JPS5838447A - Neon gas discharge lamp for optical device - Google Patents
Neon gas discharge lamp for optical deviceInfo
- Publication number
- JPS5838447A JPS5838447A JP13661181A JP13661181A JPS5838447A JP S5838447 A JPS5838447 A JP S5838447A JP 13661181 A JP13661181 A JP 13661181A JP 13661181 A JP13661181 A JP 13661181A JP S5838447 A JPS5838447 A JP S5838447A
- Authority
- JP
- Japan
- Prior art keywords
- optical device
- gas discharge
- neon
- discharge lamp
- neon gas
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/02—Details
- H01J61/12—Selection of substances for gas fillings; Specified operating pressure or temperature
- H01J61/16—Selection of substances for gas fillings; Specified operating pressure or temperature having helium, argon, neon, krypton, or xenon as the principle constituent
Landscapes
- Discharge Lamp (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は光学装置に用いられるネオンガス放電灯に関
するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a neon gas discharge lamp used in an optical device.
電子複写機、ファクシミリ、光学式文字読取装置等の光
学装置用のランプとしては、一般に白熱電球及び螢光ラ
ンプが使用されている。しかし、白熱電球は効率と寿命
が悪く問題がある。Incandescent lamps and fluorescent lamps are generally used as lamps for optical devices such as electronic copying machines, facsimiles, and optical character readers. However, incandescent light bulbs have problems with poor efficiency and longevity.
これに対し螢光ランプは効率と寿命はよいが。Fluorescent lamps, on the other hand, have better efficiency and longevity.
その特性は水銀蒸気圧に依存するため温度の影響が大き
い。す々わち周囲温度により光量が変化したり2点灯後
水銀蒸気圧が安定するまで光量が相当大巾に変化したり
する。さらに螢光ランプは螢光体の劣化などにより、寿
命中の光量の減少が太きい。これらの点は上記のような
光学装置にとって大きな欠点となる。Its properties depend on mercury vapor pressure and are therefore greatly affected by temperature. In other words, the amount of light changes depending on the ambient temperature, and the amount of light changes considerably after two lightings until the mercury vapor pressure stabilizes. Furthermore, the light intensity of fluorescent lamps decreases significantly during their lifetime due to deterioration of the fluorescent material and other factors. These points are major drawbacks for the above-mentioned optical device.
この発明は上記欠点を改善した。効率の良い光学装置用
光源を提供することを目的とするものである。This invention has improved the above drawbacks. The object is to provide an efficient light source for an optical device.
本発明者らは、−マず上記光源として希ガスの中で最も
可視光の発光効率が良いネオンを封入した低圧希ガス放
電灯を使用することに着想した。The inventors first came up with the idea of using a low-pressure rare gas discharge lamp filled with neon, which has the highest visible light emission efficiency among rare gases, as the light source.
低圧希ガス放電灯は螢光ラングに比べ、基本的に温度依
存性が少なく、かつ螢光体の劣化などの問題がないため
に、常に安定した光量を得ることができる。また放電維
持電圧と放電開始電圧を低くして良好な総合効率を得る
必要から予熱形!極を具備させることが必要で凌)る。Compared to fluorescent lamps, low-pressure rare gas discharge lamps basically have less temperature dependence and do not have problems such as deterioration of the fluorescent material, so they can always provide a stable amount of light. In addition, it is necessary to lower the discharge sustaining voltage and discharge starting voltage to obtain good overall efficiency, so it is a preheating type! It is necessary to have the poles (to overcome).
