CN103257381A - Solar spotlight Fresnel lens and its designing method - Google Patents

Solar spotlight Fresnel lens and its designing method Download PDF

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CN103257381A
CN103257381A CN2013101769789A CN201310176978A CN103257381A CN 103257381 A CN103257381 A CN 103257381A CN 2013101769789 A CN2013101769789 A CN 2013101769789A CN 201310176978 A CN201310176978 A CN 201310176978A CN 103257381 A CN103257381 A CN 103257381A
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fresnel lens
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CN103257381B (en
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仇谷烽
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Suzhou University
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Abstract

本发明涉及一种太阳能聚光菲涅尔透镜及其设计方法。它依据光学折射原理,通过逐点计算菲涅尔镜曲面各处的导数,再对导数积分,获得透镜曲面各处的矢高。本发明设计方法可借助现代计算机技术,简便、快捷地完成菲涅尔透镜的设计。本发明技术方案与纯粹的光学设计方法相比,具有简单易行的特点;相对目前传统的菲涅尔透镜的设计方法而言,本发明设计方法提供的透镜具有光斑直径小,能量分布均匀等优点,能有效提高太阳能聚光透镜的光能转换效率,尤其是针对大口径的菲涅尔透镜,优点及效果更为明显。

The invention relates to a solar concentrating Fresnel lens and a design method thereof. Based on the principle of optical refraction, it calculates the derivatives of the Fresnel mirror surface point by point, and then integrates the derivatives to obtain the vector height of the lens surface. The design method of the invention can simply and quickly complete the design of the Fresnel lens by means of modern computer technology. Compared with the pure optical design method, the technical solution of the present invention has the characteristics of simplicity and ease; compared with the current traditional Fresnel lens design method, the lens provided by the design method of the present invention has small spot diameter, uniform energy distribution, etc. Advantages, can effectively improve the light energy conversion efficiency of solar concentrating lenses, especially for large-diameter Fresnel lenses, the advantages and effects are more obvious.

Description

一种太阳能聚光菲涅尔透镜及其设计方法A solar concentrating Fresnel lens and its design method

技术领域 technical field

本发明涉及一种聚光透镜及其设计方法,特别涉及一种用于太阳能聚光的菲涅尔透镜及设计方法。 The invention relates to a concentrating lens and a design method thereof, in particular to a Fresnel lens and a design method for concentrating solar energy.

背景技术 Background technique

菲涅尔透镜是由法国物理学家Augustin Jean Fresnel在1822年所发明的一种透镜,与传统的球面或非球面透镜相比,菲涅尔透镜采用多个同轴排列或平行排列的棱镜序列组成不连续曲面取代了一般透镜的连续球面,因此,菲涅尔透镜结构简单,便于制造,在重量和体积上比一般透镜更轻、更薄,在设计上可以获得更大的孔径与焦距比。虽然菲涅尔透镜最初主要是为灯塔探照灯而设计,但目前菲涅尔透镜在投影仪、大屏幕背投电视、便携放大镜、太阳能热水器、太阳能电站以及空间飞行器的太阳能帆板等众多领域获得了广泛的应用。 Fresnel lens is a kind of lens invented by French physicist Augustin Jean Fresnel in 1822. Compared with traditional spherical or aspherical lenses, Fresnel lens adopts multiple coaxial or parallel prism sequences The discontinuous curved surface replaces the continuous spherical surface of the general lens. Therefore, the Fresnel lens has a simple structure, is easy to manufacture, is lighter and thinner than the general lens in terms of weight and volume, and can obtain a larger aperture to focal length ratio in design. . Although Fresnel lenses were originally designed for lighthouse searchlights, Fresnel lenses are currently used in many fields such as projectors, large-screen rear projection TVs, portable magnifying glasses, solar water heaters, solar power plants, and solar panels for space vehicles. Wide range of applications.

