JPH05276733A - Linear direct current motor - Google Patents

Linear direct current motor

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Publication number
JPH05276733A
JPH05276733A JP10067392A JP10067392A JPH05276733A JP H05276733 A JPH05276733 A JP H05276733A JP 10067392 A JP10067392 A JP 10067392A JP 10067392 A JP10067392 A JP 10067392A JP H05276733 A JPH05276733 A JP H05276733A
Authority
JP
Japan
Prior art keywords
pole
field magnets
width
thrust
armature
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
JP10067392A
Other languages
Japanese (ja)
Inventor
Manabu Shiraki
白木  学
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.)
Shicoh Engineering Co Ltd
Original Assignee
Shicoh Engineering 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 Shicoh Engineering Co Ltd filed Critical Shicoh Engineering Co Ltd
Priority to JP10067392A priority Critical patent/JPH05276733A/en
Publication of JPH05276733A publication Critical patent/JPH05276733A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain a smooth thrust ripple characteristic and to make the thrust larger by arranging and forming armature coils at equal intervals of a specified pitch respectively, and arranging and forming two sets of field magnets or more shifting their phases in the moving direction of a moving part by a specified distance respectively. CONSTITUTION:An armature 2 made by arranging armature coils 5 formed into the same width T as the pole width of field magnets 6 by a width pitch lambda(where lambda=T+T/8), and a stator having pole discriminating elements 7 are arranged at relatively moving positions to the field magnets 6. A moving part 3 has the field magnets 6 composed of 2 sets of field magnets 6A and 6B arranged with their phases shifted by a distance of pole width n(1+1/8)lambda (where n is an integer of 1 or larger, and lambda=T+T/8) in the moving direction of the moving part 3, on the inside bottom of a long platelike magnet yoke 8. The 2 sets of field magnets 6A and 6B are formed into a rectangular shape by arranging N- and S-magnetic poles of width T adjacent to each so that adjoining poles may be opposite poles to each other.

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,推力リップルの極めて
滑らかなリニア直流モ−タに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a linear DC motor having an extremely smooth thrust ripple.

【0002】[0002]

【従来技術】図4は,従来の多極多相型のリニア直流モ
−タとしての可動マグネット形リニア直流ブラシレスモ
−タ1−1で,これについて以下に説明する。この可動
マグネット形リニア直流ブラシレスモ−タ1−1は,図
示しない直動案内レ−ルに電機子2を配置し,上記直動
案内レ−ルに沿って移動子3−1が直線移動するように
構成されている。
2. Description of the Related Art FIG. 4 shows a movable magnet type linear DC brushless motor 1-1 as a conventional multi-pole / multi-phase type linear DC motor, which will be described below. In this movable magnet type linear DC brushless motor 1-1, an armature 2 is arranged on a linear motion guide rail (not shown), and a mover 3-1 moves linearly along the linear motion guide rail. Is configured.

【0003】図示せず直動案内レ−ルは,固定側のステ
−タヨ−クを兼ねるために磁性体でできたものを用いて
おり,その直動案内レ−ル面に適宜な手段を用いて図示
せず導電プリント配線パタ−ンを形成した長板状のプリ
ント配線基板4を配置している。
A linear motion guide rail (not shown) is made of a magnetic material in order to serve also as a stationary yoke on the fixed side, and an appropriate means is provided on the linear motion guide rail surface. A long plate-shaped printed wiring board 4 on which a conductive printed wiring pattern is formed (not shown) is arranged.

【0004】この場合,直動案内レ−ル3が磁性体でで
きたものでない場合には,磁性体板を介した後に,上記
プリント配線基板4を配置する。
In this case, when the linear guide rail 3 is not made of a magnetic material, the printed wiring board 4 is arranged after the magnetic material plate is interposed.

