organic compounds
5-Methylpyrazine-2-carboxamide
aDepartment of Chemistry, Wichita State University, Wichita, KS 67260, USA, and bCrystallographic laboratory, University of California, San Diego, LaJolla, CA 92093, USA
*Correspondence e-mail: paul.rillema@wichita.edu
The title compound, C6H7N3O, is nearly planar, with a dihedral angle of 2.14 (11)° between the pyrazine ring and the mean plane of the carboxamide group [C—C(=O)—N]. In the crystal, molecules are linked via pairs of N—H⋯O hydrogen bonds forming inversion dimers with an R22(8) ring motif. These dimers are further linked by a pair of N—H⋯N hydrogen bonds, enclosing an R22(10) ring motif, and C—H⋯O hydrogen bonds, forming ribbons lying parallel to the ab plane. The ribbons are linked by offset π–π interactions [intercentroid distance = 3.759 (1) Å], forming two sets of mutually perpendicular slabs parallel to planes (110) and (1-10).
Keywords: crystal structure; amide; pyrazine; hydrogen bonding.
CCDC reference: 1564289
Structure description
The title compound, is an intermediate in the preparation of 2-bromo-5-methylpyrazine (Madhusudhan et al., 2009). The latter compound has been used to synthesize 5,5′-dimethyl-2,2′-bipyrazine (Pefkianakis et al., 2008) derivatives as bidentate ligands to coordinate to transition metals. The molecular structure of the title compound is illustrated in Fig. 1. The bond lengths of the methylpyrazine component are similar to those found in methyl 5-methyl-2-pyrazinecarboxylate (Rillema et al., 2017). The molecule is planar with a dihedral angle of 2.14 (11)° between the pyrazine ring (N2/N3/C2–C5) and the mean plane of the carboxamide group [atoms C2—C1(=O1)—N1].
In the crystal, molecules are linked via pairs of N—H⋯O hydrogen bonds, forming classical amide–amide inversion dimers with an R22(8) ring motif (Table 1 and Fig. 2). These dimers are further linked by pairs of N—H⋯N hydrogen bonds, enclosing R22(10) ring motifs, and C—H⋯O hydrogen bonds, forming ribbons lying parallel to (001); see Table 1 and Fig. 2. The ribbons are linked in the a-axis direction by offset π–π interactions, forming two sets of mutually perpendicular slabs parallel to (110) and (10), as shown in Fig. 3 [Cg⋯Cgi,ii = 3.759 (1) Å, Cg is the centroid of the pyrazine ring, interplanar distance = 3.386 (1) Å, slippage = 1.63 Å, symmetry codes: (i) −1 + x, y, z; (ii) 1 + x, y, z].
Synthesis and crystallization
Methyl 5-methyl-2-pyrazinecarboxylate (80.0 g, 0.657 mole) (Rillema et al., 2017) was added to 600 ml of methanol in a 1 litre round-bottomed flask. The flask was immersed in an ice bath, the contents were cooled to ca 273 K, stirred with a magnetic stirrer and then purged with ammonia gas for 4 h. The reaction progress was monitored by (TLC). After completion of the reaction, the product was separated by filtration and washed with pre-cooled methanol (2 × 30 ml) to give the title compound as a light-brown coloured solid. It was recrystallized by dissolving a small amount in methanol and then allowing the methanol to evaporate slowly, yielding colourless needles.
Refinement
Crystal data, data collection and .
details are summarized in Table 2Structural data
CCDC reference: 1564289
https://doi.org/10.1107/S2414314617010902/su4158sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314617010902/su4158Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314617010902/su4158Isup3.cml
Data collection: APEX2 (Bruker, 2013); cell
SAINT (Bruker, 2013); data reduction: SAINT (Bruker, 2013); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015b); molecular graphics: OLEX2 (Dolomanov et al., 2009) and Mercury (Macrae et al., 2008); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009) and PLATON (Spek, 2009).C6H7N3O | F(000) = 288 |
Mr = 137.15 | Dx = 1.425 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 3.7592 (9) Å | Cell parameters from 1367 reflections |
b = 6.7317 (13) Å | θ = 3.1–24.9° |
c = 25.290 (5) Å | µ = 0.10 mm−1 |
β = 93.106 (14)° | T = 100 K |
V = 639.0 (2) Å3 | Needle, colourless |
Z = 4 | 0.22 × 0.11 × 0.09 mm |
Bruker X8 APEXII diffractometer | 1182 independent reflections |
