JPS6070955A - Magnetizing device - Google Patents

Magnetizing device

Info

Publication number
JPS6070955A
JPS6070955A JP17766083A JP17766083A JPS6070955A JP S6070955 A JPS6070955 A JP S6070955A JP 17766083 A JP17766083 A JP 17766083A JP 17766083 A JP17766083 A JP 17766083A JP S6070955 A JPS6070955 A JP S6070955A
Authority
JP
Japan
Prior art keywords
magnetic pole
slots
pole
forming
frequency
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
Application number
JP17766083A
Other languages
Japanese (ja)
Inventor
Norimitsu Hirano
平野 紀光
Masataka Ogawa
小川 昌貴
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP17766083A priority Critical patent/JPS6070955A/en
Publication of JPS6070955A publication Critical patent/JPS6070955A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K29/00Motors or generators having non-mechanical commutating devices, e.g. discharge tubes or semiconductor devices
    • H02K29/14Motors or generators having non-mechanical commutating devices, e.g. discharge tubes or semiconductor devices with speed sensing devices
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F13/00Apparatus or processes for magnetising or demagnetising
    • H01F13/003Methods and devices for magnetising permanent magnets
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K15/00Methods or apparatus specially adapted for manufacturing, assembling, maintaining or repairing of dynamo-electric machines
    • H02K15/02Methods or apparatus specially adapted for manufacturing, assembling, maintaining or repairing of dynamo-electric machines of stator or rotor bodies
    • H02K15/03Methods or apparatus specially adapted for manufacturing, assembling, maintaining or repairing of dynamo-electric machines of stator or rotor bodies having permanent magnets

Abstract

PURPOSE:To enable to perform a fine magnetization in a simple step by forming slots for forming a frequency detecting pole of fine pitch in the entire end of a cylinder, and winding an exciting coil in the slots. CONSTITUTION:A magnetizing yoke 14' has a cylinder 15' made of a ferromagnetic material. Thick four slots 17' which perpendicularly crosses at the center are inserted at an equal interval to the ends 16' of the cylinder 15', and exciting coil of thick diameter is wound in the slots 17'. Slots 19, 19' for forming the many frequency detecting pole of a fine interval pitch are formed over the entirety, and exciting coils are spirally wound in the slots 19, 19'.

Description

【発明の詳細な説明】 本発明は、ディスク型ブラシレスモータの主マグネット
の磁極に周波数検出用磁極を容易に重畳形成することが
できるようにした着磁装置に関する。ダイレクトドライ
ブ方式のカセットテープレフーダ等に用いるディスク型
ブラシレスモータにあっては、細かな回転速度信号を得
る必要がある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetizing device that can easily form a frequency detection magnetic pole overlapping the magnetic pole of a main magnet of a disc-type brushless motor. In a disc type brushless motor used in a direct drive type cassette tape recorder or the like, it is necessary to obtain a detailed rotational speed signal.

このようなディスク型ブラシレスモーターとしては、第
1図に示すような構造のものが知られている。このモー
ターについて説明すると、モータ軸2には円板状のロー
タヨーク3が固定され、この四−タヨーク乙の下面には
第2図に示すようなりング状の界磁マグネット4が接着
固定されている。
As such a disk type brushless motor, one having a structure as shown in FIG. 1 is known. To explain this motor, a disk-shaped rotor yoke 3 is fixed to the motor shaft 2, and a ring-shaped field magnet 4 is adhesively fixed to the lower surface of this four-way yoke B as shown in FIG. .

