JPH0629884A - High frequency power injecting device - Google Patents

High frequency power injecting device

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Publication number
JPH0629884A
JPH0629884A JP20298292A JP20298292A JPH0629884A JP H0629884 A JPH0629884 A JP H0629884A JP 20298292 A JP20298292 A JP 20298292A JP 20298292 A JP20298292 A JP 20298292A JP H0629884 A JPH0629884 A JP H0629884A
Authority
JP
Japan
Prior art keywords
oscillator
reactor
high frequency
output
frequency
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
JP20298292A
Other languages
Japanese (ja)
Inventor
Atsushi Nishidai
惇 西台
Tomoshi Tada
知史 多田
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.)
Nissin Electric Co Ltd
Original Assignee
Nissin Electric Co Ltd
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 Nissin Electric Co Ltd filed Critical Nissin Electric Co Ltd
Priority to JP20298292A priority Critical patent/JPH0629884A/en
Publication of JPH0629884A publication Critical patent/JPH0629884A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To provide the subject device with a compact and inexpensive configuration by reducing the output capacity of a high frequency oscillator. CONSTITUTION:The device is provided with a reactor 7 inserted in series into an electric power system, a secondary induction winding wire 8 added to this reactor 7, and a high frequency oscillator 6 for supplying an oscillation output to the secondary induction winding wire 8 through a blocking capacitor 9 for obstructing a system voltage. Even if an excitation impedance of the reactor 7 is small, and a secondary circuit becomes an open state against a commercial frequency of the system by the capacitor 9, an induced voltage of the commercial frequency between its terminals does not become excessive, and also, it is obstructed by the capacitor 9 that a current of a commercial frequency flows into the oscillator 6, therefore, a necessary output capacity of the oscillator 6 is reduced.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、電力系統に高周波電力
を注入する高周波電力注入装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a high frequency power injection device for injecting high frequency power into a power system.

【0002】[0002]

【従来の技術】従来、電力系統に電力線搬送制御信号或
いは波形歪みの補正信号として高周波電力を注入する場
合、図3に示す並列注入方式の高周波電力注入装置又は
図4に示す直列注入方式の高周波電力注入装置が用いら
れる。
2. Description of the Related Art Conventionally, when injecting high frequency power into a power system as a power line carrier control signal or a waveform distortion correction signal, a parallel injection type high frequency power injection device shown in FIG. 3 or a serial injection type high frequency shown in FIG. A power injection device is used.

【0003】それらの図面において、1は商用電源、2
は電源1のインピーダンスを示す等価インダクタンス、
3及び4は電力系統の線路インピーダンスを示す等価イ
ンダクタンス,等価コンデンサ、5は系統負荷、6は高
周波電力注入用の高周波発振器であり、図3では電源1
に並列接続されて電力系統に並列に設けられ、図4では
電源1に直列接続されて電力系統に直列に挿入されてい
る。そして、図3の場合は発振器6の高周波電力が電力
系統に並列注入され、図4の場合は発振器6の高周波電
力が電力系統に直列注入される。
In these drawings, 1 is a commercial power source, 2
Is an equivalent inductance indicating the impedance of the power supply 1,
3 and 4 are equivalent inductances and equivalent capacitors showing line impedance of the power system, 5 is a system load, and 6 is a high frequency oscillator for high frequency power injection.
Is connected in parallel to the power system and is provided in parallel to the power system. In FIG. 4, the power source 1 is connected in series and inserted in the power system in series. Then, in the case of FIG. 3, the high frequency power of the oscillator 6 is injected in parallel to the power system, and in the case of FIG. 4, the high frequency power of the oscillator 6 is injected in series to the power system.

【0004】[0004]

【発明が解決しようとする課題】前記図3,図4の従来
装置の場合、いずれも発振器6の出力をそのまま又は変
圧器を介して電力系統に注入するため、発振器6として
出力容量(電力)の極めて大きなものを要し、大型かつ
高価な構成になる問題点がある。
In the conventional devices shown in FIGS. 3 and 4, the output of the oscillator 6 is injected into the power system as it is or through a transformer, so that the output capacity (electric power) of the oscillator 6 is increased. However, there is a problem that a large and expensive structure is required.

