JP2003022785A - Microwave electrodeless discharge lamp device - Google Patents
Microwave electrodeless discharge lamp deviceInfo
- Publication number
- JP2003022785A JP2003022785A JP2001208138A JP2001208138A JP2003022785A JP 2003022785 A JP2003022785 A JP 2003022785A JP 2001208138 A JP2001208138 A JP 2001208138A JP 2001208138 A JP2001208138 A JP 2001208138A JP 2003022785 A JP2003022785 A JP 2003022785A
- Authority
- JP
- Japan
- Prior art keywords
- cavity resonator
- dielectric
- microwave
- internal space
- 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.)
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Landscapes
- Discharge Lamps And Accessories Thereof (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、マイクロ波により
放電発光する発光物質が内部に封入されたランプバルブ
を空洞共振器の内部空間に配置したマイクロ波無電極放
電灯装置に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a microwave electrodeless discharge lamp device in which a lamp bulb in which a light-emitting substance which emits light by discharge by microwaves is sealed is arranged in an internal space of a cavity resonator.
【0002】[0002]
【従来の技術】無電極放電灯はランプバルブ内に電極が
存在しないために一般に長寿命化が期待される。このよ
うな無電極放電灯をマイクロ波により点灯させるマイク
ロ波無電極放電灯装置が従来より提供されている(例え
ば、特開昭59−86153号公報、特開平7−451
04号公報等参照)。2. Description of the Related Art An electrodeless discharge lamp is generally expected to have a long life because there are no electrodes inside the lamp bulb. Conventionally, a microwave electrodeless discharge lamp device for lighting such an electrodeless discharge lamp by microwave has been provided (for example, JP-A-59-86153 and JP-A-7-451).
No. 04, etc.).
【0003】従来のマイクロ波無電極放電灯装置では、
適当な開口率を有する金網で形成され、マイクロ波に対
しては不透過で且つ光に対しては実質的に透過性を有す
る空洞共振器の内部空間に、絶縁性部材によって円盤状
に形成されてマイクロ波並びに光に対して不透過である
反射鏡が挿入され、この反射鏡によってランプバルブが
発する光の配光が制御されていた。In the conventional microwave electrodeless discharge lamp device,
It is formed of a wire mesh having an appropriate aperture ratio, is formed into a disc shape by an insulating member in the internal space of the cavity resonator that is opaque to microwaves and substantially transparent to light. As a result, a reflecting mirror that is opaque to microwaves and light is inserted, and this reflecting mirror controls the light distribution of the light emitted by the lamp bulb.
【0004】[0004]
【発明が解決しようとする課題】ところが、上記従来例
のように空洞共振器を金網を用いて形成した場合、ラン
プバルブで発する光を空洞共振器の内部空間から外部に
取り出すために金網の開口率を高くする必要があるため
に空洞共振器の機械的強度が弱くなってしまうという問
題があった。このように空洞共振器の機械的強度が弱い
とランプバルブの発光による熱や外部から加わる振動な
どの衝撃によって空洞共振器が変形し、内部空間の共振
周波数(共振波長)が設計値から変化してランプバルブ
とのエネルギ結合が劣化し、その結果、ランプバルブ内
に供給されるエネルギが減少して発光効率が低下すると
考えられる。However, when the cavity resonator is formed by using the wire mesh as in the above-mentioned conventional example, the opening of the wire mesh is used to extract the light emitted from the lamp bulb from the internal space of the cavity resonator to the outside. There is a problem that the mechanical strength of the cavity resonator is weakened because it is necessary to increase the rate. When the mechanical strength of the cavity resonator is weak in this way, the cavity resonator is deformed by the impact of heat generated by the light emission of the lamp bulb and vibration applied from the outside, and the resonance frequency (resonance wavelength) of the internal space changes from the design value. As a result, the energy coupling with the lamp bulb is deteriorated, and as a result, the energy supplied to the lamp bulb is reduced and the luminous efficiency is reduced.
【0005】本発明は上記事情に鑑みて為されたもので
あり、その目的とするところは、空洞共振器の機械的強
度を高めて発光効率の向上を図ったマイクロ波無電極放
電灯装置を提供することにある。The present invention has been made in view of the above circumstances, and an object of the present invention is to provide a microwave electrodeless discharge lamp device in which the mechanical strength of the cavity resonator is increased to improve the luminous efficiency. To provide.
