JPH0817560B2 - Brushless generator - Google Patents
Brushless generatorInfo
- Publication number
- JPH0817560B2 JPH0817560B2 JP62189682A JP18968287A JPH0817560B2 JP H0817560 B2 JPH0817560 B2 JP H0817560B2 JP 62189682 A JP62189682 A JP 62189682A JP 18968287 A JP18968287 A JP 18968287A JP H0817560 B2 JPH0817560 B2 JP H0817560B2
- Authority
- JP
- Japan
- Prior art keywords
- winding
- field
- poles
- magnetic
- rotor
- 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 - Lifetime
Links
- 238000004804 winding Methods 0.000 claims description 113
- 230000005284 excitation Effects 0.000 claims description 31
- 238000010248 power generation Methods 0.000 claims description 17
- 230000004907 flux Effects 0.000 claims description 16
- 239000003990 capacitor Substances 0.000 description 5
- 230000001360 synchronised effect Effects 0.000 description 5
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 3
- 238000000034 method Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 229910000976 Electrical steel Inorganic materials 0.000 description 1
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 229910000831 Steel Inorganic materials 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
Landscapes
- Synchronous Machinery (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は,ブラシレス発電機,特に固定子に巻回され
た主発電巻線の極数と励磁巻線の極数とを選択すると共
に,回転子の構成を選択し、励磁巻線に環流路を形成さ
せるだけで発電可能にした自励式同期発電機にしたブラ
シレス発電機に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention selects the number of poles of a main generator winding and the number of excitation windings wound around a brushless generator, especially a stator, and The present invention relates to a brushless generator that is a self-excited synchronous generator that can generate power simply by selecting a rotor configuration and forming an annular flow path in an excitation winding.
従来,構造が簡単で優れた特性を有するブラシレス単
相発電機として,界磁巻線に誘起される交流電圧をダイ
オードで整流して当該界磁巻線に対する界磁電流とする
方式のいわゆる野中式発電機が知られている。そして上
記野中式発電機の基本原理を応用した第7図図示の如き
ブラシレス2極三相発電機も開発された。なお第7図に
おいて,符号1は固定子,2は回転子,3は2極三相の主発
電巻線,4は単相4極の励磁巻線,5は直流電源,6−1aない
し6−1dは界磁コア,6−2aないし6−2dは突極,7aない
し7dは界磁巻線,8はダイオードを表している。Conventionally, as a brushless single-phase generator with a simple structure and excellent characteristics, a so-called Nonaka method of rectifying an AC voltage induced in a field winding with a diode to generate a field current for the field winding A generator is known. Then, a brushless two-pole three-phase generator as shown in FIG. 7 was developed by applying the basic principle of the Nonaka generator. In FIG. 7, reference numeral 1 is a stator, 2 is a rotor, 3 is a two-pole three-phase main power generation winding, 4 is a single-phase four-pole excitation winding, 5 is a DC power supply, and 6-1a to 6 -1d is a field core, 6-2a to 6-2d are salient poles, 7a to 7d are field windings, and 8 is a diode.
上記第7図図示例においては,回転子2に設けられた
4極形状の界磁コア6−1aないし6−1dに界磁巻線7aな
いし7dが巻回されている。そし該界磁巻線7aないし7dの
それぞれにダイオード8が接続され,突極6−2aないし
6−2dに順次S,S,N,Nの磁極が発生して上記界磁コア6
−1aないし6−1dが磁化されるように構成されている。
すなわち,上記第7図図示例においては,回転子2が回
転するとき,上記励磁巻線4の静止磁界により,上記界
磁巻線7aないし7dに図示矢印方向の界磁電流が流れ,上
記界磁コア6−1aないし6−1dが磁化されることにより
見掛け上2極の界磁極を構成し,2極三相の主発電巻線3
に三相交流出力が得られる。In the example shown in FIG. 7, field windings 7a to 7d are wound around quadrupole field cores 6-1a to 6-1d provided on the rotor 2. A diode 8 is connected to each of the field windings 7a to 7d, and S, S, N and N magnetic poles are sequentially generated on the salient poles 6-2a to 6-2d to generate the field core 6 described above.
-1a to 6-1d are magnetized.
That is, in the example shown in FIG. 7, when the rotor 2 rotates, the static magnetic field of the exciting winding 4 causes a field current in the direction of the arrow in the field windings 7a to 7d to flow, and The magnetic cores 6-1a to 6-1d are magnetized to form apparently two-pole field poles, and the two-pole / three-phase main power generation winding 3
A three-phase AC output can be obtained.
