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In the title compound, C15H14BrNO, there are two mol­ecules in the asymmetric unit with different conformations, as illustrated by the dihedral angles between the aromatic ring planes of 17.4 (5) and 9.7 (5)°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807049094/hb2572sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807049094/hb2572Isup2.hkl
Contains datablock I

CCDC reference: 667351

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.015 Å
  • R factor = 0.059
  • wR factor = 0.222
  • Data-to-parameter ratio = 15.1

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT111_ALERT_2_B ADDSYM Detects (Pseudo) Centre of Symmetry ..... 86 PerFi
Alert level C PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.91 PLAT154_ALERT_1_C The su's on the Cell Angles are Equal (x 10000) 200 Deg. PLAT341_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 15
Alert level G ABSTM02_ALERT_3_G When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.912 Tmax scaled 0.833 Tmin scaled 0.783 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 28.23 From the CIF: _reflns_number_total 4908 Count of symmetry unique reflns 3319 Completeness (_total/calc) 147.88% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 1589 Fraction of Friedel pairs measured 0.479 Are heavy atom types Z>Si present yes PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 3
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 4 ALERT level G = General alerts; check 2 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 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

As part of our onging studies of Schiff bases (Ma et al., 2007) we now report the synthesis and structure of the title compound, (I), arising from the condensation of p-bromobenzaldehyde with 4-ethoxyaniline.

There are two molecules in the asymmetric unit of (I) (Fig. 1) with different conformations, as quantified by the dihedral angles between the armoatic ring planes of 17.4 (5)° and 9.7 (5)° for the C1 and C16 molecules, respectively.

Related literature top

For related literature, see: Ma et al. (2007).

Experimental top

p-Ethoxyaniline (2.50 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 C15H14Br1N1O1: C 59.23, H 4.64, N 4.60%; found: C 58.98, H 4.61, N 4.72%.

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

As part of our onging studies of Schiff bases (Ma et al., 2007) we now report the synthesis and structure of the title compound, (I), arising from the condensation of p-bromobenzaldehyde with 4-ethoxyaniline.

There are two molecules in the asymmetric unit of (I) (Fig. 1) with different conformations, as quantified by the dihedral angles between the armoatic ring planes of 17.4 (5)° and 9.7 (5)° for the C1 and C16 molecules, respectively.

For related literature, see: Ma et al. (2007).

