JPH03207256A - Linear servo motor - Google Patents

Linear servo motor

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Publication number
JPH03207256A
JPH03207256A JP60090A JP60090A JPH03207256A JP H03207256 A JPH03207256 A JP H03207256A JP 60090 A JP60090 A JP 60090A JP 60090 A JP60090 A JP 60090A JP H03207256 A JPH03207256 A JP H03207256A
Authority
JP
Japan
Prior art keywords
permanent magnet
field
magnetic flux
core
linear servo
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.)
Granted
Application number
JP60090A
Other languages
Japanese (ja)
Other versions
JP2785406B2 (en
Inventor
Tetsuo Oishi
大石 哲男
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.)
Shinko Electric Co Ltd
Original Assignee
Shinko 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 Shinko Electric Co Ltd filed Critical Shinko Electric Co Ltd
Priority to JP60090A priority Critical patent/JP2785406B2/en
Publication of JPH03207256A publication Critical patent/JPH03207256A/en
Application granted granted Critical
Publication of JP2785406B2 publication Critical patent/JP2785406B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Linear Motors (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、精密位置決めや高速搬送などに用いて好適
なリニアサーボモータに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a linear servo motor suitable for use in precision positioning, high-speed conveyance, and the like.

[従来の技術] 各種の産業分野で応用されているリニアモータの中でも
、特に、界磁に永久磁石を用いたリニアサーボモータは
、その位置決め性能や速度性能に優れたサーボ特性を持
つため、精密位置決めや高速搬送などに用いられる。
[Conventional technology] Among linear motors that are applied in various industrial fields, linear servo motors that use permanent magnets in the field have excellent servo characteristics for positioning performance and speed performance, so they can be used for precision Used for positioning, high-speed conveyance, etc.

第5図は従来のリニアサーボモータの断面図、第6図は
同リニアサーボモータの界磁鉄心の上面図である。これ
らの図において、lは界磁鉄心で、その上には界磁用の
複数の永久磁石2が一定間隔でN極、S極と交互になる
ように配置されている。また、これらの永久磁石2は、
自らが発生する界磁磁束の空間分布が正弦波になるよう
にそれぞれが斜めに配列されるスキュー構造になってい
る。3は界磁鉄心1との間に空隙を有して配置される電
機子鉄心で、その下部に設けられた複数のスロット3a
のそれぞれにコイル4が巻き回されている。ところで、
永久磁石2から発生する界磁磁束φは、第5図に破線で
示すように空隙を介して電機子鉄心3に至り、背部を軸
方向に進み、再び空隙を介して隣接する永久磁石2に至
り、さらに、界磁鉄心l内を通って元の永久磁石2に戻
る。そして、この界MIFiFI束φによって、コイル
4と鎖交する磁束経路が形成され、コイル4には電機子
鉄心3の移動により誘起電圧が発生する。
FIG. 5 is a sectional view of a conventional linear servo motor, and FIG. 6 is a top view of the field core of the linear servo motor. In these figures, l is a field iron core, on which a plurality of field permanent magnets 2 are arranged so that N poles and S poles alternate at regular intervals. In addition, these permanent magnets 2 are
They have a skew structure in which they are arranged diagonally so that the spatial distribution of the field magnetic flux they generate becomes a sine wave. Reference numeral 3 denotes an armature core arranged with a gap between it and the field core 1, and a plurality of slots 3a provided at the bottom of the armature core 3.
A coil 4 is wound around each of them. by the way,
The field magnetic flux φ generated from the permanent magnet 2 reaches the armature core 3 through the air gap, as shown by the broken line in FIG. Then, it passes through the field core l and returns to the original permanent magnet 2. A magnetic flux path interlinking with the coil 4 is formed by this field MIFiFI flux φ, and an induced voltage is generated in the coil 4 due to the movement of the armature core 3.

