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Polycrystalline media

The electrical properties of a composite material composed of insulating media and conductive particles can always be modeled as a function of concentration or fraction of the conducting particles 4>. It was demonstrated in a modeling study of composite polycrystalline media composed of two typ>es of closed packed hard spheres [2], where the impedance structure of the system... [Pg.115]

FIGURE 7-2 A. Impedance (modulus) spectra for composite polycrystalline media with random distribution of conductive spheres (d> is a fraction of conductive medium) (continued on next page)... [Pg.116]

Historically, the bulk lubricant has been studied by dielectric spectroscopy and interpreted according to the Debye relaxation theory [3,4]. In impedance terms the system can also be represented according to a theory of colloidal dispersions or polycrystalline media composed of spheres of vastly different conductivities, where the contaminants become a more conductive phase suspended inside the less conductive additive/base oil matrix [6, 34]. Alternatively, when the contaminants are absent, the polar additives can be considered as a conductive discontinuous phase suspended inside insulating continuous base oil. Initially the description of the impedance representation of the fresh, uncontaminated oil will be provided, and then the effects of oxidative degradation and contaminants will be discussed. [Pg.228]

Parameter Carbon and low—medium aHoy steels High speed steels Cast cobalt alloys Carbides Cemented Coated Ceramics Polycrystalline cBN Diamond... [Pg.195]

The random laser is a simple optical system in which the strong optical scattering in the random medium forms an optical recurrent path. Recent reports on random lasers have described the emission of laser light by metal-oxide polycrystalline and micrometer-sized particles [46]. Because of its structural simplicity and small size, the single random laser is a promising miniature light source for optical devices, such as waveguides and optical switches. [Pg.214]

The chemical bath deposition of polycrystalline, zinc blende HgSe thin films on TO glass from aqueous alkaline medium has been reported [120]. Examples of electrodeposited ternary mercury compounds will be discussed in the next section. [Pg.106]

Lamy C, Leger JM, Clavilier J. 1982. Structural effects in the electrooxidation of methanol in alkahne medium. Comparison of platinum single crystal and polycrystalline electrodes. J Electroanal Chem 135 321-328. [Pg.203]

Papoutsis A, Leger JM, Lamy C. 1987. New results for the electrosorption of methanol on polycrystalline platinum in acid medium obtained by programmed potential voltammetry. J Electroanal Chem 234 315-327. [Pg.561]

An absolutely different situation occurs in case of polycrystalline adsorbent treated at high temperature in air or in other oxygen containing medium. In this case the volt-ampere analysis exhibits sharply nonlinear VAC, deviations from the Ohm law being observed at anomalously low fields [47]. This indicates an existence of high intracrystalline barriers in such adsorbents. These barriers can be attributed to crys-... [Pg.117]

CdSe CdSe was deposited on different substrates. The two-step method of the electrosynthesis of CdSe films, based on the initial chemical modification of polycrystalline gold surface with selenium overlayer was described [157]. In the second step, this overlayer was cathodically stripped as a Se in a Se(IV)-free electrolyte medium that was dosed with the requisite amounts of Cd(II) ions. [Pg.780]

Other Synthetic Materials. Many other natural gemstone materials have been duplicated in the laboratory on an experimental basis, often only in small sizes. Examples include tourmaline [1317-93-7], topaz [1302-59-6], and zircon [1490-68-2]. Of some potential is synthetic jadeite [12003-54-2], one of the two forms of jade. This crystallizes under medium pressure in polycrystalline form from an NaAlS Og glass (qv) and can be colored green by Fe or lavender by Mn (16). Many gemstone-like materials have been grown for technological purposes and such material is sometimes faceted. [Pg.218]

For a suitable doping, both effects compensate each other for some materials and lead to a broad turning point TP(e 1der/dT t=tp= 0) in the temperature dependence of er(T). As a second approach, polycrystalline mixtures of grains of different materials with opposite temperature coefficient of er lead to an effective medium with zero temperature coefficient. [Pg.106]

The presence of fluid inclusions in skeletal carbonates is not surprising. Liquid H20 serves as the medium of transport for Ca2+ and COo2 to the site of precipitation (1 7). Rapid growth of crystals in carbonate skeletons results in many twinning and growth dislocations, producing a polycrystalline material containing numerous voids (71, 72, 80, 85). [Pg.110]

The efficiency of solid-state reactions may also be decreased by degradation of the optical properties of the medium caused by accumulation of the product. This limitation is likely to be of concern in large crystalline samples where light must penetrate through reacted regions. From a preparative point of view this potential problem may be circumvented by using polycrystalline samples. [Pg.241]

Figure 2. Typical voltammogram of polycrystalline Pt in H1SO4 medium. Figure 2. Typical voltammogram of polycrystalline Pt in H1SO4 medium.
In this chapter, we overview first some recent examples of interfacial electrochemical ET of composite metalloproteins where molecular mechanistic detail has in some way been achieved. We discuss next some theoretical issues regarding in situ STM of large molecules, where resonance or environmentally activated tunnel channels are opened by the redox metal centre. This is followed by an overview of some recent achievements in the area of in situ STM/AFM of the single-metal proteins cytochrome c and azurin on polycrystalline and single-crystal platinum and gold surfaces. Such an integrated approach offers new perspectives for experimental and theoretical characterization of metalloproteins at solid surfaces in contact with the natural aqueous medium for metalloprotein function. [Pg.135]

Activation (of noble metal electrodes) — Noble metal electrodes never work well without appropriate pretreatment. Polycrystalline electrodes are polished with diamond or alumina particles of size from 10 pm to a fraction of 1 pm to obtain the mirror-like surface. The suspensions of polishing microparticles are available in aqueous and oil media. The medium employed determines the final hydrophobicity of the electrode. The mechanical treatment is often followed by electrochemical cleaning. There is no common electrochemical procedure and hundreds of papers on the electrochemical activation of -> gold and platinum (- electrode materials) aimed at a particular problem have been published in the literature. Most often, -> cyclic and - square-wave voltammetry and a sequence of potential - pulses are used. For platinum electrodes, it is important that during this prepolarization step the electrode is covered consecutively by a layer of platinum oxide and a layer of adsorbed hydrogen. In the work with single-crystal (- monocrystal) electrodes the preliminary polishing of the surface can not be done. [Pg.7]


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See also in sourсe #XX -- [ Pg.320 ]




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