JPS61164458A - Linear motor - Google Patents

Linear motor

Info

Publication number
JPS61164458A
JPS61164458A JP381285A JP381285A JPS61164458A JP S61164458 A JPS61164458 A JP S61164458A JP 381285 A JP381285 A JP 381285A JP 381285 A JP381285 A JP 381285A JP S61164458 A JPS61164458 A JP S61164458A
Authority
JP
Japan
Prior art keywords
yoke
center pole
mover
coils
pair
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
JP381285A
Other languages
Japanese (ja)
Inventor
Shiro Hasegawa
志朗 長谷川
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.)
SWCC Corp
Original Assignee
Showa Electric Wire and Cable Co
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 Showa Electric Wire and Cable Co filed Critical Showa Electric Wire and Cable Co
Priority to JP381285A priority Critical patent/JPS61164458A/en
Publication of JPS61164458A publication Critical patent/JPS61164458A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K41/00Propulsion systems in which a rigid body is moved along a path due to dynamo-electric interaction between the body and a magnetic field travelling along the path
    • H02K41/02Linear motors; Sectional motors
    • H02K41/035DC motors; Unipolar motors
    • H02K41/0352Unipolar motors
    • H02K41/0354Lorentz force motors, e.g. voice coil motors
    • H02K41/0356Lorentz force motors, e.g. voice coil motors moving along a straight path

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Electromagnetism (AREA)
  • Power Engineering (AREA)
  • Reciprocating, Oscillating Or Vibrating Motors (AREA)

Abstract

PURPOSE:To obtain small-sized products of high thrust, by fitting a pair of magnets on the inner peripheral face of one end of a cylindrical yoke so that different poles may confront with each other, and by engaging the diameter sections of two coils forming a mover, with a wide slot in the axial direction of a center pole. CONSTITUTION:A cylindrical holder 11 made of light alloy is fitted at one end of a cylindrical yoke 10 with the both opening ends, and a pair of magnets 14, 14 are fitted on the inner peripheral face of the other end so that the different poles may confront together. A wide slit 12 in the axial direction is provided for a center pole 13, and after a mover 15 is inserted into the slot, the opening end of the center pole 13 is closed by a front yoke 13b. Two semi-circular coils are lumped together at the diameter section 15a3 by the mover 15, and the mover 15 is formed with a composite coil 15a for reversing the current direction of the both coils, an intermediate pipe 15b, and a fitting head 15c, and the diameter section 15a3 is engaged with the wide slot 12. Current flowing through coils is controlled, and the mover 15 is moved, In this manner, the distribution of magnetic flux is uniformed, and small-sized products of high thrust are produced.

Description

【発明の詳細な説明】 [発明の技術分野] 本発明はりニアモータ、特にボイスコイル型リニアモー
タ(以下VCM)の改良に係る。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to improvements in linear motors, particularly voice coil linear motors (hereinafter referred to as VCM).

[発明の技術的背景とその問題点] 第6図に従来のVCMの一例を示す。この図から分るよ
うに、従来のVCMは円筒状のヨーク1と、その一端を
閉鎖する形状で設けられたリアヨーク2と、リアヨーク
の中心に立設された円柱状のセンタポール3と、サイド
ヨークの内側にその直径両端に位置して同極同士対向さ
せて配置した1対の磁石4と、センタポール3に係合さ
れたコイル5とを有する。磁石4の表面から出た磁束は
すべてセンタポール3に集中し、リアヨーク2を経由し
てヨーク1、従って磁石4の裏面に戻っている。
[Technical background of the invention and its problems] FIG. 6 shows an example of a conventional VCM. As can be seen from this figure, the conventional VCM includes a cylindrical yoke 1, a rear yoke 2 with one end closed, a cylindrical center pole 3 erected in the center of the rear yoke, and a side The yoke includes a pair of magnets 4 located at both diametrical ends of the yoke with the same poles facing each other, and a coil 5 engaged with the center pole 3. All the magnetic flux emitted from the front surface of the magnet 4 is concentrated on the center pole 3 and returns to the yoke 1 via the rear yoke 2 and, therefore, to the back surface of the magnet 4.

