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JPS62193547A - Step motor - Google Patents

Step motor

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Publication number
JPS62193547A
JPS62193547A JP3214386A JP3214386A JPS62193547A JP S62193547 A JPS62193547 A JP S62193547A JP 3214386 A JP3214386 A JP 3214386A JP 3214386 A JP3214386 A JP 3214386A JP S62193547 A JPS62193547 A JP S62193547A
Authority
JP
Japan
Prior art keywords
excitation
stator core
pole teeth
rotor
step 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
JP3214386A
Other languages
Japanese (ja)
Inventor
Tetsuya Nakayama
徹矢 中山
Takeshi Okamoto
武 岡本
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.)
Komatsu Ltd
Original Assignee
Komatsu 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 Komatsu Ltd filed Critical Komatsu Ltd
Priority to JP3214386A priority Critical patent/JPS62193547A/en
Publication of JPS62193547A publication Critical patent/JPS62193547A/en
Pending legal-status Critical Current

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  • Iron Core Of Rotating Electric Machines (AREA)

Abstract

PURPOSE:To improve output torque per space volume by winding exciting coils around portions of a stator core between pole teeth. CONSTITUTION:2X3 pole teeth 4-1 to 4-3 and 4-1' to 4-3' projecting toward a rotor 1 are formed in a stator core 3. Exciting coils C-1 and C-3 and C-1' to C-3' are respectively wound around recesses of the stator core 3 between pole teeth. The rotor 1 rotates if an exciting current with a polarity being reversed at an interval of 6pi/6 and with 2pi/6 phase difference from an adjacent phase flows between exciting coils C-1 and C-1', C-2 and C-2', and C-3 and C-3', respectively.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明はステップモータに関し、詳しくは励磁極の構造
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a step motor, and more particularly to the structure of excitation poles.

[従来の技術〕 周知のように、例えば3相ステツプモータでは、第7図
に示すように回転子1に対向して突設した2X3個の極
歯4−1〜4−3.4−1’〜4−3′をステータ鉄心
3に設け、これらの極歯4−1〜4−3.4−1’〜4
−3′のそれぞれに励磁コイルC1−C5,CI’ 〜
C3’ を巻装スルことにより、励磁極φ1〜φ3.φ
1′〜φ3′を構成し、第8図に示すようにφ1とφ1
′、φ2〜φ2′、φ3〜φ3′の組合せで各励磁極を
順次に励磁して回転子1に回転力を与えて回転させるよ
うに構成している。
[Prior Art] As is well known, for example, in a three-phase step motor, there are 2×3 pole teeth 4-1 to 4-3, 4-1 protruding from the rotor 1 as shown in FIG. '~4-3' are provided on the stator core 3, and these pole teeth 4-1~4-3.4-1'~4
-3' respectively, excitation coils C1-C5, CI' ~
By winding C3', the excitation poles φ1 to φ3. φ
1' to φ3', and φ1 and φ1 as shown in Figure 8.
', φ2 to φ2', and φ3 to φ3', the excitation poles are sequentially excited to apply rotational force to the rotor 1 and rotate it.

[発明が解決しようとする問題点] ところが、各相の励磁極を1相のみ励磁する1相励磁方
式あるいは2つの相を時間的に重ねて励磁する1−2相
励磁方式のいずれの場合であっても、回転子に対しては
1#lの励磁極のみの回転トルクが仔効となり、他の相
は回転トルクに対して同等寄与していないため、空間体
積当りの出力トルクに限界があるという問題があった。
[Problems to be Solved by the Invention] However, in either the 1-phase excitation method in which the excitation pole of each phase is excited only for one phase, or the 1-2 phase excitation method in which two phases are excited in a temporally overlapping manner, Even if there is, the rotational torque of only the 1#l excitation pole has a minor effect on the rotor, and the other phases do not contribute equally to the rotational torque, so there is a limit to the output torque per space volume. There was a problem.

本発明はこのような問題点を鑑み、空間体積当りの出力
トルクを向上させることができるステップモータを提供
することを目的とするものである。
SUMMARY OF THE INVENTION In view of these problems, it is an object of the present invention to provide a step motor that can improve the output torque per space volume.

[問題点を解決するための手段] 本発明は、励磁コイルを極歯と極歯との間のステータ鉄
心に巻装するようにしたものである。
[Means for Solving the Problems] According to the present invention, an excitation coil is wound around a stator core between pole teeth.

[作用コ 励磁コイルを極歯と極歯との間のステータ鉄心に巻装し
た場合、ステータ鉄心の厚みか大きく、また、励磁コイ
ルの巻数も多くとれるため、この分たけ回転トルクを増
加させることができる。
[When the working excitation coil is wound around the stator core between the pole teeth, the thickness of the stator core is large and the number of turns of the excitation coil can be increased, so it is necessary to increase the rotational torque by this amount.] I can do it.

