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ISSN: 2414-3146

rac,endo-9-Hy­dr­oxy-9-methyl­tri­cyclo­[5.2.2.02,6]undeca-4,10-dien-8-one

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aUniversity of Mainz, Department of Chemistry, Duesbergweg 10-14, 55099 Mainz, Germany
*Correspondence e-mail: [email protected]

Edited by M. Bolte, Goethe-Universität Frankfurt, Germany (Received 24 August 2026; accepted 25 August 2026; online 28 August 2026)

The tricyclic mol­ecule of the title compound, C12H14O2, is composed of four nearly planar subunits. Hydrogen bonds connect the ketol units to chains along the a-axis direction. The structure is further consolidated by two C—H⋯O hydrogen bonds, one to the carbonyl and one to the hy­droxy group.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

The title compound, C12H14O2 (Fig. 1[link]), was prepared in a project on tricyclic frameworks (Detert & Schollmeyer, 2020View full citation; Schollmeyer & Detert, 2025View full citation, 2026View full citation). The synthesis was performed in a Diels–Alder cyclo­addition of o-quinolacetate and cyclo­penta­diene followed by hydrolysis. The tricyclic mol­ecule is composed of a [2.2.2] propellane with an annulated cyclo­pentene. The nearly C3-symmetrical carbon framework of the propellane is composed of three C2 bridges, these are essentially coplanar with the bridgehead carbons C2, C5. Subunit C2–C1–C6–C5 is planar within 0.0284 (9) Å and subtends a dihedral angle of 58.54 (14)° with the unit C2–C10–C11–C5. The latter is planar within 0.006 (2) Å and the dihedral angle to the planar unit C2–C3–C4–C5 (max. deviation: 0.0032 Å) amounts to 58.09 (15)°. The third angle is slightly larger, 63.38 (14)°. The endo-configuration is proven by the dihedral angle between the planar cyclo­pentene [max. deviation 0.010 (2) Å] and the vinyl­ene bridge C2–C10–C11–C5 of 63.14 (14)°. Four mol­ecules fill the unit cell: they are symmetrically connected via a twofold screw axis parallel to the a-axis and physically via hydrogen bonds. The O1—H1O⋯O2 hydrogen bonds (Table 1[link], Fig. 2[link]) connect the mol­ecules into chains along the a-axis direction, and additional C—H⋯O inter­actions link the chains into ribbons.

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1O⋯O2i 0.85 (3) 1.99 (3) 2.809 (2) 162 (3)
C5—H5⋯O2ii 1.00 2.52 3.407 (3) 148
C9—H9⋯O1iii 0.95 2.55 3.450 (3) 159
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation.
[Figure 1]
Figure 1
View of the title compound. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 2]
Figure 2
Part of the packing diagram. Hydrogen bonds are shown as dashed lines. View along the c-axis direction. Hydrogen atoms not involved in hydrogen bonds are omitted for clarity. Symmetry-related mol­ecules are shown in different colors.

Synthesis and crystallization

The synthesis was performed via Diels–Alder reaction of 1.10 g (6.62 mmol) 2-methyl-o-quinolacetate (Wessely & Sinwel, 1950View full citation) in 10 ml xylenes by dropwise addition of 0.46 g (1.05 eq) cyclo­penta­diene in 1.5 ml xylenes. The mixture was refluxed for 18 h while the color changed from yellow to orange and crystals separated. The solvent was distilled off, the residue was added to a mixture of 10 ml 1 M sodium hydroxide in water and 1 ml of methanol. After 16 h, the mixture was heated to 333 K until a brown compound separated. The mixture was acidulated, the precipitate was again dissolved in sodium hydroxide/methanol and reprecipitated by addition of hydro­chloric acid. Single crystals were grown by slow evaporation of a solution of 60 mg of the precipitate in ether. After filtration through cotton, petroleum ether was added until the solution became turbid and again washed with ether. The now clear solution slowly evaporated and single crystals were collected mechanically from the partially coloured mixture. Yield 22 mg of colourless crystals with m.p. 399-402 K. Literature: 68% yield, m.p. 399-401 K. (Metlesics et al., 1958View full citation). IR (ATR): ñ (cm−1): 3403 s, 3048w, 2983w, 2965w, 2935w, 2918w, 2895w, 2876m, 2845w, 1717vs, 1619w, 1441, 1386m, 1364m, 1355m, 1301s, 1264vw, 1234w, 1200w, 1151s, 1138s, 1112s, 1090m, 1050, 1014s, 975m, 948m, 925w, 892s, 853m, 790m, 778m, 750s, 731m, 708vs, 675s, 650w, 582vs, 499s; 1H-NMR (400 MHz, CDCl3): 6.37-6.24 (m, 1H, H8), 6.13-6.01 (m, 1H, H-11), 5.70 (dq, 3J = 5.7 Hz, 4J = 2.2 Hz, 1H, H-4), 5.44 (ddd, 3J = 5.8 Hz, 3J = 3.2 Hz, 4J = 1.5 Hz, 1H, H-5), 3.30-3.15 (m, 3H, H-2,-6,-7,), 3.00 (dt, 3J = 6.7 Hz, 4J = 2.2 Hz, 1H, H-1), 2.63-2.50 (m, 2H), 2.06-1.93 (m, 1H), 1.28 (s, 3H, CH3). Annotation of NMR signals follows IUPAC nomenclature.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. The structure was refined as a racemic twin.

