JPS62128495A - Hot-cathode discharge tube burner - Google Patents

Hot-cathode discharge tube burner

Info

Publication number
JPS62128495A
JPS62128495A JP26718985A JP26718985A JPS62128495A JP S62128495 A JPS62128495 A JP S62128495A JP 26718985 A JP26718985 A JP 26718985A JP 26718985 A JP26718985 A JP 26718985A JP S62128495 A JPS62128495 A JP S62128495A
Authority
JP
Japan
Prior art keywords
discharge tube
circuit
capacitor
hot
transistor
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
JP26718985A
Other languages
Japanese (ja)
Inventor
越智 雅文
正彦 腰原
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.)
Iwasaki Denki KK
Original Assignee
Iwasaki Denki KK
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 Iwasaki Denki KK filed Critical Iwasaki Denki KK
Priority to JP26718985A priority Critical patent/JPS62128495A/en
Publication of JPS62128495A publication Critical patent/JPS62128495A/en
Pending legal-status Critical Current

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  • Circuit Arrangements For Discharge Lamps (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の属する技術分野〕 本発明は、熱陰極を有する放電管の高周波点灯装置の改
良−に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of the Invention] The present invention relates to an improvement in a high-frequency lighting device for a discharge tube having a hot cathode.

〔従来技術とその問題点〕[Prior art and its problems]

最近、螢光ランプのような熱陰極を有する放電管の点灯
装置として従来の鉄と銅よりなるチー−クコイル式安定
器に代わってトランジスタ等の半導体を用いるインバー
タ式の電子安定器が実用化され、普及に及びつつある。
Recently, inverter-type electronic ballasts using semiconductors such as transistors have been put into practical use as lighting devices for discharge tubes with hot cathodes such as fluorescent lamps, replacing the conventional teak coil ballasts made of iron and copper. , is becoming popular.

第2図がインバータ式電子安定器の代表的回路図である
。トランジスタ2石を用いた定電流インバータと呼ばれ
るもので直流電源を高周波に変換し放電灯を高周波点灯
するものである。
FIG. 2 is a typical circuit diagram of an inverter type electronic ballast. It is called a constant current inverter that uses two transistors, and converts the DC power into high frequency power to light the discharge lamp at high frequency.

同図において、Eは直流電源、Lは補助インダクタ、Q
a 、 Qhは電力用トランジスタ、R,L。
In the same figure, E is a DC power supply, L is an auxiliary inductor, and Q
a, Qh are power transistors, R, L.

R& は起動抵抗、Cは発振コンデンサ、Tはフェライ
トコアを用いた出カドランス、Nz は出カドランスT
の2次1巻線、Dは螢光ランプのような熱電積出 、 
 HjL’を有する放電管である。
R& is the starting resistance, C is the oscillation capacitor, T is the output transformer using a ferrite core, and Nz is the output transformer T.
The secondary first winding of , D is a thermoelectric generator like a fluorescent lamp,
This is a discharge tube having HjL'.

Nj は帰還捲線である。Nj is the return winding.

この電子安定器は鉄鋼式の従来のチョーク安定器に比較
し、高効率(低損失)の上小形軽量であるといった特徴
を有することは良く知られている。
It is well known that this electronic ballast has the characteristics of high efficiency (low loss), small size, and light weight compared to conventional steel choke ballasts.

しかしながら、一般に用いられつつある第2図の如き2
石ンイバータ式安定器は半導体やトランス等の主要部品
のコストが高く装置全体の価格もコスト高となるため、
なかなか一般に普及しないという問題がある。特に出カ
ドランスTは放電灯の始動に必要な高電圧(400V以
上)を発生さるせ必要があるため2次1巻線Nzの巻数
が大となるため形状が大となり、製造コスト上昇の原因
となっている。
However, as shown in Fig. 2, which is becoming commonly used,
Stone inverter type ballasts have high costs for main parts such as semiconductors and transformers, and the price of the entire device is also high.
The problem is that it is not widely available. In particular, the output transformer T needs to generate the high voltage (400V or more) required to start the discharge lamp, so the number of turns of the secondary first winding Nz is large, resulting in a large shape, which causes an increase in manufacturing costs. It has become.

〔発明の目的〕[Purpose of the invention]

本発明の目的は従来のインバータ回路のような出力回路
に昇圧用トランスを用いない、異なる昇圧方法に基づく
新規な点灯回路を提供するものである。
An object of the present invention is to provide a novel lighting circuit based on a different step-up method that does not use a step-up transformer in an output circuit like a conventional inverter circuit.