モータ軸2の先端側はセンタースピンドル5が形成され
、またその下端側は軸受6によって回転自在書ど支持さ
れている。軸受6にはステータヨーク7が固定され、こ
のステータヨーク7上には第3図に示すように3個の扇
枠状の電機子コイル8tP平面重畳しないように等間隔
配置で接着固定している。電機子コイル8の枠内空胴部
白書どは回転位置検知のためのホール素子、ホールIC
,磁気抵抗素子等の磁電変換素子9が収納配置されてい
る。
A center spindle 5 is formed at the front end of the motor shaft 2, and a rotatable shaft is supported at the lower end by a bearing 6. A stator yoke 7 is fixed to the bearing 6, and on this stator yoke 7, as shown in FIG. 3, three fan frame-shaped armature coils 8tP are adhesively fixed at equal intervals so as not to overlap in plane. . The white paper inside the frame of the armature coil 8 is a Hall element and Hall IC for detecting the rotational position.
, a magnetoelectric transducer 9 such as a magnetoresistive element is housed.

H子コイル8の上面には円板状のプリント基板10が固
定され、このプリント基板1oの表面ニはロータの回転
速度検出(周波数発電機形成)用の<シ歯状導電パター
ン11が形成されている。
A disk-shaped printed circuit board 10 is fixed to the upper surface of the H coil 8, and a tooth-shaped conductive pattern 11 for detecting the rotational speed of the rotor (forming a frequency generator) is formed on the surface of the printed circuit board 1o. ing.

プリント基板10と界磁マグネット4とは微少空隙を隔
てて対向している。
The printed circuit board 10 and the field magnet 4 face each other with a small gap in between.

第2図は第1図の界磁マグネット4の下面図である。第
2図に示すように、界磁マグネット4の主磁極12は、
N、Sの磁極を交互等間隔に有する4極のものに着磁形
成され、その周辺部にはロータ回転速度検出用の約18
0極の周波数検出用磁411!13が形成されている。
FIG. 2 is a bottom view of the field magnet 4 of FIG. 1. As shown in FIG. 2, the main magnetic pole 12 of the field magnet 4 is
It is magnetized into a 4-pole structure with N and S magnetic poles alternately spaced at equal intervals, and around the periphery there are approximately 18
A zero-pole frequency detection magnet 411!13 is formed.

N極、S極はN’ffi。The north and south poles are N'ffi.

S′極よりも強く着磁されている。従って、N’%はS
極の、S′極はN極の機能を果たすので、N極。
It is more strongly magnetized than the S' pole. Therefore, N'% is S
The S' pole of the poles functions as a north pole, so it is a north pole.

S極の周波数検出用mf5が交互に細かなピッチで着磁
形成されていることになる。
This means that the S-pole frequency detection mf5s are alternately magnetized and formed at a fine pitch.

第5図は、従来における主磁極12の着磁方法を説明す
るため着磁装置14の斜視図である。この着口装置14
は、純鉄等の強磁性体よりなる円筒体15の端面16に
、中心で直交するような溝17を入れ、これに1117
.動用の主磁極12を形成するための励磁用コイル18
を巻装したものとなっている。これをマグネットに接触
させ、励磁用コイル18に通電することによって4極の
主磁極12を着磁する。
FIG. 5 is a perspective view of the magnetizing device 14 for explaining a conventional method of magnetizing the main pole 12. As shown in FIG. This entrance device 14
In this method, a groove 17 is formed perpendicularly at the center in the end face 16 of a cylindrical body 15 made of a ferromagnetic material such as pure iron, and a groove 1117 is formed in this groove.
.. Excitation coil 18 for forming the main magnetic pole 12 for operation
It is wrapped in . By bringing this into contact with a magnet and energizing the excitation coil 18, the four main magnetic poles 12 are magnetized.

このように、まず主磁極12を着磁した後、周波数検出
用磁極13を着磁するための専用の着磁装置(図示せず
)を用いて、周波数検出用磁極13を比較的弱く着磁す
る。
In this way, after first magnetizing the main magnetic pole 12, the frequency detecting magnetic pole 13 is relatively weakly magnetized using a special magnetizing device (not shown) for magnetizing the frequency detecting magnetic pole 13. do.

従って、界磁マグネット4が形成する空隙部の磁束密度
波形は第6図のようになる。
Therefore, the magnetic flux density waveform in the gap formed by the field magnet 4 is as shown in FIG.

