JPH01225058A - Fluorescent lamp - Google Patents

Fluorescent lamp

Info

Publication number
JPH01225058A
JPH01225058A JP4973788A JP4973788A JPH01225058A JP H01225058 A JPH01225058 A JP H01225058A JP 4973788 A JP4973788 A JP 4973788A JP 4973788 A JP4973788 A JP 4973788A JP H01225058 A JPH01225058 A JP H01225058A
Authority
JP
Japan
Prior art keywords
tube wall
starting gas
anode
flickering
argon
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
JP4973788A
Other languages
Japanese (ja)
Inventor
Naoyuki Toda
尚之 戸田
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
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 filed Critical Toshiba Corp
Priority to JP4973788A priority Critical patent/JPH01225058A/en
Publication of JPH01225058A publication Critical patent/JPH01225058A/en
Pending legal-status Critical Current

Links

Landscapes

  • Discharge Lamps And Accessories Thereof (AREA)

Abstract

PURPOSE:To obtain almost no flickering of light, little blackening of a tube wall and a long life by fitting a main electrode constituted of a triple coil and an auxiliary anode, sealing the specific starting gas in a bulb, and operating a lamp under the specific tube wall load. CONSTITUTION:A main electrode 5 constituted of a triple coil and an auxiliary anode 6 are fitted to both ends of a glass bulb 1, the starting gas consisting of argon 90% or above and the remainder of neon is sealed in the bulb 1 at the pressure of 1.7-2.0Torr, the lamp is operated under the tube wall load of 500W/m<2> or above. The luminous efficiency is improved by decreasing the sealing pressure of the starting gas, the ion shock is mitigated by combining neon with small specific gravity with argon as the starting gas. The electrode is constituted of the triple coil to easily improve the electrode load and mitigate the anode vibration, the flickering of brightness resulting from the improvement of the electrode load and the decrease of the sealing pressure and the ion shock and anode vibration are further mitigated by providing the auxiliary anode. The early blackening and flickering of light can be thereby prevented.

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は明るさを向上しかつ光のちらつきと黒化を減少
して長寿命にした蛍光ランプに関し、特に高管壁負荷の
ランプに好適なものである。
[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention relates to a fluorescent lamp that has improved brightness and reduced flickering and blackening of the light to extend its life. It is suitable for load lamps.

(従来の技術) 従来の高効率蛍光ランプはガラスバルブの両端部にトリ
プルコイルからなる電極を封装し、かつ純アルゴンから
なる始動ガスを2.2Torr以上の圧力で適量の水銀
とともに封入したものである。
(Prior art) Conventional high-efficiency fluorescent lamps have electrodes made of triple coils sealed at both ends of a glass bulb, and a starting gas made of pure argon is sealed together with an appropriate amount of mercury at a pressure of 2.2 Torr or more. be.

(発明が解決しようとする課題) 近年、より明るく、より高効率のランプが要求されるに
到った。これに対し、始動ガスの封入ガス圧を低くして
発光効率を向上することが考えられるが、始動ガスの封
入圧力をあまり低くすると種々の不都合が発生するよう
になる。また、トリプルコイル電極の陽極振動抑制効果
にも限界がある。
(Problems to be Solved by the Invention) In recent years, there has been a demand for brighter and more efficient lamps. On the other hand, it is possible to improve the luminous efficiency by lowering the charging gas pressure of the starting gas, but if the charging pressure of the starting gas is too low, various problems will occur. Furthermore, there is a limit to the anode vibration suppressing effect of the triple coil electrode.

