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Stationaiy points

Analytical gradient energy expressions have been reported for many of the standard models discussed in this book. Analytical second derivatives are also widely available. The main use of analytical gradient methods is to locate stationaiy points on potential energy surfaces. So, for example, in order to find an expression for the gradient of a closed-shell HF-LCAO wavefunction we might start with the electronic energy expression from Chapter 6,... [Pg.276]

Figure 4.8 Stationaiy-point structures for the epoxidation of ethene with hydrogen peroxide in the presence of three to four molecules of H FI P, optimized at RB3LYP/6-31+G(d,p). Figure 4.8 Stationaiy-point structures for the epoxidation of ethene with hydrogen peroxide in the presence of three to four molecules of H FI P, optimized at RB3LYP/6-31+G(d,p).
If F is continuous and has continuous first and second derivatives, it is necessary that F is stationaiy with respect to all variations in the independent variables at a point ti, which is proposed as a minimum to F that is,... [Pg.484]

The point z is tested to see if it could be a minimum point. It is neces-saiy that F be stationaiy for all infinitesimal moves for z that satisfy the equahty constraints. Linearize the m equahty constraints around z, getting... [Pg.484]

Direct Mass Measurement One type of densitometer measures the natural vibration frequency and relates the amplitude to changes in density. The density sensor is a U-shaped tube held stationaiy at its node points and allowed to vibrate at its natural frequency. At the curved end of the U is an electrochemical device that periodically strikes the tube. At the other end of the U, the fluid is continuously passed through the tube. Between strikes, the tube vibrates at its natural frequency. The frequency changes directly in proportion to changes in density. A pickup device at the cui ved end of the U measures the frequency and electronically determines the fluid density. This technique is usefiil because it is not affec ted by the optical properties of the fluid. However, particulate matter in the process fluid can affect the accuracy. [Pg.764]

Stationary-Container Systems fSCS) Collec tion systems in which the containers used for the storage of wastes remain at the point of waste generation, except for occasional short trips to the collec tion vehicle, are defined as stationary-container systems. Labor requirements for mechanicallv loaded stationaiy-coutaiuer systems are essentially the same as for hauled-container systems. There are two main types of stationaiy-coutaiuer systems (1) those in which self-loading compactors are used and (2) those in which manually loaded vehicles are used. [Pg.2237]

J he boiling-point will rise and after a few minutes will remain stationaiy The temperature is noted. A second and third... [Pg.39]

When the composition of a fluid mixture varies from one point to another, each component has a tendency to fiow in the direction that will reduce the local differences in concentration. If the bulk fluid is eidier stationaiy or in laminar flow in a direction noimal to the concentration gradient, the mass transfer reducing the concentration difference occurs by a process of molecular diffusion. This mechanism is characterized by random movement of individual molecules. [Pg.406]

In carrying out the procedure for a tetrahedral species, it is convenient to let four vectors on the central atom represent the hybrid orbitals we wish to construct (Fig 3.26). Derivation of the reducible representation for these vectors involves performing on them, in turn, one symmetry operation from eadi class in the point group. As in the analysis of vibrational modes presented earlier, only those vectors that do not move will coniribute to the representatioa Thus we can determine the character for each symmetry operation we apply by simply counting the number of vectors that remain stationaiy. The result for AB4 is the reducible representation, F ... [Pg.73]

Figure 3.2 Time dependence of the probabilities Pi t) (1) and dPn ()ldt (2) for a non-stationaiy nucleation process (a schematic representation), / /and are the cooidinates of the inflection point of the function [3.16]. (With permission fh>m Elsevier Science). Figure 3.2 Time dependence of the probabilities Pi t) (1) and dPn ()ldt (2) for a non-stationaiy nucleation process (a schematic representation), / /and are the cooidinates of the inflection point of the function [3.16]. (With permission fh>m Elsevier Science).

See other pages where Stationaiy points is mentioned: [Pg.1320]    [Pg.216]    [Pg.228]    [Pg.305]    [Pg.253]    [Pg.149]    [Pg.274]    [Pg.1320]    [Pg.216]    [Pg.228]    [Pg.305]    [Pg.253]    [Pg.149]    [Pg.274]    [Pg.927]    [Pg.1213]    [Pg.1555]    [Pg.1036]    [Pg.557]    [Pg.387]    [Pg.117]    [Pg.744]    [Pg.27]    [Pg.87]    [Pg.666]    [Pg.660]    [Pg.196]    [Pg.294]    [Pg.13]   
See also in sourсe #XX -- [ Pg.421 , Pg.431 ]




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