JPH07245082A - Metal vapor discharge lamp - Google Patents
Metal vapor discharge lampInfo
- Publication number
- JPH07245082A JPH07245082A JP5836694A JP5836694A JPH07245082A JP H07245082 A JPH07245082 A JP H07245082A JP 5836694 A JP5836694 A JP 5836694A JP 5836694 A JP5836694 A JP 5836694A JP H07245082 A JPH07245082 A JP H07245082A
- Authority
- JP
- Japan
- Prior art keywords
- tin
- cobalt
- halogen
- amount
- discharge lamp
- 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
Landscapes
- Discharge Lamp (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は光化学反応や塗料乾燥用
の光源として用いられる紫外用の金属蒸気放電灯に関す
る。FIELD OF THE INVENTION The present invention relates to an ultraviolet metal vapor discharge lamp used as a light source for photochemical reactions and paint drying.
【0002】[0002]
【従来の技術】電極を備えた発光管の内部にアーク放電
を維持するに充分な量の水銀及び適量の希ガスと共にハ
ロゲン、鉄及び錫を封入した金属蒸気放電灯は紫外領
域、特に280〜420nm領域の発光効率が優れている
ことから、例えば、光化学反応や塗料乾燥用光源として
紫外用の高圧水銀ランプに代わり多用されている。2. Description of the Related Art A metal vapor discharge lamp filled with halogen, iron and tin together with a sufficient amount of mercury and an appropriate amount of rare gas to maintain an arc discharge inside an arc tube equipped with an electrode is used in the ultraviolet region, particularly 280 to 280. Because of its excellent luminous efficiency in the 420 nm region, it is often used as a light source for photochemical reactions and paint drying, instead of a high-pressure mercury lamp for ultraviolet light.
【0003】[0003]
【発明が解決しようとする課題】従来の鉄及び錫入り金
属蒸気放電灯は、図3に示すように360〜390nm領
域に多数の輝線スペクトルが集中しているため特定の範
囲を有効波長域とする光化学反応や塗料乾燥用光源とし
て効果的でない場合がある。特に、300〜360nmの
領域を有効波長域として、鉄及び錫入り金属蒸気放電灯
を用いると図3に示すように、360〜420nm領域の
輝線を含んだ比較的高い連続スペクトルは反応に寄与せ
ず光エネルギーの大部分が無駄になってしまう欠点があ
った。そこで、本発明は上記従来の欠点を解消するもの
で、特定の波長300〜360nmの波長領域に光エネル
ギーを集中した金属蒸気放電灯を提供することを目的と
するものである。In the conventional metal vapor discharge lamp containing iron and tin, as shown in FIG. 3, a large number of emission line spectra are concentrated in the 360 to 390 nm region, so that a specific range is defined as an effective wavelength region. It may not be effective as a photochemical reaction or a light source for drying paint. In particular, when a metal vapor discharge lamp containing iron and tin is used with an effective wavelength range of 300 to 360 nm, as shown in FIG. 3, a relatively high continuous spectrum including bright lines in the 360 to 420 nm range does not contribute to the reaction. However, there is a drawback that most of the light energy is wasted. Therefore, the present invention solves the above-mentioned conventional drawbacks, and an object of the present invention is to provide a metal vapor discharge lamp in which light energy is concentrated in a specific wavelength region of 300 to 360 nm.
【0004】[0004]
【課題を解決するための手段】本発明は、電極を備えた
発光管の内部にアーク放電を維持するに充分な量の水銀
及び適量の希ガスと共にハロゲン、コバルト及び錫を封
入し、ハロゲンの封入量を発光管内容積1cm3あたり
1.0×10-5〜1.0×10-8グラム原子とし、コバ
ルト及び錫の総量をハロゲン原子に対して原子比で1/
2〜3とし、かつコバルトに対する錫の量を原子比で1
/20〜1とすることにより、波長300〜360nmの
紫外線領域に光エネルギーを集中させたことを特徴とす
る。SUMMARY OF THE INVENTION The present invention encloses halogen, cobalt and tin with a sufficient amount of mercury and an appropriate amount of noble gas to maintain an arc discharge inside an arc tube equipped with electrodes. The filling amount was 1.0 × 10 −5 to 1.0 × 10 −8 gram atom per 1 cm 3 of the inner volume of the arc tube, and the total amount of cobalt and tin was 1 / atomic ratio with respect to the halogen atom.
2-3, and the atomic ratio of tin to cobalt is 1
By setting / 20 to 1, the light energy is concentrated in the ultraviolet region of wavelength 300 to 360 nm.
