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Electronic conductor.

Carbon- or metal-particle-filled plastics are the basis of a number of well-established technologies they are mentioned here only for the sake of completeness, and the reader who wishes to explore this subject further is referred to the literature (10, 15). [Pg.130]


Electrochemistry is concerned with the study of the interface between an electronic and an ionic conductor and, traditionally, has concentrated on (i) the nature of the ionic conductor, which is usually an aqueous or (more rarely) a non-aqueous solution, polymer or superionic solid containing mobile ions (ii) the structure of the electrified interface that fonns on inunersion of an electronic conductor into an ionic conductor and (iii) the electron-transfer processes that can take place at this interface and the limitations on the rates of such processes. [Pg.559]

Only Ee O and y-Ee202 are considered to be protective films. Both are adherent and good electronic conductors. Alpha-Ee202, which forms in water and steam containing oxygen, is not adherent, is less protective, and is an insulator. EeO, which does not form at temperatures below 570°C, is nonprotective. [Pg.370]

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]

On the electrode side of the double layer the excess charges are concentrated in the plane of the surface of the electronic conductor. On the electrolyte side of the double layer the charge distribution is quite complex. The potential drop occurs over several atomic dimensions and depends on the specific reactivity and atomic stmcture of the electrode surface and the electrolyte composition. The electrical double layer strongly influences the rate and pathway of electrode reactions. The reader is referred to several excellent discussions of the electrical double layer at the electrode—solution interface (26-28). [Pg.510]

Fig. 1. Logarithmic scale of the electrical conductivities of materials categorized by magnitude and carrier type, ie, ionic and electronic, conductors. The various categories and applications ate given. The wide conductivity range for the different valence/defect states of Ti oxide is highlighted. MHD is... Fig. 1. Logarithmic scale of the electrical conductivities of materials categorized by magnitude and carrier type, ie, ionic and electronic, conductors. The various categories and applications ate given. The wide conductivity range for the different valence/defect states of Ti oxide is highlighted. MHD is...
Fig. 6. Schematic of band gap energy. Eg, for the three types of electronic and ionic conductors. For electronic conductors the comparison is made of the relative occupancy of valence and conduction bands. For ionic conductors, the bands correspond to the relative occupancy of ionic sublattices. For (a),... Fig. 6. Schematic of band gap energy. Eg, for the three types of electronic and ionic conductors. For electronic conductors the comparison is made of the relative occupancy of valence and conduction bands. For ionic conductors, the bands correspond to the relative occupancy of ionic sublattices. For (a),...
The anode material in SOF(7s is a cermet (rnetal/cerarnic composite material) of 30 to 40 percent nickel in zirconia, and the cathode is lanthanum rnanganite doped with calcium oxide or strontium oxide. Both of these materials are porous and mixed ionic/electronic conductors. The bipolar separator typically is doped lanthanum chromite, but a metal can be used in cells operating below 1073 K (1472°F). The bipolar plate materials are dense and electronically conductive. [Pg.2413]

Tetrathia- and tetraselenafulvalenes, polythiophenes and related compounds, polypyridines as organic electronic conductors 97YGK410. [Pg.218]

For the corrosion process to proceed, the corrosion cell must contain an anode, a cathode, an electrolyte and an electronic conductor. When a properly prepared and conditioned mud is used, it causes preferential oil wetting on the metal. As the metal is completely enveloped and wet by an oil environment that is electrically nonconductive, corrosion does not occur. This is because the electric circuit of the corrosion cell is interrupted by the absence of an electrolyte. Excess calcium hydroxide [Ca(OH)j] is added as it reacts with hydrogen sulfide and carbon dioxide if they are present. The protective layer of oil film on the metal is not readily removed by the oil-wet solids as the fluid circulates through the hole. [Pg.1336]

Since metals are electronic conductors, the anodic and cathodic reactions will not necessarily occur at the same site, and anodic and cathodic areas can develop as in aqueous solutions. For example, wash-line attack is often a feature of corrosion by fused salts in contact with air. [Pg.439]