他方,同期発電機においては,第8図図示の如き自励
式回転界磁形(集中巻線式)の発電機が知られている。
この方式は構造が簡単であるため,広く実用に供されて
いる。なお,第8図において,符号9は固定子,10は回
転子,11は固定子磁極,12は継鉄,13は主発電巻線,14は励
磁巻線,15は自動電圧調整器(AVR),16はブラシ・スリ
ップリング,17は界磁巻線,18は回転子コア,19は突極を
表している。On the other hand, as the synchronous generator, a self-excited rotating field type (concentrated winding type) generator as shown in FIG. 8 is known.
Since this method has a simple structure, it is widely used in practice. In FIG. 8, reference numeral 9 is a stator, 10 is a rotor, 11 is a stator magnetic pole, 12 is a yoke, 13 is a main generator winding, 14 is an excitation winding, and 15 is an automatic voltage regulator (AVR). ), 16 is a brush slip ring, 17 is a field winding, 18 is a rotor core, and 19 is a salient pole.
上記第8図図示例においては,回転子10が回転すると
き,上記励磁巻線14に交差する磁界に比例した電圧が誘
起され,これによって電流がAVR15を介して界磁巻線17
に供給され,上記回転子コア18に磁化され,2極の主発電
巻線13に交流出力が得られる。In the example shown in FIG. 8, when the rotor 10 rotates, a voltage proportional to the magnetic field intersecting with the excitation winding 14 is induced, which causes a current to flow through the AVR 15 into the field winding 17
Is supplied to the rotor core 18 and is magnetized by the rotor core 18 to obtain an AC output in the two-pole main power generation winding 13.
第8図図示例では,回転子側に巻回された界磁巻線17
に対して,固定子側の励磁巻線14からの電流を供給する
必要があるため、ブラシ・スリップリング16を省略(ブ
ラシレス化)することは困難であった。In the example shown in FIG. 8, the field winding 17 wound around the rotor side
On the other hand, since it is necessary to supply the current from the excitation winding 14 on the stator side, it is difficult to omit the brush slip ring 16 (make it brushless).
これに加えて,第7図図示の従来のブラシレス発電機
では,励磁巻線4に対する励磁電流が外部の直流電源5
によって供給されるように構成されている。従って上記
第7図図示例においては,直流電源5が必要となる問題
がある。In addition to this, in the conventional brushless generator shown in FIG. 7, the exciting current to the exciting winding 4 is the external DC power source 5
Is configured to be supplied by. Therefore, in the example shown in FIG. 7, there is a problem that the DC power source 5 is required.
また,単相負荷で使用する場合,その負荷補償が小さ
いので,負荷電流が増加したときの電圧降下が大きくな
る問題があった。Also, when used with a single-phase load, the load compensation is small, so there was the problem of a large voltage drop when the load current increased.
本発明は上記の問題点を解決することを目的としてい
る。The present invention aims to solve the above problems.
本発明においては次の如き構成をもつようにされる。
即ち,全体形状がU字形の固定子を有するブラシレス発
電機において, (i) 固定子に巻回されている励磁巻線の極数と主発
電巻線の極数との関係を,いずれか一方が他方の整数倍
とし, (ii) 回転子に巻回されている界磁巻線は,励磁巻線
に接続されることなく,励磁巻線の極数に対応した極数
の磁束と主発電巻線の極数に対応した極数の磁束とを生
じるよう構成され, (iii) 励磁巻線は環流路をつくるように構成され
る。The present invention has the following structure.
That is, in a brushless generator having a U-shaped stator as a whole, (i) one of the relationship between the number of poles of the excitation winding and the number of main generator windings wound around the stator is Is an integral multiple of the other, and (ii) the field winding wound around the rotor is not connected to the excitation winding, but the magnetic flux of the number of poles corresponding to the number of poles of the excitation winding and the main power generation. It is configured to generate a magnetic flux with the number of poles corresponding to the number of winding poles. (Iii) The excitation winding is configured to form a ring flow path.
第1図は本発明に係わる回転界磁形の自励式同期発電
機の一実施例の構造を示している。FIG. 1 shows the structure of an embodiment of a rotating field type self-excited synchronous generator according to the present invention.
