JPH0195494A - Illumination device - Google Patents

Illumination device

Info

Publication number
JPH0195494A
JPH0195494A JP25291987A JP25291987A JPH0195494A JP H0195494 A JPH0195494 A JP H0195494A JP 25291987 A JP25291987 A JP 25291987A JP 25291987 A JP25291987 A JP 25291987A JP H0195494 A JPH0195494 A JP H0195494A
Authority
JP
Japan
Prior art keywords
high frequency
electromagnetic field
coil
fluorescent lamp
discharge
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
JP25291987A
Other languages
Japanese (ja)
Inventor
Shinichi Konishi
信一 小西
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 Holdings Corp
Original Assignee
Matsushita Electric Industrial Co 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 Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP25291987A priority Critical patent/JPH0195494A/en
Publication of JPH0195494A publication Critical patent/JPH0195494A/en
Pending legal-status Critical Current

Links

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  • Arrangement Of Elements, Cooling, Sealing, Or The Like Of Lighting Devices (AREA)
  • Circuit Arrangements For Discharge Lamps (AREA)
  • Discharge Lamps And Accessories Thereof (AREA)

Abstract

PURPOSE:To obtain a illumination device with efficient illumination by providing a vessel where a fluorescent material is applied and one or more kind of metal and rare gas is sealed and an electromagnetic field generation means comprising a conductor including a superconducting member applying a high frequency electronic field to the inside of this vessel. CONSTITUTION:There is no internal resistance as a coil 1b is composed of a superconducting member. When a power switch 1a is put ON and a high frequency voltage is applied to the coil 1b by a high frequency power supply 1c, the high frequency current flows to produce high frequency electromagnetic field, making rare gas sealed in a fluorescent lamp 2 start discharge. The discharge of the gas 2a vaporizes granular mercury 2b in the lamp 2 to perform discharge, mainly by mercury vapor. Then mercury vapor generates much ultraviolet light beams as well as green light beams, and the ultraviolet beams are converted into a visible light by means of phosphor material 2c applied on a tube wall to allow a fluorescent lamp 2 to illuminate. Electrical resistance is turned to be zero by composing the coil 1b of the superconducting material in this way. It is thus possible to eliminate heat generation and heat loss, and to improve the efficiency of electromagnetic field, namely illumination efficiency.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は高周波電磁界を利用して発光する照明装置に関
する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a lighting device that emits light using a high frequency electromagnetic field.

従来の技術 従来蛍光灯は、希ガス及び水銀を封入された容器の2箇
所にフィラメントを構成し、該2箇所のフィラメント間
に交流電圧を印加し、点灯していた。しかし上記の構成
によれば、フィラメントの消耗により寿命が短いと言う
問題点があった。
BACKGROUND OF THE INVENTION Conventional fluorescent lamps have filaments at two locations in a container filled with rare gas and mercury, and are lit by applying an alternating current voltage between the two filaments. However, according to the above configuration, there is a problem that the service life is short due to consumption of the filament.

この問題点を解決するために以下に示す技術が考案され
ている。
In order to solve this problem, the following techniques have been devised.

第4図は従来の問題点を解決す、る照明装置を示す概略
構成図である。第4図において31は電磁界発生手段、
31aは電磁界発生手段の電源スィッチ、32は蛍光灯
である。第5図は電磁界発生手段31の等価回路を示す
回路図である。第5図において第4図と同じ構成要素の
ものは同符号を付し説明を省略する。31bは高周波電
源、31Cは蛍光灯32に高周波電磁界を印加するコイ
ル、Rしはコイル31cの内部抵抗である。
FIG. 4 is a schematic configuration diagram showing a lighting device that solves the conventional problems. In FIG. 4, 31 is an electromagnetic field generating means;
31a is a power switch for the electromagnetic field generating means, and 32 is a fluorescent lamp. FIG. 5 is a circuit diagram showing an equivalent circuit of the electromagnetic field generating means 31. In FIG. 5, the same components as those in FIG. 4 are designated by the same reference numerals, and their explanation will be omitted. 31b is a high frequency power supply, 31C is a coil that applies a high frequency electromagnetic field to the fluorescent lamp 32, and R is an internal resistance of the coil 31c.

