JPH0254021B2 - - Google Patents

Info

Publication number
JPH0254021B2
JPH0254021B2 JP58112293A JP11229383A JPH0254021B2 JP H0254021 B2 JPH0254021 B2 JP H0254021B2 JP 58112293 A JP58112293 A JP 58112293A JP 11229383 A JP11229383 A JP 11229383A JP H0254021 B2 JPH0254021 B2 JP H0254021B2
Authority
JP
Japan
Prior art keywords
pole
magnet
series
magnetic
magnetized
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP58112293A
Other languages
Japanese (ja)
Other versions
JPS59188366A (en
Inventor
Wataru Kakigi
Yoshitaro Wada
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.)
Akai Electric Co Ltd
Original Assignee
Akai Electric 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 Akai Electric Co Ltd filed Critical Akai Electric Co Ltd
Priority to JP11229383A priority Critical patent/JPS59188366A/en
Publication of JPS59188366A publication Critical patent/JPS59188366A/en
Publication of JPH0254021B2 publication Critical patent/JPH0254021B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K21/00Synchronous motors having permanent magnets; Synchronous generators having permanent magnets
    • H02K21/12Synchronous motors having permanent magnets; Synchronous generators having permanent magnets with stationary armatures and rotating magnets
    • H02K21/24Synchronous motors having permanent magnets; Synchronous generators having permanent magnets with stationary armatures and rotating magnets with magnets axially facing the armatures, e.g. hub-type cycle dynamos

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、回転軸の回転数に応じた周波数信号
を出力する周波数発電機に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a frequency generator that outputs a frequency signal according to the number of rotations of a rotating shaft.

(従来の技術) 一般にサーボモータ等においては、周波数発電
機をモータの回転軸に連結し、周波数発電機によ
りモータの回転数に応じた周波数信号を検出し、
これを電圧に変換(F−V変換)し、さらにこの
電圧を回転速度制御電圧としてモータの回転速度
制御を行なうようにしたものが知られている。
(Prior art) Generally, in a servo motor, etc., a frequency generator is connected to the rotating shaft of the motor, and a frequency signal corresponding to the rotation speed of the motor is detected by the frequency generator.
It is known that this voltage is converted into a voltage (F-V conversion) and this voltage is used as a rotational speed control voltage to control the rotational speed of the motor.

第1図は、周波数発電機の一例の分解斜視図で
ある。第1図において、1はN極部とS極部が円
周方向に交互に均等に分割着磁された駆動用多極
マグネツトであり、2はこの駆動用多極マグネツ
ト1に固着され駆動用多極マグネツト1の外周に
配置される環状部を有し磁性体からなるロータで
ある。これらの駆動用多極マグネツト1とロータ
2は回転軸(図示せず)に固着されて回転自在に
構成される。さらに、環状部の一方の側面に、放
射状の溝部2Aにより同一ピツチで複数の凹凸部
が形成される。そして、この溝部2Aは、前記駆
動用多極マグネツト1のS極部とN極部とに対応
して電気角180゜位相がずらされるとともに、S極
部とN極部との境は凸部で連なるように形成され
る。ここで、駆動用多極マグネツト1のN極部に
対応する部分の環状部がS磁極に帯磁され、この
N極部と、S磁極に帯磁された環状部との間に形
成される磁路の磁束密度は、環状部の凸部で高
く、凹部で低くなる。また同様に、駆動用多極マ
グネツト1のS極部に対応する部分の環状部がN
磁極に帯磁され、磁束の向きは逆となるが磁束密
度は、環状部の凸部で高く、凹部で低くなる。
FIG. 1 is an exploded perspective view of an example of a frequency generator. In Fig. 1, numeral 1 is a driving multi-pole magnet in which N-pole portions and S-pole portions are magnetized alternately and equally in the circumferential direction, and numeral 2 is a driving multi-polar magnet fixed to this driving multi-polar magnet 1. It is a rotor made of a magnetic material and has an annular portion disposed around the outer periphery of a multipolar magnet 1. These driving multi-pole magnet 1 and rotor 2 are fixed to a rotating shaft (not shown) and are configured to be freely rotatable. Further, on one side of the annular portion, a plurality of uneven portions are formed at the same pitch by the radial groove portion 2A. The groove portion 2A is shifted in phase by 180 degrees in electrical angle corresponding to the S-pole portion and the N-pole portion of the driving multi-pole magnet 1, and the boundary between the S-pole portion and the N-pole portion is formed by a convex portion. It is formed in a continuous manner. Here, the annular portion of the drive multipolar magnet 1 corresponding to the N pole is magnetized to the S magnetic pole, and a magnetic path is formed between the N pole and the annular portion magnetized to the S magnetic pole. The magnetic flux density is high in the convex part of the annular part and low in the concave part. Similarly, the annular portion of the drive multipolar magnet 1 corresponding to the S pole is N
The magnetic poles are magnetized, and the direction of the magnetic flux is reversed, but the magnetic flux density is high at the convex portion of the annular portion and low at the concave portion.

