JPS5923613B2 - High frequency discharge light source device - Google Patents

High frequency discharge light source device

Info

Publication number
JPS5923613B2
JPS5923613B2 JP7859182A JP7859182A JPS5923613B2 JP S5923613 B2 JPS5923613 B2 JP S5923613B2 JP 7859182 A JP7859182 A JP 7859182A JP 7859182 A JP7859182 A JP 7859182A JP S5923613 B2 JPS5923613 B2 JP S5923613B2
Authority
JP
Japan
Prior art keywords
light
frequency
source device
light source
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
JP7859182A
Other languages
Japanese (ja)
Other versions
JPS5816458A (en
Inventor
隆 喜連川
文雄 武田
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 JP7859182A priority Critical patent/JPS5923613B2/en
Publication of JPS5816458A publication Critical patent/JPS5816458A/en
Publication of JPS5923613B2 publication Critical patent/JPS5923613B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J65/00Lamps without any electrode inside the vessel; Lamps with at least one main electrode outside the vessel
    • H01J65/04Lamps 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
    • H01J65/042Lamps 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
    • H01J65/044Lamps 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

Description

【発明の詳細な説明】 この発明は無電極放電灯を高周波エネルギーで励起し、
照明光を得る高周波放電光源装置に関する。
[Detailed description of the invention] This invention excites an electrodeless discharge lamp with high frequency energy,
The present invention relates to a high-frequency discharge light source device that obtains illumination light.

従来高周波、特にマイクロ波を利用して無電極放電灯を
点灯させる装置の一つとして、特開昭50−54172
号公報に示されているものがある。
Conventionally, as one of the devices for lighting an electrodeless discharge lamp using high frequency waves, especially microwaves, Japanese Patent Application Laid-Open No. 50-54172
There are some that are shown in the publication.

第1図はその光源装置を示すものである。第1図に於い
て、1は細長い形状した無電極の高圧蒸気放電灯、2は
この放電灯1の後方の長手方向に亘って設けられた略半
円筒形状の反射板で、マイクロ波及び放電灯1からの光
に対して不透明な部材で形成されている。
FIG. 1 shows the light source device. In Fig. 1, numeral 1 denotes an elongated electrodeless high-pressure vapor discharge lamp, and numeral 2 denotes a semi-cylindrical reflector plate installed in the longitudinal direction at the rear of the discharge lamp 1, which is used for microwave and radiation. It is made of a material that is opaque to light from the electric lamp 1.

3はこの反射板2のfitl方開口を覆い金属網等のマ
イクロ波に対して不透明でかつ放電灯1からの発光波に
対して透明な部材で形成された光透過体であり、この光
透過体3と前記反射板2によりマイクロ波空胴4を形成
している。
Reference numeral 3 denotes a light transmitting member that covers the fitl opening of the reflector plate 2 and is made of a material such as a metal net that is opaque to microwaves and transparent to the emitted waves from the discharge lamp 1. The body 3 and the reflecting plate 2 form a microwave cavity 4.

尚、5はマイクロ波発振器、6は導波管、7はマイクロ
波の結合孔である。
Note that 5 is a microwave oscillator, 6 is a waveguide, and 7 is a microwave coupling hole.

然るに以上の構成の光源装置に於ては、マイクロ波空胴
4が非共振空胴となっているため、結合孔7より空胴4
内を伝搬し、空胴4の反対端に達した時は、そのエネル
ギーはほぼ零になり、放電灯1はこの際吸収したマイク
ロ波エネルギーにより放電を持続し発光し、この放電灯
1より発した発光波は直接又は反射板2によって反射さ
れ、光透過体3を通過して空胴4外へ放射される。
However, in the light source device with the above configuration, since the microwave cavity 4 is a non-resonant cavity, the coupling hole 7 is connected to the cavity 4.
When the energy propagates inside the cavity 4 and reaches the opposite end of the cavity 4, the energy becomes almost zero, and the discharge lamp 1 continues to discharge and emit light due to the microwave energy absorbed at this time. The emitted light wave is reflected directly or by the reflection plate 2, passes through the light transmitting body 3, and is emitted to the outside of the cavity 4.

従って上記装置に於ては放電灯1及び空胴4の形状は必
然的にマイクロ波の伝搬方向に向って延在する細長い形
状にならざるを得す、そのため照明器具としての形状の
設計におのずと制限が加わり、使用分野も限定され、し
かも充分高いエネルギーを放電灯の全長に亘って均一に
供給することが困難であるという欠点が有った。
Therefore, in the above device, the shapes of the discharge lamp 1 and the cavity 4 must necessarily be elongated shapes extending in the direction of microwave propagation, and therefore, it is natural to design the shape of the lighting equipment. There are additional restrictions, the fields of use are limited, and there are disadvantages in that it is difficult to uniformly supply sufficiently high energy over the entire length of the discharge lamp.