以下第4図と第5図を用いて該照明装置の動作を説明す
る。まず電源スィッチ31aを投入し、高周波型83 
l bによりコイル31cに高周波電圧を印加するとコ
イル31cに高周波電流が流れ高周波電磁界が発生する
。発生された高周波電磁界により蛍光灯32の中に封入
された希ガスが放電を始める。希ガスの放電により蛍光
灯32中の水銀が蒸発し、水銀蒸気による放電を主とし
た放電が行われる。この放電で水銀蒸気により緑色の光
線とともに紫外線が多量に生じ、この紫外線が管壁に塗
布された蛍光物質により可視光に変換され蛍光灯32が
発光する。
The operation of the lighting device will be explained below using FIGS. 4 and 5. First, turn on the power switch 31a, and turn on the high frequency type 83.
When a high frequency voltage is applied to the coil 31c by lb, a high frequency current flows through the coil 31c and a high frequency electromagnetic field is generated. The generated high-frequency electromagnetic field causes the rare gas sealed in the fluorescent lamp 32 to start discharging. The mercury in the fluorescent lamp 32 evaporates due to the rare gas discharge, and a discharge mainly caused by mercury vapor is performed. This discharge produces a large amount of green light and ultraviolet rays due to the mercury vapor, and the ultraviolet rays are converted into visible light by the fluorescent material coated on the tube wall, causing the fluorescent lamp 32 to emit light.

上記説明した構成によれば、蛍光灯の寿命が従来のフィ
ラメントのある蛍光灯より約3から5倍程度寿命が長く
、電源投入から点灯までの時閉が短いという特徴がある
According to the configuration described above, the life of the fluorescent lamp is about 3 to 5 times longer than that of a conventional fluorescent lamp with a filament, and the lifespan of the fluorescent lamp is about 3 to 5 times longer, and the time of closing from power-on to lighting is short.

発明が解決しようとする問題点 しかし上記の構成によれば高周波電磁界を発生させる電
磁界発生手段のコイルには抵抗RLがある。
Problems to be Solved by the Invention However, according to the above configuration, there is a resistor RL in the coil of the electromagnetic field generating means for generating the high frequency electromagnetic field.

抵抗RLは導線の長さに比例し、断面積に反比例する。Resistance RL is proportional to the length of the conductor and inversely proportional to its cross-sectional area.

例えば、直径0. 5mm゛の銅線をlkm巻いたコイ
ルの場合、該コイルの抵抗は約90オームとなり、電流
をIA流したとすると、毎秒21゜6J程度の熱が発生
する。この発熱による損失により電磁界の発生効−が悪
くなる。即ち、発光効率が悪くなるという問題があった
。   −本発明は上記の問題点に鑑みてなされたもの
で、熱損失がなく電磁界の発生効率のよい電磁界発生手
段を得るとともに発光効率のよい照明装置を提供するこ
とを目的とする。
For example, diameter 0. In the case of a coil made of 1 km of 5 mm copper wire, the resistance of the coil is approximately 90 ohms, and if a current of IA is passed through the coil, heat of approximately 21° 6 J is generated per second. The loss due to this heat generation deteriorates the effectiveness of generating an electromagnetic field. That is, there was a problem that the luminous efficiency deteriorated. - The present invention has been made in view of the above-mentioned problems, and aims to provide an electromagnetic field generating means with no heat loss and high efficiency in generating an electromagnetic field, and a lighting device with high luminous efficiency.

問題点を解決するための手段 本発明は上記の目的を達成するために、少なくとも一部
に蛍光物質が塗布され一種類以上の金属と希ガスを封入
された容器と、該容器内に高周波電磁界を印加する超伝
導部材を含む導体からなる電磁界発生手段とを備えた構
成とするものである。
Means for Solving the Problems In order to achieve the above object, the present invention provides a container at least partially coated with a fluorescent substance and filled with one or more metals and a rare gas, and a high-frequency electromagnetic device inside the container. The electromagnetic field generating means includes an electromagnetic field generating means made of a conductor including a superconducting member that applies a field.

