JPS61161649A - Microwave discharging light source device - Google Patents
Microwave discharging light source deviceInfo
- Publication number
- JPS61161649A JPS61161649A JP113485A JP113485A JPS61161649A JP S61161649 A JPS61161649 A JP S61161649A JP 113485 A JP113485 A JP 113485A JP 113485 A JP113485 A JP 113485A JP S61161649 A JPS61161649 A JP S61161649A
- Authority
- JP
- Japan
- Prior art keywords
- lamp
- protrusion
- microwave
- light source
- source device
- 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
- H01J65/00—Lamps without any electrode inside the vessel; Lamps with at least one main electrode outside the vessel
- H01J65/04—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels
- H01J65/042—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels by an external electromagnetic field
- H01J65/044—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels by an external electromagnetic field the field being produced by a separate microwave unit
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Non-Portable Lighting Devices Or Systems Thereof (AREA)
- Discharge Lamps And Accessories Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明はマイクa波放IE7f!:利用した光源装置
。[Detailed Description of the Invention] [Industrial Application Field] This invention is a microphone A-wave broadcasting IE7f! : Light source device used.
とくにランプの冷却効率の向上に関するものでろる0
〔従来の技術〕
第3図は例えば実開昭59−158119に示された従
来のマイクロ波放電光源装置を示す断面図でるり2図に
おいて(1)はマグネトロン、(21はマグネトコンア
ンテナ、131は導波管、(4?は通風口、【52はマ
イクロ波共振空洞で、導波管+31の端部に接続された
空洞壁(6)と円筒型の金属メツシュよりなる光透過性
部材(7)とから構成される。(8)は空洞壁(6)に
設けられ次給電口で、導波管+31よりマイクロ波共振
空洞(5]内にマイクロ波を給電するためのものである
。193はマイクロ波共振空洞(5)内に配設された球
形の無電極ラングでbるot+Gi’!ラング支持褌で
ランプ固定部αυと接着材t13で接着され、ランプ固
定部αDは空洞壁(61にネジα3で固定されている。[Prior Art] Figure 3 is a sectional view showing a conventional microwave discharge light source device shown in, for example, Utility Model Application Publication No. 59-158119. ) is a magnetron, (21 is a magnetocon antenna, 131 is a waveguide, (4? is a ventilation hole, [52 is a microwave resonant cavity, and the cavity wall (6) is connected to the end of the waveguide +31. It consists of a light transmitting member (7) made of a cylindrical metal mesh.(8) is a secondary feed port provided in the cavity wall (6), and is connected from the waveguide +31 into the microwave resonant cavity (5). 193 is a spherical electrodeless rung placed inside the microwave resonant cavity (5), which connects the lamp fixing part αυ and the adhesive t13 with a rung supporting loincloth. The lamp fixing part αD is fixed to the cavity wall (61) with a screw α3.
a41F1ラング+91から放射された光を反射する反
射板、19はマグネトロン(11やラング191を冷却
する冷却ファン、 tteは全体を覆う箱体である。(
17’)は突起状の肉厚部でろる。A reflector that reflects the light emitted from the a41F1 rung +91, 19 is a cooling fan that cools the magnetron (11) and rung 191, and tte is a box that covers the entire thing. (
17') has a protruding thick part.
次にかかるものの動作について説明する。マグネトロン
(1)で発振されたマイクロ波はマグネトロンアンテナ
(21を通じて導波管(3)中に放射され、このマイク
ロ波は導波管(3)を伝播し、給電口(8)を通してマ
イクa波共振空洞(5)内に放射され、空洞15ン内に
マイクロ波電磁界を形成する。このマイクロ波電磁界に
よシラング(9)内のガスが放電し、管壁が熱せられ、
ランプ(9]内の水銀等の金属が蒸発し。Next, the operation of this system will be explained. The microwave oscillated by the magnetron (1) is radiated into the waveguide (3) through the magnetron antenna (21), this microwave propagates through the waveguide (3), and is transmitted through the feed port (8) into the microphone A wave. It is radiated into the resonant cavity (5) and forms a microwave electromagnetic field inside the cavity 15. This microwave electromagnetic field discharges the gas inside the silange (9) and heats the tube wall.
Metals such as mercury in the lamp (9) evaporate.
ガス化され金属ガスの放電が起る0このとき金属の種類
に応じた特有の発光スペクトルをもつ光が発生する。こ
の光は円筒形の金属メツシュ(7)を透過し、空洞(5
)の外部に放射され1反射板a4により反射され、前方
に放射される。一方マグネトロン(1)およびラング1
91 ilt冷却する必要がある九め、7アンαSによ
シ送風してマグネトロン11)を冷却し。When the metal gas is gasified and discharge occurs, light having a unique emission spectrum depending on the type of metal is generated. This light passes through the cylindrical metal mesh (7) and passes through the cavity (5).
