JPS5944962A - High magnetic flux density field for linear motor - Google Patents

High magnetic flux density field for linear motor

Info

Publication number
JPS5944962A
JPS5944962A JP15308682A JP15308682A JPS5944962A JP S5944962 A JPS5944962 A JP S5944962A JP 15308682 A JP15308682 A JP 15308682A JP 15308682 A JP15308682 A JP 15308682A JP S5944962 A JPS5944962 A JP S5944962A
Authority
JP
Japan
Prior art keywords
field
magnetic
flux density
magnetic flux
linear motor
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
JP15308682A
Other languages
Japanese (ja)
Inventor
Teruo Asakawa
輝雄 浅川
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.)
Tokyo Electron Ltd
Original Assignee
Tokyo Electron 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 Tokyo Electron Ltd filed Critical Tokyo Electron Ltd
Priority to JP15308682A priority Critical patent/JPS5944962A/en
Publication of JPS5944962A publication Critical patent/JPS5944962A/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
    • H02K41/03Synchronous motors; Motors moving step by step; Reluctance motors
    • H02K41/031Synchronous motors; Motors moving step by step; Reluctance motors of the permanent magnet type

Abstract

PURPOSE:To obtain a field which has high magnetic flux density by alternately laminating a permanent magnet and a conductor of a yoke forming a field along the moving direction of a movable element. CONSTITUTION:A permanent magnet 23 and a yoke 24 are held by nonmagnetic retaining members 21, 22, which are secured at an interval via a supporting member 25. The magnet 23 and the yoke 24 of the magnetic conductor are alternately laminated along the moving direction of a movable element 27. The magnets 23 are aligned so that N-poles and S-poles are respectively opposed each other, and aligned so that the N-poles and the S-poles are oppositely disposed at the sides of the members 21, 22, thereby forming magnetic space groups in which the direction of the magnetic field are alternately directed oppositely.

Description

【発明の詳細な説明】 本発明はリニアモーターの界磁の磁気空間群構成方法に
関する。 本発明は特に既に知られている直線上に等間
隔に並んt!交互に反対方向を向いた磁気空間群と、平
板状に巻かれた二411のコイルとから成る五−ピング
コイル?’U流リニアモーターにおいて、その界磁の構
成方法を改良する事により、より高い磁束密度を持つ界
磁を得る事を目的とする。 この種のモーターは、磁界
の「17を流れるFI流に働く力を利用するものてあろ
が、この力の大きさは磁束密度と電流との積に比例し、
従って磁束密度を高くすることにJり少ない電流で大き
な力を発生する電流対推力比特性の良いモーターが得ら
れる。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for configuring a magnetic space group of a linear motor field. The present invention is particularly suitable for t! A five-pin coil consisting of magnetic space groups facing alternately in opposite directions and 2411 coils wound into a flat plate? 'The purpose of this project is to obtain a field with higher magnetic flux density by improving the method of configuring the field in a U-style linear motor. This type of motor utilizes the force exerted on the FI flow flowing through the magnetic field, and the magnitude of this force is proportional to the product of magnetic flux density and current.
Therefore, by increasing the magnetic flux density, it is possible to obtain a motor with good current-to-thrust ratio characteristics that generates a large force with a small amount of current.

第一図に従来の界磁を用いたリニアモーターの一例の正
UJ図及び側面図の略図を示す。 1,2は磁路の一部
を構成するa1気導体であり、永久磁石3の保持部材を
兼ね、4に示す支持部材によって間隔を保ち固定されて
おり、永久磁石は5に示す磁路を構成すべく並べられ、
磁界の方向が交互に反対方向を向いた磁気空間群を構成
している。
FIG. 1 shows a schematic diagram of a front UJ view and a side view of an example of a conventional linear motor using a field. 1 and 2 are a1 conductors that constitute a part of the magnetic path, which also serve as holding members for the permanent magnet 3, and are fixed at a distance by the support member shown in 4, and the permanent magnets follow the magnetic path shown in 5. arranged to form
They form a magnetic space group in which the directions of the magnetic fields alternate in opposite directions.