【0006】[0006]
【課題を解決するための手段】請求項1の発明は、上記
目的を達成するために、マイクロ波を発生するマイクロ
波発生手段と、少なくとも一部に透光可能な部位を有し
マイクロ波発生手段で発生したマイクロ波が内部空間に
供給される空洞共振器と、マイクロ波により放電発光す
る発光物質が内部に封入され、空洞共振器の内部空間に
配置されるランプバルブとを備え、空洞共振器の内部空
間における強電界部位に誘電体が配設されたことを特徴
とする。一般に真空中での波長がλ0の電磁波が比誘電
率εの誘電体内を伝搬する場合、誘電体内での波長λは
λ=λ0/√εとなる。従って、空洞共振器の内部空間
における強電界部位に誘電体を配設すれば、誘電体内を
伝搬する際にマイクロ波の波長が短縮されることで空洞
共振器の寸法を小さくすることができる。その結果、小
型化により空洞共振器の機械的強度を高め、空洞共振器
の変形を防止して発光効率の向上が図れる。In order to achieve the above object, the invention of claim 1 is a microwave generating means for generating a microwave and a microwave generating means having at least a part capable of transmitting light. The cavity resonance is provided with a cavity resonator in which the microwave generated by the means is supplied to the internal space, and a lamp bulb in which a luminescent substance that discharges and emits light by the microwave is enclosed inside and is arranged in the interior space of the cavity resonator. It is characterized in that a dielectric is arranged at a strong electric field portion in the inner space of the container. Generally, when an electromagnetic wave having a wavelength λ0 in a vacuum propagates in a dielectric having a relative permittivity ε, the wavelength λ in the dielectric is λ = λ0 / √ε. Therefore, by disposing the dielectric in the strong electric field portion in the internal space of the cavity resonator, the size of the cavity resonator can be reduced by shortening the wavelength of the microwave when propagating in the dielectric. As a result, the mechanical strength of the cavity resonator can be increased by miniaturization, deformation of the cavity resonator can be prevented, and light emission efficiency can be improved.
【0007】請求項2の発明は、請求項1の発明におい
て、空洞共振器の内部空間で誘電体の少なくとも一部に
より誘電体自体を保持してなることを特徴とし、誘電体
を保持するための部材を別に用意する必要がなく、構造
の簡略化とコストダウンが図れる。The invention of claim 2 is characterized in that, in the invention of claim 1, the dielectric itself is held by at least a part of the dielectric in the internal space of the cavity resonator. Since it is not necessary to separately prepare the member, the structure can be simplified and the cost can be reduced.
【0008】請求項3の発明は、請求項1又は2の発明
において、誘電体の厚みを不均一としたことを特徴と
し、誘電体の厚みに応じて空洞共振器の内部空間におけ
る電界分布を制御することができ、ガラスバルブ内に高
効率でプラズマを生成することができる。The invention of claim 3 is characterized in that, in the invention of claim 1 or 2, the thickness of the dielectric is made non-uniform, and the electric field distribution in the internal space of the cavity resonator is varied according to the thickness of the dielectric. It can be controlled and plasma can be generated in the glass bulb with high efficiency.
【0009】請求項4の発明は、請求項1又は2又は3
の発明において、誘電体は多角形筒状体の集合体からな
ることを特徴とし、ガラスバルブから放射される光が誘
電体を通過して外部に放出されるため、発光効率を高め
ることができる。The invention of claim 4 is the invention of claim 1 or 2 or 3.
In the invention, the dielectric is composed of an assembly of polygonal cylindrical bodies, and the light emitted from the glass bulb passes through the dielectric and is emitted to the outside, so that the luminous efficiency can be improved. .
【0010】請求項5の発明は、請求項4の発明におい
て、多角形筒状体を六角形の筒状体としたことを特徴と
し、誘電体を軽量としながらも機械的強度を向上するこ
とができる。The invention of claim 5 is characterized in that, in the invention of claim 4, the polygonal cylindrical body is a hexagonal cylindrical body, and the mechanical strength is improved while making the dielectric material lightweight. You can
【0011】請求項6の発明は、請求項1〜5の何れか
の発明において、誘電体表面の少なくとも一部を白色と
したことを特徴とし、誘電体表面における光の反射率を
高めて発光効率を更に向上することができる。According to a sixth aspect of the present invention, in any one of the first to fifth aspects, at least a part of the surface of the dielectric is white, and the reflectance of light on the surface of the dielectric is increased to emit light. The efficiency can be further improved.
【0012】[0012]
【発明の実施の形態】(実施形態1)図2に本実施形態
のマイクロ波無電極放電灯装置の全体構成を示す。但
し、図2においては本発明の要旨である空洞共振器4の
構造については簡略して示している。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS (Embodiment 1) FIG. 2 shows the overall structure of a microwave electrodeless discharge lamp device of this embodiment. However, in FIG. 2, the structure of the cavity resonator 4, which is the gist of the present invention, is shown in a simplified manner.