最初的菲涅透镜由于当时的制作工艺和光学设计、加工技术所限,采用的是棱镜序列。但从光学原理上来说,棱镜序列不能把光聚焦在一点上,从而使这种类型菲涅尔镜的光斑很大,光斑的温度不能很高,且光斑能量不均匀。 The original Fresnel lens used a prism sequence due to the limitations of the manufacturing process, optical design and processing technology at that time. However, from an optical point of view, the prism sequence cannot focus light on one point, so that the spot of this type of Fresnel mirror is large, the temperature of the spot cannot be very high, and the energy of the spot is not uniform.

在本发明作出之前,文献“菲涅尔透镜统一设计方法”([J].太阳能学报,1991 ,12 (4) :423-426.)和“菲涅尔聚光透镜的一般设计方法及效率分析”([J].武汉理工大学学报,2010,3(6):62-66),分别在棱镜序列设计的基础上提出了一些改进的方法。现代计算机技术的发展和加工工艺水平的提高,使设计和加工更为复杂的菲涅尔透镜成为了可能,另一种基于非球面的菲涅尔透镜设计方法,采用一系列球面进行设计。从光学原理可知,球面镜对于近轴光线可很好聚焦于一点,离轴越远,聚焦就会越偏离焦点,因此,上述设计在制作大口径的菲涅尔透镜上并不太适合。 Before the present invention was made, the literature "Fresnel lens unified design method" ([J]. Solar Energy Sinica, 1991, 12 (4): 423-426.) and "General design method and efficiency of Fresnel concentrating lens Analysis” ([J]. Journal of Wuhan University of Technology, 2010,3(6):62-66), some improved methods were proposed on the basis of prism sequence design. The development of modern computer technology and the improvement of processing technology have made it possible to design and process more complex Fresnel lenses. Another Fresnel lens design method based on aspheric surfaces uses a series of spherical surfaces for design. From the principle of optics, it can be seen that the spherical mirror can focus on the paraxial light well at one point. The farther away from the axis, the more the focus will be out of focus. Therefore, the above design is not suitable for making large-diameter Fresnel lenses.

发明内容 Contents of the invention

本发明的目的在于克服现有技术存在的不足,提供了一种聚光弥散圆直径小,光能分布均匀,光斑温度高,能有效提高光能转换效率的太阳能聚光菲涅尔透镜及其设计方法。 The purpose of the present invention is to overcome the deficiencies in the prior art and provide a solar concentrating Fresnel lens with a small diameter of the concentrating diffusion circle, uniform distribution of light energy, high spot temperature, and effective improvement of light energy conversion efficiency. design method.

实现本发明目的的技术方案是提供一种太阳能聚光菲涅尔透镜的设计方法,包括如下步骤: The technical scheme that realizes the object of the present invention is to provide a kind of design method of solar concentrating Fresnel lens, comprises the steps:

1、以菲涅尔镜的母线正方向为X轴,在X轴上按等间距dx分成n等分,各节点的坐标分别为X1、X2……Xn1. Take the positive direction of the busbar of the Fresnel mirror as the X-axis, and divide it into n equal parts according to the equal distance dx on the X-axis, and the coordinates of each node are X 1 , X 2 ... X n ;

2、在                                                

Figure 2013101769789100002DEST_PATH_IMAGE001
处,设定母线矢高
Figure 90153DEST_PATH_IMAGE002
及母线在该处的导数
Figure 2013101769789100002DEST_PATH_IMAGE003
为0;  2. In
Figure 2013101769789100002DEST_PATH_IMAGE001
, set the busbar vector height
Figure 90153DEST_PATH_IMAGE002
and the derivative of the bus at that point
Figure 2013101769789100002DEST_PATH_IMAGE003
is 0;

