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Viscous motions

The ions are regarded as rigid balls moving in a liquid bath. It is assumed that the macroscopic laws of motion in a viscous medium hold, and that the electrostatic interaction is determined by the theory of continuous dielectrics. This assumption implies that the moving particles are large compared to the molecular structure of the liquid. The most successful results of continuous theories can be found in any textbook of physical chemistry Stokes , law for viscous motion, Einstein s derivation of the dependence of viscosity on the concentration... [Pg.11]

The NMR experiment can be conducted in a temperature range from liquid nitrogen (-209°C) to + 150°C. This gives the experimenter the ability to slow down rapid molecular motions to observable rates or to speed up very slow or viscous motions to measurable rates. [Pg.61]

The first group of models ( eddy models) assumes that the liquid renewal is due to small-scale eddies of the turbulent field. These models are based on idealized eddy structures of turbulence in the bubble vicinity. Lamont and Scott [1] have assumed that the small scales of turbulent motion, which extend from the smallest viscous motions to the iner-... [Pg.121]

These glassy phases may act as a lubricant for grain boundary sliding. In this case, the accommodation mechanism is the viscous motion of these secondary phases. [Pg.441]

Since tangential diffusion has been neglected, only fluid motion contributes to the tangential particle velocity. Near to the collector the fluid appears to be experiencing uniform, linear, shear how. Goldman et al. (1967b) studied the viscous motion of a sphere in Couette flow and found the particle velocity to be proportional to, hut lew than, the undisturbed fluid velocity at the particle s center ... [Pg.97]

Small Reynolds Number Flow, Re < 1. The slow viscous motion without interfacial mass transfer is described by the Hadamard (66)-Rybcynski (67) solution. For infinite liquid viscosity the result specializes to that of the Stokes flow over a rigid sphere. An approximate transient analysis to establish the internal motion has been performed (68), Some simplified heat and mass transfer analyses (69, 70) using the Hadamard-Rybcynski solution to describe the flow field also exist. These results are usually obtained through numerical integration since analytical solutions are usually difficult to obtain. [Pg.19]

Bretherton, F.P. (1962) Slow viscous motion round a cylinder in a simple shear, J. Fluid Mech. 12, 591-613. [Pg.367]

G5b. Goldman, A. J., Cox, R. G., and Brenner, H., Slow viscous motion of two identical arbitrarily oriented spheres through a viscous fluid. Chem. Eng. Sci. (in press) see also Goldman, A. J., Investigations in low Reynolds number fluid-particle dynamics. Ph.D. Dissertation, New York University, New York, 1966. [Pg.432]

Even though there is a big shift in the resonance frequency, the mass sensitivity to thin film is observed to be the same in a fluid as in a vacuum. In addition to the viscous motion, many other factors still affect the resonance frequency of QCM in a high-density fluid. Roughness of the surface is one important factor. Based on the measurement, resonance frequencies turned out to be dependent on the surface roughness [14,15]. The roughness seems to induce a shift of the resonant frequency by both the inertial contribution from the liquid mass rigidly coupled to the surface, and the viscous contribution from the viscous energy dissipation caused by the nonlaminar motion in the liquid [16]. [Pg.212]

The coefficient (m in eq. (V11.20) has no precise meaning but is a convenient reminder of the similarity with the Stokes law for viscous motion of a sphere. [Pg.210]

Figure 11.30 Craze formation and growth by the Saffman-Taylor meniscus instability mechanism (courtesy of E. J. Kramer). An anaiysis of the viscous motions with the WLF equation aiiows an estimation of the temperature of the crazes on formation. Figure 11.30 Craze formation and growth by the Saffman-Taylor meniscus instability mechanism (courtesy of E. J. Kramer). An anaiysis of the viscous motions with the WLF equation aiiows an estimation of the temperature of the crazes on formation.
For rubber there is slow, viscous motion to reach the changed conformations, steel expands by affine bond expansion (speed of sound). [Pg.436]

Tm Motor torque Parameter related to viscous Motion... [Pg.166]


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See also in sourсe #XX -- [ Pg.61 ]




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