research communications
N-o-tolylacrylamide
of 2-cyano-3,3-bis(ethylsulfanyl)-aChemistry Department, Faculty of Science, Helwan University, Cairo, Egypt, and bInstitut für Anorganische und Analytische Chemie, Technische Universität Braunschweig, Postfach 3329, D-38023 Braunschweig, Germany
*Correspondence e-mail: p.jones@tu-bs.de
In the molecule of the title compound, C15H18N2OS2, the central S2C=C(CN)C moiety is planar (r.m.s. deviation = 0.029 Å). The C=O and C—CN groups are trans to each other across their common C—C bond. In the crystal, one classical and two `weak' hydrogen bonds combine with borderline N⋯N and S⋯S contacts to form layers parallel to (10-2). One ethyl group is disordered over two positions with relative occupancy 0.721/0.279 (7).
Keywords: crystal structure; cyanoketene; thioacetal.
CCDC reference: 1544524
1. Chemical context
The synthesis of ketene S,S-acetals as potential starting materials for the preparation of novel classes of heterocycles has attracted much attention (Elgemeie et al. 2009, 2015). As part of a research program for preparing new classes of antimetabolites (Elgemeie et al. 2016, 2017a), we have recently reported successful approaches for syntheses of pyridine, pyrimidine and mercaptopurine analogues by the reaction of cyanoketene dithioacetals with active methylene compounds (Elgemeie et al., 2003, 2006, 2017b). In a continuation of this research, we report here a novel cyanoketene dithioacetal (1). Product (1) was prepared by the reaction of 2-cyano-N-(o-tolyl)acetamide with carbon disulfide in the presence of sodium ethoxide followed by alkylation with ethyl iodide. The structure of (1) was originally based on its spectroscopic data and elemental analysis (see Experimental). In order to establish the structure of the compound unambiguously, the was determined.
2. Structural commentary
The X-ray analysis confirms the exclusive presence of the form (1) in the solid state (Fig. 1). Molecular dimensions may be regarded as normal [e.g. C9—C10 1.3781 (16) and C9—C11 1.4290 (16) Å]. The molecular backbone C1, N1, C8, C9, C10, S1, S2 is planar to within an r.m.s. deviation of 0.029 Å; O1 deviates by 0.063 (1) and C11 by 0.284 (1) Å from this plane. The aromatic ring subtends an angle of 53.30 (3)° with the same plane. The C=O and C—CN groups are trans to each other across the C8—C9 bond, with a torsion angle of 167.61 (11)°.
3. Supramolecular features
Hydrogen bonds are given in Table 1, where the operators are also defined. The classical hydrogen bond N1—H01⋯N2i connects the molecules across inversion centres; associated with this interaction, the N2 atoms of both molecules are forced into a close contact of 3.061 (2) Å. Two further contacts (C—H⋯N and C—H⋯O; Table 1) may reasonably be regarded as `weak' hydrogen bonds on the basis of distance and approximately linear angles at the relevant hydrogen atoms. Finally, a borderline contact S1⋯S2ii of 3.7488 (4) Å is observed. All these secondary interactions combine to form a layer of molecules parallel to (10) (Fig. 2).
4. Database survey
A search of the Cambridge Database (Version 1.19; Groom & Allen, 2014; Groom et al., 2016) for the fragment (C—S)2C=C(CN)C=O gave six hits (MTBCEY, NUCFEW, SESHUT10, SESHUT11, ZAMQUZ, ZEDJEX). In all cases the C=O and C—CN groups are mutually trans, as in the title compound.
5. Synthesis and crystallization
2-Cyano-N-(o-tolyl)acetamide (1 mmol) was added to a stirred solution of potassium hydroxide (2 mmol) in DMF (10 ml). After stirring for 30 min at room temperature, carbon disulfide (1.5 mmol) was added. The solution was left for 12 h at room temperature and then ethyl iodide (2 mmol) was added dropwise. Stirring was continued for a further 6 h. The reaction mixture was poured onto ice–water and the solid product was filtered off, dried and crystallized from ethanol to give yellow crystals, m.p. 93°C (366 K), yield 40%.