し実施例〕 第1図は本発明を適用した3相ステツプモータの一実施
例を示す斜視図であり、ステータ鉄心3にはロータ1に
向けて突設した2×3個の極歯4−1〜4−3.4−1
’ 〜4−3′が形成されている。そして、励磁コイル
C1〜C3,CI’〜C3’ は極歯と極歯との間のス
テータ鉄心3の凹部に巻装されている。
Embodiment] FIG. 1 is a perspective view showing an embodiment of a three-phase step motor to which the present invention has been applied. 1-4-3.4-1
'~4-3' are formed. The excitation coils C1 to C3 and CI' to C3' are wound in the recesses of the stator core 3 between the pole teeth.

第2図は本発明を適用した3相リニアステツプモータの
一実施例を示す斜視図であり、第1図の実施例と同様に
、励磁コイルC1〜C3,CI’〜C3’ は極歯と極
歯との間のステータ鉄心3の四部に巻装されている。
FIG. 2 is a perspective view showing an embodiment of a three-phase linear step motor to which the present invention is applied. Similar to the embodiment of FIG. It is wound around the four parts of the stator core 3 between the pole teeth.

第3図は第1図のステップモータの各励磁を励磁する場
合の結線図であり、φ1とφ1′、φ2とφ2′、φ3
とφ3′の相合せて各励磁極か111列接続されており
、例えば第4図に示すような励磁回路によって各相の励
磁極φ1〜φ3.φ1′〜φ3′が励磁される。すなわ
ち、第5図(a)に示すように2π/6の位相差をもつ
パルス列が分配回路10に入力されると、分配回路10
は順次入力されるパルス列を第5図(b)〜(d)に示
すようにON時間が6π/6で、かつ隣接する相との位
相差が2π/6の励磁信号E1〜E3を形成し、励磁回
路11に入力する。また、励磁信号E1〜E3はインバ
ータ12〜14によってそれぞれ反転され、第5図(e
)〜(g)に示すような反転励磁信号El’ 〜E3’
 となって励磁回路11に入力される。
Figure 3 is a wiring diagram for exciting each step motor in Figure 1, φ1 and φ1', φ2 and φ2', φ3.
and φ3' are connected in 111 rows. For example, an excitation circuit as shown in FIG. 4 connects each phase's excitation poles φ1 to φ3. φ1' to φ3' are excited. That is, as shown in FIG. 5(a), when a pulse train having a phase difference of 2π/6 is input to the distribution circuit 10, the distribution circuit 10
As shown in FIGS. 5(b) to 5(d), the sequentially input pulse trains form excitation signals E1 to E3 with an ON time of 6π/6 and a phase difference between adjacent phases of 2π/6. , is input to the excitation circuit 11. Furthermore, the excitation signals E1 to E3 are inverted by inverters 12 to 14, respectively, and are inverted as shown in FIG.
) to (g), inverted excitation signals El' to E3'
and is input to the excitation circuit 11.

励磁回路11はこれらの励磁信号E1〜E3およびEl
’〜E3’が入力されたならば、信号E1とEl’を第
1相の励磁極φ1とφ1′の直列回路に、また、信号E
2とE2’を第2柑の励磁極φ2とφ2′の直列回路に
、さらに信号E3とE3’を第3相の励磁極φ3とφ3
′の直列回路に印加する。これによって、励磁極φ1と
φ1′。
The excitation circuit 11 receives these excitation signals E1 to E3 and El.
If '~E3' is input, the signals E1 and El' are connected to the series circuit of the first phase excitation poles φ1 and φ1', and the signal E
2 and E2' are connected to the series circuit of excitation poles φ2 and φ2' of the second phase, and signals E3 and E3' are connected to the excitation poles φ3 and φ3 of the third phase.
′ is applied to the series circuit. As a result, the excitation poles φ1 and φ1'.

φ2とφ2′、φ3とφ3′の間には第5図(h)〜(
J)に示すように、6π/6毎に極性が反転し、かつ隣
接する川との位相差が2π/6の励磁電流か流れる。
Between φ2 and φ2', and between φ3 and φ3', there are
As shown in J), the polarity is reversed every 6π/6, and the excitation current flows with a phase difference of 2π/6 with respect to the adjacent river.

この結果、第1相〜第3相の励磁毎に回転子との間に第
6図(a)〜(C)の矢印に示すような磁束φか順次に
形成され、回転子1が回転するようになる。
As a result, magnetic flux φ as shown by the arrows in FIG. 6(a) to (C) is sequentially formed between the rotor and the rotor each time the first to third phases are excited, and the rotor 1 rotates. It becomes like this.

