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Exchange current density steady state

Very few references are available relating to the study of the Al(III)/Al(s) reaction. Most of the earlier studies have been made in molten cryolite.56,57 Armalis and Levinskas58 have reported the overall exchange current density of the reaction under a steady state of deposition and showed that it is a moderately fast reaction. [Pg.202]

Figure 5. Measurement and analysis of steady-state i— V characteristics, (a) Following subtraction of ohmic losses (determined from impedance or current-interrupt measurements), the electrode overpotential rj is plotted vs ln(i). For systems governed by classic electrochemical kinetics, the slope at high overpotential yields anodic and cathodic transfer coefficients (Ua and aj while the intercept yields the exchange current density (i o). These parameters can be used in an empirical rate expression for the kinetics (Butler—Volmer equation) or related to more specific parameters associated with individual reaction steps.(b) Example of Mn(IV) reduction to Mn(III) at a Pt electrode in 7.5 M H2SO4 solution at 25 Below limiting current the system obeys Tafel kinetics with Ua 1/4. Data are from ref 363. (Reprinted with permission from ref 362. Copyright 2001 John Wiley Sons.)... Figure 5. Measurement and analysis of steady-state i— V characteristics, (a) Following subtraction of ohmic losses (determined from impedance or current-interrupt measurements), the electrode overpotential rj is plotted vs ln(i). For systems governed by classic electrochemical kinetics, the slope at high overpotential yields anodic and cathodic transfer coefficients (Ua and aj while the intercept yields the exchange current density (i o). These parameters can be used in an empirical rate expression for the kinetics (Butler—Volmer equation) or related to more specific parameters associated with individual reaction steps.(b) Example of Mn(IV) reduction to Mn(III) at a Pt electrode in 7.5 M H2SO4 solution at 25 Below limiting current the system obeys Tafel kinetics with Ua 1/4. Data are from ref 363. (Reprinted with permission from ref 362. Copyright 2001 John Wiley Sons.)...
Surfaces of cadmium with various morphological properties were electro-formed on the Cd electrode from sulfate solutions by varying current densities, temperature, and pulse electrolysis conditions [218]. The surface properties were defined by the values of slopes of quasi-steady state E versus logarithm current density dependencies and exchange current densities in 0.5 M CdS04 + 0.15 M H2SO4 solution. The dependence of the slope values on surface properties was explained in terms of the influence of crystallization overpotential. [Pg.782]

The link between the current density and the concentration overpotential under steady-state conditions for systems in which the exchange-current density is relatively large compared with the limiting current density (hence, the activation overpotential is negligible) was established through the concept of a limiting current iL arising from the fact that there is a maximum rate at which electron acceptors can move to an... [Pg.538]

Steady-state Current Overpotential Behaviour - For a simple single charge-transfer process equation (2.28) describes the closed-circuit behaviour. At low overpotentials, the current and overpotential are linearly related and the exchange current density can be evaluated from the gradient (see equation... [Pg.29]

The very fast metal-metal ion electrode processes, for which the exchange current density is very high. At steady state the overall rates of those electrode processes are controlled by the rates of mass transfer of the electroactive components to and from the electrode-melt interface. [Pg.501]

Rather slow electrode processes (especially in the case of gas electrodes) which have low exchange current densities. At steady state, the overall rates are generally determined by the rates of charge transfer and/or of secondary chemical reactions at the electrode-melt interface. [Pg.501]

Figure 68. The exchange current density as a function of oxygen partial pressure for different temperatures confirming the electrode kinetical model given in the text.256 (Reprinted from D. Y. Wang, A. S. Nowick, Cathodic and Anodic Polarization Phenomena at Platinum Electrodes with Doped CeC>2 as Electrolyte. I. Steady-State Overpotential. , J. Electrochem. Soc., 126, 1155-1165. Copyright 1979 with permission from The Electrochemical Society, Inc.)... Figure 68. The exchange current density as a function of oxygen partial pressure for different temperatures confirming the electrode kinetical model given in the text.256 (Reprinted from D. Y. Wang, A. S. Nowick, Cathodic and Anodic Polarization Phenomena at Platinum Electrodes with Doped CeC>2 as Electrolyte. I. Steady-State Overpotential. , J. Electrochem. Soc., 126, 1155-1165. Copyright 1979 with permission from The Electrochemical Society, Inc.)...
In Eqs. (42)-(44), i g is the steady-state current density at potential V, / the charge-transfer symmetry coefficient, io the exchange current density, I the integration constant for Eq. (41), and r (0) the initial overpotential at time t = 0. [Pg.35]

