WO2016045176A1 - Method for designing full-periphery light distribution lens and corresponding light distribution lens - Google Patents

Method for designing full-periphery light distribution lens and corresponding light distribution lens Download PDF

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Publication number
WO2016045176A1
WO2016045176A1 PCT/CN2014/091149 CN2014091149W WO2016045176A1 WO 2016045176 A1 WO2016045176 A1 WO 2016045176A1 CN 2014091149 W CN2014091149 W CN 2014091149W WO 2016045176 A1 WO2016045176 A1 WO 2016045176A1
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Prior art keywords
light distribution
light
lens
led
angle
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PCT/CN2014/091149
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French (fr)
Chinese (zh)
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陈必寿
许礼
姜玉稀
刘海波
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上海三思电子工程有限公司
上海三思科技发展有限公司
嘉善三思光电技术有限公司
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Publication of WO2016045176A1 publication Critical patent/WO2016045176A1/en

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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
    • 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
    • F21V5/046Refractors for light sources of lens shape the lens having a rotationally symmetrical shape about an axis for transmitting light in a direction mainly perpendicular to this axis, e.g. ring or annular lens with light source disposed inside the ring
    • 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
    • F21V23/00Arrangement of electric circuit elements in or on lighting devices
    • 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
    • F21Y2103/00Elongate light sources, e.g. fluorescent tubes
    • F21Y2103/30Elongate light sources, e.g. fluorescent tubes curved
    • F21Y2103/33Elongate light sources, e.g. fluorescent tubes curved annular

Definitions

  • the invention relates to a lens design method, in particular to a design method and a corresponding light distribution lens of a full-circumferential light distribution lens capable of realizing light distribution greater than 180 degrees.
  • LED Light Emitting Diode
  • Lambertian the surface of the LED chip is Lambertian, and its light-emitting angle is only 120 degrees. It cannot be directly applied to the lighting system, and only through its reasonable secondary light distribution can meet different lighting needs.
  • the secondary light distribution design of the LED light source on the market is mainly a projection type reflector and a lens. Since the light distribution beam angle is less than 180 degrees, only a single surface planar projection illumination can be realized, and the entire space cannot be realized. Three-dimensional lighting, if used in indoor lighting, it is easy to form a dark corner of the corner or ceiling lighting, which seriously affects the eye comfort of the human body.
  • the technical problem solved by the present invention is that a stepped ring circular stage free-form surface lens is used as shown in FIG. 1 , instead of the prior art projection type reflector or lens as shown in FIG. 2 , a full-circumference light distribution with a beam angle greater than 180 degrees is realized. design.
  • a method for designing a full-circumferential light distribution lens according to the present invention includes the following steps:
  • Step 1 setting a plurality of LED loops and a secondary light distribution lens surrounding the LED loops;
  • Each LED ring strip is mainly composed of an LED light source arranged in a circle in a plane;
  • the envelope surface of the plurality of LED ring strips is a round table side
  • the light distribution curve formed by the secondary light distribution lens is divided into a plurality of portions equal to the number of LED loops, and the plurality of portions are in one-to-one correspondence with the plurality of LED loop strips;
  • the light distribution angle of the partial light distribution curve is less than 180 degrees, and the light distribution angle of the partial light distribution curve is greater than or equal to 180 degrees, and the proportion of the light flux included in each part of the light distribution curve is equal to the total light flux ratio of each LED ring band;
  • Step 2 taking the plane of the optical axis of any one of the LED coils as the incident surface, and on the incident surface, dividing the angle of the light source of the LED ring on the optical axis into N small angles, wherein N ⁇ 4, that is, each The angles of the light sources are distributed at equal angular intervals;
  • Step 3 The light distribution curve separated by step 1 is divided into N small segments, and the corresponding luminous flux of each segment in the N-segment light distribution curve is equal to the luminous flux of the light source distributed in step 2;
  • Step 4 The N small angles are respectively corresponding to the N small segments of the light distribution curve
  • Step 5 taking the edge segment of the N segments as the starting segment, and starting the segment with the edge point, that is, corresponding to one of the N small corners;
  • Step 6 Find two consecutive curves corresponding to each LED band
  • Step 7 The two consecutive curves corresponding to the LED strips are sequentially connected end to end to form a closed curve, and then the closed curve is rotated around the central axis of the LED light source of the LED ring to form a full-circumference light distribution.
  • the three-dimensional shape of the optical lens
  • step 6 includes the following steps:
  • Step 6.1 according to the distance requirement of the lens entrance surface of the full-circumferential light distribution lens to leave the light source, take a point on the incident light corresponding to the initial illuminated point as the starting feature point of the lens entrance surface, At a starting feature point on the light incident surface, a line parallel to the line connecting the LED light source and the initial illuminated point forms an angle with the incident light, which is the initial light deflection angle of the secondary light distribution lens.
  • the initial ray deflection angle is divided into a first deflection angle and a second deflection angle.
  • the angular division of the first deflection angle and the second deflection angle is used as a refracting line of the incident ray passing through the lens entrance surface, and the refraction law and the corresponding a small angle of the N small angles is obtained, and a second feature point on the light incident surface adjacent to the initial feature point on the light incident surface is obtained, and the second feature point on the light incident surface corresponds to the initial illumination Pointing adjacent second illuminated points;
  • Step 6.2 Perform step 6.1 for each of the N small segments, and sequentially determine the positions of the feature points on the light incident surface of the lens corresponding to each of the N small segments:
  • Step 6.3 taking a point on the refracting line after passing the initial feature point on the light incident surface of the lens, according to the lens thickness requirement of the secondary light distribution lens, as the lens exit surface of the full-circumferential light distribution lens At the starting feature point, the position of each feature point on the light exit surface of the lens is obtained as follows:
  • Step i1 at a starting feature point on the light-emitting surface, a line parallel to the line connecting the LED light source and the initial illuminated point forms an angle with the incident light, which is a starting light deflection angle of the secondary light distribution lens,
  • the initial ray deflection angle is divided into a first deflection angle and a second deflection angle, and the angular division of the first deflection angle and the second deflection angle is used as a refracting line of the incident ray passing through the illuminating surface of the lens, and the law of refraction is Corresponding to one of the N small corners a small angle, a second feature point on the light-emitting surface adjacent to the starting feature point on the light-emitting surface is obtained, and the second feature point on the light-emitting surface corresponds to the second illuminated point adjacent to the initial illuminated point ;
  • Step i2 performing step i1 for each of the N small segments, and sequentially determining the positions of the feature points on the lens light-emitting surface corresponding to each of the N small segments;
  • Step 6.4 sequentially connecting the feature points on the light incident surface of the lens, and sequentially connecting the feature points on the light exiting surface of the lens to form two continuous curves.
