Wear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory
Se aplicaron dos recubrimientos de plasma atmosférico de ZrO 2 -Al 2 O 3 a un ladrillo refractario de aluminosilicato prensado y sinterizado , que se compararon con un refractario electrofundido de alúmina-zirconia-sílice (AZS) que se usa típicamente en la industria del vidrio por su resistencia a a...
- Autores:
-
Franco Correa, Iván David
Ageorges, Hélène
López Gómez, María Esperanza
Vargas, Fabio Alonso
- Tipo de recurso:
- Article of investigation
- Fecha de publicación:
- 2021
- Institución:
- Tecnológico de Antioquia
- Repositorio:
- Repositorio Tdea
- Idioma:
- eng
- OAI Identifier:
- oai:dspace.tdea.edu.co:tdea/2884
- Acceso en línea:
- https://dspace.tdea.edu.co/handle/tdea/2884
- Palabra clave:
- Aluminosilicatos
Materiales refractarios
Refractory materials
Silicatos de aluminio
Aluminum silicates
Recubrimientos de circona-alúmina
ZrO2-Al2O3
Atmospheric plasma coatings
Proyección térmica
Thermal projection
- Rights
- closedAccess
- License
- http://purl.org/coar/access_right/c_14cb
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oai:dspace.tdea.edu.co:tdea/2884 |
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| dc.title.none.fl_str_mv |
Wear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory |
| title |
Wear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory |
| spellingShingle |
Wear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory Aluminosilicatos Materiales refractarios Refractory materials Silicatos de aluminio Aluminum silicates Recubrimientos de circona-alúmina ZrO2-Al2O3 Atmospheric plasma coatings Proyección térmica Thermal projection |
| title_short |
Wear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory |
| title_full |
Wear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory |
| title_fullStr |
Wear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory |
| title_full_unstemmed |
Wear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory |
| title_sort |
Wear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory |
| dc.creator.fl_str_mv |
Franco Correa, Iván David Ageorges, Hélène López Gómez, María Esperanza Vargas, Fabio Alonso |
| dc.contributor.author.none.fl_str_mv |
Franco Correa, Iván David Ageorges, Hélène López Gómez, María Esperanza Vargas, Fabio Alonso |
| dc.subject.other.none.fl_str_mv |
Aluminosilicatos Materiales refractarios Refractory materials |
| topic |
Aluminosilicatos Materiales refractarios Refractory materials Silicatos de aluminio Aluminum silicates Recubrimientos de circona-alúmina ZrO2-Al2O3 Atmospheric plasma coatings Proyección térmica Thermal projection |
| dc.subject.lcshuri.none.fl_str_mv |
Silicatos de aluminio Aluminum silicates |
| dc.subject.proposal.none.fl_str_mv |
Recubrimientos de circona-alúmina ZrO2-Al2O3 Atmospheric plasma coatings Proyección térmica Thermal projection |
| description |
Se aplicaron dos recubrimientos de plasma atmosférico de ZrO 2 -Al 2 O 3 a un ladrillo refractario de aluminosilicato prensado y sinterizado , que se compararon con un refractario electrofundido de alúmina-zirconia-sílice (AZS) que se usa típicamente en la industria del vidrio por su resistencia a altas temperaturas. resistencia. Las muestras se sometieron a contacto deslizante mediante una prueba de bola en disco a 25, 500, 750 y 1000 °C y luego se realizaron caracterizaciones físicas, cristalográficas y mecánicas antes y después de las pruebas de desgaste para monitorear el desgaste . comportamiento. Ambos ZrO 2 -Al 2 O 3Los recubrimientos exhibieron un mejor comportamiento al desgaste que el refractario AZS electrofundido a todas las temperaturas evaluadas, debido a su alta dureza y tenacidad a la fractura , que se relacionaron principalmente con el aumento de las fases α-Al 2 O 3 y t-ZrO 2 a partir de γ-Al 2 O 3 y la cristalización de amorfofases respectivamente. De la misma manera, ambos recubrimientos también mostraron los mismos mecanismos de desgaste a todas las temperaturas evaluadas. A 25 °C se identificó desgaste por deformación dúctil, mientras que a 500 y 750 °C se produjo desgaste por deformación frágil, y a 1000 °C se evidenció la transición del desgaste de deformación frágil a dúctil. Para el refractario AZS electrofundido, hasta los 750 °C se desarrolló desgaste por deformación frágil, mientras que a 1000 °C se detectó desgaste por deformación tanto frágil como dúctil. |
