JPH0340077Y2 - - Google Patents

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Publication number
JPH0340077Y2
JPH0340077Y2 JP9910885U JP9910885U JPH0340077Y2 JP H0340077 Y2 JPH0340077 Y2 JP H0340077Y2 JP 9910885 U JP9910885 U JP 9910885U JP 9910885 U JP9910885 U JP 9910885U JP H0340077 Y2 JPH0340077 Y2 JP H0340077Y2
Authority
JP
Japan
Prior art keywords
phase
resistor
reactor
harmonic filter
capacitor
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
Application number
JP9910885U
Other languages
Japanese (ja)
Other versions
JPS627775U (en
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 filed Critical
Priority to JP9910885U priority Critical patent/JPH0340077Y2/ja
Publication of JPS627775U publication Critical patent/JPS627775U/ja
Application granted granted Critical
Publication of JPH0340077Y2 publication Critical patent/JPH0340077Y2/ja
Expired legal-status Critical Current

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  • Power Conversion In General (AREA)

Description

【考案の詳細な説明】 〔考案の技術的分野〕 本考案は電力用高調波フイルタ装置に関する。[Detailed explanation of the idea] [Technical field of invention] The present invention relates to a power harmonic filter device.

〔考案の技術的背景とその問題点〕[Technical background of the invention and its problems]

近年サイリスタなどの半導体を利用した電気機
器が増え、これらの機器から流出する高調波電流
により電力回路に高調波が増加し、多くの高調波
障害が発生している。これら半導体応用装置から
発生する高調波を吸収して電力系統に流出するの
を抑制するために、コンデンサとリアクトルおよ
び抵抗などからなる高調波フイルタ装置が使用さ
れている。
In recent years, the number of electrical devices using semiconductors such as thyristors has increased, and the harmonic current flowing out from these devices increases harmonics in power circuits, causing many harmonic disturbances. In order to absorb harmonics generated from these semiconductor application devices and suppress them from flowing into the power system, a harmonic filter device consisting of a capacitor, a reactor, a resistor, and the like is used.

高調波フイルタはリアクトルとコンデンサの共
振現象を利用して特定の周波数領域のインピーダ
ンスを小さくして高調波電流を流入させるもので
あり、リアクトルとコンデンサおよび抵抗の組み
合せで構成される。その中でリアクトルと抵抗を
並列に接続し、これにコンデンサを直列に配列し
た回路構成を二次形高調波フイルタという。従来
の二次形高調波フイルタ装置は、第6図に示すよ
うに、三相リアクトル2と三相抵抗3を並列に接
続した回路に三相コンデンサ1を直列に接続して
構成され、三相リアクトル2と三相抵抗3はとも
に星形に結線し、その中性点間を接続線5にて接
続している。
A harmonic filter uses the resonance phenomenon of a reactor and a capacitor to reduce the impedance in a specific frequency range and allow harmonic current to flow in, and is made up of a combination of a reactor, a capacitor, and a resistor. A circuit configuration in which a reactor and a resistor are connected in parallel, and a capacitor is arranged in series with this is called a quadratic harmonic filter. As shown in Fig. 6, the conventional quadratic harmonic filter device is constructed by connecting a three-phase capacitor 1 in series to a circuit in which a three-phase reactor 2 and a three-phase resistor 3 are connected in parallel. Both the reactor 2 and the three-phase resistor 3 are connected in a star shape, and their neutral points are connected by a connecting wire 5.

