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Cornille, H.
CEA Centre d'Etudes Nucleaires de Saclay, 91 - Gif-sur-Yvette (France). Inst. de Recherche Fondamentale (IRF)1985
CEA Centre d'Etudes Nucleaires de Saclay, 91 - Gif-sur-Yvette (France). Inst. de Recherche Fondamentale (IRF)1985
AbstractAbstract
[en] We review recent results obtained for inhomogeneous distributions, solutions of d > 1 dimensional non linear Boltzmann equations with both Maxwell particles intermolecular forces and outside forces. We find exact solutions with a structure similar to the homogeneous Bobylev-Krook-Wu distributions. However, on the one hand, unlike the Bobylev inhomogeneous solution which corresponds to a gas in expansion, here these solutions can relax towards absolute Maxwellians. On the other hand, we construct also a class of exact inhomogeneous distributions relaxing towards different oscillating Maxwellians. Two types of external forces are handled: linear spatial forces (mainly harmonic potentials) and linear velocity forces plus uniform source term
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Nov 1985; 7 p; R.C.P. 266 Meeting on inverse problems; Montpellier (France); 27-30 Nov 1985; SPHT--86-023
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Saad, S.M.; El-Guebeily, S.; Youssef, A.
National Centre for Radiation Research and Technology, Cairo (Egypt)1986
National Centre for Radiation Research and Technology, Cairo (Egypt)1986
AbstractAbstract
[en] The semi-empirical procedure, previously introduced by the authors for the determination of like and unlike interaction parameters from viscosity data, is extended to be applied to ordinary diffusion data. The L.J. (n-6) potentials, with n ranging from 7 to 90, are considered. The procedure is tested and proved successful for Ne, Ar, Xe, and their binary mixtures. The best values of n representing the interaction of these systems are found to be 11.8 (for Ne), 12.1 (for Ar), 11.6 (for Xe), 11.9 (for Ne-Ar), 12 (for Ne-Xe), and 12 (for Ar-Xe). These potentials are found to reproduce the experimental results satisfactorily to within 8%
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Journal Article
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Arab Journal of Nuclear Sciences and Applications; CODEN AJNAD; v. 19(1); p. 281-297
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AbstractAbstract
[en] From simple topological considerations on the molecular shapes, a new method for calculating the coefficients of the Girifalco intermolecular potential for various fullerenes is proposed. This eliminates the necessity for fitting the coefficients to data of measurements for each specific fullerene. We calculate them for C76 and C84 and apply this potential to perform research on the equilibrium of these fullerites with their vapors. The temperature dependence of the lattice parameters, the saturated vapor pressures and the enthalpies of sublimation is studied. Results are in good agreement with available experimental data. (orig.)
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22 refs.
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Journal Article
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European Physical Journal. B, Condensed Matter Physics; ISSN 1434-6028;
; v. 17(4); p. 629-633

