CN107919848B - Annular linear Fresnel high-power condenser - Google Patents
Annular linear Fresnel high-power condenser Download PDFInfo
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- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 claims description 6
- 230000003287 optical effect Effects 0.000 claims description 6
- 229910052709 silver Inorganic materials 0.000 claims description 6
- 239000004332 silver Substances 0.000 claims description 6
- 238000010248 power generation Methods 0.000 claims description 3
- 238000005057 refrigeration Methods 0.000 claims 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims 1
- 238000000034 method Methods 0.000 abstract description 2
- 238000010586 diagram Methods 0.000 description 4
- 238000006243 chemical reaction Methods 0.000 description 2
- 239000002826 coolant Substances 0.000 description 2
- 229910021419 crystalline silicon Inorganic materials 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005611 electricity Effects 0.000 description 2
- 230000009286 beneficial effect Effects 0.000 description 1
- 239000000428 dust Substances 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000002310 reflectometry Methods 0.000 description 1
- 239000004576 sand Substances 0.000 description 1
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02S—GENERATION OF ELECTRIC POWER BY CONVERSION OF INFRARED RADIATION, VISIBLE LIGHT OR ULTRAVIOLET LIGHT, e.g. USING PHOTOVOLTAIC [PV] MODULES
- H02S40/00—Components or accessories in combination with PV modules, not provided for in groups H02S10/00 - H02S30/00
- H02S40/20—Optical components
- H02S40/22—Light-reflecting or light-concentrating means
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- G—PHYSICS
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- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B19/00—Condensers, e.g. light collectors or similar non-imaging optics
- G02B19/0033—Condensers, e.g. light collectors or similar non-imaging optics characterised by the use
- G02B19/0038—Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with ambient light
- G02B19/0042—Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with ambient light for use with direct solar radiation
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
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- Y02E10/52—PV systems with concentrators
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Abstract
本发明公开了一种环形线性菲涅尔高倍聚光器,主要包括聚光镜、聚光平面和支架。其设计方法如下。聚光镜1为环形分布的镀银聚光镜,其形状由一固定长度的线段绕轴旋转而形成无上下底面的圆台。2为菲涅耳透镜(只保留位置,未画出),3为聚光镜底托及支架,包括镜面链接结构用于支撑整套聚光镜。4为聚光平面,聚光镜反射的光线由位于接收盘中心的高倍聚光专用的光伏电池5接收。6为聚光平面与聚光镜底托的连杆,7为连接双轴聚光系统的连接头。本聚光器具有较大的聚光比。
The invention discloses a ring-shaped linear Fresnel high-power concentrator, which mainly comprises a condensing lens, a condensing plane and a bracket. Its design method is as follows. The condensing lens 1 is a silver-plated condensing lens with annular distribution, and its shape is a circular truncated cone without an upper and lower bottom surface formed by a line segment of a fixed length rotating around an axis. 2 is the Fresnel lens (only the position is reserved, not shown), 3 is the condenser bottom bracket and bracket, including the mirror link structure to support the entire set of condensers. 4 is a condensing plane, and the light reflected by the condensing mirror is received by a photovoltaic cell 5 dedicated to high-power concentrating located in the center of the receiving disc. 6 is the connecting rod between the condensing plane and the bottom bracket of the condensing lens, and 7 is the connecting head connecting the biaxial condensing system. The concentrator has a large condensing ratio.
Description
技术领域technical field
本发明属于高倍聚光光伏领域,同时也包含了光伏光热综合利用领域。涉及一种点聚光的环形高倍聚光器和点聚光的菲涅尔透镜高倍聚光器。The invention belongs to the field of high-power concentrating photovoltaics, and also includes the field of photovoltaic photothermal comprehensive utilization. The invention relates to a point-condensed annular high-power concentrator and a point-condensed Fresnel lens high-power concentrator.
