supplementary materials


Acta Cryst. (2008). E64, o2061    [ doi:10.1107/S1600536808030675 ]

(E)-3-Bromo-N'-(5-bromo-2-hydroxybenzylidene)benzohydrazide

L.-Z. Qu, T. Yang, G.-B. Cao and X.-Y. Wang

Abstract top

The title compound, C14H10Br2N2O2, was synthesized by the reaction of 5-bromosalicylaldehyde with an equimolar quantity of 3-bromobenzohydrazide in methanol. The dihedral angle between the two benzene rings is 10.5 (4)°. In the crystal structure, molecules are linked through intermolecular N-H...O hydrogen bonds to form chains parallel to the c axis, and an intramolecular O-H...N interaction also occurs.

Comment top

We have recently reported some transition metal complexes with Schiff base ligands (Cao, 2007a,b) and a hydrazone compound (Yang et al., 2008). We report herein the crystal structure of the title compound, (I), derived from the reaction of 5-bromosalicylaldehyde with an equimolar quantity of 3-bromobenzohydrazide in methanol.

In compound (I), Fig. 1, the dihedral angle between the two benzene rings is 10.5 (4)°. All the bond values are comparable to those in other similar hydrazones (Zhen & Han, 2005; Peng & Hou, 2008; Tang, 2008; Salhin et al., 2007; Yathirajan et al., 2007). In the crystal structure, molecules are linked through intermolecular N—H···O hydrogen bonds, Table 1, to form chains parallel to the c axis, Fig. 2.

Related literature top

For related structures, see: Cao (2007a,b); Yang et al. (2008); Zhen & Han (2005); Peng & Hou (2008); Tang (2008); Salhin et al. (2007); Yathirajan et al. (2007).

Experimental top

The compound was prepared by refluxing equimolar quantities of 5-bromosalicylaldehyde with 3-bromobenzohydrazide in methanol. Colorless block-like crystals were formed when the solution was evaporated in air for about a week.

Refinement top

H2 was located in a difference Fourier map and refined isotropically, with the N–H distance restrained to 0.90 (4) Å. The other H atoms were placed in idealized positions and constrained to ride on their parent atoms, with C–H distances of 0.93 Å, the O–H distance of 0.82 Å, and with Uiso(H) set at 1.2Ueq(C) and 1.5Ueq(O).

