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Dynamics of Polymer Molecules in Dilute Solution: Viscoelasticity, Flow Birefringence and Dielectric Loss

J. Chem. Phys. 24, 269 (1956); doi:10.1063/1.1742462

Issue Date: February 1956

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Bruno H. Zimm
General Electric Research Laboratory, The Knolls, Schenectady, New York
The problem of the motions of a chain molecule diffusing in a viscous fluid under the influence of external forces or currents is considered for a particular model. This model is a chain of beads connected by ideal springs. Hydrodynamic interaction between the beads is introduced in the approximate form due to Kirkwood and Riseman. It is possible to solve this problem exactly with the use of a transformation to a set of normal coordinates. The viscosity, birefringence of flow, and dielectric and tensile relaxation behavior are calculated explicitly. The intrinsic viscosity in steady flow is somewhat different from the Kirkwood-Riseman result, and there is no change of viscosity with shear rate. The spectrum of relaxation times is similar to that found by Rouse and by F. Bueche, but has its maximum at a lower frequency than those obtained by Kuhn and Kuhn and by Kirkwood and Fuoss in other ways. The Journal of Chemical Physics is copyrighted by The American Institute of Physics.
History: Received May 24, 1955
Permalink: http://link.aip.org/link/?JCPSA6/24/269/1
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ISSN:
0021-9606 (print)   1089-7690 (online)
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REFERENCES (31)

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  25. Kirkwood (reference 14) has used a tensor notation for the same quantitites. In his case the use of generalized curvilinear coordinates made desirable explicit recognition of the tensor properties of the operators. In our case the transformation to normal coordinates emphasizes essentially matrix manipulations.
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  30. The inversion of H to obtain Eqs. (92) and (93) is not a trivial matter for the non-free-draining case. I am indebted to Dr. P. L. Auer and Dr. C. S. Gardner for a private communication containing this result. The validity of Eq. (30) with Eq. (92) can be directly established by replacing r with the substitution r = (p−1)/(p+1) and using contour integration along a branch cut on the positive real axis of p and a circle at infinity (see reference 28).
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  32. P. L. Auer and C. S. Gardner [J. Chem. Phys. 23, 1545 (1955)] have obtained a value of 2.90 from a recalculation of the Kirkwood-Riseman result.
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  35. Courant and Hilbert, Methoden der Mathematischen Physik (Verlag Julius Springer, Berlin, 1924);
  36. Margenau and Murphy, The Mathematics of Physics and Chemistry (D. van Nostrand Company, Inc., New York, 1943).

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