Abstract
In the title salt, C12H7N2O2 +·NO3 −, the monoprotonated cation is connected to the nitrate anion by a hydrogen bond. Weak C—H⋯O hydrogen bonds hold the planar cations together in a layer structure.
Related literature
For related literature, see Fujihara et al. (2004 ▶); Larsson & Ohström (2004 ▶). For the bromide salt, see: Bomfim et al. (2003 ▶).
Experimental
Crystal data
C12H7N2O2 +·NO3 −
M r = 273.21
Monoclinic,
a = 14.4860 (19) Å
b = 12.5177 (13) Å
c = 13.4535 (16) Å
β = 101.720 (12)°
V = 2388.7 (5) Å3
Z = 8
Mo Kα radiation
μ = 0.12 mm−1
T = 290 (2) K
0.30 × 0.10 × 0.08 mm
Data collection
Oxford Diffraction Xcalibur 3 CCD diffractometer
Absorption correction: numerical (X-RED; Stoe & Cie, 1997 ▶) T min = 0.960, T max = 0.989
7311 measured reflections
2095 independent reflections
635 reflections with I > 2σ(I)
R int = 0.068
Refinement
R[F 2 > 2σ(F 2)] = 0.038
wR(F 2) = 0.060
S = 0.83
2095 reflections
182 parameters
H-atom parameters constrained
Δρmax = 0.31 e Å−3
Δρmin = −0.14 e Å−3
Data collection: CrysAlis CCD (Oxford Diffraction, 2003 ▶); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2003 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997 ▶); molecular graphics: DIAMOND (Brandenburg, 2001 ▶); software used to prepare material for publication: PLATON (Spek, 2003 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536807066172/ng2405sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536807066172/ng2405Isup2.hkl
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—H1⋯O5 | 0.86 | 1.95 | 2.703 (4) | 145 |
| C8—H8⋯O5i | 0.93 | 2.48 | 3.396 (4) | 167 |
| C9—H9⋯O4i | 0.93 | 2.71 | 3.359 (5) | 128 |
| C4—H4⋯O4ii | 0.93 | 2.61 | 3.323 (4) | 134 |
| C3—H3⋯O3ii | 0.93 | 2.40 | 3.209 (4) | 146 |
| C10—H10⋯O1iii | 0.93 | 2.47 | 3.318 (5) | 151 |
| C5—H5⋯O2iv | 0.93 | 2.37 | 3.266 (5) | 162 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
.
Acknowledgments
This work was supported by grants from the University of Tehran and the Swedish Research Council. The authors are grateful to Professor Magnus Sandström for his support.
supplementary crystallographic information
Comment
From a survey of the Cambridge Structural Database [version 5.28, updated Jan. 2007], we found two complexes containing O-protonated pdon (Fujihara, et al., 2004; Larsson, & Ohström, 2004). However, up to now, only one molecule is reported for the N-protonated pdon (C12H7N2O2+, Hpdon) with bromide ions as counter ion (Bomfim et al., 2003).
The molecular structure and atom-labeling scheme for (I) are shown in Fig. 1. There is a relatively strong hydrogen bond between the nitrate ion and to the protonated nitrogen atom in Hpdon (N1—H1···O5, 2.703 (4) Å). Weak C–H···O hydrogen bonds hold the approximately planar cations together in a layer structure (Fig. 2). The packing of the layers is similar to that in the bromide salt of Hpdon (Bomfim et al., 2003) without specific directional interactions between the layers. Ring A (C1–C5/N1), B (C6–C10/N2) and C (C1/C2/C12/C11/C7/C6) in the cation (C12H7N2O2+, Hpdon) is approximately planar. The interplanar angle between the least-square planes defined by ring A and two other rings, B and C, are 1.69 (5)° and 1.17 (5)°, respectively. While, rings B and C are almost planar, 0.52 (5)°. However, the C—N—C angle is affected by protonation and causes to increase from 116.6 (3)° to 122.7 (3)° in the rings B and A, respectively. Similar effect has also been shown in the previously reported Hpdon bromide by increasing from 116.8 (3)° to 123.2 (3)° for the corresponding values. The comparison of the torsion angle, O1—C12—C11—O2, 2.5 (6)°, in (I) with the molecular pdon indicates that the N-protonation in (I) doesn't significantly affect on dione groups.