たとえば、始動ガスの封入圧力が2.0Torrを下回
ると電極に対するイオン衝撃が増大し、スパッタリング
が増大して早期黒化の原因になり、また、明るさのちら
つきが増大する。さらに、封入ガス圧が1.7Torr
を下回ると、上述の不都合に加えて、電子温度の上昇に
伴う波長185nmの遠赤外線の放射量が増大して蛍光
体の劣化を速くする欠点が生じ、さらに発光効率が低下
する。特にこの欠点は管壁負荷500W/rrr以上で
動作させた場合に著しい。
For example, if the starting gas fill pressure is below 2.0 Torr, ion bombardment against the electrodes will increase, sputtering will increase, causing early blackening, and brightness flickering will increase. Furthermore, the sealed gas pressure is 1.7 Torr.
If it falls below this, in addition to the above-mentioned disadvantages, the amount of far-infrared radiation with a wavelength of 185 nm increases as the electron temperature rises, resulting in the disadvantage of accelerating the deterioration of the phosphor and further reducing the luminous efficiency. This drawback is particularly noticeable when operating at a tube wall load of 500 W/rrr or more.

そこで、従来、封入ガス圧の下限は2 Torrが限界
とされ、これより高く維持していた。
Therefore, conventionally, the lower limit of the sealed gas pressure has been set at 2 Torr, and has been maintained higher than this.

本発明の課題は従来の常識を破って封入ガス圧を2 T
orr未満として明るくし、しかも早期黒化や光のちら
つきがなく、特に500W/新以上の高管壁負荷で動作
させるに適した蛍光ランプを提供することにある。
The problem of the present invention is to break the conventional wisdom and increase the sealed gas pressure to 2 T.
It is an object of the present invention to provide a fluorescent lamp which is bright as less than orr, has no early blackening or flickering of light, and is particularly suitable for operation at a high tube wall load of 500 W/new or more.

〔発明の構成〕[Structure of the invention]

(課題を解決するための手段) 本発明は明るさを向上しかつ光のちらつきを防止すると
ともに黒化を減少した高管壁負荷の蛍光ランプを提供す
るもので、ガラスバルブの両端部にトリプルコイルから
なる主電極および補助陽極を封装し、バルブ内にアルゴ
ンが90%以上で残部がネオンからなる始動ガスを1 
、7Torr以上2.0Torr以下の圧力で封入し5
00W/rrf以上の管壁負荷で動作させたことにより
、上記課題を解決したものである。
(Means for Solving the Problems) The present invention provides a fluorescent lamp with a high tube wall load that improves brightness, prevents light flickering, and reduces blackening. The main electrode and auxiliary anode consisting of a coil are sealed, and a starting gas consisting of 90% or more argon and the remainder neon is added to the bulb.
, sealed at a pressure of 7 Torr or more and 2.0 Torr or less5
The above problem was solved by operating with a tube wall load of 00 W/rrf or more.

(作用) 始動ガスの封入圧力を下げることによって発光効率を向
上し、封入圧力引下げに伴うイオン衝撃の増大は始動ガ
スとしてアルゴンに比重の小さいネオンを配合したこと
によってイオン衝撃を軽減し、さらに電極負荷の向上を
容易にしかつ陽極振動を軽減するための電極をトリプル
コイルで構成し、電極負荷の向上と封入圧力引下げに伴
う明るさのちらつきは補助陽極を設けたことによってイ
オン衝撃と陽極振動とを一層軽減して解決するものであ
る。そうして、本発明は以上の諸要素を適当に総合し、
組合せたことにより、上述の課題を解決し、しかもこれ
に伴う欠点が生じないようにした。さらに、このように
構成された蛍光ランプは高管壁負荷で点灯して特に明る
い効果が得られ、しかもこれによる欠点がほとんど見ら
れない利点がある。
(Function) Luminous efficiency is improved by lowering the charging pressure of the starting gas, and the increase in ion bombardment caused by lowering the charging pressure is reduced by blending neon with a small specific gravity with argon as the starting gas. In order to easily increase the load and reduce anode vibration, the electrode is configured with a triple coil, and the flickering of brightness that occurs due to the increase in electrode load and the reduction of the sealing pressure is reduced by installing an auxiliary anode, which reduces ion bombardment and anode vibration. This is to further reduce and solve the problem. Thus, the present invention appropriately integrates the above elements,
By combining the two, the above-mentioned problems are solved, and the drawbacks associated therewith are not caused. Furthermore, a fluorescent lamp constructed in this way has the advantage that it can be operated with a high tube wall load and a particularly bright effect is obtained, and the disadvantages caused by this are hardly noticeable.

