CN201532936U - Low power electrodeless lamp tube and light source - Google Patents
Low power electrodeless lamp tube and light source Download PDFInfo
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- CN201532936U CN201532936U CN2009202796994U CN200920279699U CN201532936U CN 201532936 U CN201532936 U CN 201532936U CN 2009202796994 U CN2009202796994 U CN 2009202796994U CN 200920279699 U CN200920279699 U CN 200920279699U CN 201532936 U CN201532936 U CN 201532936U
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- 230000005284 excitation Effects 0.000 claims abstract description 31
- 239000000843 powder Substances 0.000 claims description 9
- 229910000497 Amalgam Inorganic materials 0.000 claims description 7
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Abstract
Description
技术领域technical field
本实用新型涉及无极灯技术,特别是涉及一种小功率无极灯灯管及光源。The utility model relates to the technology of an electrodeless lamp, in particular to a low-power electrodeless lamp tube and a light source.
背景技术Background technique
无极灯是综合应用功率电子学,等离子体学,磁性材料学等领域最新科技成果研制开发出来的高新技术产品,其代表了照明技术领域高光效,长寿命,高显色性的未来发展方向。照明专家将这种绿色照明新光源称为“照明领域新革命的开始”,它必将成为21世纪最有发展前景的绿色节能照明光源。The electrodeless lamp is a high-tech product developed by comprehensively applying the latest scientific and technological achievements in the fields of power electronics, plasma science, and magnetic materials. It represents the future development direction of high light efficiency, long life, and high color rendering in the field of lighting technology. Lighting experts call this new green lighting source "the beginning of a new revolution in the field of lighting", and it will surely become the most promising green and energy-saving lighting source in the 21st century.
目前,常用的无极灯为电磁感应无极灯,其主要由三部分组成:高频发生器、耦合器和灯泡。高频发生器的功能类似于普通节能灯的电子镇流器,将工频市电转换为高频强信号,并传输给耦合器。耦合器的功能就像是一个发射天线,它将高频强信号耦合进灯泡,完成能量的第二次传递。灯泡是一个里面充有稀有气体及汞蒸气等工作气体的密闭空腔,灯泡的壁上涂有发光物质荧光粉。当耦合器将高频能量耦合进灯泡后,灯泡中的工作气体在强大的电磁场作用下发生气体雪崩电离形成等离子体,等离子体的受激原子返回基态时自发辐射出254nm的紫外线,紫外线激发荧光粉发出可见光,从而完成能量的第三次转换。在三次能量转换过程中,没有灯丝或电极参与工作,故无极灯的寿命仅取决于其电子线路、灯泡的制造技术和荧光粉的自然衰减,使其寿命远远高于白炽灯等传统光源,而逐渐体现其市场优势。At present, the commonly used electrodeless lamp is an electromagnetic induction electrodeless lamp, which is mainly composed of three parts: a high frequency generator, a coupler and a bulb. The function of the high-frequency generator is similar to the electronic ballast of ordinary energy-saving lamps. It converts the power frequency mains into a high-frequency strong signal and transmits it to the coupler. The function of the coupler is like a transmitting antenna, which couples the high-frequency strong signal into the bulb to complete the second transfer of energy. The light bulb is a closed cavity filled with working gases such as rare gas and mercury vapor, and the wall of the light bulb is coated with luminescent substance phosphor. When the coupler couples high-frequency energy into the bulb, the working gas in the bulb undergoes gas avalanche ionization under the action of a strong electromagnetic field to form a plasma. When the excited atoms of the plasma return to the ground state, they spontaneously radiate 254nm ultraviolet rays, and the ultraviolet rays excite fluorescence. The powder emits visible light, thus completing the third conversion of energy. During the three energy conversion processes, there is no filament or electrode involved in the work, so the life of the electrodeless lamp depends only on its electronic circuit, the manufacturing technology of the bulb and the natural attenuation of the phosphor powder, making its life much longer than that of traditional light sources such as incandescent lamps. And gradually reflect its market advantage.