【0005】プリント配線基板4面には,移動子3−1
の長手方向に沿って空心型の電機子コイル5群をそれぞ
れλ(但し,λ=T+T/8。Tは界磁マグネット6−
1の一磁極の幅)ピッチの等間隔配置で,互いに重なら
ないように隣接配置してコアレス構造のコアレスステ−
タ電機子2を形成している。
On the surface of the printed wiring board 4, a moving element 3-1 is provided.
Of the air-core type armature coils 5 along the longitudinal direction of λ (where λ = T + T / 8, where T is the field magnet 6-
The width of one magnetic pole is equal to one pitch, and the coreless stations of the coreless structure are arranged adjacent to each other so as not to overlap each other.
The armature 2 is formed.

【0006】電機子コイル5について説明すると,この
電機子コイル5は,矩形枠状の空心型のものとなるよう
に導線を用いて多数タ−ン巻回して形成されたものであ
るが,プリント手段,めっき手段あるいはエッチング手
段を用いたシ−トコイル等にて形成したものでも良い。
Explaining the armature coil 5, the armature coil 5 is formed by winding a large number of turns using a conductive wire so as to form an air-core type having a rectangular frame shape. It may be formed by a sheet coil using a means, a plating means or an etching means.

【0007】かかる空心型の電機子コイル5群による
と,効率及び性能の良好なリニア往復180度通電方式
を採用することができるように,移動子3の走行方向と
直交する方向に延びた推力の発生に寄与する2つの有効
導体部5aと5aとの開角が,後記する界磁マグネット
6−1の移動子3の走行方向におけるN極,S極の一磁
極幅をTとする時,該一磁極幅Tの開角となるように巻
線形成する。
According to the air-core type armature coil group 5 as described above, the thrust force extending in the direction orthogonal to the traveling direction of the moving element 3 is adopted so that the linear reciprocating 180-degree energization method with good efficiency and performance can be adopted. When the opening angle between the two effective conductors 5a and 5a that contributes to the generation of the magnetic field is a magnetic pole width of the N pole and the S pole in the traveling direction of the mover 3 of the field magnet 6-1 described later, The winding is formed so as to have an opening angle of the one magnetic pole width T.

【0008】尚,電機子コイル5において,移動子3の
移動方向と平行な2つの導体部5bは,あまり推力の発
生に寄与しない導体部となっている。
In the armature coil 5, the two conductor portions 5b parallel to the moving direction of the mover 3 are conductor portions that do not contribute much to the generation of thrust.

【0009】また電機子コイル5は,上記推力の発生に
寄与しない2つの導体部5bと導体部5bの外側までの
長さが,界磁マグネット6−1のその方向の幅よりも少
し短い長さのものに形成している。
In the armature coil 5, the length between the two conductor portions 5b that do not contribute to the generation of the thrust and the outside of the conductor portion 5b is slightly shorter than the width of the field magnet 6-1 in that direction. It is formed into a thing.

【0010】プリント配線基板4には,電機子コイル5
群及び界磁マグネット6の磁極状態に応じて電機子コイ
ル5群の通電の切り換えを行うための位置検知用として
のホ−ル素子等の磁極判別素子7を配置し,電機子コイ
ル5磁極判別素子7に電源を供給すると共に,出力信号
を得るための図示しない導電配線パタ−ンを形成してい
る。
The printed wiring board 4 has an armature coil 5
The magnetic pole discriminating element 7 such as a hall element for position detection for switching the energization of the armature coil 5 group according to the magnetic pole state of the group and the field magnet 6 is arranged to discriminate the magnetic pole of the armature coil 5. A power supply is supplied to the element 7 and a conductive wiring pattern (not shown) for obtaining an output signal is formed.

【0011】上記磁極判別素子7としては,ホ−ルI
C,ホ−ル素子,磁気抵抗素子等の適宜な磁電変換素子
を用いれば良い。
The magnetic pole discriminating element 7 is a hole I.
An appropriate magnetoelectric conversion element such as C, a hall element, a magnetoresistive element or the like may be used.