【0013】図2に示すように、電源1から供給される
電気エネルギがマグネトロン2によってマイクロ波エネ
ルギに変換され、導波管3を通して空洞共振器4に伝搬
される。空洞共振器4は金網によって円筒形に形成され
ており、底面における導波管3との結合部位には矩形の
結合窓4aが開口している。また、棒状の支持体5aで
支持されたランプバルブ5が空洞共振器4の内部空間に
おける中心付近に配設されている。ランプバルブ5はガ
ラスのような透光性部材によって球形に形成され、その
内部に希ガスと発光物質が封入されている。而して、従
来技術でも説明したように、空洞共振器4の外形寸法並
びに結合窓4aの寸法をマグネトロン2で変換されたマ
イクロ波の周波数に応じた適当な値に設定することによ
り、空洞共振器4の内部空間でマイクロ波が共振し、共
振によって増大されたマイクロ波エネルギがランプバル
ブ5に供給され、ランプバルブ5内にプラズマが発生し
そのプラズマによって発光物質が発光する。As shown in FIG. 2, electric energy supplied from the power source 1 is converted into microwave energy by the magnetron 2 and propagated through the waveguide 3 to the cavity resonator 4. The cavity resonator 4 is formed in a cylindrical shape by a wire mesh, and a rectangular coupling window 4a is opened at the coupling portion with the waveguide 3 on the bottom surface. A lamp bulb 5 supported by a rod-shaped support 5 a is arranged near the center of the internal space of the cavity resonator 4. The lamp bulb 5 is formed in a spherical shape by a translucent member such as glass, and a rare gas and a luminescent substance are enclosed in the inside thereof. Thus, as described in the prior art, by setting the outer dimensions of the cavity resonator 4 and the dimensions of the coupling window 4a to appropriate values according to the frequency of the microwave converted by the magnetron 2, The microwave resonates in the internal space of the container 4, the microwave energy increased by the resonance is supplied to the lamp bulb 5, plasma is generated in the lamp bulb 5, and the plasma emits the luminescent material.
【0014】例えば、マグネトロン2から出力される周
波数2.45[GHz]のマイクロ波をTE111モード
で共振させる空洞共振器4の外形寸法は、計算上で直径
76[mm]、高さ184[mm]となり、直径に対し
て高さ寸法が比較的大きく、また金網の線径が通常0.
2[mm]程度で開口部の寸法が1.6[mm]×1.
6[mm]で開口率が約80%であることから、機械的
強度が充分に得られず、輸送途中などの振動で変形して
しまう虞がある。For example, the external dimensions of the cavity resonator 4 that resonates the microwave of frequency 2.45 [GHz] output from the magnetron 2 in the TE 111 mode are calculated to have a diameter of 76 [mm] and a height of 184 []. mm], the height dimension is relatively large with respect to the diameter, and the wire diameter of the wire mesh is usually 0.
The dimension of the opening is 1.6 [mm] × 1.
Since the aperture ratio is about 80% at 6 [mm], sufficient mechanical strength cannot be obtained, and there is a risk of deformation due to vibration during transportation.
【0015】そこで本実施形態では、図1に示すように
空洞共振器4の直径に略等しい直径を有する円盤状の誘
電体6を空洞共振器4の内部空間に配設している。この
誘電体6は、円盤状の主部6aと、主部6の底面におけ
る周縁近傍に略等間隔で突設された複数本(本実施形態
では3本)の棒状支持部6bとが例えば多結晶アルミナ
によって一体に形成されている。そして、各棒状支持部
6bの先端を空洞共振器4の内底面に当接させることで
主部6aが空洞共振器4の内部空間における強電界部位
(ランプバルブ5が配設された中心近傍)に配置され
る。Therefore, in the present embodiment, as shown in FIG. 1, a disk-shaped dielectric 6 having a diameter substantially equal to the diameter of the cavity resonator 4 is arranged in the internal space of the cavity resonator 4. The dielectric 6 includes, for example, a large number of disk-shaped main portions 6a and a plurality of (three in the present embodiment) rod-shaped support portions 6b that are provided near the periphery of the bottom surface of the main portion 6 at substantially equal intervals. It is integrally formed of crystalline alumina. The tip of each rod-shaped support portion 6b is brought into contact with the inner bottom surface of the cavity resonator 4 so that the main portion 6a has a strong electric field in the internal space of the cavity resonator 4 (near the center where the lamp bulb 5 is disposed). Is located in.
