Estudio de diferentes metodologías de seguimiento solar no estándar
El presente trabajo, se estudia el desempeño de un seguidor solar por cálculos astronómicos, realizando ensayos de diferentes técnicas de seguimiento tales como: seguimiento con un eje paralelo a la dirección Norte–Sur y panel solar inclinado respecto al eje de seguimiento, seguimiento con un eje Po...
- Autores:
-
Vargas Oviedo, Ana Elena
- Tipo de recurso:
- Trabajo de grado de pregrado
- Fecha de publicación:
- 2024
- Institución:
- Universidad de Córdoba
- Repositorio:
- Repositorio Institucional Unicórdoba
- Idioma:
- spa
- OAI Identifier:
- oai:repositorio.unicordoba.edu.co:ucordoba/8992
- Acceso en línea:
- https://repositorio.unicordoba.edu.co/handle/ucordoba/8992
https://repositorio.unicordoba.edu.co
- Palabra clave:
- Sistemas fotovoltaicos
Técnicas de seguimiento solar
Radiación solar
Photovoltaic systems
Solar tracking techniques
Solar radiation
- Rights
- openAccess
- License
- https://creativecommons.org/licenses/by-nc-nd/4.0/
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Estudio de diferentes metodologías de seguimiento solar no estándar |
| title |
Estudio de diferentes metodologías de seguimiento solar no estándar |
| spellingShingle |
Estudio de diferentes metodologías de seguimiento solar no estándar Sistemas fotovoltaicos Técnicas de seguimiento solar Radiación solar Photovoltaic systems Solar tracking techniques Solar radiation |
| title_short |
Estudio de diferentes metodologías de seguimiento solar no estándar |
| title_full |
Estudio de diferentes metodologías de seguimiento solar no estándar |
| title_fullStr |
Estudio de diferentes metodologías de seguimiento solar no estándar |
| title_full_unstemmed |
Estudio de diferentes metodologías de seguimiento solar no estándar |
| title_sort |
Estudio de diferentes metodologías de seguimiento solar no estándar |
| dc.creator.fl_str_mv |
Vargas Oviedo, Ana Elena |
| dc.contributor.advisor.none.fl_str_mv |
Oviedo Cueter, Juan Manuel |
| dc.contributor.author.none.fl_str_mv |
Vargas Oviedo, Ana Elena |
| dc.subject.proposal.none.fl_str_mv |
Sistemas fotovoltaicos Técnicas de seguimiento solar Radiación solar |
| topic |
Sistemas fotovoltaicos Técnicas de seguimiento solar Radiación solar Photovoltaic systems Solar tracking techniques Solar radiation |
| dc.subject.keywords.none.fl_str_mv |
Photovoltaic systems Solar tracking techniques Solar radiation |
| description |
El presente trabajo, se estudia el desempeño de un seguidor solar por cálculos astronómicos, realizando ensayos de diferentes técnicas de seguimiento tales como: seguimiento con un eje paralelo a la dirección Norte–Sur y panel solar inclinado respecto al eje de seguimiento, seguimiento con un eje Polar (un eje inclinado con ángulo igual a la latitud del lugar) y seguimiento solar en el cual se combina un eje de seguimiento paralelo a la dirección Norte-Sur (con panel inclinado) y uno Acimutal. Este análisis es llevado a cabo bajo un modelo computacional implementado en Matlab, comparando la energía anual generada por un panel solar bajo las técnicas de seguimiento mencionadas, con la generada por un panel solar con las mismas características y considerando técnicas de seguimiento estándar tales como: Acimutal y Altacimutal, lo cual es realizado considerando la componente directa de la irradiancia solar incidente. |
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2024 |
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2024-11-11 |
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2025-02-03T17:12:18Z |
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2025-02-03T17:12:18Z |
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T. E. S. Agency. Gaia reveals the past and future of the sun Ashish Dhawan, Malik O.P. y Ravinder Kumar. Solar tracker implementation using matlab/simulink. Journal of Emerging Technologies and Innovative Research (JETIR), 2018 M. I. (Auth.). An Introduction to Solar Radiation. Academic Press, 1983 B. Blanc, P.; Espinar. Direct normal irradiance related definitions and applications: The circumsolar issue. Solar Energy, 110:561--577, 2014 Britannica. Solar panel, 2024. Catalin Alexandru. Simulation and optimization of a dual-axis solar tracking mechanism. Mathematics, 2024 P. Cooper. The absorption of radiation in solar stills. Solar