TWM516690U - Optical lens - Google Patents

Optical lens Download PDF

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Publication number
TWM516690U
TWM516690U TW104214752U TW104214752U TWM516690U TW M516690 U TWM516690 U TW M516690U TW 104214752 U TW104214752 U TW 104214752U TW 104214752 U TW104214752 U TW 104214752U TW M516690 U TWM516690 U TW M516690U
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Taiwan
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light
mirror body
curvature
optical lens
light incident
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TW104214752U
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Chinese (zh)
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忠翰 游
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格蘭照明國際股份有限公司
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Priority to TW104214752U priority Critical patent/TWM516690U/en
Publication of TWM516690U publication Critical patent/TWM516690U/en

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Description

光學透鏡 optical lens

本案係關於一種光學透鏡,詳而言之,係關於一種用於LED之光學透鏡。 This case relates to an optical lens, in particular, to an optical lens for an LED.

發光二極體(Light Emitting Diodel;LED)為一種可將電流轉換成特定波長範圍的半導體元件。發光二極體以其亮度高、工作電壓低、功耗小、易與積體電路匹配、驅動簡單、壽命長等優點,從而作為光源而廣泛應用於照明領域。 A Light Emitting Diode (LED) is a semiconductor component that converts current into a specific wavelength range. The light-emitting diode is widely used in the field of illumination as a light source because of its high brightness, low operating voltage, low power consumption, easy matching with integrated circuits, simple driving, and long life.

近年來,利用LED的照明設備取代現有的戶外照明設備已逐漸成為趨勢,例如路燈等。然而,LED的光線只以特定方向發出,並非朝全部方向發出均勻的光線,相較於以全部方向發光的現有戶外照明設備,LED照明設備與非LED的戶外照明設備之間的光線分布特性差異很大,因此LED用於戶外照明設備仍有其限制。 In recent years, the use of LED lighting equipment to replace existing outdoor lighting equipment has gradually become a trend, such as street lamps. However, the light of the LED is emitted only in a specific direction, and does not emit uniform light in all directions. Compared with the existing outdoor lighting equipment that emits light in all directions, the difference in light distribution characteristics between the LED lighting device and the non-LED outdoor lighting device It is very large, so LEDs still have limitations for outdoor lighting.

為了更好地利用發光二極體,業界通常在對發光二極體封裝後在其周圍包覆一透鏡對光進行光學校正,以達到所期望的水平和垂直光束角。 In order to make better use of the light-emitting diodes, the industry generally optically corrects the light by coating a lens around the LED package to achieve the desired horizontal and vertical beam angles.

如何提供一種出光對稱且具有預定光束角之透鏡,為目前本領域之技術人員致力研發之目標。 How to provide a lens with optical symmetry and a predetermined beam angle is the goal of current research and development by those skilled in the art.

於一實施例中,本案提供一種光學透鏡,係供覆蓋於發光單元上,該光學透鏡包括:第一鏡體,係包括第一出光面、第二出光面、相對於該第一出光面之第一入光面及第二入光面、相對於該第二出光面之第三入光面、及與該第一入光面、該第二入光面和該第三入光面連接之底面,該第一入光面、該第二入光面和該第三入光面依序連接以於該底面形成用於容納該發光單元之凹槽;第二鏡體,係連接該第一鏡體,並包括連接該第二出光面之外圍面、相對於該外圍面之第一內圍面及非平坦的第二內圍面,該第一內圍面和該第二內圍面相連接以形成空穴,且該第一內圍面連接該底面及該第三入光面;以及安裝體,係環繞且連接於該第一鏡體和該第二鏡體,並相對於該第一鏡體和該第二鏡體向外延伸。 In an embodiment, the present invention provides an optical lens for covering a light emitting unit, the optical lens comprising: a first mirror body, comprising a first light emitting surface, a second light emitting surface, and the first light emitting surface a first light incident surface and a second light incident surface, a third light incident surface opposite to the second light emitting surface, and a first light incident surface, the second light incident surface, and the third light incident surface a bottom surface, the first light incident surface, the second light incident surface, and the third light incident surface are sequentially connected to form a recess for receiving the light emitting unit; the second mirror body is connected to the first a mirror body, comprising: a peripheral surface connecting the second light-emitting surface, a first inner circumferential surface opposite to the peripheral surface, and a non-flat second inner circumferential surface, wherein the first inner circumferential surface and the second inner circumferential surface are connected Forming a cavity, and the first inner peripheral surface connects the bottom surface and the third light incident surface; and the mounting body is wound around and connected to the first mirror body and the second mirror body, and is opposite to the first The mirror body and the second mirror body extend outward.

於前述實施例中,該光學透鏡包含171.6度±10%之水平光束角以及160度±10%之垂直光束角。 In the foregoing embodiments, the optical lens comprises a horizontal beam angle of 171.6 degrees ± 10% and a vertical beam angle of 160 degrees ± 10%.

於另一實施例中,本案提供一種光學透鏡,係供覆蓋於發光單元上,該光學透鏡包括:第一鏡體,係包括出光面、相對於該出光面之第一入光面、第二入光面和非平坦的第三入光面、及與該第一入光面、第二入光面及第三入光面連接之底面,該第一入光面、第二入光面及第三入光面依序連接以於該底面形成用於容納該發光單元之凹槽;第二鏡體,係連接該第一鏡體,並包括連接該出光面之外圍面及相對於該外圍面之第一內圍面和非平坦的第二內圍 面,該第一內圍面和該第二內圍朝相連接以形成空穴,且該第一內圍面連接該底面;以及安裝體,係環繞且連接於該第一鏡體和該第二鏡體,並相對於該第一鏡體和該第二鏡體向外延伸。 In another embodiment, the present invention provides an optical lens for covering a light emitting unit. The optical lens includes: a first mirror body including a light emitting surface, a first light incident surface opposite to the light emitting surface, and a second a light incident surface and a non-flat third light incident surface, and a bottom surface connected to the first light incident surface, the second light incident surface, and the third light incident surface, the first light incident surface and the second light incident surface The third light incident surface is sequentially connected to form a recess for accommodating the light emitting unit; the second mirror body is connected to the first mirror body, and includes a peripheral surface connecting the light exiting surface and opposite to the periphery First inner circumference and non-flat second inner circumference a first inner circumferential surface and the second inner circumferential surface are connected to form a cavity, and the first inner circumferential surface is connected to the bottom surface; and the mounting body is surrounded and connected to the first mirror body and the first The second mirror body extends outward relative to the first mirror body and the second mirror body.