【0016】一般に真空中での波長がλ0の電磁波が比
誘電率εの誘電体内を伝搬する場合、誘電体内での波長
λはλ=λ0/√εとなる。例えば周波数2.45[G
Hz]のマイクロ波では真空中の波長λ0が約122
[mm]であるのに対し、誘電体内を伝搬する際の波長
λは、多結晶アルミナの比誘電率が約8.5であるから
約42[mm]と計算される。すなわち、単純に考える
と電磁波の伝搬経路を真空から誘電体に置き換えること
でその距離を約3分の1に縮めることができる。Generally, when an electromagnetic wave having a wavelength λ0 in a vacuum propagates in a dielectric having a relative permittivity ε, the wavelength λ in the dielectric is λ = λ0 / √ε. For example, frequency 2.45 [G
[Hz], the wavelength λ0 in vacuum is about 122
In contrast to [mm], the wavelength λ when propagating in the dielectric is calculated to be about 42 [mm] because the relative permittivity of polycrystalline alumina is about 8.5. That is, if simply considered, the distance can be shortened to about one third by replacing the propagation path of the electromagnetic wave from a vacuum with a dielectric.
【0017】従って、誘電体6の主部6aの厚み寸法を
約20[mm]、ランプバルブ5の直径を20[m
m]、結合窓4aの寸法を60[mm]×12[mm]
とした場合、誘電体6内を伝搬する際の波長短縮作用に
より、空洞共振器4の高さ寸法を184[mm]から1
40[mm]へと約40[mm]程度短縮することがで
きる。その結果、小型化によって空洞共振器4の機械的
強度を高めることができ、空洞共振器4の変形を防止し
て発光効率の向上が図れる。また、誘電体6を白色とす
ることで反射率を高くすれば、ランプバルブ5から放射
される光を誘電体6表面で効率よく反射させて発光効率
を更に向上させることができる。さらに、空洞共振器4
の内部空間で誘電体6の少なくとも一部である棒状支持
部6bにより誘電体6自体(主部6a)を保持している
ので、誘電体6を保持するための部材を別に用意する必
要がなく、構造の簡略化とコストダウンが図れるという
利点がある。但し、複数本の棒状支持部6bで主部6a
を支える構造とする代わりに、主部6aの厚み寸法を大
きくして主部6a自体を空洞共振器4の底面に載置する
構造としてもよく、このような構造であれば、波長を更
に短縮させることで空洞共振器4をより一層小型化し、
機械的強度をさらに向上させることができる。Therefore, the thickness of the main portion 6a of the dielectric 6 is about 20 [mm], and the diameter of the lamp bulb 5 is 20 [m].
m] and the size of the coupling window 4a is 60 [mm] × 12 [mm]
In such a case, the height dimension of the cavity resonator 4 is changed from 184 [mm] to 1 due to the wavelength shortening effect when propagating in the dielectric 6.
It can be reduced to about 40 [mm] by about 40 [mm]. As a result, the mechanical strength of the cavity resonator 4 can be increased by downsizing, the deformation of the cavity resonator 4 can be prevented, and the luminous efficiency can be improved. If the reflectance is increased by making the dielectric 6 white, the light emitted from the lamp bulb 5 can be efficiently reflected on the surface of the dielectric 6 to further improve the light emission efficiency. Furthermore, the cavity resonator 4
Since the dielectric 6 itself (main part 6a) is held by the rod-shaped support portion 6b which is at least a part of the dielectric 6 in the internal space of the above, it is not necessary to separately prepare a member for holding the dielectric 6. The advantages are that the structure can be simplified and the cost can be reduced. However, the main portion 6a is composed of a plurality of rod-shaped support portions 6b.
In place of the structure for supporting the main part 6a, the thickness of the main part 6a may be increased and the main part 6a itself may be placed on the bottom surface of the cavity resonator 4. With such a structure, the wavelength is further shortened. By making the cavity resonator 4 smaller,
The mechanical strength can be further improved.
【0018】なお、誘電体6は多結晶アルミナ以外にも
例えば石英ガラスでもよいが、石英ガラスの比誘電率が
3.8と多結晶アルミナよりも低いので波長の短縮作用
が小さくなる。よって、多結晶アルミナと同程度の効果
を得るためには誘電体の厚み寸法を大きくする必要があ
る。The dielectric 6 may be, for example, quartz glass in addition to polycrystalline alumina, but since the relative permittivity of quartz glass is 3.8, which is lower than that of polycrystalline alumina, the wavelength shortening action is reduced. Therefore, in order to obtain the same effect as polycrystalline alumina, it is necessary to increase the thickness dimension of the dielectric.
