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Van der Walls interactions

Finally, the parametrization of the van der Waals part of the QM-MM interaction must be considered. This applies to all QM-MM implementations irrespective of the quantum method being employed. From Eq. (9) it can be seen that each quantum atom needs to have two Lennard-Jones parameters associated with it in order to have a van der Walls interaction with classical atoms. Generally, there are two approaches to this problem. The first is to derive a set of parameters, e, and G, for each common atom type and then to use this standard set for any study that requires a QM-MM study. This is the most common aproach, and the derived Lennard-Jones parameters for the quantum atoms are simply the parameters found in the MM force field for the analogous atom types. For example, a study that employed a QM-MM method implemented in the program CHARMM [48] would use the appropriate Lennard-Jones parameters of the CHARMM force field [52] for the atoms in the quantum region. [Pg.225]

D.D. Richardson, A calculation of Van der Walls interactions in and between layers of atoms application to graphite. J.Phys. C Solid State Phys., 10 (1977) 3235-3242. [Pg.317]

We treat the case in which the number density of molecules within the surface layer is negligibly small compared to that in the particle core. The van der Walls interaction energy is dominated by the interaction between the particle cores, while the contribution from the surface charge layer can be neglected. Thus, we have (from Eq. (19.31))... [Pg.426]

There is some experimental evidence to support this view we have made observations on a system in which a silane surfactant (octadecyltriethoxysilane) was applied to the fused silica, rather than the PTFE. Here vacuumr-deposited CBOOA showed invariably parallel alignment. In contrast, use of the same surfactant in a bulk sample showed perpendicular (homeotropic) alignment under the microscope. As the van der Walls interaction is expected to produce perpendicular alignment (Richmond and White), its dominance in the bulk only could explain the observations. [Pg.23]

Flory et al. (1964ab) applied a partition function of the same form but with van der Walls interaction potential, which is a specific case of Lennard-Johns potential at m = 3 and n —> oo. For N molecules of an r-mer, the partition function is... [Pg.472]

The authors are of the view that the adsorption of acetaminophen involved van der Walls interactions and the adsorbed molecnle had a flat conhguration. The adsorption of N-acetylcysteine, however, showed different conhgnrations of the molecnles depending on the pH of the solution. Furthermore, the adsorption of N-acetylcysteine was more at pH = 1.2 than at pH = 7. [Pg.429]

Like all polymeric structures, keratin fibres consist of long, tightly bound molecular chains held together in many different ways from covalent bonds to weaker interactions such as hydrogen bonds, Coloumbic interactions, van der Walls interactions and, when water is present, hydrophobic bonds. Hair reactivity is complex and depends not only on the presence of reactive groups in the fibre, but also on their availability. The latter is significantly affected by fibre morphology and molecular structure [2]. Hair is mostly proteinaceous in nature, while structural hpids and other materials represent only a minor fraction of its constituents. [Pg.123]

Fig. 4 Architecture of the chalcone O-methyltransferase isoflavone (a) and O-methyltransferase (lOMT) (b) active sites. Structural analysis shows that the tertiary structures of these enzymes are highly conserved substrate selectivity is determined by variations in side chains on the active site surface that alter van der Walls interactions and hydrogen bonding patterns (From [32])... Fig. 4 Architecture of the chalcone O-methyltransferase isoflavone (a) and O-methyltransferase (lOMT) (b) active sites. Structural analysis shows that the tertiary structures of these enzymes are highly conserved substrate selectivity is determined by variations in side chains on the active site surface that alter van der Walls interactions and hydrogen bonding patterns (From [32])...
A very useful application of the formula above of the energy of the quantum oscillator resides in calculation of the energy of the weak intramolecular van der Walls interaction, specific of the biatomic molecules of noble gases (with the typical case of the molecule). Assuming a unidimensional model, or two atoms of Helium, each of them with the two valence electrons (say nos. 1 2), oscillating in the nuclei positive potential field. Then, the potential energy exerted by a system over the other (the nuclei are considered as fixed and separated at the R distance) will be (Putz, 2006) ... [Pg.99]


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See also in sourсe #XX -- [ Pg.216 ]




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