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CN111928203A - Optical lens and light-emitting device - Google Patents

Optical lens and light-emitting device Download PDF

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CN111928203A
CN111928203A CN202010744829.8A CN202010744829A CN111928203A CN 111928203 A CN111928203 A CN 111928203A CN 202010744829 A CN202010744829 A CN 202010744829A CN 111928203 A CN111928203 A CN 111928203A
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optical lens
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CN111928203B (en
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冯奇斌
唐天
吕国强
王梓
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Hefei University of Technology
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V5/00Refractors for light sources
    • F21V5/04Refractors for light sources of lens shape
    • F21V5/048Refractors for light sources of lens shape the lens being a simple lens adapted to cooperate with a point-like source for emitting mainly in one direction and having an axis coincident with the main light transmission direction, e.g. convergent or divergent lenses, plano-concave or plano-convex lenses
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21KNON-ELECTRIC LIGHT SOURCES USING LUMINESCENCE; LIGHT SOURCES USING ELECTROCHEMILUMINESCENCE; LIGHT SOURCES USING CHARGES OF COMBUSTIBLE MATERIAL; LIGHT SOURCES USING SEMICONDUCTOR DEVICES AS LIGHT-GENERATING ELEMENTS; LIGHT SOURCES NOT OTHERWISE PROVIDED FOR
    • F21K9/00Light sources using semiconductor devices as light-generating elements, e.g. using light-emitting diodes [LED] or lasers
    • F21K9/20Light sources comprising attachment means
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21YINDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO THE FORM OR THE KIND OF THE LIGHT SOURCES OR OF THE COLOUR OF THE LIGHT EMITTED
    • F21Y2115/00Light-generating elements of semiconductor light sources
    • F21Y2115/10Light-emitting diodes [LED]

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  • Physics & Mathematics (AREA)
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  • Optics & Photonics (AREA)
  • Planar Illumination Modules (AREA)
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Abstract

本发明提出一种光学透镜及发光装置,包括:光入射面,所述光入射面形成具有开口的凹穴,所述凹穴包括第一区域和第二区域,所述第二区域位于所述第一区域上;所述第一区域用于放置光源,所述光源发射的光线从所述第二区域入射;光出射面,包括一凹陷部,所述凹陷部位于所述凹穴上,所述凹穴与所述凹陷部的中心线与所述光学透镜的中心线重合;底表面,所述底表面连接所述光入射面和所述光出射面;其中,所述底表面包括至少一曲面,所述底表面包括至少一凹形区;部分所述光线从所述光出射面反射后朝向所述凹形区,进行折射,形成折射光线。本发明提出的光学透镜可以提高光斑的均匀性。

Figure 202010744829

The present invention provides an optical lens and a light-emitting device, comprising: a light incident surface, wherein a cavity with an opening is formed on the light incidence surface, the cavity includes a first area and a second area, and the second area is located in the on the first area; the first area is used to place a light source, and the light emitted by the light source is incident from the second area; the light exit surface includes a concave part, the concave part is located on the concave, so The center line of the cavity and the recessed portion coincides with the center line of the optical lens; a bottom surface, the bottom surface connects the light incident surface and the light exit surface; wherein, the bottom surface includes at least one A curved surface, the bottom surface includes at least one concave area; part of the light rays are reflected from the light exit surface and then face the concave area to be refracted to form refracted rays. The optical lens proposed by the present invention can improve the uniformity of the light spot.

Figure 202010744829

Description

一种光学透镜及发光装置Optical lens and light-emitting device

技术领域technical field

本发明涉及光学技术领域,特别涉及一种光学透镜及发光装置。The present invention relates to the field of optical technology, and in particular, to an optical lens and a light-emitting device.

背景技术Background technique

随着半导体照明技术的发展,发光二极管(Light emitting diode,LED)的光效不断提高,现正逐步取代传统光源。针对LED光源,如何有效地分配LED发出的光能是采用该LED光源的光学系统设计要解决的关键问题。目前的LED光源的出光均匀性不佳,为了实现更加均匀地照明,需要将LED光源发出的光进行调整。所以,有必要提供一种能提高光源的出光均匀性的光学透镜。With the development of semiconductor lighting technology, light emitting diodes (Light emitting diodes, LEDs) have been continuously improved in light efficiency, and are now gradually replacing traditional light sources. For the LED light source, how to effectively distribute the light energy emitted by the LED is a key problem to be solved in the design of the optical system using the LED light source. The light emitting uniformity of the current LED light source is not good. In order to achieve more uniform illumination, the light emitted by the LED light source needs to be adjusted. Therefore, it is necessary to provide an optical lens that can improve the uniformity of light output from the light source.

发明内容SUMMARY OF THE INVENTION

鉴于上述现有技术的缺陷,本发明提出一种光学透镜及发光装置,以提高光源利用率和提高出光均匀性。In view of the above-mentioned defects of the prior art, the present invention proposes an optical lens and a light-emitting device, so as to improve the utilization rate of the light source and the uniformity of light output.

为实现上述目的,本发明提出一种光学透镜,包括:In order to achieve the above object, the present invention provides an optical lens, comprising:

光入射面,所述光入射面形成具有开口的凹穴,所述凹穴包括第一区域和第二区域,所述第二区域位于所述第一区域上;所述第一区域用于放置光源,所述光源发射的光线从所述第二区域入射;a light incident surface, the light incident surface forms a cavity with an opening, the cavity includes a first area and a second area, the second area is located on the first area; the first area is used for placing a light source, the light emitted by the light source is incident from the second region;

光出射面,包括一凹陷部,所述凹陷部位于所述凹穴上,所述凹穴与所述凹陷部的中心线与所述光学透镜的中心线重合;The light exit surface includes a concave portion, the concave portion is located on the concave cavity, and the center line of the concave cavity and the concave portion coincides with the center line of the optical lens;

底表面,所述底表面连接所述光入射面和所述光出射面;a bottom surface, the bottom surface connects the light incident surface and the light exit surface;

其中,所述底表面包括至少一曲面,所述底表面包括至少一凹形区;部分所述光线从所述光出射面反射后朝向所述凹形区,进行折射,形成折射光线。Wherein, the bottom surface includes at least one curved surface, and the bottom surface includes at least one concave area; part of the light rays are reflected from the light exit surface toward the concave area, and are refracted to form refracted rays.

