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JPS6241362B2 - - Google Patents
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JPS6241362B2 - - Google Patents

Info

Publication number
JPS6241362B2
JPS6241362B2 JP8939280A JP8939280A JPS6241362B2 JP S6241362 B2 JPS6241362 B2 JP S6241362B2 JP 8939280 A JP8939280 A JP 8939280A JP 8939280 A JP8939280 A JP 8939280A JP S6241362 B2 JPS6241362 B2 JP S6241362B2
Authority
JP
Japan
Prior art keywords
magnetic field
tube
discharge lamp
fluorescent lamp
generating means
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
JP8939280A
Other languages
Japanese (ja)
Other versions
JPS5713684A (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 JP8939280A priority Critical patent/JPS5713684A/en
Publication of JPS5713684A publication Critical patent/JPS5713684A/en
Publication of JPS6241362B2 publication Critical patent/JPS6241362B2/ja
Granted legal-status Critical Current

Links

Landscapes

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

Description

【発明の詳細な説明】 本発明は所望の配光特性を得ることができる放
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 desired light distribution characteristics.

従来所望の配光特性を得ることができる放電灯
装置としては、第1図に示す反射型けい光灯があ
りけい光灯aの管壁内周面積の約2/3に反射膜b
を被着させ、さらに該反射膜bの内面と反射膜b
の被着していない管壁内周面部分とにけい光体層
Cを被着させていた。
Conventionally, as a discharge lamp device capable of obtaining desired light distribution characteristics, there is a reflective fluorescent lamp shown in Fig. 1, in which a reflective film b is applied to about two-thirds of the inner peripheral area of the tube wall of the fluorescent lamp a.
The inner surface of the reflective film b and the reflective film b
The phosphor layer C was coated on the inner circumferential surface portion of the tube wall which was not coated.

かかる反射型けい光灯においては、反射膜bで
光を多重反射させた後、反射膜bの被着していな
い部分からけい光灯a外方へ光を放出させること
により、所望の方向(図では下方)へ通常の2倍
近い光度を与えていたのであるが、管内で光が多
重反射するために管壁または反射膜b及びけい光
体層cで幾分光が吸収され、反射膜bを有しない
一般のけい光灯に比べて発光効率が15〜20%悪く
なるという欠点があつた。また、反射膜bの被着
位置や被着面積により配光特性を決定するので、
いつたんけい光灯を製造して器具に取り付ける
と、ランプを回転させない限り配光特性を変える
ことが不可能であつた。
In such a reflective fluorescent lamp, after the light is multiple-reflected by the reflective film b, the light is emitted outward from the fluorescent lamp a from the part where the reflective film b is not covered, so that the light can be reflected in a desired direction ( In the figure, the luminous intensity was almost twice as much as normal (downward in the figure), but due to multiple reflections of light within the tube, some of the light was absorbed by the tube wall or the reflective film B and the phosphor layer C, and the reflective film The drawback was that the luminous efficiency was 15 to 20% lower than that of general fluorescent lamps that did not have B. In addition, since the light distribution characteristics are determined by the deposition position and deposition area of the reflective film b,
Once a fluorescent lamp was manufactured and attached to a fixture, it was impossible to change the light distribution characteristics without rotating the lamp.

本発明は上述の欠点に鑑みてなされたもので、
その目的とするところは、発光効率が一般の放電
灯よりも良く、所望の配光特性を得ることがで
き、しかも容易に配光特性を変えることのできる
放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 lighting device that has better luminous efficiency than a general discharge lamp, can obtain desired light distribution characteristics, and can easily change the light distribution characteristics.

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2図は本発明の一実施例であつて、図におい
て、1は放電灯であるけい光灯で、該けい光灯1
の管端の口金2、2の外方には、けい光灯1の電
界と平行方向でかつ管内に不均一に分布する磁界
を発生する磁界発生手段である磁石のN極3a及
びS極3bが各々取着されていて、該N極3a及
びS極3bはけい光灯1内の所定位置での受磁量
を変えるべく、脱着可能となつている。なお、図
中4は磁力線を示す。
FIG. 2 shows one embodiment of the present invention, and in the figure, 1 is a fluorescent lamp which is a discharge lamp;
Outside the caps 2, 2 at the ends of the tube are N poles 3a and S poles 3b of magnets, which are magnetic field generating means for generating a magnetic field parallel to the electric field of the fluorescent lamp 1 and distributed unevenly within the tube. The north pole 3a and the south pole 3b are removable in order to change the amount of magnetism received at a predetermined position within the fluorescent lamp 1. Note that 4 in the figure indicates lines of magnetic force.

