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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Nov 28;68(Pt 12):o3465. doi: 10.1107/S1600536812046995

2-(4-Methyl­phen­yl)-2-oxoethyl 3-bromo­benzoate

Imtiaz Khan a,*, Aliya Ibrar a, Artur Korzański b, Maciej Kubicki b
PMCID: PMC3589039  PMID: 23476275

Abstract

The mol­ecule of the title compound, C16H13BrO3, is built of two approximately planar fragments, viz. 3-bromo­benzoate [maximum deviation = 0.055 (2) Å and 2-oxo-2-p-tolyl­ethyl [maximum deviation = 0.042 (2) Å], inclined by 46.51 (7)°. In the crystal, weak C—H⋯O hydrogen bonds and Br⋯Br contacts [3.6491 (7) Å] connect the mol­ecules into infinite layers parallel to (-221).

Related literature  

For the structures of similar compounds, see: Fun, Arshad et al. (2011); Fun, Loh et al. (2011); Fun, Ooi et al. (2011); Fun, Shahani et al. (2011).graphic file with name e-68-o3465-scheme1.jpg

Experimental  

Crystal data  

  • C16H13BrO3

  • M r = 333.17

  • Triclinic, Inline graphic

  • a = 4.7977 (3) Å

  • b = 10.9951 (7) Å

  • c = 14.1645 (8) Å

  • α = 74.829 (5)°

  • β = 87.758 (5)°

  • γ = 79.327 (5)°

  • V = 708.64 (7) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 2.90 mm−1

  • T = 295 K

  • 0.25 × 0.2 × 0.08 mm

Data collection  

  • Agilent Xcalibur Eos diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) T min = 0.335, T max = 1.000

  • 7924 measured reflections

  • 2501 independent reflections

  • 1768 reflections with I > 2σ(I)

  • R int = 0.026

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.038

  • wR(F 2) = 0.106

  • S = 1.05

  • 2501 reflections

  • 192 parameters

  • H-atom parameters constrained

  • Δρmax = 0.44 e Å−3

  • Δρmin = −0.42 e Å−3

Data collection: CrysAlis PRO (Agilent, 2010); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812046995/ng5304sup1.cif

e-68-o3465-sup1.cif (21.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812046995/ng5304Isup2.hkl

e-68-o3465-Isup2.hkl (120.3KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812046995/ng5304Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C5—H5⋯O10i 0.93 2.44 3.198 (4) 139
C9—H92⋯O7ii 0.97 2.56 3.406 (4) 146

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

supplementary crystallographic information

Comment

Keto esters, an important class of versatile intermediates, are extensively used in agrochemical, pharmaceutical, and dyestuff industries. They are also useful organic building blocks for the synthesis of complex natural products and are frequently employed synthons in organic synthesis, especially in heterocyclic synthesis. Prompted by literature findings, we herein report the synthesis of 2-(4-methylphenyl)-2-oxoethyl 3-bromobenzoate which can be used as an effective synthon in heterocyclic chemistry. The formation of keto ester (1) was confirmed by the changes in the spectral properties such as IR absorptions, 1H and 13C NMR signals for dominant functional groups. The conformation of molecule (1) can be described by the dihedral angle between two approximately planar fragments: 3-bromobenzoate (maximum deviation from the least-squares plane is 0.055 (2) Å) and 2-oxo-2-p-tolylethyl (0.042 (2) Å). In the crystal, this angle is 46.51 (7) ° (Fig. 1). In similarly substituted (para-meta) analogues, this angle was much smaller: in 2-(4-fluorophenyl)-2-oxoethyl 3-(trifluoromethyl)benzoate (Fun, Arshad et al., 2011) this angle is 20.34 (9)°, in 2-(4-chlorophenyl)-2-oxoethyl 3-(trifluoromethyl)benzoate (Fun, Loh et al., 2011) - 15.50 (8)°; on the other hand, this angle was larger in some other similar compounds: 66.66 (8)° in 2-(4-bromophenyl)-2-oxoethyl 2-methylbenzoate (Fun, Ooi et al., 2011) and 80.70 (7)° in 2-(4-bromophenyl)-2-oxoethyl 4-methylbenzoate (Fun, Shahani et al., 2011).

