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Measurement of transport diffusion

Microscopic Measurement of Transport Diffusion and Permeation Through Transport Resistances on the Crystal Surface... [Pg.181]

The measurement of transport numbers by the above electrochemical methods entails a significant amount of experimental effort to generate high-quality data. In addition, the methods do not appear applicable to many of the newer non-haloalu-minate ionic liquid systems. An interesting alternative to the above method utilizes the NMR-generated self-diffusion coefficient data discussed above. If both the cation (Dr+) and anion (Dx ) self-diffusion coefficients are measured, then both the cation (tR+) and anion (tx ) transport numbers can be determined by using the following Equations (3.6-6) and (3.6-7) [41, 44] ... [Pg.121]

The Van Deemter equation (Chapter 2) shows how diffusion and transfer processes affected HETP. Applications of GC to the measurement of transport properties of gases have shown to be... [Pg.583]

In this expression, 3 represents the increase factor of vertical diffusion due to the plume. Gaussian plume or dispersion models are based on standard deviations of the plume dimensions (crx, cry, oz). These represent a measure of the diffusive capacity of the atmosphere. They are dependent on the turbulence conditions of the atmosphere, the vertical temperature gradient (which helps to establish atmospheric turbulence in the vertical direction) and the transporting distance. [Pg.156]

Transport phenomena and other dynamic processes in lyotropic liquid crystals have received relatively little research attention. However, they can be quite important in practice because relatively long times are often required to reach equilibrium when a liquid crystal is present. Moreover, understanding of equilibrium behavior seems to have reached a point where additional work on dynamic phenomena would be productive. Accordingly, the available information on such phenomena is reviewed. It consists mainly of measurements of viscosity, diffusivity, electrical conductivity, and chemical reaction rates in liquid crystalline materials. Some possible areas for future research are identified and discussed briefly. [Pg.92]

The methods described so far for studying self-diffusion are essentially based on an observation of the diffusion paths, i.e. on the application of Einstein s relation (eq 3). Alternatively, molecular self-diffusion may also be studied on the basis of the Fick s laws by using iso-topically labeled molecules. As in the case of transport diffusion, the diffusivities are determined by comparing the measured curves of tracer exchange between the porous medium and the surroundings with the corresponding theoretical expressions. As a basic assumption of the isotopic tracer technique for studying self-diffusion, the isotopic forms are expected to have... [Pg.375]

Whereas mutual diffusion characterizes a system with a single diffusion coefficient, self-diffusion gives different diffusion coefficients for all the particles in the system. Self-diffusion thereby provides a more detailed description of the single chemical species. This is the molecular point of view [7], which makes the selfdiffusion more significant than that of the mutual diffusion. In contrast, in practice, mutual diffusion, which involves the transport of matter in many physical and chemical processes, is far more important than self-diffusion. Moreover mutual diffusion is cooperative by nature, and its theoretical description is complicated by nonequilibrium statistical mechanics. Not surprisingly, the theoretical basis of mutual diffusion is more complex than that of self-diffusion [8]. In addition, by definition, the measurements of mutual diffusion require mixtures of liquids, while self-diffusion measurements are determinable in pure liquids. [Pg.58]

An investigator in this area typically has precise information on composition of casting solutions and other physicochemical factors affecting membrane formation. Functional measurements of transport in terms of convective permeability, selectivity or diffusive permeability are usually also available. However, without proper techniques for quantitative description of membrane pore structures, and their shape and size distributions, membrane development efforts remain largely empirical. [Pg.339]

Membrane Diffusion in Dilute Solution Environments. The measurement of ionic diffusion coefficients provides useful information about the nature of transport processes in polymer membranes. Using a radioactive tracer, diffusion of an ionic species can be measured while the membrane is in equilibrium with the external solution. This enables the determination of a selfdiffusion coefficient for a polymer phase of uniform composition with no gradients in ion or water sorption. In addition, selfdiffusion coefficients are more straightforward in their interpretation compared to those of electrolyte flux experiments, where cation and anion transport rates are coupled. [Pg.45]

