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JPH0313704B2 - - Google Patents
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JPH0313704B2 - - Google Patents

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Publication number
JPH0313704B2
JPH0313704B2 JP55128326A JP12832680A JPH0313704B2 JP H0313704 B2 JPH0313704 B2 JP H0313704B2 JP 55128326 A JP55128326 A JP 55128326A JP 12832680 A JP12832680 A JP 12832680A JP H0313704 B2 JPH0313704 B2 JP H0313704B2
Authority
JP
Japan
Prior art keywords
lamp
sectional area
cross
metal halide
minimum cross
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.)
Expired - Lifetime
Application number
JP55128326A
Other languages
Japanese (ja)
Other versions
JPS5753062A (en
Inventor
Yasuki Mori
Akihiro Kamya
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 Lighting and Technology Corp
Original Assignee
Toshiba Lighting and Technology Corp
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 Lighting and Technology Corp filed Critical Toshiba Lighting and Technology Corp
Priority to JP12832680A priority Critical patent/JPS5753062A/en
Publication of JPS5753062A publication Critical patent/JPS5753062A/en
Publication of JPH0313704B2 publication Critical patent/JPH0313704B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/02Details
    • H01J61/36Seals between parts of vessels; Seals for leading-in conductors; Leading-in conductors

Landscapes

  • Vessels And Coating Films For Discharge Lamps (AREA)

Description

【発明の詳細な説明】 本発明は比較的小ワツトタイプのメタルハライ
ドランプに係り、その効率向上に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a relatively small wattage type metal halide lamp, and to improving the efficiency thereof.

近年省エネルギーの観点から効率の高い照明が
要請されており、特に従来では屋外照明として使
用されていた高効率、高演色性のメタルハライド
ランプを屋内で使用することが注目されている。
メタルハライドランプの屋内使用の条件として
は、この種ランプのもつ高効率、高演色性および
長寿命の利点に加えて小ワツト化が強く要求され
る。すなわち、メタルハライドランプは従来
250W〜2kW級の中・高ワツト形に限られてお
り、一般家庭の屋内照明として白熱電球やけい光
ランプと代替使用されるためには200W以下、特
に100W以下のランプが必要となる。
In recent years, there has been a demand for highly efficient lighting from the perspective of energy conservation, and in particular, the indoor use of high-efficiency, high-color-rendering metal halide lamps, which have traditionally been used for outdoor lighting, is attracting attention.
Conditions for indoor use of metal halide lamps are that in addition to the advantages of this type of lamp, such as high efficiency, high color rendering, and long life, low wattage is strongly required. In other words, metal halide lamps are
It is limited to medium to high wattage types in the 250W to 2kW class, and in order to be used as an alternative to incandescent bulbs and fluorescent lamps for indoor lighting in general homes, lamps of 200W or less, especially 100W or less, are required.

しかしながら小形メタルハライドランプは、従
来の中・高ワツト形の技術をそのまま相似的に適
用できない欠点がある。すなわち従来技術を小ワ
ツト形ランプにそのまま適用た場合、200W以下、
特にワツトが小さくなればなるほどランプ効率が
著しく低くなり、高効率としての利点が損われる
ものであり、これ故に小ワツト形メタルハライド
ランプの開発が遅れていた。
However, small metal halide lamps have the disadvantage that the technology for conventional medium- and high-wattage lamps cannot be applied in a similar manner. In other words, if the conventional technology is applied directly to a small wattage lamp, the power output will be 200W or less,
In particular, the smaller the wattage, the lower the lamp efficiency becomes, and the advantage of high efficiency is lost, and for this reason, the development of small wattage metal halide lamps has been delayed.