第1図において,符号21は固定子,22は回転子,23は2
極の主発電巻線,24は6極の励磁巻線,25は回転子コア
(鉄心),25−aと25−bとは突極,26は主界磁巻線,26
−aは界磁補助巻線,27及び28は夫々ダイオード,30は固
定子磁極,31は継鉄を表している。In FIG. 1, reference numeral 21 is a stator, 22 is a rotor, and 23 is 2
Pole main generator winding, 24 6-pole excitation winding, 25 rotor core (iron core), 25-a and 25-b salient poles, 26 main field winding, 26
Reference symbol -a is a field auxiliary winding, 27 and 28 are diodes, 30 is a stator pole, and 31 is a yoke.
固定子21においては,2つに分割された固定子磁極30に
夫々励磁巻線24が巻回されると共に,前記分割された磁
極30相互間を接続している継鉄31に主発電巻線23が巻回
されている。固定子21の鉄心は,例えば1乃至3.5%の
硅素を含む硅素鋼の薄板を積層して構成される。励磁巻
線24は,界磁巻線に接続されることなく,環流路を形成
する。In the stator 21, an exciting winding 24 is wound around each of the stator poles 30 divided into two, and a main generator winding is connected to a yoke 31 connecting the divided magnetic poles 30 to each other. There are 23 wound. The iron core of the stator 21 is formed by laminating thin sheets of silicon steel containing, for example, 1 to 3.5% silicon. The excitation winding 24 forms an annular flow path without being connected to the field winding.
回転子22においては,軸を中心として回転する回転子
コア25に,主界磁巻線26及び界磁補助巻線26−aが巻回
されている。回転子コア25(即ち回転子22)は主発電巻
線23の極数と同じ数の突極25−a及び25−bを有する。
回転子コア25は打ち抜き成形された鋼板を積層して形成
される。In the rotor 22, a main field winding 26 and a field auxiliary winding 26-a are wound around a rotor core 25 that rotates about an axis. The rotor core 25 (that is, the rotor 22) has the same number of salient poles 25-a and 25-b as the number of poles of the main power generation winding 23.
The rotor core 25 is formed by stacking punched steel plates.
回転子22に対して所定のギャップだけ離して,固定子
21が設けられる。すなわち,回転子22に対し,所定のギ
ャップを持って,固定子磁極30が対向させられる。この
ために,2つに分割された磁極30は,各々が実質的に半円
形状の内周面をもつ。なお,2つの磁極30は,半矩形状の
継鉄31によって結合され,固定子21は全体として実質的
にコ字状とされる。The stator is separated from the rotor 22 by a predetermined gap.
21 is provided. That is, the stator magnetic pole 30 is opposed to the rotor 22 with a predetermined gap. For this reason, each of the two divided magnetic poles 30 has a substantially semicircular inner peripheral surface. The two magnetic poles 30 are connected by a semi-rectangular yoke 31, and the stator 21 is substantially U-shaped as a whole.
第2図は,第1図図示の同期発電機についての電機子
回路及び界磁回路の概略を示している。また,第3図
は,回転子22の界磁回路の等価回路を示している。これ
ら図中の符号は第1図に対応している。FIG. 2 shows an outline of an armature circuit and a field circuit for the synchronous generator shown in FIG. Further, FIG. 3 shows an equivalent circuit of the field circuit of the rotor 22. The reference numerals in these figures correspond to those in FIG.
即ち,固定子21には2極主発電巻線23と,6極励磁巻線
24とが巻回され,6極の励磁巻線24は図示の場合には直接
短絡されて環流路が形成されている。That is, the stator 21 has a 2-pole main generator winding 23 and a 6-pole excitation winding.
24 and 6 are wound, and the 6-pole excitation winding 24 is directly short-circuited in the illustrated case to form an annular flow path.
回転子22は,図示の実施例の場合には,主発電巻線23
の極数と等しい極数(図示の場合2極)の突極25−aと
25−bとをもち,主界磁巻線26にはダイオード27が直列
に挿入されて上記2極の磁界を発生させるように構成さ
れている。そしてその上で,突極25−a上に界磁補助巻
線26−aが巻回されると共に,この界磁補助巻線26−a
が一旦交差させられた上,突極25−b上に巻回され,か
つダイオード28が界磁補助巻線26−aに直列に挿入され
ている。また,界磁補助巻線26−aは,主界磁巻線26に
対して,ダイオード28の陽極側がダイオード27の陽極側
となるように接続される。これによって,界磁補助巻線
26−aは,突極25−a面において主界磁巻線26がつくる
磁極Nを強めるように働き,他方の突極25−b面におい
ても主界磁巻線26がつくる磁極Sを強めるように働く。In the case of the illustrated embodiment, the rotor 22 is a main generator winding 23.
