JPS58210837A - Electromagnetic treating device for grinding, mixing, agitation or the like - Google Patents

Electromagnetic treating device for grinding, mixing, agitation or the like

Info

Publication number
JPS58210837A
JPS58210837A JP57093855A JP9385582A JPS58210837A JP S58210837 A JPS58210837 A JP S58210837A JP 57093855 A JP57093855 A JP 57093855A JP 9385582 A JP9385582 A JP 9385582A JP S58210837 A JPS58210837 A JP S58210837A
Authority
JP
Japan
Prior art keywords
magnetic field
materials
magnetic fields
mixing
treated
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.)
Granted
Application number
JP57093855A
Other languages
Japanese (ja)
Other versions
JPS6136452B2 (en
Inventor
Eiichi Yonezawa
米沢 栄一
Takeo Takahashi
高橋 武男
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric Co Ltd
Fuji Electric Corporate Research and Development Ltd
Fuji Electric Manufacturing Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Fuji Electric Co Ltd, Fuji Electric Corporate Research and Development Ltd, Fuji Electric Manufacturing Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP57093855A priority Critical patent/JPS58210837A/en
Publication of JPS58210837A publication Critical patent/JPS58210837A/en
Publication of JPS6136452B2 publication Critical patent/JPS6136452B2/ja
Granted legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B01PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
    • B01FMIXING, e.g. DISSOLVING, EMULSIFYING OR DISPERSING
    • B01F33/00Other mixers; Mixing plants; Combinations of mixers
    • B01F33/45Magnetic mixers; Mixers with magnetically driven stirrers
    • B01F33/451Magnetic 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

Abstract

PURPOSE:To provide a titled treating device which improves the treatment performance for materials to be treated, by the constitution wherein the electricity to be supplied to a pair of shifting magnetic field generators in opposite directions provided with a treating device in-between is set at the frequencies differing from each other so as to eliminate the dead angle space in magnetic fields. CONSTITUTION:Electricity is supplied to a magnetic field generator 4 from a three- phase power source 9 through a frequency converter 10 such as a cycle converter or the like and the electricity is supplied directly to a magnetic field generator 5 in a device which subjects materials to be treated to grinding, mixing, agitation, etc. by contg. working pieces which are ferromagnetic or non-magnetic conductive materials and the materials to be treated such as solid, powder, liquid or the like in a treating vessel 1, and acting the shifting magnetic fields phi1, phi2 in opposite directions generated by a pair of the shifting magnetic field generators 4, 5 provided with said vessel in- between thereby inducing vigorous random motion in the working pieces. The formation of the dead angle spaces in the magnetic fields where the magnetic fields negate with each other in the vessel 1 is thus obviated and the interference of the motion of the working pieces is prevented.

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
性あるいは非磁性環′亀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
させることによってソーキングピースに激しいフンダム
運動を生起させて、被処理物の粉砕、混合、攪拌等の処
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 such as a solid, powder, or liquid and a working piece made of ferromagnetic or non-magnetic ring material 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 applying a moving magnetic field from the outside to cause a soaking piece to undergo violent undum movement.

頭dピ処理装置では、被処理物の処理がワーキングピー
スの容器内における運動ないしはソーキングピースとの
衝突等によって行われるものであり。
In the head d-pi processing apparatus, processing of the object to be processed is performed by the movement of the working piece within the container or the collision with the soaking piece.

かかる処理を効率的に行わせるには、ワーキングビ ス
が処理容器内の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ン(すること
が望まれる。
In order to carry out such processing efficiently, it is desirable that the working screws be uniformly affected by the moving magnetic field at all positions within the processing container and undergo violent random movements.