かかる実施例においては、電界と同方向に磁界
が加えられるため、管壁へ向かつて動こうとする
荷電粒子は磁界により管軸中心に円運動をし、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、その結果磁界の殆どない図示
下方の部分に対し磁界のある部分での電子の通過
しにくさの度合(以下放電インピーダンスと称す
る)が極めて小さくなり、従つて磁界の存在する
部分でのみ放電が行なわれ、殆ど管壁の図示上方
部分のみが発光する。一方、N極3a及びS極3
bを各々取り外すと、管内には磁界の影響がなく
なり、管壁全体が発光する。
In this embodiment, since a magnetic field is applied in the same direction as the electric field, charged particles that are about to move toward the tube wall are caused to move circularly around the tube axis due to the magnetic field, and are separated from positively charged ions near the tube wall. The probability of recombination becomes extremely small, and as a result, the degree of difficulty for electrons to pass through the area where there is a magnetic field (hereinafter referred to as discharge impedance) becomes extremely small compared to the lower part of the figure where there is almost no magnetic field, and therefore the magnetic field The discharge occurs only in the portion where the tube wall exists, and almost only the upper portion of the tube wall in the figure emits light. On the other hand, N pole 3a and S pole 3
When each of b is removed, the influence of the magnetic field disappears inside the tube, and the entire tube wall emits light.

なお、受磁量可変手段は磁石の脱着手段である
必要はなく、放電灯に加えられる磁界の状態を変
化させるものであればどのようなものであつても
よく、例えばけい光灯1を固定して磁石をけい光
灯1の管端外面に沿つて移動させることにより、
管内所定位置での受磁量を変化させてもよいし、
強弱可変の磁界発生手段とすることにより磁界発
生手段が受磁量可変手段を兼ねてもよい。また磁
界発生手段は、放電灯の管内に設けても勿論かま
わない。
Note that the magnetic receiving amount variable means does not have to be a means for attaching and detaching a magnet, and may be any means as long as it changes the state of the magnetic field applied to the discharge lamp. For example, when the fluorescent lamp 1 is fixed By moving the magnet along the outer surface of the tube end of the fluorescent lamp 1,
The amount of magnetism received at a predetermined position within the pipe may be changed,
By using a magnetic field generating means whose intensity is variable, the magnetic field generating means may also serve as a receiving amount variable means. Furthermore, the magnetic field generating means may of course be provided within the tube of the discharge lamp.

上述のように本発明は、磁界発生手段と、該磁
界発生手段により管内に不均一な磁界を電界と平
行方向に受ける放電灯と、該放電灯内の所定位置
での磁界の強さを変える受磁量可変手段とで構成
されているから、電界と交わる方向に磁界を加え
るものに比べて明確に放電灯の管内の放電経路を
変えることができ、従つて配光特性も容易に設定
できるだけでなく、放電路が偏る上に従来反射に
より生じていた紫外線等の損失も少なく、発光効
率が著しく大きくなるという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 lamp which receives a non-uniform magnetic field within the tube in a direction parallel to the electric field by the magnetic field generating means, and a method of changing the strength of the magnetic field at a predetermined position within the discharge lamp. Since it is composed of a magnetic field variable means, it is possible to change the discharge path within the discharge lamp tube more clearly than when applying a magnetic field in a direction that intersects with the electric field, and the light distribution characteristics can also be easily set. Instead, the discharge path is biased, and the loss of ultraviolet rays, etc., which conventionally occurs due to reflection, is reduced, and the luminous efficiency is significantly increased.

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

第1図は従来の反射型けい光灯を示す断面図で
ある。第2図は本発明の実施例を示す一部省略し
た斜視図である。 a…けい光灯、b…反射膜、c…けい光体層、
1…けい光灯、2…口金、3a…N極、3b…S
極、4…磁力線。
FIG. 1 is a sectional view showing a conventional reflective fluorescent lamp. FIG. 2 is a partially omitted perspective view showing an embodiment of the present invention. a... Fluorescent lamp, b... Reflective film, c... Fluorescent layer,
1...Fluorescent lamp, 2...Base, 3a...N pole, 3b...S
Pole, 4... lines of magnetic force.

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り管内
に不均一な磁界を電界と平行方向に受ける放電灯
と、該放電灯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 lamp which receives a non-uniform magnetic field within the tube in a direction parallel to the electric field by the magnetic field generating means, and a receiving amount variable means for changing the strength of the magnetic field at a predetermined position within the discharge lamp. A discharge lamp device consisting of
JP8939280A 1980-06-30 1980-06-30 Discharge lamp unit Granted JPS5713684A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8939280A JPS5713684A (en) 1980-06-30 1980-06-30 Discharge lamp unit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8939280A JPS5713684A (en) 1980-06-30 1980-06-30 Discharge lamp unit

Publications (2)

Publication Number Publication Date
JPS5713684A JPS5713684A (en) 1982-01-23
JPS6241362B2 true JPS6241362B2 (en) 1987-09-02

Family

ID=13969376

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8939280A Granted JPS5713684A (en) 1980-06-30 1980-06-30 Discharge lamp unit

Country Status (1)

Country Link
JP (1) JPS5713684A (en)

Also Published As

Publication number Publication date
JPS5713684A (en) 1982-01-23

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