Abstract
In the unit cell of the title compound, C5H7N3O, there are two conformers (A and B) which differ in the position of the oxime group with respect to the protonated pyrazole nitrogen (trans in the A conformer and cis in the B conformer) and in the geometric parameters. The oxime group exists in the nitroso form in both conformers. In the crystal, molecules are linked by intermolecular N—H⋯O and N—H⋯N hydrogen bonds into zigzag-like chains along the b axis.
Related literature
For the use of pyrazole-based ligands, see: Mullins & Pecoraro (2008 ▶); Mukhopadhyay et al. (2004 ▶). For the magnetic properties of pyrazolate complexes, see: Aromi & Brechin (2006 ▶); Gatteschi et al. (2006 ▶). For the use of oxime substituents in the synthesis of polynuclear ligands, see: Petrusenko et al. (1997 ▶); Kanderal et al. (2005 ▶); Sachse et al. (2008 ▶); Moroz et al. (2010 ▶). For the use of 4-nitropyrazoles as ligands, see: Halcrow (2005 ▶). For related structures, see: Fletcher et al. (1997 ▶); Kovbasyuk et al. (2004 ▶); Mokhir et al. (2002 ▶); Sliva et al. (1997 ▶); Wörl, Fritsky et al. (2005 ▶); Wörl, Pritzkow et al. (2005 ▶). For the synthesis of the title compound, see: Cameron et al. (1996 ▶).
Experimental
Crystal data
C5H7N3O
M r = 125.14
Monoclinic,
a = 4.0268 (2) Å
b = 15.3793 (7) Å
c = 19.6627 (9) Å
β = 94.613 (3)°
V = 1213.75 (10) Å3
Z = 8
Mo Kα radiation
μ = 0.10 mm−1
T = 120 K
0.46 × 0.33 × 0.13 mm
Data collection
Nonius KappaCCD diffractometer
Absorption correction: multi-scan (DENZO/SCALEPACK; Otwinowski & Minor, 1997 ▶) T min = 0.955, T max = 0.987
9003 measured reflections
2747 independent reflections
1866 reflections with I > 2σ(I)
R int = 0.040
Refinement
R[F 2 > 2σ(F 2)] = 0.041
wR(F 2) = 0.109
S = 1.03
2747 reflections
175 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.23 e Å−3
Δρmin = −0.25 e Å−3
Data collection: COLLECT (Nonius, 2000 ▶); cell refinement: DENZO/SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO/SCALEPACK; program(s) used to solve structure: SIR2004 (Burla et al., 2005 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg, 2008 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811033794/jh2317sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811033794/jh2317Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811033794/jh2317Isup3.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 |
|---|---|---|---|---|
| N1B—H1B⋯O1Ai | 0.954 (18) | 1.802 (18) | 2.7526 (16) | 174.0 (15) |
| N1A—H1A⋯N2Bii | 0.915 (19) | 1.95 (2) | 2.8544 (18) | 171.5 (16) |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
Financial support from the State Fund for Fundamental Research of Ukraine (grant No. F40.3/041) and the Swedish Institute (Visby Program) is gratefully acknowledged.
supplementary crystallographic information
Comment
Pyrazole-based ligands are widely used in bioinorganic chemistry, molecular magnetism and supramolecular chemistry, as they are able to form different architectures, ranging from polynuclear clusters to metallocycles (Mullins, et al., 2008; Mukhopadhyay, et al., 2004). In addition to the ability to bridge two or more metal ions, pyrazole ligands also provide an effective magnetic exchange pathway between them (Aromi et al. 2006; Gatteschi, et al., 2006). The incorporation of other coordinating groups to the pyrazole ring can increase the variety of polynuclear compounds that can be formed. For example, introduction of the potentially bridging oxime group in the molecules of the ligands already having bridging moieties (such as pyrazolates) can lead to increase of nuclearity and complexity of the metal complexes on their basis (Petrusenko et al., 1997; Kanderal et al., 2005; Sachse et al., 2008; Moroz et al., 2010). In this work, we report the crystal structure of the title compound which contains the oxime group in the 4-position of the pyrazole ring. Unlike 4-nitropyrazoles which have been widely used for preparation of oligonuclear metal complexes (Halcrow et al., 2005), 4-nitrosopyrazoles have never been studied as ligands, and no metal complexes based on this type of ligands have been reported up to date. Crystal and molecular structures of only two 4-nitrosopyrazoles have been reported before (Cameron et al., 1996; Fletcher et al., 1997).
