Abstract
In the title salt, C6H9N2 +·C2F3O2 −, the F atoms of the anion are disordered over two sets of sites, with refined occupancies in a ratio of 0.505 (17):0.495 (17). In the crystal, cations and anions are linked via N—H⋯O hydrogen bonds, forming R 2 2(8) ring motifs. The ionic units are linked into a two-dimensional network parallel to (100) by N—H⋯O and weak C—H⋯O hydrogen bonds. The crystal structure is further stabilized by weak C—H⋯F hydrogen bonds, resulting in a three-dimensional network.
Related literature
For background to the chemistry of substituted pyridines, see: Pozharski et al. (1997 ▶); Katritzky et al. (1996 ▶). For details of hydrogen bonding, see: Jeffrey & Saenger (1991 ▶); Jeffrey (1997 ▶); Scheiner (1997 ▶). For hydrogen-bond motifs, see: Bernstein et al. (1995 ▶). For standard bond-length data, see: Allen et al. (1987 ▶). For the stability of the temperature controller used for the data collection, see: Cosier & Glazer (1986 ▶). For a related structure, see: Rodrigues et al. (2001 ▶).
Experimental
Crystal data
C6H9N2 +·C2F3O2 −
M r = 222.17
Orthorhombic,
a = 18.725 (4) Å
b = 4.6256 (10) Å
c = 11.319 (2) Å
V = 980.4 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.15 mm−1
T = 100 K
0.54 × 0.29 × 0.11 mm
Data collection
Bruker SMART APEXII DUO CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.926, T max = 0.985
12012 measured reflections
3216 independent reflections
2627 reflections with I > 2σ(I)
R int = 0.041
Refinement
R[F 2 > 2σ(F 2)] = 0.046
wR(F 2) = 0.114
S = 1.07
3216 reflections
177 parameters
1 restraint
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.23 e Å−3
Δρmin = −0.30 e Å−3
Absolute structure: Flack (1983 ▶), 1368 Friedel pairs
Flack parameter: −0.1 (7)
Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812045291/lh5549sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812045291/lh5549Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812045291/lh5549Isup3.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—H1N1⋯O2 | 0.98 (3) | 1.75 (3) | 2.7281 (19) | 177 (2) |
| N2—H2N2⋯O1 | 0.95 (3) | 1.92 (3) | 2.865 (2) | 173 (2) |
| N2—H1N2⋯O2i | 0.86 (3) | 1.99 (3) | 2.8347 (18) | 167 (3) |
| C3—H3A⋯F2ii | 0.95 | 2.51 | 3.429 (6) | 164 |
| C5—H5A⋯O1iii | 0.95 | 2.27 | 3.1910 (19) | 162 |
Symmetry codes: (i)
; (ii)
; (iii)
.
Acknowledgments
The authors thank the Malaysian Government and Universiti Sains Malaysia (USM) for the research facilities and Fundamental Research Grant Scheme (FRGS) No. 203/PFIZIK/6711171 to conduct this work. KT thanks The Academy of Sciences for the Developing World and USM for a TWAS–USM fellowship.
supplementary crystallographic information
Comment
Pyridine and its derivatives play an important role in heterocyclic chemistry (Pozharski et al., 1997; Katritzky et al., 1996). They are often involved in hydrogen-bond interactions (Jeffrey & Saenger, 1991; Jeffrey, 1997; Scheiner, 1997). Trifluoroacetic acid is a very strong carboxylic acid, easily volatile, and used for protein purification. An example of a crystal structure of a trifluoroacetate salts has been reported (Rodrigues et al., 2001). In order to study potential hydrogen bonding interactions the crystal structure determination of the title compound (I) was carried out.
The asymmetric unit (Fig. 1) contains one 2-amino-5-methylpyridinium cation and one trifluoroacetate anion. The F atoms of the anion are disordered over two sets of sites, with occupancies of 0.505 (17) and 0.495 (17). In the 2-amino-5-methylpyridinium cation, a wider than normal angle [C1—N1—C5 = 122.77 (14)°] is subtended at the protonated N1 atom. The 2-amino-5-methylpyridinium cation is essentially planar, with a maximum deviation of 0.016 (2) Å for atom N2. The bond lengths (Allen et al., 1987) and angles are normal.
In the crystal (Fig. 2), the cations and anions are linked via N—H···O hydrogen bonds to form R22(8) ring motifs (Bernstein et al., 1995). The ionic units are linked into a two-dimensional network parallel to (100) by N2—H1N2···O2i and C5—H5A···O1iii hydrogen bonds (symmetry codes in Table 1). The crystal structure is further stabilized by C3—H3A···F2ii hydrogen bonds, resulting in a three-dimensional network.