| publishDate |
2021 |
| dc.date.issued.none.fl_str_mv |
2021 |
| dc.date.accessioned.none.fl_str_mv |
2023-05-15T21:24:22Z |
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2023-05-15T21:24:22Z |
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Artículo de revista |
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http://purl.org/coar/resource_type/c_2df8fbb1 |
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Text |
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info:eu-repo/semantics/article |
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http://purl.org/redcol/resource_type/ART |
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info:eu-repo/semantics/publishedVersion |
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http://purl.org/coar/version/c_970fb48d4fbd8a85 |
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0257-8972 |
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https://dspace.tdea.edu.co/handle/tdea/2884 |
| dc.identifier.eissn.spa.fl_str_mv |
1879-3347 |
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0257-8972 1879-3347 |
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https://dspace.tdea.edu.co/handle/tdea/2884 |
| dc.language.iso.spa.fl_str_mv |
eng |
| language |
eng |
| dc.relation.citationvolume.spa.fl_str_mv |
425 |
| dc.relation.ispartofjournal.spa.fl_str_mv |
Surface & coatings technology |
| dc.relation.references.spa.fl_str_mv |
P. Nayar et al. Structural, optical and mechanical properties of amorphous and crystalline alumina thin films Thin Solid Films (2014) T.E. Fischer et al. Genesis and role of wear debris in sliding wear of ceramics Wear (2000) M. Wang et al. Effects of the powder manufacturing method on microstructure and wear performance of plasma sprayed alumina – titania coatings Surf. Coat. Technol. (2007) F. Vargas et al. Mechanical and tribological performance of Al2O3-TiO2 coatings elaborated by flame and plasma spraying Surf. Coat. Technol. (2010) J.H. Ouyang et al. Microstructure and tribological characteristics of ZrO2 – Y2O3 ceramic coatings deposited by laser – assisted plasma hybrid spraying Tribol. Int. (2002) H. Chen et al. Tribological properties of nanostructured zirconia coatings deposited by plasma spraying Wear (2002) S. Heiroth et al. Optical and mechanical properties of amorphous and crystalline yttria-stabilized zirconia thin films prepared by pulsed laser deposition Acta Mater. (2011) J. Luo et al. Porosity-dependence of elastic moduli and hardness of 3Y-TZP ceramics Ceram. Int. (1999) K.A. Habib et al. Comparison of flame sprayed Al2O3/TiO2 coatings: their microstructure, mechanical properties and tribology behavior Surf. Coat. Technol. (2006) A. González et al. Efecto de la microestructura y de la microdureza sobre la resistencia al desgaste de recubrimientos elaborados por proyección térmica por plasma atmosférico a partir de circona – alúmina, circona – itria y circona – ceria Boletín de la Sociedad Española de Cerámica y Vidrio (2015) K. Sabiruddin et al. Analysis of phase transformation in plasma sprayed alumina coatings using Rietveld refinement Surf. Coat. Technol. (2010) G.N. Heintze et al. Preparation and structures of plasma – sprayed γ– and α– Al2O3 coatings Surf. Coat. Technol. (1992) Y. Chen et al. Microstructure and properties of Al2O3-ZrO2 composite coatings prepared by air plasma spraying Appl. Surf. Sci. (2018) S. Widjaja et al. Oxidation behavior of a plasma – sprayed functionally graded ZrO2/Al2O3 thermal barrier