The Bi nanoclusters were fabricated by thermal evaporation at EX 527 cost room temperature on transmission electron microscope grids coated with an ultrathin carbon film, followed by thermal and femtosecond laser annealing. The annealed sample had an average cluster
size of similar to 14 nm along the minor axis and similar to 16 nm along the major axis. The Debye temperature of the annealed nanoclusters was found to be 53 +/- 6 K along the [012] direction and 86 +/- 9 K along the [110] direction. At T=464 +/- 6 K, the diffraction intensity started to deviate from Debye-Waller behavior due to increased lattice anharmonicity. The onset of the melting of the Bi nanoclusters was T similar to 500 +/- 6 K, as measured by the reduction of the nanocluster size through the formation of a liquid shell detected by the width of the diffraction rings. The thermal expansion coefficient of the Bi (012) and (110) planes is positive up to similar to 499 +/- 11 K. However, the expansion coefficient of the Bi (012) planes showed a transition from a positive to a negative value that occurs over the temperature range
Luminespib ic50 T(c) similar to 499 +/- 11 K to 511 +/- 8 K. For the Bi (110) planes, the thermal expansion coefficient is positive up to their melting point, which is 525 +/- 6 K. (C) 2011 American Institute of Physics. [doi: 10.1063/1.3565028]“
“This study compares the effects of two different types of nanosized fillers (silica and montmorillonite) at three different weight fractions as well their mixtures on the thermomechanical properties of polylactide (PLA). The role of aggregation and interphase
was investigated in terms of several experimental Selleckchem JIB 04 techniques, including scanning electron microscopy, wide-angle X-ray scattering (WAXS), thermogravimetric analysis, differential scanning calorimetry, dynamic mechanical analysis (DMA), and tensile measurements. The experimental results clearly suggest that silica and montmorillonite have different reinforcing and toughening effects on PLA, while the combination of the two different nanofillers has a detrimental effect on the tensile properties of the material. Four micromechanics models describing the Young’s modulus of the nanocomposites were used to study the different matrix-nanofiller interactions. The best fit of the experimental results was obtained with a model that assumes the presence of an interphase surrounding each nanoparticle. The increase of the nanofiller content above a certain amount was not accompanied by a corresponding increase of the interphase, because the total nanofiller surface area was counterbalanced by the creation of aggregates. It is postulated that the aggregation effect acts antagonistically to the interphase effect. (C) 2011 Wiley Periodicals, Inc.