JPH0388256A - Fluorescent lamp - Google Patents

Fluorescent lamp

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Publication number
JPH0388256A
JPH0388256A JP22156389A JP22156389A JPH0388256A JP H0388256 A JPH0388256 A JP H0388256A JP 22156389 A JP22156389 A JP 22156389A JP 22156389 A JP22156389 A JP 22156389A JP H0388256 A JPH0388256 A JP H0388256A
Authority
JP
Japan
Prior art keywords
cross
shape
straight
flat
section
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
JP22156389A
Other languages
Japanese (ja)
Inventor
Kunio Yuasa
湯浅 邦夫
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 JP22156389A priority Critical patent/JPH0388256A/en
Publication of JPH0388256A publication Critical patent/JPH0388256A/en
Pending legal-status Critical Current

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  • Vessels And Coating Films For Discharge Lamps (AREA)

Abstract

PURPOSE:To prevent snaking of a positive column for stabilization of flux of light thereof by forming the cross section shape of the bending part in a flat shape while making the maximum diameter of the flat shape longer than the minimum diameter of the flat cross section of a straight part. CONSTITUTION:Cross sections of the straight parts 11a, 12a of respective straight bulbs 11, 12 are formed, for instance, in a flat shape of an elliptic shape, while a discharge path to be passed through by a positive column is formed on the axis of the center of gravity Oa of the flat cross section. On the other hand, a cross section of a connection part 13 is formed, for instance, almost in a fan shape and a long diameter l0 10 is longer set up than a short diameter (s) of the cross section shape of the straight parts 11a, 12a. In this case, electron density of the positive column passed through the respective straight parts 11a, 12a is not heightened at the connection part 13 so that snaking is reduced. In this way, generation provability on snaking is lowered so as to stabilize discharge.

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は、放電路を逆U字形等に曲げる曲げ部を有する
蛍光ランプに係り、特に、曲げ部を改良した蛍光ランプ
に関する。
[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention relates to a fluorescent lamp having a bent portion that bends a discharge path into an inverted U-shape or the like, and particularly relates to a fluorescent lamp with an improved bent portion. Regarding.

(従来の技術) 従息、この種の逆U字形蛍光ランプとしては第3図およ
び第4図に示すものが知られており、第3図で示す蛍光
ランプ1は例えば2本のガラス製′直状バルブ2a、2
bの雨上端部の対向面同士を、例えば、いわゆるバーナ
吹き破り等により、連結部2Cを介して一体に連結し、
全体を逆U字状に形成している。
(Prior Art) As this type of inverted U-shaped fluorescent lamp, those shown in FIGS. 3 and 4 are known, and the fluorescent lamp 1 shown in FIG. Straight valve 2a, 2
The opposing surfaces of the rain upper ends of b are integrally connected via the connecting part 2C, for example, by so-called burner blow-out, etc.
The entire structure is shaped like an inverted U.

蛍光ランプ1は、その逆U字状両端部に一対の電極3a
、3bを封止すると共に、その内周面に蛍光膜を被着し
、その内部には水銀と希ガスとを封入している。
The fluorescent lamp 1 has a pair of electrodes 3a at both ends of the inverted U-shape.
, 3b are sealed, and a fluorescent film is attached to the inner peripheral surface thereof, and mercury and rare gas are sealed inside.

一方、第4図で示す逆U字形の蛍光ランプ4は、例えば
2本の直状ガラス製バルブ5.6の図中上端部を金属製
のメタルキャップ7により連通自在に固着することによ
り、全体を逆U字状に構成している。
On the other hand, the inverted U-shaped fluorescent lamp 4 shown in FIG. is configured in an inverted U shape.

これら両バルブ5.6の図中各下端部には左右一対の電
極ga、8bをそれぞれ気密に封止している。
A pair of left and right electrodes ga and 8b are hermetically sealed at the lower ends of both valves 5.6 in the figure.

