JPS5812252A - Small-sized metal vapor discharge lamp - Google Patents

Small-sized metal vapor discharge lamp

Info

Publication number
JPS5812252A
JPS5812252A JP10971681A JP10971681A JPS5812252A JP S5812252 A JPS5812252 A JP S5812252A JP 10971681 A JP10971681 A JP 10971681A JP 10971681 A JP10971681 A JP 10971681A JP S5812252 A JPS5812252 A JP S5812252A
Authority
JP
Japan
Prior art keywords
tube
axises
luminous
electrodes
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
Application number
JP10971681A
Other languages
Japanese (ja)
Inventor
Akihiro Inoue
昭浩 井上
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 JP10971681A priority Critical patent/JPS5812252A/en
Publication of JPS5812252A publication Critical patent/JPS5812252A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/02Details
    • H01J61/30Vessels; Containers
    • H01J61/34Double-wall vessels or containers

Landscapes

  • Vessels And Coating Films For Discharge Lamps (AREA)

Abstract

PURPOSE:To improve the luminous efficacy, prevent going out half-burnt, and avoid damages of a luminous tube by bending the luminous tube so that the angle formed by electrode axises of main electrodes provided on both ends of the tube is made zero or negative. CONSTITUTION:A quartz glas tube with an inside diameter of 3.3mm., for instance, is bent in an arc with the maximum outside dismeter D of some 20mm. to form a luminous tube 105, on both ends of which are arranged electrodes 106a, 106b. Extension lines of electrode axises 107a, 107b are crossed each other, and the crossing angle theta of these axises is made about 60 deg.. Crossing of axises means that the angle formed by the axises is in a negative range. In such a lamp, the distance between the electrodes 106a, 106b is made some 25mm. which is extremely longer compared with a conventional one, and the voltage drop ratio at the electrodes is smaller in relation to the luminous wave length, thereby the power factor is large, the lamp is reluctant to go out half-burnt, and the luminous efficacy is also improved. In addition, the space valume is large and the vapor pressure is made some six atm, thus no bursting of the luminous tube 105 occurs.

Description

【発明の詳細な説明】 本実倒は入力電力が100W以下の小形金属蒸気放電灯
(=関する。
DETAILED DESCRIPTION OF THE INVENTION This invention relates to a small metal vapor discharge lamp with an input power of 100W or less.

近年、省罐力、省エネルギーの要晴にもとづき、小形で
高効率な1iil11111度金II4蒸気放電灯の一
発が進められている。雀′峨力、省エネルギーの丸地か
らすれば、一般寂庭用の照明(二省エネルギー壁の光源
が使用されればその効果は大である。し九がって一般家
gじ使用可訃な100W以下の金属点気放鑞灯が注目さ
れている。
In recent years, based on the need to save can power and energy, small and highly efficient 1IIL 11111 degree gold II4 steam discharge lamps have been developed. Considering the power and energy-saving round area, lighting for general private gardens (if energy-saving wall light sources are used, the effect will be great. Metal point air lamps of 100W or less are attracting attention.

ところで、従来における100W以下の金属蒸気放醒灯
は、第1図(4)およびtBI Hその発光管を示しで
ある。硝1図囚のタイプは、石英ガラスチューブからな
る発光管1の互4二対向する両端に主電極1m、2bを
配置し、これら主電極j!a、Ibのそれぞれ電極軸J
a、Jbは、発光管1の鮒止部4m、4bじ封止され友
金JII4箔導体6m、lbを介して外部リード線is
By the way, a conventional metal vapor discharge lamp of 100 W or less is shown in FIG. 1 (4) and tBIH. In the type shown in Figure 1, main electrodes 1m and 2b are arranged at opposite ends of an arc tube 1 made of a quartz glass tube, and these main electrodes j! a, Ib, respectively electrode axis J
a, Jb are the sealing parts 4m, 4b of the arc tube 1, and the external lead wires are connected via the Yukin JII4 foil conductor 6m, lb.
.

