Abstract
In the title compound, C19H18, the anthracene system is almost planar, with a maximum deviation of −0.039 (1) Å. The structure is stabilized by C—H⋯π interactions. The pentene moiety is not planar and is twisted away from the attached anthracene system with a maximum torsion angle of 91.2 (1)°.
Related literature
For background to anthracene, see: de Silva et al. (1997 ▶); Klarner et al. (1998 ▶); Han et al. (2009 ▶).
Experimental
Crystal data
C19H18
M r = 246.33
Monoclinic,
a = 11.1555 (2) Å
b = 7.2678 (1) Å
c = 19.7129 (3) Å
β = 119.096 (1)°
V = 1396.55 (4) Å3
Z = 4
Mo Kα radiation
μ = 0.07 mm−1
T = 100 K
0.73 × 0.38 × 0.26 mm
Data collection
Bruker SMART APEXII CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.953, T max = 0.983
20185 measured reflections
5271 independent reflections
3948 reflections with I > 2σ(I)
R int = 0.028
Refinement
R[F 2 > 2σ(F 2)] = 0.049
wR(F 2) = 0.151
S = 1.05
5271 reflections
172 parameters
H-atom parameters constrained
Δρmax = 0.47 e Å−3
Δρmin = −0.23 e Å−3
Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811030571/ng5202sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811030571/ng5202Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811030571/ng5202Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. C—H⋯π interactions (Å, °).
Cg1 and Cg2 are the centroids of the C1–C6 and C1/C6–C8/C13/C14 rings, respectively.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C5—H5A⋯Cg2i | 0.95 | 2.63 | 3.5729 (9) | 175 |
| C7—H7A⋯Cg1i | 0.95 | 2.74 | 3.6851 (9) | 177 |
| C17—H17A⋯Cg2ii | 0.99 | 2.58 | 3.4643 (9) | 149 |
| C18—H18A⋯Cg1ii | 0.95 | 2.90 | 3.6553 (11) | 138 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
NA, AIM and UK gratefully acknowledge the Deanship of Scientific Research, College of Science, King Saud University (KSU) for funding the synthesis work under Research Grant RGP-VPP-026.
supplementary crystallographic information
Comment
Anthracene is an attractive material in its photochemical and electrochemical properties as well as used as a potential medium for photoconductive (de Silva et al., 1997) and electroluminescence (Klarner et al., 1998) devices. Furthermore, anthracene derivatives exhibited anticancer activity has also been reported recently (Han et al., 2009). As part of an ongoing study on such compounds, in this paper, we present the crystal structure of the title compound, which was synthesized as an intermediate.
All parameters in (I) within normal ranges. The anthracene is planar with maximum deviation of -0.039 (1)Å from atom C11. In the crystal, C—H···π (Table 1) interactions contribute in stabilizing the crystal structure involving Cg1 = C1—C6 and Cg2 = C1/C6–8/C13—C14.
Experimental
A solution of anthrone (1 g, 5.1 mmol) in anhydrous THF (20 ml) was slowly added to pent-4-enylmagnesium bromide (0.47 g, 6.5 mmol). The mixture was stirred for 8 h at room temperature. The reaction mixture was subsequently acidified with 10% HCl, the organic layer was separated, and the aqueous layer was extracted with ether (2 X 10 ml). The combined organic layer was washed with water, dried over MgSO4 and the solvent was evaporated under reduced pressure and the crude product was added 5 ml benzene, 1.2 g P2O5 and stirred for 6 h at room temperature. The P2O5 was filtered off and the benzene was removed under vacuum. The crude product was purified by column chromatography (hexane-dichloromethene 1:1). The product was recrystallized from EtOAc to yield title compound as colourless crystals.
Refinement
All H-atoms were positioned geometrically and refined using a riding model, with C—H = 0.95 and 0.99 Å, and with Uiso = 1.2Ueq(C).
Figures
Fig. 1.
The molecular structure, showing 50% probability displacement ellipsoids. Hydrogen atoms are shown as spheres of arbitrary radius.
