384
J Chem Crystallogr (2012) 42:381–387
collection, reduction and corrections for absorption and
decomposition were achieved using X-AREA, X-RED
software [17]. The structure was solved by SHELXS-97
and refined with SHELXL-97 [18, 19]. The positions of the
H atoms bonded to C atoms were calculated (C–H distance
known thioureido. The t (C=S) stretching vibration can be
observed at 609–724 cm-1 range that are in close agree-
ment with previously studied of other thiourea derivatives
[22–25] (Fig. 2).
˚
0.86, 0.93 and 0.97 A), and refined using a riding model.
NMR Studies
The H atom displacement parameters were restricted to be
1.2Ueq of the parent atom. The details of the X-ray data
collection, structure solution and structure refinements are
given in Table 1. Selected bond distances and angles are
listed in Table 2. The molecular structure with the atom-
numbering scheme is shown in Fig. 1. Crystallographic
data (excluding structure factors) for the structures reported
in this paper has been deposited with the Cambridge
Crystallographic Data Centre as supplementary publication
number CCDC 7802651.
The experimental 1H-NMR data of the title compound
1
corresponds to those of similar compounds. The H NMR
signal for N1–H1 and N3–H3 shifted downfield to about
11.08 (s, 1H, NH) ppm and 10.45 (s, 1H, NH) ppm, while
that N–H appeared at about *8.00 and *4.00 ppm,
respectively. The resonance values of the phenyl protons
were confirmed 7.89 (d, 4H, ph-H), 7.55 (t, 2H, ph-H), 7.44
1
(t, 4H, ph-H). The H-NMR spectra of compound (C–H)
peaks is observed at 3.85 ppm (q, 4H, CH2), 2.17 ppm (m,
2H, CH2) due to the difference in the interaction of the
CSNH group with the aliphatic groups. The most
de-shielded 13C-NMR signals correspond to C=O and C=S
groups. The carbon atoms of thiocarbonyl show the highest
value such as 180.41 ppm, due to the lower excitation
energy n–p*. It is possible that very strong electron-with-
drawing neighbors reduce the nucleophilic character of the
C=S group. The 13C-NMR signal of the carbonyl groups in
compound appeared at 167.3 ppm due to the existence of
the intra-molecular hydrogen bond related to the carbonyl
oxygen atom (Figs. 3, 4).
Results and Discussion
FT-IR Studies
Infrared spectra of title compound reveal all the expected
frequency region of the t (N–H), t (C=O), t (C=S), t (CO–
N), t (CS–N). The band at N–H 3405 and 3218 cm-1
,
correspond to the stretching t (NH) vibrations of the
hydrogen bond NH groups in the bis-thiourea group. These
assignments were supported by the literature that N(2)–
H(2)ꢀꢀꢀ(O1) can be seen at above 3200 cm-1 and the N(3)–
H(3)ꢀꢀꢀ(O3, S1) can be found at above 3000 cm-1 have
been examined due to the existence of inter- and intra-
molecular hydrogen bonding [20]. The strong absorb t
C=O band in the IR spectra of the compound appears at
about 1670 cm-1, apparently decreasing in frequencies
comparing with the ordinary carbonyl absorption
(1700 cm-1). This is interpreted as being a result of its
conjugated resonance with the phenyl ring due to a delo-
calized pi-bond in it and the possible formation of intra-
molecular hydrogen bonding with N–H [21]. In addition,
the abnormal intensity ratio between t (C=O) and 1550 and
1514 cm-1 bands revealed that intromolecular hydrogen
bonding might exist in this compound as observed in the
X-ray analysis. The t (C–N) stretching frequencies have
been found at around 1334–1317 cm-1. In fact, these
vibrational frequencies have been assigned by comparison
with the assignments of acylthiourea derivatives at
1400–1000 cm-1. The bands at ca. 1300 cm-1, such as
1317 cm-1, are assigned to the vibration of –N–C=S as
Crystallographic Study
3,30-Dibenzoyl-1,10-(propan-1,3-diyl)-bisthiourea consists
of three parts. The part A [C1, C2, C3, C4, C5, C6, C7, C8,
O1, N1 and S1; planar with a maximum deviation of
˚
0.3422(8) A for the S1 atom] and another part B [C19,
C18, C17, C16, C15, C14, C13, C12, N4, O2 and S2;
˚
planar with a maximum deviation of 0.1289(12) A for the
N2 atom] are inclined at an angle of 10.07(3)°. However, it
is accepted that it is essentially planar with the only sig-
nificant deviation for the N1–C8–S1 and N4–C12–S2
moiety.
The conformation of the compound with respect to the
thiocarbonyl and carbonyl moieties is twisted, as reflected
by the torsion angles O2–C13–C14–C19 and C11–N3–
C12–S2, -165.0°, 2.2° and benzoyl moivety is almost
planar, as reflected by the torsion angles O2–C13–C14–
C15, C7–N1–C8–N2, C12–N4–C13–O2 17.4°, -178.0°,
-6.3° respectively. Symmetrical thiourea moiety is flexible
due to C8–N2–C9–C10 and C12–N3–C11–C10, 84.5°,
106.5°, respectively.
1
Further information may be obtained from: Cambridge Crystallo-
X-ray structure determinations revealed that thio-keto
graphic Data Center (CCDC), 12 Union Road, Cambridge CB21EZ,
UK, by quoting the depository number CCDC-780265. E-mail:
deposit@ccdc.cam. ac.uk
form is favoured over the thiol-imine form. This is evident
˚
from the observed C8=S1 bond distance of 1.672(4) A,
123