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Minimization approximation

Ab-initio (nonempirical, from first principles ) methods also use the HF-SCF model but includes all electrons and uses minimal approximation. Basis sets of functions based on linear combinations of atomic orbitals (LCAO) increase in complexity from the simplest (STO-3G) to more complex (3-21G( )) to extended basis sets (6-311 + G ) for the most accurate (and most time-consuming) results. Treat systems up to 50 atoms. [Pg.130]

Eventually, this method allows quantitative measuring of the translational diffusion of proteins modified with these three labels in solution and in biomembranes. The minimal approximate volume of a sample available for the fluorescence measurement (using a regular commercial spectrofluorimeter) in this method is about 10"3 pi when the total concentration of fluorophores is close to 0.01 pM and the local concentration of radicals is about 10 pM. [Pg.13]

A line search consists of an approximate one-dimensional minimization of the objective function along the computed direction p. This produces an acceptable step X and a new iterate xk + Xp. Function and gradient evaluations of the objective function are required in each line search iteration. In contrast, the trust region strategy minimizes approximately a local quadratic model of the function using current Hessian information. An optimal step that lies within... [Pg.21]

There are good reasons for acceptance of AA instrumentation. Archaeologists universally have found that funding is a major consideration in element analysis research. However, the purchase cost of necessary AA equipment, including support equipment, is minimal (approximately 8,000- 12,000). In addition the cost of analysis per... [Pg.268]

Even though the body s requirement for iodine is minimal - approximately l-2pg/kg of body weight for adults — the intake of iodine should be met on a regular basis to prevent disorders arising from low intake, especially when associated with socioeconomic conditions that trigger nutritional risk, as is the case with a large portion of the Brazilian population (Zelaya, 1994). [Pg.1204]

The modified direct inversion in the iterative subspace (MDIIS) method combines the simplicity and relatively small memory usage of an iterational approach with the efficiency of a direct method. It comprises two stages minimization of the residual linearly approximated with last successive iterative vectors used as a current basis, and then update of the basis with the minimized approximate residual by a properly scaled parameter. [Pg.262]

To minimize approximations and adjustments, an equilibrium table can be prepared and more exact concentrations for the conjugate pair can be obtained directly. [Pg.184]

Since formulation of a dense Hessian (n entries, of which n n + l)/2 are unique) is both memory and computation intensive, many Newton techniques for minimization approximate curvature information implicitly and often progressively (i.e., as the algorithm proceeds). Limited-memory versions reduce computational and storage requirements so that they can be applied to very large problems and/or to problems where second derivatives are not available. [Pg.1146]

The device operates as described below. After switching on the power source, CB begins to be charged from Ac. CS provides direct charging current of 0.1 A that makes it possible not to exceed Ac permissible discharging current value as well as to minimize CB charging time till approximately 10s. [Pg.651]

Truncation at the first-order temi is justified when the higher-order tenns can be neglected. Wlien pe higher-order tenns small. One choice exploits the fact that a, which is the mean value of the perturbation over the reference system, provides a strict upper bound for the free energy. This is the basis of a variational approach [78, 79] in which the reference system is approximated as hard spheres, whose diameters are chosen to minimize the upper bound for the free energy. The diameter depends on the temperature as well as the density. The method was applied successfiilly to Lennard-Jones fluids, and a small correction for the softness of the repulsive part of the interaction, which differs from hard spheres, was added to improve the results. [Pg.508]

Equation (ASA. 110) represents the canonical fonn T= constant) of the variational theory. Minimization at constant energy yields the analogous microcanonical version. It is clear that, in general, this is only an approximation to the general theory, although this point has sometimes been overlooked. One may also define a free energy... [Pg.784]

Frequent approximations made in TB teclmiques in the name of achieving a fast method are the use of a minimal basis set, the lack of a self-consistent charge density, the fitting of matrix elements of the potential. [Pg.2202]

