JPH0216111B2 - - Google Patents

Info

Publication number
JPH0216111B2
JPH0216111B2 JP59053887A JP5388784A JPH0216111B2 JP H0216111 B2 JPH0216111 B2 JP H0216111B2 JP 59053887 A JP59053887 A JP 59053887A JP 5388784 A JP5388784 A JP 5388784A JP H0216111 B2 JPH0216111 B2 JP H0216111B2
Authority
JP
Japan
Prior art keywords
phase
wave rectifier
mode
controlled
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
JP59053887A
Other languages
Japanese (ja)
Other versions
JPS60197171A (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 JP59053887A priority Critical patent/JPS60197171A/en
Publication of JPS60197171A publication Critical patent/JPS60197171A/en
Publication of JPH0216111B2 publication Critical patent/JPH0216111B2/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)
  • Inverter Devices (AREA)
  • Rectifiers (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、9,1
0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、UNはU
相N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相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. 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, 1 respectively.
0 is the output line P of the three-phase full-wave rectifier unit 5, respectively.
and N, UP is the U phase P side thyristor, UN is U
thyristor on the phase N side, VP is the thyristor on the V phase P side, VN is the thyristor on the V phase N side, WP is the thyristor on the W phase P side
thyristor on the side, WN indicates the thyristor on the W-phase N side. 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, and T and W wires 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 when 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51,52,53,54,5
5,56はそれぞれ第1、第2、第3、第4、第
5、第6の3相全波整流ユニツトでそれぞれUP,
UN,VP,VN,WP,WNのサイリスタを備え
ている。L1a,L1b〜L6a,L6bはリア
クトルを示す、第1〜第6図の3相全波整流ユニ
ツト51〜56の内部構成は第1図の5と同一で
あるが、3相交流電源1との入力線の接続は第1
及び第2の3相全波整流ユニツト51,52がR
−U、S−V、T−W、第3及び第4の3相全波
整流ユニツト53,54がS−U、T−V、R−
W、第5及び第6の3相全波整流ユニツト55,
56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、又出力線P、N
はそれぞれリアクトルL1a,L1b,L2a,
L2b〜L6a,L6b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 Figure 3, 51, 52, 53, 54, 5
5 and 56 are first, second, third, fourth, fifth, and sixth three-phase full-wave rectifier units, respectively UP,
Equipped with UN, VP, VN, WP, and WN thyristors. L1a, L1b to L6a, and L6b indicate reactors.The internal configurations of the three-phase full-wave rectifier units 51 to 56 in FIGS. 1 to 6 are the same as 5 in FIG. Connect the input line to the first
and the second three-phase full-wave rectifier units 51 and 52 are R
-U, S-V, T-W, third and fourth three-phase full wave rectifier units 53, 54 are S-U, T-V, R-
W, fifth and sixth three-phase full-wave rectifier units 55,
56 are connected by switching the phases so that the connections are T-U, R-V, and S-W, and the output lines P and N
are reactors L1a, L1b, L2a, respectively.
They are mutually connected in parallel via L2b to L6a and L6b.

