8th Liquid Matter Conference September 6-10, 2011 Wien, Austria ...

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$Edge excitations of paired fractional quantum Hall states$

P7.8Thu 811:<strong>10</strong>-14:00The effect of roughness and wettability on the rate ofspontaneous imbibition in microfluidic capillariesEdo Boek, 1 Emily Chapman, 1 Jianhui Yang, 1 and John Crawshaw 11 Imperial College, Dept of Chemical Engineering, SW7 2AZ, London, United KingdomImproving our knowledge of flow phenomena associated with complex fluids in porous media isof great importance, particularly for enhanced oil recovery (EOR) and CO 2 storage applications.Here we investigate the dynamics of spontaneous imbibition using capillary flow experiments inmicrofluidic cells in combination with lattice-Boltzmann (LB) flow simulations. The purpose ofthis work is to understand how wettability (surface energy) and roughness affect the rate of spontaneousimbibition. Initially, simple smooth rectangular glass capillaries (0.05 x 0.05mm) wereinvestigated. These experiments could all be described using the Lucas-Washburn equation, wherewe observed a linear rise of the meniscus with the square root of time (〈h〉 ∼ t 1/2 ). Experimentswere also conducted using etched silicon/glass micro-models with a channel width of 50µm varyingroughness. In these micro-models, we control the roughness systematically and observe themeniscus position as a function of time with microscopy and a high-speed video camera. Most ofthe rough capillaries followed the square root of time behaviour, with the exception of the roughestcapillary. In this case, we observe ’pinning’ of the contact line within the capillary. This observationis of great importance for porous media flow applications. The cause of the ’pinning’ event isinvestigated in terms of pore geometry. For this purpose, we have used confocal microscopy andobtained a three-dimensional image of the meniscus. We compare the results with LB computersimulations of flow in the same capillaries and find a good agreement between experiment andsimulation. We are currently extending the experiments to investigate the effects of wettability onspontaneous imbibition. This is achieved by chemically altering the capillary channels through theuse of natural hydrophobic compounds found in crude oils.8
Thu 811:<strong>10</strong>-14:00P7.9Physics of antiicing action of superhydrophobic coatingsLudmila Boinovich, 1 Alexandre Emelyanenko, 1 and Darya Gudeeva 11 A. N. Frumkin Institute of Physical Chemistry and Electrochemistry, Leninsky prospect 31,119991, Moscow, Russian FederationThe anti-icing superhydrophobic nanocomposite coatings for the surface of pure aluminium andaluminium alloys have been designed and studied. The coatings developed demonstrate multimodalroughness with convex highly curved texture elements and are characterized by water contactangles 170-175 ◦ and rolling angles
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8th Liquid Matter ConferenceSeptemb
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P1.6Fri 911:10-14:00Structure and d
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P1.8Fri 911:10-14:00Surface tension
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P1.10Fri 911:10-14:00Primary relaxa
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P1.12Fri 911:10-14:00An efficient m
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P1.14Fri 911:10-14:00The single par
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P1.16Fri 911:10-14:00Computer simul
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P1.18Fri 911:10-14:00Porphyrin prep
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P1.20Fri 911:10-14:00A representati
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P1.22Fri 911:10-14:00Network of tet
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P1.24Fri 911:10-14:00Inter-cation c
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P1.26Fri 911:10-14:00Atomic structu
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P1.28Fri 911:10-14:00Proline based
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P1.30Fri 911:10-14:00Magnetic prope
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P1.32Fri 911:10-14:00On peculiariti
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P1.34Fri 911:10-14:00Densities of E
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P1.36Fri 911:10-14:00A molecular dy
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P1.38Fri 911:10-14:00The lquid-liqu
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P1.40Fri 911:10-14:00Nanoporous car
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P1.42Fri 911:10-14:00Computational
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P1.44Fri 911:10-14:00Medium range f
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P1.46Fri 911:10-14:00Structural and
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P1.48Fri 911:10-14:00How strongly i
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P1.50Fri 911:10-14:00Viscosity of S
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Session 2:Water, solutions and reac
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P2.2Tue 611:23-14:00Water + tert-bu
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P2.4Tue 611:23-14:00Experimental ev
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P2.6Tue 611:23-14:00Trapping proton
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P2.8Tue 611:23-14:00The effect of r
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P2.10Tue 611:23-14:00Equation of st
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P2.12Tue 611:23-14:00Phase transiti
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P2.14Tue 611:23-14:00Multiscale stu
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P2.16Tue 611:23-14:00Dipolar solute
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P2.18Tue 611:23-14:00Statical and d
