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R. Swisłocka et al. / Spectrochimica Acta Part A 100 (2013) 31–40
32
salts obtained were found to be anhydrous as indicated by the lack
of bonds characteristic of water of crystallization in the IR spec-
tra.
correlation between experimental and theoretical IR spectra was
noted. The correlation coefficients for IR spectra are: 0.9975 (acid),
0.9973 (Li), 0.9973 (Na) and 0.9979 (K). Raman and IR experimental
and calculated spectra of vanillic acid are presented in Fig. 1.
Characteristic vibration bands of the carboxylic group are
present in the spectra of vanillic acid, and are not observed
in the spectra of salt. There are very intense, broad stretching
The IR spectra were recorded with an Equinox 55, BRUKER FT-
IR spectrometer within the range of 400–4000 cm−1. Samples in
the solid state were measured in KBr matrix pellets which were
obtained with hydraulic press under 739 MPa pressure. Raman
spectra of solid samples in capillary tubes were recorded in the
range of 100–4000 cm−1 with a FT-Raman accessory of the Perkin-
−1
bands: ꢀ(C O): 1682 cm
(R); ꢀ(OH) in the range 2957–2571 cm
(IR), 1780 cm−1 (IRcalc.), 1642 cm−1
−1
(IR) and ꢀ C (OH):
Elmer system 2000. The resolution of spectrometer was 1 cm−1
.
1298 cm−1 (IR), 1357 cm−1 (IRcalc.), 1301 cm−1 (R). Deformation in
plane vibration bands ˇ(C O): 766 cm−1 (IR), 766 cm−1 (R) and
deformation out of plane vibration bands ꢁ(C O): 637 cm−1 (IR),
777 cm−1 (IRcalc.), 638 cm−1 (R). Moreover, in the spectra of acid
the bands of lower intensity are present, origi−n1ating from defor-
The NMR spectra of DMSO saturated solution were recorded with
the NMR AC 200 F, Bruker unit at room temperature. TMS was used
as an internal reference. The UV spectra in water solution were
recorded on a DR 5000 HACH-LANGE spectrophotometer between
190 and 400 nm. The compounds were studied in aqueous solutions
with concentrations 10−4 mol/dm3.
To calculate optimized geometrical structures the density func-
tional theory (DFT) hybrid method B3LYP with nonlocal correlation
provided by Lee–Yang–Parr expression was used. The 6-311++G**
basis set was used as the standard basis set available for all atoms
in studied molecules. The method has been successfully applied
to calculate geometrical parameters, IR spectra, atomic charges for
systems similar to these studied in this paper All theoretical calcu-
lations were performed using the GAUSSIAN 09 (rev. 11.2) package
of programs [5] running on a PC.
Five species of bacteria: Escherichia coli (PCM 2268), B. subtilis
(PCM 2021), P. vulgaris (PCM 2269), P. aeruginosa (PCM 2270), S.
aureus (PCM 2267) and one species of yeasts Candida albicans (PCM
2566) were used for antimicrobial tests. Bacterial cultures where
purchased from Polish Collection of Microorganisms (PCM). Micro-
biological analysis was carried out according to the literature [6,7].
Solutions of tested compounds were prepared by dissolving 0.2 g
of each of them in 9.8 ml of deionized water. The concentration of
compounds in the culture broth was 0.1%. 4.75 ml of broth inocu-
lated with bacteria was used and then 0.25 ml solution of tested
compound was added. The studied bacteria were inoculated on
enriched broth medium and yeast on Sabouraud broth medium and
stored in 35◦C (for yeast in 25 ◦C) for 24 h. The growth of tested cells
was standardized turbidimetrically by measuring optical density at
600 nm with Hach Lange UV/vis spectrophotometer DR 5000. The
microbiological tests for studied compounds were carried out in
deionized water medium. The samples were incubated in 35 ◦C for
bacteria and 25 ◦C for yeast. The number of colonies was directly
proportional to optical density, which was estimated similarly after
24 and 48 h incubation. Statistical calculations were performed
using Statistica 9.1 program [8].
mation vibrations ˇ(OH) located at 1205 cm
(IR), 1259 cm−1
(IRcalc.), 1206 cm−1 (R) and ꢁ(OH) 918 and 588 cm−1 (IR), 580 cm−1
(IRcalc.), 919 and 585 cm−1 (R) have also been observed. In the spec-
trum of the acid are also present bands from the aromatic ring
and functional groups of the ring (hydroxyl OHar and methoxy
OCH3 groups), which are also present in the spectra of salt.