一方、6,7は移動子を構成するコイルであり磁気空間
群内を矢印8にそって移動する。 このような構成1ζ
おいては1、界磁は各々対向する永久磁石とその磁路を
/r面にて閉じる磁気導体1,2によって構成されCい
るため、永久磁石の厚さはある程度任意に取lするが面
積は磁界の配列ピッチによって制限される。 しかし、
磁石の表面が直接磁極となっているため磁石自体の磁束
密度の限界があり、永久磁石の厚さを厚くしても前記限
界値より高い磁束密度を得ろ事は困難である。
On the other hand, numerals 6 and 7 are coils constituting a moving element, which move along the arrow 8 within the magnetic space group. Such a configuration 1ζ
In 1, the field is composed of opposing permanent magnets and magnetic conductors 1 and 2 that close their magnetic paths on the /r plane, so the thickness of the permanent magnets can be arbitrarily selected to some extent, but the area is limited by the arrangement pitch of the magnetic field. but,
Since the surface of the magnet directly serves as a magnetic pole, there is a limit to the magnetic flux density of the magnet itself, and even if the thickness of the permanent magnet is increased, it is difficult to obtain a magnetic flux density higher than the above limit value.

以下、本発明に係るリニアモーター用高磁束密度界磁に
関する詳細な説明を行なうが、この種のモーターの動作
原理は既に知られており、また、本発明は動作原理に係
るものではないので動作原理には触れない。
The high magnetic flux density field for linear motors according to the present invention will be explained in detail below, but since the operating principle of this type of motor is already known and the present invention is not related to the operating principle, I won't touch on the principle.

第二図に本発明に係るリニアモーター用高磁束密度界磁
の一応用例の正面図及び側面図の略図を示す。 図にお
いて、21.22ば磁路の構成に寄与しない非磁性体に
よる永久磁石とヨークとの保持部材であり、25に示す
支持部材により間隔を保ち固定されている。 23は永
久磁石であり、24は磁気導体のヨークであり、移動子
の移動力向に添って交互に積み重ねられている。 永久
at石はNとN、SとSが向かい合うように並べられて
おり、更に保持部材21側と22側とでは逆になるよう
に並べられており磁路は矢印26の如く閉じ、磁界の方
向が交互に反対方向を向いた磁気空間群を構成する。 
このような構成にする事により、永久磁石の厚さは磁界
の配列ピッチによりある程度制限されるがほぼ十分な厚
さが取れ、しかもそのiC1積は磁界の配列ピッチによ
り制限されることがなく、また、ヨークにより収束され
るため高い磁束密度の界磁を得ろことができる。 まj
:、本発明に係るリニアモーター用高磁束密度界磁によ
って構成される磁気空間群は従来の界磁1こよって構成
される磁気空間BYとその強度以外変わらないにめ、そ
の制御が変わること(よなく、従来のモーターとの互換
性は保たれ、電流対推力比及び電力対推力比が向上する
FIG. 2 schematically shows a front view and a side view of an application example of a high magnetic flux density field for a linear motor according to the present invention. In the figure, reference numerals 21 and 22 are non-magnetic permanent magnet and yoke holding members that do not contribute to the structure of the magnetic path, and are fixed by a support member 25 with a distance maintained between them. 23 is a permanent magnet, and 24 is a yoke of magnetic conductor, which are alternately stacked along the direction of the moving force of the moving element. The permanent AT stones are arranged so that N and N and S and S face each other, and are further arranged so that they are opposite on the holding member 21 side and 22 side, so that the magnetic path is closed as shown by the arrow 26, and the magnetic field is They constitute a magnetic space group whose directions alternately point in opposite directions.
By adopting such a configuration, the thickness of the permanent magnet is limited to some extent by the arrangement pitch of the magnetic field, but it can be almost sufficiently thick, and the iC1 product is not limited by the arrangement pitch of the magnetic field. In addition, since it is focused by the yoke, it is possible to obtain a field with a high magnetic flux density. Maj
: Since the magnetic space group constituted by the high magnetic flux density field for linear motors according to the present invention is the same as the magnetic space BY constituted by the conventional field 1 except for its strength, its control is different ( Instead, compatibility with conventional motors is maintained and the current-to-thrust and power-to-thrust ratios are improved.

