Abstract
The title compound, C10H10N8, resides on a crystallographic symmetry center and features an essentially planar molecule [r.m.s. deviation = 0.278 (1) Å]. In the C=N—N=C fragment, the C=N distance is 1.3017 (18) Å and the N—N distance is 1.403 (2) Å. In the crystal, adjacent molecules are linked by N—H⋯N hydrogen bonds into a three-dimensional network.
Related literature
For related structures, see: Armstrong et al. (1998 ▶), Xu et al. (2006 ▶), Shi et al. (2008 ▶).
Experimental
Crystal data
C10H10N8
M r = 242.26
Monoclinic,
a = 8.6576 (16) Å
b = 6.6685 (12) Å
c = 9.6162 (18) Å
β = 97.682 (4)°
V = 550.19 (18) Å3
Z = 2
Mo Kα radiation
μ = 0.10 mm−1
T = 295 K
0.30 × 0.19 × 0.16 mm
Data collection
Bruker SMART CCD diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 2000 ▶) T min = 0.970, T max = 0.984
1946 measured reflections
946 independent reflections
844 reflections with I > 2σ(I)
R int = 0.013
Refinement
R[F 2 > 2σ(F 2)] = 0.038
wR(F 2) = 0.108
S = 1.05
946 reflections
90 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.20 e Å−3
Δρmin = −0.13 e Å−3
Data collection: SMART (Bruker, 2000 ▶); cell refinement: SAINT (Bruker, 2000 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809027834/bt5007sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809027834/bt5007Isup2.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 |
|---|---|---|---|---|
| N3—H3B⋯N2i | 0.906 (18) | 2.280 (18) | 3.0539 (18) | 143.2 (14) |
| N3—H3C⋯N4ii | 0.892 (19) | 2.405 (18) | 3.1587 (18) | 142.3 (16) |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The authors thank the Program for Young Excellent Talents in Southeast University for financial support.
supplementary crystallographic information
Comment
The title compound can be regarded as a dihydrazidine with all atoms essentially coplanar and has now been shown to have trans geometry because of steric repulsion effect. In the C=N—N=C fragment, the C=N distance is 1.302 (2) Å, which is much shorter than the N—N distance of 1.403 (2) Å. All other C—N distances are 1.341 (2) Å, which are considered to have full double-bond character. Adjacent molecules are linked into a two-dimensional sheet by intermolecular N—H···N hydrogen bonds with the N···N distance of 3.054 (2) Å. Each molecule acts as double hydrogen-bond acceptors with the 2-positon N atoms of pyrazine rings and donors with the two amino groups.
Experimental
A mixture of pyrazine-2-carbonitrile (0.210 g, 2 mmol), MnSO4.H2O (0.169 g, 1 mmol), hydrazine hydrate (80%, 2 ml) and anhydrous ethanol (6 ml) was heated in a 15 ml Teflon-lined autoclave at 393 K for 3 days, followed by slow cooling (5 K h-1) to room temperature. The resulting mixture was filtered and washed with 95% ethanol, and yellow block crystals were collected and dried in vacuum. Yield (0.32 g) 26.4%.
Refinement
The H atom bonded to N were located in a difference map and freely refined. Other H atoms were positioned geometrically and refined using a riding model with C—H = 0.93 Å and with Uiso(H) = 1.2 Ueq(C).
Figures
Fig. 1.
Structure of the title compound with 30% displacement ellipsoids. [Symmetry code: (A) 2-x, -1-y, -z.]
Crystal data
| C10H10N8 | F(000) = 252 |
| Mr = 242.26 | Dx = 1.462 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 651 reflections |
| a = 8.6576 (16) Å | θ = 3.9–26.5° |
| b = 6.6685 (12) Å | µ = 0.10 mm−1 |
| c = 9.6162 (18) Å | T = 295 K |
| β = 97.682 (4)° | Block, yellow |
| V = 550.19 (18) Å3 | 0.30 × 0.19 × 0.16 mm |
| Z = 2 |
Data collection
| Bruker SMART CCD diffractometer | 946 independent reflections |
| Radiation source: fine-focus sealed tube | 844 reflections with I > 2σ(I) |
| graphite | Rint = 0.013 |
| φ and ω scans | θmax = 25.0°, θmin = 2.4° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 2000) | h = −10→4 |
| Tmin = 0.970, Tmax = 0.984 | k = −7→7 |
| 1946 measured reflections | l = −11→11 |
