organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

2-(4-Bromo­phen­yl)-2-oxo­ethyl 4-meth­­oxy­benzoate

aX-ray Crystallography Unit, School of Physics, Universiti Sains Malaysia, 11800 USM, Penang, Malaysia, bOrganic Chemistry Division, Department of Chemistry, National Institute of Technology-Karnataka, Surathkal, Mangalore 575 025, India, and cDepartment of Physics, National Institute of Technology-Karnataka, Surathkal, Mangalore 575 025, India
*Correspondence e-mail: hkfun@usm.my

(Received 16 May 2011; accepted 19 May 2011; online 25 May 2011)

In the title compound, C16H13BrO4, the benzene rings are almost perpendicular to each other, making a dihedral angle of 84.07 (8)°. In the crystal, the mol­ecules are linked into chains along the a axis via inter­molecular C—H⋯O hydrogen bonds. A C—H⋯π inter­action is also observed.

Related literature

For background to and applications of phenacyl benzoates, see: Gandhi et al. (1995[Gandhi, S. S., Bell, K. L. & Gibson, M. S. (1995). Tetrahedron, 51, 13301-13308.]); Huang et al. (1996[Huang, W., Pian, J., Chen, B., Pei, W. & Ye, X. (1996). Tetrahedron, 52, 10131-10136.]); Litera et al. (2006[Litera, J. K., Loya, A. D. & Klan, P. (2006). J. Org. Chem. 71, 713-723.]); Rather & Reid (1919[Rather, J. B. & Reid, E. (1919). J. Am. Chem. Soc. 41, 75-83.]); Ruzicka et al. (2002[Ruzicka, R., Zabadal, M. & Klan, P. (2002). Synth. Commun. 32, 2581-2590.]); Sheehan & Umezaw (1973[Sheehan, J. C. & Umezaw, K. (1973). J. Org. Chem. 58, 3771-3773.]). For the synthesis, see: Judefind & Reid (1920[Judefind, W. L. & Reid, E. E. (1920). J. Am. Chem. Soc. 42, 1043-1055.]). For bond-length data, see: Allen et al. (1987[Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1-19.]).

[Scheme 1]

Experimental

Crystal data
  • C16H13BrO4

  • Mr = 349.17

  • Triclinic, [P \overline 1]

  • a = 7.9700 (5) Å

  • b = 7.9852 (5) Å

  • c = 11.3185 (7) Å

  • α = 86.536 (1)°

  • β = 83.205 (1)°

  • γ = 89.633 (1)°

  • V = 713.97 (8) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 2.89 mm−1

  • T = 296 K

  • 0.58 × 0.34 × 0.32 mm

Data collection
  • Bruker SMART APEXII DUO CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2009[Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.286, Tmax = 0.461

  • 10671 measured reflections

  • 3270 independent reflections

  • 2767 reflections with I > 2σ(I)

  • Rint = 0.017

Refinement
  • R[F2 > 2σ(F2)] = 0.027

  • wR(F2) = 0.069

  • S = 1.05

  • 3270 reflections

  • 191 parameters

  • H-atom parameters constrained

  • Δρmax = 0.36 e Å−3

  • Δρmin = −0.52 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the C1–C6 ring.

D—H⋯A D—H H⋯A DA D—H⋯A
C2—H2A⋯O1i 0.93 2.48 3.386 (2) 164
C11—H11ACg1ii 0.93 2.81 3.6395 (18) 149
Symmetry codes: (i) x-1, y, z; (ii) -x+2, -y+1, -z+1.

Data collection: APEX2 (Bruker, 2009[Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2009[Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009[Spek, A. L. (2009). Acta Cryst. D65, 148-155.]).

Supporting information


Comment top

Phenacyl benzoates are very useful protecting groups which can be easily removed by non-chemical reactions. The advantage of photosensitive blocking groups is that they can be removed under completely neutral and mild conditions (Sheehan & Umezaw, 1973; Ruzicka et al., 2002; Litera et al., 2006) used for identification of organic acids (Rather & Reid, 1919), synthesis of oxazoles, imidazoles (Huang et al., 1996) and benzoxazepine (Gandhi et al., 1995). Keeping this in view, we hereby report the crystal structure of 2-(4-bromophenyl)-2-oxoethyl 4-methoxybenzoate of potential commercial importance.

