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The geometric parameters of the title compound, C11H13BrN2O2, are in the usual ranges. In the crystal structure, the mol­ecules are connected by N—H...O hydrogen bonds to form centrosymmetric dimers.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807033090/sg2187sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807033090/sg2187Isup2.hkl
Contains datablock I

CCDC reference: 659076

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.040
  • wR factor = 0.086
  • Data-to-parameter ratio = 22.2

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.17
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Hydrazides and their Schiff bases are useful precursors in the synthesis of several heterocyclic systems. Some substituted hydrazides and their Schiff bases are reported to exhibit carcinostatic activity against several types of tumors and also possess antimicrobial activity It is also used as an intermediate in many pharmaceutically important compounds. A new Schiff base of the hydrazide, C11H13BrN2O2 was synthesized and its crystal structure is reported.

Geometric parameters of the title compound (Fig. 1) are in the usual ranges. All seven non-H atoms of the acetone hydrazone moiety lie in a common plane (r.m.s. deviation 0.007 Å) which is almost perpendicular [88.52 (6)°] to the aromatic ring. In the crystal, the molecules are connected by N—H···O hydrogen bonds to form centrosymmetric dimers (Fig. 2).

Related literature top

For related structures, see: 2-bromo-N'-[(E)-(4-fluorophenyl)methylene]-5-methoxybenzohydrazide monohydrate (Narayana, Sunil et al., 2007); 2-bromo-5-methoxy-N'-[(E)-(2-nitrophenyl)methylene]benzohydrazide (Yathirajan, Sarojini et al., 2007); N'-[(1E)-(4-fluorophenyl)methylene]-6-methoxy-2-naphthohydrazide (Yathirajan, Narayana et al., (2007).

For related literature, see: Swain (1959); Hodnett & Dunn (1970); Cajocorius et al. (1977); Misra et al. (1981); Agarwal et al. (1983); Varma et al. (1986); Singh & Dash (1988); Narayana, Vijayaraj et al. (2005); Narayana, Ashalatha et al. (2005); Liu et al. (2006).

Experimental top

A mixture of 2-bromo-5-methoxybenzohydrazide (2.45 g, 0.01 mol) and acetone (1.2 g, 0.02 mol) in 15 ml of absolute ethanol containing 1 drop of dilute sulfuric acid was refluxed for about 4 h. On cooling, the solid that separated was filtered and recrystallized from ethyl acetate (m.p.: 404–406 K). Analysis for C11H13BrN2O2: Found (Calculated): C: 46.21 (46.33); H: 4.54 (4.60); N: 9.73% (9.82%).

Refinement top

H atoms were found in a difference map, but they were refined using a riding model with C—H = 0.95Å and Uiso(H) = 1.2Ueq(C).

Structure description top

Hydrazides and their Schiff bases are useful precursors in the synthesis of several heterocyclic systems. Some substituted hydrazides and their Schiff bases are reported to exhibit carcinostatic activity against several types of tumors and also possess antimicrobial activity It is also used as an intermediate in many pharmaceutically important compounds. A new Schiff base of the hydrazide, C11H13BrN2O2 was synthesized and its crystal structure is reported.

Geometric parameters of the title compound (Fig. 1) are in the usual ranges. All seven non-H atoms of the acetone hydrazone moiety lie in a common plane (r.m.s. deviation 0.007 Å) which is almost perpendicular [88.52 (6)°] to the aromatic ring. In the crystal, the molecules are connected by N—H···O hydrogen bonds to form centrosymmetric dimers (Fig. 2).

For related structures, see: 2-bromo-N'-[(E)-(4-fluorophenyl)methylene]-5-methoxybenzohydrazide monohydrate (Narayana, Sunil et al., 2007); 2-bromo-5-methoxy-N'-[(E)-(2-nitrophenyl)methylene]benzohydrazide (Yathirajan, Sarojini et al., 2007); N'-[(1E)-(4-fluorophenyl)methylene]-6-methoxy-2-naphthohydrazide (Yathirajan, Narayana et al., (2007).

