、その分級域Sに臨む表面上に
は多数の針状の放電極板211が密に突出配置さ
れている。 The classification section 2 includes a discharge electrode plate 21 extending vertically,
Collection plates 22a to 22d that constitute the main body of a plurality of collection elements (four in the illustrated example) are fixedly arranged on the frame vertically adjacent to each other with a gap (classification area) S in between. have. Here, the classification zone S becomes a flow path for a solid-gas multiphase flow. Discharge electrode plate 21
is fixed to the frame by an arm 23 made of an insulator (or covered with an insulator), and electrically connected to a DC high voltage power source (not shown) by an appropriate known method. Further, as shown in FIG. 2, a large number of needle-shaped discharge electrode plates 211 are densely arranged to protrude from the surface facing the classification area S.
各回収板22a〜22dにはそれぞれ多数の回
収孔が透明形成されるとともに、フード端24a
〜24dが連結されている。各フード端24a〜
24dは図示しないダクトにより吸収フアンと高
性能フイルターを具えた公知の粉体粒子小群の分
離回収部に連結されている。 A large number of recovery holes are transparently formed in each of the recovery plates 22a to 22d, and the hood end 24a
~24d are connected. Each hood end 24a~
24d is connected by a duct (not shown) to a known separation and recovery section for small powder particles, which is equipped with an absorption fan and a high-performance filter.
回収孔の開口面積はすべての回収板について同
一してもよく、同一回収板内においては同一であ
あるが回収板間では異なるようにしてもよい。例
えば、下側(固気混相流の進行方向について見れ
ば上流側)の回収板になる程回収孔の開口面積を
小さく、上側(同じく下流側)の回収板になる程
回収孔の開口面積を大きくなるように設計しても
よい。各回収板における回収孔の開口面積の大き
さおよびその回収板間での変化の度合などは、分
級されるべき粉体粒子群の粒度分布の形態および
要求される分級の程度などの工程条件に応じて適
宜これを定める。また各回収板の上下方向の寸法
は必ずしも図示のようにほぼ同一とする必要はな
く、上記のような工程条件に応じて適宜これを定
めればよい。 The opening area of the recovery hole may be the same for all recovery plates, or may be the same within the same recovery plate but may be different between recovery plates. For example, the lower the recovery plate (upstream side in the direction of solid-gas mixed phase flow), the smaller the opening area of the recovery hole, and the upper (also downstream) the recovery plate, the smaller the opening area of the recovery hole. It may be designed to be large. The size of the opening area of the collection holes in each collection plate and the degree of change between the collection plates will depend on process conditions such as the form of the particle size distribution of the powder particles to be classified and the degree of classification required. This will be determined as appropriate. Further, the vertical dimensions of each collection plate do not necessarily have to be substantially the same as shown in the drawings, but may be determined as appropriate depending on the process conditions as described above.
収容部3は分級域Sに臨んで開口する整流吸入
機構31とこれに連結されたダクト32とを有し
ている。整流吸入機構31としては供給部1に用
いた整流の吐出機構11と同じ整流機構を有した
ものを用いればよく、進行方向と直交する平面方
向に亘つて均一な速度分布を有した状態で分級域
からの搬送気流をダクト32内に吸引する働きを
する。 The housing section 3 has a rectifying suction mechanism 31 that opens facing the classification area S, and a duct 32 that is connected to the rectifying suction mechanism 31. As the rectification suction mechanism 31, it is sufficient to use one having the same rectification mechanism as the rectification discharge mechanism 11 used in the supply section 1, and the classification can be performed with a uniform velocity distribution in the plane direction perpendicular to the direction of movement. It functions to suck the conveying airflow from the area into the duct 32.
次にこのような構成を有する静電分級装置の作
用について説明する。 Next, the operation of the electrostatic classifier having such a configuration will be explained.
前記したようにホツパー14から供給された粉
体粒子群を含む固気混相流は、進行方向と直交す
る平面方向に亘つて均一な速度分布を有した状態
で、放電下にある分級域Sにプツシユ・プル方式
により整然と導かれる。 As described above, the solid-gas multiphase flow containing the powder particles supplied from the hopper 14 flows into the classification zone S under electric discharge with a uniform velocity distribution in the plane direction perpendicular to the direction of movement. It is guided in an orderly manner by the push-pull method.