【0005】すなわち、図3,図4において、定格の系
統電圧,系統電流(負荷電流)をVS ,IS とし、発振
器6の出力電圧,注入電流をVH ,IH とすると、その
出力電力はVS ・IH (図3の並列注入方式),IS
H (図4の直列注入方式)で示される。
That is, in FIGS. 3 and 4, if the rated system voltage and system current (load current) are V S and I S, and the output voltage and injection current of the oscillator 6 are V H and I H , the output Electric power is V S · I H (parallel injection method in FIG. 3), I S ·
V H (series injection method of FIG. 4).

【0006】そして、電力系統の電源インピーダンスを
定格容量ベースで5%とし、発振器6の出力周波数を商
用電源1の20倍の1KHzとすると、系統電圧の5%
の適当な高周波電圧を系統に発生するには、図3の場合
はつぎの数1の式に示すように注入電流IH として系統
電流IS の5%の電流を要し、同様に、図4の場合は出
力電圧VH として系統電圧VS の5%の電圧を要する。
If the power source impedance of the power system is 5% based on the rated capacity and the output frequency of the oscillator 6 is 1 KHz, which is 20 times the commercial power source 1, then 5% of the system voltage.
In order to generate an appropriate high frequency voltage of 3 in the system in the case of FIG. 3, 5% of the system current I S is required as the injection current I H as shown in the following equation (1). In this case, 5% of the system voltage V S is required as the output voltage V H.

【0007】[0007]

【数1】 0.05・(VS /IS )・20・IH =0.05・VS ∴IH =0.05・IS [Equation 1] 0.05 · (V S / I S ) · 20 · I H = 0.05 · V S ∴I H = 0.05 · I S

【0008】したがって、図3,図4のいずれの装置で
あっても、発振器6として系統の定格電力の5%(VS
・IS ・0.05)の大出力容量の大型かつ高価な発振
器が必要になる。本発明は、発振器の出力容量を従来よ
り大幅に少なくして適当な高周波電力の注入が行える高
周波電力注入装置を提供することを目的とする。
Therefore, in any of the devices shown in FIGS. 3 and 4, the oscillator 6 is used as 5% (V S
A large and expensive oscillator with a large output capacity of I S · 0.05) is required. It is an object of the present invention to provide a high frequency power injection device capable of injecting appropriate high frequency power by significantly reducing the output capacitance of the oscillator as compared with the conventional one.

【0009】[0009]

【課題を解決するための手段】前記の目的を達成するた
めに、本発明の高周波電力注入装置においては、電力系
統に直列挿入されたリアクトルと、このリアクトルに付
加された2次誘導巻線と、発振出力を系統電圧阻止用の
ブロッキングコンデンサを介して2次誘導巻線に供給す
る高周波発振器とを備える。
In order to achieve the above object, in a high frequency power injection apparatus of the present invention, a reactor inserted in series in a power system and a secondary induction winding added to this reactor. , A high-frequency oscillator that supplies the oscillation output to the secondary induction winding through a blocking capacitor for blocking the system voltage.

【0010】[0010]

【作用】前記のように構成された本発明の高周波電力注
入装置の場合、電力系統に直列挿入されたリアクトルに
2次誘導巻線が付加され、この巻線にブロッキングコン
デンサを介した高周波発振器の高周波の発振出力が供給
される。
In the case of the high frequency power injection device of the present invention constructed as described above, the secondary induction winding is added to the reactor inserted in series in the power system, and the high frequency oscillator of the high frequency oscillator via the blocking capacitor is added to this winding. A high frequency oscillation output is supplied.