gb+二接続されている。このような発光管1(=おい
ては、主電極1m、Ib間の距離、つまり電極間距離が
約5111程度であ如、これは97)の入力電力t−1
00W以下にするためであって極端(二短かくしである
。しかしながら電檜関距離が畑かいと、峨極亀二おける
電位降下割合が大きくて発光効率の低下を招き、力本が
儲く立m見易い不具合がある。またこの椙のものはI1
1[徐r&!1距離が短かいにも拘らずランプ電圧をt
!1OV−v、10(1’とする九め(二封入水伽重を
多くしであることから、動作状態においては蒸気圧が数
気圧以上となり、場合によっては発光管の破裂を招く惧
れ4ある。
gb+2 connected. The input power t-1 of such an arc tube 1 (=in the case of 1 m of main electrodes, the distance between Ib, that is, the distance between electrodes is about 5111, which is 97)
This is to reduce the power to less than 00W, and it is extremely short.However, if the electric distance is short, the potential drop rate at the electric pole will be large, leading to a decrease in luminous efficiency, and the power source will not be able to make a profit. m There is a problem that is easy to see.Also, this one is I1
1 [Xu r&! 1 Even though the distance is short, the lamp voltage is
! 1OV-v, 10 (1') (2) Due to the large weight of the sealed water canister, the vapor pressure will exceed several atmospheres in the operating state, which may cause the arc tube to burst.4 be.

第1図1aの場合は、石英ガラス装発光管チェープ11
の一端嘔=、主電極12畠、12bを設け、これら主電
極11s、Ilbの電極軸11a、Ilbは発光管1の
一端のみ嘔=形成され大剣止部14に封止され九金属箔
導体18m、15bを介して外部リード線1−1.Ig
bじII綬されている。この亀の4=あっても、電極開
動−はやはシ矩かくて、上記第1図国の場合と−ill
な欠点を有している。
In the case of Fig. 1 1a, the quartz glass-encased arc tube chain 11
At one end, main electrodes 12 and 12b are provided, and the electrode shafts 11a and Ilb of these main electrodes 11s and Ilb are formed only at one end of the arc tube 1, and are sealed in the large stopper part 14 and are made of metal foil conductors. 18m, external lead wire 1-1. via 15b. Ig
bji II Ribbon. Even if this turtle is 4, the electrode opening is still square, so it is different from the case of the country shown in Figure 1 above.
It has some drawbacks.

本発明はこのような事情しもとづきなされ丸亀ので、七
の目的とするところは、発光管が小形嘔二も拘らず電極
間距離を大きくシ、シかも封止部の温度上昇が促進され
るよう(二して1発光効本の向上、立消え防止および発
光管の破損解消が可能となる小形金属蒸気放電灯を提供
しようとする4のである。
The present invention was made based on the above circumstances, and the seventh object is to increase the distance between the electrodes in spite of the small size of the arc tube, so that the temperature rise in the sealed portion is promoted. (Secondly, the present invention aims to provide a small metal vapor discharge lamp that can improve the luminous efficacy, prevent the lamp from extinguishing, and eliminate damage to the arc tube.)

すなわち本発明は発光管チューブを曲成し、その両端6
二設けられ喪主電極の電極軸線相互のなす角度を零もし
くは負とすること媚=より、電極間距離を大きくするに
4拘らず発光管全体の大きさをコンパクト化てき、しか
も封止部相互が比較的接近することから封止部の温度上
昇が可能となって前記目的を遺戒できる小形金14蒸気
放電灯を特徴とする。
That is, in the present invention, the arc tube is bent, and both ends 6 of the arc tube are bent.
By making the angle between the electrode axes of the two mourner electrodes zero or negative, the overall size of the arc tube can be made more compact regardless of the distance between the two electrodes, and the sealing parts can be separated from each other. The compact gold-14 steam discharge lamp is characterized by being relatively close to each other, allowing the temperature of the sealing part to rise, thereby achieving the above purpose.

以下本発明の一賽施例を第2図鑞二もとづき説明する。An embodiment of the present invention will be described below based on FIG. 2.

第2図において101は外管であ)、白熱電球との交互
性を考慮して白熱電球のパルプとはtt rw>形とし
てあり最大径約!!011mである。
In Fig. 2, 101 is the outer bulb), and considering the alternation with incandescent bulbs, the pulp of incandescent bulbs is tt rw> shaped, with a maximum diameter of about 100 lbs. ! It is 011m.

101はステム、10Mは口金、104畠。101 is the stem, 10M is the base, and 104 is the hat.

104bはサポート兼用の内部導線を示す。Reference numeral 104b indicates an internal conductor that also serves as a support.

