Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine

There are several methods for simulating internal combustion engines. The computational fluid dynamics method is the best way to simulate these engines because it can simulate the combustion process, which is a microscopic process. In this study, the simulation of the combustion process in a closed...

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Autores:
Núñez Alvarez, José Ricardo
Tipo de recurso:
Article of investigation
Fecha de publicación:
2024
Institución:
Corporación Universidad de la Costa
Repositorio:
REDICUC - Repositorio CUC
Idioma:
eng
OAI Identifier:
oai:repositorio.cuc.edu.co:11323/13510
Acceso en línea:
https://hdl.handle.net/11323/13510
https://repositorio.cuc.edu.co/
Palabra clave:
Heat transfer coefficient
AVL Fire
Injector nozzle
Computational fluid dynamics
Pressure
Rights
openAccess
License
Atribución 4.0 Internacional (CC BY 4.0)
id RCUC2_ff6e83ce53096abeb2e43a0cd3c50c6b
oai_identifier_str oai:repositorio.cuc.edu.co:11323/13510
network_acronym_str RCUC2
network_name_str REDICUC - Repositorio CUC
repository_id_str
dc.title.none.fl_str_mv Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine
title Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine
spellingShingle Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine
Heat transfer coefficient
AVL Fire
Injector nozzle
Computational fluid dynamics
Pressure
title_short Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine
title_full Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine
title_fullStr Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine
title_full_unstemmed Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine
title_sort Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine
dc.creator.fl_str_mv Núñez Alvarez, José Ricardo
dc.contributor.author.none.fl_str_mv Núñez Alvarez, José Ricardo
dc.contributor.corporatename.none.fl_str_mv Zareei, Javad
Nuñez Alvarez, Jose Ricardo
dc.subject.proposal.eng.fl_str_mv Heat transfer coefficient
AVL Fire
Injector nozzle
Computational fluid dynamics
Pressure
topic Heat transfer coefficient
AVL Fire
Injector nozzle
Computational fluid dynamics
Pressure
description There are several methods for simulating internal combustion engines. The computational fluid dynamics method is the best way to simulate these engines because it can simulate the combustion process, which is a microscopic process. In this study, the simulation of the combustion process in a closed cycle in a diesel engine with a mixture of diesel and hydrogen is done by AVL Fire software. In order to simulate the combustion in the Species and chemical transmission section, a chemkin mechanism is coupled with AVL Fire software. In this study, the effect of 10 % hydrogen fuel and 90 % diesel fuel as well as the effect of nozzle holes (1, 3 and 6 holes) on the engine performance were directly investigated. In order to validate the results of the pressure simulation and the temperature inside the cylinder in the diesel fuel combustion mode, at 2800 rpm and 100 % load, the data were compared with the experimental data. The research also included verification of the heat transfer coefficient (HTC) results with theoretical data obtained by Woschni and Hohenberg. To accurately simulate the combustion process, the simulation data was validated by comparing the pressure and temperature inside the cylinder at a specific operating condition with experimental data. The results indicate that the maximum heat transfer coefficient is achieved at the angle of maximum pressure, with the exhaust valve having the highest coefficient. The addition of hydrogen to diesel fuel results in a 1.72 % increase in the heat transfer coefficient due to increased collisions. In addition, the introduction of hydrogen fuel increases cylinder pressure and engine power, while increasing the number of fuel nozzle holes decreases the coefficient and pressure, which affects fuel penetration and evaporation rate.
publishDate 2024
dc.date.accessioned.none.fl_str_mv 2024-10-23T16:49:15Z
dc.date.available.none.fl_str_mv 2024-10-23T16:49:15Z
dc.date.issued.none.fl_str_mv 2024-06-13
dc.type.none.fl_str_mv Artículo de revista
dc.type.coar.none.fl_str_mv http://purl.org/coar/resource_type/c_2df8fbb1
dc.type.content.none.fl_str_mv Text
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dc.identifier.citation.none.fl_str_mv Javad Zareei, Jose Ricardo Nuñez Alvarez, Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine, Data in Brief, Volume 55, 2024, 110597, ISSN 2352-3409, https://doi.org/10.1016/j.dib.2024.110597.
dc.identifier.uri.none.fl_str_mv https://hdl.handle.net/11323/13510
dc.identifier.doi.none.fl_str_mv 10.1016/j.dib.2024.110597
dc.identifier.eissn.none.fl_str_mv 2352-3409
dc.identifier.instname.none.fl_str_mv Corporación Universidad de la Costa
dc.identifier.reponame.none.fl_str_mv REDICUC - Repositorio CUC
dc.identifier.repourl.none.fl_str_mv https://repositorio.cuc.edu.co/
identifier_str_mv Javad Zareei, Jose Ricardo Nuñez Alvarez, Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine, Data in Brief, Volume 55, 2024, 110597, ISSN 2352-3409, https://doi.org/10.1016/j.dib.2024.110597.