目前,市场上常见的无极灯寿命已高于6万小时,是白炽灯的60倍,卤素灯的20倍,且与普通白炽灯相比,节能80%以上。其设计构成主要有两种形式,具体如下:At present, the service life of common electrodeless lamps on the market has exceeded 60,000 hours, which is 60 times that of incandescent lamps and 20 times that of halogen lamps. Compared with ordinary incandescent lamps, it can save energy by more than 80%. There are mainly two forms of its design composition, as follows:
第一种是将励磁线圈缠绕于铁氧体磁芯上,构成耦合器,且将耦合器内置于发光灯管的形式。具体请参考图1,高频发生器内置于金属套内,构成灯座11;耦合器12与灯座11内的高频发生器电性连接,并于组装后置于发光灯管13内,从而于发光灯管13内形成放电空间;发光灯管13内填充稀有气体和汞蒸气,且表面涂有荧光层。The first is to wind the excitation coil on the ferrite core to form a coupler, and the coupler is built into the light-emitting tube. Please refer to Figure 1 for details. The high-frequency generator is built into the metal sleeve to form the
第二种是将磁环抱箍于灯体上,即磁环耦合形式。在此种形式中,灯体需设计成闭合结构,例如闭合环形或矩形。具体请参考图2,以闭合矩形为例,于灯体21的两对称边上对称设置有磁环22,且使磁环22抱箍于灯体21之上。The second is to hoop the magnetic ring on the lamp body, that is, the magnetic ring coupling form. In this form, the lamp body needs to be designed as a closed structure, such as a closed ring or rectangle. Please refer to FIG. 2 for details. Taking a closed rectangle as an example,
以上设计结构的无极灯已具备了无极灯的众多优点,然而随着对节能要求的进一步提高,人们对小功率的无极灯的要求越来越多,同时,无极灯小型化的问题也日益受到人们的关注。以上第一种无极灯在小型化时,将碰到散热问题,如此便需要加入散热导管等元件,从而使得制造工艺复杂,且增加了制作成本。而第二种无极灯,其磁环体积与无极灯形状要求限制了其进一步小型化,其更佳适于大功率无极灯的制造。The electrodeless lamp with the above design structure has many advantages of the electrodeless lamp. However, with the further improvement of the energy saving requirements, people have more and more requirements for the electrodeless lamp with low power. people's attention. When the above first type of electrodeless lamp is miniaturized, heat dissipation will be encountered, so elements such as heat dissipation pipes need to be added, which complicates the manufacturing process and increases the manufacturing cost. As for the second type of electrodeless lamp, the volume of the magnetic ring and the shape of the electrodeless lamp limit its further miniaturization, which is more suitable for the manufacture of high-power electrodeless lamps.
为此,市场上需要一种新的无极灯,适于小功率应用,且易于小型化。For this reason, there is a need in the market for a new electrodeless lamp that is suitable for low-power applications and that is easy to miniaturize.
实用新型内容Utility model content
本实用新型所要解决的技术问题是小功率无极灯小型化的问题。The technical problem to be solved by the utility model is the miniaturization of the low-power electrodeless lamp.
为解决以上技术问题,本实用新型一种小功率无极灯灯管,其内表面具有荧光粉层,该灯管包括:两个平行管体、一个圆柱形管体和一个椭球形管体,其中两个平行管体的一端闭合,另一端与所述椭球形管体平滑连接,且内部通过所述椭球形管体连通,所述圆柱形管体,连通于所述两个平行管体之间。In order to solve the above technical problems, the utility model provides a low-power electrodeless lamp tube, which has a fluorescent powder layer on its inner surface. The tube includes: two parallel tube bodies, a cylindrical tube body and an ellipsoid tube body, wherein One end of the two parallel pipes is closed, the other end is smoothly connected to the elliptical pipe, and the inside is communicated through the elliptical pipe, and the cylindrical pipe is connected between the two parallel pipes .
