TWM451497U - Illumination led lamp with wide emission angle - Google Patents
Illumination led lamp with wide emission angle Download PDFInfo
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- TWM451497U TWM451497U TW101224496U TW101224496U TWM451497U TW M451497 U TWM451497 U TW M451497U TW 101224496 U TW101224496 U TW 101224496U TW 101224496 U TW101224496 U TW 101224496U TW M451497 U TWM451497 U TW M451497U
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本創作是關於一種以發光二極體作為光源之照明燈具,特別是指一種能形成均勻且照明光束的光強度分佈(luminous intensity distribution)角度大於135°的光型之照明燈具。The present invention relates to a lighting fixture using a light-emitting diode as a light source, and more particularly to a light-type lighting fixture capable of forming a uniform light intensity distribution with an illumination intensity distribution angle greater than 135°.
隨著科技的進步與民生經濟的發展,為人類帶來舒適而更便利的生活,而照明燈具除了在夜間提供生活上的必須光明外,也在白天上班及商業活動中居於重要的地位。在照明燈具中,白熾燈泡已為人類提供照明長達一世紀以上,傳統的白熾燈泡便宜、方便又明亮,但因為它除了發光,也會發熱,浪費了許多能量,為了節能,美國、日本和歐盟都已開始執行逐步淘汰白熾燈的計劃,其他國家也 將跟進。另外,螢光省電燈泡雖然用電量低,但消費者嫌它光束不夠柔和,而且含有少量的汞,有污染的危險,也列為下一波各國將禁用的照明燈具。相較之下,在各種照明燈具中,不含汞的LED燈具具有亮度高、體積小、省電(耗電量只有白熾燈的五分之一)、壽命長(白熾燈的二十到五十倍)的優點,為備受矚目的照明省電光源。With the advancement of science and technology and the development of the people's livelihood economy, it will bring comfort and convenience to human beings. In addition to providing the necessary light in life at night, lighting fixtures also play an important role in daytime work and business activities. In lighting fixtures, incandescent bulbs have been illuminated for more than a century. Traditional incandescent bulbs are cheap, convenient and bright, but because they emit heat, they also burn a lot of energy. In order to save energy, the United States, Japan and The EU has begun to implement plans to phase out incandescent lamps, and other countries have also Will follow up. In addition, although the fluorescent power-saving bulbs have low power consumption, consumers suspect that their beams are not soft enough, and they contain a small amount of mercury, which poses a risk of pollution and is also listed as the next wave of lighting fixtures that countries will disable. In contrast, among various lighting fixtures, mercury-free LED lamps have high brightness, small size, power saving (power consumption is only one-fifth of that of incandescent lamps), and long life (twenty-five incandescent lamps) The advantage of ten times) is the high-efficiency lighting power source.
依據美國能源之星(energy star)規範IES LM-79-80,section 10要求替換燈(replacement lamp)在0~135°區域內任一角度之光強度(luminous intensity distribution (candelas))不得低於此區域的平均光強度20%,在135~180°的區域內至少有5%的光總通量(total flux(lumens))。According to the US Energy Star specification IES LM-79-80, section 10 requires a replacement lamp to have a luminous intensity (candelas) at any angle in the range of 0 to 135°. The average light intensity in this region is 20%, and there is at least 5% total flux (lumens) in the region of 135-180°.
因此,為發展較大角度的光型以接近於美國能源之星IES LM-79-80,section 10的規範,台灣專利公開號TW201226803揭露使用入射面為方型凹孔、出射面為凹面的複合透鏡,如第10圖,複合透鏡A1應用於一個球泡燈A中,球泡燈A由LED晶片A2覆蓋上複合透鏡A1,容置於外罩A3並以E27接頭A4將電源接入,其中複合透鏡A1由中央透鏡A11、翼狀透鏡A12與環壁透鏡A13所組成,LED晶片A2容置於複合透鏡A1的環柱空間A14中心的下方,當LED晶片A2發出光束後,經由凹面的中央透鏡A11將光束向中央集中,利用環壁透鏡A13將光束分散至外圍以形成較大角度的分散,但由於光束集中在中央區域,將造成近軸區過亮而離軸區的光強度不足的缺點,且受環柱空間A14平面的入射面所影響,LED晶片A2發出的光束抵達環柱空間A14的入射面之光束入射角度較大(如0~60°),使進入環柱空間A14平面的入射面的折射角度 變小,無法使入射光束形成更大角度的分散,造成光束的分散性仍不足;更且當對於多晶片的球泡燈A,需要多個複合透鏡A1覆蓋在每一個LED晶片A2上,除影響相鄰複合透鏡A1間的光效外,其組裝不便、成本亦高,尚無法符合實用的目的。又如美國專利公開號US20110110093採用半圓形的入射面及中央為平面的出射面,雖可增大出射的角度,但仍不符合美國能源之星IES LM-79-80,section 10的規範;或如台灣專利公開號TW201121102採用出射面在近軸區為凹入尖點的光學透鏡,中國專利公開號CN201020676949.0揭露使用廣角的透鏡,在入射面採用凸面、出射面採用凹面,這二種設計係以降低中央區域(0~60°)的光強度而加強較大角度(70~80°)的光強度,但其角度仍低於光束角0~135°的規範要求;日本專利公開號JP2006-113556及美國專利US7153002係使用二個透鏡造成在透鏡中心產生一個空氣間隙,用以分配LED晶片發出的光束,以應用於LED背光上,但其主要在側方向的光束分配較多、使中央區域的光束分配較少,不適用於照明目的,且採用二個透鏡組合也增加製作成本,不利於實用化。美國專利公開號US20080151551採用入射面為凹面、出射面為平面的凹面之透鏡,將LED發出的光束進行分配,但光束分配後,其光型在中央區域(45°之內),光強度僅為最大光強度的10%,且在外圍區域光束角120°之後光強度急劇下降至最大光強度的1%,亦不符合能源之星規範的要求。Therefore, in order to develop a larger angle of light type to be close to the US Energy Star IES LM-79-80, Section 10 specification, Taiwan Patent Publication No. TW201226803 discloses the use of a composite surface having a concave surface and a concave surface. Lens, as shown in Fig. 10, the composite lens A1 is applied to a bulb A, which is covered by the LED wafer A2 to the composite lens A1, accommodated in the housing A3 and connected to the power source by the E27 connector A4, wherein the composite The lens A1 is composed of a central lens A11, a wing lens A12 and a ring wall lens A13. The LED chip A2 is accommodated under the center of the ring space A14 of the composite lens A1. After the LED chip A2 emits a light beam, the central lens is passed through the concave surface. A11 concentrates the light beam toward the center, and uses the ring wall lens A13 to disperse the light beam to the periphery to form a large angle dispersion. However, since the light beam is concentrated in the central region, the near-axis region is too bright and the