(実施例) 本発明の詳細を図示の実施例によって説明する。(Example) The details of the invention will be explained by means of illustrated embodiments.

(1)は直管形ガラスバルブ、■はこのバルブ■の内面
に形成された蛍光膜、■、■はバルブ(Dの両端を閉塞
したステム、(イ)、(イ)・・・はこのステム■、■
を貫通してバルブ(1)内に導入されたそれぞれ1対の
内導線、■、0はこれら対をなす内導線に)、(イ)・
・・間に装架された主電極、(へ)、■・・・は内導線
(イ)。
(1) is a straight glass bulb, ■ is a fluorescent film formed on the inner surface of this bulb ■, ■, ■ is a stem with both ends of the bulb (D closed), (a), (b)... are this Stem■,■
A pair of inner conducting wires are introduced into the valve (1) through the .
...The main electrode installed between (b), ■... is the inner conductor wire (a).

(へ)・・・のそれぞれに設けられて主電極0,0ごと
にその前方に突出した補助陽極、■、■はバルブ■の両
端に設けられて内導線に)、に)・・・に接続する1対
の口金である。そうして、バルブω内に始動ガスとして
アルゴンが90容量%以上で残部がネオンからなる希ガ
スと適量の水銀またはアマルガムを封入しである。
Auxiliary anodes are provided at each of the main electrodes 0 and 0 and protrude in front of the main electrodes 0 and 0, and auxiliary anodes are provided at both ends of the bulb ■ and connected to the inner conductor wires), ni)... This is a pair of caps that are connected. Then, as a starting gas, a rare gas consisting of 90% by volume or more of argon and the remainder neon, and an appropriate amount of mercury or amalgam are sealed in the valve ω.

上記主電極■は通電用のタングステン素線に一層マンド
リルを沿わせてこれにタングステン細線を巻回して一層
コイルに巻成し、ついでこの−次コイルを二次マンドリ
ルに巻回してトリプルコイルに巻成し、切断して焼鈍し
てから両マンドリルを溶解除去してなるトリプルコイル
フィラメントを内導線(イ)、(イ)間に装架し、これ
にアルカリ土類金属酸化物からなる電子放射性物質を被
着してなる。
The above main electrode (■) is made by placing a mandrill along one layer of tungsten wire for current-carrying, and winding a thin tungsten wire around this to form a single layer coil, and then winding this secondary coil around a secondary mandrel to form a triple coil. A triple coil filament made by cutting, annealing, and then dissolving and removing both mandrils is installed between the inner conductors (A) and (A), and an electron radioactive material made of an alkaline earth metal oxide is attached to this triple coil filament. It becomes covered with.

上記補助陽極0はタングステン線、モリブデン線などの
高融点金属からなる線材をほぼL字形に成形し、内導線
(イ)に導電的に固着し、その先端を主電極0よりも前
方に突出させたもので、本実施例では主電極0ごとに2
個設けられている。
The above-mentioned auxiliary anode 0 is formed by forming a wire made of a high-melting point metal such as a tungsten wire or a molybdenum wire into a nearly L-shape, and conductively fixing it to the inner conductor wire (A), with its tip protruding forward from the main electrode 0. In this example, for each main electrode 0, 2
There are several.