また、電機子鉄心3には、界磁磁束φを検出する図示し
ない検出器(ホール素子など)が取り付けられている。
Furthermore, a detector (such as a Hall element), not shown, is attached to the armature core 3 to detect the field magnetic flux φ.

5は電機子鉄心3の速度制御や位置制御等を行う制御回
路で、前言己検出器の検出信号を入力し、この入力信号
に基づく制御信号をドライバ6に供給する。そして、ド
ライバ6はこの制御信号に従って、前記した誘起電圧と
同相の駆動電流を導体7及びブラシ8を介してコイル4
に供給する。コイル4では供給された駆動電流に応じた
磁束を発生する。そして、このコイル4による磁束と永
久磁石2による界磁磁束φとの相互作用により電機子鉄
心3に推力が発生し、この電機子鉄心3が図示の矢印へ
のいずれかの方向に駆動される。
Reference numeral 5 denotes a control circuit that performs speed control, position control, etc. of the armature core 3, which receives a detection signal from the self-detector and supplies a control signal to the driver 6 based on this input signal. Then, in accordance with this control signal, the driver 6 applies a drive current that is in phase with the above-mentioned induced voltage to the coil 4 through the conductor 7 and the brush 8.
supply to. The coil 4 generates magnetic flux according to the supplied drive current. Thrust is generated in the armature core 3 due to the interaction between the magnetic flux generated by the coil 4 and the field magnetic flux φ generated by the permanent magnet 2, and the armature core 3 is driven in one of the directions shown by the arrows. .

[発明が解決しようとする課題1 ところで、リニアサーボモータの駆動原理は、一般の永
久磁石形の交流サーボモーフと同じであり、リニアサー
ボモータにとっては、速度変動や推力変動を可能な限り
抑制することがモータ特性の良否を決定する重要事項で
ある。そして、この推力変動を抑制するためには界磁磁
束の空間分布を正弦波にして、誘起電圧を正弦波にし、
発生推力を滑らかな一定値とする必要がある。
[Problem to be solved by the invention 1 By the way, the driving principle of a linear servo motor is the same as that of a general permanent magnet type AC servo morph, and for a linear servo motor, it is important to suppress speed fluctuations and thrust fluctuations as much as possible. is an important matter that determines the quality of motor characteristics. In order to suppress this thrust variation, the spatial distribution of the field magnetic flux is made into a sine wave, and the induced voltage is made into a sine wave.
It is necessary to make the generated thrust a smooth constant value.

しかし、リニアサーボモータでは界磁磁束を永久磁石に
よって発生させているため、その空間磁束分布は正弦波
より短形波に近くなってしまう。
However, in a linear servo motor, the field magnetic flux is generated by a permanent magnet, so the spatial magnetic flux distribution becomes closer to a rectangular wave than a sine wave.

そこで、従来は第6図に示すように永久磁石を斜めに配
列するスキュー構造にしたり、界磁鉄心のスロットをス
キュー構造にして、誘起電圧を正弦波に近付けていたが
、十分な効果が得られなかった。
Therefore, in the past, as shown in Figure 6, permanent magnets were arranged diagonally in a skew structure, or the slots in the field core were made in a skew structure to bring the induced voltage closer to a sine wave, but these efforts were not effective enough. I couldn't.

この発明は、前記問題に鑑みて成されたもので、界磁磁
束の空間分布を正弦波にしてモータ特性の優れたリニア
サーボモータを提供することを目的とする。
The present invention has been made in view of the above problem, and an object of the present invention is to provide a linear servo motor with excellent motor characteristics in which the spatial distribution of field magnetic flux is made into a sine wave.