しかして、近時電力機器の小形化のために、機
器の接続母線を油入管路またはガス絶縁管路で構
成した縮小形設備が採用されている。これに併せ
て、前記高調波フイルタ装置にこの構成をとり入
れると、三相コンデンサ1、三相リアクトル2お
よび三相抵抗3の各機器を接続母線で接続するこ
とになるが、この種装置では三相コンデンサ1に
急峻なサージが侵入すると三相リアクトル2や三
相抵抗3の中性点Nの電位を上昇させるので、特
に中性点側の絶縁に配慮が必要となる。このた
め、各機器の中性点ブツシングや中性点側の接続
母線に絶縁耐力の高いものを使用しなければなら
ず、機器の絶縁や接続母線が複雑になる欠点があ
つた。
Recently, in order to downsize electric power equipment, downsized equipment in which the connecting busbar of the equipment is constructed of an oil-filled pipe or a gas-insulated pipe has been adopted. In addition, if this configuration is adopted in the harmonic filter device, the three-phase capacitor 1, the three-phase reactor 2, and the three-phase resistor 3 will be connected by a connection bus, but in this type of device, When a steep surge enters the phase capacitor 1, the potential at the neutral point N of the three-phase reactor 2 and the three-phase resistor 3 increases, so special consideration must be given to the insulation on the neutral point side. For this reason, it is necessary to use materials with high dielectric strength for the neutral point bushing of each device and the connection bus bar on the neutral point side, which has the disadvantage that the insulation of the device and the connection bus bar are complicated.

〔考案の目的〕[Purpose of invention]

本考案は、各機器や接続母線の構成を簡素化
し、加えて据付工事や据付スペースの縮少を計つ
た安価な電力用高調波フイルタ装置を提供するこ
とを目的とする。
The purpose of the present invention is to provide an inexpensive power harmonic filter device that simplifies the configuration of each device and connection busbar, and also reduces installation work and installation space.

〔考案の概要〕[Summary of the idea]

本考案による電力用高調波フイルタ装置は、電
源側に三相コンデンサを配置し、さらにこれに接
続される三相リアクトルおよび抵抗をそれぞれ星
形に結線するが、それらの中性点は機器の外部に
導出しないよう構成したことを特徴とするもので
ある。
The power harmonic filter device according to the present invention has a three-phase capacitor placed on the power supply side, and the three-phase reactor and resistor connected to this are connected in a star shape, but their neutral point is outside the device. This feature is characterized in that it is configured so that it is not derived.

〔考案の実施例〕[Example of idea]

以下本考案を第1図に示す実施例について説明
する。三相コンデンサ1は、一方を電源側端子4
とし、他方を負荷側端子5としてこの負荷側端子
5に三相リアクトル2と三相抵抗3とを並列接続
する。この三相リアクトル2および三相抵抗3は
それぞれ星形に結線されているが、その中性点N
はそれぞれの機器内にあつて外部には導出しない
ように構成する。このため、この電力用高調波フ
イルタ装置を密閉構造の縮少形設備に構成する場
合には、三相コンデンサ1と三相リアクトル2お
よび三相抵抗3の相互間のみを油入管路の接続母
線で接続することになる。
The present invention will be described below with reference to an embodiment shown in FIG. The three-phase capacitor 1 has one end connected to the power supply side terminal 4.
The other terminal is used as a load-side terminal 5, and a three-phase reactor 2 and a three-phase resistor 3 are connected in parallel to this load-side terminal 5. The three-phase reactor 2 and three-phase resistor 3 are connected in a star shape, and their neutral point N
are configured so that they are located within each device and are not exposed to the outside. Therefore, when configuring this power harmonic filter device as a reduced-sized equipment with a sealed structure, only the connections between the three-phase capacitor 1, the three-phase reactor 2, and the three-phase resistor 3 are connected to the connecting bus of the oil-filled pipe. It will be connected with.

ここで、三相リアクトル2と三相抵抗3の中性
点N間を直接に接続しなくても高調波フイルタと
しての特性が変らないことを説明する。
Here, it will be explained that the characteristics as a harmonic filter do not change even if the neutral point N of the three-phase reactor 2 and the three-phase resistor 3 are not directly connected.

第6図に於いて三相リアクトル2の各相のリア
クタンスLと三相抵抗3の各相の抵抗Rはそれぞ
れ並列となつており、この合成インピーダンスZ
を計算すると次式となる。
In Fig. 6, the reactance L of each phase of the three-phase reactor 2 and the resistance R of each phase of the three-phase resistor 3 are connected in parallel, and this composite impedance Z
The calculation results in the following formula.

