Abstract
In the title molecule, C20H16O2, the dihedral angle between the phenyl rings of the diphenylmethyl group is 68.3 (2)°. The benzoate group is essentially planar, with a maximum deviation of 0.017 (2) Å for the carbonyl O atom, and the two phenyl rings are twisted by 27.5 (4) and 85.6 (9)° from this plane. In the crystal, weak C—H⋯O hydrogen bonds link molecules along [100].
Related literature
For related structures, see: Baidya et al. (2009a
▶,b
▶); Gowda et al. (2007 ▶, 2009 ▶). For standard bond lengths, see: Allen et al. (1987 ▶).
Experimental
Crystal data
C20H16O2
M r = 288.33
Monoclinic,
a = 5.75357 (19) Å
b = 16.0368 (5) Å
c = 8.3114 (3) Å
β = 95.340 (3)°
V = 763.55 (4) Å3
Z = 2
Cu Kα radiation
μ = 0.63 mm−1
T = 173 K
0.38 × 0.26 × 0.24 mm
Data collection
Agilent Xcalibur (Eos, Gemini) diffractometer
Absorption correction: multi-scan (CrysAlis PRO and CrysAlis RED; Agilent, 2012 ▶) T min = 0.912, T max = 1.000
4414 measured reflections
2659 independent reflections
2528 reflections with I > 2σ(I)
R int = 0.022
Refinement
R[F 2 > 2σ(F 2)] = 0.035
wR(F 2) = 0.094
S = 1.06
2659 reflections
200 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.21 e Å−3
Δρmin = −0.15 e Å−3
Absolute structure: Flack (1983 ▶) 1120 Friedel pairs
Flack parameter: 0.0 (2)
Data collection: CrysAlis PRO (Agilent, 2012 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis RED (Agilent, 2012 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812050064/lh5566sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812050064/lh5566Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812050064/lh5566Isup3.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 |
|---|---|---|---|---|
| C16—H16⋯O2i | 0.93 | 2.44 | 3.334 (2) | 160 |
Symmetry code: (i)
.
Acknowledgments
MK thanks the UOM for research facilities. JPJ acknowledges the NSF–MRI program (grant No. CHE-1039027) for funds to purchase the X-ray diffractometer.
supplementary crystallographic information
Comment
Benzyl Benzoate is widely used in the perfume and pharmaceutical industries. The crystal structures of some related compounds, viz., 4,4'-bis(dimethylamino)benzhydryl phenyl sulfone (Baidya et al., 2009a), benzhydryl phenyl sulfone (Baidya et al., 2009b), 4-methylphenyl benzoate (Gowda et al., 2007), 2,4-dimethylphenyl 4-methylbenzoate (Gowda et al., 2009) have been reported. In view of the importance of benzoates, the paper reports the crystal structure of the title compound, (I).
The molecular structure of the title compound is shown in Fig. 1. The dihedral angle between the two phenyl rings (C9-C14 and C15-C20) is 68.3 (2)°. The mean plane of the benzoate group (C1–C7/O1/O2, with a maximum deviation of 0.017 (2)Å for O2) is twisted by 27.5 (4)° (C9–C14) and 85.6 (9)° (C15–C20), respectively, from that of the phenyl rings. In the crystal, weak C—H···O hydrogen bonds (Table 1) link molecules along [100] (Fig. 2).
Experimental
The title compound was obtained as a gift sample from R. L. Fine Chem, Bengaluru, India. X-ray quality crystals were obtained by slow evaporation of acetone and acetone solution (m.p.: 353–355 K).
Refinement
All of the H atoms were placed in their calculated positions and then refined using the riding model with Atom—H lengths of 0.93Å (CH). Isotropic displacement parameters for these atoms were set to 1.19-1.20 (CH) times Ueq of the parent atom.
Figures
Fig. 1.
Molecular structure of the title compound showing 50% probability displacement ellipsoids.
Fig. 2.
