Abstract
In the crystal structure of the title compound, C5H6N3O2 +·H2PO4 −, the dihydrogen phosphate anions are linked through short O—H⋯O hydrogen bonds, forming infinite double chains running parallel to the b axis. Centrosymetric N—H⋯O hydrogen-bonded cationic dimers form bridges between these chains by means of intermolecular N—H⋯O and O—H⋯O hydrogen bonds, leading to a two-dimensional network parallel to (100) in which R 3 3(12), R 4 3(10) R 2 2(8) and C(4) graph-set motifs are generated. Weak intermolecular C—H⋯O hydrogen bonds connect these layers, forming a three-dimensional network.
Related literature
For hybrid compounds based on N-heterocycles, see: Akriche & Rzaigui (2007 ▶); Berrah et al. (2011a
▶,b
▶,c
▶); Ouakkaf et al. (2011 ▶). For related dihydrogenphosphte compounds, see: Lin et al. (2009 ▶); Shao et al. (2010 ▶). For hydrogen-bond motifs, see: Bernstein et al. (1995 ▶); Etter et al. (1990 ▶).
Experimental
Crystal data
C5H6N3O2 +·H2PO4 −
M r = 237.11
Monoclinic,
a = 8.6076 (5) Å
b = 4.6703 (3) Å
c = 21.9431 (13) Å
β = 95.573 (2)°
V = 877.94 (9) Å3
Z = 4
Mo Kα radiation
μ = 0.33 mm−1
T = 150 K
0.45 × 0.06 × 0.04 mm
Data collection
Bruker APEXII diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 2002 ▶) T min = 0.898, T max = 0.987
7993 measured reflections
2004 independent reflections
1781 reflections with I > 2σ(I)
R int = 0.025
Refinement
R[F 2 > 2σ(F 2)] = 0.028
wR(F 2) = 0.079
S = 1.04
2004 reflections
139 parameters
H-atom parameters constrained
Δρmax = 0.39 e Å−3
Δρmin = −0.39 e Å−3
Data collection: APEX2 (Bruker, 2001 ▶); cell refinement: SAINT (Bruker, 2001 ▶); 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 datablocks global, I. DOI: 10.1107/S1600536811017521/lh5248sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811017521/lh5248Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811017521/lh5248Isup3.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 |
|---|---|---|---|---|
| N1—H1A⋯O14 | 0.88 | 1.94 | 2.8171 (17) | 171 |
| N1—H1B⋯O9 | 0.88 | 2.09 | 2.7275 (17) | 128 |
| N1—H1B⋯O9i | 0.88 | 2.37 | 3.0640 (19) | 136 |
| N3—H3⋯O11 | 0.88 | 1.79 | 2.6690 (16) | 173 |
| O10—H10⋯O13ii | 0.84 | 1.83 | 2.6591 (16) | 169 |
| O12—H12⋯O11iii | 0.84 | 1.72 | 2.5386 (14) | 166 |
| O13—H13⋯O14iv | 0.84 | 1.64 | 2.4634 (16) | 164 |
| C4—H4⋯O11v | 0.95 | 2.43 | 3.3377 (19) | 160 |
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
In continuation of our search for new hybrids based on protonated N-heterocyclic compounds and inorganic acids we have prepared the title compound. Our recent investigation in this field has revealed the ability of N-heterocyclic derivatives to generate original networks stabilized by hydrogen bonds and has shown how anion substitution may influence the hydrogen-bonding patterns (Berrah et al., 2011a,b,c; Ouakkaf et al., 2011).
The asymmetric unit of the title conpound compound contains one 2-amino-3-carboxypyrazin-1-ium cation and one dihydrogen phosphate anion (Fig. 1). Both entities display geometry similar to that reported in related compounds (Akriche & Rzaigui 2007; Berrah et al., 2011b; Shao et al., 2010). dihydrogen phosphate anions linked through strong O—H···O hydrogen bonds (Table 1), form double infinite chains running parallel to the b axis (Fig. 2). Similar chains were previously observed in related compounds (Akriche & Rzaigui 2007; Lin et al., 2009). 2-Amino-3-carboxypyrazin-1-ium centrosymetric dimers form bridges between these chains by means of N—H···O and O—H···O hydrogen bonds (Fig. 3) leading to a two-dimensional network (Fig. 4) where R33(12), R34(10), R22(8) and C(4) graph-set motifs are generated (Fig. 2 and Fig. 3)(Etter et al., 1990; Bernstein et al., 1995). Further stabilization is provided by intermolecular C—H···O contacts.