The salient poles 25-a having the same number of poles (two poles in the figure)
25-b, a diode 27 is inserted in series in the main field winding 26 to generate the magnetic field of the two poles. Then, the auxiliary field winding 26-a is wound on the salient pole 25-a, and the auxiliary field winding 26-a is also wound.
Are crossed once, wound on salient pole 25-b, and diode 28 is inserted in series in field auxiliary winding 26-a. Further, the field auxiliary winding 26-a is connected to the main field winding 26 such that the anode side of the diode 28 is the anode side of the diode 27. This allows the field auxiliary winding
The 26-a works to strengthen the magnetic pole N formed by the main field winding 26 on the salient pole 25-a surface, and strengthens the magnetic pole S formed by the main field winding 26 on the other salient pole 25-b surface. Work like.
即ち,界磁補助巻線26−aは,6極の励磁巻線24のピッ
チの2倍よりも小さいピッチをもって,突極25−a上に
巻回れ,ダイオード28を介して主界磁巻線26に流れる電
流に対して和になる方向に電流を流し、かつ突極25−a
上に主界磁巻線26がつくる磁極と同じ極性の磁束を発生
する。また同様に,界磁補助巻線26−aは,単相6極の
励磁巻線24のピッチの2倍よりも小さいピッチをもっ
て,突極25−b上に巻回され,ダイオード28を介して主
界磁巻線26に流れる電流に対して和になる方向に電流を
流し,かつ突極25−b上に主界磁巻線26がつくる磁極と
同じ極性の磁束を発生する。That is, the field auxiliary winding 26-a is wound on the salient pole 25-a with a pitch smaller than twice the pitch of the 6-pole excitation winding 24, and the main field winding is wound via the diode 28. The current flows in the direction that is the sum of the currents flowing in 26, and the salient pole 25-a
A magnetic flux having the same polarity as the magnetic pole formed by the main field winding 26 is generated above. Similarly, the field auxiliary winding 26-a is wound on the salient pole 25-b with a pitch smaller than twice the pitch of the single-phase 6-pole exciting winding 24, and via the diode 28. A current flows in a direction that is the sum of the currents flowing in the main field winding 26, and a magnetic flux having the same polarity as the magnetic pole formed by the main field winding 26 is generated on the salient pole 25-b.
第1図図示の例の場合,回転子22の残留磁気により励
磁巻線24に電流が流れ,この電流によってつくられる磁
束(6極の)によって,界磁補助巻線26−aに電圧が誘
起される。この電圧によって,ダイオード28を介して界
磁補助巻線26−aに電流が供給され,ダイオード28を介
して主界磁巻線26に電流が供給され,図示の場合には2
極の主磁束がつくられる。この主磁束によって,2極に巻
回されている主発電巻線23に電圧が誘起され,負荷電流
が流れる。In the case of the example shown in FIG. 1, a current flows in the exciting winding 24 due to the residual magnetism of the rotor 22, and a magnetic flux (six poles) created by this current induces a voltage in the field auxiliary winding 26-a. To be done. This voltage supplies a current to the field auxiliary winding 26-a via the diode 28 and a current to the main field winding 26 via the diode 28.
The main magnetic flux of the pole is created. This main magnetic flux induces a voltage in the main power generation winding 23 wound around two poles, and a load current flows.
この負荷電流の電機子反作用によって,従来の野中式
発電機と同様に,主界磁巻線26に電圧が誘起され,主発
電巻線23に誘起される電圧が増大されるように働く。一
方,2極の主磁束は,6極に巻回されている励磁巻線24にも
電圧を誘起し,励磁電流を増加させる。この増加した励
磁電流により6極の磁束が増す結果,界磁補助巻線26−
aに誘起される電圧が増し,磁束も増す。以上の動作の
繰り返しによって,主発電巻線23の出力電圧が確立され
る。Due to the armature reaction of this load current, a voltage is induced in the main field winding 26 and the voltage induced in the main power generation winding 23 is increased, as in the conventional Nonaka generator. On the other hand, the main magnetic flux of the two poles also induces a voltage in the excitation winding 24 wound around the six poles to increase the excitation current. As a result of increasing the magnetic flux of 6 poles by this increased exciting current, the field auxiliary winding 26-
The voltage induced in a increases and the magnetic flux also increases. By repeating the above operation, the output voltage of the main power generation winding 23 is established.
