JPS628221B2 - - Google Patents
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- Publication number
- JPS628221B2 JPS628221B2 JP15534982A JP15534982A JPS628221B2 JP S628221 B2 JPS628221 B2 JP S628221B2 JP 15534982 A JP15534982 A JP 15534982A JP 15534982 A JP15534982 A JP 15534982A JP S628221 B2 JPS628221 B2 JP S628221B2
- Authority
- JP
- Japan
- Prior art keywords
- processing container
- magnetic field
- processing
- container
- moving
- 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.)
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Description
【発明の詳細な説明】
この発明は固体、粉体、液体等の被処理物と一
諸に強磁性あるいは非磁性導電材で作られたワー
キングピースを処理容器内に収容し、これに外部
より移動磁界を作用させることによつてワーキン
グピースに激しいランダム運動を生起させて、被
処理物の粉砕、混合、撹拌等の処理を行う電磁式
処理装置の改良に関する。[Detailed Description of the Invention] This invention accommodates a working piece made of ferromagnetic or non-magnetic conductive material together with a workpiece such as solid, powder, or liquid in a processing container, and The present invention relates to an improvement in an electromagnetic processing device that processes objects to be processed, such as crushing, mixing, and stirring, by causing a working piece to undergo intense random motion by applying a moving magnetic field.
この種の処理装置として第1図および第2図に
示すような装置がすでに提案されている。すなわ
ち第1図において、1は被処理物2とともに強磁
性あるいは非磁性導電材で作られた例えばスピン
ドル形状の多数のワーキングピース3を収容した
処理容器であり、この容器1を中央に挾んで、そ
の上下には移動磁界発生装置4,5が対向配置さ
れており、その発生磁界の移動方向は矢印φ1,
φ2で示すように互に逆方向に定められている。
この移動磁界発生装置4,5はいわゆるリニアモ
ータとしてよく知られており、(以下「移動磁界
発生装置」を「リニアモータ」と呼称する。)例
えば3相交流巻線6を鉄心7に沿つて多極を形成
するように巻装して構成され、多相交流電源より
給電を受けて移動磁界φ1とφ2を生成する。 As this type of processing apparatus, apparatuses as shown in FIGS. 1 and 2 have already been proposed. That is, in FIG. 1, reference numeral 1 denotes a processing container containing a number of working pieces 3 made of ferromagnetic or non-magnetic conductive material, for example, in the shape of a spindle, together with an object 2 to be processed. Moving magnetic field generators 4 and 5 are arranged above and below to face each other, and the moving direction of the generated magnetic field is indicated by the arrow φ 1 ,
As shown by φ 2 , they are set in opposite directions.
These moving magnetic field generating devices 4 and 5 are well known as so-called linear motors (hereinafter, the “moving magnetic field generating device” will be referred to as “linear motor”). It is configured by being wound to form multiple poles, and receives power from a multiphase AC power source to generate moving magnetic fields φ 1 and φ 2 .
第1図の構成により、移動磁界φ1とφ2を作
用する磁場の中に置かれたワーキングピース3は
磁化および渦電流の作用による電磁力が働き、ワ
ーキングピース3はそれ自身の重心のまわりで回
転運動を行うとともに、移動磁界φ1,φ2によ
るその移動磁界方向に向けての推進力および浮上
力に加えて、ワーキングピース同士の衝突、容器
壁面との間の衝突も加わつて、容器1の中で激し
くランダムな運動を生起する。そしてこのランダ
ム運動により、被処理物2はワーキングピース3
との衝突等により粉砕あるいは混合、撹拌が進行
する。 With the configuration shown in Fig. 1, the working piece 3 placed in a magnetic field in which the moving magnetic fields φ 1 and φ 2 act is subjected to electromagnetic force due to the action of magnetization and eddy current, and the working piece 3 moves around its own center of gravity. In addition to the propulsive force and levitation force generated by the moving magnetic fields φ 1 and φ 2 in the direction of the moving magnetic field, collisions between the working pieces and the wall of the container are also added. 1 causes intense random motion. Due to this random movement, the workpiece 2 is moved to the working piece 3.
Crushing, mixing, and agitation progress due to collisions with other materials.
