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Elemental crystals

A related advantage of studying crystalline matter is that one can have synnnetry-related operations that greatly expedite the discussion of a chemical bond. For example, in an elemental crystal of diamond, all the chemical bonds are equivalent. There are no tenninating bonds and the characterization of one bond is sufficient to understand die entire system. If one were to know the binding energy or polarizability associated with one bond, then properties of the diamond crystal associated with all the bonds could be extracted. In contrast, molecular systems often contain different bonds and always have atoms at the boundary between the molecule and the vacuum. [Pg.86]

ELEMENT CRYSTAL STRUCTURE DENSITY (g/ml) MELTING POINT (°Q HEAT OF vaporization (kcal/mole) ELECTRICAL CONDUCTIVITY (ohm-cm)r ... [Pg.381]

The high-temperature contribution of vibrational modes to the molar heat capacity of a solid at constant volume is R for each mode of vibrational motion. Hence, for an atomic solid, the molar heat capacity at constant volume is approximately 3/. (a) The specific heat capacity of a certain atomic solid is 0.392 J-K 1 -g. The chloride of this element (XC12) is 52.7% chlorine by mass. Identify the element, (b) This element crystallizes in a face-centered cubic unit cell and its atomic radius is 128 pm. What is the density of this atomic solid ... [Pg.380]

Corresponding to its inferior space filling, the body-centered cubic packing of spheres is less frequent among the element structures. None the less, 15 elements crystallize with this structure. As tungsten is one of them, the term tungsten type is sometimes used for this kind of packing. [Pg.153]

The brittle, silvery, shiny metal was long considered the last stable element of the Periodic Table. In 2003 it was unmasked as an extremely weak alpha emitter (half-life 20 billion years). Like thulium, there is only one isotope. Bismuth alloys have low melting points (fuses, fire sprinklers). As an additive in tiny amounts, it imparts special properties on a range of metals. Applied in electronics and optoelectronics. The oxichloride (BiOCl) gives rise to pearlescent pigments (cosmetics). As bismuth is practically nontoxic, its compounds have medical applications. The basic oxide neutralizes stomach acids. A multitalented element. Crystallizes with an impressive layering effect (see right). [Pg.77]

The heat balance follows a similar relationship with the rate of latent heat release in proportion with the amount of element crystallized... [Pg.362]

Element Crystal Lattice parameters Atomic Molar Density/... [Pg.517]

Silvery-white, brittle metallic element crystal system-hexagonal, rhombo-hedral also, exists in two unstable allotropic forms— a yellow modification and a dark-grey lustrous amorphous powder—both of which revert to crystalline form hardness 3.0 to 3.5 Mohs density 6.697g/cm3 melting point 630.5°C boiling point 1635°C electrical resistivity 39.1 microhm-cm at 0°C magnetic susceptibifity —0.87 x 10 emu/g. [Pg.49]

However, FriedeFs law no longer holds if a compound containing an anomalous scatterer, besides other elements, crystallizes in a non-centrosymmetric space group then the following inequalities between Friedel pairs apply ... [Pg.384]

High resolution structural information about the transmembrane elements of membrane receptors is not currently available, since it is not yet possible to obtain transmembrane receptors in crystalline form for structural analysis. Due to the hydrophobic nature of the transmembrane elements, crystallization is very difficult. [Pg.177]

The face-centred cubic lattice is very common. Many metallic elements crystallize in this form so also do many binary compounds such as alkali halides and the oxides of diva-lent metals. Thus the powder photo-... [Pg.236]

As an illustration, consider the isothermal, isobaric diffusional mixing of two elemental crystals, A and B, by a vacancy mechanism. Initially, A and B possess different vacancy concentrations Cy(A) and Cy(B). During interdiffusion, these concentrations have to change locally towards the new equilibrium values Cy(A,B), which depend on the local (A, B) composition. Vacancy relaxation will be slow if the external surfaces of the crystal, which act as the only sinks and sources, are far away. This is true for large samples. Although linear transport theory may apply for all structure elements, the (local) vacancy equilibrium is not fully established during the interdiffusion process. Consequently, the (local) transport coefficients (DA,DB), which are proportional to the vacancy concentration, are no longer functions of state (Le., dependent on composition only) but explicitly dependent on the diffusion time and the space coordinate. Non-linear transport equations are the result. [Pg.95]

