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Presented here are the synthesis, characterization and study (using single crystal X-ray diffraction, Raman scattering, quantum mechanics calculations) of the structures of a series of bi­phenyls substituted in positions 3, 3′, 4 and 4′ with a variety of R (R = methyl, acetyl, hexyl) groups connected to the bi­phenyl core through oxygen atoms. The molecular conformation, particularly the torsion angle between aromatic rings has been extensively studied both in the solid as well as in the liquid state. The results show that the compounds appearing as rigorously planar in the solid present instead a twisted conformation in the melt. The solid versus melt issue strongly suggests that the reasons for planarity are to be found in the packing restraints. A `rule of thumb' is suggested for the design of biphenyls with different molecular conformations, based on the selection of the OR substituent.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520620004102/lo5065sup1.cif
Contains datablocks I, II, IV, Vb

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520620004102/lo5065Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520620004102/lo5065IIsup3.hkl
Contains datablock II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520620004102/lo5065IVsup4.hkl
Contains datablock IV

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520620004102/lo5065Vbsup5.hkl
Contains datablock Vb

txt

Text file https://doi.org/10.1107/S2052520620004102/lo5065sup6.txt
Crystallographic data for III and Va (already deposited in the CSD) with atom labels adapted to the present MS

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520620004102/lo5065sup7.pdf
Experimental and QM computational data

CCDC references: 1992376; 1992377; 1992378; 1992379

Computing details top

Data collection: Bruker APEX2 for (I), (IV); CrysAlis PRO (Oxford Diffraction, 2009) for (II), (Vb). Cell refinement: Bruker SAINT for (I), (IV); CrysAlis PRO for (II), (Vb). Data reduction: Bruker SAINT for (I), (IV); CrysAlis PRO for (II), (Vb). For all structures, program(s) used to solve structure: SHELXS97 (Sheldrick 2008). Program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015) for (I), (IV); SHELXL2018/1 (Sheldrick, 2015) for (II), (Vb). For all structures, molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL2018, PLATON (Spek, 2009).

(I) top
Crystal data top
C36H58O4F(000) = 612
Mr = 554.82Dx = 1.109 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 22.486 (2) ÅCell parameters from 8395 reflections
b = 8.8585 (9) Åθ = 2.5–30.2°
c = 8.3874 (8) ŵ = 0.07 mm1
β = 96.221 (3)°T = 150 K
V = 1660.8 (3) Å3Fragment, colourless
Z = 20.22 × 0.16 × 0.12 mm
Data collection top
Bruker APEX-II CCD
diffractometer
3347 reflections with I > 2σ(I)
φ and ω scansRint = 0.084
Absorption correction: multi-scan
Bruker SAINT
θmax = 31.6°, θmin = 2.5°
Tmin = 0.90, Tmax = 0.96h = 3231
26569 measured reflectionsk = 1312
4907 independent reflectionsl = 1111
Refinement top
Refinement on F2Primary atom site location: direct methods