本発明は上述の如く6台の3相全波整流ユニツ
トを並列接続してインバータ運転を行うに際し、
要求される負の出力電圧レベルに応じ、各3相全
波整流ユニツトを構成する6個のサイリスタのう
ち1つのみを位相制御し他はオフ状態とするか、
π−γまたは2/3π−γで点弧するもので点弧制 御方式により後述する′,′,′A,′B
A,′Bの6つのモードに切替えて運転するも
ので、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En、3相全波整流
ユニツトの直流出力電圧をEdα、Edαの最大値
をEdoとすると、インバータ領域ではEdα=En/2π (1−cosγ)〜−3/πEncosγとなりEdo=3/πEn (コンバータ領域)となるがEdα=Edo/6(1− cosγ)〜−Edo/3cosγの場合はモード′ Edα=Edo/3cosγ〜−2/3Edo cosγの場合はモ ード′ の時はモード′A の時はモード′B の時はモード′A の時はモード′Bで第1〜第6の3相全波整流ユ
ニツト51〜56を運転するものとする。
As described above, when the present invention performs inverter operation by connecting six three-phase full-wave rectifier units in parallel,
Depending on the required negative output voltage level, only one of the six thyristors constituting each three-phase full-wave rectifier unit is controlled in phase and the others are turned off, or
It fires at π-γ or 2/3π-γ, and depending on the ignition control method, ′, ′, ′ A , ′ B ,
It is operated by switching between six modes, 'A ' and ' B.The thyristor is assumed to be an ideal rectifier, and the value of the minimum control advance angle (γ limiter) is set to γ, the line voltage wave of the three-phase AC power supply 1. If the high value is E n , the DC output voltage of the three-phase full-wave rectifier unit is E d α, and the maximum value of E d α is E d o , then in the inverter region, E d α=E n /2π (1−cosγ) ~ -3/πE n cosγ becomes E d o = 3/πE n (converter region), but if E d α = E d o/6 (1- cos γ) ~ -E d o/3 cos γ, the mode ′ E d If α=E d o/3cosγ~-2/3E d o cosγ, mode' mode ′ A mode ′ B mode ′ A In this case, the first to sixth three-phase full-wave rectifier units 51 to 56 are operated in mode ' B.

第4〜第9図は各モードに於ける点弧制御方式
を説明するもので各図に於てイは3相全波整流ユ
ニツトの出力電圧波形と各サイリスタの点弧位相
を説明する図、ロは導通サイリスタを示す図、ハ
およびニは3相全波整流ユニツトの等価回路を示
している。なお今後の説明の便宜上3相全波整流
ユニツト51,53,55をNo.1グループ、5
2,54,56をNo.2グループと称し更に3相交
流電源1の連続した2周期の最初の1周期を領域
A次の1周期を領域Bと仮称するものとする。
Figures 4 to 9 explain the firing control method in each mode. B shows a conduction thyristor, and C and D show equivalent circuits of a three-phase full-wave rectifier unit. For convenience of future explanation, three-phase full-wave rectifier units 51, 53, and 55 will be referred to as No. 1 group and No. 5 group.
2, 54, and 56 will be referred to as No. 2 group, and the first period of two consecutive periods of the three-phase AC power supply 1 will be tentatively referred to as area A, and the next one period as area B.

第4図に示す如くモード′では、領域Aに於
けるグループ1の3相全波整流ユニツト、領域B
に於けるグループ2の3相全波整流ユニツトは要
求される出力直流電圧レベルに応じてVPが制御
角α(0〜π−γ)で位相制御され、UPは2/3π −γで点弧、VNは常時導通、UN,WP,WNは
常時非導通になるよう点弧制御され、領域Bに於
けるグループ1、領域Aに於けるグループ2の3
相全波整流ユニツトは上記P側とN側のサイリス
タを対称にして、VNが制御角αで位相制御、
UNは2/3π−γで点弧、VPは常時導通、UP, WP,WNは常時非導通になるよう制御される。
このようにグループ1とグループ2で3相全波整
流ユニツトを構成するサイリスタの点弧制御方式
を対称にし、しかも3相交流電源1の1周期毎に
グループ1とグループ2の制御方式を相互に切替
えているのは、3相交流電源1の相電流をバラン
スさせるのと、中性点電位から見た上下の平均出
力電圧の差を平均的に零にするための処置で以下
の第5〜第9図に於けるモード′〜′Bでも同
様の配慮がされている。
As shown in FIG.
In the group 2 three-phase full-wave rectifier unit, VP is phase-controlled at a control angle α (0 to π-γ) according to the required output DC voltage level, and UP is fired at 2/3π-γ. , VN are always conductive, UN, WP, and WN are always non-conductive, and group 1 in area B and group 2 in area A
In the phase full-wave rectifier unit, the P-side and N-side thyristors are made symmetrical, and VN is phase controlled at the control angle α.
UN is controlled to fire at 2/3π-γ, VP is always conductive, and UP, WP, and WN are always non-conductive.
In this way, the ignition control methods of the thyristors constituting the three-phase full-wave rectifier unit are made symmetrical between groups 1 and 2, and the control methods of groups 1 and 2 are mutually controlled every cycle of the three-phase AC power supply 1. The purpose of switching is to balance the phase currents of the 3-phase AC power supply 1 and to reduce the difference between the upper and lower average output voltages to zero on average as seen from the neutral point potential, and the following steps 5 to 5 are performed. Similar consideration is given to modes '-' B in FIG.

