JPS62154497A - Stable burning of discharge tube for neon signs - Google Patents

Stable burning of discharge tube for neon signs

Info

Publication number
JPS62154497A
JPS62154497A JP29715485A JP29715485A JPS62154497A JP S62154497 A JPS62154497 A JP S62154497A JP 29715485 A JP29715485 A JP 29715485A JP 29715485 A JP29715485 A JP 29715485A JP S62154497 A JPS62154497 A JP S62154497A
Authority
JP
Japan
Prior art keywords
circuit
voltage
discharge tube
neon
present
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
JP29715485A
Other languages
Japanese (ja)
Inventor
丸森 平昭
戸内 博一
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.)
NAT ART KK
NATL ART KK
TOHO DENKI KK
TOUOU DENKI KK
Original Assignee
NAT ART KK
NATL ART KK
TOHO DENKI KK
TOUOU 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 NAT ART KK, NATL ART KK, TOHO DENKI KK, TOUOU DENKI KK filed Critical NAT ART KK
Priority to JP29715485A priority Critical patent/JPS62154497A/en
Publication of JPS62154497A publication Critical patent/JPS62154497A/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】 本発明はネオンサイン用放電管を高周波電流を用いて点
灯する(二坐り、明暗の縞模様を発生させることなく安
定に点灯させるネオンサイン用放電管の安定点灯方法に
関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for stably lighting a discharge tube for a neon sign using high-frequency current (for example, a method for stably lighting a discharge tube for a neon sign without producing a striped pattern of light and darkness). .

近年ネオンサイン用放電管を点灯させる方法として、従
来のネオントランス(二代えて、高周波インバータ回路
を用い、数〜数10 KHzの高周波電流で点灯させ、
電源装置の小型、軽量化を図ることが開発され実用化さ
れつつある。
In recent years, as a method of lighting discharge tubes for neon signs, a conventional neon transformer (instead of the conventional neon transformer), a high frequency inverter circuit is used to light the discharge tube with a high frequency current of several to several tens of KHz.
2. Description of the Related Art Techniques to make power supply devices smaller and lighter are being developed and put into practical use.

この高周波電流を用いる方法は、通常の屋外用ネオンサ
インのよ5C二、放電管を直列に複数本接続したり、文
字や図形を表現するため複雑C二曲折したりすると、放
電管に明所・暗所が交互ご二連らなる縞模様が発生して
実用(:ならない。したがってこの点灯方法はわずか(
=屋内装飾用の小製ネオンサインのみに実用されている
(−すぎない。
This method of using high-frequency current is similar to ordinary outdoor neon signs, and when multiple discharge tubes are connected in series or complicatedly bent to express characters or figures, the discharge tubes can be placed in bright places.・A striped pattern consisting of two alternating dark areas occurs, which is not practical (:).Therefore, this lighting method is only useful (
= Practical only for small neon signs for indoor decoration (not too much).

本発明はこの縞模様の発生を防止し、屋外用ネオンサイ
ンにおいても高周波電流による点灯を実用可能とするこ
とを目的として案出されたものである。
The present invention was devised for the purpose of preventing the occurrence of this striped pattern and making lighting using high-frequency current practical even in outdoor neon signs.

すなわち本発明は、正弦波の正または負の半波において
、ゼロ点からの増大部またはゼロ点への減少部に欠落部
が形成された非対称波形の電圧を有する高周波電流によ
り点灯することを特徴とするネオンサイン用放電管の安
定点灯方法である。
That is, the present invention is characterized in that lighting is performed by a high-frequency current having an asymmetric voltage waveform in which a missing portion is formed in the increasing portion from the zero point or the decreasing portion to the zero point in the positive or negative half wave of the sine wave. This is a stable lighting method for neon sign discharge tubes.

