Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration

This study presents detailed thermodynamic modeling of a supercritical Brayton cycle operating with carbon dioxide as a working fluid for electric power generation. The study incorporates a main compression intercooling configuration while elucidating the effect of operational parameters on the over...

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Autores:
Orjuela Abril, Martha Sofia
Bustos Urbano, Víctor Jhoel
PABON LEON, JHON ANTUNY
Tipo de recurso:
Article of investigation
Fecha de publicación:
2021
Institución:
Universidad Francisco de Paula Santander
Repositorio:
Repositorio Digital UFPS
Idioma:
eng
OAI Identifier:
oai:repositorio.ufps.edu.co:ufps/6553
Acceso en línea:
https://repositorio.ufps.edu.co/handle/ufps/6553
https://doi.org/10.1088/1742-6596/1938/1/012010
Palabra clave:
Brayton cycle
Carbon dioxide
Electric power generation
Electric power plants
Exergy
Iterative methods
Particle swarm optimization (PSO)
Working fluids
Convergence criterion
Energy and exergy efficiency
Exergy destructions
Operational parameters
Optimization methodology
Supercritical carbon dioxides
Thermodynamic model
Thermodynamic studies
Supercritical fluid extraction
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openAccess
License
Content from this work may be used under the terms of theCreative Commons Attribution 3.0 licence
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dc.title.eng.fl_str_mv Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration
title Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration
spellingShingle Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration
Brayton cycle
Carbon dioxide
Electric power generation
Electric power plants
Exergy
Iterative methods
Particle swarm optimization (PSO)
Working fluids
Convergence criterion
Energy and exergy efficiency
Exergy destructions
Operational parameters
Optimization methodology
Supercritical carbon dioxides
Thermodynamic model
Thermodynamic studies
Supercritical fluid extraction
title_short Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration
title_full Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration
title_fullStr Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration
title_full_unstemmed Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration
title_sort Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration
dc.creator.fl_str_mv Orjuela Abril, Martha Sofia
Bustos Urbano, Víctor Jhoel
PABON LEON, JHON ANTUNY
dc.contributor.author.none.fl_str_mv Orjuela Abril, Martha Sofia
Bustos Urbano, Víctor Jhoel
PABON LEON, JHON ANTUNY
dc.contributor.corporatename.spa.fl_str_mv Journal of Physics: Conference Series
dc.subject.proposal.eng.fl_str_mv Brayton cycle
Carbon dioxide
Electric power generation
Electric power plants
Exergy
Iterative methods
Particle swarm optimization (PSO)
Working fluids
Convergence criterion
Energy and exergy efficiency
Exergy destructions
Operational parameters
Optimization methodology
Supercritical carbon dioxides
Thermodynamic model
Thermodynamic studies
Supercritical fluid extraction
topic Brayton cycle
Carbon dioxide
Electric power generation
Electric power plants
Exergy
Iterative methods
Particle swarm optimization (PSO)
Working fluids
Convergence criterion
Energy and exergy efficiency
Exergy destructions
Operational parameters
Optimization methodology
Supercritical carbon dioxides
Thermodynamic model
Thermodynamic studies
Supercritical fluid extraction
description This study presents detailed thermodynamic modeling of a supercritical Brayton cycle operating with carbon dioxide as a working fluid for electric power generation. The study incorporates a main compression intercooling configuration while elucidating the effect of operational parameters on the overall performance based on energy and exergy perspectives. The model was carefully validated with relevant authors. Moreover, two different optimization methodologies, namely particle swarm optimization and fmincom, are evaluated based on convergence criteria. The results demonstrated that the fmincom reduced the iteration time between 140 s - 180 s. The cycle pressure played a central role in the stability of the thermophysical properties of the working fluid. The energy and exergy efficiencies present a direct relation with the inlet temperature. The air cooling and regenerators represent the biggest contributor to exergy destruction, whereas the compressors featured minimal impact on the exergy degeneration. Overall, the proposed configuration demonstrated robust performance to implement with high-grade heat sources, especially in non-interconnected areas.