3、按

Figure 546278DEST_PATH_IMAGE004
,估算
Figure 2013101769789100002DEST_PATH_IMAGE005
处的矢高,再根据光学折射原理确定
Figure 913193DEST_PATH_IMAGE006
处的导数
Figure 2013101769789100002DEST_PATH_IMAGE007
,按式
Figure 78028DEST_PATH_IMAGE008
,确定下一坐标处的矢高
Figure 2013101769789100002DEST_PATH_IMAGE009
;重复本步骤,得到任意位置处的矢高
Figure 2013101769789100002DEST_PATH_IMAGE011
; 3. Press
Figure 546278DEST_PATH_IMAGE004
, estimated
Figure 2013101769789100002DEST_PATH_IMAGE005
The sagittal height at the place is determined according to the principle of optical refraction
Figure 913193DEST_PATH_IMAGE006
derivative at
Figure 2013101769789100002DEST_PATH_IMAGE007
, press
Figure 78028DEST_PATH_IMAGE008
, determine the next coordinate Yataka
Figure 2013101769789100002DEST_PATH_IMAGE009
;Repeat this step to get any position Yataka
Figure 2013101769789100002DEST_PATH_IMAGE011
;

4、判断是否大于等于指定深度,或判断

Figure 101029DEST_PATH_IMAGE012
是否大于等于指定宽度;若是,则当前环带设计完成,执行步骤5;反之,返回步骤3; 4. Judgment Whether it is greater than or equal to the specified depth, or judge
Figure 101029DEST_PATH_IMAGE012
Whether it is greater than or equal to the specified width; if so, the current ring design is completed, and step 5 is performed; otherwise, return to step 3;

5、将下一个

Figure 964992DEST_PATH_IMAGE012
所对应的
Figure 325435DEST_PATH_IMAGE011
Figure 2013101769789100002DEST_PATH_IMAGE013
设定为0,对剩余节点的坐标x,重复步骤3~4进行下一环带的设计,依次完成全部环带的设计,得到一种太阳能聚光菲涅尔透镜。 5. Put the next
Figure 964992DEST_PATH_IMAGE012
Corresponding
Figure 325435DEST_PATH_IMAGE011
and
Figure 2013101769789100002DEST_PATH_IMAGE013
Set it to 0, repeat steps 3-4 for the next ring design for the coordinate x of the remaining nodes, complete the design of all rings in turn, and obtain a solar concentrating Fresnel lens.

本发明技术方案还包括按上述设计方法得到的一种太阳能聚光菲涅尔透镜。 The technical solution of the present invention also includes a solar concentrating Fresnel lens obtained by the above design method.

由于上述设计方案的运用,本发明与现有技术相比具有下列优点: Due to the utilization of the above-mentioned design scheme, the present invention has the following advantages compared with the prior art:

1、本发明提供的设计方法不同于传统的设计方法直接计算曲面的矢高,而是通过计算曲线各点处的导数,再对各点导数的数值积分从而获取曲线的矢高,设计中,只需给定材料折射率,口径、焦距和允许深度或宽度,就能获得需要的菲涅尔曲面,设计方法简单,调整灵活,且设计周期短,成本低。 1. The design method provided by the present invention is different from the traditional design method to directly calculate the vector height of the curved surface, but by calculating the derivative at each point of the curve, and then integrating the numerical value of the derivative at each point to obtain the vector height of the curve. In the design, only need Given the refractive index of the material, aperture, focal length and allowable depth or width, the required Fresnel surface can be obtained, the design method is simple, the adjustment is flexible, and the design cycle is short and the cost is low.

2、相对于传统的设计方法,由于本发明设计的面形理论上能把太阳光聚焦于一点,因此,得到的聚光弥散圆的光能分布均匀;还由于设计的菲涅尔透镜弥散圆直径较小,因此,在同样口径条件下,光斑能达到的温度比传统的设计要高很多,从而可大幅提高光能的转换效率。 2. Compared with the traditional design method, because the surface shape designed by the present invention can theoretically focus sunlight on one point, the light energy distribution of the obtained concentrating circle of confusion is uniform; also because the designed Fresnel lens circle of confusion The diameter is small, so under the same aperture conditions, the temperature that the spot can reach is much higher than that of the traditional design, which can greatly improve the conversion efficiency of light energy.

4.设计方法适用于任何类型的菲涅尔透镜。 4. The design method is applicable to any type of Fresnel lens.

