JPS5960958A - Low pressure mercury vapor lamp - Google Patents
Low pressure mercury vapor lampInfo
- Publication number
- JPS5960958A JPS5960958A JP16973982A JP16973982A JPS5960958A JP S5960958 A JPS5960958 A JP S5960958A JP 16973982 A JP16973982 A JP 16973982A JP 16973982 A JP16973982 A JP 16973982A JP S5960958 A JPS5960958 A JP S5960958A
- Authority
- JP
- Japan
- Prior art keywords
- anode
- bulb
- cathode
- pressure mercury
- anodes
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/70—Lamps with low-pressure unconstricted discharge having a cold pressure < 400 Torr
- H01J61/72—Lamps with low-pressure unconstricted discharge having a cold pressure < 400 Torr having a main light-emitting filling of easily vaporisable metal vapour, e.g. mercury
Landscapes
- Circuit Arrangements For Discharge Lamps (AREA)
- Discharge Lamp (AREA)
- Discharge Lamps And Accessories Thereof (AREA)
Abstract
Description
【発明の詳細な説明】 本発明は低圧水銀灯装#忙関するものである。[Detailed description of the invention] The present invention relates to a low pressure mercury lamp system.
従来の低圧水銀灯装置は発光灯や殺菌灯、光化学反応用
などに用いらhており、そのラング電流は0.4A程度
がt通である。そして超高出力型とhわhているもので
も2Aa度である。ところでラング電流を2A以上にす
れば発光部の単位長は当りのラング電力か増すことη為
ら、相対的に該装置を小型化したり放射スペクトル密度
を上げることが可能になることから光反応の収蹴金上げ
たり単位時間当りの殺菌処理Iprを増したり小米る可
能性を期待出来る。このため産業上の用途では、該装置
を大型化することなく、ラング電流の大きな低圧水銀灯
装置が望1れている。ところが、従来の低圧水銀灯装置
、にお贋ては、交流の大電流を流そうとした場合、を極
が陽極モードのとき軍子絢嘔によりWL極温麗が上昇L
′亀称に哨布しである電子放射性物質(通称ヱミツター
)の消耗が激りく、バルブの黒化や点灯不良を起1−州
壱命となる。こtlを防ぐため従来列補助陽極を設け、
電子術盤をn牙11しているものもあるが、そねでもラ
ング電流が2 A Pi’、度を・Ii1!オると緩和
効果が斤く、従来の低圧水銀灯装置゛では、小型、長寿
命不維持り六−うえで2Å以上の大14.f Iγ1.
の渾、せる産雛用の低圧水ωt(灯装置す存在L’fX
かった。Conventional low-pressure mercury lamp devices are used for luminescent lamps, germicidal lamps, photochemical reactions, etc., and their rung current is about 0.4 A per ton. And even those that are called ultra-high output types have 2Aa degrees. By the way, if the rung current is set to 2A or more, the unit length of the light emitting section increases by the rung power per unit. Therefore, it becomes possible to relatively miniaturize the device and increase the radiation spectral density, which improves the light reaction. It is expected that there will be a possibility of raising the revenue, increasing the sterilization processing Ipr per unit time, and reducing the amount of sterilization. Therefore, in industrial applications, a low-pressure mercury lamp device with a large rung current is desired without increasing the size of the device. However, with conventional low-pressure mercury lamp devices, when trying to pass a large alternating current, when the pole is in anode mode, the WL extreme temperature rises due to Gunko Ayao.
'The electronic radioactive material (commonly known as emitter) that is used in the lighting is severely consumed, causing blackening of the bulb and poor lighting, resulting in a life-threatening situation. In order to prevent this, conventional row auxiliary anodes are provided,
There are some that use an electronic technique board with a power of 11, but the rung current is 2 A Pi' and the degree is 1! If the lamp is overheated, the relaxation effect is diminished, and conventional low-pressure mercury lamp devices are small and have a long lifespan. f Iγ1.
Low-pressure water ωt for hatching chicks (lighting device exists L'fX)
won.