ところで、前記処理容器1が置かれるリニアモ
ータ4と5との間の磁場空間における磁界強度の
分布についての解析を行つたところによれば、第
3図に示すような磁界分布を示すことが明らかに
なつた。ここでリニアモータ4,5はU、V、
W3相の交流巻線が施されており、かつともに同
じ周波数の交流電源で励磁されるものとする。す
なわち鉄心7に巻装された巻線6の極ピツチをP
とすれば、処理容器内の作用空間における磁界
は、時間の経過に関係なく定常時に、その絶体値
が移動磁界方向に沿つて極ピツチPの1/2の間隔
で強、弱をくり返すような分布となる。このよう
な磁界分布は、リニアモータ4,5の各相巻線電
流とこれによつて生起される磁界の関係を時間の
進行にしたがつて遂時追跡することによつて求め
られ、またこの分布は実際に測定した磁界分布と
も一致する。ここで前記の強磁界領域の中心を
A、弱磁界領域の中心をBとして表わすと、Aと
Bが移動磁界方向に沿つて1/2極ピツチ間隔で交
互に並ぶようになる。 By the way, according to an analysis of the distribution of magnetic field strength in the magnetic field space between the linear motors 4 and 5 in which the processing container 1 is placed, it is clear that the magnetic field distribution is as shown in FIG. It became. Here, the linear motors 4 and 5 are U, V,
It is assumed that a W3-phase AC winding is provided, and both are excited by an AC power source of the same frequency. In other words, the pole pitch of the winding 6 wound around the iron core 7 is P.
If this is the case, the magnetic field in the working space inside the processing container is stable, regardless of the passage of time, and its absolute value repeatedly changes from strong to weak at intervals of 1/2 of the pole pitch P along the direction of the moving magnetic field. The distribution is as follows. Such a magnetic field distribution is obtained by tracking the relationship between the winding currents of each phase of the linear motors 4 and 5 and the magnetic fields generated thereby as time progresses. The distribution also matches the actually measured magnetic field distribution. Here, if the center of the strong magnetic field region is represented by A and the center of the weak magnetic field region is represented by B, then A and B are arranged alternately at 1/2 pole pitch intervals along the direction of the moving magnetic field.
また、上記の磁界分布のもとで処理容器内を運
動するワーキングピースの動きを高速度カメラで
観察すると、ワーキングピースは強磁界領域では
激しくランダム運動するが、弱磁界領域ではワー
キングピースの動きが緩慢になることが認められ
た。この観察結果はそのまま実際に砕料の粉砕処
理を行つた場合にも当てはまり、実機運転テスト
からも、弱磁界領域に位置する処理容器1の四隅
では、粉砕動作が十分に進行せず、この部分に粒
度の大きな砕料がそのまま多く滞留していること
が認められる。つまり、第1図に示したこの種の
処理装置は、一見したところでは処理容器内の全
域で処理動作が均一に行われているかのように見
えるが、厳密に考察すると、容器内には定常的に
磁界強度が弱く、このためにワーキングピースの
運動が活発でない不動作空間が部分的に存在して
いることが明らかになつた。 In addition, when observing the movement of the working piece inside the processing container under the above magnetic field distribution with a high-speed camera, it is found that the working piece moves violently and randomly in the strong magnetic field region, but in the weak magnetic field region, the working piece moves slowly. It was observed that it was slowing down. This observation result also applies to the actual pulverization process of crushed materials, and the actual machine operation test also shows that the pulverization operation does not progress sufficiently in the four corners of the processing container 1 located in the weak magnetic field region, and It is observed that a large amount of crushed material with large particle size remains as it is. In other words, in this type of processing apparatus shown in Fig. 1, at first glance it appears as if the processing operation is performed uniformly throughout the processing container, but if we consider it strictly, there is a steady state inside the processing container. It has become clear that the magnetic field strength is weak, and as a result, there is a partial inactive space in which the working piece does not move actively.
