JPH02207490A - Electronic lighting device for fluorescent lamp - Google Patents
Electronic lighting device for fluorescent lampInfo
- Publication number
- JPH02207490A JPH02207490A JP2629089A JP2629089A JPH02207490A JP H02207490 A JPH02207490 A JP H02207490A JP 2629089 A JP2629089 A JP 2629089A JP 2629089 A JP2629089 A JP 2629089A JP H02207490 A JPH02207490 A JP H02207490A
- Authority
- JP
- Japan
- Prior art keywords
- resistor
- voltage
- gate
- negative
- diode
- 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
- 230000015556 catabolic process Effects 0.000 description 7
- 230000006378 damage Effects 0.000 description 4
- 230000007423 decrease Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 239000003990 capacitor Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 230000000630 rising effect Effects 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- 230000000903 blocking effect Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000007858 starting material Substances 0.000 description 1
Landscapes
- Circuit Arrangements For Discharge Lamps (AREA)
Abstract
Description
【発明の詳細な説明】
[技術分野]
本発明は放電灯の点灯装置に関するもので、詳細には、
予熱電極を有する蛍光放電灯のための半導体素子を利用
した点灯始動装置に関し、特に、始動パルスの発生の安
定化を目的とした電子点灯装置に関するものである。[Detailed Description of the Invention] [Technical Field] The present invention relates to a lighting device for a discharge lamp.
The present invention relates to a lighting starting device using a semiconductor element for a fluorescent discharge lamp having a preheating electrode, and particularly to an electronic lighting device whose purpose is to stabilize the generation of a starting pulse.
従来予熱型蛍光灯の始動装置としては、主にグロースタ
ーターが用いられて来たが、始動時間が長く、又寿命が
短いなどの欠点を有していた。Conventionally, glow starters have been mainly used as starting devices for preheating fluorescent lamps, but they have drawbacks such as long starting times and short lifespans.
近年上記欠点をなくすため、半導体スイッチを利用した
、いわゆる電子点灯装置が開発されてきた。しかしこの
種の装置は回路構成が複雑となり製作コストが高く需要
の制約があった。In recent years, so-called electronic lighting devices using semiconductor switches have been developed to eliminate the above drawbacks. However, this type of device has a complicated circuit configuration, high manufacturing costs, and limited demand.
上記の要請に基づき、公知例として第1図に示す回路が
ある0図中Eは商用交流電源、FLは蛍光灯、Thyは
ゲート付単方向サイリスタ(以下説明上SCRとして記
載)、ZDはツェナーダイオード、DI。Based on the above request, there is a circuit shown in Figure 1 as a known example. In the figure, E is a commercial AC power supply, FL is a fluorescent lamp, Thy is a gated unidirectional thyristor (hereinafter referred to as SCR for explanation), and ZD is a Zener. Diode, DI.
D2は整流ダイオード、C1はコンデンサー、CHはチ
ョークトランス、R1−R3は抵抗を夫々示す。D2 is a rectifier diode, C1 is a capacitor, CH is a choke transformer, and R1-R3 are resistors.