  • the feature points are sequentially connected by a straight line or a smooth curve.
  • the number of LED loops is two, and the light distribution curve formed by the secondary light distribution lens is divided into two parts, wherein a light distribution angle of a part of the light distribution curve is less than 180 degrees, and another part of the light distribution curve The light distribution angle is greater than or equal to 180 degrees.
  • a full-circumferential light distribution lens is obtained according to the above-described design method of a full-circumferential light distribution lens.
  • the full-circumferential light distribution lens has a through hole in the middle thereof.
  • the present invention has the following beneficial effects:
  • the method of determining the surface of the lens by calculating the feature points can determine the shape of the inner and outer surfaces of the lens more accurately and quickly;
  • Figure 1 is an outline view of a conventional projection lens
  • FIG. 3 is a sectional view of a light distribution curve of a full-circumferential light distribution lens
  • FIG. 4 is a schematic view showing a method of dividing a small angle on an incident surface
  • FIG. 5 is a schematic diagram of a method for dividing a small section in an outgoing light distribution space
  • FIG. 6 is a schematic view for determining feature points on a surface of a lens and sequentially connecting them;
  • Figure 7 is a cross-sectional view of the stepped truncated cone lens of Embodiment 1;
  • Figure 8 is an external view of a stepped truncated freeform lens of Embodiment 1;
  • Figure 9 is a cross-sectional view showing a stepped truncated cone lens of Embodiment 2;
  • Figure 10 is a perspective view showing the stepped truncated free-form surface lens of the second embodiment.
  • the present invention is directed to constructing a light distribution method that achieves full-circumference light distribution greater than 180 degrees.
  • the light distribution method includes an annularly arranged LED light source 1 and a secondary light distribution lens 2, as shown in FIG.
  • the LED light source 1 is arranged in a plurality of annular loops on different horizontal planes, and forms a three-dimensional array of annular stacks in a three-dimensional space at a certain conical angle;
  • the secondary light distribution lens 2 has a stepped truncated cone shape.
  • Stepped circular table free-form lens ( Figure 2) the design steps are as follows:
  • the light distribution curve formed by the secondary light distribution lens 2 is divided into an equal number of portions.
  • the LED light sources are arranged in two annular loops, and the light distribution curve formed by the secondary light distribution lens 2 is also divided into two parts, wherein a part of the light distribution curve has a light distribution angle of less than 180 degrees, and the other part The light distribution angle of the light distribution curve is greater than or equal to 180 degrees.
  • the light distribution curve is divided into three or more parts, the light distribution angles of the three parts can be arbitrarily distributed, as long as the principle of conservation of energy with the LED circle is ensured. (As shown in Fig.
  • L1 represents a light distribution portion of less than 180 degrees
  • L2 represents a light distribution portion of more than 180 degrees
  • the ratio of the luminous flux contained in the two portions of the light distribution curve is equal to the total luminous flux ratio of the LED light source of each of the coils.
  • the design of the lens will be separately designed for the divided light distribution curves;
  • step c) dividing the light distribution curve separated by step a) (that is, the distribution of light intensity with the angle of illumination) into four sub-sections, respectively, corresponding to the luminous flux of each of the ab, bc, cd, de, and 4-segment light distribution curves
  • the angular flux of each source separated from step b) is equal;
  • the corresponding small angle of the ab segment is ⁇ 1
  • a point 1a is taken as the starting feature point on the incident surface of the lens, and at the starting feature point, parallel to the light source and the initial illuminated point a
  • the line connecting the line forms an angle ⁇ 1 with the incident light, which is the initial light deflection angle of the lens, and divides the initial light deflection angle ⁇ 1 into a first deflection angle ⁇ 11 and a second deflection angle ⁇ 12, and the two deflection angles
  • the ratio can be arbitrary.
  • ⁇ 11: ⁇ 12 1:1
  • the angular line is taken as the incident light passing through the light incident surface (the light incident surface 201 and the light exit surface 202 of the lens respectively refer to the inner surface and the outer surface of the lens).
  • the refracting line after the characteristic point 1a is determined by the law of refraction to determine the normal line n1 of the point 1a, and the line perpendicular to the normal line n1 forms an intersection with the incident surface of the light, which intersects with the corner of the small corner ⁇ 1
  • the intersection points are 1a and 1b, respectively, and the 1b point is the second feature point.
  • each feature point can be obtained--the specific method for solving the normal of each feature point is as follows: 1.
  • the feature is obtained by the incident light direction of the feature point.
  • the refractive index Nrefract of the feature point is obtained by the direction of the refracted ray of the feature point; 3.
  • a point 2a is taken as a starting feature point on the light-emitting surface 202 on the refracting line passing through the initial feature point 1a on the light-incident surface, and the refracting line is used as the lens light-emitting surface.
  • the incident ray of 202 is a refracting line of the lens exit surface 202 parallel to the line connecting the illuminated point a and the light source at the point 2a, and the direction of the incident ray and the refracting line is the second offset angle ⁇ 12 of the figure.
  • the positions of the feature points 2b, 2c, 2d, and 2e on the second surface are sequentially determined in exactly the same manner as the feature points for determining the light incident surface.
