JPH1155912A - Cylindrical synchronous generator - Google Patents

Cylindrical synchronous generator

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Publication number
JPH1155912A
JPH1155912A JP22094297A JP22094297A JPH1155912A JP H1155912 A JPH1155912 A JP H1155912A JP 22094297 A JP22094297 A JP 22094297A JP 22094297 A JP22094297 A JP 22094297A JP H1155912 A JPH1155912 A JP H1155912A
Authority
JP
Japan
Prior art keywords
winding
rotor
main
field
stator
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.)
Granted
Application number
JP22094297A
Other languages
Japanese (ja)
Other versions
JP3539148B2 (en
Inventor
Satoru Satake
覺 佐竹
Yukio Onoki
幸男 大野木
Kenji Inoue
憲治 猪上
Yukio Hosaka
幸男 保坂
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Satake Engineering Co Ltd
Original Assignee
Satake Engineering Co Ltd
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Filing date
Publication date
Application filed by Satake Engineering Co Ltd filed Critical Satake Engineering Co Ltd
Priority to JP22094297A priority Critical patent/JP3539148B2/en
Publication of JPH1155912A publication Critical patent/JPH1155912A/en
Application granted granted Critical
Publication of JP3539148B2 publication Critical patent/JP3539148B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

(57)【要約】 【課題】逆相分電流の大きさに制限されることもなく、
従来の発電機より多く負荷しうる発電機を得る。 【解決手段】三相4極主発電巻線3と該主発電巻線3の
極数の2倍の極数を有する固定子界磁巻線4とを固定子
に巻装し、固定子界磁巻線4と磁気的結合をなす回転子
励磁巻線5と、全節集中巻にして整流器8で短絡した複
数個の分布した回転子巻線7とを巻装してあると共に、
前記回転子励磁巻線5の起電力を直流に変換する回転整
流器6を備え、前記複数個の回転子巻線7のうち主発電
巻線3の主界磁に最も寄与する回転子巻線7にのみ前記
回転整流器6の出力を接続して回転子10を構成した。
(57) [Summary] [Problem] Without being limited to the magnitude of the current in the negative phase,
A generator that can load more than a conventional generator is obtained. A three-phase four-pole main power generation winding (3) and a stator field winding (4) having twice the number of poles of the main power generation winding (3) are wound around a stator, and the stator field A rotor excitation winding 5 magnetically coupled to the magnetic winding 4 and a plurality of distributed rotor windings 7 short-circuited by a rectifier 8 in a concentrated winding of all sections are wound.
A rotor rectifier 6 for converting an electromotive force of the rotor excitation winding 5 into a direct current, and a rotor winding 7 of the plurality of rotor windings 7 which most contributes to a main field of a main power generation winding 3; And the output of the rotary rectifier 6 was connected to the rotor 10 to form the rotor 10.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】不平衡負荷に対応した円筒型
同期発電機に関する。
[0001] 1. Field of the Invention [0002] The present invention relates to a cylindrical synchronous generator corresponding to an unbalanced load.

【0002】[0002]

【従来の技術】発電機が本体内に直巻励磁機能を有し、
平複巻特性の電圧を出力するブラシレス自励同期発電機
としては特開平3−245755号公報により開示され
た発電機が知られており、このブラシレス自励同期発電
機を図9に示す。
2. Description of the Related Art A generator has a series winding excitation function in a main body thereof.
As a brushless self-excited synchronous generator that outputs a voltage having a flat compound winding characteristic, a generator disclosed in Japanese Patent Application Laid-Open No. 3-245755 is known, and this brushless self-excited synchronous generator is shown in FIG.

【0003】特開平3−245755号公報のブラシレ
ス自励同期発電機は、固定子鉄心20に集中全節巻乃至
集中全節巻に準ずる巻線態様の2極(実施例)の主発電
巻線U,V,Wと該主発電巻線の極数の5倍(実施例)
の極数を有する10極(実施例)の固定子界磁巻線21
とが巻装され、回転子鉄心22には前記主発電巻線の極
数と等しい極数を有する2極(実施例)の回転子界磁巻
線23と前記固定子界磁巻線の極数と等しい極数を有
し、且つ前記主発電巻線の電流が作る電機子反作用磁界
の第5次空間高調波成分(10極磁界)とも磁気的結合
を成す10極(実施例)の回転子励磁巻線24とが巻装
されて、前記主発電巻線U,V,Wと前記固定子界磁巻
線21とは、主発電巻線U,V,Wの各相の中間タップ
u,v,wに接続された制御整流装置VR(三相全波整
流器25および可変抵抗器Rf)を介して接続され、前
記回転子励磁巻線24と前記回転子界磁巻線23とはダ
イオ−ドブリッジ回路26を介して接続されている。
The brushless self-excited synchronous generator disclosed in Japanese Patent Application Laid-Open No. 3-245755 has a two-pole (embodiment) main power generation winding having a winding form conforming to concentrated full winding or concentrated full winding on the stator core 20. U, V, W and 5 times the number of poles of the main power generation winding (Example)
(Example) stator field winding 21 having 10 poles
The rotor core 22 has two poles (example) of the rotor field winding 23 and the poles of the stator field winding having the same number of poles as the main power generation winding. Rotation of 10 poles (embodiment) having the same number of poles and magnetically coupling with the fifth spatial harmonic component (10-pole magnetic field) of the armature reaction magnetic field generated by the current of the main power generation winding. The main excitation windings 24 are wound, and the main power generation windings U, V, W and the stator field windings 21 are connected to intermediate taps u of respective phases of the main power generation windings U, V, W. , V, w connected via a control rectifier VR (a three-phase full-wave rectifier 25 and a variable resistor Rf), and the rotor excitation winding 24 and the rotor field winding 23 are Connected via a bridge circuit 26.