上記のような磁束の流れのため、センタポールの根元に
磁束が集中し、この部分で磁気飽和が生じ易く、VCM
のストロークを大きくするには、単に磁石、ヨーク、セ
ンタポールの長さを大とするだけでなく、それらを三次
元的に拡大する必要があった。そのため、長ストローク
のVCMは大重量のものとならざるを得なかった。従っ
て、大型、大推力のVCMを設計する場合にはストロー
クとのかねあいで、磁気回路を以下に軽量化するかが重
要なポイントとなっている。
Due to the above magnetic flux flow, the magnetic flux concentrates at the base of the center pole, and magnetic saturation tends to occur in this part, causing VCM
In order to increase the stroke, it was necessary not only to increase the length of the magnet, yoke, and center pole, but also to expand them three-dimensionally. Therefore, a long stroke VCM has to be heavy. Therefore, when designing a large-sized, large-thrust VCM, it is important to reduce the weight of the magnetic circuit as much as possible in consideration of the stroke.

さらに、コイルに電流を印加した場合にはAT(アンペ
アターン)による磁界が発生し、これがセンタポールに
侵入し磁石の磁界と合流し、同じ向きの時はこれを強め
、逆向きの時は弱め、推力の変動を招くという問題があ
り、両者のバランスのとれたVCMを設計するには高度
の技術を必要とする。
Furthermore, when current is applied to the coil, a magnetic field is generated due to AT (Ampere Turn), which enters the center pole and merges with the magnetic field of the magnet, strengthening it when the directions are the same and weakening it when the directions are opposite. However, there is a problem in that it causes fluctuations in thrust force, and advanced technology is required to design a VCM with a good balance between the two.

[発明の目的] 本発明は上記の事情に基きなされたもので、長ストロー
クのVCMとした場合も、ヨーク、センタポールを小型
軽量のものとすることができ、しかもコイル通電時のA
Tによる磁界の問題を解決したVCMを提供する。
[Object of the Invention] The present invention has been made based on the above circumstances, and even when a long stroke VCM is used, the yoke and center pole can be made small and lightweight, and the A when the coil is energized can be reduced.
To provide a VCM that solves the problem of magnetic fields caused by T.

[発明の概要] 本発明のVCMは、円筒状のヨークと、このヨーク内に
ヨークの直径両端に位置して配置され異る極同士対向さ
せられた1対の磁石と、前記ヨーク内に同心的に配置さ
れ円柱状をなしその直径を含む面に対称な形状の軸方向
の長孔を有するセンタポールと、略半円筒状の互いに逆
巻の1対のコイルをその直状部同士のを当接して形成さ
れ前記直状部を前記長孔に係合させた複合コイルとを有
することを特徴とする。
[Summary of the Invention] The VCM of the present invention includes a cylindrical yoke, a pair of magnets located at both diametrical ends of the yoke and having different poles facing each other, and a pair of magnets arranged concentrically within the yoke. A center pole is arranged in a cylindrical shape and has a long hole in the axial direction that is symmetrical in a plane including its diameter, and a pair of approximately semi-cylindrical coils are wound oppositely to each other. It is characterized by having a composite coil that is formed in contact with each other and has the straight portion engaged with the elongated hole.

[発明の実施例] 第1図は本発゛明−実施例のカットモデルの斜視図、第
2図はその可動子を取出して示す斜視図、第3図は可動
子コイルの斜視図、第4図は前記実施例の横断面図、第
5図はその縦断面図である。
[Embodiments of the Invention] Fig. 1 is a perspective view of a cut model of the present invention-embodiment, Fig. 2 is a perspective view showing the mover taken out, and Fig. 3 is a perspective view of the mover coil. FIG. 4 is a cross-sectional view of the embodiment, and FIG. 5 is a longitudinal cross-sectional view thereof.