【0012】磁極判別素子7群は,それぞれ電機子コイ
ル5の発生推力に寄与する導体部5aと該導体部5aと
直交して形成された推力の発生に寄与しない導体部5b
とが交叉する導体部延長線上の界磁マグネット6−1と
対向する上記プリント配線基板4面位置に配設し,上記
界磁マグネット6−1のN極,S極の磁極を検出するこ
とができるようにしている。
The magnetic pole discriminating element 7 group includes a conductor portion 5a which contributes to the thrust generated by the armature coil 5 and a conductor portion 5b which is formed orthogonal to the conductor portion 5a and does not contribute to thrust generation.
The magnetic poles of the N pole and the S pole of the field magnet 6-1 can be detected by arranging them on the surface of the printed wiring board 4 facing the field magnet 6-1 on the conductor extension line intersecting with and. I am able to do it.

【0013】磁極判別素子7からの,上記界磁マグネッ
ト6−1のN極,S極の磁極に応じた出力信号に基づい
て図示しない通電制御回路内のドライバ−が作動して所
定方向の推力が発生するように上記電機子コイル5群に
適宜方向の通電を行う。
A driver in an energization control circuit (not shown) operates based on an output signal from the magnetic pole discriminating element 7 corresponding to the magnetic poles of the N pole and the S pole of the field magnet 6-1 to operate thrust in a predetermined direction. So that the armature coil group 5 is energized in an appropriate direction.

【0014】上記電機子2と相対的直線移動する移動子
3は,長板状のマグネットヨ−ク8−1の下部内面の上
記電機子2と対向する面に空隙を介して界磁マグネット
6−1を設けて相対的移動するように構成している。
The mover 3 which moves linearly relative to the armature 2 has a field magnet 6 on the inner surface of the lower portion of the elongated plate-shaped magnet yoke 8-1 which faces the armature 2 with a gap. -1 is provided to make relative movement.

【0015】マグネットヨ−ク8−1の下部内面には,
上記移動子3の移動方向に沿って隣り配置の磁極が異極
となるようにT幅に形成したN極,S極の磁極をP(P
は2以上の整数)個等間隔に隣接配置して形成した10
極の界磁マグネット6−1を接着剤などの適宜な手段を
用いて固設している。
On the inner surface of the lower portion of the magnet yoke 8-1,
P (P
Is an integer greater than or equal to 2) 10 formed by adjoining at equal intervals.
The pole field magnet 6-1 is fixed by using an appropriate means such as an adhesive.

【0016】[0016]

【従来技術の問題点】以上のような構成からなる可動マ
グネット形リニア直流ブラシレスモ−タ1−1では,移
動子3−1が移動した場合に得られる推力(トルク)リ
ップルは,図5に示すように得られる。
2. Description of the Related Art In the movable magnet type linear DC brushless motor 1-1 having the above structure, the thrust (torque) ripple obtained when the mover 3-1 moves is shown in FIG. Obtained as shown.

【0017】図5を参照して更に説明すると,いま電機
子コイル5群は互いにλ(T+T/8)ピッチの,等間
隔配置に配置して電機子2を形成し,界磁マグネット6
−1の5極のみを取り上げるものとすると,界磁マグネ
ット6−1が電機子2と相対的移動した場合,上記λの
範囲における推力リップル曲線9−1は,図5に示すよ
うに推力リップルの荒いものとなって現れる。
Explaining further with reference to FIG. 5, the armature coil groups 5 are now arranged at equal intervals of λ (T + T / 8) pitch to form the armature 2 and the field magnet 6 is formed.
Assuming that only the five poles of -1 are taken, when the field magnet 6-1 moves relative to the armature 2, the thrust ripple curve 9-1 in the range of λ above shows the thrust ripple as shown in FIG. Appears as a rough thing.

【0018】この種の,可動マグネット形リニア直流ブ
ラシレスモ−タ1−1は,コアレス構造で,しかも多相
の構造となっているため,リニアパルスモ−タや有鉄心
形リニア直流モ−タに比較して極めて滑らかな推力リッ
プル特性を持つものとして高精密測定器などに採用され
ている。
Since the movable magnet type linear DC brushless motor 1-1 of this kind has a coreless structure and a multi-phase structure, it can be used as a linear pulse motor or an iron core type linear DC motor. It is used in high-precision measuring instruments, etc., as it has extremely smooth thrust ripple characteristics in comparison.

