organic compounds
Oxalic acid–pyridine-4-carbonitrile (1/2)
aCollege of Chemistry and Chemical Engineering, Southeast University, Nanjing 210096, People's Republic of China
*Correspondence e-mail: chenxinyuanseu@yahoo.com.cn
In the title compound, 2C6H4N2·C2H2O4, the oxalic acid molecule lies about an inversion center. The pyridine ring of the pyridine-4-carbonitrile molecule is almost planar, the largest deviation from the least-squares plane being 0.006 (1) Å; the nitrile N atom deviates from this plane by 0.114 (1) Å. In the crystal, the oxalic acid molecules and the pyridine-4-carbonitrile molecules form stacks. Neighboring molecules within the stacks are related by translation in the a direction, with interplanar distances of 3.183 (1) and 3.331 (2) Å, respectively. Each oxalic acid molecule forms strong O—H⋯N hydrogen bonds with two molecules of pyridine-4-carbonitrile. Besides this, there are also weak C—H⋯O interactions.
Related literature
For the structures and ferroelectric properties of related compounds, see: Fu et al. (2011a,b,c); Dai & Chen (2011); Xu et al. (2011); Zheng (2011). For standard bond lengths, see: Allen et al. (1987).
Experimental
Crystal data
|
Refinement
|
Data collection: CrystalClear (Rigaku, 2005); cell CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.
Supporting information
10.1107/S1600536812019137/yk2054sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812019137/yk2054Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812019137/yk2054Isup3.cml
The oxalic acid (10 mmol), pyridine-4-carbonitrile (20 mmol) and ethanol (50 mL) were put into a 100mL flask. The mixture was stirred at 60°C for 2 h, and then the precipitate was filtered off. Colourless crystals suitable for X-ray diffraction were obtained by slow evaporation of the solution.
All the H atoms attached to C atoms were placed into the idealized positions and treated as riding with C—H = 0.93 Å and with Uiso(H)=1.2Ueq(C). The positional parameters of the H atom attached to oxygen were refined freely, and at the last stage of the
they were restrained with the H—O = 0.82 (2)Å and with Uiso(H)=1.5Ueq(O).Data collection: CrystalClear (Rigaku, 2005); cell
CrystalClear (Rigaku, 2005); data reduction: CrystalClear (Rigaku, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).C6H4N2·0.5C2H2O4 | Z = 2 |
Mr = 149.13 | F(000) = 154 |
Triclinic, P1 | Dx = 1.469 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 3.6842 (6) Å | Cell parameters from 1528 reflections |
b = 7.5816 (5) Å | θ = 2.9–27.5° |
c = 12.4511 (1) Å | µ = 0.11 mm−1 |
α = 78.258 (1)° | T = 298 K |
β = 85.301 (1)° | Block, colourless |
γ = 82.547 (1)° | 0.10 × 0.03 × 0.03 mm |
V = 337.08 (6) Å3 |
Rigaku SCXmini Mercury2 diffractometer | 1528 independent reflections |
Radiation source: fine-focus sealed tube | 1268 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.024 |
Detector resolution: 13.6612 pixels mm-1 | θmax = 27.5°, θmin = 2.9° |
ω scans CCD profile fitting | h = −4→4 |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −9→9 |
Tmin = 0.910, Tmax = 1.000 | l = −16→16 |
3634 measured reflections |
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)] = 0.036 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.101 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | w = 1/[σ2(Fo2) + (0.065P)2] where P = (Fo2 + 2Fc2)/3 |
1528 reflections | (Δ/σ)max < 0.001 |
103 parameters | Δρmax = 0.46 e Å−3 |
1 restraint | Δρmin = −0.27 e Å−3 |
C6H4N2·0.5C2H2O4 | γ = 82.547 (1)° |
Mr = 149.13 | V = 337.08 (6) Å3 |
