Literature DB >> 21202158

4-Bromo-phenyl benzoate.

B Thimme Gowda, Sabine Foro, K S Babitha, Hartmut Fuess.   

Abstract

The structure of the title compound (4BPBA), C(13)H(9)BrO(2), is similar to that of phenyl benzoate (PBA), 4-methyl-phenyl benzoate (4MePBA) and 4-methoxy-phenyl benzoate, with somewhat different bond parameters. The dihedral angle between the phenyl and benzoyl rings in 4BPBA is 58.43 (17)°, compared with values of 55.7° in PBA and 60.17 (7)° in 4MPBA. The mol-ecules in the title compound are packed into infinite chains in the a-axis direction.

Entities:  

Year:  2008        PMID: 21202158      PMCID: PMC2960956          DOI: 10.1107/S1600536808008167

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For related literature, see: Adams & Morsi (1976 ▶); Gowda, Foro, Babitha & Fuess (2007 ▶); Gowda, Foro, Nayak & Fuess (2007 ▶); Nayak & Gowda (2008 ▶).

Experimental

Crystal data

C13H9BrO2 M = 277.11 Orthorhombic, a = 7.748 (1) Å b = 5.5946 (7) Å c = 26.814 (5) Å V = 1162.3 (3) Å3 Z = 4 Cu Kα radiation μ = 4.67 mm−1 T = 299 (2) K 0.38 × 0.30 × 0.08 mm

Data collection

Enraf–Nonius CAD-4 diffractometer Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.241, T max = 0.685 1986 measured reflections 1442 independent reflections 1252 reflections with I > 2σ(I) R int = 0.039 3 standard reflections frequency: 120 min intensity decay: 2.0%