本实用新型还提供一种小功率无极灯光源,包括:灯管,其内表面具有荧光粉层,且该灯管包括两个平行管体、一个圆柱形管体和一个椭球形管体,其中两个平行管体的一端闭合,另一端与所述椭球形管体平滑连接,且内部通过所述椭球形管体连通,所述圆柱形管体,连通于所述两个平行管体之间;励磁线圈,缠绕于所述圆柱形管体之上,且具有引出端,用以电性连接一激励源;汞齐,位于所述两平行管体的闭合端;稀有气体,填充于所述灯管内。The utility model also provides a low-power electrodeless light source, including: a lamp tube with a fluorescent powder layer on its inner surface, and the lamp tube includes two parallel tube bodies, a cylindrical tube body and an ellipsoid tube body, wherein One end of the two parallel pipes is closed, the other end is smoothly connected to the elliptical pipe, and the inside is communicated through the elliptical pipe, and the cylindrical pipe is connected between the two parallel pipes ; the excitation coil is wound on the cylindrical tube and has a lead-out end for electrically connecting an excitation source; the amalgam is located at the closed end of the two parallel tubes; the rare gas is filled in the Inside the tube.
进一步的,该小功率无极灯光源应用为23W时,所述励磁线圈为14匝至22匝。Further, when the low-power induction lamp light source is applied at 23W, the excitation coil has 14 turns to 22 turns.
进一步的,该小功率无极灯光源应用为15W时,所述励磁线圈为10匝至18匝。Further, when the low-power induction lamp light source is applied at 15W, the exciting coil has 10 turns to 18 turns.
进一步的,填充于所述灯管内的稀有气体压强为20Pa至200Pa。Further, the pressure of the rare gas filled in the lamp tube is 20Pa to 200Pa.
进一步的,所述励磁线圈的输入频率为2.5MHz至15MHz。Further, the input frequency of the exciting coil is 2.5MHz to 15MHz.
可见,应用以上小功率无极灯灯管,可以将励磁线圈直接缠绕于灯管之上,从而耦合电磁能量进入灯管,以激发灯管内的汞齐和稀有气体产生等离子体,等离子体的受激原子返回基态时自发辐射出紫外线,紫外线激发荧光粉发出可见光。与现有技术相比,未使用铁氧体磁芯,从而极大的减少了使用过程中的散热量,从而无需做特殊散热设计;另外,采用励磁线圈直接缠绕的方式来代替磁环,有利于其小型化的设计。It can be seen that the application of the above low-power electrodeless lamp tube can directly wrap the excitation coil on the lamp tube, thereby coupling electromagnetic energy into the lamp tube to excite the amalgam and rare gas in the lamp tube to generate plasma. When the excited atoms return to the ground state, they spontaneously radiate ultraviolet rays, and the ultraviolet rays excite the phosphor to emit visible light. Compared with the existing technology, no ferrite core is used, which greatly reduces the heat dissipation during use, so that no special heat dissipation design is required; in addition, the excitation coil is directly wound instead of the magnetic ring, which has the advantages of Conducive to its miniaturized design.
附图说明Description of drawings
图1为一种现有的无极灯结构示意图;Fig. 1 is a kind of structural schematic diagram of existing electrodeless lamp;
图2为另一种现有的无极灯结构示意图;FIG. 2 is a structural schematic diagram of another existing electrodeless lamp;
图3为本实用新型一实施例所提供的小功率无极灯光源的结构示意图;Fig. 3 is a schematic structural view of a low-power electrodeless light source provided by an embodiment of the present invention;
图4为图3中小功率无极灯光源的A-A方向的示意图;Fig. 4 is a schematic diagram of the A-A direction of the low-power electrodeless light source in Fig. 3;
图5为图3中小功率无极灯光源的B-B方向的示意图;Fig. 5 is a schematic diagram of the B-B direction of the low-power electrodeless light source in Fig. 3;
图6与图7为本实用新型一实施例所提供的小功率无极灯光源的尺寸标注示意图。FIG. 6 and FIG. 7 are schematic diagrams showing dimensions of the low-power induction lamp light source provided by an embodiment of the present invention.
具体实施方式Detailed ways
为让本实用新型的上述特征和优点能更明显易懂,下文特举示例性实施例,并配合附图,作详细说明如下。In order to make the above-mentioned features and advantages of the present invention more comprehensible, exemplary embodiments are given below, together with accompanying drawings, for a detailed description as follows.
