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Mixture data, fitting

There are relatively few kinetic data on the Friedel-Crafts reaction. Alkylation of benzene or toluene with methyl bromide or ethyl bromide with gallium bromide as catalyst is first-order in each reactant and in catalyst. With aluminum bromide as catalyst, the rate of reaction changes with time, apparently because of heterogeneity of the reaction mixture. The initial rate data fit the kinetic expression ... [Pg.580]

Example Optimization of the Four Component Flare Mixture. The formulation of the previously discussed flare example was optimized by the Complex algorithm to yield the maximum intensity. The McLean and Anderson mixture equation (9), fit using normal component values and constraints, produced an optimum formulation at X . 5232, X2 . 2299, Xj . 1669, and X . 0800. The Gorman pseudocomponent equation for the same mixture data (7), constrained using... [Pg.63]

The mixture of these compounds at 0.5 xM per component was equilibrated with a 5 pM concentration of the protein target, then the reaction was quenched with excess staurosporine (100 pM) and analyzed using ALIS every 7 min. The measured protein-ligand complex MS responses were normalized and fit to the exponential decay function above, as shown in Fig. 3.16. The raw data fit the ex-... [Pg.147]

The value of (H) for each solute was determined in each solvent mixture over 10 different linear velocities that covered the normal practical range of velocities used in LC. Measurements at each velocity were taken in triplicate which resulted in a minimum of 180 values of (H) being taken for each solute. Each data set, from each solvent mixture, was fitted to each dispersion equation and the values for the respective constants (A), (B), (C), etc. calculated, together with the index of determination for each fitting, it ia seen that the data was sufficient in both quantity, and quality to be able to dentify the most appropriate dispersion equation with some confidence. The results obtained are shown in table 2. [Pg.138]

Kamal et al. 85) examined the stoichiometric mixture of BADGE and MPD in the temperature range 57-147 °C. The data were fitted to Equation (4-11) with m = n = 1. In a later study on the same system Sourour and Kamal86) used amine to epoxide equivalent ratios (B) of 1.0 and 1.5 and found that the data fitted the Eq. [Pg.136]

Sadovnikov [6] measured the change in pressure in explosions of hydrogen mixtures at p0 — 760 mm in a cylinder of 8 liters volume. His data on the cooling of the explosion products for different hydrogen mixtures all fit very well into an empirical formula containing the same constant for all mixtures ... [Pg.393]

Figure 9.15 Percent theoretical versus percent predicted by NIRS for SMZ Form I in Form II (a) binary mixture (R2 =0.9998, SEC = 0.63 at 1608/1784nm) (b) diluted with 60% lactose (R2 = 0.9999, SEC = 0.41 at 1608/2060 nm). Solid lines represent the data fit with a linear regression model. Reprinted from Patel etal. (2000)90 with permission from Elsevier. Figure 9.15 Percent theoretical versus percent predicted by NIRS for SMZ Form I in Form II (a) binary mixture (R2 =0.9998, SEC = 0.63 at 1608/1784nm) (b) diluted with 60% lactose (R2 = 0.9999, SEC = 0.41 at 1608/2060 nm). Solid lines represent the data fit with a linear regression model. Reprinted from Patel etal. (2000)90 with permission from Elsevier.
Furthermore, quantitative structural phase analysis, for instance, is important for investigations of solid catalysts, because one frequently has to deal with more than one phase in the active or precursor state of the catalyst. Principal component analysis (PCA) permits a quantitative determination of the number of primary components in a set of experimental XANES or EXAFS spectra. Primary components are those that are sufficient to reconstruct each experimental spectrum by suitable linear combination. Secondary components are those that contain only the noise. The objective of a PCA of a set of experimental spectra is to determine how many "components" (i.e., reference spectra) are required to reconstruct the spectra within the experimental error. Provided that, first, the number of "references" and, second, potential references have been identified, a linear combination fit can be attempted to quantify the amount of each reference in each experimental spectrum. If a PCA is performed prior to XANES data fitting, no assumptions have to be made as to the number of references and the type of reference compounds used, and the fits can be performed with considerably less ambiguity than otherwise. Details of PCA are available in the literature (Malinowski and Flowery, 1980 Ressler et al., 2000). Recently, this approach has been successfully extended to the analysis of EXAFS data measured for mixtures containing various phases (Frenkel et al., 2002). [Pg.432]

The advantage of multiple regression is that methods are established, well described, and available in almost all statistical sofware packages, and that the fitting procedures have been well developed (Neter et al. 1996). Furthermore, the complete n + 1 dimensional concentration-response surface is fitted to the complete data set, taking into account that the parameters of the concentration-response relationships of the individual mixture components are actually predictors for the complete mixture data set. The model allows individual concentration-response curves to have their unique slopes. [Pg.138]

