JPH0130254B2 - - Google Patents

Info

Publication number
JPH0130254B2
JPH0130254B2 JP153786A JP153786A JPH0130254B2 JP H0130254 B2 JPH0130254 B2 JP H0130254B2 JP 153786 A JP153786 A JP 153786A JP 153786 A JP153786 A JP 153786A JP H0130254 B2 JPH0130254 B2 JP H0130254B2
Authority
JP
Japan
Prior art keywords
microwave
light
mesh plate
metal mesh
discharge lamp
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
JP153786A
Other languages
Japanese (ja)
Other versions
JPS61165950A (en
Inventor
Kenji Yoshizawa
Hitoshi Kodama
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP153786A priority Critical patent/JPS61165950A/en
Publication of JPS61165950A publication Critical patent/JPS61165950A/en
Publication of JPH0130254B2 publication Critical patent/JPH0130254B2/ja
Granted legal-status Critical Current

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  • Non-Portable Lighting Devices Or Systems Thereof (AREA)
  • Discharge Lamps And Accessories Thereof (AREA)

Description

【発明の詳細な説明】 この発明は、マイクロ波放電による発光を利用
したマイクロ波放電光源装置に関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a microwave discharge light source device that utilizes light emission by microwave discharge.

第1図は、先行技術に係るマイクロ波放電光源
装置を示すものであり、図において、1はマイク
ロ波を発生するマグネトロンであるマイクロ波発
振器、2はマグネトロンアンテナ、3はマイクロ
波を伝送する導波管、4は球面部5とこれに続く
円筒部6からなり、アルミニウム等で形成された
空胴壁、7は押えフランジ8と押えネジ9とで空
胴壁4のフランジ部10に装着された金属メツシ
ユ板で、マイクロ波は遮断するが、光を透過する
ものであり、上記空胴壁4とでマイクロ波空胴1
1を構成する。12は導波管3と空胴壁4の接合
部に設けられた給電口、13は球面部5の中心近
傍に配設された球形の放電灯で、石英ガラス等で
形成され、内部にアルゴン等の希ガス、水銀、鉄
等の金属およびヨウ素等のハロゲンが封入されて
いる。14は放電灯13の外壁の一部に設けられ
た突起で、石英ガラスのような低損失の誘電体の
放電灯支持体15の一部がフレア状となつた放電
灯支持部16に嵌合し放電灯13を支持するもの
である。17は空胴壁4の一部に設けられ、放電
灯支持体15の他端が挿入されてこれを支持する
放電灯支持体支接部、18は金属メツシユ板7よ
り外部へ放射される光を被照射面(図示せず)に
集光させるためのレンズである。
FIG. 1 shows a microwave discharge light source device according to the prior art. In the figure, 1 is a microwave oscillator that is a magnetron that generates microwaves, 2 is a magnetron antenna, and 3 is a guide that transmits microwaves. The wave tube 4 consists of a spherical part 5 and a cylindrical part 6 following it, and a cavity wall made of aluminum or the like, and 7 is attached to the flange part 10 of the cavity wall 4 with a holding flange 8 and a holding screw 9. It is a metal mesh plate that blocks microwaves but transmits light.
1. 12 is a power supply port provided at the joint between the waveguide 3 and the cavity wall 4; 13 is a spherical discharge lamp disposed near the center of the spherical portion 5; it is made of quartz glass or the like; It contains rare gases such as mercury, metals such as iron, and halogens such as iodine. 14 is a protrusion provided on a part of the outer wall of the discharge lamp 13, and a part of the discharge lamp support 15 made of a low-loss dielectric material such as quartz glass fits into the flared discharge lamp support part 16. It supports the discharge lamp 13. 17 is a discharge lamp support support part provided in a part of the cavity wall 4 into which the other end of the discharge lamp support 15 is inserted and supports it; 18 is a light emitted from the metal mesh plate 7 to the outside; This is a lens for condensing the light onto an irradiated surface (not shown).

次にこの様に構成されたマイクロ波放電光源装
置の動作について説明する。マグネトロン1によ
つて発生されたマイクロ波が、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、このマイ
クロ波が、導波管3を伝播し、給電口12を通し
てマイクロ波空胴11中に放射され、マイクロ波
空胴11中にマイクロ波電磁界により、放電灯1
3中のガスが放電し、封入金属の種類に応じた特
定の発光スペクトルを持つ光が放射される。空胴
壁4の球面部5を光反射面にしておけば、放電灯
13が球面部5の中心近傍にあるため、反射光は
再び放電灯13近傍を通過することになる。この
反射光と放電灯13の直接光が金属メツシユ板7
を通して外方へ放射される。外方へ放射された光
は集光レンズ18等で必要な被照射面に集光され
るものである。
Next, the operation of the microwave discharge light source device configured as described above will be explained. Microwaves generated by the magnetron 1 are radiated into the waveguide 3 through the magnetron antenna 2, and the microwaves propagate through the waveguide 3 and are radiated into the microwave cavity 11 through the feed port 12. The discharge lamp 1 is activated by the microwave electromagnetic field in the microwave cavity 11.
The gas in 3 is discharged, and light with a specific emission spectrum depending on the type of metal enclosed is emitted. If the spherical portion 5 of the cavity wall 4 is made a light reflecting surface, the discharge lamp 13 will be located near the center of the spherical portion 5, so that the reflected light will pass through the vicinity of the discharge lamp 13 again. This reflected light and the direct light of the discharge lamp 13 are applied to the metal mesh plate 7.
radiates outward through the The light emitted outward is condensed onto a necessary irradiated surface by a condenser lens 18 or the like.

