S.H.R. Sebastian et al. / Journal of Molecular Structure 1119 (2016) 188e199
193
4.2.4. CeCl modes
4.3. NMR spectra
The CeCl stretching vibrations give bands in the region
ꢀ
1
7
10e505 cm and for simple organic chlorine compounds the
The absolute isotropic chemical shielding was calculated by
B3LYP/GIAO model [53] and relative chemical shifts were then
ꢀ
1
CeCl absorptions are in the region 750e700 cm [36]. Renjith
et al. [46,47] reported the CeCl stretching modes in the region
estimated by using the corresponding TMS shielding:
calculated previously at the same theoretical level. Numerical
values of chemical shift calc(TMS) - calc together with
calculated values calc(TMS), are given in Tables 3 and 4. The
experimental values are: H NMR (500 MHz, DMSO)
NH), 9.14 (d, J ¼ 1.5 Hz,1H), 8.96 (d, J ¼ 1.3 Hz,1H), 8.92 (t, J ¼ 2.2 Hz,
scalc(TMS)
ꢀ
1
6
09e947 cm
and Resmi et al. [48] reported CeCl stretching
ꢀ
1
modes at 876, 644, 581 cm in Raman spectrum and at 877, 646,
88 cm theoretically. In the present case the CeCl stretching
mode is assigned at 764 cm in the IR spectrum and at 760 cm
theoretically with IR intensity 11.35, Raman activity 19.30 and a
PED of 44%.
d
calc
¼
s
s
ꢀ1
5
s
ꢀ1
ꢀ1
1
d: 11.27 (bs,1H,
13
1H), 8.31e8.26 (m,1H), 8.01e7.97 (m,1H), 7.67 (t, J ¼ 8.2 Hz,1H).
NMR (125 MHz, DMSO): : 161.78, 151.41, 148.1, 144.4, 143.5, 143.2,
39.5, 130.3, 126.9, 119.0 and 115.1.
Looking at the predicted and measured d
values for 13C NMR
C
d
1
4
.2.5. Pyrazine ring modes
The pyrazine CeH stretching modes are observed at 3090,
spectrum, the biggest difference can be observed for the carbox-
amide carbon (C10), followed by the chloro substituted pyrazine
ring carbon (C1). According to predicted values, C1 should have
ꢀ
1
ꢀ
1
3
071 cm in the IR spectrum and at 3088, 3071 cm theoretically
ꢀ
1
with PED 99% which are expected in the range 3000e3100 cm
[
(
1
49]. The pyrazine ring stretching modes are assigned at 1540, 1424
IR), 1540, 1425, 1302, 1198 (Raman) and in the range
545e1200 cm theoretically. Almost for all the modes the IR
higher d than C10 of carboxamide. In real world, it is the opposite
way. From the measured spectrum, we have assigned the carbox-
amide C10 to the peak of 161.78 ppm and chloro substituted C1 to
151.41 ppm. This assignment is based on the shifts of similar rele-
ꢀ1
intensity and Raman activities are high and the PED values are from
5
3% to 64%. Lukose et al. [27] reported pyrazine ring stretching
vant derivatives. For example the reported
boxamide carbon (measured in DMSO-d at ambient temperature)
are: N-phenylpyrazine-2-carboxamide ꢀ160.5 ppm (CDCl ) [54],
pyrazine-2-carboxamide e 165.0 ppm(DMSO-d ) [55].The typical
for chloro substituted carbon of pyrazine nucleus can be taken
d values for the car-
ꢀ
1
modes at 1545, 1153, 1059, 985 cm experimentally and at 1550,
6
ꢀ1
1518, 1193, 1152, 1045, 982 cm theoretically. The ring breathing
3
mode of the 1,4- substituted pyrazine ring is reported at 1120 (IR),
6
ꢀ1
ꢀ1
1124 (Raman), 1126 cm theoretically [50] and 1131 cm [51] and
d
1
13
for the title compound the ring breathing mode of the pyrazine ring
is assigned at 1092 cm
breathing mode has a IR intensity of 83.15 and PED value of 46%.
The CH deformation modes of the pyrazine ring are assigned at
from 2-chloropyrazine ꢀ148.6 ppm (DMSO-d
6
) [56]. The H and
C
ꢀ1
ꢀ1
(DFT) and 1088 cm
(IR). The ring
NMR signals were assigned to atoms based on expected shielding
and HeH coupling, together with comparison with published data
of relevant similar compounds.
