TWM345357U - Aspherical LED angular lens for central distribution patterns and LED assembly using the same - Google Patents

Aspherical LED angular lens for central distribution patterns and LED assembly using the same Download PDF

Info

Publication number
TWM345357U
TWM345357U TW97211645U TW97211645U TWM345357U TW M345357 U TWM345357 U TW M345357U TW 97211645 U TW97211645 U TW 97211645U TW 97211645 U TW97211645 U TW 97211645U TW M345357 U TWM345357 U TW M345357U
Authority
TW
Taiwan
Prior art keywords
optical
light
optical lens
lens
led
Prior art date
Application number
TW97211645U
Other languages
Chinese (zh)
Inventor
Bo-Yuan Shih
Kai-Mou Lin
Yi-Fan Liao
Original Assignee
E Pin Optical Industry Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by E Pin Optical Industry Co Ltd filed Critical E Pin Optical Industry Co Ltd
Priority to TW97211645U priority Critical patent/TWM345357U/en
Priority to JP2008006407U priority patent/JP3148803U/en
Publication of TWM345357U publication Critical patent/TWM345357U/en

Links

Landscapes

  • Lenses (AREA)
  • Led Device Packages (AREA)

Description

M345357 八、新型說明: 【新型所屬之技術領域】 本創作係有關一種非球面正照角發光二極體光學鏡片及其所 構成的發光二極體崎,尤指—觀用料四發絲產生光型之 光學鏡片,與所構成的發光三極體組件,而可供單顆或組成咖 陣列之照明使用。 【先前技術】 發光二極體LED具有低電壓、低耗電、壽命長的優點,已大 量應用於顯示(indicator)、照明(illuminator)等領域。然而由於led 晶片發出的光線為點光源、亮度不均勻的特性,對於光線的聚集 已有研究學者進行多項研究,如縮小晶片、提高發光效率外,使 用光學鏡片也是重要的技術開發方向。 在LED光學鏡片的設計上,可分為一次光學鏡片(primaiy optical lens)及二次光學鏡片(secondary 〇ptical lens); 一次光學鏡片 為在LED晶片上直接封裝的透鏡,一般以聚集(c〇ncentrate)光線為 主;二次光學鏡片為使用在單顆或數顆LED陣列(Array),以分散 光束為主。在習知技藝的一次光學鏡片設計上,如ES2157829使 用對稱的非球面透鏡、日本專利jP3〇32〇69、JP2002-111068、 JP2005-203499,美國專利 US2006/187653、中國專利 CN101013193 專使用球面透鏡、JP2002-221658對Bulk型之LED使用球面透鏡 等。對於高階的運用上,一次光學鏡片除要能聚集光線外,更能 在均勻的光強度(peak intensity)產生特定的光型(distribution pattern),例如大角度、小角度、圓形、橢圓形等特殊光型,以搭 配LED陣列使用,以產生最佳的光學效果。一次光學鏡片的運用 5 M345357 如圖1所示,在LED晶片21上覆有一透鏡23,當LED晶片21 發出光線,經由透鏡23聚集後發出預定的光型光線。此一次光學 鏡片在習知技藝上,如日本專利jp2〇〇4-356512、JP2005-229082、 JP2006_072874、JP2007-140524、JP2007-115708 等;美國專利 US2005/162854 > US2006/105485 、 US2006/076568 、 US2007/114551、US2007/152231、US7,344,902、US7,345,416、 US7,352,011 ;台灣專利TW M332796等使用光學鏡片以產生光 型;再如日本專利jP6〇〇〇7425、美國專利WO/2007/100837產生 橢圓光型等;或如中國專利200710118965.0產生小於160度之矩 形、正方形或條狀光型等。 隨著科技的進步,電子產品不斷地朝向輕薄短小以及多功能 的方向發展,而電子產品中如:數位相機(Digital Still Camera)、電 月自相機(PC camera)、網路相機(Network camera)、行動電話(手機) 等已具備鏡頭之外,甚至個人數位辅助器(PDA)等裝置也有加上鏡 頭的需求,因此用於這類產品的LED閃光燈或照明用的LED燈 具,常以單顆或多顆LED組件組成陣列;而為了攜帶方便及符合 人性化的需求’LED閃光燈或照明用的led燈具不僅需要符合的 光通里,以不同光型LED組件互相搭配,同時也需要有較小的體 積與車父低的成本。在LED —次光學鏡片的需求上,習知複雜外型 或具有繞射面的光學鏡片存有製造困難、塑膠射出變形、玻璃成 型不易或成本咼等缺點。因此,使用簡單外型、易於製造的發光 二極體鏡片設計與組成,可對LED發出的親轉並產生光強度 (peak intensity)為大於72。小於。之正照角圓形光型所形成的 LED組件,且光通量比值大於_的要求,為使用者迫切的需求。 【新型内容】 6 M345357 本創作主要目的乃在於提供一種非球面正照角發光二極體光 學鏡片,以應用於LED組件上。此LED組件係由一發光二極體 晶片(LED die)以發出光線、一光學鏡片以聚集光線並以均勻光強 度形成大於72°小於108°之正照角圓形光型、於光學鏡片與發光 二極體間係以封膠(sealgel)所填塞構成。其中,光學鏡片為一具有 凹面及凸面的光學材料所製成的鏡片,其凹面為向光源的光源侧 光學面,其凸面為向像侧的像側光學面,且凹面及凸面至少有一 光學面為非球面’並可滿足以下條件: 及1 一及2 <1.0 0.7 < ⑴ 8< <180 (2) (3) 0.2 <(iV,2-1)^1 <0.4 J s 其中’ fs為本光學鏡片之有效焦距(effeetive f〇cai iei^h)之長 度、R1為光源侧光學面之曲率半徑、R2為像侧光學面之曲率半 徑、d2為中心軸光學鏡片厚度、Nd2為光學鏡片的折射率。 為簡化製造,光學鏡片可更換為為一具有平凸型的光學鏡 片,其平面為向光源的光源侧光學面,其凸面為向像 學面,其像侧光學面為非球面;可滿足式⑶及式(4)條件:^ ⑶ (4) °·2^ -1)^-<0.4 J s r2 α·ζ 其中,R2為像側光學面之曲率半徑、d〇為中心軸上led晶 片厚度dl為中心軸上LED晶片表面至光學鏡片光源侧光學面距 7 M345357 離、d2為中心轴光學鏡片厚度。 本創作另一目的,為使用選擇方便,光學鏡片可為光學玻璃 或光學塑膠所製成。 本創作之又一目的在於提供一種發光二極體組件,其係包含 如本創作所述之非球面寬照角發光二極體光學鏡片及一發光二極 體晶片,其特徵在於此發光二極體組件具有大於72。小於1〇8。之 正照角圓形光型、其光通量比值大於85% (Α/α285%)的要求,並滿 • 足以下條件: μ 5< ω •φ π (5) 其中, ⑹ 其中’fs為本光學鏡片之有效焦距(effective focal length)之長 度、fg為本光學鏡片之相當焦距(relative f〇cal length)之長度、 R1為光测絲φ之曲率伟、R2為賴光學面之解半徑、2 ω為LED晶片發出光線財心軸對稱的最大角度、μ為經由光 學鏡片射出光線財心軸對稱的最大角度、α為咖晶片發出光 線的光通量、/3為像側相對無限遠處(励倍fs)光線的光通量。 藉此,本創作之非球面正照角發光二極體光學鏡片及其所 成的發光二極體組件可具有大於72。小於。之正照角圓形 f,且符合光通量比值大於85%的要求,並且該絲鏡片具有簡 早的形狀、厚度薄’胁製造’可將單顆LED或_ LED,^ 供予照明使用。 攸 8 M345357 【實施方式】 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 式,將本創作之結構及技術特徵詳述如後: 參照圖2所示,其係本創作之非球面正照角發光二極體光學 鏡片及其所構成的發光二極體組件於LED組件1〇之結構示意 圖,其沿著中心軸z排列由光源至像侧依序為:一 LED晶片^、 一封膠12及一光學鏡片13,當光線由LED晶片u發出後,經由 •封膠12後,由光學鏡片13將光線聚集並形成以對稱於中心軸z 之大於72小於1〇8。之正照角圓形光型的光束對像侧照射;光學 鏡片13為一具有凹面及凸面的光學材料所製成的鏡片,其凹面為 向光源的光源侧光學面R1,其凸面為向像侧的像侧光學面幻,且 凹面及凸面之至少一者之光學面為非球面;光學鏡片13之光學面 R1與R2及有效焦距長度間滿足式⑴、式⑺及式⑶之條件,咖 晶片11發射的角度2ω與光學鏡片13所形成的光強度形成的光 型之角度20滿足式(5)之條件。 _ 參照圖4所示,其係本創作之使用平凸型光學鏡片於led組 ,件之不意圖,其沿著中心軸z排列由光源至像侧依序為:一 led 晶片U、一封膠12及一平凸型光學鏡片14。光線由LED晶片u 發出後,經由封膠12後,由光學鏡片14將光線聚集並形成以對 稱於中心軸Z之大於72。小於繼。之正照賴形光型的光束對像 侧照射;光學鏡Η為-由光學材料所製成的鏡片,其平面為向 光源的光_光學φ R1,其凸面為向像綱賴光學面们,光學 面幻為非球面;光學鏡片14之光學面R1與R2及有效焦距長度 間滿足式⑶及式⑷之條件,LED晶片η發射的角度b與光$ 9 M345357 鏡片13所形成的光強度形成的光型之角度2 0滿足式(5)之條件。 請參閱圖2及圖4’光學鏡片13之光學面R1與R2或光學鏡 片14之光學面R2,若以非球面光學面所構成,其非球面之方程 式(Aspherical Surface Formula)為式(7) z = ch2 + AAhA + A6h6 + A%h% + 4〇/210 ⑺ 其中,c是曲率,h為鏡片高度,K為圓錐係數(Conic Constant)、M345357 VIII. New description: [New technical field] This is a kind of aspherical positive-angle LED light-emitting diode and its light-emitting diode, especially the four-wire light. The optical lens of the type, and the formed light-emitting diode assembly, can be used for illumination of a single or composed coffee array. [Prior Art] A light-emitting diode LED has advantages of low voltage, low power consumption, and long life, and has been widely used in fields such as an indicator and an illuminator. However, since the light emitted by the LED chip is a point light source and the brightness is not uniform, many researches have been conducted on the accumulation of light, such as reducing the wafer and improving the luminous efficiency, and the use of the optical lens is also an important technical development direction. In the design of the LED optical lens, it can be divided into a primary optical lens (primaiy optical lens) and a secondary optical lens (secondary optical lens); the primary optical lens is a lens directly packaged on the LED chip, generally gathered (c〇 Ncentrate) is based on light; secondary optics are used in single or several LED arrays, with a dispersion of light. In the optical lens design of the prior art, for example, the symmetrical aspherical lens is used in the ES2157829, the Japanese patents jP3〇32〇69, JP2002-111068, JP2005-203499, the US patent US2006/187653, the Chinese patent CN101013193 exclusively use a spherical lens, JP 2002-221658 uses a spherical lens or the like for a Bulk type LED. For high-order applications, in addition to being able to concentrate light, an optical lens can produce a specific distribution pattern at a uniform peak intensity, such as a large angle, a small angle, a circle, an ellipse, etc. Special light type for use with LED arrays to produce the best optical results. Application of Primary Optical Lens 5 M345357 As shown in FIG. 1, a lens 23 is coated on the LED chip 21, and when the LED chip 21 emits light, it is collected via the lens 23 to emit a predetermined light-type light. The optical lens of this time is in the prior art, such as Japanese Patent No. JP-A-4-356512, JP2005-229082, JP2006-072874, JP2007-140524, JP2007-115708, etc.; US Patent No. 2005/162854 > US2006/105485, US2006/076568, US2007/114551, US2007/152231, US7,344,902, US7,345,416, US7,352,011; Taiwan patent TW M332796, etc. use optical lenses to produce a light type; and as a Japanese patent jP6〇〇〇7425, US patent WO/2007/100837 An elliptical light type or the like is produced; or a rectangular, square or strip light type of less than 160 degrees is produced as in Chinese Patent No. 200710118965.0. With the advancement of technology, electronic products are constantly moving toward light, short, and versatile, such as digital still cameras, PC cameras, and network cameras. In addition to the lens, mobile phones (mobile phones), etc., even personal digital assistants (PDAs) and other devices have the need for lenses, so LED