JPS60167256A - Electrodeless electric-discharge lamp - Google Patents

Electrodeless electric-discharge lamp

Info

Publication number
JPS60167256A
JPS60167256A JP2248984A JP2248984A JPS60167256A JP S60167256 A JPS60167256 A JP S60167256A JP 2248984 A JP2248984 A JP 2248984A JP 2248984 A JP2248984 A JP 2248984A JP S60167256 A JPS60167256 A JP S60167256A
Authority
JP
Japan
Prior art keywords
bulbs
concave areas
discharge lamp
electric
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.)
Pending
Application number
JP2248984A
Other languages
Japanese (ja)
Inventor
Koichi Kobayashi
小林 耕一
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 JP2248984A priority Critical patent/JPS60167256A/en
Publication of JPS60167256A publication Critical patent/JPS60167256A/en
Pending 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
    • H01J65/048Lamps 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 using an excitation coil

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Discharge Lamps And Accessories Thereof (AREA)

Abstract

PURPOSE:To enable magnetic line of force to be effectually utilized for emission by placing a pair of semispherical airtight bulbs having a concave area on their bottom in such a manner as to cause the concave areas to face each other and installing high-frequency oscillating coils in the concave areas. CONSTITUTION:Semispherical airtight bulbs 10a and 10b are prepared from glass or similar material and have concave areas 11a and 11b on their bottoms. The inner surfaces of the bulbs 10a and 10b are coated with a phosphor 12 and a light-transmitting high-frequency-electric-wave-shielding film 13. The bulbs 10a and 10b are charged with mercury and an inactive gas and connected facing each other by means of a cylindrical support 14. High-frequency oscillating coils 15a and 15b are placed in the concave areas 11a and 11b and connected to a power supply 17 through an oscillator 16. Owing to the above constitution of an electrodeless electric-discharge lamp, magnetic line of force can be effectually contributed to emission by equalizing the directions of the polarities of the oscillating coils 15a and 15b. Consequently, the luminous efficiency of the lamp can be increased and the leakage of electric wave can be reduced.

Description

【発明の詳細な説明】 〔技術分野〕 本発明は、高周波電磁界によってバルブ内の金属を励起
し、けい光体を塗布したバlレブを通して可視光を発光
させる無電極放電ランプに関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to an electrodeless discharge lamp in which metal within the bulb is excited by a high-frequency electromagnetic field to emit visible light through a bulb coated with a phosphor.

〔背景技術〕[Background technology]

一般の白熱電球は、広く使用されているが、この白熱電
球は効率は低く、lO〜l5ltn/W程度であり、ま
た寿命も約i、 ooo 時間と短かい。
Although general incandescent light bulbs are widely used, the efficiency of these incandescent light bulbs is low, on the order of 10 to 15ltn/W, and the lifespan is short, about 1,000 hours.

それに対して、一般のけい光ランプは効率が50〜go
I!m/wと白熱電球に比べ高く、寿命も約5,000
時間と長いが、長い盲状のガラス管および補助の安定装
置を必要とし、家庭の白熱電球の代替は困難である。
In contrast, ordinary fluorescent lamps have an efficiency of 50~go.
I! m/w is higher than incandescent bulbs, and the lifespan is approximately 5,000 yen.
Although time consuming and requiring long blind glass tubes and auxiliary ballasts, it is difficult to replace household incandescent light bulbs.

このような背景から、現在設置されている白熱電球用器
具に直接適合し得る、白熱電球用口金を何する小型のけ
い光ランプが種々開発されており、無電極放電ランプも
その中の1つである。
Against this background, various small fluorescent lamps with different incandescent lamp bases have been developed that can be directly adapted to currently installed incandescent lamp fixtures, and electrodeless discharge lamps are one of them. It is.

$1図はかかる無電極放電ランプの一例を示すものであ
り、ガラス等の透光性拐料からなる気密性容器、いわゆ
るパルプ1は、両端部2.2′がそれぞれ向い合った半
球状であり、その間を小径円筒部3で連結されて込る。
Figure $1 shows an example of such an electrodeless discharge lamp, and an airtight container made of a translucent material such as glass, so-called pulp 1, has a hemispherical shape with both ends 2 and 2' facing each other. There is a small diameter cylindrical part 3 connected between them.

