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 75
... energy of the system , however they assume that the concentration changes within and between the phases ends at a ... free energy upon mixing is given by AGM = AH - TASm ( 1 ) Schematic plots of the free energy of mixing at a given ...
... energy of the system , however they assume that the concentration changes within and between the phases ends at a ... free energy upon mixing is given by AGM = AH - TASm ( 1 ) Schematic plots of the free energy of mixing at a given ...
Page 108
... free energy density of the chain is thus ( e / 2 ) ( de / ds ) 2 while the nematic free energy density is ( 3an S / 2 ) sin2 where is the local angle between a tangent to the chain and the nematic director n , s is the arc length ...
... free energy density of the chain is thus ( e / 2 ) ( de / ds ) 2 while the nematic free energy density is ( 3an S / 2 ) sin2 where is the local angle between a tangent to the chain and the nematic director n , s is the arc length ...
Page 110
... free energy by confinement or imposed chain - chain overlap . In certain cases the free energy of the LCP is lowered by tilt . However , this results in a distortion of the nematic medium and is thus penalized . The interplay between the ...
... free energy by confinement or imposed chain - chain overlap . In certain cases the free energy of the LCP is lowered by tilt . However , this results in a distortion of the nematic medium and is thus penalized . The interplay between the ...
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