进一步地,所述光学透镜位于表面涂有反射材料的基板上,所述折射光线通过所述反射材料反射后朝向所述凹形区。Further, the optical lens is located on the substrate whose surface is coated with a reflective material, and the refracted light is reflected by the reflective material toward the concave area.

进一步地,当所述底表面为一曲面时,所述底表面的曲率半径小于(R2+d2)/8d,其中,R表示所述底表面的半宽,d表示所述反射材料至所述第一区域上表面的高度。Further, when the bottom surface is a curved surface, the radius of curvature of the bottom surface is less than (R 2 +d 2 )/8d, where R represents the half width of the bottom surface, and d represents the reflective material to The height of the upper surface of the first region.

进一步地,当所述底表面包括N个曲面时,所述N个曲面相互连接,且具有相同的形状;所述曲面的曲率半径的最大值

Figure BDA0002607984030000011
且r×N≤R≤r×(N+1);Further, when the bottom surface includes N curved surfaces, the N curved surfaces are connected to each other and have the same shape; the maximum value of the radius of curvature of the curved surfaces is
Figure BDA0002607984030000011
And r×N≤R≤r×(N+1);

其中,N≥2,R表示所述底表面的半宽,d表示所述反射材料至所述第一区域上表面的高度。Wherein, N≧2, R represents the half width of the bottom surface, and d represents the height of the reflective material to the upper surface of the first region.

进一步地,当所述底表面包括N个曲面时,所述N个曲面具有相同的形状,且所述N个曲面之间通过平面间隔,所述曲面的曲率半径的最大值

Figure BDA0002607984030000021
Further, when the bottom surface includes N curved surfaces, the N curved surfaces have the same shape, and the N curved surfaces are separated by plane intervals, and the maximum value of the curvature radius of the curved surfaces is
Figure BDA0002607984030000021

其中,N≥2,R表示所述底表面的半宽,d表示所述反射材料至所述第一区域上表面的高度,m表示所述平面的宽度。Wherein, N≧2, R represents the half width of the bottom surface, d represents the height of the reflective material to the upper surface of the first region, and m represents the width of the plane.

进一步地,当所述底表面包括N个曲面时,所述N个曲面具有不同的形状,且所述N个曲面之间通过平面间隔,所述曲面的曲率半径的最大值

Figure BDA0002607984030000022
Further, when the bottom surface includes N curved surfaces, the N curved surfaces have different shapes, and the N curved surfaces are separated by plane intervals, and the maximum value of the curvature radius of the curved surfaces is
Figure BDA0002607984030000022

其中,N≥2,R表示所述底表面的半宽,d表示所述反射材料至所述第一区域上表面的高度,m表示所述平面的宽度,α表示N个曲面中最小的曲面对应的圆心角,β表示N个曲面中最大的曲面对应的圆心角,r1表示N个曲面中最小的曲面的半径。Wherein, N≥2, R represents the half width of the bottom surface, d represents the height of the reflective material to the upper surface of the first region, m represents the width of the plane, and α represents the smallest curved surface among the N curved surfaces The corresponding central angle, β represents the central angle corresponding to the largest surface among the N surfaces, and r 1 represents the radius of the smallest surface among the N surfaces.

进一步地,所述凹穴的高度与所述第二端至所述凹陷的中心点的距离的比值在3-6之间。Further, the ratio of the height of the recess to the distance from the second end to the center point of the recess is between 3-6.

进一步地,所述光出射面还包括凸出部和垂直部,所述凸出部连接在所述凹陷部的外周。Further, the light exit surface further includes a protruding portion and a vertical portion, and the protruding portion is connected to the outer periphery of the recessed portion.

进一步地,所述凸出部的最高点至所述凹陷部的中心点的距离在0.5-0.8mm之间。Further, the distance from the highest point of the protruding portion to the center point of the concave portion is between 0.5-0.8 mm.

进一步地,所述垂直部平行于所述光学透镜的中心线,所述垂直部连接于所述凸出部的外周,所述凸出部通过所述垂直部与所述底表面连接。Further, the vertical portion is parallel to the center line of the optical lens, the vertical portion is connected to the outer periphery of the protruding portion, and the protruding portion is connected to the bottom surface through the vertical portion.

进一步地,所述第一区域的高度小于所述第二区域的高度。Further, the height of the first area is smaller than the height of the second area.

进一步地,所述垂直部的高度小于所述凹穴的高度。Further, the height of the vertical portion is smaller than the height of the cavity.

进一步地,本发明还提出一种发光装置,包括:Further, the present invention also provides a light-emitting device, comprising:

基板;substrate;

光源,设置在所述基板上;a light source, arranged on the substrate;

光学透镜,位于所述光源上;an optical lens on the light source;

其中,所述光学透镜包括:Wherein, the optical lens includes:

光入射面,所述光入射面形成具有开口的凹穴,所述凹穴包括第一区域和第二区域,所述第二区域位于所述第一区域上;所述第一区域用于放置光源,所述光源发射的光线从所述第二区域入射;a light incident surface, the light incident surface forms a cavity with an opening, the cavity includes a first area and a second area, the second area is located on the first area; the first area is used for placing a light source, the light emitted by the light source is incident from the second region;

光出射面,包括一凹陷部,所述凹陷部位于所述凹穴上,所述凹穴与所述凹陷部的中心线与所述光学透镜的中心线重合;The light exit surface includes a concave portion, the concave portion is located on the concave cavity, and the center line of the concave cavity and the concave portion coincides with the center line of the optical lens;

底表面,所述底表面连接所述光入射面和所述光出射面;a bottom surface, the bottom surface connects the light incident surface and the light exit surface;

其中,所述底表面包括至少一曲面,所述底表面包括至少一凹形区;部分所述光线从所述光出射面反射后朝向所述凹形区,进行折射,形成折射光线。Wherein, the bottom surface includes at least one curved surface, and the bottom surface includes at least one concave area; part of the light rays are reflected from the light exit surface toward the concave area, and are refracted to form refracted rays.

