Communication
of 2 equiv Et2O with respect to Cu afforded only LiI(OEt2).[16]
However, the documented solubility of lithium iodide in Et2O
led us to suspect that this was causing the salt to largely
remain in solution during filtration of the reaction mixture and
to be subsequently crystallising. The amount of donor solvent
was therefore further restricted to promote lithium iodide pre-
cipitation and removal. Storage of the resulting filtrate at
À278C yielded crystalline blocks that X-ray crystallography
confirmed to be [{(DMP)2CuLi(OEt2)}2LiI] (7; Scheme 2).[15] As
with 5 and 6, the spectroscopic observation of NH was inter-
preted in terms of extreme moisture sensitivity.
The structures of 6 and 7 are highly analogous to that of 5
and all exhibit approximate C2 symmetry about a central lithi-
um halide axis, as shown representatively in Figure 3. In each
case the halide shows triangulated coordination and two types
of bond to Li+, with Li2ÀX being relatively extended (Li2ÀX
2.412(7), 2.592(7) and 2.971(16) ꢁ in 5, 6 and 7, respectively).
The Li1/3ÀX bonds are somewhat inequivalent: 2.354(6)/
2.301(7), 2.474(8)/2.515(8) and 2.720(13)/2.667(14) ꢁ in 5, 6 and
7, respectively. As would be expected, the metalÀhalide bonds
extend as Group VII is descended. However, this extension is
not consistent and the ratio between Li2ÀX and the mean of
Li1/3ÀX is greater for iodide (1.10) than for chloride or bromide
(1.04 in either case). This suggests that, rather than simply at-
tributing this bond extension to the ionic radius of the halide,
competition between metal stabilisation by hard and soft
donors must also be considered. Thus, in the presence of soft
iodide, Li2 is more inclined to be stabilised by the N2/3-based
DMP ligands. This is reflected also in the Li2-N-Cu angles,
which increase in response to the higher halide: Li2-N2/3-Cu1/
2 94.1(2)/94.2(2)8 (5), 97.3(2)/97.5(3)8 (6), 100.1(5)/101.2(5)8 (7).
A similar trend is seen for the remaining two (N1/4-based) li-
gands, though, consistent with the shorter Li1/3ÀX bonds, the
angles are smaller: Li1/3-N1/4-Cu1/2 87.6(2)/90.1(2)8 (5),
92.5(3)/89.0(3)8 (6), 96.1(5)/96.8(5)8 (7). The asymmetry in these
angles at nitrogen contrasts with the more symmetrical rings
in 2–4, in which the difference between Cu-N-Li and Cu-N-
Li(OEt2) was never more than 38.
Figure 4. Adduct [{(DMP)2CuLi(thf)2}2LiBr] (8). H atoms are omitted. Selected
bond lengths [ꢁ] and angles [8]: Li1-Br1 2.609(11), Li2-Br1 2.677(11), Li3-Br1
2.602(12), Li1-N1 2.067(13), Li2-N2 2.045(11), Li2-N3 2.029(11), Li3-N4
2.094(15), Li1-N1-Cu1 94.3(4), Li2-N2-Cu1 93.9(4), Li2-N3-Cu2 94.2(4), Li3-N4-
Cu2 92.0(4), N2-Li2-N3 132.2(6), Li1-Br1-Li3 147.3(4).
solid-state structures. In all cases a low-field signal (at d=2.16–
2.18 ppm) matches the dominant signal (at d=2.20 ppm) in
a DMPLi reference spectrum. For each of 5, 6 and 7 in
[D6]benzene the dominant signals are seen at d=1.83–1.84
and 1.41–1.50 ppm in a 1:2 ratio, consistent with the crystallo-
graphic data. In the case of 6’, the spectrum is more complicat-
ed, yet still consistent with crystallography. The presence of
Li(DMPH) now introduces a signal at d=1.66 ppm. However,
the proximity of this to the d=1.48 ppm signal attributable to
Li(OEt2) prevents their separate integration. Lastly, for 8 in
[D6]benzene a single environment is observed by 7Li NMR
methods, and we attribute this to the four THF molecules pres-
ent in 8, which create a more polar medium than the two
Et2O/DMPH molecules in 5–7.
Subsequent investigation focused on the reasons for the
transition in structure type from dimers 1–4 to adducts 5–8.
The possibility that solvent identity or quantity was a determin-
ing factor having been removed, competition was presumed
to be dictated by the amide. This can be seen from the chlo-
ride species shown in Figures 2 and 3. The two TMP ligands as-
sociated with any given Cu atom (see N1, N2 in Figure 2) proj-
ect away from one another so as to lie endo,endo with respect
to the structure core (Figure 5, left). In contrast, the presence
Lastly, treatment of DMPLi with CuBr in dry toluene followed
by recrystallisation in the presence of THF at À278C yielded
[{(DMP)2CuLi(thf)2}2LiBr] (8) and established that adduct forma-
tion is not limited to the deployment of Et2O (Figure 4). The
two THF-solvated Li+ ions are now pseudotetrahedral. Al-
though the crystal structure of 8 is largely analogous to that of
6, the effect of using a stronger Lewis base can be noted.
Whereas Li2ÀN2/3 bonds are essentially unaffected, both Li1À
N1 and Li3ÀN4 are extended in 8. Similarly, Li1/3ÀBr1 increases
significantly from 2.474(8)/2.515(8) ꢁ in
6 to 2.609(11)/
2.602(12) ꢁ in 8. The asymmetry in the Li-N-Cu bond angles
noted in 6 is also now absent; the four angles in 8 being es-
sentially identical. Lastly, evidence for additional stability con-
ferred by the four THF molecules in 8 comes from the observa-
tion of a substantially smaller NH resonance in the 1H NMR
spectrum (c.f. 5–7).[15]
Although 1H NMR spectroscopy on adducts 5–7 suggests
some sensitivity towards trace moisture, Li NMR spectroscopic
Figure 5. Structures of the Lipshutz-type monomers incorporated in TMP-
based 2 (left) and DMP-based 5 (right) highlighting the endo,endo and
exo,exo amide orientations.
7
analysis is consistent with a significant level of retention of the
Chem. Eur. J. 2014, 20, 3908 – 3912
3910ꢀ 2014 The Authors. Published by Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim