JPS59213274A - Linear pulse motor - Google Patents

Linear pulse motor

Info

Publication number
JPS59213274A
JPS59213274A JP8793783A JP8793783A JPS59213274A JP S59213274 A JPS59213274 A JP S59213274A JP 8793783 A JP8793783 A JP 8793783A JP 8793783 A JP8793783 A JP 8793783A JP S59213274 A JPS59213274 A JP S59213274A
Authority
JP
Japan
Prior art keywords
slider
magnetic
motor
excitation
magnetic 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.)
Granted
Application number
JP8793783A
Other languages
Japanese (ja)
Other versions
JPH0118667B2 (en
Inventor
Hiroshi Nakagawa
洋 中川
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.)
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 JP8793783A priority Critical patent/JPS59213274A/en
Publication of JPS59213274A publication Critical patent/JPS59213274A/en
Priority to US07/105,447 priority patent/US4761574A/en
Publication of JPH0118667B2 publication Critical patent/JPH0118667B2/ja
Granted 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

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Electromagnetism (AREA)
  • Power Engineering (AREA)
  • Linear Motors (AREA)

Abstract

PURPOSE:To alleviate the influence to the thermal expansion of a core and to reduce noise of a linear pulse motor by applying magnetically attracting forces of steps of a slider of the motor symmetrically to the center line of advancing direction. CONSTITUTION:A linear pulse motor is driven and controlled by a magnetic flux based on a permanent magnet 18 and a magnetic flux based on the excitation of coils 20, 21 provided on a toothed pole for a slider 12. The motor is incremented by the excitation of the poles 13a-13d, 14a-14d, 15a-15d disposed substantially at the equal distance to the center in the advancing direction of the slider 12, and the magnetic fluxes are generated independently at the respective poles. With such a structure, since the magnetically attracting forces of the steps of the motor are applied to the substantially symmetrical positions from the center of the slider 12 in the longitudinal direction of the slider 12, the balance at the front and rear can be always maintained, thereby eliminating the longitudinal movement. In this manner the influence to the thermal expansion of the core can be alleviated, and noise can be reduced.

Description

【発明の詳細な説明】 この発明は永久磁石からの磁束と各相励磁コイルの励磁
(lこ基づく磁束との相互イ′[用V(より動(Il、
 −J″るリニアパルスモークの構造に関するもので、
t’+ /:)。
DETAILED DESCRIPTION OF THE INVENTION This invention provides mutual interaction between magnetic flux from a permanent magnet and magnetic flux based on the excitation (Il,
- Concerning the structure of linear pulse smoke,
t'+ /:).

一般にり一了ノくルスモークはlr線イ)復旬’+ V
Cbklる(1確な位置決めを目的とし、た装尚゛例λ
−は数(11」制御に基つ< 、1−1’1機(戒の【
月動部、あるいtllプリり・\ノドの駆動j慴ISに
採用することか考慮さ、l′する。
Generally speaking, the smoke is lr line a) revival' + V
Cbkl (1 For the purpose of accurate positioning, the modified example λ
- is based on the number (11) control < , 1-1'1 machine (Kai's [
I'm considering whether to adopt it for the monthly movement part or the tll pre-throat drive IS.

ところで、rIt来のこの種のリニアパルスモーク目そ
の)〕;−理の一例を示すと第」図に小才構造かある。
By the way, to give an example of this kind of linear pulse smoke order since rIt;

すなわち、同第1図において、1シ1スノ1−ルて、k
llllしく歯部1aが長手方向に連λヅL的に形成さ
れ一〇いる。2 iI:lスライダーで、2個の南部9
1ノ(J−2a、2b4>Ic久(lFlイーi 2 
c Kて連結(7−c構成す11、各1′)、・し・2
a、2t)の歯部2 a、、 2 a2.2 b、、 
2 b。
In other words, in FIG.
The tooth portions 1a are formed in a continuous manner in the longitudinal direction. 2 iI:l slider, two southern 9
1 no (J-2a, 2b4>Icku (lFl E i 2
c Connect by K (7-c consists of 11, each 1'), ・2
a, 2t) tooth part 2 a,, 2 a2.2 b,,
2 b.