於前述另一實施例中,該光學透鏡包含107.9度±10%之水平光束角以及152.8度±10%之垂直光束角。 In another embodiment of the foregoing, the optical lens comprises a horizontal beam angle of 107.9 degrees ± 10% and a vertical beam angle of 152.8 degrees ± 10%.

1、4‧‧‧第一鏡體 1, 4‧‧‧ first mirror

10、40‧‧‧凹槽 10, 40‧‧‧ grooves

11‧‧‧第一出光面 11‧‧‧The first glazing

111、121‧‧‧中央區 111, 121‧‧‧ Central District

112、122‧‧‧兩側區 112, 122‧‧‧ both sides

12‧‧‧第二出光面 12‧‧‧Second glazing

13‧‧‧緩衝面 13‧‧‧ buffer surface

14、42‧‧‧第一入光面 14, 42‧‧‧ first light surface

15、43‧‧‧第二入光面 15, 43‧‧‧ second entrance

16、44‧‧‧第三入光面 16, 44‧‧‧ Third light surface

17、45‧‧‧底面 17, 45‧‧‧ bottom

2、5‧‧‧第二鏡體 2, 5‧‧‧ second mirror

20、50‧‧‧空穴 20, 50‧‧‧ hole

21、51‧‧‧外圍面 21, 51‧‧‧ peripheral surface

22、52‧‧‧第一內圍面 22, 52‧‧‧ first inner circumference

23、53‧‧‧第二內圍面 23, 53‧‧‧ Second inner circumference

231、232、531、532‧‧‧面 231, 232, 531, 532‧ ‧

3、6‧‧‧安裝體 3, 6‧‧‧Installation

31、611‧‧‧第一面 31, 611‧‧‧ first side

32、612‧‧‧第二面 32, 612‧‧‧ second side

33、613‧‧‧側面 33, 613‧‧‧ side

34、614‧‧‧安裝孔 34, 614‧‧‧ mounting holes

35、615‧‧‧出線槽 35, 615‧‧‧ outlet slot

41‧‧‧出光面 41‧‧‧Glossy

411‧‧‧平面區 411‧‧‧ flat area

412‧‧‧弧面區 412‧‧‧Arc area

61‧‧‧安裝部 61‧‧‧Installation Department

62‧‧‧連接部 62‧‧‧Connecting Department

R1、R2、R3、R4、R5、R6、R7、R8、R9、R10‧‧‧曲率 R1, R2, R3, R4, R5, R6, R7, R8, R9, R10‧‧‧ curvature

第1圖為本案之第一實施例的光學透鏡之立體圖;第2圖為本案之第一實施例的光學透鏡之仰視圖;第3圖為本案之第一實施例的光學透鏡之俯視圖;第4A圖為本案之第一實施例的光學透鏡之沿著第3圖之A-A剖面線的剖面圖;第4B圖為本案之第一實施例的光學透鏡之沿著第3圖之B-B剖面線的剖面圖;第4C圖為本案之第一實施例的光學透鏡之曲率示意圖;第5圖為本案之第一實施例的光學透鏡之光線路徑圖;第6圖為本案之第一實施例的光學透鏡之光通量分佈圖;第7A-7D圖為本案之第二實施例的光學透鏡之光強度分佈圖;第8圖為本案之第二實施例的光學透鏡之立體圖;第9圖為本案之第二實施例的光學透鏡之仰視圖; 第10圖為本案之第二實施例的光學透鏡之俯視圖;第11A圖為本案之第二實施例的光學透鏡之沿著第10圖之A-A剖面線的剖面圖;第11B圖為本案之第二實施例的光學透鏡之沿著第10圖之B-B剖面線的剖面圖;第11C圖為本案之第二實施例的光學透鏡之曲率示意圖;第12圖為本案之第二實施例的光學透鏡之光線路徑圖;第13圖為本案之第二實施例的光學透鏡之光通量分佈圖;以及第14A-14D圖為本案二第一實施例的光學透鏡之光強度分佈圖。 1 is a perspective view of an optical lens of a first embodiment of the present invention; FIG. 2 is a bottom view of the optical lens of the first embodiment of the present invention; and FIG. 3 is a plan view of the optical lens of the first embodiment of the present invention; 4A is a cross-sectional view of the optical lens of the first embodiment of the present invention taken along line AA of FIG. 3; FIG. 4B is a cross-sectional view of the optical lens of the first embodiment of the present invention taken along line BB of FIG. FIG. 4C is a view showing the curvature of the optical lens of the first embodiment of the present invention; FIG. 5 is a light path diagram of the optical lens of the first embodiment of the present invention; and FIG. 6 is an optical diagram of the first embodiment of the present invention. a light flux distribution diagram of the lens; 7A-7D is a light intensity distribution diagram of the optical lens of the second embodiment of the present invention; FIG. 8 is a perspective view of the optical lens of the second embodiment of the present invention; a bottom view of the optical lens of the second embodiment; 10 is a plan view of the optical lens of the second embodiment of the present invention; FIG. 11A is a cross-sectional view of the optical lens of the second embodiment of the present invention taken along line AA of FIG. 10; 2 is a cross-sectional view taken along line BB of FIG. 10; FIG. 11C is a schematic view showing the curvature of the optical lens of the second embodiment of the present invention; and FIG. 12 is an optical lens of the second embodiment of the present invention. FIG. 13 is a light flux distribution diagram of the optical lens of the second embodiment of the present invention; and FIG. 14A-14D is a light intensity distribution diagram of the optical lens of the first embodiment of the present invention.

以下藉由特定的具體實施例說明本案之實施方式,熟習此項技藝之人士可由本文所揭示之內容輕易地瞭解本案之其他優點及功效。須知,本說明書所附圖式所繪示之結構、比例、大小等,均僅用以配合說明書所揭示之內容,以供熟悉此技藝之人士之瞭解與閱讀,並非用以限定本案可實施之限定條件,故不具技術上之實質意義,任何結構之修飾、比例關係之改變或大小之調整,在不影響本案所能產生之功效及所能達成之目的下,均應仍落在本案所揭示之技術內容得能涵蓋之範圍內。 The embodiments of the present invention are described below by way of specific embodiments, and those skilled in the art can readily appreciate the other advantages and advantages of the present disclosure. It is to be understood that the structure, the proportions, the size and the like of the drawings are only used in conjunction with the disclosure of the specification for the understanding and reading of those skilled in the art, and are not intended to limit the practice of the present invention. The qualifications are not technically meaningful. Any modification of the structure, change of the proportional relationship or adjustment of the size should not be affected by the effects of the case and the objectives that can be achieved. The technical content can be covered.

