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Lattice bonds

When an impacting particle transfers energy to a near sinface carbon atom in an amount sufficient to overcome the lattice bond energy or surface binding energy, some carbon atoms may be displaced and move in a direction defined by the angle... [Pg.412]

It is important to note that we assume the random fracture approximation (RPA) is applicable. This assumption has certain implications, the most important of which is that it bypasses the real evolutionary details of the highly complex process of the lattice bond stress distribution a) creating bond rupture events, which influence other bond rupture events, redistribution of 0(microvoid formation, propagation, coalescence, etc., and finally, macroscopic failure. We have made real lattice fracture calculations by computer simulations but typically, the lattice size is not large enough to be within percolation criteria before the calculations become excessive. However, the fractal nature of the distributed damage clusters is always evident and the RPA, while providing an easy solution to an extremely complex process, remains physically realistic. [Pg.380]

Specific adsorption of ligands can enhance or inhibit dissolution rates by altering the strength and lability of Me-0 lattice bonds. Salicylate, oxalate, and citrate promote the dissolution of alumina (40). In the presence of ligand (L) the dissolution rate becomes (7 ) , ... [Pg.458]

Water molecules are polar and can attract charged ions bonded in a crystalline lattice. Bonds between the ions break, and a water solution results. [Pg.185]

Koutecky has shown that an atom-lattice bond may be localized with only the surface atom taking part in the bond. 9... [Pg.145]

Initially, the protein-like HP sequences were generated in [18] for the lattice chains of N = 512 monomeric units (statistical segments), using for simulations a Monte Carlo method and the lattice bond-fluctuation model [34], When the chain is a random (quasirandom) heteropolymer, an average over many different sequence distributions must be carried out explicitly to produce the final properties. Therefore, the sequence design scheme was repeated many times, and the results were averaged over different initial configurations. [Pg.11]

Fig. 8. Energy of the 3 Pr. multiplet of I. aCl3 Pr3 as a function of the host lattice equatorial and apical La—Cl distances (from Gregorian et al., 1989). The circles correspond to the multiplet energies of Pr3+ in RC13 (R = La, Pr, Nd, Gd) and the respective host-lattice bond distances at ambient pressure. Triangles denote the high-pressure... Fig. 8. Energy of the 3 Pr. multiplet of I. aCl3 Pr3 as a function of the host lattice equatorial and apical La—Cl distances (from Gregorian et al., 1989). The circles correspond to the multiplet energies of Pr3+ in RC13 (R = La, Pr, Nd, Gd) and the respective host-lattice bond distances at ambient pressure. Triangles denote the high-pressure...
The high frequency shift in the asymmetric P—O" stretching frequency caused by adsorption on hydroxyapatite appears to be a perturbation of lattice bonds as a result of surface changes. The minimum specific surface necessary to cause a lattice shift by a particular adsorbate has not been ascertained. The difference in sensitivity between different preparations of hydroxyapatite is shown in Table IV. These differences are best explained, at present, by differences in surface groups resulting from minor differences in washing procedure. Rootare, Deitz, and Carpenter (10) discuss hydrolysis reactions of surface phosphate ions and the... [Pg.137]

Figure 10 illustrates that Crw effectively inhibits the proton-promoted dissolution of goethite. Cr(III) adsorbs even at low pH and, as bi- or polynuclear surface complexes, blocks surface sites from being protonated. Furthermore, isomorphically substituted Cr3+ ions, characterized by an extremely low water-exchange rate, impart inertness to the surface lattice bonds. [Pg.23]

An interstitial atom in an antibonding (AB) site is bonded to its nearest neighbour lattice atom. This location is often found in H complexes involving a donor atom and results in the relaxation of the local lattice bonding. There also exists a special interstitial structure, the di-interstitial configuration. Incidentally, Fig. 2.5 shows the ternary symmetry of the sphalerite lattice along a <111 > direction. This is analogous with the wurtzite structure, where... [Pg.32]

Observations indicate that Ca-rich feldspars are more susceptible to organo-ligand promoted dissolution than are the Na-or K-feldspars in experiments, soils and lithified sediment (32.70.73). although the proton-promoted dissolution rates of albite, anorthite and K-feldspar are approximately equal (22). The rate of feldspar dissolution promoted by organo-ligands is proposed to increase when inner-sphere adsorption of organo-ligands on aluminosilicates weakens critical crystal lattice bonds at the site of adsorption (77). [Pg.501]