一方、上記装置の処理動作中は、処理容器内部
でのワーキングピースと砕料等の被処理物とが激
しく衝突、こすり合うことに加え、容器との間で
も衝突、こすり合いがくり返し行われることか
ら、この動作による摩擦熱が生じて処理容器自
身、およびその内部温度がかなり昇温することが
認められている。このために処理容器の熱変形、
寿命低下を来たす恐れがあるし、また被粉砕物、
被混合物等の種類によつては、高温にさらされて
変質してしまうものもあり、このような場合には
できるだけ処理容器、およびその内部の熱放散を
助成し、過度な温度上昇を抑制することが必要と
なる。かかる点、従来装置では、一般にブロア等
を用いて処理容器の周域に冷却風を強制的に送
り、冷却を図つているが、この方式では処理容器
を十分冷却することができても、その内部に収容
されている被処理物に対する十分な冷却を行うこ
とができないため、この点の改善策が望まれてい
る。他方、特別な例として種類の異なる液体の撹
拌を高温度の下で行うのが好ましい場合がある。
この場合には処理容器の周囲に熱風で送風するこ
とで対処していたが、しかし処理容器内の中央域
にまで十分に熱を与えることが困難である。 On the other hand, during the processing operation of the above-mentioned apparatus, in addition to violent collisions and rubbing between the working piece and the material to be processed, such as crushed material, inside the processing container, repeated collisions and rubbing occur with the container. It has been recognized that frictional heat generated by this operation significantly increases the temperature of the processing container itself and its internal temperature. For this purpose, thermal deformation of the processing container,
There is a risk that the service life will be shortened, and the material to be crushed,
Depending on the type of material to be mixed, there may be changes in quality when exposed to high temperatures. In such cases, assist in heat dissipation in the processing container and its interior as much as possible to suppress excessive temperature rises. This is necessary. In this regard, conventional equipment generally uses a blower or the like to forcefully send cooling air to the surrounding area of the processing container to achieve cooling, but even if this method can sufficiently cool the processing container, the Since the workpieces housed inside cannot be cooled sufficiently, an improvement in this respect is desired. On the other hand, as a special case, it may be preferable to stir different types of liquids at high temperatures.
This case has been dealt with by blowing hot air around the processing container, but it is difficult to apply sufficient heat to the central area within the processing container.
この発明は上記の点にかんがみなされたもので
あり、その目的は粉砕、混合等の処理性能を殆ど
損うことなしに、処理容器内の作用空間の冷却な
いしは必要に応じての加熱を効果的に行えるよう
にした電磁式粉砕混合等処理装置を得ることにあ
る。 This invention was made in consideration of the above points, and its purpose is to effectively cool the working space in the processing container or heat it as necessary, without substantially impairing processing performance such as crushing and mixing. The object of the present invention is to provide an electromagnetic grinding, mixing, etc. processing device that can perform the following operations.
かかる目的は、この発明により、移動磁界発生
装置の極ピツチ間隔に対応して処理容器内に定常
的に生じる各弱磁界領域を設置箇所としてここに
容器内部を仕切る二重仕切壁を設け、この二重仕
切壁の壁と壁との間に処理容器を横切る冷却ある
いは加熱体流通路を画成したことにより達成され
る。 According to the present invention, each of the weak magnetic field areas that are constantly generated in the processing container corresponding to the pole pitch spacing of the moving magnetic field generator is installed as a double partition wall that partitions the inside of the container. This is accomplished by defining a cooling or heating fluid flow path across the processing vessel between the walls of the double partition.
以下この発明を図示実施例に基づき詳述する。 The present invention will be described in detail below based on illustrated embodiments.
