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Dynamics of materials

Schoenlein R W, Leeman W P, Chin A H, Volfbein P, Glover T E, Balling P, Zolotorev M, Kim K-J, Chattopadhayay S and Shank C V 1996 Femtosecond x-ray pulses at 0.4 A generated by 90° Thomson scattering a tool for probing the structural dynamics of materials Science 274 236-8... [Pg.1990]

Multiscaling and first-principles computational approaches to predict the structure and dynamics of materials given their atomistic or molecular composition... [Pg.56]

Using two generators, E and. S, provides more flexibility in the choice of variables. The behavior of the variables x under space transformation determines the matrix L. The information related to the dynamics of material describes the friction matrix M which is related to the transport coefficients. [Pg.684]

Pair-additive interactions continued to be used in most materials-related simulations for over 20 years after Vineyard s work despite well-known deficiencies in their ability to model surface and bulk properties of most materials. Quantitative simulation of materials properties was therefore very limited. A breakthrough in materials-related atomistic simulation occurred in the 1980s, however, with the development of several many-body analytic potential energy functions that allow accurate quantitative predictions of structures and dynamics of materials.These methods demonstrated that even relatively simple analytic interatomic potential functions can capture many of the details of chemical bonding, provided the functional form is carefully derived from sound physical principles. [Pg.210]

DYNAMICS OF MATERIALS AT THE NANOSCALE SMALL-MOLECULE LIQUIDS AND POLYMER FILMS... [Pg.191]

Our current development of eFF involves adding explicit electron exchange-correlation potentials, core pseudo-potentials, and extended support for systems with significant p- and d-character. Using eFF, we re now able to study the effect of highly excited electrons in the dynamics of material subjected to extreme conditions, including those described before, as well as other open problems in interfacial shock instabilities, radiation damage, to name a few. [Pg.25]

High CRS sensitivity allowed registering not only the essential but also fine changes in the structure and dynamics of materials caused by any external influences. [Pg.203]

When the valve is opened two competing processes take place. The first is one of material transfer from the column to the drum. This has the effect of reducing column pressure. The second, because of the bypass being opened, is one of heat transfer reducing the amount of vapour condensed and so increasing pressure. Because the dynamics of material transfer are generally faster than those of heat transfer we see the first of these effects. However the drum pressure rises quickly and the material transfer slows. The heat transfer process ultimately prevails and the pressure rises above that at which it was before the control valve moved. The amount of inverse behaviour depends on the relative dynamics of the two processes. On some columns it may not be noticeable on others it may be severe. [Pg.294]

Here, we focus our attention on phase separation in complex fluids that are characterized by the large internal degrees of freedom. In all conventional theories of critical phenomena and phase separation, the same dynamics for the two components of a binary mixture, which we call dynamic symmetry between the components, has been implicitly assumed [1, 2]. However, this assumption is not always valid especially in complex fluids. Recently, we have found [3,4] that in mixtures having intrinsic dynamic asymmetry between its components (e.g. a polymer solution composed of long chain-like molecules and simple liquid molecules and a mixture composed of components whose glass-transition temperatures are quite different), critical concentration fluctuation is not necessarily only the slow mode of the system and, thus, we have to consider the interplay between critical dynamics and the slow dynamics of material itself In addition to a solid and a fluid model, we probably need a third general model for phase separation in condensed matter, which we call viscoelastic model . [Pg.179]

A.M. Donald and B.L. Thiel, Structure and Dynamics of Materials in the Mesoscopic Domain, Proceedings of the Royal Society-Unilever Indo-UK Forum in Materials Science and Engineering, 4th, Pune, India, Dec. 8-12, 1997 (1999) 1. [Pg.25]


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See also in sourсe #XX -- [ Pg.191 , Pg.195 ]




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