flashlights for LED lighting or lighting used in such products are often single. Or a plurality of LED components are formed into an array; and for the convenience of carrying and ergonomic requirements, the LED lamps for LED flash or lighting need not only meet the optical communication, but also match different light-type LED components, and also need to have smaller The volume is low with the cost of the car father. In the demand for LED-sub-optical lenses, conventional optical lenses having a complicated outer shape or having a diffraction surface have disadvantages such as difficulty in manufacturing, deformation of plastic injection, difficulty in forming glass, or cost. Thus, the design and composition of a light-emitting diode lens that is simple in shape and easy to manufacture can be used to produce an inversion of the LED and produce a peak intensity of greater than 72. Less than. The LED component formed by the circular light type of the positive angle has a luminous flux ratio greater than the requirement of _, which is an urgent requirement of the user. [New content] 6 M345357 The main purpose of this creation is to provide an aspherical positive-angle light-emitting diode optical lens for use in LED components. The LED component is composed of a light emitting diode chip (LED die) to emit light, an optical lens to collect light and form a positive angle circular light shape of more than 72° and less than 108° with uniform light intensity, and is used for optical lens and illumination. The inter-polar body is composed of a sealant. Wherein, the optical lens is a lens made of an optical material having a concave surface and a convex surface, wherein the concave surface is a light source side optical surface toward the light source, the convex surface is an image side optical surface toward the image side, and the concave surface and the convex surface have at least one optical surface. It is aspherical and can satisfy the following conditions: and 1 and 2 <1.0 0.7 < (1) 8<<180 (2) (3) 0.2 <(iV,2-1)^1 <0.4 J s Where 'fs is the length of the effective focal length of the optical lens (effeetive f〇cai iei^h), R1 is the radius of curvature of the optical surface of the light source side, R2 is the radius of curvature of the optical side of the image side, and d2 is the thickness of the optical lens of the central axis, Nd2 is the refractive index of the optical lens. In order to simplify the manufacture, the optical lens can be replaced by an optical lens having a plano-convex shape, the plane of which is a light source side optical surface toward the light source, the convex surface is an image-like surface, and the image-side optical surface is aspherical; (3) and (4) Conditions: ^ (3) (4) °·2^ -1)^-<0.4 J s r2 α·ζ where R2 is the radius of curvature of the image side optical surface, d〇 is the central axis of the led The wafer thickness dl is from the surface of the LED wafer on the central axis to the optical surface of the optical lens, and the optical surface distance is 7 M345357, and d2 is the thickness of the central axis optical lens. Another purpose of this creation is that it is convenient to use and the optical lens can be made of optical glass or optical plastic. A further object of the present invention is to provide a light-emitting diode assembly comprising the aspherical wide-angle light-emitting diode optical lens and a light-emitting diode wafer as described in the present invention, wherein the light-emitting diode is characterized in that The polar body assembly has a greater than 72. Less than 1〇8. The positive angle of the circular light type, the luminous flux ratio is greater than 85% (Α / α285%), and full • sufficient conditions: μ 5 < ω • φ π (5) where, (6) where 'fs is the optical lens The length of the effective focal length, fg is the length of the relative focal length of the optical lens, R1 is the curvature of the optical measuring wire φ, R2 is the radius of solution of the optical surface, 2 ω For the LED chip, the maximum angle of the axis of the ray is symmetrical, μ is the maximum angle of the axis of symmetry of the light emitted through the optical lens, α is the luminous flux of the ray of the coffee chip, and /3 is the relative infinity of the image side (excitation fs The luminous flux of light. Thereby, the aspherical positive-angle light-emitting diode optical lens of the present invention and the resulting light-emitting diode assembly thereof can have more than 72. Less than. The positive angle is rounded f and meets the requirement of a luminous flux ratio greater than 85%, and the silk lens has a simple shape and a thin thickness. The single LED or _LED, can be used for illumination.攸8 M345357 [Embodiment] In order to make the creation more clear and detailed, the preferred embodiment and the following drawings are used to describe the structure and technical features of the creation as follows: Referring to Figure 2, the author The aspherical positive-angle light-emitting diode optical lens and the light-emitting diode assembly thereof are arranged in the LED assembly 1 , and arranged along the central axis z from the light source to the image side in sequence: an LED wafer ^ , a glue 12 and an optical lens 13 , after the light is emitted from the LED chip u, after passing through the sealant 12 , the light is collected by the optical lens 13 and formed to be greater than 72 and less than 1 对称 8 symmetrical to the central axis z. The light beam of the circular light type is irradiated to the image side; the optical lens 13 is a lens made of an optical material having a concave surface and a convex surface, and the concave surface is a light source side optical surface R1 toward the light source, and the convex surface is the image side The image side optical surface is illusory, and the optical surface of at least one of the concave surface and the convex surface is aspherical; the optical surface R1 and R2 of the optical lens 13 and the effective focal length length satisfy the conditions of the formulas (1), (7) and (3), The angle 20 of the light pattern formed by the angle 2ω of the emission and the light intensity formed by the optical lens 13 satisfies the condition of the formula (5). _ Referring to FIG. 4, it is the use of the plano-convex optical lens in the LED group, which is not intended, and is arranged along the central axis z from the light source to the image side in order: a led wafer U, a The glue 12 and a plano-convex optical lens 14. After the light is emitted from the LED chip u, after passing through the sealant 12, the light is collected by the optical lens 14 and formed to be more than 72 symmetrical to the central axis Z. Less than the following. The light beam is irradiated to the image side of the light beam; the optical mirror is a lens made of an optical material whose plane is the light _ optical φ R1 toward the light source, and the convex surface is the optical surface of the image. The optical surface is aspherical; the optical surface R1 and R2 of the optical lens 14 and the effective focal length satisfy the conditions of the formulas (3) and (4), and the angle b emitted by the LED wafer η and the light intensity formed by the light lens 9 13 are formed. The angle of the light type 2 0 satisfies the condition of the formula (5). Please refer to FIG. 2 and FIG. 4 'the optical surfaces R1 and R2 of the optical lens 13 or the optical surface R2 of the optical lens 14 . If the aspherical optical surface is formed, the Aspherical Surface Formula is the equation (7). z = ch2 + AAhA + A6h6 + A%h% + 4〇/210 (7) where c is the curvature, h is the lens height, and K is the conic coefficient (Conic Constant),

