JPS6241364B2 - - Google Patents

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Publication number
JPS6241364B2
JPS6241364B2 JP8939480A JP8939480A JPS6241364B2 JP S6241364 B2 JPS6241364 B2 JP S6241364B2 JP 8939480 A JP8939480 A JP 8939480A JP 8939480 A JP8939480 A JP 8939480A JP S6241364 B2 JPS6241364 B2 JP S6241364B2
Authority
JP
Japan
Prior art keywords
tube
discharge
magnetic field
phosphor layer
light
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
JP8939480A
Other languages
Japanese (ja)
Other versions
JPS5713686A (en
Inventor
Makoto Toho
Seigo Wada
Minoru Yamamoto
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 JP8939480A priority Critical patent/JPS5713686A/en
Publication of JPS5713686A publication Critical patent/JPS5713686A/en
Publication of JPS6241364B2 publication Critical patent/JPS6241364B2/ja
Granted legal-status Critical Current

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

Description

【発明の詳細な説明】 本発明は一本の放電灯で複数種の性質の光を得
ることができるという放電灯装置に関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a discharge lamp device that can obtain light of a plurality of types with a single discharge lamp.

従来の放電灯装置はたとえば第1図及び第2図
に示すごとく、けい光ランプ1のガラス管2の内
壁に2種類のけい光体層3,4を分配被着し、上
記けい光ランプ1を本体5に装着することにより
2種類の光を得ている。すなわち第1図に示すよ
うに、けい光ランプ1を本体5に装着して点灯し
た場合において室内照射に有効な光は、そのほと
んどが照射面に向かつた側のけい光体層、すなわ
ち第1図においてはけい光体層4から発せられた
光である。したがつて、けい光体層4が下方にく
るように本体5に装着することにより、けい光体
層4のみをもつけい光ランプと同様な室内照明を
行なうことができ、逆に、けい光ランプ1を180
度回転させてけい光体層3を下方にすることによ
り、けい光体層3のみをもつけい光ランプと同様
な室内照明を行なうことができるというものであ
る。
In a conventional discharge lamp device, for example, as shown in FIGS. 1 and 2, two types of phosphor layers 3 and 4 are distributed and deposited on the inner wall of a glass tube 2 of a fluorescent lamp 1. By attaching it to the main body 5, two types of light are obtained. That is, as shown in FIG. 1, when the fluorescent lamp 1 is attached to the main body 5 and turned on, most of the light that is effective for indoor irradiation is emitted from the phosphor layer on the side facing the irradiation surface, that is, the phosphor layer. In FIG. 1, the light is emitted from the phosphor layer 4. Therefore, by attaching the phosphor layer 4 to the main body 5 with the phosphor layer 4 facing downward, it is possible to provide indoor lighting similar to a fluorescent lamp using only the phosphor layer 4; Lamp 1 to 180
By rotating the phosphor layer 3 so that the phosphor layer 3 is facing downward, it is possible to provide indoor lighting similar to a fluorescent lamp using only the phosphor layer 3.

然し乍ら上述した従来の放電灯装置においては
たとえば第1図に示すごとくけい光体層4を下方
に向け該けい光体層4の光のみを得ようとしても
けい光ランプ1内の放電域は略均一であるためけ
い光体層3も発光しており、けい光体層3による
光が管内で反射して下方へ出てきたり、またけい
光ランプ1外方へ照射されたのち上記本体5や天
井面で反射して下方を照らしたりするので、上記
けい光体層4の光にけい光体層3による光が混じ
り、従つて発光色の調整が甚だ困難であるだけで
なく、けい光体層4による光のみを得るには効率
が悪くならざるを得なかつた。
However, in the above-mentioned conventional discharge lamp device, even if the phosphor layer 4 is directed downward as shown in FIG. 1 to obtain only the light from the phosphor layer 4, the discharge area within the fluorescent lamp 1 is approximately Since the phosphor layer 3 is uniform, it also emits light, and the light from the phosphor layer 3 is reflected inside the tube and comes out downward, and after being irradiated outward from the phosphor lamp 1, the light from the phosphor layer 3 is emitted. Since the light from the phosphor layer 3 is mixed with the light from the phosphor layer 4 because it is reflected from the ceiling surface and illuminates the downward direction, it is not only extremely difficult to adjust the emitted light color, but also because the phosphor layer In order to obtain only light from layer 4, the efficiency had to be poor.

