JPH0379940B2 - - Google Patents
Info
- Publication number
- JPH0379940B2 JPH0379940B2 JP20922384A JP20922384A JPH0379940B2 JP H0379940 B2 JPH0379940 B2 JP H0379940B2 JP 20922384 A JP20922384 A JP 20922384A JP 20922384 A JP20922384 A JP 20922384A JP H0379940 B2 JPH0379940 B2 JP H0379940B2
- Authority
- JP
- Japan
- Prior art keywords
- rotor
- magnetic
- magnetic flux
- stator
- winding
- 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
Links
- 230000004907 flux Effects 0.000 claims description 35
- 238000004804 winding Methods 0.000 description 39
- 239000003990 capacitor Substances 0.000 description 5
- 239000002131 composite material Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 1
- 230000001771 impaired effect Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K19/00—Synchronous motors or generators
- H02K19/02—Synchronous motors
- H02K19/10—Synchronous motors for multi-phase current
- H02K19/12—Synchronous motors for multi-phase current characterised by the arrangement of exciting windings, e.g. for self-excitation, compounding or pole-changing
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K1/00—Details of the magnetic circuit
- H02K1/06—Details of the magnetic circuit characterised by the shape, form or construction
- H02K1/22—Rotating parts of the magnetic circuit
- H02K1/24—Rotor cores with salient poles ; Variable reluctance rotors
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K19/00—Synchronous motors or generators
- H02K19/16—Synchronous generators
- H02K19/26—Synchronous generators characterised by the arrangement of exciting windings
- H02K19/30—Synchronous generators characterised by the arrangement of exciting windings for compounding
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Iron Core Of Rotating Electric Machines (AREA)
- Synchronous Machinery (AREA)
Description
【発明の詳細な説明】
(A) 産業上の利用分野
本発明は、回転電機、特に例えば発電機の如き
回転電機において、電機子反作用を積極的に利用
する回転子の構造を採用してブラシレス構造とし
た回転電機に関するものである。DETAILED DESCRIPTION OF THE INVENTION (A) Industrial Field of Application The present invention is a rotating electrical machine, particularly a rotating electrical machine such as a generator, in which a rotor structure that actively utilizes armature reaction is adopted to provide a brushless motor. This relates to a rotating electric machine with a structure.
(B) 従来の技術と発明が解決しようとする問題点
従来から発電機の如き回転電機においては、電
機子反作用により生じる磁束を積極的に利用しよ
うとする例は少なく、上記電機子反作用の発生に
よつて出力波形に非所望な歪みが生じたり局部的
な磁路飽和が生じるなどのために、当該電機子反
作用の発生をさけることが望まれていた。ただ上
記電機子反作用による磁束を有効に利用するよう
にしている例の1つとして、第5図および第6図
に示す如きいわゆる野中式の発電機が知られてい
る。(B) Prior art and problems to be solved by the invention Conventionally, in rotating electric machines such as generators, there have been few examples of actively utilizing the magnetic flux generated by armature reaction, and the occurrence of the armature reaction has been limited. Since this causes undesirable distortion in the output waveform and local saturation of the magnetic path, it has been desired to avoid the armature reaction. However, a so-called Nonaka-type generator as shown in FIGS. 5 and 6 is known as one example in which the magnetic flux generated by the armature reaction is effectively utilized.
図において、1は固定子上に巻回されている電
機子巻線、2は固定子上に上記電機子巻線1に対
して電機角90°の位置に巻回されているエキサイ
タ巻線、3はエキサイタ巻線2に接続された進相
電流供給用コンデンサ、4は回転子上に巻回され
ている界磁巻線、5は界磁巻線4に接続されてい
るダイオードを表している。また6は固定子、7
は回転子を表している。 In the figure, 1 is an armature winding wound on the stator, 2 is an exciter winding wound on the stator at a position at an electrical angle of 90° with respect to the armature winding 1, 3 represents a capacitor for supplying advanced phase current connected to the exciter winding 2, 4 represents a field winding wound on the rotor, and 5 represents a diode connected to the field winding 4. . Also, 6 is a stator, 7
represents the rotor.
