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Three-dimensional grid

Partial Least Squares (PLS) regression (Section 35.7) is one of the more recent advances in QSAR which has led to the now widely accepted method of Comparative Molecular Field Analysis (CoMFA). This method makes use of local physicochemical properties such as charge, potential and steric fields that can be determined on a three-dimensional grid that is laid over the chemical stmctures. The determination of steric conformation, by means of X-ray crystallography or NMR spectroscopy, and the quantum mechanical calculation of charge and potential fields are now performed routinely on medium-sized molecules [10]. Modem optimization and prediction techniques such as neural networks (Chapter 44) also have found their way into QSAR. [Pg.385]

Some approximations are required. First, the evaluation of the integral in Eq. (3.10) within the simulation box with periodic continuation conditions is approximated by a sum of local contributions. This sum is calculated over Np test points x. 1 < k < Np which are homogeneously distributed on a three-dimensional grid covering the entire simulation box and is given by ... [Pg.63]

In a crystal atoms are joined to form a larger network with a periodical order in three dimensions. The spatial order of the atoms is called the crystal structure. When we connect the periodically repeated atoms of one kind in three space directions to a three-dimensional grid, we obtain the crystal lattice. The crystal lattice represents a three-dimensional order of points all points of the lattice are completely equivalent and have the same surroundings. We can think of the crystal lattice as generated by periodically repeating a small parallelepiped in three dimensions without gaps (Fig. 2.4 parallelepiped = body limited by six faces that are parallel in pairs). The parallelepiped is called the unit cell. [Pg.7]

Whereas the first applications of the AFDF approach were based on a numerical combination of fuzzy fragment electron densities, each stored numerically as a set density values specified at a family of points in a three-dimensional grid, a more powerful approach is the generation of approximate macromolecular density matrices within the framework of the ADMA method [142-146]. A brief summary of the main steps in the ADMA method is given below. [Pg.70]

Gradient diffusion was assumed in the species-mass-conservation model of Shir and Shieh. Integration was carried out in the space between the ground and the mixing height with zero fluxes assumed at each boundary. A first-order decay of sulfur dioxide was the only chemical reaction, and it was suggested that this reaction is important only under low wind speed. Finite-difference numerical solutions for sulfur dioxide in the St. Louis, Missouri, area were obtained with a second-order central finite-difference scheme for horizontal terms and the Crank-Nicolson technique for the vertical-diffusion terms. The three-dimensional grid had 16,800 points on a 30 x 40 x 14 mesh. [Pg.219]

In the at-risk volume approach, a three-dimensional grid of detectors is installed to assure that the hazardous gas cloud can not exist without detection. [Pg.248]

Divide space according to a three-dimensional grid. [Pg.399]

In formalism, this is really no different than the classical situation just described, except that the electronic-charge distribution is continuous, as opposed to discretized, and the non-linear character of the equations introduces an iterative component to the SCRF procedure that goes hand in hand with permitting relaxation of the charge distribution. That being the case, the methods used to represent the reaction field are essentially the same as those used in the classical situation. For example, SCRF schemes solving for the reaction field on a three-dimensional grid have been described by both Chen et al. (1994) and Tannor et al. (1994). [Pg.400]

Although complete, fully polarizable QM/MM schemes are computationally demanding, a simplified version of this formalism was arguably the first QM/MM approach to be described (Warshel and Levitt 1976), and the method still sees some use today. The simplification involves replacing explicit, polarizable MM molecules with a three-dimensional grid of fixed, polarizable dipoles - each a so-called Langevin dipole (LD) as it is required to obey... [Pg.466]

June et al. (11) also performed MD calculations to characterize the dynamics of Xe in silicalite. A fixed lattice was assumed with potential parameters close to those used in previous MD studies. The potential between zeolite and guest was determined prior to the calculation over a three-dimensional grid spanning the asymmetric unit. From these grid points, the potential at any point in the lattice could be found by interpolation. Temperatures of 200, 300, and 400 K were imposed during the simulations, which ran for 1 ns. [Pg.13]

Temperatures, mass-loss rates and luminosities of 30 galactic Wolf-Rayet stars (24 WN, 6 WC) are derived by fitting the observed equivalent widths of He I A5876 and He II A5412 and the absolute visual magnitude. A three-dimensional grid (T -R -M) of model calculations provides the theoretical values. [Pg.141]

CoMFA begins with the consistent alignment of each molecule into a separate three-dimensional grid. Alignment of the molecules must be representative of the binding conformation and orientation of the compound with the target. Three-dimensional coordinates within the grid are then probed for both steric and electrostatic interactions with the... [Pg.315]

To visualize the three-dimensional structures of these microphases more clearly, the density of A-segments was measured on a three-dimensional grid. In the A-rich domains the density of A-segments is high ( 1), and in the B-rich domains this density is low ( 0). The dividing surface between the A-rich domains and the B-rich domains is now represented by the isosurface where the density is midway between these values, i.e., 0.5. [Pg.65]

All unit cells in a given crystal are identical in orientation and content. Each atom in the unit cell is related by translational symmetry to its counterparts in all unit cells. On connecting all such equivalent atoms by straight lines the three-dimensional grid defines individual unit cells geometrically, as shown two-dimensionally in Figure 6.11. In three dimensions the grid also... [Pg.235]

To follow to actually carry out a TSA simulation a three-dimensional grid, with grid interval of about 0.2 A (5 -106 equispaced points in (132)) is built and the Helmholtz energies at all grid points are computed. Before this can be done in practice, a value for (A2) must be found. Then, local minima and the crest surfaces must be found, using the procedures given in (130,132,165). To study the dynamics of the penetrant molecules on the network of sites a Monte-Carlo procedure is employed, which is presented is some detail in (97). [Pg.149]

FIGURE 18 Three-dimensional grid plots for the S values (derived according to Eq. 9) of the polypeptide isomers, the all L-a-polypeptide, I, NH2 - DDALYDDKNWDRAPQRCYYQ-COOH (A) and (C), and its all D-a-retro-inverso isomer, 2, NH2- QYYCRQPARDWNKDDYLADD- COOH (B) and (D) as the temperature and organic solvent modifier. Data from Ref. 62. [Pg.144]

The network comprises W(IV) ions, which are connected to nearest neighbour Fe(II) ions through cyanide bridges in a three-dimensional grid-like arrangement. The Fe(II) ions are in an octahedral environment, bonded to four nearest neighbour W(IV) ions two axial water molecules complete the sixfold coordination. [Pg.300]

The MIFs obtained from qrtochrome enzymes are subsequently transformed and simplified as shown in Fig. 12.4. A three-dimensional grid map (3D map) may be viewed as a 3D matrix that contains forces of attraction and repulsion between a chemical probe and a protein. A 3D map is an image of the CYP-probe molecular interactions in which each pixel contains information about the cartesian coordinates and a physicochemical interaction. In cytochrome, where a catalytic reaction has to take place, all the 3D map information can be compressed and refers to the... [Pg.280]

Table 1 Time Complexity for Two- and Three-Dimensional Grid-Based Solution of the Time-Dependent Schrodinger equation s- rs... Table 1 Time Complexity for Two- and Three-Dimensional Grid-Based Solution of the Time-Dependent Schrodinger equation s- rs...

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See also in sourсe #XX -- [ Pg.75 ]

See also in sourсe #XX -- [ Pg.340 ]




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Molecules three-dimensional point grid

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