【0019】ここに,半導体製造装置などの更に高精度
の要求される装置において使用されるリニア直流モ−タ
では,更に滑らかな推力リップル特性を要求される。
Here, a smoother thrust ripple characteristic is required for a linear DC motor used in an apparatus requiring higher precision such as a semiconductor manufacturing apparatus.

【0020】[0020]

【本発明の課題】本発明は,上記した可動マグネット形
リニア直流ブラシレスモ−タ1−1などのリニア直流モ
−タをわずかな設計変更を試すのみで,従来のものに比
較して推力リップル数を2倍にすることで,1/2倍に
推力リップルを押さえて極めて滑らかに移動子を走行で
きるように構成すると共に,合成推力特性をも向上させ
ることを課題になされたものである。
SUMMARY OF THE INVENTION According to the present invention, a thrust ripple is compared with a conventional one by only making a slight design change to a linear DC motor such as the movable magnet type linear DC brushless motor 1-1 described above. By doubling the number, it is a subject to suppress the thrust ripple to ½ and to make the moving element run extremely smoothly, and to improve the combined thrust characteristics.

【0021】[0021]

【本発明の課題達成手段】かかる本発明の課題は,上記
電機子を構成する電機子コイルをそれぞれλピッチの等
間隔配置で形成し,上記界磁マグネットは2組以上で形
成し,該2組以上の界磁マグネットはそれぞれn(1+
1/8)λ磁極幅(但し,λ=T+T/8)の距離だけ
移動子の移動方向に位相をずらせて配置形成することに
よって達成できる。
The object of the present invention is to form the armature coils constituting the armature at regular intervals of λ pitch, and to form the field magnets in two or more sets. The field magnets of more than one set are n (1+
This can be achieved by arranging and forming the magnetic pole width of 1/8) (where λ = T + T / 8) with the phase shifted in the moving direction of the moving element.

【0022】[0022]

【発明の作用】2組の5極の界磁マグネット6Aと6B
を略々(1+1/8)λ磁極幅(但し,λ=T+T/
8)の距離だけ移動子3の移動方向に位相をずらせて配
置形成した界磁マグネット6を用いているため,移動子
3が移動した場合に得られる推力(トルク)リップル
は,図3に示すように得られ,5極の界磁マグネット6
A,6Bそれぞれが電機子2と相対的移動した場合,上
記λの範囲における5極の界磁マグネット6A,6Bそ
れぞれによって得られる推力リップル曲線9A,9Bの
ように互いに(1+1/8)λ位相がずれ,極めて滑ら
かな推力リップル特性が得られるのみならず,2つの推
力リップル曲線9A,9Bが合成された合成推力曲線1
0も高い推力レベルとなるため,より大きな推力を得る
ことのできる可動マグネット形リニア直流ブラシレスモ
−タ1となる。
Operation of the invention Two sets of five-pole field magnets 6A and 6B
Is approximately (1 + 1/8) λ magnetic pole width (where λ = T + T /
Since the field magnet 6 arranged and formed with the phase shifted by the distance of 8) in the moving direction of the moving element 3 is used, the thrust (torque) ripple obtained when the moving element 3 moves is shown in FIG. 5 pole magnetic field magnet 6
When A and 6B move relative to the armature 2, the thrust ripple curves 9A and 9B obtained by the five-pole field magnets 6A and 6B in the range of λ are (1 + 1/8) λ Deviation, and not only a very smooth thrust ripple characteristic is obtained, but also a combined thrust curve 1 in which two thrust ripple curves 9A and 9B are combined.
Since 0 is a high thrust level, it is a movable magnet type linear DC brushless motor 1 that can obtain a larger thrust.