Packing diagram of the title compound viewed along the c axis showing weak C—H···O intermolecular interactions (dashed lines) linking the molecules into columns along [100]
Crystal data
| C20H16O2 | F(000) = 304 |
| Mr = 288.33 | Dx = 1.254 Mg m−3 |
| Monoclinic, P21 | Cu Kα radiation, λ = 1.54184 Å |
| Hall symbol: P 2yb | Cell parameters from 2446 reflections |
| a = 5.75357 (19) Å | θ = 5.3–72.4° |
| b = 16.0368 (5) Å | µ = 0.63 mm−1 |
| c = 8.3114 (3) Å | T = 173 K |
| β = 95.340 (3)° | Block, colorless |
| V = 763.55 (4) Å3 | 0.38 × 0.26 × 0.24 mm |
| Z = 2 |
Data collection
| Agilent Xcalibur (Eos, Gemini) diffractometer | 2659 independent reflections |
| Radiation source: Enhance (Cu) X-ray Source | 2528 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.022 |
| Detector resolution: 16.0416 pixels mm-1 | θmax = 72.5°, θmin = 5.4° |
| ω scans | h = −7→5 |
| Absorption correction: multi-scan (CrysAlis PRO and CrysAlis RED; Agilent, 2012) | k = −17→19 |
| Tmin = 0.912, Tmax = 1.000 | l = −6→10 |
| 4414 measured reflections |
Refinement
| Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
| Least-squares matrix: full | H-atom parameters constrained |
| R[F2 > 2σ(F2)] = 0.035 | w = 1/[σ2(Fo2) + (0.0518P)2 + 0.052P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.094 | (Δ/σ)max < 0.001 |
| S = 1.06 | Δρmax = 0.21 e Å−3 |
| 2659 reflections | Δρmin = −0.15 e Å−3 |
| 200 parameters | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| 1 restraint | Extinction coefficient: 0.0104 (11) |
| Primary atom site location: structure-invariant direct methods | Absolute structure: Flack (1983) 1120 Friedel pairs |
| Secondary atom site location: difference Fourier map | Flack parameter: 0.0 (2) |
Special details
| Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 | ||
| O1 | 0.2173 (2) | 0.33454 (8) | 0.50213 (15) | 0.0376 (3) | |
| O2 | −0.1042 (2) | 0.31628 (10) | 0.63104 (18) | 0.0495 (4) | |
| C1 | 0.1598 (3) | 0.42599 (10) | 0.7144 (2) | 0.0312 (4) | |
| C2 | 0.3646 (3) | 0.46769 (11) | 0.6891 (2) | 0.0364 (4) | |
| H2 | 0.4547 | 0.4498 | 0.6085 | 0.044* | |
| C3 | 0.4349 (4) | 0.53567 (12) | 0.7833 (2) | 0.0434 (4) | |
| H3 | 0.5709 | 0.5640 | 0.7648 | 0.052* | |
| C4 | 0.3036 (4) | 0.56172 (13) | 0.9049 (2) | 0.0465 (5) | |
| H4 | 0.3514 | 0.6074 | 0.9685 | 0.056* | |
| C5 | 0.1008 (4) | 0.51969 (13) | 0.9320 (2) | 0.0491 (5) | |
| H5 | 0.0133 | 0.5370 | 1.0145 | 0.059* | |
| C6 | 0.0279 (3) | 0.45254 (12) | 0.8375 (2) | 0.0407 (4) | |
| H6 | −0.1092 | 0.4248 | 0.8556 | 0.049* | |
| C7 | 0.0735 (3) | 0.35370 (11) | 0.6150 (2) | 0.0329 (4) | |
| C8 | 0.1615 (3) | 0.26034 (11) | 0.4044 (2) | 0.0339 (4) | |
