JPS58165239A - Metal halide lamp - Google Patents

Metal halide lamp

Info

Publication number
JPS58165239A
JPS58165239A JP4856082A JP4856082A JPS58165239A JP S58165239 A JPS58165239 A JP S58165239A JP 4856082 A JP4856082 A JP 4856082A JP 4856082 A JP4856082 A JP 4856082A JP S58165239 A JPS58165239 A JP S58165239A
Authority
JP
Japan
Prior art keywords
temperature
bulb
metal halide
pulp
quartz
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
JP4856082A
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 JP4856082A priority Critical patent/JPS58165239A/en
Publication of JPS58165239A publication Critical patent/JPS58165239A/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

Abstract

PURPOSE:To improve the luminous efficiency and lengthen the lifetime, by making a whole luminous bulb of infrared ray absorption quartz to heighten the temperature of the minimum-temperature part and suppress the rise in the temperature of the maximum-temperature part. CONSTITUTION:The inside diameter d2 of the upper part of a lamp, which is vertically lighted, is made larger than that d1 of the lower part so that the volume of the upper half is larger than that of the lower half as to the lighting. Since the bulb 1 of the lamp is made of infrared ray absorption quartz, the temperature of the minimum-temperature section behind the lower electrode 2b is heightened to promote the evaporation of solidified sealed-in metal to enhance the luminous efficiency. Although the temperature of the bulb wall except the minimum-temperature section would rise because the whole bulb 1 is made of infrared ray absorption quartz, the volume of the upper half of the bulb is made larger to increase the distance between the bulb wall and the arc and the surface area of the bulb wall to diminish the bulb wall load (W/cm<2>). For that reason, the rise in the temperature of the bulb wall is suppressed toward the top of the bulb 1 to prevent thermal deterioration to lengthen the lifetime.

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における発光効率の改善
対策に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to measures for improving luminous efficiency in metal halide lamps.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

電極を備えた透光性廃光管に、水銀と金属へallン化
物および始動用希ガスを封入してなるメタルハライドラ
ンプは、高効率、高演色性のランプであるため広く普及
している。しかし慶から近時省エネルギ一対策が社会的
要請とされている折、この種メタルハライドランプのさ
らに高効率化および長寿命化が望まれている。
Metal halide lamps, which are formed by filling a transparent waste light tube equipped with electrodes with mercury, a metal aluminide, and a starting rare gas, are widely used because they are highly efficient and highly color rendering lamps. However, as energy-saving measures have recently become a social requirement, it is desired that this type of metal halide lamp be made even more efficient and have a longer lifespan.

一般にメタルハライドランプの発光効率は、封入発光金
属が同権、同一量であれば、発光管の最冷部温度に依存
することが知られてい名。
It is generally known that the luminous efficiency of a metal halide lamp depends on the temperature of the coldest part of the arc tube, provided that the luminous metals enclosed are the same and have the same amount.

すなわち、ナトリウム、スカンジウム、ディスプロシウ
ム等のハロダン化物は、発光管の最冷部に凝縮されてお
ル、最冷部の温度上昇に伴って蒸発される。したがって
最冷部の温度を上昇させると上記金属/N 四)fン化
物の蒸発量が増し、管内濃度が増加するため発光強度が
向上し、効率が高くなるものである。
That is, halodanides such as sodium, scandium, and dysprosium are condensed in the coldest part of the arc tube and evaporated as the temperature of the coldest part increases. Therefore, when the temperature of the coldest part is raised, the amount of evaporation of the metal/N4) ionide increases, and the concentration in the tube increases, so that the luminous intensity improves and the efficiency increases.

従来において発光管の最冷部温度を上昇させラスによっ
て形成する提案がなされている。赤外線吸収石英は、5
102から表る普通石英に、鉄または鉄にアルン二、ウ
ムを混合させた亀のでtbシ、赤外線を吸収すゐことK
よシ自己の温度が上昇すゐ性質をもっている。
Conventionally, proposals have been made to increase the temperature of the coldest part of the arc tube and form it with a lath. Infrared absorbing quartz is 5
It is made of ordinary quartz expressed by 102, mixed with iron or iron, and absorbs infrared rays.
It has the property of increasing its own temperature.

