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Functions of model

The sum of the squared differences between calculated and measures pressures is minimized as a function of model parameters. This method, often called Barker s method (Barker, 1953), ignores information contained in vapor-phase mole fraction measurements such information is normally only used for consistency tests, as discussed by Van Ness et al. (1973). Nevertheless, when high-quality experimental data are available. Barker s method often gives excellent results (Abbott and Van Ness, 1975). [Pg.97]

Fig. 36.10. Prediction error (RMSPE) as a function of model complexity (number of factors) obtained from leave-one-out cross-validation using PCR (o) and PLS ( ) regression. Fig. 36.10. Prediction error (RMSPE) as a function of model complexity (number of factors) obtained from leave-one-out cross-validation using PCR (o) and PLS ( ) regression.
Table 5.1. Major role and function of model catalysts [10,12]... Table 5.1. Major role and function of model catalysts [10,12]...
Figure 12.25 Conceptual plot of interference error (dotted line), estimation error (dashed line), and overall prediction error (solid line) as a function of model complexity. Figure 12.25 Conceptual plot of interference error (dotted line), estimation error (dashed line), and overall prediction error (solid line) as a function of model complexity.
Calibration Measurement Residuals Plot (Model Diagnostic) The calibration spectral residuals shown in Figure 5-53 are still structured, but are a factor of 4 smaller than the residuals when temperature was not part of the model Comparing with Figure 5-51, the residuals structure resembles the estimated pure spectrum of temperature. Recall that the calibration spectral residuals are a function of model error as well as errors in the concentration matrix (see Equation 5.18). Either of these errors can cause nonrandom features in the spectral residuals. The temperature measurement is less precise relative to the chemical concentrations and, therefore, the hypothesis is that the structure in the residuals is due to temperature errors rather than an inadequacy in the model. [Pg.301]

FIGURE 16.33 Distribution of exhaust CO and hydrocarbon (HC) vehicle exhaust emissions as a function of model year in the United States (adapted from Stephens, 1994). [Pg.904]

In Sweden, three-way catalysts have been required on all cars since 1989, and tax incentives were offered to purchase such vehicles in the 1987 and 1988 model years. Figure 16.34 shows the CO and hydrocarbon exhaust emissions as a function of model year of gasoline-powered cars, measured using a remote-sensing technique (Sjodin, 1994). There is a large decrease in the emissions from 1987 to 1988 and 1989, supporting the effectiveness of these motor vehicle exhaust controls. [Pg.904]

In any case, the cross-validation process is repeated a number of times and the squared prediction errors are summed. This leads to a statistic [predicted residual sum of squares (PRESS), the sum of the squared errors] that varies as a function of model dimensionality. Typically a graph (PRESS plot) is used to draw conclusions. The best number of components is the one that minimises the overall prediction error (see Figure 4.16). Sometimes it is possible (depending on the software you can handle) to visualise in detail how the samples behaved in the LOOCV process and, thus, detect if some sample can be considered an outlier (see Figure 4.16a). Although Figure 4.16b is close to an ideal situation because the first minimum is very well defined, two different situations frequently occur ... [Pg.206]

F. O. Raineri, H. Resat and H. L. Friedman, Static longitudinal dielectric function of model molecular fluids, J. Chem. Phys., 96 (1992) 3068-84. [Pg.387]

A number of studies have been conducted to characterize the community structure and function of model ecosystems. Some examples are presented below, providing weight of evidence that some systems correspond closely to (parts of) natural held communities. [Pg.123]

Changes in the NMR spectrum for a two-site exchange system as a function of Model... [Pg.266]

Several factors must be considered in arriving at a level of sophistication of modeling consistent with industrial objectives. This is illustrated in Figure 2, where the cost of model development is expressed as a function of model sophistication. High level models require a smaller data base but are more expensive to develop and formulate. On the other hand, empirical models, although simpler to formulate and solve, rely heavily on an extensive data base which is costly to maintain. [Pg.137]

Figure 5-2 The plot of the misfit functional value as a function of model parameters tn. The vector of the steepest ascent, l(m ), shows the direction of "climbing on the hill" along the misfit functional surface. The intersection between the vertical plane P drawn through the direction of the steepest descent at point m and the misfit functional surface is shown by a solid parabola-type curve. The steepest descent step begins at a point 0(m ) and ends at a point 0(m +i) at the minimum of this curve. The second parabola-type curve (on the left) is drawn for one of the subsequent iteration points. Repeating the steepest descent iteration, we move along the set of mutually orthogonal segments, as shown by the solid arrows in the space M of the model parameters. Figure 5-2 The plot of the misfit functional value as a function of model parameters tn. The vector of the steepest ascent, l(m ), shows the direction of "climbing on the hill" along the misfit functional surface. The intersection between the vertical plane P drawn through the direction of the steepest descent at point m and the misfit functional surface is shown by a solid parabola-type curve. The steepest descent step begins at a point 0(m ) and ends at a point 0(m +i) at the minimum of this curve. The second parabola-type curve (on the left) is drawn for one of the subsequent iteration points. Repeating the steepest descent iteration, we move along the set of mutually orthogonal segments, as shown by the solid arrows in the space M of the model parameters.
Figure 5-4 The plot of the misfit functional value as a function of model parameters m. In the framework of the Newton method one tries to solve the problem of minimization in one step. The direction of this step is shown by the arrows in the space M of model parameters and at the misfit surface. Figure 5-4 The plot of the misfit functional value as a function of model parameters m. In the framework of the Newton method one tries to solve the problem of minimization in one step. The direction of this step is shown by the arrows in the space M of model parameters and at the misfit surface.
Catalyst deactivation in large-pore slab catalysts, where intrapaiticle convection, diffusion and first order reaction are the competing processes, is analyzed by uniform and shell-progressive models. Analytical solutions arc provid as well as plots of effectiveness factors as a function of model parameters as a basis for steady-state reactor design. [Pg.380]