第5図に示す野中式発電機の場合、例えば最初
何んらかの理由によつて、界磁巻線4に電流が流
れるとダイオード5によつて整流され、回転子7
に磁極が生じる。このために、電機子巻線1とエ
キサイタ巻線2とに交番電圧が誘起される。この
とき、エキサイタ巻線2に誘起された電圧によつ
てコンデンサ3を介して進相電流が流れ、当該進
相電流のつくる磁束(第6図Φ2)によつて界磁
巻線4に電圧が誘起され、ダイオード5によつて
整流された電流が界磁巻線4内を流れ、上記電機
子巻線1やエキサイタ巻線2に誘起される電圧を
増大せしめるように動作する。 In the case of the Nonaka type generator shown in FIG. 5, for example, when current initially flows through the field winding 4 for some reason, it is rectified by the diode 5,
A magnetic pole is generated. For this reason, an alternating voltage is induced in the armature winding 1 and the exciter winding 2. At this time, a phase-advanced current flows through the capacitor 3 due to the voltage induced in the exciter winding 2, and a voltage is applied to the field winding 4 due to the magnetic flux (Φ 2 in Fig. 6) created by the phase-advanced current. is induced, a current rectified by the diode 5 flows through the field winding 4, and operates to increase the voltage induced in the armature winding 1 and the exciter winding 2.
第6図はこの場合の磁束発生の状態を示す説明
図であり、固定子6上に電機子巻線1とエキサイ
タ巻線2とが図示の如く巻回されており、回転子
7上には図示しない界磁巻線4が巻回されてい
る。 FIG. 6 is an explanatory diagram showing the state of magnetic flux generation in this case, in which the armature winding 1 and the exciter winding 2 are wound on the stator 6 as shown, and the rotor 7 is wound with the armature winding 1 and the exciter winding 2 as shown in the figure. A field winding 4 (not shown) is wound thereon.
回転子7が例えば図示矢印の如く反時計方向に
回転駆動せしめられているとし、図示Nの如く磁
極が存在しているとする。この場合、電機子巻線
1とエキサイタ巻線2とに電圧が誘起され、、電
機子巻線1に流れる負荷電流によつて図示磁束
Φ1,Φ1′が発生される。またエキサイタ巻線2に
流れる上記進相電流によつて図示磁束Φ2,Φ2′が
発生される。 Assume that the rotor 7 is driven to rotate counterclockwise, for example, as indicated by the arrow in the figure, and that there are magnetic poles as indicated by N in the figure. In this case, a voltage is induced in the armature winding 1 and the exciter winding 2, and the indicated magnetic fluxes Φ 1 and Φ 1 ' are generated by the load current flowing in the armature winding 1. In addition, the illustrated magnetic fluxes Φ 2 and Φ 2 ' are generated by the phase advancing current flowing through the exciter winding 2.
図示磁束Φ3は上記磁束Φ1とΦ2との合成磁束を
表し、磁束Φ3′は磁束Φ1′とΦ2′との合成磁束を表
している。 The illustrated magnetic flux Φ 3 represents the composite magnetic flux of the above-mentioned magnetic fluxes Φ 1 and Φ 2 , and the magnetic flux Φ 3 ′ represents the composite magnetic flux of the magnetic fluxes Φ 1 ′ and Φ 2 ′.
野中式発電機の場合、エキサイタ巻線2によつ
てつくられる磁束Φ2,Φ2′が図示磁束Nを増大す
るように働くが、上記磁束Φ3,Φ3′の如く電機子
巻線1によつてつくられる磁束が上記磁極Nを増
大するように回転子7と交差する。即ち、野中式
発電機の場合には、上述の如く電機子反作用によ
つてつくられる磁束が積極的に利用されており、
例えば電圧調整器なしに出力電圧を一定にする特
性をもつている。 In the case of the Nonaka type generator, the magnetic fluxes Φ 2 and Φ 2 ' created by the exciter winding 2 act to increase the indicated magnetic flux N, but the magnetic fluxes Φ 3 and Φ 3 ' generated by the armature winding 1 The magnetic flux created by the magnetic flux intersects the rotor 7 in such a way that the magnetic pole N increases. In other words, in the case of the Nonaka type generator, the magnetic flux created by the armature reaction is actively utilized as described above.
