| Figure 1 The molecular structure of (I ) at 290 K. Displacement ellipsoids are drawn at the 50% probability level. The dashed and dotted lines indicate strong and weak hydrogen bonds, respectively. |
Experimental
The crystals of (I
) were grown by slow evaporation, at room temperature, of an aqueous solution of equimolar amounts of pyridine and nitric acid.
Data collection
Bruker APEX CCD area-detector diffractometer ω scans Absorption correction: none 5258 measured reflections 1154 independent reflections 735 reflections with I > 2σ(I) Rint = 0.073 θmax = 25.0° h = −4 → 4 k = −14 → 14 l = −16 → 16
|
N1—C2 | 1.328 (4) | N1—C6 | 1.338 (4) | C2—C3 | 1.352 (4) | C3—C4 | 1.343 (4) | C4—C5 | 1.337 (4) | C5—C6 | 1.337 (4) | O1—N2 | 1.251 (2) | O2—N2 | 1.217 (3) | O3—N2 | 1.225 (3) | | C2—N1—C6 | 121.0 (2) | N1—C2—C3 | 119.8 (2) | C4—C3—C2 | 119.1 (2) | C5—C4—C3 | 120.6 (2) | C6—C5—C4 | 120.0 (2) | C5—C6—N1 | 119.5 (2) | O2—N2—O3 | 122.1 (2) | O2—N2—O1 | 119.5 (2) | O3—N2—O1 | 118.4 (2) | | |
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A | N1—H1⋯O1 | 0.94 (4) | 1.86 (4) | 2.787 (3) | 171 (3) | N1—H1⋯O3 | 0.94 (4) | 2.45 (4) | 3.149 (3) | 131 (3) | C2—H2⋯O3 | 0.93 | 2.78 | 3.307 (4) | 117 | C2—H2⋯O2i | 0.93 | 2.56 | 3.177 (3) | 124 | C3—H3⋯O2ii | 0.93 | 2.67 | 3.324 (3) | 128 | C4—H4⋯O3iii | 0.93 | 2.70 | 3.330 (3) | 126 | C5—H5⋯O3iii | 0.93 | 2.77 | 3.365 (4) | 123 | C6—H6⋯O1iv | 0.93 | 2.38 | 3.196 (3) | 146 | C6—H6⋯O2iv | 0.93 | 2.68 | 3.456 (3) | 141 | Symmetry codes: (i) ; (ii) ; (iii) ; (iv) -x,1-y,1-z. | |
All H atoms were located in a difference Fourier map. Atom H1 was refined in isotropic approximation [N—H = 0.94 (4) Å], other H atoms were treated as riding in idealized positions, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C).
Data collection: SMART (Bruker, 2001
); cell refinement: SAINT (Bruker, 2002
); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Bruker, 2001
); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Supporting information
Data collection: SMART (Bruker, 2001); cell refinement: SMART; data reduction: SAINT (Bruker, 2002); program(s) used to solve structure: SHELXTL (Bruker, 2001); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Crystal data top C5H6N+·NO3− | F(000) = 296 |
Mr = 142.12 | Dx = 1.454 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 1107 reflections |
a = 3.9015 (6) Å | θ = 2.2–22.4° |
b = 12.324 (2) Å | µ = 0.12 mm−1 |
c = 13.503 (2) Å | T = 290 K |
β = 90.57 (1)° | Plate, colourless |
V = 649.2 (2) Å3 | 0.42 × 0.37 × 0.03 mm |
Z = 4 | |
Data collection top ProteumM APEX CCD area-detector diffractometer | 735 reflections with I > 2σ(I) |
Radiation source: 60 W microfocus Bede Microsource with glass polycapillary optics | Rint = 0.073 |
Graphite monochromator | θmax = 25.0°, θmin = 2.2° |
Detector resolution: 8 pixels mm-1 | h = −4→4 |
ω scans | k = −14→14 |
5258 measured reflections | l = −16→16 |
1154 independent reflections | |
Refinement top 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)] = 0.050 | Hydrogen site location: difference Fourier map |
wR(F2) = 0.157 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | w = 1/[σ2(Fo2) + (0.086P)2 + 0.0078P] where P = (Fo2 + 2Fc2)/3 |
1154 reflections | (Δ/σ)max = 0.003 |
95 parameters | Δρmax = 0.22 e Å−3 |
0 restraints | Δρmin = −0.13 e Å−3 |
Special details top Experimental. The data collection nominally covered full sphere of reciprocal space, by a combination of 4 sets of ω scans, each set at different φ and/or 2θ angles and each scan (15 s exposure) covering 0.3° in ω. Crystal to detector distance 4.95 cm. Crystal decay was monitored by repeating the first 50 frames at the end of the data collection and comparing the intensities of 31 duplicate reflections. |
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. H(1) atom (N-bonded) was refined in isotropic approximation (All H-atom parameters refined), other H atoms treated as riding (H-atom parameters constrained). |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
