CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow
Polymer flooding is a widely used enhanced oil recovery (EOR) technology. The purpose of the polymer is to increase water viscosity to improve reservoir sweep efficiency. However, mechanical elements of the polymer injection facilities may impact the viscosity of the polymer negatively, decreasing i...
- Autores:
-
Herrera Quintero, Julia Jineth
Prada, Luis
Maya, Gustavo
VERGEL, JOSE
Castro Garcia, Ruben Hernan
QUINTERO, HENDERSON
Jiménez, Robinson
Pérez, Eduar
- 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/1673
- Acceso en línea:
- http://repositorio.ufps.edu.co/handle/ufps/1673
https://doi.org/10.29047/01225383.255
- Palabra clave:
- Computational Fluid-Dynamics
Mechanical Degradation
HPAM Polymeric solutions
Enhanced Oil Recovery
- Rights
- openAccess
- License
- (c) 2020 CT&F - Ciencia, Tecnología y Futuro
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CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow |
| dc.title.spa.fl_str_mv |
Simulación CFD de la degradación mecánica por restricciones en flujo turbulento de soluciones HPAM EOR |
| title |
CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow |
| spellingShingle |
CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow Computational Fluid-Dynamics Mechanical Degradation HPAM Polymeric solutions Enhanced Oil Recovery |
| title_short |
CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow |
| title_full |
CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow |
| title_fullStr |
CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow |
| title_full_unstemmed |
CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow |
| title_sort |
CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow |
| dc.creator.fl_str_mv |
Herrera Quintero, Julia Jineth Prada, Luis Maya, Gustavo VERGEL, JOSE Castro Garcia, Ruben Hernan QUINTERO, HENDERSON Jiménez, Robinson Pérez, Eduar |
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Herrera Quintero, Julia Jineth Prada, Luis Maya, Gustavo VERGEL, JOSE Castro Garcia, Ruben Hernan QUINTERO, HENDERSON Jiménez, Robinson Pérez, Eduar |
| dc.subject.proposal.eng.fl_str_mv |
Computational Fluid-Dynamics Mechanical Degradation HPAM Polymeric solutions Enhanced Oil Recovery |
| topic |
Computational Fluid-Dynamics Mechanical Degradation HPAM Polymeric solutions Enhanced Oil Recovery |
| description |
Polymer flooding is a widely used enhanced oil recovery (EOR) technology. The purpose of the polymer is to increase water viscosity to improve reservoir sweep efficiency. However, mechanical elements of the polymer injection facilities may impact the viscosity of the polymer negatively, decreasing it drastically. Mechanical degradation of the polymer occurs in case of flow restrictions with abrupt diameter changes in valves and control systems. Such flow restrictions may induce mechanical stresses along the polymer chain, which can result in its rupture. In this research, physical experiments and numerical simulations using CFD (Computational Fluid Dynamics) were used to propose a model for estimating the mechanical degradation for the flow of polymer solutions. This technique involves the calculation of velocity gradients, pressure drawdown, and polymer degradation of the fluid through geometry restriction. The simulations were validated through polymer injection experiments. The results show that with the greater volumetric flow and lower effective diameters, there is more mechanical degradation due to polymer shearing; nonetheless, this depends on the rheology properties inherent in each polymer in an aqueous solution. This method is suitable to estimate the mechanical degradation of the polymer solution in flooding facilities and accessories. Further, the results obtained could enhance the use of the polymer, calculating its actual mechanical degradation, minimizing it, or using it to support the development of new accessories. |
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2020 |
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2020-12-17 |
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2021-12-03T15:53:57Z |
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2021-12-03T15:53:57Z |