作用 本発明は上記した構成により、超伝導部材を含む導体か
ら構成した電磁界発生手段を用いることにより、熱損失
がなく電磁界の発生効率のよい電磁界発生手段とし、発
光効率のよい照明装置を得ることができる。
Effect of the Invention The present invention uses the electromagnetic field generating means made of a conductor including a superconducting member to provide an electromagnetic field generating means that has no heat loss and has high electromagnetic field generation efficiency, and provides a lighting device with high luminous efficiency. can be obtained.

実施例 第1図は本発明の一実施例を示す照明装置の概略構成図
である。第1図において1は高周波電磁界を発生する電
磁界発生手段であり、その外装は高周波電磁波を透過し
ない物質で構成されている。
Embodiment FIG. 1 is a schematic diagram of a lighting device showing an embodiment of the present invention. In FIG. 1, reference numeral 1 denotes an electromagnetic field generating means for generating a high frequency electromagnetic field, and its exterior is made of a material that does not transmit high frequency electromagnetic waves.

laは電磁界発生手段の電源スィッチ、2は蛍光灯であ
る。第2図は電磁界発生手段lの等価回路を示す回路図
である。第2図において第1図と同じ構成要素のものは
同符号を付し説明を省略する。
la is a power switch for the electromagnetic field generating means, and 2 is a fluorescent lamp. FIG. 2 is a circuit diagram showing an equivalent circuit of the electromagnetic field generating means l. In FIG. 2, the same components as in FIG. 1 are designated by the same reference numerals and their explanations will be omitted.

1bは超伝導部材で構成したコイル、lcはコイルlb
に高周波電圧を印加する高周波電源である。
1b is a coil made of superconducting material, lc is coil lb
This is a high-frequency power supply that applies a high-frequency voltage to the

ここでコイル1bは超伝導部材で構成しているので内部
抵抗は存在しない。なお超伝導部材は例えば、5rBa
YCutOe−、Y−=Ba−Cu−0、Er−Ba=
Cu−()などを用いればよい。
Here, since the coil 1b is made of a superconducting member, there is no internal resistance. Note that the superconducting member is, for example, 5rBa
YCutOe-, Y-=Ba-Cu-0, Er-Ba=
Cu-() or the like may be used.

第3図は蛍光灯2の構成を示す断面図である。FIG. 3 is a sectional view showing the structure of the fluorescent lamp 2. As shown in FIG.

第3図において2aはアルゴンガス等の希ガス、2bは
水銀、2Cは蛍光物質である。
In FIG. 3, 2a is a rare gas such as argon gas, 2b is mercury, and 2C is a fluorescent substance.

以下本実施例における照明装置の動作を第1図、第2図
及び第3図を用いて説明する。電源スィッチlaを投入
し高周波電源1cによりコイルlbに高周波電圧を印加
すると高周波電流が流れ高周波電磁界を発生する。この
高周波電磁界により蛍光灯2中に封入された希ガス2a
が放電を始める。
The operation of the lighting device in this embodiment will be explained below with reference to FIGS. 1, 2, and 3. When the power switch la is turned on and a high frequency voltage is applied to the coil lb by the high frequency power supply 1c, a high frequency current flows and a high frequency electromagnetic field is generated. The rare gas 2a sealed in the fluorescent lamp 2 by this high frequency electromagnetic field
begins to discharge.

希ガス2aの放電により蛍光灯2中の粒状の水銀2bが
蒸発し、水銀蒸気による放電を主とした放電が行われる
。この放電、で水銀蒸気により緑色の光線とともに紫外
線が多量に生じ、この紫外線が管壁に塗布された蛍光物
質2cにより可視光に変換され蛍光灯2が発光する。
Due to the discharge of the rare gas 2a, the particulate mercury 2b in the fluorescent lamp 2 evaporates, and a discharge mainly caused by mercury vapor is performed. During this discharge, a large amount of green light and ultraviolet rays are generated by the mercury vapor, and the ultraviolet rays are converted into visible light by the fluorescent material 2c applied to the tube wall, causing the fluorescent lamp 2 to emit light.