次に、回路動作を、第2図の各部波形図に従い説明する
。 図中VEは電源電圧波形、lhは予熱電流波形、V
pは蛍光灯の管電圧、即ち5CRThy(r)A−に間
の電圧波形である。今SCHの順方向阻止状態で電源電
圧VEが上昇すると(a点)蛍光灯FLの管電圧、即ち
SCRのA−に問電圧Vpも上昇し、抵抗R1,R2の
分割電圧がツェナーZDの動作電圧に達すると、波形V
B点にてSCRはターンオンし、予熱電流Ihは電源E
よりチョークトランスCH−蛍光灯ヒラメントhl−3
CRA〜に一ダイオードD2−ヒラメントh2−電源E
と流れ、各ヒラメントは予熱される。又電源Eの逆サイ
クルに於いて、電源E−ダイオードD1−3CRゲート
−3CRカツ、−ドーダイオードD2−ヒラメントh2
−電源と、SCRG−に問には逆バイアス電圧が印加さ
れ丁いる。かかる状態に於いて予熱電流Ihが減少しS
CRのアノードtlが保持電流以下となった点Cにてオ
フとなり、逆バイアス電圧効果と相まって、チョークト
ランスのリアクション電圧VPPが発生し、この電圧が
蛍光灯FLの両電極間に印加される事により、数サイク
ル後点灯にいたる0図中波形vbは点灯後の管電圧ピー
ク値波形を示し、点灯後はEの最大値のVmの間に設定
される。コンデンサーc1は管電圧ピーク値vbが特に
低温時に於いては高くなるため、この電圧のためSCR
の再点弧を防止するためのフィルター用コンデンサーで
ある。Next, the circuit operation will be explained according to the waveform diagram of each part shown in FIG. In the figure, VE is the power supply voltage waveform, lh is the preheating current waveform, and V
p is the tube voltage of the fluorescent lamp, ie, the voltage waveform between 5CRThy(r)A-. Now, when the power supply voltage VE increases in the forward blocking state of SCH (point a), the tube voltage of the fluorescent lamp FL, that is, the voltage Vp at A- of the SCR also increases, and the divided voltage of resistors R1 and R2 changes the operation of the Zener ZD. When the voltage is reached, the waveform V
The SCR turns on at point B, and the preheating current Ih is connected to the power supply E.
More choke transformer CH-fluorescent lamp Hilament HL-3
CRA ~ 1 diode D2 - Hirament h2 - Power supply E
, and each filament is preheated. Also, in the reverse cycle of power supply E, power supply E - diode D1 - 3CR gate - 3CR cut, - do diode D2 - filament h2
A reverse bias voltage is applied to the -power supply and SCRG-. In such a state, the preheating current Ih decreases and S
The anode tl of CR is turned off at point C when it becomes below the holding current, and combined with the reverse bias voltage effect, a reaction voltage VPP of the choke transformer is generated, and this voltage is applied between both electrodes of the fluorescent lamp FL. Accordingly, the waveform vb in FIG. 0, which reaches lighting after several cycles, indicates the tube voltage peak value waveform after lighting, and after lighting is set between Vm, the maximum value of E. The capacitor c1 has a tube voltage peak value vb that becomes high especially at low temperatures, so the SCR
This is a filter capacitor to prevent re-ignition.
するため、その電圧変動に対して、発生パルスも変動し
、特にサイリスタの順方向耐圧を越えてサイリスタの破
壊に至る場合がある。Therefore, in response to the voltage fluctuation, the generated pulse also fluctuates, and in particular, the forward breakdown voltage of the thyristor may be exceeded, leading to destruction of the thyristor.
2)パルス発生電圧は、特に使用温度の低域下に於ける
サイリスタのブレークダウン特性の改善及び、保持電流
の増大によって上昇する傾向にあって、ひいてはサイリ
スタの順方向耐圧を越え、サイリスタの破壊に至る場合
がある。2) The pulse generation voltage tends to increase due to the improvement of the breakdown characteristics of the thyristor and the increase in the holding current, especially at low operating temperatures, and may eventually exceed the forward breakdown voltage of the thyristor, causing destruction of the thyristor. It may lead to.
夕をブレークダウンに至らしめる可能性があり実用上の
制約があった。There was a practical restriction because it could lead to a breakdown in the evening.
[発明の目的1
本発明に於いては、係る問題点を解決する事によって、
実用的な始動装置を提供する事にある。[Objective of the invention 1 In the present invention, by solving the problems,
The purpose is to provide a practical starting device.
[発明の開示]
第3図は本発明に係る回路例を示し、図中、同符号は第
1図以下に準するものとし、R5は抵抗、ZDIはツェ
ナーダイオード、Thは負特性感温素子(以下サーミス
タと呼称)を夫々示す。[Disclosure of the Invention] FIG. 3 shows an example of a circuit according to the present invention. In the figure, the same reference numerals refer to those in FIG. (hereinafter referred to as a thermistor).
