1-PHENYL-1,2-DICARBA-CLOSO-DODECABORANE, 1-PH-1,2-CLOSO-C2B10H11 - SYNTHESIS, CHARACTERIZATION, AND STRUCTURE AS DETERMINED IN THE GAS-PHASE BY ELECTRON-DIFFRACTION, IN THE CRYSTALLINE PHASE AT 199 K BY X-RAY-DIFFRACTION, AND BY AB-INITIO COMPUTATIONS

Citation
Pt. Brain et al., 1-PHENYL-1,2-DICARBA-CLOSO-DODECABORANE, 1-PH-1,2-CLOSO-C2B10H11 - SYNTHESIS, CHARACTERIZATION, AND STRUCTURE AS DETERMINED IN THE GAS-PHASE BY ELECTRON-DIFFRACTION, IN THE CRYSTALLINE PHASE AT 199 K BY X-RAY-DIFFRACTION, AND BY AB-INITIO COMPUTATIONS, Inorganic chemistry, 35(6), 1996, pp. 1701-1708
Citations number
46
Categorie Soggetti
Chemistry Inorganic & Nuclear
Journal title
ISSN journal
00201669
Volume
35
Issue
6
Year of publication
1996
Pages
1701 - 1708
Database
ISI
SICI code
0020-1669(1996)35:6<1701:11-S>2.0.ZU;2-B
Abstract
The compound 1-phenyl-1,2-dicarba-closo-dodecaborane(12), 1-C6H5-1,2-c loso-C2B10H11 (1), has been synthesized and characterized by a complet e assignment of its B-11 NMR spectrum via B-11(H-1)/B-11{H-1} (COSY), H-1{B-11(selective)} and H-1{B-11}/H-1{B-11} (COSY) spectroscopy. An e lectron- and X-ray diffraction investigation of 1, complemented by ab initio calculations, has been undertaken. The gas-phase electron-diffr action (GED) data can be fitted by several models describing conformat ions which differ in the position of the phenyl ring with respect to t he carborane cage. Local symmetries of C-2v and D-6h for the 1,2-C2B10 and C-6 moieties, respectively, were adopted in the GED model in orde r to simplify the problem. In addition, constraints among the close-ly ing C-C and B-B bonds were employed. However, even though such simplif ications led to satisfactory refinements (R(G) = 0.069-0.071), a uniqu e, definitive solution could not be gained. The (C-C)(mean), (C-B)(mea n), and (B-B)(mean) bond lengths, r(a), are ca. 1.44, 1.72, and 1.78 A ngstrom, respectively. The C-6 hexagon, with r(a)(C-C) = ca. 1.394 Ang strom, either eclipses the C(1)-C(2) vector (overall C-s symmetry) or more or less eclipses the C(1)-B(4) cluster bond (overall C-1 symmetry ). In contrast, in the solid at 199 K, the ring lies at a position int ermediate between the two GED positions, as determined by X-ray crysta llography [C8H16B10, monoclinic P2(1)/a: a = 12.047(3) Angstrom, b = 1 8.627(4) Angstrom, c = 12.332(5) Angstrom, beta = 110.09(4)degrees, Z = 8]. The C-B distances span the range 1.681(6)-1.743(5) Angstrom, and B-B lengths lie between 1.756(6) and 1.795(6) Angstrom. A similar con formation was found for the theoretical (RHF/6-31G level) structure w hich was fully optimized in C-1 symmetry. The r(e) distances are consi stent with the dimensions derived in the experimental studies. IGLO ca lculations of the B-11 chemical shifts, in addition to SCF single-poin t energies of the GED structures, further support these observations.