JPS5937643A - Metal halide lamp - Google Patents

Metal halide lamp

Info

Publication number
JPS5937643A
JPS5937643A JP57146855A JP14685582A JPS5937643A JP S5937643 A JPS5937643 A JP S5937643A JP 57146855 A JP57146855 A JP 57146855A JP 14685582 A JP14685582 A JP 14685582A JP S5937643 A JPS5937643 A JP S5937643A
Authority
JP
Japan
Prior art keywords
less
tube
metal halide
lamp
arc tube
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
JP57146855A
Other languages
Japanese (ja)
Inventor
Toshihiko Ishigami
敏彦 石神
Ariyoshi Ishizaki
有義 石崎
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura Electric Co Ltd
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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP57146855A priority Critical patent/JPS5937643A/en
Publication of JPS5937643A publication Critical patent/JPS5937643A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/82Lamps with high-pressure unconstricted discharge having a cold pressure > 400 Torr
    • H01J61/827Metal halide arc lamps

Landscapes

  • Discharge Lamps And Accessories Thereof (AREA)

Abstract

PURPOSE:To provide a small lamp having practical light efficiency and minimized going out by forming a luminous tube having an inner volume of 1cc or less with an infrared absorption quartz, and making lamp power 70W or less, tube wall load A 12-26W/cm<2>, and limiting the L of projecting length Lmm. of an electrode to a specified length to the A. CONSTITUTION:An infrared absorption quartz luminous tube is formed by sealing electrodes at its both sides, and enclosing a rare gas for starting, mercury, and at least scandium halide as metal halides. In this tube, the inner volume is made 1cc or less, the lamp power to 70W or less, the tube wall load A to 12- 26W/cm<2>, and the projecting length Lmm. of the electrodes is limited as follows; 1/14A-5/14<=L<=1/28A+11/7.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明はメタルハライドランプ特には小形のメタルハラ
イドランプに関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to metal halide lamps, and particularly to small metal halide lamps.

〔発明の技術的背景と背景技術の問題点〕従来から両端
部に対向する電極を封着した石英発光管内に、始動用希
ガス、水銀と共に金属ハロゲン化物を封入した高効率の
メタルハライドランプは広く普及している。
[Technical background of the invention and problems with the background art] High-efficiency metal halide lamps, in which a metal halide is sealed together with a rare starting gas and mercury in a quartz arc tube with opposing electrodes sealed at both ends, have been widely used. It is widespread.

さらに、近年に至り上記メタルノ・ライドランプを商店
、事務所などの屋内照明用光源として使用する目的でラ
ンプ電力が小さい小形ランプの開発が活発に行なわれて
いる。ところで、メタルハライドランプの特性たとえば
光効率、演色性がどは発光管の最冷部温度に依存し、ま
た潰冷部温度は管壁負荷、電極の発光管内への突出長な
どに依存することは良く知られている。しかしながら9
発光管の最冷部温度をあげるため管壁負荷をあげたり、
1!極突出長を短かくすると寿命特性に悪い影響を及は
し、特に発光管容積の小さな小形メタルハライドランプ
においてはその影響が極めて大きなものがある。すなわ
ち9発光管容積の大小に関わらず電極輝点温度は変わら
ないにも拘わらず。
Furthermore, in recent years, compact lamps with low lamp power have been actively developed for the purpose of using the above-mentioned metalnolide lamps as light sources for indoor lighting in shops, offices, and the like. By the way, the characteristics of metal halide lamps, such as light efficiency and color rendering, depend on the temperature of the coldest part of the arc tube, and the temperature of the cooling part does not depend on the tube wall load, the protrusion length of the electrode into the arc tube, etc. well known. However, 9
In order to raise the temperature of the coldest part of the arc tube, the load on the tube wall is increased,
1! Shortening the pole protrusion length has a negative effect on the life characteristics, and this effect is particularly significant in small metal halide lamps with small arc tube volumes. In other words, the temperature of the electrode bright spot remains the same regardless of the volume of the arc tube.