本発明者等はこの点について種々の検討をした
結果、ランプが小形化される程封止部の影響によ
る最冷部の温度上昇が低くなり、ランプ効率の向
上を阻害することをつきとめた。すなわち従来技
術をそのまま採用したランプは第1図a,bに示
されている通り、発光管1の両端部に、円筒状の
石英チユーブを加熱して圧潰することにより形成
された封止部2,2を備えており、この封止部
2,2にはモリブデンなどの難融性金属からなる
金属箔導体3,3および4を封止し、これら各金
属箔導体3,3および4に、主電極5,5および
始動用補助電極6を接続してある。なお7,7お
よび8は外部リード線を示す。しかしてこのよう
な封止部2,2はその横幅寸法が発光管チユー
ブの外径よりも大きく広がる傾向にあり、したが
つて封止部の容積は放電空間に比べてかなり大き
な割合を占める。ランプが小形化されるに応じて
放電空間も小さくなることは自明であるが、封止
部はその加工技術の制約からたいして小形化でき
ず、よつて小ワツトランプになる程放電空間に対
する封止部の容積は相対的に増加する。この封止
部は主電極および放電空間の熱を導びいて放出さ
せるから、この封止部を通じて熱損失がきわめて
大きくなり、これ故に最冷部の温度上昇を阻害し
てランプ効率の低下を生じさせるものであつた。
As a result of various studies on this point, the inventors of the present invention found that the smaller the lamp, the lower the temperature rise in the coldest part due to the influence of the sealing part, which impedes improvement in lamp efficiency. That is, as shown in FIGS. 1a and 1b, a lamp employing the conventional technology as it is has sealing parts 2 formed at both ends of an arc tube 1 by heating and crushing a cylindrical quartz tube. . Main electrodes 5 and 5 and an auxiliary starting electrode 6 are connected. Note that 7, 7 and 8 indicate external lead wires. However, the width of such sealing parts 2, 2 tends to be larger than the outer diameter of the arc tube tube, and therefore the volume of the sealing parts occupies a considerably larger proportion than the discharge space. It is obvious that the discharge space also becomes smaller as the lamp becomes smaller, but the sealing part cannot be made much smaller due to limitations in the processing technology, and the smaller the lamp becomes, the more the sealing part for the discharge space becomes smaller. The volume of will increase relatively. Since this sealing part guides and releases the heat of the main electrode and the discharge space, heat loss through this sealing part becomes extremely large, thus inhibiting the temperature rise of the coldest part and causing a decrease in lamp efficiency. It was something that made me want to do something.

本発明はこのような事情にもとづきなされたも
ので、その目的とするところは、熱損失に影響を
及ぼす封止部の特定の位置に狭隘部を設け、その
狭隘部の断面積とランプ入力との関係を規定する
ことにより、金属箔導体の支障を誘発することな
しに、ランプ効率の向上を可能にしたメタルハラ
イドランプを提供しようとするものである。
The present invention was made based on the above circumstances, and its purpose is to provide a narrow portion at a specific position of the sealing portion that affects heat loss, and to determine the cross-sectional area of the narrow portion and the lamp input. By defining the relationship, the present invention attempts to provide a metal halide lamp that can improve lamp efficiency without causing problems with the metal foil conductor.

すなわち本発明は、少なくとも一方の封止部に
主電極の基部と金属箔導体との間に位置して最小
断面積部を形成し、この最小断面積部の断面積の
最大値と最小値をランプ入力との関係において規
制したものである。
That is, in the present invention, a minimum cross-sectional area is formed between the base of the main electrode and the metal foil conductor in at least one of the sealing parts, and the maximum and minimum values of the cross-sectional area of this minimum cross-sectional area are determined. This is regulated in relation to lamp input.

このような本願によれば、最小断面積部の最大
値を規制したので、電極の熱が封止部側に伝えら
れるのを阻止し、封止部からの放熱を規制して最
冷部の温度を高めてランプ効率の向上およびラン
プ光色のばらつきを軽減し、また最小断面積部の
最小値を規制することにより、電極の熱が電極軸
を伝わつて金属箔導体を過熱することを防止し、
箔切れなどの不具合を防止することができる。
According to the present application, since the maximum value of the minimum cross-sectional area is regulated, the heat of the electrode is prevented from being transferred to the sealing part, and the heat dissipation from the sealing part is restricted, thereby reducing the temperature of the coldest part. By increasing the temperature to improve lamp efficiency and reduce variations in lamp light color, and by regulating the minimum value of the minimum cross-sectional area, we prevent the electrode heat from transmitting through the electrode axis and overheating the metal foil conductor. death,
Problems such as foil breakage can be prevented.

以下本発明の一実施例を第2図ないし第4図に
もとづき説明する。
An embodiment of the present invention will be described below with reference to FIGS. 2 to 4.