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[en] This paper reviews the work performed under the direction of the author during the past 5-10 years and devoted to the spectral luminescence investigation of a new group of solvation (including relaxation) processes that are nonlinear in the field of the intermolecular forces. Physical models are proposed for the investigated solvation mechanisms, which are caused by the nonlinear interaction of constant and induced dipoles, and it is shown that the semiempirical theory based on them agrees quantitatively with experiment. Specific considerations are presented concerning the possibility of the practical utilization of these scientific results. 28 refs., 6 figs., 4 tabs
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Cover-to-cover Translation of Optiko-Mekhanicheskaya Promyshlennost (USSR); Translated from Opticheskii Zhurnal; 60: No. 11, 46-54(Nov 1993).
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Translation
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Curtis, R.A.; Steinbrecher, C.; Heinemann, M.; Blanch, H.W.; Prausnitz, J.M.
Ernest Orlando Lawrence Berkeley National Laboratory, Berkeley, CA (United States). Funding organisation: USDOE Director, Office of Science. Office of Basic Energy Studies. Division of Chemical Sciences (United States)2001
Ernest Orlando Lawrence Berkeley National Laboratory, Berkeley, CA (United States). Funding organisation: USDOE Director, Office of Science. Office of Basic Energy Studies. Division of Chemical Sciences (United States)2001
AbstractAbstract
No abstract available
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LBNL--47348; AC03-76SF00098; Available from Ernest Orlando Lawrence Berkeley National Laboratory, Berkeley, CA (US); Journal Publication Date: August 2, 2002
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Cieplak, Piotr; Dupradeau, Francois-Yves; Duan, Yong; Wang Junmei, E-mail: pcieplak@burnham.org2009
AbstractAbstract
[en] The focus here is on incorporating electronic polarization into classical molecular mechanical force fields used for macromolecular simulations. First, we briefly examine currently used molecular mechanical force fields and the current status of intermolecular forces as viewed by quantum mechanical approaches. Next, we demonstrate how some components of quantum mechanical energy are effectively incorporated into classical molecular mechanical force fields. Finally, we assess the modeling methods of one such energy component-polarization energy-and present an overview of polarizable force fields and their current applications. Incorporating polarization effects into current force fields paves the way to developing potentially more accurate, though more complex, parameterizations that can be used for more realistic molecular simulations. (topical review)
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S0953-8984(09)97101-6; Available from http://dx.doi.org/10.1088/0953-8984/21/33/333102; Country of input: International Atomic Energy Agency (IAEA)
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Bestehorn, Michael; Neuffer, Kai
Funding organisation: (US)2001
Funding organisation: (US)2001
AbstractAbstract
[en] We examine the fully nonlinear behavior of a thin liquid film in three spatial dimension for a large lateral extension. A partial differential equation is used for the spatiotemporal evolution of the height of the film. To take intermolecular forces in the liquid into account, we concentrate on a recently formulated model of Pismen and Pomeau, who derived an expression for the disjoining pressure only from the wetting properties of the fluid. Finally, the motion of a falling film on an inclined plane is studied within this model
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Othernumber: PRLTAO000087000004046101000001; 004131PRL
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Journal Article
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Physical Review Letters; ISSN 0031-9007;
; v. 87(4); p. 046101-046101.4

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Fornasiero, F.; Olaya, M.M.; Wagner, I.; Bruederle, F.; Prausnitz, J.M.
Ernest Orlando Lawrence Berkeley National Laboratory, Berkeley, CA (United States). Funding organisation: USDOE Director, Office of Science. Office of Basic Energy Studies. Division of Chemical Sciences (United States)2001
Ernest Orlando Lawrence Berkeley National Laboratory, Berkeley, CA (United States). Funding organisation: USDOE Director, Office of Science. Office of Basic Energy Studies. Division of Chemical Sciences (United States)2001
AbstractAbstract
No abstract available
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LBNL--48572; AC03-76SF00098; Available from Ernest Orlando Lawrence Berkeley National Laboratory, Berkeley, CA (US); Journal Publication Date: June 2002
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[en] Valence bond calculations of the potential energy surface of H+H2 have been done. In all the calculations the hydrogen molecule bond length was kept at 1.4 a0. The isotropic potential V0(r) and the leading anisotropic potential V2(R) were obtained. Our caclulated V0 is in good agreement with the experimentally determined V0 reported by Gengenbach, Hahn, and Toennies. Our calculations predict that the triangular arrangement of H2+H is favored over the linear configuration at long distances of R with alignment to the linear geometry at approximately 3.1 a0. A populaion analysis of our wavefunction is also presented
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Journal of Chemical Physics; v. 63(10); p. 4127-4132
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[en] Using material parameters determined by bulk behavior, and the lattice model presented previously by us, we study interfacial and thin-film phenomena in the mean-field approximation. The effects of free and solid surfaces on orientational ordering for the isotropic phase are found to depend on the details of the intermolecular interaction and, sufficiently far above the supercooling limit, the decay length is on the order of a molecular dimension. For some materials, we find smecticlike thin films at temperatures above the bulk nematic-isotropic transition, enhanced orientational ordering, and the possibility of multiple smecticlike phases
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Journal Article
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Phys. Rev., A; ISSN 0556-2791;
; v. 23(1); p. 305-315

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