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The mol­ecule of the title compound, C14H12BrNO2, crystallizes in a zwitterionic form, with a strong intra­molecular N—H...O hydrogen bond. The dihedral angle between the aromatic rings is 9.3 (3)°. Inter­molecular O—H...O hydrogen bonds generate C(8) chains running parallel to the [100] direction.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807055304/ci2507sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807055304/ci2507Isup2.hkl
Contains datablock I

CCDC reference: 672837

Key indicators

  • Single-crystal X-ray study
  • T = 296 K
  • Mean [sigma](C-C) = 0.008 Å
  • R factor = 0.043
  • wR factor = 0.084
  • Data-to-parameter ratio = 15.3

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT063_ALERT_3_C Crystal Probably too Large for Beam Size ....... 0.80 mm PLAT341_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 8
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 26.00 From the CIF: _reflns_number_total 2549 Count of symmetry unique reflns 1515 Completeness (_total/calc) 168.25% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 1034 Fraction of Friedel pairs measured 0.683 Are heavy atom types Z>Si present yes
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 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 have been extensively used as ligands in the field of coordination chemistry (Calligaris et al., 1972). There are two characteristic properties of Schiff bases, viz. photochromism and thermochromism (Cohen et al., 1964). These properties result from proton transfer from the hydroxyl O atom to the imine N atom (Hadjoudis et al., 1987). Schiff bases display two possible tautomeric forms, namely the phenol-imine and keto-amine forms. In the solid state, the keto-amine tautomer has been found in naphthaldimine (Hökelek et al., 2000). Nevertheless, in the solid state, it has been established that there is keto-amine tautomerism in naphthaldimine, while the phenol-imine form exists in salicylaldimine Schiff bases (Dey et al., 2001). Our investigations show that compound (I) exists in a zwitterionic form.

An ORTEP-3 (Farrugia, 1997) plot of the molecule of (I) is shown in Fig.1. The C1—C7, C7N1 and N1—C8 bond lengths are 1.406 (6), 1.289 (6) and 1.409 (6) Å, respectively (Table 1), and agree with the corresponding distances in (Z)-6-[(2-fluorophenyliminio)methylene]-2,3-dihydroxyphenolate [1.419 (3), 1.295 (2) and 1.412 (2) Å; Petek et al., 2006]. In the zwitterionic form, the molecule of the title compound is nearly planar, with a dihedral angle between the aromatic rings of 9.3 (3)°.

Fig.1 also shows a strong intramolecular hydrogen bond (N1—H1···O1) can be described as an S(6) motif (Bernstein et al., 1995). Atom O2 in the reference molecule at (x, y, z) acts as a hydrogen-bond donor, via H2, to O1 in the molecule at (1/2 + x, 3/2 - y, 1 - z), so forming a C(8) chain running parallel to the [100] direction (Fig.2).

Related literature top

Schiff base compounds can be classified by their photochromic and thermochromic characteristics (Cohen et al., 1964; Hadjoudis et al., 1987). For ring motif details, see: Bernstein et al. (1995). For related literature, see: Calligaris et al. (1972); Dey et al. (2001); Hökelek et al. (2000); Petek et al. (2006).

Experimental top

A solution of 5-bromosalicylaldehyde (0.05 g, 0.25 mmol) in ethanol (20 ml) was added to a solution of 2-hydroxy-5-nitroaniline (0.038 g 0.25 mmol) in ethanol (20 ml). The reaction mixture was stirred for 1 h under reflux. Single crystals of the title compound suitable for X-ray analysis were obtained from ethanol by slow evaporation (yield 71%; m.p. 456–459 K).

Refinement top

Atom H1 was located in a difference map and refined freely. The remaining H atoms were placed in calculated positions and constrained to ride on their parents atoms, with C—H = 0.93–0.96 Å and Uiso(H) = kUeq(parent atom), where k = 1.5 for methyl and hydroxyl H atoms, and 1.2 for other H atoms.

