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Screening approximation

In astronomy, we are interested in the optical effects of the turbulence. A wave with complex amplitude U(x) = exp[ irefractive index, resulting in a random phase structure by the time it reaches the telescope pupil. If the turbulence is weak enough, the effect of the aberrations can be approximated by summing their phase along a path (the weak phase screen approximation), then the covariance of the complex amplitude at the telescope can be shown to be... [Pg.6]

The material presented here is a compilation obtained by critically screening approximately 20,000 references from the literature (mainly from the Petroleum Abstracts Data Base and Patent Data Bases). Only materials that are accessible to the public have been included. The literature was screened from a chemist s point of view. Unfortunately several papers and patents did not disclose the chemical nature of the additives that are proposed for certain applications. In most cases it was not possible to learn the components by looking up cross-references and other sources. Papers of this kind are useless and have been omitted from the reference list. Research and procedures that are obviously not working, as well as wonder additives that are supposedly good for everything you can imagine, have also been left out. [Pg.508]

Various theoretical methods (self-consistent field molecular orbital (SCF-MO) modified neglect of diatomic overlap (MNDO), complete neglect of differential overlap (CNDO/2), intermediate neglect of differential overlap/screened approximation (INDO/S), and STO-3G ab initio) have been used to calculate the electron distribution, structural parameters, dipole moments, ionization potentials, and data relating to ultraviolet (UV), nuclear magnetic resonance (NMR), nuclear quadrupole resonance (NQR), photoelectron (PE), and microwave spectra of 1,3,4-oxadiazole and its derivatives <1984CHEC(6)427, 1996CHEC-II(4)268>. [Pg.398]

Mass spectrometry enables the type of direct analyses described, but it does have its limitations. Online operation forces detection at infusion concentrations, in salty buffer and under complex mixture conditions. General ion suppression results from the buffer and mixture components, and mixture complexity can tax the resolution of even the best mass spectrometers. Increasing compound concentration is not the answer, as this leads to problems of solubility and increased compound consumption. We have found that the online method can work successfully for up to 100 compounds per analysis, but the false negative rate becomes appreciable [21]. As an alternative for ligand discovery purposes, we have developed a FAC-LC/MS system in which FAC effluent is sampled and analyzed by LC/MS [19]. This system offers the ability to concentrate mixture components and introduces another dimension to the data in order to tolerate more complex mixtures (Fig. 6.9). Using this system, we have screened approximately 1000 modified trisaccharide acceptor analogs targeting immobilized N-... [Pg.230]

The efficient screening approximation means essentially that the final state of the core, containing a hole, is a completely relaxed state relative to its immediate surround-ing In the neighbourhood of the photoemission site, the conduction electron density of charge redistributes in such a way to suit the introduction of a core in which (differently from the normal ion cores of the metal) there is one hole in a deep bound state, and one valence electron more. The effect of a deep core hole (relative to the outer electrons), may be easily described as the addition of a positive nuclear charge (as, e.g. in P-radioactive decay). Therefore, the excited core can be described as an impurity in the metal. If the normal ion core has Z nuclear charges (Z atomic number) and v outer electrons (v metallic valence) the excited core is similar to an impurity having atomic number (Z + 1) and metalhc valence (v + 1) (e.g., for La ion core in lanthanum metal, the excited core is similar to a Ce impurity). [Pg.214]

DCIS now forms some 20% of all breast cancers diagnosed by screening. Approximately 80% of DCIS is picked up due to microcalcifications (see later in chapter). Once the radiologist has identified suspicious calcifications, these are biopsied, so that architectural and cytological information can be obtained. [Pg.330]

Grow HeLa cells in 150-mm tissue-culture dishes so that they are 70-80% confluent the day before screening. Approximately 2 109 cells (10-12 150-mm plates)... [Pg.191]