この第6図に示すように、主磁極12によって形成され
た磁束密度波形に、周波数検出用磁極13によって形成
された磁束密度波形が重畳された形となるので、主磁極
12によって形成された磁束密度波形の山又は谷部に細
かな凹凸の波形が形成される。
As shown in FIG. 6, the magnetic flux density waveform formed by the main magnetic pole 12 is superimposed on the magnetic flux density waveform formed by the frequency detection magnetic pole 13, so the magnetic flux formed by the main magnetic pole 12 A finely uneven waveform is formed at the peaks or valleys of the density waveform.

第4図は第1図のプリント基板10の平面図である。プ
リント基板10の表面における界磁マグネット4の周波
数検出用磁極13と対向する部分には、第4図に示すよ
うなくし歯状の導電パターン11が形成されている。こ
の導電パターン11のピッチは、第2図に示す周波数検
出用磁極13のピッチと同一である。導電パターン11
の放射方向の一本置きの線分群が、例えば周波数検出用
磁極のN又はS極と対向しているとき、これらの間の線
分群はぜ又はSlこ対向する。これによって各線分に周
波数検出用磁極13の回転速度に応じた同方向の起電力
が発生し、導電パターン11の図示しない出力端子から
ロータの回転速度に応じた周波数の検出出力が得られる
FIG. 4 is a plan view of the printed circuit board 10 of FIG. 1. A comb-shaped conductive pattern 11 as shown in FIG. 4 is formed on the surface of the printed circuit board 10 in a portion facing the frequency detection magnetic pole 13 of the field magnet 4. As shown in FIG. The pitch of this conductive pattern 11 is the same as the pitch of the frequency detection magnetic poles 13 shown in FIG. Conductive pattern 11
When every other line segment group in the radial direction faces, for example, the N or S pole of the frequency detection magnetic pole, the line segments between them are opposite to each other. As a result, an electromotive force is generated in the same direction in each line segment according to the rotational speed of the frequency detection magnetic pole 13, and a detection output of a frequency corresponding to the rotational speed of the rotor is obtained from an output terminal (not shown) of the conductive pattern 11.

尚、周波数検出用磁極13によるパルス状磁束は間欠的
に現われるが、導電パターン11が第4図に示すように
全周に形成されている(全周積分型となっている)ので
、検出出力は連続波で得られる。また周波数検出用磁極
13にピッチむらがあっても、複数の導電パターン11
の放射方向の線分群によってピッチむらは平均化され、
ロータの回転数が一定のとき一定の周波数の検出出力が
得られる。ロータ回転数の変動分は検出出力の周(5) 波数変温成分として取り出される。
Although the pulsed magnetic flux generated by the frequency detection magnetic pole 13 appears intermittently, since the conductive pattern 11 is formed around the entire circumference as shown in FIG. is obtained with continuous waves. Furthermore, even if the frequency detection magnetic poles 13 have pitch irregularities, the plurality of conductive patterns 11
The pitch unevenness is averaged by a group of line segments in the radial direction of
When the rotation speed of the rotor is constant, a detection output of a constant frequency is obtained. The variation in the rotor rotational speed is extracted as the frequency (5) wave number variable temperature component of the detection output.

上記した回転速度検出桟構を有するディスク型ブラシレ
スモータ1は、最近においては非常に注目を集め、各社
その開発に必死になっているところである。
The disk-type brushless motor 1 having the above-mentioned rotational speed detection frame structure has recently attracted much attention, and various companies are desperately trying to develop it.