しかしながら赤外線吸収石英によって発光管パルプ全体
を構成すると、最冷部の温度は確かに上昇されるが、最
冷部で門い部分の管壁温度11、: も高くなる。特に最高温度!分は、従来の普通石英を用
いた場合よシも温−上昇し、このため石英とハt2ダン
が反応して劣化するなど、短寿命になる欠点があった。
However, if the entire arc tube pulp is made of infrared absorbing quartz, the temperature of the coldest part will certainly rise, but the tube wall temperature 11 of the gate part in the coldest part will also increase. Especially the maximum temperature! However, the temperature rises even more than when conventional ordinary quartz is used, and as a result, the quartz and the quartz react with each other and deteriorate, resulting in a shortened lifespan.

〔発明の目的〕[Purpose of the invention]

本発明はこのような事情にもとづきなされた亀ので、そ
の目的とするところは、発光管パルプ全体を赤外線吸収
石英によシ構成して最冷部i!変を上昇させ、発光効率
の向上を図るとともに1この場合に最高温度部分の温度
上昇を抑止し、長寿命となるメタルハライドランプを提
供しようとするものである。
The present invention has been made based on these circumstances, and its purpose is to construct the entire arc tube pulp with infrared absorbing quartz to reduce the coldest part i! The purpose of this invention is to provide a metal halide lamp that not only increases the temperature change and improves the luminous efficiency, but also suppresses the rise in temperature of the highest temperature portion and has a longer life.

〔発明の概要〕[Summary of the invention]

本発明は発光管パルプを赤外線吸収石英によって形成す
ることによって最冷部温度を上昇させるとともKこの発
光管パルプの点灯φに上側に位置する放電空間は下側に
位置する放電空間より大容積とし、上側に形成される最
高温度部分のバルブ壁をアークから遠ざけかつパルプ壁
表面積を大きくして管壁負荷を下げるととKよシ上記最
高温度“−分の温度上昇を抑止した亀の、、11” である、   ・ 〔発明の実施例〕′ 以下本発明の一実施例を第1図にもとづき説明する。
The present invention increases the temperature of the coldest part by forming the arc tube pulp with infrared-absorbing quartz, and when the arc tube pulp is turned on, the discharge space located above has a larger volume than the discharge space located below. By keeping the bulb wall at the highest temperature part formed on the upper side away from the arc and increasing the surface area of the pulp wall to reduce the load on the tube wall, the temperature rise of the above maximum temperature "-" can be suppressed. , 11''. [Embodiment of the Invention]' An embodiment of the present invention will be described below with reference to FIG.

第1図は垂直点灯用メタルハライドランプの発光管を示
し、骸発光管は通常図示しない外管内に収容されて二重
管構造となる。1は発光管パルプであり、該ノ童ルプ1
は全体に亘って赤外線吸収石英によシ構成されている。
FIG. 1 shows the arc tube of a metal halide lamp for vertical lighting, and the shell arc tube is normally housed in an outer tube (not shown) to form a double tube structure. 1 is arc tube pulp;
is constructed entirely of infrared absorbing quartz.

赤外線吸収石英は、たとえば石英粉末(sio2)に微
量の酸化鉄(F・0)を混合したのち溶融して結晶化さ
せる等の手段で作ることができ石。パルプ1には主電極
1m、2bが対向して設けられておシ、これら主電極2
m、2bは封止部s*、sbに封緘されたモリブデン等
の金属箔4m、4bに接続され、とわら金属箔4 t 
a 4 bは外部導線5a*gbに接続されている。i
4ルブ1内には所定量の水銀と金属ハロダン化物および
始動用希ガスが封入されている。
Infrared absorbing quartz is a stone that can be made, for example, by mixing quartz powder (SIO2) with a small amount of iron oxide (F.0) and then melting and crystallizing it. The pulp 1 is provided with main electrodes 1m and 2b facing each other, and these main electrodes 2
m, 2b are connected to metal foils 4m, 4b such as molybdenum sealed in the sealing parts s*, sb, and the metal foils 4t
a 4 b are connected to external conductors 5a*gb. i
4 Lube 1 is filled with predetermined amounts of mercury, metal halide, and starting rare gas.