この発明で使用する電圧波形は具体的(二は、第1図6
1 、 lb) 、 le) 、 (d)に示す通りで
あり、(&)は欠落部1が正の半波のゼロ点からの増大
部に形成されたもの、(b)は正の半波のゼロ点への減
少部に形成されたもの、(clは負の半波のゼロ点から
の増大部に形成されたもの、(dlは負の半波のゼロ点
への減少部に形成されたものである。
The voltage waveform used in this invention is specific (see Fig. 1, 6).
1, lb), le), and (d), where (&) is the missing part 1 formed in the increasing part from the zero point of the positive half wave, and (b) is the positive half wave. (cl is formed in the increasing part from the zero point of the negative half-wave, (dl is formed in the decreasing part from the zero point of the negative half-wave) It is something that

なお周波数は1〜100 KHz程度、好ましくは4〜
30 KM、であり、電圧は放電管1m当り500〜1
500’程度である〇 上記の高周波電流を用いてネオンサイン用放電管を点灯
すると、縞模様を発生することな(安定4:作動する。
The frequency is about 1 to 100 KHz, preferably 4 to 100 KHz.
30 KM, and the voltage is 500 to 1 per meter of discharge tube.
500' When a discharge tube for a neon sign is lit using the above high frequency current, no striped pattern is generated (Stable 4: It works.

この縞模様の発生並びにその発生防止のメカニズムは不
明であるが、この作動は実験的に確認されたものである
Although the mechanism by which this striped pattern occurs and its prevention is unknown, this operation has been experimentally confirmed.

なお、メタルハライドランプのような高圧放電−灯を高
周波電流で点灯した際と生じる放電路すなわち発光部分
の曲折を防止する方法として、本発明のようC二電圧波
形を非対称化することが知られている(特開昭59−1
4297号公報)。この場合は、高圧放電灯の管内に生
じる音波と印加高周波との共鳴C二より放電路の曲折が
生じ、非対称化した波形の電流がこの共鳴を防止する作
用をもつという作動メカニズムが明らかとなっている。
It is known that as a method of preventing bending of the discharge path, that is, the light emitting part, which occurs when a high-pressure discharge lamp such as a metal halide lamp is lit with high-frequency current, it is known to make the C2 voltage waveform asymmetrical as in the present invention. (Unexamined Japanese Patent Publication No. 59-1
Publication No. 4297). In this case, the operating mechanism has been clarified: bending of the discharge path occurs due to resonance C2 between the sound waves generated inside the tube of the high-pressure discharge lamp and the applied high frequency, and the current with an asymmetrical waveform has the effect of preventing this resonance. ing.

しかし本発明の場合は、ネオンサイン用放電管の管内圧
力が数■Hgと低いこと等から作動メカニズムは全(異
なるものと推測される。
However, in the case of the present invention, the operating mechanism is presumed to be completely different, since the pressure inside the discharge tube for neon signs is as low as a few μHg.

次に本発明の波形を発生する回路の一例(二ついて述べ
る。
Next, two examples of circuits that generate waveforms according to the present invention will be described.

はじめC第2図に示す通常の正弦波電圧を発生する回路
10について説明する。この回路1oは、トランジスタ
11.12を有する電圧スイッチング回路13゛を直流
電源14とプラス端子15.アース端子16で接続し、
電圧スイッチング回路13の出力端17に。
First, a circuit 10 for generating a normal sinusoidal voltage shown in FIG. 2 will be described. This circuit 1o includes a voltage switching circuit 13' having transistors 11, 12 and a DC power supply 14 and a positive terminal 15. Connect with ground terminal 16,
At the output terminal 17 of the voltage switching circuit 13.

出カドランス18の1次巻線18a、コイル19を直列
(二接続し、さらにこのコイル19を、コンデンサ20
を介し【プラス端子15と、コンデンサ21を介してア
ース端子16とそれぞれ接続したものであり、出カドラ
ンス18の2次巻線18bから出力端子22 、23を
経て、ネオンサイン用放電管(図示しない)と接続する
ようにしたものである。
The primary winding 18a of the output transformer 18 and the coil 19 are connected in series, and this coil 19 is connected to the capacitor 20.
The positive terminal 15 is connected to the ground terminal 16 via the capacitor 21, and the neon sign discharge tube (not shown) is connected from the secondary winding 18b of the output transformer 18 to the output terminals 22 and 23. ).