そこで本発明の目的ね小ルリ、長寿命″f紗持したうえ
で、大1μ流のγlj(せる低圧水0灯flb、 1に
?を提供することにあり、その低圧水銀灯装#fに、陣
・(次と陰極とを組みに1−た「市1極の組み」をバル
ブ内に2絹み設け、夫々の「電極の糺み」において・陽
1ぺけ、半導体整流素子な中介することなく[賓、1軍
に接1・1、されており、陽極にl゛、陰極よりも前方
に自己1醒さね、〃為つバルブの逆方向において、バル
ブ断面オ°nの80チ以下の断面積を有し、バルブの軸
方向に5頷以上の長石を有し、バルブ内にV」、少なく
とも、点灯中の圧力で1 m+a、Hg以下の水銀を含
み、互に他の糾みに属する陽椛と(片極とが放電1−τ
、これが交互に繰り返されて放電、か持続づハることを
特徴とするものである。Therefore, the purpose of the present invention is to provide a low-pressure water lamp 0 lamps flb, 1? with a large flow of 1μ, while maintaining a small flow and a long life. 2 sets of 1-electrode assembly in the bulb, including 1-electrode assembly and 1-electrode assembly, and insert a semiconductor rectifying element in each electrode assembly. [The guest is connected to the first team, and the anode is placed in front of the anode and the cathode is placed in front of the valve. It has a cross-sectional area of The positive polarity and (unilateral polarity) are discharged 1−τ
, which is characterized by alternating repetitions of discharges or sustained charges.
以下に図面を参照1− fxから本発明な挟体的に説明
する。The present invention will be specifically explained below from 1-fx with reference to the drawings.
第1図は本発明の憫徴を含む低圧水釧灯個〕蛤′の説明
図であって、1aと2au夫々第1の組みに属する直熱
型の熱陰極と陽極、1bと2bは夫々第2の組みに属う
る直熱型の熱園傾と陽極であって、夫々の組みにおいて
@極は陰極の片仰1と陸続されている。夫々の組みの隣
接1β1(極の前方に配置され、陽極の大きさ打i、)
くルブ6の径方同における維へい高(断面積の比丘チで
表示した値)を80%以下とし、刀・つ放電経路軸方向
においての長さを5朋以上としている。この陽極と陰極
の組みが夫々バルブ6の両端部5a、+3bに耐重ば1
1.ている。そしてバルブ6内には倣すλの水銀も1−
〈は水銀とアルゴン−・どの希ガスがイit jHづれ
ている04 h′電清制限用のチョークコイル、5はト
ランスを示し二次巻線5a、5bは夫々第1、第2の耕
みに屈する直熱磨航陰(ボla、lbの電源として利用
し、二次巻線5Cが夫々の絹みに属する陽極2a12b
に接続されて放電発光に供するようにしである。−次式
1145cLは商用電源、例えば交流100vもしくは
200V電源7に接続さ力る。FIG. 1 is an explanatory diagram of a low-pressure water lamp (clam) including the features of the present invention, in which 1a and 2au respectively belong to the first set of directly heated hot cathodes and anodes, and 1b and 2b respectively A direct heating type heat field tilt and an anode that belong to the second set, and in each set, the @ pole is connected to one side of the cathode. Adjacent 1β1 of each set (placed in front of the pole, size of the anode i,)
The height of the curve 6 in the radial direction (the value expressed in terms of cross-sectional area) is 80% or less, and the length in the axial direction of the discharge path is 5 mm or more. This pair of anode and cathode is attached to both ends 5a and +3b of the bulb 6, respectively.
1. ing. And in the bulb 6, the mercury of λ is also 1-
〈 is mercury and argon - which noble gas is different? 04 h' Choke coil for limiting electrolysis, 5 indicates a transformer, and secondary windings 5a and 5b are used for the first and second windings, respectively. Anode 2a12b is used as a power source for direct heating polishing (bolla, lb), and the secondary winding 5C belongs to each silk.
It is connected to the LED to provide discharge light emission. - The following formula 1145cL is connected to a commercial power supply, for example, AC 100V or 200V power supply 7.
上記低圧水銀灯装置において放電形成は次の様にな芒れ
る。In the above-mentioned low-pressure mercury lamp device, discharge formation is as follows.