まず第4図および第5図において、リニアモー
タ4,5の巻線1に付した符号U,V,W,
U′,V′,W′は三相交流巻線の電流方向と相順を
表わしている。そして同相の巻線が上下で対向す
るB領域では、リニアモータ4と5の磁界が互に
打ち消し合うように作用するので、第3図で述べ
たように該部に定常的な弱磁界領域が生じる。ま
たこの弱磁界領域はリニアモータの極ピツチPの
間隔ごとに生成される。ところでこの発明によ
り、上記の弱磁界領域を占有するように位置を合
わせて、この部分に処理容器1の内部を移動磁界
方向φ1,φ2に沿つて区分するような二重の仕
切壁8Aと8Bからなる中仕切壁8が設置してあ
り、この二重仕切8Aと8Bの間に容器1の内部
を横切る断面巾dの通風路9が画成されている。
そして冷却媒体としての冷却風が第5図のように
側方よりブロア10によつて強制送風され、処理
容器内部の発生熱を効率よく除熱する。また特別
な処理の場合として、処理容器1内部の作動空間
を高温に保つ必要のある場合には、前記の冷却風
の代りに熱風を送り込めばよい。なお冷却、加熱
媒体は気体に限るものではなく、液体であつても
よい。この場合には、前記の通路9に外部の熱媒
液ラインが接続配管される。また通路9に面する
仕切壁8Aと8Bにフインを設けておくことによ
り一層の熱交換効率の向上が図れる。しかも前記
の二重壁構造の中仕切壁8は弱磁界領域B、つま
り粉砕、混合等の処理動作が殆ど有効に働かない
非動作空間部分に設けてあるので、いささかも処
理動作、性能を損うこともないし、加えて粉砕処
理の場合には、仕切壁で仕切られた処理室の作動
空間はすべて強磁界領域となるので、室内の四隅
に砕料が未粉砕のまま停滞することもなくなり、
より一層の性能向上の利点が得られる。 First, in FIGS. 4 and 5, the symbols U, V, W,
U′, V′, and W′ represent the current direction and phase sequence of the three-phase AC winding. In region B, where the windings of the same phase face each other at the top and bottom, the magnetic fields of the linear motors 4 and 5 act to cancel each other out, so a steady weak magnetic field region is created in this region as described in Fig. 3. arise. Further, this weak magnetic field region is generated at each interval of the pole pitch P of the linear motor. By the way, according to the present invention, a double partition wall 8A is positioned so as to occupy the above-mentioned weak magnetic field region and divide the inside of the processing container 1 along the moving magnetic field directions φ 1 and φ 2 in this portion. and 8B, and a ventilation passage 9 having a cross-sectional width d that crosses the interior of the container 1 is defined between the double partitions 8A and 8B.
Then, cooling air as a cooling medium is forcedly blown from the side by a blower 10 as shown in FIG. 5, and the heat generated inside the processing container is efficiently removed. Further, in the case of special processing, when it is necessary to maintain the working space inside the processing container 1 at a high temperature, hot air may be sent instead of the cooling air described above. Note that the cooling and heating medium is not limited to gas, and may be liquid. In this case, an external heat medium liquid line is connected to the passage 9. Further, by providing fins on the partition walls 8A and 8B facing the passage 9, the heat exchange efficiency can be further improved. Moreover, since the partition wall 8 of the double-walled structure is provided in the weak magnetic field area B, that is, in the non-operating space where processing operations such as crushing and mixing hardly work effectively, the processing operations and performance may be impaired in the slightest. In addition, in the case of pulverization processing, the working space of the processing chamber divided by partition walls becomes a strong magnetic field area, so there is no possibility of unpulverized material stagnating in the four corners of the room. ,
The advantage of further performance improvement can be obtained.
次に前記実施例の応用実施例を第6図に示す。
この実施例はリニアモータ4,5の極ピツチPよ
りも多少短かい寸法で構成された各独立した複数
個の箱形処理容器1′をリニアモータ4,5に沿
つて相互に間隔dを隔てて相並べ、かつ各容器
1′の相互を上下に配した非磁性の連結板11と
12との間に連結したものであり、かつ隣接し合
う容器1′と上下の連結板11,12とで囲まれ
た断面巾dの空間がリニアモータ4と5の間の磁
場空間における定常的な弱磁界領域Bに対応位置
するように定めてある。そして容器相互間に画成
された空間9′が冷却あるいは加熱媒体流通路と
して用いられる。 Next, an applied example of the above embodiment is shown in FIG.
In this embodiment, a plurality of independent box-shaped processing containers 1' each having a dimension slightly shorter than the pole pitch P of the linear motors 4, 5 are spaced apart from each other by a distance d along the linear motors 4, 5. The containers 1' are arranged side by side, and each container 1' is connected between non-magnetic connecting plates 11 and 12 arranged above and below, and the adjacent containers 1' and the upper and lower connecting plates 11 and 12 are connected to each other. A space with a cross-sectional width d surrounded by is determined to correspond to a stationary weak magnetic field region B in the magnetic field space between the linear motors 4 and 5. The space 9' defined between the containers is used as a cooling or heating medium flow path.
