JP3013605B2 - Skew method of magnetic resolver - Google Patents

Skew method of magnetic resolver

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Publication number
JP3013605B2
JP3013605B2 JP4145029A JP14502992A JP3013605B2 JP 3013605 B2 JP3013605 B2 JP 3013605B2 JP 4145029 A JP4145029 A JP 4145029A JP 14502992 A JP14502992 A JP 14502992A JP 3013605 B2 JP3013605 B2 JP 3013605B2
Authority
JP
Japan
Prior art keywords
magnetic
skew
resolver
stator core
key
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 - Fee Related
Application number
JP4145029A
Other languages
Japanese (ja)
Other versions
JPH05312590A (en
Inventor
豊 前田
洋 中川
Original Assignee
神鋼電機株式会社
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 神鋼電機株式会社 filed Critical 神鋼電機株式会社
Priority to JP4145029A priority Critical patent/JP3013605B2/en
Publication of JPH05312590A publication Critical patent/JPH05312590A/en
Application granted granted Critical
Publication of JP3013605B2 publication Critical patent/JP3013605B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は,ダイレクト・モ−タ等
の例えば回転制御に用いられる高分解能センサ−として
の磁気レゾルバ−のスキュ−方法に関し,特にスキュ−
効果の高い,かつ,組み立て容易なスキュ−方法に関す
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a skewing method for a magnetic resolver as a high-resolution sensor used for, for example, rotation control of a direct motor or the like, and more particularly to a skew method.
The present invention relates to a skewing method that is highly effective and easy to assemble.

【0002】[0002]

【従来の技術】従来,磁気レゾルバ−の回転中にステ−
タコアとロ−タコアとのギャツプ間に磁束密度変化(パ
−ミアンス変化)が通常発生するので,磁気レゾルバ−
からの出力正弦波が歪み,それによって例えば回転制御
等が正確に出来なくなってしまう。そこで歪みの無い正
弦波に近づけるために所謂スキュ−方法が一般に用いら
れている。即ち,磁束密度変化に基づく高調波発生によ
る正弦波の歪みを防ぐために従来種々のスキュ−方法が
行なわれている。図4乃至図6に示すものは,従来のス
キュ−方法の1例を示すものであって,図4はロ−タコ
ア1の磁極ピッチPをステ−タコア2の磁極ピッチPS
よりも大きく(または小さく)設定することにより等価
的にスキュ−を行う等価ピッチスキュ−方法である。ま
た,図5はロ−タコア1及びステ−タコア2のそれぞれ
の磁極ピッチPは同じであるが,図6に示すようにステ
−タコア2をロ−タコア1に対して斜めに傾斜して構成
された斜めスキュ−方法である。
2. Description of the Related Art Conventionally, when a magnetic resolver is rotating, a stay is stopped.
A magnetic flux density change (permeance change) usually occurs between the gap between the rotor core and the rotor core.
The output sine wave is distorted, which makes it impossible to perform, for example, rotation control accurately. Therefore, a so-called skew method is generally used to approximate a sine wave without distortion. That is, various skew methods have been conventionally used to prevent sine wave distortion due to generation of harmonics based on magnetic flux density change. 4 to 6 show an example of a conventional skew method. FIG. 4 shows the magnetic pole pitch P of the rotor core 1 as the magnetic pole pitch P S of the stator core 2.
This is an equivalent pitch skew method in which a skew is equivalently performed by setting a value larger (or smaller). FIG. 5 shows that the rotor core 1 and the stator core 2 have the same magnetic pole pitch P, but the stator core 2 is obliquely inclined with respect to the rotor core 1 as shown in FIG. Oblique skew method.

【0003】[0003]

【発明が解決しようとする課題】図4に示すような等価
ピッチスキュ−方法では,磁極ピッチがステ−タコアと
ロ−タコアとで相違するので,その磁極数(歯数)が少
ない場合にはスキュ−効果が不十分となる不都合があっ
た。また,図5及び図6に示すような斜めスキュ−方法
では,キ−溝を斜めに加工することが困難であり,ま
た,治具を使用する必要があり,さらにキ−溝による磁
気抵抗のアンバランスを生じる等の不都合があった。
In the equivalent pitch skew method shown in FIG. 4, since the magnetic pole pitch differs between the stator core and the rotor core, when the number of magnetic poles (the number of teeth) is small, the skew is increased. -There was a disadvantage that the effect was insufficient. In the oblique skew method as shown in FIGS. 5 and 6, it is difficult to machine the key groove obliquely, and it is necessary to use a jig. There were inconveniences such as unbalance.

