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Supporting information
![]() | Crystallographic Information File (CIF) https://doi.org/10.1107/S205698901501172X/hb7446sup1.cif |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S205698901501172X/hb7446Isup2.hkl |
![]() | Chemical Markup Language (CML) file https://doi.org/10.1107/S205698901501172X/hb7446Isup3.cml |
CCDC reference: 1407396
Key indicators
- Single-crystal X-ray study
- T = 296 K
- Mean
(C-C) = 0.003 Å
- R factor = 0.059
- wR factor = 0.133
- Data-to-parameter ratio = 12.6
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.1 Note PLAT906_ALERT_3_C Large K value in the Analysis of Variance ...... 12.612 Check
Alert level G PLAT002_ALERT_2_G Number of Distance or Angle Restraints on AtSite 7 Note PLAT042_ALERT_1_G Calc. and Reported MoietyFormula Strings Differ Please Check PLAT066_ALERT_1_G Predicted and Reported Tmin&Tmax Range Identical ? Check PLAT172_ALERT_4_G The CIF-Embedded .res File Contains DFIX Records 10 Report PLAT860_ALERT_3_G Number of Least-Squares Restraints ............. 5 Note
0 ALERT level A = Most likely a serious problem - resolve or explain 0 ALERT level B = A potentially serious problem, consider carefully 2 ALERT level C = Check. Ensure it is not caused by an omission or oversight 5 ALERT level G = General information/check it is not something unexpected 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check
A remarkable feature of ionothermal synthesis is the fact that ionic liquids (ILs) can act simultaneously as sustainable solvents and structure-directing agents (also known as templates). This has been widely demonstrated by their potential in the discovery of unprecedented crystalline materials (Xu et al., 2013). Following our interest in the design and preparation of new types of metal-organic frameworks (MOFs), we have been exploring the use of 5-amino-1H-1,2,4-triazole-3-carboxylic acid (H2atrc) and pyrazine-2,3-dicarboxylic acid (H2Pzdc) as a double-ligand system in the presence of transition metal centers using ionothermal synthetic conditions. In the presence of AgNO3 the obtained product revealed, however, to be an unexpected organic salt (Bond, 2007) composed of the 3-amino-2H,4H(+)-1,2,4-triazolium cation and the pyrazine-2-carboxylato anion.
The title compound is a product of decomposition of the H2atrc and H2Pzdc organic molecules by way of decarboxylation leading to, respectively, 3-amino-2H,4H-1,2,4-triazolium [(C2H5N4)+] and pyrazine-2-carboxylate [(C5H3N2O2)-]. The asymmetric unit is composed of one of each of these moieties, as depicted in both the chemical diagram and in Fig. 1.
The cation present in the title compound is rich in groups capable of forming strong N—H···N,O hydrogen-bonding interactions (see Table 1 for further geometrical details), many highly directional with the observed <(D—H···A) interaction angles being above 165°. These supramolecular contacts are the main driving force which mediate the crystal packing features of the title compound. Indeed, the donation of hydrogen atoms from the cation to the carboxylate group of an adjacent anion (N6—H6B···O2 and N5—H5···O1) forms the known structurally robust R22(8) graph-set motif (dashed pink lines in Fig. 2) (Grell et al., 1999). This graph-set motif has already been found in salts containing the title compound cation and carboxylic acids (see Database survey below). Two other interactions, N6—H6A···N1 (dashed aqua lines) and N4—H4A···O2, describe a second R22(9) hydrogen-bond motif. In contrast to the previous graph-set motif, the R22(9) ring has not been observed in structures containing the title-compound cation. The zigzag alternation of these two graph-set motifs leads to the formation of a highly coplanar supramolecular tape running parallel to the [010] direction of the unit cell (Fig. 2). Adjacent tapes interact by way of weak π–π stacking contacts between triazole and pyrazine rings, with the inter-centroid distance being 3.75 (3) Å (dashed orange lines in Fig. 2).
Triazole molecules have been extensively used in the preparation of organic co-crystals (Kastelic et al., 2011; Remenar et al., 2003), and a survey of the Cambridge Structural Database (Groom & Allen, 2014) revealed the existence of about a dozen of crystallographic reports of co-crystals of the title compound cation (Byriel et al., 1992; Essid et al., 2013; Joo et al., 2013; Luo et al., 2013; Lynch et al., 1992, 1998, 1999; Lynch, Smith, Byriel & Kennard, 1994; Lynch, Smith, Byriel, Kennard et al., 1994; Matulková et al., 2007; Smith et al., 1996). The only compounds known with both of the title compound entities present is a bimetallic complex also containing Cd2+ and NO3- ions (Chen et al., 2009) .
