ON MIXED GROUP 14-GROUP 14 BONDS .8. ASYMMETRICALLY SUBSTITUTED COMPOUNDS AR3PB-GEAR3 AND AR3PB-PBAR3 - COMPARISON OF STRUCTURE AND PHYSICAL BEHAVIOR IN THE SERIES OF BONDS SN-SN, PB-GE, PB-SN, AND PB-PB
Hj. Koglin et al., ON MIXED GROUP 14-GROUP 14 BONDS .8. ASYMMETRICALLY SUBSTITUTED COMPOUNDS AR3PB-GEAR3 AND AR3PB-PBAR3 - COMPARISON OF STRUCTURE AND PHYSICAL BEHAVIOR IN THE SERIES OF BONDS SN-SN, PB-GE, PB-SN, AND PB-PB, Organometallics, 13(7), 1994, pp. 2733-2742
A general procedure for the synthesis of hexaarylated compounds of the
type Ar3PbGeAr's from Ar3PbLi and Ar'3GeX in THF/ether at -60-degrees
-C is given. Likewise, from Ar3PbLi and Ar'PbI the asymmetrical diplum
banes Ar3PbPbAr3 could be prepared. By the use of the bulky groups Ar
and Ar', the migration of aryl groups could be suppressed, avoiding th
e appearance of the mixtures Pb2Ar6-nAr'n (n = 0-6). Nonetheless, the
resulting diplumbanes Ar3Pb-PbAr'3 were always partially contaminated
with some symmetric Pb2Ar6 and Pb2Ar'6. The structures of (p-Tol)3PbGe
Ph3 (triclinic, space group P1BAR; a = 9.983(1) b = 12.201(1) c = 15.7
28(2) angstrom; alpha = 95.73(1), beta = 103.56(1), gamma = 113.06(1)d
egrees; V = 1674(1) angstrom3; Z = 2; R = 0.0434) and (p-Tol)3PbGe-(p-
Tol)3 (trigonal, space group R3BAR; a = 13.338(1), c = 36.55(1) angstr
om; V = 5631(2) angstrom3; Z = 6; R = 0.0522) have been determined. NM
R chemical shifts delta(Sn-119) and delta(Pb-207) (40 compounds) and o
ne-bond couplings 1J(M-M') (16 compounds), stretching vibrations nu(M-
M') and force constants f(M-M') for a diatomic oscillator (38 compound
s), and bond distances d(M-M') (18 compounds) are compared for all six
combinations M/M' = Ge/Sn/Pb of Ar3M-M'Ar'3. Concerning the asymmetri
c diplumbanes Ar3Pb-PbAr'3, assignments of delta(Pb-207) resulted from
a consideration of inductivity (comparison to PbAr4/Ar'4) and an assu
med order of charge flow DELTA(Ar <-> Ar') (13 compounds). Sequences e
xist for delta(Sn-119) (Pb-Sn > Sn-Sn greater-than-or-equal-to Sn-Ge),
delta(Pb-207) (Pb-Pb > Pb-Sn almost-equal-to Pb-Ge), f (Sn-Ge > Sn-Sn
greater-than-or-equal-to Pb-Sn, and Pb-Ge > Pb-Sn greater-than-or-equ
al-to Pb-Pb), d (Sn-Ge less-than-or-equal-to Pb-Ge < Sn-Sn less-than-o
r-equal-to Pb-Sn less-than-or-equal-to Pb-Pb) and reduced spin-spin co
uplings 1K (Pb-Sn > Sn-Sn > Pb-Pb ''scatter''). The polarities Pb(delt
a-)-Ge(delta+) and Pb(delta-)-Sn(delta+) are obvious. The enhanced ele
ctronegativity of lead demonstrates the influence of its relativistica
lly contracted 6s and 6p orbitals. With regard to Ar3Pb-PbAr'3, a rela
tion between 1K(Pb-Pb) and the charge flow DELTA(Ar <-> Ar') is indica
ted.