Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress
Designing cams by Bézier Curves has become increasingly common, since the mathematical development of this method is less complex. Bezier curves are Bernstein-based polynomials under a unitary domain, and in that sense, this article presents the design of a cam using Bezier curves of degrees 5, 7 an...
- Autores:
-
Acevedo Peñaloza, Carlos Humberto
Ramón Ramón, Sergio Andrés
Bustos Urbano, Víctor Jhoel
- 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/1103
- Acceso en línea:
- http://repositorio.ufps.edu.co/handle/ufps/1103
http://dx.doi.org/10.18273/revuin.v19n4-2020002
- Palabra clave:
- Bezier curves
cam design
distortion energy
Von Mises stress
cam-follower mechanism
Bernstein base polynomials
contact theory
curvas de Bézier
diseño de levas
energía de distorsión;
esfuerzo de Von Mises;
polinomios de base Bernstein
teoría de contacto
- Rights
- openAccess
- License
- CC BY-ND 4.0
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Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress |
| dc.title.spa.fl_str_mv |
Uso de las curvas de Bezier en el diseño de la ley de desplazamiento del mecanismo de leva - seguidor: esfuerzo efectivo de Von Mises |
| title |
Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress |
| spellingShingle |
Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress Bezier curves cam design distortion energy Von Mises stress cam-follower mechanism Bernstein base polynomials contact theory curvas de Bézier diseño de levas energía de distorsión; esfuerzo de Von Mises; polinomios de base Bernstein teoría de contacto |
| title_short |
Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress |
| title_full |
Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress |
| title_fullStr |
Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress |
| title_full_unstemmed |
Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress |
| title_sort |
Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress |
| dc.creator.fl_str_mv |
Acevedo Peñaloza, Carlos Humberto Ramón Ramón, Sergio Andrés Bustos Urbano, Víctor Jhoel |
| dc.contributor.author.none.fl_str_mv |
Acevedo Peñaloza, Carlos Humberto Ramón Ramón, Sergio Andrés Bustos Urbano, Víctor Jhoel |
| dc.subject.proposal.eng.fl_str_mv |
Bezier curves cam design distortion energy Von Mises stress cam-follower mechanism Bernstein base polynomials contact theory |
| topic |
Bezier curves cam design distortion energy Von Mises stress cam-follower mechanism Bernstein base polynomials contact theory curvas de Bézier diseño de levas energía de distorsión; esfuerzo de Von Mises; polinomios de base Bernstein teoría de contacto |
| dc.subject.proposal.spa.fl_str_mv |
curvas de Bézier diseño de levas energía de distorsión; esfuerzo de Von Mises; polinomios de base Bernstein teoría de contacto |
| description |
Designing cams by Bézier Curves has become increasingly common, since the mathematical development of this method is less complex. Bezier curves are Bernstein-based polynomials under a unitary domain, and in that sense, this article presents the design of a cam using Bezier curves of degrees 5, 7 and 9. And beyond, this article seeks to show the variation of the effective effort of Von Mises in a cam-follower mechanism composed of a disc cam and a roller follower with translation movement and force closure. The expressions that allow determining the variation of Von Mises' effort for each of the curves used are presented. This variation is presented by means of graphs in which it is observed that as the degree of the curve increases, the magnitude of the efforts is greater, and this increases the probability of failure in the mechanisms. In addition, it was found that there is an inverse relationship between the stress and the radius of the primary circle of the cam. |
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2020 |
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2020-07-01 |
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2021-11-18T21:20:13Z |
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2021-11-18T21:20:13Z |
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Artículo de revista |
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eng |
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Vol.19 No.4.(2020) |
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Acevedo-Peñaloza, C. H., Ramón-Ramón, S. A., & Bustos-Urbano, V. J. (2020). Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress. Revista UIS Ingenierías, 19(4), 19-26. |
