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Average molecular structures from

AVERAGE MOLECULAR STRUCTURES FROM NMR It is convenient to think in terms of four different structures ... [Pg.151]

Herrmann and co-workers synthesized [Os(0)(Me)4] from 0s04 and dimethylzinc or methyltris(isopropoxy)titanium (180). An alternative route is by methylation of the glycolate osmium(VI) complex [0=0s(0CH2CH26)2] with dimethylzinc (180). The thermally labile ethyl derivative [Os(0)(Et)4] has also been prepared (180). [Os(0)(Me)4] is an orange, air-stable, volatile, crystalline compound that melts at 74°C without decomposition. The gas-phase average molecular structure of [Os(0)(Me)4], determined by electron diffraction techniques, is consistent with a theoretical model of C4 symmetry with d(Os—C) = 2.096(3) A, d(0s=0) = 1.681(4) A, and ZO—Os—C = 112.2(5)° (180). Cyclic voltammetric studies showed that [Os(0)(Me)4] undergoes reversible reduction at - 1.58 V and an irreversible oxidation at -f 2.2 V vs Ag/AgCl in MeCN. [Pg.270]

FIGURE 10.2 Average molecular structures of supercritical gas extracts of coal. (From Bartle, K.D. et al.. Fuel, 54, 226, 1975.)... [Pg.290]

More than anything, the structural studies of coal are limited by the continued insistence that one molecule of unlimited size can be constructed which will explain all of the properties of coal. And there appears to be a more distinctive, and recent, trend to the belief that the representation of coal by an average molecular structure is inappropriate insofar as it does not reflect the molecular diversity of the components of coal and there is an overriding tendency to ignore the known diversity of coal which is evident from petrographic studies (Chapter 4) (Given, 1984b Berkowitz, 1988 Haenel et al., 1989 Haenel, 1992). [Pg.329]

Aluminum porphyrins (98) have been used to prepare polymers with very narrow molecular weight distribution and controlled number average molecular weight from propylene oxide without complicating side reactions (99). The aluminum porphyrins have a structure as described below, where X is Cl, OH, OR, or O2CR and R is an alkyl group. [Pg.69]

Fig. 1-6). The structure obtained for thiazoie is surprisingly close to an average of the structures of thiophene (169) and 1,3,4-thiadiazole (170) (Fig. 1-7). From a comparison of the molecular structures of thiazoie, thiophene, thiadiazole. and pyridine (171), it appears that around C(4) the bond angles of thiazoie C(4)-H with both adjacent C(4)-N and C(4)-C(5) bonds show a difference of 5.4° that, compared to a difference in C(2)-H of pyridine of 4.2°, is interpreted by L. Nygaard (159) as resulting from an attraction of H(4) by the electron lone pair of nitrogen. [Pg.46]

One great advantage of the molecular mechanics model is that it can be applied to large molecules on your average PC. Apart from single molecular structure... [Pg.56]

At the present, perfluoropolyether or PFPE, a random copolymer with a linear principal chain structure, has been widely used in HDD as the lubricant. Its chemical structure can be described by A-[(0CF2CF2)p-(0CF2)g]-0-A (p/q s2/3), with the average molecular weight ranging from 2,000 to 4,000 g/mol. Here, the symbol -X denotes the end-bead (eb), corresponding to -CF3 (nonfunctional) in PFPE... [Pg.226]

As it was mentioned in Section 9.4.1, 3D structures generated by DG have to be optimized. For this purpose, MD is a well-suited tool. In addition, MD structure calculations can also be performed if no coarse structural model exists. In both cases, pairwise atom distances obtained from NMR measurements are directly used in the MD computations in order to restrain the degrees of motional freedom of defined atoms (rMD Section 9.4.2.4). To make sure that a calculated molecular conformation is rehable, the time-averaged 3D structure must be stable in a free MD run (fMD Sechon 9.4.2.5J where the distance restraints are removed and the molecule is surrounded by expMcit solvent which was also used in the NMR measurement Before both procedures are described in detail the general preparation of an MD run (Section 9.4.2.1), simulations in vacuo (Section 9.4.2.2) and the handling of distance restraints in a MD calculation (Section 9.4.2.3) are treated. Finally, a short overview of the SA technique as a special M D method is given in Sechon 9.4.2.6. [Pg.239]


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