5-Amino-1H-1,2,4-triazole-3-carboxylic acid (H2atrc, 98% purity), pyrazine-2,3-dicarboxylic acid (H2Pzdc, 97% purity), 1-methylimidazole (99%+ purity), 1-bromobutane (99% purity) and AgNO3 (99%+ purity) were purchased from Sigma–Aldrich and were used as received without further purification. 1-Butyl-3-methylimidazolium bromide ([BMI]Br) was prepared according to the literature method (Parnham & Morris, 2006) and was isolated as a pale-yellow oil (yield of ca 78%).
AgNO3 (0.0687 g; 0.400 mmol), H2atrc (0.0510 g; 0.400 mmol) and H2Pzdc (0.0607 g; 0.361 mmol) were mixed with 0.49 g of [BMI]Br and 0.3 mL of distilled water in a ca 25 mL Teflon-lined stainless-steel reaction vessel. The resulting mixture was heated to 383 K for 7 days. The vessel was then allowed to cool to ambient temperature at a rate of ca 1 K h-1. Small colourless crystals of the title compound were directly isolated from the vessel contents.
Hydrogen atoms bound to carbon were placed at idealized positions with C—H = 0.95 Å, and included in the final structural model in a riding-motion approximation with the isotropic thermal displacement parameters fixed at 1.2Ueq of the carbon atom to which they are attached. Hydrogen atoms associated with nitrogen atoms were located directly from difference Fourier maps and were included in the model with the N—H and H···H (only for the –NH2 groups) distances restrained to 0.90 (1) and 1.55 (1) Å, respectively, in order to ensure a chemically reasonable environment for these groups. These hydrogen atoms were modelled with the isotropic thermal displacement parameters fixed at 1.5Ueq(N).
Data collection: APEX2 (Bruker, 2006); cell refinement: SAINT-Plus (Bruker, 2005); data reduction: SAINT-Plus (Bruker, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: DIAMOND (Brandenburg, 2009); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).
C2H5N4+·C5H3N2O2− | F(000) = 432 |
Mr = 208.19 | Dx = 1.526 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 7.0599 (5) Å | Cell parameters from 1298 reflections |
b = 12.1868 (8) Å | θ = 2.6–19.7° |
c = 10.8385 (6) Å | µ = 0.12 mm−1 |
β = 103.593 (4)° | T = 296 K |
V = 906.40 (10) Å3 | Block, colourless |
Z = 4 | 0.09 × 0.04 × 0.03 mm |
Bruker X8 Kappa CCD APEXII diffractometer | 1037 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.077 |
ω / ϕ scans | θmax = 26.4°, θmin = 2.6° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1998) | h = −8→8 |
Tmin = 0.989, Tmax = 0.997 | k = −15→15 |
12089 measured reflections | l = −13→13 |
1858 independent reflections |
Refinement on F2 | 5 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.059 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.133 | w = 1/[σ2(Fo2) + (0.0599P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.01 | (Δ/σ)max < 0.001 |
1858 reflections | Δρmax = 0.19 e Å−3 |
148 parameters | Δρmin = −0.20 e Å−3 |
C2H5N4+·C5H3N2O2− | V = 906.40 (10) Å3 |
Mr = 208.19 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 7.0599 (5) Å | µ = 0.12 mm−1 |
b = 12.1868 (8) Å | T = 296 K |
c = 10.8385 (6) Å | 0.09 × 0.04 × 0.03 mm |
β = 103.593 (4)° |
Bruker X8 Kappa CCD APEXII diffractometer | 1858 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1998) | 1037 reflections with I > 2σ(I) |
