JPH02214474A - Resonance type inverter circuit - Google Patents

Resonance type inverter circuit

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Publication number
JPH02214474A
JPH02214474A JP1031754A JP3175489A JPH02214474A JP H02214474 A JPH02214474 A JP H02214474A JP 1031754 A JP1031754 A JP 1031754A JP 3175489 A JP3175489 A JP 3175489A JP H02214474 A JPH02214474 A JP H02214474A
Authority
JP
Japan
Prior art keywords
resonant
circuit
state
inverter circuit
power supply
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
JP1031754A
Other languages
Japanese (ja)
Inventor
Hitoshi Mori
均 森
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.)
Nichicon Corp
Original Assignee
Nichicon 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 Nichicon Corp filed Critical Nichicon Corp
Priority to JP1031754A priority Critical patent/JPH02214474A/en
Publication of JPH02214474A publication Critical patent/JPH02214474A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To freely adjust an output by designing a circuit which can operates in any two states selected from three states, and switching the state. CONSTITUTION:A resonance type inverter circuit has a serial resonance circuit of a resonance capacitor 4 and a resonance inductor 5, and a switching element 2 to supply a sine wave AC current to a load 3. The element 2 for forming a free vibrating state is added, and a switch state (contact D) for disconnecting a DC power source 1a is provided. As a result, an output regulating function can be provided by making the circuit in one of exciting, free vibrating and regeneratively braking states.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は直流電力を交流電力に°変換する共振型インバ
ータ回路に関するもので、特にその出力である交流電力
を整流して安定化直流出力を得る電源装置への適用にお
いて、その効果を発揮するものである。
[Detailed Description of the Invention] Industrial Application Field The present invention relates to a resonant inverter circuit that converts DC power into AC power, and particularly relates to a power source that rectifies the output AC power to obtain a stabilized DC output. It exhibits its effects when applied to equipment.

従来の技術 通常の方形波インバータ回路は、スイッチング素子をそ
の定格電流レベルの比較的大きな電流が流れている状態
で強制的にオフする必要があるため、小形・軽量化など
を目的として数IQkHz以上の高い周波数で動作させ
る場合、スイッチング素子のスイッチング損失による発
熱やスイッチングノイズの増加の問題が重大となり、イ
ンバータとしてのエネルギー変換効率が低いことや、電
磁障害に関する各種規格を満足させて、発生ノイズのレ
ベルを抑えるためのフィルタの価格が高くなったり、フ
ィルタ素子を通じて接地漏洩電流が増大するなどの欠点
があった。
Conventional technology In a normal square wave inverter circuit, it is necessary to forcibly turn off the switching elements while a relatively large current of the rated current level is flowing through them. When operating at a high frequency, the problem of increased heat generation and switching noise due to switching loss of switching elements becomes serious, and the energy conversion efficiency of the inverter is low, and it is necessary to satisfy various standards regarding electromagnetic interference and reduce the generated noise. The disadvantages include that the price of the filter used to suppress the level increases, and that the ground leakage current increases through the filter element.

そのため、前述の方形波インバータ回路の欠点を除くた
めに共振型インバータ回路が種々提案されている。
Therefore, various resonant inverter circuits have been proposed to eliminate the drawbacks of the above-mentioned square wave inverter circuits.

従来の共振型インバータ回路の基本回路図を第4図に示
す、第4図(a)は電流共振型と呼ばれ、共振コンデン
サ4の静電容量をC(F)共振インダフタ5のインダク
タンスをL (H)とし、これらからなる直列共振回路
の共振周波数 f、=1/(2ππ下>  (Hz)にほぼ一致した周
波数でスイッチング素子2を駆動し、回路接続の半サイ
クル毎の切替えを繰り返すことにより、負荷3に正弦波
に近い交流電流を流すことができる。
A basic circuit diagram of a conventional resonant type inverter circuit is shown in Fig. 4. Fig. 4(a) is called a current resonant type, where the capacitance of the resonant capacitor 4 is C(F) and the inductance of the resonant inductor 5 is L. (H), and drive the switching element 2 at a frequency that almost matches the resonant frequency f of the series resonant circuit consisting of these, = 1/(2ππ lower > (Hz), and repeat switching every half cycle of the circuit connection. This allows an alternating current close to a sine wave to flow through the load 3.