小形ランプにおいては電極と発光管管壁との距離が短か
くなり、その分管壁温度の上昇が著るしくなるためであ
る。管壁温度が著るしく上昇すれば封入金属ハロゲン化
物と石英管との反応が急速に促進されて管内に遊離ハロ
ゲンたとえば遊離沃素が放出され、この結果としてラン
プ電圧波形にヒゲ状の再点弧電圧が生じ、この値が電源
電圧を越えるとランプが立ち消えるという不都合な現象
を生じる。このような現象を回避するため、電極突出長
を長くしたり、あるいは発光管の管径を大きくすると屋
内照明用光源としての実用的な光効率が得られないとい
う問題があった。
This is because in a small lamp, the distance between the electrode and the wall of the arc tube becomes shorter, and the temperature of the wall of the arc tube increases significantly. If the tube wall temperature rises significantly, the reaction between the encapsulated metal halide and the quartz tube will be rapidly accelerated and free halogens, such as free iodine, will be released into the tube, resulting in a whisker-like restriking in the lamp voltage waveform. A voltage is generated, and if this value exceeds the power supply voltage, the lamp goes out, an undesirable phenomenon. In order to avoid such a phenomenon, if the protruding length of the electrode is increased or the diameter of the arc tube is increased, there is a problem that practical light efficiency as a light source for indoor lighting cannot be obtained.

〔発明の目的〕[Purpose of the invention]

本発明は屋内照明用光源として実用的な光効率が得られ
、かつ立ち消えの生じない小形のメタルハライドランプ
を提供することを目的とする。
SUMMARY OF THE INVENTION An object of the present invention is to provide a small metal halide lamp that has practical light efficiency as a light source for indoor lighting and does not turn off.

〔発明の概要〕[Summary of the invention]

本発明は両端部に電極を封着し、内部に始動用希ガス、
水銀および金属ハロゲン化物として少なくともスカンジ
ウムのハロゲン化物を封入した内容積1 c、c以下の
発光管を赤外線吸収石英で形成し、ランプ電カフ0W以
下、管壁負荷Aを12〜26 W/cm2とし、電極突
出長をLmmとしたとき。
In the present invention, electrodes are sealed at both ends, and a rare gas for starting is contained inside.
An arc tube with an internal volume of 1 c or less, filled with mercury and at least a scandium halide as a metal halide, is formed of infrared absorbing quartz, the lamp electric cuff is 0 W or less, and the tube wall load A is 12 to 26 W/cm2. , when the electrode protrusion length is Lmm.

TTA 14≦1≦28” 7 となるようにしたことを特徴とするメタルハライドラン
プである。
This metal halide lamp is characterized in that TTA 14≦1≦28”7.

〔発明の実施例〕[Embodiments of the invention]

以下に本発明の詳細につき実験例を元に説明する。まず
、ランプ電カフ0W以下で発光管内容積1 c、c以下
の小型ランプにおいては1発光管の管壁負荷Aつまりラ
ンプ電力(ワット)/管内表面積(cm” )は12〜
26W/cm2にする必要がある。この上限値を越すと
管壁温度が1000℃以上の高温となって石英が劣化し
たり、さらに封入金属ハロゲン化物特にスカンジウムS
c等の希土類金属のハロゲン化物を用いた場合には高温
で石英と反応して寿命特性が著しく低下する。一方、下
限値を下廻ると発光管からの放射光は水銀発光のみとな
って封入ハロゲン化物の金属発光は見られず光効率、演
色性共に著るしく低下してしまう。
The details of the present invention will be explained below based on experimental examples. First, in a small lamp with a lamp cuff of 0 W or less and an arc tube internal volume of 1 c or less, the tube wall load A of one arc tube, that is, the lamp power (watts)/inner tube surface area (cm") is 12~
It is necessary to set it to 26W/cm2. If this upper limit is exceeded, the temperature of the tube wall will reach a high temperature of 1000°C or higher, which will cause the quartz to deteriorate, and furthermore, the encapsulated metal halide, especially scandium S
When a rare earth metal halide such as C is used, it reacts with quartz at high temperatures, resulting in a significant decrease in life characteristics. On the other hand, below the lower limit, the light emitted from the arc tube is only mercury emission, and no metal emission from the encapsulated halide is observed, resulting in a significant decrease in both light efficiency and color rendering.

第1図は本実験に使用したランプ電力40Wのメタルハ
ライドランプ用発光管の正面図を示し。
Figure 1 shows a front view of the arc tube for a metal halide lamp with a lamp power of 40 W used in this experiment.

発光管は通常図示しない外管内に収容される。発光管(
1)の両端部には互に対向して電極(2+、 (2+が
封着され、電極(21、(2)の基端部は封止部(31
、(37に気密に封Hされたモリブデン等の金属箔(4
1、(41を介して外部導紳(5)、(5)に接続され
ている。発光管(1)の内部には始m・用希ガスとして
Ar 100 )−ル。
The arc tube is normally housed within an outer tube (not shown). Arc tube (
The electrodes (2+, (2+) are sealed to both ends of the electrode (21) facing each other, and the base end of the electrode (21, (2) is sealed to the sealing part (31).
, (metal foil such as molybdenum (4) hermetically sealed in (37)
1, (41) are connected to the external conductors (5), (5).The interior of the arc tube (1) contains Ar100) as a starting rare gas.

