Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680503953X/bh6050sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S160053680503953X/bh6050Isup2.hkl |
CCDC reference: 296520
The title compound was obtained by recrystallization of an impure batch of this compound. The crystal used for data collection was obtained by slow evaporation at 298 K of a methanol solution, over a period of one week.
C bound H atoms were placed in calculated positions and allowed to ride on their parent atoms, with C—H distances constrained to 0.93 Å and Uiso(H) = 1.2Ueq(parent C atom). The H atom of the hydroxy group was found in a difference map and refined with the O—H distance constrained to 0.82 Å and Uiso(H) = 1.5Ueq(O). In the absence of significant anomalous scattering effects, measured Friedel pairs were merged.
Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.
C5H4N2O2 | F(000) = 128 |
Mr = 124.10 | Dx = 1.558 Mg m−3 |
Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2yb | Cell parameters from 477 reflections |
a = 3.7249 (14) Å | θ = 3.5–23.7° |
b = 11.281 (4) Å | µ = 0.12 mm−1 |
c = 6.298 (2) Å | T = 294 K |
β = 91.936 (7)° | Plate, colourless |
V = 264.48 (18) Å3 | 0.30 × 0.16 × 0.10 mm |
Z = 2 |
Bruker SMART CCD area-detector diffractometer | 571 independent reflections |
Radiation source: fine-focus sealed tube | 440 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.037 |
ϕ and ω scans | θmax = 26.5°, θmin = 3.2° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −4→4 |
Tmin = 0.962, Tmax = 0.988 | k = −14→6 |
1501 measured reflections | l = −7→7 |
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)] = 0.037 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.079 | H-atom parameters constrained |
S = 1.07 | w = 1/[σ2(Fo2) + (0.032P)2 + 0.0353P] where P = (Fo2 + 2Fc2)/3 |
571 reflections | (Δ/σ)max = 0.002 |
83 parameters | Δρmax = 0.14 e Å−3 |
1 restraint | Δρmin = −0.18 e Å−3 |
C5H4N2O2 | V = 264.48 (18) Å3 |
Mr = 124.10 | Z = 2 |
Monoclinic, P21 | Mo Kα radiation |
a = 3.7249 (14) Å | µ = 0.12 mm−1 |
b = 11.281 (4) Å | T = 294 K |
c = 6.298 (2) Å | 0.30 × 0.16 × 0.10 mm |
β = 91.936 (7)° |
Bruker SMART CCD area-detector diffractometer | 571 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 440 reflections with I > 2σ(I) |
Tmin = 0.962, Tmax = 0.988 | Rint = 0.037 |
1501 measured reflections |
R[F2 > 2σ(F2)] = 0.037 | 1 restraint |
wR(F2) = 0.079 | H-atom parameters constrained |
S = 1.07 | Δρmax = 0.14 e Å−3 |
571 reflections | Δρmin = −0.18 e Å−3 |
83 parameters |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
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 > σ(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 | ||
O1 | 0.5363 (7) | 0.1006 (2) | 0.4275 (3) | 0.0448 (7) | |
H1 | 0.6043 | 0.0385 | 0.3744 | 0.067* | |
O2 | 0.2901 (7) | −0.0206 (2) | 0.6633 (4) | 0.0514 (9) | |
N1 | 0.1339 (7) | 0.1712 (2) | 0.9153 (4) | 0.0389 (8) | |
N2 | 0.2844 (7) | 0.3970 (2) | 0.7595 (4) | 0.0354 (7) | |
C1 | 0.0647 (9) | 0.2716 (4) | 1.0242 (6) | 0.0405 (9) | |
H1A | −0.0381 | 0.2652 | 1.1563 | 0.049* | |
C2 | 0.1399 (8) | 0.3820 (3) | 0.9478 (5) | 0.0374 (8) | |
H2 | 0.0887 | 0.4482 | 1.0294 | 0.045* | |
C3 | 0.3559 (8) | 0.2983 (3) | 0.6483 (5) | 0.0343 (8) | |
H3 | 0.4584 | 0.3054 | 0.5163 | 0.041* | |
C4 | 0.2812 (9) | 0.1876 (3) | 0.7253 (6) | 0.0294 (7) | |
C5 | 0.3672 (9) | 0.0771 (3) | 0.6041 (5) | 0.0342 (8) |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0725 (16) | 0.0214 (11) | 0.0421 (14) | 0.0013 (13) | 0.0255 (12) | −0.0038 (11) |
O2 | 0.078 (2) | 0.0279 (14) | 0.0505 (17) | −0.0045 (15) | 0.0307 (16) | 0.0017 (13) |
N1 | 0.0465 (16) | 0.0352 (19) | 0.0357 (14) | 0.0023 (15) | 0.0104 (13) | 0.0031 (14) |
N2 | 0.0453 (15) | 0.0243 (16) | 0.0374 (16) | 0.0001 (13) | 0.0106 (13) | −0.0027 (12) |
C1 | 0.048 (2) | 0.043 (2) | 0.0310 (18) | 0.000 (2) | 0.0082 (16) | −0.0014 (18) |
C2 | 0.0439 (18) | 0.029 (2) | 0.0403 (19) | 0.0030 (18) | 0.0079 (15) | −0.0092 (17) |
C3 | 0.040 (2) | 0.0281 (19) | 0.0354 (19) | 0.0027 (18) | 0.0106 (15) | 0.0006 (16) |
C4 | 0.0336 (15) | 0.0261 (15) | 0.0289 (19) | −0.0013 (18) | 0.0058 (13) | −0.0004 (16) |
C5 | 0.0396 (19) | 0.0267 (19) | 0.0368 (19) | −0.0004 (18) | 0.0078 (14) | −0.0019 (16) |
O1—C5 | 1.324 (4) | C1—C2 | 1.368 (5) |
