JPH0152987B2 - - Google Patents

Info

Publication number
JPH0152987B2
JPH0152987B2 JP6580383A JP6580383A JPH0152987B2 JP H0152987 B2 JPH0152987 B2 JP H0152987B2 JP 6580383 A JP6580383 A JP 6580383A JP 6580383 A JP6580383 A JP 6580383A JP H0152987 B2 JPH0152987 B2 JP H0152987B2
Authority
JP
Japan
Prior art keywords
coil
coils
cancel
generating
section
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
Application number
JP6580383A
Other languages
Japanese (ja)
Other versions
JPS59191464A (en
Inventor
Seishi Myazaki
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 Instruments Corp
Original Assignee
Sankyo Seiki Manufacturing 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 Sankyo Seiki Manufacturing Co Ltd filed Critical Sankyo Seiki Manufacturing Co Ltd
Priority to JP6580383A priority Critical patent/JPS59191464A/en
Publication of JPS59191464A publication Critical patent/JPS59191464A/en
Publication of JPH0152987B2 publication Critical patent/JPH0152987B2/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

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Permanent Magnet Type Synchronous Machine (AREA)

Description

【発明の詳細な説明】 本発明は例えば電動機の回転速度に比例した周
波数(またはパルス数)の信号を得る周波数発電
機のコイルパターンに関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a coil pattern for a frequency generator that obtains a signal with a frequency (or number of pulses) proportional to the rotational speed of an electric motor, for example.

一般に、周波数発電機を電動機内に組込んで、
この周波数発電機からの周波数信号によつて、速
度制御を行なわす場合、制御特性を良好にし、周
囲温度による影響を受けにくいなどのメリツトが
ある反面、周波数信号の検出誤差は電動機の回転
むらとなつて現われ、多大の支障をきたすことに
なる。特に、磁気変化形周波数発電方式では電動
機からの磁界及びトランスなどの外部からの磁界
による磁気誘導ノイズが問題となる。
Generally, a frequency generator is built into the electric motor,
When speed control is performed using the frequency signal from this frequency generator, there are advantages such as good control characteristics and less influence by ambient temperature. It will appear over time and cause a lot of trouble. In particular, in the magnetically variable frequency power generation system, magnetic induction noise due to the magnetic field from the motor and the magnetic field from outside such as a transformer becomes a problem.

第1図に従来例の周波数発電機の固定子部を示
す。この場合、絶縁基板A上には、発電コイル1
が囲む面積に鎖交する誘導ノイズ磁束を打消すた
めに、該発電コイル1の両端から逆方向に誘導ノ
イズ除去コイル2を設けている。
FIG. 1 shows the stator section of a conventional frequency generator. In this case, the power generating coil 1 is placed on the insulating substrate A.
In order to cancel the induced noise magnetic flux that intersects with the area surrounded by the power generating coil 1, an induced noise eliminating coil 2 is provided in the opposite direction from both ends of the power generating coil 1.

しかし、このような構成でも発電コイル1と誘
導ノイズ除去コイル2とで囲まれる面積に鎖交す
る誘導ノイズ磁束を打消すことができない。その
結果、周波数信号の発生電圧が少ない場合、上記
の誘導ノイズ磁束による誘導ノイズ電圧は電動機
の回転精度に悪影響を及ぼすことになる。
However, even with such a configuration, the induced noise magnetic flux interlinking with the area surrounded by the power generation coil 1 and the induced noise removal coil 2 cannot be canceled. As a result, if the generated voltage of the frequency signal is small, the induced noise voltage due to the above-mentioned induced noise magnetic flux will have a negative effect on the rotation accuracy of the motor.