10.1016/j.dib.2024.110597
2352-3409
Corporación Universidad de la Costa
REDICUC - Repositorio CUC
url https://hdl.handle.net/11323/13510
https://repositorio.cuc.edu.co/
dc.language.iso.none.fl_str_mv eng
language eng
dc.relation.ispartofjournal.none.fl_str_mv Elsevier
dc.relation.references.none.fl_str_mv J. Zareei, N. Alvarez, Analysis of the effect of the number of injector nozzles on the pressure and heat transfer coefficient in a hydrogen-diesel mixture diesel engine, Int. J. Hydrog. Energy (2024).
H. Alkhareef, A. Farad, M. Salem, F. Piao, H. Yusing, Z. Yang, Development of Ultra-Low Emissions Gas Turbine Combustor System, University College London, 2017.
R.R. Devetyarov, The formation of soot on the walls of the diesel combustion chamber and its effect on heat transfer in the cylinder, IOP Conf. Ser. 862 (6) (2020) 062072.
R.W. Weeks, J.J. Moskwa, Automotive engine modeling for real-time control using matlab/simulink, SAE Trans. (1995) 295–309.
M. Manikandan, S. Saraswati, K. Ananthakrishnan, CFD analysis of fluid flow inside a pentroof combustion chamber with different piston shapes, Int. J. Veh. Des. 73 (4) (2017) 281–299.
D. Szpica, G. Mieczkowski, A. Borawski, V. Leisis, S. Diliunas, T. Pilkaite, The computational fluid dynamics (CFD) analysis of the pressure sensor used in pulse-operated low-pressure gas-phase solenoid valve measurements, Sensors 21 (24) (2021) 8287.
B. Gainey, J. Gohn, Z. Yan, K. Malik, M.R. Boldaji, B. Lawler, HCCI with wet ethanol: investigating the charge cooling effect of a high latent heat of vaporization fuel in LTC, SAE Tech. Pap. (2019).
Z. Yan, B. Gainey, B. Lawler, A parametric modeling study of thermal barrier coatings in low-temperature combustion engines, Appl. Therm. Eng. 200 (2022) 117687.
S. Cho, C. Song, N. Kim, S. Oh, D. Han, K. Min, Influence of the wall temperatures of the combustion chamber and intake ports on the charge temperature and knock characteristics in a spark-ignited engine, Appl. Therm. Eng. 182 (2021) 116000.
K. Luo, Y. Huang, Z. Han, Y. Li, Y. Shi, W. Liu, C. Tang, Low-speed performance compensation of a turbocharged natural gas engine by intake strategy optimization, Fuel 324 (2022) 124748.
A. Navid, K. Ghadamkheir, A. Hasche, J. Zareei, H. Krause, S. Eckart, Combustion analysis of methane-hydrogen port injection combined with OMEn/Diesel spray injection in an RCCI engine, Int. J. Hydrog. Energy 54 (2024) 1319–1328.
M.B. Ahmed, M.W. Mekonen, Effects of injector nozzle number of holes and fuel injection pressures on the diesel engine characteristics operated with waste cooking oil biodiesel blends, Fuels 3 (2) (2022) 275–294.
C. Kavuri, C. Koci, J. Anders, K. Svensson, R. Fitzgerald, G. Martin, R. Zellers, S. Kokjohn, A. Dempsey, Experimental and computational study comparing conventional diesel injectors and diverging group hole nozzle injectors in a high temperature pressure vessel and a heavy-duty diesel engine, Int. J. Engine Res. 24 (3) (2023) 769–792.
L. Zhou, Y. Liang, Study on the transient injection rate of each nozzle hole in the combustion process of diesel engine, J. Energy Resour. Technol. 143 (7) (2021) 072301.
T. Wen, H. Zhan, D. Zhang, Flow boiling heat transfer in mini channel with serrated fins: experimental investigation and development of new correlation, Int. J. Heat Mass Transf. 128 (2019) 1081–1094.
