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JPH0147115B2 - - Google Patents
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JPH0147115B2 - - Google Patents

Info

Publication number
JPH0147115B2
JPH0147115B2 JP13615882A JP13615882A JPH0147115B2 JP H0147115 B2 JPH0147115 B2 JP H0147115B2 JP 13615882 A JP13615882 A JP 13615882A JP 13615882 A JP13615882 A JP 13615882A JP H0147115 B2 JPH0147115 B2 JP H0147115B2
Authority
JP
Japan
Prior art keywords
magnetic pole
pole pieces
field
rotor
axial direction
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.)
Expired
Application number
JP13615882A
Other languages
Japanese (ja)
Other versions
JPS5925570A (en
Inventor
Kinzo Sodeshida
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.)
Asmo Co Ltd
Original Assignee
Asmo 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 Asmo Co Ltd filed Critical Asmo Co Ltd
Priority to JP13615882A priority Critical patent/JPS5925570A/en
Publication of JPS5925570A publication Critical patent/JPS5925570A/en
Publication of JPH0147115B2 publication Critical patent/JPH0147115B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K1/00Details of the magnetic circuit
    • H02K1/06Details of the magnetic circuit characterised by the shape, form or construction
    • H02K1/12Stationary parts of the magnetic circuit
    • H02K1/14Stator cores with salient poles
    • H02K1/145Stator cores with salient poles having an annular coil, e.g. of the claw-pole type

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Permanent Magnet Type Synchronous Machine (AREA)

Description

【発明の詳細な説明】 この発明は、ステツピングモータ等において、
ロータと界磁極との間に発生するコツキング作用
による慣性的振動やベアリングの騒音を減少させ
て始動性を改善することを目的としたモータ用界
磁極に関するものである。
[Detailed Description of the Invention] This invention provides a stepping motor, etc.
The present invention relates to field poles for motors that aim to improve startability by reducing inertial vibrations and bearing noise due to the cocking effect generated between the rotor and field poles.

従来、ステツピングモータとして、第1図の分
解斜視図および第2図の組立図に示すものが使わ
れている。
Conventionally, stepping motors shown in the exploded perspective view of FIG. 1 and the assembled view of FIG. 2 have been used.

図において、1は円筒形多磁極永久磁石2と回
転軸3とからなるロータであり、4および5は、
コイルがバランス巻きされた左、右一対のコイル
ボビンである。
In the figure, 1 is a rotor consisting of a cylindrical multi-pole permanent magnet 2 and a rotating shaft 3, and 4 and 5 are:
A pair of left and right coil bobbins with balanced coil winding.

前記コイルボビン4,5のうち、コイルボビン
4は、多数の同形の磁極片6aを有するケーシン
グ兼用のステータ6と、同数同形の磁極片7aを
有するステータ7とにより両側から挾持され、か
つ他方のコイルボビン5は、それぞれ磁極片8
a,9aを有するステータ8,9により両側から
挾持されており、前記各ステータ6,7,8,9
の中心を通る前記ロータ1の回転軸3は、ケーシ
ング兼用のステータ6の軸受10および蓋体11
の軸受11aにて回転自在に支持されている。
Of the coil bobbins 4 and 5, the coil bobbin 4 is held between both sides by a stator 6 that also serves as a casing and has a large number of identically shaped magnetic pole pieces 6a, and a stator 7 that has the same number and identically shaped magnetic pole pieces 7a, and is held between the other coil bobbin 5. are respectively pole pieces 8
It is sandwiched from both sides by stators 8 and 9 having a and 9a, and each stator 6, 7, 8, 9
The rotating shaft 3 of the rotor 1 passes through the center of the bearing 10 of the stator 6, which also serves as a casing, and the lid 11.
It is rotatably supported by a bearing 11a.

