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Diffusion adsorption heat

Except for the fullerenes, carbon nanotubes, nanohoms, and schwarzites, porous carbons are usually disordered materials, and cannot at present be completely characterized experimentally. Methods such as X-ray and neutron scattering and high-resolution transmission electron microscopy (HRTEM) give partial structural information, but are not yet able to provide a complete description of the atomic structure. Nevertheless, atomistic models of carbons are needed in order to interpret experimental characterization data (adsorption isotherms, heats of adsorption, etc.). They are also a necessary ingredient of any theory or molecular simulation for the prediction of the behavior of adsorbed phases within carbons - including diffusion, adsorption, heat effects, phase transitions, and chemical reactivity. [Pg.103]

For the detailed study of reaction-transport interactions in the porous catalytic layer, the spatially 3D model computer-reconstructed washcoat section can be employed (Koci et al., 2006, 2007a). The structure of porous catalyst support is controlled in the course of washcoat preparation on two levels (i) the level of macropores, influenced by mixing of wet supporting material particles with different sizes followed by specific thermal treatment and (ii) the level of meso-/ micropores, determined by the internal nanostructure of the used materials (e.g. alumina, zeolites) and sizes of noble metal crystallites. Information about the porous structure (pore size distribution, typical sizes of particles, etc.) on the micro- and nanoscale levels can be obtained from scanning electron microscopy (SEM), transmission electron microscopy ( ), or other high-resolution imaging techniques in combination with mercury porosimetry and BET adsorption isotherm data. This information can be used in computer reconstruction of porous catalytic medium. In the reconstructed catalyst, transport (diffusion, permeation, heat conduction) and combined reaction-transport processes can be simulated on detailed level (Kosek et al., 2005). [Pg.121]

The IR bands due to species-1 formed in the single step adsorption at 180 K completely diminishes with increasing temperatures up to 270 K while the bands due to species-3 and -4 are much increased in intensity with this temperature increase. This indicates that a part of species-1 is readsorbed as these more stable species through surface diffusion upon heating,... [Pg.394]

With decreasing pore size the desorption energy from the wall to the gas phase within the pores (the maximum in the curves in Fig. 9.20) becomes smaller but remains positive. This implies that the molecules in the central part of the pore behave in a Knudsen-like marmer (i.e. no intermolecular collision) and can pass each other (region Cj, upper part of Fig. 9.20) but nevertheless are not free and follow curved trajectories (see Ref. [83] and Sections 9.4.3.1-2). In this region c we can speak of a surface flow enhanced micropore diffusion (SEMP). Because in surface diffusion the activation energy is a fraction of the adsorption heat (see... [Pg.379]

Many compounds and salts are sensitive to the presence of water vapour or moisture. When compounds interact with moisture, they retain the water by either bulk or surface adsorption, capillary condensation, chemical reaction and, in extreme cases, a solution (deliquescence). Deliquescence is where a solid dissolves and saturates a thin film of water on its surface. It has been shown that when moisture is absorbed to the extent that deliquescence takes place at a certain critical relative humidity, the liquid film surrounding the solid is saturated. This process is dictated by vapour diffusion and heat transport rates (Kontny et al. 1987). [Pg.48]

Force-field calculations could be simple energy minimization or advanced monte-carlo and molecular dynamics calculations. The major assumption here is the transferability of force-field parameters among the related materials. These calculations can provide wealth of information such as the relative ordering of adsorption sites on surface, diffusion mechanism of molecules particularly inside zeolites, energy barrier for difihision, diffusion coefficients, heats of adsorption and more importantly, the effect of temperature on all these properties. [Pg.130]

