Crystal chemistry of tetraradial species. Part 10. Tilting at windmills: conformations of the tetraphenyl species ZPh40, ±1 (Z = B, C, N)

2002 ◽  
Vol 80 (10) ◽  
pp. 1351-1366 ◽  
Author(s):  
Osvald Knop ◽  
Kathryn N Rankin ◽  
T Stanley Cameron ◽  
Russell J Boyd

The equilibrium geometries of the isoelectronic ZPh40, ±1 (Z = B, C, N) molecules have been optimized, in S4 and D2d symmetries, at the HF/6-31G(d,p) and B3LYP/6-31G(d,p) levels, with the phenyl rings constrained to be planar. The ground-state conformations of all three species are shown to be of S4 symmetry, but the difference of the energies of the S4 and the D2d conformations is estimated to amount to only ~1 kcal mol–1, with a barrier to concerted rotational reorientation of the phenyl rings of ~5.0 kcal mol–1 for BPh–4, ~6.4 kcal mol–1 for CPh4, and ~7.9 kcal mol–1 for NPh+4. A redetermination of the crystal structure of CPh4 from –60°C X-ray data agrees with the results of previous determinations at ambient temperature; the CPh4 molecule in the crystal is slightly compressed along the S4 axis relative to the free molecule, otherwise the geometries of the two are essentially the same. Correlations between the optimized geometric parameters of the ZPh40, ±1 molecules have been examined and analyzed in detail, as have the substitution-induced changes in the geometry of the phenyl ring. The results confirm and strengthen the conclusions from the statistical studies by Domenicano et al. on the geometry of benzene rings monosubstituted by atoms of elements from the first row of the Periodic system.Key words: tetraphenylborate, tetraphenylmethane, tetraphenylammonium, ab initio molecular geometries.

2002 ◽  
Vol 57 (11) ◽  
pp. 847-853 ◽  
Author(s):  
A. Pajzderska ◽  
H. Małuszyńska ◽  
J. Wa̡sicki

By X-ray diffraction it was found that at 293 K the crystals of rubidium tetraphenylborate are tetragonal, space group I42m, a = b = 11.212(2) Å, c = 8.098(2) Å , with 2 molecules of Rb+[C24H20B]- in the unit cell. The molecular reorientations as functions of temperature were studied by 1H NMR. Two types of motions were detected: an anisotropic reorientation of the tetraphenylborate anions about their mass centres, and small-angle reorientations / oscillations of the phenyl rings. The dependence of the potential energy of the anion in the crystal on the angle of the phenyl ring rotation about the B-Ph bond was obtained on the basis of atom-atom calculations. The dynamics of this compound was compared to that of tetraphenyltin.


2008 ◽  
Vol 64 (5) ◽  
pp. 534-549 ◽  
Author(s):  
Ryoko Makita ◽  
Kiyoaki Tanaka ◽  
Yoshichika Ōnuki

X-ray atomic orbital (XAO) analysis revealed that at both temperatures the electrons are transferred from B 2px (= py ) to Ce 5d and 4f orbitals. At 340 K 5d(j = 5/2)Γ8 orbitals are occupied partially, but 4f(j = 5/2)Γ8 orbitals are more populated than 4f(j = 5/2)Γ7 orbitals, in contrast to our observation at 430 K [Makita et al. (2007). Acta Cryst. B63, 683–692]. At 535 K the XAO analysis revealed clearly that the order of the energy levels of 4f(j = 5/2)Γ8 and Γ7 states reversed again and is the same as that at room temperature. It also limited the possible 5d configurations to three models among the nine possible ones. However, the XAO analysis could not decide which of the three models was the best with the present accuracy of the measurement. Two of them have partially and fully occupied 5d(j = 5/2)Γ7 orbitals and the remaining one has a fully occupied 5d(j = 3/2)Γ8 orbital. Since the lobes of 5d(j = 3/2)Γ8 or 5d(j = 5/2)Γ7 orbitals do not overlap with the 4f(j = 5/2)Γ8 orbitals as well as the 5d(j = 5/2)Γ8 orbitals, the order of the energy levels of the 4f(j = 5/2) orbitals became the same as that at room temperature. These results indicate that the crystal field varies with temperature due to the electron transfer from B 2p to Ce 5d orbitals. The difference densities after the spherical-atom refinement at the three temperatures clearly revealed the different combinations of 4f and 5d orbitals which are occupied. In the present study positive peaks due to the 4f electrons appear near the Ce nucleus and those due to 5d orbitals are found in the area outside the 4f peaks. Between the two areas there is a negative area distributed spherically at 340 K. The negative area produced by the contraction of 4f(j = 5/2)Γ8 orbitals seems to reduce the electron repulsion of the 5d(j = 5/2)Γ8 orbitals and helps the 4f(j = 5/2)Γ8 orbitals to remain as the ground state.