【0004】この構成のブラシレス自励同期発電機の作
用を以下に説明する。回転子を回転させると回転子鉄心
22の残留磁気によって主発電巻線U,V,Wに起電力
が誘導される。この誘導起電力は三相全波整流器25に
よって整流されて固定子界磁巻線21に直流電流Ifs
が流れると共に主発電巻線に交流電流が流れて、回転子
励磁巻線24には直流電流Ifsが作る静止磁界に基づ
く起電力と、主発電巻線の交流電流が作る電機子反作用
磁界の第5次空間高調波成分に基づく起電力とが重畳し
て誘導し、該重畳起電力がダイオ−ドブリッジ回路26
によって整流されて回転子界磁巻線23に直流電流If
が流れ、主磁界が増磁して主発電巻線の起電力が増加す
る。そしてこの動作を繰り返して出力電圧が自己確立す
る。なお、このとき回転子鉄心22の残留磁気が不足の
場合にはバッテリ−Bによって初期励磁を行う。
[0004] The operation of the brushless self-excited synchronous generator having this configuration will be described below. When the rotor is rotated, an electromotive force is induced in the main power generation windings U, V, W by the residual magnetism of the rotor core 22. This induced electromotive force is rectified by the three-phase full-wave rectifier 25 and the direct current Ifs is applied to the stator field winding 21.
And the alternating current flows through the main power generation winding, and the rotor excitation winding 24 has an electromotive force based on the static magnetic field generated by the DC current Ifs and the armature reaction magnetic field generated by the alternating current of the main power generation winding. The electromotive force based on the fifth harmonic component is superposed and induced, and the superimposed electromotive force is applied to the diode bridge circuit 26.
DC current If
Flows, and the main magnetic field is magnetized to increase the electromotive force of the main power generation winding. By repeating this operation, the output voltage is self-established. At this time, if the residual magnetism of the rotor core 22 is insufficient, the battery B is used to perform the initial excitation.

【0005】更に、このブラシレス自励同期発電機は三
相の抵抗および誘導性(遅れ力率)負荷においてそれぞ
れ負荷が増減すると、負荷電流の増減に比例して電機子
反作用磁界の第5次空間高調波成分が増減し、結果的に
回転子界磁巻線23の直流電流Ifが増減して出力電圧
の変動が抑制され、負荷の増減に対して平複巻特性の出
力電圧が得られる。また、発電機に三相不平衡負荷ある
いは単相負荷を接続した場合は、電機子反作用磁界の第
5次空間高調波成分による直巻励磁効果は三相平衡負荷
時に比べて減少するが、三相不平衡負荷時あるいは単相
負荷時には電機子反作用磁界の逆相分の空間基本波成分
によって回転子界磁巻線23に起電力が誘導し、該起電
力はダイオ−ドブリッジ回路26によって半波整流され
て前記直巻励磁効果の減少に基づく回転子界磁巻線23
の直流電流Ifの減少分を補償するので、三相不平衡負
荷あるいは単相負荷時の出力電圧も三相平衡負荷時と同
様に平複巻特性となる。
Further, in the brushless self-excited synchronous generator, when the load increases or decreases in a three-phase resistance and an inductive (lagging power factor) load, respectively, the fifth-order space of the armature reaction magnetic field increases in proportion to the increase or decrease of the load current. The harmonic component increases and decreases, and as a result, the DC current If of the rotor field winding 23 increases and decreases, thereby suppressing the fluctuation of the output voltage. As a result, an output voltage having a flat double winding characteristic can be obtained with respect to the increase and decrease of the load. When a three-phase unbalanced load or a single-phase load is connected to the generator, the series-wound excitation effect due to the fifth spatial harmonic component of the armature reaction magnetic field is reduced as compared with the three-phase balanced load. When a phase-unbalanced load or a single-phase load is applied, an electromotive force is induced in the rotor field winding 23 by the spatial fundamental wave component of the opposite phase of the armature reaction magnetic field, and the electromotive force is half-waved by the diode bridge circuit 26. The rotor field winding 23 is rectified and is based on the reduction of the series exciting effect.
Is compensated for, the output voltage at the time of a three-phase unbalanced load or a single-phase load also has a flat compound winding characteristic as at the time of a three-phase balanced load.

【0006】[0006]

【発明が解決しようとする課題】このブラシレス自励同
期発電機は、三相発電機の負荷を三相不平衡負荷とした
時、発電巻線には正相分と逆相分の電機子反作用磁界を
生じる。このうち正相分電機子反作用磁界は三相平衡電
流の電機子反作用と同一のものであり支障ないが、逆相
分の電機子反作用磁界は、前述のように空間基本波成分
によって回転子界磁巻線に起電力が誘導し補償作用を有
するものの、同時に界磁に2倍周波数の交流を誘起して
電機子誘起電圧を歪ませ、回転子に渦電流を誘起して回
転子を加熱する等の種々の悪影響を及ぼすことが知られ
ている。
In this brushless self-excited synchronous generator, when the load of the three-phase generator is a three-phase unbalanced load, the armature reaction for the positive phase component and the negative phase component is applied to the power generation winding. Generates a magnetic field. Of these, the positive-phase armature reaction magnetic field is the same as the armature reaction of the three-phase equilibrium current, and does not cause any problem. Although the electromotive force is induced in the magnetic winding and has a compensating effect, at the same time, a double frequency alternating current is induced in the field to distort the armature induced voltage, and an eddy current is induced in the rotor to heat the rotor. And other various adverse effects.

【0007】これは逆相分回転磁界は同期速度の2倍の
速度で界磁巻線と鎖交するから、界磁巻線には2倍の周
波数の交流電圧を誘起する。界磁巻線は単相巻線と考え
られるから電機子巻線の反作用と同様に同一速度で互い
に反対方向に回転する2つのベクトルの合成を考えれば
この磁束によって電機子巻線に3倍の周波数電圧を誘起
する。電機子回路に第3高調波の交流が流れると前記同
様の作用によりその起磁力よって界磁巻線には4倍の周
波数の交流電圧を誘起する。このように高調波電流が自
在に流れるままにしておくと、電機子巻線には基本波の
ほかに3倍、5倍、7倍等の高調波の電圧、電流を誘起
して界磁巻線には直流のほかに2倍、4倍、6倍、8倍
等の高調波電流を発生するものである。この現象は、ダ
ンパが不完全である従来の三相発電機に共通するもので
ある。
This is because the rotating magnetic field of the opposite phase interlinks with the field winding at a speed twice as fast as the synchronous speed, so that an AC voltage having twice the frequency is induced in the field winding. The field winding is considered to be a single-phase winding. Therefore, considering the combination of two vectors rotating in the opposite direction at the same speed as in the reaction of the armature winding, the magnetic flux increases the armature winding three times. Induces frequency voltage. When an AC of the third harmonic flows through the armature circuit, an AC voltage having a frequency four times higher is induced in the field winding by the magnetomotive force due to the same action as described above. If the harmonic current is allowed to flow freely, the armature winding induces a voltage, current, etc., which is 3 times, 5 times, 7 times, etc., in addition to the fundamental wave, thereby causing the field winding. The wires generate harmonic currents of 2, 4, 6, 8, etc. in addition to the direct current. This phenomenon is common to conventional three-phase generators with imperfect dampers.

【0008】このようにして発生する渦電流による回転
子の加熱作用は事故を起こすおそれがあるから見逃し難
いものであり、このようなことを考慮して一般的には逆
相分は定格正相分の15〜25%位が限度であるとされ
ている。
[0008] The heating action of the rotor due to the eddy current generated in this way is difficult to overlook because there is a risk of causing an accident. It is said that the limit is about 15 to 25%.

