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JPS6145349B2 - - Google Patents
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JPS6145349B2 - - Google Patents

Info

Publication number
JPS6145349B2
JPS6145349B2 JP17128579A JP17128579A JPS6145349B2 JP S6145349 B2 JPS6145349 B2 JP S6145349B2 JP 17128579 A JP17128579 A JP 17128579A JP 17128579 A JP17128579 A JP 17128579A JP S6145349 B2 JPS6145349 B2 JP S6145349B2
Authority
JP
Japan
Prior art keywords
tube
magnetic field
fluorescent lamp
generating device
field generating
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
JP17128579A
Other languages
Japanese (ja)
Other versions
JPS5697962A (en
Inventor
Minoru Yamamoto
Makoto Toho
Seigo Wada
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 JP17128579A priority Critical patent/JPS5697962A/en
Publication of JPS5697962A publication Critical patent/JPS5697962A/en
Publication of JPS6145349B2 publication Critical patent/JPS6145349B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/02Details
    • H01J61/04Electrodes; Screens; Shields
    • H01J61/10Shields, screens, or guides for influencing the discharge
    • H01J61/106Shields, screens, or guides for influencing the discharge using magnetic means

Landscapes

  • 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、ラピツドスタート型けい光灯に生ず
る劣化現象を防止したけい光灯点灯装置に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a fluorescent lamp lighting device that prevents the deterioration phenomenon that occurs in rapid start type fluorescent lamps.

ラピツドスタート型けい光灯は、例えば第1図
に示すように、ガラス管1の内面に透明導電性被
膜2を形成し、さらにその被膜上にけい光体膜3
を塗付し、ガラス管1内の放電空間4に所定量の
水銀及び不活性ガスを封入した構造を有してい
る。しかし、この種のけい光灯は長時間の点灯と
ともに、第2図に示すように、ランプ管端から約
10〜30cmの範囲に黒褐色ないしは黄褐色の変色部
5が生じ、これが拡大して外観を著しく損うにい
たるいわゆるアバタ現象が発生するという欠点を
有している。このアバタ現象の原因と経過は次の
ように考えられている。すなわち、まず過剰の水
銀が最冷点に凝集する。この凝集水銀と透明導電
性被膜2の間に電圧が印加され、水銀と被膜2と
の間でけい光体膜3を介して放電が生じ、その放
電エネルギーによつてけい光体膜3が破壊され
る。さらに、遊離ガス(電極やけい光体から出る
不純ガス)の作用も加わつて黒褐色や黄褐色の斑
点が発生し、次第に全体に拡大して変色部5とな
るのである。
A rapid start type fluorescent lamp, for example, as shown in FIG.
The discharge space 4 within the glass tube 1 is filled with a predetermined amount of mercury and inert gas. However, as shown in Figure 2, this type of fluorescent lamp does not only run for a long time, but also
It has the disadvantage that a blackish brown or yellowish brown discolored area 5 occurs in a range of 10 to 30 cm, and this enlarges to cause a so-called avatar phenomenon, which significantly impairs the appearance. The cause and course of this avatar phenomenon are thought to be as follows. That is, excess mercury first condenses at the coldest point. A voltage is applied between this aggregated mercury and the transparent conductive film 2, and a discharge occurs between the mercury and the film 2 through the phosphor film 3, and the phosphor film 3 is destroyed by the discharge energy. be done. Furthermore, with the addition of the action of free gas (impurity gas emitted from the electrodes and phosphor), dark brown or yellowish brown spots are generated, which gradually expand over the entire area and become the discolored area 5.

第3図a,bに全長120cmのけい光灯における
管長方向の管壁温度分布及び管内放電電位と透明
導電性被膜間の電位差の分布を示す。同図aよ
り、管壁温度は管端の電極部が最も高く(80〜90
℃)、管端から10cm〜30cmの点で急激に温度が低
くなり(約40℃)この付近に水銀が凝集すること
がわかる。しかし、この付近は同図bより明らか
なように、管内放電電位と透明導電性被膜2との
電位差が大きいため、凝集水銀と被膜2間でけい
光体膜3を介して放電が生じやすいのである。
Figures 3a and 3b show the tube wall temperature distribution in the tube length direction and the distribution of the potential difference between the discharge potential inside the tube and the transparent conductive coating in a fluorescent lamp with a total length of 120 cm. From figure a, the tube wall temperature is highest at the electrode part at the tube end (80 to 90
℃), and it can be seen that the temperature suddenly drops (approximately 40℃) at a point 10cm to 30cm from the end of the tube, and mercury condenses around this area. However, as is clear from Figure b in this area, there is a large potential difference between the discharge potential within the tube and the transparent conductive film 2, so discharge is likely to occur between the aggregated mercury and the film 2 via the phosphor film 3. be.