第2図a,bに示されるメタルハライドランプ
は、点灯中に少なくとも下側に位置される封止部
2の断面積を減少させたものであり、主電極5の
基部、つまり主電極の埋設端部と金属箔導体3と
の間に狭隘部、換言すれば最小断面積部分20が
形成されている。この最小断面積部20の断面積
S(mm2)は第2図bから判る通り、ほぼ矩形状で
あるため×tで計算される。
The metal halide lamp shown in FIGS. 2a and 2b has a reduced cross-sectional area of the sealing part 2 located at least on the lower side during lighting, and the base of the main electrode 5, that is, the buried end of the main electrode. A narrow portion, in other words, a minimum cross-sectional area portion 20 is formed between the portion and the metal foil conductor 3. As can be seen from FIG. 2b, the cross-sectional area S (mm 2 ) of the minimum cross-sectional area portion 20 is approximately rectangular, so it is calculated by xt.

しかして、上記断面積Sがある範囲内の規制さ
れるとランプ効率が大きく向上する。これは実験
にもとずき確認されたものであり、以下その実験
について説明する。
Therefore, when the cross-sectional area S is regulated within a certain range, lamp efficiency is greatly improved. This was confirmed based on an experiment, and the experiment will be explained below.

まず本発明者等は、100Wメタルハライドラン
プについて実験を行つた。すなわち、主電極5の
先端部に位置する発光管の内径が10.5mm、肉厚
1.2mmの石英チユーブ内に電極間距離が15mmとし
た100Wメタルハライドランプを作製した。バル
ブ内には水銀18mmg、ナトリウム沃化物(NaI)
とスカンジウム沃化物(ScI3)との混合物(混合
重量比NaI:ScI3=5:1)を総量10mmgおよび
アルゴンガスを40Torr封入した。このようなラ
ンプにおいて上記封止部2の最小断面積S(mm2
につき、第1図の従来のものから順次変化させ
て、各々そのランプ効率(lm/W)について調
べてみた。この結果は第3図に示されている。な
お第1図a,bに示される従来技術のものはその
断面積Sが35mm2であつた。
First, the inventors conducted an experiment using a 100W metal halide lamp. In other words, the inner diameter of the arc tube located at the tip of the main electrode 5 is 10.5 mm, and the wall thickness is 10.5 mm.
A 100W metal halide lamp with a distance between electrodes of 15mm was fabricated in a 1.2mm quartz tube. 18 mmg of mercury and sodium iodide (NaI) inside the bulb
A total of 10 mmg of a mixture of and scandium iodide (ScI 3 ) (mixed weight ratio NaI:ScI 3 =5:1) and 40 Torr of argon gas were sealed. In such a lamp, the minimum cross-sectional area S (mm 2 ) of the sealing part 2 is
The lamp efficiencies (lm/W) of each lamp were investigated by changing the lamps sequentially from the conventional one shown in FIG. The results are shown in FIG. The cross-sectional area S of the prior art shown in FIGS. 1a and 1b was 35 mm 2 .

第3図から判る通り、100Wメタルハライドラ
ンプの場合には、封止部の最小断面積Sが20mm2
下においてランプ効率が82lm/Wとなり、上記
従来のS=35mm2の場合の65lm/Wに比べて約25
%も効率の向上が認められる。またSが20mm2以下
では効率はほぼ飽和して一定値となる。
As can be seen from Figure 3, in the case of a 100W metal halide lamp, the lamp efficiency is 82lm/W when the minimum cross-sectional area S of the sealing part is 20mm2 or less, compared to 65lm/W when S = 35mm2 . compared to about 25
% improvement in efficiency is also recognized. Further, when S is 20 mm 2 or less, the efficiency is almost saturated and becomes a constant value.

