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Effect of Overlap

Mampel extended the treatment to include due allowance for three-dimensional growth of product into the particles by considering the latter to consist of a series of concentric thin spherical shells. The fractional reaction within each such shell was calculated and the total reaction found by integration to include all such shells. This analysis, which includes the effects of overlap, ingestion and also particle size of the reactant, is not amenable to general solution, but the following special cases are of interest. [Pg.57]

Using this approach, calculations can be made of volumetric, entropic and energy parameters taking account of the effect of overlapping cospheres. Some indication of the organization in the solution is also possible. The properties of a number of concentrated salt solutions have been analysed by this procedure, including simple 1 1 salts, alkaline earth salts and alkylammonium salts. [Pg.45]

Using the simplest picture (and neglecting the effect of overlap on the normalization), this doubly occupied og spatial molecular orbital can be thought of as being the symmetric linear combination of the two Is atomic orbitals on the left and right hydrogens, HL and Hr... [Pg.33]

In this case the effect of overlapping of the individual nuclei can be simply expressed in terms of the statistical Kolmogorov-Avrami theory, where the right-hand side of Eq. (5.8.6) is multiplied by the factor exp(— N X2t2/z2F2Tll) and that of Eq. (5.8.7) by the factor (—jZKh2t3/3z2F2rll). [Pg.381]

Mies FH (1968) Configuration interaction theory, effects of overlapping resonances. Phys Rev 175 164... [Pg.264]

Equations (7.8) to (7.11) show that the exponent j8 in the i oc function may vary from 1 to 3. Therefore, all models presented here predict that the current density i increases for all time (Eig. 7.4). This is not what is observed experimentally and thus is unacceptable. A new model that takes into account the effect of overlap between diffusion fields around nuclei (Eig. 7.3) is required. This is the subject of the next section. [Pg.118]

Figure 7.10. Theoretical potentiostatic current-time transient, including the effect of overlap. (From Ref. 27, with permission from Elsevier.)... Figure 7.10. Theoretical potentiostatic current-time transient, including the effect of overlap. (From Ref. 27, with permission from Elsevier.)...
The reason why it is a useful concept in actinide solid state physics (as in d-transition metals) is that it describes the effect of overlapping in forming a band therefore, in d or f unfilled bands, a critical value of the inter-atomic distance should determine whether the electron states will be acting as localized (insulator s) states, or as an unfilled (metallic) band. If we refer to the concept of f-f-overlapping, it is thinkable that across a series such as the actinides the f-f-overlapping might come to a critical value distinguishing between band and localized behaviour. [Pg.37]

The first attempts to seek a closed expression for n(t) did not include an analysis of pair correlation of defects, even at the level of pair densities, and seem at least to be ambiguous. Such an approach based on simple probabilistic considerations was first used in [24] (see also [108]). Since here we are not treating explicitly the relationship between two-particle and higher-particle densities, it is difficult to make a correct estimate of the effect of overlap of the forbiden volumes of several closely-lying defects. This leads to the need to introduce some a priori assumptions. A characteristic example is [24], where the implicit assumption of a chaotic distribution of defects through the reaction volume (along with partially taking it into account) led to a physically incorrect result - the absence of an effect of saturation of concentration doses (see Table 7.6 below and comments to it). [Pg.442]

Answer to 9 and 10. The orbital interaction diagram for the bonding is shown in Figure B3.8. The geometric changes described for ethylene, its cation radical, and its excited state reinforce our conclusions regarding the effect of overlap, namely that... [Pg.261]

The effectiveness of overlap of bonding orbitals of ihe same symmetry appears to decrease as the principal quantum number increases and as the difference between the principal quantum numbers increases. This is reflected in the bond strengths shown in Table 10, The covalent radius of hydrogen is especially subject to effects of this kind, and has the values 0.3707, 0.362, 0.306. 0.284 and 0.293 A respectively in H2. HF. HCI. HBr and HI. The apparent anomaly of the P-P, S-S. and Cl-Cl bonds being stronger than the N—N. O-O. and F—F bonds has been considered in paragraph (I). [Pg.343]

Fig. 21.18 Effect of overlap interference in the Mg 3pnd 7 = 3 spectrum (a) synthesized spectrum including interference, (b) same as (a) but using only direct-excitation terms, (c) measured spectrum, and (d) corresponding overlap integral squared (from ref. 12). Fig. 21.18 Effect of overlap interference in the Mg 3pnd 7 = 3 spectrum (a) synthesized spectrum including interference, (b) same as (a) but using only direct-excitation terms, (c) measured spectrum, and (d) corresponding overlap integral squared (from ref. 12).
Resonance poles lying within the widths of each other are called overlapping resonances. When they occur, the rapid rise of the phase shift due to one pole begins before the rise due to an adjacent pole finishes. In this sense, the effects of overlapping resonances on the phase shift and, in particular, on the cross section are difficult to separate, in general. Nonetheless, the overlapping Lorentzian profiles in the time-delay spectrum... [Pg.181]

The rather good agreement with experimental data for ECM was obtained by taking into account the effect of overlap of central ion and ligand wave function, whereas the results obtained in PCM reveal the well-known weakness of this model. [Pg.531]

Farr, T. G., Bates, B. A., Ralph, R. L. Adams, J. B. (1980) Effects of overlapping optical absorption bands of pyroxene and glass on the reflectance spectra of lunar soils. Proc. 11th Lunar Planet. Sci. Conf, Geochim. Cosmochim. Acta, Suppl. 11 (Pergamon Press, New York), pp. 19-29. [Pg.490]

In the study of mixtures, differentiation between enantiomers is a two level problem which is somewhat independent of whether the LC system is chiral or conventional. The problems common to both systems are the effects of overlapping bands on the performance of the detectorfs). Overlap can be between chiral-achiral species on the one hand and co-eluted chiral-chiral with achiral on the other. On first thought the chiral-achiral distinction should be relatively easy if a chiroptical detector is used because the achiral compounds will not interfere with the detection measurement. In addition the ability of the chiroptical detector to measure both positive and negative signals makes the confirmation of the enantiomeric structure elementary [3,4], As pointed out earlier, enantiomers co-elute from conventional columns and two detectors in sequence will provide the information to measure the enantiomeric ratio provided the mixture is not racemic. Partial or total overlap of the band for a non-chiral species with the chiral eluate band increases significantly the difficulty in measuring an enantiomeric ratio. In this instance the total absorbance that is measured may include a contribution from the non-chiral species which without correction will lead to an overestimation of the amount of chiral material and an erroneous value for the enantiomeric ratio. Under these circumstances there is no other LC option but to develop a separation that is based upon a chiral system. [Pg.282]


See other pages where Effect of Overlap is mentioned: [Pg.52]    [Pg.148]    [Pg.233]    [Pg.39]    [Pg.327]    [Pg.777]    [Pg.121]    [Pg.44]    [Pg.44]    [Pg.44]    [Pg.336]    [Pg.692]    [Pg.356]    [Pg.44]    [Pg.44]    [Pg.44]    [Pg.356]    [Pg.6]    [Pg.346]    [Pg.362]    [Pg.161]    [Pg.304]    [Pg.349]    [Pg.4]    [Pg.88]    [Pg.495]   


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Orbital Effect of Overlap

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