また、両バルブ5.6はその内周面に蛍光膜をほぼ全長
に亘って被着すると共に、水銀と希ガスを封入している
Further, both bulbs 5.6 have a fluorescent film coated on their inner peripheral surfaces over almost the entire length, and are filled with mercury and a rare gas.

(発明が解決しようとする課題) しかしながら、このような従来の蛍光ランプ1.4では
それらのバルブ2a、  2b、  5. 6の横断面
形状が長円形等の偏平形状に形成されており、しかも、
それらの逆U字状曲げ部2d、4aの内径が各ガラスバ
ルブ2a、  2b、  5.6の各内径よりも小径に
縮径されているので、これら蛍光ランプ1,4を高電流
域で点灯すると、これら曲げ部2d、4aにおいて、陽
光柱があたかもうねるような、いわゆるスネーキングが
発生し、放電を不安定にする。
(Problems to be Solved by the Invention) However, in such a conventional fluorescent lamp 1.4, the bulbs 2a, 2b, 5. The cross-sectional shape of 6 is formed into a flat shape such as an ellipse, and furthermore,
Since the inner diameters of these inverted U-shaped bent portions 2d and 4a are smaller than the inner diameters of the respective glass bulbs 2a, 2b, and 5.6, these fluorescent lamps 1 and 4 can be lit in a high current range. Then, in these bent portions 2d and 4a, so-called "snaking" occurs in which the positive column appears to undulate, making the discharge unstable.

このスネーキングが発生すると、光束に著しい時間的、
空間的不均一が生じる。
When this snaking occurs, there is a significant temporal change in the luminous flux.
Spatial non-uniformity occurs.

そこで本発明は前記事情を考慮してなされたもので、そ
の目的は陽光柱のスネーキングを防止し、その光束を安
定化することができる蛍光ランプを提供することにある
The present invention has been made in consideration of the above circumstances, and its object is to provide a fluorescent lamp capable of preventing snaking of the positive column and stabilizing its luminous flux.

〔発明の構成〕[Structure of the invention]

(課題を解決するための手段) まず、本発明者等はこのスネーキング現象の発生メカニ
ズムを前記蛍光ランプlについて解析じた。
(Means for Solving the Problems) First, the inventors analyzed the mechanism of occurrence of this snaking phenomenon for the fluorescent lamp I.

その結果、このスネーキング現象は偏平バルブに多く発
生し、そのランプ製造時の不純物濃度に比例し、かつ放
電の電子密度のほぼ二乗に比例して発生し易いという知
見を得た。
As a result, it was found that this snaking phenomenon occurs more often in flat bulbs, and that it is more likely to occur in proportion to the impurity concentration at the time of manufacturing the lamp, and approximately in proportion to the square of the electron density of the discharge.

すなわち、第3図で示す蛍光ランプ1の連通部2Cにお
いて、放電電子密度が増加すると、この部分からスネー
キングが発生する確率が高くなる。
That is, when the discharge electron density increases in the communication portion 2C of the fluorescent lamp 1 shown in FIG. 3, the probability that snaking will occur from this portion increases.

本発明者等の実験によれば、偏平断面積を有するバルブ
2の直状部2a、2bの断面積に対する連通部2cの断
面積の比とスネーキング発生確率は次表のような関係を
有する。
According to experiments conducted by the present inventors, the ratio of the cross-sectional area of the communicating portion 2c to the cross-sectional area of the straight portions 2a and 2b of the bulb 2 having a flat cross-sectional area and the probability of occurrence of snaking have a relationship as shown in the following table.