第4図は、説明のための波形例をしめす、 以下、点灯
に係る動作原理については、既に第1図、第2図に於い
て説明した通りであって、省略するとして、以下系3、
第4図に従って、サイリスタの負ゲートバイアス回路に
ついて説明すると、本発明に於いては図中抵抗R5とツ
ェナーダイオードZDI及びサーミスタThを追加した
事を特徴とするものであって、従来回路によれば、交流
電源Eに対して、ダイオードD1と抵抗R4、ダイオー
ドD2による直列回路によって11IrLされているた
め、交流電源Eの電圧変動による依存性を所有し、その
電圧変動によって、ゲートバイアス電流も比例的に変化
する。 この結果、第5因中実線で示すように、発生す
る高圧パルスVPPは、当然変化する。この発生電圧は
、サイリスタゲート特性のバラツキ等によって、交流電
源の上昇時に於いては、ブレークダウンするものが発生
しその結果、時にはサイリスタの破壊に至る場合が起こ
る。FIG. 4 shows an example of a waveform for explanation.The operating principle related to lighting is as already explained in FIGS. 1 and 2, and will be omitted hereafter.
The negative gate bias circuit of the thyristor will be explained with reference to FIG. 4. The present invention is characterized by the addition of a resistor R5, a Zener diode ZDI, and a thermistor Th in the figure, whereas the conventional circuit is , 11IrL is applied to AC power supply E by a series circuit of diode D1, resistor R4, and diode D2, so it has dependence on voltage fluctuation of AC power supply E, and the gate bias current is also proportional to that voltage fluctuation. Changes to As a result, the generated high voltage pulse VPP naturally changes as shown by the solid line for the fifth factor. Due to variations in the thyristor gate characteristics, this generated voltage may break down when the AC power source rises, and as a result, the thyristor may sometimes be destroyed.
本発明に於いては、係る問題を解消すべく成されたもの
であって、今交流電源電圧VEが上昇した場合抵抗R5
、ツェナーダイオードZDlによって、上昇電圧を一定
に制限しく第4図中VZD 1 ) 、従って、ゲート
に流入する負ゲート電流は、抵抗R4をして、略一定に
保たれる。この結果発生する高圧パルスVpPは、第5
図中点線で示したように、略一定に保たれ、その発生電
圧は、ツェナーダイオードの特性に依存する。The present invention has been made to solve this problem, and when the AC power supply voltage VE increases, the resistor R5
The rising voltage is limited to a constant level by the Zener diode ZDl (VZD 1 ) in FIG. 4. Therefore, the negative gate current flowing into the gate is kept substantially constant by the resistor R4. The resulting high voltage pulse VpP is the fifth
As shown by the dotted line in the figure, the voltage is kept approximately constant, and the generated voltage depends on the characteristics of the Zener diode.
その結果、定格状態に設定された定数下に於いては、電
源電圧が上昇しても、その発生電圧は略一定に保たれ、
少なくともサイリスタをブレークダウンに至らしめる要
因は解消された事になる。As a result, under the constant set to the rated state, even if the power supply voltage increases, the generated voltage remains approximately constant.
At least the factor that caused the thyristor to break down has been eliminated.
