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Enhancement factor for

FIG. 22-21 Enhancement factor for solids with a variety of polar functionalities in CO9 at 35 C (from bottom to top hexamethylbenzene, 2-naphthol, phthalic anhydride, anthracene, acridine). [Pg.2002]

The interpretation is straightforward. At reaction conditions the concentration in the film is lowered by reaction, and, as a consequence, the driving force for mass transfer increases. In a homogeneous system this results in high values of Ha. In a slurry reactor this enhancement can occur if the catalyst particles are so small that they accumulate in the film layer. Table 5.4-4 summarizes expressions for the reaction rate or enhancement factor for various regimes. [Pg.284]

The theory presented above accounts for the electrostatic effects on the apparent rate constant for ion transfer by relating the observed changes in to changes in c"(0), or equivalently to 0(0). In the following, we present the simulated electrical potential distributions and the corresponding enhancement factors for a cation transferring from the aqueous phase across the water-l,2-DCE interface (s" = 78.39, s° = 10.36). The rela-... [Pg.548]

FIG. 10 Simulated enhancement factor for monolayers of zwitterionic phospholipids with different molecular areas (shown on the curves) at the polarized water-1,2-DCE interface. The supporting electrolyte concentrations are c° = 20 mM and c" = 1000 mM. [Pg.550]

Fig. 23. Comparison of predicted and experimental enhancement factors for the experimental conditions of Fig. 19. Curves designated 1 and 1 are for vL = 0.86 mm/s, while curves 2 and 2 are for vL = 1.65 mm/s. The prime designates the data fits in Fig. 19. (Figure from Stcgasov et at., 1992, with permission, 1992 Elsevier Science Publishers.)... Fig. 23. Comparison of predicted and experimental enhancement factors for the experimental conditions of Fig. 19. Curves designated 1 and 1 are for vL = 0.86 mm/s, while curves 2 and 2 are for vL = 1.65 mm/s. The prime designates the data fits in Fig. 19. (Figure from Stcgasov et at., 1992, with permission, 1992 Elsevier Science Publishers.)...
When nano LC is combined with mass spectrometer detection, attamole detection can be achieved for low abundance components in biological fluids, drug metabolites, and natural products such as Chinese herb medicines. Nano LC-MS-MS has become an essential tool for complex biological and drug metabolite studies. Nano LC-MS presents two significant differences from conventional analytical HPLC (1) large enhancement factor for sample detection and (2) direct interface to MS without flow splitting. The enhancement in MS ion counts relative to a conventional 4.6 mm ID column is proportional to the ratio of the square of the column diameter ... [Pg.360]

The equations (23) to (27) can only be solved numerically. However such a numerical solution gives less insight in the factors governing the transport and conversion processes. Therefore we consider another approach. In this approach, the transport and conversion of component A are calculated under the assumption that no reaction of ozone with component B takes place. The enhancement factor for mass transfer of ozone, EA, can now be given by the equation ... [Pg.271]

The field emission properties of carbon nanotube forests and single nanotubes are described. Controlled emission is possible for aligned CNT arrays where the spacing is twice the CNT height, as grown by plasma enhanced chemical vapor deposition. This leads to the maximum field enhancement factor. For random forests, the field enhancement obeys an exponential distribution, leading to a lower emission site density and imperfect current sharing. Ballast resistors can help alleviate this problem. Random nanocarbons perform less well than CNTs. Some applications are covered. Elec-... [Pg.353]

Song, H. K. and Egk, M. J. Structural basis of degradation signal recognition by SspB, a specificity-enhancing factor for the ClpXP proteolytic machine. Mol Cell 2003, 12, 75-86. [Pg.286]