以上述べたようにこの発明は、従来では処理動
作に殆ど有効に働いてない弱磁界領域の不動作空
間部分を利用してここに容器を貫通する冷却ある
いは加熱媒体流通路を設けたものであり、したが
つて処理性能を損うことなしに処理容器内部空間
の効果的な冷却あるいは加熱を容易に達成できる
実用的効果が得られる。 As described above, the present invention utilizes the non-operating space in the weak magnetic field region, which conventionally does not work effectively for processing operations, and provides a cooling or heating medium flow path that penetrates the container. Therefore, a practical effect can be obtained in which effective cooling or heating of the internal space of the processing container can be easily achieved without impairing the processing performance.
第1図は従来における電磁式処理装置の構成原
理図、第2図は第1図の矢視−断面図、第3
図は第1図における処理容器内の磁界強度の分布
を模型的に表わした磁界分布図、第4図はこの発
明の一実施例の構成断面図、第5図は第4図にお
ける矢視−断面図、第6図は第4図と異なる
実施例の処理容器の構成断面図である。
1……処理容器、2……被処理物、3……ワー
キングピース、4,5……移動磁界発生装置、8
……二重仕切壁、9,9′……冷却、加熱媒体流
通路、φ1,φ2……移動磁界の移動方向、P…
…極ピツチ、A……強磁界領域、B……弱磁界領
域。
Fig. 1 is a diagram of the configuration principle of a conventional electromagnetic processing device, Fig. 2 is a sectional view taken in the direction of the arrow in Fig. 1, and Fig.
The figure is a magnetic field distribution diagram schematically representing the distribution of the magnetic field strength inside the processing container in FIG. 1, FIG. 6 is a cross-sectional view showing the structure of a processing container of an embodiment different from that shown in FIG. 4. 1... Processing container, 2... Processing object, 3... Working piece, 4, 5... Moving magnetic field generator, 8
...Double partition wall, 9, 9'...Cooling and heating medium flow path, φ 1 , φ 2 ...Movement direction of moving magnetic field, P...
...Pole pitch, A...Strong magnetic field region, B...Weak magnetic field region.
Claims (1)
のワーキングピースが収容された処理容器と、こ
の処理容器を中央に挾んでその両側に対向配置さ
れたその磁界の移動方向が互に逆向きな一対の移
動磁界発生装置とからなり、移動磁界との相互作
用に基づく電磁力で処理容器内に生起するワーキ
ングピースのランダム運動により、処理容器に収
容した被処理物の粉砕、混合等の処理を行うもの
において、前記移動磁界発生装置の極ピツチ間隔
に対応して処理容器内に定常的に生じる各弱磁界
領域を設置箇所としてここに容器内部を仕切る二
重仕切壁を設け、この二重仕切壁の壁と壁との間
に処理容器を横切る冷却あるいは加熱体流通路を
画成したことを特徴とする電磁式粉砕混合等処理
装置。1 A processing container containing a large number of working pieces made of magnetic or non-magnetic conductive material, and a processing container placed oppositely on both sides of the processing container with the processing container in the center, the moving directions of the magnetic fields being opposite to each other. Consisting of a pair of moving magnetic field generators, the random movement of the working piece generated in the processing container by electromagnetic force based on the interaction with the moving magnetic field performs processing such as crushing and mixing of the processed material contained in the processing container. In the case where a double partition wall is installed to partition the inside of the container as an installation location in each weak magnetic field area that is constantly generated in the processing container corresponding to the pole pitch spacing of the moving magnetic field generator, this double partition 1. An electromagnetic pulverizing, mixing, etc. processing device characterized by defining a cooling or heating body flow passage across a processing container between walls.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15534982A JPS5946149A (en) | 1982-09-07 | 1982-09-07 | Electromagnetic type crushing mixing treating device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15534982A JPS5946149A (en) | 1982-09-07 | 1982-09-07 | Electromagnetic type crushing mixing treating device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5946149A JPS5946149A (en) | 1984-03-15 |
| JPS628221B2 true JPS628221B2 (en) | 1987-02-21 |
Family
ID=15603943
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15534982A Granted JPS5946149A (en) | 1982-09-07 | 1982-09-07 | Electromagnetic type crushing mixing treating device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5946149A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2533903B2 (en) * | 1988-02-08 | 1996-09-11 | 日本電信電話株式会社 | DC compensation circuit |
-
1982
- 1982-09-07 JP JP15534982A patent/JPS5946149A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5946149A (en) | 1984-03-15 |
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