| H8 | −0.0074 | 0.2579 | 0.3758 | 0.041* | |
| C9 | 0.2833 (3) | 0.27104 (10) | 0.2523 (2) | 0.0350 (4) | |
| C10 | 0.4936 (3) | 0.31388 (13) | 0.2513 (2) | 0.0408 (4) | |
| H10 | 0.5615 | 0.3381 | 0.3459 | 0.049* | |
| C11 | 0.6021 (4) | 0.32051 (14) | 0.1099 (3) | 0.0459 (5) | |
| H11 | 0.7420 | 0.3495 | 0.1101 | 0.055* | |
| C12 | 0.5040 (4) | 0.28435 (12) | −0.0315 (2) | 0.0452 (5) | |
| H12 | 0.5776 | 0.2890 | −0.1261 | 0.054* | |
| C13 | 0.2964 (4) | 0.24132 (14) | −0.0317 (2) | 0.0459 (5) | |
| H13 | 0.2304 | 0.2166 | −0.1264 | 0.055* | |
| C14 | 0.1859 (3) | 0.23482 (12) | 0.1092 (2) | 0.0400 (4) | |
| H14 | 0.0455 | 0.2060 | 0.1081 | 0.048* | |
| C15 | 0.2380 (3) | 0.18357 (11) | 0.50053 (19) | 0.0327 (4) | |
| C16 | 0.4629 (3) | 0.17795 (12) | 0.5773 (2) | 0.0381 (4) | |
| H16 | 0.5683 | 0.2212 | 0.5672 | 0.046* | |
| C17 | 0.5304 (4) | 0.10861 (14) | 0.6684 (2) | 0.0456 (5) | |
| H17 | 0.6804 | 0.1056 | 0.7204 | 0.055* | |
| C18 | 0.3756 (4) | 0.04356 (13) | 0.6827 (2) | 0.0494 (5) | |
| H18 | 0.4206 | −0.0028 | 0.7452 | 0.059* | |
| C19 | 0.1538 (4) | 0.04782 (13) | 0.6037 (3) | 0.0514 (5) | |
| H19 | 0.0504 | 0.0038 | 0.6115 | 0.062* | |
| C20 | 0.0851 (4) | 0.11732 (13) | 0.5130 (2) | 0.0421 (4) | |
| H20 | −0.0644 | 0.1197 | 0.4601 | 0.051* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0385 (7) | 0.0341 (7) | 0.0422 (7) | −0.0057 (5) | 0.0136 (5) | −0.0087 (5) |
| O2 | 0.0401 (7) | 0.0565 (9) | 0.0543 (8) | −0.0152 (6) | 0.0172 (6) | −0.0205 (7) |
| C1 | 0.0333 (8) | 0.0287 (8) | 0.0316 (8) | 0.0040 (6) | 0.0032 (6) | 0.0031 (6) |
| C2 | 0.0354 (9) | 0.0348 (9) | 0.0396 (9) | −0.0008 (7) | 0.0058 (7) | 0.0002 (7) |
| C3 | 0.0415 (10) | 0.0386 (10) | 0.0494 (11) | −0.0062 (8) | 0.0002 (8) | 0.0021 (9) |
| C4 | 0.0569 (12) | 0.0358 (10) | 0.0451 (10) | −0.0034 (9) | −0.0047 (9) | −0.0076 (8) |
| C5 | 0.0602 (13) | 0.0475 (12) | 0.0410 (11) | 0.0031 (10) | 0.0129 (9) | −0.0103 (9) |
| C6 | 0.0410 (10) | 0.0402 (10) | 0.0419 (10) | −0.0016 (8) | 0.0082 (8) | −0.0030 (8) |
| C7 | 0.0318 (8) | 0.0333 (9) | 0.0340 (8) | 0.0016 (7) | 0.0047 (7) | −0.0001 (7) |
| C8 | 0.0327 (8) | 0.0345 (9) | 0.0349 (8) | −0.0039 (7) | 0.0050 (7) | −0.0062 (7) |
| C9 | 0.0395 (9) | 0.0303 (9) | 0.0354 (8) | 0.0045 (7) | 0.0056 (7) | 0.0010 (7) |
| C10 | 0.0428 (10) | 0.0413 (10) | 0.0393 (9) | −0.0018 (8) | 0.0088 (8) | −0.0016 (8) |
| C11 | 0.0495 (11) | 0.0415 (11) | 0.0487 (10) | 0.0004 (9) | 0.0152 (8) | 0.0058 (9) |
| C12 | 0.0589 (12) | 0.0427 (11) | 0.0363 (9) | 0.0099 (9) | 0.0172 (9) | 0.0070 (8) |
| C13 | 0.0609 (12) | 0.0443 (11) | 0.0324 (9) | 0.0086 (9) | 0.0032 (8) | −0.0021 (8) |