この理由について検討したところ、以下の現象
が考えられる。すなわち、上記ランプは点灯中に
発光管端部がアーク放電および主電極5からの熱
により加熱されるものであるが、封止部2に最小
断面積部分20を形成したので、この最小断面積
部分20によつて熱伝導が阻止され、金属箔導体
3を封止した先端側に熱伝導され難くなる。すな
わち、最小断面積部分20は断面積が小さいので
封止部2の先端側に熱が伝わるのを絞つて規制
し、このため最冷部としての電極基端部の温度が
上昇し、金属ハロゲン化物の蒸発が促される。し
たがつて、ランプ効率が上昇し、ランプ光色のば
らつきも少なくなる。
When we investigated the reason for this, we found the following phenomena. That is, in the above-mentioned lamp, the end of the arc tube is heated by arc discharge and heat from the main electrode 5 during lighting, but since the minimum cross-sectional area portion 20 is formed in the sealing portion 2, this minimum cross-sectional area Heat conduction is blocked by the portion 20, making it difficult for heat to be conducted to the sealed end side of the metal foil conductor 3. In other words, since the minimum cross-sectional area portion 20 has a small cross-sectional area, it restricts the transfer of heat to the tip side of the sealing portion 2, and as a result, the temperature of the base end of the electrode as the coldest portion increases, and the metal halogen Evaporation of compounds is promoted. Therefore, lamp efficiency is increased and variations in lamp light color are reduced.

なお、最小断面積部分20よりも下側の封止部
2先端部は、最小断面積部分20よりも大きな幅
ならびに断面積を有するので放熱性に優れ、した
がつて封止部2の温度上昇が防止される。加え
て、上記したように、最小断面積部分20が封止
部2に熱が伝わるのを規制するので封止部20の
温度上昇が一層抑止される。このため、封止部2
の熱膨張が防止され、金属箔導体3の剥れが無く
なり、リークや金属箔導体3の酸化が防止される
ものである。
Note that the tip of the sealing part 2 below the minimum cross-sectional area part 20 has a larger width and cross-sectional area than the minimum cross-sectional area part 20, so it has excellent heat dissipation, and therefore the temperature of the sealing part 2 does not increase. is prevented. In addition, as described above, since the minimum cross-sectional area portion 20 restricts heat from being transferred to the sealing portion 2, the temperature rise in the sealing portion 20 is further suppressed. For this reason, the sealing part 2
Thermal expansion of the metal foil conductor 3 is prevented, peeling of the metal foil conductor 3 is eliminated, and leakage and oxidation of the metal foil conductor 3 are prevented.

なお、Sが6.6mm2未満のランプにおいては、寿
命試験で9000時間での点灯中にモリブデン箔の酸
化および箔切れが生じるものがあり、5000時間未
満でランプ寿命が尽きるものが見られた。
In some lamps with S of less than 6.6 mm 2 , oxidation and foil breakage of the molybdenum foil occurred during 9000 hours of lighting in some lamps, and lamp life was found to run out in less than 5000 hours.

これについて検討してみると、最小断面積部分
20の断面積をあまりに小さくし過ぎる場合に
は、最冷部および電極5の温度が過度に上昇して
電極軸を通じて金属箔導体3に直接熱が伝わり、
金属箔導体自身が過度に温度上昇する。このた
め、金属箔導体3の剥れが生じ、金属箔導体3の
酸化を招いたものと推測される。
Examining this, we found that if the cross-sectional area of the minimum cross-sectional area portion 20 is made too small, the temperature of the coldest part and the electrode 5 will rise excessively, and heat will be directly transferred to the metal foil conductor 3 through the electrode axis. transmitted,
The temperature of the metal foil conductor itself increases excessively. It is presumed that this caused the metal foil conductor 3 to peel off, leading to oxidation of the metal foil conductor 3.

このことから、最小断面積部分20の断面積
は、電極軸を通じて金属箔導体3に直接伝えられ
ようとする熱を、この最小断面積部分20を通じ
て放出するのに必要な最小範囲が存在することが
判かる。
From this, it can be seen that the cross-sectional area of the minimum cross-sectional area portion 20 has a minimum range necessary to release the heat that would be directly transmitted to the metal foil conductor 3 through the electrode axis through this minimum cross-sectional area portion 20. I understand.

このような理由から、上記最小断面積部分20
の断面積Sが6.6mm2以上であれば、5000時間の点
灯を超えても箔切れなどの不具合を生じないもの
と考えられる。したがつて100W形のメタルハラ
イドランプはSを6.6mm2〜20mm2の範囲に規制すれ
ば、第1図a,bの従来のものに比べて効率にお
いて25%の向上が可能になることが判明した。
For this reason, the minimum cross-sectional area portion 20
If the cross-sectional area S is 6.6 mm 2 or more, it is considered that problems such as foil breakage will not occur even after lighting for more than 5,000 hours. Therefore, it has been found that by regulating S to a range of 6.6 mm 2 to 20 mm 2 for a 100W metal halide lamp, it is possible to improve efficiency by 25% compared to the conventional lamps shown in Figure 1 a and b. did.

