Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery
This paper analyzes the impact of the Thomson effect on the performance of thermoelectric modules. For this, different mathematical models are carried out that involves the relationship between temperature and the seebeck coefficient. These mathematical models are based on the equations that describ...
- Autores:
-
Rojas Suárez, Jhan Piero
Medina Delgado, Byron
Orjuela Abril, Martha Sofia
- Tipo de recurso:
- Article of journal
- Fecha de publicación:
- 2020
- Institución:
- Universidad Francisco de Paula Santander
- Repositorio:
- Repositorio Digital UFPS
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.ufps.edu.co:ufps/1396
- Acceso en línea:
- http://repositorio.ufps.edu.co/handle/ufps/1396
https://doi.org/10.1088/1742-6596/1708/1/012022
- Palabra clave:
- Rights
- openAccess
- License
- © Copyright 2021 IOP Publishing
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Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery |
| title |
Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery |
| spellingShingle |
Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery |
| title_short |
Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery |
| title_full |
Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery |
| title_fullStr |
Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery |
| title_full_unstemmed |
Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery |
| title_sort |
Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery |
| dc.creator.fl_str_mv |
Rojas Suárez, Jhan Piero Medina Delgado, Byron Orjuela Abril, Martha Sofia |
| dc.contributor.author.none.fl_str_mv |
Rojas Suárez, Jhan Piero Medina Delgado, Byron Orjuela Abril, Martha Sofia |
| description |
This paper analyzes the impact of the Thomson effect on the performance of thermoelectric modules. For this, different mathematical models are carried out that involves the relationship between temperature and the seebeck coefficient. These mathematical models are based on the equations that describe thermoelectric effects and are solved using finite element methods. Through linear and polynomial functions of the seebeck coefficient, the different behaviors that can occur in the Thomson coefficient and their effect on the power and efficiency of thermoelectric modules are analyzed. The results show that by not considering the Thomson effect, there is a variation of 31% and 32% in the power and efficiency of the thermoelectric module when the temperature conditions change, which makes it difficult to estimate the performance of the module. This problem can be solved by considering the Thomson effect since it predicts an approximately constant value of electrical power and efficiency for a wide temperature range. For the analyzed conditions, power and efficiency of 5.25 W and 13%, respectively, were observed. The proposed methodology allows an adequate estimation to determine the performance of the modules. Therefore, it could be implemented to search for materials that provide better thermoelectric characteristics. |
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2020 |
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2020-12-05 |
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2021-11-24T21:22:55Z |
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2021-11-24T21:22:55Z |
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Artículo de revista |
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http://repositorio.ufps.edu.co/handle/ufps/1396 |
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https://doi.org/10.1088/1742-6596/1708/1/012022 |
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eng |
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eng |
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Journal of Physics: Conference Series |
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Vol.1708 No.1.(2020) |
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7 |
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1(2020) |
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1 |
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1708 |
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Suárez, J. R., Delgado, B. M., & Abril, M. O. (2020, December). Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery. In Journal of Physics: Conference Series (Vol. 1708, No. 1, p. 012022). IOP Publishing. |
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Journal of Physics: Conference Series |
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© Copyright 2021 IOP Publishing |
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http://purl.org/coar/access_right/c_abf2 |
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info:eu-repo/semantics/openAccess |
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Atribución 4.0 Internacional (CC BY 4.0) |
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© Copyright 2021 IOP Publishing Atribución 4.0 Internacional (CC BY 4.0) http://purl.org/coar/access_right/c_abf2 |
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openAccess |
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07 páginas |
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Journal of Physics: Conference Series |
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Reino Unido |
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https://iopscience.iop.org/article/10.1088/1742-6596/1708/1/012022/meta |
