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A. A. Hassan et al. / Tetrahedron Letters 55 (2014) 2385–2388
NC
H2N
CN
NC
NC
CN
CN
H
N
H
N
EtOAc
Ph
N
N
N
H
R
N
R
+
S
S
2
1a-c
3a-c
1,3
R
Yield (%)
76
a
b
c
CH2CH3
CH2-CH=CH2 71
C6H5 67
Scheme 1. Reaction between N-substituted phenylhydrazinocarbothioamides 1a–c
and TCNE (2).
range 10.34–10.18 ppm. Also, the IR spectra of 3a–c clearly showed
CAS stretching at 1292–1286 cmÀ1, and C@N and conjugated cyclic
C@N absorptions at 1495–1486 cmÀ1 27
.
In fact, the 1H NMR spectral studies were not very informative
due to the absence of a proton on the core heterocycle. However,
the 1H NMR spectrum of 3a clearly showed the presence of triplet
and quartet signals centered at 1.28 and 3.81 ppm, respectively,
with the integral ratio 3:2 due to the CH3CH2 group, besides the
aromatic protons.
In 3b, the substituent (allyl group) gave rise to three multiplet
signals at 4.62–4.63 (allylACH2N), 5.23–5.28 (allylACH2@), and at
5.87–5.90 (allylACH@). The presence of the allyl group was evident
from the 13C DEPT-NMR spectrum which exhibited positive signals
at 133.5 ppm (allylACH@) and negative signals at 49.7, 121.4 ppm
for the allylACH2N and allylACH2@, respectively.28
Figure 2. X-ray crystal structure of 3b (ORTEP, displacement parameters are drawn
at the 50% probability level, minor disordered parts are omitted for clarity). The
crystallographic numbering does not reflect the systematic IUPAC numbering.
tra of 3a–c, dicyanovinyl-carbons C1 and C2 resonated at 171.4–
171.2 and 60.5–60.1 ppm, respectively, and were in accord with
the observed trends in the d values for C-atoms in push–pull
alkenes.31,32
The structures of the newly synthesized triazoliumthiolate
derivatives 3a–c were also confirmed by their EI mass spectra.
The mass spectra of 3a–c showed molecular ion peaks at m/z
296, 308, and 344 in conformity with their molecular formulae.
The molecular ion peaks were fairly intense suggesting the pres-
ence of a stable triazoliumthiolate ring system in these cyclized
products.
Moreover, the structures of 3a,b were confirmed unambigu-
ously by single crystal X-ray structure analyses (Figs. 1 and 2 and
Tables S1–S7, S8–S14 in the Supplementary data; note that the
crystallographic numbering does not correspond to systematic IU-
PAC numbering rules).
In contrast to the 1H NMR spectra, the 13C NMR spectra of 3a–c
were crucial for the characterization of the mesoionic ring due to
the large differences in the electronic densities between the two
regions of the triazolium ring.29,30 This difference of electronic den-
sity was apparent through positive and negative shielding of the
carbons of the mesoionic triazolium rings in 3a–c. The C-3 and
C-5 signals were centered around 169.8–169.7 and 151.7–
152.1 ppm. These results are consistent with the assignment of
chemical shifts for triazolium thiolates 3a–c. In the 13C NMR spec-
Figure 1 shows the structure of 5-(1-amino-2,2-dicyanovinyl)-
4-ethyl-1-phenyl-4H-triazol-1-ium-3-thiolate (3a). The C(1)–S(1)
bond length of 1.700(2) Å, is intermediate between the double
bond length of 1.645 Å33 and the single bond length of 1.737 Å.26
The bond lengths C(1)–N(2) 1.333 (3), C(1)–N(5) 1.403 (2), and
C(4)–N(5) 1.338 (3) Å suggest that these bonds have some double
bond character as they are comparable to the CAN
r-bond length
of 1.47 Å. The N(2)–N(3) bond length of 1.374 (2) Å is slightly
shorter than the single-bond value of 1.401 Å. The fact that the
N(2)–N(3) bond length is closer to the single bond length supports
the presence of a mesoionic ring system.34 The S(1)–C(1)–N(2)–
N(3), C(1)–N(2)–N(3)–C(4), C(31)–N(3)–C(4)–C(5), C(41)–C(4)–
N(5)–C(1), and C(1)–N(5)–C(51)–C(52) torsion angles are
À177.42 (15)°, À0.7 (2)°, 177.11 (18)°, 174.90 (18)°, and 83.4(2)°,
respectively.
In
4-allyl-3-(1-amino-2,2-dicyano-vinyl-1-phenyl-4H-1,2,4-
triazol-1-ium-3-thiolate (3b) (Fig. 2), the S(1)–C(1) and N(2)–
N(3) bond lengths are 1.6933 Å (10) and 1.3804 Å (2), respectively
(note that the crystallographic numbering does not correspond to
systematic IUPAC numbering rules), and thus are slightly shorter
than the CAS and NAN
r-bonds. The sum of the angles N(2)–
C(1)–N(5), N(2)–C(1)–S(1), and N(5)–C(1)–S(1) is close to 360° as
are the sums of the angles around N(3), C(4), N(5), C(41), and
C(33) demonstrating planarity around C(1), N(3), C(4), N(5),
C(41), and C(33). However, the sum of the angles N(5)–C(51)–
C(52), N(5)–C(51)–H(51A), and N(5)–C(51)–H(51B) is 329.69°; this
Figure 1. X-ray crystal structure of 3a (ORTEP, displacement parameters are drawn
at the 50% probability level). The crystallographic numbering does not reflect the
systematic IUPAC numbering.