光学装置の必要とする光量は、各々の機糧により異なる
のはもちろんであるが、一般的に光学装置用螢光ランプ
は10w’jたは15Wの一般照明用螢光ラングど同一
管径のもので、そのランプ電流は0.7A〜1.2人で
あり、一般照明用ランプの0.23A〜0.3人に比較
して大電流であることから明らかなように、大光量を必
要とする。さらに光学装置の高度化とともに、光量の調
整をスリットなどの機械部品によらず、螢光ランプの調
光によって行う場合がある。これらの状況を考慮すると
、光学装置用の坏オンガス放電灯に要求される条件とし
て、ネオンサインに比べ大光量を必要とするため、ラン
プ電流は少なくとも0.2 A以上で使用され、IAA
以上も効率の低下しないランプが必要である。Of course, the amount of light required by an optical device differs depending on the equipment, but in general, fluorescent lamps for optical devices have the same tube diameter, such as 10W'j or 15W fluorescent lamps for general lighting. The lamp current is 0.7A to 1.2 people, which is a large current compared to 0.23A to 0.3 people for general lighting lamps, which requires a large amount of light. shall be. Furthermore, as optical devices become more sophisticated, the amount of light may be adjusted by dimming a fluorescent lamp instead of using mechanical parts such as slits. Taking these circumstances into consideration, the conditions required for a crystalline gas discharge lamp for optical equipment are that it requires a large amount of light compared to a neon sign, so the lamp current must be at least 0.2 A, and the IAA
There is a need for a lamp that does not reduce efficiency.
一方、ネオンガス放電灯の発光効率および光出力は、封
入ガス圧力、管径、電流の相互の関係によって決まるが
2本発明者らは特に管径と電流との関係に着目し2種々
検討の結果、ある一定収上の管径であれば電流値に依存
することなく効率が決ま9,1A以上でも効率の低下し
ない実用的なネオンガス放電灯が得られることを見い出
した。On the other hand, the luminous efficiency and light output of a neon gas discharge lamp are determined by the relationship among the filled gas pressure, tube diameter, and current.2 The inventors focused on the relationship between tube diameter and current, and as a result of various studies. It has been discovered that if the tube diameter is within a certain range, the efficiency is determined regardless of the current value, and a practical neon gas discharge lamp with no decrease in efficiency even at 9.1 A or more can be obtained.
以下実施例によりさらに詳細に説明する。The present invention will be explained in more detail with reference to Examples below.
熱電子放射物質を担持したフィラメントコイ(3)
ルミ極を両端に封着した外径14龍〜26龍、長さ43
6闘の硝子管に、ネオンガス0.1 torr〜lOt
orr封入したネオンガス放電灯を製作した。点灯はチ
ョークコイルを安定器として、電極を交流3.6■で予
熱し、電極間に交流電圧を印加してなされた。測定に先
立ち、完全に安定したランプを得る目的からエージング
を行ったが、封入圧力の低いランプは電極の損傷が激し
く、長寿命のランプを得ることは不可能であることがわ
かった。本発明者らは電極の改良や、予熱電流の変更を
考慮しても1 torr未満では実用的なランプを得る
ことは不可能であると判断し、 1torr以上につ
いて検討を進めることとした。ちなみに1torr未滴
のランプはすべて100時間以内に不点となった。Filament carp carrying a thermionic emissive material (3) Luminous poles sealed on both ends, outer diameter 14 to 26, length 43
Neon gas 0.1 torr ~ lOt in a 6-hole glass tube
I made a neon gas discharge lamp filled with orr. Lighting was carried out by using a choke coil as a ballast, preheating the electrodes with 3.6 AC, and applying an AC voltage between the electrodes. Prior to measurements, aging was performed with the aim of obtaining a completely stable lamp, but it was found that lamps with low sealing pressure had severe electrode damage, making it impossible to obtain a lamp with a long life. The inventors of the present invention determined that it would be impossible to obtain a practical lamp at a pressure of less than 1 torr even if improvements in the electrodes and changes in preheating current were taken into account, and decided to proceed with the study on a value of 1 torr or more. Incidentally, all lamps with 1 torr without dripping became defective within 100 hours.
第1図、第2図、第3図は電流と発光効率の関係を表わ
すグラフで1曲線Aは管外径26n。Figures 1, 2, and 3 are graphs showing the relationship between current and luminous efficiency, and one curve A has a tube outer diameter of 26n.