附图说明 Description of drawings

图1 是本发明提供的一种太阳能聚光菲涅尔透镜的设计原理图; Fig. 1 is the design schematic diagram of a kind of solar concentrating Fresnel lens provided by the present invention;

图2 是按本发明实施例提供的设计方法得到的菲涅尔环带的结果示意图; Fig. 2 is the result schematic diagram of the Fresnel annulus that obtains by the design method that the embodiment of the present invention provides;

图3是按传统设计方法制造的菲涅尔透镜的光斑图; Fig. 3 is the light spot figure of the Fresnel lens manufactured by traditional design method;

图4是本发明实施例提供的菲涅尔透镜的光斑图。 Fig. 4 is a light spot diagram of a Fresnel lens provided by an embodiment of the present invention.

具体实施方式 Detailed ways

下面结合附图和实施例对本发明技术方案作进一步阐述。 The technical solutions of the present invention will be further elaborated below in conjunction with the accompanying drawings and embodiments.

实施例1: Example 1:

利用本发明设计如下要求的菲涅尔透镜:材料折射率n=1.499,口径D=120mm,焦距f=120,指定深度h=1mm。 Utilize the present invention to design a Fresnel lens with the following requirements: material refractive index n=1.499, aperture D=120mm, focal length f=120, specified depth h=1mm.

本实施例提供的菲涅尔镜设计方法的具体实施步骤如下: The specific implementation steps of the Fresnel mirror design method provided in this embodiment are as follows:

1、参见附图1,它是本发明提供的菲涅尔镜设计方法的原理图,设菲涅尔透镜的中心点坐标为

Figure 834651DEST_PATH_IMAGE014
,该点处的导数为
Figure 2013101769789100002DEST_PATH_IMAGE015
,把菲涅尔镜的母线沿X轴正方向按等间距dx分成N等分,第1点的坐标为
Figure 295283DEST_PATH_IMAGE016
,该点处的导数为
Figure 2013101769789100002DEST_PATH_IMAGE017
Figure 827633DEST_PATH_IMAGE018
为平行光线在
Figure 2013101769789100002DEST_PATH_IMAGE019
处的入射角。 1, referring to accompanying drawing 1, it is the schematic diagram of the Fresnel mirror design method that the present invention provides, suppose the center point coordinate of Fresnel lens is
Figure 834651DEST_PATH_IMAGE014
, the derivative at this point is
Figure 2013101769789100002DEST_PATH_IMAGE015
, divide the generatrix of the Fresnel mirror into N equal parts along the positive direction of the X-axis at equal intervals dx, and the coordinates of the first point are
Figure 295283DEST_PATH_IMAGE016
, the derivative at this point is
Figure 2013101769789100002DEST_PATH_IMAGE017
,
Figure 827633DEST_PATH_IMAGE018
for parallel rays in
Figure 2013101769789100002DEST_PATH_IMAGE019
angle of incidence at .

菲涅尔透镜的中心点坐标处的导数为

Figure 908820DEST_PATH_IMAGE015
,在中心处: Center point coordinates of Fresnel lens The derivative at is
Figure 908820DEST_PATH_IMAGE015
, at the center:

Figure 172311DEST_PATH_IMAGE020
Figure 172311DEST_PATH_IMAGE020
.

2、取dx=0.1,

Figure 2013101769789100002DEST_PATH_IMAGE021
。这时对应的z暂时以估算值:
Figure 942689DEST_PATH_IMAGE022
 近似表达。 2. Take dx=0.1,
Figure 2013101769789100002DEST_PATH_IMAGE021
. At this time, the corresponding z is temporarily estimated:
Figure 942689DEST_PATH_IMAGE022
approximate expression.