又位相制御する為のサイリスタをV相に選んで
いるのは整流動作とインバータ動作の切替時出力
電圧波形の変動を極力小さくするためで整流動作
時U相を位相制御した波形との連続性を考慮した
結果でありそれ以上の意味はない。
In addition, the reason why the thyristor for phase control is selected for the V phase is to minimize fluctuations in the output voltage waveform when switching between rectification operation and inverter operation, and to ensure continuity with the waveform of the U phase that is phase controlled during rectification operation. This is the result of consideration and has no other meaning.

第5図に示す如くモード′では領域Aにおけ
るグループ1領域Bに於けるグループ2の3相全
波整流ユニツトはVNが制御角α(γ〜π−γ)
で位相制御、UP,UWが2/3π−γ、VPがπ− γで点弧、WP,WNは常時不導通となるよう点
弧制御され、領域Bに於けるグループ1、領域A
に於けるグループ2の3相全波整流ユニツトは
VPが位相制御、UP,UNが2/3π−γ、VNがπ −γで点弧され、WP,WNが常時不導通になる
よう点弧制御される。
As shown in FIG. 5, in mode ', the three-phase full-wave rectifier unit of group 1 in region A and group 2 in region B has a control angle α (γ ~ π - γ) of VN.
The phase is controlled at
The Group 2 three-phase full-wave rectifier unit in
VP is phase controlled, UP and UN are fired at 2/3π-γ, VN is fired at π-γ, and firing is controlled so that WP and WN are always non-conducting.

第6図に示す如くモード′Aでは領域Aにおけ
るグループ1、領域Bに於けるグループ2の3相
全波整流ユニツトはVNが制御角α(−1/3π+γ 〜−γ)で位相制御すると共にπ−γでも点弧、
UP,UNが2/3π−γVP,WNがπ−γで点弧、 WPは常時非導通となるよう点弧制御され、領域
Bに於けるグループ1、領域Aに於けるグループ
2の3相全波整流ユニツトはVPが制御角αで位
相制御されると共にπ−γでも点弧、UP,UN
が2/3π−γ、VM,WPがπ−γでそれぞれ点 弧、WNは常時非導通になるよう点弧制御され
る。
As shown in Fig. 6, in mode ' A, the three-phase full-wave rectifier units of group 1 in region A and group 2 in region B are controlled in phase by VN at the control angle α (-1/3π+γ to -γ). Ignition even at π−γ,
UP, UN are ignited at 2/3π-γVP, WN is ignited at π-γ, WP is always non-conducting, and 3-phase group 1 in area B and group 2 in area A are activated. In the full-wave rectifier unit, VP is phase-controlled by the control angle α, and ignition, UP, and UN are also controlled at π-γ.
is ignited at 2/3π-γ, VM and WP are ignited at π-γ, and WN is controlled to be always non-conductive.

第7図に示す如くモード′Bでは領域Aに於け
るグループ1、領域Bに於けるグループ2の3相
全波整流ユニツトはUNが位相角α(2/3π−γ〜 π−γ)で位相制御、UPが2/3π−γ、VP, VN,WNがπ−γでそれぞれ点弧されWPは常
時非導通となるよう点弧制御され、領域Bに於け
るグループ1、領域Aに於けるグループ2の3相
全波整流ユニツトはUPが位相制御、UNが2/3π −γ、VP,VN,WPがπ−γでそれぞれ点弧さ
れ、WNは常時非導通になるよう点弧制御され
る。
As shown in Fig. 7, in mode ' B , the three-phase full-wave rectifier units of group 1 in region A and group 2 in region B have a phase angle of UN of α (2/3π-γ to π-γ). Phase control is performed so that UP is ignited at 2/3π-γ, VP, VN, and WN are ignited at π-γ, and WP is always non-conducting. In the group 2 three-phase full-wave rectifier unit, UP is phase controlled, UN is ignited at 2/3π-γ, VP, VN, and WP are ignited at π-γ, and WN is ignited so that it is always non-conducting. be done.