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.069H-atom parameters constrained
wR(F2) = 0.143 w = 1/[σ2(Fo2) + (0.0362P)2 + 0.4066P]
where P = (Fo2 + 2Fc2)/3
S = 1.25(Δ/σ)max < 0.001
4907 reflectionsΔρmax = 0.34 e Å3
183 parametersΔρmin = 0.25 e Å3
0 restraints
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.62808 (4)0.53454 (12)0.56014 (11)0.0255 (3)
O20.66405 (4)0.37790 (12)0.81108 (11)0.0271 (3)
C10.50070 (6)0.59344 (17)0.79638 (16)0.0235 (3)
H1A0.4636910.6460040.7901330.028*
C20.53584 (6)0.60466 (17)0.66974 (16)0.0233 (3)
H2A0.5223630.6639050.5785100.028*
C30.58986 (6)0.53073 (16)0.67563 (15)0.0202 (3)
C40.60933 (6)0.44426 (16)0.81256 (16)0.0206 (3)
C50.57385 (6)0.43294 (16)0.93620 (16)0.0214 (3)
H5A0.5872750.3731791.0270700.026*
C60.51860 (6)0.50686 (16)0.93197 (15)0.0191 (3)
C70.61685 (6)0.64258 (17)0.43261 (16)0.0240 (3)
H7A0.6122900.7450400.4768450.029*
H7B0.5797650.6164100.3635260.029*
C80.67018 (7)0.63693 (19)0.33730 (16)0.0268 (3)
H8A0.6641350.7105940.2482580.032*
H8B0.6726090.5351460.2896840.032*
C90.72899 (7)0.67160 (19)0.43771 (17)0.0286 (3)
H9A0.7335540.6022530.5307940.034*
H9B0.7273220.7758020.4796610.034*
C100.78390 (7)0.6569 (2)0.34676 (18)0.0305 (4)
H10A0.7805980.5628080.2827610.037*
H10B0.7847020.7427040.2713690.037*
C110.84186 (7)0.6543 (2)0.4562 (2)0.0417 (4)
H11A0.8394880.5738800.5372450.050*
H11B0.8464500.7518230.5139190.050*
C120.89717 (8)0.6275 (3)0.3699 (2)0.0491 (5)
H12A0.9325990.6214680.4487110.074*
H12B0.9018680.7110430.2957080.074*
H12C0.8925980.5325770.3096660.074*
C130.68889 (7)0.30644 (19)0.95673 (17)0.0271 (3)
H13A0.6635220.2204400.9826810.032*
H13B0.6912640.3791891.0467940.032*
C140.75054 (7)0.25185 (19)0.93039 (18)0.0297 (4)
H14A0.7473350.1889150.8322960.036*
H14B0.7655870.1864341.0216530.036*
C150.79601 (7)0.3752 (2)0.91342 (19)0.0323 (4)
H15A0.8013480.4350731.0136100.039*
H15B0.7806460.4436570.8251470.039*
C160.85627 (7)0.3125 (2)0.8791 (2)0.0383 (4)
H16A0.8699970.2386580.9637350.046*
H16B0.8509880.2576840.7756650.046*
C170.90438 (8)0.4308 (3)0.8712 (2)0.0518 (5)
H17A0.9114820.4819100.9765310.062*
H17B0.8900330.5076980.7904180.062*
C180.96299 (9)0.3659 (4)0.8282 (3)0.0780 (8)
H18A0.9918800.4478180.8209190.117*
H18B0.9562230.3138380.7247600.117*
H18C0.9787480.2941900.9112530.117*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0282 (6)0.0292 (6)0.0209 (5)0.0066 (4)0.0110 (4)0.0056 (4)
O20.0227 (5)0.0386 (7)0.0214 (5)0.0095 (5)0.0079 (4)0.0075 (4)
C10.0195 (7)0.0287 (8)0.0227 (7)0.0030 (6)0.0039 (5)0.0013 (6)
C20.0237 (7)0.0274 (8)0.0188 (6)0.0032 (6)0.0025 (5)0.0041 (6)
C30.0216 (7)0.0217 (7)0.0180 (6)0.0019 (6)0.0055 (5)0.0015 (5)
C40.0188 (7)0.0221 (7)0.0212 (6)0.0012 (5)0.0034 (5)0.0011 (5)
C50.0225 (7)0.0232 (7)0.0187 (6)0.0002 (6)0.0026 (5)0.0024 (5)
C60.0186 (7)0.0196 (7)0.0193 (6)0.0026 (5)0.0035 (5)0.0015 (5)
C70.0263 (7)0.0289 (8)0.0173 (6)0.0037 (6)0.0047 (5)0.0035 (6)
C80.0281 (8)0.0361 (9)0.0171 (6)0.0040 (7)0.0065 (5)0.0040 (6)
C90.0289 (8)0.0361 (9)0.0221 (7)0.0008 (7)0.0082 (6)0.0009 (6)
C100.0285 (8)0.0401 (10)0.0243 (7)0.0021 (7)0.0097 (6)0.0031 (7)