〔発明の構成及び作用〕[Structure and operation of the invention]

第1図に本発明の一実施例を示す。図中、C+、 Cz
 、 C3はキャパシタ、Lmは主インダクタ、Dはダ
イオード、Qはトランジスタ、Rは抵抗をそれぞれ示す
。その他の符合は第2図と共通に用いている。
FIG. 1 shows an embodiment of the present invention. In the figure, C+, Cz
, C3 is a capacitor, Lm is a main inductor, D is a diode, Q is a transistor, and R is a resistor. Other symbols are used in common with FIG. 2.

本発明は第1図に示すごとく基本的にトランジスタを1
石用いた自励発振回路である。主インダクタLmに生ず
る電圧の一部を捲線Nf によってトランジスタのベー
スへ帰還させることによって自励発振が持続し、Lm、
Cz及びDを含む主電流回路に正弦波状の高周波の交番
電流が発生し、放電管を点灯させる。なお従来例の第2
図の場合も自励発振回路であってこの場合も出カドラン
スTの出力電圧の一部をIt’線N4によりトランジス
タQ(、Qb のベースへ帰還させることによって自励
発振を生じさせる点は本発明と同様である。
The present invention basically consists of one transistor as shown in FIG.
This is a self-excited oscillation circuit using a stone. Self-oscillation is sustained by feeding back part of the voltage generated in the main inductor Lm to the base of the transistor through the winding Nf, and Lm,
A sinusoidal high frequency alternating current is generated in the main current circuit including Cz and D, lighting the discharge tube. Note that the second conventional example
The case shown in the figure is also a self-excited oscillation circuit, and the main point here is that self-oscillation is generated by feeding back a part of the output voltage of the output transformer T to the base of the transistor Q (, Qb) through the It' line N4. Similar to invention.

本発明回路の特徴は放電管りが出カドランスを介さずに
接続される点にある。この回路は放電管りの始動後は基
本的に主インダクタLm。
A feature of the circuit of the present invention is that the discharge tubes are connected without an output transformer. This circuit is basically the main inductor Lm after the discharge tube starts.

キャパシタCz及び放電管りの直列振動回路であり主電
流はLm −Cz−Dの間で流れる。放電管りの始動前
は熱陰極H+ 、 Hz間は高インピーダンスであるの
で直列振動回路はLm、Cz、)(11キヤパシタC3
、Hi間で構成される。ところが熱陰極H+  及びH
zのヒーターコイルの抵抗値は比較的小さい値であるの
で直列振動回路は極めて振動的となり回路に大きな電圧
が発生する。
It is a series oscillating circuit of a capacitor Cz and a discharge tube, and the main current flows between Lm-Cz-D. Before starting the discharge tube, there is high impedance between the hot cathode H+ and Hz, so the series oscillation circuit is Lm, Cz, ) (11 capacitor C3
, Hi. However, the hot cathodes H+ and H
Since the resistance value of the heater coil z is relatively small, the series oscillating circuit becomes extremely oscillatory and a large voltage is generated in the circuit.

振動の周波数はキャパシタCz と03 が直列的に接
続されることによりキャパシタCλのみが支配的である
始動後の通常点灯時のそれよりも高い。この高周波は高
電圧とし熱陰極H+  −Hz間にかかるとともに電流
として熱陰極H+。
The frequency of the vibration is higher than that during normal lighting after startup, in which only the capacitor Cλ is dominant because the capacitors Cz and 03 are connected in series. This high frequency is applied as a high voltage between the hot cathode H+ and the hot cathode H+ as a current.

Hzに流れるので放電管りの始動は容易に起こる。Since the current flows at Hz, starting of the discharge tube occurs easily.

始動を確かにするための電圧や電流の条件はキャパシタ
C+、C工の大きさや比によって適当な範囲に選ぶこと
ができる。因に、入力電源100vを整流して得られる
直流電源を用いる時でも実効値は300V以上の2次電
圧をキャパシタC3端子間に容易に得ることができる。
The voltage and current conditions to ensure starting can be selected within an appropriate range depending on the size and ratio of capacitors C+ and C. Incidentally, even when using a DC power source obtained by rectifying an input power source of 100 V, a secondary voltage with an effective value of 300 V or more can be easily obtained between the terminals of the capacitor C3.

