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Charge density of the biologically active molecule (2-oxo-1,3-benzoxazol-3(2<i>H</i>)-yl)acetic acid

Ai WangInstitute of Inorganic Chemistry, RWTH Aachen University, Aachen, GermanyJamshid AshurovInstitute of Bioorganic Chemistry, Academy of Sciences of Uzbekistan, UzbekistanAziz B. IbragimovInstitute of General and Inorganic Chemistry, Academy of Sciences of Uzbekistan, UzbekistanRuimin WangInstitute of Inorganic Chemistry, RWTH Aachen University, Aachen, GermanyHalima MouhibInstitute of Physical Chemistry, RWTH Aachen University, Aachen, GermanyН. С. МухамедовYunusov Institute of the Chemistry of Plant Substances, Academy of Sciences of Uzbekistan, UzbekistanUlli EnglertInstitute of Inorganic Chemistry, RWTH Aachen University, Aachen, Germany
ABI

Аннотация

(2-Oxo-1,3-benzoxazol-3(2H)-yl)acetic acid is a member of a biologically active class of compounds. Its molecular structure in the crystal has been determined by X-ray diffraction, and its gas phase structure was obtained by quantum chemical calculations at the B3LYP/6-311++G(d,p) level of theory. In order to understand the dynamics of the molecule, two presumably soft degrees of freedom associated with the relative orientation of the planar benzoxazolone system and its substituent at the N atom were varied systematically. Five conformers have been identified as local minima on the resulting two-dimensional potential energy surface within an energy window of 27 kJ mol(-1). The energetically most favourable minimum closely matches the conformation observed in the crystal. Based on high-resolution diffraction data collected at low temperature, the experimental electron density of the compound was determined. Comparison with the electron density established by theory for the isolated molecule allowed the effect of intermolecular interactions to be addressed, in particular a moderately strong O-H...O hydrogen bond with a donor...acceptor distance of 2.6177 (9) Å: the oxygen acceptor is clearly polarized in the extended solid. The hydrogen bond connects consecutive molecules to chains, and the pronounced charge separation leads to stacking between neighburs with antiparallel dipole moments perpendicular to the chain direction.

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