第一實施例 First embodiment

參閱第1-4C圖,其分別繪示本案第一實施例的光學透鏡之立體圖、仰式圖、俯視圖、A-A剖面圖、B-B剖面圖和曲率示意圖。 1-4C is a perspective view, an elevation view, a top view, an A-A cross-sectional view, a B-B cross-sectional view, and a curvature diagram of the optical lens of the first embodiment of the present invention.

於本實施例中,光學透鏡包括第一鏡體1、第二鏡體2及安裝體3。 In the embodiment, the optical lens includes a first mirror body 1, a second mirror body 2, and a mounting body 3.

第一鏡體1包括第一出光面11、第二出光面12、連接第一出光面11和第二出光面12之緩衝面13、相對於第一出光面11之第一入光面14和第二入光面15、相對於第二出光面12之第三入光面16、及連接於第一入光面14、第二入光面15和第三入光面16之底面17。第一入光面14、第二入光面15和第三入光面16依序連接以於底面17形成用於容納發光單元(未圖式,如LED)之凹槽10,凹槽10的位置在光學透鏡之中央,可容納尺寸約10.5mm至25mm的LED,且其深度朝遠離第二鏡體2的方向逐漸減少。此外,如第1和4A-4B圖所示,第一出光面11係呈兩側區112凸起而中央區111凹下之波浪狀,第二出光面12係呈兩側區122凸起而中央區121凹下之波浪狀。整體而言,第一出光面11、第二出光面12和緩衝面13與底面17基本構成了一個具有厚度之凸透鏡,該厚度朝遠離第二鏡體2的方向逐漸減少。 The first mirror body 1 includes a first light-emitting surface 11 , a second light-emitting surface 12 , a buffer surface 13 connecting the first light-emitting surface 11 and the second light-emitting surface 12 , and a first light-incident surface 14 opposite to the first light-emitting surface 11 . The second light incident surface 15 , the third light incident surface 16 opposite to the second light emitting surface 12 , and the bottom surface 17 connected to the first light incident surface 14 , the second light incident surface 15 , and the third light incident surface 16 . The first light incident surface 14 , the second light incident surface 15 , and the third light incident surface 16 are sequentially connected to form a recess 10 for accommodating a light emitting unit (not shown, such as an LED), the recess 10 Positioned in the center of the optical lens, it can accommodate LEDs having a size of about 10.5 mm to 25 mm, and its depth gradually decreases away from the second mirror body 2. In addition, as shown in FIGS. 1 and 4A-4B, the first light-emitting surface 11 has a wave shape in which the side regions 112 are convex and the central portion 111 is concave, and the second light-emitting surface 12 is formed by the two-side regions 122. The central area 121 has a concave wave shape. In general, the first light-emitting surface 11, the second light-emitting surface 12, and the buffer surface 13 and the bottom surface 17 substantially constitute a convex lens having a thickness which gradually decreases toward the second mirror body 2.

第一出光面11包含曲率R1和曲率R2,第二出光面12包含曲率R3,第一入光面14包含曲率R4、第二入光面15包含曲率R5,第三入光面16包含曲率R6和R7。所述出光面的曲率的大小依序為R1>R3>R2,所述入光面的曲 率的大小依序為R5>R4>R7>R6。於一例子中,曲率R1約93.2mm±2%,曲率R2約10.6mm±2%,曲率R3約13.3mm±2%,曲率R4約8.4mm±2%,曲率R5約20.4mm±2%,曲率R6約3.2mm±2%,曲率R7約7.6mm±2%。 The first light exit surface 11 includes a curvature R1 and a curvature R2, the second light exit surface 12 includes a curvature R3, the first light incident surface 14 includes a curvature R4, the second light incident surface 15 includes a curvature R5, and the third light incident surface 16 includes a curvature R6. And R7. The curvature of the light-emitting surface is sequentially R1>R3>R2, and the curved surface is curved. The magnitude of the rate is R5>R4>R7>R6. In one example, the curvature R1 is about 93.2 mm ± 2%, the curvature R2 is about 10.6 mm ± 2%, the curvature R3 is about 13.3 mm ± 2%, the curvature R4 is about 8.4 mm ± 2%, and the curvature R5 is about 20.4 mm ± 2%. The curvature R6 is about 3.2 mm ± 2%, and the curvature R7 is about 7.6 mm ± 2%.

第二鏡體2包括連接第二出光面12之外圍面21、相對於外圍面21且連接第三入光面16和底面17之第一內圍面22、及相對於外圍面21且非平坦(uneven)之第二內圍面23,第一內圍面22和第二內圍面23相連接以形成一空穴20,空穴20的深度朝遠離第一鏡體1的方向逐漸減少。於一例子中,第二內圍面23可形成有複數個連續的玻璃半圓柱(於圖中以格柵狀表示)於其上以使第二內圍面23成為非平坦。整體而言,第二鏡體2的形狀類似具有開口的長方體,除了該開口之外的五面構成外圍面21,而空穴20的形狀亦類似具有開口之長方體,除了該開口之外的五面中,作為空穴20的底部之一面231和面對第一鏡體1之一面232構成第二內圍面23,其餘三面構成第一內圍面22。 The second mirror body 2 includes a peripheral surface 21 connecting the second light-emitting surface 12, a first inner circumferential surface 22 connected to the peripheral surface 21 and connecting the third light-incident surface 16 and the bottom surface 17, and a non-flat surface with respect to the peripheral surface 21 The second inner peripheral surface 23 of the second inner peripheral surface 22 and the second inner peripheral surface 23 are joined to form a cavity 20, and the depth of the cavity 20 gradually decreases toward the direction away from the first mirror body 1. In one example, the second inner peripheral surface 23 may be formed with a plurality of continuous glass semi-cylinders (shown in a grid in the figure) thereon to make the second inner peripheral surface 23 non-flat. In general, the shape of the second mirror body 2 is similar to a rectangular parallelepiped having an opening, the five faces other than the opening constitute the peripheral surface 21, and the shape of the cavity 20 is similar to a rectangular parallelepiped having an opening, except for the opening In the surface, the bottom surface 231 as the bottom of the cavity 20 and the surface 232 facing the first mirror body 1 constitute the second inner circumferential surface 23, and the remaining three surfaces constitute the first inner circumferential surface 22.

