JPS6136452B2 - - Google Patents
Info
- Publication number
- JPS6136452B2 JPS6136452B2 JP57093855A JP9385582A JPS6136452B2 JP S6136452 B2 JPS6136452 B2 JP S6136452B2 JP 57093855 A JP57093855 A JP 57093855A JP 9385582 A JP9385582 A JP 9385582A JP S6136452 B2 JPS6136452 B2 JP S6136452B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- moving magnetic
- working
- 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.)
- Expired
Links
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B01—PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
- B01F—MIXING, e.g. DISSOLVING, EMULSIFYING OR DISPERSING
- B01F33/00—Other mixers; Mixing plants; Combinations of mixers
- B01F33/45—Magnetic mixers; Mixers with magnetically driven stirrers
- B01F33/451—Magnetic mixers; Mixers with magnetically driven stirrers wherein the mixture is directly exposed to an electromagnetic field without use of a stirrer, e.g. for material comprising ferromagnetic particles or for molten metal
Landscapes
- Chemical & Material Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Disintegrating Or Milling (AREA)
- Mixers With Rotating Receptacles And Mixers With Vibration Mechanisms (AREA)
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
キングビ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
グビ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 workpiece made of a ferromagnetic or non-magnetic conductive material together with a workpiece such as a solid, powder, or liquid in a processing container. The present invention relates to an improvement in an electromagnetic processing device that processes objects to be processed, such as crushing, mixing, stirring, etc., by causing violent random motion in working beads by applying a moving magnetic field.
頭記処理装置では、被処理物の処理がワーキン
グビースの容器内における運動ないしはワーキン
グビースの衝突等によつて行われるものであり、
かかる処理を効率的に行わせるには、ワーキング
ビースが処理容器内にあらゆる位置で万遍なく移
動磁界の作用を受けて激しくランダムな運動を行
うようにすることが望まれる。 In the above-mentioned processing device, processing of the object to be processed is performed by movement of working beads in a container or collision of working beads, etc.
In order to carry out such processing efficiently, it is desirable that the working beads be uniformly affected by the moving magnetic field at all positions within the processing container to perform violent random movements.
この種の処理装置として第1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
数のワーキングビース3を収容した処理容器であ
り、この容器1を中央に挟んで、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、例えば3相交流巻線を鉄心に沿
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。 An apparatus as shown in FIG. 1 has already been proposed as this type of processing apparatus. That is, in FIG. 1, reference numeral 1 denotes a processing container containing a workpiece 2 and a large number of working beads 3 made of ferromagnetic or non-magnetic conductive material, for example, in the shape of a spindle. Moving magnetic field generating devices 4 and 5 are arranged above and below to face each other, and the moving directions of the generated magnetic fields are determined to be mutually opposite directions as shown by arrows φ 1 and φ 2 . These moving magnetic field generators 4 and 5 are well known as so-called linear motors, and are constructed by, for example, winding three-phase AC windings to form multiple poles along an iron core, and are powered by a multi-phase AC power source. Moving magnetic fields φ 1 and φ 2
generate.
第1図の構成により、移動磁界φ1とφ2の中
に置かれたワーキングビース3は磁化および渦電
流の作用による電磁力が働き、ワーキングビース
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
ーキングビース同士の衝突、および容器壁面との
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はワーキングビース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 Figure 1, working bead 3 placed in moving magnetic fields φ 1 and φ 2 is subjected to electromagnetic force due to magnetization and eddy current, and working bead 3 rotates around its own center of gravity. At the same time, in addition to the propulsive force and levitation force caused by the moving magnetic fields φ 1 and φ 2 in the direction of the moving magnetic fields, collisions between the working beads and collisions with the wall surface of the container are also added, causing the movement inside the container 1. Produces violent random movements. Due to this random movement, the object 2 to be processed is pulverized, mixed, or agitated by collision with the working bead 3 or the like.