Figure 6. Isotopic enhancement factor for 0 in OJ as a function of ionizing energy and 02/He ratio at a constant ion source inlet pressure of 0.75 torr. Figure 6. Isotopic enhancement factor for 0 in OJ as a function of ionizing energy and 02/He ratio at a constant ion source inlet pressure of 0.75 torr.
In the context of the symmetry correlation schemes in Table 5, the experimental determination of enhancement factors for the individual elements, EF( C) and EF( 0), are more relevant than the directly measured EF(89) and EF(90). Because the experiment is done under natural abundance conditions, EF(90) can be taken... [Pg.182]

Figure 10, Isotopic enhancement factors for 0 and C in Ar COj as a function of ion source inlet pressure and Ar/COj ratio. Figure 10, Isotopic enhancement factors for 0 and C in Ar COj as a function of ion source inlet pressure and Ar/COj ratio.
Figure 23.4 The enhancement factor for fluid-fluid reactions as a function of Mf and modified from the numerical solution of van Krevelens and Hoftijzer (1954). Figure 23.4 The enhancement factor for fluid-fluid reactions as a function of Mf and modified from the numerical solution of van Krevelens and Hoftijzer (1954).
Fig. 5.2. Corrugation enhancement arising from different tip states. Solid curves, enhancement of tunneling matrix elements arising from different tip states. The tunneling current is proportional to the square of the tunneling matrix element. Therefore, the enhancement factor for the corrugation amplitude is the square of the enhancement factor for the tunneling matrix element, dotted curves. (Reproduced from Chen, 1990b, with permission.)... Fig. 5.2. Corrugation enhancement arising from different tip states. Solid curves, enhancement of tunneling matrix elements arising from different tip states. The tunneling current is proportional to the square of the tunneling matrix element. Therefore, the enhancement factor for the corrugation amplitude is the square of the enhancement factor for the tunneling matrix element, dotted curves. (Reproduced from Chen, 1990b, with permission.)...
The enhancement for the tunneling matrix element is shown in Fig. 5.2. The enhancement factor for the corrugation amplitude, Cl + (3iyV2K-)T, could be substantial. For example, on most closc-packcd metal surfaces, a= 2.5 A,... [Pg.127]

Fig. 5.10. Enhancement factor for different tip states. The shaded area near E=0 is the area where the corrugation amplitude is within the limit of the Fermi-level LDOS contours. In the hatched area near the bottom, the theoretical amplitude of the negative corrugation shows a spurious divergence. (Reproduced from Chen, 1992c, with permission.)... Fig. 5.10. Enhancement factor for different tip states. The shaded area near E=0 is the area where the corrugation amplitude is within the limit of the Fermi-level LDOS contours. In the hatched area near the bottom, the theoretical amplitude of the negative corrugation shows a spurious divergence. (Reproduced from Chen, 1992c, with permission.)...
A similar increase in the values for the hyperfine constants and parameters of the P,T-odd interactions when the correlations with the core shells (primarily, 5s, bp) are taken into account is also observed for the BaF molecule [93], as one can see in Table 3. Of course, the corrections from the 4/-electron excitations are not required for this molecule. The enhancement factor for the P,T-odd effects in BaF is three times smaller than in YbF mainly because of the smaller nuclear charge of Ba. [Pg.273]

The net enhancement factor for a droplet consisting of pure water can be as much as 1.6 (Madronich, 1987). Calculations by Ruggaber et al. (1997) suggest that the actinic flux inside cloud drops with a typical size distribution and dissolved particulate matter is more than a factor of two greater than in the cloud interstitial air. This effect of enhanced actinic flux inside droplets may be quite important for aqueous-phase photochemistry in fogs and clouds. [Pg.75]

Figure 6.3b shows the idealized concentration profile of an absorbed component A, obtained by the Hatta theory, for the case of a relatively slow reaction that is either first-order or pseudo first-order with respect to A. As A is consumed gradually while diffusing across the film, the gradient of concentration of A that is required for its diffusion gradually decreases with increasing distance from the interface. The enhancement factor for such cases is given by the Hatta theory as r... [Pg.83]


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