Experimental
The title compound was obtained during the reaction of thorium nitrate, Th(NO3)4.5H2O (Merck, 99%), and 1,10-phenanthroline-5,6-dione (Aldrich, 97%) in ethanolic solution. Pale-yellow crystals of Hpdon were taken from the obtained greenish precipitates. The presence of water in the ethanolic solution and the high basicity of dione ligand can be the reason for the protonation, providing the C12H7N2O2+, Hpdon cation. Thin fragile layer crystals were obtained by recrystallization from acetonitrile.
Refinement
All H atoms were geometrically positioned and constrained to ride on their parent atoms, with Uiso(H) = 1.2 times Ueq(C,N).
Figures
Fig. 1.
Molecular structure of (I), with 50% probability displacement ellipsoids. H atoms are shown as circles of arbitrary radii.
Fig. 2.
Packing view for (I), showing the hydrogen bonds as dashed lines.
Crystal data
| C12H7N2O2+·NO3– | F000 = 1120 |
| Mr = 273.21 | Dx = 1.519 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 7311 reflections |
| a = 14.4860 (19) Å | θ = 3.5–25.0º |
| b = 12.5177 (13) Å | µ = 0.12 mm−1 |
| c = 13.4535 (16) Å | T = 290 (2) K |
| β = 101.720 (12)º | Needle, pale-yellow |
| V = 2388.7 (5) Å3 | 0.30 × 0.10 × 0.08 mm |
| Z = 8 |
Data collection
| Oxford Diffraction Xcalibur 3 CCD diffractometer | 2095 independent reflections |
| Radiation source: fine-focus sealed tube | 635 reflections with I > 2σ(I) |
| Monochromator: graphite | Rint = 0.068 |
| Detector resolution: 12 pixels mm-1 | θmax = 25.0º |
| T = 290(2) K | θmin = 3.8º |
| ω–scans at different φ | h = −17→17 |
| Absorption correction: numerical(X-RED; Stoe & Cie, 1997) | k = −14→14 |
| Tmin = 0.960, Tmax = 0.989 | l = −10→15 |
| 7311 measured reflections |
Refinement
| Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
| Least-squares matrix: full | H-atom parameters constrained |
| R[F2 > 2σ(F2)] = 0.038 | w = 1/[σ2(Fo2) + (0.01P)2] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.060 | (Δ/σ)max < 0.001 |
| S = 0.83 | Δρmax = 0.31 e Å−3 |
| 2095 reflections | Δρmin = −0.14 e Å−3 |
| 182 parameters | Extinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.00072 (4) |
| Secondary atom site location: difference Fourier map |
Special details
| 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 | ||
| O1 | 0.85417 (17) | −0.13522 (19) | 0.12439 (18) | 0.0673 (8) | |
| O2 | 0.85003 (19) | 0.08376 (19) | 0.1238 (2) | 0.0834 (10) | |