For related literature, see: Swain (1959); Hodnett & Dunn (1970); Cajocorius et al. (1977); Misra et al. (1981); Agarwal et al. (1983); Varma et al. (1986); Singh & Dash (1988); Narayana, Vijayaraj et al. (2005); Narayana, Ashalatha et al. (2005); Liu et al. (2006).

Computing details top

Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. Perspective view of the title compound with the atom numbering; displacement ellipsoids are at the 50% probability level.
2-Bromo-N'-isopropylidene-5-methoxybenzohydrazide top
Crystal data top
C11H13BrN2O2F(000) = 576
Mr = 285.14Dx = 1.558 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 13368 reflections
a = 7.8311 (5) Åθ = 3.6–29.5°
b = 13.6460 (7) ŵ = 3.37 mm1
c = 11.3800 (8) ÅT = 173 K
β = 92.005 (5)°Block, colourless
V = 1215.36 (13) Å30.29 × 0.27 × 0.25 mm
Z = 4
Data collection top
Stoe IPDS II two-circle-
diffractometer
3404 independent reflections
Radiation source: fine-focus sealed tube2995 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.080
ω scansθmax = 29.6°, θmin = 3.6°
Absorption correction: multi-scan
(MULABS; Spek, 2003; Blessing, 1995)
h = 1010
Tmin = 0.398, Tmax = 0.438k = 1816
27762 measured reflectionsl = 1515
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)] = 0.040H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.086 w = 1/[σ2(Fo2) + (0.0262P)2 + 0.9527P]
where P = (Fo2 + 2Fc2)/3
S = 1.17(Δ/σ)max = 0.001
3404 reflectionsΔρmax = 0.47 e Å3
153 parametersΔρmin = 0.53 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0108 (9)
Crystal data top
C11H13BrN2O2V = 1215.36 (13) Å3
Mr = 285.14Z = 4
Monoclinic, P21/cMo Kα radiation
a = 7.8311 (5) ŵ = 3.37 mm1
b = 13.6460 (7) ÅT = 173 K
c = 11.3800 (8) Å0.29 × 0.27 × 0.25 mm
β = 92.005 (5)°
Data collection top
Stoe IPDS II two-circle-
diffractometer
3404 independent reflections
Absorption correction: multi-scan
(MULABS; Spek, 2003; Blessing, 1995)
2995 reflections with I > 2σ(I)
Tmin = 0.398, Tmax = 0.438Rint = 0.080
27762 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0400 restraints
wR(F2) = 0.086H atoms treated by a mixture of independent and constrained refinement
S = 1.17Δρmax = 0.47 e Å3
3404 reflectionsΔρmin = 0.53 e Å3
153 parameters
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
Br10.02400 (3)0.755039 (17)0.73418 (2)0.03436 (10)
N10.1881 (2)0.56917 (15)0.92316 (15)0.0241 (4)
H10.163 (4)0.553 (2)0.992 (2)0.029 (7)*
N20.3432 (2)0.61293 (15)0.89571 (15)0.0263 (4)
O10.0623 (2)0.50527 (13)0.85582 (13)0.0299 (4)