第8図に示す如くモード′AではVPが制御角
α(−1/3π+γ〜−γ)で位相制御されると共に π−γでも点弧、UPが2/3π−γ、UN,VN, WP,WNがπ−γでそれぞれ点弧されるよう位
相制御され、領域Bに於けるグループ1、領域A
に於けるグループ2の3相全波整流ユニツトは
VNが位相角αで位相制御されると共にπ−γで
も点弧、UNが2/3π−γ、UP,VP,WP,WN がπ−γでそれぞれ点弧されるよう点弧制御され
る。
As shown in Fig. 8, in mode ' A , VP is phase controlled by the control angle α (-1/3π+γ to -γ), ignition occurs even at π-γ, and UP is 2/3π-γ, UN, VN, WP. , WN are ignited at π-γ, and group 1 in region B and region A
The Group 2 three-phase full-wave rectifier unit in
VN is phase-controlled at the phase angle α and is also fired at π-γ, UN is fired at 2/3π-γ, and UP, VP, WP, and WN are fired at π-γ.

第9図に示す如くモード′Bでは領域Aに於け
るグループ1、領域Bに於けるグループ2の3相
全波整流ユニツトはUPが位相角α(2/3π−γ〜 π−γ)で位相制御、UN,VP,VN,WP,
WNがπ−γで点弧されるよう点弧制御され、領
域Bに於けるグループ1領域Aに於けるグループ
2の3相全波整流ユニツトはUNが位相制御、
UP,VP,VN,WP,WNがπ−γで点弧され
るよう点弧制御される。
As shown in Fig. 9, in mode ' B , the three-phase full-wave rectifier units of group 1 in region A and group 2 in region B have UP at a phase angle α (2/3π-γ to π-γ). Phase control, UN, VP, VN, WP,
The ignition is controlled so that WN is ignited at π-γ, and the three-phase full-wave rectifier unit of group 2 in group 1 in area B is controlled in phase by UN.
Firing control is performed so that UP, VP, VN, WP, and WN are fired at π-γ.

第10図は各モードに於ける3相全波整流ユニ
ツトの点弧制御方式を一覧表にしたもので、注記
の如く領域Aでの制御方式を示しており、前述の
理由で領域Bではグループ1とグループ2の制御
方式を相互に入れ替え、これを3相交流電源1の
1周期毎に繰り返していくものとする。
Figure 10 is a list of the ignition control methods of the three-phase full-wave rectifier unit in each mode.As noted, the control method in region A is shown, and for the reason mentioned above, the control method in region B is It is assumed that the control methods of Group 1 and Group 2 are exchanged with each other, and this is repeated every cycle of the three-phase AC power supply 1.

各モード′〜′Bにおいて、第1と第2、第
3と第4、第5と第6の3相全波整流ユニツトは
それぞれの出力電圧間に180゜の位相のずれが生じ
るよう各サイリスタを選択し制御している。また
軽負荷時各3相全波整流ユニツト51〜56の出
力電流が不連続になるのを防止するため各ユニツ
トの出力側はリアクトルL1a〜L6bを介して
相互に並列接続されている。このように構成され
た本発明による装置において、第1、第3、第5
の3相全波整流ユニツト51,53,55の出力
電圧は、入力端がそれぞれ相を入れ替えて3相電
源1の出力端に接続されているので相互に120゜づ
つの位相のづれがあり、また第2、第4、第6の
3相全波整流ユニツト52,54,56の出力電
圧も同様の理由で相互に120゜づつの位相のずれが
ある。従つて全ての3相全波整流ユニツト整ユニ
ツト51〜56の出力電圧相互間には60゜づつの
位相のずれがある事になり、クアクトルL1a〜
L6bを介して並列接続された各ユニツトの合成
出力電流は各モードに於てきわめてスムースなも
のとなる。
In each mode '~' B , the first and second, third and fourth, and fifth and sixth three-phase full-wave rectifier units operate each thyristor so that a 180° phase shift occurs between the respective output voltages. are selected and controlled. Further, in order to prevent the output currents of the three-phase full-wave rectifier units 51-56 from becoming discontinuous during light loads, the output sides of the respective units are connected in parallel to each other via reactors L1a-L6b. In the device according to the present invention configured in this way, the first, third, and fifth
The output voltages of the three-phase full-wave rectifier units 51, 53, and 55 have a phase shift of 120 degrees from each other because the input terminals are connected to the output terminal of the three-phase power supply 1 with their phases switched. Further, the output voltages of the second, fourth, and sixth three-phase full-wave rectifier units 52, 54, and 56 also have a phase shift of 120 degrees from each other for the same reason. Therefore, there is a phase shift of 60° between the output voltages of all the three-phase full-wave rectifying units 51 to 56, and the quactors L1a to 56 have a phase shift of 60°.
The combined output current of each unit connected in parallel via L6b is extremely smooth in each mode.

