JPS62126856A - Linear motor - Google Patents

Linear motor

Info

Publication number
JPS62126856A
JPS62126856A JP26688985A JP26688985A JPS62126856A JP S62126856 A JPS62126856 A JP S62126856A JP 26688985 A JP26688985 A JP 26688985A JP 26688985 A JP26688985 A JP 26688985A JP S62126856 A JPS62126856 A JP S62126856A
Authority
JP
Japan
Prior art keywords
primary side
cores
magnets
secondary side
pole
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
JP26688985A
Other languages
Japanese (ja)
Inventor
Atsuji Karita
充二 苅田
Tsutomu Shintani
勉 新谷
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 JP26688985A priority Critical patent/JPS62126856A/en
Publication of JPS62126856A publication Critical patent/JPS62126856A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To increase a magnetic flux density from a permanent magnet and to prevent the magnet from being demagnetized by providing a primary side for generating a moving magnetic field and a secondary side having a plurality of permanent magnets and cores, and magnetizing the magnets in predetermined states. CONSTITUTION:The secondary side 20 of a linear motor is composed of a frame 21, a plurality of rectangular secondary cores 22 and platelike permanent magnets 23 mounted on the frame 21. The cores 22 and the magnets 23 are alternately disposed along the moving direction of the primary side 1 or the secondary side 20, the cores 22 are interposed between the same polarity pole faces of the magnets 23 and the faces of the cores 22 facing the primary side 1 thus alternately become N-pole and S-pole surfaces. The size of the set of the cores 22 and the magnets 23 along the moving direction of the primary side 1 or the secondary side 20 is equal to the pole pitch tau of the primary side 1. The height side H of the magnet 23 can be increased with this construction without limit.

Description

【発明の詳細な説明】 「産業上の利用分野」 この発明は、外部から供給されろ電気エネルギーを直接
直線的な機械的エネルギーに変換するリニアモータに係
り、特に、回転子内部に永久磁石を内蔵した永久磁石形
同期電動機と同(口の原理で動作するリニアモータに関
する。
Detailed Description of the Invention "Field of Industrial Application" This invention relates to a linear motor that directly converts electrical energy supplied from the outside into linear mechanical energy, and in particular, relates to a linear motor that directly converts electrical energy supplied from the outside into linear mechanical energy, and in particular, a linear motor that has a permanent magnet inside the rotor. This relates to a built-in permanent magnet type synchronous motor and a linear motor that operates on the same principle.

「従来の技術」 従来、永久磁石形同期71 ![11312!を直線状
に展開した構造のリニアモータとして第4図(イ)、(
ロ)に示すものが知られている。これらの図において、
1は一次側であり、1越2a、2a・・及び溝2b、2
b・・・か打ち抜かれた電気鉄板2.2・・・を11層
してなる一次側コア3と、各it+T 2 b、  2
 b・・・に各々巻き込まれたコイル4 u、4 v、
4 wとから(1■[戊されている。
"Conventional technology" Conventional permanent magnet type synchronous 71! [11312! Figure 4 (a) and (a) show a linear motor with a structure in which
The ones shown in b) are known. In these figures,
1 is the primary side, 1 over 2a, 2a... and grooves 2b, 2
A primary side core 3 made up of 11 layers of punched electric iron plates 2.2... and each it+T 2 b, 2
Coils 4 u, 4 v, respectively wound in b...
4 W andkara (1 ■ [Haved.

