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Geometries Parameters

The Universal Force Field, UFF, is one of the so-called whole periodic table force fields. It was developed by A. Rappe, W Goddard III, and others. It is a set of simple functional forms and parameters used to model the structure, movement, and interaction of molecules containing any combination of elements in the periodic table. The parameters are defined empirically or by combining atomic parameters based on certain rules. Force constants and geometry parameters depend on hybridization considerations rather than individual values for every combination of atoms in a bond, angle, or dihedral. The equilibrium bond lengths were derived from a combination of atomic radii. The parameters [22, 23], including metal ions [24], were published in several papers. [Pg.350]

Activation energy, i.e., the energy of the transition structure relative to reactants, can be observed experimentally. However, the only way that the geometries of transition structures can be evaluated is from theory. Theory also can give energetics and geometry parameters of short-lived reaction intermediates. [Pg.17]

The material index is based on hardness and geometry parameters. The serviee faetor takes into aeeount the driving and the driven equipment eharaeteristies. The AGMA 211 standard defines K as... [Pg.534]

All properties (energy, dipole moment, atomic charges) and geometry parameters (distance, angle, dihedral angle) can be animated or stepped through. [Pg.1273]

TABLE V. Geometry parameters and K, and K2 Values for 1000 psia (Nominal) Rod-Bundle Data ... [Pg.264]

In the case of stirred vessels the values A/riL can be calculated by the following equation using the geometry parameter d/D, H/D, the Newton number Ne, the Reynolds number Re = nd /v, the energy dissipation ratio e/e and the related macro scale A/d. For standard turbines e.g. Mockel [24] found the value A/d = 0.08 close to the impeller. Corresponding to this the maximum of the dissipation ratio ,/ has to be used which can be estimated by Eq. (20). [Pg.72]

H-bond acceptor from the carboxylic sensor of the host and also as donor making a C—H. .. O type of interaction possible. In such a way, a 7-membered closed ring is formed, classified in the schematical representation as type la. This aggregate shows strong binding of the solvent molecule to the host as judged from the geometry parameters (Table 16). [Pg.102]

In reality, extensive data by Medronho (Antunes and Medronho, 1992) indicate that the product Nst50NEu is not constant but depends on the ratio of underflow to feed (R) and the feed volumetric concentration (Cv) and NEu also depends on Cv as well as VRe. The Reitema and Bradley geometries are two common families of geometrically similar designs, as defined by the geometry parameters in Table 12-3 (Antunes and Medronho, 1992). [Pg.383]

The symbols with the subscript e are the actual equilibrium molecular geometry parameters. [Pg.166]

Propene and cis-butene-2 possess the molecular symmetries C2 and C2 v (28, 29), respectively. (Fig. 4 the geometry parameters given are derived from force field calculations (19, 30) and agree well with experiment.) The barriers // observed for the rotation of the methyl groups amount to 1.98 kcal mole-1 for propene (28), and 0.75 kcal mole-1 for cis-butene-2 (29). The torsional force constants K for the methyl groups... [Pg.172]

Bartell and coworkers investigated the structures of a series of noncyclic alkanes by means of gas electron diffraction (14, 44, 45) and invoked for the interpretation of their results a simple force field which contained to a high extent vibrational spectroscopic constants of Snyder and Schachtschneider. This force field reproduces bond lengths and bond angles of acyclic hydrocarbons well, energies of isomerisation satisfactorily. As an example, Fig. 8 shows geometry parameters of tri-t-butylmethane as observed by electron diffraction and calculated with this force field (14). [Pg.187]

Figure 1 shows schematically the structure of s-trans-1,3-butadicnc. Several studies show that proper geometry parameters are only obtained with a basis set of at least double-f quality, including polarization functions for carbon atoms. Table 1 presents a selection of the results obtained at several levels of calculation, using a basis set of this kind. [Pg.5]

Controlling variables in gas atomization of melts include nozzle geometry parameters and many process parameters. An exhaustive list of these parameters is given in Tables 2.12 and 2.13, respectively, along with typical values and/or ranges of the parameters. [Pg.85]

In water atomization, a number of operation variables are to be considered in order to properly control the process. The variables include geometry parameters, process parameters, and thermophysical properties of metal/alloy and water. Each design and configuration of an atomization unit are unique and thus only some specific operation conditions may be employed. Many of the variables are interrelated. Therefore, there may exist more than one set of optimum variable combinations for a given atomization unit. [Pg.93]

Table 2.14. Geometry Parameters in Water Atomization of Melts[145l... Table 2.14. Geometry Parameters in Water Atomization of Melts[145l...
The solution of the gas flow and temperature fields in the nearnozzle region (as described in the previous subsection), along with process parameters, thermophysical properties, and atomizer geometry parameters, were used as inputs for this liquid metal breakup model to calculate the liquid film and sheet characteristics, primary and secondary breakup, as well as droplet dynamics and cooling. The trajectories and temperatures of droplets were calculated until the onset of secondary breakup, the onset of solidification, or the attainment of the computational domain boundary. This procedure was repeated for all droplet size classes. Finally, the droplets were numerically sieved and the droplet size distribution was determined. [Pg.363]

In Fig. 6 we show how the electronic energies of the neutral and anionic systems vary along the C-S bond length with all other internal geometry parameters relaxed to minimize the neutral or anion energy, respectively. These plots allow us to examine where the anion s energy surface lies relative to that of the neutral, which obviously, is directly germane to attachment of a free electron to the a orbital of the C-S bond. [Pg.245]

The inclusion of correlation effects, as known, is inevitable. The importance of correlation has been pointed out for these structures as well. The geometry parameters used in the calculations were taken from an optimization procedure at the SCF level ((Kozmutza etah, 1995)). The complex is given in Figure 6. [Pg.65]

TABLE 6.4. Geometry Parameters of the Dihydrogen-Bonded Complex [NHsH ] - H-Be-H Optimized for the Equilibrium and Dynamic Structures in Eigure 6.6... [Pg.122]

From this equation it is evident that the maximum voltage depends on the square root of the maximum heat that can be dissipated, the conductivity of the buffer, and the two geometry parameters of the capillary, length L and diameter d. Equation (19) can be rewritten to yield an expression for /i iax ... [Pg.31]


See other pages where Geometries Parameters is mentioned: [Pg.2352]    [Pg.17]    [Pg.260]    [Pg.263]    [Pg.268]    [Pg.549]    [Pg.135]    [Pg.173]    [Pg.185]    [Pg.108]    [Pg.165]    [Pg.167]    [Pg.190]    [Pg.4]    [Pg.5]    [Pg.163]    [Pg.47]    [Pg.86]    [Pg.89]    [Pg.190]    [Pg.254]    [Pg.271]    [Pg.287]    [Pg.288]    [Pg.348]    [Pg.370]    [Pg.4]    [Pg.103]   
See also in sourсe #XX -- [ Pg.93 ]




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