综上所述,本发明提出一种光学透镜及发光装置,通过在底表面设计成包括至少一个曲面,因此在底表面至少形成一个凹形区。当光源发射的光线经过光发射面反射后再次通过凹形区进行折射,形成折射光线,折射光线经过反射材料反射后再次通过凹形区,因此该凹形区可以对光线起到发散的作用,也就是对光线起到调控作用。因此,该光学透镜可以提高在目标平面上形成的光斑的均匀性,从而也可以提高光源的利用率。To sum up, the present invention provides an optical lens and a light-emitting device. By designing the bottom surface to include at least one curved surface, at least one concave area is formed on the bottom surface. When the light emitted by the light source is reflected by the light emitting surface, it is refracted through the concave area again to form a refracted light. The refracted light is reflected by the reflective material and then passes through the concave area again. Therefore, the concave area can play a role in diffusing the light. That is, it controls the light. Therefore, the optical lens can improve the uniformity of the light spot formed on the target plane, thereby also improving the utilization rate of the light source.

附图说明Description of drawings

图1:本实施例提出的光学透镜的整体图。FIG. 1 is an overall view of the optical lens proposed in this embodiment.

图2:图1的局部图。Figure 2: A partial view of Figure 1.

图3:图1的剖面图。Figure 3: Sectional view of Figure 1 .

图4:光源和第一区域的位置示意图。Figure 4: Schematic diagram of the location of the light source and the first region.

图5:光线从光出射面射出的图。Figure 5: Diagram of light rays exiting the light exit surface.

图6:光线从光出射面反射的图。Figure 6: Graph of light reflected from the light exit surface.

图7:底表面对光线调控的示意图。Figure 7: Schematic illustration of the regulation of light by the bottom surface.

图8:底面是平面和弧面的光斑亮度曲线对比图。Figure 8: The bottom surface is a comparison chart of the spot brightness curves of the flat and curved surfaces.

图9:阵列光源的简要示意图。Figure 9: Brief schematic of the array light source.

图10:阵列光源的仿真对比图。Figure 10: Simulation comparison diagram of the array light source.

图11:本实施例提出的光学透镜的剖面图。FIG. 11 is a cross-sectional view of the optical lens proposed in this embodiment.

图12:本实施例提出的光学透镜的另一剖面图。FIG. 12 is another cross-sectional view of the optical lens proposed in this embodiment.

图13:本实施例提出的光学透镜的另一剖面图。FIG. 13 is another cross-sectional view of the optical lens proposed in this embodiment.

图14:本实施例提出的发光装置的简要示意图。FIG. 14 is a schematic diagram of the light-emitting device proposed in this embodiment.

具体实施方式Detailed ways

以下通过特定的具体实例说明本发明的实施方式,本领域技术人员可由本说明书所揭露的内容轻易地了解本发明的其他优点与功效。本发明还可以通过另外不同的具体实施方式加以实施或应用,本说明书中的各项细节也可以基于不同观点与应用,在没有背离本发明的精神下进行各种修饰或改变。The embodiments of the present invention are described below through specific specific examples, and those skilled in the art can easily understand other advantages and effects of the present invention from the contents disclosed in this specification. The present invention can also be implemented or applied through other different specific embodiments, and various details in this specification can also be modified or changed based on different viewpoints and applications without departing from the spirit of the present invention.

需要说明的是,本实施例中所提供的图示仅以示意方式说明本发明的基本构想,遂图式中仅显示与本发明中有关的组件而非按照实际实施时的组件数目、形状及尺寸绘制,其实际实施时各组件的型态、数量及比例可为一种随意的改变,且其组件布局型态也可能更为复杂。It should be noted that the drawings provided in this embodiment are only to illustrate the basic concept of the present invention in a schematic way, so the drawings only show the components related to the present invention rather than the number, shape and the number of components in actual implementation. For dimension drawing, the type, quantity and proportion of each component can be changed at will in actual implementation, and the component layout may also be more complicated.

如图1-图2所示,本实施例提出一种光学透镜100,该光学透镜100包括光入射面101,光出射面102和底表面103。该光学透镜100为旋转对称结构,具有一个对称轴。该光入射面101形成一个具有开口的凹穴,因此可以将光源放置在凹穴内。光源发射的光线可以从光入射面101射入,然后从光出射面102出射。As shown in FIGS. 1-2 , this embodiment provides an optical lens 100 , and the optical lens 100 includes a light incident surface 101 , a light exit surface 102 and a bottom surface 103 . The optical lens 100 is a rotationally symmetric structure with an axis of symmetry. The light incident surface 101 forms a cavity with an opening, so that the light source can be placed in the cavity. The light emitted by the light source may enter from the light incident surface 101 and then exit from the light exit surface 102 .

如图1-图2所示,图2显示为光学透镜的局部三维图,在本实施例中,光出射面102位于光入射面101上,底表面103自光出射面102延伸出并与光入射面101连接。在本实施例中,该底表面103为曲面,该底表面103向光出射面102的方向凹进,也就是说底表面103向光学透镜100的内部凹进,因此该底表面103可以形成凹形区。As shown in FIG. 1-FIG. 2, FIG. 2 is a partial three-dimensional view of the optical lens. In this embodiment, the light exit surface 102 is located on the light entrance surface 101, and the bottom surface 103 extends from the light exit surface 102 and is connected to the light exit surface 102. The incident surface 101 is connected. In this embodiment, the bottom surface 103 is a curved surface, and the bottom surface 103 is concave in the direction of the light exit surface 102 , that is to say, the bottom surface 103 is concave toward the inside of the optical lens 100 , so the bottom surface 103 can form a concave shape area.