【0011】このとき、リアクトルは変圧器と異なりそ
の励磁インピーダンスが小さいため、ブロッキングコン
デンサにより系統の商用周波数に対してその2次回路を
開放したのと等価な回路構成になるが、リアクトル端子
間の商用周波数の誘導電圧は過大にならず、しかも、ブ
ロッキングコンデンサにより発振器に商用周波数の電流
が流入しないので、電力系統に適当な高周波電圧を生じ
させるために必要な発振器の出力容量は、従来装置より
極めて小さくなる。
At this time, since the reactor has a small exciting impedance unlike a transformer, a circuit configuration equivalent to opening the secondary circuit of the reactor with respect to the commercial frequency of the system by a blocking capacitor is provided. Since the induced voltage at the commercial frequency does not become excessive and the current at the commercial frequency does not flow into the oscillator due to the blocking capacitor, the output capacity of the oscillator required to generate an appropriate high frequency voltage in the power system is higher than that of the conventional device. It becomes extremely small.

【0012】[0012]

【実施例】1実施例について、図1及び図2を参照して
説明する。図1において、図3,図4と同一符号は同一
もしくは相当するものを示し、7は電力系統に直列挿入
された有鉄心構成のリアクトル、8はリアクトル7に付
加された2次誘導巻線であり、発振器6の出力が供給さ
れる。9は2次誘導巻線8と発振器6との間に設けられ
た商用周波数(低周波数)の系統電圧阻止用のブロッキ
ングコンデンサである。
EXAMPLE One example will be described with reference to FIGS. In FIG. 1, the same reference numerals as those in FIGS. 3 and 4 indicate the same or corresponding ones, 7 is a reactor having a core structure and is inserted in series in the power system, and 8 is a secondary induction winding added to the reactor 7. Yes, the output of the oscillator 6 is supplied. Reference numeral 9 denotes a blocking capacitor provided between the secondary induction winding 8 and the oscillator 6 for blocking a system voltage at a commercial frequency (low frequency).

【0013】そして、発振器6の出力はコンデンサ9,
2次誘導巻線8,リアクトル7を介して電力系統に直列
注入される。このとき、発振器6は2次誘導巻線8によ
り電力系統から電気的に絶縁される。
The output of the oscillator 6 is the capacitor 9,
It is injected in series into the power system via the secondary induction winding 8 and the reactor 7. At this time, the oscillator 6 is electrically insulated from the power system by the secondary induction winding 8.

【0014】また、リアクトル7に磁気的に密に結合し
た2次誘導巻線8を設けるので巻線7,8間のリーケー
ジインピーダンスが小さく、発振器6からみた負荷イン
ピーダンスは、2次誘導巻線8の巻数をリアクトル7と
同じ巻数と仮定すると、ほぼリアクトル7のインピーダ
ンスになる。さらに、2次誘導巻線8に誘起する商用周
波数の電圧は、コンデンサ9により阻止されて発振器6
への印加が防止される。
Since the secondary induction winding 8 magnetically and tightly coupled to the reactor 7 is provided, the leakage impedance between the windings 7 and 8 is small, and the load impedance seen from the oscillator 6 is the secondary induction winding 8. Assuming that the number of turns is the same as the number of turns of the reactor 7, the impedance of the reactor 7 is almost obtained. Further, the commercial frequency voltage induced in the secondary induction winding 8 is blocked by the capacitor 9 and the oscillator 6
Is prevented from being applied.

【0015】そして、説明を簡単にするため、リアクト
ル7,2次誘導巻線8の巻数比を1:1と仮定して等価
的に考えると、図1の要部は図2の等価回路で示すこと
ができる。この図2において、リアクトル7の商用周波
数の直列インピーダンスをXとし、定格の系統電圧,系
統電流(負荷電流)をVS ,IS とすると、リアクトル
7の電力容量PL はつぎの数2の式で示される。
To simplify the explanation, assuming that the turns ratio of the reactor 7 and the secondary induction winding 8 is 1: 1 and considered equivalently, the main part of FIG. 1 is the equivalent circuit of FIG. Can be shown. In this FIG. 2, assuming that the commercial frequency series impedance of the reactor 7 is X, and the rated system voltage and system current (load current) are V S and I S , the power capacity P L of the reactor 7 is expressed by the following formula 2. Indicated by.

