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 159
... simulated by a gradient percolation technique . This approach consists in performing numerical simulations of 3D percolation on a L ' x L x L cubic lattice of length L ' in the x direction . The simple case of a constant gradient along ...
... simulated by a gradient percolation technique . This approach consists in performing numerical simulations of 3D percolation on a L ' x L x L cubic lattice of length L ' in the x direction . The simple case of a constant gradient along ...
Page 168
... simulations [ 19,21-24 ] for d > 2 systems in which both reac- tants diffuse , support the above predicted values for a and B. Indeed , Cornell et al [ 23 ] argue that the upper critical dimension is d = 2 and the MF approach should ...
... simulations [ 19,21-24 ] for d > 2 systems in which both reac- tants diffuse , support the above predicted values for a and B. Indeed , Cornell et al [ 23 ] argue that the upper critical dimension is d = 2 and the MF approach should ...
Page 188
... simulations . Excellent scaling is obtained with σ = 1.05 for d = 2 , and σ = 1.11 for d = 3 . Intuitively , one expects that for d = 3 the network is more floppy than for d = 2 , and this corresponds to the higher value of o . For ...
... simulations . Excellent scaling is obtained with σ = 1.05 for d = 2 , and σ = 1.11 for d = 3 . Intuitively , one expects that for d = 3 the network is more floppy than for d = 2 , and this corresponds to the higher value of o . For ...
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 simulations smectic Soft Order solvent spinodal spinodal decomposition string of blobs structure surface temperature theory twin velocity volume