しかして上記のごとく垂直点灯されるランプにおいては
、放電空間における下部の内径d1が従来の同出力のラ
ンプと同様の大きさに形成されるのに対し、上部の内径
d2は大きく形成されておシ、いわゆる上部が太径とな
る一テーノ譬状に形成されている。このことから、点灯
中に下側に位置される下半分に比べて上半分の容積が大
きくなっている。
However, in a lamp that is lit vertically as described above, the lower inner diameter d1 in the discharge space is formed to the same size as a conventional lamp with the same output, whereas the upper inner diameter d2 is formed larger. It is shaped like a cylindrical shape with a larger diameter at the top. For this reason, the volume of the upper half is larger than that of the lower half, which is located on the lower side during lighting.

このような構成によると、点灯中において下側の電極2
bの背部(下方)に形成される最冷部は、バルブ1が赤
外線吸収石英で形成されているととkよシ、温度上昇さ
れる。つt、b赤外線吸収石英は赤外線を吸収して管壁
に熱を貯え石ので自己の温度が高くカリ、この仁とによ
シ最冷部のi!度を従来の普通石英の場合に比べて上昇
させる。したがって最冷部に凝縮されている封入金属の
蒸発を促し、発光効率を高めるものである。
According to such a configuration, during lighting, the lower electrode 2
If the bulb 1 is made of infrared absorbing quartz, the temperature of the coldest part formed at the back (lower part) of b will be increased by more than k. t, b Infrared absorbing quartz absorbs infrared rays and stores heat in the tube wall.As it is a stone, its own temperature is high, and this is the coldest part of the earth! This increases the degree of strength compared to conventional ordinary quartz. Therefore, the evaporation of the enclosed metal condensed in the coldest part is promoted, and the luminous efficiency is increased.

一般にメタルハライドランfは点灯中に、白熱電球に比
べると割合として低いが、入力電力の6〇−程度を赤外
線エネルギーとして放電する。この赤外線エネルギーの
1部が赤外線吸収石英に吸収され最冷部の温度上昇に使
用されるので発光効率の向上に寄与することになる。
Generally, when a metal halide lamp is lit, it discharges about 60 - of the input electric power as infrared energy, although the proportion is lower than that of an incandescent lamp. A part of this infrared energy is absorbed by the infrared absorbing quartz and used to raise the temperature of the coldest part, contributing to improving the luminous efficiency.

なお、上部の放電空間が大きくなることによシ、この空
間内での対流が活発化し、このことから4発光効率が向
上するととKなる。
It should be noted that as the upper discharge space becomes larger, convection within this space becomes more active, and from this, the luminous efficiency increases (K).

ノ4ルブ全体を赤外線吸収石英で作ると、上記最冷部以
外の部分でも管壁の温度上昇を招く。
If the entire tube is made of infrared absorbing quartz, the temperature of the tube wall will rise even in areas other than the coldest part.

本実施例では上手分の容積を大きくする仁とによシ、上
側ではパルプ壁がパルプ中心、りまシアークから半径方
向へ遠ざかることKなり、よってアークからの輻射熱を
受は難くなることに加えて、上部におけるパルプ壁の面
積が増すので局部的な管壁負荷(w/agりを引き下げ
る。このため上側に近づくにつれて管壁温度の上昇を抑
止す石機能が高くなる。パルプ1内における最高温度部
分は、上側電極2aの先端近くに形成されるので、この
最高温度部分の温度上昇が抑止される。よってパルプ1
、・、、の熱劣化が防止さ函 れ長寿命となる。
In this example, in order to increase the volume of the upper part, the pulp wall on the upper side moves away from the center of the pulp and the rim shear arc in the radial direction, which makes it difficult to receive radiant heat from the arc. As the area of the pulp wall increases in the upper part, the local tube wall load (w/ag) is lowered. Therefore, the closer you get to the upper side, the higher the stone function that suppresses the increase in tube wall temperature. Since the temperature portion is formed near the tip of the upper electrode 2a, the temperature rise in this highest temperature portion is suppressed.Therefore, the pulp 1
, , , thermal deterioration is prevented, resulting in a long service life.