| C14 | 0.0420 (9) | 0.0379 (10) | 0.0401 (9) | 0.0039 (8) | 0.0035 (8) | −0.0035 (8) |
| C15 | 0.0374 (9) | 0.0340 (9) | 0.0282 (8) | −0.0040 (7) | 0.0108 (7) | −0.0075 (6) |
| C16 | 0.0391 (10) | 0.0423 (10) | 0.0338 (9) | −0.0060 (8) | 0.0076 (7) | −0.0023 (7) |
| C17 | 0.0448 (11) | 0.0580 (13) | 0.0349 (9) | 0.0062 (9) | 0.0083 (8) | 0.0008 (9) |
| C18 | 0.0722 (15) | 0.0392 (11) | 0.0382 (10) | 0.0059 (10) | 0.0123 (9) | 0.0006 (8) |
| C19 | 0.0683 (14) | 0.0364 (11) | 0.0504 (11) | −0.0152 (10) | 0.0108 (10) | −0.0032 (9) |
| C20 | 0.0421 (10) | 0.0423 (10) | 0.0427 (10) | −0.0100 (8) | 0.0073 (8) | −0.0065 (8) |
Geometric parameters (Å, º)
| O1—C7 | 1.343 (2) | C10—C11 | 1.385 (3) |
| O1—C8 | 1.460 (2) | C10—H10 | 0.9300 |
| O2—C7 | 1.203 (2) | C11—C12 | 1.383 (3) |
| C1—C2 | 1.388 (2) | C11—H11 | 0.9300 |
| C1—C6 | 1.396 (2) | C12—C13 | 1.379 (3) |
| C1—C7 | 1.482 (2) | C12—H12 | 0.9300 |
| C2—C3 | 1.381 (3) | C13—C14 | 1.387 (3) |
| C2—H2 | 0.9300 | C13—H13 | 0.9300 |
| C3—C4 | 1.382 (3) | C14—H14 | 0.9300 |
| C3—H3 | 0.9300 | C15—C20 | 1.390 (2) |
| C4—C5 | 1.384 (3) | C15—C16 | 1.392 (2) |
| C4—H4 | 0.9300 | C16—C17 | 1.380 (3) |
| C5—C6 | 1.375 (3) | C16—H16 | 0.9300 |
| C5—H5 | 0.9300 | C17—C18 | 1.384 (3) |
| C6—H6 | 0.9300 | C17—H17 | 0.9300 |
| C8—C15 | 1.511 (3) | C18—C19 | 1.381 (3) |
| C8—C9 | 1.511 (2) | C18—H18 | 0.9300 |
| C8—H8 | 0.9800 | C19—C20 | 1.382 (3) |
| C9—C10 | 1.392 (3) | C19—H19 | 0.9300 |
| C9—C14 | 1.394 (3) | C20—H20 | 0.9300 |
| C7—O1—C8 | 117.21 (13) | C11—C10—H10 | 119.9 |
| C2—C1—C6 | 119.42 (17) | C9—C10—H10 | 119.9 |
| C2—C1—C7 | 122.53 (15) | C12—C11—C10 | 120.54 (19) |
| C6—C1—C7 | 118.05 (16) | C12—C11—H11 | 119.7 |
| C3—C2—C1 | 120.18 (18) | C10—C11—H11 | 119.7 |
| C3—C2—H2 | 119.9 | C13—C12—C11 | 119.72 (17) |
| C1—C2—H2 | 119.9 | C13—C12—H12 | 120.1 |
| C2—C3—C4 | 120.15 (18) | C11—C12—H12 | 120.1 |
| C2—C3—H3 | 119.9 | C12—C13—C14 | 120.08 (18) |
| C4—C3—H3 | 119.9 | C12—C13—H13 | 120.0 |
| C3—C4—C5 | 119.89 (18) | C14—C13—H13 | 120.0 |
| C3—C4—H4 | 120.1 | C13—C14—C9 | 120.65 (18) |
| C5—C4—H4 | 120.1 | C13—C14—H14 | 119.7 |
| C6—C5—C4 | 120.37 (19) | C9—C14—H14 | 119.7 |
| C6—C5—H5 | 119.8 | C20—C15—C16 | 118.97 (17) |
| C4—C5—H5 | 119.8 | C20—C15—C8 | 120.50 (16) |
| C5—C6—C1 | 119.98 (18) | C16—C15—C8 | 120.53 (16) |
| C5—C6—H6 | 120.0 | C17—C16—C15 | 120.40 (18) |
| C1—C6—H6 | 120.0 | C17—C16—H16 | 119.8 |
| O2—C7—O1 | 123.26 (16) | C15—C16—H16 | 119.8 |
| O2—C7—C1 | 124.91 (16) | C16—C17—C18 | 120.2 (2) |
| O1—C7—C1 | 111.83 (14) | C16—C17—H17 | 119.9 |
| O1—C8—C15 | 109.39 (13) | C18—C17—H17 | 119.9 |
| O1—C8—C9 | 106.13 (14) | C19—C18—C17 | 119.7 (2) |