この様に構成されたマイクロ波放電光源装置に
あつては、金属メツシユ板7はマイクロ波の外部
への漏洩が人体へ影響を及ぼさないレベル以下に
抑え、しかも光の透過率を良好に保つ必要があ
る。このためには周波数2450MHz、出力800Wの
マグネトロンを使用した場合、金属メツシユのピ
ツチ1.5mm、線巾0.1mmにすれば、金属メツシユ外
部でのマイクロ波漏洩電波レベルは1mW/cm2
下に抑えることができる。金属メツシユ板は接触
抵抗によるマイクロ波損失を避けるため、通常、
金属線を網んだものを用いず、金属薄板からエツ
チング等で製作したものを用いる。第2図はメツ
シユ板の部分拡大平面図で素線71のピツチが
wp、最大線巾がwsである。上記例では素線71
の断面形状は厚みが0.1mm、幅0.1mmの矩形状とな
るため、光の透過率は約87%であるが、斜め方向
の光透過率は低下し、マイクロ波空胴11の外方
への光の透過は全体として、87%以下となる。
In the microwave discharge light source device configured in this manner, the metal mesh plate 7 must suppress the leakage of microwaves to the outside to a level that does not affect the human body, and maintain good light transmittance. There is. For this purpose, when using a magnetron with a frequency of 2450 MHz and an output of 800 W, if the metal mesh pitch is 1.5 mm and the wire width is 0.1 mm, the microwave leakage level outside the metal mesh can be suppressed to 1 mW/cm 2 or less. Can be done. Metal mesh plates are usually used to avoid microwave loss due to contact resistance.
Instead of using a mesh of metal wires, one made from a thin metal plate by etching or the like is used. Figure 2 is a partially enlarged plan view of the mesh plate, showing the pitch of the strands 71.
w p and the maximum line width is w s . In the above example, the strand 71
Since the cross-sectional shape of is rectangular with a thickness of 0.1 mm and a width of 0.1 mm, the light transmittance is approximately 87%, but the light transmittance in the diagonal direction decreases and the light is transmitted to the outside of the microwave cavity 11. Overall, the light transmission is less than 87%.

この発明は、以上の点を鑑み、斜め方向の光透
過率の良い断面形状とした金属メツシユにするこ
とにより、光の利用効率を高めたものである。
In view of the above points, the present invention improves the efficiency of light utilization by providing a metal mesh with a cross-sectional shape that has good light transmittance in an oblique direction.

第3図はこの発明の一実施例であるメツシユ板
の断面図で、メツシユの素線71の断面を三角形
としたものである。このメツシユ板7に、図の矢
印で示す斜め光線が入射した場合、メツシユ外方
では図のsで示す領域は影となつて、透過光がさ
えぎられる。この影のB―B線で示すメツシユ面
に平行な面への投影を考えれば、第3図の拡大図
である第4図で示すように素線71の投影の巾は
Wsb、ピツチはWpbである。入射光がメツシユ面
へ垂直から図で示すθの角度までの投影では
wsb,Wpb共に、垂直入射光の投影巾Wsa、ピツチ
Wpaに等しい。すなわち、垂直からθの角度まで
は入射光透過率の低下はなく、光の利用効率は下
がらない。一方、マイクロ波の漏洩は、メツシユ
素線のピツチと最大巾によつて決まるため、ピツ
チと最大巾が同じであれば素線断面形状が変化し
ても変化はない。
FIG. 3 is a sectional view of a mesh plate according to an embodiment of the present invention, in which the cross section of the strands 71 of the mesh is triangular. When an oblique light beam shown by an arrow in the figure is incident on the mesh plate 7, the area shown by s in the figure becomes a shadow outside the mesh, and the transmitted light is blocked. Considering the projection of this shadow onto a plane parallel to the mesh plane shown by line BB, the width of the projection of the strand 71 is as shown in Figure 4, which is an enlarged view of Figure 3.
W sb and pitch are W pb . When the incident light is projected from the normal to the mesh surface to the angle θ shown in the figure,
Both w sb and W pb are the projection width W sa and pitch of vertically incident light.
W equals pa . That is, the incident light transmittance does not decrease from the vertical to the angle θ, and the light utilization efficiency does not decrease. On the other hand, microwave leakage is determined by the pitch and maximum width of the mesh strands, so if the pitch and maximum width are the same, there will be no change even if the cross-sectional shape of the strands changes.