この欠点を除くべく、第3図に示すレイアウト
が提案されている。この例では、発電コイル2に
よつて囲まれる面積に鎖交する誘導ノイズ磁束を
打消すために、第1誘導ノイズ除去コイル4、第
2誘導ノイズ除去コイル5を設け、さらに発電コ
イル3と、この発電コイル3の外周部に設ける第
1誘導ノイズ除去コイル4とで囲まれる面積に鎖
交する誘導ノイズ磁束と、発電コイル3と、この
発電コイル3の内周部に設ける第2誘導ノイズ除
去コイル5とで囲まれる面積に鎖交する誘導ノイ
ズ磁束とが打消し合うように第1誘導ノイズ除去
コイル4、発電コイル3、第2誘導ノイズ除去コ
イル5をこれらの順に直列接続している。
In order to eliminate this drawback, a layout shown in FIG. 3 has been proposed. In this example, in order to cancel the induced noise magnetic flux that intersects with the area surrounded by the generating coil 2, a first inductive noise removal coil 4 and a second inductive noise removing coil 5 are provided, and furthermore, the generating coil 3 and the second inductive noise removing coil 5 are provided. The induced noise magnetic flux that intersects with the area surrounded by the first induction noise removal coil 4 provided on the outer periphery of the power generation coil 3, and the second induction noise removal provided in the inner periphery of the power generation coil 3 and the power generation coil 3. The first induction noise removal coil 4, the power generation coil 3, and the second induction noise removal coil 5 are connected in series in this order so that the induction noise magnetic flux interlinking with the area surrounded by the coil 5 cancels each other out.

すなわち、この例では、1つの円を2分し、
180゜ずつ位相の異なる検出電圧を逆相に接続して
位相を検出し、コイル面の全面を通過する磁界の
変化に対してこれをキヤンセルする方式を採つて
いる。しかし、この例においても、発電コイル3
に対する発電ロータに回転中心或いは同心円から
磁気的にずれた磁路が形成された場合には、キヤ
ンセル用のコイルが180゜毎に分割されているの
で、1回転に1回の検出むらとなり、エラー成分
が生じ易いという問題がある。
In other words, in this example, one circle is divided into two,
A method is adopted in which the phase is detected by connecting detection voltages with phases different by 180 degrees in opposite phases, and this is canceled against changes in the magnetic field that passes across the entire surface of the coil. However, in this example as well, the generator coil 3
If a magnetic path is formed in the power generation rotor that is magnetically deviated from the center of rotation or concentric circles, the cancel coil is divided into 180° sections, resulting in detection irregularities once per rotation, resulting in errors. There is a problem that components are easily generated.

本発明は、これら従来技術における欠点や問題
点に着目してなされたもので、発電コイル全体を
通過する磁界の変化に対してもキヤンセルする効
果をもち、且つ、1回転に1回のエラー成分も出
にくい構成の周波数発電器を提供することを目的
とする。
The present invention has been made by focusing on these drawbacks and problems in the conventional technology, and has the effect of canceling changes in the magnetic field that passes through the entire generating coil, and also cancels the error component once per rotation. The purpose of the present invention is to provide a frequency generator with a configuration that makes it difficult to generate.

本発明の構成を、以下、一実施例に基づいて説
明する。
The configuration of the present invention will be described below based on one embodiment.

第3図は本発明の原理的な構成を示しており、
このコイルパターンでは、発電機用ロータマグネ
ツトの極数はいくつであつても適用できる。な
お、図中、仮想線領域のN.S表示はマグネツト移
動子の磁極を示す。又、符号6で示す区間は、1
回転エンコーダの場合は360゜を、リニアスケール
物ではスタート点7からエンド点8までに対応す
る。
FIG. 3 shows the basic configuration of the present invention,
This coil pattern can be applied to any number of poles in the generator rotor magnet. Note that in the figure, the NS symbol in the virtual line area indicates the magnetic pole of the magnetic slider. Also, the section indicated by code 6 is 1
In the case of a rotary encoder, it corresponds to 360°, and in the case of a linear scale, it corresponds to from the start point 7 to the end point 8.

このコイルパターンはa部からb部までと、b
部からc部までの2つのブロツクから成り、これ
ら各々のループは逆方向のループとして形成され
且つ、直列に接続されている。
This coil pattern is from part a to part b,
It consists of two blocks from section c to section c, each of which is formed as a loop in the opposite direction and connected in series.

又、a部からb部に至るループで囲まれる面積
と、b部からc部に至るループで囲まれる面積を
ほぼ等しく設定するとともに、a部からb部に至
るコイル区間及びc部からb部に至るコイル区間
をほぼ、区間6若しくはスタート点7からエンド
点8までの区間に対応させてある。
In addition, the area surrounded by the loop from part a to part b and the area surrounded by the loop from part b to part c are set to be approximately equal, and the coil section from part a to b and from part c to b are set to be approximately equal. The coil section up to approximately corresponds to the section 6 or the section from the start point 7 to the end point 8.

