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Separation hindered

Some applications nonrelated to the properties of the nanoporous materials but to their porous structures are their use as filtration membranes, battery separators (hindering the diffusion of ions in the narrow channels), and catalyst supports (due to their high surface area) as well as gas capture and storage or light harvesting [72]. However, the common factor of all of these applications is the requirement of an open nanoporous structure not only inside the sample but also connected to the exterior of the sample. However, the CO2 foaming process from nanostructured polymers still has not allowed obtaining nanoporous samples with all of these features. Pinto et al. [102] proposed that 25/75 PMMA/MAM nanoporous foams present appropriate inner porous structures for these kinds of applications (bicontinuous nanoporous structures with tunable pore size), but further studies are required to connect effectively this inner porous structure with the exterior of the sample. [Pg.282]

There have been numerous attempts to treat torsional motion in molecular statistical mechanics and we do not attempt to review this vast literature here. We do note, however, the ground breaking early work of Pitzer and Gwinn who proposed a separable hindered rotor model. This approach, and closely related variations, is still widely used today as the most common method to go beyond the HO-RR model. We also point out that several non-separable methods have recently been developed that appear to be promising. ... [Pg.154]

Figure 6.6 Cumulative density of states versus excitation energy above zero point for HOOH computed using three methods. The red curve is the semiclassical adiabatic method, the blue curve is the HO-RR method, and the purple curve is the separable hindered rotor approximation for torsion using the relaxed potential. Figure 6.6 Cumulative density of states versus excitation energy above zero point for HOOH computed using three methods. The red curve is the semiclassical adiabatic method, the blue curve is the HO-RR method, and the purple curve is the separable hindered rotor approximation for torsion using the relaxed potential.
Figure 6.7 Density of states for HOOH versus excitation energy (in units of torsional quanta) computed using three methods. The semiclassical adiabatic method (Equation (6.16)) is shown with the red curve, the convention HO-RR method is shown with blue, while the separable hindered rotor torsional model is shown with purple. The upper and lower panels show the same quantities for two different energy ranges. Figure 6.7 Density of states for HOOH versus excitation energy (in units of torsional quanta) computed using three methods. The semiclassical adiabatic method (Equation (6.16)) is shown with the red curve, the convention HO-RR method is shown with blue, while the separable hindered rotor torsional model is shown with purple. The upper and lower panels show the same quantities for two different energy ranges.
The overall faetor of 2J +1, not included in these formulae, thus cancels in the final expression. The result for J = 0 versus energy above the dissociation limit, 48.4 kcal/mol, is shown in Fig. 15. For comparison, the HO-RR and hindered rotor approximations are also presented. It is seen that the HO-RR method gives results that are about a factor 2-3 too low at most energies. Clearly, the harmonic approximation is inappropriate for the TS. The separable hindered rotor approximation gives an improvement over the HO-RR method. It corrects about half of that error, but still yields results that are about a factor of 1.5 too small. The coupling induced by the torsional dependence of the vibrational frequencies and rotational constants is seen to have a clear and potentially observable effect upon the rate coefficient. The lifetimes predicted by RRKM theory are of the same order of magnitude as the experimental observations. [Pg.92]

Chiral separations are concerned with separating molecules that can exist as nonsupetimposable mirror images. Examples of these types of molecules, called enantiomers or optical isomers are illustrated in Figure 1. Although chirahty is often associated with compounds containing a tetrahedral carbon with four different substituents, other atoms, such as phosphoms or sulfur, may also be chiral. In addition, molecules containing a center of asymmetry, such as hexahehcene, tetrasubstituted adamantanes, and substituted aHenes or molecules with hindered rotation, such as some 2,2 disubstituted binaphthyls, may also be chiral. Compounds exhibiting a center of asymmetry are called atropisomers. An extensive review of stereochemistry may be found under Pharmaceuticals, Chiral. [Pg.59]

The mixture can be separated by distillation. The primary phosphine is recycled for use ia the subsequent autoclave batch, the secondary phosphine is further derivatized to the corresponding phosphinic acid which is widely employed ia the iadustry for the separation of cobalt from nickel by solvent extraction. With even more hindered olefins, such as cyclohexene [110-83-8] the formation of tertiary phosphines is almost nondetectable. [Pg.319]

When the ore contains a large amount of clay minerals, these form difficult to separate slimes, which hinder the recovery of the minerals (see Clays). The tailing from the scavenger cells can be cycloned to remove the slimes before the coarse material is floated in a tailings retreatment plant. The flotation product from the rougher cells of this plant can be reground and cleaned. This additional treatment of the tailings from the main copper flotation plant may improve the recovery of metal values by 1—3%. [Pg.197]

Liquid crystals stabilize in several ways. The lamellar stmcture leads to a strong reduction of the van der Waals forces during the coalescence step. The mathematical treatment of this problem is fairly complex (28). A diagram of the van der Waals potential (Fig. 15) illustrates the phenomenon (29). Without the Hquid crystalline phase, coalescence takes place over a thin Hquid film in a distance range, where the slope of the van der Waals potential is steep, ie, there is a large van der Waals force. With the Hquid crystal present, coalescence takes place over a thick film and the slope of the van der Waals potential is small. In addition, the Hquid crystal is highly viscous, and two droplets separated by a viscous film of Hquid crystal with only a small compressive force exhibit stabiHty against coalescence. Finally, the network of Hquid crystalline leaflets (30) hinders the free mobiHty of the emulsion droplets. [Pg.203]

Ionic associates (lA) of polyoxometalates (POMs) with threephenylmethane dyes remain as perspective analytical forms for the determination of some nonmetals including P(V), As(V) and Si(IV). Several reasons hinder to the improvement of analytical characteristics of these reactions. Separation of dye excess and its lA with reagent are most important Procedure for extractive separation is often timeconsuming, complex and does not allow complete separation from reagent excess. [Pg.285]

The use of dimethyl sulfoxide-acetic anhydride as a reagent for the oxidation of unhindered steroidal alcohols does not appear to be as promising due to extensive formation of by-products. However, the reagent is sufficiently reactive to oxidize the hindered 11 j -hydroxyl group to the 11-ketone in moderate yield. The use of sulfur trioxide-pyridine complex in dimethyl sulfoxide has also been reported. The results parallel those using DCC-DMSO but reaction times are much shorter and the work-up is more facile since the separation of dicyclohexylurea is not necessary. Allylic alcohols can be oxidized by this procedure without significant side reactions. [Pg.238]


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