ここで、コイル4u、4v、4vに3tll交流を1共
拾すると、図に矢印Aまたは+3方向へ進行ずろ進行磁
界(磁束密度)が発生ずる。この進行磁界の゛IS波長
(半周JCI+の長さ)は特にポールピッチ(pole
 pitch)τと呼ばれる。一方、6は一次側1と空
隙Gを隔てて対向する二次側であり、長尺状のJ、(仮
7と、この基板7上に隣接して取り付けられた?U敗の
板状の永久磁石8,8・・・とから構成されている。こ
の場合、各永久磁石8,8・・・はポールピッチでと同
じ長さ寸法を有し、それらのN I・&而及びS極面が
交互に一次側1と対向オろように配置されている。また
、図には省略されているが、一次側1と二次側6の間に
は、空隙Gを保持才ろと、1(に、互いに図に示4′矢
印AまたはB方向へt多動自在に支持」゛る支持機!、
’4が設けられている。このような構成にtjいて、例
えば、一次側1を固定して、コイル4 u、4 v、4
 vsに3川交流を供給すると、永久磁C1影同期tI
ll!+機と同様の動f′ll11理に上って、一次側
1が発生土ろ進iテ磁界の1λ動速度に同期して二次側
6が矢印ΔまたはB方向へ移動する。同様に一1次側6
を固定しノー場合は一次側1が移動十ろ。
Here, if one 3tll alternating current is picked up in the coils 4u, 4v, and 4v, a magnetic field (magnetic flux density) is generated that advances in the direction of arrow A or +3 in the figure. The IS wavelength (half-circle JCI+ length) of this traveling magnetic field is particularly important for the pole pitch (pole pitch).
pitch) τ. On the other hand, 6 is a secondary side which faces the primary side 1 with a gap G in between, and has a long J, (temporary 7 and a ?U-shaped plate attached adjacent to this board 7). It is composed of permanent magnets 8, 8... In this case, each permanent magnet 8, 8... has the same length dimension as the pole pitch, and their N, I, and S poles. The surfaces are alternately arranged so as to face the primary side 1. Also, although not shown in the figure, a gap G is maintained between the primary side 1 and the secondary side 6. 1 (in addition, supporting machines that support each other in a freely movable manner in the direction of arrow A or B shown in the figure)
'4 is provided. With such a configuration, for example, the primary side 1 is fixed and the coils 4 u, 4 v, 4
When 3-river alternating current is supplied to vs, permanent magnetic C1 shadow synchronization tI
ll! Based on the same dynamic principle as in the machine, the secondary side 6 moves in the direction of the arrow Δ or B in synchronization with the 1λ dynamic speed of the generated magnetic field. Similarly, the primary side 6
If fixed, primary side 1 can be moved.

[発明が解決しよ・)と組る問題点」 ところで、−1= + 1−に構成のリニアモータにお
いて、効率良く推力をK)るためには、二次側6の永久
磁石8.8・・から発生ずる磁束密度を大とすることが
要求される。しかしながら、永久磁石8゜8 を隣接し
て並べて配置した構造であるため、磁束密度を大とする
ためには、高価な貴土類磁石を用いなければならないと
いう問題点があった。
By the way, in a linear motor configured as -1 = + 1-, in order to efficiently generate thrust K), the permanent magnet 8.8 on the secondary side 6 must be It is required to increase the magnetic flux density generated from... However, since it has a structure in which permanent magnets 8°8 are arranged side by side, there is a problem in that expensive precious earth magnets must be used in order to increase the magnetic flux density.

また、永久磁石8,8・・の各磁庫面が一次側1と21
向しているため、始動時などおいて、コイル・111、
・1ν、・Iwに突入電流が流れた場合、一次側コア3
の1″5歯2a、2a・から出た磁束が永久磁石8内を
t′lき、永久磁石8を減磁さυてしまうという問題が
あった。
In addition, each magnetic surface of the permanent magnets 8, 8... is the primary side 1 and 21.
Because it is facing the same direction, the coil 111,
When an inrush current flows through ・1ν, ・Iw, the primary core 3
There was a problem in that the magnetic flux emitted from the 1''5 teeth 2a, 2a of the magnet 8 travels within the permanent magnet 8, causing the permanent magnet 8 to be demagnetized.

この発明は上述した事情に鑑みてなされたらので、二次
側の永久磁石から発生ずる磁束密度を大とずろことがて
きるとノ(に、一次側で発生した磁束によって二次側の
永久磁石が減磁することがないリニアモータを1是供す
ることを目的としている。
This invention was made in view of the above-mentioned circumstances, so that when the magnetic flux density generated from the permanent magnet on the secondary side becomes large, the magnetic flux generated on the primary side causes the permanent magnet on the secondary side to The purpose is to provide a linear motor that does not become demagnetized.

「問題点を解決するための手段」 この発明は、進行磁界を発生土ろ一次側と、前記−次…
すの&li界発生而と面隙を隔てて対向し、11J1記
進行磁界の1多動力向に沿って交互に配列された(隻数
の永久磁石及びコアからなる二次側とをn INI+し
、前記各永久磁石は前記谷コアの前記一次側に対向する
各面が交互にN極面とS極面になるように着磁されてい
ることを特徴としている。
"Means for Solving the Problems" This invention provides a primary side of a soil filter that generates a traveling magnetic field, and the following...
Suno & Li field generators are opposed to each other across a face gap, and are arranged alternately along one multi-force direction of the traveling magnetic field described in 11J1. Each of the permanent magnets is characterized in that the respective surfaces of the valley core facing the primary side are magnetized so as to alternately serve as a north pole face and a south pole face.