For example, it has the characteristic of keeping the output voltage constant without the need for a voltage regulator.
(C) 問題点を解決するための手段
本発明は、上記の如き電機子反作用によつてつ
くられる磁束を積極的に利用する態様を一段と進
展せしめた回転電機を提供している。そしてその
ため、本発明の回転電機は、固定子に巻回された
電機子コイルをそなえると共に、上記固定子に対
向して微小磁気間隙を介して回転可能に支持され
る回転子と該回転子上に磁極を発生せしめる界磁
コイルとを有する回転電機において、上記回転子
の回転中心軸から上記磁極に向かう放射状線分に
対して非対称に上記回転子の形状を構成してな
り、上記放射状線分から回転子の回転方向先頭側
半分の上記固定子に対する磁気抵抗が上記回転方
向末尾側半分の上記固定子に対する磁気抵抗にく
らべて大となるよう構成され、上記電機子コイル
に流れる電流によつて発生された磁束が上記界磁
コイルによつて発生される磁束を増大せしめるよ
うにされ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。(C) Means for Solving the Problems The present invention provides a rotating electrical machine that further advances the mode of actively utilizing the magnetic flux created by the armature reaction as described above. Therefore, the rotating electrical machine of the present invention includes an armature coil wound around a stator, a rotor that is rotatably supported opposite the stator through a minute magnetic gap, and a rotor that is rotatably supported on the rotor. In a rotating electric machine having a field coil that generates magnetic poles, the shape of the rotor is configured asymmetrically with respect to a radial line segment extending from the central axis of rotation of the rotor toward the magnetic poles, and The magnetic resistance of the leading half of the rotor in the rotational direction toward the stator is configured to be larger than the magnetic resistance of the trailing half of the rotor toward the stator, and is generated by the current flowing through the armature coil. The magnetic flux generated by the field coil increases the magnetic flux generated by the field coil. This will be explained below with reference to the drawings.
(D) 実施例
第1図および第2図は本発明の回転電機の一実
施例、第3図は円型回転子に適用した一実施
例、第4図A,Bは集中電機子巻線型の発電機に
適用した一実施例を示す。(D) Embodiment Figures 1 and 2 show an embodiment of the rotating electrical machine of the present invention, Figure 3 shows an embodiment applied to a circular rotor, and Figures 4A and B show a concentrated armature winding type. An example in which the present invention is applied to a generator will be shown.
第1図および第2図において、符号1,4,
5,6,7は夫々第5図および第6図に対応し、
8は電機子巻線1に接続された進相電流供給用コ
ンデンサ、9は負荷、Φ4,Φ5は夫々磁束を表し
ている。また10,10′は夫々本発明において
もうけられるスリツトを表している。 In FIG. 1 and FIG. 2, symbols 1, 4,
5, 6, and 7 correspond to FIGS. 5 and 6, respectively,
Reference numeral 8 represents a phase-advanced current supply capacitor connected to the armature winding 1, 9 represents a load, and Φ 4 and Φ 5 represent magnetic fluxes, respectively. Further, 10 and 10' respectively represent slits formed in the present invention.
第2図図示において界磁巻線4が省略されて示
されているが、第2図に明瞭に示される如く、回
転子7が回転中心軸から磁極(図示Nの所)に向
かう放射状線分を仮想的に考えるとき、当該放射
状線分の左右で非対称な構造をもつようにされ
る。即ち、回転子7が図示矢印の如く反時計方向
に回転する場合に、第2図図示実施例の場合には
回転方向先頭側(図示左側)にスリツト10がも
うけられる。即ち第2図図示の場合、電機子巻線
1を流れる電流によつてつくられる磁束が図示磁
束Φ4の如く回転子7と交差し、図示磁束Φ5は上
記スリツト10によつて阻止されるように、上記
スリツト10,10′が形成される。 Although the field winding 4 is omitted in the illustration in FIG. 2, as clearly shown in FIG. When considered hypothetically, it has an asymmetric structure on the left and right sides of the radial segment. That is, when the rotor 7 rotates counterclockwise as indicated by the arrow in the figure, in the case of the embodiment shown in FIG. 2, the slit 10 is provided on the leading side in the rotation direction (left side in the figure). That is, in the case shown in FIG. 2, the magnetic flux created by the current flowing through the armature winding 1 crosses the rotor 7 as indicated magnetic flux Φ4 , and the indicated magnetic flux Φ5 is blocked by the slit 10. The slits 10, 10' are thus formed.
