Evaluation of surface hardness of NiCr coating using finite elements analysis

Introduction— To enhance resistance to surface damage of materials due to mechanical actions, there have been created many procedures that allow its modification for different needs. This leads to researches conducted to determine the changes achieved in the properties due to said procedures. One me...

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Autores:
Fuentes Rueda, Lauren Camila
Campillo Carreño, Diego Andres
Calderón, Luis
Martínez, Manuel Del Jesús
Tipo de recurso:
Article of journal
Fecha de publicación:
2021
Institución:
Corporación Universidad de la Costa
Repositorio:
REDICUC - Repositorio CUC
Idioma:
eng
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Acceso en línea:
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https://repositorio.cuc.edu.co/
Palabra clave:
Hardness test
Finite elements
Composite material
Coating
Simulation
Ensayo de dureza
Elementos finitos
Material compuesto
Recubrimiento
Simulación
Rights
openAccess
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Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0)
id RCUC2_7438af04a605d97509f88463b58f125a
oai_identifier_str oai:repositorio.cuc.edu.co:11323/10335
network_acronym_str RCUC2
network_name_str REDICUC - Repositorio CUC
repository_id_str
dc.title.eng.fl_str_mv Evaluation of surface hardness of NiCr coating using finite elements analysis
dc.title.translated.none.fl_str_mv Evaluación de la dureza superficial del recubrimiento de NiCr mediante el análisis de elementos finitos
title Evaluation of surface hardness of NiCr coating using finite elements analysis
spellingShingle Evaluation of surface hardness of NiCr coating using finite elements analysis
Hardness test
Finite elements
Composite material
Coating
Simulation
Ensayo de dureza
Elementos finitos
Material compuesto
Recubrimiento
Simulación
title_short Evaluation of surface hardness of NiCr coating using finite elements analysis
title_full Evaluation of surface hardness of NiCr coating using finite elements analysis
title_fullStr Evaluation of surface hardness of NiCr coating using finite elements analysis
title_full_unstemmed Evaluation of surface hardness of NiCr coating using finite elements analysis
title_sort Evaluation of surface hardness of NiCr coating using finite elements analysis
dc.creator.fl_str_mv Fuentes Rueda, Lauren Camila
Campillo Carreño, Diego Andres
Calderón, Luis
Martínez, Manuel Del Jesús
dc.contributor.author.none.fl_str_mv Fuentes Rueda, Lauren Camila
Campillo Carreño, Diego Andres
Calderón, Luis
Martínez, Manuel Del Jesús
dc.subject.proposal.eng.fl_str_mv Hardness test
Finite elements
Composite material
Coating
Simulation
topic Hardness test
Finite elements
Composite material
Coating
Simulation
Ensayo de dureza
Elementos finitos
Material compuesto
Recubrimiento
Simulación
dc.subject.proposal.spa.fl_str_mv Ensayo de dureza
Elementos finitos
Material compuesto
Recubrimiento
Simulación
description Introduction— To enhance resistance to surface damage of materials due to mechanical actions, there have been created many procedures that allow its modification for different needs. This leads to researches conducted to determine the changes achieved in the properties due to said procedures. One method commonly applied is, for example, physical means of vapor deposition of thin films on a surface. In recent years, many rational and empirical models have been proposed for the study of said properties. One of these models is computational analysis, which allows determining a great number of properties while avoiding applying destructive tests, achieving to reduce experimental time spent and costs of manufacture of test tubes as well as the test itself. In this research, the hardness of a surface coating of Nichrome (NiCr 80-20) was determined with an indentation test modeled in Ansys, based on the finite elements’ method. Objective— To design a computational model that allows determining the surface hardness of material with coating Methodology— The realization of this project was made with the software for engineering analysis ANSYS, and the model was made based on the Vickers Indentation Test regulation given by the ASTM, which states that the test must be done with a pyramidal diamond indenter, applying forces greater than 1 kgf. Results— By running the respective numerical analysis for both the substrate and the coating, a surface hardness of 197.5073 VH was obtained for NiCr coating and surface hardness of 160.5809 VH for the S235 Steel (hardness of the interface). Conclusions— It was determined that the model proposed is correct seeing as the values obtained for the Vickers’ Hardness is approximately the same as the experimental value with an error of 0.7501% for the coating layer and 0.2605% for the substrate. It was also concluded that it is possible to use this same procedure to obtain the surface hardness for different materials than those treated in this article by using this tool.
