1014
A.A.A. Emara, A.A.A. Abou-Hussen / Spectrochimica Acta Part A 64 (2006) 1010–1024
for 2 h. A brown precipitate was formed on hot. The precipi-
tate was filtered off, washed with ethanol, and then diethylether
and finally air-dried. The yield was 2.393 g (78%). Fig. 3 rep-
resents the reaction of [Cu2(Lb)(NO3)2(H2O)2]·4H2O with 4,6-
diacetylresorcinol to afford [Cu2(La)]·3H2O.
Mass spectra were performed for H4La and H2Lb, ligands to
The molecular ion peaks were observed at 436 and 278 m/e con-
firming their formula weights (F.W. 436 and 278) for H4La and
H2Lb ligands, respectively. The schematic fragmentation of the
H2Lb ligand is depicted in Fig. 4.
The 1H NMR spectrum of H4La ligand in DMSO-d6, Table 4
3. Results and discussion
a
shows signals at δ (ppm) 1.34 (s, 6H, 2CH3 ); 2.61 (s, 6H,
b
c
d
2CH3 ); 2.88 (m, 8H, 4CH2 ); 3.53 (m, 8H, 4CH2 ); 6.23
It is worthnoting that the different preparative methods,
mentioned above, leaded in most cases to the formation of
metal complexes with identical molecular formula except the
case of Ni(II) complexes of H4La ligand. The obtained metal
complexes and their physicochemical properties are shown in
Table 1.
(s, 2H, Ar-He); 8.40 (s, 2H, Ar-Hf) and 17.41 (s, br, 4H, Ar-
OHg). The H NMR spectrum of H2Lb in DMSO-d6 showed
1
a
b
signals at δ (ppm) 1.36 (s, 3H, CH3 ); 1.88 (s, 3H, CH3 );
ꢀ
2.10 (m, 2H, CH2 ); 2.44 (m, 2H, CH2c ); 3.01 (m, 2H, CH2 );
d
ꢀ
3.35 (m, 2H, CH2d ); 6.25 (s, 1H, Ar-He); 8.24 (s, 1H, Ar-Hf);
11.17 (s, br, 4H, 2NH2) and 17.45 (s, br, 2H, Ar-OHd) [13]
(see Table 4). It is observed that the signals due to the protons
17.41–17.45 ppm (Ar-OHd) and 11.17 ppm (NH2) completely
disappeared on adding D2O while the other signals still persist
at the same positions. Fig. 5 depicts the 1H NMR spectra of the
H4La and H2Lb ligands in DMSO-d6.
3.1. Schiff base, H4La and H2Lb, ligands
The Schiff base ligands were investigated by elemental anal-
ysis, infrared, UV–vis, mass spectra and 1H NMR spectra.
The physicochemical properties are listed in Table 1. The IR
spectra of the ligands, Table 2 shows broad band in the range
(3499–3378 cm−1)duetothestretchingvibrationofthephenolic
groups. The broadness may be due to the intermolecular hydro-
gen bonding between the phenolic groups and the azomethine
groups. The band at 1264–1267 cm−1 is ascribed to the phenolic
ν(C O) stretching vibrations while the strong bands observed at
1584–1602 cm−1 is assigned to the stretching vibrations of the
azomethine group [13].
3.2. Schiff base complexes of H4La and H2Lb ligands
3.2.1. Infrared spectra
The infrared spectra of the complexes exhibit broad bands
around 3499–3378 cm−1 assigned for ν(NH), ν(OH) of the
phenolic-OH group and the ν(OH) of water or ethanol molecules
associated with the complex formation which are confirmed
by elemental analysis. In addition, it is expected that the IR
spectra of all binuclear complexes show a shift of the strong
band of ν(C N) towards lower frequencies within the range of
15–25 cm−1 compared to the free ligand H4La and H2Lb spec-
trum (1584 cm−1 for H4La and 1602 cm−1 for H2Lb), but could
not be resolved due to the deformation of the crystalline water
or ethanol [14]. Therefore, the two-azomethine nitrogen atoms
The electronic spectra of the H4La and H2Lb, ligands
(10−3 M) in DMF, Table 3 shows mainly three bands at 220–230,
323 and 370–375 nm due to (1La → A1) and (1Lb → A1) tran-
sitions of the phenyl ring and → * transition within the C N
group, in addition to a broad band at 410–412 nm due to the
n → * transition which is overlapping with the intermolecular
CT from the phenyl ring to the azomethine group [13].
