JPS58212326A - Harmonic filter - Google Patents
Harmonic filterInfo
- Publication number
- JPS58212326A JPS58212326A JP57094488A JP9448882A JPS58212326A JP S58212326 A JPS58212326 A JP S58212326A JP 57094488 A JP57094488 A JP 57094488A JP 9448882 A JP9448882 A JP 9448882A JP S58212326 A JPS58212326 A JP S58212326A
- Authority
- JP
- Japan
- Prior art keywords
- harmonic
- filter
- capacitor
- reactor
- intermediate tap
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 230000000694 effects Effects 0.000 claims description 14
- 239000003990 capacitor Substances 0.000 claims description 11
- 238000010521 absorption reaction Methods 0.000 claims description 8
- 230000000903 blocking effect Effects 0.000 description 3
- 238000000034 method Methods 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/40—Arrangements for reducing harmonics
Landscapes
- Supply And Distribution Of Alternating Current (AREA)
- Filters And Equalizers (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】 タに係わる。[Detailed description of the invention] related to data.
・需要家において、電力変換設備のように高調波の発生
源を有するときは、これより発生する高調波除去のため
、高調波フィルタを設備する。- When a consumer has a source of harmonics, such as power conversion equipment, a harmonic filter is installed to remove the harmonics generated from this source.
第1図に需要家側疋設けられる通常の高調フィルタの概
略示す。図において、1は、例えば需要家に設値される
6相変換器であり、2はフィルタであり、3は交流電源
である。フィルタ2は高調波を発生する変換器1と並列
に接続される。高調波に対する電源インピーダンスをZ
s, ツーイルタインピーダンスをzF、変換器1よ
りの高調波電流をI。FIG. 1 schematically shows a normal harmonic filter provided on the consumer side. In the figure, 1 is, for example, a six-phase converter provided to a consumer, 2 is a filter, and 3 is an AC power source. Filter 2 is connected in parallel with converter 1 which generates harmonics. Power supply impedance for harmonics is Z
s, the tool tie impedance is zF, and the harmonic current from converter 1 is I.
とす扛ば、変換器運転時における需要家側より配で表わ
される。This is expressed as the distribution from the customer side when the converter is in operation.
この式で示すように、高調波フィルタ効果は、フィルタ
インピーダンスzFと高調波に対する電源インピーダン
スZsの相対関係で決定される。ところが、同−系統内
に例えば抑制対象とする6相ブリツチ変換器1以外の高
調波発生源がろると、これらの高調波がフィルタに入力
するため、フィ、ルタの設計には、対象物以外の高調波
源の調査が必要であり、フィルタ容量も過大なものとな
る。As shown in this equation, the harmonic filter effect is determined by the relative relationship between the filter impedance zF and the power source impedance Zs with respect to the harmonics. However, if there is a harmonic generation source other than the 6-phase blitz converter 1 to be suppressed in the same system, these harmonics will be input to the filter, so it is necessary to take into account the target object when designing the filter. It is necessary to investigate other harmonic sources, and the filter capacity will also be excessive.
このようなフィルタ容量の過大化防止対策として、第2
図に示すように、電源側に直列にブロッキング用リアク
トルCBR)4’を設置し、高調波フィルタに流入する
゛高調波電流分全ブロックする方式が試みられている。As a measure to prevent such an increase in filter capacity, the second
As shown in the figure, a method has been attempted in which a blocking reactor (CBR) 4' is installed in series on the power supply side to completely block the harmonic current flowing into the harmonic filter.
この方式において、高調波フィルタ効果を大きくするた
めには、BRの値を大きくしたいが、基本波の電圧降下
のため上限がある。In this method, in order to increase the harmonic filter effect, it is desirable to increase the value of BR, but there is an upper limit due to the voltage drop of the fundamental wave.
