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Structure computational determination

It has been possible to determine transition structures computationally for many years, although not always easy. Experimentally, it has only recently become possible to examine reaction mechanisms directly using femtosecond pulsed laser spectroscopy. It will be some time before these techniques can be applied to all the compounds that are accessible computationally. Furthermore, these experimental techniques yield vibrational information rather than an actual geometry for the transition structure. [Pg.148]

Simply doing electronic structure computations at the M, K, X, and T points in the Brillouin zone is not necessarily sufficient to yield a band gap. This is because the minimum and maximum energies reached by any given energy band sometimes fall between these points. Such limited calculations are sometimes done when the computational method is very CPU-intensive. For example, this type of spot check might be done at a high level of theory to determine whether complete calculations are necessary at that level. [Pg.267]

Once a number of lead compounds have been found, computational and laboratory techniques are very successful in rehning the molecular structures to yield greater drug activity and fewer side elfects. This is done both in the laboratory and computationally by examining the molecular structures to determine which aspects are responsible for both the drug activity and the side effects. These are the QSAR techniques described in Chapter 30. Recently, 3D QSAR has become very popular for this type of application. These techniques have been very successful in the rehnement of lead compounds. [Pg.297]

For a conformation in a relatively deep local minimum, a room temperature molecular dynamics simulation may not overcome the barrier and search other regions of conformational space in reasonable computing time. To overcome barriers, many conformational searches use elevated temperatures (600-1200 K) at constant energy. To search conformational space adequately, run simulations of 0.5-1.0 ps each at high temperature and save the molecular structures after each simulation. Alternatively, take a snapshot of a simulation at about one picosecond intervals to store the structure. Run a geometry optimization on each structure and compare structures to determine unique low-energy conformations. [Pg.78]

Primary structure is determined, as we ve seen, by sequencing the pTotein. Secondary, tertiary, and quaternary structures are determined by X-ray crystallography (Chapter 22 Focus On) because it s not yet possible to predict computationally how a given protein sequence will fold. [Pg.1038]

With the molecular structure thus determined, NVR subtract the computed function 3m(s) from the total structure function [Eq. (3.6)] and obtain the distinct structure function 3 (s). The resulting curve is shown in Fig. 7 e. The function 3a (s) is related to the structure functions descriptive of atom pair interactions in D20(as) by Eq. (3.4). With the structure functions oo(s) known from X-ray diffraction, it is instructive to compute a neutron structure function. [Pg.133]

Researchers can use computer programs to test the geometry of many molecular structures and determine their suitability for specific applications. For example, a specialized screen saver can check the shape of hypothetical molecules based on their suitability for cancer treatment. Anyone can upload the screen saver and use a computer s idle time... [Pg.572]

Most of the unknown structures is determined from single crystal diffraction and refined from powder diffraction. Refinement is done with the Rietveld method, which is a least square fitting of the computed pattern to the measured one, while structure parameters are treated as the primary fitting parameters. This is in contrast to the procedure in pattern decomposition, which is outlined above (where not the structure parameters, but the peak intensities were the primary fitting parameters). Beside the... [Pg.192]

Sippl, M. J. (1993). Boltzmann s principle, knowledge-based mean fields and protein folding. An approach to the computational determination of protein structures. J. Comp.-Aid. Mol. Des. 7,473-501. [Pg.447]

Selected structural data for 3-metallacyclobutanone complexes of palladium and platinum 5, obtained from both experimental and computational determinations, are provided in Table 5. The ab initio structures calculated at the self-consistent field (SCF) and Hartree-Fock (F1F) levels show good agreement with experimental values for the bond lengths of the metallacycle, but these computations deliver somewhat longer Pd-P bonds and smaller P-Pd-P... [Pg.558]

Table 4 Crystallographic and computationally determined structural parameters for a-methylenetitanacyclobutene complexes... Table 4 Crystallographic and computationally determined structural parameters for a-methylenetitanacyclobutene complexes...
Using Standard Molecular Orbital Software to Compute Single Valence Bond Structures or Determinants... [Pg.253]

Mossbauer spectrum, the positions and separations of which depend on the oxidation state, electronic configuration, magnetic ordering, coordination number and symmetry of the iron atoms in a mineral structure. Computed peak areas enable Fe3+/Fe2+ ratios and site populations of Fe2+ ions in crystal structures to be readily determined for several minerals without interference from coexisting Mn, Cr and other transition elements. [Pg.253]


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See also in sourсe #XX -- [ Pg.272 , Pg.273 ]




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Computer software crystal structure determination

Computer-assisted structure determination

Structure Determination by Computer-based Spectrum Interpretation

Structure computation

Structure determination computer-based spectrum interpretation

Using Standard Molecular Orbital Software to Compute Single Valence Bond Structures or Determinants

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