CN101994922A - Cold cathode fluorescent lamp for lighting - Google Patents
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- CN101994922A CN101994922A CN2009101613952A CN200910161395A CN101994922A CN 101994922 A CN101994922 A CN 101994922A CN 2009101613952 A CN2009101613952 A CN 2009101613952A CN 200910161395 A CN200910161395 A CN 200910161395A CN 101994922 A CN101994922 A CN 101994922A
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Abstract
一种照明用冷阴极荧光灯,包含一冷阴极荧光灯管以及一驱动单元。冷阴极荧光灯管的内管直径介于2.5mm~30mm之间,其两端各具有一电极,且冷阴极荧光灯管的电极发射电流与电极电子发射面积的比介于1.0mA/mm2~10mA/mm2之间。驱动单元与冷阴极荧光灯管的电极电性连接。承上所述,本发明提供一种大管径的冷阴极荧光灯管,其内管直径介于2.5mm~30mm之间,故其电极面积可大幅增加而能容许较高的管电流。
A cold cathode fluorescent lamp for lighting includes a cold cathode fluorescent lamp tube and a driving unit. The inner tube diameter of the cold cathode fluorescent lamp tube is between 2.5 mm and 30 mm, and each of the two ends of the cold cathode fluorescent lamp tube has an electrode, and the ratio of the electrode emission current to the electrode electron emission area of the cold cathode fluorescent lamp tube is between 1.0 mA/ mm2 and 10 mA/ mm2 . The driving unit is electrically connected to the electrode of the cold cathode fluorescent lamp tube. Based on the above, the present invention provides a large-diameter cold cathode fluorescent lamp tube, whose inner tube diameter is between 2.5 mm and 30 mm, so that the electrode area can be greatly increased to allow a higher tube current.
Description
技术领域technical field
本发明关于一种冷阴极荧光灯,特别关于一种照明用冷阴极荧光灯。The present invention relates to a cold cathode fluorescent lamp, in particular to a cold cathode fluorescent lamp for lighting.
背景技术Background technique
冷阴极荧光灯(Cold Cathode Fluorescent Lamp,CCFL)是一种汞放电灯,在通过高频高压的交流电后,灯管内部的电子撞击汞蒸气原子使其达到激发态(Excited State),被激发的汞原子会以放射紫外光的方式回到基态(Ground State),而所放射的紫外光会进一步激发冷阴极荧光灯中的荧光体,以产生可见光。A cold cathode fluorescent lamp (Cold Cathode Fluorescent Lamp, CCFL) is a mercury discharge lamp. After passing through high-frequency and high-voltage alternating current, the electrons inside the lamp tube hit the mercury vapor atoms to make them reach an excited state (Excited State), and the excited mercury The atoms will return to the ground state (Ground State) by emitting ultraviolet light, and the emitted ultraviolet light will further excite the phosphor in the cold cathode fluorescent lamp to produce visible light.
目前常见的冷阴极荧光灯管的内径大多分布在1.4~2.4mm间,而这些属于小管径的CCFL,其电极的电子发射面积也较小,导致所述灯管若操作在较高的管电流的状态下,会因电极发射电流及电极电子发射面积的比过高而造成灯管的管电流过饱和,也就是管电流超过电极电子发射面积所能负荷的能力。在此种情况下,虽然CCFL的消耗功率变高,但过多的功率消耗实际上都转换成热而不是光。为了得到较高的操作功率,且同时维持良好的效率,采用较大内径的冷阴极荧光灯管是有必要的,并且同时找出一个适合大内径CCFL的电极发射电流与电极电子发射面积的比是现今极切需要突破的课题。At present, the inner diameter of the common cold cathode fluorescent lamps is mostly distributed between 1.4 and 2.4mm, and these CCFLs with small diameters have smaller electron emission areas of the electrodes, so that if the lamps are operated at a higher tube current In the state, the tube current of the lamp tube will be oversaturated because the ratio of the electrode emission current to the electrode electron emission area is too high, that is, the tube current exceeds the capacity that the electrode electron emission area can bear. In this case, although the power consumption of the CCFL becomes high, the excessive power consumption is actually converted into heat instead of light. In order to obtain higher operating power while maintaining good efficiency, it is necessary to use a cold cathode fluorescent lamp with a larger inner diameter, and at the same time find a ratio of electrode emission current to electrode electron emission area suitable for a large inner diameter CCFL. A topic that urgently needs a breakthrough.
