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Crystallization simplifying

Theoretical representation of the behaviour of a hydrocyclone requires adequate analysis of three distinct physical phenomenon taking place in these devices, viz. the understanding of fluid flow, its interactions with the dispersed solid phase and the quantification of shear induced attrition of crystals. Simplified analytical solutions to conservation of mass and momentum equations derived from the Navier-Stokes equation can be used to quantify fluid flow in the hydrocyclone. For dilute slurries, once bulk flow has been quantified in terms of spatial components of velocity, crystal motion can then be traced by balancing forces on the crystals themselves to map out their trajectories. The trajectories for different sizes can then be used to develop a separation efficiency curve, which quantifies performance of the vessel (Bloor and Ingham, 1987). In principle, population balances can be included for crystal attrition in the above description for developing a thorough mathematical model. [Pg.115]

Fig. 47. Radiative transitions from the lowest emitting states of a tetracyanoplatinate(II) crystal (simplified). Dlh zero magnetic field Qh Hie GS H c (For the values AE and AE" see Table 6.)... Fig. 47. Radiative transitions from the lowest emitting states of a tetracyanoplatinate(II) crystal (simplified). Dlh zero magnetic field Qh Hie GS H c (For the values AE and AE" see Table 6.)...
G) Palustrine micritic limestone infilled by a dark secondary micrite associated with gypsum crystals. Simplified chart showing the evaporite precipitation sequence from waters of various compositions. [Pg.483]

The force constants now have an explicit dependence on the vector k. The periodicity of the crystal simplified the problem and we have a set of 3iVatom X 3iVatom equations for every value of k ... [Pg.163]

All measurements in the present contribution have been performed on large crystals of silicalite-1 and H-ZSM-5 zeolites. Use of large zeolite crystals simplifies significantly the modeling and experimental procedure because it allows one to avoid pelletizing of the crystals. This has the important advantage that no macropore diffusion has to be included in the hydrocarbon transport models and intracrystalline diffusion is the dominating process. [Pg.294]

How are fiindamental aspects of surface reactions studied The surface science approach uses a simplified system to model the more complicated real-world systems. At the heart of this simplified system is the use of well defined surfaces, typically in the fonn of oriented single crystals. A thorough description of these surfaces should include composition, electronic structure and geometric structure measurements, as well as an evaluation of reactivity towards different adsorbates. Furthemiore, the system should be constructed such that it can be made increasingly more complex to more closely mimic macroscopic systems. However, relating surface science results to the corresponding real-world problems often proves to be a stumbling block because of the sheer complexity of these real-world systems. [Pg.921]

This is a simplified formula for tartar emetic, for X-ray crystal analysis and infrared studies indicate that the. Sb is a part of the antimonate anion [Sb(OH)4] and forms part of a cyclic system. [Pg.115]

For crystal sulfamic acid assay, a simplified procedure of neutralization titration with sodium hydroxide solution may be used. At the end point, Bromothymol Blue (BTB) indicator changes color from yellow to yellowish green. A 1-mL solution of l/2NNaOH is equivalent to 0.0485 g of sulfamic acid. [Pg.64]

Electrochemistry and Kinetics. The electrochemistry of the nickel—iron battery and the crystal stmctures of the active materials depends on the method of preparation of the material, degree of discharge, the age (Life cycle), concentration of electrolyte, and type and degree of additives, particularly the presence of lithium and cobalt. A simplified equation representing the charge—discharge cycle can be given as ... [Pg.552]

Imagine, now, a solid held together by such little springs, linking atoms between two planes within the material as shown in Fig. 6.1. For simplicity we shall put atoms at the comers of cubes of side Tq. To be correct, of course, we should draw out the atoms in the positions dictated by the crystal structure of a particular material, but we shall not be too far out in our calculations by making our simplifying assumption - and it makes drawing the physical situation considerably easier ... [Pg.58]

As mentioned above, the unit operation of crystallization rarely exists in isolation but is normally part of a wider particulate processing system as illustrated schematically, in a very simplified form, in Figure 9.2. A particular feature of such processes is the variety of unit operations and the range of equipment types that may be employed at any stage. [Pg.262]

Crystallization proeess systems design and operation is a eomplex matter requiring extensive data for systematie evaluation. Whilst simplified design methods and heuristies are available, the simple faet remains that the more and better the data input, the better the final design and reliability of the plant. Ideally, amongst the data required are the following ... [Pg.263]

Roliani, S. and Bourne, J., 1990a. A simplified approach to the operation of a batch crystallizer. Canadian Journal of Chemical Engineering, 45, 3457-3466. [Pg.320]

The special case where only rotators are present, Np = 0, is of particular interest for the analysis of molecular crystals and will be studied below. Here we note that in the other limit, where only spherical particles are present, Vf = 0, and where only symmetrical box elongations are considered with boxes of side length S, the corresponding measure in the partition function (X Qxp[—/3Ep S, r )], involving the random variable S, can be simplified considerably, resulting in the effective Hamiltonian... [Pg.95]

Fig. 5 shows data from a simulation of TIP4P water that is confined on both sides by a rhombohedral mercury crystal with (111) surface structure. Bosio et al. [135] deduce from their X-ray studies that a solid o-mercury lattice with a larger lattice constant in the z direction may be used as a good structural model for liquid mercury. Thus, the mercury phase was modeled as a rigid crystal in order to simplify the simulations. The surface of such a crystal shows rather low corrugation. [Pg.359]

Obviously this model is very simplified, compared with the real crystal which contains many defects, dislocations and entanglements. In particular, it neglects many aspects of the true three-dimensional nature of the lamella which one may have thought to be important the influence of the stacking of folds, which is... [Pg.226]

Sadler [76] analysed the outline of the crystal edges and found that the lateral surface tension compatible with such a curvature would be a 1 — 3 kT/. Although he used a very simplified approach, it seems unlikely that its assumptions could lead to a a 20 kT/<7> as predicted by the LH theory. [Pg.278]


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See also in sourсe #XX -- [ Pg.433 ]




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