第1図において、両端開放の円筒状のヨーク10の一端
には軽合金製の環板状のリアホルダ11が取付けられ、
このリアホルダには円柱状で一直径を含む面に関し対象
形状の軸方向の長孔12を有するセンタポール13がヨ
ーク10と同心に支持されている。このセンタポール1
3は、実際には円柱状の素材13aに深い擦り割りを施
しておき、擦り割りの開口端を、円板状のフロントヨー
ク13bで閉鎖して構成する。また、円筒面の一部をな
す磁石14はヨーク10の直径両端に位置して異極同士
対向させてヨーク内面に取付けられている。一方、可動
子15は、第2図に示すように複合コイル15aと、中
間バイブ15bと、取付用ヘッド15cとを有する。複
合コイル15aは、第3図に示すように、例えば図の左
側のものが左巻で右側のものが布巻のように、互いに逆
巻とされた略半円状の2箇のコイル15a1を複合して
構成され、2箇のコイルの直状部が合体して形成する平
面部15a2はセンタポール13の長孔12に係合され
る。その組立は、次のようにして行われる。まず、セン
タポールのフロントヨークの取付前に複合コイル15の
平面部15a2を、センタポール素材の擦り割りに係合
させ、これに中間バイブ15bを結合し、次いでフロン
トヨーク13bを取付ける。上記のようにしてセンタポ
ール13に係合させた複合コイル15aに取付けた中間
バイブ15bに、取付用ヘッド15Gを連結固定する。
In FIG. 1, a ring plate-shaped rear holder 11 made of light alloy is attached to one end of a cylindrical yoke 10 with both ends open.
A center pole 13 having a cylindrical shape and having an axially elongated hole 12 having a symmetrical shape with respect to a surface including one diameter is supported concentrically with the yoke 10 on this rear holder. This center pole 1
3 is actually constructed by making a deep slit in a columnar material 13a, and closing the open end of the slit with a disc-shaped front yoke 13b. Further, the magnets 14 forming a part of the cylindrical surface are located at both diametrical ends of the yoke 10 and are attached to the inner surface of the yoke with different polarities facing each other. On the other hand, the movable element 15 has a composite coil 15a, an intermediate vibrator 15b, and a mounting head 15c, as shown in FIG. As shown in FIG. 3, the composite coil 15a is a combination of two approximately semicircular coils 15a1 wound in opposite directions, such as the one on the left in the figure being left-handed and the one on the right being cloth-wrapped. A flat portion 15a2 formed by combining the straight portions of the two coils is engaged with the elongated hole 12 of the center pole 13. Its assembly is performed as follows. First, before attaching the front yoke of the center pole, the flat portion 15a2 of the composite coil 15 is engaged with the slit in the center pole material, the intermediate vibe 15b is coupled thereto, and then the front yoke 13b is attached. The attachment head 15G is connected and fixed to the intermediate vibrator 15b attached to the composite coil 15a engaged with the center pole 13 as described above.

上記構成の本発明のVCMにおける電流の流れおよび磁
束の流れは第4図、第5図に示す通りである。まず、複
合コイル15aを構成する左側のコイルでは電流は時計
回りに流れ、右側のコイルでは反時計回りに流れる。
The current flow and magnetic flux flow in the VCM of the present invention having the above configuration are as shown in FIGS. 4 and 5. First, current flows clockwise in the left coil that constitutes the composite coil 15a, and counterclockwise in the right coil.

また、一方の磁石から出た磁束は、一旦その磁石に近接
しているセンタポールの部材13aの脚片に入るが、次
いで、フロントヨーク13bおよびリア側の部材を分流
して他方の脚片に流れ、そこからその脚片に近接した反
対側の磁石に入った後、ヨーク10を経由して元の磁石
の裏面に帰って来る。而して、前記のように互に逆巻の
コイル15a1からなる複合コイル15aに電流を印加
(電流を逆向きに流す)すれば、可動子15には推力が
生じる。
Also, the magnetic flux emitted from one magnet first enters the leg of the center pole member 13a that is close to that magnet, but then it is diverted through the front yoke 13b and the rear side member and flows into the other leg. From there, it enters the magnet on the opposite side close to the leg, and then returns to the back side of the original magnet via the yoke 10. Thus, when a current is applied to the composite coil 15a consisting of the coils 15a1 wound in opposite directions (current is caused to flow in opposite directions) as described above, thrust is generated in the movable element 15.