| O3 | 0.30299 (14) | 0.0377 (2) | 0.07097 (16) | 0.0649 (7) | |
| O4 | 0.22236 (15) | −0.03456 (19) | 0.17219 (15) | 0.0613 (6) | |
| O5 | 0.34903 (16) | −0.11186 (18) | 0.14632 (16) | 0.0622 (7) | |
| N1 | 0.52797 (19) | −0.1426 (2) | 0.12265 (18) | 0.0439 (9) | |
| H1 | 0.4776 | −0.1063 | 0.1230 | 0.053* | |
| N2 | 0.5205 (2) | 0.0692 (2) | 0.1274 (2) | 0.0488 (9) | |
| N3 | 0.29121 (19) | −0.0361 (3) | 0.1292 (2) | 0.0476 (8) | |
| C1 | 0.6089 (3) | −0.0896 (3) | 0.1224 (2) | 0.0370 (9) | |
| C2 | 0.6903 (3) | −0.1473 (3) | 0.1211 (2) | 0.0374 (10) | |
| C3 | 0.6870 (3) | −0.2573 (3) | 0.1201 (2) | 0.0528 (11) | |
| H3 | 0.7411 | −0.2969 | 0.1191 | 0.063* | |
| C4 | 0.6018 (3) | −0.3086 (3) | 0.1207 (2) | 0.0550 (11) | |
| H4 | 0.5986 | −0.3828 | 0.1198 | 0.066* | |
| C5 | 0.5228 (3) | −0.2490 (3) | 0.1224 (2) | 0.0502 (11) | |
| H5 | 0.4657 | −0.2826 | 0.1235 | 0.060* | |
| C6 | 0.6062 (3) | 0.0275 (3) | 0.1258 (2) | 0.0380 (9) | |
| C7 | 0.6867 (3) | 0.0879 (3) | 0.1278 (2) | 0.0421 (10) | |
| C8 | 0.6798 (3) | 0.1978 (3) | 0.1312 (2) | 0.0534 (13) | |
| H8 | 0.7320 | 0.2411 | 0.1319 | 0.064* | |
| C9 | 0.5922 (3) | 0.2415 (3) | 0.1336 (2) | 0.0589 (12) | |
| H9 | 0.5852 | 0.3151 | 0.1369 | 0.071* | |
| C10 | 0.5151 (3) | 0.1749 (3) | 0.1308 (3) | 0.0589 (13) | |
| H10 | 0.4568 | 0.2058 | 0.1314 | 0.071* | |
| C11 | 0.7780 (3) | 0.0351 (4) | 0.1244 (2) | 0.0526 (10) | |
| C12 | 0.7807 (3) | −0.0894 (3) | 0.1227 (2) | 0.0469 (11) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0405 (19) | 0.064 (2) | 0.102 (2) | 0.0165 (15) | 0.0270 (16) | 0.0046 (15) |
| O2 | 0.051 (2) | 0.062 (2) | 0.146 (2) | −0.0150 (16) | 0.0412 (18) | −0.0002 (17) |
| O3 | 0.0736 (19) | 0.0573 (18) | 0.0696 (16) | 0.0079 (15) | 0.0282 (13) | 0.0205 (15) |
| O4 | 0.0508 (18) | 0.0664 (15) | 0.0730 (16) | 0.0081 (16) | 0.0276 (13) | 0.0048 (14) |
| O5 | 0.0453 (17) | 0.0477 (18) | 0.0977 (18) | 0.0163 (14) | 0.0242 (14) | 0.0116 (15) |
| N1 | 0.036 (2) | 0.038 (2) | 0.0605 (19) | 0.0038 (18) | 0.0143 (17) | 0.0013 (19) |
| N2 | 0.054 (2) | 0.035 (2) | 0.0620 (19) | 0.0086 (17) | 0.0214 (18) | −0.0027 (17) |
| N3 | 0.041 (2) | 0.051 (2) | 0.053 (2) | −0.005 (2) | 0.0144 (17) | −0.001 (2) |
| C1 | 0.034 (3) | 0.038 (3) | 0.041 (2) | −0.007 (2) | 0.012 (2) | −0.003 (2) |
| C2 | 0.037 (3) | 0.033 (3) | 0.044 (2) | 0.008 (2) | 0.011 (2) | 0.006 (2) |
| C3 | 0.056 (3) | 0.043 (3) | 0.065 (3) | 0.009 (3) | 0.023 (2) | 0.002 (2) |
