JPH01293005A - Harmonic filter - Google Patents
Harmonic filterInfo
- 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
Links
- 230000007423 decrease Effects 0.000 claims 1
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 3
- 238000010521 absorption reaction Methods 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 239000002131 composite material Substances 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
Landscapes
- Filters And Equalizers (AREA)
Abstract
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.
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.
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.
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.
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.
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.
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.
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 fFigure 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)
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.
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)
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 |
-
1988
- 1988-05-20 JP JP12213888A patent/JPH01293005A/en active Pending
Cited By (3)
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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