Abstract
The title compound, C14H10BrN3O3, was obtained by a condensation reaction between 2-nitrobenzaldehyde and 4-bromobenzohydrazide. The dihedral angle between the two benzene rings is 4.1 (2)°. The molecule displays an E configuration about the C=N bond. In the crystal, molecules are linked into a chain along [100] by intermolecular N—H⋯O hydrogen bonds.
Related literature
For the biological properties of Schiff base and hydrazone compounds, see: Kucukguzel et al. (2006 ▶); Khattab et al. (2005 ▶); Karthikeyan et al. (2006 ▶); Okabe et al. (1993 ▶). For bond-length data, see: Allen et al. (1987 ▶). For related structures, see: Shan et al. (2008 ▶); Fun et al. (2008 ▶); Ma et al. (2008 ▶); Diao et al. (2008a ▶,b ▶); Ejsmont et al. (2008 ▶).
Experimental
Crystal data
C14H10BrN3O3
M r = 348.16
Triclinic,
a = 4.8718 (17) Å
b = 6.842 (2) Å
c = 10.709 (4) Å
α = 98.014 (5)°
β = 93.258 (6)°
γ = 97.413 (5)°
V = 349.5 (2) Å3
Z = 1
Mo Kα radiation
μ = 2.95 mm−1
T = 298 (2) K
0.20 × 0.18 × 0.17 mm
Data collection
Bruker SMART CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2001 ▶) T min = 0.590, T max = 0.634
2347 measured reflections
1998 independent reflections
1584 reflections with I > 2σ(I)
R int = 0.013
Refinement
R[F 2 > 2σ(F 2)] = 0.027
wR(F 2) = 0.064
S = 0.95
1998 reflections
193 parameters
3 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.22 e Å−3
Δρmin = −0.23 e Å−3
Absolute structure: Flack (1983 ▶), 235 Friedel pairs
Flack parameter: 0.021 (8)
Data collection: SMART (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809002165/ci2760sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809002165/ci2760Isup2.hkl
Table 1. Hydrogen-bond geometry (Å, °).
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
---|---|---|---|---|
N1—H1⋯O1i | 0.900 (11) | 1.909 (19) | 2.791 (3) | 166 (6) |
Symmetry code: (i) .
Acknowledgments
This project was supported by Jilin University.
supplementary crystallographic information
Comment
Hydrazones and Schiff bases have attracted much attention for their excellent biological properties, especially for their potential pharmacological and antitumor properties (Kucukguzel et al., 2006; Khattab et al., 2005; Karthikeyan et al., 2006; Okabe et al., 1993). Recently, a large number of hydrazone derivatives have been prepared and structurally characterized (Shan et al., 2008; Fun et al., 2008; Ma et al., 2008; Diao et al., 2008a,b; Ejsmont et al., 2008). As part of the ongoing study, we report herein the crystal structure of the title compound.
The molecular structure of the title compound is shown in Fig. 1. The dihedral angle between the two benzene rings is 4.1 (2)°. The molecule of the compound displays an E configuration about the C═N bond. The bond values are typical (Allen et al., 1987). The molecules are linked into a chain along the [100] by intermolecular N—H···O hydrogen bonds.
Experimental
2-Nitrobenzaldehyde (1.0 mmol, 151.1 mg) was dissolved in methanol (50 ml) and then 4-bromobenzohydrazide (1.0 mmol, 215.0 mg) was added slowly into the solution, and the mixture was kept at reflux with continuous stirring for 1 h. After the solution had cooled to room temperature colourless crystals appeared. The crystals were filtered and washed with methanol for three times. Recrystallization from an absolute methanol yielded block-shaped single crystals of the title compound.
Refinement
The amide H atom was located in a difference map and its positional parameters were refined. All other H atoms were placed in calculated positions (C-H = 0.93 Å) and refined using a riding model. The Uiso(H) values were set at 1.2Ueq(C,N).
