Modeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink
The electrolyzers work through an electrochemical process, their derivatives (H2, O2, and HHO) are used as enriching fuels due to the electrolysis of water, being cleaner than gasoline and diesel. This article presents the dynamic model of an alkaline electrolyzer that uses an electrolyte (KOH o NaH...
- Autores:
-
Rincón Castrillo, Erick Daniel
Bermudez Santaella, Jose Ricardo
Vera Duarte, Luis Emilio
garcia pabon, juan jose
- Tipo de recurso:
- Article of investigation
- Fecha de publicación:
- 2019
- Institución:
- Universidad Francisco de Paula Santander
- Repositorio:
- Repositorio Digital UFPS
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.ufps.edu.co:ufps/326
- Acceso en línea:
- http://repositorio.ufps.edu.co/handle/ufps/326
https://doi.org/10.22463/0122820X.1826
- Palabra clave:
- Dynamic model
Simulation
Matlab-Simulink
EES
Alkaline Electrolyser
Electrolizador alcalino
Modelo dinámico
Simulación
- Rights
- openAccess
- License
- https://creativecommons.org/licenses/by-nc-nd/4.0/
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dc.title.eng.fl_str_mv |
Modeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink |
dc.title.spa.fl_str_mv |
Modelamiento y simulación de un electrolizador para la producción de HHO en Matlab-Simulink |
title |
Modeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink |
spellingShingle |
Modeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink Dynamic model Simulation Matlab-Simulink EES Alkaline Electrolyser Electrolizador alcalino Modelo dinámico Simulación |
title_short |
Modeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink |
title_full |
Modeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink |
title_fullStr |
Modeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink |
title_full_unstemmed |
Modeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink |
title_sort |
Modeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink |
dc.creator.fl_str_mv |
Rincón Castrillo, Erick Daniel Bermudez Santaella, Jose Ricardo Vera Duarte, Luis Emilio garcia pabon, juan jose |
dc.contributor.author.none.fl_str_mv |
Rincón Castrillo, Erick Daniel Bermudez Santaella, Jose Ricardo Vera Duarte, Luis Emilio garcia pabon, juan jose |
dc.subject.proposal.eng.fl_str_mv |
Dynamic model Simulation Matlab-Simulink EES Alkaline Electrolyser |
topic |
Dynamic model Simulation Matlab-Simulink EES Alkaline Electrolyser Electrolizador alcalino Modelo dinámico Simulación |
dc.subject.proposal.spa.fl_str_mv |
Electrolizador alcalino Modelo dinámico Simulación |
description |
The electrolyzers work through an electrochemical process, their derivatives (H2, O2, and HHO) are used as enriching fuels due to the electrolysis of water, being cleaner than gasoline and diesel. This article presents the dynamic model of an alkaline electrolyzer that uses an electrolyte (KOH o NaHCO3) dissolved in distilled water to accelerate the production of oxyhydrogen (HHO). The model shows the phase change that occurs inside the electrolytic cell. The EES® software was used to determine the values of enthalpy, entropy, and free energy that vary during the electrochemical reaction; the equations were simulated in Matlab-Simulink® to observe their dynamic behavior. The Simulations presented varying every 5 g the electrolyte until reaching 20 g. The flow rate of HHO with potassium hydroxide (20 g) is higher than 0.02 L / s, and with sodium bicarbonate (20 g) it is above 0.0006 L / s, confirming what the literature of alkaline cells state, that the most efficient electrolyte for its energy conversion is KOH |
publishDate |
2019 |
dc.date.issued.none.fl_str_mv |
2019-05-01 |
dc.date.accessioned.none.fl_str_mv |
2021-10-15T22:40:17Z |
dc.date.available.none.fl_str_mv |
2021-10-15T22:40:17Z |
dc.type.spa.fl_str_mv |
Artículo de revista |
dc.type.coarversion.fl_str_mv |
http://purl.org/coar/version/c_970fb48d4fbd8a85 |
dc.type.coar.spa.fl_str_mv |
http://purl.org/coar/resource_type/c_2df8fbb1 |
dc.type.content.spa.fl_str_mv |
Text |
dc.type.driver.spa.fl_str_mv |
info:eu-repo/semantics/article |
dc.type.redcol.spa.fl_str_mv |
http://purl.org/redcol/resource_type/ART |
dc.type.version.spa.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
format |
http://purl.org/coar/resource_type/c_2df8fbb1 |
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publishedVersion |
dc.identifier.uri.none.fl_str_mv |
http://repositorio.ufps.edu.co/handle/ufps/326 |
dc.identifier.doi.none.fl_str_mv |
https://doi.org/10.22463/0122820X.1826 |
url |
http://repositorio.ufps.edu.co/handle/ufps/326 https://doi.org/10.22463/0122820X.1826 |