また、第4図(blは電圧共振型と呼ばれ、共振コンデ
ンサ4の静電容量をC(F) 、共振インダクタ5のイ
ンダクタンスをL (H)とし、これからなる並列共振
回路の共振周波数 fo=1/(2πf口σ)  (Hz)にほぼ一致した
周波数でスイッチング素子2を駆動し、回路接続の半サ
イクル毎の切替えを繰り返すことにより、負荷3に正弦
波に近い交流電流を印加することができる。
In addition, in Fig. 4 (bl is called a voltage resonance type, the capacitance of the resonant capacitor 4 is C (F), the inductance of the resonant inductor 5 is L (H), and the resonant frequency fo of the parallel resonant circuit consisting of this is = By driving the switching element 2 at a frequency approximately equal to 1/(2πf σ) (Hz) and repeating switching every half cycle of the circuit connection, it is possible to apply an alternating current close to a sine wave to the load 3. can.

la、1bは直vL電源である。Pは+側半波のスイッ
チ位置、Mは〜側半波のスイッチ位置を示す。
la and 1b are direct VL power supplies. P indicates the switch position for the + side half wave, and M indicates the switch position for the ~ side half wave.

発明が解決しようとする問題点 前述の従来の共振型インバータ回路には、出力の調整機
能がなく、動作点は直流電源の電圧または電流値、共振
コンデンサと共振インダクタと負荷および直流電源のイ
ンピーダンスにより決定されてしまうという欠点があっ
た。この欠点を除くため、 ■スイッチング素子を間欠動作させる。
Problems to be Solved by the Invention The conventional resonant inverter circuit described above does not have an output adjustment function, and the operating point depends on the voltage or current value of the DC power supply, the resonant capacitor, the resonant inductor, the load, and the impedance of the DC power supply. The disadvantage was that the decision was made. To eliminate this drawback, 1. Operate the switching element intermittently.

■共振回路に補助共振回路を追加して、微少な動作周波
数の変化に対して共振回路全体のインピーダンスを大き
く変化させる。
■ Adding an auxiliary resonant circuit to the resonant circuit allows the impedance of the entire resonant circuit to change significantly in response to minute changes in the operating frequency.

などの考察がなされているが、 ■では交流出力電力の変動が大きくなり、またスイッチ
ング素子の電気的性能の余裕が必要となるなどの欠点が
あり、 ■では、動作周波数の変動が必須となり、また余分な補
助共振回路を追加する必要があるなどの欠点があった。
However, in (2), there are disadvantages such as large fluctuations in AC output power and the need for a margin in the electrical performance of the switching element, while in (2), fluctuations in the operating frequency are essential. Another disadvantage is that an extra auxiliary resonant circuit needs to be added.

問題点を解決するための手段 本発明の目的は交流出力電力・動作周波数変動が少なく
、共振型インバータ回路本来の特徴を生かしつつ、出力
の調整機能を持たせた共振型インバータ回路を提供する
ことである。
Means for Solving the Problems An object of the present invention is to provide a resonant inverter circuit that has small fluctuations in AC output power and operating frequency, takes advantage of the inherent characteristics of a resonant inverter circuit, and has an output adjustment function. It is.

本発明の共振型インバータ回路では、その動作状態を共
振回路が直流電源からエネルギーを受け取って、電気的
振動を増大させる「励振状MJと、共振回路が直流電源
とのエネルギーの授受を行わず、共振回路と負荷のイン
ピーダンスで概略決まる自由振動をするF自由振動状態
」と、共振回路がその電気的振動のエネルギーを直流電
源へ与え、前記電気的振動が減衰する「回生制動状態」
との3種類のうちから2種類以上選択できる構成として
、共振回路の振動の半周期を最小時間単位として状態切
替えを行うことにより、共振回路またはこれに電磁的に
結合される負荷の交流電力を制御し、いわゆる出力調整
機能を持たせた共振型インバータ回路である。
In the resonant inverter circuit of the present invention, its operating state is defined as an excitation MJ in which the resonant circuit receives energy from the DC power source and increases electrical vibration, and a resonant circuit that does not transfer energy to or from the DC power source. "F free vibration state" in which free vibration is approximately determined by the impedance of the resonant circuit and the load, and "regenerative braking state" in which the resonant circuit gives the energy of the electrical vibration to the DC power supply and the electrical vibration is damped.
As a configuration in which two or more types can be selected from among the three types, the AC power of the resonant circuit or the load electromagnetically coupled to it can be changed by switching the state using the half period of vibration of the resonant circuit as the minimum time unit. It is a resonant inverter circuit with a so-called output adjustment function.

