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JP5201582B2 - Solid-liquid separator - Google Patents
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JP5201582B2 - Solid-liquid separator - Google Patents

Solid-liquid separator Download PDF

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JP5201582B2
JP5201582B2 JP2008215075A JP2008215075A JP5201582B2 JP 5201582 B2 JP5201582 B2 JP 5201582B2 JP 2008215075 A JP2008215075 A JP 2008215075A JP 2008215075 A JP2008215075 A JP 2008215075A JP 5201582 B2 JP5201582 B2 JP 5201582B2
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magnetic
permanent magnet
electromagnet
solid
inner cylinder
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JP2009074688A (en
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政英 大島
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Tokyo University of Science
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16CSHAFTS; FLEXIBLE SHAFTS; ELEMENTS OR CRANKSHAFT MECHANISMS; ROTARY BODIES OTHER THAN GEARING ELEMENTS; BEARINGS
    • F16C32/00Bearings not otherwise provided for
    • F16C32/04Bearings not otherwise provided for using magnetic or electric supporting means
    • F16C32/0406Magnetic bearings
    • F16C32/044Active magnetic bearings
    • F16C32/0474Active magnetic bearings for rotary movement
    • F16C32/0476Active magnetic bearings for rotary movement with active support of one degree of freedom, e.g. axial magnetic bearings
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16CSHAFTS; FLEXIBLE SHAFTS; ELEMENTS OR CRANKSHAFT MECHANISMS; ROTARY BODIES OTHER THAN GEARING ELEMENTS; BEARINGS
    • F16C32/00Bearings not otherwise provided for
    • F16C32/04Bearings not otherwise provided for using magnetic or electric supporting means
    • F16C32/0406Magnetic bearings
    • F16C32/044Active magnetic bearings
    • F16C32/0459Details of the magnetic circuit
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16CSHAFTS; FLEXIBLE SHAFTS; ELEMENTS OR CRANKSHAFT MECHANISMS; ROTARY BODIES OTHER THAN GEARING ELEMENTS; BEARINGS
    • F16C2320/00Apparatus used in separating or mixing
    • F16C2320/42Centrifuges

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  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Magnetic Bearings And Hydrostatic Bearings (AREA)
  • Centrifugal Separators (AREA)

Description

本発明は固液分離機に係わり、特に電磁石の電源が入っているときには所定の剛性を維持でき、電源が切られた際にはベアリングにタッチダウン可能で、かつ制御方向に直角な偏心に対しても有効に作用しつつこの偏心方向には磁束の漏れが少ない固液分離機に関する。 The present invention relates to a solid- liquid separator, and can maintain a predetermined rigidity, particularly when an electromagnet is turned on, and can be touched down to a bearing when the power is turned off, and against eccentricity perpendicular to the control direction. while working effectively be about solid-liquid separator has less leakage of the magnetic flux in the eccentric direction.

遠心分離機の原理で固体と液体を分離する固液分離機は化学工業や鉱業、窯業、金属工業の分野における製品製造や排水処理などに広く用いられている。例えば化学工業の分野では、携帯電話にも用いられているニッケル合金や水酸化アルミなどの合金、微粉の回収に用いられたり、鉱業、窯業、金属工業では微粉炭や金属鉱石の回収に用いられている。   Solid-liquid separators that separate solids and liquids based on the principle of centrifuges are widely used in product manufacturing and wastewater treatment in the fields of chemical industry, mining industry, ceramic industry, and metal industry. For example, in the chemical industry, nickel alloys and aluminum hydroxide alloys used in mobile phones are used to collect fine powder, and in the mining, ceramics, and metal industries, it is used to collect pulverized coal and metal ores. ing.

固液分離機としては図23に示したような横型が主流である。ところで、横型は筒底に分離水が蓄積し効率が悪いことが認識されている。そこで、この効率を改善するため、図24に示したような縦型にすると、分離水が360度方向に拡散し、効率的に固液分離が可能である。   As a solid-liquid separator, a horizontal type as shown in FIG. 23 is the mainstream. By the way, it has been recognized that the horizontal type is inefficient because separated water accumulates at the bottom of the cylinder. Therefore, in order to improve this efficiency, if the vertical type as shown in FIG. 24 is used, the separated water diffuses in the direction of 360 degrees, so that solid-liquid separation can be performed efficiently.

図25にこの縦型固液分離機100の構造を示す。この構造については特許文献1に開示がある。図25において、外筒1の内側にはアンギュラ軸受3を介して内筒5が回転自在に軸支されている。このアンギュラ軸受3により内筒5は径方向、軸方向共に安定して支持されるようになっている。   FIG. 25 shows the structure of the vertical solid-liquid separator 100. This structure is disclosed in Patent Document 1. In FIG. 25, an inner cylinder 5 is rotatably supported inside the outer cylinder 1 via an angular bearing 3. By this angular bearing 3, the inner cylinder 5 is stably supported in both the radial direction and the axial direction.

そして、この内筒5の内側には、周囲に螺旋状に突設された分流リブ板6(均等拡散装置)を備えるスクリューコンベアー7が回転自在なようになっている。このスクリューコンベアー7の中間部分には通路9が形成されている。そして、この通路9は、スクリューコンベアー7の中心を貫通する貫通穴11と連通され、更にこの貫通穴11は外筒1の上端に形成されたフィード口13と連通されている。また、外筒1の上面と内筒5、スクリューコンベアー7の間の空間には堰15が形成され、この堰15は外筒1に設けられた排出口17に通じている。   And inside this inner cylinder 5, the screw conveyor 7 provided with the shunt rib board 6 (equal spreading | diffusion apparatus) which protruded spirally around the circumference | surroundings is made rotatable. A passage 9 is formed in an intermediate portion of the screw conveyor 7. The passage 9 communicates with a through hole 11 that penetrates the center of the screw conveyor 7, and the through hole 11 communicates with a feed port 13 formed at the upper end of the outer cylinder 1. A weir 15 is formed in the space between the upper surface of the outer cylinder 1, the inner cylinder 5, and the screw conveyor 7, and the weir 15 leads to a discharge port 17 provided in the outer cylinder 1.

内筒5とスクリューコンベアー7は本体上部に取り付けられた図示しない差速装置により速度差をつけて同方向に回転される。原液を本体上部のフィード口13から投入すると貫通穴11及び通路9を介して内筒5とスクリューコンベアー7の間に形成された空間に入る。その後、遠心効果により固形物は内筒5の内壁に付着してスクリューコンベアー7で下方に排出され、比重の軽い分離液は推力によって上昇し、堰15を通って排出口17より外部に排出される。   The inner cylinder 5 and the screw conveyor 7 are rotated in the same direction with a speed difference by a differential speed device (not shown) attached to the upper part of the main body. When the stock solution is introduced from the feed port 13 at the top of the main body, it enters a space formed between the inner cylinder 5 and the screw conveyor 7 through the through hole 11 and the passage 9. Thereafter, the solid matter adheres to the inner wall of the inner cylinder 5 by the centrifugal effect and is discharged downward by the screw conveyor 7, and the separated liquid having a low specific gravity rises by thrust and is discharged to the outside through the discharge port 17 through the weir 15. The

次にこの縦型固液分離機100の特徴について説明する。スクリューコンベアー7の中程には分流リブ板6(均等拡散装置)が設けられており、供給された原液を360度方向に拡散させている。   Next, features of the vertical solid-liquid separator 100 will be described. In the middle of the screw conveyor 7, a diverting rib plate 6 (equal diffusion device) is provided, and the supplied stock solution is diffused in the direction of 360 degrees.