【0009】以上のことから、本発明の発電機は、任意
の次数の高調波成分を選択することがないので、選択し
た高調波成分の次数によってスロット数やその組み合わ
せが特定の数に限定されることがなく、逆相分電流の大
きさに制限されることもなく、単相負荷やインバ−タ等
の高調波を発生する負荷も従来の発電機より多く負荷し
うる発電機を提供することを課題とするものである。
As described above, since the generator of the present invention does not select any harmonic component of an arbitrary order, the number of slots and a combination thereof are limited to a specific number depending on the order of the selected harmonic component. The present invention provides a generator which is not limited by the magnitude of the current in the negative phase and is not limited by the magnitude of the current in the opposite phase, and can load a single-phase load, an inverter or the like which generates harmonics more than a conventional generator. That is the task.

【0010】[0010]

【課題を解決するための手段】本発明の請求項1による
と、主発電巻線と、全節集中巻にして整流器で短絡した
複数個の回転子巻線を分布して巻装し前記主発電巻線と
磁気的結合をなす円筒型界磁と、固定子界磁巻線と、該
固定子界磁巻線と磁気的結合をなす回転子励磁巻線と、
及び該回転子励磁巻線の発電出力を直流に変換する回転
整流器とから構成された円筒型同期発電機であって、前
記複数個の回転子巻線のうち主発電巻線の極数の主界磁
に最も寄与する回転子巻線にのみ前記回転整流器の出力
を接続し、他の回転子巻線をダンパ巻線とした円筒型同
期発電機により、前記課題を解決するための手段とし
た。
According to the first aspect of the present invention, the main power generation winding and a plurality of rotor windings distributed in a concentrated winding and short-circuited by a rectifier are distributed and wound. A cylindrical field that magnetically couples with the generator winding, a stator field winding, a rotor excitation winding that magnetically couples with the stator field winding,
And a rotary rectifier configured to convert the power output of the rotor excitation winding to DC. The output of the rotary rectifier is connected only to the rotor winding that most contributes to the field, and the other rotor winding is used as a means for solving the problem by a cylindrical synchronous generator having a damper winding. .

【0011】つまり、全節集中巻にして整流器で短絡し
た複数個の分布した回転子巻線を巻装し、該複数個の回
転子巻線のうち主発電巻線の極数の主界磁に最も寄与す
る回転子巻線にのみ前記回転整流器の出力を接続したこ
とにより、従来の発電機のように逆相分電流の大きさに
単相負荷が制限されることはなく、単相負荷やインバ−
タ等の高調波を発生する負荷も、従来の発電機に比べて
より多く負荷し得るものである。しかも負荷時には主界
磁巻線およびダンパ巻線にダイオ−ドによる半波整流電
流が流れてその直流分が界磁を増磁させるので、AVR
による励磁電力が減少し、損失が少なくなる。
That is, a plurality of distributed rotor windings short-circuited by a rectifier in a concentrated winding of all sections are wound, and a main field of the number of poles of a main power generation winding among the plurality of rotor windings is wound. By connecting the output of the rotary rectifier only to the rotor winding that contributes the most, the single-phase load is not limited to the magnitude of the negative-sequence component current as in the conventional generator. And Invar
Also, a load that generates harmonics, such as power, can be loaded more than a conventional generator. In addition, when a load is applied, a half-wave rectified current by a diode flows through the main field winding and the damper winding, and the DC component increases the field.
And the loss is reduced.

【0012】また、従来の発電装置に比較して、回転子
を円筒型にして大きな変更も必要としないので、従来の
発電機に容易に適用できるとともに、円筒型にすること
で主界磁巻線およびダンパ巻線が円周に均一に配置で
き、ダンパ効果を完全にするものである。
Further, as compared with the conventional power generator, the rotor is cylindrical, and no major change is required. Therefore, the rotor can be easily applied to the conventional generator, and the cylindrical type can be used for the field winding. The wire and the damper winding can be arranged uniformly around the circumference, and the damper effect is completed.

【0013】本発明の請求項2によると、主発電巻線と
該主発電巻線の極数の偶数倍の極数を有する固定子界磁
巻線とを巻装して固定子を構成し、前記固定子界磁巻線
と磁気的結合をなす回転子励磁巻線と、全節集中巻にし
て整流器で短絡して分布した複数個の回転子巻線とを巻
装してあると共に、前記回転子励磁巻線の起電力を直流
に変換する回転整流器を備え、前記複数個の回転子巻線
のうち主発電巻線の極数の主界磁に最も寄与する回転子
巻線にのみ前記回転整流器の出力を接続して回転子を構
成した円筒型同期発電機とした。
According to a second aspect of the present invention, a stator is formed by winding a main power generation winding and a stator field winding having an even number of poles of the main power generation winding. A rotor excitation winding magnetically coupled with the stator field winding, a plurality of rotor windings distributed and short-circuited by a rectifier in a concentrated winding of all nodes, A rotating rectifier that converts the electromotive force of the rotor excitation winding into direct current, and only the rotor winding that most contributes to the main field of the number of poles of the main generator winding among the plurality of rotor windings. The output of the rotary rectifier was connected to form a cylindrical synchronous generator having a rotor.

【0014】このように構成することにより、発電機を
1つの固定子に主発電巻線と固定子界磁巻線を巻装し、
1つの回転子に主界磁巻線と回転子励磁巻線を巻装した
構成にして、比較的小型の同期発電機に本発明が適用で
きるものである。
[0014] With this configuration, the generator is wound with the main generator winding and the stator field winding around one stator,
The present invention can be applied to a relatively small synchronous generator having a configuration in which a main field winding and a rotor excitation winding are wound around one rotor.

【0015】本発明の請求項3によると、主発電巻線か
らなる固定子と、全節集中巻にして整流器で短絡した複
数個の回転子巻線を分布して巻装してある円筒型回転子
と、から発電部を構成し、固定子界磁巻線からなる固定
子と、該固定子界磁巻線と磁気的結合をなす回転子励磁
巻線とから励磁部を構成した円筒型同期発電機とした。
According to a third aspect of the present invention, there is provided a cylindrical type in which a stator comprising a main power generation winding and a plurality of rotor windings distributed in a concentrated manner and short-circuited by a rectifier are wound around the stator. A cylindrical type in which a rotor and a power generating unit are configured, a stator including a stator field winding, and an exciting unit including a rotor exciting winding magnetically coupled to the stator field winding. A synchronous generator was used.

