STRUCTURE AND STEREODYNAMICS OF FE(CO)4L COMPLEXES (L = P(O-TOLYL)3, AS(O-TOLYL)3, P(O-TOLYL)2CH2PH, (O-TOLYL)2PP(O-TOLYL)2)

Citation
Jas. Howell et al., STRUCTURE AND STEREODYNAMICS OF FE(CO)4L COMPLEXES (L = P(O-TOLYL)3, AS(O-TOLYL)3, P(O-TOLYL)2CH2PH, (O-TOLYL)2PP(O-TOLYL)2), Inorganic chemistry, 32(16), 1993, pp. 3493-3500
Citations number
40
Categorie Soggetti
Chemistry Inorganic & Nuclear
Journal title
ISSN journal
00201669
Volume
32
Issue
16
Year of publication
1993
Pages
3493 - 3500
Database
ISI
SICI code
0020-1669(1993)32:16<3493:SASOFC>2.0.ZU;2-U
Abstract
The crystal structures and variable-temperature NMR spectra of (CO)4Fe P(o-tolyl)3, (CO)4FeAs(o-tolyl)3, (CO)4FeP-(o-tolyl)2CH2Ph, and (CO)4F e(o-tolyl)2PP(o-tolyl)2 (1a-d) are reported. In the solid state, compl exes 1a-c contain the phosphine in an axial position of the trigonal b ipyramid; complex 1d is equatorially substituted in the solid state bu t exists as an axial/equatorial mixture in solution. All complexes exh ibit P-C restricted rotation, which in the case of 1a may be linked to axial/equatorial CO exchange. Crystallographic data: 1a, C25H21FeO4P, monoclinic, P2(1)/n, a = 10.188(3) angstrom, b = 10.429(2) angstrom, c = 21.755(6) angstrom, beta = 99.79(2)degrees, Z = 4; 1b, C25H21AsFeO 4, monoclinic, P2(1)/n, a = 10.265(2) angstrom, b = 10.517(1) angstrom , c = 21.679(3) angstrom, beta = 99.16(2)degrees, Z = 4; 1c, C25H21FeO 4P, triclinic, P1BAR, a = 9.618(3) angstrom, b = 15.282(3) angstrom, c = 17.130(5) angstrom, alpha = 66.92(2)degrees, beta = 79.51(2)degrees , gamma = 86.42(2)degrees, Z = 4; 1d, C32H38FeO4P2, orthorbombic, Pbca , a = 15.947(6) angstrom, b = 20.009(3) angstrom, c = 15.470(4) angstr om, Z = 8.