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Crystal performance

In general, however, the vulcanizates suffer from poor low temperature crystallization performance compared to a conventional sulfur cure, and also have inferior tensile and tear properties. Urethane cross-linking systems (37), eg, Novor 950 (see Table 3) are also extremely heat resistant, but exhibit inferior tensile and dynamic properties compared to conventional sulfur-cured vulcanizates. One added virtue is that they can be used in conjunction with sulfur systems to produce an exceUent compromise according to the ratios used (38). [Pg.269]

Prediction and analysis of crystallizer performance is achieved by constructing models based on conservation equations and rate expressions respectively, as follows. In general form, the conservation equation is given by... [Pg.66]

The first, and simplest, step in predicting crystallizer performance is the calculation of crystal yield. This can easily be estimated from knowledge of solution concentration and equilibrium conditions permitting calculation of the overall mass balance... [Pg.66]

The isolation of crystalline products having mixed polymorphic compositions (often referred to as concomitant polymorphism) remains a topic of interest, even though the phase rule predicts that a system at equilibrium consisting two components (solvent + solute) and three phases (solution + Form I + Form II) is uni variant. Hence, for crystallizations performed at a fixed pressure (typically atmospheric) the system becomes nonvariant and genuine equilibrium can exist at only one temperature. Therefore, concomitant products must be obtained under nonequilibrium conditions. Flexibility in molecular conformation was attributed to the concomitant polymorphs of a spirobicyclic dione [34] and of 3-acetylcoumarin [35],... [Pg.268]

Another important development which altered our view of crystallization processes was the realization of the importance of secondary nucleation due to contact between crystals and the impeller and vessel. Secondary nucleation of this type has been shown (2-6) to often have a dominant role in determining crystallizer performance. Our understanding of crystal growth, nucleation, fluid mechanics and mixing have all greatly improved. A number of review (2r 101 have appeared in recent years which describe the advances in these and... [Pg.2]

Batch crystallizers are often used in situations in which production quantities are small or special handling of the chemicals is required. In the manufacture of speciality chemicals, for example, it is economically beneficial to perform the crystallization stage in some optimal manner. In order to design an optimal control strategy to maximize crystallizer performance, a dynamic model that can accurately simulate crystallizer behavior is required. Unfortunately, the precise details of crystallization growth and nucleation rates are unknown. This lack of fundamental knowledge suggests that a reliable method of model identification is needed. [Pg.102]

Based on our observations, we have reason to believe that single crystal performance will be approached in future thin film, polycrystalline semiconductor based solar cells with grain boundary recombination velocities reduced by strongly chemisorbed species. [Pg.75]

Three different indirect methods. Fig. 4.1, to detect and amplify a singlebase mismatch were described by Willner et al. [63]. All methods were based on a surface treatment, involving immobihzation of the thiolated DNA, hybridization and biotinylation in the presence of polymerase I of the sensing interface, resulting in functionahzed Au-quartz crystals, performed outside the QCM cell. [Pg.392]

As remarked previously, a crystal acts to decompose the continuous Fourier transform of the electron density in the unit cells into a discrete spectrum, the diffraction pattern, which we also call the weighted reciprocal lattice. Thus a crystal performs a Fourier analysis in producing its diffraction pattern. It remains to the X-ray crystallographer to provide the Fourier synthesis from this spectrum of waves and to recreate the electron density. [Pg.89]

Pictures of the crystals obtained by this procedure are shown in Fig. 7-14. Filtration rates and impurity rejection are satisfactory. Scale-up from the pilot plant to manufacturing scale (10,000 liters) resulted in no significant differences in crystallizer performance. ... [Pg.150]

The x(T) curve of PuBeI3 was measured by Brodsky and Friddle (1975) at temperatures between 2 and 300 K. MCW behaviour with jaeff = 0.74jaB/f.u., 6p = 11 K, and Xo = 0.5x10 8 m3/mol was observed above 15 K. The sharp maximum at 11.5 K was taken as evidence for an antiferromagnetic ordering in this compound. However, experiments on single crystals performed by Stewart et al. (1984b) did not confirm this assumption because no indication of a phase transition were obtained from Xac measurements. The C(T) curve displays only a broad maximum reminiscent of a situation where independent local moments are embedded in an itinerant matrix. The C/T ratio for T- 0 approaches a value of about 330 mJ/mol K2, while the extrapolation from the temperature above the maximum yields only 220 mJ/mol K2. [Pg.414]

A "modern" approach would probably go as follows Grow a nice NaCl crystal, perform an X-ray diffraction measurement to determine the electron density along the line Na-Cl, search for the minimum density somewhere between the two atoms, and then interpret this value as the crossover from the cation (Na+) to the anion (Cl ). Yet, the systems of ionic radii we know of have been generated following other recipes [8], and three approaches seem to be especially worth mentioning. [Pg.11]

PrCu2 shows hardly any anomaly while a marked anomaly is observable in the resistivity. The resistivity measurements on a PrCu2 single crystal performed by Andres et al. (1976) show strong anisotropic behaviour for the a, b, and c direction of this orthorhombic structure. Because of the temperature-independent nature of this anisotropic behaviour Andres et al. (1976) conclude that the anisotropy in the resistivity is due to the anisotropy of the Fermi surface and not due to anisotropy in the scattering cross section between conduction electrons and f-electrons. [Pg.150]

Since the pioneering work on surface-induced alignment of liquid crystals, performed by Lehmann [1], Grandjean [2], Mauguin [3], Chatelain [4], and others [5], scientist have been looking for the answer to the question why do certain surfaces align liquid crystals and others not ... [Pg.163]

Analyses of the influence of fines trapping on crystallizer performance have been made by Nauman (1971) and Nauman and Szabo (1971). [Pg.420]

Conductivity measurements on polycrystalline compressed pellets or on single crystals perform at room temperature in the salts of Table 2 showed that these are conducting salts. Some of them, such as (1b)2AuBr2 (1b) Ni(dcit)2, (1c)2AuBr2, (1g) IBr2, were found to be metallic down to low temperatures. These preliminary results indicate that the compounds are worthy of further studies. [Pg.184]

FIGURE 11.3-2 Crystallizer performance as a function of solvent removal rate. [Pg.610]

Agitated crystallizer for continuous and discontinuous operation, feed temperature 1 3, cooled to 1 1, t is also exit temperature of crystal slurry, nucleation and crystal growth at randomly adjusted equilibrium Crystallizer performance is limited by solution boil over. [Pg.514]


See other pages where Crystal performance is mentioned: [Pg.525]    [Pg.1993]    [Pg.58]    [Pg.201]    [Pg.7]    [Pg.70]    [Pg.191]    [Pg.222]    [Pg.57]    [Pg.105]    [Pg.358]    [Pg.525]    [Pg.1751]    [Pg.556]    [Pg.4]    [Pg.2162]    [Pg.162]    [Pg.197]    [Pg.34]    [Pg.525]    [Pg.266]    [Pg.580]    [Pg.1005]    [Pg.2146]    [Pg.105]    [Pg.1997]    [Pg.5934]    [Pg.580]    [Pg.68]    [Pg.514]   
See also in sourсe #XX -- [ Pg.367 ]




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