JPH0218560Y2 - - Google Patents

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Publication number
JPH0218560Y2
JPH0218560Y2 JP7287886U JP7287886U JPH0218560Y2 JP H0218560 Y2 JPH0218560 Y2 JP H0218560Y2 JP 7287886 U JP7287886 U JP 7287886U JP 7287886 U JP7287886 U JP 7287886U JP H0218560 Y2 JPH0218560 Y2 JP H0218560Y2
Authority
JP
Japan
Prior art keywords
cavity
waveguide
light
microwave
light source
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.)
Expired
Application number
JP7287886U
Other languages
Japanese (ja)
Other versions
JPS61204399U (en
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 filed Critical
Priority to JP7287886U priority Critical patent/JPH0218560Y2/ja
Publication of JPS61204399U publication Critical patent/JPS61204399U/ja
Application granted granted Critical
Publication of JPH0218560Y2 publication Critical patent/JPH0218560Y2/ja
Expired legal-status Critical Current

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  • Circuit Arrangements For Discharge Lamps (AREA)
  • Discharge Lamps And Accessories Thereof (AREA)

Description

【考案の詳細な説明】 この考案は、マイクロ波放電を利用したマイク
ロ波放電光源装置に関する。
[Detailed Description of the Invention] This invention relates to a microwave discharge light source device that utilizes microwave discharge.

最近、放電利用の光源装置として、高周波放
電、特に高周波としてマイクロ波を用いた光源装
置が注目されている。従来の有電極の光源装置で
は、ランプの寿命が電極の消耗により決定されて
いたが、マイクロ波を用いた光源装置では、ラン
プを無電極にできるため、ランプ寿命が長くなる
という特徴がある。
BACKGROUND ART Recently, light source devices that use high-frequency discharge, particularly microwaves as high-frequency waves, have been attracting attention as light source devices that utilize electric discharge. In conventional light source devices with electrodes, the life of the lamp is determined by the wear and tear of the electrodes, but in light source devices using microwaves, the lamp can be made electrodeless, so the lamp life can be extended.

さらに、電極による熱損失がなく、しかも、放
電のインピーダンスが初期状態と安定状態で差が
小さいため、安定状態でインピーダンス整合させ
た場合でも、初期状態での電力注入が容易であ
り、また、放電電力がランプ管壁に偏つているな
どのために、最大出力到達までの時間が短くなる
という特徴もある。
Furthermore, since there is no heat loss due to electrodes, and the difference in discharge impedance is small between the initial state and the stable state, it is easy to inject power in the initial state even when impedance matching is performed in the stable state. Another characteristic is that the time it takes to reach maximum output is short because the power is concentrated on the lamp tube wall.

第1図は、これらの特長を利用した本考案者ら
の先行発明によるマイクロ波放電光源装置の構成
を示す縦断面図で、1はマグネトロン、2はマグ
ネトロンアンテナ、3は導波管、4は内壁の反射
面を形成する部分を球面41に、それにつづく部
分を円筒面42に形成するとともに光通過面とな
る面を金属メツシユ板43で覆つた構成としたマ
イクロ波共振空胴、44は円筒面42を覆う光無
反射処理層、5は空胴4と導波管3の接合部に設
けられたマイクロ波給電口、6は球形に形成され
た放電灯、61は放電灯6の管壁に形成された支
持用の突起、7はマグネトロン1および放電灯6
を冷却するためのフアン、8は導波管3の一部に
設けられた通気口、10はマグネトロン1、導波
管3、空胴4等を収容する箱体、11は突起61
に嵌合して放電灯6を支持する支持棒である。
FIG. 1 is a longitudinal cross-sectional view showing the configuration of a microwave discharge light source device according to an earlier invention by the present inventors that takes advantage of these features, in which 1 is a magnetron, 2 is a magnetron antenna, 3 is a waveguide, and 4 is a A microwave resonant cavity having a configuration in which a portion of the inner wall forming a reflective surface is formed into a spherical surface 41, a portion following it is formed into a cylindrical surface 42, and the surface serving as a light passing surface is covered with a metal mesh plate 43, 44 is a cylinder. A light anti-reflection treatment layer covering the surface 42, 5 a microwave power feed port provided at the junction of the cavity 4 and the waveguide 3, 6 a spherical discharge lamp, and 61 a tube wall of the discharge lamp 6. A supporting protrusion 7 is formed on the magnetron 1 and the discharge lamp 6.
8 is a vent provided in a part of the waveguide 3; 10 is a box housing the magnetron 1, the waveguide 3, the cavity 4, etc.; 11 is a projection 61;
This is a support rod that supports the discharge lamp 6 by fitting into it.

