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Microelectrodes ohmic drop

A major advantage of microelectrodes is that electrochemical data is less distorted by ohmic drop than when recorded with electrodes of conventional size... [Pg.385]

Advantages are also found with microelectrodes used at short time scales where time-dependent currents are obtained, as the example in Figure 12.4 shows [56]. Time-dependent currents are proportional to the electrode area. Thus, for the case of a sphere, combination of the expression for the time-dependent current with the resistance shows that the ohmic drop is directly proportional to the radius. Thus, ohmic drop is always minimized by the use of a smaller electrode. [Pg.388]

The magnitude of the ohmic drop at a microelectrode can be evaluated quite readily for case 1 from a knowledge of the specific solution resistance (obtained from conductivity measurements such as in Table 12.1) and the expressions for the voltammetric current for the specific microelectrode employed. Case 2 is also straightforward if the free concentration of ions exceeds that of the electroactive species. However, the situation is somewhat more complicated for the third class. In this case, and in case 2 for fully associated electrolyte, migration as well as diffusion can affect the observed voltammetric signals. In all three cases, the situation may be further complicated by a change in structure of the double layer. However, this is ignored for now, and is considered in the section on very small electrodes. [Pg.389]

The electrode size is another important variable to analyze since the use of microelectrodes is very relevant for experimental electrochemical studies enabling the reduction of capacitative and ohmic drop effects, as indicated in Sect. 2.7. Specifically, it is of great interest to check the behavior of the system when the size of the electrode is reduced. In Fig. 4.20, the influence of the electrode radius on the... [Pg.282]

In order to avoid the distortion caused by these two effects, the usual approach is to compensate the resistance Ru by a positive feedback loop (this is imperative in systems like plasticized membranes for which the uncompensated resistance can be of the order of megaohms [32-34]). Another possibility is to use microelectrodes, for which a decrease in the measured current is obtained which minimizes the ohmic drop and charging current distortion (see Sects. 2.7 and 5.4.1). [Pg.347]

As stated in Sect. 5.2.3.4, there is always a potential difference generated by the flow of faradaic current I through an electrochemical cell, which is related to the uncompensated resistance of the whole cell (Ru). This potential drop (equal to IRU) can greatly distort the voltammetric response. At microelectrodes, the ohmic drop of potential decreases strongly compared to macroelectrodes. The resistances for a disc or spherical microelectrode of radius rd or rs are given by (see Sect. 1.9 and references [43, 48-50]). [Pg.359]

When the electrochemical properties of some materials are analyzed, the timescale of the phenomena involved requires the use of ultrafast voltammetry. Microelectrodes play an essential role for recording voltammograms at scan rates of megavolts-per-seconds, reaching nanoseconds timescales for which the perturbation is short enough, so it propagates only over a very small zone close to the electrode and the diffusion field can be considered almost planar. In these conditions, the current and the interfacial capacitance are proportional to the electrode area, whereas the ohmic drop and the cell time constant decrease linearly with the electrode characteristic dimension. For Cyclic Voltammetry, these can be written in terms of the dimensionless parameters yu and 6 given by... [Pg.361]

Now it is possible to assemble microelectrodes with extremely short response times. Nevertheless, an additional problem for the reduction of the ohmic drop is that for short times high currents arise from the large concentration surface gradients. This leads to the use of on-line and real-time electronic compensation of the cell resistance combined with the use of microelectrodes [53]. [Pg.361]

In the last 30 years, the manufacturing and use of micrometer- and nanometer-sized electrochemical interfaces, microelectrodes, and micro-ITIES have been widely extended. The main advantages associated with the reduction of the size of the interface are the fast achievement of a time-independent current-potential response (independent of the electrochemical technique employed), the decrease of the ohmic drop, the improvement of the ratio of faradaic to charge current, and the enhancement of the mass transport. Their small size has played an important role in... [Pg.369]

The main purpose of this contribution, however, is to review recent advances in solid state ionics achieved by means of microelectrodes, i.e. electrodes whose size is in the micrometer range (typically 1-250 pm). In liquid electrolytes (ultra)-microelectrodes are rather common and applied for several reasons they exhibit a very fast response in voltametric studies, facilitate the investigation of fast charge transfer reactions and strongly reduce the importance of ohmic drops in the electrolyte, thus allowing e.g. measurements in low-conductive electrolytes [33, 34], Microelectrodes are also employed to localize reactions on electrodes and to scan electrochemical properties of electrode surfaces (scanning electrochemical microscope [35, 36]) further developments refer to arrays of microelectrodes, e.g. for (partly spatially resolved) electroanalysis [37-39], applications in bioelectrochemistry and medicine [40, 41] or spatially resolved pH measurements [42], Reviews on these and other applications of microelectrodes are, for example, given in Ref. [33, 34, 43-47],... [Pg.5]

