dc.contributor.author | Vazquez-Quesada, A. | |
dc.contributor.author | Español, P. | |
dc.contributor.author | Tanner, R.I. | |
dc.contributor.author | Ellero, M. | |
dc.date.accessioned | 2019-10-21T09:21:56Z | |
dc.date.available | 2019-10-21T09:21:56Z | |
dc.date.issued | 2019 | |
dc.identifier.issn | 0022-1120 | |
dc.identifier.uri | http://hdl.handle.net/20.500.11824/1030 | |
dc.description.abstract | In this work we study the rheology of a non-colloidal suspension of rigid spherical
particles interacting with a viscoelastic matrix. Three-dimensional numerical simulations
under shear flow are performed using the smoothed particle hydrodynamics method and
compared with experimental data available in the literature using different constant-
viscosity elastic Boger fluids. The rheological properties of the Boger matrices are
matched in simulation under viscometric flow conditions. Suspension rheology under
dilute to semi-concentrated conditions (i.e. up to solid volume fraction φ = 0.3) is
explored. It is found that at small Deborah numbers (based on the macroscopic imposed
shear rate), relative suspension viscosities ηr exhibit a plateau at every concentration
investigated. By increasing the Deborah number De shear-thickening is observed which is
related to the extensional-thickening of the underlying viscoelastic matrix. Under dilute
conditions (φ = 0.05) numerical results for ηr agree quantitatively with experimental
data both in the De- and φ-dependencies. Even under dilute conditions, simulations of
full many-particle systems with no ’a priori’ specification of their spatial distribution
need to be considered to recover precisely experimental values. By increasing the solid
volume fraction towards φ = 0.3, despite the fact that the trend is well captured, the
agreement remains qualitative with discrepancies arising in the absolute values of ηr
obtained from simulations and experiments but also with large deviations existing among
different experiments. With regard to the specific mechanism of elastic thickening, the
microstructural analysis shows that elastic thickening correlates well with the averaged
viscoelastic dissipation function θ_elast, requiring a scaling as θ_elasti ∼De^α with α > 2
to take place. Locally, despite the fact that regions of large polymer stretching (and
viscoelastic dissipation) can occur everywhere in the domain, flow regions uniquely responsible
of the elastic thickening are well correlated to areas with significant extensional
component. | en_US |
dc.format | application/pdf | en_US |
dc.language.iso | eng | en_US |
dc.rights | Reconocimiento-NoComercial-CompartirIgual 3.0 España | en_US |
dc.rights.uri | http://creativecommons.org/licenses/by-nc-sa/3.0/es/ | en_US |
dc.title | Shear-thickening of a non-colloidal suspension with a viscoelastic matrix | en_US |
dc.type | info:eu-repo/semantics/article | en_US |
dc.identifier.doi | 10.1017/jfm.2019.753 | |
dc.relation.publisherversion | https://doi.org/10.1017/jfm.2019.753 | en_US |
dc.relation.projectID | ES/2PE/RTI2018-094595-B-I00 | en_US |
dc.rights.accessRights | info:eu-repo/semantics/openAccess | en_US |
dc.type.hasVersion | info:eu-repo/semantics/publishedVersion | en_US |
dc.journal.title | Journal of Fluid Mechanics | en_US |