coating Mater. Lett. (2002) G.I. Vázquez et al. Microstructure and mechanical behavior of alumina – zirconia – mullite refractory materials Ceram. Int. (2012) V.Y. Dzyuzer Electrofused AZS refractories for high – capacity glass – founding furnaces Refract. Ind. Ceram. (2013) V.Y. Dzyuzer Features of initial heating of glass – founding furnaces Refract. Ind. Ceram. (2015) A. M. Guzmán, D. I. Martínez, R. González, Corrosion – erosion wear of refractory bricks in glass furnaces, Eng. Fail.... D. Sarkar, S. Adak, M. C. Chu, S. J. Cho, N. K. Mitra, Influence of ZrO2 on the thermo-mechanical response of nano-ZTA,... B. Liang, H. Liao, C. Ding, C. Coddet, Nanostructured zirconia – 30 vol.% alumina composite coatings deposited by... X. Song et al. Fabrication and characterization of amorphous alumina – Yttria – stabilized zirconia coatings by air plasma spraying J. Therm. Spray Technol. (2014) F. Tarasi, M. Medraj, A. Dolatabadi, J. Oberste – Berghaus, C. Moreau, Structural considerations in plasma spraying of... |
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Franco Correa, Iván David26c724b0-2de0-4689-87ea-a11c560018c9Ageorges, Hélène15bd62a4-bfb2-414e-b11d-7f11928d5f3aLópez Gómez, María Esperanza813f3de0-1e85-4e24-a98b-3e2a56fe2c86Vargas, Fabio Alonso9b445d6d-affe-4993-87d5-baa905637eda2023-05-15T21:24:22Z2023-05-15T21:24:22Z20210257-8972https://dspace.tdea.edu.co/handle/tdea/28841879-3347Se aplicaron dos recubrimientos de plasma atmosférico de ZrO 2 -Al 2 O 3 a un ladrillo refractario de aluminosilicato prensado y sinterizado , que se compararon con un refractario electrofundido de alúmina-zirconia-sílice (AZS) que se usa típicamente en la industria del vidrio por su resistencia a altas temperaturas. resistencia. Las muestras se sometieron a contacto deslizante mediante una prueba de bola en disco a 25, 500, 750 y 1000 °C y luego se realizaron caracterizaciones físicas, cristalográficas y mecánicas antes y después de las pruebas de desgaste para monitorear el desgaste . comportamiento. Ambos ZrO 2 -Al 2 O 3Los recubrimientos exhibieron un mejor comportamiento al desgaste que el refractario AZS electrofundido a todas las temperaturas evaluadas, debido a su alta dureza y tenacidad a la fractura , que se relacionaron principalmente con el aumento de las fases α-Al 2 O 3 y t-ZrO 2 a partir de γ-Al 2 O 3 y la cristalización de amorfofases respectivamente. De la misma manera, ambos recubrimientos también mostraron los mismos mecanismos de desgaste a todas las temperaturas evaluadas. A 25 °C se identificó desgaste por deformación dúctil, mientras que a 500 y 750 °C se produjo desgaste por deformación frágil, y a 1000 °C se evidenció la transición del desgaste de deformación frágil a dúctil. Para el refractario AZS electrofundido, hasta los 750 °C se desarrolló desgaste por deformación frágil, mientras que a 1000 °C se detectó desgaste por deformación tanto frágil como dúctil.image/jpegengElsevier BVSuizahttps://www.sciencedirect.com/science/article/abs/pii/S0257897221008896#preview-section-abstractAluminosilicatosMateriales refractariosRefractory materialsSilicatos de aluminioAluminum silicatesRecubrimientos de circona-alúminaZrO2-Al2O3Atmospheric plasma coatingsProyección térmicaThermal projectionWear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractoryArtículo 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_970fb48d4fbd8a85425Surface & coatings technologyP. Nayar et al. Structural, optical and mechanical properties of amorphous and crystalline alumina thin films Thin Solid Films (2014)T.E. Fischer et al. Genesis and role of wear debris in sliding wear of ceramics Wear (2000)M. Wang et al. Effects of the powder manufacturing method on microstructure and wear performance of plasma sprayed alumina – titania coatings Surf. Coat. Technol. (2007)F. Vargas et al. Mechanical and tribological performance of Al2O3-TiO2 coatings elaborated by flame and plasma spraying Surf. Coat. Technol. (2010)J.H. Ouyang