C」、1/1小のtll’lすv(南部2 a、 、 
2 a2及o’ Ih jolt 2 b、 、 2b
2ぞλ′1ぞれの間隔はス)1−ル爾部1aに4.・り
る1/2ヒツチのすれを有1−2、南部2a 、2bと
u ス’r −ル歯昌13」aン(おける’/4ビノナ
のずれを牛しる。Lう(t(l固)J−さJするo 2
 d 、 2 e klコイルで、二Jイル2 d (
Iel、山部2 a、 、 2 a2に71シて巻回し
方向を)又メ・Iにして連続的に装着される。もう−力
の=ノイル2C姓1鉄・し=2bの各歯部2 b、 、
 21.)2に図示の1川りの巻回し方向にて装ノθさ
れている。
C", 1/1 small tll'lsuv (Southern 2 a, ,
2 a2 and o' Ih jolt 2 b, , 2b
The spacing between 2 and λ'1 is 4.・The gap between Ruru 1/2 hits is 1-2, southern part 2a, 2b and u S'r - Lu Tosho 13'a (Osukeru'/4 Binona's gap is indicated.Lu(t( l solid) J-sa J suru o 2
d, 2 e kl coil, 2 J il 2 d (
It is attached continuously to the peaks 2a, 2a2 with the winding direction set in the direction of 71) or in the direction of the winding direction. Each tooth part 2 b, ,
21. ) 2 is wound in one direction as shown in the figure.

ゴ記第1図に示すリニアパルスモータの原理図において
、各コイル2d 、2eの励磁方向を誼め1っれだ順序
に切替制御を行うことにより水久磁イ62 c カらノ
Iiθ束との相If作用によってスフ1−ル歯γ1μの
IA ビノザずつスライダー2の歩ユ11動作を得る。
In the principle diagram of a linear pulse motor shown in Fig. 1, by controlling the excitation directions of each coil 2d and 2e in a decreasing order, we can obtain a magnetic flux of 62 c and a flux of Iiθ. By the phase If action, the movement of the slider 2 is obtained by the IA binoza of the tooth γ1μ.

ところが、上記従来のリニアパルスモークのよ′)々(
Ill極の配列ないし間隔、並ひに巻線(44成におい
ては、励磁1n条件、周囲温度の影響に伴い、リニJ′
・ζルス七−夕の温度変化を来し、コア、連結板なとが
伸縮J−ることにより磁極ピッチのずれを牛りる。こ7
1.に関連して■停止精度が悪くなる、(12)+tt
力の相関バラツキが犬となる。従って、電子!イブライ
タの文字送り用モータとしてリニア・・ルスモークを使
J[1シた場合、上記■の項目により文′]修ll (
′f消し)不良を発生し、@の項l」しく」、リタンピ
ンク不良を発生し、印手品質を著しく低−トき■る。
However, unlike the conventional linear pulse smoke mentioned above,
Depending on the arrangement or spacing of Ill poles, parallel winding (for 44 configurations, linear J'
・Due to the Tanabata temperature change, the core and connecting plates expand and contract to compensate for the deviation in the magnetic pole pitch. This 7
1. ■ Stopping accuracy deteriorates in relation to (12) + tt
Variation in the correlation of forces becomes a dog. Therefore, electronic! If a linear smoke is used as the character feed motor of the ibritor, the text will be corrected according to the item in ■ above.
``f erasing)'' causes defects, and ``@'' causes return pink defects, which significantly lowers the quality of stamps.