In the unit cell there are two types of conformers (A and B) of the title compound which differs significantly by the geometrical parameters and by the position of the oxime group with respect to the protonated pyrazole nitrogen (Fig. 1). In the conformer A, the oxime group is trans- with respect to the pyrazole hydrogen, while in the conformer B the oxime-group is cis-situated. In the conformers A and B the bond lengths markedly differs, first of all it is noticeable upon comparing the interatomic distances within the oxime groups. In the conformer B, the difference in bond lengths between C—N (1.3902 (19) Å) and N=O (1.2412 (16) Å) bonds of the oxime groups is quite large (ca 0.15 Å) while in the conformer A (C—N 1.3553 (19) Å and N=O 1.2701 (16) Å) it is much less pronounced (less than 0.08 Å). This clearly indicates that the CNO moiety in both conformers exists in the nitroso-form (Sliva et al. (1997); Mokhir et al., 2002), however, in the conformer A there is a noticeable contribution of the isonitroso-form. Such a difference can be a consequence of the involvement of the oxime oxygen O1A in formation of the intermolecular H-bond, while O1B does not participate in any H-bond (Table 1).
The differences in geometrical and electronic structure of the oxime groups significantly influence on the C—C, C—N, N—N bond lengths within the pyrazole rings which are deviated from normal values (Kovbasyuk et al., 2004; Wörl, Fritsky et al., 2005; Wörl, Pritzkow et al., 2005). Thus, there are signs of conjugation of the C(3B)—C(4B) bond with the O(1B)—N(3B) bond which results in noticeable shortening of the former (1.405 (2) Å) as compare to that observed in the conformer A, C(3)—C(4) = 1.442 (2) Å.
In the crystal, the molecules are linked by intermolecular N—H···O and N—H···N hydrogen bonds building zigzag chains along the b axis (Fig.2, Table 1). The translational along a axis chains form walls which are united into the crystal by van der Waals interactions.
Experimental
3,5-dimethyl-4-nitrozo-1H-pyrazole was synthesized by using a literature procedure (Cameron et al., 1996) from acetylacetone, sodium nitrite and hydrazine hydrate in aqueous hydrochloric acid. The crude product was collected by filtration and purified by recrystallization from benzene. Colorless crystals suitable for the X-ray diffraction were obtained after several hours (yield 78%).
Refinement
The aromatic NH H atoms were located from the difference Fourier map and refined isotropically. Other H atoms were positioned geometrically and allowed to ride on their parent atoms, with C—H = 0.98 Å, and Uiso = 1.5 Ueq (parent atom).
Figures
Fig. 1.
The two independent molecules of (I) in the unit cell, showing the atom numbering scheme.
Fig. 2.
The crystal packing of the title compound showing the intermolecular hydrogen bonds by dashed lines.
