Abstract
The title compound, C14H24O2, was synthesized from ilicic acid, which was isolated from the aerial part of Inula Viscosa (L) Aiton [or Dittrichia Viscosa (L) Greuter]. The molecule contains two fused six-membered rings, which both display a chair conformation. In the crystal, molecules are linked into chains propagating along the b axis by intermolecular O—H⋯O hydrogen bonds.
Related literature
For the synthesis, see: Barrero et al. (2009 ▶). For the medicinal interest in Inula Viscosa (L) Aiton [or Dittrichia Viscosa (L) Greuter], see: Shtacher & Kasshman, (1970 ▶); Bohlmann et al. (1977 ▶); Chiappini et al. (1982 ▶) and for the pharmacological interest, see: Azoulay et al. (1986 ▶); Bohlmann et al. (1977 ▶); Ceccherelli et al. (1988 ▶). For background to phytochemical studies of plants, see: Geissman & Toribio (1967 ▶). For conformational analysis, see: Cremer & Pople (1975 ▶).
Experimental
Crystal data
C14H24O2
M r = 224.33
Monoclinic,
a = 6.4919 (7) Å
b = 9.4057 (9) Å
c = 10.3638 (11) Å
β = 97.286 (10)°
V = 627.71 (11) Å3
Z = 2
Mo Kα radiation
μ = 0.08 mm−1
T = 180 K
0.6 × 0.25 × 0.15 mm
Data collection
Agilent Eos Gemini Ultra diffractometer
6571 measured reflections
1362 independent reflections
1262 reflections with I > 2σ(I)
R int = 0.047
Refinement
R[F 2 > 2σ(F 2)] = 0.043
wR(F 2) = 0.119
S = 1.09
1362 reflections
152 parameters
1 restraint
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.28 e Å−3
Δρmin = −0.24 e Å−3
Data collection: CrysAlis PRO (Agilent, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXL97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶) and PLATON (Spek, 2009 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811004454/fj2393sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004454/fj2393Isup2.hkl
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 |
|---|---|---|---|---|
| O1—H2⋯O2i | 0.84 (3) | 2.05 (3) | 2.883 (2) | 169 (3) |
Symmetry code: (i)
.
Acknowledgments
The authors thank the Unit of Support for Technical and Scientific Research (UATRS, CNRST) for the X-ray measurements.
supplementary crystallographic information
Comment
The ilicic acid is one of the main components of the extracts of the aerial parts Inula viscose. This natural acid is a major constituent of the dichloromethane extract of the Inula Viscosa (L) Aiton [or Dittrichia Viscosa (L) Greuter]. This plant is widespread in Mediterranean area and extends to the Atlantic cost of Morocco. It is a well known medicinal plant (Shtacher & Kasshman, 1970; Chiappini et al., 1982) and has some pharmacological activities (Azoulay et al., 1986). the Inula Viscosa (L) Aiton has been the subject of chemical investigation in terms of isolating sesquiterpene lactones (Bohlmann et al., 1977), sesquiterpene acids (Ceccherelli et al., 1988; Geissman et al.1967). The literature report one article on the transformation of the ilicic acid (Barrero et al., 2009). In order to prepare products with high added value, used in the industry pharmacological or cosmetic, we have studied the reactivity of this acid. Thus, with the reaction Curtius, we synthesized the title compound(1R, 2R, 6R, 9R)-9-acethyl-2,6-dimethylbicyclo [4.4.0]decan-2-ol) with à yield 50%. The structure of this new derivative of ilicic acid was determined by NMR spectral analysis of 1H, 13 C and mass spectroscopy and confirmed by its single-crystal X-ray structure. The molecule is built up from two fused six-membered rings. The molecular structure of (I),Fig.1, shows the two rings to adopt a perfect chair conformation as indicated by Cremer & Pople (1975) puckering parameters Q(T)= 0.554 (2)Å and spherical polar angle θ = 178.1 (2)° with φ = 36 (7)° for the first ring (C1,C2··· C6) and Q(T)= 0.597 (2)Å with a spherical polar angle θ = 178.71 (19)° and φ = 108 (5)° for the second ring (C1, C6···C10)(Cremer and Pople,1975). In the crystal structure, molecules are linked into chains (Fig. 2) running along the b axis by intermolecular O—H···O hydrogen bonds (Table 1) involving the O1 and O2 atoms.
