JPS61121753A - Flat motor - Google Patents
Flat motorInfo
- Publication number
- JPS61121753A JPS61121753A JP23971684A JP23971684A JPS61121753A JP S61121753 A JPS61121753 A JP S61121753A JP 23971684 A JP23971684 A JP 23971684A JP 23971684 A JP23971684 A JP 23971684A JP S61121753 A JPS61121753 A JP S61121753A
- Authority
- JP
- Japan
- Prior art keywords
- rotor magnet
- poles
- pattern
- flat
- magnet
- 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
Links
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K21/00—Synchronous motors having permanent magnets; Synchronous generators having permanent magnets
- H02K21/12—Synchronous motors having permanent magnets; Synchronous generators having permanent magnets with stationary armatures and rotating magnets
- H02K21/24—Synchronous motors having permanent magnets; Synchronous generators having permanent magnets with stationary armatures and rotating magnets with magnets axially facing the armatures, e.g. hub-type cycle dynamos
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K29/00—Motors or generators having non-mechanical commutating devices, e.g. discharge tubes or semiconductor devices
- H02K29/14—Motors or generators having non-mechanical commutating devices, e.g. discharge tubes or semiconductor devices with speed sensing devices
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Brushless Motors (AREA)
- Permanent Magnet Type Synchronous Machine (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、平面対向形のロータ磁石とステータコイルを
持ちかつ回転パルス発生器を内蔵した偏平形電動機に関
するものである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a flat type electric motor having a rotor magnet and a stator coil that are opposed to each other in a plane, and having a built-in rotary pulse generator.
従来例の構成とその問題点
従来の篩平形電動機の構成の一例を第2図に示す。同図
に於いて1はシャフト、2は偏平形ロータ磁石、3はロ
ータヨーク、4はロータヨーク3をシャフトに固定する
ためのロータボス、6はベアリングである。又6はステ
ータヨーク、7はステータヨーク上に配置かつ固着され
た多極偏平形の無鉄芯ステータコイルであシ、さらに8
は、ステータコイルγ上に固着された回転パルス発生用
プリント基板である。ここでプリント基板8はステータ
コイル7の端末処理用パターンも形成している。Structure of a conventional example and its problems An example of the structure of a conventional sieve type electric motor is shown in FIG. In the figure, 1 is a shaft, 2 is a flat rotor magnet, 3 is a rotor yoke, 4 is a rotor boss for fixing the rotor yoke 3 to the shaft, and 6 is a bearing. Further, 6 is a stator yoke, 7 is a multipolar flat iron coreless stator coil arranged and fixed on the stator yoke, and 8 is a stator coil.
is a rotational pulse generating printed circuit board fixed on the stator coil γ. Here, the printed circuit board 8 also forms a pattern for terminal processing of the stator coil 7.
第3図はロータ磁石2の着磁状態を示している。FIG. 3 shows the magnetized state of the rotor magnet 2. As shown in FIG.
同図の内径側着磁部2−1は主磁束用着磁部であシ、8
極着磁の場合を示している。又外径側着磁部2−2は回
転パルス発生用着磁部で66、s4極着磁の場合を示し
ており、各々等間隔に着磁されている。The inner diameter side magnetized part 2-1 in the figure is the main magnetic flux magnetized part, 8
The case of polar magnetization is shown. Further, the outer diameter side magnetized portion 2-2 is a magnetized portion for generating rotational pulses, and a case of 66 and s4 pole magnetization is shown, and each is magnetized at equal intervals.
第4図は、回転パルス発生用プリント基板8の回転パル
ス発生用パターンを示している。第4図のパターンの極
数は第3図に示したロータ磁石2の回転パルス発生用着
磁部2−2の極数と一致しており、ロータ磁石2が回転
した場合の第4図a−す間の鎖交磁束φ及び誘起電圧e
は第5図の様になり、2/極数回転毎に回転パルスを得
る事ができる。FIG. 4 shows a pattern for generating rotational pulses on the printed circuit board 8 for generating rotational pulses. The number of poles in the pattern of FIG. 4 matches the number of poles of the rotational pulse generation magnetized part 2-2 of the rotor magnet 2 shown in FIG. 3, and the number of poles in the pattern shown in FIG. - Interlinkage magnetic flux φ and induced voltage e
is as shown in Fig. 5, and a rotation pulse can be obtained every 2/number of pole rotations.
