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Potential characteristic

The quality and quantity of sites which are capable of reversible lithium accommodation depend in a complex manner on the crystallinity, the texture, the (mi-cro)structure, and the (micro)morphology of the carbonaceous host material [7, 19, 22, 40-57]. The type of carbon determines the current/potential characteristics of the electrochemical intercalation reaction and also potential side-reactions. Carbonaceous materials suitable for lithium intercalation are commercially available in many types and qualities [19, 43, 58-61], Many exotic carbons have been specially synthesized on a laboratory scale by pyrolysis of various precursors, e.g., carbons with a remarkably high lithium storage capacity (see Secs. [Pg.386]

Very little can be concluded form the experimental results with respwt to theoretical current-potential characteristics in the dark and under illumination derived in the previous chapter. Since in none of these cases a complete i-U-curve was pubhshed or... [Pg.90]

The interfacial capacity is then obtained by calculating the profiles for various potential drops A0 and subsequent differentiation. Figure 7 shows several examples of capacity-potential characteristics for several widths of the interface. Obviously, the wider the interface, the higher the capacity. In all cases investigated it was higher than that calculated from the Verwey-Niessen model, in which ... [Pg.174]

Fig. 5.61 Current density-potential characteristics of n-semiconductor electrode in the dark and upon illumination... Fig. 5.61 Current density-potential characteristics of n-semiconductor electrode in the dark and upon illumination...
Figure 14. Cyclic voltammograms of /<2c-Re(bpy)(CO)3Cl in acetonitrile-0.1 M Bu4NPF6 at a Pt electrode.144 Scan rate 0.2 V/s. The lower voltammograms show the switching potential characteristics A and F, reversible one-electron wave B and D, redox couple due to a dimer of the complex C, the second metal-based wave. The upper curves show the effect of C02 on the voltammogram. See also Figure 15. Figure 14. Cyclic voltammograms of /<2c-Re(bpy)(CO)3Cl in acetonitrile-0.1 M Bu4NPF6 at a Pt electrode.144 Scan rate 0.2 V/s. The lower voltammograms show the switching potential characteristics A and F, reversible one-electron wave B and D, redox couple due to a dimer of the complex C, the second metal-based wave. The upper curves show the effect of C02 on the voltammogram. See also Figure 15.
Figure 3,55 Cyclic vollammograms of Re(Bipy)(CO)3CI in CH3CN/0.l M letrabutylammonium hexafluorophosphate as supporting electrolyte at a button Pt electrode, and with a sweep rate of 200 mV s (a) The switching potential characteristics of the coupled chemical reactions in the ahsence of C02. The lettered redox processes are discussed in the text. (b> The effect of saturating the solution with C02. From Sullivan et al. (1985). Figure 3,55 Cyclic vollammograms of Re(Bipy)(CO)3CI in CH3CN/0.l M letrabutylammonium hexafluorophosphate as supporting electrolyte at a button Pt electrode, and with a sweep rate of 200 mV s (a) The switching potential characteristics of the coupled chemical reactions in the ahsence of C02. The lettered redox processes are discussed in the text. (b> The effect of saturating the solution with C02. From Sullivan et al. (1985).
Diffusion Currents. Half-wave Potentials. Characteristics of the DME. Quantitative Analysis. Modes of Operation Used in Polarography. The Dissolved Oxygen Electrode and Biochemical Enzyme Sensors. Amperometric Titrations. Applications of Polarography and Amperometric Titrations. [Pg.8]

Figure 7.7 Current-potential characteristics for a redox reaction via the conduction band or via the valence band. The current was normalized by setting jo = 1- In this example the redox system overlaps more strongly with the conduction than with the valence band. Figure 7.7 Current-potential characteristics for a redox reaction via the conduction band or via the valence band. The current was normalized by setting jo = 1- In this example the redox system overlaps more strongly with the conduction than with the valence band.
Figure 7.9 Current-potential characteristics for an n-type semiconductor in the dark and under illumination. The difference between the two curves is the photocurrent. Figure 7.9 Current-potential characteristics for an n-type semiconductor in the dark and under illumination. The difference between the two curves is the photocurrent.
The current-potential characteristics of a redox reaction can thus be measured in the following way An overpotential rj is applied, and the current is measured for various rotation rates in. From a Koutecky-Levich plot the corresponding kinetic current jk(rj) is extrapolated. This procedure is repeated for a series of overpotentials, and the dependence of jk on rj is determined. [Pg.190]

