JPS58198156A - Frequency generator - Google Patents

Frequency generator

Info

Publication number
JPS58198156A
JPS58198156A JP7817782A JP7817782A JPS58198156A JP S58198156 A JPS58198156 A JP S58198156A JP 7817782 A JP7817782 A JP 7817782A JP 7817782 A JP7817782 A JP 7817782A JP S58198156 A JPS58198156 A JP S58198156A
Authority
JP
Japan
Prior art keywords
permanent magnet
frequency generator
rotor
poles
armature winding
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
JP7817782A
Other languages
Japanese (ja)
Inventor
Kuniyoshi Nakamura
邦義 中村
Hiroshi Saito
博 斉藤
Masashi Ochiai
落合 正志
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.)
Nidec Advanced Motor Corp
Original Assignee
Nidec Servo Corp
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 Nidec Servo Corp filed Critical Nidec Servo Corp
Priority to JP7817782A priority Critical patent/JPS58198156A/en
Publication of JPS58198156A publication Critical patent/JPS58198156A/en
Pending 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

Abstract

PURPOSE:To improve the generating efficiency of a frequency generator by forming 2n pieces of small projections per one pole of a permanent magnet at an equal pitch on the surface of the permanent magnet which is opposed to an armature coil. CONSTITUTION:A rotor is composed of a permanent magnet 9 which is magnetized totally in number P alternately at N poles and S-poles circumferentially at an equal pitch. An armature coil 11 is composed by connecting generating strands of (2n+1)XP pieces radially arranged in series with each other. Further, 2n pieces of small projections d1 are formed on all poles in the prescribed height t at the same pitch as that of the generating strands of the coil 11. In this manner, the generating voltage can be increased.

Description

【発明の詳細な説明】 本発明は周波数発電機、特に円周方向に等ピッチでN極
S極交互に着磁され九永久磁石を回転子とし、はソ半径
方向に配設された複数の発電線素を直列に接続しで成る
電機子巻線を空隙を介して上記回転子に対向配設し、こ
の電機子巻線に回転子の回転速度に比例した周波数の交
流電圧を発生せしめるようにした周波数発電機の改良に
関するものでおる。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a frequency generator, in particular a rotor consisting of nine permanent magnets magnetized alternately with N and S poles at equal pitches in the circumferential direction, and a plurality of permanent magnets arranged in the radial direction. An armature winding made up of power generating wire elements connected in series is disposed opposite to the rotor with a gap in between, and an alternating current voltage with a frequency proportional to the rotational speed of the rotor is generated in the armature winding. This paper concerns the improvement of frequency generators.

本発明の目的は簡単な構成に依りその出力電圧を増加さ
せることができる周波数発電機を得るにある。
An object of the present invention is to obtain a frequency generator whose output voltage can be increased with a simple construction.

本発明の周波数発電機は、円周方向に等ピッチでN極S
極交互に合計P極に着磁された永久磁石を回転子とし、
はゾ牛径方向に配設された(2n+x)xP本(但しn
=1*2t3・・・・・・・・・正の整数)の発電線素
を直列に接続して成るtm子巻線を空隙を介して上記回
転子と対向配役し、この電機子巻線に回転子の回転速度
に比例した周波数の交流電圧を発生せしめるようKL7
h周波数発電機に於て、上記永久磁石の電機子巻線と対
向する表面に、該永久磁石の1極分について2n個の小
突起を等ピッチでかつ等しい萬さで設けた事を特徴とす
る。
The frequency generator of the present invention has N poles S at equal pitches in the circumferential direction.
A permanent magnet whose poles are alternately magnetized to a total of P poles is used as a rotor,
is (2n+x)xP books arranged in the radial direction (however, n
A tm child winding consisting of power generation line elements of =1*2t3 (positive integer) connected in series is arranged opposite to the rotor through a gap, and this armature winding KL7 to generate an AC voltage with a frequency proportional to the rotation speed of the rotor.
The h-frequency generator is characterized in that 2n small protrusions are provided on the surface of the permanent magnet facing the armature winding at equal pitches and with equal thickness for one pole of the permanent magnet. do.

以下図面に従い従来及び本発明の周波数発電機の実施例
について説明する。
Embodiments of the conventional frequency generator and the present invention will be described below with reference to the drawings.