| C4 | 0.067 (4) | 0.034 (3) | 0.066 (3) | 0.001 (3) | 0.020 (2) | 0.004 (2) |
| C5 | 0.050 (3) | 0.035 (3) | 0.068 (3) | −0.007 (2) | 0.017 (2) | 0.000 (2) |
| C6 | 0.037 (3) | 0.035 (3) | 0.042 (2) | −0.001 (3) | 0.0093 (19) | −0.010 (3) |
| C7 | 0.038 (3) | 0.036 (3) | 0.053 (2) | 0.002 (2) | 0.011 (2) | 0.002 (2) |
| C8 | 0.060 (4) | 0.030 (3) | 0.070 (3) | −0.005 (2) | 0.012 (2) | 0.003 (2) |
| C9 | 0.073 (4) | 0.037 (3) | 0.065 (3) | 0.015 (3) | 0.010 (3) | −0.001 (2) |
| C10 | 0.058 (4) | 0.045 (3) | 0.075 (3) | 0.005 (2) | 0.016 (3) | −0.003 (2) |
| C11 | 0.052 (3) | 0.051 (3) | 0.059 (2) | −0.002 (3) | 0.021 (2) | 0.001 (3) |
| C12 | 0.050 (3) | 0.048 (3) | 0.046 (2) | 0.000 (3) | 0.018 (2) | −0.002 (2) |
Geometric parameters (Å, °)
| O1—C12 | 1.206 (4) | C3—C4 | 1.392 (4) |
| O2—C11 | 1.210 (3) | C3—H3 | 0.9300 |
| O3—N3 | 1.244 (3) | C4—C5 | 1.371 (4) |
| O4—N3 | 1.251 (3) | C4—H4 | 0.9300 |
| O5—N3 | 1.256 (3) | C5—H5 | 0.9300 |
| N1—C5 | 1.335 (4) | C6—C7 | 1.385 (4) |
| N1—C1 | 1.347 (4) | C7—C8 | 1.381 (4) |
| N1—H1 | 0.8600 | C7—C11 | 1.488 (4) |
| N2—C10 | 1.326 (4) | C8—C9 | 1.387 (4) |
| N2—C6 | 1.350 (4) | C8—H8 | 0.9300 |
| C1—C2 | 1.387 (4) | C9—C10 | 1.389 (4) |
| C1—C6 | 1.467 (4) | C9—H9 | 0.9300 |
| C2—C3 | 1.377 (4) | C10—H10 | 0.9300 |
| C2—C12 | 1.492 (4) | C11—C12 | 1.559 (4) |
| C5—N1—C1 | 122.7 (3) | N2—C6—C7 | 124.1 (4) |
| C5—N1—H1 | 118.7 | N2—C6—C1 | 114.7 (4) |
| C1—N1—H1 | 118.7 | C7—C6—C1 | 121.2 (4) |
| C10—N2—C6 | 116.6 (3) | C8—C7—C6 | 118.5 (4) |
| O3—N3—O4 | 120.3 (3) | C8—C7—C11 | 120.9 (4) |
| O3—N3—O5 | 120.3 (3) | C6—C7—C11 | 120.5 (4) |
| O4—N3—O5 | 119.4 (3) | C7—C8—C9 | 117.8 (4) |
| N1—C1—C2 | 119.1 (4) | C7—C8—H8 | 121.1 |
| N1—C1—C6 | 117.6 (4) | C9—C8—H8 | 121.1 |
| C2—C1—C6 | 123.3 (4) | C8—C9—C10 | 119.8 (4) |
| C3—C2—C1 | 119.5 (4) | C8—C9—H9 | 120.1 |
| C3—C2—C12 | 121.0 (4) | C10—C9—H9 | 120.1 |
| C1—C2—C12 | 119.5 (4) | N2—C10—C9 | 123.1 (4) |
| C2—C3—C4 | 119.4 (4) | N2—C10—H10 | 118.4 |
| C2—C3—H3 | 120.3 | C9—C10—H10 | 118.4 |
| C4—C3—H3 | 120.3 | O2—C11—C7 | 123.4 (5) |
| C5—C4—C3 | 119.6 (4) | O2—C11—C12 | 118.6 (4) |
| C5—C4—H4 | 120.2 | C7—C11—C12 | 118.0 (4) |
| C3—C4—H4 | 120.2 | O1—C12—C2 | 122.5 (4) |
| N1—C5—C4 | 119.8 (4) | O1—C12—C11 | 120.0 (4) |
| N1—C5—H5 | 120.1 | C2—C12—C11 | 117.5 (4) |
| C4—C5—H5 | 120.1 | ||
| C5—N1—C1—C2 | 0.5 (5) | N2—C6—C7—C11 | −179.1 (3) |
