A.P. Härter Vaniel et al. / Journal of Molecular Structure 1083 (2015) 311–318
313
Table 2
which was then stirred for a further 24 h. After slow evaporation of
the solvents, red prism-shaped crystals suitable for X-ray analysis
were obtained. Yield of the crystallized complex: 50%, based on
free ligand. Anal. Calc. for C28H27N8O4Pd (645.98 g/mol): C,53.01;
H,4.17; N,17.33%. Found: C,52.8; H,4.11; N, 17.1%. Melting point:
208–212 °C (decomposition). IR (KBr/cmꢂ1) of the free ligand O2-
Selected bond lengths (Å) and angles (°) for [Pd(dmba)(L1)(py)] (1) and [Pd(dmba)(L2)
(py)]ꢁpy (2).
Complex (1)
Complex (2)
Bond lengths
PdAC(31)
PdAN(13)
PdAN(6)
PdAN(5)
Bond lengths
PdAC(41)
PdAN(6)
PdAN(7)
PdAN(11)
1.981(6)
2.047(5)
2.094(5)
2.180(6)
1.363(8)
1.334(6)
1.282(6)
1.987(4)
2.036(3)
2.083(3)
2.149(3)
1.313(4)
NC6H4NNN(H)C6H4NO2: 3282 [s,
[m, (N@N)]; 1326 [vs,
s(NO2)]; and 1170 cmꢂ1 [vs,
[Pd(dmba)(L1)(py)] (2): the
NAH band is absent. 1475 [s,
1322 [s, as(NNN)].
s(NO2)], and 1275 cmꢂ1 [vs,
m
(NAH)]; 1518 [vs,
m
as(NO2)];1405
s(NAN)];
as(NO2)],
m
m
m
m
m
FAC(12)
N(11)AN(12)
Bond angles
m
m
N(13)AN(12)
N(11)AN(12)
Bond angles
C(31)APdAN(13)
C(31)APdAN(6)
N(13)APdAN(6)
C(31)APdAN(5)
N(13)APdAN(5)
N(6)APdAN(5)
C(41)APdAN(6)
C(41)APdAN(7)
N(6)APdAN(7)
C(41)APdAN(11)
N(6)APdAN(11)
N(7)APdAN(11)
C(35)AN(6)APd
N(12)AN(11)APd
93.68(14)
82.48(15)
174.98(13)
176.47(15)
88.27(13)
95.73(13)
117.6(3)
Computational details
93.3(2)
82.8(2)
170.62(19)
174.6(2)
86.5(2)
Density functional theory (DFT) calculations have been per-
formed to study the electronic structure and to determine the reac-
tivity indices (Fukui function) using the Gaussian 09 package [34].
The correlation and exchange functional was described by the
hybrid B3LYP functional [35–36]. The molecular orbitals of the H,
C, N, O, and F atoms were represented by the 6-31G basis set aug-
mented by p and d polarization functions. The Pd orbitals were
described by the compact effective potential with split valence
basis set (CEP-31G) [37]. Geometry optimizations were performed
and the obtained geometries were verified to exhibit only real
infrared frequencies. Local softness maps [38] have been obtained
as differences between calculated electronic densities of the rele-
vant charge states of each studied systems. The resulting 3D maps
were generated through the ChemCraft package [39].
98.2(2)
122.9(3)
coordination geometry around the Pd2+ ion is nearly square-planar
(r.m.s. deviation of 0.1237 Å). The metal center is surrounded
by the C and N atoms of the ortho metallated dmba ligand, a
deprotonated 1-(2-fluorophenyl)-3-(4-nitrophenyl)triazenido ion
[FC6H4NNNC6H4NO2]ꢂ acts as
a monodentate (two-electron
donor), and a neutral pyridine molecule is in a trans position to
the carbon atom of the dmba. The elevation of Pd from the plane
formed by the atoms C31, N13, N5, and N6, is 0.026(3) Å.
The structural parameters of the Pd(dmba) fragment are similar
to those found in other complexes containing this ligand. The
PdAC31 bond distance [1.980(6) Å] and the PdAN6 bond distance
[2.093(5) Å] are in good agreement with the distances found in
other palladium-dmba complexes [22,24,40].
Results and discussion
The dimeric precursor [Pd(dmba)(l-N3)]2 readily undergoes
The PdAN5py bond distance [2.181 Å], which is trans to the
r-
bridge cleavage reactions with deprotonated 1-(2-fluorophenyl)-
3-(4-nitrophenyl)triazene or 1,3-bis(4-nitrophenyl)triazene, in the
presence of pyridine, to afford the monomeric, neutral complexes
[Pd(dmba)(L1)(py)] (1) and [Pd(dmba)(L2)(py)]ꢁpy (2), respectively,
as yellow colored solids (Scheme 1).
bonded aryl group, is longer than the sum of the covalent radii
which is 2.08 Å [41]. The pyridine ring (N5AC45) is planar within
experimental accuracy (r.m.s. = 0.0105 Å). The PdAN5 bond dis-
tance of 2.181(6) Å is longer than the sum of the covalent radii,
which totals 2.08 Å [42], and is in good agreement with values
found in the compounds [PdANPy = 2.03 Å] [43] and [Pd(dmba)-
Py(Cl)] [PdANPy = 2.042 Å] [42].
The IR spectra (KBr pellets) of (1) and (2) show the absence of
the absorption assigned to
mas(N3), which is observed as a very
strong band at 2059 cmꢂ1 in the IR spectrum of [Pd(dmba)(
l
-
The PdAN11 bond length of 2.047(5) Å between the metallic
center and the nitrogen atom of the triazenido chain agrees well
with the Pd-N bond length of 2.034(7) Å observed in the palladacy-
cle [Pd(C6H4NHN@C(CH3)C5H4N)(p-tolNNNp-tol)] [44].
If we take into account the triazenido ligand, we can observe
that it shows a strong deviation from planarity, with the largest
interplanar angle of 26.0(6)° occurring between the phenyl ring
of the ortho-fluorophenyl group and the plane defined by the
N3)]2 [24]. The absence of the
mNAH band in the 3100–
3200 cmꢂ1 region demonstrates the coordination of the triazenido
anions originated by deprotonation of the respective free triazenes,
and this is characterized by strong m
asNNN bands at 1292 cmꢂ1 for
(1) and 1275 cmꢂ1 for (2), respectively.
Crystal data and experimental parameters are given in Table 1.
Selected bond distances and angles of the title complexes are listed
in Table 2. Fig. 1 shows the molecular structure of the entities of
[Pd(dmba)(L1)(py)] (1) in a thermal ellipsoid representation [25–
27].
NNN moiety. Due to the delocalization of the
p electrons over
the nitro group, and the C11AC16 phenyl ring extended over the
N11AN12@N13 chain, in this part of the triazenido ligand the devi-
ation from planarity is less accentuated, with interplanar angles of
The molecular structure of (1) is depicted in Fig. 1. The X-ray
structure analysis shows that, in the monomeric complex, the
R1
H
N
NH2
H2N
Pd
N
N
N
N
N
(i , ii)
(iii)
N
+
N
R2
NO2
R2
R1
NO2
R2
R1
NO2
R1 = F - complex 1
R2 = NO2 - complex 2
(i) NaNO2, HAc, 0-5oC; (ii) H2O, NaCOOCH3; (iii) [Pd(dmba)(N3)]2, KOH, MeOH, pyridine
Scheme 1.