500
V.V. Aswathy et al. / Journal of Molecular Structure 1141 (2017) 495e511
treating phenylaceticacid with thionylchloride. The compound was
prepared as a new product. The structure of title compound was
supported by spectral data. The 1H NMR, mass spectra and
elemental analysis results are in agreement with the proposed
structure.
values are at 1520 cmꢁ1 [53] and at 1536 cmꢁ1 [54]. In the present
casae, the CeN stretching modes are assigned at 1190, 1098 cmꢁ1
(IR), 1192 cmꢁ1 (Raman) and at 1222, 1188, 1100 cmꢁ1 theoretically
with PED contribution 34, 35, 40% as expected [52,55]. The CeOeC
stretching modes of the title compound are assigned at 1137 and
956 cmꢁ1 theoretically with PEDs 35 and 40%, with low IR in-
tensities and the reported the CeOeC stretching modes are 1191,
1187, 988 and 993 cmꢁ1 [53,56].
4.2. Antimicrobialactivities of the NBBPA
The newly synthesized was evaluated for their antibacterial
activity against S. aureus, E. faecalis as Gram-positive, E. coli, P.
aeruginosa as Gram-negative bacteria and their drug-resistant
clinical isolate. All the microbiological result were shown in
Table 1. According to antibacterial results NBBPA showed moderate
activity against the tested microorganisms. The compound indi-
The NeH modes are normally expected in the regions,
3400
40 cmꢁ1 (stretching mode), 1510e1500, 1400e1300,
740e730 cmꢁ1 (deformation modes) according to literature [50,51].
For NBBPA, the PED analysis gives the NH modes at 3450, 1524,
1262, 671 cmꢁ1 theoretically with 99% PED for stretching mode,
45e37% PEDs for deformation modes and the deformation modes
1524 and 1262 cmꢁ1 possess high Raman activity. Experimentally
bands are observed at 3455, 3262, 1527, 1260, 670 cmꢁ1 in the IR
spectrum and at 1526 cmꢁ1 in the Raman spectrum. The splitting in
the IR spectrum and red shift from the computed value of the NH
stretching vibration indicates the weakening of the NH bond as
reported in literature [57].
cated more effect against drug-resistant S. aureus (64
E. coli (128 g/ml) than standard drug Gentamycin (128
256 g/ml, respectively). Moreover, this molecule found to be more
mg/ml) and
m
mg/ml,
m
active against E. Faecalis than tested the other microorganisms.
4.3. Computational and spectral studies
Normally the CH2 vibrational modes appear in the ranges,
2950e2850 cmꢁ1 (stretching), 1470e900 cmꢁ1 (deformations
modes) [51,52,55] and the bands at 2936, 1422, 1165 cmꢁ1 (IR),
2975, 2936, 1423, 1166 cmꢁ1 (Raman) and 2969, 2934, 1425, 1285,
1167, 900 cmꢁ1 (DFT) are assigned as the stretching and deforma-
tion modes of the CH2 group of NBBPA.
The mono-, tri-, 1,2-substituted phenyl rings and benzoxazole
ring are designated as PhI, PhII, PhIII and PhIV in the following
discussions.
4.3.1. Geometrical parameters
The CeC bond lengths in the phenyl ring lie in the range
1.3978e1.4055 Å for PhI phenyl ring, 1.3830e1.4168 Å for PhII
phenyl ring and 1.3889e1.4145 Å for PhIII phenyl ring and for
benzene the CeC bond length is 1.3993 Å [45]. The CeN bond
lengths of the NBBPA, C3eN24 ¼ 1.4198 Å, C5eN10 ¼ 1.4103 Å and
The phenyl ring CH stretching modes are assigned at 3033 cmꢁ1
(IR), 3071, 3050, 3020 cmꢁ1 (Raman) for PhI and 3082, 3065 cmꢁ1
(IR) for PhIII rings. The DFT calculations give these modes in the
ranges, 3068e3036, 3118e3058 and 3094e3052 cmꢁ1 for PhI, PhII
and PhIII rings, respectively as expected [51]. The phenyl ring
stretching modes are assigned at 1470, 1320 cmꢁ1 (IR), 1588 cmꢁ1
(Raman), 1585e1317 cmꢁ1 (DFT) for PhI, 1577, 1541, 1391 cmꢁ1 (IR),
1543, 1310 cmꢁ1 (Raman), 1579e1309 cmꢁ1 (DFT) for PhII and
1447 cmꢁ1 (IR), 1605, 1567 cmꢁ1 (Raman), 1597e1275 cmꢁ1 (DFT)
for PhIII rings which are in agreement with literature [51]. All the
phenyl ring stretching modes possess a PED contribution equal or
