Monte Carlo Ray-Tracing Simulation of a Cassegrain Solar Concentrator Module for CPV

The concentration ratio is one of the most important characteristics in designing a Cassegrain solar concentrator since it directly affects the performance of high-density solar energy applications such as concentrated photovoltaics (CPVs). In this study, solar concentrator modules that have differe...

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Main Authors: Seung Jin Oh, Hyungchan Kim, Youngsun Hong
Format: Article
Language:English
Published: Frontiers Media S.A. 2021-10-01
Series:Frontiers in Energy Research
Subjects:
Online Access:https://www.frontiersin.org/articles/10.3389/fenrg.2021.722842/full
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author Seung Jin Oh
Hyungchan Kim
Youngsun Hong
author_facet Seung Jin Oh
Hyungchan Kim
Youngsun Hong
author_sort Seung Jin Oh
collection DOAJ
description The concentration ratio is one of the most important characteristics in designing a Cassegrain solar concentrator since it directly affects the performance of high-density solar energy applications such as concentrated photovoltaics (CPVs). In this study, solar concentrator modules that have different configurations were proposed and their performances were compared by means of a Monte Carlo ray-tracing algorithm to identify the optimal configurations. The first solar concentrator design includes a primary parabolic concentrator, a parabolic secondary reflector, and a homogenizer. The second design, on the other hand, includes a parabolic primary concentrator, a secondary hyperbolic concentrator, and a homogenizer. Two different reflectance were applied to find the ideal concentration ratio and the actual concentration ratio. In addition, uniform rays and solar rays also were compared to estimate their efficiency. Results revealed that both modules show identical concentration ratios of 610 when the tracking error is not considered. However, the concentration ratio of the first design rapidly drops when the sun tracking error overshoots even 0.1°, whereas the concentration ratio of the second design remained constant within the range of the 0.8° tracking error. It was concluded that a paraboloidal reflector is not appropriate for the second mirror in a Cassegrain concentrator due to its low acceptance angle. The maximum collection efficiency was achieved when the f-number is smaller and the rim angle is bigger and when the secondary reflector is in a hyperboloid shape. The target area has to be rather bigger with a shorter focal length for the secondary reflector to obtain a wider acceptance angle.
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spelling doaj.art-7b4d5568a8bc4006a4ef1dc1f2520c2c2022-12-21T22:38:46ZengFrontiers Media S.A.Frontiers in Energy Research2296-598X2021-10-01910.3389/fenrg.2021.722842722842Monte Carlo Ray-Tracing Simulation of a Cassegrain Solar Concentrator Module for CPVSeung Jin OhHyungchan KimYoungsun HongThe concentration ratio is one of the most important characteristics in designing a Cassegrain solar concentrator since it directly affects the performance of high-density solar energy applications such as concentrated photovoltaics (CPVs). In this study, solar concentrator modules that have different configurations were proposed and their performances were compared by means of a Monte Carlo ray-tracing algorithm to identify the optimal configurations. The first solar concentrator design includes a primary parabolic concentrator, a parabolic secondary reflector, and a homogenizer. The second design, on the other hand, includes a parabolic primary concentrator, a secondary hyperbolic concentrator, and a homogenizer. Two different reflectance were applied to find the ideal concentration ratio and the actual concentration ratio. In addition, uniform rays and solar rays also were compared to estimate their efficiency. Results revealed that both modules show identical concentration ratios of 610 when the tracking error is not considered. However, the concentration ratio of the first design rapidly drops when the sun tracking error overshoots even 0.1°, whereas the concentration ratio of the second design remained constant within the range of the 0.8° tracking error. It was concluded that a paraboloidal reflector is not appropriate for the second mirror in a Cassegrain concentrator due to its low acceptance angle. The maximum collection efficiency was achieved when the f-number is smaller and the rim angle is bigger and when the secondary reflector is in a hyperboloid shape. The target area has to be rather bigger with a shorter focal length for the secondary reflector to obtain a wider acceptance angle.https://www.frontiersin.org/articles/10.3389/fenrg.2021.722842/fullCassegrain solar concentratorhigh concentrated photovoltaicsMonte Carlo ray-tracingconcentration ratiofocal point
spellingShingle Seung Jin Oh
Hyungchan Kim
Youngsun Hong
Monte Carlo Ray-Tracing Simulation of a Cassegrain Solar Concentrator Module for CPV
Frontiers in Energy Research
Cassegrain solar concentrator
high concentrated photovoltaics
Monte Carlo ray-tracing
concentration ratio
focal point
title Monte Carlo Ray-Tracing Simulation of a Cassegrain Solar Concentrator Module for CPV
title_full Monte Carlo Ray-Tracing Simulation of a Cassegrain Solar Concentrator Module for CPV
title_fullStr Monte Carlo Ray-Tracing Simulation of a Cassegrain Solar Concentrator Module for CPV
title_full_unstemmed Monte Carlo Ray-Tracing Simulation of a Cassegrain Solar Concentrator Module for CPV
title_short Monte Carlo Ray-Tracing Simulation of a Cassegrain Solar Concentrator Module for CPV
title_sort monte carlo ray tracing simulation of a cassegrain solar concentrator module for cpv
topic Cassegrain solar concentrator
high concentrated photovoltaics
Monte Carlo ray-tracing
concentration ratio
focal point
url https://www.frontiersin.org/articles/10.3389/fenrg.2021.722842/full
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