Experimental
To a hot methanol solution (20 ml) of 2-amino-5-methylpyridine (54 mg, Aldrich) was added a few drops of trifluoroacetic acid. The solution was warmed over a heating magnetic stirrer hotplate for a few minutes. The resulting solution was allowed to cool slowly at room temperature and crystals of the title compound (I) appeared after a few days.
Refinement
The F atoms of the anion are disordered over two sets of sites, with occupancies of 0.505 (17):0.495 (17). Atoms H1N1, H1N2 and H2N2 were located in a difference Fourier maps and refined freely. The remaining hydrogen atoms were positioned geometrically [C–H= 0.95–0.98 Å] and were refined using a riding model, with Uiso(H)=1.2 Ueq(C) or 1.5Ueq(methyl C). A rotating group model was used for the methyl group.
Figures
Fig. 1.
The molecular structure of the title compound, showing 50% probability displacement ellipsoids and the atom-numbering scheme. Both disorder components are shown.
Fig. 2.
The crystal packing diagram of the title compound. Only major disorder component is shown. Hydrogen bonds are shown as dashed lines.
Crystal data
| C6H9N2+·C2F3O2− | F(000) = 456 |
| Mr = 222.17 | Dx = 1.505 Mg m−3 |
| Orthorhombic, Pna21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2c -2n | Cell parameters from 4200 reflections |
| a = 18.725 (4) Å | θ = 2.8–32.5° |
| b = 4.6256 (10) Å | µ = 0.15 mm−1 |
| c = 11.319 (2) Å | T = 100 K |
| V = 980.4 (3) Å3 | Plate, colourless |
| Z = 4 | 0.54 × 0.29 × 0.11 mm |
Data collection
| Bruker SMART APEXII DUO CCD area-detector diffractometer | 3216 independent reflections |
| Radiation source: fine-focus sealed tube | 2627 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.041 |
| φ and ω scans | θmax = 32.7°, θmin = 2.2° |
| Absorption correction: multi-scan (SADABS; Bruker, 2009) | h = −28→28 |
| Tmin = 0.926, Tmax = 0.985 | k = −6→6 |
| 12012 measured reflections | l = −16→17 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.046 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.114 | w = 1/[σ2(Fo2) + (0.0538P)2 + 0.1405P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.07 | (Δ/σ)max < 0.001 |
| 3216 reflections | Δρmax = 0.23 e Å−3 |
| 177 parameters | Δρmin = −0.30 e Å−3 |
| 1 restraint | Absolute structure: Flack (1983), 1368 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: −0.1 (7) |
Special details
| Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K. |
| 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 | Occ. (<1) | |
| F1 | 0.5951 (6) | −0.360 (3) | 0.6163 (9) | 0.0636 (17) | 0.505 (17) |
| F2 | 0.5409 (3) | 0.0250 (13) | 0.6382 (9) | 0.075 (2) | 0.505 (17) |
| F3 | 0.5859 (5) | −0.076 (4) | 0.4723 (7) | 0.104 (4) | 0.505 (17) |
| F1X | 0.6094 (7) | −0.352 (2) | 0.5755 (15) | 0.097 (4) | 0.495 (17) |
| F2X | 0.5478 (4) | −0.032 (2) | 0.6626 (5) | 0.080 (2) | 0.495 (17) |
| F3X | 0.5752 (3) | 0.0168 (15) | 0.4869 (6) | 0.0479 (14) | 0.495 (17) |
