Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids
A Brayton cycle analysis with regeneration fed by heat input from a central concentration solar energy tower and a combustion chamber that uses natural gas is presented. The thermodynamic model includes the irreversibility of the different components of a conventional Brayton cycle system and a sola...
- Autores:
-
Moreno Gamboa, Faustino
Nieto Londoño, Cesar
Sanin Villa, Daniel
- Tipo de recurso:
- Article of journal
- Fecha de publicación:
- 2024
- Institución:
- Universidad Francisco de Paula Santander
- Repositorio:
- Repositorio Digital UFPS
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.ufps.edu.co:ufps/9158
- Acceso en línea:
- https://repositorio.ufps.edu.co/handle/ufps/9158
- Palabra clave:
- Power plant
Solar power plant
Hybrid Brayton cycle
Energy
Exergy
- Rights
- openAccess
- License
- https://creativecommons.org/licenses/by-nc-nd/4.0/
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Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids |
| title |
Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids |
| spellingShingle |
Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids Power plant Solar power plant Hybrid Brayton cycle Energy Exergy |
| title_short |
Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids |
| title_full |
Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids |
| title_fullStr |
Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids |
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Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids |
| title_sort |
Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids |
| dc.creator.fl_str_mv |
Moreno Gamboa, Faustino Nieto Londoño, Cesar Sanin Villa, Daniel |
| dc.contributor.author.none.fl_str_mv |
Moreno Gamboa, Faustino Nieto Londoño, Cesar Sanin Villa, Daniel |
| dc.subject.proposal.eng.fl_str_mv |
Power plant Solar power plant Hybrid Brayton cycle Energy Exergy |
| topic |
Power plant Solar power plant Hybrid Brayton cycle Energy Exergy |
| description |
A Brayton cycle analysis with regeneration fed by heat input from a central concentration solar energy tower and a combustion chamber that uses natural gas is presented. The thermodynamic model includes the irreversibility of the different components of a conventional Brayton cycle system and a solar concentration system through energy and exergy considerations. The environmental conditions of Barranquilla are used for the plant analysis using different working fluids throughout the day, where the carbon dioxide cycle presents an overall efficiency of 28.8 %, the cycle with air efficiency is 26.6 %, and the Helium cycle is 20.2 %. The model considers the energy flows within the plant and the exergy destruction. In this sense, the solar concentration system contributes an energy fraction of 0.209 when operating with air, while the exergy destruction fraction is 0.189 when operating with carbon dioxide when solar radiation is maximum. Finally, an estimation of the Levelized Cost of Energy is presented. |
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2024 |
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2024-05-14 |
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2025-03-03T16:31:01Z |
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2025-03-03T16:31:01Z |
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https://repositorio.ufps.edu.co/handle/ufps/9158 |
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10.1016/j.ijft.2024.100693 |
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10.1016/j.ijft.2024.100693 |
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(2024) |