しかし、従来において、主磁極12.及び周波数検出用
磁極13を有する界磁マグネット4を形成するのに非常
に手間がかかっていた。即ち、主磁極12の着磁と、周
波数検出用磁極13の着磁とを分離して行なわなければ
ならなかったためである。そのために、主磁極12を形
成する着磁装置と、周波数検出用磁極13を形成する着
磁装置を必要とするので非常に高価なものとなっていた
However, in the past, the main magnetic pole 12. Also, it took a lot of effort to form the field magnet 4 having the frequency detection magnetic pole 13. That is, this is because the magnetization of the main magnetic pole 12 and the magnetization of the frequency detection magnetic pole 13 had to be performed separately. For this purpose, a magnetizing device for forming the main magnetic pole 12 and a magnetizing device for forming the frequency detecting magnetic pole 13 are required, resulting in a very expensive device.

また第4図を参照して導電パターン11は普通半径方向
に1個形成されているが、半径方向の導体部11aと1
1a′との幅をつめることは、現今の技術では非常にや
っかいであった。そのためζこ、より精度の良い回転速
度信号が得られないため、より性能の良い回転速度制御
がなし得ないものとなっていた。本発明はかかる事情に
基づいてなさく6) れた着磁装置で、主磁極と周波数検出用磁極とを同時に
着磁できるようにして、着磁工程の簡略をはかれるよう
にし、また安価に着磁装置を構成できるようにすると共
に、より細かな精度の良い回転速度信号を得るために周
波数信号をより多く取れるようにすることを目的として
なされたものである。
Further, referring to FIG. 4, one conductive pattern 11 is normally formed in the radial direction, but the conductive pattern 11 in the radial direction
Reducing the width of 1a' is extremely troublesome with current technology. Therefore, a more accurate rotational speed signal cannot be obtained, making it impossible to control the rotational speed with better performance. The present invention has been developed based on the above circumstances.6) It is possible to simultaneously magnetize the main magnetic pole and the frequency detection magnetic pole using a magnetizing device, thereby simplifying the magnetizing process and reducing the cost. This was done for the purpose of making it possible to construct a magnetic device and also to be able to obtain more frequency signals in order to obtain finer and more accurate rotational speed signals.

本発明のかかる目的は、駆動用の主磁極を形成するため
の励磁用コイルを巻装するための、磁性体よりなる円筒
体の端面に中心で直交する溝を設けた着磁装置において
、上記端面全体に細かなピッチの周波数検出用磁極を形
成するために細かなピッチで中心で直交する周波数構1
隻!極形成用溝を多数形成し、該溝に励磁用フィルを巻
装してなることを特徴とする着磁装置において、上記周
波幻 数構出用磁極形成用溝を周波数検出用磁極伐2分の1ピ
ッチ周方向に位相をずらせて上記端面の内外周に2段設
けたことを特徴とする着磁装置を提供することによって
達成される。
An object of the present invention is to provide a magnetizing device in which a groove orthogonal to the center is provided in the end face of a cylindrical body made of a magnetic material for winding an excitation coil for forming a main magnetic pole for driving. In order to form frequency detection magnetic poles with a fine pitch over the entire end face, the frequency structure 1 is made perpendicular to each other at the center with a fine pitch.
Ship! In a magnetizing device characterized in that a large number of pole forming grooves are formed and an excitation fill is wound around the grooves, the magnetic pole forming groove for frequency phantom number formation is formed with a magnetic pole section for frequency detection of 2 minutes. This is achieved by providing a magnetizing device characterized in that two stages are provided on the inner and outer peripheries of the end face with the phase shifted by one pitch in the circumferential direction.

以下第8図以下を参照して本発明の着磁装置の(7) 実施例を説明していく。尚、第5図と共通する部分には
、ダラシを符することとする。
Embodiment (7) of the magnetizing device of the present invention will be described below with reference to FIG. 8 and subsequent figures. Note that parts that are common to those in FIG. 5 are marked with dashes.

