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 83
... correlation length spans the sample , is connected , and is the matrix from which the " new phase " grows . A ... correlation length is obtained from the wave number at which the power spectrum attains its maximum . The " phase - phase ...
... correlation length spans the sample , is connected , and is the matrix from which the " new phase " grows . A ... correlation length is obtained from the wave number at which the power spectrum attains its maximum . The " phase - phase ...
Page 87
... correlation length , see Fig . 10. , also exhibits an initial growth period , followed by a plateau , and another rapid growth period . It is to be expected that the correlation length and area density behave similarly since the objects ...
... correlation length , see Fig . 10. , also exhibits an initial growth period , followed by a plateau , and another rapid growth period . It is to be expected that the correlation length and area density behave similarly since the objects ...
Page 156
... length of this model is Lc = [ y2 a2 / A ( 0 ) ] 1 / e , where = 4 - d . For d < de = 4 , the interface is kept ... correlation length & can be introduced as the characteristic length above which the term vt in the random force g ( x ...
... length of this model is Lc = [ y2 a2 / A ( 0 ) ] 1 / e , where = 4 - d . For d < de = 4 , the interface is kept ... correlation length & can be introduced as the characteristic length above which the term vt in the random force g ( x ...
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