JPH01293603A - Magnetization device - Google Patents
Magnetization deviceInfo
- Publication number
- JPH01293603A JPH01293603A JP12529688A JP12529688A JPH01293603A JP H01293603 A JPH01293603 A JP H01293603A JP 12529688 A JP12529688 A JP 12529688A JP 12529688 A JP12529688 A JP 12529688A JP H01293603 A JPH01293603 A JP H01293603A
- Authority
- JP
- Japan
- Prior art keywords
- magnetization
- magnetized
- yoke
- magnetizing
- rotor
- 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.)
- Pending
Links
- 230000005415 magnetization Effects 0.000 title abstract description 26
- 239000000463 material Substances 0.000 claims abstract description 27
- 230000005611 electricity Effects 0.000 claims abstract 2
- 238000004804 winding Methods 0.000 claims description 23
- 238000000034 method Methods 0.000 abstract description 2
- 230000005291 magnetic effect Effects 0.000 description 6
- 230000000694 effects Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 230000004907 flux Effects 0.000 description 4
- 239000011248 coating agent Substances 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- 230000005292 diamagnetic effect Effects 0.000 description 2
- 238000003780 insertion Methods 0.000 description 2
- 230000037431 insertion Effects 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- 239000000779 smoke Substances 0.000 description 2
- 229910000859 α-Fe Inorganic materials 0.000 description 2
- UZFMKSXYXFSTAP-UHFFFAOYSA-N barium yttrium Chemical compound [Y].[Ba] UZFMKSXYXFSTAP-UHFFFAOYSA-N 0.000 description 1
- 239000002826 coolant Substances 0.000 description 1
- 239000003822 epoxy resin Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 229920000647 polyepoxide Polymers 0.000 description 1
- 238000010248 power generation Methods 0.000 description 1
Landscapes
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
[発明の目的]
(産業上の利用分野)
本発明は着磁ヨークに巻装された巻線にa電することに
より被着磁体に着磁する着磁装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a magnetizing device that magnetizes a magnetized body by applying a current to a winding wound around a magnetizing yoke.
(従来の技術)
従来、この種の着磁装置例えば回転電機たるアキシャル
ギャップ形ブラシレスモークのロータにおける周波数発
電機用磁石部の着磁装置は、第4図に示すように、着磁
ヨークlの複数個の極2に、隣接するものが逆方向とな
るようにして巻線3を巻装し、その巻線3に直流の着磁
電源により通電することにより被着磁体たるロータの周
波数発電機用磁石部に着磁する構成となっている。これ
によって、周波数発電機用磁石部は、第5図に示すよう
に、周方向(ロータの回転角度θ方向)に沿って交互に
N極とS極が着磁された着磁パターンを得るものである
。(Prior Art) Conventionally, this type of magnetizing device, for example, a magnetizing device for a magnet part for a frequency generator in a rotor of an axial gap type brushless smoke of a rotating electric machine, as shown in FIG. Winding wires 3 are wound around a plurality of poles 2 so that adjacent ones are in opposite directions, and the windings 3 are energized by a DC magnetizing power source to create a frequency generator for the rotor, which is a magnetized object. The structure is such that the magnet section is magnetized. As a result, the frequency generator magnet section obtains a magnetization pattern in which N poles and S poles are alternately magnetized along the circumferential direction (rotor rotation angle θ direction). It is.