greater than 40%. In the case of tri-substituted phenyl rings with
mixed substituents, the ring breathing mode is expected between
600 and 750 cmꢁ1 [51,58] and in the present case the mode at
749 cmꢁ1 (DFT) is assigned as the ring breathing mode of the tri-
substituted benzene and the reported values are at 764 cmꢁ1 (IR),
766 cmꢁ1 (Raman) and at769 cmꢁ1 (DFT) [59]. The ring breathing
mode at 749 cmꢁ1 has a PED of 50% with a high IR intensity and low
Raman activity. For the NBBPA compound, the DFT calculations give
the ring breathing mode of ortho substituted phenyl ring at
1111 cmꢁ1 with a PED of 46% which is in agreement with literature
[58] and the reported value is at 1087 cmꢁ1 [60]. The band at
978 cmꢁ1 with a PED of 40% is assigned as the ring breathing mode
of the mono substituted phenyl ring of the NBBPA compound as
expected [51,58]. Both the above two ring breathing modes have
low IR intensities and experimentally no bands are seen in the IR
spectrum. The in-plane CH bending modes of the phenyl rings are
observed at 1282, 1070, 1017 cmꢁ1 (IR), 1283, 1018 cmꢁ1 (Raman)
for PhI, 1129 cmꢁ1 (IR), 1128 cmꢁ1 (Raman) for PhII and at
1044 cmꢁ1 (IR), 1246, 1045 cmꢁ1 (Raman) for PhIII. The corre-
sponding theoretical CH deformation modes of the phenyl rings are
in the ranges,1281e1013 cmꢁ1 for PhI,1235e1126 cmꢁ1 for PhII and
1243e1043 cmꢁ1 for PhIII [51]. The out-of-plane CH deformation
modes of the phenyl rings are assigned at 968, 910, 725 cmꢁ1 in the
IR spectrum, 971, 726 cmꢁ1in the Raman spectrum for PhI, 951, 851,
824 cmꢁ1 in the IR spectrum, 846 cmꢁ1 in the Raman spectrum for
PhII and no bands are seen experimentally for PhIII. The PED
analysis gives these modes in the ranges, 969e726 cmꢁ1 for PhI,
951e826 cmꢁ1 for PhII and 960e741 cmꢁ1 for PhIII rings,
C
26eN24 ¼ 1.3708 Å are less than the normal CeN bond (1.48 Å)
shows some resonance in this section of the molecule [46]. The
bond lengths, C6eO22 ¼ 1.3988 Å, C11eO22 ¼ 1.4273 Å and C11
]
N10 ¼ 1.3080 Å are in agreement with that of similar derivative [47].
The bond length C26]O27 ¼ 1.2509 Å is in agreement with the
reported values [48]. In the present case, the CeBr bond length is
1.9469 Å which is in agreement with literature [49]. At C13 position,
the bond angles are,C12eC13eC15 ¼ 120.7ꢀ, C12eC13eBr23 ¼ 123.7ꢀ
and C15eC13eBr23 ¼ 115.6ꢀ and this asymmetry shows the repul-
sion between bromine and benzoxazle ring. Similarly at C12 and C11
positions, the angles, C13eC12eC14 ¼ 117.4ꢀ, C13eC12eC11 ¼ 125.2ꢀ,
C
N
14eC12eC11
¼
117.4ꢀ
and
N
10eC11eC12
¼
131.5ꢀ,
10eC11eO22 ¼ 113.0ꢀ, C12eC11eO22 ¼ 115.5ꢀ which shows the
interaction between O22 and H17 atoms. The interaction between
NH and neighbouring units is revealed by the bond angles around
C26 and N24 which are respectively,
C
39eC26eN24 ¼ 116.4ꢀ,
C
39eC26eO27
¼
119.5ꢀ,
N24eC26eO27
¼
124.1ꢀ
and
C26eN24eC3 ¼ 129.3ꢀ, C26eN24eH25 ¼115.6ꢀ, C3eN24eH25 ¼115.1ꢀ.
4.3.2. IR and Raman spectra
The observed IR, Raman bands are vibratioal assignments
together with calculated scaled wavenumbers are given in Table 3.
The C]O stretching vibration is observed in the range
1800e1550 cmꢁ1 [50], and for NBBPA the band observed at
1670 cmꢁ1 experimentally is assigned as the C]O stretching mode
which agrees with the computed value at 1673 cmꢁ1 with a PED of
73% and high IR intensity of 398.27 and Raman activity of 59.03. In
substituted benzenes, stretching vibrations of CeBr is expected in
the range 635 85 cmꢁ1 [51] and for the NBBPA, this vibration is
assigned at 687 cmꢁ1 theoretically with PED 32% and this is in
agreement with the reported values [49]. According to literature
[52] the C]N stretching modes are expected in the region
1650e1500 cmꢁ1 and for the NBBPA, this mode is assigned at
1511 cmꢁ1 theoretically with a PED of 39% while the reported