これに対し第3図及び第4図に示すごとくけい
光ランプ1の一端に2個の電極6,7を設け、該
電極6,7に各々対向する他端の電極(図示して
いない)への放電路を各々独立させるための分離
壁8をガラス管2内に設け、各々の放電路9,1
0に互いに異なつたけい光体層11,12を被着
させ、上記放電路9,10を流れる電流を互いに
調整することにより発光色を変えるという放電灯
装置も提示されてはいたが、けい光ランプ1の製
造方法が甚だ複雑であるし、二対の電極をけい光
ランプ1が有するため点灯回路にも工夫を要する
という不都合があつた。
On the other hand, as shown in FIGS. 3 and 4, two electrodes 6 and 7 are provided at one end of the fluorescent lamp 1, and electrodes (not shown) at the other end opposite to the electrodes 6 and 7 are connected to each other. A separation wall 8 is provided in the glass tube 2 to separate the discharge paths 9 and 1 from each other.
A discharge lamp device has also been proposed in which different luminescent layers 11 and 12 are applied to the discharge paths 9 and 10, and the color of the emitted light is changed by mutually adjusting the current flowing through the discharge paths 9 and 10. The manufacturing method of the lamp 1 is extremely complicated, and since the fluorescent lamp 1 has two pairs of electrodes, the lighting circuit also needs to be devised.

本発明は上述の欠点に鑑みてなされたもので、
その目的とする所は構成を複雑にすることなく光
色などの光の性質を変化させることができる放電
灯装置を提供するにある。
The present invention has been made in view of the above-mentioned drawbacks.
The purpose is to provide a discharge lamp device that can change light properties such as light color without complicating the structure.

以下図に示す実施例に基づき本発明を説明す
る。
The present invention will be explained below based on embodiments shown in the figures.

第5図は本発明の第一実施例であり、図におい
て、13は放電管で、該放電管13の管壁内周面
には該放電管13の光の性質を決定するための光
質決定体である3種類のけい光体層14a,14
b,14cが各々上記内周面を等分すべく分配被
着されており、上記けい光体層14bが被着され
た管壁部とは管軸をはさんで反対側の管壁部の外
方に磁界発生手段である棒状の磁石15が放電管
13の管長にわたつて配置されている。そしてけ
い光体層に対応する放電管13内の所定位置での
受磁量を変えるべく、磁石15は脱着自在になつ
ている。
FIG. 5 shows a first embodiment of the present invention. In the figure, 13 is a discharge tube, and the inner circumferential surface of the tube wall of the discharge tube 13 has a light quality mark for determining the light properties of the discharge tube 13. Three types of phosphor layers 14a, 14 as determinants
b and 14c are deposited on the tube wall portion on the opposite side of the tube axis across the tube axis from the tube wall portion on which the phosphor layer 14b is coated. A rod-shaped magnet 15 serving as a magnetic field generating means is disposed outwardly over the length of the discharge tube 13. The magnet 15 is detachable in order to change the amount of magnetism received at a predetermined position within the discharge tube 13 corresponding to the phosphor layer.