【0016】この構成により、比較的大型の発電機とし
て構成でき、同一回転軸上に主界磁巻線を巻装した回転
子と主発電巻線を巻装した固定子とにより発電部を、ま
たこの主界磁を励磁する回転子励磁巻線を巻装した励磁
機回転子と固定子界磁巻線のを巻装した固定子とにより
励磁部を構成して併設し、発電部の主界磁巻線と励磁部
の回転子励磁巻線とを回転整流器で接続したという従来
の大型発電機とほとんど変わらない構成であっても、従
来では十分ではなかった不平衡負荷や高調波を発生する
負荷への対応が十分できるできる発電機となった。
With this configuration, a relatively large generator can be configured, and a power generator is formed by a rotor having a main field winding wound on the same rotating shaft and a stator having a main power winding wound thereon. Further, an exciting unit is constituted by an exciter rotor around which a rotor exciting winding for exciting the main field is wound and a stator around which a stator field winding is wound. Even if the configuration is almost the same as a conventional large generator in which the field winding and the rotor excitation winding of the excitation unit are connected by a rotary rectifier, unbalanced loads and harmonics that were not sufficient in the past are generated. The generator is capable of responding to the changing load.

【0017】請求項4によると、回転整流器の出力を接
続した、主発電巻線の極数の主界磁に寄与する回転子巻
線は、回転子励磁巻線の出力特性に応じて、直列または
並列に接続することができるので、回転子励磁巻線の出
力特性に応じて、回転子巻線と回転子励磁巻線が自由に
結線できるので、回転子巻線に関係なく回転子励磁巻線
は有効に作用して発電機出力特性を低下させることがな
い。
According to the fourth aspect, the rotor winding connected to the output of the rotary rectifier and contributing to the main field of the number of poles of the main power generation winding is connected in series according to the output characteristics of the rotor excitation winding. Or, since they can be connected in parallel, the rotor winding and the rotor excitation winding can be freely connected according to the output characteristics of the rotor excitation winding, so that the rotor excitation winding is independent of the rotor winding. The wires work effectively and do not degrade the generator output characteristics.

【0018】[0018]

【発明の実施の形態】本発明の同期発電機1は一例とし
て三相仕様によるものを以下に示す。第1の実施例は図
1のように、固定子2に三相4極主発電巻線3と該主発
電巻線3の極数の偶数倍である8極の固定子界磁巻線4
が巻装されている。また回転子10には前記固定子界磁
巻線4と磁気的結合をなす三相8極の回転子励磁巻線5
を巻装すると共に、前記主発電巻線3と同一極数の複数
個の主界磁巻線7とダンパ巻線9を巻装してそれぞれの
巻線をダイオ−ド8で短絡してあり、更に前記回転子励
磁巻線5の起電力を直流に変換する回転整流器6を備え
ており、該回転整流器6の出力を回転子10の主界磁に
寄与する主界磁巻線7にのみ供与してある。ここで複数
個の主界磁巻線7とダンパ巻線9はすべて全節集中巻で
図2のように円筒型回転子に形成してある。ここで換言
すれば、回転子のスロットすべてに全節集中巻で複数個
の巻線を巻装し、その巻線を主磁界に寄与する(主磁界
とほぼ直角に巻装された)巻線として主界磁巻線7と
し、磁極の中心にある(主磁界とほぼ同じ方向に巻装さ
れた)ダンパ巻線9にわけて、主界磁巻線7には回転整
流器6の出力を供給するようにしてある。ここで全節集
中巻というのは、例えば主発電巻線3の極数を基本に、
回転子に巻装した主界磁巻線7とダンパ巻線9のコイル
ピッチを電気角πとすることを指している。なお前記固
定子界磁巻線4には任意の直流電源11が接続される。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A synchronous generator 1 according to the present invention will be described below by way of example with a three-phase specification. In the first embodiment, as shown in FIG. 1, a stator 2 has a three-phase four-pole main power generation winding 3 and an eight-pole stator field winding 4 which is an even multiple of the number of poles of the main power generation winding 3.
Is wound. The rotor 10 has a three-phase eight-pole rotor excitation winding 5 magnetically coupled to the stator field winding 4.
And a plurality of main field windings 7 and damper windings 9 having the same number of poles as the main power generation winding 3 are wound, and each of the windings is short-circuited by a diode 8. And a rotary rectifier 6 for converting the electromotive force of the rotor excitation winding 5 into a direct current. The output of the rotary rectifier 6 is applied only to the main field winding 7 that contributes to the main field of the rotor 10. Provided. Here, all of the plurality of main field windings 7 and damper windings 9 are formed in a cylindrical rotor as shown in FIG. In other words, a plurality of windings are wound around all the slots of the rotor by concentrated winding of all the sections, and the windings contribute to the main magnetic field (the windings are wound substantially perpendicular to the main magnetic field). The main field winding 7 is divided into a damper winding 9 (wound in the same direction as the main magnetic field) at the center of the magnetic pole, and the output of the rotary rectifier 6 is supplied to the main field winding 7. I have to do it. Here, the whole section concentrated winding means, for example, based on the number of poles of the main power generation winding 3,
This means that the coil pitch between the main field winding 7 and the damper winding 9 wound on the rotor is set to the electrical angle π. An arbitrary DC power supply 11 is connected to the stator field winding 4.

【0019】図2の例では、主界磁に寄与する主界磁巻
線7をW1 ,W2 ,W3 及びW4 とし、W5 とW6 をダ
ンパ巻線9として使用するものである。また前記W1 ,
W2,W3 及びW4 の接続は、W1 とW2 及びW3 とW4
をそれぞれ直列に接続すると共にそれらを並列に接続
して回転整流器6の出力を接続してある。これら直列や
並列の接続は本例に限定されるものではなく、回転子励
磁巻線5の出力特性に応じて接続形態は異なるものであ
る。
In the example shown in FIG. 2, the main field windings 7 that contribute to the main field are W1, W2, W3 and W4, and W5 and W6 are used as damper windings 9. W1,
W2, W3 and W4 are connected by W1 and W2 and W3 and W4.
Are connected in series with each other, and the outputs of the rotary rectifier 6 are connected by connecting them in parallel. These series and parallel connections are not limited to this example, and the connection form differs depending on the output characteristics of the rotor excitation winding 5.

【0020】また図3では回転子コアを平面に展開して
回転子の主界磁巻線7とダンパ巻線9及び回転子励磁巻
線5のそれぞれの巻線配列の一例を示している。図2を
参考に回転子24スロットの場合を例にしており、主界
磁巻線7を4スロットに配置し続いてダンパ巻線9を2
スロットに配置している。回転子励磁巻線5は三相8極
の場合を示しており、三相の各相を導体の形状を変えて
示している。なお本発明は単相でも実施可能であるた
め、図3に回転子態様が限定されることはない。
FIG. 3 shows an example of a winding arrangement of the main field winding 7, the damper winding 9, and the rotor excitation winding 5 of the rotor by developing the rotor core in a plane. Referring to FIG. 2, an example of a rotor having 24 slots is shown, in which the main field winding 7 is arranged in 4 slots, and then the damper winding 9 is connected to 2 slots.
Placed in slots. The case where the rotor excitation winding 5 has three phases and eight poles is shown, and each of the three phases is shown by changing the shape of the conductor. Note that the present invention can be implemented with a single phase, so that the rotor mode is not limited to FIG.