ツノ、i、l、;気吸引)Jを発生−する1r赳]・つ
りかリ−つ′・・ハスモータの111動了のi(L行方
向VCZJ−J−る中心線の利称の缶j1′/l、 v
(二ろ′らないため、進行lJ向Cζt、い−(両ψj
1.;にイfするダ1.゛J都拐 (へつ′リンク)K
加わる磁気吸引’、IJの強弱か交D−K反11v、[
2、リニアパルス七−りjり動jの前f友(/(二お・
いてかなりの振動をもた1)シ、ひいて0.]騒門レし
ルの」−Yiをきたずイ頃向かあっ/(、O(−の発明
の1−1的は、リニアパルスモータの1次側、薇東発生
装置(スライダー)の各スデノブごとの磁気吸引)Jが
進1]方向の中ノ1.・線に月し7て幻Jdj・(r(
二加2−ら〕する」うに巻線方法及び磁極間隔をカーめ
るCと)r」、り上記従来の欠点を除去し、コノ゛の、
熱膨張に月する影響度を軽減するとともに18Ai′f
の低1・を(rlかることVCある。
Tsuno, i, l,; air suction) 1r 赳] ・Tsurikari-tsu'... 111 movement of the helical motor i (L row direction VCZJ-J- can of the center line) j1′/l, v
(Because there is no double, the progression lJ direction Cζt, i-(both ψj
1. 1. K
Applied magnetic attraction', strength of IJ, cross D-K anti-11v, [
2. Linear pulse
1), which caused considerable vibration, and then 0. ] I was heading towards the time when I was going to start the '-Yi of Reshiru Noimon. Magnetic attraction for each Sden knob)
The above-mentioned conventional drawbacks have been eliminated, and the winding method and magnetic pole spacing can be reduced using the following methods:
18Ai'f while reducing the degree of influence on thermal expansion.
There is a VC that finds the low 1 of (rl).

リド、図示する実施例について封体的に説1す]する。[1] The illustrated embodiment will be described in detail.

第21ノ11t、この発明に係る原理を小ずd−面図、
第、3図(r↓第2図のA−A断面]Vである。各図V
(4゜いC,++ロスケールで、中失爾i庇II a及
び当1ib中央歯tjl(Ilaを挟んで両側vc @
+;)力歯’j<B 、+1 Ill 、 1111.
 A備λてる・す、各側方歯部II b、 、 II 
+)2のリニアパルス■5−り1.11目1動子の進行
方向と[ら角をなす相i1位置t、1一致さぜろと々も
に、中央tai H’ B目aと側方歯1’lt 11
 b、 + II t)2 トl’:l半ビy + ’
7) スレライ■L テ’/” 6 モのこする1、そ
して、中央歯部月aの長さくd倶]力歯Fj1i It
 11. 、1111.の各南部の長さの2倍に定めで
ある。
No. 21, 11t, a small d-side view of the principle of this invention,
Figure 3 (r↓ A-A cross section in Figure 2) V. Each figure V
(4° C, ++ low scale, middle loss II eaves II a and this 1ib central tooth tjl (both sides across Ila vc @
+;) Force tooth'j<B, +1 Ill, 1111.
A equipment, each lateral tooth part II b, , II
+) Linear pulse of 2■ 5-ri 1.11 The phase i that forms an angle with the moving direction of the 1st mover 1 position t, 1 coincidence Sazuro and Tomo, center tai H' B eye a and side Square tooth 1'lt 11
b, + II t)2 tl':lhalf biy +'
7) Slerai■L Te'/" 6 Mo rubs 1, and the length of the central tooth part a is d〶] force tooth Fj1i It
11. , 1111. It is determined to be twice the length of each southern part of the area.

12(riミスライダー、3分割された磁極鉄・し・l
:う、14゜15、スベー−1lI(i 、 17、永
久磁石18、ハックプレー119、コイル2G 、 2
1 J:り構成される。
12 (ri misrider, magnetic pole iron divided into 3
: U, 14゜15, sub-1lI (i, 17, permanent magnet 18, hack play 119, coil 2G, 2
1 J: Constructed.

