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JP4601348B2 - Power generator for distributed power supply - Google Patents
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JP4601348B2 - Power generator for distributed power supply - Google Patents

Power generator for distributed power supply Download PDF

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JP4601348B2
JP4601348B2 JP2004211613A JP2004211613A JP4601348B2 JP 4601348 B2 JP4601348 B2 JP 4601348B2 JP 2004211613 A JP2004211613 A JP 2004211613A JP 2004211613 A JP2004211613 A JP 2004211613A JP 4601348 B2 JP4601348 B2 JP 4601348B2
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generator
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JP2006034038A (en
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剛 塩田
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Toyo Electric Manufacturing Ltd
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Description

本発明は、風車又は水車により駆動される発電機から、風速又は流速に関わらず、風又は水より得られる概略の最大出力を取り出すための分散電源用発電装置に関するものである。   The present invention relates to a power generator for a distributed power source for extracting an approximate maximum output obtained from wind or water, regardless of wind speed or flow velocity, from a generator driven by a wind turbine or water turbine.

本出願人は先に、風車又は水車に接続された永久磁石型発電機より、PWMコンバータを用いずに交流を直流に変換して概略の最大出力を取り出すために、永久磁石型発電機の異なる大きさの誘起電圧を発生する複数の巻線の出力端子にリアクトルを経て直列に整流器を接続し、この整流器の直流出力を並列接続して外部に出力する分散電源用発電装置について提案している(例えば、特許文献1参照。)。   In order to obtain an approximate maximum output from a permanent magnet generator connected to a windmill or a water turbine without using a PWM converter, the present applicant firstly uses a different permanent magnet generator. We have proposed a power generator for distributed power supply that connects a rectifier in series via a reactor to the output terminals of a plurality of windings that generate an induced voltage of magnitude, and outputs the DC output of this rectifier in parallel and outputs it to the outside. (For example, refer to Patent Document 1).

かかる先願技術を、図9の風車に接続された小型風力発電装置を示す主回路単線結線図を参照して詳述する。
図9において、1は風車、2は先願技術の小型風力発電装置、3は永久磁石型発電機、4〜6は第1〜第3のリアクトル、7〜9は第1〜第3の整流器、10は正側出力端子、11は負側出力端子、12はバッテリーである。
The prior application technique will be described in detail with reference to a main circuit single line connection diagram showing a small wind power generator connected to the wind turbine of FIG.
In FIG. 9, 1 is a windmill, 2 is a small wind power generator of the prior application, 3 is a permanent magnet generator, 4 to 6 are first to third reactors, and 7 to 9 are first to third rectifiers. 10 is a positive output terminal, 11 is a negative output terminal, and 12 is a battery.

この永久磁石型発電機3は、絶縁され、かつ誘起電圧の大きさの異なる3巻線を有し、3巻線の中の巻数が一番少ないために一番誘起電圧の低い第1の巻線W1は、第1のリアクトル4に接続され、さらに第1の整流器7に接続される。
次に巻数が多い第2の巻線W2は、第2のリアクトル5に接続され、さらに第2の整流器8に接続される。
又、巻数が一番多いために一番誘起電圧の高い第3の巻線W3は、第3のリアクトル6に接続され、さらに第3の整流器9に接続される。
上記第1〜第3の整流器7〜9の各直流側は、正側出力端子10及び負側出力端子11に並列接続され、各巻線の合計出力がバッテリー12に接続される。
The permanent magnet generator 3 has three windings that are insulated and have different induced voltage levels. Since the number of turns in the three windings is the smallest, the first winding having the lowest induced voltage is used. The line W1 is connected to the first reactor 4 and further connected to the first rectifier 7.
Next, the second winding W <b> 2 with the largest number of turns is connected to the second reactor 5 and further connected to the second rectifier 8.
The third winding W3 having the highest induced voltage due to the largest number of turns is connected to the third reactor 6 and further to the third rectifier 9.
The direct current sides of the first to third rectifiers 7 to 9 are connected in parallel to the positive output terminal 10 and the negative output terminal 11, and the total output of each winding is connected to the battery 12.

