TWM439152U - LED optical transparent lens with multiple media - Google Patents

LED optical transparent lens with multiple media Download PDF

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Publication number
TWM439152U
TWM439152U TW101208416U TW101208416U TWM439152U TW M439152 U TWM439152 U TW M439152U TW 101208416 U TW101208416 U TW 101208416U TW 101208416 U TW101208416 U TW 101208416U TW M439152 U TWM439152 U TW M439152U
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Taiwan
Prior art keywords
light
medium
led
optical lens
light source
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TW101208416U
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Chinese (zh)
Inventor
De-Long Tang
wei-qiang Huang
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Ledlink Optics Inc
Ledlink Optics Co Ltd
Yangzhou Ledlink Optics Inc
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Priority to TW101208416U priority Critical patent/TWM439152U/en
Publication of TWM439152U publication Critical patent/TWM439152U/en

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Description

M439152 五、新型說明: 【新型所屬之技術領域】 本創作孫與光學透鏡之技術領域相關’特別是關於 種利用二次光學之折射或反射原理改變原發光二極體 發光角度之具複數介質之led光學透鏡,以提增照明範 圍而適用於各式燈具之不同需求。 【先前技術】M439152 V. New description: [New technology field] This creation is related to the technical field of optical lenses. In particular, it is about the use of multiple media by changing the angle of illumination of the original light-emitting diode by the principle of refraction or reflection of secondary optics. Led optical lens, to increase the range of illumination, is suitable for the different needs of various lamps. [Prior Art]