金匡ハロゲン化物として少なくともスカンジウムScの
ハロゲン什物を含むもの、たとえば沃化スカンジウム8
cI3 o、 5 rrllgと沃化ナトリウムNaI
 2.51T1gが、またラン:j電圧が約70Vとな
る量の水銀がそれぞれ封入されている。
The halogen containing at least scandium Sc, for example, scandium 8 iodide.
cI3o, 5rrllg and sodium iodide NaI
2.51 T1 g and mercury in an amount such that the run:j voltage is about 70 V are each sealed.

また1発光管(1)はほぼ球状に形成され、その材料と
しては普通の石英と赤外線吸収石英とをそれぞれ比較す
るために使用した。赤外線吸収石英は。
Further, one arc tube (1) was formed into a substantially spherical shape, and its materials were used to compare ordinary quartz and infrared absorbing quartz. Infrared absorbing quartz.

たとえば普通石英に鉄または鉄とアルミニウムとを混合
したもので、−例として石英粉末(8i02)に微欧の
酸化鉄(FeO)を混合溶融して結晶化させる等の手段
で製造されたもので、赤外線吸収作用によって内部に熱
が蓄積されて、それ自体が高温となるものである。
For example, it is a mixture of ordinary quartz and iron or iron and aluminum.For example, it is manufactured by mixing quartz powder (8i02) with fine iron oxide (FeO) and melting it and crystallizing it. , heat is accumulated inside due to infrared absorption, and the temperature itself becomes high.

このような40W球状発光管の内表面積はπR2である
から、V槽負荷Aつまりランプ電力W(ワット)/管内
表面積(cm2)は40W/πR2で、この値を上記の
通り12〜26 W / cm2の範囲内にするためR
(球状発光管の直径)を約7〜10mmの範囲に設定し
た。
Since the inner surface area of such a 40W spherical arc tube is πR2, the V tank load A, that is, the lamp power W (watts)/tube inner surface area (cm2) is 40W/πR2, and this value is converted to 12 to 26 W/as described above. R to be within the range of cm2
(diameter of the spherical arc tube) was set in a range of approximately 7 to 10 mm.

次に上記した各種要件を組合せたランプについて、さら
に電極(2)の発光管内への突出長りを0.2〜3.5
 mmの範囲内において種々変化させたランプを作シ、
それぞれの光効率および立ち消えについて実験した結果
を第2図に示す。図において縦軸は電極突出長Lmme
横軸は管壁負荷Aをとり、線1     11 28” 7 をそれぞれ示すものである。
Next, for a lamp that combines the above-mentioned various requirements, the protrusion length of the electrode (2) into the arc tube should be set to 0.2 to 3.5.
Producing lamps with various changes within the range of mm,
FIG. 2 shows the results of experiments regarding the light efficiency and extinction of each type. In the figure, the vertical axis is the electrode protrusion length Lmm
The horizontal axis represents the pipe wall load A, and lines 1, 11, 28''7 are shown, respectively.

制2Xよシ下方の領域りつまり電極突出長りの小さな領
域では発光管材料として普通石英を使用したものは光効
率60 、、gm/W以上、赤外線吸収石英を使用した
ものは755m/W以上とそれぞれ光効率は目標とする
屋内照明光源として実用的な60#1/Wを達成できる
が、ランプ始動時に立ち消えを生じるので好ましくない
。一方、線Yより上方の領域Eつまシミ極突出長りの大
きな領域では普通石英を使用したものは勿論のこと赤外
線吸収石英を使用したものでさえ光効率は60 徊/W
未満となり、目標値を達成できないことが判った。これ
に対し、線XとmYとの間の領域Fでは普通石英の場合
は6 Q−Qm/W未満であったが、赤外線吸収石英を
使用したものは608n/W以上の光効率が得られ、か
つ立ち消えを生じるものもなかった。
In the area below the control 2X, that is, the area where the electrode protrusion length is small, the luminous efficiency is 60 gm/W or more for those using ordinary quartz as the arc tube material, and 755 m/W or more for those using infrared absorbing quartz. Although it is possible to achieve the desired light efficiency of 60#1/W, which is practical as a target indoor lighting light source, the lamp goes out when it is started, which is not preferable. On the other hand, in the region E above the line Y where the protruding length of the stain pole is large, the light efficiency is 60 W/W, not to mention those using ordinary quartz, and even those using infrared absorbing quartz.
It was found that the target value could not be achieved. On the other hand, in the region F between lines , and there were no disappearances.

