organic compounds
Pyridinium nitrate at 290 K
aDepartment of Chemistry, University of Durham, South Road, Durham DH1 3LE, England
*Correspondence e-mail: a.s.batsanov@durham.ac.uk
A previous structural study [Serewicz et al. (1965). J. Phys. Chem. 69, 1915–1921] of pyridinium nitrate, C5H6N+·NO3−, has been repeated at 290 K.
Comment
The ), as determined by Serewicz et al. (1965), implied the existence of a strong hydrogen bond between the pyridinium and nitrate ions, but the precision of the data (measured at room temperature by the Weissenberg method) was insufficient to locate H atoms directly. We have redetermined this structure at two temperatures in the course of screening for materials suitable for neutron-diffraction and charge-density studies of hydrogen bonds. The 290 K structure (Fig. 1 and Table 1) is reported here. The results reported by Serewicz et al. (1965) are essentially confirmed, though the is slightly larger than reported previously (without s.u. values): a = 3.905, b = 12.286, c = 13.470 Å, β = 90.5° and V = 646 Å3.
of pyridinium nitrate, (IFor the low-temperature results and the general discussion, see Batsanov (2004).
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.
Crystal data
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Data collection
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Refinement
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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 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
https://doi.org/10.1107/S1600536804030168/lh6318sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536804030168/lh6318Isup2.hkl
Data collection: SMART (Bruker, 2001); cell
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.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 |
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 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 |
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). |
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) |
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) |
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 |
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. |
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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