この表1中、スネーキング発生確率が例えば5%とは、
連結部2cの直状部2a、2bに対する断面積比が20
%の蛍光ランプ1を仮に100本製造したときに、一定
の明るさ(例えば電子密度5X1017個/n’ )で
点灯したときに、5本の蛍光ランプ1にスネーキング現
象が発生したことを示す。
In Table 1, if the probability of occurrence of snaking is, for example, 5%,
The cross-sectional area ratio of the connecting portion 2c to the straight portions 2a and 2b is 20.
This shows that when 100 % fluorescent lamps 1 were manufactured and they were lit at a constant brightness (for example, electron density 5×10 17 /n'), a snaking phenomenon occurred in 5 fluorescent lamps 1.

したがって、この表1によれば、連通部2Cの横断面積
の直状部2a、2bの横断面積に対する比を増大させる
ことにより、スネーキングを低減することができる。
Therefore, according to Table 1, snaking can be reduced by increasing the ratio of the cross-sectional area of the communicating portion 2C to the cross-sectional area of the straight portions 2a and 2b.

また、曲げ部2dでは放電が最短経路を通るために曲げ
内周部側へ偏位し、内周部側のUV(紫外線)強度を外
周側よりも高め、内、外周部で明度差を発生させる。
In addition, in the bent part 2d, the discharge takes the shortest path, so it deviates toward the inner circumference of the bend, making the UV (ultraviolet ray) intensity on the inner circumference higher than on the outer circumference, creating a difference in brightness between the inner and outer circumference. let

そこで、この曲げ部2dの中心軸をその曲げ外周部側へ
若干偏位させることにより、陽光柱が曲げ内周部側へ偏
位するのを防止し、内外周部での明度差を均等化するこ
とができる。
Therefore, by slightly deviating the central axis of the bent portion 2d toward the outer circumference of the bend, the positive column is prevented from shifting toward the inner circumference of the bend, and the difference in brightness between the inner and outer circumferences is equalized. can do.

そのために、本発明は、曲げ部2dの連通部2Cの横断
面積の拡大を図ると共に、その横断面形の重心を曲げ部
2dの外周部側へ若干移動させるように形成した。
To this end, in the present invention, the cross-sectional area of the communicating portion 2C of the bent portion 2d is expanded, and the center of gravity of the cross-sectional shape is slightly moved toward the outer peripheral portion of the bent portion 2d.

すなわち本発明は、次のように構成される。That is, the present invention is configured as follows.

偏平状のバルブにより放電路が直状に規制される直状部
と、その直状放電路を曲げる曲げ部とを有する蛍光ラン
プにおいて、前記曲げ部は、その横断面形状を偏平形状
に形成すると共に、その偏平形の最大径を前記直状部の
偏平横断面の最小径よりも長くしてなることを特徴とす
る。
In a fluorescent lamp having a straight portion in which a discharge path is regulated to be straight by a flat bulb, and a bent portion that bends the straight discharge path, the bent portion has a cross-sectional shape formed in a flat shape. Further, it is characterized in that the maximum diameter of the flat shape is longer than the minimum diameter of the flat cross section of the straight portion.

(作用) 本発明の蛍光ランプの曲げ部は、その横断面形状を偏平
形状に形成すると共に、その偏平形の最大径を前記直状
部の偏平横断面の最小径よりも長くしたので、バルブの
直状部の横断面積に対する曲げ部の横断面積の比が増大
する。
(Function) The bent portion of the fluorescent lamp of the present invention has a flat cross-sectional shape, and the maximum diameter of the flat shape is longer than the minimum diameter of the flat cross-section of the straight portion. The ratio of the cross-sectional area of the bent portion to the cross-sectional area of the straight portion increases.

したがって本発明によれば、表1より明らかなように曲
げ部における放電時のスネーキングの低減を図ることが
でき、光束の安定化を図ることができる。
Therefore, according to the present invention, as is clear from Table 1, it is possible to reduce snaking during discharge at the bent portion, and it is possible to stabilize the luminous flux.

(実施例) 以下本発明の実施例を第1図および第2図に基づいて説
明する。
(Example) An example of the present invention will be described below based on FIGS. 1 and 2.

