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JP2008148491A - Motor and motor armature - Google Patents

Motor and motor armature Download PDF

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Publication number
JP2008148491A
JP2008148491A JP2006334441A JP2006334441A JP2008148491A JP 2008148491 A JP2008148491 A JP 2008148491A JP 2006334441 A JP2006334441 A JP 2006334441A JP 2006334441 A JP2006334441 A JP 2006334441A JP 2008148491 A JP2008148491 A JP 2008148491A
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Japan
Prior art keywords
magnet
armature
coil
magnetic body
pole
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JP2006334441A
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Japanese (ja)
Inventor
Chiaki Nishikawa
千曉 西川
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Priority to JP2006334441A priority Critical patent/JP2008148491A/en
Priority to KR1020070030206A priority patent/KR100901896B1/en
Publication of JP2008148491A publication Critical patent/JP2008148491A/en
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K7/00Arrangements for handling mechanical energy structurally associated with dynamo-electric machines, e.g. structural association with mechanical driving motors or auxiliary dynamo-electric machines
    • H02K7/06Means for converting reciprocating motion into rotary motion or vice versa
    • H02K7/065Electromechanical oscillators; Vibrating magnetic drives
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B06GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06BMETHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B1/00Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
    • B06B1/10Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of mechanical energy
    • B06B1/16Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of mechanical energy operating with systems involving rotary unbalanced masses
    • 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
    • H02K1/22Rotating parts of the magnetic circuit
    • H02K1/27Rotor cores with permanent magnets
    • H02K1/2793Rotors axially facing stators
    • 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
    • H02K1/34Reciprocating, oscillating or vibrating parts of the magnetic circuit
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K13/00Structural associations of current collectors with motors or generators, e.g. brush mounting plates or connections to windings; Disposition of current collectors in motors or generators; Arrangements for improving commutation
    • H02K13/006Structural associations of commutators
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K23/00DC commutator motors or generators having mechanical commutator; Universal AC/DC commutator motors
    • H02K23/54Disc armature motors or generators
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K7/00Arrangements for handling mechanical energy structurally associated with dynamo-electric machines, e.g. structural association with mechanical driving motors or auxiliary dynamo-electric machines
    • H02K7/06Means for converting reciprocating motion into rotary motion or vice versa
    • H02K7/061Means for converting reciprocating motion into rotary motion or vice versa using rotary unbalanced masses
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K2213/00Specific aspects, not otherwise provided for and not covered by codes H02K2201/00 - H02K2211/00
    • H02K2213/03Machines characterised by numerical values, ranges, mathematical expressions or similar information

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  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Mechanical Engineering (AREA)
  • Dc Machiner (AREA)

Abstract

<P>PROBLEM TO BE SOLVED: To provide an armature which can be surely and smoothly started in rotation, even when the armature consists of one coil. <P>SOLUTION: A motor includes a flat plate-like magnet magnetized at a plurality of poles at a substantially equal angle, and an armature rotatably and pivotably supported facing the magnet and having a coil. A magnetic material is provided to the armature, and even when the magnetic material is positioned either at the boundary of each magnetized area of the magnet or at the center of each magnetized area of the magnet, the magnetic material is disposed at a position where the coil can be started. <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

本発明は、偏平モータに関し、特に、1個のコイルを備える電機子の構造に関する。   The present invention relates to a flat motor, and more particularly, to an armature structure including one coil.

携帯電話機等に利用される偏平モータとして、例えば、特開平6−205565号公報に開示された偏平型のコアレス振動モータが知られている。特開平6−205565号公報に開示された偏平コアレス振動モータは、ケーシングの底部に固定された平板状の円形磁石と、この磁石と面対向するように配置された回転自在の電機子と、電機子のかなめに配されたシャフトと、によって構成されている。電機子は、3個のコイルを扇形になるように配置し、樹脂フレームと一体成形されている。また、電機子は各コイルと共に回転する整流子を備え、整流子がケーシングの下部から延伸した2本の電極ブラシに接触することによって3個のコイルの極性が交互に切り替わり、そのたびに磁石3との間で引合力と反発力が発生するために電機子が回転する。特に、振動モータとして用いる場合には、前述のように電機子自体を大きく偏心させることによって、電機子が大きな遠心力を持って回転するため、振動モータに強い振動が発生することなる。   As a flat motor used for a cellular phone or the like, for example, a flat coreless vibration motor disclosed in Japanese Patent Laid-Open No. 6-205565 is known. A flat coreless vibration motor disclosed in Japanese Patent Laid-Open No. 6-205565 includes a flat circular magnet fixed to the bottom of a casing, a rotatable armature disposed so as to face the magnet, And a shaft arranged in the center of the child. The armature has three coils arranged in a fan shape and is integrally formed with the resin frame. The armature includes a commutator that rotates together with each coil. When the commutator comes into contact with two electrode brushes extending from the lower portion of the casing, the polarities of the three coils are alternately switched. Since an attractive force and a repulsive force are generated between the armature and the armature, the armature rotates. In particular, when used as a vibration motor, the armature itself is greatly decentered as described above, so that the armature rotates with a large centrifugal force, so that strong vibration is generated in the vibration motor.

また、電機子に1個のコイルを含む偏平モータとして、例えば、特許第3039857号公報に開示された偏平モータが知られている。特許第3039857号公報に開示された偏平モータは、電機子に磁性体を設け、電機子の回転を停止させた時に磁性体を磁石のN極とS極との境界に位置させ、コイルが起動可能位置にくるようにしている。
特開平6−205565号公報 特許第3039857号公報
Moreover, as a flat motor including one coil in an armature, for example, a flat motor disclosed in Japanese Patent No. 3039857 is known. In the flat motor disclosed in Japanese Patent No. 3039857, the armature is provided with a magnetic body, and when the armature stops rotating, the magnetic body is positioned at the boundary between the north and south poles of the magnet, and the coil is activated. It tries to come to a possible position.
JP-A-6-205565 Japanese Patent No. 3039857

前述した電機子に1個のコイルを含む偏平モータでは電機子に磁性体を設け、電機子の回転を停止させた時に磁性体を磁石のN極とS極との境界に位置させている。しかし、電機子の回転を停止させた時に磁性体を磁石のN極とS極との境界に位置しても、コイルと磁性体との位置関係を適切に定めなければ、コイルが起動可能位置に停止しないことがある。   In the above-described flat motor including one coil in the armature, the armature is provided with a magnetic body, and the magnetic body is positioned at the boundary between the N pole and the S pole of the magnet when the rotation of the armature is stopped. However, even if the magnetic body is positioned at the boundary between the north and south poles of the magnet when the armature stops rotating, if the positional relationship between the coil and the magnetic body is not properly determined, the coil can be activated. May not stop.