この回路10では、トランジスタ11.12が交互【ニ
オン・オフ動作をし、トランジスタ11がオン状態のと
き、プラス端子15からトランジスタ11.出カドラン
ス18.コイル19を経てコンデンサ21を充電する電
流及びコンデンサ20からのトランジスタ11゜出カド
ランス18.コイル19を経て流れる放電電流が流れる
@また逆にトランジスタ12がオン状態のときには、コ
ンデンサ20を充電するコイル19.出カドランス18
、トランジスタ12を経てアース端子16に流れる電流
及びコンデンサ21からのコイル19゜出カドランス1
8.トランジスタ12を経て流れる放電電流が流れる。
In this circuit 10, the transistors 11 and 12 alternately perform on-off operation, and when the transistor 11 is in the on state, the positive terminal 15 is connected to the transistor 11. Output Lance 18. Current charging capacitor 21 via coil 19 and transistor 11° output voltage 18 from capacitor 20. A discharge current flows through the coil 19 @ and conversely, when the transistor 12 is on, the coil 19 charges the capacitor 20. Dekadrance 18
, the current flowing to the ground terminal 16 via the transistor 12 and the coil 19° output transformer 1 from the capacitor 21.
8. A discharge current flows through transistor 12.

すなわちこの回路1oの出力端17の電圧V17は第4
図(mlに示すように最大値が直流電源の電圧vcであ
る矩形波であり、出力端子22゜23の電圧v22,2
3はコイ/I/19.  :7ンデy?20.21並び
に負荷のりアクタンス分により同図(c)のように位相
ずれを有する正弦波となる。
That is, the voltage V17 at the output terminal 17 of this circuit 1o is
As shown in the figure (ml), it is a rectangular wave whose maximum value is the voltage vc of the DC power supply, and the voltage v22,2
3 is carp/I/19. :7 days? 20.21 and the load actance result in a sine wave with a phase shift as shown in FIG.

ここで回路10のトランス18とコイル19の間の点2
4の電圧V24に着目すると、この電圧V24は、出力
端の電圧V17から、出力電圧V22,23と相似の電
圧を差引いたものであって第4図(b)に示すような波
形となり、トランジスタ11がオン状態のときにグラス
端子の電圧すなわち直流電源の電圧70以上となる時、
トランジスタ12がオン状態のときにアース端子16の
電圧すなわちゼロ以下となる時がある。そこでこの期間
出方トランスに電流が流れないよう(=すると、本発明
の波形が得られる。
Here, point 2 between transformer 18 and coil 19 of circuit 10
4, this voltage V24 is obtained by subtracting a voltage similar to the output voltages V22 and V23 from the voltage V17 at the output terminal, and has a waveform as shown in FIG. 4(b), and the transistor 11 is in the on state, when the voltage of the glass terminal, that is, the voltage of the DC power supply becomes 70 or more,
When the transistor 12 is in the on state, there are times when the voltage at the ground terminal 16 becomes less than zero. Therefore, if no current flows through the output transformer during this period, the waveform of the present invention can be obtained.

すなわち本発明の波形は第3図g二足す回路110によ
って得られる。この回路110は前記回路1oと全く同
様であり、出カドランス118とコイ/L/119の間
の点124とアース端子116とをダイオード125で
接続したことが異なるだけである。なおこの図(:おい
て、前記回路1oの各箇所に対応する箇所C;その参照
符号に100を加えた数を付して示しである。
That is, the waveform of the present invention is obtained by the g2-summing circuit 110 in FIG. This circuit 110 is exactly the same as the circuit 1o described above, and the only difference is that a diode 125 is used to connect a point 124 between the output transformer 118 and the coil/L/119 to the ground terminal 116. Note that in this figure (:), locations C corresponding to each location of the circuit 1o are indicated by adding 100 to their reference numerals.

したがってこの回路110も前記回路1oと同様に作動
する。しかし点124の電圧■124が負となるべき期
間はダイオード125によりアース端子116と短絡さ
れ、第5図(&)に示すようにゼロとなり、この間の出
力電圧V122.123はゼロとなり第5図(b)に示
す波形が出力される。
Therefore, this circuit 110 also operates in the same manner as the circuit 1o. However, during the period when the voltage at point 124 should be negative, it is short-circuited to the ground terminal 116 by the diode 125 and becomes zero as shown in FIG. The waveform shown in (b) is output.

上記回路110は本発明を実施するための回路の一例で
あり、他g:も本発明の波形は各種の回路によって実現
しうろことはい5までもない。
The circuit 110 described above is an example of a circuit for implementing the present invention, and the waveforms of the present invention may be realized by various circuits.

