JPH0216110B2 - - Google Patents

Info

Publication number
JPH0216110B2
JPH0216110B2 JP59053886A JP5388684A JPH0216110B2 JP H0216110 B2 JPH0216110 B2 JP H0216110B2 JP 59053886 A JP59053886 A JP 59053886A JP 5388684 A JP5388684 A JP 5388684A JP H0216110 B2 JPH0216110 B2 JP H0216110B2
Authority
JP
Japan
Prior art keywords
phase
wave rectifier
mode
rectifier unit
full
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
Application number
JP59053886A
Other languages
Japanese (ja)
Other versions
JPS60197170A (en
Inventor
Isao Takahashi
Hirohide Hirayama
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP59053886A priority Critical patent/JPS60197170A/en
Publication of JPS60197170A publication Critical patent/JPS60197170A/en
Publication of JPH0216110B2 publication Critical patent/JPH0216110B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02MAPPARATUS FOR CONVERSION BETWEEN AC AND AC, BETWEEN AC AND DC, OR BETWEEN DC AND DC, AND FOR USE WITH MAINS OR SIMILAR POWER SUPPLY SYSTEMS; CONVERSION OF DC OR AC INPUT POWER INTO SURGE OUTPUT POWER; CONTROL OR REGULATION THEREOF
    • H02M7/00Conversion of AC power input into DC power output; Conversion of DC power input into AC power output
    • H02M7/02Conversion of AC power input into DC power output without possibility of reversal
    • H02M7/04Conversion of AC power input into DC power output without possibility of reversal by static converters
    • H02M7/12Conversion of AC power input into DC power output without possibility of reversal by static converters using discharge tubes with control electrode or semiconductor devices with control electrode
    • H02M7/145Conversion of AC power input into DC power output without possibility of reversal by static converters using discharge tubes with control electrode or semiconductor devices with control electrode using devices of a thyratron or thyristor type requiring extinguishing means
    • H02M7/155Conversion of AC power input into DC power output without possibility of reversal by static converters using discharge tubes with control electrode or semiconductor devices with control electrode using devices of a thyratron or thyristor type requiring extinguishing means using semiconductor devices only
    • H02M7/17Conversion of AC power input into DC power output without possibility of reversal by static converters using discharge tubes with control electrode or semiconductor devices with control electrode using devices of a thyratron or thyristor type requiring extinguishing means using semiconductor devices only arranged for operation in parallel

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Rectifiers (AREA)
  • Inverter Devices (AREA)

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は可変直流電圧を発生する整流装置に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a rectifier that generates a variable DC voltage.

〔従来の技術〕[Conventional technology]

第1図は3相全波整流装置の基本構成を示すも
ので、1は3相交流電源、2,3,4はそれぞれ
この3相交流電源のR相、S相、T相、5は3相
全波整流ユニツト、6,7,8はそれぞれ3相全
波整流ユニツトの入力線U相、V相、W相、9,
10はそれぞれ3相全波整流ユニツト5の出力線
P及びN、UPはU相P側のサイリスタ、VPはV
相P側のサイリスタ、VNはV相N側のサイリス
タ、WPはW相P側のサイリスタ、WNはW側N
側のサイリスタを示す。なお3相交流電源1の相
名称R、S、T相と3相全波整流ユニツト5の入
力線U、V、W相を別名称としたのは後の説明を
分り易くする為であり、通常RとU、SとV、T
とWの各線が接続されている。
Figure 1 shows the basic configuration of a three-phase full-wave rectifier, where 1 is a 3-phase AC power supply, 2, 3, and 4 are R, S, and T phases of this 3-phase AC power supply, and 5 is a 3-phase AC power supply. Phase full wave rectifier unit, 6, 7, 8 are the input lines of the 3 phase full wave rectifier unit U phase, V phase, W phase, 9,
10 are the output lines P and N of the three-phase full-wave rectifier unit 5, UP is the thyristor on the U-phase P side, and VP is the V
The thyristor on the phase P side, VN is the thyristor on the V phase N side, WP is the thyristor on the W phase P side, WN is the thyristor on the W side N
The side thyristor is shown. Note that the R, S, and T phases of the three-phase AC power supply 1 and the input lines U, V, and W phases of the three-phase full-wave rectifier unit 5 are given different names to make the explanation easier to understand later. Usually R and U, S and V, T
and W are connected.