  • the lens in another embodiment, in order to achieve a better heat dissipation effect, can also be designed as a middle belt through hole in the shape of a middle band through hole.
  • the full circumference light distribution lens The principle of optical design is the same as the first The method of an embodiment is only designed from the position edge of the central band through hole, and the optical curve is obtained, and then connected, and then rotated around the central axis to form a stereoscopic switch of the lens, as shown in FIG. 9 and FIG.

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  • General Engineering & Computer Science (AREA)
  • Non-Portable Lighting Devices Or Systems Thereof (AREA)
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Abstract

A method for designing a full-periphery light distribution lens and the corresponding light distribution lens. The method comprises: arranging multiple LED ring strips (1) and secondary light distribution lenses (2) surrounding the LED ring strips (1); using the optical axis plane of any LED ring strip as an incident plane, equally dividing the light source angle of the LED ring strip on one side of the optical axis into N small angles and N small sections of the corresponding light distribution curve according to the distribution rule of the light intensity versus the light-emitting angle, the edge small section of the N small sections being used as an initial irradiated small section, and an edge point being used as an initial irradiated point; calculating two continuous curves corresponding to each LED ring strip, connecting the respective curves to form a closed curve, then rotating the closed curve to form the three-dimensional shape of the full-periphery light distribution lens. The full-periphery light distribution illumination with the angle larger than 180 degrees can be achieved.

Description

全周光配光透镜的设计方法及相应的配光透镜Design method of full-period light distribution lens and corresponding light distribution lens 技术领域Technical field
本发明涉及一种透镜设计方法,尤其涉及一种可实现大于180度配光的全周光配光透镜的设计方法及相应的配光透镜。The invention relates to a lens design method, in particular to a design method and a corresponding light distribution lens of a full-circumferential light distribution lens capable of realizing light distribution greater than 180 degrees.
背景技术Background technique
LED(Light Emitting Diode)以其效率高,光色纯、能耗低、寿命长、无污染等优点成为21世纪最具竞争力的新型光源。随着LED光通量及光效的不断提高,LED在照明领域的应用也越来越广泛。然而,LED芯片的表面出光为Lambertian分布,本身的出光角度只有120度,无法直接应用于照明系统,只有通过对其合理的二次配光才能满足不同的照明需求。LED (Light Emitting Diode) has become the most competitive new light source in the 21st century due to its high efficiency, pure light color, low energy consumption, long life and no pollution. With the continuous improvement of LED luminous flux and light efficiency, LEDs are increasingly used in the field of lighting. However, the surface of the LED chip is Lambertian, and its light-emitting angle is only 120 degrees. It cannot be directly applied to the lighting system, and only through its reasonable secondary light distribution can meet different lighting needs.
目前,市场上对LED光源的二次配光设计以投射型反射器和透镜为主,由于其配光光束角小于180度而只能实现单一表面的平面式投射式照明,不能实现整个空间的立体式照明,若用于室内灯具上很容易形成墙角或天花板照明暗区,严重影响人体的眼睛舒适度。At present, the secondary light distribution design of the LED light source on the market is mainly a projection type reflector and a lens. Since the light distribution beam angle is less than 180 degrees, only a single surface planar projection illumination can be realized, and the entire space cannot be realized. Three-dimensional lighting, if used in indoor lighting, it is easy to form a dark corner of the corner or ceiling lighting, which seriously affects the eye comfort of the human body.
发明内容Summary of the invention
针对现有技术中的缺陷,本发明的目的是提供一种全周光配光透镜的设计方法。In view of the deficiencies in the prior art, it is an object of the present invention to provide a method of designing a full-circumferential light distribution lens.
本发明解决的技术问题是:采用阶梯环圆形台自由曲面透镜如图1,代替现有技术中的投射型反射器或者透镜如图2,实现了光束角大于180度的全周光配光设计。The technical problem solved by the present invention is that a stepped ring circular stage free-form surface lens is used as shown in FIG. 1 , instead of the prior art projection type reflector or lens as shown in FIG. 2 , a full-circumference light distribution with a beam angle greater than 180 degrees is realized. design.
根据本发明提供的一种全周光配光透镜的设计方法,包括如下步骤:A method for designing a full-circumferential light distribution lens according to the present invention includes the following steps:
步骤1:设置多条LED圈带以及环绕于LED圈带的二次配光透镜;Step 1: setting a plurality of LED loops and a secondary light distribution lens surrounding the LED loops;
每条LED圈带均主要由在一平面内环形排列的LED光源构成;Each LED ring strip is mainly composed of an LED light source arranged in a circle in a plane;
所述多条LED圈带的包络面为一圆台侧面;The envelope surface of the plurality of LED ring strips is a round table side;
所述二次配光透镜形成的配光曲线分隔为与LED圈带数量相等的多个部分,所述多个部分与所述多个LED圈带一一对应;The light distribution curve formed by the secondary light distribution lens is divided into a plurality of portions equal to the number of LED loops, and the plurality of portions are in one-to-one correspondence with the plurality of LED loop strips;
部分配光曲线的配光角度小于180度,部分配光曲线的配光角度大于等于180度,各部分配光曲线所包含光通量比例等于各LED圈带的总光通比例; The light distribution angle of the partial light distribution curve is less than 180 degrees, and the light distribution angle of the partial light distribution curve is greater than or equal to 180 degrees, and the proportion of the light flux included in each part of the light distribution curve is equal to the total light flux ratio of each LED ring band;
步骤2:以任意一条LED圈带的光轴平面作为入射面,在所述入射面上,将光轴一侧的LED圈带的光源角度等分为N个小角,其中N≥4,即各光源角度按相等的角度间隔进行分配;Step 2: taking the plane of the optical axis of any one of the LED coils as the incident surface, and on the incident surface, dividing the angle of the light source of the LED ring on the optical axis into N small angles, wherein N≥4, that is, each The angles of the light sources are distributed at equal angular intervals;
