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Continuum modeling approach

For the description of a solution of alanine in water two models were compared and combined with one another (79), namely the continuum model approach and the cluster ansatz approach (148,149). In the cluster approach snapshots along a trajectory are harvested and subsequent quantum chemical analysis is carried out. In order to learn more about the structure and the effects of the solvent shell, the molecular dipole moments were computed. To harvest a trajectory and for comparison AIMD (here CPMD) simulations were carried out (79). The calculations contained one alanine molecule dissolved in 60 water molecules. The average dipole moments for alanine and water were derived by means of maximally localized Wannier functions (MLWF) (67-72). For the water molecules different solvent shells were selected according to the three radial pair distributions between water and the functional groups. An overview about the findings is given in Tables II and III. [Pg.127]

Applications of continuum solvation approaches to MCSCF wavefunctions have required a more developed formulation with respect to the HF or DFT level. Even for an isolated molecule, the optimization of MCSFCF wavefunctions represents a difficult computational problem, owing to the marked nonlinearity of the MCSCF energy with respect to the orbital and configurational variational parameters. Only with the introduction of second-order optimization methods and of the variational parameters expressed in an exponential form, has the calculation of MCSCF wavefunction became routine. Thus, the requirements of the development of a second-order optimization method has been mandatory for any successful extension of the MCSCF approach to continuum solvation methods. In 1988 Mikkelsen el ol. [10] pioneered the second-order MCSCF within a multipole continuum model approach in a spherical cavity. Aguilar et al. [11] proposed the first implementation of the MCSCF method for the DPCM solvation model in 1991, and their PCM-MCSCF method has been the basis of many extensions to more robust second-order MCSCF optimization algorithms [12],... [Pg.88]

L. Bondesson, L. Frediani, H. Agren, B. Mennucci, Solvation of N3- at the water surface The polarizable continuum model approach. J. Phys. Chem. B 110, 11361 (2006)... [Pg.34]

R. Cammi, B. Mennucci, Structure and properties of molecular solutes in electronic excited states A polarizable continuum model approach based on the time-dependent density functional theory, in Radiation Induced Molecular Phenomena in Nucleic Acids A Comprehensive Theoretical and Experimental Analysis, ed. by M.K. Shukla, J. Leszczynski. Series Challenges and Advances in Computational Chemistry and Physics, vol 5 (Springer, Netherlands 2008)... [Pg.35]

A POLARIZABLE CONTINUUM MODEL APPROACH BASED ON THE TIME-DEPENDENT DENSITY FUNCTIONAL THEORY... [Pg.179]

It can therefore be concluded that irrespective of the precise boundary conditions, it is important to consider sub-continuum modeling approaches in the silicon layer. Notice that applying Fourier diffusion in the silicon channel layer leads to a substantial underprediction of the maximum hotspot temperature. [Pg.395]

The continuum scale is an intermediate range in terms of flow modelling, in that some methods are based on detailed or discrete modelling to predict average properties of dispersion, while others are based on continuum modelling approaches using aver-age/statistical descriptions of the aggregated properties of the canopy and the flow (see Table 2.7). [Pg.73]

Computational Modelling of the Solvent Effects on Molecular Properties An Overview of the Polarizable Continuum Model Approach (R. Cammi, B. Mennucci J. Tomasi)... [Pg.333]

The conceptual model in Figure 2, combined with a continuum model approach, is shown to be appropriate for the analysis of THM processes at the DST because the rock mass is highly fractured, forming a dense, wellfracture network for fluid flow. This differs from many other fractured rock sites in Canada, Europe, and Asia, where underground tests have been conducted in sparsely fractured crystalline rocks (Rutqvist and Stephansson, 2003). In those formations, fluid flow is dominated by a few widely spaced fractures, which means that a continuum approach may not apply on the drift scale. In relation to other fractured rock sites, the rock mass at Yucca Mountain is relatively homogenous (ubiquitously fractured), with much less variability in rock-mass mechanical and hydrological properties. [Pg.165]

A continuum model approach is appropriate for simulating relevant coupled THM processes at the DST. [Pg.166]

MD simulations using Tersoff- Brenner potential to simulate covalent bonds while using Lennard-Jones to model interlayer interactions 1.4 for armchair 1.2 for zigzag Evaluating the influence of surface effect resulting in relaxed unstrained deformation and in-layer nonbonded interactions using atomistic continuum modeling approach... [Pg.245]

In the continuum model approach, the two-dimensional temperature equation under the finite volume approach for the entire monolithic structure of the honeycomb catalytic combustor was solved in cylindrical coordinates ... [Pg.26]


See other pages where Continuum modeling approach is mentioned: [Pg.129]    [Pg.138]    [Pg.389]    [Pg.396]    [Pg.724]    [Pg.289]    [Pg.161]    [Pg.162]    [Pg.248]    [Pg.262]    [Pg.202]    [Pg.101]    [Pg.101]    [Pg.51]   


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