发明内容Contents of the invention
有鉴于上述课题,本发明的目的是提供一种合适大管径的冷阴极荧光灯使用的电极发射电流及电极电子发射面积的比,以提升冷阴极荧光灯的功率及发光效率。In view of the above problems, the purpose of the present invention is to provide a ratio of electrode emission current and electrode electron emission area suitable for large-diameter cold cathode fluorescent lamps, so as to improve the power and luminous efficiency of cold cathode fluorescent lamps.
本发明可采用以下技术方案来实现的。The present invention can be realized by adopting the following technical solutions.
依据本发明的一种照明用冷阴极荧光灯包含一冷阴极荧光灯管以及一驱动单元。冷阴极荧光灯管的内管直径介于2.5mm~30mm的间,其两端各具有一电极,且冷阴极荧光灯管的电极发射电流与电极电子发射面积的比介于1.0mA/mm2~10mA/mm2之间。驱动单元与冷阴极荧光灯管的电极电性连接。A cold cathode fluorescent lamp for illumination according to the present invention includes a cold cathode fluorescent lamp tube and a driving unit. The diameter of the inner tube of the cold cathode fluorescent lamp is between 2.5mm and 30mm, and each of its two ends has an electrode, and the ratio of the electrode emission current of the cold cathode fluorescent lamp to the electron emission area of the electrode is between 1.0mA/mm2 and 10mA/ between mm2. The driving unit is electrically connected with the electrodes of the CCFL.
前述的照明用冷阴极荧光,其中所述冷阴极荧光灯管的封入惰性气体气压介于1torr~100torr之间。In the aforementioned cold cathode fluorescent lamp for lighting, the pressure of the inert gas enclosed in the cold cathode fluorescent tube is between 1 torr and 100 torr.
前述的照明用冷阴极荧光,其中所述电极的材料是钨、钼、铌、镍或其合金。The aforementioned cold cathode fluorescent light for lighting, wherein the material of the electrode is tungsten, molybdenum, niobium, nickel or alloys thereof.
前述的照明用冷阴极荧光,其中所述电极是通过粉末冶金工艺而形成。In the aforementioned cold cathode fluorescent lighting, the electrodes are formed by powder metallurgy process.
前述的照明用冷阴极荧光,其中所述冷阴极荧光灯管的发光功率大于5W。The aforementioned cold cathode fluorescent lamp for lighting, wherein the luminous power of the cold cathode fluorescent tube is greater than 5W.
前述的照明用冷阴极荧光,其中所述冷阴极荧光灯管为直管、或U管、或C管、或环形管、或单螺旋管、或双螺旋管。The aforementioned cold cathode fluorescent lamp for lighting, wherein the cold cathode fluorescent tube is a straight tube, or a U tube, or a C tube, or an annular tube, or a single helical tube, or a double helical tube.