Experimental
A solution containing the ilicic acid 1 g (3.96 mmol) and Et3N 0.82 ml (5.895 mmol) in dry THF (100 ml) was cooled at -10 °C. Ethyl chloroformate 0,56 ml (5.95 mm l) was added dropwise and the reaction mixture was stirred at this temperature for 1 h. A solution of NaN3 0.43 g (6.74 mmol) in H2O (10 ml) was then added in one portion. After 1.5 h at 0 °C, the resulting heterogeous mixture was filttered, the organic solvent was removed under reduced pressure and the aqueous phase was extracted tree time with ether (3 × 50 ml). The combined organic layers were dried over MgSO4, and concentrated in vacuo. The crude acyl-azide was then dissolved in toluene (50 ml) and the resulting solution was refluxed for 1 h. Then a solution of hydrochloric acid at 10% was added to the reaction mixture which is remized at reflux for 2 h. After extraction, the organic phase is washed with water and brine, dried over anhydrous Na2SO4, filtered and concentrated under vacuum. The product was purified by column chromatography over silica gel (hexane/ethyl acetate 95/5). The title compound was recrystallized in dichloromethane.
Refinement
Except H2, all H atoms were fixed geometrically and treated as riding with C—H = 0.96 Å (methyl),0.97 Å (methylene), 0.98Å (methine) with Uiso(H) = 1.2Ueq(methylene, methine and OH) or Uiso(H) = 1.5Ueq(methyl). In the absence of significant anomalous scattering, the absolute configuration could not be reliably determined and thus 1167 Friedel pairs were merged and any references to the Flack parameter were removed.
Figures
Fig. 1.
Molecular structure of the title compound with the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are represented as small spheres of arbitrary radii.
Fig. 2.
Partial packing view showing the O—H···O interactions (dashed lines)and the formation of a chain parallel to the b axis. H atoms not involved in hydrogen bonding have been omitted for clarity. [Symmetry code: (i)1 - x,-1/2 + y,-z + 2]
Crystal data
| C14H24O2 | F(000) = 248 |
| Mr = 224.33 | Dx = 1.187 Mg m−3 |
| Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2yb | Cell parameters from 6571 reflections |
| a = 6.4919 (7) Å | θ = 2.9–26.4° |
| b = 9.4057 (9) Å | µ = 0.08 mm−1 |
| c = 10.3638 (11) Å | T = 180 K |
| β = 97.286 (10)° | Prism, colourless |
| V = 627.71 (11) Å3 | 0.6 × 0.25 × 0.15 mm |
| Z = 2 |
Data collection
| Agilent Eos Gemini Ultra diffractometer | 1262 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.047 |