The data shown in Figure 2.36 were gathered at constant current with a value of the current density that brought the electrode potential at the foot of the current-potential characteristic of the system. The concentration of substrate may thus be considered as constant. As discussed in Section 2.5, we consider only the case where the second electron transfer in the radical-substrate coupling pathway occurs at the electrode (ECE). The following equations and conditions apply. [Pg.422]

The oxidation of thioesters of phospho-rus(III) acids (S -ethyldiphenylphosphi-nite, S, S -diethylphenylphosphonite and triethylthiophosphite) in AN/NaCl04 occurs at potentials characteristic for thioethers with substituents other than for phosphorus(III) groups, which suggests the contribution of the lone pair of sulfur to the HOMO to be predominant. The process is thought to proceed via an intermediate cation radical with the number of electrons n varying from 0.65 to 0.85, which suggests a catalytic mechanism [12-15]. [Pg.239]

Figure 5.38 illustrates the experimental setup for water photoelectrolysis measurements with the nanotuhe arrays used as the photoanodes from which oxygen is evolved. The 1-V characteristics of 400 nm long short titania nanotuhe array electrodes, photocurrent density vs. potential, measured in IM KOH electrolyte as a function of anodization hath temperature under UV (320-400 nm, lOOmW/cm ) illumination are shown in Fig. 5.39. The samples were fabricated using a HF electrolyte. At 1.5V the photocurrent density of the 5°C anodized sample is more than three times the value for the sample anodized at 50°C. The lower anodization temperature also increases the slope of the photocurrent—potential characteristic. On seeing the photoresponse of a 10 V 5°C anodized sample to monochromatic 337 nm 2.7 mW/cm illumination, it was found that at high anodic polarization, greater than IV, the quantum efficiency is larger than 90%. Figure 5.38 illustrates the experimental setup for water photoelectrolysis measurements with the nanotuhe arrays used as the photoanodes from which oxygen is evolved. The 1-V characteristics of 400 nm long short titania nanotuhe array electrodes, photocurrent density vs. potential, measured in IM KOH electrolyte as a function of anodization hath temperature under UV (320-400 nm, lOOmW/cm ) illumination are shown in Fig. 5.39. The samples were fabricated using a HF electrolyte. At 1.5V the photocurrent density of the 5°C anodized sample is more than three times the value for the sample anodized at 50°C. The lower anodization temperature also increases the slope of the photocurrent—potential characteristic. On seeing the photoresponse of a 10 V 5°C anodized sample to monochromatic 337 nm 2.7 mW/cm illumination, it was found that at high anodic polarization, greater than IV, the quantum efficiency is larger than 90%.
Smith, J. R. (1968). Self-consistent many-electron theory of electron work functions and surface potential characteristics for selected metals. Phys. Rev. 181, 522-529. [Pg.401]

The experimental practice for the study of current/potential characteristics requires the formation of an ohmic contact on the back of the electrode. The simplest technique consists in the application of a very thin layer of Ga—In eutectic liquid alloy, which wets the surface easily. But in the most rigorous method used in production lines, a highly doped 750-nm... [Pg.308]

The formalism developed to describe current-potential characteristics for the Cd(II)/Cd(Hg) multistep electrode... [Pg.773]

There are several difficulties in the application of this technique to the analysis of sodium barrier properties of these polyimide films. First, as we have seen above, large shifts in the surface potential characteristics of MPOS structures can be associated with electronic conduction in the polyimide and charging of the polyimide-oxide interface. These shifts are not readily separable from any that might be caused by the inward drift of sodium ions. Second, the effect of the electronic charging process is to buck out the electric field in the polyimide which is needed to drive the ion drift mechanism. As seen in Figure 6, the electric field is reduced to very small values in a matter of minutes or less, particularly at the higher temperatures where ion drift would normally be measured. [Pg.161]

A solar cell was constructed from a p—fCH- film and a single crystalline n-Si wafer. The current-potential characteristic of the battery is shown in Fig. 20 73). A conversion efficiency of 4.3 % was obtained. The most sincere problem for poly-(acetylene) is its instability against air oxidation. If it could be solved, practical use of light weight and easily moldable solar cell from polymer films might be possible. [Pg.31]