第11図は上述の如くインバータ運転に於て要
求される出力直流電圧レベルに応じ6つのモード
に切替え非対称制御を行つた場合の制御角αと出
力電圧Edα/Edoの関係を示す特性図、第12
図は横軸に出力電圧Edα/Edo、縦軸に無効電
力Q/Edo・Id(但しQは基本波無効電力、Id
直流出力電流を示す)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による非対称制御に
よる場合aと通常の3相全波整流の場合bとを示
しており、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bにくらべ本発
明の場合aは1/6となつており無効電力の発生が
大巾に少くなつている。
Figure 11 shows the relationship between the control angle α and the output voltage E d α / E d o when asymmetric control is performed by switching to six modes according to the output DC voltage level required in inverter operation as described above. Characteristic diagram, 12th
The figure shows the output voltage E d α / E d o on the horizontal axis and the reactive power Q / E d o・I d on the vertical axis (however, Q is the fundamental wave reactive power and I d is the DC output current). For comparison, the power circle diagram shows the case of asymmetric control according to the present invention and the case of normal three-phase full-wave rectification, and as is clear from the figure, the arc in the power circle diagram In the case of the present invention, the radius of a is 1/6 of that of the normal three-phase full-wave system b, and the generation of reactive power is greatly reduced.

第13図は基本波力率cosφ1と出力電圧Edα/
Edoの関係を示すaは本発明によるもの、bは
通常の3相全波整流の場合である。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 13 shows the fundamental wave power factor cosφ 1 and the output voltage E d α/
A showing the relationship of E d o is the one according to the present invention, and b is the case of normal three-phase full-wave rectification. As is clear from the figure, the fundamental wave power factor in the low-medium power range has been greatly improved.