如图1-图3所示,图3显示为图1的剖面图。在本实施例中,该光学透镜100包括一中心线100a,该中心线100a也可以作为该光学透镜100的旋转轴。该光入射面101包括第一面101a和第二面101b,第二面101b位于第一面101a上。第一面101a为竖直面,第二面101b为曲面,第二面101b可以为自由曲面。经过中心线100a旋转之后,第一面101a形成第一区域11,第二面101b形成第二区域12,第二区域12位于第一区域11上,本实施例将第一区域11和第二区域12定义为凹穴10。在本实施例中,由于第一面101a为竖直面,因此第一区域11为圆柱状,因此第一区域11的内径保持不变。由于第二面101b为曲面,因此第二区域12的内径是变化的。第二区域12的内径从第一端向第二端逐渐变小,第二区域12与第一区域11接触的一端可以定义为第一端,第二区域12远离第一区域11的一端定义为第二端;同时第二端也可以定义为第二区域12的最高点。在本实施例中,第一区域11的内径小于3.6mm,例如为3.18mm,因此第二区域12的最大内径为3.18mm,也就是第一端的内径,第二区域12的最小内径为0,也就是第二端;也就是说第二区域12的内径从3.18mm逐渐减小至0。As shown in FIGS. 1-3 , FIG. 3 is a cross-sectional view of FIG. 1 . In this embodiment, the optical lens 100 includes a center line 100 a, and the center line 100 a can also be used as the rotation axis of the optical lens 100 . The light incident surface 101 includes a first surface 101a and a second surface 101b, and the second surface 101b is located on the first surface 101a. The first surface 101a is a vertical surface, the second surface 101b is a curved surface, and the second surface 101b may be a free-form surface. After the centerline 100a is rotated, the first surface 101a forms the first area 11, the second surface 101b forms the second area 12, and the second area 12 is located on the first area 11. In this embodiment, the first area 11 and the second area are 12 is defined as pocket 10 . In this embodiment, since the first surface 101a is a vertical surface, the first region 11 is cylindrical, and thus the inner diameter of the first region 11 remains unchanged. Since the second surface 101b is a curved surface, the inner diameter of the second region 12 varies. The inner diameter of the second area 12 gradually decreases from the first end to the second end, the end of the second area 12 in contact with the first area 11 can be defined as the first end, and the end of the second area 12 away from the first area 11 is defined as The second end; meanwhile, the second end can also be defined as the highest point of the second region 12 . In this embodiment, the inner diameter of the first region 11 is less than 3.6 mm, for example, 3.18 mm, so the maximum inner diameter of the second region 12 is 3.18 mm, which is the inner diameter of the first end, and the minimum inner diameter of the second region 12 is 0 , that is, the second end; that is, the inner diameter of the second region 12 gradually decreases from 3.18 mm to 0.

如图3图4所示,在本实施例中,光源105放置在第一区域11内,因此第一区域11的高度D也可以定义为光源105的厚度,也就是说光源105排列在第一区域11与第二区域12的连接面上。从图1中可以看出,第一区域11和第二区域12之间是联通的,因此可以将第二区域12的第一端定义为第一区域11和第二区域12的连接面。当光源105放置在第一区域11内时,光源105发射的光线L从连接面发射,从第二区域12入射。As shown in FIGS. 3 and 4 , in this embodiment, the light source 105 is placed in the first area 11 , so the height D of the first area 11 can also be defined as the thickness of the light source 105 , that is to say, the light source 105 is arranged in the first area 105 . The connecting surface of the region 11 and the second region 12 . It can be seen from FIG. 1 that the first area 11 and the second area 12 are connected, so the first end of the second area 12 can be defined as the connection surface of the first area 11 and the second area 12 . When the light source 105 is placed in the first area 11 , the light L emitted by the light source 105 is emitted from the connecting surface and incident from the second area 12 .

如图3所示,在本实施例中,光出射面102为对称于中心线100a的非球面。光出射面102包括一凹陷部1021,凸出部1022和垂直部1023。凹陷部1021位于光出射面102的中央,也就是位于光学透镜100的中央,凹陷部1021位于凹穴10的正上方,也就是说凹陷部1021和凹穴10的中心连线与中心线100a重合。在本实施例中,凹陷部1021的高度为A,也就是凸出部1022的最高点至凹陷部1021的中心点的距离为A。在本实施例中,凹陷部1021的高度可以在0.5-0.8mm之间,例如为0.64mm。As shown in FIG. 3 , in this embodiment, the light exit surface 102 is an aspheric surface symmetrical to the center line 100 a. The light exit surface 102 includes a concave portion 1021 , a protruding portion 1022 and a vertical portion 1023 . The concave portion 1021 is located in the center of the light exit surface 102, that is, in the center of the optical lens 100, and the concave portion 1021 is located directly above the cavity 10, that is to say, the center line connecting the concave portion 1021 and the cavity 10 coincides with the center line 100a . In this embodiment, the height of the concave portion 1021 is A, that is, the distance from the highest point of the protruding portion 1022 to the center point of the concave portion 1021 is A. In this embodiment, the height of the recessed portion 1021 may be between 0.5-0.8 mm, for example, 0.64 mm.

如图3所示,在本实施例中,凸出部1022位于凹陷部1021的外周,该凸出部1022同样关于中心线100a对称。凸出部1022与凹陷部1021接触的点可以定义为光学透镜100的最高点,也就是自光出射面102任一点沿着中心线100a方向至光入射面101或底表面103具有最大距离的对应位置。同时该位置至中心线100a的距离可以定义为凹陷部1021的最大直径Rmax,凹陷部1021的最大直径Rmax可以大于凹陷部1021的高度A。As shown in FIG. 3 , in this embodiment, the protruding portion 1022 is located on the outer periphery of the recessed portion 1021 , and the protruding portion 1022 is also symmetrical about the center line 100 a. The point where the convex part 1022 contacts the concave part 1021 can be defined as the highest point of the optical lens 100 , that is, the corresponding point with the maximum distance from any point of the light exit surface 102 along the centerline 100 a direction to the light entrance surface 101 or the bottom surface 103 . Location. Meanwhile, the distance from the position to the center line 100 a may be defined as the maximum diameter Rmax of the recessed portion 1021 , and the maximum diameter Rmax of the recessed portion 1021 may be greater than the height A of the recessed portion 1021 .

如图3所示,在本实施例中,垂直部1023位于凸出部1022的外周,垂直部1023连接底表面103和凸出部1022。垂直部1023平行或基本平行于中线100a,垂直部1023的高度小于凹穴10的高度。As shown in FIG. 3 , in this embodiment, the vertical portion 1023 is located on the outer periphery of the protruding portion 1022 , and the vertical portion 1023 connects the bottom surface 103 and the protruding portion 1022 . The vertical portion 1023 is parallel or substantially parallel to the center line 100 a, and the height of the vertical portion 1023 is smaller than the height of the cavity 10 .