), is reflected by the first reflecting plate a4, and is emitted forward. On the other hand, magnetron (1) and rung 1
91 It is necessary to cool the magnetron 11) by blowing air through the 7th An αS.
さらにこの送気は通気口(旬および給電口(8)を通し
てランプ19)を冷却した後円筒形金属メツシュ(7)
より排気される。Furthermore, this air cools the lamp 19 through the ventilation port (transmission and power supply port (8)), and then the cylindrical metal mesh (7).
More exhaust.
C考案が解決しようとする問題点〕
上記のような従来のマイクロ波放電光源装置におけるラ
ンプ(9)の冷却は、冷風の直接当るランプ193の給
電口(8)側がよく冷却されろが、給電口(8)と反対
側は冷却され難く、ランプの過熱による劣化が難しく、
短寿命の原因でめった。この発明は。Problems to be Solved by the C Design] The cooling of the lamp (9) in the conventional microwave discharge light source device as described above is such that the power supply port (8) side of the lamp 193, which is directly exposed to the cold air, is well cooled. The side opposite the opening (8) is difficult to cool and is difficult to deteriorate due to overheating of the lamp.
Rare due to short lifespan. This invention.
か\る問題点を解決するためになされたもので。This was done to solve the following problems.
ラングの給電口と反対flllをも効果的に冷却し、過
熱を防止し、ランプの劣化を防止し、ラングの長寿命化
を目的とする。更にラングの高出力化をも可能にするも
のである。The aim is to effectively cool the power supply port and the opposite flll of the rung, prevent overheating, prevent deterioration of the lamp, and extend the life of the rung. Furthermore, it is possible to increase the output of the rung.
この発明に係るマイクロ波放電光源装置は、気体の吹き
出し方向と反対側のラング管壁部分に長さ100以上の
突起を設けたものである。またこの発明の別の発明に係
るマイクロ波放電光源装置は、気体の吹き出し方向と反
対側のラング管壁に設は次突起の頂部をマイクロ波空洞
壁に接触させたものである。The microwave discharge light source device according to the present invention has a projection having a length of 100 or more on the wall portion of the rung tube on the opposite side to the gas blowing direction. Further, in a microwave discharge light source device according to another aspect of the present invention, the top of a protrusion is provided on the rung tube wall on the opposite side to the gas blowing direction, and the top of the protrusion is brought into contact with the microwave cavity wall.
ランプに向けて吹き出され乏気体が、ランプに設けた長
さが101I11以上の突起に泪って流れるようになる
念め、従来気体が直接的に当り忙くかつ之気体の吹き出
し方向と反対側の管壁の熱放散が促進される。また、突
起を空洞壁に直接接触させたので、ラングからの熱が空
洞壁に移動し、一層の冷却効果が期待できる。In order to ensure that the poor gas blown out toward the lamp flows through a protrusion with a length of 101111 or more provided on the lamp, conventionally, the gas is directly hit and the opposite side to the direction of the gas blowing out. heat dissipation from the tube wall is promoted. In addition, since the protrusions are brought into direct contact with the cavity wall, heat from the rung is transferred to the cavity wall, and further cooling effects can be expected.
第1図はこの発明の一実施例を示すマイクロ波数′鑞光
源装置の断面図でおり、第2図はこの装置に使用される
改良されたラングの構造を示す断面図でわろ。図におい
て、(l]〜αeFi上記従来装置と全く同一のもつで
ある。傾はランプ支持棒1(Iと反対側のランプ管壁に
設けられた長さ10麿以上の突起でるる。この突起an
は空洞壁(7)に接触させてもよい。この場合は長さが
必らずしもtOW以上でるる必要はない。(11Iは給
゛電口(8)から吹き出される冷風の流れを示した流線
でめる0
給鑞口(8:から吹き出された冷風はランプの給電口1
8)側をよく冷却し、給電口(8)の反対側は冷風によ
る冷却よりも、給電口(8)と反対側に設けられた1a
wt以上の突起αnからの熱伝導により冷却される。な
お突起aηの長さ10I未満の場合は効果が不充分であ
った。ところで上記説明では、ランプの支持棒四側から
冷却風をランプに轟てろ場合について述べたが、これ以
外の方向からラングに冷却風を当てる場合にも適用でき
ることは云うまでもない。FIG. 1 is a cross-sectional view of a microwave number 100-degree light source device showing one embodiment of the present invention, and FIG. 2 is a cross-sectional view showing the structure of an improved rung used in this device. In the figure, (l) to αeFi are exactly the same as the above-mentioned conventional device. an
may be in contact with the cavity wall (7). In this case, the length does not necessarily have to be greater than tOW. (11I is defined by a streamline showing the flow of cold air blown from the power supply port (8).) The cold air blown from the power supply port (8) is
8) side, and the opposite side of the power supply port (8) is cooled by cold air.