第1図(JL)は本発明に係る周波数発電機を装着した
偏平形電動機の断面図を示し、1は電動機の外側ケース
を兼ねる固定子ヨーク、2はこの固定子ヨーク1に固定
し九ブラケット、3は上記固定子ヨーク1に固定した電
動機の固定子巻線、4はこの固定子巻線3と周波数発電
機とを装着した絶縁板、6は回転子軸、5はその軸受、
8は回転子ヨーク、9はこの回転子ヨーク8に固定した
永久磁石、7は上記回転子ヨーク8と永久磁石9とより
成る回転子のボス、10は上記絶縁板4と永久磁石9間
の空隙、11は上記絶縁板4に装着し九周波数発電機の
電機子巻線である。
FIG. 1 (JL) shows a cross-sectional view of a flat motor equipped with a frequency generator according to the present invention, in which 1 is a stator yoke that also serves as the outer case of the motor, and 2 is a nine bracket fixed to this stator yoke 1. , 3 is a stator winding of the motor fixed to the stator yoke 1, 4 is an insulating plate on which the stator winding 3 and the frequency generator are attached, 6 is a rotor shaft, 5 is a bearing thereof,
8 is a rotor yoke, 9 is a permanent magnet fixed to the rotor yoke 8, 7 is a boss of the rotor consisting of the rotor yoke 8 and the permanent magnet 9, and 10 is a space between the insulating plate 4 and the permanent magnet 9. The air gap 11 is attached to the insulating plate 4 and is an armature winding of a nine-frequency generator.

第1図伽)は上記絶縁板4に装着した周波数発電機の電
機子巻線11の詳細図で、この電機子巻線11は中心よ
シ半径方向に放射状に延在させた(2n+1)X’P本
(但しn = 11213−曲曲正の−数、Pは永久磁
石の極数)の発電線素11−1を円周方向に等ピッチで
配設し、該発電線素の相隣接し丸線の両端を外側の渡り
線11−2と内側の渡シ線11−3とで交互に接続して
全部の発電線素を直列に接続して成り外部に引出された
端子A、Bより永久磁石の回転速度に比例した周波数の
交流電圧が取り出され、この電圧が電動機の速度制御回
路に速度帰還信号として加えられ電動機の速度が設定速
度と一致されるように制御される。
Figure 1) is a detailed view of the armature winding 11 of the frequency generator mounted on the insulating plate 4, and the armature winding 11 extends radially from the center in the (2n+1)X ' P power generation line elements 11-1 (where n = 11213 - the number of positive curves, P is the number of poles of the permanent magnet) are arranged at equal pitches in the circumferential direction, and the power generation line elements are arranged adjacent to each other. Both ends of the round wire are connected alternately with the outer connecting wire 11-2 and the inner connecting wire 11-3, and all the generating line elements are connected in series, and the terminals A and B are drawn out to the outside. An alternating current voltage with a frequency more proportional to the rotational speed of the permanent magnet is taken out, and this voltage is applied as a speed feedback signal to the speed control circuit of the motor to control the speed of the motor to match the set speed.

第1図(e)は永久磁石9の着磁の状態を示す説明図で
、例えば全部で6極にN@S極交互に等ピッチで着磁さ
れる。磁束は紙面を貫通する方向に流れる。発電線素1
1−1の数は(2n+1)X2本でn=2.P=6の場
合を例示すれば発電線素の数は(2X2+1)X6=3
0本である。
FIG. 1(e) is an explanatory diagram showing the state of magnetization of the permanent magnet 9. For example, the permanent magnet 9 is magnetized into six poles in total, with N and S poles alternately arranged at equal pitches. The magnetic flux flows in a direction penetrating the plane of the paper. Power generation line element 1
The number of 1-1 is (2n+1)×2, n=2. Taking the case of P=6 as an example, the number of power generation line elements is (2X2+1)X6=3
There are 0 pieces.

この発電機の動作を説明する為に電機子巻線11と永久
磁石9の各磁極との相関々係を示す展開図を第2図(1
)に示す。第2図Φ)は永久磁石の磁束分布を直線形に
示した説明図である。
In order to explain the operation of this generator, a developed diagram showing the relationship between the armature winding 11 and each magnetic pole of the permanent magnet 9 is shown in FIG.
). FIG. 2 Φ) is an explanatory diagram showing a linear magnetic flux distribution of a permanent magnet.