Hydrocarbon species, particularly the CH,j (x = 0-3) radicals, compete with atomic H to cap the open radical sites, although the hydrocarbon adsorption reactions are much slower than the H termination reaction. Once a gas-phase hydrocarbon has been adsorbed onto the surface or has inserted into a surfiice bond, subsequent reactions take place to form additional bonds with adjacent surface carbon species, eventually concluding when a carbon atom has formed all four (if diamond) or three (ifgraphitic material) of its lattice bonds. [Pg.18]

Figure 18.2.2 Energy bands and two-dimensional representation of an intrinsic semiconductor lattice, (a) At absolute zero (or Eg >> 47), assuming a perfect lattice no holes or electrons exist. (b) At a temperature where some lattice bonds are broken, yielding electrons in the conduction band and holes in the valence band. Ep represents the Fermi level in this intrinsic semiconductor. Figure 18.2.2 Energy bands and two-dimensional representation of an intrinsic semiconductor lattice, (a) At absolute zero (or Eg >> 47), assuming a perfect lattice no holes or electrons exist. (b) At a temperature where some lattice bonds are broken, yielding electrons in the conduction band and holes in the valence band. Ep represents the Fermi level in this intrinsic semiconductor.
Information such as spacing in the crystal lattice, bond lengths and angles, crystal size, purity and texture can all be obtained using XRD. Information about thermal motion can also be obtained. Overall, a picture of the molecules, unit cells and the crystal can be built up. [Pg.171]

The preceding definitions are centered on lattice sites a fraction of sites are randomly assigned to correspond to the extracellular space. A tissue could also be defined, based on lattice bonds by allowing the probability p to represent the fraction of open bonds in the lattice. Interconnected extracellular space then exists at all sites that are connected by open bonds. Bond percolation and site percolation are two distinct methods of describing space each leads to quantitative predictions of material properties. The site percolation description corresponds more naturally to the porous materials for example, in site percolation, the lattice probability p is exactly equal to the extracellular volume fraction. [Pg.84]

Chemical bonds may be understood as the physical forces which hold together chemical systems such as molecules and lattices. Bonds hold molecules together (both internally, and to one another), because work must be done against electrical forces to separate the parts of the system. Bonds form because of those electrical forces. [Pg.227]

Fig. 3 In the BFM model each monomer occupies a unit cube in a 3D simple cubic lattice. Bonds between monomers are taken in a range between 2 and /lO lattice units which ensure cut-avoiding during local moves. In a Monte Carlo step a monomer is chosen randomly and tries to move into one of the six possible nearest neighbor positions. The move is rejected if the new lattice places are occupied by other monomers (excluded volume). If the energy difference between the new and the old monomer position is positive, the move is only accepted with the corresponding Metropohs rate. The interaction energy between different monomer species (A and B) is calculated in three shells around the given monomer as indicated in the figure. We implement only repulsive interaction between different monomer species. AH other interactions are athermal... Fig. 3 In the BFM model each monomer occupies a unit cube in a 3D simple cubic lattice. Bonds between monomers are taken in a range between 2 and /lO lattice units which ensure cut-avoiding during local moves. In a Monte Carlo step a monomer is chosen randomly and tries to move into one of the six possible nearest neighbor positions. The move is rejected if the new lattice places are occupied by other monomers (excluded volume). If the energy difference between the new and the old monomer position is positive, the move is only accepted with the corresponding Metropohs rate. The interaction energy between different monomer species (A and B) is calculated in three shells around the given monomer as indicated in the figure. We implement only repulsive interaction between different monomer species. AH other interactions are athermal...

See other pages where Lattice bonds is mentioned: [Pg.311]    [Pg.37]    [Pg.351]    [Pg.162]    [Pg.174]    [Pg.457]    [Pg.23]    [Pg.52]    [Pg.155]    [Pg.776]    [Pg.781]    [Pg.351]    [Pg.132]    [Pg.79]    [Pg.39]    [Pg.221]    [Pg.36]    [Pg.82]    [Pg.105]    [Pg.325]    [Pg.653]    [Pg.654]    [Pg.170]    [Pg.269]    [Pg.294]    [Pg.480]    [Pg.38]    [Pg.54]    [Pg.59]   
See also in sourсe #XX -- [ Pg.18 ]




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Bonding lattices

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