The effect of phase-separated morphology on the rheological properties of polystyrene/poly(vinyl methyl ether) (PS/PVME) blend was investigated by optical microscopy (OM), light scattering (LS) method, and rheology. T...
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The crystallization, melting, and dissolution behavior of zinc stearate (ZnSt) in ZnSt-filled sulfonated poly(ethylene-co-propylene-co-ethylidene norbornene) (SEPDM) ionomers was studied by synchrotron small-angle X-r...
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The effect of liquid–liquid phase-separation (LLPS) on the crystallization behavior and mechanical properties of poly(ethylene- ran -vinyl acetate) (EVA) with various amounts of vinyl acetate and paraffin wax blend w...
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A new class of hydrogel precursor, dextran-maleic acid (Dex-MA), was synthesized by the reaction of dextran with maleic anhydride in the presence of the catalyst triethylamine. The effects of temperature, time, cataly...
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Thermal diffusivity measurements on three polymer melts were made using the Forced Rayleigh Light Scattering technique. The polymers, which were tested at room temperature where they are in the molten state, included ...
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A highly deacetylated chitosan from shrimp with a degree of deacetylation of 95.28 ± 3.03% was prepared and spun into a monofilament fiber using a solution of 4% (w/v) chitosan in 4% (v/v) aqueous acetic acid. Sa...
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Poly(amic acid) (PAA) and poly(amic diethyl ester) (PAE) precursors of poly(4,4′-oxydiphenylene biphenyltetracarboximide) (BPDA-ODA PI) were synthesized. Miscibility behaviors of these precursors with poly(arylene et...
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The dynamic mechanical properties and morphology of carboxylated polysulfone ionomers were investigated by dynamic mechanical thermal analysis and small-angle X-ray scattering (SAXS) techniques. It was found that at 2...
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Dewetting of polystyrene films on a silicon substrate is investigated as a function of film thickness h. We observe the nucleation of holes in the early stage of dewetting for relatively thick films (h>100Å), as ob...
Dewetting of polystyrene films on a silicon substrate is investigated as a function of film thickness h. We observe the nucleation of holes in the early stage of dewetting for relatively thick films (h>100Å), as observed previously, but the breakup of thinner films occurs through the growth of uniformly distributed surface undulations (“spinodal dewetting”). The average amplitude δh of these undulations increases exponentially up to the film rupture point where δh becomes comparable to h, as predicted by a capillary wave instability model.
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