% IMPORTANT: The following is UTF-8 encoded.  This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.

@ARTICLE{Ripoll:464,
      author       = {Ripoll, M. and Winkler, R. G. and Mussawisade, K. and
                      Gompper, G.},
      title        = {{M}esoscale hydrodynamics simulations of attractive
                      rod-like colloids in shear flow},
      journal      = {Journal of physics / Condensed matter},
      volume       = {20},
      issn         = {0953-8984},
      address      = {Bristol},
      publisher    = {IOP Publ.},
      reportid     = {PreJuSER-464},
      pages        = {404209},
      year         = {2008},
      note         = {Record converted from VDB: 12.11.2012},
      abstract     = {Suspensions of rod-like colloids show in equilibrium an
                      isotropic-nematic coexistence region, which depends on the
                      strength of an attractive interaction between the rods. We
                      study the behavior of this system in shear flow for various
                      interaction strengths. A hybrid simulation approach is
                      employed, which consists of a mesoscale particle-based
                      hydrodynamics technique (multi-particle collision dynamics)
                      for the solvent and molecular dynamics simulations for the
                      colloidal rods. The shear flow induces alignment in the
                      initially isotropic phase, which generated an additional
                      free volume around each rod and causes the densification of
                      the isotropic phase at the expense of an erosion of the
                      initially nematic phase. Furthermore, the nematic phase
                      exhibits a collective rotational motion. The associated
                      rotational time decreases linearly in 1/(gamma)over dot with
                      increasing shear rate (gamma)over dot, and increases with
                      increasing attraction strength between the rods. The density
                      difference between these two regions at different shear
                      rates allows us to determine the binodal line of the phase
                      diagram. For large applied shear rates, the difference
                      between the phases disappears in favor of a homogeneous
                      flow-aligned state.},
      keywords     = {J (WoSType)},
      cin          = {IFF-2 / JARA-SIM},
      ddc          = {530},
      cid          = {I:(DE-Juel1)VDB782 / I:(DE-Juel1)VDB1045},
      pnm          = {Kondensierte Materie},
      pid          = {G:(DE-Juel1)FUEK414},
      shelfmark    = {Physics, Condensed Matter},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000259153200010},
      doi          = {10.1088/0953-8984/20/40/404209},
      url          = {https://juser.fz-juelich.de/record/464},
}