本発明はこのような従来例の問題点を解決する
ことを目的としてなされたもので、ラピツドスタ
ート型けい光灯の両方の管端から管の中央部へ向
けて長手方向に沿つて少なくとも全長の1/4の範
囲にそれぞれ磁界発生装置を設け、この磁界発生
装置によつて放電経路に対して交叉する方向に磁
界を発生することにより、変色部の発生を防止し
たけい光灯点灯装置を提供したものである。
The present invention has been made with the aim of solving the problems of the conventional method. A fluorescent lamp lighting device is provided in which a magnetic field generating device is installed in each of the 1/4 ranges, and this magnetic field generating device generates a magnetic field in a direction crossing the discharge path, thereby preventing the generation of discolored parts. This is what was provided.

以下、図示の実施例により本発明を説明する。
第4図は本発明を点灯装置のけい光灯に実施した
例であり、ガラス管1の内面に透明導電性被膜
2、けい光体膜3が形成され、放電空間4に所定
量の水銀及び不活性ガスが封入されている点は、
従来のものと同様である。6はガラス管1の外側
に両方の管端から管の中央部へ向けて長手方向に
沿つてそれぞれ設けられた磁界発生装置であり、
その長さは少なくともガラス管1の全長の1/4の
範囲にわたる寸法に選んであり、例えば全長120
cmのけい光灯においては30cmとなる。この磁界発
生装置6は、放電経路に対して交叉する方向に磁
界を発生するものであり、例えば1200ガウスの表
面磁束密度を有するフエライト製の永久磁石をガ
ラス管1の表面に密着させて構成する。
The present invention will be explained below with reference to illustrated embodiments.
FIG. 4 shows an example in which the present invention is applied to a fluorescent lamp of a lighting device, in which a transparent conductive film 2 and a phosphor film 3 are formed on the inner surface of a glass tube 1, and a predetermined amount of mercury and The fact that it is filled with inert gas is that
It is the same as the conventional one. Reference numeral 6 denotes a magnetic field generating device provided on the outside of the glass tube 1 along the longitudinal direction from both tube ends toward the center of the tube,
Its length is selected to be at least 1/4 of the total length of the glass tube 1, for example, the total length is 120 mm.
For cm fluorescent lamps, it is 30 cm. This magnetic field generator 6 generates a magnetic field in a direction crossing the discharge path, and is constructed by, for example, a permanent magnet made of ferrite having a surface magnetic flux density of 1200 Gauss closely attached to the surface of the glass tube 1. .