なお,前記電機子反作用によって生じた磁束が主界磁
巻線26と鎖交するとき,主界磁巻線26はダイオード27に
よって短絡されているため,短絡電流が増加し、2極の
主磁束を増加させる。このため,主発電巻線23に発生す
る電圧が上昇し,電圧補償となる。When the magnetic flux generated by the armature reaction interlinks with the main field winding 26, the main field winding 26 is short-circuited by the diode 27, so that the short-circuit current increases and the main magnetic flux of the two poles increases. To increase. For this reason, the voltage generated in the main power generation winding 23 rises and the voltage is compensated.
また,主界磁巻線26のつくる磁束は,界磁補助巻線26
−aのつくる磁束を強めるように働く。In addition, the magnetic flux generated by the main field winding 26 is
-Work to strengthen the magnetic flux created by a.
なお,仮に,主発電巻線23が2極に巻回されておりか
つ励磁巻線24が4極に巻回されているような場合でも,
波形に歪みが生じるけれども,仕様によっては許容でき
るものとなる。Even if the main generator winding 23 is wound around two poles and the excitation winding 24 is wound around four poles,
Although the waveform is distorted, it is acceptable depending on the specifications.
第1図図示の場合には,励磁巻線24は還流路をつくる
ように接続すればよく,上述の第7図図示の場合のよう
に他励の形式にする必要はない。In the case shown in FIG. 1, the excitation winding 24 may be connected so as to form a return path, and it is not necessary to use the separately excited form as in the case shown in FIG.
第4図は2極の構成に巻回した主発電巻線の態様を示
し,第5図(A)(B)(C)は6極の構成に巻回され
た励磁巻線に対して環流路を形成させる態様を示してい
る。図中の符号23,24は第1図に対応しており,32は直接
短絡した還流路,33はダイオードであり当該ダイオード3
3を介して環流路が形成されるもの,34はコンデンサであ
って当該コンデンサ34を介して環流路が形成されるもの
を表している。Fig. 4 shows the mode of the main power generation winding wound in a 2-pole configuration, and Figs. 5 (A), (B), and (C) show the circulation of the excitation winding wound in a 6-pole configuration. The mode which forms a path | route is shown. Reference numerals 23 and 24 in the figure correspond to those in FIG. 1, 32 is a directly short-circuited return path, 33 is a diode, and the diode 3
Reference numeral 34 denotes a ring flow path formed via 3, and reference numeral 34 denotes a capacitor having a ring flow path formed via the capacitor 34.
本発明の場合,第4図の主発電巻線23と,第5図
(A)(B)(C)のいずれか1つの形の励磁巻線環流
路形成態様との組み合わせを採用することができる。In the case of the present invention, a combination of the main power generation winding 23 of FIG. 4 and the excitation winding ring flow path forming mode of any one of FIGS. 5 (A) (B) (C) may be adopted. it can.
第5図(B)図示の場合には,励磁巻線24上に直流が
流れ,これによって回転子22上の主界磁巻線26又は界磁
補助巻線26−a上に電圧が誘起される形となる。第5図
(C)図示の場合には,励磁巻線24上には交流電流が流
れ,これによって回転子22上の主界磁巻線26又は界磁補
助巻線26−a上に電圧が誘起される形となる。なお第5
図(C)図示の場合の如き構成が採用される際には,励
磁巻線24の極数と主発電巻線23の極数と等しいものとし
た場合のコンデンサの容量にくらべて,コンデンサ34の
容量を十分に小さく選ぶことが可能となる。In the case shown in FIG. 5 (B), a direct current flows through the excitation winding 24, which induces a voltage on the main field winding 26 or the field auxiliary winding 26-a on the rotor 22. Becomes a shape. In the case shown in FIG. 5 (C), an alternating current flows through the excitation winding 24, which causes a voltage to appear on the main field winding 26 or the field auxiliary winding 26-a on the rotor 22. It will be an induced form. The fifth
When the configuration as shown in FIG. (C) is adopted, the capacitance of the capacitor 34 is larger than the capacitance of the capacitor when the number of poles of the excitation winding 24 and the number of poles of the main power generation winding 23 are equal. It is possible to select a sufficiently small capacity.