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)] = 0.038 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.108 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0659P)2 + 0.0834P] where P = (Fo2 + 2Fc2)/3 |
| 946 reflections | (Δ/σ)max < 0.001 |
| 90 parameters | Δρmax = 0.20 e Å−3 |
| 0 restraints | Δρmin = −0.13 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 | ||
| C1 | 0.71263 (17) | −0.1470 (2) | −0.12888 (15) | 0.0400 (4) | |
| H1A | 0.7177 | −0.2641 | −0.1806 | 0.048* | |
| C2 | 0.61260 (19) | 0.1595 (2) | −0.10119 (17) | 0.0459 (4) | |
| H2A | 0.5502 | 0.2669 | −0.1353 | 0.055* | |
| C3 | 0.69636 (18) | 0.1731 (2) | 0.03029 (16) | 0.0421 (4) | |
| H3A | 0.6851 | 0.2866 | 0.0842 | 0.050* | |
| C4 | 0.80524 (15) | −0.1312 (2) | 0.00078 (14) | 0.0326 (4) | |
| C5 | 0.92285 (16) | −0.2845 (2) | 0.05271 (14) | 0.0322 (4) | |
| N1 | 0.61789 (15) | −0.0024 (2) | −0.18134 (13) | 0.0462 (4) | |
| N2 | 0.79325 (14) | 0.02862 (18) | 0.08288 (12) | 0.0372 (4) | |
| N3 | 1.00358 (16) | −0.2540 (2) | 0.17988 (13) | 0.0431 (4) | |
| H3B | 1.071 (2) | −0.351 (3) | 0.2148 (18) | 0.045 (4)* | |
| H3C | 0.974 (2) | −0.154 (3) | 0.2320 (19) | 0.050 (5)* | |
| N4 | 0.94266 (14) | −0.43331 (17) | −0.03069 (11) | 0.0356 (4) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0420 (8) | 0.0408 (8) | 0.0350 (8) | 0.0018 (6) | −0.0029 (6) | −0.0042 (7) |
| C2 | 0.0441 (9) | 0.0435 (9) | 0.0475 (9) | 0.0069 (7) | −0.0038 (7) | 0.0066 (7) |
| C3 | 0.0468 (9) | 0.0355 (8) | 0.0426 (9) | 0.0047 (6) | 0.0013 (7) | −0.0023 (7) |
| C4 | 0.0353 (8) | 0.0329 (8) | 0.0295 (7) | −0.0030 (6) | 0.0039 (6) | 0.0006 (6) |
| C5 | 0.0363 (8) | 0.0316 (7) | 0.0280 (7) | −0.0025 (6) | 0.0017 (6) | 0.0015 (6) |
| N1 | 0.0459 (8) | 0.0486 (8) | 0.0405 (8) | 0.0040 (6) | −0.0078 (6) | 0.0010 (6) |
| N2 | 0.0429 (7) | 0.0339 (7) | 0.0335 (7) | 0.0024 (5) | −0.0002 (5) | −0.0018 (5) |
| N3 | 0.0534 (9) | 0.0409 (8) | 0.0317 (7) | 0.0145 (6) | −0.0068 (6) | −0.0050 (6) |
| N4 | 0.0425 (7) | 0.0312 (7) | 0.0313 (7) | 0.0042 (5) | −0.0016 (5) | −0.0001 (5) |
Geometric parameters (Å, °)
| C1—N1 | 1.3219 (19) | C4—N2 | 1.3386 (18) |
| C1—C4 | 1.393 (2) | C4—C5 | 1.4815 (19) |
| C1—H1A | 0.9300 | C5—N4 | 1.3017 (18) |
| C2—N1 | 1.331 (2) | C5—N3 | 1.3405 (18) |
| C2—C3 | 1.374 (2) | N3—H3B | 0.906 (18) |
| C2—H2A | 0.9300 | N3—H3C | 0.893 (19) |
| C3—N2 | 1.3318 (19) | N4—N4i | 1.403 (2) |
| C3—H3A | 0.9300 | ||
| N1—C1—C4 | 122.66 (14) | C1—C4—C5 | 122.46 (13) |
| N1—C1—H1A | 118.7 | N4—C5—N3 | 125.59 (13) |
| C4—C1—H1A | 118.7 | N4—C5—C4 | 117.36 (12) |
| N1—C2—C3 | 122.11 (14) | N3—C5—C4 | 117.01 (13) |
| N1—C2—H2A | 118.9 | C1—N1—C2 | 116.02 (13) |
| C3—C2—H2A | 118.9 | C3—N2—C4 | 116.52 (12) |
| N2—C3—C2 | 122.01 (14) | C5—N3—H3B | 117.6 (10) |
| N2—C3—H3A | 119.0 | C5—N3—H3C | 118.3 (11) |
| C2—C3—H3A | 119.0 | H3B—N3—H3C | 123.0 (15) |
| N2—C4—C1 | 120.49 (13) | C5—N4—N4i | 111.61 (13) |
| N2—C4—C5 | 117.03 (12) |
Symmetry codes: (i) −x+2, −y−1, −z.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N3—H3B···N2ii | 0.906 (18) | 2.280 (18) | 3.0539 (18) | 143.2 (14) |
| N3—H3C···N4iii | 0.892 (19) | 2.405 (18) | 3.1587 (18) | 142.3 (16) |
Symmetry codes: (ii) −x+2, y−1/2, −z+1/2; (iii) x, −y−1/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5007).
References
- Armstrong, J. A., Barnes, J. C. & Weakley, T. J. R. (1998). Acta Cryst. C54, 1923–1925.
- Bruker (2000). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
- Sheldrick, G. M. (2000). SADABS University of Göttingen, Germany.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Shi, S., Yao, T., Geng, X., Chen, L. & Ji, L. (2008). Acta Cryst. E64, o272. [DOI] [PMC free article] [PubMed]
- Xu, R.-H., Zhou, J., Xu, Y., Qi, L., Shen, X. & Zhu, D.-R. (2006). Acta Cryst. E62, o5234–o5235.
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/S1600536809027834/bt5007sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809027834/bt5007Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

