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Circuit parameters electrode

FIG. 6 Complex impedance plots for the electrode reaction of [Fe(CN)6] on bare (open circle) and DNA-modilied (filled circle) An electrodes. An equivalent circuit for the electrode system is shown in the inset and solid lines represent theoretical responses from the circuit. Parameters used in simulation are cited in the text. Electrode potential, + 205 mV (vs. Ag/AgCl) AC amplitude, 25 mV (p-p). Other conditions are the same as those in Fig. 5. [Pg.524]

Knowing /data operational limits during select and deselect times, it is important that the pixel electrode circuit parameters are carefully designed to balance those two limits and to achieve largest possible /data operational range. [Pg.594]

A schematic representation of a 2-D distribution for an ideally polarized disk electrode is presented in Figure 13.1(a). For a 2-D distribution, the circuit parameters, e.g., capacitance and Ohmic resistance, could be a function of radial position... [Pg.234]

Figure 2. Equivalent circuit of a bacteriorhodopsin membrane that includes the circuit parameters of the inert supporting structure and the access impedance of the measuring system. Re is the access impedance, which includes the input impedance of the measuring device, the electrode impedance, and the electrolyte impedance between the membrane and the electrodes. Rm and Cm are the resistance and the capacitance of the membrane, C p is the chemical capacitance, Rp is the internal resistance of the photoelectric voltage source, Ep(U, which is a function of the illuminating light power, and Rs is the transmembrane resistance encountered by the dc photocurrent. (Reproduced from reference 19. Figure 2. Equivalent circuit of a bacteriorhodopsin membrane that includes the circuit parameters of the inert supporting structure and the access impedance of the measuring system. Re is the access impedance, which includes the input impedance of the measuring device, the electrode impedance, and the electrolyte impedance between the membrane and the electrodes. Rm and Cm are the resistance and the capacitance of the membrane, C p is the chemical capacitance, Rp is the internal resistance of the photoelectric voltage source, Ep(U, which is a function of the illuminating light power, and Rs is the transmembrane resistance encountered by the dc photocurrent. (Reproduced from reference 19.
Although a more complicated nonlinear least squares procedure has been described by Tsai and Whitmore [1982] which allows analysis of two arcs with some overlap, approximate analysis of two or more arcs without much overlap does not require this approach and CNLS fitting is more appropriate for one or more arcs with or without appreciable overlap when accurate results are needed. In this section we have discussed some simple methods of obtaining approximate estimates of some equivalent circuit parameters, particularly those related to the common symmetrical depressed arc, the ZARC. An important aspect of material-electrode characterization is the identification of derived parameters with specific physicochemical processes in the system. This matter is discussed in detail in Sections 2.2 and 3.3 and will not be repeated here. Until such identification has been made, however, one cannot relate the parameter estimates, such as Rr, Cr, and y/zc, to specific microscopic quantities of interest such as mobilities, reaction rates, and activation energies. It is this final step, however, yielding estimates of parameters immediately involved in the elemental processes occurring in the electrode-material system, which is the heart of characterization and an important part of IS. [Pg.20]

Aging in crystal oscillators generally refers to any change over time that affects the frequency characteristics of the oscillator or the physical parameters that describe the device, for example, motional time constant and equivalent circuit parameters. Some factors that influence aging include surface deterioration, surface contamination, electrode composition, and environmental conditions. [Pg.253]

At present, the microwave electrochemical technique is still in its infancy and only exploits a portion of the experimental research possibilities that are provided by microwave technology. Much experience still has to be gained with the improvement of experimental cells for microwave studies and in the adjustment of the parameters that determine the sensitivity and reliability of microwave measurements. Many research possibilities are still unexplored, especially in the field of transient PMC measurements at semiconductor electrodes and in the application of phase-sensitive microwave conductivity measurements, which may be successfully combined with electrochemical impedance measurements for a more detailed exploration of surface states and representative electrical circuits of semiconductor liquid junctions. [Pg.519]