第8図は本発明の着磁ヨーク14′の斜視図で、この着
磁ヨーク14′は4極の主磁極12を形成するものとし
て構成されている。着磁ヨーク14′はこの溝17′に
第5図の場合と同様に太い線径の励磁用コイル18を巻
装し、上記端面16′に細がなピッチの周波数検出用磁
極13を界磁マグネットし、該溝19A、19bに第9
図で示すように細い線径の周波数検出用磁極13形成の
ための励磁用コイル21−1.21−2を螺旋状に巻装
している。上記端面16′(ど半径方向に2段に渡って
設けた溝19aと19bは、周方向において当該溝19
a、19bの2分の1幅だけ位相をずらせて形成してい
る。このようにしたのは、上記した形状の着磁ヨーク1
4′(第8図及び第9図参照)を(8) 用いて、例えば、第10図に示すような周波数検出用磁
極13及び主磁極(駆動用磁極)12を有する円環状の
界磁マグネット14′を形成するためである。
FIG. 8 is a perspective view of the magnetizing yoke 14' of the present invention, and the magnetizing yoke 14' is configured to form four main magnetic poles 12. In the magnetizing yoke 14', an excitation coil 18 with a thick wire diameter is wound around the groove 17' as in the case of FIG. magnet, and the ninth groove is placed in the grooves 19A and 19b.
As shown in the figure, excitation coils 21-1 and 21-2 for forming the frequency detecting magnetic pole 13 having a thin wire diameter are wound in a spiral manner. The grooves 19a and 19b provided in two stages in the radial direction of the end surface 16' (the grooves 19a and 19b in the circumferential direction
A and 19b are formed with a phase shift of one-half width. This was done because of the magnetizing yoke 1 having the above-mentioned shape.
4' (see FIGS. 8 and 9) (8), for example, an annular field magnet having a frequency detection magnetic pole 13 and a main magnetic pole (driving magnetic pole) 12 as shown in FIG. 14'.

従って、まずこの着磁ヨーク14′を用いて励磁用コイ
ル181ど電流を流して着磁してやると、当然のことな
がら、第2図に示すよう番ζN、Sの磁極を有する4極
の主磁極12が形成される。その後、励磁用コイル21
1.21−2に電流を流してやると、半径方向に2段に
渡って互いに周波数検出用磁極16の2分の1磁極だけ
周方向に位相のずれた2個の周波数検出用磁極13−1
゜13−2が主磁極12の中に形成され、第10図に示
す界磁マグネット4′が得られる。尚、励磁用コイル2
1は細い線径となっていることから、周波数検出用磁極
13は主磁極12に比較して比較的弱く着磁される。従
って、周波数検出用磁極13によるパルス状の磁束が電
機子コイル8に影響を与えることはほとんどない。
Therefore, when the magnetizing yoke 14' is first used to apply current to the excitation coil 181 to magnetize it, it is natural that four main magnetic poles having magnetic poles numbers ζN and S as shown in FIG. 12 is formed. After that, the excitation coil 21
1.21-2, two frequency detecting magnetic poles 13-1 whose phase is shifted in the circumferential direction from each other by one-half magnetic pole of the frequency detecting magnetic pole 16 in two steps in the radial direction
13-2 is formed in the main pole 12, and a field magnet 4' shown in FIG. 10 is obtained. In addition, excitation coil 2
Since the wire 1 has a small diameter, the frequency detection magnetic pole 13 is magnetized relatively weakly compared to the main magnetic pole 12. Therefore, the pulsed magnetic flux generated by the frequency detection magnetic pole 13 hardly affects the armature coil 8.