publishDate 2021
dc.date.issued.none.fl_str_mv 2021-06-09
dc.date.accessioned.none.fl_str_mv 2022-11-19T13:46:13Z
dc.date.available.none.fl_str_mv 2022-11-19T13:46:13Z
dc.type.spa.fl_str_mv Artículo de revista
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dc.type.content.spa.fl_str_mv Text
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dc.identifier.uri.none.fl_str_mv https://repositorio.ufps.edu.co/handle/ufps/6553
dc.identifier.doi.none.fl_str_mv https://doi.org/10.1088/1742-6596/1938/1/012010
url https://repositorio.ufps.edu.co/handle/ufps/6553
https://doi.org/10.1088/1742-6596/1938/1/012010
dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.ispartof.none.fl_str_mv Journal of Physics: Conference Series. Vol.1938 N°.1. (2021)
dc.relation.citationedition.spa.fl_str_mv Vol. 1938 N°.1. (2021)
dc.relation.citationendpage.spa.fl_str_mv 7
dc.relation.citationissue.spa.fl_str_mv 1(2021)
dc.relation.citationstartpage.spa.fl_str_mv 1
dc.relation.citationvolume.spa.fl_str_mv 1938
dc.relation.cites.none.fl_str_mv Abril, M. O., Urbano, V. B., & León, J. P. (2021, May). Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration. In Journal of Physics: Conference Series (Vol. 1938, No. 1, p. 012010). IOP Publishing.
dc.relation.ispartofjournal.spa.fl_str_mv Journal of Physics: Conference Series
dc.rights.eng.fl_str_mv Content from this work may be used under the terms of theCreative Commons Attribution 3.0 licence
dc.rights.coar.fl_str_mv http://purl.org/coar/access_right/c_abf2
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rights_invalid_str_mv Content from this work may be used under the terms of theCreative Commons Attribution 3.0 licence
https://creativecommons.org/licenses/by/4.0/
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eu_rights_str_mv openAccess
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dc.publisher.spa.fl_str_mv Journal of Physics: Conference Series
dc.publisher.place.spa.fl_str_mv Reino Unido
dc.source.spa.fl_str_mv https://iopscience.iop.org/article/10.1088/1742-6596/1938/1/012010/pdf
institution Universidad Francisco de Paula Santander
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spelling Orjuela Abril, Martha Sofia c7eb007995ff675aa1fb2ed07939a53e600 Bustos Urbano, Víctor Jhoel fb27e064ee73b90c23f2dd8aa19685d7600PABON LEON, JHON ANTUNY2adb8fd3199076e6826e922ebbf380bd600Journal of Physics: Conference Series2022-11-19T13:46:13Z2022-11-19T13:46:13Z2021-06-09https://repositorio.ufps.edu.co/handle/ufps/6553https://doi.org/10.1088/1742-6596/1938/1/012010This study presents detailed thermodynamic modeling of a supercritical Brayton cycle operating with carbon dioxide as a working fluid for electric power generation. The study incorporates a main compression intercooling configuration while elucidating the effect of operational parameters on the overall performance based on energy and exergy perspectives. The model was carefully validated with relevant authors. Moreover, two different optimization methodologies, namely particle swarm optimization and fmincom, are evaluated based on convergence criteria. The results demonstrated that the fmincom reduced the iteration time between 140 s - 180 s. The cycle pressure played a central role in the stability of the thermophysical properties of the working fluid. The energy and exergy efficiencies present a direct relation with the inlet temperature. The air cooling and regenerators represent the biggest contributor to exergy destruction, whereas the compressors featured minimal impact on the exergy degeneration. Overall, the proposed configuration demonstrated robust performance to implement with high-grade heat sources, especially