106は本発明蝋二係る発光管であり、たとえば円径λ
3Uの石英ガラスチューブを曲成し、e人外ykDが2
011118f嘔;した円弧状(二形成しである。褪光
管108の両端部には゛鑵極106m、101bを配置
してあ〉、電極軸101a。
106 is an arc tube according to the present invention, for example, the circular diameter λ
A 3U quartz glass tube is bent, and the e-human ykD is 2.
011118f The electrode shaft 101a has a circular arc shape (two-shaped). At both ends of the fader tube 108, electrodes 106m and 101b are arranged.

xorbはそれぞれ封止部101m、1011b(;刺
止した金属箔導体109m、1011bを介して外部リ
ードlillJJ(1m、JJabに接続されている。
xorb is connected to external leads lillJJ(1m, JJab) via sealed metal foil conductors 109m, 1011b, respectively.

これら外部リード線110mおよび110bは1IIT
配内部導線104m、104b(二参M′t−れている
。上記構成の発光管tartにおいては、電極間il!
鴫が石英ガラスチューブの中心軸上砿二沿っておシ、約
25WJとなっている。
These external lead wires 110m and 110b are 1IIT
The internal conductors 104m and 104b (two-layer M't) are connected. In the arc tube tart with the above configuration, the distance between the electrodes is il!
The weight is approximately 25 WJ along the central axis of the quartz glass tube.

を九鬼極軸101m、10rbの軸線の延長線は互に交
差されてお夛、これら軸線の交差角−はl5Ofとなっ
ている。なお軸線が交差することは、これら軸線のなす
角度が負の範囲にあることを意味している。上記発光管
101内には始動用希ガスとしてアルゴンガスが50 
Torrと、水銀か3−およびスカンジウム(8c)と
ナトリウム(N1)の沃化物が10mp封入されている
The extension lines of the 101m and 10rb axes of the Kuki polar axis intersect with each other, and the intersection angle of these axes is 15Of. Note that the fact that the axes intersect means that the angle formed by these axes is in a negative range. Argon gas is contained in the arc tube 101 as a starting rare gas.
Torr, 10 mp of mercury, 3-, scandium (8c) and sodium (N1) iodides are enclosed.

このような構成C二係る小形メタルハライドランプC二
あっては、ランプ電圧が130Vであシ。
In the small metal halide lamp C2 having such a configuration C2, the lamp voltage is 130V.

ランプ入力電力が5oWの場合−二おける発光効41k
i 7!Sjm/W  、平均演色評価数は6o凡烏で
あつ九。
When the lamp input power is 5oW, the luminous efficiency at -2 is 41k
i7! Sjm/W, average color rendering index is 6o mediocre and 9.

しかしてこのようなランプにおいては、電極間距離が2
51u111fとなるので、従来の第1図(船やIBI
に示されたもの鴫二比べて極めて長くな)、よって電極
における電位降下割合が発光長c二比べて小さいため力
率4大きく立消剋1いげがヤでなく、発光効率が向上す
る本のである。tたこのような電極間距離が長いこと(
二加えて、電極軸101m、10Wbの延長線が交差す
ることは両端封止部101a、l01lbか互に接近す
ることC:なるため、それぞれの封止部10am、10
abiニおけh発熱が互c二他方の封止部を加熱し合う
から、これら刺止部近傍の封入金属の蒸発を促して発光
効率の向上に寄与するものである。さらC二ま九発光管
ios内砿=おいては従来纏;比べて空間容積が大きく
、蒸気圧が6気圧糊変となり、この九め発光@101の
破裂などを生じない。
However, in such a lamp, the distance between the electrodes is 2
51u111f, so the conventional figure 1 (ship or IBI
Therefore, since the potential drop rate at the electrode is smaller than the emission length c2, the power factor increases by 4, and the power factor does not increase by 1, which improves the luminous efficiency. It is. tThe distance between the electrodes is long like an octopus (
2. In addition, when the extension lines of the electrode axes 101m and 10Wb intersect, the sealing portions 101a and 10lb at both ends approach each other.
Since the heat generated in the two holes mutually heats the sealing portions on the other side, the evaporation of the sealed metal in the vicinity of these piercing portions is promoted, contributing to an improvement in luminous efficiency. In addition, the space volume is larger than that of the conventional one, and the vapor pressure changes by 6 atmospheres, so that the explosion of this nine-light emission tube @101 does not occur.

