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 ▶).
Experimental
Crystal data
C16H13BrO3
M r = 333.17
Triclinic,
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
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812046995/ng5304Isup2.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 | 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)
; (ii)
.
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.

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.
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 m−3 |
| 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 mm−1 |
| 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 Å−3 |
| 0 restraints | Δρmin = −0.42 e Å−3 |
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
- Agilent (2010). CrysAlis PRO Agilent Technologies, Yarnton, England.
- Altomare, A., Cascarano, G., Giacovazzo, C. & Guagliardi, A. (1993). J. Appl. Cryst. 26, 343–350.
- Fun, H.-K., Arshad, S., Garudachari, B., Isloor, A. M. & Shivananda, K. N. (2011). Acta Cryst. E67, o2836. [DOI] [PMC free article] [PubMed]
- Fun, H.-K., Loh, W.-S., Garudachari, B., Isloor, A. M. & Satyanarayan, M. N. (2011). Acta Cryst. E67, o1597. [DOI] [PMC free article] [PubMed]
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- Fun, H.-K., Shahani, T., Garudachari, B., Isloor, A. M. & Satyanarayan, M. N. (2011). Acta Cryst. E67, o3154. [DOI] [PMC free article] [PubMed]
- 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.
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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
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812046995/ng5304Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812046995/ng5304Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

