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Local gradient

The HE, GVB, local MP2, and DFT methods are available, as well as local, gradient-corrected, and hybrid density functionals. The GVB-RCI (restricted configuration interaction) method is available to give correlation and correct bond dissociation with a minimum amount of CPU time. There is also a GVB-DFT calculation available, which is a GVB-SCF calculation with a post-SCF DFT calculation. In addition, GVB-MP2 calculations are possible. Geometry optimizations can be performed with constraints. Both quasi-Newton and QST transition structure finding algorithms are available, as well as the SCRF solvation method. [Pg.337]

These Huctuations lead to two more components to the Gibbs energy changes in the process. The hrst arises from the fact that the Huctuations represent a local gradient in composition, and hence there is a change in the number of... [Pg.191]

Halls, M. D., Schlegel, H. B., 1998, Comparison of the Performance of Local, Gradient-Corrected, and Hybrid Density Functional Models in Predicting Infrared Intensities , J. Chem. Phys., 109, 10587. [Pg.290]

In Section 21.5, the treatment is based on the pseudohomogeneous assumption for the catalyst + fluid system (Section 21.4). In this section, we consider the local gradients in concentration and temperature that may exist both within a catalyst particle and in the surrounding gas film. The system is then heterogeneous. We retain the assumptions of... [Pg.544]

Figure 3.11 The steepest-descent method the search in one direction is discontinued when no further decrease is possible, i.e., when the search direction is parallel to the local contour line. The next step starts in a perpendicular direction, i.e., in the direction opposite to the local gradient. Figure 3.11 The steepest-descent method the search in one direction is discontinued when no further decrease is possible, i.e., when the search direction is parallel to the local contour line. The next step starts in a perpendicular direction, i.e., in the direction opposite to the local gradient.
This Newton step can be repeated, but if the function is not ill-behaved, it may prove simpler to restart the whole loop and recalculate the local gradient. [Pg.335]

The wave functions are expended in a plane wave basis set, and the effective potential of ions is described by ultrasoft pseudo potential. The generalized gradient approximation (GGA)-PW91, and local gradient-corrected exchange-correlation functional (LDA)-CAPZ are used for the exchange-correlation functional. [Pg.221]

When fluctuations are present, the system is inhomogeneous in space and (j)(r) is a function of the spatial coordinate r. Also any local gradients V(j)(r) cost in free energy. Now, the change in free energy to excite a fluctuation / = ( — c o (where cj)o is the equilibrium value) is given by the Landau-Ginzburg form... [Pg.38]

What is the mechanism which results in rapid coalescence if mass transfer occurs from the drops but slow or no coalescence if both phases are mutually saturated Interfacial turbulence caused by local gradients in interfacial tension looks promising. [Pg.91]

The concept of entropy-enthalpy compensation resulting in the critical conditions of enthalpic interactions and the molar mass independent sample retention turned out useful also for the understanding several other coupled methods of polymer HPLC. It is accepted [195,196] that the polymer species tend to elute at the critical conditions also when either eluent strength or quality change within the HPLC system in the course of the HPLC experiment that is in the continuous and local gradient methods (Sections 16.5.3, 16.5.4, and 16.5.6). Irrespective of the problems and limitations of LC CC, its concept belongs to the important breakthroughs in polymer HPLC. [Pg.479]

Fig. 1. Model of subarachnoidal space, CSF flow, and molecular flux (N1). After CSF production in choroid plexus of the ventricles (1,2,3), CSF passes the aperture (4,5), reaches the cistemae (6-9), and divides into a cortical and a lumbar branch of the subarachnoidal space. Finally, CSF drains through the arachnoid villi into venous blood. The illustration represents an idealized cross section through the subarachnoid space. Molecules diffuse from serum with a concentration C(ser) flu ough tissue along the diffusion path x into the subarachnoid space with a concentration C(csF)- Th molecular flux J depends on the local gradient Ac/Ax or dddx and the diffusion constant D. The CSF concentration increases with decreasing volume exchange, i.e., decreasing CSF volume bulk flow (F= 500 ml/day). The flow rate of a molecule in CSF is r= FIA, where A is the varying cross section of the subarachnoid space. Fig. 1. Model of subarachnoidal space, CSF flow, and molecular flux (N1). After CSF production in choroid plexus of the ventricles (1,2,3), CSF passes the aperture (4,5), reaches the cistemae (6-9), and divides into a cortical and a lumbar branch of the subarachnoidal space. Finally, CSF drains through the arachnoid villi into venous blood. The illustration represents an idealized cross section through the subarachnoid space. Molecules diffuse from serum with a concentration C(ser) flu ough tissue along the diffusion path x into the subarachnoid space with a concentration C(csF)- Th molecular flux J depends on the local gradient Ac/Ax or dddx and the diffusion constant D. The CSF concentration increases with decreasing volume exchange, i.e., decreasing CSF volume bulk flow (F= 500 ml/day). The flow rate of a molecule in CSF is r= FIA, where A is the varying cross section of the subarachnoid space.
The discussion up to this point has been concerned essentially with metal alloys in which the atoms are necessarily electrically neutral. In ionic systems, an electric diffusion potential builds up during the spinodal decomposition process. The local gradient of this potential provides an additional driving force, which acts upon the diffusing species and this has to be taken into account in the derivation of the equivalents of Eqns. (12.28) and (12.30). The formal treatment of this situation has not yet been carried out satisfactorily [A.V. Virkar, M. R. Plichta (1983)]. We can expect that the spinodal process is governed by the slower cation, for example, in a ternary AX-BX crystal. The electrical part of the driving force is generally nonlinear so that linearized kinetic equations cannot immediately be applied. [Pg.311]

The fluxes of mass, momentum, and energy of phase k transported in a laminar or turbulent multiphase flow can be expressed in terms of the local gradients and the transport coefficients. In a gas-solid multiphase flow, the transport coefficients of the gas phase may be reasonably represented by those in a single-phase flow although certain modifications... [Pg.196]

The simplest exchange-correlation functionals, derived from the density alone, give reasonable results for many molecular properties. However, it has been found that adding terms proportional to the local gradient of the density in both the exchange and correlation integrands leads to much more accurate results. Most modern DFT computations use these so-called non-local or gradient-corrected functionals. [Pg.161]

The solidification kinetics and compositional fluctuations in the melt will decide over the crystallization pathway which can be followed by all of the melt. If local gradients in temperature or composition exist in the system the crystallization pathway can be locally inhomogeneous and create different metastable solids at different locations in the macroscopic solidified blocks. [Pg.20]


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See also in sourсe #XX -- [ Pg.39 ]




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Dynamic interfacial tension gradient, local

Generalized gradient approximation local hybrid

Gradient Correction to Local Exchange and Correlation Energy

Gradient localized spectroscopy

Local density gradients

Local gradient operator

Local gradient-corrected exchange-correlation functional

Local radial velocity gradient

Non-local gradient corrections

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