永久磁石の各磁極の中性線にはn−1〜n−6と符号を
付し、電機子巻線110発電線素の導体には1〜30の
番号を付す。第2図41) 、 (b)に於て永久磁石
が→印の方向に回転すれば、発電線素の導体1〜30の
中で1.6.11,16,21゜26の6本の導体は永
久磁石の各a極間の中性線n−1r n−2tn−Ln
−4+n−Ln−6と夫々対向して相対的に運動するの
で、夫々の導体と鎖交する磁束がN極からS極へ、ある
いはS極よシN極へと急激に変化するので夫々の各導体
にはdφ −eLTTK従った起電力が発生し、しかも導体1.6
111,16,21.26の各導体は1本毎に逆向きと
なるように全部が直列に接続され、且つ鎖交する磁束の
変化の方向が逆となっているので、各導体に発生する起
電力の方向が一致し、端子A、Hに生ずる電圧は各導体
に誘起する電圧の合計となる。一方上記の導体i、6,
11゜16.21.26以外の他の導体と永久磁石よシ
発する磁束との鎖交状態は第2図φ)の磁束分布で明ら
かなように変化していないから誘起電圧は発生し・てい
ない。
The neutral wire of each magnetic pole of the permanent magnet is numbered n-1 to n-6, and the conductors of the armature winding 110 generating line elements are numbered 1 to 30. In Fig. 2 41), (b), if the permanent magnet rotates in the direction of the → mark, six of the conductors 1 to 30 of the power generating line element, 1, 6, 11, 16, 21°26 The conductor is the neutral line n-1r n-2tn-Ln between each a pole of the permanent magnet.
-4+n-Ln-6 and move relative to each other, the magnetic flux interlinking with each conductor changes rapidly from N pole to S pole, or from S pole to S N pole. An electromotive force according to dφ −eLTTK is generated in each conductor, and the conductor is 1.6
The conductors 111, 16, 21, and 26 are all connected in series so that each conductor is in the opposite direction, and the direction of change in the interlinking magnetic flux is opposite, so the magnetic flux generated in each conductor is The directions of the electromotive forces match, and the voltage generated at terminals A and H is the sum of the voltages induced in each conductor. On the other hand, the above conductors i, 6,
11゜16.21.26 The state of interlinkage between the magnetic flux generated by the permanent magnet and other conductors does not change as shown in the magnetic flux distribution in Figure 2 φ), so no induced voltage is generated. do not have.

次に永久磁石が回転を続け、中性線n−1が導体2と対
向する位置に達する位1となると導体2,7,12.1
7,22.27が夫々永久磁石の中性線n−1+ n−
2+ n−3r n−4+ n−5+ n−6と対向d
φ して鎖交磁束が急変し、各導体’−eL−a7に従つ九
起電力が発生し、全部の起電力の合計が端子A、Bに現
われる。このように第1図(&)〜(e)に示す構造の
周波数発電機に於ては、永久磁石の中性線と対向する発
電S素の導体とが対向(〜て相対運動する毎に導体に起
電力が発生し、その起電力の方向は1本毎に逆向となる
交流電圧となり、この交流電圧の周波数fは発電線素の
数をCとし永久磁石の回転数をN(r、p、rn)とす
ると N f−丁×菌(Hz) と表わす事ができ、出力電圧の周波数fは電動機の回転
速度と発電線素の数Cとに比例することになるので、電
動機の速度制御の質を高める為発電機の周波数を高くす
るには発電線素の数を多く配置すれば良く、又永久磁石
の極数を増加すると、同時に中性線と鎖交する導体数が
極数に比例して増加するので発生電圧を増加する事がで
きるという利点がある。しかしながら永久磁石の極数は
電動機の永久磁石と共用するものでは電動機の特性から
定められるのであまり多くする事ができず電機子巻線の
発電線素の中で電圧発生に役立っている導体の数は永久
磁石の極数と同数の導体のみで他の導体は休止している
ので発電効率が悪いという欠点があった。
Next, the permanent magnet continues to rotate, and when the neutral wire n-1 reaches a position facing the conductor 2, the conductors 2, 7, 12.1
7, 22.27 are the neutral wires of the permanent magnets n-1+ n-
2+ n-3r n-4+ n-5+ Opposed to n-6 d
φ, the interlinkage magnetic flux suddenly changes, nine electromotive forces are generated according to each conductor'-eL-a7, and the sum of all electromotive forces appears at terminals A and B. In this way, in the frequency generator having the structure shown in Fig. 1 (&) to (e), the neutral wire of the permanent magnet and the conductor of the opposing power generating S element are opposed to each other (... An electromotive force is generated in the conductor, and the direction of the electromotive force becomes an alternating voltage that is reversed for each conductor.The frequency f of this alternating current voltage is determined by the number of generating line elements being C and the rotation speed of the permanent magnet being N(r, p, rn), it can be expressed as N f-ton × bacteria (Hz), and since the frequency f of the output voltage is proportional to the rotational speed of the motor and the number C of generating line elements, the speed of the motor In order to increase the frequency of the generator in order to improve the quality of control, it is sufficient to arrange a large number of generating line elements, and when the number of poles of the permanent magnet is increased, the number of conductors interlinked with the neutral wire also increases. It has the advantage that the generated voltage can be increased because it increases in proportion to .However, if the permanent magnet is used in common with the permanent magnet of the motor, the number of poles of the permanent magnet cannot be increased too much because it is determined by the characteristics of the motor. The number of conductors that help generate voltage in the power generation wire element of the armature winding is only the same number as the number of poles of the permanent magnet, and the other conductors are at rest, which has the disadvantage of poor power generation efficiency. .