第2図は第1図のような3相全波整流装置でイ
ンバータ運転を行い負の可変直流電圧を発生させ
る場合の従来の一般的な点弧制御による出力電圧
波形と導通サイリスタの時間的変化を示すもの
で、図から明らかな如く一定直流出力電圧に対し
ては、各サイリスタとも同一の位相角αで対称的
に点弧制御されている。衆知の如く、このような
整流方式では電圧に対する電流の位相を制御する
ものである為、出力電圧の絶対値が小さい場合は
力率が悪く大きな無効電力を発生する欠点があ
る。
Figure 2 shows the output voltage waveform and the temporal change in the conduction thyristor due to conventional general ignition control when a three-phase full-wave rectifier as shown in Figure 1 is operated with an inverter to generate a negative variable DC voltage. As is clear from the figure, for a constant DC output voltage, each thyristor is symmetrically controlled to fire at the same phase angle α. As is well known, such a rectification method controls the phase of current with respect to voltage, so if the absolute value of the output voltage is small, the power factor is poor and a large amount of reactive power is generated.

〔発明の概要〕[Summary of the invention]

この発明は上述の如く、第1図に示すようなサ
イリスタを整流素子とする3相全波整流装置で、
第2図に示すような対称位相制御によるインバー
タ運転で負の可変直流出力電圧を発生させた場
合、特に出力電圧の絶対値が小さい場合には力率
が悪く、大きな無効電力を発生する欠点があるの
を除去し、低出力域(出力電圧の絶対値が小さい
領域)の力率を向上させ、無効電力の発生の少い
整流方式、点弧制御方式を提供する為になされた
ものである。
As mentioned above, the present invention is a three-phase full-wave rectifier using a thyristor as a rectifying element as shown in FIG.
When a negative variable DC output voltage is generated by inverter operation using symmetrical phase control as shown in Figure 2, the power factor is poor and large reactive power is generated, especially when the absolute value of the output voltage is small. This was done to improve the power factor in the low output range (area where the absolute value of the output voltage is small), and to provide a rectification method and ignition control method that generate less reactive power. .

〔発明の実施例〕[Embodiments of the invention]

以下この発明の一実施例を図について説明す
る。第3図に於て、51,52,53はそれぞれ
第1、第2及び第3の3相全波整流ユニツト、L
1a,L1b,L2a,L2b,L3a,L3b
はそれぞれリアクトルを示す。上記第1〜第3の
3相全波整流ユニツト51〜53の内部構成は第
1図の3相全波整流ユニツト5と同一であるが、
3相交流電源1に対する入力線の接続は、第1の
3相全波整流ユニツト51がR−U、S−V、T
−Wであり、第2の3相全波整流ユニツト52が
S−U、T−V、R−Wであり、第3の3相全波
整流ユニツト53がT−U、R−V、S−Wの接
続となるよう相を入れ替えて接続されており、
又、それぞれのユニツト51〜53の出力線P、
NはそれぞれリアクトルL1a,L1b,L2
a,L2b,L3a,L3bを介して相互に並列
接続されている。
An embodiment of the present invention will be described below with reference to the drawings. In FIG. 3, 51, 52, and 53 are first, second, and third three-phase full-wave rectifier units, respectively, and L
1a, L1b, L2a, L2b, L3a, L3b
each indicates a reactor. The internal configurations of the first to third three-phase full-wave rectifier units 51 to 53 are the same as the three-phase full-wave rectifier unit 5 in FIG.
The connection of input lines to the three-phase AC power supply 1 is such that the first three-phase full-wave rectifier unit 51 connects R-U, S-V, T
-W, the second three-phase full-wave rectifier unit 52 is S-U, TV, R-W, and the third three-phase full-wave rectifier unit 53 is T-U, RV, S-W. - They are connected by switching the phases to make a W connection,
In addition, the output lines P of each unit 51 to 53,
N are reactors L1a, L1b, L2, respectively
They are mutually connected in parallel via a, L2b, L3a, and L3b.