本発明は上記構成からなるため、主磁極を形成するため
の着磁装置と、周波数検出用の着磁装置を一体化しであ
るので、主磁極及び周波数検出用磁極の着磁を容易に行
なうことができ、第10図で示す界磁マグネットを安価
に量産できる。また、かかる機能を有する着磁装置を一
体化して小型にしているので、安価に形成できる効果が
ある。また、半径方向に2段に渡って設けた2個の周波
数検出用磁極を周方向に位相をずらせて形成しているの
で、形成されるべきディスク型ブラシレスモータにおい
て上記2個の周波数検出用磁極13−1.13−2.及
び該磁極13−1.13−2と面対向する2個の導電パ
ターン11−1.11−2とによって、2倍の速度検出
用の周波数が得られるので、F−9(周波数−電圧)変
換回路を用いることで、回転速度制御のしやすい滑らか
且つ高い回転速度電圧が得られるので、精度の良いディ
スク型ブラシレスモータが安価へ容易に得られる効果が
ある着磁装置が得られる効果中鳴喝。また、2個の導電
パターン11−1.11−2それぞれから得られる回転
速度信号は、周波数検出用磁極16の2分の1ピツチだ
け位相をずらせて形成しているので、これを利用して、
A相及びB相の2つの相の回転速度信号が得られるので
、かかるA相、B相信号に基いてディスク型ブラシレス
モータの回転方向を知ることができるので、特に複雑且
つ高価になる手段を設けることをしなくても、当該ブラ
シレスモータの正逆回転方向制御が容易に行なえる効果
がある。
Since the present invention has the above configuration, the magnetizing device for forming the main magnetic pole and the magnetizing device for frequency detection are integrated, so that the main magnetic pole and the frequency detection magnetic pole can be easily magnetized. Therefore, the field magnet shown in FIG. 10 can be mass-produced at low cost. Furthermore, since the magnetizing device having such a function is integrated and made compact, there is an advantage that it can be manufactured at low cost. In addition, since the two frequency detection magnetic poles provided in two steps in the radial direction are formed with a phase shift in the circumferential direction, the two frequency detection magnetic poles in the disk type brushless motor to be formed are 13-1.13-2. Since the frequency for speed detection is twice as high due to the magnetic pole 13-1.13-2 and the two conductive patterns 11-1.11-2 facing each other, F-9 (frequency-voltage) By using a conversion circuit, it is possible to obtain a smooth and high rotational speed voltage that is easy to control the rotational speed, so a highly accurate disc-type brushless motor can be easily obtained at low cost. Drink. Furthermore, since the rotational speed signals obtained from each of the two conductive patterns 11-1 and 11-2 are formed with a phase shift of one-half pitch of the frequency detection magnetic pole 16, this can be used to ,
Since the rotational speed signals of two phases, A phase and B phase, can be obtained, the rotation direction of the disc type brushless motor can be known based on the A phase and B phase signals, which eliminates the need for particularly complicated and expensive means. There is an effect that the forward and reverse rotation directions of the brushless motor can be easily controlled without the need for such a configuration.