Figures
Crystal data
C14H10BrN3O3 | Z = 1 |
Mr = 348.16 | F(000) = 174 |
Triclinic, P1 | Dx = 1.654 Mg m−3 |
Hall symbol: P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 4.8718 (17) Å | Cell parameters from 1163 reflections |
b = 6.842 (2) Å | θ = 2.8–26.3° |
c = 10.709 (4) Å | µ = 2.95 mm−1 |
α = 98.014 (5)° | T = 298 K |
β = 93.258 (6)° | Block, colourless |
γ = 97.413 (5)° | 0.20 × 0.18 × 0.17 mm |
V = 349.5 (2) Å3 |
Data collection
Bruker SMART CCD area-detector diffractometer | 1998 independent reflections |
Radiation source: fine-focus sealed tube | 1584 reflections with I > 2σ(I) |
graphite | Rint = 0.013 |
ω scans | θmax = 30.7°, θmin = 1.9° |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −6→6 |
Tmin = 0.590, Tmax = 0.634 | k = −8→8 |
2347 measured reflections | l = −11→15 |
Refinement
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.027 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.064 | w = 1/[σ2(Fo2) + (0.0058P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.95 | (Δ/σ)max = 0.001 |
1998 reflections | Δρmax = 0.22 e Å−3 |
193 parameters | Δρmin = −0.23 e Å−3 |
3 restraints | Absolute structure: Flack (1983), 235 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Flack parameter: 0.021 (8) |
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 | ||
Br1 | 0.28524 (6) | −0.18204 (5) | −0.03061 (4) | 0.08281 (18) | |
O1 | 0.9938 (4) | 0.7003 (4) | 0.2644 (2) | 0.0599 (6) | |
O2 | 0.1064 (8) | 1.2188 (6) | 0.7780 (3) | 0.0860 (11) | |
O3 | 0.2286 (10) | 0.9674 (5) | 0.6631 (3) | 0.1064 (15) | |
N1 | 0.5685 (5) | 0.7559 (4) | 0.3185 (2) | 0.0399 (5) | |
H1 | 0.394 (9) | 0.725 (7) | 0.293 (4) | 0.048* | |
N2 | 0.6709 (5) | 0.9301 (4) | 0.3980 (2) | 0.0405 (5) | |
N3 | 0.2485 (7) | 1.1447 (5) | 0.6997 (3) | 0.0584 (8) | |
C1 | 0.6174 (7) | 0.4513 (5) | 0.1848 (3) | 0.0385 (7) | |
C2 | 0.7401 (7) | 0.3754 (5) | 0.0775 (3) | 0.0506 (8) | |
H2 | 0.8910 | 0.4505 | 0.0495 | 0.061* | |
C3 | 0.6386 (8) | 0.1890 (6) | 0.0126 (3) | 0.0564 (9) | |
H3 | 0.7180 | 0.1400 | −0.0602 | 0.068* | |
C4 | 0.4217 (8) | 0.0767 (5) | 0.0555 (3) | 0.0504 (8) | |
C5 | 0.2932 (7) | 0.1486 (5) | 0.1614 (3) | 0.0447 (7) | |
H5 | 0.1429 | 0.0722 | 0.1889 | 0.054* | |
C6 | 0.3932 (6) | 0.3357 (5) | 0.2250 (3) | 0.0420 (7) | |
H6 | 0.3090 | 0.3855 | 0.2962 | 0.050* | |
C7 | 0.7440 (6) | 0.6473 (4) | 0.2577 (3) | 0.0404 (6) | |
C8 | 0.4917 (6) | 1.0171 (4) | 0.4562 (3) | 0.0384 (6) | |
H8 | 0.3061 | 0.9609 | 0.4479 | 0.046* | |
C9 | 0.5831 (6) | 1.2100 (4) | 0.5376 (3) | 0.0393 (6) | |
C10 | 0.4633 (7) | 1.2766 (5) | 0.6481 (3) | 0.0433 (7) | |
C11 | 0.5462 (8) | 1.4635 (6) | 0.7158 (3) | 0.0607 (9) | |
H11 | 0.4634 | 1.5029 | 0.7896 | 0.073* | |