本発明は上述のような欠点を改善するため、1台のコン
デンサと1台の中間タップ付リアクトルで構成される高
調波吸収用フィルタにおいて、前記中間タップ欠有する
リブクトイレ8一端を電源に、中間タップを高調波発生
源となる負荷に、他端をコンデンサに接続した高調波フ
ィルタにあり、汎用性の高い高調波フィルタを提供する
ものである。In order to improve the above-mentioned drawbacks, the present invention provides a harmonic absorption filter composed of one capacitor and one reactor with an intermediate tap, in which one end of the rib toilet 8 lacking the intermediate tap is used as a power source, and the intermediate tap is connected to the intermediate tap. The harmonic filter has one end connected to a load that is a source of harmonics, and the other end connected to a capacitor, providing a highly versatile harmonic filter.
以下図面に示す実施例について説明する。The embodiments shown in the drawings will be described below.
第3図は本発明の実施例である。同一鉄心に巻かれた中
間タップ付リアクトル5の一端Pにおいて交流電源3に
接続され、中間夕・ンプSにより6相ブリツヂ変換器1
に接続され、他端Tにおいてコンデンサ6に接続される
。FIG. 3 shows an embodiment of the invention. A reactor with an intermediate tap 5 wound around the same iron core is connected to an AC power source 3 at one end P, and a six-phase bridge converter 1 is connected by an intermediate tap S.
The other end T is connected to the capacitor 6.
全体のコイル巻数を1+αとし、Pより中間夕・ノブ点
5t−rの巻数比を1、中間タップ点Sより他端Tまで
の巻数比をαとすれば、実施例は第4図に示す等価回路
で表わされる。If the overall number of turns of the coil is 1+α, the turns ratio from P to the intermediate tap point 5t-r is 1, and the turns ratio from the intermediate tap point S to the other end T is α, the embodiment is shown in FIG. Represented by an equivalent circuit.
コイル間の結合係数が100%とすればこの等価回路に
おいて、リアクタンスXpの大きさはl+α、リアクタ
ンスx5の大きさは一α、リアクタンスX丁の大きさは
α+α2になる。If the coupling coefficient between the coils is 100%, in this equivalent circuit, the magnitude of reactance Xp is l+α, the magnitude of reactance x5 is 1α, and the magnitude of reactance X is α+α2.
このような本実施例においてもすでに示した第2図のも
のと同様に、次のことを考慮する必要がある。
::1″
(1)基本波の電圧降下を少なくするため、中間タップ
付BRのリアクタンスに上限がある(負荷容量ベースで
4〜15%程度 第4図の等イ曲回ではXP+ x、=
1がこれに相当する〕。In this embodiment as well, as in the case shown in FIG. 2, the following needs to be taken into consideration.
::1'' (1) In order to reduce the voltage drop of the fundamental wave, there is an upper limit to the reactance of the BR with an intermediate tap (approximately 4 to 15% based on load capacity.
1 corresponds to this].
(2) 並列に接続されるコンデンサは、負荷の力率
改善も兼用するが、進相になるのを防ぐため、上限があ
る(負荷容量ベースでダイオードブリッヂで40%、サ
イリスタブリッヂで60%程度の進相容量であり、リア
クタンスで示せば250%と167%になる)。(2) Capacitors connected in parallel also serve to improve the power factor of the load, but there is an upper limit to prevent phase advance (40% for a diode bridge and 60% for a thyristor bridge based on load capacitance) (The phase advance capacity is 250% and 167% if expressed as reactance.)