Note that a number of complicating factors have been left out for clarity For instance, in the EMF equation, activities instead of concentrations should be used. Activities are related to concentrations by a multiplicative activity coefficient that itself is sensitive to the concentrations of all ions in the solution. The reference electrode necessary to close the circuit also generates a (diffusion) potential that is a complex function of activities and ion mobilities. Furthermore, the slope S of the electrode function is an experimentally determined parameter subject to error. The essential point, though, is that the DVM-clipped voltages appear in the exponent and that cheap equipment extracts a heavy price in terms of accuracy and precision (viz. quantization noise such an instrument typically displays the result in a 1 mV, 0.1 mV, 0.01 mV, or 0.001 mV format a two-decimal instrument clips a 345.678. .. mV result to 345.67 mV, that is it does not round up ... 78 to ... 8 ). [Pg.231]

But when considered over a wide range of frequencies, the properties of a real electrode do not match those of the equivalent circuits shown in Fig. 12.12 the actual frequency dependence of Z and a does not obey Eq. (12.21) or (12.22). In other words, the actual values of R and or R and are not constant but depend on frequency. In this sense the equivalent circuits described are simplified. In practice they are used only for recording the original experimental data. The values of R and Cj (or R and C ) found experimentally for each frequency are displayed as functions of frequency. In a subsequent analysis of these data, more complex equivalent circuits are explored which might describe the experimental frequency dependence and where the parameters of the individual elements remain constant. It is the task of theory to interpret the circuits obtained and find the physical significance of the individual elements. [Pg.209]

Under this electrochemical configuration, it is commonly accepted that the system can be expressed by the Randles-type equivalent circuit (Fig. 6, inset) [23]. For reactions on the bare Au electrode, mathematical simsulations based on the equivalent circuit satisfactorily reproduced the experimental data. The parameters used for the simulation are as follows solution resistance, = 40 kS2 cm double-layer capacitance, C = 28 /xF cm equivalent resistance of Warburg element, W — R = 1.1 x 10 cm equivalent capacitance of Warburg element, IF—7 =l.lxl0 F cm (

charge-transfer resistance, R = 80 kf2 cm. Note that these equivalent parameters are normalized to the electrode geometrical area. On the other hand, results of the mathematical simulation were unsatisfactory due to the nonideal impedance behavior of the DNA adlayer. This should... [Pg.523]

Ion transport across membranes can be evaluated by using mucosal and serosal electrodes to read transepithelial current (I) and potential difference OP). With these parameters, equivalent circuit analysis can be utilized to account for the relative contributions of transcellular and paracellular pathways. Ionic flux (J) is defined by the Nernst-Planck equation,... [Pg.180]

We found an equivalent electrical circuit that fits best the LixC6 electrode behavior at high frequency. The circuit consists of a resistor R in parallel with a constant phase element (CPE). The latter is defined with a pseudo-capacitance Q and a parameter a with 0< a <1 [6], The impedance of... [Pg.263]

C Linewidth Control, This parameter refers to the necessity of maintaining the correct features size across an entire substrate and from one substrate to another. This is important since the successful performance of most devices depends upon control of the size of critical structures, as for example in the gate electrode structure in an MOS device. As feature size is decreased and circuit elements packed closer together, the margin of error on feature size control is reduced. The allowable size variation on structures is generally a fixed fraction of the nominal feature size. A rule of thumb is that the dimensions must be controlled to tolerances of at least 1/5 the minimum feature size. Linewidth control is affected by a variety of parame-... [Pg.172]


See other pages where Circuit parameters electrode is mentioned: [Pg.207]    [Pg.132]    [Pg.145]    [Pg.542]    [Pg.139]    [Pg.152]    [Pg.166]    [Pg.138]    [Pg.306]    [Pg.268]    [Pg.76]    [Pg.58]    [Pg.1283]    [Pg.239]    [Pg.167]    [Pg.61]    [Pg.376]    [Pg.542]    [Pg.509]    [Pg.570]    [Pg.477]    [Pg.363]    [Pg.552]    [Pg.88]    [Pg.105]    [Pg.274]    [Pg.195]    [Pg.208]    [Pg.346]    [Pg.370]    [Pg.236]    [Pg.592]    [Pg.594]    [Pg.603]    [Pg.251]    [Pg.481]   
See also in sourсe #XX -- [ Pg.498 ]




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