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Correction schemes

LT installations may be subject to frequent load variations and inductive switchings. It will be more desirable in such cases to provide them with an automatic p.f. correction scheme than manual correction. It may be... [Pg.766]

The energies of several intermediates that could arise from the reaction of diazoazoles with alkenes have been estimated [90JCS(P2)1943] by means of the MNDO, AMI SCF-MO, and ab initio methods. The calculations suggest a 1,4-dipole behavior (also viewed as a 1,7-dipole) for most diazoazoles when reacting with electron-rich alkenes it is believed that the approach between 438 and alkenes is asynchronous. On the basis of that study, some errors have been corrected (Scheme 95). [Pg.94]

Certain features of the reaction schemes manifest themselves in the rate law in a regular way. These features guide the investigator to one or more mechanisms consistent with the data. The same considerations allow one to reject certain alternatives. Listed here is a set of rules, or more properly clues, that are useful guides to the correct scheme. Each is accompanied by examples as to how they can be applied. [Pg.127]

A pressure correction scheme based on such an approximation is known as the SIMPLEC algorithm [89]. The SIMPLEC algorithm does not require under relaxation of the pressure correction, is efficient and has found widespread applications. [Pg.159]

Vahron, P., Vibok, A., Mayer, I., 1993, Comparision of a Posteriori and a Priori BSSE Correction Schemes for SCF Intermolecular Energies , J. Comput. Chem., 14, 401. [Pg.303]

In 1988, Becke proposed a gradient-corrected scheme for the exchange functional ( B88 ), ensuring that this should have the correct asymptotic limit (1/r) as oo [16] ... [Pg.118]

The density functional methods assessed in this study (B3LYP, BLYP, and LDA) all perform much worse for the enthalpies of formation of the larger molecules in the G3/99 set. This is due to a cumulative effect in the errors for the larger molecules in this test set. The errors are found to be approximately proportional to the number of pairs of electrons in the molecules but the methods are not improved significantly when a higher-level correction such as that used in G2 or G3 theory is added the DFT methods. Further correction schemes may be necessary to improve the performance of density functional methods for large molecules. [Pg.95]

Different baseline correction methods vary with respect to the both the properties of the baseline component d and the means of determining the constant k. One of the simpler options, baseline ojfset correction, nses a flat-line baseline component (d = vector of Is), where k can be simply assigned to a single intensity of the spectrum x at a specific variable, or the mean of several intensities in the spectrum. More elaborate baseline correction schemes allow for more complex baseline components, such as linear, quadratic or user-defined functions. These schemes can also utilize different methods for determining k, such as least-squares regression. [Pg.370]

Data for 31 elements can be rapidly determined but result in some interferences between elements. No spectral curve fitting or matrix (ZAF) correction schemes were used in this survey study. ZAF correction does not seem to markedly aid the cluster analysis... [Pg.125]

Early claims to have prepared 4-hydroxy-4H-imidazoles from benzami-dine hydrochloride (27) and 2,3-butanedione (28), or phenylethane-1,2-dione (29), appear to be substantially correct (Scheme 9). Although this work has not been repeated, analogous intermediates have been observed subsequently in related reactions. Waugh and co-workers recognized that 30 might well have been the rearranged isomer 31. (see Section IV,A,l,b). [Pg.420]

A somewhat more chemically based empirical correction scheme is the bond-additivity correction (BAG) methodology. In the BAG-MP4 approach, for instance, the energy of a molecule is computed as... [Pg.243]

In DFT, Koopmans theorem does not apply, but the eigenvalue of the highest KS orbital has been proven to be the IP if the functional is exact. Unfortunately, with the prevailing approximate functionals in use today, that eigenvalue is usually a rather poor predictor of the IP, although use of linear correction schemes can make this approximation fruitful. ASCF approaches in DFT can be successful, but it is important that the radical cation not be subject to any of the instabilities that can occasionally plague the DFT description of open-shell species. [Pg.331]

The G2 and G3 methods go beyond extrapolation to include small and entirely general empirical corrections associated with the total numbers of paired and unpaired electrons. When sufficient experimental data are available to permit more constrained parameterizations, such empirical corrections can be associated with more specific properties, e.g., with individual bonds. Such bond-specific corrections are employed by the BAG method described in Section 7.7.3. Note that this approach is different from those above insofar as the fundamentally modified quantity is not Feiec, but rather A/7. That is, the goal of the method is to predict improved heats of formation, not to compute more accurate electronic energies, per se. Irikura (2002) has expanded upon this idea by proposing correction schemes that depend not only on types of bonds, but also on their lengths and their electron densities at their midpoints. Such detailed correction schemes can offer very high accuracy, but require extensive sets of high quality experimental data for their formulation. [Pg.371]

Friesner (2002) have reported average errors of about 150 mV for various organometallic species in different organic solutions. As already discussed for pA gS, still better accuracy in redox potentials can often be achieved through the use of isodesmic equations or functional-group-speciflc correction schemes (see, for example, Winget et al. 2000). [Pg.415]

We will not carry this analysis further, since in writing the correction function on the form e(z,y) we have not explicitly included the dependence on derivatives of f. However, we note that this section provides reason for a classification of defect correction schemes by a new concept, called convergence order. A procedure which guarantees the asymptotic inequalities (within some disk)... [Pg.18]

Now we want to apply this to some simple defect-correction schemes. Simplest is of course... [Pg.30]

B is correct. Scheme 1, step 1 shows an anhydride reacting with an aromatic ring in the presence of A1C1- to form a carboxylic acid and a ketone. This reaction has the same form. This is a Friedel-Crafts reaction. [Pg.135]

Recently, a software approach using multiple polystyrene absorption bands was developed for infrared spectroscopy.30 In this section, we present a similar method that was developed concurrently, which calibrates on multiple Raman peaks to generate a curvature map. This curvature mapping method shows significant improvement over first-order correction schemes. [Pg.400]

Scheme 3 in [179] is incorrect the correct Scheme can be found in [180] (Scheme 2 therein) or in this review (Scheme 33 herein). [Pg.17]

The manufacturer provides specifications for the performance of the OMA, including linearity of counts as a function of intensity and the geometric distortion and channel-to-channel crosstalk of the vidicon. However, the user needs methods for verifying the performance of his OMA. operating with his system. This information is needed both for designing correction schemes if distortion is found and for determining whether further improvements in the system are needed. Ideally the methods should be simple so that the testing can be performed on a routine basis. [Pg.324]

Alternative background correction schemes can be incorporated for more complicated situations. For example, if the background signal is curved and multiple valleys are available in the spectrum, it may be possible to fit a polynomial function... [Pg.80]

A more fundamental problem with DFT methods is that gradient corrections to the local-density approximation are always required to give reasonable reaction barrier heights, as the LDA always overestimates the binding of the free molecule. There are, sadly, many variations on the gradient correction scheme, and which to choose is often a question of which is known to work best for the atomic species present. Estimates of barrier heights can vary considerably according to the choice of GGA [52],... [Pg.35]

Likura H, Tsuneda T, Yanai T, Hirao K (2001) A long-range correction scheme for generalized-gradient-approximation exchange functionals, J Chem Phys, 115 3540—3544... [Pg.199]


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Correction schemes asymptotic corrections

Correction schemes electron correlation

Correction schemes exchange-correlation

Correction schemes orthogonalization

Density functional theory conventional correction schemes

Density functional theory correction schemes

Externally corrected MMCC schemes

Possible and correct invisible signatures in existing schemes

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