ところで放電下にある固気混相流中の粉体粒子
群を構成する種々の粒度の超微粒子の挙動につい
てみると、個々に独立して気流中に浮遊している
るのではなく、放電によつて積極的な荷重を受け
てクローン作用力や静電分極による双極子モーメ
ント作用力のような静電気的作用の影響で衝突
し、所謂静電凝集を惹き起す。この静電凝集は比
較的粒度の近い超微粒子間に起き、そのような超
微粒子が凝集してある粒度範囲に亘る一種の団塊
を形成する。 By the way, when we look at the behavior of ultrafine particles of various particle sizes that make up the powder particle group in a solid-gas mixed phase flow under an electric discharge, we find that they are not floating individually in the air flow, but are caused by the electric discharge. When they are subjected to positive loading, they collide under the influence of electrostatic forces such as Crohn's action force and dipole moment action force due to electrostatic polarization, causing so-called electrostatic aggregation. This electrostatic aggregation occurs between ultrafine particles with relatively similar particle sizes, and such ultrafine particles aggregate to form a type of agglomerate over a certain particle size range.
この際に、小径の(即ち低位の粒度範囲にあ
る)超微粒子程荷電傾向が少ないから荷電量が小
さく、これに働く静電引力が小さい。従つて分級
域S内を進行中の空気同伴イオン流に乗つて固気
混相流の進行方向から偏向移動する度合が少な
い。即ち直進傾向が大である。従つて小径の超微
粒子程分級域S中での滞留時間が長くなり、大き
な団塊を形成し易い。 At this time, the smaller the diameter of the ultrafine particles (that is, the lower the particle size range), the smaller the tendency to be charged, so the amount of charge is smaller, and the electrostatic attraction acting on the particles is smaller. Therefore, the degree to which the ions are deflected from the direction of movement of the solid-gas multiphase flow by riding on the air-entrained ion flow progressing within the classification zone S is small. In other words, there is a strong tendency to go straight. Therefore, the smaller the diameter of the ultrafine particles, the longer the residence time in the classification zone S, and the more likely they are to form large agglomerates.
これに対して、大径の(即ち高位の粒度範囲に
ある。超微粒子程荷電傾向が多いから荷電量が大
きく、これに働く静電引力が大きい。従つて分級
域S内を進行中に空気同伴イオン流に乗つて固気
混相流の進行方向から偏向移動する度合が大き
い。即ち直進傾向が小である。従つて分級域S中
に滞留時間が短いので小さな団塊のまま偏向移動
してしまう。 On the other hand, particles with a large diameter (that is, in a high particle size range) have a larger tendency to charge, so the amount of charge is larger, and the electrostatic attraction that acts on them is larger. Riding on the entrained ion flow, the degree of deflection from the advancing direction of the solid-gas multiphase flow is large.In other words, the tendency to move straight is small.Therefore, since the residence time in the classification zone S is short, the ions are deflected and moved as small lumps. .
この発明は上記したような放電下にある分級域
S内における、超微粒子の粒度に応じた直進傾向
の差を利用したものである。 This invention utilizes the difference in the straight-line propensity of ultrafine particles depending on their particle size within the classification zone S under discharge as described above.
ここで説明の便宜上、ホツパー14内の粉体粒
子群が粒度範囲が大きい方から順に〜のグル
ープに分けられるものと仮定する。するとグルー
プに属する超微粒子は、粉体粒子群中では最も
高位の粒度範囲に属するから、最も小さな団塊
(「団塊」と称する。以下同じ)を形成し易く、
またた分級域S内を進行中の直進傾向が最も小で
ある。グループに属する超微粒子は、粉体粒子
群中では最も低位の粒度範囲に属するから、最も
大きな団塊を形成し易く、また分級域S内を進
行中の直進傾向が最も大である。放電極板21と
回収板22a〜22dとの間の分級域S内に導か
れた固気混相流はこのような挙動の異なる雑多な
超微粒子を含んでいる。 For convenience of explanation, it is assumed here that the powder particle group in the hopper 14 is divided into groups .about. in descending order of particle size range. Then, since the ultrafine particles belonging to the group belong to the highest particle size range in the powder particle group, they tend to form the smallest nodule (referred to as "nodule", hereinafter the same),
Furthermore, the tendency of the vehicle to move straight in the classification zone S is the smallest. Since the ultrafine particles belonging to the group belong to the lowest particle size range among the powder particles, they are most likely to form the largest agglomerates, and have the greatest tendency to move straight through the classification zone S. The solid-gas mixed phase flow guided into the classification zone S between the discharge electrode plate 21 and the collection plates 22a to 22d contains such miscellaneous ultrafine particles with different behaviors.