O1—H1 | 0.8200 | C1—H1A | 0.9300 |
O2—C5 | 1.201 (4) | C2—H2 | 0.9300 |
N1—C4 | 1.346 (4) | C3—C4 | 1.372 (5) |
N1—C1 | 1.354 (5) | C3—H3 | 0.9300 |
N2—C2 | 1.329 (4) | C4—C5 | 1.502 (4) |
N2—C3 | 1.346 (4) | ||
C5—O1—H1 | 109.5 | N2—C3—C4 | 121.5 (3) |
C4—N1—C1 | 115.2 (3) | N2—C3—H3 | 119.2 |
C2—N2—C3 | 116.9 (3) | C4—C3—H3 | 119.2 |
N1—C1—C2 | 122.6 (3) | N1—C4—C3 | 122.2 (3) |
N1—C1—H1A | 118.7 | N1—C4—C5 | 116.0 (3) |
C2—C1—H1A | 118.7 | C3—C4—C5 | 121.8 (3) |
N2—C2—C1 | 121.6 (3) | O2—C5—O1 | 124.8 (3) |
N2—C2—H2 | 119.2 | O2—C5—C4 | 123.1 (3) |
C1—C2—H2 | 119.2 | O1—C5—C4 | 112.1 (3) |
C4—N1—C1—C2 | −0.3 (5) | N2—C3—C4—N1 | −0.2 (5) |
C3—N2—C2—C1 | −0.5 (5) | N2—C3—C4—C5 | −178.7 (3) |
N1—C1—C2—N2 | 0.5 (6) | N1—C4—C5—O2 | 4.8 (4) |
C2—N2—C3—C4 | 0.4 (4) | C3—C4—C5—O2 | −176.5 (4) |
C1—N1—C4—C3 | 0.1 (4) | N1—C4—C5—O1 | −175.0 (3) |
C1—N1—C4—C5 | 178.7 (3) | C3—C4—C5—O1 | 3.6 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···N2i | 0.82 | 1.86 | 2.676 (3) | 175 |
C2—H2···O2ii | 0.93 | 2.46 | 3.168 (4) | 133 |
C3—H3···O1 | 0.93 | 2.40 | 2.725 (4) | 101 |
C3—H3···O2iii | 0.93 | 2.47 | 3.152 (4) | 131 |
Symmetry codes: (i) −x+1, y−1/2, −z+1; (ii) −x, y+1/2, −z+2; (iii) −x+1, y+1/2, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C5H4N2O2 |
Mr | 124.10 |
Crystal system, space group | Monoclinic, P21 |
Temperature (K) | 294 |
a, b, c (Å) | 3.7249 (14), 11.281 (4), 6.298 (2) |
β (°) | 91.936 (7) |
V (Å3) | 264.48 (18) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.12 |
Crystal size (mm) | 0.30 × 0.16 × 0.10 |
Data collection | |
Diffractometer | Bruker SMART CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.962, 0.988 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 1501, 571, 440 |
Rint | 0.037 |
(sin θ/λ)max (Å−1) | 0.628 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.037, 0.079, 1.07 |
No. of reflections | 571 |
No. of parameters | 83 |
No. of restraints | 1 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.14, −0.18 |
Computer programs: SMART (Bruker, 1997), SAINT (Bruker, 1997), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1997), SHELXTL.
O1—C5 | 1.324 (4) | N1—C1 | 1.354 (5) |
O2—C5 | 1.201 (4) | N2—C2 | 1.329 (4) |
N1—C4 | 1.346 (4) | N2—C3 | 1.346 (4) |
C4—N1—C1 | 115.2 (3) | C2—N2—C3 | 116.9 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···N2i | 0.82 | 1.86 | 2.676 (3) | 175 |
C2—H2···O2ii | 0.93 | 2.46 | 3.168 (4) | 133 |
C3—H3···O1 | 0.93 | 2.40 | 2.725 (4) | 101 |
C3—H3···O2iii | 0.93 | 2.47 | 3.152 (4) | 131 |
Symmetry codes: (i) −x+1, y−1/2, −z+1; (ii) −x, y+1/2, −z+2; (iii) −x+1, y+1/2, −z+1. |
Pyrazinic acid (pyrazine-2-carboxylic acid) is one of the most important materials for the preparation of pyrazine derivatives of pyrazinoyl chloride and pyrazinamide. Some pyrazine derivatives possess bacteriostatic activity. They are widely used in the treatment of tuberculosis and also exhibit fungicidal activity (Kushner et al., 1952). We have designed and synthesized a number of compounds for testing their effective antibacterial activity compared with that of pyrazinic acid. When recrystallizing a commercial impure batch of the title molecule, (I), we get single crystals of a new monoclinic polymorph for this compound.
The title compound, C5H4N2O2, crystallizes in space group P21 with the expected geometry (Table 1). The molecule is almost planar. A weak intramolecular hydrogen bond involves the C3/H3 and hydroxy groups (Fig. 1). Atom N2 of the pyrazine ring is connected to atom H1 of the hydroxy group, while atom H3 is linked to atom O2 of the carbonyl group (Table 2). As a result, molecules form zigzag chains along the [010] axis. Between two neighbouring zigzag chains, carboxylic O2 atoms interact with atoms H2 of the pyrazine rings to form C—H···O hydrogen bonds (Table 2). These hydrogen bonds further extend the one-dimensional zigzag chains along the bc plane, forming a quasi-two-dimensional network, as illustrated in Fig. 2.
In addition, face-to-face π–π stacking interactions are observed in the crystal, with a separation of ca 3.36 Å between the centroids of the pyrazine rings (Fig. 3). The complete crystal structure presents a different topology from that of the previously reported orthorhombic polymorph (Tukusagawa et al., 1974).