Figure 6.9 Diagram of instrumental configuration of the LC/MS system used for annually screening approximately 100,000 natural product extracts. (Gilbert and Lewer 1998.)... Figure 6.9 Diagram of instrumental configuration of the LC/MS system used for annually screening approximately 100,000 natural product extracts. (Gilbert and Lewer 1998.)...
High expression levels of soluble and active Mur enzymes in E. coli enabled the rapid purification of large amounts of enzyme for the high-throughput screen. Approximately 120 mg of purified Mur enzymes could be purified from each liter of expression culture. [Pg.293]

In the route to BO-2727 (18), a broad-spectrum P-methyl carbapenem being developed by Merck, a bioreduction catalyzed by the fungus Mortierella alpina MF 5534 is used to form a precursor (7 )-P-hydroxy ester 19 (Scheme 19.12).102 This fungal culture was a result of screening approximately 260 strains of microorganisms and resulted in the production of gram quantities of product with a de of >98%. [Pg.367]

The extra electron that has been added to the crystal will be attracted to the impurity nucleus just as an electron is attracted to a proton in free space, but the attraction is greatly reduced by the dielectric constant. In addition, the electron will behave as if its mass is very small, as will be seen in Chapter 6. Both effects expand the radius of the bound orbital so that it lies mainly in the region where the dielectric screening approximation is good, and so that the binding may be only of the order of 0.01 electron volts at normal temperature these impurity states will be empty and the corresponding electrons will move freely through the crystal. In Chapter 6 we shall examine such states. [Pg.128]

Having obtained the zero frequency limit of the dynamic polarizability i.e., a = Iin, o7 (—wja ), we use a simplified approach to evaluate the screened dynamic response. This is necessary, since the expression given above, Eq. (40), for the polarizability neglects the induced collective effects essentially due to direct and exchange terms of the Coulomb interaction. To treat this screening approximately, we have used the simplified approach of Bertsch et al. [96] to include the induced electron interaction in the Ceo molecule, by a simple RPA type correction [92,95]... [Pg.20]

An important point is the existence of a critical magnitude of this parameter, X 4, that weakly depends on the other plasma parameters. It is interesting to note that this critical magnitude is much larger than unity, which means that the linear screening approximation is well accurate even for the the expansion parameter (2) ranging somewhere between 4 and 5. [Pg.297]

Synthesized and screened approximately twenty electrolyte and monomer compounds for high temperature membranes... [Pg.391]

After screening approximately 70 dyes, Peterson et al. [114] foimd perylene dibutyrate (Colour Index No. 59 075) adsorbed on Amberlite XAD-4 resin beads to be a most useful probe It has excitation and emission maxima of 468 and 514 mn, respectively, is stable and is effl-... [Pg.196]

Gurgel etalS applied the multi-tiered screening approach to a-lactalbumin (a-La), a whey protein of significance to the food industry. Eighteen sequences were identified as potential a-La binders by screening approximately 2% of a solid phase hexameric peptide... [Pg.74]

INDO/S Intermediate neglect of differential overlap/screened approximation. [Pg.116]

In response to the unsuccessful PANIS/polystyrene blends, other polymers were examined. In addition, in order to reduce the particle size and improve the consistency of the powder, PANIS and the host polymer were ground to a fine powder. The polymer was placed into a small plastic rotary tumbler with nickel shot. Ten to twelve grams of powder were masticated for approximately thirty minutes, resulting in a very uniform powder. The powder was then separated from the shot using a fine mesh screen (approximately 42 mesh or 0.350mm opening). [Pg.177]


See other pages where Screening approximation is mentioned: [Pg.329]    [Pg.329]    [Pg.97]    [Pg.83]    [Pg.12]    [Pg.255]    [Pg.125]    [Pg.126]    [Pg.128]    [Pg.140]    [Pg.56]    [Pg.139]    [Pg.84]    [Pg.535]    [Pg.739]    [Pg.107]    [Pg.40]    [Pg.310]    [Pg.254]    [Pg.24]    [Pg.557]    [Pg.425]    [Pg.645]    [Pg.74]    [Pg.119]    [Pg.132]    [Pg.188]    [Pg.325]   
See also in sourсe #XX -- [ Pg.125 , Pg.126 , Pg.128 ]




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