A*、Αό、As、A1()分別四、六、八、十階的非球面係數(Nth〇rder Aspherical Coefficient)。 5月參閱圖3 ’為本創作LED光學鏡片於LED組件之光路示意 圖,圖中,LED晶片11發出光線的最大角度為2ω(以中心轴z對 稱)’經由光學鏡片13聚集並折射後以2ψ角度(以中心軸ζ對稱) 形成所需要的光型及/?/〇^7〇%的要求,其中,α為LED晶片發出 光線的光通量、β為像側相對無限遠處(1〇〇倍fs)光線的光通量, 且忽略空氣的折射(refraction)與散射(scattering)等效應。再者,該 ,光學鏡片13可以光學玻璃或以光學塑膠所製成。 〜 參關5所示,為本創作制平凸猶球面正照紐光二極 ‘體光學鏡片及其所構成的發光二極體組件之光路示意圖,LED晶 片11發出光線的最大角度為2ω(以中心軸z對稱),經由光學鏡 片Η聚集並折射後以20角度(以中心軸z對稱)形成所需要的光 型及__的要求,其中,α為咖晶片發出光線的光通量、 /5為像侧相對無限遠處⑽倍fs)光線的光通量,且忽略空氣 的折射(refraction)與散射(越ering)等效應。再者,該光學鏡片14 可以光學玻璃或以光學塑膠所製成。 藉上述結構’本創作球面賴角發光二極體光學鏡片及其所 M345357 構成的發光二極體組件可符合大於72。小於1〇8°之正照角圓形光 型,使LED組件10可發出預定的光型,且符合光通量比值大於 85% β/α285%)的要求,可為單顆使用或以不同光型組成陣列使 用。 為說明本創作實際應用的實施例,以LED晶片11使用 1.0x1.0mm尺寸的晶片、光學鏡片13(或光學鏡片14)使用直徑5mm 為說明,以利於比較各實施例的應用情形;然而,LED晶片11尺 寸與光學鏡片13(或光學鏡片14)直徑,並非如以上述尺寸所限。 以下於第一實施例至第四實施例係使用具有凹面及凸面的光 學鏡片所構成的發光二極體組件、第五實施例至第八實施例係使 用平凸型的光學鏡片所構成的發光二極體組件。 <第一實施例> 請參考圖2及圖6所示,其分別係本創作之使用led光學鏡 片之LED組件示意圖及第一實施例之光強度分佈與照角之極座標 關係圖。 下列表(一)中分別列有由光源侧至像侧沿中心軸Z之LED 晶片11、封膠12、光學鏡片13之光源侧光學面]^與像侧光學面 R2 之曲率半徑 R (單位:mm) (the radius 0f curvature r)、間距 d (單位:mm) (the on-axis surface spacing),LED 晶片 11 發出光 線的最大角度為2ω(度deg)、光學鏡片13發出光線光型之最大角 度20(度deg),各折射率(Nd)各厚度(thickness)、各阿貝數 (Abbe, s number) v d ° 表(一) 11 M345357 2ω= ΐ3〇 2ψ= 92A*, Αό, As, and A1() have four, six, eight, and tenth order aspheric coefficients (Nth〇rder Aspherical Coefficient). Referring to FIG. 3 in May, a schematic diagram of the optical path of the LED optical lens for the LED component is shown. In the figure, the maximum angle of the LED chip 11 emitting light is 2ω (symmetric with the central axis z) 'aggregated by the optical lens 13 and refracted by 2ψ The angle (symmetric with the central axis) forms the required light pattern and /?/〇^7〇%, where α is the luminous flux of the LED chip, and β is the image side relatively infinity (1〇〇) Fs) the luminous flux of light, and ignoring the effects of air refraction and scattering. Furthermore, the optical lens 13 can be made of optical glass or optical plastic. ~ As shown in Figure 5, this is a schematic diagram of the light path of the illuminating and convex illuminating lens of the illuminating illuminating lens and the illuminating diode assembly. The maximum angle of the LED chip 11 is 2ω (to the center) The axis z is symmetrical, and is concentrated and refracted via the optical lens 以 to form a desired light pattern and __ at a 20 angle (symmetric with the central axis z), wherein α is the luminous flux of the coffee wafer, and /5 is the image. The side is at least infinity (10) times fs) the luminous flux of the light, and ignores the effects of air refraction and scattering (ering). Furthermore, the optical lens 14 can be made of optical glass or optical plastic. By the above structure, the present spherical spherical light-emitting diode optical lens and the light-emitting diode assembly thereof constituted by M345357 can satisfy more than 72. The circular light pattern of less than 1〇8° enables the LED assembly 10 to emit a predetermined light pattern and meets the requirement of a luminous flux ratio greater than 85% β/α285%), and can be used for single use or with different light types. The array is used. To illustrate the practical application of the present invention, the use of a 1.0 x 1.0 mm wafer, an optical lens 13 (or an optical lens 14) of the LED wafer 11 using a diameter of 5 mm is used to facilitate comparison of the application of the embodiments; however, The size of the LED wafer 11 and the diameter of the optical lens 13 (or optical lens 14) are not limited as described above. Hereinafter, in the first to fourth embodiments, the light-emitting diode assembly using the concave and convex optical lenses, and the fifth to eighth embodiments are formed using the plano-convex optical lenses. Diode assembly. <First Embodiment> Referring to Fig. 2 and Fig. 6, respectively, it is a schematic diagram of an LED component using a led optical lens of the present invention and a polar coordinate relationship between the light intensity distribution and the illumination angle of the first embodiment. In the following list (1), the radius of curvature R of the LED chip 11, the sealant 12, the light source side optical surface of the optical lens 13 and the image side optical surface R2 from the light source side to the image side along the central axis Z are respectively listed. :mm) (the radius 0f curvature r), the distance d (unit: mm) (the on-axis surface spacing), the maximum angle at which the LED wafer 11 emits light is 2ω (degree deg), and the optical lens 13 emits a light pattern. Maximum angle 20 (degree deg), each refractive index (Nd) thickness, each Abbe number (sbe) s number vd ° Table (1) 11 M345357 2ω = ΐ3〇2ψ = 92

0.100 m 0.430 70.000 23〇〇 2.4000.100 m 0.430 70.000 23〇〇 2.400

光源 矽膠 R1 R2Light source Silicone R1 R2

㈡各光學面之非 下列表(2) Non-optical surfaces

• 本實知例中,封膠12係利用折射率Ndl為1·527、阿貝數> dl 、為34的透明光學石夕膠所填塞;光學鏡片13侧用折射率難為 U83、阿貝數^d2為61·7的玻璃材質製成。藉由搭配封膠η及 光學鏡片13之折射係數與阿貝數,形成光線折射角度。LED晶片 11發出α =12.15流明的藍光、有效的最大角度為130。,光學鏡片 • 13的有效焦距之長度fs為4.20 mm;經由此光學鏡片13聚集後, 以92。正照角於無限遠處(以丨〇〇倍為計)之々=11 ·〇92流明c忽略 空氣的折射與散射等效應);式(1)、(2)、(3)、(5)及式⑹分別為·· 3·尖·Λ 一• In the present embodiment, the sealant 12 is filled with a transparent optical fiber which has a refractive index Nd1 of 1.527, an Abbe number > dl, and 34; the refractive index of the optical lens 13 is difficult to be U83, Abbe The number ^d2 is made of glass material of 61·7. The light refraction angle is formed by matching the refractive index of the sealant η and the optical lens 13 with the Abbe number. The LED chip 11 emits blue light with α = 12.15 lumens, and the effective maximum angle is 130. , optical lens • The effective focal length of 13 has a length fs of 4.20 mm; after this optical lens 13 is gathered, it is 92. The positive angle is at infinity (in 丨〇〇 times) 々 = 11 · 〇 92 lumens c ignores the effects of air refraction and scattering); formula (1), (2), (3), (5) And (6) are respectively ··················