Experimental
The title compound was synthesized by reacting 3-amino-pyrazine-2-carboxylic acid with phosphoricic acid in a solution of equal volume of H2O and CH3OH. Slow evaporation leads to well crystallized colourless needles.
Refinement
H atoms were located in Fourier maps but introduced in calculated positions and treated as riding on their parent atoms (C, N or O) with C—H = 0.95 Å, O—H = 0.84 Å and N—H = 0.88 Å with Uiso(H) = 1.2 Ueq(C or N) and Uiso(H = 1.5 Ueq(O).
Figures
Fig. 1.
The asymmetric unit of the title compound. Displacement are drawn at the 50% probability level. Hydrogen bonds are shown as dashed lines.
Fig. 2.
Part of the crystal structure viewed along [001] showing infinite double chains. Hydrogen bonds are shown as dashed lines.
Fig. 3.
A view parallel to (010) showing cationic dimers and how they link double infinite anionic chains. C—H···O contacts have been omitted for clarity.
Fig. 4.
The two-dimensional packing. Hydrogen bonds are shown as dashed lines.
Crystal data
| C5H6N3O2+·H2PO4− | F(000) = 488 |
| Mr = 237.11 | Dx = 1.794 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 4062 reflections |
| a = 8.6076 (5) Å | θ = 3.2–27.5° |
| b = 4.6703 (3) Å | µ = 0.33 mm−1 |
| c = 21.9431 (13) Å | T = 150 K |
| β = 95.573 (2)° | Needle, colourless |
| V = 877.94 (9) Å3 | 0.45 × 0.06 × 0.04 mm |
| Z = 4 |
Data collection
| Bruker APEXII diffractometer | 1781 reflections with I > 2σ(I) |
| graphite | Rint = 0.025 |
| CCD rotation images, thin slices scans | θmax = 27.5°, θmin = 3.2° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 2002) | h = −11→7 |
| Tmin = 0.898, Tmax = 0.987 | k = −6→6 |
| 7993 measured reflections | l = −28→28 |
| 2004 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)] = 0.028 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.079 | H-atom parameters constrained |
| S = 1.04 | w = 1/[σ2(Fo2) + (0.0383P)2 + 0.6558P] where P = (Fo2 + 2Fc2)/3 |
| 2004 reflections | (Δ/σ)max = 0.001 |
| 139 parameters | Δρmax = 0.39 e Å−3 |
| 0 restraints | Δρmin = −0.39 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 | ||
| N1 | 0.86142 (15) | 0.8016 (3) | 0.90992 (6) | 0.0173 (3) | |
| H1A | 0.8733 | 0.8741 | 0.8736 | 0.021* | |
| H1B | 0.9191 | 0.8645 | 0.9425 | 0.021* | |
| C2 | 0.75718 (17) | 0.5988 (3) | 0.91547 (6) | 0.0137 (3) | |
| N3 | 0.66953 (15) | 0.5047 (3) | 0.86483 (5) | 0.0149 (3) | |
| H3 | 0.6834 | 0.583 | 0.8293 | 0.018* | |