【0016】[0016]

【数2】PL =(IS 2 ・X[Formula 2] P L = (I S ) 2 · X

【0017】さらに、X=KL ・(VS /IS )とし
(KL は係数)、定格負荷容量(=VS ・IS )をPl
とすると、数2の式からつぎの数3の式が得られる。
Further, X = K L · (V S / I S ) (K L is a coefficient), and the rated load capacity (= V S · I S ) is Pl.
Then, the following equation 3 is obtained from the equation 2.

【0018】[0018]

【数3】 PL =(IS 2 ・KL ・(VS /IS )=KL ・VS ・IS =KL ・Pl[Formula 3] P L = (I S ) 2 · K L · (V S / I S ) = K L · V S · I S = K L · Pl

【0019】一方、リアクトル7の両端間に出力電圧V
H を印加するのに必要な発振器6の出力容量PH は、発
振器6の出力周波数が商用周波数より十分高く、コンデ
ンサ9のインピーダンスを無視できるため、つぎの数4
の式で示される。
On the other hand, the output voltage V is applied across the reactor 7.
Output capacity P H of the oscillator 6 need to apply the H, the output frequency of the oscillator 6 is sufficiently higher than the commercial frequency, it is possible to ignore the impedance of the capacitor 9, the number of the next 4
It is shown by the formula.

【0020】[0020]

【数4】PH =(VH 2 /(Kf・X)[Formula 4] P H = (V H ) 2 / (Kf · X)

【0021】なお、Kfは発振器6の出力周波数(高周
波数)の商用周波数に対する周波数倍数を示す。そし
て、電力系統に系統電圧VS の5%の適当な高周波電圧
を発生する場合、リアクトル7の両端間の印加電圧VH
を0.05・VS にするため、発振器6の必要な出力容
量PH はつぎの数5の式で示される。
Kf represents the frequency multiple of the output frequency (high frequency) of the oscillator 6 with respect to the commercial frequency. When an appropriate high frequency voltage of 5% of the system voltage V S is generated in the power system, the applied voltage V H across the reactor 7 is applied.
To 0.05 · V S and indicated by the number 5 Formula of the required output capacity P H Hatsugi oscillator 6.

【0022】[0022]

【数5】 PH ={(0.05)2 /Kf}・〔(VS 2 /{KL ・(VS /IS )}〕 ={(0.05)2 /(Kf・KL )}・PlP H = {(0.05) 2 / Kf} · [(V S ) 2 / {K L · (V S / I S )}] = {(0.05) 2 / (Kf · K L)} · Pl

【0023】したがって、数3,数5の式からも明らか
なように、リアクトル7を用いた直列挿入の場合、係数
L がリアクトル7の出力容量PL と発振器6の出力容
量PH とのトレードオフの要因となる。そして、発振器
6の出力容量PH を極力小さくするため、PH =0.0
3・PL にするときは、PH ,PL がPlに対してそれ
ぞれつぎに説明する大きさになる。
Therefore, as is clear from the equations (3) and (5), in the case of the series insertion using the reactor 7, the coefficient K L is the output capacitance P L of the reactor 7 and the output capacitance P H of the oscillator 6. It becomes a factor of trade-off. Then, in order to make the output capacitance P H of the oscillator 6 as small as possible, P H = 0.0
When setting 3 · P L , P H and P L have the sizes described below with respect to P 1, respectively.

【0024】すなわち、数3,数5の式とPH =0.0
3・PL の関係とからつぎの数6の式が得られる。
That is, the equations of the equations 3 and 5 and P H = 0.0
The following equation 6 is obtained from the relationship of 3 · P L.

【0025】[0025]

【数6】 0.03・KL ・Pl={(0.05)2 /(Kf・KL )}・Pl[Equation 6] 0.03 · K L · Pl = {(0.05) 2 / (Kf · K L )} · Pl

【0026】さらに、数6の式からつぎの数7の式が得
られる。
Further, the following equation 7 is obtained from the equation 6.