借由上述技术方案,本发明的照明用冷阴极荧光至少具有下列优点:With the above technical solution, the cold cathode fluorescent light for lighting of the present invention has at least the following advantages:
承上所述,本发明提供一种大管径的冷阴极荧光灯管,其内管直径介于2.5mm~30mm之间,故其电极面积可大幅增加而能容许较高的管电流。经由实验证实,本发明找出合适的电极发射电流与电极电子发射面积的比大于1.0mA/mm2时,可使冷阴极荧光灯开始达到高功率,而电极发射电流与电极电子发射面积的比小于10mA/mm2时,可避免冷阴极荧光灯管造成管电流过饱和,进而避免部分功率转成热,以提升发光效率。Based on the above, the present invention provides a CCFL tube with a large tube diameter. The inner tube diameter is between 2.5 mm and 30 mm, so the electrode area can be greatly increased and a higher tube current can be tolerated. It is confirmed by experiments that the present invention finds out that when the ratio of the electrode emission current to the electrode electron emission area is greater than 1.0mA/mm2, the cold cathode fluorescent lamp can start to reach high power, while the ratio of the electrode emission current to the electrode electron emission area is less than 10mA /mm2, it can avoid the oversaturation of the tube current caused by the cold cathode fluorescent tube, thereby preventing part of the power from being converted into heat, so as to improve the luminous efficiency.
附图说明Description of drawings
图1是本发明优选实施例的一种照明用冷阴极荧光灯的示意图。Fig. 1 is a schematic diagram of a cold cathode fluorescent lamp for illumination according to a preferred embodiment of the present invention.
主要组件符号说明:Description of main component symbols:
1:冷阴极荧光灯1: Cold Cathode Fluorescent Lamp
11:冷阴极荧光灯管11: cold cathode fluorescent tube
111:管体111: tube body
112:电极112: electrode
113:荧光体113: Phosphor
114:惰性气体114: Inert gas
12:驱动单元12: Drive unit
D1:内管直径D1: inner tube diameter
D2:电极直径D2: electrode diameter
具体实施方式Detailed ways
以下将参照相关图式,说明依本发明优选实施例的一种照明用冷阴极荧光灯。A cold cathode fluorescent lamp for lighting according to a preferred embodiment of the present invention will be described below with reference to related drawings.
如图1所示,本发明优选实施例的照明用冷阴极荧光灯1包含一冷阴极荧光灯管11以及一驱动单元12。As shown in FIG. 1 , a cold cathode
本发明不限制冷阴极荧光灯管11的型态,其可例如是直管、或U管、或C管、或环形管、或单螺旋管、或双螺旋管,在此以直管为例作说明。冷阴极荧光灯管11包含一管体111,管体111的内管直径D1介于2.5mm~30mm之间,其属于大管径的冷阴极荧光灯管。本实施例的内管直径D1以3mm为例。The present invention does not limit the type of
冷阴极荧光灯管11的两端各具有一电极112。本发明不限制电极112的形状,其可例如是直条形、圆形、椭圆形或杯状等等,在此以直条形为例,且其剖面是圆形。在本实施例中,冷阴极荧光灯管11的电极发射电流与电极电子发射面积的比介于1.0mA/mm2~10mA/mm2之间。其中,电极发射电流即所谓的「管电流」,在本实施例中电极发射电流以11mA~12mA为例。电极电子发射面积以电极112的剖面面积来作为计算值,电极112的直径D2是2.6mm(半径是1.3mm)。故以本实施例中电极发射电流是11mA,电极112的半径是1.3mm来计算,可得到电极发射电流与电极电子发射面积的比如下:Two ends of the
11/(π*1.3*1.3)=2.07(mA/mm2)11/(π*1.3*1.3)=2.07(mA/mm2)
另外,在其它实施例可计算出其它值。例如若以电极直径是2.1mm(半径是1.05mm),电极发射电流是8mA来计算时(计算公式同上),电极发射电流与电极电子发射面积的比约是2.31(mA/mm2);若以电极直径是3.7mm(半径是1.85mm),电极发射电流是27mA来计算时,电极发射电流与电极电子发射面积的比约是2.5(mA/mm2)。Additionally, other values may be calculated in other embodiments. For example, if the electrode diameter is 2.1mm (radius is 1.05mm), and the electrode emission current is 8mA (the calculation formula is the same as above), the ratio of the electrode emission current to the electrode electron emission area is about 2.31 (mA/mm2); The electrode diameter is 3.7mm (radius is 1.85mm), and when the electrode emission current is 27mA, the ratio of the electrode emission current to the electrode electron emission area is about 2.5 (mA/mm2).