Table 2
Experimental details

Crystal data
Chemical formula C12H14O2
Mr 190.23
Crystal system, space group Orthorhombic, P212121
Temperature (K) 120
a, b, c (Å) 7.3829 (3), 10.7318 (3), 12.2961 (4)
V3) 974.24 (6)
Z 4
Radiation type Cu Kα
μ (mm−1) 0.70
Crystal size (mm) 0.56 × 0.25 × 0.24
 
Data collection
Diffractometer Stoe Stadivari
No. of measured, independent and observed [I > 2σ(I)] reflections 5863, 1798, 1754
Rint 0.019
(sin θ/λ)max−1) 0.607
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.033, 0.091, 1.12
No. of reflections 1798
No. of parameters 134
H-atom treatment H atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3) 0.30, −0.14
Absolute structure Refined as an inversion twin
Absolute structure parameter 0.5 (3)
Computer programs: X-AREA WinXpose, X-AREA Recipe and X-AREA Integrate (Stoe & Cie, 2020View full citation), SHELXT2014 (Sheldrick, 2015aView full citation), SHELXL2019/2 (Sheldrick, 2015bView full citation) and PLATON (Spek, 2009View full citation).

Structural data


Computing details top

rac,endo-9-Hydroxy-9-methyltricyclo[5.2.2.02,6]undeca-4,10-dien-8-one top
Crystal data top
C12H14O2Dx = 1.297 Mg m3
Mr = 190.23Cu Kα radiation, λ = 1.54178 Å
Orthorhombic, P212121Cell parameters from 11043 reflections
a = 7.3829 (3) Åθ = 3.6–69.9°
b = 10.7318 (3) ŵ = 0.70 mm1
c = 12.2961 (4) ÅT = 120 K
V = 974.24 (6) Å3Block, colorless
Z = 40.56 × 0.25 × 0.24 mm
F(000) = 408
Data collection top
Stoe Stadivari
diffractometer
1754 reflections with I > 2σ(I)
Radiation source: microfocus tubeRint = 0.019
Detector resolution: 13.33 pixels mm-1θmax = 69.5°, θmin = 5.5°
rotation method, ω scansh = 88
5863 measured reflectionsk = 1311
1798 independent reflectionsl = 1414
Refinement top
Refinement on F2H atoms treated by a mixture of independent and constrained refinement
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0498P)2 + 0.2628P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.033(Δ/σ)max < 0.001
wR(F2) = 0.091Δρmax = 0.30 e Å3
S = 1.12Δρmin = 0.14 e Å3
1798 reflectionsExtinction correction: SHELXL2019/2 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
134 parametersExtinction coefficient: 0.027 (2)
0 restraintsAbsolute structure: Refined as an inversion twin
Primary atom site location: dualAbsolute structure parameter: 0.5 (3)
Hydrogen site location: mixed
Special details top

