JPS62163253A - Fluorescent lamp - Google Patents
Fluorescent lampInfo
- Publication number
- JPS62163253A JPS62163253A JP521386A JP521386A JPS62163253A JP S62163253 A JPS62163253 A JP S62163253A JP 521386 A JP521386 A JP 521386A JP 521386 A JP521386 A JP 521386A JP S62163253 A JPS62163253 A JP S62163253A
- Authority
- JP
- Japan
- Prior art keywords
- gas
- anode
- light emission
- cathode
- voltage
- 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
Abstract
Description
【発明の詳細な説明】
[技術分野]
本発明は低圧ガスを封入した管内にアノード及びカソー
ドを設けたいわゆる電子ビーム方式の蛍[背景技術1
従来より第1図に示すように、管体1内に水銀蒸気のよ
うな励起発光性ガス2を封入し、フィラメントで加熱さ
れたカソード3とメツシュ状のアノード4を管内に設け
、アノードカソード間で電子を加速して、アノードの背
後の空間Sで電子とがス原子との衝突により励起発光を
行ない、放射された紫外線を管壁に塗布された蛍光物質
により可視光に変換する方式の蛍光ランプが、特開昭5
7−130364号等で提案されている。図中、5はフ
ィラメント加熱用電源、6は電子加速用電源である。こ
の方式によれば電流−電圧特性が正であるために安定器
等の限流要素が不要となり、軽量でコンパクトな蛍光灯
が実現できるという可能性がある。Detailed Description of the Invention [Technical Field] The present invention relates to a so-called electron beam type firefly in which an anode and a cathode are provided in a tube filled with low-pressure gas [Background Art 1 As shown in FIG. An excited luminescent gas 2 such as mercury vapor is sealed inside the tube, and a cathode 3 heated by a filament and a mesh-like anode 4 are provided in the tube, and electrons are accelerated between the anode and cathode to create a space S behind the anode. A fluorescent lamp in which excited light is emitted by the collision of electrons with sulfur atoms and the emitted ultraviolet rays are converted into visible light by a fluorescent substance coated on the tube wall was developed in Japanese Patent Application Laid-Open No. 5.
It has been proposed in No. 7-130364, etc. In the figure, 5 is a filament heating power source, and 6 is an electron acceleration power source. According to this method, since the current-voltage characteristic is positive, current-limiting elements such as ballasts are not required, and there is a possibility that a lightweight and compact fluorescent lamp can be realized.
しかし上記の従来方式においては、アノードを通過させ
て電子をトリアドさせるために、アノードの背後の空間
に電子によって形成される空間電荷を除去してやらなけ
ればならない。そのためにメートには比較的高い電圧(
約10数■)を印加しでいる。従って管内の電子には水
銀原子を励起発光させるのに最適なエネルギ(約6eV
)よりもはるかに高いエネルギが与えられ、これがラン
プの発光効率を低下させていた。However, in the above-described conventional method, in order to triad the electrons by passing through the anode, the space charge formed by the electrons in the space behind the anode must be removed. Therefore, the mate has a relatively high voltage (
Approximately 10 cm) has been applied. Therefore, the electrons in the tube have the optimum energy (approximately 6 eV) to excite the mercury atoms and cause them to emit light.
), which reduced the luminous efficiency of the lamp.
[発明の目的]
本発明は上記の問題点に鑑み為されたものであり、その
目的とするところは、上記のように限流要素を不要とす
る電子ビーム方式において、発光効率の高い蛍光ランプ
を提供するにある。[Object of the Invention] The present invention has been made in view of the above problems, and its purpose is to provide a fluorescent lamp with high luminous efficiency in the electron beam method that does not require a current limiting element as described above. is to provide.
[発明の開示]
しかして本発明による蛍光ランプは、励起発光性ガスを
封入した透光性管体内にカソードとメツシュ状の7メー
ドとを電子の平均自由行程より短い距離だけ離間させて
配設し、アノードの背後の空間でガス原子を励起発光さ
せるようにした蛍光ランプにおいて、上記励起発光性ガ
スの最適励起電圧付近に電離電圧を有する金属蒸気を上
記励起発光性ガスと共に封入したものであり、励起発光
と電離の役割を分離して2種類のガスにそれぞれ分担さ
せることにより、励起発光と電離を最適電圧で行なわせ
るようにした点に特徴を有するものである。[Disclosure of the Invention] Accordingly, the fluorescent lamp according to the present invention has a cathode and a mesh-like 7-meter spaced apart from each other by a distance shorter than the mean free path of electrons in a translucent tube filled with an excited luminescent gas. In a fluorescent lamp in which gas atoms are excited to emit light in the space behind the anode, a metal vapor having an ionization voltage near the optimum excitation voltage of the excited luminescent gas is sealed together with the excited luminescent gas. This method is characterized in that the roles of excited light emission and ionization are separated and assigned to two types of gas, respectively, so that excited light emission and ionization can be performed at optimal voltages.
