Ç
S. Ide et al. / Journal of Molecular Structure 562 (2001) 1±9
6
vibration bands occur between 380 and 325 cm21
[5]. In our study, these bands could not be observed,
because of the inadequacy of the spectrophotometer
as it can work at 4000±400 cm21 range.
Table 1
The fundamental vibrational wavenumber (cm21
) of Ni(II)
complexes
Ni(C13H9NSBr)2 Ni(C14H12NS)2 Ni(C14H12NSO)2 Assignments
The bands due to n(Ni±N) stretching vibration are
usually found between 580 and 430 cm21 [6]. In the
metal complexes of bromo, methyl and methoxy
derivatives, these bands occurred at 494, 499 and
510 cm21, respectively.
3059
2926
2852
3055
2920
2850
3059
2926
2850
n(C±H)
n(C±H)
(CHyN)
n(CyN)
nring
1585
1574
1483
1458
1439
±
1599
1574
1510
1456
1400
1371
1603
1550
1508
1458
1425
1304
1
The H NMR spectra of these compounds were
nring
nring
recorded in CDCl3 at 400 MHz using two-dimen-
sional (2-D) NMR techniques and all proton signals
were completely assigned (Table 2).
nring
d(C±H)
(±CH3)
n(C±O)
n(C±N)
(Ar±N)
d(CCH)
dring
Although ±CHyN protons usually absorb in the 8±
9 d range, in all three of our complexes the proton
resonance of the ±CHyN± group was observed
between the 7 and 8 d range, as shown in Table 2.
These high-®eld signals are explained in terms of
complex formation through the ±CHyN± bond. H6
(H9) proton signals d values are increasing with
respect to the substituents order of ±OCH3 , ±
CH3 , ±Br. This increasing is in accordance with
the electron-donating effect in the ±OCH3 . ±
CH3 . ±Br order.
±
±
1259
1280
1281
1286
1174
1070
1011
1173
1065
1032
1171
1065
1028
n(CC)
d(CH)
d(CCH)
d(CCH)
n(C±S)
(Ar±S)
n(Ni±N)
808
748
592
802
742
590
825
750
590
494
499
510
Single crystal X-ray diffraction method could not be
used, because of poor single crystal quality, to obtain
certain crystal and molecular structures. The unit cell
of nickel(II) complexes of N-(4-bromobenzylidene)-2-
mercaptoaniline, N-(4-methylbenzylidene)-2-mercap-
toaniline and N-(4-methoxybenzylidene)-2-mercaptoa-
niline were compared with the spectra of 2-(3,4,5-
trimethoxyphenyl)-benzothiazole [4].
parameters
mercaptoanilinato(nickel(II) (I) were determined by
of
bis(N-(4-methoxybenzylidene)-2-
using the xrd calculator program [7] as follows:
Ê
a 13.665(5);
b 12.983(5);
c 15.150(9) A;
Ê 3
The important vibrational bands of these complexes
were recorded in Table 1. In the infrared spectra of
these complexes, the bands observed at about
2850 cm21 were assigned to the C±H (CHyN)
stretching vibrations. It was shown that the formation
of the benzothiazole ring did not occur. The band of
S±H stretching vibration was not observed. There-
fore, it is believed that the {S,N}-chelated complexes
of Schiff bases were formed. In the infrared spectra of
2-(3,4,5-trimethoxyphenyl)-benzothiazole [4], the
band due to n(C±S) stretching vibration disappeared
in the IR spectra of complexes. Because of complex
formation, the band of CyN stretching vibration
shifts to a lower wavenumber in all metal complexes.
This shift suggests that coordination has taken place
through the nitrogen of the azomethine group.
According to the literature, (Ni±S) stretching
b 112.58(5)8; and V 2481.7(2) A . The probable
crystal systems for bis[N-(4-methylbenzylidene)-2-
mercaptoanilinato] nickel(II) (II) and bis[N-(4-bromo-
benzylidene)-2-mercaptoanilinato] nickel(II) (III)
are also monoclinic because the interplanar distances
of bis(N-(4-chlorobenzylidene)-2-mercaptoanilinato]
nickel(II) crystals [8] are in agreement with those of II
and III. These consistences were obtained using Table 3
and unit cell knowledge of bis(N-(4-chlorobenzyli-
dene)-2-mercaptoanilinato] nickel(II) [8].
alchemy 2000 packet program was used to mini-
mize the molecular energies [9]. The lowest energy
values have been determined as 88.973(7), 148.961(6)
and 90.595(7) kcal/mol for I, II and III, respectively.
The big energy value for II shows that the structures
of I and III are more stable than the structure of II.
The effect of this unstable form of II can also be seen