JPH0456059A - Electrodeless discharge lamp device - Google Patents

Electrodeless discharge lamp device

Info

Publication number
JPH0456059A
JPH0456059A JP16339190A JP16339190A JPH0456059A JP H0456059 A JPH0456059 A JP H0456059A JP 16339190 A JP16339190 A JP 16339190A JP 16339190 A JP16339190 A JP 16339190A JP H0456059 A JPH0456059 A JP H0456059A
Authority
JP
Japan
Prior art keywords
high frequency
electrode
tube
electric field
light emission
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
Application number
JP16339190A
Other languages
Japanese (ja)
Inventor
Makoto Ukekawa
信 請川
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.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works Ltd
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 Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP16339190A priority Critical patent/JPH0456059A/en
Publication of JPH0456059A publication Critical patent/JPH0456059A/en
Pending legal-status Critical Current

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  • Discharge Lamps And Accessories Thereof (AREA)

Abstract

PURPOSE:To provide a high output spot-form light source, facilitate manufacture, and prolong the lifetime by furnishing an electrode consisting of foil-form conductor on the wall of a light emission tube, and with this electrode, connecting a high frequency generating circuit for impression of a high frequency voltage only at the time of starting. CONSTITUTION:At the other end of a light emission tube 1, a pair of electrode 4, 4 consisting of foil-form conductor are wrapped in the form in tight contact with the tube wall and connected with a high frequency generating circuit 5 through a matching circuit. When a high frequency voltage is impressed between these two electrodes 4, 4, the intra-tube discharge space is tied with electrode 4 in electrostatic bond, and a high frequency electric field is produced around the electrodes 4, 4 in the intra-tube space. Under this electric field electron collides with Xe atom and causes dissociation of Xe atom. If high frequency current is fed to an induction coil 2 in the condition that electrons are supplied sufficiently in this manner, an alternate magnetic field is generated around the induction coil, particularly inside of the light emission tube 1, and inductive electric field is produced in the form as creeping on the inner wall of the light emission tube 1. Thereby discharge is maintained by this inductive electric field.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、ランプ内部に電極を持たず、外部からの高周
波電磁界によってランプ内部の放電ガスを励起発光させ
る無電極放電灯装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an electrodeless discharge lamp device that does not have electrodes inside the lamp and excites discharge gas inside the lamp to emit light using a high-frequency electromagnetic field from the outside.

[従来の技術] 従来より、無電極放電ランプは小型で高出力、長寿命と
いった特徴を有する為、各所で研究開発されている。そ
の用途は様々であるが、例えば、高出力点光源としての
利用が考えられている。
[Prior Art] Electrodeless discharge lamps have been researched and developed in various places since they have characteristics such as small size, high output, and long life. Although its uses are various, for example, it is being considered to be used as a high-output point light source.

このような無電極放電ランプのうち、例えば、特開昭5
7−78766号公報に開示されたランプでは、第5図
に示すように、空芯コイルlOを被うようなバルブ11
を形成し、この空芯コイルlOに高周波電流を流して発
生する電磁界によってバルブll内の水銀蒸気を放電さ
せるもので、ここで使われる円筒形コイルによる磁界は
、その内部で最も強いものであるが、この例ではその部
分に放電空間は存在せず、専らコイル外部の磁界を利用
する形でバルブ11が形成されている。
Among such electrodeless discharge lamps, for example,
In the lamp disclosed in Japanese Patent No. 7-78766, as shown in FIG.
The mercury vapor inside the bulb 1 is discharged by the electromagnetic field generated by passing a high-frequency current through this air-core coil 1.The magnetic field produced by the cylindrical coil used here is the strongest inside the bulb. However, in this example, there is no discharge space in that part, and the bulb 11 is formed using only the magnetic field outside the coil.

