Optimize the shape of curved-Fresnel lens to maximize its transmittance

Abstract This study is to determine the range of incidence angles for a required transmittance of elementary prisms in a curved Fresnel lens and hence to determine the curvature of the lens. The p-polarized light and s-polarized light is considered separately. Calculations indicated that the transmittance of s-polarized light is always lower than p-polarized light and the total transmittance generally decreases with the increase of incidence angle monotonously according to the Fresnel equations, and therefore the transmittance of s-polarized light was recommended as the target for a lens’ design. Stokes’ reversible relation was derived by Fresnel formulas, which illustrates the reflectivity on both sides of the interface is equivalent when light goes through two media along with a certain path no matter which direction it is transmitted. It is found there is the optimal transmittance condition of prism (OTCP) when the incidence angle changes for a given refractive index bases on Stokes’ reversible relation. According to OTCP, the transmittance of a curved Fresnel lens can be calculated for a given curvature and focus and therefore the shape of lens can be optimized. The incidence angles for the required transmittance values of 0.95, 0.90, 0.85, 0.80 and 0.75, respectively, are given for different refractive indices. For example, for the refractive index n21 = 1.49 (a value for the common PMMA), the range of incidence angle of s-polarized light is 0–22° if the required transmittance is 0.90; it becomes 0–48° when the required transmittance is reduced to 0.80.

[1]  Peter Kane,et al.  Modeling of solar tracking for giant Fresnel lens solar stoves , 2013 .

[2]  Takayuki Funatsu,et al.  High-efficiency and economical solar-energy-pumped laser with Fresnel lens and chromium codoped laser medium , 2007 .

[3]  Yuehong Su,et al.  Design and experimental analysis of a cylindrical compound Fresnel solar concentrator , 2014 .

[4]  O. E. Miller,et al.  Thin Sheet Plastic Fresnel Lenses of High Aperture , 1951 .

[5]  E. Kritchman,et al.  Color-corrected Fresnel lens for solar concentration. , 1980, Optics letters.

[6]  Takao Kashiwagi,et al.  DESIGN OF A NONIMAGING FRESNEL LENS FOR SOLAR CONCENTRATORS 1 1 Paper presented at the ISES Solar Wo , 1999 .

[7]  A A Friesem,et al.  Highly concentrating Fresnel lenses. , 1979, Applied optics.

[8]  M. Steiner,et al.  Estimation of the influence of Fresnel lens temperature on energy generation of a concentrator photovoltaic system , 2012 .

[9]  Ruzhu Wang,et al.  Concentrated solar energy applications using Fresnel lenses: A review , 2011 .

[10]  Khalil E.J. Al-Jumaily,et al.  The study of the performance and efficiency of flat linear Fresnel lens collector with sun tracking system in Iraq , 1998 .

[11]  Aris Tsangrassoulis,et al.  On the energy efficiency of a prototype hybrid daylighting system , 2005 .

[12]  David C. Miller,et al.  Durability of Fresnel lenses: A review specific to the concentrating photovoltaic application , 2011 .

[13]  Hofler,et al.  Design and construction of a solar-powered, thermoacoustically driven, thermoacoustic refrigerator , 2000, The Journal of the Acoustical Society of America.

[14]  D. L. Evans,et al.  Linear Fresnel lens concentrators , 1975 .

[15]  Naichia Yeh,et al.  Optical geometry approach for elliptical Fresnel lens design and chromatic aberration , 2009 .