7)−6、このスライダー32の具体的構成シ(ついて
11I)へることとする。寸ず、磁極釦、・し−13、
14、15(dスライタ−12の進イ〕方向と直角方向
の相削位置を同じく−4る11イiB%13a−13d
 、 Ida〜14d 、 15a〜15(]をイI:
ii jt、相カー間にスベー4ノ16 、17を斤在
さば−C(み急曲のしゃ断状態をイ4tている。そして
、磁極鉄心口を代入して磁極の位置関係を説明すると、
41;i (iili l:l a 、 I3d l’
J’、 !jいにス勺゛−ルth gl(tでQ1+、
、て1/21−]−+1のノーt′1を有し、コイル2
0が互いに逆向きに叶肩1的しく178回さJ]ている
。−力、磁極14 t) 、 14 (・(1rIいp
(i’ビノナのず11をイjし、刀)つ’aB & +
3 a 。
7)-6. Let's move on to the specific configuration of this slider 32 (see 11I). Sunzu, magnetic pole button, shi-13,
14, 15 (advance of d slider 12) The matching position in the direction perpendicular to the direction is also -4 11iB% 13a-13d
, Ida~14d, 15a~15(] I:
ii jt, Sube 4 Nos 16 and 17 are placed between the phase cars (I 4t indicates the cutoff state of the sharp turn. Then, substituting the magnetic pole iron core opening and explaining the positional relationship of the magnetic poles,
41;i (iii l:la, I3d l'
J',! j ini sql th gl (Q1+ with t,
, has a note t'1 of 1/21-]-+1, and the coil 2
0 is repeated 178 times in opposite directions. - force, magnetic pole 14 t), 14 (・(1rIp
(i'Binona Nozu 11 and sword) Tsu'aB & +
3 a.

冒d (に+1してシーJ、’/4e)千のずれを治し
2て′:j1ル21かlJ−いl′(逆向きの方向にて
連続的(・′(べ回さ]1]−いる。次に水久峰石18
(!ユ各磁極鉄、シ・目、l・1.15+’)背面i/
(おい(図示の極性1′(店磁して配置さtl・、)3
、・iだ、ハノ′ノブレ−li′Jj!l磁路形jノ’
y、 5−用い、1第捧鉄−614ノI(+’ミc;I
他)118極鉄心1:(、+5(外fl]1](l(配
置へt161則)の)“ノさくfc比し7て2 (ンこ
の1ソさ6.イjす4)ものとする。
Expansion d (+1 to sea J, '/4e) Correct the deviation of 1,000 and 2': j1 le 21 or lJ-i l' (continuous in the opposite direction (・' (be rotation sa) 1 ]-There is.Next is Mizukumineishi 18
(!Yu each magnetic pole iron, shi・eye, l・1.15+') back i/
(Oi (Illustrated polarity 1' (store magnetically arranged tl,) 3
,・It's me, Hano'Noble-li'Jj! l magnetic path type j'
y, 5-use, 1st iron - 614 no I (+'mic; I
etc.) 118-pole iron core 1: (, +5 (outer fl] 1] (l (arrangement to t161 rule)) "Nosaku fc ratio 7 to 2 (N this 1 so 6. I j s 4) do.

1、;C第2図及び第、う図に示す実施例の構成K :
l;−レゾC1その作用を第4図〜第71ンjにlJり
1動イノ1力j曹111図をもと1・(説明する。寸ず
、第4図(イ)cc小−4」・)にコイル205−励磁
18すると磁J、lll1I3a 、 Lla 、 1
5aノシ0’ 4θ極I(d 、 Is d 、 15
dが図示の′上流方向(1(ン(起磁力を発ノ11−る
。この起磁カ々水久イ1好イー118の(+6束とのL
t’、l連で、第41ソ神フ)に示ず各磁極1、(a〜
13d。
1.;C Structure K of the embodiment shown in Fig. 2 and Figs.
l;-Reso C1 The action is shown in Figures 4 to 71. "・) When the coil 205-excites 18, the magnetic J, lll1I3a, Lla, 1
5a no 0' 4θ pole I (d, Is d, 15
d generates a magnetomotive force in the upstream direction (1(n) shown in the figure.
t', l series, each magnetic pole 1, (a~
13d.