第2図は本発明の一実施例の全体構成を示す一部切欠正
面図であり、図において、本実施例の蛍光ランプ10は
例えば2本のガラス製直状バルブ11.12の図中上端
部同士を連結部13により一体に連結することにより、
全体をほぼ逆U字状に形成している。
FIG. 2 is a partially cutaway front view showing the overall configuration of an embodiment of the present invention. By connecting the parts together by the connecting part 13,
The entire structure is shaped like an inverted U.

各直状バルブ11.12はその図中下端部に左右一対の
電極14 a、  14 bをそれぞれ気密に封止し、
その電極封止端をピンチシール15a、15bによりシ
ールしている。
Each straight valve 11.12 has a pair of left and right electrodes 14a, 14b hermetically sealed at its lower end in the figure.
The electrode sealed ends are sealed with pinch seals 15a and 15b.

両バルブ11.12および連結部13はその内周面に図
示しない蛍光膜をほぼ全面的にかつほぼ全長に被着して
おり、その内部に水銀と希ガスとを封入している。
Both bulbs 11, 12 and the connecting portion 13 have a fluorescent film (not shown) coated on their inner peripheral surfaces almost entirely and over almost their entire length, and mercury and rare gas are sealed inside.

連結部13は例えばバーナ吹き破りにより形成される。The connecting portion 13 is formed, for example, by blowing out a burner.

これは並設した両バルブ11.12の図中上端部対向面
をバーナ炎により加熱軟化させてから、一対の電極14
a、14bを封止する前に、図中下端開口より所定圧の
エアを吹き込み、これら加熱軟化部のガラス壁を吹き破
る。
This is done by heating and softening the opposing surfaces of the upper ends of both bulbs 11 and 12 in the figure, which are arranged in parallel, using a burner flame, and then connecting the pair of electrodes 14.
Before sealing parts a and 14b, air at a predetermined pressure is blown from the opening at the lower end in the figure to blow out the glass walls of these heat-softened parts.

この吹き破りにより開口した開口周縁部には両バルブ1
1.12の対向方向にそれぞれ若干突出する円筒状の突
出壁が形成される。
Both valves 1 are attached to the periphery of the opening opened by this blow-out
1. Cylindrical protruding walls are formed that protrude slightly in opposite directions.

そこで、この両突出壁同士を突き合せて融着し、さらに
この融着箇所とその周辺部をバーナ炎により再び加熱し
てアニールし、この加熱軟化部を金型内に挿入して、各
バルブ11.12内に所定圧のエアを吹き込むことによ
りモールド成型する。
Therefore, these two protruding walls are butted together and fused together, and the fused area and its surrounding area are heated again with a burner flame to anneal, and this heated and softened part is inserted into the mold to form each valve. 11. Molding is carried out by blowing air at a predetermined pressure into 12.

この成型により、連結部13およびその前後のバルブ1
1.12の曲げ部16の肉厚を殆ど均等化し、歪みを低
減し、機械的強度を高めることができる。
By this molding, the connecting part 13 and the valve 1 before and after it
The thickness of the bent portion 16 of 1.12 can be made almost equal, distortion can be reduced, and mechanical strength can be increased.

このようにして蛍光ランプ10は直状のバルブ11.1
2内に形成される直状放電路をほぼ逆U字状に曲げる曲
げ部16を一体に形成することができる。
In this way, the fluorescent lamp 10 is constructed using a straight bulb 11.1.
A bending portion 16 that bends the straight discharge path formed in the discharge path 2 into a substantially inverted U shape can be integrally formed.

そして、各直状バルブ11.12の直状部11a、12
aの横断面は第1図(A)に示すように例えば長円形の
偏平形状に形成され、例えば、最小径である短径Sが8
11II111最大径である長径lが20m+aにそれ
ぞれ設定され、短径/長径の偏平度が0.4に形成され
ている。
and the straight portions 11a, 12 of each straight valve 11.12.
The cross section of a is formed, for example, in an elliptical flat shape as shown in FIG.
The long axis l, which is the maximum diameter of 11II111, is set to 20 m+a, and the flatness of the short axis/long axis is 0.4.