et al. Microstructure and tribological characteristics of ZrO2 – Y2O3 ceramic coatings deposited by laser – assisted plasma hybrid spraying Tribol. Int. (2002)H. Chen et al. Tribological properties of nanostructured zirconia coatings deposited by plasma spraying Wear (2002)S. Heiroth et al. Optical and mechanical properties of amorphous and crystalline yttria-stabilized zirconia thin films prepared by pulsed laser deposition Acta Mater. (2011)J. Luo et al. Porosity-dependence of elastic moduli and hardness of 3Y-TZP ceramics Ceram. Int. (1999)K.A. Habib et al. Comparison of flame sprayed Al2O3/TiO2 coatings: their microstructure, mechanical properties and tribology behavior Surf. Coat. Technol. (2006)A. González et al. Efecto de la microestructura y de la microdureza sobre la resistencia al desgaste de recubrimientos elaborados por proyección térmica por plasma atmosférico a partir de circona – alúmina, circona – itria y circona – ceria Boletín de la Sociedad Española de Cerámica y Vidrio (2015)K. Sabiruddin et al. Analysis of phase transformation in plasma sprayed alumina coatings using Rietveld refinement Surf. Coat. Technol. (2010)G.N. Heintze et al. Preparation and structures of plasma – sprayed γ– and α– Al2O3 coatings Surf. Coat. Technol. (1992)Y. Chen et al. Microstructure and properties of Al2O3-ZrO2 composite coatings prepared by air plasma spraying Appl. Surf. Sci. (2018)S. Widjaja et al. Oxidation behavior of a plasma – sprayed functionally graded ZrO2/Al2O3 thermal barrier coating Mater. Lett. (2002)G.I. Vázquez et al. Microstructure and mechanical behavior of alumina – zirconia – mullite refractory materials Ceram. Int. (2012)V.Y. Dzyuzer Electrofused AZS refractories for high – capacity glass – founding furnaces Refract. Ind. Ceram. (2013)V.Y. Dzyuzer Features of initial heating of glass – founding furnaces Refract. Ind. Ceram. (2015)A. M. Guzmán, D. I. Martínez, R. González, Corrosion – erosion wear of refractory bricks in glass furnaces, Eng. Fail....D. Sarkar, S. Adak, M. C. Chu, S. J. Cho, N. K. Mitra, Influence of ZrO2 on the thermo-mechanical response of nano-ZTA,...B. Liang, H. Liao, C. Ding, C. Coddet, Nanostructured zirconia – 30 vol.% alumina composite coatings deposited by...X. Song et al. Fabrication and characterization of amorphous alumina – Yttria – stabilized zirconia coatings by air plasma spraying J. Therm. Spray Technol. (2014)F. Tarasi, M. Medraj, A. Dolatabadi, J. Oberste – Berghaus, C. Moreau, Structural considerations in plasma spraying of...info:eu-repo/semantics/closedAccesshttp://purl.org/coar/access_right/c_14cbORIGINALWear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory.jpgWear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory.jpgSolo datos del documentoimage/jpeg1630359https://dspace.tdea.edu.co/bitstream/tdea/2884/1/Wear%20behavior%20at%20high%20temperatures%20of%20ZrO2%c2%a0-%20Al2O3%c2%a0plasma%20sprayed%20coatings%20and%20an%20electro-melted%20AZS%20refractory.jpg29a58c95ed3a59f11f2f0865ca5e11ddMD51open accessLICENSElicense.txtlicense.txttext/plain; charset=utf-814828https://dspace.tdea.edu.co/bitstream/tdea/2884/2/license.txt2f9959eaf5b71fae44bbf9ec84150c7aMD52open accessTHUMBNAILWear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory.jpg.jpgWear behavior at high temperatures of ZrO2 - Al2O3 plasma sprayed coatings and an electro-melted AZS refractory.jpg.jpgGenerated Thumbnailimage/jpeg1757https://dspace.tdea.edu.co/bitstream/tdea/2884/3/Wear%20behavior%20at%20high%20temperatures%20of%20ZrO2%c2%a0-%20Al2O3%c2%a0plasma%20sprayed%20coatings%20and%20an%20electro-melted%20AZS%20refractory.jpg.jpg4535669a5c6111465cf60cf6d9a3015eMD53open accesstdea/2884oai:dspace.tdea.edu.co:tdea/28842023-05-16 03:01:02.588open accessRepositorio Institucional Tecnologico de 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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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