最初の交流半サイクルでは、矢印8で示すように市、流
が加ね、次の焚流半サイクルでは、矢印9で示すように
電流が流れる。こJ9が交互に繰り仮でわて放電、が持
続される。1組電流の同きは、Ilt子の流れと逆の同
=i採用している。In the first alternating current half cycle, current flows as shown by arrow 8, and in the next half cycle, current flows as shown by arrow 9. This J9 is repeated alternately, and the discharge continues. For the current of one set, the opposite flow of the Ilt element is adopted.
つまり、放電り、互に他の組みに端する陽・庫と陰極と
か対になって、交互に、同−放電媒体を通して形成され
ている。In other words, a discharge is formed in pairs, such as a positive electrode, a negative electrode, and a negative electrode, each ending in another pair, alternately passing through the same discharge medium.
上記低圧水銀灯装置の基本的長所t T i(+“に列
挙する。The basic advantages of the above-mentioned low-pressure mercury lamp device are listed below.
(1)1揚極と陰極とけ、夫々設計思旬が界なるので、
本発明の場合d1陽極に陽諏の設計思想にのみ基いて、
1u」陰庫の設計思想にのみ基いて夫々設置・できるの
で、結果として、大電流の低圧水銀灯装置か椋供で炒る
。その他、使用寿命の長い電極設計や、放電開始電圧の
低い電極設計が若易になる。(1) 1. Since the positive pole and the negative pole are different from each other, the design considerations are different.
In the case of the present invention, based only on the design concept of the positive electrode for the d1 anode,
Since it can be installed and installed based only on the design concept of a 1U" shade room, it can be roasted using a high-current, low-pressure mercury lamp device or a steamer. In addition, it becomes easier to design an electrode with a long service life and a low discharge starting voltage.
(2) アーク長の長い金属#気散電灯ン、従来、形
式の自流用放電灯とE2て股ぎ士すると、金鴎イオンが
陰極側へ片寄り、発光ムラの発生をともなうが、本発明
の方式では、そのような欠点か解消さ冶、る。(2) When a metal diffuser lamp with a long arc length is mixed with a conventional self-flow discharge lamp and an E2 type, the metal ions are biased toward the cathode side, causing uneven light emission, but the present invention This method eliminates such drawbacks.
上記長所は、次の設計91.1をみると史によく理解で
きる。The above advantages can be clearly understood by looking at the following design 91.1.
バルブとして、自掃10闘のオゾンレス石英を採用しい
アーク長を300wとL1放放電体としてけ放′rJ1
発光中の蒸気圧が6 X 1. OrnmHgとなる水
銀と、アルゴンガスif0 、3+++rvHg封入す
る。この場合、低圧水ψμ灯の電圧は約59Vで、電波
を4A帷して消Q電力は約200W、!!−なった。そ
して陰極としては夕/ゲステンフィラメントに、(Ba
SrCa))3e(4(バリウムストロンチウム力ルン
ウム3元ベリレイト)を塗布l−τ、最もm子放射性の
良い投縛1とな1−1@極として幻、大電子が・の伽殻
に耐えられるようにタングステンのロッドT JAY
IJVL1丈夫さを基本としてis、NtLでいる。し
、たがって、上Bじ低圧水沁灯装Wは、従来σ)太キ格
に比べ、祥さか6分の1程度に小型になったげ力・りで
〃く、電流イ(自か著しく大巻くすることができ、結果
として、紫外線数#!も著しく増大せしめることができ
る。The bulb uses ozone-free quartz with a self-sweeping rating of 10%.The arc length is 300W and the L1 discharge body is used as the discharge source.
The vapor pressure during light emission is 6 x 1. Mercury to become OrnmHg and argon gas if0, 3+++rvHg are sealed. In this case, the voltage of the low-pressure water ψμ lamp is about 59V, the radio wave is 4A, and the Q power consumption is about 200W! ! -It became. And as a cathode, (Ba
SrCa)) 3e (4 (barium strontium trinium berylate) is coated l-τ, which is the most m-emissive binding 1 and 1-1@pole, which can withstand the shell of large electrons. Like tungsten rod T JAY
IJVL1 Is and NtL based on robustness. Therefore, the low-pressure water lantern W shown above is about one-sixth the size of the conventional σ), has a smaller power and power, and has a significantly higher current. It is possible to make a large roll, and as a result, the number of ultraviolet rays #! can be significantly increased.