| C15—C8—C9 | 113.59 (14) | C19—C18—H18 | 120.1 |
| O1—C8—H8 | 109.2 | C17—C18—H18 | 120.1 |
| C15—C8—H8 | 109.2 | C18—C19—C20 | 120.2 (2) |
| C9—C8—H8 | 109.2 | C18—C19—H19 | 119.9 |
| C10—C9—C14 | 118.75 (16) | C20—C19—H19 | 119.9 |
| C10—C9—C8 | 122.17 (15) | C19—C20—C15 | 120.42 (19) |
| C14—C9—C8 | 119.06 (16) | C19—C20—H20 | 119.8 |
| C11—C10—C9 | 120.26 (18) | C15—C20—H20 | 119.8 |
| C6—C1—C2—C3 | −1.1 (3) | C14—C9—C10—C11 | 0.4 (3) |
| C7—C1—C2—C3 | 178.80 (17) | C8—C9—C10—C11 | 178.47 (18) |
| C1—C2—C3—C4 | 1.0 (3) | C9—C10—C11—C12 | −0.4 (3) |
| C2—C3—C4—C5 | −0.2 (3) | C10—C11—C12—C13 | 0.0 (3) |
| C3—C4—C5—C6 | −0.6 (3) | C11—C12—C13—C14 | 0.4 (3) |
| C4—C5—C6—C1 | 0.5 (3) | C12—C13—C14—C9 | −0.4 (3) |
| C2—C1—C6—C5 | 0.3 (3) | C10—C9—C14—C13 | 0.0 (3) |
| C7—C1—C6—C5 | −179.60 (17) | C8—C9—C14—C13 | −178.14 (17) |
| C8—O1—C7—O2 | −5.1 (3) | O1—C8—C15—C20 | 129.89 (16) |
| C8—O1—C7—C1 | 175.31 (13) | C9—C8—C15—C20 | −111.75 (18) |
| C2—C1—C7—O2 | −179.04 (19) | O1—C8—C15—C16 | −50.40 (19) |
| C6—C1—C7—O2 | 0.8 (3) | C9—C8—C15—C16 | 68.0 (2) |
| C2—C1—C7—O1 | 0.5 (2) | C20—C15—C16—C17 | −1.9 (3) |
| C6—C1—C7—O1 | −179.61 (16) | C8—C15—C16—C17 | 178.38 (15) |
| C7—O1—C8—C15 | −78.53 (17) | C15—C16—C17—C18 | 0.7 (3) |
| C7—O1—C8—C9 | 158.56 (14) | C16—C17—C18—C19 | 0.8 (3) |
| O1—C8—C9—C10 | 31.5 (2) | C17—C18—C19—C20 | −1.1 (3) |
| C15—C8—C9—C10 | −88.7 (2) | C18—C19—C20—C15 | −0.1 (3) |
| O1—C8—C9—C14 | −150.37 (15) | C16—C15—C20—C19 | 1.6 (3) |
| C15—C8—C9—C14 | 89.40 (19) | C8—C15—C20—C19 | −178.71 (17) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C16—H16···O2i | 0.93 | 2.44 | 3.334 (2) | 160 |
Symmetry code: (i) x+1, y, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5566).
References
- Agilent (2012). CrysAlis PRO and CrysAlis RED Agilent Technologies, Yarnton, England.
- 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.
- Baidya, M., Mayr, H. & Mayer, P. (2009a). Acta Cryst. E65, o3035. [DOI] [PMC free article] [PubMed]
- Baidya, M., Mayr, H. & Mayer, P. (2009b). Acta Cryst. E65, o3224. [DOI] [PMC free article] [PubMed]
- Flack, H. D. (1983). Acta Cryst. A39, 876–881.
- Gowda, B. T., Foro, S., Nayak, R. & Fuess, H. (2007). Acta Cryst. E63, o3563.
- Gowda, B. T., Tokarčík, M., Kožíšek, J., Suchetan, P. A. & Fuess, H. (2009). Acta Cryst. E65, o2599. [DOI] [PMC free article] [PubMed]
- 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) global, I. DOI: 10.1107/S1600536812050064/lh5566sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812050064/lh5566Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812050064/lh5566Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