【0027】[0027]

【数7】KL 2 =(0.05)2 /(0.03・Kf) ∴KL ≒0.29・(1/√Kf)[Formula 7] K L 2 = (0.05) 2 /(0.03·Kf) ∴K L ≈0.29 · (1 / √Kf)

【0028】この数7の式は、係数KL が発振器6の出
力周波数に依存して定まることを示す。そして、発振器
6の出力周波数を商用周波数の20倍の1KHzとする
と、Kf=20,KL ≒0.06となる。
The equation (7) shows that the coefficient K L is determined depending on the output frequency of the oscillator 6. When the output frequency of the oscillator 6 is 1 KHz, which is 20 times the commercial frequency, Kf = 20 and K L ≈0.06.

【0029】さらに、これらの値を数5の式に代入する
と、PH はつぎの数8の式に示す値になる。
Furthermore, substituting these values into the numerical formula 5, the values shown in the numerical formula 8 P H Hatsugi.

【0030】[0030]

【数8】 PH ={(0.05)2 /(20・0.06)}・Pl ≒2.1・10-3・Pl[Formula 8] P H = {(0.05) 2 /(20·0.06)}·Pl ≈ 2.1 · 10 −3 · Pl

【0031】また、PL は数3の式によりつぎの数9の
式に示す値になる。
Further, P L becomes a value shown in the following equation 9 by the equation 3

【0032】[0032]

【数9】PL =0.06・Pl[Equation 9] P L = 0.06 · Pl

【0033】したがって、リアクトル7の出力容量PL
を0.06・Plにすると、発振器6の出力容量PH
2.1・10-3・Plの極めて小容量にして電力系統に
系統電圧VS の5%の高周波電圧を発生することができ
る。なお、従来装置であれば発振器6の出力容量PH
して、概に数1の式に関して説明したように0.05・
Plの容量を要する。
Therefore, the output capacitance P L of the reactor 7
When the 0.06 · Pl and that by the output capacitance P H of the oscillator 6 in a very small volume of 2.1 · 10 -3 · Pl to generate the 5% of the high-frequency voltage of the system voltage V S to the power system it can. In the case of the conventional device, the output capacitance P H of the oscillator 6 is set to 0.05.
Requires a capacity of Pl.

【0034】そして、出力容量PH ,PL は種々に設定
できるが、実用上からは、リアクトル7の大きさ等を考
慮し、そのインピーダンスXが定格負荷インピーダンス
の1〜数%程度になる範囲に設定することが好ましい。
The output capacitances P H and P L can be set variously, but from the practical point of view, considering the size of the reactor 7 and the like, the impedance X thereof is in the range of 1 to several% of the rated load impedance. It is preferable to set to.

【0035】また、前記実施例においては発振器6の出
力を直接リアクトル7に供給する等価回路で説明した
が、発振器6を電力系統から絶縁するため、発振器6の
出力を変圧器を介して2次誘導巻線8に供給してもよ
い。
In the above embodiment, the equivalent circuit for directly supplying the output of the oscillator 6 to the reactor 7 has been described. However, in order to insulate the oscillator 6 from the power system, the output of the oscillator 6 is secondary through a transformer. It may be supplied to the induction winding 8.

【0036】[0036]

