F. Aydın et al. / Journal of Molecular Structure xxx (xxxx) xxx
3
2.4. Computational studies
organic solvent (THF, CH3CN and DMSO) in the range of
300e600 nm (Fig. 2), where. two bands were observed. The high-
density bands at 340, 344 and 348 nm for THF, CH3CN and DMSO
The molecular structure of title compound was optimized using
DFT in the ground state by B3LYP [29] method with the 6-311G (d,p)
[30] basis sets included in Gaussian 09 program [31]. Molecular
structure of the title compound optimized by 6-311G (d,p) basis set
displayed frontier molecular orbitals, and electrostatic potential
were simulated. In addition, thermodynamic parameters (i.e., heat
capacity, enthalpy and entropy values) for the title molecule were
calculated.
solvents, respectively, are due to the transition
p /p * of the
nitrogen-carbon-sulfur (-N-C]S) group on dithiocarbamate moi-
ety conjugated with benzoyl. It also appears as a shoulder on the
transition n/p* localized on sulfur connected with undecyl moi-
ety observed at 408, 411 and 415 nm. Optical band gaps (Eg, eV)
value from the electronic absorption spectra of the title compound
in different solvents were calculated for these transitions and the
2
optical energy were determined from the (
energy (h
ah
y)
versus photon
is the ab-
y
) graph using Tauc equation [36], where
a
3. Results and discussion
sorption coefficient (Fig. 3). From the value of Tauc equation, for the
title compound in THF, CH3CN and DMSO, the band gaps corre-
3.1. FT-IR and NMR spectral studies
sponding to n-
respectively.
p* transitions were calculated 3.59, 3.55 and 3.51 eV,
The IR spectra of the title compound showed significant ab-
sorption of the carbonyl group at 1697 cmꢀ1 y (C]O) and the amide
DFT (B3LYP) calculations and energy levels of the HOMO-1,
HOMO and LUMO, LUMOþ1 orbitals was used for determine the
low-lying excited states of compound [37,38]. Energy difference
HOMO-1, HOMO and LUMO, LUMOþ1 were calculated as 6.5769,
6.2841 and 2.2201, 1.1649 eV, respectively (Fig. 4). Large HOMO-
LUMO gap energy value of 4.064 eV indicates that the title com-
pound is in steady state. Fig. 4 also showed that the electronic
density on the HOMO of the title compound was localized primarily
on dithiocarbamate skeleton and carbonyl group, whereas the
LUMO orbital of it was localized on dithiocarbamate skeleton along
the phenyl ring and its amide group due to intramolecular charge
transfer. Energy level of LUMO, which is related to the electron
affinity, implies that the title compound is susceptible to nucleo-
philic attacks [39].
group at 3313 cmꢀ1
(
y
NeH), respectively. Vibration bands with the
wave numbers of 3055 and 3050 cmꢀ1
CeH, AreH) and 1553 and
1502 cmꢀ1
(y
(y C]C) were observed as the result of the vibration of
phenyl ring. The frequencies of 2955, 2918 and 2850 cmꢀ1 and
1250 cmꢀ1 were assigned to the stretching vibrations (CeH) and
(CeC) in undecyl moiety, respectively [32]. The dithiocarbamate
compounds exhibit a characteristic band in the range (1580-1450)
cm-1 assignable to the y
(CeN) [33]. Additional bands at 1431 cmꢀ1
(y
ꢀCOeN) and 1207 cmꢀ1 (NꢀCS) were observed. The band of
747 cmꢀ1
(y C]S) was attributed to thiocarbonyl group (C]S)
symmetric stretching vibration [34,35] (Fig. S1).
1H NMR and 13C NMR spectra for title compound are shown in
Figs. S2 and S3 (Supplemental Materials). 1H NMR spectra exhibits
all expected resonances for (ꢀCeOeNH) and (ꢀCeSeCH2ꢀ)
groups at 12.65 ppm and 3.20 ppm, respectively. The 1H NMR signal
for NeH proton of amide or thioureide moiety due to the resonance
with the carbonyl (C]O) and thiocarbonyl (C]S) groups shifted
downfield to about 12.65 ppm, while that NeH appeared at about
~8.00 ppm. Three signals were appeared at 7.53 (d, 2H), 7.66 (m,1H)
and 7.94 (d, 2H) for phenyl protons. In addition, the title compound
has an undecyl moiety and aliphatic protons were assigned at 1.68
(2H, m), 1.40 (2H, m) 1.25 (16 H, m) and 0.86 (3H, t) ppm.
In the 13C NMR spectra of the title compound, aromatic proton
signals were appeared in the region 133.0, 131.8, 128.7 and
128.4 ppm for phenyl moiety. Functional groups in the structure of
aroyl dithiocarbamate derivative were confirmed with at 204.6
d
(C]S), 165.3
d
(C]O), 35.9
d
(SeCH2ꢀ), 13.9 ppm
d
(ꢀCH3) and
(ꢀCH2)nꢀ) within range of
d (31.3e22.1) ppm for title compound,
respectively (Scheme 2).
3.2. Electronic spectral studies and HOMO-LUMO analysis
High chemical reactivity, more polarizability and the transfer of
charge within a molecule are associated with the frontier orbital
gap (i.e., energy gap between HOMO and LUMO). The UVeVis
spectra of the title compound were recorded in different polarity
Fig. 2. UVevis spectra of title compound in THF, CH3CN and DMSO solvents.
Scheme 2. 1H and 13C NMR chemical shifts of the title compound in DMSO‑d6.
Please cite this article as: F. Aydın et al., N-Benzoyl-S-(undecyl)-dithiocarbamate: Synthesis, characterization, X-ray single crystal structure,