また、最近各所で開発されている電磁波によって発光さ
せる高出力無電極放電ランプの形状は、第6図に示すよ
うに球状であり、透明石英等で形成されたバルブ12内
に希ガスと発光物質が封入され、バルブ12の回りに誘
導コイル13が巻かれている。このような形状で点光源
が必要とされる場合、バルブ12の径を小さくしなけれ
ばならないが、球状で、例えば径が10Il111のバ
ルブ12で、かつ内部に放電ガスが封入されたものを作
るのは非常に困難である。また、このような球状で小さ
なものを作ったとしても、管壁負荷、つまり(人力/表
面+1)が大きくなり、ランプ寿命が短くなるという欠
点を存する。さらに、金属蒸気の放電を利用する場合に
は、放電中に蒸気圧が著しく上昇し、瞬時再始動が困難
となるという欠点を有する。
In addition, the shape of high-output electrodeless discharge lamps that emit light using electromagnetic waves, which have recently been developed in various places, is spherical as shown in FIG. is enclosed, and an induction coil 13 is wound around the valve 12. If a point light source with such a shape is required, the diameter of the bulb 12 must be reduced, but the bulb 12 is spherical, for example, with a diameter of 10 Il 111, and a discharge gas is sealed inside. is very difficult. Furthermore, even if such a small spherical tube is made, the tube wall load, that is, (manpower/surface + 1) increases, and the lamp life is shortened. Furthermore, when using metal vapor discharge, there is a drawback that the vapor pressure increases significantly during discharge, making instantaneous restart difficult.

[発明が解決しようとする課題] 本発明は上記欠点に鑑みなされたもので、その目的とす
るところは、高出力で点状光源であり、しかも製造容易
で長寿命の無電極放電灯装置を従供するにある。
[Problems to be Solved by the Invention] The present invention has been made in view of the above-mentioned drawbacks, and its purpose is to provide an electrodeless discharge lamp device that is a high-output point light source, is easy to manufacture, and has a long life. It is to obey.

[課題を解決するための手段] 本発明は上記!iBを解決するため、透光性を有する細
長い管状の発光管の一部分に誘導コイルを巻回するとと
もに、該誘導コイルに高周波電流を通電することにより
、前記発光管内空間のうち前記コイル壱同部のみを発光
させて成る無電極放電灯装置において、前記発光管の管
壁に箔状導体よりなる電極を配設するとともに、該電極
に始動時のみ高周波電圧を印加する高周波発生回路を接
続したことを特徴とするものである。
[Means for Solving the Problems] The present invention has the above features! In order to solve the iB problem, an induction coil is wound around a part of a thin and thin light-transmitting arc tube, and a high-frequency current is applied to the induction coil, whereby the same part of the inner space of the arc tube as described above is removed. In the electrodeless discharge lamp device, an electrode made of a foil-like conductor is disposed on the wall of the arc tube, and a high-frequency generating circuit is connected to the electrode for applying a high-frequency voltage only at the time of starting. It is characterized by:

[実施例1] 第1図は本発明の第1の実施例を示すもので、1は長管
状の発光管であって、気密性で透光性を有し、内部には
放電ガスとしてキセノン(Xe)ガス100Torrが
封入されている。なお、発光管1の内径は5Mである。
[Example 1] Fig. 1 shows a first example of the present invention, in which 1 is a long tube-shaped arc tube, which is airtight and translucent, and contains xenon as a discharge gas inside. (Xe) gas of 100 Torr is sealed. Note that the inner diameter of the arc tube 1 is 5M.

2は誘導コイルであって、前記発光管lの一端にソレノ
イド状に数ターン、例えば3ターン巻かれており、コイ
ル2の両端はマツチング回路(図示せず)を経て高周波
発生回路3に接続されている。また、発光管1の他端に
は箔状の導体よりなる一対の電極4.4が、例えば0.
5amの間隔をもって管壁に密着する形で巻き付けられ
ている。そして、各電極4,4はマツチング回路(図示
せず)を経て高周波発生回路5に接続されている。
Reference numeral 2 denotes an induction coil, which is wound around one end of the arc tube l in the shape of a solenoid for several turns, for example three turns, and both ends of the coil 2 are connected to a high frequency generation circuit 3 via a matching circuit (not shown). ing. Further, at the other end of the arc tube 1, a pair of electrodes 4.4 made of a foil-like conductor are provided, for example, with a diameter of 0.5 mm.
It is wound tightly around the tube wall with an interval of 5 am. Each electrode 4, 4 is connected to a high frequency generation circuit 5 via a matching circuit (not shown).