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Artículo de revista |
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https://doi.org/10.29047/01225383.255 |
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eng |
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eng |
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CT&F - Ciencia, Tecnología y Futuro |
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Vol.10 No.2.(2020) |
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129 |
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2(2020) |
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Herrera, J., Prada, L., Maya, G., Gomez, J. L., Castro, R., Quintero, H., Diaz, R., & Perez, E. (2020). CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow. CT&F - Ciencia, Tecnología Y Futuro, 10(2), 115-129. https://doi.org/10.29047/01225383.255 |
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CT&F - Ciencia, Tecnología y Futuro |
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(c) 2020 CT&F - Ciencia, Tecnología y Futuro |
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Atribución-NoComercial-CompartirIgual 4.0 Internacional (CC BY-NC-SA 4.0) |
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16 páginas |
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CT&F - Ciencia, Tecnología y Futuro |
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Colombia |
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Herrera Quintero, Julia Jineth 7384684079019dbf6f7b083b8e9c623c600Prada, Luis540a0a4155e709d6771021de479e5e5d600Maya, Gustavo27e0392fef57f2d01c4677fe93fc45b3600VERGEL, JOSE07f5e35123d8f50b6614313a454c0765600Castro Garcia, Ruben Hernan8fac01a98dbc9837f3b3c3850cbedfdd600QUINTERO, HENDERSONe94fb50ce8080d05a2e7d529b52e0429600Jiménez, Robinson0dfe1c3e0d71a31f96e859b810475f70600Pérez, Eduar 4f664f5393a466dce30a8fd6974e8f626002021-12-03T15:53:57Z2021-12-03T15:53:57Z2020-12-17http://repositorio.ufps.edu.co/handle/ufps/1673https://doi.org/10.29047/01225383.255Polymer flooding is a widely used enhanced oil recovery (EOR) technology. The purpose of the polymer is to increase water viscosity to improve reservoir sweep efficiency. However, mechanical elements of the polymer injection facilities may impact the viscosity of the polymer negatively, decreasing it drastically. Mechanical degradation of the polymer occurs in case of flow restrictions with abrupt diameter changes in valves and control systems. Such flow restrictions may induce mechanical stresses along the polymer chain, which can result in its rupture. In this research, physical experiments and numerical simulations using CFD (Computational Fluid Dynamics) were used to propose a model for estimating the mechanical degradation for the flow of polymer solutions. This technique involves the calculation of velocity gradients, pressure drawdown, and polymer degradation of the fluid through geometry restriction. The simulations were validated through polymer injection experiments. The results show that with the greater volumetric flow and lower effective diameters, there is more mechanical degradation due to polymer shearing; nonetheless, this depends on the rheology properties inherent in each polymer in an aqueous solution. This method is suitable to estimate the mechanical degradation of the polymer solution in flooding facilities and accessories. Further, the results obtained could enhance the use of the polymer, calculating its actual mechanical degradation, minimizing it, or using it to support the development of new accessories.La inyección de polímeros es un método de recobro de petróleo ampliamente utilizada. El propósito del polímero es incrementar la viscosidad del agua para mejorar la eficiencia de barrido, sin embargo, el paso del fluido por algunos equipos de las facilidades de inyección puede impactar la viscosidad del polímero, disminuyéndola drásticamente. La reducción de la viscosidad es debido a la degradación mecánica del polímero que ocurre en las restricciones del flujo donde hay cambios abruptos de diámetro como en válvulas y sistemas de control. Estas restricciones de flujo inducen altos esfuerzos mecánicos o de corte en la cadena del polímero, que pueden resultar en el rompimiento de estas.Experimentos