A typical impedance spectrum obtained on LSM microelectrodes is shown in Fig. 42a. The arc represents the impedance due to the electrochemical reaction at the LSM microelectrode. A small ohmic drop caused by the YSZ electrolyte (and partly by the sheet resistance due to the finite electronic conductivity of the LSM electrode) is more than three orders of magnitude smaller than the electrode resistance and not visible in the figure. The impedance spectra for nominally identical microelectrodes turned out to be reproducible with a standard deviation <15%. The data of Fig. 42b display the relation between the electrode resistance Rei and the microelectrode diameter dme several series of experiments with different electrode thicknesses consistently revealed that the resistance Rei is approximately proportional to dmc 2. and hence to the inverse electrode area. [Pg.73]

Attractive features of microelectrodes relative to conventionally sized electrodes include increased current density, reduced charging currents and reduced ohmic drop (see Section 2). The last of these permits experiments to... [Pg.63]

Platinum, glasslike carbon, and tungsten are often used as inert working electrodes for the fundamental electrochemical studies in the ionic liquids. For such transient electrochemical techniques as cyclic voltammetry, chronoamperometry, and chronopotentiometry, it is safer to use the working electrode with a small active area. This is because most of the ionic liquids will have low conductivity, and this often causes the ohmic drop in the measured potentials by the current flowing between the working and counter electrode. Microelectrodes may be useful for the electrochemical measurements in the case of handling low conductive media. [Pg.29]

The peak-potential difference A p depends mainly on the kinetic parameter i/t, as illustrated in Table 2. By measurement of A p as a function of v for a given system, k° can be estimated. However, great care should be exerted to ensure that uncompensated resistance does not contribute to the value of A p, since this would hamper the procedure. Clearly, the use of ultramicroelectrodes can be recommended for this kind of measurements, as the ohmic drop is much smaller here compared to microelectrodes of normal size. This is particularly true when high sweep rates are required for determining large values of k° (see Section 2.4)... [Pg.522]

Unfortunately the use of planar and (hemi)spherical electrodes is not always appropriate or possible in electrochemical studies. Electrodes with large areas lead to problems derived from large ohmic drop and capacitive effects, and the fabrication of (hemi)spherical microelectrodes is difficult. Consequently microdisc electrodes are ubiquitous in electrochemical experiments since they allow for the reduction of the above undesirable effects and are easy to manufacture and clean. This is also true in the case of band electrodes and electrodes with heterogeneous surfaces due to the non-... [Pg.10]

A microdisc electrode is a micron-scale flat conducting disc of radius r. that is embedded in an insulating surface, with the disc surface flush with that of the insulator. It is assumed that electron transfer takes place only on the surface of the disc and that the supporting smlace is completely electroinactive under the conditions of the experiment. These electrodes are widely employed in electrochemical measurements since they offer the advantages of microelectrodes (reduced ohmic drop and capacitive effects, miniaturisation of electrochemical devices) and are easy to fabricate and clean for surface regeneration. In Chapter 2, we considered a disc-shaped electrode of size on the order of 1 mm. In that case we could approximate the system as one-dimensional because the electrode was large in comparison to the thickness of the diffusion layer, such that the current was essentially uniform across the entire electrode surface. Due to the small size of the microdisc, this approximation is no longer valid so we must work in terms of a three-dimensional coordinate system. While the microdisc can... [Pg.175]

Figure 7 Background-subtracted experimental (solid lines) and simulated (open circles) cyclic voltammograms for a solution of ferrocene (10 mmol I h in acetonitrile containing 0.6 mol I TEAR. Sweep rates are 100, 200, and 500 kV s and the gold microelectrode radius is 5 pm. Simulations allow for ohmic drop and RC constant and k° is 3.1 cms k (Reproduced with the permission of the American Chemical Society from Analytical Chemistry GO (1988) 305. Figure 7 Background-subtracted experimental (solid lines) and simulated (open circles) cyclic voltammograms for a solution of ferrocene (10 mmol I h in acetonitrile containing 0.6 mol I TEAR. Sweep rates are 100, 200, and 500 kV s and the gold microelectrode radius is 5 pm. Simulations allow for ohmic drop and RC constant and k° is 3.1 cms k (Reproduced with the permission of the American Chemical Society from Analytical Chemistry GO (1988) 305.

See other pages where Microelectrodes ohmic drop is mentioned: [Pg.39]    [Pg.381]    [Pg.369]    [Pg.385]    [Pg.386]    [Pg.387]    [Pg.388]    [Pg.393]    [Pg.398]    [Pg.731]    [Pg.172]    [Pg.120]    [Pg.359]    [Pg.39]    [Pg.37]    [Pg.523]    [Pg.532]    [Pg.321]    [Pg.317]    [Pg.201]    [Pg.176]    [Pg.182]    [Pg.1365]    [Pg.368]    [Pg.4929]    [Pg.4942]    [Pg.4942]    [Pg.4947]    [Pg.1191]    [Pg.1197]    [Pg.2007]    [Pg.69]    [Pg.205]   
See also in sourсe #XX -- [ Pg.158 , Pg.163 , Pg.167 ]




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