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Lattice equation

For a sample of a homogeneous chemical composition, such as polymer lattices, Equation 12.30 can be rearranged in order to determine both particle diameter and sample density [22] ... [Pg.346]

To design a supercritical fluid extraction process for the separation of bioactive substances from natural products, a quantitative knowledge of phase equilibria between target biosolutes and solvent is necessary. The solubility of bioactive coumarin and its various derivatives (i.e., hydroxy-, methyl-, and methoxy-derivatives) in SCCO2 were measured at 308.15-328.15 K and 10-30 MPa. Also, the pure physical properties such as normal boiling point, critical constants, acentric factor, molar volume, and standard vapor pressure for coumarin and its derivatives were estimated. By this estimated information, the measured solubilities were quantitatively correlated by an approximate lattice equation of state (Yoo et al., 1997). [Pg.157]

Similar methods have been used to integrate thermodynamic properties of harmonic lattice vibrations over the spectral density of lattice vibration frequencies.21,34 Very accurate error bounds are obtained for properties like the heat capacity,34 using just the moments of the lattice vibrational frequency spectrum.35 These moments are known35 in terms of the force constants and masses and lattice type, so that one need not actually solve the lattice equations of motion to obtain thermodynamic properties of the lattice. In this way, one can avoid the usual stochastic method36 in lattice dynamics, which solves a random sample of the (factored) secular determinants for the lattice vibration frequencies. Figure 3 gives a typical set of error bounds to the heat capacity of a lattice, derived from moments of the spectrum of lattice vibrations.34 Useful error bounds are obtained... [Pg.93]

In this Chapter we introduce a stochastic ansatz which can be used to model systems with surface reactions. These systems may include mono-and bimolecular steps, like particle adsorption, desorption, reaction and diffusion. We take advantage of the Markovian behaviour of these systems using master equations for their description. The resulting infinite set of equations is truncated at a certain level in a small lattice region we solve the exact lattice equations and connect their solution to continuous functions which represent the behaviour of the system for large distances from a reference point. The stochastic ansatz is used to model different surface reaction systems, such as the oxidation of CO molecules on a metal (Pt) surface, or the formation of NH3. [Pg.515]

Reducing Agents Smectites may be reduced in one of several differ-ent ways (Table I), either in aqueous suspension or in the dry state, but the most effective methods require intimate contact between the clay surfaces and the reducing agent. The diffusion of reactants and products, such as the diffusion of H20 out of or H into the clay lattice (Equations 2 and 3, p. 350), appears to be an important aspect... [Pg.332]

The parameter S measures the interaction between the dopant ion and the vibrating lattice. Equation [5] shows that if S is large, the Stokes shift is also large. Equation [4] shows that S is immediately related to the offset of the parabolas in the configurational coordinate diagram (Fig. 3). This offset, AQ = Q o - Qo), may vary considerably as a function of the dopant ion and as a function of the vibrating lattice, as we will see below. [Pg.325]

If the quasi-lattice equations for the activity coefficients will be expanded up to the second order AS, we obtain... [Pg.134]

Here, e is the electronic chaige unit (e = 4.8 X 10"esu), Nq is Avogadro s number, A is the Madelung constant, and n is a parameter arising from repulsive forces that build up as atoms come into contact and atomic orbitals begin to overlap. The distance between ion pairs, r, can be determined for an ionic solid from the known radii of the constituent ions. For solid KQ, as an example, the radii of and Cl" are 1.33 A (Angstrom) and 1.81 A, respectively. The value of is then 1.33 + 1.81 = 3.14 A, and n is known to be 9 for this particular lattice. Equation 1.3 can then be used to calculate the overall lattice energy of KCl and other ionic solids. [Pg.5]

Combining equations 5.13 and 5.15 gives an expression for the lattice energy that is based on an electrostatic model and takes into account Coulombic attractions, Coulombic repulsions and Born repulsions between ions in the crystal lattice. Equation 5.16 is the Born-Lande equation. [Pg.154]

In order to understand the origin of the paraelectric to ferroelectric transition and the accompanying structural phase transitions it is important to understand how the local field is affected by the polarization of the lattice. Equation (14A.3), which relates the local field Eioc to the applied field , and the polarization P can be generalized to read... [Pg.540]

We now develop the matrix representation for the wavelet transform that allows us to represent the pyramidal synthesis and analysis lattice equations for finite length signals in a convenient matrix computational framework. We first introduce the concept of a wavelet matrix in the context of infinite signals. [Pg.95]

The decomposition and reconstruction lattice equations can then be rewritten as a simple recursive matrix multiplication. [Pg.96]

For reasons of convenience, and as will be shown in Chapter 6. the decomposition and reconstruction lattice equations can also be written as a pair of equations of recursive matrix products where we separate out the low-pass and high-pass filter coefficients in the form of infinite matrices Cj and Dy. That is. [Pg.97]

It is also assumed, following Simkovich (13.), that protons can dissolve interstitially in the iron sulfide lattice (equation 24). The requirement for electroneutrality in the iron sulfide lattice leads to equation 25. Assuming the ratio of hydrogen partial pressure to hydrogen sulfide partial pressure to be constant, equations 23 through 25 can be rearranged to ... [Pg.313]

BEC Beckmann, E.J., Koningsveld, R., and Porter, R.S., Mean-field lattice equations of state. 3. [Pg.546]

Harrison and colleagues [40] measured the interfadal tension between SCCO2 and polyethylene glycol (MW 600) using a tandem variable-volume pendent drop tensiometer, as shown schematically in Fig. 10.3. At 45 °C the interfacial tension between the PEG-CO2 rich phase and the SCCO2 phase was reduced from 6.9 dyn cm at 100 bar to 3.08 dyn cm at 300 bar. Experimental observations were accurately predicted using a gradient model which utilized the lattice equation of state. In another piece of work, the effect of surfactants on poly-mer/C02 interfacial tension was addressed [42]. [Pg.211]

Landau-Zener theory, 2-4 Langmuir-Blodgett, 9-17, 9-29 Laser action, 22-1-22-69 Lasing, 4-11 Latex, 8-8-8-9, 8-12 Lattice equation of motion, 2-5-6 Layer, 18-4, 18-7, 18-13, 18-27 Layer-by-layer films, 14-30, 14-45 Layer-by-layer self-assembly of rr-pATs,... [Pg.1021]

Lattice Boltzmann equation can be obtain through two ways, first is through of "cellular automaton" and second starting from Boltzmann equation, it was review previously, for carries out derivation of Boltzmann s lattice equation is necessary the space time discretization. Immediately presents brief description of second way, it shows by p>ace series. [Pg.80]

R. Koningsveld, L.A. Kleintjens, A.M. Leblans-Vinck, Mean-field lattice equations of state. 1. Possible molecular basis for empirical parameters. J. Phys. Oiem. 91, 6423-6428 (1987)... [Pg.1724]

Mumford, D. An algebra-geometric construction of commuting operators and of solution to the Toda lattice equation and related nonlinear equations. Proc, Intern, Symp, on Algebraic Geometry, Kyoto (1977), 115-153. [Pg.330]


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See also in sourсe #XX -- [ Pg.224 ]




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Bragg equation reciprocal lattice

Lattice Boltzmann equation

Lattice diffusion equation

Lattice dynamics basic equation

Lattices Bragg equation

Sanchez-Lacombe lattice fluid equation

Sanchez-Lacombe lattice fluid equation state

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