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Polarography reversible systems

An increase in co from 400 to 1600rpm tints results in a twofold increase of the signal. A deviation from linearity of a plot of z) vs. col/1 suggests some kinetic limitations. In addition, at veiy low rotation speeds (0-100 rpm), a slight upward bend is observed due to contribution by natural convection. The voltammetric wave has a sigmoidal shape for reversible systems it is identical to that common in DC polarography (described in Section 3-2), and independent of to. [Pg.112]

Redox switching, 126 Reference electrodes, 100, 105, 142 Reflectance spectroscopy, 44 Resistance, 22, 105 Resolution 50, 71 Reverse pulse polarography, 68 Reversible systems, 4, 31 Reticulated vitreous carbon, 114, 115 Riboflavin, 37... [Pg.209]

Chronopotentiometry at a dme appeared to be impossible until Kies828 recently developed polarography with controlled current density, i.e., with a current density sweep. He explained the method as follows. The high current density during the first stage of the drop life results in the initiation of a secondary electrolysis process at a more negative electrode potential followed by a reverse reaction with rapid (reversible) systems because of the increase in the electrode potential. [Pg.189]

The shape of the current-voltage curves recorded by this technique resembles those obtained by DC polarography. The currents reach a limiting value that is a linear function of concentration of the electroactive species The limiting currents are additive and the half-wave potentials characterize the electroactive species qualitatively. The shape of I-E curves is still affected by the charging current and limiting current can be measured for electrochemically reversible systems to somewhat lower concentrations, up to about 1 x 10-7 mol L-1. [Pg.517]

The only tetrahedral IrIV compound so far known is the tetramesityl,98 Ir(mes)4, made by the interaction of Li mes with partially dehydrated IrCl3 nH20 in Et20. It can be oxidized by AgPF6 to [Irv(mes)4]PF6- This cation is also tetrahedral. Polarography shows the reversible system Irin(mes)4 IrIV(mes)4 Irv(mes)4 but the anion could not be isolated. [Pg.1058]

For reversible systems (with fast eleetron-transfer kinetics), the shape of the polarographie wave can be deseribed by the Heyrovsky—Ilkovic equation ... [Pg.65]

Equation (1.2.40) is very frequently used to determine the formal potential of a redox system with the help of cyclic voltammetry however, one should never forget that it holds true only for reversible systems, and provided that the symmetry coefficient a = 0.5 (see Chap. 1.3). To be cautious, it is better to refer to the value determined by Eq. (1.2.40) as the mid-peak potential determined by cyclic voltammetry. The formal potential E has the same meaning as discussed above for direct current polarography. Hence Eqs. (1.2.32) and (1.2.34) can be applied accordingly. [Pg.29]

Polarography is here taken to mean the use of a dropping mercury electrode (D.M.E.) with a potential scan that is slow enough that each drop sees a virtually constant potential. Considering a reversible system, we have seen that the current leads the potential phasorby 45°. The amplitude / of the current density is measured for a fixed amplitude A of the alternating potential, and is given by... [Pg.270]

In organic polarography X is practically always hydrogen ion. That means that for reversible systems, the pi o-values can be determined from the shift of half-wave potentials with pH in well-buffered solutions, as intersections of the linear portions on 2 i/a-pH plots. [Pg.232]

In view of the range of conclusions which will be derived from the approximate identification of EV2 with E0 it is appropriate to clarify what is involved. We mean here that EV2 = E6 + x the term x is omitted in the subsequent treatment because, as we will show below, it is both small and approximately constant under the relevant conditions. From the theory of polarography it follows that for reversible, one-electron systems... [Pg.225]

Polarography is valuable not only for studies of reactions which take place in the bulk of the solution, but also for the determination of both equilibrium and rate constants of fast reactions that occur in the vicinity of the electrode. Nevertheless, the study of kinetics is practically restricted to the study of reversible reactions, whereas in bulk reactions irreversible processes can also be followed. The study of fast reactions is in principle a perturbation method the system is displaced from equilibrium by electrolysis and the re-establishment of equilibrium is followed. Methodologically, the approach is also different for rapidly established equilibria the shift of the half-wave potential is followed to obtain approximate information on the value of the equilibrium constant. The rate constants of reactions in the vicinity of the electrode surface can be determined for such reactions in which the re-establishment of the equilibria is fast and comparable with the drop-time (3 s) but not for extremely fast reactions. For the calculation, it is important to measure the value of the limiting current ( ) under conditions when the reestablishment of the equilibrium is not extremely fast, and to measure the diffusion current (id) under conditions when the chemical reaction is extremely fast finally, it is important to have access to a value of the equilibrium constant measured by an independent method. [Pg.26]

Often the first step in the electrochemical characterization of a compound is to ascertain its oxidation-reduction reversibility. In our opinion, cyclic voltammetry is the most convenient and reliable technique for this and related qualitative characterizations of a new system, although newer forms of pulse polarography may prove more suitable for quantitative determination of the electrochemical parameters. The discussion in Chapter 3 outlines the specific procedures and relationships. The next step in the characterization usually is the determination of the electron stoichiometry of the oxidation-reduction steps of the compound. Controlled-potential coulometry (discussed in Chapter 3) provides a rigorously quantitative means for such evaluations. [Pg.8]


See other pages where Polarography reversible systems is mentioned: [Pg.155]    [Pg.65]    [Pg.471]    [Pg.515]    [Pg.516]    [Pg.250]    [Pg.163]    [Pg.163]    [Pg.141]    [Pg.141]    [Pg.389]    [Pg.65]    [Pg.112]    [Pg.398]    [Pg.383]    [Pg.385]    [Pg.273]    [Pg.471]    [Pg.515]    [Pg.516]    [Pg.285]    [Pg.72]    [Pg.1005]    [Pg.1005]    [Pg.168]    [Pg.355]    [Pg.360]    [Pg.272]    [Pg.285]    [Pg.148]    [Pg.96]    [Pg.81]    [Pg.1038]    [Pg.130]   
See also in sourсe #XX -- [ Pg.272 ]




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