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Physical properties effective medium model

The most striking feature of the earth, and one lacking from the neighboring planets, is the extensive hydrosphere. Water is the solvent and transport medium, participant, and catalyst in nearly all chemical reactions occurring in the environment. It is a necessary condition for life and represents a necessary resource for humans. It is an extraordinarily complex substance. Stmctural models of Hquid water depend on concepts of the electronic stmcture of the water molecule and the stmcture of ice. Hydrogen bonding between H2O molecules has an effect on almost every physical property of Hquid water. [Pg.207]

The physical properties of atoms and molecules embedded in polar liquids have usually been described in the frame of the effective medium approximation. Within this model, the solute-solvent interactions are accounted for by means of the RF theory [1-3], The basic quantity of this formalism is the RF potential. It is usually variationally derived from a model energy functional describing the effective energy of the solute in the field of an external electrostatic perturbation. For instance, if a singly negative or positive charged atomic system is considered, the RF potential is simply given by... [Pg.82]

The constitutive equations of transport in porous media comprise both physical properties of components and pairs of components and simplifying assumptions about the geometrical characteristics of the porous medium. Two advanced effective-scale (i.e., space-averaged) models are commonly applied for description of combined bulk diffusion, Knudsen diffusion and permeation transport of multicomponent gas mixtures—Mean Transport-Pore Model (MTPM)—and Dusty Gas Model (DGM) cf. Mason and Malinauskas (1983), Schneider and Gelbin (1984), and Krishna and Wesseling (1997). The molar flux intensity of the z th component A) is the sum of the diffusion Nc- and permeation N contributions,... [Pg.159]

Fig. 7 Schematic representations of (a) the experimental system and (b) the three-layer theoretical model, where sjy and represent the imaginary and real dielectric constants of the JV layer. [Reprinted with permission from by Z.-F. Su, S.-G. Sun, C.-X. Wu and Z.-P. Cai, Study of anomalous infrared properties of nanomaterials through effective medium theory , J. Chem. Phys., 2008, 129, 044707. Copyright 2008, American Institute of Physics.]... Fig. 7 Schematic representations of (a) the experimental system and (b) the three-layer theoretical model, where sjy and represent the imaginary and real dielectric constants of the JV layer. [Reprinted with permission from by Z.-F. Su, S.-G. Sun, C.-X. Wu and Z.-P. Cai, Study of anomalous infrared properties of nanomaterials through effective medium theory , J. Chem. Phys., 2008, 129, 044707. Copyright 2008, American Institute of Physics.]...
The future development of porous silicon (PS)-based optoelectronic devices depends on a proper understanding of electrical transport properties of the PS material. Electrical transport in PS is influenced not only by each step of processing and fabrication methods but also by the properties of the initial base substrate. This chapter endeavors to chronologically document how the knowledge base on the nature of carrier transport in PS and the factors governing the electrical properties has evolved over the past years. The topics covered include the proposed electrical transport models including those based on effective medium theories, studies on contacts, studies on physical factors influencing electrical transport, anisotropy in electrical transport, and attempts to classify the PS material. [Pg.144]

The two-step strategy in physical modeling of catalyst layer operation is depicted in Figure 8.1 In the first step, it relates structure to physical properties of the layer considered as an effective medium. In the second step it relates these effective properties to performance. The overall relations between structure and performance can be complicated by the formation of liquid water, which affects effective properties and performance. Solution of such a model provides full relations between structure, properties, and performance, which in turn allow predicting architectures of materials and operating conditions that optimize fuel cell operation. [Pg.397]

Approach (iii) listed above refers to the use of effective medium theory (Kirkpatrick, 1973 Koplik, 1982 Levine and Cuthiell, 1986) for calculating certain average flow properties in idealised porous media models—usually simple networks. Cannella et al (1988) have recently applied this approach to the flow of power law fluids through networks of capillaries. They use this method to derive an expression for the apparent viscosity of the polymer in the porous medium which has the same overall form as the capillary bundle expression (e.g. Equation 6.18). They then adjusted the parameters in the effective medium formula in order to match their particular form of the capillary bundle formula with C = 6 (Equation 6.18). The values of the effective medium parameters are physically interpretable, and Cannella et al (1988) deduced from these that the effective radius for the flow of a power law fluid is larger than that for the flow of a Newtonian fluid. They also... [Pg.194]

The radius thus calculated from the theory of Smith and Symons does not correspond to any known property of halide ions. However, when the acceptable physical model of Franck and Platzman is combined with the concept of a variable radius, as proposed by Smith and Symons, both absolute value and environmental effects can be accounted for. This was done in the theory of Stein and Treinin (18, 19, 47), using an improved energetic cycle to obtain absolute values of r, the spectroscopically effective radius of the cavity containing the X ion. These values were then found to correspond to the known partial ionic radii in solution, as did values of dr/dT to values obtained from other experiments. The specific effects of temperature, solvents, and added salts could be used to differentiate between internal and such CTTS transitions where the electron interacts in the excited state strongly with the medium. These spectroscopic aspects of the theory were examined later in detail and compared with experiment by Treinin and his co-workers (3, 4, 32, 33, 42,48). [Pg.238]

Inorganic kineticists with an interest in solvent medium effects have not been generously supplied with reviews recently. Solvent paths and solvento-inter-mediates in substitution at square-planar centres have been discussed in a well referenced review. Unfortunately, another fully referenced and undoubtedly important review, on solvent properties of significance in determining reactivity in substitution at nickel(ii), has appeared in a periodical access to which may prove difficult for many readers. The contents of another, more general, review of solvent effects on kinetics, which includes discussion of appropriate physical models, may prove equally elusive. ... [Pg.287]


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See also in sourсe #XX -- [ Pg.163 ]

See also in sourсe #XX -- [ Pg.163 ]




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