つぎに、この実施例蛍光ランプの作用を説明する。この
実施例蛍光ランプは管壁負荷がたとえば810W/rr
l’で動作するように定められている。いま、始動して
主電極(ハ)、0間に放電させると、電子放射は総て主
電極0,0が負担し、イオン流入は補助陽極0,0・・
・が主となり、主電極0,0が従となる。この結果、主
電極■のイオン流入に伴う衝撃が小さくなって、アノー
ドスポットが小さくなるとともにスパッタリングが少な
くなりかつ陽極振動がほとんどなくなる。この結果、明
るさのちらつきがほとんど感じられなくなり、また管壁
黒化が激減した。また、本実施例蛍光ランプは封入ガス
圧が1.7〜2.0Torrと小さいので、発光効率が
増大して明るくなったが、その反面イオン衝撃が大きく
なるはずであったが、始動ガスとしてアルゴンにネオン
を若干配合したことと、補助陽極を設けたこととによっ
てイオン衝撃が小さくなり、やはり明るさのちらつきと
管壁黒化が減少した。
Next, the operation of the fluorescent lamp of this embodiment will be explained. The fluorescent lamp of this embodiment has a tube wall load of, for example, 810 W/rr.
It is specified to operate at l'. Now, when starting and discharging between the main electrodes (c) and 0, the main electrodes 0, 0 will bear all the electron emission, and the ion inflow will be carried out by the auxiliary anodes 0, 0...
* is the main electrode, and main electrodes 0 and 0 are the subordinate electrodes. As a result, the impact accompanying the influx of ions into the main electrode (2) becomes smaller, the anode spot becomes smaller, sputtering is reduced, and anode vibration is almost eliminated. As a result, flickering in brightness was almost no longer perceptible, and darkening of the tube wall was drastically reduced. In addition, the fluorescent lamp of this example had a small filler gas pressure of 1.7 to 2.0 Torr, so the luminous efficiency increased and it became brighter, but on the other hand, the ion bombardment was supposed to be large, but the starting gas The addition of a small amount of neon to the argon and the provision of an auxiliary anode reduced ion bombardment, which also reduced brightness flickering and tube wall blackening.

このように、本実施例蛍光ランプは封入ガス圧を下げた
ことと管壁負荷を増大させた結果得られる明るさの増大
は予定通り享受し、その欠点である明るさのちらつきと
管壁黒化は始動ガスにネオンを配合することと補助陽極
を設けたこととによりほとんど回避できた。
In this way, the fluorescent lamp of this example enjoys the expected increase in brightness resulting from lowering the filler gas pressure and increasing the load on the tube wall. Most of these problems could be avoided by adding neon to the starting gas and providing an auxiliary anode.

また、管壁負荷が500W/m未満のものについては、
アルゴンが90容量%の前後で明るさはあまり変化しな
い。また、同様に500W/rrF未満では封入ガス圧
が1.7〜2.0Torrの範囲の内外で明るさや黒化
があまり変化しない。すなわち、管壁負荷500W/n
−F以上において、アルゴンの容量比および封入ガス圧
が明るさや黒化に対して臨界的に影響してくることが解
った。
In addition, for pipe wall loads of less than 500 W/m,
The brightness does not change much when argon is around 90% by volume. Similarly, when the gas pressure is less than 500 W/rrF, the brightness and blackening do not change much within the range of 1.7 to 2.0 Torr. That is, the tube wall load is 500W/n
It was found that at temperatures above -F, the argon volume ratio and the sealed gas pressure have a critical effect on brightness and blackening.

つぎに、本実施例蛍光ランプを上述の管壁負荷807.
1W/nfで点灯した場合と従来の補助陽極を有せず純
アルゴンを2.4Torrで封入して通常の管壁負荷7
g3.6W/n(で点灯した場合とで動程特性を比較し
た。この結果を第2図に示す。図は横軸に点灯時間をH
rの単位でとり、縦軸に全光束を両者共通の相対値でと
ったものである。この図から明らかなように、本実施例
のものは全光束値が0〜1000時間の範囲において従
来よりはるかに大きく、しかも1000時間以後におい
ても従来例より劣ることがない。
Next, the fluorescent lamp of this embodiment is subjected to the above-mentioned tube wall load 807.
When lit at 1W/nf and when pure argon is filled at 2.4 Torr without a conventional auxiliary anode, the normal tube wall load is 7.
The travel characteristics were compared with the case of lighting at 3.6 W/n (H).The results are shown in Figure 2.
It is taken in units of r, and the vertical axis shows the total luminous flux as a relative value common to both. As is clear from this figure, the total luminous flux value of this example is much larger than that of the conventional example in the range from 0 to 1000 hours, and is not inferior to the conventional example even after 1000 hours.

