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Interfaces fluctuations

This type of analysis is useful for studying the phase separation phenomena, also in detecting influences of external fields [218] (strain, etc.). In particular, by investigating speckles on scattering patterns, a certain information about interface fluctuations can be obtained [214]. [Pg.202]

Fig. 9.3. A schematic bell-shaped diagram of the distribution of electronic states of redox ions at an electrode/solution interface (fluctuation theory). (Reprinted with permission of the American Institute of Physics from J. O M. Bockris and S. U. M. Khan, Appl. Phys. Lett. 42 124 (1983). Fig. 9.3. A schematic bell-shaped diagram of the distribution of electronic states of redox ions at an electrode/solution interface (fluctuation theory). (Reprinted with permission of the American Institute of Physics from J. O M. Bockris and S. U. M. Khan, Appl. Phys. Lett. 42 124 (1983).
The interface itself is dynamics, non-planar and ill-defined, due to important local solvent mixing, and the position of the complexes with respect to the interface fluctuates much more than at classical aqueous interfaces. There is thus likely an equilibrium involving two types of positions for the strontium complex at the interface, which is consistent with cation exchange, as well as anion co-extraction mechanisms. [Pg.343]

The net dipoles of the water layer forming the interface fluctuate primarily around an axis with a tilt angle to the interface. Without any assumptions there are two opposite orientations of the water molecules possible directed to the air (or oil) phase are either the oxygen or hydrogen atoms directed to the air (or oil) phase. Frumkin (1956) suggests an orientation of the oxygen atoms to the gas phase. By evaluations of experimental data from the second harmonic generation Goh et al. (1988) have recently confirmed Frumkin s idea. [Pg.34]

Overall membrane compression Lipid-domain interface fluctuations Free volume fluctuations Local depressions and distortions Transient hydrophobic pores Transient hydrophilic pores Foot-in-the-door hydrophilic pores Composite hydrophilic pores Membrane enzyme changes Membrane macromolecule protrusion changes Rupture and REB not actually described (5) Suggested alternative to transient pores (6) Transport of nonpolar species (7) Possible precursors to hydrophilic pores (8, 9) Possible precursor to hydrophilic pores (10) Key to quantitative descriptions (10-16) Candidate metastable pores" Candidate metastable pores Coupling to membrane macromolecules (17) Candidate signaling change mechanism... [Pg.443]

Interface fluctuations are characterized by the parallel correlation length I, which determines the spatial decay of the height-height correlation function of the interface for large lateral distances R-R1,R = (x,y) ... [Pg.93]

Bare Ion Hopping For a high barrier in the electrochemical potential of the ion, the transfer is completely determined by the slow transition over this barrier, and the interface fluctuations just follow the ionic motion. Then, the derived equation for the rate constant reduces to the one obtained by Gurevich and Kharkats [117,118] and by Schmickler [120]. [Pg.35]

The mass of liquid in the container at any time was determined by means of a differential pressure measurement, taken with both manometers and differential pressure transducers, between the top and the bottom of the container and at intermediate points. Interface fluctuations were detectable but not significant for... [Pg.461]

Fig. 10.7 Data from a lithium tantalate crystal growth run showing the desired diameter (smooth curve), the measured diameter and the process power (arbitrary units). The run was restarted after 45 h. In addition to the interface transition at point A, which repeats at point D, the minor interface fluctuations at points B and C repeat at points E and F. Fig. 10.7 Data from a lithium tantalate crystal growth run showing the desired diameter (smooth curve), the measured diameter and the process power (arbitrary units). The run was restarted after 45 h. In addition to the interface transition at point A, which repeats at point D, the minor interface fluctuations at points B and C repeat at points E and F.
The disadvantage of this method is that the two phases have to coexist in the same simulation cell, including two interfaces (Due to the periodic boundary conditions, the interfaces are oriented parallel to a surface of the cubic simulation box, generating the fluid in a slab-like configuration. Hence, one faces the problem of slow equilibration of interface fluctuations, and to distinguish bulk properties from those of the interface region [97, 98, 99,100]). [Pg.15]


See other pages where Interfaces fluctuations is mentioned: [Pg.151]    [Pg.110]    [Pg.208]    [Pg.283]    [Pg.25]    [Pg.67]    [Pg.827]    [Pg.25]    [Pg.408]    [Pg.96]    [Pg.107]    [Pg.107]    [Pg.107]    [Pg.134]    [Pg.364]    [Pg.215]    [Pg.215]    [Pg.275]    [Pg.84]    [Pg.74]    [Pg.158]   
See also in sourсe #XX -- [ Pg.80 , Pg.83 ]




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