4
P.T. Morse et al. / Polyhedron xxx (2015) xxx–xxx
Table 5
3.3. Crystal structures of the complex
Selected bond lengths (Å) and angles (°) for structure 4.
3.3.1. Crystal structures of the 1:3 Th–ligand complex from MeOH and
CHCl3
1:1 Th(IV)–ligand complex
1:2 Th(IV)–ligand complex
Th1–O1
2.381(5)
Th2–O3
Th2–O4
Th2–O5
Th2–O6
Th2–O22
Th2–O23
Th2–O25
Th2–O26
2.348(5)
2.342(5)
2.377(4)
2.351(5)
2.557(6)
2.589(6)
2.573(5)
2.543(5)
2.627(5)
2.550(5)
73.63(17)
72.35(17)
48.31(18)
50.03(16)
48.80(18)
Crystals suitable for X-Ray diffraction of the Th(NO3)2-13ꢂ(NO3)2
complex were grown by slow vapor diffusion of benzene into a
concentrated solution of the complex in methanol to give structure
2. Alternatively, crystals were also obtained by the vapor diffusion
of carbon tetrachloride into a concentrated solution of the complex
in chloroform to give structure 3. Crystal structure and refinement
data for structures 2 and 3 are given in Table 2.
Th1–O2
Th1–O7
Th1–O8
Th1–O10
Th1–O11
Th1–O13
Th1–O14
Th1–O16
Th1–O17
Th1–O19
Th1–O20
O1–Th1–O2
O7–Th1–O8
O10–Th1–O11
O13–Th1–O14
O16–Th1–O17
O19–Th1–O20
2.360(5)
2.593(6)
2.643(5)
2.601(5)
2.550(5)
2.636(5)
2.619(5)
2.597(5)
2.607(6)
2.656(5)
2.618(5)
68.23(17)
48.60(17)
49.41(16)
48.44(15)
48.85(16)
47.98(16)
Th2–O28
Th2–O29
ꢀ
Complex 2 crystallized in the triclinic space group P1. The
O3–Th2–O4
O5–Th2–O6
O22–Th2–O23
O25–Th2–O26
O28–Th2–O29
asymmetric unit consists of one ten-coordinate 1:3 Th(NO3)2–
ligand complex and two outer sphere nitrate anions (Fig. 2) with
Th–O distances ranging from 2.394 to 2.641 Å. The overall metal
coordination geometry resembles a distorted bicapped square
antiprism where the bidentate nitrato groups occupy the apical
positions. Three ligands, all bidentate, are coordinated along the
equator of the Th(IV) ion. Two of these coordinated ligands are
bound nearly parallel to one another and the equator, while the
third is coordinated in a perpendicular orientation (O5 and O6).
To accommodate this orientation, the coordination of the apical
nitrato groups is tilted slightly away from O5 and O6 of the third
ligand.
Extensive pi–pi and CH–pi interactions exist both intramolecu-
larly and intermolecularly throughout the crystal lattice. One phe-
nyl ring (C74–79) is disordered and was modeled with 50%
occupancy over two positions. Both orientations of this disordered
ring engage in pi-stacking interactions with nearby phenyl rings.
One outer sphere nitrate was ordered in the matrix, however the
second nitrate ion along with, we suspect, solvent methanol or
water was disordered in a large space within the crystal lattice
(see packing diagram, Fig. 3). Attempts to model these disordered
molecules were unsuccessful. The intensity contribution of the
disordered nitrate and solvent molecules was removed using the
BYPASS procedure [27] as implemented in OLEX2 [21,22]. This
space is located at average x, y, z coordinates of [ꢁ0.537, 0.000,
ꢁ0.478], has a calculated size of 998.5 Å3, and contains approxi-
mately 170 electrons.
Table 6
Selected bond lengths (Å) and angles (°) for structure 5.
Th1–O1
Th1–O2
Th1–O3
Th1–O4
Th1–O5
Th1–O6
Th1–O7
Th1–O8
2.435(3)
2.489(3)
2.377(3)
2.411(3)
2.413(3)
2.403(3)
2.616(3)
2.585(3)
2.543(3)
2.642(3)
1.4334(7)
1.439(6)
68.86(10)
69.31(10)
71.11(11)
48.83(10)
48.95(11)
60.9(4)
Th1–O10
Th1–O11
C1–O13
C2–O13
O1–Th1–O2
O3–Th1–O4
O5–Th1–O6
O7–Th1–O8
O10–Th1–O11
C1–O13–C2
scale, and the observed broadening in the 1H NMR spectrum is
caused by the presence of the Th(IV) metal.
The coordination environment of the Th(IV) metal center in
structure 3, grown out of the non-coordinating solvent chloroform,
is very similar to that of 2 grown from methanol (Fig. 4). Complex 3
crystallized in the monoclinic space group P21/n. The asymmetric
unit consists of one ten-coordinate 1:3 Th(NO3)2–ligand complex,
two outer sphere nitrate anions, and one molecule of solvent car-
bon tetrachloride. This complex, again, is ten-coordinate with a
similar arrangement of three ligands and two nitrato groups bound
to the Th(IV) center having Th–O bond distances ranging from
2.3857 to 2.6497 Å. Extensive pi–pi stacking interactions can be
seen between adjacent molecules of the complex, as shown in
Fig. 4. One of the aromatic rings, C73–C78, was disordered over
two positions (80:20 ratio) where both orientations could partici-
pate in favorable CH–pi interactions with neighboring phenyl
rings. Due to the close packing of the aromatic groups in this struc-
ture, the two orientations of ring C73–C78 affected the position of
ring C43–C48 ever so slightly, but enough to merit the modeling of
this ring in two separate orientations as well. Since this disorder is
localized to the pendant aromatic rings and does not affect the
metal center, we show both models only in the Supporting
Information.
A different picture of the dynamics emerges when the complex
Th(NO3)2-13ꢂ(NO3)2 is dissolved in the non-coordinating solvent
CDCl3. The signals in the 1H NMR spectra are severely broadened
and, unfortunately, uninterpretable. The 31P{H} NMR spectrum
shows three sharp singlets corresponding to what, we propose,
are three different magnetic environments for the phosphorus
atoms in the ligands (Fig. 1). The signal at 21.5 ppm likely
corresponds to free, uncoordinated ligand as this chemical shift is
the same as observed for 1 alone in CDCl3. The signals at 31.5 and
33.9 ppm likely correspond to metal bound ligands in complexes of
different stoichiometry (i.e. 1:2, 1:3).
As to why different 31P{H} NMR spectra are observed for the
complex dissolved in these two different solvents, we can employ
a relatively simple explanation related to the solvent’s role in
assisting ligand dissociation. In the case of CD3OD, the solvent
likely aids in the dissociation mechanism of the ligand by occupy-
ing a metal coordination site when the ligand detaches from the
metal. This reduces the energy barrier of the dissociation process,
resulting in a time averaged signal for the ligand in both the 1H
and 31P{H} NMR spectra. Conversely, in CDCl3 there is no assistance
from the solvent in this ligand exchange mechanism and the
process slows on the 31P NMR time scale and multiple species
can be observed in solution as separated phosphorus signals. The
1H NMR spectrum is difficult to interpret because the multiple
species have overlapping signals and interfere with one another.
Two spaces, both having volumes of 1307 Å3 and containing
approximately 506 electrons, are also present in the unit cell with
average x, y, z coordinates of [ꢁ0.019, 0.000, 0.000] and [ꢁ0.209,
0.500, 0.500]. We suspect these spaces contain a mixture of
disordered chloroform and carbon tetrachloride molecules. The