metal-organic compounds
Figure 3
The one-dimensional chain structure in (I). [Symmetry codes: (ii) 1 ꢀ x, 1 ꢀ y, 1 ꢀ z; (iii) ꢀ x, 1 ꢀ y, 1 ꢀ z.]
Structural views of (I) and (II) are shown in Figs. 1 and 2,
respectively, and selected bond lengths and angles are given in
Tables 1 and 3. In complex (I), the CuII ion displays a highly
Jahn–Teller-distorted CuN2O4 octahedron, with the equatorial
plane defined by the two N atoms (pyridyl N1 and hydrazine
N2) of the Lꢀ ligand and atoms O4 and O5 of the acetyl-
acetonate ligand. The Cu1—N1 and Cu1—N2 distances are
similar to the values reported for other copper complexes
involving N-donor ligands (Table 4). The Cu1—O4 and
Cu1—O5 bond lengths correspond to the distances observed
in other Cu–acetylacetonate complexes (Heinze & Reinhart,
2006). There is no significant deviation of the metal centre
from the N2O2 equatorial plane, which shows a small but
significant tetrahedral distortion. The maximum displace-
ments from the least-squares plane through atoms N1, N2, O4
and carboxyl atom O1iii of an Lꢀ ligand [symmetry code: (iii)
ꢀx, 1 ꢀ y, 1 ꢀ z], with two weak coordination bonds of
˚
2.847 (3) and 2.894 (3) A, respectively (Das & Pal, 2005;
Heinze & Reinhart, 2006).
The tridentate hydrazone ligand Lꢀ is a bridging ligand to
coordinating to two neighbouring CuII ions through its donors
carboxyl atom O2, hydrazine atom N2 and phenolic atom O1.
In addition, acetylacetonate atom O5 acts as a bridging atom
linking Cu1 and Cu1ii. Therefore, a one-dimensional chain is
built up, consisting of CuN2O4 octahedra connected alter-
nately by pairs of the different ligands along the a axis, shown
in Fig. 3.
The planes through the acetylacetonate (O4/C15–C19/O5)
and picoloylhydrazone (C1–C5/N1/C6/O1/N2/N3) groups
make dihedral angles of 17.40 (18) and 8.60 (18)ꢂ, respectively,
with the equatorial N2O2 plane. More buckling of acetyl-
acetonate than picoloylhydrazone allows for a closer approach
of atom O5 towards Cu1ii and simultaneously reduces the
steric interaction between the two ligands (Bhadbhade &
Srinivas, 1993) (Fig. 3). The O—H function of the vanillin
group connects to the carboxyl O atom of the adjacent chain
via an O3—H3Bꢁ ꢁ ꢁO1i hydrogen bond [symmetry code: (i) x,
˚
and O5 are ꢀ0.0798 (15) and 0.0824 (15) A for atoms N2 and
˚
N1, respectively; Cu1 is 0.0339 (16) A below this plane. The
two axial positions are occupied by carbonyl atom O5ii of an
acetylacetonate ligand [symmetry code: (ii) 1 ꢀ x, 1 ꢀ y, 1 ꢀ z]
1
2
1
2
ꢀ y, ꢀ + z], giving rise to a three-dimensional supra-
molecular assembly, as shown in Fig. 4.
In complex (II), atom Cu1 displays a square-planar coor-
dination geometry (Fig. 2). The Cu1—N and Cu1—O bond
lengths in the N2O4 plane are comparable with those found in
(I) (Table 3). However, unlike (I), (II) does not form chains
but is rather a simple discrete complex. The closest distance
between a CuII ion and an O atom from a neighbouring
iii
˚
molecule is 3.334 (4) A for Cu1ꢁ ꢁ ꢁO3 , indicating that no
intermolecular interactions are present. Just as in (I), there is
no significant deviation of the metal centre from the N2O2
coordination plane and the distortion of this plane is even
smaller. The maximum displacements from the least-squares
plane through atoms N1, N2, O3 and O4 are ꢀ0.042 (2) and
Figure 4
The three-dimensional supramolecular structure of (I). [Symmetry code:
˚
1
2
1
2
0.043 (2) A for atoms N2 and N1, respectively; Cu1 is
(i) x, ꢀ y, ꢀ + z.]
ꢃ
m376 Li-Fang Jiang [Cu(C14H12N3O3)(C5H7O2)] and [Cu(C14H12N3O2)(C5H7O2)]
Acta Cryst. (2010). C66, m375–m378