JPS6367413B2 - - Google Patents
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- Publication number
- JPS6367413B2 JPS6367413B2 JP56076078A JP7607881A JPS6367413B2 JP S6367413 B2 JPS6367413 B2 JP S6367413B2 JP 56076078 A JP56076078 A JP 56076078A JP 7607881 A JP7607881 A JP 7607881A JP S6367413 B2 JPS6367413 B2 JP S6367413B2
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- JP
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- Prior art keywords
- converter
- pole
- power
- starting
- converters
- 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.)
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- Inverter Devices (AREA)
- Supply And Distribution Of Alternating Current (AREA)
- Direct Current Feeding And Distribution (AREA)
Description
【発明の詳細な説明】
本発明は、系統に接続された交直変換設備や原
子力発電所などと直結された交直変換設備におけ
る交直変換装置の起動方式に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for starting an AC/DC converter in an AC/DC converter that is connected to a grid or directly connected to a nuclear power plant or the like.
第1図は、原子力発電と直結した双極1回線の
直流送電の構成図を示す、第1図において、原子
炉1で発生した蒸気はタービン2へ送られ、その
タービン出力は発電機3、昇圧用変圧器4を介し
て、交流母線5に接続される。交流母線5は、変
換用変圧器6,7を介して順変換器8,9に接続
され、前記変換器8,9は原子力発電によつて得
られた交流電力を直流電力に変換し、前記変換さ
れた直流電力は更に逆変換器10,11により交
流電力に変換され負荷に供給される。12,1
3,14,15は平滑リアクトル、16,17は
本線、18は中性線である。尚、説明の便宜上、
順変換器8、本線16、逆変換器10、中性線1
8で構成された極をP1極、他の極をP2極と称す。 Figure 1 shows a configuration diagram of bipolar single-line DC power transmission directly connected to nuclear power generation. It is connected to an AC bus 5 via a transformer 4 . The AC bus 5 is connected to forward converters 8 and 9 via conversion transformers 6 and 7, and the converters 8 and 9 convert AC power obtained by nuclear power generation into DC power, and convert the AC power obtained by nuclear power generation into DC power. The converted DC power is further converted into AC power by inverters 10 and 11 and supplied to the load. 12,1
3, 14, and 15 are smooth reactors, 16, 17 are main lines, and 18 is a neutral line. For convenience of explanation,
Forward converter 8, main line 16, inverse converter 10, neutral line 1
The pole composed of 8 is called the P 1 pole, and the other poles are called the P 2 pole.
さて、一般的に変換器を起動する場合、系統へ
及ぼす影響を極力小さくする為に通常最小運転電
力値で起動する。第2図はその1例を示す。第2
図においては、起動時の直流は定格の10%であ
る。直流電流をあまり小さくすると電流が断続
し、変換器を構成しているサイリスタ素子にとつ
て好ましくない為に、通常は上記のごとく定格の
10%程度である。又、第2図における時点T1、
即ち送電電力が定格の10%に立上がる迄の時間は
通常200ms〜300msである。一方、原子力発電で
は、無負荷状態から定格負荷をとる場合、長時間
かけてゆつくりと行なう。第3図にその1例を示
す。即ち、起動当初は、発電機出力G1は、定格
の数%で、T1の時点は数10秒、T1からT2迄の時
間は10分程度、発電機出力G1から発電機出力G2
(通常、定格の数10%)迄立上げる時間、即ちT2
からT3迄の時間は約1日、発電機出力G2から定
格出力迄立上げる時間、即ちT4からT5迄の時間
は約1時間である。 Generally, when starting a converter, it is usually started at the minimum operating power value in order to minimize the influence on the grid. FIG. 2 shows one example. Second
In the figure, the DC at startup is 10% of the rated value. If the DC current is too small, the current will be intermittent, which is unfavorable for the thyristor elements that make up the converter.
It is about 10%. Also, time T 1 in FIG. 2,
That is, the time it takes for the transmitted power to rise to 10% of the rated power is usually 200ms to 300ms. On the other hand, in nuclear power generation, when the rated load is taken from a no-load state, it is done slowly over a long period of time. An example is shown in FIG. That is, at the beginning of startup, the generator output G 1 is a few percent of the rated value, the time of T 1 is several tens of seconds, the time from T 1 to T 2 is about 10 minutes, and the generator output G 1 is a few percent of the rated value. G 2
(usually 10% of the rating), i.e. T 2
The time from T 3 to T 3 is about one day, and the time from T 4 to T 5 , which is the time to start up the generator output from G 2 to the rated output, is about 1 hour.