IR (KBr), 3430 (NH), 2220 (CN), 1670 (C=O) cm−1; 1H NMR (400 MHz, DMSO-d6): δ 1.25 (t, J = 8 Hz, 3H, CH2CH3), 1.31 (t, J = 8 Hz, 3H, CH2CH3), 2.51 (s, 3H, CH3), 3.03 (q, J = 6.8 Hz, 2H, CH2CH3), 3.12 (q, J = 6.8 Hz, 2H, CH2CH3), 7.15–7.36 (m, 4H, C6H4), 10.05 (s, 1H, NH), Analysis calculated for C15H18ON2S2 (306.43): C, 58.82; H, 5.88, N, 9.15, S, 20.91%; Found: C, 58.70; H, 5.65, N, 9.00, S, 20.77%.
6. Refinement
Crystal data, data collection and structure . The ethyl group C14/15 is disordered over two positions with relative occupancy 0.721 (7)/0.279 (7). Appropriate restraints were employed to improve stability, but the dimensions of disordered groups should be interpreted with caution.
details are summarized in Table 2The NH hydrogen was refined freely. Methyl H atoms were refined as idealized rigid groups (C—H 0.98 Å, H—C—H 109.5°) allowed to rotate but not tip (exception: minor disorder component at C15′, set ideally staggered with AFIX 33). Other hydrogen atoms were included using a riding model starting from calculated positions, with Carom—H 0.95, Cmethylene—H 0.99 Å, with Uiso(H) = 1.5Ueq(C-methyl) and 1.2Ueq(C) for other H atoms.
Supporting information
CCDC reference: 1544524
https://doi.org/10.1107/S2056989017005783/hg5488sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989017005783/hg5488Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2056989017005783/hg5488Isup3.cml
Data collection: CrysAlis PRO (Rigaku Oxford Diffraction, 2015); cell
CrysAlis PRO (Rigaku Oxford Diffraction, 2015); data reduction: CrysAlis PRO (Rigaku Oxford Diffraction, 2015); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP (Siemens, 1994); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).C15H18N2OS2 | F(000) = 648 |
Mr = 306.43 | Dx = 1.329 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 10087 reflections |
a = 9.4104 (4) Å | θ = 2.7–30.4° |
b = 12.8350 (4) Å | µ = 0.35 mm−1 |
c = 13.0774 (5) Å | T = 100 K |
β = 104.198 (4)° | Block, pale yellow |
V = 1531.28 (10) Å3 | 0.35 × 0.35 × 0.30 mm |
Z = 4 |
Oxford Diffraction Xcalibur Eos diffractometer | 4682 independent reflections |
Radiation source: fine-focus sealed X-ray tube | 3985 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.043 |
Detector resolution: 16.1419 pixels mm-1 | θmax = 31.2°, θmin = 2.2° |
ω scan | h = −13→13 |
Absorption correction: multi-scan (CrysAlis PRO; Rigaku Oxford Diffraction, 2015) | k = −18→18 |
Tmin = 0.986, Tmax = 1.000 | l = −18→18 |
42164 measured reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.081 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.03 | w = 1/[σ2(Fo2) + (0.0309P)2 + 0.7259P] where P = (Fo2 + 2Fc2)/3 |