Crystal data
| C19H18 | F(000) = 528 |
| Mr = 246.33 | Dx = 1.172 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 5794 reflections |
| a = 11.1555 (2) Å | θ = 2.4–33.0° |
| b = 7.2678 (1) Å | µ = 0.07 mm−1 |
| c = 19.7129 (3) Å | T = 100 K |
| β = 119.096 (1)° | Block, colourless |
| V = 1396.55 (4) Å3 | 0.73 × 0.38 × 0.26 mm |
| Z = 4 |
Data collection
| Bruker SMART APEXII CCD area-detector diffractometer | 5271 independent reflections |
| Radiation source: fine-focus sealed tube | 3948 reflections with I > 2σ(I) |
| graphite | Rint = 0.028 |
| φ and ω scans | θmax = 33.1°, θmin = 2.1° |
| Absorption correction: multi-scan (SADABS; Bruker, 2009) | h = −17→16 |
| Tmin = 0.953, Tmax = 0.983 | k = −9→11 |
| 20185 measured reflections | l = −30→30 |
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)] = 0.049 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.151 | H-atom parameters constrained |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0816P)2 + 0.1778P] where P = (Fo2 + 2Fc2)/3 |
| 5271 reflections | (Δ/σ)max = 0.001 |
| 172 parameters | Δρmax = 0.47 e Å−3 |
| 0 restraints | Δρmin = −0.23 e Å−3 |
Special details
| Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K. |
| 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)
| x | y | z | Uiso*/Ueq | ||
| C1 | 0.12149 (8) | 0.51562 (11) | 0.87949 (5) | 0.01455 (16) | |
| C2 | 0.03754 (9) | 0.45215 (12) | 0.91135 (5) | 0.01904 (17) | |
| H2A | 0.0693 | 0.3540 | 0.9478 | 0.023* | |
| C3 | −0.08723 (9) | 0.53006 (14) | 0.89033 (5) | 0.02260 (19) | |
| H3A | −0.1405 | 0.4860 | 0.9126 | 0.027* | |
| C4 | −0.13826 (9) | 0.67610 (14) | 0.83556 (6) | 0.02333 (19) | |
| H4A | −0.2250 | 0.7294 | 0.8216 | 0.028* | |
| C5 | −0.06301 (9) | 0.73990 (12) | 0.80296 (5) | 0.01996 (18) | |
| H5A | −0.0981 | 0.8372 | 0.7662 | 0.024* | |
| C6 | 0.06813 (8) | 0.66222 (11) | 0.82341 (5) | 0.01545 (16) | |
| C7 | 0.14534 (8) | 0.72875 (11) | 0.79022 (5) | 0.01635 (16) | |
| H7A | 0.1101 | 0.8263 | 0.7536 | 0.020* | |
| C8 | 0.27345 (8) | 0.65400 (11) | 0.81012 (5) | 0.01535 (16) | |
| C9 | 0.35206 (9) | 0.72202 (13) | 0.77582 (5) | 0.02136 (18) | |
| H9A | 0.3178 | 0.8221 | 0.7404 | 0.026* | |
| C10 | 0.47518 (9) | 0.64570 (14) | 0.79301 (6) | 0.0248 (2) | |
| H10A | 0.5258 | 0.6919 | 0.7695 | 0.030* | |
| C11 | 0.52754 (9) | 0.49685 (14) | 0.84623 (6) | 0.02274 (19) | |
| H11A | 0.6129 | 0.4430 | 0.8575 | 0.027* | |
| C12 | 0.45707 (8) | 0.43008 (12) | 0.88137 (5) | 0.01865 (17) | |
| H12A | 0.4948 | 0.3312 | 0.9172 | 0.022* | |