以上説明したごとく、直流送電のような直流連
系の利点の一つは高速潮流制御にあるわけである
が、その利点が、第1図に示すような原子力発電
と直結したシステム構成では逆に欠点となり、起
動時においては両者間の制御は全く協調がとれな
い為に新しい起動方式が要望されている。 As explained above, one of the advantages of DC interconnection such as DC power transmission is high-speed power flow control, but this advantage is reversed in a system configuration directly connected to nuclear power generation as shown in Figure 1. This is a drawback, since the control between the two cannot be coordinated at all during startup, so a new startup method is required.
従つて、本発明の目的は、このような要望を満
たすべくなされたものであつて、原子力発電と直
流連系との協調を図つた直流連系設備、即ち変換
器の起動方式を提供することにある。 Therefore, an object of the present invention has been made to meet such demands, and is to provide a DC interconnection equipment, that is, a converter startup method that allows coordination between nuclear power generation and DC interconnection. It is in.
以下本発明の一実施例を図面を参照して説明す
る。 An embodiment of the present invention will be described below with reference to the drawings.
通常第1図に示すようなシステム構成では、高
信頼度、高稼動率を図る為に、各変換器8,9,
10,11の起動停止制御回路を含む制御回路は
独立しており、P1極とP2極は各々独立に運転で
きるようになつている。従つて、従来用いられて
いる起動方式によつて、P1極の変換器8は順変
換器として起動し、変換器10は逆変換器として
起動する。一方、P2極の変換器9は逆変換器と
して起動し、変換器11は、順変換器として起動
することは従来の起動方式で可能であり、何らむ
つかしいことはない。この時、P1極とP2極の運
転電力値は同じ値にする。 Normally, in a system configuration as shown in Fig. 1, each converter 8, 9,
The control circuits including the start/stop control circuits 10 and 11 are independent, and the P1 pole and P2 pole can each be operated independently. Accordingly, according to the conventional starting scheme, the P 1 -pole converter 8 is started as a forward converter and the converter 10 is started as an inverse converter. On the other hand, the P2 - pole converter 9 can be activated as an inverse converter, and the converter 11 can be activated as a forward converter using the conventional activation method, and there is no difficulty at all. At this time, the operating power value of P1 pole and P2 pole should be the same value.
次に作用について述べる。 Next, we will discuss the effect.
上述のごとく、P1極とP2極の運転電力値を同
じ値にして、ほぼ同時にP1極の変換器8、P2極
の変換器11を順変換器として起動すれば、(従
つて、P1極の変換器10及びP2極の変換器11
は逆変換器として起動することになる。)原子力
側から眺めた負荷は差し引き零となる。即ち、上
述した起動方式により、変換器を起動すれば原子
力発電の初負荷は零となる。このようにして変換
器を起動して、所定時間後に原子力側の発電電力
値に応じて、変換器の送電電力を増加させれば、
原子力側と協調のとれた運転が可能である。第4
図は、本発明の一実施例にもとづくタイムチヤー
トであり、本タイムチヤートにより、更に本発明
の作用を詳細に説明する。 As mentioned above, if the operating power values of P 1 pole and P 2 pole are set to the same value and P 1 pole converter 8 and P 2 pole converter 11 are started as forward converters at almost the same time, (therefore, , P 1- pole transducer 10 and P 2- pole transducer 11
will be activated as an inverse transformer. ) The load seen from the nuclear power side becomes zero. That is, when the converter is started using the above-mentioned starting method, the initial load of nuclear power generation becomes zero. If the converter is started in this way and the power transmitted by the converter is increased according to the generated power value on the nuclear power side after a predetermined time,
It is possible to operate in coordination with the nuclear power side. Fourth
The figure is a time chart based on one embodiment of the present invention, and the operation of the present invention will be explained in further detail using this time chart.