【0004】[0004]

【課題を解決するための手段】本発明は,磁気レゾルバ
−のステ−タコア及びロ−タコアが複数の薄い磁性板の
積層体で構成される場合に,その積層体を構成する磁性
板のそれぞれ1枚1枚に複数のキ−溝を所定間隔θで設
け,その磁性板を1枚づつ積層する度にそのキ−溝をず
らしながら積み重ねるように構成した。
SUMMARY OF THE INVENTION In the present invention, when the stator core and the rotor core of a magnetic resolver are constituted by a laminate of a plurality of thin magnetic plates, each of the magnetic plates constituting the laminate is provided. A plurality of key grooves are provided on each sheet at a predetermined interval θ, and each time the magnetic plates are stacked one by one, the key grooves are shifted while being stacked.

【0005】[0005]

【作用】本発明のものでは,鉄心を積層するとき,キ−
溝をずらして積層していくだけで所定のスキュ−角度S
を得ることができ,また,そのようなスキュ−溝を有し
たステ−タコアまたはロ−タコアの製作が容易に行うこ
とができる。
According to the present invention, when the iron core is laminated, the key is
A predetermined skew angle S can be obtained simply by shifting the groove and stacking.
Can be obtained, and a stator core or a rotor core having such a skew groove can be easily manufactured.

【0006】[0006]

【実施例】以下,図1乃至図3に示した各実施例により
本発明を具体的に説明する。 第1の実施例:図1は本発明の第1の実施例を示もの
で,同実施例の磁気レゾルバ−において,ロ−タコア3
の内側にはステ−タコア4が配置されており,ステ−タ
コア4には例えば16個の磁極4A,4B,4C,・・
・4O,及び4Pのが設けられている。各磁極にはそれ
ぞれ磁極コイル(図示を省略)が設けられている。この
場合,各磁極はリニアパルスモ−タの構造と同様に順に
A,B,−A,−B,A,B,−A,・・・の等間隔極
配列となっている。各磁極には,磁極と反対側(内部
側)にそれぞれ1個のキ−溝5A,5B,5C・・・5
Pが合計16個設けられている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, the present invention will be described in detail with reference to the embodiments shown in FIGS. FIG. 1 shows a first embodiment of the present invention. In the magnetic resolver of the embodiment, a rotor core 3 is used.
A stator core 4 is disposed inside the stator core 4. The stator core 4 has, for example, 16 magnetic poles 4A, 4B, 4C,.
・ 4O and 4P are provided. Each magnetic pole is provided with a magnetic pole coil (not shown). In this case, each magnetic pole has an equally spaced pole array of A, B, -A, -B, A, B, -A,... Similarly to the structure of the linear pulse motor. Each of the magnetic poles has one key groove 5A, 5B, 5C,.
A total of 16 Ps are provided.

【0007】ステ−タコア4の円周上に等間隔に配置さ
れた16個のキ−溝の間隔,即ちキ−溝角度θは,一般
式で(1)式で表される。 θ=(360°/K)±(S/K)・・・・・・・・(1) ここで,Kはキ−溝の数,Sはスキュ−角度(S=P/
N),Pは磁極ピッチで,P=360°/Kとなり,ま
たNは歪みの原因となる高調波次数に対応して設定され
る整数である。この第1の実施例においては,K=1
6,P=360°/16=22.5,N=3に設定され
ているので,上記キ−溝角度θは,(2)式となる。 θ=22.5±0.47・・・・・・・・(2) ここで,キ−溝数Kは磁極数と同数である。また,整数
Nは通常3程度が望ましい。
The interval between 16 key grooves arranged at equal intervals on the circumference of the stator core 4, that is, the key groove angle θ is expressed by the general formula (1). θ = (360 ° / K) ± (S / K) (1) where K is the number of key grooves and S is the skew angle (S = P /
N) and P are magnetic pole pitches, P = 360 ° / K, and N is an integer set corresponding to the harmonic order causing distortion. In this first embodiment, K = 1
6, P = 360 ° / 16 = 22.5 and N = 3, the key groove angle θ is given by the following equation (2). θ = 22.5 ± 0.47 (2) Here, the number of key grooves K is the same as the number of magnetic poles. The integer N is usually desirably about 3.