4682 reflections | (Δ/σ)max = 0.001 |
197 parameters | Δρmax = 0.37 e Å−3 |
15 restraints | Δρmin = −0.22 e Å−3 |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane) 7.3265 (0.0012) x + 3.0782 (0.0029) y - 9.8498 (0.0015) z = 0.3852 (0.0018) * -0.0120 (0.0007) C1 * 0.0262 (0.0010) C8 * 0.0574 (0.0010) C9 * -0.0136 (0.0009) C10 * -0.0055 (0.0004) S1 * -0.0220 (0.0005) S2 * -0.0304 (0.0009) N1 0.0632 (0.0010) O1 0.2839 (0.0014) C11 Rms deviation of fitted atoms = 0.0287 8.1736 (0.0024) x - 6.3013 (0.0055) y - 3.6411 (0.0064) z = 1.1855 (0.0026) Angle to previous plane (with approximate esd) = 53.30 ( 0.03 ) * -0.0174 (0.0008) C1 * 0.0106 (0.0008) C2 * 0.0039 (0.0009) C3 * -0.0118 (0.0009) C4 * 0.0052 (0.0009) C5 * 0.0095 (0.0008) C6 Rms deviation of fitted atoms = 0.0107 |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > 2sigma(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
C1 | 0.48134 (12) | 0.21516 (9) | 0.38738 (9) | 0.0144 (2) | |
C2 | 0.46128 (12) | 0.24547 (9) | 0.28216 (9) | 0.0156 (2) | |
C3 | 0.37643 (14) | 0.18128 (10) | 0.20464 (9) | 0.0206 (2) | |
H3 | 0.3601 | 0.2008 | 0.1326 | 0.025* | |
C4 | 0.31546 (14) | 0.08976 (10) | 0.23047 (10) | 0.0222 (2) | |
H4 | 0.2564 | 0.0480 | 0.1765 | 0.027* | |
C5 | 0.34046 (14) | 0.05902 (9) | 0.33513 (10) | 0.0200 (2) | |
H5 | 0.3005 | −0.0045 | 0.3529 | 0.024* | |
C6 | 0.42423 (13) | 0.12172 (9) | 0.41347 (9) | 0.0173 (2) | |
H6 | 0.4427 | 0.1008 | 0.4852 | 0.021* | |
C7 | 0.53257 (14) | 0.34242 (10) | 0.25430 (10) | 0.0214 (2) | |
H7A | 0.4999 | 0.4026 | 0.2886 | 0.032* | |
H7B | 0.5051 | 0.3522 | 0.1776 | 0.032* | |
H7C | 0.6393 | 0.3357 | 0.2784 | 0.032* | |
C8 | 0.67932 (12) | 0.25551 (9) | 0.54338 (9) | 0.0148 (2) | |
C9 | 0.74786 (13) | 0.33969 (9) | 0.61750 (9) | 0.0157 (2) | |
C10 | 0.86223 (13) | 0.32278 (9) | 0.70449 (9) | 0.0156 (2) | |
C11 | 0.69858 (13) | 0.44369 (9) | 0.59035 (9) | 0.0176 (2) | |
S1 | 0.94594 (3) | 0.20139 (2) | 0.72800 (2) | 0.01904 (8) | |
C12 | 1.07266 (14) | 0.21116 (10) | 0.85705 (10) | 0.0222 (2) | |
H12A | 1.1520 | 0.1594 | 0.8617 | 0.027* | |
H12B | 1.1179 | 0.2813 | 0.8647 | 0.027* | |
C13 | 1.00032 (18) | 0.19311 (12) | 0.94728 (11) | 0.0324 (3) | |
H13A | 0.9294 | 0.2489 | 0.9481 | 0.049* | |
H13B | 1.0752 | 0.1930 | 1.0142 | 0.049* | |
H13C | 0.9496 | 0.1258 | 0.9378 | 0.049* | |
S2 | 0.93498 (3) | 0.42489 (2) | 0.79137 (2) | 0.02058 (8) | |
C14 | 0.77925 (19) | 0.4973 (2) | 0.81670 (17) | 0.0211 (6) | 0.721 (7) |
H14A | 0.7472 | 0.5518 | 0.7624 | 0.025* | 0.721 (7) |
H14B | 0.6959 | 0.4496 | 0.8145 | 0.025* | 0.721 (7) |
C15 | 0.8290 (3) | 0.5466 (2) | 0.9252 (2) | 0.0234 (5) | 0.721 (7) |
H15A | 0.8431 | 0.4922 | 0.9793 | 0.035* | 0.721 (7) |