Crystal data
| C5H7N3O | F(000) = 528 |
| Mr = 125.14 | Dx = 1.370 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 4238 reflections |
| a = 4.0268 (2) Å | θ = 1.0–27.5° |
| b = 15.3793 (7) Å | µ = 0.10 mm−1 |
| c = 19.6627 (9) Å | T = 120 K |
| β = 94.613 (3)° | Plate, blue |
| V = 1213.75 (10) Å3 | 0.46 × 0.33 × 0.13 mm |
| Z = 8 |
Data collection
| Nonius KappaCCD diffractometer | 2747 independent reflections |
| Radiation source: fine-focus sealed tube | 1866 reflections with I > 2σ(I) |
| horizontally mounted graphite crystal | Rint = 0.040 |
| Detector resolution: 9 pixels mm-1 | θmax = 27.4°, θmin = 2.5° |
| φ scans and ω scans with κ offset | h = −4→5 |
| Absorption correction: multi-scan (DENZO/SCALEPACK; Otwinowski & Minor, 1997) | k = −18→19 |
| Tmin = 0.955, Tmax = 0.987 | l = −25→25 |
| 9003 measured reflections |
Refinement
| 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)] = 0.041 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.109 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.03 | w = 1/[σ2(Fo2) + (0.0516P)2 + 0.0988P] where P = (Fo2 + 2Fc2)/3 |
| 2747 reflections | (Δ/σ)max < 0.001 |
| 175 parameters | Δρmax = 0.23 e Å−3 |
| 0 restraints | Δρmin = −0.25 e Å−3 |
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 | ||
| O1A | −0.1796 (3) | 0.16615 (7) | 0.22546 (5) | 0.0279 (3) | |
| N1A | 0.3665 (3) | −0.05073 (9) | 0.32527 (7) | 0.0241 (3) | |
| N2A | 0.4403 (3) | 0.02548 (8) | 0.36162 (6) | 0.0243 (3) | |
| N3A | −0.1316 (3) | 0.08489 (8) | 0.22016 (7) | 0.0240 (3) | |
| C1A | 0.2710 (3) | 0.08712 (10) | 0.32773 (8) | 0.0210 (4) | |
| C2A | 0.2872 (4) | 0.17879 (10) | 0.35059 (8) | 0.0258 (4) | |
| H2A | 0.4408 | 0.1837 | 0.3917 | 0.039* | |
| H2B | 0.0648 | 0.1981 | 0.3609 | 0.039* | |
| H2C | 0.3667 | 0.2152 | 0.3144 | 0.039* | |
| C3A | 0.0867 (4) | 0.05016 (9) | 0.26876 (8) | 0.0202 (4) | |
| C4A | 0.1598 (4) | −0.03950 (10) | 0.27044 (8) | 0.0225 (4) | |
| C5A | 0.0466 (4) | −0.11093 (10) | 0.22306 (9) | 0.0308 (4) | |
| H5A | 0.1902 | −0.1133 | 0.1852 | 0.046* | |
| H5B | −0.1839 | −0.1001 | 0.2052 | 0.046* | |
| H5C | 0.0589 | −0.1664 | 0.2476 | 0.046* | |
| O1B | −0.2132 (3) | 0.13230 (7) | −0.04852 (6) | 0.0356 (3) | |
| N1B | 0.3699 (3) | 0.21423 (8) | 0.11942 (7) | 0.0216 (3) | |
| N2B | 0.3158 (3) | 0.30207 (8) | 0.10938 (7) | 0.0226 (3) | |
| N3B | −0.1646 (3) | 0.20960 (9) | −0.03253 (7) | 0.0275 (3) | |
| C1B | 0.1150 (4) | 0.30759 (10) | 0.05258 (8) | 0.0214 (4) | |
| C2B | 0.0044 (4) | 0.39331 (10) | 0.02337 (8) | 0.0267 (4) | |
| H2B1 | 0.0884 | 0.4400 | 0.0540 | 0.040* | |
| H2B2 | −0.2395 | 0.3953 | 0.0182 | 0.040* | |
| H2B3 | 0.0918 | 0.4009 | −0.0213 | 0.040* | |
| C3B | 0.0397 (4) | 0.22318 (10) | 0.02693 (7) | 0.0201 (3) | |
| C4B | 0.2123 (4) | 0.16456 (10) | 0.07173 (8) | 0.0208 (4) | |