In the title compound (Fig. 1), the C1–C6 benzene ring [maximum deviation of 0.005 (2) Å at atom C6] is almost perpendicular with the C10–C15 benzene ring [maximum deviation of 0.014 (2) Å at atom C13] with a dihedral angle of 84.07 (8)°. Bond lengths (Allen et al., 1987) and angles are within the normal ranges.

In the crystal packing (Fig. 2), the molecules are linked into chains along the a axis via intermolecular C2—H2A···O1 hydrogen bonds (Table 1). The crystal packing is further consolidated by C—H···π interactions, involving the centroids of C1–C6 phenyl ring.

Related literature top

For background to and applications of phenacyl benzoates, see: Gandhi et al. (1995); Huang et al. (1996); Litera et al. (2006); Rather & Reid (1919); Ruzicka et al. (2002); Sheehan & Umezaw (1973). For the synthesis, see: Judefind & Reid (1920). For bond-length data, see: Allen et al. (1987).

Experimental top

The mixture of 4-methoxy benzoic acid (1.0 g, 0.0065 mol) sodium carbonate (0.766 g, 0.0072 mol) and 2-bromo-1-(4-bromophenyl)ethanone (2.00 g, 0.0072 mol) in dimethyl formamide (10 ml) was stirred at room temperature for 2 h. On cooling, the separated colourless needle-shaped crystals of 2-(4-bromophenyl)-2-oxoethyl 4-methoxybenzoate were collected by filtration. Compound was recrystallized from ethanol. Yield: 2.1 g (91.70%), m.p.: 429–430 K (Judefind & Reid, 1920).

Refinement top

All the H atoms were positioned geometrically and refined with a riding model with Uiso(H) = 1.2 or 1.5Ueq(C) (C—H = 0.93 or 0.96 Å). A rotating group model was applied to the methyl groups.