The photoelectron emission microscopy (PEEM) investigations of Imbihl and coworkers [91] (Eigure 22) have nicely confirmed not only the potential-controlled variation in the work function of model Pt electrodes deposited on YSZ but also the Eermi-level pinning between Pt and YSZ. [Pg.722]

The proper comparison of correlation functions of models with experimental results is important and nontrivial. To avoid an all-too-common superficial comparison, refer to the work of Wright et al. [17,39]. [Pg.340]

Let Ml be a model containing pi parameters and let M2 be a model containing p2 parameters, which are supposed to be a subset of the parameters of model Mi, thus Pi > P2. The likelihood ratio statistic LR M.2Mi) = -21og[/(M2)//(Mi)], where /(Mj) and /(M2) are maximized likelihood functions of models Mi and Mj, respectively, and would follow a central distribution with pi > p2 degrees of freedom under the null hypothesis that additional parameters contained in the model Mj are aU zero. [Pg.232]

The Defense Priority Model (DPM) is designed to provide an estimate of the relative potential risk to human health and the environment from sites containing hazardous materials. The DPM evolved from a model called the Hazard Assessment Risk Model (HARM) developed by Oak Ridge National Laboratory from 1984-1986 for the Air Force. The automation of DPM was done first in KES(r) and then in Arity Prolog(r) for use on an IBM-PC/AT class machine. The computerized model has already become more sophisticated than the paper model and as development continues, it is possible to take advantage of additional expert system features. This paper is designed as a case study of DPM development and presents the reasons for the choice of expert system environment and its evolution, the current scope of the model, and planned additions that will increase the functionality of model in the future. The methodology used to evaluate this expert system is also described. [Pg.212]

Standard errors and confidence intervals for functions of model parameters can be found using expectation theory, in the case of a linear function, or using the delta method (which is also sometimes called propagation of errors), in the case of a nonlinear function (Rice, 1988). Begin by assuming that 0 is the estimator for 0 and X is the variance-covariance matrix for 0. For a linear combination of observed model parameters... [Pg.106]

The known properties of the PDF can be used to improve the solution a. Indeed, the modeled measurement errors f = F - f(a) for a a should reproduce the known statistical properties of measurement errors as closely as possible. The agreement of modeled f with known error distribution can be evaluated using the known PDF as a function of modeled errors P( f ) the higher P( f ) the closer the modeled f to the known statistical properties. Thus, the best solution a should result in modeled errors corresponding to the most probable error realization, i.e. to PDF maximum ... [Pg.70]

The analyses of the Auger spectra suggest the relative insensitivity of sulfur adsorption to temperature similar to the observations noted with the ceria-only model catalyst analysis. As previously indicated, the lack of discernible temperature dependencies may be attributed to the minimum reduction and oxidation temperatures for cerium oxides [15]. Because of the lack of discemable temperature dependencies, the data were averaged as a function of temperature and considered for pressure dependence. The pressure dependence on the extent of sulfur adsorption is clearly evident as a function of model catalyst composition. [Pg.251]

Determination of the junction point functionality of model networks turned out to be the most difficult task. It is impossible to experimentally measure/and so the effect of functionahty on network swelling can only be estimated by an indirect route. Computer simulation shows [125] that Q decreases with an increase in/and reaches a Hmited value when/> 10 (Fig. 1.6). Weiss et al. [126] confirmed experimentally such a profile of Q = (f) (Fig. 1.7). Swelling of real networks, indeed, proves to be smaller if a higher quantity of DVB molecules per Hving chain end is introduced into a precursor polystyrene solution however, more than five DVB molecules do not cause any further decrease in swelling (irrespective of the type of DVB isomers). [Pg.34]

Bethe and Salpeter [24] as well as Gell-Mann and Low [21] argue that a similar equation can be set up for a two-particle wave function. We assume we have a singlereference situation and let the Dyson equation act on the unperturbed wave function of model function (xo, Xq) (with to = t o = -oo). With... [Pg.109]

The archival function of models implies that they should also serve a valuable teaching function, as indeed they do in the physical sciences. Dynamic respiratory models, especially in their computerized interactive format, should be very valuable in teaching physiologists, medical students, and physicians the essence of normal and pathological pulmonary physiology. [Pg.13]


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