【0023】[0023]

【本発明の実施例】図1は,本発明の可動マグネット形
リニア直流ブラシレスモ−タ1の概略分解斜視図で,図
2は同リニア直流ブラシレスモ−タ1の界磁マグネット
6と電機子コイル5群からなる電機子2との展開図で,
図3は本発明によって得られる推力リップル曲線及び合
成推力曲線の説明図で,上記図4及び図5を参照して説
明した共通する箇所説明を省略し,異なる箇所において
のみ,以下に本発明の説明を行う。また共通する箇所
は,同じ符号を用いて説明する。
1 is a schematic exploded perspective view of a movable magnet type linear DC brushless motor 1 of the present invention, and FIG. 2 is a field magnet 6 and armature of the linear DC brushless motor 1. In the development view with the armature 2 consisting of 5 coils,
FIG. 3 is an explanatory view of a thrust ripple curve and a combined thrust curve obtained by the present invention, omitting the description of the common parts described with reference to FIGS. I will explain. Also, common points will be described using the same reference numerals.

【0024】本発明の可動マグネット形リニア直流ブラ
シレスモ−タ1では,上記リニア直流ブラシレスモ−タ
1−1同様に推力に寄与する導体部5aと5aの開角幅
を界磁マグネット6−1の一磁極幅Tと同じT幅に形成
した電機子コイル5をλ(但し,λ=T+T/8)幅ピ
ッチで配設した電機子2と,上記条件と同じ条件位置に
配設した磁極判別素子7を持つ固定子を,後記する界磁
マグネット6と相対的移動する位置に配設している点
は,上記可動マグネット形リニア直流ブラシレスモ−タ
1−1同様で,異なる点は界磁マグネット6を持つ移動
子3の構成にある。
In the movable magnet type linear DC brushless motor 1 of the present invention, like the linear DC brushless motor 1-1, the open angle width of the conductor portions 5a and 5a contributing to the thrust is set to the field magnet 6-1. The armature coil 5 formed with the same T width as the one magnetic pole width T is arranged at a λ (where λ = T + T / 8) width pitch, and the magnetic pole discrimination arranged at the same condition position as the above condition. The stator having the element 7 is arranged at a position that moves relative to the field magnet 6 described later, as in the movable magnet type linear DC brushless motor 1-1 described above. This is in the configuration of the mover 3 having the magnet 6.

【0025】移動子3は,上記マグネットヨ−ク8−1
同様の長板状のマグネットヨ−ク8の内部下面に2組の
界磁マグネット6Aと6Bを略々n(1+1/8)λ
(nは1以上の整数。この実施例で,n=1を選択して
いる)磁極幅(但し,λ=T+T/8)の距離だけ移動
子3の移動方向に位相をずらせて配置形成した界磁マグ
ネット6を設ける。
The mover 3 is the magnet yoke 8-1.
Two sets of field magnets 6A and 6B are formed on the inner lower surface of a similar long plate-shaped magnet yoke 8 in a substantially n (1 + 1/8) λ range.
(N is an integer greater than or equal to 1. In this embodiment, n = 1 is selected) The magnetic pole width is arranged and formed by shifting the phase in the moving direction of the moving element 3 by a distance of λ = T + T / 8. A field magnet 6 is provided.

【0026】2組の界磁マグネット6A,6Bは,隣接
する磁極が異極となるように略々T幅の磁極のN極,S
極の磁極を隣接配置して形成した5極の長板状のものに
形成する。
The two sets of field magnets 6A and 6B have N-poles and S-poles of approximately T-width so that adjacent magnetic poles have different poles.
It is formed as a five-pole elongated plate formed by arranging magnetic poles adjacent to each other.

【0027】2組の界磁マグネット6Aと6B間のマグ
ネットヨ−ク8間には,樹脂,接着剤,銅,アルミニウ
ム等の非磁性体からなる界磁マグネット位置決め部材1
1を設けている。
Between the two pairs of field magnets 6A and 6B, between the magnet yokes 8 is a field magnet positioning member 1 made of a non-magnetic material such as resin, adhesive, copper or aluminum.
1 is provided.