本発明は上述のような従来技術の発電機の問題点を解決
し発電効率の高い周波数発電機を提供するものである。
The present invention solves the problems of the conventional generators as described above and provides a frequency generator with high power generation efficiency.

本発明の第1の実施例に於ては第3図(a)に示すよう
に永久磁石9の磁極の発電線素と対向する面に、電機予
巻@11の発電線素11−1のピッチと同じピッチで2
n個の小突起d1を一定の高さtとなるよう全磁極につ
いて設ける。
In the first embodiment of the present invention, as shown in FIG. 3(a), the generating line element 11-1 of the electric machine pre-winding@11 is placed on the surface of the permanent magnet 9 facing the generating line element of the magnetic pole. 2 at the same pitch as the pitch
N small protrusions d1 are provided on all magnetic poles so as to have a constant height t.

本発明周波数発電機は上記のような構成であるから対向
する発電線素と鎖交する磁束の分布は第3図(b)のよ
うに、中性線n−1とn−2の間は一様でなく、小突起
d1のある部分の磁束は多く、突起の無いd、の部分は
磁束が少なくなり、発電線素の導体のピッチと同じピッ
チで磁束が増加あるいは減少する磁束の急変点が構成δ
れるO 従って第3図(a)の構成の発電機に於ては永久磁石の
回転により電圧発生に役立つ導体は中性線と対向してい
る導体1,6.11,16,21.26以外の導体2.
3,4.5〜27.28,29.30も永久磁石の小突
起d1の段差の部分に対向し、−ダする磁束が急変する
ので、この導体に於てもdφ ”7Tなる起電力が発生し、この起電力は上記の中性−
と対向している導体に発生している起電力と同じ方向で
あるから全部の起電力が互に加わシ出力電圧が増大する
ようになる利点がある。しかし永久磁石のme子巻機と
対向する面に突起を設けであるので、空隙の平均長が増
加したことになり電機子巻線と鎖交する磁束が減少する
ので、出力電圧の増加は平坦な永久磁石を備えた従来の
発電機に比し30嘩根度である。しかしながら制御回路
の味を改善するにtよ去きな効果がある。又、このよう
な突起を磁極り表面に設けることはプラスチックス磁石
等で容易に製造することができる。
Since the frequency generator of the present invention has the above-described configuration, the distribution of magnetic flux interlinking with the opposing power generation line elements is as shown in FIG. 3(b), and between the neutral lines n-1 and n-2, The magnetic flux is not uniform, and the magnetic flux is large in the part with the small protrusion d1, and the magnetic flux is less in the part d, where there is no protrusion, and there is a sudden change point in the magnetic flux where the magnetic flux increases or decreases at the same pitch as the pitch of the conductor of the power generation line element. is composed of δ
Therefore, in the generator with the configuration shown in Figure 3(a), the conductors that are useful for generating voltage due to the rotation of the permanent magnet are the conductors other than conductors 1, 6, 11, 16, and 21, 26 that face the neutral line. Conductor 2.
3, 4.5 - 27.28, 29.30 also face the step part of the small protrusion d1 of the permanent magnet, and the magnetic flux to -da changes suddenly, so an electromotive force of dφ "7T" is generated in this conductor as well. This electromotive force is the neutral −
Since the direction is the same as that of the electromotive force generated in the conductor facing the conductor, there is an advantage that all the electromotive forces are added together and the output voltage increases. However, since the protrusion is provided on the surface facing the permanent magnet me slave winder, the average length of the air gap increases and the magnetic flux interlinking with the armature winding decreases, so the increase in output voltage remains flat. This is 30 degrees stronger than conventional generators with permanent magnets. However, it has a significant effect on improving the taste of the control circuit. Moreover, providing such projections on the surface of the magnetic pole can be easily manufactured using a plastic magnet or the like.