低圧水銀灯において、電流値を増大させf′Lば、紫外
線放射が増大することは既知であったが小形長寿命の低
圧水銀灯装置は、従来の設h1思想では全く得ら刺ない
。これは、親、在市1jljの螢光灼、イ氏圧水銀灯、
#菌灯の電流値が1べて2A−采/!:Tあることを考
えねば明らかである。It has been known that in a low-pressure mercury lamp, the ultraviolet radiation increases as the current value f'L increases, but a compact, long-life low-pressure mercury lamp device cannot be achieved at all with the conventional design concept. This is a parent, a fluorescent burner in the city, Mr. Lee's pressure mercury lamp,
#The current value of the fungal lamp is 2A-1/! :T It's obvious if you think about it.
前記した従来の200W程変の殺菌灯と、上b1″の低
圧水銀灯装置との比較を、2537 Aの1σ7当りの
アーク畏からの放射量で行うと、本発明で1、放射強度
が数十倍にまで及ぶので、産ヴ用に使用【−た場合の生
産性の高さしj1比較にならないぐらい高い。Comparing the conventional germicidal lamp with a power of about 200 W and the low-pressure mercury lamp device with a top b1'' in terms of the amount of radiation from the arc per 1σ7 of 2537 A, the present invention has a radiation intensity of 1, while the radiation intensity is several dozen. The productivity is so high that it is incomparable when used for childbirth.
上記低圧水銀灯装置の1役耐例からも理ブゲr略わるよ
うに、
(3)電流値が数十A N ffで使用できる1、小型
、長寿命の低圧水銀灯装置も容易VC得られ従来の他の
技術と組み合せると、
(4) バルブの材質として、1849 Aを°民〈
透isする石英ガラスとずれば、強力なオゾン発生用の
低圧水銀灯+5置が得られる。As can be seen from the example of durability of the low-pressure mercury lamp device mentioned above, (3) A small, long-life low-pressure mercury lamp device that can be used with a current value of several tens of A Nff can easily obtain a VC compared to the conventional one. (4) 1849 A as the valve material
If you use transparent quartz glass, you can get a low-pressure mercury lamp +5 units for powerful ozone generation.
(5ン バルブの材質として、オゾンレス0英カラス
も1−(は殺菌灯用硬質ガラス不一選べ1げ、オゾンの
発生の斤い強力な殺菌装置が得らハる。(5) Ozone-free bulbs can be made of hard glass for germicidal lamps, and a powerful sterilizing device that generates ozone can be obtained.
と言う長所がある。There are advantages to saying that.
石英ガラス、オゾンレス石英ガラス、殺菌灯用ガラスは
いず?も市販はれていて、分光透過率特性娃、例えば、
東芝レビュー(34巻5刊第448頁)ガラス工学ハン
ドブックm 670 R(114倉書店昭オlI48年
6月20日 10版発h)にも記載嘔t]ているところ
のものである。上記材質の他、透光性セラミックチュー
ブ、例えば多結晶アルミナ(問品名ルカロツクス)等も
使える。What about quartz glass, ozone-free quartz glass, and glass for germicidal lamps? There are also commercially available products with spectral transmittance characteristics, for example,
It is also described in Toshiba Review (Volume 34, Issue 5, Page 448) Glass Engineering Handbook M670R (114 Kura Shoten, June 20, 1948, 10th edition). In addition to the above-mentioned materials, translucent ceramic tubes such as polycrystalline alumina (trade name: Lucarox) can also be used.
放電発光中の水@蒸気圧の制御は、放電灼製r「時妊お
ける水銀封入竜で決めても良いし、バルブに水調質めを
設けておき、水調質めの温度をPlr定の一定値に保つ
ことによって達成しても良I/′LL 。The water @ vapor pressure during discharge light emission can be controlled by using a mercury-enclosed tank made by discharge firing, or by setting a water conditioning device in the bulb and setting the temperature of the water conditioning device by PLR. This can be achieved by keeping I/'LL at a constant value.
凍た、熱陰極としては傍熱型を使用しても良い。An indirectly heated type may be used as the frozen or hot cathode.