Energy, 12:333--346, 1969 I. I. ELÉCTRICA. ¿de qué están hechos los paneles solares? Farhan A. Salem. Ahmad A. Mahfouz. Modeling and simulation issues on standalone two axis sun tracker. Saudi Journal Of Engineering and Technology, 2016 P. Gilman. Sam photovoltaic model technical reference. p. gilman. National Renewable Energy Laboratory. NREL. U.S. Department of Energy. Office of Energy Efficiency Renewable Energy. Operated by the Alliance for Sustainable Energy, LLC. Laboratory (NREL), 2004 González Acevedo, H. Muñoz Maldonado Y. Ospino Castro, A. Serrano, J. Atencio, A. Jaimes Saavedra C. Design and performance evaluation of a solar tracking panel ofsingle axis in colombia. International Journal of Electrical and Computer Engineering (IJECE), 2021 R. Grena. Five new algorithms for the computation of sun position from 2010 to 2110. Solar Energy, 86(5):1323--1337, 2012 R. Hassanian, M. Riedel, N. Yeganeh, and R. Unnthorsson. A practical approach for estimating the optimum tilt angle of a photovoltaic panel for a long period—experimental recorded data. Solar, 1(1):41--51, 2021 IDEAM. La radiación solar y su paso por la atmósfera IDEAM. Atlas de la radiación solar, 2015 W. A. B. John A. Duffie. Solar Engineering of Thermal Processes. Wiley, 2nd ed edition, 1991 F. Kasten. A simple parameterization of the pyrheliometric formula for determining the linke turbidity factor. Meteorologische Rundschau, 1980 F. Kininger. Photovoltaic Systems Technology. Universität Kassel – Rationelle Energiewandlung, Kassel, Alemania, 1 edition, 2003 K. Y. Kondratyev and G. E. H. (Auth.). Weather and Climate on Planets. Pergamon Press, 1st edi tion, 1982 A. K. A. Kotti, M.C.; Argiriou. Estimation of direct normal irradiance from measured global and corrected diffuse horizontal irradiance. Energy, 70:382--392, 2014 J. A. Kratochvil, W. E. Boyson, and D. L. King. Photovoltaic array performance model. In Photo voltaic array performance model., 2004 F. Linke. Transmissions-koeffizient und trubungsfaktor. Beitr. Phys. fr. Atmos, 10:91--103, 1922 B. Liu and R. Jordan. A rational procedure for predicting the long-term average performance of flat-plate solar-energy collectors. Solar Energy, 7(2):53--74, 1963 Marcu, A. Alexandu, C. Barbu, I. Modeling and simulation of dual - axis solar tracker for pv modules. IOP Conference Series Materials Science and Engineering, 2019 J. S. S. Matthew J. Reno, Clifford W. Hansen. Global horizontal irradiance clear sky models implementation and analysis. Sandia National Laboratories, 2012 J. J. Michalsky. The astronomical almanac’s algorithm for approximate solar position (1950–2050). Solar Energy, 40:227--235, 1988 Mitton S, editor. The Cambridge Enclyclopedia of Astronomy. Crown Publishers, 1977 Y. Nassar and S. Alsadi. View factors of flat solar collectors array in flat, inclined, and step-like solar fields. Journal of Solar Energy Engineering, 138, 08 2016 Negron Llacuachaqui, F. H. y Salcedo Rosas, J. M. Comparación de la eficiencia de sistemas fotovoltaicos mediante seguimiento solar. Universidad Nacional Del Centro Del Perú, 2017 p. Gilman. Sam photovoltaic model technical reference. National Renewable Energy Laboratory (NREL), 2015 P. I. R. Perez. A new airmass independent formulation for the linke turbidity coefficient. Solar Energy, 73:151--157, 2002 R. Perez, P. Ineichen, R. Seals, J. Michalsky, and R. Stewart. Modeling daylight availability and irradiance components from direct and global irradiance. Solar Energy, 44(5):271--289, 1990 R. Perez, R. Stewart, R. Seals, and T. Guertin. The development and verification of the perez diffuse radiation model. Technical Report SAN88-7030, Sandia National Laboratories, Albuquerque, NM, 1988 O. Perpiñán. Energía Solar Fotovoltaica, 2023 C. L. Pitman and L. L. Vant-Hull. Errors in locating the sun and their effect on solar intensity predictions. American Section of the International Solar Energy Society, pages 701--706, 1978 I. Reda and A. Andreas. Solar position algorithm for solar radiation applications. Technical Report TP-560-34302, National Renewable Energy Laboratory, 2003 I. Reda and A. Andreass. Solar position algorithm for solar radiation application. Technical report, National Renewable Energy Laboratory, 2008 D. Reindl. Estimating diffuse radiation on horizontal surfaces and total radiation on tilted