When two different metals are immersed in the same electrolyte solution they will usually exhibit different electrode potentials. If they are then connected by an electronic conductor there will be a tendency for the potentials of the two metals to move towards one another they are said to mutually polarise. The polarisation will be accompanied by a flow of ionic current through the solution from the more negative metal (the anode) to the more positive metal (the cathode), and electrons will be transferred through the conductor from the anode to the cathode. Thus the cathode will benefit from the supply of electrons, in that it will dissolve at a reduced rate. It is said to be cathodically protected . Conversely, in supplying electrons to the cathode the anode will be consumed more rapidly, and thus will act as a sacrificial anode. [Pg.135]

For use in high resistivity soils, the most common mixture is 75% gypsum, 20% bentonite and 5% sodium sulphate. This has a resistivity of approximately 50 ohm cm when saturated with moisture. It is important to realise that carbonaceous backfills are relevant to impressed current anode systems and must not be used with sacrificial anodes. A carbonaceous backfill is an electronic conductor and noble to both sacrificial anodes and steel. A galvanic cell would therefore be created causing enhanced dissolution of the anode, and eventually corrosion of the structure. [Pg.159]

Numerous materials fall into the category of electronic conductors and hence may be utilised as impressed-current anode material. That only a small number of these materials have a practical application is a function of their cost per unit of energy emitted and their electrochemical inertness and mechanical durability. These major factors are interrelated and —as with any held of practical engineering—the choice of a particular material can only be related to total cost. Within this cost must be considered the initial cost of the cathodic protection system and maintenance, operation and refurbishment costs during the required life of both the structure to be protected and the cathodic protection system. [Pg.162]

Electrode an electron conductor by means of which electrons are provided for, or removed from, an electrode reaction. [Pg.1367]

Galvanic Cell an electrochemical cell having two electronic conductors (commonly dissimilar metals) as electrodes. [Pg.1369]

Electrolytic Conduction. The same treatment is easily applied to ionic conduction, if the plane AB in Fig. 1C is taken to be a plane in an electrolytic conductor, similar to the electronic conductor discussed above. In the absence of a field the number of negative ions which cross AB in unit time in one direction will not differ appreciably from the number that cross AB in the reverse direction and, treating the positive ions separately, we may make the same remark about the positive ions. [Pg.44]

Materials in which there is a substantial difference in energy between occupied and vacant MOs are poor electron conductors. Diamond, where the gap between the filled valence band and the empty conduction band is 500 kj/mol, is an insulator. Silicon and germanium, where the gaps are 100 kj/mol and 60 kj/mol respectively, are semiconductors. [Pg.655]

If these two electrodes are connected by an electronic conductor, the electron flow starts from the negative electrode (with higher electron density) to the positive electrode. The electrode A/electrolyte system tries to keep the electron density constant. As a consequence additional metal A dissolves at the negative electrode, forming A+ in solution and electrons e, which are located on the surface of metal A ... [Pg.4]

For increased power requirements, electrode constructions have been developed which bring the electronic conductors in closer contact with the active material particles first, around 1930, the sinter electrode [110], recently in sealed cells largely replaced by the nichel-foam electrode, and then, around 1980, the fiber structure electrode [111]. In order to take full advantage of their increased perform-... [Pg.283]

Lithium is isolated in a protective film [8]. During the deposition of lithium, the protective film may be heated locally by ion transport in the film itself. As a result of this local heating, part of the protective film (SEI) becomes an electronic conductor, and therefore lithium metal is deposited in the film. If local heating does not occur during stripping, the isolated lithium becomes electrochemically inactive. [Pg.343]

A quite different approach was introduced in the early 1980s [44-46], in which a dense solid electrode is fabricated which has a composite microstructure in which particles of the reactant phase are finely dispersed within a solid, electronically conducting matrix in which the electroactive species is also mobile. There is thus a large internal reactant/mixed-conductor matrix interfacial area. The electroactive species is transported through the solid matrix to this interfacial region, where it undergoes the chemical part of the electrode reaction. Since the matrix material is also an electronic conductor, it can also act as the electrode s current collector. The electrochemical part of the reaction takes place on the outer surface of the composite electrode. [Pg.375]

From Eq. (18) the concentration of electrons, and according to Eq. (11) the concentration of holes also, depend on the lithium activity of the electrode phases with which the electrolyte is in contact. Since anode and cathode have quite different lithium activities, the electronic concentration may vary to a large extent and an ionically conducting material may readily turn into an electronic conductor. [Pg.530]

