270
N.M. El-Metwaly, M.G. El-Ghalban / Journal of Molecular Liquids 220 (2016) 265–276
Table 9
Significant bond distances (Å) and dipole moment (Debye) of H3L ligand with its complexes.
1,4,5
2,3
CN15
CN14
CN20
CN19
13O–C
21O–C
22O–C
22O–C
M–N15
M–N14
M–N20
M–N19
M–O13
M–O21
M–O22
M–O22
Dipole moment
1)
2)
3)
4)
5)
1.28024
1.28744
1.44181
1.28199
1.28031
1.279270
1.280491
1.356362
1.280228
1.280206
1.363189
1.363025
–
–
–
–
5.4067
12.1226
7.8208
2.2841
2.9709
1.363221
1.36391
1.36304
1.36301
1.363098
1.36310
1.36301
1.36301
5.457591
3.053270
5.213593
5.213593
4.875687
2.846109
4.884031
4.884031
6.201717
3.838932
–
–
6.226970
3.584711
–
–
transitions, respectively in an octahedral geometry (Fig. 2). The lower
energy shift for d-d transitions is attached with bulk ligands, which
perhaps introduce weak coordination [39]. The spectral parameters
(10Dq, B and β) are also calculated [40]. The values are found to be
11,218, 560.9 and 0.539. The 10Dq value is found within the range of
3A2g → 3T2g (F) (υ1) transition. The β value indicates high covalent inter-
action of sites which convenient with known NiN6 and NiO6 structures
[41]. Generally, the shortage in β value is strongly associated with the re-
duction in the effective positive charge of central atom [42]. The Racah
inter-electronic repulsion parameter values are varied for 3d transition
metal complexes with changing Z and q values. Whereas, Z is the effective
cationic charge and q is the occupation number of the dq shell. The Racah
parameter is well-expressed by the relation: B (cm−1) = 384 +
58q + 124(z + 1) − 540 / (z + 1). The z value of cobalt is +1.103, con-
siderably below the formal oxidation state (II) this reduction in oxidation
state is suitable for M–N or M–O bonds [43]. Whereas, the value for nickel
is −0.256, which reflects the overcoming of ligand anionic character on
the nickel charge. The electronic spectra of two diamagnetic complexes,
[Pd(Cl)2(C15H14N4O2S)](H2O) and [Pt(Cl)2(C15H14N4O2S)](H2O) are in-
dicative for square-planar geometries (Fig. 2). Three spin-allowed
singlet-singlet d-d transitions are anticipated for the geometry proposed.
The ground states 1A1g, 1B1g and 1Eg are in order of increasing energy in
low spin d8 systems. 1A1g → 1A2g (υ1) and 1A1g → 1B1g (υ2) transitions
observed at ≈20,000 and 22,000 cm−1 are characteristic for four arms
surround the nucleus in planar state. Also, charge transfer bands observed
in all investigated spectra in the range of 28,000–30,000 cm−1 may assign
for N → M and O → M bands. Intra-ligand transition bands expose to little
the line width at half maximum height, Cu/Kα (λ) = 1.5406 Å. The
inner crystal plane d-spacing values were determined by using Bragg
equation: nλ = 2dsin(θ) at n = 1. The sizes calculated are distinguished
in nanometer sized range (below 15 nm). The edge lengths of the parti-
cles for imaginative cubic shapes are as fellow; 93.72(H3L), 101.78(Co).
79.04(Ni), 79.11(Pd) and 70.03(Pt) Å.
3.5. Transmission electron microscopy
TEM has turn out as widely employed method for illustrating the
particle shape and size. High resolution transmission electron micro-
graph images were extracted (Fig. 3S). The micrographs exhibit nano-
meter sized particles for Co(II) and Ni(II) complexes with diameter
range 10.2–91.5 nm. The size determined for the ligand, Pd(II) or
Pt(II) complexes display their presence in micro-scale. This appearance
may refer to the aggregation for the particles which prohibit the exact
determination. The images show the spherical shape as the main aspect
except Pd(II) complex appears by rocky shape [37]. The spherical shape
of nano-particles may be attributed to highly symmetric spherical
chlorido groups introducing the complexation area. These topologies
of the complexes pointed to the presence of metal ions have a signifi-
cant influence on the formation of the nanometer particles [47]. The
spherical shapes observed express that these morphologies are consti-
tuted by a distinct accumulation of several individual particles in poly-
crystalline nature. The aspect of moderately strong diffraction spots
rather than diffraction rings confirms the formation of moderately sin-
gle crystalline cube of complexes [48,49]. The dark areas in micrographs,
are related to the high concentration of the particles naturally com-
bined. The nanometer sized aspect may improve the properties in
current application concerning the biological activity area with respect
to bulk analogue. This feature may facilitate the penetration of particles
inside the cell membrane. The out of comparison in-between the XRD
and SEM results may clarify the difference between two techniques
with the priority of XRD.
shifted appearance around 31,000–35,000 cm−1 attributed to n → π and
⁎
⁎
π → π transitions.
3.4. X-ray diffraction
XRD patterns were carried out in the 10° b 2θ b 90° range for the free
ligand and its complexes [Figs. 3, 2S] to give an apparent seeing about
the lattice dynamics of solid compounds. The clear patterns exhibit
the absence of contamination of starting materials. Known methods
[44] were used to emphasize on the obscurity of peaks attributed to
the reactants. All the patterns reflect comparatively nano-crystalline
features for all compounds [45,46]. This may be attributed to the forma-
tion of a well-defined distorted crystalline structures. The θ, d values,
full width at half maximum (FWHM) of prominent intensity peak,
relative intensity (%) and particle size of compounds were existed in
Table 5. The crystallite size was calculated by applying FWHM of the
characteristic peaks using Deby–Scherrer equation: B = 0.94 λ /
(S Cos θ), where S is the crystallite size, θ is the diffraction angle, B is
3.6. Thermal analysis
The plausible degradation behavior of all interested compounds over
the stages was translated to the data displayed in Table 6. The Schiff base
ligand was decomposed completely over three stages till reaching
550 °C with carbons residue. The degradation process for all investigat-
ed complexes was started at low temperature. The first step contributes
to the removal of solvent molecules attached physically with the coordi-
nation sphere. The coordinating sphere starts its decomposition approx-
imately with the first step which takes a broad range of temperature.
Table 10
Molecular docking energy values obtained for Schiff base ligand towards different receptors.
Receptor
Est. free energy of binding
(kCal/mol)
Est. inhibition constant
(Ki) (uM)
vdW + bond + desolve
energy (kCal/mol)
Electrostatic energy
(kCal/mol)
Total intercooled energy
(kCal/mol)
Frequency
Interact
surface
2ylh
3t88
3cku
3ty7
2jrs
−6.53
−4.92
−2.82
−3.60
−3.34
16.30
246.46
8.52
2.31
3.59
−8.38
−7.26
−4.67
−5.30
−5.74
−0.22
+0.05
+0.05
−0.17
−0.06
−8.60
−7.22
−4.62
−5.47
−5.80
30%
10%
10%
10%
30%
686.011
721.741
451.107
538.005
631.708