light intensity of the off-axis region is insufficient. And affected by the incident surface of the ring space A14 plane, the beam emitted by the LED chip A2 reaches the incident surface of the ring space A14, and the incident angle of the beam is large (such as 0~60°), so that the plane enters the ring space A14 plane. Fold of the incident surface Angle Smaller, it is impossible to make the incident beam form a larger angle of dispersion, resulting in insufficient dispersion of the beam; moreover, for the multi-wafer bulb A, a plurality of composite lenses A1 are required to cover each LED chip A2, except In addition to affecting the light effect between adjacent composite lenses A1, the assembly is inconvenient and the cost is high, which is not satisfactory for practical purposes. For example, U.S. Patent Publication No. US20110110093 adopts a semi-circular incident surface and a plane-emitting surface, which can increase the angle of exit, but still does not meet the specifications of the US Energy Star IES LM-79-80, section 10; Or, as disclosed in Taiwan Patent Publication No. TW201121102, an optical lens having a concave apex in the paraxial region is used. Chinese Patent Publication No. CN201020676949.0 discloses the use of a wide-angle lens, a convex surface on the incident surface, and a concave surface on the exit surface. The design enhances the light intensity at a large angle (70~80°) by reducing the light intensity in the central region (0~60°), but the angle is still lower than the specification of the beam angle 0~135°; Japanese Patent Publication No. JP2006-113556 and U.S. Patent No. 7,715,002 use two lenses to create an air gap at the center of the lens for distributing the light beam emitted by the LED chip for application to the LED backlight, but the beam distribution is mainly in the lateral direction. The central region has less light beam distribution and is not suitable for illumination purposes, and the use of two lens combinations also increases the manufacturing cost, which is not conducive to practical use. U.S. Patent Publication No. US20080151551 uses a concave lens whose entrance surface is concave and whose exit surface is flat, and distributes the light beam emitted by the LED. However, after the light beam is distributed, the light pattern is in the central region (within 45°), and the light intensity is only The maximum light intensity is 10%, and the light intensity drops sharply to 1% of the maximum light intensity after the beam angle of the peripheral region is 120°, which does not meet the requirements of the ENERGY STAR specification.
在商品方面台灣隆達電子(Lextar)在2012年3月提出LED燈泡,係運用LED晶片的排列將LED燈泡達到光束 角160°以上的光型,其係使用多顆LED佈置於立體柱狀的支柱上,而非使用透鏡進行光的分配,雖經由多顆LED以不同高度與角度產生大角度的光型,但其需使用相對較多的LED,成本昂貴且組裝工序困難。In terms of commodities, Taiwan’s Lextar proposed LED bulbs in March 2012, using LED arrays to achieve LED bulbs. A light pattern with an angle of 160° or more, which uses a plurality of LEDs arranged on a three-dimensional columnar pillar instead of using a lens to distribute light, although a plurality of LEDs generate a large angle of light at different heights and angles, but It requires a relatively large number of LEDs, which is expensive and difficult to assemble.
由於LED具有低耗能的優點,應用LED構成的照明器具將可降低在照明能源的需求,但由於LED發出的光線具有方向性,與人類傳統照明需求不同,因此如何將LED發出的光線能提高光發散角度(emission angle)與光強度均勻性,以分配形成所需要的光型,為亟待解決的問題。但對於單一個LED晶片而言,LED晶片的光強度(單位為Candela)在光軸處最強,且愈遠離光軸的光強度將愈弱,因此於習知技術中,對於LED照明光源的設計上,往往藉由增加光出射面與光入射面的折射能力以減小其近軸區的光強度,並將光強度補償至遠軸區域以增加光均勻度,然而,如此一來將導致光束於光出射面發生菲涅爾反射現象,而造成光通量降低的副作用;尤其對於需要使用許多個LED晶片組成LED照明燈具的發光光源而言,更需要設計一個能控制多個LED晶片發出的光線的透鏡,讓光線能減少損失,甚至達到能源之星規範的要求,仍為業界亟待解決的課題。Due to the low energy consumption of LEDs, the use of LED lighting fixtures will reduce the need for lighting energy, but because the light emitted by LEDs is directional, unlike traditional human lighting requirements, how to increase the light emitted by LEDs The light emission angle and the light intensity uniformity are distributed to form the required light type, which is an urgent problem to be solved. However, for a single LED chip, the light intensity (in Candela) of the LED chip is the strongest at the optical axis, and the light intensity away from the optical axis will be weaker. Therefore, in the prior art, the design of the LED illumination source is In addition, the light intensity of the paraxial region is often reduced by increasing the refractive power of the light exit surface and the light incident surface, and the light intensity is compensated to the far axis region to increase the light uniformity. However, this will result in the light beam. Fresnel reflection occurs on the light exit surface, which causes side effects of reduced luminous flux; especially for an illuminating light source that requires many LED chips to form an LED lighting fixture, it is more necessary to design a light that can control the emission of multiple LED chips. Lenses, which allow light to reduce losses, even meet the requirements of the ENERGY STAR specification, remain an urgent issue for the industry.
