JPH0536484A - Discharge lamp lighting apparatus - Google Patents
Discharge lamp lighting apparatusInfo
- Publication number
- JPH0536484A JPH0536484A JP3212983A JP21298391A JPH0536484A JP H0536484 A JPH0536484 A JP H0536484A JP 3212983 A JP3212983 A JP 3212983A JP 21298391 A JP21298391 A JP 21298391A JP H0536484 A JPH0536484 A JP H0536484A
- Authority
- JP
- Japan
- Prior art keywords
- discharge lamp
- starting
- rectangular wave
- circuit
- voltage
- 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.)
- Granted
Links
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02B—CLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO BUILDINGS, e.g. HOUSING, HOUSE APPLIANCES OR RELATED END-USER APPLICATIONS
- Y02B20/00—Energy efficient lighting technologies, e.g. halogen lamps or gas discharge lamps
Landscapes
- Circuit Arrangements For Discharge Lamps (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は、インバータを用いて
矩形波点灯するようにした、メタルハライドランプ等の
高輝度放電灯の点灯装置の改良に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an improvement of a lighting device for a high-intensity discharge lamp such as a metal halide lamp, which is lit by a rectangular wave using an inverter.
【0002】[0002]
【従来の技術】近年、メタルハライドランプ等の高輝度
放電灯が各種光源として普及し始めており、かかる放電
灯の点灯装置も、従来の漏洩変圧器と主コンデンサとか
らなる進相型安定器など銅鉄形の安定器を用いてランプ
を点灯する方式から、高周波インバータを用いた方式、
更にはインバータを用いた矩形波点灯方式へと、小型軽
量化が計られるようになってきている。2. Description of the Related Art In recent years, high-intensity discharge lamps such as metal halide lamps have begun to spread as various light sources. Lighting devices for such discharge lamps are also used in conventional phase-advancing ballasts such as leakage transformers and main capacitors. From a method of lighting a lamp using an iron ballast to a method using a high frequency inverter,
Furthermore, the rectangular wave lighting system using an inverter is being reduced in size and weight.
【0003】図4は、従来の矩形波点灯方式の点灯装置
の構成例を示す図で、1は商用電源、2は整流素子、3
は平滑コンデンサからなる平滑回路、4は電流制御を行
うための降圧形チョッパ回路、5はフルブリッジ形イン
バータであり、6は始動用パルストランス、7は前記フ
ルブリッジ形インバータ5の出力端子間に抵抗8を介し
て接続された双方向性二端子半導体スイッチング素子
(SSS)、9は前記始動用パルストランス6の中間タ
ップと、前記半導体スイッチング素子7と抵抗8との接
続点間に接続されたコンデンサであり、これらの始動用
パルストランス6と半導体スイッチング素子7と抵抗8
とコンデンサ9とで始動回路を構成している。なお10は
前記フルブリッジ形インバータ5の出力端子に前記始動
回路を介して接続されたメタルハライドランプである。FIG. 4 is a diagram showing an example of the configuration of a conventional rectangular wave lighting type lighting device, in which 1 is a commercial power source, 2 is a rectifying element, and 3 is a rectifier.
Is a smoothing circuit composed of a smoothing capacitor, 4 is a step-down chopper circuit for controlling current, 5 is a full bridge inverter, 6 is a starting pulse transformer, and 7 is between the output terminals of the full bridge inverter 5. A bidirectional two-terminal semiconductor switching element (SSS) 9 connected through a resistor 8 was connected between the intermediate tap of the starting pulse transformer 6 and a connection point between the semiconductor switching element 7 and the resistor 8. A capacitor, a starting pulse transformer 6, a semiconductor switching element 7, and a resistor 8
The capacitor 9 and the capacitor 9 constitute a starting circuit. Reference numeral 10 is a metal halide lamp connected to the output terminal of the full-bridge inverter 5 via the starting circuit.