作用 本発明の共振型インバータ回路の基本回路を第1図に示
す。
Operation The basic circuit of the resonant inverter circuit of the present invention is shown in FIG.

第1図(a)は電流共振型インバータ回路の基本回路図
であり、第4図(a)の従来の電流共振型インバータ回
路との相違点は、自由振動状態を作るためのスイッチン
グ素子2′が追加され、直流電源1aを切り離すスイッ
チ状M(接点記号D)が存在することである。スイッチ
接点りが選択された状態では、直流電源1からのエネル
ギー供給は停止され、共振コンデンサ4と共振インダク
タ5からなる直列共振回路のエネルギーが負荷3で消費
される自由振動状態となる。また上記直列共振回路の振
動を増大させるべく、スイッチ接点PとMを半周期毎に
交互に選択する状態は第4図(a)の従来の電流共振型
インバータの動作と同一であり、本発明では、励振状態
と呼んでいるものである。
FIG. 1(a) is a basic circuit diagram of a current resonant inverter circuit, and the difference from the conventional current resonant inverter circuit shown in FIG. 4(a) is that the switching element 2' is used to create a free vibration state. is added, and there is a switch-like M (contact symbol D) that disconnects the DC power supply 1a. When the switch contact is selected, the energy supply from the DC power source 1 is stopped, and a free vibration state is created in which the energy of the series resonant circuit consisting of the resonant capacitor 4 and the resonant inductor 5 is consumed by the load 3. Further, in order to increase the vibration of the series resonant circuit, the state in which switch contacts P and M are alternately selected every half cycle is the same as the operation of the conventional current resonant inverter shown in FIG. 4(a), and the present invention This is what we call the excitation state.

さらに上記直列共振回路の振動を打ち消す方向にスイッ
チ接点PとMを半周期毎に交互に選択する状態が設定で
き、この状態が上記直流電源1aへ上記直列共振回路の
振動エネルギーを戻す回生制動状態である。
Furthermore, a state can be set in which the switch contacts P and M are alternately selected every half cycle in a direction to cancel the vibration of the series resonant circuit, and this state is a regenerative braking state in which the vibration energy of the series resonant circuit is returned to the DC power supply 1a. It is.

第1図(b)は電圧共振型インバータ回路の基本回路図
であり、第2図(b)の従来の電圧共振型インバータ回
路との相違点はスイッチング素子2に新たな接点りが設
けられたことにある。接点りが選択された状態では、直
流電源1bは短絡され、共振コンデンサ4、共振インダ
クタ5、負荷3からなる並列共振回路は切り離されて、
その振動エネルギーが負荷で消費される自由振動状態と
なる。また前記並列共振回路の振動を増大させるべく、
スイッチ接点PとMとを半サイクル毎に交互に選択する
状態は第4図中)の従来の電圧共振型インバータの動作
と同一であり、本発明では励振状態と呼んでいるもので
ある。さらに前記並列共振回路の振動を打ち消す方向に
スイッチ接点PとMとを半周期毎に交互に選択する状態
が設定でき、この状態が前記直流電源1bへ前記並列共
振回路の振動エネルギーを戻す回生制動状態である。
Fig. 1(b) is a basic circuit diagram of a voltage resonant inverter circuit, and the difference from the conventional voltage resonant inverter circuit shown in Fig. 2(b) is that a new contact is provided in the switching element 2. There is a particular thing. When the contact is selected, the DC power supply 1b is short-circuited, and the parallel resonant circuit consisting of the resonant capacitor 4, resonant inductor 5, and load 3 is disconnected.
It becomes a free vibration state in which the vibration energy is consumed by the load. Furthermore, in order to increase the vibration of the parallel resonant circuit,
The state in which switch contacts P and M are alternately selected every half cycle is the same as the operation of the conventional voltage resonant inverter shown in FIG. 4, and is called an excitation state in the present invention. Further, a state can be set in which switch contacts P and M are alternately selected every half cycle in a direction to cancel the vibration of the parallel resonant circuit, and this state is a regenerative braking that returns the vibration energy of the parallel resonant circuit to the DC power supply 1b. state.