(発明が解決しようとする課題)
このように周方向に沿って第5図のような波形状のる磁
パターンを形成された周波数発電機用磁石部は、ロータ
とともに回転して鎖交磁束が変化することにより回転速
度に応じた周波数信号を発生させるものであるので、例
えば、回転速度を精度よく検出できるものを得るには、
1回転あたりの周波数を多くすべく周波数発電機用磁石
部に小さい間隔で波形状をなす着磁パターンを形成すれ
ばよい。ところが、このような小さい間隔で波形状をな
す着磁パターンを形成する場合、従来の構成では、着磁
ヨーク1の着磁面の極2を多数に分割して設ける必要が
あるので、極数の増加にともなって着磁ヨーク1の構造
が複雑となるばかりか、幅狭な極2に対して交互に逆向
きに巻線3を巻装することになるので、巻線3の巻装作
業が複雑になって巻線3の絶縁被覆の破損にともなう着
磁ヨーク1と巻vA3との間での短絡事故の発生率が大
きくなってしまうという問題があった。また、この場合
、巻線3を巻装するため、相隣る極2゜2の間に所定の
間隔を設けねばならず、これによって形成可能な極の数
が制限されてしまうという問題があった。(Problem to be Solved by the Invention) In this way, the frequency generator magnet part, which is formed with a wave-shaped magnetic pattern as shown in FIG. It generates a frequency signal according to the rotational speed by changing the frequency, so for example, in order to obtain one that can accurately detect the rotational speed,
In order to increase the frequency per rotation, a wave-shaped magnetization pattern may be formed at small intervals on the frequency generator magnet. However, when forming a wave-shaped magnetization pattern with such small intervals, in the conventional configuration, it is necessary to divide the pole 2 of the magnetization surface of the magnetization yoke 1 into a large number of parts. Not only does the structure of the magnetizing yoke 1 become complicated as There is a problem in that the process becomes complicated and the probability of short-circuit accidents between the magnetizing yoke 1 and the winding vA3 due to damage to the insulation coating of the winding 3 increases. In addition, in this case, in order to wind the winding 3, it is necessary to provide a predetermined interval between adjacent poles 2.2, which causes the problem that the number of poles that can be formed is limited. Ta.
本発明は、上記事情に鑑みてなされたもので、その目的
は、被着磁体に小さい間隔で交互に強着磁部分と弱また
は無着磁部分とをもった着磁パターンを形成し得、この
場合でも青磁ヨークの構造は簡単で製作が容易であり、
巻線の短絡事故の発生率を小になし得る着磁装置を提供
するにある。The present invention has been made in view of the above-mentioned circumstances, and its object is to form a magnetized pattern on a magnetized body having strongly magnetized portions and weakly or non-magnetized portions alternately at small intervals; Even in this case, the structure of the celadon yoke is simple and easy to manufacture.
An object of the present invention is to provide a magnetizing device that can reduce the incidence of winding short-circuit accidents.
[発明の構成]
(課題を解決するための手段)
本発明の着磁装置は、着磁ヨークに巻装された巻線に通
電することにより被青磁体を同一極に着磁するようにし
たものにおいて、前記着磁ヨークの着磁面に等配に複数
の超伝導物質を設け、その超伝導物質を超伝導状態にし
て前記巻線に通電する構成に特徴を有する。[Structure of the Invention] (Means for Solving the Problems) The magnetizing device of the present invention magnetizes the celadon magnetized materials to the same polarity by energizing the windings wound around the magnetizing yoke. The present invention is characterized in that a plurality of superconducting materials are provided equidistantly on the magnetizing surface of the magnetizing yoke, and the superconducting materials are brought into a superconducting state to energize the winding.
(作用)
本発明の着磁装置によれば、超伝導物質は超伝導状態で
はマイスナ効果により反磁性を示すようになることから
、被青磁体の超伝導物質に対応する部分には磁束が作用
せずに青磁は行なわれず若しくはほとんど行なわれず、
従って、着磁ヨークに等配に設ける複数の超伝導物質の
配設の仕方により被青磁体に小さい間隔で強青磁部分と
弱または無着磁部分とをもった着磁パターンを施こすこ
とができる。(Function) According to the magnetization device of the present invention, since the superconducting material exhibits diamagnetic properties due to the Meissner effect in the superconducting state, magnetic flux acts on the portion of the celadon magnetized material corresponding to the superconducting material. Celadon is not done or is rarely done without
Therefore, by arranging a plurality of superconducting materials evenly spaced on the magnetizing yoke, it is possible to create a magnetized pattern on the celadon-magnetized material, which has strongly celadon-magnetic parts and weakly magnetized or non-magnetized parts at small intervals. can.
(実施例)
以下、本発明の一実施例につき第1図乃至第3図を参照
しながら説明する。(Example) Hereinafter, an example of the present invention will be described with reference to FIGS. 1 to 3.