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dc.date.accessioned.none.fl_str_mv 2023-07-21T21:03:47Z
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dc.identifier.citation.spa.fl_str_mv L. Fuentes Rueda, D. Campillo Carreño & L. Calderón Vergel, “ Evaluation of surface hardness of NiCr coating using Finite Elements Analysis”, INGECUC, vol. 17. no. 1, pp. 329–339. DOI: http://doi.org/10.17981/ingecuc.17.1.2021.24
dc.identifier.issn.spa.fl_str_mv 0122-6517
dc.identifier.uri.none.fl_str_mv https://hdl.handle.net/11323/10335
dc.identifier.doi.none.fl_str_mv 10.17981/ingecuc.17.1.2021.24
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dc.identifier.instname.spa.fl_str_mv Corporación Universidad de la Costa
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identifier_str_mv L. Fuentes Rueda, D. Campillo Carreño & L. Calderón Vergel, “ Evaluation of surface hardness of NiCr coating using Finite Elements Analysis”, INGECUC, vol. 17. no. 1, pp. 329–339. DOI: http://doi.org/10.17981/ingecuc.17.1.2021.24
0122-6517
10.17981/ingecuc.17.1.2021.24
2382-4700
Corporación Universidad de la Costa
REDICUC - Repositorio CUC
url https://hdl.handle.net/11323/10335
https://repositorio.cuc.edu.co/
dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.ispartofjournal.spa.fl_str_mv INGE CUC
dc.relation.references.spa.fl_str_mv [1] Eurocode.com, “Table of design material properties for structural steel,” eurocodeapplied.com, [online], 1993. Available: https://www.eurocodeapplied.com/design/en1993/steel-design-properties
[2] N. F. Ak, C. Tekmen, I. Ozdemir, H. S. Soykan & E. Celik, “NiCr coatings on stainless steel by HVOF technique,” Surf Coat Technol, vol. 174-175, pp. 1070–1073, Sep. 2003. https://doi.org/10.1016/S0257- 8972(03)00367-0
[3] G. Faraji, H. S. Kim, & H. T. Kashi, “Chapter 7 - Mechanical Properties of Ultrafine-Grained and Nanostructured Metals,” in Severe Plastic Deformation, THR, IRN: Elsevier, pp. 223–257, 2018.
[4] Z.-Q. Chen, H. Niu, D. Li & Y. Li, “Modeling hardness of polycrystalline materials and bulk metallic glasses,” Intermetallics, vol. 19, no. 9, pp. 1275–1281, Sep. 2011. https://doi.org/10.1016/j.intermet.2011.03.026
[5] J. Gong, J. Wu & Z. Guan, “Examination of the indentation size effect in low-load vickers hardness testing of ceramics,” J Eur Ceram Soc, vol. 19, no. 15, pp. 2625–2631, Nov. 1999. https://doi.org/10.1016/ S0955-2219(99)00043-6
[6] J. M. Antunes, L. F. Menezes, & J. V. Fernande, “Three-dimensional numerical simulation of Vickers indentation tests,” Inter J Solids Struct, no. 43, pp. 784–806, 2006. https://doi.org/10.1016/j.ijsolstr.2005.02.048
[7] A. Harish, “Finite Element Method – What Is It? FEM and FEA Explained”, simscale blog, Oct. 2020. Available: https://www.simscale.com/blog/2016/10/what-is-finite-element-method/
[8] J. Zottis, C. A. T. Soares Diehl & A. da S. Roch, “Evaluation of experimentally observed asymmetric distributions of hardness, strain and residual stress in cold drawn bars by FEM-simulation,” J Mater Res Technol, vol. 7, no. 4, pp. 469–478, 2018. https://doi.org/10.1016/j.jmrt.2018.01.004
[9] W. Han, K. Kuepper, P. Hou, W. Akram & H. Eickmeier, “Free-Sustaining Three-Dimensional S235 Steel-Based Porous Electrocatalyst for Highly Efficient and Durable Oxygen Evolution,” ChemSusChem, vol. 11, no. 20, pp. 3661–3671,Oct. 2018. https://doi.org/10.1002/cssc.201801351
[10] H. Schäfer, K. Küpper, J. Wollshläger, N. Kashavae, J. Hardege, L. Walder, S. M. Beladi-Mousavi, B. Hartmann-Azanza, M. Steinhart, S. Sadaf & F. Dorn, “Oxidized Mild Steel S235: An Efficient Anode for Electrocatalytically Initiated Water Splitting,” ChemSusChem, vol. 8, no. 18, pp. 3099–3110, Sep. 2015. https://doi.org/10.1002/cssc.201500666
[11] G. Marot, M. Martínez & J. Lesage, Modelado Computacional de un Ensayo Interfacial de Dos Materiales, 2007.
