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The title compound, C24H30O5, has been redetermined at 173 K. In contrast to the structure determination of Tu et al. [Chin. J. Struct. Chem. (Jiegou Huaxue) (1998), 17, 409-412] at room temperature, we were able to locate all H atoms. There is an intermolecular hydrogen bond between the hydroxyl group and the carbonyl O atom of the cyclo­hexenone ring.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680100160X/na6041sup1.cif
Contains datablocks rd8, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680100160X/na6041Isup2.hkl
Contains datablock I

CCDC reference: 159758

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.041
  • wR factor = 0.111
  • Data-to-parameter ratio = 18.0

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry
Yellow Alert Alert Level C:
PLAT_601 Alert C Structure contains solvent accessible VOIDS of 34.00 A   3
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

The title compound, (I), was synthesized in the course of a search for twinned crystal structures (Bolte et al., 1997, 2001b; Bolte & Scholtyssik, 1997). These compounds can easily be prepared (Hünig et al., 1979). We hoped to find more twinned crystal structures in order to understand why some of these simple compounds containing the common bis-dimedone skeleton are twinned. Unfortunately, neither any of these nor the title compound turned out to be twinned. Whereas the reaction of dimedone with 2,6-dichlorobenzaldehyde leads to four stereoisomers (two enantiomeric pairs of diastereomers) of 3,3,6,6-tetramethyl-4a-hydroxy-9-(2,6-dichlorophenyl)-1,8-dioxo- 2,3,4,4a,5,6,7,8,9,9a-decahydro-1H-xanthene which can all be found in the same crystal (Bolte et al., 2001a), the crystals of the title compound just contain two stereomers. The conformation of the cyclohexane ring can be described as a chair. The other two rings display an approximate sofa conformation with five atoms in a common plane and one atom [C14 0.653 (2) Å; C21 0.592 (2) Å] deviating from this plane. The crystal packing is stabilized by a hydrogen bond between the hydroxyl group and the carbonyl group attached to the cyclohexene ring of an adjacent molecule translated along y. The crystal structure of the title compound agrees well with the structure of Tu et al. (1998) recently determined at room temperature, however, we have also determined the positions of the H atoms, including the hydroxyl group.

Experimental top

The title compound was synthesized according to Cremlyn & Saunders (1993).

Refinement top

All H atoms were located by difference Fourier synthesis and refined with fixed individual displacement parameters [U(H) = 1.5Ueq(Cmethyl), U(H) = 1.2Ueq(C) or U(H) = 1.2Ueq(O)] using a riding model with O—H = 0.84, C—H(aromatic) = 0.95, CH(methyl) = 0.98, C—H(secondary) = 0.99 or C—H(tertiary) = 1.00 Å. Additionally the torsion angle about the C—O bond of the hydroxyl group was refined.

Computing details top

Data collection: SMART (Siemens, 1995); cell refinement: SMART; data reduction: SAINT (Siemens, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 1991).

Figures top
[Figure 1] Fig. 1. Perspective view of the title compound with the atom numbering; displacement ellipsoids are at the 50% probability level; Only tertiary and hydroxyl H atoms have been shown.
(rd8) top
Crystal data top
C24H30O5F(000) = 1712
Mr = 398.48Dx = 1.231 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 33.845 (4) ÅCell parameters from 7436 reflections
b = 7.214 (1) Åθ = 0–25°
c = 22.605 (3) ŵ = 0.09 mm1
β = 128.82 (1)°T = 173 K
V = 4300.1 (10) Å3Block, colourless
Z = 80.60 × 0.50 × 0.50 mm
Data collection top
Siemens CCD three-circle
diffractometer
4750 independent reflections
Radiation source: fine-focus sealed tube4193 reflections with I > 2σs(I)
Graphite monochromatorRint = 0.024
ω scansθmax = 27.1°, θmin = 1.5°
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
h = 4343
Tmin = 0.951, Tmax = 0.959k = 99
39326 measured reflectionsl = 2828
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.041Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.111H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0558P)2 + 3.6403P]
where P = (Fo2 + 2Fc2)/3
4750 reflections(Δ/σ)max < 0.001
264 parametersΔρmax = 0.34 e Å3
0 restraintsΔρmin = 0.23 e Å3
Crystal data top
C24H30O5V = 4300.1 (10) Å3
Mr = 398.48Z = 8
Monoclinic, C2/cMo Kα radiation
a = 33.845 (4) ŵ = 0.09 mm1
b = 7.214 (1) ÅT = 173 K
c = 22.605 (3) Å0.60 × 0.50 × 0.50 mm
β = 128.82 (1)°
Data collection top
Siemens CCD three-circle
diffractometer
4750 independent reflections
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
4193 reflections with I > 2σs(I)
Tmin = 0.951, Tmax = 0.959Rint = 0.024
39326 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0410 restraints
wR(F2) = 0.111H atoms treated by a mixture of independent and constrained refinement
S = 1.04Δρmax = 0.34 e Å3
4750 reflectionsΔρmin = 0.23 e Å3
264 parameters
Special details top

