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Structural properties of materials

Structural properties of materials Sub-lattice Substrate Surface phonoas Surface defects m transition metals Surface segregation SupeqDlastic properties and lic[uid phase effect Susceptibility... [Pg.516]

What does an atom experience in an encounter with another atom The nucleus, which contains most of the atom s mass, is confined to a tiny volume. Electrons, on the other hand, are spread out through space. Therefore, a collision between two atoms is a collision of their electron clouds. The electron clouds repel each other but are attracted by the nuclei. Chemists describe molecular structure, properties of materials, and chemical reactions in terms of how electrons respond to these electrical forces. [Pg.437]

We should note that the Schrodinger equation is non-relativistic since we derived it from the non-relativistic expression for the energy eqn (2.26). The Dirac equation is the relativistic analogue that is based on the relativistic expression for the energy, namely eqn (26). It led directly to the novel concept of electron spin. Since the valence electrons, which control the cohesive and structural properties of materials, usually travel with velocity v c, they are adequately described by the Schrodinger equation. For the heavier elements, such as the lanthanides and actinides, relativistic effects can be included perturbatively when necessary. Photons, the quanta of the... [Pg.30]

E. F. Schubert, Delta-Doping of Semiconductors Electronic, Optical and Structural Properties of Materials and Devices... [Pg.188]

Ni-Mo and Ni-W carbides phases supported on mesostructured MCM-41 with polymeric carbon were prepared in order to give structural stability to support. Surfaces as well as the structural properties of materials were studied. XRD and TEM analysis showed a similar structure before and after the treatment although geometrical and periodicity arrangements decrease lightly. [Pg.47]

The Mossbauer (transmission and scattering) spectroscopy has been used for in-situ characterization of the micro structural properties of materials. For thick samples, the MS is done in reflection geometry. As shown in Table 4.1, the range with X-rays is ss 20 pm, but with conversion electrons (GEMS)... [Pg.206]

Bums, W. A. Structural Properties of Materials for NPR Primary Piping, HW-7167O. November 6, 1961. [Pg.406]

Department of Structural Properties of Materials The Technical University of Denmark, Building 307 DK-2800 Lyngby, Denmark... [Pg.283]

The structural properties of materials are usually evaluated by the X-ray diffraction analysis. However, the X-ray diffraction relies on coherent scattering from the spatial average of a large number of unit cells. It is, therefore, insensitive to subtle structural characteristics and symmetry changes. Therefore, X-ray diffraction analysis is just a measure of the global structure of nanocrystalline materials. To probe the local structure of nanocrystalline materials, other techniques that are sensitive to a local structure are indispensable. [Pg.237]

The Institute has many-year experience of investigations and developments in the field of NDT. These are, mainly, developments which allowed creation of a series of eddy current flaw detectors for various applications. The Institute has traditionally studied the physico-mechanical properties of materials, their stressed-strained state, fracture mechanics and developed on this basis the procedures and instruments which measure the properties and predict the behaviour of materials. Quite important are also developments of technologies and equipment for control of thickness and adhesion of thin protective coatings on various bases, corrosion control of underground pipelines by indirect method, acoustic emission control of hydrogen and corrosion cracking in structural materials, etc. [Pg.970]

Computational solid-state physics and chemistry are vibrant areas of research. The all-electron methods for high-accuracy electronic stnicture calculations mentioned in section B3.2.3.2 are in active development, and with PAW, an efficient new all-electron method has recently been introduced. Ever more powerfiil computers enable more detailed predictions on systems of increasing size. At the same time, new, more complex materials require methods that are able to describe their large unit cells and diverse atomic make-up. Here, the new orbital-free DFT method may lead the way. More powerful teclmiques are also necessary for the accurate treatment of surfaces and their interaction with atoms and, possibly complex, molecules. Combined with recent progress in embedding theory, these developments make possible increasingly sophisticated predictions of the quantum structural properties of solids and solid surfaces. [Pg.2228]

S. Modry and M. Svata, eds.. Pore Structures, Properties, and Materials, Proceedings of the International Symposium, Scademia, Prague, Czechoslovakia, 1974. [Pg.38]

W. G. Moffatt, G. W. Pearsall, andj. Wulff, The Structure and Properties of Materials, Vol. 1, John Wiley Sons, Inc., New York, 1964. [Pg.481]

In photoluminescence one measures physical and chemical properties of materials by using photons to induce excited electronic states in the material system and analyzing the optical emission as these states relax. Typically, light is directed onto the sample for excitation, and the emitted luminescence is collected by a lens and passed through an optical spectrometer onto a photodetector. The spectral distribution and time dependence of the emission are related to electronic transition probabilities within the sample, and can be used to provide qualitative and, sometimes, quantitative information about chemical composition, structure (bonding, disorder, interfaces, quantum wells), impurities, kinetic processes, and energy transfer. [Pg.29]

In 1964, two competing series of slender volumes appeared one, the Macmillan Series in Materials Science , came from Northwestern Morris Fine wrote a fine account of Phase Transformations in Comlen.ted Systems, accompanied by Marvin Wayman s Introduction to the Crystallography of Martensite Transformations and by Elementary Dislocation Theory, written by Johannes and Julia Weertman. The second series, edited at MIT by John Wulff, was entitled The Structure and Properties of Materials , and included slim volumes on Structure, Thermodynamics of Structure, Mechanical Behaviour and Electronic Properties. [Pg.518]

J. C. Seferis and L. Nicolais, (eds.). The Role of the Polymeric Matrix in the Processing and Structural Properties of Composite Materials, Plenum, New York (1983). [Pg.663]

Though in this paper we have used the relativistic KKR wave functions ets betsis functions, the present approach may be easUy realized within any existing method for calculating the electron states. This will allow the electronic properties of materials with complex magnetic structure to be readily calculated without loss of accuracy. The present technique, being most eflicient for the SDW-type systems, can be also used for helical magnetic structures. In the latter case, however, the spin-polarizing part of potential (18) should be appropriately re-defined. [Pg.149]

Thermodynamic, statistical This discipline tries to compute macroscopic properties of materials from more basic structures of matter. These properties are not necessarily static properties as in conventional mechanics. The problems in statistical thermodynamics fall into two categories. First it involves the study of the structure of phenomenological frameworks and the interrelations among observable macroscopic quantities. The secondary category involves the calculations of the actual values of phenomenology parameters such as viscosity or phase transition temperatures from more microscopic parameters. With this technique, understanding general relations requires only a model specified by fairly broad and abstract conditions. Realistically detailed models are not needed to un-... [Pg.644]

The properties of materials are consequences of their structures at the molecular level. Solids are the mainstays of technology, and it is hardly surprising that so much effort has gone into the development and understanding of their properties. We dealt with their electrical properties in Sections 3.13 and 3.14. Here we explore some of their other physical properties as well as the properties of the much softer materials known as liquid crystals. [Pg.323]

The scanning acoustic microscope is a powerful new tool for the study of the physical properties of materials and has been successfully used for imaging interior structures and for nondestructive evaluation in materials science and biology. [Pg.30]


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See also in sourсe #XX -- [ Pg.69 ]




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