This work consisted of the mathematical modeling of a parabolic trough concentrator. To this end, a heat balance has been established for the different parts of the parabolic trough concentrator, which are the heat transfer fluid, the absorber and the glass. This allowed us to establish a system of equation whose resolution was done by the finite difference method. This digital resolution made it possible to obtain the temperatures of the different parts of our parabolic trough concentrator, namely, the heat transfer fluid, the absorber and the glass. The simulation of the heating process of the fluid is done in time steps of one hour, from six hours to eighteen hours. The results obtained show that the temperature difference between the inlet and the outlet of the solar collector is very large. A computer program has been developed to simulate the temperatures of the heat transfer fluid, the absorber tube and the glass as a function of time and space. These results were obtained for a typical day with regard to the variation of the temperatures of the heat transfer fluid, the absorber and the glass, as well as the powers and efficiency of the parabolic trough concentrator and various factors for the sake of improve the performance of our prototype.
Published in | Engineering Physics (Volume 5, Issue 2) |
DOI | 10.11648/j.ep.20210502.14 |
Page(s) | 54-62 |
Creative Commons |
This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
Copyright |
Copyright © The Author(s), 2021. Published by Science Publishing Group |
Modeling, Simulation, Parabolic Trough Concentrator, Heat Transfer Fluid, Temperature
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[9] | Mullick, S. C. and Nanda, S. 1989. An improved technique for computing the heat loss factor of tubular absorber, Solar Energy Vol. 42, N°1, pp 1-7. |
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APA Style
Kpeusseu Angeline Kouambla Epse Yeo, Bati Ernest Boya Bi, Prosper Gbaha. (2021). Modeling and Simulation of a Parabolic Trough Solar Concentrator. Engineering Physics, 5(2), 54-62. https://doi.org/10.11648/j.ep.20210502.14
ACS Style
Kpeusseu Angeline Kouambla Epse Yeo; Bati Ernest Boya Bi; Prosper Gbaha. Modeling and Simulation of a Parabolic Trough Solar Concentrator. Eng. Phys. 2021, 5(2), 54-62. doi: 10.11648/j.ep.20210502.14
AMA Style
Kpeusseu Angeline Kouambla Epse Yeo, Bati Ernest Boya Bi, Prosper Gbaha. Modeling and Simulation of a Parabolic Trough Solar Concentrator. Eng Phys. 2021;5(2):54-62. doi: 10.11648/j.ep.20210502.14
@article{10.11648/j.ep.20210502.14, author = {Kpeusseu Angeline Kouambla Epse Yeo and Bati Ernest Boya Bi and Prosper Gbaha}, title = {Modeling and Simulation of a Parabolic Trough Solar Concentrator}, journal = {Engineering Physics}, volume = {5}, number = {2}, pages = {54-62}, doi = {10.11648/j.ep.20210502.14}, url = {https://doi.org/10.11648/j.ep.20210502.14}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ep.20210502.14}, abstract = {This work consisted of the mathematical modeling of a parabolic trough concentrator. To this end, a heat balance has been established for the different parts of the parabolic trough concentrator, which are the heat transfer fluid, the absorber and the glass. This allowed us to establish a system of equation whose resolution was done by the finite difference method. This digital resolution made it possible to obtain the temperatures of the different parts of our parabolic trough concentrator, namely, the heat transfer fluid, the absorber and the glass. The simulation of the heating process of the fluid is done in time steps of one hour, from six hours to eighteen hours. The results obtained show that the temperature difference between the inlet and the outlet of the solar collector is very large. A computer program has been developed to simulate the temperatures of the heat transfer fluid, the absorber tube and the glass as a function of time and space. These results were obtained for a typical day with regard to the variation of the temperatures of the heat transfer fluid, the absorber and the glass, as well as the powers and efficiency of the parabolic trough concentrator and various factors for the sake of improve the performance of our prototype.}, year = {2021} }
TY - JOUR T1 - Modeling and Simulation of a Parabolic Trough Solar Concentrator AU - Kpeusseu Angeline Kouambla Epse Yeo AU - Bati Ernest Boya Bi AU - Prosper Gbaha Y1 - 2021/12/24 PY - 2021 N1 - https://doi.org/10.11648/j.ep.20210502.14 DO - 10.11648/j.ep.20210502.14 T2 - Engineering Physics JF - Engineering Physics JO - Engineering Physics SP - 54 EP - 62 PB - Science Publishing Group SN - 2640-1029 UR - https://doi.org/10.11648/j.ep.20210502.14 AB - This work consisted of the mathematical modeling of a parabolic trough concentrator. To this end, a heat balance has been established for the different parts of the parabolic trough concentrator, which are the heat transfer fluid, the absorber and the glass. This allowed us to establish a system of equation whose resolution was done by the finite difference method. This digital resolution made it possible to obtain the temperatures of the different parts of our parabolic trough concentrator, namely, the heat transfer fluid, the absorber and the glass. The simulation of the heating process of the fluid is done in time steps of one hour, from six hours to eighteen hours. The results obtained show that the temperature difference between the inlet and the outlet of the solar collector is very large. A computer program has been developed to simulate the temperatures of the heat transfer fluid, the absorber tube and the glass as a function of time and space. These results were obtained for a typical day with regard to the variation of the temperatures of the heat transfer fluid, the absorber and the glass, as well as the powers and efficiency of the parabolic trough concentrator and various factors for the sake of improve the performance of our prototype. VL - 5 IS - 2 ER -