以上で、本発明に係るリニアモーター用高磁束密度界磁
に関する詳細な説明を終るが、本発明の主旨を変えるこ
となく磁気空間BYを構成する部材の形状や構成等が変
更、可能てあることは言うよでもない。
This concludes the detailed explanation of the high magnetic flux density field for linear motors according to the present invention, but it is possible to change the shape and configuration of the members constituting the magnetic space BY without changing the gist of the present invention. I can't say that.

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

第一図は従来の界磁を用いたリニアモーターの一例の正
面図及び側面図の略図であり、第二図は本発明に係るリ
ニアモーター用′R磁束密度界磁の一応用例の正面図及
び側面図の略図である。 特許出願人  東京エレクl−ロン株式会社茎2団 手続補正書(方式) 1.事件の表示     昭和57年特許願第1530
86号2、考案の名称     リニアモーター月J 
1NEI! 54−七度界泣(3、補正をずろ者 5、補正の対象     願書及び明細書6、補正の内
容     別紙の通り
Fig. 1 is a front view and a schematic side view of an example of a linear motor using a conventional field, and Fig. 2 is a front view and a schematic diagram of an example of an application of a 'R magnetic flux density field for a linear motor according to the present invention. FIG. 3 is a schematic side view. Patent Applicant: Tokyo Elecron Co., Ltd. 2nd Group Procedural Amendment (Method) 1. Display of case 1982 Patent Application No. 1530
86 No. 2, name of invention Linear motor month J
1NEI! 54-Seven Degrees (3, Those who missed the amendment 5, Subject of amendment Application and specification 6, Contents of amendment As shown in the attached sheet)

Claims (1)

【特許請求の範囲】 移動子の移動方向に添って、磁界の方向が前記移動方向
と垂直かつ交互に反対方向を向いた磁気空間群を等間隔
に一直線上に配列した界磁を持つリニアモーターにおい
て、その界磁を構成ずろ永久磁石と磁気導体のヨークと
が、移@rの移動方向に添って交互に積み重ねられてい
るり【を特徴とするリニアモーター用高磁束密度界磁。
[Scope of Claims] A linear motor having a field in which, along the moving direction of a moving element, magnetic space groups whose magnetic field directions are perpendicular to the moving direction and alternately oriented in opposite directions are arranged in a straight line at equal intervals. A high magnetic flux density field for a linear motor, characterized in that permanent magnets and magnetic conductor yokes forming the field are stacked alternately along the moving direction of the displacement.
JP15308682A 1982-09-02 1982-09-02 High magnetic flux density field for linear motor Pending JPS5944962A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15308682A JPS5944962A (en) 1982-09-02 1982-09-02 High magnetic flux density field for linear motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15308682A JPS5944962A (en) 1982-09-02 1982-09-02 High magnetic flux density field for linear motor

Publications (1)

Publication Number Publication Date
JPS5944962A true JPS5944962A (en) 1984-03-13

Family

ID=15554664

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15308682A Pending JPS5944962A (en) 1982-09-02 1982-09-02 High magnetic flux density field for linear motor

Country Status (1)

Country Link
JP (1) JPS5944962A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60213258A (en) * 1984-04-06 1985-10-25 Tokyo Seimitsu Co Ltd Linear motor
JPS60237854A (en) * 1984-05-11 1985-11-26 Tokyo Seimitsu Co Ltd Linear motor
JPH08509353A (en) * 1993-04-14 1996-10-01 バーデュ、エルバート Levitation propulsion system using permanent magnets and iron and steel inserted between them
US6748907B2 (en) 1999-12-22 2004-06-15 Abb Ab Device including a combustion engine, a use of the device, and a vehicle

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60213258A (en) * 1984-04-06 1985-10-25 Tokyo Seimitsu Co Ltd Linear motor
JPS60237854A (en) * 1984-05-11 1985-11-26 Tokyo Seimitsu Co Ltd Linear motor
JPH08509353A (en) * 1993-04-14 1996-10-01 バーデュ、エルバート Levitation propulsion system using permanent magnets and iron and steel inserted between them
US6748907B2 (en) 1999-12-22 2004-06-15 Abb Ab Device including a combustion engine, a use of the device, and a vehicle

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