以上のような條件を考慮して、中間タップ付BRの基本
波リアクタンスを6%、10%として、6相ダイオ−ド
ブリッチ負荷りおよび6相サイリスタブリツヂ負荷SC
Rについて、本発明実施における最適な定数を求め、更
に第2図のものと対比して高調仮吸収効果求めた。その
結果を表1に示す。なお、第2図との比較に於ては、第
2図のフィルタが、第5分路1組であ、9BRの値−と
コンデンサの進相容量が同じものであるとしており、表
1においてXcはコンデンサ基本波リアクタンスである
。従っ“て吸収効果とあるのは、第2図の高調波フィル
タとの対比であるが、本発明に於ては、−封←ミ季Hし
−BRの交流電源側等価リアク
タンスXPがBRの基本波リアクタンスよシも太きくな
る分だけ吸収効果が犬きくなる。Considering the above conditions, the fundamental wave reactance of the intermediate tapped BR is set to 6% and 10%, and the 6-phase diode bridge load and the 6-phase thyristor bridge load SC
Regarding R, the optimum constant for implementing the present invention was determined, and furthermore, the harmonic temporary absorption effect was determined by comparing it with that shown in FIG. The results are shown in Table 1. In comparison with Fig. 2, it is assumed that the filter in Fig. 2 has one set of fifth shunts, and the value of 9BR and the phase advance capacitance of the capacitor are the same, and in Table 1, Xc is the capacitor fundamental wave reactance. Therefore, the term "absorption effect" is a comparison with the harmonic filter shown in Fig. 2, but in the present invention, the equivalent reactance XP on the AC power supply side of BR is equal to The absorption effect becomes stronger as the fundamental wave reactance becomes thicker.
表 1
(a)Xo/X7=25=(5)2. Xp= (1
+ a)x BR、X7= (a+a”)XBR、吸収
効果=Xp/XBR、X、=−(yX BR第5図に表
1の4つ例につき、さらに高調波次数(n) につい
て、フィルタ効果を示した。フィルタ効果は電源側に流
出する高調波電流ISnと高調波発生源電流Inの比で
表わしている。Table 1 (a) Xo/X7=25=(5)2. Xp= (1
+ a) x BR, X7= (a+a”)XBR, absorption effect = Xp/XBR, The filter effect is expressed as the ratio of the harmonic current ISn flowing to the power supply side and the harmonic generation source current In.
表1ならびに第5図によれは、フィルタ効果Iri電源
側リアクタンスxPが大きい方が効果が太きい。According to Table 1 and FIG. 5, the larger the filter effect Iri and the power supply side reactance xP, the greater the effect.
この点本発明では相互リアクタンスを利用するととによ
り、1.4〜1.9倍の効果を得ることができる。In this regard, in the present invention, by utilizing mutual reactance, an effect of 1.4 to 1.9 times can be obtained.
また第2図に示す袋筒においては、BR4と第5高調波
分路用リアクトルの2台のりアクドルが必要であるが、
本発明によれば1台でよい。Furthermore, in the case of the bag cylinder shown in Fig. 2, two accelerators are required: BR4 and the reactor for the fifth harmonic shunt.
According to the present invention, only one device is required.
また第6図に示すようにSとTとの間に制動抵抗7を挿
入することにより、高次の高調波吸収効果を大きくする
ことができる。この場会抵抗は負荷容量ベースで100
〜100096程度に設定される。Further, by inserting a braking resistor 7 between S and T as shown in FIG. 6, the effect of absorbing higher harmonics can be increased. The field resistance is 100 based on the load capacity.
It is set to about 100096.
前記の実施例は高調波発生源をもつ三相負荷についての
説明であるが、単相負荷についても同様の効果を有する
ことはあきらかである。但し、定数につ′ハては別途配
慮する必要がある。Although the above embodiment describes a three-phase load having a harmonic generation source, it is clear that the same effect can be obtained for a single-phase load as well. However, it is necessary to give special consideration to constants.
以上説明したように、本発明によれば、サイリスタ、ダ
イオードのような高調波発生源をもつ回路のみでなく、
例えばテレビなどひろく高調波発生源を含む回路に通用
することができる。As explained above, according to the present invention, not only circuits having harmonic generation sources such as thyristors and diodes, but also
For example, it can be used in circuits that widely include harmonic generation sources, such as televisions.
4図面の簡単な説明 ′:1第1図は需要家
側に設けられる通常の高調波フィルタの一例Iである。4 Brief Explanation of the Drawings ':1 Figure 1 is an example I of a normal harmonic filter provided on the consumer side.
第2図は高調波流入を抑制する高調波フィルタの一例で
ある。FIG. 2 is an example of a harmonic filter that suppresses the inflow of harmonics.
第3図は本発明の一実施例を示す。FIG. 3 shows an embodiment of the invention.