Computing details top

Data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA (Stoe & Cie, 2002); data reduction: X-RED32 (Stoe & Cie, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 40% probability level.
[Figure 2] Fig. 2. View of the crystal packing of (I). Hydrogen bonds are drawn as dashed lines. H atoms not involved in the interactions have been omitted for clarity.
(E)-4-Bromo-2-[(2-hydroxy-5-methylphenyl)iminomethyl]phenol top
Crystal data top
C14H12BrNO2F(000) = 616
Mr = 306.16Dx = 1.548 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P2ac 2abCell parameters from 5730 reflections
a = 8.2763 (8) Åθ = 2.2–29.5°
b = 8.4451 (9) ŵ = 3.12 mm1
c = 18.795 (2) ÅT = 296 K
V = 1313.7 (2) Å3Prism, brown
Z = 40.80 × 0.37 × 0.13 mm
Data collection top
Stoe IPDS II
diffractometer
2549 independent reflections
Radiation source: fine-focus sealed tube1541 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.073
Detector resolution: 6.67 pixels mm-1θmax = 26.0°, θmin = 2.2°
rotation method scansh = 1010
Absorption correction: integration
(X-RED32; Stoe & Cie, 2002)
k = 106
Tmin = 0.289, Tmax = 0.680l = 2323
6028 measured reflections
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)] = 0.043H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.084 w = 1/[σ2(Fo2) + (0.0287P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.91(Δ/σ)max = 0.001
2549 reflectionsΔρmax = 0.31 e Å3
167 parametersΔρmin = 0.30 e Å3
0 restraintsAbsolute structure: Flack (1983); 1052 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.010 (15)
Crystal data top
C14H12BrNO2V = 1313.7 (2) Å3
Mr = 306.16Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 8.2763 (8) ŵ = 3.12 mm1
b = 8.4451 (9) ÅT = 296 K
c = 18.795 (2) Å0.80 × 0.37 × 0.13 mm
Data collection top
Stoe IPDS II
diffractometer
2549 independent reflections
Absorption correction: integration
(X-RED32; Stoe & Cie, 2002)
1541 reflections with I > 2σ(I)
Tmin = 0.289, Tmax = 0.680Rint = 0.073
6028 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.043H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.084Δρmax = 0.31 e Å3
S = 0.91Δρmin = 0.30 e Å3
2549 reflectionsAbsolute structure: Flack (1983); 1052 Friedel pairs
167 parametersAbsolute structure parameter: 0.010 (15)
0 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
C10.5123 (5)0.4814 (6)0.6768 (3)0.0472 (11)
C20.4416 (5)0.6051 (8)0.6358 (2)0.0529 (15)
C30.2843 (5)0.6545 (7)0.6554 (3)0.0558 (15)
H30.23550.73660.63040.067*
C40.2033 (6)0.5854 (7)0.7097 (3)0.0551 (16)
H40.09910.61850.72070.066*
C50.2749 (6)0.4652 (7)0.7491 (2)0.0509 (14)
