JPS59141158A - Plate-type discharge lamp device - Google Patents
Plate-type discharge lamp deviceInfo
- Publication number
- JPS59141158A JPS59141158A JP1473983A JP1473983A JPS59141158A JP S59141158 A JPS59141158 A JP S59141158A JP 1473983 A JP1473983 A JP 1473983A JP 1473983 A JP1473983 A JP 1473983A JP S59141158 A JPS59141158 A JP S59141158A
- Authority
- JP
- Japan
- Prior art keywords
- discharge lamp
- magnetic field
- plate
- electrodes
- plate surface
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/70—Lamps with low-pressure unconstricted discharge having a cold pressure < 400 Torr
- H01J61/72—Lamps with low-pressure unconstricted discharge having a cold pressure < 400 Torr having a main light-emitting filling of easily vaporisable metal vapour, e.g. mercury
Abstract
Description
【発明の詳細な説明】 (技術分野) 本発明は、管断面が扁平な平板形放電灯装置に関する。[Detailed description of the invention] (Technical field) The present invention relates to a flat discharge lamp device having a flat tube cross section.
(背景技術)
従来2.管断面が扁平な、いわゆる平板形ランプと称す
るものが提案されており、一部商品化もされている。こ
のタイプのランプは面全体が発光するので、面光源とし
て新しい照明の分野を築くものであると考えられている
。しかし、ランプの形状だけをただ平板状にしただけで
は均一な輝度は得られない。つまり、第1図fat、
(b)に示すようGこ点灯した状態で、管Aの中央部の
輝度が高く、周辺に行く程暗くなる、輝度むらが生じる
という欠点がある。これは放電が両電極B、B間の最短
距離で生じる(放電エネルギーが最小になるような経路
を通る)ためである。なお、図中斜線領域Cは放電域を
示す。(Background technology) Conventional 2. So-called flat lamps with a flat tube cross section have been proposed, and some have even been commercialized. Since this type of lamp emits light from its entire surface, it is thought to create a new field of lighting as a surface light source. However, uniform brightness cannot be obtained by simply changing the shape of the lamp into a flat plate. In other words, in Figure 1 fat,
As shown in (b), when the tube A is turned on, the brightness is high in the center of the tube A and becomes darker toward the periphery, which is a drawback in that uneven brightness occurs. This is because the discharge occurs at the shortest distance between the two electrodes B (traversing the path that minimizes the discharge energy). Note that the shaded area C in the figure indicates the discharge area.
また、上記欠点を改良したものとして第2図(al、(
b)に示すように、ランプ管A内に複数個の仕切板りを
設け、放電域Cを蛇行させて輝度を均一にしたものも提
案されているが、ランプ構造が非雷に複雑になり、製造
が困難で重量も重くなるといった欠点を有する。In addition, as an improved version of the above-mentioned drawback, Fig. 2 (al, (
As shown in b), it has been proposed that multiple partition plates are provided inside the lamp tube A to make the discharge area C meander to make the brightness uniform, but this makes the lamp structure unnecessarily complicated. However, it has the drawbacks of being difficult to manufacture and heavy.
(発明の目的)
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、簡単な構成で、放電灯の平板面全体の輝度
が実質的に均一になる平板形放電灯装置を提供するにあ
る。(Object of the Invention) The present invention has been made in view of the above-mentioned drawbacks, and an object of the present invention is to provide a flat discharge lamp device that has a simple configuration and has substantially uniform brightness over the entire flat surface of the discharge lamp. It is on offer.
(発明の開示)
本発明は、管断面が扁平で管中央に一対の電極を具備し
た平板形放電灯の平板面に略直交する回較値界を印加す
ることにより、平板面全体の輝度が実質的に均一になる
ようにしたものである。 。(Disclosure of the Invention) The present invention applies a calibrated value field substantially perpendicular to the flat plate surface of a flat discharge lamp having a flat tube cross section and a pair of electrodes at the center of the tube, thereby increasing the brightness of the entire flat plate surface. It is made to be substantially uniform. .
以下、本発明を実施例に基づき説明する。The present invention will be explained below based on examples.
