JPH01309249A - Discharge lamp - Google Patents
Discharge lampInfo
- Publication number
- JPH01309249A JPH01309249A JP13892388A JP13892388A JPH01309249A JP H01309249 A JPH01309249 A JP H01309249A JP 13892388 A JP13892388 A JP 13892388A JP 13892388 A JP13892388 A JP 13892388A JP H01309249 A JPH01309249 A JP H01309249A
- Authority
- JP
- Japan
- Prior art keywords
- glass bulb
- conductors
- conductor
- discharge lamp
- recessed
- 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
- 239000004020 conductor Substances 0.000 claims abstract description 37
- 239000011521 glass Substances 0.000 claims abstract description 35
- 229910052751 metal Inorganic materials 0.000 abstract description 9
- 239000002184 metal Substances 0.000 abstract description 9
- 238000010586 diagram Methods 0.000 description 4
- 239000007789 gas Substances 0.000 description 4
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 230000010355 oscillation Effects 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- 238000009412 basement excavation Methods 0.000 description 2
- 239000011261 inert gas Substances 0.000 description 2
- 229910052786 argon Inorganic materials 0.000 description 1
- 238000007599 discharging Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 1
- 229910052753 mercury Inorganic materials 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Non-Portable Lighting Devices Or Systems Thereof (AREA)
- Discharge Lamps And Accessories Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、略直管状のガラスバルブの両端付近に設け
た一対の電極に高周波電圧を印加1−ることにより、ガ
ラスバルブ内の放電ガスを放電させて発光させる無電極
の放電灯に関するものである。Detailed Description of the Invention [Industrial Application Field] This invention applies a high frequency voltage to a pair of electrodes provided near both ends of a substantially straight glass bulb, thereby reducing discharge gas within the glass bulb. The present invention relates to an electrodeless discharge lamp that emits light by discharging it.
第2図は例えば特開昭62−185857号公報に示さ
れたこの種の従来の放電灯の概略を示す構成図であり、
一部を切欠いて示している。図において、1は水≦14
等の金属蒸気及び不活性ガスが封入された直管状のガラ
スバルブ、2はその開「1部で、この開口部2を除いた
ガラスバルブ1の内面には反射1]!23が設けられ、
また蛍光体4が塗11iされている。5.6はガラスバ
ルブ1の両端付近に設けられた一対の導体、7はこの一
対の導体5.6に高周波電圧を印加する高周波発振回路
、8は交流電源である。FIG. 2 is a block diagram schematically showing a conventional discharge lamp of this kind disclosed in, for example, Japanese Patent Application Laid-Open No. 62-185857.
A portion is shown cut away. In the figure, 1 is water≦14
A straight glass bulb filled with metal vapor and inert gas such as
Further, the phosphor 4 is coated 11i. 5.6 is a pair of conductors provided near both ends of the glass bulb 1, 7 is a high frequency oscillation circuit that applies a high frequency voltage to the pair of conductors 5.6, and 8 is an AC power source.
上記のように構成された放電灯において、電源没入によ
り高周波発振回路7が作動して導体5゜6に高周波電圧
が印加されると、この導体間に高周波T1.磁界が発生
し、ガラスバルブ1に封入された金属蒸気か励起される
。そして、この金属蒸気の励起により紫外線か放出され
、この紫外線かガラスバルブ1の内面に塗布された蛍光
体4によって可視光に変化し、開口部2から外部に放射
される。In the discharge lamp configured as described above, when the high frequency oscillation circuit 7 is activated by power supply insertion and a high frequency voltage is applied to the conductor 5.6, a high frequency T1. A magnetic field is generated and the metal vapor sealed in the glass bulb 1 is excited. The excitation of this metal vapor emits ultraviolet light, which is converted into visible light by the phosphor 4 applied to the inner surface of the glass bulb 1 and radiated to the outside through the opening 2.
このような放電灯は、ガラスバルブ1の内部にフィラメ
ントを有した電極を持っていないので、長寿命であり、
管端部の黒化現象も生じない。しかし、ガラスバルブ1
の両端付近を導体5.6で覆っているため、その分だけ
発光量が減少し、ガラスバルブ1の軸方向の実質的な有
効長(発光長)か短かくなる。また、導体5,6の面積
が広い程、大きな発光量を得るのに有利である。Such a discharge lamp does not have an electrode with a filament inside the glass bulb 1, so it has a long life.
There is no blackening phenomenon at the end of the tube. However, glass bulb 1
Since both ends of the glass bulb 1 are covered with conductors 5.6, the amount of light emitted is reduced accordingly, and the effective length (emission length) of the glass bulb 1 in the axial direction is shortened. Further, the larger the area of the conductors 5 and 6, the more advantageous it is to obtain a large amount of light emission.