| O1 | 0.67666 (7) | 0.0887 (3) | 0.73348 (10) | 0.0384 (3) | |
| O2 | 0.70767 (6) | 0.1522 (3) | 0.54434 (9) | 0.0312 (3) | |
| N1 | 0.80834 (7) | 0.5530 (3) | 0.60374 (10) | 0.0248 (3) | |
| N2 | 0.78211 (9) | 0.5050 (4) | 0.80182 (12) | 0.0320 (3) | |
| C1 | 0.81952 (8) | 0.6336 (4) | 0.71687 (12) | 0.0257 (3) | |
| C2 | 0.87136 (9) | 0.8495 (4) | 0.73742 (14) | 0.0307 (3) | |
| H2A | 0.8806 | 0.9141 | 0.8156 | 0.037* | |
| C3 | 0.90806 (9) | 0.9649 (4) | 0.64496 (15) | 0.0316 (3) | |
| H3A | 0.9432 | 1.1084 | 0.6599 | 0.038* | |
| C4 | 0.89527 (8) | 0.8768 (4) | 0.52703 (13) | 0.0279 (3) | |
| C5 | 0.84486 (8) | 0.6703 (4) | 0.51114 (12) | 0.0257 (3) | |
| H5A | 0.8347 | 0.6054 | 0.4333 | 0.031* | |
| C6 | 0.93586 (10) | 1.0012 (4) | 0.42471 (17) | 0.0364 (4) | |
| H6A | 0.9186 | 0.9147 | 0.3510 | 0.055* | |
| H6B | 0.9868 | 0.9594 | 0.4342 | 0.055* | |
| H6C | 0.9286 | 1.2110 | 0.4221 | 0.055* | |
| C7 | 0.59832 (9) | −0.0794 (4) | 0.58757 (15) | 0.0312 (3) | |
| C8 | 0.66781 (9) | 0.0707 (4) | 0.62616 (13) | 0.0268 (3) | |
| H2N2 | 0.7456 (13) | 0.369 (6) | 0.785 (2) | 0.040 (6)* | |
| H1N2 | 0.7919 (14) | 0.558 (6) | 0.873 (3) | 0.050 (7)* | |
| H1N1 | 0.7723 (13) | 0.405 (6) | 0.585 (2) | 0.043 (6)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| F1 | 0.075 (3) | 0.027 (2) | 0.089 (4) | −0.0046 (19) | −0.017 (2) | 0.007 (2) |
| F2 | 0.0328 (17) | 0.044 (2) | 0.148 (6) | 0.0071 (15) | 0.004 (3) | −0.043 (3) |
| F3 | 0.093 (4) | 0.194 (10) | 0.0252 (15) | −0.097 (5) | −0.010 (2) | 0.014 (4) |
| F1X | 0.092 (6) | 0.021 (2) | 0.177 (11) | 0.005 (3) | −0.069 (7) | −0.017 (5) |
| F2X | 0.041 (3) | 0.154 (6) | 0.044 (2) | −0.038 (3) | 0.0180 (16) | −0.011 (3) |
| F3X | 0.0410 (16) | 0.060 (3) | 0.042 (3) | −0.0108 (16) | −0.0251 (16) | 0.0201 (19) |
| O1 | 0.0462 (7) | 0.0534 (9) | 0.0156 (5) | −0.0029 (6) | 0.0001 (4) | 0.0020 (5) |
| O2 | 0.0337 (5) | 0.0450 (7) | 0.0149 (4) | −0.0038 (5) | 0.0021 (4) | −0.0058 (5) |
| N1 | 0.0316 (6) | 0.0292 (7) | 0.0136 (5) | 0.0038 (5) | −0.0025 (4) | −0.0004 (5) |
| N2 | 0.0454 (8) | 0.0368 (9) | 0.0138 (5) | 0.0023 (7) | 0.0001 (5) | −0.0032 (5) |
| C1 | 0.0341 (7) | 0.0277 (8) | 0.0154 (6) | 0.0089 (6) | −0.0027 (5) | −0.0032 (6) |
| C2 | 0.0412 (8) | 0.0290 (9) | 0.0220 (6) | 0.0061 (7) | −0.0067 (6) | −0.0064 (6) |
| C3 | 0.0351 (8) | 0.0299 (9) | 0.0298 (7) | 0.0036 (6) | −0.0051 (6) | −0.0059 (7) |
| C4 | 0.0305 (7) | 0.0298 (9) | 0.0235 (7) | 0.0075 (6) | −0.0013 (5) | 0.0003 (6) |
| C5 | 0.0321 (6) | 0.0302 (8) | 0.0147 (5) | 0.0069 (6) | −0.0025 (5) | −0.0014 (5) |
| C6 | 0.0394 (8) | 0.0377 (10) | 0.0320 (7) | 0.0008 (7) | 0.0038 (7) | 0.0033 (8) |
| C7 | 0.0380 (7) | 0.0299 (9) | 0.0255 (6) | −0.0003 (6) | −0.0007 (6) | 0.0037 (6) |
| C8 | 0.0318 (7) | 0.0305 (8) | 0.0181 (6) | 0.0052 (6) | −0.0001 (5) | −0.0008 (6) |
Geometric parameters (Å, º)