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 the molecular structure of (I), with displacement ellipsoids drawn at the 50% probability level (H atoms are drawn as spheres of arbitrary radius).
N-(4-Bromobenzylidene)-4-ethoxyaniline top
Crystal data top
C15H14BrNOZ = 2
Mr = 304.17F(000) = 308
Triclinic, P1Dx = 1.506 Mg m3
Hall symbol: P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.0793 (10) ÅCell parameters from 2326 reflections
b = 8.5700 (11) Åθ = 2.5–24.4°
c = 10.3148 (13) ŵ = 3.05 mm1
α = 88.390 (2)°T = 293 K
β = 85.615 (2)°Block, colourless
γ = 70.393 (2)°0.10 × 0.10 × 0.06 mm
V = 670.81 (15) Å3
Data collection top
Bruker SMART CCD
diffractometer
4908 independent reflections
Radiation source: fine-focus sealed tube2957 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.058
ω scansθmax = 28.2°, θmin = 2.0°
Absorption correction: multi-scan
(SADABS; Bruker, 1997)
h = 1010
Tmin = 0.858, Tmax = 0.913k = 1111
7771 measured reflectionsl = 1312
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)] = 0.059H-atom parameters constrained
wR(F2) = 0.222 w = 1/[σ2(Fo2) + (0.1355P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
4908 reflectionsΔρmax = 0.67 e Å3
325 parametersΔρmin = 0.38 e Å3
3 restraintsAbsolute structure: Flack (1983), 1589 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.125 (19)
Crystal data top
C15H14BrNOγ = 70.393 (2)°
Mr = 304.17V = 670.81 (15) Å3
Triclinic, P1Z = 2
a = 8.0793 (10) ÅMo Kα radiation
b = 8.5700 (11) ŵ = 3.05 mm1
c = 10.3148 (13) ÅT = 293 K
α = 88.390 (2)°0.10 × 0.10 × 0.06 mm
β = 85.615 (2)°
Data collection top
Bruker SMART CCD
diffractometer
4908 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 1997)
2957 reflections with I > 2σ(I)
Tmin = 0.858, Tmax = 0.913Rint = 0.058
7771 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.059H-atom parameters constrained
wR(F2) = 0.222Δρmax = 0.67 e Å3
S = 1.03Δρmin = 0.38 e Å3
4908 reflectionsAbsolute structure: Flack (1983), 1589 Friedel pairs
325 parametersAbsolute structure parameter: 0.125 (19)
3 restraints
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
Br10.22363 (11)0.10639 (12)0.46304 (9)0.0755 (5)
Br20.24929 (11)0.45540 (12)0.45854 (9)0.0746 (5)
C70.2988 (14)0.1021 (14)0.7530 (13)0.051 (3)
H7A0.40050.10890.70820.061*
C20.0784 (14)0.0185 (13)0.4837 (10)0.058 (3)
H2A0.09320.03400.39420.070*
C220.8171 (15)0.5733 (14)0.7634 (10)0.044 (3)
H22A0.93470.51870.73720.053*
C90.5246 (13)0.2394 (11)0.8860 (9)0.046 (2)
H9A0.53300.25580.79660.055*
C80.4014 (12)0.1767 (12)0.9370 (10)0.044 (2)
C241.0866 (13)0.5919 (12)0.9241 (11)0.050 (2)
H24A1.12930.50460.86550.060*
N20.7844 (11)0.6655 (10)0.8580 (8)0.0442 (18)