如图3所示,在本实施例中,底表面103为一个曲面,具体地,该底表面103向光出射面102凹进,也就是说底表面103向光学透镜100的内部凹进,底表面103围绕中心线100a旋转,形成凹形区;凹形区的一端连接光出射面102,凹形区的另一端连接光入射面101。从图中可以看出,凹穴10位于底表面103的中心位置上,也就是位于凹形区的中心位置上,因此也可以说凹形区的一端连接垂直部1023,凹形区的另一端连接凹穴10。该底表面103可以为自由曲面,也可以为曲率半径为定值的曲面。As shown in FIG. 3 , in this embodiment, the bottom surface 103 is a curved surface. Specifically, the bottom surface 103 is concave toward the light exit surface 102 , that is to say, the bottom surface 103 is concave toward the inside of the optical lens 100 . The surface 103 rotates around the center line 100 a to form a concave area; one end of the concave area is connected to the light exit surface 102 , and the other end of the concave area is connected to the light incident surface 101 . As can be seen from the figure, the cavity 10 is located at the center of the bottom surface 103, that is, at the center of the concave area. Therefore, it can also be said that one end of the concave area is connected to the vertical portion 1023, and the other end of the concave area is connected to the vertical portion 1023. Connection pocket 10. The bottom surface 103 may be a free-form surface or a surface with a constant curvature radius.

如图3所示,在本实施例中,由于第二面101b为弧面,因此第二区域12是开口朝向第一区域11的抛物面,因此第二区域12具有最高点。本实施例中,将第二区域12的最高点至凹陷部1021中心点的距离定义为距离B。凹穴10的高度等于第一区域11的高度与第二区域12的高度之和。第一区域11的高度等于D,第二区域12的高度等于C,因此凹穴10的高度等于(C+D)。在本实施例中,凹穴10的高度与第二区域12的最高点至凹陷部1021中心点的距离的比值在3-6之间,例如为4或5,也就是说(C+D)/B在3-6之间。在本实施例中,(C+D)/B的比值可以为4.5,也就是凹穴10的高度为4.5mm,将第二区域12的最高点至凹陷部1021中心点的距离定义为1mm。As shown in FIG. 3 , in this embodiment, since the second surface 101 b is an arc surface, the second area 12 is a paraboloid with an opening facing the first area 11 , so the second area 12 has the highest point. In this embodiment, the distance B is defined as the distance from the highest point of the second region 12 to the center point of the recessed portion 1021 . The height of the cavity 10 is equal to the sum of the height of the first region 11 and the height of the second region 12 . The height of the first area 11 is equal to D, the height of the second area 12 is equal to C, so the height of the cavity 10 is equal to (C+D). In this embodiment, the ratio of the height of the cavity 10 to the distance from the highest point of the second region 12 to the center point of the concave portion 1021 is between 3-6, for example, 4 or 5, that is, (C+D) /B is between 3-6. In this embodiment, the ratio of (C+D)/B may be 4.5, that is, the height of the cavity 10 is 4.5 mm, and the distance from the highest point of the second region 12 to the center point of the recess 1021 is defined as 1 mm.

如图3所示,在本实施例中,由于该底表面103为曲面,底表面103的曲率半径与第一区域11上表面到基板106的高度d和底表面103的半宽R有关,因此经过计算得知,底表面103的曲率半径的最大值等于(R2+d2)/8d,因此底表面103的曲率半径大于0,且小于(R2+d2)/8d。需要说明的是,该光学透镜100是安装在基板106上,基板106表面涂有反射材料。在本实施例中,第一区域11的上表面至基板106的高度为d,也就是说基板106至光源的发光面的距离,也可以说反射材料至光源发光面的高度为d。As shown in FIG. 3 , in this embodiment, since the bottom surface 103 is a curved surface, the radius of curvature of the bottom surface 103 is related to the height d from the top surface of the first region 11 to the substrate 106 and the half-width R of the bottom surface 103 , so After calculation, the maximum value of the radius of curvature of the bottom surface 103 is equal to (R 2 +d 2 )/8d, so the radius of curvature of the bottom surface 103 is greater than 0 and less than (R 2 +d 2 )/8d. It should be noted that the optical lens 100 is mounted on the substrate 106, and the surface of the substrate 106 is coated with a reflective material. In this embodiment, the height from the upper surface of the first region 11 to the substrate 106 is d, that is, the distance from the substrate 106 to the light emitting surface of the light source, or the height from the reflective material to the light emitting surface of the light source is d.

如图3所示,在本实施例中,底表面103的外周轮廓线104接触基板106,因此底表面103相对于PCB基板向光学透镜100的方向凹进。需要说明的是,在本实施例中,外周轮廓线104还设置有引脚(未显示),因此可以接触基板106。As shown in FIG. 3 , in this embodiment, the outer peripheral contour line 104 of the bottom surface 103 contacts the substrate 106 , so the bottom surface 103 is concave in the direction of the optical lens 100 relative to the PCB substrate. It should be noted that, in this embodiment, the outer peripheral outline 104 is also provided with pins (not shown), so it can contact the substrate 106 .

如图5所示,首先将光源105设置在基板106上,基板106表面涂有反光材料。然后将光学透镜100设置在光源105上,即光源105位于凹穴10内。当光源105发射光线L时,部分光线L通过光入射面101射入,然后从光出射面102射出,在目标平面107上形成光斑。需要说明的是,图5中仅画出一条光线L进行说明。As shown in FIG. 5 , the light source 105 is first set on the substrate 106 , and the surface of the substrate 106 is coated with a reflective material. The optical lens 100 is then arranged on the light source 105 , ie the light source 105 is located in the cavity 10 . When the light source 105 emits light L, part of the light L enters through the light incident surface 101 and then exits from the light exit surface 102 to form a light spot on the target plane 107 . It should be noted that only one ray L is drawn for illustration in FIG. 5 .

如图5-图6所示,在本实施例中,部分光线L通过光出射面102射出,部分光线L由于光出射面102的全反射未能到达目标平面107上,而是通过底表面103射出至基板106上。As shown in FIGS. 5 to 6 , in this embodiment, part of the light L exits through the light exit surface 102 , and part of the light L fails to reach the target plane 107 due to the total reflection of the light exit surface 102 , but passes through the bottom surface 103 ejected onto the substrate 106 .