【0028】以上のような2組の界磁マグネット6Aと
6Bから構成された界磁マグネット6を持つ移動子3と
磁極判別素子7群及び電機子コイル5群からなる電機子
2との展開図は,図2に示すように現すことができる。
A development view of the mover 3 having the field magnet 6 composed of the two sets of field magnets 6A and 6B as described above, and the armature 2 including the magnetic pole discriminating element 7 group and the armature coil 5 group. Can be represented as shown in FIG.

【0029】尚,磁極判別素子7としては,4端子ホ−
ル素子を用いるものとし,2つの電源端子及び2つの出
力端子は,図示しない制御回路に接続する。
As the magnetic pole discriminating element 7, a 4-terminal hole is used.
2 power supply terminals and 2 output terminals are connected to a control circuit (not shown).

【0030】制御回路の電源が閉成され,可動マグネッ
ト形リニア直流ブラシレスモ−タ1を動作可能な状態に
しておくと,界磁マグネット6A,6BのN極,S極の
磁極を検出している磁極判別素子7からの出力に基づい
て,当該界磁マグネット6A,6Bと対向している電機
子コイル5には,所定方向の通電がなされ,所定方向の
推力を得て移動子3は,所定方向に図示しないエンコ−
ダと制御回路からの信号に制御されて走り出す。
When the power source of the control circuit is closed and the movable magnet type linear DC brushless motor 1 is in an operable state, the magnetic poles of the N pole and S pole of the field magnets 6A and 6B are detected. Based on the output from the magnetic pole discriminating element 7, the armature coil 5 facing the field magnets 6A and 6B is energized in a predetermined direction, and a thrust force in a predetermined direction is obtained to move the mover 3. Encoder not shown in the specified direction
Starts under the control of signals from the control circuit.

【0031】可動マグネット形リニア直流ブラシレスモ
−タ1の場合,2組の5極の界磁マグネット6Aと6B
を略々(1+1/8)λ磁極幅(但し,λ=T+T/
8)の距離だけ移動子3の移動方向に位相をずらせて配
置形成した界磁マグネット6を用いているため,移動子
3が移動した場合に得られる推力(トルク)リップル
は,図3に示すように得られる。
In the case of the movable magnet type linear DC brushless motor 1, two sets of 5-pole field magnets 6A and 6B are used.
Is approximately (1 + 1/8) λ magnetic pole width (where λ = T + T /
Since the field magnet 6 arranged and formed with the phase shifted by the distance of 8) in the moving direction of the moving element 3 is used, the thrust (torque) ripple obtained when the moving element 3 moves is shown in FIG. Is obtained as.

【0032】図3を参照して更に説明すると,いま電機
子コイル5群は互いにλ(T+T/8)ピッチの,等間
隔配置に配置して電機子2を形成し,5極の界磁マグネ
ット6A,6Bそれぞれが電機子2と相対的移動した場
合,上記λの範囲における5極の界磁マグネット6A,
6Bそれぞれによって得られる推力リップル曲線9A,
9Bのように互いに(1+1/8)λ位相がずれて得ら
れる。
Explaining further with reference to FIG. 3, now, the armature coil groups 5 are arranged at equal intervals of λ (T + T / 8) pitch to form the armature 2 and form a 5-pole field magnet. When each of 6A and 6B moves relative to the armature 2, a 5-pole field magnet 6A,
6B, thrust ripple curves 9A,
9B, the phases are (1 + 1/8) λ deviated from each other.

【0033】2つの推力リップル曲線9A,9Bによれ
ば,従来の可動マグネット形リニア直流ブラシレスモ−
タ1−1によって得られる図5に示す推力リップル曲線
9−1に比較して2倍のリップル数が得られるので,2
つの推力リップル曲線9A,9Bが合成された推力リッ
プル曲線は,従来図5に示す推力リップル曲線9−1に
比較して1/2の滑らかな推力リップル特性を持つ極め
て滑らかな推力リップル特性の可動マグネット形リニア
直流ブラシレスモ−タ1を得ることができる。
According to the two thrust ripple curves 9A and 9B, the conventional movable magnet type linear DC brushless motor is used.
2 is obtained because the double ripple number is obtained as compared with the thrust ripple curve 9-1 shown in FIG.
The thrust ripple curve composed of the two thrust ripple curves 9A and 9B has an extremely smooth thrust ripple characteristic that is 1/2 as smooth as the thrust ripple curve 9-1 shown in FIG. The magnet type linear DC brushless motor 1 can be obtained.