これら娃いづtl、も既知の方法が使用できる。史にバ
ルブ6の内面′4!lL <は外面に螢光体を塗布して
強力な発光の得られゐ螢光灯とL″r構成1−でもよ0
ところT′上記設計例の低圧水銀灯峙f%VC:L−m
で、!川波に使用するには、夫々の組みにおける陽極と
陰極は前述[、た様に夫々股計思イυが異なるので交流
の半サイクルごとに電離の滓?Iは完全に1効吟と陰極
に流れ込む様にLなけ)1けならない。そしてそねに夫
々の矩、極の位置、4多状及び寸ρ゛に大政〈依存する
。卯1の1.i−1みの電極を例にしてdψ明すると、
自1σ)椙みの電、極が、第2σ)絹みの電極、に71
してフラス電位の半サイクルτ゛←r電びt(l−J
完全に陽極力・ら流れねばならない。陰極から電流が1
11.ね出ずということは、陰極に対し %i子iΔi
75’8があるということを意Kt−、ラング電流か本
発明のラングのように大きいと救は、墜碌の幅度か非常
に高くなる。そL T (Ba5rCa)BeQ、のm
5vxミツター1刹、激な蓋発を引き起して%y÷よか
暑しく19A合となる。Known methods can also be used for these preparations. The inside of valve 6'4 in history! lL < means that a fluorescent lamp is coated on the outer surface to obtain strong light emission.Also, it is possible to use a fluorescent lamp and L″r configuration 1-0. However, T′ is compared to the low-pressure mercury lamp of the above design example f%VC:L-m
in,! For use in river waves, the anode and cathode in each set have different radial values, as described above, so ionization sludge is generated every half cycle of alternating current. I must be completely 1 effect and L must be 1 so that it flows into the cathode. And it really depends on each rectangle, the position of the poles, the four shapes, and the dimensions. Rabbit 1 no 1. Taking the i-1 electrode as an example and clarifying dψ,
Self 1σ) Soft electrode, pole is 2nd σ) Silky electrode, 71
half cycle of the frass potential τ゛←r electric current t(l-J
The anode force must flow completely. The current from the cathode is 1
11. No leakage means that %i Δi with respect to the cathode
75'8 means that if the rung current is as large as the rung of the present invention, the width of failure will be very high. SoL T (Ba5rCa)BeQ, m
5vx mitsuta 1 moment, it caused a violent opening and became a %y ÷ 19A match.
以上の41を防ぐためにけ結線位置3a、3b知お論で
、半承体斡流李子のカンードf陽極に、アノード(r−
1衾イ呵に夫々接岬する方法(特願)1?J 55−6
3422 発明者荒川外2名)があるが、本発明でl
d−ヒ記半遺体整流素子な1−で114極の位置と大と
さを規♀することにより同様の頬摺を外ようとするもの
であって、飢1の組みの常、極が陽イタモードのとき電
流か陽極〃・ら完全に流ねるために、各tirQ)実験
を行った結果以下の条件が必要であることか分った。In order to prevent the above 41, the anode (r-
How to attach each cape to each other (special request) 1? J55-6
3422 Inventor Arakawa and two others), but the present invention
d-H Note 1-, which is a half-body rectifier, attempts to eliminate the similar problem by regulating the position and size of the 114 poles. As a result of various tirQ) experiments, it was found that the following conditions were necessary in order for the current to flow completely from the anode in the tidal mode.
(1)1堵シ極は陰極の前に設憧嘔れねばならない。(1) The first pole must be placed before the cathode.
こflは、陽極、陰極とも結線位置3aで接続嘔ねでい
るため同電位であり、放電経路Ftil力η・ら移動し
てくる電子(d j襲も近い電極に流れ込むたlbであ
る。Since both the anode and the cathode are connected at the connection position 3a, they have the same potential, and the electrons (dj attack also flow into the nearby electrode) from the discharge path Ftil force η.