H15B | 0.7544 | 0.5959 | 0.9358 | 0.035* | 0.721 (7) |
H15C | 0.9217 | 0.5836 | 0.9306 | 0.035* | 0.721 (7) |
C14' | 0.7812 (5) | 0.4548 (6) | 0.8430 (5) | 0.0206 (13)* | 0.279 (7) |
H14C | 0.6907 | 0.4573 | 0.7853 | 0.025* | 0.279 (7) |
H14D | 0.7689 | 0.4007 | 0.8941 | 0.025* | 0.279 (7) |
C15' | 0.8087 (9) | 0.5593 (6) | 0.8967 (7) | 0.029 (2)* | 0.279 (7) |
H15D | 0.7263 | 0.5771 | 0.9269 | 0.044* | 0.279 (7) |
H15E | 0.8186 | 0.6125 | 0.8451 | 0.044* | 0.279 (7) |
H15F | 0.8991 | 0.5563 | 0.9530 | 0.044* | 0.279 (7) |
N1 | 0.55847 (11) | 0.28375 (8) | 0.46806 (8) | 0.0169 (2) | |
H01 | 0.5279 (18) | 0.3435 (14) | 0.4655 (12) | 0.026 (4)* | |
N2 | 0.65583 (12) | 0.52547 (8) | 0.56292 (9) | 0.0244 (2) | |
O1 | 0.73077 (10) | 0.16749 (7) | 0.55038 (7) | 0.01999 (18) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0152 (5) | 0.0127 (5) | 0.0153 (5) | 0.0007 (4) | 0.0036 (4) | −0.0020 (4) |
C2 | 0.0157 (5) | 0.0146 (5) | 0.0170 (5) | 0.0021 (4) | 0.0048 (4) | 0.0008 (4) |
C3 | 0.0233 (6) | 0.0228 (6) | 0.0149 (5) | 0.0019 (5) | 0.0032 (4) | −0.0014 (4) |
C4 | 0.0219 (6) | 0.0191 (6) | 0.0236 (6) | −0.0007 (5) | 0.0018 (5) | −0.0073 (5) |
C5 | 0.0205 (6) | 0.0130 (5) | 0.0272 (6) | −0.0016 (4) | 0.0074 (5) | −0.0019 (4) |
C6 | 0.0208 (6) | 0.0144 (5) | 0.0179 (5) | 0.0010 (4) | 0.0071 (4) | 0.0005 (4) |
C7 | 0.0230 (6) | 0.0202 (6) | 0.0221 (6) | −0.0010 (5) | 0.0075 (5) | 0.0048 (5) |
C8 | 0.0166 (5) | 0.0134 (5) | 0.0153 (5) | −0.0007 (4) | 0.0055 (4) | 0.0004 (4) |
C9 | 0.0170 (5) | 0.0121 (5) | 0.0172 (5) | 0.0008 (4) | 0.0025 (4) | −0.0005 (4) |
C10 | 0.0150 (5) | 0.0141 (5) | 0.0179 (5) | 0.0010 (4) | 0.0046 (4) | −0.0003 (4) |
C11 | 0.0173 (5) | 0.0155 (5) | 0.0175 (5) | −0.0013 (4) | −0.0007 (4) | −0.0032 (4) |
S1 | 0.02006 (15) | 0.01621 (14) | 0.01943 (14) | 0.00640 (11) | 0.00213 (11) | −0.00021 (10) |
C12 | 0.0184 (6) | 0.0217 (6) | 0.0232 (6) | 0.0053 (5) | −0.0010 (4) | 0.0018 (5) |
C13 | 0.0391 (8) | 0.0344 (8) | 0.0218 (6) | 0.0005 (6) | 0.0036 (6) | 0.0036 (6) |
S2 | 0.01549 (14) | 0.01860 (15) | 0.02518 (15) | 0.00178 (10) | 0.00028 (11) | −0.00709 (11) |
C14 | 0.0192 (9) | 0.0211 (12) | 0.0238 (9) | 0.0043 (7) | 0.0069 (6) | −0.0028 (8) |
C15 | 0.0326 (12) | 0.0214 (10) | 0.0185 (11) | 0.0020 (8) | 0.0105 (10) | −0.0036 (9) |
N1 | 0.0210 (5) | 0.0107 (4) | 0.0167 (4) | 0.0021 (4) | 0.0001 (4) | −0.0014 (4) |
N2 | 0.0239 (6) | 0.0151 (5) | 0.0278 (5) | −0.0002 (4) | −0.0061 (4) | −0.0021 (4) |
O1 | 0.0224 (4) | 0.0132 (4) | 0.0227 (4) | 0.0037 (3) | 0.0025 (3) | −0.0014 (3) |
C1—C6 | 1.3905 (16) | C3—H3 | 0.9500 |
C1—C2 | 1.3975 (15) | C4—H4 | 0.9500 |
C1—N1 | 1.4282 (14) | C5—H5 | 0.9500 |
