JPH08241669A - Single-side base type fluorescent lamp lighting device - Google Patents

Single-side base type fluorescent lamp lighting device

Info

Publication number
JPH08241669A
JPH08241669A JP7092295A JP7092295A JPH08241669A JP H08241669 A JPH08241669 A JP H08241669A JP 7092295 A JP7092295 A JP 7092295A JP 7092295 A JP7092295 A JP 7092295A JP H08241669 A JPH08241669 A JP H08241669A
Authority
JP
Japan
Prior art keywords
fluorescent lamp
lamp
temperature
base
opening
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
Application number
JP7092295A
Other languages
Japanese (ja)
Other versions
JP3190228B2 (en
Inventor
Takashi Osawa
隆司 大澤
Takeshi Yoshikawa
剛 吉川
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.)
OSURAMU MELCO KK
Original Assignee
OSURAMU MELCO KK
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 OSURAMU MELCO KK filed Critical OSURAMU MELCO KK
Priority to JP7092295A priority Critical patent/JP3190228B2/en
Publication of JPH08241669A publication Critical patent/JPH08241669A/en
Application granted granted Critical
Publication of JP3190228B2 publication Critical patent/JP3190228B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE: To suppress the mercury vapor pressure with no use of amalgam and enhance the lightness by lighting the lamp with a high frequency, and furnishing an opening penetrating from the outside to inside of a lamp base. CONSTITUTION: A glass bulb 1 is fitted with a lamp base 2 which bridges the two ends of the bulb. The lamp base 2 is made of polycarbonate and has an upper body part 2a and lower body part 2b formed in a cylinder. Four base pins 3 are implanted in the lower body part 2b and connected with leads, not illustrated, which are led out of an electrode 4. The upper body part 2a is furnished with an opening 5 bored in the form of a lattice. When this annular fluorescent lamp is lighted up using a high frequency lighting fixture, current is fed to the coil part of the electrode 4, and electric discharge is commenced between it and the other electrode. At this time the inside of the lamp is heated, and encapsulated mercury is vaporized, and the lamp is filled with a mercury vapor corresponding to its coldest point of temperature.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、例えば密閉形照明器具
等の高周囲温度となる雰囲気で点灯される管壁負荷4W
/cm2以上の片口金形蛍光ランプの明るさ向上に関する。
なお、本発明でいう片口金形蛍光ランプとは環形蛍光ラ
ンプ、コンパクト形蛍光ランプ等をいう。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a tube wall load of 4 W which is turned on in an atmosphere having a high ambient temperature, such as a closed type lighting fixture.
The invention relates to improving the brightness of single-ended fluorescent lamps of / cm 2 or more.
The single-ended metal fluorescent lamp used in the present invention means a ring fluorescent lamp, a compact fluorescent lamp, or the like.

【0002】[0002]