请参考图3,其为本实用新型一实施例所提供的小功率无极灯光源的结构示意图。且合并参考图4与图5,其分别为图3中小功率无极灯光源的A-A和B-B方向的示意图。Please refer to FIG. 3 , which is a schematic structural diagram of a low-power electrodeless light source provided by an embodiment of the present invention. And refer to FIG. 4 and FIG. 5 , which are schematic diagrams of directions A-A and B-B of the low-power induction lamp light source in FIG. 3 , respectively.
如图所示,该小功率无极灯光源的灯管100经过设计而应用于小功率无极灯,可直接于其上缠绕励磁线圈200,来取代现有的耦合器,耦合电磁能量进入灯管100,以激发灯管100内的汞齐和稀有气体产生等离子体,等离子体的受激原子返回基态时自发辐射出紫外线,紫外线激发荧光粉发出可见光。与现有技术相比,本实施例所提供的无极灯光源未使用铁氧体磁芯,从而极大的减少了使用过程中的散热量,从而无需做特殊散热设计;另外,采用励磁线圈200直接缠绕的方式来代替磁环,有利于其小型化的设计。As shown in the figure, the
具体而言,灯管100由两个平行管体110、一个圆柱形管体120和一个椭球形管体130平滑连接而成;其中两个平行管体110的一端闭合,另一端与椭球形管体130平滑连接,且内部通过椭球形管体130连通;圆柱形管体120则连通于两个平行管体110之间。Specifically, the
如此,励磁线圈200可以直接缠绕于圆柱形管体120之上,且具有引出端210,用以电性连接一激励源。另外,灯管100的内表面具有荧光粉层101,其内填充有稀有气体,且两平行管体110的闭合端处设置有汞齐300。In this way, the
以上小功率无极灯光源,将线圈直接绕制于灯管上,形成闭合梨型放电管,通过其产生的高频电流耦合电磁场能量进入灯管内,激发其内的汞齐和稀有气体,而产生等离子体,等离子体的受激原子返回基态时自发辐射出紫外线,紫外线激发荧光粉发出可见光。具体原理如下:The above low-power electrodeless light source, the coil is directly wound on the lamp tube to form a closed pear-shaped discharge tube, and the high-frequency current coupled electromagnetic field energy generated by it enters the lamp tube to excite the amalgam and rare gas in it, and Plasma is generated, and when the excited atoms of the plasma return to the ground state, they spontaneously radiate ultraviolet rays, and the ultraviolet rays excite the fluorescent powder to emit visible light. The specific principles are as follows:
首先,将励磁线圈缠绕于圆柱形管体作为能量输入初级侧;其次,励磁线圈通以MHz级频率的电流作为耦合电信号;最后,高频电流产生的高频电磁能耦合进入灯管内,激发等离子辐射发光。此类光源内部是以高频电场电离汞原子形成放电电流(Hg电离电位为10.4eV),其激发电离原理与普通荧光灯无异:Hg激发态——63P1原子(激发电位为4.89eV)自发跃迁至基态时,产生253.7nm光子;253.7nm光子激发管壁内荧光粉层,产生三基色可见光,并形成白光输出。Firstly, the excitation coil is wound around the cylindrical tube body as the energy input primary side; secondly, the excitation coil passes a current with MHz frequency as the coupled electrical signal; finally, the high-frequency electromagnetic energy generated by the high-frequency current is coupled into the lamp tube, Excited plasma radiates luminescence. This type of light source uses a high-frequency electric field to ionize mercury atoms to form a discharge current (the ionization potential of Hg is 10.4eV ). ) when it spontaneously transitions to the ground state, 253.7nm photons are generated; the 253.7nm photons excite the phosphor layer in the tube wall to generate three primary colors of visible light and form white light output.
较佳的,以上励磁线圈缠绕方式为密布平行缠绕的方式,且线圈的匝数可以根据实际需要的光源功率变动,以缠满整个圆柱形管体为限。以下,结合图6与图7,并通过两个具体实施例来加以说明。Preferably, the above excitation coil is wound in a densely parallel winding manner, and the number of turns of the coil can be changed according to the actual power of the light source required, and is limited to wrapping the entire cylindrical tube body. Hereinafter, it will be described with reference to FIG. 6 and FIG. 7 through two specific embodiments.