さて第2図において、最も下側の回収板22a
がカバーする分級区域Saにおいては、最も直進
傾向の小さな(最も高位な粒度範囲の)直進傾向
の超微粒子からなる団塊が空気同伴イオン流
に乗り、図中矢印で示すように固気混相流の進行
方向から偏向して回収板22aの方に向つて移動
し、回収板22aに到達して吸引捕捉され、固気
混相流から分離される。団塊〜もある程度は
偏向されるが、その直進傾向の故に、まだこの段
階では回収板側に到達して吸引捕捉される迄には
至らない。 Now, in FIG. 2, the lowest collection plate 22a
In the classification area Sa covered by , agglomerates consisting of ultrafine particles with the smallest tendency to move in a straight line (in the highest particle size range) ride the air-entrained ion flow, and as shown by the arrow in the figure, the agglomerates consisting of ultrafine particles with the smallest straight tendency to move in a straight line ride on the air-entrained ion flow, and as shown by the arrow in the figure, the solid-gas multiphase flow It is deflected from the traveling direction and moves toward the recovery plate 22a, reaches the recovery plate 22a, is sucked and captured, and is separated from the solid-gas multiphase flow. The baby booms are also deflected to some extent, but because of their tendency to move straight, at this stage they have not yet reached the collection plate side and are captured by suction.
次に下から2番目の回収板22bがカバーする
分級区域Sbにおいては、直進傾向の若干大きな
(2番目に高位な粒度範囲の)グループの超微
粒子からなる団塊が空気同伴イオン流に乗り、
固気混相流の進行方向から偏向して回収板22b
の方に向つて移動し、回収板22bに到達して吸
引捕捉され、固気混相流から分離される。団塊
、も更にある程度は偏向されるが、その大き
な直進傾向の故に、まだこの段階では回収板側に
到達して吸引捕捉される迄には至らない。 Next, in the classification zone Sb covered by the second collection plate 22b from the bottom, agglomerates consisting of ultrafine particles of a group with a slightly larger tendency to move straight (in the second highest particle size range) ride the air-entrained ion flow,
The recovery plate 22b is deflected from the advancing direction of the solid-gas multiphase flow.
It moves toward the recovery plate 22b, where it is sucked and captured and separated from the solid-gas mixed phase flow. The nodules are also deflected to some extent, but because of their large tendency to move straight, they have not yet reached the collection plate side and are captured by suction at this stage.
次に下から3番目の回収板22cがカバーする
分級区域Cにおいては、更に直進傾向の大きな
(3番目に高位な粒度範囲の)グループの超微
粒子からなる団塊が空気同伴イオン流に乗り、
固気混相流の進行方向から偏向して回収板22c
の方に向つて移動し、回収板22cに到達して吸
引捕捉され、固気混相流から分離される。団塊
も当に偏向されるが、その大きな直進傾向の故
に、まだこの段階では回収板側に到達して吸引捕
捉される迄には至らない。 Next, in the classification area C covered by the third collection plate 22c from the bottom, agglomerates made of ultrafine particles of a group with a greater tendency to move straight (in the third highest particle size range) ride the air-entrained ion flow,
The recovery plate 22c is deflected from the advancing direction of the solid-gas multiphase flow.
It moves towards the recovery plate 22c, where it is sucked and captured and separated from the solid-gas mixed phase flow. The nodules are also deflected, but because of their large tendency to move straight, at this stage they have not yet reached the collection plate side and are captured by suction.
更に最も上側の回収板22dがカバーする分級
区域Sdにおいては、最も直進傾向の大きな(最
も低位な粒度範囲の)グループの超微粒子から
なる団塊も空気同伴イオン流に乗り、固気混相
流から偏向して回収板22dの方に向つて移動
し、遂に回収板22dに到達して吸引捕捉され、
分離される。 Furthermore, in the classification zone Sd covered by the uppermost collection plate 22d, agglomerates made of ultrafine particles of the group with the greatest tendency to move straight (in the lowest particle size range) also ride the air-entrained ion flow and are deflected from the solid-gas multiphase flow. and moves toward the collection plate 22d, finally reaching the collection plate 22d and being suctioned and captured.
Separated.