【0004】このように構成された点灯装置において
は、商用電源1は整流素子2で整流され、平滑回路3及
びチョッパ回路4を介してフルブリッジ形インバータ5
に入力される。そして該インバータ5の動作により矩形
波交番電圧が始動回路を介してメタルハライドランプ10
に印加される。始動回路に矩形波交番電圧が印加される
と、コンデンサ9が充電を開始し、その充電電圧が半導
体スイッチング素子7のブレークオーバ電圧を越える
と、半導体スイッチング素子7がオン状態になり、コン
デンサ9の放電電流が半導体スイッチング素子7を介し
てパルストランス6に急激に流れる。これによりパルス
トランス6に高圧パルスが発生し、メタルハライドラン
プ10に印加されて、該ランプ10が始動し、矩形波点灯が
行われる。この矩形波点灯方式は、矩形波が印加される
ため、ランプのちらつきが少なく良好な点灯が行われ
る。In the lighting device configured as described above, the commercial power source 1 is rectified by the rectifying element 2, and the full bridge inverter 5 is passed through the smoothing circuit 3 and the chopper circuit 4.
Entered in. Then, by the operation of the inverter 5, a rectangular wave alternating voltage is supplied to the metal halide lamp 10 via the starting circuit.
Applied to. When a rectangular wave alternating voltage is applied to the starting circuit, the capacitor 9 starts charging, and when the charging voltage exceeds the breakover voltage of the semiconductor switching element 7, the semiconductor switching element 7 is turned on and the capacitor 9 The discharge current suddenly flows into the pulse transformer 6 via the semiconductor switching element 7. As a result, a high-voltage pulse is generated in the pulse transformer 6 and applied to the metal halide lamp 10, the lamp 10 is started, and rectangular wave lighting is performed. In this rectangular wave lighting method, since a rectangular wave is applied, flicker of the lamp is reduced and good lighting is performed.
【0005】[0005]
【発明が解決しようとする課題】ところで、上記のよう
な矩形波点灯方式の放電灯点灯装置は、始動後は矩形波
の印加により良好な点灯が行われるが、始動時において
は、パルストランス6,半導体スイッチング素子7,抵
抗8,コンデンサ9からなる始動回路において発生する
始動パルスの幅が狭く、したがって始動パルスエネルギ
ーが小さく、始動が困難である。By the way, in the discharge lamp lighting device of the rectangular wave lighting type as described above, good lighting is performed by applying the rectangular wave after starting, but at the time of starting, the pulse transformer 6 is used. The width of the starting pulse generated in the starting circuit consisting of the semiconductor switching element 7, the resistor 8 and the capacitor 9 is narrow, and therefore the starting pulse energy is small and the starting is difficult.
【0006】始動パルス幅を広くするには、パルストラ
ンス6のインダクタンスLとコンデンサ9の容量Cを大
きくすれば可能であるが、点灯装置の大型化を招き、イ
ンバータを用い小型軽量化するという目的に反すること
になる。また半導体スイッチング素子7の電流容量の制
限からもコンデンサ9の容量はさほど大きくできない。
また始動パルスの発生数は多いほど始動が容易になる
が、上記始動回路における始動パルスの発生数は、半導
体スイッチング素子のブレークオーバ電圧とコンデンサ
及び抵抗の時定数とで決まるので、パルス幅の広い始動
パルスの発生数を大にするには、パルス幅に対応してコ
ンデンサを大きくしている関係上、抵抗値を小さくしな
ければならず、高ワットの抵抗が必要となり大型化する
という問題点が生ずる。The starting pulse width can be widened by increasing the inductance L of the pulse transformer 6 and the capacitance C of the capacitor 9, but the purpose is to increase the size of the lighting device and to reduce the size and weight of the inverter. Will be contrary to. Further, due to the limitation of the current capacity of the semiconductor switching element 7, the capacity of the capacitor 9 cannot be so large.
