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Geometries location

Fig. 57. The theoretical relationships between the Peclet number, Pe, and the Sherwood number, Sh, as calculated by Alkire et al. [183] for various 2-dimensional pit geometries (located adjacent). The labels a, b, and c refer to zones in which the whole surface is below saturation, partially saturated, and completely above saturation with respect to dissolution products. Fig. 57. The theoretical relationships between the Peclet number, Pe, and the Sherwood number, Sh, as calculated by Alkire et al. [183] for various 2-dimensional pit geometries (located adjacent). The labels a, b, and c refer to zones in which the whole surface is below saturation, partially saturated, and completely above saturation with respect to dissolution products.
Ribs and bosses geometry, locations, spacing between ribs or bosses... [Pg.22]

There are various levels of structural organization of proteins primary, secondary, tertiary and quaternary. The primary structure has been defined as the sequential order of amino acid residues linked by covalent peptide bonds. The secondary structure refers to the molecular geometry located in the polypeptide chains within ordered structures, such as a-helix, (3-sheet and random coil (unordered). The tertiary structure contains the information on how the elements of the secondary structure are folded. Finally, the quaternary structure of a protein with more than one polypeptide chain shows how the different principal chains are associated and oriented with one another. The structure of proteins is stabilized by different types of interactions covalent and hydrogen bonds, hydrophobic interactions, electrostatic and van der Waals forces [3,4]. [Pg.468]

The disparities in the nature, size, geometry, location and orientation of flaws between nominally identical test specimens explain the great variations in the stress frequently observed. [Pg.275]

For an industrial application it is necessary to separate the response of a real crack from artifacts, and to derive information about the geometry and the location of the crack. For this purpose we have developed a filter which is sensitive to the characteristic features of a signal caused by a crack and amplifies it, whereas signals without these typical features are suppressed. In Fig. 5.1 first results obtained with such an iterative filter algorithm are shown. [Pg.261]

Today the demand for inspection of components with complex geometry, difficult access conditions or location in a hazardous environment is steadily increasing. Documentation, reproducibility and minimised health risk for the inspection staff are key issues. This leads to an increased demand for automated inspection, resulting in a need for new, advanced scarmer systems for NDE. [Pg.799]

Electron Spin Resonance Spectroscopy. Several ESR studies have been reported for adsorption systems [85-90]. ESR signals are strong enough to allow the detection of quite small amounts of unpaired electrons, and the shape of the signal can, in the case of adsorbed transition metal ions, give an indication of the geometry of the adsorption site. Ref. 91 provides a contemporary example of the use of ESR and of electron spin echo modulation (ESEM) to locate the environment of Cu(II) relative to in a microporous aluminophosphate molecular sieve. [Pg.586]

At any geometry g.], the gradient vector having components d EjJd Q. provides the forces (F. = -d Ej l d 2.) along each of the coordinates Q-. These forces are used in molecular dynamics simulations which solve the Newton F = ma equations and in molecular mechanics studies which are aimed at locating those geometries where the F vector vanishes (i.e. tire stable isomers and transition states discussed above). [Pg.2157]

Transition stale search algorithms rather climb up the potential energy surface, unlike geometry optimi/.ation routines where an energy minimum is searched for. The characterization of even a simple reaction potential surface may result in location of more than one transition structure, and is likely to require many more individual calculations than are necessary to obtain et nilibrinm geometries for either reactant or product. [Pg.17]

Schlegel H B 1989. Some Practical Suggestions for Optimizing Geometries and Locating Transition States. In Bertran J and IG Csizmadia (Editors). New Theoretical Concepts for Understanding Organic Reactions. Dordrecht, Kluwer, pp. 33-53. [Pg.315]


See other pages where Geometries location is mentioned: [Pg.356]    [Pg.981]    [Pg.22]    [Pg.25]    [Pg.374]    [Pg.374]    [Pg.377]    [Pg.27]    [Pg.34]    [Pg.230]    [Pg.110]    [Pg.229]    [Pg.497]    [Pg.310]    [Pg.356]    [Pg.981]    [Pg.22]    [Pg.25]    [Pg.374]    [Pg.374]    [Pg.377]    [Pg.27]    [Pg.34]    [Pg.230]    [Pg.110]    [Pg.229]    [Pg.497]    [Pg.310]    [Pg.20]    [Pg.166]    [Pg.170]    [Pg.372]    [Pg.489]    [Pg.741]    [Pg.799]    [Pg.1829]    [Pg.2156]    [Pg.2334]    [Pg.2350]    [Pg.358]    [Pg.378]    [Pg.378]    [Pg.387]    [Pg.141]    [Pg.307]    [Pg.194]    [Pg.234]    [Pg.278]    [Pg.300]    [Pg.303]    [Pg.518]    [Pg.705]    [Pg.110]    [Pg.162]    [Pg.513]   
See also in sourсe #XX -- [ Pg.107 ]




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