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Faradaic charge transfer

In the case of a simple system considered throughout Sect. 2, it is already clear that both the faradaic charge transfer and the non-faradaic double-layer charging will contribute to the impedance of the electrode-solution interface. In addition to this, we have to account for the ohmic resistances between the connections to indicator and counter electrodes. This was already illustrated in Sect. 1.1, Fig. 1. The first conclusion is therefore that the total impedance can be written as the summation... [Pg.243]

Both the double-layer charging and the faradaic charge transfer are non-linear processes, i.e. the charging current density, jc, and the faradaic... [Pg.252]

What makes a /wcwc/ocapacitance Obviously, it is the fact that it is intimately related to, and indeed dependent on, faradaic charge transfer across the interphase. The equivalent circuit that represents... [Pg.469]

An additional unique feature of electrosorption is that the coverage is a function of potential, at constant concentration in solution. Thus, we can discuss two types of isotherms those yielding 0 as a function of C and those describing the dependence of 0 on E. This is not a result of faradaic charge transfer. Neither is it due to electrostatic interactions of the adsorbed species with the field inside Ihc compact part of the double layer, since a potential dependence is observed even for neutral organic species having no permanent dipole moment. As we shall see, it turns out that the potential dependence of 0 is due to the dependence of the free energy of adsorption of water molecules on potential. [Pg.477]

Figure 16. Equivalent circuit (a) and a simulated Nyquist plot (b) for the charge transfer pathway illustrated in Figure 15. The capacitance C represents that of the space-charge layer and the parallel branch components represent the Faradaic charge transfer process. Refer to the original work for further details. (Reproduced with permission from Ref. [84).)... Figure 16. Equivalent circuit (a) and a simulated Nyquist plot (b) for the charge transfer pathway illustrated in Figure 15. The capacitance C represents that of the space-charge layer and the parallel branch components represent the Faradaic charge transfer process. Refer to the original work for further details. (Reproduced with permission from Ref. [84).)...
A metal surface exposed to light generally will eject electrons that travel 20 to 100 A into the electrolyte and then become solvated. These electrons are reactive and produce some interesting chemistry if scavengers are available to interact with them. In the absence of such species, the electrons return to the electrode by diffusion, and no net loss of charge is detected. If a scavenger exists, for example N2O in water, some react and fail to return, and therefore the faradaic charge transfer can be detected ... [Pg.760]

Pseudocapacitors store charge based on reversible (faradaic) charge transfer reactions with ions in the electrolyte. For example, in a metal oxide (such as RUO2 or I1O2) electrode, charge storage results from a sequence of redox reactions. Electrochemical capacitors (ECs) based on such pseudocapacitive materials will have both faradaic and nonfaradaic contributions. The optimization of both EDLCs and pseudocapacitors depends on understanding how features at the nanoscale (e.g. pore size distribution, crystaUite or particle size) affect ion and electron transport and the fundamental properties of electrochemical interfaces. [Pg.521]

The models clearly have not assigned any atomic structure to the metal side. With a metallic substrate Rice, in 1928,- showed the electric field penetration was indeed slight. Consequently, this model was adequate for the ideal polarizable electrode without Faradaic charge transfer. [Pg.21]

Fig.3 is a schematic of the procedure. As mentioned earlier, the faradaic charge transfer cannot be viewed as a linear component in the circuit. However, provided the amplitude is small enough, no more than a few millivolts, one can use Eq.l as a reasonable approximation. ... [Pg.23]

As shown in Figure 1.7, the pseudocapacitance can also arise from the intercalation of electrolyte ions (e.g., LF) into the tunnels, van der Waals gaps, or lattice of redox-active electrode materials (e.g., M0O3) accompanied by a faradaic charge transfer [11,77-79]. It is worth noting that only when such intercalation process is fast enough, the electrode exhibits pseudocapacitive behavior. Otherwise, it will behave like a battery-type electrode. [Pg.18]

Improved charge transfer capacity is commonly estimated by using a reversible charge injection process through either double layer capacitive reactions and reversible faradaic charge transfer reactions at the electrode/electrolyte interface as... [Pg.7]

Since such surface redox reactions usually involve Faradaic charge transfer, the specific pseudocapacitances that can be manifested are some five to ten times larger than the specific double-layer capacitance (always present and significant at aU electrode interfaces) at the same electrode. Hence such pseudocapacitor systems are of importance for practical development as has been the case with RUO2, but mainly for military applications owing to the high cost of that material. [Pg.489]

The frequency dependence of a simple response of an electrochemical cell consists of three contributions (i) double-layer charging with a linear dependence on co (via the term coC) (ii) the frequency independent faradaic charge transfer (Ret) (hi) the diffusional contribution with dependence and, finally, (iv) the solution resistance acting in series with all contributions listed (i-iii). [Pg.16]

The ionic actuators with carbonaceous electrodes are considered, as a rule, as being non-Faradaic, i.e., the electromechanical effects are governed by the electrochemical double-layer buildup at the electrode-electrolyte boundary (Kosidlo et al. 2013). The absence of Faradaic charge-transfer reactions, which can deteriorate the actuator s performance in the long run, can be assured by not exceeding the electrochemical stability window (ESW) of the electrolyte. [Pg.479]

Above this critical frequency a high-frequency impedance region exists (co>cO jj.) where the impedance is determined by the double-layer capacitance as well as the bulk-solution impedance, resistance of the wires, film thickness of bulk polymer, etc. In the second, medium-frequency (co > co > co ) region, the impedance characteristic depends on Faradaic charge transfer and infinite... [Pg.90]

When Faradaic charge transfer is absent and the interfacial impedance is represented only by a low-frequency (differential) capacitance C j, the impedance in pores becomes ... [Pg.154]

A more complicated expression for pore impedance develops when Faradaic charge transfer is present [68], such as that for the impedance of an electrode consisting of cylindrical pores in the absence of DC current (that is, in the absence of diffusion) and represented by a parallel combination of charge-... [Pg.154]

The variation of the impedance with frequency has been examined for various geometries of a single pore, and the results are summarized in Figure 7-21 for cases with no Faradaic charge transfer, where all interfacial impedance is determined by the double-layer capacitance (Eq. 7-68) [69]. It can be shown that the more occluded the shape of a pore, the more the impedance exhibits a pseudo-transfer resistance. The RC transmission line model was also successfully applied to the impedance analysis of more complicated electrodes representing fractal structures composed of variable sizes of double and triple pores [70]. [Pg.157]


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See also in sourсe #XX -- [ Pg.302 ]




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