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In the title compound, C14H12BrNO, the torsion angle about the central C=N double bond is 170.4 (3)° and the dihedral angle between the aromatic rings is 9.6 (3)°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807046855/hb2554sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807046855/hb2554Isup2.hkl
Contains datablock I

CCDC reference: 663856

Key indicators

  • Single-crystal X-ray study
  • T = 292 K
  • Mean [sigma](C-C) = 0.009 Å
  • R factor = 0.064
  • wR factor = 0.121
  • Data-to-parameter ratio = 15.1

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.96 PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT341_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 9 PLAT431_ALERT_2_C Short Inter HL..A Contact Br1 .. O1 .. 3.13 Ang.
Alert level G REFLT03_ALERT_4_G WARNING: Large fraction of Friedel related reflns may be needed to determine absolute structure From the CIF: _diffrn_reflns_theta_max 28.28 From the CIF: _reflns_number_total 2349 Count of symmetry unique reflns 1585 Completeness (_total/calc) 148.20% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 764 Fraction of Friedel pairs measured 0.482 Are heavy atom types Z>Si present yes PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 1
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 1 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 3 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Schiff bases such as those derived from salicylaldehyde and aniline are readily synthesized. The Schiff base of N-(4-Bromobenzylidene)-3-nitroaniline had been reported before (Sun et al., 2006). As part of a project to examine the catalytic activity of Schiff bases that in the form of their nickel complexes (Gao et al., 2004), the title p-bromobenzaldehyde derivative, (I), was obtained by reaction with 4-methoxyaniline (Fig. 1). The molecule is not planar as the two aromatic rings are twisted about the double bond in order to relieve steric strain.

Related literature top

For related literature, see: Gao et al. (2004); Sun et al. (2006).

Experimental top

p-Methoxyaniline (2.24 g, 18.2 mmol) and p-bromobenzaldehyde (3.33 g, 18.0 mmol) were dissolved in ethanol (35 ml) along with 1 ml of formic acid. The solution was refluxed for 8 h. Removal of the solvent followed by recrystallization from a 1:1 v/v ethanol/dichloromethane mixture (35 ml) gave the title compound in about 70% yield. Colourless blocks of (I) were grown from ethanol. Elemental analysis: calculated for C14H12Br1N1O1: C 57.95, H 4.17, N 4.83%; found: C 57.80, H 4.01, N 5.02%.

Refinement top

The H atoms were placed in calculated positions (C—H = 0.93 Å) and refined as riding with Uiso(H) = 1.2Ueq(C).

Structure description top

Schiff bases such as those derived from salicylaldehyde and aniline are readily synthesized. The Schiff base of N-(4-Bromobenzylidene)-3-nitroaniline had been reported before (Sun et al., 2006). As part of a project to examine the catalytic activity of Schiff bases that in the form of their nickel complexes (Gao et al., 2004), the title p-bromobenzaldehyde derivative, (I), was obtained by reaction with 4-methoxyaniline (Fig. 1). The molecule is not planar as the two aromatic rings are twisted about the double bond in order to relieve steric strain.

For related literature, see: Gao et al. (2004); Sun et al. (2006).

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL (Bruker, 1997).

