Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene
This work describes the production and characterization of a composite material based on magnetite filled HDPE, which is commonly known for its magnetic properties. Composites of this kind are used in different applications such as microwave absorption, transducers and biomedical applications like d...
- Autores:
-
Garzón, Andrés
Landínez, David A.
Roa-Rojas, Jairo
Fajardo Tolosa, Fabio Enrique
Peña Rodriguez, Gabriel
Parra-Vargas, C.A
- Tipo de recurso:
- Article of journal
- Fecha de publicación:
- 2017
- Institución:
- Universidad Francisco de Paula Santander
- Repositorio:
- Repositorio Digital UFPS
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.ufps.edu.co:ufps/681
- Acceso en línea:
- http://repositorio.ufps.edu.co/handle/ufps/681
https://doi.org/10.18257/raccefyn.422
- Palabra clave:
- High density polyethylene
Magnetite
Plastic composites
Structural properties electric properties
Magnetic properties
Polietileno de alta densidad
Magnetita
Materiales plásticos compuestos
Propiedades estructurales
Propiedades eléctricas
Propiedades magnéticas
- Rights
- openAccess
- License
- Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0)
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dc.title.spa.fl_str_mv |
Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene |
dc.title.translated.none.fl_str_mv |
Producción y caracterización estructural, eléctrica y magnética de un material compuesto a base de magnetita pulverizada y polietileno de alta densidad. |
title |
Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene |
spellingShingle |
Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene High density polyethylene Magnetite Plastic composites Structural properties electric properties Magnetic properties Polietileno de alta densidad Magnetita Materiales plásticos compuestos Propiedades estructurales Propiedades eléctricas Propiedades magnéticas |
title_short |
Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene |
title_full |
Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene |
title_fullStr |
Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene |
title_full_unstemmed |
Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene |
title_sort |
Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene |
dc.creator.fl_str_mv |
Garzón, Andrés Landínez, David A. Roa-Rojas, Jairo Fajardo Tolosa, Fabio Enrique Peña Rodriguez, Gabriel Parra-Vargas, C.A |
dc.contributor.author.none.fl_str_mv |
Garzón, Andrés Landínez, David A. Roa-Rojas, Jairo Fajardo Tolosa, Fabio Enrique Peña Rodriguez, Gabriel Parra-Vargas, C.A |
dc.subject.proposal.eng.fl_str_mv |
High density polyethylene Magnetite Plastic composites Structural properties electric properties Magnetic properties |
topic |
High density polyethylene Magnetite Plastic composites Structural properties electric properties Magnetic properties Polietileno de alta densidad Magnetita Materiales plásticos compuestos Propiedades estructurales Propiedades eléctricas Propiedades magnéticas |
dc.subject.proposal.spa.fl_str_mv |
Polietileno de alta densidad Magnetita Materiales plásticos compuestos Propiedades estructurales Propiedades eléctricas Propiedades magnéticas |
description |
This work describes the production and characterization of a composite material based on magnetite filled HDPE, which is commonly known for its magnetic properties. Composites of this kind are used in different applications such as microwave absorption, transducers and biomedical applications like drug delivery, organs tagging, etc. The samples were produced according to different volume ratios of magnetite and HDPE. The semiquantitative analysis conducted by XRD revealed the presence of hematite within the mineral magnetite used as a filler in the composites. The crystallinity degree was calculated through X-ray diffraction tests. The XRD results showed how there is an amorphous-crystalline transition due to the magnetite increasing content. The crystallinity percent (χc ) for samples filled with 40% of magnetite volume was 90% while the (χc ) for samples filled with 10% of magnetite volume was 80%. Which may be related to the increased magnetite particles into the plastic matrix for reinforcement contents up to 30% by volume, as evidenced in the images obtained through scanning