【従来の技術】蛍光ランプの明るさ向上及び効率改善に
はさまざまな研究がされている。例えば、点灯方式に関
しては、照明学会誌 VOL78 No.4 1994”蛍光
灯のイメージチェンジの主役−インバーター−”に示さ
れたように、高周波点灯することにより効率が向上す
る。一方、蛍光ランプの全光束は、ライティングハンド
ブック 社団法人照明学会1987に示されたように周
囲温度と共に変化することが知られており、通常、蛍光
ランプが点灯している周囲温度が25℃の時、最も明る
くなる。これは、水銀蒸気圧は蛍光ランプの最冷点温度
により決定されており、最冷点温度が低すぎると暗く、
また高すぎた場合も水銀の自己吸収により暗くなる。最
冷点温度に関しては、特開平4-298953 号公報にも示さ
れるように、蛍光ランプの場合は40℃が最適であり、
その時に発光効率が最大となる。この最冷点は、通常故
意(人為的)に制御するものではなかったが、特開平4
-298953 号公報に示されるように、純水銀に代りアマル
ガムを用いることにより、アマルガムの水銀蒸気圧特性
は純水銀の蒸気圧特性よりも低い為、周囲温度が高温の
場合、または最冷点温度が40℃を超える時は純水銀よ
りも明るくなることも知られている。
2. Description of the Related Art Various researches have been made on improving the brightness and efficiency of fluorescent lamps. For example, as for the lighting system, efficiency is improved by high-frequency lighting, as shown in ILL78, VOL78 No.4, 1994, "Main character of image change of fluorescent lamp-inverter-". On the other hand, it is known that the total luminous flux of a fluorescent lamp changes with the ambient temperature as shown in the Lighting Handbook, The Institute of Lighting, 1987. Normally, when the ambient temperature when the fluorescent lamp is lit is 25 ° C. , The brightest. This is because the mercury vapor pressure is determined by the coldest spot temperature of the fluorescent lamp, and it becomes dark when the coldest spot temperature is too low,
If it is too high, it will become dark due to self-absorption of mercury. As for the coldest spot temperature, as shown in Japanese Patent Application Laid-Open No. 4-298953, 40 ° C. is optimum for a fluorescent lamp,
At that time, the luminous efficiency becomes maximum. This coldest point is not normally controlled intentionally (artificially),
-298953 gazette, by using amalgam instead of pure water silver, the mercury vapor pressure characteristic of amalgam is lower than that of pure water silver. It is also known that when the temperature exceeds 40 ° C., it becomes brighter than pure silver.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、アマル
ガムを使用した場合コストが上昇するとともに、ランプ
始動特性を悪くする問題があった。一方、最近は蛍光ラ
ンプの周囲を器具で覆う密閉形器具等が多く普及し、ラ
ンプから見て、その点灯中の周囲温度が高くなり過ぎる
傾向にある。従って蛍光ランプの最冷点温度も高くな
り、アマルガム等の特別な手段を講じないと明るさが低
下する問題が頻発し、ランプコストの上昇や始動特性を
悪くさせずに明るさの向上が可能な蛍光ランプの出現が
強く望まれていた。従って、本発明の目的はランプコス
トを上げることなく、しかも始動特性を低下させずに周
囲温度が30℃を超えても明るさを向上できる管壁負荷4
W/cm2以上の片口金形蛍光ランプ点灯装置を提供しよう
とするものである。
However, when amalgam is used, the cost is increased and the lamp starting characteristic is deteriorated. On the other hand, recently, a lot of hermetically-sealed appliances that cover the circumference of a fluorescent lamp with appliances have become widespread, and the ambient temperature during lighting of the lamp tends to be too high when viewed from the lamp. Therefore, the coldest spot temperature of the fluorescent lamp also becomes high, and the problem that the brightness decreases frequently unless special measures such as amalgam are taken, and it is possible to improve the brightness without increasing the lamp cost and deteriorating the starting characteristics. The emergence of new fluorescent lamps was strongly desired. Therefore, an object of the present invention is to increase the brightness of the tube wall load 4 without increasing the lamp cost and without deteriorating the starting characteristics even when the ambient temperature exceeds 30 ° C.
It is an object of the present invention to provide a single-ended fluorescent lamp lighting device having a W / cm 2 or more.

【0004】[0004]

【課題を解決するための手段】本発明に係る蛍光ランプ
点灯装置は周囲温度が30℃を超え、かつ管壁負荷4W/c
m2以上の片口金形蛍光ランプを、35KHz以上の高周
波で点灯するとともに、ランプ口金に内外に貫通した開
口部を設けたものである。また、開口部を互いに独立し
複数個の孔に構成したものである。さらに、開口部を5
%以上の開口率に構成したものである。
The fluorescent lamp lighting device according to the present invention has an ambient temperature exceeding 30 ° C. and a tube wall load of 4 W / c.
A single-ended metal fluorescent lamp of m 2 or more is lit at a high frequency of 35 KHz or more, and an opening penetrating inside and outside is provided in the lamp base. Also, the openings are formed as a plurality of holes independent of each other. In addition, 5 openings
It is configured to have an aperture ratio of at least%.

