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Electrochemistry reference electrode, position

Let us note one vital point, which is of methodological importance. It has been traditionally accepted in electrochemistry to choose the positive direction of the electrode potential

positive electrode charge. Here the zero potential is assumed to be that of the reference electrode, which coincides, within a constant, with the potential in the solution bulk (— oo). On the other hand, in physics of semiconductor surface the potential is usually reckoned from the value in the semiconductor bulk ( ) the enrichment of the surface with electrons, i.e., the formation of a negative space charge, corresponding to the positive potential of the surface. In particular, this statement directly follows from the Boltzmann distribution for electrons and holes in the space-charge region in a semiconductor ... [Pg.265]

Because of its ability to position an electrode tip with high spatial resolution in three dimensions, SECM can be used to probe electrochemistry in a small volume of liquid (e.g., on a conductive substrate that serves as a counter/ reference electrode). For example, a solution volume of 3-20 /jlL was used to probe the adsorption isotherms on a mineral surface (30). Probing even smaller volumes, e.g., of liquids contained in pores, should be possible. Since electrochemical generation is an ideal method for producing small, controlled amounts of reactants, studies in which one wants to probe chemistry with very limited amounts of sample appear to be a good application. In such studies, means to maintain the sample volume and prevent evaporation, for example, by close control of the humidity or using an overlayer of an immiscible liquid, will be required. [Pg.13]

The term electrode is widely used in electrochemistry. However, it designates objects that can significantly vary depending on the situation. For the purposes of this document, in examples chosen to illustrate simple electrochemical systems, the term will most often refer to the metal which constitutes one of the terminals in the system in question. For instance, a platinum electrode or a copper rotating disc electrode will be mentioned. When the system includes more than three materials, then the term electrode usually refers to the whole set of successive materials inserted between the metallic ending and the electrolyte material which makes up the core of the system. For instance, the term modified electrode will be used to refer to a metal whose surface has been covered with a film of conducting material or the term positive electrode in a battery will be used to refer to the composite material which is in contact with the electrolyte. In a third context, the term electrode will be used for an electrochemical half-cell this is the case with the electrode or reference electrode. In the final version of its meaning, the term electrode even stands for two half-cells combined to form the device, e.g., in the case of commercial systems for pH measurements by means of a combined electrode... [Pg.23]

EPR spectrometers use radiation in the giga-hertz range (GHz is 109 Hz), and the most common type of spectrometer operates with radiation in the X-band of micro-waves (i.e., a frequency of circa 9-10 GHz). For a resonance frequency of 9.500 GHz (9500 MHz), and a g-value of 2.00232, the resonance field is 0.338987 tesla. The value ge = 2.00232 is a theoretical one calculated for a free unpaired electron in vacuo. Although this esoteric entity may perhaps not strike us as being of high (bio) chemical relevance, it is in fact the reference system of EPR spectroscopy, and thus of comparable importance as the chemical-shift position of the II line of tetra-methylsilane in NMR spectroscopy, or the reduction potential of the normal hydrogen electrode in electrochemistry. [Pg.11]

We call the electrode of interest - that at which the electrochemical changes of interest occur - the working electrode (WE). When we cite an overpotential, we cite the potential of the working electrode with respect to the potential of the reference. The overpotential t] is seen to be positive during anodic electrochemistry and negative during cathodic electrode processes. [Pg.133]

A schemahc diagram of the DEMS apparatus is shown in Fig. 5. The electrochemistry compartment corrsists of a circular block of passivated htanirrm (a) that rests above a stainless-steel support (1) cormected to the mass spectrometer. The space between the cell body and the snpport is a Teflon membrane (j) embedded on a steel mesh (k) the membrane is 75 pm thick, has 50% porosity and pore width of 0.02 pm. The single-crystal disk (h) is the working electrode its face is in contact with the electrolyte solution and separated from the cell body by another Teflon membrane (i) that functions as a spacer to form a ca 100-pm thick electrolyte layer (j). Stop-flow or continnons-flow electrolysis can be performed with this arrangement. For the latter, flow rates have to be minimal, ca 1 pL/s, to allow ample time (ca 2 s) for the electrogenerated products to diffuse to the upper Teflon membrane. Two capillaries positioned at opposite sides of the cell body (b, e) serve as electrolyte inlet and outlet as well as connection ports to the reference (f) and two auxiliary Pt-wire electrodes (d, f). [Pg.285]

In 1941 Albert Szent-Gyorgyi suggested the role of solid-state electronic processes in biology (for a review, see references 2 and 24-27). Many attempts have been made during the intervening years to demonstrate that such electronic processes can occur in biomembranes and their constituents such as proteins and lipids (see reference 24). The concept of electronic processes in membranes and related systems was first reviewed in 1971 (14, 28), and the phenomenon known as electrostenolysis was stressed. In this connection, the term electrodics has been proposed (10, 28). In the language of membrane electrochemistry, electrostenolysis simply means that a reduction reaction takes place on the side of the membrane (or barrier) where the positive electrode is situated and oxidation occurs on the other side... [Pg.507]

Fig. 15 Cyclic voltammogram for Cu UPD on a well-ordered Au(lll) electrode in 0.1 M H2SO4 - -1 mM CUSO4, scan rate 1 mV (reproduced from L Kibler, Preparation and Characterization of Noble Metal Single-Crystal Electrodes. Copyright 2000 by International Society of Electrochemistry), and electrochemically derived Cu coverage (normalized charge referring to one complete Cu UPD ML) as a function of potentiai, determined by potential steps in the positive direction. The Cu adlayer structures are also shown (adapted from Ref [360]). Fig. 15 Cyclic voltammogram for Cu UPD on a well-ordered Au(lll) electrode in 0.1 M H2SO4 - -1 mM CUSO4, scan rate 1 mV (reproduced from L Kibler, Preparation and Characterization of Noble Metal Single-Crystal Electrodes. Copyright 2000 by International Society of Electrochemistry), and electrochemically derived Cu coverage (normalized charge referring to one complete Cu UPD ML) as a function of potentiai, determined by potential steps in the positive direction. The Cu adlayer structures are also shown (adapted from Ref [360]).
In above two equations, rrij is an integer constant which takes values of -1, +1, and 0 for species R(z-i) Os and inert electrolyte species respectively if the reduction current is considered positive p refers to the thickness of the compact EDL Fq refers to the radius of electrode y is the ratio between the standard rate constant of ET reaction and the mass transport coefficient of the electroactive species. It can be seen that the current density, which is given in a dimensionless form through normalization with the limiting diffusion current density (i, and the electrostatic potential distribution appear simultaneously in the two equations. Equation 2.2 could be approximated to the PB equation at low current density, while Equation 2.3 would reduce to Eq. 2.4, which is the diffusion-corrected Butler-Volmer equation and has been used to perform voltammetric analysis in conventional electrochemistry, as exp(-Zj/ rcp/F)=1, that is, electrostatic potentials in CDL are close to zero. These conditions are approximately satisfied in large electrode systems, suggesting that the voltammetric behaviour and the EDL structure can be treated separately at large electrode interface ... [Pg.34]


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See also in sourсe #XX -- [ Pg.24 ]




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