C2—C3 | 1.3953 (16) | C6—H6 | 0.9500 |
C2—C7 | 1.5004 (16) | C7—H7A | 0.9800 |
C3—C4 | 1.3850 (18) | C7—H7B | 0.9800 |
C4—C5 | 1.3879 (18) | C7—H7C | 0.9800 |
C5—C6 | 1.3865 (17) | C12—H12A | 0.9900 |
C8—O1 | 1.2236 (14) | C12—H12B | 0.9900 |
C8—N1 | 1.3585 (15) | C13—H13A | 0.9800 |
C8—C9 | 1.4888 (16) | C13—H13B | 0.9800 |
C9—C10 | 1.3781 (16) | C13—H13C | 0.9800 |
C9—C11 | 1.4290 (16) | C14—H14A | 0.9900 |
C10—S1 | 1.7390 (12) | C14—H14B | 0.9900 |
C10—S2 | 1.7594 (12) | C15—H15A | 0.9800 |
C11—N2 | 1.1496 (16) | C15—H15B | 0.9800 |
S1—C12 | 1.8162 (13) | C15—H15C | 0.9800 |
C12—C13 | 1.518 (2) | C14'—H14C | 0.9900 |
S2—C14' | 1.783 (5) | C14'—H14D | 0.9900 |
S2—C14 | 1.8326 (18) | C15'—H15D | 0.9800 |
C14—C15 | 1.519 (3) | C15'—H15E | 0.9800 |
C14'—C15' | 1.507 (9) | C15'—H15F | 0.9800 |
N1—H01 | 0.817 (17) | ||
C6—C1—C2 | 120.98 (10) | C2—C7—H7A | 109.5 |
C6—C1—N1 | 120.49 (10) | C2—C7—H7B | 109.5 |
C2—C1—N1 | 118.50 (10) | H7A—C7—H7B | 109.5 |
C3—C2—C1 | 117.77 (11) | C2—C7—H7C | 109.5 |
C3—C2—C7 | 121.57 (11) | H7A—C7—H7C | 109.5 |
C1—C2—C7 | 120.63 (10) | H7B—C7—H7C | 109.5 |
C4—C3—C2 | 121.40 (11) | C13—C12—H12A | 108.9 |
C3—C4—C5 | 120.10 (11) | S1—C12—H12A | 108.9 |
C6—C5—C4 | 119.46 (11) | C13—C12—H12B | 108.9 |
C5—C6—C1 | 120.21 (11) | S1—C12—H12B | 108.9 |
O1—C8—N1 | 123.11 (11) | H12A—C12—H12B | 107.7 |
O1—C8—C9 | 121.40 (10) | C12—C13—H13A | 109.5 |
N1—C8—C9 | 115.49 (10) | C12—C13—H13B | 109.5 |
C10—C9—C11 | 119.50 (10) | H13A—C13—H13B | 109.5 |
C10—C9—C8 | 123.30 (10) | C12—C13—H13C | 109.5 |
C11—C9—C8 | 116.99 (10) | H13A—C13—H13C | 109.5 |
C9—C10—S1 | 121.02 (9) | H13B—C13—H13C | 109.5 |
C9—C10—S2 | 121.14 (9) | C15—C14—H14A | 110.2 |
S1—C10—S2 | 117.75 (7) | S2—C14—H14A | 110.2 |
N2—C11—C9 | 176.23 (12) | C15—C14—H14B | 110.2 |
C10—S1—C12 | 105.56 (6) | S2—C14—H14B | 110.2 |
C13—C12—S1 | 113.23 (10) | H14A—C14—H14B | 108.5 |
C10—S2—C14' | 100.46 (17) | C15'—C14'—H14C | 110.1 |
C10—S2—C14 | 107.01 (7) | S2—C14'—H14C | 110.1 |
C15—C14—S2 | 107.65 (16) | C15'—C14'—H14D | 110.1 |
C15'—C14'—S2 | 107.8 (5) | S2—C14'—H14D | 110.1 |
C8—N1—C1 | 123.68 (10) | H14C—C14'—H14D | 108.5 |
C4—C3—H3 | 119.3 | C14'—C15'—H15D | 109.5 |
C2—C3—H3 | 119.3 | C14'—C15'—H15E | 109.5 |
C3—C4—H4 | 120.0 | H15D—C15'—H15E | 109.5 |
C5—C4—H4 | 120.0 | C14'—C15'—H15F | 109.5 |
C6—C5—H5 | 120.3 | H15D—C15'—H15F | 109.5 |
C4—C5—H5 | 120.3 | H15E—C15'—H15F | 109.5 |
C5—C6—H6 | 119.9 | C8—N1—H01 | 120.2 (11) |
C1—C6—H6 | 119.9 | C1—N1—H01 | 116.0 (11) |
C6—C1—C2—C3 | 2.91 (17) | C11—C9—C10—S2 | 7.34 (16) |
N1—C1—C2—C3 | −175.34 (11) | C8—C9—C10—S2 | −178.08 (9) |
C6—C1—C2—C7 | −175.44 (11) | C9—C10—S1—C12 | −173.24 (10) |
N1—C1—C2—C7 | 6.31 (16) | S2—C10—S1—C12 | 10.20 (9) |