また、この偏平横断面の重心軸Oaには陽光柱が通る放
電路が形成される。
Further, a discharge path through which a positive column passes is formed at the center of gravity axis Oa of this flat cross section.

一方、連結部13の横断面は第1図(B)に示すように
、例えばほぼ扇形に形成され、その最大径である長径i
oが10mmで、扇形中心角17゜に形成されており、
この長径to 10は直状部11a、12aの横断面形
状の短径58mmより長く設定されている。
On the other hand, as shown in FIG. 1(B), the cross section of the connecting portion 13 is formed, for example, in a substantially fan shape, with the major axis i being the maximum diameter.
o is 10 mm, it is formed with a fan-shaped center angle of 17 degrees,
The major axis to 10 is set longer than the minor axis 58 mm of the cross-sectional shape of the straight portions 11a and 12a.

そして、この連結部13の横断面積は直状部11a、1
2aの横断面積に対して約70%を占めており、前記表
1より明らかなように連結部13におけるスネーキング
発生確率は約0.1%以下に低減された。
The cross-sectional area of this connecting portion 13 is the straight portion 11a, 1
It occupies about 70% of the cross-sectional area of 2a, and as is clear from Table 1, the probability of occurrence of snaking in the connecting portion 13 has been reduced to about 0.1% or less.

すなわち、各直状部11a、12aを通ってきた陽光柱
の電子密度が連結部13にて著しく高まらないので、ス
ネーキングを著しく低減することができる。
That is, since the electron density of the positive column that has passed through each of the straight portions 11a and 12a does not increase significantly at the connecting portion 13, it is possible to significantly reduce snaking.

また、第1図(B)に示すように連結部13の横断面形
状を扇形に形成したので、その重心軸Obが曲げ部16
の内周部d側からその外周部U側へ寄るように偏心させ
ることができ、この重心軸Obに沿って通る陽光柱の放
電路を扇形のほぼ重心部に位置させることができる。
Further, as shown in FIG. 1(B), since the cross-sectional shape of the connecting portion 13 is fan-shaped, the center axis Ob of the connecting portion 13 is aligned with the bent portion 16.
can be eccentrically moved from the inner peripheral part d side to the outer peripheral part U side, and the discharge path of the positive column passing along the center axis Ob can be located almost at the center of gravity of the sector.

そのために、陽光柱が連結部13において曲げ内周部d
側へ寄って、その内周部d側の明るさを外周部U側より
も高め、内、外周部d、  uで明度差が発生するのを
防止し、明るさの均等化を図ることができる。
For this reason, the positive pillar is bent at the inner circumferential portion d at the connecting portion 13.
By moving closer to the side, the brightness on the inner periphery d side is made higher than on the outer periphery U side, preventing a difference in brightness from occurring between the inner and outer periphery parts d and u, and equalizing the brightness. can.

しかしながら、このような放電路の偏りは封入ガス圧や
放電電流にも依存するので、本発明では必ずしも連結部
13の横断面形状を扇形に限定するものではなく、連結
部13の横断面積を直状部11a、12aの横断面積に
対して極端に小さくならなように面積比を拡大し、直状
部11a、12aと曲げ部16の放電電子密度の差を低
減するものであればよい。
However, since the deviation of such a discharge path also depends on the pressure of the filled gas and the discharge current, the present invention does not necessarily limit the cross-sectional shape of the connecting portion 13 to a fan shape, but rather the cross-sectional area of the connecting portion 13 is directly It is sufficient that the area ratio is increased so as not to be extremely small with respect to the cross-sectional area of the shaped portions 11a, 12a, and the difference in discharge electron density between the straight portions 11a, 12a and the bent portion 16 is reduced.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、蛍光ランプの曲げ部の横
断面形状を偏平形状に形成すると共に、その偏平形の最
大径を前記直状部の偏平横断面の最小径よりも長くした
ので、放電路直状部における横断面積に対する放電路曲
げ部の横断面積の比が増大する。
As explained above, in the present invention, the cross-sectional shape of the bent portion of the fluorescent lamp is formed into a flat shape, and the maximum diameter of the flat shape is made longer than the minimum diameter of the flat cross-section of the straight portion. The ratio of the cross-sectional area of the bent portion of the discharge path to the cross-sectional area of the straight portion of the discharge path increases.