如图7所示,当光线L到达基板106上,由于基板106上具有反射材料,因此对光线L进行反射,由于底表面103为曲面,因此底表面103对光线L起到发散的作用,因此当光线L经过光出射面102射出时,光线L到达目标平面107上相当于被打散了,因此在目标平面107上形成的光斑变得更加均匀。As shown in FIG. 7 , when the light L reaches the substrate 106, since the substrate 106 has a reflective material, the light L is reflected. Since the bottom surface 103 is a curved surface, the bottom surface 103 plays a role in diffusing the light L, so When the light ray L exits through the light exit surface 102 , the light ray L reaches the target plane 107 and is equivalent to being scattered, so the light spot formed on the target plane 107 becomes more uniform.

如图8所示,图8显示为本发明的光学透镜和现有的光学透镜的光斑对比图。其中,曲线1显示为底面为平面的光学透镜形成的光斑亮度分布图,曲线2显示为本发明的光学透镜形成的光斑照度分布图。从图中可以得知,对于底面是平面的光学透镜,当全反射光线到底基板106时,基板106上的反射材料将光线反射进入光学透镜后向中心汇聚,造成中心区域亮度偏高。当光学透镜的底面是曲面时,基板106反射的光线经过该曲面时将光线进行了发散,从而降低中心区域的亮度,提高了光斑的均匀性。As shown in FIG. 8 , FIG. 8 is a light spot comparison diagram of the optical lens of the present invention and the conventional optical lens. Wherein, curve 1 is shown as a light spot luminance distribution diagram formed by an optical lens with a flat bottom surface, and curve 2 is shown as a light spot illuminance distribution diagram formed by the optical lens of the present invention. As can be seen from the figure, for an optical lens with a flat bottom surface, when the light is totally reflected to the bottom substrate 106, the reflective material on the substrate 106 reflects the light into the optical lens and converges toward the center, resulting in high brightness in the central area. When the bottom surface of the optical lens is a curved surface, the light reflected by the substrate 106 diverges when passing through the curved surface, thereby reducing the brightness of the central area and improving the uniformity of the light spot.

如图9所示,在本实施例中,将四个光源105按照矩阵方式排列,例如选择2×2矩阵,所述光源105可以为发光二极管。在X方向上光源105之间的间距例如为145mm,在Y方向上光源105之间的间距例如为140mm。光源105的发射角度可以在0-180°之间,例如为80°。需要说明的是,光源105可以按照其他矩阵排列,例如3×5矩阵或5×8矩阵。As shown in FIG. 9 , in this embodiment, four light sources 105 are arranged in a matrix manner, for example, a 2×2 matrix is selected, and the light sources 105 may be light emitting diodes. The spacing between the light sources 105 in the X direction is, for example, 145 mm, and the spacing between the light sources 105 in the Y direction is, for example, 140 mm. The emission angle of the light source 105 may be between 0-180°, eg, 80°. It should be noted that the light sources 105 may be arranged in other matrices, for example, a 3×5 matrix or a 5×8 matrix.

如图10所示,图10(a)是底面为平面的光学透镜的阵列仿真照度图,图10(b)是本发明的底面为曲面的光学透镜的阵列仿真照度图。图10(a)和图10(b)均采用2×2矩阵的光源。从图10(a)可以看出,由于光学透镜的底面是平面,全反射光线通过基板106上的反射材料反射达到光学透镜的底面平面时,光学透镜的底面平面将光线向中心汇聚,导致4个LED中心区域亮度过高(中心区域亮度为6170nit),而4个LED之间交叠区域的亮度明显低于LED中心区域的亮度(交叠区域亮度为4050nit),均匀性较差。从图10(b)可以看出,采用底面是弧面的光学透镜后,全反射光线通过基板106上的反射材料反射进行底面弧面时,底面弧面将光线向边缘区域发散,可以有效弥补4个LED之间交叠区域的亮度(交叠区域亮度为4530nit),进而降低LED中心区域的亮度(中心区域亮度为5670nit),缩小了中心区域和交叠区域的亮度差,提高了均匀性。需要说明的是,图10(b)中使用的光学透镜的底表面为曲面,且底表面的曲率半径可以为15.30。As shown in FIG. 10 , FIG. 10( a ) is an array simulation illuminance diagram of an optical lens with a flat bottom surface, and FIG. 10( b ) is an array simulation illuminance diagram of an optical lens with a curved bottom surface of the present invention. Figures 10(a) and 10(b) both use a 2×2 matrix of light sources. As can be seen from Figure 10(a), since the bottom surface of the optical lens is a plane, when the total reflection light is reflected by the reflective material on the substrate 106 and reaches the bottom plane of the optical lens, the bottom plane of the optical lens will converge the light to the center, resulting in 4 The brightness of the central area of each LED is too high (the brightness of the central area is 6170 nits), and the brightness of the overlapping area between the four LEDs is significantly lower than that of the central area of the LEDs (the brightness of the overlapping area is 4050 nits), with poor uniformity. It can be seen from Fig. 10(b) that after using the optical lens whose bottom surface is a curved surface, when the total reflection light is reflected by the reflective material on the substrate 106 to make the bottom surface curved surface, the bottom curved surface scatters the light to the edge area, which can effectively compensate for The brightness of the overlapping area between the 4 LEDs (the brightness of the overlapping area is 4530nit), which reduces the brightness of the central area of the LED (the brightness of the central area is 5670nit), reduces the brightness difference between the center area and the overlapping area, and improves the uniformity . It should be noted that the bottom surface of the optical lens used in FIG. 10( b ) is a curved surface, and the curvature radius of the bottom surface may be 15.30.

如图11所示,本实施例还提出另一种光学透镜,该光学透镜的底表面103由N个曲面103a组成,N个曲面103a相互连接,且N个曲面103a的形状相同。N个曲面103a的切线为虚线108。在这种情况下,曲面103a的曲率半径的最大值为

Figure BDA0002607984030000071
并且,r×N≤R≤r×(N+1)。需要说明的是,R表示底表面103的半宽,d表示基板106至第一区域上表面的高度,也就是反射材料至第一区域上表面的高度。需要说明的是,N可以大于或等于2。As shown in FIG. 11 , this embodiment also proposes another optical lens. The bottom surface 103 of the optical lens is composed of N curved surfaces 103a, the N curved surfaces 103a are connected to each other, and the N curved surfaces 103a have the same shape. The tangents of the N curved surfaces 103 a are dotted lines 108 . In this case, the maximum value of the radius of curvature of the curved surface 103a is
Figure BDA0002607984030000071
Also, r×N≦R≦r×(N+1). It should be noted that R represents the half width of the bottom surface 103 , and d represents the height from the substrate 106 to the upper surface of the first region, that is, the height from the reflective material to the upper surface of the first region. It should be noted that N can be greater than or equal to 2.