(〜-1),= J s 0.9337 169.0802 0.3192 1.750 12 M345357(~-1), = J s 0.9337 169.0802 0.3192 1.750 12 M345357

β! a = 10.5839 91.29% 可γ滿足餅式⑴、(2)、⑶及式(5)。圖3為led 光線,經過封膠12及學鏡片13之光路圖示意圖,圖6為== 施例之LED組件光強度分佈與照肖之極座標_圖。由上述表 (一)、表(二)及圖6所示’藉此可證明本創作之非球面正昭^ 發光二極縣學鏡片及其所構成的發光二極體組件具有簡單的面 形,易於製造且有預定的光型,其各角度之絲度均— 本創作之應用性。 幵 <第二實施例> 0月參考圖2一及圖7所示,其分別係本創作之使用LE〇光學鏡 片於LED組件tf之意圖及第—實細之光強度分佈無角之極座 標關係圖。 下列表(三)中分別列有由光源侧至像側沿中心轴z之各光 學面曲率半徑R、間距d,LED晶片U發出光線的最大角度為如、 光學鏡片I3發出光線光型之最大角度2Ψ,各折射率⑽、各阿 貝數Vd。表(四)為各光學面之非球面式⑺之各項係數。 13 M345357 表(三)β! a = 10.5839 91.29% γ can satisfy the formulas (1), (2), (3) and (5). FIG. 3 is a schematic diagram of the light path of the LED light passing through the sealant 12 and the lens 13 , and FIG. 6 is a light coordinate distribution of the LED component of the embodiment of FIG. From the above table (1), Table (2) and FIG. 6 , it can be proved that the aspherical surface of the present invention and the light-emitting diode assembly formed by the present invention have a simple surface shape. It is easy to manufacture and has a predetermined light pattern, and the angle of each angle is the applicability of this creation.幵<Second Embodiment> 0 refers to FIG. 2 and FIG. 7 respectively, which are respectively the intention of using the LE〇 optical lens in the LED component tf and the light intensity distribution of the first solid Polar coordinate diagram. In the following list (3), the radius of curvature R and the spacing d of each optical surface from the light source side to the image side along the central axis z are respectively listed, and the maximum angle of the light emitted by the LED wafer U is as large as that of the optical lens I3. Angle 2Ψ, each refractive index (10), each Abbe number Vd. Table (4) shows the coefficients of the aspherical type (7) of each optical surface. 13 M345357 Table (3)

表(四)Table (4)

• 本實施例中,封膠12係利用折射率Ndl為1·527、阿貝數Vdl 為34的透明光學矽膠所填塞;光學鏡片13係利用折射率N也為 1.583、阿貝數々2為61.7的玻璃材質製成。LED晶片η發出α=1215 流明的藍光、有效的最大角度為130°,光學鏡片13的有效焦距之 長度fs為5.66 mm ;經由此光學鏡片13聚集後,以92。正照角於 • 無限遠處(以1〇〇倍fs為計)之β=11·57流明(忽略空氣的折射與散 射等效應);式(1)、(2)、(3)、(5)及式⑹分別為: ϋ = 0.7410 -Al_= 9.0579 〇·2676 M345357• In the present embodiment, the sealant 12 is filled with a transparent optical silicone having a refractive index Ndl of 1.527 and an Abbe number Vdl of 34; the optical lens 13 is also made of a refractive index N of 1.583 and an Abbe number 々2. Made of 61.7 glass. The LED wafer η emits blue light with α = 1215 lumens, the effective maximum angle is 130°, and the effective focal length of the optical lens 13 has a length fs of 5.66 mm; after the optical lens 13 is collected, it is 92. The positive angle is at the infinity (in 1 〇〇 fs) β = 11.57 lumens (ignoring the effects of air refraction and scattering); equations (1), (2), (3), (5 And equation (6) are: ϋ = 0.7410 -Al_= 9.0579 〇·2676 M345357

β I cc = 5.4518 95.22% 二條件⑴、(2)、⑶及式(5) ’圖7為第二實施例之LED組 件光強度分佈與照角之極座標_圖。由μ表卜>、表 =7所示,藉此可證明本創作之非球面正照角發光二極縣學 =片及,、所構成的發光二極體組件具有簡單的面形,祕製造且 有預定的紐’其各肖度之錢度均―,可提昇本創作之應用性。 <第三實施例> 請參考圖2及圖8所示,其分別係本創作之使用led光學鏡 片於LED_之示意鼠第三魏狀光賊分佈無角之極座 標關係圖。 下列表(五)中分別列有由光源側至像侧沿中心軸2之各光 學面曲率伟R、_d,LED晶片„發出絲的最大肖度為仏、 光學鏡片13發出光線光型之最大角度20,各折射率⑽)、各 厚度(thiCkneSS)、各阿貝數Μ。表(六)為各光學面之非球面式 (7)之各項係數。 表(五)β I cc = 5.4518 95.22% Two conditions (1), (2), (3) and (5) ′ Fig. 7 is a diagram showing the light intensity distribution of the LED component of the second embodiment and the polar coordinates of the illumination angle. It is shown by the μ table and the table=7, which proves that the aspherical positive-angle illumination of the creation is a piece of light, and the light-emitting diode assembly has a simple surface shape. And there is a predetermined New Zealand's "the degree of money", which can enhance the applicability of this creation. <Third Embodiment> Referring to Fig. 2 and Fig. 8, respectively, it is a polar coordinate relationship between the use of the led optical lens and the LED of the present invention. In the following table (5), the curvatures of the respective optical surfaces from the light source side to the image side along the central axis 2 are respectively listed as R, _d, and the maximum diametry of the LED wafer „ is 仏, and the optical lens 13 emits the largest light pattern. Angle 20, each refractive index (10)), each thickness (thiCkneSS), and each Abbe number Μ. Table (6) is the coefficient of the aspherical surface (7) of each optical surface. Table (5)

#非球面 15 M345357 表(六) K A4 A6 A8 A10 *R1 *R2 3.0000Ε-01 -L0000E+00 -1.0000E - 04 -3.0000E-02 O.OOOOE+OO 1.3079E-02 0.0000E+00 -1.4006E-04 0.0000E+00 -1.9145E-04 本實施例中,封膠12係利用折射率Ndl為ΐ·527、阿貝數Vdl 為34的透明光學矽膠所填塞;光學鏡片13係利用折射率Nd2為 1.583、阿貝數^為61·7的玻璃材質製成。LED晶片^發出^厶^ 流明的藍光、有效的最大角度為11〇。,光學鏡片13的有效焦距之 長度fs為4·20 mm ;經由此光學鏡片13聚集後,以91。正照角於 無限遠處(以100倍fs為計)之β=11·277流明(忽略空氣的折射與散 射等效應);式⑴、(2)、(3)、(5)及式⑹分別為··#非球面15 M345357 表(六) K A4 A6 A8 A10 *R1 *R2 3.0000Ε-01 -L0000E+00 -1.0000E - 04 -3.0000E-02 O.OOOOE+OO 1.3079E-02 0.0000E+00 - 1.4006E-04 0.0000E+00 -1.9145E-04 In this embodiment, the sealant 12 is filled with a transparent optical silicone having a refractive index Ndl of ΐ·527 and an Abbe number Vdl of 34; the optical lens 13 is refracted. It is made of a glass material having a Nd2 of 1.583 and an Abbe number of 61.7. The LED chip emits a blue light with a lumen, and the effective maximum angle is 11 〇. The effective focal length of the optical lens 13 has a length fs of 4·20 mm; after passing through the optical lens 13, it is 91. The positive angle is β=11·277 lumens at infinity (in terms of 100 times fs) (ignoring the effects of refraction and scattering of air); equations (1), (2), (3), (5), and (6) are respectively for··

