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Porous history

As a general rule, boiler section deposits initially are often soft and porous but are prone to become harder and more adherent as they age. Thus, the presence of hard, dense scales and deposits in a boiler indicates that deposition has been occurring for a considerable time. The deposition of scales often produces a layered effect similar to the rings of a tree, indicating periodic changes in the water chemistry and perhaps providing some clues as to the history of the deposits. [Pg.234]

The effective diffusivity depends on the statistical distribution of the pore transport coefficients W j. The derivation shows that the semi-empirical volume-averaging method can only be regarded as an approximation to a more complex dynamic behavior which depends non-locally on the history of the system. Under certain circumstances the long-time (t —> oo) diffusivity will not depend on t (for further details, see [191]). In such a case, the usual Pick diffusion scenario applies. The derivation presented above can, with minor revisions, be applied to the problem of flow in porous media. When considering the heat conduction problem, however, some new aspects have to be taken into accoimt, as heat is transported not only inside the pore space, but also inside the solid phase. [Pg.245]

Optical lithography, in compound semiconductor processing, 22 193 Optically active citronellol, 24 506 Optically transparent porous gel-silica, 23 75, 76 Optical materials nonlinear, 17 442-460 second-order nonlinear, 17 444—453 third-order nonlinear, 17 453-457 Optical memory, photochromic material application, 6 602 Optical microscopy, 16 467-487 history of, 16 467-469 in kinetic studies, 14 622 liquid immersion, 15 186 Optical mode density, 14 849, 850-852 Optical multichannel analyzers (OMAs), 23 143... [Pg.649]

Some opportunities of such approximations are well illustrated by considering two characteristic examples. The first example will be a dusty-gas model, where porous media is considered as one of components of a gas mix of huge molecules (or particles of a dust), mobile or rigidly fixed in space [249,252,253], Such a model allows a direct application of methods and results of kinetic theory of gases and is effectively applied to the description of mass transfer processes in PS. The history of such an approach, the origins of which can be found in the works by Thomas Graham (1830 to 1840) is considered in Ref. [249], Actually, the model was first proposed by James Maxwell (1860), further it was independently reported by Deryagin and Bakanov (1957), and then also independently reported by Evans, Watson, and Mason (1961 see Refs. [249,252]). [Pg.325]

The first part of the book documents the history, structure, chemistry, formulation and characterizations of zeolites in Chapters 1-4. The past 60 years have seen a progression in molecular sieve materials from aluminosilicate zeolites to micro-porous silica polymorphs, microporous aluminophosphate-based polymorphs, metallosihcate and metallophosphate compositions, octahedral-tetrahedral frameworks, mesoporous molecular sieves and, most recently, hybrid metal organic frameworks (MOFs). [Pg.625]

Figure 42. Impedance characteristics of porous LSM electrodes on YSZ, measured at zero bias and 945 °C in air, as a function of polarization history and processing conditions. U-11, U-12, and U-13 correspond to firing temperatures of 1100, 1200, and 1300 °C, respectively. Bold line initial impedance. Thin line impedance measured 2 min following cathodic polarization at 100 mA/cm for 30— 90 min. Dashed line impedance measured 30 min following cathodic polarization. (Reprinted with permission from ref 209. Copyright 1997 The Electrochemical Society, Inc.)... Figure 42. Impedance characteristics of porous LSM electrodes on YSZ, measured at zero bias and 945 °C in air, as a function of polarization history and processing conditions. U-11, U-12, and U-13 correspond to firing temperatures of 1100, 1200, and 1300 °C, respectively. Bold line initial impedance. Thin line impedance measured 2 min following cathodic polarization at 100 mA/cm for 30— 90 min. Dashed line impedance measured 30 min following cathodic polarization. (Reprinted with permission from ref 209. Copyright 1997 The Electrochemical Society, Inc.)...
Anions travel toward the anode to balance the charges of the Zn2+ ions formed by the oxidation of the zinc electrode. Cations travel toward the cathode, to replace the charges of the Cu2+ ions that have been deposited as copper metal. Ions move between the two compartments (through the porous cup) to prevent the buildup of electrical charge inside the cell compartments and to complete the electrical circuit. Daniell s and his contemporaries inspiration to separate the half-reactions physically changed the course of technological history by making available portable sources of electricity. [Pg.704]

The RF thermal plasmas are suitable tools for making oxide ceramic microspheres, either dense or hollow. The microstructure of the product can principally be influenced by the structure of feedstock materials and to a less extent by the plasma operating conditions. Highly porous raw materials and/or the presence of blowing agents facilitate formation of hollow spheres. By varying the process conditions, one can primarily affect the thermal history of particles, hereby the degree of evaporation. [Pg.224]

The electrical parameters, especially the conductivity, were investigated early in history of ZnO research. An overwiew over electronic properties of ZnO up to the end of the 1950s was given by Heiland et al. in 1959 [7]. Most of the early investigations up to about 1955 were performed on sintered polycrystalline ZnO samples [4,8], which suffered from the general problem of conduction in porous, inhomogeneous materials with a lower density compared with... [Pg.36]


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See also in sourсe #XX -- [ Pg.39 ]




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Brief History of Porous Electrode Theory

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