P.K. Singh, D.N. Kumar / Spectrochimica Acta Part A 64 (2006) 853–858
855
Table 2
IR spectral data of ν(OH), ν(NH), ν(C O), ν(C N), δ(N H), ν(N N), ν(C N) + δ(N H), ν(N H) + δ(C O), ν(M O) and ν(M N) in cm
−
1
Compound
ν(OH)
ν(NH)
ν(C O)
(C N)
δ(N H)
ν(N N)
ν(C N) + δ(N H)
ν(N H) + δ(C O)
ν(M O)
ν(M N)
H2L1
1
3495
3160
1650
1550
1535
1525
1535
1580
1530
1520
1536
1490
960
1000
995
1000
965
1015
1025
1020
[
[
[
CoL ]·2H2O
3350a
1630
1635
1625
1335
1340
1345
470
480
465
345
360
365
1
a
NiL ]·2H2O
3360
1
3385a
3510
CuL ]·2H2O
2
H2L
3280
1640
1520
2
3385a
[
[
[
CoL ]·H2O
1635
1630
1630
1330
1335
1345
480
485
465
350
365
345
2
a
NiL ]·2H2O
3380
3390a
2
CuL ]·2H2O
a
Due to water molecule.
stable in air. The melting points of the complexes are higher than
that of the ligands revealing that the complexes are much more
stable than the ligands. Due to insolubility of the complexes
in benzene/nitrobenzene, the molecular weights could not be
obtained by cryoscopy. The molar conductance values (Table 1)
3
.2. 1H NMR spectra
The 1H NMR spectra of the ligands (H2L1 and H2L2)
recorded in DMSO-d . The down field shift of the OH pro-
ton in the ligand which resonates at 10.4 ppm in its H NMR
spectrum indicates that the OH proton in ligands are proba-
bly involved in the formation of strong intramolecular hydrogen
bonding (Fig. 1).
6
1
−
1
2
−1
of the complexes lies in the range 18.3–25.2 ꢀ cm mol (at
◦
1
5 C) which indicates that the complexes are of non-electrolytic
nature [9].
The NMR spectrum of the ligands exhibits NH proton at
1
1.16 ppm, a >CH proton at 4.65 ppm, naphthalene ring pro-
3
.1. Infrared spectra
tons at 6.2–8.68 ppm (multiplets), isonicotinyl protons at 9.00
and 8.10 ppm (each as a doublet) and theonyl protons at 7.75
and 8.79 ppm (each as a doublet). The H NMR spectra of the
complexes cannot be obtained due to interference in their para-
magnetic properties.
The IR spectra (Table 2) of the ligands show characteris-
1
tic absorption bands at 3490–3515, 3150–3280, 1630–1660,
−
1
1
545–1590, 1485–1530 and 958–969 cm
due to ν(O H),
ν(N H), ν(C O), ν(C N), δ(N H) and ν(N N), respectively.
The IR spectra (Fig. 2(A)–(F)) of the complexes reveal signifi-
cant changes compared to those of the ligands. The absorption
bands at 3450–3490 cm for ν(O H) in the free ligand dis-
appeared on complexation indicating coordination through a
deprotonatedoxygen. Theabsorptionbandattributedto ν(N H),
ν(C O) and δ(N H) disappeared in the complexes and two new
3.3. Ligand field spectra and magnetic moments
−
1
The ligand field spectra (Table 3) of all the complexes were
recorded in DMF at room temperature.
The electronic spectra of Co(II) complexes displayed three
−
1
−1
bands at 7900–8150 cm (ν1), 16 300–16 400 cm (ν2) and
1
−
bands due to conjugate system ν(>C N N C<) and ν(C O )
−
1
4
4
9 600–20 150 cm
(ν3) corresponding to T1 g (F) → T2 g
−
1
[
8] appeared in the regions 1620–1635 and 1330–1345 cm
,
4
4
4 4
(
F), T1 g (F) → A2 g and T1 g → T1 g (P) transitions, respec-
tively, characteristic of octahedral geometry of complexes
11,12].
The values of transition ratio ν2/ν1 and β lies in the range
respectively. The band for ν(C N) undergoes a bathochromic
shift of 15–25 cm (in H2L ) and 50–60 cm (in H2L ) and
ν(N N) band exhibited a hypsochronic shift of 35–45 cm (in
−
1
1
−1
2
[
−
1
1
−1
2
H2L ) and 50–60 cm (in H2L ) which indicate that the metal
ions form neutral coordination compounds with the ligand in the
enol form through the azomethine nitrogen and amide oxygen
negative ion [10]. A shift of ν(C N) band to a lower frequency
is due to the conjugation of the p-orbital on the double bond with
the d-orbital on metal ion with reduction of the force constant.
A shift of ν(N N) band to a higher frequency is attributed to the
electron attracting inductive effect when forming the conjugated
system [8].
The characteristic absorption bands of the ligands and com-
plexes attributed to (C C) and (C H) of the naphthalene ring
appear at 1565–1590 and 730–745 cm regions, respectively.
The new absorption band at 3350–3410 cm in all the com-
plexes, assignable to hydroxyl stretching vibration of the crystal
water involved in the complexes. In the far—IR region two new
2
.06−2.09 and 0.87, respectively, providing further evidences
for octahedral geometry for cobalt(II) complexes. The room
temperature magnetic moment values of Co(II) complexes are
within the range 4.28−4.99 BM suggest spin free octahedral
geometry [12,13].
The nickel(II) complexes displayed three bands 8880–
− −1
1
9000 cm (ν1), 14 850–14 950 cm (ν2) and 25 000–25 100
Table 3
Ligand field spectral data (cm 1) of complexes
−
Compound
ν1
ν2
ν3
ν2/ν1
β
−
1
1
[
[
CoL ]·2H2O
7900
16350
14870
19000
16380
14900
20000
19700
25050
2.070
1.673
0.87
0.90
−
1
1
NiL ]·2H2O
8890
14500
7950
8900
15600
1
[CuL ]·2H2O
2
[
CoL ]·H2O
20140
25000
2.060
1.674
0.88
0.91
2
−
1
[NiL ]·2H2O
bands around 465–485 and 340–365 cm in the complexes can
be assigned to ν(M O) and ν(M N), respectively.
2
[
CuL ]·2H2O