【0005】[0005]

【作用】この発明の片口金形蛍光ランプ点灯装置におい
ては、最冷点が口金内のランプ部分に移動し、その温度
が従来の蛍光ランプの最冷点温度よりも低くなることが
実験的に確認された。従って周囲温度が30℃を超えて
も、最冷点温度が低いことから、アマルガムを用いずに
水銀蒸気圧が抑制される為、コストアップや始動特性低
下を招くことなく従来の片口金形蛍光ランプよりも明る
さを向上させる。また、開口部を独立した複数個の孔と
したので、充電部の露出を防ぎつつ口金の強度をあまり
落すことなく開口部としての効果的な貫通孔を形成する
ことができる。さらに、開口部の開口率を5%以上とし
たため、口金内のランプ部分に確実に最冷点を形成でき
る。
In the single-ended type fluorescent lamp lighting device of the present invention, it has been experimentally found that the coldest point moves to the lamp portion in the base and the temperature becomes lower than the coldest point temperature of the conventional fluorescent lamp. confirmed. Therefore, even if the ambient temperature exceeds 30 ° C, since the coldest spot temperature is low, the mercury vapor pressure is suppressed without the use of amalgam, so that the conventional single-ended die fluorescent light does not cause cost increase and start-up characteristic deterioration. Improve the brightness than the lamp. Moreover, since the opening is formed of a plurality of independent holes, it is possible to form an effective through hole as the opening while preventing the charging portion from being exposed and without significantly lowering the strength of the base. Furthermore, since the opening ratio of the opening is set to 5% or more, the coldest spot can be reliably formed in the lamp portion in the base.

【0006】[0006]

