Finally, the attenuation behavior of stress waves and particle ve

Finally, the attenuation behavior of stress waves and particle velocities in the depth of the target

is analyzed, and it indicates an exponential decay. The corresponding empirical CA3 manufacturer formulas for the attenuation behavior are given based on the numerical results. (C) 2011 American Institute of Physics. [doi:10.1063/1.3633266]“
“The dielectric relaxation characteristics of conductive carbon black (CCB) reinforced ethylene acrylic elastomer (AEM) vulcanizates have been studied as a function of frequency (10(1)-10(6) Hz) at different filler loading over a wide range of temperatures (30-120 degrees C). The effect of filler loadings on the dielectric permittivity (epsilon’), loss tangent (tan delta), complex impedance (Z*), and electrical conductivity (sigma(ac)) were studied. The variation of epsilon’ with filler loading has been explained based on the interfacial polarization of the fillers within a heterogeneous system. The effect of filler loading on the imaginary AZD7762 (Z ”) and real (Z’) part of Z* were distinctly visible, which may be due to the relaxation dynamics of polymer chains at the polymerfiller interface. The frequency dependency of sigma(ac) has been investigated using percolation theory. The phenomenon of percolation in the composites has been discussed in terms of sigma(ac). The percolation threshold (phi(crit)) occurred in the range of 20-30 phr (parts per hundred) of filler loading. The effect

of temperature on tan delta, epsilon’, sigma(ac), and Nyquist plots VX-809 cell line of CCB-based AEM vulcanizates has been investigated. The CCB was uniformly dispersed within the AEM matrix as studied from the transmission electron microscope (TEM) photomicrographs. (C) 2011 Wiley Periodicals, Inc. J Appl Polym Sci, 2012″
“When a gash or gouge is made in a confluent layer of epithelial cells, the cells move to fill in the “”wound.” In some cases, such as in wounded embryonic chick wing buds, the movement of the cells is driven by cortical actin contraction (i.e., a purse string mechanism). In adult tissue, though, cells apparently crawl to close wounds. At the single cell level, this crawling is driven by the dynamics

of the cell’s actin cytoskeleton, which is regulated by a complex biochemical network, and cell signaling has been proposed to play a significant role in directing cells to move into the denuded area. However, wounds made in monolayers of Madin-Darby canine kidney (MDCK) cells still close even when a row of cells is deactivated at the periphery of the wound, and recent experiments show complex, highly-correlated cellular motions that extend tens of cell lengths away from the boundary. These experiments suggest a dominant role for mechanics in wound healing. Here we present a biophysical description of the collective migration of epithelial cells during wound healing based on the basic motility of single cells and cell-cell interactions.

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