安裝體3環繞並連接於第一鏡體1和第二鏡體2,並包括與第一出光面11、第二出光面12、緩衝面13、外圍面21連接之第一面31、相對於第一面31且連接底面17及第二內圍面23之第二面32、連接第一面31和第二面32之側面33、形成於側面33供螺絲穿過之安裝孔34、形成於第二面32供發光單元(LED)的導線穿出之出線槽35。安裝體3相對於相連接的第一鏡體1和第二鏡體2為向外延伸。 The mounting body 3 surrounds and is connected to the first mirror body 1 and the second mirror body 2, and includes a first surface 31 connected to the first light-emitting surface 11, the second light-emitting surface 12, the buffer surface 13, and the peripheral surface 21, with respect to a first surface 31 and a second surface 32 connecting the bottom surface 17 and the second inner circumferential surface 23, a side surface 33 connecting the first surface 31 and the second surface 32, and a mounting hole 34 formed on the side surface 33 for the screw to pass therethrough The second face 32 is for the wire exit slot 35 through which the wires of the light-emitting unit (LED) pass. The mounting body 3 extends outward relative to the first mirror body 1 and the second mirror body 2 that are connected.

第二鏡體2與第一鏡體1相比,第二鏡體2相對於安裝體3之高度大於第一鏡體1的厚度,且空穴20的深度大於凹槽10的深度。 The height of the second mirror body 2 relative to the mounting body 3 is greater than the thickness of the first mirror body 1 and the depth of the cavity 20 is greater than the depth of the groove 10, compared to the first mirror body 1.

參閱第5圖,為避免圖式過於複雜,第5圖僅概略表示本實施例之光學透鏡的光線路徑,關於光學透鏡之元件符號請參閱第1-4C圖。一發光單元(未圖示)置於凹槽10中,從該發光單元射出之光線大多經過第一入光面14、第二入光面15或第三入光面16進入第一鏡體1,再經過第一出光面11、第二出光面12或緩衝面13離開第一鏡體1,且在進入及離開第一鏡體1時光線皆會發生折射,以大體上從第一鏡體1朝遠離第二鏡體2的方向射出,因此,本實施例之光學透鏡主要由第一鏡體1出光。其次,極少數的光線可能會經由第一鏡體1進入第二鏡體2,惟,第二鏡體2之外圍面21、第一內圍面22和第二內圍面23之曲率係經設計以使進入第二鏡體2的光線發生全反射,進而導入安裝體3而穿出,故不會影響到第一鏡體1的出光。再其次,漏未進入第一鏡體1的光線或可直接進入了第二鏡體2,惟,第二鏡體2的第二內圍面23上的不平坦部分能使入射於其上的光線不發生反射而直接穿出第二鏡體2,也就是說,第二鏡體2可將沒有進入第一鏡體1的光線散射掉,故,也不會影響到第一鏡體1的出光。 Referring to Fig. 5, in order to avoid the complexity of the drawing, Fig. 5 only schematically shows the light path of the optical lens of the present embodiment. For the symbol of the optical lens, please refer to Fig. 1-4C. An illuminating unit (not shown) is disposed in the recess 10, and the light emitted from the illuminating unit enters the first mirror body 1 through the first light incident surface 14, the second light incident surface 15 or the third light incident surface 16 . And then exiting the first mirror body 1 through the first light-emitting surface 11, the second light-emitting surface 12 or the buffer surface 13, and the light is refracted when entering and leaving the first mirror body 1 to substantially circulate from the first mirror body. 1 is emitted away from the second mirror body 2, and therefore, the optical lens of the present embodiment is mainly emitted by the first mirror body 1. Secondly, a very small amount of light may enter the second mirror body 2 via the first mirror body 1. However, the curvature of the peripheral surface 21, the first inner circumferential surface 22 and the second inner circumferential surface 23 of the second mirror body 2 is It is designed such that the light entering the second mirror body 2 is totally reflected and guided into the mounting body 3, so that the light emitted from the first mirror body 1 is not affected. Secondly, the light that has not entered the first mirror body 1 or directly enters the second mirror body 2, but the uneven portion on the second inner peripheral surface 23 of the second mirror body 2 can be incident thereon. The light does not reflect and directly passes through the second mirror body 2, that is, the second mirror body 2 can scatter the light that does not enter the first mirror body 1, so that the first mirror body 1 is not affected. sold out.

參閱第6圖,其概略表示本實施例之光學透鏡的光通量分佈圖。於本實施例中,光學透鏡覆蓋LED經具體執行為路燈,橫軸表示路燈所在的道路寬度與燈具高度之比 例,縱軸表示利用係數(coefficients of utilization),其為光線照射到工作面上的光通量(flux)相較於燈具全部光通量之比。由第6圖可看出,HS(House Side)線的光通量比例較SS(Stree Side)線的光通量比例低,表示本實施例之路燈的光線大多照射在道路上。因此,根據第5和6圖可知,本案之光學透鏡主要透過第一鏡體1出光而照射在道路側,第二鏡體2可散射光線以使其避免照射在房屋側。 Referring to Fig. 6, there is schematically shown a luminous flux distribution diagram of the optical lens of the present embodiment. In this embodiment, the optical lens covering LED is specifically implemented as a street light, and the horizontal axis represents the ratio of the road width where the street light is located to the height of the light. For example, the vertical axis represents the coefficient of utilization, which is the ratio of the flux of light that impinges on the working surface to the total luminous flux of the luminaire. As can be seen from Fig. 6, the luminous flux ratio of the HS (House Side) line is lower than the luminous flux ratio of the SS (Stree Side) line, indicating that the light of the street lamp of the present embodiment is mostly irradiated on the road. Therefore, according to the fifth and sixth figures, the optical lens of the present invention is mainly irradiated on the road side through the first mirror body 1, and the second mirror body 2 can scatter light so as not to be irradiated on the house side.

接著參閱第7A-7D圖,第7A和7B圖顯示通過水平角0°-180°和180°-0°的垂直面(vertical plane through horizontal angles)之光強度分佈,對照至第3圖,光學透鏡之光軸為垂直出射圖式面的軸,通過水平角0°-180°和180°-0°的垂直面為切過A-A剖面線的面。由第3和7A-7B圖可知,本實施例之光學透鏡的光強度主要分佈在偏離光軸約30度之處,也就是往第一鏡體1的方向。另對照至第3圖,以A-A剖面線的右端穿過第一鏡體1之處視為水平角0度,A-A剖面線的左端穿過第二鏡體2之處為水平角180度,則第7C圖顯示通過水平角45°-225°的垂直面之光強度分佈圖。再參閱第7D圖,其為通過垂直角60度的水平錐體(horizontal cone through vertical angle)之光強度分佈圖,光線自光學透鏡射出所形成的圓錐體在垂直角60度而水平角90度之處約有最大燭光767 cd,且從第7D圖可看出本實施例之出光主要在第一鏡體1,尤其主要從第一鏡體1的兩側區112和122出光。 Referring next to Figures 7A-7D, Figures 7A and 7B show light intensity distributions through vertical planes of horizontal angles of 0°-180° and 180°-0°, contrast to Figure 3, optics The optical axis of the lens is the axis perpendicular to the exit pattern plane, and the vertical plane passing through the horizontal angles of 0°-180° and 180°-0° is the plane cut through the AA hatching. As can be seen from the figures 3 and 7A-7B, the light intensity of the optical lens of the present embodiment is mainly distributed at about 30 degrees from the optical axis, that is, toward the first mirror body 1. In addition, to the third figure, the right end of the AA hatching line passes through the first mirror body 1 as a horizontal angle of 0 degrees, and the left end of the AA hatching line passes through the second mirror body 2 at a horizontal angle of 180 degrees. Figure 7C shows a light intensity distribution through a vertical plane with a horizontal angle of 45° - 225°. Referring again to Fig. 7D, which is a light intensity distribution diagram of a horizontal cone through vertical angle of 60 degrees, the cone formed by the light from the optical lens is at a vertical angle of 60 degrees and a horizontal angle of 90 degrees. There is about a maximum candle light of 767 cd, and it can be seen from Fig. 7D that the light emitted by this embodiment is mainly in the first mirror body 1, especially from the two side regions 112 and 122 of the first mirror body 1.

