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Conductive phase

When two conducting phases come into contact with each other, a redistribution of charge occurs as a result of any electron energy level difference between the phases. If the two phases are metals, electrons flow from one metal to the other until the electron levels equiUbrate. When an electrode, ie, electronic conductor, is immersed in an electrolyte, ie, ionic conductor, an electrical double layer forms at the electrode—solution interface resulting from the unequal tendency for distribution of electrical charges in the two phases. Because overall electrical neutrality must be maintained, this separation of charge between the electrode and solution gives rise to a potential difference between the two phases, equal to that needed to ensure equiUbrium. [Pg.510]

Electrical double layers are not confined to the interface between conducting phases. SoHd particles of active mass, or of conductive additives of... [Pg.510]

Equation (3-42) is not valid for conducting systems consisting of several conducting phases (e.g., steel pipeline in soil). Figure 3-15 shows an example for the measured results (3). [Pg.114]

Previous considerations have shown that the interface between two conducting phases is characterised by an unequal distribution of electrical charge which gives rise to an electrical double layer and to an electrical potential diflFerence. This can be illustrated by considering the transport of charge (metal ions or electrons) that occurs immediately an isolated metal is immersed in a solution of its cations ... [Pg.1249]

A third approach, not yet fully demonstrated at the limit of dispersed catalysts, is the induction of electrochemical promotion without an intermediate conductive phase (Fig. 12.3). This approach will be discussed in Section 12.3 in relation to the concept of the bipolar design. [Pg.518]

Most frequently platinum is used as electronically conducting phase of the hydrogen electrode, thus it is mentioned only when explicitly stated also in the original report. [Pg.120]

As outlined in chapter 1 the term electrode is used - contrary to the suggestion of W. Nemst - to designate the electronically conducting phase only, the term electrolyte solution covers all types of ionically conducting phases (solutions, melts, solids) being in contact with the former phase. [Pg.264]

The authors explain these high conductivities by an ion transport through a conducting phase consisting of a number of oxyethylene chains. Being obtained from polystyrene derivatives, these values also indicate that the flexibility of the backbone is not essential to achieve a high conductivity. [Pg.208]

The existence of Galvani potentials between two different conducting phases is connected with the formation of an electric double layer (EDL) at the phase boundary (i.e., of two parallel layers of charges with opposite signs, each on the surface of one of the contacting phases). It is a special feature of such an EDL that the two layers forming the double layer are a very small (molecular) distance apart, between 0.1 and 0.4nm. For this reason EDL capacitances are very high (i.e., tenths of pF/cm ). [Pg.25]

Equilibria at interfaces between conducting phases are dynamic every second a certain number of charges cross the interface in one direction, and an equal number of charges cross over in the other direction. Thus, even though the overall current is zero, partial currents constantly cross the interface in both directions, and we observe an exchange of charged particles between the two phases. [Pg.26]

Experimentally undefined parameters, which have a real physical meaning that is, they reflect an actual physical phenomenon but cannot be determined from the experimental data (even a thought experiment to measure them cannot be conceived) or by a thermodynamic calculation. In isolated cases such parameters can be calculated on the basis of nonthermodynamic models. The equations used for calculations generally contain sums, differences, or other combinations of such parameters that are measurable. The Galvani potential at the interface between two dissimilar conducting phases is an example. [Pg.35]

The four main phases involved in a field soil dissipation study are (I) planning and design phase, (II) field-conduct phase, (III) sample processing/analysis phase, and (IV) data handling/reporting phase. Each phase is vitally linked to the next and each is critical to study success. Results from an otherwise perfectly executed study may be made useless by uneven test substance application or improper sampling, sample handling, and/or analytical techniques. Each of these phases is discussed below. [Pg.841]

Measurement of electrical potential differences requires a complete electrical circuit, i.e., the electrochemical cell. An electrochemical galvanic cell consisting of all conducting phases, and among them at least one interface separating two immiscible electrolyte solutions is called for short a liquid galvanic cell. In contrast, the system composed of con-... [Pg.25]

The term interface will be distinguished from a related term, the interfacial region or interphase. This term denotes the region between the two phases where the properties vary markedly in contrast to those in the bulk of the phases. In the case of electrically conducting phases, charge distribution occurs in this region. [Pg.155]

Trasatti, S., and R. Parsons, Interphases in systems of conducting phases, Pure Appl. Chem., 55, 1251 (1983). [Pg.180]

This chapter will be concerned with the kinetics of charge transfer across an electrically charged interface and the transport and chemical processes accompanying this phenomenon. Processes at membranes that often have analogous features will be considered in Chapter 6. The interface that is most often studied is that between an electronically conductive phase (mostly a metal electrode) and an electrolyte, and thus these systems will be dealt with first. [Pg.256]

For example, the investigations of the current-generating mechanism for the polyaniline (PANI) electrode have shown that at least within the main range of potential AEn the "capacitor" model of ion electrosorption/ desorption in well conducting emeraldine salt phase is more preferable. Nevertheless, the possibilities of redox processes at the limits and beyond this range of potentials AEn should be taken into account. At the same time, these processes can lead to the fast formation of thin insulation passive layers of new poorly conducting phases (leucoemeraldine salt, leucoemeraldine base, etc.) near the current collector (Figure 7). The formation of such phases even in small amounts rapidly inhibits and discontinues the electrochemical process. [Pg.319]