実施例1
第3図(al、 (blは本発明の第1の実施例を示し
、図中1は環状の回転磁界発生装置、2は平板−面が円
形の平板形放電灯で、管内面には螢光体が塗布されてお
り、管内には数Torrの不活性ガスと適量の水銀が封
入されている。3a、3bは電極物質が塗布された電極
で、熱陰極でもよい。4は電極3a、3bと外部回路と
を電気的に接続する接続線である。Embodiment 1 Figure 3 (al, (bl) shows the first embodiment of the present invention, in which 1 is an annular rotating magnetic field generator, 2 is a flat plate discharge lamp with a circular flat plate surface, and the inner surface of the tube is is coated with a phosphor, and the tube is filled with several Torr of inert gas and an appropriate amount of mercury.3a and 3b are electrodes coated with an electrode material, and may be hot cathodes.4 is This is a connection line that electrically connects the electrodes 3a, 3b and an external circuit.
実施例2
第4図(a) 、 (b)は本発明の第2の実施例を示
し、実施例1の電極部分を改良したものであり、管中心
に凹部5を設け、該凹部5に接続線4を配設したもので
ある。なお、一方の電極3bはリング状に形成されてい
る。Embodiment 2 FIGS. 4(a) and 4(b) show a second embodiment of the present invention, in which the electrode part of Embodiment 1 is improved, and a recess 5 is provided in the center of the tube, and the recess 5 is A connection line 4 is provided. Note that one electrode 3b is formed in a ring shape.
実施例3
第5図(al、 (blは本発明の第3の実施例を示し
、管内中心部に上端開口の筒部6を形成し、該筒部6内
に一方の電極3aを配設し、他方の電極3bを筒部6の
外周にリング状に配設したものである。Embodiment 3 FIGS. 5(al) and (bl) show a third embodiment of the present invention, in which a cylindrical portion 6 with an open top end is formed in the center of the tube, and one electrode 3a is disposed within the cylindrical portion 6. However, the other electrode 3b is arranged in a ring shape around the outer periphery of the cylindrical portion 6.
次に、かかる構成における回転磁界発生装置1の動作を
説明する。本発明に用いた回転磁界発生装置1は誘導電
動機の固定子と同様の構造であり、3相交流の場合につ
いて説明する。Next, the operation of the rotating magnetic field generating device 1 with such a configuration will be explained. The rotating magnetic field generating device 1 used in the present invention has a structure similar to the stator of an induction motor, and the case of three-phase alternating current will be described.
第6図に示すような3相交流電流1a、Ib。Three-phase alternating currents 1a, Ib as shown in FIG.
rcが、第7図(al 〜(C1に示すような巻線Ma
、Mb、Mcにそれぞれ流れるものとすると、第6図に
示す位相r、n、mにおける瞬時電流によってできる磁
界は、それぞれ第7図tag、 fbl、 (C)のよ
うになる。而して、第6図から明らかなように位相■か
ら位相■及び位相■から位相■までの位相角はそれぞれ
30°で、3相交流電流1a、Ib。rc is a winding Ma as shown in FIG.
, Mb, and Mc, the magnetic fields generated by the instantaneous currents in phases r, n, and m shown in FIG. 6 are as shown in FIG. 7, tag, fbl, and (C), respectively. As is clear from FIG. 6, the phase angles from phase (1) to phase (2) and from phase (2) to phase (2) are each 30°, and the three-phase alternating currents 1a, Ib.
Icによってできる磁界の方向も30°ずつ回転してい
る。すなわち、電流の位相がGO”移る間に磁界も60
°回転しており、このようにして回転磁界が得られる。The direction of the magnetic field created by Ic is also rotated by 30°. In other words, while the phase of the current shifts to GO'', the magnetic field also changes by 60
°, and thus a rotating magnetic field is obtained.