如图12所示,本实施例还提出另一种光学透镜,该光学透镜的底表面103包括N个曲面103a和M个平面109组成,N个曲面103a和M个平面109间隔分布。平面109的宽度为m,也就是曲面103a之间的间距为m。在这种情况下,曲面103a的曲率半径的最大值为

Figure BDA0002607984030000072
As shown in FIG. 12 , another optical lens is also proposed in this embodiment. The bottom surface 103 of the optical lens includes N curved surfaces 103 a and M flat surfaces 109 , and the N curved surfaces 103 a and M flat surfaces 109 are distributed at intervals. The width of the plane 109 is m, that is, the distance between the curved surfaces 103a is m. In this case, the maximum value of the radius of curvature of the curved surface 103a is
Figure BDA0002607984030000072

其中,R表示底表面103的半宽,d表示反射材料至第一区域上表面的高度。需要说明的是,N可以大于或等于2。在本实施例中,曲面和平面的数量的差值为1,也就是说曲面的数量可以比平面的数量多一个,或者曲面的数量可以比平面的数量少一个。Wherein, R represents the half width of the bottom surface 103, and d represents the height of the reflective material to the upper surface of the first region. It should be noted that N can be greater than or equal to 2. In this embodiment, the difference between the number of curved surfaces and the number of planes is 1, that is to say, the number of curved surfaces can be one more than the number of planes, or the number of curved surfaces can be one less than the number of planes.

如图13所示,本实施例还提出另一种光学透镜,该光学透镜的底表面103由第一曲面103b,第二曲面103c和平面109组成。第一曲面103b和第二曲面103c之间通过平面109间隔。第一曲面103b的圆弧小于第二曲面103c的圆弧,也就是第一曲面103b的曲率半径小于第二曲面103c的曲率半径。在这种情况下,第二曲面103c的曲率半径的最大值为

Figure BDA0002607984030000073
其中,R表示底表面103的半宽,d表示基板106至第一区域上表面的高度,也就是反射材料至第一区域上表面的高度,m表示平面109的宽度,α表示第一曲面103b对应的圆心角,β表示第二曲面103c对应的圆心角,r1表示第一曲面103b的半径。需要说明的是,N可以大于或等于2。α也可以表示所有的曲面中最小的曲面对应的圆心角,β也可以表示所有的曲面中最大的曲面对应的圆心角。As shown in FIG. 13 , this embodiment further proposes another optical lens. The bottom surface 103 of the optical lens is composed of a first curved surface 103 b , a second curved surface 103 c and a flat surface 109 . A plane 109 is spaced between the first curved surface 103b and the second curved surface 103c. The arc of the first curved surface 103b is smaller than that of the second curved surface 103c, that is, the radius of curvature of the first curved surface 103b is smaller than the radius of curvature of the second curved surface 103c. In this case, the maximum value of the radius of curvature of the second curved surface 103c is
Figure BDA0002607984030000073
Wherein, R represents the half width of the bottom surface 103, d represents the height from the substrate 106 to the upper surface of the first area, that is, the height from the reflective material to the upper surface of the first area, m represents the width of the plane 109, and α represents the first curved surface 103b The corresponding central angle, β represents the central angle corresponding to the second curved surface 103c, and r 1 represents the radius of the first curved surface 103b. It should be noted that N can be greater than or equal to 2. α can also represent the central angle corresponding to the smallest surface among all the surfaces, and β can also represent the central angle corresponding to the largest surface among all the surfaces.

如图14所示,本实施例还提出一种发光装置200,该发光装置200包括基板106,光源105,光学透镜100。As shown in FIG. 14 , this embodiment further provides a light-emitting device 200 . The light-emitting device 200 includes a substrate 106 , a light source 105 , and an optical lens 100 .

如图14所示,在本实施例中,光源105封装在基板106上,基板106上设置有反射材料。基板106可以为PCB基板,光源105可以为LED。在本实施例中,光源105可以按照M×N矩阵的方式设置在基板106上,其中,M可以等于N,也可以不等于N。As shown in FIG. 14 , in this embodiment, the light source 105 is packaged on the substrate 106 , and the substrate 106 is provided with a reflective material. The substrate 106 may be a PCB substrate, and the light source 105 may be an LED. In this embodiment, the light sources 105 may be arranged on the substrate 106 in an M×N matrix, where M may be equal to or not equal to N.

如图14所示,在本实施例中,光学透镜100设置在光源105上,光学透镜100的具体形状可以参阅图1,在此不再阐述光学透镜100的形状。As shown in FIG. 14 , in this embodiment, the optical lens 100 is disposed on the light source 105 , and the specific shape of the optical lens 100 may refer to FIG. 1 , and the shape of the optical lens 100 will not be described here.

如图14所示,在本实施例中,在光学透镜100上还设置有扩散膜202和第一增亮膜203和第二增亮膜204。第一增亮膜203位于扩散膜202上,第二增亮膜204位于第一增亮膜203上。扩散膜202和第一增亮膜203和第二增亮膜204均可以对光斑起到调控作用。As shown in FIG. 14 , in this embodiment, a diffusion film 202 , a first brightness enhancement film 203 and a second brightness enhancement film 204 are further provided on the optical lens 100 . The first brightness enhancement film 203 is located on the diffusion film 202 , and the second brightness enhancement film 204 is located on the first brightness enhancement film 203 . The diffusion film 202, the first brightness enhancement film 203 and the second brightness enhancement film 204 can all play a role in regulating the light spot.

如图14所示,在本实施例中,由于光学透镜100可以对光线起到调控作用,因此可以缩小发光装置200的厚度。该发光装置200可以用于多个电子设备中,例如用于显示设备中。As shown in FIG. 14 , in this embodiment, since the optical lens 100 can regulate the light, the thickness of the light emitting device 200 can be reduced. The light-emitting device 200 can be used in a plurality of electronic devices, for example, in a display device.

