| Literature DB >> 24046689 |
Bernhard Bugenhagen1, Yosef Al Jasem, Bassam Al Hindawi, Nathir Al Rawashdeh, Thies Thiemann.
Abstract
In the title mol-ecule, C18H13BrO2, the anthracene unit forms an angle of 46.91 (2)° with the mean plane of the methyl acrylate moiety. In the crystal, the mol-ecules arrange themselves into strands parallel to [010] and, due to the crystal symmetry, there are eight strands crossing the unit cell. In each strand, mol-ecules form short C-H⋯O and C-H⋯π contacts and have their anthracene groups parallel to each other. Neighboring strands, related by a c-glide operation, are connected via C-H⋯O inter-actions and form a layer parallel to (100). The arrangement of the acrylate and anthracene groups in the crystal do not allow for [2 + 2] or [4 + 4] cyclo-addition.Entities:
Year: 2013 PMID: 24046689 PMCID: PMC3770404 DOI: 10.1107/S1600536813016905
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| C18H13BrO2 | |
| Melting point: 425 K | |
| Orthorhombic, | Cu |
| Cell parameters from 13502 reflections | |
| θ = 4.3–76.3° | |
| µ = 3.98 mm−1 | |
| Block, light yellow | |
| 0.21 × 0.19 × 0.13 mm |
| Oxford Diffraction SuperNova, Dual, Cu at zero, Atlas diffractometer | 2961 independent reflections |
| Radiation source: SuperNova (Cu) X-ray Source | 2900 reflections with |
| Mirror monochromator | |
| Detector resolution: 10.4127 pixels mm-1 | θmax = 76.3°, θmin = 4.4° |
| ω scans | |
| Absorption correction: analytical ( | |
| 25313 measured reflections |
| Refinement on | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| H-atom parameters constrained | |
| (Δ/σ)max = 0.003 | |
| 2961 reflections | Δρmax = 0.31 e Å−3 |
| 191 parameters | Δρmin = −0.44 e Å−3 |
| 0 restraints |
| 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. |
| Br1 | 0.28462 (2) | 1.11853 (4) | 0.77185 (2) | 0.01637 (8) | |
| C1 | 0.32116 (4) | 0.9076 (3) | 0.73973 (14) | 0.0125 (4) | |
| C10 | 0.34022 (5) | 0.3729 (3) | 0.56492 (14) | 0.0143 (4) | |
| C11 | 0.31165 (5) | 0.3554 (4) | 0.51014 (14) | 0.0159 (4) | |
| C12 | 0.28558 (4) | 0.5263 (4) | 0.52784 (14) | 0.0157 (4) | |
| C13 | 0.28813 (4) | 0.7045 (4) | 0.60248 (14) | 0.0141 (4) | |
| C14 | 0.31732 (4) | 0.7266 (3) | 0.66306 (13) | 0.0121 (3) | |
| C15 | 0.40212 (4) | 0.4163 (3) | 0.67191 (14) | 0.0132 (4) | |
| C16 | 0.43266 (4) | 0.4937 (4) | 0.65111 (14) | 0.0145 (4) | |