曲線Bは20鰭2曲線Cは14鰭の場合である。Curve B is for 20 fins, and curve C is for 14 fins.
l第1図はネオンの封入圧力1 torrの場合であり
。Figure 1 shows the case where the neon sealing pressure is 1 torr.
第2図は5torr、第3図は1Qtorrの場合であ
る。FIG. 2 shows the case of 5 torr, and FIG. 3 shows the case of 1 Qtorr.
(4)
いずれの場合も管径の大きいほど、電流の増加に伴う効
率の低下は小さい。換言すれば、管径が大きいほど電流
の増加による光量の飽和する傾向が小さくなる。(4) In either case, the larger the pipe diameter, the smaller the decrease in efficiency accompanying an increase in current. In other words, the larger the tube diameter, the less the tendency for the amount of light to saturate due to an increase in current.
第4図は電流を0.2 AからIA増加した際の効率の
減少割合と管外径の関係を示すものであり。FIG. 4 shows the relationship between the rate of decrease in efficiency and the tube outer diameter when the current is increased from 0.2 A to IA.
曲線a、b、cはそれぞれネオンの封入圧力1torr
。Curves a, b, and c each have a neon sealing pressure of 1 torr.
.
5 torr、 10 torrの場合を表わす。第4
図より管外径20龍以上であれば、電流に対してほぼ一
定効率となるランプが得られることがわかる。The cases of 5 torr and 10 torr are shown. Fourth
From the figure, it can be seen that if the outer diameter of the tube is 20 mm or more, a lamp with substantially constant efficiency with respect to current can be obtained.
なお上記データは商用電源によるものであるが、 20
KHz程度の高周波或いは直流点灯においてもほぼ同様
な結果が得られることを確認した。The above data is based on commercial power supply, but 20
It was confirmed that almost the same results could be obtained with high frequency on the order of KHz or direct current lighting.
この発明は以上説明したとおり、管外径を20鰭以上、
封入ネオン圧力を1 torr以上とすることにより、
0.2A以上で高効率となる光学装置用ネオンガス放電
灯が得られるという効果がある。As explained above, this invention has a tube outer diameter of 20 fins or more,
By setting the sealed neon pressure to 1 torr or more,
This has the effect of providing a neon gas discharge lamp for optical devices that is highly efficient at 0.2 A or more.
第1図、第2図、第3図は電流と発光効率の関係;、第
4図rrz管外径と発光効率の減少割合の関係図である
。
代理人 葛 野 信 −
!!1図
θ:2 0.4 0.6 # 1
0 1.2電 夫 tA>
第2図
電 1(A)
@3図
o、2o、4ty、6a、fjlθ 12e i
CΔ→第4F!llI
管外径 (mITI)FIGS. 1, 2, and 3 show the relationship between current and luminous efficiency; FIG. 4 shows the relationship between the outer diameter of the RRZ tube and the rate of decrease in luminous efficiency. Agent Shin Kuzuno −! ! Figure 1 θ: 2 0.4 0.6 # 1
0 1.2 Den tA> 2nd figure 1(A) @3 figure o, 2o, 4ty, 6a, fjlθ 12e i
CΔ→4th F! llI tube outer diameter (mITI)
Claims (1)
ネオンと予熱形電極を封入した定格ラング電流0.2Å
以上の光学装置用ネオンガス放電灯。A rated rung current of 0.2 Å is made by enclosing neon of 1 torr or more and a preheated electrode in a glass tube with an outer diameter of 20 iI11 or more.
Neon gas discharge lamp for optical equipment.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13661181A JPS5838447A (en) | 1981-08-31 | 1981-08-31 | Neon gas discharge lamp for optical device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13661181A JPS5838447A (en) | 1981-08-31 | 1981-08-31 | Neon gas discharge lamp for optical device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5838447A true JPS5838447A (en) | 1983-03-05 |
Family
ID=15179340
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13661181A Pending JPS5838447A (en) | 1981-08-31 | 1981-08-31 | Neon gas discharge lamp for optical device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5838447A (en) |
-
1981
- 1981-08-31 JP JP13661181A patent/JPS5838447A/en active Pending
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