この装置の動作は次のようである。マグネトロ
ン1によつて発生したマイクロ波は、マグネトロ
ンアンテナ2を通じて導波管3中に放射される。
このマイクロ波は、導波管3を伝播し、給電口5
を通して空胴4中に放射され、空胴4中にマイク
ロ波電磁界を形成する。このマイクロ波電磁界に
より、放電灯6中のガスが放電し、放電灯の内壁
が熱せられ、管中にある水銀等の金属が蒸発しガ
ス化されて、放電は金属ガスの放電に移る。この
時、金属の種類に応じた特定の発光スペクトルを
持つ光が発生するので、これを光源として用い
る。この放電灯6からの光を有効に利用するた
め、空胴4の球面部分を反射板として用い、前面
はマイクロ波は遮断するが光は透過する金属メツ
シユ板43で構成して光を前方のみに放射させ
る。一方、マグネトロン1および放電灯6は動作
中冷却する必要があるため、冷却フアン7により
送風し、この冷却空気は通気口8、導波管3およ
び給電口5を経てランプ6を冷却した後メツシユ
板10から排気される。
The operation of this device is as follows. Microwaves generated by the magnetron 1 are radiated into a waveguide 3 through a magnetron antenna 2.
This microwave propagates through the waveguide 3 and feeds into the feed port 5.
is radiated into the cavity 4 through the microwave, forming a microwave electromagnetic field within the cavity 4. Due to this microwave electromagnetic field, the gas in the discharge lamp 6 is discharged, the inner wall of the discharge lamp is heated, the metal such as mercury in the tube is evaporated and gasified, and the discharge shifts to a discharge of metal gas. At this time, light with a specific emission spectrum depending on the type of metal is generated, and this is used as a light source. In order to effectively utilize the light from the discharge lamp 6, the spherical part of the cavity 4 is used as a reflector, and the front surface is made up of a metal mesh plate 43 that blocks microwaves but transmits light, so that the light is directed only in front. radiate to. On the other hand, since the magnetron 1 and the discharge lamp 6 need to be cooled during operation, they are blown by a cooling fan 7, and this cooling air passes through the vent 8, the waveguide 3, and the power supply port 5, cools the lamp 6, and then cools the mesh. Air is exhausted from the plate 10.

第2図は、第1図−から空胴4を、メツシ
ユ板43および箱体10を取り去つて見た給電口
5の位置を示す図で、導波管3の位置を破線で示
す。空胴4の内壁の球面部分41は光の反射面と
して使用するため、アルミニウム等を用いて鏡面
に仕上げている。このように構成された装置で
は、放電灯6が球面部分41の中心付近に位置し
ていれば、球面での反射光が放電灯6付近に集合
するため、前面へ放射される光は、点光源からの
光に近似したものとなる。しかし、球面部分41
の一部には給電口5が開口しているため、反射面
とはならずに、この部分に当たる光は導波管3内
へ漏れ、この分だけ前面へ取り出せる光の量が少
なくなる。
FIG. 2 is a diagram showing the position of the feed port 5 when the cavity 4 is viewed from FIG. 1 with the mesh plate 43 and the box body 10 removed, and the position of the waveguide 3 is shown by a broken line. The spherical surface portion 41 of the inner wall of the cavity 4 is used as a light reflecting surface, so it is finished with a mirror surface using aluminum or the like. In the device configured in this way, if the discharge lamp 6 is located near the center of the spherical portion 41, the light reflected from the spherical surface will be concentrated near the discharge lamp 6, so that the light emitted to the front will become a point. It approximates the light from a light source. However, the spherical part 41
Since the feed port 5 is open in a part of the mirror, the light that hits this part leaks into the waveguide 3 without serving as a reflective surface, and the amount of light that can be taken out to the front is reduced by this amount.

