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Potential switching curves

Fig. 20-5 Potential-time curves for a TiPt anode in the switching-off and switching-on phase (schematic) in the measurements in Ref. 7. Fig. 20-5 Potential-time curves for a TiPt anode in the switching-off and switching-on phase (schematic) in the measurements in Ref. 7.
FIGURE 12.11 Potential decay curves recorded after switching off the current (a) at short times (b) at long times. [Pg.206]

A second important aspect of electrochromism is the temporal response under alternating potentials ( 0.55 V). The DG showed sharp and distinct transitions between the colored/oxidized and bleached/reduced state across the entire visible spectrum (Fig. 6.10b). This time-resolved switching behavior was analyzed in more detail at A = 630 nm (Fig. 6.10c). The DG device showed short characteristic response times of 53 ms for the bleaching step and 63 ms for the reverse process, determined by fitting exponential functions to the switching curves. These short response times which are close to video rate (24 frames per second) are enabled by the short ion diffusion distance through the only >= 5 nm thick NiO nanotube wall. [Pg.130]

Figure 6.26 The flexoelectric effect in BaTiO (a) the evolution of the potential energy curve under a homogeneous stress and in a strain gradient (b) domain switching via mechanical stress imposed by a probe (Original data from Lu et al. (2012))... Figure 6.26 The flexoelectric effect in BaTiO (a) the evolution of the potential energy curve under a homogeneous stress and in a strain gradient (b) domain switching via mechanical stress imposed by a probe (Original data from Lu et al. (2012))...
Supramolecular complexes and assemblies are frequently held together by multiple weak noncovalent bonds. These bonds may be switched parallel or in series (Figure 4). While the depth of the minimum of the overall potential energy curve is identical, the distance along the reaction coordinate differs. [Pg.3484]

The convergence of two potential energy curves so as to allow an efficient switch of the nuclei between them is known as curve crossing. How can we know if curve crossing is possible The only guidance is either physical reasoning or an appeal to a proper quantum chemical computation or, post factum, from the nature of the observed results. [Pg.380]

FIGURE 1. SERS intensity versus a triangular sweep potential for the 1006-cm band of pyridine as a function of switching potential and scan rate. Solution 0.05 M pyridine and 0.1 M KCl. (a) Intensity versus potential (/-V) curves shows no hysteresis for a switching potential of -0.9 V versus SCE at a scan rate of 100 mV s. (b) /- V curve shows hysteresis is observed for a switching potential of -1.2 V versus SCE at a scan rate of 5 mV s V At slower scan rates, still more hysteresis develops. (c) 7-V curve shows no hysteresis for a switching potential of -1.2 V versus SCE at a scan rate of 500 mV s ... [Pg.268]

If in the potential range corresponding to the polarization curve the concentration of adsorbed azide radicals depended strongly on the potential (as was assumed by Thomas), we should observe high pseudocapacitance of the order of iUUO jjF cm on the curves for potential decay after the current has been switched off (this value of capacitance is obtained for the linear part of the charging curve presented in [371]). Actually, however, the capacity calculated from the slope of the initial section of the potential decay curve for T = 0 turned out to be equal to 70 )jF per square centimeter of the visible surface. [Pg.203]

Example For two atoms having point charges of 0.616 and -0.504 e and a constant dielectric function, the energy curve shows a switching function turned on (Ron) at a nonbonded distance of 10 A and off (Roff) at a distance of 14 A. Compare the switched potential with the abruptly truncated potential. [Pg.29]

The determination and evaluation of potentiodynamic curves can only be used as a preliminary assessment of corrosion behavior. The protection current requirement and the limiting value for the potential control can only be determined from so-called chronopotentiostatic experiments as in DIN 50918. in systems that react with spontaneous activation after the protection current is switched off or there is a change in the operating conditions, quick-acting protection current devices must be used. Figure 8-6 shows the circuit diagram for such a potentiostat. [Pg.477]

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.
Typical anodization curves of silicon electrodes in aqueous electrolytes are shown in Fig. 5.1 [Pa9]. The oxidation can be performed under potential control or under current control. For the potentiostatic case the current density in the first few seconds of anodization is only limited by the electrolyte conductivity [Ba2]. In this respect the oxide formation in this time interval is not truly under potentiostatic control, which may cause irreproducible results [Ba7]. In aqueous electrolytes of low resistivity the potentiostatic characteristic shows a sharp current peak when the potential is switched to a positive value at t=0. After this first current peak a second broader one is observed for potentials of 16 V and higher, as shown in Fig. 5.1a. The first sharp peak due to anodic oxidation is also observed in low concentrated HF, as shown in Fig. 4.14. In order to avoid the initial current peak, the oxidation can be performed under potentiodynamic conditions (V/f =const), as shown in Fig. 5.1b. In this case the current increases slowly near t=0, but shows a pronounced first maximum at a constant bias of about 19 V, independently of scan rate. The charge consumed between t=0 and this first maximum is in the order of 0.2 mAs cnT2. After this first maximum several other maxima at different bias are observed. [Pg.79]

Such anion adsorption can be prevented by chemisorbing a mono-layer of a strongly adherent thiol molecule to the Au surfaces [97,98]. 1-Propanethiol (PT) was used here because the gold nanotubules can still be wetted with water after chemisorption of the PT monolayer [97].t The Em versus applied potential curves for an untreated and PT-treated gold nanotubule membrane, with KBr solutions present on either side of the membrane, are shown in Fig. 13. The untreated membrane shows only cation permselectivity, but the permselectivity of the PT-treated membrane can be switched, exactly as was the case with the nonadsorbing electrolyte (Fig. 12). [Pg.29]

Transition-state switching may also occur in SACM, either for single-channel potential curves or for groups of channels such as in microcanonical variational versions with adiabatic channel states. [Pg.852]

To belabor this point, let us consider in more detail a simple case, Refs. [78, 79], where the bound states of the Coulomb potential, through successive switching of a short-range barrier potential, becomes associated with resonances in the continuum. The simplicity of the problem demonstrates that resonances have decisively bound state properties, yields insights into the curve-crossing problem, and displays the tolerance of Jordan blocks. The potential has the form... [Pg.61]


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