第1-7D圖已說明本案之第一實施例的光學透鏡的基 本結構及出光或配光示意圖,由上述可知本實施例之光學透鏡之光束水平角可達171.6度±10%,光束垂直角可達160度±10%。 Figures 1-7D have illustrated the base of the optical lens of the first embodiment of the present invention. According to the structure and the light-emitting or light-distributing diagram, it can be seen from the above that the horizontal angle of the beam of the optical lens of the embodiment can reach 171.6 degrees ± 10%, and the vertical angle of the light beam can reach 160 degrees ± 10%.

第二實施例 Second embodiment

參閱第8-11C圖,其分別繪示本案第二實施例的光學透鏡之立體圖、仰式圖、俯視圖、A-A剖面圖、B-B剖面圖和曲率示意圖。 Referring to FIGS. 8-11C, a perspective view, an elevation view, a top view, an A-A cross-sectional view, a B-B cross-sectional view, and a curvature diagram of the optical lens of the second embodiment of the present invention are respectively illustrated.

於本實施例中,光學透鏡包括第一鏡體4、第二鏡體5及安裝體6。 In the embodiment, the optical lens includes a first mirror body 4, a second mirror body 5, and a mounting body 6.

第一鏡體4包括出光面41、相對於出光面41之第一入光面42、第二入光面43和非平坦的第三入光面44、及與第一入光面42、第二入光面43及第三入光面44連接之底面45。第一入光面42、第二入光面43及第三入光面44依序連接以於底面45形成用於容納發光單元(未圖式,如LED)之凹槽40,凹槽40的位置在光學透鏡之中央,可容納尺寸約10.5mm至25mm的LED,且其深度朝遠離第二鏡體5的方向逐漸減少。於一例子中,第三入光面44可形成有複數個連續的玻璃半圓柱(於圖中以格柵狀表示)於其上以使第三入光面44成為非平坦。此外,出光面41包含平面區411及在平面區411周圍並與安裝體3連接之弧面區412。整體而言,出光面41與底面45基本構成了一個具有厚度之凸透鏡,該厚度朝遠離第二鏡體5的方向逐漸減少。 The first mirror body 4 includes a light-emitting surface 41, a first light-incident surface 42 with respect to the light-emitting surface 41, a second light-incident surface 43 and a non-flat third light-incident surface 44, and a first light-incident surface 42, The bottom surface 45 to which the second light incident surface 43 and the third light incident surface 44 are connected. The first light incident surface 42 , the second light incident surface 43 , and the third light incident surface 44 are sequentially connected to form a recess 40 for accommodating the light emitting unit (not shown, such as an LED) on the bottom surface 45, the recess 40 Positioned in the center of the optical lens, it can accommodate LEDs having a size of about 10.5 mm to 25 mm, and its depth gradually decreases away from the second mirror body 5. In one example, the third light incident surface 44 may be formed with a plurality of continuous glass semi-cylinders (shown in a grid in the figure) thereon to make the third light incident surface 44 non-flat. Further, the light exit surface 41 includes a flat area 411 and a curved surface area 412 around the flat area 411 and connected to the mounting body 3. In general, the light-emitting surface 41 and the bottom surface 45 substantially constitute a convex lens having a thickness which gradually decreases toward the direction away from the second mirror body 5.

出光面41的弧面區412包含曲率R8,第一入光面42 包含曲率R9、第二入光面43包含曲率R10,所述入光面的曲率的大小依序為R10>R9。於一例子中,曲率R8約16.4mm±2%、曲率R9約16.41mm±2%、曲率R10約306.35mm±2%。 The curved surface area 412 of the light exit surface 41 includes a curvature R8, and the first light incident surface 42 The curvature R9 is included, and the second light incident surface 43 includes a curvature R10. The magnitude of the curvature of the light incident surface is R10>R9. In one example, the curvature R8 is about 16.4 mm ± 2%, the curvature R9 is about 16.41 mm ± 2%, and the curvature R10 is about 306.35 mm ± 2%.

第二鏡體5包括連接出光面41之外圍面51及相對於外圍面51之第一內圍面52和非平坦的第二內圍面53,第一內圍面52和第二內圍53朝相連接以形成空穴50,其深度朝遠離第一鏡體4的方向逐漸減少。於一例子中,第二內圍面53可形成有複數個連續的玻璃半圓柱(於圖中以格柵狀表示)於其上以使第二內圍面53成為非平坦。整體而言,第二鏡體5的形狀類似具有開口的長方體,除了該開口之外的五面構成外圍面51,而空穴50的形狀亦類似具有開口之長方體,除了該開口之外的五面中,作為空穴50的底部之一面531和面對第一鏡體1之一面532構成第二內圍面53,其餘三面構成第一內圍面52。 The second mirror body 5 includes a peripheral surface 51 connecting the light exit surface 41 and a first inner circumferential surface 52 opposite to the peripheral surface 51 and a non-flat second inner circumferential surface 53, the first inner circumferential surface 52 and the second inner circumference 53 The phases are joined to form a cavity 50 whose depth gradually decreases in a direction away from the first mirror body 4. In one example, the second inner peripheral surface 53 may be formed with a plurality of continuous glass semi-cylinders (shown in a grid in the figure) thereon to make the second inner circumferential surface 53 non-flat. In general, the shape of the second mirror body 5 is similar to a rectangular parallelepiped having an opening, and the five faces other than the opening constitute the peripheral surface 51, and the shape of the cavity 50 is similar to a rectangular parallelepiped having an opening, except for the opening In the surface, the bottom surface 531 as the bottom of the cavity 50 and the surface 532 facing the first mirror body 1 constitute the second inner circumferential surface 53, and the remaining three surfaces constitute the first inner circumferential surface 52.

