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High friction approximation

For a harmonic oscillator immersed in a Brownian medium, the displacement—in the high-friction approximation—is a position Ornstein-Uhlenbeck process. With U(x) = mwV/2, the solution of Eqs. (4.152) and (4.153) is... [Pg.108]

As we have already discussed, further parameters of interest are the frequencies u>Q and U) deriving from the hi onic approximation at the bottom of the reactant well and the top of the barrier, respectively. Carmeli and Nitzan evaluated the reaction rate throughout the entire friction dominion ranging from the low-friction regime (w > y) to the high-friction regime. (This has also been commented on in S on II.B.) They also studied the dependence of the reaction rate on the correlation time... [Pg.433]

Figure 12 shows the obtained yield points and their linear approximations for the internal friction, i.e., ftiction between sugar particles. The mean wall yield locus measured using the stainless steel wall element is presented in Fig. 13. The obtained parameters are Hsted in Table 3. The investigated material has a negligible cohesion and a high friction. The mean values of the measured friction coefficients between particles is /tp.p = 0.86 it 0.07. The obtained wall fnction coefficient is //p stt.ei = 0.482 0.021. The value of flow function at ffc = 34 shows that nearly spherical sugar pellets can be characterized as free flowing. Figure 12 shows the obtained yield points and their linear approximations for the internal friction, i.e., ftiction between sugar particles. The mean wall yield locus measured using the stainless steel wall element is presented in Fig. 13. The obtained parameters are Hsted in Table 3. The investigated material has a negligible cohesion and a high friction. The mean values of the measured friction coefficients between particles is /tp.p = 0.86 it 0.07. The obtained wall fnction coefficient is //p stt.ei = 0.482 0.021. The value of flow function at ffc = 34 shows that nearly spherical sugar pellets can be characterized as free flowing.
As discussed above the errors in the trajectory are correlated with the missing rapid motions. In contrast to the friction approach of estimating the variance, which may affect long time phenomena, we identify our errors as the missing ( filtered ) high frequency modes. We therefore attempt to account approximately for the fast motions by choosing the trajectory variance accordingly. [Pg.274]

The developed theory of two-phase laminar flow with a distinct interface which is based on a one-dimensional approximation, takes into account the major features of the process the inertia, gravity, surface tension and friction forces and leads to the physically realistic pattern of a laminar flow in a heated micro-channel. This allows one to use the present theory to study the regimes of flow as well as optimizing a cooling system of electronic devices with high power densities. [Pg.422]


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See also in sourсe #XX -- [ Pg.108 ]




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