第5図はこの発明の他の実施例を示す断面図
で、素線71の断面形状を円弧をあわせたレンズ
状としたもので、この例では入射光の入射角が垂
直からθの角度まで変化しても透過率の変化はな
い。
FIG. 5 is a cross-sectional view showing another embodiment of the present invention, in which the cross-sectional shape of the wire 71 is shaped like a lens with circular arcs, and in this example, the incident angle of the incident light ranges from the vertical to the angle θ. Even if it changes, there is no change in transmittance.

なお以上例示したような素線の断面形状の加工
は、例えば第5図に示したものは、フオトエツチ
ングで断面形状をまず矩形状に成形したものを、
さらに融かし込みを加減して複数個エツチング加
工を施せば成形できる。又、第4図に示した三角
形のものは、まず矩形状に成形したのちプレス加
工により成形する。なおこの成形方法は第5図に
示したレンズ状のものにも適用できる。
The processing of the cross-sectional shape of the wire as exemplified above, for example, shown in FIG. 5, involves first forming the cross-sectional shape into a rectangular shape by photo etching, then
Furthermore, it can be molded by adjusting the melting and etching multiple pieces. Further, the triangular shape shown in FIG. 4 is first formed into a rectangular shape and then formed by press working. Note that this molding method can also be applied to the lens-shaped product shown in FIG.

以上のように、本願発明のマイクロ波放電光源
装置では、マイクロ波漏洩は増加せずに、光の利
用効率を高めることができる。
As described above, in the microwave discharge light source device of the present invention, the light utilization efficiency can be improved without increasing microwave leakage.

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

第1図はマイクロ波放電光源装置の要部断面
図、第2図はメツシユ板の部分拡大平面図、第3
図はこの発明の一実施例の要部であるメツシユ板
の一部拡大断面図、第4図はその光透過率を説明
するための部分拡大図、第5図はこの発明の他の
実施例の拡大断面図である。 図において、4は空胴壁、7は金属メツシユ
板、11はマイクロ波空胴、13は無電極放電
灯、71は金属メツシユ板の素線である。なお、
各図中同一符号はそれぞれ同一、又は相当部分を
示す。
Figure 1 is a sectional view of the main parts of the microwave discharge light source device, Figure 2 is a partially enlarged plan view of the mesh plate, and Figure 3 is a partially enlarged plan view of the mesh plate.
The figure is a partially enlarged cross-sectional view of a mesh plate which is the main part of an embodiment of this invention, FIG. 4 is a partially enlarged view for explaining its light transmittance, and FIG. 5 is another embodiment of this invention. FIG. In the figure, 4 is a cavity wall, 7 is a metal mesh plate, 11 is a microwave cavity, 13 is an electrodeless discharge lamp, and 71 is a wire of the metal mesh plate. In addition,
The same reference numerals in each figure indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 1 マイクロ波が導入される給電口を有し、少な
くとも一面が開口せる空胴壁と、上記開口を塞ぐ
金属メツシユ板とで構成されたマイクロ波空胴
と、このマイクロ波空胴内に配設され、内部に希
ガスと水銀とが封入されている無電極放電灯とを
備えたものにおいて、上記金属メツシユ板は電気
的に連続した金属板より形成され、かつそのメツ
シユ素線の断面形状を、三角形または偏平凸レン
ズ状としたことを特徴とするマイクロ波放電光源
装置。
1. A microwave cavity that has a power supply port into which microwaves are introduced and is composed of a cavity wall that is open on at least one side, and a metal mesh plate that closes the opening, and a microwave cavity that is disposed within the microwave cavity. The metal mesh plate is formed of an electrically continuous metal plate, and the cross-sectional shape of the mesh wire is , a microwave discharge light source device characterized by having a triangular or oblate convex lens shape.
JP153786A 1986-01-08 1986-01-08 Microwave discharge light source device Granted JPS61165950A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP153786A JPS61165950A (en) 1986-01-08 1986-01-08 Microwave discharge light source device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP153786A JPS61165950A (en) 1986-01-08 1986-01-08 Microwave discharge light source device

Publications (2)

Publication Number Publication Date
JPS61165950A JPS61165950A (en) 1986-07-26
JPH0130254B2 true JPH0130254B2 (en) 1989-06-19

Family

ID=11504271

Family Applications (1)

Application Number Title Priority Date Filing Date
JP153786A Granted JPS61165950A (en) 1986-01-08 1986-01-08 Microwave discharge light source device

Country Status (1)

Country Link
JP (1) JPS61165950A (en)

Also Published As

Publication number Publication date
JPS61165950A (en) 1986-07-26

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