| C13 | 0.32723 (8) | 0.50604 (11) | 0.86544 (5) | 0.01458 (15) | |
| C14 | 0.25201 (8) | 0.43960 (11) | 0.90096 (5) | 0.01431 (15) | |
| C15 | 0.30778 (9) | 0.28354 (11) | 0.95877 (5) | 0.01744 (17) | |
| H15A | 0.2711 | 0.2941 | 0.9953 | 0.021* | |
| H15B | 0.4089 | 0.2943 | 0.9891 | 0.021* | |
| C16 | 0.27031 (9) | 0.09379 (11) | 0.91969 (5) | 0.01856 (17) | |
| H16A | 0.3180 | 0.0757 | 0.8890 | 0.022* | |
| H16B | 0.1703 | 0.0887 | 0.8836 | 0.022* | |
| C17 | 0.31046 (9) | −0.06170 (12) | 0.97964 (5) | 0.01997 (18) | |
| H17A | 0.3154 | −0.1789 | 0.9555 | 0.024* | |
| H17B | 0.4028 | −0.0361 | 1.0238 | 0.024* | |
| C18 | 0.21099 (11) | −0.08229 (13) | 1.00944 (6) | 0.0254 (2) | |
| H18A | 0.1204 | −0.1198 | 0.9734 | 0.031* | |
| C19 | 0.23850 (14) | −0.05277 (16) | 1.08162 (7) | 0.0363 (3) | |
| H19A | 0.3279 | −0.0151 | 1.1195 | 0.044* | |
| H19C | 0.1689 | −0.0692 | 1.0957 | 0.044* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0157 (3) | 0.0131 (3) | 0.0142 (3) | −0.0012 (2) | 0.0068 (3) | −0.0018 (3) |
| C2 | 0.0204 (4) | 0.0205 (4) | 0.0175 (4) | −0.0032 (3) | 0.0101 (3) | −0.0017 (3) |
| C3 | 0.0200 (4) | 0.0287 (4) | 0.0226 (4) | −0.0048 (3) | 0.0131 (3) | −0.0049 (4) |
| C4 | 0.0156 (4) | 0.0283 (4) | 0.0260 (4) | 0.0005 (3) | 0.0100 (3) | −0.0056 (4) |
| C5 | 0.0165 (3) | 0.0199 (4) | 0.0207 (4) | 0.0034 (3) | 0.0069 (3) | −0.0005 (3) |
| C6 | 0.0146 (3) | 0.0147 (3) | 0.0157 (3) | 0.0005 (3) | 0.0063 (3) | −0.0014 (3) |
| C7 | 0.0170 (3) | 0.0144 (3) | 0.0164 (4) | 0.0015 (3) | 0.0071 (3) | 0.0018 (3) |
| C8 | 0.0159 (3) | 0.0150 (3) | 0.0151 (3) | −0.0003 (3) | 0.0075 (3) | 0.0001 (3) |
| C9 | 0.0208 (4) | 0.0235 (4) | 0.0215 (4) | −0.0012 (3) | 0.0116 (3) | 0.0027 (3) |
| C10 | 0.0209 (4) | 0.0321 (5) | 0.0253 (4) | −0.0029 (3) | 0.0144 (4) | 0.0003 (4) |
| C11 | 0.0165 (4) | 0.0276 (4) | 0.0245 (4) | 0.0010 (3) | 0.0103 (3) | −0.0046 (4) |
| C12 | 0.0162 (3) | 0.0173 (4) | 0.0203 (4) | 0.0020 (3) | 0.0071 (3) | −0.0017 (3) |
| C13 | 0.0141 (3) | 0.0132 (3) | 0.0152 (3) | 0.0003 (2) | 0.0061 (3) | −0.0022 (3) |
| C14 | 0.0159 (3) | 0.0115 (3) | 0.0139 (3) | 0.0000 (2) | 0.0060 (3) | −0.0008 (3) |
| C15 | 0.0201 (4) | 0.0139 (3) | 0.0155 (3) | 0.0004 (3) | 0.0065 (3) | 0.0009 (3) |
| C16 | 0.0220 (4) | 0.0140 (3) | 0.0171 (4) | 0.0002 (3) | 0.0074 (3) | 0.0004 (3) |
| C17 | 0.0230 (4) | 0.0135 (3) | 0.0200 (4) | 0.0013 (3) | 0.0078 (3) | 0.0019 (3) |
| C18 | 0.0320 (5) | 0.0180 (4) | 0.0272 (5) | −0.0009 (3) | 0.0151 (4) | 0.0021 (3) |
| C19 | 0.0531 (7) | 0.0295 (5) | 0.0336 (6) | 0.0003 (5) | 0.0267 (5) | 0.0015 (5) |