C60.4245 (6)0.4155 (7)0.7336 (2)0.0558 (16)
H60.47120.33590.76090.067*
C70.6666 (6)0.4226 (6)0.6601 (2)0.0526 (13)
H70.70820.33970.68700.063*
C80.9084 (5)0.4353 (7)0.5857 (2)0.0450 (13)
C90.9898 (6)0.3034 (7)0.6103 (2)0.0498 (13)
H90.94240.23990.64490.060*
C101.1407 (7)0.2646 (7)0.5841 (3)0.0591 (14)
C111.2065 (6)0.3619 (10)0.5315 (3)0.0684 (17)
H111.30660.33640.51210.082*
C121.1267 (6)0.4950 (8)0.5073 (2)0.0607 (15)
H121.17380.55890.47270.073*
C130.9777 (6)0.5331 (7)0.5346 (2)0.0497 (13)
C141.2316 (7)0.1219 (9)0.6121 (3)0.086 (2)
H14A1.21180.11070.66220.129*
H14B1.34530.13610.60410.129*
H14C1.19540.02850.58780.129*
N10.7527 (5)0.4790 (6)0.6088 (2)0.0493 (12)
H10.703 (6)0.544 (7)0.585 (2)0.059*
O10.5191 (4)0.6667 (5)0.58287 (17)0.0631 (12)
O20.8903 (4)0.6614 (5)0.51439 (17)0.0657 (11)
H20.94040.71110.48410.098*
Br10.15523 (6)0.36922 (9)0.82415 (3)0.0725 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.045 (2)0.043 (3)0.053 (2)0.004 (2)0.001 (3)0.009 (3)
C20.058 (3)0.049 (5)0.052 (3)0.008 (3)0.014 (2)0.001 (3)
C30.059 (3)0.036 (4)0.072 (3)0.009 (3)0.016 (2)0.003 (3)
C40.047 (3)0.057 (5)0.061 (3)0.005 (3)0.004 (2)0.008 (3)
C50.054 (3)0.048 (4)0.051 (3)0.002 (3)0.001 (2)0.001 (3)
C60.054 (3)0.053 (5)0.060 (3)0.005 (3)0.000 (2)0.014 (3)
C70.059 (3)0.051 (3)0.047 (3)0.000 (3)0.001 (2)0.020 (2)
C80.050 (3)0.042 (4)0.043 (2)0.004 (2)0.002 (2)0.006 (2)
C90.058 (3)0.044 (4)0.048 (3)0.003 (3)0.009 (2)0.008 (2)
C100.068 (3)0.040 (4)0.069 (3)0.003 (3)0.009 (3)0.006 (3)
C110.071 (3)0.067 (5)0.067 (3)0.000 (4)0.028 (3)0.019 (4)
C120.075 (4)0.055 (4)0.052 (3)0.014 (3)0.010 (3)0.004 (3)
C130.059 (3)0.039 (4)0.051 (3)0.006 (3)0.001 (2)0.004 (3)
C140.085 (4)0.056 (5)0.117 (5)0.022 (4)0.025 (3)0.016 (5)
N10.047 (2)0.046 (3)0.054 (3)0.004 (2)0.0036 (19)0.013 (2)
O10.064 (2)0.056 (3)0.069 (2)0.003 (2)0.0036 (17)0.031 (2)
O20.073 (2)0.058 (3)0.0655 (19)0.003 (2)0.0138 (17)0.030 (2)
Br10.0639 (3)0.0783 (5)0.0753 (3)0.0022 (4)0.0147 (3)0.0103 (4)
Geometric parameters (Å, º) top
C1—C61.406 (6)C8—N11.409 (6)
C1—C71.406 (6)C9—C101.382 (7)
C1—C21.424 (7)C9—H90.93
C2—O11.293 (6)C10—C111.397 (8)
C2—C31.415 (7)C10—C141.515 (8)
C3—C41.354 (7)C11—C121.380 (9)
C3—H30.93C11—H110.93
C4—C51.389 (7)C12—C131.373 (7)
C4—H40.93C12—H120.93
C5—C61.340 (6)C13—O21.357 (6)
C5—Br11.905 (5)C14—H14A0.96
C6—H60.93C14—H14B0.96
C7—N11.289 (6)C14—H14C0.96
C7—H70.93N1—H10.82 (5)
C8—C91.381 (7)O2—H20.82
C8—C131.390 (7)
C6—C1—C7119.9 (5)C8—C9—H9119.6
C6—C1—C2119.3 (4)C10—C9—H9119.6
C7—C1—C2120.8 (4)C9—C10—C11117.7 (5)
O1—C2—C3122.5 (5)C9—C10—C14121.0 (5)
O1—C2—C1120.5 (4)C11—C10—C14121.4 (5)