| graphite | θmax = 26.4°, θmin = 2.9° |
| Detector resolution: 16.1978 pixels mm-1 | h = −8→8 |
| φ and ω scans | k = −11→11 |
| 6571 measured reflections | l = −12→12 |
| 1362 independent reflections |
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)] = 0.043 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.119 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.09 | w = 1/[σ2(Fo2) + (0.0935P)2 + 0.0033P] where P = (Fo2 + 2Fc2)/3 |
| 1362 reflections | (Δ/σ)max < 0.001 |
| 152 parameters | Δρmax = 0.28 e Å−3 |
| 1 restraint | Δρmin = −0.24 e Å−3 |
Special details
| Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 | ||
| H2 | 0.822 (5) | 0.709 (4) | 0.829 (3) | 0.039 (8)* | |
| C1 | 0.8653 (3) | 0.9919 (2) | 0.80775 (19) | 0.0185 (4) | |
| H1 | 0.9924 | 0.9851 | 0.8695 | 0.022* | |
| C2 | 0.8777 (3) | 0.8642 (2) | 0.7154 (2) | 0.0214 (4) | |
| C3 | 1.0704 (3) | 0.8816 (2) | 0.6454 (2) | 0.0261 (5) | |
| H3A | 1.1934 | 0.8693 | 0.7081 | 0.031* | |
| H3B | 1.0705 | 0.8072 | 0.5806 | 0.031* | |
| C4 | 1.0826 (3) | 1.0251 (3) | 0.5791 (2) | 0.0296 (5) | |
| H4A | 0.9684 | 1.0339 | 0.5095 | 0.036* | |
| H4B | 1.2114 | 1.0311 | 0.5411 | 0.036* | |
| C5 | 1.0729 (3) | 1.1462 (2) | 0.6757 (2) | 0.0269 (5) | |
| H5A | 1.0766 | 1.2360 | 0.6300 | 0.032* | |
| H5B | 1.1947 | 1.1420 | 0.7403 | 0.032* | |
| C6 | 0.8776 (3) | 1.1420 (2) | 0.7452 (2) | 0.0220 (5) | |
| C7 | 0.9014 (4) | 1.2512 (2) | 0.8558 (2) | 0.0262 (5) | |
| H7A | 1.0348 | 1.2372 | 0.9079 | 0.031* | |
| H7B | 0.9008 | 1.3459 | 0.8186 | 0.031* | |
| C8 | 0.7305 (4) | 1.2420 (2) | 0.9442 (2) | 0.0267 (5) | |
| H8A | 0.5973 | 1.2638 | 0.8945 | 0.032* | |
| H8B | 0.7565 | 1.3112 | 1.0137 | 0.032* | |
| C9 | 0.7245 (3) | 1.0926 (2) | 1.0020 (2) | 0.0225 (4) | |
| H9 | 0.8596 | 1.0737 | 1.0527 | 0.027* | |
| C10 | 0.6895 (3) | 0.9817 (2) | 0.89272 (19) | 0.0208 (4) | |
| H10A | 0.6867 | 0.8871 | 0.9298 | 0.025* | |
| H10B | 0.5572 | 0.9987 | 0.8402 | 0.025* | |
| C11 | 0.6816 (3) | 0.8367 (3) | 0.6205 (2) | 0.0281 (5) | |
| H11A | 0.5633 | 0.8342 | 0.6674 | 0.042* | |
| H11B | 0.6942 | 0.7472 | 0.5776 | 0.042* | |
| H11C | 0.6643 | 0.9114 | 0.5570 | 0.042* | |
| C12 | 0.6859 (4) | 1.1824 (3) | 0.6488 (2) | 0.0291 (5) | |
| H12A | 0.6890 | 1.1314 | 0.5688 | 0.044* | |
| H12B | 0.6873 | 1.2827 | 0.6321 | 0.044* | |
| H12C | 0.5619 | 1.1581 | 0.6854 | 0.044* | |
| C13 | 0.5607 (4) | 1.0824 (2) | 1.0919 (2) | 0.0254 (5) | |
| C14 | 0.6262 (4) | 1.0246 (3) | 1.2248 (2) | 0.0365 (6) | |