背景技术Background technique
在太阳能聚光利用系统中,聚光器的选择直接影响了整个系统的布置。有别于非聚光光伏和低倍聚光光伏,高倍聚光光伏具有较高的转化率和效率。除了高转化率之外,高倍聚光光伏还具有温度系数小、电网匹配性好(日发电量高)、对环境友好(占地少、土地可综合利用)、效率可提升性强等特点。首先,应用于高倍聚光光伏的多结Ⅲ-Ⅴ族电池电池本身可以在较高温度下工作并能维持较好的效率,而且每一个聚光电池后面都配有一个散热器,因此在外部温度变化较大的情况下,相比较晶硅及薄膜电池,其本身的效率影响不会很大。据测算,聚光光伏电池在气温每升高一度后,效率的降低仅仅是晶硅电池的三分之一。因此,高倍聚光对于PV/T领域有着极大的作用。而高倍聚光需要与之对应的高倍聚光器,因此槽式聚光器,塔式聚光,线性菲涅尔聚光器都是效果相当好的高倍聚光器。而本专利提出的环形线性菲涅尔就是由线性菲涅尔聚光器改进而来。In the solar energy concentrating utilization system, the choice of the concentrator directly affects the arrangement of the whole system. Different from non-concentrating photovoltaics and low-power concentrating photovoltaics, high-power concentrating photovoltaics have higher conversion rates and efficiencies. In addition to high conversion rate, high-power CPV also has the characteristics of small temperature coefficient, good grid matching (high daily power generation), environmental friendliness (small land occupation, comprehensive utilization of land), and strong efficiency improvement. First, the multi-junction III-V cells used in high-power concentrator photovoltaics can work at higher temperatures and maintain better efficiency, and each concentrator is equipped with a heat sink behind it, so the external temperature In the case of large changes, compared with crystalline silicon and thin film batteries, its own efficiency will not be greatly affected. It is estimated that the efficiency of concentrating photovoltaic cells is only one-third of that of crystalline silicon cells when the temperature increases by one degree. Therefore, high-power concentration has a great effect on the PV/T field. High-power condensers require corresponding high-power condensers, so trough condensers, tower condensers, and linear Fresnel condensers are all high-power condensers with good effects. The annular linear Fresnel proposed in this patent is improved from the linear Fresnel concentrator.
专利内容Patent content
本专利提出的环形线性菲涅尔聚光器的目的是为了改变光线路径,将线性菲涅尔聚光器的线聚光方式转变为点聚光方式,这样会使聚光器的聚光比大大提高。环形分布的镀银聚光镜1中的每一环都为由一固定长度的线段绕轴旋转而形成无上下底面的圆台。且每条固定长度的线段的位置和倾角都不同。垂直入射的太阳光线通过环形分布的反光镜可以汇集在位于接收盘中央的高倍光伏电池5上。光伏电池5的背部装有专用散热器,以将光伏电池的热量带走,既可以降低光伏电池的温度,提高发电效率,同时带走的热量还可以用作产生生活热水或用作制冷等其它用途。每条环形分布的镀银聚光镜1互不遮挡,且对于每条环形聚光镜的横截面所形成的线段,上方线段的顶部端点与下方线段的底部端点所形成的直线与旋转轴平行。以保证每条环形聚光镜互不遮挡。整个装置采用带自动跟踪的双轴跟踪,以保证整个装置的中心轴正对太阳,保持阳光直射。聚光器中心有一光轴为整个装置对称轴的菲涅尔聚光透镜,其直径与装置没有反光镜的部分相同。聚光器中心的菲涅尔透镜的焦点与环形聚光镜的焦点重合,均在接收盘5上。阳光直射到环形分布的反光镜以及中心的菲涅尔透镜后,经反射和折射到接收盘5上的太阳能电池上,可产生电能,电池背部有冷却剂冷却,可产生热量。The purpose of the annular linear Fresnel concentrator proposed in this patent is to change the light path and convert the linear condensing mode of the linear Fresnel concentrator to the point condensing mode, which will make the condensing ratio of the concentrator higher. Greatly improve. Each ring in the annularly distributed silver-coated
本发明的有益效果为:The beneficial effects of the present invention are:
1、改进线性菲涅尔聚光器的光线分布路径,由线性改为环形,将沿地表分布的聚光器由水平改为垂直方向,可以节省面积。1. Improve the light distribution path of the linear Fresnel concentrator, from linear to circular, and change the concentrator distributed along the surface from horizontal to vertical, which can save area.
2、光线经反射镜和菲涅尔透镜照射到太阳能电池上后,可以产生电能,太阳能电池背部有冷却剂冷却,可以产生热能。2. After the light is irradiated on the solar cell by the reflector and the Fresnel lens, it can generate electricity, and the back of the solar cell is cooled by a coolant, which can generate heat energy.
3、空间利用率高。3. High space utilization rate.
4、聚光比高,光线汇聚后的能量密度大。4. The light concentration ratio is high, and the energy density after the light is concentrated is large.
Qn=-Htan2βn Q n = -Htan2β n
附图说明Description of drawings
附图1为本发明装置构造图。附图2为本发明边缘两块环形镜面的光路图,附图3为光路图的细节放大图。Accompanying
具体实施方式:Detailed ways:
下面结合附图和具体实施方式对本发明做进一步说明The present invention will be further described below in conjunction with the accompanying drawings and specific embodiments
如附图1,整个装置沿中心轴对称。环形分布的镀银聚光镜1中的每一环都为由一固定长度的线段绕轴旋转而形成无上下底面的圆台。且每条固定长度的线段的位置和倾角都不同。垂直入射的太阳光线通过环形分布的反光镜可以汇集在位于接收盘中央的高倍光伏电池5上。光伏电池5的背部装有专用散热器,以将光伏电池的热量带走。As shown in Figure 1, the entire device is symmetrical along the central axis. Each ring in the annularly distributed silver-coated
所述的环形线性菲涅尔高倍聚光器沿中心轴对称。The annular linear Fresnel high-power concentrator is symmetrical along the central axis.
