Monomeric Tin(II) Diamide and Chlorotin(II) Amide Trimer
Figure 2. Thermal ellipsoid plot of 2 shown at the 30% probability level.
Selected bond lengths (Å) and bond angles (deg): Sn(1)-N(1) 2.0890(19),
Sn(1)-Cl(1) 2.6844(6), Sn(1)-Cl(3) 2.6868(6), Sn(2)-N(2) 2.0703(18),
Sn(2)-Cl(2) 2.5789(6), Sn(2)-Cl(1) 2.6201(6), Sn(3)-N(3) 2.0864(19),
Si(1)-N(1) 1.744(2), Si(2)-N(2) 1.746(2), Si(3)-N(3) 1.744(2); N(1)-
Sn(1)-Cl(1) 92.56(5), N(1)-Sn(1)-Cl(3) 96.20(5), Cl(1)-Sn(1)-Cl(3)
84.99(2), N(2)-Sn(2)-Cl(1) 98.35(5), N(2)-Sn(2)-Cl(2) 92.83(5),
Cl(1)-Sn(2)-Cl(2) 91.33(2), N(3)-Sn(3)-Cl(2) 93.27(5), N(3)-Sn(3)-
Cl(3) 96.43(5), Cl(2)-Sn(3)-Cl(3) 83.32(2), Sn(1)-Cl(1)-Sn(2) 114.16(2),
Sn(2)-Cl(2)-Sn(3) 116.96(2), Sn(1)-Cl(3)-Sn(3) 113.99(2).
Figure 1. Thermal ellipsoid plot for one of the two independent molecules
of 1 shown at the 50% probability level. Selected bond lengths (Å) and
bond angles (deg) for the two independent molecules: Sn(1)-N(2) 2.060(3)
(2.057(3)), Sn(1)-N(1) 2.058(3) (2.057(3)), Si(1)-N(1) 1.743(3) (1.742(3)),
Si(2)-N(2) 1.740(3) (1.744(3)); N(1)-Sn(1)-N(2) 105.8(1) (105.6(1)),
Sn(1)-N(1)-Si(1) 114.9(1) (114.9(1)), Sn(1)-N(1)-C(1) 126.1(2) (125.7(2)),
Si(1)-N(1)-C(1) 118.6(2) (118.5(2)), Sn(1)-N(2)-Si(2) 114.8(1) (115.6(1)),
Sn(1)-N(2)-C(13) 125.2(2) (126.0(2)), Si(2)-N(2)-C(13) 119.1(2)
(117.8(2)).
isopropylphenyl)]2, a significantly more sterically crowded
analogue prepared previously by Sita, a molecule in which
the rings are twisted away from each other.11
the mesityl group are at δ 20.86 (4-position) and 21.56 ppm
(2,6-positions), and the four aromatic carbons are found at
δ 128.64 (3,5-positions), 130.54 (4-position), 131.88 (2,6-
positions), and 147.13 ppm (1-position). The single resonance
at 473 ppm in the 119Sn NMR spectrum of 1 indicated that
a monomeric structure was likely. This value was similar to
the value of 501 ppm obtained by Sita for Sn[N(SiMe2Ph)2]2,
a monomer whose existence was established by X-ray
diffraction.11 Since the nuclearity of 1 could not be deter-
mined with certainty via NMR, it was necessary to determine
this by single-crystal X-ray diffraction analysis.
Crystals of 1 suitable for X-ray structural analysis were
grown from a hexane solution by cooling to -20 °C for
several days. There are two symmetrically independent
molecules in the crystal of 1. As can be seen in Figure 1,
the overall structure is monomeric, similar to the structure
of Sn[N(SiMe3)2]2 reported previously by Lappert.12 The Sn
atom in 1 resides at the bottom of a pocket formed by the
two phenyl rings of the mesityl groups which are essentially
parallel to each other (in both independent molecules the
two rings are approximately 1.5° removed from coplanarity).
The distance between the two parallel phenyl ring centers is
approximately 3.60 Å. While the rings are not absolutely
concentric, they do provide a pocket that should be accessible
by other atoms and molecules. Interestingly, in the solid state
1 adopts a planar zigzag conformation in the Si(1)-N(1)-
Sn-N(2)-Si(2) backbone. Furthermore, due to the pseudo-
C2 axis that is present in this conformation, the two-aryl
groups are essentially identical. It is also interesting to note
that the structure of 1, with parallel aromatic rings, is quite
different from the solid state structure of Sn[N(SiMe3)(2,6-
Compound 2 was prepared in 70% yield in a manner
similar to that of 1; however, in this case 1 equiv of SnCl2
was used. Yellow crystals of 2 were obtained by recrystal-
lization from a toluene/hexane solution at -20 °C. This
compound is air-sensitive in solution, yet is relatively stable
1
to air in solid state. The H NMR spectrum in d6-benzene
again consisted of four peaks, which are shifted slightly to
higher chemical field when compared with the corresponding
peaks in compound 1. The -SiMe3 resonance for 2 is seen
at δ 0.26 ppm, the two distinct methyl resonances from the
mesityl group are at δ 2.11 (4-position) and 2.30 ppm (2,6-
positions), and the two protons on the mesityl ring are found
at δ 6.79 ppm. In the 13C NMR spectra, the -SiMe3
resonance is found at δ 4.00 ppm, the two different methyl
peaks from the mesityl group are at δ 20.75 (4-position) and
21.37 ppm (2,6-positions), and the four aromatic carbons are
found at δ 129.55 (3,5-positions), 132.63 (4-position), 136.61
(2,6-positions), and 143.24 ppm (1-position). Again, both
1H NMR and 13C NMR data indicate retention of the basic
ligand structure. The 119Sn NMR spectrum of 2, however,
was a single peak at 67 ppm, at significantly higher field
than found in 1. This value is at even higher field than the
119Sn shifts of 181 and 193 ppm seen earlier by Lappert with
the binuclear µ-chlorotin(II) amides.7 This indicated to us
that the structure of 2 may well be different from that seen
in the solid state with the dimeric species. To examine the
exact structure, we studied the structure of 2 using single-
crystal X-ray diffraction analysis (Table 1).
As is shown in Figure 2, the crystal structure indicates
that the molecule adopts a chairlike configuration in the solid
state. Two of the -[N(mesityl)(SiMe3)] groups lie on one
side of the six membered ring (up), while the third group is
located on the opposite side of the ring (down). This can be
(11) Babcock, J. R.; Liable-Sands, L.; Rheingold, A. L.; Sita, L. R.
Organometallics 1999, 18, 4437.
(12) Fjeldberg, T.; Hope, H.; Lappert, M. F.; Power, P. P.; Thorne, A. J.
J. Chem. Soc., Chem. Commun. 1983, 639.
Inorganic Chemistry, Vol. 43, No. 22, 2004 7241