(発明が解決しようとする課題)
従来の放電灯は上記のように構成されており、ガラスバ
ルブ!がほぼ同一な管径を持った直管状に形成されてい
るため、発光量を十分前ようとして金属導体5,6の面
積を広げるためには導体5.6の幅を広くしなければな
らず、従ってガラスバルブ1の発光に寄与する軸方向の
有効長が短かくなるという問題点があった。(Problem to be Solved by the Invention) Conventional discharge lamps are constructed as described above, and include glass bulbs! are formed in the shape of a straight tube with approximately the same diameter, so in order to increase the area of the metal conductors 5 and 6 in order to increase the amount of light emitted sufficiently, the width of the conductor 5 and 6 must be made wider. Therefore, there is a problem in that the effective length in the axial direction of the glass bulb 1 that contributes to light emission is shortened.
この発明は、このような問題点を解消するためになされ
たもので、導体の幅を広くすることなく面積を大きくと
ることができ、ガラスバルブの有効長の長い放電灯を得
ることを目的としている。This invention was made to solve these problems, and its purpose is to obtain a discharge lamp that can have a large area without increasing the width of the conductor and has a long effective length of the glass bulb. There is.
(課題を解決するための手段〕
この発明の放電灯は、放電ガスを封入した略直管状のガ
ラスバルブの両端付近に凹凸部を形成し、この凹凸部を
含む外表面に高周波電圧を印加するための導体を配設し
たものである。(Means for Solving the Problems) In the discharge lamp of the present invention, uneven portions are formed near both ends of a substantially straight glass bulb filled with discharge gas, and a high-frequency voltage is applied to the outer surface including the uneven portions. A conductor is provided for this purpose.
この発明の放電灯においては、ガラスバルブの両端付近
に凹凸部が形成さねており、その部分のバルブ表面J+
’tが凹凸によって拡大されている。そして、この表面
に沿って導体が配設されているので、導体の幅が小さく
ても十分な面積が得られる。In the discharge lamp of the present invention, uneven portions are formed near both ends of the glass bulb, and the bulb surface J +
't is enlarged by the unevenness. Since the conductor is arranged along this surface, a sufficient area can be obtained even if the width of the conductor is small.
(実施例)
第1図はこの発明の一実施例を示す構成図である。図に
おいて、5.6は放電ガスが封入された略直管状のガラ
スバルブ9の両端付近の表面に配設された導体で、この
ガラスバルブ9の導体5゜6の配設部分には複数の凹み
によって形成された凹凸部to、11かあり、導体5.
6はその凹凸部10.11を含む表面に沿って設けられ
ている。(Embodiment) FIG. 1 is a block diagram showing an embodiment of the present invention. In the figure, reference numeral 5.6 denotes a conductor disposed on the surface near both ends of a substantially straight glass bulb 9 filled with discharge gas. There are uneven portions to, 11 formed by recesses, and the conductor 5.
6 is provided along the surface including the uneven portions 10.11.
7は上記導体5.6に高周波電圧を印加する高周波発掘
回路、8は交流電源、12は発光部分である。7 is a high frequency excavation circuit that applies a high frequency voltage to the conductor 5.6, 8 is an AC power source, and 12 is a light emitting portion.
なお、上記ガラスバルブ9の内部には、放電ガスとして
水銀等の金属蒸気が封入され、またアルゴン等の不活性
ガスも封入されている。そして、図示していないがガラ
スバルブ9の内面には、第2図と同様間[1部を残して
反射膜が設けられ、また蛍光体が塗布されている。Note that the inside of the glass bulb 9 is filled with metal vapor such as mercury as a discharge gas, and also with an inert gas such as argon. Although not shown, a reflective film is provided on the inner surface of the glass bulb 9 except for one part, as in FIG. 2, and a fluorescent material is coated.
このように構成された放電灯は、従来と同様、電源投入
により高周波発掘回路7が作動し、導体5.6に高周波
電圧が印加されると、ガラスバルブ9内の金属蒸気が電
離し、導体間で放電が発生する。そして、ガラスバルブ
9に封入された金属蒸気が励起され、この金属蒸気より
紫外線が放出される。そして、この紫外線がガラスバル
ブ9の内壁面に塗布された蛍光体により可視光に変化し
、直接あるいは反射膜を介してガラスバルブ9の開[1
部から略同一方向に放射される。In the discharge lamp configured in this way, when the power is turned on, the high-frequency excavation circuit 7 is activated, and when a high-frequency voltage is applied to the conductor 5.6, the metal vapor in the glass bulb 9 is ionized, and the conductor A discharge occurs between the two. Then, the metal vapor sealed in the glass bulb 9 is excited, and ultraviolet rays are emitted from this metal vapor. Then, this ultraviolet light is converted into visible light by the phosphor coated on the inner wall surface of the glass bulb 9, and the glass bulb 9 is opened [1] either directly or through a reflective film.
are emitted from the same direction in approximately the same direction.