第4図において、P1極とP2極の運転電力値を
同じ値にして前述した起動方式で、P1極とP2極
の各変換器を同時に起動する。いま、第4図にお
けるP1極とP2極の運転電力値は定格の10%と仮
定する。第4図より明白なごとく、起動当初は、
P1極の変換器8は順変換器として、定格の10%
の電力を送電するが、逆にP2極の変換器9は逆
変換器として定格の10%の電力を受電する為に、
第1図における交流母線5、従つて原子力発電の
負荷出力はほぼ零となる。この状態での原子力発
電電力は、バイパス弁を介してバイパスしてお
く。このような状態から、原子力発電電力値が20
%程度まで立上がつた時点、(第4図のta)で、
P2極の潮流を反転させて、P2極の変換器9を逆
変換器運転から順変換器運転へ逆転させれば、潮
流反転が完了した時点(第4図のtb)では、送電
電力は20%とする。その後は、原子力発電の運転
電力指令値に応じて、変換器の送電電力を増加さ
せればよい。 In FIG. 4, the P 1 and P 2 pole converters are started at the same time using the above-mentioned startup method, with the operating power values of the P 1 pole and P 2 pole being set to the same value. Now, it is assumed that the operating power value of P1 pole and P2 pole in Fig. 4 is 10% of the rated value. As is clear from Figure 4, at the beginning of startup,
P 1- pole converter 8 is a forward converter with 10% of the rating
On the other hand, P 2- pole converter 9 receives 10% of the rated power as an inverse converter.
The load output of the AC bus 5 in FIG. 1, and thus of the nuclear power generation, becomes almost zero. Nuclear power in this state is bypassed via a bypass valve. In this situation, the nuclear power generation value is 20
When the temperature rises to about % (ta in Figure 4),
If the P 2- pole power flow is reversed and the P 2- pole converter 9 is reversed from reverse converter operation to forward converter operation, at the time when the power flow reversal is completed (tb in Figure 4), the transmitted power shall be 20%. Thereafter, the power transmitted by the converter may be increased in accordance with the nuclear power generation operating power command value.
第5図は、もつときめ細かい制御を実施した場
合のタイムチヤートを示す。第3図において説明
したごとく、原子力側では数%の初負荷は許容値
以内である為に、この点に着目して、P1極の変
換器8は、例えば定格の15%、P2極の変換器9
は、例えば定格の10%で起動する。そうすると、
第5図に示すごとく、交流母線5の負荷出力は5
%となり、この状態で所定時間運転する。その
後、原子力発電出力に応じて、P1極の送電電力
のみ増加させて、P2極の受電電力は一定のまま
で運転を継続させ、原子力発電出力が20%程度の
出力になつた時点(第5図のt3)で、P1極の送電
電力を10%まで減少させると同時に、P2極の潮
流を反転させる操作を行なう。 FIG. 5 shows a time chart when fine-grained control is implemented. As explained in Fig. 3, on the nuclear power side, an initial load of several percent is within the allowable value, so paying attention to this point, converter 8 with P 1 pole is changed to 15% of the rating, P 2 poles, etc. converter 9
will start at, for example, 10% of the rated value. Then,
As shown in Fig. 5, the load output of the AC bus 5 is 5
%, and the machine is operated in this state for a predetermined period of time. After that, depending on the nuclear power output, only the power transmitted from the P1 pole is increased, and the operation continues with the power received from the P2 pole kept constant, until the nuclear power output reaches about 20% ( At t3 ) in Fig. 5, the power transmitted from the P1 pole is reduced to 10%, and at the same time, the power flow at the P2 pole is reversed.
このようにすれば、第5図に示すごとく、潮流
反転が完了した時点(第5図のt4)では、送電電
力はほぼ20%となる。その後は再び、原子力発電
出力に応じて、P1極とP2極の送電電力を増加さ
せればよい。又、これまでの説明では双極1回線
に限つているが、双極多回線でも、各回線毎に上
記の方法が適用できることは明らかである。又、
原子力発電機の単機容量及び発電機台数と変換器
の単機容量及び変換器台数に応じて、発電機の許
容値以内になるように、送電端側の複数の変換器
を順変換器として起動し、残りの変換器を逆変換
器として起動することもできる。 In this way, as shown in FIG. 5, the transmitted power will be approximately 20% at the time when the power flow reversal is completed (t 4 in FIG. 5). After that, it is only necessary to increase the power transmitted to the P1 pole and P2 pole again according to the nuclear power generation output. Further, although the explanation so far has been limited to one bipolar line, it is clear that the above method can be applied to each line even in the case of multiple bipolar lines. or,
Depending on the single unit capacity of the nuclear power generator, the number of generators, the single unit capacity of the converter, and the number of converters, multiple converters on the power transmission end are activated as forward converters so that the values are within the allowable values of the generator. , the remaining transducers can also be activated as inverse transducers.