及1+及2 尽2 3·^-Λ Λ ω — φ π Λ β! a 0.9337 169.0802 0.3191 1.7501 5.2919 91.82% 可以滿足條件⑴、(2)、⑶及式⑶,圖8為本創作之第三實施例之 LED組件光強度分佈與照肖之極座標關細。由上述表(一)、表 (二)及_ 8所示,藉此可證明本創作之非球面正照角發光二極 16 M345357 =二Γ簡單的面形,易於製造且有預定的光型,其各角 度之先賊均-,可提昇糊叙應用性。 <第四實施例> Η於:=2及圖9所7^,其分別係本創作之使社ED光學鏡 _及細實_之錢度分佈無角之極座 標關係圖。 - 下列表_(七)中分別列有由光源側至像側沿中心轴Z之各光 :面曲率半徑R、間距d,LED晶片i i發出光線的最大角度為Μ、 光學鏡片13發出光線光型之最大角度20,各折射率⑽)、各 厚度(thickness)、各阿賊vd。表⑷為各光學面之非球面式 (7)之各項係數。 表(七) ζω= :120 2ψ= =92 編號 光學面 曲率丰徑 厚度 Nd Vd 0 光源 0.100 1 矽膠 0.430 1.527 34 2 R1 37.635 1.850 1.530 57 *3 R2 2.400 。1 4 像側 *非球面 表(八)And 1+ and 2 2 2·^-Λ Λ ω — φ π Λ β! a 0.9337 169.0802 0.3191 1.7501 5.2919 91.82% The conditions (1), (2), (3) and (3) can be satisfied, and Figure 8 is the third of the creation. The light intensity distribution of the LED component of the embodiment is close to the polar coordinate of the illumination. From the above table (1), Table (2) and _ 8, it can be proved that the aspherical positive-angled light-emitting diode of the present invention 16 M345357 = two-dimensional simple surface shape, easy to manufacture and has a predetermined light pattern, The thief of all angles - can improve the application of the paste. <Fourth Embodiment> The following is a description of the polar coordinate relationship between the ED optical mirror _ and the fine _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ - In the following list _ (seven), the light from the light source side to the image side along the central axis Z is respectively listed: the radius of curvature R of the surface, the spacing d, the maximum angle at which the LED wafer ii emits light is Μ, and the optical lens 13 emits light. The maximum angle of the type 20, each refractive index (10)), each thickness (thickness), each thief vd. Table (4) shows the coefficients of the aspherical type (7) of each optical surface. Table (7) ζω= :120 2ψ= =92 No. Optical surface Curvature diameter Thickness Nd Vd 0 Light source 0.100 1 Silicone 0.430 1.527 34 2 R1 37.635 1.850 1.530 57 *3 R2 2.400. 1 4 image side * aspheric surface table (eight)

本實施例中,封膠12係利用折射率Ndl為1527、阿貝數 為34的透明光學石夕膠所填塞·,光學鏡片13係利用折射率!^2為 1.530、阿貝數vd2為57的塑膠材質製成。LED晶片u發^ α=12·15流明的藍光、有效的最大角度為120。,光學鏡片13的有 17 M345357 效焦距之長度fs為4.30 mm ;經由此光學鏡片聚集後,以92。 正照角於無限遠處(以100倍fs為計)之/5=11.741流明(忽略空氣 的折射與散射等效應);式(1)、(2)、(3)、(5)及式(6)分別為: ϋ = W 3·尖·Λ — (义2 -1)夺= J sIn the present embodiment, the sealant 12 is filled with a transparent optical ray enamel having a refractive index Ndl of 1527 and an Abbe number of 34, and the optical lens 13 is made of a refractive index! ^2 is made of 1.530, and the Abbe number vd2 is 57. The LED chip has a blue light of α=12·15 lumens, and the effective maximum angle is 120. The length Ls of the optical lens 13 having a focal length of 17 M345357 is 4.30 mm; after gathering through the optical lens, it is 92. The positive angle is at infinity (in terms of 100 times fs) /5=11.741 lumens (ignoring the effects of air refraction and scattering); equations (1), (2), (3), (5), and 6) They are: ϋ = W 3·尖·Λ — (义 2 -1) 夺 = J s

(d)_人 Λ =(d) _ person Λ =

•Λ= β I cc = 0.8801 59.3053 0.2278 1.7931 7.9905 96.63% 可以滿足條件(1)、(2)、(3)及式(5),圖9為光強度分佈與照角之極 座標關係圖。由上述表(一)、表(二)及圖9所示,藉此可證明 本創作之非球面正照角發光二極體光學鏡片及其所構成的發光二 極體組件具有簡單的面形,易於製造且有預定的光型,其各角度 之光強度均一,可提昇本創作之應用性。 <第五實施例> π參考圖4及圖1〇所示,其分別係本創作之使用平凸型 光學鏡片於LED組件光路示意圖及第五實施例之光強度 昭 角之極座標關係圖。 ^/、… 下歹〗表(九)中分別列有由光源側至像侧沿中心軸z之led 曰曰片U、封膠12、光學鏡片14之光源侧光學面R1與像側光學面 M345357 R2之曲率半徑r (單位:mm)、間距d (單位:㈣,咖晶片 Π發出光線的最大角度為h(度deg)、光學鏡片w發出光線光型 之最大角度冰度deg) ’各折射率⑽、各厚度脚咖㈣、各 阿貝數yd。表⑴為各光學面之非球面式⑺之各項係數: 表(九) 2ω= 120 2ψ= 90 _編號 光學面 曲率半徑 厚度 Nd Vd 0 光源 0.100 1 矽膠 0.330 1.527 34 2 R1 〇〇 2.800 1.583 61.7 *3 R2 2.975 4 像侧 *非球面 --- 在表(九)中,光學面(Surf)有標註*者為非球面光學面。 表(十)• Λ = β I cc = 0.8801 59.3053 0.2278 1.7931 7.9905 96.63% The conditions (1), (2), (3) and (5) can be satisfied. Figure 9 is a plot of the relationship between the light intensity distribution and the angle of illumination. From the above table (1), Table (2) and FIG. 9, it can be proved that the aspherical positive-angle light-emitting diode optical lens of the present invention and the light-emitting diode assembly thereof have a simple surface shape. It is easy to manufacture and has a predetermined light type, and its light intensity at each angle is uniform, which can enhance the applicability of the creation. <Fifth Embodiment> π Referring to FIG. 4 and FIG. 1A, which are schematic diagrams of the optical path of the LED assembly using the plano-convex optical lens and the polar coordinate relationship of the fifth embodiment. . The light source side optical surface R1 and the image side optical surface of the led film U, the sealant 12, and the optical lens 14 from the light source side to the image side along the central axis z are respectively listed in the table (9). M345357 R2 radius of curvature r (unit: mm), spacing d (unit: (four), the maximum angle of light emitted by the coffee chip h is h (degree deg), the maximum angle of the optical lens w emits light glaze deg) Refractive index (10), each thickness of the feet (four), each Abbe number yd. Table (1) is the coefficient of the aspherical type (7) of each optical surface: Table (9) 2ω=120 2ψ= 90 _Number optical surface curvature radius thickness Nd Vd 0 Light source 0.100 1 Silicone 0.330 1.527 34 2 R1 〇〇2.800 1.583 61.7 *3 R2 2.975 4 Image side*Aspherical surface--- In Table (9), the optical surface (Surf) is marked with an aspherical optical surface. Table (10)

本實施例中,封膠12係利用折射率Ndl為1527、阿貝數Vdi 為34的透明光學矽膠所填塞;光學鏡片14係利用折射率Nd2為 1.583、阿貝數vd2為61.7的玻璃材質製成。藉由搭配封膠12及光 學鏡片14之折射係數與阿貝數’形成光線折射角度。led晶片 11發出α=12·15流明的藍光、有效的最大角度為12〇。,光學鏡片 14的有效焦距之長度色為5.091 mm;經由此光學鏡片14聚集後, M345357 以90。正照角於無限遠處(以100倍fs為計)之β=11·668流明(忽略 空氣的折射與散射等效應);式(3)、(4)、(5)及式(6)分別為: 1.7112 1.0852 1.7112 8.1705 96.03% (^2-1)1 = fs (d〇 ^dx +d2) (0 — ωIn the present embodiment, the sealant 12 is filled with a transparent optical silicone having a refractive index Ndl of 1527 and an Abbe number Vdi of 34; the optical lens 14 is made of a glass material having a refractive index Nd2 of 1.583 and an Abbe number of vd2 of 61.7. to make. The light refraction angle is formed by matching the refractive index of the sealant 12 and the optical lens 14 with the Abbe number. The led chip 11 emits blue light with α=12·15 lumens, and the effective maximum angle is 12 〇. The effective focal length of the optical lens 14 has a length of 5.091 mm; after the optical lens 14 is collected, the M345357 is at 90. The positive angle is β=11·668 lumens at infinity (in terms of 100 times fs) (ignoring the effects of refraction and scattering of air); equations (3), (4), (5), and (6) are respectively For: 1.7112 1.0852 1.7112 8.1705 96.03% (^2-1)1 = fs (d〇^dx +d2) (0 — ω

