TY - JOUR
T1 - Diffusion of Spheres in Entangled Polymer Solutions
T2 - A Return to Stokes-Einstein\ Behavior
AU - Won, Jongok
AU - Onyenemezu, Clement
AU - Miller, Wilmer G.
AU - Lodge, Timothy P.
N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 1994/12/1
Y1 - 1994/12/1
N2 - Dynamic light scattering has been used to follow the tracer diffusion of polystyrene spheres (R ≈ 200 nm) in dilute, semidilute, and entangled solutions of poly(vinyl methyl ether) (Mw = 1.3 × 106). Over this range of matrix concentrations, 0 ≤ c[ƞ] ⩽ 36, the diffusivity drops by almost 5 orders of magnitude. Near c* (≈[ƞ]−1) for the matrix, the diffusivity exceeds that estimated from the bulk solution viscosity via the Stokes-Einstein relation by a factor of about 3. Such “positive deviations” from Stokes-Einstein behavior have been reported previously in several systems. However, once the matrix concentration is sufficiently high for entanglements to be effective, Stokes-Einstein behavior is recovered. This new result was confirmed via forced Rayleigh scattering. In addition, these data can reconcile measurements of sphere diffusion with reptation-based models for chain mobility in well-entangled systems. The behavior near c* is discussed in terms of the matrix correlation length, ξ, which has a maximum at ξ ≈ Rg for c ≈ c*. It is noted that the fluid layer within a distance ξ of the sphere surface will, in general, differ in composition from the bulk solution, and consequently the sphere mobility may well not sense the macroscopic solution viscosity, particularly near c*. As a corollary, for large matrix chains, dynamic light scattering may not monitor the long-time diffusion of the spheres near c*, because q ξ ≈ qRg ≈ 1, rather than q ξ ≪ 1.
AB - Dynamic light scattering has been used to follow the tracer diffusion of polystyrene spheres (R ≈ 200 nm) in dilute, semidilute, and entangled solutions of poly(vinyl methyl ether) (Mw = 1.3 × 106). Over this range of matrix concentrations, 0 ≤ c[ƞ] ⩽ 36, the diffusivity drops by almost 5 orders of magnitude. Near c* (≈[ƞ]−1) for the matrix, the diffusivity exceeds that estimated from the bulk solution viscosity via the Stokes-Einstein relation by a factor of about 3. Such “positive deviations” from Stokes-Einstein behavior have been reported previously in several systems. However, once the matrix concentration is sufficiently high for entanglements to be effective, Stokes-Einstein behavior is recovered. This new result was confirmed via forced Rayleigh scattering. In addition, these data can reconcile measurements of sphere diffusion with reptation-based models for chain mobility in well-entangled systems. The behavior near c* is discussed in terms of the matrix correlation length, ξ, which has a maximum at ξ ≈ Rg for c ≈ c*. It is noted that the fluid layer within a distance ξ of the sphere surface will, in general, differ in composition from the bulk solution, and consequently the sphere mobility may well not sense the macroscopic solution viscosity, particularly near c*. As a corollary, for large matrix chains, dynamic light scattering may not monitor the long-time diffusion of the spheres near c*, because q ξ ≈ qRg ≈ 1, rather than q ξ ≪ 1.
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U2 - 10.1021/ma00103a020
DO - 10.1021/ma00103a020
M3 - Article
AN - SCOPUS:0028765985
SN - 0024-9297
VL - 27
SP - 7389
EP - 7396
JO - Macromolecules
JF - Macromolecules
IS - 25
ER -