【0008】図2は,第1の実施例におけるステ−タコ
ア4を構成する複数の磁性板の積み重ね方法を説明する
ための図で,同一のキ−溝が形成された同一形状の各磁
性板(合計16枚)を,キ−溝(5A,5B,5C・・
・5P)の幅だけずらしながら一枚づつ積み重ねて行く
と図2のように全体として斜めに積み重ねられたステ−
タコア4が形成され得る。この時,傾斜の度合がスキュ
−角度Sで表されるが,この実施例の場合N=3である
から,スキュ−角度Sは磁極ピッチPの1/3となる。
FIG. 2 is a view for explaining a method of stacking a plurality of magnetic plates constituting the stator core 4 in the first embodiment. Each magnetic plate having the same shape and having the same key groove is formed. (16 sheets in total) with key grooves (5A, 5B, 5C ...
When the sheets are stacked one by one while being shifted by the width of 5P), the stays stacked obliquely as a whole as shown in FIG.
Tacos 4 can be formed. At this time, the degree of the inclination is represented by the skew angle S. In this embodiment, since N = 3, the skew angle S is 1 / of the magnetic pole pitch P.

【0009】第2の実施例:図3は,本発明の第2の実
施例を示すもので,第1の実施例と相違するのはキ−溝
がロ−タコア3側に設けられている点であり,キ−溝角
度θが各キ−溝ごとにずれて構成されている点である。
この実施例の場合にはキ−溝を磁極に対応させて配置す
る必要がなく,従って磁極数よりも多くのキ−溝を設け
られる点に特長がある。このため,高調波の打ち消し度
合が滑らかとなりスキュ−効果が一層高いものとなる。
Second Embodiment FIG. 3 shows a second embodiment of the present invention. The difference from the first embodiment is that a key groove is provided on the rotor core 3 side. And the key groove angle θ is shifted for each key groove.
In the case of this embodiment, it is not necessary to arrange the key grooves corresponding to the magnetic poles, and therefore, it is characterized in that more key grooves can be provided than the number of magnetic poles. For this reason, the degree of cancellation of harmonics is smooth, and the skew effect is further enhanced.

【0010】[0010]

【発明の効果】本発明は上記のように磁気レゾルバ−の
ロ−タコア側またはステ−タコア側に,磁極数と対応し
てキ−溝を多数個設けることが出来るので,極めて高い
スキュ−効果が得られるのみならず,このようなスキュ
−溝を備えたステ−タコアまたはロ−タコアの容易な組
み立てが達成できるという優れた効果を有する。とく
に,ロ−タコア側にキ−溝を設ける場合は,高調波の打
ち消し度合いがさらに円滑となる点で優れている。
According to the present invention, since a large number of key grooves can be provided on the rotor core side or the stator core side of the magnetic resolver in accordance with the number of magnetic poles as described above, an extremely high skew effect can be obtained. Not only can be obtained, but also the stator core or rotor core having such a skew groove can be easily assembled. In particular, when a key groove is provided on the rotor core side, it is excellent in that the degree of cancellation of harmonics is further smoothed.

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

【図1】本発明の第1の実施例を示すステ−タコア側に
設けられたキ−溝の配列構成を示す平面図である。
FIG. 1 is a plan view showing an arrangement of key grooves provided on a stator core side according to a first embodiment of the present invention.

【図2】図1に示すステ−タコアの積み重ね方法を説明
するための要部側面図である。
FIG. 2 is a main part side view for explaining a method of stacking the stator core shown in FIG. 1;

【図3】本発明の第2の実施例を示すロ−タコア及びス
テ−タコアの平面図である。
FIG. 3 is a plan view of a rotor core and a stator core showing a second embodiment of the present invention.

【図4】従来の磁気レゾルバ−のスキュ−方法の第1例
を説明するための図である。
FIG. 4 is a view for explaining a first example of a conventional magnetic resolver skew method.

【図5】従来の磁気レゾルバ−のスキュ−方法の第2例
を説明するための図である。
FIG. 5 is a view for explaining a second example of the conventional magnetic resolver skew method.

【図6】従来の磁気レゾルバ−のスキュ−方法の第2例
を補足説明するための図である。
FIG. 6 is a diagram for supplementarily explaining a second example of a conventional magnetic resolver skew method.