そして、部品一つ一つのバランスを取り、均等に重量配分させて安定構造となっているため、微振動型で安定している。脱水効果は、従来型の脱水機と比較して、5〜20%以上の低含水率である。固液の分離は、遠心力と固形物と液体の比重差で分離させているので、比重差のある固体スラリーであれば、サブミクロンの微細粒子の回収ができる。また、脱水から濃縮まで幅広く対応が可能である。   And since each component is balanced and the weight is evenly distributed to form a stable structure, it is stable with a fine vibration type. The dehydration effect has a low water content of 5 to 20% or more as compared with a conventional dehydrator. Since the solid-liquid separation is performed by centrifugal force and the specific gravity difference between the solid and the liquid, sub-micron fine particles can be recovered if the solid slurry has a specific gravity difference. In addition, it can handle a wide range from dehydration to concentration.

ところで、上述した固液分離作業の効率をより一層上昇させるためには、装置を大型にして処理容量の増加を図ることが望まれる。この際には、装置の大型化にともない、アンギュラ軸受3の径を広げる必要がある。しかしながら、規格により現状のものより大きなアンギュラ軸受3は存在しない。   By the way, in order to further increase the efficiency of the solid-liquid separation operation described above, it is desired to increase the processing capacity by increasing the size of the apparatus. At this time, it is necessary to increase the diameter of the angular bearing 3 as the apparatus becomes larger. However, there is no angular bearing 3 larger than the current one according to the standard.

そこで、この問題を解決するため、今回発明者等によりアンギュラ軸受3の替わりに磁気軸受を採用することが提案及び検討された。この装置の大型化に伴い電磁力としては軸方向にほぼ7000(N)程度以上必要であることも検討された。ここに、磁気軸受により軸方向や径方向を支持する先行技術として、従来、例えば特許文献2や特許文献3が知られている。
特開2007−038068号公報 特開2005−121157号公報(図8) 特開平8−296645号公報(図8)
Therefore, in order to solve this problem, the present inventors have proposed and studied to adopt a magnetic bearing instead of the angular bearing 3. With the increase in the size of this apparatus, it has also been examined that the electromagnetic force is required to be approximately 7000 (N) or more in the axial direction. Heretofore, for example, Patent Document 2 and Patent Document 3 are known as prior arts that support the axial direction and the radial direction by a magnetic bearing.
JP 2007-038068 A Japanese Patent Laying-Open No. 2005-121157 (FIG. 8) JP-A-8-296645 (FIG. 8)

ところで、従来の特許文献2や特許文献3による方法では電磁石と永久磁石との組み合わせにより吸引力を発生させるものであり、電磁石の鉄心の向きと永久磁石の起磁力の向きとが一致するように配設されている。このため、電磁石の電源を切った後でも永久磁石の鉄心に対する作用により吸引力が残ってしまう。従って、別途配設されたベアリングにタッチダウンさせる形で装置を停止することが出来なかった。   By the way, in the conventional methods according to Patent Document 2 and Patent Document 3, an attractive force is generated by a combination of an electromagnet and a permanent magnet, and the direction of the iron core of the electromagnet and the direction of the magnetomotive force of the permanent magnet match. It is arranged. For this reason, even after the electromagnet is turned off, an attractive force remains due to the action of the permanent magnet on the iron core. Therefore, the apparatus could not be stopped by touching down separately provided bearings.

本発明はこのような従来の課題に鑑みてなされたもので、電磁石の電源が入っているときには所定の剛性を維持でき、電源が切られた際にはベアリングにタッチダウン可能で、かつ制御方向に直角な偏心に対しても有効に作用しつつこの偏心方向には磁束の漏れが少ない固液分離機を提供することを目的とする。 The present invention has been made in view of such a conventional problem, and can maintain a predetermined rigidity when the electromagnet is turned on, can touch down the bearing when the power is turned off, and has a control direction. and to provide a solid-liquid separator has less leakage of the magnetic flux in the eccentric direction while effectively acts against perpendicular eccentricity.

このため本発明(請求項1)は、回転軸を中心に回転する回転体に形成された回転コアと、該回転コアに配設され軸方向に磁極を有する永久磁石と、該永久磁石と対峙して配設され軸方向に磁極を有し前記回転軸回りに均等配設された複数の電磁石と、該電磁石が取り付けられた固定子コアと、前記回転体の軸方向位置を検出する位置センサと、該位置センサで検出した位置信号に基づき前記回転体の軸方向の位置を調整する軸方向位置調整手段とを有し、前記永久磁石が軸方向に一つ配設された磁気軸受装置を搭載した縦型の固液分離機であって、前記回転体が内筒であり、該内筒の内側に該内筒とは異なる速度にて駆動されるスクリューを備え、該スクリューを貫通する貫通穴を通じて流入した固体及び液体の混合原液が前記内筒と前記スクリューの間に回転しつつ通されることで固体と液体とが分離されることを特徴とする
以上により、軸方向に作用する起磁力を所望としている起磁力の大きさに調整できる。
内筒の内部を流れる原液が磁性体の場合、原液が磁気軸受付近を通過する際に磁気軸受が作る磁場により影響を受ける恐れがある。しかしながら、本磁気軸受を搭載した固液分離機においては、運転中には磁束は閉磁路を流れ、一方、停止のときには永久磁石の磁界の大部分が比透磁率の高い材質からなる回転コアを流れる漏れ磁束となるため外部に対し磁場の影響を与えることがない。
また、本発明(請求項2)は、前記電磁石及び前記永久磁石により発生した磁束が前記固定子コアと内筒側ギャップと前記内筒と前記回転コアを通る第1の閉磁路と、前記電磁石及び前記永久磁石により発生した磁束が前記固定子コアと該固定子コアに連設する外筒と外筒側ギャップと前記回転コアを通る第2の閉磁路とが形成されることを特徴とする。
For this reason, the present invention (Claim 1) includes a rotating core formed on a rotating body that rotates about a rotating shaft, a permanent magnet that is disposed on the rotating core and has a magnetic pole in the axial direction, and the permanent magnet is opposed to the rotating magnet. A plurality of electromagnets that have magnetic poles in the axial direction and are evenly arranged around the rotation axis, a stator core to which the electromagnets are attached, and a position sensor that detects the axial position of the rotating body And an axial position adjusting means for adjusting an axial position of the rotating body based on a position signal detected by the position sensor, and a magnetic bearing device in which one permanent magnet is disposed in the axial direction. A vertical solid-liquid separator mounted, wherein the rotating body is an inner cylinder, and a screw driven at a speed different from that of the inner cylinder is provided inside the inner cylinder, and passes through the screw. The mixed stock solution of solid and liquid flowing in through the hole The solid and liquid by being passed while rotating between the clew is characterized in that it is separated
As described above, the magnetomotive force acting in the axial direction can be adjusted to the desired magnitude of the magnetomotive force.
When the undiluted solution flowing inside the inner cylinder is a magnetic material, the undiluted solution may be affected by the magnetic field generated by the magnetic bearing when it passes near the magnetic bearing. However, in a solid-liquid separator equipped with this magnetic bearing, the magnetic flux flows in a closed magnetic path during operation, while when stopped, a rotating core made of a material having a high relative permeability is used for the majority of the magnetic field of the permanent magnet. Since it is a leakage flux that flows, there is no influence of the magnetic field on the outside.
In addition, the present invention (Claim 2) includes a first closed magnetic path in which magnetic flux generated by the electromagnet and the permanent magnet passes through the stator core, the inner cylinder side gap, the inner cylinder, and the rotating core, and the electromagnet. And a magnetic flux generated by the permanent magnet is formed with the stator core, an outer cylinder connected to the stator core, an outer cylinder side gap, and a second closed magnetic path passing through the rotating core. .