| F1—C7 | 1.341 (11) | N2—H1N2 | 0.86 (3) |
| F2—C7 | 1.311 (6) | C1—C2 | 1.412 (2) |
| F3—C7 | 1.325 (8) | C2—C3 | 1.361 (3) |
| F1X—C7 | 1.287 (11) | C2—H2A | 0.9500 |
| F2X—C7 | 1.290 (5) | C3—C4 | 1.416 (2) |
| F3X—C7 | 1.297 (6) | C3—H3A | 0.9500 |
| O1—C8 | 1.2289 (18) | C4—C5 | 1.355 (2) |
| O2—C8 | 1.2478 (19) | C4—C6 | 1.500 (2) |
| N1—C1 | 1.3500 (18) | C5—H5A | 0.9500 |
| N1—C5 | 1.3640 (19) | C6—H6A | 0.9800 |
| N1—H1N1 | 0.98 (3) | C6—H6B | 0.9800 |
| N2—C1 | 1.330 (2) | C6—H6C | 0.9800 |
| N2—H2N2 | 0.95 (3) | C7—C8 | 1.538 (2) |
| C1—N1—C5 | 122.78 (14) | C4—C6—H6A | 109.5 |
| C1—N1—H1N1 | 119.9 (15) | C4—C6—H6B | 109.5 |
| C5—N1—H1N1 | 117.3 (15) | H6A—C6—H6B | 109.5 |
| C1—N2—H2N2 | 121.8 (14) | C4—C6—H6C | 109.5 |
| C1—N2—H1N2 | 116.0 (19) | H6A—C6—H6C | 109.5 |
| H2N2—N2—H1N2 | 122 (2) | H6B—C6—H6C | 109.5 |
| N2—C1—N1 | 118.73 (15) | F1X—C7—F2X | 110.9 (7) |
| N2—C1—C2 | 124.01 (14) | F1X—C7—F3X | 107.3 (7) |
| N1—C1—C2 | 117.26 (14) | F2X—C7—F3X | 106.0 (5) |
| C3—C2—C1 | 119.86 (14) | F2—C7—F1 | 102.4 (6) |
| C3—C2—H2A | 120.1 | F3—C7—F1 | 104.0 (8) |
| C1—C2—H2A | 120.1 | F1X—C7—C8 | 109.7 (5) |
| C2—C3—C4 | 121.77 (16) | F2X—C7—C8 | 110.8 (3) |
| C2—C3—H3A | 119.1 | F3X—C7—C8 | 112.1 (3) |
| C4—C3—H3A | 119.1 | F2—C7—C8 | 113.8 (3) |
| C5—C4—C3 | 116.49 (14) | F3—C7—C8 | 115.0 (4) |
| C5—C4—C6 | 121.40 (14) | F1—C7—C8 | 114.0 (5) |
| C3—C4—C6 | 122.10 (16) | O1—C8—O2 | 129.24 (16) |
| C4—C5—N1 | 121.84 (13) | O1—C8—C7 | 115.18 (15) |
| C4—C5—H5A | 119.1 | O2—C8—C7 | 115.57 (13) |
| N1—C5—H5A | 119.1 | ||
| C5—N1—C1—N2 | −179.15 (15) | F2X—C7—C8—O1 | 32.3 (6) |
| C5—N1—C1—C2 | 0.2 (2) | F3X—C7—C8—O1 | 150.5 (4) |
| N2—C1—C2—C3 | 178.70 (16) | F2—C7—C8—O1 | 51.3 (5) |
| N1—C1—C2—C3 | −0.6 (2) | F3—C7—C8—O1 | 174.4 (9) |
| C1—C2—C3—C4 | 0.7 (2) | F1—C7—C8—O1 | −65.7 (5) |
| C2—C3—C4—C5 | −0.4 (2) | F1X—C7—C8—O2 | 88.4 (9) |
| C2—C3—C4—C6 | −179.53 (17) | F2X—C7—C8—O2 | −148.9 (5) |
| C3—C4—C5—N1 | −0.1 (2) | F3X—C7—C8—O2 | −30.7 (4) |
| C6—C4—C5—N1 | 179.11 (15) | F2—C7—C8—O2 | −129.9 (5) |
| C1—N1—C5—C4 | 0.1 (2) | F3—C7—C8—O2 | −6.8 (9) |
| F1X—C7—C8—O1 | −90.5 (9) | F1—C7—C8—O2 | 113.2 (5) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1N1···O2 | 0.98 (3) | 1.75 (3) | 2.7281 (19) | 177 (2) |
| N2—H2N2···O1 | 0.95 (3) | 1.92 (3) | 2.865 (2) | 173 (2) |
| N2—H1N2···O2i | 0.86 (3) | 1.99 (3) | 2.8347 (18) | 167 (3) |
| C3—H3A···F2ii | 0.95 | 2.51 | 3.429 (6) | 164 |
| C5—H5A···O1iii | 0.95 | 2.27 | 3.1910 (19) | 162 |
Symmetry codes: (i) −x+3/2, y+1/2, z+1/2; (ii) x+1/2, −y+3/2, z; (iii) −x+3/2, y+1/2, z−1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5549).
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/S1600536812045291/lh5549sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812045291/lh5549Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812045291/lh5549Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