Radiation source: sealed tube, fine-focus | 849 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.046 |
Detector resolution: 7.9 pixels mm-1 | θmax = 25.4°, θmin = 3.1° |
ω and φ scans | h = −4→4 |
Absorption correction: multi-scan (SADABS; Bruker, 2013) | k = −8→8 |
Tmin = 0.218, Tmax = 0.259 | l = −30→30 |
7302 measured reflections |
Refinement on F2 | Primary atom site location: dual |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.043 | Hydrogen site location: mixed |
wR(F2) = 0.104 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.03 | w = 1/[σ2(Fo2) + (0.0525P)2 + 0.1949P] where P = (Fo2 + 2Fc2)/3 |
1182 reflections | (Δ/σ)max < 0.001 |
100 parameters | Δρmax = 0.20 e Å−3 |
2 restraints | Δρmin = −0.21 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. |
x | y | z | Uiso*/Ueq | ||
O1 | 0.9776 (4) | 0.95545 (19) | 0.42480 (5) | 0.0240 (4) | |
N1 | 0.7790 (5) | 0.7706 (3) | 0.49219 (7) | 0.0237 (5) | |
H1A | 0.668 (5) | 0.654 (3) | 0.5011 (9) | 0.034 (6)* | |
H1B | 0.853 (6) | 0.861 (3) | 0.5190 (8) | 0.039 (7)* | |
N2 | 0.5554 (4) | 0.4823 (2) | 0.42240 (6) | 0.0179 (4) | |
N3 | 0.6419 (4) | 0.5310 (2) | 0.31371 (6) | 0.0183 (4) | |
C1 | 0.8296 (5) | 0.8043 (3) | 0.44120 (7) | 0.0181 (5) | |
C2 | 0.7022 (5) | 0.6467 (3) | 0.40302 (7) | 0.0155 (5) | |
C3 | 0.7440 (5) | 0.6691 (3) | 0.34927 (7) | 0.0176 (5) | |
H3 | 0.8497 | 0.7877 | 0.3372 | 0.021* | |
C4 | 0.4559 (5) | 0.3434 (3) | 0.38712 (7) | 0.0177 (5) | |
H4 | 0.3536 | 0.2241 | 0.3994 | 0.021* | |
C5 | 0.4955 (5) | 0.3657 (3) | 0.33261 (7) | 0.0164 (5) | |
C6 | 0.3727 (5) | 0.2094 (3) | 0.29402 (8) | 0.0229 (5) | |
H6A | 0.1921 | 0.2653 | 0.2689 | 0.034* | |
H6B | 0.2696 | 0.0984 | 0.3131 | 0.034* | |
H6C | 0.5755 | 0.1619 | 0.2748 | 0.034* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0332 (9) | 0.0174 (7) | 0.0215 (8) | −0.0117 (6) | 0.0037 (6) | 0.0002 (6) |
N1 | 0.0357 (11) | 0.0195 (9) | 0.0161 (9) | −0.0138 (8) | 0.0031 (8) | −0.0022 (8) |
N2 | 0.0205 (10) | 0.0153 (8) | 0.0179 (9) | −0.0030 (7) | 0.0007 (7) | 0.0014 (7) |
N3 | 0.0186 (9) | 0.0183 (8) | 0.0179 (9) | −0.0014 (7) | 0.0001 (7) | 0.0000 (7) |
C1 | 0.0180 (11) | 0.0173 (10) | 0.0190 (11) | −0.0019 (9) | 0.0005 (9) | 0.0005 (8) |
C2 | 0.0141 (11) | 0.0146 (10) | 0.0176 (10) | −0.0003 (8) | −0.0014 (8) | 0.0008 (8) |
C3 | 0.0166 (11) | 0.0167 (9) | 0.0194 (11) | −0.0029 (8) | 0.0017 (9) | 0.0038 (8) |
C4 | 0.0199 (11) | 0.0127 (9) | 0.0206 (11) | −0.0029 (8) | 0.0026 (9) | 0.0005 (8) |
C5 | 0.0123 (10) | 0.0168 (10) | 0.0200 (11) | 0.0004 (8) | 0.0009 (8) | −0.0009 (8) |
C6 | 0.0225 (12) | 0.0243 (11) | 0.0223 (11) | −0.0050 (9) | 0.0035 (9) | −0.0059 (9) |
O1—C1 | 1.241 (2) | C2—C3 | 1.385 (3) |
N1—H1A | 0.923 (16) | C3—H3 | 0.9500 |
N1—H1B | 0.941 (16) | C4—H4 | 0.9500 |
N1—C1 | 1.333 (2) | C4—C5 | 1.403 (3) |
N2—C2 | 1.341 (2) | C5—C6 | 1.491 (3) |
N2—C4 | 1.332 (2) | C6—H6A | 0.9800 |
N3—C3 | 1.335 (2) | C6—H6B | 0.9800 |
N3—C5 | 1.341 (2) | C6—H6C | 0.9800 |
C1—C2 | 1.496 (3) | ||
H1A—N1—H1B | 120 (2) | C2—C3—H3 | 118.6 |
C1—N1—H1A | 118.2 (14) | N2—C4—H4 | 118.6 |
C1—N1—H1B | 122.3 (14) | N2—C4—C5 | 122.85 (17) |
C4—N2—C2 | 116.15 (16) | C5—C4—H4 | 118.6 |
C3—N3—C5 | 116.50 (16) | N3—C5—C4 | 120.43 (17) |
O1—C1—N1 | 123.55 (18) | N3—C5—C6 | 118.08 (17) |
O1—C1—C2 | 119.96 (16) | C4—C5—C6 | 121.48 (17) |
N1—C1—C2 | 116.48 (16) | C5—C6—H6A | 109.5 |
N2—C2—C1 | 118.25 (16) | C5—C6—H6B | 109.5 |
N2—C2—C3 | 121.26 (17) | C5—C6—H6C | 109.5 |
C3—C2—C1 | 120.47 (16) | H6A—C6—H6B | 109.5 |
N3—C3—C2 | 122.80 (17) | H6A—C6—H6C | 109.5 |
N3—C3—H3 | 118.6 | H6B—C6—H6C | 109.5 |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1B···O1i | 0.94 (2) | 1.96 (2) | 2.905 (2) | 178 (2) |
N1—H1A···N2ii | 0.92 (2) | 2.34 (2) | 3.072 (2) | 136 (2) |
C4—H4···O1iii | 0.95 | 2.40 | 3.339 (3) | 168 |
Symmetry codes: (i) −x+2, −y+2, −z+1; (ii) −x+1, −y+1, −z+1; (iii) x−1, y−1, z. |
Funding information
We are grateful for support from the National Science Foundation (EPSCoR), the Wichita State University Office of Research and the Department of Energy.
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