【0021】[0021]

【実施例】次に正常な三相平衡負荷時の運転状況を図1
により説明する。原動機(図示せず)で回転子を回転さ
せ固定子界磁巻線4に直流電源11を接続して直流電流
を流すと、固定子及び回転子鉄心に8極の磁界が形成さ
れ、回転子励磁巻線5に起電力が生じて補償電流が流
れ、回転整流器6によって直流に変換され、主界磁巻線
7に直流電流が流れて4極の界磁磁束を生じ、それによ
って主発電巻線3に起電力が生じて負荷12に電力を供
給するものとなる。
FIG. 1 shows an operation state under a normal three-phase balanced load.
This will be described below. When a rotor is rotated by a prime mover (not shown) and a DC power supply 11 is connected to the stator field winding 4 to flow a DC current, an 8-pole magnetic field is formed on the stator and the rotor core, and the rotor is rotated. An electromotive force is generated in the exciting winding 5 and a compensating current flows, and is converted into DC by the rotary rectifier 6, and a DC current flows in the main field winding 7 to generate a four-pole field magnetic flux, thereby generating a main power generating winding. An electromotive force is generated in the line 3 to supply power to the load 12.

【0022】ここで固定子界磁巻線4によって形成され
る8極の磁界によって主界磁巻線7及びダンパ巻線9を
短絡しているダイオ−ド8に電流が流れないことを証明
する。つまり図4に示すように、固定子界磁巻線4によ
って形成される8極の静止磁界の基本波に、回転子10
に巻装された4極の主界磁巻線7及びダンパ巻線9が回
転により鎖交すると、巻線の導体部にe1 ,e2 ,e3
及びe4 の電圧が誘起するが、その総和すなわちダイオ
−ド8に架かる電圧Vは(1)式のように零となる。
Here, it is proved that no current flows through the diode 8 which short-circuits the main field winding 7 and the damper winding 9 by the eight-pole magnetic field formed by the stator field winding 4. . That is, as shown in FIG. 4, the fundamental wave of the eight-pole static magnetic field formed by the stator field winding 4 is added to the rotor 10.
When the four-pole main field winding 7 and the damper winding 9 wound on each other are linked by rotation, e1, e2, e3 are added to the conductors of the windings.
And the voltage of e4 is induced, and the sum of the voltages, that is, the voltage V applied to the diode 8, becomes zero as shown in the equation (1).

【0023】[0023]

【数1】 従ってダイオ−ド8は点弧せず、本発明の発電機は従来
の発電機と同様に動作することになる。なお固定子界磁
巻線4と回転子励磁巻線5は従来の励磁機と同様の電力
増幅作用があるのでAVR(自動電圧調整装置)の容量
を小さくできる利点がある。
(Equation 1) Accordingly, the diode 8 does not fire and the generator of the present invention operates similarly to a conventional generator. Since the stator field winding 4 and the rotor excitation winding 5 have the same power amplifying action as the conventional exciter, there is an advantage that the capacity of the AVR (automatic voltage regulator) can be reduced.

【0024】次に単相負荷が三相負荷に混在して三相不
平衡負荷になった場合の本発明による発電機の作用効果
を説明する。つまり、発電機1に三相不平衡負荷がかか
ると主発電巻線3に逆相電流が流れる。この逆相電流に
よって主発電巻線3は4極の逆相回転磁界を作り、この
逆相回転磁界は回転子10の回転方向とは逆方向に回転
するので回転子10に巻装してある主界磁巻線7とダン
パ巻線9に電圧を誘起する。この誘起電圧に対してダイ
オ−ド8がどのように作用するかを説明する。
Next, the operation and effect of the generator according to the present invention when a single-phase load is mixed with a three-phase load and becomes a three-phase unbalanced load will be described. That is, when a three-phase unbalanced load is applied to the generator 1, a negative-phase current flows through the main generator winding 3. Due to the negative phase current, the main power generation winding 3 generates a four-pole negative phase rotating magnetic field, which is wound around the rotor 10 because the negative phase rotating magnetic field rotates in a direction opposite to the rotating direction of the rotor 10. A voltage is induced in the main field winding 7 and the damper winding 9. How the diode 8 acts on this induced voltage will be described.

【0025】図5に示すように、回転子10に巻装され
た4極の主界磁巻線7及びダンパ巻線9が逆相回転磁界
と鎖交するとその巻線の導体部にe1 ,e2 ,e3 及び
e4の電圧が誘起し、その総和すなわちダイオ−ド8に
かかる電圧Vは(2)式のように4E’となる。従って
この4E’の電圧によってダイオ−ド8を通じて巻線に
半波整流電流が流れる。
As shown in FIG. 5, when the four-pole main field winding 7 and the damper winding 9 wound around the rotor 10 interlink with the anti-phase rotating magnetic field, e1,, The voltages of e2, e3 and e4 are induced, and the sum of them, that is, the voltage V applied to the diode 8 becomes 4E 'as shown in the equation (2). Therefore, a half-wave rectified current flows through the winding through the diode 8 by the voltage of 4E '.

【0026】[0026]

【数2】 この半波整流電流は直流分と交流分に分解でき、直流分
は回転整流器6の直流出力電流に重畳されて、界磁電流
が増加するように作用するこの現象をさらに詳細に説明
する。図6(a)に示すように回転整流器6の直流出力
電流I1 は主界磁巻線7のWを通じて流れ、ダイオ−ド
8には逆極性になるので流れない。また逆相回転磁界に
よって主界磁巻線7のWに誘起した交流電圧eによるダ
イオ−ド8を通じて流れる半波整流電流中の直流分I2
は、ダイオ−ド8の極性によって図6(b)のように流
れる。従って図6(c)のようにI1 とI2 は重畳され
て(I1 +I2 )となり界磁電流が増加するように作用
する。
(Equation 2) This half-wave rectified current can be decomposed into a DC component and an AC component, and the DC component is superimposed on the DC output current of the rotary rectifier 6, and this phenomenon that acts to increase the field current will be described in further detail. As shown in FIG. 6 (a), the DC output current I1 of the rotary rectifier 6 flows through the W of the main field winding 7 and does not flow to the diode 8 because it has the opposite polarity. The DC component I2 in the half-wave rectified current flowing through the diode 8 due to the AC voltage e induced in the W of the main field winding 7 by the reversed-phase rotating magnetic field.
Flows according to the polarity of the diode 8 as shown in FIG. Therefore, as shown in FIG. 6 (c), I1 and I2 are superimposed to become (I1 + I2), which acts to increase the field current.

