The dilatational rheology of the poly͑vinylacetate͒ monolayer onto an aqueous subphase with pHϭ2.0 has been studied between 1°C and 25°C. The combination of several techniques, relaxation after a step compression, oscillatory barrier experiments, electrocapillary waves, and surface light scattering ͑SLS͒ by thermal capillary waves, has allowed us to explore a broad frequency range. The relaxation experiments show multiexponential decay curves, whose complexity increases with decreasing the temperature. A regularization technique has been used to obtain the relaxation spectra from the relaxation curves and the dilatational viscoelastic parameters have been calculated from the spectra. The oscillatory barrier experiments confirm the results obtained from the step compression experiments. The dilatational viscosity increases very steeply in the frequency range 0.1-0.001 Hz. The shapes of the relaxation spectra follow the qualitative trends predicted a model recently proposed by Noskov ͓Colloid Polym. Sci. 273, 263 ͑1995͔͒. The temperature dependence of the fundamental relaxation time follows a Williams-Landel-Ferry equation above 14°C. These results correspond to the many-chain dynamics regime. The kilohertz region has been explored by the SLS technique. These results are compatible with the existence of a single Maxwell mode, with a relaxation time that has an Arrhenius-type temperature dependence. In the intermediate-frequency regime ͑10 Hz to 2 kHz͒ a further Maxwell process is found. It might correspond to the dynamics of loops and tails out of the surface plane.
Surface pressure isotherms and ellipsometric measurements of monolayers of two triblock symmetric
copolymers, poly(ethylene oxide)−poly(propylene oxide)−poly(ethylene oxide) (PEO−PPO−PEO), at the
air−water interface have been carried out. These copolymers are water-soluble, and the difference in
hydrophobicity between the blocks is small. This represents a different scenario for brush formation than
for most of the hydrophobic−hydrophilic block copolymers reported so far. The surface pressure curves
show two different phase transitions. The ellipsometric measurements indicate a thickness transition
when the monolayer saturates, which supports the hypothesis for brush formation. The experimental data
have been analyzed in terms of the scaling theory of adsorption of polymer brushes. Despite the possibility
of diffusion from the interface, the PPO block acts as an efficient anchoring element in the formation of
an adsorbed brush, once the adsorption sites at the interface are fully occupied. This is analogous to what
has been reported for diblock copolymers with a much larger difference in the hydrophobicity of the blocks.
The hydrophobicity of a particle surface can be tuned by the addition of surfactants that change the surface free energy for their attachment to a liquid interface. In this work, we report an experimental study where the wettability properties of silica nanoparticles are modified by the adsorption of alkyltrimethylammonium surfactants (C n TAB, n ¼ 12, 16) on the surface of the particles. We have pointed out that the wettability of the complexes is controlled by an intricate balance of electrostatic and hydrophobic interactions between the particle surface and the surfactant. These interactions play an important role in the structure of the surfactant-particle nanocomposite interfacial layer.
Multilayers of sodium salt of poly(4-styrene sulfonate) (PSS) and poly(diallyl dimethyl ammonium) chloride (PDADMAC) have been built layer by layer (LbL) both at the solid/aqueous interface (solid supported) and the air/aqueous interface (liquid supported). For the solid-supported multilayers, the adsorption kinetics and the complex shear modulus were measured using a dissipative quartz crystal microbalance and a null ellipsometer. A bubble tensiometer was used to measure the adsorption kinetics and the elasticity modulus of the liquid-supported multilayers. At the solid/aqueous interface, adsorption kinetics changes with the number of adsorbed layers. However, at the air/aqueous interface, PSS dynamics were the same for all adsorbed layers except the first. Conversely, the adsorption kinetics of PDADMAC at the air/water surface differed between those layers close to the interface and those far from it. Multilayers grow at the air/water interface by an intrinsic-charge-compensation process, whereas, for the same ionic strengths, solid-supported layers deposit by the extrinsic-charge-compensation process. No significant differences were found between the recoverable dilational storage modulus of the liquid-supported multilayers and the real part of the shear modulus of the solid-supported ones built at the same ionic strength. The values of the modulus are in the MPa range, which corresponds to gel-like films. This result is in agreement with the strong hydration degree of the LbL films calculated from ellipsometry measurements.
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