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Surface diffusion/reaction coupling

At higher current densities, the primary electron transfer rate is usually no longer limiting instead, limitations arise tluough the slow transport of reactants from the solution to the electrode surface or, conversely, the slow transport of the product away from the electrode (diffusion overpotential) or tluough the inability of chemical reactions coupled to the electron transfer step to keep pace (reaction overpotential). [Pg.603]

Very recently, considerable effort has been devoted to the simulation of the oscillatory behavior which has been observed experimentally in various surface reactions. So far, the most studied reaction is the catalytic oxidation of carbon monoxide, where it is well known that oscillations are coupled to reversible reconstructions of the surface via structure-sensitive sticking coefficients of the reactants. A careful evaluation of the simulation results is necessary in order to ensure that oscillations remain in the thermodynamic limit. The roles of surface diffusion of the reactants versus direct adsorption from the gas phase, at the onset of selforganization and synchronized behavior, is a topic which merits further investigation. [Pg.430]

The oxidation or reduction of a substrate suffering from sluggish electron transfer kinetics at the electrode surface is mediated by a redox system that can exchange electrons rapidly with the electrode and the substrate. The situation is clear when the half-wave potential of the mediator is equal to or more positive than that of the substrate (for oxidations, and vice versa for reductions). The mediated reaction path is favored over direct electrochemistry of the substrate at the electrode because, by the diffusion/reaction layer of the redox mediator, the electron transfer step takes place in a three-dimensional reaction zone rather than at the surface Mediation can also occur when the half-wave potential of the mediator is on the thermodynamically less favorable side, in cases where the redox equilibrium between mediator and substrate is disturbed by an irreversible follow-up reaction of the latter. The requirement of sufficiently fast electron transfer reactions of the mediator is usually fulfilled by such revemible redox couples PjQ in which bond and solvate... [Pg.61]

The previous models were developed for Brownian particles, i.e. particles that are smaller than about 1 pm. Since most times particles that are industrially codeposited are larger than this, Fransaer developed a model for the codeposition of non-Brownian particles [38, 50], This model is based on a trajectory analysis of particles, including convective mass transport, geometrical interception, and migration under specific forces, coupled to a surface immobilization reaction. The codeposition process was separated in two sub-processes the reduction of metal ions and the concurrent deposition of particles. The rate of metal deposition was obtained from the diffusion... [Pg.217]

The simulation of reacting flows in packed tubes by CFD is still in its earliest stages. So far, only isothermal surface reactions for simplified geometries and elementary reactions have been attempted. Heterogeneous catalysis with diffusion, reaction, and heat transfer in solid particles coupled to the flow, species, and temperature fields external to the particles remains a challenge for the future. [Pg.383]

Lionbashevski et al. (2007) proposed a quantitative model that accounts for the magnetic held effect on electrochemical reactions at planar electrode surfaces, with the uniform or nonuniform held being perpendicular to the surface. The model couples the thickness of the diffusion boundary layer, resulting from the electrochemical process, with the convective hydrodynamic flow of the solution at the electrode interface induced by the magnetic held as a result of the magnetic force action. The model can serve as a background for future development of the problem. [Pg.278]

When dealing with two-dimensional formation of patterns in lipidic-proteic membranes (fluid membranes), not only does the coupling between the chemical reaction in the membrane and the surface diffusion have to be considered (i.e., the Thiele modulus), but one must also consider the coupling with the onset of convection (Navier-Stokes equa-... [Pg.236]

The incorporation of guest molecules can be achieved during their growth or is executed at defect sites and holes via wet chemistry, by surface diffusion and gas-phase transport. Encapsulated fullerenes tend to form chains that are coupled by van der Waals forces. Upon annealing, the encapsulated fullerenes coalesce in the interior of the SWCNTs, resulting in pill-shaped, concentric, endohedral capsules a few nanometers in length [265], The progress of such reactions inside the tubes could be monitored in real time by use of HR-TEM [266],... [Pg.44]

