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Parameter cases

In table 2 and 3 we present our results for the elastic constants and bulk moduli of the above metals and compare with experiment and first-principles calculations. The elastic constants are calculated by imposing an external strain on the crystal, relaxing any internal parameters (case of hep crystals) to obtain the energy as a function of the strain[8]. These calculations are also an output of onr TB approach, and especially for the hep materials, they would be very costly to be performed from first-principles. For the cubic materials the elastic constants are consistent with the LAPW values and are to within 1.5% of experiment. This is the accepted standard of comparison between first-principles calculations and experiment. An exception is Sr which has a very soft lattice and the accurate determination of elastic constants is problematic. For the hep materials our results are less accurate and specifically in Zr the is seriously underestimated. ... [Pg.257]

The computation of the above surface in the parameter space is not trivial. For the two-parameter case (p=2), the joint confidence region on the krk2 plane can be determined by using any contouring method. The contour line is approximated from many function evaluations of S(k) over a dense grid of (k, k2) values. [Pg.179]

It is important to note that wastewater is subject to great variability in terms of its components and processes. Procedures 1 to 4, therefore, correspond to a typical analytical method for the determination of the characteristic components and the stoichiometric and kinetic parameters. Cases where the procedure described in Sections 7.2.1-1.2 A is either difficult or not feasible to follow may exist. A detailed knowledge on wastewater characteristics and experience from laboratory and modeling studies may be crucial in such situations for finding alternative variants of the procedures 1 to 4. [Pg.182]

Instead of developing a program that performs the task as just explained, we move to the 2-parameter case. Subsequently, we generalise to the np-parameter case and then we analyse the relationship with the Newton-Gauss algorithm for least-squares fitting. [Pg.199]

For the 2-parameter case, consider a function of the kind represented in Figure 4-5, where we plotted the sum of squares as a function of two parameters. In analogy to Figure 4-56, we start with an initial guess for the parameters pi and p2 and at this point compute the first and second derivatives... [Pg.200]

Equation (7.197) can be solved using any of the standard methods such as bisection or Newton s method. However it is more instructive to solve it graphically by plotting G(y) and R(y) versus y as shown in Figure 4 (A-2) for a parameter case with maximally three steady states. [Pg.555]

Both the Parameter and Reconcile cases determine (calculate) the same set of parameters. However, these cases do not get the same values for each parameter. A Parameter case has an equal number of unknowns and equations, therefore is considered "square" in mathematical jargon. In the Parameter case, there is no objective function that drives or affects the solution. There are typically the same measurements, and typically many redundant measurements in both the Parameter and Reconcile case. In the Parameter case we determine, by engineering analysis beforehand (before commissioning an online system for instance) by looking at numerous data sets, which measurements are most reliable (consistent and accurate). We "believe" these, that is, we force the model and measurements to be exactly the same at the solution. Some of these measurements may have final control elements (valves) associated with them and others do not. The former are of FIC, TIC, PIC, AIC type whereas the latter are of FI, TI, PI, AI type. How is any model value forced to be exactly equal to the measured value The "offset" between plant and model value is forced to be zero. For normally independent variables such as plant feed rate, tower... [Pg.128]

For the CO2 capture system, the parameter cases update all significant equipment performance to match observed data. The primary performance of this system is the CO2 absorber slip and the energy required to regenerate the solution to semilean and lean solution quality. The model can be made to match observed performance in several ways. Measurements are available for the lean and semilean... [Pg.146]

Note that S(b) is given directly below the constant b (i.e., the X coefficient ) in the output of Fig. 2. Curiously, S a) is usually not given in the simplest Lotus 1-2-3 and Quattro Pro Regression formats. For the simple two-parameter case, it can be calculated from... [Pg.75]

For the trivial one-parameter case in which the parameter to be determined is the arithmetic mean,... [Pg.679]