Experimental. ;

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) top
xyzUiso*/Ueq
C10.12122 (4)0.66923 (16)0.04378 (6)0.0188 (2)
H10.11380.78840.01590.023*
C110.17833 (4)0.65689 (16)0.10174 (6)0.0200 (2)
C120.20475 (4)0.51162 (17)0.10450 (6)0.0201 (2)
O120.18343 (3)0.35659 (12)0.06152 (5)0.02137 (19)
C130.26153 (4)0.50279 (18)0.15320 (7)0.0246 (3)
H13A0.27080.43690.12510.030*
H13B0.27490.43010.19950.030*
C140.28656 (5)0.69446 (19)0.17659 (7)0.0263 (3)
C170.27656 (6)0.7943 (2)0.10856 (9)0.0406 (4)
H17A0.29280.91640.12450.061*
H17B0.23990.80950.06860.061*
H17C0.29050.72100.08900.061*
C180.34396 (5)0.6714 (2)0.23959 (9)0.0366 (3)
H18A0.36020.79360.25480.055*
H18B0.35800.59590.22070.055*
H18C0.35030.61000.28350.055*
C150.26359 (5)0.80402 (19)0.20666 (8)0.0281 (3)
H15A0.27300.74290.25310.034*
H15B0.27820.93040.22070.034*
C160.20637 (4)0.81829 (17)0.14927 (7)0.0212 (2)
O160.18464 (3)0.96186 (12)0.14399 (5)0.0268 (2)
C210.10176 (4)0.51451 (16)0.01524 (6)0.0193 (2)
H210.06490.49530.04140.023*
C220.12931 (4)0.32929 (16)0.02023 (6)0.0187 (2)
O220.12165 (3)0.27385 (12)0.07151 (5)0.02163 (19)
H220.13800.17600.09340.026*
C230.11263 (5)0.17950 (17)0.03909 (7)0.0216 (2)
H23A0.07830.13740.05980.026*
H23B0.13580.07230.01290.026*
C240.11117 (5)0.23308 (18)0.10672 (7)0.0256 (3)
C270.16458 (6)0.2393 (2)0.08351 (9)0.0346 (3)
H27A0.18500.33190.04340.052*
H27B0.16230.27270.12760.052*
H27C0.18060.11720.06470.052*
C280.07951 (6)0.0878 (2)0.16954 (8)0.0363 (3)
H28A0.04530.08310.18470.054*
H28B0.09560.03400.15060.054*
H28C0.07740.12160.21350.054*
C250.08516 (5)0.42429 (19)0.13828 (7)0.0297 (3)
H25A0.08950.46830.17540.036*
H25B0.04840.41150.16510.036*
C260.10745 (5)0.56471 (18)0.07526 (7)0.0243 (3)
O260.12935 (4)0.70318 (14)0.07108 (6)0.0354 (2)
C310.09319 (4)0.67912 (16)0.07631 (7)0.0200 (2)
C320.04118 (4)0.72515 (17)0.02731 (7)0.0223 (2)
O3210.02079 (3)0.75913 (13)0.04656 (5)0.0274 (2)
C3210.03313 (5)0.7844 (2)0.10058 (8)0.0314 (3)
H32A0.04320.79840.15150.047*
H32B0.04280.89580.08750.047*
H32C0.05020.67620.09960.047*
C330.01372 (5)0.73613 (18)0.05401 (8)0.0274 (3)
H330.02150.76290.02010.033*
C340.03847 (5)0.7076 (2)0.13078 (8)0.0304 (3)
H340.02000.71640.14940.036*
C350.08967 (5)0.66640 (19)0.18022 (8)0.0290 (3)
H350.10650.64850.23270.035*
C360.11644 (5)0.65137 (17)0.15230 (7)0.0242 (3)
H360.15150.62130.18630.029*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0164 (5)0.0183 (5)0.0206 (5)0.0020 (4)0.0110 (5)0.0019 (4)
C110.0173 (5)0.0219 (6)0.0210 (5)0.0005 (4)0.0122 (5)0.0015 (4)
C120.0186 (5)0.0227 (6)0.0195 (5)0.0002 (4)0.0121 (5)0.0007 (4)
O120.0167 (4)0.0210 (4)0.0254 (4)0.0014 (3)0.0128 (4)0.0011 (3)