さらに、電機子に設けられた磁性体は磁石のN極とS極との境界の他、各極の中央に停止することがある。この状態では、磁石によって生じる磁力が弱い点(磁束密度が少ない点)に、コイルが停止することから、電機子が起動しない可能性がある。   Furthermore, the magnetic body provided in the armature may stop at the center of each pole in addition to the boundary between the N pole and S pole of the magnet. In this state, since the coil stops at a point where the magnetic force generated by the magnet is weak (a point where the magnetic flux density is low), the armature may not start.

この問題点を具体的に説明するために、一例として、電機子のコイルと磁性体とがなす角度(電機子の経方向に電流が流れる点(A点及びB点)のうち磁性体と近い点と、磁性体の中心とのなす角度)が45度である場合を考える。   In order to specifically explain this problem, as an example, the angle between the coil of the armature and the magnetic body (the point where the current flows in the longitudinal direction of the armature (points A and B) is close to the magnetic body. Let us consider a case where the angle between the point and the center of the magnetic body is 45 degrees.

図7に示すように、電機子4に設けられた磁性体10が磁石3のN極とS極との境界に停止した場合、コイル6のA点及びB点は磁石3の中央部(すなわち、磁束密度の大きい点)に位置する。よって、コイル6に電流が流れたときに、コイル6には強い電磁力が加わり、電機子が回転する。   As shown in FIG. 7, when the magnetic body 10 provided in the armature 4 stops at the boundary between the north pole and the south pole of the magnet 3, the point A and the point B of the coil 6 are the center part of the magnet 3 (that is, , Located at a point where the magnetic flux density is large. Therefore, when a current flows through the coil 6, a strong electromagnetic force is applied to the coil 6 and the armature rotates.

一方、図8に示すように、電機子4に設けられた磁性体10が磁石3のN極の中央に停止した場合、コイル6のA点及びB点は磁石3の境界(すなわち、磁束密度の少ない点)に位置する。よって、コイル6に電流が流れたときに、コイル6に加わる電磁力は弱く、電機子4が回転を始めるトルクには足りず、モータが起動しないことがある。   On the other hand, as shown in FIG. 8, when the magnetic body 10 provided in the armature 4 stops at the center of the north pole of the magnet 3, the points A and B of the coil 6 are the boundaries of the magnet 3 (that is, the magnetic flux density). It is located at a point with less. Therefore, when a current flows through the coil 6, the electromagnetic force applied to the coil 6 is weak, the torque at which the armature 4 starts to rotate is insufficient, and the motor may not start.

なお、磁石は、通常、電機子の整流子側に配置されるが、図7及び図8では、説明のため電機子の後側に図示した。   The magnet is usually arranged on the commutator side of the armature, but in FIGS. 7 and 8, it is shown on the rear side of the armature for the sake of explanation.

そこで、本発明は、1個のコイルで電機子を構成した場合にも、回転が確実かつスムーズに起動される電機子によって、信頼性の高いモータを提供することを目的とする。   Therefore, an object of the present invention is to provide a highly reliable motor by an armature that is reliably and smoothly started even when an armature is constituted by a single coil.

第1の発明は、略均等な角度で複数極に着磁された平板状の磁石と、前記磁石に対向して回転可能に軸支され、コイルを有する電機子と、を備えるモータであって、前記電機子に磁性体を設け、前記磁性体が前記磁石の各着磁領域の境界及び前記磁石の各着磁領域の中央の何れに位置した場合でも、前記コイルが起動可能となる位置に前記磁性体を配置した。   A first invention is a motor comprising: a plate-like magnet magnetized with a plurality of poles at substantially equal angles; and an armature that is rotatably supported so as to face the magnet and has a coil. The armature is provided with a magnetic body, and the coil can be activated even when the magnetic body is located at either the boundary of the magnetized regions of the magnet or the center of the magnetized regions of the magnet. The magnetic body was disposed.

第2の発明は、第1の発明において、前記コイルの端部は、前記磁性体が前記磁石の各着磁領域の境界及び前記磁石の各着磁領域の中央の何れに位置した場合でも、前記各着磁領域の境界から所定距離だけ離れた位置に配置されることを特徴とする請求項1に記載のモータ。   According to a second aspect of the present invention, in the first aspect, the end of the coil may be located at any of the boundary between the magnetized regions of the magnet and the center of the magnetized regions of the magnet. The motor according to claim 1, wherein the motor is disposed at a position away from a boundary of each magnetized region by a predetermined distance.

第3の発明は、第1又は第2の発明において、前記コイルの中心角は前記各着磁領域の中心角と略等しく、前記磁性体は、前記各着磁領域の中心角をθとした場合、前記コイルの一端から、中心角が(2n+1)×0.25×θ(nは整数)を満たす位置に配置される。   According to a third invention, in the first or second invention, a central angle of the coil is substantially equal to a central angle of each of the magnetized regions, and the magnetic body has a central angle of each of the magnetized regions as θ. In this case, the coil is disposed at a position where the central angle satisfies (2n + 1) × 0.25 × θ (n is an integer) from one end of the coil.

第4の発明は、第1から第3の発明において、前記コイルの中心角は前記各着磁領域の中心角と略等しく、前記磁性体は、前記コイルの一端から、前記各着磁領域の中心角の0.25倍及び0.75倍の少なくとも一方の位置に配置される。   According to a fourth invention, in the first to third inventions, a central angle of the coil is substantially equal to a central angle of each of the magnetized regions, and the magnetic body extends from one end of the coil to each of the magnetized regions. It arrange | positions in at least one position of 0.25 times and 0.75 times of a central angle.

第5の発明は、第1から第4の発明において、前記磁石は4極に着磁されており、前記磁性体は、前記コイルの一端から、中心角が22.5度及び67.5度の少なくとも一方の位置に配置される。   According to a fifth invention, in the first to fourth inventions, the magnet is magnetized into four poles, and the magnetic body has center angles of 22.5 degrees and 67.5 degrees from one end of the coil. It arrange | positions in at least one position.

第6の発明は、略均等な角度で複数極に着磁された平面を含む磁石を有するモータ内で、前記磁石に対向して回転可能に軸支される電機子であって、コイル及び磁性体を備え、前記磁性体が前記磁石の各着磁領域の境界及び前記磁石の各着磁領域の中央の何れに位置した場合でも、前記コイルが起動可能となる位置に前記磁性体を配置した。   A sixth invention is an armature that is rotatably supported opposite to a magnet in a motor having a magnet including a plane magnetized with a plurality of poles at substantially equal angles, the coil and the magnet The magnetic body is disposed at a position where the coil can be activated regardless of whether the magnetic body is located at the boundary between the magnetized regions of the magnet or at the center of the magnetized region of the magnet. .