図において、c部からe部までの区間を第1の
発電コイル、b部からd部までの区間を第2の発
電コイル、e部からb部までの区間を第1のキヤ
ンセルコイル、a部からd部までの区間を第2の
キヤンセルコイルとすれば、第1、第2の各発電
コイルは後述のマグネツト移動子たる周波数発電
機用ロータ11(第5図参照)に面対向してこの
ロータ11の磁極(N.S)間隔とほぼ等しいピツ
チの矩形状に形成されている。
In the figure, the section from c to e is the first generating coil, the section from b to d is the second generating coil, the section from e to b is the first cancel coil, and the section a is the second generating coil. If the section from to part d is used as a second cancel coil, each of the first and second power generation coils faces a frequency generator rotor 11 (see Fig. 5), which is a magnet mover, which will be described later. It is formed into a rectangular shape with a pitch approximately equal to the magnetic pole (NS) spacing of the rotor 11.

そして、これら両発電コイルはクランク状に曲
折して互いに入り込ませてこの2つの発電コイル
の線素を同一の磁気信号が感磁できる位置に形成
されており、2本が近接した平行線として配置さ
れている。また、これら両発電コイルの全域の両
側には、第1及び第2のキヤンセルコイルが各1
本ずつ並設されており、第1の発電コイル→第1
のキヤンセルコイル→第2の発電コイル→第2の
キヤンセルコイルというように第1及び第2の発
電コイル同士を電気的に同相に、第1及び第2の
キヤンセルコイル同士を電気的に逆相になるよう
に交互に直列接続されている。
These two generating coils are bent into a crank shape and inserted into each other, so that the wire elements of the two generating coils are formed in a position where the same magnetic signal can be sensed, and the two are arranged as parallel lines close to each other. has been done. Furthermore, on both sides of the entire area of both of these generating coils, there are one first and second cancel coil.
They are arranged side by side, with the first generating coil → the first generating coil.
cancel coil → second generator coil → second cancel coil, so that the first and second generator coils are electrically in phase with each other, and the first and second cancel coils are electrically in opposite phase with each other. They are connected alternately in series so that

この結果、第1の発電コイルと第1のキヤンセ
ルコイルとにより1相分の閉ループが形成され、
第2の発電コイルと第2のキヤンセルコイルとに
より2相分の閉ループが形成され、且つ、両閉ル
ープは互いに逆相(電気的に180゜の位相差)に形
成される。
As a result, a closed loop for one phase is formed by the first power generation coil and the first cancel coil,
A closed loop for two phases is formed by the second power generation coil and the second cancel coil, and both closed loops are formed in opposite phases (electrical phase difference of 180°).

そして、これら第1及び第2の各発電コイルか
らは、周知の発電原理に従い、多極着磁された発
電機用ロータの磁極による交番磁界が矩形波状の
発電コイルの発電作用導体部分を横切るごとに発
電を行なう。このとき、第1及び第2の各発電コ
イルの2本が近接している平行線であり且つ、直
列に接続されているので、これらの発電コイルか
らは従来例のものと比較して2倍の発電電圧が得
られる。
According to the well-known power generation principle, each of the first and second power generation coils generates an alternating magnetic field generated by the magnetic poles of the multi-pole magnetized generator rotor as it crosses the power generation conductor portion of the rectangular waveform power generation coil. will generate electricity. At this time, since the first and second power generating coils are parallel lines that are close to each other and are connected in series, the power from these power generating coils is twice that of the conventional example. The generated voltage can be obtained.

図の構成部分に、発電機用ロータ以外の外部か
ら誘導ノイズ磁束が鎖交した場合は、上記1相分
の閉ループと上記2相分の閉ループの面積が等し
く且つ、互いに逆相であるので互いに打消し合う
様に作用する。従つて、例え、誘導ノイズ磁束が
部分的にむらを生じたとしても全域にわたり同面
積であるので、これに起因して検出むらを生ずる
ことはない。
If induced noise magnetic flux is linked to the component shown in the figure from outside other than the generator rotor, the areas of the closed loop for one phase and the closed loop for two phases are equal and opposite to each other, so they are mutually connected. They act to cancel each other out. Therefore, even if the induced noise magnetic flux is partially uneven, since the area is the same over the entire area, this will not cause detection unevenness.

