V. Tirtaatmadja et al., SUPERPOSITION OF OSCILLATIONS ON STEADY SHEAR-FLOW AS A TECHNIQUE FORINVESTIGATING THE STRUCTURE OF ASSOCIATIVE POLYMERS, Macromolecules, 30(5), 1997, pp. 1426-1433
The viscoelastic properties over a range of steady shear conditions of
an alkali-swellable associative polymer have been determined using th
e technique of superposition of oscillations upon steady shear now, th
us enabling the structure of the polymer to be investigated. The assoc
iative polymer studied consists of a backbone of metharcylic acid and
ethyl acrylate to which is attached macromolecules containing C-20 hyd
rophobes via an ethylene oxide-isocyanate linkage. A 1 wt % solution w
ith its pH adjusted to 9.5 was used. At high pHs, the polymer solubili
zes to form a network of both intra- and intermolecular associating hy
drophobic junctions. The solution shows a non-power-law sheer-thinning
behavior: the viscosity now curve, when plotted against sheer stress,
shows two distinct regions where network rupture is prominent, at str
ess of 2 Pa and between 40 and 50 Pa By superimposing small amplitude
oscillations on to shear now at constant stresses, the network structu
re of the polymer is unperturbed and linear viscoelastic properties of
the polymer under the applied stress conditions can be obtained. At a
n applied stress of 2 Pa and above, bath the storage and loss moduli o
f the polymer are greatly reduced at low frequencies, with the G' appr
oaching second-order behavior and eta' tending toward constant values.
By analogy to Maxwell relaxation time, an estimate of the relaxation
time of the associative polymer at different stress conditions can be
made. The results show that the relaxation time is reduced by up to 4
orders of magnitude as the stress is increased from 1 to 60 Pa, while
a much smaller decrease in viscosity is observed. At sufficiently high
frequencies, both the storage and loss moduli show an increase above
their linear viscoelastic values as the strain amplitude is increased.
This behavior is believed to be dependent on the relaxation time of t
he polymer which is a function of the state of network disruption. Thu
s the technique may prove to be a powerful tool for probing the struct
ure of network polymer in solution.