以上の如くして固気混相流から分離されて回収
板22a〜22dに個別に吸引捕捉された粉体粒
子小群はそれぞれのフード端24a〜24dから
前記したように回収部に送られて回収される。回
収後の超微粒子はそのまま使用に供してもよい
し、更に細かな静電分級に掛けてもよい。かくし
て固気混相流からは少なくとも理論的には全ての
超微粒子が分級分離されたことになるから、残つ
て搬送気流だけ収容部3によつて収容されること
になる。しかし実際にはこの搬送気流中には超微
粒子が皆無とは言えないこともあるので、必要に
応じて収容部にてこれを適宜なフイルターに通し
たり、一旦収容した後で更に細かな静電分級に掛
けることもある。 The small groups of powder particles separated from the solid-gas mixed phase flow and individually sucked and captured by the collection plates 22a to 22d as described above are sent to the collection section from the respective hood ends 24a to 24d and collected as described above. be done. The collected ultrafine particles may be used as is, or may be subjected to even finer electrostatic classification. In this way, at least theoretically, all the ultrafine particles have been classified and separated from the solid-gas mixed phase flow, so that only the conveying air flow remains to be accommodated in the storage section 3. However, in reality, it may not be possible to say that there are no ultrafine particles in this carrier airflow, so if necessary, the particles may be passed through an appropriate filter in the storage section, or even finer electrostatic particles may be removed once they are contained. It may also be used for classification.
以上説明した例においては、回収要素として多
孔板状の回収板を用いたが、回収要素の態様は必
ずしもこれに限定されるものではない。例えば第
3図Aに示すように、分級域に臨んで棚状開口4
1を有した回収箱4を用いてもよく、あるいは第
3図Bに示すように分級域に臨んで網目状開口5
1を有した回収箱5を用いてもよい。このほかに
もノズル状あるいはリング状の開口を有したも
の、グリツド状による開口を有したものなど、通
気性開口構造を分級域に臨んで有した種々の回収
要素を用いることができる。更に前記のような回
収孔の場合には、回収孔の周縁にリング状電極な
どを付設すれば、静電引力と空気同伴イオン流の
働きを更に盛んなものとすることができる。 In the example described above, a perforated recovery plate was used as the recovery element, but the mode of the recovery element is not necessarily limited to this. For example, as shown in Figure 3A, a shelf opening 4 facing the classification area
Alternatively, a collection box 4 having a mesh opening 5 facing the classification area may be used as shown in FIG.
1 may be used. In addition, various collection elements having an air-permeable opening structure facing the classification area can be used, such as one having a nozzle-shaped or ring-shaped opening, or one having a grid-shaped opening. Furthermore, in the case of the recovery hole as described above, if a ring-shaped electrode or the like is attached to the periphery of the recovery hole, the effects of electrostatic attraction and air-entrained ion flow can be further enhanced.
ところで上記の静電分級に際しては放電極板2
1上の各放電極板211と、回収要素上の各開口
(例えば回収孔、格子の目あるいはネツトの網目)
とが相互に対応するものであり、従つて回収要素
上の開口のピツチは放電極板21上の放電極針の
ピツチに対応させるのが望ましい。 By the way, in the above electrostatic classification, the discharge electrode plate 2
1 on each discharge electrode plate 211 and each opening (e.g. collection hole, grid opening or net mesh) on the collection element.
Therefore, it is desirable that the pitch of the openings on the recovery element correspond to the pitch of the discharge electrode needles on the discharge electrode plate 21.
さて第1,2図に示す実施態様においては、1
個の放電極板21を複数個の回収板22a〜22
dと組合せて静電放電による分級を行なつている
から、各分級区域における静電印加電圧は同一で
ある。従つて従来技術に比べれば遥かに高精度で
かつ高度な分級を行なうことはできるものの、精
度において更に一段と高いものが要求され、しか
も工程条件の微妙な変化に対する対応の柔軟性に
おいて、更に豊かなものが要求されることがあ
る。 Now, in the embodiment shown in FIGS. 1 and 2, 1
discharge electrode plates 21 and a plurality of recovery plates 22a to 22
Since classification is performed by electrostatic discharge in combination with d, the electrostatic applied voltage in each classification area is the same. Therefore, although it is possible to perform far more accurate and advanced classification than conventional technology, it requires even higher accuracy and is more flexible in responding to subtle changes in process conditions. Sometimes things are required.
第4図に示すのはそのような要求に応える実施
態様のひとつの例であつて、印加電圧を高電圧に
した場合に静電凝集が顕著となることを利用し
て、分級を更に細分化しようとするものである。
なお簡便のため図中には第1図の場合と同じ4段
階の分級を示したが、一般に第1図のような構造
を第4図のようにした場合には更に多段階の分級
を行なうことが可能である。 Figure 4 shows an example of an embodiment that meets such requirements, in which the classification is further subdivided by taking advantage of the fact that electrostatic aggregation becomes more pronounced when the applied voltage is increased. This is what I am trying to do.
For simplicity, the same four-stage classification as in Figure 1 is shown in the figure, but in general, when the structure shown in Figure 1 is changed to the one shown in Figure 4, more stages of classification are performed. Is possible.