このように構成される分散電源用発電装置2より、概略の風車最大出力を得る方法を以下に示す。
図8は、風速をパラメータとした時の、風車の回転数対出力特性の概要を説明した図である。
風車は、風車の形状及び風速Uが決まると、風車回転数Nに対する風車出力Pが一義的に定まり、例えば風速Ux及びUyに対する風車出力Pは、それぞれ図8の実線で示される。そして、種々の風速に対する風車出力Pのピークは、図8の一点鎖線で示す最大出力曲線のようになる。
すなわち、図8の風車の回転数対出力特性において、風速がUxの時は、風速Uxの風車出力曲線と最大出力曲線との交点Sxに示すように、風車回転数Nxにおいて、風車最大出力Pxとなる。
又、風速がUyの時は、風車回転数Nyにおいて、風速Uyでの風車最大出力Pyとなる。
A method of obtaining a rough maximum wind turbine output from the power generator 2 for distributed power supply configured as described above will be described below.
FIG. 8 is a diagram for explaining the outline of the rotational speed versus the output characteristic of the windmill when the wind speed is used as a parameter.
When the shape of the windmill and the wind speed U are determined, the windmill output P with respect to the windmill rotation speed N is uniquely determined. For example, the windmill output P with respect to the wind speeds Ux and Uy is indicated by a solid line in FIG. And the peak of the windmill output P with respect to various wind speeds becomes like the maximum output curve shown with the dashed-dotted line of FIG.
That is, when the wind speed is Ux in the rotational speed vs. output characteristics of the windmill in FIG. 8, the maximum windmill output Px at the windmill rotational speed Nx as indicated by the intersection Sx between the windmill output curve of the wind speed Ux and the maximum output curve. It becomes.
When the wind speed is Uy, the windmill maximum output Py at the wind speed Uy is obtained at the windmill rotational speed Ny.

すなわち、図8の最大出力曲線を見方を変えて見ると、風から最大出力を得るためには、風車回転数Nが決まると、その時の永久磁石型発電機の出力Pを一義的に、最大出力曲線上の値に定めれば良いことを表している。   In other words, looking at the maximum output curve in FIG. 8 in order to obtain the maximum output from the wind, when the wind turbine rotation speed N is determined, the output P of the permanent magnet generator at that time is uniquely determined to be the maximum. This indicates that the value on the output curve may be determined.

図7は、先願技術が対象とする分散電源用発電装置2の直流出力をバッテリー等の定電圧源に接続した場合の説明図であり、小型風力発電装置2の永久磁石型発電機内3の第1〜第3の巻線W1〜W3の各出力は、各巻線の誘起電圧値の違い、及び各巻線内部インダクタンスと各巻線出力に接続されるリアクトルによる電圧降下のために、図7の各巻線による風車の回転数対出力特性に示すP1〜P3のようになる。   FIG. 7 is an explanatory diagram in the case where the direct current output of the distributed power generator 2 targeted by the prior application technology is connected to a constant voltage source such as a battery, in the permanent magnet generator 3 of the small wind power generator 2. Each output of the first to third windings W1 to W3 is different from each other in FIG. 7 due to the difference in the induced voltage value of each winding and the voltage drop due to the internal inductance of each winding and the reactor connected to each winding output. It becomes like P1-P3 shown to the rotation speed versus output characteristic of the windmill by a line.

すなわち、風車回転数Nが低い場合には、第3の巻線W3の発生電圧V3がバッテリー電圧Vbより低いために、バッテリーには充電されない。しかし、風車回転数Nが上昇して、N3付近になると、電流が流れ始めて、風車回転数NがN3になると、第3の巻線W3の出力P3はP31となる。これ以上に風車回転数Nが上昇して誘起電圧が上昇しても、バッテリー電圧Vbは、ほぼ一定であり、第3の巻線W3および第3のリアクトルのインダクタンス等によるインピーダンスが周波数に比例するために、出力P3はP31よりも漸増するに留まる。
第2の巻線W2については、さらに回転数Nが上昇することにより誘起電圧が上昇して出力が取れ始めるが、内部インダクタンス等が小さいために大きな出力が取れる。第1の巻線W1については、さらに回転数Nが上昇したときに、さらに大きな出力が取れる。
That is, when the wind turbine rotation speed N is low, the voltage V3 generated by the third winding W3 is lower than the battery voltage Vb, so that the battery is not charged. However, when the wind turbine rotational speed N rises and approaches N3, current starts to flow, and when the wind turbine rotational speed N reaches N3, the output P3 of the third winding W3 becomes P31. Even if the wind turbine speed N increases further and the induced voltage rises, the battery voltage Vb is substantially constant, and the impedance due to the inductance of the third winding W3 and the third reactor is proportional to the frequency. Therefore, the output P3 only increases gradually from P31.
As for the second winding W2, the induced voltage rises as the rotational speed N further rises, and an output begins to be obtained. However, since the internal inductance and the like are small, a large output can be obtained. With respect to the first winding W1, a larger output can be obtained when the rotational speed N further increases.