[課題を解決するための手段] 前記目的を達成するために、この発明では、界磁鉄心の
一面に配置された複数の永久磁石によって界磁磁束を発
生し、電機子鉄心に巻き回されたコイルによって前記界
磁磁束に相互作用をする磁束を発生し、当該電機子鉄心
を直線移動させるリニアサーボモータにおいて、前記永
久磁石の長手方向断面形状が2つの平行な円弧、2つの
平行な楕円弧又は2つの平行な双曲線の一部で画定され
、前記電機子鉄心の界磁鉄心と対向する囲器こ前記永久
磁石の内周面が整合できる突部が長平方向に等間隔に設
けられ、この突部と前記永久磁石の内周面が整合されて
いる。
[Means for Solving the Problems] In order to achieve the above object, the present invention generates a field magnetic flux by a plurality of permanent magnets arranged on one side of a field core, and generates a field magnetic flux that is wound around an armature core. In a linear servo motor that generates a magnetic flux that interacts with the field magnetic flux by a coil and moves the armature core in a straight line, the longitudinal cross-sectional shape of the permanent magnet has two parallel arcs, two parallel elliptical arcs, or two parallel elliptical arcs. The enclosure, which is defined by parts of two parallel hyperbolas and faces the field core of the armature core, is provided with protrusions at equal intervals in the longitudinal direction, with which the inner circumferential surface of the permanent magnet can be aligned. The inner peripheral surface of the permanent magnet is aligned with the inner peripheral surface of the permanent magnet.

〔作 用] この発明では、永久磁石の断面形状が2つの平行な円弧
、楕円弧又は双曲線の一部で画定されているので、界磁
鉄心と永久磁石との間の空隙長が永久磁石の中心で最も
短く、端部にいくにしたがって長(なり、隣接する永久
磁石の間で一番長くなっている。従って、磁気回路のパ
ーミアンスは、永久磁石の中心で最も高く、端部Gこし
)<番こしたがって低くなり、隣接する永久磁石の間で
一番低くなる。
[Function] In this invention, since the cross-sectional shape of the permanent magnet is defined by a part of two parallel arcs, elliptical arcs, or hyperbolas, the gap length between the field core and the permanent magnet is equal to the center of the permanent magnet. The permeance of the magnetic circuit is highest at the center of the permanent magnet, and the permeance of the magnetic circuit is highest at the center of the permanent magnet, and the permeance is the longest at the center of the permanent magnet. It becomes lower as the number increases, and is the lowest among adjacent permanent magnets.

このことは、永久磁石側から見れば、永久磁石各部の動
作点が極中心から遠ざかるのむこ従って徐々に低くなり
、永久磁石の発生する磁束量力5少くなっていると見る
ことができ、従って、界磁磁束の空間分布は正弦波に近
付き、界磁鉄心【こカロわる推力は滑らかな一定値にな
る。
From the perspective of the permanent magnet, it can be seen that the operating point of each part of the permanent magnet gradually becomes lower as it moves away from the pole center, and the amount of magnetic flux generated by the permanent magnet decreases. Therefore, The spatial distribution of the field magnetic flux approaches a sine wave, and the thrust force generated by the field core becomes a smooth constant value.

〔実施例1 次に図面を参照してこの発明の実施側番こりし)で説明
する。
[Embodiment 1] Next, an explanation will be given of the implementation of the present invention with reference to the drawings.

第1図はこの発明の第1の実施例の構成を示す断面図で
ある。なお、この図において、第5図Gこ示す従来例の
各部に対応する部分につ5tで同一の符号を付して説明
を省略する。
FIG. 1 is a sectional view showing the structure of a first embodiment of the present invention. In this figure, parts corresponding to those of the conventional example shown in FIG.

