Molecular dynamics and Monte Carlo simulations often rely on Lennard-Jones (LJ) potentials for nonbond interactions. We present 12-6 and 9-6 LJ parameters for several face-centered cubic metals (Ag, Al, Au, Cu, Ni, Pb, Pd, Pt) which reproduce densities, surface tensions, interface properties with water and (bio)organic molecules, as well as mechanical properties in quantitative (<0.1%) to good qualitative (25%) agreement with experiment under ambient conditions. Deviations associated with earlier LJ models have been reduced by 1 order of magnitude due to the precise fit of the new models to densities and surface tensions under standard conditions, which also leads to significantly improved results for surface energy anisotropies, interface tensions, and mechanical properties. The performance is comparable to tight-binding and embedded atom models at up to a million times lower computational cost. The models extend classical simulation methods to metals and a variety of interfaces with biopolymers, surfactants, and other nanostructured materials through compatibility with widely used force fields, including AMBER, CHARMM, COMPASS, CVFF, OPLS-AA, and PCFF. Limitations include the neglect of electronic structure effects and the restriction to noncovalent interactions with the metals.
The effect of silicate functionalization, anneal temperature,
polymer molecular weight, and
constituent interactions on polymer melt intercalation of a variety of
styrene-derivative polymers in
alkylammonium-functionalized silicates is examined. Hybrid
formation requires an optimal interlayer
structure for the organically-modified layered silicate (OLS), with
respect to the number per host area
and size of the alkylammonium chains, as well as the presence of polar
interactions between the OLS
and polymer. From these observations and the qualitative
predictions of the mean-field lattice-based
model of polymer melt intercalation (preceding paper in this issue),
general guidelines may be established
for selecting potentially compatible polymer−OLS systems. The
interlayer structure of the OLS should
be optimized to maximize the configurational freedom of the
functionalizing chains upon layer separation
while maximizing potential interaction sites with the surface. The
most successful polymers for
intercalation exhibited polar character or contained Lewis-acid/base
groups.
The thermal stability of organically modified layered silicate (OLS) plays a key role in the synthesis and processing of polymer-layered silicate (PLS) nanocomposites. The nonoxidative thermal degradation of montmorillonite and alkyl quaternary ammonium-modified montmorillonite were examined using conventional and high-resolution TGA combined with Fourier transform infrared spectroscopy and mass spectrometry (TG-FTIR-MS) and pyrolysis/GC-MS. The onset temperature of decomposition of these OLSs was approximately 155 °C via TGA and 180 °C via TGA-MS, where TGA-MS enables the differentiation of water desorbtion from true organic decomposition. Analysis of products (GC-MS) indicates that the initial degradation of the surfactant in the OLS follows a Hoffmann elimination reaction and that the architecture (trimethyl or dimethyl), chain length, surfactant mixture, exchanged ratio, or preconditioning (washing) does not alter the initial onset temperatures. Catalytic sites on the aluminosilicate layer reduce thermal stability of a fraction of the surfactants by an average of 15-25 °C relative to the parent alkyl quaternary ammonium salt. Finally, the release of organic compounds from the OLS is staged and is associated with retardation of product transfer arising from the morphology of the OLS. These observations have implications to understanding the factors impacting the interfacial strength between polymer and silicate and the subsequent impact on mechanical properties as well as clarifying the role (advantageous or detrimental) of the decomposition products in the fundamental thermodynamic and kinetic aspects of polymer melt intercalation.
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