次にこの磁界発生装置6の作用について説明す
ると、このような磁界発生装置6を設けた場合、
管壁温度分布は第5図に示す実線Aのようにな
る。なお点線Bは磁界発生装置6のない従来例の
場合を示す。この理由は次のとおりである。すな
わち、放電空間4内では、放電経路に交叉する磁
界を印加することにより、内部の電子が加速され
て電子温度が上昇し、陽光柱電位傾度が上昇す
る。一方放電電流は連続であるため磁界印加部の
電力が上昇し、その点の管壁温度が上昇する。通
常は管端部より10cmくらいの所で急激に管壁温度
が低下し、電極近傍で熱せられた水銀蒸気が管中
央部へ拡散して行き、この点で急激に冷却されて
擬集水銀としてけい光体膜3の表面に付着するの
であるが、本実施例のように管端から中央部へ向
けて一定の範囲に磁界を印加することにより、前
述のように磁界印加物の電力が上昇してその部分
における管壁温度の急激な低下が緩和され、水銀
蒸気はその部分に凝集することなく管中央部へと
拡散して行き、中央部に水銀が凝集するようにな
る。ところで、管内放電電位と透明導電性被膜2
間の電位差は、第3図bに示すように管中央部に
行くほど低くなる。このため、たとえ水銀が凝集
してもその部分における管内放電電位と透明導電
性被膜2間の電位差は低く、もはや凝集水銀と被
膜2間での放電現象は生じなくなるのである。こ
の放電現象は、管内放電電位と透明導電性被膜と
の電位差が最大電位差の1/2以下になるとほとん
ど生じなくなることが確認されており、この電位
は第3図bのように直線的に変化するから、両端
から少なくとも管全長の1/4の範囲に磁界発生装
置6を設けておけば、実用上問題のあるような変
色部の発生を防止できるのである。
Next, to explain the operation of this magnetic field generating device 6, when such a magnetic field generating device 6 is provided,
The tube wall temperature distribution becomes as shown by the solid line A shown in FIG. Note that the dotted line B shows the case of a conventional example without the magnetic field generating device 6. The reason for this is as follows. That is, in the discharge space 4, by applying a magnetic field that crosses the discharge path, electrons therein are accelerated, the electron temperature rises, and the positive column potential gradient rises. On the other hand, since the discharge current is continuous, the power of the magnetic field application section increases, and the temperature of the tube wall at that point increases. Normally, the temperature of the tube wall drops rapidly at about 10 cm from the end of the tube, and the mercury vapor heated near the electrodes diffuses into the center of the tube, where it is rapidly cooled and becomes pseudo-mercury. It adheres to the surface of the phosphor film 3, but by applying a magnetic field in a certain range from the end of the tube to the center as in this example, the power of the object to which the magnetic field is applied increases as described above. As a result, the rapid drop in tube wall temperature at that portion is alleviated, and mercury vapor diffuses to the center of the tube without condensing in that portion, and mercury comes to condense in the center. By the way, the discharge potential inside the tube and the transparent conductive coating 2
The potential difference between the tubes becomes lower toward the center of the tube, as shown in FIG. 3b. Therefore, even if the mercury aggregates, the potential difference between the discharge potential within the tube and the transparent conductive coating 2 at that part is low, and no discharge phenomenon occurs between the aggregated mercury and the coating 2. It has been confirmed that this discharge phenomenon hardly occurs when the potential difference between the discharge potential inside the tube and the transparent conductive coating becomes less than 1/2 of the maximum potential difference, and this potential changes linearly as shown in Figure 3b. Therefore, by providing the magnetic field generating device 6 within a range of at least 1/4 of the total length of the tube from both ends, it is possible to prevent the occurrence of discolored portions that pose a practical problem.

第6図は本発明の他の実施例を示したもので、
点灯装置の器具本体7に磁界発生装置6を設けた
ものであり、磁界発生装置6は使用されるけい光
灯8の全長の1/4にわたつて両端に設けられ、放
電経路に対して交叉する方向に磁界を発生するよ
うにしてある。本実施例のように磁界発生装置6
を器具本体7に設けた場合、けい光灯8の外壁と
の間に空隙が生ずるので、けい光灯に磁界発生装
置を直接設けた場合と同一の効果を得るためには
より強力な磁界発生装置が必要となるが、一方通
常のラピツドスタート型のけい光灯を使用できる
という利点がある。
FIG. 6 shows another embodiment of the present invention,
A magnetic field generating device 6 is provided in the main body 7 of the lighting device, and the magnetic field generating device 6 is provided at both ends of the fluorescent lamp 8 that spans 1/4 of the total length, and crosses the discharge path. It is designed to generate a magnetic field in the direction of As in this embodiment, the magnetic field generator 6
If a magnetic field generating device is installed in the fixture body 7, a gap will be created between the fluorescent lamp 8 and the outer wall of the fluorescent lamp 8. Therefore, in order to obtain the same effect as when a magnetic field generating device is directly installed in the fluorescent lamp, a stronger magnetic field must be generated. equipment is required, but the advantage is that conventional rapid-start fluorescent lamps can be used.