放電管りが始動した後は該放電管りのインピーダンスが
小さくなり管電圧(熱陰極HI   HL間の電圧)が
小さくなるので、キャパシタCJの経路(ヒーター回路
)に流れる電流は減少しキャパシタC2Lを含む主電流
回路の電流が増加して放電管りは通常の点灯状態に達す
る。
After the discharge tube starts, the impedance of the discharge tube decreases and the tube voltage (voltage between hot cathodes HI and HL) decreases, so the current flowing through the path of capacitor CJ (heater circuit) decreases and the current flowing through capacitor C2L decreases. The current in the main current circuit increases and the discharge tube reaches its normal lighting state.

このように本発明は放電管始動のための高電圧を従来方
式の如く出カドランスの昇圧によらずL−C−Rの直列
振動回路の共振現象を用いる点が異なり次のように種々
の長所を持つものである。
As described above, the present invention differs in that it uses the resonance phenomenon of the L-C-R series oscillation circuit to generate the high voltage for starting the discharge tube, instead of relying on boosting the output voltage as in the conventional method, and has various advantages as follows. It is something that has.

〔発明考案の効果〕[Effect of invention idea]

出カドランスを用いないので小形、安価とすることがで
きる。トランジスタが1石ですむ上、回路部分も少ない
ので小形、経済的であるばかりでなく故障も少ない。
Since no output transformer is used, it can be made small and inexpensive. Not only does it require a single transistor, it also has fewer circuit parts, making it compact, economical, and less likely to break down.

更に回路の変換効率も90%以上に設計することも可能
でありながら装置全体を従来の2石式(回路の変換効率
 80〜85%)に比べ小形、軽量にすることがで、き
る。
Furthermore, it is possible to design a circuit with a conversion efficiency of 90% or more, while making the entire device smaller and lighter than the conventional two-stone type (circuit conversion efficiency of 80-85%).

なお、本発明は自励回路について述べたが、トランジス
タの駆動を主インダクタからの帰還電圧によらず、別の
信号源の電圧を用いて他励式としても本発明の効果は同
様である。
Although the present invention has been described with respect to a self-excited circuit, the effects of the present invention are the same even if the transistor is driven by a separately excited type using the voltage of another signal source instead of relying on the feedback voltage from the main inductor.

4、図の簡単な説明 第1図は本発明に係る点灯装置の実施例、第2図は従来
の点灯措置の実施例を示す。
4. Brief Description of the Figures FIG. 1 shows an embodiment of a lighting device according to the present invention, and FIG. 2 shows an embodiment of a conventional lighting device.

Claims (2)

【特許請求の範囲】[Claims] (1)直流電源若しくは交流電源を整流して得られる直
流電源から補助インダクタを介して接続される、少なく
ともトランジスタと第1のキャパシタからなる並列接続
回路に対して並列に主インダクタと第2のキャパシタ及
び2個の熱陰極を有する放電管との直列回路を接続して
なり、該熱陰極の間に第3のキャパシタが接続されてい
ることを特徴とする放電管の点灯装置。
(1) A main inductor and a second capacitor connected in parallel to a parallel connection circuit consisting of at least a transistor and a first capacitor, which is connected via an auxiliary inductor from a DC power source obtained by rectifying a DC power source or an AC power source. and a discharge tube having two hot cathodes connected in a series circuit, and a third capacitor being connected between the hot cathodes.
(2)トランジスタが主インダクタに発生する帰還電圧
により駆動されることにより自励発振するように構成し
たことを特徴とする特許請求の範囲第1項記載の放電管
の点灯装置。
(2) The discharge tube lighting device according to claim 1, wherein the transistor is configured to self-oscillate by being driven by a feedback voltage generated in the main inductor.
JP26718985A 1985-11-29 1985-11-29 Hot-cathode discharge tube burner Pending JPS62128495A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26718985A JPS62128495A (en) 1985-11-29 1985-11-29 Hot-cathode discharge tube burner

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26718985A JPS62128495A (en) 1985-11-29 1985-11-29 Hot-cathode discharge tube burner

Publications (1)

Publication Number Publication Date
JPS62128495A true JPS62128495A (en) 1987-06-10

Family

ID=17441350

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26718985A Pending JPS62128495A (en) 1985-11-29 1985-11-29 Hot-cathode discharge tube burner

Country Status (1)

Country Link
JP (1) JPS62128495A (en)

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