C12 | 0.7486 (9) | 1.5906 (6) | 0.6752 (4) | 0.0660 (10) | |
H12 | 0.8015 | 1.7178 | 0.7199 | 0.079* | |
C13 | 0.8755 (8) | 1.5290 (5) | 0.5668 (3) | 0.0550 (9) | |
H13 | 1.0172 | 1.6139 | 0.5397 | 0.066* | |
C14 | 0.7919 (8) | 1.3419 (6) | 0.4990 (3) | 0.0489 (9) | |
H14 | 0.8772 | 1.3031 | 0.4258 | 0.059* |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.1255 (4) | 0.04369 (19) | 0.0679 (2) | −0.00267 (18) | 0.00284 (18) | −0.01585 (13) |
O1 | 0.0231 (11) | 0.0608 (15) | 0.0872 (15) | −0.0003 (10) | 0.0026 (10) | −0.0128 (12) |
O2 | 0.082 (2) | 0.113 (3) | 0.074 (2) | 0.030 (2) | 0.0420 (17) | 0.0233 (19) |
O3 | 0.149 (4) | 0.068 (3) | 0.087 (2) | −0.047 (2) | 0.049 (2) | −0.0006 (17) |
N1 | 0.0237 (12) | 0.0358 (13) | 0.0545 (13) | −0.0004 (10) | −0.0015 (10) | −0.0072 (11) |
N2 | 0.0343 (13) | 0.0331 (12) | 0.0494 (12) | −0.0022 (10) | −0.0040 (10) | −0.0015 (10) |
N3 | 0.057 (2) | 0.068 (2) | 0.0476 (14) | −0.0014 (16) | 0.0036 (14) | 0.0092 (14) |
C1 | 0.0303 (16) | 0.0361 (15) | 0.0469 (15) | 0.0039 (13) | −0.0061 (13) | 0.0027 (12) |
C2 | 0.0450 (19) | 0.050 (2) | 0.0551 (17) | 0.0058 (15) | 0.0104 (14) | 0.0015 (15) |
C3 | 0.067 (2) | 0.057 (2) | 0.0417 (15) | 0.0094 (18) | 0.0084 (15) | −0.0075 (14) |
C4 | 0.062 (2) | 0.0360 (16) | 0.0488 (16) | 0.0072 (15) | −0.0087 (15) | −0.0032 (13) |
C5 | 0.0430 (18) | 0.0365 (16) | 0.0515 (16) | −0.0015 (13) | 0.0030 (14) | 0.0024 (13) |
C6 | 0.0379 (17) | 0.0418 (17) | 0.0438 (15) | 0.0048 (13) | 0.0031 (13) | −0.0008 (13) |
C7 | 0.0318 (16) | 0.0389 (16) | 0.0484 (14) | 0.0018 (12) | −0.0009 (12) | 0.0038 (12) |
C8 | 0.0322 (15) | 0.0356 (15) | 0.0435 (14) | −0.0016 (13) | 0.0004 (12) | −0.0006 (12) |
C9 | 0.0385 (16) | 0.0325 (15) | 0.0444 (14) | −0.0001 (12) | −0.0029 (12) | 0.0039 (12) |
C10 | 0.0401 (17) | 0.0418 (16) | 0.0464 (14) | 0.0022 (13) | 0.0033 (13) | 0.0042 (12) |
C11 | 0.070 (2) | 0.053 (2) | 0.0542 (17) | 0.0114 (19) | 0.0013 (17) | −0.0095 (15) |
C12 | 0.079 (3) | 0.0351 (17) | 0.075 (2) | −0.0046 (18) | −0.004 (2) | −0.0064 (16) |
C13 | 0.058 (2) | 0.0404 (19) | 0.0614 (19) | −0.0124 (15) | 0.0002 (17) | 0.0091 (15) |
C14 | 0.0495 (18) | 0.041 (2) | 0.051 (2) | −0.0091 (15) | 0.0001 (17) | 0.0075 (18) |
Geometric parameters (Å, °)
Br1—C4 | 1.897 (3) | C4—C5 | 1.387 (5) |
O1—C7 | 1.219 (4) | C5—C6 | 1.377 (4) |
O2—N3 | 1.216 (5) | C5—H5 | 0.93 |
O3—N3 | 1.211 (5) | C6—H6 | 0.93 |
N1—C7 | 1.341 (4) | C8—C9 | 1.478 (4) |
N1—N2 | 1.382 (3) | C8—H8 | 0.93 |
N1—H1 | 0.87 (4) | C9—C14 | 1.391 (5) |
N2—C8 | 1.264 (4) | C9—C10 | 1.395 (4) |
N3—C10 | 1.474 (5) | C10—C11 | 1.378 (4) |
C1—C6 | 1.389 (5) | C11—C12 | 1.360 (6) |
C1—C2 | 1.393 (5) | C11—H11 | 0.93 |
