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Mean limiting diffusion current

By using the mean surface area during the drop life the mean limiting diffusion current can be derived... [Pg.3735]

Mean limiting diffusion current is proportional to the square root of the mercury height... [Pg.3736]

Considering diffusion to a planar electrode with a surface area increasing with time for description of the transport to a growing mercury drop, Ilkovic derived for the mean limiting diffusion current (i(j) Equation 1, bearing his name ... [Pg.349]

However, advantageous applications of micro- and ultramicroelectrodes are not limited to fundamental investigations. Such electrodes open up possibilities for work in very low concentrations of solute. Whatever can be done at a planar electrode can be done at a concentration about a thousand times lower by using an ultramicroelectrode without reaching the limiting diffusion current. This means that one could even obtain responses from solutes of 1 ppb (assuming a measured current density of 1 pA cm-2). [Pg.381]

Equations (3.105)-(3.107) point out the existence of three different polarization causes. So, 7km is a kinetically controlled current which is independent of the diffusion coefficient and of the geometry of the diffusion field, i.e., it is a pure kinetic current. The other two currents have a diffusive character, and, therefore, depend on the geometry of the diffusion field. I((((s corresponds to the maximum current achieved for very negative potentials and I N is a current controlled by diffusion and by the applied potential which has no physical meaning since it exceeds the limiting diffusion current 7 ss when the applied potential is lower than the formal potential (E < Ef"). This behavior is indicated by Oldham in the case of spherical microelectrodes [15, 20, 25]. [Pg.167]

Thus, instead of a limiting diffusion current density plateau, a curve inflection point or a short inclined plateau can be expected on the polarization curve in Ohmic-controlled electrodeposition of metals, as observed in the case of silver electrodeposition from nitrate solutions. The exchange current density of the silver reaction in nitrate electrolytes is sufficiently large to permit Ohmic-controlled deposition as well as dendritic growth at low overpotentials.27 After a linear increase of the deposition current density with increasing overpotential, an exponential increase after the inflection point appears, meaning the elimination of mass-transfer limitations due to the initiation of dendritic growth. [Pg.194]

A study of the interaction of hafiiium with the NaCl-KCl-K2HfF6 melt indicates the absence of metal -salt reaction with the formation of lower oxidation states [7]. It has been shown [8] that at low anodic current densities (up to about 0.02 A/cm ) the mean valence of hafiiium is close to four in the melt NaCl-KCl-K2HfF6 (10 w/o). This is due to the fact that this current density is not above the limiting diffusion current density for hafiiium dissolution according to reaction ... [Pg.191]

Noise analysis has been particularly fruitfiil in characterizing various aspects of hydrodynamics, as noted above for the specific case of corrosion processes. First of all, multiphase flows were investigated, either gas/water [78], solid/liquid [79, 80], oil/water [81] or oil/brine [82]. In these flows, fluctuations are due primarily either to fluctuations in transport rates to an electrode or to fluctuations in electrolyte resistance. If one phase preferentially wets the electrode, then there may be fluctuations due to variation in the effective electrode area. Each of these phenomena has a characteristic spectral signature. Turbulent flows close to a wall have been investigated by means of electrochemical noise by using electrochemical probes of various shapes, by measuring the power spectral density of the limiting diffusion current fluctuations [83-86],... [Pg.215]

The mean of the limiting diffusion current in the DC polarogram is obtained from Equation (7) by integration over the entire drop time ... [Pg.789]

The other major limitation of membrane simulations is the time and length scale we are able to simulate. We are currently able to reach a microsecond, but tens to hundreds of nanosecond simulations are more common, especially in free energy calculations. The slow diffusion of lipids means we are not able to observe many biologically interesting phenomena using equilibrium simulations. For example, we would not observe pore formation in an unperturbed bilayer system during an equilibrium simulation, and even pore dissipation is at the limits of current computational accessibility. [Pg.7]

When it is possible to control the drop-time of the mercmy electrode (whilst keeping the flow rate m of mercmy constant), the mean limiting current (i) is found to be proportional to for kinetic currents and to for diffusion currents. It is best to determine the slope of a plot of log against log i. A simple way to study the dependence of current on drop-time is to measure the limiting currents and the drop-time with the... [Pg.36]

The limiting current of the second wave (ij) is a diffusion current Curve 2 of Fig. 10 shows the relationship between this current and the equilibrium potential. In the range of high electron concentrations, this relationship can be expressed as Eq = const — (0.029 0.002) Ig i. The value of the proportionality constant 0.029 = 2.3 RT/nF, where n = 2 (see Eq. (8)), indicates that the electrode is in thermodynamic equilibrium with the electrons in solution, which are practically completely bound to form non-paramagnetic complexes containing two electrons. On decreasing the concentration of electrons, the slope of curve 2 is observed to increase (which means a decrease in the effective value of n). This happens due to partial dissociation of the associate. In Ref. 178 an increase in the height of the first... [Pg.183]