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Revista UIS Ingenierías |
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Acevedo Peñaloza, Carlos Humberto1f12a99f8d5bcc67d1eb10c7c07c76a3600Ramón Ramón, Sergio Andrésa99d8c5df65c36476bfda5ed281cbfd5600 Bustos Urbano, Víctor Jhoel fb27e064ee73b90c23f2dd8aa19685d76002021-11-18T21:20:13Z2021-11-18T21:20:13Z2020-07-011657-4583http://repositorio.ufps.edu.co/handle/ufps/11032145-8456http://dx.doi.org/10.18273/revuin.v19n4-2020002Designing cams by Bézier Curves has become increasingly common, since the mathematical development of this method is less complex. Bezier curves are Bernstein-based polynomials under a unitary domain, and in that sense, this article presents the design of a cam using Bezier curves of degrees 5, 7 and 9. And beyond, this article seeks to show the variation of the effective effort of Von Mises in a cam-follower mechanism composed of a disc cam and a roller follower with translation movement and force closure. The expressions that allow determining the variation of Von Mises' effort for each of the curves used are presented. This variation is presented by means of graphs in which it is observed that as the degree of the curve increases, the magnitude of the efforts is greater, and this increases the probability of failure in the mechanisms. In addition, it was found that there is an inverse relationship between the stress and the radius of the primary circle of the cam.Diseñar levas por Curvas de Bézier se ha hecho cada vez más frecuente, puesto que el desarrollo matemático de este método es menos complejo. Las curvas de Bézier son polinomios de base Bernstein bajo un dominio unitario, y en ese sentido, este artículo presenta el diseño de una leva se mediante curvas Bézier de grados 5, 7 y 9. Y más allá, este artículo busca mostrar la variación del esfuerzo efectivo de Von Mises en un mecanismo leva-seguidor compuesto por una leva de disco y un seguidor de rodillo con movimiento de traslación y cierre de fuerza. Se plantean las expresiones que permiten determinar la variación del esfuerzo de Von Mises para cada una de las curvas utilizadas. Esta variación se presenta mediante gráficos en los que se observa que a medida que aumenta el grado de la curva, la magnitud de los esfuerzos es mayor y esto aumenta la probabilidad de fallas en los mecanismos. Además, se encontró que hay una relación inversa entre el esfuerzo y el radio del círculo primario de la leva.07 páginasapplication/pdfengRevista UIS IngenieríasColombiaRevista UIS IngenieríasVol.19 No.4.(2020)264(2020)1919Acevedo-Peñaloza, C. H., Ramón-Ramón, S. A., & Bustos-Urbano, V. J. (2020). Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective Stress. Revista UIS Ingenierías, 19(4), 19-26.Revista UIS IngenieríasCC BY-ND 4.0info:eu-repo/semantics/openAccessAtribución-SinDerivadas 4.0 Internacional (CC BY-ND 4.0)http://purl.org/coar/access_right/c_abf2https://revistas.uis.edu.co/index.php/revistauisingenierias/article/view/10751Use of Bézier curves in the design of the displacement law of the cam-follower mechanism: Von Mises effective StressUso de las curvas de Bezier en el diseño de la ley de desplazamiento del mecanismo de leva - seguidor: esfuerzo efectivo de Von MisesArtículo 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_970fb48d4fbd8a85Bezier curvescam designdistortion energyVon Mises stresscam-follower mechanismBernstein base polynomialscontact theorycurvas de Bézierdiseño de levasenergía de distorsión;esfuerzo de Von Mises;polinomios de base Bernsteinteoría de contactoR. C. Juvinall, Engineering Considerations of Stress, Strain, and Strength, New York: McGraw-Hill, 1967.A. Torabi, S. Akbarzadeh, M. R. Salimpour, M. Khonsari, “On the running-in behavior of cam-follower mechanism,” Tribology International, vol. 118, pp. 301- 313, 2018, doi: 10.1016/j.triboint.2017.09.034C. H. Acevedo Peñaloza, “Estudio del ángulo de presión y de la presión de contacto en mecanismos leva palpador cuya ley de desplazamiento se diseña por curvas de Bézier,” tesis doctoral, Universidad Politécnica de Cataluña, Barcelona, 2005.F. P. Beer, E. R. J. Jonhnston, J. T. DeWolf, D. F. Mazurek, Mecánica de Materiales, México D.F.: McGraw-Hill, 2010.O. A. González-Estrada, S. Natarajan, C. Graciano, “Reconstrucción de tensiones para el método de elementos finitos con mallas poligonales,” Rev. UIS Ingenierías, vol. 16, no. 1, pp. 23-34, 2017, doi: 10.18273/revuin.v16n1-2017003T. T. Nga Nguyen, S. Kurtenbach, M. Hüsing, B. Corves, “A