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P2.20Tue 611:23-14:00Long-lived sub
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P2.22Tue 611:23-14:00Water-like ano
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P2.24Tue 611:23-14:00Study of supra
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P2.26Tue 611:23-14:00Local thermody
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P2.28Tue 611:23-14:00Ultrasonic evi
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P2.30Tue 611:23-14:00The theoretica
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P2.32Tue 611:23-14:00High frequency
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P2.34Tue 611:23-14:00Towards a mole
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P2.36Tue 611:23-14:00Crystallizatio
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P2.38Tue 611:23-14:00A study of die
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P2.40Tue 611:23-14:00Virial equatio
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P2.42Tue 611:23-14:00Compensation e
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P2.44Tue 611:23-14:00The electric p
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P2.46Tue 611:23-14:00The hydrophobi
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P2.48Tue 611:23-14:00Treating hydro
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P2.50Tue 611:23-14:00Correlations i
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P2.52Tue 611:23-14:00Hydrogen bond
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P2.54Tue 611:23-14:00Water structur
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P2.56Tue 611:23-14:00Rationalizing
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P2.58Tue 611:23-14:00Collective beh
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P2.60Tue 611:23-14:00Solute-solvent
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P2.62Tue 611:23-14:00Anomalous beha
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P2.64Tue 611:23-14:00The micro-stru
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P2.66Tue 611:23-14:00Parameterizati
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P2.68Tue 611:23-14:00Is there a ris
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P2.70Tue 611:23-14:00Excess entropy
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P2.72Tue 611:23-14:00Solid/liquid a
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P2.74Tue 611:23-14:00Percolation li
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P2.76Tue 611:23-14:00Regularities i
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P2.78Tue 611:23-14:00A molecular dy
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P2.80Tue 611:23-14:00Complex phase
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P2.82Tue 611:23-14:00Understanding
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P2.84Tue 611:23-14:00Guanidinium in
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P2.86Tue 611:23-14:00Theoretical st
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P2.88Tue 611:23-14:00Effects of int
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Session 3:Liquid crystalsP3
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P3.2Fri 911:10-14:00Studies in Cds-
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P3.4Fri 911:10-14:00Undulation inst
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P3.6Fri 911:10-14:00Translation dif
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P3.8Fri 911:10-14:00Electro-optic r
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P3.10Fri 911:10-14:00Isotropic to n
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P3.12Fri 911:10-14:00The influence
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P3.14Fri 911:10-14:00Tuning diffusi
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P3.16Fri 911:10-14:00Instability pa
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P3.18Fri 911:10-14:00Study of new p
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P3.20Fri 911:10-14:00Stereo-specifi
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P3.22Fri 911:10-14:00Colloidal part
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P3.24Fri 911:10-14:00Polymorphism o
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P3.28Fri 911:10-14:00Direct observa
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P3.30Fri 911:10-14:00Spatio-tempora
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P3.32Fri 911:10-14:00Continuum theo
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P3.34Fri 911:10-14:00Isotropic lasi
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P3.36Fri 911:10-14:00Effect of poly
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P3.38Fri 911:10-14:00Liquid crystal
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P3.40Fri 911:10-14:00Multiscale sim
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Session 4:Polymers, polyelectrolyte
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P4.2Fri 911:10-14:00Experiments and
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P4.4Fri 911:10-14:00Online monitori
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P4.6Fri 911:10-14:00Single chain dy
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P4.8Fri 911:10-14:00Helix specific
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P4.10Fri 911:10-14:00Exploring the
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P4.12Fri 911:10-14:00Monte Carlo si
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P4.14Fri 911:10-14:00Spherical vs p
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P4.16Fri 911:10-14:00Structural stu
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P4.18Fri 911:10-14:00The Influence
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P4.20Fri 911:10-14:00Viscoelasticit
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P4.22Fri 911:10-14:00Competitive ad