The larger the number of starting pulses generated, the easier the starting. However, since the number of starting pulses generated in the above-mentioned starting circuit is determined by the breakover voltage of the semiconductor switching element and the time constant of the capacitor and the resistor, the pulse width is wide. In order to increase the number of start-up pulses generated, the resistance value must be reduced because the capacitor is enlarged corresponding to the pulse width, and a high wattage resistance is required, resulting in an increase in size. Occurs.
【0007】本発明は、従来の矩形波点灯方式の放電灯
点灯装置における上記問題点を解消するためになされた
もので、パルスエネルギーの大なる始動パルスを発生で
きる始動回路を備え始動の容易な放電灯点灯装置を提供
することを目的とする。The present invention has been made in order to solve the above problems in the discharge lamp lighting device of the conventional rectangular wave lighting system, and is provided with a starting circuit capable of generating a starting pulse with a large pulse energy and is easy to start. An object is to provide a discharge lamp lighting device.
【0008】[0008]
【課題を解決するための手段及び作用】上記問題点を解
決するため、本発明は、直流を降圧形チョッパ回路に入
力して電流制御を行い該降圧形チョッパ回路の出力をイ
ンバータに入力し、該インバータの出力端に放電灯を接
続して矩形波点灯する放電灯点灯装置において、前記放
電灯に直列に接続したインダクタと該放電灯に並列に接
続した非線形コンデンサとからなる始動回路を設けるも
のである。In order to solve the above-mentioned problems, the present invention inputs direct current to a step-down chopper circuit for current control and inputs the output of the step-down chopper circuit to an inverter, A discharge lamp lighting device for connecting a discharge lamp to an output terminal of the inverter and lighting a rectangular wave, wherein a starting circuit including an inductor connected in series to the discharge lamp and a non-linear capacitor connected in parallel to the discharge lamp is provided. Is.
【0009】このような構成の始動回路を設けた放電灯
点灯装置においては、インバータから出力される矩形波
交流電圧の立ち上がり及び立ち下がりの大きな電圧変化
時に、非線形コンデンサに急激に充電電流が流れ、充電
電荷が直ちに飽和して非線形コンデンサの飽和電圧に達
し、充電電流は急激に零となる。この時、直列インダク
タにより矩形波交流電圧と同極性の高圧パルスが発生
し、放電灯に印加される。この高圧パルスは、非線形コ
ンデンサの特性上、パルス幅が大きく、したがって放電
灯は半導体スイッチング素子を要することなく、大なる
エネルギーのパルスにより容易に始動する。In the discharge lamp lighting device provided with the starter circuit having such a configuration, when the rectangular wave AC voltage output from the inverter changes greatly at rising and falling, a charging current rapidly flows through the non-linear capacitor, The charge immediately saturates and reaches the saturation voltage of the non-linear capacitor, and the charge current rapidly drops to zero. At this time, a high voltage pulse having the same polarity as the rectangular wave AC voltage is generated by the series inductor and applied to the discharge lamp. This high-voltage pulse has a large pulse width due to the characteristics of the non-linear capacitor, and therefore the discharge lamp does not require a semiconductor switching element and can be easily started by a pulse of large energy.
【0010】[0010]
【実施例】次に実施例について説明する。図1は、本発
明に係る放電灯点灯装置の一実施例を示す回路構成図で
あり、図4に示した従来の放電灯点灯装置と同一又は対
応する部材には同一符号を付して、その説明を省略す
る。本発明における始動回路は、フルブリッジ形インバ
ータ5の出力端子からメタルハライドランプ10へ矩形波
交流電圧を印加する回路に直列に挿入したインダクタ11
と、メタルハライドランプ10に並列に接続した非線形V
−Q特性を有する強誘電体からなる非線形コンデンサ12
とで構成されている。EXAMPLES Next, examples will be described. FIG. 1 is a circuit configuration diagram showing an embodiment of the discharge lamp lighting device according to the present invention, and the same or corresponding members as those of the conventional discharge lamp lighting device shown in FIG. The description is omitted. The starting circuit in the present invention is an inductor 11 inserted in series with a circuit for applying a rectangular wave AC voltage from the output terminal of the full-bridge inverter 5 to the metal halide lamp 10.
