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Introduction properties

Nonmineralized SGA flows freely, and is often known as sandy alumina because it easily covers the cryoflte bath of aluminum electrolysis cells (see Aluminum compounds, introduction). Properties typical of a sandy SGA are shown in Table 1. Aluminum smelting technology in the United States is primarily based upon sandy alumina. Older European smelting technology, however, is based upon a poor flowing, low bulk density, highly mineralized SGA called floury alumina, composed principally of a-Al O. ... [Pg.159]

L.R. Radovic, C. Sudhakar, (H. Marsh, E.A. Heintz, F. Rodriguez-Reinoso, eds.), Carbon as Catalyst Support Introduction, properties, and applications. In Introduction to Carbon Technologies, University of Alicante, Alicante, Spain, 1997. [Pg.230]

As alluded to in the introduction, properties of aromatic polyamides differ significantly from those of their aliphatic counterparts. This led the U.S. Federal Trade Commission to adopt the term aramid to designate fibers of the aromatic polyamide type in which at least 85% of the amide linkages are attached directly to two aromatic rings. [Pg.977]

For practical applications, not only the mechanical strength is important but also processing times, drying behavior, and, as mentioned in the introduction, properties of the AeroSand such as thermal conductivity, gas permeability, thermal decomposition, resistance to metal penetration, gas evolution, and baking behavior. All these parameters were investigated. [Pg.769]

Introduction Properties of Nanoscale Systrans and Classification of Nanocompoates... [Pg.81]

Material introduction Properties of the support Current status... [Pg.474]

Perfluoroalkyl derivatives have important technical uses, e.g. sulphonic acids as surfactants introduction of perfluoroalkyl groups confers useful properties on many drugs. [Pg.299]

The introduction of monomers containing polar groups such as tertiary amines, imidazoles, pyrrolidones, pyridines, etc., gives the polymer dispersant properties that will be discussed in the article on dispersant additives for lubricants. [Pg.357]

Russel W B, Seville D A and Schowalter W R 1989 Colloidal Dispersions (Cambridge Cambridge University Press) General textbook, emphasizing the physical equilibrium and non-equilibrium properties of colloids Shaw D J 1996 Introduction to Colloid and Surface Chemistry (Oxford Butterworth-Heinemann)... [Pg.2696]

All teclmologically important properties of semiconductors are detennined by defect-associated energy levels in the gap. The conductivity of pure semiconductors varies as g expf-A CgT), where is the gap. In most semiconductors with practical applications, the size of the gap, E 1-2 eV, makes the thennal excitation of electrons across the gap a relatively unimportant process. The introduction of shallow states into the gap through doping, with either donors or acceptors, allows for large changes in conductivity (figure C2.16.1). The donor and acceptor levels are typically a few meV below the CB and a few tens of meV above the VB, respectively. The depth of these levels usually scales with the size of the gap (see below). [Pg.2882]

Note the curious return property exhibited by the energy in the symplectic method this is a manifestation of the nearby Hamiltonian mentioned in the introduction (see [7, 18, 28]). [Pg.361]

The physical, chemical cind biological properties of a molecule often depend critically upo the three-dimensional structures, or conformations, that it can adopt. Conformational analysi is the study of the conformations of a molecule and their influence on its properties. Th development of modem conformational analysis is often attributed to D H R Bcirton, wh showed in 1950 that the reactivity of substituted cyclohexanes wcis influenced by th equatoricil or axial nature of the substituents [Beirton 1950]. An equcilly important reaso for the development of conformatiorml analysis at that time Wcis the introduction c analytic il techniques such as infreired spectroscopy, NMR and X-ray crystaillograph] which actucilly enabled the conformation to be determined. [Pg.473]

This is an introduction to the techniques used for the calculation of electronic excited states of molecules (sometimes called eximers). Specifically, these are methods for obtaining wave functions for the excited states of a molecule from which energies and other molecular properties can be calculated. These calculations are an important tool for the analysis of spectroscopy, reaction mechanisms, and other excited-state phenomena. [Pg.216]

In the introduction we noted that both Berzelius and Wohler were fascinated by the fact that two different compounds with different properties ammonium cyanate and urea pos sessed exactly the same molecular formula CH4N2O Berzelius had studied examples of similar phenomena earlier and invented the word isomer to describe different compounds that have the same molecular formula... [Pg.23]

Focuses on force field calculations for understanding the dynamic properties of proteins and nucleic acids. Provides a useful introduction to several computational techniques, including molecular mechanics minimization and molecular dynamics. Includes discussions of research involving structural changes and short time scale dynamics of these biomolecules, and the influence of solvent in these processes. [Pg.4]

Descriptive properties for a basic group of approximately 1400 inorganic compounds are compiled in Section 3. These follow a concise, revised introduction to inorganic nomenclature that follows the recommendations of the lUPAC published in 1990. In this section are given the exact atomic (or formula) weight of the elements accompanied, when available, by the uncertainty in the final figure given in parentheses. [Pg.1286]

Morawitz, H., Macromolecules in Solution, Interscience, New York, 1965. Richards, E. G., An Introduction to the Physical Properties of Large Molecules in Solution, Cambridge University Press, Cambridge, 1980. [Pg.582]


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See also in sourсe #XX -- [ Pg.2 ]




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