Determining the limits of geometrical tortuosity from seepage flow calculations in porous media
Recent investigations have found a distinct correlation of effective properties of porous media to sigmoidal functions, where one axis is the Reynolds number Re and the other is the effective property dependent of Re, Θ = S (Re) -- One of these properties is tortuosity -- At very low Re (seepage flo...
- Autores:
-
Uribe, David
Osorno, María
Sivanesapillai, Rakulan
Steeb, Holger
Ruíz, Óscar
- Tipo de recurso:
- Fecha de publicación:
- 2014
- Institución:
- Universidad EAFIT
- Repositorio:
- Repositorio EAFIT
- Idioma:
- eng
- OAI Identifier:
- oai:repository.eafit.edu.co:10784/9666
- Acceso en línea:
- http://hdl.handle.net/10784/9666
- Palabra clave:
- MATERIALES POROSOS
DISTRIBUCIÓN DE GAUSS
ASÍNTOTAS
NÚMERO DE REYNOLDS
Porous materials
Gauss distribution
Asymptotes
Reynolds number
Porous materials
Gauss distribution
Asymptotes
Reynolds number
Función sigmoide
Factor de Tortuosidad
Algoritmo de esqueletización
- Rights
- License
- Acceso cerrado
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|
dc.title.eng.fl_str_mv |
Determining the limits of geometrical tortuosity from seepage flow calculations in porous media |
title |
Determining the limits of geometrical tortuosity from seepage flow calculations in porous media |
spellingShingle |
Determining the limits of geometrical tortuosity from seepage flow calculations in porous media MATERIALES POROSOS DISTRIBUCIÓN DE GAUSS ASÍNTOTAS NÚMERO DE REYNOLDS Porous materials Gauss distribution Asymptotes Reynolds number Porous materials Gauss distribution Asymptotes Reynolds number Función sigmoide Factor de Tortuosidad Algoritmo de esqueletización |
title_short |
Determining the limits of geometrical tortuosity from seepage flow calculations in porous media |
title_full |
Determining the limits of geometrical tortuosity from seepage flow calculations in porous media |
title_fullStr |
Determining the limits of geometrical tortuosity from seepage flow calculations in porous media |
title_full_unstemmed |
Determining the limits of geometrical tortuosity from seepage flow calculations in porous media |
title_sort |
Determining the limits of geometrical tortuosity from seepage flow calculations in porous media |
dc.creator.fl_str_mv |
Uribe, David Osorno, María Sivanesapillai, Rakulan Steeb, Holger Ruíz, Óscar |
dc.contributor.department.spa.fl_str_mv |
Universidad EAFIT. Departamento de Ingeniería Mecánica |
dc.contributor.author.none.fl_str_mv |
Uribe, David Osorno, María Sivanesapillai, Rakulan Steeb, Holger Ruíz, Óscar |
dc.contributor.researchgroup.spa.fl_str_mv |
Laboratorio CAD/CAM/CAE |
dc.subject.lemb.spa.fl_str_mv |
MATERIALES POROSOS DISTRIBUCIÓN DE GAUSS ASÍNTOTAS NÚMERO DE REYNOLDS |
topic |
MATERIALES POROSOS DISTRIBUCIÓN DE GAUSS ASÍNTOTAS NÚMERO DE REYNOLDS Porous materials Gauss distribution Asymptotes Reynolds number Porous materials Gauss distribution Asymptotes Reynolds number Función sigmoide Factor de Tortuosidad Algoritmo de esqueletización |
dc.subject.keyword.spa.fl_str_mv |
Porous materials Gauss distribution Asymptotes Reynolds number |
dc.subject.keyword.eng.fl_str_mv |
Porous materials Gauss distribution Asymptotes Reynolds number |
dc.subject.keyword..keywor.fl_str_mv |
Función sigmoide Factor de Tortuosidad Algoritmo de esqueletización |
description |
Recent investigations have found a distinct correlation of effective properties of porous media to sigmoidal functions, where one axis is the Reynolds number Re and the other is the effective property dependent of Re, Θ = S (Re) -- One of these properties is tortuosity -- At very low Re (seepage flow), there is a characteristic value of tortuosity, and it is the upper horizontal asymptote of the sigmoidal function -- With higher values of Re (transient flow) the tortuosity value decreases, until a lower asymptote is reached (turbulent flow) -- Estimations of this parameter have been limited to the low Reynolds regime in the study of porous media -- The current state of the art presents different numerical measurements of tortuosity, such as skeletization, centroid binding, and arc length of streamlines -- These are solutions for the low Re regime. So far, for high Re, only the arc length of stream lines has been used to calculate tortuosity -- The present approach involves the simulation of fluid flow in large domains and high Re, which requires numerous resources, and often presents convergence problems -- In response to this, we propose a geometrical method to estimate the limit of tortuosity of porous media at Re → ∞, from the streamlines calculated at low Re limit -- We test our method by calculating the tortuosity limits in a fibrous porous media, and comparing the estimated values with numerical benchmark results -- Ongoing work includes the geometric estimation of different intrinsic properties of porous media |
