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

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$Edge excitations of paired fractional quantum Hall states$

P9.32Tue 611:23-14:00Stresses and structure of colloidal gels under shearNick Koumakis 1 and George Petekidis 11 FORTH-IESL, Polymer Group, FORTH-IESL, P. O. Box 1527, Vassilika Vouton 711<strong>10</strong>,Heraklion, Crete, Greece32
Tue 611:23-14:00P9.33Dynamics and rheology of vesicle suspension in shearflowAntonio Lamura 1 and Gerhard Gompper 21 IAC CNR, Via Amendola, 122/D, 70126, Bari, Italy2 ICS FZ Juelich, Juelich, GermanyWe consider a two-dimensional suspension of deflated vesicles under shear flow at finite temperaturefor different concentrations. The system is simulated in a hydrodynamic solvent by usingthe multi-particle collision technique. First we analyze the interaction of two vesicles in the tanktreadingregime. They slide over and around each other increasing their vertical separation afterscattering with strong fluctuations of vesicle shape and inclination angle. This result is in goodquantitative agreement with experimental results. The dependence of the suspension intrinsic viscosityon the viscosity ratio between inner and outer fluids, λ, is found to be monotonic with λ atthe fixed outer fluid viscosity for λ in dilute and semi-dilute regimes. The behavior of concentratedsuspensions is even more interesting being characterized by a shear thinning behavior since the intrinsicviscosity decreases with the shear rate over more then one decade for different values of λ.Moreover, there is also a clear indication of the formation of vesicle-free boundary layers of finitethickness, ∆, next to the system walls. ∆ increases with the shear rate reaching saturation. Whenincreasing the system width, the values of ∆ grow as also observed in two-dimensional simulationsof red blood cells in small vessels. Finally, it is found a non-linear dependence of ∆ on λ withthe boundary layer decreasing at high values of the viscosity contrast attaining a maximum at thetank-treading to tumbling transition.33
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8th Liquid Matter ConferenceSeptemb
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P1.6Fri 911:10-14:00Structure and d
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P2.2Tue 611:23-14:00Water + tert-bu
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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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P2.48Tue 611:23-14:00Treating hydro
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P2.56Tue 611:23-14:00Rationalizing
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P2.60Tue 611:23-14:00Solute-solvent
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P2.74Tue 611:23-14:00Percolation li
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P2.82Tue 611:23-14:00Understanding
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TartagliaWed 711:10-14:00P5.65How s
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Session 6:Films, foams, surfactants
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Thu 811:10-14:00P7.105Theory and si
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Thu 811:10-14:00P7.109Grain boundar
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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
Page 682 and 683: P8.50Thu 811:10-14:00Study of the k
Page 684 and 685: P8.52Thu 811:10-14:00Particle corre
Page 686 and 687: P8.54Thu 811:10-14:00Activity in su
Page 688 and 689: P8.56Thu 811:10-14:00Avalanche exci
Page 690 and 691: P8.58Thu 811:10-14:00Effect of size
Page 692 and 693: P8.60Thu 811:10-14:00Gauge theory o
Page 694 and 695: P8.62Thu 811:10-14:00Phase-separati
Page 696 and 697: P8.64Thu 811:10-14:00Quasi-equilibr
Page 698 and 699: P8.66Thu 811:10-14:00Bond dynamics
Page 701 and 702: Tue 611:23-14:00P9.1Viscosity of su
Page 703 and 704: Tue 611:23-14:00P9.3Influence of hy
Page 705 and 706: Tue 611:23-14:00P9.5Molecular dynam
Page 707 and 708: Tue 611:23-14:00P9.7A microscopic d
Page 709 and 710: Tue 611:23-14:00P9.9Rotation and mi
Page 711 and 712: Tue 611:23-14:00P9.11A novel optica
Page 713 and 714: Tue 611:23-14:00P9.13Evolution of d
Page 715 and 716: Tue 611:23-14:00P9.15Stress oversho
Page 717 and 718: Tue 611:23-14:00P9.17Effects of a n
Page 719 and 720: Tue 611:23-14:00P9.19Modifying defo
Page 721 and 722: Tue 611:23-14:00P9.21Efficiently ac
Page 723 and 724: Tue 611:23-14:00P9.23Soft matter in
Page 725 and 726: Tue 611:23-14:00P9.25Droplet mobili
Page 727 and 728: Tue 611:23-14:00P9.27Cell-level can
Page 729 and 730: Tue 611:23-14:00P9.29Active microrh
Page 731: Tue 611:23-14:00P9.31Subdiffusive i
Page 735 and 736: Tue 611:23-14:00P9.35Single file di
Page 737 and 738: Tue 611:23-14:00P9.37Complex dynami
Page 739 and 740: Tue 611:23-14:00P9.39Dynamic approa
Page 741 and 742: Tue 611:23-14:00P9.41On mechanism o
Page 743 and 744: Tue 611:23-14:00P9.43Peclet number
Page 745 and 746: Tue 611:23-14:00P9.45Heat transport
Page 747 and 748: Tue 611:23-14:00P9.47Rheology of di
Page 749 and 750: Tue 611:23-14:00P9.49Oscillatory fl
Page 751 and 752: Tue 611:23-14:00P9.51Scaling equati
Page 753 and 754: Tue 611:23-14:00P9.53Transport prop
Page 755 and 756: 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
Page 763 and 764: Tue 611:23-14:00P9.63Transition mec
Page 765 and 766: Tue 611:23-14:00P9.65Nonequilibrium
Page 767 and 768: Tue 611:23-14:00P9.67Phase-field mo
Page 769 and 770: Tue 611:23-14:00P9.69Enhanced shear
Page 771 and 772: Tue 611:23-14:00P9.71Dynamics of th
Page 773 and 774: Tue 611:23-14:00P9.73Real-time moni
Page 775: Tue 611:23-14:00P9.75Universal diss
Page 779 and 780: Tue 611:23-14:00P10.1Mechanical gro
Page 781 and 782: 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
Page 787 and 788:
Tue 611:23-14:00P10.9Electrical res
Page 789 and 790:
Tue 611:23-14:00P10.11Entropy drive
Page 791 and 792:
Tue 611:23-14:00P10.13Curvature ind
Page 793 and 794:
Tue 611:23-14:00P10.15Enhanced diff
Page 795 and 796:
Tue 611:23-14:00P10.17New approach
Page 797 and 798:
Tue 611:23-14:00P10.19Spatial struc
Page 799 and 800:
Tue 611:23-14:00P10.21Cell motility
Page 801 and 802:
Tue 611:23-14:00P10.23Effect of bou
Page 803 and 804:
Tue 611:23-14:00P10.25Self-organiza
Page 805 and 806:
Tue 611:23-14:00P10.27Magnetic bire
Page 807 and 808:
Tue 611:23-14:00P10.29Swimming beha
Page 809 and 810:
Tue 611:23-14:00P10.31Hydrodynamica
Page 811 and 812:
Tue 611:23-14:00P10.33Hydrodynamic
Page 813 and 814:
Tue 611:23-14:00P10.35Membrane late
Page 815 and 816:
Tue 611:23-14:00P10.37Protein-prote
Page 817:
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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