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>Dynamics of helical wormhyphen;like chains. XI. Translational diffusion with fluctuating hydrodynamic interaction
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Dynamics of helical wormhyphen;like chains. XI. Translational diffusion with fluctuating hydrodynamic interaction
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机译:Dynamics of helical wormhyphen;like chains. XI. Translational diffusion with fluctuating hydrodynamic interaction
The translational diffusion coefficientDof long enough polymer chains without excluded volume is studied on the basis of the discrete helical wormhyphen;like (HW) chain with partially fluctuating (orientationhyphen;dependent) hydrodynamic interaction (HI). In order to evaluateD(infin;) in the long time limit, which corresponds to diffusion experiments usually done on the long time scales, the timehyphen;dependent part ofDis explicitly treated by an application of the projection operator method. The result may be written asD(infin;)=D(Z)(1minus;dgr;0minus;dgr;1), whereD(Z)is the Zimm value with preaveraged HI, dgr;0is the relative decrease at timet=0 due to constraints, and dgr;1is the additional relative decrease att=infin; due to coupling between the translational motion and the Rouse vector (dielectric) modes for the HW chain, especially the long wavelength ones. It is found thatD(infin;) is decreased as the local conformation of the chain becomes rather compact, and thatD(infin;)=D(Z)(i.e., dgr;0=dgr;1=0) in the stiffhyphen;chain limit. Thus the ratio rgr; of the roothyphen;meanhyphen;square radius of gyration to the hydrodynamic radius defined fromDis not a universal constant but depends on the chain conformation and stiffness. A comparison of theory with experiment is made with respect to rgr;, and it is found that the theory may well explain experimental results. For comparison, also for the Gaussian chain (springndash;bead model), which is an unconstrained chain,D(infin;) is evaluated, and it is found that dgr;0=0 but dgr;1ne;0.
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