supplementary materials


fj2106 scheme

Acta Cryst. (2008). E64, o745    [ doi:10.1107/S1600536808007514 ]

2,4-Dinitrobenzaldehyde hydrazone

N. Zhang, R. Wang, C. Tan, Y. Jiang and Y. Zhao

Abstract top

The title compound, C7H6N4O4, plays an important role in the synthesis of biologically active compounds. The planar hydrazone group is oriented at a dihedral angle of 8.27 (3)° with respect to the benzene ring. In the crystal structure, intermolecular N-H...O and N-H...N hydrogen bonds link the molecules.

Comment top

Benzaldehyde hydrazone and its analogues are important intermediates in heterocyclic chemistry, and they have been widely used for the synthesis of biologically active compounds such as [1,2,4]triazino[6,5-f]quinolines, pyrazolo[3,4-f]quinolines (Kawakami et al., 2000), 1,3-dithiol-2-ylidene derivatives (Moreno-Mañas et al., 2001), and oligo-RNAs with photocaged adenosine 2'-hydroxyls (Chaulk et al., 2007). Here we report the synthesis and crystal structure of a nitro-analogue: 2,4-dinitrobenzaldehyde hydrazone. The molecule of the title compound (Fig. 1) contains a benzene ring, a hydrazone chain and two nitryl groups. Most of the bond lengths and angles are within normal ranges (Allen et al., 1987). Because of the pi-pi conjugation and two nitryl groups electron withdrawing effect, the distance of C=N bond (1.282 (3) Å) is obviously shorter than that of the normal range (1.34–1.38 Å). The molecule is essentially planar, with a dihedral angle of 8.27° between the hydrazone group and the benzene ring. In the crystal structure, the molecules are linked by intermolecular N—H···O and N—H···N hydrogen bonds (Table 1, Fig. 2), which seem to be effective in the stabilization of the structure.

Related literature top

For related literature, see: Allen et al. (1987); Chaulk et al. (2007); Kawakami et al. (2000); Moreno-Mañas et al. (2001).

Experimental top

2,4-Dinitrobenzaldehyde (1.96 g, 10 mmol) was dissolved in 100 ml absolute ethanol, after which hydrazine hydrate (0.96 ml, 20 mmol) was added. The mixture was stirred at about 353 K for 5 h. The solution was cooled and kept at about 279 K overnight. Brown powder was collected by filtration (1.41 g, yield 67%) and then single crystals suitable for X-ray measurements were obtained by recrystallization from ethanol.

Refinement top

All non-H atoms were refined anisotropically. All H atoms were placed in calculated positions, with N–H = 0.9 Å and C–H = 0.93 Å. Final difference Fourier maps showed the highest and lowest electron densities of 0.160 and -0.177 e Å-3, respectively.

