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Cations atomic structure

Heterogeneities associated with a metal have been classified in Table 1.1 as atomic see Fig. 1.1), microscopic (visible under an optical microscope), and macroscopic, and their effects are considered in various sections of the present work. It is relevant to observe, however, that the detailed mechanism of all aspects of corrosion, e.g. the passage of a metallic cation from the lattice to the solution, specific effects of ions and species in solution in accelerating or inhibiting corrosion or causing stress-corrosion cracking, etc. must involve a consideration of the detailed atomic structure of the metal or alloy. [Pg.9]

Fig. 4 Proposed defect cluster model in as-made zeolites with quaternary ammonium cations as structure directing agents (SDAs) hydrogen bond distances of 1.68 A are determined experimentally from the H NMR chemical shift of 10.2 ppm X and Y are atoms not further specified in the SDA the interaction between the SDA and the SiO- group is assumed based on bond valence arguments (see text)... Fig. 4 Proposed defect cluster model in as-made zeolites with quaternary ammonium cations as structure directing agents (SDAs) hydrogen bond distances of 1.68 A are determined experimentally from the H NMR chemical shift of 10.2 ppm X and Y are atoms not further specified in the SDA the interaction between the SDA and the SiO- group is assumed based on bond valence arguments (see text)...
Typically, functional porins are homotrimers, which assemble from monomers and then integrate into the outer membrane. The general porins, water-filled diffusion pores, allow the passage of hydrophilic molecules up to a size of approximately 600 Daltons. They do not show particular substrate specificity, but display some selectivity for either anions or cations, and some discrimination with respect to the size of the solutes. The first published crystal structure of a bacterial porin was that of R. capsulatus [48]. Together with the atomic structures of two proteins from E. coli, the phosphate limitation-induced anion-selective PhoE porin and the osmotically regulated cation-selective OmpF porin, a common scheme was found [49]. Each monomer consists of 16 (3-strands spanning the outer membrane and forming a barrel-like structure. [Pg.285]

Fig. 30 The hydrogen-bonded chloride-mediated 1 -D chain in the structure of [Cu(Lee)2]C12-H20 showing the alternating arrangement of [Cu(Lee)2]2+ cations (atom identification as for Fig. 1 plus copper large light grey circles chlorine large dark grey circles) [61]... Fig. 30 The hydrogen-bonded chloride-mediated 1 -D chain in the structure of [Cu(Lee)2]C12-H20 showing the alternating arrangement of [Cu(Lee)2]2+ cations (atom identification as for Fig. 1 plus copper large light grey circles chlorine large dark grey circles) [61]...
Fig. 2. Transient absorption of Pe -Tripod probed at 570 nm (squares). The measured signals a superposition of cation absorption and stimulated emission (negative signal). The data were fitted to a three-exponential rise (solid line) revealing time constants of 30 fs (42%), 720 fs (33%) and 4.3 ps (25%). The inset illustrates the atomic structure of the Pe -Tripod and its LUMO state, both calculated on a semi-empirical level. Fig. 2. Transient absorption of Pe -Tripod probed at 570 nm (squares). The measured signals a superposition of cation absorption and stimulated emission (negative signal). The data were fitted to a three-exponential rise (solid line) revealing time constants of 30 fs (42%), 720 fs (33%) and 4.3 ps (25%). The inset illustrates the atomic structure of the Pe -Tripod and its LUMO state, both calculated on a semi-empirical level.
Solid-state NMR spectroscopy is a powerful technique for the determination of structure in amorphous solids and for species in solution. Extensive studies of NMR shieldings of electropositive or cationic atoms, such as Si, have established that shieldings are strongly influenced by the composition of the 1st coordination sphere and also show significant, consistent and easily measurable trends related to the identify and geometry of 2nd coordination sphere atoms. Atoms in the 3rd and more distant coordinate spheres generally have little effect upon the shielding. [Pg.304]

From the discussion above, it can be seen how the atomic structure of phyllosilicate clays plays a key role in determining the final state of clay particles in aqueous media. The presence of structural charges, neutralizing cations, and the capacity of forming hydrogen bonds between different layers produces a system that can be completely delaminated, completely flocculated, or in an intermediate state having floes mixed with isolated layers. Whether the more stable situation corresponds to isolated layers, floes, or a mixture depends on the type of clay, its concentration, pH, concentration and type of supporting electrolyte, and so on. [Pg.92]

It is also possible to prepare crystalline electrides in which a trapped electron acts in effect as the anion. The bnUc of the excess electron density in electrides resides in the X-ray empty cavities and in the intercoimecting chaimels. Stmctures of electri-dides [Li(2,l,l-crypt)]+ e [K(2,2,2-crypt)]+ e , [Rb(2,2,2-crypt)]+ e, [Cs(18-crown-6)2]+ e, [Cs(15-crown-5)2]" e and mixed-sandwich electride [Cs(18-crown-6)(15-crown-5)+e ]6 18-crown-6 are known. Silica-zeolites with pore diameters of vA have been used to prepare silica-based electrides. The potassium species contains weakly bound electron pairs which appear to be delocalized, whereas the cesium species have optical and magnetic properties indicative of electron locahzation in cavities with little interaction between the electrons or between them and the cation. The structural model of the stable cesium electride synthesized by intercalating cesium in zeohte ITQ-4 has been coirfirmed by the atomic pair distribution function (PDF) analysis. The synthetic methods, structures, spectroscopic properties, and magnetic behavior of some electrides have been reviewed. Theoretical study on structural and electronic properties of inorganic electrides has also been addressed recently. ... [Pg.64]

Distortion such as this may result in the exclusion of one or more of the crown O atoms from the coordination sphere of the metal. This situation is found in another Na+ complex of 18-crown-6 (92), again showing that subtle structural differences can occur for the same cation-crown combination. Extremely large and flexible crown ethers can completely encapsulate metal ions, as is found in the K+ complex of a 30-crown-10 ligand, and the Na+ complex of a 24-crown-8 derivative, for example. This wrapping of the cation bears structural... [Pg.5072]

Indeed, the preparation of a truly stoichiometric metal antimonate, MSb04 (M = metal), is a difficult task. The method of preparation employed affects the nature of the catalysts prepared, but in general non-stoichiometry is a particular feature of these systems [47-50]. The most striking case is the V/Sb/O system, for which the composition Vo.92Sbo.92O4 (quasi-VSh04) has been reported for the catalyst with the V/Sb atomic ratio equal to 1/1 [49]. This cation-deficient structure, which has 0.04 cationic positions unoccupied per anion, contains Sb, while... [Pg.786]

The essential condition for ferromagnetic behaviour is the presence of magnetic dipoles in a substance. This is set by atomic structure. At least one of the ferrite cations must have one or more unpaired electrons. The spinning unpaired electron will impart to the ion a magnetic moment. This condition is complied with in the group of transition elements (Mn, Fe, Co, Ni, Cu, etc.). [Pg.379]


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See also in sourсe #XX -- [ Pg.40 ]




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