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Transfer across the interface

Solute gas is diffusing into a stationary liquid, virtually free of solvent, and of sufficient depth lot it to be regarded as semi-infinite in extent, in what depth of fluid below die surface will 90% of die material which has been transferred across the interface have accumulated in the first minute )... [Pg.856]

Since a metal is immersed in a solution of an inactive electrolyte and no charge transfer across the interface is possible, the only phenomena occurring are the reorientation of solvent molecules at the metal surface and the redistribution of surface metal electrons.6,7 The potential drop thus consists only of dipolar contributions, so that Eq. (5) applies. Therefore the potential of zero charge is directly established at such an interface.3,8-10 Experimentally, difficulties may arise because of impurities and local microreactions,9 but this is irrelevant from the ideal point of view. [Pg.3]

Henry s law constant. The overall driving force for mass transfer is Ug—K ay and the rate of mass transfer across the interface is... [Pg.384]

These component balances are conceptually identical to a component balance written for a homogeneous system. Equation (1.6), but there is now a source term due to mass transfer across the interface. There are two equations (ODEs) and two primary unknowns, Og and a . The concentrations at the interface, a and a, are also unknown but can be found using the equilibrium relationship, Equation (11.4), and the equality of transfer rates. Equation (11.5). For membrane reactors. Equation (11.9) replaces Equation (11.4). Solution is possible whether or not Kjj is constant, but the case where it is constant allows a and a to be eliminated directly... [Pg.387]

The use of interpenetrating donor-acceptor heterojunctions, such as PPVs/C60 composites, polymer/CdS composites, and interpenetrating polymer networks, substantially improves photoconductivity, and thus the quantum efficiency, of polymer-based photo-voltaics. In these devices, an exciton is photogenerated in the active material, diffuses toward the donor-acceptor interface, and dissociates via charge transfer across the interface. The internal electric field set up by the difference between the electrode energy levels, along with the donor-acceptor morphology, controls the quantum efficiency of the PV cell (Fig. 51). [Pg.202]

Similar results have recently been reported by Aspnes and Heller. They proposed an autocatalytic model for photoactive systems involving metal/compound semiconductor interfaces. To explain induction times in CdS systems (.9), they suggest that hydrogen incorporated in the solid lowers the barrier to charge transfer across the interface and thereby accelerates H2 production rates. [Pg.570]

Insulators lack free charges (mobile electrons or ions). At interfaces with electrolyte solutions, steady-state electrochemical reactions involving charge transfer across the interface cannot occur. It would seem, for this reason, that there is no basis at this interface for the development of interfacial potentials. [Pg.598]

The situation that no charge transfer across the interface occurs is named the ideal polarized or blocked interface. Such interfaces do not permit, due to thermodynamic or kinetic reasons, either electron or ion transfer. They possess Galvani potentials fixed by the electrolyte and charge. Of course, the ideal polarizable interface is practically a limiting case of the interfaces with charge transfer, because any interface is always permeable to ions to some extent. Therefore, only an approximation of the ideal polarizable interface can be realized experimentally (Section III.D). [Pg.20]

Equation (41) is valid if none of the ionic components are transferable across the interface, and the only common charged components are electrons. [Pg.29]

DCE interface in the presence of TPBCl [43,82]. The accumulation of products of the redox reactions were followed by spectrophotometry in situ, and quantitative relationships were obtained between the accumulation of products and the charge transfer across the interface. These results confirmed the higher stability of this anion in comparison to TPB . It was also reported that the redox potential of TPBCP is 0.51V more positive than (see Fig. 3). However, the redox stability of the chlorinated derivative of tetra-phenylborate is not sufficient in the presence of highly reactive species such as photoex-cited water-soluble porphyrins. Fermin et al. have shown that TPBCP can be oxidized by adsorbed zinc tetrakis-(carboxyphenyl)porphyrin at the water-DCE interface under illumination [50]. Under these conditions, the fully fluorinated derivative TPFB has proved to be extremely stable and consequently ideal for photoinduced ET studies [49,83]. Another anion which exhibits high redox stability is PFg- however, its solubility in the water phase restricts the positive end of the ideally polarizable window to < —0.2V [85]. [Pg.200]

Similarly to experiments under potentiostatic conditions, success in the analysis of ET kinetics relies on the fact that neither products nor reactants can transfer across the interface. Various redox couples in the aqueous phase have been studied, including Fe(CN) /, Ru(CN) / Mo(CN) /, FeEDTA / IrClg and Co(III)/(II)... [Pg.202]