【0019】(実施形態2)本実施形態は、図3に示す
ように円筒形の空洞共振器4の内周面に沿って配設され
る円筒部6cを誘電体6に追加した点に特徴がある。(Embodiment 2) This embodiment is characterized in that a cylindrical portion 6c arranged along the inner peripheral surface of a cylindrical cavity resonator 4 is added to a dielectric 6 as shown in FIG. There is.
【0020】すなわち、誘電体6を形成する多結晶アル
ミナは断熱性の高い材料であるから、ランプバルブ5の
発する熱から空洞共振器4を保護し、金網の酸化を防止
することができる。また、このように円筒部6cを空洞
共振器4内に配設する構造とすれば、空洞共振器4の周
面を金網とする必要がなくなるから、上下底面を除く周
面を金属板で形成することによって空洞共振器4の機械
的強度が更に向上できる。なお、本実施形態では誘電体
6の主部6aを円筒部6cで保持しているために棒状保
持部6bは不要となる。That is, since the polycrystalline alumina forming the dielectric 6 is a material having a high heat insulating property, it is possible to protect the cavity resonator 4 from the heat generated by the lamp bulb 5 and prevent oxidation of the wire mesh. Further, with the structure in which the cylindrical portion 6c is arranged in the cavity resonator 4 as described above, the peripheral surface of the cavity resonator 4 does not need to be a wire mesh, and therefore the peripheral surface excluding the upper and lower bottom surfaces is formed of a metal plate. By doing so, the mechanical strength of the cavity resonator 4 can be further improved. In this embodiment, since the main portion 6a of the dielectric 6 is held by the cylindrical portion 6c, the rod-shaped holding portion 6b is unnecessary.
【0021】(実施形態3)本実施形態は、図4に示す
ように円筒部6cと、ランプバルブ5の下方における空
洞共振器4の内部空間に多結晶アルミナ等のセラミック
ス材料を充填してなる充填部6dとを誘電体6として設
けた点に特徴がある。(Embodiment 3) In this embodiment, as shown in FIG. 4, a cylindrical portion 6c and the internal space of the cavity resonator 4 below the lamp bulb 5 are filled with a ceramic material such as polycrystalline alumina. The feature is that the filling portion 6d is provided as the dielectric 6.
【0022】本実施形態によれば、実施形態2に比較し
てさらに波長を短縮することができるから、空洞共振器
4の高さ寸法を一層小型化して機械的強度の向上が図れ
る。なお、図5に示すように充填部6dでランプバルブ
5を支持する構造とすれば、支持体5aが不要となって
コストダウンが図れる。According to this embodiment, the wavelength can be further shortened as compared with the second embodiment, so that the height dimension of the cavity resonator 4 can be further reduced and the mechanical strength can be improved. If the filling portion 6d is used to support the lamp bulb 5 as shown in FIG. 5, the support 5a is not required and the cost can be reduced.
【0023】(実施形態4)本実施形態は、図6に示す
ように主部6aの略中央に貫通孔6eを形成し、この貫
通孔6eの内部にランプバルブ5を配置した点に特徴が
ある。(Embodiment 4) This embodiment is characterized in that a through hole 6e is formed substantially in the center of the main portion 6a as shown in FIG. 6, and the lamp bulb 5 is arranged inside this through hole 6e. is there.
【0024】而して、誘電体6の主部6aの略中央に貫
通孔6eを設けることで厚みが不均一となり、さらに、
この貫通孔6eの内部にランプバルブ5を配置すること
によってランプバルブ5の周囲の電界を制御することが
可能となる。そのため、ランプバルブ5に効率よくマイ
クロ波エネルギを供給して発光効率を更に高めることが
できる。By providing the through hole 6e at the substantially center of the main portion 6a of the dielectric 6, the thickness becomes non-uniform, and further,
The electric field around the lamp bulb 5 can be controlled by disposing the lamp bulb 5 inside the through hole 6e. Therefore, the microwave energy can be efficiently supplied to the lamp bulb 5 to further improve the light emission efficiency.
【0025】(実施形態5)ところで、空洞共振器4の
内部空間におけるマイクロ波がTM010モードである
場合、空洞共振器4の軸方向(高さ方向)に電界が発生
するために空洞共振器4の上底面に比較的大きな電流が
流れて熱による劣化が促進されてしまう。(Embodiment 5) When the microwave in the internal space of the cavity resonator 4 is in the TM010 mode, an electric field is generated in the axial direction (height direction) of the cavity resonator 4 so that the cavity resonator 4 is generated. A relatively large electric current flows on the upper and lower surfaces of the upper bottom surface to accelerate the deterioration due to heat.
