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Subject transport parameters

Mapping of transport parameters in complex pore spaces is of interest for many respects. Apart from classical porous materials such as rock, brick, paper and tissue, one can think of objects used in microsystem technology. Recent developments such as lab-on-a-chip devices require detailed knowledge of transport properties. More detailed information can be found in new journals such as Lab on a Chip [1] and Microfluidics and Nanofluidics [2], for example, devoted especially to this subject. Electrokinetic effects in microscopic pore spaces are discussed in Ref. [3]. [Pg.205]

In Fig. 1, various elements involved with the development of detailed chemical kinetic mechanisms are illustrated. Generally, the objective of this effort is to predict macroscopic phenomena, e.g., species concentration profiles and heat release in a chemical reactor, from the knowledge of fundamental chemical and physical parameters, together with a mathematical model of the process. Some of the fundamental chemical parameters of interest are the thermochemistry of species, i.e., standard state heats of formation (A//f(To)), and absolute entropies (S(Tq)), and temperature-dependent specific heats (Cp(7)), and the rate parameter constants A, n, and E, for the associated elementary reactions (see Eq. (1)). As noted above, evaluated compilations exist for the determination of these parameters. Fundamental physical parameters of interest may be the Lennard-Jones parameters (e/ic, c), dipole moments (fi), polarizabilities (a), and rotational relaxation numbers (z ,) that are necessary for the calculation of transport parameters such as the viscosity (fx) and the thermal conductivity (k) of the mixture and species diffusion coefficients (Dij). These data, together with their associated uncertainties, are then used in modeling the macroscopic behavior of the chemically reacting system. The model is then subjected to sensitivity analysis to identify its elements that are most important in influencing predictions. [Pg.99]

Of this list, hb interactions can be sensitive to steric effects. This has been established for amino acid transport parameters such as the hydrophobicities and partition coefficients. There is some evidence that charge transfer interactions are also subject to steric effects. [Pg.4]

Reverse-Osmosis Experiments. All reverse-osmosis experiments were performed with continuous-flow cells. Each membrane was subjected to an initial pure water pressure of 2068 kPag (300 psig) for 2 h pure water was used as feed to minimize the compaction effect. The specifications of all the membranes in terms of the solute transport parameter [(Dam/ 6)Naci]> the pure water permeability constant (A), the separation, and the product rate (PR) are given in Table I. These were determined by Kimura-Sourirajan analysis (7) of experimental reverse-osmosis data with sodium chloride solution at a feed concentration of 0.06 m unless otherwise stated. All other reverse-osmosis experiments were carried out at laboratory temperature (23-25 °C), an operating pressure of 1724 kPag (250 psig), a feed concentration of 100 ppm, and a feed flow rate >400 cmVmin. The fraction solute separation (/) is defined as follows ... [Pg.145]

As an example (ft, 27 >, Figure 3 presents molecular transport parameters of methane in zeolite MaCaA, which has previously been subjected to an atmosphere of extreme humidity Pw i.,- - DO kPa at diilerent temperatures (373 373 Kc over a period of 7 and 14 h, respectively. Whilst I>,. . is found to be essentially independent... [Pg.386]

In general, one will not be surprised to find a marked asymmetry in transport parameters. The transport rate constants can have any values subject only to the constraint that in the absence of an external source of energy there is no net movement of substrate when the concentration at each face of the membrane is the same. This implies that h,/2 = for the simple pore or that h,/2k = 2/1 2 for the simple carrier. It is the value of the transport resistance / ,2 and /(ji hat will determine whether or not the system will behave asymmetrically. This can be seen by taking the ratio of the derivable half-saturation concentration and maximum velocities as follows ... [Pg.145]

The nature of the bottlenecks for proton conductance in the dry membrane state or on the way to it is, however, still the subject of debates. This wiU only be resolved after more detailed experimental studies (of macroscopic transport parameters such as proton conductance and electro-osmotic coefficients as a function of water content, or gas and liquid permeability before and after operation, and of microscopic structural probes such as small-angle neutron and X-ray scattering) will have discriminated between competing models. By and large, the direction of effects that go with dehydration is obvious enough to be introduced into phenomenological models of overall cell performance. [Pg.48]

