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Potential current-time domain

The second group of electrochemical methods is aimed at measuring any special characteristics of the films, which cannot be directly obtained from standard electrochemical measurements in the potential-current-time (E-i-t) domain. In this case, in addition to a potentiostat/galvanostat, some specialized equipment and suitable electrochemical cells are required. This group of techniques includes ... [Pg.376]

The micro reactor properties concern process control in the time domain and process refinement in the space domain [65]. As a result, uniform electrical fields are generated and efficiency is thought to be high. Furthermore, electrical potential and currents can be directly measured without needing transducer elements. The reactor fabrication methods for electrical connectors employ the same methods as used for microelectronics which have proven to satisfy mass-fabrication demands. [Pg.548]

As the Laplace transformed current—potential relationship is a much simpler function than its counterpart in the time domain, it has been suggested [76, 77] that it may be advantageous to analyze experimental data in the Laplace domain. In the present case, this would require some procedure to perform Laplace transformation of current datajF(0> i.e. to calculate the integral, according to eqn. (88)... [Pg.266]

For the time domain responses of the CPE, the current density difference (A/)/scan rate (v) relation is expressed by the following power-law during the potential scanning199... [Pg.178]

Figure 5.49 Time course for the limiting current at gold modified with the oligonucleotide 2/4 in methylviologen (MV+2) solution (0.1 mM in 0.1 NaCl) at an applied potential of 0 mV (vs. Ag/AgCl). The inset shows the time domain in which the electrode is alternatively exposed to and shielded from 346 nm illumination the arrows indicate when the shutter is open or closed. From R. S. Reese and M. A. Fox, Spectral and cyclic voltammetric characterization of self-assembled monolayers on gold of pyrene end-labeled oligonucleotide duplexes, Can.. Chem., 77,1077-1084 (1999), with permission from The National Research Council of Canada... Figure 5.49 Time course for the limiting current at gold modified with the oligonucleotide 2/4 in methylviologen (MV+2) solution (0.1 mM in 0.1 NaCl) at an applied potential of 0 mV (vs. Ag/AgCl). The inset shows the time domain in which the electrode is alternatively exposed to and shielded from 346 nm illumination the arrows indicate when the shutter is open or closed. From R. S. Reese and M. A. Fox, Spectral and cyclic voltammetric characterization of self-assembled monolayers on gold of pyrene end-labeled oligonucleotide duplexes, Can.. Chem., 77,1077-1084 (1999), with permission from The National Research Council of Canada...
A common time domain analysis involves computing the standard deviation of the potential (oe) and the standard deviation of the current (of) from the time series data and taking their ratio to compute a noise resistance Rn ... [Pg.451]

These circuits naturally have a frequency-dependent impedance, and it is this that is measured in impedance spectroscopy experiments. The components of the circuit also determine the response of the reaction in the real time domain to any dc perturbation, for example, an electrical pulse or termination of a prior steady current (potential-relaxation experiment). [Pg.29]

The integration converts the time-domain quantities into the respective frequency-domain quantities. Integration is carried out over a period T comprising an integer number of cycles. This serves to filter errors in the measurement. The complex current Ir + jlj and potential Vr + jVj are the coefficients Ci of the Fourier series expressed as equation (7.30). [Pg.121]

Figure 8.7 Lissajous representation for current and applied potential time-domain signals corresponding to a system presented in Figure 7.8 but with a potential perturbation amplitude AV = 100 mV. Figure 8.7 Lissajous representation for current and applied potential time-domain signals corresponding to a system presented in Figure 7.8 but with a potential perturbation amplitude AV = 100 mV.
Add normally distributed stochastic errors to the time-domain potential and current signals for the system described in Example 7.1. Then apply the Fourier analysis to calculate the impedance response at the characteristic frequency. Repeat this process, refreshing the random numbers used, so as to calculate the standard deviation of the resulting impedance. How does this result depend on the number of cycles used for the integration ... [Pg.426]

Analysis of Eq. (17) indicates that the current represents a vector of the length ( o = EqI z, which rotates with the frequency ffl. Current and potential are rotating vectors in the time domain, as represented in Figme 1(a). Using complex notation, they may be described by... [Pg.149]

In time domain measurements, the electrochemical system is subjected to a potential variation that is the resultant of many frequencies, like a pulse or white noise signal, and the time-dependent current from the cell is recorded. The stimulus and the response can be converted via Fourier transform methods to spectral representations of amplitude and phase angle frequency, from which the desired impedance can be computed as a function of frequency. [Pg.407]

There are many instances in electrochemistry when we find it very difficult to obtain an explicit relationship between current, potential, and time. Either the system itself is intrinsically complex (e.g., a quasireversible charge transfer involving adsorbed and diffusing reactant species) or the experimental conditions are less than ideal (e.g., step experiments carried out on a time domain so short that the rise time of the potentiostat is not negligible). It is usually true in these and other cases that much simpler relationships exist in the Laplace domain between the perturbations and the observables. Thus it can be useful to transform the data and carry out the analysis in transform space (39-42). [Pg.410]

Within the electrochemical framework of this classical example of a redox process whose rate is limited by the transport by diffusion, it was shown that, even for a reversible redox process, the derivation of the current response in the time domain is far from simple. In contrast, the impedance approach allows the more difficult case of an irreversible (finite reaction rate constants) redox process to be derived. Using the same approach, we will now examine the case of a multistep reaction, which is very difficult to investigate using techniques of potential step cyclic voltammetry. [Pg.124]

Refinements of the above volume diffusion concept have been made by a model that includes a contribution of surface-diffusion processes to the dissolution reaction of the more active component at subcritical potentials. By adjustment of different parameters, this model allows for the calculation of current-time transients and concentration-depth profiles of the alloy components [102]. In addition to this, mixed control of the dissolution rate of the more active component by both charge transfer and volume diffusion has been discussed. This case is particularly interesting for short polarization times. The analysis yields, for example, the concentration-depth profile and the surface concentration of the more noble component, c, in dependency on the product ky/(t/D), where is a kinetic factor, t is the polarization time, and D is the interdiffusion coefficient. Moreover, it predicts the occurrence of different time domains in the dissolution current transients [109]. [Pg.176]

Fig.3. (A) Time domain potential signal e(i) and (B) the current response i(t). An inverse Fourier transformation gives frequency domain signals E lj) and I uj). Frequency domain admittance, y(o ), can be calculated (C). Fig.3. (A) Time domain potential signal e(i) and (B) the current response i(t). An inverse Fourier transformation gives frequency domain signals E lj) and I uj). Frequency domain admittance, y(o ), can be calculated (C).

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