Weak but directional C—H···O hydrogen bonds and C—Br···Br(-1 - x,1 - y,-z) halogen interactions (Br···Br 3.6491 (7) Å, C—Br···Br 164.37 (10) °) connect molecules into layers approximately parallel to (-221) plane (Fig. 2); these planes are interacting with one another by means of weak C—H···O contacts and van der Waals interactions.

Experimental

2-(4-Methylphenyl)-2-oxoethyl 3-bromobenzoate (1) was synthesized by treating 3-bromobenzoic acid (0.01 mol) with the solution of 2-bromo-1-p-tolylethanone (0.01 mol) in N,N-dimethylformamide (DMF) using triethylamine (TEA) as a catalyst at room temperature for 2 h. Yield: 87%; m.p 96–97°C; Rf: 0.27 (n-hexane: ethyl acetate, 9: 1); IR (neat, cm-1): 3034 (Csp2-H), 2924, 2853 (Csp3-H), 1728 (C=Oester), 1685 (C=Oketo), 1585, 1561 (C=C), 1230 (C—O); 1H NMR (300 MHz, CDCl3): δ 8.08–8.04 (m, 1H, Ar—H), 7.88 (d, 2H, J = 8.4 Hz, Ar—H), 7.72–7.68 (m, 1H, Ar—H), 7.45–7.36 (m, 2H, Ar—H), 7.35–7.28 (m, 2H, Ar—H), 5.59 (s, 2H, OCH2), 2.44 (s, 3H, CH3); 13C NMR (75 MHz, CDCl3): δ 191.33, 165.44, 145.06, 134.42, 133.02, 132.04, 131.61, 131.21, 129.64, 127.94, 127.30, 122.07, 66.65, 21.85.

Crystals were obtained by recrystallization from ethyl acetate.

Refinement

Hydrogen atoms were placed geometrically and refined as riding model with isotropic thermal parameters.

Figures

Fig. 1.

Fig. 1.

Anisotropic ellipsoid representation of 1 together with atom labelling scheme. The ellipsoids are drawn at 50% probability level, hydrogen atoms are depicted as spheres with arbitrary radii.

Fig. 2.

Fig. 2.

The layer of the molecules connected by weak C—H···O and Br···Br interactions

Crystal data

C16H13BrO3 Z = 2
Mr = 333.17 F(000) = 336
Triclinic, P1 Dx = 1.561 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 4.7977 (3) Å Cell parameters from 2186 reflections
b = 10.9951 (7) Å θ = 3.0–29.0°
c = 14.1645 (8) Å µ = 2.90 mm1
α = 74.829 (5)° T = 295 K
β = 87.758 (5)° Plate, colourless
γ = 79.327 (5)° 0.25 × 0.2 × 0.08 mm
V = 708.64 (7) Å3

Data collection

Agilent Xcalibur Eos diffractometer 2501 independent reflections
Radiation source: Enhance (Mo) X-ray Source 1768 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.026
Detector resolution: 16.1544 pixels mm-1 θmax = 25.0°, θmin = 3.0°
ω–scan h = −5→5
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) k = −12→13
Tmin = 0.335, Tmax = 1.000 l = −16→16
7924 measured reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.106 H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.053P)2 + 0.0904P] where P = (Fo2 + 2Fc2)/3
2501 reflections (Δ/σ)max = 0.001
192 parameters Δρmax = 0.44 e Å3
0 restraints Δρmin = −0.42 e Å3