1
1
Table 2
Infrared frequencies of the characteristic bands of the Schiff base ligands (H4La and H2Lb) and their transition metal complexes
Ligand/complex
ν(OH) and ν(NH2) ν(C N) and δ(H2O) ν(C O)
ν(CH3) δ(NH2) ν(NO3)
ν(M O) ν(M N)
ꢀ
νs
νs
νas
H4La
H2Lb
3383 s, br
3499 m, 3378 m
3400 s, br
1584 vs
1602 s
1634 s
1636 s
1605 s
1636 s
1638 vs
1636 vs, 1602 s
1264 vs
1267 vs
1384 s, 1360 s 2987 m –
1384 s, 1362 s 3003 m –
1384 s, 1362 s 2924 m –
1384 s, 1360 s 2924 m –
–
–
–
–
–
–
–
–
–
–
–
–
–
–
1533 m –
(1a) [Ni2(La)]·H2O
–
–
498 m
465 m
356 w
345 w
358 w
348 w
370 w
365 w
348 w
376 w
384 w
345 w
364 w
375 w
356 w
357 w
374 w
(1b) [Ni2(La)(H2O)4]·EtOH·4H2O
3400 s, br
(1c) [Ni2(H4La)(NO3)4]·2EtOH·6H2O 3422 s, br
1315 s 1008 s 1415 m 458 w
456 w
(2) [Cu2(La)]·3H2O
3400 s, br
3455 s, br
3496 s, br
–
–
–
(3) [Co2(H2La)(NO3)2]·2EtOH
(4) [Fe2(H2La)(NO3)4]·2H2O
(5) [Cr2(H2La)(NO3)4]·4EtOH
(6) [Zn2(H2La)(NO3)2]·3EtOH
(7) [Cd2(H2La)(NO3)2]·7H2O
(8) [Cu2(Lb)(NO3)2(H2O)2]·4H2O
(9) [Co2(Lb)(NO3)2(H2O)2]·2H2O
(10) [Fe2(H2Lb)(NO3)6]·4H2O
(11) [Cr2(Lb)(NO3)2(H2O)2]·4H2O
(12) [Zn2(Lb)(NO3)2(H2O)2]·4H2O
(13) [Cd2(Lb)(NO3)2(H2O)2]·3H2O
1384 s
2902 m –
1290 s 1008 s 1476 m 465 m
1315 s 1008 s 1410 m 460 m
1315 s 1008 s 1412 m 455 w
1290 s 1008 s 1472 m 465 m
1290 s 1008 s 1470 m 455 w
1384 s, 1366 s 2926 m –
1384 s, 1370 s 2924 m –
3412 s, br, 3350 m 1644 s, 1600 s
3422 s, br
3436 s, br
3428 s, br
3382 m
3382 m
3438 m
1641 vs, 1590 vs
1646 vs, 1590 vs
1586 s
1630 vs, 1590 s
1633 vs, 1591 vs
1640 vs, 1583 s
1604 vs, 1630 vs
1630 vs, 1602 s
1370 s
1381 s
1384 s
1385 s
1384 s
1384 s
1368 s
1368 s
2920 m –
2925 m –
2924 m 1530 s 1290 s 1008 s 1470 m 475 w
2924 m 1536 s 1290 s 1008 s 1475 m 471 w
2920 m 1536 s 1315 s 1008 s 1420 m 454 w
2924 m 1532 s 1315 s 1008 s 1412 m 434 w
2929 m 1534 s 1290 s 1008 s 1470 m 468 w
2925 m 1532 s 1290 s 1008 s 1472 m 475 w
3402 m
3498 m
s: strong, w: weak, m: medium, and br: broad, νs: a single degenerate state which is symmetrical about the principle axis, νas: antisymmetrical state with respect to
ꢀ
the three C2v axis, νs : a symmetrical state with respect to the three C2v axes.