ここで第1図に示す装置の容器1が置かれるべ
き移動磁界発生装置4,5の間の作用空間内の磁
界分布を概念的に示せば第3図のごとくなる。す
なわち第3図において、移動磁界発生装置4,5
は矢印φ1,φ2で示す方向の移動磁界を発生す
るために、第2図に示すように、鉄心6のコイル
スロツト7にU―X,V―Y,W―Zで示す三相
交流巻線8が例えば波巻式に巻装されており、そ
の相順は装置4においては右方向へU―V1―W
―U1―V―W1―U(UとU1,VとV1,WとW1
はそれぞれ同相で逆向きのコイル導体を示す)。
の順に、一方装置5においては、右方向にU―
W1―V―U1―W―V1―Uの様に配列されてい
る。なお巻線の極ピツチP(U―U1間の距離)
は双方とも等しい。第3図においては、装置4の
U相巻線装置5の同じくU相巻線と対向位置して
書かれているが、実際の処理装置としては、どの
相の巻線が対向しているかは、その特性等に影響
をおよぼさない。また第3図において、移動磁界
発生装置4,5は共に同じ周波数の電源から給電
を受けており、矢印HはU相巻線の電流が最大
(巻線電流は正弦波としている。)となつた時点で
の各地点における磁界ベクトルを示している。更
に楕円Aは巻線電流が1サイクル分の変化をした
時の、この地点における磁界ベクトルHの軌跡を
表わしている。すなわち、空間内のほとんどの地
点で磁界は反時計方向に向きを変える楕円形回転
磁界と見なすことが出来る。 Here, the magnetic field distribution in the working space between the moving magnetic field generators 4 and 5 where the container 1 of the apparatus shown in FIG. 1 is placed is conceptually shown in FIG. 3. That is, in FIG. 3, the moving magnetic field generators 4, 5
In order to generate a moving magnetic field in the directions indicated by arrows φ 1 and φ 2 , three-phase AC windings indicated by U-X, V-Y, and W-Z are installed in the coil slot 7 of the iron core 6, as shown in FIG. The wire 8 is wound, for example, in a wave-wound manner, and the phase sequence is U-V 1 -W to the right in the device 4.
-U 1 -V-W 1 -U (U and U 1 , V and V 1 , W and W 1
(respectively indicate coil conductors in phase and opposite directions).
On the other hand, in the device 5, the U-
They are arranged like W 1 -V-U 1 -W-V 1 -U. In addition, the pole pitch P of the winding (distance between U and U 1 )
are both equal. In FIG. 3, the U-phase winding device 5 of the device 4 is shown facing the U-phase winding, but in the actual processing device, it is difficult to tell which phase winding is facing the U-phase winding. , does not affect its characteristics etc. Furthermore, in FIG. 3, both the moving magnetic field generators 4 and 5 are supplied with power from power sources with the same frequency, and the arrow H indicates the point where the current in the U-phase winding is maximum (the winding current is a sine wave). It shows the magnetic field vector at each point at the time. Furthermore, ellipse A represents the locus of the magnetic field vector H at this point when the winding current changes by one cycle. In other words, the magnetic field can be regarded as an elliptical rotating magnetic field that changes direction counterclockwise at most points in space.
ここで第3図において、装置4と5のそれぞれ
U相巻線を結ぶ直線上の各地点の磁界について考
察してみると、この線上での磁界は2つのU相巻
線へ流れる同相の電流による磁界が常に互に打消
す様に働き、1サイクルを通じて全体的に磁界強
さの絶対値は小さな値を示す。特にこの直線上の
中央地点においては、2つのU相巻線による磁界
が完全に打消し合い、経時的に常に磁界は零とな
つている。この様子は巻線U―Uの対向する線上
から横方向へ極ピツチP分だけ移動した巻線U1
―U1の対向する線上でも全く同様であり、多極
巻線を施した移動磁界発生装置4,5においては
同相巻線U―UおよびU1―U1の対向するすべて
の線上地点では同じ現象が現われる。一方、第3
図において巻線U―Uの対向する線上より極ピツ
チPの1/2だけ横方向に移動した線上地点での磁
界は、前記とは逆に磁界が互に加算れるように働
き、磁界強さの絶対値は他の線上地点と較べて大
きくなる。この様に移動磁界発生装置4,5の極
ピツチP、電源周波数が互に等しい場合には、作
用空間内における磁界は、その絶対値が移動磁界
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。なお第3図において、
特に装置4,5のU相巻線同士が対向している場
合について説明したが、この傾向は装置4,5の
V相巻線同士、あるいはW相巻線同士が対向して
いても必ず生ずることが、巻線電流と磁界の関係
を時間の進行に従つて逐時追跡することで確認す
ることができる。 Now, in Fig. 3, if we consider the magnetic field at each point on the straight line connecting the U-phase windings of devices 4 and 5, the magnetic field on this line is the in-phase current flowing to the two U-phase windings. The magnetic fields always cancel each other out, and the absolute value of the magnetic field strength shows a small value throughout one cycle. Particularly at the center point on this straight line, the magnetic fields from the two U-phase windings completely cancel each other out, and the magnetic field always becomes zero over time. This situation shows that the winding U 1 is moved laterally by the pole pitch P from the opposite line of the winding U-U.
