H-1-NMR SELF-DIFFUSION AND MULTIFIELD H-2 SPIN RELAXATION STUDY OF MODEL ASSOCIATIVE POLYMER AND SODIUM DODECYL-SULFATE AGGREGATION IN AQUEOUS-SOLUTION
S. Abrahmsenalami et P. Stilbs, H-1-NMR SELF-DIFFUSION AND MULTIFIELD H-2 SPIN RELAXATION STUDY OF MODEL ASSOCIATIVE POLYMER AND SODIUM DODECYL-SULFATE AGGREGATION IN AQUEOUS-SOLUTION, Journal of physical chemistry, 98(25), 1994, pp. 6359-6367
H-1 NMR self-diffusion and multifield H-2 spin relaxation measurements
were applied in a study of the aggregation of a model associative pol
ymer (MAP) in aqueous solution. The polymer is based on a poly(oxyethy
lene) backbone with ether-linked alkyl chains ends. The aggregation wa
s studied also in presence of sodium dodecyl sulfate (SDS) at a high c
oncentration. Associative polymers self-assemble in aqueous solution i
nto what is generally believed to be micelle-like aggregates with the
hydrophobic end groups situated in the micellar core. In binary soluti
ons of polymer and water such polymer aggregates were found to display
an extensive polydispersity which increased with polymer concentratio
n, as based on experimental self-diffusion data. Corresponding measure
ments on mixed solutions of high SDS concentration, on the other hand,
indicate that SDS micelles act as seeds for aggregation, promoting a
markedly lower polydispersity for these mixed aggregates. H-2 spin rel
axation data on SDS molecules in mixed aggregates were found to be con
sistent with a two-step motional model for chain reorientation. The fa
st local anisotropic motions of the SDS molecules inside the aggregate
s were found not to be particularly influenced by the addition of poly
mer, whereas the slow isotropic motions of the SDS molecules, such as
aggregate tumbling and lateral diffusion of SDS over the curved aggreg
ate surface, were considerably retarded. The increased size of the mix
ed aggregates upon addition of polymer is probably the main reason for
this retardation of reorientational dynamics. However, the motion of
the polymer in the mixed aggregates and in single-component polymer ag
gregates could not be described by the same motional model; instead a
three-step motional model had to be applied. The additional very slow
motion component was interpreted to be a reptational or exchange motio
n of the polymer inside or between aggregates.