Special details

Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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)

x y z Uiso*/Ueq
C1 −0.0123 (5) 0.2958 (2) 0.3969 (2) 0.0458 (6)
C2 −0.0749 (6) 0.3618 (3) 0.3014 (2) 0.0526 (7)
H2 −0.0098 0.4380 0.2744 0.049 (8)*
C3 −0.2350 (6) 0.3141 (3) 0.2459 (2) 0.0600 (8)
Br3 −0.32035 (10) 0.40451 (4) 0.11376 (3) 0.1043 (2)
C4 −0.3331 (7) 0.2016 (3) 0.2848 (3) 0.0694 (9)
H4 −0.4406 0.1701 0.2467 0.079 (10)*
C5 −0.2713 (7) 0.1369 (3) 0.3799 (3) 0.0715 (9)
H5 −0.3383 0.0612 0.4067 0.088 (12)*
C6 −0.1099 (6) 0.1829 (3) 0.4368 (2) 0.0576 (7)
H6 −0.0674 0.1381 0.5015 0.069 (9)*
C7 0.1605 (6) 0.3501 (3) 0.4556 (2) 0.0473 (7)
O7 0.2638 (5) 0.4429 (2) 0.42375 (15) 0.0679 (6)
O8 0.1859 (5) 0.2813 (2) 0.54790 (14) 0.0658 (6)
C9 0.3630 (7) 0.3139 (3) 0.6129 (2) 0.0609 (8)
H91 0.2473 0.3539 0.6581 0.081 (11)*
H92 0.4775 0.3739 0.5760 0.071 (10)*
C10 0.5507 (6) 0.1933 (3) 0.6681 (2) 0.0524 (7)
O10 0.5558 (5) 0.0932 (2) 0.64683 (19) 0.0828 (7)
C11 0.7323 (6) 0.1995 (3) 0.74883 (19) 0.0492 (7)
C12 0.9153 (7) 0.0901 (3) 0.7958 (2) 0.0662 (8)
H12 0.9238 0.0154 0.7758 0.084 (11)*
C13 1.0847 (7) 0.0896 (3) 0.8713 (3) 0.0729 (9)
H13 1.2053 0.0143 0.9022 0.090 (11)*
C14 1.0804 (6) 0.1984 (3) 0.9026 (2) 0.0621 (8)
C141 1.2672 (8) 0.1975 (4) 0.9864 (3) 0.0861 (11)
H14A 1.2630 0.2839 0.9899 0.129*
H14B 1.4583 0.1588 0.9760 0.129*
H14C 1.1988 0.1493 1.0466 0.129*
C15 0.8999 (7) 0.3084 (3) 0.8553 (2) 0.0625 (8)
H15 0.8935 0.3831 0.8751 0.087 (12)*
C16 0.7272 (6) 0.3098 (3) 0.7786 (2) 0.0567 (8)
H16 0.6078 0.3852 0.7471 0.057 (8)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0446 (15) 0.0450 (15) 0.0505 (16) −0.0089 (12) −0.0063 (12) −0.0156 (12)
C2 0.0567 (17) 0.0521 (17) 0.0504 (16) −0.0082 (13) −0.0129 (13) −0.0148 (13)
C3 0.0624 (19) 0.0616 (19) 0.0565 (18) 0.0044 (15) −0.0214 (14) −0.0239 (15)
Br3 0.1370 (4) 0.1121 (4) 0.0632 (3) −0.0071 (3) −0.0476 (2) −0.0254 (2)
C4 0.063 (2) 0.070 (2) 0.086 (2) −0.0042 (16) −0.0257 (17) −0.0422 (19)
C5 0.076 (2) 0.0570 (19) 0.089 (3) −0.0188 (16) −0.0179 (19) −0.0251 (18)
C6 0.0611 (19) 0.0512 (17) 0.0621 (19) −0.0100 (14) −0.0132 (14) −0.0155 (15)
C7 0.0496 (16) 0.0497 (16) 0.0443 (15) −0.0114 (13) −0.0086 (12) −0.0124 (13)
O7 0.0873 (16) 0.0654 (13) 0.0551 (12) −0.0380 (12) −0.0191 (11) −0.0034 (10)
O8 0.0865 (15) 0.0708 (13) 0.0456 (12) −0.0411 (11) −0.0199 (10) −0.0032 (10)
C9 0.077 (2) 0.0640 (18) 0.0477 (17) −0.0278 (16) −0.0182 (16) −0.0116 (15)
C10 0.0626 (18) 0.0583 (18) 0.0428 (15) −0.0261 (14) 0.0009 (13) −0.0140 (13)
O10 0.1036 (18) 0.0669 (14) 0.0898 (17) −0.0245 (13) −0.0233 (14) −0.0314 (13)
C11 0.0514 (17) 0.0560 (16) 0.0409 (15) −0.0174 (13) −0.0016 (12) −0.0080 (13)
C12 0.067 (2) 0.0602 (19) 0.071 (2) −0.0069 (15) −0.0087 (17) −0.0184 (16)
C13 0.061 (2) 0.074 (2) 0.075 (2) 0.0002 (17) −0.0183 (17) −0.0108 (18)
C14 0.0527 (18) 0.085 (2) 0.0456 (16) −0.0219 (16) −0.0094 (13) −0.0029 (16)
C141 0.072 (2) 0.114 (3) 0.068 (2) −0.025 (2) −0.0261 (18) −0.006 (2)
C15 0.071 (2) 0.071 (2) 0.0503 (17) −0.0276 (16) −0.0097 (15) −0.0121 (15)
C16 0.069 (2) 0.0532 (17) 0.0463 (16) −0.0164 (14) −0.0158 (14) −0.0035 (14)