実施例 以下、本発明の実施例を第2図および第3図により説明
する。
EXAMPLE Hereinafter, an example of the present invention will be explained with reference to FIGS. 2 and 3.

まず、第2図に示す回路図は一般にハーフブリフジと呼
ばれるインバータ回路で構成した本発明の実施例である
。前述の励振状態では、共振コンデンサ4、共振インダ
クタ5および絶縁トランス8で結合された負荷3からな
る共振回路のインピーダンスで決まる振動周期に合致さ
せて、スイッチング素子2p、2mを半サイクル毎に交
互にオン・オフを繰り返しさせ、スイッチング素子2′
はオフの状態に保って直流電源1から交流振動のエネル
ギーを得る。また上述の自由振動状態ではスイッチング
素子2p、2mはオフに保ち、スイッチング素子2′を
オンの状態に保って、共振コンデンサ4、共振インダク
タ5の電気振動エネルギーを負荷3で消費させる。さら
に前述の回生制動状態では、スイッチング素子2 p 
12 m、 2’を全てオフの状態に保ち、ダイオード
6a、6bにより前記共振回路のエネルギーを整流して
バイパスコンデンサ7a、7bを通じ、直流電源1に返
す。
First, the circuit diagram shown in FIG. 2 is an embodiment of the present invention constructed with an inverter circuit generally called a half bridge. In the above-mentioned excitation state, the switching elements 2p and 2m are alternately activated every half cycle to match the vibration period determined by the impedance of the resonant circuit consisting of the resonant capacitor 4, the resonant inductor 5, and the load 3 coupled by the isolation transformer 8. The switching element 2' is repeatedly turned on and off.
is kept in an off state to obtain alternating current vibration energy from the direct current power supply 1. Further, in the above-mentioned free vibration state, the switching elements 2p and 2m are kept off, the switching element 2' is kept on, and the electrical vibration energy of the resonant capacitor 4 and the resonant inductor 5 is consumed by the load 3. Furthermore, in the regenerative braking state described above, the switching element 2 p
12m and 2' are all kept off, and the energy of the resonant circuit is rectified by diodes 6a and 6b and returned to the DC power supply 1 through bypass capacitors 7a and 7b.

次に第3図に示す回路図は一般にフルブリッジと呼ばれ
る電流共振型インバータ回路であり、回路図上は従来の
電流共振型インバータ回路と本発明の電流共振型インバ
ータ回路で殆ど差はないが、その制御方法が異なってお
り、本発明の特許請求の範囲を構成している。
Next, the circuit diagram shown in FIG. 3 is a current resonance type inverter circuit generally called a full bridge, and although there is almost no difference between the conventional current resonance type inverter circuit and the current resonance type inverter circuit of the present invention on the circuit diagram, The control method is different and constitutes the scope of the claims of the present invention.