更に、本発明は、回転軸を中心に回転する回転体に形成され比透磁率の高い材質からなる回転コアと、該回転コアに対し前記回転軸を中心に環状に形成された複数の磁性体部と、該磁性体部の間に挟装され、径方向に磁極を有する少なくとも一つの永久磁石と、前記磁性体部と対峙して環状に配設され前記永久磁石を介し閉磁路が形成されるように軸方向に向けた磁極をそれぞれ有する複数の電磁石と、該電磁石が取り付けられた固定子コアと、前記回転体の軸方向位置を検出する位置センサと、該位置センサで検出した位置信号に基づき前記回転体の軸方向の位置を調整する軸方向位置調整手段とを備えて構成してもよい Furthermore, the onset Ming, a rotary core of material with high relative permeability is formed on the rotating body which rotates about a rotation axis, a plurality of magnetic formed annularly around the rotation axis with respect to the rotating core A body part, at least one permanent magnet sandwiched between the magnetic body parts and having magnetic poles in the radial direction, and a ring disposed opposite to the magnetic body part to form a closed magnetic path via the permanent magnets A plurality of electromagnets each having a magnetic pole directed in the axial direction, a stator core to which the electromagnet is attached, a position sensor for detecting the axial position of the rotating body, and a position detected by the position sensor An axial position adjusting means for adjusting the axial position of the rotating body based on the signal may be provided .

比透磁率は7000以上であることが望ましい。電磁石に流れる電流を切ると閉磁路を流れていた電磁石による磁束は消滅する。このとき、永久磁石の磁界は大部分が比透磁率の高い材質からなる回転コアを流れる漏れ磁束となるため軸方向に作用する磁界は極度に弱まり、回転体は自重により落下し、ベアリング等にタッチダウンする。   The relative magnetic permeability is desirably 7000 or more. When the current flowing through the electromagnet is cut off, the magnetic flux generated by the electromagnet flowing through the closed magnetic path disappears. At this time, the magnetic field of the permanent magnet is mostly leakage magnetic flux that flows through the rotating core made of a material with high relative permeability, so that the magnetic field acting in the axial direction is extremely weakened, and the rotating body falls by its own weight and falls to the bearing etc. Touch down.

また、電磁石が環状であり、永久磁石も同様に環状に形成される。このため、電磁石及び磁性体部には永久磁石を介し閉磁路が形成され、半径方向にも復元力を有することができる。このことにより、回転体が半径方向にずれたときにも復元力が働くので半径方向への支持が可能になる。   Further, the electromagnet is annular, and the permanent magnet is similarly annularly formed. For this reason, a closed magnetic circuit is formed in the electromagnet and the magnetic body part via the permanent magnet, and it can have a restoring force in the radial direction. As a result, the restoring force works even when the rotating body is displaced in the radial direction, so that it is possible to support in the radial direction.

以上説明したように本発明によれば、回転コアに配設され軸方向に磁極を有する永久磁石と、この永久磁石と対峙して固定子コアに配設され軸方向に磁極を有し回転軸回りに均等配設された複数の電磁石とを備えて構成したので、軸方向に作用する起磁力を所望としている起磁力の大きさに調整できる。   As described above, according to the present invention, a permanent magnet disposed on a rotating core and having a magnetic pole in the axial direction, and a rotating magnet having a magnetic pole in the axial direction disposed on the stator core opposite to the permanent magnet. Since it comprises a plurality of electromagnets arranged evenly around, the magnetomotive force acting in the axial direction can be adjusted to the desired magnitude of the magnetomotive force.

以下、本発明の実施形態について説明する。本発明の第1実施形態である固液分離機200の磁気軸受周辺の概念構成図を図1に示す。図1において、外筒21の内壁には外筒21の上端面27と平行に固定子コア29が環状に内側に向けて突設されている。   Hereinafter, embodiments of the present invention will be described. The conceptual block diagram of the magnetic bearing periphery of the solid-liquid separator 200 which is 1st Embodiment of this invention is shown in FIG. In FIG. 1, a stator core 29 is provided on the inner wall of the outer cylinder 21 so as to protrude inward in an annular shape in parallel with the upper end surface 27 of the outer cylinder 21.

そして、この固定子コア29の下面には、図2に示すように4つの電磁石33A、33B、33C、33D及びギャップセンサ34A、34B、34C、34Dが配設されている。電磁石33A、33B、33C、33Dは上側がN極、下側がS極に励磁されるようになっている。   As shown in FIG. 2, four electromagnets 33A, 33B, 33C, 33D and gap sensors 34A, 34B, 34C, 34D are disposed on the lower surface of the stator core 29. The electromagnets 33 </ b> A, 33 </ b> B, 33 </ b> C, and 33 </ b> D are excited to have an N pole on the upper side and an S pole on the lower side.

また、内筒25の中央部付近には回転子コア35が周状に突設されている。そして、この回転子コア35の上面には図3に示すように中空環状の永久磁石37が固着されている。永久磁石37は上側がN極、下側がS極に着磁されている。内筒25は、回転軸を中心に回転するようになっている。また、外筒21の上端面と内筒25の外周壁との間にはタッチダウンベアリング23が環状に介設されている。   In addition, a rotor core 35 is provided in a projecting manner in the vicinity of the center of the inner cylinder 25. A hollow annular permanent magnet 37 is fixed to the upper surface of the rotor core 35 as shown in FIG. The permanent magnet 37 is magnetized with an N pole on the upper side and an S pole on the lower side. The inner cylinder 25 rotates around the rotation axis. A touchdown bearing 23 is interposed between the upper end surface of the outer cylinder 21 and the outer peripheral wall of the inner cylinder 25 in an annular shape.