3相交流での回転磁界を得る場合について述べたが、単
相交流で回転磁界を(Mる場合には、回転磁界発生装置
1のコイルの巻き方を、くまとりコイル型にするか、コ
ンデンサを用いたコンデンサ分相型にすれば、単相交流
でも回転磁界が得られる。We have described the case of obtaining a rotating magnetic field using three-phase alternating current, but if you want to generate a rotating magnetic field using single-phase alternating current, the coil of the rotating magnetic field generator 1 should be wound in a round coil type, or by using a capacitor. If you use a split-phase type capacitor using , you can obtain a rotating magnetic field even with single-phase AC.
次に、第8図に基づいて回転磁界と放電との関係を述べ
る。第8図(alは平面図で、同図(blは断面図であ
り、磁界が同図(a)において矢印線Hで示す方向で、
同図fblにおいて紙面の表から裏に向かう方向に印加
され、同図(blにおいて下方の電極3bに正の、上方
の電極3aに負の電圧が印加され放電を行なっている。Next, the relationship between the rotating magnetic field and discharge will be described based on FIG. Fig. 8 (al is a plan view, bl is a cross-sectional view, and the magnetic field is in the direction indicated by the arrow line H in Fig. 8 (a),
In the figure fbl, a voltage is applied in the direction from the front to the back of the paper, and in the figure (bl), a positive voltage is applied to the lower electrode 3b and a negative voltage is applied to the upper electrode 3a, causing discharge.
このような状態では、プラズマ中の電子はローレンツ力
を受け、プラズマPは同図fblに示ずように蛇行する
。このプラズマPの蛇行を上から見ると同図(alのよ
うになる。従って、上述のように磁界が回転するとプラ
ズマPも回転し、放電灯2の平板面全体が発光したよう
になる。なお、第9図は放電灯2と外部回路の接続状態
を示す一例で、図中7は点灯回路、8は回転磁界発生装
置1に接続された回転磁界発生回路、9は電源である。In such a state, electrons in the plasma are subjected to Lorentz force, and the plasma P meanderes as shown in fbl in the figure. The meandering of the plasma P is viewed from above as shown in the same figure (al). Therefore, when the magnetic field rotates as described above, the plasma P also rotates, and the entire flat surface of the discharge lamp 2 appears to be emitting light. , FIG. 9 shows an example of a connection state between the discharge lamp 2 and an external circuit. In the figure, 7 is a lighting circuit, 8 is a rotating magnetic field generating circuit connected to the rotating magnetic field generating device 1, and 9 is a power source.
なお、上記ローレンツ力を変化させることにより、第1
0図(al、 (blに示すようにプラズマPの偏向の
程度を、図においてPlからP2に変化させることが可
能となり、従って、放電域の面積を変えることができる
ので放電灯2の調光が可能となる。すなわち、ローレン
ツ力Fは、F=qVB (qは電荷、■は電荷の速度、
Bは磁束密度)であり、放電電流を変化させるとqvが
変化し、回転磁界発生装置1の巻線に流れる電流を変化
させると磁束密度Bが変化する。従って、回転磁界発生
回路8により放電電流または巻線に流れる電流を変化さ
せることにより、容易にローレンツ力を変化させること
ができる。In addition, by changing the above Lorentz force, the first
As shown in Figure 0 (al, (bl), it is possible to change the degree of deflection of the plasma P from Pl to P2 in the figure, and therefore the area of the discharge region can be changed, so the dimming of the discharge lamp 2 can be adjusted. In other words, the Lorentz force F is F=qVB (q is the charge, ■ is the speed of the charge,
B is the magnetic flux density), and when the discharge current is changed, qv is changed, and when the current flowing through the winding of the rotating magnetic field generator 1 is changed, the magnetic flux density B is changed. Therefore, by changing the discharge current or the current flowing through the windings using the rotating magnetic field generating circuit 8, the Lorentz force can be easily changed.
(発明の効果)
本発明は上記のように、管断面が扁平で管中央に一対の
電極を具備した平板形放電灯に、該放電灯の平板面に略
直交する回転磁界を印加することにより、平板面全体の
輝度が実質的に均一になる平板形放電灯装置を簡単な構
成で提供できた。(Effects of the Invention) As described above, the present invention provides a flat discharge lamp having a flat tube cross section and a pair of electrodes at the center of the tube by applying a rotating magnetic field substantially orthogonal to the flat surface of the discharge lamp. , it was possible to provide a flat discharge lamp device with a simple configuration in which the luminance of the entire flat plate surface is substantially uniform.
