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Cross-Sectional Effects

Here, V is the volume of the hydrocarbon chain(s) of the surfactant, the mean cross-sectional (effective) headgroup surface area, and 4 is the length of the hydrocarbon tail in the all-trans configuration. Surfactants with Pcone-shaped and form spherical micelles. For l/3truncated-cone-shaped, resulting in wormlike micelles (the term wormlike is preferred over rodlike to highlight the highly dynamic nature of these micelles). [Pg.5]

This calculation is for spherical micelles, but a similar calculation could be used to obtain estimates of salt concentrations for ionic wormlike micelles. Such salt concentrations for wormlike micelles are expected to be increased in comparison to spherical micelles. In fact, the addition of counterions or a sufficient increase in surfactant concentration often leads to a transition from spherical micelles to wormlike micelles. As the free counterion concentration in solution increases, so does the counterion binding. As a result, electrostatic repulsion between the charged head-groups is increasingly shielded and the mean cross-sectional (effective) headgroup... [Pg.6]

A theoretical model predicting the shape-structure relationship between the monomeric units and their aggregates was developed by Israelachvili and was based on statistical mechanics of phospholipids.23 This model predicts the type of the aggregate formed on the basis of the packing parameter (P), which relates the volume of the molecule (V) to its length (1) and to the mean cross-sectional (effective) head group surface area (a) ... [Pg.121]

There are photoionization cross section effects to be considered. XPS ( 1 keV soft X-ray photon excitation) is used to study the core-electron energy levels, while UPS ( 20-40 eV photons) is used to study the valence electron energy distribution. UPS has the... [Pg.44]

Lastly, it is generally assumed that 0.5eV is the best possible resolution for solid state XPS measurements and the experimental resolution function is reasonably well reproduced by a Gaussian of full width f at half maximum of 0.7eV. A final "theoretical XPS spectrum" is obtained after correction of the basic density of states function by cross-section effects and convolution by the experimental resolution function (16) ... [Pg.157]

Figure 5. Theoretical (FSGO) and experimental XPS valence spectra of various fluaro-polyethylenes (theoretical results do not include any cross-section effects)... Figure 5. Theoretical (FSGO) and experimental XPS valence spectra of various fluaro-polyethylenes (theoretical results do not include any cross-section effects)...
Figure 6-39. Effect of vibrational excitation of molecules on G-factor of ozone synthesis in atmospheric-pressure pulsed corona discharges in air as function of specific energy input (1) taking into account the contribution of the effect of saturation of vibrational excitation (2) total contribution of vibrational excitation including the cross-sectional effect. Figure 6-39. Effect of vibrational excitation of molecules on G-factor of ozone synthesis in atmospheric-pressure pulsed corona discharges in air as function of specific energy input (1) taking into account the contribution of the effect of saturation of vibrational excitation (2) total contribution of vibrational excitation including the cross-sectional effect.
Yawalkar et al. (2001) has developed a model for a three-phase reactor based on the use of a dense polymeric composite membrane containing discrete cubic zeolite particles (Fig. 4.5) for the epoxidation reaction of alkene. Catalytic particles of the same size are assumed vdth a cubic shape and uniformly dispersed across the polymer membrane cross-section. Effects of various parameters, such as peroxide and alkene concentration in liquid phase, sorption coefficient of the membrane for peroxide and alkene, membrane-catalyst distribution coefficient for peroxide and alkene and catalyst loading, have been studied. The results have been discussed in terms of a peroxide effidency defined as the ratio of flux of peroxide through the membrane utilized for alkene oxidation to the total flux of organic peroxide through the membrane. The paper aimed to show that, by using an organophilic dense membrane and the catalysts confined in the polymeric matrix, the oxidant concentration (in that reaction peroxides) can be controlled on the active site with an improvement of the peroxide efficiency and selectivity to desired products. [Pg.169]

In a recent publication, Cox et al. (1992) presents photoemission data for Am metal and AmHj. Both materials are expected to exhibit fully localized rare-earth-like spectra nevertheless, as shown in fig. 21, the 5f peak distribution is still dominant with its centroid about 3eV from the Fermi level. As with the rare earths, a reduced conduction-band intensity can be seen quite clearly. Positive chemical shifts for all the metal levels (4f, 5p, 4d and 3d) indicate electron transfer from the metal. As expected, the 6p3/2 binding energy for AmHj increases by about 0.6 eV, an amount similar to that found for Ce and Pr. Although the peak maximum for AmHj appears to shift to lower binding energies, the centroid is actually coincident with that for Am metal. In spite of these complications, cross-section effects and initial-final state considerations, the Am-I-H system is clearly the first unambiguously rare-earth-like actinide-hydride system. These observations are corroborated by resistivity measurements described in section 6.3.1. [Pg.334]

Fig. 14 Grid bar cross-sections. Effective open grid surface area Fo for equal section modulus of bars Fq = 1.5 Fq ... Fig. 14 Grid bar cross-sections. Effective open grid surface area Fo for equal section modulus of bars Fq = 1.5 Fq ...
The errors shown in Table II are estimates only, and it is seen that on the basis of existing information there will be considerable uncertainty in temperature coefficient calculations in therrnal reactors with appreciable amounts of Pu present. It does appear that for BER the temperature coefficient may become less negative as Pu builds up. It can also be seen from Table II that the dross section temperature coefficient at the operating temperattxrejnay be positive (given approximately by averaging the last two columns). The over-all temperature coefficient consists, of course, of the cross section effect and a nvimber of other effects, the chief of which is the density effect. [Pg.55]

In paper [6] it has been shown that the glass transition temperature is connected with the macromolecule cross-sectional effective area S and the characteristic ratio C as follows ... [Pg.204]

Figure 5.6 The dependences of macromolecule cross-sectional effective area S on chemical crosslinking effective density for non-modified EP-1 and EP-2 (1), EP-3 (2) and EP-4 (3). In insert schematic representation of crosslinked polymer... Figure 5.6 The dependences of macromolecule cross-sectional effective area S on chemical crosslinking effective density for non-modified EP-1 and EP-2 (1), EP-3 (2) and EP-4 (3). In insert schematic representation of crosslinked polymer...

See other pages where Cross-Sectional Effects is mentioned: [Pg.86]    [Pg.77]    [Pg.99]    [Pg.377]    [Pg.156]    [Pg.163]    [Pg.223]    [Pg.264]    [Pg.363]    [Pg.1017]    [Pg.236]    [Pg.398]    [Pg.196]    [Pg.377]    [Pg.133]    [Pg.54]    [Pg.412]    [Pg.865]    [Pg.363]    [Pg.211]    [Pg.168]   
See also in sourсe #XX -- [ Pg.169 ]




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Collision effective cross-section

Cross effect

Cross section effective absorption

Cross section effective escape

Cross section, Mossbauer effect

Cross-section effective

Effect of permanent dipole on Langevin cross-section

Effective capillary cross sectional area

Effective collision cross section argon

Effective collision cross section classical trajectory calculations

Effective collision cross section mixtures

Effective collision cross section nitrogen

Effective cross section for collision

Effective cross section, absorption removal

Effective cross-sectional area

Energy effects on reaction channels and cross-sections

Fission products effective cross section

Isotope effects cross section)

Polarization effects cross-sections

The effect of optical cross-section

The effects of polymer in real-field cross-sections

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