しかしながら上記従来例では、ロータ磁石2上に、回転
パルス発生用着磁部2−2が必要となシ、言いかえれば
、それだけ主磁束用着磁部2−1の面積が減少し、従っ
てモータ出力が減少するという欠点を有していた。However, in the above conventional example, the magnetized part 2-2 for generating rotational pulses is not required on the rotor magnet 2. In other words, the area of the magnetized part 2-1 for main magnetic flux is reduced accordingly, and therefore the motor It had the disadvantage of reduced output.
発明の目的
そこで本発明は、上記従来例の欠点に鑑みなされたもの
であシ、ロータ磁石上の回転パルス用着磁部を不要とし
つつ、従来例と同様な回転パルス信号を得る事ができる
偏平形電動機を可能とし、小形で高出力の電動機を供給
しようとするものである。Purpose of the Invention The present invention was developed in view of the drawbacks of the conventional example described above, and it is possible to obtain a rotation pulse signal similar to that of the conventional example while eliminating the need for a magnetized part for rotation pulses on the rotor magnet. The aim is to make a flat motor possible and to supply a small, high-output motor.
発明の構成
本発明は、円周方向に同一角度で多極着磁された平面対
向形の偏平ロータ磁石と前記ロータ磁石と対向する様に
配置された多極ステータコイルと、前記ロータ磁石と対
向する様に配置されかつ放射状のジグザグパターンを有
した回転パルス発生用フリント基板より構成されている
。Structure of the Invention The present invention provides a planar flat rotor magnet magnetized with multiple poles at the same angle in the circumferential direction, a multipolar stator coil arranged to face the rotor magnet, and a multipolar stator coil facing the rotor magnet. It is composed of a rotating pulse generating flint substrate which is arranged so as to have a radial zigzag pattern.
実施例の説明
本発明に係る偏平形電動機の全体構成は、第2図に示し
た従来例と同じであるので説明を省略し、従来例と異る
、回転パルス発生用プリント基板とロータ磁石について
説明する。DESCRIPTION OF EMBODIMENTS The overall configuration of the flat electric motor according to the present invention is the same as the conventional example shown in FIG. 2, so the explanation will be omitted. explain.
第1図aはステータ側に固定された本発明にかかる回転
パルス発生用プリント基板11の回転パルス発生用パタ
ーン12を示しており、従来例の第4図とは異り、ロー
タ磁石に対向した全面に、回転パルス発生用パターン1
2が描かれている。FIG. 1a shows the rotational pulse generation pattern 12 of the rotational pulse generation printed circuit board 11 according to the present invention fixed to the stator side, and unlike the conventional example shown in FIG. Pattern 1 for generating rotational pulses on the entire surface
2 is depicted.
第1図すは本発明にかかるロータ磁石13の着磁状態を
示しておシ、従来例の第3図と異なり、ロータ磁石13
の全面に主磁束用着磁を施しており、回転パルス発生用
の着磁部は無い。尚、第1図に於いては、ロータ磁石1
3の極数は8極として説明している。FIG. 1 shows the magnetized state of the rotor magnet 13 according to the present invention, and unlike FIG. 3 of the conventional example, the rotor magnet 13
The entire surface is magnetized for main magnetic flux, and there is no magnetized part for generating rotational pulses. In addition, in FIG. 1, the rotor magnet 1
The number of poles in 3 is explained as 8 poles.
以下第6図でもう少し詳しく説明する。第6図に於いて
、ロータ磁石13と回転パルス発生用パターン12の対
向状態を直線状に引き伸した状態を示している。This will be explained in more detail below in Figure 6. In FIG. 6, a state in which the rotor magnet 13 and the rotating pulse generating pattern 12 face each other is shown stretched out in a straight line.
