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Full model

Figure 12.5. (a) Lattice model showing a polymer chain of 200 beads , originally in a random configuration, after 10,000 Monte Carlo steps. The full model has 90% of lattice sites occupied by chains and 10% vacant, (b) Half of a lattice model eontaining two similar chain populations placed in contact. The left-hand side population is shown after 50,0000 Monte Carlo steps the short lines show the loeation of the original polymer interface (courtesy K. Anderson). [Pg.480]

No fixed rules can be given it is up to the experience of the engineer to judge the necessary steps. Good advice, however, is to define a model with only the flow feature of concern, to test several levels of simplification on this model, and to decide from these numerical experiments the level of simplification for the full model under investigation. [Pg.1052]

Note that since both AND and XOR yield zero whenever ai-i and [Pg.348]

The optimize command maximizes a statistical "likelihood function". The higher this function, the more likely is the parameter to be the correct one. In the figure below, the symbols represent points calculated by the program Topaz (the full model), and the solid lines are the values calculated from the reduced-order model using the parameters determined by the program. [Pg.499]

Complex models are often slow in execution owing to the large number of equations involved and the large range of time constants. Under these circumstances it is often useful to approximate the transient behaviour of the full model by a simpler model representation which is faster to compute. Such simplifications are commonly achieved by a combination of first-order lags and time delays and are often represented in Laplace transform form, especially when the sub-model is to be used as part of a control engineering application. [Pg.81]

The reasons for the deviation of the constant-composition model from the full model are apparent when the concentrations of Red] and Red2 are examined. Due to the axi-symmetrical SECM geometry, the eoncentration profiles of Red] and Red2 are best shown as cross-sections over the domain / > 0, Z > 0, as illustrated sehematically in Fig. 6. Note that in this figure the tip position has been inverted eompared to that in Fig. 4. Figure 7... [Pg.301]

As discussed in Section IV, many studies of ET kinetics with SECM have been under conditions where constant composition in phase 2 can be assumed, but this severely restricts the range of kinetics that can be studied. With the availability of a full model for diffusion, outlined in Section IV, that lifts this restriction, Barker et al. [49] studied the reaction between ZnPor in benzene or benzonitrile and aqueous reductants, using CIO4 or tetrafluoroborate as potential-determining ions. [Pg.317]

In these equations, = 0 is the bottom of the catalyst bed and Xx is the conversion in the flow direction from bottom to top, while X2 is the conversion in the opposite flow direction. Bunimovich et al. (1990) suggest using Eqs. (52) to (54) for an initial estimate of the temperature profiles in order to speed up conversion on integration of the full model equations in Table X. This step would only be taken if it were the stationary cyclic state profiles that are wanted. [Pg.238]

The full model is described in Section 3.3.1.5 and consists of a countercurrent stagewise extraction cascade with backmixing in both phases. [Pg.453]

In case that the decay of impact kinetic energy due to viscous dissipation is the predominant mechanism in droplet flattening, Madejski s full model reduces to ... [Pg.307]

The values of the Weber number pertinent to this correlation were suggested to be sufficiently small so that viscous and solidification effects can be neglected. Another analytical expression, derived from Madej ski s full model after simplification under the conditions... [Pg.308]

In Madejski s full model,l401 solidification of melt droplets is formulated using the solution of analogous Stefan problem. Assuming a disk shape for both liquid and solid layers, the flattening ratio is derived from the numerical results of the solidification model for large Reynolds and Weber numbers ... [Pg.310]

Stepwise Perform a stepwise variable selection in both directions start once from the empty model, and once from the full model the AIC is used for measuring the performance. [Pg.160]

O Full model A Correlation + Variance x Stepwise O Best-subset V GA... [Pg.161]

An exhaustive search for an optimal variable subset is impossible for this data set because the number of variables is too high. Even an algorithm like leaps-and-bound cannot be applied (Section 4.5.4). Instead, variable selection can be based on a stepwise procedure (Section 4.5.3). Since it is impossible to start with the full model, we start with the empty model (regress the y-variable on a constant), with the scope... [Pg.196]

With sets of rules providing the facts from which a full model can be constructed, the program is informed regarding the origin of the spectrum to be analyzed. A coirparison is then made between model and actual spectra. Anomalous features are thus identified. [Pg.348]

The predictions that result from the offset and day-of-the-week terms (7.0715176 -1.2063679 ) are shown in the top panel of Figure 10.15 the residuals are shown in the bottom panel. Again, when all of these factor effects are combined into the full model, the results shown in Figure 10.12 are obtained. [Pg.194]

For the example used in Section 15.5, there would be three y s and four x s (or, perhaps, four y s and three t s). If y is associated with the qualitative factor univalent cation , then y would be the average block difference in response between the experiments involving Li and the overall mean y and y, would be the corresponding differences for experiments involving Na and K. Similarly, x g, Xj-, x, and Xgj would be the average treatment differences for experiments involving the divalent cations Mg, Ca, Sr, and Ba. Thus, the full model would be... [Pg.385]

Since a larger sample volume is presumed to be probed, the use of transmission mode has led to simpler, more accurate models requiring fewer calibration samples [50]. Scientists at AstraZeneca found that with a transmission Raman approach as few as three calibration samples were required to obtain prediction errors nearly equivalent to their full model [42]. For a fixed 10-s acquisition time, the transmission system had prediction errors as much as 30% less than the WAI system, though both approaches had low errors. It is hoped that this approach in combination with advanced data analysis techniques, such as band target entropy minimization (BTEM) [51], might help improve Raman s quantitative sensitivity further. [Pg.210]


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See also in sourсe #XX -- [ Pg.748 , Pg.750 ]

See also in sourсe #XX -- [ Pg.157 ]




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A Model for the Full Adhesive Formulations SIS-SI-Resin

Cold flow model, full-scale

Correlated models full configuration interaction

First-Order Equations with Full, Three-Variable Model

Full Bayesian model

Full PDF models

Full Scope SLP PSA Models

Full axisymmetric model

Full cubic model

Full density models the SCDS-Pixel method

Full linear model, with

Full linear model, with adsorption-desorption

Full optimized reaction space model

Full optimized reaction space model FORS)

Full scalar and vector models

Full scalar model

Full stochastic model

Full-Scale Mechanistic Gray-Box Modeling

Full-quadratic model

Full-scale fire modeling

Full-scale fire modeling combustion

Full-scale fire modeling heat transfer

Full-thickness model

Hysteresis full model

Intervals for Full Second-Order Polynomial Models

Models full chemical balance

Models full second-order

Models full second-order polynomial

The flexing geometry of full second-order polynomial models

The full schema model

Two-Dimensional, Full-Elliptic Flow Model

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