实施例一:Embodiment one:
请合并参考图6、图7以及表1,其中表1为本实用新型应用于23W无极灯时的尺寸列表。Please refer to Figure 6, Figure 7 and Table 1 together, where Table 1 is a list of dimensions when the utility model is applied to a 23W electrodeless lamp.
表1Table 1
此时,励磁线圈200的匝数不低于14匝,且由于圆柱形管体120的长度L2限制,其最多可缠绕22匝。At this time, the number of turns of the
以14匝为例,励磁线圈200的输入频率在2.5MHz~15MHz的情况下,匹配2KV以上耐压值的一定容抗的安规电容,通过调整激励电压,发光灯管功率从10W~40W之间可任意调节。同样条件下,励磁线圈200为18匝时,发光灯管功率从10W~45W之间可任意调节。同样条件下,磁线圈200为22匝时,发光灯管功率从10W~55W之间均可任意调节。Taking 14 turns as an example, when the input frequency of the
值得一提的是,以上发光灯管功率增加时,发光呈现逐步扩散的趋势和特点。即发光功率小时,发光区域主要聚集在励磁线圈周围;而当功率逐步扩大时,发光区域发展到两边平行管体,并逐渐向椭球形管体扩散。而最终功率在大于16W之后(无论线圈匝数还是输入频率变化),发光面积覆盖整个灯管,即覆盖到了整个无极灯。而,如果功率缩减到12W以下时,发光面积骤减到只有发光线圈内部的小区域(无论线圈匝数还是输入频率变化)。It is worth mentioning that when the power of the above-mentioned light-emitting tubes increases, the light will show a tendency and characteristics of gradual diffusion. That is to say, when the luminous power is small, the luminous area mainly gathers around the excitation coil; when the power gradually increases, the luminous area develops to the parallel tubes on both sides, and gradually spreads to the ellipsoidal tube. After the final power is greater than 16W (regardless of the number of coil turns or the input frequency), the light emitting area covers the entire lamp tube, that is, the entire electrodeless lamp. However, if the power is reduced to below 12W, the light-emitting area is suddenly reduced to only a small area inside the light-emitting coil (regardless of the number of coil turns or the input frequency change).
实施例二:Embodiment two:
请合并参考图6、图7以及表2,其中表2为本实用新型应用于15W无极灯时的尺寸列表。Please refer to Figure 6, Figure 7 and Table 2 together, where Table 2 is a list of dimensions when the utility model is applied to a 15W electrodeless lamp.
表2Table 2
此时,励磁线圈200的匝数不低于10匝,且由于圆柱形管体120的长度L2限制,其最多可缠绕18匝。At this time, the number of turns of the
以10匝为例,励磁线圈200的输入频率在2.5MHz~15MHz的情况下,匹配2KV以上耐压值的一定容抗的安规电容,通过调整激励电压,发光灯管功率从5W~30W之间可任意调节。同样条件下,励磁线圈200为14匝时,发光灯管功率从5W~35W之间可任意调节。同样条件下,磁线圈200为18匝时,发光灯管功率从5W~40W之间可任意调节。Taking 10 turns as an example, when the input frequency of the
同实施例一,以上发光灯管功率增加时,发光呈现逐步扩散的趋势和特点。即发光功率小时,发光区域主要聚集在励磁线圈周围;而当功率逐步扩大时,发光区域发展到两边的平行管体,并逐渐向椭球形管体扩散。而最终功率在大于16W之后(无论线圈匝数还是输入频率变化),发光面积覆盖整个灯管,即覆盖到了整个无极灯。而,如果功率缩减到12W以下时,发光面积骤减到只有发光线圈内部的小区域(无论线圈匝数还是输入频率变化)。Same as in Embodiment 1, when the power of the above-mentioned light-emitting lamp tubes increases, the light emission presents a tendency and characteristic of gradual diffusion. That is to say, when the luminous power is small, the luminous area mainly gathers around the excitation coil; when the power gradually increases, the luminous area develops to the parallel tubes on both sides, and gradually spreads to the elliptical tube. After the final power is greater than 16W (regardless of the number of coil turns or the input frequency), the light emitting area covers the entire lamp tube, that is, the entire electrodeless lamp. However, if the power is reduced to below 12W, the light-emitting area is suddenly reduced to only a small area inside the light-emitting coil (regardless of the number of coil turns or the input frequency change).