步骤3:将步骤1分隔好的配光曲线分为N个小段,N段配光曲线中的每段对应的光通量均与步骤2分配的光源角度光通量相等;Step 3: The light distribution curve separated by step 1 is divided into N small segments, and the corresponding luminous flux of each segment in the N-segment light distribution curve is equal to the luminous flux of the light source distributed in step 2;
步骤4:将所述N个小角与所述配光曲线N个小段一一对应;Step 4: The N small angles are respectively corresponding to the N small segments of the light distribution curve;
步骤5:以所述N个小段中的边缘小段作为起始被照小段,以边缘点为起始被照点,即对应所述N个小角中的一个小角;Step 5: taking the edge segment of the N segments as the starting segment, and starting the segment with the edge point, that is, corresponding to one of the N small corners;
步骤6:求出每条LED圈带所对应的两条连续曲线;Step 6: Find two consecutive curves corresponding to each LED band;
步骤7:将各条LED圈带所对应的两条连续曲线依次首尾连接形成一个封闭的曲线,然后将所述封闭的曲线绕LED圈带的LED光源的排列中心轴线旋转,形成全周光配光透镜的立体形状;Step 7: The two consecutive curves corresponding to the LED strips are sequentially connected end to end to form a closed curve, and then the closed curve is rotated around the central axis of the LED light source of the LED ring to form a full-circumference light distribution. The three-dimensional shape of the optical lens;
其中,所述步骤6包括如下步骤:Wherein, the step 6 includes the following steps:
步骤6.1:根据全周光配光透镜的透镜入光面离开光源的距离要求,在与起始被照点对应的入射光线上取一点作为所述透镜入光面上的起始特征点,在该入光面上的起始特征点处,平行于LED光源与起始被照点连线的直线同入射光线形成一夹角,为二次配光透镜的起始光线偏折角,将所述起始光线偏折角分成第一偏折角和第二偏折角,第一偏折角和第二偏折角的角分线作为入射光线经过所述透镜入光面后的折射线,通过折射定律以及对应所述N个小角中的一个小角,求出与入光面上的起始特征点相邻的入光面上的第二特征点,该入光面上的第二特征点对应与起始被照点相邻的第二被照点;Step 6.1: according to the distance requirement of the lens entrance surface of the full-circumferential light distribution lens to leave the light source, take a point on the incident light corresponding to the initial illuminated point as the starting feature point of the lens entrance surface, At a starting feature point on the light incident surface, a line parallel to the line connecting the LED light source and the initial illuminated point forms an angle with the incident light, which is the initial light deflection angle of the secondary light distribution lens. The initial ray deflection angle is divided into a first deflection angle and a second deflection angle. The angular division of the first deflection angle and the second deflection angle is used as a refracting line of the incident ray passing through the lens entrance surface, and the refraction law and the corresponding a small angle of the N small angles is obtained, and a second feature point on the light incident surface adjacent to the initial feature point on the light incident surface is obtained, and the second feature point on the light incident surface corresponds to the initial illumination Pointing adjacent second illuminated points;
步骤6.2:针对N个小段中的每一个小段执行步骤6.1,依次求出N个小段中的各个被照点所对应的透镜入光面上的各特征点的位置:Step 6.2: Perform step 6.1 for each of the N small segments, and sequentially determine the positions of the feature points on the light incident surface of the lens corresponding to each of the N small segments:
步骤6.3:在经过所述透镜入光面上的起始特征点后的折射线上,根据二次配光透镜的透镜厚度要求取一点,作为全周光配光透镜的透镜出光面上的起始特征点,采用如下方式,求出透镜出光面上的各特征点的位置:Step 6.3: taking a point on the refracting line after passing the initial feature point on the light incident surface of the lens, according to the lens thickness requirement of the secondary light distribution lens, as the lens exit surface of the full-circumferential light distribution lens At the starting feature point, the position of each feature point on the light exit surface of the lens is obtained as follows:
步骤i1:在该出光面上的起始特征点处,平行于LED光源与起始被照点连线的直线同入射光线形成一夹角,为二次配光透镜的起始光线偏折角,将所述起始光线偏折角分成第一偏折角和第二偏折角,第一偏折角和第二偏折角的角分线作为入射光线经过所述透镜出光面后的折射线,通过折射定律以及对应所述N个小角中的一 个小角,求出与出光面上的起始特征点相邻的出光面上的第二特征点,该出光面上的第二特征点对应与起始被照点相邻的第二被照点;Step i1: at a starting feature point on the light-emitting surface, a line parallel to the line connecting the LED light source and the initial illuminated point forms an angle with the incident light, which is a starting light deflection angle of the secondary light distribution lens, The initial ray deflection angle is divided into a first deflection angle and a second deflection angle, and the angular division of the first deflection angle and the second deflection angle is used as a refracting line of the incident ray passing through the illuminating surface of the lens, and the law of refraction is Corresponding to one of the N small corners a small angle, a second feature point on the light-emitting surface adjacent to the starting feature point on the light-emitting surface is obtained, and the second feature point on the light-emitting surface corresponds to the second illuminated point adjacent to the initial illuminated point ;
步骤i2:针对N个小段中的每一个小段执行步骤i1,依次求出N个小段中的各个被照点所对应的透镜出光面上的各特征点的位置;Step i2: performing step i1 for each of the N small segments, and sequentially determining the positions of the feature points on the lens light-emitting surface corresponding to each of the N small segments;
步骤6.4:将所述透镜入光面上的各特征点依次连接,将所述透镜出光面上的各特征点依次连接,形成两条连续曲线。Step 6.4: sequentially connecting the feature points on the light incident surface of the lens, and sequentially connecting the feature points on the light exiting surface of the lens to form two continuous curves.
优选地,所述各特征点依次用直线或平滑曲线连接起来。Preferably, the feature points are sequentially connected by a straight line or a smooth curve.
优选地,LED圈带的数量为2条,所述二次配光透镜形成的配光曲线分隔为2个部分,其中,一部分配光曲线的配光角度小于180度,另一部分配光曲线的配光角度大于等于180度。Preferably, the number of LED loops is two, and the light distribution curve formed by the secondary light distribution lens is divided into two parts, wherein a light distribution angle of a part of the light distribution curve is less than 180 degrees, and another part of the light distribution curve The light distribution angle is greater than or equal to 180 degrees.