2014 ◽  
Vol 22 (1) ◽  
pp. 25-38 ◽  
Author(s):  
Vasilichia Antoci ◽  
Mircea Apostu ◽  
Catalina Ciobanu ◽  
Dorina Mantu

Abstract The structural NMR and X-ray studies of 6,6’-(Oxybis(4,1- phenylene))bis-(2-allylpyridazin-3(2H)-one), a bis-pyridazine derivative heterocycle, are reported in this study. Both 1H- and 13C- NMR confirm the proposed structure of compound. In order to establish unequivocally the structure of compound, the X-ray data analysis was performed. The compound crystallizes in the triclinic P-1(2) space group with a = 10.3699(7) Å, b = 10.6972(6) Å, c = 11.0449(4) Å, α = 87.941(5)°, β = 75.564(5)°, γ = 72.055(5)°, V= 1127.68 (12) Å3 and Z = 2. Molecular and crystal packing parameters for the novel heterocyclic system were obtained from intensity data collected at room temperature. The two phenyl rings (from the diphenyl ether moiety) are perpendicular one to each other and, on its turn, each phenyl ring is almost coplanar with the pyridazine ring


Author(s):  
C. F. Annie ◽  
M. Sithambaresan ◽  
M. R. Prathapachandra Kurup

The title compound, C21H19N3O3, has anEconformation about the azomethine double bond. The central moiety of the hydrazinecarboxamide moiety [–N—N—C(=O)—N–] has an almost coplanar arrangement [maximum deviation for the C atom = 0.010 (2) Å]. This central moiety is flanked by three aromatic rings and its mean plane makes dihedral angles of 24.7 (1), 72.91 (12) and 34.26 (11) Å, respectively, with the phenolic ring, the phenyl ring attached to the same C atom as the phenolic ring, and the phenylhydrazine ring. The adjacent phenolic and phenyl rings are twisted away from each other to reduce steric hindrance and make a dihedral angle of 80.59 (12)°. The phenolic and phenylhydrazine rings are inclined to one another by 28.89 (11)°. The rigidity of the molecule is increased by an intramolecular O—H...N hydrogen bond involving the phenolic hydrogen and the azomethine N atom. In the crystal, the carbonyl O atom forms bifurcated hydrogen bonds with the two NH atoms of the hydrazinic group, leading to the formation of chains propagating along [001]. Within the chains there are also C—H...O hydrogen bonds present. The chains are linkedviaC=O...π [3.4316 (18) Å] and parallel slipped π–π interactions, involving inversion-related benzene rings [centroid–centroid distance = 3.8850 (14) Å; inter-planar distance = 3.3895 (10) Å; slippage = 1.899 Å], forming sheets lying parallel to (100).


1985 ◽  
Vol 38 (8) ◽  
pp. 1223
Author(s):  
JM Coxon ◽  
MJ O'Connell ◽  
PJ Steel

The crystal structures of exo- and endo- 1,7,8,9- tetraphenyltricyclo [5.2.1.02,6]deca-3,8-dien-10-one (8) and (9) are reported. Crystals of the exo adduct (8) are triclinic: Pī , a 9.863(2), b 10.738(2), c 13.634(2) Ǻ, α 82.90(1), β 68.87(1), γ 66.87(1)°, Z 2; crystals of the endo adduct (9) are monoclinic: P21/c, a 11.610(1), b 7.862(2), c 27.675(3) Ǻ, β 100.223(9)°, Z 4. The structures were refined to R 0.039 and 0.049 respectively. The relative orientations of the four phenyl rings in the two structures are similar.


