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SUMMARY:The dynamics of confined droplets
DTSTART:20170425T141500
DTEND:20170425T151500
DTSTAMP:20260924T071711Z
UID:217a6a1e6e5693e68e1a6a465c3f5d5952e3e8e762d78e5d2e1eef0b
CATEGORIES:Conferences - Seminars
DESCRIPTION:Etienne Reyssat and Ludovic Keiser Laboratoire de Physique et 
 Mécanique des Milieux Hétérogènes (PMMH\, ESPCI) Paris\nThe dynamics o
 f confined droplets has been extensively studied during the last decades\,
  in the footsteps of the development of digital microfluidics. In the fiel
 d of oil recovery\, numerous phenomena lead to the emulsification of petro
 leum while transported across a reservoir\, e.g. viscous fingering or snap
 -off. The understanding of the peculiar dynamics of confined droplets and 
 emulsions is thus of crucial importance.\nIn a first part\, we will discus
 s the shapes and velocities of completely wetting droplets of oil sliding 
 under gravity between closely spaced parallel walls (Hele-Shaw cell). Visc
 ous dissipation opposing the motion takes place both in the bulk of the li
 quid and in the vicinity of contact lines. In this model geometry\, bulk a
 nd line effects may be measured independently. We investigate contact line
  dissipation by studying the motion of droplets on pre-wetted surfaces\, a
  way to regularize the contact line singularity in a controlled way.\n\nIn
  a second part\, we focus on the dynamics of non-wetting droplets of oil c
 onﬁned in a vertical Hele-Shaw cell ﬁlled with a much less viscous sur
 factant solution. The oil droplets are denser than the aqueous solution an
 d move at constant speed driven by gravity. The surfactant solution comple
 tely wets the walls\, and a thin lubrication film separates the oil drople
 ts from the walls. For a cell with smooth walls\, two main dynamical regim
 es are characterized as the gap between the walls is varied. Viscous dissi
 pation is found to dominate either in the droplet or in the lubrication fi
 lm. A sharp transition between both regimes is observed and successfully c
 aptured by asymptotic models. For a cell with rough walls\, that transitio
 n is found to be dramatically altered. We show that droplets are generally
  much slower in a rough Hele-Shaw cell\, in comparison with a similar smoo
 th cell. Building up on the seminal work of Seiwert et al. (JFM\, 2011) on
  film deposition by dip coating on a rough surface\, we shed light on non-
 trivial friction processes resulting from the interplay of viscous dissipa
 tion at the front of the droplet\, in the lubrication film and in the bulk
  of the droplet.\n\nThe dynamics of confined droplets has been extensively
  studied during the last decades\, in the footsteps of the development of 
 digital microfluidics. In the field of oil recovery\, numerous phenomena l
 ead to the emulsification of petroleum while transported across a reservoi
 r\, e.g. viscous fingering or snap-off. The understanding of the peculiar 
 dynamics of confined droplets and emulsions is thus of crucial importance.
 \n\nIn a first part\, we will discuss the shapes and velocities of complet
 ely wetting droplets of oil sliding under gravity between closely spaced p
 arallel walls (Hele-Shaw cell). Viscous dissipation opposing the motion ta
 kes place both in the bulk of the liquid and in the vicinity of contact li
 nes. In this model geometry\, bulk and line effects may be measured indepe
 ndently. We investigate contact line dissipation by studying the motion of
  droplets on pre-wetted surfaces\, a way to regularize the contact line si
 ngularity in a controlled way.\n\nIn a second part\, we focus on the dynam
 ics of non-wetting droplets of oil conﬁned in a vertical Hele-Shaw cell 
 ﬁlled with a much less viscous surfactant solution. The oil droplets are
  denser than the aqueous solution and move at constant speed driven by gra
 vity. The surfactant solution completely wets the walls\, and a thin lubri
 cation film separates the oil droplets from the walls. For a cell with smo
 oth walls\, two main dynamical regimes are characterized as the gap betwee
 n the walls is varied. Viscous dissipation is found to dominate either in 
 the droplet or in the lubrication film. A sharp transition between both re
 gimes is observed and successfully captured by asymptotic models. For a ce
 ll with rough walls\, that transition is found to be dramatically altered.
  We show that droplets are generally much slower in a rough Hele-Shaw cell
 \, in comparison with a similar smooth cell. Building up on the seminal wo
 rk of Seiwert et al. (JFM\, 2011) on film deposition by dip coating on a r
 ough surface\, we shed light on non-trivial friction processes resulting f
 rom the interplay of viscous dissipation at the front of the droplet\, in 
 the lubrication film and in the bulk of the droplet.\n 
LOCATION:ME B10 https://plan.epfl.ch/theme/generalite_thm_plan_public?dim_
 floor=1&lang=fr&dim_lang=fr&baselayer_ref=grp_backgrounds&tree_groups=cent
 res_nevralgiques%2Cacces%2Cmobilite_reduite%2Censeignement%2Ccommerc
STATUS:CONFIRMED
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