本発明の第2の実施例に於ては第4図<&)に下すよう
に永久磁石9の磁極面は平坦に形成し、永久磁石9の電
機子巻線11と対向する面に、対向する発電線素と同じ
ピッチで磁極の1極について2n個の小突起Qを等しい
高さt、の鉄等の磁性材料を当接固着せしめる。
In the second embodiment of the present invention, the magnetic pole surface of the permanent magnet 9 is formed flat as shown in FIG. For each magnetic pole, 2n small protrusions Q are brought into contact with and fixed to a magnetic material such as iron with the same height t at the same pitch as the power generating line elements.

この実施例に於ては第3図(&)の実施例と同じように
永久磁石が回転することに依り対向する発電線素の中で
永久磁石の中性線と対向した導体のみでなく、他の導体
も永久磁石の表面に固着した磁性材料製の小突起と永久
磁石の表面との段差部に対向するので鎖交磁束が急変し
、起電力が発生し、かつ全部の導体に発生する起電力の
方向が閤じであるから互に加算されて出力が増加するよ
うになる。第4図(jL)に於ける実施例に於ても永久
磁石の対向面に小突起Qを設けた為に、平均空隙が増加
するので平均磁束が減少する結果、出力電圧の増加は約
30%程度である。
In this embodiment, as in the embodiment of FIG. Since the other conductors also face the step between the small protrusion made of magnetic material fixed to the surface of the permanent magnet and the surface of the permanent magnet, the interlinkage magnetic flux changes suddenly and an electromotive force is generated, which is generated in all the conductors. Since the directions of the electromotive forces are uniform, they are added together and the output increases. In the embodiment shown in Fig. 4 (jL), since the small protrusion Q is provided on the facing surface of the permanent magnet, the average gap increases and the average magnetic flux decreases, resulting in an increase in the output voltage of approximately 30 It is about %.

本発明の第30夾施例に於ては第5図(JL) 、 (
b)K示すように永久磁石9を着磁する際に使用−fる
着磁用ヨーク12に着磁電流を流す層f71i川尋体l
3を収容する#lSの外に、溝SとSとの閾に対向する
発電線素と同じピッチで永久磁石l極当り2n個の溝R
を一様な深さt、で設け、この溝Rには着磁用導体13
は設けず、との溝Sと@Rとを設けた面に着磁される水
久峨わ9の面を密着させて、着磁用導体13にtl!、
流を流して着磁せしめる。このようにずれば永久磁石9
に第5図(c)に示したような磁束分布となる層両を行
うことができる。
In the 30th embodiment of the present invention, FIG. 5 (JL), (
b) As shown in K, a layer used when magnetizing the permanent magnet 9 to flow a magnetizing current to the magnetizing yoke 12 f71i Kawahiro body l
In addition to #lS that accommodates #3, there are 2n grooves R per permanent magnet l pole with the same pitch as the generating line element facing the threshold between grooves S and S.
is provided with a uniform depth t, and a magnetizing conductor 13 is placed in this groove R.
is not provided, but the surface of the Mizuku wa 9 to be magnetized is brought into close contact with the surface provided with the grooves S and @R, and the magnetization conductor 13 is tl! ,
Let the current flow through it and magnetize it. If it shifts like this, the permanent magnet 9
In addition, it is possible to form a layer with a magnetic flux distribution as shown in FIG. 5(c).