| C5B | 0.2411 (4) | 0.06867 (10) | 0.07173 (8) | 0.0264 (4) | |
| H5B1 | 0.3957 | 0.0502 | 0.1100 | 0.040* | |
| H5B2 | 0.3250 | 0.0494 | 0.0288 | 0.040* | |
| H5B3 | 0.0216 | 0.0428 | 0.0763 | 0.040* | |
| H1A | 0.453 (4) | −0.1013 (13) | 0.3437 (9) | 0.040 (5)* | |
| H1B | 0.515 (4) | 0.1949 (11) | 0.1572 (9) | 0.035 (5)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1A | 0.0312 (6) | 0.0231 (6) | 0.0288 (7) | 0.0049 (5) | −0.0017 (5) | 0.0031 (5) |
| N1A | 0.0283 (7) | 0.0183 (7) | 0.0252 (8) | 0.0026 (6) | −0.0006 (6) | 0.0023 (6) |
| N2A | 0.0268 (7) | 0.0221 (8) | 0.0236 (7) | 0.0000 (6) | 0.0000 (6) | 0.0000 (6) |
| N3A | 0.0240 (7) | 0.0244 (8) | 0.0236 (7) | 0.0010 (6) | 0.0024 (6) | 0.0034 (6) |
| C1A | 0.0187 (8) | 0.0230 (9) | 0.0216 (8) | 0.0002 (6) | 0.0028 (6) | 0.0019 (6) |
| C2A | 0.0259 (8) | 0.0246 (9) | 0.0261 (9) | 0.0004 (7) | −0.0024 (7) | −0.0031 (7) |
| C3A | 0.0198 (8) | 0.0204 (8) | 0.0205 (8) | −0.0002 (6) | 0.0023 (6) | 0.0010 (6) |
| C4A | 0.0224 (8) | 0.0218 (9) | 0.0235 (9) | −0.0005 (7) | 0.0039 (7) | 0.0021 (6) |
| C5A | 0.0352 (9) | 0.0228 (9) | 0.0337 (10) | −0.0011 (7) | −0.0005 (8) | −0.0046 (7) |
| O1B | 0.0459 (7) | 0.0269 (7) | 0.0328 (7) | −0.0057 (6) | −0.0044 (6) | −0.0041 (5) |
| N1B | 0.0249 (7) | 0.0172 (7) | 0.0222 (7) | 0.0014 (6) | −0.0014 (6) | 0.0019 (5) |
| N2B | 0.0270 (7) | 0.0153 (7) | 0.0250 (7) | 0.0008 (5) | −0.0008 (6) | 0.0011 (5) |
| N3B | 0.0295 (7) | 0.0247 (8) | 0.0280 (8) | −0.0038 (6) | 0.0007 (6) | −0.0014 (6) |
| C1B | 0.0220 (8) | 0.0203 (8) | 0.0223 (8) | 0.0005 (6) | 0.0037 (7) | 0.0001 (6) |
| C2B | 0.0308 (9) | 0.0205 (8) | 0.0282 (9) | 0.0013 (7) | −0.0010 (7) | 0.0030 (7) |
| C3B | 0.0212 (8) | 0.0194 (8) | 0.0198 (8) | −0.0005 (6) | 0.0020 (6) | 0.0002 (6) |
| C4B | 0.0204 (8) | 0.0211 (8) | 0.0214 (8) | −0.0018 (6) | 0.0041 (7) | −0.0013 (6) |
| C5B | 0.0313 (9) | 0.0184 (8) | 0.0294 (9) | 0.0012 (7) | 0.0017 (7) | −0.0003 (7) |
Geometric parameters (Å, °)
| O1A—N3A | 1.2701 (16) | O1B—N3B | 1.2412 (16) |
| N1A—C4A | 1.319 (2) | N1B—C4B | 1.330 (2) |
| N1A—N2A | 1.3922 (18) | N1B—N2B | 1.3801 (17) |
| N1A—H1A | 0.915 (19) | N1B—H1B | 0.954 (18) |
| N2A—C1A | 1.3170 (19) | N2B—C1B | 1.3279 (19) |
| N3A—C3A | 1.3553 (19) | N3B—C3B | 1.3902 (19) |
| C1A—C3A | 1.442 (2) | C1B—C3B | 1.417 (2) |
| C1A—C2A | 1.479 (2) | C1B—C2B | 1.492 (2) |
| C2A—H2A | 0.9800 | C2B—H2B1 | 0.9800 |
| C2A—H2B | 0.9800 | C2B—H2B2 | 0.9800 |
| C2A—H2C | 0.9800 | C2B—H2B3 | 0.9800 |
| C3A—C4A | 1.410 (2) | C3B—C4B | 1.405 (2) |
| C4A—C5A | 1.488 (2) | C4B—C5B | 1.479 (2) |
| C5A—H5A | 0.9800 | C5B—H5B1 | 0.9800 |
| C5A—H5B | 0.9800 | C5B—H5B2 | 0.9800 |
| C5A—H5C | 0.9800 | C5B—H5B3 | 0.9800 |
| C4A—N1A—N2A | 113.82 (13) | C4B—N1B—N2B | 113.61 (12) |
| C4A—N1A—H1A | 129.1 (11) | C4B—N1B—H1B | 126.7 (10) |
| N2A—N1A—H1A | 116.9 (11) | N2B—N1B—H1B | 119.7 (10) |