(2) 陽極はある一定以一ヒの大炒さを持つ必要が
ある。夫々の電極の組みにおいて、陽極モードのと@陽
極力・ら電流か流flない。ブなわち電子が流れ込オな
囚様にするに1士陽極は)ある一定置上の大微さを持つ
必要がある。そi7C印、1図、第2図においてバルブ
径方向の断面における陽極による放霜;経路に対する遮
へい率すなわち、(d/D)2が帆8(80%)以下で
、かつ陽極のかrh:経路の軸方向洋甥1が5鼎以上必
萼である。(2) The anode needs to have a certain degree of strength. In each electrode set, there is no current fl from the anode force in the anode mode. In other words, in order for electrons to flow into it, the anode must have a certain degree of fineness. So i7C mark, Figures 1 and 2 show frost removal by the anode in the cross section in the radial direction of the bulb; the shielding rate for the path, that is, (d/D)2 is less than sail 8 (80%), and the rh of the anode: path The calyx must have 5 or more calyxes in the axial direction.
陽極−通常側電子#I膠性の高いタングステンを用いる
。その為(d/1)fが0.8’i越えることC陰極モ
ードのとき放電経路を大きくしぼることになるので放電
抵抗を上げて点灯性r悪くする。Anode - Normal side electron #I Tungsten with high adhesiveness is used. Therefore, if (d/1)f exceeds 0.8'i, the discharge path will be greatly constricted in the C cathode mode, which will increase the discharge resistance and worsen the lighting performance.
そして遮へい率は大体10〜30チが好オしい。And the shielding rate is preferably 10 to 30 inches.
いずれにしてt放′可状別におl/’1ては陽極は放電
経路の軸方向に長嘔1をもつがそわが充分でない場合、
いわゆる電子の1しみ出LJによr)陰極へ電子が到達
してし1つ。すなわち、ある交流放電の半サイクルにお
けるランプ電流な11、陽極力・ら流れる電性’、 f
Ia、陰(水から流ねる宙、流を■cとすれF′1I
l=la+Ic に’fz り I’4ft 4fi
< モードのときけ 11= Ia 陰極モードのと
きけII = ICKな力は良い。陽極モードのとき電
子の「しみ出し」があると鋒は 工C六〇 KなりC
/IIがある割合になる。こねf1体的に四囲すると、
例えば、バルブ径 D=10mm i臀碌PFd =
3.6mm アーク長を300ynmト(−放’[
$体として放電発光中の蒸気圧が6X10*iHEとな
る水銀とアルゴンガスを0.3vmHE刊人する。In any case, the anode has a long elongation 1 in the axial direction of the discharge path depending on the discharge state, but if the elongation is not sufficient,
Due to the so-called electron seepage LJ, one electron reaches the cathode. That is, the lamp current in a half cycle of an AC discharge is 11, the electric current flowing from the anode force, f
Ia, Yin (air flowing from water, let the flow be ■c F'1I
l=la+Ic ni'fz ri I'4ft 4fi
<Mode's threshold 11 = Ia Cathode mode's threshold II = ICK force is good. When in anode mode, if there is electron ``seepage'', Feng C60 K becomes C
/II becomes a certain ratio. If you surround f1 physically,
For example, valve diameter D = 10 mm i buttock PFd =
3.6mm Arc length 300ynm (-radiation'[
Mercury and argon gas whose vapor pressure during discharge light emission is 6X10*iHE are 0.3vmHE.
そして陽極の趣へい率が13 %、ランプ市、流〃;5
Aにおいて陽極の放電経路軸力回長さ1を変えながらI
C/■1を測定すると第3図の1r+!りになった。ラ
ング電流を2〜20Aまで変化させてもそれぞれの1に
おけるic/ilの割合はあ1り変化しな力・つた。す
なわち(d/D )2か0.8以下においては、1か5
間以上あ負げ電子の「しみ出し」により′に極が陽極モ
ードのとき1(ス極刀1ら電流が流ねる串がない。従っ
て夫々の電極は千〇設宣十思11汗に基いて使用される
ことになり大電流の低圧水優灯装置か提供Tきる。升を
(り9極モードの晧はタングステンでで久た陽極とり(
1λげ(BaSrCa)B802i 塗布した+5<;
極ではq rm:4 hて一ハる物9ησ)什小14
1数が大きく違うt−め陽弾〃工ら電子が放射される硝
Iけ普・辿和゛ない。And the anode failure rate is 13%, lamp city, flow; 5
I while changing the anode discharge path axial force rotation length 1 at A.
