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Electrolyte contact

Figure 4 shows the application (6) of potentials to the Pt and Au electrodes of the sandwich (vs. a reference electrode elsewhere in the contacting electrolyte solution) so that they span the E° of the poly-[Co(II/I)TPP] couple (Fig. 4B). There is a consequent redistribution of the concentrations of the sites in the two oxidation states to achieve the steady state linear gradients shown in the inset. Figure 4C represents surface profilometry of a different film sample in order to determine the film thickness from that the actual porphyrin site concentration (0.85M). The flow of self exchange-supported current is experimentally parameterized by applying Fick s first law to the concentration-distance diagram in Fig. 4B ... Figure 4 shows the application (6) of potentials to the Pt and Au electrodes of the sandwich (vs. a reference electrode elsewhere in the contacting electrolyte solution) so that they span the E° of the poly-[Co(II/I)TPP] couple (Fig. 4B). There is a consequent redistribution of the concentrations of the sites in the two oxidation states to achieve the steady state linear gradients shown in the inset. Figure 4C represents surface profilometry of a different film sample in order to determine the film thickness from that the actual porphyrin site concentration (0.85M). The flow of self exchange-supported current is experimentally parameterized by applying Fick s first law to the concentration-distance diagram in Fig. 4B ...
These experiments address a number of issues which are of importance for immobilized polymer layers in general. First of all, the layer structure and thickness is strongly dependent on the nature of the contacting electrolyte. Therefore, in cases where liquid-polymer interfaces are envisaged to allow for particular applications, this interaction needs to be considered in detail. As discussed below in Chapter 5, in order to understand the charge transport properties of these layers the interplay between polymer layer and contacting liquids needs to be considered seriously. [Pg.147]

Figure 5.15 Cyclic voltammograms obtained for a mercury electrode immersed in a 5 mM solution of 2,7-AQDS as the pH of the unbuffered contacting electrolyte solution (0.1 M UCIO4) is varied by using either HCIO4 or NaOH. The pH values, from left to right, are 2.8, 3.5, 4.8 and 6.1. The scan rate is 0.1 V s, with an initial potential of —1.000 V. The inset shows the dependence of the formal potential on the solution pH in unbuffered solution. Reprinted from. Electroanal. Chem., 498, R. J. Forster and J. P. O Kelly, Protonation reactions of anthroquinone-2,7-disulfonic acid in solution and within monolayers, 127-135, Copyright (2001), with permission of Elsevier Science... Figure 5.15 Cyclic voltammograms obtained for a mercury electrode immersed in a 5 mM solution of 2,7-AQDS as the pH of the unbuffered contacting electrolyte solution (0.1 M UCIO4) is varied by using either HCIO4 or NaOH. The pH values, from left to right, are 2.8, 3.5, 4.8 and 6.1. The scan rate is 0.1 V s, with an initial potential of —1.000 V. The inset shows the dependence of the formal potential on the solution pH in unbuffered solution. Reprinted from. Electroanal. Chem., 498, R. J. Forster and J. P. O Kelly, Protonation reactions of anthroquinone-2,7-disulfonic acid in solution and within monolayers, 127-135, Copyright (2001), with permission of Elsevier Science...
The strong dependence of the layer structure on the nature of the contacting electrolyte has been further investigated by using the electrochemical quartz crystal microbalance (EQCM). As discussed above in Chapter 3, this technique is based on the measurement of the frequency with which a coated quartz crystal vibrates, and this frequency can then be related to the mass of this crystal provided that the material attached to the surface is rigid. In this way, the changes that occur in thin films as a result of redox processes can be monitored. [Pg.248]

The above example shows how the interfacial processes occurring at thin polymer films can be manipulated by a change in the contacting electrolyte. This section... [Pg.254]

Marcus has recently returned to this problem [133] and, by analogy with the problem of donor-acceptor electron transfer at the interface between two immiscible liquids, has derived the following expression for ka, the heterogeneous rate constant for electron transfer from a semiconductor to a species in a contacting electrolyte ... [Pg.306]