surfaces. Master’s thesis, University of Wisconsin Madison, Solar Energy Laboratory, 1988 M. J. Reno, C. W. Hansen, and J. S. Stein. Global horizontal irradiance clear sky models: Implementation and analysis. Technical Report SAND2012-2389, Sandia National Laboratories, March 2012 A. Sinton, Ronald A.; Cuevas. Contactless determination of current–voltage characteristics and minority-carrier lifetimes in semiconductors from quasi-steady-state photoconductance data. Applied Physics Letters, 69:2510, 1996 Spencer, J.W. Fourier series representation of the position of the sun. Search, 2(5):172+, may 1971 A. B. Sproul. Derivation of the solar geometric relationships using vector analysis. Renewable Energy, 32:1187--1205, 2007 Strous, L. Position of the sun, 2011 J. C. Subtil Lacerda, Juliana; van den Bergh. Diversity in solar photovoltaic energy: Implications for innovation and policy. Renewable and Sustainable Energy Reviews, 54:331--340, 2016 Vijay, M. Deepu and Shah, Kamlesh and Bhuvaneswari, G. and Singh, Bhim. Led based street lighting with automatic intensity control using solar pv. IEEE IAS Joint Industrial and Commercial Power Systems / Petroleum and Chemical Industry Conference (ICPSPCIC), 2015 R. Walraven. Calculating the position of the sun. Solar Energy, 20(5):393--397, 1978 Yusuf S.J. y Romanus I.O. Construction and simulation of dual axes automatic solar tracking system. International Journal of Pure and Applied Science. Published by Cambridge Research and Publications, 2019 Zyrianov, Fedor. Diseño e implementación del sistema de control de un seguidor solar. 2017 |
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Oviedo Cueter, Juan Manuele02d4ae1-3ef7-415a-b62e-266d5a5c2a38600Vargas Oviedo, Ana Elena0b2c5546-56c4-4602-b96c-ca5d7ba6abab-12025-02-03T17:12:18Z2025-02-03T17:12:18Z2024-11-11https://repositorio.unicordoba.edu.co/handle/ucordoba/8992Universidad de CórdobaRepositorio Institucional Unicórdobahttps://repositorio.unicordoba.edu.coEl presente trabajo, se estudia el desempeño de un seguidor solar por cálculos astronómicos, realizando ensayos de diferentes técnicas de seguimiento tales como: seguimiento con un eje paralelo a la dirección Norte–Sur y panel solar inclinado respecto al eje de seguimiento, seguimiento con un eje Polar (un eje inclinado con ángulo igual a la latitud del lugar) y seguimiento solar en el cual se combina un eje de seguimiento paralelo a la dirección Norte-Sur (con panel inclinado) y uno Acimutal. Este análisis es llevado a cabo bajo un modelo computacional implementado en Matlab, comparando la energía anual generada por un panel solar bajo las técnicas de seguimiento mencionadas, con la generada por un panel solar con las mismas características y considerando técnicas de seguimiento estándar tales como: Acimutal y Altacimutal, lo cual es realizado considerando la componente directa de la irradiancia solar incidente.In this work, the performance of a solar tracker is studied by astronomical calculations, performing tests of different tracking techniques such as: tracking with an axis parallel to the North-South direction and solar panel inclined with respect to the tracking axis, tracking with a Polar axis (an axis inclined with an angle equal to the latitude of the place) and solar tracking in which a tracking axis parallel to the North-South direction (with an inclined panel) and an Azimuthal one are combined. This analysis is carried out under a computational model implemented in Matlab, comparing the annual energy generated by a solar panel under the mentioned tracking techniques, with that generated by a solar panel with the same characteristics and considering standard tracking techniques such as: Azimuthal and Altazimuthal, which is carried out considering the direct component of the incident solar irradiance.DedicatoriaResumenIntroducciónObjetivosLista de figurasLista de tablasMarco teóricoGeometría solarPosición del Sol en un sistema de referencia localHora oficial y hora solar verdaderaMedida del tiempoTiempo solar verdadero (TSV)Tiempo solar medio (TSM)Determinación de la posición aparente del SolRadiación solarInteracción de la radiación solar y la atmósfera terrestreIrradiancia Global HorizontalComponente de la Irradiancia Directa en plano horizontalIrradiancia Difusa HorizontalIrradiancia sobre un plano generador