electron microscopy (SEM). The samples were electrically characterized through volume resistivity measurements and electric polarization. The results showed that for ratios less than the 20% of magnetite there is no substantial reduction in the resistivity of the composite samples compared to the unfilled HDPE samples, but for magnetite ratios above 30% the composite samples showed a substantial reduction of six orders of magnitude in their volumetric resistivity. The electric polarization showed how the composite material undergoes a transition, going from an insulating material (for samples with 10% of magnetite volume) to a resistive material where the current and voltage are in phase (for samples with 30% and 40% of magnetite volume). The magnetization curves showed that the saturation magnetization (from 17,3 to 60,5 emu/g) and remanence (from 0,94 to 5 emu/g) increase in samples with high magnetite contents. The presence of the hematite phase in the samples could have affected the magnetization saturation and the remanence values in the hysteresis curves. Magnetization curves as a function of temperature showed the Verwey samples transition around the 120K and confirmed that the magnetization increases as the magnetite volume within the matrix increases. © 2017. Acad. Colomb. Cienc. Ex. Fis. Nat. |
publishDate |
2017 |
dc.date.issued.none.fl_str_mv |
2017-06-30 |
dc.date.accessioned.none.fl_str_mv |
2021-11-05T20:01:47Z |
dc.date.available.none.fl_str_mv |
2021-11-05T20:01:47Z |
dc.type.spa.fl_str_mv |
Artículo de revista |
dc.type.coar.fl_str_mv |
http://purl.org/coar/resource_type/c_2df8fbb1 |
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_6501 |
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_6501 |
status_str |
publishedVersion |
dc.identifier.uri.none.fl_str_mv |
http://repositorio.ufps.edu.co/handle/ufps/681 |
dc.identifier.doi.none.fl_str_mv |
https://doi.org/10.18257/raccefyn.422 |
url |
http://repositorio.ufps.edu.co/handle/ufps/681 https://doi.org/10.18257/raccefyn.422 |
dc.language.iso.spa.fl_str_mv |
eng |
language |
eng |
dc.relation.ispartof.none.fl_str_mv |
Revista De La Academia Colombiana De Ciencias Exactas, Físicas Y Naturales |
dc.relation.citationedition.spa.fl_str_mv |
Vol.41 No.159.(2017) |
dc.relation.citationendpage.spa.fl_str_mv |
167 |
dc.relation.citationissue.spa.fl_str_mv |
159 (2017) |
dc.relation.citationstartpage.spa.fl_str_mv |
154 |
dc.relation.citationvolume.spa.fl_str_mv |
41 |
dc.relation.cites.none.fl_str_mv |
Garzón, A. O., Landínez, D. A., Roa-Rojas, J., Fajardo-Tolosa, F. E., Peña-Rodríguez, G., & Parra-Vargas, C. A. (2017). Producción y caracterización estructural, eléctrica y magnética de un material compuesto a base de magnetita pulverizada y polietileno de alta densidad. RACCEFYN, 41(159), 154–167. https://doi.org/10.18257/raccefyn.422 |
dc.relation.ispartofjournal.spa.fl_str_mv |
Revista De La Academia Colombiana De Ciencias Exactas, Físicas Y Naturales |
dc.rights.coar.fl_str_mv |
http://purl.org/coar/access_right/c_abf2 |
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) |
eu_rights_str_mv |
openAccess |
rights_invalid_str_mv |
Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0) http://purl.org/coar/access_right/c_abf2 |
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application/pdf |
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Revista De La Academia Colombiana De Ciencias Exactas, Físicas Y Naturales |
dc.publisher.place.spa.fl_str_mv |
Colombia |
dc.source.spa.fl_str_mv |
https://raccefyn.co/index.php/raccefyn/article/view/422 |
institution |
Universidad Francisco de Paula Santander |
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Garzón, Andrés5f235907d9dc243af6d549c09e702abf600Landínez, David A.06817f63b9fb4e9c2880e362e8ee3e69Roa-Rojas, Jairo07f67cd42f02e686a14bccff900b3b5f600Fajardo Tolosa, Fabio Enriquea870ee7a8450d4aed3baaf030c8db662600Peña Rodriguez, Gabriel4eaba0408a3f49f82929dc957fa8eee1600Parra-Vargas, C.A3cbb2fdafb4522eb5413387d9bd2f1ef2021-11-05T20:01:47Z2021-11-05T20:01:47Z2017-06-30http://repositorio.ufps.edu.co/handle/ufps/681https://doi.org/10.18257/raccefyn.422This work describes the production and characterization of a composite material based on magnetite filled HDPE, which is commonly known for its magnetic properties. Composites of this kind are used in