以上の説明に於いては、電源電圧(VE)の変動による
ものであったが、次に使用温度(T a )が変化した
場合、特に低温条件下に於いてサイリスタのブレークダ
ウン特性の温度依存性による改善、及び保持電流の上昇
に相まって、発生パルスは上昇し、(第5図中1点鎖線
)、時にはブレークダウンに至る。 本発明に於いては
、抵抗R4と並列的にサーミスタThを挿入した事であ
って、今、使用温度が低下した場合、サーミスタThの
動抵抗は増大する特性を有するため、結果的に抵抗R4
との合成抵抗値が増大する方向に働くため、その結果ゲ
ート負バイアス電流は減少すべく作用し、従って発生す
るパルス電圧VPPは制限され減少する。又反対に、温
度が上昇した場合は、抵抗R4との合成抵抗が減少し、
結果的に、ゲート負電流が上昇し、発生パルスは上昇方
向に作用し、略一定に補正される。In the above explanation, it was due to fluctuations in the power supply voltage (VE), but next, when the operating temperature (T a ) changes, the breakdown characteristics of the thyristor are affected by temperature dependence, especially under low temperature conditions. Coupled with the improvement in performance and the increase in holding current, the number of generated pulses increases (dotted chain line in FIG. 5), sometimes leading to breakdown. In the present invention, the thermistor Th is inserted in parallel with the resistor R4, and if the operating temperature decreases, the dynamic resistance of the thermistor Th has a characteristic that increases.As a result, the resistance R4
As a result, the gate negative bias current acts to decrease, and therefore the generated pulse voltage VPP is limited and reduced. Conversely, when the temperature rises, the combined resistance with resistor R4 decreases,
As a result, the gate negative current rises, and the generated pulse acts in the rising direction and is corrected to be substantially constant.
第1図は、従来の点灯装置の動作を説明するための回路
例。
第2図は従来動作を説明するための波形図。
第3図は本発明の回路例。
第4図は本発明の波形図。
第5図は、本発明の特性図を夫々示す。
[発明の効果]
以上説明した如く、従来電源電圧の変動及び使用温度変
化によって、発生するパルス電圧が変動し、時によって
はサイリスタの順方向耐圧を超過して、ブレークダウン
に至り、結果サイリスタの破壊に至る場合が発才す尽FIG. 1 is a circuit example for explaining the operation of a conventional lighting device. FIG. 2 is a waveform diagram for explaining conventional operation. FIG. 3 shows an example of a circuit according to the present invention. FIG. 4 is a waveform diagram of the present invention. FIG. 5 shows characteristic diagrams of the present invention. [Effects of the Invention] As explained above, conventionally, due to fluctuations in power supply voltage and changes in operating temperature, the generated pulse voltage fluctuates and sometimes exceeds the forward withstand voltage of the thyristor, leading to breakdown, resulting in damage to the thyristor. The case that leads to destruction is the cause of death.
Claims (1)
の直列回路と前記放電灯の非電源側予熱電極間に、ゲー
ト付単方向サイリスタを接線して、該非電源側検知電圧
で、サイリスタを躯動する回路と更に該サイリスタのゲ
ートに高圧パルス発生のための負ゲートバイアス電圧を
交流電源より供給するための、ゲート負電流制限用抵抗
と負方向ダイオードを直列接続した回路に於いて、ツェ
ナー用直列抵抗とツェナーダイオードを並列的に介在し
、更に電流制限用抵抗に負特性感温素子を並列に接続し
た事を特徴とする蛍光灯電子点灯装置。A unidirectional thyristor with a gate is connected tangentially between the series circuit of the AC power supply, the choke transformer, and the discharge lamp with a preheating electrode, and the non-power supply side preheating electrode of the discharge lamp, and the thyristor is rotated by the detected voltage on the non-power supply side. In addition, in a circuit in which a gate negative current limiting resistor and a negative diode are connected in series to supply a negative gate bias voltage for generating high voltage pulses to the gate of the thyristor from an AC power supply, An electronic lighting device for a fluorescent lamp, characterized in that a resistor and a Zener diode are interposed in parallel, and a negative temperature sensing element is connected in parallel to the current limiting resistor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2629089A JPH02207490A (en) | 1989-02-03 | 1989-02-03 | Electronic lighting device for fluorescent lamp |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2629089A JPH02207490A (en) | 1989-02-03 | 1989-02-03 | Electronic lighting device for fluorescent lamp |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02207490A true JPH02207490A (en) | 1990-08-17 |
Family
ID=12189172
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2629089A Pending JPH02207490A (en) | 1989-02-03 | 1989-02-03 | Electronic lighting device for fluorescent lamp |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02207490A (en) |
-
1989
- 1989-02-03 JP JP2629089A patent/JPH02207490A/en active Pending
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