JPH0312048Y2 - - Google Patents

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Publication number
JPH0312048Y2
JPH0312048Y2 JP8935485U JP8935485U JPH0312048Y2 JP H0312048 Y2 JPH0312048 Y2 JP H0312048Y2 JP 8935485 U JP8935485 U JP 8935485U JP 8935485 U JP8935485 U JP 8935485U JP H0312048 Y2 JPH0312048 Y2 JP H0312048Y2
Authority
JP
Japan
Prior art keywords
winding
short
poles
permanent magnet
circuited
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
JP8935485U
Other languages
Japanese (ja)
Other versions
JPS61205240U (en
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 filed Critical
Priority to JP8935485U priority Critical patent/JPH0312048Y2/ja
Publication of JPS61205240U publication Critical patent/JPS61205240U/ja
Application granted granted Critical
Publication of JPH0312048Y2 publication Critical patent/JPH0312048Y2/ja
Expired legal-status Critical Current

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  • Permanent Magnet Type Synchronous Machine (AREA)
  • Dc Machiner (AREA)
  • Iron Core Of Rotating Electric Machines (AREA)

Description

【考案の詳細な説明】 (産業上の利用分野) 本考案は、磁石式モータ、特にモータの正逆両
回転において同一トルク特性を有するようにした
構造の磁石式モータに関するものである。
[Detailed Description of the Invention] (Industrial Application Field) The present invention relates to a magnet type motor, and particularly to a magnet type motor having a structure such that the motor has the same torque characteristics in both forward and reverse rotations.

(従来の技術) 従来の補極を有する磁石式モータの構造は、第
2図に示された如くモーク1の内部に界磁を形成
する円弧状の永久磁石2が固定され、該永久磁石
2の近傍に直巻特性を得るための補極3が設けら
れていた。同図において符号4は電機子のロー
タ、5は電機子巻線を表している。
(Prior Art) As shown in FIG. 2, the structure of a conventional magnetic motor with commutated poles is such that an arc-shaped permanent magnet 2 that forms a field is fixed inside a moke 1. A commutating pole 3 was provided in the vicinity of to obtain a series winding characteristic. In the figure, numeral 4 represents the rotor of the armature, and 5 represents the armature winding.

電機子巻線5に第2図図示の如く電機子電流を
流すと、すなわち紙面に垂直に紙面の裏側から表
側に向かつて直流電流を流すと、電機子のロータ
4は点線矢印で示された時計方向に回転する。こ
の場合、電機子巻線5に電機子電流が流れ、該電
機子反作用によつて生じる磁束は磁気抵抗の小さ
い図示された補極3、該補極3の部分の空隙、ロ
ータ4、補極3に対に設けられている図示されて
いない補極部の空隙、図示されていない補極、ヨ
ーク1の磁気回路を流れ、補極3および対で設け
られている図示されていない補極部分がそれぞれ
増磁され、補極3を備えた磁石式モータは、いわ
ゆる直巻特性を有する。
When an armature current is passed through the armature winding 5 as shown in Figure 2, that is, when a direct current is passed perpendicularly to the page from the back side of the page to the front side, the armature rotor 4 is shown by the dotted arrow. Rotate clockwise. In this case, an armature current flows through the armature winding 5, and the magnetic flux generated by the armature reaction is transmitted to the illustrated commutator 3, which has a small magnetic resistance, to the air gap in the part of the commutator 3, to the rotor 4, to the commutator. The air flows through the magnetic circuit of the yoke 1, the gap between the commutating pole parts (not shown) provided in pairs in the commutating pole 3, the commutating poles (not shown), and the commutating pole parts (not shown) provided in pairs in the yoke 1. A magnetic motor having a commutated pole 3, which is magnetized respectively, has a so-called series winding characteristic.