Tmin = 0.989, Tmax = 0.997 | Rint = 0.077 |
12089 measured reflections |
R[F2 > 2σ(F2)] = 0.059 | 5 restraints |
wR(F2) = 0.133 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.01 | Δρmax = 0.19 e Å−3 |
1858 reflections | Δρmin = −0.20 e Å−3 |
148 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. |
x | y | z | Uiso*/Ueq | ||
N1 | 0.2890 (3) | 0.79063 (17) | 0.49872 (19) | 0.0389 (6) | |
N2 | 0.0664 (3) | 0.79145 (18) | 0.2472 (2) | 0.0468 (6) | |
C1 | 0.2177 (4) | 0.8840 (2) | 0.4404 (2) | 0.0334 (6) | |
C2 | 0.1066 (4) | 0.8815 (2) | 0.3165 (2) | 0.0412 (7) | |
H2 | 0.0571 | 0.9476 | 0.2797 | 0.049* | |
C3 | 0.1381 (4) | 0.6995 (2) | 0.3059 (2) | 0.0448 (7) | |
H3 | 0.1147 | 0.6334 | 0.2623 | 0.054* | |
C4 | 0.2461 (4) | 0.6993 (2) | 0.4297 (3) | 0.0442 (7) | |
H4 | 0.2912 | 0.6326 | 0.4668 | 0.053* | |
C5 | 0.2560 (4) | 0.9921 (2) | 0.5101 (2) | 0.0378 (7) | |
O1 | 0.1745 (3) | 1.07442 (14) | 0.45075 (15) | 0.0481 (6) | |
O2 | 0.3628 (3) | 0.99415 (14) | 0.61986 (16) | 0.0543 (6) | |
N3 | 0.7128 (4) | 0.94320 (19) | 0.8957 (2) | 0.0622 (8) | |
N4 | 0.6167 (4) | 0.88117 (19) | 0.7929 (2) | 0.0476 (6) | |
H4A | 0.535 (3) | 0.912 (2) | 0.7253 (18) | 0.071* | |
N5 | 0.7480 (3) | 0.76575 (18) | 0.93596 (19) | 0.0417 (6) | |
H5 | 0.778 (4) | 0.6996 (13) | 0.972 (2) | 0.063* | |
N6 | 0.5628 (4) | 0.6942 (2) | 0.7405 (2) | 0.0540 (7) | |
H6A | 0.473 (3) | 0.714 (2) | 0.6709 (19) | 0.081* | |
H6B | 0.585 (5) | 0.6271 (13) | 0.775 (3) | 0.081* | |
C6 | 0.6369 (4) | 0.7751 (2) | 0.8181 (2) | 0.0365 (7) | |
C7 | 0.7892 (5) | 0.8695 (2) | 0.9782 (3) | 0.0553 (8) | |
H7 | 0.8649 | 0.8861 | 1.0584 | 0.066* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0450 (14) | 0.0290 (13) | 0.0400 (12) | −0.0006 (11) | 0.0049 (10) | 0.0005 (10) |
N2 | 0.0557 (16) | 0.0387 (14) | 0.0406 (12) | 0.0008 (12) | 0.0005 (11) | −0.0086 (12) |
C1 | 0.0331 (15) | 0.0309 (15) | 0.0355 (13) | −0.0004 (13) | 0.0067 (11) | 0.0022 (12) |
C2 | 0.0495 (18) | 0.0320 (16) | 0.0367 (14) | 0.0061 (14) | −0.0007 (13) | 0.0020 (12) |
C3 | 0.0487 (19) | 0.0352 (17) | 0.0478 (16) | −0.0016 (15) | 0.0059 (14) | −0.0099 (13) |
C4 | 0.0499 (18) | 0.0299 (16) | 0.0497 (16) | 0.0036 (14) | 0.0056 (14) | 0.0028 (13) |
C5 | 0.0420 (17) | 0.0344 (16) | 0.0330 (13) | 0.0001 (14) | 0.0006 (12) | 0.0036 (12) |
O1 | 0.0625 (14) | 0.0319 (11) | 0.0402 (10) | 0.0058 (9) | −0.0074 (9) | 0.0021 (8) |
O2 | 0.0708 (14) | 0.0375 (12) | 0.0399 (10) | 0.0067 (10) | −0.0165 (10) | −0.0025 (9) |
N3 | 0.089 (2) | 0.0419 (15) | 0.0461 (14) | 0.0029 (15) | −0.0032 (13) | 0.0024 (12) |
N4 | 0.0625 (18) | 0.0367 (15) | 0.0386 (13) | 0.0037 (13) | 0.0019 (12) | 0.0061 (11) |
N5 | 0.0480 (14) | 0.0362 (15) | 0.0359 (12) | 0.0025 (12) | −0.0004 (11) | 0.0083 (11) |
N6 | 0.0607 (18) | 0.0440 (16) | 0.0491 (15) | −0.0005 (15) | −0.0038 (13) | 0.0030 (13) |
C6 | 0.0391 (17) | 0.0349 (18) | 0.0348 (13) | 0.0044 (13) | 0.0068 (12) | 0.0057 (12) |
C7 | 0.074 (2) | 0.046 (2) | 0.0383 (15) | 0.0020 (17) | −0.0026 (15) | 0.0012 (14) |
N1—C4 | 1.335 (3) | N3—C7 | 1.293 (3) |
N1—C1 | 1.341 (3) | N3—N4 | 1.384 (3) |
N2—C2 | 1.323 (3) | N4—C6 | 1.322 (3) |