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Moreno-Gamboa F, Nieto-Londoño C, Sanin-Villa D. Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids. International Journal of Thermofluids. 2024 May;22:100693. doi: 10.1016/j.ijft.2024.100693 |
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International journal of thermofluids |
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Moreno Gamboa, FaustinoNieto Londoño, CesarSanin Villa, Daniel2025-03-03T16:31:01Z2025-03-03T16:31:01Z2024-05-14https://repositorio.ufps.edu.co/handle/ufps/915810.1016/j.ijft.2024.100693A Brayton cycle analysis with regeneration fed by heat input from a central concentration solar energy tower and a combustion chamber that uses natural gas is presented. The thermodynamic model includes the irreversibility of the different components of a conventional Brayton cycle system and a solar concentration system through energy and exergy considerations. The environmental conditions of Barranquilla are used for the plant analysis using different working fluids throughout the day, where the carbon dioxide cycle presents an overall efficiency of 28.8 %, the cycle with air efficiency is 26.6 %, and the Helium cycle is 20.2 %. The model considers the energy flows within the plant and the exergy destruction. In this sense, the solar concentration system contributes an energy fraction of 0.209 when operating with air, while the exergy destruction fraction is 0.189 when operating with carbon dioxide when solar radiation is maximum. Finally, an estimation of the Levelized Cost of Energy is presented.13 Páginasapplication/pdfengInternational journal of thermofluidsThis is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/bync-nd/4.0/).https://creativecommons.org/licenses/by-nc-nd/4.0/info:eu-repo/semantics/openAccessAtribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0)http://purl.org/coar/access_right/c_abf2https://investigacion.upb.edu.co/en/publications/thermoeconomic-analysis-for-hybrid-solar-brayton-cycles-operatingThermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluidsArtículo de revistahttp://purl.org/coar/resource_type/c_6501http://purl.org/coar/resource_type/c_2df8fbb1Textinfo:eu-repo/semantics/articlehttp://purl.org/redcol/resource_type/ARTinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/version/c_970fb48d4fbd8a85Vol.22 No. (2024)13(2024)122Moreno-Gamboa F, Nieto-Londoño C, Sanin-Villa D. Thermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids. International Journal of Thermofluids. 2024 May;22:100693. doi: 10.1016/j.ijft.2024.100693Power plantSolar power plantHybrid Brayton cycleEnergyExergy[1] L.A. Weinstein, J. Loomis, B. Bhatia, D.M. Bierman, E.N. Wang, G. Chen, Concentrating Solar Power, Chem. Rev. 115 (23) (2015) 12797–12838.[2] K. Obaideen, et al., On the contribution of solar energy to sustainable developments goals: Case study on Mohammed bin Rashid Al Maktoum Solar Park, Int. J. Thermofluids 12 (2021) 100123.[3] O. Behar, Solar thermal power plants - A review of configurations and performance comparison, Renew. Sustain. Energy Rev. 92 (2017) 608–627. October2018.[4] REN21, “Renewables 2023-global status report, Energy Supply Module.,” Paris, 2023.[5] A.H. Alami, et al., Concentrating solar power (CSP)[6] J. Horlock, W. Bathie, Advanced Gas Turbine Cycles, 1st ed., 1, Elsevier Science Ltd., Oxford, 2004.[7] S. Ramakrishnan, C.F. Edwards, Maximum-efficiency architectures for heat- and work-regenerative gas turbine engines, Energy 100 (2016) 115–128. Apr.[8] M.R. Meas, T. Bello-Ochende, Thermodynamic design optimisation of an open air recuperative twin-shaft solar thermal Brayton cycle with combined or exclusive reheating and intercooling, Energy Convers. Manag. 