したがって本発明によれば、この曲げ部と直状部におけ
る放電電子密度の差を縮小することができ、曲げ部のス
ネーキング発生確率を低減し、放電を安定させることが
できる。
Therefore, according to the present invention, the difference in discharge electron density between the bent portion and the straight portion can be reduced, the probability of occurrence of snaking in the bent portion can be reduced, and the discharge can be stabilized.

その結果、蛍光ランプの発光が安定する。As a result, the luminescence of the fluorescent lamp becomes stable.

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

第1図(A)は第2図で示す本発明に係る蛍光ランプの
一実施例の放電路直状部の横断面を示す横断面図、第1
図(B)は第2図で示す連結部の横断面を示す横断面図
、第2図は本発明に係る蛍光ランプの一実施例の一部切
欠正面図、第3図および第4図は従来の逆U字状蛍光ラ
ンプの構成図である。 10・・・蛍光ランプ、11.12・・・バルブ、11
’a、12a・・・直状部、13・・・連結部、16・
・・曲げ部、Oa、Ob・・・中心軸、p、IO・・・
長径(最大径)、S・・・短径(最小径)。
FIG. 1(A) is a cross-sectional view showing a cross section of a straight portion of a discharge path of an embodiment of the fluorescent lamp according to the present invention shown in FIG.
Figure (B) is a cross-sectional view showing the cross section of the connecting part shown in Figure 2, Figure 2 is a partially cutaway front view of an embodiment of the fluorescent lamp according to the present invention, and Figures 3 and 4 are FIG. 1 is a configuration diagram of a conventional inverted U-shaped fluorescent lamp. 10...Fluorescent lamp, 11.12...Bulb, 11
'a, 12a... straight part, 13... connecting part, 16.
...Bending part, Oa, Ob... Central axis, p, IO...
Long axis (maximum diameter), S... short axis (minimum diameter).

Claims (1)

【特許請求の範囲】[Claims] 偏平状のバルブにより放電路が直状に規制される直状部
と、その直状放電路を曲げる曲げ部とを有する蛍光ラン
プにおいて、前記曲げ部は、その横断面形状を偏平形状
に形成すると共に、その偏平形の最大径を前記直状部の
偏平横断面の最小径よりも長くしてなることを特徴とす
る蛍光ランプ。
In a fluorescent lamp having a straight portion in which a discharge path is regulated to be straight by a flat bulb, and a bent portion that bends the straight discharge path, the bent portion has a cross-sectional shape formed in a flat shape. Further, a fluorescent lamp characterized in that the maximum diameter of the flat shape is longer than the minimum diameter of the flat cross section of the straight portion.
JP22156389A 1989-08-30 1989-08-30 Fluorescent lamp Pending JPH0388256A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22156389A JPH0388256A (en) 1989-08-30 1989-08-30 Fluorescent lamp

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22156389A JPH0388256A (en) 1989-08-30 1989-08-30 Fluorescent lamp

Publications (1)

Publication Number Publication Date
JPH0388256A true JPH0388256A (en) 1991-04-12

Family

ID=16768691

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22156389A Pending JPH0388256A (en) 1989-08-30 1989-08-30 Fluorescent lamp

Country Status (1)

Country Link
JP (1) JPH0388256A (en)

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