general framework for motion design of the follower in cam mechanisms by using non-uniform rational B-spline,” Mechanism and Machine Theory, vol. 137, pp. 374-385, 2019, doi: 10.1016/j.mechmachtheory.2019.03.029M. Shirzadegan, A. Almqvist, R. Larsson, “Fully coupled EHL model for simulation of finite length line cam-roller follower contacts,” Tribology International, vol. 103, pp. 584-598, 2016, doi: 10.1016/j.triboint.2016.08.017C. H. Acevedo Peñaloza, E. Zayas Figueras, S. Cardona Foix, “Introducción al diseño de perfil de levas por Curvas de Bézier,” Respuestas, vol. 9, no. 1, pp. 39- 44, 2004.G. N. Băsescu, I. V. Crîșmaru, S. I. Strugaru, . C. Paulin, E. S. Bârcă, C. Munteanu, “The Stress Distribution of a Layered Contact Cam Mechanism Using Finite Element,” Advanced Materials Research, vol. 837, pp. 316-321, 2014, doi: 10.4028/www.scientific.net/AMR.837.316H. F. Quintero, L. Vanegas, “Use of the VAP function in the design of cam-follower mechanisms,” Ingeniería y Competitividad, vol. 18, no. 2, pp. 207-216, 2016, doi: 10.25100/iyc.v18i2.2169M. Hidalgo Martínez, E. Sanmiguel Rojas, and M. A. Burgos Olmos, “Design of cams with negative radius follower using Bézier curves,” Mechanism and Machine Theory, vol. 82, pp. 87-96, 2014, doi: 10.1016/j.mechmachtheory.2014.08.001S. C. Foix and D. C. Costa, Teoria de Màquines, Barcelona: Ediciones UPC, 2000.J. F. Olmedo Salazar, E. A. Vasconez Endara, B. H. Culqui Culqui, M. T. Piovan, “Aplicación de Curvas de Bézier en el diseño y optimización de levas para alta velocidad,” Ciencia, vol. 20, no. 2, pp. 144 -159, 2018, doi: 10.24133/ciencia.v20i2.1212R. L. Norton, Cam design and manufacturing handbook, New York: Industrial Press, Inc., 2009.S. P. Timoshenko and J. N. Goodier, Theory of Elasticity, New York: McGraw-Hill, 1970.M. Dežman and A. Gams, “Rotatable cam-based variable-ratio lever compliant actuator for wearable devices,” Mechanism and Machine Theory, vol. 130, pp. 508-522, 2018, doi: 10.1016/j.mechmachtheory.2018.09.006A. Ponter, M. Engelhardt, “Shakedown limits for a general yield condition: implementation and application for a Von Mises yield condition,” European Journal of Mechanics - A/Solids, vol. 19, no. 3, pp. 423 - 445, 2000, doi: 10.1016/S0997-7538(00)00171-6C. Acevedo Peñaloza, S. Ramón Ramón, G. Prada Botia, “Comparison of the Concentration Factor of Stresses on Flat Sheets with Two Holes with Low and High Speed Voltage Test,” Contemporary Engineering Sciences, vol. 11, no. 55, pp. 2707 - 2714, 2018, doi: 10.12988/ces.2018.86288ORIGINALUso de las curvas de Bezier en el diseño de la ley de desplazamiento del mecanismo de leva - seguidor esfuerzo efectivo de Von Mises.pdfUso de las curvas de Bezier en el diseño de la ley de desplazamiento del mecanismo de leva - seguidor esfuerzo efectivo de Von Mises.pdfapplication/pdf501948https://repositorio.ufps.edu.co/bitstream/ufps/1103/1/Uso%20de%20las%20curvas%20de%20Bezier%20en%20el%20dise%c3%b1o%20de%20la%20ley%20de%20desplazamiento%20del%20mecanismo%20de%20leva%20-%20seguidor%20esfuerzo%20efectivo%20de%20Von%20Mises.pdfbe2d1ea67e897bdb789b6335158d81c8MD51open accessLICENSElicense.txtlicense.txttext/plain; charset=utf-814828https://repositorio.ufps.edu.co/bitstream/ufps/1103/2/license.txt2f9959eaf5b71fae44bbf9ec84150c7aMD52open accessTEXTUso de las curvas de Bezier en el diseño de la ley de desplazamiento del mecanismo de leva - seguidor esfuerzo efectivo de Von Mises.pdf.txtUso de las curvas de Bezier en el diseño de la ley de desplazamiento del mecanismo de leva - seguidor esfuerzo efectivo de Von Mises.pdf.txtExtracted texttext/plain21092https://repositorio.ufps.edu.co/bitstream/ufps/1103/3/Uso%20de%20las%20curvas%20de%20Bezier%20en%20el%20dise%c3%b1o%20de%20la%20ley%20de%20desplazamiento%20del%20mecanismo%20de%20leva%20-%20seguidor%20esfuerzo%20efectivo%20de%20Von%20Mises.pdf.txt8187f1b8703753f8850f95bbd4b62b8eMD53open accessTHUMBNAILUso de las curvas de Bezier en el diseño de la ley de desplazamiento del mecanismo de leva - seguidor esfuerzo efectivo de Von Mises.pdf.jpgUso de las curvas de Bezier en el diseño de la ley de desplazamiento del mecanismo de leva - seguidor esfuerzo efectivo de Von Mises.pdf.jpgGenerated 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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.
0000-0002-5049-87541f12a99f8d5bcc67d1eb10c7c07c76a36000000-0002-1310-9182a99d8c5df65c36476bfda5ed281cbfd56000000-0001-6954-2260fb27e064ee73b90c23f2dd8aa19685d7600 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