この発明は上記の欠点を除去するためになされたもので
、共振空胴中に球形の無電極放電灯を設けることにより
、空胴の形状を細長くする必要がなく、しかも充分高い
エネルギーを放電灯に均一に供給する高周波放電光源装
置を供給する事な目的としたものである。
This invention was made in order to eliminate the above-mentioned drawbacks. By providing a spherical electrodeless discharge lamp in the resonant cavity, there is no need to make the cavity shape elongated, and moreover, the discharge lamp can generate sufficiently high energy. The purpose of this device is to provide a high-frequency discharge light source device that uniformly supplies light.

以下、実施例に基づいてこの発明を説明する。The present invention will be explained below based on examples.

第2図はこの発明の一実施例を示す破断側面図である。FIG. 2 is a cutaway side view showing one embodiment of the present invention.

図に於て1は内壁面に螢光体膜8を被着し内部にアルゴ
ン及び水銀を封入した球形の無電極値光灯、2はこの無
電極値光灯を囲繞し、マイクロ波及び前記無電極値光灯
1からの発光波に対して不透明で回転放物面形状を有す
る光反射板、3はこの反射板2の開口面を覆いマイクロ
波に対して不透明で、かつ無電極値光灯からの発光波は
実質上通過させる金属網より成る光透過体であり、この
透過体3と前記反射板2によりマイクロ波共振空胴4を
形成している。
In the figure, 1 is a spherical electrodeless light lamp with a phosphor film 8 coated on the inner wall surface and argon and mercury sealed inside, and 2 is a spherical electrodeless light lamp that surrounds this electrodeless light lamp and is used to transmit microwaves and A light reflecting plate 3 is opaque to the light emitted from the electrodeless light lamp 1 and has a paraboloid of revolution shape, and a light reflecting plate 3 covers the aperture surface of the reflecting plate 2 and is opaque to the microwave and reflects the electrodeless light. It is a light transmitting body made of a metal net that substantially allows the emitted waves from the lamp to pass through, and this transmitting body 3 and the reflecting plate 2 form a microwave resonant cavity 4.

尚、7は反射板2に設けられたマイクロ波の結合孔、5
は共振空胴4内に結合孔7を介してマイクロ波を供給す
るマイクロ波発振器、9は発振器内に電力を供給するた
めのケーブルである。
In addition, 7 is a microwave coupling hole provided in the reflection plate 2;
9 is a microwave oscillator that supplies microwaves into the resonant cavity 4 through the coupling hole 7, and 9 is a cable that supplies power into the oscillator.

この様に構成された高周波放電光源装置に於ては、発振
器5によって励振されたマイクロ波エネルギーは結合孔
7を介して共振空胴4内に供給され、共振空胴壁面で反
射をくり返しながら共振空胴4内にマイクロ波電磁界を
形成する。
In the high-frequency discharge light source device configured in this way, the microwave energy excited by the oscillator 5 is supplied into the resonant cavity 4 through the coupling hole 7, and resonates while being repeatedly reflected on the resonant cavity wall surface. A microwave electromagnetic field is created within the cavity 4.

螢光灯1はこのマイクロ波電磁界のエネルギーを吸収す
る事によって放電を持続する。
The fluorescent lamp 1 sustains the discharge by absorbing the energy of this microwave electromagnetic field.

この放電によって発生した紫外線が螢光灯内壁面に被着
した螢光体膜を照射する事により可視光が発生する。
Visible light is generated by irradiating the phosphor film attached to the inner wall of the fluorescent lamp with the ultraviolet rays generated by this discharge.

この可視光は直接あるいは反射板2LK−より反射され
た後、光透過体3を通過して照明光として用いられる。
This visible light passes through the light transmitting body 3 either directly or after being reflected from the reflecting plate 2LK-, and is used as illumination light.

つまり螢光灯1はマイクロ波が反射を繰り返しながら共
振空胴4内に形成したマイクロ波電磁界よりエネルギー
を吸収し放電を持続する。
In other words, the fluorescent lamp 1 absorbs energy from the microwave electromagnetic field formed within the resonant cavity 4 while the microwave is repeatedly reflected, and continues to discharge.

そのため非共振空胴4内で点灯する場合と異り、マイク
ロ波エネルギーの伝搬方向に延在させて細長い螢光灯1
を配設する必要は無い。
Therefore, unlike the case of lighting inside the non-resonant cavity 4, the fluorescent lamp 1 is elongated and extended in the propagation direction of microwave energy.
There is no need to install .