【0027】また、ダンパ巻線9に誘起した交流電圧e
によるダイオ−ド8を通じて流れる半波整流電流中の直
流分は、ダイオ−ド8の極性によって図6(b)のよう
に流れ、この直流電流によるダンパ巻線9の起磁力は図
7のように界磁束を増加させる作用を有する。なおダン
パ巻線9のダイオ−ド8による短絡は、界磁束の増加が
大きすぎて支障のある場合は、その一部または全てをダ
イオ−ド8を使用しない単なる短絡としてもよい。
The AC voltage e induced in the damper winding 9
The DC component in the half-wave rectified current flowing through the diode 8 flows as shown in FIG. 6B depending on the polarity of the diode 8, and the magnetomotive force of the damper winding 9 due to this DC current is as shown in FIG. Has the effect of increasing the field flux. If the increase of the field magnetic flux is too large to cause a short circuit in the damper winding 9 due to the diode 8, a part or all of the short circuit may be a simple short circuit without using the diode 8.

【0028】以上のように逆相電流が多くなると発電機
1の出力電圧が上昇する。しかし発電機電圧はAVRに
よって定格電圧に保持されるので、結果として固定子界
磁巻線4に流れる電流がAVRによって減少することに
なる。このことはAVRを介して供給される励磁電力が
減少することになり、発電機の損失を軽減し、効率をよ
くすることになる。
As described above, when the reverse phase current increases, the output voltage of the generator 1 increases. However, the generator voltage is maintained at the rated voltage by the AVR, and as a result, the current flowing through the stator field winding 4 is reduced by the AVR. This means that the excitation power supplied via the AVR is reduced, which reduces generator losses and improves efficiency.

【0029】他方、ダイオ−ド8による半波整流電流の
交流分は、主界磁巻線7とダンパ巻線9が多相に巻装さ
れているので、それらによって形成される磁束が逆相回
転磁界を打ち消すように作用することになる。すなわち
主界磁巻線7とダンパ巻線9がすべてダンパ作用をする
ことになる。このことは誘導電動機の原理と同様であ
る。以上要するに逆相回転磁界は主界磁巻線7とダンパ
巻線9にダイオ−ドの作用によって吸収されて界磁電流
に変換されることで増磁作用をすることになる。
On the other hand, since the alternating current component of the half-wave rectified current by the diode 8 has a multi-phase winding of the main field winding 7 and the damper winding 9, the magnetic flux formed by them is in the opposite phase. It will act to cancel the rotating magnetic field. That is, the main field winding 7 and the damper winding 9 all act as a damper. This is the same as the principle of the induction motor. In short, the reversed-phase rotating magnetic field is absorbed by the main field winding 7 and the damper winding 9 by the action of the diode and is converted into a field current, thereby performing a magnetizing action.

【0030】次にインバ−タのような高調波電流を含む
負荷が接続されたときの本発明の発電機の作用効果を説
明する。高調波電流によって主発電巻線3が作る磁界は
時間高調波であるから、図5におけるe1 ,e2 ,e3
及びe4 は次のようになる。
Next, the operation and effect of the generator of the present invention when a load including a harmonic current such as an inverter is connected will be described. Since the magnetic field generated by the main power generation winding 3 by the harmonic current is a time harmonic, e1, e2, e3 in FIG.
And e4 are as follows:

【0031】[0031]

【数3】 従ってダイオ−ドにかかる電圧Vは次式のようになる。(Equation 3) Therefore, the voltage V applied to the diode is as follows.

【0032】[0032]

【数4】 すなわち電圧Vの大きさは4E”であり、ダイオ−ド8
を通じて半波整流電流が流れる。従って主発電巻線3に
高調波電流が流れたときも、主界磁巻線7とダンパ巻線
9がダイオ−ド8によってダンパ作用と増磁作用をする
ことに変わりはない。
(Equation 4) That is, the magnitude of the voltage V is 4E "and the diode 8
Through which a half-wave rectified current flows. Therefore, even when a harmonic current flows in the main power generation winding 3, the diode 8 causes the main field winding 7 and the damper winding 9 to function as a damper and a magnetizer.

【0033】次に、第2の実施例として、大型の発電機
に本発明を適用した場合を図8に示す。なお説明におい
て、構成の大小に関わらず第1の実施例と同じ作用を有
する構成については同符号を付している。
Next, as a second embodiment, FIG. 8 shows a case where the present invention is applied to a large generator. In the description, the same reference numerals are given to components having the same operation as the first embodiment regardless of the size of the components.

【0034】符号14は発電部を示し、固定子側に三相
4極主発電巻線3が巻装され、回転子側には前記主発電
巻線3と同一極数の複数個の主界磁巻線7とダンパ巻線
9を巻装してそれぞれの巻線をダイオ−ド8で短絡して
ある。また符号15は励磁部を示し、固定子側には固定
子界磁巻線4が巻装され、また回転子側には前記固定子
界磁巻線4と磁気的結合をなす三相の回転子励磁巻線5
を巻装すると共に、前記回転子励磁巻線5の起電力を直
流に変換する回転整流器6を備えている。更に励磁部1
5の回転子側の回転整流器6の出力を、発電部14の回
転子側の主界磁に寄与する主界磁巻線7にのみ供与して
ある。
Reference numeral 14 denotes a power generation unit, in which a three-phase four-pole main power generation winding 3 is wound on the stator side, and a plurality of main fields having the same number of poles as the main power generation winding 3 are mounted on the rotor side. A magnetic winding 7 and a damper winding 9 are wound, and each winding is short-circuited by a diode 8. Reference numeral 15 denotes an excitation unit, on which a stator field winding 4 is wound on the stator side, and a three-phase rotation which magnetically couples with the stator field winding 4 on the rotor side. Child excitation winding 5
And a rotary rectifier 6 for converting the electromotive force of the rotor excitation winding 5 into DC. Excitation unit 1
5, the output of the rotary rectifier 6 on the rotor side is provided only to the main field winding 7 that contributes to the main field on the rotor side of the power generation unit 14.