本発明によると、磁性体が磁石の各着磁領域の境界及び磁石の各着磁領域の中央の何れに位置した場合でも、コイルが起動可能となる位置に停止するので、コイルの回転力を生じる巻線部分が磁石内に停止する。すなわち、コイルの回転力を生じる巻線部分が各着磁領域の境界に停止しないので、電機子の起動に十分な電磁力を得ることができ、電機子の回転をスムーズに起動することができる。   According to the present invention, the coil stops at the position where the coil can be activated regardless of whether the magnetic body is located at the boundary between the magnetized regions of the magnet or the center of the magnetized region of the magnet. The resulting winding part stops in the magnet. That is, since the winding portion that generates the rotational force of the coil does not stop at the boundary of each magnetized region, an electromagnetic force sufficient for starting the armature can be obtained, and the rotation of the armature can be started smoothly. .

また、1個のコイルで電機子を構成した場合でも、電機子の回転が確実かつスムーズに起動され、偏平モータのより一層の極小化及び軽量化を図ることができ、さらに、製造コストを低減することができる。   In addition, even when the armature is composed of a single coil, the rotation of the armature can be started reliably and smoothly, and the flat motor can be further minimized and reduced in weight, further reducing the manufacturing cost. can do.

以下、図面に基づいて本発明に係る偏平モータの構造を説明する。   Hereinafter, the structure of the flat motor according to the present invention will be described with reference to the drawings.

図1は、本発明の実施の形態の偏平モータの一例を示す縦断面図である。   FIG. 1 is a longitudinal sectional view showing an example of a flat motor according to an embodiment of the present invention.

本実施の形態の偏平モータ1は、その構成要素が上部ケーシング2A及び下部ケーシング2Bによって形成された空間に収容されている。下部ケーシング2Bには、その内側に、平板状の磁石3が固定されている。磁石3は、略円盤形(より正確には、中央部が欠落したドーナッツ形の板状)に形成されており、複数極に分割して着磁されている。よって、分割して着磁された一つの着磁領域によって、N極とS極とを含む一つの磁石が形成される。なお、本実施の形態では、円板を4等分してN極とS極を交互に配列した4極着磁の磁石を示すが、他の極数(例えば、6極、8極等)に着磁された磁石を用いてもよい。   The flat motor 1 of the present embodiment is housed in a space formed by the upper casing 2A and the lower casing 2B. A flat magnet 3 is fixed to the inside of the lower casing 2B. The magnet 3 is formed in a substantially disk shape (more precisely, a donut-shaped plate shape with a missing central portion), and is magnetized by being divided into a plurality of poles. Therefore, one magnet including the N pole and the S pole is formed by one magnetized region that is divided and magnetized. In the present embodiment, a four-pole magnetized magnet is shown in which a disc is divided into four equal parts and N poles and S poles are alternately arranged, but other numbers of poles (for example, 6 poles, 8 poles, etc.) You may use the magnet magnetized by.

上部ケーシング2Aの中心部及び下部ケーシング2Bの中心部には、各々、軸受12、13が設けられている。軸受12、13には、回転自在にシャフト5が取り付けられている。シャフト5には、樹脂フレーム7によって構成された電機子4が取り付けられている。よって、電機子4は、軸受け12及び13を介して、ケーシング2A及び2Bに対し回転可能に取り付けられている。   Bearings 12 and 13 are provided at the center of the upper casing 2A and the center of the lower casing 2B, respectively. A shaft 5 is rotatably attached to the bearings 12 and 13. An armature 4 composed of a resin frame 7 is attached to the shaft 5. Therefore, the armature 4 is rotatably attached to the casings 2A and 2B via the bearings 12 and 13.

なお、図1には、シャフト5が軸受12及び13を貫通するように図示したが、シャフト5が軸受12及び13を貫通せず、シャフト5の端部が露出しないように構成してもよい。また、軸受12及び13をケーシング2A及び2Bに設け、シャフト5がケーシング2A及び2Bに対し回転可能に設けられているが、シャフト5をケーシング2A及び2Bに固定し、電機子4に軸受を設けて、電機子4がシャフト5に対して回転可能な構造(いわゆる、固定シャフト構造)にしてもよい。   In FIG. 1, the shaft 5 is illustrated so as to penetrate the bearings 12 and 13. However, the shaft 5 may not penetrate the bearings 12 and 13 and the end portion of the shaft 5 may not be exposed. . Further, the bearings 12 and 13 are provided in the casings 2A and 2B, and the shaft 5 is rotatably provided to the casings 2A and 2B. The shaft 5 is fixed to the casings 2A and 2B, and the armature 4 is provided with a bearing. Thus, the armature 4 may be structured to be rotatable with respect to the shaft 5 (so-called fixed shaft structure).

電機子4の樹脂フレーム7には、略台形状(中心部分が欠落した扇形)のコイル6が一体成形されている。   The resin frame 7 of the armature 4 is integrally formed with a coil 6 having a substantially trapezoidal shape (a sector having a missing central portion).

また、電機子4は、コイル6に接続された整流子8を備えている。下部ケーシング2Bには、内側に延伸する2本のブラシ9が設けられている。ブラシ9の一端は、偏平モータに対し直流電源が供給される電源供給端子(図示省略)に接続されている。ブラシ9の他端(接触部)は整流子8と接触している。整流子8とブラシ9との接触によって、コイル6へ電流が供給される。そして、電機子4が回転することによって、整流子8とブラシ9との接触点が移動して、コイル6の極性が切り替わる。コイル6の極性が切り替わるたびに、コイル6と磁石3との間で引合力と反発力が発生するため、電機子4が回転し続ける。   The armature 4 includes a commutator 8 connected to the coil 6. The lower casing 2B is provided with two brushes 9 extending inward. One end of the brush 9 is connected to a power supply terminal (not shown) through which DC power is supplied to the flat motor. The other end (contact portion) of the brush 9 is in contact with the commutator 8. A current is supplied to the coil 6 by the contact between the commutator 8 and the brush 9. When the armature 4 rotates, the contact point between the commutator 8 and the brush 9 moves, and the polarity of the coil 6 is switched. Every time the polarity of the coil 6 is switched, an attracting force and a repulsive force are generated between the coil 6 and the magnet 3, so that the armature 4 continues to rotate.

図2は、本発明の実施の形態の電機子4の構成を示す裏面図(整流子8方向から見た図)である。   FIG. 2 is a rear view (viewed from the direction of the commutator 8) showing the configuration of the armature 4 according to the embodiment of the present invention.

電機子4は、前述したように、略台形状のコイル6が一体成形された樹脂フレーム7によって構成されている。さらに、樹脂フレーム7の裏面側には、シャフト5を中心として4極に分割された整流子8を備えている。すなわち、電機子4は、樹脂フレーム7の内部に1個の略1/4円形のコアレスコイル6、及び、磁性体10を配置して、これらを一体に扇形に成形したものである。なお、図2に示すように、電機子4を形成する扇形の中心角は180度を超えてもよい。   As described above, the armature 4 is constituted by the resin frame 7 in which the substantially trapezoidal coil 6 is integrally formed. Further, a commutator 8 divided into four poles around the shaft 5 is provided on the back side of the resin frame 7. In other words, the armature 4 is formed by disposing one substantially quarter circular coreless coil 6 and a magnetic body 10 inside a resin frame 7 and integrally molding them into a fan shape. In addition, as shown in FIG. 2, the center angle of the sector which forms the armature 4 may exceed 180 degree | times.