この考案は、上記のような無効光の割合を少な
くするためなされたもので、給電口5を、空胴4
の反射面を形成しない部分に設けることで、無効
光の割合の少ないマイクロ波放電光源装置を提供
することを目的としている。
This idea was made to reduce the proportion of invalid light as described above, and the power feed port 5 is connected to the cavity 4.
It is an object of the present invention to provide a microwave discharge light source device in which the proportion of invalid light is small by providing the reflective surface in a portion where no reflective surface is formed.

第3図は、この考案の一実施例の構成を示す縦
断面図、第4図は、第3図−より空胴4を、
メツシユ板43を取り去つて前面より見た図で、
円筒部分42に給電口5を設けている。給電口5
の位置は、空胴内の電磁界モードと導波管内の電
磁界モードに密接に関係がある。
FIG. 3 is a vertical sectional view showing the configuration of an embodiment of this invention, and FIG. 4 shows the cavity 4 from FIG. 3.
This is a view seen from the front with the mesh plate 43 removed.
A power feeding port 5 is provided in the cylindrical portion 42. Power supply port 5
The position of is closely related to the electromagnetic field modes within the cavity and the electromagnetic field modes within the waveguide.

第5図は、第1図のような、空胴4の後面に導
波管3の端面より給電する構成とした場合に、給
電可能なモードの例を中心軸を含むある断面で見
た図、第6図は、第5図−線から見た断面図
である。図中Eは電界を、Hは磁界を示し、図の
ように、導波管3のモードと結合し易いモードが
給電可能となる。一方、第3図のような、空胴4
の側面に導波管3の端面より給電した場合に、給
電できるモードの一例を第7図、第8図に示す。
第7図は中心軸を含むある断面で見た図、第8図
は第7図−線よりみた断面図である。第7
図、第8図で示すように、側面より給電する場合
には、後面より給電する場合と異なつたモードを
励振することになる。このため、空胴の寸法は異
なつた寸法になる。
FIG. 5 is a cross-sectional view of an example of a mode that can be fed when power is fed to the rear surface of the cavity 4 from the end face of the waveguide 3, as shown in FIG. , FIG. 6 is a sectional view taken along the line of FIG. In the figure, E indicates an electric field and H indicates a magnetic field, and as shown in the figure, a mode that easily couples with the mode of the waveguide 3 can be fed. On the other hand, as shown in Figure 3, the cavity 4
An example of a mode in which power can be supplied when power is supplied to the side surface of the waveguide 3 from the end face of the waveguide 3 is shown in FIGS. 7 and 8.
FIG. 7 is a cross-sectional view including the central axis, and FIG. 8 is a cross-sectional view taken along the line of FIG. 7. 7th
As shown in FIG. 8, when power is supplied from the side, a different mode is excited than when power is supplied from the rear. For this reason, the dimensions of the cavities will be of different dimensions.

すなわち、側面より給電した場合、給電できる
電磁界モードに対する空胴の寸法を円筒部分42
の長さを変えて求めれば、反射面である球面41
の寸法を変えずに、すなわち光に対しては大きな
影響を与えずに空胴の寸法を決定できる。
In other words, when power is supplied from the side, the dimensions of the cavity for the electromagnetic field mode that can be supplied are determined by the cylindrical portion 42.
If we change the length of
The dimensions of the cavity can be determined without changing the dimensions of the cavity, that is, without significantly affecting the light.

このようにして、反射面として使用しない側面
に給電口を設けることができ、球面部分41はす
べて反射面となるため、前面へ取り出せる光の量
を多くできる。
In this way, the power supply port can be provided on the side surface that is not used as a reflective surface, and since the entire spherical portion 41 becomes a reflective surface, it is possible to increase the amount of light that can be taken out to the front surface.

