–1
Spectroscopic data. IR (ATR; ν , cm ): 3228, 2927, 2872, 2235, 1597, 1493, 1453, 1338, 1163, 1091, 1068, 968,
max
1
957, 945, 913, 857, 844, 818, 789, 745, 732, 703, 677, 582, 549. H NMR (300 MHz, CDCl ): δ 2.43 (s, 3H, CH ), 5.02-5.08
3
3
2 2
(m, 2H, NH and H-1), 6.00 (d, 1H, J = 1.0 Hz, H-9a), 6.07 (d, 1H, J = 1.0 Hz, H-9b), 7.07-7.15 (m, 1H, H-5), 7.26-
HH
HH
3 13
7.30 (m, 4H, H-3, H-4, H-6 and H-7), 7.30-7.33 (m, 2H, H-3′ and H-5′), 7.69-7.73 (d, 2H, J = 9.0 Hz, H-2′ and H-6′). C
HH
NMR (75 MHz, CDCl ): δ 21.6 (C-7′), 59.8 (C-1), 116.5 (C-8), 123.3 (CN), 126.8 (C-2′ and C-6′), 127.3 (C-4 and C-6),
3
129.1 (C-5), 129.3 (C-3′ and C-5′), 129.8 (C-3 and C-7), 131.8 (C-9), 136.1 (C-2), 136.7 (C-4′), 144.1 (C-1′). HR-ESI-MS
–
(anionic mode): Anal. Calcd. for C H N O S : 311.0854, Found: 311.0863.
17 15
2
2
X-ray crystallography. The X-ray diffraction data were collected on a Bruker APEX II-DUO diffractometer
equipped with a CCD area detector and a graphite monochromator with CuK radiation (λ = 0.54178 Å) at 273 K. APEX II
α
and SAINT software packages [5] were used for the unit cell determination, data collection and integration. The structure was
2
solved using direct methods and refined successfully using full-matrix least-squares on F with SHELXL-2014 [6] with
anisotropic atomic displacement parameters for non-hydrogen atoms. All hydrogen atoms were stereochemically positioned and
refined with the riding model. Absorption correction (GAUSSIAN) was applied for the compound using the SORTAV program [7].
The crystallographic data are as follows: chemical formula, M = 312.38, dimensions 0.344×0.262×0.262 mm,
3
monoclinic, P2 /n, а = 10.7646(3) Å, b = 11.1715(3) Å, с = 14.7311(4) Å, β = 109.7(1)°, V = 1667.5(1) Å , Z = 4,
1
3
–1
d
= 1.244 g/cm , μ = 1.790 mm , T /T = 0.578/0.651. The resulting values are: S = 1.072, R1 = 0.0681 for all 3423
min max
cal
reflections and R1 = 0.0569 for 2808 reflections with I > 2σ(I) and 212 refined parameters. The complete data of the X-ray
crystallographic analysis containing atomic coordinates, bond lengths, and bond angles have been deposited at the Cambridge
Crystallographic Data Centre (CCDC No. 1531585).
RESULTS AND DISCUSSION
–1 –1
Spectroscopic studies. The characteristic sulfonamide bands were observed at 3228 cm (νNH), 1338 cm , and
–1
1163 cm (νSO asymmetric and symmetric, respectively) in the IR spectrum of compound 3. The νCN band at 2235 cm
–1
2
–1 –1
was shifted to higher wavenumbers with respect to precursors 1 and 2 (2229 cm and 2228 cm , respectively). The expected
–1 1
disubstituted CH band was observed at 857 cm . In the H NMR spectrum of compound 3, the region between δ 7.07 and
2
7.73 showed four multiplets integrating an area of nine hydrogen atoms due to the aromatic rings. The most important
diagnostic signals were the singlet at δ 2.43 due to the methyl group and two coupled doublets (J = 1 Hz) of the methylidene
13
group at δ 6.00 and 6.07. The H1 and NH signals superimposed at ca. δ 5.05. The C NMR spectrum of compound 3 showed
all the expected signals. The C=CH signals were observed at δ 116.5 (C8) and 131.8 (C9), and the C1 signal at δ 129.8. The
2
methyl and nitrile signals appeared at δ 21.6 and 123.3, respectively. The remaining signals were assigned to the aromatic
carbon atoms.
X-ray structural description. Fig. 1a shows the ORTEP [8] drawing of the asymmetric unit of compound 3,
including the numbering scheme.
The C–C bond lengths in phenyl ring 1 (C1′ to C6′) range from 1.363(5) to 1.390(4) Å. The C4′–C7′ (1.571(4) Å)
distance is longer than the other observed values in correlated compounds [9, 10]. The sulfur atom exhibits a distorted
tetrahedral geometry (angles ranging from 105.3(1)° to 120.6(2)°), probably due to non-bonded intramolecular distances
O1–O2, O1–N1, O2–N1, O1–C1′, and O2–C1′, resulting in structures with less steric interferences. The S–C, S=O, S–N, and
N–C bond lengths present values similar to the other reported structures of sulfonamides [2, 10].
3
The C1–N1–S [121.9(2)°] angle is larger than the value expected for the sp hybrid character of the N1 atom. The
C1–C8 (1.518(3) Å) distance is consistent with the expected value for a single bond [11]. The C8–C10, C8=C9, and C10≡N2
distances are consistent with the values reported by the other authors [12]. The C–C in phenyl ring 2 (C2 to C7) and C1–C2
bond lengths are similar to the observed values in 2-chloro-2,3-diphenyl-3-(tosylamino)propionitrile [10].
The phenyl rings are essentially planar, with r.m.s.d. of 0.0042 Å (ring 1) and 0.0011 Å (ring 2) from the least-
squares plane defined by the atoms. The dihedral angles between these planes is 86.8(1)°. The deviation of the C1 atom to
1193