Computing details top

Data collection: SMART (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); 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. The molecular structure of (I) with ellipsoids drawn at the 30% probability level. Dashed lines indicate intramolecular hydrogen bond.
[Figure 2] Fig. 2. The molecular packing of (I), viewed along the a axis. Hydrogen bonds are drawn as dashed lines.
(E)-3-Bromo-N'-(5-bromo-2-hydroxybenzylidene)benzohydrazide top
Crystal data top
C14H10Br2N2O2F(000) = 776
Mr = 398.06Dx = 1.858 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 5.657 (5) ÅCell parameters from 1979 reflections
b = 32.08 (3) Åθ = 2.5–25.3°
c = 7.856 (7) ŵ = 5.70 mm1
β = 93.217 (13)°T = 298 K
V = 1423 (2) Å3Block, colorless
Z = 40.13 × 0.08 × 0.07 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
3227 independent reflections
Radiation source: fine-focus sealed tube1830 reflections with I > 2σ(I)
graphiteRint = 0.044
ω scansθmax = 27.5°, θmin = 2.5°
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
h = 75
Tmin = 0.525, Tmax = 0.691k = 4040
8526 measured reflectionsl = 108
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.048Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.108H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0261P)2 + 2.1967P]
where P = (Fo2 + 2Fc2)/3
3227 reflections(Δ/σ)max = 0.001
185 parametersΔρmax = 0.36 e Å3
1 restraintΔρmin = 0.62 e Å3
Crystal data top
C14H10Br2N2O2V = 1423 (2) Å3
Mr = 398.06Z = 4
Monoclinic, P21/nMo Kα radiation
a = 5.657 (5) ŵ = 5.70 mm1
b = 32.08 (3) ÅT = 298 K
c = 7.856 (7) Å0.13 × 0.08 × 0.07 mm
β = 93.217 (13)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
3227 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
1830 reflections with I > 2σ(I)
Tmin = 0.525, Tmax = 0.691Rint = 0.044
8526 measured reflectionsθmax = 27.5°
Refinement top
R[F2 > 2σ(F2)] = 0.048H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.108Δρmax = 0.36 e Å3
S = 1.06Δρmin = 0.62 e Å3
3227 reflectionsAbsolute structure: ?
185 parametersFlack parameter: ?
1 restraintRogers parameter: ?
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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
Br10.52024 (14)0.488709 (18)0.25097 (9)0.0871 (3)
Br20.48529 (11)0.059801 (15)0.43970 (8)0.0683 (2)
O10.9846 (6)0.33095 (11)0.5203 (5)0.0569 (9)
H10.89270.31120.51170.085*
O20.6434 (6)0.22201 (10)0.6015 (4)0.0607 (10)
N10.5896 (7)0.29247 (11)0.4185 (5)0.0451 (9)
N20.4480 (7)0.25766 (12)0.3888 (5)0.0482 (10)
C10.6522 (8)0.36456 (14)0.3700 (5)0.0398 (10)
C20.8762 (8)0.36571 (15)0.4560 (6)0.0455 (11)
C30.9919 (10)0.40362 (17)0.4777 (7)0.0596 (14)
H31.14090.40450.53390.072*
C40.8888 (11)0.43984 (17)0.4170 (7)0.0655 (15)
H40.96870.46500.43170.079*
C50.6659 (10)0.43900 (15)0.3338 (6)0.0572 (13)
C60.5510 (9)0.40199 (14)0.3089 (6)0.0485 (12)
H60.40340.40150.25050.058*
C70.5168 (8)0.32626 (14)0.3474 (6)0.0437 (11)
H70.37580.32640.28060.052*
C80.4901 (8)0.22345 (14)0.4857 (6)0.0431 (11)
C90.3421 (8)0.18595 (14)0.4356 (5)0.0398 (10)
C100.4437 (8)0.14749 (13)0.4676 (5)0.0419 (11)
H100.59080.14560.52610.050*
C110.3267 (9)0.11187 (14)0.4127 (6)0.0472 (12)
C120.1049 (9)0.11408 (17)0.3310 (6)0.0568 (14)
H120.02700.08990.29390.068*