ここで、回転パルス発生用パターン12のジグザグパタ
ーン1極分の角度θ0を、ロータ磁石13の2極分の角
20mの奇数分の1となる様に定める。言いかえれば、
回転パルス発生用パターンの極数mを、m=(2n+1
)・−・・・・・・・・(1)式但し、P:ロータ磁
石13の極数、n=1.2゜3・・・・・・ となる様
に定める。Here, the angle θ0 of one pole of the zigzag pattern of the rotational pulse generation pattern 12 is determined to be an odd-numbered fraction of the angle 20 m of the two poles of the rotor magnet 13. In other words,
The number of poles m of the rotational pulse generation pattern is m=(2n+1
)・−・・・・・・・・・・(1) Formula, where P: Number of poles of rotor magnet 13, n=1.2°3・・・・・・・Determine so that it becomes.
今、n=2とし、かつロータ磁石13のNとSの極間が
、回転パルス発生用のジグザグパターンに一致する場合
を第6図乙に示す。同図から明らかな様に回転パルス発
生用パターン12かN極と鎖交する磁束数とS極と鎖交
する磁束数との間に回転パルス発生用パターン−極分に
相幽する差が有シ、ロータ磁石の一極当シの全磁束をΦ
m とすると、ロータ磁石の一極対当シの回転パルス発
生用パターンの磁束鎖交数’roは
To==Φ11r / (2n+ 1) ・・・
=・−12)式%式%
しており、同様に、回転パルス発生用バター7のロータ
磁石−極対当シの鎖交磁束数ToはTO=−Φm/ (
2n+1 ) −−−(31式%式%
ロータ磁石の全周にわたる、回転パルス発生用パターン
12の総磁束鎖交数では(21式及び(1式にP/2
を各々乗じれば得られる。FIG. 6B shows a case where n=2 and the distance between the N and S poles of the rotor magnet 13 corresponds to a zigzag pattern for generating rotational pulses. As is clear from the figure, there is a difference between the number of magnetic fluxes interlinking with the north pole and the number of magnetic fluxes interlinking with the south pole of the rotational pulse generation pattern 12, which is similar to the polarity of the rotational pulse generation pattern 12. The total magnetic flux at one pole of the rotor magnet is Φ
m, then the magnetic flux linkage 'ro of the rotational pulse generation pattern between one pole of the rotor magnet is To==Φ11r/(2n+1)...
=・-12) Expression % Formula % Similarly, the number of interlinkage magnetic flux To of the rotor magnet-pole pair of the rotating pulse generating butter 7 is TO=-Φm/ (
2n+1) ---(Formula 31%Formula %For the total magnetic flux linkage of the rotating pulse generation pattern 12 over the entire circumference of the rotor magnet, (21 and (1) have P/2
You can get it by multiplying each.
第7図に、回転パルス発生用パターンの総磁束鎖交数T
のロータ磁石13の回転角に対する変化の様子を示す。Figure 7 shows the total magnetic flux linkage T of the rotational pulse generation pattern.
2 shows how the rotor magnet 13 changes with respect to the rotation angle.
第7図に於いて、回転パルス発生パターン12の−極分
の回転角即ち3eo/m= 360°・乏/(2n+1
)だけロータ磁石13か回転すると、回転パルス発の間
を1サイクル変化する。In FIG. 7, the rotation angle of the negative pole of the rotational pulse generation pattern 12, that is, 3eo/m=360°・min/(2n+1
) when the rotor magnet 13 rotates, the period of rotation pulse generation changes by one cycle.
ここで仮に0mX2を一定と仮定すると、回転パルス発
生用パターン12の総鎖交磁束数は、nの増加と共に小
さくなるが、−回転当りのパルス数は増大してゆく事が
わかる。Here, assuming that 0 mX2 is constant, it can be seen that the total number of interlinked magnetic fluxes of the rotational pulse generating pattern 12 decreases as n increases, but the number of pulses per -rotation increases.
発明の効果
上記述べた様に、本発明によれば、ロータ磁石に、回転
パルス発生用着磁部か不要となり、ロータ磁石の全面を
主磁束用とする事かでき、電動機の小形化、高出力化か
はかれる。Effects of the Invention As described above, according to the present invention, the rotor magnet does not require a magnetized part for generating rotational pulses, and the entire surface of the rotor magnet can be used for the main magnetic flux, resulting in downsizing and increasing the size of the motor. It can be outputted or measured.