かかる構成の実施例においては、第6図に示す
ごとく、磁石15による磁界は上記放電管13の
管軸と交又する方向に加えられ、その磁界の強さ
Hは磁石15からの距離Lが大きくなるにつれて
指数関係的に減少し、管断面のうち比較的磁石1
5に近い領域16では磁界が大きく磁石15に遠
い領域17では磁界は小さい。従つて領域17に
比して領域16では電子の受けるローレンツカが
強く、領域16は電荷の通りにくい空間となり、
放電域18は領域17へ偏ることになる。これに
より、上記けい光体層14a,14cへの紫外線
の到達率は著しく小さくなる一方けい光体層14
bには多くの紫外線が入射し、第5図図示下方向
にけい光体層14bを主体とした光が強く照射さ
れる。次に、磁石15を放電管13から遠ざけて
管内各位置の受磁量をゼロにすると、放電域18
が放電管13の管内に一様に応がるため、上記け
い光体層14a,14b,14cは全て発光し、
図示下方ではけい光体層14bの色にけい光体1
4a,14cの色が幾分混じり合つたような色が
得られる。
In an embodiment with such a configuration, as shown in FIG. 6, a magnetic field by the magnet 15 is applied in a direction perpendicular to the tube axis of the discharge tube 13, and the strength H of the magnetic field is determined by the distance L from the magnet 15. As the size increases, it decreases exponentially, and relatively magnet 1 in the tube cross section
The magnetic field is large in the region 16 close to the magnet 15, and small in the region 17 far from the magnet 15. Therefore, compared to region 17, the Lorentz force that electrons receive is stronger in region 16, and region 16 becomes a space where it is difficult for charges to pass through.
The discharge area 18 will be biased towards the area 17. As a result, the rate of ultraviolet rays reaching the phosphor layers 14a and 14c is significantly reduced, while the phosphor layer 14
A large amount of ultraviolet rays enter b, and the phosphor layer 14b is strongly irradiated downward in FIG. Next, when the magnet 15 is moved away from the discharge tube 13 and the amount of magnetism received at each position in the tube is zero, the discharge area 18
is applied uniformly within the discharge tube 13, so the phosphor layers 14a, 14b, and 14c all emit light,
In the lower part of the figure, the color of the phosphor layer 14b corresponds to the color of the phosphor layer 14b.
A color that looks like a mixture of colors 4a and 14c is obtained.

かかる実施例の具体例として放電管13上方に
磁石15を設け、管壁内面の下側半分に色温度
3000〓程度以下のハロリン酸カルシウムで成るけ
い光体層を被着させ、上側半分に色温度6500〓程
度以上のハロリン酸カルシウムで成るけい光体層
を被着させ、磁石15に適当な磁界の強さの値を
選ぶと、上記放電管13下方では3500〜4000〓位
の温白状の光色が得られ、一方放電管13を管軸
中心に反転させれば5000〜6000〓位の昼光色状の
光色が得られさらに磁界を取り去ると4500〜5000
〓位の白色状光色を得ることができた。
As a specific example of such an embodiment, a magnet 15 is provided above the discharge tube 13, and the color temperature is
A phosphor layer made of calcium halophosphate with a color temperature of about 3000 or less is deposited, a phosphor layer made of calcium halophosphate with a color temperature of about 6500 or more is deposited on the upper half, and the magnetic field strength of the magnet 15 is set to an appropriate level. If the value of is selected, a warm white light color of about 3,500 to 4,000 degrees will be obtained below the discharge tube 13, while daylight color of about 5,000 to 6,000 degrees will be obtained if the discharge tube 13 is reversed around the tube axis. When the color is obtained and the magnetic field is removed, it becomes 4500 to 5000.
We were able to obtain a white-like light color.

