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Rigidity threshold

The temperature at the surface of the sphere is determined by the evaporation rate obtained from simultaneous mass and heat transfer. Under some drying conditions, the heat transfer is the slow step, limiting evaporation, and in others the mass transfer is the slow step. The surface of the green body will continue to stay wet if the green body shrinks, expelling the solution, or sm-face tension driven flow continues to supply liquid. Shrinkage stops when the rigidity threshold of the particle network is reached. [Pg.694]

Several muscle problems may occur at higher doses. Examples include involuntary tremors, writhing, shivering, and jerky movements catatonia, a zombielike state characterized by changes in muscle tone and bizarre posturing muscle rigidity and immobility and loss of balance and dizziness. Many PCP abusers will notice an anesthetic effect resulting in increased pain threshold or numbness. [Pg.413]

The matrix polymer has to be rather rigid to conserve the empty imprinted sites after extraction of the template, this is achieved by extensive crosslinking. Generally, the crosslinker content of a mixture has to exceed a threshold value (>40%) to obtain selectivity [444,447]. Further, the chemical structure of the polymer network is of minor importance for the selectivity, though its polarity should be adapted to the imprinting molecule [444]. To obtain a maximum number of accessible sites,... [Pg.158]

The percolation model suggests that it may not be necessary to have a rigid geometry and definite pathway for conduction, as implied by the proton-wire model of membrane transport (Nagle and Mille, 1981). For proton pumps the fluctuating random percolation networks would serve for diffusion of the ion across the water-poor protein surface, to where the active site would apply a vectorial kick. In this view the special nonrandom structure of the active site would be limited in size to a dimension commensurate with that found for active sites of proteins such as enzymes. Control is possible conduction could be switched on or off by the addition or subtraction of a few elements, shifting the fractional occupancy up or down across the percolation threshold. Statistical assemblies of conducting elements need only partially fill a surface or volume to obtain conduction. For a surface the percolation threshold is at half-saturation of the sites. For a three-dimensional pore only one-sixth of the sites need be filled. [Pg.150]

We do not know a lot however about the second point, because the deformability of a highly polydisperse brush is not easy to model. We have begun to understand how a monodisperse brush responds to a shear stress [25], and qualitatively we expect these dense structures to be far more rigid than the weakly dense surface layers investigated in 3.2. It is thus plausible that the threshold for the onset of strong slip appears at higher shear rates for dense surface layers than for weakly dense ones, as observed experimentally. Up to now we do not have predictions for the molecular weight dependence of these thresholds. [Pg.352]

The results of calculations of the effective Poisson s ratio vp dependence on the bulk concentration of a rigid phase p at various values of a = log i/C/Au) are shown in Fig. 53. The calculations were made for Poisson s ratios of the phases ranging from 0.1 to 0.4. It can be seen that at percolation threshold Poisson s ratio of the isotropic fractal composite is vp = 0.2, when K jK > 0 it is also independent of the Poisson s ratios of the individual components of the composite. The Poisson s ratio obtained by us near the percolation threshold is in agreement with computer simulation results and the conjecture of Arbabi and Sahimi [161]. It has been shown that an approximate theoretical treatment of percolation on a cubic lattice exactly reproduces the Poisson s ratio obtained in computer simulation at the percolation threshold. This result may encourage one to use this approximation to describe various elastic properties of composites. It is worth noting that some critical indices have been calculated recently with a high degree of accuracy in the context of the present model. [Pg.214]


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