この図において、10は界磁鉄心であり、第2図に示す
複数の電気鉄板10a、10a、・・−・・−力)ら構
成されている。この電気鉄板10aの長手方向の一辺に
は、打ち抜き加工等による円弧状の突部11が一定間隔
で設けられており、この電気鉄板を同−向きで積層する
ことによって、上記界磁鉄心10が形成されている。ま
た、上述のように積層することで、界磁鉄心10の上部
には円弧状の突部11.11.−・・・・・が一定間隔
で形成されることになる。一方、永久磁石13は第2図
に示すようにその長平方向断面形状が2つの平行な円弧
で画定されており、その内周面13aは界磁鉄心10の
突部11と整合している。永久磁石13は、それ自身の
上部に現れる磁極がN極、S極と交互に現れるよう配置
されている。
In this figure, 10 is a field iron core, which is composed of a plurality of electric iron plates 10a, 10a, . . . shown in FIG. On one longitudinal side of the electric iron plate 10a, circular arc-shaped protrusions 11 are provided at regular intervals by punching or the like, and by stacking the electric iron plates in the same direction, the field iron core 10 is formed. It is formed. Further, by stacking the layers as described above, the upper part of the field core 10 has arc-shaped protrusions 11, 11, . -... will be formed at regular intervals. On the other hand, as shown in FIG. 2, the permanent magnet 13 has a longitudinal cross-sectional shape defined by two parallel circular arcs, and its inner peripheral surface 13a is aligned with the protrusion 11 of the field core 10. The permanent magnet 13 is arranged so that the magnetic poles appearing on the upper part of the permanent magnet 13 alternate with north poles and south poles.

このように、界磁鉄心10に断面形状が2つの平行な円
弧で画定されている永久磁石13を設けることにより、
界磁鉄心10と電機子鉄心3の空隙のパーミアンス(磁
気抵抗の逆数)が一定ではな(なり、所定の空間分布を
持つようになる。
In this way, by providing the field core 10 with the permanent magnet 13 whose cross-sectional shape is defined by two parallel arcs,
The permeance (reciprocal of magnetic resistance) of the air gap between the field core 10 and the armature core 3 is not constant, but has a predetermined spatial distribution.

すなわら、空隙のパーミアンスは、第3図に示す実線の
ように磁極中心で最も高く、磁極切り換わり点で最も低
くなり、界磁磁束Φの分布は矩形波から正弦波に近付く
。(なお、第3図中の一点鎖線は第5図に示す従来のリ
ニアサーボモータの界磁磁束Φの分布を示している)し
たがって、電機子鉄心3は、ドライバ6から供給される
駆動電流によって滑らかに駆動される。
That is, the permeance of the air gap is highest at the center of the magnetic pole and lowest at the magnetic pole switching point, as shown by the solid line in FIG. 3, and the distribution of the field magnetic flux Φ approaches a sine wave from a rectangular wave. (The dashed line in FIG. 3 shows the distribution of field magnetic flux Φ of the conventional linear servo motor shown in FIG. 5.) Therefore, the armature core 3 is driven by the drive current supplied from the driver 6. Drives smoothly.

次に、この発明の第2の実施例によるリニアサーボモー
タの断面図を第4図に示す。この実施例では、界磁鉄心
lOの突部11が楕円形で、永久磁石13の長手方向断
面形状が2つの平行な楕円弧で画定されている以外は第
1実施例と全く同様である。この例の場合も、第1図の
実施例と同様に、空隙のパーミアンスは、磁極中心で最
も高く、磁極切り換わり点で最も低くなり、界磁磁束Φ
の分布は正弦波に近付く。したがって、電機子鉄心3は
ドライバ6から供給される駆動電流によって滑らかに駆
動される。
Next, FIG. 4 shows a sectional view of a linear servo motor according to a second embodiment of the present invention. This embodiment is completely the same as the first embodiment except that the protrusion 11 of the field core IO is elliptical and the longitudinal cross-sectional shape of the permanent magnet 13 is defined by two parallel elliptical arcs. In this example, as in the example shown in FIG.
The distribution approaches a sine wave. Therefore, the armature core 3 is smoothly driven by the drive current supplied from the driver 6.