148 (2017) 770–784. Sep.[9] G. Gonca, Exergetic and ecological performance analyses of a gas turbine system with two intercoolers and two re-heaters, Energy 124 (2017) 579–588. Apr.[10] R. Korzynietz, et al., Solugas - Comprehensive analysis of the solar hybrid Brayton plant, Sol. Energy 135 (2016) 578–589.[11] M.T. Dunham, B.D. Iverson, High-efficiency thermodynamic power cycles for concentrated solar power systems, Renew. Sustain. Energy Rev. 30 (2014) 758–770.[12] M. Saghafifar, M. Gadalla, Thermo-economic analysis of conventional combined cycle hybridization: United Arab Emirates case study, Energy Convers. Manag. 111 (2016) 358–374.[13] A. Durante, G. Pena-vergara, P.L. Curto-risso, A. Medina, A.C. Hernandez, ´ Thermodynamic simulation of a multi-step externally fired gas turbine powered by biomass, Energy Convers. Manag. 140 (2017) 182–191.[14] M. Quero, R. Korzynietz, M. Ebert, A.A. Jim´enez, A. Río, J.A. Brioso, Solugas – Operation experience of the first solar hybrid gas turbine system at MW scale, Energy Procedia 49 (2014) 1820–1830.[15] Q. Liu, Z. Bai, X. Wang, J. Lei, H. Jin, Investigation of thermodynamic performances for two solar-biomass hybrid combined cycle power generation systems, Energy Convers. Manag. 122 (2016) 252–262. Aug.[16] R.K. Bhargava, M. Bianchi, A. De Pascale, G. Negri di Montenegro, A. Peretto, Gas Turbine Based Power Cycles - A State-of-the-Art Review. Challenges of Power Engineering and Environment, Springer Berlin Heidelberg, Berlin, Heidelberg, 2007, pp. 309–319.[17] D. Olivenza-Leon, ´ A. Medina, A.Calvo Hernandez, ´ Thermodynamic modeling of a hybrid solar gas-turbine power plant, Energy Convers. Manag. 93 (2015) 435–447.[18] I.I. Enagi, K.A. Al-attab, Z.A. Zainal, Liquid biofuels utilization for gas turbines: A review, Renewable and Sustainable Energy Reviews 90 (2018) 43–55, 01-Jul-.[19] R.P. Merchan, ´ M.J. Santos, I. Heras, J. Gonzalez-Ayala, A. Medina, A.C. Hern´ andez, On-design pre-optimization and off-design analysis of hybrid Brayton thermosolar tower power plants for different fluids and plant configurations, Renew. Sustain. Energy Rev. 119 (2020).[20] Y. Liu, Y. Wang, D. Huang, Supercritical CO2 Brayton cycle: A state-of-the-art review, Energy 189 (2019) 115900.[21] T. Neises, C. Turchi, A comparison of supercritical carbon dioxide power cycle configurations with an emphasis on CSP applications, Energy Procedia 49 (2014) 1187–1196.[22] X. Lei, R. Peng, Z. Guo, H. Li, K. Ali, X. Zhou, Experimental comparison of the heat transfer of carbon dioxide under subcritical and supercritical pressures, Int. J. Heat Mass Transf. 152 (2020) 119562.[23] M.J. Santos, C. Miguel-Barbero, R.P. Merchan, ´ A. Medina, A.Calvo Hern´ andez, Roads to improve the performance of hybrid thermosolar gas turbine power plants: Working fluids and multi-stage configurations, Energy Convers. Manag. 165 (2017) 578–592. December2018.[24] O. Olumayegun, M. Wang, G. Kelsall, Closed-cycle gas turbine for power generation: A state-of-the-art review, Fuel 180 (2016) 694–717.[25] C.F. McDonald, Helium turbomachinery operating experience from gas turbine power plants and test facilities, Appl. Therm. Eng. 44 (2012) 108–142, 01-Nov-.[26] T.K. Ibrahim, et al., Thermal performance of gas turbine power plant based on exergy analysis, Appl. Therm. Eng. 115 (2017) 977–985. Mar.[27] M.A. Vakilabadi, M. Bidi, A.F. Najafi, M.H. Ahmadi, Exergy analysis of a hybrid solar-fossil fuel power plant, Energy Sci. Eng. 7 (1) (2019) 146–161. Feb.[28] H. Zhai, Y.J. Dai, J.Y. Wu, R.Z. Wang, Energy and exergy analyses on a novel hybrid solar heating, cooling and power generation system for remote areas, Appl. Energy 86 (9) (2009) 1395–1404. Sep.