dc.language.iso.spa.fl_str_mv |
eng |
language |
eng |
dc.relation.citationedition.spa.fl_str_mv |
Vol.24 No.2.(2019) |
dc.relation.citationendpage.spa.fl_str_mv |
15 |
dc.relation.citationissue.spa.fl_str_mv |
2(2019) |
dc.relation.citationstartpage.spa.fl_str_mv |
6 |
dc.relation.citationvolume.spa.fl_str_mv |
24 |
dc.relation.cites.none.fl_str_mv |
E.D. Rincon-Castrillo, J.R. Bermudez-Santaella, L.E. Vera-Duarte, J.J. García-Pabón,“Modeling and simulation of an electrolyser for the production of HHO in Matlab-Simulink®”. Respuestas, vol. 24, no. 2, pp. 6-15, 2019. |
dc.relation.ispartofjournal.spa.fl_str_mv |
Respuestas |
dc.rights.coar.fl_str_mv |
http://purl.org/coar/access_right/c_abf2 |
dc.rights.uri.spa.fl_str_mv |
https://creativecommons.org/licenses/by-nc-nd/4.0/ |
dc.rights.accessrights.spa.fl_str_mv |
info:eu-repo/semantics/openAccess |
dc.rights.creativecommons.spa.fl_str_mv |
Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0) |
rights_invalid_str_mv |
https://creativecommons.org/licenses/by-nc-nd/4.0/ Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0) http://purl.org/coar/access_right/c_abf2 |
eu_rights_str_mv |
openAccess |
dc.format.extent.spa.fl_str_mv |
10 páginas |
dc.format.mimetype.spa.fl_str_mv |
application/pdf |
dc.publisher.place.spa.fl_str_mv |
Colombia |
dc.source.spa.fl_str_mv |
https://ufps.metarevistas.org/index.php/respuestas/article/view/1826 |
institution |
Universidad Francisco de Paula Santander |
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Rincón Castrillo, Erick Daniel4cda91fc6f68e0d1a090f2e34e0bf9b6600Bermudez Santaella, Jose Ricardo3e5142f9c02dda931c75880316d051dc600Vera Duarte, Luis Emilio39ee491fd4a8fd816b6dbd58cc40d497600garcia pabon, juan jose99683da3464a659047c3970827a1497a6002021-10-15T22:40:17Z2021-10-15T22:40:17Z2019-05-01http://repositorio.ufps.edu.co/handle/ufps/326https://doi.org/10.22463/0122820X.1826The electrolyzers work through an electrochemical process, their derivatives (H2, O2, and HHO) are used as enriching fuels due to the electrolysis of water, being cleaner than gasoline and diesel. This article presents the dynamic model of an alkaline electrolyzer that uses an electrolyte (KOH o NaHCO3) dissolved in distilled water to accelerate the production of oxyhydrogen (HHO). The model shows the phase change that occurs inside the electrolytic cell. The EES® software was used to determine the values of enthalpy, entropy, and free energy that vary during the electrochemical reaction; the equations were simulated in Matlab-Simulink® to observe their dynamic behavior. The Simulations presented varying every 5 g the electrolyte until reaching 20 g. The flow rate of HHO with potassium hydroxide (20 g) is higher than 0.02 L / s, and with sodium bicarbonate (20 g) it is above 0.0006 L / s, confirming what the literature of alkaline cells state, that the most efficient electrolyte for its energy conversion is KOHLos electrolizadores funcionan mediante un proceso electroquímico, sus derivados (H2, O2, y HHO) debido a la electrólisis del agua son utilizados como combustibles enriquecedores, siendo más limpios que la gasolina y diesel. Este artículo presenta el modelo dinámico de un electrolizador alcalino que utiliza un electrolito (KOH o NaHCO3) disuelto en agua destilada para acelerar la producción de oxihidrógeno (HHO). El modelo muestra el cambio de fase que ocurre en el interior de la celda electrolítica. Se utilizó el software EES® para determinar los valores de entalpía, entropía, y energía libre que varían durante la reacción electroquímica, las ecuaciones fueron simuladas en Matlab-Simulink® para observar su comportamiento dinámico. Las simulaciones fueron realizadas variando cada 5 g el electrolito hasta llegar a 20 g. El caudal de HHO con hidróxido de potasio (20 g) es superior a 0.02 L/s, y con bicarbonato de sodio (20 g) está por encima de 0.0006 L/s, permitiendo confirmar lo que se enuncia en la literatura de celdas alcalinas, donde se establece que el electrolito más eficiente para su conversión energética es KOH.10 páginasapplication/pdfengPeer review is the responsibility of the Universidad Francisco de Paula Santander. This is an article under the license CC BY-ND (http://creativecommons.org/licenses/by-nc-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://ufps.metarevistas.org/index.php/respuestas/article/view/1826Modeling and simulation of an electrolyser for the production of HHO in Matlab- SimulinkModelamiento y simulación de un electrolizador para la producción de HHO en Matlab-SimulinkArtículo 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_970fb48d4fbd8a85ColombiaVol.24 No.2.