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 25
... molecules are normal to the surface ; within the islands occupied by the bases of FCD - I's the molecules are tangentially anchored , see Fig.16 c . The surface energies // and σ for these two types of molecular alignment are not equal ...
... molecules are normal to the surface ; within the islands occupied by the bases of FCD - I's the molecules are tangentially anchored , see Fig.16 c . The surface energies // and σ for these two types of molecular alignment are not equal ...
Page 129
... molecules , whose structure may be described by a collection of N binary variables , S1 = ± 1 , i = 1,2 , ... , N. Then the fractions of molecules of structure S = ( S1 , S2 , ... , SN ) obeys the following evolution equation : 1 xg ( t ...
... molecules , whose structure may be described by a collection of N binary variables , S1 = ± 1 , i = 1,2 , ... , N. Then the fractions of molecules of structure S = ( S1 , S2 , ... , SN ) obeys the following evolution equation : 1 xg ( t ...
Page 130
... molecules are non- overlapping and that the number of molecules in the population is sufficiently large to neglect fluctuations in the x ( t ) . It was shown by I. Leuthäusser3 that the quasi - species model corresponds to a problem in ...
... molecules are non- overlapping and that the number of molecules in the population is sufficiently large to neglect fluctuations in the x ( t ) . It was shown by I. Leuthäusser3 that the quasi - species model corresponds to a problem in ...
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