Anisotropic drop morphologies on corrugated surfaces.

Langmuir 24:14 (2008) 7299-7308

Authors:

H Kusumaatmaja, RJ Vrancken, CWM Bastiaansen, JM Yeomans

Abstract:

The spreading of liquid drops on surfaces corrugated with micrometer-scale parallel grooves is studied both experimentally and numerically. Because of the surface patterning, the typical final drop shape is no longer spherical. The elongation direction can be either parallel or perpendicular to the direction of the grooves, depending on the initial drop conditions. We interpret this result as a consequence of both the anisotropy of the contact line movement over the surface and the difference in the motion of the advancing and receding contact lines. Parallel to the grooves, we find little hysteresis due to the surface patterning and that the average contact angle approximately conforms to Wenzel's law as long as the drop radius is much larger than the typical length scale of the grooves. Perpendicular to the grooves, the contact line can be pinned at the edges of the ridges, leading to large contact angle hysteresis.

Lattice Boltzmann simulation techniques for simulating microscopic swimmers

COMPUT PHYS COMMUN 179:1-3 (2008) 159-164

Authors:

CM Pooley, JM Yeomans

Abstract:

We use two different sub-gridscale lattice Boltzmann methods to simulate the swimming motion of a model swimmer. We systematically characterise the discretisation errors associated with placing a continuous object on a grid, and place limits on how low the Reynolds number needs to be in order to reach the characteristic zero Reynolds number regime. (C) 2008 Elsevier B.V. All rights reserved.

Link invariants, the chromatic polynomial and the Potts model

(2008)

Authors:

Paul Fendley, Vyacheslav Krushkal

Slowest relaxation mode of the partially asymmetric exclusion process with open boundaries

(2008)

Authors:

Jan de Gier, Fabian HL Essler

Excitations of the One Dimensional Bose-Einstein Condensates in a Random Potential

ArXiv 0806.2322 (2008)

Authors:

V Gurarie, G Refael, JT Chalker

Abstract:

We examine bosons hopping on a one-dimensional lattice in the presence of a random potential at zero temperature. Bogoliubov excitations of the Bose-Einstein condensate formed under such conditions are localized, with the localization length diverging at low frequency as $\ell(\omega)\sim 1/\omega^\alpha$. We show that the well known result $\alpha=2$ applies only for sufficiently weak random potential. As the random potential is increased beyond a certain strength, $\alpha$ starts decreasing. At a critical strength of the potential, when the system of bosons is at the transition from a superfluid to an insulator, $\alpha=1$. This result is relevant for understanding the behavior of the atomic Bose-Einstein condensates in the presence of random potential, and of the disordered Josephson junction arrays.