上記説明では簡単のため、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、必要とされる電圧、電流値によ
つてサイリスタ素子を直並列に接続しても、また
3相全波整流ユニツト自体の一個分を直並列或は
逆方向の出力電流が得られるよう逆並列に接続し
たものについても上記実施例と同様の効果を奏す
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。又第
4図〜第10図で説明した如く位相制御するサイ
リスタを選定したのは先に特許出願中の“整流装
置”(APE0124)記載の整流モード(UP又はUN
を制御角αで位相制御)も含めて各モード切替時
の出力電圧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51〜56の各3相全波
整流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, we have explained the most basic three-phase full-wave rectifier unit consisting of six thyristors, but depending on the required voltage and current values, thyristor elements can be connected in series and parallel. However, the same effect as in the above embodiment can be obtained even if one three-phase full-wave rectifier unit itself is connected in series-parallel or in anti-parallel so as to obtain an output current in the opposite direction. 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. In addition, as explained in Figs. 4 to 10, the thyristor that performs phase control was selected based on the rectification mode (UP or UN) described in the patent-pending "rectifier" (APE0124).
This is done to minimize fluctuations in the output voltage waveform when switching each mode, including phase control at the control angle α, to obtain smooth changes. If each of the three-phase full-wave rectifier units 51 to 56 are modified in the same way, the effects of the present invention will remain the same.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によれば、複数対の整
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
モードを切替え、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、無効電力の発生が
少い整流方式が得られる効果があり、且つ入力電
源の相を各対毎に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衝も防止出来る効果
がある。
As described above, according to the present invention, when performing inverter operation by connecting multiple pairs of rectifier units in parallel, the mode is switched according to the required output DC voltage level, and the switching elements constituting the rectifier units are asymmetrically connected. By controlling the ignition, it is possible to obtain a rectification system that has a good power factor even in the low output voltage range and generates little reactive power, and also allows the phases of the input power supply to be shifted for each pair. This has the effect of preventing 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〜第9図は第3図の
構成による整流装置の各モードに於ける出力電圧
波形、点弧サイリスタ、等価回路等点弧制御方式
を説明する図、第10図は第3図の構成による整
流装置によるサイリスタの各モードに於ける点弧
制御方式を示す一覧表、第11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12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13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、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相N側のサイリス
タ、51〜56はそれぞれNo.1〜No.6の3相全波
整流ユニツト、L1a,L1b〜L6a,L6b
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. The configuration diagram of the rectifier according to the embodiment, FIGS. 4 to 9 are diagrams explaining the output voltage waveform, firing thyristor, equivalent circuit, etc. in each mode of the rectifier having the configuration shown in FIG. 3, Fig. 10 is a list showing the firing control method in each mode of the thyristor by the rectifier having the configuration shown in Fig. 3, and Fig. 11 is a characteristic showing the relationship between the control angle α and the output voltage by the rectifier of the present invention. 12 is a power circle diagram showing the relationship between output voltage and reactive power, and FIG. 13 is a characteristic diagram showing the relationship between fundamental wave power factor and output voltage. 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, VN is the thyristor on the V phase N side, and WP is the W thyristor.
Thyristor on the phase P side, WN is the thyristor on the W phase N side, 51 to 56 are three-phase full wave rectifier units No. 1 to No. 6, respectively, L1a, L1b to L6a, L6b
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対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上記整流ユニツ
トの各対毎に互に異る相関係でそれぞれ接続する
とともに各整流ユニツトの出力端を共通接続し、
かつ上記それぞれの整流ユニツトをその発生し得
る直流出力電圧の値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3対設けられ、各対はそれ
ぞれ2個の3相全波整流ユニツトから成り、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Edo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1/6Edo(1−cosγ)〜−Edo/3cosγの