Fig. 1. Microcirculation of a human colon carcinoma grown in the dorsal skin chamber in a severe-combined immunodeficient mouse. (Adapted from Leunig et al., 1992b.) Note that angiogenesis leads to formation of numerous blood vessels. Such a transparent preparation can permit noninvasive, continuous measurement of transport processes in normal and tumor tissues (Jain, 1985b). Parameters we can measure include hemodynamic (e.g., blood flow, vasomotion) metabolic (e.g., pH, p02, Ca2+) transport (e.g., permeability, diffusion, binding), and cell-cell interactions (e.g., adhesion, deformability). Fig. 1. Microcirculation of a human colon carcinoma grown in the dorsal skin chamber in a severe-combined immunodeficient mouse. (Adapted from Leunig et al., 1992b.) Note that angiogenesis leads to formation of numerous blood vessels. Such a transparent preparation can permit noninvasive, continuous measurement of transport processes in normal and tumor tissues (Jain, 1985b). Parameters we can measure include hemodynamic (e.g., blood flow, vasomotion) metabolic (e.g., pH, p02, Ca2+) transport (e.g., permeability, diffusion, binding), and cell-cell interactions (e.g., adhesion, deformability).
In real situations, where the concentration of solute is finite, the mutual diffusion coefficient is often the relevant measure of transport rate. Mutual diffusion coefficients provide a quantitative measure of the rate of molecular diffusion when gradients are present i.e., when solute and solvent molecules are both diffusing in an attempt to eliminate differences in chemical potential. The mutual diffusion coefficient is defined by Fick s law (recall Equation 3-19) ... [Pg.63]

Since the transport in chromia is by electron transfer, chromia does not exhibit the Hall effect, photoconductivity, or carrier injection. Inconsistent results have been obtained from direct measurements of the diffusion of chromic ions in chromia 191,192). The dielectric constant was measured by Fang and Brower 193). The energy distribution curve of the photoelectrons emitted by chromia shows a spread of many electron volts 194), as is typical of insulators. The adsorption of gases such as ethanol shifts the limit of the photoeffect to longer wavelengths 195). Photoconductivity was not detected in chromia 196). Chemisorption of oxygen on chromia was not influenced by a previous nuclear irradiation in vacuo 189). [Pg.297]

Fig. 48 Comparison of simulated and experimental profiles for pressure steps 0 to 5 mbar (a), 5 to 0 mbar (b), 0 to 10 mbar (c), 10 to 0 mbar (d), 0 to 40 mbar (e), 40 to 0 mbar (f), 0 to 80 mbar (g), and 80 to 0 mbar (h). Tbe points refer to experimental measurements. Tbe lines are simulated from tbe 2-D finite difference solution with the same concentration dependence of transport diffusivities as determined from Fig. 47 (full line) and the surface permeabilities determined from the use of Eqs. 7 and 8. For the simulations it is implied that Dz > Dy... Fig. 48 Comparison of simulated and experimental profiles for pressure steps 0 to 5 mbar (a), 5 to 0 mbar (b), 0 to 10 mbar (c), 10 to 0 mbar (d), 0 to 40 mbar (e), 40 to 0 mbar (f), 0 to 80 mbar (g), and 80 to 0 mbar (h). Tbe points refer to experimental measurements. Tbe lines are simulated from tbe 2-D finite difference solution with the same concentration dependence of transport diffusivities as determined from Fig. 47 (full line) and the surface permeabilities determined from the use of Eqs. 7 and 8. For the simulations it is implied that Dz > Dy...
Fundamentals of sorption and sorption kinetics by zeohtes are described and analyzed in the first Chapter which was written by D. M. Ruthven. It includes the treatment of the sorption equilibrium in microporous sohds as described by basic laws as well as the discussion of appropriate models such as the Ideal Langmuir Model for mono- and multi-component systems, the Dual-Site Langmuir Model, the Unilan and Toth Model, and the Simphfied Statistical Model. Similarly, the Gibbs Adsorption Isotherm, the Dubinin-Polanyi Theory, and the Ideal Adsorbed Solution Theory are discussed. With respect to sorption kinetics, the cases of self-diffusion and transport diffusion are discriminated, their relationship is analyzed and, in this context, the Maxwell-Stefan Model discussed. Finally, basic aspects of measurements of micropore diffusion both under equilibrium and non-equilibrium conditions are elucidated. The important role of micropore diffusion in separation and catalytic processes is illustrated. [Pg.411]


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