[12] Designation E92-17: Standard Test Methods for Vickers Hardness and Knoop Hardness of Metallic Materials, ASTM E92, ASTM, 2017. https://doi.org/10.1520/E0092-17
[13] D. R. Askenland, Ciencia e Ingeniería de los Materiales, 7 ed, BOS, USA: Cengage Learning, 2016.
[14] A. Singh, K. Ramachandra & A. R. Devarhubli, “Evaluation and comparison of shear bond strength o porcelain to a beryllium-free alloy of nickel-chromium, nickel and beryllium free alloy of cobalt-chromium, and titanium: An in vitro study,” J Indian Prosthodont Socv, vol. 17, no. 3, pp. 261–266, 2017. https://doi.org/10.4103/jips.jips_337_16
[15] SharcNet, “Ansys (Application),” sharcnet.ca, [online], 2016. Available: https://www.sharcnet.ca/my/ software/show/22
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dc.rights.spa.fl_str_mv Derechos de autor 2021 INGE CUC
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https://creativecommons.org/licenses/by-nc-nd/4.0/
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spelling Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0)Derechos de autor 2021 INGE CUChttps://creativecommons.org/licenses/by-nc-nd/4.0/info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2Fuentes Rueda, Lauren CamilaCampillo Carreño, Diego AndresCalderón, Luis Martínez, Manuel Del Jesús2023-07-21T21:03:47Z2023-07-21T21:03:47Z2021L. Fuentes Rueda, D. Campillo Carreño & L. Calderón Vergel, “ Evaluation of surface hardness of NiCr coating using Finite Elements Analysis”, INGECUC, vol. 17. no. 1, pp. 329–339. DOI: http://doi.org/10.17981/ingecuc.17.1.2021.240122-6517https://hdl.handle.net/11323/1033510.17981/ingecuc.17.1.2021.242382-4700Corporación Universidad de la CostaREDICUC - Repositorio CUChttps://repositorio.cuc.edu.co/Introduction— To enhance resistance to surface damage of materials due to mechanical actions, there have been created many procedures that allow its modification for different needs. This leads to researches conducted to determine the changes achieved in the properties due to said procedures. One method commonly applied is, for example, physical means of vapor deposition of thin films on a surface. In recent years, many rational and empirical models have been proposed for the study of said properties. One of these models is computational analysis, which allows determining a great number of properties while avoiding applying destructive tests, achieving to reduce experimental time spent and costs of manufacture of test tubes as well as the test itself. In this research, the hardness of a surface coating of Nichrome (NiCr 80-20) was determined with an indentation test modeled in Ansys, based on the finite elements’ method. Objective— To design a computational model that allows determining the surface hardness of material with coating Methodology— The realization of this project was made with the software for engineering analysis ANSYS, and the model was made based on the Vickers Indentation Test regulation given by the ASTM, which states that the test must be done with a pyramidal diamond indenter, applying forces greater than 1 kgf. Results— By running the respective numerical analysis for both the substrate and the coating, a surface hardness of 197.5073 VH was obtained for NiCr coating and surface hardness of 160.5809 VH for the S235 Steel (hardness of the interface). Conclusions— It was determined that the model proposed is correct seeing as the values obtained for the Vickers’ Hardness is approximately the same as the experimental value