第49は第3図実施例の等価回路を示す。49 shows an equivalent circuit of the embodiment of FIG. 3.
第5図は本発明による高調波吸収効果を示すグラフであ
る。FIG. 5 is a graph showing the harmonic absorption effect according to the present invention.
第6図は本発明の他の実施例を示す。FIG. 6 shows another embodiment of the invention.
1・・・6相ブリツジ変換器、高調波フィルタ、3・・
・父流宵源、4・・ブロッキング用リアクトル(BR)
、5・・・中間タップ付ブロッキング用リアクトル、6
・・・コンデンサ、7・制動抵抗。1... 6-phase bridge converter, harmonic filter, 3...
・Chichiryu Yoigen, 4...Blocking reactor (BR)
, 5... Blocking reactor with intermediate tap, 6
... Capacitor, 7. Braking resistor.
代理人 弁理士 青 木 秀 貫 −°÷11 芳1図 7r2図Agent Patent Attorney Hidekan Aoki −°÷11 Yoshi 1 figure 7r2 figure
Claims (3)
ルで構成される高調波吸収用フィルタにおいて、前記中
間タップを有するリアクトルの一端を電源に、中間タッ
プを高調波発生源に、他端をコンデンサに接続すること
を特徴とする高調波フィルタ。(1) In a harmonic absorption filter consisting of one capacitor and one reactor with an intermediate tap, one end of the reactor having the intermediate tap is used as a power source, the intermediate tap is used as a harmonic generation source, and the other end is used as a power source. A harmonic filter characterized by connecting a capacitor to a capacitor.
スを負荷容量ベースで4〜15%、前記リアクトルの巻
数比を04〜1.0、コンデンサの基本波リアクタンス
を150〜300%に選定することを特徴とする特許請
求の範囲第1項記載の高調波フィルタ。(2) The fundamental wave reactance of the intermediate tapped reactor is selected to be 4 to 15% based on the load capacity, the turns ratio of the reactor is selected to be 04 to 1.0, and the fundamental wave reactance of the capacitor is selected to be 150 to 300%. A harmonic filter according to claim 1.
トルの中間タップとコンデンサとの間に100〜100
0%の制動抵抗を挿入することを特徴とする特許請求の
範囲第1項または第2項記載の高調波フィルタ。(3) To improve the harmonic absorption effect, 100 to 100
3. The harmonic filter according to claim 1 or 2, wherein a 0% braking resistance is inserted.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57094488A JPS58212326A (en) | 1982-06-01 | 1982-06-01 | Harmonic filter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57094488A JPS58212326A (en) | 1982-06-01 | 1982-06-01 | Harmonic filter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58212326A true JPS58212326A (en) | 1983-12-10 |
| JPH0341007B2 JPH0341007B2 (en) | 1991-06-20 |
Family
ID=14111673
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57094488A Granted JPS58212326A (en) | 1982-06-01 | 1982-06-01 | Harmonic filter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58212326A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03143227A (en) * | 1989-10-25 | 1991-06-18 | Toyo Electric Mfg Co Ltd | Harmonic voltage suppressor |
| JPH03207222A (en) * | 1989-10-30 | 1991-09-10 | Fuji Electric Co Ltd | Higher harmonic suppressor |
| JPH04236129A (en) * | 1991-01-16 | 1992-08-25 | Fuji Electric Co Ltd | Higher harmonic preventing/suppressing device |
-
1982
- 1982-06-01 JP JP57094488A patent/JPS58212326A/en active Granted
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03143227A (en) * | 1989-10-25 | 1991-06-18 | Toyo Electric Mfg Co Ltd | Harmonic voltage suppressor |
| JPH03207222A (en) * | 1989-10-30 | 1991-09-10 | Fuji Electric Co Ltd | Higher harmonic suppressor |
| JPH04236129A (en) * | 1991-01-16 | 1992-08-25 | Fuji Electric Co Ltd | Higher harmonic preventing/suppressing device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0341007B2 (en) | 1991-06-20 |
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