以上のように、この考案のマイクロ波放電光源
装置によれば、空胴を光反射面を構成する球面部
分とこれにつづく光無反射処理が施されている円
筒部分とこの円筒部分の開口部を覆う金属メツシ
ユ板とで構成し、上記無電極放電灯を上記球面部
分の中心に配設するとともに上記円筒部分に上記
導波管の給電口を設けたので、前面へ取り出せる
光の量を多くでき、しかも均一性を向上させるこ
とができる。
As described above, according to the microwave discharge light source device of this invention, the cavity consists of a spherical part constituting a light reflecting surface, a cylindrical part that is subjected to anti-reflection treatment, and an opening in this cylindrical part. The electrodeless discharge lamp is arranged in the center of the spherical part, and the power supply port of the waveguide is provided in the cylindrical part, so that a large amount of light can be taken out to the front. Moreover, the uniformity can be improved.

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

第1図は従来のマイクロ波放電光源装置の構成
を示す縦断面図、第2図は第1図−線より空
胴を見た図、第3図はこの考案の一実施例を示す
縦断面図、第4図は第3図−線より空胴を見
た図、第5図および第6図は従来のマイクロ波放
電光源装置の空胴内電磁界の一例を示す図、第7
図および第8図はこの考案のマイクロ波放電光源
装置の空胴内電磁界の一例を示す図である。 図において1はマグネトロン、3は導波管、4
はマイクロ波共振空胴、41は球面部分、42は
円筒部分、43はメツシユ板、44は無反射処理
層、5は給電口、6は無電極放電灯、61は支持
用突起、11は支持棒である。なお、図中同一符
号はそれぞれ同一または相当部分を示す。
Fig. 1 is a longitudinal cross-sectional view showing the configuration of a conventional microwave discharge light source device, Fig. 2 is a view of the cavity seen from the line in Fig. 1, and Fig. 3 is a longitudinal cross-sectional view showing an embodiment of this invention. Figure 4 is a view of the cavity seen from the line in Figure 3, Figures 5 and 6 are diagrams showing an example of the electromagnetic field inside the cavity of a conventional microwave discharge light source device,
8 and 8 are diagrams showing an example of the electromagnetic field within the cavity of the microwave discharge light source device of this invention. In the figure, 1 is a magnetron, 3 is a waveguide, and 4
is a microwave resonant cavity, 41 is a spherical part, 42 is a cylindrical part, 43 is a mesh plate, 44 is a non-reflection treated layer, 5 is a power feed port, 6 is an electrodeless discharge lamp, 61 is a supporting protrusion, 11 is a support It's a stick. Note that the same reference numerals in the figures indicate the same or corresponding parts.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] マイクロ波発振器から導波管で球形の無電極放
電灯を収容せる空胴内にマイクロ波を導入し、上
記空胴の一面を形成せる金属メツシユ板をとおし
て光を放射させるように構成したものにおいて、
上記空胴を光反射面を構成する球面部分とこれに
つづく光無反射処理が施されている円筒部分とこ
の円筒部分の開口部を覆う金属メツシユ板とで構
成し、上記無電極放電灯を上記球面部分の中心に
配設するとともに上記円筒部分に上記導波管の給
電口を設けた構成としたことを特徴とするマイク
ロ波放電光源装置。
A device configured so that microwaves are introduced from a microwave oscillator into a cavity that accommodates a spherical electrodeless discharge lamp using a waveguide, and the light is emitted through a metal mesh plate that forms one side of the cavity. In,
The cavity is composed of a spherical part that constitutes a light reflecting surface, a cylindrical part that is treated with anti-reflection treatment, and a metal mesh plate that covers the opening of this cylindrical part, and the electrodeless discharge lamp is A microwave discharge light source device characterized in that the microwave discharge light source device is arranged at the center of the spherical portion and has a power feeding port of the waveguide provided in the cylindrical portion.
JP7287886U 1986-05-15 1986-05-15 Expired JPH0218560Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7287886U JPH0218560Y2 (en) 1986-05-15 1986-05-15

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7287886U JPH0218560Y2 (en) 1986-05-15 1986-05-15

Publications (2)

Publication Number Publication Date
JPS61204399U JPS61204399U (en) 1986-12-23
JPH0218560Y2 true JPH0218560Y2 (en) 1990-05-23

Family

ID=30611705

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7287886U Expired JPH0218560Y2 (en) 1986-05-15 1986-05-15

Country Status (1)

Country Link
JP (1) JPH0218560Y2 (en)

Also Published As

Publication number Publication date
JPS61204399U (en) 1986-12-23

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