C110.0286 (9)0.0635 (13)0.0338 (9)0.0032 (8)0.0078 (7)0.0019 (8)
C120.0275 (9)0.0708 (15)0.0503 (11)0.0006 (9)0.0104 (8)0.0022 (10)
C130.0259 (8)0.0332 (9)0.0228 (7)0.0056 (6)0.0059 (6)0.0078 (6)
C140.0270 (8)0.0347 (9)0.0278 (7)0.0077 (7)0.0043 (6)0.0044 (6)
C150.0247 (8)0.0411 (10)0.0309 (8)0.0030 (7)0.0025 (6)0.0017 (7)
C160.0257 (8)0.0562 (12)0.0332 (8)0.0049 (8)0.0041 (7)0.0015 (8)
C170.0291 (9)0.0788 (16)0.0473 (11)0.0053 (10)0.0032 (8)0.0021 (10)
C180.0297 (11)0.136 (3)0.0700 (15)0.0082 (14)0.0141 (10)0.0142 (16)
Geometric parameters (Å, º) top
O1—C31.3633 (16)C10—H10B0.9900
O1—C71.4371 (16)C11—C121.524 (2)
O2—C41.3649 (17)C11—H11A0.9900
O2—C131.4342 (17)C11—H11B0.9900
C1—C21.3945 (19)C12—H12A0.9801
C1—C61.3944 (19)C12—H12B0.9801
C1—H1A0.9500C12—H12C0.9801
C2—C31.376 (2)C13—C141.507 (2)
C2—H2A0.9500C13—H13A0.9900
C3—C41.4101 (19)C13—H13B0.9900
C4—C51.3788 (19)C14—C151.514 (2)
C5—C61.4013 (19)C14—H14A0.9900
C5—H5A0.9500C14—H14B0.9900
C6—C6i1.491 (3)C15—C161.520 (2)
C7—C81.5125 (19)C15—H15A0.9900
C7—H7A0.9900C15—H15B0.9900
C7—H7B0.9900C16—C171.512 (3)
C8—C91.520 (2)C16—H16A0.9900
C8—H8A0.9900C16—H16B0.9900
C8—H8B0.9900C17—C181.517 (3)
C9—C101.526 (2)C17—H17A0.9900
C9—H9A0.9900C17—H17B0.9900
C9—H9B0.9900C18—H18A0.9801
C10—C111.511 (2)C18—H18B0.9801
C10—H10A0.9900C18—H18C0.9801
C3—O1—C7118.15 (11)C12—C11—H11A108.7
C4—O2—C13116.79 (10)C10—C11—H11B108.7
C2—C1—C6121.54 (13)C12—C11—H11B108.7
C2—C1—H1A119.2H11A—C11—H11B107.6
C6—C1—H1A119.2C11—C12—H12A109.5
C3—C2—C1120.64 (13)C11—C12—H12B109.5
C3—C2—H2A119.7H12A—C12—H12B109.5
C1—C2—H2A119.7C11—C12—H12C109.5
O1—C3—C2125.78 (12)H12A—C12—H12C109.5
O1—C3—C4115.36 (12)H12B—C12—H12C109.5
C2—C3—C4118.86 (12)O2—C13—C14107.24 (11)
O2—C4—C5124.83 (12)O2—C13—H13A110.3
O2—C4—C3115.28 (11)C14—C13—H13A110.3
C5—C4—C3119.88 (13)O2—C13—H13B110.3
C4—C5—C6122.04 (13)C14—C13—H13B110.3
C4—C5—H5A119.0H13A—C13—H13B108.5
C6—C5—H5A119.0C13—C14—C15115.07 (14)
C1—C6—C5117.03 (12)C13—C14—H14A108.5
C1—C6—C6i122.18 (15)C15—C14—H14A108.5
C5—C6—C6i120.79 (15)C13—C14—H14B108.5
O1—C7—C8106.61 (11)C15—C14—H14B108.5
O1—C7—H7A110.4H14A—C14—H14B107.5
C8—C7—H7A110.4C14—C15—C16112.29 (15)
O1—C7—H7B110.4C14—C15—H15A109.1
C8—C7—H7B110.4C16—C15—H15A109.1
H7A—C7—H7B108.6C14—C15—H15B109.1
C7—C8—C9113.11 (11)C16—C15—H15B109.1
C7—C8—H8A109.0H15A—C15—H15B107.9
C9—C8—H8A109.0C17—C16—C15114.31 (17)
C7—C8—H8B109.0C17—C16—H16A108.7
C9—C8—H8B109.0C15—C16—H16A108.7
H8A—C8—H8B107.8C17—C16—H16B108.7
C8—C9—C10114.10 (12)C15—C16—H16B108.7
C8—C9—H9A108.7H16A—C16—H16B107.6
C10—C9—H9A108.7C16—C17—C18113.1 (2)
C8—C9—H9B108.7C16—C17—H17A109.0
C10—C9—H9B108.7C18—C17—H17A109.0
H9A—C9—H9B107.6C16—C17—H17B109.0
C11—C10—C9112.89 (12)C18—C17—H17B109.0
C11—C10—H10A109.0H17A—C17—H17B107.8
C9—C10—H10A109.0C17—C18—H18A109.5
C11—C10—H10B109.0C17—C18—H18B109.5
C9—C10—H10B109.0H18A—C18—H18B109.5
H10A—C10—H10B107.8C17—C18—H18C109.5
C10—C11—C12114.09 (14)H18A—C18—H18C109.5
C10—C11—H11A108.7H18B—C18—H18C109.5
Symmetry code: (i) x+1, y+1, z+2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C13—H13A···O1ii0.992.503.4645 (19)163
Symmetry code: (ii) x, y+1/2, z+1/2.
