The electrostatic binding of two anionic probe molecules, pyrenetetrasulfonic acid (4-PSA)
and 6-carboxyfluorescein (6-CF), to poly(allylamine hydrochloride) (PAH)/poly(sodium 4-styrenesulfonate)
(PSS) and poly(diallyldimethylammonium chloride) (PDADMAC)/PSS ultrathin multilayer films assembled
onto polystyrene (PS) latex particles has been examined using fluorescence spectroscopy. At the probe
concentrations studied, binding was observed only when the outermost layer was oppositely (positively)
charged to the probe. The amount of probe bound was found to increase linearly with polyelectrolyte
layer number up to about 11 layers (15 nm in thickness for the PAH/PSS films), with saturation binding
occurring beyond 11 layers. The binding data reveal that a minimum of about 10−30% of the cationic
charges of the polycations in the upper region of the multilayer films (where the probe binds) are not
directly electrostatically utilized in the multilayer assembly process through ion-pair binding to oppositely
charged sites on the polyanions. The removal of probe bound to multilayers of different thicknesses upon
subsequent exposure to PSS has also been examined. Evidence that polyelectrolyte multilayer films are
long-range electrostatically coupled systems is presented. The results obtained provide some insight into
the role and extent of electrostatic interactions in polyelectrolyte multilayers.
Osmotically induced deformations (invaginations) of polyelectrolyte capsules were observed in poly(styrene sulfonate, sodium salt) (PSS) solution since PSS of Mw 70 000 is excluded from the capsule interior. It was found that there is a critical osmotic pressure difference at which the initial spherical capsule shape becomes unstable and invaginations are formed. This critical osmotic pressure was obtained as a function of the wall thickness and the capsule size. A theoretical model is provided which describes the relationship between the critical osmotic pressure, the elasticity modulus, the capsule wall thickness, and the capsule radius. The model was verified by measuring the invagination onset as a function of particle radius and wall thickness. The elasticity modulus of the PSS/PAH (polyallylamine hydrochloride) polyelectrolyte multilayer was measured as a function of wall thickness and capsule diameter. The modulus ranges between 500 and 750 MPa, which indicates a relatively strongly interconnected polyelectrolyte multilayer structure. With higher molecular weight PAH the elasticity modulus of the PSS/PAH multilayer was slightly enhanced.PACS. 46.32.+x Static buckling and instability -68.60.Bs Mechanical and acoustical properties
Layer-by-layer (LbL) assembly of oppositely charged polyelectrolytes was used to coat fluorescein particles.
These particles, with a size of 4−9 μm, were prepared by precipitation of fluorescein at pH 2.
Polystyrensulfonate (PSS) and polyallylamine (PAH) were used to form a polyelectrolyte shell on the fluorescein
core. The permeation of fluorescein molecules through the polyelectrolyte shell during core dissolution was
monitored at pH 8 by the increasing fluorescence intensity as a result of dequenching. The number of
polyelectrolyte layers sufficient to sustain fluorescein release was found to be 8−10. Increasing the number
of layers prolonged the core dissolution time for minutes. The permeability of polyelectrolyte multilayers of
the thickness of 20 nm for fluorescein is about 10-9 m/s. The features of the release profile and possible
applications of the LbL method for shell formation in order to control release properties for entrapped materials
are outlined.
Exact control of the film thickness of polyelectrolyte shells (a transmission electron microscopy image is shown) is achieved by colloid-templated consecutive adsorption of polyanions and polycations followed by decomposition of the templating core. Possible areas of application for these shells range from the pharmaceutical, food, cosmetic, and paint industries to catalysis and microcrystallization.
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