DYNAMIC LIGHT-SCATTERING AND DYNAMIC VISCOELASTICITY OF POLY(VINYL ALCOHOL) IN AQUEOUS BORAX SOLUTIONS - 4 - FURTHER INVESTIGATION ON POLYMER CONCENTRATION AND MOLECULAR-WEIGHT DEPENDENCIES
A. Takada et al., DYNAMIC LIGHT-SCATTERING AND DYNAMIC VISCOELASTICITY OF POLY(VINYL ALCOHOL) IN AQUEOUS BORAX SOLUTIONS - 4 - FURTHER INVESTIGATION ON POLYMER CONCENTRATION AND MOLECULAR-WEIGHT DEPENDENCIES, Macromolecules, 31(2), 1998, pp. 436-443
Viscosity measurements are made on aqueous borax solutions of poly(vin
yl alcohol) (PVA) samples over a wide range of PVA concentration, C, t
o examine the hydrodynamic properties of associated polymers compared
to those of neutral polymers. The dynamic viscoelastic data are reanal
yzed using a statistical-mechanical theory for elastically effective c
hains in transient gels developed by Tanaka and Ishida. The viscosity
data are not superposed in the plot of viscosity against C[eta] using
the Huggins relationship, especially around and over a critical concen
tration, C-N, at which the dynamical behaviors drastically change and
an inflection point of a curve in the plot of the viscosity against C
is located. On the other hand, when we assume that the chain dimension
around C-N is the uperturbed one, the viscosity data around C-N is we
ll-superposed on a curve in the plot of viscosity against C/C-up wher
e C-up is the overlapping concentration of the unperturbed chain. The
inflection point of this composite curve is located at C/C-up = 1, w
hich infers that C-N corresponds to the overlapping concentration. All
data of the density of elastically effective chains, nu(eff), are sup
erposed on a curve in the plot of nu(eff)/nu against (C-C-N)/C-N where
nu is the density of polymer chains, which implies that C-N should be
regarded as a kind of gel point. Some discrepancies between the exper
imental data and the theoretical curve were observed, some of which ca
nnot be explained using the pairwise association of PVA chains.