【実施例】本発明について、図面に示す一実施例に基づ
き説明する。図1の(A)は環形蛍光ランプ(FCL3
0)の部分断面図であり、図において1はガラスバルブ
である。このガラスバルブ1の内面には蛍光体被膜(図
示せず)が塗布されている。また、ガラスバルブ1内に
は所定量の水銀とアルゴン等の希ガスが封入されてい
る。さらにガラスバルブ1の内部には電極4が設けられ
ており、そのコイル部にはBao、SrO、CaO等の
電子放出物質が塗布されている。ガラスバルブ1の端部
にはその両端部を橋絡する口金2が装着されている。こ
の口金2はポリカーボネート製であり、一対の上面体部
2aと下面体部2bとで円筒形を形成されている。3は
この口金下面体部2bに植設された4本の口金ピンで、
電極4より導出された図示しないリード線と接続されて
いる。(B)は(A)の口金2近傍の部分拡大断面図
で、5は口金上面体部2aに格子状に穿孔された開口部
である。このように構成された環形蛍光ランプを高周波
点灯照明器具にて点灯すると、電極4のコイル部が通電
され、他方の電極との間で放電が開始される。その際、
ランプ内は加熱され、封入されている水銀が蒸発し、ラ
ンプ内はその蛍光ランプの最冷点温度に見合った水銀蒸
気圧で満たされる。図2にこの実施例の環形蛍光ランプ
(a)と従来の口金に開口部の無い環形蛍光ランプ
(b)を40KHzの高周波点灯回路で点灯した場合の
管壁温度分布を示す。これらランプの温度測定点は図3
に示すとおり、ランプ全長の中央部分(pos.1)、同じ
く4分の1部分(pos.2)、管端部から約10cm部分(po
s.3 )および口金内に位置する管端部(pos.4 )の4箇
所である。従来の環形蛍光ランプでは pos.1が最冷点と
なるが、本実施例の環形蛍光ランプでは最冷点が pos.
4に移る。そして、本実施例の環形蛍光ランプの最冷点
温度は従来の環形蛍光ランプの最冷点温度に比べおよそ
10℃低下する。図4に、本発明の実施例環形蛍光ラン
プ(a)と従来の環形蛍光ランプ(b)の温度特性を示
す。従来の環形蛍光ランプは、周囲温度25℃の時、明
るさが最大となり、それ以上の温度では明るさは低下す
る。しかし、本発明の環形蛍光ランプは周囲温度が35
℃の時に光束が最大となる為、周囲温度30℃以上では
従来の環形蛍光ランプよりも明るくなる。このように、
本発明の環形蛍光ランプを高周波点灯照明器具にて点灯
した場合、蛍光ランプの明るさを決定する最冷点が口金
内に移動し、しかも従来の環形蛍光ランプに比べ最冷点
が10℃低下する為、周囲温度が30℃以上では従来品
に比べ明るさの向上が見られる。ただし、本発明の環形
蛍光ランプの点灯中の周囲温度が30℃未満の時は、最冷
点温度が低くなり、水銀蒸気圧が過少となる為、逆効果
となる。また、磁気回路式安定器等で点灯した場合、環
形蛍光ランプの最冷点は図3のpos. 1にあり、本発明
同様の口金を施しても最冷点がpos. 4に移ることはな
く、また最冷点温度も変化はなく、その効果は得られな
い。この理由として、上記実施例の点灯周波数40KH
zにおいては、電極部の降下電圧が50Hz(60H
z)等商用周波数点灯に比べ小さくなり、従って電極部
の発熱量が少なくなり電極より、反放電路側のランプ管
面温度が下がる傾向にあるが、商用周波では比較的電極
での発熱が大きく、従って反放電路側のランプ管壁温度
も高く、本発明を用いても冷却が十分行われず、この結
果、本発明を施さない場合の最冷点温度より低下するこ
とがないためと推測される。高周波点灯においては、電
極部の発熱が小さくなり、本発明の効果が現れ、商用の
低周波では効果が現れないことは上述の通りであるが、
この効果の可否、すなわち最冷点移動の有無の臨界周波
数は凡そ35KHzであった。従って、本発明の効果を
得るには、35KHz以上の周波数で点灯する必要があ
る。管壁負荷4W/cm2未満のランプにおいては、電極部
の発熱は、4W/cm2以上のランプに比べあまり変化がな
いにもかかわらずランプ本体(放電路部)の発熱が小さ
いため、ランプ本体の温度が低く、その結果最冷点の温
度も低くなり、本発明の構成を用いても、最冷点が移動
(電極後方の方がより低温となる)することはない。ラ
ンプ始動特性は、上記実施例の環形蛍光ランプと従来の
環形蛍光ランプを点灯周波数40KHzの点灯回路にて
点灯した場合、その始動電圧は全て84〜86Vであ
り、両者間には全く差は見られなかった。また、開口部
の開口率を変化させた実験結果を図5に示す。環形蛍光
ランプの口金表面積を100 %とし、その開口部面積比で
開口率を示した。たて軸には口金を装着しない場合の低
下温度を100 %とし、各々の温度低下率を相対値で示し
た。図に示すように開口率と共に低下温度は上昇する。
図より明らかなとおり、開口部の開口率は5%以上が望
ましい。なお、口金の開口部形状及び設ける箇所も本実
施例のみに限定はされず、例えば図6ないし図8に示す
ものも適宜選択可能である。ところで、上記実施例では
FCL30タイプの環形蛍光ランプについて説明をした
が、他のワット、種々の光色に於ても同様な結果が得ら
れた。さらに、本発明は図9に示すようなコンパクト形
蛍光ランプにも適用できる。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described based on an embodiment shown in the drawings. FIG. 1A shows a ring-shaped fluorescent lamp (FCL3
It is a partial cross-sectional view of (0), in which 1 is a glass bulb. A phosphor coating (not shown) is applied to the inner surface of the glass bulb 1. The glass bulb 1 is filled with a predetermined amount of mercury and a rare gas such as argon. Further, an electrode 4 is provided inside the glass bulb 1, and the coil portion thereof is coated with an electron emitting substance such as Bao, SrO or CaO. At the end of the glass bulb 1, a mouthpiece 2 bridging both ends thereof is attached. The base 2 is made of polycarbonate, and has a cylindrical shape with a pair of upper body 2a and lower body 2b. Reference numeral 3 denotes four ferrule pins which are planted in the lower face body portion 2b of the ferrule,
It is connected to a lead wire (not shown) led out from the electrode 4. (B) is a partially enlarged cross-sectional view of the vicinity of the base 2 of (A), and 5 is an opening formed in the base body 2a of the base in a lattice shape. When the ring-shaped fluorescent lamp configured as described above is lit by the high-frequency lighting luminaire, the coil portion of the electrode 4 is energized, and the discharge with the other electrode is started. that time,
The interior of the lamp is heated, the enclosed mercury evaporates, and the interior of the lamp is filled with mercury vapor pressure that matches the coldest spot temperature of the fluorescent lamp. FIG. 2 shows tube wall temperature distributions when the ring-shaped fluorescent lamp (a) of this embodiment and the ring-shaped fluorescent lamp (b) of the related art having no opening are lit by a high-frequency lighting circuit of 40 KHz. The temperature measurement points of these lamps are shown in Fig. 3.
As shown in, the central part (pos.1) of the entire length of the lamp, the same quarter part (pos.2), and about 10 cm part from the tube end (po
s.3) and the pipe end (pos.4) located in the base. The coldest spot is pos.1 in the conventional ring-shaped fluorescent lamp, but the coldest spot is pos. 1 in the ring-shaped fluorescent lamp of the present embodiment.