第4図は第3図の3相全波整流ユニツト51〜
53の点弧制御方式と出力電圧波形を示すもの
で、イは単相モード(以下モード′と称する)、
ロ,ハは3相モード(以下モード′と称し、更
にこれをロの′Aモード、ハの′Bモードに区分
する)での出力電圧波形、導通サイリスタ、3相
全波整流ユニツトの等価回路、ニは各モードに於
けるサイリスタ点弧制御の一覧表を夫々示してい
る。この発明はインバータ領域で要求される出力
直流電圧レベルに応じ、各3相全波整流ユニツト
をモード′、′A、′Bに切替えて運転し、か
つ、各3相全波整流ユニツト51〜53の合成出
力を得ようとするものである。即ちサイリスタを
理想整流素子と仮定し、最小制御進み角(γリミ
ツター)の値をγ、3相交流電源1の線間電圧の
波高値をEm、3相全波整流ユニツトの直流出力
電圧をEd〓、Ed〓最大値をEdpとすると、インバー
タ領域ではEd〓=En/π(1−cosγ)〜−En/πcosγ
と なりEdpはEdp=3/πEmであるが、Ed〓=Edp/3(1 −cosγ)〜−2/3Edpcosγの場合はモード′、 の場合はモード′Aの場合はモード′Bで第1〜第3の3相全波整流
ユニツト51〜53を運転するものとし、しかも
第1〜第3の3相全波整流ユニツトを構成するサ
イリスタ11〜16は、第4図に示す如くモード
′ではVPとVNが要求される出力直流電圧レベ
ルが要求される出力直流電圧レベルに応じて制御
角α(0<α<π−γ)で位相制御され、UPと
UNはπ−γで点弧、WPとWNは常時非導通と
され、モード′AではVPとVNが制御角α(−
π/3+γ<α<−γ)で位相制御されると共にπ −γでも点弧され、UPとUNは2/3π−γで点 弧、WPとWNはπ−γで点弧され、モード′B
ではUPとUNが制御角α(2/3π−γ<α<π− γ)で位相制御、VP、VN、WP、WNはπ−γ
で点弧制御されるよう各モードで非対称点弧制御
を行う。又前記したように第1〜第3の3相全波
整流ユニツト51〜53は3相交流電源1に対す
る入力線の接続がそれぞれずらされており、かつ
リアクトルL1a〜L3bを介して相互に並列接
続されているので、合成直流出力電流は軽負荷時
においても不連続になることはない。第5図は上
述の如く出力直流電圧Ed〓のレベルに応じてモー
ド′、モード′A、モード′Bの各モードに切
替えて非対称点弧制御を行つた場合の制御角αと
出力直流電圧Ed〓の関係を示す特性図、第6図は
横軸に出力電圧Ed〓/Edp、縦軸に無効電力Q/
Edp・Id(但しQは基本波無効電力、Idは出力直流
電流を示す)をとつて両者の関係を示す電力円線
図で、比較の為本発明の実施例による場合による
aと従来の対称制御による3相全波整流の場合b
とを示している。第6図から明らかな如く、電力
円線図に於ける弧の半径は、通常の3相全波方式
にくらべ本発明による場合は1/3になつており、
無効電力の発生が大巾に少くなつている。又第7
図は、基本波力率cosφ1と出力電圧の関係を示す
もので、aは本発明による非対称制御による場
合、bは通常の3相全波方式の場合である。図か
ら明らかなように低中出力域における基本波力率
が大巾に改善されている。
Figure 4 shows the three-phase full-wave rectifier unit 51 to Figure 3.
53 shows the ignition control method and output voltage waveform, A is single-phase mode (hereinafter referred to as mode'),
B and C show the output voltage waveform in the three-phase mode (hereinafter referred to as mode', which is further divided into B's A mode and C's B mode), the conduction thyristor, and the equivalent circuit of the three-phase full-wave rectifier unit. , D show a list of thyristor firing control in each mode. This invention operates by switching each three-phase full-wave rectifier unit to modes ', ' A , and ' B according to the output DC voltage level required in the inverter region, and operates each three-phase full-wave rectifier unit 51 to 53. The purpose is to obtain the composite output of That is, assuming that the thyristor is an ideal rectifying element, the value of the minimum control advance angle (γ limiter) is γ, the peak value of the line voltage of the three-phase AC power supply 1 is Em, and the DC output voltage of the three-phase full-wave rectifier unit is E. d 〓, E d 〓If the maximum value is E dp , in the inverter region E d 〓=E n /π(1-cosγ) ~ −E n /πcosγ
Therefore, E dp is E dp = 3/πEm, but if E d 〓 = E dp / 3 (1 - cos γ) ~ -2/3E dp cos γ, mode ′, If mode ′ A , In this case, the first to third three-phase full-wave rectifier units 51 to 53 are operated in mode ' B , and the thyristors 11 to 16 constituting the first to third three-phase full-wave rectifier units are As shown in Figure 4, in mode ', VP and VN are phase-controlled according to the required output DC voltage level at a control angle α (0 < α < π - γ), and UP and
UN is fired at π−γ, WP and WN are always non-conducting, and in mode ′ A , VP and VN are controlled at the control angle α(−
The phase is controlled by π/3+γ<α<-γ) and is also fired at π-γ, UP and UN are fired at 2/3π-γ, WP and WN are fired at π-γ, and mode ′ B
In this case, UP and UN are phase controlled by control angle α (2/3π−γ<α<π−γ), and VP, VN, WP, and WN are controlled by π−γ.
Asymmetric ignition control is performed in each mode so that ignition is controlled at Further, as described above, the input lines of the first to third three-phase full-wave rectifier units 51 to 53 to the three-phase AC power supply 1 are shifted from each other, and are connected in parallel to each other via the reactors L1a to L3b. Therefore, the combined DC output current does not become discontinuous even under light loads. Figure 5 shows the control angle α and the output DC voltage when asymmetric ignition control is performed by switching to Mode ', Mode ' A , and Mode ' B according to the level of the output DC voltage E d 〓 as described above. In Figure 6, the horizontal axis shows the output voltage E d 〓/E dp , and the vertical axis shows the reactive power Q/E dp .
This is a power circle diagram showing the relationship between E dp and I d (where Q is the fundamental wave reactive power and I d is the output DC current), and for comparison, a and a according to the embodiment of the present invention are shown. In the case of three-phase full-wave rectification with conventional symmetrical control b
It shows. As is clear from FIG. 6, the radius of the arc in the power circle diagram is 1/3 that of the normal three-phase full-wave system according to the present invention.
The generation of reactive power has been significantly reduced. Also the 7th
The figure shows the relationship between the fundamental wave power factor cosφ 1 and the output voltage, where a shows the case where the asymmetric control according to the present invention is used, and b shows the case where the normal three-phase full-wave system is used. As is clear from the figure, the fundamental wave power factor in the low-medium power range has been greatly improved.