【発明の効果】本発明は、以上説明したように構成され
ているため、以下に記載する効果を奏する。電力系統に
リアクトル7を直列に挿入するとともに、このリアクト
ル7に2次誘導巻線8を付加し、高周波発振器6の発振
出力をブロッキングコンデンサ9,2次誘導巻線8を介
してリアクトル7に供給し、電力系統に高周波電力を注
入したため、リアクトル7の励磁インピーダンスが小さ
く、コンデンサ9により商用周波数に対して2次回路開
放状態になってもその端子間の商用周波数の誘導電圧が
過大にならず、しかも、コンデンサ9により商用周波数
の電流の発振器6への流入が阻止され、電力系統に適当
な高周波電圧が発生するために必要な発振器6の出力容
量が従来装置の場合より極めて小さくなり、発振器6が
小型かつ安価になって装置の小型化及び低価格化が図れ
る。
Since the present invention is configured as described above, it has the following effects. A reactor 7 is inserted in series in the power system, a secondary induction winding 8 is added to this reactor 7, and the oscillation output of the high-frequency oscillator 6 is supplied to the reactor 7 via the blocking capacitor 9 and the secondary induction winding 8. However, since high-frequency power is injected into the power system, the exciting impedance of the reactor 7 is small, and even if the secondary circuit is opened to the commercial frequency by the capacitor 9, the induced voltage at the commercial frequency between the terminals does not become excessive. Moreover, the capacitor 9 prevents the commercial frequency current from flowing into the oscillator 6, and the output capacity of the oscillator 6 required for generating an appropriate high frequency voltage in the power system becomes much smaller than that of the conventional device. Since 6 is small and inexpensive, the device can be downsized and the cost can be reduced.

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

【図1】本発明の高周波電力注入装置の1実施例の結線
図である。
FIG. 1 is a connection diagram of an embodiment of a high frequency power injection device of the present invention.

【図2】図1の要部の等価回路図である。FIG. 2 is an equivalent circuit diagram of a main part of FIG.

【図3】従来装置の1例の結線図である。FIG. 3 is a connection diagram of an example of a conventional device.

【図4】従来装置の他の例の結線図である。FIG. 4 is a connection diagram of another example of the conventional device.

【符号の説明】[Explanation of symbols]

6 高周波発振器 7 リアクトル 8 2次誘導巻線 9 ブロッキングコンデンサ 6 High-frequency oscillator 7 Reactor 8 Secondary induction winding 9 Blocking capacitor

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 電力系統に直列挿入されたリアクトル
と、 該リアクトルに付加された2次誘導巻線と、 発振出力を系統電圧阻止用のブロッキングコンデンサを
介して前記2次誘導巻線に供給する高周波発振器とを備
えたことを特徴とする高周波電力注入装置。
1. A reactor inserted in series in a power system, a secondary induction winding added to the reactor, and an oscillation output supplied to the secondary induction winding through a blocking capacitor for blocking the system voltage. A high frequency power injection device comprising a high frequency oscillator.
JP20298292A 1992-07-06 1992-07-06 High frequency power injecting device Pending JPH0629884A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20298292A JPH0629884A (en) 1992-07-06 1992-07-06 High frequency power injecting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20298292A JPH0629884A (en) 1992-07-06 1992-07-06 High frequency power injecting device

Publications (1)

Publication Number Publication Date
JPH0629884A true JPH0629884A (en) 1994-02-04

Family

ID=16466376

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20298292A Pending JPH0629884A (en) 1992-07-06 1992-07-06 High frequency power injecting device

Country Status (1)

Country Link
JP (1) JPH0629884A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005088858A1 (en) * 2004-03-15 2005-09-22 Mitsubishi Denki Kabushiki Kaisha High frequency bypass unit
JPWO2006095402A1 (en) * 2005-03-07 2008-08-14 三菱電機株式会社 Signal bypass device
US9031404B2 (en) 2008-08-21 2015-05-12 Nistica, Inc. Optical channel monitor

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005088858A1 (en) * 2004-03-15 2005-09-22 Mitsubishi Denki Kabushiki Kaisha High frequency bypass unit
JPWO2005088858A1 (en) * 2004-03-15 2007-08-30 三菱電機株式会社 High frequency bypass
JPWO2006095402A1 (en) * 2005-03-07 2008-08-14 三菱電機株式会社 Signal bypass device
JP4633787B2 (en) * 2005-03-07 2011-02-16 三菱電機株式会社 Signal bypass device
US9031404B2 (en) 2008-08-21 2015-05-12 Nistica, Inc. Optical channel monitor

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