C1—C2—C3—C4 | −0.85 (18) | C10—S1—C12—C13 | 83.40 (11) |
C7—C2—C3—C4 | 177.48 (12) | C9—C10—S2—C14' | 64.9 (3) |
C2—C3—C4—C5 | −1.27 (19) | S1—C10—S2—C14' | −118.6 (3) |
C3—C4—C5—C6 | 1.35 (19) | C9—C10—S2—C14 | 44.96 (14) |
C4—C5—C6—C1 | 0.68 (18) | S1—C10—S2—C14 | −138.48 (11) |
C2—C1—C6—C5 | −2.86 (18) | C10—S2—C14—C15 | 152.32 (19) |
N1—C1—C6—C5 | 175.35 (11) | C14'—S2—C14—C15 | 78.5 (5) |
O1—C8—C9—C10 | −7.09 (18) | C10—S2—C14'—C15' | −164.9 (5) |
N1—C8—C9—C10 | 173.60 (11) | C14—S2—C14'—C15' | −53.9 (6) |
O1—C8—C9—C11 | 167.61 (11) | O1—C8—N1—C1 | −1.97 (18) |
N1—C8—C9—C11 | −11.70 (15) | C9—C8—N1—C1 | 177.32 (10) |
C11—C9—C10—S1 | −169.10 (9) | C6—C1—N1—C8 | 57.60 (16) |
C8—C9—C10—S1 | 5.47 (16) | C2—C1—N1—C8 | −124.15 (12) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H01···N2i | 0.817 (17) | 2.375 (17) | 3.1346 (15) | 155.0 (15) |
C12—H12A···N2ii | 0.99 | 2.51 | 3.4628 (16) | 160 |
C5—H5···O1iii | 0.95 | 2.50 | 3.4110 (15) | 161 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+2, y−1/2, −z+3/2; (iii) −x+1, −y, −z+1. |
References
Elgemeie, G. H., Abou-Zeid, M., Alsaid, S., Hebishy, A. & Essa, H. (2015). Nucleosides Nucleotides Nucleic Acids, 34, 659–673. Web of Science CrossRef CAS PubMed Google Scholar
Elgemeie, G. H., Abu-Zaied, M. & Azzam, R. (2016). Nucleosides Nucleotides Nucleic Acids, 35, 211–222. Web of Science CrossRef CAS PubMed Google Scholar
Elgemeie, G. H., El-Ezbawy, S. R. & Sood, S. A. (2003). Synth. Commun. 33, 2095–2101. Web of Science CrossRef CAS Google Scholar
Elgemeie, G. H., Elsayed, S. H. & Hassan, A. S. (2009). Synth. Commun. 39, 1781–1792. Web of Science CrossRef CAS Google Scholar
Elgemeie, G. H., Elzanaty, A. M., Elghandour, A. H. & Ahmed, S. A. (2006). Synth. Commun. 36, 825–834. CrossRef CAS Google Scholar
Elgemeie, G. H., Fathy, N., Zaghary, W. & Farag, A. (2017b). Nucleosides Nucleotides Nucleic Acids, 36, 198–212. CrossRef CAS PubMed Google Scholar
Elgemeie, G. H., Salah, A. M., Abbas, N. S., Hussein, H. A. & Mohamed, R. A. (2017a). Nucleosides Nucleotides Nucleic Acids, 36, 213–223. CrossRef CAS PubMed Google Scholar
Groom, C. R. & Allen, F. H. (2014). Angew. Chem. Int. Ed. 53, 662–671. Web of Science CSD CrossRef CAS Google Scholar
Groom, C. R., Bruno, I. J., Lightfoot, M. P. & Ward, S. C. (2016). Acta Cryst. B72, 171–179. Web of Science CSD CrossRef IUCr Journals Google Scholar
Rigaku Oxford Diffraction (2015). CrysAlis PRO. Rigaku Oxford Diffraction Ltd, Yarnton, England. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Siemens (1994). XP. Siemens Analytical X-ray Instruments, Madison, Wisconsin, USA. Google Scholar
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