Computing details top

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound, showing 30% probability displacement ellipsoids and the atom-numbering scheme.
[Figure 2] Fig. 2. The crystal packing of the title compound, viewed along the c axis. H atoms not involved in the intermolecular interactions (dashed lines) have been omitted for clarity.
2-(4-Bromophenyl)-2-oxoethyl 4-methoxybenzoate top
Crystal data top
C16H13BrO4Z = 2
Mr = 349.17F(000) = 352
Triclinic, P1Dx = 1.624 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.9700 (5) ÅCell parameters from 4684 reflections
b = 7.9852 (5) Åθ = 3.0–30.0°
c = 11.3185 (7) ŵ = 2.89 mm1
α = 86.536 (1)°T = 296 K
β = 83.205 (1)°Block, colourless
γ = 89.633 (1)°0.58 × 0.34 × 0.32 mm
V = 713.97 (8) Å3
Data collection top
Bruker SMART APEXII DUO CCD area-detector
diffractometer
3270 independent reflections
Radiation source: fine-focus sealed tube2767 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.017
ϕ and ω scansθmax = 27.5°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Bruker, 2009)
h = 1010
Tmin = 0.286, Tmax = 0.461k = 1010
10671 measured reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.027Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.069H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0314P)2 + 0.2047P]
where P = (Fo2 + 2Fc2)/3
3270 reflections(Δ/σ)max = 0.001
191 parametersΔρmax = 0.36 e Å3
0 restraintsΔρmin = 0.52 e Å3
Crystal data top
C16H13BrO4γ = 89.633 (1)°
Mr = 349.17V = 713.97 (8) Å3
Triclinic, P1Z = 2
a = 7.9700 (5) ÅMo Kα radiation
b = 7.9852 (5) ŵ = 2.89 mm1
c = 11.3185 (7) ÅT = 296 K
α = 86.536 (1)°0.58 × 0.34 × 0.32 mm
β = 83.205 (1)°
Data collection top
Bruker SMART APEXII DUO CCD area-detector
diffractometer
3270 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2009)
2767 reflections with I > 2σ(I)
Tmin = 0.286, Tmax = 0.461Rint = 0.017
10671 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0270 restraints
wR(F2) = 0.069H-atom parameters constrained
S = 1.05Δρmax = 0.36 e Å3
3270 reflectionsΔρmin = 0.52 e Å3
191 parameters
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
Br10.26530 (3)0.93852 (3)0.738521 (19)0.06416 (9)
O11.05611 (17)0.7434 (2)0.48016 (14)0.0727 (4)
O21.07533 (16)0.58534 (16)0.28028 (12)0.0543 (3)
O31.07066 (18)0.84361 (18)0.19107 (14)0.0628 (4)
O41.82176 (17)0.60709 (18)0.03308 (13)0.0589 (3)
C10.6023 (2)0.7176 (2)0.48878 (16)0.0451 (4)
H1A0.59620.65220.42420.054*
C20.4543 (2)0.7690 (2)0.55394 (16)0.0471 (4)
H2A0.34950.73820.53370.057*
C30.4655 (2)0.8663 (2)0.64896 (16)0.0458 (4)
C40.6205 (3)0.9145 (2)0.67953 (17)0.0521 (4)
H4A0.62610.98160.74330.062*
C50.7661 (2)0.8622 (2)0.61464 (17)0.0502 (4)
H5A0.87050.89390.63510.060*
C60.7594 (2)0.7624 (2)0.51864 (15)0.0426 (4)
C70.9203 (2)0.7110 (2)0.44998 (17)0.0483 (4)
C80.9105 (2)0.6156 (3)0.33964 (18)0.0517 (4)
H8A0.85350.50940.36180.062*
H8B0.84490.67960.28580.062*
C91.1450 (2)0.7150 (2)0.21027 (16)0.0462 (4)
C101.3205 (2)0.6803 (2)0.16089 (15)0.0413 (4)
C111.4168 (2)0.5522 (2)0.20810 (16)0.0443 (4)
H11A1.36860.48080.27080.053*
C121.5823 (2)0.5308 (2)0.16269 (17)0.0464 (4)
H12A1.64530.44470.19460.056*
C131.6566 (2)0.6365 (2)0.06941 (16)0.0439 (4)
C141.5604 (2)0.7614 (2)0.01947 (16)0.0492 (4)
H14A1.60770.83050.04480.059*
C151.3943 (2)0.7820 (2)0.06586 (16)0.0487 (4)
H15A1.33040.86630.03250.058*
C161.9073 (3)0.7168 (3)0.0585 (2)0.0675 (6)
H16A2.02380.68430.07270.101*
H16B1.90030.82990.03410.101*
H16C1.85540.71000.13040.101*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.06137 (14)0.06633 (15)0.05890 (14)0.01421 (10)0.01096 (9)0.00724 (9)
O10.0370 (7)0.1133 (13)0.0702 (10)0.0055 (8)0.0113 (7)0.0132 (9)
O20.0440 (7)0.0500 (7)0.0654 (8)0.0035 (5)0.0050 (6)0.0008 (6)
