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Model Davidson

Davidson model. Thus the bed contains bubbles surrounded by thin clouds rising through an emulsion. We ignore the upflow of gas through the cloud because the cloud volume is small compared to that of the bubble. This is the regime where (see Fig. 20.8). [Pg.455]

Figure 5. Gas flow for isolated rising bubbles in the Davidson model [30]. Figure 5. Gas flow for isolated rising bubbles in the Davidson model [30].
It has been shown by Chavarie and Grace (15) that the decomposition of ozone in a fluidized-bed is best described by Kunii and Levenspiel s model (16) but that the Orcutt and Davidson models (17) gave the next best approximation for the overall behaviour and are easier to use and were chosen for the simulation. They suppose a uniform bubble size distribution with mass transfer accomplished by percolation and diffusion. The difference between the two models is the presumption of the type of gas flow in the emulsion phase piston flow, PF, for one model and a perfectly mixed, PM, emulsion phase for the other model. The two models give the following expressions at the surface of the fluidized bed for first-order reaction mechanism ... [Pg.59]

Using the definition of slip velocity given by equation (1), it is seen that the Field-Davidson model requires P to be identically zero, while the Joshi-Sharma modification suggests the unrealistic result that P is negative if the slip velocity definition is obeyed. [Pg.272]

Sturz and DoUe measured the temperature dependent dipolar spin-lattice relaxation rates and cross-correlation rates between the dipolar and the chemical-shift anisotropy relaxation mechanisms for different nuclei in toluene. They found that the reorientation about the axis in the molecular plane is approximately 2 to 3 times slower than the one perpendicular to the C-2 axis. Suchanski et al measured spin-lattice relaxation times Ti and NOE factors of chemically non-equivalent carbons in meta-fluoroanihne. The analysis showed that the correlation function describing molecular dynamics could be well described in terms of an asymmetric distribution of correlation times predicted by the Cole-Davidson model. In a comprehensive simulation study of neat formic acid Minary et al found good agreement with NMR relaxation time experiments in the liquid phase. Iwahashi et al measured self-diffusion coefficients and spin-lattice relaxation times to study the dynamical conformation of n-saturated and unsaturated fatty acids. [Pg.211]

Kunii and Levenspiel s modiflcation (see their book, 1991, for original references) of the Davidson model and formulation of reactor design procedures for the different... [Pg.822]

FIGURE CS5.1 Schematics of several fluidized-bed reactor models (a) Davidson model, (b) Kunii-Levenspiel model, (c) Miyauchi model, (d), (e) Fryer-Potter and Jayaraman-Kulkami-Doraiswamy models. [Pg.886]

The Cole-Davidson model These kinds of diagram are also symmetrical or non-symmetrical and may be fairly described by an analytical relationship proposed by Davidson and Cole [77] (Eq. 46) ... [Pg.31]

An important feature of fluidized-bed reactors is mass transfer between bubble and emulsion. Several models have been proposed for this exchange. The Davidson model assumes no cloud, so that only one mass transfer coefficient be (for direct bubble-emulsion exchange) is involved. On the other hand, the... [Pg.381]

The flow of gas in the vicinity of rising bubbles follows the Davidson model (Davidson and Harrison, 1963). [Pg.251]


See other pages where Model Davidson is mentioned: [Pg.111]    [Pg.69]    [Pg.80]    [Pg.885]    [Pg.888]    [Pg.235]    [Pg.203]    [Pg.37]    [Pg.266]    [Pg.407]   
See also in sourсe #XX -- [ Pg.885 , Pg.888 ]




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