【0026】そこで、本実施形態では、図7及び図8に
示すように空洞共振器4の上底面の金網4bを多数の六
角形からなる、いわゆるハニカム構造とし、さらに、六
角形の筒状体の集合体からなるハニカム構造の支持部6
fを円筒部6cの一端側(図7における上側端)に設け
て空洞共振器4の金網4bを下方から支持する構造とし
ている。ここで、誘電体6の支持部6fは空洞共振器4
の上底面に形成されるハニカム構造と同形状並びに同寸
法で形成されている。Therefore, in this embodiment, as shown in FIGS. 7 and 8, the wire netting 4b on the upper and bottom surfaces of the cavity resonator 4 has a so-called honeycomb structure composed of a large number of hexagons, and further, a hexagonal tubular body. Support part 6 having a honeycomb structure composed of an aggregate of
f is provided on one end side (upper end in FIG. 7) of the cylindrical portion 6c to support the wire netting 4b of the cavity resonator 4 from below. Here, the supporting portion 6f of the dielectric 6 is the cavity resonator 4
The honeycomb structure is formed in the same shape and the same size as the honeycomb structure formed on the upper bottom surface.
【0027】本実施形態はこのような構造を採用したこ
とにより、ランプバルブ5から放射された光が保持部6
fによって遮られて空洞共振器4の上底部に直接照射さ
れる光の量が減少するから、空洞共振器4の機械的強度
を向上させることができる。なお、誘電体6の支持部6
fは空洞共振器4の金網4b全体を支持する必要はな
く、部分的に支持する構造であっても良い。By adopting such a structure in this embodiment, the light emitted from the lamp bulb 5 is held by the holding portion 6.
Since the amount of light that is blocked by f and directly irradiates the upper bottom of the cavity resonator 4 is reduced, the mechanical strength of the cavity resonator 4 can be improved. The supporting portion 6 of the dielectric 6
It is not necessary for f to support the entire wire mesh 4b of the cavity resonator 4, and a structure for partially supporting it may be used.
【0028】(実施形態6)本実施形態は、図9に示す
ように誘電体6を多数の六角形筒状体の集合物で構成し
たハニカム構造とした点に特徴がある。(Embodiment 6) This embodiment is characterized in that the dielectric body 6 has a honeycomb structure composed of an assembly of a large number of hexagonal cylindrical bodies as shown in FIG.
【0029】而して本実施形態によれば、誘電体6をハ
ニカム構造とすることで共振周波数を調整し空洞共振器
4の小型化が図れると同時に、空洞共振器4の内部空間
における気流の整流作用によって所望の対流を生じさせ
ることにより、空洞共振器4の内部空間の温度分布を制
御することができる。Thus, according to the present embodiment, by making the dielectric 6 a honeycomb structure, the resonance frequency can be adjusted and the size of the cavity resonator 4 can be reduced, and at the same time, the air flow in the internal space of the cavity resonator 4 can be reduced. The temperature distribution in the internal space of the cavity resonator 4 can be controlled by generating a desired convection by the rectifying action.
【0030】[0030]
【発明の効果】請求項1の発明は、マイクロ波を発生す
るマイクロ波発生手段と、少なくとも一部に透光可能な
部位を有しマイクロ波発生手段で発生したマイクロ波が
内部空間に供給される空洞共振器と、マイクロ波により
放電発光する発光物質が内部に封入され、空洞共振器の
内部空間に配置されるランプバルブとを備え、空洞共振
器の内部空間における強電界部位に誘電体が配設された
ので、誘電体内を伝搬する際にマイクロ波の波長が短縮
されることで空洞共振器の寸法を小さくすることがで
き、その結果、小型化により空洞共振器の機械的強度を
高め、空洞共振器の変形を防止して発光効率の向上が図
れるという効果がある。According to the first aspect of the present invention, the microwave generating means for generating a microwave and the microwave generated by the microwave generating means having at least a part capable of transmitting light are supplied to the internal space. A cavity resonator and a lamp bulb in which a light-emitting substance that discharges and emits light by microwaves is sealed inside, and a lamp bulb disposed in the interior space of the cavity resonator. Since it is arranged, the size of the cavity resonator can be reduced by shortening the wavelength of the microwave when propagating in the dielectric, and as a result, the mechanical strength of the cavity resonator can be increased by miniaturization. Further, there is an effect that the deformation of the cavity resonator can be prevented and the luminous efficiency can be improved.
