2016
DOI: 10.1016/j.solener.2016.06.046
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Angular distribution of annual collectible radiation on solar cells of CPC based photovoltaic systems

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Cited by 9 publications
(17 citation statements)
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“…In this work, CPV-θ a /θ e with θ a < 2θ e − 0.5π is investigated, and for such CPVs, radiation irradiating on plane mirrors will arrive on solar cells after one reflection as indicated by Yu et al [27]. The imaging principle of plane mirrors indicates that solar rays pointing to solar cells' image formed by a plane mirror will hit on solar cells after reflection, therefore, for θ p ≤ θ a , all radiation irradiating on the entire right mirror (BD) will strike on the solar cells after reflection (see Figure 4a); for θ a < θ p ≤ θ t , the radiation irradiating on lower part of mirror (MB) (see Figure 4b), will redirect onto the solar cells, and for θ t < θ p < θ p,c1 , the plane mirror is partially irradiated, thus only radiation irradiating on the middle part of the mirror will redirect onto the solar cells (see Figure 4c), whereas for θ p > θ p,c1 , no radiation arrives on solar cells from the plane mirror (see Figure 4d).…”
Section: Calculation Of F 2 and ηmentioning
confidence: 99%
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“…In this work, CPV-θ a /θ e with θ a < 2θ e − 0.5π is investigated, and for such CPVs, radiation irradiating on plane mirrors will arrive on solar cells after one reflection as indicated by Yu et al [27]. The imaging principle of plane mirrors indicates that solar rays pointing to solar cells' image formed by a plane mirror will hit on solar cells after reflection, therefore, for θ p ≤ θ a , all radiation irradiating on the entire right mirror (BD) will strike on the solar cells after reflection (see Figure 4a); for θ a < θ p ≤ θ t , the radiation irradiating on lower part of mirror (MB) (see Figure 4b), will redirect onto the solar cells, and for θ t < θ p < θ p,c1 , the plane mirror is partially irradiated, thus only radiation irradiating on the middle part of the mirror will redirect onto the solar cells (see Figure 4c), whereas for θ p > θ p,c1 , no radiation arrives on solar cells from the plane mirror (see Figure 4d).…”
Section: Calculation Of F 2 and ηmentioning
confidence: 99%
“…The earlier work by Rabl and Winston indicated that the use of CPCs with a restricted exit angle (CPC-θ a /θ e ) can improve the photovoltaic performance of CPVs thanks to the limited solar incident/exit angle [26]. For CPC-θ a /θ e , the solar incidence angle on the absorber is limited within θ e for the radiation within its acceptance angle (θ a ), and common CPC, the one without restriction of exit angle, is a special case of CPC-θ a /θ e for θ e = 90 • [27]. An comparative study conducted by Yu et al showed that, in comparison with CPV-20/90, power output increases of 2.1%, 5.4% and 8.17% from CPV-20/65 were measured for projected incident angle θ p = 0 • , 10 • and 16 • , respectively.…”
Section: Introductionmentioning
confidence: 99%
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“…As literature [20] proved, Beta distribution function is used to describe solar radiation intensity as…”
Section: Pv Output Power Modelmentioning
confidence: 99%