ところでこのような補極3を永久磁石2の近傍
に設けられた磁石式モータに電源電圧を逆に接続
し、第3図図示の如く電機子電流を流した場合、
すなわち図示実線矢印の如く逆転させた場合、第
3図図示の如く補極3の部分が電機子反作用によ
り、減磁する方向に作用し、その特性が著しく低
下する。
By the way, when such a commutating pole 3 is connected to a magnetic motor installed near the permanent magnet 2 with the power supply voltage reversed, and an armature current is caused to flow as shown in FIG.
That is, when the magnet is reversed as shown by the solid line arrow in the figure, the part of the commutating pole 3 acts in the direction of demagnetization due to the armature reaction, as shown in FIG. 3, and its characteristics are significantly deteriorated.

(考案が解決しようとする問題点) このように補極3を備えた直巻特性を有する磁
石式モータにあつても、ほぼ同一の直巻特性を有
する正逆両回転が可能なモータの実現が強く要望
されている。
(Problems to be solved by the invention) Even in the case of a magnetic motor having a series winding characteristic and having a commutating pole 3, it is possible to realize a motor that can rotate in both forward and reverse directions and has almost the same series winding characteristic. is strongly requested.

本考案は上記の点を鑑みなされたものであり、
界磁を形成する永久磁石の両側端に補極をそれぞ
れ設けると共に、正逆いずれの回転方向において
も常に一方の補極が増磁方向に作用するような構
造にすることにより、正逆いずれの方向にも特性
がほぼ同一の直巻特性を有する磁石式モータを提
供することを目的としている。そしてそのため本
考案の磁石式モータは界磁を形成する円弧状の永
久磁石をヨークに備えると共に、該ヨークに補極
を備えた磁石式モータにおいて、 上記永久磁石の両側端近接に上記補極をそれぞ
れ設けると共に、 ダイオードで短絡された短絡巻線を上記補極に
それぞれ対応して設け、 かつ上記ダイオードは、上記永久磁石界磁に関
して回転方向の遅れ側に位置する補極における短
絡巻線には当該短絡巻線に誘起される電圧によつ
て生じる電流を阻止し、かつ回転方向の進み側に
位置する補極における短絡巻線には当該短絡巻線
に誘起される電圧によつて生じる電流を流す方向
に挿入されている ことを特徴としている。以下図面を参照しつつ説
明する。
This invention was made in consideration of the above points,
By providing commutative poles at both ends of the permanent magnet that forms the field, and by creating a structure in which one commutating pole always acts in the magnetizing direction in both forward and reverse rotation directions, It is an object of the present invention to provide a magnetic motor having series winding characteristics that are almost the same in both directions. For this reason, the magnet type motor of the present invention is equipped with an arc-shaped permanent magnet in the yoke that forms a field, and in a magnet type motor in which the yoke is equipped with commutating poles, the above-mentioned commutating poles are provided near both ends of the permanent magnet. In addition, a short-circuited winding short-circuited by a diode is provided corresponding to each of the above-mentioned commutative poles, and the above-mentioned diode is connected to the short-circuited winding of the commutative pole located on the lagging side in the rotational direction with respect to the above-mentioned permanent magnet field. The current generated by the voltage induced in the short-circuited winding is blocked, and the current generated by the voltage induced in the short-circuited winding is blocked in the short-circuited winding of the commutative pole located on the advancing side of the rotation direction. It is characterized by being inserted in the direction of flow. This will be explained below with reference to the drawings.

(実施例) 第1図は本考案に係る磁石式モータの一実施例
の部分説明図を示している。第1図において、符
号1,2,4,5は第2図、第3図のものに対応
している。符号6,7は補極、8,9は巻線、1
0,11はダイオードを表している。
(Embodiment) FIG. 1 shows a partial explanatory diagram of an embodiment of a magnet type motor according to the present invention. In FIG. 1, numerals 1, 2, 4, and 5 correspond to those in FIGS. 2 and 3. Symbols 6 and 7 are complementary poles, 8 and 9 are windings, 1
0 and 11 represent diodes.