先ず、第1図及び第2図に基いて全体の構成について述
べる。11は容器であり、内部には着磁台12が配設さ
れている。13は円柱状をなす着磁ヨークであり、その
着磁面13aには中心部に軸挿入用穴14が形成されて
いるとともに中心部から放射状に所定の角度をもって多
数の溝部15が等配に形成されている。これら多数の溝
部15には例えばイツトリウム−バリウム系の材料より
なる超伝導物質16が埋設され、夫々の上面は着磁ヨー
ク13の着磁面13aと面一になるように設定されてい
る。17は巻線であり、これは、着磁ヨーク13の外周
部に巻装されたもので、巻装された部分にはエポキシ樹
脂等によるモールド層18が形成されている。19は着
磁ヨーク13の外周部を覆うようにして配設された円筒
状のヨークであり、これは、後述する被青磁体がセット
されると着磁ヨーク13とともに閉磁路を形成するのも
である。尚、ヨーク19の側壁には挿通孔19aが設け
られて巻線17の両端子を導出できるようになっている
。20は被着磁体たる例えばアキシャルギャップ形ブラ
シレスモークのロータであり、これは、シャフト21a
を有する円盤状のロータヨーク21の上面部にフェライ
ト製の主磁石部22を装着し、下面部にフ、エライト製
の周波数発電用磁石部23を装着して構成されている。First, the overall configuration will be described based on FIGS. 1 and 2. 11 is a container, and a magnetizing table 12 is disposed inside thereof. Reference numeral 13 denotes a magnetizing yoke having a cylindrical shape, and its magnetizing surface 13a has a shaft insertion hole 14 formed in the center thereof, and a large number of grooves 15 are equally distributed at a predetermined angle radially from the center. It is formed. A superconducting material 16 made of, for example, yttrium-barium material is embedded in these many grooves 15, and the upper surface of each groove is set to be flush with the magnetized surface 13a of the magnetized yoke 13. A winding 17 is wound around the outer periphery of the magnetizing yoke 13, and a mold layer 18 made of epoxy resin or the like is formed on the wound portion. Reference numeral 19 denotes a cylindrical yoke disposed to cover the outer periphery of the magnetizing yoke 13. This yoke forms a closed magnetic path together with the magnetizing yoke 13 when a celadon-magnetized material, which will be described later, is set. It is. Incidentally, an insertion hole 19a is provided in the side wall of the yoke 19 so that both terminals of the winding 17 can be led out. Reference numeral 20 denotes a magnetized body, for example, an axial gap type brushless smoke rotor, which is connected to a shaft 21a.
A main magnet part 22 made of ferrite is attached to the upper surface of a disc-shaped rotor yoke 21 having a shape, and a frequency power generation magnet part 23 made of ferrite is attached to the lower surface thereof.
そして、このロータ20はヨ〜り19の上部開口部に装
着された環状のヨーク24に嵌合された状態で着磁ヨー
ク13の着磁面13aに載置されている。この場合、ロ
ータ20の周波数発電機用磁石部23が着磁ヨーク13
の着磁面13aに接していることは勿論である。The rotor 20 is placed on the magnetized surface 13a of the magnetized yoke 13 in a state where it is fitted into an annular yoke 24 attached to the upper opening of the yoke 19. In this case, the frequency generator magnet section 23 of the rotor 20 is connected to the magnetizing yoke 13.
Of course, it is in contact with the magnetized surface 13a of.
次に、本実施例の作用につき第3図をも参照して説明す
る。Next, the operation of this embodiment will be explained with reference to FIG. 3 as well.
容器11内に液体ヘリウム等の冷却剤25を注入すると
、着磁ヨーク13の各超伝導物質16は超伝導状態にな
る。このような状態で巻線17に直流の着磁電源から高
電圧(例えば500乃至800ボルト)、高電流(例え
ば1000乃至2000アンペア)を短時間(例えば数
ミリ秒)だけ通電すると、着磁ヨーク13に発生する磁
束によりロータ20の周波数発電機用磁石部23に例え
ばN極が着磁される。この場合、超伝導物質16が超伝
導状態にあってはマイスナ効果により反磁性を示してい
るので、着磁ヨーク13から発生する磁束は着磁面13
aの溝部15を除いた部分のみを通るようになり、ロー
タ20の周波数発電機用磁石部23の着磁パターンは第
3図に示すように超伝導物質16部分が弱または無着磁
部分となる波形状になる。尚、第3図において、θはロ
ータ20の回転角度を示す。When a coolant 25 such as liquid helium is injected into the container 11, each superconducting material 16 of the magnetizing yoke 13 becomes superconductive. In this state, when a high voltage (e.g. 500 to 800 volts) and high current (e.g. 1000 to 2000 amperes) are applied to the winding 17 from a DC magnetizing power source for a short period of time (e.g. several milliseconds), the magnetizing yoke The frequency generator magnet section 23 of the rotor 20 is magnetized to, for example, an N pole by the magnetic flux generated in the magnet section 13 . In this case, since the superconducting material 16 exhibits diamagnetic properties due to the Meissner effect when it is in a superconducting state, the magnetic flux generated from the magnetizing yoke 13 is transferred to the magnetizing surface 13.
