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Diffraction techniques, physical

Figure 2.116 Work function Figure 2.116 Work function <D of an emersed gold electrode in UHV as a function of emersion potential (0.1 M HC104). Dashed lines indicate devalue for emersion at 0 V vs. NHE. From Kolb, Lehmpfuhl and Zci in Spectroscopic and Diffraction Techniques in Interfacial Electrochemistry. cds. C. Gutierrez and C. Mclendres. Nato ASI Scries. Series C Mathematical and Physical Sciences, Vol. 320, Chapter It, Kluwer Academic Publishers, Dordrecht, 1990.
Gutierrez, C. and Melendres, C. (1990) Spectroscopic and Diffraction Techniques in Interfacial Electrochemistry. Nato ASI Series, Series C Mathematical and Physical Sciences, Vol. 320, Kluwer Academic Publishers, Dordrecht. [Pg.232]

Whittig LD, Allardice WR. X-ray diffraction techniques. In Klute A (ed.), Methods of Soil Analysis Part 1 Physical and Mineralogical Methods, 2nd ed. Madison, WI American Society of Agronomy, Soil Science Society of America, and Agronomy Society of America 1986, pp. 331-361. [Pg.319]

Physical properties and detection of liquid Zintl compounds have been discussed and problems of gradual development of stoichiometries in non-clustering liquid ionic alloys, and their agreement with those persisting in the solid, have been considered. Neutron diffraction techniques and the results of their applications (Ga, Tl, alkali alloys) have been described. [Pg.85]

The physical properties of parent lithium cyclopentadienyl are those of a typical sait22-24 [MeLi]4 (1), it is insoluble in hydrocarbons, has a high melting point and a low volatility. Developments in powder diffraction techniques just recently enabled the structure determination of [CpLijoo (38). [Pg.63]

The last subject where time-resolved X-ray diffraction techniques proved their exceptional potential concerns chemical physics of gold nanoparticles in water. Belonging jointly to X-ray and nanoparticle physics, this subject is in a certain sense on the borderline of the present chapter [82-84]. Nevertheless, the possibilities offered by time-resolved X-ray techniques in this domain are fascinating. The heart of the problem is as follows. A suspension of gold... [Pg.22]

Like group theory, diffraction techniques ebb from and flow into physical chemistry courses. 1 think X-ray diffraction, at least, should be presented because it is so central to molecular biology and the steady state. Moreover, it provides an excellent opportunity for demonstrating the power of Fourier transforms in the understanding of physical phenomena. Indeed, it could be very interesting to develop a Fourier course that embraced diffraction and modem techniques of spectroscopy. [Pg.50]

X-ray diffraction has been a part of the physical chemistry laboratory curriculum for a long time, but mostly using the relatively simple powder diffraction technique. However a new experiment introduces the more complex method of single crystal X-ray diffraction (80). Another new experiment uses the technique to investigate the structure of alloys (81). [Pg.124]

In order to better understand the mechanism of antiwear functions it is essential to identify the compounds, as well as the elements, constituting the tribofilm. With the exception of XPS and X-ray diffraction techniques, all other physical techniques to date have focused on elemental analysis. Extended X-ray absorption, fine structure EXAFS and, in particular, X-ray absorption near-edge structure XANES techniques have, been shown to be very sensitive for structural and chemical speciation. The K-edge EXAFS spectroscopy has been used to study antiwear additives and tribofilms of some metals (Koningsberger and Prins, 1988 Martin et al., 1986a Belin et al., 1989). [Pg.121]

More directly, solid state physics contributed to the emergence of materials science, because of one of its foci. Spencer Weart identified three pillars on which solid state physics was erected First, X-ray diffraction techniques provided precise atomic picture of solids second, quantum mechanics provided the theoretical foundations for the description of solids and the third, more subtle pillar was the attempt to discriminate between properties depending on the idealized crystal pattern and properties dependent on accidents of either the inner arrangement or the surface of the solid. [13] This focus on structure-sensitive-properties can be seen as the main investigative pathway, to resume Frederic L. Holmes s concept, which lead to materials science. [Pg.261]

ZA is the charge on nucleus A, located at RA and p(r ) is the molecule s electronic density function. The sign of V(r) in any region depends upon whether the positive contribution of the nuclei or the negative one of the electrons is dominant there. It is important to note that V(r) is a physical observable, which can be obtained experimentally, by diffraction techniques [49, 50], as well as computationally. [Pg.155]

Sidhu, S. S., C. R. Heaton, and M. H. Matter Neutron Diffraction Techniques and Their Applications to some Problems in Physics. J. Appl. Phys. 30, 1323 (1959). [Pg.106]

Documentation exists in the literature as to the observation of anomalies in the temperature dependence of some physical properties of vanadium in the range 175-325 K. Although the anomaly was attributed by different workers to an antiferromagnetic transition, a small distortion of the body-centered cubic crystal structure, and impurities, Finkel et al. ( ) recently ascribed the anomaly to a second order phase transition at 230 K. Using low temperature x-ray diffraction techniques in the study of a single crystal of vanadium, Finkel et al. observed a decrease in crystal lattice symmetry form body-centered cubic (T > 230... [Pg.1827]

The particles comprising aquifer sediments range in size from sand (2-0.5 mm diameter (Allaby and Allaby, 1990) to colloid (between 1 nm and 1 xm in diameter (Stumm, 1992). Smaller-sized particles and/or those with complex shapes have a higher surface area-to-volume ratio and more reactive surface area (i.e., the fraction of total surface area that participates in interfacial reactions) per unit mass than larger, simply shaped particles (Parks, 1990). As a result, the smallest particles may dominate the overall mass transfer in aquifer sediments. These particles are commonly x-ray amorphous, meaning that their structure cannot be resolved using standard x-ray diffraction techniques. However, they are partially ordered, with crystalline domains typically < 15 A in diameter (Waychunas et al., 1996). Commonly, the smallest particles are also physically or chemically attached to the surface of larger particles. [Pg.28]

X-ray diffraction technique is a non-destructive analytical technique that reveals information about crystallographic structure, chemical composition and physical properties of nanostructured materials. UV/Vis spectroscopy is routinely used in the quantitative determination of films of nanostructured metal oxides. The size, shape (nanocomb and nanorods etc,) and arrangement of the nanoparticles can be observed through transmission electron microscope (TEM) studies. Surface morphology of nanostructured metal oxides can be observed in atomic force microscopy (AFM) and scanning electron microscopy (SEM) studies. [Pg.218]

It is relevant that attention should now be drawn to the recent work, by Patterson, Pyke, Reid, Tilley, McAteer, et al. (12-16), who have examined several aspects of the structural and catalytic character of coprecipitated tin-antimony oxides. The structure characterization by Pyke, Reid, and Tilley (12) by X-ray diffraction techniques clearly showed that bulk equilibrium is difficult to establish in this system. This observation alone places some earlier data in a different perspective and implicitly demands a high degree of caution in the interpretation of physical and spectroscopic data recorded from these materials. The phase diagram (Fig. 1) defines the... [Pg.102]

For some cases, it is possible to use refinement techniques (6) to obtain very accurate structural data. This is especially true for the well understood diffraction techniques and, therefore, for characterizations of polycrystalline material. With an increasing level of physical understanding the number of techniques which are suitable for use in refinement is bound to grow. Because of the local minimum problem, the starting model should already be close to reality for single-technique refinements. We expect that the... [Pg.196]


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Diffraction techniques

Diffraction techniques, physical chemistry course

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