ここで、放電灯の発光量は前述したように導体5.6の
面積に関わってくるが、本実施例てはガラスバルブ9の
導体5.6の配設部分に凹凸部10.11があるため従
来のように全長にわたってほぼ同一管径のガラスバルブ
1の導体5,6を設ける場合に比べ、狭い幅の導体5.
6で十分な面)11か得られる。従7て、導体5,6の
幅を広くすることなく面積を十分大きくとることができ
、ガラスバルブ9の有効長を大きくとることができる。Here, the amount of light emitted by the discharge lamp is related to the area of the conductor 5.6 as described above, but in this embodiment, there is an uneven portion 10.11 in the area where the conductor 5.6 of the glass bulb 9 is disposed. Therefore, compared to the conventional case where the conductors 5 and 6 of the glass bulb 1 are provided with substantially the same tube diameter over the entire length, the conductors 5 and 6 have a narrower width.
6 is enough) 11 is obtained. Therefore, the area can be made sufficiently large without increasing the width of the conductors 5 and 6, and the effective length of the glass bulb 9 can be made large.
なお、上記実施例では導体5,6が配設されるガラスバ
ルブ9の両端付近に凹みによる凹凸部to、ttを形成
したが、突出部を設けることにより凹凸部を形成するよ
うにしても良く、同様の効果が得られる。In addition, in the above embodiment, the uneven parts to and tt are formed by recesses near both ends of the glass bulb 9 where the conductors 5 and 6 are disposed, but the uneven parts may be formed by providing protruding parts. , a similar effect can be obtained.
以上のように、この発明によれば、ガラスバルブの両端
付近に凹凸部を形成し、その表面に沿って導体を配設し
たため、導体の幅を広くすることなく導体の面積を大き
くとることができ、従ってガラスバルブの有効長を大き
くとることができるという効果がある。As described above, according to the present invention, the uneven portions are formed near both ends of the glass bulb, and the conductor is arranged along the surface. Therefore, the area of the conductor can be increased without increasing the width of the conductor. Therefore, the effective length of the glass bulb can be increased.
第1図はこの発明の一実施例を示す構成図、第2図は従
来の放電灯の概略を示す構成図である。
5.6・・・・・・導体
7・・・・・・高周波発振回路
8・・・・・・交流電源
9・・・・・・ガラスバルブ
10.11−・・・・凹凸部
なお、図中同一符号は同一または相当部分を示す。FIG. 1 is a block diagram showing an embodiment of the present invention, and FIG. 2 is a block diagram schematically showing a conventional discharge lamp. 5.6...Conductor 7...High frequency oscillation circuit 8...AC power supply 9...Glass bulb 10.11-...Irregularities The same reference numerals in the figures indicate the same or corresponding parts.
Claims (1)
の外面に導体を配設し、この導体に高周波電圧を印加す
ることにより前記放電ガスを放電させて発光させる放電
灯において、前記ガラスバルブの両端付近に凹凸部を形
成し、この凹凸部を含む外表面に前記導体を配設したこ
とを特徴とする放電灯。In a discharge lamp, a conductor is arranged on the outer surface near both ends of a substantially straight glass bulb filled with a discharge gas, and a high frequency voltage is applied to the conductor to discharge the discharge gas and emit light. A discharge lamp characterized in that uneven portions are formed near both ends, and the conductor is disposed on the outer surface including the uneven portions.
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13892388A JPH01309249A (en) | 1988-06-06 | 1988-06-06 | Discharge lamp |
US07/311,350 US5013966A (en) | 1988-02-17 | 1989-02-15 | Discharge lamp with external electrodes |
EP89102691A EP0329143B1 (en) | 1988-02-17 | 1989-02-16 | Discharge lamp |
CA000591290A CA1305510C (en) | 1988-02-17 | 1989-02-16 | Discharge lamp |
DE68915022T DE68915022T2 (en) | 1988-02-17 | 1989-02-16 | Discharge lamp. |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13892388A JPH01309249A (en) | 1988-06-06 | 1988-06-06 | Discharge lamp |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01309249A true JPH01309249A (en) | 1989-12-13 |
Family
ID=15233294
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13892388A Pending JPH01309249A (en) | 1988-02-17 | 1988-06-06 | Discharge lamp |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01309249A (en) |
-
1988
- 1988-06-06 JP JP13892388A patent/JPH01309249A/en active Pending
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