综上所述,本发明提出一种光学透镜及发光装置,通过在底表面设计成包括至少一个曲面,因此在底表面至少形成一个凹形区。当光源发射的光线经过光发射面反射后再次通过凹形区进行折射,形成折射光线,折射光线经过反射材料反射后再次通过凹形区,因此该凹形区可以对光线起到发散的作用,也就是对光线起到调控作用。因此,该光学透镜可以提高在目标平面上形成的光斑的均匀性,从而也可以提高光源的利用率。To sum up, the present invention provides an optical lens and a light-emitting device. By designing the bottom surface to include at least one curved surface, at least one concave area is formed on the bottom surface. When the light emitted by the light source is reflected by the light emitting surface, it is refracted through the concave area again to form a refracted light. The refracted light is reflected by the reflective material and then passes through the concave area again. Therefore, the concave area can play a role in diffusing the light. That is, it controls the light. Therefore, the optical lens can improve the uniformity of the light spot formed on the target plane, thereby also improving the utilization rate of the light source.

以上描述仅为本申请的较佳实施例以及对所运用技术原理的说明,本领域技术人员应当理解,本申请中所涉及的发明范围,并不限于上述技术特征的特定组合而成的技术方案,同时也应涵盖在不脱离所述发明构思的情况下,由上述技术特征或其等同特征进行任意组合而形成的其它技术方案,例如上述特征与本申请中公开的(但不限于)具有类似功能的技术特征进行互相替换而形成的技术方案。The above description is only a preferred embodiment of the application and an illustration of the applied technical principle. Those skilled in the art should understand that the scope of the invention involved in this application is not limited to the technical solution formed by the specific combination of the above technical features , and shall also cover other technical solutions formed by any combination of the above technical features or their equivalent features without departing from the inventive concept, for example, the above features are similar to those disclosed in this application (but not limited to) A technical solution formed by replacing the technical features of the functions with each other.

除说明书所述的技术特征外,其余技术特征为本领域技术人员的已知技术,为突出本发明的创新特点,其余技术特征在此不再赘述。Except for the technical features described in the specification, the other technical features are known technologies by those skilled in the art, and in order to highlight the innovative features of the present invention, the remaining technical features are not repeated here.

Claims (10)

1. An optical lens, comprising:
a light incident surface forming a pocket having an opening, the pocket including a first region and a second region, the second region being on the first region; the first area is used for placing a light source, and light rays emitted by the light source are incident from the second area;
the light emitting surface comprises a concave part, the concave part is positioned on the concave cavity, and the center lines of the concave cavity and the concave part are superposed with the center line of the optical lens;
a bottom surface connecting the light incident surface and the light exit surface;
wherein the bottom surface comprises at least one curved surface, and the bottom surface comprises at least one concave area; and part of the light rays are reflected from the light emergent surface and then are refracted towards the concave area to form refracted light rays.
2. The optical lens of claim 1 wherein the optical lens is disposed on a reflective material, and the refracted light rays are reflected by the reflective material toward the concave region.
3. The optical lens of claim 2 wherein when said bottom surface is curved, said bottom surface has a radius of curvature less than (R)2+d2) And/8 d, wherein R represents the half width of the bottom surface, and d represents the height of the reflecting material to the upper surface of the first region.
4. The optical lens of claim 2, wherein when the bottom surface comprises N curved surfaces, the N curved surfaces are connected to each other and have the same shape; maximum value of curvature radius of the curved surface
Figure FDA0002607984020000011
And R x N is not more than R x (N + 1);
wherein N ≧ 2, R represents a half-width of the bottom surface, and d represents a height of the reflective material to an upper surface of the first region.
5. The optical lens of claim 2 wherein when the bottom surface comprises N curved surfaces, the N curved surfaces have the same shape and the N curved surfaces are separated by a plane, the maximum value of the radius of curvature of the curved surfaces
Figure FDA0002607984020000012
Wherein N ≧ 2, R represents a half-width of the bottom surface, d represents a height of the reflective material to the upper surface of the first region, and m represents a width of the plane.
6. The optical lens of claim 2 wherein when the bottom surface comprises N curved surfaces, the N curved surfaces have different shapes and the N curved surfaces are separated by a planar space, the maximum of the radius of curvature of the curved surfaces
Figure FDA0002607984020000013
Wherein N is more than or equal to 2, R represents the half width of the bottom surface, d represents the height from the reflecting material to the upper surface of the first area, m represents the width of the plane, alpha represents the central angle corresponding to the minimum curved surface of the N curved surfaces, beta represents the central angle corresponding to the maximum curved surface of the N curved surfaces, and R represents the central angle corresponding to the maximum curved surface of the N curved surfaces1Representing the radius of the smallest of the N curved surfaces.
7. The optical lens of claim 1 wherein a ratio of a height of the recess to a distance from the second end to a center point of the recess is between 3-6.
8. An optical lens according to claim 1, characterized in that the distance from the highest point of the protrusion to the center point of the depression is between 0.5 and 0.8 mm.
9. An optical lens according to claim 1, wherein the light exit surface further comprises a convex portion and a vertical portion, the convex portion being connected to an outer periphery of the concave portion; the vertical portion is parallel to a center line of the optical lens, the vertical portion is connected to an outer circumference of the protrusion, and the protrusion is connected to the bottom surface through the vertical portion.
10. A light-emitting device, comprising:
a substrate;
a light source disposed on the substrate;
an optical lens positioned on the light source;
wherein the optical lens includes:
a light incident surface forming a pocket having an opening, the pocket including a first region and a second region, the second region being on the first region; the first area is used for placing a light source, and light rays emitted by the light source are incident from the second area;
the light emitting surface comprises a concave part, the concave part is positioned on the concave cavity, and the center lines of the concave cavity and the concave part are superposed with the center line of the optical lens;
a bottom surface connecting the light incident surface and the light exit surface;
wherein the bottom surface comprises at least one curved surface, and the bottom surface comprises at least one concave area; and part of the light rays are reflected from the light emergent surface and then are refracted towards the concave area to form refracted light rays.
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