コイル6は、樹脂フレーム7の形状に略対応した形状の1巻きのコアレスコイルであり、両側縁(コイルの巻線に直径方向に電流が流れる部分)の開き角度θは約90度である。なお、偏平モータ1を振動モータとして利用する場合には、遠心力を大きくするためにコイル6の空心部に錘を配設するとよい。   The coil 6 is a single coreless coil having a shape substantially corresponding to the shape of the resin frame 7, and an opening angle θ of both side edges (portions where current flows in the diameter direction of the coil winding) is about 90 degrees. When the flat motor 1 is used as a vibration motor, a weight may be disposed in the air core of the coil 6 in order to increase the centrifugal force.

樹脂フレーム7のかなめ部分には円を略4等分した四つの電極を有する整流子8が設けられている。整流子8の中心(電機子4の回転中心と等しい位置)には、軸孔が開設されており、軸孔にはシャフト5が挿入されている。また、整流子8は、対角線方向で対向する2個の電極がそれぞれ接続されており、一方の電極にコアレスコイル6の内側の端部が接続され、他方の電極に外側の端部が接続されている。   The crimped portion of the resin frame 7 is provided with a commutator 8 having four electrodes obtained by dividing a circle into four equal parts. A shaft hole is formed at the center of the commutator 8 (position equal to the rotation center of the armature 4), and the shaft 5 is inserted into the shaft hole. The commutator 8 is connected to two electrodes facing each other in the diagonal direction, one end of which is connected to the inner end of the coreless coil 6, and the other electrode is connected to the outer end. ing.

なお、本実施の形態で、電機子4は、約90度の角度をもつ略1/4円形のコイル6を備えているが、コイルの形状はこれに限定されない。コイル6が略1/4円形であることは、磁石3が4極に分割して着磁されていることに対応するものである。すなわち、コイルの中心角は、磁石3が分割して着磁されている一つの着磁領域の中心角とほぼ同じ角度である。よって、本実施の形態のように磁石3が4極に着磁されている場合は、コイル6は約90度の中心角で形成される。また、例えば、磁石3が6極に分割して着磁されている場合には、コイルは約60度の角度をもつ略1/6円形に形成されることが望ましい。なお、整流子8もコイル6の中心角に応じてその電極が分割されている。   In the present embodiment, the armature 4 includes a substantially quarter circular coil 6 having an angle of about 90 degrees, but the shape of the coil is not limited to this. The fact that the coil 6 has a substantially quarter circle corresponds to the magnet 3 being divided into four poles and magnetized. That is, the central angle of the coil is substantially the same as the central angle of one magnetized region where the magnet 3 is divided and magnetized. Therefore, when the magnet 3 is magnetized to four poles as in the present embodiment, the coil 6 is formed with a central angle of about 90 degrees. Further, for example, when the magnet 3 is divided into 6 poles and magnetized, the coil is preferably formed in a substantially 1/6 circle having an angle of about 60 degrees. The commutator 8 also has its electrodes divided according to the center angle of the coil 6.

また、電機子4の樹脂フレーム7に配置された磁性体10は、鉄製の細い丸棒で形成することができ、電機子4の回転方向(又は、逆回転方向)と略平行に配置される。なお、磁性体10は細い丸棒に限らず、平板状の小片であっても、長方形断面の角棒であってもよい。磁性体10を回転方向に沿って長く形成することによって、磁性体10の両側にN極とS極とが形成され易くなる。本発明では、電機子4が停止するときに、磁性体10には所定の位置で電機子を強制的に停止させる磁力が必要である。さらに、電機子4の回転運動を妨げない程度の磁力であることが必要である。   Further, the magnetic body 10 disposed on the resin frame 7 of the armature 4 can be formed of a thin round bar made of iron, and is disposed substantially parallel to the rotation direction (or reverse rotation direction) of the armature 4. . In addition, the magnetic body 10 is not limited to a thin round bar, and may be a flat piece or a square bar having a rectangular cross section. By forming the magnetic body 10 long along the rotation direction, the N pole and the S pole are easily formed on both sides of the magnetic body 10. In the present invention, when the armature 4 stops, the magnetic body 10 needs a magnetic force for forcibly stopping the armature at a predetermined position. Furthermore, it is necessary to have a magnetic force that does not hinder the rotational movement of the armature 4.

磁性体10は、その中央がコイル6の一端(A点)から略67.5度の中心角の位置に配置されている。この位置は、後述するように、磁石の一つの着磁領域の中心角(90度)の3/4に相当する。   The center of the magnetic body 10 is disposed at a central angle of about 67.5 degrees from one end (point A) of the coil 6. As will be described later, this position corresponds to 3/4 of the central angle (90 degrees) of one magnetized region of the magnet.

磁性体10は、回転方向と略平行に配置されているが、磁性体10の両側にN極及びS極を発生させることができれば、必ずしも直交していなくてもよい。   Although the magnetic body 10 is disposed substantially parallel to the rotation direction, the magnetic body 10 may not necessarily be orthogonal as long as the N pole and the S pole can be generated on both sides of the magnetic body 10.

また、図5に示すように、磁性体10を、その中央がコイル6の一端(A点)から略22.5度の中心角の位置に配置してもよい。この位置は、後述するように、磁石の一つの着磁領域の中心角(90度)の1/4に相当する位置である。   In addition, as shown in FIG. 5, the magnetic body 10 may be disposed at a center angle of about 22.5 degrees from the one end (point A) of the coil 6. As will be described later, this position corresponds to a quarter of the central angle (90 degrees) of one magnetized region of the magnet.

また、図6に示すように、磁性体10をコイル6の空心部に設けてもよい。この場合、磁性体10の中央は、コイル6の一端(A点)から略67.5度の中心角で、コイル6の他端(B点)から略22.5度の中心角の位置に配置されている。この位置は、後述するように、磁石3の一つの着磁領域の中心角(90度)の3/4(B点からは1/4)に相当する位置である。   In addition, as shown in FIG. 6, the magnetic body 10 may be provided in the air core portion of the coil 6. In this case, the center of the magnetic body 10 is at a center angle of about 67.5 degrees from one end (point A) of the coil 6 and at a center angle of about 22.5 degrees from the other end (point B) of the coil 6. Has been placed. As will be described later, this position corresponds to 3/4 of the central angle (90 degrees) of one magnetized region of the magnet 3 (1/4 from the point B).