下表は、電極間距離42 m58eI55889 、N
a11□ 25 ”? 、HE 7011I9、アルコ9ンガス5
0Torrとした条件を同にして400W級ランプを比
較実験した結果を示す。
The table below shows the distance between the electrodes: 42 m58eI55889, N
a11□ 25”?, HE 7011I9, Alcon 9 gas 5
The results of a comparative experiment using 400W class lamps under the same conditions of 0 Torr are shown.

上記サンデルCは第1図の構成に係るものである。サン
プルBはサンプル皇に比べて発光効率が向上するけれど
も寿命において約2/3キ肴しか耐用できない、サンプ
ルCは発光効率においてサンプル皇よシ優れ、また寿命
においてサンプル皇と遜色ないことが確められた。
Sandel C has the configuration shown in FIG. Although Sample B has improved luminous efficiency compared to Sample Empress, it can withstand only about 2/3 of the lifespan.Sample C has been confirmed to be superior to Sample Empress in luminous efficiency and comparable to Sample Empress in terms of lifespan. It was done.

第2図は水平点灯するランプについて示す。FIG. 2 shows a horizontally lit lamp.

水平点灯の場合にはアークが上方に湾曲される。In the case of horizontal lighting, the arc is curved upwards.

したがって最冷部は第2図のP点で示すようにパルプの
中央部における下部に発生する。また最高温度部分は繭
・1−図の9点で示されるようにノクルブの中央部の上
部に発生する。中央部上部(9点)に最高温度部分が発
生されるのはアークの湾曲に原因している。
Therefore, the coldest part occurs at the lower part of the center of the pulp, as shown by point P in FIG. The highest temperature area occurs at the upper center of the nokurubu, as shown by the 9 points in Figure 1. The reason why the highest temperature occurs at the upper center (point 9) is due to the curvature of the arc.

本実施例では赤外Ii!吸収石英からなるパルプ1のパ
ルプ軸よシ上半部の内容積を下半部よりも大きくしであ
る。つまシ実質的に上向匈パル!壁を上方へ湾曲せしめ
である。このようにすれば、最高温度部分Qがアークか
ら離間されることに加えて、局部的管壁負荷が低下され
るので9点の温度上昇を抑止する。
In this example, infrared Ii! The internal volume of the upper half of the pulp 1 made of absorbed quartz is larger than that of the lower half. Tsumashi is practically an up-and-coming man! The wall is curved upwards. In this way, in addition to separating the highest temperature portion Q from the arc, the local tube wall load is reduced, thereby suppressing the temperature rise at the nine points.

次表は、電極間距離65 IIIIs 8efs 10
”F%NaI 50iy、 Hg 60iyおよびアh
fンガス50Torrの各条件を同一とした700Wメ
メルハライドラングについて比較実験した結果を示す・
なお趨部内径d′、および中央部内径d′2はagz図
の図示位置を示す。
The following table shows the distance between electrodes: 65 IIIs 8efs 10
"F%NaI 50iy, Hg 60iy and Ah
The results of a comparative experiment on 700W memel halide lungs under the same conditions of f gas 50 Torr are shown.
Note that the inner diameter d' of the tail portion and the inner diameter d'2 of the center portion indicate the illustrated positions in the agz diagram.

1率 W) サンプルA B’はサングルA A’より寿命において
約2/3に低下する。サンプルI6c′が第2図の構造
に対する亀ので′6シ効率において最屯優れ、寿命にお
いてはすンデルA A’と遜色ないことを確かめえ。
1 rate W) Sample A B' decreases by about 2/3 in life compared to sample A A'. Confirm that sample I6c' has the highest efficiency in comparison to the structure shown in FIG. 2, and is comparable to Sundel AA' in terms of service life.