【0034】また従来の可動マグネット形リニア直流ブ
ラシレスモ−タ1−1によって得られる図5に示す推力
リップル曲線9−1に比較して2倍のリップル数が得ら
れるので,2つの推力リップル曲線9A,9Bが合成さ
れた合成推力曲線10も図3に示すように,高い推力レ
ベルとなるためより大きな推力を得ることのできる可動
マグネット形リニア直流ブラシレスモ−タ1を得ること
ができる。
Further, as compared with the thrust ripple curve 9-1 shown in FIG. 5 obtained by the conventional movable magnet type linear DC brushless motor 1-1, the number of ripples is doubled, so that two thrust ripple curves are obtained. As shown in FIG. 3, the combined thrust curve 10 in which 9A and 9B are combined also has a high thrust level, so that the movable magnet type linear DC brushless motor 1 capable of obtaining a larger thrust can be obtained.

【0035】[0035]

【その他の実施例】上記実施例では,2組の5極の界磁
マグネット6A,6Bを用いた例を示したが,それぞれ
の界磁マグネットは3極以上のもので形成しても良く,
また本発明の効果が得られるように配設してあるならば
3組以上の界磁マグネットを用いて形成しても良く,ま
た電機子側を移動子とし,界磁マグネット側を固定子と
した可動電機子型リニア直流モ−タに形成しても良いこ
とは言うまでもない。更にまた,リニア直流ブラシレス
モ−タに限らず,ブラシとコミュテ−タを用いて整流す
る形式のリニア直流モ−タにも当然本発明は適用され
る。
Other Embodiments In the above embodiment, an example using two sets of five-pole field magnets 6A and 6B is shown, but each field magnet may be formed of three or more poles.
Further, if it is arranged so as to obtain the effect of the present invention, it may be formed by using three or more sets of field magnets, and the armature side is the moving element and the field magnet side is the stator. It goes without saying that the movable armature type linear DC motor may be formed. Furthermore, the present invention is naturally applied to not only linear DC brushless motors but also linear DC motors of the type that uses a brush and a commutator for rectification.

【0036】[0036]

【発明の効果】本発明のリニア直流モ−タによれば,わ
ずかにN極,S極の磁極を隣接配置して形成した界磁マ
グネットを2組以上で形成し,該2組以上の界磁マグネ
ットをそれぞれn(1+1/8)λ(nは1以上の整
数)磁極幅(但し,λ=T+T/8)の距離だけ移動子
の移動子の移動方向に位相をずらせて配置形成したする
のみで,従来のものに比較して極めて推力リップル特性
をなめらかにでき,また推力特性を向上させることがで
きる。
According to the linear DC motor of the present invention, two or more sets of field magnets are formed by slightly arranging N and S poles adjacent to each other. The magnetic magnets are arranged and formed by shifting the phase in the moving direction of the moving element of the moving element by a distance of n (1 + 1/8) λ (n is an integer of 1 or more) magnetic pole width (where λ = T + T / 8). Only by doing so, the thrust ripple characteristic can be made extremely smooth and the thrust characteristic can be improved compared to the conventional one.

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

【図1】 本発明の1実施例を示す多極多相型の可動マ
グネット形リニア直流ブラシレスモ−タの概略分解斜視
図ある。
FIG. 1 is a schematic exploded perspective view of a multipole / multiphase movable magnet type linear DC brushless motor according to an embodiment of the present invention.

【図2】 同リニア直流ブラシレスモ−タの2組の界磁
マグネットと電機子コイル群からなる電機子との展開図
である。
FIG. 2 is a development view of two sets of field magnets and an armature including an armature coil group of the same linear DC brushless motor.