なお、上記第1、第2の各発電コイル及び第
1、第2の各キヤンセルコイルは、絶縁基板の片
面にプリント配線技術で形成される。
The first and second power generation coils and the first and second cancel coils are formed on one side of the insulating substrate by printed wiring technology.

又、磁性鉄板に絶縁層を設け、この絶縁層の表
面に両コイルを形成してもよく、この場合はロー
タとの間に磁気的閉ループが形成され、効率が一
層向上する。
Alternatively, an insulating layer may be provided on the magnetic iron plate, and both coils may be formed on the surface of this insulating layer. In this case, a magnetic closed loop is formed with the rotor, further improving efficiency.

第3図に示す構成を絶縁基板たる円板8上に形
成したのが第4図に示す例である。
The example shown in FIG. 4 is an example in which the structure shown in FIG. 3 is formed on a disk 8, which is an insulating substrate.

第4図における符号a′,b′,c′,d′,e′は第3
図における符号a,b,c,d,eに各々対応す
る。
The symbols a′, b′, c′, d′, and e′ in Fig. 4 are the third
They correspond to symbols a, b, c, d, and e in the figure, respectively.

そしてさらに、この第4図に示す構成をブラシ
レスモータに適用したのが第5図に示す例であ
る。
Furthermore, the example shown in FIG. 5 is an example in which the configuration shown in FIG. 4 is applied to a brushless motor.

本発明に係るコイルパターンを形成された円板
8は、基板9に固定されたホルダー10に装着さ
れており、その対向部には周波数発電機用ロータ
11が位置している。
A disk 8 on which a coil pattern according to the present invention is formed is attached to a holder 10 fixed to a substrate 9, and a frequency generator rotor 11 is positioned opposite to the holder 10.

当該ブラシレスモータの基本構成は周知である
ので以下、各部材名称を列記すれば次の通りであ
る。
Since the basic configuration of the brushless motor is well known, the names of each component will be listed below.

符号12は軸受、符号13は回転軸、符号14
はボス、符号15はロータヨーク、符号16はロ
ータマグネツト、符号17はステータコア、符号
18は駆動コイルを各々示す。
Reference numeral 12 is a bearing, reference numeral 13 is a rotating shaft, reference numeral 14
15 is a boss, 15 is a rotor yoke, 16 is a rotor magnet, 17 is a stator core, and 18 is a drive coil.

本発明によれば、既に述べたように、発電コイ
ルを第1及び第2の発電コイルを互いに入り込ま
せこの2つの発電コイルの線素をマグネツト移動
子の同一の磁気信号を感磁できる位置に近接配置
し、第1の発電コイルと第2の発電コイルを同相
となるように直列接続して近接したことから、各
2線素には同一の発電電圧が発生されるので、こ
の発電コイルからは従来のものと比較して2倍の
発電電圧が得られる。また、第1及び第2のキヤ
ンセルコイルを各々第1及び第2の発電コイルの
全域両側に並設し、第1及び第2のキヤンセルコ
イル同士を電気的に逆相に直列接続しているの
で、キヤンセルコイルに生ずる誘導ノイズは逆相
で加算されることから打消され、誘導磁界による
影響は全くなくなると共に、第1の発電コイルと
第1のキヤンセルコイルからなる第1のループ
と、第2の発電コイルと第2のキヤンセルコイル
からなる第2のループとは逆位相のループになる
ように直列接続されるため、外部ノイズによる影
響が全くなくなる上に、上記に述べたとおり、2
倍の発電電圧が得られることから、S/N比の非
常に高い優れた周波数発電機が得られるという本
願発明特有の効果を奏する。さらに、コイルパタ
ーンが片面に形成されるので、量産しやすく、高
性能なエンコーダを安価に且つ高い信頼性で製造
することが可能である。
According to the present invention, as described above, the first and second generating coils are inserted into each other, and the wire elements of the two generating coils are placed in a position where they can be sensitive to the same magnetic signal of the magnet mover. Since the first generating coil and the second generating coil are connected in series and close to each other so that they are in the same phase, the same generated voltage is generated in each two wire element. The generated voltage can be doubled compared to the conventional one. In addition, the first and second cancel coils are arranged in parallel on both sides of the entire area of the first and second generating coils, and the first and second cancel coils are electrically connected in series with opposite phases. , the induced noise generated in the cancel coil is canceled out because it is added in reverse phase, and the influence of the induced magnetic field is completely eliminated. Since the second loop consisting of the generator coil and the second cancel coil is connected in series so that the loop is in opposite phase, there is no influence from external noise, and as mentioned above,
Since twice the generated voltage can be obtained, an effect unique to the present invention is achieved in that an excellent frequency generator with an extremely high S/N ratio can be obtained. Furthermore, since the coil pattern is formed on one side, mass production is easy, and high performance encoders can be manufactured at low cost and with high reliability.

