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Kossel crystal model

Let us assume that the constituent units of both a crystal and that of growth are simple cubes. This kind of model crystal is called a Kossel crystal, and is shown in Fig. 3.9. The 100 face is completely paved by the unit, and the surface is atomically flat. This face is called the complete plane. The 111 face, however, consists of kinks, as can be seen in Fig. 3.9, and has an uneven surface, and so it is called an incomplete plane. In contrast to [111], [110] corresponds to a face consisting entirely of steps. Kossel did not give a particular name to this t3TJe of crystal face. [Pg.38]

Figure 2 Simple faceting model based on Kossel crystal explanation. Condensation leads to faceting (a) while sublimation generates a rounding of the grains (b). Figure 2 Simple faceting model based on Kossel crystal explanation. Condensation leads to faceting (a) while sublimation generates a rounding of the grains (b).
Figure 6.6. Schematic diagram of a Kossel crystal showing F-, S-, and K-faces predicted by the PBC theory along with features predicted by various growth models. Based on Figure 1 in Sleutel ef al. (2012). Figure 6.6. Schematic diagram of a Kossel crystal showing F-, S-, and K-faces predicted by the PBC theory along with features predicted by various growth models. Based on Figure 1 in Sleutel ef al. (2012).
Fig. 3. Kossel s model of molecular attachment kinetics (layer-by-layer growth). Building blocks from a liquid nutrient phase are attached (adsorbed) by a growing crystal surface at a site (A) and migrate on it to join the most beneficial attachment places with the largest number of free bonds to be saturated by such a linking (kink sites K). (S) and (F) correspond to the stepped and closely packed (flat) faces, respectively. Fig. 3. Kossel s model of molecular attachment kinetics (layer-by-layer growth). Building blocks from a liquid nutrient phase are attached (adsorbed) by a growing crystal surface at a site (A) and migrate on it to join the most beneficial attachment places with the largest number of free bonds to be saturated by such a linking (kink sites K). (S) and (F) correspond to the stepped and closely packed (flat) faces, respectively.
Growth theories of surfaces have received considerable attention over the last sixty years as summarized by Laudise et al. [53] and Jackson [54]. The well-known model of the crystal surface incorporating adatoms, ledges and kinks was first introduced by Kossel [55] and Stranski [56]. Becker and Doring [57] calculated the rates of nucleation of new layers of atoms, and Papapetrou [58] investigated dendritic crystallization. [Pg.236]

Illustrated in Fig. 15, Frank s model suggests a crystal imperfection of the type that would result if a cut were made part way through the crystal and the two sides skewed a distance of one layer at the edge of the crystal. Growth normal to the step occurs by filling of the Kossel... [Pg.25]

As illustrated in Figure 3.9, the Kossel model divides the crystal interface into regions having unique structural attributes ... [Pg.71]

Figure 6.26. Sites for impurity adsorption on a growing crystal, based on the Kossel model a) kink (b) step (c) ledge face). After Davey and Mullin, 1974)... Figure 6.26. Sites for impurity adsorption on a growing crystal, based on the Kossel model a) kink (b) step (c) ledge face). After Davey and Mullin, 1974)...
Even for very smooth surface, it is still very rough on an atomic scale. A popular model of single crystal surface evolved from investigation on the crystal growth can trace back to the early work of Stranski and Kossel, further developed by Hirth and Pound. ... [Pg.80]

The explanations based on the crystal structure model of Kossel and Stranski of Fig. 1-35 still require detailed investigations. The development of scanning tunneling microscopy provides a valuable in situ tool to follow the structural details of electrochemical alloy corrosion. Although mechanistic studies of this kind require complicated investigations and a careful preparation technique for single crystal surfaces the application of these methods promises progress in the near future. [Pg.50]

Fig. 5.24 The Kossel model of a surface lower dimensional defects within the surface as a two dimensional imperfection. The differing energies of the structural elements with varying numbers of contacts (see numbering) are of particular importance for reactivity and growth [104], The triple contact corresponds to the so-called half-crystal site. Fig. 5.24 The Kossel model of a surface lower dimensional defects within the surface as a two dimensional imperfection. The differing energies of the structural elements with varying numbers of contacts (see numbering) are of particular importance for reactivity and growth [104], The triple contact corresponds to the so-called half-crystal site.

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See also in sourсe #XX -- [ Pg.123 ]




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