C130.0001 (9)0.15246 (17)0.3051 (6)0.0547 (13)
H130.15130.15420.25300.066*
C140.1181 (8)0.18839 (15)0.3557 (6)0.0471 (12)
H140.04720.21420.33620.057*
H20.339 (7)0.2580 (16)0.301 (5)0.080*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.1139 (6)0.0458 (3)0.1014 (5)0.0013 (3)0.0025 (4)0.0130 (3)
Br20.0836 (4)0.0420 (3)0.0786 (4)0.0039 (3)0.0013 (3)0.0049 (3)
O10.038 (2)0.064 (2)0.067 (2)0.0044 (17)0.0141 (17)0.0082 (19)
O20.068 (2)0.0479 (19)0.062 (2)0.0009 (17)0.0422 (19)0.0007 (16)
N10.049 (2)0.039 (2)0.045 (2)0.0038 (18)0.0151 (18)0.0009 (17)
N20.051 (3)0.040 (2)0.051 (2)0.0048 (19)0.027 (2)0.0026 (18)
C10.034 (3)0.050 (3)0.035 (2)0.002 (2)0.002 (2)0.006 (2)
C20.040 (3)0.052 (3)0.044 (3)0.007 (2)0.001 (2)0.001 (2)
C30.050 (3)0.069 (4)0.058 (3)0.013 (3)0.007 (3)0.010 (3)
C40.073 (4)0.057 (3)0.065 (4)0.027 (3)0.001 (3)0.006 (3)
C50.070 (4)0.047 (3)0.055 (3)0.007 (3)0.006 (3)0.002 (2)
C60.060 (3)0.046 (3)0.039 (3)0.002 (2)0.002 (2)0.001 (2)
C70.039 (3)0.052 (3)0.039 (3)0.003 (2)0.009 (2)0.002 (2)
C80.043 (3)0.043 (3)0.042 (3)0.004 (2)0.011 (2)0.001 (2)
C90.042 (3)0.049 (3)0.027 (2)0.002 (2)0.009 (2)0.0001 (19)
C100.039 (3)0.049 (3)0.037 (3)0.000 (2)0.007 (2)0.001 (2)
C110.057 (3)0.046 (3)0.039 (3)0.005 (2)0.003 (2)0.001 (2)
C120.053 (3)0.061 (3)0.056 (3)0.022 (3)0.002 (3)0.002 (3)
C130.039 (3)0.072 (4)0.052 (3)0.011 (3)0.008 (2)0.004 (3)
C140.038 (3)0.059 (3)0.043 (3)0.000 (2)0.001 (2)0.001 (2)
Geometric parameters (Å, °) top
Br1—C51.893 (5)C4—H40.9300
Br2—C111.902 (5)C5—C61.362 (6)
O1—C21.356 (5)C6—H60.9300
O1—H10.8200C7—H70.9300
O2—C81.222 (5)C8—C91.505 (6)
N1—C71.277 (5)C9—C101.378 (6)
N1—N21.386 (5)C9—C141.385 (6)
N2—C81.349 (6)C10—C111.377 (6)
N2—H20.90 (4)C10—H100.9300
C1—C21.402 (6)C11—C121.379 (7)
C1—C61.403 (6)C12—C131.376 (7)
C1—C71.453 (6)C12—H120.9300
C2—C31.387 (6)C13—C141.379 (6)
C3—C41.373 (7)C13—H130.9300
C3—H30.9300C14—H140.9300
C4—C51.387 (7)
C2—O1—H1109.5N1—C7—H7119.7
C7—N1—N2116.2 (4)C1—C7—H7119.7
C8—N2—N1118.6 (3)O2—C8—N2123.1 (4)
C8—N2—H2122 (4)O2—C8—C9121.7 (4)
N1—N2—H2119 (4)N2—C8—C9115.1 (4)
C2—C1—C6118.9 (4)C10—C9—C14119.7 (4)
C2—C1—C7122.5 (4)C10—C9—C8116.6 (4)
C6—C1—C7118.6 (4)C14—C9—C8123.7 (4)
O1—C2—C3118.3 (4)C11—C10—C9119.8 (4)
O1—C2—C1122.3 (4)C11—C10—H10120.1
C3—C2—C1119.3 (5)C9—C10—H10120.1
C4—C3—C2120.7 (5)C10—C11—C12120.8 (5)
C4—C3—H3119.6C10—C11—Br2118.6 (4)
C2—C3—H3119.6C12—C11—Br2120.6 (4)
C3—C4—C5120.3 (5)C13—C12—C11119.2 (5)
C3—C4—H4119.9C13—C12—H12120.4
C5—C4—H4119.9C11—C12—H12120.4
C6—C5—C4119.9 (5)C12—C13—C14120.5 (5)
C6—C5—Br1119.3 (4)C12—C13—H13119.8
C4—C5—Br1120.8 (4)C14—C13—H13119.8
C5—C6—C1120.9 (5)C13—C14—C9119.9 (5)
C5—C6—H6119.5C13—C14—H14120.0
C1—C6—H6119.5C9—C14—H14120.0
N1—C7—C1120.6 (4)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1—H1···N10.821.922.638 (5)145
N2—H2···O2i0.90 (4)1.98 (2)2.838 (5)160 (5)
Symmetry codes: (i) x−1/2, −y+1/2, z−1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O1—H1···N10.821.922.638 (5)145
N2—H2···O2i0.90 (4)1.98 (2)2.838 (5)160 (5)
Symmetry codes: (i) x−1/2, −y+1/2, z−1/2.
Acknowledgements top

The Natural Scientific Research Foundation of the Education Office of Shanxi Province (project No. 07 J K177) is acknowledged.

references
References top

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