この攬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因において、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n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−ト下には移動磁界発生−装置14 、5が対向配
置されておシ、その発生磁界の移動方向は矢印ψ1.φ
2で示すように互に逆方向に定めら扛ている。この移動
磁界発生装[4、5Fiいわゆるリニアモータとしてよ
〈知られており、例えば3相交流巻線を鉄心に沿う作用
による電磁力が働き、ワーキングピース3tまそれ自身
の重心のまわりで回転運!IIhヲ有う2ともに、移動
磁界φ1.φ2によるその移!ll1lll磁界方向に
向けての推進力および浮上刃に加えで1.ワーキングピ
ース同士の衝突、および容器壁面との間の衝突も〃口わ
って容器1の中で激しくランダムな連動を生起する。そ
してこのランダム運動により、扱処理物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、攪拌が進
行する。
A device as shown in FIG. 1 has already been proposed as a processing device for this purpose. That is, in the first factor, 1 is a processing container that houses 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, and this container 1 is sandwiched in the center. Well,
Moving magnetic field generating devices 14 and 5 are disposed opposite to each other below that, and the moving direction of the generated magnetic field is indicated by the arrow ψ1. φ
As shown in 2, they are set in opposite directions. This moving magnetic field generator [4,5Fi] is also known as a so-called linear motor, in which, for example, electromagnetic force acts on the three-phase AC winding along the iron core, and the working piece 3t is rotated around its own center of gravity. ! In both cases, the moving magnetic field φ1. The transfer by φ2! In addition to the propulsion force in the direction of the magnetic field and the floating blade, 1. Collisions between the working pieces and the walls of the container also cause violent random interlocking in the container 1. Due to this random movement, the object 2 to be treated is pulverized, mixed, or agitated by collision with the working piece 3 or the like.

ここで第1図に示す装置の容器1が直かれるべき移動磁
界発生装[4と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
1.移動磁界方向装[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のコイルスロット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においては右方同−Ll−%” −V
IUI −V−W’−u(uとu’、vとv’、wとw
’  はそれぞれ同相で逆向きのコイル導体を示す。)
のI[に、−刃装置5においては、右方向にu−w+−
v−u+−w−v“−Uの様に配列さ扛ていQ。なお巻
線の惨ピッチP(U−01間の距11m)は双方とも等
しい。第3図においては、装置4のU相巻線が装置5の
同じくU相巻線と対向位置して門かれているが、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#全およほさない。また第3図において
、移動磁界発生装置4,5は共に同じ周波秋の電源から
給電を受けており、矢印HはU相巻線の電流が最大(巻
!!i屯流は正弦波としている。)となった時点での各
地点における磁界ベクトルを示している。史に楕円Aは
巻線電流が1サイクル分の変化音した時の、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
、空間内のはとんどの地点で磁界は反ll−7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 generator [4 and 5] in which the container 1 of the apparatus shown in FIG. 1 is to be repaired is conceptually shown in FIG. 3. That is, in Fig. 3, 1. Moving magnetic field direction device [4, 5 is arrow φ1. In order to generate a moving magnetic field in the direction indicated by φ2, as shown in FIG.
Three-phase AC windings 8 indicated by U-X, V-Y, and W-Z are wound in the coil slot 7 of the iron core 6, for example, in a wave winding style.
The phase order is the same on the right in device 4 -Ll-%" -V
IUI -V-W'-u (u and u', v and v', w and w
' indicate coil conductors that are in phase and in opposite directions. )
In the blade device 5, move u-w+- to the right.
The windings are arranged like v-u+-w-v"-U.The pitch P of the windings (the distance between U-01 is 11 m) is the same for both. In FIG. The phase winding is located opposite to the U-phase winding of device 5, but in an actual processing device, it is difficult to tell which phase winding is facing the U-phase winding.
It does not affect its characteristics, etc. In addition, in Fig. 3, the moving magnetic field generators 4 and 5 are both receiving power from a power source with the same frequency, and the arrow H indicates the maximum current in the U-phase winding (the current is a sine wave). ) shows the magnetic field vector at each point. The ellipse A represents the locus of the magnetic field vector H at this point when the winding current changes for one cycle. That is, the magnetic field can be regarded as an elliptical rotating magnetic field that changes direction in the anti-ll-7 direction at most points in space.

ここで第3図において、装置it4と5のでれそれの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″′−)のU相巻線へ流れ
る同相の電流による磁界が常lこ互にI]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。待にこの直線上の中央地点においては、2
つのU相巻#VC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っている。この様子は巻li!11
U−Uの対向する線上から横方向へ極ピッチ2分だけ移
動しまた巻線し1jJI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f![4、5
vr−おいては同相巻線U−υおよびυ′−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−υの対向する線上より極ピッチ
Pの1/2だけ横方向に移動した線上地点での磁界は。
Here, in FIG. 3, the U of the devices it4 and it5
Considering the magnetic field at each point on the straight line connecting the phase windings, we find that the magnetic field on this line is 2''-), and the magnetic field due to the same phase current flowing to the U phase winding is always 1 The absolute value of the magnetic field strength shows a small value throughout one cycle.At the center point on this straight line, 2
The magnetic fields caused by the two U-phase windings #VC completely cancel each other out, and the magnetic field always becomes zero over time. This situation is volume li! 11
The moving magnetic field generator with multi-pole winding f! [4,5
In vr-, the same phenomenon appears at all opposing line points of the in-phase windings U-υ and υ'-U1. on the other hand,
In FIG. 3, the magnetic field at a point on a line that is laterally moved by 1/2 of the pole pitch P from the opposing line of the winding U-υ is:

前記とは逆に磁界が互に加算されるように鋤さ。Contrary to the above, the magnetic fields are added to each other.

