Titlebook: Statistical Mechanics and Statistical Methods in Theory and Applications; Uzi Landman Book 1977 Springer Science+Business Media New York 1

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M. D. Srinivas,E. Wolfiserklärung berücksichtigt werden müssen. Kinder und Minderjährige können selbst keine Einverständniserklärung unterzeichnen. Während ältere Kinder durchaus in bestimmte Entscheidungen miteinbezogen werden sollten, müssen für Neugeborene, Kleinkinder und jüngere Kinder die Eltern bzw. Erziehungsbere

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Structure and Thermodynamics of Interfaces,r. In Figure 1 we see a hypothetical profile of the density p as a function of the distance z perpendicular to the interface, in liquid-vapor equilibrium. Such profiles constitute what we may call the . of the interface. We wish to determine this structure theoreticfally, and also the interfacial tension, and to relate the latter to the former.

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Scaled Particle Theory of Hard Sphere Fluids To 1976,ased on the application of the thermodynamics and statistical thermodynamics of curved boundary layers are reviewed. Recent work in which scaled particle theory is applied to the derivation of the radial distribution function is discussed. Finally, in the last section, some new results are reported.

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On the Iterative Solution of a Stochastic Mapping,this mapping is so simple that it could be studied on a pocket-calculator its analytic solution is not available. This is probably due to the fact that it . so successful in imitating the behavior of a “non- integrable” Hamiltonian system of differential equations.

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Optical Spectra Line Shape for Mixed Crystals,e crystals, while the line shift is as large as 30% of the phonon frequency. This fact does not have any reasonable explanation up to now. The reason is that there is no general theory of disordered systems applicable at arbitrary concentrations.

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Critical Points and Multicritical Points,but powerful theoretical concepts: nonclassical critical exponents, physical analogies (based on simplified theoretical models), and scaling theory. Ordinary critical points in fluids, fluid mixtures, magnets and superfluids are surveyed briefly. The geometry of critical or lambda lines and critical

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Structure and Thermodynamics of Interfaces,ynamic densities are not uniform, but rather vary continuously from the values they have in one of the bulk phases to the values they have in the other. In Figure 1 we see a hypothetical profile of the density p as a function of the distance z perpendicular to the interface, in liquid-vapor equilibr

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A Van Der Waals Fixed Point,dynamic and other properties in the neighborhood of a critical point or continuous phase transition [.]. In pursuing this interest it has been easy to lose sight of the fact that global features of many phase transitions are satisfactorily described by a physical picture which in the context of liqu