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Band model liquids

Wilson JA (1977) A Generalized Configuration - Dependent Band Model for Lanthanide Compounds and Conditions for Interconfiguration Fluctuations. 32 57-91 Wilson MR (1999) Atomistic Simulations of Liquid Crystals. 94 41-64 Winkler H, see Trautwein AX (1991) 78 1-96... [Pg.258]

C with a water content of 0.075 kg/kg. Although heat and mass transfer rates were relatively insensitive to the choice of the model, the amount of fog formation was not. The models neglect the effects of condensation within the boundary layer, thus underestimating fog formation by a factor of up to three. The amount of fog formed in flue-gas washing plants increased up to a maximum value with decreasing feed-water temperature over a narrow band of liquid-to-gas ratios. [Pg.307]

Fig. 3.3. The simplest band model for an amorphous or liquid semiconductor (a). Fig. 3.3. The simplest band model for an amorphous or liquid semiconductor (a).
Band theory is basically a one-electron theory. Electron-electron interactions are only included in the form of an average contribution to the effective electron-ion interaction potential. Thus, band theory should be most informative for modeling the electronic structure of liquids for which the MNM transition is of the Bloch-Wilson band-overlap variety. Fig. 2.13 illustrates some typical results for the electronic density of states of mercury in a series of structures with constant interatomic separation. With increasing density, the band-overlap transition is clearly evident as the gap closes between the lower, predominantly s-like band and the upper p-band. These results agree qualitatively with the observed electronic properties of expanded mercury although, as we shall see in chapter 4, the actual MNM transition occurs in a density range for which the band model still predicts a nonvanishing density of states at the Fermi level. [Pg.44]

An important consequence of the energy band model is the dependence of the electron energy W in a band on the wave vector k. The details of W(k) depend on the crystal structure (which we assume to be maintained also in the liquid near the melting point). In some cases, W(k) for the conduction and valence band can be approximated by parabolic functions... [Pg.3]

There are three broad versions of Fermi liquid models in the literature, each is applicable for specific problems. The one-band model has provided the first understanding of the low-temperature thermodynamic and transport properties. The interpretation of inelastic neutron scattering data requires a two-band hybridization model. The band model based on the local-density functional approximation is by far the most elaborate noninteracting Fermi fluid model. We will discuss only the basic principle of this approach because the details appear elsewhere in this volume. [Pg.105]

However, the relation between frequency and conformational disorder is not linear. This necessitates the use of a simple two-component overlapping band model to obtain the proportions of gel and liquid crystal phases (26). [Pg.133]

The interpretation of these remarkable properties has excited considerable interest whilst there is still some uncertainty as to detail, it is now generally agreed that in dilute solution the alkali metals ionize to give a cation M+ and a quasi-free electron which is distributed over a cavity in the solvent of radius 300-340 pm formed by displacement of 2-3 NH3 molecules. This species has a broad absorption band extending into the infrared with a maximum at 1500nm and it is the short wavelength tail of this band which gives rise to the deep-blue colour of the solutions. The cavity model also interprets the fact that dissolution occurs with considerable expansion of volume so that the solutions have densities that are appreciably lower than that of liquid ammonia itself. The variation of properties with concentration can best be explained in terms of three equilibria between five solute species M, M2, M+, M and e ... [Pg.77]

Jupiter s moon Europa has only been the subject of intense scientific investigation in recent years it is considered to be a member of that small group of heavenly bodies which could perhaps accommodate life (or a precursor of life). About 20 years ago, the Voyager passes afforded sensational pictures of Europa. These showed a network of linear bands, of differing breadths, on a very bright surface. The mean density was calculated as 3,018 35 kg/m3, and the surface temperature measured was 90-95 K. Circumstantial evidence points to either a surface consisting of water ice, or the presence of liquid water or warm ice under the surface. Three models were proposed (Oro et al., 1992) ... [Pg.49]


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