上述のように本発明は、ネオンサイン用放電管を高周波
電流により点灯するに当り、電圧波形を正弦波の手技の
ゼロ点付近部分C二欠落部を設は非対称としたので、明
暗の縞模様の発生を防止することができる。したがって
屋外用の大型で、複数本直列に接続され、複雑に曲折さ
れた放電管についても高周波電流を用いて点灯すること
が可能となり、’を像装置の小型、軽量化を実現するこ
とができる。
As described above, in the present invention, when lighting a discharge tube for a neon sign with a high-frequency current, the voltage waveform is made asymmetrical in the two missing parts near the zero point of the sine wave technique, so that a bright and dark striped pattern is created. can be prevented from occurring. Therefore, it is possible to use high-frequency current to light even large, outdoor-use discharge tubes connected in series and complicatedly bent, making it possible to make the image device smaller and lighter. .

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

第1図は本発明で使用する電圧波形を示すグラフ、第2
図は通常の正弦波電圧を発生する回路を示す回路図、第
3図は本発明の電圧波形を発生する回路を示す回路図、
第4図は第3図の回路の各部屯圧を示すグラフ、第5図
は第4図の回路の各部電圧を示すグラフである。 1・・・・欠落部。 第1図 第2図 り 第3図 第4図 第5図
Figure 1 is a graph showing the voltage waveform used in the present invention, Figure 2 is a graph showing the voltage waveform used in the present invention.
The figure is a circuit diagram showing a circuit that generates a normal sine wave voltage, FIG. 3 is a circuit diagram showing a circuit that generates a voltage waveform of the present invention,
FIG. 4 is a graph showing voltages at various parts of the circuit shown in FIG. 3, and FIG. 5 is a graph showing voltages at various parts of the circuit shown in FIG. 1... Missing part. Figure 1 Figure 2 Diagram Figure 3 Figure 4 Figure 5

Claims (1)

【特許請求の範囲】[Claims] 1、正弦波の正または負の半波において、ゼロ点からの
増大部またはゼロ点への減少部に欠落部が形成された非
対称波形の電圧を有する高周波電流により点灯すること
を特徴とするネオンサイン用放電管の安定点灯方法。
1. A neon light that is lit by a high-frequency current having an asymmetrical voltage waveform in which a missing part is formed in the increasing part from the zero point or the decreasing part to the zero point in the positive or negative half wave of a sine wave. Stable lighting method for sign discharge tubes.
JP29715485A 1985-12-26 1985-12-26 Stable burning of discharge tube for neon signs Pending JPS62154497A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29715485A JPS62154497A (en) 1985-12-26 1985-12-26 Stable burning of discharge tube for neon signs

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29715485A JPS62154497A (en) 1985-12-26 1985-12-26 Stable burning of discharge tube for neon signs

Publications (1)

Publication Number Publication Date
JPS62154497A true JPS62154497A (en) 1987-07-09

Family

ID=17842894

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29715485A Pending JPS62154497A (en) 1985-12-26 1985-12-26 Stable burning of discharge tube for neon signs

Country Status (1)

Country Link
JP (1) JPS62154497A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6054813A (en) * 1995-04-19 2000-04-25 Harison Electric Co., Ltd. Neon discharging lamp lighting apparatus with improved lighting

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5946795A (en) * 1982-09-10 1984-03-16 東芝ライテック株式会社 Device for firing discharge lamp
JPS59181497A (en) * 1983-03-31 1984-10-15 東芝ライテック株式会社 Fluorescent lamp firing device
JPS6030093A (en) * 1983-07-29 1985-02-15 三菱電機株式会社 Low pressure mercury vapor discharge lamp unit

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5946795A (en) * 1982-09-10 1984-03-16 東芝ライテック株式会社 Device for firing discharge lamp
JPS59181497A (en) * 1983-03-31 1984-10-15 東芝ライテック株式会社 Fluorescent lamp firing device
JPS6030093A (en) * 1983-07-29 1985-02-15 三菱電機株式会社 Low pressure mercury vapor discharge lamp unit

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6054813A (en) * 1995-04-19 2000-04-25 Harison Electric Co., Ltd. Neon discharging lamp lighting apparatus with improved lighting

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