O20.3225 (2)0.42571 (13)0.48012 (14)0.0322 (4)
C10.0758 (3)0.54460 (15)0.83589 (17)0.0213 (4)
C20.4445 (3)0.63696 (17)0.98164 (19)0.0266 (4)
C30.4144 (3)0.6235 (2)1.11038 (19)0.0342 (5)
H3A0.30390.65211.12920.051*
H3B0.50560.65611.15680.051*
H3C0.41410.55341.12910.051*
C40.6117 (3)0.6825 (2)0.9500 (2)0.0433 (7)
H4A0.61760.68640.86420.065*
H4B0.70620.64220.98140.065*
H4C0.62010.74850.98360.065*
C110.1243 (2)0.56409 (16)0.71060 (16)0.0200 (4)
C120.0821 (3)0.65109 (16)0.65255 (18)0.0229 (4)
C130.1178 (3)0.66386 (17)0.53468 (18)0.0274 (4)
H130.08810.72350.49610.033*
C140.1971 (3)0.58937 (17)0.47296 (17)0.0264 (4)
H140.22150.59800.39240.032*
C150.2403 (3)0.50254 (16)0.52987 (17)0.0230 (4)
C160.2025 (3)0.48971 (16)0.64868 (17)0.0226 (4)
H160.23060.42970.68700.027*
C170.3679 (3)0.4361 (2)0.35960 (19)0.0350 (5)
H17A0.26390.44190.30970.053*
H17B0.43290.37850.33580.053*
H17C0.43790.49510.35110.053*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.04829 (16)0.02903 (13)0.02596 (13)0.00271 (11)0.00392 (9)0.00287 (9)
N10.0230 (8)0.0368 (10)0.0127 (7)0.0085 (7)0.0021 (6)0.0033 (7)
N20.0242 (9)0.0351 (10)0.0199 (8)0.0105 (7)0.0052 (7)0.0027 (7)
O10.0236 (8)0.0489 (10)0.0173 (7)0.0125 (7)0.0005 (6)0.0073 (7)
O20.0361 (9)0.0403 (9)0.0204 (7)0.0059 (7)0.0062 (6)0.0018 (7)
C10.0222 (9)0.0275 (10)0.0142 (8)0.0030 (7)0.0018 (7)0.0038 (7)
C20.0251 (10)0.0322 (11)0.0226 (10)0.0060 (8)0.0032 (8)0.0028 (8)
C30.0315 (12)0.0510 (15)0.0199 (10)0.0089 (11)0.0038 (8)0.0015 (10)
C40.0359 (13)0.0602 (18)0.0341 (13)0.0239 (13)0.0062 (11)0.0121 (12)
C110.0192 (9)0.0281 (10)0.0129 (8)0.0068 (7)0.0004 (7)0.0020 (7)
C120.0263 (10)0.0255 (10)0.0169 (9)0.0041 (8)0.0005 (7)0.0020 (7)
C130.0375 (12)0.0279 (10)0.0166 (9)0.0039 (9)0.0007 (8)0.0055 (8)
C140.0298 (11)0.0376 (12)0.0119 (8)0.0059 (9)0.0012 (7)0.0032 (8)
C150.0205 (9)0.0321 (11)0.0164 (8)0.0039 (8)0.0002 (7)0.0009 (8)
C160.0225 (10)0.0282 (10)0.0168 (9)0.0028 (8)0.0006 (7)0.0045 (7)
C170.0291 (11)0.0572 (16)0.0189 (10)0.0024 (11)0.0031 (8)0.0072 (10)
Geometric parameters (Å, º) top
Br1—C121.902 (2)C4—H4B0.9800
N1—C11.346 (3)C4—H4C0.9800
N1—N21.398 (2)C11—C161.390 (3)
N1—H10.85 (3)C11—C121.393 (3)
N2—C21.280 (3)C12—C131.391 (3)
O1—C11.235 (2)C13—C141.394 (3)
O2—C151.364 (3)C13—H130.9500
O2—C171.436 (3)C14—C151.386 (3)
C1—C111.512 (3)C14—H140.9500
C2—C31.503 (3)C15—C161.405 (3)
C2—C41.505 (3)C16—H160.9500
C3—H3A0.9800C17—H17A0.9800
C3—H3B0.9800C17—H17B0.9800
C3—H3C0.9800C17—H17C0.9800
C4—H4A0.9800
C1—N1—N2119.46 (16)C16—C11—C1118.64 (18)