このように構成された無電極放電灯装置において、上記
両電極4.4間に高周波電圧を印加すると、電極4と管
内放電空間の間が静電的な結合で結ばれ、管内空間にお
いて両電極4.4間に高周波電界が発生する。この電界
によりエネルギーを得た電子がXe原子を衝突TIHさ
せる。そして、このように電子が十分に供給された状態
で上記誘導コイル2に高周波電流を流すと、誘導コイル
2の回り、特に発光管lの内部に交番磁界が生じ、その
磁界によって発光管1の内壁に沿うような形で誘導電界
が生しる。従って、この誘導電界によって放電が維持さ
れることになる。誘導電界による放電が維持されると、
始動初期の電極4による放電は不必要となるので、電極
4への高周波電圧印加をやめる。
In the electrodeless discharge lamp device configured as described above, when a high frequency voltage is applied between the two electrodes 4.4, the electrode 4 and the discharge space in the tube are connected by electrostatic coupling, and the two electrodes in the space in the tube are connected by electrostatic coupling. A high frequency electric field is generated between 4.4 and 4. Electrons that have gained energy due to this electric field collide with Xe atoms to cause TIH. When a high-frequency current is passed through the induction coil 2 with a sufficient supply of electrons in this way, an alternating magnetic field is generated around the induction coil 2, especially inside the arc tube 1, and this magnetic field causes the arc tube 1 to move. An induced electric field is generated along the inner wall. Therefore, the discharge is maintained by this induced electric field. When the discharge due to the induced electric field is maintained,
Since the discharge by the electrode 4 at the initial stage of startup becomes unnecessary, the high frequency voltage application to the electrode 4 is stopped.

このようにすると、始動時、両ti4.4間にかかる電
界による放電は管軸方向に伸び、発光管1内全体が発光
するが、誘導コイル2による放電は、コイル壱回部のみ
の発光強度の強いリング状放電となり、非常に点光源に
近い光源が得られる。
In this way, at the time of starting, the discharge due to the electric field applied between both Ti4. This results in a strong ring-shaped discharge, resulting in a light source that is very close to a point light source.

なお、本実施例では放電ガスをキセノンとしたが、上記
給電手段で放電維持できるガスや金属であれば、その種
類、圧力に限定されものでないことは勿論である。
Although xenon was used as the discharge gas in this embodiment, it is needless to say that the type and pressure of the gas or metal are not limited as long as the discharge gas can be maintained by the power supply means.

[実施例21 第2図は本発明の第2の実施例を示すもので、前記実施
例1と異なる点は、発光管1をU字状に屈曲し、その屈
曲部に誘導コイル2を配設したことで、他の構成は前記
実施例1と同様であるので、同等構成に同一符号を付す
ことにより説明を省略する。
Embodiment 21 FIG. 2 shows a second embodiment of the present invention, which differs from the first embodiment in that the arc tube 1 is bent into a U-shape and the induction coil 2 is arranged at the bent part. Since the other configurations are the same as those of the first embodiment, explanations will be omitted by assigning the same reference numerals to the equivalent configurations.

このように構成することにより、同じ体積の発光管lを
使用する場合に、装置全体の大きさをコンパクトに構成
することができる。なお、発光管lを略環状にしても同
様の効果が得られることは勿論である。
With this configuration, when using arc tubes l of the same volume, the overall size of the device can be made compact. Note that, of course, the same effect can be obtained even if the arc tube l is formed into a substantially annular shape.

[実施例3] 第3図は本発明の第3の実施例を示すもので、前記実施
例1と異なる点は、実施例1の構成に加えて、例えば圧
電素子の如き高電圧を発生するような高電圧発生素子6
を、上記電極4の近傍で発光管lに高電圧がかかるよう
な形で配設したことで、他の構成は前記実施例1と同様
であるので、同等構成に同一符号を付すことにより説明
を省略する。
[Embodiment 3] FIG. 3 shows a third embodiment of the present invention, which differs from the first embodiment in that in addition to the structure of the first embodiment, a high voltage generating device such as a piezoelectric element is used. High voltage generating element 6 such as
is arranged in such a way that a high voltage is applied to the arc tube l in the vicinity of the electrode 4, and the other configurations are the same as in Example 1, so the description will be given by assigning the same reference numerals to the equivalent configurations. omitted.

このように構成することにより、さらに始動が困難な状
況でも放電を始動させることが可能となる。つまり、1
段目の始動を高電圧発生素子6で行い、2段目の始動を
画電極4.4間の電界で行い、最終の放電維持は誘導コ
イル2で発生させた誘導電界で行うことにより可能とな
る。
With this configuration, it becomes possible to start the discharge even in situations where starting is more difficult. In other words, 1
The high voltage generating element 6 is used to start the first stage, the second stage is started using the electric field between the picture electrodes 4 and 4, and the final discharge is maintained using the induced electric field generated by the induction coil 2. Become.