第7図は本発明の第二実施例を示すもので、放
電管13の断面のみ周部上方の異なる位置に2個
の棒状の磁石15a,15bが設けられ、互いの
磁石15a,15c間の磁力線19が放電管13
内の放電路18を横切るべく異極同士が放電管1
3側に向いており、非放電灯側の他極はヨーク2
0により互いに連結されている。そして磁石15
a,15bはけい光体層に対応する管内各位置で
の磁界の強さを変えるべく脱着自在になつてい
る。
FIG. 7 shows a second embodiment of the present invention, in which two rod-shaped magnets 15a, 15b are provided at different positions above the circumference only in the cross section of the discharge tube 13, and the space between the magnets 15a, 15c is The magnetic field lines 19 are the discharge tube 13
Discharge tubes 1 with different polarities cross the discharge path 18 inside.
The other pole on the non-discharge lamp side is yoke 2.
They are connected to each other by 0. and magnet 15
a and 15b are detachable so as to change the strength of the magnetic field at each position within the tube corresponding to the phosphor layer.

かかる第二実施例においては磁力線19は放電
管13の管内の図示上方部分を主として通過する
ため、放電域18は管内下方の磁界の弱い部分に
偏り、管壁内面に被着されたけい光体層により第
一実施例と同様に発光色を変えることができるの
であるが、特に本実施例においては、磁界を加え
た際、放電域18と該放電域18以外の管内部と
の磁界の差が第一実施例における磁界の差より極
めて大きいので放電域18をより偏在させること
が可能となり色の変化がより明確になるという特
別の効果がある。
In the second embodiment, the magnetic lines of force 19 mainly pass through the upper part of the discharge tube 13 as shown in the figure, so the discharge area 18 is biased towards the lower part of the tube where the magnetic field is weaker, and the phosphor attached to the inner surface of the tube wall The color of the emitted light can be changed depending on the layer as in the first embodiment, but in this embodiment in particular, when a magnetic field is applied, the difference in magnetic field between the discharge region 18 and the inside of the tube other than the discharge region 18 is is much larger than the difference in magnetic field in the first embodiment, so there is a special effect that the discharge area 18 can be more unevenly distributed and the color change becomes more clear.

第8図は本発明の第三実施例を示すもので、磁
界が管軸方向に印加されるべく両管端部に各々脱
着自在の磁石15a,15bが設けられており互
いに異極同士が管長をはさんで対向し、そして他
面同士はヨーク20で連結されている。
FIG. 8 shows a third embodiment of the present invention, in which removable magnets 15a and 15b are provided at both ends of the tube so that a magnetic field is applied in the tube axis direction. The two faces face each other with a yoke 20 in between, and the other faces are connected to each other by a yoke 20.

かかる第三実施例においては複数のけい光体層
を有する放電管13管内の電界方向と管外の磁石
15a,15bによる磁界方向とが平行になるの
であるが、磁界の強い部分が放電域18となる。
これは管壁方向へ動こうとする電荷がローレンツ
カを受けて磁束を中心に円運動をするため、管壁
付近で正に帯電したイオンと再結合する確率が著
しく小さくなり、従つて磁界の弱い部分に比べて
放電が著しく行なわれやすいからであると考えら
れる。
In this third embodiment, the direction of the electric field inside the discharge tube 13 having a plurality of phosphor layers is parallel to the direction of the magnetic field generated by the magnets 15a and 15b outside the tube, but the portion where the magnetic field is strong is located in the discharge region 18. becomes.
This is because the charge trying to move toward the tube wall receives the Lorentz force and moves circularly around the magnetic flux, so the probability of recombination with positively charged ions near the tube wall becomes extremely small, and therefore the magnetic field decreases. This is thought to be because discharge is much easier to occur than in weaker parts.