con inclinación y orientación arbitrariaIrradiancia de un haz incidente en plano inclinadoIrradiancia difusa que incide sobre una superficie inclinadaModelo isotrópicoModelo anisotrópicoModelo de PerezIrradiancia incidente en plano inclinado reflejada por el sueloCelda solar fotovoltaicaUnión p-nParámetros que caracterizan la celda solarCorriente de cortocircuito (Isc)Voltaje de circuito abierto (Voc)Potencia máxima de la celdaFactor de llenado (FF)Eficiencia de conversión (η)Funcionamiento de la celda solarPanel solarEnergía generada por un panel solarSistemas FotovoltaicosSistemas Fotovoltaicos AutónomosSistemas Fotovoltaicos de Conexión a RedTécnicas de seguimiento solarSistemas de seguimiento de doble ejeSistemas de seguimiento de un único ejeMetodologíaDeterminación de la posición del SolEstimación de las componentes directa de la irradiancia solar global sobre una superficie horizontalEstimación de la componente directa de la irradiancia solar global sobre una superficie inclinadaEstimación de la componente directa de la irradiancia solar sobre un sistema fotovoltaico bajo las diferentes técnicas de seguimiento solarResultados y AnálisisMapas de contorno de irradiancia solar sobre un panel para las técnicas de seguimiento solar seleccionadasIrradiación sobre un plano generador y densidad de energía generada por este para los sistemas de seguimiento estudiadosTécnicas de seguimiento de referencia: Acimutal y AltacimutalComparación de los valores de irradiaciòn anual y densidad de energía anual producida bajo las técnicas de seguimiento estudiadas respecto a las técnicas de referenciaConclusionesApéndice AReferenciasPregradoFísico(a)Trabajos de Investigación y/o Extensiónapplication/pdfspaUniversidad de CórdobaFacultad de Ciencias BásicasMontería, Córdoba, ColombiaFísicahttps://creativecommons.org/licenses/by-nc-nd/4.0/Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0)info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2Estudio de diferentes metodologías de seguimiento solar no estándarTrabajo de grado - Pregradoinfo:eu-repo/semantics/bachelorThesishttp://purl.org/coar/resource_type/c_7a1finfo:eu-repo/semantics/acceptedVersionTextT. E. S. Agency. Gaia reveals the past and future of the sunAshish Dhawan, Malik O.P. y Ravinder Kumar. Solar tracker implementation using matlab/simulink. Journal of Emerging Technologies and Innovative Research (JETIR), 2018M. I. (Auth.). An Introduction to Solar Radiation. Academic Press, 1983B. Blanc, P.; Espinar. Direct normal irradiance related definitions and applications: The circumsolar issue. Solar Energy, 110:561--577, 2014Britannica. Solar panel, 2024.Catalin Alexandru. Simulation and optimization of a dual-axis solar tracking mechanism. Mathematics, 2024P. Cooper. The absorption of radiation in solar stills. Solar Energy, 12:333--346, 1969I. I. ELÉCTRICA. ¿de qué están hechos los paneles solares?Farhan A. Salem. Ahmad A. Mahfouz. Modeling and simulation issues on standalone two axis sun tracker. Saudi Journal Of Engineering and Technology, 2016P. Gilman. Sam photovoltaic model technical reference. p. gilman. National Renewable Energy Laboratory. NREL. U.S. Department of Energy. Office of Energy Efficiency Renewable Energy. Operated by the Alliance for Sustainable Energy, LLC. Laboratory (NREL), 2004González Acevedo, H. Muñoz Maldonado Y. Ospino Castro, A. Serrano, J. Atencio, A. Jaimes Saavedra C. Design and performance evaluation of a solar tracking panel ofsingle axis in colombia. International Journal of Electrical and Computer Engineering (IJECE), 2021R. Grena. Five new algorithms for the computation of sun position from 2010 to 2110. Solar Energy, 86(5):1323--1337, 2012R. Hassanian, M. Riedel, N. Yeganeh, and R. Unnthorsson. A practical approach for estimating the optimum tilt angle of a photovoltaic panel for a long period—experimental recorded data. Solar, 1(1):41--51, 2021IDEAM. La radiación solar y su paso por la atmósferaIDEAM. Atlas de la radiación solar, 2015W. A. B. John A. Duffie. Solar Engineering of Thermal Processes. Wiley, 2nd ed edition, 1991F. Kasten. A simple parameterization of the pyrheliometric formula for determining the linke turbidity factor. Meteorologische Rundschau, 1980F. Kininger. Photovoltaic Systems Technology. Universität Kassel – Rationelle Energiewandlung, Kassel, Alemania, 1 edition, 