organic compounds
(E)-N,N′-(1,2-Dicyanoethene-1,2-diyl)dipicolinamide
aInstitute of Chemistry, University of Neuchâtel, Av de Bellevaux 51, CH-2000 Neuchâtel, Switzerland, and bInstitute of Physics, University of Neuchâtel, rue Emile-Argand 11, CH-2000 Neuchâtel, Switzerland
*Correspondence e-mail: helen.stoeckli-evans@unine.ch
The whole molecule of the title dicyanoethene derivative, C16H10N6O2, is generated by inversion symmetry. The conformation about the central C=C bond, which is situated about the inversion center, is E. There are short intramolecular N—H⋯N contacts present and the molecule is slightly twisted, with the plane of the amide C(=O)N group being inclined to the pyridine ring by 10.6 (4)°, and by 20.2 (4)° to the plane of the dicyanoethene unit (N≡C—C=C—C≡N). In the crystal, molecules are linked by C—H⋯O and C—H⋯N hydrogen bonds, forming sheets parallel to (1-21), enclosing R22(10), R22(22) and R44(22) ring motifs.
Keywords: crystal structure; picolinamide; dicyanoethene; hydrogen bonding.
CCDC reference: 1504520
Structure description
When synthesizing 2,3-bis(2-pyridyl)-5,6-dicyanopyrazine, whose structure and an alternative synthesis have been described (Du et al., 2001), an orange–brown precipitate was formed. This precipitate was recrystallized from a mixture of solvents (see below) and found to be the title compound. From the filtrate, colourless crystals of 2,3-bis(2-pyridyl)-5,6-dicyanopyrazine were obtained.
The whole molecule of the title dicyanoethene derivative, Fig. 1, is generated by inversion symmetry. The conformation about the central C7=C7i bond [symmetry code: (i) −x + 1, −y + 1, −z + 1], situated about the inversion center, is E. There are short intramolecular N—H⋯N contacts present and the molecule is slightly twisted, with the plane of the amide C(=O)N group being inclined to the pyridine ring by 10.6 (4)°, and by 20.2 (4)° to the plane of the dicyanoethene unit (N≡C—C=C—C≡ N).
In the crystal, molecules are linked by C—H⋯O and C—H⋯N hydrogen bonds, forming sheets parallel to (11), enclosing (10), (22) and (22) ring motifs (Table 1 and Fig. 2).
Synthesis and crystallization
In a round-bottomed flask outfitted with a reflux condenser, 9.3663 g (0.0 3 mol) of 2,2′-pyridyl were dissolved in 15 ml of dry n-butanol. A solution of 2.7026 g (0.025 mol) of diaminomaleonitrile in 15 ml of dry n-butanol was then added at 333 K with stirring. The mixture was refluxed for 3 h. After stopping the reaction, the mixture was filtered to remove the orange–brown precipitate that had formed. This orange–brown precipitate was recrystallized from a mixture of methanol/acetonitrile/acetylacetone (3/3/1), which resulted in the formation of yellow needle-like crystals of the title compound on slow evaporation of the solvents (yield 2.5 g, 32%; m.p. > 360 K). From the filtrate, colourless crystals of 2,3-bis(2-pyridyl)-5,6-dicyanopyrazine were obtained on slow evaporation of the solvent n-butanol.
The mechanism for the synthesis of the title compound is unknown. However, Du et al. (2001) did note that 2,3-bis(2-pyridyl)-5,6-dicyanopyrazine is not stable when exposed to air for several months. Hence, we may postulate that the title compound may be formed by oxidation of 2,3-bis(2-pyridyl)-5,6-dicyanopyrazine.
Refinement
Crystal data, data collection and structure . The NH H atom was located in a difference Fourier map and freely refined. Only one equivalent of data was measured, hence Rint = 0.