第1図及び第2図はそれぞれ従来例を示し、第1図(a
lは平面図、第1図(blは断面図、第2図ta+は平
面図、第2図[blは断面図である。第3図乃至第5図
はそれぞれ本発明に係る実施例を示し、各図において(
a)は示面図、(b)は断面図である。第6図は3相交
流を示す図、第7図+aL (bl、 (C1はそれぞ
れ磁界発生装置の動作を説明する図、第8図は磁界の方
向と放電の関係を示す図で、ta)は平面図、(b目よ
断面図である。第9図は放電灯と外部回路の接続状態の
一例を示すブロック図、第10図はローレンツ力を変化
させ場合の説明図で、ra)は平面図、(blは断面図
である。
1・・・回転磁界発生装置、2・・・平板形放電灯、3
a、3b・・・電極、4・・・接続線。
特許出願人
松下電工株式会社
代理人 弁理士 竹元敏丸
(ばか2名)Fig. 1 and Fig. 2 respectively show conventional examples, and Fig. 1 (a
1 is a plan view, FIG. 1 is a sectional view, FIG. , in each figure (
(a) is a diagram, and (b) is a cross-sectional view. Figure 6 is a diagram showing three-phase AC, Figure 7 +aL (bl, (C1 is a diagram explaining the operation of the magnetic field generator, respectively, and Figure 8 is a diagram showing the relationship between the direction of the magnetic field and discharge, ta) (b) is a plan view, (b) is a cross-sectional view. Fig. 9 is a block diagram showing an example of the connection state between the discharge lamp and the external circuit, Fig. 10 is an explanatory diagram when changing the Lorentz force, and ra) is a cross-sectional view. Plan view, (bl is a sectional view. 1... Rotating magnetic field generator, 2... Flat discharge lamp, 3
a, 3b...electrode, 4...connection line. Patent applicant Matsushita Electric Works Co., Ltd. Agent Patent attorney Toshimaru Takemoto (Two idiots)
Claims (1)
板形放電灯と、該放電灯の平板面に略直交し且つ回転す
る磁界印加手段とより成る平板形放電灯装置。(1) A flat discharge lamp device comprising a flat discharge lamp having a flat tube cross section and a pair of electrodes at the center of the tube, and a rotating magnetic field application means that is substantially orthogonal to the flat surface of the discharge lamp.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1473983A JPS59141158A (en) | 1983-01-31 | 1983-01-31 | Plate-type discharge lamp device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1473983A JPS59141158A (en) | 1983-01-31 | 1983-01-31 | Plate-type discharge lamp device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59141158A true JPS59141158A (en) | 1984-08-13 |
JPH0117229B2 JPH0117229B2 (en) | 1989-03-29 |
Family
ID=11869484
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1473983A Granted JPS59141158A (en) | 1983-01-31 | 1983-01-31 | Plate-type discharge lamp device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59141158A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61269848A (en) * | 1985-05-25 | 1986-11-29 | Matsushita Electric Works Ltd | Plane type low pressure discharge lamp |
WO2007079650A1 (en) * | 2006-01-13 | 2007-07-19 | Cheng-Rui Xiong | A method for controlling and dissipating harmful plasma in industrial production by motive magnetic field and a motive magnetic field generating device |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2581819Y2 (en) * | 1996-04-25 | 1998-09-24 | 日本シグマックス株式会社 | Knee support |
-
1983
- 1983-01-31 JP JP1473983A patent/JPS59141158A/en active Granted
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61269848A (en) * | 1985-05-25 | 1986-11-29 | Matsushita Electric Works Ltd | Plane type low pressure discharge lamp |
WO2007079650A1 (en) * | 2006-01-13 | 2007-07-19 | Cheng-Rui Xiong | A method for controlling and dissipating harmful plasma in industrial production by motive magnetic field and a motive magnetic field generating device |
Also Published As
Publication number | Publication date |
---|---|
JPH0117229B2 (en) | 1989-03-29 |
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