なお、受磁量可変手段は磁石15の脱着手段で
ある必要はなく、磁石15を固定する一方放電管
13を管軸中心に回動自在にすることによりけい
光体層に対応する管内所定位置での受磁量を変化
させてもよいし、逆に、放電管13を固定する一
方磁石15を放電管13の管壁または管端部表面
などに沿つて移動するようにしてもよい。実際
に、第5図に示す第一実施例において、けい光体
層14bをタングステン酸マグネシウム等の青色
けい光体、けい光体層14cを硅酸亜鉛等の緑色
けい光体、けい光体層14aを砒酸マグネシウム
等の赤色けい光体で各々形成し、上方に固定され
た磁石15に対して放電灯13を管軸を中心に左
方向に徐々に回転させると、下方への照射光は青
系から緑系を経て赤系へと変化し略全部の色の緩
やかな変化を得ることができたし放電管13を固
定して磁石15を右方向に管壁に沿つて移動させ
ても、照射方向が変わつてはゆくが同様の色の変
化を得ることができた。また磁石15を磁界を強
弱変化させ得る磁界発生手段にして、けい光体層
に対応する放電管13内の所定位置での受磁量を
変化させても勿論差し支えない。
Note that the magnetic receiving amount variable means does not have to be a means for attaching and detaching the magnet 15, but by fixing the magnet 15 and making the discharge tube 13 rotatable around the tube axis, it can be fixed at a predetermined position in the tube corresponding to the phosphor layer. The amount of magnetism received at the discharge tube 13 may be changed, or conversely, the discharge tube 13 may be fixed while the magnet 15 may be moved along the wall or end surface of the discharge tube 13. Actually, in the first embodiment shown in FIG. 5, the phosphor layer 14b is a blue phosphor such as magnesium tungstate, the phosphor layer 14c is a green phosphor such as zinc silicate, and the phosphor layer 14c is a green phosphor such as zinc silicate. 14a are each made of a red phosphor such as magnesium arsenate, and when the discharge lamp 13 is gradually rotated to the left around the tube axis with respect to the magnet 15 fixed above, the downward irradiation light is blue. It was possible to obtain a gradual change in almost all the colors, from green to red, and even when the discharge tube 13 was fixed and the magnet 15 was moved to the right along the tube wall, Although the irradiation direction changed, the same color change could be obtained. Furthermore, it is of course possible to use the magnet 15 as a magnetic field generating means that can change the strength of the magnetic field to change the amount of magnetism received at a predetermined position in the discharge tube 13 corresponding to the phosphor layer.

また、本発明でいう光質決定体は前記したごと
く光の性質を決めるものであればどのようなもの
でもよく、管壁に密着させる必要もなく、たとえ
ば管壁の一部を単にガラスのみにし、他の部分に
けい光体層を被着させてけい光灯と殺菌灯の両方
に用いたりすることも可能であるし、光の性質の
うち特に色を変えたい場合でも、フイルタなどを
管壁外方に別途取り付けて色を変えたりしてもか
まわない。
Furthermore, the light quality determining body referred to in the present invention may be any substance as long as it determines the properties of light as described above, and it does not need to be in close contact with the tube wall; for example, a portion of the tube wall may be simply made of glass. It is also possible to coat other parts with a phosphor layer and use it as both a fluorescent lamp and a germicidal lamp, and even if you want to change the color of the light, you can use a filter etc. You can also attach it separately to the outside of the wall and change the color.

さらに磁界発生手段は永久磁石以外のものでも
よく、管壁内側などに設けても勿論かまわない。
Furthermore, the magnetic field generating means may be other than a permanent magnet, and may of course be provided inside the tube wall.

上述のように本発明は、磁界発生手段と、該磁
界発生手段による磁界を受け管壁の内面及び外面
の少なく共一方が複数種の光質決定体に覆われた
放電管と、光質決定体に対応する該放電管内の所
定位置での磁界の強さを変える受磁量可変手段と
より構成されているから、管内の放電路を磁界で
変えるだけで二種以上の性質の相異なる光を得る
ことができ、磁界による放電域の偏在効果により
発光効率が向上し、配光性能も向上し、さらには
受磁量可変手段により所望の光が容易に得られる
という著しい効果を有するものである。
As described above, the present invention provides a magnetic field generating means, a discharge tube in which at least one of the inner and outer surfaces of the tube wall receiving the magnetic field generated by the magnetic field generating means is covered with a plurality of types of light quality determining bodies; Since it is composed of a magnet receiving amount variable means that changes the strength of the magnetic field at a predetermined position in the discharge tube corresponding to the body, two or more different types of light with different properties can be generated by simply changing the discharge path in the tube with the magnetic field. It has the remarkable effect of improving the luminous efficiency and light distribution performance due to the uneven distribution effect of the discharge area due to the magnetic field, and furthermore, the desired light can be easily obtained by means of varying the amount of received magnetism. be.

