K. Karami et al. / Polyhedron 61 (2013) 143–150
145
coupled with two different P nuclei (PPh3 and P = C(H)). Also, the
the anti-symbiotic effect [28], while in 7 the 4-MePy ligand is cis
to the PdꢀCylide. A similar behavior was observed earlier in the case
of ylide complexes of palladium (II) containing the 4-MePy ligand
[8].
orthometallated carbon atoms (C1) in 5 and 8 appear at 126.23
2
2
(d, JPC = 11.6 Hz) and 126.33 ppm (d, JPC = 11.4 Hz), respectively,
coupling with the P atom in the ring, while a coupling with a trans
phosphine should give a coupling constant of about 110–130 Hz
[29,30]. Moreover, in the 1H NMR spectra, the H6 proton of the
orthometallated C6H4 group is shifted to lower frequencies for 5
(6.58 ppm) and 8 (6.60 ppm) because of the anisotropic shielding
from the phenyl ring [27,31]. These data support the structure
shown in Scheme 1 for 5 and 8, in which the PPh3 ligand is trans
to the ylidic C atom, in good agreement with the transphobia be-
tween the PPh3 group and the arylic carbon [20,29,32].
2.3. Theoretical studies
2.3.1. Optimized structures
We have attempted to study important aspects of the prepared
molecules by computational methods. In this part, two complexes
(6 and 7) have been investigated. The X-ray structures of these two
complexes were also obtained. Therefore, we have optimized the
structures of both the cis and trans (CylideꢀPdꢀN) isomers of com-
plexes 6 and 7. The optimized structures of these four molecules
are shown in Fig. 4.
According to the the X-ray structures, complexes 6 and 7 have a
trans and cis geometry, respectively. The calculation of the Gibbs
free energies of both complexes showed that the trans isomers
The 1H NMR spectrum of 7 shows two signals for the P = C(H)
group that are assigned to a fast equilibrium between the cis and
trans isomers or a dynamic activity for exchange of 4-MePy and
Cl groups in solution [1] (Fig. 1).
The major isomer 7a has been characterized as that containing
the 4-MePy ligand cis with respect to the ylidic carbon. This assign-
ment of the structures 7a and 7b has been carried out by compar-
ison of the chemical shifts of the H6 proton of the C6H4 group (ortho
to the metallated position) in the two isomers. Thus, the major iso-
mer 7a shows the signal corresponding to H6 at d = 7.02 ppm, while
the minor isomer 7b shows the corresponding signal at
d = 6.52 ppm. This clear upfield shift can be due to the anisotropic
shielding undergone by H6, which is promoted by the cis pyridine
ligand in 7b. We have also observed the cis structure of complex 7,
with a cis-configuration of the coordinated 4-MePy to the carbon
(C1) of ylide, in the solid state.
are more stable than the cis isomers. The calculated
DGcis–trans val-
ues for 6 and 7 are 5.96 and 1.54 kcal/mol in the gas phase and 3.03
and 0.70 kcal/mol in the solvent (CH2Cl2), respectively. Therefore,
since
DGcis–trans for complex 7 is very low, its cis isomer might be
prepared. In addition, we have calculated the dipole moment of
these complexes. The calculated dipole moments of complexes
6trans, 6cis, 7trans and 7cis are respectively 11.58, 12.29, 13.01 and
12.08 Debye. Interestingly, in each complex, the isomer with a les-
ser dipole moment is the major isomer (trans in complex 6 and cis
in complex 7). We have not found any reasonable evidence for this
observation.
2.2. Crystal structures
From the optimized structures, molecular parameters can be
obtained. The most important parameters for the optimized
structures, in comparison with the X-ray parameters, are listed in
Table 2. A comparison between the calculated parameters of 6cis
and 7trans with those of the X-ray structures confirms that these
structures are close to the real structures. In addition, according
to the data, in both complexes, the PdꢀBr bond length in the cis
isomer is less than that in the trans isomer, and the PdꢀN bond
length in the trans isomer is less than that in the cis isomer. This
observation shows that the phenyl substituent increases the bond
length between the central metal and the opposite ligand, in agree-
Single crystals suitable for structure determinations were ob-
tained by slow evaporation of a concentrated CH2Cl2ꢀhexane solu-
tion of 6 and 7, respectively. Crystallographic data and parameters
concerning data collection and structure solution and refinement
are summarized in Table 1. Figs. 2 and 3 show the ORTEP plot of com-
plexes 6 and 7, and selected bond distances and angles, respec-
tively. The square planar coordination geometry of the Pd atoms
is slightly but not negligibly tetrahedrally distorted, with the metal
atoms protruding from the plane of the C2NBr core by 0.065 and
0.006 Å in 6 and 7, respectively. The distortion from the regular
square planar geometry is indicated by the values of the bond an-
gles subtended at the Pd centers (Figs. 2 and 3).
The P1–C1 bond lengths in 6 and 7 are significantly longer than
that observed in the related free ylide (1.711 Å) of the formula
PPh3C(H)COPh [33]. The PdꢀC bond distances involving the ortho-
metallated carbon and the ylide carbon atoms in 6 and 7 are not
significantly different from those found in related ortho-palladated
complexes (1.991(3), 2.017(5) and 2.115 (3), 2.117(5) Å [6]),
respectively.
The stabilized resonance structure for the parent ylide is de-
stroyed due to the complexation, thus the C19ꢀC20 and C1ꢀC2
bond lengths (1.435(9) and 1.470(3) Å) in 6 and 7, respectively,
are significantly longer than the corresponding distances found
in the similar uncomplexed phosphoranes (1.407(8) Å [34]), mean-
ing that this bond has been relaxed, while the C20ꢀO1 and C2ꢀO1
bond lengths (1.241(8) and 1.221(3) Å in 6 and 7, respectively) are
shorter than that observed in a similar ligand (1.256(2) Å) [34],
which indicates that the C-bonding of the ligand fixes the density
charge at the C atom and breaks the conjugation.
ment with a greater trans influence of Caryl in relation to Cylide
.
Moreover, the BrꢀPdꢀN bond angles in the cis isomer of both com-
plexes are smaller than in the trans isomers.
2.3.2. NBO and population analyses: frontier orbitals and partial
charges
We employed population analyses for all the geometric isomers
to extract the energies of the frontier molecular orbitals (FMOs).
Graphical presentations of the HOMO and LUMO of all the isomers
and their energies (eV) are shown in Fig. 5.
Fig. 5 shows noticeable different electron density distributions
in the frontier orbitals of the cis and trans isomers of each complex
and the electron density in both the LUMO and HOMO orbitals are
different from each other. These differences are related to the loca-
tion of the electron density and its quantity. Therefore, it is obvious
that the reactivity of these complexes is different and the energy
values of the frontier orbitals confirm these differences. By com-
paring the energies of the frontier orbitals, the LUMO–HOMO en-
ergy gap in the cis isomers are less than that in the trans isomers
in both complexes, which shows maybe the cis isomers are more
reactive than trans isomers for these two complexes.
In the crystal structure of 7, the PdC3P five-membered metalla-
cycle assumes an envelope conformation, with the atoms Pd1 and
C1 displaced from the mean plane of the remaining four atoms by
0.3995(2) and 0.2556(3) Å.
Comparing 6 and 7, the crystal structure of 6 shows that the
Me3Py ligand and PdꢀCylide are trans to each other, according to
NBO calculations are used as a useful method for the determi-
nation of many properties, especially for the reproduction of more
exact partial atomic charges. The results of these calculations for
both isomers of complexes 6 and 7 showed that the carbon atoms