2003K. Y. Kondratyev and G. E. H. (Auth.). Weather and Climate on Planets. Pergamon Press, 1st edi tion, 1982A. K. A. Kotti, M.C.; Argiriou. Estimation of direct normal irradiance from measured global and corrected diffuse horizontal irradiance. Energy, 70:382--392, 2014J. A. Kratochvil, W. E. Boyson, and D. L. King. Photovoltaic array performance model. In Photo voltaic array performance model., 2004F. Linke. Transmissions-koeffizient und trubungsfaktor. Beitr. Phys. fr. Atmos, 10:91--103, 1922B. Liu and R. Jordan. A rational procedure for predicting the long-term average performance of flat-plate solar-energy collectors. Solar Energy, 7(2):53--74, 1963Marcu, A. Alexandu, C. Barbu, I. Modeling and simulation of dual - axis solar tracker for pv modules. IOP Conference Series Materials Science and Engineering, 2019J. S. S. Matthew J. Reno, Clifford W. Hansen. Global horizontal irradiance clear sky models implementation and analysis. Sandia National Laboratories, 2012J. J. Michalsky. The astronomical almanac’s algorithm for approximate solar position (1950–2050). Solar Energy, 40:227--235, 1988Mitton S, editor. The Cambridge Enclyclopedia of Astronomy. Crown Publishers, 1977Y. Nassar and S. Alsadi. View factors of flat solar collectors array in flat, inclined, and step-like solar fields. Journal of Solar Energy Engineering, 138, 08 2016Negron Llacuachaqui, F. H. y Salcedo Rosas, J. M. Comparación de la eficiencia de sistemas fotovoltaicos mediante seguimiento solar. Universidad Nacional Del Centro Del Perú, 2017p. Gilman. Sam photovoltaic model technical reference. National Renewable Energy Laboratory (NREL), 2015P. I. R. Perez. A new airmass independent formulation for the linke turbidity coefficient. Solar Energy, 73:151--157, 2002R. Perez, P. Ineichen, R. Seals, J. Michalsky, and R. Stewart. Modeling daylight availability and irradiance components from direct and global irradiance. Solar Energy, 44(5):271--289, 1990R. Perez, R. Stewart, R. Seals, and T. Guertin. The development and verification of the perez diffuse radiation model. Technical Report SAN88-7030, Sandia National Laboratories, Albuquerque, NM, 1988O. Perpiñán. Energía Solar Fotovoltaica, 2023C. L. Pitman and L. L. Vant-Hull. Errors in locating the sun and their effect on solar intensity predictions. American Section of the International Solar Energy Society, pages 701--706, 1978I. Reda and A. Andreas. Solar position algorithm for solar radiation applications. Technical Report TP-560-34302, National Renewable Energy Laboratory, 2003I. Reda and A. Andreass. Solar position algorithm for solar radiation application. Technical report, National Renewable Energy Laboratory, 2008D. Reindl. Estimating diffuse radiation on horizontal surfaces and total radiation on tilted surfaces. Master’s thesis, University of Wisconsin Madison, Solar Energy Laboratory, 1988M. J. Reno, C. W. Hansen, and J. S. Stein. Global horizontal irradiance clear sky models: Implementation and analysis. Technical Report SAND2012-2389, Sandia National Laboratories, March 2012A. Sinton, Ronald A.; Cuevas. Contactless determination of current–voltage characteristics and minority-carrier lifetimes in semiconductors from quasi-steady-state photoconductance data. Applied Physics Letters, 69:2510, 1996Spencer, J.W. Fourier series representation of the position of the sun. Search, 2(5):172+, may 1971A. B. Sproul. Derivation of the solar geometric relationships using vector analysis. Renewable Energy, 32:1187--1205, 2007Strous, L. Position of the sun, 2011J. C. Subtil Lacerda, Juliana; van den Bergh. Diversity in solar photovoltaic energy: Implications for innovation and policy. Renewable and Sustainable Energy Reviews, 54:331--340, 2016Vijay, M. Deepu and Shah, Kamlesh and Bhuvaneswari, G. and Singh, Bhim. Led based street lighting with automatic intensity control using solar pv. IEEE IAS Joint Industrial and Commercial Power Systems / Petroleum and Chemical Industry Conference (ICPSPCIC), 2015R. Walraven. Calculating the position of the sun. Solar Energy, 20(5):393--397, 1978Yusuf S.J. y Romanus I.O. Construction and simulation of dual axes automatic solar tracking system. International Journal of Pure and Applied Science. Published by Cambridge Research and Publications, 2019Zyrianov, Fedor. 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