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

第1図、第2図は各々従来技術に係る周波数発
電機の固定子部の正面図、第3図は本発明に係る
周波数発電機の固定子部の原理的な説明図、第4
図は本発明の一実施例として円板上に形成した周
波数発電機の固定子部の正面図、第5図は同上図
の固定子部を使用したブラシレスモータの断面図
である。 11……(マグネツト移動子としての)周波数
発電機用ロータ、c部〜e部、c′部〜e′部……第
1の発電コイル、b部〜d部、b′部〜d′部……第
2の発電コイル、e部〜b部、e′部〜b′部……第
1のキヤンセルコイル、a部〜d部、a′部〜d′部
……第2のキヤンセルコイル。
1 and 2 are front views of a stator section of a frequency generator according to the prior art, FIG. 3 is a principle explanatory diagram of a stator section of a frequency generator according to the present invention, and FIG.
The figure is a front view of a stator section of a frequency generator formed on a disk as an embodiment of the present invention, and FIG. 5 is a sectional view of a brushless motor using the stator section of the same figure. 11...Rotor for frequency generator (as a magnet mover), parts c to e, parts c' to e'...first generating coil, parts b to d, parts b' to d' . . . Second generating coil, e section to b section, e' section to b' section... First cancel coil, a section to d section, a' section to d' section... second cancel coil.

Claims (1)

【特許請求の範囲】[Claims] 1 複数の磁極が着磁されたマグネツト移動子に
面対向して所定ピツチの第1及び第2の発電コイ
ルを互いに入り込ませてこの2つの発電コイルの
線素を上記マグネツト移動子の同一の磁気信号が
感磁できる位置に近接配置すると共に、これらの
第1及び第2の各発電コイルの全域両側に第1及
び第2のキヤンセルコイルを各々並設し、これら
の第1及び第2のキヤンセルコイル同士を電気的
に逆相に、上記第1及び第2の発電コイル同士を
電気的に同相にかつ、第1及び第2のキヤンセル
コイルと上記第1及び第2の発電コイルを交互に
直列接続したことを特徴とする周波数発電機のコ
イルパターン。
1. A plurality of magnetic poles are placed face-to-face on a magnetized mover, and the first and second power generation coils are inserted at a predetermined pitch into each other, and the wire elements of these two power generation coils are connected to the same magnetism of the magnet mover. The first and second cancel coils are arranged in close proximity to a position where the signal can be magnetically sensitive, and the first and second cancel coils are arranged in parallel on both sides of the entire area of each of the first and second generating coils, and the first and second cancel coils The coils are electrically in opposite phases, the first and second generating coils are electrically in phase, and the first and second cancel coils and the first and second generating coils are alternately connected in series. A coil pattern of a frequency generator characterized by connected.
JP6580383A 1983-04-14 1983-04-14 Coil pattern of frequency generator Granted JPS59191464A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6580383A JPS59191464A (en) 1983-04-14 1983-04-14 Coil pattern of frequency generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6580383A JPS59191464A (en) 1983-04-14 1983-04-14 Coil pattern of frequency generator

Publications (2)

Publication Number Publication Date
JPS59191464A JPS59191464A (en) 1984-10-30
JPH0152987B2 true JPH0152987B2 (en) 1989-11-10

Family

ID=13297548

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6580383A Granted JPS59191464A (en) 1983-04-14 1983-04-14 Coil pattern of frequency generator

Country Status (1)

Country Link
JP (1) JPS59191464A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61277354A (en) * 1985-05-31 1986-12-08 Sony Corp Flat type motor with frequency generator

Also Published As

Publication number Publication date
JPS59191464A (en) 1984-10-30

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