C130.0171 (5)0.0272 (6)0.0279 (6)0.0026 (5)0.0133 (5)0.0009 (5)
C140.0180 (6)0.0301 (7)0.0296 (6)0.0024 (5)0.0143 (5)0.0038 (5)
C170.0353 (8)0.0478 (9)0.0471 (9)0.0042 (7)0.0299 (7)0.0063 (7)
C180.0181 (6)0.0434 (8)0.0398 (8)0.0029 (6)0.0140 (6)0.0114 (6)
C150.0185 (6)0.0304 (7)0.0277 (6)0.0010 (5)0.0108 (5)0.0071 (5)
C160.0203 (6)0.0230 (6)0.0212 (5)0.0003 (5)0.0134 (5)0.0009 (5)
O160.0254 (4)0.0223 (4)0.0286 (5)0.0029 (3)0.0149 (4)0.0006 (4)
C210.0171 (5)0.0209 (6)0.0193 (5)0.0025 (4)0.0111 (4)0.0020 (4)
C220.0171 (5)0.0201 (5)0.0200 (5)0.0006 (4)0.0122 (5)0.0014 (4)
O220.0242 (4)0.0228 (4)0.0220 (4)0.0037 (3)0.0165 (4)0.0048 (3)
C230.0230 (6)0.0203 (6)0.0224 (6)0.0008 (4)0.0147 (5)0.0002 (5)
C240.0315 (6)0.0260 (6)0.0232 (6)0.0030 (5)0.0190 (6)0.0013 (5)
C270.0402 (8)0.0406 (8)0.0383 (8)0.0061 (6)0.0319 (7)0.0037 (6)
C280.0499 (9)0.0307 (7)0.0267 (7)0.0017 (6)0.0232 (7)0.0021 (6)
C250.0389 (7)0.0296 (7)0.0233 (6)0.0061 (6)0.0208 (6)0.0042 (5)
C260.0272 (6)0.0233 (6)0.0245 (6)0.0084 (5)0.0171 (5)0.0076 (5)
O260.0504 (6)0.0276 (5)0.0419 (6)0.0003 (4)0.0355 (5)0.0055 (4)
C310.0186 (5)0.0175 (5)0.0251 (6)0.0000 (4)0.0142 (5)0.0019 (4)
C320.0196 (6)0.0204 (6)0.0245 (6)0.0003 (4)0.0127 (5)0.0020 (4)
O3210.0164 (4)0.0352 (5)0.0243 (4)0.0052 (4)0.0097 (4)0.0033 (4)
C3210.0167 (6)0.0320 (7)0.0302 (7)0.0036 (5)0.0072 (5)0.0012 (5)
C330.0204 (6)0.0268 (6)0.0367 (7)0.0003 (5)0.0187 (6)0.0047 (5)
C340.0331 (7)0.0310 (7)0.0401 (7)0.0035 (5)0.0292 (6)0.0068 (6)
C350.0345 (7)0.0307 (7)0.0274 (6)0.0024 (5)0.0220 (6)0.0034 (5)
C360.0218 (6)0.0249 (6)0.0245 (6)0.0005 (5)0.0138 (5)0.0001 (5)
Geometric parameters (Å, º) top
C1—C111.5118 (15)C23—C241.5474 (17)
C1—C311.5233 (16)C23—H23A0.9900
C1—C211.5356 (16)C23—H23B0.9900
C1—H11.0000C24—C281.5346 (19)
C11—C121.3533 (17)C24—C271.5347 (19)
C11—C161.4602 (17)C24—C251.5490 (18)
C12—O121.3551 (14)C27—H27A0.9800
C12—C131.5021 (16)C27—H27B0.9800
O12—C221.4567 (13)C27—H27C0.9800
C13—C141.5322 (18)C28—H28A0.9800
C13—H13A0.9900C28—H28B0.9800
C13—H13B0.9900C28—H28C0.9800
C14—C171.531 (2)C25—C261.5091 (19)
C14—C151.5342 (18)C25—H25A0.9900
C14—C181.5366 (18)C25—H25B0.9900
C17—H17A0.9800C26—O261.2118 (16)
C17—H17B0.9800C31—C361.3840 (17)
C17—H17C0.9800C31—C321.4111 (16)
C18—H18A0.9800C32—O3211.3712 (15)
C18—H18B0.9800C32—C331.3918 (17)
C18—H18C0.9800O321—C3211.4356 (15)
C15—C161.5145 (16)C321—H32A0.9800
C15—H15A0.9900C321—H32B0.9800
C15—H15B0.9900C321—H32C0.9800
C16—O161.2322 (15)C33—C341.390 (2)
C21—C261.5284 (16)C33—H330.9500
C21—C221.5363 (16)C34—C351.382 (2)
C21—H211.0000C34—H340.9500
C22—O221.3956 (14)C35—C361.3957 (18)
C22—C231.5281 (16)C35—H350.9500