| C5—N1—C1—C6 | −178.2 (3) | C1—C6—C7—C11 | 1.2 (5) |
| N1—C1—C2—C3 | 0.0 (5) | C6—C7—C8—C9 | 0.7 (5) |
| C6—C1—C2—C3 | 178.6 (3) | C11—C7—C8—C9 | 179.5 (3) |
| N1—C1—C2—C12 | −178.9 (3) | C7—C8—C9—C10 | −1.0 (5) |
| C6—C1—C2—C12 | −0.3 (5) | C6—N2—C10—C9 | −0.5 (5) |
| C1—C2—C3—C4 | −0.1 (5) | C8—C9—C10—N2 | 1.0 (6) |
| C12—C2—C3—C4 | 178.7 (3) | C8—C7—C11—O2 | −0.4 (5) |
| C2—C3—C4—C5 | −0.2 (5) | C6—C7—C11—O2 | 178.4 (3) |
| C1—N1—C5—C4 | −0.8 (5) | C8—C7—C11—C12 | 178.9 (3) |
| C3—C4—C5—N1 | 0.6 (6) | C6—C7—C11—C12 | −2.3 (5) |
| C10—N2—C6—C7 | 0.2 (5) | C3—C2—C12—O1 | −0.9 (5) |
| C10—N2—C6—C1 | 179.8 (3) | C1—C2—C12—O1 | 178.0 (4) |
| N1—C1—C6—N2 | −0.9 (5) | C3—C2—C12—C11 | −179.6 (3) |
| C2—C1—C6—N2 | −179.5 (3) | C1—C2—C12—C11 | −0.8 (4) |
| N1—C1—C6—C7 | 178.7 (3) | O2—C11—C12—O1 | 2.5 (6) |
| C2—C1—C6—C7 | 0.1 (5) | C7—C11—C12—O1 | −176.8 (3) |
| N2—C6—C7—C8 | −0.3 (5) | O2—C11—C12—C2 | −178.6 (3) |
| C1—C6—C7—C8 | −179.9 (3) | C7—C11—C12—C2 | 2.1 (5) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1···O5 | 0.86 | 1.95 | 2.703 (4) | 145 |
| C8—H8···O5i | 0.93 | 2.48 | 3.396 (4) | 167 |
| C9—H9···O4i | 0.93 | 2.71 | 3.359 (5) | 128 |
| C4—H4···O4ii | 0.93 | 2.61 | 3.323 (4) | 134 |
| C3—H3···O3ii | 0.93 | 2.40 | 3.209 (4) | 146 |
| C10—H10···O1iii | 0.93 | 2.47 | 3.318 (5) | 151 |
| C5—H5···O2iv | 0.93 | 2.37 | 3.266 (5) | 162 |
Symmetry codes: (i) x+1/2, y+1/2, z; (ii) x+1/2, y−1/2, z; (iii) x−1/2, y+1/2, z; (iv) x−1/2, y−1/2, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG2405).
References
- Bomfim, J. A. S., Filgueiras, C. A. L., Howie, R. A. & Wardell, J. L. (2003). Acta Cryst. E59, o244–o246. [DOI] [PubMed]
- Brandenburg, K. (2001). DIAMOND Version 2.1e. Crystal Impact GbR, Bonn, Germany.
- Fujihara, T., Wada, T. & Tanaka, K. (2004). Dalton Trans. pp. 645–652. [DOI] [PubMed]
- Larsson, K. & Ohström, L. (2004). Inorg. Chim. Acta, 357, 657–664.
- Oxford Diffraction (2003). CrysAlis CCD and CrysAlis RED Versions 1.171.29.2. Oxford Diffraction Ltd, Abingdon, Oxfordshire, England.
- Sheldrick, G. M. (1997). SHELXS97 and SHELXL97 University of Göttingen, Germany.
- Spek, A. L. (2003). J. Appl. Cryst.36, 7–13.
- Stoe & Cie (1997). X-RED Version 1.09. Stoe & Cie GmbH, Darmstadt, Germany.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536807066172/ng2405sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536807066172/ng2405Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