安裝體6環繞且連接於第一鏡體4和第二鏡體5,並包括安裝部61及連接安裝部61、第一鏡體4及第二鏡體5之連接部62。安裝部61包括連接第二鏡體5和連接部62之第一面611、相對第一面611且與底面45和第二內圍面53連接之第二面612、連接第一面611和第二面612之側面613、形成於側面613供螺絲穿過之安裝孔614及形成於該第二面供發光單元(LED)的導線穿出之出線槽615。安裝體6相對於相連接的第一鏡體4和第二鏡體5為向外延伸。 The mounting body 6 is wound around and connected to the first mirror body 4 and the second mirror body 5, and includes a mounting portion 61 and a connecting portion 62 connecting the mounting portion 61, the first mirror body 4, and the second mirror body 5. The mounting portion 61 includes a first surface 611 connecting the second mirror body 5 and the connecting portion 62, a second surface 612 opposite to the first surface 611 and connected to the bottom surface 45 and the second inner circumferential surface 53, and a first surface 611 and a first surface The side surface 613 of the two sides 612 is formed on the side surface 613 for the screw to pass through the mounting hole 614 and the wire slot 615 formed by the wire for forming the light emitting unit (LED) on the second surface. The mounting body 6 extends outwardly relative to the first mirror body 4 and the second mirror body 5 that are connected.

第二鏡體5與第一鏡體4相比,第二鏡體5相對於安裝體6之高度大於第一鏡體4的厚度,且空穴50的深度大於凹槽40的深度。 The height of the second mirror body 5 relative to the mounting body 6 is greater than the thickness of the first mirror body 4, and the depth of the cavity 50 is greater than the depth of the groove 40, compared to the first mirror body 4.

參閱第12圖,為避免圖式過於複雜,第12圖僅概略表示本實施例之光學透鏡的光線路徑,關於光學透鏡之元件符號請參閱第8-11C圖。一發光單元(未圖示)置於凹槽40中,從該發光單元射出之光線大多經過第一入光面42或第二入光面43進入第一鏡體4,再經過出光面41離開第一鏡體4,且在進入及離開第一鏡體4時光線皆會發生折射,以大體上從第一鏡體4往遠離第二鏡體5的方向射出,因此,本實施例之光學透鏡主要由第一鏡體4出光。其次,極少數的光線可能會經由第一鏡體4的第三入光面44進入第二鏡體5,惟,第三入光面44的不平坦部分可讓入射於上的光線不發生反射而直接穿入第二鏡體5,而第二鏡體5之外圍面51、第一內圍面52和第二內圍面53之曲率係經設計以將進入第二鏡體5的光線在第二透鏡5內發生全反射,進而導入安裝體6而穿出,故不會影響到第一鏡體4的出光。或者,第二鏡體5的第二內圍面53上的不平坦部分能使入射於其上的光線不發生反射而直接穿出第二鏡體5,也就是說,第二鏡體5可將光線散射掉,故,也不會影響到第一鏡體5的出光。 Referring to Fig. 12, in order to avoid the complexity of the drawing, Fig. 12 only schematically shows the light path of the optical lens of the present embodiment. For the symbol of the optical lens, please refer to Fig. 8-11C. A light-emitting unit (not shown) is disposed in the recess 40, and the light emitted from the light-emitting unit enters the first mirror body 4 through the first light-incident surface 42 or the second light-incident surface 43 and exits through the light-emitting surface 41. The first mirror body 4, when entering and leaving the first mirror body 4, refracts light to substantially exit from the first mirror body 4 in a direction away from the second mirror body 5. Therefore, the optical body of the embodiment The lens is mainly emitted by the first mirror body 4. Secondly, a very small amount of light may enter the second mirror body 5 via the third light incident surface 44 of the first mirror body 4. However, the uneven portion of the third light incident surface 44 allows the incident light to be reflected. The second mirror body 5 is directly penetrated, and the curvatures of the peripheral surface 51, the first inner circumferential surface 52 and the second inner circumferential surface 53 of the second mirror body 5 are designed to pass the light entering the second mirror body 5 at Since the second lens 5 is totally reflected in the inside of the second lens 5 and is guided into the mounting body 6, it does not affect the light emitted from the first mirror body 4. Alternatively, the uneven portion on the second inner peripheral surface 53 of the second mirror body 5 can cause the light incident thereon to be directly reflected out of the second mirror body 5 without being reflected, that is, the second mirror body 5 can be The light is scattered, so that the light from the first mirror 5 is not affected.

參閱第13圖,其概略表示本實施例之光學透鏡的光通量分佈圖。於本實施例中,光學透鏡覆蓋LED經具體執行為路燈,橫軸表示路燈所在的道路寬度與燈具高度之比 例,縱軸表示利用係數(coefficients of utilization),其為光線照射到工作面上的光通量(flux)相較於燈具全部光通量之比。由第13圖可看出,HS(House Side)線的光通量比例較SS(Stree Side)線的光通量比例低,表示本實施例之路燈的光線大多照射在道路上。因此,根據第12和13圖可知,本案之光學透鏡主要透過第一鏡體出光而照射在道路側,第二鏡體可散射光線以使其避免照射在房屋側。 Referring to Fig. 13, there is schematically shown a luminous flux distribution diagram of the optical lens of the present embodiment. In this embodiment, the optical lens covering LED is specifically implemented as a street light, and the horizontal axis represents the ratio of the road width where the street light is located to the height of the light. For example, the vertical axis represents the coefficient of utilization, which is the ratio of the flux of light that impinges on the working surface to the total luminous flux of the luminaire. As can be seen from Fig. 13, the luminous flux ratio of the HS (House Side) line is lower than the luminous flux ratio of the SS (Stree Side) line, indicating that the light of the street lamp of the present embodiment is mostly irradiated on the road. Therefore, according to the figures 12 and 13, the optical lens of the present invention is mainly irradiated on the road side through the first mirror body, and the second mirror body can scatter light so as to avoid being irradiated on the house side.