根据本发明提供的一种全周光配光透镜,所述全周光配光透镜是根据上述的全周光配光透镜的设计方法得到的。According to the present invention, a full-circumferential light distribution lens is obtained according to the above-described design method of a full-circumferential light distribution lens.
优选地,所述全周光配光透镜的中间带有通孔。Preferably, the full-circumferential light distribution lens has a through hole in the middle thereof.
与现有技术相比,本发明具有如下的有益效果:Compared with the prior art, the present invention has the following beneficial effects:
(1)可实现大于180度的全周光配光照明;(1) Full-perimeter light distribution illumination greater than 180 degrees can be achieved;
(2)采用计算特征点确定透镜曲面的办法可以更加准确快速地确定透镜内外表面形状;(2) The method of determining the surface of the lens by calculating the feature points can determine the shape of the inner and outer surfaces of the lens more accurately and quickly;
(3)采用整体透镜配光的形式,避免了单体透镜装配对配光的影响。(3) The form of integral lens light distribution avoids the influence of single lens assembly on light distribution.
附图说明DRAWINGS
通过阅读参照以下附图对非限制性实施例所作的详细描述,本发明的其它特征、目的和优点将会变得更明显:Other features, objects, and advantages of the present invention will become apparent from the Detailed Description of Description
图1为传统投射式透镜外形图;Figure 1 is an outline view of a conventional projection lens;
图2为全周光配光系统整体结构图;2 is an overall structural view of a full-circumference light distribution system;
图3为全周光配光透镜配光曲线分割图;3 is a sectional view of a light distribution curve of a full-circumferential light distribution lens;
图4为在入射面上划分小角的方法示意图;4 is a schematic view showing a method of dividing a small angle on an incident surface;
图5为在出射的配光空间划分小段的方法示意图;FIG. 5 is a schematic diagram of a method for dividing a small section in an outgoing light distribution space; FIG.
图6为确定透镜表面上各特征点并依次连接的示意图;6 is a schematic view for determining feature points on a surface of a lens and sequentially connecting them;
图7为实施例1阶梯状圆台形透镜截面图示;Figure 7 is a cross-sectional view of the stepped truncated cone lens of Embodiment 1;
图8为实施例1阶梯状圆台形自由曲面透镜外形图;Figure 8 is an external view of a stepped truncated freeform lens of Embodiment 1;
图9为实施例2阶梯状圆台形透镜截面图示; Figure 9 is a cross-sectional view showing a stepped truncated cone lens of Embodiment 2;
图10为实施例2阶梯状圆台形自由曲面透镜外形图。Figure 10 is a perspective view showing the stepped truncated free-form surface lens of the second embodiment.
具体实施方式detailed description
下面结合具体实施例对本发明进行详细说明。以下实施例将有助于本领域的技术人员进一步理解本发明,但不以任何形式限制本发明。应当指出的是,对本领域的普通技术人员来说,在不脱离本发明构思的前提下,还可以做出若干变形和改进。这些都属于本发明的保护范围。The invention will now be described in detail in connection with specific embodiments. The following examples are intended to further understand the invention, but are not intended to limit the invention in any way. It should be noted that a number of variations and modifications may be made by those skilled in the art without departing from the inventive concept. These are all within the scope of protection of the present invention.
本发明旨在构造一种可实现大于180度全周光配光的配光方法。该配光方法包括环形排列的LED光源1以及二次配光透镜2,如图2所示。所述LED光源1在不同水平面上排列成多个环形的圈带,并且以一定的圆锥角度在立体空间形成环形堆叠的三维排列形式;所述二次配光透镜2为阶梯状圆台形。阶梯状圆形台自由曲面透镜(如图2),其设计步骤如下:The present invention is directed to constructing a light distribution method that achieves full-circumference light distribution greater than 180 degrees. The light distribution method includes an annularly arranged LED light source 1 and a secondary light distribution lens 2, as shown in FIG. The LED light source 1 is arranged in a plurality of annular loops on different horizontal planes, and forms a three-dimensional array of annular stacks in a three-dimensional space at a certain conical angle; the secondary light distribution lens 2 has a stepped truncated cone shape. Stepped circular table free-form lens (Figure 2), the design steps are as follows:
a)跟据LED光源的圈带数目,将二次配光透镜2形成的配光曲线分隔为相等数量的多个部分。例如图2中LED光源排列成2个环形的圈带,则二次配光透镜2形成的配光曲线也分隔为两个部分,其中,一部分配光曲线的配光角度小于180度,另一部分配光曲线的配光角度大于等于180度,当配光曲线分成3个以上的部分时,这三个部分的配光角度可以进行任意分配,只要保证与LED圈带能量守恒的原则即可。(如图3所示,L1表示小于180度的配光部分,L2表示大于180度的配光部分),并且这两部分配光曲线所包含光通量比例等于各圈带LED光源的总光通比例,透镜的设计将针对分隔好的各部分配光曲线进行分别设计;a) According to the number of loops of the LED light source, the light distribution curve formed by the secondary light distribution lens 2 is divided into an equal number of portions. For example, in FIG. 2, the LED light sources are arranged in two annular loops, and the light distribution curve formed by the secondary light distribution lens 2 is also divided into two parts, wherein a part of the light distribution curve has a light distribution angle of less than 180 degrees, and the other part The light distribution angle of the light distribution curve is greater than or equal to 180 degrees. When the light distribution curve is divided into three or more parts, the light distribution angles of the three parts can be arbitrarily distributed, as long as the principle of conservation of energy with the LED circle is ensured. (As shown in Fig. 3, L1 represents a light distribution portion of less than 180 degrees, L2 represents a light distribution portion of more than 180 degrees), and the ratio of the luminous flux contained in the two portions of the light distribution curve is equal to the total luminous flux ratio of the LED light source of each of the coils. The design of the lens will be separately designed for the divided light distribution curves;
b)以任意一条环形LED光源构成LED光源圈带的光轴平面作为入射面,在所述入射面上,将光轴一侧的光源角度等分为N个小角,其中N≥4,即各光源角度是按相等的角度间隔进行分配。为使图形清晰,本实施例取N=4,即划分为4个小角,分别为ɑ1、ɑ2、ɑ3、ɑ4。;b) forming an optical axis plane of the LED light source ring with any one of the ring-shaped LED light sources as an incident surface, and dividing the light source angle of the optical axis side into N small angles on the incident surface, wherein N≥4, that is, each The source angles are assigned at equal angular intervals. In order to make the figure clear, this embodiment takes N=4, that is, it is divided into 4 small angles, which are ɑ1, ɑ2, ɑ3, ɑ4, respectively. ;