【0035】ここで複数個の主界磁巻線7とダンパ巻線
9はすべて全節集中巻で図2のように円筒型回転子に形
成してある。ここで換言すれば、回転子のスロットすべ
てに全節集中巻で複数個の巻線を巻装し、その巻線を主
磁界に寄与する(主磁界とほぼ直角に巻装された)巻線
として主界磁巻線7とし、磁極の中心にある(主磁界と
ほぼ同じ方向に巻装された)ダンパ巻線9にわけて、主
界磁巻線7には回転整流器6の出力を供給するようにし
てある。ここで全節集中巻というのは、例えば主発電巻
線3の極数を基本に、回転子に巻装した主界磁巻線7と
ダンパ巻線9のコイルピッチを電気角πとすることを指
している。前記固定子界磁巻線4には任意の直流電源1
1が接続される。なお本実施例の場合、発電部14と励
磁部15の磁極数は相互に干渉せず、第1の実施例の主
界磁巻線と回転子励磁巻線との関係のように磁極数が限
定されることはない。
Here, the plurality of main field windings 7 and the damper windings 9 are all formed by concentrated winding of all sections to form a cylindrical rotor as shown in FIG. In other words, a plurality of windings are wound around all the slots of the rotor by concentrated winding of all the sections, and the windings contribute to the main magnetic field (the windings are wound substantially perpendicular to the main magnetic field). The main field winding 7 is divided into a damper winding 9 (wound in the same direction as the main magnetic field) at the center of the magnetic pole, and the output of the rotary rectifier 6 is supplied to the main field winding 7. I have to do it. Here, the whole-section concentrated winding means, for example, that the coil pitch of the main field winding 7 and the damper winding 9 wound on the rotor is an electrical angle π based on the number of poles of the main power generation winding 3. Pointing to. An arbitrary DC power source 1 is connected to the stator field winding 4.
1 is connected. In the case of the present embodiment, the number of magnetic poles of the power generation unit 14 and the exciting unit 15 does not interfere with each other, and the number of magnetic poles is different from the number of magnetic poles as in the relationship between the main field winding and the rotor exciting winding of the first embodiment. It is not limited.

【0036】以上のように構成した円筒型同期発電機の
本発明の作用は、第1の実施例と同様であり、従って小
出力から大出力の発電機において、本発明は適用するこ
とができるものであり、不平衡負荷や高調波を発生する
負荷に対して十分に適用範囲を拡大することができる。
The operation of the cylindrical synchronous generator constructed as described above according to the present invention is the same as that of the first embodiment. Therefore, the present invention can be applied to a generator having a small output to a large output. Therefore, the range of application can be sufficiently expanded for unbalanced loads and loads that generate harmonics.

【0037】[0037]

【発明の効果】以上のことから請求項1によると、本発
明の発電機は、従来の発電機のように逆相分電流の大き
さに単相負荷が制限されることはなく、単相負荷やイン
バ−タ等の高調波を発生する負荷も従来の発電機より多
く負荷し得るものである。しかも負荷時には主界磁巻線
およびダンパ巻線にダイオ−ドによる半波整流電流が流
れてその直流分が界磁を増磁させるので、AVRによる
励磁電力が減少し、損失が少なくなる。
As described above, according to the first aspect, the generator according to the present invention does not limit the single-phase load to the magnitude of the reverse-phase current as in the conventional generator. Loads that generate harmonics, such as loads and inverters, can also be loaded more than conventional generators. In addition, when a load is applied, a half-wave rectified current flows from the diode to the main field winding and the damper winding, and the DC component increases the field, so that the excitation power by the AVR is reduced and the loss is reduced.

【0038】請求項2によると、このように構成するこ
とにより、発電機を1つの固定子に主発電巻線と固定子
界磁巻線を巻装し、1つの回転子に主界磁巻線と回転子
励磁巻線を巻装した構成にして、比較的小型の同期発電
機に本発明が適用できるものである。
According to the second aspect of the present invention, the generator is wound with the main generator winding and the stator field winding around one stator, and the main field winding is wound around one rotor. The present invention can be applied to a relatively small synchronous generator having a configuration in which a wire and a rotor excitation winding are wound.

【0039】請求項3によると、この構成により、比較
的大型の発電機として構成でき、同一回転軸上に主界磁
巻線を巻装した回転子と主発電巻線を巻装した固定子と
により発電部を、またこの主界磁を励磁する回転子励磁
巻線を巻装した励磁機回転子と固定子界磁巻線を巻装し
た固定子とにより励磁部を構成して併設し、発電部の主
界磁巻線と励磁部の回転子励磁巻線とを回転整流器で接
続したという従来の大型発電機とほとんど変わらない構
成であっても、従来では十分ではなかった不平衡負荷や
高調波を発生する負荷への対応が十分できるできる発電
機となった。
According to the third aspect of the present invention, a relatively large generator can be configured by this configuration, and a rotor having a main field winding wound on the same rotating shaft and a stator having a main generator winding wound thereon. An exciter is constructed by an exciter rotor wound with a rotor exciting winding for exciting the main field and a stator wound with a stator field winding. The unbalanced load, which was not sufficient in the past, even though the configuration was almost the same as that of the conventional large generator in which the main field winding of the power generation unit and the rotor excitation winding of the excitation unit were connected by a rotary rectifier. And a generator that can sufficiently handle loads that generate high harmonics.

【0040】請求項4によると、回転子励磁巻線の出力
特性に応じて、回転子巻線と回転子励磁巻線が自由に結
線できるので、回転子巻線に関係なく回転子励磁巻線は
有効に作用して発電機出力特性を低下させることがな
い。
According to the fourth aspect, since the rotor winding and the rotor excitation winding can be freely connected in accordance with the output characteristics of the rotor excitation winding, the rotor excitation winding is independent of the rotor winding. Works effectively and does not lower the generator output characteristics.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明による同期発電機の回路図である。FIG. 1 is a circuit diagram of a synchronous generator according to the present invention.

【図2】複数の分布した回転子巻線を示した図である。FIG. 2 shows a plurality of distributed rotor windings.

【図3】回転子スロットを展開した図である。FIG. 3 is an expanded view of a rotor slot.

【図4】正常運転時における主界磁巻線およびダンパ巻
線の誘起電圧を示した図である。
FIG. 4 is a diagram showing induced voltages of a main field winding and a damper winding during normal operation.

【図5】不平衡負荷時における主界磁巻線及びダンパ巻
線の誘起電圧を示した図である。
FIG. 5 is a diagram showing induced voltages of a main field winding and a damper winding under an unbalanced load.

【図6】主界磁巻線及びダンパ巻線を短絡したダイオ−
ドの増磁作用を示した図である。
FIG. 6 shows a diode in which the main field winding and the damper winding are short-circuited.
FIG. 4 is a diagram showing the magnetizing action of

【図7】主界磁巻線及びダンパ巻線の起磁力分布を示し
た図である。
FIG. 7 is a diagram showing a magnetomotive force distribution of a main field winding and a damper winding.