このように構成される分散電源用発電装置2のバッテリー12等の定電圧源への出力は、第1〜第3の巻線の出力P1〜P3を加算して得られる合計出力と同じであり、図6の点線で示す近似出力曲線で表される。従って、図6に示すように、この合計出力は図6の実線で示す最大出力曲線の近似を実現している。
特開2004−64928号(図1)
The output to the constant voltage source such as the battery 12 of the power generator 2 for the distributed power source configured as described above is the same as the total output obtained by adding the outputs P1 to P3 of the first to third windings. This is represented by an approximate output curve indicated by a dotted line in FIG. Therefore, as shown in FIG. 6, this total output realizes an approximation of the maximum output curve shown by the solid line in FIG.
JP 2004-64928 A (FIG. 1)

解決しようとする問題点は、上記のように3種類の巻線と3種類のリアクトルにより構成される小型風力発電装置2においては、多くのリアクトルが必要であり、永久磁石型発電機3内の巻線構成が複雑なので製作工数も多くなり、高価になるという点である。 The problem to be solved is that in the small wind power generator 2 composed of three types of windings and three types of reactors as described above, a large number of reactors are necessary. Since the winding configuration is complicated, the number of manufacturing steps is increased and the cost is increased.

本発明は上記事情に鑑みなされたものであって、風車又は水車より概略の最大出力を得るために、永久磁石型発電機内3内の巻線の種類を減らし、外部に接続するリアクトルを飽和リアクトルにより構成することを特徴とする分散電源用発電装置である。   The present invention has been made in view of the above circumstances, and in order to obtain an approximate maximum output from a wind turbine or a water turbine, the types of windings in the permanent magnet generator 3 are reduced, and the reactor connected to the outside is a saturated reactor. It is comprised by these, It is the electric power generating apparatus for distributed power supplies characterized by the above-mentioned.

本発明の分散電源用発電装置2は、永久磁石型発電機内3内の巻線の種類およびリアクトルが減少したために、製作工数が少なくなり、価格を下げることができる。   The power generator 2 for a distributed power source according to the present invention can reduce the number of manufacturing steps and reduce the price because the types of windings and reactors in the permanent magnet generator 3 are reduced.

永久磁石型発電機内3内の巻線を誘起電圧の大きさの異なる2種類の巻線とし、該2種類の巻線に接続されるリアクトルの内、誘起電圧の大きさが低い巻線に接続されるリアクトルを、飽和リアクトルにすることにより構成した。   The winding in the permanent magnet generator 3 is made of two types of windings with different induced voltages, and the reactor connected to the two types of windings is connected to the winding with the lower induced voltage. The reactor to be made was constituted by making it a saturated reactor.

図1は、本発明を風車に適用した場合であり、風車により駆動される分散電源用発電装置の主回路単線結線図である。
同図において、2は分散電源用発電装置、3は永久磁石型発電機、13は飽和リアクトル、5は第2のリアクトル、7、8は第1、第2の整流器、10は正側出力端子、11は負側出力端子であり、図9と同一番号は同一構成部品を表す。
以下、図1について説明する。
FIG. 1 shows a case where the present invention is applied to a windmill, and is a main circuit single line connection diagram of a power generator for a distributed power source driven by the windmill.
In the figure, 2 is a generator for a distributed power source, 3 is a permanent magnet generator, 13 is a saturated reactor, 5 is a second reactor, 7 and 8 are first and second rectifiers, and 10 is a positive output terminal. , 11 are negative output terminals, and the same numbers as those in FIG. 9 represent the same components.
Hereinafter, FIG. 1 will be described.