Most electrochemical reactions occur at an interface between an electronic conductor system and an ionic conductor system. An interface has three components the two systems and the surface of separation. The electronic conductor stores one of the required chemicals electrons or wide electronic levels. The ionic conductor stores the other chemical needed for an electrochemical reaction the electroactive substance. A reaction occurs only if both components meet physically at the interface separating the two systems. [Pg.307]

Here we introduce a personal point of view about the interactions between conducting polymers and electrochemistry their synthesis, electrochemical properties, and electrochemical applications. Conducting polymers are new materials that were developed in the late 1970s as intrinsically electronic conductors at the molecular level. Ideal monodimensional chains of poly acetylene, polypyrrole, polythiophene, etc. can be seen in Fig. 1. One of the most fascinating aspects of these polymeric... [Pg.308]

At that time it was first reported that the catalytic activity and selectivity of conductive catalysts deposited on solid electrolytes can be altered in a very pronounced, reversible and, to some extent, predictable manner by applying electrical currents or potentials (typically up to 2 V) between the catalyst and a second electronic conductor (counter electrode) also deposited... [Pg.1]

II. Ease of electrical connection Here the main problem is that of efficient electrical current collection, ideally with only two electrical leads entering the reactor and without an excessive number of interconnects, as in fuel cells. This is because the competitor of an electrochemically promoted chemical reactor is not a fuel cell but a classical chemical reactor. The main breakthrough here is the recent discovery of bipolar or wireless NEMCA,8 11 i.e. electrochemical promotion induced on catalyst films deposited on a solid electrolyte but not directly connected to an electronic conductor (wire). [Pg.515]

Metals and semiconductors are electronic conductors in which an electric current is carried by delocalized electrons. A metallic conductor is an electronic conductor in which the electrical conductivity decreases as the temperature is raised. A semiconductor is an electronic conductor in which the electrical conductivity increases as the temperature is raised. In most cases, a metallic conductor has a much higher electrical conductivity than a semiconductor, but it is the temperature dependence of the conductivity that distinguishes the two types of conductors. An insulator does not conduct electricity. A superconductor is a solid that has zero resistance to an electric current. Some metals become superconductors at very low temperatures, at about 20 K or less, and some compounds also show superconductivity (see Box 5.2). High-temperature superconductors have enormous technological potential because they offer the prospect of more efficient power transmission and the generation of high magnetic fields for use in transport systems (Fig. 3.42). [Pg.249]


See other pages where Electronic conductor. is mentioned: [Pg.108]    [Pg.515]    [Pg.2409]    [Pg.2411]    [Pg.250]    [Pg.125]    [Pg.125]    [Pg.176]    [Pg.178]    [Pg.336]    [Pg.813]    [Pg.33]    [Pg.422]    [Pg.423]    [Pg.548]    [Pg.573]    [Pg.609]    [Pg.1]    [Pg.1]    [Pg.94]    [Pg.948]    [Pg.949]    [Pg.954]    [Pg.957]   
See also in sourсe #XX -- [ Pg.581 ]

See also in sourсe #XX -- [ Pg.267 ]




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CVD in Electronic Applications Conductors, Insulators, and Diffusion Barriers

Conductor band, electron movement

Conductor electronic/ionic

Conductor proton/electronic

Electrochemical techniques electronic conductor

Electrodes electronic conductor

Electron conductor

Electron conductor

Electron conductor membranes

Electron flow conductors

Electron transfer semi-conductors

Electron-conductor separating oil-water

Electronic and Electrolytic Conductors

Electronic conductor system

Examples of Defect Chemistry in Electronic and Mixed Conductors

Fluxes in a Mixed Proton and Electron Conductor

Fluxes in a Mixed Proton, Oxygen Ion, and Electron Conductor

Fluxes in a Mixed Proton, Oxygen Ion, and Electron Conductor Revisited

Junctions between Two Electronic Conductors

Metal and Electronic Conductor Properties

Mixed ionic-electronic conductor MIEC)

Mixed ionic-electronic conductors

Mixed ionic-electronic conductors MIECs)

Mixed proton—electron conductor

Scanning electron microscopy conductor

Solid mixed ionic-electronic conductors

Surface mixed proton-electron conductors

Thin films transparent electronic conductor

Transport mixed protonic-electronic conductors

Transport of ions and electrons in mixed conductors

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