c)将步骤a)分隔好的配光曲线(即光强随发光角度的分布)分为4个小段,分别为ab,bc,cd,de,4段配光曲线中的每段对应的光通量与步骤b)分隔的每个光源角度光通量相等;c) dividing the light distribution curve separated by step a) (that is, the distribution of light intensity with the angle of illumination) into four sub-sections, respectively, corresponding to the luminous flux of each of the ab, bc, cd, de, and 4-segment light distribution curves The angular flux of each source separated from step b) is equal;
d)将所述LED光源圈带的4个小角与所述配光曲线4个小段一一对应;d) aligning the four small corners of the LED light source ring with the four small segments of the light distribution curve;
e)以所述ab小段作为起始被照小段,以a点为起始被照点,则ab段对应的小角为ɑ1,根据透镜入光面201离开光源的距离要求,在与a点对应的入射光线上取一点1a作为透镜入光面上的起始特征点,在该起始特征点处,平行于光源与起始被照点a 的连线的直线同入射光线形成一夹角β1,为透镜的起始光线偏折角,将所述起始光线偏折角β1分成第一偏折角β11和第二偏折角β12,两个偏折角大小比例可以为任意,本实施例取β11:β12=1:1,角分线作为入射光线经过入光面(透镜的入光面201和出光面202分别指透镜的内表面和外表面)的起始特征点1a后的折射线,通过折射定律,确定1a点的法线n1,垂直于法线n1的直线与所述的光线入射面形成一交线,该交线与小角ɑ1的角边的交点分别为1a和1b,1b点即作为第二特征点,在第二被照小段bc上,取b点为第二被照点,则b点对应了该第二特征点1b。由上面的方法可知,只要求出各征点的法线就能求出各个特征点----各特征点法线的具体求解方法如下:1、通过该特征点入射光线方向求出该特征点的入射向量Nin;2、通过该特征点的折射光线方向求出该特征点的折射向量Nrefract;3、通过折射定律的如下向量表达式就可以求出各特征点的法向量:Nf=n*Nrefract–n0*Nin;其中Nf为该特征点的法向量,n为折射光线所在介质折射率,n0为入射光线所在介质折射率。e) taking the ab small segment as the starting small segment, starting from the point a, the corresponding small angle of the ab segment is ɑ1, according to the distance requirement of the lens entering the light surface 201 leaving the light source, corresponding to the point a A point 1a is taken as the starting feature point on the incident surface of the lens, and at the starting feature point, parallel to the light source and the initial illuminated point a The line connecting the line forms an angle β1 with the incident light, which is the initial light deflection angle of the lens, and divides the initial light deflection angle β1 into a first deflection angle β11 and a second deflection angle β12, and the two deflection angles The ratio can be arbitrary. In this embodiment, β11:β12=1:1, and the angular line is taken as the incident light passing through the light incident surface (the light incident surface 201 and the light exit surface 202 of the lens respectively refer to the inner surface and the outer surface of the lens). The refracting line after the characteristic point 1a is determined by the law of refraction to determine the normal line n1 of the point 1a, and the line perpendicular to the normal line n1 forms an intersection with the incident surface of the light, which intersects with the corner of the small corner ɑ1 The intersection points are 1a and 1b, respectively, and the 1b point is the second feature point. On the second illuminated segment bc, the b point is taken as the second illuminated point, and the b point corresponds to the second feature point 1b. According to the above method, as long as the normal line of each sign is obtained, each feature point can be obtained--the specific method for solving the normal of each feature point is as follows: 1. The feature is obtained by the incident light direction of the feature point. The incident vector Nin of the point; 2. The refractive index Nrefract of the feature point is obtained by the direction of the refracted ray of the feature point; 3. The normal vector of each feature point can be obtained by the following vector expression of the law of refraction: Nf=n *Nrefract–n0*Nin; where Nf is the normal vector of the feature point, n is the refractive index of the medium where the ray is refracted, and n0 is the refractive index of the medium where the incident ray is located.
f)同上一步骤,依次求出4个小段中的各个被照点c,d,e所对应的透镜入光面201上的各特征点1c,1d,1e的位置;f) in the same step as above, sequentially determining the positions of the feature points 1c, 1d, 1e on the lens entrance surface 201 corresponding to the respective illuminated points c, d, e of the four segments;
g)在经过所述透镜入光面201上的起始特征点1a后的折射线上,根据透镜厚度要求取一点2a,作为透镜出光面202上的起始特征点,采用与得到入光面上的特征点类似的方法,求出透镜出光面202上的各特征点的位置;具体为:g) taking a point 2a according to the lens thickness requirement on the refracting line after passing through the starting feature point 1a on the lens entrance surface 201, as the starting feature point on the lens exit surface 202, adopting and obtaining the illuminating surface A similar method is used to determine the position of each feature point on the light exiting surface 202 of the lens; specifically:
根据全周光配光透镜厚度的要求,在经过入光面上的起始特征点1a后的折射线上取一点2a作为出光面202上的起始特征点,以该折射线作为透镜出光面202的入射线,以在该2a点平行于被照点a与光源的连线的直线为透镜出光面202的折射线,该入射线和折射线方向即为图示的第二偏折角β12的两个角边方向,采用与确定入光面的特征点完全相同的方法,依次求得第二面上的特征点2b、2c、2d、2e的位置。According to the requirement of the thickness of the full-circumferential light distribution lens, a point 2a is taken as a starting feature point on the light-emitting surface 202 on the refracting line passing through the initial feature point 1a on the light-incident surface, and the refracting line is used as the lens light-emitting surface. The incident ray of 202 is a refracting line of the lens exit surface 202 parallel to the line connecting the illuminated point a and the light source at the point 2a, and the direction of the incident ray and the refracting line is the second offset angle β12 of the figure. In the two corner directions, the positions of the feature points 2b, 2c, 2d, and 2e on the second surface are sequentially determined in exactly the same manner as the feature points for determining the light incident surface.