本発明の分散電源用発電装置2を構成する永久磁石型発電機は、絶縁された巻数の異なる2巻線を有し、2巻線の中の誘起電圧の大きさが低い巻線W1は、飽和リアクトル13に接続され、さらに第1の整流器7に接続される。
誘起電圧の大きさが高い巻線W2は、第2のリアクトル5に接続され、さらに第2の整流器8に接続される。
上記第1、第2の整流器7、8の各々の直流側は、正側出力端子10及び負側出力端子11に接続され、さらにバッテリー12に接続される。
The permanent magnet generator constituting the power generator 2 for a distributed power source of the present invention has two insulated windings having different numbers of windings, and the winding W1 having a low induced voltage in the two windings is: It is connected to the saturation reactor 13 and further connected to the first rectifier 7.
The winding W <b> 2 having a high induced voltage is connected to the second reactor 5 and further connected to the second rectifier 8.
The DC side of each of the first and second rectifiers 7 and 8 is connected to the positive output terminal 10 and the negative output terminal 11 and further connected to the battery 12.

この飽和リアクトル13として、図5の飽和リアクトルの電流対インダクタンス特性に示すように、電流の増加によりリアクトルを構成する鉄心が飽和して、インダクタンス値が減少するような特性を有するものを用いる。すなわち、電流IxではインダクタンスLxであるが、それ以上の電流ではインダクタンスが減少する特性を有する。
このような飽和リアクトルは、鉄心、ギャップの寸法および巻数を最適にすることにより実現できる。
従って、図1の分散電源用発電装置2では、図9の分散電源用発電装置2の巻線W3およびリアクトル6を削除するために、巻線W1に接続される第1のリアクトル4を第1の飽和リアクトル13で構成している。
As the saturated reactor 13, as shown in the current vs. inductance characteristic of the saturated reactor in FIG. 5, the one having a characteristic that the iron core constituting the reactor is saturated due to an increase in current and the inductance value decreases is used. In other words, the current Ix is the inductance Lx, but the current decreases more than that.
Such a saturated reactor can be realized by optimizing the iron core, gap size and number of turns.
Accordingly, in the distributed power generation device 2 in FIG. 1, the first reactor 4 connected to the winding W1 is the first in order to delete the winding W3 and the reactor 6 of the distributed power generation device 2 in FIG. 9. The saturated reactor 13 is configured.

このように構成される分散電源用発電装置2より、種々の風速において、風車の形状より一義的に定まる最大出力を、近似的に取り出す方法を、図3の本発明の分散電源用発電装置の回転数対出力特性図、および図4の本発明の分散電源用発電装置の各巻線の回転数対出力特性図を参照して説明する。
図4の本発明の分散電源用発電装置の各巻線の回転数対出力特性図においては、図9におけるインダクタンス値が一定なリアクトルが接続される第1の巻線W1の出力と異なり、インダクタンス値が電流の上昇とともに小さくなる第1の飽和リアクトル13が接続された巻線W1の出力P1は回転数の上昇とともに、より右上がりのカーブで上昇する。
この巻線W1の出力特性は、回転数、誘起電圧、電流値によって変化しない永久磁石型発電機3内の巻線W1の内部インダクタンス値、および第1の飽和リアクトル13のインダクタンス値に依存する。
A method of approximating the maximum output uniquely determined from the shape of the windmill at various wind speeds from the distributed power generator 2 configured as described above is shown in FIG. A description will be given with reference to the rotational speed versus output characteristic diagram and the rotational speed versus output characteristic diagram of each winding of the power generator for the distributed power source of the present invention in FIG.
In the rotational speed versus output characteristics diagram of each winding of the power generator for a distributed power source of FIG. 4, the inductance value differs from the output of the first winding W1 to which the reactor having a constant inductance value in FIG. 9 is connected. The output P1 of the winding W1 to which the first saturation reactor 13 that becomes smaller as the current increases is connected and rises with a curve that rises to the right as the rotational speed increases.
The output characteristics of the winding W1 depend on the internal inductance value of the winding W1 in the permanent magnet generator 3 and the inductance value of the first saturation reactor 13, which do not vary with the rotational speed, the induced voltage, and the current value.