本創作的主要目的在於提供一種具有大發光角度之LED燈具,以增加發光二極體的光利用率並可將發光二極體發出的光束控制分配,進而形成更均勻且照明光束的光強度分佈(luminous intensity distribution)角度大於135°的 光型。The main purpose of the present invention is to provide an LED luminaire with a large illuminating angle to increase the light utilization efficiency of the illuminating diode and to control the distribution of the light emitted by the illuminating diode, thereby forming a more uniform light intensity distribution of the illuminating beam. (luminous intensity distribution) angle greater than 135° Light type.
根據本創作之目的,提出一種具有大發光角度之LED燈具。該LED燈具主要包括一光源裝置與一接頭。該光源裝置包括一發光二極體元件及一光控制透鏡,該光控制透鏡設置於該發光二極體元件的一發光面之上緣;該光源裝置尚包括一電路基板,該發光二極體元件電性連結於該電路基板上。該LED燈具進一步包括一燈罩及一散熱體,該散熱體具有第一端及第二端,該第一端設置一載面,該載面供設置光源裝置,該第二端連結該接頭,該燈罩與該散熱體之第一端結合,並將光源裝置包夾於其中。該發光二極體元件可為單一發光二極體晶片或複數個發光二極體晶片之組合。According to the purpose of the present creation, an LED lamp having a large illumination angle is proposed. The LED lamp mainly comprises a light source device and a joint. The light source device includes a light emitting diode element and a light control lens disposed on an upper edge of a light emitting surface of the light emitting diode element; the light source device further includes a circuit substrate, the light emitting diode The component is electrically connected to the circuit substrate. The LED lamp further includes a lamp cover and a heat dissipating body, the heat dissipating body has a first end and a second end, the first end is provided with a carrying surface, the carrying surface is provided with a light source device, and the second end is connected to the joint, The lamp cover is coupled to the first end of the heat sink and sandwiches the light source device therein. The light emitting diode element can be a single light emitting diode chip or a combination of a plurality of light emitting diode chips.
該光控制透鏡為軸對稱且對稱於該發光二極體元件的一光軸,包括一光入射面、一光出射面與一透鏡底表面,該透鏡底表面係自該光入射面延伸出並與該光出射面相接。該透鏡底表面等角度設置複數透鏡腳,該等透鏡腳固定在該發光二極體元件周圍的一平面上,使光控制透鏡能位於該發光二極體元件的發光面上緣。該光出射面包含一出射光學面及一出射端面,該出射端面鄰接於該透鏡底表面與該出射光學面,該出射光學面為非球面或自由曲面其一。該出射光學面包含一出射光程變化點,自該發光二極體元件的該發光面中心發出的光束自光軸起算向出射端面,於該出射光程變化點開始產生全反射。該光入射面包含一入射光學面及一入射端面,該入射端面係鄰接於該透鏡底表面與該入射光學面,該入射光學面係為非球面或自由曲面其一。較佳地,該出射光學面可設計為,於光束出 射方向,在近光軸處為凸面、向該出射端面方向起算,經反曲點後轉變為凹面、再經反曲點後轉變為凸面。該入射光學面可設計為,面向光束入射方向,在近光軸處為凸面,經一個反曲點後轉變為凹面,再經至少一個反曲點後轉變為凸面。或者,入射光學面可設計為,面向光束入射方向,在近光軸處為凹面,經至少一個反曲點後轉變為凸面。The light control lens is axisymmetric and symmetrical to an optical axis of the light emitting diode element, and includes a light incident surface, a light exit surface and a lens bottom surface, the lens bottom surface extending from the light incident surface and It is connected to the light exit surface. The lens bottom surface is equiangularly provided with a plurality of lens legs fixed on a plane around the light emitting diode element so that the light control lens can be located on the light emitting surface edge of the light emitting diode element. The light exit surface includes an exit optical surface and an exit end surface adjacent to the lens bottom surface and the exit optical surface, and the exit optical surface is an aspherical surface or a free curved surface. The exiting optical surface includes an exiting optical path change point, and the light beam emitted from the center of the light emitting surface of the light emitting diode element is calculated from the optical axis to the exit end surface, and total reflection begins to occur at the exiting optical path change point. The light incident surface includes an incident optical surface and an incident end surface adjacent to the bottom surface of the lens and the incident optical surface, and the incident optical surface is an aspherical surface or a free curved surface. Preferably, the exiting optical surface can be designed to be out of the light beam The direction of the beam is convex at the near-optical axis, and starts from the direction of the exit end face. After the inflection point, it changes to a concave surface, and then passes through the inflection point and then transforms into a convex surface. The incident optical surface can be designed to face the incident direction of the light beam, be convex at the near optical axis, transform into a concave surface after an inflection point, and then transform into a convex surface after at least one inflection point. Alternatively, the incident optical surface may be designed to face the incident direction of the light beam, be concave at the near optical axis, and transform into a convex surface after at least one inflection point.