つぎに本発明者等は上記100Wランプと同様な
実験を、40W、250W、400Wの各ランプにおいて
も実験した。この結果を第4図に示す。
Next, the inventors conducted experiments similar to those for the 100W lamp described above using 40W, 250W, and 400W lamps. The results are shown in FIG.

第4図において特性Aは各ランプにおいてラン
プ効率が向上する境界点を結んだものであり、
ほゞ直線になつている。また特性Bは寿命中にモ
リブデン箔の箔切れなどが生じない限界点を結ん
だものであり、この特性もほゞ直線になつてい
る。したがつて特性Aと特性Bとで囲まれた斜線
の領域内に最小断面積Sを設定すれば、高効率で
長寿命のメタルハライドランプが得られることが
判る。特性Aは S=16.6log10P−13.2 …(1) で示され、また特性Bは S=5.6log10P−4.6 …(2) で示される。
In Figure 4, characteristic A connects the boundary points where lamp efficiency improves in each lamp,
It's almost a straight line. Characteristic B connects the limit points at which the molybdenum foil does not break during its life, and this characteristic is also a substantially straight line. Therefore, it can be seen that if the minimum cross-sectional area S is set within the shaded area surrounded by characteristics A and B, a metal halide lamp with high efficiency and long life can be obtained. Characteristic A is expressed as S=16.6log 10 P−13.2 …(1), and characteristic B is expressed as S=5.6log 10 P−4.6 …(2).

したがつて最小断面積S(mm2)はランプ入力P
(watt)に対して 5.6log10P−4.6≦S≦16.6log10P−13.2 …(3) を満足すればよいことになる。
Therefore, the minimum cross-sectional area S (mm 2 ) is the lamp input P
(watt), it is sufficient to satisfy 5.6log 10 P−4.6≦S≦16.6log 10 P−13.2 …(3).

なお第4図中破線Cで示される特性は第1図
a,bに示される従来タイプにおける平均値であ
る。
Note that the characteristics indicated by the broken line C in FIG. 4 are average values for the conventional type shown in FIGS. 1a and 1b.

上記第(3)式を満足すればランプ効率の点で40W
クラスは40%、100Wクラスは25%、250Wクラス
は15%および400Wクラスは10%程度の向上が確
認さており、小ワツトタイプ程、本発明が効果的
であることが判る。
If the above equation (3) is satisfied, the lamp efficiency will be 40W.
It has been confirmed that the improvement is 40% for the 100W class, 25% for the 100W class, 15% for the 250W class, and 10% for the 400W class, indicating that the present invention is more effective for smaller wattage types.

なお、700Wや1kWのメタルハライドランプの
場合、放電空間(電極間距離)に比べて封止部の
容積の割合が小さいので本発明を適用してもその
効果はあまり期待できない。よつて本発明は
400W級以下のランプでその効果が認められるも
のである。
Note that in the case of a 700 W or 1 kW metal halide lamp, the volume ratio of the sealing part is small compared to the discharge space (distance between electrodes), so even if the present invention is applied, not much effect can be expected. Therefore, the present invention
This effect is recognized in lamps of 400W class or less.

なお、第2図の構造は最小断面積部分20の断
面形状を偏平な矩形形状としたが、本発明は第5
図および第6図にそれぞれ他の実施例として示す
ように、最小断面積部分20の断面形状を楕円形
や円形にしてもよい。
Note that in the structure shown in FIG. 2, the cross-sectional shape of the minimum cross-sectional area portion 20 is a flat rectangular shape, but the present invention
As shown in FIG. 6 and FIG. 6 as other embodiments, the cross-sectional shape of the minimum cross-sectional area portion 20 may be oval or circular.