接著參閱第14A-14D圖,第14A和14B圖顯示通過水平角0°-180°和180°-0°的垂直面(vertical plane through horizontal angles)之光強度分佈,對照至第10圖,光學透鏡之光軸為垂直出射圖式面的軸,通過水平角0°-180°和180°-0°的垂直面切過A-A剖面線。由第10和14A-14B圖可知,本實施例之光學透鏡的光強度主要分佈在偏離光軸約60度之處,也就是往第一鏡體4的方向。另對照至第10圖,以A-A剖面線的右端穿過第一鏡體4之處視為水平角0度,A-A剖面線的左端穿過第二鏡體5之處為水平角180度,則第14C圖顯示通過水平角45°-225°的垂直面之光強度分佈圖。再參閱第14D圖,其為通過垂直角70度的水平錐體(horizontal cone through vertical angle)之光強度分佈圖,光線自光學透鏡射出所形成的圓錐體在垂直角70度而水平角30度之處約有最大燭光994 cd,且從第14D圖可看出本實施例之出光主要在第一鏡體4,尤其主要從第一鏡體4的弧面區412出光。 Referring next to Figures 14A-14D, Figures 14A and 14B show light intensity distributions through vertical planes of horizontal angles of 0°-180° and 180°-0°, contrast to Figure 10, optics The optical axis of the lens is the axis of the vertical exit pattern plane, and the AA hatching is cut through the vertical planes of the horizontal angles of 0°-180° and 180°-0°. As can be seen from the figures 10 and 14A-14B, the light intensity of the optical lens of the present embodiment is mainly distributed at about 60 degrees from the optical axis, that is, toward the first mirror body 4. In addition, to the 10th figure, the right end of the AA hatching line passes through the first mirror body 4 as a horizontal angle of 0 degrees, and the left end of the AA hatching line passes through the second mirror body 5 at a horizontal angle of 180 degrees. Figure 14C shows the light intensity distribution through a vertical plane with a horizontal angle of 45° - 225°. Referring again to Figure 14D, which is a light intensity distribution diagram of a horizontal cone through vertical angle of 70 degrees, the cone formed by the light from the optical lens is at a vertical angle of 70 degrees and a horizontal angle of 30 degrees. The maximum candle light is about 994 cd, and it can be seen from Fig. 14D that the light emitted by the present embodiment is mainly emitted from the first mirror body 4, especially from the arc surface area 412 of the first mirror body 4.

第8-14D圖已說明本案之第二實施例的光學透鏡的基 本結構及出光或配光示意圖,由上述可知本實施例之光學透鏡之光束水平角可達107.9度±10%,光束垂直角可達152.8度±10%。 Figures 8-14D have illustrated the base of the optical lens of the second embodiment of the present invention. According to the structure and the light-emitting or light-distributing diagram, it can be seen from the above that the horizontal angle of the beam of the optical lens of the embodiment can reach 107.9 degrees ± 10%, and the vertical angle of the light beam can reach 152.8 degrees ± 10%.

綜上所述,本案之各實施例的光學透鏡能將往房屋側之光線散射,而使光線往道路側照射,且往道路側照射之光線相對於中央較集中於兩側,藉此獲得較大的水平光束角。 In summary, the optical lens of each embodiment of the present invention can scatter light to the side of the house, and illuminate the light toward the road side, and the light illuminating the road side is concentrated on both sides with respect to the center, thereby obtaining Large horizontal beam angle.

上述實施樣態僅例示性說明本案之功效,而非用於限制本案,任何熟習此項技藝之人士均可在不違背本案之精神及範疇下,對上述該些實施態樣進行修飾與改變。此外,在上述該些實施態樣中之結構的數目僅為例示性說明,亦非用於限制本案。因此本案之權利保護範圍,應如後述之申請專利範圍所列。 The above-described embodiments are merely illustrative of the effects of the present invention, and are not intended to limit the scope of the present invention, and those skilled in the art can modify and modify the above-described embodiments without departing from the spirit and scope of the present invention. Moreover, the number of structures in the above-described embodiments is merely illustrative and is not intended to limit the present invention. Therefore, the scope of protection of the rights in this case should be listed in the scope of the patent application mentioned later.

1‧‧‧第一鏡體 1‧‧‧ first mirror

2‧‧‧第二鏡體 2‧‧‧Second mirror

3‧‧‧安裝體 3‧‧‧Installation

Claims (10)