The magnetization pattern of the frequency generator magnet part 23 of the rotor 20 is such that the superconducting material 16 part is weakly magnetized or non-magnetized part as shown in FIG. It becomes a wave shape. In addition, in FIG. 3, θ indicates the rotation angle of the rotor 20.
ところで、この周波数発電機用磁石部23はその周方向
に沿りて磁束が変化していることを利用して回転数に対
応した周波数信号を取り出すようにしたものであって、
従来はN極及びS極を交互に形成することによって第5
図に示すような着磁パターンを作り出しているが、本実
施例では同一の極性で強着磁部分と弱または無青磁部分
とを交互に形成することによって第3図に示すような着
磁パターンを作り出しているものであり、これによって
も周波数発電機用磁石としての機能を果すものである。By the way, this frequency generator magnet section 23 is designed to take out a frequency signal corresponding to the rotation speed by utilizing the fact that the magnetic flux changes along its circumferential direction.
Conventionally, the fifth
The magnetized pattern shown in the figure is created, but in this example, the magnetized pattern shown in Figure 3 is created by alternately forming strongly magnetized parts and weakly or non-cyanomagnetized parts with the same polarity. , which also functions as a frequency generator magnet.
このような本実施例によれば、次のような効果を得るこ
とができる。即ち、着磁ヨーク13の着磁面13aに放
射状に等配に設けた多数の溝部15に超伝導物質16を
埋設し、これらの超伝導物質16を超伝導状態にして巻
線17に通電することによりロータ20の周波数発電機
用磁石部23に着磁するようにしたので、ロータ20の
周波数発電機用磁石部23に対する着磁パターンを周方
向に沿って小さい間隔で強着磁部分と弱または無着磁部
分とを交互に配した波形状に容易にすることができ、従
って、アキシャルギャップ形ブラシレスモータのロータ
20の回転速度を精度よく検出することができるように
なる。そして、この場合でも、着磁ヨーク1に多数の極
2を設けて巻線3を巻装する従来の構成と異なり、着磁
ヨーク13は、着磁面13aに超伝導物質16を配し、
巻線17を外周に巻装するという簡単な構成で良く、巻
m17の巻装時に絶縁被覆が破損することは少なくなっ
て、短絡事故の発生率を小にすることができるものであ
る。According to this embodiment, the following effects can be obtained. That is, superconducting materials 16 are embedded in a large number of grooves 15 provided radially and equidistantly on the magnetizing surface 13a of the magnetizing yoke 13, and these superconducting materials 16 are brought into a superconducting state to energize the winding 17. As a result, the frequency generator magnet portion 23 of the rotor 20 is magnetized, so that the magnetization pattern for the frequency generator magnet portion 23 of the rotor 20 is divided into strongly magnetized portions and weakly magnetized portions at small intervals along the circumferential direction. Alternatively, it is possible to easily form a wave shape in which non-magnetized portions are alternately arranged, and therefore, the rotational speed of the rotor 20 of the axial gap type brushless motor can be detected with high accuracy. Also in this case, unlike the conventional configuration in which a large number of poles 2 are provided on the magnetizing yoke 1 and the winding 3 is wound thereon, the magnetizing yoke 13 has a superconducting material 16 disposed on the magnetizing surface 13a,
A simple configuration in which the winding 17 is wound around the outer periphery is sufficient, and the insulation coating is less likely to be damaged when winding the winding m17, thereby reducing the incidence of short circuit accidents.
尚、上記実施例では青磁ヨーク13の着磁面13aに中
心部から放射状の溝部15を設けてこれらに超伝導物質
16を埋設するようにしたが、これらの位置、長さ及び
個数は適宜設定し得ることは勿論である。In the above embodiment, grooves 15 radiating from the center are provided in the magnetized surface 13a of the celadon yoke 13, and the superconducting material 16 is buried in these grooves, but the positions, lengths, and numbers of these grooves may be set as appropriate. Of course it is possible.