磁界強さの絶対値は他の線上地点と較べて太きくなる。The absolute value of the magnetic field strength is thicker than at other points on the line.

この様に#励磁界発生装置4,5の極ピッチP1電源周
波数が互に等しい場合にrよ1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って極ヒツチPの1
/2の間隔で強弱をくシ返すよう1分溜となる。なお第
3図においては、特に装置4.5のU相巻−同士が対向
している場合について祝明したが、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
ても必ず生することが1巻線′亀流と磁界の関係を時間
の進行に従って遂時追跡することで確認することができ
る。
In this way, when the pole pitch P1 of the excitation field generators 4 and 5 is equal to each other, the magnetic field in the r1 action space has an absolute value equal to 1 of the pole pitch P along the direction of the moving magnetic field.
It becomes a 1-minute accumulation so that the strength is alternated at intervals of /2. In addition, in FIG. 3, the case in which the U-phase windings of device 4.5 are opposed to each other is explained in particular, but this tendency is not observed in devices 4 and 5.
By tracking the relationship between the 1st winding's current and the magnetic field over time, it can be confirmed that this phenomenon always occurs even if the V-phase windings or the W-phase windings of 5 are opposed to each other. can.

一力、先に述べた磁界分布の中でワーキングピースがど
の様な運動を行うかを観察するために。
First, to observe how the working piece moves in the magnetic field distribution mentioned above.

第1図に示す様に容器1の中にワーキングピース3を納
め、その運動を^速カメラで撮影した結果仄の様な傾向
が認められた。すなわちスピンドル形状の個々のワーキ
ングピース3は作用空間内の回転磁界により、その重心
の回りで回転運IIdJを行うと共に、全体としては移
動磁界φ1.ψ2の移動方間に沿って移動していく。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扛、全体の41dJ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。
As shown in Fig. 1, a working piece 3 was placed in a container 1, and its movement was photographed using a high-speed camera. As a result, the following tendency was observed. That is, each spindle-shaped working piece 3 performs a rotation movement IIdJ around its center of gravity due to the rotating magnetic field in the working space, and as a whole, the moving magnetic field φ1. It moves along the direction of movement of ψ2. 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 41 dJ path follows the path shown by arrow B in FIG. 3.

これは先に述べた様に第3図において、巻線U−Uおよ
び[J’ −[J’の対向する線上では磁界の絶対値が
小さく、ワーキングピース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年越するため
であり、結局ワーキングピース3の運動は磁界の強い部
分を中心とした極ピンチ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、したがってワーキングピ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 5ては、 Ail記の現象により第3図における巻
1111ilv−UおよびU’ −(J’の対向線上地
点では粉砕等の処理作用が十分に行われず、このことが
処理性症の向上を防ける大きな兼因となっている2、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
目的は上記従来装賑の欠点を除去し、処理容器内窒…1
の全域にわたって磁界の死角9間を形成させることなく
ワーキングピースを一抹にランダム4動させるようにし
て被処m物の処理性能の同上を図ることにある。
This is because, as mentioned earlier, in Fig. 3, the absolute value of the magnetic field is small on the opposing lines of windings U-U and [J'-[J', and working piece 3 crosses this area and increases the strength of the adjacent magnetic field. This is because the electromagnetic force that drives in the lateral direction up to the magnetic field area is overdue, and the movement of the working piece 3 is ultimately limited to circular movement within the range of the polar pinch P around the strong magnetic field area, and the movement within the processing vessel The magnetic field is weak between the strong magnetic field regions, thus creating a blind space where the movement of the working piece is weak. Moreover, since it is an electromagnetic processing device, due to the phenomenon described in Ail, the processing action such as crushing is not performed sufficiently at the point on the opposite line of volumes 1111ilv-U and U'-(J' in Fig. 3, and this causes the processing 2. This invention was made in consideration of the above points, and its purpose is to eliminate the drawbacks of the conventional equipment described above, and to reduce the amount of nitrogen in the processing container.
The object of the present invention is to improve the treatment performance of objects to be treated by moving the working piece randomly in one stroke without forming a blind spot of the magnetic field over the entire area.

