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Brownian motion disordered systems

Polymerization in microemulsions allows the synthesis of ultrafine latex particles in the size range of 5 to 50 nm with a narrow size distribution [33], The deposition of an ordered monolayer of such spheres is known to be increasingly difficult as the diameter of such particles decreases [34], Vigorous Brownian motion and capillary effects create a state of disorder in the system that is difficult... [Pg.294]

To characterize the dynamic movement of particles on a fractal object, one needs two additional parameters the spectral or fracton dimension ds and the random-walk dimension dw. Both terms are quite important when diffusion phenomena are studied in disordered systems. This is so since the path of a particle or a molecule undergoing Brownian motion is a random fractal. A typical example of a random fractal is the percolation cluster shown in Figure 1.5. [Pg.26]

Chapter 8 by W. T. Coffey, Y. P. Kalmykov, and S. V. Titov, entitled Fractional Rotational Diffusion and Anomalous Dielectric Relaxation in Dipole Systems, provides an introduction to the theory of fractional rotational Brownian motion and microscopic models for dielectric relaxation in disordered systems. The authors indicate how anomalous relaxation has its origins in anomalous diffusion and that a physical explanation of anomalous diffusion may be given via the continuous time random walk model. It is demonstrated how this model may be used to justify the fractional diffusion equation. In particular, the Debye theory of dielectric relaxation of an assembly of polar molecules is reformulated using a fractional noninertial Fokker-Planck equation for the purpose of extending that theory to explain anomalous dielectric relaxation. Thus, the authors show how the Debye rotational diffusion model of dielectric relaxation of polar molecules (which may be described in microscopic fashion as the diffusion limit of a discrete time random walk on the surface of the unit sphere) may be extended via the continuous-time random walk to yield the empirical Cole-Cole, Cole-Davidson, and Havriliak-Negami equations of anomalous dielectric relaxation from a microscopic model based on a... [Pg.586]

During the flow through the capillary the macromolecules are orientated to the direction of the force action. According to the Boltzmann s theory, any process of molecular orientation corresponds to an entropycal state lower than that characteristic of the entirely random state. Hence, the polymer entropy at the capillary outlet is lower than the initial one. On the other hand, the brownian motion tends to disorder the system and in case of a slow flow this process can prevail preventing from the orientation. But in case of the rapid flow of very big macromolecules the orientation effect is quite marked. [Pg.38]


See other pages where Brownian motion disordered systems is mentioned: [Pg.397]    [Pg.286]    [Pg.419]    [Pg.426]    [Pg.741]    [Pg.47]    [Pg.194]    [Pg.17]    [Pg.494]    [Pg.136]    [Pg.494]   
See also in sourсe #XX -- [ Pg.287 , Pg.288 , Pg.289 , Pg.290 , Pg.291 , Pg.292 ]

See also in sourсe #XX -- [ Pg.287 , Pg.288 , Pg.289 , Pg.290 , Pg.291 , Pg.292 ]




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Brownian motion

Disordered systems

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