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Special geometries

Using the coordinates of special geometries, minima, and saddle points, together with the nearby values of potential energy, you can calculate spectroscopic properties and macroscopic therm ody-riatriic and kinetic parameters, sncfi as enthalpies, entropies, and thermal rate constants. HyperChem can provide the geometries and energy values for many of these ealeulatiori s. [Pg.32]

Similar results are obtained from incineration of polymeric materials with octabromo- and pentabromodiphenyl ether (refs. 11,12). The temperature with the maximum PBDF-yield depends on the kind of polymeric matrix. All three bromo ethers 1-2 give the same isomer distribution pattern with preference for tetrabrominated dibenzofiirans. The overall yield of PBDF is lower for incineration of pentabromobiphenyl ether 2, 4 % at 700°C compared to 29 % for ether 1 at 500 °C (ref. 12). The preferred formation of tetrabrominated fiirans observed at all temperatures cannot be a result of thermodynamic control of the cyclisation reaction it is likely due to the special geometry of the furnaces. One explanation is that a spontaneous reaction occurs at approximately 400°C while the pyrolysis products are transferred to the cooler zones of the reactor details can be found elsewhere (ref. 12). [Pg.372]

Ruland and Smarsly [9,84,240] can analyze their recorded data in the classical Born approximation, but have to correct for the special geometry of the grazing incidence experiment. They propose not to carry out the necessary corrections in a... [Pg.200]

FDM is one of the methods where the whole problem is fully discretized in both transversal coordinates and no suppositions concerning a special geometry are made. For a standard uniform mesh grid-points (x , yt), are located at x =(i-l)Ax and y =(k-l)Ay, respectively. Derivatives are approximated by finite differences by e.g. [Pg.259]

Geometry No special geometry required anri-coplanarity required... [Pg.232]

For three special geometries, the Laplacian operator can be written in a simpler form. These are the class A geometries the infinite slab, the infinite circular cylinder, and the sphere. For these we can write... [Pg.241]

Exceptions to such a correlation can easily occur, however, because of the heterogeneity of the surface. Indeed, it is found that the bond strength often depends on the degree of coverage. Another factor is the special geometry at the active site of the catalyst. Finally, it may be remarked that a concerted mechanism can occur in which the Me—O bond strengths are only relevant in close connection with the complex to be oxidized. [Pg.233]

Fig. IX Schematic view of the scattering geometry. The unusual tilt of the sample became necessary due to the special geometry of the sample holder... Fig. IX Schematic view of the scattering geometry. The unusual tilt of the sample became necessary due to the special geometry of the sample holder...
The use of films as electrodes makes possible numerous experiments that would be difficult or impractical to implement with the conventional bulk electrodes. Discussion here emphasises either thin (< 5 pm thick usually quite a bit thinner) or thick (> 5 pm usually quite a bit thicker) film electrode materials, consisting of a conductor, either a continuous or a spatially patterned film, most commonly deposited on a suitably prepared insulating substrate. Films consisting primarily of insulators are not considered here, except to the extent that they may be used to form patterned arrays or electrodes with special geometries. A view of applications and properties of film... [Pg.603]

The pentamer of tetrafluoroethene (66) (Scheme 29) is an unusual example of type (96) and reacts readily with nucleophiles [129] (Scheme 65). In contrast, (66) undergoes a remarkable reaction with aqueous triethylamine, producing the dihydrofuran derivative (101) and the process formally involves a direct intramolecular displacement of fluorine from a saturated site and a mechanism has been advanced (Scheme 66) which accounts for the product formed [126]. Understandably, this process is not easily accepted [3, 130] because it has essentially no precedent. Indeed, it is well established that nucleophilic displacement from saturated sites in fluorocarbons occurs only in exceptional circumstances. Consequently, other mechanisms have been advanced, which seem no more convincing [3, 130]. It should be remembered that the major point in favour of the step (100) to (101) (Scheme 66) is that the nucleophile is generated in close proximity to the reaction centre because of the special geometry of this situation. Consequently, much of the otherwise high energy/entropy barrier has already been overcome in this case. [Pg.29]

All of the above advantages stem from the special geometry of the Monoliths as compared to that of the usual catalyst particles. [Pg.216]

The C-N peptide bond has an interesting property It is planar and very rigid. This special geometry of the peptide bond makes it very stable and ideal to maintain the structure of proteins. [Pg.15]

The bulkiness of dendritic side chains can force the polymer backbone to adopt special geometries [84]. The overall contour of the polymer can then be spherical or rod-hke so that the polymers adopt Uquid crystalUne phases. Even when the driving force of this behavior is caused by the bulkiness of the side chain, these polymers show MCLCP-Uke behavior. [Pg.78]

Transport (TMTSF)2X. In a metallic system where phonons and impurities play little role in the scattering rate of carriers, the temperature dependence of resistivity is controlled by electron-electron scattering rate. In a Fermi liquid, it is then governed by the decay rate of quasi-particles. Dropping the logarithmic factors due to either the special geometry of the Fermi surface or the proximity of the SDW transition, one gets a quadratic temperature dependence of the form [29, 34, 75] ... [Pg.225]


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See also in sourсe #XX -- [ Pg.157 ]




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