上記構成の本発明VCMにあっては、従来のVCMに見
られた磁束の集中はなく、センタポール、ヨークに特に
磁気飽和を生じ易い部位はないので、従来のVCMの1
/2〜1/3の重量のセンタポール、ヨークで同一の出
力を得ることができる。
In the VCM of the present invention having the above configuration, there is no concentration of magnetic flux seen in conventional VCMs, and there are no parts in the center pole or yoke that are particularly prone to magnetic saturation.
The same output can be obtained with a center pole and yoke that are 1/2 to 1/3 the weight.

また、VCMのストロークを大きくする場合にもセンタ
ポールσ等の重iを増加させる必要はない。
Also, when increasing the stroke of the VCM, there is no need to increase the weight i of the center pole σ, etc.

さらに、磁束の流れは円筒状のヨークを通って他方の磁
石の裏面に入るから、リアホルダは非磁性体である軽金
属とすることができ、この面からも重量の軽減を図るこ
とができる。
Furthermore, since the flow of magnetic flux passes through the cylindrical yoke and enters the back surface of the other magnet, the rear holder can be made of a non-magnetic light metal, which also contributes to weight reduction.

さらに、従来のVCMにおいては、コイルに通電するこ
とにより生じるAT(アンペアターン)磁界は、磁石お
よびヨークに侵入し、磁石の発生する磁力線に変動を及
ぼし、推力に変動を生じるおそれがあり、著しい場合に
は磁石の永久減磁を惹起する。本発明のVCMでは、複
合コイネルを構成する2箇のコイルノ発生する磁束の流
れはセンタポール内に限定され、磁石に影響を与え難い
ため前記のような問題は全くないので、ピーク電流値を
高く設定することができ、VCMの起動、□停止時に有
利である。
Furthermore, in conventional VCMs, the AT (ampere-turn) magnetic field generated by energizing the coil enters the magnet and yoke, causing fluctuations in the magnetic field lines generated by the magnet, which can cause significant fluctuations in thrust force. In some cases, this may cause permanent demagnetization of the magnet. In the VCM of the present invention, the flow of magnetic flux generated by the two coils that make up the composite coil is limited to the center pole and does not easily affect the magnet, so there is no problem as described above, so the peak current value can be set high. It can be set, which is advantageous when starting and stopping VCM.

なお、コイルはボビン付、ボビン無の何れであってもよ
いし、またコイルの線材は丸線、平角線の何れであって
もよい。また、本発明は例示のショートコイル型のみで
なく、ロングコイル型にも適用し得ることは勿論である
The coil may be with or without a bobbin, and the wire of the coil may be either a round wire or a rectangular wire. Furthermore, it goes without saying that the present invention can be applied not only to the illustrated short coil type but also to a long coil type.

C発明の効果] 上記から明らかなように、本発明のVCMは同一出力で
あれば従来のVCMより、も格段に小形化することがで
き、逆に同一の大きざ1重量であれば、著しく出力の大
きなVCMとすることができる。また、ストロークの大
きなVCMであっても、従来のようにセンタポール等の
磁気飽和につき考慮する必要がないので、容易に設計を
することができる。
C Effect of the Invention] As is clear from the above, the VCM of the present invention can be made much smaller than the conventional VCM if the output is the same, and conversely, if the size and weight are the same, it is significantly smaller. It can be a VCM with a large output. Further, even a VCM with a large stroke can be easily designed because there is no need to consider magnetic saturation of a center pole or the like as in the conventional case.