When all the above conditions are met, as shown in Fig. 10.18, protruding and recess areas are in different electrochemical conditions. The protruding area directly contacts electrolyte and electrochemical dissolution occurs under ohmic control that is, its dissolution rate (/ d) is determined by the polarization... [Pg.315]

H. C. Harten, The surface recombination on silicon contacting electrolyte, J. Phys. Chem. Solids 14, 220, 1960. [Pg.463]

Most of the reported electrochemistry with solid electrodes involves polycrystalline materials. Such electrodes consist of a variety of small domains with different crystal faces and edges presented to the contacting electrolyte. As discussed below, different crystal faces exhibit different properties (e.g., PZC or work function) so that the behavior observed at a polycrystalline electrode represents an average of that for a number of different crystal... [Pg.557]

Relatively scant attention has been given to the synthesis of new polymeric materials which could photoelectrochemically split water. An obvious reason for this is the consideration that if everyday insulating polymers are subject to photodegrada-tlon in routine environmental exposures, what chance would a semiconducting or conducting polymer, with more reactive centers such c=Q, have to survive under yet more harsh chemical conditions. Such odds have not deterred polymer chemists in the past, however, and now that the attention of more chemists has been stimulated, rapid developments in this area may be anticipated. In fact even the labile polyacetylene has been found to be significantly stabilized when physically mixed with polyethylene (27c) or when Cl is available in the contacting electrolyte (27d). [Pg.482]

Skin electrodes have the largest commercial product volume, most of them are pregelled ready-to-use nonsterile products. Some of them have a snap-action wire contact others are prewired, for instance, adapted for babies. There is a contact electrolyte between the skin and the electrode metal. Dry SC is a poor conductor and this easily results in poor (high impedance) contact and noise. The contact area with the skin should be as large as practically possible, and reducing the SCs thickness by sandpaper abrasion is useful. Hydrating the skin with contact electrolyte or by the covering effect of the electrode will usually reduce the contact impedance with time (minutes to hours). [Pg.157]

Figure 2.3 shows how the actual conductivity may he lower because the dependence is not linear. Molar conductivity, Ao, relates to the limiting value at low concentrations. For NaCI, the relationship is quite linear up to the physiological concentration of 0.9% by weight. Sweat concentrations are somewhat lower, urine concentrations vary but may be higher, and seawater concentrations are approximately 3.5%. Much higher concentrations are sometimes used for contact electrolytes (cf. Section 7.4). [Pg.22]

A surface electrode with the contact electrolyte covering a part of the skin may influence... [Pg.101]

Osmotic transport of water to or from the contact electrolyte. [Pg.101]

With a dry electrode plate, the moisture buildup and admittance increase in the SC start at the moment of electrode onset. With a hydrogel, admittance may increase or decrease. With wet gel or a liquid, the initial admittance is high, and with strong contact electrolytes the admittance will further increase for many hours and days (Figure 4.20). Because the outer layers of SC may be wet or dry according to the ambient air, it will not be possible to find a general contact medium that just stabilizes the water content in the state it was before electrode onset the onset of the electrode will generally influence the parameters measured. [Pg.101]

The electric double layer is the most central part of an electrode. It is a very thin layer formed at the sharp boundary (interphase) between an electronic conductor and an ionic conductor (e.g., between a metal plate and an electrolyte). The double layer is described in Section 7.5. The electronic conductors are described now and the ionic conductor (contact electrolyte) will be described in file next Section 7.4 (Table 7.1). [Pg.180]


See other pages where Electrolyte contact is mentioned: [Pg.141]    [Pg.411]    [Pg.418]    [Pg.81]    [Pg.119]    [Pg.127]    [Pg.131]    [Pg.143]    [Pg.144]    [Pg.146]    [Pg.170]    [Pg.244]    [Pg.245]    [Pg.286]    [Pg.120]    [Pg.128]    [Pg.276]    [Pg.330]    [Pg.483]    [Pg.2919]    [Pg.3799]    [Pg.20]    [Pg.229]    [Pg.233]    [Pg.158]    [Pg.580]    [Pg.173]    [Pg.187]    [Pg.206]    [Pg.208]    [Pg.217]    [Pg.226]    [Pg.182]    [Pg.180]   
See also in sourсe #XX -- [ Pg.40 , Pg.49 ]




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