上述のように、本発明はけい光灯の管端部分に
磁界発生装置を設けて、管端から中央部へかけて
の管壁温度の急激な低下をなくしているので、管
内放電電位と透明導電性被膜間の電位差が大きい
管端付近で水銀が凝集することがなく、けい光体
膜が破壊されて管端付近に黒褐色や黄褐色の変色
部が生ずる劣化現象を防止できる利点がある。
As mentioned above, the present invention provides a magnetic field generating device at the tube end of a fluorescent lamp to eliminate a sudden drop in tube wall temperature from the tube end to the center, thereby reducing the internal discharge potential and transparency. This has the advantage that mercury does not aggregate near the end of the tube where the potential difference between the conductive coatings is large, and the deterioration phenomenon in which the phosphor film is destroyed and a discolored area of blackish brown or yellowish brown occurs near the end of the tube can be prevented.

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

第1図は従来のけい光灯の一部破断側面図、第
2図は同上の劣化時の外観を示す側面図、第3図
a,bは同上の管壁温度の分布図及び管内放電電
位と透明導電性被膜間の電位差の分布図、第4図
a,bは本発明の一実施例によるけい光灯の正面
図および一部破断側面図、第5図は同上の管壁温
度の分布図、第6図は他の実施例の側面図であ
る。 1はガラス管、2は透明導電性被膜、3はけい
光体膜、6は磁界発生装置、7は器具本体、8は
けい光灯である。
Figure 1 is a partially cutaway side view of a conventional fluorescent lamp, Figure 2 is a side view showing the appearance of the same as above when it has deteriorated, and Figures 3a and b are distribution diagrams of tube wall temperature and discharge potential in the tube as above. 4a and 4b are a front view and a partially cutaway side view of a fluorescent lamp according to an embodiment of the present invention, and FIG. 5 is a distribution diagram of the temperature of the tube wall of the same as above. FIG. 6 is a side view of another embodiment. 1 is a glass tube, 2 is a transparent conductive coating, 3 is a phosphor film, 6 is a magnetic field generator, 7 is an instrument body, and 8 is a fluorescent lamp.

Claims (1)

【特許請求の範囲】[Claims] 1 ガラス管内面に透明導電性被膜を被覆し、そ
の被膜上にけい光体を塗付したラピツドスタート
型けい光灯を使用し、両方の管端から管の中央部
へ向けて長手方向に沿つて少なくとも全長の1/4
の範囲にそれぞれ磁界発生装置を設け、この磁界
発生装置によつて放電経路に対して交叉する方向
に磁界を発生することを特徴とするけい光灯点灯
装置。
1 Using a rapid-start type fluorescent lamp with a transparent conductive coating coated on the inner surface of a glass tube and a phosphor coated on the coating, light is applied in the longitudinal direction from both ends of the tube toward the center of the tube. along at least 1/4 of the total length
A fluorescent lamp lighting device characterized in that a magnetic field generating device is provided in each of the ranges, and the magnetic field generating device generates a magnetic field in a direction crossing the discharge path.
JP17128579A 1979-12-29 1979-12-29 Lighting device for fluorescent lamp Granted JPS5697962A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17128579A JPS5697962A (en) 1979-12-29 1979-12-29 Lighting device for fluorescent lamp

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17128579A JPS5697962A (en) 1979-12-29 1979-12-29 Lighting device for fluorescent lamp

Publications (2)

Publication Number Publication Date
JPS5697962A JPS5697962A (en) 1981-08-07
JPS6145349B2 true JPS6145349B2 (en) 1986-10-07

Family

ID=15920480

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17128579A Granted JPS5697962A (en) 1979-12-29 1979-12-29 Lighting device for fluorescent lamp

Country Status (1)

Country Link
JP (1) JPS5697962A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0581052U (en) * 1992-04-02 1993-11-02 株式会社吉野工業所 Liquid injection device

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5842156A (en) * 1981-09-04 1983-03-11 Matsushita Electric Works Ltd Prevention against end flicker of low pressure discharge lamp
JPS58115455A (en) * 1981-12-28 1983-07-09 Seiko Epson Corp printing device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0581052U (en) * 1992-04-02 1993-11-02 株式会社吉野工業所 Liquid injection device

Also Published As

Publication number Publication date
JPS5697962A (en) 1981-08-07

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