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Unconstrained Geometry Optimization

HyperChem has a set of optimizers available to explore potential surfaces. These differ in their generality, convergence properties and computational requirements. One must be somewhat pragmatic about optimization and switch optimizers or restart an optimizer when it encounters specific problems. [Pg.302]

HyperChem includes only unconstrained optimization. That is, given the coordinates X, Y, of a set of atoms A (the inde- [Pg.302]

HyperChem does not use constrained optimization but it is possible to restrain molecular mechanics and quantum mechanics calculations by adding extra restraining forces. [Pg.303]


Clearly f will go to zero when E2 = Et, independently of the magnitude of. Note, however, that the gradient will also go to zero if Et is different from E2 but the two surfaces are parallel (i.e., Xj, the gradient difference vector, has zero length). In this case the method would fail. This situation will occur for a Renner-Teller-like degeneracy, for example. Of course, in this case, the geometry can be found by normal unconstrained geometry optimization. [Pg.112]

In general, the accuracy of a simulated spectrum depends on the quality of the description of both the initial and the final electronic states of the transition. This is obviously related to the proper choice of a well-suited computational model a reliable description of equilibrium structures, harmonic frequencies, normal modes, and electronic transition energy is necessary. In the study of the A Bj Aj electronic transition of phenyl radical the structural and vibrational properties have been obtained with the B3LYP/TDB3LYP//N07D model, designed for computational studies of free radicals. Unconstrained geometry optimizations lead to planar... [Pg.134]

The consistent embedding of the QM/EPE approach enables one to build multifunctional models of isolated sites by means of unconstrained geometry optimization, where the polarization of the cluster surrounding is completely... [Pg.376]

The use of different models for the geometry optimization can lead to rather different structures (Pig. 4). Calculated electron densities and spin densities on Cu" arc different for structures obtained with the combined model or with the constrained or unconstrained cluster model optimizations (Fig. 4c, 4b, and 4d, respectively). Therefore, the calculated properties (e. g., electronic spectra, ESR, IR of probe molecule, or adsorption energies) will depend on the choice of the model and method. [Pg.259]

The location of critical points requires addressing a problem of unconstrained optimization, for the solution of which there exist a number of efficient algorithms. In this chapter a number of simple optimization projects are proposed to those students with little or no experience with geometry optimizations. As well, we have included some more challenging projects for the experienced students. [Pg.412]

Over the next decade MNDO parameters were derived for lithium, beryllium, boron, fluorine, aluminum, silicon, phosphorus, sulfur, chlorine,zinc, germanium, bromine, iodine, tin, mercury, and lead. " In 1983 the first MOPAC program was written, containing both the MINDO/3 and MNDO mediods, which allowed various geometric operations, such as geometry optimization, constrained and unconstrained, with and without symmetry, transition state localization by use of a reaction co-... [Pg.56]

Geometry optimization problems for molecules in the context of standard all-atom force fields in computational chemistry are typically of the multivariate, continuous, and nonlinear type. They can be formulated as constrained (as in adiabatic relaxation) or unconstrained. Discontinuities in the derivatives may be a problem in certain formulations involving truncation, such as of the nonbonded terms (see Section 7). [Pg.1144]

The use of quantum-chemistry computer codes for the determination of the equilibrium geometries of molecules is now almost routine owing to the availability of analytical gradients at SCF, MC-SCF and CP levels of theory and to the robust methods available from the held of numerical analysis for the unconstrained optimization of multi-variable functions (see, for example. Ref. 21). In general, one assumes a quadratic Taylor series expansion of the energy about the current position... [Pg.161]


See other pages where Unconstrained Geometry Optimization is mentioned: [Pg.302]    [Pg.302]    [Pg.354]    [Pg.275]    [Pg.162]    [Pg.715]    [Pg.111]    [Pg.302]    [Pg.302]    [Pg.354]    [Pg.275]    [Pg.162]    [Pg.715]    [Pg.111]    [Pg.240]    [Pg.338]    [Pg.344]    [Pg.78]    [Pg.340]    [Pg.257]    [Pg.202]    [Pg.180]    [Pg.48]    [Pg.49]    [Pg.258]    [Pg.310]    [Pg.243]    [Pg.1138]    [Pg.330]    [Pg.131]    [Pg.183]    [Pg.590]    [Pg.168]    [Pg.196]    [Pg.123]    [Pg.99]    [Pg.163]    [Pg.338]    [Pg.199]    [Pg.1939]   


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Geometries, optimized

Optimization geometry

Optimizing geometries

Unconstrained

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