Triclinic, P1 | Z = 2 |
a = 3.6842 (6) Å | Mo Kα radiation |
b = 7.5816 (5) Å | µ = 0.11 mm−1 |
c = 12.4511 (1) Å | T = 298 K |
α = 78.258 (1)° | 0.10 × 0.03 × 0.03 mm |
β = 85.301 (1)° |
Rigaku SCXmini Mercury2 diffractometer | 1528 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | 1268 reflections with I > 2σ(I) |
Tmin = 0.910, Tmax = 1.000 | Rint = 0.024 |
3634 measured reflections |
R[F2 > 2σ(F2)] = 0.036 | 1 restraint |
wR(F2) = 0.101 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | Δρmax = 0.46 e Å−3 |
1528 reflections | Δρmin = −0.27 e Å−3 |
103 parameters |
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2sigma(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 | 0.8019 (2) | 0.10266 (10) | 0.37597 (6) | 0.0195 (2) | |
H1 | 0.753 (4) | 0.2095 (6) | 0.3465 (11) | 0.029* | |
O2 | 1.0250 (2) | 0.22804 (10) | 0.50208 (6) | 0.0196 (2) | |
N1 | 0.6137 (3) | 0.43796 (12) | 0.27800 (8) | 0.0157 (2) | |
N2 | 0.1419 (3) | 1.12502 (13) | 0.09513 (8) | 0.0207 (2) | |
C4 | 0.5310 (3) | 0.75440 (15) | 0.28546 (9) | 0.0147 (3) | |
H4A | 0.5545 | 0.8461 | 0.3231 | 0.018* | |
C1 | 0.4759 (3) | 0.47781 (15) | 0.17793 (9) | 0.0158 (3) | |
H1A | 0.4592 | 0.3835 | 0.1417 | 0.019* | |
C3 | 0.3848 (3) | 0.79346 (14) | 0.18234 (9) | 0.0141 (3) | |
C5 | 0.6404 (3) | 0.57355 (15) | 0.33014 (9) | 0.0152 (3) | |
H5A | 0.7362 | 0.5455 | 0.3992 | 0.018* | |
C2 | 0.3578 (3) | 0.65365 (14) | 0.12654 (9) | 0.0150 (3) | |
H2A | 0.2638 | 0.6777 | 0.0573 | 0.018* | |
C6 | 0.2532 (3) | 0.97886 (14) | 0.13355 (9) | 0.0161 (3) | |
C7 | 0.9557 (3) | 0.09891 (14) | 0.46785 (8) | 0.0140 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0299 (5) | 0.0114 (4) | 0.0174 (4) | −0.0004 (3) | −0.0102 (4) | −0.0010 (3) |
O2 | 0.0269 (5) | 0.0140 (4) | 0.0189 (4) | −0.0026 (3) | −0.0066 (3) | −0.0033 (3) |
N1 | 0.0164 (5) | 0.0147 (5) | 0.0158 (5) | −0.0021 (4) | −0.0022 (4) | −0.0020 (4) |
N2 | 0.0244 (6) | 0.0171 (5) | 0.0210 (5) | −0.0016 (4) | −0.0067 (4) | −0.0029 (4) |
C4 | 0.0142 (5) | 0.0151 (5) | 0.0159 (5) | −0.0027 (4) | −0.0002 (4) | −0.0049 (4) |
C1 | 0.0169 (6) | 0.0153 (5) | 0.0164 (5) | −0.0030 (4) | −0.0017 (4) | −0.0048 (4) |
C3 | 0.0118 (5) | 0.0130 (5) | 0.0167 (5) | −0.0018 (4) | −0.0004 (4) | −0.0011 (4) |
C5 | 0.0157 (5) | 0.0169 (6) | 0.0131 (5) | −0.0027 (4) | −0.0025 (4) | −0.0019 (4) |
C2 | 0.0156 (6) | 0.0169 (6) | 0.0126 (5) | −0.0025 (4) | −0.0023 (4) | −0.0024 (4) |
C6 | 0.0162 (6) | 0.0177 (6) | 0.0155 (5) | −0.0043 (4) | −0.0014 (4) | −0.0042 (4) |
C7 | 0.0144 (5) | 0.0143 (5) | 0.0131 (5) | −0.0010 (4) | −0.0012 (4) | −0.0024 (4) |
O1—C7 | 1.3113 (12) | C4—H4A | 0.9300 |
O1—H1 | 0.822 (2) | C1—C2 | 1.3871 (15) |
O2—C7 | 1.2075 (13) | C1—H1A | 0.9300 |
N1—C5 | 1.3403 (14) | C3—C2 | 1.3981 (15) |
N1—C1 | 1.3462 (13) | C3—C6 | 1.4505 (14) |
N2—C6 | 1.1503 (14) | C5—H5A | 0.9300 |
C4—C5 | 1.3910 (15) | C2—H2A | 0.9300 |
C4—C3 | 1.3940 (14) | C7—C7i | 1.557 (2) |
C7—O1—H1 | 107.8 (11) | N1—C5—C4 | 122.85 (10) |
C5—N1—C1 | 118.83 (9) | N1—C5—H5A | 118.6 |
C5—C4—C3 | 117.70 (10) | C4—C5—H5A | 118.6 |
C5—C4—H4A | 121.1 | C1—C2—C3 | 117.75 (10) |
C3—C4—H4A | 121.1 | C1—C2—H2A | 121.1 |
N1—C1—C2 | 122.74 (10) | C3—C2—H2A | 121.1 |
N1—C1—H1A | 118.6 | N2—C6—C3 | 178.67 (12) |
C2—C1—H1A | 118.6 | O2—C7—O1 | 126.63 (10) |
C4—C3—C2 | 120.13 (10) | O2—C7—C7i | 121.93 (12) |
C4—C3—C6 | 120.12 (9) | O1—C7—C7i | 111.44 (11) |
C2—C3—C6 | 119.74 (10) |
Symmetry code: (i) −x+2, −y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···N1 | 0.82 (1) | 1.80 (1) | 2.6173 (12) | 176 (2) |