C1—C7 | 1.493 (4) | C12—C13 | 1.386 (6) |
C2—C3 | 1.380 (5) | C12—H12 | 0.93 |
C2—H2 | 0.93 | C13—C14 | 1.380 (5) |
C3—C4 | 1.364 (5) | C13—H13 | 0.93 |
C3—H3 | 0.93 | C14—H14 | 0.93 |
C7—N1—N2 | 119.9 (2) | O1—C7—N1 | 122.7 (3) |
C7—N1—H1 | 116 (3) | O1—C7—C1 | 121.2 (3) |
N2—N1—H1 | 123 (3) | N1—C7—C1 | 116.0 (2) |
C8—N2—N1 | 115.5 (2) | N2—C8—C9 | 118.6 (3) |
O3—N3—O2 | 123.8 (4) | N2—C8—H8 | 120.7 |
O3—N3—C10 | 117.7 (3) | C9—C8—H8 | 120.7 |
O2—N3—C10 | 118.5 (4) | C14—C9—C10 | 116.6 (3) |
C6—C1—C2 | 118.7 (3) | C14—C9—C8 | 118.6 (3) |
C6—C1—C7 | 122.3 (3) | C10—C9—C8 | 124.7 (3) |
C2—C1—C7 | 118.8 (3) | C11—C10—C9 | 121.9 (3) |
C3—C2—C1 | 120.2 (3) | C11—C10—N3 | 117.4 (3) |
C3—C2—H2 | 119.9 | C9—C10—N3 | 120.7 (3) |
C1—C2—H2 | 119.9 | C12—C11—C10 | 120.3 (3) |
C4—C3—C2 | 119.9 (3) | C12—C11—H11 | 119.8 |
C4—C3—H3 | 120.1 | C10—C11—H11 | 119.8 |
C2—C3—H3 | 120.1 | C11—C12—C13 | 119.5 (3) |
C3—C4—C5 | 121.3 (3) | C11—C12—H12 | 120.3 |
C3—C4—Br1 | 120.4 (3) | C13—C12—H12 | 120.3 |
C5—C4—Br1 | 118.3 (3) | C14—C13—C12 | 120.1 (3) |
C6—C5—C4 | 118.6 (3) | C14—C13—H13 | 119.9 |
C6—C5—H5 | 120.7 | C12—C13—H13 | 119.9 |
C4—C5—H5 | 120.7 | C13—C14—C9 | 121.5 (3) |
C5—C6—C1 | 121.3 (3) | C13—C14—H14 | 119.2 |
C5—C6—H6 | 119.4 | C9—C14—H14 | 119.2 |
C1—C6—H6 | 119.4 | ||
C7—N1—N2—C8 | −176.5 (3) | N2—C8—C9—C14 | 36.5 (4) |
C6—C1—C2—C3 | 0.3 (5) | N2—C8—C9—C10 | −147.7 (3) |
C7—C1—C2—C3 | 175.9 (3) | C14—C9—C10—C11 | 0.1 (4) |
C1—C2—C3—C4 | −1.6 (5) | C8—C9—C10—C11 | −175.8 (3) |
C2—C3—C4—C5 | 2.2 (5) | C14—C9—C10—N3 | −177.4 (3) |
C2—C3—C4—Br1 | −178.6 (3) | C8—C9—C10—N3 | 6.6 (4) |
C3—C4—C5—C6 | −1.4 (5) | O3—N3—C10—C11 | −160.0 (4) |
Br1—C4—C5—C6 | 179.4 (2) | O2—N3—C10—C11 | 18.4 (5) |
C4—C5—C6—C1 | 0.1 (4) | O3—N3—C10—C9 | 17.7 (5) |
C2—C1—C6—C5 | 0.4 (4) | O2—N3—C10—C9 | −163.9 (3) |
C7—C1—C6—C5 | −175.0 (3) | C9—C10—C11—C12 | 0.6 (5) |
N2—N1—C7—O1 | −3.6 (4) | N3—C10—C11—C12 | 178.3 (4) |
N2—N1—C7—C1 | 173.8 (2) | C10—C11—C12—C13 | −1.5 (6) |
C6—C1—C7—O1 | 143.2 (3) | C11—C12—C13—C14 | 1.6 (6) |
C2—C1—C7—O1 | −32.3 (4) | C12—C13—C14—C9 | −0.8 (6) |
C6—C1—C7—N1 | −34.3 (4) | C10—C9—C14—C13 | 0.0 (5) |
C2—C1—C7—N1 | 150.3 (3) | C8—C9—C14—C13 | 176.1 (3) |
N1—N2—C8—C9 | −176.7 (2) |
Hydrogen-bond geometry (Å, °)
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.900 (11) | 1.909 (19) | 2.791 (3) | 166 (6) |
Symmetry codes: (i) x−1, y, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CI2760).
References
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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 datablocks global, I. DOI: 10.1107/S1600536809002165/ci2760sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809002165/ci2760Isup2.hkl