發光二極體(Light Emitting Diode, LED )具有低耗 電、兩效能及壽命長等特性而廣泛應用於各式背光源或 燈/包燈f中。然而’ LED之發光角度一般僅約12〇。,使 ’、、、明範圍文限制,且因LED之發光光線一般係較集中於 中心處,造成中心處與周邊處之亮度大小差異甚鉅而無 法提供均勻的照明效果。如此,採用LED作為光源之各 式LED照明裝置將因受限於LED光源之原發光角度及 原光線分佈性而具有較小的照明範圍及較差之光均度, 難以付合使用者需求。有鑑於此,led照明裝置多配置 有光學透鏡,以利用光學透鏡之二次光學原理調整LED 光源所發射之光,使針對原LED光源之投射照度、發光 角度及照射光之均勻度進行改善後產生各類適用性較佳 的光形佈局,而可於各種不同之使用條件下皆提 之照明狀態。 一 又’受裝置微型化的趨勢影響,或為符合高均光' 高照度及高照射範圍等市場需求,單一 LED^ =裝置 可能裝設有多顆LED,又每一顆LED皆配置_ ^學 鏡,..故.連.帶使光學.透鏡之構造設計及外觀體積受限=, M439152 影響光學透鏡所能產生的二 裝置無法提、供最佳之照明狀/:效果,造成LED照明 三次光學之折射及反射原理提該:昼:何進-步利用 功能’即為本領域相關從宰:光學透鏡之光徑調整 系者極欲改善之課題。 【新型内容】 有鑑於習知技藝之問題 種利用三次光學原理之本創作之目的在於提供- 提增原LED之發光角度”介質之LED光學透鏡,以 根據本創作之目的又,U^LED之適用性。 係供以组奘# ”複數"質之LED光學透鏡 1示货以組裝於—LED光湄,甘七a 少一井#人哲 九/原,其包含一光密介質本體及至 二士:二質。該光密介質本體之折射率為 二本第二本體’該第-本體具有開放式之至 二Hi第:本體具有開放式之至少-第二孔 一1 孔八數量係等於該第一孔穴數量,又該第 一本體與該第二本體對合連接設置而报占兮上—人新 适按°又置而形成該光密介質本 m穴位置係對應該第二孔穴位置而形成封 晉1至乂各置至。並且,該光疏介質係填充於該容 至,’且其折射率為112,並滿足η丨>n2之關係式。 為利用三次光學之折射或反射原理改善該led光 "、之f挂走向,該光疏介質填充於該容置室後形成一反 或手奴供以將該led光源所發射之光經該反射手段後 二光予反射。或者,該光疏介質填充於該容置室後形成 斤射手奴,供以將該LED光源所發射之光經該折射手 •^後為光學折射。 •立其中,該第一本體與該第二本體之側表面係設有一 '光均勻手^又,供以將該光源所發射之光經該側- 部先巧巧 射分佈:::後針對一側部目標照射區域呈均勻之光照 部光s 本體與該第二本體之頂表面係設有一頂 光均:=二t供以將該LED光源所發射之光經該頂部 分佈==後針對一頂部目標照射區域呈均勻之光照射 二二亚且’該第一本體上係設有-第-插合孔與-第 插::件,該第二本體上係設有—第二插合孔與一第二 ,且該第一插合孔係對應該第二插合件設置, •:體=件係對應該第二插合孔設置;另外該光密“ _ 係為㈣,該光疏介f係為空氣。 光學:ί係:達上述目的’本創作之具複數介質之LED 複數介質裝於一LED光源,其特徵在於:該具 介暫太ΐ ED光學透鏡具有一光密介質本體,該光密 ψ . 之折射率為nl’且該光密介質本體係為一體成 本體中設有至少一光疏介質,該光疏介 之折射率為h,並滿足ηι>η2之關係式。 :或’為達上述目的,本創作之具複數介質之[ED • 系供以組裝於一LED光源,其特徵在於:該具 ”質之LED光學透鏡係由至少三個光密介質本體 二而成,並於内部形成封閉式之至少一容置室,該容 折:真充至少一光疏介質,且各該光密介質本體之 斤:率為ηι’而該光疏介質之折射率為〜,並滿 之關係式。Light Emitting Diodes (LEDs) are widely used in various backlights or lamps/package lamps f due to their low power consumption, dual performance and long life. However, the angle of illumination of LEDs is generally only about 12 inches. Therefore, the range of ', , and Ming is limited, and because the illuminating light of the LED is generally concentrated at the center, the brightness difference between the center and the periphery is very large, and it is impossible to provide a uniform illumination effect. In this way, various LED illumination devices using LEDs as light sources will have a smaller illumination range and poorer light uniformity due to the limitation of the original illumination angle and the original light distribution of the LED light source, which is difficult to meet the needs of users. In view of this, the LED illumination device is often provided with an optical lens to adjust the light emitted by the LED light source by using the secondary optical principle of the optical lens, so as to improve the uniformity of the projection illumination, the illumination angle and the illumination light for the original LED light source. Produce a variety of suitable light shape layouts, and can be illuminated under a variety of different conditions of use. In addition, due to the trend of miniaturization of the device, or in order to meet the market demand of high-light and high illumination range, a single LED^= device may be equipped with multiple LEDs, and each LED is configured. ,.. Therefore, the belt makes the optics. The structural design of the lens and the appearance of the volume are limited =, M439152 affects the two devices that can be produced by the optical lens can not be raised, for the best illumination / effect, resulting in LED illumination three optics The principle of refraction and reflection is mentioned: 