C210.3703 (14)0.6083 (11)0.6459 (9)0.047 (2)
H21A0.25200.66850.66540.056*
O11.2500 (11)0.7989 (10)1.1729 (8)0.051 (2)
C280.8533 (12)0.8233 (11)1.0187 (9)0.044 (2)
H28A0.73510.88901.02630.053*
C170.5989 (12)0.4026 (12)0.5183 (10)0.053 (2)
H17A0.62990.32700.45030.064*
C60.0879 (12)0.0166 (12)0.6807 (9)0.047 (2)
H6A0.18580.03120.72590.057*
O20.7400 (10)0.2858 (10)1.1812 (7)0.048 (2)
C100.6409 (13)0.2811 (11)0.9618 (10)0.048 (2)
H10A0.72140.32680.92230.058*
C251.1941 (15)0.6240 (13)1.0027 (12)0.058 (3)
H25A1.31060.55401.00050.070*
C130.3944 (13)0.1517 (10)1.0740 (8)0.042 (2)
H13A0.31150.10821.11260.051*
C40.1760 (13)0.0553 (12)0.6805 (11)0.048 (2)
C230.9093 (15)0.6902 (12)0.9303 (11)0.046 (3)
C270.9710 (12)0.8582 (10)1.0945 (8)0.043 (2)
H27A0.93250.95021.14880.052*
C261.1393 (15)0.7604 (12)1.0900 (10)0.042 (2)
N10.2768 (12)0.1336 (10)0.8706 (8)0.0482 (19)
C110.6364 (15)0.2543 (11)1.0960 (10)0.041 (2)
C150.9732 (15)0.3761 (15)1.2359 (10)0.058 (3)
H15A1.05990.42291.20120.088*
H15B1.03090.27021.27420.088*
H15C0.89650.44871.30090.088*
C301.5091 (16)0.7643 (12)1.2688 (9)0.054 (3)
H30A1.63140.69971.27250.082*
H30B1.44840.76241.35230.082*
H30C1.49800.87651.24590.082*
C30.1990 (14)0.0285 (13)0.5487 (10)0.057 (2)
H3A0.29650.04200.50210.068*
C140.8666 (13)0.3548 (12)1.1279 (9)0.051 (2)
H14A0.80840.46121.08820.061*
H14B0.94330.28211.06150.061*
C190.6839 (15)0.5442 (12)0.6899 (9)0.044 (2)
C200.5079 (13)0.6343 (12)0.7134 (10)0.046 (2)
H20A0.47640.71650.77660.056*
C291.4326 (13)0.6951 (14)1.1719 (10)0.052 (2)
H29A1.49220.69651.08680.062*
H29B1.44220.58171.19380.062*
C180.7266 (13)0.4298 (12)0.5881 (11)0.057 (3)
H18A0.84450.37010.56650.068*
C10.0611 (15)0.0413 (13)0.5533 (11)0.057 (3)
C120.5048 (12)0.1892 (11)1.1491 (9)0.043 (2)
H12A0.49490.17221.23840.051*
C50.0303 (13)0.0308 (12)0.7459 (11)0.049 (2)
H5A0.01190.04660.83540.059*
C160.4229 (14)0.4914 (12)0.5527 (9)0.048 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0730 (10)0.0956 (11)0.0752 (9)0.0457 (10)0.0265 (8)0.0109 (9)
Br20.0686 (10)0.0923 (11)0.0770 (9)0.0416 (9)0.0176 (7)0.0163 (9)
C70.029 (5)0.053 (6)0.070 (8)0.008 (4)0.021 (5)0.025 (5)
C20.060 (6)0.074 (7)0.048 (6)0.031 (5)0.002 (5)0.020 (5)
C220.043 (6)0.062 (6)0.031 (6)0.020 (5)0.007 (5)0.002 (5)
C90.047 (6)0.043 (5)0.042 (6)0.008 (4)0.005 (5)0.001 (4)
C80.033 (5)0.042 (5)0.048 (6)0.002 (4)0.007 (4)0.014 (4)
C240.038 (5)0.040 (5)0.068 (7)0.005 (4)0.008 (5)0.020 (5)
N20.040 (4)0.044 (4)0.051 (5)0.016 (4)0.005 (4)0.004 (4)
C210.054 (6)0.048 (5)0.039 (5)0.018 (4)0.003 (4)0.008 (4)
O10.053 (5)0.057 (4)0.048 (4)0.023 (4)0.008 (4)0.017 (3)
C280.037 (5)0.035 (5)0.048 (5)0.006 (4)0.006 (4)0.004 (4)