〔発明の効果〕 以上詳述したように本発明は発光管パルプを赤外線吸収
石英によ多構成したため、このパルプの赤外線吸収機能
によシ最冷部付近の管壁温度が上昇して最冷部温度を上
昇させるので発光効率が向上する。tた点灯中に上側に
位置する放電空間を下側に比べて大きくしたことによシ
、上側に発生されゐ最高温度部分の管壁がアークから実
質的に遠くな)かつ局部的管壁負荷が低くなって最高温
度部分の管壁温度上昇を抑止する。このため赤外線吸収
石英を用いるにも拘らず寿命の低下が防止される。
[Effects of the Invention] As detailed above, in the present invention, the arc tube pulp is made of infrared-absorbing quartz, so the infrared-absorbing function of this pulp increases the temperature of the tube wall near the coldest part. Since the temperature of the part increases, the luminous efficiency improves. By making the discharge space located on the upper side larger than the lower side during lighting, the tube wall at the highest temperature part generated on the upper side is substantially farther from the arc) and the local tube wall load is reduced. becomes low, suppressing the rise in tube wall temperature at the highest temperature section. For this reason, even though infrared absorbing quartz is used, a decrease in life is prevented.

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

第1図は本発明の一実施例を示し垂直点灯用発光管を示
す構成図、第2図は本発明の他の実雄側を示し水平点灯
用発光管を示す構成図である。 1・・・発光管バルブ、jlm、2b・・・電極。 出願人代理人  弁理士 鈴 江 武 彦1″′ 牙1図 才2図 、:い
FIG. 1 is a block diagram showing one embodiment of the present invention and shows a vertical lighting arc tube, and FIG. 2 is a block diagram showing another actual side of the invention and showing a horizontal lighting arc tube. 1... Arc tube bulb, jlm, 2b... electrode. Applicant's agent Patent attorney Takehiko Suzue 1″′ Fang 1 figure, 2 figures:

Claims (3)

【特許請求の範囲】[Claims] (1)  電極を備えたパルプに水銀と金属ノ・ロダン
化物および始動用希ガスを封入した発光管を有するメタ
ルハライドランプにおいて、上記ノ々ルブは赤外線吸収
石英からなシ、かつ点灯中に上側に位置する放電空間の
容積は下側に位置する放電空間の容積よシ大きく形成し
たことを特徴とするメタルハライドランプ。
(1) In a metal halide lamp that has an arc tube in which mercury, a metal rhodanide, and a starting rare gas are sealed in pulp with electrodes, the bulb is not made of infrared-absorbing quartz, and the bulb is not made of infrared-absorbing quartz and is A metal halide lamp characterized in that the volume of the discharging space is larger than the volume of the discharging space located below.
(2)管軸が垂直姿勢で使用されるメタル・・ライドラ
ンプにおいては、電極間の中央部よりも上側のパルプ径
を下側のパルプ径よル大きく形成したことを特徴とする
特許請求の範囲第(1)項記載のメタルハライドランプ
(2) In a metal ride lamp in which the tube shaft is used in a vertical position, the diameter of the upper pulp is made larger than the diameter of the lower pulp than the central part between the electrodes. A metal halide lamp as described in scope item (1).
(3)管軸が水平姿勢で使用されるメタルハライドラン
プにおいては、バルブ軸よりも上半部のパルプ壁は上方
に彎曲させたことを特徴とする特許請求の範囲第(1)
項記載のメタルハライドランプ。
(3) Claim (1) characterized in that in a metal halide lamp in which the tube shaft is used in a horizontal position, the pulp wall in the upper half of the bulb shaft is curved upward.
Metal halide lamps listed in section.
JP4856082A 1982-03-26 1982-03-26 Metal halide lamp Pending JPS58165239A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4856082A JPS58165239A (en) 1982-03-26 1982-03-26 Metal halide lamp

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4856082A JPS58165239A (en) 1982-03-26 1982-03-26 Metal halide lamp

Publications (1)

Publication Number Publication Date
JPS58165239A true JPS58165239A (en) 1983-09-30

Family

ID=12806766

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4856082A Pending JPS58165239A (en) 1982-03-26 1982-03-26 Metal halide lamp

Country Status (1)

Country Link
JP (1) JPS58165239A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08142U (en) * 1990-10-15 1996-01-23 ゼネラル・エレクトリック・カンパニイ Heat removal means for discharge lamps
JP2012023055A (en) * 2005-05-23 2012-02-02 Koninkl Philips Electronics Nv High intensity discharge lamp

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08142U (en) * 1990-10-15 1996-01-23 ゼネラル・エレクトリック・カンパニイ Heat removal means for discharge lamps
JP2012023055A (en) * 2005-05-23 2012-02-02 Koninkl Philips Electronics Nv High intensity discharge lamp

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