即ちこの実施態様の場合には4個の回収板22
a〜22dに対して4個の放電極板21a〜2
1dを上下に並設し、それぞれ異なる直流電圧電
源に電気的に接続したものである。更に詳しく言
うと、固気混相流を分級域S内に上昇させるとき
には、上側の放電極板程高い電圧の直流高電圧電
源に接続する。従つてこの場合印加電圧は上側の
分級区域における程高くなる。また固気混相流を
分級域S内で下降させるときには、下側の放電極
板程高い電圧の直流高電圧電源に接続する。従つ
て印加電圧は下側の分級区域における程高くな
る。 That is, in this embodiment, there are four collection plates 22.
4 discharge electrode plates 21a-2 for a-22d
1d are arranged vertically in parallel, each electrically connected to a different DC voltage power source. More specifically, when the solid-gas mixed phase flow is raised into the classification zone S, the upper discharge electrode plate is connected to a DC high voltage power source with a higher voltage. In this case, therefore, the applied voltage is higher in the upper classification zone. Furthermore, when the solid-gas multiphase flow is lowered within the classification zone S, the lower discharge electrode plates are connected to a DC high-voltage power source with a higher voltage. The applied voltage is therefore higher in the lower classification zone.
この実施態様の場合には静電印加電圧を調節す
ることにより静電凝集を制御し更には超微粒子の
固気混相気流中における直進傾向を制御してい
る。従つて例えば第1図の実施態様において1段
階の分級が行なわれる1分級区域を2分割して、
上下並設した2個の回収板に対応して2個の放電
極板を上下並設し、それぞれ異なる直流高電圧電
源に接続すれば、分級が2段階に細分され高度と
なる。 In this embodiment, the electrostatic aggregation is controlled by adjusting the electrostatic applied voltage, and furthermore, the tendency of the ultrafine particles to move straight in the solid-gas mixed phase airflow is controlled. Therefore, for example, in the embodiment of FIG. 1, one classification area where one stage of classification is performed is divided into two,
If two discharge electrode plates are arranged vertically in parallel corresponding to the two collecting plates arranged vertically in parallel and connected to different DC high-voltage power supplies, the classification can be subdivided into two stages and the degree of sophistication can be achieved.
第5図に示すのは前記したような要求に答える
実施態様の他の例であつて、分級域の横断面積
(固気混相流の進行方向と直交する平面面積)を
大にした場合に静電凝集が促進されることを利用
そて、分級を更に細分化しようとするものであ
る。なお簡便のため図中に第1図の場合と同じ4
段階の分級を示しが、一般に第1図のような構造
を第5図のようにした場合には更に他段階の分級
を行なうことが可能である。 Figure 5 shows another example of an embodiment that satisfies the above-mentioned requirements. This is an attempt to further refine the classification by taking advantage of the fact that electrocoagulation is promoted. For simplicity, the same 4 as in Figure 1 is used in the figure.
Although the classification is shown in stages, in general, if the structure shown in FIG. 1 is changed to the one shown in FIG. 5, it is possible to further perform classification in other stages.
即ちこの実施態様の場合には、固気混相流の進
行方向に沿つて分級域の横断面積を漸増させたも
のであるが、段階的に増加させてもよい。更に詳
しく言うと、固気混相流を分級域S内で上昇させ
せるときには、図示のように上側になる程分級域
Sの横断面積を大にする。従つて流量さえ一定で
あれば、下側の分級区域になる程固気混相流は低
速となり、滞留時間が長くなり、所望の偏向移動
効果が得られ易くなる。また固気混相流を分級域
S内で下降させるときには下側になる程分級域S
の横断面積を大にする。従つて流量され一定であ
れば、下側の分級区域になる程固気混相流は低速
となり、滞留時間が長くなり、静電凝集は促進さ
れる。 That is, in the case of this embodiment, the cross-sectional area of the classification zone is gradually increased along the traveling direction of the solid-gas multiphase flow, but it may be increased in steps. More specifically, when the solid-gas mixed phase flow is raised within the classification zone S, the cross-sectional area of the classification zone S is made larger as it moves upwards as shown in the figure. Therefore, as long as the flow rate is constant, the lower the classification zone, the lower the velocity of the solid-gas mixed phase flow, the longer the residence time, and the easier it is to obtain the desired deflection movement effect. In addition, when the solid-gas multiphase flow is lowered within the classification area S, the lower the position, the more the classification area S
Increase the cross-sectional area of Therefore, if the flow rate is constant, the lower the classification zone, the lower the velocity of the solid-gas multiphase flow, the longer the residence time, and the more electrostatic aggregation will be promoted.