かかる目的ンゴこの発明により、処8!容器ケ挾んで対
同配宵された一対の移動S界発生装置への給電周波aを
互に素なる周波数にシtめたことにより達成される。
According to this invention, the purpose of this invention is 8! This is achieved by setting the power supply frequencies a to a pair of moving S field generators placed in the same pair across the container to be disjoint frequencies.

以−トこの発明を図示実施例に基ついて説明する。The present invention will now be explained based on illustrated embodiments.

第4図において、移動磁界発生装貧4と5はそれぞれ3
相屯諒9より給電を受けて移動磁界φ1゜ψ、會生成す
るわけであるが、この場合に一方の装置4の給電回路に
は1例えr丁すイクl−J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i5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, the moving magnetic field generating devices 4 and 5 are each 3
A moving magnetic field φ1゜ψ is generated by receiving power from the power source 9. In this case, the power supply circuit of one of the devices 4 is equipped with a frequency converter such as an r-to-to-J converter. A device 10 is inserted to change the frequency of the power supply to the device 4 with respect to the frequency of the power source 9 to which the device i5 is directly supplied with power.

今、装置4への給電周波数を装置5への給電周波数比2
倍に設定した場合全人mVuとして、矢に処理容器内部
の作用空間におけるA6.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め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ろり、その巻線
配列は弔2図と同様である。まfc凶示状悪Vユ、装置
4と5におけるそれぞれのU相の巻#Mを流れる電流が
ともに止あるいは負の同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1図示の矢印口はこの時点に
おける各地点での磁界ベクトル軌跡表わしている。
Now, the power supply frequency to device 4 is set to the power supply frequency ratio of 2 to device 5.
When set to double, the whole person's mVu is set to A6 in the action space inside the processing container. The field distribution will be described with reference to Figure 5. FIG. 5 is drawn in correspondence with FIG. 3, which shows the conventional magnetic field distribution where the feeding frequency is the same, and the winding arrangement is the same as that in Figure 2. 1 shows the state at the time when the currents flowing through the U-phase windings #M of devices 4 and 5 are both stopped or in the same negative direction and the instantaneous values of the currents are equal. The arrowheads in the figure represent the magnetic field vector locus at each point at this point in time.

ま死因中における円は、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、このうち特に二ム円として描かれたベク
トル軌跡のうちの不肖Alrt。
As described in Figure 3, each circle in the cause of death represents a vector locus for one cycle of a sine wave current, but among these, the vector locus drawn as a bim circle is particularly Unworthy Alrt.

装[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おる期間のベクトル軌跡を表わし
ており、この期間には装#L4と5の磁界が互に打ち消
し合うように干渉する3、これに対し大円A”は電流方
向が互に正、狛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ICは磁界が互に強め合うように作用
する。−t′fC#c直5に最も近い部分の各地点での
ベクトル軌跡が一貞円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の磁界のおよばず影豐が小さく、ベクトルHの
軌跡円か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。
The vector locus represents a period in which the directions of current flowing through the windings of the same phase in L4 and L5 are both positive or negative, and during this period, the magnetic fields of L4 and L5 cancel each other out. Interfering 3. On the other hand, the great circle A'' represents a vector locus during a period in which the current directions are positive and opposite in the direction of the current, and in this case, the IC acts so that the magnetic fields strengthen each other.-t 'fC#c The vector trajectory at each point closest to the straight 5 is drawn as Issada circle A because this point is far away from the device 4 and changes at twice the frequency of the device 4. This shows that the influence and influence of the magnetic field is small, and the locus circle of vector H is only slightly deformed, but does not reach the point of becoming a double circle.

上記第51の磁界分布を第3図に示した従来方式の4I
nIy+−分伯とを比較すると、同一周波数で給電した
揚台にIK磁界が苓となった巻−U−Uおよびu’−u
″が対向する線上地やの中点では、第5図によれば二つ
のU相巻線の周波数か弘Vこ異なるために磁界苓の状態
は回転磁界の1サイクルのうち双方の′1渡波形が交叉
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Icなる。またこの線上から極ピッ
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計よび磁界の絶対
値ともAil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、ワーキングピースの運動を妨
け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。
The 51st magnetic field distribution is shown in Figure 3.
Comparing nIy+-branch, windings -U-U and u'-u where the IK magnetic field is reduced to the lifting platform fed with the same frequency.
At the midpoint of the two opposite wires, as shown in Figure 5, since the frequencies of the two U-phase windings are different, the state of the magnetic field is equal to the 1-pass of both in one cycle of the rotating magnetic field. It is only for a moment that the waveforms intersect, and a rotating magnetic field whose magnitude always changes is formed.Also, even on a line moved laterally by 1/2 of the pole pitch from this line, the phase of the % magnetic field is Although it is different, the vector locus shape meter and the absolute value of the magnetic field are the same as on the winding U-U opposing line marked Ail, and the local strength of the magnetic field inside the processing container that is formed in the conventional method is eliminated, and the working There is no magnetic blind space that hinders the movement of the pieces.As a result, the working pieces can move sufficiently randomly in all parts of the processing container, improving processing performance such as pulverization, crushing, and mixing. I can do it.