| C1A—N2A—N1A | 105.42 (12) | C1B—N2B—N1B | 105.14 (12) |
| O1A—N3A—C3A | 115.11 (12) | O1B—N3B—C3B | 115.32 (13) |
| N2A—C1A—C3A | 109.56 (13) | N2B—C1B—C3B | 109.83 (13) |
| N2A—C1A—C2A | 121.60 (13) | N2B—C1B—C2B | 121.54 (13) |
| C3A—C1A—C2A | 128.84 (13) | C3B—C1B—C2B | 128.62 (14) |
| C1A—C2A—H2A | 109.5 | C1B—C2B—H2B1 | 109.5 |
| C1A—C2A—H2B | 109.5 | C1B—C2B—H2B2 | 109.5 |
| H2A—C2A—H2B | 109.5 | H2B1—C2B—H2B2 | 109.5 |
| C1A—C2A—H2C | 109.5 | C1B—C2B—H2B3 | 109.5 |
| H2A—C2A—H2C | 109.5 | H2B1—C2B—H2B3 | 109.5 |
| H2B—C2A—H2C | 109.5 | H2B2—C2B—H2B3 | 109.5 |
| N3A—C3A—C4A | 121.63 (13) | N3B—C3B—C4B | 131.33 (14) |
| N3A—C3A—C1A | 132.39 (14) | N3B—C3B—C1B | 122.16 (14) |
| C4A—C3A—C1A | 105.89 (13) | C4B—C3B—C1B | 106.50 (13) |
| N1A—C4A—C3A | 105.30 (13) | N1B—C4B—C3B | 104.92 (13) |
| N1A—C4A—C5A | 123.80 (14) | N1B—C4B—C5B | 122.65 (14) |
| C3A—C4A—C5A | 130.89 (14) | C3B—C4B—C5B | 132.42 (14) |
| C4A—C5A—H5A | 109.5 | C4B—C5B—H5B1 | 109.5 |
| C4A—C5A—H5B | 109.5 | C4B—C5B—H5B2 | 109.5 |
| H5A—C5A—H5B | 109.5 | H5B1—C5B—H5B2 | 109.5 |
| C4A—C5A—H5C | 109.5 | C4B—C5B—H5B3 | 109.5 |
| H5A—C5A—H5C | 109.5 | H5B1—C5B—H5B3 | 109.5 |
| H5B—C5A—H5C | 109.5 | H5B2—C5B—H5B3 | 109.5 |
| C4A—N1A—N2A—C1A | 0.03 (17) | C4B—N1B—N2B—C1B | −0.10 (17) |
| N1A—N2A—C1A—C3A | −0.15 (16) | N1B—N2B—C1B—C3B | 0.46 (17) |
| N1A—N2A—C1A—C2A | −179.56 (13) | N1B—N2B—C1B—C2B | −178.40 (13) |
| O1A—N3A—C3A—C4A | 178.61 (13) | O1B—N3B—C3B—C4B | 2.4 (2) |
| O1A—N3A—C3A—C1A | 2.4 (2) | O1B—N3B—C3B—C1B | −179.01 (14) |
| N2A—C1A—C3A—N3A | 176.84 (15) | N2B—C1B—C3B—N3B | −179.59 (13) |
| C2A—C1A—C3A—N3A | −3.8 (3) | C2B—C1B—C3B—N3B | −0.8 (2) |
| N2A—C1A—C3A—C4A | 0.22 (16) | N2B—C1B—C3B—C4B | −0.65 (17) |
| C2A—C1A—C3A—C4A | 179.57 (15) | C2B—C1B—C3B—C4B | 178.11 (15) |
| N2A—N1A—C4A—C3A | 0.11 (17) | N2B—N1B—C4B—C3B | −0.30 (16) |
| N2A—N1A—C4A—C5A | 179.38 (14) | N2B—N1B—C4B—C5B | 178.69 (13) |
| N3A—C3A—C4A—N1A | −177.26 (14) | N3B—C3B—C4B—N1B | 179.36 (15) |
| C1A—C3A—C4A—N1A | −0.19 (16) | C1B—C3B—C4B—N1B | 0.56 (16) |
| N3A—C3A—C4A—C5A | 3.5 (3) | N3B—C3B—C4B—C5B | 0.5 (3) |
| C1A—C3A—C4A—C5A | −179.39 (16) | C1B—C3B—C4B—C5B | −178.29 (15) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1B—H1B···O1Ai | 0.954 (18) | 1.802 (18) | 2.7526 (16) | 174.0 (15) |
| N1A—H1A···N2Bii | 0.915 (19) | 1.95 (2) | 2.8544 (18) | 171.5 (16) |
Symmetry codes: (i) x+1, y, z; (ii) −x+1, y−1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JH2317).
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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) I, global. DOI: 10.1107/S1600536811033794/jh2317sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811033794/jh2317Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811033794/jh2317Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