そして、その小径円筒部3には、高周波発振コイル4が
装着されている。
A high frequency oscillation coil 4 is attached to the small diameter cylindrical portion 3.

高周波発振コイル・4は高周波発振器5を介して電源6
に接続されている。また、上記バ7レブ1の内部7には
、けい光励起ガスとして、水銀等の金属蒸気およびアル
ゴン等の不活性ガスが封入されて1おり、バルブ1の内
面には、紫外線を可視光に変換するためのけい光体8及
び高周波電磁界による電波漏洩を防ぐための透光性の高
周波電波遮へい膜9が被着されている。
The high frequency oscillation coil 4 is connected to the power supply 6 via the high frequency oscillator 5.
It is connected to the. Further, the inside 7 of the valve 7 rev 1 is filled with metal vapor such as mercury and inert gas such as argon as a fluorescence excitation gas. A phosphor 8 for preventing leakage of radio waves due to high frequency electromagnetic fields and a translucent high frequency radio wave shielding film 9 for preventing leakage of radio waves due to high frequency electromagnetic fields are attached.

かかる放電ランプは、高周波発振コイル4によって、高
周波電場および磁場が作り出され、この電磁場が、コイ
ル4の両端部に配されたバルブ両側部2.2/内の金属
蒸気を励起させ、この金属蒸気が電離して発生した紫外
線が、パルプ1内面のけい光体8を通過して可視光とな
りバlレプ1外部に放射される。その時の磁力線は、第
1図において破線で示したように、発振コイル4の内面
からパルプ1の一方の端部2から外部に出て、外周を経
てパlレプ1の他方の端部21から内部に入ってくる。
In such a discharge lamp, a high-frequency electric field and a magnetic field are created by a high-frequency oscillation coil 4, and this electromagnetic field excites the metal vapor within the bulb both sides 2.2/ disposed at both ends of the coil 4. The ultraviolet light generated by ionization passes through the phosphor 8 on the inner surface of the pulp 1 and becomes visible light, which is emitted to the outside of the pulp 1. At that time, the lines of magnetic force go from the inner surface of the oscillation coil 4 to the outside from one end 2 of the pulp 1, pass through the outer periphery, and exit from the other end 21 of the pulp 1, as shown by the broken line in FIG. come inside.

その時バルブ1の内面には、高周波′嵯波遮へい膜9が
被着されており、電波障害等の原因となる磁力線が、バ
ルブ1の外部に出ることを防止しているが、実際問題と
して、完全に遮へいできず、ある程度外部に洩れる。そ
の場合、磁力線はコイ/L/4による円筒空間の中心部
より外周部に近い所から発生し、短かいル−プを描くよ
うな磁場を持つ。すなわちバlレプ1の中心線付近より
側部付近の方が磁場が強い。このことより、電波漏洩も
パルプ両端部2.2/と、それらを連結している小径円
筒部3との接合面付近が最も電波漏洩が高くなる。しか
し、この付近の磁力線は、バルブ1内を通過する距離は
短かく、放電による発光ということにあまり寄与してい
ない。
At this time, a high frequency wave shielding film 9 is coated on the inner surface of the bulb 1 to prevent lines of magnetic force that may cause radio wave interference from exiting the bulb 1, but as a practical matter, It cannot be completely shielded and leaks to the outside to some extent. In this case, the lines of magnetic force are generated closer to the outer periphery than the center of the cylindrical space formed by the coil/L/4, and have a magnetic field that draws a short loop. That is, the magnetic field is stronger near the side of the valve 1 than near the center line. From this, the radio wave leakage is highest near the joint surface between the pulp both ends 2.2/ and the small diameter cylindrical part 3 connecting them. However, the magnetic field lines in this vicinity have a short distance to pass through the inside of the bulb 1, and do not contribute much to light emission due to discharge.