(II) top
Crystal data top
C28H38O6Z = 1
Mr = 470.58F(000) = 254
Triclinic, P1Dx = 1.194 Mg m3
a = 8.554 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.6844 (17) ÅCell parameters from 706 reflections
c = 9.810 (3) Åθ = 3.7–26.2°
α = 100.26 (2)°µ = 0.08 mm1
β = 109.10 (3)°T = 294 K
γ = 100.53 (2)°Fragment, colourless
V = 654.4 (3) Å30.28 × 0.18 × 0.14 mm
Data collection top
Oxford Diffraction Gemini CCD S Ultra
diffractometer
1554 reflections with I > 2σ(I)
ω scans, thick slicesRint = 0.146
Absorption correction: multi-scan
CrysAlisPro, Oxford Diffraction (2009)
θmax = 29.0°, θmin = 3.6°
Tmin = 0.96, Tmax = 0.99h = 1111
4799 measured reflectionsk = 811
2919 independent reflectionsl = 1311
Refinement top
Refinement on F2Primary atom site location: direct methods
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.069H-atom parameters constrained
wR(F2) = 0.183 w = 1/[σ2(Fo2) + (0.0729P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.99(Δ/σ)max < 0.001
2919 reflectionsΔρmax = 0.28 e Å3
154 parametersΔρmin = 0.30 e Å3
0 restraints
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.70994 (19)0.57970 (17)0.73363 (17)0.0500 (5)
O20.5616 (2)0.78025 (17)0.86529 (17)0.0519 (5)
O30.3331 (2)0.5636 (2)0.7495 (2)0.0625 (5)
C10.6055 (3)0.8298 (2)0.4675 (3)0.0493 (6)
H1A0.6157860.8398680.3757590.059*
C20.6652 (3)0.7110 (3)0.5291 (3)0.0500 (6)
H2A0.7163440.6430380.4800930.060*
C30.6512 (3)0.6900 (3)0.6611 (3)0.0441 (6)
C40.5718 (3)0.7916 (3)0.7265 (3)0.0428 (6)
C50.5139 (3)0.9086 (3)0.6652 (3)0.0453 (6)
H5A0.4599820.9741630.7132640.054*
C60.5308 (3)0.9361 (2)0.5333 (3)0.0415 (5)
C70.7953 (3)0.4775 (3)0.6664 (3)0.0479 (6)
H7A0.8950590.5452410.6559600.058*
H7B0.7155710.4117790.5659050.058*
C80.8530 (3)0.3692 (3)0.7643 (3)0.0496 (6)
H8A0.7520300.3032830.7744890.060*
H8B0.9303650.4367130.8648750.060*
C90.9458 (3)0.2565 (3)0.7048 (3)0.0489 (6)
H9A0.8702330.1922400.6024900.059*
H9B1.0494430.3224700.6985160.059*
C100.9983 (3)0.1416 (3)0.8006 (3)0.0497 (6)
H10A1.0793200.2062240.9010280.060*
H10B0.8954890.0811160.8121700.060*
C111.0812 (3)0.0213 (3)0.7385 (3)0.0601 (7)
H11A1.0022030.0404780.6365050.072*
H11B1.1868360.0815450.7309880.072*
C121.1264 (3)0.0968 (3)0.8322 (3)0.0668 (8)
H12A1.1799480.1716700.7857760.100*
H12B1.2076780.0363000.9339060.100*
H12C1.0210080.1596600.8381960.100*
C130.4325 (4)0.6594 (3)0.8625 (3)0.0539 (7)
C140.4350 (4)0.6716 (3)1.0175 (3)0.0681 (8)
H14A0.3423550.5848331.0152740.102*
H14B0.5453050.6608031.0817440.102*
H14C0.4187950.7769131.0567540.102*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0578 (10)0.0510 (9)0.0627 (12)0.0233 (8)0.0431 (9)0.0178 (8)
O20.0647 (10)0.0506 (9)0.0563 (12)0.0177 (8)0.0406 (9)0.0152 (8)
O30.0712 (12)0.0572 (10)0.0725 (14)0.0099 (9)0.0505 (11)0.0109 (10)