つぎに、本実施例蛍光ランプにつき封入した始動ガス組
成とその圧力とを異ならせてその黒化状態を調査し、こ
の結果を上記従来例と比較した。
Next, the composition and pressure of the starting gas sealed in the fluorescent lamp of this example were varied to investigate the blackening state, and the results were compared with the above-mentioned conventional example.

黒化の評価は黒化の全く認められないものを10点とし
、ランプ管端部全周にわたり甚だしく黒化したものを1
点とし、その間を視感により10段階評価し得点を与え
た。この結果を層表に示す。
For evaluation of blackening, a score of 10 is given for no blackening at all, and a score of 1 is given for a case where there is severe blackening all around the end of the lamp tube.
points, and the points between them were evaluated on a 10-point scale based on visual perception. The results are shown in the layer table.

(以下余白) 注.■ 表中ASはアノードスポットの略■ 表中EB
はエンドバンドの略 ■ 表中Mはランプのマーク側の端部の略■ 表中NM
はランプのマークのない側の端部の略(ハ)蛍光ランプ
はバルブの片端だけにランプマークを打刻しであるため
、管端の一方を指定するどき■,Q)のような表現をす
る。
(Left below) Note. ■ AS in the table stands for anode spot ■ EB in the table
is an abbreviation for end band ■ M in the table is an abbreviation for the end of the lamp on the mark side ■ NM in the table
stands for the unmarked end of the lamp (c) Fluorescent lamps have a lamp mark engraved on only one end of the bulb, so when specifying one end of the tube, expressions such as ■, Q) are used. do.

この表から明らかなとおり、封入ガス圧が1.8Tor
rのものは総て従来例より黒化状態が良く、また、2.
2Torrのものは1 、8Torrのものと同程度で
ある。これに対し、封入ガス圧が1 、2Torrのも
のは総て従来より黒化状態が悪かった。また、アルゴン
90〜100容量%の範囲で良かった。
As is clear from this table, the sealed gas pressure is 1.8 Torr.
The blackening state of all the products of r is better than that of the conventional example, and 2.
The value of 2 Torr is comparable to that of 1 and 8 Torr. On the other hand, in all cases where the filled gas pressure was 1 or 2 Torr, the blackening state was worse than in the conventional case. Further, the argon content was preferably in the range of 90 to 100% by volume.

なお、引続いての実験において、封入ガス圧が2.2T
orrのものは1.8Torrのものより明るさが劣っ
た。さらに、番号1〜9のものは総て光のちらつきがな
かった。これは上記1〜9のものがいずれも主電極にト
リプルコイルを採用し、かつ補助陽極を設けたためと考
えられる。トリプルコイルはその構造上陽極振動が停止
するが、その停止状態が一時的で、その後陽極振動発生
の過渡期においてランプ放電電流の変動が補助陽極によ
って防止され、この結果、ちらつきがほぼ完全に防止さ
れたものと考える。
In addition, in the subsequent experiment, the sealed gas pressure was 2.2T.
The one with orr was inferior in brightness than the one with 1.8 Torr. Furthermore, all of the samples with numbers 1 to 9 had no flicker of light. This is thought to be because all of the above-mentioned samples 1 to 9 adopted a triple coil as the main electrode and were provided with an auxiliary anode. Due to the structure of the triple coil, the anode vibration stops, but this stop state is temporary, and the auxiliary anode prevents fluctuations in the lamp discharge current during the transition period when the anode vibration occurs, and as a result, flickering is almost completely prevented. I think it was done.

