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Amplitude method

These electron transfer reactions are very fast, among the fastest known. This is the reason that impedance methods were used originally to determine the standard rate constant,13,61 at a time when the instrumentation available for these methods was allowing shorter measurement times (high frequencies) to be reached than large-amplitude methods such as cyclic voltammetry. The latter techniques have later been improved so as to reach the same range of fast electron transfer kinetics.22,63... [Pg.77]

Application to large amplitude methods analysis in the Laplace domain... [Pg.265]

Application to small amplitude methods the operational impedance the Fast Fourier Transform... [Pg.267]

As in large-amplitude methods, one can control the potential and observe the current changes, or control the current and observe the change in potential. Irrespective of whether current or potential is controlled, the small-amplitude limitation applies to the potential excursion. [Pg.145]

The vast majority of small-amplitude methods are based on small-amplitude potential excitations with potential control of the surface concentrations. In earlier chapters, the relationship between surface concentration and electrode potential was explored and the concept of concentration profiles was presented. Whenever there is a flux of electrons at the electrode surface, the concentration profiles of at least two species will exhibit nonzero slopes at the electrode surface, as the electrochemical conversion of one member of a couple into another takes place and mass transport processes act to reestablish a uniform concentration distribution. These processes occur irrespective of whether the current flux arises from a potential or current excitation of the cell. In either case, they result in a perturbation from the previously existing concentration profile. The initial surface concentrations (which existed prior to the application of the new perturbation) are often termed the dc surface concentrations. It is useful to note that at any time, the distance integral of the concentration excess or defect is directly proportional to the charge passed due to that per-... [Pg.147]

The faradaic impedance method is the grandparent of all other small-amplitude methods. The first known experiments were reported by Warburg in 1899 [2]. [Pg.148]

Active electrochemical techniques are not confined to pulse and linear sweep waveforms, which are considered large amplitude methods. A-C voltammetry, considered a small amplitude method because an alternating voltage <10 mV is applied to actively couple through the double-layer capacitance, can also be used (15). An excellent source of additional information concerning active electroanalytical techniques can be found in References 16—18. Reference 18, although directed toward clinical chemistry and medicine, also contains an excellent review of electroanalytical techniques (see also... [Pg.55]

The artificial intelligence-superexchange method in which the details of the electronic structure of the protein medium are taken into account was used for estimating the electronic coupling in the metalloproteins (Siddarth and Marcus, 1993a,b,c). Fig.2.11 demonstrates a correlation of experimental and calculated ET rate constants for cytochrome c derivatives, modified by Ru complexes. The influence of the special mutual orientation of the donor and acceptor orbitals in Ru(bpy)2im HisX-cytochrome c on the rate of electron transfer was analyzed by the transition amplitude methods (Stuchebrukhov and Marcus, 1995). In this reaction the transferring electron in the initial and the final states occupies the 3d shell of the Fe atom and the 4d shell of Ru, respectively. It was shown that the electron is localized on t2g subshells of the metal ions. Due to the near-... [Pg.54]

The direct method (DM) for solution of this set of equations was proposed by Atherton et al. [5], and in a somewhat a modified form by Dickinson and Gelinas [4] who solved r sets of equations each of size In consisting of Eq. (1) coupled with a particular j—value of Eq. (2). Shuler and coworkers [5] took an alternative approach in the Fourier Amplitude method in which a characteristic periodic variation is ascribed to each a, and the resulting solution of (1) is Fourier analyzed for the component frequencies. These authors estimate that 1.2r2 5 solutions of Eq. (1) together with the appropriate Fourier analyses are required for the complete determination of the problem. Since even a modest reaction mechanism (e.g. in atmospheric chemistry or hydrocarbon cracking or oxidation) may easily involve 100 reactions with several tens of species, it is seen that a formidable amount of computation can result. [Pg.84]

In a similar fashion, spectral sensitivity can be defined using (7) by detecting spectral shift in the bandgap center (wavelength of the fiber lowest loss) resulting in a spectral sensitivity Sx 5,300 nm/RIU. Assuming that 0.1 nm spectral shift in the position of a bandgap center can be detected reliably, this results in the sensor resolution of Re(A a)miji 2 x 10 RIU, which is comparable to the resolution achieved by the amplitude method. [Pg.54]

To measure the particle size and -potential of pigment TiC>2 by the ESA (Electrokinetic Sonic Amplitude) method, the Acoustosizer 2 device ( Colloidal Dynamics , Sydney) was used. [Pg.387]

The following techniques have been introduced to reduce particle sizing errors when using signal amplitude methods ... [Pg.258]

The particle size-dependent radius of the measurement volume r(Di) may be determined in-situ by using the burst length method (Saffman 1987 b)) or the so-called logarithmic mean amplitude method (Qiu and Sommerfeld 1992). The latter is more reliable for noisy signals, i.e. low signal to noise ratio as demonstrated by Qiu and Sommerfeld (1992). [Pg.289]

