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Diffusion mechanism exchange

There is a qualitative distinction between these two types of mass transfer. In the case of vapour phase transport, matter is subtracted from the exposed faces of the particles via dre gas phase at a rate determined by the vapour pressure of the solid, and deposited in the necks. In solid state sintering atoms are removed from the surface and the interior of the particles via the various diffusion vacancy-exchange mechanisms, and the centre-to-cenU e distance of two particles undergoing sintering decreases with time. [Pg.204]

The exchange process in a chelating resin is generally slower than in the ordinary type of exchanger, the rate apparently being controlled by a particle diffusion mechanism. [Pg.202]

Further evidence for the OHb pairs is given in an STM movie recorded at approximately 187 K. The movie shows the OHb pairs separating across the Ob rows via proton exchange with water molecules [19]. Key frames from the movie are shown in Figure 8.5. This water-assisted OHb diffusion mechanism is supported by calculations, which show that the barrier to diffusion is lowered by the exchange with water. The same diffusion mechanism is also observed for isolated OHb and because of the misassignment of OHb and Ob-vacs by Schaub et al. [15], this water-mediated diffusion of OHb was incorrectly reported as oxygen-mediated diffusion of Ob-vacs [32, 33] via a mechanism inconsistent with subsequent isotope studies [34],... [Pg.224]

Figure 5.11 Diffusion mechanisms (a) exchange (e) and ring (r) diffusion (b) kick-out diffusion, leading to (c) a substitutional defect and a self-interstitial. Figure 5.11 Diffusion mechanisms (a) exchange (e) and ring (r) diffusion (b) kick-out diffusion, leading to (c) a substitutional defect and a self-interstitial.
Figure 4.40 Illustration of diffusion mechanisms in alloys and ionic solids (a) interchange (exchange) (b) ring rotation (rare) (c) interstitial migration and (d) vacancy migration. From W. D. Kingery, H. K. Bowen, and D. R. Uhlmann, Introduction to Ceramics. Copyright 1976 by John Wiley Sons, Inc. This material is used by permission of John Wiley Sons, Inc. Figure 4.40 Illustration of diffusion mechanisms in alloys and ionic solids (a) interchange (exchange) (b) ring rotation (rare) (c) interstitial migration and (d) vacancy migration. From W. D. Kingery, H. K. Bowen, and D. R. Uhlmann, Introduction to Ceramics. Copyright 1976 by John Wiley Sons, Inc. This material is used by permission of John Wiley Sons, Inc.
The systems considered here are isothermal and at mechanical equilibrium but open to exchanges of matter. Hydrodynamic motion such as convection are not considered. Inside the volume V of Fig. 8, N chemical species may react and diffuse. The exchanges of matter with the environment are controlled through the boundary conditions maintained on the surface S. It should be emphasized that the consideration of a bounded medium is essential. In an unbounded medium, chemical reactions and diffusion are not coupled in the same way and the convergence in time toward a well-defined and asymptotic state is generally not ensured. Conversely, some regimes that exist in an unbounded medium can only be transient in bounded systems. We approximate diffusion by Fick s law, although this simplification is not essential. As a result, the concentration of chemicals Xt (i = 1,2,..., r with r sN) will obey equations of the form... [Pg.7]

For exchange with a copper adatom the diffusion mechanism is illustrated in Fig. 3. In the measurements, embedded indium atoms are observed to make jumps of several atomic spacings. For the adatom mechanism, this would imply that the indium adatoms reinsert themselves into the terrace after making... [Pg.354]

Kawano et al. used a microelectrode technique and the Dahms-Ruff equation to explore the diffusion mechanism of the iodide/triiodide redox couple and explain the physical diffusion accompanying an exchange reaction [22]. They showed that when high concentrations of iodide and tiiiodide are added to a RTCL as the solvent, the diffusion coefficient derived from the exchange reaction, expressed by / + —> /f + / , become significant and superior to the simple physical dif-... [Pg.195]

Figure 3 Defects and associated diffusion mechanism 1 and 2, diffusion mechanism by direct exchange 3, diffusion through vacancy 4, direct interstitial mechanism 5, indirect interstitial or caterpillar mechanism 6, Frenkel defect 7, indirect exchange 8, Schottky defect. (Ref 9. Reproduced by permission of Cambridge University Press)... Figure 3 Defects and associated diffusion mechanism 1 and 2, diffusion mechanism by direct exchange 3, diffusion through vacancy 4, direct interstitial mechanism 5, indirect interstitial or caterpillar mechanism 6, Frenkel defect 7, indirect exchange 8, Schottky defect. (Ref 9. Reproduced by permission of Cambridge University Press)...
Figure 6.6 The effect of interruption upon the rate of exchange according to controlling diffusion mechanism (schematic)... Figure 6.6 The effect of interruption upon the rate of exchange according to controlling diffusion mechanism (schematic)...
The second mechanism is the one more relevant to the action of amphetamine and related agents. This mechanism is illustrated in Fig. 4.1. Amphetamine, and other small molecular weight compounds with similar structures, are substrates at the monoamine uptake carriers and are transported into the neuron. The uptake carrier has an extracellular and intracellular face, and after transporting a substrate (amphetamine, etc.) into the neuron, the intracellular carrier face can bind to dopamine and transport it back to the extracellular face. This exchange diffusion mechanism is calcium independent, and is capable of robustly increasing synaptic transmitter levels. This process is often described as a "reversal" of the normal uptake carrier process. [Pg.180]

For single file diffusion mechanism, with no possible counter-exchange between adsorbed species, these equations simplify to... [Pg.239]

Por single file diffusion mechanism, it is assumed that no coimter-exchange is possible between the adsorbed solutes i and j. For single file diffusion mechanism the Pick surface diffusivity matrix is given by ... [Pg.766]

Exchange Mechanisms for Surface Diffusion. Our discussion of transition state theory in chap. 7 showed that in those cases when we are lucky enough to know the details of the transition pathway associated with a given diffusion mechanism, atomic-level analysis can shed important light on the process of diffusion. On the other hand, as we have already emphasized, the successful application of the ideas of transition state theory ultimately requires a knowledge of the transition pathway. Field-ion microscopy in conjunction with first-principles analysis of the energetics of metal surfaces has led to a convincing picture of surface diffusion in some instances that is entirely contrary to the ideas built around intuition. [Pg.589]

Fig. 11.1. Competing surface diffusion mechanisms on an fee (001) surface (adapted from Feibel-man (1990)) (a) intuitive mechanism in which adatom moves from one fourfold site to another by passing across bridge site, and (b) exchange mechanism in which diffusion occurs by concerted motion both of adatom and its subsurface partner. Fig. 11.1. Competing surface diffusion mechanisms on an fee (001) surface (adapted from Feibel-man (1990)) (a) intuitive mechanism in which adatom moves from one fourfold site to another by passing across bridge site, and (b) exchange mechanism in which diffusion occurs by concerted motion both of adatom and its subsurface partner.

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See also in sourсe #XX -- [ Pg.219 ]




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