Computing details top

Data collection: XSCANS (Bruker, 1997); cell refinement: XSCANS (Bruker, 1997); data reduction: XSCANS (Bruker, 1997); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. Perspective drawing of the title compound, with the atomic numbering scheme. Displacement ellipsoids are shown at the 35% probability level.
[Figure 2] Fig. 2. The unit cell packing of the title compound, viewed along the a direction.
2,4-Dinitrobenzaldehyde hydrazone top
Crystal data top
C7H6N4O4Z = 2
Mr = 210.16F000 = 216
Triclinic, P1Dx = 1.613 Mg m3
Hall symbol: -P 1Mo Kα radiation
λ = 0.71073 Å
a = 4.5839 (7) ÅCell parameters from 39 reflections
b = 9.6840 (16) Åθ = 5.9–12.5º
c = 9.9287 (15) ŵ = 0.14 mm1
α = 90.785 (12)ºT = 295 (2) K
β = 96.149 (11)ºPrism, yellow
γ = 98.955 (13)º0.4 × 0.3 × 0.2 mm
V = 432.66 (12) Å3
Data collection top
Bruker P4
diffractometer
Rint = 0.027
Radiation source: fine-focus sealed tubeθmax = 25.5º
Monochromator: graphiteθmin = 2.1º
T = 295(2) Kh = 5→1
ω scansk = 11→11
Absorption correction: nonel = 11→11
2238 measured reflections3 standard reflections
1616 independent reflections every 97 reflections
1160 reflections with I > 2σ(I) intensity decay: none
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.048H-atom parameters constrained
wR(F2) = 0.116  w = 1/[σ2(Fo2) + (0.001P)2 + 0.38P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
1616 reflectionsΔρmax = 0.16 e Å3
136 parametersΔρmin = 0.18 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
C7H6N4O4γ = 98.955 (13)º
Mr = 210.16V = 432.66 (12) Å3
Triclinic, P1Z = 2
a = 4.5839 (7) ÅMo Kα
b = 9.6840 (16) ŵ = 0.14 mm1
c = 9.9287 (15) ÅT = 295 (2) K
α = 90.785 (12)º0.4 × 0.3 × 0.2 mm
β = 96.149 (11)º
Data collection top
Bruker P4
diffractometer
Rint = 0.027
Absorption correction: none3 standard reflections
2238 measured reflections every 97 reflections
1616 independent reflections intensity decay: none
1160 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.048136 parameters
wR(F2) = 0.116H-atom parameters constrained
S = 1.07Δρmax = 0.16 e Å3
1616 reflectionsΔρmin = 0.18 e Å3
Special details top