C170.041 (5)0.055 (6)0.065 (7)0.015 (4)0.010 (5)0.021 (5)
C60.032 (5)0.068 (6)0.048 (6)0.026 (4)0.003 (4)0.012 (4)
O20.053 (5)0.063 (4)0.036 (4)0.028 (4)0.008 (3)0.008 (3)
C100.053 (6)0.036 (5)0.057 (6)0.015 (4)0.005 (5)0.003 (4)
C250.045 (6)0.037 (5)0.082 (8)0.005 (5)0.016 (6)0.019 (5)
C130.054 (6)0.043 (5)0.033 (5)0.022 (4)0.002 (4)0.002 (4)
C40.041 (5)0.046 (5)0.058 (6)0.013 (4)0.003 (5)0.014 (4)
C230.040 (6)0.035 (5)0.055 (7)0.004 (4)0.007 (5)0.004 (4)
C270.048 (5)0.036 (4)0.040 (5)0.007 (4)0.000 (4)0.007 (4)
C260.042 (5)0.041 (5)0.040 (5)0.007 (4)0.008 (4)0.007 (4)
N10.053 (5)0.050 (5)0.042 (5)0.017 (4)0.003 (4)0.014 (4)
C110.052 (5)0.028 (4)0.037 (5)0.004 (4)0.003 (4)0.000 (3)
C150.061 (7)0.083 (8)0.044 (6)0.040 (6)0.009 (5)0.002 (5)
C300.086 (8)0.051 (6)0.030 (5)0.025 (6)0.019 (5)0.006 (4)
C30.059 (6)0.068 (6)0.053 (6)0.031 (5)0.003 (5)0.015 (5)
C140.048 (6)0.060 (6)0.049 (6)0.026 (5)0.003 (5)0.002 (5)
C190.063 (7)0.044 (5)0.031 (5)0.024 (5)0.000 (5)0.002 (4)
C200.043 (6)0.048 (5)0.047 (6)0.013 (4)0.001 (5)0.018 (4)
C290.045 (6)0.070 (7)0.042 (6)0.020 (5)0.011 (5)0.003 (5)
C180.043 (5)0.052 (5)0.075 (7)0.012 (4)0.005 (5)0.023 (5)
C10.054 (6)0.053 (6)0.065 (7)0.015 (5)0.025 (5)0.010 (5)
C120.046 (5)0.049 (5)0.031 (5)0.013 (4)0.001 (4)0.007 (4)
C50.043 (5)0.057 (6)0.052 (6)0.019 (4)0.005 (5)0.020 (5)
C160.062 (7)0.054 (6)0.041 (5)0.034 (5)0.018 (5)0.007 (4)
Geometric parameters (Å, º) top
Br1—C11.900 (10)C6—H6A0.9300
Br2—C161.877 (9)O2—C111.350 (12)
C7—N11.237 (14)O2—C141.415 (12)
C7—C41.449 (13)C10—C111.397 (14)
C7—H7A0.9300C10—H10A0.9300
C2—C11.356 (16)C25—C261.423 (14)
C2—C31.392 (13)C25—H25A0.9300
C2—H2A0.9300C13—C121.346 (12)
C22—N21.228 (13)C13—H13A0.9300
C22—C191.453 (14)C4—C31.374 (15)
C22—H22A0.9300C4—C51.386 (14)
C9—C81.349 (15)C27—C261.335 (14)
C9—C101.405 (13)C27—H27A0.9300
C9—H9A0.9300C11—C121.426 (14)
C8—N11.410 (12)C15—C141.509 (13)
C8—C131.423 (13)C15—H15A0.9600
C24—C251.329 (15)C15—H15B0.9600
C24—C231.395 (14)C15—H15C0.9600
C24—H24A0.9300C30—C291.451 (13)
N2—C231.373 (13)C30—H30A0.9600
C21—C161.347 (14)C30—H30B0.9600
C21—C201.437 (14)C30—H30C0.9600
C21—H21A0.9300C3—H3A0.9300
O1—C261.404 (12)C14—H14A0.9700
O1—C291.444 (13)C14—H14B0.9700
C28—C271.387 (12)C19—C201.378 (14)
C28—C231.410 (14)C19—C181.400 (14)
C28—H28A0.9300C20—H20A0.9300
C17—C181.386 (13)C29—H29A0.9700
C17—C161.392 (14)C29—H29B0.9700
C17—H17A0.9300C18—H18A0.9300
C6—C11.327 (14)C12—H12A0.9300
C6—C51.379 (13)C5—H5A0.9300
N1—C7—C4124.2 (12)O1—C26—C25124.5 (11)
N1—C7—H7A117.9C7—N1—C8122.0 (10)
C4—C7—H7A117.9O2—C11—C10127.5 (9)
C1—C2—C3118.9 (9)O2—C11—C12116.5 (8)
C1—C2—H2A120.6C10—C11—C12116.0 (9)
C3—C2—H2A120.6C14—C15—H15A109.5