O30.0581 (8)0.0542 (8)0.0725 (9)0.0160 (6)0.0025 (7)0.0021 (7)
O40.0462 (7)0.0601 (8)0.0664 (9)0.0025 (6)0.0045 (6)0.0077 (7)
C10.0393 (8)0.0515 (10)0.0449 (9)0.0038 (7)0.0073 (7)0.0007 (7)
C20.0381 (8)0.0516 (10)0.0510 (10)0.0043 (7)0.0067 (7)0.0056 (8)
C30.0470 (9)0.0429 (9)0.0442 (9)0.0036 (7)0.0014 (7)0.0103 (7)
C40.0621 (11)0.0497 (10)0.0441 (10)0.0045 (8)0.0064 (8)0.0000 (8)
C50.0470 (9)0.0553 (11)0.0489 (10)0.0104 (8)0.0114 (8)0.0032 (8)
C60.0388 (8)0.0468 (9)0.0416 (9)0.0048 (7)0.0064 (7)0.0069 (7)
C70.0370 (8)0.0565 (11)0.0505 (10)0.0035 (7)0.0067 (7)0.0072 (8)
C80.0383 (9)0.0569 (11)0.0586 (11)0.0000 (8)0.0005 (8)0.0037 (9)
C90.0481 (9)0.0445 (9)0.0462 (9)0.0032 (7)0.0050 (7)0.0057 (7)
C100.0448 (9)0.0388 (8)0.0408 (9)0.0015 (7)0.0050 (7)0.0058 (7)
C110.0463 (9)0.0410 (9)0.0448 (9)0.0028 (7)0.0049 (7)0.0036 (7)
C120.0464 (9)0.0416 (9)0.0510 (10)0.0008 (7)0.0091 (8)0.0047 (7)
C130.0445 (9)0.0430 (9)0.0439 (9)0.0021 (7)0.0025 (7)0.0056 (7)
C140.0572 (11)0.0451 (10)0.0429 (9)0.0013 (8)0.0012 (8)0.0030 (7)
C150.0563 (10)0.0422 (9)0.0465 (9)0.0076 (8)0.0039 (8)0.0018 (7)
C160.0556 (12)0.0722 (14)0.0686 (14)0.0042 (10)0.0125 (10)0.0063 (11)
Geometric parameters (Å, º) top
Br1—C31.8925 (18)C7—C81.511 (3)
O1—C71.207 (2)C8—H8A0.9700
O2—C91.346 (2)C8—H8B0.9700
O2—C81.429 (2)C9—C101.475 (2)
O3—C91.203 (2)C10—C151.384 (3)
O4—C131.356 (2)C10—C111.394 (2)
O4—C161.428 (2)C11—C121.371 (2)
C1—C21.389 (2)C11—H11A0.9300
C1—C61.389 (2)C12—C131.389 (2)
C1—H1A0.9300C12—H12A0.9300
C2—C31.376 (3)C13—C141.387 (3)
C2—H2A0.9300C14—C151.378 (3)
C3—C41.385 (3)C14—H14A0.9300
C4—C51.374 (3)C15—H15A0.9300
C4—H4A0.9300C16—H16A0.9600
C5—C61.392 (3)C16—H16B0.9600
C5—H5A0.9300C16—H16C0.9600
C6—C71.488 (2)
C9—O2—C8115.26 (14)H8A—C8—H8B108.0
C13—O4—C16118.49 (15)O3—C9—O2123.12 (17)
C2—C1—C6121.02 (17)O3—C9—C10124.67 (17)
C2—C1—H1A119.5O2—C9—C10112.21 (14)
C6—C1—H1A119.5C15—C10—C11118.55 (16)
C3—C2—C1118.78 (16)C15—C10—C9118.67 (15)
C3—C2—H2A120.6C11—C10—C9122.75 (16)
C1—C2—H2A120.6C12—C11—C10120.37 (16)
C2—C3—C4121.30 (17)C12—C11—H11A119.8
C2—C3—Br1119.48 (14)C10—C11—H11A119.8
C4—C3—Br1119.22 (14)C11—C12—C13120.61 (16)
C5—C4—C3119.33 (18)C11—C12—H12A119.7
C5—C4—H4A120.3C13—C12—H12A119.7
C3—C4—H4A120.3O4—C13—C14124.61 (16)
C4—C5—C6120.87 (17)O4—C13—C12115.91 (16)
C4—C5—H5A119.6C14—C13—C12119.48 (16)
C6—C5—H5A119.6C15—C14—C13119.44 (17)
C1—C6—C5118.69 (17)C15—C14—H14A120.3
C1—C6—C7122.38 (16)C13—C14—H14A120.3
C5—C6—C7118.91 (16)C14—C15—C10121.49 (17)
O1—C7—C6121.84 (18)C14—C15—H15A119.3
O1—C7—C8119.99 (17)C10—C15—H15A119.3
C6—C7—C8118.17 (15)O4—C16—H16A109.5
O2—C8—C7111.04 (15)O4—C16—H16B109.5
O2—C8—H8A109.4H16A—C16—H16B109.5
C7—C8—H8A109.4O4—C16—H16C109.5
O2—C8—H8B109.4H16A—C16—H16C109.5
C7—C8—H8B109.4H16B—C16—H16C109.5
C6—C1—C2—C30.3 (3)C8—O2—C9—C10174.72 (15)
C1—C2—C3—C40.6 (3)O3—C9—C10—C1515.5 (3)
C1—C2—C3—Br1179.71 (13)O2—C9—C10—C15164.40 (16)
C2—C3—C4—C50.9 (3)O3—C9—C10—C11162.56 (18)
Br1—C3—C4—C5179.99 (14)O2—C9—C10—C1117.5 (2)
C3—C4—C5—C60.3 (3)C15—C10—C11—C121.5 (3)
C2—C1—C6—C50.8 (3)C9—C10—C11—C12176.60 (17)
C2—C1—C6—C7179.34 (17)C10—C11—C12—C130.2 (3)
C4—C5—C6—C10.5 (3)C16—O4—C13—C143.6 (3)
C4—C5—C6—C7179.10 (17)C16—O4—C13—C12176.97 (18)
C1—C6—C7—O1176.21 (19)C11—C12—C13—O4178.46 (17)
C5—C6—C7—O15.3 (3)C11—C12—C13—C142.1 (3)
C1—C6—C7—C83.8 (3)O4—C13—C14—C15178.44 (17)
C5—C6—C7—C8174.72 (17)C12—C13—C14—C152.2 (3)
C9—O2—C8—C780.8 (2)C13—C14—C15—C100.4 (3)
O1—C7—C8—O23.7 (3)C11—C10—C15—C141.4 (3)
C6—C7—C8—O2176.31 (15)C9—C10—C15—C14176.76 (17)
C8—O2—C9—O35.3 (3)
Hydrogen-bond geometry (Å, º) top
Cg1 is the centroid of the C1–C6 ring.
D—H···AD—HH···AD···AD—H···A
C2—H2A···O1i0.932.483.386 (2)164
C11—H11A···Cg1ii0.932.813.6395 (18)149
Symmetry codes: (i) x1, y, z; (ii) x+2, y+1, z+1.