- It is exactly the same on the opposing wires of U 1 , and in the moving magnetic field generators 4 and 5 with multi-pole windings, it is the same at all points on the opposing wires of in-phase winding U-U and U 1 - U 1 . A phenomenon appears. On the other hand, the third
In the figure, the magnetic field at a point on the line that is moved laterally by 1/2 of the pole pitch P from the opposing line of the winding U-U acts so that the magnetic fields are added to each other, contrary to the above, and the magnetic field strength increases. The absolute value of is larger than other points on the line. In this way, when the pole pitch P and power supply frequency of the moving magnetic field generators 4 and 5 are equal, the absolute value of the magnetic field in the working space is 1/2 of the pole pitch P along the direction of the moving magnetic field. The distribution is such that the strength repeats at intervals. In addition, in Figure 3,
In particular, we have explained the case where the U-phase windings of devices 4 and 5 are facing each other, but this tendency always occurs even if the V-phase windings of devices 4 and 5 or the W-phase windings are facing each other. This can be confirmed by tracking the relationship between the winding current and the magnetic field over time.
一方、先に述べた磁界分布の中でワーキングビ
ースがどの様な運動を行うかを観察するために、
第1図に示す様に容器1の中ワーキングビース3
を納め、その運動を高速カメラで撮影した結果次
の様な傾向が認められた。すなわちスピンドル形
状の個々のワーキングビース3は作用空間内の回
転磁界により、その重心の周りで回転運動を行う
と共に、全体としては移動磁界φ1,φ2の移動
方向に沿つて移動していく。しかしながらこの移
動磁界方向への移動の範囲はほとんどが1極ピツ
チの範囲に限られ、全体の運動経路としては、第
3図の矢印Bに示す経路をたどるようになる。こ
れは先に述べた様に第3図において、巻線U―U
およびU1―U1の対向する線上では磁界の絶対値
が小さく、ワーキングビース3がこの領域を越え
て隣りの強磁界領域まで横方向に駆動する電磁力
が不足するためであり、結局ワーキングビース3
の運動は磁界の強い部分を中心として極ピツチP
の範囲内の周回運動に限定され、処理容器内にお
ける前記強磁界領域の相互間には磁界が弱く、し
たがつてワーキングビース運動の弱い死角空間が
生成されることになる。しかも電磁式処理装置と
しては、前記の現象により第3図における巻線U
―Uおよび1―U1の対向線地点では粉砕等の処
理作用が十分に行われず、このことが処理性能の
向上を防げる大きな要因となつている。 On the other hand, in order to observe how the working bead moves in the magnetic field distribution mentioned above,
As shown in Figure 1, the working bead 3 inside the container 1
The movement was photographed using a high-speed camera, and the following trends were observed. That is, each spindle-shaped working bead 3 rotates around its center of gravity due to the rotating magnetic field in the working space, and moves as a whole along the moving direction of the moving magnetic fields φ 1 and φ 2 . However, the range of movement in the direction of the moving magnetic field is mostly limited to the range of one pole pitch, and the overall movement path follows the path shown by arrow B in FIG. 3. As mentioned earlier, in Figure 3, this means that the windings U-U
This is because the absolute value of the magnetic field is small on the opposing line U 1 - U 1 , and there is insufficient electromagnetic force to drive the working bead 3 laterally across this area to the adjacent strong magnetic field area. 3
The motion of is centered on the part where the magnetic field is strong and the pole pitch P
The magnetic field is weak between the strong magnetic field regions in the processing container, and therefore a blind space where the working bead movement is weak is created. Moreover, as an electromagnetic processing device, due to the above phenomenon, the winding U in FIG.