N1 | 0.3970 (5) | 0.31105 (19) | 0.5473 (2) | 0.0746 (7) | |
H1 | 0.260 (9) | 0.365 (3) | 0.577 (3) | 0.123 (11)* | |
C2 | 0.4746 (7) | 0.2227 (3) | 0.59912 (17) | 0.0723 (8) | |
H2 | 0.4203 | 0.2188 | 0.6659 | 0.087* | |
C3 | 0.6325 (7) | 0.1385 (2) | 0.5545 (2) | 0.0721 (8) | |
H3 | 0.6882 | 0.0763 | 0.5902 | 0.086* | |
C4 | 0.7081 (6) | 0.1458 (2) | 0.4579 (2) | 0.0696 (7) | |
H4 | 0.8141 | 0.0879 | 0.4264 | 0.084* | |
C5 | 0.6317 (7) | 0.2356 (2) | 0.40669 (18) | 0.0739 (8) | |
H5 | 0.6891 | 0.2405 | 0.3402 | 0.089* | |
C6 | 0.4739 (7) | 0.3184 (2) | 0.4512 (2) | 0.0713 (8) | |
H6 | 0.4175 | 0.3805 | 0.4156 | 0.086* | |
O1 | 0.0061 (6) | 0.48422 (14) | 0.61596 (12) | 0.0860 (7) | |
O2 | −0.1119 (6) | 0.5580 (2) | 0.75437 (14) | 0.1064 (8) | |
O3 | 0.1348 (6) | 0.4033 (2) | 0.75035 (14) | 0.1090 (8) | |
N2 | 0.0100 (6) | 0.48242 (17) | 0.70861 (15) | 0.0665 (6) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
N1 | 0.0566 (13) | 0.0572 (13) | 0.110 (2) | −0.0043 (10) | 0.0108 (12) | −0.0313 (14) |
C2 | 0.0796 (18) | 0.089 (2) | 0.0482 (14) | −0.0210 (15) | 0.0028 (12) | −0.0044 (13) |
C3 | 0.0750 (18) | 0.0580 (16) | 0.0828 (19) | 0.0013 (13) | −0.0170 (14) | 0.0139 (13) |
C4 | 0.0602 (16) | 0.0644 (17) | 0.0842 (18) | 0.0078 (12) | 0.0030 (13) | −0.0192 (13) |
C5 | 0.0761 (18) | 0.095 (2) | 0.0507 (14) | −0.0087 (15) | 0.0043 (12) | −0.0001 (13) |
C6 | 0.0641 (16) | 0.0586 (16) | 0.091 (2) | −0.0029 (12) | −0.0099 (14) | 0.0235 (13) |
O1 | 0.1372 (18) | 0.0713 (12) | 0.0496 (10) | 0.0160 (11) | 0.0042 (9) | −0.0017 (7) |
O2 | 0.129 (2) | 0.1131 (16) | 0.0774 (13) | 0.0207 (14) | 0.0102 (12) | −0.0367 (11) |
O3 | 0.130 (2) | 0.1229 (18) | 0.0742 (13) | 0.0350 (14) | 0.0169 (12) | 0.0369 (12) |
N2 | 0.0795 (15) | 0.0677 (14) | 0.0524 (12) | −0.0064 (11) | 0.0099 (10) | −0.0057 (10) |
Geometric parameters (Å, º) top N1—C2 | 1.328 (4) | C4—H4 | 0.9300 |
N1—C6 | 1.338 (4) | C5—C6 | 1.337 (4) |
N1—H1 | 0.94 (4) | C5—H5 | 0.9300 |
C2—C3 | 1.352 (4) | C6—H6 | 0.9300 |
C2—H2 | 0.9300 | O1—N2 | 1.251 (2) |
C3—C4 | 1.343 (4) | O2—N2 | 1.217 (3) |
C3—H3 | 0.9300 | O3—N2 | 1.225 (3) |
C4—C5 | 1.337 (4) | | |
| | | |
C2—N1—C6 | 121.0 (2) | C3—C4—H4 | 119.7 |
C2—N1—H1 | 119 (2) | C6—C5—C4 | 120.0 (2) |
C6—N1—H1 | 120 (2) | C6—C5—H5 | 120.0 |
N1—C2—C3 | 119.8 (2) | C4—C5—H5 | 120.0 |
N1—C2—H2 | 120.1 | C5—C6—N1 | 119.5 (2) |
C3—C2—H2 | 120.1 | C5—C6—H6 | 120.3 |
C4—C3—C2 | 119.1 (2) | N1—C6—H6 | 120.2 |
C4—C3—H3 | 120.4 | O2—N2—O3 | 122.1 (2) |
C2—C3—H3 | 120.5 | O2—N2—O1 | 119.5 (2) |
C5—C4—C3 | 120.6 (2) | O3—N2—O1 | 118.4 (2) |
C5—C4—H4 | 119.7 | | |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1 | 0.94 (4) | 1.86 (4) | 2.787 (3) | 171 (3) |
N1—H1···O3 | 0.94 (4) | 2.45 (4) | 3.149 (3) | 131 (3) |
C2—H2···O3 | 0.93 | 2.78 | 3.307 (4) | 117 |
C2—H2···O2i | 0.93 | 2.56 | 3.177 (3) | 124 |
C3—H3···O2ii | 0.93 | 2.67 | 3.324 (3) | 128 |
C4—H4···O3iii | 0.93 | 2.70 | 3.330 (3) | 126 |
C5—H5···O3iii | 0.93 | 2.77 | 3.365 (4) | 123 |
C6—H6···O1iv | 0.93 | 2.38 | 3.196 (3) | 146 |
C6—H6···O2iv | 0.93 | 2.68 | 3.456 (3) | 141 |
Symmetry codes: (i) −x, y−1/2, −z+3/2; (ii) −x+1, y−1/2, −z+3/2; (iii) x+1, −y+1/2, z−1/2; (iv) −x, −y+1, −z+1. |
Acknowledgements
The author thanks Dr I. F. Perepichka for providing single crystals of (I
).
References
Batsanov, A. S. (2004). Acta Cryst. E60, o2426–o2428. CSD CrossRef IUCr Journals Google Scholar
Bruker (2001). SMART (Version 5.625) & SHELXTL (Version 6.12). Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Bruker (2002). SAINT. Version 6.28A. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Serewicz, A. J., Robertson, B. K. & Meyers, E. A. (1965). J. Phys. Chem. 69, 1915–1921. CrossRef CAS Web of Science Google Scholar
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