すなわち、本発明を適用した偏平モータの電機子4では、磁性体はコイルの一端から磁石3の一つの着磁領域の中心角をθとしたときに、
(2n+1)×0.25×θ (nは整数)
を満たす位置にあればよい。
That is, in the armature 4 of the flat motor to which the present invention is applied, the magnetic body has a central angle of one magnetized region of the magnet 3 from one end of the coil as θ,
(2n + 1) × 0.25 × θ (n is an integer)
It suffices if it is in a position that satisfies

さらに、図6に破線で図示するように、電機子4の応用として、電機子4に二つの磁性体を設け、一つの磁性体10の中央はコイル6の一端(A点)から略22.5度(B点から略67.5度)の中心角で、他方の磁性体11の中央はコイル6の他端(B点)から略22.5度(A点から略67.5度)の中心角の位置に配置することもできる。この位置は、後述するように、磁石の一つの着磁領域の中心角(90度)の1/4に相当する位置である。   Further, as shown by a broken line in FIG. 6, as an application of the armature 4, two armatures are provided in the armature 4, and the center of one magnetic body 10 is approximately 22.2 from one end (point A) of the coil 6. The center angle of the other magnetic body 11 is about 22.5 degrees from the other end (point B) of the coil 6 (about 67.5 degrees from the point A) with a central angle of 5 degrees (approximately 67.5 degrees from the point B). It can also be arranged at the center angle position. As will be described later, this position corresponds to a quarter of the central angle (90 degrees) of one magnetized region of the magnet.

またさらに、図2、図5及び図6に示す配置の磁性体を複数備えるように電機子4を構成してもよい。例えば、図2に示すようにコイル6のA点から外側に67.5度の位置に第1の磁性体10を設け、図6に示すようにコイル6のA点から内側に22.5度の位置に第2の磁性体11を設けてもよい。この磁性体の数及び磁性体の位置の組み合わせは、前述した磁性体の配置位置の条件を満たせば、任意に選択することができる。   Furthermore, the armature 4 may be configured to include a plurality of magnetic bodies arranged as shown in FIGS. 2, 5, and 6. For example, the first magnetic body 10 is provided at a position of 67.5 degrees outward from the point A of the coil 6 as shown in FIG. 2, and 22.5 degrees inward from the point A of the coil 6 as shown in FIG. The second magnetic body 11 may be provided at this position. The combination of the number of magnetic bodies and the positions of the magnetic bodies can be arbitrarily selected as long as the above-described conditions for the arrangement positions of the magnetic bodies are satisfied.

なお、磁性体10は、図2に示すように、樹脂フレーム7の中に埋め込んで一体成形されなくても、公知技術である特許第3039857号公報の図1に示すように、樹脂フレーム7の一側縁から側方(回転方向)に突出してもよい。この場合、磁性体10は、円弧の一部を構成するように内側にやや湾曲するとよい。   As shown in FIG. 1 of FIG. 1 of Japanese Patent No. 3039857, which is a known technique, the magnetic body 10 is not embedded and integrally molded in the resin frame 7 as shown in FIG. You may protrude in the side (rotation direction) from one side edge. In this case, the magnetic body 10 may be slightly curved inward so as to constitute a part of the arc.

次に、本発明の実施の形態の偏平モータ1の回転原理について説明する。   Next, the rotation principle of the flat motor 1 according to the embodiment of the present invention will be described.

図1に示すように、下部ケーシング2Bからは2本のブラシ9が延伸しており、その先端部に設けられた接触部と電機子4の整流子8の各電極とが接触する。そして、各ブラシ9は、電機子4の回転に伴って整流子8の上を所定の角度(例えば、約90度)ずれて摺動しながら、順次、整流子8との接触点を移動していく。   As shown in FIG. 1, two brushes 9 extend from the lower casing 2 </ b> B, and a contact portion provided at the tip of the brush 9 contacts each electrode of the commutator 8 of the armature 4. Each brush 9 sequentially moves at the contact point with the commutator 8 while sliding on the commutator 8 at a predetermined angle (for example, about 90 degrees) as the armature 4 rotates. To go.

図3に電機子4が停止している時の状態を示す。図3に示す状態では、コイル6の大部分が磁石3の一つのS極上に重なっており、一部分が磁石3の一つのN極上に重なっている。この状態で偏平モータ1に電源を供給すると、ブラシ9の先端が接触する整流子8の電極を介してコイル6に電流が流れることによって、コイル6に磁界が発生する。このときコイル6の磁石3と向かい合う側(図面において手前側)に発生した磁界の極性がS極であるとすると、その近傍の磁石3のS極との間で反発力が発生する。また、磁石3の隣のN極とは互いに引き合うために、その方向(反時計回り方向)に回転力が発生して電機子4の回転が起動する。なお、磁石3は、本来、電機子4の裏面側(整流子8の側)に配置されているが、図3及び図4では、説明のため電機子の後側に図示した。   FIG. 3 shows a state when the armature 4 is stopped. In the state shown in FIG. 3, most of the coil 6 overlaps with one S pole of the magnet 3, and a part overlaps with one N pole of the magnet 3. When power is supplied to the flat motor 1 in this state, a current flows through the coil 6 through the electrode of the commutator 8 with which the tip of the brush 9 contacts, thereby generating a magnetic field in the coil 6. If the polarity of the magnetic field generated on the side of the coil 6 facing the magnet 3 (front side in the drawing) is the S pole, a repulsive force is generated between the S pole of the magnet 3 in the vicinity thereof. Further, since the N poles adjacent to the magnet 3 attract each other, a rotational force is generated in that direction (counterclockwise direction), and the armature 4 starts to rotate. The magnet 3 is originally disposed on the back surface side (commutator 8 side) of the armature 4, but in FIG. 3 and FIG. 4, it is illustrated on the rear side of the armature for explanation.

そして、さらに電機子4が回転すると、整流子8の隣の電極がブラシ9の接触部を接触することからコイル6には図3に示す状態と逆方向の電流が流れる。このため、コイル6には磁石3と向かい合う側に逆の極性(N極)が発生し、磁石3の下側のN極と反発し合い、同じ方向の回転力が付与されて回り続ける。   When the armature 4 is further rotated, the electrode adjacent to the commutator 8 contacts the contact portion of the brush 9, so that a current in the direction opposite to that shown in FIG. For this reason, a reverse polarity (N pole) is generated in the coil 6 on the side facing the magnet 3, repels the N pole on the lower side of the magnet 3, and a rotating force in the same direction is applied to keep rotating.

このように、電機子4の回転に従って、コイル6はN極とS極とを交互に繰り返し、磁石3との間で反発と引き合いを繰り返す。これによって、電機子4は回転し続けることができる。   Thus, according to the rotation of the armature 4, the coil 6 alternately repeats the N pole and the S pole, and repeats repulsion and attraction with the magnet 3. As a result, the armature 4 can continue to rotate.

なお、電機子4を逆方向(時計回り方向)に回転させる場合には、電流の供給方向を逆にするか、又は、コイル6の巻き方向を逆にする。   When the armature 4 is rotated in the reverse direction (clockwise direction), the current supply direction is reversed or the winding direction of the coil 6 is reversed.