つまり、第1図に示すような構度の無電極放電ランプに
おいては、高周波発振コイIし4による円筒空間の外周
部付近から発生する磁力線は、ランプの発光効率の点で
は無意味で、ただ電波漏洩を引き起こすだけのものであ
り、発光効率の割に、電波漏洩北軍が普く大きな欠点と
なる。
In other words, in an electrodeless discharge lamp configured as shown in Fig. 1, the magnetic lines of force generated near the outer periphery of the cylindrical space by the high-frequency oscillating coil I and 4 are meaningless in terms of luminous efficiency of the lamp, and are simply It only causes radio wave leakage, and despite its luminous efficiency, radio wave leakage is a major drawback.

〔発明の目的〕[Purpose of the invention]

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、高周波発振コイルによって発生した磁力線
で発光に寄与しない磁力線を低減すると共に、ランプか
らの電波漏洩を低減した無電極・放電ランプを提供する
にある。
The present invention was made in view of the above-mentioned drawbacks, and its purpose is to reduce the magnetic lines of force generated by a high-frequency oscillation coil that do not contribute to light emission, and to reduce the leakage of radio waves from the lamp in an electrodeless discharge lamp. is to provide.

〔発明の開示〕[Disclosure of the invention]

以下、本発明を第2図に示す実施例に基づき説・、盟5
する・ 第2図において、lOa、lobはそれぞれ底面に空洞
部11a、llbを有する半球状のパルプであって、ガ
ラス等の透光性材料で気密に形成され、内面にはけい光
体稔及び透光性を有する高周波電波遮へい脱Bが被着さ
れている。14は上記1対のパルプLOa、lObを連
結する円筒状の支持体、15a、15bは上記空洞部1
1a、llbに配設された高周波発振コイルであって、
上記支持体14の内部に収納された高周波発振器16を
介して、電源17に接続されている。
Hereinafter, the present invention will be explained based on the embodiment shown in FIG.
In Fig. 2, lOa and lob are hemispherical pulps having cavities 11a and llb on the bottom, respectively, and are airtightly formed of a translucent material such as glass, and the inner surface has phosphor particles and A high-frequency radio wave shielding layer B having translucent properties is applied. 14 is a cylindrical support that connects the pair of pulps LOa and LOb; 15a and 15b are the hollow portions 1;
A high frequency oscillation coil disposed in 1a and llb,
It is connected to a power source 17 via a high frequency oscillator 16 housed inside the support body 14 .

なお、上記バルブlOa、lObの内部には、従来例と
同様に、水銀等の金属蒸気及びアルゴン等の不活性ガス
が少なくとも1種類封入されている。
Note that, like the conventional example, at least one kind of metal vapor such as mercury and inert gas such as argon is sealed inside the valves lOa and lOb.

而して、発振コイル15a、 15bの極性を、例えば
、第2図に示す如く上部をN極とし下部をS極とすると
、電源17投入後、両発振コイ1v15a、15bから
発生する磁力線は、それぞれパルプIOa、IOb側(
図において左側の発振コイル15aでは左側、右側の発
振コイル15bでは右側)へ多く発生し、ランプ中心部
方向(図において左側の発振コイ/L/15aでは右側
、右側の発振コイル15bでは左側)へ発生する磁力線
は、両発振コイル15a、15bの極性が同じことから
反発し合い少なくなる。
If the polarities of the oscillating coils 15a and 15b are, for example, as shown in FIG. 2, with the upper part being the N pole and the lower part being the S pole, then after the power supply 17 is turned on, the lines of magnetic force generated from both the oscillating coils 1v15a and 15b are as follows. Pulp IOa and IOb side (
In the diagram, most of the generation occurs to the left in the oscillation coil 15a on the left, to the right in the oscillation coil 15b on the right), and toward the center of the lamp (to the right in the oscillation coil L/15a on the left in the diagram, and to the left in the oscillation coil 15b on the right). Since the polarities of both oscillation coils 15a and 15b are the same, the generated lines of magnetic force repel each other and are reduced.

各パルプlOa、lOb側へ出た磁力線は、バMプ内の
水銀等の金属蒸気を励起させ、その電離によって発生し
た紫外線が、パVプ内面に塗布したけい光体臣を透過し
て可視光となって外部に出る。このことから、発振コイ
ル15a、15bによって発生した磁力線の大部分は有
効にパルプloa、lOb内を通過し、発光に薔与する
ことになり、発光効率は同上する。
The magnetic lines of force coming out to each pulp lOa and lOb side excites metal vapor such as mercury in the pulp, and the ultraviolet rays generated by the ionization pass through the phosphor coated on the inside of the pulp and become visible. It becomes light and goes outside. From this, most of the magnetic lines of force generated by the oscillation coils 15a and 15b effectively pass through the pulps loa and lOb and contribute to light emission, so that the luminous efficiency is the same as above.