すなわち、従来の電流共振型インバータ回路では、本発
明で励振状態と呼んでいる状態で運転される。共振コン
デンサ4、共振インダクタ5および絶縁トランス8を介
して結合された負荷3からなる共振回路のインピーダン
スで決まる振動周期に合致させて、スイッチング素子2
a、2dの組と、スイッチング素子2b、2cの組を半
周期毎に交互にオン・オフを繰り返すものである。この
状態では常に直流電源lからのエネルギーが共振回路へ
与えられるために、負荷3を含む共振回路全体のエネル
ギー消費が少なくなった場合など過大な共振電流が流れ
、スイッチング素子や、共振コンデンサや共振インダク
タに損傷を与える恐れがあった。
That is, the conventional current resonance type inverter circuit is operated in a state called an excitation state in the present invention. The switching element 2 is adjusted to match the vibration period determined by the impedance of the resonant circuit consisting of the resonant capacitor 4, the resonant inductor 5, and the load 3 coupled via the isolation transformer 8.
The set of switching elements a and 2d and the set of switching elements 2b and 2c are alternately turned on and off every half cycle. In this state, energy from the DC power source 1 is always given to the resonant circuit, so when the energy consumption of the entire resonant circuit including the load 3 is low, an excessive resonant current flows, causing the switching element, resonant capacitor, and resonant There was a risk of damaging the inductor.

これに対し、本発明の自由振動状態では、スイッチング
素子2 a s 2 b 12c −2dを1個ずつ前
記共振回路の振動周期の半周期だけ順にオンさせて、例
えばスイッチング素子2aがオンの時はダイオード6c
が導通し、(スイッチング素子)2a−(絶縁トランス
)8−(共振インダクタ)5−(共振コンデンサ)4−
(ダイオード)6cの回路に電流を通じ、次の半周期で
はスイッチング素子2bをオンとし、(スイッチング素
子)2b−(絶縁トランス) 8−(共振インダクタ)
 5−(共振コンデンサ)4−(ダイオード)6dの回
路に電流を通じる。この状態では直流電源1と共振回路
との間のエネルギー授受けなくなる。さらに回生制動状
態では、スイッチング素子2a、2b、2゜C0,2d
をオフの状態に保ち、共振回路のエネルギーがダイオー
ド6aと6dの組、タイオード6bと60の組を通じて
整流され、直流電源1に戻される。
On the other hand, in the free vibration state of the present invention, the switching elements 2a s 2 b 12c - 2d are turned on one by one for half the vibration period of the resonant circuit, and for example, when the switching element 2a is on, diode 6c
is conductive, (switching element) 2a- (insulation transformer) 8- (resonant inductor) 5- (resonant capacitor) 4-
Current is passed through the circuit of (diode) 6c, and in the next half cycle, switching element 2b is turned on, (switching element) 2b - (insulation transformer) 8 - (resonant inductor)
Current passes through the circuit of 5-(resonant capacitor) 4-(diode) 6d. In this state, no energy is exchanged between the DC power supply 1 and the resonant circuit. Furthermore, in the regenerative braking state, switching elements 2a, 2b, 2°C0, 2d
is kept off, and the energy of the resonant circuit is rectified through the set of diodes 6a and 6d and the set of diodes 6b and 60, and is returned to the DC power supply 1.

出力制御のためには、共振回路の電流値または電圧値を
モニタしてその交流値を整流して制御系に対し、フィー
ドバックする方法が普通であるが、インバータ回路の出
力を整流・平滑して直流電源装置とする場合、その平滑
後の直流電圧値や直流電流値をフィードバックすること
も当然考えられる。
For output control, the usual method is to monitor the current or voltage value of the resonant circuit, rectify the AC value, and feed it back to the control system. In the case of a DC power supply, it is of course possible to feed back the smoothed DC voltage value and DC current value.

また、本発明の共振型インバータ回路は励振状態、自由
振動状態、回生制動状態の3状B(またはこのうちの2
状B)を取ることから、デジタル演算回路により、各状
態間の遷移を決定することが妥当であり、マイクロプロ
セッサによりプログラム制御することなど適宜応用でき
るものである。
Further, the resonant inverter circuit of the present invention has three states B (or two of these states): an excitation state, a free vibration state, and a regenerative braking state.
Since condition B) is taken, it is appropriate to determine the transition between each state by a digital arithmetic circuit, and it is possible to apply program control by a microprocessor as appropriate.