[29] T. Yue, N. Lior, Thermal hybrid power systems using multiple heat sources of different temperature: Thermodynamic analysis for Brayton cycles, Energy 165 (2018) 639–665.[30] U S Energy Information Administration, “Levelized Cost and Levelized Avoided Cost of New Generation Resources in the Annual Energy Outlook AEO2020,” Washington, 2020.[31] International Renewable Energy Agency (IRENA), “Renewable Power Generation Costs in 2019,” Abu Dabi, United Arab Emirates, 2019.[32] UPME, “BALANCE ENERGETICO COLOMBIANO - BECO.” [Online]. Available: http s://www1.upme.gov.co/InformacionCifras/Paginas/BalanceEnergetico.aspx. [Accessed: 23-Oct-2019].[33] L. Guzman, A. Henao, R. Vasquez, Simulation and optimization of a parabolic trough solar power plant in the city of Barranquilla by using system advisor model (SAM), Energy Procedia 57 (2014) 497–506.[34] C.A. Gueymard, Prediction and performance assessment of mean hourly global radiation, Sol. Energy 68 (3) (2000) 285–303.[35] R. Mejdoul, M. Taqi, S. Ben, U. Hassan, I.I. Mohammedia, The Mean Hourly Global Radiation Prediction Models Investigation in Two Different Climate Regions in Morocco, Int. J. Renew. Energy Res. 2 (4) (2012).[36] W. Yao, Z. Li, T. Xiu, Y. Lu, X. Li, New decomposition models to estimate hourly global solar radiation from the daily value, Sol. Energy 120 (2015) 87–99.[37] F. Moreno-Gamboa, A. Escudero-Atehortua, C. Nieto-Londono, ˜ Performance evaluation of external fired hybrid solar gas-turbine power plant in Colombia using energy and exergy methods, Therm. Sci. Eng. Prog. 20 (2020) 100679.[38] Y. Goswami, Principles of Solar Engineering, Third edit, CRC Press Taylor & Francis Group, Boca Raton, FL, 2015.[39] The National Aeronautics and Space Administration (NASA), “Power Data Access Viewer,” 2020. [Online]. Available: https://power.larc.nasa.gov/data-access -viewer/. [Accessed: 01-Mar-2020].[40] M. Romero, R. Buck, J.E. Pacheco, An Update on Solar Central Receiver Systems, Projects, and Technologies, J. Sol. Energy Eng. 124 (2) (2002) 98–109. May.[41] J. Duffie, W. Beckman, Solar Engineering of Thermal Processes, Fourth Edi, John Wiley & Sons, New Jersey, 2013. [42] Y.A. Cengel and M.E. Boles, Thermo[44] L.E. Parrot, Theoretical upper limit to the conversion efficiency of solar energy, Sol. Energy 21 (6) (1978) 227–229.[45] J. Spelling, PhD Thesis, KTH Royal Institute of Technology, Stockholm, Sweden, 2013[46] Meteosevilla, “Estacion Meterologica ´ Santiponce, Sevilla, Espana. ˜ ” [Online]. Available: www.meteosevilla.com. [Accessed: 25-Jun-2021].[47] National Aeronautic and Space Administration. (NASA), “Power Data Access Viewer,” 2022. [Online]. avaible https://power.larc.nasa.gov/data-access-viewer/ [Accesed: 30-Jun-2022].[48] Caterpillar Company, “Mercury 50 - Power Generation Packages | Solar Turbines.” [Online]. Available: https://www.solarturbines.com/en_US/products/power -generation-packages/mercury-50.html. [Accessed: 01-Mar-2019].[49] M.J. Santos, R.P. Merchan, ´ A. Medina, A.Calvo Hernandez, ´ Seasonal thermodynamic prediction of the performance of a hybrid solar gas-turbine power plant, Energy Convers. Manag. 115 (2016) 89–102.[50] F. Moreno-Gamboa, C. Nieto-Londono, ˜ Energy and exergetic performance analysis of a hybrid solar multi-stage Brayton cycle with different working fluids, Int. J. Thermofluids 20 (2023). August.[51] M. Kulhanek, ´ V. Dost´ al, Supercritical Carbon Dioxide Cycles Thermodynamic Analysis and Comparison, in: Supercritical CO2 power cycle symposium, 2011.[52] S.J. Bae, J. Lee, Y. Ahn, J.I. Lee, Preliminary studies of compact Brayton cycle performance for small modular high temperature Gas-cooled reactor system, Ann. Nucl. Energy 75 (Aug. 2014) 11–19.