尚上記説明では簡単の為、3相全波整流ユニツ
トはサイリスタ6個で構成される最も基本的なも
ので説明したが、電圧電流値によつてサイリスタ
素子を直並列に接続しても、又3相全波整流ユニ
ツト自体の一個分を直並列域は逆方向の出力電流
が得られるよう逆並列接続したものについても上
記実施例と同様の効果を生ずる。更に3相全波整
流ユニツトの構成素子はサイリスタで説明した
が、導通位相制御可能な他の素子、例えばトラン
ジスタ、ゲートターンオフサイリスタ等であつて
も同様の効果が得られる。又、実施例として第4
図に基いて説明したようにサイリスタを位相制御
する場合を設定したのは、各モード切替時の整流
波形の変動を極力少くし円滑な変化が得られるよ
うにとの配慮によるものであるが、位相制御する
相を変更しても(例えはモード′でUP、UNを
位相制御、VP、VNをπ−γで点弧)51〜5
3の各ユニツト共同じように変更されるなら本発
明の効果としては変らない。
In the above explanation, for simplicity, the three-phase full-wave rectifier unit was explained as the most basic one consisting of six thyristors, but depending on the voltage and current value, thyristor elements can be connected in series or parallel. An effect similar to that of the above embodiment can also be obtained by connecting one three-phase full-wave rectifier unit itself in anti-parallel connection so that output currents in opposite directions can be obtained in the series-parallel region. Furthermore, although the three-phase full-wave rectifier unit has been described using a thyristor as a constituent element, the same effect can be obtained by using other elements whose conduction phase can be controlled, such as a transistor or a gate turn-off thyristor. Also, as an example, the fourth
The reason for setting the case where the thyristor is phase controlled as explained based on the figure is to minimize the fluctuation of the rectified waveform when switching each mode and to obtain a smooth change. Even if the phase to be controlled is changed (for example, UP and UN are phase controlled in mode ', VP and VN are fired at π-γ)51~5
If each unit of 3 is changed in the same way, the effect of the present invention will not change.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によれば、複数個の整
流ユニツトを並列接続してインバータ運転を行う
に際し、要求される出力直流電圧レベルに応じて
単相モード又は3相モードに切替え、各整流ユニ
ツトを構成するスイツチング素子を非対称点弧制
御する事により、低出力電圧域に於ても力率が良
く無効電力の発生の少い整流方式が得られる効果
があり、且つ入力電源の相を各整流ユニツトでず
らせて接続しているので、非対称制御による電源
側の不平衡も防止出来る効果がある。
As described above, according to the present invention, when performing inverter operation by connecting a plurality of rectifier units in parallel, each rectifier unit is switched to single-phase mode or three-phase mode depending on the required output DC voltage level. By controlling the switching elements constituting the switch asymmetrically, it is possible to obtain a rectification method that has a good power factor and generates little reactive power even in the low output voltage range, and also rectifies each phase of the input power supply. Since the units are connected in a staggered manner, it is possible to prevent unbalance on the power supply side due to asymmetric control.