昼: 何进-step utilization function is the subject of the field of the optical path adjustment of the optical lens. [New content] In view of the problems of the prior art, the purpose of using the three-optical principle is to provide an LED optical lens that increases the illumination angle of the original LED, in accordance with the purpose of the creation, U^LED Applicability. For the group 奘 # ” complex number of “Quality LED optical lens 1 display to assemble in - LED light 湄, Gan Qia a Shaoyi well #人哲九/原, which contains a light-tight medium body and Two people: two quality. The refractive index of the body of the optically dense medium is two second bodies. The first body has an open type to two Hi: the body has an open type at least - the second hole has a number of holes and the number of holes is equal to the number of the first holes. And the first body and the second body are connected to each other to be placed on the top of the body, and the human body is placed in accordance with the angle to form the optically dense medium. The position of the m hole corresponds to the position of the second hole to form a seal. As for each set. Further, the light-draining medium is filled in the space, and its refractive index is 112, and satisfies the relationship of η 丨 > n2. In order to improve the led light by using the principle of three-dimensional optical refraction or reflection, the light-draining medium is filled in the accommodating chamber to form a counter or slave to supply the light emitted by the LED light source. After the reflection means, the two lights are reflected. Alternatively, the light-diffusing medium is filled in the accommodating chamber to form a smuggler, and the light emitted by the LED light source is optically refracted by the refracting hand. The first body and the side surface of the second body are provided with a 'light uniform hand', and the light emitted by the light source is distributed by the side-part: The one side target illumination area is uniform and the illumination part s main body and the top surface of the second body are provided with a top light:=two t for the light emitted by the LED light source to be distributed through the top== A top target illumination area is irradiated with uniform light and the second body is provided with a - first-insert hole and a - first insert: the second body is provided with a second plug a hole and a second, and the first insertion hole is disposed corresponding to the second connector, • the body=piece corresponds to the second insertion hole; and the light density “ _ is (4), the light The optical system is air. Optical: 系: For the above purpose The body, the optical density, has a refractive index of nl', and the optically dense medium has at least one of the integrated body For the medium, the refractive index of the light is h, and satisfies the relationship of ηι > η2 : : or 'for the above purpose, the creation of the plural medium [ED • is provided for assembly in an LED light source, The utility model is characterized in that: the "LED" optical lens is made up of at least three optically dense medium bodies, and forms at least one accommodating chamber in a closed state, and the content is: at least one light-draining medium is charged, and Each of the optically dense medium bodies has a mass ratio of ηι' and the refractive index of the light-diffusing medium is ~, and is in a relational expression.