このようにして、環状部の凹凸部により一磁極
に対応する部分で、2n+1(n=1、2、3…)
回の周期的な磁束の変化がもたらされている。
In this way, due to the unevenness of the annular part, 2n+1 (n=1, 2, 3...) is formed in the part corresponding to one magnetic pole.
This results in periodic changes in magnetic flux.

また、ロータ2の環状部の溝部2Aが設けられ
た側面に対面するようにプリント基板(図示せ
ず)が配設され、その対向する一面に、溝部2A
に臨んで溝部2Aと同一ピツチで放射状に複数の
発電線素3が配設されてジグザグ状に直列接続さ
れた発電コイルが形成される。なお、この発電コ
イルは適宜に固定されている。
Further, a printed circuit board (not shown) is disposed so as to face the side surface of the annular portion of the rotor 2 on which the groove portion 2A is provided, and the groove portion 2A is provided on one surface facing the printed circuit board (not shown).
A plurality of power generation line elements 3 are arranged radially at the same pitch as the groove portion 2A facing the groove 2A, thereby forming a power generation coil connected in series in a zigzag pattern. Note that this power generation coil is fixed as appropriate.

かかる構成において、回転軸の回転にともない
ロータ2が発電線素3に対し同心で回転すると、
溝部2Aで得られる磁束の変化によつて、発電線
素3を透過する磁界の強さの変化により発電線素
3に電圧が誘起される。そして、発電コイルの出
力端子からの発電線素3の全周にわたつて積分
(加算)された電圧が、ロータ2の回転数に応じ
た周波数信号として出力される。
In such a configuration, when the rotor 2 rotates concentrically with respect to the power generating line element 3 as the rotating shaft rotates,
A voltage is induced in the power generation line element 3 due to a change in the strength of the magnetic field passing through the power generation line element 3 due to a change in the magnetic flux obtained in the groove portion 2A. Then, the voltage integrated (added) over the entire circumference of the power generation line element 3 from the output terminal of the power generation coil is output as a frequency signal corresponding to the rotation speed of the rotor 2.

ここで、磁束の変化は駆動用多極マグネツト1
の1個の磁極に対応する部分において2n+1(n
=1、2、3、…)回の周期的な磁束の変化を生
ずる。なお、第1図に示した一例においては、11
回の周期的な磁束の変化を生ずる。
Here, the change in magnetic flux is determined by the driving multipole magnet 1.
2n+1(n
= 1, 2, 3, ...) periodic magnetic flux changes occur. In addition, in the example shown in Figure 1, 11
This causes a periodic change in magnetic flux.