y simulaciones numéricas usando Dinámica de Fluidos Computacional fueron realizadas para proponer un modelo que estime la tasa de degradación mecánica para el flujo de soluciones poliméricas, que involucran el cálculo de gradientes de velocidad, caídas de presión y degradaciones de polímero en el paso del fluido a través de geometrías de equipos que presentan restricciones al flujo. Las simulaciones fueron validadas mediante comparaciones con los resultados de las pruebas de laboratorio. Los resultados muestran que a mayores flujos volumétricos y menores diámetros efectivos de restricción se producen mayores degradaciones mecánicas por cizallamiento del polímero, sin embargo, esto depende de las propiedades reológicas propias de cada polímero en solución acuosa.El modelo desarrollado es muy útil para estimar la degradación mecánica del polímero en su paso por instalaciones y equipos de las facilidades de inyección, además los resultados obtenidos podrían optimizar el uso del polímero calculando la degradación mecánica real de cada polímero y minimizándola o como soporte en el diseño de nuevos equipos o accesorios con menor degradación mecánica.16 páginasapplication/pdfengCT&F - Ciencia, Tecnología y FuturoColombiaCT&F - Ciencia, Tecnología y FuturoVol.10 No.2.(2020)1292(2020)11510Herrera, J., Prada, L., Maya, G., Gomez, J. L., Castro, R., Quintero, H., Diaz, R., & Perez, E. (2020). CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flow. CT&F - Ciencia, Tecnología Y Futuro, 10(2), 115-129. https://doi.org/10.29047/01225383.255CT&F - Ciencia, Tecnología y Futuro(c) 2020 CT&F - Ciencia, Tecnología y Futuroinfo:eu-repo/semantics/openAccessAtribución-NoComercial-CompartirIgual 4.0 Internacional (CC BY-NC-SA 4.0)http://purl.org/coar/access_right/c_abf2https://ctyf.journal.ecopetrol.com.co/index.php/ctyf/article/view/255CFD simulation of HPAM EOR solutions mechanical degradation by restrictions in turbulent flowSimulación CFD de la degradación mecánica por restricciones en flujo turbulento de soluciones HPAM EORArtículo 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_970fb48d4fbd8a85Computational Fluid-DynamicsMechanical DegradationHPAM Polymeric solutionsEnhanced Oil RecoveryKing, M. J., and Dunayevsky, V. A. (1989). Why Waterflood Works: A Linearized Stability Analysis. Society of Petroleum Engineers. https://doi.org/10.2118/SPE-19648-MS.Zaitoun, A., Makakou, P., Blin, N., Al-Maamari, R. S., Al-Hashmi, A.-A. R., and Abdel-Goad, M. (2012). Shear Stability of EOR Polymers. Society of Petroleum Engineers. https://doi.org/10.2118/141113-PA.Maerker, J., 1976. Mechanical Degradation of Partially Hydrolyzed Polyacrylamide Solutions in Unconsolidated Porous Media. Society of Petroleum Engineers Journal, 16(04), pp. 172-174. https://doi.org/10.2118/5672-PANoik, C. H., Delaplace, P. H., and Muller, G. (1995). Physico-chemical characteristics of polyacrylamide solutions after mechanical degradation through a porous medium. In SPE International symposium on oilfield chemistry. Society of Petroleum Engineers. https://doi.org/10.2118/28954-MSSorbie, K., 1991. Polymer Improved Oil Recovery. Glasgow and London: Blackie and Son Ltd. https://doi.org/10.1007/978-94-011-3044-8Al Hashmi, A. R., Al Maamari, R. S., Al Shabibi, I. S., Mansoor, A. M., Zaitoun, A., and Al Sharji, H. H. (2013). Rheology and mechanical degradation of high-molecular-weight partially hydrolyzed polyacrylamide during flow through capillaries. Journal of Petroleum Science and Engineering, 105, 100-106. https://doi.org/10.1016/j.petrol.2013.03.021.Manrique, E., Ahmadi, M., Samani, S. (2017). Historical and recent observations in Polymer Floods: An Update Review.CT&F - Ciencia, Tecnología y Futuro, 6(5), 17 - 48. https://doi.org/10.29047/01225383.72.Morel, D. C., Jouenne, S., Vert, M., and Nahas, E. (2008). Polymer injection in deep offshore field: the Dalia Angola case. In SPE annual technical conference and exhibition. Society of Petroleum Engineers. https://doi.org/10.2118/116672-MS.Theriot, T. P., et al., 2018. Evaluation of Viscosity Loss of Viscosified Brine Solutions Due to Shear Degradation in Distribution System Components. Society of Petroleum Engineers, pp. SPE-190178-MS. https://doi.org/10.2118/190178-MS.Standnes, D. C. and