なお1石英ガラスチューブを曲成して4その最大径Dg
!OU機縦であるから、白熱璽球製の外管(最大径50
MU)内に充分収容することができる利点もある。
Note that 1. when bending a quartz glass tube, 4. its maximum diameter Dg
! Since the OU machine is vertical, the outer tube made of incandescent bulb (maximum diameter 50mm)
It also has the advantage of being able to be accommodated sufficiently within the MU.

第3図(二は本発明の他の実施例(=優る発光管を示し
である。この発光管131は石英ガラスチューブをはげ
U字状C−曲成したもので、電極軸101m、10rb
のなす角Haは零、つ1ヤ鉦に平行をなしている。
FIG. 3 (2) shows another embodiment (= superior arc tube) of the present invention. This arc tube 131 is made by bending a quartz glass tube into a bald U-shape.
The angle Ha formed by this is zero and is parallel to the arrow.

鈍光管121は内径8Uの石英ガラスチューブをU字状
(二重成し、確極間距離を2513とした場合、始動用
ガスとしてキセノンガスを100Tart、氷像4mj
’%および沃化タリウム、沃化す) IJウム、沃化イ
ンジウム、沃化錫の混合物を5 m?封入しである。こ
のような発光管JJJを第2図のような外管101円C
二収容し、外管101内(=窒累ガス200 Torr
封入したものは、ランプ電圧125V、ランプ入力電力
SOWで竜元効JI701s/W 、平均演色評価数は
80 Ra であった。
The obtuse light tube 121 is a U-shaped quartz glass tube with an inner diameter of 8U (double structure, when the distance between the poles is 2513, xenon gas is 100 Tart as a starting gas, and ice image is 4 mj).
'% and thallium iodide, thallium iodide) 5 m? It is enclosed. Convert such a luminous tube JJJ to an outer tube 101 yen C as shown in Figure 2.
Nitrogen gas is stored in the outer tube 101 (= 200 Torr of nitrogen gas).
The enclosed lamp had a lamp voltage of 125 V, a lamp input power SOW, a dragon effect of JI 701 s/W, and an average color rendering index of 80 Ra.

この第3−の例も、電゛極関距−か大きく、かつ封止部
相互4二近接していることから第2図の場合とrMj様
な効果を奏するものである。
This third example also has an effect similar to that of the case of FIG. 2, since the electrode distance is large and the sealing portions are close to each other.

なお、1I21Klの場合および第3図の場合のいづれ
であっても%#E3図鑑二示されたような赤外線反射膜
をコーティングし九耐熱透光性スリー1200を被せる
と発光管から放射される熱4二よ)外管101を保護す
るばか〕でなく、よ配スリーブ5oot二よって反射さ
れた熱で発光管の湿度上昇を促すので%蒸気圧が上昇し
%発光効率の向上が可dtニなる。
In addition, in both the case of 1I21Kl and the case of Figure 3, if you coat it with an infrared reflective film as shown in %#E3 Encyclopedia 2 and cover it with 9 heat-resistant translucent 3 1200, the heat radiated from the arc tube will be reduced. 42) Instead of protecting the outer tube 101, the heat reflected by the outer sleeve 5oot2 promotes an increase in the humidity of the arc tube, increasing the vapor pressure and improving the luminous efficiency. .

しかして第2図および第3!9CIの場合、電極軸10
1m、10rbのなす内縦が負もしくは零としたこと(
二よp封止811J##畠、101bが互に近接するこ
と1二な如、これに比べて誹1図囚および(Blの従来
例は電極軸のなす角f#が180@および正の@鯖とな
るものであることが判る。しかもこれら第1図(A)お
よび(Bの吃のはチェー′プを曲成し九ものてはないか
ら本発明のごとき効果は期待できないものである。
However, in the case of FIGS. 2 and 3!9CI, the electrode axis 10
The inner length of 1m and 10rb is negative or zero (
Compared to this, in the conventional example of Bl, the angle f# formed by the electrode axis is 180 @ and positive. It can be seen that the stutters in Figures 1 (A) and (B) are curved chains and there are no nine, so the effect of the present invention cannot be expected. .

なお本発明はメタルハライドランプ一二は−らず、為圧
ナトリウムランプや高圧水−灯など6二おいてもX I
ll二冥施可訃である。
Note that the present invention does not apply to metal halide lamps, but also applies to pressurized sodium lamps, high-pressure water lamps, etc.
It's possible to do so.