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。また上記の給酸周波数の設定に加えて、対向する
移動磁界発生装置11i!t4と5の他ピッチを互に異
なるように設定すれば、より−1−の効果が期待できる
Note that the power feeding frequency ratio to the % devices 4 and 5 is not limited to the illustrated example of 2=1, but the same effect can be obtained by setting it to an arbitrary ratio. In addition to the above-described setting of the oxygen supply frequency, the opposing moving magnetic field generator 11i! If the other pitches of t4 and t5 are set to be different from each other, a more -1- effect 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、したがって同一周波数で給電を行った場
合に、処理容器内に磁界の強弱が極ピッチの1/2の間
隔で交互に生じるという磁界分布が容器内のはif全空
間で平等に数音され、ワーキングピ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< L、て処理容
器内の全空間で十分な粉砕、混合等の処理作用か行われ
、電磁式処理装置の性能同上を図ることができる。
As described above, according to the present invention, the power supply frequencies to the opposing moving magnetic field generators are set to different frequencies, so that when power is supplied at the same frequency, the strength of the magnetic field inside the processing container is different. A magnetic field distribution in which the magnetic fields are generated alternately at intervals of 1/2 of the pole pitch is distributed evenly over the entire space in the container, and magnetic dead space that impedes the movement of the working piece is eliminated. In this case, sufficient processing operations such as crushing and mixing can be performed in the entire space inside the processing container, and the performance of the electromagnetic processing device can be improved.

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

纂1図はこの発明の対象でおる電磁式処理装置の原理図
、第2図は第1図における移m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・・・仮処理物、3・・・ワーキ
ングピース、4.5・・・移動磁界発生装置、8・・・
巻線。 9・・・電源、10・・・周波数変換器、φ1.ψ2・
・・移動磁界、H・・・磁界ベクトル。
Figure 1 is a principle diagram of the electromagnetic processing device that is the subject of this invention, Figure 2 is a winding diagram of the shifting magnetic field generator in Figure 1,
FIG. 3 is a conventional magnetic field distribution diagram in the working space, FIG. 4 is a power supply circuit diagram according to an embodiment of the present invention, and FIG. 5 is a magnetic field distribution diagram according to an embodiment of the present invention corresponding to FIG. DESCRIPTION OF SYMBOLS 1... Processing container, 2... Temporarily processed material, 3... Working piece, 4.5... Moving magnetic field generator, 8...
winding. 9...Power supply, 10...Frequency converter, φ1. ψ2・
...Moving magnetic field, H...Magnetic field vector.

Claims (1)

【特許請求の範囲】[Claims] 1)強磁性あるいは非磁性導電材のソーキングピースが
収容された処理容器と、それぞれが多相装置された一対
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
電磁力でソーキングピ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、攪拌等を
行う処理装置において、前記一対の移動磁界発生装置−
\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、攪拌等処理装置。
1) A processing container containing a soaking piece made of a ferromagnetic or non-magnetic conductive material, and a pair of moving magnetic field generators, each of which is a multi-phase device, are constructed, and the magnetic field generator is generated by supplying power to the moving magnetic field generators. In the processing apparatus for pulverizing, mixing, stirring, etc. a workpiece housed in a processing container by causing a random motion in a soaking piece using electromagnetic force based on the action of a moving magnetic field, the pair of moving magnetic field generating devices-
An electromagnetic grinding, mixing, stirring, etc. processing device characterized by setting the power supply frequencies of \ to different frequencies.
JP57093855A 1982-06-01 1982-06-01 Electromagnetic treating device for grinding, mixing, agitation or the like Granted JPS58210837A (en)

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 true JPS58210837A (en) 1983-12-08
JPS6136452B2 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)

Cited By (2)

* Cited by examiner, † Cited by third party
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

Cited By (2)

* Cited by examiner, † Cited by third party
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

Also Published As

Publication number Publication date
JPS6136452B2 (en) 1986-08-19

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