(2019)152(2019)624E.D. Rincon-Castrillo, J.R. Bermudez-Santaella, L.E. Vera-Duarte, J.J. García-Pabón,“Modeling and simulation of an electrolyser for the production of HHO in Matlab-Simulink®”. Respuestas, vol. 24, no. 2, pp. 6-15, 2019.RespuestasDynamic modelSimulationMatlab-SimulinkEESAlkaline ElectrolyserElectrolizador alcalinoModelo dinámicoSimulaciónA. C. Turkmen, S. Solmaz and C. Celik,“Analysis of fuel cell vehicles with advisorsoftware”,Renewable & Sustainable EnergyReviews, vol. 70, pp. 1066–1071, 2016.E. D. Rincón, J. J. García and J. R. Bermúdez,“ESTADO DEL ARTE DE LAS CELDAS DECOMBUSTIBLE”, Revista Colombiana deTecnologías de Avanzada, vol. 1, no. 33, pp.36–49, 2019.P. L. Cabot, F. Alcaide and E. Brillas,“Applications - Stationary | Cogeneration ofEnergy and Chemicals: Fuel Cells”,ReferenceModule in Chemistry, Molecular Sciences andChemical Engineering, pp. 146–156, 2013J. Alvarado, “Estudio comparativo delas diferentes tecnologías de celdas decombustible”,Boletín de la Sociedad Españolade Cerámica y Vidrio, vol. 52, no. 3, pp. 105–117, 2013.Á. O. Díaz, J. E. González and O. A.González, “Análisis de un generador de HHOde celda seca para su aplicación en motores decombustión interna”,Revista UIS Ingenierías,vol. 17, no. 1, pp. 143–154, 2018.W. Osorio and Ó. H. Giraldo, “Sobre la termodinámica de las soluciones electrolíticas”, Revista Facultad de Ingeniería Universidad de Antioquia, vol. 40, pp. 7–21, 2007R. Battino, “Comments on the teaching ofchemistry, doing chemistry demonstrations,and a passion for chemical thermodynamics”,The Journal of Chemical Thermodynamics,vol. 123, pp. 74–78, 2018.M. L. Lladó and A. H. Jubert, “Trabajo útil y surelación con la variación de energía de Gibbs”,Educación Química, vol. 22, no. 3, pp. 271–276, 2011.T. Wilberforce et al., “Modelling and simulation of Proton Exchange Membrane fuel cell withserpentine bipolar plate using MATLAB”,International Journal of Hydrogen Energy,vol. 42, no. 40, pp. 25639–25662, 2017.M. M. De Souza, R. S. Gomes and A. L. DeBortoli, “A model for direct ethanol fuel cellsconsidering variations in the concentrationof the species”,International Journal ofHydrogen Energy, vol. 43, no. 29, pp. 13475–13488, 2018.O. Ulleberg, “Modeling of advanced alkalineelectrolyzers: a system simulation approach”,International Journal of Hydrogen Energy,vol. 28, pp. 21–33, 2003.A. Ursúa and P. Sanchis, “Static-dynamicmodelling of the electrical behaviour ofa commercial advanced alkaline waterelectrolyser”, International Journal ofHydrogen Energy, vol. 37, no. 24, pp. 18598–18614, 2012.M. Sánchez, E. Amores, L. Rodríguez andC.Clemente-Jul, “Modelado y simulaciónde sistemas de producción de hidrógenovía electrolisis alcalina a partir de energíasrenovables”, in Congreso Iberoamericano deHidrógeno y Pilas de Combustible 2017, pp. 183–186, 2017.G. Yan et al., “An Arrhenius equation-basedmodel to predict the residual stress relief ofpost weld heat treatment of Ti-6Al-4V plate”,Journal of Manufacturing Processes, vol. 32,pp. 763–772, 2018.D. Michel, “Test of the formal basis ofArrhenius law with heat capacities”,PhysicaA: Statistical Mechanics and its Applications,vol. 510, pp. 188–199, 2018.K. Naveršnik and R. Jurečič, “Humidity-corrected Arrhenius equation: The referencecondition approach”,International JournalofPharmaceutics, vol. 500, no. 1–2, pp. 360–365, 2016.M. Hammoudi, C. Henao, K. Agbossou,Y.Dubé and M. L. Doumbia, “New multi-physics approach for modelling and design ofalkaline electrolyzers”,International Journalof Hydrogen Energy, vol. 37, no. 19, pp.13895–13913, 2012.ORIGINALModeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink.pdfModeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink.pdfapplication/pdf15139599https://repositorio.ufps.edu.co/bitstream/ufps/326/1/Modeling%20and%20simulation%20of%20an%20electrolyser%20for%20the%20production%20of%20HHO%20in%20Matlab-%20Simulink.pdfc00db4aec32e167ad4c0f66863505311MD51open accessLICENSElicense.txtlicense.txttext/plain; charset=utf-814828https://repositorio.ufps.edu.co/bitstream/ufps/326/2/license.txt2f9959eaf5b71fae44bbf9ec84150c7aMD52open accessTEXTModeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink.pdf.txtModeling and simulation of an electrolyser for the production of HHO in Matlab- Simulink.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.
0000-0001-9265-00833e5142f9c02dda931c75880316d051dc6000000-0001-8756-777939ee491fd4a8fd816b6dbd58cc40d4976000000-0002-1894-534X99683da3464a659047c3970827a1497a600 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