Experimental details

Crystal data
Chemical formulaC16H13BrO4
Mr349.17
Crystal system, space groupTriclinic, P1
Temperature (K)296
a, b, c (Å)7.9700 (5), 7.9852 (5), 11.3185 (7)
α, β, γ (°)86.536 (1), 83.205 (1), 89.633 (1)
V3)713.97 (8)
Z2
Radiation typeMo Kα
µ (mm1)2.89
Crystal size (mm)0.58 × 0.34 × 0.32
Data collection
DiffractometerBruker SMART APEXII DUO CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2009)
Tmin, Tmax0.286, 0.461
No. of measured, independent and
observed [I > 2σ(I)] reflections
10671, 3270, 2767
Rint0.017
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.027, 0.069, 1.05
No. of reflections3270
No. of parameters191
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.36, 0.52

Computer programs: APEX2 (Bruker, 2009), SAINT (Bruker, 2009), SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).

Hydrogen-bond geometry (Å, º) top
Cg1 is the centroid of the C1–C6 ring.
D—H···AD—HH···AD···AD—H···A
C2—H2A···O1i0.932.483.386 (2)164
C11—H11A···Cg1ii0.932.813.6395 (18)149
Symmetry codes: (i) x1, y, z; (ii) x+2, y+1, z+1.
 

Footnotes

Thomson Reuters ResearcherID: A-3561-2009.

§Thomson Reuters ResearcherID: C-7581-2009.

Acknowledgements

HKF and WSL thank Universiti Sains Malaysia (USM) for the Research University Grant (1001/PFIZIK/811160). WSL also thanks the Malaysian Government and USM for the award of a Research Fellowship. AMI is thankful to the Department of Atomic Energy, Board for Research in Nuclear Sciences, Government of India for a `Young scientist' award. GB thanks the Department of Information Technology, New Delhi, India, for financial support.

References

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