上所述’該具複數介質之咖光學透鏡係利用光 ,傳輸於不同介質間所產生的偏移角度調整及改變該 LED光源之原光徑方向,使提升照射光之均勻度,並且, 夕偏移角度達最大值而形成全反射時,即可提增該LED M439152 圍 範 明 照 大 擴 而 度 角 光 3 發 式 原 方 之 施 源 實 [ 為使責審查委員能清楚 列說明搭配圖式,敬請參閱。 |作之内容,謹以下 一第1〜4圖,其係為本創作第-較佳實施例之 如圖所+兮曰 觀圖、剖視圖及光跡圖。 如圖所不’該具複數介質之LED : 於- LED光源(圖未示),其兄係供以組裝 -伽本社八所 先畨介質本體10及 二個先疏"貝π,且該光密介質本體 質所製成之圓柱狀設置,而該光疏介質"可為由空塑氣膠: m光密玄介質本體10之折射率nl係大於該光疏介質 U之折射率n2。該LED光學透鏡】可非一體成型,即 該光密介質本體10具有—第一本體ι〇〇及一第二本體 ιοί’該第一本體1〇〇設有開放式之三個第一孔穴1〇〇〇 一第一插合孔1001及一第一插合件1〇〇2,而該第二本 體101設有與該等第一孔穴1〇〇〇相同數量之三個開放式 第二孔穴1010、一第二插合孔1011與一第二插合件 1012,且該第二插合孔1〇11對應該第一插合件1〇〇2設 置,該第二插合件丨〇丨2對應該第一插合孔i 〇〇丨設置。 透過該第一插合件1002嵌合該第二插合孔1〇11,及該 第一插合件1012嵌合該第一插合孔1〇〇1,使該第一本 體100與該第二本體1〇1對合連接而形成該光密介質本 趙1〇’並且,各該第一孔穴1〇〇〇之位置係對應各該第 一孔穴1010位置而形成封閉式之三個容置室,供以容置 該光疏介質11。 ——又’該第一本體1 〇〇廣該第·二本體—j j之頂表-面可 M439152 設有-頂部光均勻手段,例如於該 接之複數個平面12,供以將該LEd 2面周緣設置相連 該頂部光均勻手段後針對一頂部 听所發射♦之·光'經 光照射分佈。該第一本體1〇〇 =區域呈均勾之 面設有—側部光均句手段,以透過掷:鱗則表 葉13使該LED光源所發射之光經J = = = 後,針對-侧部目標照射區域 =勻手奴 得注意的是,該等凸葉"呈平面狀且2 值 該第-本體100與該第二本體1〇1之側=_於 一層的葉環,使於圖3之剖視圖中, 成一層 社筮-士触Λ 这第一本體100與 該第一本體1 0 1之側邊緣係呈鋸齒狀。 ,實施態樣t,該等容置室係分別呈漏斗狀空間结 構,其尖嘴端均朝向該led光學透鏡丨底部,且該等六 置室相距該LED光學透鏡!底部之距離越遠,則漏斗= 空間結構越大《使該光疏介質丨丨填充於該容置室即形成 一反射手段,供以將該LED光源所發射之光經該反射手 段後為光學反射,換言之,當該led光源之光欲穿射最 鄰近該LED光學透鏡1底部之第一容置室時,因該光密 介質本體10及該光疏介質11之折射率滿足n1>Il2之關 係式,故依全反射原理’該LED光源所發射之部份光將 全反射於該第一谷置室下表面。又,另一部份光經該第 一容置室折射後持續朝該LED光學透鏡1頂部傳送,使 進一步反射於該第二容置室或該第三容置室之下表面, 如此,透過疊置之該等光疏介質11即可有效提增發光角 度及照明範圍。 承上,請再參閱第5、6圖,其係為本創作第一較佳 7 M439152 實施例之另-實施態樣之剖視圖及光跡圖。如圖所示, 為使該光疏介f u填充於該容置室後形成一折射手 段,供以將WED光源所發射之光經該折射手段後為光 學折射,該等容置室将丨5 不刀另J呈半橢圓狀空間結構,其弧 邊均朝向該LED光學透鏡"頁部設置,且該等容置室相 距該LED光學透鏡!底部之距離越遠,則半满圓狀空間 結構越大H步折射該LED光源所發射之光而提升 均光度》 請參閱第7、8圖’其係分別為本創作第二較佳實施 :之立體外觀圖及剖視示意圖。如圖所示,該具複數介 質之LED光學透鏡2係供以組|於—咖光源(圖未 示以透過三次光學之反射原理改善該led光源之原 發光角度及照明範圍。該LED光學透鏡2具有一光密介 質本體2〇及一光疏介質2卜該光密介質本體20可由塑 膠材質-體成形而製成上寬下窄之杯體結構,且其折射 率為n】,而該光疏介f 21可呈漏斗狀設置並設於該光 密介質本體201又,該光疏介f2i可為线,故其 折射率h係小於該光密介質本體2〇之折射率⑴。如此, 當該LED光源之光徑偏移達角度時,將全反射於該 光疏介質2丨,使該LED光源具有較廣之照明範圍。 請參閱第9、10圖,其係分別為本創作第三較佳實 施例之立體外觀圖及剖視示意圖。如圖所示,肖具複數 介質之LED光學透鏡3係供以組裝於一㈣光源(圖 未不)’且該LED光學透鏡.3為由三個光密介質本體 接合而成之塑膠杯體,並於内部形成封閉式之一容置 室。該容置室可呈半橢圓狀空間結構,供以填充透明之 8 M439152 一光疏介質31,且該光密介質本體30 而該光疏介質31之折射率為n2,使滿 式。如此,該LED光源所發射垂直射入 光將因該光疏介質31而產生折射,使加 明範圍。 以上所述僅為舉例性之較佳實施例 者。任何未脫離本創作之精神與範疇, 效修改或變更’均應包含於後附之申請 之折射率為η丨, 足η丨>η2之關係 該容置室之部分 強發散以提升照 ,而非為限制性 而對其進行之等 專利範圍中。 M439152 【圖式簡單說明】 第1圖 係為本創作第一較佳實施例之一實施態樣之分 解圖。 第2圖 係為本創作第一較佳實施例之一實施態樣之立 體外觀圖。 第3圖 係為本創作第一較佳實施例之一實施態樣之剖 視圖。 第4圖 係為本創作第一較佳實施例之一實施態樣之光 跡圖。 第5圖 係為本創作第一較佳實施例之另一實施態樣之 剖視圖 第6圖 係為本創作第一較佳實施例之另一實施態樣之 光跡圖。 第7圖 係為本創作第二較佳實施例之立體外觀圖。 第8圖 係為本創作第二較佳實施例之剖視示意圖。 第9圖 係為本創作第三較佳實施例之立體外觀圖。 第1 0圖係為本創作第三較佳實施例之剖視示意圖。 【主要元件符號說明】 第一較佳實施例 1 LED光學透鏡 10 光密介質本體 100 第一本體 1000第一孔穴 1001第一插合孔 1002第一插合件 101 第二本體 ·- 10 M439152 1 Ο 1 0第二孔穴 1 Ο 1 1第二插合孔 1 Ο 1 2第二插合件 11 光疏介質 12 平面 13 凸葉 第二較佳實施例 2 LED光學透鏡The above-mentioned coffee optical lens with a plurality of media uses the offset angle generated by light transmitted between different media to adjust and change the original light path direction of the LED light source, so as to improve the uniformity of the illumination light, and When the offset angle reaches the maximum value and the total reflection is formed, the LED can be increased. M439152 is widely used for the expansion of the angle and the angle of the light is 3, and the source of the original method is used. Please see. The contents of the following are shown in Figures 1 to 4, which are the drawings, cross-sectional views and light traces of the first preferred embodiment of the present invention. As shown in the figure, the LED with a plurality of media: in - LED light source (not shown), its brother is supplied with assembly - Gabon Society eight first media body 10 and two first sparse "be π, and The light-tight medium body is formed in a cylindrical shape, and the light-diffusing medium may be an empty plastic gas: the refractive index nl of the m-light medium body 10 is greater than the refractive index n2 of the light-transmissive