Unfortunately, the redox potential of the Pt4 + /3+ couple is not known in literature. Although some stable Ptm compounds have been isolated and characterized (37), the oxidation state III is reached usually only in unstable intermediates of photoaquation reactions (38-40) and on titania surfaces as detected by time resolved diffuse reflectance spectroscopy (41). To estimate the potential of the reductive surface center one has to recall that the injection of an electron into the conduction band of titania (TH) occurs at pH = 7, as confirmed by photocurrent measurements. Therefore, the redox potential of the surface Pt4 + /3+ couple should be equal or more negative than —0.28 V, i.e., the flatband potential of 4.0% H2[PtClal/ TH at pH = 7. From these results a potential energy diagram can be constructed as summarized in Scheme 2 for 4.0% H2[PtCl6]/TH at pH = 7. It includes the experimentally obtained positions of valence and conduction band edges, estimated redox potentials of the excited state of the surface platinum complex and other relevant potentials taken from literature. An important remark which should be made here is concerned with the error of the estimated potentials. Usually they are measured in simplified systems - for instance in the absence of titania - while adsorption at the surface, presence of various redox couples and other parameters can influence their values. Therefore the presented data may be connected with a rather large error. [Pg.256]

During the time dt, the thickness of the ArBs layer increases by dyA3 at interface 3 as a result of diffusion of the A atoms from interface 2 to interface 3 and their subsequent partial chemical reaction (4.2) with the surface B atoms. In the ApBq-B reaction couple the ApBq phase acts as a source of diffusing A atoms. It must be clear, however, that the content of component A in this phase cannot be less than the lower limit of its homogeneity range. Hence, as reaction (4.2) proceeds, the ApBq compound becomes unstable and therefore should undergo a partial transformation into another compound of the A-B multiphase binary system. To reveal the essence of this transformation, let us consider one of the simplest cases, in... [Pg.181]

Coupling between surface diffusion and reaction. If this mode is dominating [such as with the CO oxidation on Pt(100)], chemical waves propagating across the surface will give rise to spatiotemporal pattern formation. [Pg.272]

The diffusion coefficients can be assessed studying the product formation rate in diffusion couples, or the diffusion rate from a gas phase or a liquid into a solid material (e.g., metal oxidation rates) [i-iii]. In this case, however, the results may be affected by microstructural and interfacial factors due to transport in pores, surface diffusion, limited contact area between solid phases, formation of multiple reaction products, etc. [Pg.154]

Theoretical studies of the properties of the individual components of nanocat-alytic systems (including metal nanoclusters, finite or extended supporting substrates, and molecular reactants and products), and of their assemblies (that is, a metal cluster anchored to the surface of a solid support material with molecular reactants adsorbed on either the cluster, the support surface, or both), employ an arsenal of diverse theoretical methodologies and techniques for a recent perspective article about computations in materials science and condensed matter studies [254], These theoretical tools include quantum mechanical electronic structure calculations coupled with structural optimizations (that is, determination of equilibrium, ground state nuclear configurations), searches for reaction pathways and microscopic reaction mechanisms, ab initio investigations of the dynamics of adsorption and reactive processes, statistical mechanical techniques (quantum, semiclassical, and classical) for determination of reaction rates, and evaluation of probabilities for reactive encounters between adsorbed reactants using kinetic equation for multiparticle adsorption, surface diffusion, and collisions between mobile adsorbed species, as well as explorations of spatiotemporal distributions of reactants and products. [Pg.71]


See other pages where Surface diffusion/reaction coupling is mentioned: [Pg.179]    [Pg.249]    [Pg.2926]    [Pg.46]    [Pg.149]    [Pg.19]    [Pg.551]    [Pg.236]    [Pg.123]    [Pg.65]    [Pg.14]    [Pg.237]    [Pg.220]    [Pg.370]    [Pg.215]    [Pg.250]    [Pg.257]    [Pg.31]    [Pg.311]    [Pg.462]    [Pg.488]    [Pg.658]    [Pg.21]    [Pg.159]    [Pg.269]    [Pg.111]    [Pg.112]    [Pg.230]    [Pg.437]    [Pg.583]    [Pg.148]    [Pg.324]    [Pg.611]   
See also in sourсe #XX -- [ Pg.27 , Pg.250 , Pg.272 ]




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Diffuse surface

Diffusion couple

Diffusion coupled

Diffusion reactions

Diffusive coupling

Diffusivity reactions

Reaction-diffusion coupling

Surface diffusion

Surface diffusion Diffusivity

Surface diffusivity

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