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Titlebook: Observation, Prediction and Simulation of Phase Transitions in Complex Fluids; Marc Baus,Luis F. Rull,Jean-Paul Ryckaert Book 1995 Springe

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11#
發(fā)表于 2025-3-23 11:37:23 | 只看該作者
Liquid Crystal Interfacese triple point these three phases coexist, while the (first-order) coexistence line of the two fluid phases (liquid and gas) ends at a critical point. At temperatures higher than .. there is a single fluid phase.
12#
發(fā)表于 2025-3-23 16:04:58 | 只看該作者
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發(fā)表于 2025-3-23 20:21:12 | 只看該作者
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發(fā)表于 2025-3-24 00:22:02 | 只看該作者
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發(fā)表于 2025-3-24 02:29:55 | 只看該作者
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發(fā)表于 2025-3-24 08:57:17 | 只看該作者
Gibbs Ensemble Techniquesn of considerable interest to predict, as accurately as possible, the phase behavior of a simplified system containing the essential interactions of interest. Computer simulations are a natural choice for this purpose, as they allow complete freedom in specification of the potential model. However,
17#
發(fā)表于 2025-3-24 12:49:54 | 只看該作者
18#
發(fā)表于 2025-3-24 18:33:42 | 只看該作者
Simulations and Phase Behaviour of Liquid Crystalsuid crystal phase transitions and properties. Simulations sit between theory and experiment and, depending on the kind of model that is used, can contribute to either field. In principle, a fully realistic simulation of a specific molecular system could be compared directly with measurements made in
19#
發(fā)表于 2025-3-24 22:04:55 | 只看該作者
20#
發(fā)表于 2025-3-25 03:05:53 | 只看該作者
Dynamics of N-Nonadecane Chains in Urea Inclusion Compounds as seen by Incoherent Quasielastic Neutrith urea [1]. In these inclusion compounds, the hydrogen bonded network of urea molecules (hereafter called the host) contains essentially ‘infinite’, parallel tunnels of 5.2? approximate diameter (at room temperature) in which the .-alkane chains are trapped in an almost fully extended “all trans”
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