in non-interconnected areas.07 páginasapplication/pdfengJournal of Physics: Conference SeriesReino UnidoJournal of Physics: Conference Series. Vol.1938 N°.1. (2021)Vol. 1938 N°.1. (2021)71(2021)11938Abril, M. O., Urbano, V. B., & León, J. P. (2021, May). Thermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configuration. In Journal of Physics: Conference Series (Vol. 1938, No. 1, p. 012010). IOP Publishing.Journal of Physics: Conference SeriesContent from this work may be used under the terms of theCreative Commons Attribution 3.0 licencehttps://creativecommons.org/licenses/by/4.0/info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2https://iopscience.iop.org/article/10.1088/1742-6596/1938/1/012010/pdfThermodynamic study of a supercritical carbon dioxide Brayton cycle based on main compression intercooling configurationArtículo de revistahttp://purl.org/coar/resource_type/c_2df8fbb1Textinfo:eu-repo/semantics/articlehttp://purl.org/redcol/resource_type/ARTinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/version/c_970fb48d4fbd8a85Brayton cycleCarbon dioxideElectric power generationElectric power plantsExergyIterative methodsParticle swarm optimization (PSO)Working fluidsConvergence criterionEnergy and exergy efficiencyExergy destructionsOperational parametersOptimization methodologySupercritical carbon dioxidesThermodynamic modelThermodynamic studiesSupercritical fluid extractionConsuegra F, Bula A, Guillín W, Sánchez J, Duarte Forero J 2019 Energies 12(8) 1437Valencia Ochoa G, Isaza-Roldan C, Duarte Forero J 2020 Energies 13(6) 1317Valencia Ochoa G, Cárdenas Gutierrez J, Duarte Forero J 2020 Resources 9(1) 2Orozco W, Acuña N, Duarte J 2019 International Review of Mechanical Engineering 13(7) 420Duarte J, Garcia J, Jiménez J, Sanjuan M, Bula A, González J 2017 Journal of Energy Resources Technology 139(2) 022201:1Obregon L, Valencia G, Duarte Forero J 2019 International Review on Modelling and Simulations 12(4) 245Alibaba M, Pourdarbani R, Manesh M H K, Ochoa G V, Forero J D 2020 Heliyon 6(4) e03758Orozco T, Herrera M, Duarte Forero J 2019 CFD Study of heat exchangers applied in brayton cycles: A case study in supercritical condition using carbon dioxide as working fluid Int. Rev. Model. Simulations 12(2) 72Chu W, Bennett K, Cheng J, Chen Y, Wang Q 2019 Numerical study on a novel hyperbolic inlet header in straight-channel printed circuit heat exchanger Appl. Therm. Eng. 146(5) 805Padilla R V, Soo Too Y C, Benito R, Stein W 2015 Exergetic analysis of supercritical CO2 Brayton cycles integrated with solar central receivers Applied Energy 148 348Diaz G A, et al. 2017 Journal of Energy Resources Technology 139(3) 032903Marchionni M, Chai L, Bianchi G, Tassou S A 2019 Applied Thermal Engineering 161(1) 114190Duarte Forero J, López Taborda J, Bula Silvera A 2019 International Review of Mechanical Engineering 13(1) 11Sharma O P, Kaushik S C, Manjunath K 2017 Thermal Science and Engineering Progress 3(1) 62Iglesias Garcia S, Ferreiro Garcia R, Carbia Carril J, Iglesias Garcia D 2017 Energy Conversion and Management 148(1) 844Sarkar J 2009 Energy 34(9) 1172ORIGINALOrjuela_Abril_2021_J._Phys.__Conf._Ser._1938_012010.pdfOrjuela_Abril_2021_J._Phys.__Conf._Ser._1938_012010.pdfapplication/pdf883981https://repositorio.ufps.edu.co/bitstream/ufps/6553/1/Orjuela_Abril_2021_J._Phys.__Conf._Ser._1938_012010.pdf302cd4cbf8b18ff220120f6bb000ad47MD51open 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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.
0000-0002-9742-8673c7eb007995ff675aa1fb2ed07939a53e6000000-0001-6954-2260fb27e064ee73b90c23f2dd8aa19685d76000000-0002-1078-28572adb8fd3199076e6826e922ebbf380bd600