different applications such as microwave absorption, transducers and biomedical applications like drug delivery, organs tagging, etc. The samples were produced according to different volume ratios of magnetite and HDPE. The semiquantitative analysis conducted by XRD revealed the presence of hematite within the mineral magnetite used as a filler in the composites. The crystallinity degree was calculated through X-ray diffraction tests. The XRD results showed how there is an amorphous-crystalline transition due to the magnetite increasing content. The crystallinity percent (χc ) for samples filled with 40% of magnetite volume was 90% while the (χc ) for samples filled with 10% of magnetite volume was 80%. Which may be related to the increased magnetite particles into the plastic matrix for reinforcement contents up to 30% by volume, as evidenced in the images obtained through scanning electron microscopy (SEM). The samples were electrically characterized through volume resistivity measurements and electric polarization. The results showed that for ratios less than the 20% of magnetite there is no substantial reduction in the resistivity of the composite samples compared to the unfilled HDPE samples, but for magnetite ratios above 30% the composite samples showed a substantial reduction of six orders of magnitude in their volumetric resistivity. The electric polarization showed how the composite material undergoes a transition, going from an insulating material (for samples with 10% of magnetite volume) to a resistive material where the current and voltage are in phase (for samples with 30% and 40% of magnetite volume). The magnetization curves showed that the saturation magnetization (from 17,3 to 60,5 emu/g) and remanence (from 0,94 to 5 emu/g) increase in samples with high magnetite contents. The presence of the hematite phase in the samples could have affected the magnetization saturation and the remanence values in the hysteresis curves. Magnetization curves as a function of temperature showed the Verwey samples transition around the 120K and confirmed that the magnetization increases as the magnetite volume within the matrix increases. © 2017. Acad. Colomb. Cienc. Ex. Fis. Nat.Se describe la producción y caracterización de un material compuesto basado en matrices de polietileno de alta densidad (HDPE) reforzadas con magnetita pulverizada. Compuestos de este tipo son usados para diferentes aplicaciones como la fabricación de escudos de absorción electromagnética, transductores, entrega focalizada de medicamentos, marcación de órganos, etc. Las muestras fueron producidas de acuerdo a diferentes proporciones en volumen de magnetita y HDPE. Los análisis semicuantitativos llevados a cabo por medio de DRX dejan en evidencia la presencia de hematita al interior de la magnetita mineral usada como refuerzo del compuesto. El porcentaje de cristalinidad de los compuestos se calculó a través de difracción de rayos X. Los resultados de la difracción mostraron una transición amorfo-cristalino del compuesto, debida al creciente contenido de magnetita al interior de la matriz. El porcentaje de cristalinidad (χc) de las muestras reforzadas con un 40% en volumen de magnetita fue del 90% mientras que para las muestras reforzadas con el 10% en volumen la cristalinidad fue del 80%. Esto puede estar ligado a la mayor proliferación de partículas de magnetita al interior de la matriz plástica para contenidos de refuerzo superiores al 30% en volumen, tal y como se evidenció en las imágenes obtenidas a través de microscopía electrónica de barrido (SEM). Las muestras fueron eléctricamente caracterizadas a través de medidas de resistividad volumétrica y polarización eléctrica. Los resultados mostraron que para proporciones del refuerzo de magnetita iguales o inferiores al 20% no hay una reducción substancial en la resistividad de los compuestos comparada con la del polietileno sin reforzar. En cambio, para proporciones de magnetita iguales o superiores al 30% en volumen los compuestos muestran una reducción en la resistividad de hasta seis ordenes de magnitud. La polarización eléctrica deja en evidencia como el material compuesto presenta una transición al pasar de ser completamente aislante (10% en volumen de magnetita) a ser un material resistivo donde la corriente y el voltaje se encuentran en