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Mercury lattice structure

Fig. 5 shows data from a simulation of TIP4P water that is confined on both sides by a rhombohedral mercury crystal with (111) surface structure. Bosio et al. [135] deduce from their X-ray studies that a solid o-mercury lattice with a larger lattice constant in the z direction may be used as a good structural model for liquid mercury. Thus, the mercury phase was modeled as a rigid crystal in order to simplify the simulations. The surface of such a crystal shows rather low corrugation. [Pg.359]

Table 4 DFT results for lattice structure of solid mercury. Calculated lattice parameters are in A and cohesive energies are in eV. [We use negative values throughout as not all our calculated values (e.g., in Hartree-Fock) are binding.]... [Pg.181]

D Lattice structure of mercury influence of electronic correlation... [Pg.187]

Figure 28.16 The Radial Distribution Function of Solid and Liquid Mercury. Since the solid has a lattice structure, the positions of neighboring atoms give narrow blips in the radial distribution function. In the liquid, the disorder that is present makes the function into a smooth curve, which shows vestiges of the crystal lattice. From D. Tabor, Gases, Liquids and Solids, 2nd ed., Cambridge University Press, Cambridge, England, 1979, p. 197. Figure 28.16 The Radial Distribution Function of Solid and Liquid Mercury. Since the solid has a lattice structure, the positions of neighboring atoms give narrow blips in the radial distribution function. In the liquid, the disorder that is present makes the function into a smooth curve, which shows vestiges of the crystal lattice. From D. Tabor, Gases, Liquids and Solids, 2nd ed., Cambridge University Press, Cambridge, England, 1979, p. 197.
The evidence for the existence of the reported third modification of tin is very weak. The hexagonal crystals which are formed by tin in the presence of mercury26 have a simple structure, with atoms at the points of a hexagonal lattice,26 with lattice constants27 o0 = 3.198 A. arid c0 = 2.980 A. for the alloy with 4.9% mercury. Neglecting the effect of the small number of atoms of mercury (which differ little in size from the atoms of tin), we calculate the value f (l) = 1.401 A. from the coordination 2.980 (2), 3.198 (6) and the valence v = 2.44. Hence in this alloy tin has its lower valence. [Pg.356]

Figure 27. Crystal lattice of cadmium pigments (wurtzite structure) a) Sulfur (selenium) b) Cadmium (zinc, mercury)... Figure 27. Crystal lattice of cadmium pigments (wurtzite structure) a) Sulfur (selenium) b) Cadmium (zinc, mercury)...
In 1954, Perutz introduced the isomorphous replacement method for determining phases. In this procedure a heavy metal, such as mercury or platinum, is introduced at one or more locations in the protein molecule. A favorite procedure is to use mercury derivatives that combine with SH groups. The resulting heavy metal-containing crystals must be isomorphous with the native, i.e., the molecules must be packed the same and the dimensions of the crystal lattice must be the same. However, the presence of the heavy metal alters the intensities of the spots in the diffraction pattern and from these changes in intensity the phases can be determined. Besides the solution to the phase problem, another development that was absolutely essential was the construction of large and fast computers. It would have been impossible for Perutz to determine the structure of hemoglobin in 1937, even if he had already known how to use heavy metals to determine phases. [Pg.133]

What factors determine whether an elemental substance adopts a metallic or a covalent structure From the simple model for metallic bonding, which views a metal as a lattice of cations embedded in a sea of delocalised electrons, it may be supposed that atoms having low ionisation potentials are most likely to become assembled as metallic substances. This correlation is far from perfect, however. Thus the first and second ionisation energies of mercury are comparable with those of sulphur, but the alchemists viewed elemental mercury and sulphur as the quintessential metal and nonmetal respectively. A closely-related correlation can be found with electronegativity. [Pg.269]

An x-ray study of allopurinol (53) indicates that it exists in the 1H form. It is apparent that hydrogen bonding patterns in the crystal lattice may be responsible for the preferred protonation site in the solid state. Intramolecular N(l)-H-N(7) and N(5)-H-0(4) contacts for allopurinol and N(2)-H-0(4) contacts for allopurinol cation are observed. The crystal structure of the methyl mercury complex (56) indicated that N-l and N-5 are respective coordination sites. Similar structures have been proposed for allopurinol copper complexes <87ZN(B)195>. [Pg.436]

Mercury is not a typical electrode material it is liquid, and there is constant movement of atoms on the surface in contact with solution. A solid electrode has a well-defined structure, probably polycrystalline and in some cases monocrystalline. In a solid metallic electrode conduction is predominantly electronic owing to the free movement of valence electrons, the energy of the electrons that traverse the interface being that of the Fermi level, EF (Section 3.6), giving rise to effects from the electronic distribution of the atoms in the metallic lattice already mentioned. [Pg.56]


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See also in sourсe #XX -- [ Pg.135 ]




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Mercury structure

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