medium U . The LED optical lens can be non-integrally formed, that is, the optically dense medium body 10 has a first body ι and a second body ιοί'. The first body 1 〇〇 is provided with three open first holes 1 a first insertion hole 1001 and a first coupling member 1〇〇2, and the second body 101 is provided with the same number of three open second holes as the first holes 1〇〇〇 1010, a second insertion hole 1011 and a second connector 1012, and the second insertion hole 1〇11 is disposed corresponding to the first connector 1〇〇2, the second connector 丨〇丨2 corresponds to the first insertion hole i 〇〇丨 setting. The second insertion hole 1〇11 is fitted through the first connector 1002, and the first insertion hole 1012 is fitted into the first insertion hole 1〇〇1 to make the first body 100 and the first body 100 The two bodies 1对1 are connected to each other to form the optically dense medium, and the positions of the first holes 1〇〇〇 are corresponding to the positions of the first holes 1010 to form three closed contents. a chamber for accommodating the light-dissipating medium 11. - 'The first body 1 〇〇 该 the second body - jj top table - face M439152 is provided - top light uniform means, for example, the plurality of planes 12 connected to the LEd 2 The peripheral edge of the face is connected to the top light uniform means to emit a light-irradiated distribution for a top listener. The first body 1 〇〇 = area is provided with a side hook surface means - a side light average sentence means to pass the throw: the scale surface 13 causes the light emitted by the LED light source to pass J = = = Side target illumination area = uniform handy note that the lobes " are planar and 2 values of the first body 100 and the side of the second body 1 = 1 = _ on one layer of the leaf ring, so that In the cross-sectional view of FIG. 3, the first body 100 and the side edge of the first body 110 are serrated. In the embodiment, the accommodating chambers have a funnel-shaped space structure, and the tip ends thereof face the bottom of the led optical lens, and the six chambers are apart from the LED optical lens! The farther the distance from the bottom is, the larger the space structure is. The filling of the light-dissipating medium into the accommodating chamber forms a reflection means for the light emitted by the LED light source to pass through the reflection means. The reflection, in other words, when the light of the LED light source is intended to pass through the first accommodating chamber closest to the bottom of the LED optical lens 1, the refractive index of the optically dense medium body 10 and the optically thin medium 11 satisfies n1>Il2 According to the principle of total reflection, part of the light emitted by the LED light source will be totally reflected on the lower surface of the first valley chamber. In addition, another portion of the light is refracted by the first accommodating chamber and continues to be transmitted toward the top of the LED optical lens 1 to be further reflected on the lower surface of the second accommodating chamber or the third accommodating chamber. The light-dissipating medium 11 stacked thereon can effectively increase the illumination angle and the illumination range. Please refer to Figures 5 and 6 again for a cross-sectional view and a trace diagram of another embodiment of the first preferred embodiment of the M M M M M M M M M. As shown in the figure, in order to fill the accommodating chamber, a refraction means is formed for optically refracting the light emitted by the WED source through the refracting means, and the accommodating chambers are 丨5 The other side of the J is a semi-elliptical space structure, the arc edges are all facing the LED optical lens " page portion, and the housing chamber is away from the LED optical lens! The farther the