Z=jωL・R/R+jωL …(1) こゝでωは角速度で周波数をHz、円周率をπ
とすると2πに等しい。
Z=jωL・R/R+jωL …(1) Here, ω is the angular velocity, the frequency is Hz, and pi is π.
Then, it is equal to 2π.

第2図は第1図に示す本考案の高調波フイルタ
装置の等価回路図でコンデンサの一相分の静電容
量をC、一相分のリアクタンスをL、一相分の抵
抗をRとして示してある。
Figure 2 is an equivalent circuit diagram of the harmonic filter device of the present invention shown in Figure 1, where C is the capacitance for one phase of the capacitor, L is the reactance for one phase, and R is the resistance for one phase. There is.

この回路をインピーダンスの等しい三角結線に
変換すると第3図となる。第3図で三角結線の一
辺に相当する一相分のリアクタンスをL′、一相分
の抵抗をR′とすると第2図に示す回路と第3図
に示す回路とが等価なインピーダンスとなるため
には、 L′=3L,R′=3R …(2) の関係になければならない。
When this circuit is converted into a triangular connection with equal impedance, the result is shown in FIG. In Figure 3, if the reactance for one phase corresponding to one side of the triangular connection is L', and the resistance for one phase is R', the circuit shown in Figure 2 and the circuit shown in Figure 3 have equivalent impedance. In order to do so, the relationship L′=3L, R′=3R…(2) must exist.

第3図をリアクトルL′と抵抗R′のそれぞれの三
角結線を重ねる様に描くと第4図となる。こゝで
各相のリアクタンスL′と抵抗R′はそれぞれ並列と
なつており、この両者の合成インピーダンスを
Z′とすると次式となる。
If Figure 3 is drawn so that the triangular connections of reactor L' and resistor R' are overlapped, Figure 4 is obtained. Here, the reactance L′ and resistance R′ of each phase are connected in parallel, and the combined impedance of both is
Letting Z' be the following equation.

Z′=jωL′・R′/R′+jωL′ …(3) 第4図でリアクタンスL′と抵抗R′の合成インピ
ーダンスZ′は三角結線であるがこれを等価なイン
ピーダンスを有する星形結線に変換すると第5図
となる。この図で変換された星形結線のインピー
ダンスの一相分をZとすると、Z=Z′/3の関係
にある。従つて(2)式と(3)式の関係を用いてZを求
めると次のようになる。
Z'=jωL'・R'/R'+jωL'...(3) In Figure 4, the combined impedance Z' of reactance L' and resistance R' is a triangular connection, but it can be changed to a star connection with equivalent impedance. When converted, it becomes Figure 5. If Z is one phase of the impedance of the converted star-shaped connection in this figure, then there is a relationship of Z=Z'/3. Therefore, when calculating Z using the relationship between equations (2) and (3), the result is as follows.

Z=Z′/3 =jωL′・R′/3(R′+jωL′) =jωL・R/R+jωL …(4) 即ち従来のリアクトル2および抵抗3の中性点
Nを接続線6で結んだ構成のインピーダンスであ
る(1)式と本考案の構成のインピーダンスである(4)
式とは同一の値となり、高調波フイルタとしての
特性が変わらないことが判る。
Z=Z'/3 =jωL'・R'/3(R'+jωL') =jωL・R/R+jωL...(4) In other words, the neutral point N of the conventional reactor 2 and resistor 3 is connected with the connecting wire 6. Equation (1), which is the impedance of the configuration, and (4), which is the impedance of the configuration of the present invention.
The value is the same as the formula, and it can be seen that the characteristics as a harmonic filter do not change.