经由数次实验证实,本发明找出合适的电极发射电流与电极电子发射面积的比大于1.0mA/mm2时(本实施例是2.07mA/mm2),可使冷阴极荧光灯1的发光功率开始达到高功率(例如大于5W),而电极发射电流与电极电子发射面积的比小于10mA/mm2时,可避免冷阴极荧光灯管11的管电流造成过饱和,进而避免部分功率消耗转成热,以提升发光效率。It has been confirmed through several experiments that the present invention finds out that when the ratio of the electrode emission current to the electrode electron emission area is greater than 1.0mA/mm2 (the present embodiment is 2.07mA/mm2), the luminous power of the cold cathode
冷阴极荧光灯管11还具有少量惰性气体114(例如氩、氖)封入其内,而封入惰性气体的气压介于1torr~100torr之间。此种低压的环境有助于电极发射电流与电极电子发射面积的比的提升,进而提升发光效率。The
另外,本实施例的电极112材料可使用耐离子轰击材料,例如钨、钼、铌、镍或其合金。由于冷阴极荧光灯管11内的电浆离子会轰击电极112而损耗电极,通过耐离子轰击材料可容许更高的电极发射电流与电极电子发射面积的比,进而提升发光效率。在本实施例中,电极112是通过粉末冶金工艺而形成。In addition, the material of the
驱动单元12与冷阴极荧光灯管11的电极112电性连接,以驱动冷阴极荧光灯管11发光。驱动单元12可包含换流电路(inverter)以提供高压的交流电。驱动单元12可以单边驱动方式驱动冷阴极荧光灯管11,或是以双边驱动方式驱动冷阴极荧光灯管11,在此以双边驱动方式为例。The
综上所述,本发明提供一种大管径的冷阴极荧光灯管,其内管直径介于2.5mm~30mm之间,故其电极面积可大幅增加而能容许较高的管电流。经由实验证实,本发明找出合适的电极发射电流与电极电子发射面积的比大于1.0mA/mm2时,可使冷阴极荧光灯开始达到高功率,而电极发射电流与电极电子发射面积的比小于10mA/mm2时,可避免冷阴极荧光灯管造成过饱和,进而避免部分功率转成热而非光以提升发光效率。To sum up, the present invention provides a CCFL tube with a large tube diameter. The inner tube diameter is between 2.5 mm and 30 mm, so the electrode area can be greatly increased and a higher tube current can be tolerated. It is confirmed by experiments that the present invention finds out that when the ratio of the electrode emission current to the electrode electron emission area is greater than 1.0mA/mm2, the cold cathode fluorescent lamp can start to reach high power, while the ratio of the electrode emission current to the electrode electron emission area is less than 10mA /mm2, it can avoid oversaturation of cold cathode fluorescent tubes, and then prevent part of the power from being converted into heat instead of light to improve luminous efficiency.
以上所述仅为举例性,而非为限制性者。任何未脱离本发明的精神与范畴,而对其进行的等效修改或变更,均应包含在后附的权利要求中。The above descriptions are illustrative only, not restrictive. Any equivalent modifications or changes made without departing from the spirit and scope of the present invention shall be included in the appended claims.
Claims (6)
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Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
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CN105390366A (en) * | 2014-08-28 | 2016-03-09 | 优志旺电机株式会社 | Long arc-type electric-discharge lamp |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
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CN105390366A (en) * | 2014-08-28 | 2016-03-09 | 优志旺电机株式会社 | Long arc-type electric-discharge lamp |
CN105390366B (en) * | 2014-08-28 | 2018-03-16 | 优志旺电机株式会社 | Long arc discharge lamp |
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Open date: 20110330 |