Wks図(&) 、 (b)の実施例に於ては溝Rを設
けた部分では永久磁石9と着磁用ヨーク12との間に空
隙が生じ、着磁用導体13に着磁電流を流した時に溝R
が対向する永久磁石90部分の磁化力が減少する結果#
c5図(C)のような磁束分布となる。
In the embodiment shown in Figures (&) and (b), a gap is created between the permanent magnet 9 and the magnetizing yoke 12 in the part where the groove R is provided, and the magnetizing current is not applied to the magnetizing conductor 13. Groove R when flowing
The result is that the magnetizing force of the part of the permanent magnet 90 that faces decreases #
The magnetic flux distribution will be as shown in Figure c5 (C).

この実施例に於ては本発明の第1及び第2の実施例と同
じように発電線素の全導体が電圧発生に役立つので出力
電圧が加算され発生電圧を増大させる効果があシ、上記
第3図、第4図に示す他の実施例のように永久磁石に突
起を設けたプ他の磁性材料の突起を当接固着する等の別
の材料部品を必要としない利点がある。
In this embodiment, as in the first and second embodiments of the present invention, all the conductors of the power generating line element serve to generate voltage, so the output voltage is added and there is an effect of increasing the generated voltage. Unlike the other embodiments shown in FIGS. 3 and 4, there is an advantage that there is no need for a separate material component such as a permanent magnet provided with a protrusion or other material for abutting and fixing the protrusion of another magnetic material.

【図面の簡単な説明】 第1図(1)は周波数発電機を装着し九個平形電動機の
断面図、第1図(b)はその電機子巻線の説明用平面図
、第1図(c)はその回転子の永久磁石の着磁状11説
明図、第2図(a)は従来の周波数発電機の電機子巻線
と永久磁石の各磁極との相関関係を示す展開図、#!2
図(b)は永久磁石の磁束分布を直線形で示した説明図
、第3図(a)は本発明周波数発電機の電機子巻線と永
久磁石の各磁極との相関々係を示す展開図、第3図(b
)は永久磁石の磁束分布を直線形で示した説明図、第4
図−)は本発明の他の実施例に於ける電機子巻線と永久
磁石の各磁極との相関々係を示す展開図、第4図(b)
は永久磁石の磁束分布説明図、第5図(a)は本発明の
更に他の実施例に於ける永久磁石の着磁状態説明図、第
5図(b)はそり着磁用ヨークの平面図、第5図(e)
は永久磁石の磁束分布説明図である。 1・・・固定子ヨーク、2・・・ブラケット、3・・・
固定子巻線、4・・・絶縁板、5・・・軸受、6・・・
回転子細、・7・・・回転子のボス、8・・・回転子ヨ
ーク、9・・・永久磁石、10・・・空隙、11・・・
電機子巻線、11−1・・・発電線素、11−2・・・
外側の渡り線、11−3・・・内側のIltシ線、12
・・・着磁用ヨーク、13・・・着磁用導体、R,S・
・・溝、A、B・・・趨子、n−1〜n−6・・・中性
線、1〜30・・・導体、f・・・周波数、C・・・発
電線素の数、N・・・永久磁石の回転数、d、・・・小
突起、d!・・・突起のない部分、Q・・・小突起、t
・・・高さ、【、・・・高さ、t、・・・深さ。 +1 (0) (b) (C)
[Brief explanation of the drawings] Figure 1 (1) is a cross-sectional view of a nine-piece flat motor equipped with a frequency generator, Figure 1 (b) is a plan view for explaining its armature windings, and Figure 1 ( c) is an explanatory diagram of the magnetized state 11 of the permanent magnet of the rotor, and FIG. 2(a) is a developed diagram showing the correlation between the armature winding of a conventional frequency generator and each magnetic pole of the permanent magnet. ! 2
Figure (b) is an explanatory diagram showing the magnetic flux distribution of the permanent magnet in a linear form, and Figure 3 (a) is a development showing the correlation between the armature winding of the frequency generator of the present invention and each magnetic pole of the permanent magnet. Figure, Figure 3 (b
) is an explanatory diagram showing the magnetic flux distribution of a permanent magnet in a linear form.
Figure 4(b) is a developed view showing the relationship between the armature winding and each magnetic pole of the permanent magnet in another embodiment of the present invention.
5(a) is an explanatory diagram of the magnetic flux distribution of the permanent magnet, FIG. 5(a) is an explanatory diagram of the magnetized state of the permanent magnet in yet another embodiment of the present invention, and FIG. 5(b) is the plane of the warp magnetizing yoke. Figure, Figure 5(e)
is an explanatory diagram of magnetic flux distribution of a permanent magnet. 1... Stator yoke, 2... Bracket, 3...
Stator winding, 4... Insulating plate, 5... Bearing, 6...
Rotor thin, 7... Rotor boss, 8... Rotor yoke, 9... Permanent magnet, 10... Air gap, 11...
Armature winding, 11-1...Generating wire element, 11-2...
Outside crossover wire, 11-3...Inner Iltshi wire, 12
... Magnetizing yoke, 13... Magnetizing conductor, R, S.
...Groove, A, B...Trail, n-1 to n-6...Neutral wire, 1 to 30...Conductor, f...Frequency, C...Number of power generation line elements , N... Number of rotations of permanent magnet, d,... Small protrusion, d! ...Part without protrusion, Q...Small protrusion, t
...height, [, ...height, t, ...depth. +1 (0) (b) (C)