このように構成される分散電源用風力発電装置2のバッテリー12等の定電圧源への出力は、巻線W1、W2の出力P1、P2を加算して得られる合計出力と同じであり、図3の点線で示す近似出力曲線で表される。従って、図3に示すように、この合計出力は実線で示す最大出力曲線の近似を実現している。   The output to the constant voltage source such as the battery 12 of the wind turbine generator 2 for the distributed power source configured as described above is the same as the total output obtained by adding the outputs P1 and P2 of the windings W1 and W2. It is represented by an approximate output curve indicated by a dotted line 3. Therefore, as shown in FIG. 3, this total output realizes an approximation of a maximum output curve indicated by a solid line.

本発明において、図3で示す近似出力曲線を、より最大出力曲線に近づけて、風からのエネルギーを可能な限り取り出すためには、本発明の永久磁石型発電機3の各巻線W1、W2の誘起電圧値及び内部インダクタンス値と、第1の飽和リアクトル13及び第2のリアクトル5のインダクタンス値を加減する事により可能である。
すなわち、図3で示す最大出力曲線は、風車回転数に対して3次曲線であるが、複数の各巻線の内部インダクタンスとリアクトルによる電圧降下は、風車回転数に比例する。又、複数の各巻線の誘起電圧は巻数に比例するが、内部インダクタンスは巻数の2乗に比例すること等を考慮して、設計される。
In the present invention, the approximate output curve shown in FIG. 3 is made closer to the maximum output curve, and in order to extract the energy from the wind as much as possible, each winding W1, W2 of the permanent magnet generator 3 of the present invention is used. This is possible by adjusting the induced voltage value and the internal inductance value and the inductance values of the first saturated reactor 13 and the second reactor 5.
That is, the maximum output curve shown in FIG. 3 is a cubic curve with respect to the wind turbine speed, but the internal inductance of each of the plurality of windings and the voltage drop due to the reactor are proportional to the wind turbine speed. The induced voltage of each of the plurality of windings is proportional to the number of turns, but the internal inductance is designed in consideration of the fact that it is proportional to the square of the number of turns.

以上、本発明の実施例では、分散電源用発電装置2を構成する永久磁石型発電機3は、異なる誘起電圧及び出力を発生するために、各巻線は異なる巻数で構成されると共に、大きな電流の流れる巻線W1の断面積は巻線W2の断面積より大きく構成される。
又、永久磁石型発電機3は、絶対値の異なる誘起電圧及び出力を発生するように、内部巻線を構成すれば良く、必ずしも、同一の固定子スロットに、巻数の異なる巻線を納める必要は無い。
さらに、本発明の分散電源用発電装置2は、3相に限らず、他の相数でも可能である。
As described above, in the embodiment of the present invention, the permanent magnet generator 3 that constitutes the power generator 2 for the distributed power source generates different induced voltages and outputs. The cross-sectional area of the winding W1 through which the current flows is larger than the cross-sectional area of the winding W2.
In addition, the permanent magnet generator 3 only needs to be configured with internal windings so as to generate induced voltages and outputs having different absolute values, and the windings having different numbers of windings are necessarily placed in the same stator slot. There is no.
Furthermore, the power generator 2 for a distributed power source according to the present invention is not limited to three phases, but can be any number of phases.