このために、電機子巻線1を流れる電流によつ
てつくられる磁束が回転子7の磁極Nを強める方
向に働くこととなる。即ち電機子反作用によつて
生じる磁束が積極的に利用された形となる。 For this reason, the magnetic flux created by the current flowing through the armature winding 1 acts in a direction that strengthens the magnetic pole N of the rotor 7. In other words, the magnetic flux generated by the armature reaction is actively utilized.
第1図とあわせ考えるとき、次の如く動作する
と考えてよい。即ち、例えば最初に何んらかの理
由により回転子7上に磁極Nが発生したとする
と、これによつて電機子巻線1に電圧が誘起され
る。該誘起された電圧によつて、負荷9に電流が
供給されるが、あわせてコンデンサ8に進相電流
が流入する。電機子巻線1に流れる電流は全体と
して進相電流が流れるように構成されており、当
該進相電流によつて第2図図示磁束Φ4がつくら
れる。該磁束Φ4によつて界磁巻線4に電圧が誘
起され、ダイオード5によつて整流され、磁極N
を強めるように働く。 When considered in conjunction with FIG. 1, it may be considered that the operation is as follows. That is, for example, if a magnetic pole N is first generated on the rotor 7 for some reason, a voltage is induced in the armature winding 1 due to this. A current is supplied to the load 9 by the induced voltage, and a phase-advanced current also flows into the capacitor 8. The current flowing through the armature winding 1 is configured so that a phase-advanced current flows as a whole, and the magnetic flux Φ 4 shown in the second diagram is created by the phase-advanced current. A voltage is induced in the field winding 4 by the magnetic flux Φ 4 , which is rectified by the diode 5, and the magnetic pole N
Works to strengthen.
第1図図示構成の場合には、第5図および第6
図図示構成にくらべて、エキサイタ巻線2を別個
にもうけることが必ずしも必要でなくなる。 In the case of the configuration shown in Figure 1, Figures 5 and 6
Compared to the illustrated configuration, it is no longer necessary to provide the exciter winding 2 separately.
第3図図示の場合には、円型回転子を用いた
例を示しているが、界磁巻線4が回転子上のスロ
ツト内に埋め込まれているだけであり、第2図図
示の場合と同様にスリツト10,10′が第2図
図示の磁束Φ5を阻止することは同じである。 The case shown in Fig. 3 shows an example using a circular rotor, but the field winding 4 is only embedded in the slot on the rotor, and the case shown in Fig. 2 shows an example using a circular rotor. Similarly, the slits 10, 10' block the magnetic flux Φ 5 shown in FIG.
第4図A,Bは集中電機子巻線型の発電機の場
合を示している。図中の符号1,6,7,10,
10′,Φ4,Φ5は夫々第2図に対応している。第
4図Bは第4図Aの回転子7が180°回転した位置
にある場合を示している。図示実施例の場合に
も、磁束Φ5が阻止されて磁束Φ4が磁極N(又は
S)を強めるように働くことに変わりはない。 Figures 4A and 4B show the case of a concentrated armature winding type generator. Codes 1, 6, 7, 10 in the figure,
10', Φ 4 and Φ 5 correspond to FIG. 2, respectively. FIG. 4B shows the rotor 7 of FIG. 4A in a position rotated by 180°. Even in the illustrated embodiment, the magnetic flux Φ 5 is blocked and the magnetic flux Φ 4 acts to strengthen the magnetic pole N (or S).
