Abstract
In the crystal structure of the title compound, C6H7N2O2 +·NO3 −, the cations are linked via C—H⋯O hydrogen bonds, forming infinite chains running along the b axis. These chains are further linked through N—H⋯O, O—H⋯O and C—H⋯O hydrogen bonds to the nitrate anions, forming well-separated infinite planar layers parallel to (001).
Related literature
For hybrid compounds based on nicotinic acid, see: Athimoolam et al. (2005 ▶); Athimoolam & Rajaram (2005a
▶,b
▶); Chen (2009 ▶); Slouf (2001 ▶); Ye et al. (2010 ▶). For hybrid compounds based on amino-nicotinic acid derivatives, see: Akriche & Rzaigui (2007 ▶); Berrah et al. (2011a
▶); Giantsidis & Turnbull (2000 ▶). For related nitrate compounds, see: Berrah et al. (2011b
▶); Jebas et al. (2006 ▶).
Experimental
Crystal data
C6H7N2O2 +·NO3 −
M r = 201.15
Tetragonal,
a = 16.122 (2) Å
c = 12.446 (3) Å
V = 3235.0 (11) Å3
Z = 16
Mo Kα radiation
μ = 0.15 mm−1
T = 150 K
0.39 × 0.07 × 0.05 mm
Data collection
Bruker APEXII diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 2002 ▶) T min = 0.476, T max = 0.993
5438 measured reflections
1509 independent reflections
921 reflections with I > 2σ(I)
R int = 0.112
Refinement
R[F 2 > 2σ(F 2)] = 0.059
wR(F 2) = 0.158
S = 0.97
1509 reflections
128 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.41 e Å−3
Δρmin = −0.28 e Å−3
Data collection: APEX2 (Bruker, 2006 ▶); cell refinement: SAINT (Bruker, 2006 ▶); data reduction: SAINT; program(s) used to solve structure: SIR2002 (Burla et al., 2005 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶) and DIAMOND (Brandenburg & Berndt, 2001 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811027978/lx2193sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811027978/lx2193Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811027978/lx2193Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N2—H2⋯O3i | 0.86 | 1.97 | 2.803 (4) | 162 |
| N3—H3A⋯O2i | 0.86 | 2.18 | 3.017 (4) | 165 |
| N3—H3A⋯O2ii | 0.86 | 2.43 | 2.967 (4) | 121 |
| N3—H3B⋯O4 | 0.86 | 2.10 | 2.716 (5) | 128 |
| O5—H51⋯O3iii | 0.82 | 1.85 | 2.670 (4) | 180 |
| C4—H4⋯O1iv | 0.93 | 2.42 | 3.197 (6) | 141 |
| C5—H5⋯O4v | 0.93 | 2.30 | 3.216 (6) | 167 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
; (v)
.
Acknowledgments
We are grateful to the LCATM Laboratory, Université Larbi Ben M’hidi, Oum El Bouaghi, Algeria, for financial support.
supplementary crystallographic information
Comment
Crystal structures of hybrid compounds based on nicotinic acid or its amino derivatives and inorganic acids have been reported (Athimoolam et al., 2005; Athimoolam & Rajaram, 2005a, b; Chen, 2009; Giantsidis & Turnbull, 2000; Jebas et al., 2006; Slouf, 2001; Ye et al., 2010) showing interesting structural diversity governed mainly by hydrogen bonds. Anion substitution seems to have an important influence on hydrogen bound patterns. In attempt to elucidate this influence and as part of our search for new hybrid compounds based on protonated N-hyterocycle, we report in this paper the new structure of 2-aminonicotinium nitrate; its homologues obtained with phosphate and sulfate anions have been described previously (Akriche & Rzaigui, 2007; Berrah et al., 2011a).