with an error of 0.7501% for the coating layer and 0.2605% for the substrate. It was also concluded that it is possible to use this same procedure to obtain the surface hardness for different materials than those treated in this article by using this tool.Introducción— Para mejorar la resistencia al daño superficial de los materiales debido a acciones mecánicas, se han creado muchos procedimientos que permiten su modificación para diferentes necesidades. Esto hace que se realicen investigaciones para determinar los cambios logrados en las propiedades debido a dichos procedimientos. Uno de los métodos comúnmente aplicados es, por ejemplo, los medios físicos de deposición de vapor de películas delgadas sobre una superficie. En los últimos años se han propuesto muchos modelos racionales y empíricos para el estudio de dichas propiedades. Uno de estos modelos es el análisis computacional, que permite determinar un gran número de propiedades evitando la aplicación de ensayos destructivos, consiguiendo reducir el tiempo experimental empleado y los costes de fabricación de las probetas, así como el propio ensayo. En esta investigación se determinó la dureza de un recubrimiento superficial de Nichrome (NiCr 80-20) con un ensayo de indentación modelado en Ansys, basado en el método de elementos finitos. Objetivo— Diseñar un modelo computacional que permita determinar la dureza superficial de un material con recubrimiento. Metodología— La realización de este proyecto se hizo con el software de análisis de ingeniería ANSYS, y el modelo se hizo con base en la norma de ensayo de indentación Vickers dada por la ASTM, la cual establece que el ensayo debe hacerse con un indentador de diamante piramidal, aplicando fuerzas mayores a 1 kgf. Resultados— Al ejecutar el respectivo análisis numérico tanto para el sustrato como para el recubrimiento, se obtuvo una dureza superficial de 197.5073 VH para el recubrimiento de NiCr y una dureza superficial de 160,5809 VH para el Acero S235 (dureza de la interfase). Conclusiones— Se determinó que el modelo propuesto es correcto ya que los valores obtenidos para la Dureza Vickers es aproximadamente igual al valor experimental con un error de 0.7501% para la capa de recubrimiento y 0.2605% para el sustrato. También se concluyó que es posible utilizar este mismo procedimiento para obtener la dureza superficial para materiales diferentes a los tratados en este artículo utilizando esta herramienta.11 páginasapplication/pdfengCorporación Universidad de la CostaColombiahttps://revistascientificas.cuc.edu.co/ingecuc/article/view/3249Evaluation of surface hardness of NiCr coating using finite elements analysisEvaluación de la dureza superficial del recubrimiento de NiCr mediante el análisis de elementos finitosArtículo 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_970fb48d4fbd8a85INGE CUC[1] Eurocode.com, “Table of design material properties for structural steel,” eurocodeapplied.com, [online], 1993. Available: https://www.eurocodeapplied.com/design/en1993/steel-design-properties[2] N. F. Ak, C. Tekmen, I. Ozdemir, H. S. Soykan & E. Celik, “NiCr coatings on stainless steel by HVOF technique,” Surf Coat Technol, vol. 174-175, pp. 1070–1073, Sep. 2003. https://doi.org/10.1016/S0257- 8972(03)00367-0[3] G. Faraji, H. S. Kim, & H. T. Kashi, “Chapter 7 - Mechanical Properties of Ultrafine-Grained and Nanostructured Metals,” in Severe Plastic Deformation, THR, IRN: Elsevier, pp. 223–257, 2018.[4] Z.