なお上記説明においては、スリツト10,1
0′をもうけることによつて、磁気抵抗を非対称
としており、回転子の機械的強度がそこなわれる
ことがない。しかし、上記磁気抵抗を非対称にす
る手段としては上記に限られるものではなく、例
えば第2図図示の回転子7における磁極において
回転方向先頭側の磁極チツプ端を削り取つた形状
などの構成を採用することもできる。 In the above description, the slits 10, 1
By providing 0', the magnetic resistance is made asymmetrical, and the mechanical strength of the rotor is not impaired. However, the means for making the magnetic resistance asymmetric is not limited to the above, and for example, a configuration such as a shape in which the leading end of the magnetic pole tip in the rotation direction of the magnetic pole of the rotor 7 shown in FIG. 2 is shaved off is adopted. You can also.
(E) 発明の効果
以上説明した如く、本発明によれば、電機子電
流によつてつくられる磁束を有効に利用するよう
にしたブラシレス構造の回転電機を提供すること
が可能となる。(E) Effects of the Invention As explained above, according to the present invention, it is possible to provide a rotating electrical machine with a brushless structure that effectively utilizes the magnetic flux created by the armature current.
第1図および第2図は本発明の回転電機の一実
施例、第3図は円型回転子に適用した一実施
例、第4図A,Bは集中電機子巻線型の発電機に
適用した一実施例を示す。また第5図および第6
図は従来の発電機を示す。
図中、1は電機子巻線、4は界磁巻線、5はダ
イオード、6は固定子、7は回転子、8はコンデ
ンサ、9は負荷、10,10′は夫々スリツトを
表す。
Figures 1 and 2 show an embodiment of the rotating electric machine of the present invention, Figure 3 shows an embodiment applied to a circular rotor, and Figures 4A and B show an example applied to a concentrated armature winding type generator. An example is shown below. Also, Figures 5 and 6
The figure shows a conventional generator. In the figure, 1 is an armature winding, 4 is a field winding, 5 is a diode, 6 is a stator, 7 is a rotor, 8 is a capacitor, 9 is a load, and 10 and 10' are slits, respectively.
Claims (1)
と共に、上記固定子に対向して微小磁気間隙を介
して回転可能に支持される回転子と該回転子上に
磁極を発生せしめる界磁コイルとを有する回転電
機において、上記回転子の回転中心軸から上記磁
極に向かう放射状線分に対して非対称に上記回転
子の形状を構成してなり、上記放射状線分から回
転子の回転方向先頭側半分の上記固定子に対する
磁気抵抗が上記回転方向末尾側半分の上記固定子
に対する磁気抵抗にくらべて大となるよう構成さ
れ、上記電機子コイルに流れる電流によつて発生
された磁束が上記界磁コイルによつて発生される
磁束を増大せしめるようにされることを特徴とす
る回転電機。1. A rotor is provided with an armature coil wound around a stator, and is rotatably supported opposite the stator through a minute magnetic gap; and a field coil that generates magnetic poles on the rotor. In the rotating electric machine, the shape of the rotor is configured asymmetrically with respect to a radial line segment extending from the central axis of rotation of the rotor toward the magnetic poles, and the radial line extends from the leading half of the rotor in the rotational direction. The magnetic resistance to the stator is larger than the magnetic resistance to the stator in the rear half of the rotation direction, and the magnetic flux generated by the current flowing through the armature coil is directed to the field coil. A rotating electrical machine characterized by increasing the magnetic flux generated.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20922384A JPS6188736A (en) | 1984-10-05 | 1984-10-05 | rotating electric machine |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20922384A JPS6188736A (en) | 1984-10-05 | 1984-10-05 | rotating electric machine |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6188736A JPS6188736A (en) | 1986-05-07 |
| JPH0379940B2 true JPH0379940B2 (en) | 1991-12-20 |
Family
ID=16569385
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP20922384A Granted JPS6188736A (en) | 1984-10-05 | 1984-10-05 | rotating electric machine |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6188736A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE102004002326A1 (en) * | 2004-01-16 | 2005-08-04 | Forschungszentrum Jülich GmbH | rotor |
-
1984
- 1984-10-05 JP JP20922384A patent/JPS6188736A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6188736A (en) | 1986-05-07 |
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