根据光学折射原理可导出方程如式(1)所示: According to the principle of optical refraction, the equation can be derived as shown in formula (1):

Figure 2013101769789100002DEST_PATH_IMAGE023
                (1) ;
Figure 2013101769789100002DEST_PATH_IMAGE023
(1) ;

式中,f为焦距,n为材料的折射率,在本实施例中,f=120,n=1.499;从方程式(1)中求解出

Figure 458702DEST_PATH_IMAGE024
,则对应的
Figure 2013101769789100002DEST_PATH_IMAGE025
。在求出后,将实际对应的z值确定为:
Figure 65318DEST_PATH_IMAGE026
。 In the formula, f is the focal length, n is the refractive index of the material, in this embodiment, f=120, n=1.499; from the equation (1) to solve
Figure 458702DEST_PATH_IMAGE024
, then the corresponding
Figure 2013101769789100002DEST_PATH_IMAGE025
. in seeking After that, the actual corresponding z value is determined as:
Figure 65318DEST_PATH_IMAGE026
.

3、重复步骤2,可依次计算出: 3. Repeat step 2 to calculate in turn:

Figure 2013101769789100002DEST_PATH_IMAGE027
 
Figure 572261DEST_PATH_IMAGE028
Figure 2013101769789100002DEST_PATH_IMAGE027
 
Figure 572261DEST_PATH_IMAGE028

…… ...

   

第一环带计算结束。可用计算机软件编写一个简单的计算程序,完成上述的计算。 The calculation of the first ring is completed. A simple calculation program can be written with computer software to complete the above calculations.

4、第一环带的结束x坐标为

Figure 2013101769789100002DEST_PATH_IMAGE031
。重新设定起始点(
Figure 343743DEST_PATH_IMAGE032
): 4. The end x-coordinate of the first ring is
Figure 2013101769789100002DEST_PATH_IMAGE031
. Reset the starting point (
Figure 343743DEST_PATH_IMAGE032
):

Figure 73671DEST_PATH_IMAGE034
,
Figure 73671DEST_PATH_IMAGE034

根据光学折射原理计算出对应的:

Figure 2013101769789100002DEST_PATH_IMAGE035
。 Calculate the corresponding according to the principle of optical refraction:
Figure 2013101769789100002DEST_PATH_IMAGE035
.

5、重复步骤2、3可完成第二环带的设计。 5. Repeat steps 2 and 3 to complete the design of the second ring.

Figure 547203DEST_PATH_IMAGE036
 
Figure 2013101769789100002DEST_PATH_IMAGE037
Figure 547203DEST_PATH_IMAGE036
 
Figure 2013101769789100002DEST_PATH_IMAGE037

…… ...

Figure 840519DEST_PATH_IMAGE038
 
Figure 2013101769789100002DEST_PATH_IMAGE039
Figure 840519DEST_PATH_IMAGE038
 
Figure 2013101769789100002DEST_PATH_IMAGE039

6、重复步骤4、5可完成任意个环带的设计,从而完成整个菲涅尔透镜的设计。 6. Repeat steps 4 and 5 to complete the design of any rings, thereby completing the design of the entire Fresnel lens.

本实施例设计的最后一个环带是第26环带,X26=59.500000000001 The last ring designed in this embodiment is the 26th ring, X 26 =59.500000000001

Figure 721756DEST_PATH_IMAGE040
 
Figure 2013101769789100002DEST_PATH_IMAGE041
Figure 721756DEST_PATH_IMAGE040
 
Figure 2013101769789100002DEST_PATH_IMAGE041

…… ...

   

参见附图2,它是按上述步骤得到的菲涅尔透镜的环带结果示意图(图中的坐标单位均为mm)。 See accompanying drawing 2, which is a schematic diagram of the annular zone results of the Fresnel lens obtained according to the above steps (the coordinate units in the figure are all in mm).