Go to 4. The coldest spot temperature of the ring-shaped fluorescent lamp of this embodiment is about 10 ° C lower than the coldest spot temperature of the conventional ring-shaped fluorescent lamp. FIG. 4 shows the temperature characteristics of the example ring fluorescent lamp (a) of the present invention and the conventional ring fluorescent lamp (b). The brightness of the conventional ring-shaped fluorescent lamp is maximized at an ambient temperature of 25 ° C., and the brightness is reduced at a temperature higher than that. However, the ring fluorescent lamp of the present invention has an ambient temperature of 35.
Since the luminous flux becomes maximum when the temperature is ℃, it becomes brighter than the conventional ring fluorescent lamp at the ambient temperature of 30 ℃ or more. in this way,
When the ring-shaped fluorescent lamp of the present invention is lit by a high-frequency lighting luminaire, the coldest point that determines the brightness of the fluorescent lamp moves into the base, and the coldest point is reduced by 10 ° C. as compared with the conventional ring-shaped fluorescent lamp. Therefore, when the ambient temperature is 30 ° C. or higher, the brightness is improved as compared with the conventional product. However, when the ambient temperature during the lighting of the ring fluorescent lamp of the present invention is lower than 30 ° C., the coldest spot temperature becomes low and the mercury vapor pressure becomes too low, which has the opposite effect. Further, when the lamp is turned on by a magnetic circuit type ballast or the like, the coldest spot of the ring-shaped fluorescent lamp is at pos. 1 in FIG. 3, and even if the same base as the present invention is applied, the coldest spot does not move to pos. In addition, there is no change in the coldest spot temperature, and the effect cannot be obtained. The reason for this is that the lighting frequency of the above embodiment is 40 KH.
In z, the voltage drop of the electrode part is 50Hz (60H
z) and the like, which is smaller than that of commercial frequency lighting, and therefore the amount of heat generated in the electrode portion is smaller and the lamp surface temperature on the side opposite to the discharge path tends to be lower than that of the electrode. Therefore, it is presumed that the temperature of the lamp tube wall on the anti-discharge path side is also high, the cooling is not sufficiently performed even by using the present invention, and as a result, the temperature does not fall below the coldest point temperature when the present invention is not applied. As described above, in high-frequency lighting, the heat generation of the electrode portion is reduced, the effect of the present invention appears, and the effect does not appear at a commercial low frequency.
Whether or not this effect is possible, that is, the critical frequency with or without movement of the coldest spot was about 35 KHz. Therefore, in order to obtain the effect of the present invention, it is necessary to light at a frequency of 35 KHz or higher. For lamps with a tube wall load of less than 4 W / cm 2 , the heat generated in the electrode part does not change much compared to lamps with a load of 4 W / cm 2 or more, but the heat generated in the lamp body (discharge path) is small, so the lamp The temperature of the main body is low, and as a result, the temperature of the coldest spot is also low, and even when the configuration of the present invention is used, the coldest spot does not move (the temperature behind the electrode becomes lower). Regarding the lamp starting characteristics, when the ring fluorescent lamp of the above-mentioned embodiment and the conventional ring fluorescent lamp are lighted by a lighting circuit having a lighting frequency of 40 KHz, the starting voltages are all 84 to 86 V, and there is no difference between them. I couldn't do it. Moreover, the experimental result which changed the aperture ratio of the opening part is shown in FIG. The surface area of the base of the ring-shaped fluorescent lamp was 100%, and the aperture ratio was shown by the area ratio of the openings. The temperature drop when the die was not attached to the vertical shaft was set to 100%, and the temperature drop rate was shown as a relative value. As shown in the figure, the lowering temperature increases with the aperture ratio.
As is clear from the figure, the aperture ratio of the opening is preferably 5% or more. It should be noted that the shape and location of the opening of the die are not limited to those in this embodiment, and for example, those shown in FIGS. 6 to 8 can be selected as appropriate. By the way, although the FCL30 type ring fluorescent lamp has been described in the above embodiment, similar results were obtained with other watts and various light colors. Further, the present invention can be applied to a compact fluorescent lamp as shown in FIG.