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P4.24Fri 911:10-14:00Initial steps
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P4.26Fri 911:10-14:00Diffusion of t
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P4.30Fri 911:10-14:00Slow dynamics
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P4.32Fri 911:10-14:00Orientation mo
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P4.34Fri 911:10-14:00Structure and
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P4.36Fri 911:10-14:00Hierarchically
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P4.38Fri 911:10-14:00Microphase sep
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P4.40Fri 911:10-14:00Adsorption of
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P4.42Fri 911:10-14:00Theoretical an
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P4.44Fri 911:10-14:00Possible mecha
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P4.46Fri 911:10-14:00Monte Carlo si
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P4.48Fri 911:10-14:00Influence of t
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P4.50Fri 911:10-14:00Application of
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P4.52Fri 911:10-14:00Lamellae forma
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P4.54Fri 911:10-14:00Thermorheologi
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P4.56Fri 911:10-14:00Wrinkling laby
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P4.58Fri 911:10-14:00Dielectric rel
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P4.60Fri 911:10-14:00Anomalous stru
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P4.62Fri 911:10-14:00Effect of addi
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P4.64Fri 911:10-14:00Large-scale mo
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P4.66Fri 911:10-14:00On the physica
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P4.68Fri 911:10-14:00Tuning protein
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Wed 711:10-14:00P5.1Using symmetry
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Wed 711:10-14:00P5.3Monte Carlo sim
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Wed 711:10-14:00P5.5Long-time dynam
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Wed 711:10-14:00P5.7The role of bou
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Wed 711:10-14:00P5.9Stability of or
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Wed 711:10-14:00P5.11Diffusive moti
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Wed 711:10-14:00P5.13Crystallizatio
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Wed 711:10-14:00P5.15Collective dyn
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Wed 711:10-14:00P5.17Calculation of
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Wed 711:10-14:00P5.19Detection of e
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Wed 711:10-14:00P5.21Bulk liquid st
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Wed 711:10-14:00P5.23Charged colloi
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Wed 711:10-14:00P5.25Dielectric res
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Wed 711:10-14:00P5.27Colloids in co
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Wed 711:10-14:00P5.29Phase behavior
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Wed 711:10-14:00P5.31Mesoscopic the
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Wed 711:10-14:00P5.33The renormaliz
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Wed 711:10-14:00P5.35When depletion
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Wed 711:10-14:00P5.37Confined dryin
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Wed 711:10-14:00P5.39Predicting cry
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Wed 711:10-14:00P5.41Competition be
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Wed 711:10-14:00P5.43Interactions b
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Wed 711:10-14:00P5.45Electrostatic
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Wed 711:10-14:00P5.47Homogeneous nu
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Wed 711:10-14:00P5.49Measuring coll
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Wed 711:10-14:00P5.51Influence of i
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Wed 711:10-14:00P5.53Particle dynam
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Wed 711:10-14:00P5.55Friction contr
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Wed 711:10-14:00P5.57Monte Carlo si
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Wed 711:10-14:00P5.59Key role of hy
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Wed 711:10-14:00P5.61The Kern-Frenk
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Wed 711:10-14:00P5.63Phase diagram
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TartagliaWed 711:10-14:00P5.65How s
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Wed 711:10-14:00P5.67Field induced
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Wed 711:10-14:00P5.69A modified sof
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Wed 711:10-14:00P5.71Three dimensio
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Wed 711:10-14:00P5.73Rod-like parti
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Wed 711:10-14:00P5.75Diffusion of c
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Wed 711:10-14:00P5.77Structure form
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Wed 711:10-14:00P5.79Effective forc
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Wed 711:10-14:00P5.81Nucleation lin
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Wed 711:10-14:00P5.83Glass transiti
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Wed 711:10-14:00P5.85Fluctuation do
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Wed 711:10-14:00P5.87Deformation an
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Wed 711:10-14:00P5.89Concentration