The experimental procedure for conducting phase solubility analysis is rather simple it consists of mixing increasing amounts of sample with a fixed volume of solvent and then determining the mass of sample that has dissolved after each addition. It is not necessary to exceed the solubility limit of the analyte species, but attainment of this condition makes it easier to recognize trend within the plots. An experimental protocol for phase solubility analyses is available [39]. The data are most commonly plotted with the system composition (total mass of sample added per gram solvent) on the x axis, and the solution composition (mass of solute actually dissolved per gram of solvent) on the y axis. [Pg.334]

The addition of an ionic conductive phase, such as GDC, also promotes the elec-trocatalytic activity of an MIEC cathode. Hwang et al. [108] studied the electrochemical activity of LSCF6428/GDC composites for the 02 reduction and found that the activation energy decreased from 142 kJmol-1 for the pure LSCF electrode to 122 kJmol1 for the LSCF/GDC composite electrodes. Thus, the promotion effect of the GDC is most effective at low-operation temperatures (Figure 3.12). This is due to the high ionic conductivity of the GDC phase at reduced temperatures. [Pg.153]

To meet the requirements for electronic conductivity in both the SOFC anode and cathode, a metallic electronic conductor, usually nickel, is typically used in the anode, and a conductive perovskite, such as lanthanum strontium manganite (LSM), is typically used in the cathode. Because the electrochemical reactions in fuel cell electrodes can only occur at surfaces where electronic and ionically conductive phases and the gas phase are in contact with each other (Figure 6.1), it is common... [Pg.242]

MIEC with an additional ionically conductive phase, such as GDC or SDC, typically extends the electrochemically active region still further due to the higher ionic conductivity of GDC and SDC compared to that of the perovskites. The optimal composition of a two-phase composite depends in part on the operation temperature, due to the larger dependence of ionic conductivity on temperature compared to electronic conductivity. A two-phase composite of LSCF-GDC therefore has an increasingly large optimal GDC content as the operating temperature is reduced [14], A minimum cathode Rp for temperatures above approximately 650°C has been found for 70-30 wt% LSCF-GDC composite cathodes, while at lower temperatures, a 50-50 wt% LSCF-SDC composite cathode was found to have a lower Rp [15]. [Pg.244]

In addition to bilayered electrodes with a functional layer and a support layer, electrodes have also been produced with multilayered or graded structures in which the composition, microstructure, or both are varied either continuously or in a series of steps across the electrode thickness to improve the cell performance compared to that of a single- or bilayered electrode. For example, triple-layer electrodes commonly utilize a functional layer with high surface area and small particle size, a second functional layer (e.g., reference [26]) or diffusion layer with high porosity and coarse structure, and a current collector layer with coarse porosity and only the electronically conductive phase (e.g., reference [27]) to improve the contact with the interconnect. [Pg.249]

A similar infiltration method was used to form anodes with Cu-Co alloys as the electronically conducting phase, with Co added to enhance the anode catalytic activity without catalyzing carbon deposition [85], in contrast with Ni-Cu alloys, which were found to catalyze carbon deposition even when small quantities of Ni were present [86], The authors of the studies [84-86] have reported that the percolation of the infiltrated phases is incomplete following the processing of the cells, such that subsequent carbon deposition can actually serve to connect previously isolated islands of the metallic phase, thus increasing the electronic conductivity and decreasing Rs in the short term. Since carbon deposition was observed by the same authors to cause severe... [Pg.262]

Clinical trials are divided into four phases. These are Phase I to Phase IV (Fig. 6.1). These trials are conducted with specihc purposes to evaluate the safety and effectiveness of the drug in defined population groups. A recent proposal is to conduct Phase 0 —a microdosing trial on subjects. Exhibit 6.4 provides more details on this new topic. [Pg.181]

Distinguish the various phases of chnical trials, 1 to IV. Provide a reason for conducting Phase IV trials. [Pg.205]

The high temperature, a polymorph of Li2S04 has a very high Li" " ion conductivity, >1 Scm between 575 °C and the melting point, 870 °C. Many attempts have been made to dope Li2S04 and stabilise the highly conducting a polymorph to lower temperatures but these have met with limited success (Lunden, 1987) transformation to the low conductivity P polymorph, or other low conductivity phases, always occurs when the temperature decreases below 500 °C. [Pg.37]

So, in general when two conducting phases are brought into contact, an interphase electric potential vill develop. The exploitation of this phenomenon is one of the subjects of electrochemistry and we can define electrochemical reactions as ones in which... [Pg.227]


See other pages where Conductive phase is mentioned: [Pg.1960]    [Pg.200]    [Pg.517]    [Pg.557]    [Pg.270]    [Pg.400]    [Pg.410]    [Pg.331]    [Pg.331]    [Pg.17]    [Pg.168]    [Pg.229]    [Pg.321]    [Pg.503]    [Pg.355]    [Pg.250]    [Pg.271]    [Pg.271]    [Pg.171]    [Pg.791]    [Pg.367]    [Pg.491]    [Pg.182]    [Pg.226]   
See also in sourсe #XX -- [ Pg.171 ]




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Condensed-phase pyrolysis heat conduction

Conducting phases, interactions between

Conduction in the solid phase

Conductivity Measurements Across the Phase Boundary

Conductivity columnar phases

Conductivity phase transitions

Doping Influence on the Defect Structure and Ionic Conductivity of Fluorine-containing Phases

Electrical conductivity, columnar phases

Heat conduction with phase transition

Ionic conductivity background phases

Ionic conductivity, phase diagrams

Liquid-phase conductance

Lithium Conduction in NASICON-Related Phases

Phase behavior and conductivity

Phase diagrams crystallinity and conductivity

Phase transitions proton conductivity

Phonon Conductivity in Single-Phase Glasses

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