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

第1図は3相全波整流装置の基本構成図、第2
図は第1図の構成によりインバータ運転で可変直
流出力電圧を発生する場合の従来の点弧制御方式
による出力電圧波形と導通サイリスタの時間的変
化を示す説明図、第3図はこの発明の一実施例に
よる整流装置の構成図、第4図は第3図の構成に
よる整流装置の各モードに於ける等価回路、出力
電圧波形、点弧制御方式を説明する図、第5図は
この発明の整流装置による制御角αと出力電圧の
関係を示す特性図、第6図は同じく出力電圧と無
効電力の関係を示す電力円線図、第7図は同じく
基本波力率と出力電圧の関係を示す特性図であ
る。 図に於て1は3相交流電源、2は3相交流電源
のR相、3はS相、4はT相、5は3相全波整流
ユニツト、6は3相全波整流ユニツトのU相、7
はV相、8はW相、9は3相全波整流ユニツトの
出力線P、10は出力線N、UPは3相全波整流
ユニツトを構成するU相P側のサイリスタ、UN
はU相N側のサイリスタ、VPはV相P側のサイ
リスタ、VWはV相N側のサイリスタ、WPはW
相P側のサイリスタ、51,52,53はそれぞ
れNo.1、No.2、No.3の各3相全波整流ユニツト、
L1a,L1b,L2a,L2b,L3a,L3
bはリアクトルを示す。なお図中同一符号は同一
又は相当部分を示す。
Figure 1 is a basic configuration diagram of a three-phase full-wave rectifier, Figure 2
The figure is an explanatory diagram showing the output voltage waveform and the time change of the conduction thyristor according to the conventional ignition control method when a variable DC output voltage is generated by inverter operation using the configuration shown in Fig. 1. FIG. 4 is a diagram illustrating the equivalent circuit, output voltage waveform, and ignition control method in each mode of the rectifier having the configuration shown in FIG. 3, and FIG. A characteristic diagram showing the relationship between the control angle α and the output voltage by the rectifier, FIG. 6 is a power circle diagram showing the relationship between the output voltage and reactive power, and FIG. 7 is the same diagram showing the relationship between the fundamental wave power factor and the output voltage. FIG. In the figure, 1 is the 3-phase AC power supply, 2 is the R phase of the 3-phase AC power supply, 3 is the S phase, 4 is the T phase, 5 is the 3-phase full-wave rectifier unit, and 6 is the U of the 3-phase full-wave rectifier unit. phase, 7
is the V phase, 8 is the W phase, 9 is the output line P of the 3-phase full-wave rectifier unit, 10 is the output line N, UP is the thyristor on the U-phase P side that constitutes the 3-phase full-wave rectifier unit, UN
is the thyristor on the U phase N side, VP is the thyristor on the V phase P side, VW is the thyristor on the V phase N side, and WP is the W thyristor.
Thyristors 51, 52, and 53 on the phase P side are No. 1, No. 2, and No. 3 three-phase full-wave rectifier units, respectively.
L1a, L1b, L2a, L2b, L3a, L3
b indicates a reactor. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】 1 導通位相制御可能な複数のスイツチング素子
により構成された整流ユニツトを交流電源に接続
し、上記スイツチング素子を導通制御してインバ
ータ運転を行い、上記整流ユニツトの出力側から
負の直流出力電圧を得るようにしたものに於て、
上記整流ユニツトを複数個設け、これらの整流ユ
ニツトの入力端を上記交流電源に対して互いに異
なる相関係でそれぞれ接続すると共に各整流ユニ
ツトの出力端をリアクトルを介して共通接続し、
かつ上記それぞれ整流ユニツトを、その発生しう
る直流出力電圧レベルに応じ単相運転モード又は
多相運転モードに切替えて運転するようにした事
を特徴とする整流装置。 2 各整流ユニツトは第1、第2及び第3の3相
全波整流ユニツトよりなり、上記各3相全波整流
ユニツトは、その発生し得る直流出力電圧の最大
値をEdp、最小制御進み角(γリミツター)の値
をγとするとき、要求される出力電圧値がEdp/3 (1−cosγ)〜−2/3Edpcosγの時は単相モードで あるモード′で運転され、要求される出力電圧
値が の場合は3相モードの一つである′Aモードで運
転され、要求される出力電圧レベルが の時は3相モードの一つである′Bモードで運転
するようにした事を特徴とする特許請求の範囲第
1項に記載の整流装置。 3 3相交流電源の出力端の相をR相、S相、T
相とし、第1、第2、第3の3相全波整流ユニツ
トの入力端の相をそれぞれ、U相、V相、W相と
した時、上記3相交流電源の出力端と第1、第2
及び第3の3相全波整流ユニツトの入力端との接
続はそれぞれ、(R−U、S−V、T−W)、(S
−U、T−V、R−W)、(T−U、R−V、S−
W)となるよう相を替えて接続すると共に各3相
全波整流ユニツトの正側出力端P及び負荷出力端
Nをそれぞれリアクトルを介して並列接続し、か
つ各3相全波整流ユニツトを構成するスイツチン
グ素子のU相P側をUP、U相N側をUN、V相
P側をVP、V相N側をVN、W相P側をWP、W
相N側をWNとするとき、モード′の時は、各
3相全波整流ユニツトは上記スイツチング素子
VPとVNを位相制御し、UPとUNは2/3π−γで 点弧され、WPとWNは常時非導通になるよう制
御され、モード′Aの時は各3相全波整流ユニツ
トは上記スイツチング素子VP、VNを位相制御
するとともに位相角π−γでも点弧し、UPと