The asymmetric unit of the title compound (Fig. 1) contains one cation and one anion with geometry similar to that observed in similar compounds (Akriche & Rzaigui, 2007; Berrah et al., 2011a, b; Jebas et al., 2006). However in this structure, cations do not form dimers via N–H···O hydrogen bonds as observed in the structures obtained with phosphate and sulfate anions but they are linked to each other via C–H···O hydrogen bonds to form infinite chains running along the b axis (Table 1 & Fig. 2,). These chains are further linked, through N–H···O, O–H···O and C–H···O hydrogen contacts, to nitrate anions to form well separated infinite planar layers parallel to (001) (Fig. 3). A such two-dimensional network have been already observed in compounds including nicotinium entities (Giantsidis & Turnbull, 2000; Slouf, 2001; Ye et al., 2010).
Experimental
The title compound was synthesized by reacting 3-amino-pyridine-2-carboxylic acid (0.138 mg, 1 mmol) with nitriic acid (1 mmol)in a solution of equal volume of H2O and CH3OH. Slow evaporation leads to well crystallized colourless needles.
Refinement
All the Friedel pairs were merged. All non-H atoms were refined with anisotropic atomic displacement parameters. The remaining H atoms were localized on Fourier maps but introduced in calculated positions and treated as riding on their parent atoms (C, N or O) with C–H = 0.93 Å, O–H = 0.82 Å and N–H = 0.86 Å with Uiso(H) = 1.2 Ueq(C or N) and Uiso(H = 1.5 Ueq(O).
Figures
Fig. 1.
The structure of the title compound with the atomic labelling scheme. Displacement are drawn at the 50% probability level.
Fig. 2.
A part of crystal packing showing cationic infinite chains linked to nitrate anions via [N–H···O, O–H···O and C–H···O] hydrogen contacts. Hydrogen bonds are shown as dashed lines. [Symmetry codes: (i) y + 1/2, -x, z - 1/4; (ii) -y + 1/2, x, z - 1/4; (iii) -y, -x + 1/2, z - 1/4; (iv) y, x - 1/2, z - 1/4; (v) -x + 1/2, y - 1/2, z.]
Fig. 3.
Layered packing of the structure viewed down the b axis.
Crystal data
| C6H7N2O2+·NO3− | Dx = 1.652 Mg m−3 |
| Mr = 201.15 | Mo Kα radiation, λ = 0.71073 Å |
| Tetragonal, I41cd | Cell parameters from 491 reflections |
| Hall symbol: I 4bw -2c | θ = 3.3–20.3° |
| a = 16.122 (2) Å | µ = 0.15 mm−1 |
| c = 12.446 (3) Å | T = 150 K |
| V = 3235.0 (11) Å3 | Needle, colourless |
| Z = 16 | 0.39 × 0.07 × 0.05 mm |
| F(000) = 1664 |
Data collection
| Bruker APEXII diffractometer | 921 reflections with I > 2σ(I) |
| graphite | Rint = 0.112 |
| CCD rotation images, thin slices scans | θmax = 27.5°, θmin = 3.3° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 2002) | h = −16→20 |