| C17 | 0.45923 (4) | 0.3109 (4) | 0.63028 (14) | 0.0147 (4) | |
| C18 | 0.51645 (5) | 0.2672 (4) | 0.60385 (19) | 0.0263 (5) | |
| C2 | 0.35047 (4) | 0.9392 (3) | 0.79499 (14) | 0.0122 (3) | |
| C3 | 0.35474 (5) | 1.1300 (3) | 0.87078 (14) | 0.0144 (4) | |
| C4 | 0.38315 (5) | 1.1478 (4) | 0.92569 (14) | 0.0165 (4) | |
| C5 | 0.40887 (4) | 0.9717 (4) | 0.91069 (14) | 0.0160 (4) | |
| C6 | 0.40616 (4) | 0.7915 (4) | 0.83732 (14) | 0.0148 (4) | |
| C7 | 0.37738 (4) | 0.7705 (3) | 0.77405 (13) | 0.0119 (3) | |
| C8 | 0.37435 (4) | 0.5854 (3) | 0.69716 (14) | 0.0120 (3) | |
| C9 | 0.34444 (4) | 0.5594 (3) | 0.64271 (14) | 0.0120 (3) | |
| H10 | 0.3573 | 0.2613 | 0.5514 | 0.017* | |
| H11 | 0.3093 | 0.2304 | 0.4609 | 0.019* | |
| H12 | 0.2666 | 0.5171 | 0.4883 | 0.019* | |
| H13 | 0.2706 | 0.8133 | 0.6141 | 0.017* | |
| H15 | 0.3980 | 0.2444 | 0.6704 | 0.016* | |
| H16 | 0.4373 | 0.6648 | 0.6497 | 0.017* | |
| H18A | 0.5146 | 0.1947 | 0.5368 | 0.039* | |
| H18B | 0.5169 | 0.1357 | 0.6541 | 0.039* | |
| H18C | 0.5364 | 0.3639 | 0.6081 | 0.039* | |
| H3 | 0.3378 | 1.2440 | 0.8828 | 0.017* | |
| H4 | 0.3857 | 1.2763 | 0.9733 | 0.020* | |
| H5 | 0.4277 | 0.9793 | 0.9512 | 0.019* | |
| H6 | 0.4234 | 0.6788 | 0.8279 | 0.018* | |
| O1 | 0.48841 (3) | 0.4289 (3) | 0.62263 (12) | 0.0218 (3) | |
| O2 | 0.45611 (3) | 0.0860 (3) | 0.62159 (11) | 0.0188 (3) |
| Br1 | 0.01322 (11) | 0.01739 (12) | 0.01851 (12) | 0.00440 (7) | 0.00145 (7) | −0.00092 (7) |
| C1 | 0.0115 (8) | 0.0126 (8) | 0.0134 (8) | 0.0022 (7) | 0.0032 (7) | 0.0026 (7) |
| C10 | 0.0131 (8) | 0.0149 (9) | 0.0150 (8) | −0.0007 (7) | 0.0037 (7) | −0.0002 (7) |
| C11 | 0.0174 (9) | 0.0177 (9) | 0.0126 (8) | −0.0038 (7) | 0.0028 (7) | −0.0025 (7) |
| C12 | 0.0129 (8) | 0.0203 (10) | 0.0140 (9) | −0.0035 (7) | −0.0003 (7) | 0.0027 (8) |
| C13 | 0.0115 (8) | 0.0151 (9) | 0.0155 (9) | 0.0000 (7) | 0.0014 (7) | 0.0039 (8) |
| C14 | 0.0111 (8) | 0.0130 (8) | 0.0122 (8) | −0.0004 (7) | 0.0020 (6) | 0.0030 (7) |
| C15 | 0.0141 (8) | 0.0119 (8) | 0.0137 (8) | 0.0019 (7) | −0.0009 (7) | −0.0001 (7) |
| C16 | 0.0145 (8) | 0.0111 (8) | 0.0180 (9) | 0.0009 (7) | 0.0015 (7) | 0.0005 (7) |
| C17 | 0.0118 (8) | 0.0175 (9) | 0.0149 (8) | −0.0002 (7) | −0.0009 (7) | −0.0021 (7) |
| C18 | 0.0111 (9) | 0.0307 (12) | 0.0371 (12) | 0.0045 (8) | 0.0014 (8) | −0.0118 (10) |
| C2 | 0.0119 (8) | 0.0121 (8) | 0.0126 (8) | −0.0005 (7) | 0.0024 (7) | 0.0030 (7) |