C4—H4A···O1ii | 0.93 | 2.48 | 3.3640 (13) | 160 |
Symmetry code: (ii) x, y+1, z. |
Experimental details
Crystal data | |
Chemical formula | C6H4N2·0.5C2H2O4 |
Mr | 149.13 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 298 |
a, b, c (Å) | 3.6842 (6), 7.5816 (5), 12.4511 (1) |
α, β, γ (°) | 78.258 (1), 85.301 (1), 82.547 (1) |
V (Å3) | 337.08 (6) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.11 |
Crystal size (mm) | 0.10 × 0.03 × 0.03 |
Data collection | |
Diffractometer | Rigaku SCXmini Mercury2 diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku, 2005) |
Tmin, Tmax | 0.910, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3634, 1528, 1268 |
Rint | 0.024 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.036, 0.101, 1.04 |
No. of reflections | 1528 |
No. of parameters | 103 |
No. of restraints | 1 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.46, −0.27 |
Computer programs: CrystalClear (Rigaku, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···N1 | 0.822 (2) | 1.797 (3) | 2.6173 (12) | 175.5 (15) |
C4—H4A···O1i | 0.93 | 2.480 | 3.3640 (13) | 159.9 |
Symmetry code: (i) x, y+1, z. |
Acknowledgements
This work was supported by a start-up grant from Southeast University, China.
References
Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19. CrossRef Web of Science Google Scholar
Dai, J. & Chen, X.-Y. (2011). Acta Cryst. E67, o287. Web of Science CSD CrossRef IUCr Journals Google Scholar
Fu, D.-W., Zhang, W., Cai, H.-L., Ge, J.-Z., Zhang, Y. & Xiong, R.-G. (2011c). Adv. Mater. 23, 5658–5662. Web of Science CSD CrossRef CAS PubMed Google Scholar
Fu, D.-W., Zhang, W., Cai, H.-L., Zhang, Y., Ge, J.-Z., Xiong, R.-G. & Huang, S. P. D. (2011a). J. Am. Chem. Soc. 133, 12780–12786. Web of Science CSD CrossRef CAS PubMed Google Scholar
Fu, D.-W., Zhang, W., Cai, H.-L., Zhang, Y., Ge, J.-Z., Xiong, R.-G., Huang, S. P. D. & Nakamura, T. (2011b). Angew. Chem. Int. Ed. 50, 11947–11951. Web of Science CSD CrossRef CAS Google Scholar
Rigaku (2005). CrystalClear. Rigaku Corporation, Tokyo, Japan. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Xu, R.-J., Fu, D.-W., Dai, J., Zhang, Y., Ge, J.-Z. & Ye, H.-Y. (2011). Inorg. Chem. Commun. 14, 1093–1096. Web of Science CSD CrossRef CAS Google Scholar
Zheng, W.-N. (2011). Acta Cryst. E67, m344. Web of Science CSD CrossRef IUCr Journals Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Simple organic salts containing strong intermolecular H-bonds have attracted an attention as materials which display ferroelectric-paraelectric phase transitions (Fu et al., 2011a,b,c). With the purpose of obtaining crystals of organic salts exhibiting ferroelectric phase transitions, various organic compounds have been studied and the series of new materials have been elaborated (Dai & Chen, 2011; Xu et al., 2011; Zheng, 2011). Herewith we present the synthesis and crystal structure of the title molecular complex, pyridine-4-carbonitrile–oxalic acid (2/1).
All bond lengths and angles in the studied structure have expected values (Allen et al., 1987). The dihedral angle between the pyridine ring and the oxalic acid molecule is 10.29 (8)°. The H atoms of oxalic acid are involved in strong intramolecular O—H···N hydrogen bonds (Fig. 1 and Table 1), with the O···N distance of 2.617 (3)Å. The weak intermolecular C—H···O interaction is also presented in this structure, with C4···O1 = 3.364 (2)Å. The crystal packing is further stabilized by the π···π interactions between the pyridine rings of the neighbouring pyridine-4-carbonitrile molecules (Fig. 2).