3
46
A. Rujiwatra et al. / Polyhedron 31 (2012) 345–351
0
2+
homogeneous under magnification. X-ray diffraction analysis of
several crystals at room temperature confirmed this. Satisfactory
chemical analysis data were obtained for 2.
with Z = 1. Each Ni is approximately octahedral in coordination
0
geometry, bound to a bidentate molecule of 2,2 -bipyridine, three
molecules of water, and a monodentate nitrate. The lengths of
the coordination bonds about nickel are in good agreement with
others of similar complexes. The CCDC [2] has 133 structures
containing nickel, bipyridine, and ligated water. For these, the
mean Ni–O (water) and Ni–N bond lengths are 2.08(4) and
.07(4) Å, respectively, while the mean N–Ni–N angle is
79.0(15)°. For form 2 at 120 K, the bond lengths are 2.054(4),
.078(4) and 2.083(5) Å (Ni–O), and 2.050(5) and 2.081(5) Å (Ni–
N), while the N–Ni–N angle is 79.4(2)°. For 63 structures with
monodentate nitrate and at least two pyridyl donors, the mean
Ni–O (nitrate) bond length is 2.10(7)Å and for 2 this bond length
is 2.082(4). A further uncoordinated nitrate anion forms hydrogen
bonds to the bound water. The distance between hydrogen atoms
of water and unbound nitrate are: 1.91(3) Å (O1–H1BꢀꢀꢀO10) and
1.94(3) Å (O2–H2BꢀꢀꢀO9). An ORTEP representation of 2 is shown
in Fig. 1. Basic crystal data are given in Table 1.
The bound nitrate forms a single hydrogen bond to water in an
adjacent complex. Every hydrogen atom of the three water mole-
cules is involved in hydrogen bonding to nitrate. A full list of these
is given in Table 2. There is a tendency to short, linear, hydrogen
bonds with few bifurcated interactions (Fig. 2b). The combination
of hydrogen bonds between the complexes and unbound nitrate
generates infinite puckered sheets of thickness 5.552 Å that extend
in the xy plane. These sheets are two molecules thick and the
2.2. X-ray diffraction analysis
Routine X-ray diffraction data collection and structure solution
2
procedures were adopted.
0
A
single crystal of dimensions
.21 ꢁ 0.11 ꢁ 0.06 mm was cut from a larger aggregate, coated
in perfluoropolyether oil and mounted at the end of a glass fibre.
Data were collected in series of -scans using a Stoe IPDS2 diffrac-
3
2
x
tometer operating with Mo radiation. The crystal temperature was
maintained using an Oxford Instruments nitrogen gas cryostream.
The structure was solved by direct methods [12]. Full matrix least
2
squares refinement against F implemented within SHELXL [12] was
employed for structure refinement.
0
Hydrogen atoms attached to 2,2 -bipyridine were positioned
and refined using a riding model. Those of water were located in
difference Fourier maps and their positions refined subject to the
restraint that all O–H bond lengths were the same with a standard
deviation 0.03 Å. Sensible restraints were also applied to the geom-
etry of the water molecules.
For the first data collection the crystal was held at 120 K and a
full set of data collected. Subsequently, the crystal was glued to the
fibre and further sets of data frames collected, sufficient to deter-
mine the unit cell. The unit cell was determined at a further nine
temperatures. A set of twenty data frames were collected at
0
+
[
2 3 3
Ni(2,2 -bipyridine)(H O) NO ] ions are arranged such that the
aromatic rings of the bipyridine are approximately perpendicular
to the layers and project above and below them. The sheets are
c in ABAB fashion at a separation of c/2
10.903(4) Å). This arrangement facilitates two types of intermo-
3
53 K and the data from these were used to refine the structure
at this temperature.
stacked along
Routine X-ray diffraction data collection and structure solution
(
procedures were adopted for form 1 using a crystal of dimensions
3
lecular interactions. The hydrogen bonding within the layer is
illustrated in Fig. 2. Interdigitation of the aromatic rings on adja-
0
.48 ꢁ 0.12 ꢁ 0.11 mm .
cent layers leads to relatively close approach of the
p-systems of
2
.3. Spectroscopic characterisation
neighbouring bipyridine ligands. The distance between these is of
i
the order of 3.43 Å; for example C7 (i = x ꢂ ½, y, 1 ꢂ z) lies
IR spectra were collected from ground crystals of 2 as a KBr disc,
ꢂ1
3.376(6) Å above the ring formed from N1 and C1–C5. This close
using a Bruker Tensor 27 FT-IR spectrometer (4000–400 cm , res-
olution 0.5 cm ).
ꢂ1
approach is suggestive of a p–p interaction. In addition the prox-
ii
imity of H3 to an adjacent bipyridine (H3ꢀꢀꢀC9 = 2.80 Å, ii = ꢂx,
UV–Vis reflectance spectra were collected from lightly ground
crystals loaded in a BaSO
Spectrophotometer.
4
matrix using a Cary 5E UV-vis-NIR
2.4. Thermogravimetry
Samples were placed into platinum pans, loaded into a Mettler-
Toledo TGA/DSC1 Thermogravimetric Analyzer and heated under a
flow of nitrogen from room temperature to 1000 °C at a ramp rate
ꢂ1
of 30 °C min
.
3
. Results and discussion
3.1. Crystal structure analysis
0
A report of the structure of [Ni(2,2 -bipyridine)(H
at room temperature has appeared previously [13]. This compound
hereafter 1) crystallises in the centrosymmetric monoclinic space
group P2 /c and is isostructural with the manganese analogue [14].
2 3 3 3
O) NO ](NO )
(
1
Here we describe a second crystal form (2) for this compound ob-
tained under microwave-assisted hydrothermal conditions that
displays the same connectivity as 1, but differs in the orientation
of the groups present. A description of the structure of 1 and its
relation to 2 appears later.
Fig. 1. ORTEP plot of the asymmetric unit of 2. Atoms are shown as 30% thermal
ellipsoids. Hydrogen bonds are illustrated by dashed lines. Selected bond lengths:
Ni1–N1 2.081(5) Å, Ni1–N2 2.050(5) Å, Ni1–O1 2.054(4) Å, Ni1–O2 2.078(4) Å, Ni1–
O3 2.083(5) Å, Ni1–O4 2.082(4) Å.
The structure of 2 was initially determined at 120 K. At this
0
temperature [Ni(2,2 -bipyridine)(H
O)
2 3
3 3
NO ](NO ) was found to
crystallise in the centrosymmetric space group Pbca (number 61)