Soft Order in Physical SystemsYitzhak Rabin, Robijn Bruinsma Une Perspective Historique; Y. Ne'eman. REVIEW PAPERS: Focal Conic Domains in Smectics; P. Boltenhagen, et al. On Polymer Brushes and Blobology; A. Halperin. RESEARCH PAPERS: Polymer Physics: NonDebye Screening in Polyelectrolyte Solutions; K. Kremer, et al. Polymers in a Random Environment and Molecular Quasi-Species; L. Peliti. Crystallography: Twins in Diamond Films; D. Shechtman. Dynamics of Disordered Systems/Glasses: Dynamics of Interface Depinning in a Disordered Medium; S. Stepanow, et al. Percolation, Diffusion, and Fractons: Hull of Percolation Clusters in Three Dimensions; J.M. Debierre. Dynamics of Diffusion and Invasion Fronts; J.F. Gouyet. Surfactants and Liquid Crystals: Vesicles of High Topological Genus; X. Michalet, et al. SCIENCE AND SOCIETY: Neo-Darwinian Processes in the Evolution of Science and of Human Societies; Y. Ne'eman. 19 additional articles. Index. |
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Page 165
... EQUATION OF THE CLUSTER DISTRIBUTION Using the connection - disconnection probabilities , it is in principle possible to formulate a Smoluchowski's rate equation for the distribution of clusters during a diffusion process : = ank 1 ...
... EQUATION OF THE CLUSTER DISTRIBUTION Using the connection - disconnection probabilities , it is in principle possible to formulate a Smoluchowski's rate equation for the distribution of clusters during a diffusion process : = ank 1 ...
Page 210
... equation 3 . If the income effect is larger than the price effect then dƊ / dp is positive . That means that the demand is an upward sloping function of the price level . If the price effect is larger than the income effect , then dD ...
... equation 3 . If the income effect is larger than the price effect then dƊ / dp is positive . That means that the demand is an upward sloping function of the price level . If the price effect is larger than the income effect , then dD ...
Page 233
... equation , 64 Ising model helicity flip , 178 liquid crystalline polymers in nematic solvents , 108-111 quasi - species model , 130 random - field , 156 Isotropic interface , FCDs , 26 Isotropic light scattering , 178 , 180 Iteration ...
... equation , 64 Ising model helicity flip , 178 liquid crystalline polymers in nematic solvents , 108-111 quasi - species model , 130 random - field , 156 Isotropic interface , FCDs , 26 Isotropic light scattering , 178 , 180 Iteration ...
Contents
An Historical Perspective Une Perspective Historique | 1 |
An Introduction | 33 |
The Adhesion Between Elastomers | 57 |
Copyright | |
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adsorption aerogels aggregate demand Alexander Alexander model area density behavior binodal blobological blobs boundary brush Chem concentration constant correlation length crosslinking crystal curve cyclide decrease deformation diffusion dimensional droplet Dupin cyclide dynamics edited elastic elastomers equation equilibrium experimental exponent FCD-I FCD's Figure film finite fluctuations focal conic domains fractal dimension fracton free energy function Gaussian curvature Gennes geometry grafted growth heptane income effect income redistribution increases inflation interactions interface Kleman lattice length scales Lett Macromolecules mixture molecules monomers nematic nucleation observed obtained Order in Physical parameter particles PDMS chains percolation clusters phase separation Phys Physical Systems plane polymer price level Rabin radius random walk regime region relaxation sample scattering semi-dilute solution shape factor smectic Soft Order solvent spinodal decomposition string of blobs structure surface temperature theory twin velocity volume