第6図は第1図図示の実施例の場合の変形を表す実施
例を示している。第6図は第1図に対応し,回転子22の
構成は第1図と同じであるので省略している。FIG. 6 shows an embodiment showing a modification of the embodiment shown in FIG. FIG. 6 corresponds to FIG. 1, and the structure of the rotor 22 is the same as that of FIG.
第6図において,6極の磁束をつくるための励磁巻線24
は,第1図図示の例と同じピッチで,図示の如く固定子
21の極数30上に6極を形成するように巻回されている。In Fig. 6, the excitation winding 24 for creating magnetic flux of 6 poles
Is the same pitch as the example shown in FIG.
It is wound so as to form 6 poles on 30 poles of 21.
第6図図示の例の場合,励磁巻線24の環流路の態様
は,第5図(A)(B)(C)のいずれか1つの形の環
流路形成態様によって,形成される。In the case of the example shown in FIG. 6, the mode of the annular flow path of the excitation winding 24 is formed by the annular flow path forming mode of any one of FIGS. 5 (A), (B) and (C).
以上説明した如く,本発明によれば,回転界磁形の同
期発電機を全体U字形状の固定子をもつブラシレス発電
機の構成とすることが可能となる。As described above, according to the present invention, the rotating field synchronous generator can be configured as a brushless generator having a U-shaped stator as a whole.
第1図は本発明の一実施例,第2図は第1図の発電機の
界磁回路の概略の構成,第3図は等価回路,第4図は2
極の構成に巻回した主発電巻線の態様,第5図(A)
(B)(C)は6極の構成に巻回態様,第5図(A)
(B)(C)は6極の構成に巻回された励磁巻線に対し
て環流路を形成させる態様,第6図は本発明の変形を表
す実施例の場合における固定子の構成,第7図と第8図
とは夫々従来の発電機の構成を示す。 図中,21は固定子,22は回転子,23は主発電巻線,24は励磁
巻線,25は回転子コア,26は主界磁巻線,26−aは界磁補
助巻線,27,28はダイオード,30は固定子磁極,31は継鉄,3
3はダイオード,34はコンデンサを表す。1 is an embodiment of the present invention, FIG. 2 is a schematic configuration of a field circuit of the generator shown in FIG. 1, FIG. 3 is an equivalent circuit, and FIG.
Aspects of the main generator winding wound in a pole configuration, Fig. 5 (A)
(B) and (C) are winding patterns in a 6-pole configuration, FIG. 5 (A)
(B) and (C) are modes in which an annular flow path is formed with respect to the excitation winding wound in a 6-pole configuration, and FIG. 6 is a configuration of a stator in the case of an embodiment representing a modification of the present invention, FIG. 7 and FIG. 8 show the construction of a conventional generator, respectively. In the figure, 21 is a stator, 22 is a rotor, 23 is a main power generation winding, 24 is an excitation winding, 25 is a rotor core, 26 is a main field winding, 26-a is a field auxiliary winding, 27 and 28 are diodes, 30 is a stator pole, 31 is a yoke, 3
3 is a diode and 34 is a capacitor.