| C4 | 0.56229 (17) | 0.2967 (3) | 0.86666 (7) | 0.0165 (3) | |
| H4 | 0.5045 | 0.2339 | 0.83 | 0.02* | |
| C5 | 0.53675 (17) | 0.1756 (3) | 0.92166 (7) | 0.0171 (3) | |
| H5 | 0.4608 | 0.0288 | 0.923 | 0.02* | |
| N6 | 0.61838 (15) | 0.2626 (3) | 0.97404 (6) | 0.0166 (3) | |
| C7 | 0.72487 (17) | 0.4646 (3) | 0.97204 (6) | 0.0142 (3) | |
| C8 | 0.81279 (17) | 0.5559 (3) | 1.03115 (7) | 0.0155 (3) | |
| O9 | 0.91059 (13) | 0.7446 (2) | 1.03400 (5) | 0.0214 (3) | |
| O10 | 0.77252 (13) | 0.4096 (3) | 1.07821 (5) | 0.0212 (3) | |
| H10 | 0.8219 | 0.4712 | 1.1104 | 0.032* | |
| P1 | 0.79097 (4) | 0.97152 (8) | 0.740127 (16) | 0.01125 (11) | |
| O11 | 0.70388 (12) | 0.7004 (2) | 0.75265 (5) | 0.0161 (2) | |
| O12 | 0.66950 (12) | 1.1937 (2) | 0.71167 (5) | 0.0162 (2) | |
| H12 | 0.696 | 1.3588 | 0.7238 | 0.024* | |
| O13 | 0.89962 (12) | 0.9251 (2) | 0.68787 (5) | 0.0183 (2) | |
| H13 | 0.9697 | 0.8065 | 0.6994 | 0.027* | |
| O14 | 0.88101 (12) | 1.0854 (2) | 0.79764 (5) | 0.0158 (2) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N1 | 0.0199 (6) | 0.0194 (7) | 0.0125 (6) | −0.0029 (5) | 0.0013 (5) | 0.0017 (5) |
| C2 | 0.0139 (7) | 0.0139 (7) | 0.0134 (6) | 0.0041 (5) | 0.0019 (5) | −0.0008 (5) |
| N3 | 0.0177 (6) | 0.0157 (6) | 0.0113 (6) | 0.0025 (5) | 0.0013 (5) | 0.0010 (5) |
| C4 | 0.0150 (7) | 0.0166 (7) | 0.0173 (7) | 0.0029 (6) | −0.0014 (6) | −0.0021 (6) |
| C5 | 0.0141 (7) | 0.0177 (7) | 0.0193 (7) | −0.0006 (6) | 0.0015 (6) | −0.0016 (6) |
| N6 | 0.0160 (6) | 0.0182 (6) | 0.0158 (6) | 0.0017 (5) | 0.0027 (5) | 0.0000 (5) |
| C7 | 0.0144 (7) | 0.0160 (7) | 0.0123 (6) | 0.0027 (5) | 0.0020 (5) | −0.0003 (5) |
| C8 | 0.0160 (7) | 0.0172 (7) | 0.0135 (7) | 0.0028 (6) | 0.0023 (5) | −0.0006 (5) |
| O9 | 0.0245 (6) | 0.0223 (6) | 0.0168 (5) | −0.0050 (5) | −0.0003 (4) | −0.0013 (4) |
| O10 | 0.0233 (6) | 0.0296 (6) | 0.0106 (5) | −0.0056 (5) | 0.0011 (4) | 0.0010 (4) |
| P1 | 0.01218 (19) | 0.01066 (18) | 0.01087 (18) | 0.00067 (13) | 0.00093 (13) | −0.00036 (13) |
| O11 | 0.0213 (5) | 0.0112 (5) | 0.0156 (5) | −0.0021 (4) | 0.0010 (4) | −0.0006 (4) |
| O12 | 0.0158 (5) | 0.0107 (5) | 0.0212 (5) | 0.0021 (4) | −0.0025 (4) | −0.0026 (4) |
| O13 | 0.0182 (5) | 0.0239 (6) | 0.0132 (5) | 0.0094 (4) | 0.0034 (4) | 0.0031 (4) |
| O14 | 0.0168 (5) | 0.0181 (5) | 0.0121 (5) | −0.0043 (4) | 0.0004 (4) | 0.0003 (4) |
Geometric parameters (Å, °)
| N1—C2 | 1.319 (2) | N6—C7 | 1.319 (2) |
| N1—H1A | 0.88 | C7—C8 | 1.4987 (19) |
| N1—H1B | 0.88 | C8—O9 | 1.2161 (19) |