(実施例)
放電下への印加電圧は25〜100KVの範囲が好
ましく、分級域の幅は印加電圧との関係で定まる
が40〜400mm.の範囲が一般的である。放電極と
しては例えば直径1.6mm.×10mm.の針状電極を用
いる。固気混相流の流速は0.5〜3.0m/sec位の範
囲が好ましい。回収要素全体のカバー領域の大き
さは固気混相流の流速や流量によつて定まるが、
一例を上げると幅375mm.×長さ1340mm.位であ
る。(Example) The voltage applied to the discharge is preferably in the range of 25 to 100 KV, and the width of the classification area is determined by the relationship with the applied voltage, but it is 40 to 400 mm. range is common. For example, the discharge electrode has a diameter of 1.6 mm. ×10mm. needle-like electrodes are used. The flow rate of the solid-gas mixed phase flow is preferably in the range of about 0.5 to 3.0 m/sec. The size of the coverage area of the entire recovery element is determined by the flow rate and flow rate of the solid-gas multiphase flow.
For example, the width is 375mm. ×Length 1340mm. It is the rank.
(発明の効果)
以上から明らかなようにこの発明によれば、非
常に広い粒度範囲に亘る超微粒子を含んだ粒子か
らなる粉体粒子群を、予め、選定された異なる粒
度範囲に亘る超微粒子を含む複数の粉体粒子小群
に整然と分級することができるので、使用目的に
応じて高い均等粒度の精度を有した超微粒子材料
を供給することが可能となる。(Effects of the Invention) As is clear from the above, according to the present invention, a powder particle group consisting of particles containing ultrafine particles over a very wide range of particle sizes can be divided into ultrafine particles over different particle size ranges selected in advance. Since it is possible to orderly classify powder particles into a plurality of small groups containing powder particles, it is possible to supply ultrafine particle materials with high uniform particle size accuracy depending on the purpose of use.
また分級操作は実質的に密閉された分級室内で
行なわれるので、作業、公害環境を汚染すること
もなく、一般に貴重な高価な超微粒子材料をやた
らに散失させることもない。 In addition, since the classification operation is carried out in a substantially sealed classification chamber, there is no possibility of contaminating the working environment, and no excessive scattering of generally valuable and expensive ultrafine particle materials.
更に搬送気流の特性、放電の強さ、放電の段
数、回収要素の段数、分級域の横断面積及びその
変化などの諸工程要因を適宜調節しかつ組合せる
ことにより、要求に応じて非常に高度でかつ多岐
に亘る分級を行なうことができる。特に分級域S
の流路にプツシユ・プルによる整流方式を採用し
た効用について詳述すれば、S流路での流れが、
偏流、乱流を生じた場合は前述来の粒径に応じて
の遂次偏向移動による分級制度は著しく阻害され
る。即ち各超微粒子がこの分級域Sの流路におい
て、いかに均等に分散して上昇するかが粒径に応
じての荷電、静電凝集が整然と得られるための最
重要なポイントといえる。また他の効用として、
在来電気集塵機などで最も困難視されていたプツ
シユまたはプルのみの単独含塵気流流れでは放電
極板と集塵極板との間の流路を管路とする必要が
あり、その平面極板の両側面を密閉化する場合、
相互極板間の絶縁性を完璧にする問題がある。こ
れに対し、この発明によれば、放電極板21と回
収要素とは分級室内の自由空間内に対面立設され
ており、分級域Sの流路の両面側は開放された状
態で空気絶縁が行なわれている。即ちプツシユ・
プル気流の対応強度作用(側風なしのプツシユ・
プルエアカーテンに見られる)によつて分級室内
に充満、充溢などの懸念は皆無であり、所要流路
のみの形成が自制規制的になわれるものである。 Furthermore, by appropriately adjusting and combining various process factors such as the characteristics of the conveying air flow, the intensity of the discharge, the number of stages of the discharge, the number of stages of the collection element, the cross-sectional area of the classification zone and its changes, we can achieve very high performance according to the requirements. It is possible to carry out a wide variety of classifications. Especially classification area S
To explain in detail the effect of adopting the push-pull rectification method in the S flow path, the flow in the S flow path is
When drifting or turbulent flow occurs, the conventional classification system based on successive deflection and movement according to the particle size is significantly impaired. That is, the most important point in order to obtain charge and electrostatic aggregation according to the particle size in an orderly manner is how the ultrafine particles are evenly dispersed and raised in the flow path of the classification zone S. In addition, as other benefits,
In the single push or pull dust-containing air flow, which was considered the most difficult in conventional electrostatic precipitators, the flow path between the discharge electrode plate and the dust collection electrode plate must be a conduit, and the flat electrode plate When sealing both sides of
There is a problem of perfecting the insulation between mutual electrode plates. In contrast, according to the present invention, the discharge electrode plate 21 and the recovery element are installed facing each other in the free space of the classification chamber, and both sides of the flow path of the classification area S are left open and air-insulated. is being carried out. In other words, push
Corresponding strength effect of pull airflow (pushing without side wind)
There is no concern that the classification chamber will be overfilled or overflowed due to a pull air curtain (as seen in pull air curtains), and only the necessary flow paths can be formed in a self-restrictive manner.