A quantum mechanical treatment of molecular systems usually starts with the Bom-Oppenlieimer approximation, i.e., the separation of the electronic and nuclear degrees of freedom. This is a very good approximation for well separated electronic states. The expectation value of the total energy in this case is a fiinction of the nuclear coordinates and the parameters in the electronic wavefunction, e.g., orbital coefficients. The wavefiinction parameters are most often detennined by tire variation theorem the electronic energy is made stationary (in the most important ground-state case it is minimized) with respect to them. The... [Pg.2331]

The EF algoritlnn [ ] is based on the work of Cerjan and Miller [ ] and, in particular, Simons and coworkers [70,1Y. It is closely related to the augmented Hessian (rational fiinction) approach[25]. We have seen in section B3.5.2.5 that this is equivalent to addmg a constant level shift (damping factor) to the diagonal elements of the approximate Hessian H. An appropriate level shift effectively makes the Hessian positive definite, suitable for minimization. [Pg.2351]

These methods, which probably deserve more attention than they have received to date, simultaneously optimize the positions of a number of points along the reaction path. The method of Elber and Karpins [91] was developed to find transition states. It fiimishes, however, an approximation to the reaction path. In this method, a number (typically 10-20) equidistant points are chosen along an approximate reaction path coimecting two stationary points a and b, and the average of their energies is minimized under the constraint that their spacing remains equal. This is obviously a numerical quadrature of the integral s f ( (.v)where... [Pg.2354]

Within this contimiiim approach Calm and Flilliard [48] have studied the universal properties of interfaces. While their elegant scheme is applicable to arbitrary free-energy fiinctionals with a square gradient fomi we illustrate it here for the important special case of the Ginzburg-Landau fomi. For an ideally planar mterface the profile depends only on the distance z from the interfacial plane. In mean field approximation, the profile m(z) minimizes the free-energy fiinctional (B3.6.11). This yields the Euler-Lagrange equation... [Pg.2370]

In this minimal END approximation, the electronic basis functions are centered on the average nuclear positions, which are dynamical variables. In the limit of classical nuclei, these are conventional basis functions used in moleculai electronic structure theoiy, and they follow the dynamically changing nuclear positions. As can be seen from the equations of motion discussed above the evolution of the nuclear positions and momenta is governed by Newton-like equations with Hellman-Feynman forces, while the electronic dynamical variables are complex molecular orbital coefficients that follow equations that look like those of the time-dependent Hartree-Fock (TDHF) approximation [24]. The coupling terms in the dynamical metric are the well-known nonadiabatic terms due to the fact that the basis moves with the dynamically changing nuclear positions. [Pg.228]

The approximations defining minimal END, that is, direct nonadiabatic dynamics with classical nuclei and quantum electrons described by a single complex determinantal wave function constructed from nonoithogonal spin... [Pg.233]

By using this approach, it is possible to calculate vibrational state-selected cross-sections from minimal END trajectories obtained with a classical description of the nuclei. We have studied vibrationally excited H2(v) molecules produced in collisions with 30-eV protons [42,43]. The relevant experiments were performed by Toennies et al. [46] with comparisons to theoretical studies using the trajectory surface hopping model [11,47] fTSHM). This system has also stimulated a quantum mechanical study [48] using diatomics-in-molecule (DIM) surfaces [49] and invoicing the infinite-onler sudden approximation (lOSA). [Pg.241]

The first study in which a full CASSCE treatment was used for the non-adiabatic dynamics of a polyatomic system was a study on a model of the retinal chromophore [86]. The cis-trans photoisomerization of retinal is the primary event in vision, but despite much study the mechanism for this process is still unclear. The minimal model for retinal is l-cis-CjH NHj, which had been studied in an earlier quantum chemisti7 study [230]. There, it had been established that a conical intersection exists between the Si and So states with the cis-trans defining torsion angle at approximately a = 80° (cis is at 0°). Two... [Pg.305]

To calculate the matrix elements for H2 in the minimal basis set, we approximate the Slater Is orbital with a Gaussian function. That is, we replace the Is radial wave function... [Pg.436]


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See also in sourсe #XX -- [ Pg.44 ]




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Approximation minimal coupling

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