2013 ◽  
Vol 69 (11) ◽  
pp. o1719-o1720
Author(s):  
Chamseddine Derabli ◽  
Raouf Boulcina ◽  
Sofiane Bouacida ◽  
Hocine Merazig ◽  
Abdelmadjid Debache

In the title compound, C24H18ClN3, the dihydroquinazoline and methyl-substituted quinoline benzene rings make a dihedral angle of 78.18 (4)° and form dihedral angles of 45.91 (5) and 79.80 (4)°, respectively, with the phenyl ring. The dihedral angle between the phenyl ring of dihydroquinazoline and the methyl-substituted benzene ring of quinoline is 78.18 (4)°. The crystal packing can be described as crossed layers parallel to the (011) and (0-11) planes. The structure features N—H...N hydrogen bonds and π–π interactions [centroid–centroid distance between phenyl rings = 3.7301 (9) Å].


Author(s):  
Georgii Bogdanov ◽  
Evgenii Oskolkov ◽  
Jenna Bustos ◽  
Viktor Glebov ◽  
John P. Tillotson ◽  
...  

The title compound DBNB, C24H20N2O6, has been crystallized and studied by X-ray diffraction, spectroscopic and computational methods. In the title molecule, which is based on a 1,4-distyryl-2,5-dimethoxybenzene core with p-nitro-substituted terminal benzene rings, the dihedral angle between mean planes of the central fragment and the terminal phenyl ring is 16.46 (6)°. The crystal packing is stabilized by π–π interactions. DFT calculations at the B3LYP/6–311 G(d,p) level of theory were used to compare the optimized structures with the experimental data. Energy parameters, including HOMO and LUMO energies, their difference, and vertical excitation and emission energies were obtained.


1982 ◽  
Vol 37 (12) ◽  
pp. 1606-1611
Author(s):  
Alfred Gieren ◽  
Viktor Lamm

The title compound crystallizes in the monoclinic space group P21/n with a - 8.761(3), b - 9.773(5), c = 18.727(7) Å, y = 100.86(3)°, V = 1574.7.Å3, Z = 4. The structure was solved by direct methods and the refinement converged for 2030 independent reflections to an JR-value of 0.060 (Rw = 0.071). The N-N distances in the mesoionic -N⊖-N⊕(R) = Nmoiety are asymmetric with 1.304 and 1.263 Å, respectively. The almost planar heterocyclic pyrazolinium ring system and the plane of the aromatic pentafluorophenyl group include an angle of 60° caused mainly by a torsion around the N-C bond to the phenyl ring. The crystal packing contains columnar stacks of parallel phenyl rings with distances of 3.30 and 3.35 Å. Also H-F contacts play a dominant role


2014 ◽  
Vol 70 (3) ◽  
pp. o238-o239 ◽  
Author(s):  
Bilge Eren ◽  
Selçuk Demir ◽  
Hakan Dal ◽  
Tuncer Hökelek

The whole molecule of the title compound, C20H19NO4S2, is generated by twofold rotational symmetry. The N atom is located on the twofold rotation axis and has a trigonal-planar geometry. It is bonded by two S atoms of two symmetry-related 4-methylphenylsulfonyl groups and by the C atom of the phenyl ring, which is bisected by the twofold rotation axis. The benzene and phenyl rings are oriented at a dihedral angle of 51.48 (5)° while the pendant benzene rings are inclined to one another by 87.76 (9)°. In the crystal, weak C—H...O hydrogen bonds link the molecules, forming a three-dimensional network.


2014 ◽  
Vol 926-930 ◽  
pp. 262-265
Author(s):  
Huan Mei Guo ◽  
Yun Chen Zhang ◽  
Yu Feng Li

1N-Acetyl-3-phenyl-5-(3,4,5-trimethoxyl-phenyl)-2-pyrazoline has been synthesized and the crystal structure has been determined by means of single-crystal X-ray diffraction. The pyrazolinyl ring and the phenyl rings at 3 positions of the pyrazoline are almost coplane , with their dihedral angle to be 6.63(2) o. Phenyl ring at 5 positions and pyrazolinyl ring are almost perpendicular, the dihedral angle is 78.03(3) o.


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