{"title":"Inertial forces and elastohydrodynamic interaction of spherical particles in wall-bounded sedimentation experiments at low particle Reynolds number","authors":"Isabell Noichl, Clarissa Schönecker","doi":"arxiv-2409.07209","DOIUrl":null,"url":null,"abstract":"Wall-bounded sedimentation of spherical particles at low particle Reynolds\nnumbers $Re_\\text{P}\\lessapprox 0.1$ under the influence of elastic deformation\nwas investigated experimentally. The complete kinematics of both elastic and\nrigid spheres sedimenting from rest near a rigid or an elastic plane wall in a\nrectangular duct were recorded. Several specific phenomena related to both\ninertial and elastohydrodynamic effects were identified and discussed. Among\nthese phenomena is an inertial wall attraction, i.e., particles approach the\nwall while being accelerated from rest. It was found, that this initial\nattraction was a universal, purely hydrodynamic phenomenon which occurred in\nall experiments at $Re_\\text{P}\\lessapprox 0.1$. After the initial stage, rigid\nspheres sedimenting at $Re_\\text{P}\\approx O(10^{-1}$) near the wall behaved in\nthe classical way, showing linear migration due to hydrodynamic lift forces.\nNon-classic evolution of the particle velocity with respect to the wall\ndistance was observed for both rigid and elastic spheres sedimenting at\n$Re_\\text{P}\\approx O(10^{-2}$). Sedimentation was persistently unsteady and\nthe spheres decelerated although the wall distance was increased. Another\nphenomenon is that very soft spheres showed instationarities superimposed by\nnonlinearities. These peculiarities in the kinematics are attributed to the\nnon-trivial coupling between particle-fluid inertial forces and elastic\neffects, i.e., to the existence of elastohydrodynamic memory. Instationarities\nwere also observed during the sedimentation of rigid spheres along an elastic\nwall. For example, in the near-wall region, elastohydrodynamic interactions\ndamped the dynamics during mass acceleration. Meanwhile, persistent undulating\nmotion towards the wall was observed, i.e., elastohydrodynamic particle\ntrapping instead of hydrodynamic lift was observed.","PeriodicalId":501125,"journal":{"name":"arXiv - PHYS - Fluid Dynamics","volume":"2 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Fluid Dynamics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.07209","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Wall-bounded sedimentation of spherical particles at low particle Reynolds
numbers $Re_\text{P}\lessapprox 0.1$ under the influence of elastic deformation
was investigated experimentally. The complete kinematics of both elastic and
rigid spheres sedimenting from rest near a rigid or an elastic plane wall in a
rectangular duct were recorded. Several specific phenomena related to both
inertial and elastohydrodynamic effects were identified and discussed. Among
these phenomena is an inertial wall attraction, i.e., particles approach the
wall while being accelerated from rest. It was found, that this initial
attraction was a universal, purely hydrodynamic phenomenon which occurred in
all experiments at $Re_\text{P}\lessapprox 0.1$. After the initial stage, rigid
spheres sedimenting at $Re_\text{P}\approx O(10^{-1}$) near the wall behaved in
the classical way, showing linear migration due to hydrodynamic lift forces.
Non-classic evolution of the particle velocity with respect to the wall
distance was observed for both rigid and elastic spheres sedimenting at
$Re_\text{P}\approx O(10^{-2}$). Sedimentation was persistently unsteady and
the spheres decelerated although the wall distance was increased. Another
phenomenon is that very soft spheres showed instationarities superimposed by
nonlinearities. These peculiarities in the kinematics are attributed to the
non-trivial coupling between particle-fluid inertial forces and elastic
effects, i.e., to the existence of elastohydrodynamic memory. Instationarities
were also observed during the sedimentation of rigid spheres along an elastic
wall. For example, in the near-wall region, elastohydrodynamic interactions
damped the dynamics during mass acceleration. Meanwhile, persistent undulating
motion towards the wall was observed, i.e., elastohydrodynamic particle
trapping instead of hydrodynamic lift was observed.