UNは2/3π−γ、WPとWNはπ−γで点弧さ れ、モード′Bの時は各3相全波整流ユニツトは
上記スイツチング素子UPとUNを位相制御し、
VP、VN、WP及びWNは位相角π−γで点弧す
るよう制御されるようにした事を特徴とする特許
請求範囲第2項に記載の整流装置。
[Scope of Claims] 1. A rectifier unit constituted by a plurality of switching elements whose conduction phase can be controlled is connected to an AC power source, and the switching elements are controlled to conduction to perform inverter operation, and a negative voltage is output from the output side of the rectifier unit. In a device designed to obtain a DC output voltage of
A plurality of the rectifier units are provided, the input ends of these rectifier units are respectively connected to the AC power source in mutually different phase relationships, and the output ends of the rectifier units are commonly connected via a reactor,
A rectifying device characterized in that each of the rectifying units described above is operated by switching to a single-phase operation mode or a multi-phase operation mode depending on the DC output voltage level that can be generated. 2. Each rectifier unit consists of a first, second, and third three-phase full-wave rectifier unit, and each of the three-phase full-wave rectifier units has a maximum DC output voltage that can be generated by E dp and a minimum control advance. When the value of the angle (γ limiter) is γ, when the required output voltage value is E dp /3 (1-cos γ) to -2/3E dp cos γ, it is operated in mode ', which is the single-phase mode, The required output voltage value is In the case of 2. The rectifier according to claim 1, wherein the rectifier is operated in ' B mode, which is one of the three-phase modes. 3 Set the output end phases of the 3-phase AC power supply to R phase, S phase, and T phase.
phase, and the input terminal phases of the first, second, and third three-phase full-wave rectifier units are U phase, V phase, and W phase, respectively, and the output terminal of the three-phase AC power supply and the first, Second
The connections with the input terminal of the third three-phase full-wave rectifier unit are (R-U, S-V, T-W) and (S-W), respectively.
-U, T-V, R-W), (T-U, R-V, S-
W), and the positive output terminal P and load output terminal N of each three-phase full-wave rectifier unit are connected in parallel via a reactor, and each three-phase full-wave rectifier unit is configured. The U-phase P side of the switching element is UP, the U-phase N side is UN, the V-phase P side is VP, the V-phase N side is VN, and the W-phase P side is WP, W.
When the phase N side is WN, in mode ', each three-phase full-wave rectifier unit is connected to the above switching element.
VP and VN are phase controlled, UP and UN are ignited at 2/3π-γ, WP and WN are controlled to be constantly non-conducting, and in mode ' A , each three-phase full-wave rectifier unit is controlled as described above. The switching elements VP and VN are controlled in phase, and are also fired at the phase angle π-γ.
UN is ignited at 2/3π-γ, WP and WN are ignited at π-γ, and in mode ' B , each three-phase full-wave rectifier unit controls the phase of the switching elements UP and UN,
3. The rectifier device according to claim 2, wherein VP, VN, WP, and WN are controlled to fire at a phase angle of π-γ.
JP59053886A 1984-03-21 1984-03-21 Rectifier Granted JPS60197170A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59053886A JPS60197170A (en) 1984-03-21 1984-03-21 Rectifier