【0007】[0007]

【発明の効果】以上説明したように、本発明によれば3
5KHz以上の高周波で点灯し、かつ口金に、口金内外
に貫通した開口部を設けることによって、最冷点は口金
内に移り、その温度は従来の管壁負荷4W/cm2以上の片
口金形蛍光ランプよりも低下する為、アマルガムを用い
ることなく水銀蒸気圧が抑制され、周囲温度が30℃以
上の時でもコストアップや始動特性低下を招くことな
く、明るさを向上することができる。さらに、開口部を
設けることにより材料の使用量を減らせ原価低減や、開
口部より口金内部の光を外部に放出させ得るため、密閉
タイプの照明器具に使用した場合等口金部の陰を目立た
なくし外観を向上させる等の付随的効果も期待できる。
また、開口部を互いに独立した複数個の孔としたため、
所望の箇所への最冷点の形成を確保しつつ、口金強度の
低下や充電部露出を防止できる。さらにまた、開口部の
開口率を5%以上としたことにより、最冷部を口金内に
確実に形成させ得る効果がある。
As described above, according to the present invention, 3
By illuminating at a high frequency of 5 KHz or more, and providing the base with an opening that penetrates the inside and outside of the base, the coldest point moves to the inside of the base, and the temperature is a single-sided mold with a conventional tube wall load of 4 W / cm 2 Since it is lower than that of a fluorescent lamp, the mercury vapor pressure is suppressed without using an amalgam, and the brightness can be improved even when the ambient temperature is 30 ° C. or higher without inviting cost increase and starting characteristic deterioration. Furthermore, by providing an opening, the amount of material used can be reduced, cost can be reduced, and the light inside the base can be emitted from the opening to the outside, so the shadow of the base will not be conspicuous when used in a closed type lighting fixture. Ancillary effects such as improving the appearance can also be expected.
Also, because the opening is a plurality of holes independent of each other,
It is possible to prevent lowering of the die strength and exposure of the charged part while ensuring formation of the coldest spot at a desired location. Furthermore, by setting the opening ratio of the opening portion to 5% or more, there is an effect that the coldest portion can be reliably formed in the die.

【図面の簡単な説明】[Brief description of drawings]

【図1】 本発明の一実施例を示す環形蛍光ランプの一
部切欠正面図及びランプ口金部の詳細図である。
FIG. 1 is a partially cutaway front view of a ring-shaped fluorescent lamp showing an embodiment of the present invention and a detailed view of a lamp cap portion.

【図2】 本発明環形蛍光ランプと従来の環形蛍光ラン
プの温度特性図である。
FIG. 2 is a temperature characteristic diagram of the ring fluorescent lamp of the present invention and a conventional ring fluorescent lamp.

【図3】 環形蛍光ランプの管壁温度測定点を示す図で
ある。
FIG. 3 is a diagram showing tube wall temperature measurement points of a ring-shaped fluorescent lamp.

【図4】 本発明環形蛍光ランプと従来の環形蛍光ラン
プの管壁温度分布図である。
FIG. 4 is a tube wall temperature distribution diagram of the ring fluorescent lamp of the present invention and a conventional ring fluorescent lamp.

【図5】 本発明環形蛍光ランプの口金カバー開口率と
相対低下温度特性図である。
FIG. 5 is a characteristic view of a base cover opening ratio and a relative decrease temperature of the ring fluorescent lamp of the present invention.

【図6】 本発明の他の実施例を示す開口部を設けた口
金上面体の斜視図である。
FIG. 6 is a perspective view of a base body having a base provided with an opening according to another embodiment of the present invention.