Figures top
[Figure 1] Fig. 1. Vew of (I), with displacement ellipsoids drawn at the 50% probability level. The H atoms are drawn as spheres of arbitrary radius.
N-(4-Bromobenzylidene)-4-methoxyaniline top
Crystal data top
C14H12BrNOF(000) = 584
Mr = 290.15Dx = 1.543 Mg m3
Orthorhombic, Pca21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2c -2acCell parameters from 1585 reflections
a = 6.1510 (8) Åθ = 2.1–28.3°
b = 7.2726 (9) ŵ = 3.27 mm1
c = 27.914 (4) ÅT = 292 K
V = 1248.7 (3) Å3Block, colorless
Z = 40.10 × 0.10 × 0.06 mm
Data collection top
Bruker SMART CCD
diffractometer
2349 independent reflections
Radiation source: fine-focus sealed tube1512 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.063
ω scansθmax = 28.3°, θmin = 2.8°
Absorption correction: multi-scan
(SADABS; Bruker, 1997)
h = 77
Tmin = 0.728, Tmax = 0.822k = 97
8336 measured reflectionsl = 2636
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)] = 0.064H-atom parameters constrained
wR(F2) = 0.121 w = 1/[σ2(Fo2) + (0.0415P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.005
2349 reflectionsΔρmax = 0.51 e Å3
156 parametersΔρmin = 0.32 e Å3
1 restraintAbsolute structure: Flack (1983), 764 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.016 (18)
Crystal data top
C14H12BrNOV = 1248.7 (3) Å3
Mr = 290.15Z = 4
Orthorhombic, Pca21Mo Kα radiation
a = 6.1510 (8) ŵ = 3.27 mm1
b = 7.2726 (9) ÅT = 292 K
c = 27.914 (4) Å0.10 × 0.10 × 0.06 mm
Data collection top
Bruker SMART CCD
diffractometer
2349 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 1997)
1512 reflections with I > 2σ(I)
Tmin = 0.728, Tmax = 0.822Rint = 0.063
8336 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.064H-atom parameters constrained
wR(F2) = 0.121Δρmax = 0.51 e Å3
S = 1.06Δρmin = 0.32 e Å3
2349 reflectionsAbsolute structure: Flack (1983), 764 Friedel pairs
156 parametersAbsolute structure parameter: 0.016 (18)
1 restraint
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
Br10.03907 (11)0.72700 (9)0.51664 (4)0.0716 (3)
C10.2243 (10)0.7455 (7)0.3597 (2)0.0396 (15)
C20.3529 (11)0.8085 (8)0.3978 (3)0.0467 (16)
H20.49260.85180.39190.056*
C30.2744 (11)0.8067 (9)0.4438 (3)0.0530 (17)
H30.35830.85260.46880.064*
C40.0688 (12)0.7360 (8)0.4527 (3)0.0497 (17)
C50.0597 (10)0.6762 (8)0.4166 (2)0.0468 (16)
H50.19850.63180.42300.056*
C60.0186 (11)0.6820 (12)0.3697 (3)0.049 (2)
H60.07000.64230.34470.059*
C70.3079 (11)0.7367 (8)0.3107 (3)0.0463 (16)
H70.21080.70990.28620.056*
C80.5757 (9)0.7501 (6)0.2515 (2)0.0350 (14)
C90.7727 (8)0.8355 (7)0.2403 (2)0.0356 (14)
H90.85070.89370.26450.043*
C100.8535 (9)0.8355 (7)0.1949 (2)0.0388 (14)
H100.98330.89560.18800.047*
C110.7415 (9)0.7457 (7)0.1590 (2)0.0342 (13)
C120.5511 (10)0.6601 (10)0.1690 (2)0.0375 (16)
H120.47710.60010.14460.045*
C130.4639 (9)0.6596 (7)0.2147 (2)0.0381 (14)
H130.33310.60000.22090.046*
C141.0077 (11)0.8162 (12)0.0993 (3)0.068 (2)
H14A0.99310.94750.10050.102*
H14B1.04720.77970.06740.102*
H14C1.11860.77770.12130.102*
N10.5029 (8)0.7632 (7)0.3001 (2)0.0428 (13)
O10.8083 (7)0.7336 (5)0.11189 (16)0.0498 (12)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0775 (5)0.0926 (6)0.0447 (4)0.0006 (3)0.0177 (5)0.0023 (8)