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Rojas Suárez, Jhan Piero96cb752d974d2a7f4f66513af6ebbf8d600Medina Delgado, Byron77a81f47bf20466c22fcea2d1e82a753600Orjuela Abril, Martha Sofia c7eb007995ff675aa1fb2ed07939a53e6002021-11-24T21:22:55Z2021-11-24T21:22:55Z2020-12-05http://repositorio.ufps.edu.co/handle/ufps/1396https://doi.org/10.1088/1742-6596/1708/1/012022This paper analyzes the impact of the Thomson effect on the performance of thermoelectric modules. For this, different mathematical models are carried out that involves the relationship between temperature and the seebeck coefficient. These mathematical models are based on the equations that describe thermoelectric effects and are solved using finite element methods. Through linear and polynomial functions of the seebeck coefficient, the different behaviors that can occur in the Thomson coefficient and their effect on the power and efficiency of thermoelectric modules are analyzed. The results show that by not considering the Thomson effect, there is a variation of 31% and 32% in the power and efficiency of the thermoelectric module when the temperature conditions change, which makes it difficult to estimate the performance of the module. This problem can be solved by considering the Thomson effect since it predicts an approximately constant value of electrical power and efficiency for a wide temperature range. For the analyzed conditions, power and efficiency of 5.25 W and 13%, respectively, were observed. The proposed methodology allows an adequate estimation to determine the performance of the modules. Therefore, it could be implemented to search for materials that provide better thermoelectric characteristics.07 páginasapplication/pdfengJournal of Physics: Conference SeriesReino UnidoJournal of Physics: Conference SeriesVol.1708 No.1.(2020)71(2020)11708Suárez, J. R., Delgado, B. M., & Abril, M. O. (2020, December). Study of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery. In Journal of Physics: Conference Series (Vol. 1708, No. 1, p. 012022). IOP Publishing.Journal of Physics: Conference Series© Copyright 2021 IOP Publishinginfo:eu-repo/semantics/openAccessAtribución 4.0 Internacional (CC BY 4.0)http://purl.org/coar/access_right/c_abf2https://iopscience.iop.org/article/10.1088/1742-6596/1708/1/012022/metaStudy of the Thomson effect on the performance of thermoelectric modules with application to the energy recoveryArtículo 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_970fb48d4fbd8a85Rowe D M 2018 Thermoelectrics Handbook (Boca Ratón: CRC Press)Luo D, Wang R, Yu W and Zhou W 2020 Parametric study of a thermoelectric module used for both power generation and cooling Renew. Energy 154 542Orr B, Akbarzadeh A, Mochizuki M and Singh R 2016 A review of car waste heat recovery systems utilising thermoelectric generators and heat pipes Appl. Therm. Eng. 101 490Högblom O and Andersson R 2016 A simulation framework for prediction of thermoelectric generator system performance Appl. Energy 180 472Zhang Y, Wang X, Cleary M, Schoensee L, Kempf N and Richardson J 2016 High-performance nanostructured thermoelectric generators for micro combined heat and power systems Appl. Therm. Eng. 96 83Wu S, Zhang H and Ni M 2016 Performance assessment of a hybrid system integrating a molten carbonate fuel cell and a thermoelectric generator Energy 112 520Rezania A, Rosendahl L A and Yin H 2014 Parametric optimization of thermoelectric elements footprint for maximum power generation J. Power Sources 255 151Ibrahim A, Rahnamayan S, Vargas Martin M and Yilbas B 2014 Multi-objective thermal analysis of a thermoelectric device: Influence of geometric features on device characteristics Energy 77 305Kim T Y, Negash A and Cho G 2017 Direct contact thermoelectric generator (DCTEG): A concept for removing the contact resistance between thermoelectric modules and heat source Energy Convers. Manag. 142 20Chen W-H, Huang S-R, Wang X-D, Wu P-H and Lin Y-L 2017 Performance of a thermoelectric generator intensified by temperature oscillation Energy 133 257Dresselhaus M S, Chen G, Tang M Y, Yang R G, Lee H, Wang D Z, Ren Z F, Fleurial J-P and Gogna P 2007 New Directions for Low-Dimensional Thermoelectric Materials Adv. Mater. 19 1043Wang S, Yang B and Lu C 2014 Influences of Thomson effect and additional thermal resistance on the performance of thermoelectric module Journal Tianjin Univ. Sci. Technol. 47 15Yamashita O 2008 Effect of linear temperature dependence of thermoelectric properties on energy conversion efficiency Energy Convers. Manag. 49 3163Kim H S, Liu W and Ren Z 2015 Efficiency and output power of thermoelectric module by taking into account corrected Joule and Thomson heat J. Appl. Phys. 118 115103Cheng F Q, Hong Y J and Zhu C 2013 Thermoelectric Physical model with Thomson effect and experiment comparison Appl. Mech. Mater. 437 1077Antonova E E and Looman D C 2005 24th International Conference on Thermoelectric (USA: IEEE) Finite elements for thermoelectric device analysis in ANSYSManzanares J A, Jokinen M and Cervera J 2015 On the different formalisms for the transport equations of thermoelectricity: A review J. Non-Equilibrium Thermodyn. 40 1Landau L D, Lifshitz E M and King A L 1961 Electrodynamics of continuous media Am. J. Phys. 29 647Lee H 2013 The Thomson effect and the ideal equation on thermoelectric coolers Energy 56 61Meng F K, Chen L G and Sun F R 2010 Extreme working temperature differences for thermoelectric refrigerating and heat pumping devices driven by thermoelectric generator J. Energy Inst. 83 108Feng Y, Chen L, Meng F and Sun F 2018 Thermodynamic analysis of TEG-TEC device including influence of Thomson effect J. Non-Equilibrium Thermodyn. 43 75Sandoz-Rosado E J, Weinstein S J and Stevens R J 2013 On the Thomson effect in thermoelectric power devices Int. J. Therm. Sci. 66 1ORIGINALStudy of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery.pdfStudy of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery.pdfapplication/pdf1341714https://repositorio.ufps.edu.co/bitstream/ufps/1396/1/Study%20of%20the%20Thomson%20effect%20on%20the%20performance%20of%20thermoelectric%20modules%20with%20application%20to%20the%20energy%20recovery.pdf98faca034c6281a7eefbcd4eaa2eb0b8MD51open accessLICENSElicense.txtlicense.txttext/plain; charset=utf-814828https://repositorio.ufps.edu.co/bitstream/ufps/1396/2/license.txt2f9959eaf5b71fae44bbf9ec84150c7aMD52open accessTEXTStudy of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery.pdf.txtStudy of the Thomson effect on the performance of thermoelectric modules with application to the energy recovery.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.
0000-0003-2682-988096cb752d974d2a7f4f66513af6ebbf8d6000000-0003-0754-862977a81f47bf20466c22fcea2d1e82a7536000000-0002-9742-8673c7eb007995ff675aa1fb2ed07939a53e600 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