O22—H220.8400C36—H360.9500
C11—C1—C31115.42 (10)C22—C23—C24117.11 (10)
C11—C1—C21109.22 (9)C22—C23—H23A108.0
C31—C1—C21113.31 (9)C24—C23—H23A108.0
C11—C1—H1106.1C22—C23—H23B108.0
C31—C1—H1106.1C24—C23—H23B108.0
C21—C1—H1106.1H23A—C23—H23B107.3
C12—C11—C16118.53 (10)C28—C24—C27109.02 (11)
C12—C11—C1122.30 (11)C28—C24—C23108.36 (11)
C16—C11—C1118.61 (10)C27—C24—C23111.60 (11)
C11—C12—O12124.51 (10)C28—C24—C25108.44 (11)
C11—C12—C13124.84 (11)C27—C24—C25109.82 (11)
O12—C12—C13110.61 (10)C23—C24—C25109.53 (10)
C12—O12—C22117.48 (9)C24—C27—H27A109.5
C12—C13—C14113.03 (10)C24—C27—H27B109.5
C12—C13—H13A109.0H27A—C27—H27B109.5
C14—C13—H13A109.0C24—C27—H27C109.5
C12—C13—H13B109.0H27A—C27—H27C109.5
C14—C13—H13B109.0H27B—C27—H27C109.5
H13A—C13—H13B107.8C24—C28—H28A109.5
C17—C14—C13110.59 (11)C24—C28—H28B109.5
C17—C14—C15110.37 (12)H28A—C28—H28B109.5
C13—C14—C15107.07 (10)C24—C28—H28C109.5
C17—C14—C18109.68 (12)H28A—C28—H28C109.5
C13—C14—C18109.06 (11)H28B—C28—H28C109.5
C15—C14—C18110.03 (11)C26—C25—C24111.08 (10)
C14—C17—H17A109.5C26—C25—H25A109.4
C14—C17—H17B109.5C24—C25—H25A109.4
H17A—C17—H17B109.5C26—C25—H25B109.4
C14—C17—H17C109.5C24—C25—H25B109.4
H17A—C17—H17C109.5H25A—C25—H25B108.0
H17B—C17—H17C109.5O26—C26—C25123.11 (12)
C14—C18—H18A109.5O26—C26—C21122.51 (12)
C14—C18—H18B109.5C25—C26—C21114.35 (11)
H18A—C18—H18B109.5C36—C31—C32117.85 (11)
C14—C18—H18C109.5C36—C31—C1123.42 (10)
H18A—C18—H18C109.5C32—C31—C1118.70 (10)
H18B—C18—H18C109.5O321—C32—C33123.70 (11)
C16—C15—C14112.73 (10)O321—C32—C31115.20 (10)
C16—C15—H15A109.0C33—C32—C31121.10 (12)
C14—C15—H15A109.0C32—O321—C321117.35 (10)
C16—C15—H15B109.0O321—C321—H32A109.5
C14—C15—H15B109.0O321—C321—H32B109.5
H15A—C15—H15B107.8H32A—C321—H32B109.5
O16—C16—C11121.72 (11)O321—C321—H32C109.5
O16—C16—C15120.35 (11)H32A—C321—H32C109.5
C11—C16—C15117.93 (10)H32B—C321—H32C109.5
C26—C21—C1112.02 (10)C34—C33—C32119.28 (12)
C26—C21—C22107.24 (9)C34—C33—H33120.4
C1—C21—C22112.91 (9)C32—C33—H33120.4
C26—C21—H21108.2C35—C34—C33120.67 (12)
C1—C21—H21108.2C35—C34—H34119.7
C22—C21—H21108.2C33—C34—H34119.7
O22—C22—O12108.68 (9)C34—C35—C36119.41 (12)
O22—C22—C23111.56 (9)C34—C35—H35120.3
O12—C22—C23106.39 (9)C36—C35—H35120.3
O22—C22—C21108.35 (9)C31—C36—C35121.66 (12)
O12—C22—C21108.95 (9)C31—C36—H36119.2
C23—C22—C21112.81 (9)C35—C36—H36119.2
C22—O22—H22109.5
C31—C1—C11—C12119.68 (12)C26—C21—C22—C2351.88 (12)
C21—C1—C11—C129.34 (15)C1—C21—C22—C23175.76 (9)
C31—C1—C11—C1669.03 (14)O22—C22—C23—C24170.82 (10)
C21—C1—C11—C16161.95 (10)O12—C22—C23—C2470.80 (12)
C16—C11—C12—O12177.59 (10)C21—C22—C23—C2448.60 (14)
C1—C11—C12—O126.29 (18)C22—C23—C24—C28163.68 (11)