Eor the two-parameter case of the linear relationship we may apply Eqs. (28) and (40) to the estimation of the standard deviations in the intercept uq and the slope of the corresponding straight line. Erom Eq. (22) we have... [Pg.679]

Knowledge of estimated standard deviations is not by itself very useful, especially when they are unthinkingly accepted without regard to the validity of the model and of the weighting scheme. Assuming that these aspects are assuredly satisfactory, we are usually more interested in confidence limits for the parameters at a stated probability level P, as in the one-parameter case of the algebraic mean discussed in the section on confidence limits in Chapter II. Equation (11-29) for the one-parameter case applies also to the n-parameter case for 95 percent confidence,... [Pg.679]

The general treatment of least squares presented by Deming eliminates these problems and is not much more complicated than the closed form of the equations given above. In addition, the transformation of a nonlinear equation to a linear one can be accomplished quite simply with the proper weights. We will not present a derivation of the procedure since it has been described previously. We will simply present examples of the steps in the procedure for a two-parameter case. The extension to more than two variables is simple since there is no increase in the size of the matrix to be inverted. The extension to more than two parameters does involve an increase in the size of the matrix but is apparent. [Pg.342]

For this one parameter case, the 100 (1 — Ctr) percent confidence interval becomes... [Pg.778]

The simplex optimization is a very simple and robust technique for optimizing any function of a moderate number of variables. Only the function values for different variable sets are needed. In this case, the function to be optimized is the penalty function, and the variables to vary are the force field parameters. To initialize a simplex optimization of N parameters, one must first select Ai + 1 linearly independent trial sets. A very simple way to achieve this is to start with the initial parameter estimate and then to vary each parameter in turn by a small amount, yielding N new trial sets. This is illustrated for a two-parameter case in Fig. 7. With two parameters, the shape of the simplex is a triangle, with three parameters a tetrahedron, and so on. [Pg.23]

Catalyst optimization, application scope, reaction parameters, case studies Microorganism screening, recombinant biocatalyst, reaction parameters, product isolation... [Pg.8]

Compute the partial differentials and the standard deviations for the one-parameter case... [Pg.446]

Compute the partial differentials for the multi-parameter case Else... [Pg.447]

D Yu Murzin, T Salmi. Isothermal multiplicity in catalytic surface reactions with coverage dependent parameters case of polyatomic species. Chem. Eng. Sci. 51 55-62, 1996. [Pg.605]

This familiar procedure, and in particular the availability of confidence limits from its application, has created the expectation that comparable values can be reported in all fittings, regardless of the complexity of the governing dependencies or the extent of parameter correlation in a given case. The search for a means to make such quantities universally available has led to a number of attempts (see Bates and Watts (1988)) to calculate error limits in non-linear, multi-parameter cases, ranging from the simplistic to the highly idiosyncratic. [Pg.211]

These results highlight a) Photodegradation reaction rates should be defined on the basis of phenomenologically meaningful parameters, case of W rr, b) Reaction rate evaluation is a task that should be developed carefully, accounting for possible nonidealities in the photocatalytic reactor such as particle wall fouling. [Pg.10]

As is done in the GL-theory for a single even-parity order parameter, we write the free energy density difference between the superconducting state and the norma state as an expansion in even powers of the complex gap function A(k), which is related to the anomalous thermal average of the microscopic theory [28] where c is the electron annihilation operator with wave vector k and spin t. However, for the multiple-order parameter case we must expand A(k) as a linear combination of the angular momentum basis functions Yj(k)),... [Pg.19]

Parameter Case A Case B Case Cl Case C2 Case D1 Case D2... [Pg.2082]

We will call Cases to the group of simulations realized under the same parameters. Case 1 corresponds to the gain constants found by the CRA applying only the decomposition reaction in experiment No. 6 these gains obtained the smallest velocity error (8.13e-005). [Pg.37]


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See also in sourсe #XX -- [ Pg.128 ]




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