可见,本实用新型所提供的无极灯光源,可实现光源亮度的调节,进而可根据不同领域对于光源亮度的需求,进而灵活的进行应用。It can be seen that the electrodeless light source provided by the utility model can realize the adjustment of the brightness of the light source, and can be flexibly applied according to the requirements for the brightness of the light source in different fields.
另外,可以通过荧光粉的选配,配置从2700K~6500K等不同色温发光灯管。In addition, through the selection of phosphor powder, it is possible to configure light-emitting lamps with different color temperatures from 2700K to 6500K.
实验表明,本实用新型所提供的小功率无极灯光源可保证光效达到20~40lm/W,且与传统荧光灯相比,其具有高效、故障率低、寿命长等特点。此外,实验表明,填充于灯管内的稀有气体压强为20至200Pa时,光源的寿命较长,例如,50Pa的氪气。当然本实用新型不以此为限,也可以于灯管内填充其他稀有气体,当然,也可以填充多种稀有气体构成的混合气体,甚至填充稀有气体与汞蒸气构成的混合气体。Experiments show that the low-power electrodeless light source provided by the utility model can guarantee a light effect of 20-40lm/W, and compared with traditional fluorescent lamps, it has the characteristics of high efficiency, low failure rate, and long life. In addition, experiments have shown that when the pressure of the rare gas filled in the lamp tube is 20 to 200 Pa, the life of the light source is longer, for example, 50 Pa of krypton gas. Of course, the utility model is not limited thereto, and the lamp tube can also be filled with other rare gases, of course, it can also be filled with a mixture of various rare gases, or even a mixture of rare gases and mercury vapor.
综上所述,应用以上小功率无极灯灯管,可以将励磁线圈直接缠绕于灯管之上,从而耦合电磁能量进入灯管,以激发灯管内的汞齐和稀有气体产生等离子体,等离子体的受激原子返回基态时自发辐射出紫外线,紫外线激发荧光粉发出可见光。与现有技术相比,未使用铁氧体磁芯,从而极大的减少了使用过程中的散热量,从而无需做特殊散热设计;另外,采用励磁线圈直接缠绕的方式来代替磁环,有利于其小型化的设计。To sum up, using the above low-power electrodeless lamp tube, the excitation coil can be directly wound on the lamp tube, so as to couple electromagnetic energy into the lamp tube to excite the amalgam and rare gas in the lamp tube to generate plasma. When the excited atoms of the body return to the ground state, they spontaneously emit ultraviolet rays, and the ultraviolet rays excite the phosphor to emit visible light. Compared with the existing technology, no ferrite core is used, which greatly reduces the heat dissipation during use, so that no special heat dissipation design is required; in addition, the excitation coil is directly wound instead of the magnetic ring, which has the advantages of Conducive to its miniaturized design.
进而,得到的无极灯光源是一种通过线圈直接缠绕放电管耦合电磁能量进而发光的无极荧光光源。在保证光效达到20~40lm/W的同时,与传统荧光灯相比,其未使用铁氧体磁芯,从而极大的减少了使用过程中的散热量,从而无需做特殊散热设计;另外,采用励磁线圈直接缠绕的方式来代替磁环等,有利于其小型化的设计。而小型、紧凑的外形结构可使其在各种探照照明,施工及维修照明以及民用照明等情况下具有应用价值。Furthermore, the obtained electrodeless light source is an electrodeless fluorescent light source that directly winds the discharge tube through a coil to couple electromagnetic energy and then emit light. While ensuring the light effect reaches 20-40lm/W, compared with traditional fluorescent lamps, it does not use ferrite cores, which greatly reduces the heat dissipation during use, so that no special heat dissipation design is required; in addition, The method of directly winding the excitation coil instead of the magnetic ring is beneficial to its miniaturization design. The small and compact shape structure can make it have application value in various search lighting, construction and maintenance lighting, and civil lighting.
以上仅为举例,并非用以限定本实用新型,本实用新型的保护范围应当以权利要求书所涵盖的范围为准。The above are examples only, and are not intended to limit the utility model, and the protection scope of the utility model shall be subject to the scope covered by the claims.
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