[実施例1
第1図は本発明の一実施例を示したもので、1は内面に
蛍光物質が塗布されたプラス製管体であり、管体1内に
はフィラメントで加熱されるカソード3が配置され、こ
のカソード3から電子の平均自由行程以内の距離(例え
ば1c111)だけm関してメツシュ状の電子通過性ア
ノード4が配設されている。以上の構成は従来と同じで
あるが、本発明においては封入ガス2として、例えば水
銀のような励起発光性ガスと共に、励起発光性ガスの最
適励起電圧付近に電離電圧を有する金属蒸気を封入した
点が異なっている。[Embodiment 1] Fig. 1 shows an embodiment of the present invention, in which numeral 1 is a tube made of plastic whose inner surface is coated with fluorescent material, and inside tube 1 is a cathode 3 heated by a filament. is disposed, and a mesh-like electron-transmissive anode 4 is disposed at a distance m within the mean free path of electrons (for example, 1c111) from the cathode 3. The above configuration is the same as the conventional one, but in the present invention, as the sealed gas 2, a metal vapor having an ionization voltage near the optimum excitation voltage of the excited luminescent gas is sealed together with an excited luminescent gas such as mercury. The points are different.
第1表は封入ガスの例を示したもので、同表に示すよう
に、励起発光性ガスとして用いる水銀の最適励起電圧5
.6■に対して、それよりもやや低い電離電圧を持つセ
シウム(電離電圧3,89V)またはナトリウム(電離
電圧5.14V)が電離電圧のみに着目した場合には好
適と言える。Table 1 shows examples of filled gases, and as shown in the table, the optimum excitation voltage of mercury used as an excited luminescent gas
.. Cesium (ionization voltage: 3.89 V) or sodium (ionization voltage: 5.14 V), which have a slightly lower ionization voltage than 6.6, are preferable when focusing only on the ionization voltage.
しかし飽和蒸気圧について見ると、水銀とセシウムの場
合は、励起発光性ガスに対して電離用ガスが1/100
0程度であるから飽和状態で充分使用できるが、水銀と
ナトリウムの場合は、ナトリウムの蒸気圧が非常に低い
ために、管内を高温にしてナトリウム蒸気圧を増加させ
る必要がある上に、その温度において水銀の蒸気圧(不
飽和)が最適となるように水銀の封入量をコントロール
する必要がある。以上の、r:1.から本発明蛍光ラン
プには、水銀とセシウムの組み合わせが最適と言える。However, when looking at the saturated vapor pressure, in the case of mercury and cesium, the ionizing gas is 1/100 of the excited luminescent gas.
However, in the case of mercury and sodium, the vapor pressure of sodium is very low, so it is necessary to raise the temperature inside the tube to increase the sodium vapor pressure. It is necessary to control the amount of mercury enclosed so that the vapor pressure (unsaturation) of mercury is optimal. Above, r:1. Therefore, it can be said that the combination of mercury and cesium is optimal for the fluorescent lamp of the present invention.
[発明の効果]
上述のように本発明においては、電子の急増を防止して
正の電圧−電流特性を持たせ、安定器等の限流要素を省
略するために、アノードカンード開匣離を電子の平均自
由行程よりも短くし、アノードの背後の空間で封入ガス
原子の励起発光を行なわせるようにした蛍光ランプにお
いて、7/−ドの背後空間に発生する空間電荷を中和す
るために管内に弱電離プラズマを形成するための電離作
用を、励起発光用ガスとは別の電離用ガスを用いて行な
わせるようにし、電離用ガスとしてその電離電圧が励起
発光用ガスの最適励起電圧付近にあるものを選んだもの
であるから、励起発光用ガス自体を電aさせる必要がな
く、従って従来例に比しアノード電圧を低くして電子を
最適エネルギレベルに制御することができ、それによっ
てランプの発光効率を高めることができるという利点が
ある。[Effects of the Invention] As described above, in the present invention, in order to prevent a rapid increase in electrons, provide positive voltage-current characteristics, and omit current-limiting elements such as ballasts, the anode cand opening is made by electronics. In a fluorescent lamp whose mean free path is shorter than the mean free path of the anode, the excitation of the gas atoms in the enclosed gas is emitted in the space behind the anode. The ionization effect for forming weakly ionized plasma is performed using an ionization gas different from the excitation emission gas, and the ionization voltage of the ionization gas is close to the optimum excitation voltage of the excitation emission gas. Since it is selected from a certain type of material, there is no need to electrify the gas for excitation and luminescence itself, and therefore the anode voltage can be lowered compared to the conventional example to control the electrons to the optimum energy level, thereby increasing the lamp energy. It has the advantage of increasing the luminous efficiency of.