次に、本発明の第1実施形態の動作を説明する。
ギャップセンサ34A、34B、34C、34Dで回転子コア35までの軸方向の距離(ギャップ)を測る。そして、この計測した距離が所望の値となるように電磁石33A、33B、33C、33Dに流す電流を変化させる。このことより、運転中の軸方向位置を調整可能である。
Next, the operation of the first embodiment of the present invention will be described.
The distance (gap) in the axial direction to the rotor core 35 is measured by the gap sensors 34A, 34B, 34C, and 34D. And the electric current sent through electromagnet 33A, 33B, 33C, 33D is changed so that this measured distance may become a desired value. This makes it possible to adjust the axial position during operation.

なお、図1中には点線で磁束の方向を示している。磁束は、永久磁石37と電磁石33A、33B、33C、33Dとにより発生し、一方のルートは外筒21を通る磁路により形成され、他方のルートは内筒25を通る磁路により形成される。   In FIG. 1, the direction of the magnetic flux is indicated by a dotted line. The magnetic flux is generated by the permanent magnet 37 and the electromagnets 33A, 33B, 33C, and 33D. One route is formed by a magnetic path passing through the outer cylinder 21, and the other route is formed by a magnetic path passing through the inner cylinder 25. .

このため、電磁石磁束、永久磁石磁束ともに漏れ磁束が少ない。電磁石33A、33B、33C、33Dの電源が入っているときには所定の剛性を維持でき、電源が切られた際には自重により内筒25は落下し、タッチダウンベアリング23にタッチダウンする。   For this reason, both the electromagnet magnetic flux and the permanent magnet magnetic flux have little leakage magnetic flux. Predetermined rigidity can be maintained when the electromagnets 33A, 33B, 33C, and 33D are turned on. When the power is turned off, the inner cylinder 25 falls due to its own weight and touches down the touch-down bearing 23.

ここに、軸方向にどの程度の起磁力を発生可能かシミュレーションを行った。シミュレーションは、磁気軸受のモデリングと電磁力解析に有限要素法解析ソフトを用いた。基本となる簡易モデルの固定子側の図面を図4に、回転子側の図面を図5に、シミュレーションに用いた材料及び仕様を図6に示す。   Here, a simulation was performed to determine how much magnetomotive force can be generated in the axial direction. The simulation used finite element method analysis software for magnetic bearing modeling and electromagnetic force analysis. FIG. 4 shows the drawing of the basic simplified model on the stator side, FIG. 5 shows the drawing on the rotor side, and FIG. 6 shows the materials and specifications used in the simulation.

なお、図4に示すように、固定子コア29には電磁石鉄心29aが4箇所突設され、その周囲にコイルが巻かれて電磁石33A、33B、33C、33Dが形成されている。しかしながら、この電磁石は4個とは限らず、2個若しくは3個等とされてもよい。ギャップセンサ34A、34B、34C、34Dも電磁石に合わせて4個配置したが、X軸方向に一つY軸方向に一つ配設されるようにしてもよい。   As shown in FIG. 4, the stator core 29 is provided with four electromagnet cores 29a, and coils are wound around the electromagnet cores 29a to form electromagnets 33A, 33B, 33C, and 33D. However, the number of electromagnets is not limited to four, and may be two or three. Although four gap sensors 34A, 34B, 34C, and 34D are arranged in accordance with the electromagnets, one gap sensor 34A, 34B, 34C, and 34D may be arranged in the Y-axis direction.

電磁石33A、33B、33C、33Dは有効ギャップ断面積を広く取れるため、アキシャル電磁力が大きい。
このように電磁石を複数個に分割することでアキシャル方向位置制御に加えて、傾き制御も可能である。
Since the electromagnets 33A, 33B, 33C, and 33D have a wide effective gap cross-sectional area, the axial electromagnetic force is large.
In this way, by dividing the electromagnet into a plurality of pieces, in addition to axial position control, tilt control is also possible.

解析結果を図7に示す。このことより、電流6(A)程度を流せば軸方向に作用する起磁力が所望としている起磁力7000(N)を超えることが分かる。   The analysis results are shown in FIG. From this, it can be seen that the magnetomotive force acting in the axial direction exceeds the desired magnetomotive force 7000 (N) when a current of about 6 (A) is passed.

次に、本発明の第2実施形態について説明する。
本発明の第2実施形態である固液分離機300の磁気軸受周辺の概念構成図を図8に示す。なお、図1と同一要素のものについては同一符号を付して説明は省略する。図8において、固定子コア29の下面には2つの電磁石鉄心29a、29bが突設されている。
Next, a second embodiment of the present invention will be described.
The conceptual block diagram of the magnetic bearing periphery of the solid-liquid separator 300 which is 2nd Embodiment of this invention is shown in FIG. Note that the same elements as those in FIG. 1 are denoted by the same reference numerals and description thereof is omitted. In FIG. 8, two electromagnet cores 29 a and 29 b protrude from the lower surface of the stator core 29.

そして、この2つの電磁石鉄心29a、29bの間に一つの環状スロット49が形成されている。そして、この環状スロット49と電磁石鉄心29aの内側及び環状スロット49と電磁石鉄心29bの外側とにそれぞれ巻線を配設する。磁束の方向は図8に示す通り電磁石鉄心29aについては上向きであり、電磁石鉄心29bについては下向きである。   One annular slot 49 is formed between the two electromagnet cores 29a and 29b. Then, windings are disposed on the annular slot 49 and the inner side of the electromagnet core 29a and on the outer side of the annular slot 49 and the electromagnet core 29b, respectively. As shown in FIG. 8, the direction of the magnetic flux is upward for the electromagnet core 29a and downward for the electromagnet core 29b.

その結果、この環状スロット49を挟んだ形で回転軸を中心として環状に電磁石43、45が形成される。一方、回転子コア35の上面には、この電磁石鉄心29a、29bに対峙するように回転軸を中心として環状に磁性体51、53が突設されている。   As a result, the electromagnets 43 and 45 are formed in an annular shape around the rotation axis with the annular slot 49 interposed therebetween. On the other hand, on the upper surface of the rotor core 35, magnetic bodies 51 and 53 project in a ring shape around the rotation axis so as to face the electromagnet cores 29a and 29b.

そして、この磁性体51、53の間に環状の永久磁石55が固着されている。永久磁石55は径方向に設置され内側がN極、外側がS極に構成されている。即ち、永久磁石55の磁極の向きは電磁石43、45の鉄心コア29a、29bの突設方向に対し直角に配設されている。   An annular permanent magnet 55 is fixed between the magnetic bodies 51 and 53. The permanent magnet 55 is installed in the radial direction and has an N pole on the inner side and an S pole on the outer side. That is, the direction of the magnetic pole of the permanent magnet 55 is arranged at right angles to the protruding direction of the iron cores 29a and 29b of the electromagnets 43 and 45.

次に、本発明の第2実施形態の動作を説明する。
ギャップセンサ44で回転子コア35までの軸方向の距離(ギャップ)を測る。そして、この計測した距離が所望の値となるように電磁石43、45に流す電流を変化させる。
Next, the operation of the second embodiment of the present invention will be described.
The gap sensor 44 measures the axial distance (gap) to the rotor core 35. And the electric current sent through the electromagnets 43 and 45 is changed so that this measured distance may become a desired value.

