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 59
... plane shear mode ( mode II ) , and ( c ) the antiplane shear mode ( mode III ) , as depicted in figure 2. The superposition of the three modes describes the general case of loading . The mode I is technically the most important since it ...
... plane shear mode ( mode II ) , and ( c ) the antiplane shear mode ( mode III ) , as depicted in figure 2. The superposition of the three modes describes the general case of loading . The mode I is technically the most important since it ...
Page 126
... plane Imw > 0 of the plane w as a discrete subgroup of group of motion of Lobachevsky plane defined via relation : W → aw + b cw + d ' ad - bc = 1 Thus we can reduce our problem to the investigation of the random walk on the Lobachevsky ...
... plane Imw > 0 of the plane w as a discrete subgroup of group of motion of Lobachevsky plane defined via relation : W → aw + b cw + d ' ad - bc = 1 Thus we can reduce our problem to the investigation of the random walk on the Lobachevsky ...
Page 160
... planes cst ( i.e. , p = cst ) . This function is averaged over pairs of black particles which belong to the intersection of the hull with the plane at abscissa r and are a distance r apart . In the plane x = x , where p ( xc ) = Pc ...
... planes cst ( i.e. , p = cst ) . This function is averaged over pairs of black particles which belong to the intersection of the hull with the plane at abscissa r and are a distance r apart . In the plane x = x , where p ( xc ) = Pc ...
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