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Bonding parameters

One can start building up a list of MM3 parameters by use of the TINKER analyze command. Don t expect to build up the entire set, which occupies about 100 pages in the MM3 user s manual, but do obtain a few representative examples to get an idea of how a parameter set is constr ucted. From previous exercises and projects, you should have input and output geometries for an alkene, an alkane, and water. From these, the object is to determine the stretching and bending parameters for the C—C, C=C, C—H, and O—H bonds. The C—H bond parameters are not the same... [Pg.117]

The OPLS atom types are a superset of the AMBER united atom types and the bonding parameters are just those of AMBER, supplemented where needed by the OPLS developers. The bond stretch, angle bending, dihedral angle and improper dihedral angle terms are identical to those of AMBER. Unlike AMBER, different combination rules are used for the van der Waals parameters, no hydrogen bonding term is used and no lone pairs are used. [Pg.192]

The quality of bonding is related direcdy to the size and distribution of solidified melt pockets along the interface, especially for dissimilar metal systems that form intermetaUic compounds. The pockets of solidified melt are brittle and contain localized defects which do not affect the composite properties. Explosion-bonding parameters for dissimilar metal systems normally are chosen to minimize the pockets of melt associated with the interface. [Pg.147]

Presented in Table 1 is a list of the parameters in Eqs. (2) and (3) and the type of target data used for their optimization. The infonnation in Table 1 is separated into categories associated with those parameters. It should be noted that separation into the different categories represents a simplification in practice there is extensive correlation between the different parameters, as discussed above for example, changes in bond parameters that affect the geometry may also have an influence on AGsoivation for a given model compound. These correlations require that parameter optimization protocols include iterative approaches, as will be discussed below. [Pg.18]

Using the calculated phonon modes of a SWCNT, the Raman intensities of the modes are calculated within the non-resonant bond polarisation theory, in which empirical bond polarisation parameters are used [18]. The bond parameters that we used in this chapter are an - aj = 0.04 A, aji + 2a = 4.7 A and an - a = 4.0 A, where a and a are the polarisability parameters and their derivatives with respect to bond length, respectively [12]. The Raman intensities for the various Raman-active modes in CNTs are calculated at a phonon temperature of 300K which appears in the formula for the Bose distribution function for phonons. The eigenfunctions for the various vibrational modes are calculated numerically at the T point k=Q). [Pg.55]

Three other all-atom force fields have also received much recent attention in the literature MMFF94 [36-40], AMBER94 [9] and OPLS-AA [41, 42] and are becoming widely used. The latter two force fields both use non-bonded parameters which have been adjusted in order to reproduce experimental liquid phase densities and heats of vaporisation of small organic molecules. For example, OPLS-AA includes calculations on alkanes, alkenes, alcohols. [Pg.44]

Fig. 3. Selected bonding parameters (bond lengths in Angstroms, bond angles in degrees) of substituted iminophosphanes, 14... Fig. 3. Selected bonding parameters (bond lengths in Angstroms, bond angles in degrees) of substituted iminophosphanes, 14...
Fig. 4. Push-pull substituted diphosphanes, bonding parameters in Angstroms and degrees... Fig. 4. Push-pull substituted diphosphanes, bonding parameters in Angstroms and degrees...
Figure 11.12 Badly deformed bonded array of microchannels with poorly understood design and intermediate phase diffusion-bonding parameters. Figure 11.12 Badly deformed bonded array of microchannels with poorly understood design and intermediate phase diffusion-bonding parameters.
Apart from minor exceptions all other parameters are given the same values as in standard INDO (electroneguivities, Slater-Condon parameters, bonding parameters) or CNDO/S (one-centre repulsion integrals) methods. Two-centre repulsion integrals are usually evaluted by the Ohno-Klopman formula. [Pg.382]

Polar intermolecular interactions encoded in partition coefficients an indirect estimation of hydrogen-bond parameters of polyfunctional solutes. J. Phys. Chem. 1992, 96,1455-1459. [Pg.46]

Dearden,. C., Ghafourian, T. Hydrogen bonding parameters for QSAR comparison of indicator variables, hydrogen bond counts, molecular orbital and other parameters. J. Chem. Inf. Comput. Sci. 1999, 39, 231-235. [Pg.46]

Another extension of the E-state descriptors describes the bond parameters derived from intrinsic states. Bond E-state indices are based on intrinsic values that are the geometric mean of the atom intrinsic value [20] ... [Pg.90]

Short description of 3D H-bonding parameters and descriptors is included in... [Pg.134]

Three-dimensional H-bond Descriptors 135 Tab. 6.3 Three-dimensional H-bonding parameters and descriptors. [Pg.135]


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See also in sourсe #XX -- [ Pg.21 ]

See also in sourсe #XX -- [ Pg.292 ]

See also in sourсe #XX -- [ Pg.292 ]

See also in sourсe #XX -- [ Pg.97 ]




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Bond parameters

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