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Wed 711:10-14:00P5.91Investigation
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Wed 711:10-14:00P5.93Arrest and dyn
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Wed 711:10-14:00P5.95Two dimensiona
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Wed 711:10-14:00P5.97Connecting sti
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Wed 711:10-14:00P5.99Thermodynamic
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Wed 711:10-14:00P5.101Consolidation
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Wed 711:10-14:00P5.103Crystallizati
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Wed 711:10-14:00P5.105Coarse-graini
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Wed 711:10-14:00P5.107Monolayers of
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Wed 711:10-14:00P5.109Dissipative t
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Wed 711:10-14:00P5.111Coarse graini
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Wed 711:10-14:00P5.113Structure, ph
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Wed 711:10-14:00P5.115A new model f
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Wed 711:10-14:00P5.117Dynamics in d
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Wed 711:10-14:00P5.119Phase behavio
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Wed 711:10-14:00P5.121Shear melting
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Wed 711:10-14:00P5.123Driven crysta
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Wed 711:10-14:00P5.125Patchy, fluor
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Wed 711:10-14:00P5.127Electrorheolo
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Wed 711:10-14:00P5.129Clogging and
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Wed 711:10-14:00P5.131Dynamics of l
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Wed 711:10-14:00P5.133Anistropic di
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Wed 711:10-14:00P5.135Equilibrium p
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Wed 711:10-14:00P5.137Exploring pro
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Wed 711:10-14:00P5.139Accurate simu
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Wed 711:10-14:00P5.141Two-particle
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Wed 711:10-14:00P5.143Attraction be
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Wed 711:10-14:00P5.145Exact solutio
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Wed 711:10-14:00P5.147Self-aggregat
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Wed 711:10-14:00P5.149Kinetics of m
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Wed 711:10-14:00P5.151Light scatter
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Wed 711:10-14:00P5.153Frustrated co
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Wed 711:10-14:00P5.155Colloidal cub
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Wed 711:10-14:00P5.157Nonequilibriu
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Wed 711:10-14:00P5.159Numerical stu
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Wed 711:10-14:00P5.161Aging phenome
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Wed 711:10-14:00P5.163Depletion att
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Wed 711:10-14:00P5.165Trapping coll
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Wed 711:10-14:00P5.167Electrostatic
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Wed 711:10-14:00P5.169Dynamical sig
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Wed 711:10-14:00P5.171Tomographic c
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Wed 711:10-14:00P5.173Colloidal mic
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Wed 711:10-14:00P5.175Effect of cro
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Wed 711:10-14:00P5.177Fluidization
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Wed 711:10-14:00P5.1792-dimensional
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Wed 711:10-14:00P5.181Thermophysica
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Wed 711:10-14:00P5.183Structure of
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Wed 711:10-14:00P5.185Non-hard sphe
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Wed 711:10-14:00P5.187Freezing beha
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Wed 711:10-14:00P5.189Criticality a
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Session 6:Films, foams, surfactants
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P6.2Fri 911:10-14:00Measurement of
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Page 468 and 469: P6.12Fri 911:10-14:00Studies on nan
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Page 472 and 473: P6.16Fri 911:10-14:00Phase diagram
Page 474 and 475: P6.18Fri 911:10-14:00SAFT-gamma coa
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Page 486 and 487: P6.30Fri 911:10-14:00Nascent nanoem
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Page 492 and 493: P6.36Fri 911:10-14:00Mixture of PEG
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Page 503 and 504: Thu 811:10-14:00P7.1Dissipative par
Page 505 and 506: Thu 811:10-14:00P7.3Two-dimensional
Page 507 and 508: Thu 811:10-14:00P7.5Wall-fluid inte
Page 509: Thu 811:10-14:00P7.7Interfacial ten
Page 513 and 514: Thu 811:10-14:00P7.11Diffusion phen
Page 515 and 516: Thu 811:10-14:00P7.13Water cavitati
Page 517 and 518: Thu 811:10-14:00P7.15Freezing of si
Page 519 and 520: Thu 811:10-14:00P7.17Thermodynamics
Page 521 and 522: Thu 811:10-14:00P7.19Non-equilibriu
Page 523 and 524: Thu 811:10-14:00P7.21The role of me
Page 525 and 526: Thu 811:10-14:00P7.23Computational
Page 527 and 528: Thu 811:10-14:00P7.25Ion specificit
Page 529 and 530: Thu 811:10-14:00P7.27Raman scatteri
Page 531 and 532: Thu 811:10-14:00P7.29Coarse-grained