したがって9本発明の目的を達成できる領域Fは管壁負
荷Aが12〜26 W/c、m2の範囲で、かつ電極突
出長Lmmと管壁負荷の関係が。
Therefore, the region F in which the object of the present invention can be achieved is a range in which the tube wall load A is 12 to 26 W/c, m2, and the relationship between the electrode protrusion length Lmm and the tube wall load.

IA−一塁一<、t、 <−!−A +−LL14  
  14 −−  −−28     7を満足する範
囲内にあることが判る。
IA-1st base 1<, t, <-! -A +-LL14
14 -- -- 28 It can be seen that it is within the range that satisfies 7.

なお、上記例は40Wの場合について述べたものである
が、70W以下においては同様の効果が得られるもので
ある。
Note that although the above example describes the case of 40W, the same effect can be obtained at 70W or less.

〔発明の効果〕〔Effect of the invention〕

以上詳述したように9本発明によれば屋内照明用光源と
して実用的な光効率を有し、かつ立ち消えの生じない小
形のメタルハライドランプが得られる。
As detailed above, according to the present invention, it is possible to obtain a small metal halide lamp which has a practical light efficiency as a light source for indoor lighting and which does not turn off or go out.

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

第1図は小形のメタルノ・ライドランプ用発光管の正面
図、第2図は本発明による小形のメクルノ・ライドラン
プにおける管壁負荷と電極突出長との関係を示すグラフ
である。 (1)・・・発光管、(2)・・・電極、(3)・・・
発光管封止部。 (4)・・・金属箔、(5)・・・外部導線。 代理人 弁理士  則 近 憲 佑 (ほか1名)
FIG. 1 is a front view of an arc tube for a small-sized metalno-ride lamp, and FIG. 2 is a graph showing the relationship between tube wall load and electrode protrusion length in a small-sized metalno-ride lamp according to the present invention. (1)... Arc tube, (2)... Electrode, (3)...
Arc tube sealing part. (4)...Metal foil, (5)...External conductor. Agent: Patent attorney Kensuke Chika (and 1 other person)

Claims (1)

【特許請求の範囲】 両端部に電極を封着し、内部に始動用希ガス。 水銀および金属ハロゲン化物として少なくともスカンジ
ウムのハロゲン化物を封入した赤外線吸収石英製発光管
の内容積、をl c、c以下、ランプ電カフ0W以下、
管壁負荷Aを12〜26W/cm2とし。 上記電極突出長をLmmとしたとき。 1  5     J   11 − A−一≦L≦了7<A+丁 14  14 となるようにしたこと4特徴とするメタルハライドラン
プ。
[Claims] Electrodes are sealed at both ends, and a rare gas for starting is contained inside. The internal volume of an infrared absorbing quartz arc tube filled with mercury and at least scandium halide as a metal halide is l c, c or less, lamp electric cuff 0 W or less,
The tube wall load A is 12 to 26 W/cm2. When the above electrode protrusion length is Lmm. 1 5 J 11 - A-1 ≦ L ≦ 7 < A + 14 14 A metal halide lamp characterized by 4.
JP57146855A 1982-08-26 1982-08-26 Metal halide lamp Pending JPS5937643A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57146855A JPS5937643A (en) 1982-08-26 1982-08-26 Metal halide lamp

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57146855A JPS5937643A (en) 1982-08-26 1982-08-26 Metal halide lamp

Publications (1)

Publication Number Publication Date
JPS5937643A true JPS5937643A (en) 1984-03-01

Family

ID=15417074

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57146855A Pending JPS5937643A (en) 1982-08-26 1982-08-26 Metal halide lamp

Country Status (1)

Country Link
JP (1) JPS5937643A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08504040A (en) * 1992-09-23 1996-04-30 セントラル リサーチ ラボラトリーズ リミティド FLCD gray scale addressing method
CN1328754C (en) * 2005-01-28 2007-07-25 广东雪莱特光电科技股份有限公司 Mercury free or low-mercury high-strong discharge lamp

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08504040A (en) * 1992-09-23 1996-04-30 セントラル リサーチ ラボラトリーズ リミティド FLCD gray scale addressing method
CN1328754C (en) * 2005-01-28 2007-07-25 广东雪莱特光电科技股份有限公司 Mercury free or low-mercury high-strong discharge lamp

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