較佳地,該光控制透鏡可更滿足以下條件,使得本創作的光控制透鏡可具有適當的光束分配能力,可將該發光二極體元件發出的光束分配至更大的角度,該出射光程變化點至該發光二極體元件的發光面中心的連線與光軸間夾角為θ0
,該θ0
可介於30°至45°之間,即滿足下列條件:
另,所述LED燈具進一步包括一墊體,該墊體設置於 所述載面上,並供承載所述光源裝置,當光控制透鏡的直徑較小時,藉由該墊體增加光源裝置所在位置高度,可避免從發光二極體元件發射進入光控制透鏡入射角度較小(較接近發光面之入射光線)之光線被所述散熱體遮蔽,確保LED燈具的照明光束能達到135°。In addition, the LED lamp further includes a pad body, and the pad body is disposed on Carrying the light source device on the carrying surface, when the diameter of the light control lens is small, the position of the light source device is increased by the pad body, and the light emitted from the light emitting diode element into the light control lens can be avoided. Light with a small angle (incident light closer to the illuminating surface) is shielded by the heat sink, ensuring that the illumination beam of the LED luminaire can reach 135°.
又,所述光控制透鏡上方可設置一均光元件,該均光元件可為一擴散片,或者為具有一菲涅爾光學面(fresnel optical surface)之透鏡或者為具有一微結構光學面(micro-structure optical surface)之透鏡。In addition, a light homogenizing element may be disposed above the light control lens, and the light homogenizing element may be a diffusion sheet, or a lens having a Fresnel optical surface or having a microstructured optical surface ( Micro-structure optical surface lens.
本創作之具有大發光角度之LED燈具,具有下列優點:The LED lamp with a large illumination angle of the present invention has the following advantages:
<1>藉由本發明的式(1),其代表著LED燈具之發光面中心所發出的光束進入光入射面後在出射光程變化點會開始產生全反射,將光束控制及分配至更大的角度,且為能有較佳的光效,出射光程變化點位置可在特定的角度範圍內,使得本發明的發光二極體光控制透鏡可進一步地具有適當的光束控制及分配,以增進光源裝置的均光性。<1> By the formula (1) of the present invention, it represents that the light beam emitted from the center of the light-emitting surface of the LED lamp enters the light incident surface and starts to generate total reflection at the exiting optical path change point, and the light beam is controlled and distributed to a larger extent. Angle, and in order to have better light efficiency, the position of the exiting optical path change point can be within a specific angular range, so that the light-emitting diode light control lens of the present invention can further have appropriate beam control and distribution, Improve the uniformity of the light source device.
<2>進一步地,藉由本發明的式(2),其代表著LED燈具所發出的光束,可控制及分配至135°以上,且不低於最高光強度的30%,不但符合能源之星在0~135°區域內任一角度之光強度不得低於此區域的平均光強度20%的要求,更遠高於能源之星規範的要求。<2> Further, by the formula (2) of the present invention, it represents a light beam emitted by an LED lamp, which can be controlled and distributed to 135° or more, and not lower than 30% of the highest light intensity, not only in accordance with Energy Star. The light intensity at any angle in the 0~135° region shall not be lower than the average light intensity of 20% in this region, and is much higher than the requirements of the ENERGY STAR specification.
為使本創作更加明確詳實,茲列舉較佳實施例並配合下列圖示,將本創作之結構及其技術特徵詳述如後。In order to make the present invention more clear and detailed, the preferred embodiment and the following drawings are used to describe the structure of the present invention and its technical features as follows.
請參閱第1圖,其為本創作具有大發光角度之LED燈 具第一實施例組合示意圖。本創作具有大發光角度之LED燈具之結構主要包括有一光源裝置1及一接頭2,該光源裝置1包括一發光二極體元件11及設置在該發光二極體元件之一發光面111上緣的光控制透鏡12。該發光二極體元件11與該接頭2電性連結,該接頭2可使用E27規格的接頭用以與市電連接。其中,該發光二極體元件11是設置在一電路基板13上。基於散熱考量,該LED燈具還可包括一散熱體3,該散熱體具有第一端31及第二端32,該第一端31設置一載面311,該載面供設置光源裝置1,該第二端32連結接頭2,該散熱體3的表面可以為平滑面或如圖所示製成鰭片狀,以提升散熱效率。基於柔光及安全考量,該LED燈具還可包括一燈罩4,該燈罩4與該散熱體之第一端31結合,並將該光源裝置1包夾於其中。Please refer to Figure 1, which is an LED lamp with a large illumination angle. A schematic diagram of the combination of the first embodiment. The structure of the LED lamp having a large illumination angle mainly includes a light source device 1 and a connector 2, the light source device 1 includes a light emitting diode element 11 and an upper edge of a light emitting surface 111 disposed on the light emitting diode element The light controls the lens 12. The light-emitting diode element 11 is electrically connected to the joint 2, and the joint 2 can be connected to the mains by using an E27-type joint. The light emitting diode element 11 is disposed on a circuit substrate 13. The LED lamp may further include a heat dissipating body 3 having a first end 31 and a second end 32. The first end 31 is provided with a loading surface 311 for providing the light source device 1 . The second end 32 is connected to the joint 2, and the surface of the heat sink 3 may be a smooth surface or formed into a fin shape as shown to improve heat dissipation efficiency. Based on soft light and safety considerations, the LED lamp can further include a lamp cover 4 that is coupled to the first end 31 of the heat sink and encloses the light source device 1 therein.