又、本発明の分散電源用発電装置から、バッテリー12等の定電圧源へ充電する場合について説明したが、充電により直流電圧が上昇するような場合には、上昇した直流電圧に充電しようとするために、図3の分散電源用発電装置の近似出力曲線は最大出力曲線から右側に乖離して、出力が減少する。これは、バッテリー12等の定電圧源への充電が、風力発電により十分に行われた結果の電圧上昇であり、バッテリー12等の定電圧源を含めたシステム全体として、何ら不具合となるものでは無い。さらに電圧上昇するようなシステムにおいては、バッテリー12等の定電圧源を切り離すか、風車を停止すれば良い。
さらに、充電電流の大きさにより直流電圧が変化するような場合には、分散電源用発電装置の近似出力曲線を最大出力曲線に、最も近づけるように巻数、飽和リアクトルを設計すれば良い。
Further, the case of charging a constant voltage source such as the battery 12 from the power generator for the distributed power source according to the present invention has been described. However, when the DC voltage rises due to charging, it tries to charge the increased DC voltage. For this reason, the approximate output curve of the distributed power generation device of FIG. 3 deviates to the right from the maximum output curve, and the output decreases. This is a voltage increase as a result of sufficiently charging the constant voltage source such as the battery 12 by wind power generation, and there is no problem with the entire system including the constant voltage source such as the battery 12. No. In a system that further increases the voltage, a constant voltage source such as the battery 12 may be disconnected or the windmill may be stopped.
Furthermore, when the DC voltage changes depending on the magnitude of the charging current, the number of turns and the saturation reactor may be designed so that the approximate output curve of the power generator for distributed power supply is closest to the maximum output curve.

図2に本発明の第2の実施例を示す。
図において、分散電源用発電装置2は、永久磁石型発電機3、第1および第2の飽和リアクトル13および14、第1および第2の整流器7および8、バッテリー12により構成され、図1と同一番号は同一構成部品を表す
本発明の第1の実施例では、第1の巻線W1に接続されるリアクトルを飽和リアクトルで構成するとして説明したが、本発明の第2の実施例では、第2の巻線W2に接続されるリアクトルも飽和リアクトルとしたものである。
すなわち、回転数の上昇とともに、図4の出力P2を上昇させる構成とすることにより、図3の分散電源用発電装置2の近似出力曲線を、より最大出力曲線に近づける構成としたものである。
FIG. 2 shows a second embodiment of the present invention.
In the figure, the distributed power generator 2 is composed of a permanent magnet generator 3, first and second saturated reactors 13 and 14, first and second rectifiers 7 and 8, and a battery 12. The same number represents the same component In the first embodiment of the present invention, the reactor connected to the first winding W1 is described as being constituted by a saturated reactor, but in the second embodiment of the present invention, The reactor connected to the second winding W2 is also a saturated reactor.
That is, the configuration in which the output P2 in FIG. 4 is increased with the increase in the rotational speed is such that the approximate output curve of the distributed power generation device 2 in FIG. 3 is made closer to the maximum output curve.

本発明の分散電源用発電装置2によれば、風速計や高価なPWMコンバータが不要であり、さらに永久磁石型発電機内3内の巻線の種類およびリアクトルを減少させたために、安価に構成することができ、前記PWMコンバータでは必要となる待機電力が不要になるので、年間を通した発電量を増加させる事ができ、実用上おおいに有用である。
ここでリアクトルおよび飽和リアクトルにはタップを設けて、微調整が可能な構正とすることにより、近似出力曲線を、より最大出力曲線に近づけて、風からのエネルギーを可能な限り取り出すことができる。
上記は、風力により説明したが、例えば、水力のように水車の形状が定まれば、最大出力を取り出すときの回転数対出力特性が一義的に定まるような用途にも適用可能である。
According to the distributed power generator 2 of the present invention, an anemometer or an expensive PWM converter is not required, and the number of windings and reactors in the permanent magnet generator 3 are reduced, so that the configuration is inexpensive. In addition, since the standby power required in the PWM converter is not necessary, the amount of power generation throughout the year can be increased, which is very useful in practice.
Here, the reactor and the saturated reactor are provided with taps, so that fine adjustment is possible, so that the approximate output curve can be made closer to the maximum output curve and energy from the wind can be extracted as much as possible. .
The above has been described with reference to wind power. However, for example, if the shape of a water turbine is determined like hydraulic power, the present invention can also be applied to applications in which the rotational speed versus output characteristics when the maximum output is taken out are uniquely determined.