The small value of RMS %6P showirfor 363.15 K (90°C) iirdicates both the suitability of the van Laar equatioir for correlation of the VLE data and the capability of the equation of state to reproduce the data. A direct fit of these data with the van Laar equation by the ganmra/phi procedure yields RMS % 6 P = 0.19. The results at 423.15 to473.15K(150 and 200°C) are based oirly on vapor-pressuredata for the pure species and on mixture data at lower temperatures. Tlre quality of prediction is indicated by the P-x-y diagram of Fig. 14.10, wlrich reflects the uncertainty of the data as well. [Pg.534]

Zhou et al. [44] used this model to compare the experimental band profiles of mixtures of the enantiomers of 1-indanol on a cellulose derivative and the profiles calculated using the FOR model. The single component data fitted very closely to the Bilangmuir model. A competitive Bilangmuir model was derived from these... [Pg.760]

In principle the surface complexation model is suitable for small ions, but other applications can be also found in literature. For example, humic acid and related substances were modeled as a mixture of four to five monoprotic acids forming different types of surface complexes (electrostatic position, number of protons released) [102], However, such approach can be only considered as data fitting model. [Pg.697]

The idea of competitive adsorption on pair-sites has also been used to describe the interaction of Ho and H2O with magnetite ( ). When isotherms were collected using M2/H2O mixtures following the same approach as discussed above, it was found that the data fit a model where H2 adsorbed dissociatively and H2O adsorbed associative-ly, with both species competing for pair-sites. These studies were conducted at water-gas shift reaction temperatures (e.g., 650 K) and as for the adsorption of CO and CO2, only a fraction of the magnetite surface was capable of adsorbing H2 and H2O. [Pg.328]

A Gennan academic group has provided a software package called PE [43] that may be used to perform phase-equilibrium and density calculations with many different equations of state and mixing rules. Parameters are built in for a limited number of components and mixtures, but the software also has the capability to fit parameters to pure-component and mixture data. [Pg.12]

Bofh EOS and activity-coefficient methods require binary interaction parameters. In process simulation software, the necessary parameters may already be built into a data bank. Sometimes, parameters for the system of interest may be found in the literature. If not, however, the parameters must be fitted to mixture data. [Pg.14]

Equations (4.345) and (4.346) are the van Laar activity-coefQcient equations that are used for fitting data by adjusting the parameters A21 and A 2- Although these parameters are derived from pure-component parameters, as shown in Equations (4.347) and (4.348), they are, nevertheless, considered mixture-specific binary interaction parameters and are thus indicated with subscripts because they are determined by fitting binary mixture data. Equations (4.347) and (4.348), while showing the source of derivation of the parameters, are not used for their determination. [Pg.332]

The Sanchez-Lacombe EOS is a mean-field equation that does not directly account for hydrogen bonding and polar interactions. But Sanchez and Balazs (1989) show that it is possible to mimic the trends in the experimental data if the mixture parameters are allowed to vary with temperature. Therefore, when dealing with polar polymers or polar solvents, it may be necessary to force the mixture parameters to vary with temperature to obtain a representative fit of experimental data. In some cases, improved fits of the Sanchez-Lacombe equation to experimental data can also be obtained if the characteristic parameters of the solvent and the solute are obtained by fitting P-V-T data in the region where the mixture data were obtained. The improved fit of mixture data with characteristic parameters of the light component obtained in this manner is usually at the expense of a poor fit of the vapor pressure curve. [Pg.127]

Figure 5.15 A comparison of the calculated (lines) and experimental (symbols) pressure-composition data for the naphthalene-xenon system using the Peng-Robinson equation with two mixture parameters fitted to the SLV line (McHugh et al., 1988). Figure 5.15 A comparison of the calculated (lines) and experimental (symbols) pressure-composition data for the naphthalene-xenon system using the Peng-Robinson equation with two mixture parameters fitted to the SLV line (McHugh et al., 1988).
Here a new parameter jiry, known as the binary interaction parameter, has been introduced to result in more accurate mixture equation-of-state calculations. This parameter is found by fitting the equation of state to mixture data (usually vapor-liquid equilibrium data, as discussed in Chapter 10). Values of the binary interaction parameter k - that have been reported for a number of binary mixtures appear in Table 9.4-1. Equations 9.4-8 and 9.4-9 are referred to as the van der Waals one-fluid mixing rules. The term one-fluid derives from the fact that the mixture is being described by the same equation of state as the pure fluids, but with concentration-dependent parameters. [Pg.423]

Equations 14 and 15 define vq and Kq as the dimensionless cross-inter-action constants. At the present stage they have to be determined from fitting mixture data. [Pg.223]


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See also in sourсe #XX -- [ Pg.220 , Pg.221 ]




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Data fitting

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