C10.043 (4)0.036 (4)0.040 (4)0.009 (3)0.000 (3)0.004 (3)
C20.038 (4)0.050 (4)0.052 (4)0.003 (3)0.004 (3)0.003 (3)
C30.059 (5)0.059 (4)0.042 (4)0.011 (3)0.007 (3)0.004 (3)
C40.070 (5)0.040 (4)0.040 (4)0.002 (3)0.012 (3)0.002 (3)
C50.043 (4)0.049 (4)0.049 (4)0.006 (3)0.009 (3)0.004 (3)
C60.041 (4)0.055 (5)0.052 (6)0.001 (3)0.012 (4)0.006 (4)
C70.048 (4)0.045 (4)0.046 (4)0.002 (3)0.007 (3)0.003 (3)
C80.038 (3)0.024 (3)0.043 (4)0.003 (2)0.002 (3)0.008 (3)
C90.033 (3)0.035 (3)0.039 (4)0.002 (2)0.008 (3)0.000 (3)
C100.032 (3)0.032 (3)0.052 (4)0.005 (2)0.001 (3)0.004 (3)
C110.036 (3)0.035 (3)0.032 (3)0.013 (3)0.003 (3)0.005 (3)
C120.032 (3)0.044 (4)0.037 (4)0.005 (3)0.001 (3)0.006 (3)
C130.032 (3)0.035 (3)0.047 (4)0.008 (2)0.003 (3)0.000 (3)
C140.055 (5)0.106 (6)0.043 (5)0.005 (4)0.004 (3)0.014 (4)
N10.042 (3)0.047 (3)0.039 (3)0.007 (2)0.003 (2)0.005 (2)
O10.048 (3)0.063 (3)0.039 (3)0.0046 (19)0.003 (2)0.004 (2)
Geometric parameters (Å, º) top
Br1—C41.905 (7)C8—C131.400 (9)
C1—C61.376 (9)C8—N11.431 (9)
C1—C21.404 (9)C9—C101.363 (7)
C1—C71.461 (9)C9—H90.9300
C2—C31.370 (9)C10—C111.379 (8)
C2—H20.9300C10—H100.9300
C3—C41.388 (9)C11—C121.356 (8)
C3—H30.9300C11—O11.381 (7)
C4—C51.352 (10)C12—C131.383 (9)
C5—C61.397 (10)C12—H120.9300
C5—H50.9300C13—H130.9300
C6—H60.9300C14—O11.411 (8)
C7—N11.251 (8)C14—H14A0.9600
C7—H70.9300C14—H14B0.9600
C8—C91.397 (7)C14—H14C0.9600
C6—C1—C2118.3 (7)C10—C9—C8121.6 (6)
C6—C1—C7119.9 (6)C10—C9—H9119.2
C2—C1—C7121.7 (6)C8—C9—H9119.2
C3—C2—C1120.6 (7)C9—C10—C11119.6 (5)
C3—C2—H2119.7C9—C10—H10120.2
C1—C2—H2119.7C11—C10—H10120.2
C2—C3—C4119.5 (7)C12—C11—C10119.9 (6)
C2—C3—H3120.2C12—C11—O1115.1 (6)
C4—C3—H3120.2C10—C11—O1124.9 (5)
C5—C4—C3121.2 (7)C11—C12—C13121.8 (6)
C5—C4—Br1118.9 (5)C11—C12—H12119.1
C3—C4—Br1119.9 (6)C13—C12—H12119.1
C4—C5—C6119.2 (6)C12—C13—C8119.0 (5)
C4—C5—H5120.4C12—C13—H13120.5
C6—C5—H5120.4C8—C13—H13120.5
C1—C6—C5121.2 (7)O1—C14—H14A109.5
C1—C6—H6119.4O1—C14—H14B109.5
C5—C6—H6119.4H14A—C14—H14B109.5
N1—C7—C1123.6 (6)O1—C14—H14C109.5
N1—C7—H7118.2H14A—C14—H14C109.5
C1—C7—H7118.2H14B—C14—H14C109.5
C9—C8—C13118.2 (6)C7—N1—C8121.0 (6)
C9—C8—N1116.9 (5)C11—O1—C14118.0 (5)
C13—C8—N1124.9 (5)

Experimental details

Crystal data
Chemical formulaC14H12BrNO
Mr290.15
Crystal system, space groupOrthorhombic, Pca21
Temperature (K)292
a, b, c (Å)6.1510 (8), 7.2726 (9), 27.914 (4)
V3)1248.7 (3)
Z4
Radiation typeMo Kα
µ (mm1)3.27
Crystal size (mm)0.10 × 0.10 × 0.06
Data collection
DiffractometerBruker SMART CCD
Absorption correctionMulti-scan
(SADABS; Bruker, 1997)
Tmin, Tmax0.728, 0.822
No. of measured, independent and
observed [I > 2σ(I)] reflections
8336, 2349, 1512
Rint0.063
(sin θ/λ)max1)0.667
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.064, 0.121, 1.06
No. of reflections2349
No. of parameters156
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.51, 0.32
Absolute structureFlack (1983), 764 Friedel pairs
Absolute structure parameter0.016 (18)

Computer programs: SMART (Bruker, 1997), SAINT (Bruker, 1997), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1997).

 

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