次に、第2図を用いて、第1図に示したものの
動作を詳細に説明する。第2図においてA及びB
は発電線素3及びロータ2の円周方向断面図であ
り、Cは上記発電線素3を透過する磁束の変化の
様子を簡略化し、スイツチング動作に置きかえて
示した図である。この第2図Cにおいて、実際上
は、ロータ2の帯磁における磁極の境は磁束が緩
やかに変化しており、図示のごとく急速に変化し
ない。なお、第2図のAにおいて、誘起される電
圧の方向を(図面の前方から後方の方向)ある
いは○†ぁ平淕未慮緤
Next, the operation shown in FIG. 1 will be explained in detail using FIG. 2. A and B in Figure 2
1 is a circumferential cross-sectional view of the power generating line element 3 and the rotor 2, and C is a diagram showing a simplified state of change in the magnetic flux passing through the power generating line element 3, replacing it with a switching operation. In this FIG. 2C, in reality, the magnetic flux changes slowly at the boundaries of the magnetic poles in the magnetization of the rotor 2, and does not change rapidly as shown in the figure. In addition, in A of Figure 2, the direction of the induced voltage can be expressed as (from the front to the rear of the drawing) or

Claims (1)

【特許請求の範囲】[Claims] 1 回転軸に固定されて回動自在であり円周方向
に分割着磁された駆動用多極マグネツトに、磁性
体からなり前記駆動用多極マグネツトの外周に配
置される環状部を有するロータを固着し、前記環
状部の一方の側面に放射状の溝部によつて同一ピ
ツチで複数の凹凸部を形成し、前記駆動用多極マ
グネツトのS極部とN極部とに対応する前記溝部
を電気角180゜ずらすとともに前記S極部とN極部
との境が凸部の連なりと凹部の連なりが交互とな
るようにし、前記駆動用多極マグネツトの磁極に
より帯磁される前記環状部が一磁極に対応する部
分で2n(n=1、2、3…)回の周期的な磁束の
変化をさせ、前記環状部の凹凸部に臨んで前記凹
凸部と同一ピツチで放射状の発電線素がジグザグ
状に直列接続された発電コイルを固定配設したこ
とを特徴とする周波数発電機。
1. A rotor having an annular portion made of a magnetic material and arranged around the outer periphery of the multi-polar driving magnet is attached to a multi-polar driving magnet that is fixed to a rotating shaft and is freely rotatable and magnetized in sections in the circumferential direction. A plurality of uneven parts are formed at the same pitch by radial grooves on one side of the annular part, and the grooves corresponding to the S and N poles of the driving multipolar magnet are electrically connected. The corner is shifted by 180 degrees, and the boundary between the S and N poles is made so that a series of convex parts and a series of concave parts alternate, and the annular part magnetized by the magnetic pole of the multi-pole drive magnet has one magnetic pole. The periodic magnetic flux is changed 2n (n=1, 2, 3...) times in the part corresponding to A frequency generator characterized by a fixed arrangement of generating coils connected in series.
JP11229383A 1983-06-22 1983-06-22 Frequency generator of servo motor or the like Granted JPS59188366A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11229383A JPS59188366A (en) 1983-06-22 1983-06-22 Frequency generator of servo motor or the like

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11229383A JPS59188366A (en) 1983-06-22 1983-06-22 Frequency generator of servo motor or the like

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP6193083A Division JPS59188365A (en) 1983-04-07 1983-04-07 Frequency generator of servo motor or the like

Publications (2)

Publication Number Publication Date
JPS59188366A JPS59188366A (en) 1984-10-25
JPH0254021B2 true JPH0254021B2 (en) 1990-11-20

Family

ID=14583060

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11229383A Granted JPS59188366A (en) 1983-06-22 1983-06-22 Frequency generator of servo motor or the like

Country Status (1)

Country Link
JP (1) JPS59188366A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS53115012A (en) * 1977-03-18 1978-10-07 Matsushita Electric Ind Co Ltd Motor with frequency generator
JPS5498905A (en) * 1978-01-20 1979-08-04 Matsushita Electric Ind Co Ltd Motor with frequency generator

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS53115012A (en) * 1977-03-18 1978-10-07 Matsushita Electric Ind Co Ltd Motor with frequency generator
JPS5498905A (en) * 1978-01-20 1979-08-04 Matsushita Electric Ind Co Ltd Motor with frequency generator

Also Published As

Publication number Publication date
JPS59188366A (en) 1984-10-25

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