TY - JOUR
T1 - Liquid morphologies and capillary forces between three spherical beads
AU - Semprebon, Ciro
AU - Scheel, Mario
AU - Herminghaus, Stephan
AU - Seemann, Ralf
AU - Brinkmann, Martin
PY - 2016/7/29
Y1 - 2016/7/29
N2 - Equilibrium shapes of coalesced pendular bridges in a static assembly of spherical beads are computed by numerical minimization of the interfacial energy. Our present study focuses on generic bead configurations involving three beads, one of which is in contact to the two others while there is a gap of variable size between the latter. In agreement with previous experimental studies, we find interfacial 'trimer' morphologies consisting of three coalesced pendular bridges, and 'dimers' of two coalesced bridges. In a certain range of the gap opening we observe a bistability between the dimer and trimer morphology during shrinking and growth. The magnitude of the corresponding capillary forces in presence of a trimer or dimer depends, besides the gap opening only on the volume or Laplace pressure of liquid. For a given Laplace pressure, the capillary forces in presence of a trimer are slightly larger than the force of a single bridges at the same gap opening, which could explain the shallow maximum and plateau of the capillary cohesion of a wetting liquid for saturations in the funicular regime.
AB - Equilibrium shapes of coalesced pendular bridges in a static assembly of spherical beads are computed by numerical minimization of the interfacial energy. Our present study focuses on generic bead configurations involving three beads, one of which is in contact to the two others while there is a gap of variable size between the latter. In agreement with previous experimental studies, we find interfacial 'trimer' morphologies consisting of three coalesced pendular bridges, and 'dimers' of two coalesced bridges. In a certain range of the gap opening we observe a bistability between the dimer and trimer morphology during shrinking and growth. The magnitude of the corresponding capillary forces in presence of a trimer or dimer depends, besides the gap opening only on the volume or Laplace pressure of liquid. For a given Laplace pressure, the capillary forces in presence of a trimer are slightly larger than the force of a single bridges at the same gap opening, which could explain the shallow maximum and plateau of the capillary cohesion of a wetting liquid for saturations in the funicular regime.
UR - https://www.scopus.com/pages/publications/84980315181
U2 - 10.1103/PhysRevE.94.012907
DO - 10.1103/PhysRevE.94.012907
M3 - Article
C2 - 27575206
SN - 2470-0045
VL - 94
JO - Physical Review E
JF - Physical Review E
IS - 1
M1 - 012907
ER -