C10.0570 (14)0.0469 (12)0.0641 (17)0.0159 (11)0.0450 (14)0.0179 (12)
C20.0504 (13)0.0472 (13)0.0692 (18)0.0149 (11)0.0427 (13)0.0142 (12)
C30.0494 (13)0.0412 (11)0.0546 (16)0.0144 (10)0.0324 (12)0.0159 (11)
C40.0507 (13)0.0440 (11)0.0437 (15)0.0134 (10)0.0298 (12)0.0111 (11)
C50.0471 (13)0.0415 (11)0.0593 (17)0.0150 (10)0.0351 (13)0.0096 (11)
C60.0423 (12)0.0414 (11)0.0487 (15)0.0074 (10)0.0292 (12)0.0106 (10)
C70.0472 (13)0.0480 (12)0.0640 (17)0.0182 (11)0.0385 (13)0.0118 (12)
C80.0532 (14)0.0512 (13)0.0587 (17)0.0202 (11)0.0346 (13)0.0153 (12)
C90.0481 (13)0.0520 (13)0.0633 (17)0.0162 (11)0.0386 (13)0.0181 (12)
C100.0458 (12)0.0564 (13)0.0628 (17)0.0201 (11)0.0343 (13)0.0199 (13)
C110.0578 (15)0.0585 (14)0.089 (2)0.0257 (12)0.0508 (15)0.0255 (14)
C120.0590 (15)0.0601 (15)0.094 (2)0.0286 (13)0.0374 (16)0.0203 (15)
C130.0710 (17)0.0515 (14)0.067 (2)0.0322 (13)0.0492 (16)0.0218 (14)
C140.103 (2)0.0689 (16)0.071 (2)0.0439 (16)0.0617 (18)0.0336 (15)
Geometric parameters (Å, º) top
O1—C31.364 (3)C8—H8A0.9900
O1—C71.448 (2)C8—H8B0.9900
O2—C131.367 (3)C9—C101.517 (3)
O2—C41.412 (2)C9—H9A0.9900
O3—C131.200 (3)C9—H9B0.9900
C1—C21.379 (3)C10—C111.514 (3)
C1—C61.397 (3)C10—H10A0.9900
C1—H1A0.9500C10—H10B0.9900
C2—C31.379 (3)C11—C121.515 (3)
C2—H2A0.9500C11—H11A0.9900
C3—C41.398 (3)C11—H11B0.9900
C4—C51.359 (3)C12—H12A0.9901
C5—C61.404 (3)C12—H12B0.9900
C5—H5A0.9500C12—H12C0.9900
C6—C6i1.477 (4)C13—C141.498 (3)
C7—C81.494 (3)C14—H14A0.9800
C7—H7A0.9900C14—H14B0.9800
C7—H7B0.9900C14—H14C0.9800
C8—C91.520 (3)
C3—O1—C7116.94 (17)C10—C9—H9A108.9
C13—O2—C4116.82 (19)C8—C9—H9A108.9
C2—C1—C6123.3 (2)C10—C9—H9B108.9
C2—C1—H1A118.4C8—C9—H9B108.9
C6—C1—H1A118.4H9A—C9—H9B107.7
C3—C2—C1120.6 (2)C11—C10—C9114.2 (2)
C3—C2—H2A119.7C11—C10—H10A108.7
C1—C2—H2A119.7C9—C10—H10A108.7
O1—C3—C2125.46 (19)C11—C10—H10B108.7
O1—C3—C4117.5 (2)C9—C10—H10B108.7
C2—C3—C4117.1 (2)H10A—C10—H10B107.6
C5—C4—C3121.8 (2)C12—C11—C10113.6 (2)
C5—C4—O2118.71 (19)C12—C11—H11A108.9
C3—C4—O2119.31 (19)C10—C11—H11A108.9
C4—C5—C6122.4 (2)C12—C11—H11B108.9
C4—C5—H5A118.8C10—C11—H11B108.9
C6—C5—H5A118.8H11A—C11—H11B107.7
C1—C6—C5114.7 (2)C11—C12—H12A109.5
C1—C6—C6i122.6 (3)C11—C12—H12B109.5
C5—C6—C6i122.7 (2)H12A—C12—H12B109.5
O1—C7—C8108.50 (18)C11—C12—H12C109.4
O1—C7—H7A110.0H12A—C12—H12C109.5
C8—C7—H7A110.0H12B—C12—H12C109.5
O1—C7—H7B110.0O3—C13—O2122.9 (2)
C8—C7—H7B110.0O3—C13—C14127.5 (2)
H7A—C7—H7B108.4O2—C13—C14109.5 (2)
C7—C8—C9113.11 (19)C13—C14—H14A109.4
C7—C8—H8A109.0C13—C14—H14B109.5
C9—C8—H8A109.0H14A—C14—H14B109.5
C7—C8—H8B109.0C13—C14—H14C109.5
C9—C8—H8B109.0H14A—C14—H14C109.5
H8A—C8—H8B107.8H14B—C14—H14C109.5
C10—C9—C8113.2 (2)
Symmetry code: (i) x+1, y+2, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2A···O3ii0.952.483.298 (3)145
Symmetry code: (ii) x+1, y+1, z+1.