更に放電には比較的高電圧を用いるが、電流そ
のものは非常に小さくてよいので、消費電力は小
さく、従つてランニングコストが低く、経済的で
ある。 Furthermore, although a relatively high voltage is used for discharging, the current itself may be very small, so the power consumption is low, and therefore the running cost is low, making it economical.
第1図はこの発明の静電分級装置の要部の一例
を示す斜視図、第2図はその分級作用を説明する
側面図、第3図A,Bは回収要素の例を示す斜視
図、第4,5図はこの発明の静電分級装置の要部
の他の例を示す側面図である。
1……供給部、31……整流吐出機構、14…
…ホツパー、2……分級部、21,21a〜21
d……放電板、22a〜22d……回収板、3…
…収容部、31……整流吸入機構。
FIG. 1 is a perspective view showing an example of the essential parts of the electrostatic classifier of the present invention, FIG. 2 is a side view illustrating its classification action, and FIGS. 3A and B are perspective views showing an example of the collection element. 4 and 5 are side views showing other examples of essential parts of the electrostatic classifier of the present invention. 1... Supply section, 31... Rectification discharge mechanism, 14...
...Hopper, 2...Classification department, 21, 21a-21
d...discharge plate, 22a-22d...recovery plate, 3...
...accommodating section, 31... rectification suction mechanism.
Claims (1)
を搬送気流に混入して固気混相流を形成し、 プツシユ・プル整流方式により、この固気混相
流の速度分布をその進行方向と直交する平面方向
に亘つて均一となし、 上記の固気混相流をして、実質的に密閉された
環境内に画定形成された上下方向に延在する分級
域内を、進行せしめ、 この分級域の一側方から上記の固気混相流に対
して静電高電圧による放電を行ない、かつ この放電下に上記の分級域の他側方において、
高位の粒度範囲を有する予め選定された粉体粒子
小群ごとに順次個別に、進行中の固気混相流から
分離して捕捉回収する ことを特徴とする粉体粒子の静電分級方法。 2 前記の分級域において、固気混相流の進行方
向について、下流側ほど高い静電高電圧により放
電を行なう ことを特徴とする特許請求の範囲第1項記載の方
法。 3 実質的に密閉状の分級室内には、静電高電圧
電源に接続された放電極板21が上下方向に延在
して設けられており、 縦長の分級域Sを間に置いてこの放電極板に対
面して、分級域に臨む通気性開口構造を有した回
収要素が、少なくとも2個上下に並設されて、そ
れぞれ個別の粉体粒子小群回収部に連結されてお
り、 分級域Sの長手方向一端に面して、広い粒度範
囲に亘る超微粒子を含む粉体粒子群と搬送気流と
の固気混相流をその進行方向と直交する平面方向
に亘つて均一な速度分布で吐出する整流機構11
を具えた、供給部1が設けられており、かつ、 分級域Sの長手方向他端に面して、分級済の搬
送気流その進行方向と直交する平面方向に亘つて
均一な速度分布で吸入する整流機構31を具え
た、収容部3が設けられていることを特徴とする
粉体粒子の静電分級装置。 4 前記の放電極板が上下方向に並設された少な
くとも2個以上の放電極板21a〜21dに分割
されており、かつ、 分級域内における固気混相流の進行方向につい
て、下流側の放電極板ほど高い電圧の静電高電圧
電源に接続されている ことを特徴とする特許請求の範囲第3項記載の装
置。 5 前記の分級域の横断面積が、分級域内におけ
る固気混相流の進行方向について、下流側ほど大
となるように構成されている ことを特徴とする特許請求の範囲第3もしくは4
項記載の装置。 6 前記の回収要素が、通気性開口構造として回
収孔を有した回収板22a〜22dである ことを特徴とする特許請求の範囲第3〜5のいず
れかの項記載の装置。 7 前記の回収要素が、通気性開口構造として棚
状開口を有した回収箱4である ことを特徴とする特許請求の範囲第3〜5のいず
れかの項記載の装置。 8 前記の回収要素が、通気性開口構造として網
目状開口を有した回収箱5である ことを特徴とする特許請求の範囲第3〜5のいず
れかの項記載の装置。 9 前記の回収要素が通気性開口構造としてグリ
ツドを有している ことを特徴とする特許請求の範囲第3〜5のいず
れかの項記載の装置。[Claims] 1. Powder particles including ultrafine particles over a wide particle size range are mixed into a conveying air flow to form a solid-gas multiphase flow, and the velocity distribution of this solid-gas multiphase flow is controlled by a push-pull rectification method. The above-mentioned solid-gas multiphase flow is made uniform over a plane direction perpendicular to the direction of movement, and is caused to proceed within a classification zone extending in the vertical direction that is defined and formed in a substantially sealed environment. , A discharge using electrostatic high voltage is applied to the above-mentioned solid-gas multiphase flow from one side of this classification area, and under this discharge, on the other side of the above-mentioned classification area,
A method for electrostatic classification of powder particles, characterized in that preselected small groups of powder particles having a high particle size range are sequentially and individually separated from an ongoing solid-gas mixed phase flow and captured and recovered. 