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

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$Edge excitations of paired fractional quantum Hall states$

P5.172Wed 711:10-14:00Biopolymer based colloidal particles as functionaldelivery systemsKrassimir Velikov 1 and Ashok Patel 11 Unilever RD Vlaardingen, Olivier van Noortlaan 120, 3133 AT, Vlaardingen,NetherlandsThere is a great interest in natural polymeric materials for development of colloidal delivery systemsfor bioactive molecules. The current talk will focus on the synthesis and characterisation ofcolloidal particles from zein, a water insoluble protein from maize. We will discuss the preparation,characterisation and application of zein-curcumin composite colloidal particles. Particle sizeand morphology are studied with dynamic light scattering and transmission electron microscopy.Differential scanning calorimetry and X-ray diffraction are used to quantify the crystalline stateof the entrapped curcumin. UV irradiation is used to study the photostability of curcumin. Theparticle stability is studied at different physiologically relevant pH values and in simulated gastrointestinalconditions. Finally, the mucoadhesion properties of the particles are evaluated using invitro washed off method on agarose gels and mucin association on Caco-2 cells.172
Wed 711:10-14:00P5.173Colloidal micelles of patchy dumbbellsTeun Vissers, 1 Frank Smallenburg, 1 Francesco Sciortino, 2 Emanuela Zaccarelli, 2and Marjolein Dijkstra 11 Utrecht University, Princetonplein 5, 3584 CC, Utrecht, Netherlands2 Universita di Roma La Sapienza, Roma, ItalyPatchy colloids are particles with a number of patches on their surface that enable them toundergo highly directional interactions which depend on the physical and chemical properties ofthe patches, e. g. hydrophilicity, charge, and surface roughness. Patchy colloids can be used asbuilding blocks to design completely new structures [1, 2], and often display surprising phasebehavior compared to particles with isotropic interactions [3]. Recently, Kraft et al. synthesizeddumbbell particles consisting of one sphere with a smooth and one sphere with a rough surface [4].By the addition of polymer, depletion attractions can be induced exclusively between the smoothspheres. As a result, micellar structures of dumbbells form, with the smooth sides directed inwardsand the rough sides pointing outwards. Since such dumbbells are made by inducing protrusionsout of existing spheres, the two spheres can have different sizes and partially overlap. In computersimulations, Janus particles with one hemisphere interacting via square well attractions and theother one via hard-core interactions, were used as a simple model system for surfactants to studythe formation of micelles [5]. A gas of micelles, a liquid of free Janus particles and a coexistenceregion between them was found. Here, we present computer simulations of dumbbell particlesconsisting of a smooth sphere and a rough sphere which are allowed to overlap partially. Thesmooth spheres interact attractively with smooth spheres on other dumbbells. The rough spheresonly experience hard-core interactions. The effects of size ratio and the degree of overlap betweenthe smooth and the rough sphere are explored.[1] Q. Chen et al. , Nature, 469, 381 (2011).[2] F. Romano and F. Sciortino, Nat. Mater. News amp; Views, 10, 171 (2011).[3] B. Ruzicka, et al. , Nat. Mater, 10, 56 (2011).[4] D. J. Kraft et al. , submitted (2011).[5] F. Sciortino et al. , Phys. Rev. Lett. , 103, 237801 (2009).173
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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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Session 2:Water, solutions and reac
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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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P3.2Fri 911:10-14:00Studies in Cds-
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Wed 711:10-14:00P5.1Using symmetry
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Wed 711:10-14:00P5.5Long-time dynam
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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 711:10-14:00P5.27Colloids in co
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Wed 711:10-14:00P5.31Mesoscopic the
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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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TartagliaWed 711:10-14:00P5.65How s
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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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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
Page 625 and 626:
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
Page 631:
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
Page 672 and 673:
P8.40Thu 811:10-14:00Computer simul
Page 674 and 675:
P8.42Thu 811:10-14:00Clear structur
Page 676 and 677:
P8.44Thu 811:10-14:00From ”isomor
Page 678 and 679:
P8.46Thu 811:10-14:00Presence and a
Page 680 and 681:
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
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P8.54Thu 811:10-14:00Activity in su
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P8.56Thu 811:10-14:00Avalanche exci
Page 690 and 691:
P8.58Thu 811:10-14:00Effect of size
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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
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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
Page 713 and 714:
Tue 611:23-14:00P9.13Evolution of d
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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 and 732:
Tue 611:23-14:00P9.31Subdiffusive i
Page 733 and 734:
Tue 611:23-14:00P9.33Dynamics and r
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
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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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