フロントページの続き (72)発明者 小檜山 博 群馬県新田郡新田町大字早川字早川3番地 澤藤電機株式会社新田工場内 (56)参考文献 特開 昭62−23348(JP,A)Continuation of front page (72) Inventor Hiroshi Kohiyama, No. 3 Hayakawa, Hayakawa, Nitta-cho, Nitta-gun, Gunma Sawafuji Electric Co., Ltd., Nitta factory (56) Reference JP-A-62-23348 (JP, A)
Claims (1)
を接続する継鉄と該継鉄に巻回された主発電巻線を有す
る全体形状U字状の固定子を備え, 回転子に発生する磁界が上記主発電巻線に鎖交すること
により当該主発電巻線に電圧が誘起される構成のブラシ
レス発電機において, 固定子には上記2つの磁極の端面上に夫々形成された溝
内に巻回されて回転子の磁界と鎖交して磁界を発生させ
る励磁巻線を備え 当該励磁巻線の極数と上記主発電巻線の極数とのいずれ
か一方が他方に対して整数倍の関係をもつよう構成され
ると共に, 回転子には上記励磁巻線のピッチの2倍より小さいピッ
チをもって巻回された界磁補助巻線と上記主発電巻線の
極数に等しい極数の主界磁巻線とを有し かつ当該主界磁巻線と当該主界磁巻線によってつくられ
る主界磁磁極の端面上の溝内に巻回された当該界磁補助
巻線との両者が夫々同一種類の極の磁束を発生するよう
ダイオードを接続されてなり, 上記励磁巻線は励磁電流が流れるよう還流路を形成され
ている ことを特徴とするブラシレス発電機。1. A rotor for generating a magnetic field, two magnetic poles provided facing the rotor, a yoke connecting the magnetic poles, and a main power generation winding wound around the yoke. A brushless generator having a U-shaped stator having an overall shape, and a voltage is induced in the main power generation winding by interlinking the magnetic field generated in the rotor with the main power generation winding. The child is provided with exciting windings wound in the grooves respectively formed on the end faces of the two magnetic poles and interlinking with the magnetic field of the rotor to generate a magnetic field. One of the poles of the generator winding has an integral multiple relationship with the other, and the rotor has a field wound with a pitch smaller than twice the pitch of the excitation winding. It has a magnetic auxiliary winding and a main field winding with the same number of poles as the number of poles of the main power generation winding. In addition, both the main field winding and the field auxiliary winding wound in the groove on the end face of the main field magnetic pole formed by the main field winding respectively generate magnetic fluxes of the same type of pole. A brushless generator characterized in that a diode is connected to generate the current, and the excitation winding has a return path formed so that an excitation current flows.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62189682A JPH0817560B2 (en) | 1987-07-29 | 1987-07-29 | Brushless generator |
| US07/163,768 US4851758A (en) | 1987-03-09 | 1988-03-03 | Brushless generator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62189682A JPH0817560B2 (en) | 1987-07-29 | 1987-07-29 | Brushless generator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6439249A JPS6439249A (en) | 1989-02-09 |
| JPH0817560B2 true JPH0817560B2 (en) | 1996-02-21 |
Family
ID=16245417
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62189682A Expired - Lifetime JPH0817560B2 (en) | 1987-03-09 | 1987-07-29 | Brushless generator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0817560B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2006149148A (en) * | 2004-11-24 | 2006-06-08 | Ntt Data Ex Techno Corp | Generator |
| JP4821770B2 (en) * | 2005-07-19 | 2011-11-24 | 株式会社デンソー | AC motor and its control device |
| WO2007037020A1 (en) * | 2005-09-29 | 2007-04-05 | Hideo Nakata | Single-phase ac composite generator |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6223348A (en) * | 1985-07-22 | 1987-01-31 | Sawafuji Electric Co Ltd | Brushless generator |
-
1987
- 1987-07-29 JP JP62189682A patent/JPH0817560B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6439249A (en) | 1989-02-09 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US4851758A (en) | Brushless generator | |
| JPH0288500U (en) | ||
| JP2003504996A (en) | Electrical equipment | |
| JPH0865976A (en) | Brushless self-excited three-phase synchronous generator | |
| JPS5837799B2 (en) | electric motor device | |
| JP3788494B2 (en) | Brushless three-phase synchronous generator | |
| JP3165968B2 (en) | Brushless synchronous machine | |
| JP2887686B2 (en) | Brushless self-excited synchronous generator | |
| JPS6223348A (en) | Brushless generator | |
| JPH01103143A (en) | Self-excited brushless synchronous motor | |
| JP3539148B2 (en) | Cylindrical synchronous generator | |
| JP3223710B2 (en) | Salient pole rotating field type alternator | |
| JPH0739334Y2 (en) | AC output combined welding generator | |
| JPS62155796A (en) | High power-factor control method for permanent-magnet synchronous motor | |
| JPH06269151A (en) | Brushless synchronous generator | |
| JP2753721B2 (en) | Brushless self-excited synchronous generator | |
| JPH0424782Y2 (en) | ||
| JPH0540698Y2 (en) | ||
| JPH01264551A (en) | Brushless self-excited synchronous generator | |
| RU1798864C (en) | Electromachine unit | |
| JP2530297B2 (en) | AC generator | |
| SU1293798A1 (en) | Forward-backward motor-amplifier | |
| JPS6022450A (en) | Structure of rotary electric machine | |
| JPH0626063Y2 (en) | Brushless 4-pole 3-phase generator | |
| SU758416A1 (en) | Power-diode electric motor |