It is cooled by heat conduction from the protrusion αn which is larger than wt. Note that when the length of the protrusion aη was less than 10I, the effect was insufficient. By the way, in the above explanation, the case where the cooling air is blown onto the lamp from the four sides of the support rod of the lamp has been described, but it goes without saying that the present invention can also be applied to the case where the cooling air is blown onto the rung from other directions.
この発明は以上説明し友とおり、冷却風の吹き出し方向
と反対側のランプ管壁部分に10f1以上の突起を設け
るという簡単な構造により、冷却風の影になる吹出し方
向と反対側のラング管壁の過熱を防止し、ランプの短寿
命を防止できろ。また。As described above, this invention has a simple structure in which a protrusion of 10 f1 or more is provided on the lamp tube wall portion on the opposite side to the cooling air blowing direction. Prevent the lamp from overheating and shorten the life of the lamp. Also.
突起をマイクロ波空洞壁に接触させたため+ ’*
の冷却効果が向上し、ラング全体の過熱防止もでき、高
出力化も可能となる効果がろる。Because the protrusion was in contact with the microwave cavity wall + '*
This improves the cooling effect of the rung, prevents overheating of the entire rung, and enables higher output.
第1図はこの発明の一実施例を示す断面図、第2図は改
良され念ランプ構造を示す断面図、第3図は従来のマイ
クロ波放電光源装置を示す断面図でおる。
図において、 (1)はマグネトロン、(2:はマグネ
トロンアンテナ、(31は導波管、(41は通風口、(
5)はマイクロ波共振空洞、(6:は空洞壁、(7)は
光透過性部材、(8)は給電口、(9Jはランプ、αl
はラング支持棒。
αDはラング固定部、惺zは接着材、(13はネジ、(
14は反射板、α9は冷却ファン、IIsは箱体、α刀
は突起2(17°)は突起状の肉厚部、 (USは流線
である。なお。
各図中同一符号は同一ま九は相当部分を示す。FIG. 1 is a sectional view showing an embodiment of the present invention, FIG. 2 is a sectional view showing an improved thought lamp structure, and FIG. 3 is a sectional view showing a conventional microwave discharge light source device. In the figure, (1) is a magnetron, (2: is a magnetron antenna, (31 is a waveguide, (41 is a ventilation hole, (
5) is a microwave resonant cavity, (6: is a cavity wall, (7) is a light-transmitting member, (8) is a power supply port, (9J is a lamp, αl
is a rung support rod. αD is the rung fixing part, z is the adhesive, (13 is the screw, (
14 is a reflector, α9 is a cooling fan, IIs is a box body, α sword protrusion 2 (17°) is a protruding thick part, (US is a streamline. Note that the same symbols in each figure are the same or different. 9 indicates a considerable portion.
Claims (2)
される無電極放電ランプ、このランプに気体を吹き付け
て冷却させるランプ強制冷却手段を有するものにおいて
、気体の吹き出し方向と反対側のランプ管壁部分に長さ
が10mm以上となる突起を設けたことを特徴とするマ
イクロ波放電光源装置。(1) In an electrodeless discharge lamp that emits light excited by microwaves in a microwave cavity, and has forced lamp cooling means for cooling the lamp by blowing gas onto it, the lamp tube wall portion on the opposite side from the direction in which the gas is blown out. A microwave discharge light source device, characterized in that a protrusion having a length of 10 mm or more is provided.
される無電極放電ランプ、このランプに気体を吹き付け
て冷却させるランプ強制冷却手段を有するものにおいて
、気体の吹き出し方向と反対側のランプ管壁部分に任意
の長さの突起を設け、この突起の頂部をマイクロ波空洞
の壁面に接触させたことを特徴とするマイクロ波放電光
源装置。(2) In an electrodeless discharge lamp that emits light excited by microwaves in a microwave cavity, and has forced lamp cooling means for cooling the lamp by blowing gas onto it, the lamp tube wall portion on the side opposite to the direction in which the gas is blown out. 1. A microwave discharge light source device characterized in that a protrusion of arbitrary length is provided on the holder, and the top of the protrusion is brought into contact with a wall surface of a microwave cavity.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP113485A JPS61161649A (en) | 1985-01-08 | 1985-01-08 | Microwave discharging light source device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP113485A JPS61161649A (en) | 1985-01-08 | 1985-01-08 | Microwave discharging light source device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61161649A true JPS61161649A (en) | 1986-07-22 |
Family
ID=11492971
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP113485A Pending JPS61161649A (en) | 1985-01-08 | 1985-01-08 | Microwave discharging light source device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61161649A (en) |
-
1985
- 1985-01-08 JP JP113485A patent/JPS61161649A/en active Pending
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