The ultimate objective of this handbook is to enable the user to obtain numerical estimates of mass transport parameters for inclusion in quantitative models describing chemical fate. All quantitative models that address chemical fate derive their origin from the Lavoisier mass balance. On the subject of calcinations of metals (i.e., oxidation) he wrote I realize that the property of increasing weight by calcinations, which is simply a slower combustion, was not particular to metals, as has been thought, but that it was a general law in nature to which a large number of solid and liquid bodies... [Pg.7]

For the Berry phase, we shall quote a definition given in [164] ""The phase that can be acquired by a state moving adiabatically (slowly) around a closed path in the parameter space of the system. There is a further, somewhat more general phase, that appears in any cyclic motion, not necessarily slow in the Hilbert space, which is the Aharonov-Anandan phase [10]. Other developments and applications are abundant. An interim summai was published in 1990 [78]. A further, more up-to-date summary, especially on progress in experimental developments, is much needed. (In Section IV we list some publications that report on the experimental determinations of the Berry phase.) Regarding theoretical advances, we note (in a somewhat subjective and selective mode) some clarifications regarding parallel transport, e.g., [165], This paper discusses the projective Hilbert space and its metric (the Fubini-Study metric). The projective Hilbert space arises from the Hilbert space of the electronic manifold by the removal of the overall phase and is therefore a central geometrical concept in any treatment of the component phases, such as this chapter. [Pg.105]

Modeling relaxation-influenced processes has been the subject of much theoretical work, which provides valuable insight into the physical process of solvent sorption [119], But these models are too complex to be useful in correlating data. However, in cases where the transport exponent is 0.5, it is simple to apply a diffusion analysis to the data. Such an analysis can usually fit such data well with a single parameter and provides dimensional scaling directly, plus the rate constant—the diffusion coefficient—has more intuitive significance than an empirical parameter like k. [Pg.525]

One must understand the physical mechanisms by which mass transfer takes place in catalyst pores to comprehend the development of mathematical models that can be used in engineering design calculations to estimate what fraction of the catalyst surface is effective in promoting reaction. There are several factors that complicate efforts to analyze mass transfer within such systems. They include the facts that (1) the pore geometry is extremely complex, and not subject to realistic modeling in terms of a small number of parameters, and that (2) different molecular phenomena are responsible for the mass transfer. Consequently, it is often useful to characterize the mass transfer process in terms of an effective diffusivity, i.e., a transport coefficient that pertains to a porous material in which the calculations are based on total area (void plus solid) normal to the direction of transport. For example, in a spherical catalyst pellet, the appropriate area to use in characterizing diffusion in the radial direction is 47ir2. [Pg.432]

Cultivation and isolation of bacteria are in some respects more similar to an art than to a scientific method, since there is a strong element of subjectivity involved. Many diverse parameters influence the result of cultivation experiments, including the precise source of the sample (it is probably almost impossible to extract identical samples from nature), the pre-treatment of the sample (storage, cooHng, transport, mixing, sieving, filtering, etc.), the enrichment pro-... [Pg.212]

In summary, as we shall see throughout this book, meteorological parameters are extremely important, not only in determining the dispersion and transport of pollutants but also in determining their chemistry. The reader is encouraged to consult meteorology texts for a much more detailed treatment of this subject. [Pg.30]

The lifetime of emulsions is a function of various extrinsic parameters. During production, transport, and storage, emulsions are subject to a variety of fluctuating external stresses... [Pg.599]

Another subject that captured the attention of researchers in the 1970s was the identification of reaction conditions under which catalyzed and uncatalyzed reactions exhibit multiple steady states and/or oscillatory behavior. Theoretical investigations demonstrated that such behavior could arise from the nonlinear character of the reaction kinetics or from an interplay between the kinetics of a reaction and mass transport processes. A rich body of literature has now emerged detailing the space of reaction conditions and parameters within which multiple steady states and oscillations can be expected [15]. [Pg.208]


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See also in sourсe #XX -- [ Pg.779 ]




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