β! a- 可以滿足條件式⑶、(4)及式(5)。圖10為光強度分佈與照角之極 座標關係圖。由上述表(一)、表(二)及圖10所示,藉此可證 明本創作之非球面正照角發光二極體光學鏡片及其所構成的發光 二極體組件具有簡單的面形,易於製造且有預定的光型,其各角 度之光強度均一,可提昇本創作之應用性。 <第六實施例> 凊參考圖4及圖η所示,其分別係本創作使用平凸型光學鏡 片於LED組件之示意圖及第六實施例之光強度分佈與照角之極座 標關係圖。 下列表(十一)中分別列有由光源侧至像侧沿中心軸Z之LED 晶片n、封膠12、光學鏡片14之光源侧光學面Rl與像侧光學面 R2之曲率半徑R、間距d,LED晶片U發出光_最大角度為如、 光學鏡片14發出光線光型之最大角度2ψ,各折射率(%)、各阿 20 M345357 貝數vd。表(十二) 表(十一)β! a- can satisfy the conditional expressions (3), (4) and (5). Figure 10 is a graph showing the relationship between the light intensity distribution and the angle of the illumination. From the above-mentioned Table (1), Table (2) and FIG. 10, it can be proved that the aspherical positive-angle LED light-emitting lens of the present invention and the LED assembly thereof have a simple surface shape. It is easy to manufacture and has a predetermined light type, and its light intensity at each angle is uniform, which can enhance the applicability of the creation. <Sixth Embodiment> Referring to FIG. 4 and FIG. 7 , respectively, the schematic diagram of the relationship between the light intensity distribution and the illumination angle of the sixth embodiment using the plano-convex optical lens in the LED assembly is shown. . In the following list (11), the radius of curvature R and the pitch of the light source side optical surface R1 and the image side optical surface R2 of the LED wafer n, the sealant 12, and the optical lens 14 from the light source side to the image side are respectively listed. d, the LED wafer U emits light _ maximum angle is, for example, the maximum angle 2 ψ of the optical lens 14 emits light, each refractive index (%), each 20 M345357 number of vd. Table (12) Table (11)

4各光學Φ之非球面式⑺之各項係數·4 The coefficients of the aspherical type (7) of each optical Φ·

表(十二)Table (12)

m ΛΑ^例中’封膠12係利用折射率蘭為1·527、阿貝數^dl 1、如、、&目月*光學石夕膠所填塞;光學鏡片14係利用折射率Nd2為 " 為61·7的玻璃材質製成。藉由搭配封膠12及In the case of m ΛΑ^, the sealant 12 system is filled with a refractive index of 1.527, an Abbe number ^dl 1, a ray, and an optical lens, which is filled with a refractive index Nd2. " Made of glass material of 61·7. By matching the sealant 12 and

“子鏡片14之折射係數與阿錄,形成滅折射角度。LED晶片 11發出78·5流明的白光、有效的最大減為m。,光學鏡片 的有效焦距之長度色為5.091 mm;經由此光學鏡片14聚集後, 以9〇正照角於無限遠處(以100倍fs為計)之/3=74.5流明(忽略空 氣的折射與散射等效應);式(3)、(4)、(5)及式(6)分別為: ^d2 = J s (^o + rfj + d 2) i— 0.3205 1.0857 1.7111 21 M345357"The refractive index of the sub-lens 14 and the A-recorded lens form an extinction angle. The LED wafer 11 emits 78. 5 lumens of white light, and the effective maximum is reduced to m. The effective focal length of the optical lens is 5.091 mm; After the lens 14 is gathered, the angle of 9 〇 is at infinity (in terms of 100 times fs) / 3 = 74.5 lumens (ignoring the effects of refraction and scattering of air); formulas (3), (4), (5) And equation (6) are: ^d2 = J s (^o + rfj + d 2) i—0.3205 1.0857 1.7111 21 M345357

8.1705 94.92% - 可以滿足條件式(3)、(4)及式(5)。圖11為光強度分佈與照角之極 •座標關係圖。由上述表(-)、表(二)及圖11所示,藉此可證 明本創作之非球面正照角發光二極體光學鏡片及其所構成的發光 一極,組件具有簡單的面形,易於製造且有預定的光型,其各角 修度之光強度均-,可提昇本創作之應用性。 <第七實施例> 請參考圖4及圖12所示,其分別係本創作之使用平凸型led •光學鏡片於LED組件之示意圖及第七實施例之光強度分佈鱼昭角 • 之極座標關係圖。 冉 下列表(十三)中分別列有由光源侧至像侧沿中心軸z之LED 晶片11、封膠12、光學鏡片14之光源侧光學面幻愈 • R2之曲率半徑R、間距d,LED晶片出光線的最大角^ 2ω、光學鏡片14發出光線光型之最大角度20,各折射率^)、 各厚度(thichkness)、各阿貝數^ d。表(十四)為各光學面 域 面式(7)之各項係數: 22 M345357 表(十三)8.1705 94.92% - Conditional formulas (3), (4), and (5) can be satisfied. Figure 11 is a diagram showing the relationship between the light intensity distribution and the illumination angle. From the above table (-), Table (2) and FIG. 11, the aspherical positive-angle light-emitting diode optical lens of the present invention and the light-emitting pole formed thereby can be proved, and the assembly has a simple surface shape. It is easy to manufacture and has a predetermined light pattern, and the intensity of light at each corner is improved, which can enhance the applicability of the creation. <Seventh Embodiment> Referring to FIG. 4 and FIG. 12, which are respectively used in the present invention, a plano-convex type LED is used. The optical lens is shown in the schematic view of the LED module and the light intensity distribution of the seventh embodiment is shown in FIG. The polar coordinate diagram. In the following list (13), the light source side of the LED chip 11, the sealant 12, and the optical lens 14 from the light source side to the image side along the central axis z respectively, the curvature radius R, the distance d of the R2, The maximum angle of the light emitted by the LED wafer is 2 2ω, and the maximum angle 20 of the light pattern of the optical lens 14 is obtained, and each refractive index ^), each thickness (thichkness), and each Abbe number ^ d. Table (14) is the respective coefficients of the surface area (7): 22 M345357 Table (13)

1 矽膠 0.430 1.527 34 2 R1 ⑺ 2.600 1.530 57 *3 R2 2.975 — 4 像側____ *非球面 --^ _ 表(十四)1 Silicone 0.430 1.527 34 2 R1 (7) 2.600 1.530 57 *3 R2 2.975 — 4 Image side ____ *Aspherical surface --^ _ Table (fourteen)

. 本實施例中,封膠U係利用折射率麵為b27、阿貝數⑽ 為34的透明光學石夕騎填塞;光學鏡片14係利用折射率丽為 1.530、阿貝數2;犯為57的塑膠材質製成。藉由搭配封膠及^ 學鏡片14之折射係數與阿貝數,形成光線折射角度。LED晶片 Φ 11發出0==12.15流明的藍光、有效的最大角度為120。,光學鏡片 14的有效焦距之長度fs為5.091 mm;經由此光學鏡片14聚集後, 以90。正照角於無限遠處(以1〇〇倍fs為計)之沒=11·74流明(忽略 空氣的折射與散射等效應);式(3)、(4)、(5)及式(6)分別為: (Nd2—x^: 0.2707 fs (^0 + c/j + ) 1.0521 及2 一 1.7111 23 M345357In this embodiment, the sealant U is made of a transparent optical stone with a refractive index of b27 and an Abbe number of (10) of 34; the optical lens 14 has a refractive index of 1.530 and an Abbe number of 2; Made of plastic material. The angle of refraction of the light is formed by matching the refractive index of the encapsulant and the lens 14 with the Abbe number. The LED chip Φ 11 emits blue light with 0 = 12.15 lumens, and the effective maximum angle is 120. The effective focal length of the optical lens 14 has a length fs of 5.091 mm; after passing through the optical lens 14, it is 90. The positive angle is at infinity (in terms of 1〇〇 fs), not =11·74 lumens (ignoring the effects of air refraction and scattering); equations (3), (4), (5), and (6) ) are: (Nd2—x^: 0.2707 fs (^0 + c/j + ) 1.0521 and 2 a 1.7111 23 M345357