[53] Z. Tian, B. Jiang, A. Malik, Q. Zheng, Axial helium compressor for hightemperature gas-cooled reactor: A review, Ann. Nucl. Energy 130 (2019) 54–68.[54] E. Ramírez-Cerpa, M. Acosta-Coll, J. V´elez-Zapata, An´ alisis de condiciones climatologicas ´ de precipitaciones de corto plazo en zonas urbanas: caso de estudio Barranquilla, Colombia, Idesia (Arica) 35 (2017) 0, ahead–0.[55] M. Romero, A. Steinfeld, Concentrating solar thermal power and thermochemical fuels, Energy Environ. Sci. 5 (11) (2012) 9234–9245.[56] G.J. Nathan, et al., Solar thermal hybrids for combustion power plant: A growing opportunity, Prog. Energy Combust. Sci. 64 (Jan. 2018) 4–28.[57] M. Martín S´ anchez, “Evaluacion ´ t´ecnico economica ´ de centrales solares de torre con receptores de aire presurizado integrados en turbinas de gas.,” Universidad de Sevilla, 2018.[58] Glacier Media Group, “Markets single - MINING.COM.” [Online]. Available: https://www.mining.com/markets/commodity/natural-gas/1-year/. [Accessed: 16-Oct-2021].[59] International Renewable Energy Agency, “Global LCOE and Auction values.” [Online]. Available: https://www.irena.org/Statistics/View-Data-by-Topic/Cost s/Global-LCOE-and-Auction-values. [Accessed: 18-Oct-2021].[60] International Energy Agency, “Projected Costs of Generating Electricity 2020 – Analysis - IEA.” [Online]. Available: https://www.iea.org/reports/projected-costs -of-generating-electricity-2020. [Accessed: 25-Oct-2021].[61] F. Moreno-Gamboa, E. Florez-Solano, E. Espinel-Blanco, Effect of concentration areas in sensitive analysis of a hybrid solar Brayton cycle, J. Phys. Conf. Ser. 2073 (1) (2021) 012013.[62] A. Valero, M.A. Lozano, and L. Serra, “CGAM Problem : Definition and Conventional Solution,” vol. I, no. 3, pp. 278–286, 1994.[63] F. Carl Knopf, Modeling, Analysis and Optimization of Process and Energy Systems, John Wiley & Sons, New Jersey, 2012.[64] R. Turton, R. Bailie, W. Whiting, J. Shaeiwitz, D. Bhattacharyya, Analysis, Synthesis, and Design of Chemical Processes, Four Editi, Prentice Hall, 2012.[65] P. Schwarzbo, R. Buck, C. Sugarmen, A. Ring, P. Altwegg, and J. Enrile, “Solar gas turbine systems : Design, cost and perspectives,” vol. 80, pp. 1231–1240, 2006.[66] B.L. Kistler, “A user’s manual for DELSOL3: a computer code for calculating the optical performance and optimal system design for solar thermal central receiver plants,” Livermore, CA (USA), 1986.[67] Frangopoulos, A. C, Intelligent functional approach; A method for analysis and optimal synthesis-design-operation of complex systems, Int. J. EnergyEnvironment-Economics; (United States 1 (4) (1991). Jan.[68] S. Pelster, “Environomic modeling and optimization of advanced combined cycle cogeneration power plants including CO2 separation options,” 1998.[69] R.P. Merch´ an, M.J. Santos, A. Medina, A.Calvo Hern´ andez, Thermodynamic model of a hybrid Brayton thermosolar plant, Renew. Energy 128 (2018) 473–483.PublicationORIGINALThermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids.pdfThermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids.pdfArtículo de Investigaciónapplication/pdf4958339https://repositorio.ufps.edu.co/bitstreams/527e331d-d5ce-4c02-a788-dc36ae08f8fc/download71895c640509db6cf058e88f54b4f123MD51trueAnonymousREADLICENSElicense.txtlicense.txttext/plain; charset=utf-814828https://repositorio.ufps.edu.co/bitstreams/c915bf7a-acea-448e-9ac2-2a31d1253b26/download2f9959eaf5b71fae44bbf9ec84150c7aMD52falseAnonymousREADTEXTThermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids.pdf.txtThermoeconomic analysis for hybrid solar Brayton cycles operating with different working fluids.pdf.txtExtracted 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 incorporada en las Obras Colectivas.

