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Determination from experimental data

Determine from experimental data the Reynolds number exponent for the s) stem, or use information in Figure 5-40 if the systems of Table 5-8 can be considered similar, use proper coefficients and solve for outside film coefficient, hg. [Pg.333]

The parameters A, B,. .., depend on temperature but not on pressure, and must be determined from experimental data for the binary mixture. [Pg.169]

Equations (13) and (14) comprise the complete theoretical model for predicting polymerization conversion (C) from the fractional areas data from the GC. However, the two parameters and g need to be determined from experimental data. [Pg.299]

Like its chemical potential, the activity of an individnal ion cannot be determined from experimental data. For this reason the parameters of electrolyte activity % and mean ionic activity are nsed, which are defined as follows ... [Pg.40]

Rate equations are differential equations of the general form dcjdt = kf (Cj, c2,... cn) = kf (.c), where i is the particular product or reactant, and C is its molar concentration (NJV). The constant k goes by a number of names such as velocity coefficient, velocity constant specific reaction rate, rate constant, etc., of the particular reaction. Physically, it stands for the rate of the reaction when the concentrations of all the reactants are unity. The function fc) and the rate constant k are determined from experimental data. [Pg.295]

A mechanistic model for the kinetics of gas hydrate formation was proposed by Englezos et al. (1987). The model contains one adjustable parameter for each gas hydrate forming substance. The parameters for methane and ethane were determined from experimental data in a semi-batch agitated gas-liquid vessel. During a typical experiment in such a vessel one monitors the rate of methane or ethane gas consumption, the temperature and the pressure. Gas hydrate formation is a crystallization process but the fact that it occurs from a gas-liquid system under pressure makes it difficult to measure and monitor in situ the particle size and particle size distribution as well as the concentration of the methane or ethane in the water phase. [Pg.314]

Group contribution techniques are based on the concept that a particular physical property of a compound can be considered to be made up of contributions from the constituent atoms, groups, and bonds the contributions being determined from experimental data. They provide the designer with simple, convenient, methods for physical property estimation requiring only a knowledge of the structural formula of the compound. [Pg.314]

For each binary pair, there are two adjustable parameters that must be determined from experimental data, that is, (uy - ujj), which are temperature dependent. Pure component properties rl and ql measure molecular van der Waals volumes and surface areas and have been tabulated6. [Pg.63]

The errors that result from the use of average transport coefficients are not particularly serious. The correlations that are normally employed to predict these parameters are themselves determined from experimental data on packed beds. Therefore, the applications of the correlations and the data on which they are based correspond to similar physical configurations. [Pg.475]

The values of a A, and EA must be determined from experimental data to establish the form of the rate law for a particular reaction. As far as possible, it is conventional to assign small, integral values to a2, etc., giving rise to expressions like first-order, second-order, etc. reactions. However, it may be necessary to assign zero, fractional and even negative values. For a zero-order reaction with respect to a particular substance, the rate is independent of the concentration of that substance. A negative order for a particular substance signifies that the rate decreases (is inhibited) as the concentration of that substance increases. [Pg.65]

Model parameters are usually determined from experimental data. In doing this, sensitivity analysis is valuable in identifying the best experimental conditions for the estimation of a particular model parameter. Sensitivity analysis is easy effected with MADONNA, and sensitivity analysis is also provided in other more advanced software packages, such as ACSL-OPTIMIZE. [Pg.87]

In this paper, a set of approximate solutions to model equations will be presented in a way intended to make clear which parameters can be determined from experimental data. This leads to a methodology of extracting a maximum amount of information from V o/o o/pH data. [Pg.80]

Surface site densities used in the computation of the oxide site concentrations presented in this paper were determined by either rapid tritium exchange or acquired from published values (18). Reported total site densities for hydrous metal oxides show relatively little variation generally they range by less than a factor of 3. Since [M], [SOM], [H] and x are known or can be determined from experimental data, uncertainties in estimates of the total site concentration are directly translated into uncertainties in the calculated partitioning coefficient. [Pg.170]

The rate law must be determined from experimental data. Review how to determine the rate law from kinetics data. [Pg.210]

RSEs for a broader selection of substituted methyl radicals, as well as MADs and MDs from experiment and CBS-RAD values, are presented in Tables 6.12 and 6.13. We noted in the previous section that our highest-level procedure, namely Wl, gives accurate BDEs, and this observation carries over to the RSEs calculated at this level. The MAD from experiment for the Wl method is 3.1 kJ/mol. The Wl RSEs tend to be slightly lower than those determined from experimental data [MD(Exp.) of -2.2 kJ/mol]. [Pg.178]

However, in this formulation, G /8 is simply a fitted parameter, since there is no rigorous molecular definition for this form of the interfacial energy. In addition, this model suffers the same problem as do other continuum models, in that it contains parameters that must be determined from experimental data and that cannot be estimated a priori from molecular techniques. [Pg.71]

Values of a diffusion coefficient matrix, in principle, can be determined from multicomponent diffusion experiments. For ternary systems, the diffusivity matrix is 2 by 2, and there are four values to be determined for a matrix at each composition. For quaternary systems, there are nine unknowns to be determined. For natural silicate melts with many components, there are many unknowns to be determined from experimental data by fitting experimental diffusion profiles. When there are so many unknowns, the fitting of experimental concentration... [Pg.257]

This equation includes the particular cases of an nth order reaction model with g(a) = 1, and the autocatalytic model with g(a) = 1 + la, where / is the autocatalysis intensity. In general, the form of g(a) must be determined from experimental data. [Pg.243]

To reduce the number of parameters in the kinetic equations that are to be determined from experimental data, we used the following considerations. The values klt k2, and k4 that enter into the definition of the constant L, (236), are of analogous nature they indicate the fraction of the number of impacts of gas molecules upon a surface site resulting in the reaction. So the corresponding preexponential factors should be approximately the same (if these elementary reactions are adiabatic). Then, since k1, k2, and k4 are of the same order of magnitude, their activation energies should be almost identical. It follows that L can be considered temperature independent. [Pg.238]

In contrast to the just discussed classical models [43,44], authors of works [38, 39] treated the problem of the dynamical polarizability ay(carbon cage quantum-mechanically, utilizing the 5-potential model concept, where the C60 cage is simulated by the Dirac 5-potential, V(r) = —Vo8(Rc—r). However, instead of calculating cy( >) directly, the latter was determined from experimental data on the C60 photoabsorption cross section a (o>) [60, 61] with the help of the dispersion relations for the real Re ay and imaginary Imay parts of the dipole polarizability ay ( >) ... [Pg.30]


See other pages where Determination from experimental data is mentioned: [Pg.20]    [Pg.491]    [Pg.345]    [Pg.542]    [Pg.202]    [Pg.871]    [Pg.130]    [Pg.358]    [Pg.104]    [Pg.545]    [Pg.75]    [Pg.77]    [Pg.62]    [Pg.66]    [Pg.158]    [Pg.202]    [Pg.252]    [Pg.120]    [Pg.321]    [Pg.319]    [Pg.233]    [Pg.491]    [Pg.567]    [Pg.248]    [Pg.403]    [Pg.297]    [Pg.63]    [Pg.331]    [Pg.301]   
See also in sourсe #XX -- [ Pg.90 ]




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