| C3 | 0.0144 (8) | 0.0137 (9) | 0.0151 (9) | 0.0008 (7) | 0.0033 (7) | 0.0000 (7) |
| C4 | 0.0189 (9) | 0.0173 (9) | 0.0134 (8) | −0.0037 (7) | 0.0027 (7) | −0.0017 (7) |
| C5 | 0.0124 (8) | 0.0207 (10) | 0.0148 (8) | −0.0030 (7) | −0.0016 (7) | 0.0015 (8) |
| C6 | 0.0117 (8) | 0.0161 (9) | 0.0167 (9) | 0.0009 (7) | 0.0005 (7) | 0.0022 (7) |
| C7 | 0.0117 (8) | 0.0113 (8) | 0.0128 (8) | −0.0008 (7) | 0.0019 (6) | 0.0031 (7) |
| C8 | 0.0114 (8) | 0.0109 (8) | 0.0138 (8) | 0.0005 (7) | 0.0021 (7) | 0.0032 (7) |
| C9 | 0.0119 (8) | 0.0113 (8) | 0.0128 (8) | −0.0009 (7) | 0.0031 (6) | 0.0011 (7) |
| O1 | 0.0098 (6) | 0.0199 (7) | 0.0356 (8) | −0.0004 (5) | 0.0041 (6) | −0.0088 (6) |
| O2 | 0.0162 (6) | 0.0136 (7) | 0.0266 (7) | 0.0024 (5) | 0.0007 (6) | −0.0016 (6) |
| C1—Br1 | 1.9068 (18) | C18—H18C | 0.9600 |
| C1—C14 | 1.398 (3) | C18—H18B | 0.9600 |
| C1—C2 | 1.402 (3) | C18—H18A | 0.9600 |
| C10—C11 | 1.366 (3) | C2—C7 | 1.440 (2) |
| C10—H10 | 0.9300 | C2—C3 | 1.429 (3) |
| C11—C12 | 1.414 (3) | C3—C4 | 1.361 (3) |
| C11—H11 | 0.9300 | C3—H3 | 0.9300 |
| C12—C13 | 1.364 (3) | C4—C5 | 1.416 (3) |
| C12—H12 | 0.9300 | C4—H4 | 0.9300 |
| C13—C14 | 1.430 (2) | C5—C6 | 1.361 (3) |
| C13—H13 | 0.9300 | C5—H5 | 0.9300 |
| C15—C16 | 1.334 (3) | C6—C7 | 1.435 (2) |
| C15—H15 | 0.9300 | C6—H6 | 0.9300 |
| C16—C17 | 1.478 (3) | C7—C8 | 1.413 (3) |
| C16—H16 | 0.9300 | C8—C15 | 1.479 (2) |
| C17—O2 | 1.208 (2) | C8—C9 | 1.414 (2) |
| C17—O1 | 1.344 (2) | C9—C14 | 1.440 (2) |
| C18—O1 | 1.448 (2) | C9—C10 | 1.431 (3) |
| C2—C1—Br1 | 118.41 (14) | C11—C10—H10 | 119.3 |
| C14—C1—C2 | 123.12 (17) | C10—C11—H11 | 119.8 |
| C14—C1—Br1 | 118.46 (14) | C10—C11—C12 | 120.37 (18) |
| C1—C2—C3 | 123.06 (17) | C12—C11—H11 | 119.8 |
| C1—C2—C7 | 118.09 (17) | C11—C12—H12 | 119.8 |
| C3—C2—C7 | 118.85 (17) | C13—C12—C11 | 120.48 (17) |
| C2—C3—H3 | 119.4 | C13—C12—H12 | 119.8 |
| C4—C3—C2 | 121.20 (18) | C12—C13—H13 | 119.5 |
| C4—C3—H3 | 119.4 | C12—C13—C14 | 121.07 (17) |
| C3—C4—H4 | 119.8 | C14—C13—H13 | 119.5 |
| C3—C4—C5 | 120.32 (18) | C1—C14—C9 | 118.22 (16) |
| C5—C4—H4 | 119.8 | C1—C14—C13 | 123.08 (17) |
| C4—C5—H5 | 119.9 | C13—C14—C9 | 118.68 (17) |
| C6—C5—C4 | 120.29 (17) | C8—C15—H15 | 117.8 |
| C6—C5—H5 | 119.9 | C16—C15—C8 | 124.45 (17) |
| C5—C6—H6 | 119.1 | C16—C15—H15 | 117.8 |
| C5—C6—C7 | 121.77 (17) | C15—C16—H16 | 119.6 |