N2—C22—C19124.2 (11)C14—C15—H15B109.5
N2—C22—H22A117.9H15A—C15—H15B109.5
C19—C22—H22A117.9C14—C15—H15C109.5
C8—C9—C10123.0 (9)H15A—C15—H15C109.5
C8—C9—H9A118.5H15B—C15—H15C109.5
C10—C9—H9A118.5C29—C30—H30A109.5
C9—C8—N1127.6 (9)C29—C30—H30B109.5
C9—C8—C13116.7 (9)H30A—C30—H30B109.5
N1—C8—C13115.7 (9)C29—C30—H30C109.5
C25—C24—C23119.5 (11)H30A—C30—H30C109.5
C25—C24—H24A120.3H30B—C30—H30C109.5
C23—C24—H24A120.3C4—C3—C2120.9 (10)
C22—N2—C23124.6 (11)C4—C3—H3A119.5
C16—C21—C20115.9 (9)C2—C3—H3A119.5
C16—C21—H21A122.0O2—C14—C15108.5 (8)
C20—C21—H21A122.0O2—C14—H14A110.0
C26—O1—C29119.2 (8)C15—C14—H14A110.0
C27—C28—C23121.3 (9)O2—C14—H14B110.0
C27—C28—H28A119.4C15—C14—H14B110.0
C23—C28—H28A119.4H14A—C14—H14B108.4
C18—C17—C16118.3 (8)C20—C19—C18116.3 (10)
C18—C17—H17A120.8C20—C19—C22121.2 (10)
C16—C17—H17A120.8C18—C19—C22122.4 (10)
C1—C6—C5119.6 (9)C19—C20—C21123.6 (9)
C1—C6—H6A120.2C19—C20—H20A118.2
C5—C6—H6A120.2C21—C20—H20A118.2
C11—O2—C14116.0 (8)O1—C29—C30105.8 (9)
C11—C10—C9120.5 (9)O1—C29—H29A110.6
C11—C10—H10A119.8C30—C29—H29A110.6
C9—C10—H10A119.8O1—C29—H29B110.6
C24—C25—C26123.1 (11)C30—C29—H29B110.6
C24—C25—H25A118.4H29A—C29—H29B108.7
C26—C25—H25A118.4C17—C18—C19122.1 (9)
C12—C13—C8121.7 (9)C17—C18—H18A119.0
C12—C13—H13A119.1C19—C18—H18A119.0
C8—C13—H13A119.1C6—C1—C2121.9 (10)
C3—C4—C5117.4 (10)C6—C1—Br1119.8 (9)
C3—C4—C7123.1 (10)C2—C1—Br1118.2 (8)
C5—C4—C7119.5 (10)C13—C12—C11122.0 (8)
N2—C23—C24124.9 (10)C13—C12—H12A119.0
N2—C23—C28117.5 (9)C11—C12—H12A119.0
C24—C23—C28117.6 (11)C6—C5—C4121.2 (10)
C26—C27—C28120.3 (8)C6—C5—H5A119.4
C26—C27—H27A119.8C4—C5—H5A119.4
C28—C27—H27A119.8C21—C16—C17123.5 (9)
C27—C26—O1117.5 (9)C21—C16—Br2117.8 (8)
C27—C26—C25118.0 (10)C17—C16—Br2118.5 (7)

Experimental details

Crystal data
Chemical formulaC15H14BrNO
Mr304.17
Crystal system, space groupTriclinic, P1
Temperature (K)293
a, b, c (Å)8.0793 (10), 8.5700 (11), 10.3148 (13)
α, β, γ (°)88.390 (2), 85.615 (2), 70.393 (2)
V3)670.81 (15)
Z2
Radiation typeMo Kα
µ (mm1)3.05
Crystal size (mm)0.10 × 0.10 × 0.06
Data collection
DiffractometerBruker SMART CCD
Absorption correctionMulti-scan
(SADABS; Bruker, 1997)
Tmin, Tmax0.858, 0.913
No. of measured, independent and
observed [I > 2σ(I)] reflections
7771, 4908, 2957
Rint0.058
(sin θ/λ)max1)0.666
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.059, 0.222, 1.03
No. of reflections4908
No. of parameters325
No. of restraints3
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.67, 0.38
Absolute structureFlack (1983), 1589 Friedel pairs
Absolute structure parameter0.125 (19)

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

 

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