【0005】[0005]
【作用】発明者は、300〜360nmの紫外領域に光エ
ネルギーを集中させるにはコバルト及び錫が有効である
ことを見出し、調査研究した結果、コバルト、錫および
ハロゲンの封入量を所定の範囲に規定することにより、
300〜360nmの紫外領域にわたり輝線を含んだ比較
的高い連続スペクトルを放射し、かつこれ以外の波長範
囲のエネルギー比は小さくなることを確認した。The inventor has found that cobalt and tin are effective for concentrating light energy in the ultraviolet region of 300 to 360 nm, and as a result of research and study, the amount of cobalt, tin and halogen enclosed was set within a predetermined range. By stipulating,
It was confirmed that a relatively high continuous spectrum including emission lines was emitted over the ultraviolet region of 300 to 360 nm, and that the energy ratio in the other wavelength range was smaller.
【0006】以下、本発明を図面に基づき説明する。図
1において、1は石英ガラスのような耐熱透光性材料か
らなる発光管、2は発光管両端に封着した電極、3は金
属箔、4は外部リード線、5は電極近傍の発光管の管壁
温度を最適値に保持するためのAl2O3等よりなる保温
膜である。又、発光管1の内部にはアーク放電を維持す
るに充分な量の水銀と適量の希ガス及びハロゲン、並び
にコバルトと錫が封入してある。The present invention will be described below with reference to the drawings. In FIG. 1, 1 is an arc tube made of a heat-resistant translucent material such as quartz glass, 2 is electrodes sealed at both ends of the arc tube, 3 is a metal foil, 4 is an external lead wire, 5 is an arc tube near the electrode Is a heat insulating film made of Al 2 O 3 or the like for keeping the tube wall temperature of the above at an optimum value. Further, the arc tube 1 is filled with a sufficient amount of mercury, an appropriate amount of rare gas and halogen, and cobalt and tin to maintain arc discharge.
【0007】ここで、発光管に封入すべきハロゲンは発
光管の内容積1cm3あたり1.0×10-5〜1.0×1
0-8グラム原子に規定する。この範囲より少ないとコバ
ルト及び錫の分光エネルギーは極端に減少し単なる水銀
放電のスペクトルに近くなり、上記範囲より大きいと放
電灯の始動電圧、再点弧電圧及びランプ電圧が上昇して
電気特性が悪くなる。また、発光管に封入すべきコバル
ト及び錫の総量はハロゲンに対して原子比で1/2〜3
の範囲が望ましい。この範囲より少ないと充分な紫外線
出力が得られない。反対に上記範囲より大きいとコバル
ト及び錫が発光管内に付着して減光の原因となる。更
に、発光管に封入すべき錫はコバルトに対して原子比で
1/20〜1でなければならない。錫が上記範囲より少
ないと発光管内に封入したコバルトが蒸発し、管内壁に
被着して黒化現象が起こり、減光の原因となる。前記範
囲より多いとコバルトの発光効率が低下し、スペクトル
分布が極めて弱いものとなる。Here, the halogen to be sealed in the arc tube is 1.0 × 10 −5 to 1.0 × 1 per 1 cm 3 of the internal volume of the arc tube.
Specify 0 to 8 grams atom. If it is less than this range, the spectral energies of cobalt and tin are extremely reduced and become close to the spectrum of mere mercury discharge. If it is more than the above range, the starting voltage, re-ignition voltage and lamp voltage of the discharge lamp are increased and the electrical characteristics are become worse. Further, the total amount of cobalt and tin to be sealed in the arc tube is 1/2 to 3 in atomic ratio with respect to halogen.
The range of is desirable. If it is less than this range, sufficient UV output cannot be obtained. On the other hand, if it is larger than the above range, cobalt and tin adhere to the inside of the arc tube and cause dimming. Furthermore, the tin to be sealed in the arc tube must have an atomic ratio of 1/20 to 1 with respect to cobalt. When the amount of tin is less than the above range, cobalt enclosed in the arc tube evaporates and adheres to the inner wall of the tube to cause a blackening phenomenon, which causes dimming. If it exceeds the above range, the luminous efficiency of cobalt is lowered and the spectral distribution becomes extremely weak.