時 はモードI′で単相運転され、要求される出力電圧
が−Edo/3cosγ〜−2/3Edo cosγの時は上記モ ードI′とは異るモード′で単相運転され、要求
される出力電圧が の時はモード′Aで3相運転され、要求される出
力電圧が の時は上記′Aとは異るモード′Bで3相運転さ
れ、要求される出力電圧が の時は上記′ABとは異るモード′Aで3相運
転され、更に要求される出力電圧が の時は上記′A,′B,′Aとは異るモード′B
で3相運転される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、各対のそれぞれの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
とき、上記3相交流電源の出力端と各3対の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
各対毎に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及び負側出力端Nを
それぞれリアクトルを介して並列接続し且つ各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としたとき、モードI′の単相運転の時は、
各対を構成する2個の3相全波整流ユニツトのう
ちの一方はそれぞれ上記スイツチング素子VPを
位相制御、UPを2/3π−γで点弧、VNは常時導 通、UN,WP,WNは常時非導通となるよう制
御され、かつ各対を構成する2個の3相全波整流
ユニツトのうちの他方はそれぞれ上記スイツチン
グ素子VNを位相制御、UNを2/3π−γで点弧、 VPは常時導通、UP,WP,WNは常時非導通に
なるよう制御され、モード′の単相運転の時は、
各対を構成する2個の3相全波整流ユニツトのう
ちの一方はそれぞれ上記スイツチング素子VNを
位相制御、UP,UNを2/3π−γ、VPをπ−γ でそれぞれ点弧、WP,WNは常時不導通とする
よう制御され、かつ各対を構成する2個の3相全
波整流ユニツトのうち他方はそれぞれ上記スイツ
チング素子VPを位相制御、UP,UNを2/3π− γ、VNをπ−γでそれぞれ点弧、WP,WNは
常時不導通となるよう制御され、モード′Aの3
相運転の時は、各対を構成する2個の3相全波整
流ユニツトのうちの一方はそれぞれ上記スイツチ
ング素子VNを位相制御すると共にπ−γでも点
弧、UP,UNを2/3π−γ、VP,WNをπ−γ でそれぞれ点弧、WPは常時非導通となるよう制
御され、かつ各対を構成する2個の3相全波整流
ユニツトのうち他方はそれぞれ上記スイツチング
素子VPを位相制御すると共にπ−γでも点弧、
UP,UNを2/3π−γ、VN,WPをπ−γでそ れぞれ点弧、WNは常時非導通となるよう制御さ
れ、モード′Bの3相運転の時は各対を構成する
2個の3相全波整流ユニツトのうちの一方はそれ
ぞれ上記スイツチング素子UNを位相制御、UP
を2/3π−γ、VP,VN,WNをπ−γでそれぞ れ点弧しWPは常時非導通となるよう制御され、
かつ各対を構成する2個の3相全波整流ユニツト
のうちの他方はそれぞれ上記スイツチング素子
UPを位相制御、UNを2/3π−γ、VP,VN, WPをπ−γでそれぞれ点弧し、WNは常時非導
通となるよう制御され、モード′Aの3相運転の
時は各対を構成する2個の3相全波整流ユニツト
のうち一方はそれぞれ上記スイツチング素子VP
を位相制御すると共にπ−γでも点弧、UPを2/3 π−γ、UN,VN,WP,WNをπ−γでそれぞ
れ点弧するよう制御され、かつ各対を構成する2
個の3相全波整流ユニツトのうち他方はそれぞれ
上記スイツチング素子VNを位相制御すると共に
π−γでも点弧UNを2/3π−γ、UP,VP, WP,WNをπ−γでそれぞれ点弧するよう制御
され、モード′Bの3相運転の時は各対を構成す
る2個の3相全波整流ユニツトのうち一方はそれ
ぞれ上記スイツチング素子UPを位相制御、UN,
VP,VN,WP,WNをπ−γで点弧するよう制
御され、かつ各対を構成する2個の3相全波整流
ユニツトのうち他方はそれぞれ上記スイツチング
素子UNを位相制御、UP,VP,VN,WP,WN
をπ−γで点弧するよう制御されるようにし、更
に3対の整流ユニツトを構成する2個の3相全波
整流ユニツトは交流電源の一周期毎に点弧制御方
式を相互に切替える事を特徴とする特許請求の範
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 an output voltage of At the same time, connect the output ends of each rectifier unit in common,
A rectifying device characterized in that each of the rectifying units is operated in a single-phase operation mode or a multi-phase operation mode depending on the value of the DC output voltage that can be generated. 2 Each rectifier unit is provided in three pairs, each pair consisting of two three-phase full-wave rectifier units, and each three-phase full-wave rectifier unit has a maximum value of the DC output voltage that can be generated. When the value of the minimum control advance angle (γ limiter) is γ, when the required output voltage value is 1/6 E d o (1-cos γ) to -E d o/3 cos γ, single-phase operation is performed in mode I'. When the required output voltage is -E d o / 3 cos γ to -2/3 E d o cos γ, single-phase operation is performed in a mode ' different from the above mode I', and the required output voltage is When , three-phase operation is performed in mode ′ A , and the required output voltage is When , three-phase operation is performed in mode ' B , which is different from ' A ' above, and the required output voltage is When , three-phase operation is performed in mode `` A '' which is different from `` A '' B above, and the required output voltage is When , the mode ′ B is different from the above ′ A , ′ B , and ′ A .
The rectifying device according to claim 1, which is operated in three phases. 3 Set the output end phases of the 3-phase AC power supply to R phase, S phase, and T phase.
When the input terminal phases of each pair of three-phase full-wave rectifier units are respectively U phase, V phase, and W phase, the output terminal of the three-phase AC power supply and each three-phase full-wave rectifier unit are The connections to the input terminal of the rectifier unit are (R-U, S-V, T-W), (S-U, T-V,
R-W), (T-U, R-V, S-W) by changing the phase for each pair, and connecting the positive side output terminal P and negative side output of each three-phase full-wave rectifier unit. Terminals N are connected in parallel via reactors, and each 3
The U-phase P side of the switching elements constituting the phase full-wave rectifier unit is UP, the U-phase N side is UN, and the V-phase P side is
