JPH022267B2 - - Google Patents
Info
- Publication number
- JPH022267B2 JPH022267B2 JP22809283A JP22809283A JPH022267B2 JP H022267 B2 JPH022267 B2 JP H022267B2 JP 22809283 A JP22809283 A JP 22809283A JP 22809283 A JP22809283 A JP 22809283A JP H022267 B2 JPH022267 B2 JP H022267B2
- Authority
- JP
- Japan
- Prior art keywords
- magnet
- discharge path
- tube
- yoke
- discharge 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.)
- Expired
Links
- 239000011521 glass Substances 0.000 claims description 9
- 230000001105 regulatory effect Effects 0.000 claims description 9
- 239000000696 magnetic material Substances 0.000 claims description 2
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 7
- 230000004907 flux Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 3
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 239000011248 coating agent Substances 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- 239000003086 colorant Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 1
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 1
- 229910052753 mercury Inorganic materials 0.000 description 1
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
Landscapes
- Discharge Lamps And Accessories Thereof (AREA)
- Vessels And Coating Films For Discharge Lamps (AREA)
Description
【発明の詳細な説明】
(技術分野)
本発明は、螢光ランプの如き低圧放電灯を用い
た低圧放電灯装置に関する。DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to a low pressure discharge lamp device using a low pressure discharge lamp such as a fluorescent lamp.
(背景技術)
一般に、螢光ランプでは管内中央部を通る放電
路から発生した紫外線が、管内壁に塗布された蛍
光体によつて、その蛍光体特有色の可視光に変換
されて発光する。このようなランプの従来例を第
1図に示す。図中、1はガラス管、2は蛍光体被
膜、3は所定量の水銀及び希ガスが封入された気
密空間、4はエミツタが充填されたフイラメン
ト、5はリード線、6はガラスステム、7は口金
である。このようなランプにおいては、通常の点
灯状態では放電路の位置は略一定であり、発光色
も唯一種類に限定される。(Background Art) Generally, in a fluorescent lamp, ultraviolet light generated from a discharge path passing through the center of the tube is converted by a phosphor coated on the inner wall of the tube into visible light having a characteristic color of the phosphor, and then emitted. A conventional example of such a lamp is shown in FIG. In the figure, 1 is a glass tube, 2 is a phosphor coating, 3 is an airtight space filled with a predetermined amount of mercury and a rare gas, 4 is a filament filled with an emitter, 5 is a lead wire, 6 is a glass stem, and 7 is the base. In such a lamp, the position of the discharge path is substantially constant under normal lighting conditions, and the emitted light color is limited to only one type.
また、上述の如き一般の螢光ランプとは異な
り、1本のランプによつて配光特性あるいは発光
色を変化させることが可能な螢光ランプも種々提
案されている。 Furthermore, unlike the above-mentioned general fluorescent lamps, various fluorescent lamps have been proposed in which the light distribution characteristics or emission color can be changed with a single lamp.
第2図はかかる螢光ランプの一例を示すもので
あり、上述の如き一般の螢光ランプと異なる点
は、円柱状の放電路規制体8が管内に配設され、
管外に磁石9が配設されると共に、ガラス管1の
内面に塗布される蛍光体2が、異なる発光色の複
数の蛍光体2a,2bで塗り分けられていること
で、他の構成は第1図に示す構成と同様であるの
で、同等構成に同一符号を付すことにより説明を
省略する。 FIG. 2 shows an example of such a fluorescent lamp, which differs from the general fluorescent lamp described above in that a cylindrical discharge path regulating body 8 is disposed inside the tube.
A magnet 9 is disposed outside the tube, and the phosphor 2 coated on the inner surface of the glass tube 1 is coated with a plurality of phosphors 2a and 2b of different luminescent colors, so that the other configurations are different from each other. Since the configuration is similar to that shown in FIG. 1, the explanation will be omitted by assigning the same reference numerals to the equivalent configurations.
次に、上記螢光ランプの動作原理を第3図を参
照して説明する。磁石9によつて同図aに示す如
く管軸方向に垂直な磁界を印加すると、管断面方
向で点a−b間の磁束密度Bの分布は、同図bに
示すようになり、磁石9から遠ざかるに従つて減
少する(例えば、磁界始端のa点で200ガウス、
点bの部分で30ガウス程度になる)。 Next, the principle of operation of the above fluorescent lamp will be explained with reference to FIG. When a magnetic field perpendicular to the tube axis direction is applied using the magnet 9 as shown in FIG. (For example, 200 Gauss at point a at the beginning of the magnetic field,
It will be about 30 Gauss at point b).