There were several early discussions on the application of transition state theory to activated diffusional transport in crystals [W. Jost (1955)]. The Vineyard treatment [G. Vineyard (1957)] adapts Eyring s concept to the case of vacancy diffusion in a (elemental) crystal and clarifies it by taking into account the many-body features of this diffusion process. [Pg.102]

Each rubidium halide (Group VIIA element) crystallizing in the NaCl-type lattice has a unit cell length 30 pm greater than that for the corresponding potassium salt of the same halogen. What is the ionic radius of Rb+ computed from these data ... [Pg.179]

In an illustrative way, the standard enthalpy of monatomic gaseous elements can be seen as the dissociation enthalpy of a (macromolecular) elemental crystal [39,40]. This value is a substantial constituent of the binding enthalpy of compounds [41], Therefore, a coupling between the standard or the atomic standard formation enthalpies of solid and gaseous compounds and the standard enthalpy of monatomic gaseous elements can be expected and is certainly observed, e.g., see Figure 4. [Pg.222]

Let us consider an elemental crystal first (with defect d). If Nd identical defects are formed in such a crystal of N identical elements, a local free enthalpy of Agd° is required to form a single defect, and if interactions can be neglected, the Gibbs energy of the defective crystal (GP refers to the perfect crystal) is... [Pg.13]

For a description of how Ag° can be atomistically computed, the reader is referred to the literature.18 3840) Owing to the infinitely steep decrease of the configurational entropy term (cf. last term in Eq. 24) there is a minimum in G (see Fig. 4) that occurs in our elemental crystal if the... [Pg.14]

The element crystallizes in a diamond cubic lattice. It is brittle, and has a bright metalhc luster. Ge can absorb H2,02,... [Pg.1406]

The BFS strain energy can be computed by any method appropriate for the calculation of pure element crystals. Due to its consistency with the determination of the chemical energy contribution, we choose the ECT [25,26] for its computation. [Pg.39]


See other pages where Elemental crystals is mentioned: [Pg.196]    [Pg.87]    [Pg.1265]    [Pg.173]    [Pg.332]    [Pg.29]    [Pg.179]    [Pg.179]    [Pg.173]    [Pg.179]    [Pg.872]    [Pg.35]    [Pg.126]    [Pg.49]    [Pg.242]    [Pg.7]    [Pg.193]    [Pg.227]    [Pg.252]    [Pg.253]    [Pg.305]    [Pg.345]    [Pg.381]    [Pg.446]    [Pg.423]    [Pg.5]    [Pg.241]    [Pg.544]    [Pg.38]   
See also in sourсe #XX -- [ Pg.339 , Pg.340 , Pg.372 , Pg.373 ]




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Assimilation of Trace Elements in Crystals

Changes in element and isotope ratios upon closed-system crystallization

Crystal Structures of Some Elements

Crystal chemistry elements

Crystal divalent elements

Crystal elements

Crystal field theory matrix elements

Crystal growth 25 symmetry elements

Crystal matrix elements

Crystal optical properties elements

Crystal structure elements

Crystal structure elements, phase transitions

Crystal structure of elements

Crystal structure rare earth elements

Crystal systems characteristic symmetry element

Crystallizing volume element

Crystals symmetry elements

Cubic crystal system, crystallographic elements

Elements crystal ionic radii

Elements crystal phase transitions

Elements, crystal radii

Equilibria in Elemental Crystals

Lanthanide elements crystal field effects

Lanthanide elements, actinides compared crystal structures

Liquid Crystal Logic Elements

Microscopic Symmetry Elements in Crystals

Nano element crystal

Partitioning of Elements Between Aqueous Solution and Crystal

Point defects in crystals of elements

Quartz-crystal measuring element

Rare earth elements crystallization

Rare earth elements fractional crystallization

Structures of the Elements and Some Molecular Crystals

Symmetry elements in crystals

Transition element ions, crystal field

Transition element ions, crystal field splittings

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