1作用」 各永久磁石の、一次側の磁界発生面と直交セろ方向への
寸法を無制限に大と十ろごとができるので磁束密度を大
とずろことができ、また一次側で発生した磁束が二次側
のコア内を通過するため、姶すノ時に一次側に突入電流
が供給された場合などにおいてら永久磁石が減磁十ろこ
とがない。
1 action" The dimensions of each permanent magnet in the direction perpendicular to the magnetic field generation surface on the primary side can be adjusted to an unlimited size, so the magnetic flux density can be varied greatly, and the magnetic flux generated on the primary side Since the permanent magnet passes through the core of the secondary side, the permanent magnet will not be demagnetized even if an inrush current is supplied to the primary side at the same time.

「実施例」 以F、図面を参照し、この発明の実施例について説明1
′ろ、。
"Embodiments" Hereinafter, embodiments of the present invention will be explained 1 with reference to the drawings.
'reactor,.

第1図(イ)及び(ロ)はこの発明の一実施例の構成を
示十図であり、第・1図(イ)及び(ロ)の各部にχl
応4′ろ部分には同一のIT 、j;を付し、その説明
を6略4−ろ。
Figures 1 (a) and (b) are 10 diagrams showing the configuration of one embodiment of the present invention, and each part in Figures 1 (a) and (b) is
The same IT, j; is attached to the part corresponding to 4', and the explanation thereof is 6 or 4-ro.

これらの図にi5いて、20はリニアモータの二次側で
あり、例えばアルミ等の非磁性(4料にJ、って(1■
成された枠体21と、この枠体21上に取り(・I’l
lらイまた)9敗の直方体状の二次側コア22.22 
及び仮状の永久磁石23.23・・・とから構成されて
いる。この場合、二次側コア22.22・・及び永久磁
石23.23・は一次側Iまたは二次1!III Gの
I) YJJ方向(矢印AまたはB方向)に沿って交1
1に配置されろとノ1ζに、各二次側コア22.22は
永久磁石23.23・の同極面によって各々秋111、
これにより、h二次側コア22.22・・・の一次側1
に2を向ずろ谷面は交互にN圃面とS作曲となっている
。また、ひとつの二次側=1ア22と永久磁石23の組
みの、一次側1または二次側20の移動方向に沿う寸法
は、一次側1のポールピブヂrと等しくなっている。
In these figures, 20 is the secondary side of the linear motor, for example, non-magnetic material such as aluminum (4 materials, J, (1)
The frame 21 that has been made and the frame 21 that is
(Also) Rectangular parallelepiped secondary core with 9 losses 22.22
and temporary permanent magnets 23, 23... In this case, the secondary cores 22, 22... and the permanent magnets 23, 23 are the primary I or the secondary 1! III G of I) Intersect 1 along the YJJ direction (arrow A or B direction)
1 and 1ζ, each secondary core 22.22 is oriented 111 by the same polar plane of the permanent magnet 23.23, respectively.
As a result, h secondary side core 22, 22... primary side 1
The 2nd and 2nd valley sides are alternately N and S compositions. Further, the dimension of one pair of secondary side 1a 22 and permanent magnet 23 along the moving direction of the primary side 1 or the secondary side 20 is equal to the pole pivot r of the primary side 1.

このような(+育成によれば、各永久磁石23の高さ寸
法I【、つまり一次側1の各歯2a、2a・・・の5.
1面の磁界発生面と直交4°ろ方向の11法!1を11
1制限に大と4°ろことができるので、高f+lliな
貴」二類磁石などを用い4“に、安1dlIなフェライ
ト磁石などを用いて磁束密度を大とすることができろ。
According to such (+ growth), the height dimension I of each permanent magnet 23 is 5.
11 methods perpendicular to one magnetic field generation surface by 4 degrees! 1 to 11
Since it is possible to deviate from 1 degree to 4 degrees within the limit, the magnetic flux density can be increased by using a high f+lli noble class 2 magnet or the like, or by using a cheap 1dlI ferrite magnet or the like.

また始動時などにおいて、コイル・Iu、4v、4wに
突入′Xl1i流が流れた場合、一次側コア3のrst
442 n、 2 a  から出た磁束は各二次側コア
22.22・・・内を通過するため、従来のように永久
磁石23が711’dlしてしまうことがない。
In addition, when an inrush current flows through the coils Iu, 4v, and 4w during startup, etc., the
Since the magnetic flux emitted from 442 n, 2 a passes through each secondary core 22, 22..., the permanent magnet 23 does not move 711'dl as in the conventional case.

