M. Amirnasr et al. / Polyhedron 29 (2010) 985–990
989
The electronic absorption spectral data of the ligand L and its
metal complexes are listed in Table 2. The ligand is a deep red solid
and its solution in acetonitrile has a strong absorption at 492 nm
(e
= 1167) assigned to a n ?
p* transition arising from the interac-
tion of the ketone oxygen lone pairs with the
p
system of the mol-
ecule. This transition is slightly red shifted when the pyridines are
protonated (512 nm) or coordinated to the metal ions (510–
526 nm). The absorption at wavelengths less than 400 nm in the li-
gand are assigned to
p ? p* transitions of the rings. Additional CT
transitions are expected for the metal complexes which appear be-
low 400 nm. The ligand field transitions for CoLCl2 (1) and CoLBr2
(2) complexes (Fig. 1) include the intense multicomponent bands
in the near-infrared region (6000–11000 cmꢁ1) and in the visible
region (14500–22000 cmꢁ1) as expected for a pseudotetrahedral
stereochemistry [15].
The electronic spectra of nickel complexes, NiLCl2 (3) and NiL-
Br2 (4), (Table 2) is consistent with a pseudotetrahedral structure
(Fig. 2). The broad absorption bands near 7000 cmꢁ1 (components
of 3T2) and 10000 cmꢁ1 (3A2) and the shoulder at 17000 cmꢁ1
(components of 3T1(P)) which overlaps with the n ?
p* of the li-
gand are in accord with a C2v symmetry of these complexes [15].
On the basis of the striking similarity of the spectroscopic proper-
ties of CoLBr2 (2) and NiLCl2 (3) complexes with those of CoLCl2 (1)
and NiLBr2 (4) for which the X-ray structures have been deter-
mined (vide infra) a similar structure can also be inferred for (2)
and (3) complexes.
3.3. Crystal and molecular structures of (1) and (4)
The crystallographic and refinement data are summarized in
Table 1 and the selected bond distances, bond and torsion angles
are given in Table 3. The molecular structures of (1) and (4) are
illustrated in Figs. 3A, 3B and 4, respectively with metal atoms
coordinated by the bidentate bis(2-pyridyl) ligand and two halo-
gen atoms.
Fig. 6. Projection of the structure of 4 along the a-axis. Coordination tetrahedra of
Ni atoms are shown in green. (For interpretation of the references to colour in this
figure legend, the reader is referred to the web version of this article.)
membered ring is highly puckered with endocyclic torsion angles
given in Table 3.
The structure of CoLCl2ꢀ0.5CH3CN (1) consists of two, chemically
identical but conformationally different molecules in the asym-
metric unit. A highly puckered seven-membered chelation ring is
formed with endocyclic torsion angles presented in Table 3. The
The packing of both compounds in the crystals is very different
and it is shown in Fig. 5 and 6. In crystal structure of (1), there is
apart from weak hydrogen bond of C–Hꢀ ꢀ ꢀCl, C–Hꢀ ꢀ ꢀN and C–
0
0
average Co–N [2.034(10) ÅA] and Co–Cl [2.224(7) AÅ] bond distances
and the N–Co–N [93.82(16)°] and Cl–Co–Cl [114.7(14)°] bond
angles conform to those reported for the related complex [di-
chloro(2,5-diphenyl-3,4-di-2-pyridyl-1H-pyrrole-N,N0)cobalt(II)] [2].
The structural parameters such as the crystal system, space group,
unit cell dimensions, and the crystal packing of compound (1) (tri-
Hꢀ ꢀ ꢀO types a quite strong
p–p interaction present between the
aromatic phenyl rings C41Aꢀ ꢀ ꢀC46A and C41Bꢀ ꢀ ꢀC46B (symmetry
operation: 2 ꢁ x, 1 ꢁ y, 1 ꢁ z) with a centroid–centroid distance
of 3.7185(8) Å. In crystal structure of (2), there are weak H-bond
interactions of type C–Hꢀ ꢀ ꢀBr present, but no
p–p interaction was
interaction between the chloro-
observed there. Instead, a C–Hꢀ ꢀ ꢀ
p
ꢀ
clinic, space group P1 and Z = 2) are different from those of CoLCl2
form molecule and the phenyl ring C41ꢀ ꢀ ꢀC26, with hydrogen atom
distance to the centroid of this ring being 2.83 Å, has been
recognized.
(monoclinic, space group P21/c, Z = 4), that we have reported previ-
ously [16]. Compound (1) involves solvent molecules in its unit
cell, which is apparently the source of these structural differences.
It is interesting to compare the structure of CoLCl2 (1) with that
of the unchelated analogue, Co(3-pic)2Cl2 [17]. The two structures
are similar, with pseudotetrahedral cobalt coordination. However,
the N–Co–N angle is 104.19(8)° in the unchelated complex
whereas it is 93.71(4)° and 93.93(4)° in the chelate CoLCl2. This
large deviation is presumably the source of some strain in the
structure of the complex, leading to the release of the L ligand in
strongly coordinating solvents.
4. Conclusion
The present study revealed tetrahedral geometry around Co(II)
and Ni(II), where the metal atoms are coordinated by the bidentate
bis(2-pyridyl) ligand and two halogen atoms. These complexes
proved to be unstable in strongly coordinating solvents, presum-
ably due to the strain imparted by the structurally rigid L ligand.
A convenient method of synthesis for the preparation of these
complexes in chloroform was concluded.
The NiLBr2 complex (4) also adopts a pseudotetrahedral struc-
ture where the tetrahedron is somewhat distorted by a small N–
Ni–N angle being 94.84(9)°. The Br–Ni–Br angle has opened up to
125.08(2)°. The Ni–N distances ranging from 2.008(2) to
Supplementary data
0
2.018(3) ÅA are considered normal and comparable to those for (1)
and relate0d complexes [2,16]. The average Ni–Br distance of
2.365(14) ÅA agrees well with normal Ni–Br bond distances in the
related complex, Ni(Phca2en)Br2 [18]. As in CoLCl2 (1), the seven
CCDC 661283 and 661284 contain the supplementary crystallo-
graphic data for 1 and 4. These data can be obtained free of charge