There are alternative approaches that could avoid this problem. One attractive method was recently proposed by Balint-Kurti and co-workers in which the photofragmentation amplitude is obtained by integrating over time the amplitude of the wave function at a large asymptotic distance (54). We recently presented a TD flux approach (35) which calculates the flux of the wavefunction instead of evaluating the overlap integral. The main advantage of the flux method or the amplitude method of Balint-Kurti et al. is that one does not need to project out the bound state components because they do not contribute to the flux or amplitude outside the interaction potential. In the following we present this TD method based on the flux formula. The discussion essentially follows that of Ref. 35. [Pg.247]

Further, let us also underline that a tedious procedure of the phase convention in calculating the matrix elements of different operators is avoided in the energy approach, although certainly the final formulae must coincide with the formulae obtained using the traditional amplitude method. Therefore, the energy approach simplifies an analysis of complex atomic processes including processes with the interference of different kinds of channels (i.e., radiation and autoionization decay channels, etc.). [Pg.240]

Photoelectrodes, consisting of CdS nanocrystals that are directly attached to an electrode (gold or conducting oxide) or indirectly via a dithiol molecular linker have been studied extensively [19, 20, 116-120]. Here, we will focus on work that demonstrates the power of small-amplitude methods in photoelectrochemical characterization [26, 123, 124]. By measuring the photoelectrochemical activity of gold/Q-CdS electrodes, as the potential of the gold electrode was varied, it could be concluded that photoinduced electron transfer between the gold surface... [Pg.85]

In the amplitude method, the motion of the ions over many oscillation periods (typically 10 periods) is integrated such that it is the modulation frequency-dependent amplitude that is observed. The most precise determinations of the normal mode frequencies are found through fitting the relevant expression for z (co) (that is Equation 10.14 for identical ions and Equation 10.16 for non-identical ions) to the measured amplitudes of the laser-cooled ion as a function of the drive frequency, as shown in... [Pg.304]

In the estimates of Am above, it has been assumed tacitly that the damping coefficient Yi is much larger than is the inverse exposure time that, indeed, is the case in these experiments. When this assumption is not fulfilled, the width of a resonance has an additional contribution from the inverse integration time. In the extreme case of Yi [Pg.320]

FIGURE 10.15 Running average and statistical uncertainties of the COM mode frequency for two °Ca ions obtained (a) with the amplitude method and (b) with the phase method. For the amplitude method, the CCD exposure time was 100 ms and S/N ca 17, while for the phase method the exposure time was 500 ms and SJN ca 6. Yi is 2it x 113 Hz in both cases, yielding Aco ca 2jt x 27 Hz for the amplitude method and A(0 is ca 2n x 19 Hz for the phase method. These values are in reasonable agreement with the statistical uncertainty of about 2jt x 7 Hz for both methods. The total measurement times for the amplitude measurements and the phase measurements were 13 minutes and 23 minutes, respectively. [Pg.321]

The linear approximation results in loss of direct information about the transfer coefficient Uq, and in small amplitude methods it is therefore necessary to measure Iq as a function of Cq and Cr in order to obtain o c indirectly via Equations (3.19) and (3.20). [Pg.85]

Why Large Amplitude Methods Should not be Used to Obtain D pp s for Electronically Conductive Polymers... [Pg.120]

First, because the polymer is in the reduced form, the electrode area is just the substrate Pt area and, because this Pt electrode is a disk, diffusion must be linear. Second, because the polymer is never converted to a conductor, the large, unknown "capacitive-like" current associated with the conductive form is not observed. The only capacitive current is that associated with charging the double layer at the Pt/film interface and this can be easily measured and corrected (30). Finally, because this is a small amplitude method, the problem of converting one material into a second, very different, material during the course of the experiment is clearly obviated. [Pg.121]

First, because this is a small amplitude method, the electrochemical, chemical and morphological properties of the film are not greatly perturb by the analysis. Because electroactive pol3nner films may show dramatic changes in solvent content, ionic character, morphology, etc. upon oxidation or... [Pg.135]

As we shall see, the discussion presented applies to chronocoulometry and other large amplitude methods also. [Pg.137]

In the assumption that the TNPC interaction constant 1, and in analogy with the calculation of the P-odd amplitude method [27], we shall use the distorted wave Bom approximation in the first power of g,... [Pg.98]

In this constant-load-amplitude method, crack length is measured visually or by an equivalent method as a fimction of elapsed cycles, and these data are subjected to numerical analysis to establish die rate of crack growth. Crack growth rates are ttien expessed as a function of crack tip stress intensity range AAT, which is calculated from expressions basal on linear-elastic stress analysis. [Pg.129]


See other pages where Amplitude method is mentioned: [Pg.150]    [Pg.158]    [Pg.421]    [Pg.384]    [Pg.384]    [Pg.460]    [Pg.320]    [Pg.320]    [Pg.323]    [Pg.104]    [Pg.120]    [Pg.120]    [Pg.121]    [Pg.136]    [Pg.458]   
See also in sourсe #XX -- [ Pg.304 , Pg.320 , Pg.321 , Pg.323 ]




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