Refinement

R[F 2 > 2σ(F 2)] = 0.059 wR(F 2) = 0.189 S = 1.15 1442 reflections 145 parameters 1 restraint H-atom parameters constrained Δρmax = 1.04 e Å−3 Δρmin = −1.32 e Å−3 Absolute structure: Flack (1983 ▶), with 375 Friedel pairs Flack parameter: −0.04 (6) Data collection: CAD-4-PC Software (Enraf–Nonius, 1996 ▶); cell refinement: CAD-4-PC Software; data reduction: REDU4 (Stoe & Cie, 1987 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2003 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808008167/om2221sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808008167/om2221Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C13H9BrO2F000 = 552
Mr = 277.11Dx = 1.584 Mg m3
Orthorhombic, Pca21Cu Kα radiation λ = 1.54180 Å
Hall symbol: P 2c -2acCell parameters from 25 reflections
a = 7.748 (1) Åθ = 9.9–23.4º
b = 5.5946 (7) ŵ = 4.67 mm1
c = 26.814 (5) ÅT = 299 (2) K
V = 1162.3 (3) Å3Plate, colourless
Z = 40.38 × 0.30 × 0.08 mm
Enraf–Nonius CAD-4 diffractometerRint = 0.039
Radiation source: fine-focus sealed tubeθmax = 66.9º
Monochromator: graphiteθmin = 3.3º
T = 299(2) Kh = −1→9
ω/2θ scansk = −1→6
Absorption correction: ψ scan(North et al., 1968)l = −8→32
Tmin = 0.242, Tmax = 0.6853 standard reflections
1986 measured reflections every 120 min
1442 independent reflections intensity decay: 2.0%
1252 reflections with I > 2σ(I)
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.059  w = 1/[σ2(Fo2) + (0.1268P)2 + 0.565P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.189(Δ/σ)max = 0.001
S = 1.15Δρmax = 1.04 e Å3
1442 reflectionsΔρmin = −1.32 e Å3
145 parametersExtinction correction: none
1 restraintAbsolute structure: Flack (1983), with 375 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: −0.04 (6)
Secondary atom site location: difference Fourier map
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.
xyzUiso*/Ueq
Br10.29159 (16)0.2659 (2)−0.12742 (8)0.0950 (5)
O10.4692 (6)0.1882 (9)0.0901 (2)0.0581 (13)
O20.3231 (11)0.5195 (14)0.1104 (3)0.107 (3)
C10.4260 (8)0.2190 (10)0.0403 (3)0.0463 (14)
C20.4854 (8)0.4121 (12)0.0127 (3)0.0544 (16)
H20.55000.53210.02780.065*
C30.4478 (8)0.4229 (12)−0.0367 (3)0.0560 (17)
H30.48880.5492−0.05590.067*
C40.3474 (11)0.2440 (12)−0.0586 (3)0.0559 (17)
C50.2920 (9)0.0437 (12)−0.0313 (3)0.0589 (18)
H50.2301−0.0794−0.04620.071*
C60.3332 (9)0.0389 (13)0.0176 (3)0.0583 (17)
H60.2977−0.09080.03680.070*
C70.4106 (9)0.3510 (14)0.1226 (3)0.0577 (17)
C80.4601 (9)0.2976 (12)0.1748 (3)0.0521 (15)
C90.5527 (8)0.0900 (13)0.1879 (3)0.0585 (17)
H90.5846−0.02090.16380.070*
C100.5943 (10)0.0558 (13)0.2368 (4)0.0644 (19)
H100.6544−0.08200.24540.077*
C110.5530 (10)0.2107 (14)0.2731 (4)0.0627 (19)
H110.58340.18030.30600.075*
C120.4636 (9)0.4180 (14)0.2604 (3)0.0602 (17)
H120.43530.52840.28510.072*
C130.4164 (9)0.4607 (13)0.2112 (3)0.0585 (16)
H130.35580.59850.20290.070*
U11U22U33U12U13U23
Br10.1056 (8)0.1322 (9)0.0472 (6)0.0167 (6)−0.0058 (7)−0.0056 (7)
O10.053 (2)0.064 (3)0.058 (3)0.008 (2)−0.003 (2)−0.011 (3)
O20.145 (6)0.117 (5)0.059 (4)0.089 (5)0.005 (4)0.001 (4)
C10.044 (3)0.047 (3)0.049 (4)0.003 (2)−0.001 (3)−0.003 (3)
C20.046 (3)0.052 (3)0.066 (5)−0.007 (3)0.004 (3)−0.009 (3)
C30.055 (3)0.052 (3)0.061 (5)0.007 (3)0.011 (3)0.005 (3)
C40.058 (4)0.067 (4)0.042 (4)0.006 (3)0.005 (4)−0.006 (3)
C50.062 (4)0.049 (3)0.066 (5)−0.004 (3)−0.005 (4)−0.006 (3)
C60.054 (3)0.058 (4)0.063 (5)−0.012 (3)0.002 (4)0.010 (4)
C70.050 (3)0.068 (4)0.055 (4)0.019 (3)0.004 (3)0.002 (4)
C80.051 (3)0.055 (3)0.050 (4)−0.005 (3)0.006 (3)−0.001 (3)
C90.053 (3)0.062 (3)0.061 (4)0.017 (3)−0.004 (3)−0.010 (4)
C100.057 (3)0.062 (4)0.074 (5)0.007 (3)−0.008 (4)0.015 (4)
C110.056 (3)0.082 (5)0.050 (5)−0.001 (3)−0.002 (3)0.003 (4)
C120.064 (4)0.065 (4)0.052 (4)−0.007 (3)0.005 (4)−0.002 (4)
C130.056 (3)0.059 (4)0.060 (4)0.010 (3)−0.003 (3)0.001 (3)
Br1—C41.899 (9)C6—H60.9300
O1—C71.340 (10)C7—C81.481 (12)
O1—C11.388 (10)C8—C131.379 (11)
O2—C71.206 (9)C8—C91.410 (10)
C1—C61.379 (10)C9—C101.364 (12)
C1—C21.388 (10)C9—H90.9300
C2—C31.356 (12)C10—C111.342 (12)
C2—H20.9300C10—H100.9300
C3—C41.398 (11)C11—C121.392 (11)
C3—H30.9300C11—H110.9300
C4—C51.406 (11)C12—C131.390 (12)
C5—C61.351 (12)C12—H120.9300
C5—H50.9300C13—H130.9300
C7—O1—C1117.4 (5)O2—C7—C8124.1 (7)
C6—C1—C2120.4 (8)O1—C7—C8112.9 (6)
C6—C1—O1117.3 (6)C13—C8—C9119.5 (8)
C2—C1—O1122.0 (6)C13—C8—C7118.2 (6)
C3—C2—C1118.9 (6)C9—C8—C7122.2 (7)
C3—C2—H2120.5C10—C9—C8118.4 (7)
C1—C2—H2120.5C10—C9—H9120.8
C2—C3—C4119.9 (7)C8—C9—H9120.8
C2—C3—H3120.1C11—C10—C9123.4 (7)
C4—C3—H3120.1C11—C10—H10118.3
C3—C4—C5121.4 (8)C9—C10—H10118.3
C3—C4—Br1119.3 (6)C10—C11—C12118.7 (8)
C5—C4—Br1119.2 (6)C10—C11—H11120.7
C6—C5—C4116.7 (7)C12—C11—H11120.7
C6—C5—H5121.6C13—C12—C11120.4 (8)
C4—C5—H5121.6C13—C12—H12119.8
C5—C6—C1122.4 (7)C11—C12—H12119.8
C5—C6—H6118.8C8—C13—C12119.6 (7)
C1—C6—H6118.8C8—C13—H13120.2
O2—C7—O1123.0 (8)C12—C13—H13120.2
C7—O1—C1—C6−120.1 (7)C1—O1—C7—C8178.5 (6)
C7—O1—C1—C265.4 (9)O2—C7—C8—C13−5.8 (12)
C6—C1—C2—C31.3 (10)O1—C7—C8—C13175.9 (6)
O1—C1—C2—C3175.6 (6)O2—C7—C8—C9175.6 (9)
C1—C2—C3—C41.4 (10)O1—C7—C8—C9−2.7 (10)
C2—C3—C4—C5−3.8 (10)C13—C8—C9—C100.9 (10)
C2—C3—C4—Br1178.5 (5)C7—C8—C9—C10179.5 (7)
C3—C4—C5—C63.2 (10)C8—C9—C10—C11−0.6 (12)
Br1—C4—C5—C6−179.1 (6)C9—C10—C11—C12−0.3 (12)
C4—C5—C6—C1−0.5 (11)C10—C11—C12—C130.9 (11)
C2—C1—C6—C5−1.8 (11)C9—C8—C13—C12−0.3 (11)
O1—C1—C6—C5−176.4 (7)C7—C8—C13—C12−178.9 (7)
C1—O1—C7—O20.2 (12)C11—C12—C13—C8−0.6 (11)
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