Steady-state polarization curves, such as that presented in Figure 5.4(a), provide a means of identifying such important electrochemical parameters as exchange current densities, Tafel slopes, and diffusion coefficients. The influence of exchange current density and Tafel slopes on the steady-state current density can be seen in equations (5.17) and (5.18), and the influence of mass transfer and diffusivities on the current density is described in Section 5.3.3. Steady-state measmements, however, cannot provide information on the RC time constants of the electrochemical process. Such properties must be identified by using transient measurements. [Pg.109]

A representative anodic polarization curve for iron in a buffered environment of pH = 7 is shown in Fig. 5.4. The solid curve is representative of experimental observations the dashed curve is an extrapolation of the Tafel region to the equilibrium half-cell potential of -620 mV (SHE) and aFg2- = 10 6. This extrapolation allows estimation of an exchange current density of 0.03 mA/m2. The essentially steady minimum current density of the passive state is ip = 1 mA/m2. [Pg.188]

Figure 18. Dependence of the exchange current density on step density on an Ag (100) face intersected by screw dislocations ( 5 x 10 disl. cm ). Before each series of impedance measurements for the evaluation of the exchange current density, the face was grown at the indicated overpotential IR corrected) until a steady state profile is obtained. Step densities Lg calculated from the overpotential of growth according to Eq. (38)/26.34,35)... Figure 18. Dependence of the exchange current density on step density on an Ag (100) face intersected by screw dislocations ( 5 x 10 disl. cm ). Before each series of impedance measurements for the evaluation of the exchange current density, the face was grown at the indicated overpotential IR corrected) until a steady state profile is obtained. Step densities Lg calculated from the overpotential of growth according to Eq. (38)/26.34,35)...
CV peak current in the backward process, Eq. (92) CV peak current in the forward process, Eq. (92) quasi-reversible LSV current, Eq. (88) reduction current, Eq. (6) ring current, Eq. (121) sampled current, Eq. (42) staircase current square-wave current, Eq. (64) steady state current transformed LSV current, Eq. (94) alternating current, Eq. (56) amplitude of the AC peak-to-peak distance in the 2nd derivative DCP current density, Eq. (2) exchange current density, Eq. (9) limiting current density, Eq. (119)... [Pg.151]

As discussed above, f is a static materials property. It is the product of the specific electrocatalytic activity of the catalyst surface times statistical factors that arise at all scales due to the random morphology and distribution of the catalyst in the composite CL, as considered in Equation 8.2. The reaction penetration depth is a steady state property, which is mainly determined by the nonlinear coupling between transport of oxygen and protons and exchange current density. Together, both parameters, f and, determine the overall effectiveness of catalyst utilization. [Pg.393]

The exchange current density f is a static materials property defined in the section Catalyst Activity. The reaction penetration depth 8cl is a steady-state property determined by the interplay of transport properties of the layer and local electro-catalytic activity, embodied in f. Together, both parameters f and Scl determine the overall effectiveness of catalyst utilization. For illustration purposes, a simple scenario of this interplay for the case of severely limited oxygen diffusion will be considered below. [Pg.175]

Fig. 7.69. In a multistep electron-exchange reaction, each step produces its individual current density. At a steady state, all these currents must be equal. Fig. 7.69. In a multistep electron-exchange reaction, each step produces its individual current density. At a steady state, all these currents must be equal.

See other pages where Exchange current density steady state is mentioned: [Pg.286]    [Pg.563]    [Pg.252]    [Pg.48]    [Pg.150]    [Pg.9]    [Pg.205]    [Pg.206]    [Pg.256]    [Pg.334]    [Pg.339]    [Pg.341]    [Pg.1950]    [Pg.473]    [Pg.492]    [Pg.115]    [Pg.94]    [Pg.129]    [Pg.72]    [Pg.174]    [Pg.29]    [Pg.84]    [Pg.143]    [Pg.161]    [Pg.246]    [Pg.574]    [Pg.200]    [Pg.458]    [Pg.197]    [Pg.221]   
See also in sourсe #XX -- [ Pg.25 , Pg.43 , Pg.85 ]




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