図3及び図4は、本発明の図2に示す実施の形態の電機子4の回転原理を示す起動時の説明図であり、図3は、電機子4に設けられた磁性体10が磁石3のN極とS極との境界に停止した状態を、図4は、電機子4に設けられた磁性体10が磁石3のN極の中央に停止した状態を示す。   3 and 4 are explanatory diagrams at the time of start-up showing the rotation principle of the armature 4 of the embodiment shown in FIG. 2 of the present invention, and FIG. 3 shows that the magnetic body 10 provided in the armature 4 is a magnet. FIG. 4 shows a state where the magnetic body 10 provided in the armature 4 is stopped at the center of the N pole of the magnet 3.

以上説明した構造を有する本実施の形態の電機子4は、電機子4を磁石3上で時計回り(又は、反時計回り)に回転させた後、電機子4のコイル6に供給される電源を遮断すると、図3に示すように、磁性体10の長手方向の中央が磁石3のN極とS極との境界線21上に位置した状態で停止する。これは、磁性体10が磁石3のN極とS極との境界線21上に位置すると、磁石3の影響によって磁性体10の長手方向の一端がS極に磁化され、他端がN極に磁化されることから、磁石3と磁性体10とが引き合い、電機子4の自由回転に打ち勝ってその位置で停止する安定した状態になるからである。   In the armature 4 of the present embodiment having the structure described above, after the armature 4 is rotated clockwise (or counterclockwise) on the magnet 3, the power supplied to the coil 6 of the armature 4 is supplied. 3, the center of the magnetic body 10 in the longitudinal direction is stopped on the boundary line 21 between the N pole and the S pole of the magnet 3 as shown in FIG. This is because when the magnetic body 10 is positioned on the boundary line 21 between the N pole and the S pole of the magnet 3, one end in the longitudinal direction of the magnetic body 10 is magnetized to the S pole by the influence of the magnet 3, and the other end is the N pole. This is because the magnet 3 and the magnetic body 10 are attracted to each other and overcome the free rotation of the armature 4 to be in a stable state where it stops at that position.

このとき、電機子4に設けられた磁性体10が磁石3のN極とS極との境界に停止した場合、コイル6のA点及びB点は磁石3のN極の中央又はS極の中央から約22.5度離れた点に位置する。よって、コイル6に電流が流れたときに、電機子4の起動に十分な電磁力がコイル6に加わり、電機子4が回転する。   At this time, when the magnetic body 10 provided in the armature 4 stops at the boundary between the N pole and the S pole of the magnet 3, the points A and B of the coil 6 are the center of the N pole of the magnet 3 or the S pole. It is located at a point about 22.5 degrees away from the center. Therefore, when a current flows through the coil 6, an electromagnetic force sufficient for starting the armature 4 is applied to the coil 6 and the armature 4 rotates.

また、本実施の形態の電機子4は、電機子4を磁石3上で時計回り(又は、反時計回り)に回転させた後、電機子4のコイル6に供給される電源を遮断すると、図4に示すように、磁性体10の長手方向の中央が磁石3のS極(又は、N極)の中央に位置した状態でも停止する。これは、磁石3のN極(又は、S極)の中央部は磁束密度が大きいことから、磁性体10が磁石3のS極(又は、S極)の中央に引き寄せられ、電機子4の自由回転に打ち勝ってその位置で停止する安定した状態になるからである。   Further, the armature 4 of the present embodiment, when the armature 4 is rotated clockwise (or counterclockwise) on the magnet 3 and then the power supplied to the coil 6 of the armature 4 is cut off, As shown in FIG. 4, the magnetic body 10 stops even when the center in the longitudinal direction is located at the center of the south pole (or north pole) of the magnet 3. This is because the magnetic part 10 is attracted to the center of the S pole (or S pole) of the magnet 3 because the magnetic flux density is large in the center part of the N pole (or S pole) of the magnet 3. It is because it will be in a stable state where it overcomes the free rotation and stops at that position.

このとき、電機子4に設けられた磁性体10が磁石3のS極の中央に停止した場合(N極の中央に停止した場合も同じ)、コイル6のA点及びB点は磁石3のN極の中央又はS極の中央から約22.5度離れた点に位置する。よって、コイル6に電流が流れたときに、電機子4の起動に十分な電磁力がコイル6に加わり、電機子4が回転する。   At this time, when the magnetic body 10 provided in the armature 4 stops at the center of the S pole of the magnet 3 (the same applies when it stops at the center of the N pole), the points A and B of the coil 6 are It is located at a point about 22.5 degrees away from the center of the north pole or the center of the south pole. Therefore, when a current flows through the coil 6, an electromagnetic force sufficient for starting the armature 4 is applied to the coil 6 and the armature 4 rotates.

すなわち、本実施の形態の偏平モータ1は、磁性体10の作用によって電機子4が何れの位置に停止しても、磁石3のS極の中央又はN極の中央から約22.5度離れた点にコイル6の回転力を生じる巻線部分(A点及びB点)が停止する。以上の説明から分かるように、この22.5度離れた位置は、磁石3のS極(又は、N極)の中央とS極とN極との境界部の中間点である。   That is, the flat motor 1 according to the present embodiment is about 22.5 degrees away from the center of the S pole or the center of the N pole of the magnet 3 regardless of the position of the armature 4 due to the action of the magnetic body 10. The winding portion (point A and point B) that generates the rotational force of the coil 6 stops at the point. As can be seen from the above description, the position 22.5 degrees apart is the midpoint of the boundary between the center of the south pole (or north pole) of the magnet 3 and the south pole and north pole.

なお、本実施形態で示した、22.5度は磁石3の一つの着磁領域の中心角(90度)の1/4に相当し、67.5度は磁石3の一つの着磁領域の中心角(90度)の3/4に相当する。すなわち、22.5度は磁石3の一つの着磁領域の中央と隣接した着磁領域との境界とのなす角の半分である。この半分の角度の位置に磁性体10を配置すれば、磁性体10が磁石3のN極とS極との境界に停止した場合と、磁性体10が磁石3のN極(又は、S極)の中央に停止した場合とで、均等な電磁力が得られて、電機子4のスムーズな起動を実現することができる。   In addition, 22.5 degree | times shown by this embodiment are equivalent to 1/4 of the center angle (90 degree | times) of one magnetization area | region of the magnet 3, and 67.5 degree | times is one magnetization area | region of the magnet 3. Is equivalent to 3/4 of the central angle (90 degrees). That is, 22.5 degrees is half the angle formed by the center of one magnetized region of the magnet 3 and the boundary between adjacent magnetized regions. If the magnetic body 10 is arranged at the half angle position, the magnetic body 10 stops at the boundary between the N pole and the S pole of the magnet 3, and the magnetic body 10 has the N pole (or S pole) of the magnet 3. ) And the case where the armature 4 is stopped at the center, an even electromagnetic force can be obtained and the armature 4 can be smoothly started.