なお、永久磁石13の形状は上述したものに限られるも
のではなく、電機子鉄心と永久磁石との間の空隙長がそ
れぞれの永久磁石の中心部で1番長く、端部にいくに従
って短くなるように永久磁石の形状を定めて、つまり長
手方向断面形状が2つの平行な双曲線の一部で画定され
るようにし、その永久磁石の内面と整合するように突部
を形成してもよい。いいかえれば、パーミアンス分布が
磁極中心で最も高く、磁極切り換わり点で最も低くなり
モータの空隙長との相関で、空間高調波が最も少なくな
るようにすればよい。
Note that the shape of the permanent magnets 13 is not limited to the one described above, and the gap length between the armature core and the permanent magnets is longest at the center of each permanent magnet and becomes shorter toward the ends. The permanent magnet may be shaped so that its longitudinal cross-sectional shape is defined by parts of two parallel hyperbolas, and the projections may be formed to align with the inner surface of the permanent magnet. In other words, the permeance distribution is highest at the magnetic pole center and lowest at the magnetic pole switching point, so that spatial harmonics are minimized in correlation with the motor air gap length.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、この発明は、長手方向断面形状が
平行な2つの円弧・楕円弧または双曲線の一部で画定さ
れている永久磁石を用い、この永久磁石の内周面を界磁
鉄心に設けた突部に整合させているので、空隙のパーミ
アンス分布を永久磁石の磁極中心で最も高<、磁極切り
換わり点で最も低くなるようにでき、界M1磁束の空間
分布を正弦波を近付けることができる。この結果、発生
推力を一定にすることができ、特性の優れたリニアサー
ボモータを提供できる。
As explained above, the present invention uses a permanent magnet whose longitudinal cross-sectional shape is defined by a part of two parallel circular arcs, elliptical arcs, or hyperbolas, and the inner circumferential surface of this permanent magnet is attached to the field core. Since the permeance distribution of the air gap is the highest at the magnetic pole center of the permanent magnet and the lowest at the magnetic pole switching point, the spatial distribution of the field M1 magnetic flux can be made closer to the sine wave. can. As a result, the generated thrust can be made constant, and a linear servo motor with excellent characteristics can be provided.

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

第1図はこの発明の第1の実施例の構成を示す断面図、
第2図は同実施例の界磁鉄心及び永久磁石の構造を示す
斜視図、第3図は同実施例の永久磁石が発生する界Fi
Ii磁束を示す磁束密度曲線図、第4図は同発明の第2
の実施例の構成を示す断面図、第5図は従来のリニアサ
ーボモータの断面図、第6図は同リニアサーボモータの
界磁鉄心の上面図である。 3・・・電機子鉄心、10・・・界磁鉄心、11−・突
部、   13・・・永久磁石。
FIG. 1 is a sectional view showing the configuration of a first embodiment of the present invention;
Fig. 2 is a perspective view showing the structure of the field core and permanent magnet of the same embodiment, and Fig. 3 is a field Fi generated by the permanent magnet of the same embodiment.
A magnetic flux density curve diagram showing the Ii magnetic flux, FIG. 4 is the second diagram of the same invention.
FIG. 5 is a cross-sectional view of a conventional linear servo motor, and FIG. 6 is a top view of the field core of the linear servo motor. 3... Armature core, 10... Field core, 11--Protrusion, 13... Permanent magnet.

Claims (1)

【特許請求の範囲】[Claims] 界磁鉄心の一面に配置された複数の永久磁石によって界
磁磁束を発生し、電機子鉄心に巻き回されたコイルによ
って前記界磁磁束に相互作用をする磁束を発生し、当該
電機子鉄心を直線移動させるリニアサーボモータにおい
て、前記永久磁石の長手方向断面形状が2つの平行な円
弧、2つの平行な楕円弧又は2つの平行な双曲線の一部
で画定され、前記界磁鉄心の前記電機子鉄心と対向する
面に前記永久磁石の内周面が整合できる突部が長手方向
に等間隔に設けられ、この突部と前記永久磁石の内周面
が整合されていることを特徴とするリニアサーボモータ
A field magnetic flux is generated by a plurality of permanent magnets arranged on one side of the field core, and a magnetic flux that interacts with the field magnetic flux is generated by a coil wound around the armature core. In the linear servo motor for linear movement, the longitudinal cross-sectional shape of the permanent magnet is defined by parts of two parallel arcs, two parallel elliptical arcs, or two parallel hyperbolas, and the armature core of the field core A linear servo characterized in that protrusions are provided at equal intervals in the longitudinal direction on a surface facing the permanent magnet so that the inner circumferential surface of the permanent magnet can be aligned, and the protrusions and the inner circumferential surface of the permanent magnet are aligned. motor.
JP60090A 1990-01-08 1990-01-08 Linear servo motor Expired - Fee Related JP2785406B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60090A JP2785406B2 (en) 1990-01-08 1990-01-08 Linear servo motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60090A JP2785406B2 (en) 1990-01-08 1990-01-08 Linear servo motor