【0008】表1は、コバルトと錫の原子比を上記範囲
に限定すべき根拠を示す実験結果である。実験に供した
ランプは内径20mm、内容積42.4ccの発光管にアー
クを形成するに必要な水銀と適量のアルゴンガスと、コ
バルト及び錫の総量に等しい化学当量の沃素と、表1に
示すようにコバルト及び錫の封入量を選定したものであ
る。表1から明らかなように、コバルトに対する錫の原
子比が1/20〜1の範囲で300〜360nmの波長領
域に放射エネルギーの大部分が集中しこのランプを点灯
したところ図2に示す様な分光分布特性が得られた。Table 1 shows the experimental results showing the reason why the atomic ratio of cobalt and tin should be limited to the above range. The lamps used in the experiment are shown in Table 1 with mercury and an appropriate amount of argon gas required to form an arc in an arc tube having an inner diameter of 20 mm and an internal volume of 42.4 cc, and a chemical equivalent iodine equivalent to the total amount of cobalt and tin. Thus, the amount of cobalt and tin enclosed is selected. As is clear from Table 1, when the atomic ratio of tin to cobalt is in the range of 1/20 to 1, most of the radiant energy is concentrated in the wavelength region of 300 to 360 nm and the lamp is lit, as shown in FIG. The spectral distribution characteristics were obtained.
【0009】[0009]
【発明の効果】本発明によれば、発光管内に水銀及び希
ガスと共に所定量のハロゲン、コバルト及び錫を封入す
ることにより、300〜360mmの紫外領域に光エネル
ギーを集中させることが可能となり、300〜360mm
波長領域を有効波長域とする光化学反応や塗料乾燥用の
光源として最適な高圧金属放電灯を得ることができる。According to the present invention, by enclosing a predetermined amount of halogen, cobalt and tin together with mercury and a rare gas in the arc tube, it becomes possible to concentrate the light energy in the ultraviolet region of 300 to 360 mm, 300-360 mm
It is possible to obtain a high pressure metal discharge lamp that is optimal as a light source for photochemical reaction or coating drying in which the wavelength range is the effective wavelength range.
【図1】本発明に係わる金属蒸気放電灯の一部縦断側面
図。FIG. 1 is a partially longitudinal side view of a metal vapor discharge lamp according to the present invention.
【図2】前記同放電灯の分光エネルギー分布図。FIG. 2 is a spectral energy distribution diagram of the discharge lamp.
【図3】従来の金属蒸気放電灯のエネルギー分布図。FIG. 3 is an energy distribution diagram of a conventional metal vapor discharge lamp.
1 発光管 2 電極 3 金属箔 4 外部リード線 5 保温膜 1 arc tube 2 electrode 3 metal foil 4 external lead wire 5 heat insulating film
【表1】 [Table 1]
Claims (1)
電を維持するに充分な量の水銀及び適量の希ガスと共に
ハロゲン、コバルト及び錫を封入し、ハロゲンの封入量
を発光管内容積1cm3あたり1.0×10-5〜1.0×
10-8グラム原子とし、コバルト及び錫の総量をハロゲ
ン原子に対して原子比で1/2〜3とし、かつコバルト
に対する錫の量を原子比で1/20〜1とすることによ
り、波長300〜360nmの紫外線領域に光エネルギー
を集中させたことを特徴とする金属蒸気放電灯。1. An arc tube equipped with an electrode is filled with halogen, cobalt and tin together with a sufficient amount of mercury and an appropriate amount of rare gas to maintain an arc discharge, and the enclosed amount of halogen is 1 cm of the internal volume of the arc tube. 1.0 x 10 -5 to 1.0 x per 3
A wavelength of 300 is obtained by setting the amount of cobalt and tin to 10 −8 gram atom, the total amount of cobalt and tin in the atomic ratio of 1/2 to 3 with respect to the halogen atom, and the amount of tin to cobalt in the atomic ratio of 1/20 to 1. A metal vapor discharge lamp characterized by concentrating light energy in the ultraviolet region of up to 360 nm.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5836694A JPH07245082A (en) | 1994-03-04 | 1994-03-04 | Metal vapor discharge lamp |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5836694A JPH07245082A (en) | 1994-03-04 | 1994-03-04 | Metal vapor discharge lamp |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH07245082A true JPH07245082A (en) | 1995-09-19 |
Family
ID=13082330
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5836694A Pending JPH07245082A (en) | 1994-03-04 | 1994-03-04 | Metal vapor discharge lamp |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH07245082A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008282748A (en) * | 2007-05-14 | 2008-11-20 | Harison Toshiba Lighting Corp | Metal halide lamp |
JP2009064725A (en) * | 2007-09-07 | 2009-03-26 | Harison Toshiba Lighting Corp | Metal halide lamp |
-
1994
- 1994-03-04 JP JP5836694A patent/JPH07245082A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008282748A (en) * | 2007-05-14 | 2008-11-20 | Harison Toshiba Lighting Corp | Metal halide lamp |
JP2009064725A (en) * | 2007-09-07 | 2009-03-26 | Harison Toshiba Lighting Corp | Metal halide lamp |
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