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Systematic component calculating

Overall uncertainty can be estimated by identifying all factors which contribute to the uncertainty. Their contributions are estimated as standard deviations, either from repeated observations (for random components), or from other sources of information (for systematic components). The combined standard uncertainty is calculated by combining the variances of the uncertainty components, and is expressed as a standard deviation. The combined standard uncertainty is multiplied by a coverage factor of 2 to give a 95% level of confidence (approximately). [Pg.297]

We now turn to a few specific examples of 4-coraponent basis sets and their applications. It should be realized that the derivation and testing of relativistic basis sets has not been a very systematic exercise. This is due to the fact that the calculations themselves are demanding, and in particular for the heavy elements, where the relativistic efiects are likely to be most noticable. Thus many basis sets have been developed and applied only for specific applications on one, or a limited number of molecules. Here we will review mostly those developments that have a direct bearing on the present state of molecular 4-component calculations. [Pg.282]

Within the Central Electricity Generating Board (CEGB), the "double contingency" principle is adopted in considering criticality in the CAGR fuel routes. Thus, at least two Independent low-probability events must occur before criticality can be reached. For clearances based on calculations a criterion is adopted that if one such event takes place, the cMculated Keff plus an appropriate allowance for uncertainties should be <0.95. This uncertainty allowance includes a systematic component and a random component, statistics plus data, etc., taken at the three standard deviation levels. Two computer codes are employed, the lattice code WIMS (Ref. 1) for survey work and the Monte Carlo cbcle MONK (Ref. 2) for... [Pg.589]

The goal of any forecasting method is to predict the systanatic component of danand and estimate the random component. In its most general form, the systematic component of demand data contains a level, a trend, and a seasonal factor. The equation for calculating the systematic component may take a variety of forms ... [Pg.182]

The calculation of A x) and Ax x ) can be done in a systematic manner. First the calculation of A x) is coded, and then this is differentiated with respect to each of the components of x to yield code for Ax x). An example of this procedure for the leapfrog method is given in Appendix B. [Pg.326]

The methodical elaboration is included for estimation of random and systematic errors by using of single factor dispersion analysis. For this aim the set of reference samples is used. X-ray analyses of reference samples are performed with followed calculation of mass parts of components and comparison of results with real chemical compositions. Metrological characteristics of x-ray fluorescence silicate analysis are established both for a-correction method and simplified fundamental parameter method. It is established, that systematic error of simplified FPM is less than a-correction method, if the correction of zero approximation for simplified FPM is used by preliminary established correlation between theoretical and experimental set data. [Pg.234]

The marching-ahead technique systematically overestimates when component A is a reactant since the rate is evaluated at the old concentrations where a and 0t A are higher. This creates a systematic error similar to the numerical integration error shown in Figure 2.1. The error can be dramatically reduced by the use of more sophisticated numerical techniques. It can also be reduced by the simple expedient of reducing At and repeating the calculation. [Pg.40]

A third class of compound methods are the extrapolation-based procedures due to Martin [5], which attempt to approximate infinite-basis-set URCCSD(T) calculations. In the Wl method [16] calculations are performed at the URCCSD and URCCSD(T) levels of theory with basis sets of systematically increasing size. Separate extrapolations are then performed to determine the SCF, URCCSD valence-correlation, and triple-excitation components of the total atomization energy at... [Pg.165]

The A scp term is calculated using the standard CP-method. At the correlated MP2 level, we have shown for several systems [7-10], that the AE terms are usually and systematically smaller than the dominant ( )+ Ecj) terms. The sum of these two terms provides a good approximation to the total interaction energy at the correlated level. It is important to emphasize that the AE values were obtained by making the difference with the values of the CP-corrected subsystems i.e. taking into consideration the "benefit effect" of the superposition of the basis set [3, 6]. As the charge-transfer components are of importance in the two-body interaction, (see a discussion in ref. 10), we will also investigate them separately for the three-body terms in the studied systems. [Pg.239]

Using the F ion as a prototype, the convergence of the many-body perturbation theory second-order energy component for negative ions is studied when a systematic procedure for the construction of even-tempered btisis sets of primitive Gaussian type functions is employed. Calculations are reported for sequences of even-tempered basis sets originally developed for neutral atoms and for basis sets containing supplementary diffuse functions. [Pg.283]

The second order correlation energy component, E Ne [IVe]) calculated for the ground state of the neon atom using systematic sequences of even-tempered basis sets of Gaussian functions designed for the Ne atom and designated [2nsnp] with n = 3,4,..., 13 are also collected in Table 1. [Pg.287]


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