参见附图3和图4,它们分别是按传统方法设计的菲涅尔透镜的光斑图及采用本实施例设计方法设计的菲涅尔透镜的光斑图;对比图3和图4的结果可以看出,传统方法设计的菲涅尔透镜的光斑直径约为50mm,是个弥散斑;本实施例提供的菲涅尔透镜的光斑直径缩小至10mm左右,由于其光斑直径较小,因此,在相同口径条件下,光斑能达到的温度比传统设计的透镜要高得多,从而可大幅提高光能的转换效率。 Referring to accompanying drawing 3 and Fig. 4, they are respectively the spot pattern of the Fresnel lens designed by traditional method and the spot pattern of the Fresnel lens that adopts the present embodiment design method to design; Contrast the result of Fig. 3 and Fig. 4 and can see It can be seen that the spot diameter of the Fresnel lens designed by the traditional method is about 50 mm, which is a diffuse spot; the spot diameter of the Fresnel lens provided by this embodiment is reduced to about 10 mm. Under certain conditions, the temperature that the light spot can reach is much higher than that of the traditionally designed lens, which can greatly improve the conversion efficiency of light energy.

菲涅尔透镜的设计一般有二种准则:等宽度和等深。由于考虑到实际应用中,中心区域的光是主要的光能,因此应当保证中心区域的环带尽可能宽。因此等深设计的菲涅尔透镜更为实用,本实施例的步骤是基于等深设计的。对于等宽设计同样适用,只需要把环带变换的标准换成等宽即可。本发明设计方法比较简单,只需给定材料折射率n、透镜焦距f、透镜口径D及透镜深度h或宽度w就能快速计算出菲涅尔透镜的矢高数据。 There are generally two criteria for the design of Fresnel lenses: equal width and equal depth. Considering that in practical applications, the light in the central area is the main light energy, it should be ensured that the annular zone in the central area is as wide as possible. Therefore, a Fresnel lens with a constant depth design is more practical, and the steps in this embodiment are based on the constant depth design. It is also applicable to the equal width design, only need to change the standard of ring belt transformation to equal width. The design method of the invention is relatively simple, and the sagittal height data of the Fresnel lens can be quickly calculated only by giving the refractive index n of the material, the focal length f of the lens, the aperture D of the lens, and the depth h or width w of the lens.

Claims (2)

1. the method for designing of a Salar light-gathering Fresnel Lenses is characterized in that comprising the steps:
(1) the bus positive dirction with the Fresnel mirror is X-axis, is divided into the n five equilibrium by equidistant dx on X-axis, and the coordinate of each node is respectively X 1, X 2X n
(2) exist
Figure 423880DEST_PATH_IMAGE001
The place sets the bus rise
Figure 436836DEST_PATH_IMAGE002
And bus is at the derivative at this place
Figure 443975DEST_PATH_IMAGE003
Be 0;
(3) press
Figure 125621DEST_PATH_IMAGE004
, estimation
Figure 192804DEST_PATH_IMAGE005
The rise at place is determined according to the light refraction principle again
Figure 755372DEST_PATH_IMAGE006
The derivative at place
Figure 238306DEST_PATH_IMAGE007
, by formula
Figure 835509DEST_PATH_IMAGE008
, determine next coordinate
Figure 260543DEST_PATH_IMAGE006
The rise at place
Figure 310408DEST_PATH_IMAGE009
Repeat this step, obtain the optional position
Figure 665209DEST_PATH_IMAGE010
The rise at place
(4) judge
Figure 198007DEST_PATH_IMAGE011
Whether more than or equal to designated depth, or judge
Figure 922118DEST_PATH_IMAGE012
Whether more than or equal to specified width, which width; If then execution in step (5) is finished in current endless belt design; Otherwise, return step (3);
(5) with the next one
Figure 12434DEST_PATH_IMAGE012
Corresponding
Figure 318651DEST_PATH_IMAGE011
With
Figure 814049DEST_PATH_IMAGE013
Be set at 0, to the coordinate x of residue node, the design of next endless belt is carried out in repeating step (3)~(4), finishes the design of whole endless belt successively, obtains a kind of Salar light-gathering Fresnel Lenses.
2. a kind of Salar light-gathering Fresnel Lenses that obtains by the described method for designing of claim 1.
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CN114295082A (en) * 2021-12-10 2022-04-08 散裂中子源科学中心 High-precision detection method for curved wavefront and surface shape based on near-field speckle
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