當市電進入該具有大發光角度之LED燈具的E27接頭2後,在該接頭2的電路可將市電轉為該發光二極體元件11的適用電壓與電流,經由該電路基板13與該發光二極體元件11電性連接,使該發光二極體元件11發出光束並藉由該光控制透鏡12均勻控制並分配光束至大角度,由該燈罩4射出後供為照明使用;該散熱體3則可將該發光二極體元件11產生的熱能經熱傳導與熱輻射導至外界。After the mains enters the E27 connector 2 of the LED lamp having a large illumination angle, the circuit of the connector 2 can convert the commercial power into the applicable voltage and current of the LED component 11, via the circuit substrate 13 and the illumination II. The polar body element 11 is electrically connected, so that the light emitting diode element 11 emits a light beam and the light control lens 12 uniformly controls and distributes the light beam to a large angle, and is emitted by the light cover 4 for illumination; the heat sink 3 is used; Then, the thermal energy generated by the light-emitting diode element 11 can be conducted to the outside through heat conduction and heat radiation.
請參閱第2圖,其為第一實施例之光源裝置結構示意圖。該發光二極體元件11通常包含有發光二極體晶片(未於圖上繪示)及螢光黏膠層(未於圖上繪示),螢光黏膠層係覆蓋在發光二極體晶片上,當發光二極體晶片受激發而發出光線時,經由螢光黏膠層進行波長轉換,而在螢光黏膠層表面發出光束,該發出光束的表面即為該發光面111, 該發光面具有一幾何中心O點。該光控制透鏡12包括一光入射面121、一光出射面122與一透鏡底表面123,其中該透鏡底表面123係自該光入射面121延伸出並與該光出射面122相接。該光出射面122包含一出射光學面1221及一出射端面1222,該出射端面1222鄰接於該透鏡底表面123與該出射光學面1221;該出射光學面1221可使用非球面或自由曲面設計的光學面,該出射光學面1221於光束出射方向在近光軸處為凸面、向該出射端面1222方向經過至少一個反曲點P 0 後轉變為凹面,凹面的最低點為P 1 ,該出射光學面1221再經至少一個反曲點P 2 後轉變為凸面;該出射光學面1221包含有一出射光程變化點P 3 。該光入射面121包含一入射光學面1211及一入射端面1212,該入射端面1212係鄰接於該透鏡底表面123與該入射光學面1211;該入射光學面1211可使用非球面或自由曲面設計的光學面,為能最大利用入射的光束及將光束入射後的角度進行適當的分配,入射光學面的面形,可如第2圖所示,該入射光學面1211面向光束入射方向,在近光軸處為凹面,經至少一個反曲點P 4 後轉變為凸面。或者如第3圖所示,面向光束入射方向,在近光軸處為凸面,經一個反曲點P 5 後轉變為凹面,再經至少一個反曲點P 6 後轉變為凸面。該光控制透鏡12之透鏡底表面123等角度設置複數個透鏡腳124,對於不同的應用實施例,該透鏡腳124可為環狀,以利於製造。Please refer to FIG. 2, which is a schematic structural view of a light source device of the first embodiment. The LED component 11 generally includes a light-emitting diode chip (not shown) and a fluorescent adhesive layer (not shown), and the fluorescent adhesive layer covers the light-emitting diode. On the wafer, when the light emitting diode chip is excited to emit light, wavelength conversion is performed through the fluorescent adhesive layer, and a light beam is emitted on the surface of the fluorescent adhesive layer, and the surface of the emitted light beam is the light emitting surface 111. The illuminating mask has a geometric center O point. The light control lens 12 includes a light incident surface 121, a light exit surface 122 and a lens bottom surface 123. The lens bottom surface 123 extends from the light incident surface 121 and is in contact with the light exit surface 122. The light exit surface 122 includes an exit optical surface 1221 and an exit end surface 1222 adjacent to the lens bottom surface 123 and the exit optical surface 1221. The exit optical surface 1221 can use an aspheric or free-form surface design. The exiting optical surface 1221 is convex at the near optical axis in the beam exit direction, and is transformed into a concave surface after passing through at least one inflection point P 0 in the direction of the exit end surface 1222. The lowest point of the concave surface is P 1 , and the exit optical surface 1221 is further converted into a convex surface by at least one inflection point P 2 ; the outgoing optical surface 1221 includes an exit optical path change point P 3 . The light incident surface 121 includes an incident optical surface 1211 and an incident end surface 1212 adjacent to the lens bottom surface 123 and the incident optical surface 1211. The incident optical surface 1211 can be designed using an aspherical or free-form surface. The optical surface can be used to maximize the use of the incident beam and the angle at which the beam is incident, and the surface shape of the incident optical surface can be as shown in Fig. 2, the incident optical surface 1211 faces the incident direction of the beam, and the low beam The shaft is concave and transforms into a convex surface after at least one inflection point P 4 . Or, as shown in Fig. 3, facing the incident direction of the light beam, it is a convex surface at the near optical axis, and becomes a concave surface after passing through an inflection point P 5 , and then becomes a convex surface after passing through at least one inflection point P 6 . The lens bottom surface 123 of the light control lens 12 is equiangularly provided with a plurality of lens legs 124. For different application embodiments, the lens legs 124 may be annular to facilitate manufacturing.