このように、三相リアクトル2および三相抵抗
3の中性点端子Nを外部に引出さないため、中性
点ブツシングおよび中性点側接続母線が不要とな
り、しかも急峻なサージの侵入による中性点Nの
電位の上昇に対しても機器内部の絶縁で充分に対
応でき、特別に絶縁を強化する部分がなくなる。
In this way, since the neutral point terminal N of the three-phase reactor 2 and three-phase resistor 3 is not drawn out, the neutral point bushing and the neutral point side connection bus bar are not required, and moreover, the neutral point terminal N of the three-phase reactor 2 and the three-phase resistor 3 is not drawn out. The internal insulation of the device can sufficiently cope with the increase in the potential of the electric point N, and there is no need to specially strengthen the insulation.

さらに中性点N側には従来のような接続線がな
いため三相リアクトル2と三相抵抗3の配置に自
由度が増し、接続母線の低減と相俟つて据付スペ
ース、据付工事の縮少が図れて安価に構成でき
る。
Furthermore, since there is no connection line on the neutral point N side, there is more freedom in the placement of the three-phase reactor 2 and three-phase resistor 3, which reduces the number of connection buses and reduces installation space and installation work. can be configured at low cost.

〔考案の効果〕[Effect of idea]

以上のように本考案によれば、三相コンデンサ
を電源側に配置し、さらに三相リアクトルおよび
三相抵抗をそれぞれ星形結線とし、かつその中性
点を互いに接続しないことにより、中性点の接続
線が不用になることから、機器の絶縁や接続母線
の低減が図れるとともに据付工事や据付スペース
が縮少され安価に構成できる利点を有する。
As described above, according to the present invention, the three-phase capacitor is placed on the power supply side, the three-phase reactor and the three-phase resistor are connected in a star shape, and their neutral points are not connected to each other. This eliminates the need for connecting wires, which reduces equipment insulation and connection busbars, reduces installation work and installation space, and has the advantage of being inexpensive.

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

第1図は本考案による電力用高調波フイルタ装
置の一実施例を示す回路図、第2図ないし第5図
は本考案の作用を説明するための種々の等価回路
図、第6図は従来の高調波フイルタ装置を示す回
路図である。 1……三相コンデンサ、2……三相リアクト
ル、3……三相抵抗、4……電源側端子、5……
負荷側端子。
Fig. 1 is a circuit diagram showing one embodiment of a power harmonic filter device according to the present invention, Figs. 2 to 5 are various equivalent circuit diagrams for explaining the operation of the present invention, and Fig. 6 is a conventional circuit diagram. FIG. 2 is a circuit diagram showing a harmonic filter device of FIG. 1... Three-phase capacitor, 2... Three-phase reactor, 3... Three-phase resistor, 4... Power supply side terminal, 5...
Load side terminal.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 三相リアクトルと三相抵抗を並列に接続しこれ
と直列に三相コンデンサを接続してなる電力用高
調波フイルタ装置において、三相コンデンサを電
源側に配置し、さらに三相リアクトルおよび三相
抵抗をそれぞれ星形に結線しかつその中性点を互
に接続しないことを特徴とする電力用高調波フイ
ルタ装置。
In a power harmonic filter device that consists of a three-phase reactor and three-phase resistor connected in parallel and a three-phase capacitor connected in series, the three-phase capacitor is placed on the power supply side, and the three-phase reactor and three-phase resistor are connected in series. A power harmonic filter device characterized in that the wires are connected in a star shape, and their neutral points are not connected to each other.
JP9910885U 1985-07-01 1985-07-01 Expired JPH0340077Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9910885U JPH0340077Y2 (en) 1985-07-01 1985-07-01

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9910885U JPH0340077Y2 (en) 1985-07-01 1985-07-01

Publications (2)

Publication Number Publication Date
JPS627775U JPS627775U (en) 1987-01-17
JPH0340077Y2 true JPH0340077Y2 (en) 1991-08-22

Family

ID=30967688

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9910885U Expired JPH0340077Y2 (en) 1985-07-01 1985-07-01

Country Status (1)

Country Link
JP (1) JPH0340077Y2 (en)

Also Published As

Publication number Publication date
JPS627775U (en) 1987-01-17

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