そしてこのような各形状の最小断面積部分を得
る方法としては、従来の圧潰封止工程後にカツタ
ーやレーザビーム光を利用して所定形状に切断加
工するようにしてもよく、または量産性を考慮す
れば封止前に予め石英チユーブの端部を縮径して
おく小径チユーブを連結しておくなどの手段も実
施可能である。
As a method of obtaining the minimum cross-sectional area of each shape, it is possible to cut into a predetermined shape using a cutter or laser beam after the conventional crushing and sealing process, or considering mass production. In this case, it is also possible to take measures such as connecting small-diameter tubes by reducing the diameter of the ends of the quartz tubes before sealing.

ところで上述のどとき本発明によればランプ光
色のらつき幅を小さくできる結果もある。すなわ
ち従来のものは、特に小ワツトのランプ程発光管
の封止形状、電極高さなどの製造上のわずかなば
らつきによつてもランプの色温度が大きく変化
し、許容製造ばらつき範囲内で色温度が1500〓も
差異があつた。しかしながら本発明に係るもの
は、発光管の最冷部温度が小ワツト形ランプ程上
昇される割合が大きいもので、上記と同一許容ば
らつき範囲内であつても色温度のばらつきは500
〓の範囲に抑えることができた。
By the way, according to the present invention as described above, there is also the result that the width of fluctuation in lamp light color can be reduced. In other words, with conventional lamps, the color temperature of the lamp changes greatly even with slight manufacturing variations in the sealing shape of the arc tube, electrode height, etc. There was a difference in temperature of 1500〓. However, in the case of the present invention, the temperature of the coldest part of the arc tube is increased at a higher rate as the smaller the wattage type lamp is, and even within the same allowable variation range as above, the variation in color temperature is 500%.
I was able to keep it within the range of .

また他の効果として以下のごとき利点を奏す
る。つまり通常メタルハライドランプは点灯時に
下側となる発光管の端部に、主電極を覆うように
してアルミナ等の保温膜を形成している。本発明
によるとこの保温膜を省略もしくはその塗布範囲
を少くでき、アルミナの使用量を減少できる。ま
たこのアルミナ保温膜による光束低下を解消でき
る。たとえば100W形の場合、発光管端部に塗布
されるアルミナの高さは電極高さと同等の高さと
なるようにしてあるが、本発明によれば少なくと
も電極高さの1/2の高さまで低くすることができ
る。この結果光束が5%向上でき、アルミナの使
用量も従来の50〜70%で充分である。
In addition, the following advantages are achieved as other effects. In other words, normally in a metal halide lamp, a heat insulating film made of alumina or the like is formed on the end of the arc tube, which is the lower side when the lamp is lit, so as to cover the main electrode. According to the present invention, this heat-retaining film can be omitted or its application area can be reduced, and the amount of alumina used can be reduced. Furthermore, the reduction in luminous flux caused by this alumina heat-retaining film can be eliminated. For example, in the case of the 100W type, the height of the alumina applied to the end of the arc tube is set to be the same height as the electrode height, but according to the present invention, the height of the alumina applied to the end of the arc tube is reduced to at least 1/2 of the electrode height. can do. As a result, the luminous flux can be improved by 5%, and the amount of alumina used is sufficient at 50 to 70% of the conventional amount.

以上詳述したように本発明は、主電極の埋設端
部と金属箔との間に位置する封止部に狭隘部を形
成し、狭隘部の断面積Sとランプ入力Pとの関係
を 5.6log10P−4.6≦S≦16.6log10P−13.2に規定し
たので、ランプ効率が向上し、ランプ寿命も延長
されるとともにランプ光色のばらつきも縮少さ
れ、しかも金属箔導体の酸化による箔切れや封止
部のリークも防止され、小中ワツト形ランプとし
て実行に供し得るメタルハライドランプを可能に
する利点がある。
As detailed above, the present invention forms a narrow part in the sealing part located between the buried end of the main electrode and the metal foil, and the relationship between the cross-sectional area S of the narrow part and the lamp input P is expressed as follows. Since log 10 P−4.6≦S≦16.6log 10 P−13.2 is specified, lamp efficiency is improved, lamp life is extended, and variations in lamp light color are reduced. This has the advantage of preventing breakage and leakage from the sealing portion, making it possible to produce a metal halide lamp that can be used as a small or medium Watt type lamp.