S.H. Abidi, M.M. Hasan, Variation of turbulent kinetic energy due to dimples in intake manifold for diesel engine, Case Stud. Therm. Eng. 27 (2021) 101299.
dc.relation.citationendpage.none.fl_str_mv 10
dc.relation.citationstartpage.none.fl_str_mv 1
dc.relation.citationissue.none.fl_str_mv 110597
dc.relation.citationvolume.none.fl_str_mv Volumen 55
dc.rights.none.fl_str_mv © 2024 The Authors.
dc.rights.license.none.fl_str_mv Atribución 4.0 Internacional (CC BY 4.0)
dc.rights.uri.none.fl_str_mv https://creativecommons.org/licenses/by/4.0/
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dc.rights.coar.none.fl_str_mv http://purl.org/coar/access_right/c_abf2
rights_invalid_str_mv Atribución 4.0 Internacional (CC BY 4.0)
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spelling Atribución 4.0 Internacional (CC BY 4.0)© 2024 The Authors.https://creativecommons.org/licenses/by/4.0/info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2Núñez Alvarez, José Ricardovirtual::1757-1Zareei, JavadNuñez Alvarez, Jose Ricardo2024-10-23T16:49:15Z2024-10-23T16:49:15Z2024-06-13Javad Zareei, Jose Ricardo Nuñez Alvarez, Dataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engine, Data in Brief, Volume 55, 2024, 110597, ISSN 2352-3409, https://doi.org/10.1016/j.dib.2024.110597.https://hdl.handle.net/11323/1351010.1016/j.dib.2024.1105972352-3409Corporación Universidad de la CostaREDICUC - Repositorio CUChttps://repositorio.cuc.edu.co/There are several methods for simulating internal combustion engines. The computational fluid dynamics method is the best way to simulate these engines because it can simulate the combustion process, which is a microscopic process. In this study, the simulation of the combustion process in a closed cycle in a diesel engine with a mixture of diesel and hydrogen is done by AVL Fire software. In order to simulate the combustion in the Species and chemical transmission section, a chemkin mechanism is coupled with AVL Fire software. In this study, the effect of 10 % hydrogen fuel and 90 % diesel fuel as well as the effect of nozzle holes (1, 3 and 6 holes) on the engine performance were directly investigated. In order to validate the results of the pressure simulation and the temperature inside the cylinder in the diesel fuel combustion mode, at 2800 rpm and 100 % load, the data were compared with the experimental data. The research also included verification of the heat transfer coefficient (HTC) results with theoretical data obtained by Woschni and Hohenberg. To accurately simulate the combustion process, the simulation data was validated by comparing the pressure and temperature inside the cylinder at a specific operating condition with experimental data. The results indicate that the maximum heat transfer coefficient is achieved at the angle of maximum pressure, with the exhaust valve having the highest coefficient. The addition of hydrogen to diesel fuel results in a 1.72 % increase in the heat transfer coefficient due to increased collisions. In addition, the introduction of hydrogen fuel increases cylinder pressure and engine power, while increasing the number of fuel nozzle holes decreases the coefficient and pressure, which affects fuel penetration and evaporation rate.10 páginasapplication/pdfengCorporación Universidad de la CostaUnited stateshttps://www.sciencedirect.com/science/article/pii/S235234092400564X?via%3DihubDataset of the effect of the number of injector holes on the heat transfer coefficient and the pressure in the combustion chamber of a hydrogen-diesel engineArtículo de revistahttp://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_970fb48d4fbd8a85ElsevierJ. Zareei, N. Alvarez, Analysis of the effect of the number of injector nozzles on the pressure and heat transfer coefficient in a hydrogen-diesel mixture diesel engine, Int. J. Hydrog. Energy (2024).H. Alkhareef, A. Farad, M. Salem, F. Piao, H. Yusing, Z. Yang, Development of Ultra-Low Emissions Gas Turbine Combustor System, University College London, 2017.R.R. Devetyarov, The formation of soot on the walls of the diesel combustion chamber and its effect on heat transfer in the cylinder, IOP Conf. Ser. 862 (6) (2020) 062072.R.W. Weeks, J.J. Moskwa, Automotive engine modeling for real-time control using matlab/simulink, SAE Trans. (1995) 295–309.M. Manikandan, S. Saraswati, K. Ananthakrishnan, CFD analysis of fluid flow inside a pentroof combustion chamber with different piston shapes, Int. J. Veh. Des. 73 (4) (2017) 281–299.D. Szpica, G. Mieczkowski, A. Borawski, V. Leisis, S. Diliunas, T. Pilkaite, The computational fluid dynamics (CFD) analysis of the pressure sensor used in pulse-operated low-pressure gas-phase solenoid valve measurements, Sensors 21 (24) (2021) 8287.B. Gainey, J. Gohn, Z. Yan, K. Malik, M.R. Boldaji, B. Lawler, HCCI with wet ethanol: investigating the charge cooling effect of a high latent heat of vaporization fuel in LTC, SAE Tech. Pap. (2019).Z. Yan, B. Gainey, B. Lawler, A