2. The method according to claim 1, wherein in the classification zone, discharge is performed using an electrostatic high voltage that is higher toward the downstream side in the advancing direction of the solid-gas multiphase flow. 3 In the substantially sealed classification chamber, a discharge electrode plate 21 connected to an electrostatic high-voltage power source is provided extending vertically, and the discharge electrode plate 21 is connected to a vertically long classification area S in between. At least two collection elements each having a permeable opening structure facing the electrode plate and facing the classification area are arranged one above the other and each connected to an individual powder particle small group collection section, Facing one end in the longitudinal direction of S, a solid-gas mixed phase flow of powder particles containing ultrafine particles over a wide particle size range and a conveying air stream is discharged with a uniform velocity distribution over a plane direction perpendicular to the direction of movement of the powder particles. Rectifying mechanism 11
A supply section 1 is provided, and facing the other end in the longitudinal direction of the classification zone S, suctions the classified carrier air with a uniform velocity distribution over a plane direction perpendicular to its traveling direction. An electrostatic classification device for powder particles, characterized in that a storage section 3 is provided with a rectification mechanism 31 for straightening the particles. 4 The discharge electrode plate is divided into at least two or more discharge electrode plates 21a to 21d arranged in parallel in the vertical direction, and the discharge electrode on the downstream side with respect to the advancing direction of the solid-gas multiphase flow within the classification area. 4. The device according to claim 3, wherein the device is connected to an electrostatic high-voltage power supply whose voltage is higher than the plate. 5. Claim 3 or 4, characterized in that the cross-sectional area of the classification zone is configured such that the cross-sectional area of the classification zone increases toward the downstream side with respect to the advancing direction of the solid-gas mixed phase flow within the classification zone.
Apparatus described in section. 6. The device according to any one of claims 3 to 5, wherein the collection element is a collection plate 22a to 22d having a collection hole as an air-permeable opening structure. 7. The device according to any one of claims 3 to 5, wherein the collection element is a collection box 4 having a shelf-like opening as a ventilation opening structure. 8. The device according to any one of claims 3 to 5, wherein the collection element is a collection box 5 having a mesh opening as a ventilation opening structure. 9. Device according to any one of claims 3 to 5, characterized in that the collection element has a grid as the ventilation opening structure.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8745484A JPS60232261A (en) | 1984-04-27 | 1984-04-27 | Method and apparatus for electrostatic classification of powdery particle |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8745484A JPS60232261A (en) | 1984-04-27 | 1984-04-27 | Method and apparatus for electrostatic classification of powdery particle |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60232261A JPS60232261A (en) | 1985-11-18 |
| JPH0131428B2 true JPH0131428B2 (en) | 1989-06-26 |
Family
ID=13915302
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8745484A Granted JPS60232261A (en) | 1984-04-27 | 1984-04-27 | Method and apparatus for electrostatic classification of powdery particle |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60232261A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4682423B2 (en) * | 2001-01-10 | 2011-05-11 | パナソニック株式会社 | Electrostatic sorting device |
| JP5750711B2 (en) * | 2011-05-09 | 2015-07-22 | 学校法人 芝浦工業大学 | Electrostatic sorting device |
-
1984
- 1984-04-27 JP JP8745484A patent/JPS60232261A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60232261A (en) | 1985-11-18 |
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