b.	Distribuir copias o fonogramas de las Obras, exhibirlas públicamente, ejecutarlas públicamente y/o ponerlas a disposición pública, incluyéndolas como incorporadas en Obras Colectivas, según corresponda.

c.	Distribuir copias de las Obras Derivadas que se generen, exhibirlas públicamente, ejecutarlas públicamente y/o ponerlas a disposición pública.
Los derechos mencionados anteriormente pueden ser ejercidos en todos los medios y formatos, actualmente conocidos o que se inventen en el futuro. Los derechos antes mencionados incluyen el derecho a realizar dichas modificaciones en la medida que sean técnicamente necesarias para ejercer los derechos en otro medio o formatos, pero de otra manera usted no está autorizado para realizar obras derivadas. Todos los derechos no otorgados expresamente por el Licenciante quedan por este medio reservados, incluyendo pero sin limitarse a aquellos que se mencionan en las secciones 4(d) y 4(e).

4. Restricciones.
La licencia otorgada en la anterior Sección 3 está expresamente sujeta y limitada por las siguientes restricciones:

a.	Usted puede distribuir, exhibir públicamente, ejecutar públicamente, o poner a disposición pública la Obra sólo bajo las condiciones de esta Licencia, y Usted debe incluir una copia de esta licencia o del Identificador Universal de Recursos de la misma con cada copia de la Obra que distribuya, exhiba públicamente, ejecute públicamente o ponga a disposición pública. No es posible ofrecer o imponer ninguna condición sobre la Obra que altere o limite las condiciones de esta Licencia o el ejercicio de los derechos de los destinatarios otorgados en este documento. No es posible sublicenciar la Obra. Usted debe mantener intactos todos los avisos que hagan referencia a esta Licencia y a la cláusula de limitación de garantías. Usted no puede distribuir, exhibir públicamente, ejecutar públicamente, o poner a disposición pública la Obra con alguna medida tecnológica que controle el acceso o la utilización de ella de una forma que sea inconsistente con las condiciones de esta Licencia. Lo anterior se aplica a la Obra incorporada a una Obra Colectiva, pero esto no exige que la Obra Colectiva aparte de la obra misma quede sujeta a las condiciones de esta Licencia. Si Usted crea una Obra Colectiva, previo aviso de cualquier Licenciante debe, en la medida de lo posible, eliminar de la Obra Colectiva cualquier referencia a dicho Licenciante o al Autor Original, según lo solicitado por el Licenciante y conforme lo exige la cláusula 4(c).