parametric modeling study of thermal barrier coatings in low-temperature combustion engines, Appl. Therm. Eng. 200 (2022) 117687.S. Cho, C. Song, N. Kim, S. Oh, D. Han, K. Min, Influence of the wall temperatures of the combustion chamber and intake ports on the charge temperature and knock characteristics in a spark-ignited engine, Appl. Therm. Eng. 182 (2021) 116000.K. Luo, Y. Huang, Z. Han, Y. Li, Y. Shi, W. Liu, C. Tang, Low-speed performance compensation of a turbocharged natural gas engine by intake strategy optimization, Fuel 324 (2022) 124748.A. Navid, K. Ghadamkheir, A. Hasche, J. Zareei, H. Krause, S. Eckart, Combustion analysis of methane-hydrogen port injection combined with OMEn/Diesel spray injection in an RCCI engine, Int. J. Hydrog. Energy 54 (2024) 1319–1328.M.B. Ahmed, M.W. Mekonen, Effects of injector nozzle number of holes and fuel injection pressures on the diesel engine characteristics operated with waste cooking oil biodiesel blends, Fuels 3 (2) (2022) 275–294.C. Kavuri, C. Koci, J. Anders, K. Svensson, R. Fitzgerald, G. Martin, R. Zellers, S. Kokjohn, A. Dempsey, Experimental and computational study comparing conventional diesel injectors and diverging group hole nozzle injectors in a high temperature pressure vessel and a heavy-duty diesel engine, Int. J. Engine Res. 24 (3) (2023) 769–792.L. Zhou, Y. Liang, Study on the transient injection rate of each nozzle hole in the combustion process of diesel engine, J. Energy Resour. Technol. 143 (7) (2021) 072301.T. Wen, H. Zhan, D. Zhang, Flow boiling heat transfer in mini channel with serrated fins: experimental investigation and development of new correlation, Int. J. Heat Mass Transf. 128 (2019) 1081–1094.S.H. Abidi, M.M. Hasan, Variation of turbulent kinetic energy due to dimples in intake manifold for diesel engine, Case Stud. Therm. Eng. 27 (2021) 101299.101110597Volumen 55Heat transfer coefficientAVL FireInjector nozzleComputational fluid dynamicsPressurePublicationf2f0534f-a529-4c16-9e9c-72275e09951dvirtual::1757-1f2f0534f-a529-4c16-9e9c-72275e09951dvirtual::1757-1https://scholar.google.com.co/citations?user=M5TXcO4AAAAJ&hl=esvirtual::1757-10000-0002-6607-7305virtual::1757-1LICENSElicense.txtlicense.txttext/plain; charset=utf-815543https://repositorio.cuc.edu.co/bitstreams/0d50242e-0464-4763-9846-21fbe13f4689/download73a5432e0b76442b22b026844140d683MD51ORIGINALDataset of the effect of the number of injector.htmDataset of the effect of the number of injector.htmtext/html167086https://repositorio.cuc.edu.co/bitstreams/f5753f51-de3c-4734-a89a-c7f6ea87d02c/download87d7ae7c14e7f4fd1e83522afe348716MD52TEXTDataset of the effect of the number of injector.htm.txtDataset of the effect of the number of injector.htm.txtExtracted 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ara ejercer estos derechos sobre la Obra tal y como se indica a continuación:</p>
    <ol type="a">
      <li>Reproducir la Obra, incorporar la Obra en una o más Obras Colectivas, y reproducir la Obra incorporada en las Obras Colectivas.</li>
      <li>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.</li>
      <li>Distribuir copias de las Obras Derivadas que se generen, exhibirlas públicamente, ejecutarlas públicamente y/o ponerlas a disposición pública.</li>
    </ol>
    <p>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).</p>
  </li>
  <br/>
  <li>
    Restricciones.
    <p>La licencia otorgada en la anterior Sección 3 está expresamente sujeta y limitada por las siguientes restricciones:</p>
    <ol type="a">
      <li>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).</li>
      <li>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.</li>
      <li>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.</li>
      <li>
        Para evitar toda confusión, el Licenciante aclara que, cuando la obra es una composición musical:
        <ol type="i">
          <li>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.</li>
          <li>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.</li>
        </ol>
      </li>
      <li>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.</li>
    </ol>
  </li>
  <br/>
  <li>
    Representaciones, Garantías y Limitaciones de Responsabilidad.
    <p>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.</p>
  </li>
  <br/>
  <li>
    Limitación de responsabilidad.
    <p>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.</p>
  </li>
  <br/>
  <li>
    Término.
    <ol type="a">
      <li>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.</li>
      <li>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.</li>
    </ol>
  </li>
  <br/>
  <li>
    Varios.
    <ol type="a">
      <li>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.</li>
      <li>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.</li>
      <li>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.</li>
      <li>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.</li>
    </ol>
  </li>
  <br/>
</ol>