fase (muestras reforzadas con 30%-40% de volumen de magnetita). Las curvas de histéresis magnética en función del campo aplicado muestran un incremento constante en la magnetización de saturación (de 17,3 a 60,5 emu/g) y en la magnetización remanente (de 0.94 emu/g a 5 emu/g), al aumentarse el contenido de magnetita en las muestras. La presencia de hematita en las muestras pudo haber afectado los valores de la magnetización de saturación y de remanencia en las curvas de histéresis magnética. Las curvas de magnetización en función de la temperatura dejan en evidencia la transición de Verwey de la magnetita alrededor de los 120K, a la vez que confirman el aumento en la magnetización de las muestras conforme el contenido del refuerzo aumenta al interior de la matriz. © 2017. Acad. Colomb. Cienc. Ex. Fis. Nat.application/pdfengRevista De La Academia Colombiana De Ciencias Exactas, Físicas Y NaturalesColombiaRevista De La Academia Colombiana De Ciencias Exactas, Físicas Y NaturalesVol.41 No.159.(2017)167159 (2017)15441Garzón, A. O., Landínez, D. A., Roa-Rojas, J., Fajardo-Tolosa, F. E., Peña-Rodríguez, G., & Parra-Vargas, C. A. (2017). Producción y caracterización estructural, eléctrica y magnética de un material compuesto a base de magnetita pulverizada y polietileno de alta densidad. RACCEFYN, 41(159), 154–167. https://doi.org/10.18257/raccefyn.422Revista De La Academia Colombiana De Ciencias Exactas, Físicas Y NaturalesEsta obra está bajo una licencia internacional Creative Commons Atribución-NoComercial-SinDerivadas 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://raccefyn.co/index.php/raccefyn/article/view/422Production and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethyleneProducción y caracterización estructural, eléctrica y magnética de un material compuesto a base de magnetita pulverizada y polietileno de alta densidad.Artículo 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_970fb48d4fbd8a85High density polyethyleneMagnetitePlastic compositesStructural properties electric propertiesMagnetic propertiesPolietileno de alta densidadMagnetitaMateriales plásticos compuestosPropiedades estructuralesPropiedades eléctricasPropiedades magnéticasBoettcher, C J F. (1952). Theory of electric polarization. Amsterdam: Elsevier.Bohra M., Prasad S, Venketaramani N, Kumar N, Sahoo S C, Krishnan R. (2009). Magnetic properties of magnetite thin films close to the Verwey transition. Journal of Magnetism and Magnetic Materials. 321 (22): 3738-3741.Bruggeman, D A G. (1935). Berechnung verschieddener physikalischer konstanten von heterogenen Substanzen. Ann Phys. 24: 636-664.Buschow, K H J. (2014). Handbook of Magnetic Materials. North Holland: Elsevier B.V.Carporzen L, Gilder S A, Hart R J. (2006). Origin and implications of two Verwey transitions in the basement rocks of the Vredefort meteorite crater, South Africa. Earth and Planetary Science Letters. 251 (3-4): 305-317.Costa A L, Ballarin B, Spegni A, Casoli F, Gardini D. (2012). Synthesis of nanostructured magnetic photocatalyst by colloidal approach and spray–drying technique. Journal of colloid and interface science. 388 (1): 31-39.Demir A, Baykal A, Sözeri H, Topkaya R. (2014). 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Journal of magnetism and magnetic materials. 224 (1): 39-48.TEXTProduction and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene.pdf.txtProduction and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene.pdf.txtExtracted texttext/plain71653https://repositorio.ufps.edu.co/bitstream/ufps/681/3/Production%20and%20structural%2c%20electrical%20and%20magnetic%20characterization%20of%20a%20composite%20material%20based%20on%20powdered%20magnetite%20and%20high%20density%20polyethylene.pdf.txt8cce05ddfbe65783209f3d85bcaf62d3MD53open accessTHUMBNAILProduction and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high density polyethylene.pdf.jpgProduction and structural, electrical and magnetic characterization of a composite material based on powdered magnetite and high 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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.
0000-0002-3364-03925f235907d9dc243af6d549c09e702abf6000000-0002-5080-849207f67cd42f02e686a14bccff900b3b5f6000000-0002-5452-7559a870ee7a8450d4aed3baaf030c8db662600 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