| C7—C6—H6 | 119.1 | C15—C16—C17 | 120.83 (18) |
| C6—C7—C2 | 117.34 (16) | C17—C16—H16 | 119.6 |
| C8—C7—C2 | 120.27 (16) | O1—C17—C16 | 110.43 (17) |
| C8—C7—C6 | 122.32 (17) | O2—C17—C16 | 126.35 (18) |
| C7—C8—C9 | 120.06 (16) | O2—C17—O1 | 123.22 (18) |
| C7—C8—C15 | 121.10 (16) | H18A—C18—H18B | 109.5 |
| C9—C8—C15 | 118.84 (16) | H18A—C18—H18C | 109.5 |
| C8—C9—C10 | 121.88 (17) | H18B—C18—H18C | 109.5 |
| C8—C9—C14 | 120.18 (16) | O1—C18—H18A | 109.5 |
| C10—C9—C14 | 117.93 (16) | O1—C18—H18B | 109.5 |
| C9—C10—H10 | 119.3 | O1—C18—H18C | 109.5 |
| C11—C10—C9 | 121.42 (18) | C17—O1—C18 | 115.31 (16) |
| C1—C2—C3—C4 | 177.29 (18) | C8—C15—C16—C17 | 177.77 (17) |
| C1—C2—C7—C6 | −174.75 (17) | C9—C8—C15—C16 | 128.8 (2) |
| C1—C2—C7—C8 | 2.3 (3) | C9—C10—C11—C12 | 1.3 (3) |
| C2—C1—C14—C9 | 2.3 (3) | C10—C9—C14—C1 | 179.34 (16) |
| C2—C1—C14—C13 | −176.07 (17) | C10—C9—C14—C13 | −2.2 (3) |
| C2—C3—C4—C5 | −1.8 (3) | C10—C11—C12—C13 | −2.5 (3) |
| C2—C7—C8—C9 | −2.1 (3) | C11—C12—C13—C14 | 1.3 (3) |
| C2—C7—C8—C15 | 177.76 (16) | C12—C13—C14—C1 | 179.44 (18) |
| C3—C2—C7—C6 | 5.1 (2) | C12—C13—C14—C9 | 1.1 (3) |
| C3—C2—C7—C8 | −177.85 (16) | C14—C1—C2—C3 | 177.70 (17) |
| C3—C4—C5—C6 | 3.6 (3) | C14—C1—C2—C7 | −2.4 (3) |
| C4—C5—C6—C7 | −0.9 (3) | C14—C9—C10—C11 | 1.1 (3) |
| C5—C6—C7—C2 | −3.5 (3) | C15—C8—C9—C10 | 0.7 (3) |
| C5—C6—C7—C8 | 179.56 (18) | C15—C8—C9—C14 | −177.88 (16) |
| C6—C7—C8—C9 | 174.75 (17) | C15—C16—C17—O1 | −173.18 (18) |
| C6—C7—C8—C15 | −5.4 (3) | C15—C16—C17—O2 | 6.3 (3) |
| C7—C2—C3—C4 | −2.6 (3) | C16—C17—O1—C18 | 179.04 (17) |
| C7—C8—C9—C10 | −179.43 (17) | O2—C17—O1—C18 | −0.5 (3) |
| C7—C8—C9—C14 | 2.0 (3) | Br1—C1—C2—C3 | −3.1 (2) |
| C7—C8—C15—C16 | −51.1 (3) | Br1—C1—C2—C7 | 176.78 (13) |
| C8—C9—C10—C11 | −177.55 (18) | Br1—C1—C14—C9 | −176.89 (13) |
| C8—C9—C14—C1 | −2.0 (3) | Br1—C1—C14—C13 | 4.7 (2) |
| C8—C9—C14—C13 | 176.41 (17) |
| H··· | ||||
| C15—H15··· | 0.93 | 2.91 (2) | 3.5055 (19) | 123 |
| C16—H16···O2ii | 0.93 | 2.40 | 3.315 (3) | 170 |
| C5—H5···O2iii | 0.93 | 2.53 | 3.372 (2) | 150 |
Hydrogen-bond geometry (Å, °)
Cg1 is the centroid of the C2–C7 ring.
|
|
| H⋯ |
|
|
|---|---|---|---|---|
| C15—H15⋯ | 0.93 | 2.91 (2) | 3.5055 (19) | 123 |
| C16—H16⋯O2ii | 0.93 | 2.40 | 3.315 (3) | 170 |
| C5—H5⋯O2iii | 0.93 | 2.53 | 3.372 (2) | 150 |
Symmetry codes: (i) ; (ii) ; (iii) .