[実施例4] 第4図は本発明の第4の実施例を示すもので、本実施例
は、誘導コイル2の接地電位側のコイル端に近接して箔
状の導体よりなる電極4を配設するとともに、誘導コイ
ル2の接地電位側端と電極4との間に高周波電圧を印加
する高周波発生回路5を設けたことを特徴とするもので
あり、このように構成することにより、電極4は1つで
済み、実施例1に比べて構成が簡単になる。
[Embodiment 4] FIG. 4 shows a fourth embodiment of the present invention. In this embodiment, an electrode 4 made of a foil-like conductor is placed close to the coil end on the ground potential side of the induction coil 2. It is characterized in that it is provided with a high frequency generating circuit 5 that applies a high frequency voltage between the ground potential side end of the induction coil 2 and the electrode 4. Only one number 4 is required, and the configuration is simpler than that of the first embodiment.

[発明の効果] 本発明に係る無電極放電灯装置は、上記のように構成し
たことにより、始動時は箔状導体よりなる電極による放
電によるため始動が容易となると共に、始動後は誘導コ
イルによる放電、つまり、コイル巻回部のみの発光強度
の強いリング状放電となるため、非常に点光源に近い長
寿命の光源が得られる。また、発光管は管状であるため
製造も容易である。
[Effects of the Invention] Since the electrodeless discharge lamp device according to the present invention is configured as described above, starting is facilitated by discharge from the electrode made of a foil-like conductor at the time of starting, and the induction coil is activated after starting. In other words, the discharge is a ring-shaped discharge with a strong emission intensity only at the coil winding portion, so a long-life light source that is very close to a point light source can be obtained. Furthermore, since the arc tube is tubular, it is easy to manufacture.

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

第1図は本発明の第1の実施例を示す簡略図、第2図は
本発明の第2の実施例を示す簡略図、第3図は本発明の
第3の実施例を示す簡略図、第4図は本発明の第4の実
施例を示す簡略図、第5図は従来例を示す一部断面の正
面図、第6図は異なる従来例を示す簡略図である。 l・・・発光管、2・・・誘導コイル、3・・・高周波
発生回路、4・・・電極、5・・・高周波発生回路、6
・・・高電圧発生素子。
FIG. 1 is a simplified diagram showing a first embodiment of the invention, FIG. 2 is a simplified diagram showing a second embodiment of the invention, and FIG. 3 is a simplified diagram showing a third embodiment of the invention. , FIG. 4 is a simplified diagram showing a fourth embodiment of the present invention, FIG. 5 is a partially sectional front view showing a conventional example, and FIG. 6 is a simplified diagram showing a different conventional example. l... Arc tube, 2... Induction coil, 3... High frequency generation circuit, 4... Electrode, 5... High frequency generation circuit, 6
...High voltage generating element.

Claims (1)

【特許請求の範囲】[Claims] (1)透光性を有する細長い管状の発光管の一部分に誘
導コイルを巻回するとともに、該誘導コイルに高周波電
流を通電することにより、前記発光管内空間のうち前記
コイル巻回部のみを発光させて成る無電極放電灯装置に
おいて、前記発光管の管壁に箔状導体よりなる電極を配
設するとともに、該電極に始動時のみ高周波電圧を印加
する高周波発生回路を接続したことを特徴とする無電極
放電灯装置。
(1) By winding an induction coil around a portion of a long, thin, translucent tubular arc tube and passing a high-frequency current through the induction coil, only the coil-wound portion of the space within the arc tube emits light. The electrodeless discharge lamp device is characterized in that an electrode made of a foil-like conductor is disposed on the wall of the arc tube, and a high-frequency generating circuit is connected to the electrode for applying a high-frequency voltage only at the time of starting. Electrodeless discharge lamp device.
JP16339190A 1990-06-21 1990-06-21 Electrodeless discharge lamp device Pending JPH0456059A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16339190A JPH0456059A (en) 1990-06-21 1990-06-21 Electrodeless discharge lamp device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16339190A JPH0456059A (en) 1990-06-21 1990-06-21 Electrodeless discharge lamp device

Publications (1)

Publication Number Publication Date
JPH0456059A true JPH0456059A (en) 1992-02-24

Family

ID=15772998

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16339190A Pending JPH0456059A (en) 1990-06-21 1990-06-21 Electrodeless discharge lamp device

Country Status (1)

Country Link
JP (1) JPH0456059A (en)

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