次に、第2図及び第3図は二の発明のその池の実施例の
(I■成を示す図である。
Next, FIGS. 2 and 3 are diagrams showing the construction of the pond according to the second embodiment of the invention.

ま「第2図において、上述した一実施例と異なる点は、
凸永久磁石23の高さ一1法11を一次側コア22より
も低くし、二次側コア22のg1部を取り除いて斜面2
2aを形成した点にある。この上゛)にすることにより
、永久磁石23.23  ・から発生し、空隙G内に広
がった磁束密度の分布状態が正弦波形に近づき、したが
って、いわゆるトルクリプルが減少し、低連移動時にお
ける動作の安定化か図られる。
``In FIG. 2, the points that differ from the above-mentioned embodiment are as follows.
The height of the convex permanent magnet 23 is made lower than the primary core 22, and the g1 portion of the secondary core 22 is removed to form the slope 2.
It is at the point where 2a was formed. By doing this, the distribution state of the magnetic flux density generated from the permanent magnet 23.23 and spread within the air gap G approaches a sine waveform, so that the so-called torque ripple is reduced, and the operation during low continuous movement. Stabilization will be attempted.

次に、第3図においては、第1図(イ)に示4−枠1(
ζ21を取り除いた二次側20aを秋むようにして一対
の一次側1a及びlb会設置Jでいろ。、な才j、この
図において、空隙Ga及びG l)を保111すると1
村に、二次側20aと一対の一次側1 a、 I bと
の間にJ5いて、互いに終りJ自+’Eに支持]゛ろ支
持機構の図示は省略されている。これによれば、一次側
1a及び1bの吸引力が互いに反対方向に発生するため
、R賊的なバランスが取れる。
Next, in FIG. 3, the 4-frame 1 (
Install a pair of primary sides 1a and LB by folding the secondary side 20a with ζ21 removed. In this figure, if the voids Ga and G l) are kept 111, then 1
The supporting mechanism is omitted in the figure.J5 is located between the secondary side 20a and the pair of primary sides 1a and Ib, and the ends of each other are supported at J+'E. According to this, the suction forces of the primary sides 1a and 1b are generated in opposite directions, so that an R-like balance can be achieved.

以上説明した6実施例において、一次側!と二次側20
(20a)のt11σの位置関係を検出し、この位2゛
シ検出信号に基づいてコrル4u、、1v、4wの励磁
を制i卸ず1tばザーボモータとしてrll用4゛ろこ
とがてきる。1ノニ、コギンク力を減少さするためには
、一般の回転四におけろスキューと同(L1こ、二次側
コア22と永久磁石23を、一次側1または二次側20
の1に動方向に対して直r「1方向ではなく、斜めの状
態となるように配置4ればよい。
In the six embodiments described above, the primary side! and secondary side 20
The positional relationship of t11σ in (20a) is detected, and based on the detected signal, the excitation of the coils 4u, 1v, and 4w is controlled. Ru. 1. In order to reduce the cogging force, the same as the skew in general rotation (L1), the secondary side core 22 and the permanent magnet 23 are connected to the primary side 1 or the secondary side 20.
1, it is only necessary to arrange it so that it is not in one direction but at an angle with respect to the direction of movement.

「発明の効果」 以上説明したように、この発明によれば、進行磁界を発
生する一次側と、前記一次側の磁界発生面と空隙を隔て
て対向し、1;J記進行磁界の移動方向に沿って交互に
配列された’I’d t’<の7に久磁石伎びコアから
なる二次側とを1備し、II:j記古永久磁石は前記各
コアの前記一次側に対向4゛る各面が交互にN極面とs
 +b而になるように青磁さ(1ているので、各永久磁
石の、一次側の磁界発生面と直交する方向への寸法を無
制限に大とすることができ、これにより、安価なフェラ
イト磁石などを用いた場合でも磁束密度を大とすること
ができ、さらに、一次側で発生した磁束が二次側のコア
内を通過4−るため、始動時に一次側に突入電流が供給
された場合などにおいてら永久磁石か減磁することhく
ないという効果が11られろ。
"Effects of the Invention" As explained above, according to the present invention, a primary side that generates a traveling magnetic field and a magnetic field generating surface of the primary side are opposed to each other across an air gap, and 1; II: j old permanent magnets are arranged alternately along the primary side of each of the cores. Each of the 4 opposing surfaces alternates with the N-pole surface and s
Since the celadon magnetism (1) is so as to be +b, the dimension of each permanent magnet in the direction perpendicular to the primary side magnetic field generation surface can be increased without limit. The magnetic flux density can be increased even when using This has the effect that permanent magnets do not demagnetize when placed in a magnet.