なお、22.5度及び67.5度は、本発明によって提案される最適な角度値であるが、この角度が少し(例えば、数度)ずれても、二つの停止状態で電機子4の起動時の電磁力がアンバランスになるが、電機子4の起動に大きな影響はない範囲であれば構わない。例えば、磁性体10が磁石3のN極とS極との境界に停止した場合に、コイル6のA点が磁石のN極(又は、S極)の中央から15度になるようにすれば、磁性体10が磁石3のN極(又は、S極)の中央に停止した場合には、コイル6のA点は磁石のN極(又は、S極)の中央から30度だけ離れる。この場合でも電機子4の起動に大きな影響はない。   Note that 22.5 degrees and 67.5 degrees are the optimum angle values proposed by the present invention, but even if this angle is slightly deviated (for example, several degrees), the armature 4 is in two stopped states. The electromagnetic force at the time of starting becomes unbalanced, but it does not matter as long as it does not have a great influence on the starting of the armature 4. For example, when the magnetic body 10 stops at the boundary between the N pole and the S pole of the magnet 3, the point A of the coil 6 is set to 15 degrees from the center of the N pole (or S pole) of the magnet. When the magnetic body 10 stops at the center of the N pole (or S pole) of the magnet 3, the point A of the coil 6 is separated by 30 degrees from the center of the N pole (or S pole) of the magnet. Even in this case, the start-up of the armature 4 is not greatly affected.

よって、本実施の形態の偏平モータ1は、何れの場合でも、コイル6のA点及びB点が磁石3のS極とN極との境界部に位置しないので、電機子4の起動に十分な電磁力を得ることができ、電機子4の回転をスムーズに起動することができる。   Therefore, in any case, the flat motor 1 of the present embodiment is sufficient for starting the armature 4 because the points A and B of the coil 6 are not located at the boundary between the S pole and the N pole of the magnet 3. Electromagnetic force can be obtained, and the rotation of the armature 4 can be started smoothly.

同様に、磁石3の一つの着磁領域の中心角の5/4、7/4に相当する位置でも、磁石3のS極の中央又はN極の中央から約22.5度離れた点にコイル6の回転力を生じる巻線部分(A点及びB点)が停止することから、電機子4の起動に十分な電磁力を得ることができる。   Similarly, at a position corresponding to 5/4 and 7/4 of the central angle of one magnetized region of the magnet 3, at a point about 22.5 degrees away from the center of the S pole or the center of the N pole of the magnet 3. Since the winding portions (points A and B) that generate the rotational force of the coil 6 are stopped, an electromagnetic force sufficient for starting the armature 4 can be obtained.

つまり、本実施の形態の偏平モータ1では、磁石3のS極(又は、N極)の中央とS極とN極との境界部の中間点にコイル6が必ず位置するように、電機子4を停止させる(A点及びB点が磁石3の各着磁領域の境界部に停止させない)。このことが、本発明の本質である。   In other words, in the flat motor 1 of the present embodiment, the armature is such that the coil 6 is necessarily located at the midpoint between the center of the S pole (or N pole) of the magnet 3 and the boundary between the S pole and the N pole. 4 is stopped (the points A and B are not stopped at the boundaries between the magnetized regions of the magnet 3). This is the essence of the present invention.

同様に、図5に示す実施の形態の電機子4、及び図6に示す実施の形態の電機子4は、磁性体10が磁石3のN極とS極との境界に停止した場合でも、磁性体10が磁石3のN極(又は、S極)の中央に停止した場合でも、磁石3のS極の中央又はN極の中央から約22.5度離れた点にコイル6の回転力を生じる巻線部分(A点及びB点)が停止する。よって、図5に示す実施の形態の偏平モータ1も、コイル6のA点及びB点が磁石3のS極とN極との境界部に停止しないので、電機子4の起動に十分な電磁力を得ることができ、電機子4の回転をスムーズに起動することができる。   Similarly, the armature 4 according to the embodiment shown in FIG. 5 and the armature 4 according to the embodiment shown in FIG. 6 are arranged even when the magnetic body 10 stops at the boundary between the N pole and the S pole of the magnet 3. Even when the magnetic body 10 stops at the center of the N pole (or S pole) of the magnet 3, the rotational force of the coil 6 is about 22.5 degrees away from the center of the S pole or the center of the N pole of the magnet 3. The winding part (point A and point B) that generates the point stops. Therefore, the flat motor 1 according to the embodiment shown in FIG. 5 also does not stop at the boundary between the S pole and the N pole of the magnet 3 at the points A and B of the coil 6. A force can be obtained, and the rotation of the armature 4 can be started smoothly.

以上、4極に分割して着磁されている磁石を用いた偏平モータについて説明したが、6極に着磁されている磁石を用いた偏平モータにも本発明を適用することができる。すなわち、6極に着磁されている磁石では、一つの着磁領域の中心角が60度である。このとき、何れの停止位置でも、電機子4の起動に十分な電磁力を得るためには、磁石3のS極(又は、N極)の中央とS極とN極との境界部の中間にコイル6のA点及びB点を停止させるためには、磁性体10の中央を、コイル6の一端(A点)から、磁石の一つの着磁領域の中心角(60度)の1/4に相当する略15度の位置、3/4に相当する略45度の位置、さらには、(2n+1)/4に相当する角度の位置に配置すればよい。なお、nは整数である。   The flat motor using the magnet divided and magnetized into four poles has been described above, but the present invention can also be applied to a flat motor using a magnet magnetized into six poles. That is, in the magnet magnetized with 6 poles, the central angle of one magnetized region is 60 degrees. At this time, in order to obtain an electromagnetic force sufficient for starting the armature 4 at any stop position, the center of the S pole (or N pole) of the magnet 3 and the middle of the boundary between the S pole and N pole. In order to stop the points A and B of the coil 6, the center of the magnetic body 10 is moved from one end (point A) of the coil 6 to 1 / of the central angle (60 degrees) of one magnetized region of the magnet. It may be arranged at a position of approximately 15 degrees corresponding to 4, a position of approximately 45 degrees corresponding to 3/4, and a position of an angle corresponding to (2n + 1) / 4. Note that n is an integer.

同様に、8極に着磁されている磁石を用いた偏平モータに本発明を適用すると、磁性体10の中央を、コイル6の一端(A点)から、磁石の一つの着磁領域の中心角(45度)の1/4に相当する略11.25度の位置、3/4に相当する略33.75度の位置、さらには、(2n+1)/4に相当する角度の位置に配置すればよい。なお、nは整数である。   Similarly, when the present invention is applied to a flat motor using a magnet magnetized in eight poles, the center of the magnetic body 10 is centered from one end (point A) of the coil 6 in one magnetized region of the magnet. Arranged at a position of approximately 11.25 degrees corresponding to 1/4 of the angle (45 degrees), a position of approximately 33.75 degrees corresponding to 3/4, and a position of an angle corresponding to (2n + 1) / 4 do it. Note that n is an integer.