界磁を形成する円弧状の永久磁石2の両側端近
傍に強磁性体の補極6,7が配設されている。こ
れらの補極6,7には巻線8,9がそれぞれ巻回
され、各巻線8,9の始端及び終端はダイオード
10,11でそれぞれ短絡されている。
Compensating poles 6 and 7 made of ferromagnetic material are arranged near both ends of the arc-shaped permanent magnet 2 that forms the field. Windings 8 and 9 are wound around these commutating poles 6 and 7, respectively, and the starting and ending ends of each winding 8 and 9 are short-circuited by diodes 10 and 11, respectively.

今、第1図図示の如く電機子巻線5に電流を流
すと、ロータ4は逆回転、すなわち反時計方向に
回転する。電機子巻線5に流れる電流によつて発
生する磁界、特にロータ4に設けられているスロ
ツトにより上記磁界にスロツトリプルの変化が生
じ、該磁界の変化によつて補極6,7に巻回され
ている巻線8,9に誘起電圧が発生する。該誘起
電圧は、補極6側ではダイオード10に順方向電
圧が印加され、ダイオード10を介して巻線8に
電流が流れるように動作するのに対し、補極7側
ではダイオード11に逆方向電圧が印加され、ダ
イオード11によつて巻線9に電流が流れるのを
阻止し、巻線9に電流が流れない動作をする電圧
となつている。従つて電機子巻線5に流れる電機
子反作用は、増磁作用が行われる補極7側の空隙
の磁束密度を第1図で説明した理由により大きく
し、減磁作用が行われる補極6側の空隙の磁束密
度を小さくするように働くが、図示の場合には実
質上補極7だけが設けられ、補極6が存在しない
従来の一方向回転の構造と同様の効果を発揮す
る。
Now, when a current is applied to the armature winding 5 as shown in FIG. 1, the rotor 4 rotates in the opposite direction, that is, counterclockwise. The magnetic field generated by the current flowing through the armature winding 5, particularly the slot provided in the rotor 4, causes a slot triple change in the magnetic field, and the change in the magnetic field causes the magnetic field to be wound around the commutating poles 6, 7. An induced voltage is generated in the windings 8 and 9. The induced voltage is caused by applying a forward voltage to the diode 10 on the side of the commutator 6, causing current to flow through the diode 10 to the winding 8, whereas on the side of the commutator 7, a voltage in the reverse direction is applied to the diode 11. When a voltage is applied, the diode 11 blocks current from flowing through the winding 9, and the voltage is such that no current flows through the winding 9. Therefore, the armature reaction flowing in the armature winding 5 increases the magnetic flux density in the air gap on the side of the commutator pole 7 where the magnetizing action is performed for the reason explained in FIG. This works to reduce the magnetic flux density in the side air gap, but in the case shown in the figure, only the commutative pole 7 is provided, and the same effect as the conventional unidirectional rotation structure in which the commutative pole 6 is not present is achieved.

また逆に電機子のロータ4が正回転、すなわち
時計方向回転する場合にあつては、補極7に巻回
された巻線9に電流が流れず、補極6に巻回され
た巻線8に電流が流れるように動作する。その結
果、増磁作用が行われる補極6側の空隙の磁束密
度は大きくなる。
Conversely, when the rotor 4 of the armature rotates in the forward direction, that is, in the clockwise direction, no current flows through the winding 9 wound around the commutative pole 7, and the winding wound around the commutative pole 6 It operates so that current flows through 8. As a result, the magnetic flux density in the air gap on the side of the commutator 6 where the magnetizing action is performed increases.

なお上記説明では永久磁石2について説明して
きたが、この永久磁石2と対をなす磁極、すなわ
ち図示されていない対を構成する永久磁石につい
ても全く同様に、該永久磁石の両側端近傍に補極
をそれぞれ設け、ダイオードで短絡された巻線を
上記の補極にそれぞれ巻回した構造に構成されて
いることは言うまでもない。そしてその動作につ
いても上記説明と全く同様である。
In the above explanation, the permanent magnet 2 has been explained, but the magnetic poles that form a pair with the permanent magnet 2, that is, the permanent magnets forming a pair (not shown), are also provided with commutating poles near both ends of the permanent magnet. Needless to say, the structure is such that a winding short-circuited by a diode is wound around each of the above-mentioned commutative poles. The operation is also exactly the same as described above.