ꢀ1
1242 (IR), 1242 (Raman), 1255, 1240 cm (DFT) with PEDs 49 and
4
ꢀ
1
5% (in-plane bending) and 944 (IR), 945 (Raman), 946, 897 cm
4.4. Nonlinear optical properties
(
[
DFT) (out-of-plane bending) with PEDs 80 and 50% as expected
36,40].
Nonlinear optics deals with the interaction of applied electro-
magnetic fields in various materials to generate new electromag-
netic fields, altered in wavenumber, phase, or other physical
properties [57]. Quantum chemical calculations have been shown
to be useful in the description of the relationship between the
electronic structure of systems and its NLO response [58]. The
computational approach allows the determination of molecular
NLO properties as an inexpensive way to design molecules by
analyzing their potential before synthesis and to determine high
order hyperpolarizability tensors of the molecules. The calculated
values of the dipole moment and polarizability are 6.8 Debye and
4
.2.6. Phenyl ring modes
For the title compound, the phenyl CeH stretching modes are
assigned at 3120, 3052 (IR), 3118, 3055 (Raman) and 3147, 3121,
3
are almost 100%. The phenyl ring stretching modes are expected in
the range 1615e1260 cm [36] and for the title compound, the
ꢀ1
078, 3052 cm (DFT) as expected [36]. The PEDs of these modes
ꢀ1
bands observed 1618, 1452, 1330 (IR), 1620, 1585, 1457, 1410
ꢀ
1
(
Raman) and in the range 1615e1327 cm theoretically. All the
phenyl ring stretching modes are IR and Raman active according to
the theoretical calculations and having PEDs in the range 44e80%.
The sixth phenyl ring stretching mode or ring breathing mode
appears as a weak band near 1000 cm
benzene and in the present case this mode is assigned at 973 cm
ꢀ
23
2
.61 ꢂ 10 e.s.u. The first order hyperpolarizability of the title
ꢀ
30
compound is calculated and is found to be 5.76 ꢂ 10 e.s.u which
is comparable with the reported values of similar derivatives
ꢀ1
in 1,3-di substituted
[27,50]. The calculated hyperpolarizability of the title compound is
ꢀ
1
4
4.31 times that of the standard NLO material urea
theoretically as expected [36,52]. For the title compound, the ring
breathing mode has low IR intensity (0.31) and Raman activity
(
8.12) according to the calculations and no band is observed
Table 3
ꢀ
1
Comparison of calculated and predicted shifts of 13C NMR spectrum of 5-chloro-N-
experimentally. The ring breathing mode is reported at 983 cm
theoretically by Raju et al. [41]. For the title compound, the in-plane
(3-nitrophenyl)pyrazine-2-carboxamide (sorted by decreasing d measured values).
and out-of-plane CeH modes of the phenyl ring are assigned at
Atom
Predicted
d
(ppm)
Measured
d
(ppm)
Difference d (ppm)
1
242, 1136 (IR), 1242, 1140, 1068, 1048 (Raman), 1240, 1135, 1064,
C10
C1
C18
C5
C2
C4
C13
C14
C12
C16
C15
157.60
163.33
151.35
147.80
143.60
143.45
140.26
129.88
123.19
121.28
116.87
161.78
151.41
148.04
144.40
143.46
143.18
139.48
130.24
126.87
118.98
115.05
ꢀ4.18
11.92
3.31
3.40
0.14
0.38
0.78
ꢀ0.36
ꢀ3.68
2.30
ꢀ
1
1050 cm (DFT) (in-plane deformation) and 889, 789 (IR), 886
ꢀ
1
(
Raman), 960, 930, 889, 788 cm (DFT) (out-of-plane deformation)
as expected [36]. The in-plane CH bending modes have PED values
of 39, 78, 58 and 44% and out-of-plane bending modes have these
values of 86, 72, 80 and 55%.
The RMS error of the observed IR and Raman modes are 3.55 and
.28 respectively for B3LYP/CC-pVDZ (5D, 7F) methods. The small
3
difference is due to the fact that experimental results belong to the
solid phase and theoretical calculations belong to gaseous phase.
1.83