請參閱第3圖,該光控制透鏡12與該發光二極體元件11的組合方式,可以先使該光控制透鏡12的光軸Z基本上垂直於該發光二極體元件之發光面111,並進一步大致 上使光軸Z通過該發光二極體元件11之發光面111之幾何中心O點,再將該透鏡腳124固定在該發光二極體元件11周圍的平面(電路基板13或載面311的平面)上,藉由該透鏡腳124的支撐,使該光控制透鏡12的透鏡底表面123位於該發光二極體元件的發光面111之上緣,且該透鏡底表面123所處的平面可與該發光面111所處的平面位在同一平面,或者該透鏡底表面123所處的平面可與該發光面111所處的平面間具有一間距h,該間距h有利於散熱。Referring to FIG. 3, the light control lens 12 and the LED element 11 are combined in such a manner that the optical axis Z of the light control lens 12 is substantially perpendicular to the light emitting surface 111 of the LED component. And further The optical axis Z is passed through the geometric center O of the light-emitting surface 111 of the light-emitting diode element 11, and the lens leg 124 is fixed to the plane around the light-emitting diode element 11 (the circuit board 13 or the carrier surface 311). The lens bottom surface 123 of the light control lens 12 is located at the upper edge of the light emitting surface 111 of the light emitting diode element, and the plane of the lens bottom surface 123 is The plane in which the light-emitting surface 111 is located is in the same plane, or the plane in which the lens bottom surface 123 is located may have a spacing h from the plane in which the light-emitting surface 111 is located, which is advantageous for heat dissipation.
請參閱第4圖,其為光控制透鏡相關角度符號表示圖。自該發光二極體元件的發光面111中心O發出的光束,自光軸Z起算向該出射端面1222方向,於該出射光程變化點P 3
開始產生全反射。較佳地,該光控制透鏡12可更滿足以下條件,使得本創作的光控制透鏡可具有適當的光束分配能力,可將發光二極體元件發出的光束分配至更大的角度,該出射光程變化點P 3
至該發光二極體元件的該發光面111中心O的連線與該光軸間夾角為θ 0
,較佳地該θ 0
可介於30°至45°之間,即滿足下列條件:
請參閱第6圖,為本創作具有大發光角度之LED燈具之照明光束以積分球實際測試的配光曲線示意圖。本創作
LED燈具之發光二極體元件所發出的光束,通過光控制透鏡所產生的照明光束,滿足下列條件:
請參閱第7圖,其為本創作具有大發光角度之LED燈具第二實施例組合示意圖。對於不同應用目的,該發光二極體元件11可為單一個發光二極體或可為複數個發光二極體所組成,當發光二極體元件由複數個發光二極體所組成時,該發光二極體元件11之發光面111係由各該發光二極體的發光面111及其間隙所組合而成。第8圖中表現採用多個發光二極體構成該發光二極體元件11作為光源,該等發光二極體可沿光源裝置的中心軸對稱設置或大致平均位置所設置,該光控制透鏡12則涵蓋該等發光二極體元件11。對於不限定的實施方式,該發光二極體元件11也可由多個發光二極體以COB(Chip On Board)封裝製程所製造成單一顆的發光二極體元件11。透過該光控制透鏡12,能達到增加發光二極體的光利用率並可將發光二極體發出的光束控制分配,進而形成更均勻的光強度分佈(luminous intensity distribution)且照明光束在135°的光強度滿足至少為I max 的30%光型之目的。Please refer to FIG. 7 , which is a schematic diagram of a second embodiment of an LED lamp with a large illumination angle. For different application purposes, the LED component 11 can be a single LED or can be composed of a plurality of LEDs. When the LED component is composed of a plurality of LEDs, the LED component is composed of a plurality of LEDs. The light-emitting surface 111 of the light-emitting diode element 11 is formed by combining the light-emitting surfaces 111 of the light-emitting diodes and their gaps. In the eighth embodiment, the light-emitting diode elements 11 are formed as a light source by using a plurality of light-emitting diodes, and the light-emitting diodes can be disposed symmetrically or substantially at an average position along a central axis of the light source device. The light control lens 12 is disposed. These light emitting diode elements 11 are then covered. For a non-limiting embodiment, the light-emitting diode element 11 can also be fabricated as a single light-emitting diode element 11 by a COB (Chip On Board) packaging process using a plurality of light-emitting diodes. Through the light control lens 12, the light utilization efficiency of the light emitting diode can be increased and the light beam emitted by the light emitting diode can be controlled and distributed, thereby forming a more uniform light intensity distribution and the illumination beam is at 135°. The light intensity satisfies the purpose of at least a 30% light pattern of I max .