C16—C11—C12—C130.09 (18)C22—C23—C24—C2776.27 (14)
C1—C11—C12—C13171.21 (11)C22—C23—C24—C2545.56 (15)
C11—C12—O12—C2211.87 (16)C28—C24—C25—C26167.44 (11)
C13—C12—O12—C22170.33 (9)C27—C24—C25—C2673.52 (13)
C11—C12—C13—C1422.08 (17)C23—C24—C25—C2649.37 (14)
O12—C12—C13—C14155.71 (10)C24—C25—C26—O26117.29 (14)
C12—C13—C14—C1771.77 (14)C24—C25—C26—C2160.66 (14)
C12—C13—C14—C1548.52 (14)C1—C21—C26—O266.63 (16)
C12—C13—C14—C18167.54 (11)C22—C21—C26—O26117.79 (13)
C17—C14—C15—C1663.51 (15)C1—C21—C26—C25175.40 (10)
C13—C14—C15—C1656.92 (14)C22—C21—C26—C2560.18 (13)
C18—C14—C15—C16175.32 (11)C11—C1—C31—C369.33 (16)
C12—C11—C16—O16172.75 (11)C21—C1—C31—C36117.66 (12)
C1—C11—C16—O161.12 (17)C11—C1—C31—C32168.41 (11)
C12—C11—C16—C157.96 (17)C21—C1—C31—C3264.60 (14)
C1—C11—C16—C15179.58 (10)C36—C31—C32—O321177.19 (11)
C14—C15—C16—O16142.63 (12)C1—C31—C32—O3210.68 (16)
C14—C15—C16—C1138.06 (16)C36—C31—C32—C332.13 (18)
C11—C1—C21—C2680.52 (11)C1—C31—C32—C33180.00 (11)
C31—C1—C21—C26149.30 (10)C33—C32—O321—C3218.05 (18)
C11—C1—C21—C2240.68 (12)C31—C32—O321—C321172.64 (11)
C31—C1—C21—C2289.50 (11)O321—C32—C33—C34177.00 (12)
C12—O12—C22—O2275.24 (12)C31—C32—C33—C342.27 (19)
C12—O12—C22—C23164.51 (9)C32—C33—C34—C350.8 (2)
C12—O12—C22—C2142.63 (13)C33—C34—C35—C360.8 (2)
C26—C21—C22—O22175.90 (9)C32—C31—C36—C350.54 (18)
C1—C21—C22—O2260.23 (12)C1—C31—C36—C35178.30 (12)
C26—C21—C22—O1266.03 (11)C34—C35—C36—C310.9 (2)
C1—C21—C22—O1257.84 (12)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O22—H22···O16i0.841.982.814 (1)171
Symmetry code: (i) x, y1, z.

Experimental details

Crystal data
Chemical formulaC24H30O5
Mr398.48
Crystal system, space groupMonoclinic, C2/c
Temperature (K)173
a, b, c (Å)33.845 (4), 7.214 (1), 22.605 (3)
β (°) 128.82 (1)
V3)4300.1 (10)
Z8
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.60 × 0.50 × 0.50
Data collection
DiffractometerSiemens CCD three-circle
diffractometer
Absorption correctionEmpirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.951, 0.959
No. of measured, independent and
observed [I > 2σs(I)] reflections
39326, 4750, 4193
Rint0.024
(sin θ/λ)max1)0.641
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.041, 0.111, 1.04
No. of reflections4750
No. of parameters264
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.34, 0.23

Computer programs: SMART (Siemens, 1995), SMART, SAINT (Siemens, 1995), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), XP in SHELXTL-Plus (Sheldrick, 1991).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O22—H22···O16i0.841.982.814 (1)171
Symmetry code: (i) x, y1, z.
 

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