β I a = 7.8982 96.90% 可以滿足條件式(3)、⑷及式(5) 座標關係㈠、表強度分佈與照角之極 明本創作之非球面正照角發光^^二斤:接藉此可證 二極簡單的面形,易於:造==成= 度之光強度均-,可提昇本_之應祕。 ,、各角 <第八實施例> 請參考圖4及圖I3所示’其分別係本創作使用平凸型㈣ 光學鏡片於LED組件之示意圖及第人實施例之光強 之極座標關係圖。 下列表(十五)中分別列有由光源侧至像侧沿中心轴z之㈣ 晶片11、封膠12、光學鏡片14之光源侧光學㈣丨與像侧光學面 R2之曲率半徑R、間距d,LED晶片u發出光線的最大角度為 2ω、光學鏡片14發出光線光型之最大角度20,各折射率(Nd)、 各阿貝數yd。表(十六)為各光學面之非球面式⑺之各項係數: 表(十五) 2ω= 130 2ψ= =92 編號 光學面 曲率半徑 厚度 Nd Vd 0 光源 0.100 1 矽膠 0.430 1.527 34 2 R1 〇〇 2.600 1.583 61.7 *3 R2 2.975 4 像側 *非球面 — 24 M345357 表(十六) K A4 A6 A8 A10 *R2 4.0000E-01 5.0000E-03 -1.0000E-03 3.0000E-04 -6.3827E-07 本實施例中,封膠12係利用折射率Ndl為1.527、阿貝數udl 為34的透明光學矽膠所填塞;光學鏡片14係利用折射率Nd2為 1.583、阿貝數2; d2為61.7的玻璃材質製成。藉由搭配封膠12及 光學鏡片14之折射係數與阿貝數,形成光線折射角度。LED晶片 11發出α=12·15流明的藍光'有效的最大角度為130°,光學鏡片 14的有效焦距之長度fs為5.091 mm;經由此光學鏡片14聚集後, 以92。正照角於無限遠處(以100倍fs為計)之冷=11.51流明(忽略 空氣的折射與散射等效應);式(3)、(4)、(5)及式(6)分別為: -1)仝= fs 0.2976 ⑷+ d\ +d2) 1.0521 及2 一 Λ == = 1.7112 φ 10.3493 β ! a - 94.70% 座標關係圖。式()°圖為度/刀佈與照角之極 明本創作之= ㈠、表(二)及圖12所示,藉此可證 邦球面正照角發光二極體光學鏡片及其所構成的發光 25 M345357 .产:::::有簡單的面形,易於製造且有預定的光型,其各角 度之先強度均-,可提昇本創作之應用性。 w 述’本創作之非球面正照肖發光二極體光I鏡片及其 • 娜*+^光二極敎件之功效在於其具有鮮的面形,可利用 、形或杈造玻璃等製程所大量生產製造而不容易變形, • 降低生產成本。其中,絲鏡片亦可使用平凸型非球面光 學鏡片以簡化製造流程。 _ 摘作之非麵賴角發光二極體光學偏及其所構成的發 I一極體組件之另—功效,因可使從LED晶片所投射之光源能具 有一預定之光型,而可適用於照明。 • 本創作之非球面正照角發光二極體光學鏡片及其所構成的發 各ί極體ί件之又一功效在於其使從LED晶片所投射之光源能於 度均能維持均勻之照明強度,使成像面不會有部份區域過亮 或過暗之現象發生,因而能提升照明品質。 _ 以上所示僅為本創作實施例,對本創作而言僅是說明性的, 非限制性的。本專業技術人員理解,在本創作權利要求所限定 老精神和範圍内可對其進行許多改變、修改、甚至等效變更,但 15將落入本創作的權利範圍内。 26 M345357 【圖式簡單說明】 圖1係習知之使用led光學鏡片於led組件之示意圖; 圖2係本創作之使用LED光學鏡片於LED組件之示意圖; 圖3係本創作之led光學鏡片於LED組件光路示意圖; 圖4係本創作之使用平凸型Lm)光學鏡片於LED組件之示意圖; 圖5係本創作之使用平凸型光學鏡片於組件光路示意 S3 · 團, 圖6係本創作之第一實施例之LED組件光強度分佈與照角之極座 標關係圖; 圖7係本創作之第二實施例之LED組件光強度分佈與照角之極座 標關係圖; 圖8係本創作之第三實施例之LED組件光強度分佈與照角之極座 標關係圖; 圖9係本創作之第四實施例之LED組件光強度分佈與照角之極座 標關係圖; 圖10係本創作之第五實施例之LED組件光強度分佈與照角之極 座標關係圖; 圖U係本創作之第六實施例之LED組件光強度分佈與照角之極 座標關係圖; 圖12係本創作之第七實施例之LED組件光強度分佈與照角之極 座標關係圖;以及 圖13係本創作之第八實施例之LED組件光強度分佈與照角之極 27 M345357 座標關係圖。 【主要元件符號說明】 10 : LED 組件; 11、21 : LED 晶片; 12 :封膠; 13 :光學鏡片; 14 :光學鏡片; 23 :透鏡; • R1 :光源侧光學面或其曲率半徑; R2 :像侧光學面或其曲率半徑; d0 :中心軸上LED晶片厚度; dl :中心軸上LED晶片表面至光學鏡片光源侧之光學面距離; ' d2 :中心軸光學鏡片厚度; . co:LED晶片發出光線的最大角度的一半; Ψ:光學鏡片發出光型之最大角度的一半;β I a = 7.8982 96.90% Can satisfy the conditional formulas (3), (4) and (5) Coordinate relationship (1), the intensity distribution of the table and the illumination angle. The aspherical positive illumination of the creation is ^^2 kg: It can be proved that the two-pole simple surface shape is easy: the light intensity of the ==== degree is -, which can improve the secret of this _. , each corner <eighth embodiment> Please refer to FIG. 4 and FIG. 13 for the schematic diagram of the use of the plano-convex (four) optical lens on the LED component and the polar coordinate relationship of the first embodiment. Figure. In the following table (fifteen), the radius of curvature R, the distance between the light source side optical (four) 丨 and the image side optical surface R2 of the wafer 11, the sealant 12, and the optical lens 14 from the light source side to the image side along the central axis z are respectively listed. d, the maximum angle at which the LED chip u emits light is 2ω, the maximum angle 20 of the light pattern emitted by the optical lens 14, the refractive index (Nd), and the Abbe number yd. Table (16) is the coefficient of the aspherical type (7) of each optical surface: Table (fifteen) 2ω= 130 2ψ= =92 No. Optical surface curvature radius Thickness Nd Vd 0 Light source 0.100 1 Silicone 0.430 1.527 34 2 R1 〇 〇 2.600 1.583 61.7 *3 R2 2.975 4 Image side * aspherical surface - 24 M345357 Table (16) K A4 A6 A8 A10 *R2 4.0000E-01 5.0000E-03 -1.0000E-03 3.0000E-04 -6.3827E- In this embodiment, the sealant 12 is filled with a transparent optical silicone having a refractive index Ndl of 1.527 and an Abbe number udl of 34; the optical lens 14 has a refractive index Nd2 of 1.583 and an Abbe number of 2; d2 is 61.7. Made of glass. The light refraction angle is formed by matching the refractive index of the sealant 12 and the optical lens 14 with the Abbe number. The LED wafer 11 emits a blue light of α = 12·15 lumens, the effective maximum angle is 130°, and the effective focal length of the optical lens 14 has a length fs of 5.091 mm; after being concentrated by the optical lens 14, it is 92. The positive angle is at infinity (in terms of 100 times fs) cold = 11.51 lumens (ignoring the effects of air refraction and scattering); equations (3), (4), (5) and (6) are: -1) Same as = fs 0.2976 (4) + d\ +d2) 1.0521 and 2 Λ == = 1.7112 φ 10.3493 β ! a - 94.70% Coordinate relationship diagram. The formula () ° is the degree / knife cloth and the angle of the lens of the original creation = (a), table (two) and Figure 12, which can be used to prove the state of the spherical positive-angle light-emitting diode optical lens and its composition Luminescence 25 M345357.Product::::: has a simple surface shape, is easy to manufacture and has a predetermined light pattern, the first intensity of each angle - can enhance the application of this creation. w “The aspherical positive-lighting dipole light I lens of this creation and its • The effect of the Na*+^ photo-polar element is that it has a fresh surface shape, and can be used in a large number of processes such as glass, etc. Manufacturing is not easy to deform, • Reduce production costs. Among them, the wire lens can also use a plano-convex aspherical optical lens to simplify the manufacturing process. _ The non-face-to-face illuminating diode optical bias and the other effect of the illuminating diode assembly can make the light source projected from the LED chip have a predetermined light type. Suitable for lighting. • The aspherical positive-illuminated diode optic lens of this creation and its constituent hair-emitting elements are further effective in maintaining a uniform illumination intensity from the light source projected from the LED chip. Therefore, the image surface will not be partially bright or too dark, which will improve the lighting quality. The above is only the present embodiment, and is merely illustrative and non-limiting for the present creation. It will be understood by those skilled in the art that many changes, modifications, and equivalents may be made in the scope of the present invention. 26 M345357 [Simple description of the diagram] Figure 1 is a schematic diagram of the use of led optical lens on the LED assembly; Figure 2 is a schematic diagram of the use of LED optical lens in the LED assembly; Figure 3 is the LED optical lens of the present invention in the LED Figure 4 is a schematic diagram of the use of a plano-convex Lm) optical lens in the LED component of the present invention; Figure 5 is a schematic view of the use of a plano-convex optical lens in the component light path S3 · group, Figure 6 is the creation of this FIG. 7 is a diagram showing the relationship between the light intensity distribution of the LED component of the first embodiment and the polar coordinate of the illumination angle; FIG. 7 is the relationship between the light intensity distribution of the LED component of the second embodiment of the present invention and the polar coordinate of the illumination angle; FIG. 9 is a diagram showing the relationship between the light intensity distribution of the LED component and the polar coordinate of the illumination unit according to the fourth embodiment of the present invention; FIG. 10 is a fifth embodiment of the present invention. Figure 8 is a diagram showing the relationship between the light intensity distribution of the LED component and the polar coordinate of the illumination angle; Figure U is the relationship between the light intensity distribution of the LED component and the polar coordinate of the illumination angle of the sixth embodiment of the present invention; LED assembly embodiment of a light intensity distribution according to the angle of polar diagram; FIG. 13, and the light intensity of LED module system embodiment according to the distribution of the extreme angle of the eighth embodiment of the present Creation 27 M345357 coordinate diagram. [Main component symbol description] 10 : LED component; 11, 21 : LED chip; 12 : sealant; 13 : optical lens; 14 : optical lens; 23 : lens; • R1 : optical side of the light source or its radius of curvature; R2 : image side optical surface or radius of curvature thereof; d0 : LED wafer thickness on the central axis; dl: optical surface distance from the LED wafer surface on the central axis to the optical lens source side; ' d2 : central axis optical lens thickness; . co: LED Half of the maximum angle at which the wafer emits light; Ψ: half of the maximum angle at which the optical lens emits light;