14 a −1=l d 、 15 a 〜1.5 d
のスフ1−ルとの幻向面の(漫末光牛伏況(!1斜絢に
示ず西りとなる。次にコイル20への励磁を切ると同時
にコイル21の励磁1μを行う (このときの磁極13
 b 、 14 b 、 1.5 bノルひ磁極1.3
c 、 14c 、 15cKオける71i ficの
向きを・第5+:81(イ) j((小J−、jl、Q
りと1−る)と今度は各磁極]、i a 〜]:(d 
、 lda〜14d 、 15a−15dスケールlj
向而の6図束発生状r’t?、 if第C〕図や)にて
斜線で示す通りとなる。この第・1図から第5図のモー
 ト切替(で伴ってスケールj4・固尾側とし/こ場合
、スライダーJ2がh側に1/。
14 a -1=ld, 15 a ~ 1.5 d
The direction of the phantom direction with the second circle (!1 is not shown in the diagram, but is westward.) Next, at the same time as the excitation to the coil 20 is cut off, the excitation of the coil 21 is energized by 1μ (at this time magnetic pole 13
b, 14 b, 1.5 b nordhi magnetic pole 1.3
c, 14c, 15c
) and now each magnetic pole], i a ~]: (d
, lda~14d, 15a-15d scale lj
What is the state of occurrence of the 6-figure bundle r't? , if it is as indicated by diagonal lines in Figure C]. In this case, slider J2 is moved 1/1 to the h side when switching the mote shown in Figures 1 to 5.

ピッチ移動する。さらに、第6図(イ)K示すように−
Jコイル0を励磁すると同第6図fO) K斜線で小ず
(直極面かC,磁束か出て81′!5図の位置より1/
4ピツチスライダ12が変f命、する。次に再度コイル
20からフィル21へ励磁を第7図(イ)の極性にて磁
極+3 b 、 1111)、 +5 +]、及び13
 c、 14 c 、 15 cを励磁すると磁束発牛
七−]・Pa+第7図(ロ)に示すようrCなる。こノ
しく〆(、,1,’ =)−C内層1/4 ビノヂ変缶
する。以l・、第4図(/(小−1−七−1・に戻り同
様の動作を繰返してIA ビy−f〕’−)歩、イL動
作が達成される。
Move the pitch. Furthermore, as shown in Figure 6 (a) K -
When J coil 0 is energized, a small drop (fO in Fig. 6 in the same figure) is shown by K diagonal line (orthogonal surface or C, magnetic flux comes out, 81'!1/1 from the position in Fig. 5).
4-pitch slider 12 changes its function. Next, the coil 20 is energized again from the fill 21 with the polarity shown in FIG.
When C, 14 C, and 15 C are excited, the magnetic flux becomes rC as shown in FIG. 7(B). Konoshiku〆(,,1,'=)-C inner layer 1/4 binoji change can. From then on, the steps shown in FIG. 4 (/(return to elementary school-1-7-1) and repeat the same actions to achieve the IA biy-f]'-) step and iL action.

l」3・、−1−記の説明においては磁極を1つの南部
とする最li)基本的機構について述べたものであるが
太際の磁極には複数の歯部が形成さノ′tている。
The explanations in Sections 3 and 1 describe the most basic mechanism in which the magnetic pole is one southern part, but the thickest magnetic pole is formed with multiple teeth. There is.