また、上記実施例ではアキシャルギャップ形ブラシレス
モータのロータ20の周波数発電機用磁石部23に着磁
する場合について述べたが、これに限らず、ラジアルギ
ャップ形ブラシレスモータのロータの周波数発電機用磁
石部の着磁にも適用できるものであり、さらに、これに
限らず、着磁を必要とする回転電機全般に適用し得るも
のである。Further, in the above embodiment, a case has been described in which the frequency generator magnet section 23 of the rotor 20 of an axial gap type brushless motor is magnetized, but the present invention is not limited to this. Furthermore, the present invention is not limited to this, and can be applied to all rotating electric machines that require magnetization.
その他、本発明は上記し且つ図面に示す実施例のみに限
定されるものではなく、要旨を逸脱しない範囲内で適宜
変形して実施し得ることは勿論である。In addition, it goes without saying that the present invention is not limited to the embodiments described above and shown in the drawings, and can be implemented with appropriate modifications within the scope of the invention.
[発明の効果]
本発明の着磁装置は以上説明したように、巻線を有する
着磁ヨークの着磁面に等配に複数の超伝導物質を設け、
この超伝導物質を超伝導状態にして、前記巻線に通電す
ることにより被着磁体に着磁するようにしたので、小さ
い間隔で弱または無着磁の部分を多数有する着磁パター
ンを容易に形成することができ、この場合でも、青磁ヨ
ークの構成が複雑化することがなく巻線の短絡事故の発
生率を小にすることができるという優れた効果を奏する
ものである。[Effects of the Invention] As explained above, the magnetization device of the present invention includes a plurality of superconducting materials arranged equidistantly on the magnetization surface of a magnetization yoke having a winding,
By making this superconducting material into a superconducting state and energizing the winding, the object to be magnetized is magnetized, making it easy to create a magnetized pattern that has many weakly or non-magnetized parts at small intervals. Even in this case, the structure of the celadon yoke does not become complicated, and the occurrence rate of winding short-circuit accidents can be reduced, which is an excellent effect.
第1図乃至第3図は本発明の一実施例を示すもので、第
1図は着磁ヨークの斜視図、第2図は全体の縦断面図、
第3図は着磁パターンを示す図であり、第4図及び第5
図は従来例を示す第1図相当図び第3図相当図である。
図面中、13は着磁ヨーク、13aは着磁面、16は超
伝導物質、17は巻線、20はロータ、23は周波数発
電機用磁石部(被む礁体)を示す。1 to 3 show an embodiment of the present invention, in which FIG. 1 is a perspective view of a magnetizing yoke, FIG. 2 is a longitudinal cross-sectional view of the entire structure, and FIG.
Figure 3 is a diagram showing the magnetization pattern, and Figures 4 and 5 are diagrams showing the magnetization pattern.
The figures are a diagram corresponding to FIG. 1 and a diagram corresponding to FIG. 3 showing a conventional example. In the drawing, 13 is a magnetizing yoke, 13a is a magnetizing surface, 16 is a superconducting material, 17 is a winding, 20 is a rotor, and 23 is a frequency generator magnet (covering reef body).
Claims (1)
被着磁体を同一極に着磁するようにしたものにおいて、
前記着磁ヨークの着磁面に等配に複数の超伝導物質を設
け、その超伝導物質を超伝導状態にして前記巻線に通電
することを特徴とする着磁装置。1. In a device in which the magnetized objects are magnetized to the same polarity by energizing the windings wound around the magnetizing yoke,
A magnetizing device characterized in that a plurality of superconducting materials are provided equidistantly on a magnetizing surface of the magnetizing yoke, and the superconducting materials are brought into a superconducting state and electricity is applied to the winding.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12529688A JPH01293603A (en) | 1988-05-23 | 1988-05-23 | Magnetization device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12529688A JPH01293603A (en) | 1988-05-23 | 1988-05-23 | Magnetization device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01293603A true JPH01293603A (en) | 1989-11-27 |
Family
ID=14906573
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12529688A Pending JPH01293603A (en) | 1988-05-23 | 1988-05-23 | Magnetization device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01293603A (en) |
-
1988
- 1988-05-23 JP JP12529688A patent/JPH01293603A/en active Pending
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