| Tmin = 0.476, Tmax = 0.993 | k = −13→20 |
| 5438 measured reflections | l = −16→10 |
| 1509 independent reflections |
Refinement
| 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)] = 0.059 | Hydrogen site location: difference Fourier map |
| wR(F2) = 0.158 | H-atom parameters constrained |
| S = 0.97 | w = 1/[σ2(Fo2) + (0.076P)2] where P = (Fo2 + 2Fc2)/3 |
| 1509 reflections | (Δ/σ)max < 0.001 |
| 128 parameters | Δρmax = 0.41 e Å−3 |
| 1 restraint | Δρmin = −0.28 e Å−3 |
Special details
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| C1 | 0.1754 (3) | 0.1137 (3) | 0.0309 (6) | 0.0288 (11) | |
| C2 | 0.1875 (3) | 0.0223 (2) | 0.0276 (6) | 0.0229 (10) | |
| C3 | 0.1218 (3) | −0.0300 (3) | 0.0259 (6) | 0.0295 (12) | |
| H3 | 0.0686 | −0.0078 | 0.0264 | 0.035* | |
| C4 | 0.1311 (3) | −0.1174 (3) | 0.0233 (7) | 0.0309 (11) | |
| H4 | 0.0854 | −0.1526 | 0.0215 | 0.037* | |
| C5 | 0.2092 (3) | −0.1469 (3) | 0.0235 (7) | 0.0302 (12) | |
| H5 | 0.2179 | −0.2039 | 0.0221 | 0.036* | |
| C6 | 0.2702 (2) | −0.0099 (3) | 0.0279 (10) | 0.0234 (10) | |
| N1 | 0.1623 (2) | −0.0149 (2) | 0.2777 (8) | 0.0247 (8) | |
| N2 | 0.2755 (2) | −0.0950 (2) | 0.0256 (5) | 0.0269 (9) | |
| H2 | 0.3242 | −0.1168 | 0.0256 | 0.032* | |
| N3 | 0.3388 (2) | 0.0327 (2) | 0.0312 (5) | 0.0308 (10) | |
| H3A | 0.3858 | 0.0075 | 0.032 | 0.037* | |
| H3B | 0.3371 | 0.086 | 0.0326 | 0.037* | |
| O1 | 0.20156 (19) | 0.05016 (19) | 0.2755 (4) | 0.0313 (8) | |
| O2 | 0.08451 (16) | −0.01536 (18) | 0.2757 (5) | 0.0293 (8) | |
| O3 | 0.19907 (18) | −0.08530 (18) | 0.2798 (5) | 0.0309 (8) | |
| O5 | 0.09671 (19) | 0.13575 (18) | 0.0242 (4) | 0.0342 (9) | |
| H51 | 0.0932 | 0.1865 | 0.0259 | 0.051* | |
| O4 | 0.2318 (2) | 0.1628 (2) | 0.0360 (4) | 0.0355 (10) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.035 (3) | 0.017 (2) | 0.035 (3) | −0.002 (2) | −0.001 (4) | −0.004 (3) |
| C2 | 0.020 (2) | 0.021 (3) | 0.028 (2) | 0.0022 (16) | 0.001 (3) | 0.002 (4) |
| C3 | 0.025 (3) | 0.021 (2) | 0.042 (3) | −0.0068 (19) | 0.000 (4) | 0.003 (3) |
| C4 | 0.042 (3) | 0.016 (3) | 0.035 (3) | −0.001 (2) | −0.003 (5) | 0.000 (3) |
| C5 | 0.040 (3) | 0.014 (2) | 0.036 (3) | −0.014 (2) | −0.004 (4) | −0.001 (4) |
| C6 | 0.022 (2) | 0.026 (3) | 0.022 (2) | −0.0025 (18) | −0.006 (5) | 0.003 (3) |
| N1 | 0.0198 (18) | 0.020 (2) | 0.0341 (18) | −0.0058 (16) | 0.006 (4) | −0.001 (4) |
| N2 | 0.024 (2) | 0.022 (2) | 0.035 (2) | 0.0103 (15) | −0.005 (3) | −0.002 (3) |
| N3 | 0.0137 (19) | 0.029 (2) | 0.050 (2) | −0.0035 (15) | 0.003 (3) | 0.002 (3) |
| O1 | 0.0253 (18) | 0.0256 (17) | 0.043 (2) | −0.0062 (15) | 0.000 (3) | −0.006 (3) |
