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Local mixing

Application of this procedure to inadvertently ignited safety valve discharges can involve a special problem. Certain combinations of pressure ratio and length of safety valve riser can result in choked flow, with a pressure discontinuity at the exit. The pressure of the jet then adjusts to atmospheric pressure in a system of shock waves or expansion waves over a distance of a few pipe diameters. These waves can affect the local mixing of the jet with the crosswind. Since the calculation procedure incorporates correlations for subsonic jets, it cannot be expected to be entirely accurate in this case. Nevertheless, since the wave system... [Pg.290]

As our first approach to the model, we considered the controlling step to be the mass transfer from gas to liquid, the mass transfer from liquid to catalyst, or the catalytic surface reaction step. The other steps were eliminated since convective transport with small catalyst particles and high local mixing should offer virtually no resistance to the overall reaction scheme. Mathematical models were constructed for each of these three steps. [Pg.162]

Marchello and Toor (M2) proposed a mixing model for transfer near a boundary which assumes that localized mixing occurs rather than gross displacement of the fluid elements. This model can be said to be a modified penetration-type model. Kishinevsky (K6-K8) assumed a surface-renewal mechanism with eddy diffusion rather than molecular diffusion controlling the transfer at the interface. [Pg.387]

In summary, the Mossbauer data presented by Fee et al. (5) gave the first conclusive evidence that Rieske clusters contain noncysteine ligands bound to the Fe" site of a localized mixed valence cluster. In addition, strong similarities with [2Fe-2S] clusters in bacterial dioxy-... [Pg.118]

Another type of complex for which it is obvious thatQlarge structural changes occur on excitation (probably 0.2-0.3 A) along particular coordinates are the infinite-chain mixed-valence complexes of platinum and palladium (class II, or localized mixed-valence complexes) (11).. These Pti [/PtIV, PdIVPtIV or Pdi [/PdIV... [Pg.493]

These methods hardly take spatial distributions of velocity field and chemical species or transient phenomena into account, although most chemical reactors are operated in the turbulent regime and/or a multiphase flow mode. As a result, yield and selectivity of commercial chemical reactors often deviate from the values at their laboratory or pilot-scale prototypes. Scale-up of many chemical reactors, in particular the multiphase types, is still surrounded by a fame of mystery indeed. Another problem relates to the occurrence of thermal runaways due to hot spots as a result of poor local mixing effects. [Pg.209]

The degree of local mixing in a RANS simulation is measured by the scalar variance (complete mixing (i.e., (j> — (j>) is uniform at the SGS) up to (4>max — (4>))((4>) — 4>min) where () is the mean concentration and max and r/>min are the maximum and minimum values, respectively. The rate of local mixing is controlled by the scalar dissipation rate (Fox, 2003). The scalar time scale analogous to the turbulence integral time scale is (Fox, 2003) as follows ... [Pg.241]

Local mixing is best defined in terms of stochastic models. However, this condition is meant to mle out models based on jump processes where the scalar variables jump large distances in composition space for arbitrarily small df. It also rales out interactions between points in composition space and global statistics such as the mean. [Pg.283]

As will be shown for the CD model, early mixing models used stochastic jump processes to describe turbulent scalar mixing. However, since the mixing model is supposed to mimic molecular diffusion, which is continuous in space and time, jumping in composition space is inherently unphysical. The flame-sheet example (Norris and Pope 1991 Norris and Pope 1995) provides the best illustration of what can go wrong with non-local mixing models. For this example, a one-step reaction is described in terms of a reaction-progress variable Y and the mixture fraction p, and the reaction rate is localized near the stoichiometric point. In Fig. 6.3, the reaction zone is the box below the flame-sheet lines in the upper left-hand corner. In physical space, the points with p = 0 are initially assumed to be separated from the points with p = 1 by a thin flame sheet centered at... [Pg.287]

X-Ray photoelectric ionization is believed to take place in a time interval of about 10-18 s. Therefore separate XPS peaks are possible for atoms if the lifetime of the asymmetric electronic state is greater than about 10 18 s, whether or not the atoms are structurally equivalent. We may represent the ground state of a localized mixed valence compound (involving two metal atoms differing in oxidation state by one unit) by the following formula, where the dot represents the extra valence electron M—M. The two possible XPS transitions can then be represented as follows, where the asterisk indicates core ionization,... [Pg.181]