publishDate |
2014 |
dc.date.issued.none.fl_str_mv |
2014 |
dc.date.available.none.fl_str_mv |
2016-11-18T21:53:09Z |
dc.date.accessioned.none.fl_str_mv |
2016-11-18T21:53:09Z |
dc.type.eng.fl_str_mv |
info:eu-repo/semantics/article article info:eu-repo/semantics/publishedVersion publishedVersion |
dc.type.coarversion.fl_str_mv |
http://purl.org/coar/version/c_970fb48d4fbd8a85 |
dc.type.coar.fl_str_mv |
http://purl.org/coar/resource_type/c_6501 http://purl.org/coar/resource_type/c_2df8fbb1 |
dc.type.local.spa.fl_str_mv |
Artículo |
status_str |
publishedVersion |
dc.identifier.issn.none.fl_str_mv |
1617-7061 |
dc.identifier.uri.none.fl_str_mv |
http://hdl.handle.net/10784/9666 |
dc.identifier.doi.none.fl_str_mv |
10.1002/pamm.201410214 |
identifier_str_mv |
1617-7061 10.1002/pamm.201410214 |
url |
http://hdl.handle.net/10784/9666 |
dc.language.iso.eng.fl_str_mv |
eng |
language |
eng |
dc.relation.ispartof.spa.fl_str_mv |
PAMM, Volume 14, Issue 1, pp 453-454 |
dc.relation.uri.none.fl_str_mv |
http://onlinelibrary.wiley.com/doi/10.1002/pamm.201410214/abstract |
dc.rights.coar.fl_str_mv |
http://purl.org/coar/access_right/c_14cb |
dc.rights.local.spa.fl_str_mv |
Acceso cerrado |
rights_invalid_str_mv |
Acceso cerrado http://purl.org/coar/access_right/c_14cb |
dc.format.eng.fl_str_mv |
application/pdf |
dc.publisher.spa.fl_str_mv |
WILEY-VCH Verlag |
institution |
Universidad EAFIT |
bitstream.url.fl_str_mv |
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1814110140619554816 |
spelling |
2016-11-18T21:53:09Z20142016-11-18T21:53:09Z1617-7061http://hdl.handle.net/10784/966610.1002/pamm.201410214Recent investigations have found a distinct correlation of effective properties of porous media to sigmoidal functions, where one axis is the Reynolds number Re and the other is the effective property dependent of Re, Θ = S (Re) -- One of these properties is tortuosity -- At very low Re (seepage flow), there is a characteristic value of tortuosity, and it is the upper horizontal asymptote of the sigmoidal function -- With higher values of Re (transient flow) the tortuosity value decreases, until a lower asymptote is reached (turbulent flow) -- Estimations of this parameter have been limited to the low Reynolds regime in the study of porous media -- The current state of the art presents different numerical measurements of tortuosity, such as skeletization, centroid binding, and arc length of streamlines -- These are solutions for the low Re regime. So far, for high Re, only the arc length of stream lines has been used to calculate tortuosity -- The present approach involves the simulation of fluid flow in large domains and high Re, which requires numerous resources, and often presents convergence problems -- In response to this, we propose a geometrical method to estimate the limit of tortuosity of porous media at Re → ∞, from the streamlines calculated at low Re limit -- We test our method by calculating the tortuosity limits in a fibrous porous media, and comparing the estimated values with numerical benchmark results -- Ongoing work includes the geometric estimation of different intrinsic properties of porous mediaapplication/pdfengWILEY-VCH VerlagPAMM, Volume 14, Issue 1, pp 453-454http://onlinelibrary.wiley.com/doi/10.1002/pamm.201410214/abstractAcceso cerradohttp://purl.org/coar/access_right/c_14cbDetermining the limits of geometrical tortuosity from seepage flow calculations in porous mediainfo:eu-repo/semantics/articlearticleinfo:eu-repo/semantics/publishedVersionpublishedVersionArtículohttp://purl.org/coar/version/c_970fb48d4fbd8a85http://purl.org/coar/resource_type/c_6501http://purl.org/coar/resource_type/c_2df8fbb1MATERIALES POROSOSDISTRIBUCIÓN DE GAUSSASÍNTOTASNÚMERO DE REYNOLDSPorous materialsGauss distributionAsymptotesReynolds numberPorous materialsGauss distributionAsymptotesReynolds numberFunción sigmoideFactor de TortuosidadAlgoritmo de esqueletizaciónUniversidad EAFIT. Departamento de Ingeniería MecánicaUribe, DavidOsorno, MaríaSivanesapillai, RakulanSteeb, HolgerRuíz, ÓscarLaboratorio CAD/CAM/CAEPAMMPAMM141453454LICENSElicense.txtlicense.txttext/plain; charset=utf-82556https://repository.eafit.edu.co/bitstreams/958d967d-619e-41c6-a9e0-8badc094c34f/download76025f86b095439b7ac65b367055d40cMD51ORIGINALDetermining_the_limits.htmlDetermining_the_limits.htmltext/html266https://repository.eafit.edu.co/bitstreams/7fa63b30-0157-4601-ab5c-9e79f0cf86bc/downloaddbec2adabbe4389295d973f7b0877779MD52Determining_the_limits.pdfDetermining_the_limits.pdfWeb Page Printapplication/pdf137051https://repository.eafit.edu.co/bitstreams/a36325fb-d2e4-4d51-a17b-8d18f46adb64/download50e2f5934e93de0a65ffa7b6d51dea50MD5310784/9666oai:repository.eafit.edu.co:10784/96662021-09-03 15:43:37.907open.accesshttps://repository.eafit.edu.coRepositorio Institucional Universidad EAFITrepositorio@eafit.edu.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 |