Abstract In this work, a detailed mathematical procedure to estimate collectible radiation on the base of a V-trough concentrator, to which solar cells are attached, was developed based on the imaging principle of planar mirrors, solar geometry and monthly horizontal radiation. This model allows predicting the optical performance of V-troughs with any structural and installation parameters, and optimizing the design of such concentrator. Calculation results showed that for fixed east–west aligned V-troughs (EW-V troughs, in short) with given geometric concentration factor ( C g ) and side wall reflectivity ( ρ ), the annual solar gain depended on its opening angle, tilt-angle of the aperture and climatic conditions in sites, and a set of optimal opening angle and aperture tilt-angle for maximizing annual solar gain could be obtained by iterative calculations for different opening angles and tilt-angles. It was also found that for fixed EW-V troughs with C g = 2 and ρ = 0.9, taking the site latitude as quasi optimal tilt-angle was reasonable over all area of China, 15° deviation of azimuth angle from the due south would resulted in reduction of the annual collectible radiation less than 1%, and 10° deviation of the geometric axial line from the crossing line between the horizon and the extended aperture of V-troughs resulted in the reduction of annual solar gain less than 1%. For EW-V troughs with the tilt-angle of the aperture being yearly adjusted four times at three fixed tilt-angle (3T-EW-V troughs), the annual solar gain captured by 3T-EW-V troughs with given C g and ρ in a specific site was approximately a function of the opening angle, and the optimal opening angle for maximizing annual solar gain could be simply estimated by iterative calculations for different opening angles. Compared with fixed EW-V troughs, the annual solar gain on the base of 3T-EW-V troughs increased significantly, especially for those with a large C g , and the monthly average daily solar gain was more stable over a year. This implied that several tilt-angle adjustments in a year were required to make EW-V troughs with C g > 2 efficiently concentrate radiation onto their coupling solar cells in all days of a year.
[1]
Björn Karlsson,et al.
Design of concentrating elements with CIS thin-film solar cells for facade integration
,
2003
.
[2]
Ari Rabl,et al.
Active solar collectors and their applications
,
1985
.
[3]
A. Rabl,et al.
The average distribution of solar radiation-correlations between diffuse and hemispherical and between daily and hourly insolation values
,
1979
.
[4]
Brian Norton,et al.
Power losses in an asymmetric compound parabolic photovoltaic concentrator
,
2007
.
[5]
K.G.T. Hollands,et al.
A concentrator for thin-film solar cells
,
1971
.
[6]
Chetan Singh Solanki,et al.
Experimental evaluation of V-trough (2 suns) PV concentrator system using commercial PV modules
,
2007
.
[7]
R. Tang,et al.
Feasibility and optical performance of one axis three positions sun-tracking polar-axis aligned CPCs for photovoltaic applications
,
2010
.
[8]
W. Belcher,et al.
Effect of film thickness and morphology on the performance of photoelectrochemical cells based on poly(terthiophene)
,
2007
.
[9]
Tapas K. Mallick,et al.
Non-concentrating and asymmetric compound parabolic concentrating building façade integrated photovoltaics: An experimental comparison
,
2006
.
[10]
Tapas K. Mallick,et al.
The design and experimental characterisation of an asymmetric compound parabolic photovoltaic concentrator for building façade integration in the UK
,
2004
.
[11]
Naum Fraidenraich,et al.
OPTICAL PROPERTIES OF V-TROUGH CONCENTRATORS
,
1991
.
[12]
Chetan Singh Solanki,et al.
Enhanced heat dissipation of V-trough PV modules for better performance
,
2008
.
[13]
Ming Li,et al.
Optical performance of fixed east–west aligned CPCs used in China
,
2010
.