Geometric parameters (Å, º)

C1—C2 1.372 (4) C9—H92 0.9700
C1—C6 1.382 (4) C10—O10 1.210 (4)
C1—C7 1.494 (4) C10—C11 1.488 (4)
C2—C3 1.376 (4) C11—C12 1.378 (4)
C2—H2 0.9300 C11—C16 1.379 (4)
C3—C4 1.376 (5) C12—C13 1.367 (5)
C3—Br3 1.895 (3) C12—H12 0.9300
C4—C5 1.364 (5) C13—C14 1.376 (5)
C4—H4 0.9300 C13—H13 0.9300
C5—C6 1.382 (4) C14—C15 1.377 (4)
C5—H5 0.9300 C14—C141 1.512 (4)
C6—H6 0.9300 C141—H14A 0.9600
C7—O7 1.191 (3) C141—H14B 0.9600
C7—O8 1.325 (3) C141—H14C 0.9600
O8—C9 1.430 (3) C15—C16 1.387 (4)
C9—C10 1.501 (4) C15—H15 0.9300
C9—H91 0.9700 C16—H16 0.9300
C2—C1—C6 120.2 (3) O10—C10—C11 120.7 (3)
C2—C1—C7 118.2 (2) O10—C10—C9 120.7 (3)
C6—C1—C7 121.5 (2) C11—C10—C9 118.6 (3)
C1—C2—C3 119.4 (3) C12—C11—C16 118.4 (3)
C1—C2—H2 120.3 C12—C11—C10 118.4 (3)
C3—C2—H2 120.3 C16—C11—C10 123.2 (3)
C4—C3—C2 120.9 (3) C13—C12—C11 121.0 (3)
C4—C3—Br3 119.6 (2) C13—C12—H12 119.5
C2—C3—Br3 119.5 (2) C11—C12—H12 119.5
C5—C4—C3 119.4 (3) C12—C13—C14 121.4 (3)
C5—C4—H4 120.3 C12—C13—H13 119.3
C3—C4—H4 120.3 C14—C13—H13 119.3
C4—C5—C6 120.6 (3) C13—C14—C15 117.9 (3)
C4—C5—H5 119.7 C13—C14—C141 121.3 (3)
C6—C5—H5 119.7 C15—C14—C141 120.9 (3)
C1—C6—C5 119.5 (3) C14—C141—H14A 109.5
C1—C6—H6 120.3 C14—C141—H14B 109.5
C5—C6—H6 120.3 H14A—C141—H14B 109.5
O7—C7—O8 124.1 (3) C14—C141—H14C 109.5
O7—C7—C1 124.5 (2) H14A—C141—H14C 109.5
O8—C7—C1 111.3 (2) H14B—C141—H14C 109.5
C7—O8—C9 118.8 (2) C14—C15—C16 121.2 (3)
O8—C9—C10 108.3 (2) C14—C15—H15 119.4
O8—C9—H91 110.0 C16—C15—H15 119.4
C10—C9—H91 110.0 C11—C16—C15 120.1 (3)
O8—C9—H92 110.0 C11—C16—H16 119.9
C10—C9—H92 110.0 C15—C16—H16 119.9
H91—C9—H92 108.4
C6—C1—C2—C3 −0.2 (4) O8—C9—C10—O10 7.5 (4)
C7—C1—C2—C3 −179.7 (2) O8—C9—C10—C11 −173.0 (2)
C1—C2—C3—C4 0.1 (4) O10—C10—C11—C12 2.9 (4)
C1—C2—C3—Br3 −179.7 (2) C9—C10—C11—C12 −176.6 (3)
C2—C3—C4—C5 0.2 (5) O10—C10—C11—C16 −177.5 (3)
Br3—C3—C4—C5 −180.0 (2) C9—C10—C11—C16 3.1 (4)
C3—C4—C5—C6 −0.5 (5) C16—C11—C12—C13 1.2 (5)
C2—C1—C6—C5 −0.1 (4) C10—C11—C12—C13 −179.2 (3)
C7—C1—C6—C5 179.4 (3) C11—C12—C13—C14 −0.5 (5)
C4—C5—C6—C1 0.4 (5) C12—C13—C14—C15 −0.1 (5)
C2—C1—C7—O7 −5.0 (4) C12—C13—C14—C141 179.8 (3)
C6—C1—C7—O7 175.5 (3) C13—C14—C15—C16 0.1 (5)
C2—C1—C7—O8 175.4 (2) C141—C14—C15—C16 −179.8 (3)
C6—C1—C7—O8 −4.1 (4) C12—C11—C16—C15 −1.2 (4)
O7—C7—O8—C9 −4.4 (4) C10—C11—C16—C15 179.2 (3)
C1—C7—O8—C9 175.2 (2) C14—C15—C16—C11 0.5 (5)
C7—O8—C9—C10 −132.6 (3)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C5—H5···O10i 0.93 2.44 3.198 (4) 139
C9—H92···O7ii 0.97 2.56 3.406 (4) 146