このような理由により、本実施例蛍光ランプは明るく、
光のちらつきがなく、長時間点灯しても黒化が従来と同
程度で、したがって同程度の寿命が得られる。
For these reasons, the fluorescent lamp of this example is bright and
There is no flickering of light, and even if the light is turned on for a long time, the blackening is at the same level as before, so the same level of lifespan can be obtained.

なお、本発明において、始動ガスはアルゴンが90容量
%以上(純アルゴンを含む。)でその封入圧力が1.7
〜2.0Torrであれば総て上述した効果がある。
In addition, in the present invention, the starting gas contains 90% by volume or more of argon (including pure argon) and the sealed pressure is 1.7.
-2.0 Torr has all the above-mentioned effects.

すなわち、アルゴンが90容量%未満では従来並の明る
さしか得られず、また1 、 7Torr未満では光束
維持率が下がり、2.0Torrを越えると従来並の明
るさしか得られないことが実験結果から判った。
In other words, experimental results show that if the argon content is less than 90% by volume, only the same level of brightness as before can be obtained, and if it is less than 1 or 7 Torr, the luminous flux maintenance rate decreases, and if it exceeds 2.0 Torr, only the same level of brightness as before can be obtained. I understood from.

また、管壁負荷が500W/r&未満のものについては
、アルゴンが90容量%前後で明るさはあまり変化しな
い。また、同様に500W/mでは封入ガス圧が1.7
〜2.0Torrの範囲の内外で明るさや黒化があまり
変化しない。すなわち、管壁負荷500W/rrr以上
において、アルゴンの容量比および封入ガス圧が明るさ
や黒化に対して臨界的に影響してくることが判った。
Further, for tube wall loads of less than 500 W/r&, the brightness does not change much when argon is around 90% by volume. Similarly, at 500 W/m, the filled gas pressure is 1.7
Brightness and blackening do not change much within and outside the range of ~2.0 Torr. That is, it was found that at tube wall loads of 500 W/rrr or more, the argon capacity ratio and the sealed gas pressure have a critical effect on brightness and blackening.

また、補助陽極は図示の棒状に限らず、板、金網などで
もよく、さらに補助陽極にシールド効果を併有させても
よい。そうして、水銀源として適当なアマルガムを用い
れば高管壁負荷に伴う高水銀蒸気圧を抑制して高効率を
維持できる利点がある。
Further, the auxiliary anode is not limited to the rod shape shown in the figure, but may be a plate, a wire mesh, or the like, and the auxiliary anode may also have a shielding effect. If a suitable amalgam is used as the mercury source, the high mercury vapor pressure caused by the high tube wall load can be suppressed and high efficiency can be maintained.

さらに、本発明においてはバルブ形状は前述の例に限ら
ず、たとえば、環形、U字形、M字形など、他の形状で
も同様である。
Further, in the present invention, the shape of the valve is not limited to the above-mentioned example, and other shapes such as an annular shape, a U-shape, and an M-shape are also applicable.

〔発明の効果〕〔Effect of the invention〕

このように、本発明の蛍光ランプはトリプルコイルから
なる主電極および補助陽極を封装し、バルブ内にアルゴ
ンが90容量%以上で残部がネオンからなる始動ガスを
1.7〜2.0Torrの圧力で封入し500W/m以
上の管壁負荷で動作させるので、明るく、光のちらつき
がほとんどなく、管壁黒化が少なく長寿命である。
As described above, the fluorescent lamp of the present invention has a main electrode and an auxiliary anode made up of triple coils sealed, and a starting gas consisting of 90% by volume or more of argon and the remainder of neon is supplied into the bulb at a pressure of 1.7 to 2.0 Torr. Since the tube wall is sealed with 500 W/m or more and operated with a tube wall load of 500 W/m or more, it is bright, has almost no light flickering, and has a long life with little blackening of the tube wall.