And a non-linear V connected in parallel to the metal halide lamp 10.
Non-linear capacitor 12 made of ferroelectric material having -Q characteristic
It consists of and.
【0011】次にこのように構成した始動回路を備えた
放電灯点灯装置の動作について説明する。フルブリッジ
形インバータ5から出力される矩形波交流電圧が始動回
路に印加されると、矩形波交流電圧の立ち上がり及び立
ち下がりの大きな電圧変化時に、非線形コンデンサ12に
急激に充電電流が流れ、充電電荷が直ちに飽和して非線
形コンデンサ12の飽和電圧に達し、充電電流は急激に零
となる。この時、図2に示すように、直列インダクタ11
により矩形波交流電圧と同極性の高圧パルスPが発生
し、メタルハライドランプ10に印加される。なお図2に
おいては、比較のため、図4に示した従来の放電灯点灯
装置において発生する始動パルスP′を波線で示してい
る。このこの高圧始動パルスPは、非線形コンデンサ12
の特性上、図3の(A)の拡大図で示すように、図3の
(B)の拡大図で示す従来装置の高圧始動パルスP′に
比べ、パルス幅が大きく、メタルハライドランプ10は容
易に始動する。Next, the operation of the discharge lamp lighting device having the starting circuit configured as described above will be described. When the rectangular-wave AC voltage output from the full-bridge inverter 5 is applied to the starting circuit, a charging current suddenly flows through the nonlinear capacitor 12 when the rectangular-wave AC voltage changes greatly at rising and falling, and the charging charge is increased. Is immediately saturated and reaches the saturation voltage of the non-linear capacitor 12, and the charging current suddenly becomes zero. At this time, as shown in FIG.
As a result, a high-voltage pulse P having the same polarity as the rectangular wave AC voltage is generated and applied to the metal halide lamp 10. In FIG. 2, for comparison, a starting pulse P ′ generated in the conventional discharge lamp lighting device shown in FIG. 4 is shown by a wavy line. This high-voltage starting pulse P is applied to the nonlinear capacitor 12
3A, the pulse width is larger than that of the high-pressure starting pulse P'of the conventional device shown in the enlarged view of FIG. 3B, and the metal halide lamp 10 is easy to use. To start.
【0012】このように本発明においては、矩形波点灯
方式と非線形コンデンサからなる始動回路との組み合わ
せにより、通常の商用電源電圧とは異なり、矩形波交流
電圧の急激な立ち上がり及び立ち下がり時に、同極性の
パルス幅の大なるパルスが発生する。したがって半導体
スイッチング素子を要することなく、サイクル毎に確実
に大きなエネルギーをもつ高圧パルスが発生し、容易に
ランプを始動させることができ、始動回路を更に小型,
軽量化することができる。As described above, in the present invention, the combination of the rectangular wave lighting system and the starting circuit composed of the non-linear capacitor, unlike the normal commercial power supply voltage, causes the same time when the rectangular wave AC voltage rapidly rises and falls. A pulse with a large polarity pulse width is generated. Therefore, without the need for a semiconductor switching element, a high-voltage pulse with a large amount of energy is generated reliably in each cycle, the lamp can be easily started, and the starting circuit can be made smaller and smaller.
The weight can be reduced.
【0013】[0013]
【発明の効果】以上実施例に基づいて説明したように、
本発明は、矩形波点灯方式の放電灯点灯装置における始
動回路をインダクタと非線形コンデンサとで構成したの
で、パルス幅の広い始動パルスをサイクル毎に発生させ
ることができ、矩形波点灯方式において放電灯を容易に
始動させることができる。As described above on the basis of the embodiments,
According to the present invention, since the starting circuit in the discharge lamp lighting device of the rectangular wave lighting system is composed of the inductor and the non-linear capacitor, a starting pulse having a wide pulse width can be generated in each cycle, and the discharge lamp in the rectangular wave lighting system is generated. Can be easily started.