ここで無電極放電灯1の形状を球形にしたことの利点に
ついて述べると、放電灯1からの放射光は全方向に亘っ
て放射状に均一となるため、その放射光を利用するにあ
たり、反射面の設計上の制約が少なく、配光設計が容易
となる。
Here, we will talk about the advantage of making the electrodeless discharge lamp 1 spherical. Since the emitted light from the discharge lamp 1 is radially uniform in all directions, when using the emitted light, it is necessary to There are fewer restrictions on design, making light distribution design easier.

また、放電灯1で放電が発生するとき、放電灯1内のガ
ス圧が著しく上昇するが、放電灯1の壁面でのガス圧が
均一となるため、放電灯1が割れ難い。
Further, when discharge occurs in the discharge lamp 1, the gas pressure within the discharge lamp 1 increases significantly, but the gas pressure on the wall surface of the discharge lamp 1 becomes uniform, so that the discharge lamp 1 is difficult to break.

また、放電灯1の形状が3次元方向に等しくない場合比
はマイクロ波放電により発光ムラが生ずる可能性がある
が、そのような可能性はない。
Furthermore, if the shapes of the discharge lamps 1 are not equal in three dimensions, there is a possibility that uneven light emission will occur due to microwave discharge, but such a possibility does not exist.

さらにマイクロ波空胴を共振空胴とした場合、反射器の
形状を変更と、共振空胴の共振周波数が使用マイクロ波
の周波数からずれるという問題が生ずる。
Furthermore, when the microwave cavity is a resonant cavity, changing the shape of the reflector causes a problem in that the resonant frequency of the resonant cavity deviates from the frequency of the microwave used.

これは共振空胴の形状を相似的に変化させる事によって
その共振周波数を使用マイクロ波の周波数に合致させる
事が容易に出来る。
By changing the shape of the resonant cavity in a similar manner, the resonant frequency can be easily matched to the frequency of the microwave used.

この場合、発光源である無電極放電灯の形状が点光源に
近似しやすい球形状であるので照明器具としての配光分
布を大きく変化させない。
In this case, the shape of the electrodeless discharge lamp serving as the light emitting source is a spherical shape that easily approximates a point light source, so the light distribution as a lighting fixture does not change significantly.

なお、空胴共振器の形状も配光分布を大きく変化させな
いためには回転対称形状である事が望ましく、上記共振
器の内表面形状が焦点を有する場合は、その形状はラン
プ配設位置に焦点を結ぶ事が望ましい。
In addition, it is desirable that the shape of the cavity resonator be rotationally symmetrical in order not to greatly change the light distribution.If the inner surface shape of the resonator has a focal point, the shape should be adjusted to the lamp installation position. It is desirable to focus.

この実施例では空胴共振器4として、光透過体で構成さ
れる部分以外は光反射性を有する部材で構成されている
ものについて述べたが、この部分は特に光反射性を有し
ている必要は無く、要はマイクロ波を反射する部材であ
れば良い。
In this embodiment, the cavity resonator 4 is made of a light-reflecting member except for the part made of a light transmitting material, but this part is particularly light-reflecting. It is not necessary, and any member that reflects microwaves is sufficient.

従って、被照射面に要求される配光分布に従い光反射性
を有する部材の一部又は全部に光吸収性の塗膜を施して
もよい。
Therefore, a light-absorbing coating may be applied to part or all of the light-reflecting member according to the light distribution required for the irradiated surface.

又、前記実施例では無電極放電灯として低圧水銀蒸気放
電によって発生する紫外線によって螢光体を発光させる
螢光灯1の例について述べたが、この発明に於ては、無
電極高圧金属蒸気放電灯を発光させる事も可能である。
Further, in the above embodiment, an example of the fluorescent lamp 1 was described as an electrodeless discharge lamp in which the phosphor emits light using ultraviolet rays generated by low-pressure mercury vapor discharge, but in this invention, an electrodeless high-pressure metal vapor discharge It is also possible to make electric lights emit light.

しかしながら、無電極放電灯に於ては、放電灯はその壁
面よりマイクロ波エネルギーを吸収し放電するため、右
型極放電の場合と異り、放電が壁付近に偏在するという
特徴がある。
However, in an electrodeless discharge lamp, since the discharge lamp absorbs microwave energy from its wall surface and discharges it, unlike the case of a right-hand polar discharge, the discharge lamp is characterized in that the discharge is unevenly distributed near the wall.

このため、無電極低圧水銀蒸気放電灯に於ては、従来の
右型極低圧水銀蒸気放電を利用する螢光灯の発光効率低
下要因の1つであった共鳴線の自己吸収が減少し、高い
発光効率が得られるという特徴を有している。
For this reason, in electrodeless low-pressure mercury vapor discharge lamps, self-absorption of resonance lines, which was one of the factors that reduced the luminous efficiency of conventional right-handed fluorescent lamps that utilize extremely low-pressure mercury vapor discharge, is reduced. It is characterized by high luminous efficiency.