details are summarized in Table 2Structural data
CCDC reference: 1504520
10.1107/S2414314616014644/hg4014sup1.cif
contains datablocks I, Global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S2414314616014644/hg4014Isup2.hkl
Supporting information file. DOI: 10.1107/S2414314616014644/hg4014Isup3.cml
Data collection: STADI4 (Stoe & Cie, 1997); cell
STADI4 (Stoe & Cie, 1997); data reduction: X-RED (Stoe & Cie, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014/6 (Sheldrick, 2015); molecular graphics: PLATON (Spek, 2009) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL2014/6 (Sheldrick, 2015), PLATON (Spek, 2009) and publCIF (Westrip, 2010).C16H10N6O2 | Z = 1 |
Mr = 318.30 | F(000) = 164 |
Triclinic, P1 | Dx = 1.444 Mg m−3 |
a = 5.1939 (11) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 8.0697 (17) Å | Cell parameters from 18 reflections |
c = 9.1482 (15) Å | θ = 12.5–19.5° |
α = 106.819 (19)° | µ = 0.10 mm−1 |
β = 96.077 (18)° | T = 293 K |
γ = 92.804 (18)° | Needle, yellow |
V = 363.69 (13) Å3 | 0.72 × 0.30 × 0.30 mm |
STOE–Siemens AED2, 4-circle diffractometer | Rint = 0.0 |
Radiation source: fine-focus sealed tube | θmax = 25.0°, θmin = 2.7° |
Plane graphite monochromator | h = −6→6 |
ω/2θ scans | k = −9→9 |
1281 measured reflections | l = 0→10 |
1281 independent reflections | 3 standard reflections every 60 min |
1196 reflections with I > 2σ(I) | intensity decay: 4% |
Refinement on F2 | Hydrogen site location: mixed |
Least-squares matrix: full | H atoms treated by a mixture of independent and constrained refinement |
R[F2 > 2σ(F2)] = 0.073 | w = 1/[σ2(Fo2) + (0.0451P)2 + 0.1443P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.155 | (Δ/σ)max < 0.001 |
S = 1.40 | Δρmax = 0.17 e Å−3 |
1281 reflections | Δρmin = −0.17 e Å−3 |
114 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.063 (14) |
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. |
x | y | z | Uiso*/Ueq | ||
O1 | 0.8969 (4) | 0.4716 (3) | 0.2158 (2) | 0.0663 (7) | |
N1 | 0.3495 (4) | 0.1893 (3) | 0.0137 (3) | 0.0459 (6) | |
N2 | 0.5113 (4) | 0.4118 (3) | 0.2910 (3) | 0.0440 (6) | |
H2N | 0.359 (7) | 0.360 (4) | 0.255 (4) | 0.069 (10)* | |
N3 | 0.9259 (6) | 0.7628 (4) | 0.5384 (3) | 0.0728 (9) | |
C1 | 0.2632 (5) | 0.0829 (4) | −0.1254 (3) | 0.0524 (8) | |
H1 | 0.1094 | 0.0137 | −0.1371 | 0.063* | |
C2 | 0.3889 (6) | 0.0691 (4) | −0.2533 (3) | 0.0573 (8) | |
H2 | 0.3210 | −0.0075 | −0.3483 | 0.069* | |
C3 | 0.6154 (6) | 0.1702 (4) | −0.2379 (3) | 0.0573 (8) | |
H3 | 0.7030 | 0.1644 | −0.3226 | 0.069* | |
C4 | 0.7115 (6) | 0.2807 (4) | −0.0949 (3) | 0.0492 (7) | |
H4 | 0.8652 | 0.3506 | −0.0807 | 0.059* | |
C5 | 0.5737 (5) | 0.2848 (3) | 0.0266 (3) | 0.0405 (6) | |
C6 | 0.6791 (5) | 0.3986 (4) | 0.1837 (3) | 0.0441 (7) | |
C7 | 0.5678 (5) | 0.5119 (3) | 0.4442 (3) | 0.0396 (6) | |