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. Refined as a 2-component inversion twin. The hydroxyl H atom was freely refined. Hydrogen atoms attached to carbons were placed at calculated positions and were refined in the riding-model approximation with Ctertiary–H = 1.00 Å, Csecondary–H = 0.99 Å, Cmethyl–H = 0.98 Å, Csp2–H = 0.95 Å, and with Uiso(H) = 1.5 Ueq(Cmethyl) or with Uiso(H) = 1.2 Ueq(C) for the remaining H atoms. The methyl group was allowed to rotate but not to tip.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.2635 (2)0.40578 (15)0.39744 (12)0.0250 (4)
H1O0.210 (4)0.346 (3)0.429 (2)0.044 (9)*
O20.5241 (2)0.27907 (14)0.52851 (13)0.0278 (4)
C10.3673 (3)0.46715 (19)0.47879 (17)0.0224 (5)
C20.4350 (3)0.5909 (2)0.43046 (17)0.0240 (5)
H20.3312300.6477130.4140500.029*
C30.5447 (3)0.56246 (19)0.32649 (17)0.0232 (5)
H30.4663780.5165110.2736510.028*
C40.7112 (3)0.4804 (2)0.35644 (16)0.0230 (5)
H40.7064490.3998430.3157080.028*
C50.7129 (3)0.45495 (18)0.48239 (16)0.0227 (5)
H50.8202560.4048310.5056970.027*
C60.5363 (3)0.38798 (19)0.50245 (15)0.0217 (5)
C70.6217 (3)0.6810 (2)0.27121 (19)0.0291 (5)
H7A0.5787510.6877410.1951580.035*
H7B0.5852960.7569030.3114090.035*
C80.8233 (3)0.6633 (2)0.27516 (18)0.0294 (5)
H80.9074990.7228080.2485440.035*
C90.8712 (3)0.5560 (2)0.31960 (18)0.0280 (5)
H90.9933640.5295700.3273630.034*
C100.5610 (3)0.64894 (19)0.51272 (18)0.0252 (5)
H100.5409610.7293780.5426660.030*
C110.7019 (3)0.5787 (2)0.53996 (17)0.0248 (5)
H110.7894730.6046300.5918910.030*
C120.2556 (3)0.4843 (2)0.58199 (18)0.0295 (5)
H12A0.1448340.5306090.5648300.044*
H12B0.3266310.5308350.6357100.044*
H12C0.2236180.4025260.6117830.044*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0209 (8)0.0261 (8)0.0279 (8)0.0035 (6)0.0034 (6)0.0023 (6)
O20.0274 (8)0.0234 (8)0.0325 (8)0.0008 (6)0.0017 (7)0.0033 (6)
C10.0192 (10)0.0224 (10)0.0255 (10)0.0013 (8)0.0007 (8)0.0000 (8)
C20.0202 (10)0.0216 (10)0.0302 (11)0.0021 (8)0.0001 (8)0.0002 (9)
C30.0201 (10)0.0262 (11)0.0231 (10)0.0008 (8)0.0030 (8)0.0018 (8)
C40.0217 (10)0.0251 (10)0.0223 (10)0.0015 (9)0.0004 (8)0.0020 (8)
C50.0183 (10)0.0246 (10)0.0252 (10)0.0019 (8)0.0016 (8)0.0013 (8)
C60.0224 (10)0.0252 (11)0.0174 (9)0.0005 (9)0.0010 (8)0.0010 (8)
C70.0291 (12)0.0288 (11)0.0294 (11)0.0026 (9)0.0015 (9)0.0048 (9)
C80.0268 (12)0.0379 (13)0.0236 (10)0.0081 (10)0.0019 (9)0.0009 (9)
C90.0213 (11)0.0389 (13)0.0237 (10)0.0015 (9)0.0037 (9)0.0026 (9)
C100.0250 (10)0.0242 (10)0.0265 (11)0.0030 (9)0.0042 (8)0.0037 (8)
C110.0241 (10)0.0279 (11)0.0223 (10)0.0054 (8)0.0000 (8)0.0014 (8)
C120.0260 (11)0.0326 (12)0.0301 (11)0.0018 (9)0.0058 (9)0.0019 (9)
Geometric parameters (Å, º) top
O1—C11.422 (3)C5—C111.508 (3)
O1—H1O0.85 (3)C5—C61.509 (3)
O2—C61.215 (3)C5—H51.0000
C1—C121.524 (3)C7—C81.501 (3)
C1—C61.538 (3)C7—H7A0.9900
C1—C21.538 (3)C7—H7B0.9900
C2—C101.509 (3)C8—C91.323 (3)
C2—C31.544 (3)C8—H80.9500
C2—H21.0000C9—H90.9500
C3—C71.550 (3)C10—C111.328 (3)
C3—C41.556 (3)C10—H100.9500
C3—H31.0000C11—H110.9500
C4—C91.503 (3)C12—H12A0.9800
C4—C51.573 (3)C12—H12B0.9800