By applying an appropriate perturbation to a relevant parameter of a system under equilibrium, various frequency modulation methods have been used to obtain kinetic parameters of chemical reactions, adsorption-desorption constants on surfaces, effective diffusivities and heat transfer within porous solid materials, etc., in continuous flow or batch systems [1-24]. In principle, it is possible to use the FR technique to discriminate between all of the kinetic mechanisms and to estimate the kinetic parameters of the dynamic processes occurring concurrently in heterogeneous catalytic systems as long as a wide enough frequency range of the perturbation can be accessed experimentally and the theoretical descriptions which properly account for the coupling of all of the dynamic processes can be derived. [Pg.238]

More recently, continuous flow or open FR systems have been developed to measure the adsorption and diffusion properties of sorbate molecules in microporous materials [13-15]. hi these systems, either the concentration of the sorbate feed [13] or the pressure within the reactor [14,15] is oscillated and the resulting changes at the exit stream are measured by using mass spectrometry or a mass flow meter. For a flow FR system, the effect of adsorption heat is reduced as the flowing gases attenuates the temperature change. [Pg.241]

Table 10.2-2 Adsorption heat activation energy for micropore diffusion for some systems... Table 10.2-2 Adsorption heat activation energy for micropore diffusion for some systems...
Interfacial phenomraia involving heat and mass transfer are described and analyzed in Chapter 6. Much of the chapter again deals with stability, in this case the Marangoni instability produced by interfacial trasion gradients associated with temperature and eoneentration gradients along the interface. Time-dependent variation of interfadal tension resulting from diffusion, adsorption, and desorption of various species is also diseussed. [Pg.2]

Somers, S.A., et al.. Binary fluids in planar nanopores Adsorptive selectivity, heat capacity and self-diffusivity. Adsorption, 2(1), 33-40 (1996). [Pg.1001]

This indicates that the permeation flux is dependent on the difference between the adsorption heat and the diffusion activation energy. [Pg.79]

CHjOH). This means that a comparison of the catalysts in a fixed-bed reactor at different conversion levels or at different methanol flow rates and equal conversion may potentially mean different temperatures and is relatively tricky. That is a reason why most of the publications use a highly diluted methanol feed [29,92,93]. The dilution media acts as a heat vector in this case to smooth over the adiabatic temperature increase. However, the presence of dilution media greatly decreases methanol partial pressure. The latter masks mechanistic details and may change reaction pathways. Some important studies also highlight the role of diffusion, adsorption equilibrium, role of water, and the role of surface species, which could hardly be seen with diluted feed [24,28,60,119]. [Pg.244]

From experimental data. A force field can be fitted in such a way that experimental data like diffusion coefficients, heats of adsorption, or phase equilibria can be reproduced. This force field can then be used to compute other properties of other molecules. [Pg.3]

Work in the area of simultaneous heat and mass transfer has centered on the solution of equations such as 1—18 for cases where the stmcture and properties of a soHd phase must also be considered, as in drying (qv) or adsorption (qv), or where a chemical reaction takes place. Drying simulation (45—47) and drying of foods (48,49) have been particularly active subjects. In the adsorption area the separation of multicomponent fluid mixtures is influenced by comparative rates of diffusion and by interface temperatures (50,51). In the area of reactor studies there has been much interest in monolithic and honeycomb catalytic reactions (52,53) (see Exhaust control, industrial). Eor these kinds of appHcations psychrometric charts for systems other than air—water would be useful. The constmction of such has been considered (54). [Pg.106]

Surface Area Determination The surface-to-volume ratio is an important powder property since it governs the rate at which a powder interacts with its surroundings. Surface area may be determined from size-distribution data or measured directly by flow through a powder bed or the adsorption of gas molecules on the powder surface. Other methods such as gas diffusion, dye adsorption from solution, and heats of adsorption have also been used. It is emphasized that a powder does not have a unique surface, unless the surface is considered to be absolutely smooth, and the magnitude of the measured surface depends upon the level of scrutiny (e.g., the smaller the gas molecules used for gas adsorption measurement the larger the measured surface). [Pg.1827]


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See also in sourсe #XX -- [ Pg.142 ]




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