このことにより、運転中の軸方向位置を調整可能である。なお、図8中には点線で磁束の方向を示している。磁束は、永久磁石55と電磁石43、45とにより生成され、固定子コア29及び磁性体51、53を通り閉磁路が形成される。回転子コア35は電磁鋼板で形成されており、比透磁率が高いため磁束が通り易くなっている。ここに、回転子コア35は電磁鋼板に限らず、炭素鋼であってもよい。比透磁率は7000以上であることが望ましい。   As a result, the axial position during operation can be adjusted. In FIG. 8, the direction of the magnetic flux is indicated by a dotted line. The magnetic flux is generated by the permanent magnet 55 and the electromagnets 43 and 45, and a closed magnetic path is formed through the stator core 29 and the magnetic bodies 51 and 53. The rotor core 35 is made of an electromagnetic steel plate and has a high relative permeability so that magnetic flux can easily pass therethrough. Here, the rotor core 35 is not limited to an electromagnetic steel plate, and may be carbon steel. The relative magnetic permeability is desirably 7000 or more.

電磁石43、45に流れる電流を切ると閉磁路を流れていた電磁石43、45による磁束は消滅する。このとき、軸方向に作用する磁界は極度に弱まり、内筒25は自重により落下し、タッチダウンベアリング23にタッチダウンする。   When the current flowing through the electromagnets 43 and 45 is cut off, the magnetic flux generated by the electromagnets 43 and 45 flowing through the closed magnetic path disappears. At this time, the magnetic field acting in the axial direction is extremely weakened, and the inner cylinder 25 falls due to its own weight and touches down the touch-down bearing 23.

ここに、特許文献2や特許文献3に開示のある方法では、永久磁石の磁極の向きと電磁石の鉄心コアの向きとが一致しているため、電磁石の電流を切った後でも永久磁石の磁界が直接電磁石の鉄心コアに作用し続け吸引力があまり消滅しない。このため、内筒25をタッチダウンベアリング23にタッチダウンさせることはできない。   Here, in the methods disclosed in Patent Document 2 and Patent Document 3, since the direction of the magnetic pole of the permanent magnet and the direction of the iron core of the electromagnet coincide with each other, the magnetic field of the permanent magnet even after the current of the electromagnet is cut off. Will continue to act directly on the iron core of the electromagnet and the attractive force will not disappear much. For this reason, the inner cylinder 25 cannot be touched down to the touchdown bearing 23.

また、電磁石43、45が環状であり、断面が図8に示すようにコの字状であり、これに対峙する磁性体51、53及び永久磁石55も同様に環状に形成され、断面が図8に示すようにコの字状である。このため、電磁石43、45及び永久磁石55により発生する磁束は回転子コア35及び磁性体51、53及び固定子コア29を通り閉磁路が形成されており、半径方向にも復元力を有することができる。このことにより、内筒25が半径方向にずれたときにも復元力が働くので半径方向への支持が可能になる。なお、電磁石43、45の配設方法は環状に限定されるものではなく、電磁石43、45を一つの組として回転軸回りに必要組数(例えば図2に示すように4組)配設されてもよい。   Further, the electromagnets 43 and 45 are annular, and the cross section is a U-shape as shown in FIG. 8, and the magnetic bodies 51 and 53 and the permanent magnet 55 facing the same are also formed in an annular shape, and the cross section is illustrated. As shown in FIG. Therefore, the magnetic flux generated by the electromagnets 43 and 45 and the permanent magnet 55 passes through the rotor core 35, the magnetic bodies 51 and 53, and the stator core 29 to form a closed magnetic path, and has a restoring force in the radial direction. Can do. As a result, a restoring force is exerted even when the inner cylinder 25 is displaced in the radial direction, so that support in the radial direction is possible. The arrangement method of the electromagnets 43 and 45 is not limited to the ring shape, and the necessary number of the electromagnets 43 and 45 (for example, four sets as shown in FIG. 2) is arranged around the rotation axis. May be.

更に、内筒25の内部を流れる原液が磁性体の場合、原液が磁気軸受付近を通過する際に磁気軸受が作る磁場により影響を受ける恐れがある。しかしながら、本実施形態の磁気軸受を搭載した固液分離機300においては、運転中には磁束は閉磁路を流れ、一方、停止のときには永久磁石55の磁界の大部分が電磁鋼板を流れる磁束となるため外部に対し磁場の影響を与えることがない。   Furthermore, when the undiluted solution flowing inside the inner cylinder 25 is a magnetic material, the undiluted solution may be affected by the magnetic field generated by the magnetic bearing when it passes near the magnetic bearing. However, in the solid-liquid separator 300 equipped with the magnetic bearing of the present embodiment, the magnetic flux flows in the closed magnetic path during operation, while the magnetic field of the permanent magnet 55 is mostly the magnetic flux that flows through the magnetic steel sheet when stopped. Therefore, there is no influence of the magnetic field on the outside.

ここに、第2実施形態の磁気軸受について軸方向にどの程度の起磁力を発生可能かシミュレーションを行った。シミュレーションは、磁気軸受のモデリングと電磁力解析に有限要素法解析ソフトを用いた。基本となる簡易モデルの固定子側の図面を図9に、回転子側の図面を図10に示す。解析結果を図11及び図12に示す。   Here, a simulation was performed to determine how much magnetomotive force can be generated in the axial direction for the magnetic bearing of the second embodiment. The simulation used finite element method analysis software for magnetic bearing modeling and electromagnetic force analysis. FIG. 9 shows a drawing of a basic simplified model on the stator side, and FIG. 10 shows a drawing on the rotor side. The analysis results are shown in FIGS.

このことより、電磁石の電流を切ったとき、即ち電流値0(A)のときに軸方向に働く電磁力が750(N)程度と小さいため内筒25をタッチダウンベアリング23にタッチダウンさせることができる。更に、図12より半径方向にも十分な大きさの復元力を作用させることができることが分かる。   From this, when the current of the electromagnet is cut off, that is, when the current value is 0 (A), the electromagnetic force acting in the axial direction is as small as about 750 (N), so the inner cylinder 25 is touched down to the touch-down bearing 23. Can do. Furthermore, it can be seen from FIG. 12 that a sufficiently large restoring force can be applied in the radial direction.

次に、本実施形態のように永久磁石55を回転子コア35に対し水平に配設したことによる利点について説明する。   Next, the advantage by having arrange | positioned the permanent magnet 55 horizontally with respect to the rotor core 35 like this embodiment is demonstrated.

仮に、この永久磁石55が配設されなかった場合には、図13に示すように、電磁石磁束により回転子コア35内が磁気飽和すると、アキシャル(軸)方向電磁力も飽和してしまう。このため、大きな電磁力を得るには、回転子コア35を厚くしなければならず、磁気軸受が大型化し好ましくない。   If the permanent magnet 55 is not disposed, as shown in FIG. 13, when the rotor core 35 is magnetically saturated by the electromagnet magnetic flux, the axial (axial) electromagnetic force is also saturated. For this reason, in order to obtain a large electromagnetic force, the rotor core 35 must be thickened, which is not preferable because the magnetic bearing becomes large.