For the smelt-water case. Nelson suggested the water in contact with the very hot smelt was, initially, separated by a thin vapor film. Either because the smelt cooled—or because of some outside disturbance— there was a collapse of the vapor film to allow direct liquid-liquid contact. The water was then heated to the superheat-limit temperature and underwent homogeneous nucleation with an explosive formation of vapor. The localized shocks either led to other superheat-limit explosions elsewhere in the smelt-water mass or caused intense local mixing of the smelt and water to allow steam formation by normal heat transfer modes. [Pg.156]

The usefulness of baffles in mixing operations is offset by increased clean-up problems (due to particulate entrapment by the baffles or congealing of product adjacent to the baffles). Furthermore, overbaffling —excessive use of baffles—reduces mass flow and localizes mixing, which may be counterproductive. [Pg.98]

Remark 1 If no approximation is introduced in the PFR model, then the mathematical model will consist of both algebraic and differential equations with their related boundary conditions (Horn and Tsai, 1967 Jackson, 1968). If in addition local mixing effects are considered, then binary variables need to be introduced (Ravimohan, 1971), and as a result the mathematical model will be a mixed-integer optimization problem with both algebraic and differential equations. Note, however, that there do not exist at present algorithmic procedures for solving this class of problems. [Pg.413]

Fig. 5. The vibronic orbitals describing the main part of electron structure change when turning from delocalized to localized mixed valence in hypothetical molecule [A12C16]2. ... Fig. 5. The vibronic orbitals describing the main part of electron structure change when turning from delocalized to localized mixed valence in hypothetical molecule [A12C16]2. ...
Further, mixing/turbulent diffusivity derived by considering that the mixing process in a liquid is caused by the random movement of inner substances based on the turbulent flow can also be used as an index for the evaluation of the local mixing rate. The mass balance in the flow field is written as... [Pg.24]

Each local mixing capacity defined by Eq. (2.27) has a value from zero for the no-mixing state to unity for the perfect-mixing state ... [Pg.58]

Needless to say, the whole mixing capacity can also be derived by taking the average of the local mixing capacity (MGj(R) or Mlj(R) or MLj(R)) in all the regions. [Pg.59]

Until now, a quantitative evaluation of the local mixing capacity and whole mixing capacity based on the movement of the inner substances among regions has been shown. [Pg.59]

The transition probabilities Ptj and Pjt in 0.2 s for both the impellers are estimated based on the experimental data in Challenge 2.3 (the change in the spatial distribution of the tracer concentration with time when the tracer is injected into an impeller position under an impeller rotational speed of 200 rpm) by using a computer. Based on the transition probabilities, the local mixing capacity and whole mixing capacity of both the impellers are calculated by using Eqs. (2.27) and (2.30) under the condition of V0 = 100 cm3. [Pg.60]

Figure 2.12 (Contour line maps of the local mixing capacities on the semivertical cross-section of the vessel for each impeller style). Figure 2.12 (Contour line maps of the local mixing capacities on the semivertical cross-section of the vessel for each impeller style).
Figure 2.12 Local mixing capacity map in case of FBDT impeller and 45° PBT impeller in... Figure 2.12 Local mixing capacity map in case of FBDT impeller and 45° PBT impeller in...
The 45° PBT impeller has a larger value than the FBDT impeller, and this result is contrary to the case in which the tracer is injected into the impeller position described in Challenge 2.3. This difference is caused by the difference in the local mixing capacity at the region where the impeller discharge flow reaches. In other words, the change in the spatial distribution of the tracer concentration with time is significantly affected by the position of the tracer injection. [Pg.63]


See other pages where Local mixing is mentioned: [Pg.440]    [Pg.434]    [Pg.101]    [Pg.154]    [Pg.209]    [Pg.356]    [Pg.288]    [Pg.288]    [Pg.87]    [Pg.23]    [Pg.104]    [Pg.147]    [Pg.254]    [Pg.1083]    [Pg.199]    [Pg.152]    [Pg.407]    [Pg.408]    [Pg.84]    [Pg.260]    [Pg.264]    [Pg.57]    [Pg.63]    [Pg.63]   
See also in sourсe #XX -- [ Pg.355 , Pg.356 ]




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