Publications (2)

Publication Number Publication Date
JPH03207256A true JPH03207256A (en) 1991-09-10
JP2785406B2 JP2785406B2 (en) 1998-08-13

Family

ID=11478227

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60090A Expired - Fee Related JP2785406B2 (en) 1990-01-08 1990-01-08 Linear servo motor

Country Status (1)

Country Link
JP (1) JP2785406B2 (en)

Cited By (7)

* Cited by examiner, † Cited by third party
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WO2000001059A1 (en) * 1998-06-29 2000-01-06 Siemens Aktiengesellschaft Linear synchronous motor
EP1164684A3 (en) * 2000-06-16 2004-01-02 Fanuc Ltd Rotor for synchronous motor
EP1372251A3 (en) * 2002-06-11 2004-03-10 Fanuc Ltd Linear motor
WO2009057442A1 (en) * 2007-10-31 2009-05-07 Thk Co., Ltd. Linear motor, and linear motor system
JP2010104136A (en) * 2008-10-23 2010-05-06 Mitsubishi Electric Corp Linear motor
EP1615322A4 (en) * 2003-03-25 2010-05-26 Thk Co Ltd Linear motor actuator
CN101789677A (en) * 2010-03-15 2010-07-28 哈尔滨工业大学 Secondary structure of low-thrust waved sine wave permanent magnet liner synchronous motor

Cited By (13)

* Cited by examiner, † Cited by third party
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WO2000001059A1 (en) * 1998-06-29 2000-01-06 Siemens Aktiengesellschaft Linear synchronous motor
US6713899B1 (en) 1998-06-29 2004-03-30 Siemens Aktiengesellschaft Linear synchronous motor
US6812614B2 (en) 2000-06-16 2004-11-02 Fanuc Ltd. Rotor for a synchronous motor defined by a hyperbolic function
EP1164684A3 (en) * 2000-06-16 2004-01-02 Fanuc Ltd Rotor for synchronous motor
EP1619780A1 (en) * 2002-06-11 2006-01-25 Fanuc Ltd Linear motor
US6873066B2 (en) 2002-06-11 2005-03-29 Fanuc Ltd Linear motor
EP1372251A3 (en) * 2002-06-11 2004-03-10 Fanuc Ltd Linear motor
EP1615322A4 (en) * 2003-03-25 2010-05-26 Thk Co Ltd Linear motor actuator
WO2009057442A1 (en) * 2007-10-31 2009-05-07 Thk Co., Ltd. Linear motor, and linear motor system
JPWO2009057442A1 (en) * 2007-10-31 2011-03-10 Thk株式会社 Linear motor and linear motor system
JP2010104136A (en) * 2008-10-23 2010-05-06 Mitsubishi Electric Corp Linear motor
CN101789677A (en) * 2010-03-15 2010-07-28 哈尔滨工业大学 Secondary structure of low-thrust waved sine wave permanent magnet liner synchronous motor
CN101789677B (en) 2010-03-15 2011-11-09 哈尔滨工业大学 Secondary structure of low-thrust waved sine wave permanent magnet liner synchronous motor

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