本発明の第1の実施例であり、風車に適用した分散電源用発電装置の主回路単線結線図である。BRIEF DESCRIPTION OF THE DRAWINGS It is the 1st Example of this invention, and is the main circuit single wire connection diagram of the generator device for distributed power supplies applied to the windmill. 本発明の第2の実施例であり、風車に適用した分散電源用発電装置の主回路単線結線図である。It is a 2nd Example of this invention, and is the main circuit single wire connection diagram of the generator device for distributed power supplies applied to the windmill. 本発明の第1の実施例における分散電源用発電装置の回転数対風車出力特性図である。It is a rotation speed versus windmill output characteristic figure of the power generator for distributed power in the 1st example of the present invention. 本発明の第1の実施例における分散電源用発電装置の各巻線の回転数対出力特性図である。It is a rotation speed versus output characteristic figure of each winding of the power generator for distributed power in the 1st example of the present invention. 飽和リアクトルのインダクタンスを説明するための図である。It is a figure for demonstrating the inductance of a saturation reactor. 従来の分散電源用発電装置の回転数対風車出力特性図である。It is a rotation speed vs. windmill output characteristic figure of the conventional power generator for distributed power supplies. 従来の分散電源用発電装置の各巻線の回転数対出力特性図である。It is a rotation speed versus output characteristic figure of each winding of the conventional power generator for distributed power supplies. 風速をパラメータとした時の、風車の回転数対出力特性の概要を説明する図である。It is a figure explaining the outline | summary of the rotation speed versus output characteristic of a windmill when a wind speed is made into a parameter. 従来の分散電源用発電装置の主回路単線結線図である。It is a main circuit single line connection diagram of the conventional power generator for distributed power supplies.

符号の説明Explanation of symbols

1 風車
2 分散電源用発電装置
3 永久磁石型発電機
4〜6 第1〜第3のリアクトル
7〜9 第1〜第3のダイオード整流器
10 正側出力端子
11 負側出力端子
12 バッテリー
13 第1の飽和リアクトル
14 第2の飽和リアクトル
DESCRIPTION OF SYMBOLS 1 Windmill 2 Distributed power generator 3 Permanent magnet type generators 4-6 First to third reactors 7-9 First to third diode rectifiers 10 Positive output terminal 11 Negative output terminal 12 Battery 13 First Saturating reactor 14 Second saturated reactor

Claims (2)

風車又は水車により駆動される永久磁石型発電機の交流出力を整流して直流出力する分散電源用発電装置において、前記永久磁石型発電機を誘起電圧の大きさの異なる2種類の巻線により構成し、該2種類の巻線の誘起電圧の大きさが低い巻線の交流出力は電流値がある一定値より大きくなるとインダクタンス値が次第に減少する特性を有する飽和リアクトルの直列接続を経て整流し、前記2種類の巻線の誘起電圧の大きさが高い巻線の交流出力は非飽和リアクトルの直列接続を経て整流し、各整流出力を並列接続することを特徴とする分散電源用発電装置。 In a distributed power generator for rectifying an alternating current output of a permanent magnet generator driven by a windmill or a water turbine and outputting the direct current, the permanent magnet generator is composed of two types of windings having different induced voltages. Then, the AC output of the winding having a low induced voltage of the two types of windings is rectified through a series connection of saturated reactors having a characteristic that the inductance value gradually decreases when the current value exceeds a certain value , An AC output of a winding having a high induced voltage of the two types of windings is rectified through a series connection of unsaturated reactors, and the rectified outputs are connected in parallel. 風車又は水車により駆動される永久磁石型発電機の交流出力を整流して直流出力する分散電源用発電装置において、前記永久磁石型発電機を誘起電圧の大きさの異なる2種類の巻線により構成し、該2種類の巻線の各交流出力は電流値がある一定値より大きくなるとインダクタンス値が次第に減少する特性を有する各飽和リアクトルの直列接続を経て整流し、各整流出力を並列接続することを特徴とする分散電源用発電装置。 In a distributed power generator for rectifying an alternating current output of a permanent magnet generator driven by a windmill or a water turbine and outputting the direct current, the permanent magnet generator is composed of two types of windings having different induced voltages. Then, the AC outputs of the two types of windings are rectified through series connection of saturated reactors having a characteristic that the inductance value gradually decreases when the current value exceeds a certain value , and the rectified outputs are connected in parallel. A power generator for a distributed power source.
JP2004211613A 2004-07-20 2004-07-20 Power generator for distributed power supply Expired - Fee Related JP4601348B2 (en)

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