distance from the bottom is, the larger the semi-full circular space structure is. The H step refracts the light emitted by the LED light source to enhance the homogenization. Please refer to Figures 7 and 8 for the second preferred implementation of the creation: The three-dimensional appearance and cross-sectional view. As shown in the figure, the LED optical lens 2 with a plurality of media is provided with a group of light source (the figure is not shown to improve the original light-emitting angle and illumination range of the LED light source by the principle of three-dimensional optical reflection. The LED optical lens 2 having a light-tight medium body 2〇 and a light-diffusing medium 2, the light-tight medium body 20 can be formed by a plastic material body to form a cup structure having an upper width and a lower width, and the refractive index thereof is n], and the refractive index is n] The light scattering device f 21 may be disposed in a funnel shape and disposed on the optically dense medium body 201. The light scattering medium f2i may be a line, so that the refractive index h is smaller than the refractive index (1) of the optically dense medium body 2 。. When the optical path of the LED light source is offset by an angle, it is totally reflected on the light-dissipating medium 2丨, so that the LED light source has a wide illumination range. Please refer to Figures 9 and 10, respectively. A perspective view and a cross-sectional view of a third preferred embodiment. As shown, an LED optical lens 3 of a plurality of dielectrics is provided for assembly in a (four) light source (not shown) and the LED optical lens. It is a plastic cup body made of three light-tight medium bodies, and is internally shaped. The accommodating chamber is a semi-elliptical space structure for filling a transparent 8 M439152-light-diffusing medium 31, and the optical-dense medium body 30 and the refractive index of the light-storing medium 31 For n2, the full mode is obtained. Thus, the vertical incident light emitted by the LED light source will be refracted by the light-diffusing medium 31 to make the range of the clarification. The above description is only an exemplary preferred embodiment. Deviation from the spirit and scope of this creation, effect modification or alteration 'should be included in the attached application's refractive index η丨, ηη丨>η2 relationship, the part of the containment chamber is strongly divergent to enhance the photo, not For the sake of limitation, it is in the scope of patents. M439152 [Simplified description of the drawings] Fig. 1 is an exploded view of an embodiment of the first preferred embodiment of the present invention. A perspective view of an embodiment of a preferred embodiment. Fig. 3 is a cross-sectional view showing an embodiment of the first preferred embodiment of the present invention. Fig. 4 is a first preferred embodiment of the present invention. A light trace of an implementation. Figure 5 is a creation BRIEF DESCRIPTION OF THE DRAWINGS FIG. 6 is a light trace diagram of another embodiment of the first preferred embodiment of the present invention. FIG. 7 is a second preferred embodiment of the present invention. Figure 8 is a schematic cross-sectional view of a second preferred embodiment of the present invention. Figure 9 is a perspective view of the third preferred embodiment of the present invention. 3 is a cross-sectional view of a preferred embodiment. [First element symbol description] First preferred embodiment 1 LED optical lens 10 Optically dense medium body 100 First body 1000 first hole 1001 First insertion hole 1002 first insertion Member 101 Second body·- 10 M439152 1 Ο 1 0 second hole 1 Ο 1 1 second insertion hole 1 Ο 1 2 second connector 11 light-draining medium 12 plane 13 convex second preferred embodiment 2 LED optical lens