Skjevrak, I., 2014. Literature review of implemented polymer field projects. Journal of Petroleum Science and Engineering, Volumen 122, pp. 761-775. https://doi.org/10.1016/j.petrol.2014.08.024.Stavland, A., Asen, S. M., Mebratu, A., and Gathier, F. (2016). Impact of Choke Valves on the IOR Polymer Flooding: Lessons Learned from Large Scale Tests. Proc., IOR. Norway, 18-22.Dupas, A., Henaut, I., Rousseau, D., Poulain, P., Tabary, R., Argillier, J. F., and Aubry, T. (2013). Impact of polymer mechanical degradation on shear and extensional viscosities: toward better injectivity forecasts in polymer flooding operations. In SPE international symposium on oilfield chemistry. Society of Petroleum Engineers. https://doi.org/10.2118/164083-MS.Jouenne, S., Chakibi, H., and Levitt, D. (2018). Polymer stability after successive mechanical-degradation events. SPE journal, 23 (01), 18-33. https://doi.org/10.2118/186103-PA.Culter, J. D., Zakin, J. L., and Patterson, G. K. (1975). Mechanical degradation of dilute solutions of high polymers in capillary tube flow. Journal of Applied Polymer Science, 19( 12), 3235-3240. https://doi.org/10.1002/app.1975.070191210.Binding, T., Phillips, P. and Phillips, T., 2006. Contraction/expansion flows: the pressure drop and related issue. J. Non-Newton. Fluid Mech., Volumen 137, pp. 31-38. https://doi.org/10.1016/j.jnnfm.2006.03.006.Gupta, R. and Sridhar, T., 1985. Viscoelastic effects in non-newtonian flows through porous media. Rheologica Acta, 24(2), pp. 148-151. https://doi.org/10.1007/BF01333242.Aguayo, J., Tamaddon-Jahromi, H. and Webster, M., 2008. Excess pressure-drop estimation in contraction and expansion flows for constant shear-viscosity, extension strain-hardening fluids. J. Non-Newtonian Fluid Mech. , Volumen 153, pp. 157-176. https://doi.org/10.1016/j.jnnfm.2008.05.004.Baloch, A., Townsend, P. and Webster, M., 1996. On vortex development in viscoelastic expansion and contraction flows. Journal of Non-newtonian Fluid Mechanics, 65 (2-3), pp. 133-149. https://doi.org/10.1016/0377-0257(96)01470-X.Oliveira, P. J., 2003. Asymmetric flows of viscoelastic fluids in symmetric planar expansion geometries. Journal of Non-newtonian Fluid Mechanics, 114(1), pp. 33-63. https://doi.org/10.1016/S0377-0257(03)00117-4.Missirlis, K., Assimacopoulos, D., and Mitsoulis, E., 1998. A finite volume approach in the simulation of viscoelastic expansion flows. Journal of Non-newtonian Fluid Mechanics, 78(), pp. 91-118. https://doi.org/10.1016/S0377-0257(98)00057-3.Walters, P. T. a. K., 1994. Expansion flows on non-newtonian liquids. Chemical Engineering Science, 49(5), pp. 748-763. https://doi.org/10.1016/0009-2509(94)85020-8.ANSYS fluent 18.1. ANSYS, Canonsburg, PA (2017).Castro, R., Maya, G., Jimenez R., Quintero, H., Díaz, V., Colmenares, K., Palma J., Delgadillo, C., and Perez, R.(2016). Polymer flooding to improve volumetric sweep efficiency in waterflooding processes. CT y F - Ciencia, Tecnologia y Futuro. 6(3).pp 71-90. https://doi.org/10.29047/01225383.10.Bestul, A. B. (1956). Kinetics of capillary shear degradation in concentrated polymer solutions. The Journal of Chemical Physics, 24(6), 1196-1201. https://doi.org/10.1063/1.1742739.RP63, A. P. I. (1990). Recommended Practices for Evaluation of Polymers Used in API RP63. Recommended Practices for Evaluation of Polymers Used in enhanced oil recovery operations. Washington.MATLAB and Statistics Toolbox Release 2012b, The MathWorks, Inc., Natick, Massachusetts, United States.Fluent, A. N. S. Y. S. 16.2: Fluent Theory Guide. ANSYS Help Viewer.Wang, D., Cheng, J., Yang, Q., Wenchao, G., Qun, L., and Chen, F. (2000). Viscous-elastic polymer can increase microscale displacement efficiency in cores. In SPE annual technical conference and exhibition. Society of Petroleum Engineers. https://doi.org/10.2118/63227-MS.Culter, J. D., Zakin, J. L., and Patterson, G. K. (1975). Mechanical degradation of dilute solutions of high polymers in capillary tube flow. 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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.
0000-0001-5544-6593540a0a4155e709d6771021de479e5e5d6000000-0002-4177-442Xe94fb50ce8080d05a2e7d529b52e0429600 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