1/こ、(iB極り、屯・を3分割する例について述べ
ているが、この+:li成r↓スライター12の走行方
向における中・b部6−1芹2して左右均等に磁気吸引
力を加える(1青成てあればよく、スライタ゛−12の
A二?−rlj向(・(二月し、てl(1角力向kc 
2分割しても」、い。
1/This is an example of dividing the iB polarity into three parts. Apply magnetic attraction force (it is sufficient if it is 1 blue, in the direction of A2?-rlj of the slider -12).
Even if it's split into two, no.

力、スケーノL側においてIjいに半ピノ−fJ)4−
才′1をイjする南部を形成しているが、スライダー1
111の汀j部を各磁極VcJxいて半ピツチずノまた
)ζ1i分タt1′4成−4るようにし、でもよいrl
さらに、この発明の応用]としC11,1ピ2イ1」モ
ータのみ4・らず秒11えは、14」モータとL−C3
勾の6図極をイl1fiえ、1/6ビノチずっの歩ノイ
L動1′1を担わせることも]1」能である。
force, Ij on the scale L side, half pino-fj) 4-
Although it forms the southern part of the island, slider 1
111 is set so that each magnetic pole VcJ
Further, application of this invention] C11, 1 pin 2, 1" motor only 4, 2 seconds 11, 14" motor and L-C3
It is also possible to set the 6 poles of the gradient and make it carry the 1/6th of the 1/6 inch length of the movement 1'1.

1ノ、−1,述へたよう+l(、この発明に係るリニー
j′ハルスT:−タ((II水久イ1μイー1((、J
、(つく磁束とスライター用1g3 i+B 6F!t
’4< K 倫(らしft J イ/L/ I)励磁に
基ッ< +14.4! >rとの相!r、’、 (’+
川に上って駆動制御をなす基本11″4成V(おいて、
スライダーの進行方向にトシする中心、’: ?:Iは
等y+J離+f(ある各一対の磁(壷の励磁18により
歩、イ(動作6牛せ1.め、かつ磁束が各(み極それそ
ノ′シにj、いてJJ! 1′7.1−(発生させるよ
うにしたものである。この構成(′ご基つい−Cリニア
パルスモータの各ステップととの&i磁気吸引力スライ
タ゛−の長手方向の中・し−f1ン置より絹はグ・」称
の位(b/cに加えら、1するがら前後のバランスが′
7i’; IIC8fl持でき前後動を生じない。従つ
″C,振動の14!l後モー1・かなく、騒督の低減を
に↓かることがて゛きる。
1 no, -1, as mentioned +l(, Liny j' Hals T:-ta((II Mizukui 1μE1((, J
, (1g3 i+B 6F!t for magnetic flux and slighter
'4 < K Rin (Rashift J I/L/I) Based on excitation < +14.4! > A phase with r! r,', ('+
A basic 11" 4-V (up to the river and controlling the drive)
Center to move in the direction of slider movement, ': ? : I is equal to y + J separation + f (each pair of magnets (by excitation 18 of the jar, step, i (movement 6 cow se 1.), and the magnetic flux is each (the poles are j, and JJ! 1) '7.1- (This configuration is based on the following: - The magnetic attraction force of each step of the C linear pulse motor and the magnetic attraction force in the longitudinal direction of the slider. Silk is gu・'' (in addition to b/c, the front and back balance is ′
7i'; IIC can hold 8fl and does not move back and forth. Therefore, after 14!L of vibration, it is possible to reduce the noise.

力、同u、14に励(iBを受りる各一対の磁極V(ツ
、・(^−C1’+’+! ’/こ磁気センター (女
定点)が定するので、φ・ノ(膨張による=ノアの伸O
・が生じても特性の変化する余地4・く、畠しこi、+
7桶な停止lti度が11IらJする。
Since the magnetic center (female fixed point) of each pair of magnetic poles V (tsu, ・(^−C1'+'+! '/) which receives excitation (iB) is determined by force, u, 14, φ・ノ( Due to expansion = Noah's elongation O
Even if ・occurs, there is room for the characteristics to change 4・ku, Hatakeshiko i, +
The 7th stop lti degree is 11I to J.

