JPH01293005A - Harmonic filter - Google Patents

Harmonic filter

Info

Publication number
JPH01293005A
JPH01293005A JP12213888A JP12213888A JPH01293005A JP H01293005 A JPH01293005 A JP H01293005A JP 12213888 A JP12213888 A JP 12213888A JP 12213888 A JP12213888 A JP 12213888A JP H01293005 A JPH01293005 A JP H01293005A
Authority
JP
Japan
Prior art keywords
frequency
impedance
capacitance
inductance
value
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.)
Pending
Application number
JP12213888A
Other languages
Japanese (ja)
Inventor
Katsutake Tsuboi
坪井 克剛
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 JP12213888A priority Critical patent/JPH01293005A/en
Publication of JPH01293005A publication Critical patent/JPH01293005A/en
Pending legal-status Critical Current

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  • Filters And Equalizers (AREA)

Abstract

PURPOSE:To obtain a harmonic filter which has excellent higher harmonic absorbing characteristics and can be miniaturized by constituting an inductance with a superconducting coil. CONSTITUTION:A series resonance circuit is constituted of the superconducting coil 6 and a capacitance 2. The frequency characteristics of the resultant impedance of the coil 6 and capacitance 2 show the lowest impedance Z0 at a resonance frequency fo as indicated by the Z1+2 of the appended figure. The frequency characteristics of power source impedance Z4, moreover, is as shown in the figure. Therefore, when the resonance frequency fo which can be set by using the L-value of the coil 6 and C-value of the capacitance 2 is selected so that the frequency fo can coincide with the frequency of a higher harmonic current, the value of the power source impedance Z4 becomes Zo at the resonance frequency fo. Therefore, it is possible to cause the higher harmonic current In flowing out of a nonlinear load 5 to be absorbed by the series resonance circuit so that the current cannot flow out to a power source.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は高調波フィルタに関するものである。[Detailed description of the invention] [Industrial application field] This invention relates to a harmonic filter.

〔従来の技術〕[Conventional technology]

第3図は従来の高調波フィルタを示す回路図であり、図
において、1はインダクタンス、2はインダクタンス1
に直列に接続されたキャパシタンスで、このキャパシタ
ンス2とインダクタンス1とで直列共振回路を構成する
。3は電源、4は電源3のインピーダンス、5は非線形
負荷で、この非線形負荷5は直列共振回路を介して接地
されている。
Figure 3 is a circuit diagram showing a conventional harmonic filter. In the figure, 1 is the inductance, 2 is the inductance 1
This capacitance 2 and inductance 1 constitute a series resonant circuit. 3 is a power supply, 4 is an impedance of the power supply 3, and 5 is a nonlinear load, and this nonlinear load 5 is grounded via a series resonant circuit.

次に動作について説明する。インダクタンス1とキャパ
シタンス2との合成インピーダンスz1+2の周波数特
性は第4図に21+2として示すように、共振周波数f
0で最低インピーダンスZoを示すのは周知の通りであ
る。一方、電源のインピーダンス4の周波数特性は第4
図にZ、として示すようになる。インダクタンス1の値
りとキャパシタンス2の値Cをその共振周波数f0と一
致するように選び、その共振周波数f0において、電源
インピーダンスZ4の値が2.> 2゜どなるように選
ぶことによって、非線形負荷5から流出した高調波電流
Inをインダクタンス1とキャパシタンス2側に吸収し
、電源3側にできるだけ流出させないようにする。
Next, the operation will be explained. The frequency characteristic of the composite impedance z1+2 of inductance 1 and capacitance 2 is the resonance frequency f, as shown as 21+2 in Figure 4.
It is well known that the minimum impedance Zo is 0. On the other hand, the frequency characteristic of impedance 4 of the power supply is
It is shown as Z in the figure. The value of inductance 1 and the value C of capacitance 2 are selected to match the resonance frequency f0, and at the resonance frequency f0, the value of power supply impedance Z4 is 2. > 2°, the harmonic current In flowing out from the nonlinear load 5 is absorbed into the inductance 1 and capacitance 2 side, and is prevented from flowing to the power source 3 side as much as possible.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

従来の高調波フィルタは以上のように構成されているの
で、電源3側に流出する高調波電流は非線形負荷5から
流出した高調波型、流InのZo/(Z 4 +Z o
 )となる、また、電源インピーダンスZ4は電源1の
条件より決まるもので、広い範囲で任意に選べるもので
はない、従って、フィルタの性能を上げるには最低イン
ピーダンスZoをより小さくしなければならない、とこ
ろが、最低インピーダンスZ0はほとんどインダクタン
ス1の内部抵抗やインダクタンス1に使われる鉄心の鉄
損などにより制限され無制限に小さくすることはできな
いという問題点があった。
Since the conventional harmonic filter is configured as described above, the harmonic current flowing out to the power supply 3 side is the harmonic type flowing out from the nonlinear load 5.
), and the power supply impedance Z4 is determined by the conditions of the power supply 1, and cannot be arbitrarily selected within a wide range. Therefore, in order to improve the filter performance, the minimum impedance Zo must be made smaller. However, there is a problem in that the minimum impedance Z0 is almost limited by the internal resistance of the inductance 1 and the iron loss of the iron core used for the inductance 1, and cannot be reduced indefinitely.

この発明は上記のような問題点を解消するためになされ
たもので、小形で吸収特性の良い高調波フィルタを得る
ことを目的とする。
This invention was made to solve the above-mentioned problems, and an object thereof is to obtain a harmonic filter that is small and has good absorption characteristics.