【0031】請求項2の発明は、請求項1の発明におい
て、空洞共振器の内部空間で誘電体の少なくとも一部に
より誘電体自体を保持してなるので、誘電体を保持する
ための部材を別に用意する必要がなく、構造の簡略化と
コストダウンが図れるという効果がある。According to a second aspect of the invention, in the first aspect of the invention, since the dielectric itself is held by at least a part of the dielectric in the internal space of the cavity resonator, a member for holding the dielectric is provided. It is not necessary to prepare separately, and there is an effect that the structure can be simplified and the cost can be reduced.
【0032】請求項3の発明は、請求項1又は2の発明
において、誘電体の厚みを不均一としたので、誘電体の
厚みに応じて空洞共振器の内部空間における電界分布を
制御することができ、ガラスバルブ内に高効率でプラズ
マを生成することができるという効果がある。According to the invention of claim 3, in the invention of claim 1 or 2, since the thickness of the dielectric is made nonuniform, the electric field distribution in the internal space of the cavity resonator is controlled according to the thickness of the dielectric. Therefore, there is an effect that plasma can be generated in the glass bulb with high efficiency.
【0033】請求項4の発明は、請求項1又は2又は3
の発明において、誘電体は多角形筒状体の集合体からな
るので、ガラスバルブから放射される光が誘電体を通過
して外部に放出されるために発光効率を高めることがで
きるという効果がある。The invention of claim 4 is the invention of claim 1 or 2 or 3.
In the invention, since the dielectric body is composed of an assembly of polygonal cylindrical bodies, the light emitted from the glass bulb passes through the dielectric body and is emitted to the outside, so that the luminous efficiency can be improved. is there.
【0034】請求項5の発明は、請求項4の発明におい
て、多角形筒状体を六角形の筒状体としたので、誘電体
を軽量としながらも機械的強度を向上することができる
という効果がある。According to the invention of claim 5, in the invention of claim 4, since the polygonal cylindrical body is a hexagonal cylindrical body, it is possible to improve the mechanical strength while making the dielectric material lightweight. effective.
【0035】請求項6の発明は、請求項1〜5の何れか
の発明において、誘電体表面の少なくとも一部を白色と
したので、誘電体表面における光の反射率を高めて発光
効率を更に向上することができるという効果がある。According to a sixth aspect of the present invention, in any one of the first to fifth aspects, at least part of the surface of the dielectric is white, so that the reflectance of light on the surface of the dielectric is increased to further improve the luminous efficiency. There is an effect that it can be improved.
【図1】実施形態1の要部を示す斜視図である。FIG. 1 is a perspective view showing a main part of a first embodiment.
【図2】同上のブロック図である。FIG. 2 is a block diagram of the above.
【図3】実施形態2の要部を示す断面図である。FIG. 3 is a cross-sectional view showing the main parts of the second embodiment.
【図4】実施形態3の要部を示す断面図である。FIG. 4 is a cross-sectional view showing the main parts of the third embodiment.
【図5】同上の他の構成を示す断面図である。FIG. 5 is a cross-sectional view showing another configuration of the above.
【図6】実施形態4の要部を示す断面図である。FIG. 6 is a sectional view showing a main part of a fourth embodiment.
【図7】実施形態5の要部を示す断面図である。FIG. 7 is a cross-sectional view showing the main parts of the fifth embodiment.
【図8】同上における空洞共振器の要部平面図である。FIG. 8 is a plan view of an essential part of the cavity resonator of the above.
【図9】実施形態6の要部を示す断面図である。FIG. 9 is a cross-sectional view showing the main parts of the sixth embodiment.
4 空洞共振器 4a 結合窓 5 ランプバルブ 6 誘電体 4 cavity 4a Combined window 5 lamp bulbs 6 Dielectric
フロントページの続き (72)発明者 請川 信 大阪府門真市大字門真1048番地松下電工株 式会社内 Fターム(参考) 5C039 PP02 PP04 PP08 PP09 PP16Continued front page (72) Inventor Shin Ogawa 1048, Kadoma, Kadoma-shi, Osaka Matsushita Electric Works Co., Ltd. Inside the company F term (reference) 5C039 PP02 PP04 PP08 PP09 PP16
Claims (6)
段と、少なくとも一部に透光可能な部位を有しマイクロ
波発生手段で発生したマイクロ波が内部空間に供給され
る空洞共振器と、マイクロ波により放電発光する発光物
質が内部に封入され、空洞共振器の内部空間に配置され
るランプバルブとを備え、空洞共振器の内部空間におけ
る強電界部位に誘電体が配設されたことを特徴とするマ
イクロ波無電極放電灯装置。1. A microwave generating means for generating a microwave, a cavity resonator having at least a part capable of transmitting light and having a microwave generated by the microwave generating means supplied to an internal space, and a microwave. And a lamp bulb which is disposed in an internal space of the cavity resonator, in which a luminescent material which discharges and emits light by waves is enclosed, and a dielectric is disposed in a strong electric field portion in the internal space of the cavity resonator. Microwave electrodeless discharge lamp device.