| O2 | 0.0124 (15) | 0.0231 (18) | 0.052 (2) | 0.0030 (13) | 0.004 (3) | 0.004 (3) |
| O3 | 0.0130 (16) | 0.0233 (17) | 0.056 (2) | 0.0049 (13) | −0.002 (3) | −0.007 (3) |
| O5 | 0.0233 (17) | 0.0205 (19) | 0.059 (2) | 0.0042 (14) | 0.004 (3) | 0.000 (3) |
| O4 | 0.0253 (19) | 0.0212 (18) | 0.060 (3) | 0.0027 (15) | −0.003 (3) | −0.005 (3) |
Geometric parameters (Å, °)
| C1—O4 | 1.207 (6) | C5—H5 | 0.93 |
| C1—O5 | 1.319 (6) | C6—N3 | 1.303 (5) |
| C1—C2 | 1.487 (6) | C6—N2 | 1.375 (6) |
| C2—C3 | 1.354 (6) | N1—O1 | 1.225 (4) |
| C2—C6 | 1.431 (5) | N1—O2 | 1.255 (4) |
| C3—C4 | 1.417 (6) | N1—O3 | 1.281 (4) |
| C3—H3 | 0.93 | N2—H2 | 0.86 |
| C4—C5 | 1.347 (8) | N3—H3A | 0.86 |
| C4—H4 | 0.93 | N3—H3B | 0.86 |
| C5—N2 | 1.359 (6) | O5—H51 | 0.82 |
| O4—C1—O5 | 123.4 (4) | N2—C5—H5 | 119.4 |
| O4—C1—C2 | 123.5 (4) | N3—C6—N2 | 118.2 (4) |
| O5—C1—C2 | 113.0 (4) | N3—C6—C2 | 126.9 (5) |
| C3—C2—C6 | 120.2 (4) | N2—C6—C2 | 114.8 (4) |
| C3—C2—C1 | 121.0 (4) | O1—N1—O2 | 121.4 (4) |
| C6—C2—C1 | 118.8 (4) | O1—N1—O3 | 121.4 (3) |
| C2—C3—C4 | 122.5 (4) | O2—N1—O3 | 117.2 (3) |
| C2—C3—H3 | 118.8 | C5—N2—C6 | 124.5 (4) |
| C4—C3—H3 | 118.8 | C5—N2—H2 | 117.8 |
| C5—C4—C3 | 116.8 (4) | C6—N2—H2 | 117.8 |
| C5—C4—H4 | 121.6 | C6—N3—H3A | 120 |
| C3—C4—H4 | 121.6 | C6—N3—H3B | 120 |
| C4—C5—N2 | 121.2 (4) | H3A—N3—H3B | 120 |
| C4—C5—H5 | 119.4 | C1—O5—H51 | 109.5 |
| O4—C1—C2—C3 | 177.5 (7) | C3—C2—C6—N3 | −178.8 (9) |
| O5—C1—C2—C3 | −4.4 (11) | C1—C2—C6—N3 | 0.4 (17) |
| O4—C1—C2—C6 | −1.6 (13) | C3—C2—C6—N2 | 0.3 (14) |
| O5—C1—C2—C6 | 176.4 (9) | C1—C2—C6—N2 | 179.5 (7) |
| C6—C2—C3—C4 | −0.6 (12) | C4—C5—N2—C6 | 0.0 (14) |
| C1—C2—C3—C4 | −179.7 (7) | N3—C6—N2—C5 | 179.1 (8) |
| C2—C3—C4—C5 | 0.5 (11) | C2—C6—N2—C5 | −0.1 (15) |
| C3—C4—C5—N2 | −0.3 (12) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2···O3i | 0.86 | 1.97 | 2.803 (4) | 162 |
| N3—H3A···O2i | 0.86 | 2.18 | 3.017 (4) | 165 |
| N3—H3A···O2ii | 0.86 | 2.43 | 2.967 (4) | 121 |
| N3—H3B···O4 | 0.86 | 2.10 | 2.716 (5) | 128 |
| O5—H51···O3iii | 0.82 | 1.85 | 2.670 (4) | 180 |
| C4—H4···O1iv | 0.93 | 2.42 | 3.197 (6) | 141 |
| C5—H5···O4v | 0.93 | 2.30 | 3.216 (6) | 167 |
Symmetry codes: (i) y+1/2, −x, z−1/4; (ii) −y+1/2, x, z−1/4; (iii) −y, −x+1/2, z−1/4; (iv) y, x−1/2, z−1/4; (v) −x+1/2, y−1/2, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LX2193).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811027978/lx2193sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811027978/lx2193Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811027978/lx2193Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