(考案の効果) 以上説明した如く、本考案によれば、界磁を構
成する永久磁石の両側端近傍にそれぞれ補極を設
け、該補極にダイオードで短絡された巻線をそれ
ぞれ巻回しておく構造で、正逆両回転で同一特性
を出力することができる。
(Effects of the invention) As explained above, according to the invention, commutative poles are provided near both ends of the permanent magnets constituting the field, and windings short-circuited by diodes are wound around the commutative poles. The structure allows the same characteristics to be output in both forward and reverse rotations.

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

第1図は本考案に係る磁石式モータの一実施例
の部分説明図、第2図、第3図は従来の磁石式モ
ータの電機子反作用を説明している部分説明図を
示している。 図中、1はヨーク、2は永久磁石、3は補極、
4はロータ、5は電機子巻線、6,7は補極、
8,9は巻線、10,11はダイオードを表して
いる。
FIG. 1 is a partial explanatory diagram of an embodiment of a magnet type motor according to the present invention, and FIGS. 2 and 3 are partial explanatory diagrams illustrating the armature reaction of a conventional magnet type motor. In the figure, 1 is a yoke, 2 is a permanent magnet, 3 is a commutator,
4 is the rotor, 5 is the armature winding, 6 and 7 are the commutating poles,
8 and 9 represent windings, and 10 and 11 represent diodes.

Claims (1)

【実用新案登録請求の範囲】 界磁を形成する円弧状の永久磁石をヨークに備
えると共に、該ヨークに補極を備えた磁石式モー
タにおいて、 上記永久磁石の両側端近接に上記補極をそれぞ
れ設けると共に、 ダイオードで短絡された短絡巻線を上記補極に
それぞれ対応して設け、 かつ上記ダイオードは、上記永久磁石界磁に関
して回転方向の遅れ側に位置する補極における短
絡巻線には当該短絡巻線に誘起される電圧によつ
て生じる電流を阻止し、かつ回転方向の進み側に
位置する補極における短絡巻線には当該短絡巻線
に誘起される電圧によつて生じる電流を流す方向
に挿入されている ことを特徴とする磁石式モータ。
[Scope of Claim for Utility Model Registration] In a magnetic motor, the yoke is equipped with an arc-shaped permanent magnet that forms a field, and the yoke is equipped with commutating poles, wherein the commutating poles are provided near both ends of the permanent magnet, respectively. At the same time, a short-circuited winding short-circuited by a diode is provided corresponding to each of the commutative poles, and the diode is connected to the short-circuited winding of the commutative pole located on the lagging side in the rotational direction with respect to the permanent magnet field. Blocking the current generated by the voltage induced in the short-circuited winding, and allowing the current generated by the voltage induced in the short-circuited winding to flow through the shorted winding of the complementary pole located on the advancing side of the rotation direction. A magnetic motor characterized by being inserted in the direction.
JP8935485U 1985-06-13 1985-06-13 Expired JPH0312048Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8935485U JPH0312048Y2 (en) 1985-06-13 1985-06-13

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8935485U JPH0312048Y2 (en) 1985-06-13 1985-06-13

Publications (2)

Publication Number Publication Date
JPS61205240U JPS61205240U (en) 1986-12-24
JPH0312048Y2 true JPH0312048Y2 (en) 1991-03-22

Family

ID=30643349

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8935485U Expired JPH0312048Y2 (en) 1985-06-13 1985-06-13

Country Status (1)

Country Link
JP (1) JPH0312048Y2 (en)

Also Published As

Publication number Publication date
JPS61205240U (en) 1986-12-24

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