とも一部により誘電体自体を保持してなることを特徴と
する請求項1記載のマイクロ波無電極放電灯装置。2. The microwave electrodeless discharge lamp device according to claim 1, wherein the dielectric itself is held by at least a part of the dielectric in the internal space of the cavity resonator.
とする請求項1又は2記載のマイクロ波無電極放電灯装
置。3. The microwave electrodeless discharge lamp device according to claim 1, wherein the dielectric has a nonuniform thickness.
ことを特徴とする請求項1又は2又は3記載のマイクロ
波無電極放電灯装置。4. The microwave electrodeless discharge lamp device according to claim 1, wherein the dielectric body is an assembly of polygonal cylindrical bodies.
とを特徴とする請求項4記載のマイクロ波無電極放電灯
装置。5. The microwave electrodeless discharge lamp device according to claim 4, wherein the polygonal tubular body is a hexagonal tubular body.
たことを特徴とする請求項1〜5の何れかに記載のマイ
クロ波無電極放電灯装置。6. The microwave electrodeless discharge lamp device according to claim 1, wherein at least a part of the surface of the dielectric is white.
Priority Applications (1)
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JP2001208138A JP2003022785A (en) | 2001-07-09 | 2001-07-09 | Microwave electrodeless discharge lamp device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2001208138A JP2003022785A (en) | 2001-07-09 | 2001-07-09 | Microwave electrodeless discharge lamp device |
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JP2003022785A true JP2003022785A (en) | 2003-01-24 |
Family
ID=19044015
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Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100548277B1 (en) * | 2003-09-08 | 2006-02-02 | 엘지전자 주식회사 | Lamp cover structure of electrodeless lighting system |
EP1703543A2 (en) * | 2005-03-14 | 2006-09-20 | LG Electronics Inc. | Electrodeless lighting apparatus |
US7276860B2 (en) | 2003-12-13 | 2007-10-02 | Lg Electronics Inc. | Electrodeless lighting system |
JP2012527720A (en) * | 2009-05-20 | 2012-11-08 | セラビジョン・リミテッド | Translucent plasma crucible |
JP2014506379A (en) * | 2010-12-21 | 2014-03-13 | セラビジョン・リミテッド | Translucent wave guide electromagnetic wave plasma light source |
JP2015528977A (en) * | 2012-05-10 | 2015-10-01 | セラビジョン リミテッド | Translucent waveguide electromagnetic wave plasma light source |
EP2962529A4 (en) * | 2013-03-01 | 2016-09-14 | Soo Yong Park | Sulfur lamp |
-
2001
- 2001-07-09 JP JP2001208138A patent/JP2003022785A/en not_active Withdrawn
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100548277B1 (en) * | 2003-09-08 | 2006-02-02 | 엘지전자 주식회사 | Lamp cover structure of electrodeless lighting system |
US7276860B2 (en) | 2003-12-13 | 2007-10-02 | Lg Electronics Inc. | Electrodeless lighting system |
EP1703543A2 (en) * | 2005-03-14 | 2006-09-20 | LG Electronics Inc. | Electrodeless lighting apparatus |
JP2006261098A (en) * | 2005-03-14 | 2006-09-28 | Lg Electronics Inc | Electrodeless lighting apparatus |
EP1703543A3 (en) * | 2005-03-14 | 2007-12-26 | LG Electronics Inc. | Electrodeless lighting apparatus |
JP2012527720A (en) * | 2009-05-20 | 2012-11-08 | セラビジョン・リミテッド | Translucent plasma crucible |
JP2014506379A (en) * | 2010-12-21 | 2014-03-13 | セラビジョン・リミテッド | Translucent wave guide electromagnetic wave plasma light source |
JP2015528977A (en) * | 2012-05-10 | 2015-10-01 | セラビジョン リミテッド | Translucent waveguide electromagnetic wave plasma light source |
EP2962529A4 (en) * | 2013-03-01 | 2016-09-14 | Soo Yong Park | Sulfur lamp |
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