前記ステツピングモータの構成において、各ス
テータの同形の磁極片6aと7a、および8aと
9aは接触することなく、交互に向い合つて位置
づけられると共に左右のコイルボビン4と5間で
は各磁極の位相がずれた状態に位置づけられてい
る。
In the configuration of the stepping motor, the same-shaped magnetic pole pieces 6a and 7a and 8a and 9a of each stator are positioned alternately facing each other without contacting each other, and the phase of each magnetic pole is adjusted between the left and right coil bobbins 4 and 5. It is positioned in a shifted position.

しかして、前述した従来のステツピングモータ
にあつては、ステータを形成している櫛歯状の磁
極片である多極界磁極は、第3図に示すように、
方形歯、矩形歯が一般的であり、その磁極片どう
しは間隙を残して対向しているが、その間隙の寸
法については、特に考慮されていない。すなわ
ち、ステータの軸線方向における歯形基端部間の
距離aと歯先間の距離bとの差が大きくなつてお
り、この間隙寸法の差が磁気力の変化としてあら
われ、それがコツキング現象の発生原因となつて
いる。そのために、残留トルクが大きくなり、ト
ルク損失も増え、効率の低下を招き、振動や騒音
の原因となり、特に前記に起因する軸受損のため
に寿命が短かくなる等の欠点がある。
However, in the conventional stepping motor described above, the multi-pole field poles, which are comb-shaped magnetic pole pieces forming the stator, are as shown in FIG.
Square teeth and rectangular teeth are common, and their magnetic pole pieces face each other with a gap left, but no particular consideration is given to the size of that gap. In other words, the difference between the distance a between the base ends of the tooth profiles and the distance b between the tooth tips in the axial direction of the stator is increasing, and this difference in gap size appears as a change in magnetic force, which causes the occurrence of the cocking phenomenon. It is the cause. Therefore, residual torque increases, torque loss increases, efficiency decreases, vibrations and noise are caused, and bearing loss caused by the above causes shortened life.

この発明は、上述した従来の欠点を解決するた
めになされたもので、ステツピングモータ等にお
けるロータと界磁極間に発生するコツキング現象
を無くすため、ステータの櫛歯形磁極片の形状と
配置を考慮し、交互に向い合つて配置されるステ
ータの磁極片の周囲の隙間が軸線方向において等
しくなるように設定したことを特徴とするモータ
用界磁極を提供するものである。
This invention was made to solve the above-mentioned conventional drawbacks, and in order to eliminate the knocking phenomenon that occurs between the rotor and field poles in stepping motors, etc., the shape and arrangement of the comb-shaped magnetic pole pieces of the stator are taken into consideration. The present invention also provides field poles for a motor, characterized in that the gaps around the magnetic pole pieces of the stators that are alternately arranged facing each other are set to be equal in the axial direction.

まず、この発明による基本原理を第4図および
第5図にもとづいて説明する。つまり、コツキン
グ現象のない状態とは、第4図に示すように、円
筒型磁石のロータRに対して同軸に円筒状の界磁
極用磁性鉄板Sを配置し、ロータRを回転した場
合であつて、この場合には磁気抵抗の変化がない
ため、コツキングは起らない。
First, the basic principle of this invention will be explained based on FIGS. 4 and 5. In other words, as shown in Fig. 4, the state in which there is no "knocking" phenomenon is when a cylindrical field pole magnetic iron plate S is placed coaxially with the rotor R of the cylindrical magnet, and the rotor R is rotated. In this case, there is no change in magnetic resistance, so no twitching occurs.

また、仮に上記円筒状磁性鉄板Sを中央部で輪
切りにした場合、あるいは輪切りにしたものを同
軸のまま軸線方向に若干移動した場合でも磁気低
抗の変化がなく、コツキングは起らない。
Further, even if the cylindrical magnetic iron plate S is cut into rounds at the center, or even if the slices are slightly moved in the axial direction while remaining coaxial, there is no change in magnetic resistance and no sagging occurs.