杭1Mg土木登RJ1労ナランブの一宇施仔11を示す
欅型図であり、1は管体、2は封入ガス、3はカソード
、4はアノード、5はフィラメント用電源、6は電子加
速用電源である。
代理人 弁理士 石 1)長 七
第1図
手続補正書(自発)
昭和61年3月22日It is a keyaki-shaped diagram showing the pile 1Mg civil engineering climbing RJ1 labor naranbu Ichiusesai 11, where 1 is the tube body, 2 is the sealed gas, 3 is the cathode, 4 is the anode, 5 is the power source for filament, and 6 is for electron acceleration. It is a power source. Agent Patent Attorney Ishi 1) Chief 7 Figure 1 procedural amendment (voluntary) March 22, 1986
Claims (2)
ドとメッシュ状のアノードとを電子の平均自由行程より
短い距離だけ離間させて配設し、アノードの背後の空間
でガス原子を励起発光させるようにした蛍光ランプにお
いて、上記励起発光性ガスの最適励起電圧付近に電離電
圧を有する金属蒸気を上記励起発光性ガスと共に封入し
て成る蛍光ランプ。(1) A cathode and a mesh anode are placed in a transparent tube filled with an excited luminescent gas, separated by a distance shorter than the mean free path of electrons, and gas atoms are excited in the space behind the anode. What is claimed is: 1. A fluorescent lamp that emits light, the fluorescent lamp comprising a metal vapor having an ionization voltage near the optimal excitation voltage of the excited luminescent gas and sealed therein with the excited luminescent gas.
属蒸気としてセシウムを使用して成る特許請求の範囲第
1項記載の蛍光ランプ。(2) The fluorescent lamp according to claim 1, wherein mercury is used as the excited luminescent gas and cesium is used as the metal vapor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP521386A JPS62163253A (en) | 1986-01-14 | 1986-01-14 | Fluorescent lamp |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP521386A JPS62163253A (en) | 1986-01-14 | 1986-01-14 | Fluorescent lamp |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS62163253A true JPS62163253A (en) | 1987-07-20 |
JPH0582705B2 JPH0582705B2 (en) | 1993-11-22 |
Family
ID=11604913
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP521386A Granted JPS62163253A (en) | 1986-01-14 | 1986-01-14 | Fluorescent lamp |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62163253A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5003178A (en) * | 1988-11-14 | 1991-03-26 | Electron Vision Corporation | Large-area uniform electron source |
-
1986
- 1986-01-14 JP JP521386A patent/JPS62163253A/en active Granted
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5003178A (en) * | 1988-11-14 | 1991-03-26 | Electron Vision Corporation | Large-area uniform electron source |
Also Published As
Publication number | Publication date |
---|---|
JPH0582705B2 (en) | 1993-11-22 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JPS63141256A (en) | Discharge lamp | |
JP2005513732A (en) | Structure and method for emitting light | |
KR100622439B1 (en) | Method and device for generating optical radiation | |
JPS62163253A (en) | Fluorescent lamp | |
DK73582A (en) | LIGHTING SYSTEM | |
JPH0564417B2 (en) | ||
RU2210140C2 (en) | Method and device for producing optical radiation | |
JPH01102847A (en) | Lighting device for luminous radiating electron tube | |
JPS62163252A (en) | Fluorescent lamp | |
JPS6119049A (en) | Light-emitting electron tube | |
JPS63264859A (en) | Light emitting electron tube | |
JPS61284050A (en) | Light emitting electron tube | |
JPH0531266B2 (en) | ||
JPS6122560A (en) | Light emitting electron tube | |
JPS61101948A (en) | Light emitting electron tube | |
JPS6119050A (en) | Light-emitting electron tube | |
JPS581963A (en) | Low pressure mercury-vapor discharge lamp | |
JPS6212058A (en) | Luminous radiation electron tube | |
JPH0584633B2 (en) | ||
JPS61190851A (en) | Light-emission electron tube | |
JPH0670899B2 (en) | Light emitting electron tube | |
JPS6122559A (en) | Light emitting electron tube | |
JPS62276750A (en) | Luminous radiation electron tube | |
JPS62163254A (en) | Electron tube for light emission | |
JPS61267255A (en) | Light-emission electron tube |