請參閱第8圖,其為本創作具有大發光角度之LED燈具第三實施例組合示意圖。主要表現,於該散熱體3的載 面311上增設一具適當高度之墊體5。當該光控制透鏡12的直徑較小時,藉由該墊體5增加光源裝置所在位置高度,可避免從該發光二極體元件11發射進入該光控制透鏡12入射角度較小(較接近發光面之入射光線)之光線射出該光控制透鏡12後的照明光束被該散熱體3遮蔽,確保LED燈具的照明光束能達到135°。Please refer to FIG. 8 , which is a schematic diagram of a third embodiment of an LED lamp with a large illumination angle. Main performance, the load of the heat sink 3 A pad 5 of a suitable height is added to the surface 311. When the diameter of the light control lens 12 is small, the height of the position of the light source device is increased by the pad body 5, and the incident angle of the light control lens 12 from the light emitting diode element 11 can be prevented from being smaller (closer to the light). The illumination beam emitted by the light incident on the light control lens 12 is shielded by the heat sink 3, ensuring that the illumination beam of the LED lamp can reach 135°.
請參閱第9圖,其為本創作具有大發光角度之LED燈具第四實施例組合示意圖。為均光目的,於該光控制透鏡12上方設置一均光元件6。該均光元件6設置的方式可為黏合或者可於該均光元件6及該光控制透鏡12之間設置接合結構(圖未示),利用接合結構可將該均光元件6固定在該光控制透鏡12上方。其中,該均光元件6可為一擴散片,或者為具有一菲涅爾光學面(fresnel optical surface)之透鏡(圖未示)或者為具有一微結構光學面(micro-structure optical surface)之透鏡(圖未示)。所述均光元件可以塑膠或壓克力材質製成。Please refer to FIG. 9 , which is a schematic diagram of a fourth embodiment of an LED lamp with a large illumination angle. For the purpose of uniform light, a light homogenizing element 6 is disposed above the light control lens 12. The light-collecting element 6 can be disposed in a manner of bonding or can be disposed between the light-homogenizing element 6 and the light-controlling lens 12 (not shown). The light-storing element 6 can be fixed to the light by the bonding structure. Above the control lens 12. Wherein, the light homogenizing element 6 can be a diffusion sheet, or a lens having a Fresnel optical surface (not shown) or having a micro-structure optical surface. Lens (not shown). The light homogenizing element can be made of plastic or acrylic material.
本創作LED燈具之該光控制透鏡12可將發光二極體元件發出的光束,經由該光控制透鏡12的光入射面121入射且出射於該光出射面122,形成以光軸為中心且照明光束大於135°,並在135°時的光強度分佈提高至最大光強度的30%以上,以超越能源之星對於發光二極體球泡燈的規範要求。The light control lens 12 of the LED lamp of the present invention can inject a light beam emitted from the light emitting diode element through the light incident surface 121 of the light control lens 12 and exit the light exit surface 122 to form an illumination centered on the light axis. The beam is greater than 135° and the light intensity distribution at 135° is increased to more than 30% of the maximum light intensity to exceed ENERGY STAR specifications for LED bulbs.
以上所示僅為本創作之優選實施例,對本創作而言僅是說明性的,而非限制性的。本技術領域具通常知識人員理解,在本創作權利要求所限定的精神和範圍內可對其進行許多改變、修改、甚至等效變更,但都將落入本創作的 權利範圍內。The above description is only the preferred embodiment of the present invention, and is merely illustrative and not limiting. It will be apparent to those skilled in the art that many changes, modifications, and equivalent changes may be made in the spirit and scope of the present invention as defined by the appended claims. Within the scope of rights.
1‧‧‧光源裝置1‧‧‧Light source device
2‧‧‧接頭2‧‧‧Connectors
11‧‧‧發光二極體元件11‧‧‧Lighting diode components
111‧‧‧發光面111‧‧‧Lighting surface
12‧‧‧光控制透鏡12‧‧‧Light control lens
121‧‧‧光入射面121‧‧‧Light incident surface
1211‧‧‧入射光學面1211‧‧‧Injecting optical surface
1212‧‧‧入射端面1212‧‧‧ incident end face
122‧‧‧光出射面122‧‧‧Light exit surface
1221‧‧‧出射光學面1221‧‧‧Out of the optical surface
1222‧‧‧出射端面1222‧‧‧ exit end face
123‧‧‧透鏡底表面123‧‧‧ lens bottom surface
124‧‧‧透鏡腳124‧‧‧Lens feet
13‧‧‧電路基板13‧‧‧ circuit substrate
3‧‧‧散熱體3‧‧‧ Heat sink
31‧‧‧第一端31‧‧‧ first end
311‧‧‧載面311‧‧‧Sales
32‧‧‧第二端32‧‧‧second end
4‧‧‧燈罩4‧‧‧shade
5‧‧‧墊體5‧‧‧ cushion body
6‧‧‧均光元件6‧‧‧Homogeneous components
P 1 ‧‧‧凹面的最低點為The lowest point of the concave surface of P 1 ‧ ‧ is
P 2 ‧‧‧反曲點 P 2 ‧ ‧ recurve
P 3 ‧‧‧出射光程變化點 P 3 ‧‧‧Outset optical path change point
P 4 ‧‧‧反曲點 P 4 ‧ ‧ recurve
P 5 ‧‧‧反曲點 P 5 ‧ ‧ recurve
P 6 ‧‧‧反曲點 P 6 ‧ ‧ recurve
O‧‧‧發光面中心O‧‧‧Lighting surface center
H‧‧‧光軸上發光面中心至透鏡底表面之間的距離H‧‧‧Distance between the center of the light-emitting surface on the optical axis and the bottom surface of the lens
Z‧‧‧光軸Z‧‧‧ optical axis
θ 0 ‧‧‧出射光程變化點至發光面中心的連線與光軸間的夾角 θ 0 ‧‧‧An angle between the line connecting the optical path change point to the center of the light-emitting surface and the optical axis