したがつて、上記輪切りの方法を変えて、輪切
り部を中心線にして円周上に任意の形状、たとえ
ば第5図に示すごとく三角波、あるいは正弦波、
台形波の形状で切断し、円筒状磁性鉄板S,S′を
軸線方向に一定距離移動しても前記と同様にコツ
キングが起らないものである。
Therefore, by changing the above-mentioned method of slicing, we can cut any shape on the circumference with the slit as the center line, such as a triangular wave or a sine wave as shown in Fig. 5.
Even if the cylindrical magnetic iron plates S and S' are moved a certain distance in the axial direction after cutting in the shape of a trapezoidal wave, no twitching will occur as described above.

この場合、円筒状磁性鉄板S,S′の軸線方向の
一定距離とは、軸線方向にいずれの点でも等間隔
に設定されることであり、交互に噛み合わされ、
しかも同一形状であることが必要である。
In this case, the constant distance in the axial direction of the cylindrical magnetic iron plates S and S' means that the cylindrical magnetic iron plates S and S' are set at equal intervals at any point in the axial direction, and are meshed alternately.
Moreover, it is necessary that they have the same shape.

第6図に示したものは、前記基本原理にもとづ
いて構成されたこの発明による一実施例であつ
て、櫛歯形のステータ20,21は展開図で示さ
れている。このステータ20,21の磁極片20
a,21aは、台形状に成形され、隙間をとつて
交互に噛み合わされ、磁極片の全周の隙間は、軸
線方向での間隔dがいずれの点でも等しくなるよ
うに設定されている。
What is shown in FIG. 6 is an embodiment of the present invention constructed based on the above-mentioned basic principle, in which the comb-shaped stators 20 and 21 are shown in a developed view. The magnetic pole piece 20 of this stator 20, 21
a, 21a are formed into a trapezoidal shape and are meshed alternately with a gap therebetween, and the gap around the entire circumference of the magnetic pole pieces is set so that the distance d in the axial direction is equal at all points.

上記のように、隣り合う磁極片の全周の隙間
が、軸線方向において等しく形成されていれば、
ロータの磁極に対する界磁面績はロータの回転位
置にかゝわらず常に一定とされるから、コツキン
グ現象は起らない。
As mentioned above, if the gaps around the entire circumference of adjacent magnetic pole pieces are formed equally in the axial direction,
Since the field surface relative to the magnetic poles of the rotor is always constant regardless of the rotational position of the rotor, no twitching phenomenon occurs.

なお、前記ステータ20,21の磁極片20
a,21aの形状は台形に限定されるものではな
く、軸線方向での間隔をいずれの点でも等しくで
きるものであればよく、たとえば、三角波、正弦
波などの形状も任意に選定できるものである。
Note that the magnetic pole pieces 20 of the stators 20 and 21
The shapes of a and 21a are not limited to trapezoids, but may be any shape as long as the spacing in the axial direction can be made equal at all points; for example, shapes such as triangular waves and sine waves can be arbitrarily selected. .

以上に述べたように、この発明によれば、軸線
方向に向けられた同一形状の多数の磁極片が円周
方向に同一ピツチでN、S交互に配列されてなる
モータ用界磁極において、隣り合う磁極片の全周
の隙間が、軸線方向にわたつて等しくなるように
形成されているので、ロータの磁極に対する界磁
面積はロータの回転位置にかかわらず常に一定と
され、リラクタンスの変化は実質的にないと考え
てよいから、従来のモータのごとく、リラクタン
ス最少の位置は存在せず、リラクタンス最少位置
にロータが吸引されたために、始動時の位置を脱
出させるトルクを必要とする現象、すなわちコツ
キング現象は起らないから、モータの操作におい
て安定した回転が得られる。
As described above, according to the present invention, in a motor field pole in which a large number of magnetic pole pieces of the same shape and oriented in the axial direction are arranged alternately N and S at the same pitch in the circumferential direction, adjacent Since the gaps around the entire circumference of the matching magnetic pole pieces are formed to be equal in the axial direction, the field area relative to the rotor's magnetic poles is always constant regardless of the rotor's rotational position, and changes in reluctance are virtually constant. Since there is no minimum reluctance position like in conventional motors, there is a phenomenon in which the rotor is attracted to the minimum reluctance position and requires torque to escape from the starting position, i.e. Since no twitching phenomenon occurs, stable rotation can be obtained during motor operation.