本実施例では蛍光灯は管状のものを使用しているが、蛍
光灯の形状はどんな形状でもよい。また本実施例では蛍
光灯に封入する金属を水銀としたが同じ効果を示すよう
な金属であればよい。
In this embodiment, a tubular fluorescent lamp is used, but the fluorescent lamp may have any shape. Further, in this embodiment, the metal sealed in the fluorescent lamp was mercury, but any metal that exhibits the same effect may be used.

以上のように電磁界発生手段のコイルを超伝導部材で構
成することにより電気抵抗が零となるためコイルの発熱
がなく熱損失は零となり、電磁Wの発生効率、即ち発光
効率がよくなる。またコイルの熱損失がなく電磁界の発
生効率がよくなるので、従来と同じ強度の電磁界を得る
のに必要な高周波電源は従来に比べて小型に構成するこ
とができる。
As described above, by configuring the coil of the electromagnetic field generating means from a superconducting member, the electrical resistance becomes zero, so the coil does not generate heat and heat loss becomes zero, improving the electromagnetic W generation efficiency, that is, the luminous efficiency. Furthermore, since there is no heat loss in the coil and the efficiency of electromagnetic field generation is improved, the high frequency power supply required to obtain the same electromagnetic field strength as the conventional one can be configured to be smaller than the conventional one.

発明の詳細 な説明したように、本発明によれは電磁界発生手段の発
熱による熱ti失は零となり、電磁界発生手段の電磁界
の発生効率、即ち発光効率がよくなるので実用上極めて
有効である。
As described in detail, according to the present invention, the loss of heat due to heat generated by the electromagnetic field generating means is reduced to zero, and the electromagnetic field generating efficiency of the electromagnetic field generating means, that is, the luminous efficiency is improved, so that it is extremely effective in practice. be.

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

第1図は本発明の一実施例を示す照明装置の概略構成図
、第2図は同装置の電磁界発生手段の等価回路を示す回
路図、第3図は同装置の蛍光灯の構成を示す断面図、第
4図は従来の照明装置を示す概略構成図、第5図は同装
置の電磁界発生手段の等価回路を示す回路図である。 l・・・電磁界発生手段、2・・・蛍光灯。 代理人の氏名 弁理士 中尾敏男 はか1名第1図 第2図 第3図
Fig. 1 is a schematic configuration diagram of a lighting device showing an embodiment of the present invention, Fig. 2 is a circuit diagram showing an equivalent circuit of the electromagnetic field generating means of the same device, and Fig. 3 is a diagram showing the configuration of a fluorescent lamp of the same device. 4 is a schematic configuration diagram showing a conventional illumination device, and FIG. 5 is a circuit diagram showing an equivalent circuit of an electromagnetic field generating means of the same device. 1... Electromagnetic field generating means, 2... Fluorescent lamp. Name of agent: Patent attorney Toshio Nakao (1 person) Figure 1 Figure 2 Figure 3

Claims (1)

【特許請求の範囲】[Claims] 少なくとも一部に蛍光物質が塗布され一種類以上の金属
と希ガスを封入された容器と、この容器内に高周波電磁
界を印加する超伝導部材を含む導体からなる電磁界発生
手段とを備えたことを特徴とする照明装置。
A container having at least a portion coated with a fluorescent substance and filled with one or more metals and a rare gas, and an electromagnetic field generating means made of a conductor including a superconducting member that applies a high frequency electromagnetic field to the container. A lighting device characterized by:
JP25291987A 1987-10-07 1987-10-07 Illumination device Pending JPH0195494A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25291987A JPH0195494A (en) 1987-10-07 1987-10-07 Illumination device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25291987A JPH0195494A (en) 1987-10-07 1987-10-07 Illumination device

Publications (1)

Publication Number Publication Date
JPH0195494A true JPH0195494A (en) 1989-04-13

Family

ID=17243993

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25291987A Pending JPH0195494A (en) 1987-10-07 1987-10-07 Illumination device

Country Status (1)

Country Link
JP (1) JPH0195494A (en)

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