これに対し、永久磁石55を回転子コア35に対し水平に配設した場合であって、かつ電磁石43、45に対し、電流を流さなかったときには、永久磁石55の磁束が図14のように通過する。即ち、永久磁石55の磁束は主磁路を通る一方で永久磁石55の漏れ磁束が主磁路とは別に回転子コア35内を通っている。   On the other hand, when the permanent magnet 55 is disposed horizontally with respect to the rotor core 35 and no current is supplied to the electromagnets 43 and 45, the magnetic flux of the permanent magnet 55 is as shown in FIG. pass. That is, the magnetic flux of the permanent magnet 55 passes through the main magnetic path, while the leakage magnetic flux of the permanent magnet 55 passes through the rotor core 35 separately from the main magnetic path.

そして、次に電磁石43、45に対し、電流を流した場合には、図15に示すように電磁石磁束が発生し、この電磁石磁束は透磁率の低い永久磁石55を通らず回転子コア35内を通過するため、この回転子コア35内では、電磁石磁束が永久磁石55の漏れ磁束と相殺される形になる。このように、永久磁石55の漏れ磁束が主磁路と逆方向に通過していたため、磁気飽和しにくい。   Then, when an electric current is passed next to the electromagnets 43 and 45, an electromagnet magnetic flux is generated as shown in FIG. 15, and this electromagnet magnetic flux does not pass through the permanent magnet 55 having a low magnetic permeability and enters the rotor core 35. Therefore, in the rotor core 35, the electromagnet magnetic flux is offset with the leakage magnetic flux of the permanent magnet 55. Thus, since the leakage magnetic flux of the permanent magnet 55 has passed in the direction opposite to the main magnetic path, magnetic saturation is difficult.

そして、電磁石磁束が大きくなるに連れ、永久磁石55の漏れ磁束分は次第に無くなり、この漏れ磁束が主磁路へ流れるようになる。
このことにより、回転子コア35は薄くでき、磁気軸受の小型、軽量化につながる。また、高ギャップ磁束密度となるため、高電磁力を発生できる。
As the electromagnet magnetic flux increases, the leakage magnetic flux of the permanent magnet 55 gradually disappears, and this leakage magnetic flux flows into the main magnetic path.
As a result, the rotor core 35 can be made thin, leading to a reduction in size and weight of the magnetic bearing. Moreover, since it becomes a high gap magnetic flux density, a high electromagnetic force can be generated.

次に、上記永久磁石55を配設したことに伴う効果を立証するため電磁界解析を行った。図16に示すように、磁性体51、53の表面(図中(イ)と示す)と、回転子コア35内(図中(ロ)と示す)の2箇所の磁束密度とアキシャル方向電磁力を解析により求めた。   Next, an electromagnetic field analysis was performed in order to verify the effect associated with the arrangement of the permanent magnet 55. As shown in FIG. 16, the magnetic flux density and the axial electromagnetic force at two locations on the surface of the magnetic bodies 51 and 53 (shown as (A) in the figure) and inside the rotor core 35 (shown as (B) in the figure). Was obtained by analysis.

図17には、磁性体51、53の表面の磁束密度と電磁石電流との関係を、永久磁石(図中、PMと略す)を配設した場合と配設しない場合について示す。即ち、永久磁石55を配設しなかった場合には、電流3A付近で磁気飽和の兆候が現れている。一方、永久磁石55を配設した場合には、電流9Aでも磁気飽和の兆候が見られない。   FIG. 17 shows the relationship between the magnetic flux density on the surfaces of the magnetic bodies 51 and 53 and the electromagnet current when a permanent magnet (abbreviated as PM in the figure) is provided and when it is not provided. That is, when the permanent magnet 55 is not provided, a sign of magnetic saturation appears near the current 3A. On the other hand, in the case where the permanent magnet 55 is provided, no sign of magnetic saturation is observed even with the current 9A.

また、図18には、回転子コア内の磁束密度と電磁石電流との関係を、永久磁石を配設した場合と配設しない場合について示す。即ち、図17の場合と同様、永久磁石55を配設しなかった場合には、電流3A付近で磁気飽和の兆候が現れている。一方、永久磁石55を配設した場合には、電流9Aでも磁気飽和の兆候が見られない。但し、電流0Aのときに磁束密度が負になっているのは、永久磁石55の漏れ磁束の存在によるためである。   FIG. 18 shows the relationship between the magnetic flux density in the rotor core and the electromagnet current when a permanent magnet is provided and when it is not provided. That is, as in the case of FIG. 17, in the case where the permanent magnet 55 is not provided, a sign of magnetic saturation appears near the current 3A. On the other hand, in the case where the permanent magnet 55 is provided, no sign of magnetic saturation is observed even with the current 9A. However, the magnetic flux density is negative when the current is 0 A because the leakage magnetic flux of the permanent magnet 55 exists.

更に、図19には、アキシャル方向電磁力と電磁石電流との関係を、永久磁石を配設した場合と配設しない場合について示す。即ち、図17で、永久磁石55を配設しなかった場合に電流9Aのときに0.58T程度であるのに対し、永久磁石55を配設した場合には0.83Tに達し、その結果、アキシャル方向電磁力は図19に示すように約4200Nから7200Nに増加することが分かる。   Further, FIG. 19 shows the relationship between the axial electromagnetic force and the electromagnet current when the permanent magnet is disposed and when it is not disposed. That is, in FIG. 17, when the permanent magnet 55 is not provided, it is about 0.58T when the current is 9A, whereas when the permanent magnet 55 is provided, it reaches 0.83T. It can be seen that the axial electromagnetic force increases from about 4200 N to 7200 N as shown in FIG.

次に、本発明の第3実施形態について説明する。
本発明の第3実施形態である固液分離機400の磁気軸受周辺の概念構成図を図20に示す。なお、図1、図8と同一要素のものについては同一符号を付して説明は省略する。図20において、固定子コア29の下面には回転軸を中心として環状に3つの電磁石鉄心29a、29b、29cが突設されている。
Next, a third embodiment of the present invention will be described.
The conceptual block diagram of the magnetic bearing periphery of the solid-liquid separator 400 which is 3rd Embodiment of this invention is shown in FIG. The same elements as those in FIG. 1 and FIG. In FIG. 20, three electromagnet cores 29a, 29b, and 29c project from the lower surface of the stator core 29 in an annular shape around the rotation axis.

そして、この3つの電磁石鉄心29a、29b、29cの間に二つの環状スロット61、63が形成されている。そして、この環状スロット61、63と電磁石鉄心29aの内側及び電磁石鉄心29cの外側とにそれぞれ巻線を配設することで電磁石を構成する。電流の方向は図20に示す通りである。   Two annular slots 61, 63 are formed between the three electromagnet cores 29a, 29b, 29c. And an electromagnet is comprised by arrange | positioning coil | winding to these annular slots 61 and 63, the inner side of the electromagnet core 29a, and the outer side of the electromagnet core 29c, respectively. The direction of current is as shown in FIG.