Replacement of the carboxylic group hydrogen with a metal ion
brought about characteristic changes in the IR and Raman spectra
of the metal vanillates in comparison with the spectra of vanil-
lic acid. One can observe appearance of bands of the symmetric
and asymmetric vibrations of the carboxylate anion: ꢀas(COO−)
in the range: 1558–1549 cm−1 (IR), 1554–1535 cm−1 (IRcalc.),
1566–1546 cm−1 (R), ꢀs(COO−) in the range: 1395–1385 cm−1 (IR),
1426–1394 cm−1 (IRcalc.), 1396–1371 cm−1 (R); ˇs(COO−) in the
range: 961–957 cm−1 (IR), 835–810 cm−1 (IRcalc.), 968–953 cm−1
(R), ˇas(COO−) in the range: 488–461 cm−1 (IR), 490–461 cm−1
(R) and ꢁs(COO−) in the range: 781–777 cm−1 (IR), in the range
802–786 cm−1 (IRcalc.), in the range 785–778 cm−1 (R).
In the spectra of acid and salts there are present bands o
from the hydroxyl group attached to the aromatic ring: ꢀ(OH)ar
3485 cm−1 (IR), 3764 cm−1 (IRcalc.) in the spectrum of vanillic
acidand3455–3443 cm−1 (IR), 3768–3749 cm−1 (IRcalc.), ꢀC (OH)ar
1225–1219 cm−1 (IR), 1301–1270 cm−1 (IRcalc.), 1226–1217 cm−1
(R); ˇ(OH)ar 1253–1236 cm−1 (IRcalc.); ꢁ(OH)ar 928 cm−1 (IR),
932–929 and 645–640 cm−1 (R) in the spectra of salts.
Stretching vibrations ꢀas(CH3) give the bands in the ranges:
2948–2938 cm−1 (IR), 3147–3133 and 3088–3072 cm−1 (IRcalc.),
2944–2939 cm−1 (R) and ꢀs(CH3) in the ranges: 2841–2835 cm−1
(IR), 3023–3012 cm−1 (IRcalc.), 2841–2836 cm−1 (R).
The ıas(CH3) (in plane bending) bands that occur in the
ranges: 1474–1464, 1454–1447 and 1030–1026 cm−1 (IR),
1506–1494, 1492–1481 cm−1 (IRcalc.), 1474–1466, 1454–1448 and
1033–1026 cm−1 (R) and ıs(CH3) in the range: 1379–1354 cm−1
(IR), 1484–1478 cm−1 (IRcalc.), 1381–1351 cm−1 (R), as well as
rocking vibration bands ꢂ(CH3) in the range: 1222–1216 and
1171–1168 cm−1 (Rcalc.). The bands of the ꢀO (CH3) vibrations
are located in the range 1186–1182 cm−1 (IR), 1060–1043 cm−1
(IRcalc.), 1184–1178 and 1074–1064 cm−1 (R).
3. Results and discussion
3.1. Vibrational spectra
The vibrational spectra of vanillic acid and the synthesized
lithium, sodium, potassium, rubidium and caesium vanillates were
recorded and assigned. The observed Raman and IR bands together
with their relative intensities and band assignments of studied
metal salts are presented in Table 1 (vanillic acid) and 2 (vanil-
lates), respectively. The symbol “ꢀ” denotes stretching vibrations,
“ˇ”: in-plane bending modes, “ꢁ”: out-of-plane bending modes;
“ϕ(CCC)”: the aromatic ring out-of-plane bending modes, “˛(CCC)”:
the aromatic ring in-plane bending modes, “ı(CH3)”: the methyl
deformations. The bands are numbered along with the notation
used by Varsányi [9]. Theoretical calculations by B3LYP method
at 6-311++G** level were used to obtain values of wavenumbers
and intensities of IR and Raman spectra (Tables 1 and 2 ). Good
3.2. NMR spectra
lithium, sodium and potassium vanillates were obtained (Table 3).
Geometrical structures of studied compounds were optimized by
B3LYP/6-311++G** method. The atom positions were numbered as
in Fig. 2. The signals from protons no. 3 and 4 are shifted down-
field in comparison to the appropriate signals in the spectrum of
ligand. In the 1H NMR spectra of vanillates no regularity can be
observed in the chemical shifts of hydrogen along the series of
alkali metal vanillates. Chemical shift values of signals traced for
vanillic acid werer compared with those traced for m-anisic acid