Geometric parameters (Å, °)
| C1—C14 | 1.4159 (11) | C11—C12 | 1.3650 (13) |
| C1—C2 | 1.4340 (11) | C11—H11A | 0.9500 |
| C1—C6 | 1.4393 (11) | C12—C13 | 1.4349 (11) |
| C2—C3 | 1.3670 (12) | C12—H12A | 0.9500 |
| C2—H2A | 0.9500 | C13—C14 | 1.4139 (11) |
| C3—C4 | 1.4208 (14) | C14—C15 | 1.5108 (11) |
| C3—H3A | 0.9500 | C15—C16 | 1.5352 (11) |
| C4—C5 | 1.3628 (13) | C15—H15A | 0.9900 |
| C4—H4A | 0.9500 | C15—H15B | 0.9900 |
| C5—C6 | 1.4311 (11) | C16—C17 | 1.5361 (12) |
| C5—H5A | 0.9500 | C16—H16A | 0.9900 |
| C6—C7 | 1.3971 (12) | C16—H16B | 0.9900 |
| C7—C8 | 1.3950 (11) | C17—C18 | 1.4941 (14) |
| C7—H7A | 0.9500 | C17—H17A | 0.9900 |
| C8—C9 | 1.4309 (12) | C17—H17B | 0.9900 |
| C8—C13 | 1.4385 (11) | C18—C19 | 1.3193 (15) |
| C9—C10 | 1.3625 (13) | C18—H18A | 0.9500 |
| C9—H9A | 0.9500 | C19—H19A | 0.9500 |
| C10—C11 | 1.4199 (14) | C19—H19C | 0.9500 |
| C10—H10A | 0.9500 | ||
| C14—C1—C2 | 122.63 (7) | C11—C12—C13 | 121.42 (8) |
| C14—C1—C6 | 119.97 (7) | C11—C12—H12A | 119.3 |
| C2—C1—C6 | 117.40 (7) | C13—C12—H12A | 119.3 |
| C3—C2—C1 | 121.30 (8) | C14—C13—C12 | 122.63 (7) |
| C3—C2—H2A | 119.3 | C14—C13—C8 | 120.10 (7) |
| C1—C2—H2A | 119.3 | C12—C13—C8 | 117.26 (7) |
| C2—C3—C4 | 120.83 (8) | C13—C14—C1 | 119.36 (7) |
| C2—C3—H3A | 119.6 | C13—C14—C15 | 120.27 (7) |
| C4—C3—H3A | 119.6 | C1—C14—C15 | 120.32 (7) |
| C5—C4—C3 | 120.09 (8) | C14—C15—C16 | 112.59 (7) |
| C5—C4—H4A | 120.0 | C14—C15—H15A | 109.1 |
| C3—C4—H4A | 120.0 | C16—C15—H15A | 109.1 |
| C4—C5—C6 | 120.84 (8) | C14—C15—H15B | 109.1 |
| C4—C5—H5A | 119.6 | C16—C15—H15B | 109.1 |
| C6—C5—H5A | 119.6 | H15A—C15—H15B | 107.8 |
| C7—C6—C5 | 120.67 (8) | C15—C16—C17 | 111.62 (7) |
| C7—C6—C1 | 119.80 (7) | C15—C16—H16A | 109.3 |
| C5—C6—C1 | 119.52 (8) | C17—C16—H16A | 109.3 |
| C8—C7—C6 | 120.93 (7) | C15—C16—H16B | 109.3 |
| C8—C7—H7A | 119.5 | C17—C16—H16B | 109.3 |
| C6—C7—H7A | 119.5 | H16A—C16—H16B | 108.0 |
| C7—C8—C9 | 120.79 (8) | C18—C17—C16 | 112.44 (7) |
| C7—C8—C13 | 119.79 (7) | C18—C17—H17A | 109.1 |
| C9—C8—C13 | 119.41 (7) | C16—C17—H17A | 109.1 |
| C10—C9—C8 | 121.14 (8) | C18—C17—H17B | 109.1 |
| C10—C9—H9A | 119.4 | C16—C17—H17B | 109.1 |
| C8—C9—H9A | 119.4 | H17A—C17—H17B | 107.8 |
| C9—C10—C11 | 119.78 (8) | C19—C18—C17 | 125.45 (10) |
| C9—C10—H10A | 120.1 | C19—C18—H18A | 117.3 |
| C11—C10—H10A | 120.1 | C17—C18—H18A | 117.3 |
| C12—C11—C10 | 120.96 (8) | C18—C19—H19A | 120.0 |
| C12—C11—H11A | 119.5 | C18—C19—H19C | 120.0 |
| C10—C11—H11A | 119.5 | H19A—C19—H19C | 120.0 |
