ISOLATION AND STRUCTURAL CHARACTERIZATION OF UNSOLVATED LITHIUM ARYLS

Citation
K. Ruhlandtsenge et al., ISOLATION AND STRUCTURAL CHARACTERIZATION OF UNSOLVATED LITHIUM ARYLS, Journal of the American Chemical Society, 115(24), 1993, pp. 11353-11357
Citations number
48
Categorie Soggetti
Chemistry
ISSN journal
00027863
Volume
115
Issue
24
Year of publication
1993
Pages
11353 - 11357
Database
ISI
SICI code
0002-7863(1993)115:24<11353:IASCOU>2.0.ZU;2-E
Abstract
The synthesis and characterization of three examples of unsolvated lit hium aryls are described. The compounds {Li(Trip)}4 (1, Trip = 2,4,6-i -Pr3C6H2), (Li(2,6-Mes2C6H3)}2 (2, Mes = 2,4,6-Me3C6H2), {Li(n-Bu)}2(L iMes)2 (3), and {Li(n-Bu)12(LiMes*)2.Mes*Br (3.Mes*Br, Mes* = 2,4,6-t -Bu3C6H2) were synthesized by a metal-halogen exchange reaction betwee n n-butyllithium and the appropriate aryl bromide (I and 3) or iodide (2). The X-ray crystal structures of 1 and 3 show that they are tetram etallic lithium species involving almost planar arrays of four lithium atoms. The bonding involves both sigma- and pi-interactions to the ar yl ligands. In contrast, the structure of 2 is dimeric with the two ar yl groups linked by two mu2-bridging lithiums which are primarily sigm a-bonded to ipso carbons. Weaker interactions were also observed betwe en the ortho mesityl substituents and the lithiums. The structure of 3 -MesBr shows that the halide starting material Mes*Br can be included in the isolated crystals. This is a consequence of the fact that the metal-halogen exchange reaction used in their synthesis is sluggish. T he main reasons for this probably are the use of hydrocarbon rather th an ether solvent and the large size of the aryl ligands. The compounds were characterized by H-1, C-13, and Li-7 NMR spectroscopy and X-ray crystallography and represent the first examples of structurally chara cterized simple, nonsolvated, sigma-bonded lithium aryls. Crystal data with Mo Kalpha (lambda = 0.71069 angstrom) at 130 K: 1, a = b = 13.09 8(2) angstrom, c = 16.791(8) angstrom, V = 2881(2) angstrom3, Z = 2, s pace group I4BAR, 597 (I > 2sigma(1)) data, R = 0.089; 2, a = 30.190(7 ) angstrom, b = 13.423(2) angstrom, c = 19.048(4) angstrom, V = 7719(3 ) angstrom3, Z = 8 (two independent molecules), space group Pnna, 3419 (I > 2sigma(I)) data, R = 0.097; 3, a = 22.721(11) angstrom, b = 10.0 72(5) angstrom, c = 19.327(8) angstrom, V = 4423(3) angstrom3, Z = 4, space group Pna2(1), 1811 (I > 2.5sigma(I)) data, R = 0.082; 3-MesBr, a = 11.385(2) angstrom, b = 15.261(3) angstrom, c = 17.458(5) angstro m, beta = 91.16(2)degrees, V = 3032.4(12) angstrom3, Z = 2, space grou p C2/m, 1821 (I > 3sigma(I)) data, R = 0.104.