Page 533 and 534: Thu 811:10-14:00P7.31Thickness and
Page 535 and 536: Thu 811:10-14:00P7.33Morphological
Page 537 and 538: Thu 811:10-14:00P7.35Kinetics of fl
Page 539 and 540: Thu 811:10-14:00P7.37Dielectric hea
Page 541 and 542: Thu 811:10-14:00P7.39Morphology and
Page 543 and 544: Thu 811:10-14:00P7.41The crystal-fl
Page 545 and 546: Thu 811:10-14:00P7.43Adsorption of
Page 547 and 548: Thu 811:10-14:00P7.45Hard sphere fl
Page 549 and 550: Thu 811:10-14:00P7.47Adsorption of
Page 551 and 552: Thu 811:10-14:00P7.49Complications
Page 553 and 554: Thu 811:10-14:00P7.51New method for
Page 555 and 556: Thu 811:10-14:00P7.53Numerical simu
Page 557 and 558: Thu 811:10-14:00P7.55Identifying in
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Thu 811:10-14:00P7.59Computing pres
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Thu 811:10-14:00P7.61Nanofluidics:
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Thu 811:10-14:00P7.63Calculation of
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Thu 811:10-14:00P7.65The effect of
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Thu 811:10-14:00P7.67Adsorption beh
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Thu 811:10-14:00P7.69Thermal capill
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Thu 811:10-14:00P7.71Aqueous electr
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Thu 811:10-14:00P7.73Critical Casim
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Thu 811:10-14:00P7.75Drag reduction
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Thu 811:10-14:00P7.77Formation of n
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Thu 811:10-14:00P7.79Viscous dissip
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Thu 811:10-14:00P7.81Bouncing jets
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Thu 811:10-14:00P7.83Pair correlati
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Thu 811:10-14:00P7.85Shaping liquid
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Thu 811:10-14:00P7.87On the scaling
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Thu 811:10-14:00P7.89Adsorption of
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Thu 811:10-14:00P7.91Experimental s
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Thu 811:10-14:00P7.93Hexatic phase
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Thu 811:10-14:00P7.95Spontaneous sp
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Thu 811:10-14:00P7.97Glass transiti
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Thu 811:10-14:00P7.99Complex ions i
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Thu 811:10-14:00P7.101Coaxial cross
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Thu 811:10-14:00P7.103Ordering beha
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Thu 811:10-14:00P7.105Theory and si
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Thu 811:10-14:00P7.107The Saffman-T
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Thu 811:10-14:00P7.109Grain boundar
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Thu 811:10-14:00P7.111Unusual capil
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Thu 811:10-14:00P7.113Motion and os
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Thu 811:10-14:00P7.115Dissolution b
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Thu 811:10-14:00P7.117Suspension of
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Thu 811:10-14:00P7.119Nucleation on
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Thu 811:10-14:00P7.121Monte Carlo s
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Thu 811:10-14:00P7.123Forces betwee
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Thu 811:10-14:00P7.125Size selectiv
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Thu 811:10-14:00P7.127Structure and
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Session 8:Supercooled liquids, glas
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P8.2Thu 811:10-14:00Hyperacoustic r
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P8.4Thu 811:10-14:00Glass transitio
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P8.6Thu 811:10-14:00Sudden network
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P8.8Thu 811:10-14:00Metastable high
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P8.10Thu 811:10-14:00Measurements o
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P8.12Thu 811:10-14:00Time resolved
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P8.14Thu 811:10-14:00Freezing of wa
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P8.16Thu 811:10-14:00Connecting str
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P8.18Thu 811:10-14:00Multi-scale mi
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P8.20Thu 811:10-14:00Structure of c
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P8.22Thu 811:10-14:00Nonlinear stre
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P8.24Thu 811:10-14:00Bond order in
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P8.26Thu 811:10-14:00Structure and
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P8.28Thu 811:10-14:00Connecting dif
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P8.30Thu 811:10-14:00Vitrification
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P8.32Thu 811:10-14:00Dynamic hetero
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P8.34Thu 811:10-14:00A leading mode
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P8.36Thu 811:10-14:00Factors contri
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P8.38Thu 811:10-14:00Theoretical st
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P8.40Thu 811:10-14:00Computer simul
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P8.42Thu 811:10-14:00Clear structur
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P8.44Thu 811:10-14:00From ”isomor
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P8.46Thu 811:10-14:00Presence and a