以上説明したように、本発明は、4極に着磁された磁石を用いた偏平モータの他、他の極数(例えば、6極、8極等)に着磁された磁石を用いた偏平モータにも適用することができる。   As described above, the present invention is not limited to a flat motor using magnets magnetized to four poles, but also to flat motors using magnets magnetized to other pole numbers (for example, six poles, eight poles, etc.). It can also be applied to motors.

本発明の実施の形態の偏平モータの一例を示す縦断面図である。It is a longitudinal section showing an example of a flat motor of an embodiment of the invention. 本発明の実施の形態の電機子の構成を示す裏面図である。It is a reverse view which shows the structure of the armature of embodiment of this invention. 本発明の実施の形態の電機子の回転原理を示す起動時の説明図である。It is explanatory drawing at the time of the start which shows the rotation principle of the armature of embodiment of this invention. 本発明の実施の形態の電機子の回転原理を示す起動時の説明図である。It is explanatory drawing at the time of the start which shows the rotation principle of the armature of embodiment of this invention. 本発明の実施の形態の電機子の別な構成を示す裏面図である。It is a reverse view which shows another structure of the armature of embodiment of this invention. 本発明の実施の形態の電機子の別な構成を示す裏面図である。It is a reverse view which shows another structure of the armature of embodiment of this invention. 従来の電機子の起動時の問題点を示す説明図である。It is explanatory drawing which shows the problem at the time of the starting of the conventional armature. 従来の電機子の起動時の問題点を示す説明図である。It is explanatory drawing which shows the problem at the time of the starting of the conventional armature.

符号の説明Explanation of symbols

1 偏平モータ
2A 上部ケーシング
2B 下部ケーシング
3 磁石
4 電機子
5 シャフト
6 コアレスコイル
7 樹脂フレーム
8 整流子
9 ブラシ
10、11 磁性体
12、13 軸受
DESCRIPTION OF SYMBOLS 1 Flat motor 2A Upper casing 2B Lower casing 3 Magnet 4 Armature 5 Shaft 6 Coreless coil 7 Resin frame 8 Commutator 9 Brush 10, 11 Magnetic body 12, 13 Bearing

Claims (6)

略均等な角度で複数極に着磁された平板状の磁石と、前記磁石に対向して回転可能に軸支され、コイルを有する電機子と、を備えるモータであって、
前記電機子に磁性体を設け、
前記磁性体が前記磁石の各着磁領域の境界及び前記磁石の各着磁領域の中央の何れに位置した場合でも、前記コイルが起動可能となる位置に前記磁性体を配置したことを特徴とするモータ。
A motor comprising: a plate-like magnet magnetized in a plurality of poles at substantially equal angles; and an armature that is rotatably supported opposite to the magnet and has a coil,
A magnetic body is provided in the armature,
The magnetic body is arranged at a position where the coil can be activated regardless of whether the magnetic body is located at the boundary between the magnetized regions of the magnet or at the center of the magnetized region of the magnet. Motor.
前記コイルの端部は、前記磁性体が前記磁石の各着磁領域の境界及び前記磁石の各着磁領域の中央の何れに位置した場合でも、前記各着磁領域の境界から所定距離だけ離れた位置に配置されることを特徴とする請求項1に記載のモータ。   The end of the coil is separated from the boundary of each magnetized region by a predetermined distance regardless of whether the magnetic body is located at the boundary between the magnetized regions of the magnet or the center of each magnetized region of the magnet. The motor according to claim 1, wherein the motor is disposed at a different position. 前記コイルの中心角は前記各着磁領域の中心角と略等しく、
前記磁性体は、前記各着磁領域の中心角をθとした場合、前記コイルの一端から、中心角が(2n+1)×0.25×θ(nは整数)を満たす位置に配置されることを特徴とする請求項1又は2に記載のモータ。
The central angle of the coil is substantially equal to the central angle of each magnetized region,
The magnetic body is disposed at a position where the central angle satisfies (2n + 1) × 0.25 × θ (n is an integer) from one end of the coil, where θ is the central angle of each magnetized region. The motor according to claim 1 or 2.
前記コイルの中心角は前記各着磁領域の中心角と略等しく、
前記磁性体は、前記コイルの一端から、前記各着磁領域の中心角の0.25倍及び0.75倍の少なくとも一方の位置に配置されることを特徴とする請求項1から3のいずれか一つに記載のモータ。
The central angle of the coil is substantially equal to the central angle of each magnetized region,
The said magnetic body is arrange | positioned in the at least one position of 0.25 times and 0.75 times the central angle of each said magnetization area | region from the end of the said coil. The motor as described in one.
前記磁石は4極に着磁されており、
前記磁性体は、前記コイルの一端から、中心角が22.5度及び67.5度の少なくとも一方の位置に配置されることを特徴とする請求項1から4のいずれか一つに記載のモータ。
The magnet is magnetized to 4 poles,
5. The magnetic body according to claim 1, wherein the magnetic body is disposed at at least one of a central angle of 22.5 degrees and 67.5 degrees from one end of the coil. motor.
略均等な角度で複数極に着磁された平面を含む磁石を有するモータ内で、前記磁石に対向して回転可能に軸支される電機子であって、
コイル及び磁性体を備え、
前記磁性体が前記磁石の各着磁領域の境界及び前記磁石の各着磁領域の中央の何れに位置した場合でも、前記コイルが起動可能となる位置に前記磁性体を配置したことを特徴とするモータ用電機子。
In a motor having a magnet including a plane magnetized with a plurality of poles at substantially equal angles, the armature is pivotally supported so as to face the magnet,
A coil and a magnetic body;
The magnetic body is arranged at a position where the coil can be activated regardless of whether the magnetic body is located at the boundary between the magnetized regions of the magnet or at the center of the magnetized region of the magnet. Armature for motor.
JP2006334441A 2006-12-12 2006-12-12 Motor and motor armature Pending JP2008148491A (en)

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Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006014502A (en) * 2004-06-25 2006-01-12 Nidec Copal Corp Vibrating motor
JP2006101601A (en) * 2004-09-28 2006-04-13 Nidec Copal Corp Vibration motor
JP2006101667A (en) * 2004-09-30 2006-04-13 Nidec Copal Corp Vibration motor

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH10174361A (en) 1996-12-17 1998-06-26 Symtec:Kk Flat coreless oscillatory motor
JP3039857B2 (en) * 1997-05-27 2000-05-08 株式会社ティーケーエス Armature structure of flat motor
JPH11191950A (en) 1997-12-25 1999-07-13 Tks:Kk Armature construction of flat motor
KR100512301B1 (en) * 2002-12-30 2005-09-02 삼성전기주식회사 Brushless vibration motor

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006014502A (en) * 2004-06-25 2006-01-12 Nidec Copal Corp Vibrating motor
JP2006101601A (en) * 2004-09-28 2006-04-13 Nidec Copal Corp Vibration motor
JP2006101667A (en) * 2004-09-30 2006-04-13 Nidec Copal Corp Vibration motor

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