ところで、上記ガラス管1と放電路規制体8と
が完全な同心円になるように配置されておれば、
放電路はこの両者間の円筒状気密空間のどの部分
も同じ確率で存在し得る。しかし、前述のような
磁界を印加すると、上下での磁束密度Bの差によ
つて、比較的磁束密度Bの大きな上部a点付近で
は、放電インピーダンスが等価的に大きく、逆
に、比較的磁束密度Bの小さな下部b点付近で
は、放電インピーダンスも小となり、結果として
放電路Hはb点付近に押しやられる。このとき、
放電路H側の蛍光体被膜2bが発光する。逆に、
磁石9をb点側に移せば蛍光体2aによる発光が
得られる。 By the way, if the glass tube 1 and the discharge path regulating body 8 are arranged in perfect concentric circles,
A discharge path can exist in any part of the cylindrical airtight space between the two with the same probability. However, when the above-mentioned magnetic field is applied, due to the difference in the magnetic flux density B between the upper and lower parts, the discharge impedance is equivalently large near the upper point a where the magnetic flux density B is relatively large; Near the lower point b where the density B is small, the discharge impedance also becomes small, and as a result, the discharge path H is pushed to the vicinity of the point b. At this time,
The phosphor coating 2b on the side of the discharge path H emits light. vice versa,
If the magnet 9 is moved to the point b side, light emission by the phosphor 2a can be obtained.
しかしながら、上記従来例においては、第3図
bに示す磁束密度分布からも明らかなように、上
下での磁束密度Bの差は大きくないため、放電路
規制体8の配設位置の偏りによつて、放電路Hが
所望位置に形成されない場合があつた。 However, in the above conventional example, as is clear from the magnetic flux density distribution shown in FIG. Therefore, there were cases where the discharge path H was not formed at the desired position.
(発明の目的)
本発明は上記の点に鑑みなされたもので、その
目的とするところは、磁界作用による放電路の形
成が所望位置に、より確実にできる低圧放電灯装
置を提供するにある。(Object of the Invention) The present invention has been made in view of the above points, and its object is to provide a low-pressure discharge lamp device that can more reliably form a discharge path at a desired position by the action of a magnetic field. .
(発明の開示)
本発明の構成及び動作原理を第4図に示す。本
発明は、前記第2図及び第3図に示す従来例の構
成において、磁石9のガラス管1との非接触側極
(第4図においてはS極側)に連結された、磁性
体(例えば電磁純鉄)から成るヨーク10の他端
側、すなわち磁石9との非連結側を、少なくとも
一端が閉塞された円筒状の放電路規制体8の内部
に、磁石9と対向するようにガラス管1の軸方向
に沿つて配設したことを特徴とする。なお、第4
図では磁石9のヨーク10との連結側がS極とな
つている場合を図示しているので、ヨーク10も
当然S極となる。また、第4図ではヨーク10の
うち、磁石9との連結部と放電路規制体8との中
間部分の図示は省略している。(Disclosure of the Invention) The configuration and operating principle of the present invention are shown in FIG. In the conventional configuration shown in FIGS. 2 and 3, the present invention provides a magnetic material ( The other end side of the yoke 10 (for example, electromagnetic pure iron), that is, the side not connected to the magnet 9, is placed inside a cylindrical discharge path regulating body 8 with at least one end closed, and a glass plate is placed so as to face the magnet 9. It is characterized by being arranged along the axial direction of the tube 1. In addition, the fourth
The figure shows a case where the side of the magnet 9 connected to the yoke 10 is the south pole, so the yoke 10 is naturally also the south pole. In addition, in FIG. 4, an intermediate portion of the yoke 10 between the connecting portion with the magnet 9 and the discharge path regulating body 8 is omitted.
このように構成することにより、ヨーク10の
うち放電路規制体8に沿い、かつ磁石9に対向し
た部分が、磁界の始端あるいは終端となつて、磁
石9との間に磁界を形成する。すなわち、磁力線
は殆ど他に漏れることなく、磁石9とヨーク10
との間に終始する。 With this configuration, the portion of the yoke 10 along the discharge path regulating body 8 and facing the magnet 9 becomes the starting end or the ending end of the magnetic field, and forms a magnetic field between the yoke 10 and the magnet 9. In other words, the lines of magnetic force hardly leak anywhere else, and the magnetic lines are connected to the magnet 9 and the yoke 10.
It ends between.
従つて、かかる場合のガラス管1の断面上下方
向点a−b間での磁束密度Bの分布は、第4図b
に示すようになり、前述の第3図bに示す特性曲
線と比べると、a点付近とb点付近との磁束密度
Bの差はより顕著となり、放電路Hはより確実に
偏向されることになる。 Therefore, in this case, the distribution of magnetic flux density B between points a and b in the vertical direction of the cross section of the glass tube 1 is as shown in FIG.
Compared to the characteristic curve shown in Figure 3b above, the difference in magnetic flux density B near point a and point b becomes more significant, and the discharge path H is deflected more reliably. become.
次に、本発明の具体的な実施例を第5図に示
す。構成は前述の構成と略同等であるので、同等
部分に同一符号を付すことにより説明を省略す
る。なお、本実施例は放電路規制体8の内部にヨ
ーク10を配設した例であり、磁石9とヨーク1
0との間の漏れ磁界を低減するため、ヨーク10
のうち磁石9に対向する部分は10aは、残りの
部分に比べて寸法をより大きくし、磁石9との対
向面積を増やしている。 Next, a specific embodiment of the present invention is shown in FIG. Since the configuration is substantially the same as the above-mentioned configuration, the explanation will be omitted by assigning the same reference numerals to the equivalent parts. Note that this embodiment is an example in which a yoke 10 is disposed inside the discharge path regulating body 8, and the magnet 9 and the yoke 1
In order to reduce the leakage magnetic field between the yoke 10 and
Among them, the portion 10a facing the magnet 9 is made larger in size than the remaining portion, increasing the area facing the magnet 9.