b.	Usted no puede ejercer ninguno de los derechos que le han sido otorgados en la Sección 3 precedente de modo que estén principalmente destinados o directamente dirigidos a conseguir un provecho comercial o una compensación monetaria privada. El intercambio de la Obra por otras obras protegidas por derechos de autor, ya sea a través de un sistema para compartir archivos digitales (digital file-sharing) o de cualquier otra manera no será considerado como estar destinado principalmente o dirigido directamente a conseguir un provecho comercial o una compensación monetaria privada, siempre que no se realice un pago mediante una compensación monetaria en relación con el intercambio de obras protegidas por el derecho de autor.

c.	Si usted distribuye, exhibe públicamente, ejecuta públicamente o ejecuta públicamente en forma digital la Obra o cualquier Obra Derivada u Obra Colectiva, Usted debe mantener intacta toda la información de derecho de autor de la Obra y proporcionar, de forma razonable según el medio o manera que Usted esté utilizando: (i) el nombre del Autor Original si está provisto (o seudónimo, si fuere aplicable), y/o (ii) el nombre de la parte o las partes que el Autor Original y/o el Licenciante hubieren designado para la atribución (v.g., un instituto patrocinador, editorial, publicación) en la información de los derechos de autor del Licenciante, términos de servicios o de otras formas razonables; el título de la Obra si está provisto; en la medida de lo razonablemente factible y, si está provisto, el Identificador Uniforme de Recursos (Uniform Resource Identifier) que el Licenciante especifica para ser asociado con la Obra, salvo que tal URI no se refiera a la nota sobre los derechos de autor o a la información sobre el licenciamiento de la Obra; y en el caso de una Obra Derivada, atribuir el crédito identificando el uso de la Obra en la Obra Derivada (v.g., "Traducción Francesa de la Obra del Autor Original," o "Guión Cinematográfico basado en la Obra original del Autor Original"). Tal crédito puede ser implementado de cualquier forma razonable; en el caso, sin embargo, de Obras Derivadas u Obras Colectivas, tal crédito aparecerá, como mínimo, donde aparece el crédito de cualquier otro autor comparable y de una manera, al menos, tan destacada como el crédito de otro autor comparable.

d.	Para evitar toda confusión, el Licenciante aclara que, cuando la obra es una composición musical:

i.	Regalías por interpretación y ejecución bajo licencias generales. El Licenciante se reserva el derecho exclusivo de autorizar la ejecución pública o la ejecución pública digital de la obra y de recolectar, sea individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, SAYCO), las regalías por la ejecución pública o por la ejecución pública digital de la obra (por ejemplo Webcast) licenciada bajo licencias generales, si la interpretación o ejecución de la obra está primordialmente orientada por o dirigida a la obtención de una ventaja comercial o una compensación monetaria privada.

ii.	Regalías por Fonogramas. El Licenciante se reserva el derecho exclusivo de recolectar, individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, los consagrados por la SAYCO), una agencia de derechos musicales o algún agente designado, las regalías por cualquier fonograma que Usted cree a partir de la obra (“versión cover”) y distribuya, en los términos del régimen de derechos de autor, si la creación o distribución de esa versión cover está primordialmente destinada o dirigida a obtener una ventaja comercial o una compensación monetaria privada.

e.	Gestión de Derechos de Autor sobre Interpretaciones y Ejecuciones Digitales (WebCasting). Para evitar toda confusión, el Licenciante aclara que, cuando la obra sea un fonograma, el Licenciante se reserva el derecho exclusivo de autorizar la ejecución pública digital de la obra (por ejemplo, webcast) y de recolectar, individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, ACINPRO), las regalías por la ejecución pública digital de la obra (por ejemplo, webcast), sujeta a las disposiciones aplicables del régimen de Derecho de Autor, si esta ejecución pública digital está primordialmente dirigida a obtener una ventaja comercial o una compensación monetaria privada.

5. Representaciones, Garantías y Limitaciones de Responsabilidad.
A MENOS QUE LAS PARTES LO ACORDARAN DE OTRA FORMA POR ESCRITO, EL LICENCIANTE OFRECE LA OBRA (EN EL ESTADO EN EL QUE SE ENCUENTRA) “TAL CUAL”, SIN BRINDAR GARANTÍAS DE CLASE ALGUNA RESPECTO DE LA OBRA, YA SEA EXPRESA, IMPLÍCITA, LEGAL O CUALQUIERA OTRA, INCLUYENDO, SIN LIMITARSE A ELLAS, GARANTÍAS DE TITULARIDAD, COMERCIABILIDAD, ADAPTABILIDAD O ADECUACIÓN A PROPÓSITO DETERMINADO, AUSENCIA DE INFRACCIÓN, DE AUSENCIA DE DEFECTOS LATENTES O DE OTRO TIPO, O LA PRESENCIA O AUSENCIA DE ERRORES, SEAN O NO DESCUBRIBLES (PUEDAN O NO SER ESTOS DESCUBIERTOS). ALGUNAS JURISDICCIONES NO PERMITEN LA EXCLUSIÓN DE GARANTÍAS IMPLÍCITAS, EN CUYO CASO ESTA EXCLUSIÓN PUEDE NO APLICARSE A USTED.