C3—C2—C1117.0 (5)C12—C11—C10121.7 (5)
C4—C3—C2121.6 (5)C12—C11—H11119.1
C4—C3—H3119.2C10—C11—H11119.1
C2—C3—H3119.2C13—C12—C11119.8 (5)
C3—C4—C5120.4 (5)C13—C12—H12120.1
C3—C4—H4119.8C11—C12—H12120.1
C5—C4—H4119.8O2—C13—C12124.1 (5)
C6—C5—C4120.5 (5)O2—C13—C8116.6 (4)
C6—C5—Br1120.5 (4)C12—C13—C8119.3 (5)
C4—C5—Br1118.9 (4)C10—C14—H14A109.5
C5—C6—C1121.2 (5)C10—C14—H14B109.5
C5—C6—H6119.4H14A—C14—H14B109.5
C1—C6—H6119.4C10—C14—H14C109.5
N1—C7—C1122.6 (5)H14A—C14—H14C109.5
N1—C7—H7118.7H14B—C14—H14C109.5
C1—C7—H7118.7C7—N1—C8129.7 (5)
C9—C8—C13120.6 (5)C7—N1—H1112 (3)
C9—C8—N1123.6 (5)C8—N1—H1118 (3)
C13—C8—N1115.8 (5)C13—O2—H2109.5
C8—C9—C10120.9 (5)
C6—C1—C2—O1179.4 (5)N1—C8—C9—C10178.3 (5)
C7—C1—C2—O10.7 (8)C8—C9—C10—C110.9 (8)
C6—C1—C2—C30.0 (8)C8—C9—C10—C14178.7 (5)
C7—C1—C2—C3178.6 (5)C9—C10—C11—C121.8 (9)
O1—C2—C3—C4178.0 (5)C14—C10—C11—C12177.8 (6)
C1—C2—C3—C41.3 (8)C10—C11—C12—C131.0 (9)
C2—C3—C4—C51.5 (8)C11—C12—C13—O2179.8 (5)
C3—C4—C5—C60.4 (8)C11—C12—C13—C80.7 (8)
C3—C4—C5—Br1179.2 (4)C9—C8—C13—O2178.9 (4)
C4—C5—C6—C10.9 (8)N1—C8—C13—O21.9 (6)
Br1—C5—C6—C1177.8 (4)C9—C8—C13—C121.6 (7)
C7—C1—C6—C5177.5 (5)N1—C8—C13—C12177.6 (5)
C2—C1—C6—C51.1 (8)C1—C7—N1—C8179.4 (5)
C6—C1—C7—N1179.6 (5)C9—C8—N1—C79.0 (8)
C2—C1—C7—N11.7 (8)C13—C8—N1—C7171.8 (5)
C13—C8—C9—C100.8 (7)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···O1i0.821.752.566 (5)171
N1—H1···O10.82 (5)1.84 (5)2.547 (6)144 (5)
Symmetry code: (i) x+1/2, y+3/2, z+1.

Experimental details

Crystal data
Chemical formulaC14H12BrNO2
Mr306.16
Crystal system, space groupOrthorhombic, P212121
Temperature (K)296
a, b, c (Å)8.2763 (8), 8.4451 (9), 18.795 (2)
V3)1313.7 (2)
Z4
Radiation typeMo Kα
µ (mm1)3.12
Crystal size (mm)0.80 × 0.37 × 0.13
Data collection
DiffractometerStoe IPDS II
diffractometer
Absorption correctionIntegration
(X-RED32; Stoe & Cie, 2002)
Tmin, Tmax0.289, 0.680
No. of measured, independent and
observed [I > 2σ(I)] reflections
6028, 2549, 1541
Rint0.073
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.084, 0.91
No. of reflections2549
No. of parameters167
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.31, 0.30
Absolute structureFlack (1983); 1052 Friedel pairs
Absolute structure parameter0.010 (15)

Computer programs: X-AREA (Stoe & Cie, 2002), X-RED32 (Stoe & Cie, 2002), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), WinGX (Farrugia, 1999).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···O1i0.821.752.566 (5)171
N1—H1···O10.82 (5)1.84 (5)2.547 (6)144 (5)
Symmetry code: (i) x+1/2, y+3/2, z+1.
 

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