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Waves, of concentration

The solution of the first kind is stable and arises as the limit, t —> oo, of the non-stationary kinetic equations. Contrary, the solution of the second kind is unstable, i.e., the solution of non-stationary kinetic equations oscillates periodically in time. The joint density of similar particles remains monotonously increasing with coordinate r, unlike that for dissimilar particles. The autowave motion observed could be classified as the non-linear standing waves. Note however, that by nature these waves are not standing waves of concentrations in a real 3d space, but these are more the waves of the joint correlation functions, whose oscillation period does not coincide with that for concentrations. Speaking of the auto-oscillatory regime, we mean first of all the asymptotic solution, as t —> oo. For small t the transient regime holds depending on the initial conditions. [Pg.483]

Figure 2..30. Schematic of light scattering on Debye s thermoelastic waves or on fluctuation waves of concentration... Figure 2..30. Schematic of light scattering on Debye s thermoelastic waves or on fluctuation waves of concentration...
Now consider planes or waves of higher concentration which rise from the base of the vessel. At time t a plane of concentration C has risen a distance h from the base. Thus the velocity at which a plane of concentration C rises from the base is h/t. This plane or wave of concentration passes up through the suspension. The velocity of the particles relative to the plane is therefore ... [Pg.60]

Here, is the velocity with which a wave of concentration Cg travels along the column (the z-direction). For a given Cg, the above expression provides a unique relation between the location z along the column and time t since... [Pg.491]

As discussed in Section 1.6, there have been several waves of concentrated fuel cell research and development, each driven by a somewhat different impetus. Throughout the... [Pg.1]

Fig. 3.17 The two possible sets of standing waves at the Brillouin zone boundary. Standing wave A concentrates electron density at the nuclei, whereas wave B concentrates electron density between the nuclei. Wave A thus has a lower energy than wave B. Fig. 3.17 The two possible sets of standing waves at the Brillouin zone boundary. Standing wave A concentrates electron density at the nuclei, whereas wave B concentrates electron density between the nuclei. Wave A thus has a lower energy than wave B.
Eor a linear system f (c) = if, so the wave velocity becomes independent of concentration and, in the absence of dispersive effects such as mass transfer resistance or axial mixing, a concentration perturbation propagates without changing its shape. The propagation velocity is inversely dependent on the adsorption equiUbrium constant. [Pg.261]

As the nanotube diameter increases, more wave vectors become allowed for the circumferential direction, the nanotubes become more two-dimensional and the semiconducting band gap disappears, as is illustrated in Fig. 19 which shows the semiconducting band gap to be proportional to the reciprocal diameter l/dt. At a nanotube diameter of dt 3 nm (Fig. 19), the bandgap becomes comparable to thermal energies at room temperature, showing that small diameter nanotubes are needed to observe these quantum effects. Calculation of the electronic structure for two concentric nanotubes shows that pairs of concentric metal-semiconductor or semiconductor-metal nanotubes are stable [178]. [Pg.71]

An explosion is defined by StrelUow and Baker " as an event in wliich energy is released over a sufficiently small period of time and in a sufficiently small volmne to generate a pressure wave of finite amplitude traveling away from tlie source. Tliis energy may have been originally stored in tlie system as chemical, nuclear, electrical, or pressure energy. However, tlie release is not considered to be explosive unless it is rapid and concentrated enough to produce a pressure wave tliat can be heard. [Pg.221]

The accuracy of the method depends upon the precision with which the two volumes of solution and the corresponding diffusion currents are measured. The material added should be contained in a medium of the same composition as the supporting electrolyte, so that the latter is not altered by the addition. The assumption is made that the wave height is a linear function of the concentration in the range of concentration employed. The best results would appear to be obtained when the wave height is about doubled by the addition of the known amount of standard solution. This procedure is sometimes referred to as spiking. [Pg.605]

Two procedures may be employed (1) that dependent upon wave height-concentration plots, and (2) the method of standard additions. The theory has been given in Section 16.5. [Pg.619]

Wave-height-concentration plot 604 Wave height measurement of, 605 Wavelengths approximate of colours, 646 limits of various types of radiation, 647 units for, 647 Wave numbers 646... [Pg.877]

Fig. 4 Concentration waves of CO observed at the reactor outlet after reaching cyclic steady state... Fig. 4 Concentration waves of CO observed at the reactor outlet after reaching cyclic steady state...
The reduction wave of peroxydisulphate at dme starts at the potential of the anodic dissolution of mercury. The current-potential curve exhibits certain anomalous characteristics under various conditions. At potentials more negative than the electrocapillary maximum, a current minimum can be observed this is due to the electrostatic repulsion of the peroxydisulphate ion by the negatively charged electrode surface. The current minimum depends on the concentration and nature of the supporting electrolyte, and can be eliminated by the adsorption of capillary active cations of the type NR4. ... [Pg.548]

In Range Al, a negative current wave was found in the polarogram at the W/DCE interface (cf Fig. 8). After the electrolysis by applying E ppi in the range at the W/DCE interface, CQ was produced as the dominant species in DCE, H2O2 of concentration less than that of CQ was produced in W, and an obvious change of pH in W was observed in the absence of pH buffer. The reaction of Eq. (18) is consistent with the experimental results ... [Pg.510]

Although NMRI is a very well-suited experimental technique for quantifying emulsion properties such as velocity profiles, droplet concentration distributions and microstructural information, several alternative techniques can provide similar or complementary information to that obtained by NMRI. Two such techniques, ultrasonic spectroscopy and diffusing wave spectroscopy, can be employed in the characterization of concentrated emulsions in situ and without dilution [45],... [Pg.434]

Dieker et al.67 used a similar method but applied a dropping amalgam electrode (DAE) and followed amperometrically by means of pulse polarography the anodic dissolution wave of mercury in the presence of an excess of ligand by appropriate choices of pH and titrant they achieved selective determinations of metal ions at low concentrations. [Pg.178]


See other pages where Waves, of concentration is mentioned: [Pg.5]    [Pg.321]    [Pg.48]    [Pg.5]    [Pg.321]    [Pg.48]    [Pg.1106]    [Pg.1324]    [Pg.3065]    [Pg.213]    [Pg.512]    [Pg.398]    [Pg.202]    [Pg.1223]    [Pg.485]    [Pg.602]    [Pg.604]    [Pg.605]    [Pg.619]    [Pg.620]    [Pg.485]    [Pg.827]    [Pg.807]    [Pg.81]    [Pg.202]    [Pg.400]    [Pg.631]    [Pg.145]    [Pg.297]    [Pg.175]    [Pg.197]    [Pg.159]    [Pg.174]    [Pg.220]    [Pg.348]   
See also in sourсe #XX -- [ Pg.15 , Pg.16 , Pg.17 , Pg.18 , Pg.19 , Pg.20 , Pg.30 ]




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