- U and 1 - U 1 Processing actions such as crushing are not sufficiently performed at the opposing line points, and this is a major factor preventing improvement in processing performance.
この発明は上記の点にかんがみなされたもので
あり、その目的は上記従来装置の欠点を除去し、
処理容器内空間の全域にわたつて磁界の死角空間
を形成させることなくワーキングビースを一様に
ランダム運動させるようにして被処理物の処理性
能の向上を図ることがある。 The present invention has been made in view of the above points, and its purpose is to eliminate the drawbacks of the above-mentioned conventional devices,
The processing performance of the object to be processed may be improved by uniformly and randomly moving the working beads without forming a blind area of the magnetic field throughout the interior space of the processing container.
かかる目的はこの発明により、処理容器を挟ん
で対向配置された一対の移動磁界発生装置への給
電周波数を互に異なる周波数に定めたことにより
達成される。 According to the present invention, this object is achieved by setting the power feeding frequencies to a pair of moving magnetic field generators disposed opposite to each other with a processing container in between to be different frequencies.
以下この発明を図示実施例に基づいて説明す
る。 The present invention will be explained below based on illustrated embodiments.
第4図において、移動磁界発生装置4と5はそ
れぞれ3相電源9より給電を受けて移動磁界φ
1,φ2を生成するわけであるが、この場合に一
方の装置4の給電回路路には、例えばサイクロコ
ンバータのような周波数変換器10が介挿されて
おり、装置5が直接給電を受ける電源9の周波数
に対して装置4への給電周波数を変えるようにさ
れている。 In FIG. 4, moving magnetic field generators 4 and 5 each receive power from a three-phase power supply 9 to generate a moving magnetic field φ.
1 and φ 2. In this case, a frequency converter 10 such as a cycloconverter is inserted in the power supply circuit path of one of the devices 4, and the device 5 receives power directly. The power supply frequency to the device 4 is changed with respect to the frequency of the power source 9.
今、装置4への給電周波数を装置5への給電周
波数の2倍に設定した場合実施例として、次に処
理容器内部の作用空間における磁界分布を第5図
について述べる。第5図は給電周波数が同一であ
る従来の磁界分布を示した第3図と対応させて描
いたものであり、その巻線配列は第2図と同様で
ある。また図示状態は、装置4と5におけるそれ
ぞれU相の巻線を流れる電流がともに正あるいは
負の方向でかつ電流の瞬時値が等しい時点の状態
を示しており、図示の矢印Hはこの時点における
各地点での磁界ベクトルを表わしている。また図
中における円は、それぞれ第3図で述べたように
正弦波電流の1サイクル分のベクトルの軌跡を表
わしたものであるが、このうち特に二重円として
描かれたベクトル軌跡のうちの小円A′は、装置
4と5における同相同士の巻線に流れる電流方向
がともに正あるいは負である期間のベクトル軌跡
を表わしており、この期間には装置4と5の磁界
が互に打ち消し合うように干渉する。これに対し
大円A″は電流方向が互に正、負で逆である期間
のベクトル軌跡を表わしており、この場合には磁
界が互に強め合うように作用する。また装置5に
最も近い部分の各地点でのベクトル軌跡が一重円
Aとして描かれているのは、この地点が装置4か
ら遠く離れていて2倍の周波数で変化する装置4
の磁界のおよぼす影響が小さく、ベクトルHの軌
跡円が多少変形するのみで二重円になるまで至ら
ないことを示めしている。 Now, as an example where the power supply frequency to the device 4 is set to twice the power supply frequency to the device 5, the magnetic field distribution in the working space inside the processing container will be described with reference to FIG. FIG. 5 is drawn in correspondence with FIG. 3, which shows the conventional magnetic field distribution with the same feeding frequency, and the winding arrangement is the same as that in FIG. 2. The illustrated state shows the state at the time when the currents flowing through the U-phase windings of devices 4 and 5 are both in the positive or negative direction and the instantaneous values of the currents are equal, and the illustrated arrow H indicates the state at this point. It represents the magnetic field vector at each point. In addition, each circle in the figure represents a vector locus for one cycle of the sine wave current as described in Figure 3, but among these, the vector locus drawn as a double circle is particularly The small circle A' represents the vector locus during the period when the directions of the currents flowing through the in-phase windings of devices 4 and 5 are both positive or negative, and during this period the magnetic fields of devices 4 and 5 mutually interact. Interfere to cancel each other out. On the other hand, the great circle A'' represents a vector locus during a period when the current direction is positive and negative, and in this case, the magnetic fields act to strengthen each other. The vector locus at each point in the section is drawn as a single circle A because this point is far away from device 4 and changes at twice the frequency of device 4.