When C/■1 is measured, it is 1r+ in Figure 3! It became Even if the rung current was changed from 2 to 20 A, the ratio of IC/IL at each point did not change at all. In other words, when (d/D) is 2 or less than 0.8, it is 1 or 5.
When the electrode is in the anode mode due to the ``seepage'' of electrons over a period of time, the electrode is in anode mode. Since it will be used in a high-current, low-pressure water-powered lamp device, it will be possible to provide a large-current, low-pressure water-powered lamp device.
1λ Ge (BaSrCa) B802i applied +5
At the pole, q rm: 4 h = 9ησ) tithe 14
It is impossible to trace the difference in the number of electrons emitted from a solar bomb.
第1図は本発明の低圧水釧灯撃ff1jσ劫l゛の口9
明図、第2図し1第1図II −II線vCおける障テ
rn’、i図!、第3図標テータの砦、明図である。
1a、1b−、陰4+@2 a、 2 b−・・陽極4
・・・チョークコイル 5・・・トランス6・・・バ
ルブ
出願人 ウシオ′醜機株式会社
代理人 弁理士 ′EH身寅之助Figure 1 shows the low-pressure water tank light attack ff1jσkal゛ mouth 9 of the present invention.
Clear figure, Figure 2 and 1 Obstacle rn' on line vC in Figure 1 II-II, Figure i! , Figure 3: The Fortress of Theta, a clear map. 1a, 1b-, negative 4+@2 a, 2 b-...anode 4
...Choke coil 5...Transformer 6...Valve Applicant Ushio Ushio Co., Ltd. Agent Patent attorney EH Toranosuke
Claims (1)
2組み設け、 夫々の「電極の組み」において、陽極は半導体整流素子
を中介することなく陰極に接続されており、 陽罹柑、陰極エリも前方に配IWホ力、かつバルブの径
方向において、バルブ断面積の80q6J−1下の断面
積を有し、バルブの軸方向に5 ttrm以上の長さを
有し、 バルブ内には、少なくとも1点灯中の圧力で1罪、Hq
以下の水銀を含み、 互に他の組みに属する陽極と陰極とが放’/If、 し
て、これが父互に繰り返されて放電が持続でれることを
特徴とする低圧水銀灯装置。[Claims] Two sets of "electrode sets" each consisting of an anode and a cathode are provided in the bulb, and in each "electrode set", the anode is connected to the cathode without intervening a semiconductor rectifying element. The positive and negative electrodes are also located in front of the IW force, and have a cross-sectional area of 80q6J-1 below the valve cross-sectional area in the radial direction of the valve, and a length of 5 ttrm or more in the axial direction of the valve. The pressure inside the bulb is at least 1 Hz during lighting, Hq
A low-pressure mercury lamp device containing the following mercury, characterized in that an anode and a cathode belonging to different pairs discharge '/If, and this is repeated to sustain a discharge.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16973982A JPS5960958A (en) | 1982-09-30 | 1982-09-30 | Low pressure mercury vapor lamp |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16973982A JPS5960958A (en) | 1982-09-30 | 1982-09-30 | Low pressure mercury vapor lamp |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5960958A true JPS5960958A (en) | 1984-04-07 |
JPS6349340B2 JPS6349340B2 (en) | 1988-10-04 |
Family
ID=15891943
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP16973982A Granted JPS5960958A (en) | 1982-09-30 | 1982-09-30 | Low pressure mercury vapor lamp |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5960958A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6319749A (en) * | 1986-07-14 | 1988-01-27 | Toshiba Corp | Low pressure discharge lamp device |
JPH02121255A (en) * | 1988-09-20 | 1990-05-09 | General Electric Co (Ge) | High-efficiency discharge lamp having large-sized anode |
-
1982
- 1982-09-30 JP JP16973982A patent/JPS5960958A/en active Granted
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6319749A (en) * | 1986-07-14 | 1988-01-27 | Toshiba Corp | Low pressure discharge lamp device |
JPH02121255A (en) * | 1988-09-20 | 1990-05-09 | General Electric Co (Ge) | High-efficiency discharge lamp having large-sized anode |
Also Published As
Publication number | Publication date |
---|---|
JPS6349340B2 (en) | 1988-10-04 |
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