【図7】 本発明の他の実施例を示す開口部を設けた口
金上面体の斜視図である。
FIG. 7 is a perspective view of a cap upper surface body provided with an opening according to another embodiment of the present invention.

【図8】 本発明の他の実施例を示す開口部を設けた口
金上面体の斜視図である。
FIG. 8 is a perspective view of a cap upper surface body having an opening according to another embodiment of the present invention.

【図9】 本発明をコンパクト形蛍光ランプに適用した
実施例を示す正面図である。
FIG. 9 is a front view showing an embodiment in which the present invention is applied to a compact fluorescent lamp.

【符号の説明】[Explanation of symbols]

1 ガラスバルブ、2 口金、5 開口部。 1 glass bulb, 2 bases, 5 openings.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 高周波で片口金形の蛍光ランプを点灯す
るものであって、ランプ点灯中の周囲温度が30℃を超
え、かつ管壁負荷が4W/cm2以上となる片口金形蛍光ラ
ンプ点灯装置において、上記高周波を35KHz以上と
するとともに、上記蛍光ランプの口金に、この口金の内
外に貫通する開口部を設けたことを特徴とする片口金形
蛍光ランプ点灯装置。
1. A single-ended fluorescent lamp for lighting a single-ended fluorescent lamp at high frequency, wherein the ambient temperature during lighting of the lamp exceeds 30 ° C. and the tube wall load is 4 W / cm 2 or more. In the lighting device, the high frequency is set to 35 KHz or more, and the base of the fluorescent lamp is provided with an opening penetrating inside and outside of the base.
【請求項2】 開口部は互いに独立した複数個の孔とし
たことを特徴とする請求項1記載の片口金形蛍光ランプ
点灯装置。
2. The single-ended metal fluorescent lamp lighting device according to claim 1, wherein the opening is a plurality of holes independent of each other.
【請求項3】 開口部の開口率を5%以上としたことを
特徴とする請求項1記載の片口金形蛍光ランプ点灯装
置。
3. The single-ended fluorescent lamp lighting device according to claim 1, wherein the opening ratio of the opening is 5% or more.
JP7092295A 1995-03-03 1995-03-03 Single die fluorescent lamp lighting device Expired - Lifetime JP3190228B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7092295A JP3190228B2 (en) 1995-03-03 1995-03-03 Single die fluorescent lamp lighting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7092295A JP3190228B2 (en) 1995-03-03 1995-03-03 Single die fluorescent lamp lighting device

Related Child Applications (3)

Application Number Title Priority Date Filing Date
JP2001022449A Division JP3467477B2 (en) 2001-01-30 2001-01-30 Ring fluorescent lamp
JP2001106703A Division JP3490979B2 (en) 2001-04-05 2001-04-05 Single-base fluorescent lamp lighting device, ring-shaped fluorescent lamp, method of manufacturing ring-shaped fluorescent lamp, method of manufacturing base of ring-shaped fluorescent lamp, and method of lighting ring-shaped fluorescent lamp
JP2001106688A Division JP3467480B2 (en) 2001-04-05 2001-04-05 Single die fluorescent lamp lighting device

Publications (2)

Publication Number Publication Date
JPH08241669A true JPH08241669A (en) 1996-09-17
JP3190228B2 JP3190228B2 (en) 2001-07-23

Family

ID=13445490

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7092295A Expired - Lifetime JP3190228B2 (en) 1995-03-03 1995-03-03 Single die fluorescent lamp lighting device

Country Status (1)

Country Link
JP (1) JP3190228B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6031324A (en) * 1997-03-31 2000-02-29 Matsushita Electric Industrial Co., Ltd. Annulus fluorescent lamp
JP2001307680A (en) * 2000-04-24 2001-11-02 Matsushita Electric Works Ltd Lighting apparatus of discharge lamp

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6031324A (en) * 1997-03-31 2000-02-29 Matsushita Electric Industrial Co., Ltd. Annulus fluorescent lamp
JP2001307680A (en) * 2000-04-24 2001-11-02 Matsushita Electric Works Ltd Lighting apparatus of discharge lamp

Also Published As

Publication number Publication date
JP3190228B2 (en) 2001-07-23

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