【図1】本発明に係る放電灯点灯装置の一実施例を示す
回路構成図である。FIG. 1 is a circuit configuration diagram showing an embodiment of a discharge lamp lighting device according to the present invention.
【図2】図1に示した実施例における始動回路による高
圧始動パルスの発生態様を示す図である。FIG. 2 is a diagram showing how a high-voltage starting pulse is generated by a starting circuit in the embodiment shown in FIG.
【図3】図2の拡大部分図である。FIG. 3 is an enlarged partial view of FIG.
【図4】従来の放電灯点灯装置の構成例を示す回路構成
図である。FIG. 4 is a circuit configuration diagram showing a configuration example of a conventional discharge lamp lighting device.
1 商用電源 2 整流素子 3 平滑回路 4 降圧形チョッパ回路 5 フルブリッジ形インバータ 10 メタルハライドランプ 11 インダクタ 12 非線形コンデンサ 1 Commercial power supply 2 Rectifier element 3 Smoothing circuit 4 Step-down type chopper circuit 5 Full bridge type inverter 10 Metal halide lamp 11 Inductor 12 Non-linear capacitor
フロントページの続き (72)発明者 寺山 一郎 埼玉県北埼玉郡川里村赤城台212−10 株 式会社アイ・ライテイング・システム埼玉 製作所内 (72)発明者 佐々木 俊一 埼玉県行田市壱里山町1−1 岩崎電気株 式会社埼玉製作所内Front Page Continuation (72) Ichiro Terayama, Inventor Ichiro Terayama 212-10 Akagidai, Kawasato-mura, Kita-Saitama-gun, Saitama I-Liting System Saitama Factory (72) Inventor Shunichi Sasaki 1-1, Iriyama-cho, Gyoda-shi, Saitama Iwasaki Electric Co., Ltd. Saitama Factory
Claims (1)
流制御を行い該降圧形チョッパ回路の出力をインバータ
に入力し、該インバータの出力端に放電灯を接続して矩
形波点灯する放電灯点灯装置において、前記放電灯に直
列に接続したインダクタと該放電灯に並列に接続した非
線形コンデンサとからなる始動回路を備えたことを特徴
とする放電灯点灯装置。1. A discharge lamp for inputting direct current to a step-down chopper circuit to control current, inputting an output of the step-down chopper circuit to an inverter, and connecting a discharge lamp to an output end of the inverter to illuminate a rectangular wave. A discharge lamp lighting device, comprising: a starting circuit including an inductor connected in series to the discharge lamp and a non-linear capacitor connected in parallel to the discharge lamp.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21298391A JP3323521B2 (en) | 1991-07-31 | 1991-07-31 | Discharge lamp lighting device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21298391A JP3323521B2 (en) | 1991-07-31 | 1991-07-31 | Discharge lamp lighting device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0536484A true JPH0536484A (en) | 1993-02-12 |
JP3323521B2 JP3323521B2 (en) | 2002-09-09 |
Family
ID=16631529
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP21298391A Expired - Fee Related JP3323521B2 (en) | 1991-07-31 | 1991-07-31 | Discharge lamp lighting device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3323521B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2009158495A (en) * | 2009-04-14 | 2009-07-16 | Eye Lighting Syst Corp | Discharge lamp lighting device |
-
1991
- 1991-07-31 JP JP21298391A patent/JP3323521B2/en not_active Expired - Fee Related
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2009158495A (en) * | 2009-04-14 | 2009-07-16 | Eye Lighting Syst Corp | Discharge lamp lighting device |
Also Published As
Publication number | Publication date |
---|---|
JP3323521B2 (en) | 2002-09-09 |
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