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Current transfer

A ground with locally constant values of S and I in full space is regarded as conductor phase II. Therefore d0 = dU. A linear current density-potential function is assumed for the current transfer ... [Pg.550]

The e.m.f. would thus be 0.048 volt, and its sign would be such that the spontaneous current transfers HC1 from ethanol to water. This is the sign that the resultant e.m.f. of equimolal cells, placed back to back, is found to have the value, extrapolated to infinite dilution, is either 0.296... [Pg.221]

To further substantiate the proposed model, they have carried out some investigations connected with modification of semiconductor electron subsystem [174, 175]. Temperature is one of the important factors. Having no effect on the electron emission from the metal under the action of RGMAs, temperature strongly affects the current-transfer processes at the metal - semiconductor contacts. The impact of temperature on the interaction of RGMAs with Au/ZnO structures can be evaluated as follows. [Pg.335]

The value of t is the time taken to compensate for a charge arising at a metal particle as a result of its interaction with a metastable atom. This time can be evaluated within the scope of the theory of current transfer over the barrier [176] and in a first approximation it takes the form... [Pg.336]

FIGURE 1.19 Circuit diagram (upper panel) and current transfer ratio, I0jl (lower panel) of the polymer optocoupler. The photodiode was biased at —10 V. [Pg.25]

In the above expression, ci k is the concentration of species i in phase k, and si kj is the stoichiometric coefficient of species i in phase k participating in heterogeneous reaction 1 (see eq 8). is the specific surface area (surface area per unit total volume) of the interface between phases k and p. ih.k- is the normal interfacial current transferred per unit interfacial area across the interface between the electronically conducting phase and phase k due to electron-transfer reaction h, and it is positive in the anodic direction. In the above expression, Faraday s law... [Pg.451]

Figure 9 Voltage vs current and onset of resistance above the critical current for (A) "ideal case", (B) premature thermal runaway, (C) damaged sample, and (D) inadequate current transfer length between voltage and current taps as discussed for low temperature superconductors. Ref. 26. Figure 9 Voltage vs current and onset of resistance above the critical current for (A) "ideal case", (B) premature thermal runaway, (C) damaged sample, and (D) inadequate current transfer length between voltage and current taps as discussed for low temperature superconductors. Ref. 26.
The current transfer problem that had been identified with low temperature superconducting composites deserves additional mention for the high temperature superconductors, that in the bulk material are frequently not fully dense. Making the electrical connection in such a manner as to obtain uniform current distribution throughout the cross section of the material is difficult. The method described by Jin, et al. (24) with embedded wires or particles may provide for a significant improvement but the present techniques used to determine the critical current by a surface contact on the ceramic sample are subject to this problem. A discussion for the multifilamentary wire of NbsSn is provided by Goodrich and Fickett (30) and this discussion is likely to be similar to the high temperature materials that are not fully dense. [Pg.644]

Einer-Jensen, N. 1992. Counter-current transfer between blood vessels in the ovarian adnex. Acta Obstet Gynecol Scand 71 566. [Pg.433]

Designating the part of the total current transferred by cation as t+ and the part transferred by anion as < then dividing the equations (IV-2) an (TV-3) by (IV-l) we get the following important formulae ... [Pg.46]

Abstract Electron transmission through chiral molecules induced by circularly polarized light can be very different for mirror image structures. This behavior is described in terms of current transfer, the transfer of both charge and momentum. We review recent theoretical developments on the theory of current transfer and discuss related experimental studies of electron transmission through chiral molecular structures adsorbed on surfaces. [Pg.259]

Keywords Chiral control, Current transfer, Dephasing, Molecules, Junctions, Polarized laser pulses, Quantum model simulations... [Pg.259]

Steady-State Current Transfer with Dephasing. 274... [Pg.259]

Here, we review tight-binding models that account for the above-mentioned ET yield asymmetries in the context of the more general phenomenon of current transfer [38 -01. Current transfer is charge transfer where the transferred charge carrier maintains at least some of its linear and/or angular momentum (phase). A recent photoemission experiment [41] demonstrated current transfer a biased linear momentum distribution on a Cu (100) surface was established based on the angular distribution of the photoemitted current. [Pg.260]

The current transfer described here is a coherent phenomenon, sensitive to dephasing. To investigate environmental dephasing effects, we incorporate additional relaxation of coherences in the site representation of the Liouville equation for the system s density matrix (DM) p ... [Pg.264]

Fig. 4 Simple models of current transfer. In both models a driving current /d in wire D is transferred to wire A. In (a) the transfer is direct while in (b) it is mediated by a bridge wire B... Fig. 4 Simple models of current transfer. In both models a driving current /d in wire D is transferred to wire A. In (a) the transfer is direct while in (b) it is mediated by a bridge wire B...
Substantial current transfer asymmetry is indicated by the large asymmetry factors in Figs. 6 and 7 for both direct and bridge-assisted transfer. The calculated asymmetry factors are much smaller for short bridges. The steady-state scenario is different from the transient process considered in Sect. 3 where, for short pulses, reflection does not set in appreciably during the process lifetime. [Pg.273]

Figure 8 shows the current-transfer process in the DBA system for the off-resonance regime, EB > 0.03. In Fig. 8 the current transfer property decays quickly as we go into the off-resonance transfer regime. We find a strong exponential damping of the current transfer property expressed by the asymmetry factor A2. [Pg.274]


See other pages where Current transfer is mentioned: [Pg.87]    [Pg.185]    [Pg.73]    [Pg.130]    [Pg.106]    [Pg.24]    [Pg.150]    [Pg.642]    [Pg.642]    [Pg.80]    [Pg.266]    [Pg.189]    [Pg.87]    [Pg.97]    [Pg.91]    [Pg.259]    [Pg.260]    [Pg.261]    [Pg.263]    [Pg.265]    [Pg.267]    [Pg.267]    [Pg.268]    [Pg.269]    [Pg.271]    [Pg.271]    [Pg.271]    [Pg.273]    [Pg.273]    [Pg.274]    [Pg.275]   
See also in sourсe #XX -- [ Pg.259 , Pg.260 ]




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