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P8.48Thu 811:10-14:00Glass transiti
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P8.50Thu 811:10-14:00Study of the k
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P8.52Thu 811:10-14:00Particle corre
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P8.54Thu 811:10-14:00Activity in su
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P8.56Thu 811:10-14:00Avalanche exci
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P8.58Thu 811:10-14:00Effect of size
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P8.60Thu 811:10-14:00Gauge theory o
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P8.62Thu 811:10-14:00Phase-separati
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P8.64Thu 811:10-14:00Quasi-equilibr
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P8.66Thu 811:10-14:00Bond dynamics
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Tue 611:23-14:00P9.1Viscosity of su
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Tue 611:23-14:00P9.3Influence of hy
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Tue 611:23-14:00P9.5Molecular dynam
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Tue 611:23-14:00P9.7A microscopic d
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Tue 611:23-14:00P9.9Rotation and mi
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Tue 611:23-14:00P9.11A novel optica
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Tue 611:23-14:00P9.13Evolution of d
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Tue 611:23-14:00P9.15Stress oversho
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Tue 611:23-14:00P9.17Effects of a n
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Tue 611:23-14:00P9.19Modifying defo
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Tue 611:23-14:00P9.21Efficiently ac
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Tue 611:23-14:00P9.23Soft matter in
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Tue 611:23-14:00P9.25Droplet mobili
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Tue 611:23-14:00P9.27Cell-level can
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Tue 611:23-14:00P9.29Active microrh
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Tue 611:23-14:00P9.31Subdiffusive i
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Tue 611:23-14:00P9.33Dynamics and r
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Tue 611:23-14:00P9.35Single file di
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Tue 611:23-14:00P9.37Complex dynami
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Tue 611:23-14:00P9.39Dynamic approa
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Tue 611:23-14:00P9.41On mechanism o
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Tue 611:23-14:00P9.43Peclet number
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Tue 611:23-14:00P9.45Heat transport
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Tue 611:23-14:00P9.47Rheology of di
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Tue 611:23-14:00P9.49Oscillatory fl
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Tue 611:23-14:00P9.51Scaling equati
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Tue 611:23-14:00P9.53Transport prop
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Tue 611:23-14:00P9.55Simulation stu
Page 757 and 758:
Tue 611:23-14:00P9.57A rheological
Page 759 and 760:
Tue 611:23-14:00P9.59Limestone fill
Page 761 and 762:
Tue 611:23-14:00P9.61Incomplete equ
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Tue 611:23-14:00P9.63Transition mec
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Tue 611:23-14:00P9.65Nonequilibrium
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Tue 611:23-14:00P9.67Phase-field mo
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Tue 611:23-14:00P9.69Enhanced shear
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Tue 611:23-14:00P9.71Dynamics of th
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Tue 611:23-14:00P9.73Real-time moni
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Tue 611:23-14:00P9.75Universal diss
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Tue 611:23-14:00P10.1Mechanical gro
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Tue 611:23-14:00P10.3Modeling twitc
Page 783 and 784:
Tue 611:23-14:00P10.5One-step metho
Page 785 and 786:
Tue 611:23-14:00P10.7Anesthetic mol
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Tue 611:23-14:00P10.9Electrical res
Page 789 and 790:
Tue 611:23-14:00P10.11Entropy drive
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Tue 611:23-14:00P10.13Curvature ind
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Tue 611:23-14:00P10.15Enhanced diff
Page 795 and 796:
Tue 611:23-14:00P10.17New approach
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Tue 611:23-14:00P10.19Spatial struc
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Tue 611:23-14:00P10.21Cell motility
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Tue 611:23-14:00P10.23Effect of bou
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Tue 611:23-14:00P10.25Self-organiza
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Tue 611:23-14:00P10.27Magnetic bire
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Tue 611:23-14:00P10.29Swimming beha
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Tue 611:23-14:00P10.31Hydrodynamica
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Tue 611:23-14:00P10.33Hydrodynamic
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Tue 611:23-14:00P10.35Membrane late
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Tue 611:23-14:00P10.37Protein-prote
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Tue 611:23-14:00P10.39Mesoscale hyd
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8th Liquid Matter Conference September 6-10, 2011 Wien, Austria ...

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