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

第1図は本発明の蛍光ランプの一実施例の断面図、第2
図は同じく効果を説明するグラフである。 (υ・・・バルブ      ■・・・蛍光膜■・・・
ステム      (イ)・・・内導線■・・・主電極
      0・・・補助陽極=12−
FIG. 1 is a cross-sectional view of one embodiment of the fluorescent lamp of the present invention, and FIG.
The figure is also a graph explaining the effect. (υ...Bulb ■...Fluorescent film■...
Stem (A)...Inner conductor ■...Main electrode 0...Auxiliary anode = 12-

Claims (1)

【特許請求の範囲】[Claims] (1)ガラスバルブの両端部にトリプルコイルからなる
主電極および補助陽極を封装し、上記バルブ内にアルゴ
ンが90容量%以上で残部がネオンからなる始動ガスを
1.7Torr以上2.0Torr以下の圧力で封入し
てなり500W/m^2以上の管壁負荷で動作すること
を特徴とする蛍光ランプ。
(1) A main electrode and an auxiliary anode consisting of a triple coil are sealed at both ends of a glass bulb, and a starting gas consisting of 90% by volume or more of argon and the remainder of neon is supplied into the bulb at a temperature of 1.7 Torr or more and 2.0 Torr or less. A fluorescent lamp characterized in that it is sealed under pressure and operates with a tube wall load of 500 W/m^2 or more.
JP4973788A 1988-03-04 1988-03-04 Fluorescent lamp Pending JPH01225058A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4973788A JPH01225058A (en) 1988-03-04 1988-03-04 Fluorescent lamp

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4973788A JPH01225058A (en) 1988-03-04 1988-03-04 Fluorescent lamp

Publications (1)

Publication Number Publication Date
JPH01225058A true JPH01225058A (en) 1989-09-07

Family

ID=12839503

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4973788A Pending JPH01225058A (en) 1988-03-04 1988-03-04 Fluorescent lamp

Country Status (1)

Country Link
JP (1) JPH01225058A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003109542A (en) * 2001-09-28 2003-04-11 Toshiba Lighting & Technology Corp Fluorescent lamp, bulb shape fluorescent lamp and illumination apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003109542A (en) * 2001-09-28 2003-04-11 Toshiba Lighting & Technology Corp Fluorescent lamp, bulb shape fluorescent lamp and illumination apparatus

Similar Documents

Publication Publication Date Title
US6265827B1 (en) Mercury-free metal halide lamp
US6809478B2 (en) Metal halide lamp for automobile headlight
US7057350B2 (en) Metal halide lamp with improved lumen value maintenance
JP3701222B2 (en) High pressure discharge lamp and high pressure discharge lamp system using the same
JP2003016998A (en) Metal halide lamp
US20070138964A1 (en) Mercury-free high-pressure discharge lamp and luminaire using the same
US5103133A (en) Fluorescent lamp having low cathode fall voltage
US4625149A (en) Metal vapor discharge lamp including an inner burner having tapered ends
US20110266947A1 (en) Ceramic gas discharge metal halide lamp
JP3761365B2 (en) Light bulb shaped fluorescent lamp
US7786674B2 (en) Quartz metal halide lamp with improved lumen maintenance
JP2007115652A (en) High-pressure discharge lamp and lighting device
JP3388539B2 (en) Mercury-free metal halide lamp
JP2002110091A (en) Electrode material, high pressure discharge lamp and lighting system
JPH01225058A (en) Fluorescent lamp
US3569766A (en) Metal vapor discharge lamp
US4929868A (en) Glow discharge lamp containing nitrogen
US3373303A (en) Amalgam-containing fluorescent lamp with integral starting aid
JP4411749B2 (en) Metal vapor discharge lamp
JPH05144412A (en) Fluorescent lamp
JPH05334992A (en) Metallic vapor electric discharge lamp
JP3074651B2 (en) Fluorescent lamp
JP2000243348A (en) No-mercury metal halide lamp
JP3127608B2 (en) Metal halide lamp and method of manufacturing the same
EP1041601A1 (en) Fluorescent lamp