【符号の説明】[Explanation of symbols]

3:ロ−タコア 4:ステ−タコア 4A〜4P:磁極 5A〜5P:キ−溝 3: rotor core 4: stator core 4A to 4P: magnetic pole 5A to 5P: key groove

───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.7,DB名) G01D 5/00 - 5/252 G01D 5/39 G01B 7/00 - 7/34 ──────────────────────────────────────────────────続 き Continued on the front page (58) Fields investigated (Int. Cl. 7 , DB name) G01D 5/00-5/252 G01D 5/39 G01B 7/00-7/34

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 磁気レゾルバ−のステ−タコア及びロ−
タコアが複数の薄い磁性板の積層体で構成される磁気レ
ゾルバ−のスキュ−方法において,該磁気レゾルバ−の
ロ−タコアまたはステ−タコアの磁性板において,複数
のキ−溝が数式 θ=(360°/K)±(S/K)度
で表されるキ−溝角度θの間隔で設けられており,か
つ,前記各磁性板を積層する際に前記キ−溝をずらしな
がら積み重ねることによりスキュ−角度Sを得るように
したことを特徴とする磁気レゾルバ−のスキュ−方法。
但し,S=P/N,Pは磁極ピッチ,Nは整数,Kはキ
−溝数,Sはスキュ−角とする。
A stator and a rotor of a magnetic resolver.
In a skewing method of a magnetic resolver in which a core is composed of a laminate of a plurality of thin magnetic plates, a plurality of key grooves in a rotor core of the magnetic resolver or a magnetic plate of a stator core are represented by the formula θ = ( 360 ° / K) ± (S / K) degrees are provided at intervals of a key groove angle θ, and when the magnetic plates are stacked, they are stacked while shifting the key grooves. A skewing method for a magnetic resolver, wherein a skew angle S is obtained.
Here, S = P / N, P is the magnetic pole pitch, N is an integer, K is the number of key grooves, and S is the skew angle.
【請求項2】 請求項1のスキュ−方法において,前記
キ−溝が前記ステ−タコア側に設けられている磁気レゾ
ルバ−のスキュ−方法。
2. A skew method for a magnetic resolver according to claim 1, wherein said key groove is provided on said stator core.
【請求項3】 請求項1のスキュ−方法において,前記
キ−溝が前記ロ−タコア側に設けられている磁気レゾル
バ−のスキュ−方法。
3. The skewing method according to claim 1, wherein said key groove is provided on said rotor core side.
JP4145029A 1992-05-12 1992-05-12 Skew method of magnetic resolver Expired - Fee Related JP3013605B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4145029A JP3013605B2 (en) 1992-05-12 1992-05-12 Skew method of magnetic resolver

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4145029A JP3013605B2 (en) 1992-05-12 1992-05-12 Skew method of magnetic resolver

Publications (2)

Publication Number Publication Date
JPH05312590A JPH05312590A (en) 1993-11-22
JP3013605B2 true JP3013605B2 (en) 2000-02-28

Family

ID=15375770

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4145029A Expired - Fee Related JP3013605B2 (en) 1992-05-12 1992-05-12 Skew method of magnetic resolver

Country Status (1)

Country Link
JP (1) JP3013605B2 (en)

Families Citing this family (9)

* Cited by examiner, † Cited by third party
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JP4656378B2 (en) * 2004-07-08 2011-03-23 日本精工株式会社 Resolver and axial center position adjusting method of stator, starter coil position adjusting method, and absolute accuracy measuring method
JP4997214B2 (en) * 2008-11-19 2012-08-08 愛三工業株式会社 Resolver
US8269487B2 (en) 2008-11-11 2012-09-18 Aisan Kogyo Kabushiki Kaisha Sheet coil type resolver
JP4997213B2 (en) * 2008-11-11 2012-08-08 愛三工業株式会社 Resolver
US8310228B2 (en) 2008-11-12 2012-11-13 Aisan Kogyo Kabushiki Kaisha Resolver
JP5371092B2 (en) * 2009-03-30 2013-12-18 多摩川精機株式会社 Resolver and method for producing resolver
JP5467310B2 (en) * 2009-04-17 2014-04-09 多摩川精機株式会社 Resolver and method for producing resolver
GB2481406B (en) * 2010-06-22 2016-01-20 Ametek Airtechnology Group Ltd A resolver
WO2012086050A1 (en) * 2010-12-24 2012-06-28 トヨタ自動車株式会社 Press board laminate and press-fitting method for same

Also Published As

Publication number Publication date
JPH05312590A (en) 1993-11-22

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