-Q. Chen, H. Niu, D. Li & Y. Li, “Modeling hardness of polycrystalline materials and bulk metallic glasses,” Intermetallics, vol. 19, no. 9, pp. 1275–1281, Sep. 2011. https://doi.org/10.1016/j.intermet.2011.03.026[5] J. Gong, J. Wu & Z. Guan, “Examination of the indentation size effect in low-load vickers hardness testing of ceramics,” J Eur Ceram Soc, vol. 19, no. 15, pp. 2625–2631, Nov. 1999. https://doi.org/10.1016/ S0955-2219(99)00043-6[6] J. M. Antunes, L. F. Menezes, & J. V. Fernande, “Three-dimensional numerical simulation of Vickers indentation tests,” Inter J Solids Struct, no. 43, pp. 784–806, 2006. https://doi.org/10.1016/j.ijsolstr.2005.02.048[7] A. Harish, “Finite Element Method – What Is It? FEM and FEA Explained”, simscale blog, Oct. 2020. Available: https://www.simscale.com/blog/2016/10/what-is-finite-element-method/[8] J. Zottis, C. A. T. Soares Diehl & A. da S. Roch, “Evaluation of experimentally observed asymmetric distributions of hardness, strain and residual stress in cold drawn bars by FEM-simulation,” J Mater Res Technol, vol. 7, no. 4, pp. 469–478, 2018. https://doi.org/10.1016/j.jmrt.2018.01.004[9] W. Han, K. Kuepper, P. Hou, W. Akram & H. Eickmeier, “Free-Sustaining Three-Dimensional S235 Steel-Based Porous Electrocatalyst for Highly Efficient and Durable Oxygen Evolution,” ChemSusChem, vol. 11, no. 20, pp. 3661–3671,Oct. 2018. https://doi.org/10.1002/cssc.201801351[10] H. Schäfer, K. Küpper, J. Wollshläger, N. Kashavae, J. Hardege, L. Walder, S. M. Beladi-Mousavi, B. Hartmann-Azanza, M. Steinhart, S. Sadaf & F. Dorn, “Oxidized Mild Steel S235: An Efficient Anode for Electrocatalytically Initiated Water Splitting,” ChemSusChem, vol. 8, no. 18, pp. 3099–3110, Sep. 2015. https://doi.org/10.1002/cssc.201500666[11] G. Marot, M. Martínez & J. Lesage, Modelado Computacional de un Ensayo Interfacial de Dos Materiales, 2007.[12] Designation E92-17: Standard Test Methods for Vickers Hardness and Knoop Hardness of Metallic Materials, ASTM E92, ASTM, 2017. https://doi.org/10.1520/E0092-17[13] D. R. Askenland, Ciencia e Ingeniería de los Materiales, 7 ed, BOS, USA: Cengage Learning, 2016.[14] A. Singh, K. Ramachandra & A. R. Devarhubli, “Evaluation and comparison of shear bond strength o porcelain to a beryllium-free alloy of nickel-chromium, nickel and beryllium free alloy of cobalt-chromium, and titanium: An in vitro study,” J Indian Prosthodont Socv, vol. 17, no. 3, pp. 261–266, 2017. https://doi.org/10.4103/jips.jips_337_16[15] SharcNet, “Ansys (Application),” sharcnet.ca, [online], 2016. Available: https://www.sharcnet.ca/my/ software/show/22339329117Hardness testFinite elementsComposite materialCoatingSimulationEnsayo de durezaElementos finitosMaterial compuestoRecubrimientoSimulaciónPublicationORIGINALEvaluation of surface hardness of NiCr coating using Finite Elements Analysis.pdfEvaluation of surface hardness of NiCr coating using Finite Elements Analysis.pdfArtículoapplication/pdf613276https://repositorio.cuc.edu.co/bitstreams/62608cfd-df52-45ca-883a-60a3e0ab43cb/download6b3464e9e33123940ede0f6b08ded843MD51LICENSElicense.txtlicense.txttext/plain; charset=utf-814828https://repositorio.cuc.edu.co/bitstreams/5ede0c86-fef4-4c41-a7a2-c711aece713c/download2f9959eaf5b71fae44bbf9ec84150c7aMD52TEXTEvaluation of surface hardness of NiCr coating using Finite Elements Analysis.pdf.txtEvaluation of surface hardness of NiCr coating using Finite Elements Analysis.pdf.txtExtracted 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ada 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.