h)将所述的入光面201和出光面202上的各特征点依次连接,分别形成两条连续曲线;h) sequentially connecting the feature points on the light-incident surface 201 and the light-emitting surface 202 to form two continuous curves;
i)同以上步骤,求出另一条圈带LED光源构成LED光源环带所对应的两条连续曲线203和204;i) with the above steps, find another circle with LED light source to form two continuous curves 203 and 204 corresponding to the LED light source ring;
j)将所述四条曲线两两连接形成一个封闭的曲线,绕圈带光源的排列中心轴线205旋转,形成透镜的立体形状。j) The four curves are connected in pairs to form a closed curve, and the central axis 205 of the circled light source is rotated to form a three-dimensional shape of the lens.
本发明的另一种实施方式,为了达到更好的散热效果,配合中间带通孔的灯座使用,透镜还可以设计为中间带通孔的形状,在设计时,全周光配光透镜的光学设计原理同第 一实施例的方法,只是从中央带通孔的位置边缘开始设计,求出光学曲线,然后连接起来,再绕中心轴线旋转,形成透镜的立体开关,如图9、图10所示。In another embodiment of the present invention, in order to achieve a better heat dissipation effect, the lens can also be designed as a middle belt through hole in the shape of a middle band through hole. In design, the full circumference light distribution lens The principle of optical design is the same as the first The method of an embodiment is only designed from the position edge of the central band through hole, and the optical curve is obtained, and then connected, and then rotated around the central axis to form a stereoscopic switch of the lens, as shown in FIG. 9 and FIG.
以上对本发明的具体实施例进行了描述。需要理解的是,本发明并不局限于上述特定实施方式,本领域技术人员可以在权利要求的范围内做出各种变形或修改,这并不影响本发明的实质内容。 The specific embodiments of the present invention have been described above. It is to be understood that the invention is not limited to the specific embodiments described above, and various modifications and changes may be made by those skilled in the art without departing from the scope of the invention.

Claims (5)

  1. 一种全周光配光透镜的设计方法,其特征在于,包括如下步骤:A method for designing a full-circumferential light distribution lens, comprising the steps of:
    步骤1:设置多条LED圈带以及环绕于LED圈带的二次配光透镜;Step 1: setting a plurality of LED loops and a secondary light distribution lens surrounding the LED loops;
    每条LED圈带均主要由在一平面内环形排列的LED光源构成;Each LED ring strip is mainly composed of an LED light source arranged in a circle in a plane;
    所述多条LED圈带的包络面为一圆台侧面;The envelope surface of the plurality of LED ring strips is a round table side;
    所述二次配光透镜形成的配光曲线分隔为与LED圈带数量相等的多个部分,所述多个部分与所述多个LED圈带一一对应;The light distribution curve formed by the secondary light distribution lens is divided into a plurality of portions equal to the number of LED loops, and the plurality of portions are in one-to-one correspondence with the plurality of LED loop strips;
    部分配光曲线的配光角度小于180度,部分配光曲线的配光角度大于等于180度,各部分配光曲线所包含光通量比例等于各LED圈带的总光通比例;The light distribution angle of the partial light distribution curve is less than 180 degrees, and the light distribution angle of the partial light distribution curve is greater than or equal to 180 degrees, and the proportion of the light flux included in each part of the light distribution curve is equal to the total light flux ratio of each LED ring band;
    步骤2:以任意一条LED圈带的光轴平面作为入射面,在所述入射面上,将光轴一侧的LED圈带的光源角度等分为N个小角,其中N≥4,即各光源角度按相等的角度间隔进行分配;Step 2: taking the plane of the optical axis of any one of the LED coils as the incident surface, and on the incident surface, dividing the angle of the light source of the LED ring on the optical axis into N small angles, wherein N≥4, that is, each The angles of the light sources are distributed at equal angular intervals;
    步骤3:将步骤1分隔好的配光曲线分为N个小段,N段配光曲线中的每段对应的光通量均与步骤2分配的光源角度光通量相等;Step 3: The light distribution curve separated by step 1 is divided into N small segments, and the corresponding luminous flux of each segment in the N-segment light distribution curve is equal to the luminous flux of the light source distributed in step 2;
    步骤4:将所述N个小角与所述配光曲线N个小段一一对应;Step 4: The N small angles are respectively corresponding to the N small segments of the light distribution curve;
    步骤5:以所述N个小段中的边缘小段作为起始被照小段,以边缘点为起始被照点,即对应所述N个小角中的一个小角;Step 5: taking the edge segment of the N segments as the starting segment, and starting the segment with the edge point, that is, corresponding to one of the N small corners;
    步骤6:求出每条LED圈带所对应的两条连续曲线;Step 6: Find two consecutive curves corresponding to each LED band;
    步骤7:将各条LED圈带所对应的两条连续曲线依次首尾连接形成一个封闭的曲线,然后将所述封闭的曲线绕LED圈带的LED光源的排列中心轴线旋转,形成全周光配光透镜的立体形状;Step 7: The two consecutive curves corresponding to the LED strips are sequentially connected end to end to form a closed curve, and then the closed curve is rotated around the central axis of the LED light source of the LED ring to form a full-circumference light distribution. The three-dimensional shape of the optical lens;
    其中,所述步骤6包括如下步骤:Wherein, the step 6 includes the following steps:
    步骤6.1:根据全周光配光透镜的透镜入光面离开光源的距离要求,在与起始被照点对应的入射光线上取一点作为所述透镜入光面上的起始特征点,在该入光面上的起始特征点处,平行于LED光源与起始被照点连线的直线同入射光线形成一夹角,为二次配光透镜的起始光线偏折角,将所述起始光线偏折角分成第一偏折角和第二偏折角,第一偏折角和第二偏折角的角分线作为入射光线经过所述透镜入光面后的折射线,通过折射定律以及对应所述N个小角中的一个小角,求出与入光面上的起始特征点相邻的入光面上的第二特征点,该入光面上的第二特征点对应与起始被照点相邻的第二被照点; Step 6.1: according to the distance requirement of the lens entrance surface of the full-circumferential light distribution lens to leave the light source, take a point on the incident light corresponding to the initial illuminated point as the starting feature point of the lens entrance surface, At a starting feature point on the light incident surface, a line parallel to the line connecting the LED light source and the initial illuminated point forms an angle with the incident light, which is the initial light deflection angle of the secondary light distribution lens. The initial ray deflection angle is divided into a first deflection angle and a second deflection angle. The angular division of the first deflection angle and the second deflection angle is used as a refracting line of the incident ray passing through the lens entrance surface, and the refraction law and the corresponding a small angle of the N small angles is obtained, and a second feature point on the light incident surface adjacent to the initial feature point on the light incident surface is obtained, and the second feature point on the light incident surface corresponds to the initial illumination Pointing adjacent second illuminated points;
    步骤6.2:针对N个小段中的每一个小段执行步骤6.1,依次求出N个小段中的各个被照点所对应的透镜入光面上的各特征点的位置;Step 6.2: Perform step 6.1 for each of the N small segments, and sequentially determine the positions of the feature points on the light incident surface of the lens corresponding to each of the N small segments;
    步骤6.3:在经过所述透镜入光面上的起始特征点后的折射线上,根据二次配光透镜的透镜厚度要求取一点,作为全周光配光透镜的透镜出光面上的起始特征点,采用如下方式,求出透镜出光面上的各特征点的位置:Step 6.3: taking a point on the refracting line after passing the initial feature point on the light incident surface of the lens, according to the lens thickness requirement of the secondary light distribution lens, as the lens exit surface of the full-circumferential light distribution lens At the starting feature point, the position of each feature point on the light exit surface of the lens is obtained as follows:
    步骤i1:在该出光面上的起始特征点处,平行于LED光源与起始被照点连线的直线同入射光线形成一夹角,为二次配光透镜的起始光线偏折角,将所述起始光线偏折角分成第一偏折角和第二偏折角,第一偏折角和第二偏折角的角分线作为入射光线经过所述透镜出光面后的折射线,通过折射定律以及对应所述N个小角中的一个小角,求出与出光面上的起始特征点相邻的出光面上的第二特征点,该出光面上的第二特征点对应与起始被照点相邻的第二被照点;Step i1: at a starting feature point on the light-emitting surface, a line parallel to the line connecting the LED light source and the initial illuminated point forms an angle with the incident light, which is a starting light deflection angle of the secondary light distribution lens, The initial ray deflection angle is divided into a first deflection angle and a second deflection angle, and the angular division of the first deflection angle and the second deflection angle is used as a refracting line of the incident ray passing through the illuminating surface of the lens, and the law of refraction is Corresponding to one of the N small angles, determining a second feature point on the light exit surface adjacent to the starting feature point on the light exiting surface, the second feature point on the light exiting surface corresponding to the initial illuminated point Adjacent second illuminated point;
    步骤i2:针对N个小段中的每一个小段执行步骤i1,依次求出N个小段中的各个被照点所对应的透镜出光面上的各特征点的位置;Step i2: performing step i1 for each of the N small segments, and sequentially determining the positions of the feature points on the lens light-emitting surface corresponding to each of the N small segments;
    步骤6.4:将所述透镜入光面上的各特征点依次连接,将所述透镜出光面上的各特征点依次连接,形成两条连续曲线。Step 6.4: sequentially connecting the feature points on the light incident surface of the lens, and sequentially connecting the feature points on the light exiting surface of the lens to form two continuous curves.
  2. 根据权利要求1所述的一种具有全周光配光透镜设计方法,其特征在于:所述各特征点依次用直线或平滑曲线连接起来。A method for designing a full-circumferential light distribution lens according to claim 1, wherein each of the feature points is sequentially connected by a straight line or a smooth curve.
  3. 根据权利要求1所述的全周光配光透镜的设计方法,其特征在于,LED圈带的数量为2条,所述二次配光透镜形成的配光曲线分隔为2个部分,其中,一部分配光曲线的配光角度小于180度,另一部分配光曲线的配光角度大于等于180度。The method for designing a full-circumferential light distribution lens according to claim 1, wherein the number of LED loops is two, and the light distribution curve formed by the secondary light distribution lens is divided into two parts, wherein The light distribution angle of a part of the light distribution curve is less than 180 degrees, and the light distribution angle of the other part of the light distribution curve is greater than or equal to 180 degrees.
  4. 一种全周光配光透镜,其特征在于,所述配光透镜是根据权利要求1至3中任一项所述的全周光配光透镜的设计方法制造得到的。A full-perimeter light distribution lens obtained by the design method of the full-perimeter light distribution lens according to any one of claims 1 to 3.
  5. 根据权利要求4所述的全周光配光透镜,其特征在于,所述全周光配光透镜的中间带有通孔。 The full-perimeter light distribution lens according to claim 4, wherein the entire peripheral light distribution lens has a through hole in the middle thereof.
PCT/CN2014/091149 2014-09-23 2014-11-14 Method for designing full-periphery light distribution lens and corresponding light distribution lens WO2016045176A1 (en)

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