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

第1図は本発明一実施例のカットモデルの斜視図、第2
図はその可動子の斜視図、第3図はその複合コイルの斜
視図、第4図は前記実施例の横断面図、第5図はその縦
断面図、第6図は従来のVCMの縦断面図である。 1o・・・ヨーク    11・・・リアホルダ12・
・・長孔     13・・・センタポール14・・・
磁石    15・・・可動子15a・・・複合コイル 第1図 第2図 Oc 第3図 第4図 式ノa。
Fig. 1 is a perspective view of a cut model according to an embodiment of the present invention;
Figure 3 is a perspective view of the movable element, Figure 3 is a perspective view of the composite coil, Figure 4 is a cross-sectional view of the embodiment, Figure 5 is a vertical cross-section thereof, and Figure 6 is a vertical cross-section of a conventional VCM. It is a front view. 1o... Yoke 11... Rear holder 12.
...Long hole 13...Center pole 14...
Magnet 15...Mover 15a...Composite coil Fig. 1 Fig. 2 Oc Fig. 3 Fig. 4 Diagram No.a.

Claims (1)

【特許請求の範囲】[Claims] 円筒状のヨークと、このヨーク内にヨークの直径両端に
位置して配置され異る極同士対向させられた1対の磁石
と、前記ヨーク内に同心的に配置され円柱状をなしその
直径を含む面に対称な形状の軸方向の長孔を有するセン
タポールと、略半円筒状の互いに逆巻の1対のコイルを
その直状部同士のを当接して形成され前記直状部を前記
長孔に係合させた複合コイルとを有することを特徴とす
るリニアモータ。
A cylindrical yoke, a pair of magnets arranged within the yoke at both ends of the diameter of the yoke with different poles facing each other, and a pair of magnets arranged concentrically within the yoke and having a cylindrical shape and whose diameter A center pole having a long hole in the axial direction symmetrical to the plane containing the center pole, and a pair of approximately semi-cylindrical coils wound oppositely to each other are formed by abutting the straight parts of the coils. A linear motor characterized by having a composite coil engaged with a long hole.
JP381285A 1985-01-11 1985-01-11 Linear motor Pending JPS61164458A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP381285A JPS61164458A (en) 1985-01-11 1985-01-11 Linear motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP381285A JPS61164458A (en) 1985-01-11 1985-01-11 Linear motor

Publications (1)

Publication Number Publication Date
JPS61164458A true JPS61164458A (en) 1986-07-25

Family

ID=11567602

Family Applications (1)

Application Number Title Priority Date Filing Date
JP381285A Pending JPS61164458A (en) 1985-01-11 1985-01-11 Linear motor

Country Status (1)

Country Link
JP (1) JPS61164458A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0410582U (en) * 1990-05-15 1992-01-29

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0410582U (en) * 1990-05-15 1992-01-29

Similar Documents

Publication Publication Date Title
JPS61164458A (en) Linear motor
JPS61164459A (en) Linear motor
JPH02165606A (en) Plunger type electromagnet
JP2576443B2 (en) Electromagnet device
JPS61161951A (en) Linear motor
JPS6014491B2 (en) electromagnetic drive equipment
JPS59171314U (en) electromagnet device
GB1008735A (en) Improvements relating to electrical devices for producing a controlled and reversibleforce or movement in a linear direction
JPS5926791Y2 (en) linear motor
JPS6084805A (en) Three-dimensionally stabilized electromagnet apparatus
JP3296890B2 (en) Polarized linear actuator
JPH05251230A (en) Polarized electromagnet
JPH08163850A (en) Single pole dc linear motor
JPH0442884Y2 (en)
JPH0117797Y2 (en)
JPS609357A (en) Linear motor
JPH0134837Y2 (en)
JPS6311893Y2 (en)
JP2002142428A (en) Linear motor
JPS6334613B2 (en)
JP2574367Y2 (en) Linear actuator
JPH0316192Y2 (en)
JPH0232749A (en) linear actuator
JPH0722048B2 (en) Electromagnetic device
JPS6178106A (en) Electromagnet device