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000016810 084__ $$2WoS$$aPhysics, Fluids & Plasmas
000016810 084__ $$2WoS$$aPhysics, Mathematical
000016810 1001_ $$0P:(DE-HGF)0$$aPouget, E.$$b0
000016810 245__ $$aDynamics in the smectic phase of stiff viral rods
000016810 260__ $$aCollege Park, Md.$$bAPS$$c2011
000016810 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2011-10-17
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000016810 440_0 $$04924$$aPhysical Review E$$v84$$x1539-3755$$y4
000016810 500__ $$aThis project was supported by the European network of excellence SoftComp. We would like to thank Z. Dogic for providing us with the strain of the mutant virus fd-Y21M.
000016810 520__ $$aWe report on the dynamics in colloidal suspensions of stiff viral rods, called fd-Y21M. This mutant filamentous virus exhibits a persistence length 3.5 times larger than the wild-type fd-wt. Such a virus system can be used as a model system of rodlike particles for studying their self-diffusion. In this paper, the physical features, such as rod contour length and polydispersity have been determined for both viruses. The effect of viral rod flexibility on the location of the nematic-smectic phase transition has been investigated, with a focus on the underlying dynamics studied more specifically in the smectic phase. Direct visualization of the stiff fd-Y21M at the scale of a single particle has shown the mass transport between adjacent smectic layers, as found earlier for the more flexible rods. We could relate this hindered diffusion with the smectic ordering potentials for varying rod concentrations. The self-diffusion within the layers is far more pronounced for the stiff rods as compared to the more flexible fd-wt viral rod.
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000016810 7001_ $$0P:(DE-HGF)0$$aGrelet, E.$$b1
000016810 7001_ $$0P:(DE-Juel1)130797$$aLettinga, M.P.$$b2$$uFZJ
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000016810 8567_ $$uhttp://dx.doi.org/10.1103/PhysRevE.84.041704
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