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

第1図a,bは従来のメタルハライドランプを
示し、第1図aは正面図、第1図bは第1図a中
B−B線に沿う断面図、第2図a,bないし
第4図は本発明の一実施例を示し、第2図aは正
面図、第2図bは第2図a中B−B線に沿う
断面図、第3図は100Wメタルハライドランプに
おけるランプ効率と最小断面積との関係を示す特
性図、第4図は最小断面積とランプ入力との関係
を示す特性図、第5図および第6図はそれぞれ断
面形状の変形例を示す断面図である。 1…発光管、2…封止部、3…金属箔導体、5
…主電極、20…最小断面積部分。
1A and 1B show a conventional metal halide lamp, FIG. 1A is a front view, FIG. 1B is a sectional view taken along line B-B in FIG. The figures show an embodiment of the present invention, in which Fig. 2a is a front view, Fig. 2b is a sectional view taken along line B-B in Fig. 2a, and Fig. 3 is a lamp efficiency and minimum FIG. 4 is a characteristic diagram showing the relationship between the minimum cross-sectional area and the lamp input, and FIGS. 5 and 6 are cross-sectional views showing modified examples of the cross-sectional shape. DESCRIPTION OF SYMBOLS 1... Arc tube, 2... Sealing part, 3... Metal foil conductor, 5
...Main electrode, 20...Minimum cross-sectional area portion.

Claims (1)

【特許請求の範囲】 1 主電極軸の一部を埋設し保持すると共に、主
電極に接続する金属箔導体を封着した封止部を有
する発光管内に、水銀、金属ハロゲン化物および
始動用希ガスを封入した400W級以下のメタルハ
ライドランプであつて、前記主電極の埋設端部と
前記金属箔との間に位置する前記封止部に狭隘部
を形成して成り、前記狭隘部の断面積S(mm2)と
ランプ入力P(watt)との関係が 5.6log10P−4.6≦S≦16.6log10P−13.2であるこ
とを特徴とするメタルハライドランプ。
[Scope of Claims] 1. Mercury, metal halides, and a starting rare substance are contained in an arc tube that has a sealing part that embeds and holds a part of the main electrode shaft and seals a metal foil conductor connected to the main electrode. A gas-filled metal halide lamp of 400W class or less, comprising a narrow part formed in the sealing part located between the buried end of the main electrode and the metal foil, and the cross-sectional area of the narrow part is A metal halide lamp characterized in that the relationship between S (mm 2 ) and lamp input P (watt) is 5.6log 10 P−4.6≦S≦16.6log 10 P−13.2.
JP12832680A 1980-09-16 1980-09-16 Halide lamp Granted JPS5753062A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12832680A JPS5753062A (en) 1980-09-16 1980-09-16 Halide lamp

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12832680A JPS5753062A (en) 1980-09-16 1980-09-16 Halide lamp

Publications (2)

Publication Number Publication Date
JPS5753062A JPS5753062A (en) 1982-03-29
JPH0313704B2 true JPH0313704B2 (en) 1991-02-25

Family

ID=14982007

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12832680A Granted JPS5753062A (en) 1980-09-16 1980-09-16 Halide lamp

Country Status (1)

Country Link
JP (1) JPS5753062A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5993057U (en) * 1982-12-16 1984-06-23 岩崎電気株式会社 high pressure metal vapor discharge lamp
JPS59115557U (en) * 1983-01-25 1984-08-04 岩崎電気株式会社 high pressure metal vapor discharge lamp
US5055740A (en) * 1987-02-25 1991-10-08 Venture Lighting Interntional, Inc. Horizontal burning metal halide lamp
EP0451647B1 (en) * 1990-04-12 1995-07-05 Patent-Treuhand-Gesellschaft für elektrische Glühlampen mbH High-pressure discharge lamp and method for its manufacture

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5238788A (en) * 1975-09-19 1977-03-25 Matsushita Electronics Corp Manufacturing method of vaporized metal discharge lamp
JPS54481A (en) * 1978-05-29 1979-01-05 Mitsubishi Electric Corp Method of manufacturing light emitting tubes for high-voltage discharge lamp
JPS55161358A (en) * 1979-06-05 1980-12-15 Mitsubishi Electric Corp High voltage metal vapour discharge lamp

Also Published As

Publication number Publication date
JPS5753062A (en) 1982-03-29

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