【図3】 同リニア直流ブラシレスモ−タによって得ら
れる推力リップル曲線及び合成推力曲線の説明図であ
る。
FIG. 3 is an explanatory diagram of a thrust ripple curve and a combined thrust curve obtained by the linear DC brushless motor.

【図4】 従来の多極多相型の可動マグネット形リニア
直流ブラシレスモ−タの概略分解斜視図ある。
FIG. 4 is a schematic exploded perspective view of a conventional multi-pole / multi-phase movable magnet type linear DC brushless motor.

【図5】 同リニア直流ブラシレスモ−タによって得ら
れる推力リップル曲線の説明図である。
FIG. 5 is an explanatory diagram of a thrust ripple curve obtained by the linear DC brushless motor.

【符号の説明】[Explanation of symbols]

1,1−1 可動マグネット形リニア直流ブラシレスモ
−タ 2 コアレスステ−タ電機子 3 移動子 4 プリント配線基板 5 電機子コイル 5a 推力の発生に寄与する導体部 5b 推力の発生に寄与しない導体部 6,6A,6B,6−1 界磁マグネット 7 磁極判別素子 8,8−1 マグネットヨ−ク 9A,9B,9−1 推力リップル曲線 10 合成推力曲線 11 界磁マグネット位置決め部材
1,1-1 Movable magnet type linear DC brushless motor 2 Coreless stator Armature 3 Moving element 4 Printed wiring board 5 Armature coil 5a Conductor part 5b that contributes to thrust generation 5b Conductor part that does not contribute to thrust generation 6 , 6A, 6B, 6-1 Field magnet 7 Magnetic pole discrimination element 8, 8-1 Magnet yoke 9A, 9B, 9-1 Thrust ripple curve 10 Combined thrust curve 11 Field magnet positioning member

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 移動子の走行方向に沿って隣接する磁極
が異極となるようにT幅の等しい幅で着磁されたN極,
S極の磁極を有するP(Pは2以上の整数)極の界磁マ
グネットを備え,該界磁マグネットと相対的移動するよ
うに電機子コイルを等間隔配置して形成した電機子を備
え,該電機子若しくは上記界磁マグネットのいずれか一
方を移動子とし,他方を固定子としたリニア直流モ−タ
において,上記電機子を構成する電機子コイルはそれぞ
れλ(但し,λ=T+T/8)ピッチの等間隔配置で形
成し,上記界磁マグネットは2組以上で形成し,該2組
以上の界磁マグネットはそれぞれn(1+1/8)λ
(nは1以上の整数)磁極幅の距離だけ移動子の移動子
の移動方向に位相をずらせて配置形成したことを特徴と
するリニア直流モ−タ。
1. An N pole magnetized with a width equal to T width so that adjacent magnetic poles along the traveling direction of the mover have different poles.
A field magnet having a P (P is an integer of 2 or more) pole having an S pole, and armatures formed by arranging armature coils at equal intervals so as to move relative to the field magnet, In a linear DC motor having one of the armature and the field magnet as a mover and the other as a stator, the armature coils constituting the armature are each λ (where λ = T + T / 8). ) The magnetic field magnets are formed at equal intervals, and the field magnets are formed in two or more sets, and each of the two or more sets of field magnets is n (1 + 1/8) λ.
(N is an integer of 1 or more) A linear DC motor characterized in that it is arranged and formed by shifting the phase of the moving element in the moving direction of the moving element by the distance of the magnetic pole width.
JP10067392A 1992-03-26 1992-03-26 Linear direct current motor Pending JPH05276733A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10067392A JPH05276733A (en) 1992-03-26 1992-03-26 Linear direct current motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10067392A JPH05276733A (en) 1992-03-26 1992-03-26 Linear direct current motor

Publications (1)

Publication Number Publication Date
JPH05276733A true JPH05276733A (en) 1993-10-22

Family

ID=14280286

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10067392A Pending JPH05276733A (en) 1992-03-26 1992-03-26 Linear direct current motor

Country Status (1)

Country Link
JP (1) JPH05276733A (en)

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