When VP, V-phase N side is VN, W-phase P side is WP, and W-phase N side is WN, in single-phase operation in mode I',
One of the two three-phase full-wave rectifier units that make up each pair controls the phase of the switching element VP, UP is fired at 2/3π-γ, VN is always conductive, and UN, WP, and WN are The other of the two three-phase full-wave rectifier units constituting each pair, which is controlled to be non-conductive at all times, controls the phase of the switching element VN, turns UN at 2/3π-γ, and VP. is always conductive and UP, WP, and WN are always non-conductive, and in single-phase operation in mode ′,
One of the two three-phase full-wave rectifier units constituting each pair controls the switching element VN in phase, ignites UP and UN at 2/3π-γ and VP at π-γ, respectively, and ignites WP, WN is controlled to be non-conductive at all times, and the other of the two three-phase full-wave rectifier units constituting each pair controls the phase of the switching element VP, and controls UP, UN by 2/3π-γ, VN. are ignited at π−γ, WP and WN are controlled to be always non-conducting, and mode ′ A is set to 3.
During phase operation, one of the two three-phase full-wave rectifier units constituting each pair controls the phase of the switching element VN, and also controls the ignition even at π-γ, and controls UP and UN at 2/3π-. γ, VP, and WN are ignited at π-γ, respectively, and WP is controlled to be non-conductive at all times, and the other of the two three-phase full-wave rectifier units constituting each pair is connected to the switching element VP, respectively. In addition to phase control, ignition is also possible at π-γ.
UP and UN are ignited at 2/3π-γ, VN and WP are ignited at π-γ, respectively, and WN is controlled to be always non-conducting, and when operating in 3-phase mode ' B , the two ignition units constituting each pair are One of the three-phase full-wave rectifier units controls the phase of the above-mentioned switching element UN, respectively.
is ignited at 2/3π-γ, VP, VN, and WN are ignited at π-γ, and WP is controlled so that it is always non-conducting.
The other of the two three-phase full-wave rectifier units constituting each pair is connected to the above-mentioned switching element.
UP is controlled in phase, UN is ignited at 2/3π-γ, VP, VN, and WP are ignited at π-γ, and WN is controlled to be always non-conducting. During 3-phase operation in mode ' A , each One of the two three-phase full-wave rectifier units forming the pair is connected to the above-mentioned switching element VP.
It is controlled in such a way that the phase of the
The other of the three-phase full-wave rectifier units controls the phase of the switching element VN, and also controls the ignition UN at 2/3π-γ and UP, VP, WP, and WN at π-γ. During three-phase operation in mode ' B , one of the two three-phase full-wave rectifier units constituting each pair controls the switching element UP, UN,
VP, VN, WP, and WN are controlled to ignite at π-γ, and the other of the two three-phase full-wave rectifier units forming each pair controls the switching elements UN in phase, UP, VP, respectively. ,VN,WP,WN
The two three-phase full-wave rectifier units constituting the three pairs of rectifier units are controlled to ignite at π-γ, and the ignition control method is mutually switched for each cycle of the AC power supply. A rectifying device according to claim 2, characterized in that:
JP59053887A 1984-03-21 1984-03-21 rectifier Granted JPS60197171A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59053887A JPS60197171A (en) 1984-03-21 1984-03-21 rectifier

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59053887A JPS60197171A (en) 1984-03-21 1984-03-21 rectifier

Publications (2)

Publication Number Publication Date
JPS60197171A JPS60197171A (en) 1985-10-05
JPH0216111B2 true JPH0216111B2 (en) 1990-04-16

Family

ID=12955237

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59053887A Granted JPS60197171A (en) 1984-03-21 1984-03-21 rectifier

Country Status (1)

Country Link
JP (1) JPS60197171A (en)

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JPS60197171A (en) 1985-10-05

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