(発明の効果)
本発明は上記のように、管内に配設せる放電路
規制体の内部に、管外に配設せる磁石に対応する
ヨークを配設したことにより、磁界が1ケ所に集
中するため、管内における放電インピーダンス差
が明確となる。従つて、放電路の偏向がより明確
となり、例えば、管内に塗布する蛍光体を異なる
発光色に塗り分けた場合、発光色の変化を明確に
することができる。また、配光特性を変化させる
場合でも、所望通りの配光特性にすることができ
る。(Effects of the Invention) As described above, the present invention provides a yoke that corresponds to a magnet disposed outside the tube inside the discharge path regulating body disposed inside the tube, so that the magnetic field is concentrated in one place. Therefore, the difference in discharge impedance within the tube becomes clear. Therefore, the deflection of the discharge path becomes clearer, and for example, when the phosphor coated inside the tube is painted with different luminescent colors, the change in luminescent color can be made clear. Further, even when changing the light distribution characteristics, the desired light distribution characteristics can be achieved.
第1図及び第2図は従来例を示し、各図におい
てaは一部破断正面図、bは横断面図である。第
3図は第2図に示す如き従来例の動作原理を示す
図、第4図は本発明の動作原理を示す図、第5図
は本発明の一実施例を示す簡略図である。
1……ガラス管、4……電極、8……放電路規
制体、9……磁石、10……ヨーク。
1 and 2 show a conventional example, and in each figure, a is a partially cutaway front view, and b is a cross-sectional view. FIG. 3 is a diagram showing the operating principle of the conventional example shown in FIG. 2, FIG. 4 is a diagram showing the operating principle of the present invention, and FIG. 5 is a simplified diagram showing one embodiment of the present invention. DESCRIPTION OF SYMBOLS 1...Glass tube, 4...Electrode, 8...Discharge path regulator, 9...Magnet, 10...Yoke.
Claims (1)
電灯のガラス管内に、少なくとも一端が閉塞され
た円筒状の放電路規制体を、管と放電路規制体が
略同心円筒を形成するように配設すると共に、管
外に管軸と略垂直方向の磁界を発生する磁石を管
軸方向に沿つて配設し、上記磁石の磁界作用によ
り放電路を上記同心円筒間の所望位置に形成せし
めて成る低圧放電灯装置において、一端が上記磁
石のガラス管との非接触側極に連結された磁性体
から成るヨークの他端側を、上記放電路規制体の
内部に、上記磁石と対向するように管軸方向に沿
つて配設したことを特徴とする低圧放電灯装置。 2 上記ヨークの中、放電路規制体に沿う部分の
磁石との対向面幅を、ヨークの残りの部分より大
きくしたことを特徴とする特許請求の範囲第1項
記載の低圧放電灯装置。[Scope of Claims] 1. A cylindrical discharge path regulating body with at least one end closed is placed in a glass tube of a straight tube type low-pressure discharge lamp having a pair of electrodes arranged at both ends, and the tube and the discharge path regulating body are connected to each other. They are arranged so as to form substantially concentric cylinders, and a magnet that generates a magnetic field in a direction substantially perpendicular to the tube axis is arranged outside the tube along the direction of the tube axis, and the discharge path is caused to form a concentric cylinder by the action of the magnetic field of the magnet. In a low pressure discharge lamp device formed at a desired position between the cylinders, the other end of the yoke, which is made of a magnetic material and one end of which is connected to the non-contact side pole of the magnet with the glass tube, is connected to the discharge path regulator. A low-pressure discharge lamp device, characterized in that the device is disposed inside along the tube axis direction so as to face the magnet. 2. The low-pressure discharge lamp device according to claim 1, wherein the width of the surface facing the magnet of the portion of the yoke along the discharge path regulator is made larger than that of the remaining portion of the yoke.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22809283A JPS60119070A (en) | 1983-11-30 | 1983-11-30 | Low pressure discharge lamp device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22809283A JPS60119070A (en) | 1983-11-30 | 1983-11-30 | Low pressure discharge lamp device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60119070A JPS60119070A (en) | 1985-06-26 |
| JPH022267B2 true JPH022267B2 (en) | 1990-01-17 |
Family
ID=16871058
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22809283A Granted JPS60119070A (en) | 1983-11-30 | 1983-11-30 | Low pressure discharge lamp device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60119070A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6479950B2 (en) * | 1999-12-22 | 2002-11-12 | Matsushita Electric Industrial Co., Ltd. | High intensity discharge lamp, driving apparatus for high intensity discharge lamp, and high intensity discharge lamp system |
-
1983
- 1983-11-30 JP JP22809283A patent/JPS60119070A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60119070A (en) | 1985-06-26 |
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