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

第1図(イ)はこの発明の一実施例の構成を示す一部切
り欠き正面図、第1図(ロ)は第1図(イ)のC−C線
i見断面図、第2図及び第3図はこの発明のその他の実
施例の構成を示す一部切り欠き正面図、第・1図(イ)
はtit来のリニアモータの構成を示−J−iE而面、
第4図(ロ)は第4図(イ)のD −1)線視図である
。 1・・ 一次側、2a・・・・・・1”19(磁界発生
面)、20・・二次側、22 ・・・二次側コア、23
・・・永久磁石、2!・・・枠体、G・・・・・・空隙
FIG. 1(a) is a partially cutaway front view showing the configuration of an embodiment of the present invention, FIG. 1(b) is a sectional view taken along line C-C in FIG. 1(a), and FIG. and FIG. 3 is a partially cutaway front view showing the configuration of another embodiment of the present invention, and FIG. 1 (A)
shows the configuration of the linear motor since Tit-J-iE surface,
FIG. 4(B) is a view taken along line D-1) of FIG. 4(A). 1...Primary side, 2a...1''19 (magnetic field generation surface), 20...Secondary side, 22...Secondary side core, 23
...Permanent magnet, 2! ...Frame, G...Void.

Claims (1)

【特許請求の範囲】[Claims] 進行磁界を発生する一次側と、前記一次側の磁界発生面
と空隙を隔てて対向し、前記進行磁界の移動方向に沿っ
て交互に配列された複数の永久磁石及びコアからなる二
次側とを具備し、前記各永久磁石は前記各コアの前記一
次側に対向する各面が交互にN極面とS極面になるよう
に着磁されていることを特徴とするリニアモータ。
a primary side that generates a traveling magnetic field, and a secondary side that faces the magnetic field generation surface of the primary side across an air gap and is made up of a plurality of permanent magnets and cores arranged alternately along the moving direction of the traveling magnetic field. A linear motor, characterized in that each of the permanent magnets is magnetized so that each surface facing the primary side of each core is alternately a N-pole surface and an S-pole surface.
JP26688985A 1985-11-27 1985-11-27 Linear motor Pending JPS62126856A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26688985A JPS62126856A (en) 1985-11-27 1985-11-27 Linear motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26688985A JPS62126856A (en) 1985-11-27 1985-11-27 Linear motor

Publications (1)

Publication Number Publication Date
JPS62126856A true JPS62126856A (en) 1987-06-09

Family

ID=17437058

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26688985A Pending JPS62126856A (en) 1985-11-27 1985-11-27 Linear motor

Country Status (1)

Country Link
JP (1) JPS62126856A (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0232750A (en) * 1988-07-20 1990-02-02 Shinko Electric Co Ltd Pulse motor
JPH02131350A (en) * 1988-11-08 1990-05-21 Shinko Electric Co Ltd Pulse motor
JPH02133060A (en) * 1988-11-14 1990-05-22 Shinko Electric Co Ltd Pulse motor
JPH0326470A (en) * 1989-06-16 1991-02-05 Robert Bosch Gmbh Angle driver
JPH03124254A (en) * 1989-10-05 1991-05-27 Shinko Electric Co Ltd Pulse motor
JPH03139160A (en) * 1989-10-20 1991-06-13 Shinko Electric Co Ltd Pulse motor
CN102684449A (en) * 2012-06-01 2012-09-19 哈尔滨工程大学 High-power density permanent magnet linear motor
CN105529900A (en) * 2016-01-28 2016-04-27 焦作市华鹰机电技术有限公司 Magnetic force balance type switch flux linkage linear motor

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0232750A (en) * 1988-07-20 1990-02-02 Shinko Electric Co Ltd Pulse motor
JPH02131350A (en) * 1988-11-08 1990-05-21 Shinko Electric Co Ltd Pulse motor
JPH02133060A (en) * 1988-11-14 1990-05-22 Shinko Electric Co Ltd Pulse motor
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JPH03139160A (en) * 1989-10-20 1991-06-13 Shinko Electric Co Ltd Pulse motor
CN102684449A (en) * 2012-06-01 2012-09-19 哈尔滨工程大学 High-power density permanent magnet linear motor
CN105529900A (en) * 2016-01-28 2016-04-27 焦作市华鹰机电技术有限公司 Magnetic force balance type switch flux linkage linear motor

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