【図8】本発明の別の実施例を示した図である。FIG. 8 is a diagram showing another embodiment of the present invention.

【図9】従来の同期発電機の回路図を示した図である。FIG. 9 is a diagram showing a circuit diagram of a conventional synchronous generator.

【符号の説明】[Explanation of symbols]

1 三相円筒型同期発電機 2 固定子 3 三相4極主発電巻線 4 固定子界磁巻線 5 回転子励磁巻線 6 回転整流器 7 主界磁巻線 8 ダイオ−ド 9 ダンパ巻線 10 回転子 11 直流電源 12 負荷 13 三相円筒型同期発電機 14 発電部 15 励磁部 20 固定子鉄心 21 固定子界磁巻線 22 回転子鉄心 23 回転子界磁巻線 24 回転子励磁巻線 25 三相全波整流器 26 ダイオ−ドブリッジ回路 DESCRIPTION OF SYMBOLS 1 Three-phase cylindrical synchronous generator 2 Stator 3 Three-phase four-pole main generator winding 4 Stator field winding 5 Rotor excitation winding 6 Rotary rectifier 7 Main field winding 8 Diode 9 Damper winding DESCRIPTION OF SYMBOLS 10 Rotor 11 DC power supply 12 Load 13 Three-phase cylindrical synchronous generator 14 Power generation part 15 Excitation part 20 Stator core 21 Stator field winding 22 Rotor core 23 Rotor field winding 24 Rotor excitation winding 25 Three-phase full-wave rectifier 26 Diode bridge circuit

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】主発電巻線と、全節集中巻にして整流器で
短絡した複数個の回転子巻線を分布して巻装し前記主発
電巻線と磁気的結合をなす円筒型界磁と、固定子界磁巻
線と、該固定子界磁巻線と磁気的結合をなす回転子励磁
巻線と、及び該回転子励磁巻線の発電出力を直流に変換
する回転整流器とから構成された円筒型同期発電機であ
って、前記複数個の回転子巻線のうち主発電巻線の極数
の主界磁に最も寄与する回転子巻線にのみ前記回転整流
器の出力を接続し、他の回転子巻線をダンパ巻線とした
ことを特徴とする円筒型同期発電機。
1. A cylindrical field which magnetically couples with a main power generation winding and a plurality of rotor windings distributed in a concentrated winding and short-circuited by a rectifier. A stator field winding, a rotor excitation winding magnetically coupled to the stator field winding, and a rotary rectifier for converting the power output of the rotor excitation winding to DC. The synchronous rectifier, wherein the output of the rotary rectifier is connected only to the rotor winding that most contributes to the main field of the number of poles of the main generator winding among the plurality of rotor windings. A cylindrical synchronous generator characterized in that another rotor winding is a damper winding.
【請求項2】主発電巻線と該主発電巻線の極数の偶数倍
の極数を有する固定子界磁巻線とを巻装して固定子を構
成し、 前記固定子界磁巻線と磁気的結合をなす回転子励磁巻線
と、全節集中巻にして整流器で短絡して分布した複数個
の回転子巻線とを巻装してあると共に、前記回転子励磁
巻線の起電力を直流に変換する回転整流器を備え、前記
複数個の回転子巻線のうち主発電巻線の極数の主界磁に
最も寄与する回転子巻線にのみ前記回転整流器の出力を
接続して回転子を構成したことを特徴とする請求項1記
載の円筒型同期発電機。
2. A stator is formed by winding a main generator winding and a stator field winding having an even number of poles of the main generator winding. A rotor excitation winding magnetically coupled to a wire, and a plurality of rotor windings distributed by short-circuiting with a rectifier in a concentrated winding of all sections are wound. A rotary rectifier for converting an electromotive force into direct current, and connecting an output of the rotary rectifier only to a rotor winding that most contributes to a main field of the number of poles of a main generator winding among the plurality of rotor windings. 2. The cylindrical synchronous generator according to claim 1, wherein the rotor is formed as a rotor.
【請求項3】主発電巻線からなる固定子と、全節集中巻
にして整流器で短絡した複数個の回転子巻線を分布して
巻装してある円筒型回転子と、から発電部を構成し、固
定子界磁巻線からなる固定子と、該固定子界磁巻線と磁
気的結合をなす回転子励磁巻線とから励磁部を構成した
ことを特徴とする請求項1記載の円筒型同期発電機。
3. A power generation unit comprising: a stator comprising a main power generation winding; and a cylindrical rotor in which a plurality of rotor windings distributed in a concentrated winding and short-circuited by a rectifier are wound. 2. An exciting unit comprising: a stator comprising a stator field winding; and a rotor excitation winding magnetically coupled to the stator field winding. Cylindrical synchronous generator.
【請求項4】回転整流器の出力を接続した、主発電巻線
の極数の主界磁に寄与する回転子巻線は、回転子励磁巻
線の出力特性に応じて、直列または並列に接続してなる
ことを特徴とする請求項2または3記載の円筒型同期発
電機。
4. A rotor winding connected to the output of the rotary rectifier and contributing to the main field of the number of poles of the main generator winding is connected in series or in parallel according to the output characteristics of the rotor excitation winding. The cylindrical synchronous generator according to claim 2 or 3, wherein:
JP22094297A 1997-07-31 1997-07-31 Cylindrical synchronous generator Expired - Fee Related JP3539148B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22094297A JP3539148B2 (en) 1997-07-31 1997-07-31 Cylindrical synchronous generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22094297A JP3539148B2 (en) 1997-07-31 1997-07-31 Cylindrical synchronous generator

Publications (2)

Publication Number Publication Date
JPH1155912A true JPH1155912A (en) 1999-02-26
JP3539148B2 JP3539148B2 (en) 2004-07-07

Family

ID=16758977

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22094297A Expired - Fee Related JP3539148B2 (en) 1997-07-31 1997-07-31 Cylindrical synchronous generator

Country Status (1)

Country Link
JP (1) JP3539148B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006057206A1 (en) * 2004-11-24 2006-06-01 Ntt Data Ex Techno Corporation Generator
WO2007010934A1 (en) * 2005-07-19 2007-01-25 Denso Corporation Ac motor and its control device
WO2013034313A3 (en) * 2011-09-08 2013-09-06 Theresia Heil-Ostovic Doubly excited synchronous machine

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006057206A1 (en) * 2004-11-24 2006-06-01 Ntt Data Ex Techno Corporation Generator
WO2007010934A1 (en) * 2005-07-19 2007-01-25 Denso Corporation Ac motor and its control device
WO2013034313A3 (en) * 2011-09-08 2013-09-06 Theresia Heil-Ostovic Doubly excited synchronous machine

Also Published As

Publication number Publication date
JP3539148B2 (en) 2004-07-07

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