| C14—C1—C2—C3 | 179.04 (8) | C11—C12—C13—C14 | 179.98 (8) |
| C6—C1—C2—C3 | −1.14 (12) | C11—C12—C13—C8 | 0.79 (12) |
| C1—C2—C3—C4 | 0.48 (14) | C7—C8—C13—C14 | −1.54 (12) |
| C2—C3—C4—C5 | 0.28 (14) | C9—C8—C13—C14 | 178.80 (8) |
| C3—C4—C5—C6 | −0.31 (14) | C7—C8—C13—C12 | 177.67 (7) |
| C4—C5—C6—C7 | −179.61 (8) | C9—C8—C13—C12 | −1.98 (11) |
| C4—C5—C6—C1 | −0.39 (13) | C12—C13—C14—C1 | −176.95 (7) |
| C14—C1—C6—C7 | 0.14 (12) | C8—C13—C14—C1 | 2.22 (12) |
| C2—C1—C6—C7 | −179.68 (7) | C12—C13—C14—C15 | 0.50 (12) |
| C14—C1—C6—C5 | −179.09 (7) | C8—C13—C14—C15 | 179.67 (7) |
| C2—C1—C6—C5 | 1.09 (12) | C2—C1—C14—C13 | 178.29 (7) |
| C5—C6—C7—C8 | 179.78 (8) | C6—C1—C14—C13 | −1.52 (12) |
| C1—C6—C7—C8 | 0.56 (12) | C2—C1—C14—C15 | 0.84 (12) |
| C6—C7—C8—C9 | 179.78 (8) | C6—C1—C14—C15 | −178.97 (7) |
| C6—C7—C8—C13 | 0.13 (12) | C13—C14—C15—C16 | −86.19 (9) |
| C7—C8—C9—C10 | −177.80 (8) | C1—C14—C15—C16 | 91.23 (9) |
| C13—C8—C9—C10 | 1.85 (13) | C14—C15—C16—C17 | −172.08 (7) |
| C8—C9—C10—C11 | −0.43 (14) | C15—C16—C17—C18 | 78.26 (9) |
| C9—C10—C11—C12 | −0.83 (15) | C16—C17—C18—C19 | −114.87 (11) |
| C10—C11—C12—C13 | 0.63 (14) |
Hydrogen-bond geometry (Å, °)
| Cg1 and Cg2 are the centroids of the C1–C6 and C1/C6–C8/C13/C14 rings, respectively. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| C5—H5A···Cg2i | 0.95 | 2.63 | 3.5729 (9) | 175 |
| C7—H7A···Cg1i | 0.95 | 2.74 | 3.6851 (9) | 177 |
| C17—H17A···Cg2ii | 0.99 | 2.58 | 3.4643 (9) | 149 |
| C18—H18A···Cg1ii | 0.95 | 2.90 | 3.6553 (11) | 138 |
Symmetry codes: (i) −x, y+1/2, −z+3/2; (ii) x, y−1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG5202).
References
- Bruker (2009). APEX2, SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
- Han, X., Li, C., Mosher, M. D., Rider, K. C., Zhou, P., Crawford, R. L., Fusco, W., Paszczynski, A. & Natale, N. R. (2009). Bioorg. Med. Chem. 17, 1671–1680. [DOI] [PMC free article] [PubMed]
- Klarner, G., Davey, M. H., Chen, W.-D., Scott, J. C. & Miller, R. D. (1998). Adv. Mater. 10, 993–997.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Silva, A. P. de, Gunaratne, H. Q. N. & Mc Coy, C. P. (1997). J. Am. Chem. Soc. 119, 7891–7892.
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [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) I, global. DOI: 10.1107/S1600536811030571/ng5202sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811030571/ng5202Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811030571/ng5202Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