さらに、回転パルス発生用パターンを、半径方向に、ロ
ータ磁石の主磁束着磁分と同一の大きさまでとる事かで
きるため、磁束鎖交の変化分が大きく、従って、大きな
回転パルス信号を得る事ができ、その実用的価値は非常
に大きなものがある。Furthermore, since the rotational pulse generation pattern can have the same size in the radial direction as the main magnetic flux magnetization of the rotor magnet, the change in magnetic flux linkage is large, and therefore a large rotational pulse signal can be obtained. , and its practical value is enormous.
第1図乱は各々、本発明にかかる回転パルス発生用プリ
ント基板のパターン図、第1 [J bはロータ磁石の
着磁状態を示す説明図、第2図は従来例の偏平電動機の
断面図、第3図は従来例のロータ磁石の着磁状態を示す
説明図、第4図は従来例の回転パルス発生用プリント基
板のパターン図、・甫5図は従来例の回転パルス信号の
波形図、第6図a、bは本発明にか\る回転パルス発生
用パターンの説明図、第7図は本発明にかかる回転パル
ス信号の説明図である。
13・・・・・偏平形ロータ磁石、12・−・・・回転
パルス発生用パターン、7・・・・ステータコイル。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図
(山2
第 2 図
巴3図
第4図
叫
第6図
第7図The first diagram is a pattern diagram of a printed circuit board for generating rotational pulses according to the present invention, the first diagram is an explanatory diagram showing the magnetized state of the rotor magnet, and the second diagram is a cross-sectional diagram of a conventional flat motor. , Figure 3 is an explanatory diagram showing the magnetized state of the rotor magnet in the conventional example, Figure 4 is a pattern diagram of the printed circuit board for generating rotational pulses in the conventional example, and Figure 5 is a waveform diagram of the rotational pulse signal in the conventional example. , FIGS. 6a and 6b are explanatory diagrams of a rotational pulse generation pattern according to the present invention, and FIG. 7 is an explanatory diagram of a rotational pulse signal according to the present invention. 13... Flat rotor magnet, 12... Pattern for generating rotational pulses, 7... Stator coil. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure (Mountain 2 Figure 2 Tomoe Figure 4 Figure 6 Figure 7
Claims (1)
ロータ磁石と、前記ロータ磁石と対向する様に配置され
た多極ステータコイルと、前記ロータ磁石と対向する様
に配置されかつ放射状のジグザグパターンを有した回転
パルス発生用プリント基板とを備え、前記プリント基板
の放射状ジグザグパターンの極数mを m=(2n+1)・P/2 P=ロータ磁石の極数 n=1、2、3・・・・・・ とした偏平形電動機。[Scope of Claims] A planar facing flat rotor magnet magnetized with multiple poles at the same angle in the circumferential direction, a multipolar stator coil arranged to face the rotor magnet, and a multipolar stator coil facing the rotor magnet. a rotational pulse generating printed circuit board having a radial zigzag pattern arranged so as to A flat electric motor with the number n=1, 2, 3...
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP23971684A JPS61121753A (en) | 1984-11-13 | 1984-11-13 | Flat motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP23971684A JPS61121753A (en) | 1984-11-13 | 1984-11-13 | Flat motor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61121753A true JPS61121753A (en) | 1986-06-09 |
Family
ID=17048859
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP23971684A Pending JPS61121753A (en) | 1984-11-13 | 1984-11-13 | Flat motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61121753A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100444973B1 (en) * | 2002-05-09 | 2004-08-21 | 자화전자 주식회사 | Vibration motor |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5251510A (en) * | 1975-10-23 | 1977-04-25 | Hitachi Ltd | Frequency generator and motor with that generator |
-
1984
- 1984-11-13 JP JP23971684A patent/JPS61121753A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5251510A (en) * | 1975-10-23 | 1977-04-25 | Hitachi Ltd | Frequency generator and motor with that generator |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100444973B1 (en) * | 2002-05-09 | 2004-08-21 | 자화전자 주식회사 | Vibration motor |
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