Articles you may be interested inStructural optimization of molecular clusters with density functional theory combined with basin hopping Conformational distribution of a ferroelectric liquid crystal revealed using fingerprint vibrational spectroscopy and the density functional theory Structure and conformation properties of 1-alkyl-3-methylimidazolium halide ionic liquids: A density-functional theory study Investigation of structure of liquid 2,2,2 trifluoroethanol: Neutron diffraction, molecular dynamics, and ab initio quantum chemical study First the conformations of various ortho and di-ortho substituted toluenes calculated by quantum chemistry methods are discussed as well as the hindering potentials deduced from the latter results and those established experimentally by microwaves and fluorescence techniques. It appears that methyl ͑Me͒ groups are much less hindered in di-ortho than in ortho substituted compounds. Then the study of the 1,3,5-triiodo-2,4,6-trimethylbenzene ͑triiodomesitylene or TIM͒ is reported. Density functional theory ͑DFT͒ calculations indicate that two conformations of the TIM molecule have the same formation energies. One has C 3h symmetry, the other with the C s symmetry is obtained from the C 3h by a rotation of 60°for one Me. Experimentally, the TIM structure has been determined at 15 K using single-crystal neutron diffraction data. TIM crystallizes in the triclinic space group P Ϫ1. Molecules are stacked in an antiferroelectric manner along the oblique a axis. For two Me groups the experimental conformation is close to the C s one, but the third Me group has a C-H bond nearly orthogonal to the ring plane. Such conformation is unstable in the gas state, but it is stabilized in the crystal by intermolecular interactions, nevertheless DFT predicts accurate bond lengths and angles when the Me conformations are constrained to the experimental ones. The three Me groups, having different environments, experience different hindering potentials, this explains why they are tunnelling at different energies as found by inelastic neutron scattering ͑INS͒. Using INS results, we deduced the potentials hindering the Me groups rotation in the crystal. The proton probability densities ͑PPD͒ calculated from these potentials are in concordance with the crystallographic results. Hence the quantum origin of the broad spreading of PPD observed at 15 K is established. Moreover, it is demonstrated that the crystal field is responsible for the larger part of the potentials hindering the Me groups in the solid state.

In the structure of triiodomesitylene (1,3,5-triiodo-2,4,6-trimethylbenzene), C(9)H(9)I(3), at 293 K, the benzene ring is found to be significantly distorted from ideal D(6h) symmetry; the average endocyclic angles facing the I atoms and the methyl groups are 123.8 (3) and 116.2 (3) degrees, respectively. The angle between the normal to the molecular plane and the normal to the (100) plane is 5.1 degrees. No disorder was detected at 293 K. The thermal motion was investigated by a rigid-body motion tensor analysis. Intra- and intermolecular contacts are described and topological differences compared with the isomorphous compounds trichloromesitylene and tribromomesitylene are discussed.

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Abstract. Mr= 147.87, orthorhombic, Pna21, a= 6.416 (2), b= 7.727 (3), c= 7.298 (2) A, V= 361-8 A 3, Z = 4, D x = 2.72 g cm -3, 2(Ag Ka) = 0-5608 A, g = 5.14 cm -1, F(000) = 280, T = 293 K.Final R = 0.018 for 1700 unique observed reflections. The absolute crystal structure has been solved. LiH 2-AsO 4 is isostructural with LiH2PO 4, but one of the two independent hydrogen bonds (these bonds involve the

The title compound, C7H5Cl2NO2[systematic name: 1,3-dichloro-2-methyl-5-nitrobenzene], crystallizes in the chiral space groupP212121with a Flack parameter of −0.03 (5). The methyl C atom, the Cl atoms and the N atom of the nitro substituent all lie extremely close to the plane of the benzene ring; the deviations are 0.028 (3) Å for the methyl C atom, −0.016 (1) and 0.007 (1) Å for the two Cl atoms, and −0.017 (3) Å for the nitro N atom. Hence, no significant steric hindrance of the methyl group by theorthohalogen atoms is observed. The nitro group is inclined to the benzene ring by 9.8 (3)°. In the crystal, molecules are linked by weak C—H...O and C—H...Cl hydrogen bonds, forming layers parallel to theabplane.

In the title compound, C16H14O2Se, the dihedral angle between the benzene rings is 87.08 (11)°. In the crystal, mol­ecules are linked into layers parallel to the bc plane by inter­molecular C—H⋯O hydrogen bonds.