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

第1図乃至第4図は従来の放電灯装置を示すも
ので、第1図は放電灯装置の外観図、第2図は同
じく断面図であり、第3図は異なる従来の放電灯
装置の一部切欠いた斜視図であり、第4図はその
断面図である。第5図乃至第8図は本発明の実施
例を示すもので、第5図イは第一実施例の断面模
式図、同図ロは側面模式図であり、第6図は磁界
の強さと磁石からの距離との関係を示す模式図及
びグラフであり、第7図は本発明の第二実施例を
示す装置の断面模式図であり、第8図は第三実施
例を示す装置の側面模式図である。 13…放電管、14a,14b,14c…けい
光体層、15,15a,15b…磁石、18…放
電域、19…磁力線、20…ヨーク。
Figures 1 to 4 show conventional discharge lamp devices. Figure 1 is an external view of the discharge lamp device, Figure 2 is a sectional view of the same, and Figure 3 is a diagram of a different conventional discharge lamp device. FIG. 4 is a partially cutaway perspective view, and FIG. 4 is a sectional view thereof. 5 to 8 show embodiments of the present invention. FIG. 5A is a schematic cross-sectional view of the first embodiment, FIG. 5B is a schematic side view, and FIG. FIG. 7 is a schematic cross-sectional view of the device showing the second embodiment of the present invention, and FIG. 8 is a side view of the device showing the third embodiment. It is a schematic diagram. 13... Discharge tube, 14a, 14b, 14c... Fluorescent layer, 15, 15a, 15b... Magnet, 18... Discharge area, 19... Line of magnetic force, 20... Yoke.

Claims (1)

【特許請求の範囲】[Claims] 1 磁界発生手段と、該磁界発生手段による磁界
を受け管壁の内面及び外面の少なく共一方が複数
種の光質決定体に覆われた放電管と、光質決定体
に対応する該放電管内の所定位置での磁界の強さ
を変える受磁量可変手段とより成る放電灯装置。
1. A magnetic field generating means, a discharge tube in which at least one of the inner and outer surfaces of the tube wall receiving the magnetic field generated by the magnetic field generating means is covered with a plurality of types of light quality determining bodies, and a portion within the discharge tube corresponding to the light quality determining body. A discharge lamp device comprising: magnetic receiving amount variable means for changing the strength of the magnetic field at a predetermined position.
JP8939480A 1980-06-30 1980-06-30 Discharge lamp unit Granted JPS5713686A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8939480A JPS5713686A (en) 1980-06-30 1980-06-30 Discharge lamp unit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8939480A JPS5713686A (en) 1980-06-30 1980-06-30 Discharge lamp unit

Publications (2)

Publication Number Publication Date
JPS5713686A JPS5713686A (en) 1982-01-23
JPS6241364B2 true JPS6241364B2 (en) 1987-09-02

Family

ID=13969427

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8939480A Granted JPS5713686A (en) 1980-06-30 1980-06-30 Discharge lamp unit

Country Status (1)

Country Link
JP (1) JPS5713686A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0161863U (en) * 1987-10-13 1989-04-20
JPH0161865U (en) * 1987-10-13 1989-04-20

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH047228Y2 (en) * 1986-01-30 1992-02-26
JPH0521532Y2 (en) * 1986-01-31 1993-06-02

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0161863U (en) * 1987-10-13 1989-04-20
JPH0161865U (en) * 1987-10-13 1989-04-20

Also Published As

Publication number Publication date
JPS5713686A (en) 1982-01-23

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