C1—N1—H1116.7 (19)C12—C11—C1122.28 (18)
N2—N1—H1123.7 (19)C13—C12—C11120.8 (2)
C2—N2—N1117.28 (17)C13—C12—Br1118.92 (17)
C15—O2—C17117.17 (19)C11—C12—Br1120.29 (15)
O1—C1—N1121.77 (18)C12—C13—C14120.2 (2)
O1—C1—C11120.00 (18)C12—C13—H13119.9
N1—C1—C11118.21 (17)C14—C13—H13119.9
N2—C2—C3126.8 (2)C15—C14—C13119.57 (18)
N2—C2—C4116.3 (2)C15—C14—H14120.2
C3—C2—C4116.8 (2)C13—C14—H14120.2
C2—C3—H3A109.5O2—C15—C14125.03 (18)
C2—C3—H3B109.5O2—C15—C16114.97 (19)
H3A—C3—H3B109.5C14—C15—C16120.0 (2)
C2—C3—H3C109.5C11—C16—C15120.54 (19)
H3A—C3—H3C109.5C11—C16—H16119.7
H3B—C3—H3C109.5C15—C16—H16119.7
C2—C4—H4A109.5O2—C17—H17A109.5
C2—C4—H4B109.5O2—C17—H17B109.5
H4A—C4—H4B109.5H17A—C17—H17B109.5
C2—C4—H4C109.5O2—C17—H17C109.5
H4A—C4—H4C109.5H17A—C17—H17C109.5
H4B—C4—H4C109.5H17B—C17—H17C109.5
C16—C11—C12118.91 (17)
C1—N1—N2—C2178.5 (2)C1—C11—C12—Br15.2 (3)
N2—N1—C1—O1179.5 (2)C11—C12—C13—C140.2 (3)
N2—N1—C1—C111.0 (3)Br1—C12—C13—C14179.32 (17)
N1—N2—C2—C30.2 (4)C12—C13—C14—C150.1 (3)
N1—N2—C2—C4179.1 (2)C17—O2—C15—C140.2 (3)
O1—C1—C11—C1685.5 (3)C17—O2—C15—C16178.48 (19)
N1—C1—C11—C1693.0 (2)C13—C14—C15—O2178.0 (2)
O1—C1—C11—C1289.7 (3)C13—C14—C15—C160.6 (3)
N1—C1—C11—C1291.8 (3)C12—C11—C16—C150.8 (3)
C16—C11—C12—C130.2 (3)C1—C11—C16—C15176.12 (18)
C1—C11—C12—C13175.3 (2)O2—C15—C16—C11177.74 (19)
C16—C11—C12—Br1179.67 (15)C14—C15—C16—C111.0 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1i0.85 (3)2.08 (3)2.916 (2)168 (3)
Symmetry code: (i) x, y+1, z+2.

Experimental details

Crystal data
Chemical formulaC11H13BrN2O2
Mr285.14
Crystal system, space groupMonoclinic, P21/c
Temperature (K)173
a, b, c (Å)7.8311 (5), 13.6460 (7), 11.3800 (8)
β (°) 92.005 (5)
V3)1215.36 (13)
Z4
Radiation typeMo Kα
µ (mm1)3.37
Crystal size (mm)0.29 × 0.27 × 0.25
Data collection
DiffractometerStoe IPDS II two-circle-
diffractometer
Absorption correctionMulti-scan
(MULABS; Spek, 2003; Blessing, 1995)
Tmin, Tmax0.398, 0.438
No. of measured, independent and
observed [I > 2σ(I)] reflections
27762, 3404, 2995
Rint0.080
(sin θ/λ)max1)0.696
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.040, 0.086, 1.17
No. of reflections3404
No. of parameters153
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.47, 0.53

Computer programs: X-AREA (Stoe & Cie, 2001), X-AREA, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003), SHELXL97.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1i0.85 (3)2.08 (3)2.916 (2)168 (3)
Symmetry code: (i) x, y+1, z+2.
 

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