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Diffusion of a sphere in a dilute solution of polymer coils
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10.1063/1.3216108
/content/aip/journal/jcp/131/9/10.1063/1.3216108
http://aip.metastore.ingenta.com/content/aip/journal/jcp/131/9/10.1063/1.3216108

Figures

Image of FIG. 1.
FIG. 1.

A tracer sphere with radius is suspended in a dilute solution of polymer coils with radii of gyration . In a model with hard-sphere interactions, the centers of mass of the polymer coils cannot pass the dashed surface with radius .

Image of FIG. 2.
FIG. 2.

We model the polymer coils as hard spheres of radius concerning the interactions with the tracer sphere and as solid sphere of radius and a no-slip boundary condition on the surface concerning the interactions with the solvent.

Image of FIG. 3.
FIG. 3.

and (solid blue and dashed red lines, respectively) defined via as functions of for different values of the ratio . The value of for neighboring curves for the lowest six curves differs by 0.1. Squares and circles indicate the results for the long and short time diffusion constants of hard spheres , respectively, according to Ref. 5.

Image of FIG. 4.
FIG. 4.

and (solid blue and dashed red lines, respectively) for large polymers in good solvent conditions as function of . Also shown is the result for the generalized Stokes–Einstein relation equation (28), which is independent of . In this approximation short and long time diffusion constants are equal.

Image of FIG. 5.
FIG. 5.

Diffusion coefficient of a polystyrene sphere of radius in a solution of PEO polymers with molecular masses of 18 500 amu (squares), (circles), and (triangles) from Ref. 8. The solid, dashed, and dashed-dotted lines, respectively, indicate the theoretical predictions for according to Eq. (25). There is no adjustable parameter.

Image of FIG. 6.
FIG. 6.

Normalized diffusion coefficients of spheres with radius and 51.7 nm (circle and square, respectively) in a solution of PEO with a molecular mass of from Ref. 8. Dashed and dashed-dotted lines are theoretical predictions for and for in first order in polymer concentration from Eqs. (25) and (21), respectively. For , and are almost identical (corresponding to , see Fig. 4) and we only plot (solid line).

Tables

Generic image for table
Table I.

The exponents from Eq. (31) as measured in experiments compared to our theoretical prediction given by Eq. (33).

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/content/aip/journal/jcp/131/9/10.1063/1.3216108
2009-09-01
2014-04-16
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Diffusion of a sphere in a dilute solution of polymer coils
http://aip.metastore.ingenta.com/content/aip/journal/jcp/131/9/10.1063/1.3216108
10.1063/1.3216108
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