従って無電極放電灯を低圧水銀蒸気放電灯とする事は共
鳴線の自己吸収が発光効率低下の大きな原因とならない
高圧金属蒸気放電灯と比較してより優れた点を有してい
る。
Therefore, using a low-pressure mercury vapor discharge lamp as an electrodeless discharge lamp has an advantage over a high-pressure metal vapor discharge lamp, in which self-absorption of resonance lines does not cause a large decrease in luminous efficiency.

以上説明した様にこの発明によれば、高周波空胴を少な
くとも一面に高周波を遮断し光を通過させる部材を有す
る共振空胴とし、かつこの共振空胴内に球形の無電極放
電灯を配したので、高いエネルギーを放電灯に供給でき
、しかも、配光設計上の制約が少なく、また発光ムラが
少ない上に放電灯が割れ難いという種々の効果を有する
As explained above, according to the present invention, the high-frequency cavity is a resonant cavity having a member on at least one surface that blocks high-frequency waves and allows light to pass through, and a spherical electrodeless discharge lamp is disposed within the resonant cavity. Therefore, high energy can be supplied to the discharge lamp, there are fewer restrictions on light distribution design, there is less uneven light emission, and the discharge lamp is less likely to break.

【図面の簡単な説明】 第1図は従来の無電極放電灯光源装置を示す概略構成図
、第2図はこの発明の一実施例を示す高周波放電光源装
置の破断側面図である。 図中、1は無電極放電灯、2は光反射板、3は光透過体
、4はマイクロ波空胴、5は高周波発振器、8は螢光体
膜。 尚、図中同一符号は同−又は相当部分を示す。
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a schematic configuration diagram showing a conventional electrodeless discharge lamp light source device, and FIG. 2 is a cutaway side view of a high frequency discharge light source device showing an embodiment of the present invention. In the figure, 1 is an electrodeless discharge lamp, 2 is a light reflecting plate, 3 is a light transmitting body, 4 is a microwave cavity, 5 is a high frequency oscillator, and 8 is a fluorescent film. Note that the same reference numerals in the figures indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】 1 高周波発振器、この高周波発振器によって励振され
た高周波によって、共振状態となり、かつ少なくとも一
面に高周波を遮断し光を通過させる部材を有する高周波
空胴共振器、この空胴共振器内に配設され内部に可電離
媒体を封入した球形の無電極放電灯からなる高周波放電
光源装置。 2 空胴共振器の内面形状を回転対称形状とした事を特
徴とする特許請求の範囲第1項記載の高周波放電光源装
置。 3 空胴共振器は内表面形状が放物面状を有している事
を特徴とする特許請求の範囲第2項記載の高周波放電光
源装置。
[Claims] 1. A high-frequency oscillator, a high-frequency cavity resonator that is brought into a resonant state by high-frequency waves excited by the high-frequency oscillator, and has a member on at least one surface that blocks high-frequency waves and allows light to pass through, and this cavity resonator A high-frequency discharge light source device consisting of a spherical electrodeless discharge lamp that is disposed inside and encapsulates an ionizable medium. 2. The high-frequency discharge light source device according to claim 1, wherein the inner surface of the cavity resonator has a rotationally symmetrical shape. 3. The high frequency discharge light source device according to claim 2, wherein the cavity resonator has an inner surface shape of a paraboloid.
JP7859182A 1982-05-11 1982-05-11 High frequency discharge light source device Expired JPS5923613B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7859182A JPS5923613B2 (en) 1982-05-11 1982-05-11 High frequency discharge light source device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7859182A JPS5923613B2 (en) 1982-05-11 1982-05-11 High frequency discharge light source device

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP15087977A Division JPS581511B2 (en) 1977-12-15 1977-12-15 electrodeless fluorescent lamp

Publications (2)

Publication Number Publication Date
JPS5816458A JPS5816458A (en) 1983-01-31
JPS5923613B2 true JPS5923613B2 (en) 1984-06-04

Family

ID=13666148

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7859182A Expired JPS5923613B2 (en) 1982-05-11 1982-05-11 High frequency discharge light source device

Country Status (1)

Country Link
JP (1) JPS5923613B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61231419A (en) * 1985-04-08 1986-10-15 Nok Corp Method for measuring minute amount of organic substance

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20010055802A (en) * 1999-12-13 2001-07-04 구자홍 Combined structure of resonator and reflector in electrodeless lamp
KR101271226B1 (en) * 2006-02-16 2013-06-03 삼성디스플레이 주식회사 Back light unit and liquid crystal display including the same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61231419A (en) * 1985-04-08 1986-10-15 Nok Corp Method for measuring minute amount of organic substance

Also Published As

Publication number Publication date
JPS5816458A (en) 1983-01-31

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