3 research outputs found
Substituent Effect on the σ- and π‑Electron Structure of the Nitro Group and the Ring in <i>Meta</i>- and <i>Para</i>-Substituted Nitrobenzenes
An
application of quantum chemical modeling allowed us to investigate
a substituent effect on a σ and π electron structure of
a ring and the nitro group in a series of <i>meta</i>- and <i>para</i>-X-substituted nitrobenzene derivatives (X = NMe<sub>2</sub>, NHMe, NH<sub>2</sub>, OH, OMe, Me, H, F, Cl, CF<sub>3</sub>, CN, CHO, COMe, CONH<sub>2</sub>, COOH, NO<sub>2</sub>, and NO).
The obtained pEDA and sEDA parameters (the π- and σ-electron
structure characteristics of a given planar fragment of the system
obtained by the summation of π- and σ-orbital occupancies,
respectively) of the NO<sub>2</sub> group and the benzene ring allowed
us to reveal the impact of the substituents on their mutual relations
as well as to analyze them from the viewpoint of substituent characteristics.
The decisive factor for dependence of pEDA on sEDA of the ring is
electronegativity of the atom linking the substituent with the ring;
in subgroups an increase of sEDA is associated with a decrease of
pEDA. The obtained mutual relation between pEDAÂ(NO<sub>2</sub>) and
pEDAÂ(ring) characteristics documents strong resonance interactions
for electron-donating substituents in the <i>para</i> position.
The observed substituent effect on the σ-electron structure
of the nitro group, sEDAÂ(NO<sub>2</sub>), is significantly greater
(∼1.6 times) for <i>meta</i> derivatives than for
the <i>para</i> ones
Dependence of the Substituent Effect on Solvent Properties
The influence of
a solvent on the substituent effect (SE) in 1,4-disubstituted
derivatives of benzene (BEN), cyclohexa-1,3-diene (CHD), and bicyclo[2.2.2]Âoctane
(BCO) is studied by the use of polarizable continuum model method.
In all X–R–Y systems for the functional group Y (NO<sub>2</sub>, COOH, OH, and NH<sub>2</sub>), the following substituents
X have been chosen: NO<sub>2</sub>, CHO, H, OH, and NH<sub>2</sub>. The substituent effect is characterized by the charge of the substituent
active region (cSARÂ(X)), substituent effect stabilization energy (SESE),
and substituent constants σ or <i>F</i> descriptors,
the functional groups by cSARÂ(Y), whereas Ï€-electron delocalization
of transmitting moieties (BEN and CHD) is characterized by a geometry-based
index, harmonic oscillator model of aromaticity. All computations
were carried out by means of B3LYP/6-311++GÂ(d,p) method. An application
of quantum chemistry SE models (cSAR and SESE) allows to compare the
SE in water solutions and in the gas phase. Results of performed analyses
indicate an enhancement of the SE by water. The obtained Hammett-type
relationships document different nature of interactions between Y
and X in aromatic and olefinic systems (a coexistence of resonance
and inductive effects) than in saturated ones (only the inductive
effect). An increase of electric permittivity clearly enhances communications
between X and Y for BEN and CHD systems