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59053886A JPS60197170A (en) 1984-03-21 1984-03-21 Rectifier

Publications (2)

Publication Number Publication Date
JPS60197170A JPS60197170A (en) 1985-10-05
JPH0216110B2 true JPH0216110B2 (en) 1990-04-16

Family

ID=12955214

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59053886A Granted JPS60197170A (en) 1984-03-21 1984-03-21 Rectifier

Country Status (1)

Country Link
JP (1) JPS60197170A (en)

Also Published As

Publication number Publication date
JPS60197170A (en) 1985-10-05

Similar Documents

Publication Publication Date Title
US6847531B2 (en) System and method for regenerative PWM AC power conversion
US6542390B2 (en) System and method for regenerative PWM AC power conversion
US5483140A (en) Thyristor based DC link current source power conversion system for motor driven operation
CA1073529A (en) Current fed inverter with commutation independent of load inductance
JPS58186373A (en) Regenerative rectifier circuit
US5198972A (en) Turn-off switch phase control with improved ripple and power factor
US5943221A (en) Portable power unit
Naik et al. A novel grid interface for photovoltaic, wind-electric, and fuel-cell systems with a controllable power factor of operation
JP2000139085A (en) Power converter
JP2001218470A (en) Power supply
JP3900444B2 (en) Three-phase wide input power conversion circuit
JPH0210669B2 (en)
JPS6035892B2 (en) power converter
JPH0216111B2 (en)
Bushman et al. Calculation of neutral voltage shift in LCI driven induction motors
JPS5943914B2 (en) Protection method of controlled rectifier
JP3367830B2 (en) Power supply
JPH1052046A (en) Portable power supply
JP3493330B2 (en) Power supply
JP3446793B2 (en) Power supply
JP2580108B2 (en) Power converter
JPH0219704B2 (en)
Park et al. A new thyristor phase-controlled voltage source converter with bidirectional power flow capability
JPS60197170A (en) Rectifier
JPH0472468B2 (en)