一種光學透鏡,係供覆蓋於發光單元上,該光學透鏡包括:第一鏡體,係包括第一出光面、第二出光面、相對於該第一出光面之第一入光面及第二入光面、相對於該第二出光面之第三入光面、及與該第一入光面、該第二入光面和該第三入光面連接之底面,該第一入光面、該第二入光面和該第三入光面依序連接以於該底面形成用於容納該發光單元之凹槽;第二鏡體,係連接該第一鏡體,並包括連接該第二出光面之外圍面、相對於該外圍面之第一內圍面及非平坦的第二內圍面,該第一內圍面和該第二內圍面相連接以形成空穴,且該第一內圍面連接該底面及該第三入光面;以及安裝體,係環繞且連接於該第一鏡體和該第二鏡體,並相對於該第一鏡體和該第二鏡體向外延伸。 An optical lens for covering a light-emitting unit, the optical lens comprising: a first mirror body, comprising a first light-emitting surface, a second light-emitting surface, a first light-incident surface relative to the first light-emitting surface, and a second a first light incident surface, a third light incident surface opposite to the second light emitting surface, and a bottom surface connected to the first light incident surface, the second light incident surface, and the third light incident surface The second light incident surface and the third light incident surface are sequentially connected to form a recess for receiving the light emitting unit on the bottom surface; the second mirror body is connected to the first mirror body, and includes the connection a peripheral surface of the second light exiting surface, a first inner circumferential surface opposite to the outer peripheral surface, and a non-flat second inner circumferential surface, the first inner circumferential surface and the second inner circumferential surface are connected to form a cavity, and the first An inner peripheral surface connecting the bottom surface and the third light incident surface; and a mounting body surrounding and connected to the first mirror body and the second mirror body, and opposite to the first mirror body and the second mirror body Extend outward. 如申請專利範圍第1項之光學透鏡,其中,該第一出光面包含第一曲率和第二曲率、該第二出光面包含第三曲率、該第一入光面包含第四曲率、該第二入光面包含第五曲率、該第三入光面包含第六曲率和第七曲率;其中,該第一曲率大於該第三曲率、該第三曲率大於該第二曲率,且該第五曲率大於該第四曲率、該第四曲率大於該第七曲率、該第七曲率大於該第六曲率;該光學透鏡包含171.6度±10%之水平光束角以及 160度±10%之垂直光束角。 The optical lens of claim 1, wherein the first light-emitting surface comprises a first curvature and a second curvature, the second light-emitting surface comprises a third curvature, and the first light-incident surface comprises a fourth curvature, the first The second light entrance surface includes a fifth curvature, the third light incident surface includes a sixth curvature and a seventh curvature; wherein the first curvature is greater than the third curvature, the third curvature is greater than the second curvature, and the fifth The curvature is greater than the fourth curvature, the fourth curvature is greater than the seventh curvature, and the seventh curvature is greater than the sixth curvature; the optical lens comprises a horizontal beam angle of 171.6 degrees ± 10% and Vertical beam angle of 160 degrees ± 10%. 如申請專利範圍第1項之光學透鏡,其中,該第一出光面及該第二出光面之各者係兩側為凸而中央為凹之波浪狀;其中,該第二鏡體相對於該安裝體之高度大於該第一鏡體之厚度,且該第一鏡體之該厚度朝遠離該第二鏡體的方向逐漸減少,而該空穴的深度大於該凹槽的深度,該空穴之該深度朝遠離該第一鏡體的方向逐漸減少,該凹槽之該深度朝遠離該第二鏡體的方向逐漸減少。 The optical lens of claim 1, wherein each of the first light-emitting surface and the second light-emitting surface is convex and has a concave wave shape at the center; wherein the second mirror body is opposite to the The height of the mounting body is greater than the thickness of the first mirror body, and the thickness of the first mirror body gradually decreases away from the second mirror body, and the depth of the cavity is greater than the depth of the groove, the cavity The depth gradually decreases toward a direction away from the first mirror body, and the depth of the groove gradually decreases toward a direction away from the second mirror body. 如申請專利範圍第1項之光學透鏡,其中,該安裝體包括與該第一出光面、該第二出光面及該外圍面連接之第一面、與該底面和該第二內圍面連接之第二面、連接該第一面和該第二面之側面、形成於該側面之安裝孔及形成於該第二面之出線槽。 The optical lens of claim 1, wherein the mounting body comprises a first surface connected to the first light emitting surface, the second light emitting surface and the peripheral surface, and the bottom surface and the second inner circumferential surface are connected The second surface, the side surface connecting the first surface and the second surface, the mounting hole formed on the side surface, and the outlet groove formed on the second surface. 如申請專利範圍第1項之光學透鏡,其中,該光學透鏡之材料包括玻璃;其中,該第二內圍面形成有複數個玻璃製半圓柱體於其上,以導致該第二內圍面的非平坦。 The optical lens of claim 1, wherein the material of the optical lens comprises glass; wherein the second inner peripheral surface is formed with a plurality of glass semi-cylindrical bodies thereon to cause the second inner circumferential surface Non-flat. 一種光學透鏡,係供覆蓋於發光單元上,該光學透鏡包括:第一鏡體,係包括出光面、相對於該出光面之第一入光面、第二入光面和非平坦的第三入光面、及與該第一入光面、第二入光面及第三入光面連接之底面,該第一入光面、第二入光面及第三入光面依序連 接以於該底面形成用於容納該發光單元之凹槽;第二鏡體,係連接該第一鏡體,並包括連接該出光面之外圍面及相對於該外圍面之第一內圍面和非平坦的第二內圍面,該第一內圍面和該第二內圍朝相連接以形成空穴,且該第一內圍面連接該底面;以及安裝體,係環繞且連接於該第一鏡體和該第二鏡體,並相對於該第一鏡體和該第二鏡體向外延伸。 An optical lens for covering a light-emitting unit, the optical lens comprising: a first mirror body, comprising a light-emitting surface, a first light-incident surface opposite to the light-emitting surface, a second light-incident surface, and a non-flat third a light incident surface, and a bottom surface connected to the first light incident surface, the second light incident surface, and the third light incident surface, wherein the first light incident surface, the second light incident surface, and the third light incident surface are sequentially connected Forming a recess for receiving the light emitting unit on the bottom surface; the second mirror body is connected to the first mirror body, and includes a peripheral surface connecting the light exiting surface and a first inner circumferential surface opposite to the peripheral surface And a non-flat second inner circumferential surface, the first inner circumferential surface and the second inner circumferential surface are connected to form a cavity, and the first inner circumferential surface is connected to the bottom surface; and the mounting body is surrounded and connected The first mirror body and the second mirror body extend outward relative to the first mirror body and the second mirror body. 如申請專利範圍第6項之光學透鏡,其中,該出光面包含第八曲率,該第一入光面包含第九曲率,該第二入光面包含第十曲率;其中,該第十曲率大於該第九曲率;該光學透鏡包含107.9度±10%之水平光束角及152.8度±10%之垂直光束角。 The optical lens of claim 6, wherein the light exiting surface comprises an eighth curvature, the first light incident surface comprises a ninth curvature, and the second light incident surface comprises a tenth curvature; wherein the tenth curvature is greater than The ninth curvature; the optical lens comprises a horizontal beam angle of 107.9 degrees ± 10% and a vertical beam angle of 152.8 degrees ± 10%. 如申請專利範圍第6項之光學透鏡,其中,該第二鏡體相對於該安裝體之高度大於該第一鏡體之厚度,且該第一鏡體之該厚度朝遠離該第二鏡體的方向逐漸減少,而該空穴的深度大於該凹槽的深度,該空穴之該深度朝遠離該第一鏡體的方向逐漸減少,該凹槽之該深度朝遠離該第二鏡體的方向逐漸減少。 The optical lens of claim 6, wherein the height of the second mirror body relative to the mounting body is greater than the thickness of the first mirror body, and the thickness of the first mirror body is away from the second mirror body. The direction of the hole is gradually reduced, and the depth of the cavity is greater than the depth of the groove, the depth of the hole gradually decreasing toward a direction away from the first mirror body, the depth of the groove being away from the second mirror body The direction is gradually decreasing. 如申請專利範圍第6項之光學透鏡,其中,該安裝體包括安裝部及連接該安裝部、該第一鏡體及該第二鏡體之連接部,該安裝部包括與該連接部和該外圍面連接之第一面、與該底面和該第二內圍面連接之第二面、連接該第一面和該第二面之側面、形成於該側面之安裝孔及形成於該第二面之出線槽。 The optical lens of claim 6, wherein the mounting body includes a mounting portion and a connecting portion connecting the mounting portion, the first mirror body and the second mirror body, the mounting portion including the connecting portion and the connecting portion a first surface of the peripheral surface connection, a second surface connected to the bottom surface and the second inner circumferential surface, a side surface connecting the first surface and the second surface, and a mounting hole formed on the side surface and formed in the second surface Out of the line slot. 如申請專利範圍第6項之光學透鏡,該光學透鏡係由玻璃構成;其中,該第二內圍面及該第三入光面之各者形成有複數個玻璃製半圓柱體於其上,以分別導致該第二內圍面和該第三入光面的非平坦。 The optical lens of claim 6, wherein the optical lens is made of glass; wherein each of the second inner circumferential surface and the third light incident surface is formed with a plurality of glass semi-cylindrical bodies thereon, To cause the second inner peripheral surface and the third light incident surface to be uneven.
TW104214752U 2015-09-11 2015-09-11 Optical lens TWM516690U (en)

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