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000204910 041__ $$aEnglish
000204910 1001_ $$0P:(DE-Juel1)131034$$aWiegand, Simone$$b0$$eCorresponding author$$ufzj
000204910 1112_ $$aInternational Symposium on Fluctuation and Structure out of Equilibrium 2015$$cKyoto$$d2015-08-20 - 2015-08-23$$gSFS2015$$wJapan
000204910 245__ $$aThermophoresis of charged colloidal spheres and rods
000204910 260__ $$c2015
000204910 3367_ $$0PUB:(DE-HGF)24$$2PUB:(DE-HGF)$$aPoster$$bposter$$mposter$$s1441718544_16206
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000204910 520__ $$aRecently Dhont and Briels [1] calculated the double-layer contribution to the single-particle thermal diffusion coefficient of charged, spherical colloids with arbitrary double-layer thickness. In this approach three forces are taken into account, which contribute to the total thermophoretic force on a charged colloidal sphere due its double layer: This concept has successfully been used to describe the Soret coefficient of Ludox particles as function of the Debye length [2]. A good agreement between experiment and theory was found with only one adjustable parameter, the intercept at zero Debye length, which measures the contribution of the solvation layer and possibly the colloid core material to the Soret coefficient.Later the concept was extended for charged colloidal rods [3]. As model system we used the charged, rod-like fd-virus. The Soret coefficient of the fd-viruses increases monotonically with increasing Debye length, while there is a relatively weak dependence on the rod-concentration when the ionic strength is kept constant. Additionally to the intercept at zero Debye length we used the surface charge density as an adjustable parameter. Applying the theoretical model to the experimental data we found a surface charge density, which compares well the one determined by electrophoresis measurements taking into account the ion condensation. Additionally we studied the interplay between steric and charge contribution by grafting polyethylene glycol chains to the fd-virus. For short Debye lengths we find a clear contribution of the polymer chains to the thermodiffusion coefficient, which fades out for longer Debye lengths, when the polymer chains fit into the electrostatic layer. On the other hand it turns out that the diffusion coefficient is less sensitive to the grafting and the theoretical expression of the second virial coefficient of rods can be applied to the bare and the grafted fd-virus. REFERENCES1.	J.K.G. Dhont and W.J. Briels, Eur. Phys. J. E 25, 61(2008).2.	H. Ning, J.K.G. Dhont, and S. Wiegand, Langmuir, 24, 2426(2008).3.	Z. Wang, H. Kriegs, J. Buitenhuis, J.K.G. Dhont, and S. Wiegand, Soft Matter, 9, 8697(2013).
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000204910 7001_ $$0P:(DE-Juel1)144087$$aWang, Zilin$$b1$$ufzj
000204910 7001_ $$0P:(DE-Juel1)130577$$aBuitenhuis, Johan$$b2$$ufzj
000204910 7001_ $$0P:(DE-Juel1)130616$$aDhont, Jan K.G.$$b3$$ufzj
000204910 8564_ $$uhttps://juser.fz-juelich.de/record/204910/files/SFS2015Wiegandnew.doc$$yOpenAccess
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