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

第1図はディスク型ブラシレスモータの縦断面図、第2
図は主磁極及び周波数検出用磁極を有する界磁マグネッ
トの下面図、第3図は電機子コイル群の配設方法を示す
ための説明図、第4図は導電パターンを有するプリント
基板の平面図、第5図は従来の主磁極を形成するための
着磁方法を示す着磁ヨークの斜視図、第6図は第2図の
界磁マグネットが形成する空隙磁束密度の波形図、第7
図は本発明の導電パターンを半径方向に2段に渡って設
けたプリント基板の平面図、第8図は本発明の一実施例
を示す着磁ヨークの斜視図、第9図は第8図の着磁ヨー
クに周波数検出用の励磁コイルを巻装したものの平面図
、第10図は本発明によって得られる主磁極及び周波数
検出用磁極を有する界磁マグネットの斜視図である。 1・・・ディスク型ブラシレスモータ、2・・・モータ
軸、3・・・ロータヨーク、4.4′・・・界磁マグネ
ット、 5・・・センタースピンドル、6・・・軸受、
7・・・ステータヨーク、8・・−電機子コイル、9・
・・磁電変換素子、10・・・プリント基板、11・・
・導電、<ターン、12・・・主磁極、16・・・周波
数検出用磁極、14.14’・・・着磁ヨーク、15.
15’・・・円筒体、 16.16’・・・端面、特許
出願人 高 橋 義 照@ 第5図 第6図 第7図 II(1”” 17−1 7−2 〆 第8図 (C(:○力)! へ悼虞−i。 /4’ 第9図 第1Q図
Figure 1 is a longitudinal cross-sectional view of a disc-type brushless motor, Figure 2
The figure is a bottom view of a field magnet that has a main magnetic pole and a frequency detection magnetic pole, Figure 3 is an explanatory diagram showing how to arrange the armature coil group, and Figure 4 is a plan view of a printed circuit board with a conductive pattern. , FIG. 5 is a perspective view of a magnetizing yoke showing a conventional magnetization method for forming a main magnetic pole, FIG. 6 is a waveform diagram of the air gap magnetic flux density formed by the field magnet in FIG. 2, and FIG.
The figure is a plan view of a printed circuit board on which the conductive pattern of the present invention is provided in two stages in the radial direction, FIG. 8 is a perspective view of a magnetizing yoke showing an embodiment of the present invention, and FIG. FIG. 10 is a plan view of a magnetizing yoke in which an excitation coil for frequency detection is wound, and FIG. 10 is a perspective view of a field magnet having a main magnetic pole and a frequency detection magnetic pole obtained by the present invention. DESCRIPTION OF SYMBOLS 1... Disk type brushless motor, 2... Motor shaft, 3... Rotor yoke, 4.4'... Field magnet, 5... Center spindle, 6... Bearing,
7...Stator yoke, 8...-armature coil, 9...
... Magnetoelectric conversion element, 10... Printed circuit board, 11...
・Conductivity, <turn, 12...Main magnetic pole, 16...Magnetic pole for frequency detection, 14.14'...Magnetizing yoke, 15.
15'... Cylindrical body, 16.16'... End face, patent applicant Yoshiteru Takahashi @ Figure 5 Figure 6 Figure 7 II (1"" 17-1 7-2 〆Figure 8 ( C(:○力)! へ う -i. /4' Figure 9 Figure 1Q

Claims (1)

【特許請求の範囲】 駆動用の主磁極を形成するための励磁用コイルを巻装す
るために、磁性体よりなる円筒体の端面に中心で直交す
る溝を設けた着磁装置において、上記端面に細かなピッ
チの周波数検出用磁極を形用 成するために細かなピッチで周波数検苧極形成用溝を多
数形成し、該溝に励磁用コイルを巻装してなることを特
徴とする着磁ヨークにおいて、上面の内外周半径方向に
2段設けたことを特徴とする着磁装置。
[Scope of Claims] A magnetizing device in which a groove orthogonal at the center is provided in the end face of a cylindrical body made of a magnetic material in order to wind an excitation coil for forming a main magnetic pole for driving. In order to form frequency detecting magnetic poles with a fine pitch, a large number of frequency detecting pole forming grooves are formed at a fine pitch, and an excitation coil is wound around the grooves. A magnetizing device characterized in that a magnetic yoke is provided with two stages in the radial direction of the inner and outer circumferences of the upper surface.
JP17766083A 1983-09-26 1983-09-26 Magnetizing device Pending JPS6070955A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17766083A JPS6070955A (en) 1983-09-26 1983-09-26 Magnetizing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17766083A JPS6070955A (en) 1983-09-26 1983-09-26 Magnetizing device

Publications (1)

Publication Number Publication Date
JPS6070955A true JPS6070955A (en) 1985-04-22

Family

ID=16034871

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17766083A Pending JPS6070955A (en) 1983-09-26 1983-09-26 Magnetizing device

Country Status (1)

Country Link
JP (1) JPS6070955A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0836020A2 (en) * 1996-10-11 1998-04-15 Nsk Ltd Rolling bearing unit with rotating speed sensor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0836020A2 (en) * 1996-10-11 1998-04-15 Nsk Ltd Rolling bearing unit with rotating speed sensor
EP0836020A3 (en) * 1996-10-11 1999-03-31 Nsk Ltd Rolling bearing unit with rotating speed sensor

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