6. Limitación de responsabilidad.
A MENOS QUE LO EXIJA EXPRESAMENTE LA LEY APLICABLE, EL LICENCIANTE NO SERÁ RESPONSABLE ANTE USTED POR DAÑO ALGUNO, SEA POR RESPONSABILIDAD EXTRACONTRACTUAL, PRECONTRACTUAL O CONTRACTUAL, OBJETIVA O SUBJETIVA, SE TRATE DE DAÑOS MORALES O PATRIMONIALES, DIRECTOS O INDIRECTOS, PREVISTOS O IMPREVISTOS PRODUCIDOS POR EL USO DE ESTA LICENCIA O DE LA OBRA, AUN CUANDO EL LICENCIANTE HAYA SIDO ADVERTIDO DE LA POSIBILIDAD DE DICHOS DAÑOS. ALGUNAS LEYES NO PERMITEN LA EXCLUSIÓN DE CIERTA RESPONSABILIDAD, EN CUYO CASO ESTA EXCLUSIÓN PUEDE NO APLICARSE A USTED.

7. Término.

a.	Esta Licencia y los derechos otorgados en virtud de ella terminarán automáticamente si Usted infringe alguna condición establecida en ella. Sin embargo, los individuos o entidades que han recibido Obras Derivadas o Colectivas de Usted de conformidad con esta Licencia, no verán terminadas sus licencias, siempre que estos individuos o entidades sigan cumpliendo íntegramente las condiciones de estas licencias. Las Secciones 1, 2, 5, 6, 7, y 8 subsistirán a cualquier terminación de esta Licencia.

b.	Sujeta a las condiciones y términos anteriores, la licencia otorgada aquí es perpetua (durante el período de vigencia de los derechos de autor de la obra). No obstante lo anterior, el Licenciante se reserva el derecho a publicar y/o estrenar la Obra bajo condiciones de licencia diferentes o a dejar de distribuirla en los términos de esta Licencia en cualquier momento; en el entendido, sin embargo, que esa elección no servirá para revocar esta licencia o que deba ser otorgada , bajo los términos de esta licencia), y esta licencia continuará en pleno vigor y efecto a menos que sea terminada como se expresa atrás. La Licencia revocada continuará siendo plenamente vigente y efectiva si no se le da término en las condiciones indicadas anteriormente.

8. Varios.

a.	Cada vez que Usted distribuya o ponga a disposición pública la Obra o una Obra Colectiva, el Licenciante ofrecerá al destinatario una licencia en los mismos términos y condiciones que la licencia otorgada a Usted bajo esta Licencia.

b.	Si alguna disposición de esta Licencia resulta invalidada o no exigible, según la legislación vigente, esto no afectará ni la validez ni la aplicabilidad del resto de condiciones de esta Licencia y, sin acción adicional por parte de los sujetos de este acuerdo, aquélla se entenderá reformada lo mínimo necesario para hacer que dicha disposición sea válida y exigible.

c.	Ningún término o disposición de esta Licencia se estimará renunciada y ninguna violación de ella será consentida a menos que esa renuncia o consentimiento sea otorgado por escrito y firmado por la parte que renuncie o consienta.

d.	Esta Licencia refleja el acuerdo pleno entre las partes respecto a la Obra aquí licenciada. No hay arreglos, acuerdos o declaraciones respecto a la Obra que no estén especificados en este documento. El Licenciante no se verá limitado por ninguna disposición adicional que pueda surgir en alguna comunicación emanada de Usted. Esta Licencia no puede ser modificada sin el consentimiento mutuo por escrito del Licenciante y Usted.
 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