また、上記実施例においては、両パルプloa。Moreover, in the above example, both pulp loa.

tabを連結する支持体14の内部に高周波発振器16
を収納する構成であるため、小型化を図ることができる
A high frequency oscillator 16 is installed inside the support 14 that connects the tab.
Since it is configured to accommodate the following, it is possible to achieve miniaturization.

〔発明の効果〕〔Effect of the invention〕

本発明は上記のように、底面側に空洞を有する1対の半
球状見苦容器でバルブを構成すると共に、上記各空洞内
に高周波発振コイルをそれぞれ収納し、かつ両発振コイ
ルの極性を同方回としたので、発振コイルより発生する
磁力線を発光に有効に寄与することができ、発光効率の
向上が図れ、しかも電波漏洩の少ない無電極放電ランプ
を提供できた。
As described above, the present invention comprises a bulb consisting of a pair of unsightly hemispherical containers each having a cavity on the bottom side, a high frequency oscillation coil is housed in each of the cavities, and the polarities of both oscillation coils are set to be the same. Since the magnetic field lines generated by the oscillation coil can effectively contribute to light emission, it is possible to improve luminous efficiency and provide an electrodeless discharge lamp with less radio wave leakage.

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

第1図は従来例の簡略断面1伯、第2図は本発明の一実
施例を示す商略断面図である。 10a、lob・・・パルプ、lla、 llb・・・
空洞、ν・・・けい光体、15 a * 15 b・・
・高周波発振コイM0特許出願人 松下電工株式会社 代理人弁理士 竹元敏丸(ほか2名) 第1図 第2図
FIG. 1 is a simplified cross-sectional view of a conventional example, and FIG. 2 is a commercially simplified cross-sectional view of an embodiment of the present invention. 10a, lob...pulp, lla, llb...
Cavity, ν...phosphor, 15 a * 15 b...
・High-frequency oscillation carp M0 patent applicant Matsushita Electric Works Co., Ltd. Representative patent attorney Toshimaru Takemoto (and 2 others) Figure 1 Figure 2

Claims (1)

【特許請求の範囲】[Claims] (1) バルブ内に封入した金属蒸気を、高周波発振コ
イpによって発生させた電磁場によって励起させると共
に、バルブ内面に塗布したけい光体を介してバルブ外に
可視光を発光させて成る無電極放電ランプにおいて、上
記パルプを、底面側に空洞を有する1対の半球状気密容
器を該空洞が相対するように配置して形成すると共に、
上記高周波発振コイルを上記各空洞内に、互いに極性が
同方向になるように配設したことを特徴とする無電極放
電ランプ。
(1) An electrodeless discharge in which metal vapor sealed inside a bulb is excited by an electromagnetic field generated by a high-frequency oscillating coil p, and visible light is emitted outside the bulb via a phosphor coated on the inner surface of the bulb. In the lamp, the pulp is formed by arranging a pair of hemispherical airtight containers having cavities on the bottom side so that the cavities face each other, and
An electrodeless discharge lamp characterized in that the high frequency oscillation coils are arranged in each of the cavities so that their polarities are in the same direction.
JP2248984A 1984-02-08 1984-02-08 Electrodeless electric-discharge lamp Pending JPS60167256A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2248984A JPS60167256A (en) 1984-02-08 1984-02-08 Electrodeless electric-discharge lamp

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2248984A JPS60167256A (en) 1984-02-08 1984-02-08 Electrodeless electric-discharge lamp

Publications (1)

Publication Number Publication Date
JPS60167256A true JPS60167256A (en) 1985-08-30

Family

ID=12084138

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2248984A Pending JPS60167256A (en) 1984-02-08 1984-02-08 Electrodeless electric-discharge lamp

Country Status (1)

Country Link
JP (1) JPS60167256A (en)

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