Symmetry codes: (i) −x, −y, −z+1; (ii) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG5304).

References

  1. Agilent (2010). CrysAlis PRO Agilent Technologies, Yarnton, England.
  2. Altomare, A., Cascarano, G., Giacovazzo, C. & Guagliardi, A. (1993). J. Appl. Cryst. 26, 343–350.
  3. Fun, H.-K., Arshad, S., Garudachari, B., Isloor, A. M. & Shivananda, K. N. (2011). Acta Cryst. E67, o2836. [DOI] [PMC free article] [PubMed]
  4. Fun, H.-K., Loh, W.-S., Garudachari, B., Isloor, A. M. & Satyanarayan, M. N. (2011). Acta Cryst. E67, o1597. [DOI] [PMC free article] [PubMed]
  5. Fun, H.-K., Ooi, C. W., Garudachari, B., Isloor, A. M. & Satyanarayan, M. N. (2011). Acta Cryst. E67, o3119. [DOI] [PMC free article] [PubMed]
  6. Fun, H.-K., Shahani, T., Garudachari, B., Isloor, A. M. & Satyanarayan, M. N. (2011). Acta Cryst. E67, o3154. [DOI] [PMC free article] [PubMed]
  7. Macrae, C. F., Bruno, I. J., Chisholm, J. A., Edgington, P. R., McCabe, P., Pidcock, E., Rodriguez-Monge, L., Taylor, R., van de Streek, J. & Wood, P. A. (2008). J. Appl. Cryst. 41, 466–470.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812046995/ng5304sup1.cif

e-68-o3465-sup1.cif (21.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812046995/ng5304Isup2.hkl

e-68-o3465-Isup2.hkl (120.3KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812046995/ng5304Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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