One of the most important chronic alterations in the heart is the chronic phase after myocardial infarction. The postinfarction period is known to be associated with an increased risk for sudden cardiac death and for the occurrence of cardiac arrhythmia. Changes in conduction properties have been identified [Dillon et al., 1988], although the cells exhibit normal or near normal action potential characteristics [Wit and Janse, 1992]. Thus, cellular electrophysiology does not explain the complete pathophysiology of the arrhythmogenic substrate. Thus, other factors, for example structural changes and passive electrical properties, have to be taken into account. [Pg.79]

Although the entire discussion of electrochemistry thus far has been in terms of aqueous solutions, the same principles apply equaly well to nonaqueous solvents. As a result of differences in solvation energies, electrode potentials may vary considerably from those found in aqueous solution. In addition the oxidation and reduction potentials characteristic of the solvent vary with the chemical behavior of the solvent. as a result of these two effects, it is often possible to carry out reactions in a nonaqueous solvent that would be impossible in water. For example, both sodium and beryllium are too reactive to be electroplated from aqueous solution, but beryllium can be electroplated from liquid ammonia and sodium from solutions in pyridine. 0 Unfortunately, the thermodynamic data necessary to construct complete tables of standard potential values are lacking for most solvents other than water. Jolly 1 has compiled such a table for liquid ammonia. The hydrogen electrode is used as the reference point to establish the scale as in water ... [Pg.736]

However, it should not be surprising if the anodic and the cathodic Tafel plots do not intersect at E = Ecorr as the two reactions participating in the corrosion process are actually studied at potentials far removed from the corrosion potential. Moreover, it is not quite realistic to rely on the very simple model described here. Therefore, it appears more useful to record a complete current-potential characteristic and to attempt its interpretation in terms of simultaneous processes that can possibly be expected. Several practical examples have been extensively reviewed [93]. [Pg.275]

If the electrode reaction proceeds via a non-linear mechanism, a rate equation of the type of eqn. (123) or (124) serves as a boundary condition in the mathematics of the diffusion problem. Then, a rigorous analytical derivation of the eventual current—potential characteristic is not feasible because the Laplace transfrom method fails if terms like Co and c are present. The most rigorous numerical approach will be... [Pg.291]

Since natural waters are generally in a dynamic rather than an equilibrium condition, even the concept of a single oxidation-reduction potential characteristic of the aqueous system cannot be maintained. At best, measurement can reveal an Eh value applicable to a particular system or systems in partial chemical equilibrium and then only if the systems are electrochemically reversible at the electrode surface at a rate that is rapid compared with the electron drain or supply by way of the measuring electrode. Electrochemical reversibility can be characterized... [Pg.285]

Figure 8. Current-potential characteristics of CdSe/h + RbAgJs interface under chopped illumination (voltage scan rate 40 mV/s)... Figure 8. Current-potential characteristics of CdSe/h + RbAgJs interface under chopped illumination (voltage scan rate 40 mV/s)...
The conductivity of the sample 4, decreases by the formation of the cation vacancy clusters. In the case of 17.2 mol % Gd2(S0A)3 mixed sample( 5), the oT becomes higher at relatively lower temperature. However, the discontinuity exists at about 543 K and the conductivity becomes lower than that of the samples 1-3. From these results, the samples which maintain potential characteristics for the electrolyte are 1-3. [Pg.124]

Finally, unlike bronze, prime matter in both senses is devoid of primary actual (as opposed to potential) characteristics. For instance, both bronze as such and the bronze of such and such a statue are primarily hard. But, there is no primary actual characteristic of either prime matter as such or the prime matter of such and such a statue. So again, the naturelessness of prime matter is preserved. [Pg.47]

The concept of atomic operators is related to the question whether or not it is possible to define universal purely monoelectronic potentials characteristic of specific atoms. By universal is meant that the same atomic potential can be applied to a specific atom, carbon say, for a whole class of carbon-containing molecules. Potentials of this type should not include explicidy the wavefuncrions of the other electrons in the system, i.e., this approach is not subject to the iterative SCF solution method discussed above in connection with the HF theory. Calculations based on atomic operators are therefore rather fast. [Pg.17]


See other pages where Potential characteristic is mentioned: [Pg.404]    [Pg.275]    [Pg.419]    [Pg.417]    [Pg.127]    [Pg.64]    [Pg.89]    [Pg.121]    [Pg.123]    [Pg.317]    [Pg.109]    [Pg.193]    [Pg.119]    [Pg.11]    [Pg.77]    [Pg.731]    [Pg.212]    [Pg.272]    [Pg.292]    [Pg.391]    [Pg.395]    [Pg.45]   
See also in sourсe #XX -- [ Pg.46 , Pg.169 ]




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