I 135 ° ‧‧‧光源裝置在與光軸夾角為135°時,在相對無限遠 處的光強度 I 135 ° ‧‧‧Light intensity at a relatively infinity when the light source is at an angle of 135° to the optical axis
I max ‧‧‧光源裝置在與光軸任一夾角處,在相對無限遠處的任一點光強度的最高值 I max ‧‧‧The highest value of light intensity at any point relative to infinity at any angle with the optical axis
A‧‧‧球泡燈A‧‧‧Bub Light
A1‧‧‧複合透鏡A1‧‧‧ compound lens
A2‧‧‧LED晶片A2‧‧‧LED chip
A3‧‧‧外罩A3‧‧‧ outer cover
A4‧‧‧E27接頭A4‧‧‧E27 connector
A11‧‧‧中央透鏡A11‧‧‧ central lens
A12‧‧‧翼狀透鏡A12‧‧‧ wing lens
A13‧‧‧環壁透鏡A13‧‧‧Ring lens
A14‧‧‧環柱空間A14‧‧‧ Ring Space
第1圖為該第一實施例之LED燈具組合示意圖;第2圖為該第一實施例之光源裝置結構示意圖;第3圖為該第一實施例所延伸之另一實施例的光源裝置結構示意圖;第4圖為本創作光控制透鏡之相關角度符號表示圖;第5圖為本創作第一實施例之LED燈具發光示意圖;第6圖為本創作具有大發光角度之LED燈具之照明光束以積分球實際測試的配光曲線示意圖;第7圖為本創作具有大發光角度之LED燈具第二實施例組合示意圖;第8圖為本創作具有大發光角度之LED燈具第三實施例組合示意圖;第9圖為本創作具有大發光角度之LED燈具第四實施例組合示意圖;及第10圖為習知球泡燈結構示意圖。1 is a schematic view showing the combination of the LED lamp of the first embodiment; FIG. 2 is a schematic structural view of the light source device of the first embodiment; and FIG. 3 is a structure of the light source device according to another embodiment of the first embodiment. FIG. 4 is a schematic diagram showing the relative angle of the light control lens of the present invention; FIG. 5 is a schematic diagram of the illumination of the LED lamp of the first embodiment; FIG. 6 is an illumination beam of the LED lamp having a large illumination angle. Schematic diagram of the light distribution curve actually tested by the integrating sphere; FIG. 7 is a schematic diagram of the second embodiment of the LED lamp with a large illumination angle; FIG. 8 is a schematic diagram of the third embodiment of the LED lamp with a large illumination angle. Fig. 9 is a schematic view showing the combination of the fourth embodiment of the LED lamp having a large illumination angle; and Fig. 10 is a schematic view showing the structure of the conventional bulb lamp.
1‧‧‧光源裝置1‧‧‧Light source device
11‧‧‧發光二極體元件11‧‧‧Lighting diode components
111‧‧‧發光面111‧‧‧Lighting surface
12‧‧‧光控制透鏡12‧‧‧Light control lens
124‧‧‧透鏡腳124‧‧‧Lens feet
13‧‧‧電路基板13‧‧‧ circuit substrate
2‧‧‧接頭2‧‧‧Connectors
3‧‧‧散熱體3‧‧‧ Heat sink
31‧‧‧第一端31‧‧‧ first end
311‧‧‧載面311‧‧‧Sales
32‧‧‧第二端32‧‧‧second end
4‧‧‧燈罩4‧‧‧shade
Claims (13)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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TW101224496U TWM451497U (en) | 2012-12-18 | 2012-12-18 | Illumination led lamp with wide emission angle |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW101224496U TWM451497U (en) | 2012-12-18 | 2012-12-18 | Illumination led lamp with wide emission angle |
Publications (1)
Publication Number | Publication Date |
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TWM451497U true TWM451497U (en) | 2013-04-21 |
Family
ID=48801807
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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TW101224496U TWM451497U (en) | 2012-12-18 | 2012-12-18 | Illumination led lamp with wide emission angle |
Country Status (1)
Country | Link |
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TW (1) | TWM451497U (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105465627A (en) * | 2015-12-30 | 2016-04-06 | 欧普照明股份有限公司 | Light beam control device and light-emitting device |
TWI581011B (en) * | 2016-03-11 | 2017-05-01 | Optical lens | |
CN106949404A (en) * | 2017-04-25 | 2017-07-14 | 北京小米移动软件有限公司 | Night-light |
CN111981429A (en) * | 2020-08-06 | 2020-11-24 | 珠海市正远光电科技有限公司 | LED car lamp module |
-
2012
- 2012-12-18 TW TW101224496U patent/TWM451497U/en not_active IP Right Cessation
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105465627A (en) * | 2015-12-30 | 2016-04-06 | 欧普照明股份有限公司 | Light beam control device and light-emitting device |
CN105465627B (en) * | 2015-12-30 | 2024-03-22 | 欧普照明股份有限公司 | Beam control device and light emitting device |
TWI581011B (en) * | 2016-03-11 | 2017-05-01 | Optical lens | |
CN106949404A (en) * | 2017-04-25 | 2017-07-14 | 北京小米移动软件有限公司 | Night-light |
CN111981429A (en) * | 2020-08-06 | 2020-11-24 | 珠海市正远光电科技有限公司 | LED car lamp module |
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