| H14A | 0.5094 | 1.0239 | 1.2732 | 0.055* | |
| H14B | 0.7341 | 1.0832 | 1.2688 | 0.055* | |
| H14C | 0.6770 | 0.9293 | 1.2181 | 0.055* | |
| O1 | 0.9229 (2) | 0.73764 (16) | 0.79125 (15) | 0.0258 (4) | |
| O2 | 0.3823 (3) | 1.1216 (2) | 1.05879 (17) | 0.0368 (4) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0181 (9) | 0.0150 (9) | 0.0221 (10) | 0.0001 (7) | 0.0013 (7) | 0.0000 (7) |
| C2 | 0.0234 (11) | 0.0173 (9) | 0.0236 (10) | 0.0027 (8) | 0.0035 (8) | 0.0001 (8) |
| C3 | 0.0265 (11) | 0.0247 (11) | 0.0283 (11) | 0.0026 (8) | 0.0079 (8) | −0.0005 (9) |
| C4 | 0.0300 (11) | 0.0311 (12) | 0.0299 (11) | −0.0018 (9) | 0.0119 (9) | 0.0033 (9) |
| C5 | 0.0256 (11) | 0.0237 (11) | 0.0322 (11) | −0.0027 (8) | 0.0065 (8) | 0.0053 (9) |
| C6 | 0.0200 (10) | 0.0188 (10) | 0.0269 (10) | −0.0005 (7) | 0.0017 (7) | 0.0025 (8) |
| C7 | 0.0299 (11) | 0.0163 (10) | 0.0319 (11) | −0.0033 (8) | 0.0016 (9) | −0.0003 (8) |
| C8 | 0.0308 (11) | 0.0180 (10) | 0.0309 (11) | 0.0017 (9) | 0.0024 (9) | −0.0025 (8) |
| C9 | 0.0258 (10) | 0.0185 (10) | 0.0229 (10) | 0.0003 (8) | 0.0026 (8) | −0.0020 (7) |
| C10 | 0.0236 (10) | 0.0149 (9) | 0.0241 (10) | 0.0001 (8) | 0.0040 (7) | −0.0014 (7) |
| C11 | 0.0253 (11) | 0.0266 (11) | 0.0321 (11) | −0.0011 (8) | 0.0024 (9) | −0.0068 (9) |
| C12 | 0.0298 (12) | 0.0263 (11) | 0.0304 (11) | 0.0037 (9) | 0.0003 (9) | 0.0055 (9) |
| C13 | 0.0325 (12) | 0.0149 (9) | 0.0296 (11) | 0.0006 (8) | 0.0070 (8) | −0.0058 (8) |
| C14 | 0.0463 (14) | 0.0321 (13) | 0.0324 (12) | −0.0030 (11) | 0.0097 (10) | 0.0025 (10) |
| O1 | 0.0279 (8) | 0.0172 (7) | 0.0341 (8) | 0.0036 (6) | 0.0103 (6) | 0.0028 (6) |
| O2 | 0.0336 (9) | 0.0360 (10) | 0.0429 (9) | 0.0095 (7) | 0.0132 (7) | 0.0005 (8) |
Geometric parameters (Å, °)
| C1—C10 | 1.530 (3) | C8—C9 | 1.530 (3) |
| C1—C2 | 1.545 (3) | C8—H8A | 0.9700 |
| C1—C6 | 1.560 (3) | C8—H8B | 0.9700 |
| C1—H1 | 0.9800 | C9—C13 | 1.503 (3) |
| C2—O1 | 1.436 (3) | C9—C10 | 1.535 (3) |
| C2—C11 | 1.529 (3) | C9—H9 | 0.9800 |
| C2—C3 | 1.532 (3) | C10—H10A | 0.9700 |
| C3—C4 | 1.521 (3) | C10—H10B | 0.9700 |
| C3—H3A | 0.9700 | C11—H11A | 0.9600 |
| C3—H3B | 0.9700 | C11—H11B | 0.9600 |
| C4—C5 | 1.524 (3) | C11—H11C | 0.9600 |
| C4—H4A | 0.9700 | C12—H12A | 0.9600 |
| C4—H4B | 0.9700 | C12—H12B | 0.9600 |
| C5—C6 | 1.536 (3) | C12—H12C | 0.9600 |
| C5—H5A | 0.9700 | C13—O2 | 1.222 (3) |
| C5—H5B | 0.9700 | C13—C14 | 1.493 (3) |
| C6—C7 | 1.533 (3) | C14—H14A | 0.9600 |