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) top
xyzUiso*/Ueq
O10.7840 (6)0.1234 (3)0.5319 (2)0.0887 (8)
O20.4576 (6)0.2314 (2)0.6030 (2)0.0798 (7)
O30.0003 (6)0.5548 (2)0.3362 (3)0.0872 (8)
O40.1241 (6)0.5961 (3)0.1351 (3)0.0946 (9)
N10.9783 (6)0.0870 (3)0.1463 (3)0.0758 (8)
H1B1.01670.13640.22040.091*
H1C1.05810.10430.07000.091*
N20.8489 (5)0.0275 (2)0.1456 (2)0.0578 (6)
N30.5907 (6)0.1955 (2)0.5116 (2)0.0569 (6)
N40.1273 (6)0.5291 (3)0.2381 (3)0.0675 (7)
C10.7626 (6)0.0654 (3)0.2571 (3)0.0520 (7)
H1A0.79840.01690.33580.062*
C20.6075 (6)0.1858 (3)0.2585 (3)0.0471 (6)
C30.5165 (6)0.2445 (3)0.3752 (3)0.0470 (6)
C40.3552 (6)0.3540 (3)0.3687 (3)0.0518 (7)
H4A0.29180.38850.44660.062*
C50.2906 (6)0.4105 (3)0.2464 (3)0.0534 (7)
C60.3755 (6)0.3582 (3)0.1277 (3)0.0580 (7)
H6A0.33020.39780.04480.070*
C70.5269 (6)0.2473 (3)0.1360 (3)0.0561 (7)
H7A0.57910.21080.05650.067*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.117 (2)0.1053 (19)0.0558 (13)0.0634 (17)0.0041 (13)0.0040 (12)
O20.1006 (18)0.0891 (16)0.0580 (13)0.0258 (14)0.0307 (12)0.0011 (11)
O30.0851 (17)0.0709 (15)0.115 (2)0.0314 (13)0.0264 (15)0.0126 (14)
O40.136 (2)0.0714 (16)0.0829 (17)0.0524 (16)0.0107 (16)0.0009 (13)
N10.109 (2)0.0739 (17)0.0583 (15)0.0542 (17)0.0153 (15)0.0001 (13)
N20.0690 (15)0.0583 (14)0.0517 (14)0.0267 (12)0.0088 (11)0.0026 (11)
N30.0658 (15)0.0538 (14)0.0513 (14)0.0095 (12)0.0085 (12)0.0042 (11)
N40.0686 (17)0.0521 (15)0.083 (2)0.0200 (13)0.0023 (15)0.0111 (14)
C10.0609 (17)0.0507 (15)0.0484 (15)0.0176 (13)0.0106 (13)0.0035 (12)
C20.0447 (14)0.0465 (14)0.0510 (15)0.0082 (11)0.0085 (12)0.0016 (11)
C30.0482 (15)0.0464 (14)0.0459 (15)0.0056 (12)0.0063 (11)0.0001 (11)
C40.0494 (15)0.0486 (15)0.0578 (17)0.0080 (12)0.0091 (13)0.0096 (12)
C50.0505 (15)0.0449 (15)0.0661 (18)0.0140 (12)0.0029 (13)0.0031 (13)
C60.0649 (18)0.0569 (17)0.0542 (17)0.0183 (14)0.0027 (14)0.0034 (13)
C70.0661 (18)0.0586 (17)0.0473 (15)0.0211 (14)0.0073 (13)0.0027 (12)
Geometric parameters (Å, °) top
O1—N31.214 (3)C1—H1A0.9300
O2—N31.221 (3)C2—C71.400 (4)
O3—N41.229 (3)C2—C31.414 (3)
O4—N41.219 (3)C3—C41.382 (3)
N1—N21.336 (3)C4—C51.361 (4)
N1—H1B0.8999C4—H4A0.9300
N1—H1C0.9000C5—C61.393 (4)
N2—C11.282 (3)C6—C71.365 (4)
N3—C31.464 (3)C6—H6A0.9300
N4—C51.463 (3)C7—H7A0.9300
C1—C21.458 (3)
N2—N1—H1B124.3C4—C3—C2122.2 (2)
N2—N1—H1C115.3C4—C3—N3115.3 (2)
H1B—N1—H1C119.5C2—C3—N3122.5 (2)
C1—N2—N1117.5 (2)C5—C4—C3118.9 (2)
O1—N3—O2121.8 (3)C5—C4—H4A120.6
O1—N3—C3119.9 (2)C3—C4—H4A120.6
O2—N3—C3118.3 (2)C4—C5—C6121.7 (3)
O4—N4—O3123.8 (3)C4—C5—N4119.6 (3)
O4—N4—C5118.6 (3)C6—C5—N4118.7 (3)
O3—N4—C5117.6 (3)C7—C6—C5118.4 (3)
N2—C1—C2118.9 (2)C7—C6—H6A120.8
N2—C1—H1A120.5C5—C6—H6A120.8
C2—C1—H1A120.5C6—C7—C2123.2 (3)
C7—C2—C3115.5 (2)C6—C7—H7A118.4
C7—C2—C1119.4 (2)C2—C7—H7A118.4
C3—C2—C1125.0 (2)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O1i0.902.523.305 (3)146
N1—H1C···N2ii0.902.343.123 (4)146
Symmetry codes: (i) −x+2, −y, −z+1; (ii) −x+2, −y, −z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O1i0.902.523.305 (3)146
N1—H1C···N2ii0.902.343.123 (4)146
Symmetry codes: (i) −x+2, −y, −z+1; (ii) −x+2, −y, −z.
Acknowledgements top

The authors acnowledge financial support from the Ministry of Science and Technology of China (2005CCA03400, 2007 A A02Z160), the Chinese National Natural Science Foundation (20572060, 20472043), and the Department of Science and Technology of Guangdong Province (2005 A11601008).

references
References top

Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.

Bruker (1997). XSCANS. Bruker AXS Inc., Madison, Wisconsin, USA.

Chaulk, S. G. & MacMillan, A. M. (2007). Nat. Protoc. 2, 1052–1058.

Kawakami, T., Uehata, K. & Suzuki, H. (2000). Org. Lett. 2, 413–415.

Moreno-Mañas, M., Pleixats, R., Andreu, R., Garín, J., Orduna, J., Villacampa, B., Levillain, E. & Sallé, M. (2001). J. Mater. Chem. 11, 374–380.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.