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

第11ソI k、’1.4iL来のリニア・ぐルスモー
タの1例を)1〈−1−1’i++成図、第2図はこの
発明に係る1に了・” +1/ス−(−−−夕の11而
しJ、1、第゛う図V11ノ図のA−A断面図、第41
Ji、第5Iン1、第6図、第7図(dこの発明の動1
′1ζL、、(1・明するだめの動作原理図である。 11   スクール
11th Ik, '1.4iL An example of a linear motor is shown in Figure 2. --- Evening 11 J, 1, A-A sectional view of Figure V11, No. 41
Ji, 5th Inn 1, Fig. 6, Fig. 7 (dMovement 1 of this invention
'1ζL,, (1. This is a diagram of the operating principle of the clearing mechanism. 11 School

Claims (1)

【特許請求の範囲】[Claims] ■永久磁石に基づく磁束とスライダー川歯部磁極に(+
iiiえられ/Cコイルの励磁に基づく磁束との相々作
用によって駆動力を得る基本構成において、十記スライ
ダーの進行方向に対して直角方向に磁極鉄心を複数に分
割し、それぞれの磁極鉄・1.・をスケール歯部に対す
る磁気吸引力が互いに均舌になる2群に分け、各磁極に
おける2つの鉄・b!jYがスケール歯部に対して1/
2ピツチのバーをイ」シー(ス・J向させるように構成
し、各磁極はスライダーの進行方向における中〕し・位
置を境にしてほぼ等距離にある磁極同志を対とし、各対
の磁極の励磁を順次切替えて一定ビノチずつの歩進を行
わせる手段を備えたことを%徴とするリニーノ′パルス
七−タ。
■Magnetic flux based on permanent magnet and slider river tooth magnetic pole (+
In the basic configuration in which the driving force is obtained through interaction with the magnetic flux based on the excitation of the iii/C coil, the magnetic pole iron core is divided into a plurality of pieces in a direction perpendicular to the direction of movement of the slider, and each magnetic pole iron and 1.・ is divided into two groups whose magnetic attraction forces to the scale teeth are evenly distributed, and the two iron ・b! jY is 1/with respect to the scale teeth
The two-pitch bar is configured so as to face I, S, and J, and each magnetic pole is paired with magnetic poles that are approximately equidistant from each other with the middle position in the slider's advancing direction. A linino' pulse septator characterized by being equipped with means for sequentially switching the excitation of the magnetic poles to step by a constant number of steps.
JP8793783A 1983-05-18 1983-05-18 Linear pulse motor Granted JPS59213274A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP8793783A JPS59213274A (en) 1983-05-18 1983-05-18 Linear pulse motor
US07/105,447 US4761574A (en) 1983-05-18 1987-10-02 Linear pulse motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8793783A JPS59213274A (en) 1983-05-18 1983-05-18 Linear pulse motor

Publications (2)

Publication Number Publication Date
JPS59213274A true JPS59213274A (en) 1984-12-03
JPH0118667B2 JPH0118667B2 (en) 1989-04-06

Family

ID=13928813

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8793783A Granted JPS59213274A (en) 1983-05-18 1983-05-18 Linear pulse motor

Country Status (1)

Country Link
JP (1) JPS59213274A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61113583U (en) * 1984-12-24 1986-07-18

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57199467A (en) * 1981-06-03 1982-12-07 Shinko Electric Co Ltd Linear pulse motor

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57199467A (en) * 1981-06-03 1982-12-07 Shinko Electric Co Ltd Linear pulse motor

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61113583U (en) * 1984-12-24 1986-07-18

Also Published As

Publication number Publication date
JPH0118667B2 (en) 1989-04-06

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