| C6—C12 | 1.541 (3) | C14—H14B | 0.9600 |
| C7—C8 | 1.528 (3) | C14—H14C | 0.9600 |
| C7—H7A | 0.9700 | O1—H2 | 0.85 (3) |
| C7—H7B | 0.9700 | ||
| C10—C1—C2 | 114.14 (16) | H7A—C7—H7B | 107.7 |
| C10—C1—C6 | 112.18 (15) | C7—C8—C9 | 110.07 (17) |
| C2—C1—C6 | 115.90 (15) | C7—C8—H8A | 109.6 |
| C10—C1—H1 | 104.3 | C9—C8—H8A | 109.6 |
| C2—C1—H1 | 104.3 | C7—C8—H8B | 109.6 |
| C6—C1—H1 | 104.3 | C9—C8—H8B | 109.6 |
| O1—C2—C11 | 107.93 (18) | H8A—C8—H8B | 108.2 |
| O1—C2—C3 | 103.02 (16) | C13—C9—C8 | 110.87 (17) |
| C11—C2—C3 | 112.14 (17) | C13—C9—C10 | 111.32 (17) |
| O1—C2—C1 | 109.18 (15) | C8—C9—C10 | 110.12 (16) |
| C11—C2—C1 | 115.19 (16) | C13—C9—H9 | 108.1 |
| C3—C2—C1 | 108.64 (17) | C8—C9—H9 | 108.1 |
| C4—C3—C2 | 113.69 (17) | C10—C9—H9 | 108.1 |
| C4—C3—H3A | 108.8 | C1—C10—C9 | 109.28 (15) |
| C2—C3—H3A | 108.8 | C1—C10—H10A | 109.8 |
| C4—C3—H3B | 108.8 | C9—C10—H10A | 109.8 |
| C2—C3—H3B | 108.8 | C1—C10—H10B | 109.8 |
| H3A—C3—H3B | 107.7 | C9—C10—H10B | 109.8 |
| C3—C4—C5 | 110.96 (17) | H10A—C10—H10B | 108.3 |
| C3—C4—H4A | 109.4 | C2—C11—H11A | 109.5 |
| C5—C4—H4A | 109.4 | C2—C11—H11B | 109.5 |
| C3—C4—H4B | 109.4 | H11A—C11—H11B | 109.5 |
| C5—C4—H4B | 109.4 | C2—C11—H11C | 109.5 |
| H4A—C4—H4B | 108.0 | H11A—C11—H11C | 109.5 |
| C4—C5—C6 | 113.21 (17) | H11B—C11—H11C | 109.5 |
| C4—C5—H5A | 108.9 | C6—C12—H12A | 109.5 |
| C6—C5—H5A | 108.9 | C6—C12—H12B | 109.5 |
| C4—C5—H5B | 108.9 | H12A—C12—H12B | 109.5 |
| C6—C5—H5B | 108.9 | C6—C12—H12C | 109.5 |
| H5A—C5—H5B | 107.7 | H12A—C12—H12C | 109.5 |
| C7—C6—C5 | 108.80 (16) | H12B—C12—H12C | 109.5 |
| C7—C6—C12 | 108.44 (18) | O2—C13—C14 | 121.2 (2) |
| C5—C6—C12 | 109.67 (17) | O2—C13—C9 | 121.8 (2) |
| C7—C6—C1 | 107.52 (17) | C14—C13—C9 | 117.03 (19) |
| C5—C6—C1 | 107.90 (16) | C13—C14—H14A | 109.5 |
| C12—C6—C1 | 114.38 (18) | C13—C14—H14B | 109.5 |
| C8—C7—C6 | 113.48 (17) | H14A—C14—H14B | 109.5 |
| C8—C7—H7A | 108.9 | C13—C14—H14C | 109.5 |
| C6—C7—H7A | 108.9 | H14A—C14—H14C | 109.5 |
| C8—C7—H7B | 108.9 | H14B—C14—H14C | 109.5 |
| C6—C7—H7B | 108.9 | C2—O1—H2 | 113 (2) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1—H2···O2i | 0.84 (3) | 2.05 (3) | 2.883 (2) | 169 (3) |
Symmetry codes: (i) −x+1, y−1/2, −z+2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FJ2393).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811004454/fj2393sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004454/fj2393Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