所述的环形线性菲涅尔高倍聚光器中环形分布的反光镜采用全反射镀银表面,以保证较高的反射率。The annularly distributed reflector in the annular linear Fresnel high-power concentrator adopts a total reflection silver-plated surface to ensure high reflectivity.
整个组件需加装自动跟踪系统以保证电池板5所在的平面与太阳光入射方向保持垂直。The entire assembly needs to be equipped with an automatic tracking system to ensure that the plane where the solar panel 5 is located is vertical to the incident direction of sunlight.
所述的支撑结构需有效地支撑起镜面部分,并可以承受住一定程度的大风和沙尘天气影响。The supporting structure needs to effectively support the mirror surface portion, and can withstand the influence of strong wind and sand and dust weather to a certain extent.
所述的镜面较细较薄,需使用强度较高的玻璃。The mirror surface is thinner and thinner, and glass with higher strength needs to be used.
所述的镜面连接结构与镜面需直接连接,以保证结构强度。The mirror surface connection structure and the mirror surface need to be directly connected to ensure the structural strength.
所述的镜面各参数均由计算获得。All the parameters of the mirror surface are obtained by calculation.
图2和图3为边缘两块镜子的光路图,所述的各镜镜面位置及倾斜角度计算如下:Fig. 2 and Fig. 3 are the optical path diagrams of two mirrors on the edge, and the position of the mirror surface and the angle of inclination of each mirror are calculated as follows:
设最边缘的环形镜面为第n块环形镜面,向内依次为第n-1,n-2块,每块镜面横截面宽度为D。Let the most edge annular mirror surface be the nth annular mirror surface, and the inwards are the n-1th and n-2th pieces in turn, and the cross-sectional width of each mirror surface is D.
第n块镜面的上边缘坐标为中心坐标为(xn,yn),下边缘坐标为The coordinates of the upper edge of the nth mirror are The center coordinates are (x n , y n ), and the lower edge coordinates are
以第n块镜子中心点在对称轴上的水平投影为原点,沿水平和竖直方向建立平面直角坐标系;Taking the horizontal projection of the center point of the nth mirror on the symmetry axis as the origin, establish a plane rectangular coordinate system along the horizontal and vertical directions;
令第n块环形镜面中心距离聚光点的水平距离为Qn,垂直距离为Hn Let the horizontal distance from the center of the nth annular mirror to the condensing point be Q n , and the vertical distance be H n
令第n块环形镜面中心为(Qn,0),Let the center of the nth annular mirror be (Q n , 0),
则第n块镜子上边缘坐标为 Then the coordinates of the upper edge of the nth mirror are
第n块镜子下边缘横坐标为The abscissa of the lower edge of the nth mirror is
第n-1块镜子上边缘的横坐标与第n块镜子的下边缘横坐标相同,The abscissa of the upper edge of the n-1th mirror is the same as the abscissa of the lower edge of the nth mirror,
因此therefore
为for
第n-1块镜子中心横坐标为The abscissa of the center of the n-1th mirror is
下面求其纵坐标,Find its ordinate below,
对第n块镜子上边缘建立直线方程:Establish a straight line equation for the upper edge of the nth mirror:
可化简为:Can be simplified to:
因此therefore
则每块镜子的纵坐标可以用下式表示:Then the ordinate of each mirror can be expressed by the following formula:
由第n-1块镜子中心纵坐标:From the ordinate of the center of the n-1th mirror:
可得出:It can be concluded that:
由直线方程可得出:From the equation of the straight line, we can get:
可推得第n-1块镜子中心纵坐标:The ordinate of the center of the n-1th mirror can be derived:
由几何关系可得:From the geometric relationship, we can get:
βn-1-λn-1+βn-1=90°β n-1 -λ n-1 +β n-1 =90°
因此:therefore:
2βn-1=90°+λn-1 2β n-1 =90°+λ n-1
λn-1=2βn-1-90°λ n-1 =2β n-1 -90°
由三角关系:By the triangular relationship:
可得方程:Available equation:
由三角关系可得:From the trigonometric relationship we get:
Qn=-Htan2βn Q n = -Htan2β n
带入得相连两镜子位置的迭代方程:Bring in the iterative equation for the positions of two connected mirrors:
因此由最边缘镜子的距离聚光点高度、镜子横截面宽度和倾斜角度可得到其余每块镜子的这三个参数。Therefore, these three parameters of each of the remaining mirrors can be obtained from the height from the condensing point of the most edge mirror, the width of the mirror cross-section and the inclination angle.
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