20 光密介質本體 21 光疏介質 第三較佳實施例 3 LED光學透鏡 30 光密介質本體 3 1 光疏介質20 Optically dense medium body 21 Light-diffusing medium Third preferred embodiment 3 LED optical lens 30 Optically dense medium body 3 1 Light-dissolving medium

Claims (1)

六、申請專利範圍: 1· 一種具複數介質之led光學透鏡, 认 τ ^ &規係供以組裝 於一 LED光源,其包含: 第-本體’具有開放式之至少一3第一孔 一光密介質本體’其折射率為…,包人 六;及 一第二本體,具有開放式之至少一第二孔 穴,且該第二孔穴數量係等於該第一孔;數 量,又該第一本體與該第二本體係對合連接設 置而形成該光密介質本體,且該第一孔穴位^ 係對應該第二孔穴位置而形成封閉式:至少 一容置室;及 夕 至少一光疏介質,係填充於該容置室内,且其 折射率為η2 ’並滿足ηι>η2之關係式。 2.如申請專利範圍第1項所述之具複數介質之LED 光學透鏡,其中該光疏介質填充於該容置室後形成 一反射手段,供以將該LED光源所發射之光經該 反射手段後為光學反射》 3·如申請專利範圍第1項所述之具複數介質之LED 光學透鏡,其中該光疏介質填充於該容置室後形成 一折射手段,供以將該LED光源所發射之光經該 折射手段後為光學折射。 ‘ 4.如申請專利範圍第2或3項所述之具複數介質之 LED光學透鏡,其中該第一本體與該第二本體之側 表面係設有一側部光均勻手段,供以將該LED光 源所發射之光經該側部光均勻手段後針對一側部 12 M439152 目標照射區域呈均勻之光照射分佈。 5·如:::利範圍第4項所述之具複數介質之l£D 光:古:,其中該第一本體與該第二本體之頂表面 係》又 頂部光均勻手段,供以將1¾ LED光源所 發射之先經該頂部光均句手段後針對一頂部目構 照射區域呈岣勻之光照射分佈。 6.如申請專利範圍第5項所述之具複數介質之咖 光學透鏡,其中該第-本體上係設有-第一插合孔 與一第:插合件,該第二本體上係設有一第二插合 孔ΐ:!二插合件;且該第一插合孔係對應該第二 插&件没置’該第—插合件係對應該第二插合孔設 置;另外該光密介質本體係為塑膠,該光疏介質係 為空氣。 7· -種具複數介質之LED光學透鏡,係供以組裝於 一 LED光源,其特徵在於: 該具複數介質之LED光學透鏡係具有一光密 介質本體,1¾光密介質本體之折射率Am,且該光 • 密介質本體係為一體成形;該光密介質本體中設有 至少一光疏介質,該光疏介質之折射率為n2,並滿 足n!>n2之關係式。 8. -種具複數介質之LED *學透鏡,係供以組裝於 一 LED光源,其特徵在於: 該具複數介質之LED光學透鏡係由至少三個 光密介質本體接合而成,並於内部形成封閉式之至 少-容置室’該容置室供以填充至少一光疏介質, 且各該光密介質本體之折射率為1,而該光疏介質 M439152Sixth, the scope of application for patents: 1. A led optical lens with a plurality of media, the τ ^ & regulation is provided for assembly in an LED light source, comprising: the first body - having an open type of at least one of the first holes and a light dense The medium body 'having a refractive index of ..., a person's six; and a second body having an open type of at least one second hole, and the number of the second holes is equal to the first hole; the number, the first body and The second system is connected to form the optically-tight medium body, and the first hole position is corresponding to the second cavity position to form a closed type: at least one housing chamber; and at least one light-smoothing medium, It is filled in the accommodating chamber, and its refractive index is η2 ' and satisfies the relationship of ηι > η2. 2. The LED optical lens with a plurality of media according to claim 1, wherein the light-diffusing medium is filled in the accommodating chamber to form a reflecting means for transmitting the light emitted by the LED light source through the reflection The LED optical lens with a plurality of media as described in claim 1, wherein the light-diffusing medium is filled in the accommodating chamber to form a refraction means for the LED light source The emitted light is optically refracted by the means of refraction. 4. The LED optical lens with a plurality of media according to the second or third aspect of the invention, wherein the side surfaces of the first body and the second body are provided with a side light uniform means for the LED The light emitted by the light source is uniformly distributed by the side light uniform means for the side illumination portion of the side portion 12 M439152. 5·如::: The l£D light of the plural medium described in item 4 of the profit range: ancient: wherein the first body and the top surface of the second body are both top light uniform means for The light emitted by the LED light source is firstly distributed by the top light means for a uniform illumination of the top surface. 6. The coffee optical lens with a plurality of media according to claim 5, wherein the first body is provided with a first insertion hole and a first: a connector, and the second body is provided There is a second insertion hole !:! two insertion members; and the first insertion hole is corresponding to the second insertion & the member is not set to the first insertion member corresponding to the second insertion hole; The optically dense medium is a plastic, and the light-diffusing medium is air. 7. An LED optical lens with a plurality of dielectrics for assembly in an LED light source, characterized in that: the LED optical lens with a plurality of dielectrics has an optically dense medium body, and the refractive index of the optically dense medium body is Am The light-tight medium system is integrally formed; the light-tight medium body is provided with at least one light-smoothing medium having a refractive index of n2 and satisfying the relationship of n!>n2. 8. An LED with a plurality of media, the lens is assembled for use in an LED light source, characterized in that: the LED optical lens with a plurality of media is formed by joining at least three optically dense media bodies and internally Forming a closed-type at least-receiving chamber, wherein the accommodating chamber is filled with at least one light-storing medium, and each of the optical-tight medium bodies has a refractive index of 1, and the light-draining medium M439152
TW101208416U 2012-05-04 2012-05-04 LED optical transparent lens with multiple media TWM439152U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
TW101208416U TWM439152U (en) 2012-05-04 2012-05-04 LED optical transparent lens with multiple media

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
TW101208416U TWM439152U (en) 2012-05-04 2012-05-04 LED optical transparent lens with multiple media

Publications (1)

Publication Number Publication Date
TWM439152U true TWM439152U (en) 2012-10-11

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Family Applications (1)

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