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Energies, calculation

Quantum-mechanical calculations on the conformational energy map of tryptophanyl residues by an all-valence-electrons method (PCILO) were carried out by Pullman and coworkers 243). The conformational map for the ground state of N-acetyl-N -methyl-tryptophanamide revealed as the most stable form the which corresponds to a seven-membered hydrogen-bonded ring, the hydrogen bond taking place [Pg.402]

Suppose we wish to compare the calculated energy of regular polyacetylene to that of a bond-alternating version, or that of PPP with PPP-N2. How do we get energies from the band calculations for these two cases In a Hiickel-type calculation of a molecule, we simply add up the one-electron energies. In a band calculation we are faced with a very large set of one-electron energies—one for each k value. How do we deal with this  [Pg.562]

The problem, then, is to calculate an accurate average energy for each of the filled bands, the average being over the first Brillouin zone, and then multiply each such average energy by the number of electrons in that band, per unit cell. The sum of these is the Hiickel total energy per unit cell. (This procedure assumes that the bands are not partially filled.) [Pg.562]

Achieving accurate average CO energies from values at a few k points is possible if those points are sensibly chosen and if appropriate weighting factors are employed. The problem of choosing the correct few points and their weight factors has been worked out by Chadi and Cohen [5] for multidimensional systems of various symmetries. Although this is a matter of real practical interest, we will not explore it further here. [Pg.562]

Approximate energies of the molecular orbitals are obtained by solving the secular equation Hy - WGy = 0. There is one secular equation to solve for each type of orbital. Thus, we have alg, eg, t2g, and tlu secular equations in O symmetry. [Pg.102]

The exchange integrals are assumed to be proportional to the overlap integrals since -GML O M + l l)  [Pg.104]

A value of k of about 2 has been used in most cases. [Pg.104]


Microcrystals of SrS04 of 30 A diameter have a solubility product at 25°C which is 6.4 times that for large crystals. Calculate the surface tension of the SrS04-H20 interface. Equating surface tension and surface energy, calculate the increase in heat of solution of this SrS04 powder in joules per mole. [Pg.380]

Douketis C, Socles G, Marchetti S, Zen M and Thakkar A J 1982 Intermolecular forces via hybrid Hartree-Fock SCF plus damped dispersion (HFD) energy calculations. An improved spherical model J. Chem. Phys. 76 3057... [Pg.216]

Jorgenson W 1989 Free energy calculations a breakthrough in modeling organic chemistry in solution Accounts Chem. Res. 22 184... [Pg.555]

Reynolds C, King P M and Richards W G 1992 Free energy calculations in molecular biophysics Mol. Phys. 76 251... [Pg.558]

Once the requisite one- and two-electron integrals are available in the MO basis, the multiconfigurational wavefunction and energy calculation can begin. Each of these methods has its own approach to describing tlie configurations d),. j included m the calculation and how the C,.] amplitudes and the total energy E are to be... [Pg.2185]

Feibelman P J 1987 Force and total-energy calculations for a spatially compact adsorbate on an extended, metallic crystal surface Phys. Rev. B 35 2626... [Pg.2237]

Truhlar D G and Horowitz C J 1978 Functional representation of Liu and Siegbahn s accurate ab initio potential energy calculations for H + H2 J. Chem. Phys. 68 2466... [Pg.2331]

Payne M C, Teter M P, Allan D C, Arias T A and Joanopoulos J D 1992 Iterative minimization techniques for ab /M/o total energy calculations molecular dynamics and conjugate gradient Rev. Mod. Phys. 64 1045... [Pg.2356]

We assume that the unbinding reaction takes place on a time scale long ( ompared to the relaxation times of all other degrees of freedom of the system, so that the friction coefficient can be considered independent of time. This condition is difficult to satisfy on the time scales achievable in MD simulations. It is, however, the most favorable case for the reconstruction of energy landscapes without the assumption of thermodynamic reversibility, which is central in the majority of established methods for calculating free energies from simulations (McCammon and Harvey, 1987 Elber, 1996) (for applications and discussion of free energy calculation methods see also the chapters by Helms and McCammon, Hermans et al., and Mark et al. in this volume). [Pg.55]

Accurate Energy Calculations of a Protein in Diflferent Conformations... [Pg.67]

S. Miyamoto and P. A. Kollman. Absolute and relative binding free energy calculations of the interaction of biotin and its analogs with streptavidin using molecular dynamics/free energy perturbation approaches. Proteins, 16 226-245, 1993. [Pg.96]

A linear dependence approximately describes the results in a range of extraction times between 1 ps and 50 ps, and this extrapolates to a value of Ws not far from that observed for the 100 ps extractions. However, for the simulations with extraction times, tg > 50 ps, the work decreases more rapidly with l/tg, which indicates that the 100 ps extractions still have a significant frictional contribution. As additional evidence for this, we cite the statistical error in the set of extractions from different starting points (Fig. 2). As was shown by one of us in the context of free energy calculations[12], and more recently again by others specifically for the extraction process [1], the statistical error in the work and the frictional component of the work, Wp are related. For a simple system obeying the Fokker-Planck equation, both friction and mean square deviation are proportional to the rate, and... [Pg.144]

Hermans, J., Yun, R. H., Anderson, A. G. Precision of free-energies calculated by molecular dynamics simulations of peptides in solution. J. Comp. Chem. 13 (1992) 429-442... [Pg.146]

Vorobjev, Y., Almagro, J. C., Hermans, J. Conformational free energy calculated by a new iiK thod from dynamics simulation and continuum dielectric... [Pg.147]

Radmer, R.. 1., Kollman, P. A. Approximate free energy calculation methods and structiire based ligand design. J. Comp. Aid. Mol. Desgn (in press)... [Pg.161]

Amadei, A., Apol, M. E. F., Di Nola, A., Berendsen, H. J. C. The quasi-Gaussian entropy theory Free energy calculations based on the potential energy distribution function. J. Chem. Phys. 104 (1996) 1560-1574... [Pg.162]

Beutler, T. C., Mark, A. E., van Schaik, R. C., Gerber, P. R., van Gunsteren, W. F. Avoiding singularities and numerical instabilities in free energy calculations based on molecular simulations. Chem. Phys. Letters 222 (1994) 529-539... [Pg.162]

MP2 correlation energy calculations may increase the computational lime because a tw o-electron integral Iran sfonnalion from atomic orbitals (.40 s) to molecular orbitals (MO s) is ret]uired. HyperClicrn rnayalso need additional main memory arul/orcxtra disk space to store the two-eleetron integrals of the MO s. [Pg.113]

Quantum mechanical calculations are restricted to systems with relatively small numbers of atoms, and so storing the Hessian matrix is not a problem. As the energy calculation is often the most time-consuming part of the calculation, it is desirable that the minimisation method chosen takes as few steps as possible to reach the minimum. For many levels of quantum mechanics theory analytical first derivatives are available. However, analytical second derivatives are only available for a few levels of theory and can be expensive to compute. The quasi-Newton methods are thus particularly popular for quantum mechanical calculations. [Pg.289]


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