Claims (1)

【特許請求の範囲】 (11円周方向に勢ピッチでN極S極交互に合!rtP
極に着磁された永久磁石を回転子とし、はソ半径方向に
配設された(2n+1)xP本(但しn−1,2,3・
・・・・・・・・正の整数)の発電線素を直列に接続し
て成る電機子巻線を空隙を介して上記回転子と対向配設
し、この電機子巻線に回転子の回転速度に比例した周波
数の交流電圧を発生せしめるようにした周波数発電機に
於て、上記永久磁石の電機子巻線と対向する表面に、該
永久磁石の1極分について2n個の小突起を等ピッチで
かつ等しい高さで設けた事を特徴とする周波数発電機。 (2)上記小突起を永久磁石材料でない磁性材料を上記
永久磁石に当接して形成したことを特徴とする特許請求
の範囲第1項に記載の周波数発電機0 (3)  円周方向に等ピッチでN極S極交互に合計P
極に着磁された永久磁石を回転子とし、はy半径方向に
配設されA(Zn+))XP本(但しn=1.2.3・
・・・・・・・・正の整数)の発電線素を直列に接続し
て成る電機子巻線を空隙を介して上記回転子 −と対向
配設し、この電機子巻線に回転子の回転速度に比例した
周波数の交流電圧を発生せしめるようにし九周波数発電
機に於て、着磁電流を流す導体を収容する溝と溝との間
に1極分について2n個の導体を収容しない溝を等しい
ピッチでかつ等しい深さに設は九着磁ヨークにより着磁
した永久磁石を用いることをq#黴とする周波数発電機
[Claims] (11 Alternating north and south poles at pitches in the circumferential direction! rtP
The rotor is a permanent magnet magnetized to the poles, and (2n+1)xP pieces are arranged in the radial direction (however, n-1, 2, 3,
An armature winding consisting of power generation wire elements connected in series (a positive integer) is disposed opposite the rotor through a gap, and the rotor is connected to the armature winding. In a frequency generator that generates an alternating current voltage with a frequency proportional to the rotation speed, 2n small protrusions are provided for one pole of the permanent magnet on the surface of the permanent magnet facing the armature winding. A frequency generator characterized by being installed at equal pitches and at equal heights. (2) The frequency generator according to claim 1, wherein the small protrusions are formed by a magnetic material other than a permanent magnet material being brought into contact with the permanent magnet. Pitch alternates between north and south poles, total P
A permanent magnet with magnetized poles is used as a rotor, and A(Zn+))XP pieces are arranged in the y radial direction (where n=1.2.3.
An armature winding consisting of power generation wire elements of . In a nine-frequency generator that generates an alternating current voltage with a frequency proportional to the rotational speed of the generator, 2n conductors for one pole are not accommodated between the grooves that accommodate the conductors through which the magnetizing current flows. A frequency generator that uses permanent magnets magnetized by nine magnetized yokes with grooves arranged at equal pitches and equal depths.
JP7817782A 1982-05-12 1982-05-12 Frequency generator Pending JPS58198156A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7817782A JPS58198156A (en) 1982-05-12 1982-05-12 Frequency generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7817782A JPS58198156A (en) 1982-05-12 1982-05-12 Frequency generator

Publications (1)

Publication Number Publication Date
JPS58198156A true JPS58198156A (en) 1983-11-18

Family

ID=13654676

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7817782A Pending JPS58198156A (en) 1982-05-12 1982-05-12 Frequency generator

Country Status (1)

Country Link
JP (1) JPS58198156A (en)

Citations (1)

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

Patent Citations (1)

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

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