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Parametric relations

A common alternative is to synthesize approximate state functions by linear combination of algebraic forms that resemble hydrogenic wave functions. Another strategy is to solve one-particle problems on assuming model potentials parametrically related to molecular size. This approach, known as free-electron simulation, is widely used in solid-state and semiconductor physics. It is the quantum-mechanical extension of the classic (1900) Drude model that pictures a metal as a regular array of cations, immersed in a sea of electrons. Another way to deal with problems of chemical interaction is to describe them as quantum effects, presumably too subtle for the ininitiated to ponder. Two prime examples are, the so-called dispersion interaction that explains van der Waals attraction, and Born repulsion, assumed to occur in ionic crystals. Most chemists are in fact sufficiently intimidated by such claims to consider the problem solved, although not understood. [Pg.121]

The most straightforward example of this approach is the use of scatterometer data to obtain estimates of U that are then combined with a parametrization relating k to U (see Section... [Pg.2916]

The second option is to use the step test method usually for developing parametric relations for control systems. By making a small step change to the manipulatable (independent) variable (for example, feed rate), a response from the control variable... [Pg.46]

The pore size distribution function (a) appears parametrically in the flux relations of Feng and Stewart, so their models certainly cannot be completely predictive in nature unless this distribution is known. It is... [Pg.75]

Because of the uncertainties related to the parametrization of an sp C, this approach is unsuitable for the study of protomeric equilibria for structures 4 through 8. We must lay stress on the fact that this simple treatment does not include (a) medium effects which are known to be important and b) the existence of associated species (see Chapter VII, Section I. LB) whose consequences have been thoroughly studied in pyridone series (1688). [Pg.5]

In a given motion, a particular material particle will experience a strain history The stress rate relation (5.4) and flow rule (5.11), together with suitable initial conditions, may be integrated to obtain the eorresponding stress history for the particle. Conversely, using (5.16) instead of (5.4), may be obtained from by an analogous ealeulation. As before, may be represented by a continuous curve, parametrized by time, in six-dimensional symmetric stress spaee. [Pg.127]

The only problem with the foregoing approach to molecular interactions is that the accurate solution of Schrddinger s equation is possible only for very small systems, due to the limitations in current algorithms and computer power. Eor systems of biological interest, molecular interactions must be approximated by the use of empirical force fields made up of parametrized tenns, most of which bear no recognizable relation to Coulomb s law. Nonetheless the force fields in use today all include tenns describing electrostatic interactions. This is due at least in part to the following facts. [Pg.95]

Structured uncertainty relates to parametric variations in the plant dynamics, i.e. uncertain variations in coefficients in plant differential equations. [Pg.303]

Each force field achieves good results only for a limited class of molecules, related to those for which it was parametrized. No force field can be generally used for all molecular systems of interest. [Pg.5]

Parametric studies showed that mass diffusion in the gas phase could be neglected under most conditions. The calculations also show that the selection of the hypergolic combination (i.e., the gaseous oxidizer and the propellant system) fixes all of the parameters except the initial temperature and the oxidizer concentration. A general solution of the model shows that the ignition-delay time is approximately rated to the gaseous oxidizer concentration by the relation... [Pg.17]

The domain of the stable flow is located to the right of the boundary PeL(i ) (the shaded region in the graph). To the left of this curve is the domain in which stable flows in a heated capillary cannot occur. From the relation between the parameters and Ja, the parametric plane Pep — may be subdivided into two domains (1) < Ja, and (2) > Ja. Within the first of these the stable flows cannot occur... [Pg.392]

The system of Eqs. (10.22-10.24) and relations (10.26-10.31) contains five dimensionless parametrical groups Eu, Fr, We, 7g and Jl, which completely determine the problem. [Pg.409]

The critical decisions in the modeling problem are related to the other three elements. The space G is most often defined as the linear span of a finite number, m, of basis functions, 0 ), each parametrized by a set of unknown coefficients w according to the formula... [Pg.167]

As was discussed in the previous part, the temperature elevation in the solutions can be ascribed to the absorption of the NIR light by the solvents. In order to quantitatively explain the temperature elevation coefficient, AT/AP, for other solvents, we proposed a simple model that can parametrize the temperature elevation. As easily predicted, the AT/AP value is closely related to the extinction coefficient of light absorption, a, and the thermal conductivity, X. Heat generated at the focal point ofthe NIR beam is proportional to the extinction coefficient, a, and the incident laser power, P, as represented by Eq. (8.5). [Pg.144]

Figure 5. Concordia diagram similar to Figure 4 illustrating the concordia curve for initial = 150 (appropriate for marine samples), with age in ka depicted parametrically along concordia. Also illustrated are continuous uranium gain/loss model curves for samples with primary ages of 80 ka (dashed) and 150 ka (thin solid curve). See text for discussion of this model and related models (after Cheng etal. 1998). Figure 5. Concordia diagram similar to Figure 4 illustrating the concordia curve for initial = 150 (appropriate for marine samples), with age in ka depicted parametrically along concordia. Also illustrated are continuous uranium gain/loss model curves for samples with primary ages of 80 ka (dashed) and 150 ka (thin solid curve). See text for discussion of this model and related models (after Cheng etal. 1998).
The Ph Eur mentions the possibility of parametric release for certain terminal sterilization processes (saturated steam, dry heat and irradiation) where sterilization parameters can be accurately monitored and recorded and controlled. Much of the information in the two draft documents relates to parametric release of sterile products, but the possibility of parametric... [Pg.661]


See other pages where Parametric relations is mentioned: [Pg.568]    [Pg.241]    [Pg.246]    [Pg.211]    [Pg.228]    [Pg.174]    [Pg.175]    [Pg.14]    [Pg.394]    [Pg.700]    [Pg.710]    [Pg.37]    [Pg.572]    [Pg.149]    [Pg.1906]    [Pg.203]    [Pg.568]    [Pg.241]    [Pg.246]    [Pg.211]    [Pg.228]    [Pg.174]    [Pg.175]    [Pg.14]    [Pg.394]    [Pg.700]    [Pg.710]    [Pg.37]    [Pg.572]    [Pg.149]    [Pg.1906]    [Pg.203]    [Pg.636]    [Pg.440]    [Pg.141]    [Pg.147]    [Pg.148]    [Pg.402]    [Pg.402]    [Pg.119]    [Pg.240]    [Pg.260]    [Pg.220]    [Pg.146]    [Pg.441]    [Pg.661]    [Pg.18]    [Pg.3]    [Pg.312]    [Pg.301]   
See also in sourсe #XX -- [ Pg.25 ]




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Parametric

Parametrization

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