発明の効果 従来の共振型インバータ回路では、直流電源からのエネ
ルギーの流れは常に流れ出す方向であったために、出力
調整機能がなかったのが、本発明の共振型インバータ回
路では、前述の従来の問題点を解消し、直流電源からの
エネルギーの流れの停止状態あるいは共振回路から直流
電源へのエネルギーの逆流状態を持つことによって、そ
の出力を自由に調整できる顕著な効果がある。
Effects of the Invention In conventional resonant inverter circuits, the flow of energy from the DC power source was always in the direction of outflow, so there was no output adjustment function.However, the resonant inverter circuit of the present invention solves the above-mentioned conventional problem. By solving this problem and creating a state in which the flow of energy from the DC power supply is stopped or a state in which energy flows back from the resonant circuit to the DC power supply, there is a remarkable effect that the output can be freely adjusted.

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

第1図(a)、(b)は本発明に係る共振型インバータ
回路の基本回路例、第2図および第3図は本発明の共振
型インバータ回路の各々異なる実施例の要部の回路図、
第4図(a)、(blは従来の共振型インバータ回路の
基本回路例である。 1.1a、1b=直流電源 2.2′、2p、2m、2a、2b、2c、2dニスイ
ツチング素子 3:負荷  4:共振コンデンサ 5:共振インダクタ
FIGS. 1(a) and (b) are basic circuit examples of a resonant inverter circuit according to the present invention, and FIGS. 2 and 3 are circuit diagrams of main parts of different embodiments of the resonant inverter circuit of the present invention. ,
Figures 4(a) and bl are basic circuit examples of conventional resonant inverter circuits. 1.1a, 1b = DC power supply 2.2', 2p, 2m, 2a, 2b, 2c, 2d switching elements 3 : Load 4: Resonant capacitor 5: Resonant inductor

Claims (1)

【特許請求の範囲】[Claims] コンデンサおよびインダクタからなる共振回路を有し、
該共振回路が直流電源からエネルギーを受け取る励振状
態と、直流電源とエネルギーの授受をしない自由振動状
態と、直流電源にエネルギーを与える回生制動状態との
3種類のうちから2種類以上の動作状態を共振回路の振
動の半周期を最小時間単位として、切替える手段を有し
、この切替えによって上記共振回路またはこれに電磁的
に結合される負荷の交流電力を制御することを特徴とす
る共振型インバータ回路。
It has a resonant circuit consisting of a capacitor and an inductor,
Two or more operating states are selected from three types: an excitation state in which the resonant circuit receives energy from the DC power supply, a free vibration state in which it does not exchange energy with the DC power supply, and a regenerative braking state in which it provides energy to the DC power supply. A resonant inverter circuit characterized in that it has means for switching using a half period of vibration of the resonant circuit as the minimum time unit, and by this switching, the AC power of the resonant circuit or a load electromagnetically coupled thereto is controlled. .
JP1031754A 1989-02-10 1989-02-10 Resonance type inverter circuit Pending JPH02214474A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1031754A JPH02214474A (en) 1989-02-10 1989-02-10 Resonance type inverter circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1031754A JPH02214474A (en) 1989-02-10 1989-02-10 Resonance type inverter circuit

Publications (1)

Publication Number Publication Date
JPH02214474A true JPH02214474A (en) 1990-08-27

Family

ID=12339809

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1031754A Pending JPH02214474A (en) 1989-02-10 1989-02-10 Resonance type inverter circuit

Country Status (1)

Country Link
JP (1) JPH02214474A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19540437B4 (en) * 1994-10-31 2004-04-01 Toyoda Gosei Co., Ltd. High-gloss molded part made of resin
JP2007174881A (en) * 2005-12-22 2007-07-05 Samsung Electronics Co Ltd Inverter circuit, backlight device, and liquid crystal display device made thereby
US9954635B2 (en) 1999-03-05 2018-04-24 Intel Corporation Variable rate coding for enabling high performance communication

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19540437B4 (en) * 1994-10-31 2004-04-01 Toyoda Gosei Co., Ltd. High-gloss molded part made of resin
US9954635B2 (en) 1999-03-05 2018-04-24 Intel Corporation Variable rate coding for enabling high performance communication
JP2007174881A (en) * 2005-12-22 2007-07-05 Samsung Electronics Co Ltd Inverter circuit, backlight device, and liquid crystal display device made thereby

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