C4—H41.0000C12—H12C0.9800
C1—O1—H1O106 (2)C6—C5—H5112.5
O1—C1—C12110.50 (17)C4—C5—H5112.5
O1—C1—C6108.33 (16)O2—C6—C5124.45 (19)
C12—C1—C6110.38 (17)O2—C6—C1121.39 (19)
O1—C1—C2107.65 (16)C5—C6—C1114.02 (16)
C12—C1—C2113.15 (17)C8—C7—C3104.18 (18)
C6—C1—C2106.63 (16)C8—C7—H7A110.9
C10—C2—C1107.33 (17)C3—C7—H7A110.9
C10—C2—C3108.26 (18)C8—C7—H7B110.9
C1—C2—C3108.67 (17)C3—C7—H7B110.9
C10—C2—H2110.8H7A—C7—H7B108.9
C1—C2—H2110.8C9—C8—C7112.9 (2)
C3—C2—H2110.8C9—C8—H8123.5
C2—C3—C7113.16 (18)C7—C8—H8123.5
C2—C3—C4109.28 (17)C8—C9—C4112.6 (2)
C7—C3—C4106.19 (18)C8—C9—H9123.7
C2—C3—H3109.4C4—C9—H9123.7
C7—C3—H3109.4C11—C10—C2114.70 (19)
C4—C3—H3109.4C11—C10—H10122.7
C9—C4—C3104.15 (17)C2—C10—H10122.7
C9—C4—C5112.61 (18)C10—C11—C5115.05 (19)
C3—C4—C5109.73 (17)C10—C11—H11122.5
C9—C4—H4110.1C5—C11—H11122.5
C3—C4—H4110.1C1—C12—H12A109.5
C5—C4—H4110.1C1—C12—H12B109.5
C11—C5—C6107.27 (16)H12A—C12—H12B109.5
C11—C5—C4107.98 (16)C1—C12—H12C109.5
C6—C5—C4103.71 (16)H12A—C12—H12C109.5
C11—C5—H5112.5H12B—C12—H12C109.5
O1—C1—C2—C10174.12 (16)C11—C5—C6—C149.8 (2)
C12—C1—C2—C1063.5 (2)C4—C5—C6—C164.3 (2)
C6—C1—C2—C1058.0 (2)O1—C1—C6—O255.1 (2)
O1—C1—C2—C357.2 (2)C12—C1—C6—O266.0 (2)
C12—C1—C2—C3179.65 (18)C2—C1—C6—O2170.69 (18)
C6—C1—C2—C358.8 (2)O1—C1—C6—C5120.74 (18)
C10—C2—C3—C763.2 (2)C12—C1—C6—C5118.15 (19)
C1—C2—C3—C7179.44 (17)C2—C1—C6—C55.1 (2)
C10—C2—C3—C454.9 (2)C2—C3—C7—C8118.3 (2)
C1—C2—C3—C461.4 (2)C4—C3—C7—C81.6 (2)
C2—C3—C4—C9121.26 (19)C3—C7—C8—C91.6 (3)
C7—C3—C4—C91.1 (2)C7—C8—C9—C41.0 (3)
C2—C3—C4—C50.5 (2)C3—C4—C9—C80.1 (2)
C7—C3—C4—C5121.89 (18)C5—C4—C9—C8119.0 (2)
C9—C4—C5—C1162.1 (2)C1—C2—C10—C1158.2 (2)
C3—C4—C5—C1153.4 (2)C3—C2—C10—C1158.9 (2)
C9—C4—C5—C6175.74 (17)C2—C10—C11—C51.1 (3)
C3—C4—C5—C660.2 (2)C6—C5—C11—C1055.4 (2)
C11—C5—C6—O2134.5 (2)C4—C5—C11—C1055.8 (2)
C4—C5—C6—O2111.4 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1O···O2i0.85 (3)1.99 (3)2.809 (2)162 (3)
C5—H5···O2ii1.002.523.407 (3)148
C9—H9···O1iii0.952.553.450 (3)159
Symmetry codes: (i) x1/2, y+1/2, z+1; (ii) x+1/2, y+1/2, z+1; (iii) x+1, y, z.
 

References

Return to citationDetert, H. & Schollmeyer, D. (2020). IUCrData 5, x201585.  Google Scholar
Return to citationMetlesics, W., Wessely, F. & Budzikiewicz, H. (1958). Monatsh. Chem. 89, 102–109.  CrossRef CAS Google Scholar
Return to citationSchollmeyer, D. & Detert, H. (2025). IUCrData 10, x251132.  Google Scholar
Return to citationSchollmeyer, D. & Detert, H. (2026). IUCrData 11, x260499.  Google Scholar
Return to citationSheldrick, G. M. (2015a). Acta Cryst. A71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSheldrick, G. M. (2015b). Acta Cryst. C71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSpek, A. L. (2009). Acta Cryst. D65, 148–155.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationStoe & Cie (2020). X-AREA WinXpose, X-AREA Recipe and X-AREA Integrate. Stoe & Cie, Darmstadt, Germany.  Google Scholar
Return to citationWessely, F. & Sinwel, F. (1950). Monatsh. Chem. 81, 1055–1070.  CrossRef CAS Google Scholar

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