N2—C3 | 1.328 (3) | N4—H4A | 0.902 (10) |
C1—C2 | 1.387 (3) | N5—C6 | 1.338 (3) |
C1—C5 | 1.512 (3) | N5—C7 | 1.353 (3) |
C2—H2 | 0.9300 | N5—H5 | 0.901 (10) |
C3—C4 | 1.379 (4) | N6—C6 | 1.321 (3) |
C3—H3 | 0.9300 | N6—H6A | 0.899 (10) |
C4—H4 | 0.9300 | N6—H6B | 0.896 (10) |
C5—O2 | 1.250 (2) | C7—H7 | 0.9300 |
C5—O1 | 1.256 (3) | ||
C4—N1—C1 | 115.6 (2) | C7—N3—N4 | 102.9 (2) |
C2—N2—C3 | 114.9 (2) | C6—N4—N3 | 111.1 (2) |
N1—C1—C2 | 120.2 (2) | C6—N4—H4A | 126 (2) |
N1—C1—C5 | 120.1 (2) | N3—N4—H4A | 121.7 (19) |
C2—C1—C5 | 119.8 (2) | C6—N5—C7 | 105.9 (2) |
N2—C2—C1 | 124.4 (2) | C6—N5—H5 | 121.3 (18) |
N2—C2—H2 | 117.8 | C7—N5—H5 | 132.7 (18) |
C1—C2—H2 | 117.8 | C6—N6—H6A | 115 (2) |
N2—C3—C4 | 122.0 (2) | C6—N6—H6B | 115 (2) |
N2—C3—H3 | 119.0 | H6A—N6—H6B | 128 (3) |
C4—C3—H3 | 119.0 | N6—C6—N4 | 126.2 (2) |
N1—C4—C3 | 123.0 (2) | N6—C6—N5 | 126.9 (2) |
N1—C4—H4 | 118.5 | N4—C6—N5 | 106.9 (2) |
C3—C4—H4 | 118.5 | N3—C7—N5 | 113.2 (2) |
O2—C5—O1 | 125.0 (2) | N3—C7—H7 | 123.4 |
O2—C5—C1 | 119.3 (2) | N5—C7—H7 | 123.4 |
O1—C5—C1 | 115.7 (2) | ||
C4—N1—C1—C2 | 0.3 (4) | N1—C1—C5—O1 | −176.1 (2) |
C4—N1—C1—C5 | 179.5 (2) | C2—C1—C5—O1 | 3.1 (4) |
C3—N2—C2—C1 | 1.2 (4) | C7—N3—N4—C6 | 0.8 (3) |
N1—C1—C2—N2 | −1.4 (4) | N3—N4—C6—N6 | 179.8 (3) |
C5—C1—C2—N2 | 179.4 (2) | N3—N4—C6—N5 | −0.9 (3) |
C2—N2—C3—C4 | −0.1 (4) | C7—N5—C6—N6 | 179.9 (3) |
C1—N1—C4—C3 | 0.8 (4) | C7—N5—C6—N4 | 0.6 (3) |
N2—C3—C4—N1 | −1.0 (4) | N4—N3—C7—N5 | −0.4 (4) |
N1—C1—C5—O2 | 3.7 (4) | C6—N5—C7—N3 | −0.1 (4) |
C2—C1—C5—O2 | −177.1 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
N4—H4A···O2 | 0.90 (1) | 1.77 (1) | 2.655 (3) | 166 (3) |
N5—H5···O1i | 0.90 (1) | 1.73 (1) | 2.632 (3) | 176 (3) |
N6—H6B···O2i | 0.90 (1) | 1.97 (1) | 2.853 (3) | 169 (3) |
N6—H6A···N1 | 0.90 (1) | 2.21 (1) | 3.099 (3) | 169 (3) |
Symmetry code: (i) −x+1, y−1/2, −z+3/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
N4—H4A···O2 | 0.902 (10) | 1.769 (12) | 2.655 (3) | 166 (3) |
N5—H5···O1i | 0.901 (10) | 1.733 (11) | 2.632 (3) | 176 (3) |
N6—H6B···O2i | 0.896 (10) | 1.968 (12) | 2.853 (3) | 169 (3) |
N6—H6A···N1 | 0.899 (10) | 2.212 (12) | 3.099 (3) | 169 (3) |
Symmetry code: (i) −x+1, y−1/2, −z+3/2. |
Experimental details
Crystal data | |
Chemical formula | C2H5N4+·C5H3N2O2− |
Mr | 208.19 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 296 |
a, b, c (Å) | 7.0599 (5), 12.1868 (8), 10.8385 (6) |
β (°) | 103.593 (4) |
V (Å3) | 906.40 (10) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.12 |
Crystal size (mm) | 0.09 × 0.04 × 0.03 |
Data collection | |
Diffractometer | Bruker X8 Kappa CCD APEXII diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1998) |
Tmin, Tmax | 0.989, 0.997 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12089, 1858, 1037 |
Rint | 0.077 |
(sin θ/λ)max (Å−1) | 0.625 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.059, 0.133, 1.01 |
No. of reflections | 1858 |
No. of parameters | 148 |
No. of restraints | 5 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.19, −0.20 |
Computer programs: APEX2 (Bruker, 2006), SAINT-Plus (Bruker, 2005), SHELXS97 (Sheldrick, 2008), SHELXL2014 (Sheldrick, 2015), DIAMOND (Brandenburg, 2009), SHELXTL (Sheldrick, 2008).