| C2—N3 | 1.3543 (18) | C8—O10 | 1.3127 (18) |
| C2—C7 | 1.442 (2) | O10—H10 | 0.84 |
| N3—C4 | 1.343 (2) | P1—O11 | 1.5101 (11) |
| N3—H3 | 0.88 | P1—O14 | 1.5120 (10) |
| C4—C5 | 1.370 (2) | P1—O12 | 1.5597 (11) |
| C4—H4 | 0.95 | P1—O13 | 1.5636 (11) |
| C5—N6 | 1.3503 (19) | O12—H12 | 0.84 |
| C5—H5 | 0.95 | O13—H13 | 0.84 |
| C2—N1—H1A | 120 | N6—C7—C2 | 122.16 (13) |
| C2—N1—H1B | 120 | N6—C7—C8 | 117.96 (13) |
| H1A—N1—H1B | 120 | C2—C7—C8 | 119.88 (13) |
| N1—C2—N3 | 119.16 (13) | O9—C8—O10 | 124.84 (14) |
| N1—C2—C7 | 125.57 (13) | O9—C8—C7 | 122.65 (14) |
| N3—C2—C7 | 115.26 (13) | O10—C8—C7 | 112.51 (13) |
| C4—N3—C2 | 122.68 (13) | C8—O10—H10 | 109.5 |
| C4—N3—H3 | 118.7 | O11—P1—O14 | 111.49 (6) |
| C2—N3—H3 | 118.7 | O11—P1—O12 | 107.77 (6) |
| N3—C4—C5 | 119.62 (14) | O14—P1—O12 | 111.69 (6) |
| N3—C4—H4 | 120.2 | O11—P1—O13 | 111.11 (6) |
| C5—C4—H4 | 120.2 | O14—P1—O13 | 111.48 (6) |
| N6—C5—C4 | 120.73 (14) | O12—P1—O13 | 102.94 (6) |
| N6—C5—H5 | 119.6 | P1—O12—H12 | 109.5 |
| C4—C5—H5 | 119.6 | P1—O13—H13 | 109.5 |
| C7—N6—C5 | 119.53 (13) | ||
| N1—C2—N3—C4 | 179.23 (13) | N3—C2—C7—N6 | 0.6 (2) |
| C7—C2—N3—C4 | −1.4 (2) | N1—C2—C7—C8 | 0.5 (2) |
| C2—N3—C4—C5 | 1.2 (2) | N3—C2—C7—C8 | −178.86 (12) |
| N3—C4—C5—N6 | −0.1 (2) | N6—C7—C8—O9 | −178.37 (14) |
| C4—C5—N6—C7 | −0.6 (2) | C2—C7—C8—O9 | 1.1 (2) |
| C5—N6—C7—C2 | 0.4 (2) | N6—C7—C8—O10 | 1.9 (2) |
| C5—N6—C7—C8 | 179.86 (13) | C2—C7—C8—O10 | −178.58 (13) |
| N1—C2—C7—N6 | 179.93 (14) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···O14 | 0.88 | 1.94 | 2.8171 (17) | 171 |
| N1—H1B···O9 | 0.88 | 2.09 | 2.7275 (17) | 128 |
| N1—H1B···O9i | 0.88 | 2.37 | 3.0640 (19) | 136 |
| N3—H3···O11 | 0.88 | 1.79 | 2.6690 (16) | 173 |
| O10—H10···O13ii | 0.84 | 1.83 | 2.6591 (16) | 169 |
| O12—H12···O11iii | 0.84 | 1.72 | 2.5386 (14) | 166 |
| O13—H13···O14iv | 0.84 | 1.64 | 2.4634 (16) | 164 |
| C4—H4···O11v | 0.95 | 2.43 | 3.3377 (19) | 160 |
Symmetry codes: (i) −x+2, −y+2, −z+2; (ii) x, −y+3/2, z+1/2; (iii) x, y+1, z; (iv) −x+2, y−1/2, −z+3/2; (v) −x+1, y−1/2, −z+3/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5248).
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 datablocks global, I. DOI: 10.1107/S1600536811017521/lh5248sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811017521/lh5248Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811017521/lh5248Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report