This shows that the influence of the magnetic field is small, and the locus circle of vector H is only slightly deformed, but does not become a double circle.
上記第5図の磁界分布を第3図を示した従来方
式の磁界分布とを比較すると、同一周波数で給電
した場合に常に磁界が零となつた巻線U―Uおよ
びU1―U1が対向する線上地点の中点では、第5
図によれば二つのU相巻線の周波数が互に異なる
ために磁界零の状態は回転磁界の1サイクルのう
ち双方の電流波形が交叉し合うほんの一瞬であ
り、常時は大きさの変化する回転磁界が形成され
る様になる。またこの線上から極ピツチの1/2だ
け横方向に移動した線上でも、磁界の位相は異な
るものの、ベクトル軌跡の形状および磁界の絶対
値とも前記した巻線U―U対向線上と同程度とな
り従来方式の場合に形成された処理容器内におけ
る局部的な磁界の強弱がなくなり、、ワーキング
ビースの運動を妨げる磁気的な死角空間がなくな
る。この結果ワーキングピースは処理容器の空間
内すべての部分で十分なランダム運動が可能とな
り、粉砕、混合等の処理性能の向上を図ることが
できる。なお、装置4と5への給電周波数比は例
示した2:1に限らず、任意の比率にしても同様
の効果を得ることができる。また上記の給電周波
数の設定に加えて、対向する移動磁界発生装置4
と5の極ピツチを互に異なるように設定すれば、
より一層の効果が期待できる。 Comparing the magnetic field distribution shown in Figure 5 above with the magnetic field distribution of the conventional system shown in Figure 3, it is found that the windings U-U and U1 - U1 , where the magnetic field is always zero when fed at the same frequency, are At the midpoint of the opposing line points, the fifth
According to the figure, since the frequencies of the two U-phase windings are different from each other, the state of zero magnetic field is only for a moment when both current waveforms intersect in one cycle of the rotating magnetic field, and the magnitude always changes. A rotating magnetic field comes to be formed. Also, even on a line moved laterally from this line by 1/2 of the pole pitch, although the phase of the magnetic field is different, the shape of the vector locus and the absolute value of the magnetic field are the same as on the line opposite the winding U-U, which is the same as in the conventional method. This eliminates the local strength of the magnetic field within the processing container that is created in the case of this method, and eliminates the magnetic dead space that impedes the movement of the working beads. As a result, the working piece can move sufficiently randomly in all parts of the space of the processing container, and processing performance such as crushing and mixing can be improved. Note that the power feeding frequency ratio to the devices 4 and 5 is not limited to the illustrated 2:1, but the same effect can be obtained by setting it to any ratio. In addition to the above-mentioned setting of the power supply frequency, the opposing moving magnetic field generator 4
If we set the pole pitches of and 5 to be different from each other,
Further effects can be expected.
以上述べたようにこの発明によれば、対向する
移動磁界発生装置への給電周波数をそれぞれ異な
る周波数に定めたものであり、したがつて同一周
波数で給電を行つた場合に、処理容器内に磁界の
強弱が極ピツチ1/2の間隔で交互に生じるという
磁界分布が容器内のほぼ全空間で平等に改善さ
れ、ワーキングビースの運動を妨げる磁気的な死
角空間が取り除かれる。かくして処理容器内の全
空間で十分な粉砕、混合等の処理作用が行われ、
電磁式処理装置の性能向上を図ることができる。 As described above, according to the present invention, the power feeding frequencies to the opposing moving magnetic field generators are set to different frequencies. Therefore, when power is fed at the same frequency, the magnetic field inside the processing container is The magnetic field distribution, in which the strength of the magnetic field alternates at intervals of 1/2 the pole pitch, is improved evenly in almost the entire space inside the container, and the magnetic blind space that impedes the movement of the working bead is eliminated. In this way, sufficient processing actions such as crushing and mixing are performed in the entire space inside the processing container.