(IV) top
Crystal data top
C18H18O6F(000) = 696
Mr = 330.32Dx = 1.398 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 11.304 (2) ÅCell parameters from 6780 reflections
b = 10.064 (2) Åθ = 3.1–29.8°
c = 14.496 (3) ŵ = 0.11 mm1
β = 107.822 (10)°T = 150 K
V = 1570.0 (6) Å3Fragment, colourless
Z = 40.28 × 0.18 × 0.10 mm
Data collection top
Bruker APEX-II CCD
diffractometer
7986 reflections with I > 2σ(I)
φ and ω scansRint = 0.030
Absorption correction: multi-scan
Bruker SAINT
θmax = 32.8°, θmin = 2.7°
Tmin = 0.90, Tmax = 0.96h = 1616
25745 measured reflectionsk = 1514
9921 independent reflectionsl = 2220
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.063 w = 1/[σ2(Fo2) + (0.0853P)2 + 1.1735P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.179(Δ/σ)max < 0.001
S = 1.03Δρmax = 0.65 e Å3
9921 reflectionsΔρmin = 0.40 e Å3
440 parametersAbsolute structure: Flack x determined using 3206 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
355 restraintsAbsolute structure parameter: 0.0 (2)
Primary atom site location: direct methods
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O1A1.0052 (2)0.8249 (3)0.45851 (17)0.0385 (7)
O2A0.8332 (4)0.9299 (4)0.3706 (2)0.0522 (8)
O3A0.8249 (2)0.6430 (2)0.44977 (16)0.0244 (5)
C1A0.9678 (3)0.8630 (5)0.6991 (2)0.0375 (9)
H1AA1.0031850.9137950.7561590.045*
C2A1.0025 (4)0.8909 (5)0.6161 (3)0.0391 (9)
H2AA1.0543700.9644140.6140620.047*
C3A0.9582 (3)0.8075 (4)0.5375 (2)0.0257 (6)
C4A0.8692 (3)0.7097 (3)0.53479 (19)0.0158 (5)
C5A0.8277 (3)0.6915 (3)0.6143 (2)0.0156 (5)
H5AA0.7619670.6308560.6104920.019*
C6A0.8816 (2)0.7615 (3)0.70047 (18)0.0148 (5)
C7A0.9328 (4)0.8848 (4)0.3781 (3)0.0379 (7)
C8A0.9925 (5)0.8791 (6)0.2989 (3)0.0566 (14)
H8AA0.9964570.9688380.2736080.085*
H8AB0.9433450.8217530.2464880.085*
H8AC1.0768180.8431750.3247370.085*
C9A0.7317 (4)0.5446 (4)0.4460 (3)0.0330 (8)
H9AA0.6969870.5125210.3792710.049*
H9AB0.6653660.5840410.4675080.049*
H9AC0.7690650.4701640.4884690.049*
O1A'0.71824 (19)0.6785 (2)1.02983 (14)0.0172 (4)
O2A'0.9005 (2)0.5937 (3)1.12222 (15)0.0271 (5)
O3A'0.8857 (2)0.8711 (2)1.03354 (14)0.0214 (4)
C1A'0.7579 (2)0.6341 (3)0.78943 (18)0.0143 (5)
H1AB0.7283120.5774010.7347870.017*
C2A'0.7192 (3)0.6138 (3)0.87088 (19)0.0166 (5)
H2AB0.6612050.5455250.8708720.020*
C3A'0.7653 (2)0.6930 (3)0.95128 (18)0.0129 (4)
C4A'0.8476 (2)0.7969 (2)0.95118 (18)0.0115 (4)
C5A'0.8852 (2)0.8172 (2)0.86969 (17)0.0116 (4)
H5AB0.9424520.8863830.8698690.014*
C6A'0.8405 (2)0.7377 (2)0.78759 (16)0.0103 (4)
C7A'0.7966 (3)0.6300 (3)1.1138 (2)0.0190 (5)
C8A'0.7327 (4)0.6280 (4)1.1897 (2)0.0312 (7)
H8AD0.7833240.5783321.2461330.047*
H8AE0.6514540.5850841.1638080.047*
H8AF0.7214350.7192991.2089610.047*
C9A'0.9809 (3)0.9653 (3)1.03937 (19)0.0213 (5)
H9AD1.0093311.0028151.1048610.032*
H9AE0.9485781.0365600.9923400.032*
H9AF1.0507010.9215451.0249320.032*