以上−達した通夛本発明は100W以下のランプ1二お
いて、発光管チューブを曲成しこの発光管チェー1の両
端I:配taれ九主゛峨極の電極軸線相互のなす角度が
零もしくは負となるように構成したものである。したが
ってこのものは発光管を小形;ンバクト化できる6二も
拘らず電接開動−を長くすることができる良め発光効率
の同士が可lF!堪二なシ立消え4少く、かつ蒸気圧を
低くして発光管の破横も防止できる。轡に発光管の封止
部が互鑞:近接することから、封止部相互がm*上昇を
促して発光効率の向上砿二大きく寄与する利点かある。
According to the present invention, in a lamp 12 of 100 W or less, the arc tube tube is bent, and the angle between the electrode axes of the nine main electrodes is arranged at both ends I of the arc tube chain 1. It is configured to be zero or negative. Therefore, this product has a small arc tube; it can be compacted, it can lengthen the electrical connection operation, and it can have a good luminous efficiency. It is possible to reduce the number of times the arc tube disappears, and to lower the vapor pressure to prevent the arc tube from breaking. Since the sealing portions of the arc tube are close to each other, there is an advantage that the sealing portions promote an increase in m* and greatly contribute to improving luminous efficiency.

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

IIIL1図囚および(Bは従来の発光管を示す断面図
、第2WJは本発明の一実馳例を示す全体の側th図、
第3図は本発明の変形例を示す斜視−である。 108.111・・・発光管%7018゜J II #
 k−・・主電極、Jarm、101b”・電極軸、、
jJ Ol a 、 J 08 b−・・封止部。 出願入代通人 弁理士 鈴 圧式 彦 第1図 第2図 第3図
FIG.
FIG. 3 is a perspective view showing a modification of the present invention. 108.111... Arc tube %7018゜J II #
k-・Main electrode, Jarm, 101b”・electrode axis,
jJOla, J08b-...Sealing part. Patent Attorney Suzu Hiko, Figure 1, Figure 2, Figure 3

Claims (1)

【特許請求の範囲】 発光管チューブの両端(ニ一対の主電極を設け。 咳チューブ内(=始動用希ガスと水鋏および発光金属も
しくは金属ハイゲン化物を封入し、かつランプの入力電
力が100W以下である小形金属蒸気放電灯(二おいて
、上記発光管チューブを曲成し、その1LIJI端の一
対の主11極(二おける電極軸線相互のなす内雇が苓も
しくは負であることを特徴とする小形金属蒸気放電灯。
[Scope of Claims] A pair of main electrodes are provided at both ends of the arc tube tube. Inside the cough tube (=starting rare gas, water scissors, and luminescent metal or metal hygenide are sealed, and the input power of the lamp is 100 W. The following is a small metal vapor discharge lamp (the above-mentioned arc tube tube is bent in two positions, and a pair of main 11 poles at one LIJI end thereof (characterized in that the internal relationship between the electrode axes in the two positions is negative or negative) A small metal vapor discharge lamp.
JP10971681A 1981-07-14 1981-07-14 Small-sized metal vapor discharge lamp Pending JPS5812252A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10971681A JPS5812252A (en) 1981-07-14 1981-07-14 Small-sized metal vapor discharge lamp

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10971681A JPS5812252A (en) 1981-07-14 1981-07-14 Small-sized metal vapor discharge lamp

Publications (1)

Publication Number Publication Date
JPS5812252A true JPS5812252A (en) 1983-01-24

Family

ID=14517409

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10971681A Pending JPS5812252A (en) 1981-07-14 1981-07-14 Small-sized metal vapor discharge lamp

Country Status (1)

Country Link
JP (1) JPS5812252A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03144632A (en) * 1989-10-31 1991-06-20 Fuji Photo Film Co Ltd Silver halide photographic sensitive material
EP1111654A1 (en) * 1999-12-23 2001-06-27 General Electric Company Single ended ceramic arc discharge lamp and method of making the same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03144632A (en) * 1989-10-31 1991-06-20 Fuji Photo Film Co Ltd Silver halide photographic sensitive material
EP1111654A1 (en) * 1999-12-23 2001-06-27 General Electric Company Single ended ceramic arc discharge lamp and method of making the same

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