Solvent extraction is intrinsically dependent on the mass transfer across the interface and the chemical inversion at the interfacial region. Researchers in the field of solvent extraction, especially in the field of analytical chemistry and hydrometallurgy, observed effects of interfacial phenomena in the solvent extraction systems. This gave them a strong motivation to measure what happened at the interface. [Pg.361]

Note that Eqs. (4) and (5) implicitly consider the transfer across the interface as the rate-determining step in the ion transfer processes [51], and neglect other steps involved in the process such as the ion transport across the diffusion boundary layers [55] and across the diffuse electrical double layer [50]. [Pg.546]

As shown in Fig. 10, Eq. (28) does not depend upon pH, and the predominance domain of the two ionic species in both phases [denoted MO (w) and MO (o)] are thus separated by a horizontal line, indicating that a simple ion transfer reaction occurs upon a change of Ag(p (MO transfers across the interface). The position of this boundary line indicates the energy required for this transfer and hence directly reflects the lipophilicity of the ion. [Pg.748]

The problem of ion transfer across the interface has been treated in detail by Sato,26,27 Scully,28 and also Valand and Heus-ler,29 following the general theory of Vetter.30 Valand and Heusler assumed the same type of activation-controlled charge transfer kinetics, except that the dominant charge here is that on the O2-ions (or OH- ions) obtained by splitting water at the interface. The electrochemical double layer here is of the usual type for aqueous systems and the equilibrium p.d. is determined by the main charge transfer reaction... [Pg.412]

As a consequence it is difficult to separate ion transport to the interface from ion transfer across the interface. [Pg.163]

Adsorption of acetic acid on Pt(lll) surface was studied the surface concentration data were correlated with voltammetric profiles of the Pt(lll) electrode in perchloric acid electrolyte containing 0.5 mM of CHoCOOH. It is concluded that acetic acid adsorption is associative and occurs without a significant charge transfer across the interface. Instead, the recorded currents are due to adsorption/desorption processes of hydrogen, processes which are much better resolved on Pt(lll) than on polycrystalline platinum. A classification of adsorption processes on catalytic electrodes and atmospheric methods of preparation of single crystal electrodes are discussed. [Pg.245]

Thus, the electrochemical potential difference between an electron in the solution and in the electrode is related to the absolute electrode potential. If the solution composition is assumed to be constant with potential, the chemical potential and dipole potential of the solution are constant. Thus, the ability of an electron to transfer across the interface for a given solution composition is controlled exclusively by the electrode potential. [Pg.310]

Electroanalyte movement through solution. If electron conduction through the electrode and electron transfer across the interface are both fast, then the rate that limits the overall rate of charge flow will be that at which the electroactive material moves from the solution to approach close enough to the electrode for electron transfer to occur. [Pg.19]

The significance of Rosen s work lies in the attempt of quantifying the efficiency of stress transfer across the interface with respect to the fiber length, by introducing the concept of ineffective length . The ineffective fiber length, (2L), was defined by specifying some fraction, (f>, of the undisturbed stress value below which the fiber shall be considered ineffective. (2i) normalized with fiber diameter, 2a, is derived as... [Pg.100]

FIGURE 5.16 Schematic of resistance model for diffusion, uptake, and reaction of gases with liquids. Tg represents the transport of gases to the surface of the particle, a the mass accommodation coefficient for transfer across the interface, rso, the solubilization and diffusion in the liquid phase, riM the bulk liquid-phase reaction, and rinlcrl.ll c the reaction of the gas at the interface. [Pg.160]

As intuitively expected, the rate of transfer across the interface depends on the difference in the liquid-phase concentrations at the interface and in the bulk and on the diffusion coefficient in the liquid. In addition, it depends inversely on the time of exposure of the liquid to the gas because of the increasing importance of reevaporation back to the gas phase at longer times. When cl bulk = 0, Eq. (EEE) becomes... [Pg.161]


See other pages where Transfer across the interface is mentioned: [Pg.591]    [Pg.4]    [Pg.385]    [Pg.815]    [Pg.91]    [Pg.221]    [Pg.634]    [Pg.156]    [Pg.412]    [Pg.443]    [Pg.156]    [Pg.250]    [Pg.310]    [Pg.81]    [Pg.97]    [Pg.202]    [Pg.279]    [Pg.280]    [Pg.3]    [Pg.50]    [Pg.93]    [Pg.114]    [Pg.137]    [Pg.20]    [Pg.30]    [Pg.205]    [Pg.331]    [Pg.708]   
See also in sourсe #XX -- [ Pg.324 ]

See also in sourсe #XX -- [ Pg.461 ]




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The Interface

Transfer across interface

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