Nd :折射率; vd :阿貝數; φ a : LED晶片發出光線的光通量;以及 β:像侧相對無限遠處光線的光通量。 28Nd : refractive index; vd : Abbe number; φ a : luminous flux of light emitted from the LED chip; and β: luminous flux of light on the image side with respect to infinity. 28

Claims (1)

M345357 九、申請專利範圍: 1、一種非球面正照角發光二極體光學鏡片,其係使用於發光二極 體組件中,沿著中心轴由光源側至像侧排列之一發光二極體晶 片、一封膠及一光學鏡片;其特徵在於: 该光學鏡片為一具有一凹面及一凸面的玻璃光學材料所製成的 鏡片,該凹面為向光源的光源侧光學面,該凸面為向像侧的像 侧光學面,其至少一個光學面為非球面;並滿足以下條件·· 0.7 < 及1 一及2 + i?2 <1.0 其中,R〗為該光學鏡片光源侧光學面之曲率半徑、心為該光學 鏡片像侧光學面之曲率半徑。 2如申印專利範圍第1項所述之非球面正照角發光二極體光學鏡 片,其中該光學鏡片係進一步滿足以下條件: ^ <180 8< 3·尖·Λ =,fS為該光學鏡片之有效焦距之長度、Ri為該光學鏡 源側光學面之轉半徑、d2為中心軸上該光學鏡片厚度。ΓΓΤ球面正照角發光二極體光學鏡 乃具中鑌光學鏡片係進一步滿足以下條件: 其^,fs為該光學鏡片之有效焦距之長度、也為中心轴上 予鏡片厚度、Nd2為該絲鏡μ的折射率。 μ 4、2項所述之非球面正照角發光二極體光學鏡 片,其中該光學鏡片係進-步滿足以下條件: 光干鏡 29M345357 IX. Patent application scope: 1. An aspherical positive-angle illumination LED optical lens, which is used in a light-emitting diode assembly, and arranges one of the light-emitting diode chips from the light source side to the image side along the central axis. An adhesive lens and an optical lens; wherein the optical lens is a lens made of a glass optical material having a concave surface and a convex surface, the concave surface being a light source side optical surface toward the light source, the convex surface being an image orientation The image side optical surface of the side, at least one of the optical surfaces is aspherical; and satisfies the following conditions: 0.7 < and 1 and 2 + i? 2 < 1.0 wherein R is the optical surface of the optical lens The radius of curvature and the center of the heart are the radius of curvature of the optical surface of the optical lens image side. 2. The aspherical positive-angle illumination LED optical lens according to claim 1, wherein the optical lens further satisfies the following condition: ^ <180 8<3·point·Λ =, fS is the optical The length of the effective focal length of the lens, Ri is the radius of rotation of the optical surface of the optical source, and d2 is the thickness of the optical lens on the central axis. The ΓΓΤ spherical positive-angle illuminating diode optical mirror is a medium-sized optical lens system that further satisfies the following conditions: ^, fs is the length of the effective focal length of the optical lens, also the thickness of the lens on the central axis, and Nd2 is the wire mirror The refractive index of μ. The aspherical positive-angle illumination light-emitting diode of the item 4, 2, wherein the optical lens is subjected to the following conditions: light-drying mirror 29
TW97211645U 2008-06-30 2008-06-30 Aspherical LED angular lens for central distribution patterns and LED assembly using the same TWM345357U (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
TW97211645U TWM345357U (en) 2008-06-30 2008-06-30 Aspherical LED angular lens for central distribution patterns and LED assembly using the same
JP2008006407U JP3148803U (en) 2008-06-30 2008-09-10 Optical lens of aspherical positive irradiation angle light emitting diode and light emitting diode component constituting the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
TW97211645U TWM345357U (en) 2008-06-30 2008-06-30 Aspherical LED angular lens for central distribution patterns and LED assembly using the same

Publications (1)

Publication Number Publication Date
TWM345357U true TWM345357U (en) 2008-11-21

Family

ID=44337837

Family Applications (1)

Application Number Title Priority Date Filing Date
TW97211645U TWM345357U (en) 2008-06-30 2008-06-30 Aspherical LED angular lens for central distribution patterns and LED assembly using the same

Country Status (2)

Country Link
JP (1) JP3148803U (en)
TW (1) TWM345357U (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5313181B2 (en) * 2010-01-26 2013-10-09 パナソニック株式会社 Lighting device
JP5901036B2 (en) * 2012-07-27 2016-04-06 シャープ株式会社 Lighting device
JP2014063651A (en) * 2012-09-21 2014-04-10 Toshiba Corp Illuminating device and lens for illumination

Also Published As

Publication number Publication date
JP3148803U (en) 2009-03-05

Similar Documents

Publication Publication Date Title
TWI361261B (en) Aspherical led angular lens for wide distribution patterns and led assembly using the same
TWI364120B (en) Convex-fresnel led lens for angular distribution patterns and led assembly thereof
TW201011349A (en) Plano-Fresnel LED lens for angular distribution patterns and LED assembly thereof
TWI357164B (en) Aspherical led angular lens for narrow distributio
TWM368029U (en) Fresnel LED lens and LED assembly thereof
TWI376822B (en) Light-emitting diode package
TW201033537A (en) Lens for LED illumination
TWI395908B (en) Aspherical led angular lens for central distribution patterns and led assembly using the same
TWI479107B (en) Led light distributing lens and light source apparatus using the same
CN101676615B (en) Convex Fresnel LED optical lens for angular distribution patterns and LED assembly thereof
TWM361594U (en) Flexible light-emitting apparatus
TWM345357U (en) Aspherical LED angular lens for central distribution patterns and LED assembly using the same
CN201273524Y (en) Convex surface Fresnel LED optical lens and LED component composed by the same
JP2012142142A (en) Surface light source device
JP3147939U (en) Planar Fresnel LED lens and LED assembly thereof
TWM345355U (en) Aspherical LED angular lens for wide distribution patterns and LED assembly using the same
TWM345356U (en) Aspherical LED angular lens for narrow distribution patterns and LED assembly using the same
CN101676616B (en) Plane Fresnel LED optical lens and LED assembly thereof
JP3164215U (en) Fresnel LED lens and its LED assembly (FresnelLEDLensandLEDAssemblyThereof)
TWM347534U (en) Convex-Fresnel LED lens for angular distribution patterns and LED assembly thereof
TWI480489B (en) Led light control lens and light source apparatus using the same
CN101626052B (en) Aspherical narrow irradiation-angle optical lens and light-emitting diode (LED) component formed by same
TW201903438A (en) lens
TWM347533U (en) Plano-Fresnel LED lens for angular distribution patterns and LED assembly thereof
JPWO2012141029A1 (en) Lens and lighting device

Legal Events

Date Code Title Description
MM4K Annulment or lapse of a utility model due to non-payment of fees