以上説明したごとく、本発明によれば、弱い系
統に接続された、或いは発電機と直結された送電
端側の複数台の変換器の内、幾台かを順変換器、
残りを逆変換器として起動し、全送電電力が、系
統或いは発電機出力条件の許容値以内になるよう
に運転することにより、系統の電圧変動を抑制、
或いは発電機の初負荷の問題や変換器の電流断続
の問題を解決することができ、且つ従来の実績の
ある起動方式を適用できると云う著しい効果を有
する。 As explained above, according to the present invention, some of the plurality of converters on the transmission end side connected to a weak power system or directly connected to a generator are converted into forward converters,
By starting the remaining part as an inverter and operating it so that the total transmitted power is within the allowable value of the grid or generator output conditions, voltage fluctuations in the grid are suppressed.
Alternatively, it has the remarkable effect of being able to solve the problem of the initial load of the generator and the problem of intermittent current of the converter, and also being able to apply the conventional proven starting method.
第1図は、双極1回線の直流送電設備の構成
図、第2図は従来の変換設備の起動パターンを示
す図、第3図は、原子力発電機器出力の負荷立上
げパターンを示す図、第4図、第5図は本発明に
もとづく変換器起動時のタイムチヤートを示す図
である。
1……原子炉、2……タービン、3……発電
機、4……昇圧用変圧器、5……交流母線、6,
7……変換用変圧器、8,9,10,11……変
換器、12,13,14,15……平滑リアクト
ル、16,17……本線、18……中性線。
Figure 1 is a configuration diagram of a bipolar single-line DC power transmission facility, Figure 2 is a diagram showing the startup pattern of conventional conversion equipment, Figure 3 is a diagram showing the load startup pattern of nuclear power generation equipment output, 4 and 5 are diagrams showing time charts at the time of starting the converter based on the present invention. 1... Nuclear reactor, 2... Turbine, 3... Generator, 4... Step-up transformer, 5... AC bus, 6,
7... Conversion transformer, 8, 9, 10, 11... Converter, 12, 13, 14, 15... Smoothing reactor, 16, 17... Main line, 18... Neutral line.
Claims (1)
換器を起動する際には、一方の極の送電端側の変
換器を順変換器で起動し、他方の極の送電端側の
変換器を逆変換器で起動し、起動時の送電電力を
所定値以下にして起動することを特徴とする交直
変換装置の起動方式。 2 双極多回線の交直変換システムにおいて、変
換器を起動する際には、各双極単位に、一方の極
の送電端側の変換器を順変換器で起動し、他方の
極の送電端側の変換器を逆変換器で起動すること
を特徴とする交直変換装置の起動方式。 3 多極多回線の交直変換システムにおいて、変
換器を起動する際には、送電端側の複数台の変換
器を順変換器で起動し、残りの送電端側の変換器
を逆変換器で起動することを特徴とする交直変換
装置の起動方式。[Claims] 1. In a bipolar single-line AC/DC conversion system, when starting a converter, the converter on the power transmission end side of one pole is started up as a forward converter, and the converter on the power transmission end side of the other pole is activated as a forward converter. A method for starting an AC/DC converter, characterized in that the converter is started by an inverse converter, and the power transmitted at the time of start-up is set to a predetermined value or less. 2. In a bipolar multi-line AC/DC conversion system, when starting the converters, for each bipolar unit, start the converter on the power transmission end side of one pole using the forward converter, and start the converter on the power transmission end side of the other pole. A starting method for an AC/DC converter, characterized in that a converter is started by an inverse converter. 3. In a multi-pole, multi-line AC/DC conversion system, when starting up the converters, start up multiple converters on the power transmission end using the forward converter, and start the remaining converters on the power transmission end using the inverse converter. A starting method for an AC/DC converter characterized by starting.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56076078A JPS57193939A (en) | 1981-05-20 | 1981-05-20 | Starting system for ac/dc converter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56076078A JPS57193939A (en) | 1981-05-20 | 1981-05-20 | Starting system for ac/dc converter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57193939A JPS57193939A (en) | 1982-11-29 |
| JPS6367413B2 true JPS6367413B2 (en) | 1988-12-26 |
Family
ID=13594770
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56076078A Granted JPS57193939A (en) | 1981-05-20 | 1981-05-20 | Starting system for ac/dc converter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57193939A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57202836A (en) * | 1981-06-05 | 1982-12-11 | Denriyoku Chuo Kenkyusho | Method of starting and stopping dc single transmission system |
-
1981
- 1981-05-20 JP JP56076078A patent/JPS57193939A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57193939A (en) | 1982-11-29 |
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