O1B0.4505 (4)0.3141 (5)0.5243 (2)0.0737 (14)
O2B0.6190 (2)0.4214 (3)0.61168 (17)0.0299 (5)
O3B0.6257 (4)0.1488 (4)0.5262 (3)0.0656 (10)
C1B0.4834 (3)0.3818 (4)0.2824 (3)0.0344 (7)
H1BA0.4510780.4390870.2284460.041*
C2B0.4429 (4)0.3932 (6)0.3643 (3)0.0458 (10)
H2BA0.3809530.4563290.3655160.055*
C3B0.4939 (4)0.3117 (5)0.4432 (3)0.0447 (8)
C4B0.5827 (5)0.2226 (5)0.4456 (3)0.0468 (9)
C5B0.6210 (5)0.2085 (4)0.3616 (3)0.0414 (9)
H5BA0.6822910.1442530.3609960.050*
C6B0.5707 (3)0.2865 (3)0.2807 (2)0.0273 (6)
C7B0.5261 (4)0.3632 (5)0.6074 (3)0.0409 (9)
C8B0.4681 (4)0.3427 (7)0.6864 (3)0.0566 (15)
H8BA0.5107610.3981940.7422470.085*
H8BB0.4754910.2490440.7058510.085*
H8BC0.3800850.3675090.6628220.085*
C9B0.7420 (8)0.0805 (8)0.5416 (6)0.094 (2)
H9BA0.7881600.0794610.6109280.141*
H9BB0.7283760.0109460.5174560.141*
H9BC0.7899220.1289670.5064700.141*
O1B'0.7652 (2)0.2704 (2)0.03688 (16)0.0282 (5)
O2B'0.6418 (4)0.1059 (3)0.1127 (2)0.0526 (9)
O3B'0.5377 (2)0.3698 (2)0.06364 (14)0.0222 (4)
C1B'0.7365 (3)0.2234 (4)0.2059 (2)0.0307 (6)
H1BB0.7852640.1916670.2675200.037*
C2B'0.7831 (3)0.2164 (4)0.1278 (2)0.0317 (7)
H2BB0.8620090.1775820.1349380.038*
C3B'0.7121 (3)0.2672 (3)0.0391 (2)0.0225 (5)
C4B'0.5955 (3)0.3233 (3)0.0264 (2)0.0181 (5)
C5B'0.5499 (3)0.3284 (3)0.1049 (2)0.0191 (5)
H5BB0.4710350.3676150.0973670.023*
C6B'0.6184 (3)0.2766 (3)0.1950 (2)0.0222 (5)
C7B'0.7195 (4)0.1861 (4)0.1104 (3)0.0320 (6)
C8B'0.7793 (5)0.2072 (5)0.1882 (3)0.0483 (11)
H8BD0.7421200.1467840.2423840.072*
H8BE0.8686310.1892630.1621790.072*
H8BF0.7664360.2993050.2110400.072*
C9B'0.4328 (3)0.4554 (3)0.0724 (2)0.0289 (7)
H9BD0.4032540.4914180.1383020.043*
H9BE0.4577560.5285430.0258470.043*
H9BF0.3660000.4044310.0589930.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O1A0.0292 (12)0.073 (2)0.0197 (10)0.0189 (12)0.0173 (9)0.0055 (11)
O2A0.0733 (19)0.0501 (17)0.0391 (16)0.0001 (16)0.0258 (15)0.0126 (14)
O3A0.0380 (12)0.0247 (10)0.0166 (9)0.0080 (9)0.0172 (9)0.0063 (8)
C1A0.0357 (17)0.058 (2)0.0219 (14)0.0286 (17)0.0134 (13)0.0123 (15)
C2A0.0377 (18)0.059 (2)0.0251 (14)0.0262 (17)0.0162 (14)0.0102 (14)
C3A0.0218 (13)0.0430 (17)0.0167 (12)0.0097 (12)0.0126 (10)0.0026 (11)
C4A0.0166 (11)0.0203 (12)0.0113 (10)0.0018 (9)0.0053 (8)0.0007 (8)
C5A0.0187 (11)0.0150 (11)0.0146 (10)0.0023 (9)0.0073 (9)0.0009 (8)
C6A0.0108 (10)0.0253 (12)0.0085 (9)0.0003 (9)0.0033 (8)0.0005 (8)
C7A0.0536 (17)0.0408 (19)0.0225 (13)0.0267 (14)0.0162 (13)0.0038 (13)
C8A0.069 (3)0.082 (4)0.0286 (18)0.040 (3)0.0292 (19)0.009 (2)
C9A0.050 (2)0.0270 (15)0.0301 (16)0.0158 (14)0.0240 (16)0.0157 (13)
O1A'0.0200 (9)0.0238 (9)0.0105 (8)0.0015 (7)0.0085 (7)0.0006 (7)
O2A'0.0317 (11)0.0374 (12)0.0122 (9)0.0088 (10)0.0068 (8)0.0058 (9)
O3A'0.0347 (11)0.0225 (9)0.0122 (8)0.0063 (8)0.0151 (8)0.0060 (7)
C1A'0.0149 (11)0.0184 (11)0.0096 (10)0.0011 (9)0.0039 (8)0.0016 (9)