〔課題を解決するための手段〕[Means to solve the problem]

この発明に係る高調波フィルタは直列共振回路のインダ
クタンスを超電導コイルで構成したものである。
The harmonic filter according to the present invention is one in which the inductance of a series resonant circuit is composed of a superconducting coil.

〔作 用〕[For production]

この発明におけるインダクタンスは低損失であるため、
低いインピーダンスとすることができ、吸収特性の良い
ものが得られる。
Since the inductance in this invention has low loss,
Low impedance can be obtained, and good absorption characteristics can be obtained.

〔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1
図において、キャパシタンス2、電源3、電源3のイン
ピーダンス4および非線形負荷5は第3図に示した従来
例と同一なので、それらの説明は省略する。6はキャパ
シタンス2と直列接続される超電導コイルで、この超電
導コイル6とキャパシタンス2とで直列共振回路を構成
する。
An embodiment of the present invention will be described below with reference to the drawings. 1st
In the figure, the capacitance 2, the power source 3, the impedance 4 of the power source 3, and the nonlinear load 5 are the same as those in the conventional example shown in FIG. 3, so their explanation will be omitted. A superconducting coil 6 is connected in series with the capacitance 2, and the superconducting coil 6 and the capacitance 2 constitute a series resonant circuit.

次に動作について説明する。Next, the operation will be explained.

超電導コイル6とキャパシタンス2との合成インピーダ
ンスの周波数特性は第2図に21+1として示すように
共振周波数f0で最低インピーダンスZ0を示す、また
、電源インピーダンスZ4の周波数特性は第2図に示す
とおりである。よって、超電導コイル6のL値とキャパ
シタンス2のC値とにより設定できる共振周波数f0を
吸収すべき高調波電流周波数に一致するように選ぶこと
によってその共振周波数foにおいて、電源インピーダ
ンスZ4の値がZ−>Zoとなる。したがって、非線形
負荷5から流出した高調波電流Inを直列共振回路側に
吸収させ、電源3に流出させないようにすることができ
る。
The frequency characteristics of the combined impedance of the superconducting coil 6 and the capacitance 2 are as shown in FIG. 2 as 21+1, which shows the lowest impedance Z0 at the resonance frequency f0, and the frequency characteristics of the power supply impedance Z4 are as shown in FIG. . Therefore, by selecting the resonant frequency f0, which can be set by the L value of the superconducting coil 6 and the C value of the capacitance 2, to match the frequency of the harmonic current to be absorbed, the value of the power supply impedance Z4 can be changed to Z at the resonant frequency fo. ->Zo. Therefore, the harmonic current In flowing out from the nonlinear load 5 can be absorbed by the series resonant circuit side, and can be prevented from flowing out to the power supply 3.

〔発明の効果〕〔Effect of the invention〕

以上のようにこの発明によれば直列共振回路のインダク
タンスを超電導コイルにより構成したので、高調波吸収
特性の非常によく、また装置の小形化が可能なものが得
られる効果がある。
As described above, according to the present invention, since the inductance of the series resonant circuit is constituted by a superconducting coil, it is possible to obtain an apparatus which has very good harmonic absorption characteristics and can be miniaturized.

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

第1図はこの発明の一実施例による高調波フィルタを示
す回路図、第2図はその周波数特性、第3図は従来の高
調波フィルタを示す回路図、第4図はその周波数特性で
ある。 2はキャパシタンス、6は超電導コイル。 なお、図中、同一符号は同一または相当部分を示す。 第1図 og f
Figure 1 is a circuit diagram showing a harmonic filter according to an embodiment of the present invention, Figure 2 is its frequency characteristics, Figure 3 is a circuit diagram showing a conventional harmonic filter, and Figure 4 is its frequency characteristics. . 2 is a capacitance, and 6 is a superconducting coil. In addition, in the figures, the same reference numerals indicate the same or corresponding parts. Figure 1 og f

Claims (1)

【特許請求の範囲】[Claims]  インダクタンスとキャパシタンスとを直列接続した直
列共振回路の直列共振点でインピーダンスが低下するこ
とを利用して特定周波数の電流を吸収するようにした高
調波フィルタにおいて、上記インダクタンスを超電導コ
イルで構成したことを特徴とする高調波フィルタ。
In a harmonic filter that absorbs current at a specific frequency by taking advantage of the fact that the impedance decreases at the series resonance point of a series resonant circuit in which an inductance and a capacitance are connected in series, the above inductance is constructed with a superconducting coil. Characteristic harmonic filter.
JP12213888A 1988-05-20 1988-05-20 Harmonic filter Pending JPH01293005A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12213888A JPH01293005A (en) 1988-05-20 1988-05-20 Harmonic filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12213888A JPH01293005A (en) 1988-05-20 1988-05-20 Harmonic filter

Publications (1)

Publication Number Publication Date
JPH01293005A true JPH01293005A (en) 1989-11-27

Family

ID=14828553

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12213888A Pending JPH01293005A (en) 1988-05-20 1988-05-20 Harmonic filter

Country Status (1)

Country Link
JP (1) JPH01293005A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2008052509A1 (en) * 2006-11-03 2008-05-08 Conti Temic Microelectronic Gmbh Energy supply device for an electrical circuit
US8745850B2 (en) 2009-12-18 2014-06-10 International Business Machines Corporation Method of manufacturing superconducting low pass filter for quantum computing

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2008052509A1 (en) * 2006-11-03 2008-05-08 Conti Temic Microelectronic Gmbh Energy supply device for an electrical circuit
US8111049B2 (en) 2006-11-03 2012-02-07 Conti Temic Microelectronic Gmbh Power supply device for an electric circuit
US8745850B2 (en) 2009-12-18 2014-06-10 International Business Machines Corporation Method of manufacturing superconducting low pass filter for quantum computing

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