C8 | 0.7738 (5) | 0.6490 (4) | 0.4874 (3) | 0.0473 (7) |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0450 (12) | 0.0910 (17) | 0.0489 (13) | −0.0214 (11) | 0.0134 (9) | 0.0003 (11) |
N1 | 0.0381 (12) | 0.0477 (13) | 0.0495 (14) | −0.0021 (10) | 0.0072 (10) | 0.0110 (11) |
N2 | 0.0359 (12) | 0.0535 (14) | 0.0370 (13) | −0.0098 (10) | 0.0077 (10) | 0.0059 (10) |
N3 | 0.0664 (18) | 0.0739 (19) | 0.0645 (18) | −0.0321 (16) | 0.0050 (14) | 0.0064 (15) |
C1 | 0.0429 (16) | 0.0514 (17) | 0.0549 (19) | −0.0035 (13) | −0.0033 (13) | 0.0077 (14) |
C2 | 0.0615 (19) | 0.0557 (18) | 0.0441 (17) | 0.0014 (15) | −0.0043 (14) | 0.0027 (14) |
C3 | 0.0638 (19) | 0.067 (2) | 0.0387 (16) | 0.0033 (16) | 0.0120 (14) | 0.0109 (14) |
C4 | 0.0456 (16) | 0.0547 (17) | 0.0454 (17) | −0.0026 (13) | 0.0110 (12) | 0.0110 (13) |
C5 | 0.0391 (14) | 0.0423 (14) | 0.0387 (15) | 0.0025 (11) | 0.0071 (11) | 0.0093 (11) |
C6 | 0.0383 (14) | 0.0499 (16) | 0.0437 (16) | −0.0027 (12) | 0.0097 (12) | 0.0127 (12) |
C7 | 0.0335 (13) | 0.0436 (15) | 0.0394 (15) | −0.0050 (11) | 0.0071 (10) | 0.0094 (11) |
C8 | 0.0426 (15) | 0.0563 (17) | 0.0391 (15) | −0.0094 (13) | 0.0082 (12) | 0.0093 (13) |
O1—C6 | 1.215 (3) | C2—C3 | 1.369 (4) |
N1—C1 | 1.329 (3) | C2—H2 | 0.9300 |
N1—C5 | 1.339 (3) | C3—C4 | 1.378 (4) |
N2—C6 | 1.365 (3) | C3—H3 | 0.9300 |
N2—C7 | 1.392 (3) | C4—C5 | 1.378 (4) |
N2—H2N | 0.86 (3) | C4—H4 | 0.9300 |
N3—C8 | 1.135 (4) | C5—C6 | 1.493 (4) |
C1—C2 | 1.379 (4) | C7—C7i | 1.352 (5) |
C1—H1 | 0.9300 | C7—C8 | 1.438 (4) |
C1—N1—C5 | 116.4 (2) | C5—C4—C3 | 118.2 (3) |
C6—N2—C7 | 124.1 (2) | C5—C4—H4 | 120.9 |
C6—N2—H2N | 115 (2) | C3—C4—H4 | 120.9 |
C7—N2—H2N | 121 (2) | N1—C5—C4 | 123.9 (3) |
N1—C1—C2 | 123.7 (3) | N1—C5—C6 | 116.9 (2) |
N1—C1—H1 | 118.1 | C4—C5—C6 | 119.2 (2) |
C2—C1—H1 | 118.1 | O1—C6—N2 | 122.1 (3) |
C3—C2—C1 | 118.8 (3) | O1—C6—C5 | 123.5 (2) |
C3—C2—H2 | 120.6 | N2—C6—C5 | 114.3 (2) |
C1—C2—H2 | 120.6 | C7i—C7—N2 | 122.5 (3) |
C2—C3—C4 | 118.9 (3) | C7i—C7—C8 | 117.8 (3) |
C2—C3—H3 | 120.5 | N2—C7—C8 | 119.7 (2) |
C4—C3—H3 | 120.5 | N3—C8—C7 | 171.7 (3) |
C5—N1—C1—C2 | −1.0 (4) | C7—N2—C6—O1 | 1.8 (5) |
N1—C1—C2—C3 | −0.1 (5) | C7—N2—C6—C5 | −179.4 (2) |
C1—C2—C3—C4 | 0.7 (5) | N1—C5—C6—O1 | 168.8 (3) |
C2—C3—C4—C5 | −0.2 (4) | C4—C5—C6—O1 | −10.0 (4) |
C1—N1—C5—C4 | 1.6 (4) | N1—C5—C6—N2 | −10.0 (4) |
C1—N1—C5—C6 | −177.1 (2) | C4—C5—C6—N2 | 171.2 (3) |
C3—C4—C5—N1 | −1.0 (4) | C6—N2—C7—C7i | −161.8 (3) |
C3—C4—C5—C6 | 177.7 (3) | C6—N2—C7—C8 | 19.5 (4) |
Symmetry code: (i) −x+1, −y+1, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2N···N1 | 0.86 (3) | 2.23 (3) | 2.671 (3) | 111 (3) |
C2—H2···N3ii | 0.93 | 2.61 | 3.354 (4) | 138 |
C4—H4···O1iii | 0.93 | 2.51 | 3.274 (4) | 140 |
Symmetry codes: (ii) x−1, y−1, z−1; (iii) −x+2, −y+1, −z. |
Acknowledgements
We are grateful to the Swiss National Science Foundation and the University of Neuchâtel for financial support.
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