一方、回転子コア35の上面には、この電磁石鉄心29a、29b、29cに対峙するように環状に磁性体71、73、75が突設されている。そして、この磁性体71、73、75の間に永久磁石85、87が固着されている。永久磁石85は水平方向に設置され内側がS極、外側がN極に構成されている。永久磁石87も同様に水平方向に設置されるが、永久磁石85とは異なり内側がN極、外側がS極に構成されている。   On the other hand, on the upper surface of the rotor core 35, magnetic bodies 71, 73, 75 project in a ring shape so as to face the electromagnet cores 29 a, 29 b, 29 c. And permanent magnets 85 and 87 are fixed between the magnetic bodies 71, 73 and 75. The permanent magnet 85 is installed in the horizontal direction and has an S pole on the inner side and an N pole on the outer side. The permanent magnet 87 is similarly installed in the horizontal direction, but unlike the permanent magnet 85, the inner side is configured as an N pole and the outer side is configured as an S pole.

かかる構成において、永久磁石85、87のN極から発した磁束は磁性体73を通り電磁石鉄心29bを通った後分岐し、それぞれ電磁石鉄心29aと電磁石鉄心29cとを通る。その後、電磁石鉄心29aを通った磁束は磁性体71を介して永久磁石85のS極に戻る。電磁石鉄心29cを通った磁束は磁性体75を介して永久磁石87のS極に戻る。   In such a configuration, the magnetic flux generated from the N poles of the permanent magnets 85 and 87 passes through the magnetic body 73 and then passes through the electromagnet core 29b, and then branches through the electromagnet core 29a and the electromagnet core 29c. Thereafter, the magnetic flux passing through the electromagnet core 29 a returns to the S pole of the permanent magnet 85 through the magnetic body 71. The magnetic flux that has passed through the electromagnet core 29 c returns to the S pole of the permanent magnet 87 via the magnetic body 75.

ここに、電磁石鉄心29a、29b、29cの面積及び磁性体71、73、75の面積が増加することで軸方向の電磁力はこの面積比分増加する。また、電磁石鉄心29a、29b、29cの周囲及び磁性体71、73、75の周囲には第2実施形態に比べより多くの磁束を生じており、半径方向にも一層強い復元力を有することができる。このため、内筒25が半径方向にずれたときにもこの復元力により半径方向への支持が一層安定する。   Here, as the area of the electromagnet cores 29a, 29b, 29c and the area of the magnetic bodies 71, 73, 75 increase, the electromagnetic force in the axial direction increases by this area ratio. Further, more magnetic flux is generated around the electromagnet cores 29a, 29b, and 29c and around the magnetic bodies 71, 73, and 75 than in the second embodiment, and it has a stronger restoring force in the radial direction. it can. For this reason, even when the inner cylinder 25 is displaced in the radial direction, the support in the radial direction is further stabilized by this restoring force.

また、電磁石に流れる電流を切ると閉磁路を流れていた電磁石による磁束は消滅する。このとき、軸方向に作用する磁界は極度に弱まり、内筒25は自重により落下し、タッチダウンベアリング23にタッチダウンする。   Further, when the current flowing through the electromagnet is cut off, the magnetic flux generated by the electromagnet flowing through the closed magnetic path disappears. At this time, the magnetic field acting in the axial direction is extremely weakened, and the inner cylinder 25 falls due to its own weight and touches down the touch-down bearing 23.

更に、本実施形態の磁気軸受を搭載した固液分離機400においては、第2実施形態と同様に磁束は閉磁路を流れるため外部に対し磁場の影響を与えることがない。このため、内筒25の内部を流れる原液が磁性体の場合であっても磁場により影響を与えることはない。   Further, in the solid-liquid separator 400 equipped with the magnetic bearing of the present embodiment, the magnetic flux flows through the closed magnetic path as in the second embodiment, so that the magnetic field does not affect the outside. For this reason, even if the undiluted solution flowing through the inner cylinder 25 is a magnetic material, it is not affected by the magnetic field.

なお、本実施形態では環状スロットの数を2つとしたが、この数に限定するものではない。   In the present embodiment, the number of annular slots is two, but the number is not limited to this.

なお、本発明の第2実施形態である固液分離機300の磁気軸受については試作を行い、以下の通り磁気支持特性の測定と評価を行った。
まず、電磁石43、45を一つの組として回転軸回りに4組配設した。そして、磁気軸受の制御に必要な巻線の時定数を得るため、巻線抵抗とインダクタンスを測定した。表1、2に巻線抵抗、インダクタンスの測定結果をそれぞれ示す。
The magnetic bearing of the solid-liquid separator 300 according to the second embodiment of the present invention was prototyped, and the magnetic support characteristics were measured and evaluated as follows.
First, four sets of electromagnets 43 and 45 were arranged around the rotation axis as one set. The winding resistance and inductance were measured in order to obtain the winding time constant necessary for controlling the magnetic bearing. Tables 1 and 2 show the measurement results of winding resistance and inductance, respectively.

Figure 0005201582
Figure 0005201582

Figure 0005201582
Figure 0005201582

なお、インダクタンスについては、有限要素法による電磁界解析結果も併せて示した。抵抗、インダクタンスともに4つの電磁石でほぼ平衡が取れている。また、インダクタンスの実測値は解析値に比べ9%程度小さいが、これは漏れ磁束の影響によるものと思われる。   For inductance, the results of electromagnetic field analysis by the finite element method are also shown. Both the resistance and inductance are almost balanced by four electromagnets. In addition, the actual measured value of inductance is about 9% smaller than the analytical value, which seems to be due to the influence of leakage magnetic flux.

ギャップセンサ44A、44B、44C、44Dを各電磁石の組に対しそれぞれ1個ずつ合計4個取り付け、磁気浮上試験を行った。実験は無荷重で行い、その際の回転浮上部の重量は1,500Nであった。静止浮上時はギャップ2.5mm、電磁石電流3Aで安定に磁気支持できることを確認した。   A total of four gap sensors 44A, 44B, 44C, and 44D were attached to each electromagnet group, and a magnetic levitation test was performed. The experiment was performed with no load, and the weight of the rotating floating part at that time was 1,500N. It was confirmed that the magnetic support could be stably performed with a gap of 2.5 mm and an electromagnet current of 3 A during static levitation.

図21はギャップ長をパラメータにして、電磁石電流とアキシャル方向の電磁力の関係を有限要素法により解析した結果である。また、図22は電磁力1,500N(一定)時のギャップ長と電磁石電流の関係である。ギャップ2.5mmのとき必要な電磁石電流は3Aであり、実測値は解析値によく一致した。   FIG. 21 shows the result of analyzing the relationship between the electromagnet current and the electromagnetic force in the axial direction by the finite element method using the gap length as a parameter. FIG. 22 shows the relationship between the gap length and the electromagnetic current when the electromagnetic force is 1,500 N (constant). When the gap is 2.5 mm, the required electromagnet current is 3 A, and the measured value is in good agreement with the analysis value.