Suppose we now consider a series of step experiments in the anthracene solution discussed earlier. Between each experiment the solution is stirred, so that the initial conditions are always the same. Similarly, the initial potential (before the step) is chosen to be at a constant value where no faradaic processes occur. The change from experiment to experiment is in the step potential, as depicted in Figure 5.1.3a. Suppose, further, that experiment 1 involves a step to a potential at which anthracene is not yet electroactive that experiments 2 and 3 involve potentials where anthracene is reduced, but not so effectively that its surface concentration is zero and that experiments 4 and 5 have step potentials in the mass-transfer-limited region. Obviously experiment 1 yields no faradaic current, and experiments 4 and 5 yield the same current obtained in the chronoamperometric case above. In both 4 and 5, the surface concentration is zero hence anthracene arrives as fast as diffusion can bring it, and the current is limited by this factor. Once the electrode potential becomes so extreme that this condition applies, the potential no longer influences the electrolytic current. In experiments 2 and 3 the story is different because the reduction process is not so dominant that some anthracene cannot coexist with the electrode. Still, its concentration is less than the bulk value, so anthracene does diffuse to the surface where it must be eliminated by reduction. Since the difference between the bulk and surface concentrations is smaller than in the mass-transfer-limited case, less material arrives at the surface per unit time, and the currents for corresponding times are smaller than in experiments 4 and 5. Nonetheless, the depletion effect still applies, which means that the current still decays with time. [Pg.158]

This condition is fulfilled for sufficiently large water concentrations at the inlet and/or large parameter r. Physically, large r means a high rate of back diffusion of liquid water in membrane and/or a low rate of water vapor leakage to the channel. In both these cases, the upper limit of current density, which satisfies (6.115) increases. [Pg.242]

If the special conditions (e.g., nernstian behavior or diffusion limiting current) are not valid, the solution of the differential equations are more difficult. In electro-analytical chemistry, techniques are used where the current-potential relationship is relatively simple consequently, the evaluation of the data is straightforward. This means that the current is directly proportional to the concentration (quantitative analysis) or the characteristic potential (peak potential, half-wave potential, etc.) values can easily and unambiguously be determined (qualitative analysis). In most cases, the experimental conditions can be varied in such a way that the desirable situation is realized. [Pg.54]

If the potential amplitude of the step is less than 2 - E, i.e., the step is made to any potential in the rising portion of the voltammogram, either charge transfer control or mixed kinetic-diffusional control prevails, i.e., the concentration of the reactant is not zero at the electrode surface. Still, cr (x = 0) < c, so R does diffuse to the electrode surface where it is oxidized. Since the difference between the bulk and surface eoncentration is smaller than in the case of mass transport control, less material arrives at the surface per unit time, and the currents for corresponding times are smaller than in the diffusion-limited situation. Nevertheless, the concentration gradient for R still increases, which means that the current still decreases with time, albeit to a smaller extent. The current-time curves when the potential is stepped from 2 > E2 > E22 are shown in Fig. II.4.6. [Pg.155]

Note that/(jin Eqn (6.31) is not necessarily the limiting current. If at the beginning of the reaction there is no H2O2 in the solution, which means the bulk concentration of H2O2 is zero, the diffusion current for H2O2 removal from the disk electrode should be... [Pg.217]

Fig. 24. Comparison of the faradaic currents in the DCP, NPP, and DPP. 1, the mean diffusion limited DCP current 2, Ip and Ep the coordinates of the DPP peak 3, the current-potential plot in the NPP technique I, the NPP (sampled) diffusion-limited current i, the DCP (sampled) limiting current. Note the shift of Ep vs. Ej/2 and the mutual heights of the limiting (peak) currents i, Ij, and Ip under identical experimental conditions. Fig. 24. Comparison of the faradaic currents in the DCP, NPP, and DPP. 1, the mean diffusion limited DCP current 2, Ip and Ep the coordinates of the DPP peak 3, the current-potential plot in the NPP technique I, the NPP (sampled) diffusion-limited current i, the DCP (sampled) limiting current. Note the shift of Ep vs. Ej/2 and the mutual heights of the limiting (peak) currents i, Ij, and Ip under identical experimental conditions.
As a useful diagnostic tool that could verify the proposed mechanism the plots of E[/2 (and the mean limiting current Ij) on pH have been applied [50]. The reactions (a) and (b) respond to the ECp mechanism. Since the limiting current in the whole pH range is constant, diffusion control of the whole electrode process may be considered. Under such conditions the E,/2-pH dependence is given as follows... [Pg.179]

Concentrations of the order 10 or even 10 m can be achieved by means of some catalytic waves, e.g. vitamin (cobalamin). On the other hand waves for some kinetic currents, where the limiting current is only a fraction of the hypothetical diffusion current, 0-01 to OT M solutions are used for polarographic investigations. [Pg.78]


See other pages where Mean limiting diffusion current is mentioned: [Pg.308]    [Pg.308]    [Pg.304]    [Pg.206]    [Pg.112]    [Pg.225]    [Pg.226]    [Pg.240]    [Pg.694]    [Pg.209]    [Pg.695]    [Pg.365]    [Pg.60]    [Pg.281]    [Pg.385]    [Pg.228]    [Pg.452]    [Pg.209]    [Pg.309]    [Pg.116]    [Pg.655]    [Pg.86]    [Pg.123]    [Pg.6308]    [Pg.6308]    [Pg.698]    [Pg.142]    [Pg.65]    [Pg.787]    [Pg.476]   
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