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Charge distribution aniline

The second way in which the substituent R affects the charge distribution of the molecule is called the resonance effect (or sometimes the tautomeric or electromeric effect). This results when the molecule resonates among several electronic structures. For example, for aniline the structures... [Pg.194]

By introducing reasonable values (about 2 for nitrogen, 4 for oxygen) for the electron affinity parameter relative to carbon, 8, and for the induced electron affinity for adjacent atoms (32/8i = Vio), we have shown that the calculated permanent charge distributions for pyridine, toluene, phenyltrimethylammonium ion, nitrobenzene, benzoic acid, benzaldehyde, acetophenone, benzo-nitrile, furan, thiophene, pyrrole, aniline, and phenol can be satisfactorily correlated qualitatively with the observed positions and rates of substitution. For naphthalene and the halogen benzenes this calculation does not lead to results... [Pg.201]

To sum up, for pyrrole the situation seems to be clearer in the sense that the conjugative effect overcomes the inductive, leading to a charge distribution similar to that of aniline. This hypothesis is confirmed by the fact that pyrrole itself is a weak acid and that the basic center is not the nitrogen atom but the a-carbon.42 For furan... [Pg.242]

The first topic to be dealt with in this article dates back to the early days of pulse radiolysis and is concerned with intermediates generated from organic nitro and nitroso compounds in some elementary redox processes. This will be followed by a presentation of some most recent results on aminyl radicals derived from amino acids, exemplifying the diversity of possible reactions of a seemingly simple type of radicals. The third example on aniline and aniline radicals aims to demonstrate the potential of time-resolved resonance Raman spectroscopy. A common message of all these studies on N-centered radicals hints at the importance of acid/base properties of radicals. The aniline system, in particular, also draws attention to spin and charge distribution, and possible implications to the chemistry of radical species. [Pg.342]

As an ion travels through the drift gas, there are several types of interactions between the ion and the nentral molecules of the drift gas (see Chapter 10). These interactions depend on the characteristics of the ion (size, total charge, charge distribution within the ion, and shape) and the drift gas molecnle (size, dipole and qnadrnpole moments, and polarizability). The magnitude of these interactions determines the drift velocity of the ion, namely, the mobility. This is the basis for elncidation of ion structure or conformation from mobility measurements and has been applied to elncidate the strnctnre of small ions like anilines and diamines as well as that of large ions like protonated polyglycine and polyalanine. ... [Pg.376]

In 12, the donor and acceptor moieties are chiral, and, as noted by the authors, the molecule therefore exists as a pair of diastereomers which are separable by chromatography. However, rotation about the linkages between the porphyrin macrocycle and the attached aryl rings must be very slow on the time scale of electron transfer. Thus, non-interconverting diastereomers should be present, with slightly different separations and orientations between the aniline donor and the quinone acceptor. This distribution would be expected to influence the decay kinetics of D+-P-QT if charge recombination is via direct electron transfer. If a... [Pg.122]

FIGURE 5. Summary of electronic distribution in aniline, (a) Bond distances (A), NBO charges [bracket, in au] and Wiberg indices (parentheses, in au). (b) Topology of the electron density determined from atom-in-molecule calculations p(r) = electron density, L = Laplacian of the density defined as L(r) = —V2p(r) and e = ellipticity of the bond critical point, (c) Laplacian map of the density, (d) Iso-surfaces of the electron localization function, ELF = 0.87 the values are the populations of the valence basins... [Pg.86]

An alternate and more economical procedure consists in cooling and settling the reaction mass from the autoclaves, whereby the charge separates into two layers—a dark-brown lower layer, comprising principally aniline, and an almost colorless upper aqueous layer, which rapidly becomes blue on exposure to air. The volume of the water layer will, of course, be considerably greater than that of the aniline layer and will vary with the ammonia liquor ratio. When 5 moles of 32 per cent anunonia aiid 0.1 mole of cuprous oxide were used per mole chlorobedzene, Vorozhtzov and Kobelev found that the products of reaction were distributed as follows ... [Pg.459]


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Charge distribution

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