また、前記コツキング現象の解消により、慣性
的振動やベアリング騒音も減少し、始動および停
止改善を図ることができる等の効果もある。
Moreover, by eliminating the above-mentioned twitching phenomenon, inertial vibrations and bearing noise are also reduced, and there are other effects such as improvement in starting and stopping.

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

第1図はステツピングモータの分解斜視図、第
2図は組立て状態を示す一部断面側面図、第3図
は第2図の磁極片の配置状態を示す拡大側面図、
第4図および第5図はこの発明による基本原理を
説明するモータ要部の斜視図、第6図はこの発明
の一実施例を示すステータの展開図である。 1……ロータ、2……円筒磁石、3……回転
軸、4,5……コイルボビン、6,7,8,9…
…ステータ、6a,7a,8a,9a……磁極
片、10……軸受、11……蓋体、11a……軸
受、R……ロータ、S,S′……界磁用円筒鉄板、
20,21……ステータ、20a,21a……磁
極片。
FIG. 1 is an exploded perspective view of the stepping motor, FIG. 2 is a partially sectional side view showing the assembled state, and FIG. 3 is an enlarged side view showing the arrangement of the magnetic pole pieces in FIG.
4 and 5 are perspective views of main parts of a motor for explaining the basic principle of the invention, and FIG. 6 is an exploded view of a stator showing an embodiment of the invention. 1... Rotor, 2... Cylindrical magnet, 3... Rotating shaft, 4, 5... Coil bobbin, 6, 7, 8, 9...
...Stator, 6a, 7a, 8a, 9a...Pole piece, 10...Bearing, 11...Lid, 11a...Bearing, R...Rotor, S, S'...Cylindrical iron plate for field,
20, 21... Stator, 20a, 21a... Magnetic pole piece.

Claims (1)

【特許請求の範囲】[Claims] 1 軸線方向に向けられた同一形状の多数の磁極
片が円周方向に同一ピツチでN、S交互に配列さ
れてなるモータ用界磁極において、隣り合う磁極
片の全周の隙間が、軸線方向にわたつて等しくな
るように形成されていることを特徴とするモータ
用界磁極。
1. In a motor field pole in which a large number of magnetic pole pieces of the same shape oriented in the axial direction are arranged alternately N and S at the same pitch in the circumferential direction, the gap around the entire circumference between adjacent magnetic pole pieces is A field pole for a motor, characterized in that the field poles are formed to be equal across the field.
JP13615882A 1982-08-04 1982-08-04 Field pole of motor Granted JPS5925570A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13615882A JPS5925570A (en) 1982-08-04 1982-08-04 Field pole of motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13615882A JPS5925570A (en) 1982-08-04 1982-08-04 Field pole of motor

Publications (2)

Publication Number Publication Date
JPS5925570A JPS5925570A (en) 1984-02-09
JPH0147115B2 true JPH0147115B2 (en) 1989-10-12

Family

ID=15168666

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13615882A Granted JPS5925570A (en) 1982-08-04 1982-08-04 Field pole of motor

Country Status (1)

Country Link
JP (1) JPS5925570A (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0721102Y2 (en) * 1985-12-27 1995-05-15 ジューキ株式会社 Stepping motor
JPS63156566U (en) * 1987-03-30 1988-10-13
JPH02214457A (en) * 1989-02-14 1990-08-27 Seiko Electronic Components Ltd Cylindrical dc brushless motor structure
JP2573866Y2 (en) * 1992-09-24 1998-06-04 ジェコー株式会社 PM type step motor
JP2003079126A (en) * 2001-08-31 2003-03-14 Canon Electronics Inc Motor
KR101163982B1 (en) * 2010-01-22 2012-07-09 주식회사 모아텍 Step motor for reduction of detent torque

Also Published As

Publication number Publication date
JPS5925570A (en) 1984-02-09

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