The performance of the electromagnetic processing device can be improved.
第1図はこの発明の対象である電磁式処理装置
の原理図、第2図は第1図における移動磁界発生
装置の巻線図、第3図は従来における作用空間の
磁界分布図、第4図はこの発明の実施例の給電回
路図、第5図は第3図に対応するこの発明の実施
例による磁界分布図である。
1…処理容器、2…被処理物、3…ワーキング
ビース、4,5…移動磁界発生装置、8…巻線、
9…電源、10…周波数変換器、φ1,φ2…移
動磁界、H…磁界ベクトル。
Fig. 1 is a principle diagram of the electromagnetic processing device that is the object of the present invention, Fig. 2 is a winding diagram of the moving magnetic field generator shown in Fig. 1, Fig. 3 is a conventional magnetic field distribution diagram in the working space, and Fig. 4 is The figure is a power supply circuit diagram of an embodiment of the present invention, and FIG. 5 is a magnetic field distribution diagram of the embodiment of the present invention corresponding to FIG. DESCRIPTION OF SYMBOLS 1... Processing container, 2... Processing object, 3... Working piece, 4, 5... Moving magnetic field generator, 8... Winding wire,
9...Power supply, 10...Frequency converter, φ1 , φ2 ...Moving magnetic field, H...Magnetic field vector.
Claims (1)
ースが収容された処理容器と、それぞれが多相交
流電源から給電される巻線を備えかつ互にその移
動磁界方向を逆に定めて前記処理容器の両側に対
向配置された一対の移動磁界発生装置とを備えて
構成され、前記移動磁界発生装置への給電により
生じた移動磁界の作用に基づく電磁力でワーキン
グビースにランダム運動を生起させて処理容器へ
収容された被処理物の粉砕、混合、撹拌等を行う
処理装置において、前記一対の移動磁界発生装置
への給電周波数を互に異なる周波数に定めたこと
を特徴とする電磁式粉砕、混合、撹拌等処理装
置。1. A processing container containing working beads made of ferromagnetic or non-magnetic conductive material, each of which has a winding powered by a multiphase AC power source, and whose moving magnetic field directions are set opposite to each other so that the working beads are arranged on both sides of the processing container. and a pair of moving magnetic field generators disposed opposite to each other, the working beads are caused to move randomly by electromagnetic force based on the action of the moving magnetic field generated by supplying power to the moving magnetic field generators, and are moved toward the processing container. An electromagnetic pulverization, mixing, and agitation processing apparatus for pulverizing, mixing, stirring, etc., a housed object to be processed, characterized in that the power supply frequencies to the pair of moving magnetic field generators are set to different frequencies. Equal processing equipment.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57093855A JPS58210837A (en) | 1982-06-01 | 1982-06-01 | Electromagnetic treating device for grinding, mixing, agitation or the like |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57093855A JPS58210837A (en) | 1982-06-01 | 1982-06-01 | Electromagnetic treating device for grinding, mixing, agitation or the like |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58210837A JPS58210837A (en) | 1983-12-08 |
| JPS6136452B2 true JPS6136452B2 (en) | 1986-08-19 |
Family
ID=14094029
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57093855A Granted JPS58210837A (en) | 1982-06-01 | 1982-06-01 | Electromagnetic treating device for grinding, mixing, agitation or the like |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58210837A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6182830A (en) * | 1984-09-28 | 1986-04-26 | Mita Ind Co Ltd | Mixing method of powder |
| JPS61125343U (en) * | 1985-01-21 | 1986-08-06 |
-
1982
- 1982-06-01 JP JP57093855A patent/JPS58210837A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58210837A (en) | 1983-12-08 |
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