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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Results 1-3 of 27
Page 157
... exponent z is obtained by combining ( 11 ) with the relation ( L ) t ~ L2 as z = 2 - ( e ) / 3 . The velocity exponent is derived from v = μ ( L ) ƒ by using ( 11 ) with L ~ έ as = 1-1 . The correlation length exponent § 0 vis obtained ...
... exponent z is obtained by combining ( 11 ) with the relation ( L ) t ~ L2 as z = 2 - ( e ) / 3 . The velocity exponent is derived from v = μ ( L ) ƒ by using ( 11 ) with L ~ έ as = 1-1 . The correlation length exponent § 0 vis obtained ...
Page 163
... exponent . The Roux - Guyon result giving the invasion probability of finite clusters during a slow drainage process is shown to be valid only in d = 2 dimensions . The disconnection - reconnection exponent Y valid in d = 1 , 2 and 6 ...
... exponent . The Roux - Guyon result giving the invasion probability of finite clusters during a slow drainage process is shown to be valid only in d = 2 dimensions . The disconnection - reconnection exponent Y valid in d = 1 , 2 and 6 ...
Page 184
Yitzhak Rabin, Robijn Bruinsma. μ is the conductivity exponent and the exponent of the transverse susceptibility X1 defined as x1 ( p ) x ( p − pc ) ̄ ” , respectively . - For έ , one has f ( x ) x x1 - AP for « 1 , reflecting the ...
Yitzhak Rabin, Robijn Bruinsma. μ is the conductivity exponent and the exponent of the transverse susceptibility X1 defined as x1 ( p ) x ( p − pc ) ̄ ” , respectively . - For έ , one has f ( x ) x x1 - AP for « 1 , reflecting 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