次にモータを使って外部駆動によりベルト伝達で磁気軸受回転部を回転させ、回転浮上試験を行った。回転部は回転速度0−300r/minの範囲でタッチダウンせず安定に支持できることを確認した。   Next, the rotating part of the magnetic bearing was rotated by belt transmission by external drive using a motor, and a rotational levitation test was performed. It was confirmed that the rotating part could be supported stably without touching down in the range of the rotational speed of 0-300 r / min.

本発明の第1実施形態である固液分離機の磁気軸受周辺の概念構成図The conceptual block diagram of the magnetic bearing periphery of the solid-liquid separator which is 1st Embodiment of this invention 固定子コアの下面の様子State of the lower surface of the stator core 回転子コアの上面の様子Top view of the rotor core 簡易モデルの固定子側の断面図Cross section of the stator side of the simplified model 簡易モデルの回転子側の断面図Cross section of the simplified model on the rotor side シミュレーションに用いた材料及び仕様Materials and specifications used for simulation シミュレーションの解析結果Simulation analysis results 本発明の第2実施形態である固液分離機の磁気軸受周辺の概念構成図The conceptual block diagram of the magnetic bearing periphery of the solid-liquid separator which is 2nd Embodiment of this invention 簡易モデルの固定子側の断面図Cross section of the stator side of the simplified model 簡易モデルの回転子側の断面図Cross section of the simplified model on the rotor side シミュレーションの解析結果Simulation analysis results シミュレーションの解析結果Simulation analysis results 永久磁石を回転子コアに対し配設しなかった場合When a permanent magnet is not installed on the rotor core 永久磁石を回転子コアに対し配設した場合(その1)When permanent magnets are installed on the rotor core (part 1) 永久磁石を回転子コアに対し配設した場合(その2)When permanent magnets are installed on the rotor core (part 2) 磁束密度とアキシャル方向電磁力の解析を行った地点Point where magnetic flux density and axial electromagnetic force were analyzed 磁性体の表面の磁束密度と電磁石電流との関係(永久磁石を配設した場合と配設しない場合)Relationship between magnetic flux density on magnetic surface and electromagnet current (with or without permanent magnet) 回転子コア内の磁束密度と電磁石電流との関係(永久磁石を配設した場合と配設しない場合)Relationship between magnetic flux density in rotor core and electromagnet current (with or without permanent magnet) アキシャル方向電磁力と電磁石電流との関係(永久磁石を配設した場合と配設しない場合)Relationship between axial electromagnetic force and electromagnet current (with or without permanent magnet) 本発明の第3実施形態である固液分離機の磁気軸受周辺の概念構成図The conceptual block diagram of the magnetic bearing periphery of the solid-liquid separator which is 3rd Embodiment of this invention 電磁石電流とアキシャル方向の電磁力の関係を有限要素法により解析した結果Results of analyzing the relation between electromagnetic current and electromagnetic force in the axial direction by the finite element method 電磁力一定時のギャップ長と電磁石電流の関係Relationship between gap length and electromagnetic current when electromagnetic force is constant 固液分離機(横型)の概念図Conceptual diagram of solid-liquid separator (horizontal type) 固液分離機(縦型)の概念図Conceptual diagram of solid-liquid separator (vertical type) 縦型固液分離機の構造Structure of vertical solid-liquid separator

符号の説明Explanation of symbols

1 外筒
5 、25 内筒
6 分流リブ板
7 スクリューコンベアー
9 通路
11 貫通穴
13 フィード口
17 排出口
21 外筒
23 タッチダウンベアリング
29 固定子コア
33、43 電磁石
34、44 ギャップセンサ
35 回転子コア
37、55、85、87 永久磁石
49、61 環状スロット
51、71、73、75 磁性体
200 、300、400固液分離機
DESCRIPTION OF SYMBOLS 1 Outer cylinder 5, 25 Inner cylinder 6 Dividing rib board 7 Screw conveyor 9 Passage 11 Through hole 13 Feed port 17 Outlet 21 Outer cylinder 23 Touchdown bearing 29 Stator core 33, 43 Electromagnet 34, 44 Gap sensor 35 Rotor core 37, 55, 85, 87 Permanent magnet 49, 61 Annular slot 51, 71, 73, 75 Magnetic body 200, 300, 400 Solid-liquid separator

Claims (2)

回転軸を中心に回転する回転体に形成された回転コアと、
該回転コアに配設され軸方向に磁極を有する永久磁石と、
該永久磁石と対峙して配設され軸方向に磁極を有し前記回転軸回りに均等配設された複数の電磁石と、
該電磁石が取り付けられた固定子コアと、
前記回転体の軸方向位置を検出する位置センサと、
該位置センサで検出した位置信号に基づき前記回転体の軸方向の位置を調整する軸方向位置調整手段とを有し、
前記永久磁石が軸方向に一つ配設された磁気軸受装置を搭載した縦型の固液分離機であって、
前記回転体が内筒であり、該内筒の内側に該内筒とは異なる速度にて駆動されるスクリューを備え、
該スクリューを貫通する貫通穴を通じて流入した固体及び液体の混合原液が前記内筒と前記スクリューの間に回転しつつ通されることで固体と液体とが分離されることを特徴とする固液分離機。
A rotating core formed on a rotating body that rotates about a rotation axis;
A permanent magnet disposed on the rotating core and having a magnetic pole in the axial direction;
A plurality of electromagnets arranged opposite to the permanent magnets and having magnetic poles in the axial direction and evenly arranged around the rotation axis;
A stator core to which the electromagnet is attached;
A position sensor for detecting an axial position of the rotating body;
Axial position adjusting means for adjusting the axial position of the rotating body based on the position signal detected by the position sensor ;
A vertical solid-liquid separator equipped with a magnetic bearing device in which one permanent magnet is disposed in the axial direction,
The rotating body is an inner cylinder, and includes a screw driven at a speed different from that of the inner cylinder inside the inner cylinder,
Solid-liquid separation characterized in that solid and liquid are separated by passing a mixed stock solution of solid and liquid flowing in through a through-hole passing through the screw while rotating between the inner cylinder and the screw. Machine.
前記電磁石及び前記永久磁石により発生した磁束が前記固定子コアと内筒側ギャップと前記内筒と前記回転コアを通る第1の閉磁路と、A first closed magnetic path through which the magnetic flux generated by the electromagnet and the permanent magnet passes through the stator core, the inner cylinder side gap, the inner cylinder, and the rotating core;
前記電磁石及び前記永久磁石により発生した磁束が前記固定子コアと該固定子コアに連設する外筒と外筒側ギャップと前記回転コアを通る第2の閉磁路とが形成されることを特徴とする請求項1記載の固液分離機。The magnetic flux generated by the electromagnet and the permanent magnet is formed with the stator core, an outer cylinder connected to the stator core, an outer cylinder side gap, and a second closed magnetic path passing through the rotating core. The solid-liquid separator according to claim 1.
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