この場合、回転子1を回転させる推力FはF寓1/28
N I・t・・・(1) となる。但し、Bは回転子1と極歯との間のエアギャッ
プにおける磁束密度、Nは1励磁極当りのコイル巻数、
■は励磁電流、tは励磁極の厚みである。
In this case, the thrust F that rotates the rotor 1 is F 1/28
N I・t...(1) becomes. However, B is the magnetic flux density in the air gap between the rotor 1 and the pole teeth, N is the number of coil turns per excited pole,
(2) is the excitation current, and t is the thickness of the excitation pole.

従って、励磁極の厚みtは極歯に対し極歯と極歯との間
のステータ鉄心3の方が一般的に大きいために、この分
たけ推力Fが向上する。
Therefore, since the thickness t of the excitation pole is generally greater in the stator core 3 between the pole teeth than in the pole teeth, the thrust force F is improved by this amount.

[発明の効果コ 以上説明したように本発明によれば、極歯と極歯との間
のステータ鉄心に励磁コイルを巻装するようにしたため
、空間体積当りの出力トルクを向上させることができる
。換言すれば、同一出力トルクのものに対して形状を小
さくすることができる効果がある。
[Effects of the Invention] As explained above, according to the present invention, since the excitation coil is wound around the stator core between the pole teeth, the output torque per space volume can be improved. . In other words, the shape can be made smaller compared to those with the same output torque.

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

第1図は本発明を適用した3相ステ・ンブモータの一実
施例を示す斜視図、第2図は本発明を適用した3相リニ
アステツプモータの一実施例を示す斜視図、第3図は励
磁コイルの結線図、第4図は励磁回路の一例を示す回路
図、第5図は第4図の励磁回路の入出力波形を示すタイ
ムチャート、第6図は第1図のステップモータの励磁状
態の変遷を示す図、第7図は従来のステップモータの構
成を示す断面図、第8図は第7図のステップモータの励
磁状態の変遷を示す図である。 1・・・回転子、3・・・鉄心、4−1〜4−3.4−
1°〜4−3゜・・・極歯、C1〜C3,CI’ 〜C
3’ ・・・励磁コイル、φ1〜φ3.φ1′〜φ3′
・・・励磁極、11・・・励磁回路。 )。 第1図 4’−1’ 第2図 第3図 第4図 ((1)  E3’ 第5図
FIG. 1 is a perspective view showing an embodiment of a three-phase step motor to which the present invention is applied, FIG. 2 is a perspective view showing an embodiment of a three-phase linear step motor to which the present invention is applied, and FIG. A wiring diagram of the excitation coil, Fig. 4 is a circuit diagram showing an example of an excitation circuit, Fig. 5 is a time chart showing input and output waveforms of the excitation circuit of Fig. 4, and Fig. 6 is an excitation of the step motor shown in Fig. 1. FIG. 7 is a cross-sectional view showing the configuration of a conventional step motor, and FIG. 8 is a diagram showing changes in the excitation state of the step motor shown in FIG. 7. 1... Rotor, 3... Iron core, 4-1 to 4-3.4-
1°~4-3°...Polar teeth, C1~C3, CI'~C
3'... Excitation coil, φ1 to φ3. φ1′~φ3′
... Excitation pole, 11... Excitation circuit. ). Figure 1 4'-1' Figure 2 Figure 3 Figure 4 ((1) E3' Figure 5

Claims (1)

【特許請求の範囲】  回転子に対向して突設した2n個(n≧3)の極歯を
有し、各極歯に励磁コイルを巻装してなるステップモー
タにおいて、 前記励磁コイルを極歯と極歯との間のステータ鉄心に巻
装したことを特徴とするステップモータ。
[Scope of Claims] A step motor having 2n (n≧3) pole teeth protruding from a rotor and having an excitation coil wound around each pole tooth, comprising: A step motor characterized by being wound around a stator core between teeth and pole teeth.
JP3214386A 1986-02-17 1986-02-17 Step motor Pending JPS62193547A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3214386A JPS62193547A (en) 1986-02-17 1986-02-17 Step motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3214386A JPS62193547A (en) 1986-02-17 1986-02-17 Step motor

Publications (1)

Publication Number Publication Date
JPS62193547A true JPS62193547A (en) 1987-08-25

Family

ID=12350671

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3214386A Pending JPS62193547A (en) 1986-02-17 1986-02-17 Step motor

Country Status (1)

Country Link
JP (1) JPS62193547A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5798591A (en) * 1993-07-19 1998-08-25 T-Flux Pty Limited Electromagnetic machine with permanent magnet rotor
AU696370B2 (en) * 1993-07-19 1998-09-10 T-Flux Pty. Limited Electromagnetic machine with permanent magnet rotor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5798591A (en) * 1993-07-19 1998-08-25 T-Flux Pty Limited Electromagnetic machine with permanent magnet rotor
AU696370B2 (en) * 1993-07-19 1998-09-10 T-Flux Pty. Limited Electromagnetic machine with permanent magnet rotor

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