C2A'0.0162 (11)0.0230 (12)0.0113 (10)0.0038 (10)0.0054 (8)0.0016 (9)
C3A'0.0140 (10)0.0166 (10)0.0089 (9)0.0010 (8)0.0050 (8)0.0028 (8)
C4A'0.0149 (10)0.0110 (9)0.0096 (9)0.0034 (8)0.0050 (8)0.0006 (7)
C5A'0.0155 (10)0.0119 (9)0.0084 (9)0.0015 (8)0.0053 (8)0.0013 (7)
C6A'0.0099 (9)0.0129 (9)0.0078 (9)0.0021 (7)0.0020 (7)0.0017 (7)
C7A'0.0292 (12)0.0203 (12)0.0095 (10)0.0009 (10)0.0086 (9)0.0030 (9)
C8A'0.0448 (19)0.0382 (18)0.0170 (13)0.0014 (15)0.0190 (13)0.0025 (12)
C9A'0.0295 (14)0.0263 (13)0.0102 (10)0.0053 (11)0.0094 (10)0.0034 (10)
O1B0.064 (2)0.129 (4)0.0337 (15)0.053 (2)0.0245 (14)0.0229 (19)
O2B0.0371 (12)0.0355 (12)0.0205 (11)0.0113 (10)0.0137 (10)0.0084 (9)
O3B0.104 (3)0.051 (2)0.0499 (19)0.0019 (19)0.036 (2)0.0040 (15)
C1B0.0298 (16)0.052 (2)0.0228 (14)0.0043 (14)0.0107 (12)0.0032 (14)
C2B0.0358 (19)0.077 (3)0.0292 (16)0.0054 (18)0.0172 (14)0.0074 (16)
C3B0.047 (2)0.061 (2)0.0283 (15)0.0242 (15)0.0162 (14)0.0101 (15)
C4B0.061 (2)0.044 (2)0.0372 (17)0.0223 (16)0.0186 (17)0.0050 (15)
C5B0.062 (2)0.0302 (17)0.0354 (17)0.0059 (16)0.0199 (17)0.0009 (13)
C6B0.0358 (15)0.0262 (14)0.0217 (12)0.0141 (11)0.0117 (11)0.0100 (10)
C7B0.0372 (16)0.062 (2)0.0286 (15)0.0162 (17)0.0173 (13)0.0120 (16)
C8B0.037 (2)0.111 (5)0.0258 (17)0.024 (3)0.0158 (15)0.014 (2)
C9B0.136 (5)0.079 (5)0.080 (5)0.036 (4)0.053 (4)0.034 (4)
O1B'0.0371 (12)0.0339 (11)0.0223 (10)0.0046 (10)0.0220 (9)0.0027 (8)
O2B'0.082 (2)0.0435 (15)0.0485 (18)0.0115 (15)0.0439 (17)0.0187 (14)
O3B'0.0364 (11)0.0215 (9)0.0144 (8)0.0028 (8)0.0161 (8)0.0008 (7)
C1B'0.0396 (16)0.0359 (16)0.0190 (12)0.0035 (13)0.0125 (12)0.0006 (12)
C2B'0.0353 (16)0.0416 (18)0.0224 (13)0.0079 (14)0.0152 (12)0.0010 (12)
C3B'0.0329 (13)0.0211 (12)0.0203 (11)0.0012 (10)0.0183 (10)0.0001 (10)
C4B'0.0289 (12)0.0145 (10)0.0163 (10)0.0039 (9)0.0149 (9)0.0016 (8)
C5B'0.0298 (13)0.0168 (11)0.0150 (11)0.0057 (10)0.0132 (10)0.0029 (9)
C6B'0.0342 (13)0.0170 (11)0.0190 (11)0.0081 (10)0.0133 (10)0.0033 (9)
C7B'0.0481 (18)0.0303 (14)0.0242 (13)0.0133 (12)0.0209 (13)0.0037 (11)
C8B'0.067 (3)0.063 (3)0.0269 (17)0.028 (2)0.0314 (18)0.0138 (17)
C9B'0.0425 (17)0.0292 (15)0.0236 (14)0.0067 (12)0.0228 (13)0.0005 (11)
Geometric parameters (Å, º) top
O1A—C7A1.345 (5)O1B—C7B1.340 (5)
O1A—C3A1.412 (3)O1B—C3B1.405 (5)
O2A—C7A1.187 (6)O2B—C7B1.188 (5)
O3A—C4A1.357 (3)O3B—C4B1.344 (6)
O3A—C9A1.434 (4)O3B—C9B1.440 (9)
C1A—C2A1.404 (5)C1B—C6B1.381 (5)
C1A—C6A1.415 (4)C1B—C2B1.402 (5)
C1A—H1AA0.9500C1B—H1BA0.9500
C2A—C3A1.380 (5)C2B—C3B1.382 (7)
C2A—H2AA0.9500C2B—H2BA0.9500
C3A—C4A1.400 (4)C3B—C4B1.338 (7)
C4A—C5A1.384 (4)C4B—C5B1.418 (6)
C5A—C6A1.400 (4)C5B—C6B1.381 (5)
C5A—H5AA0.9500C5B—H5BA0.9500
C6A—C6A'1.493 (3)C6B—C6B'1.502 (4)
C7A—C8A1.502 (5)C7B—C8B1.497 (5)
C8A—H8AA0.9801C8B—H8BA0.9801
C8A—H8AB0.9801C8B—H8BB0.9801
C8A—H8AC0.9801C8B—H8BC0.9801
C9A—H9AA0.9801C9B—H9BA0.9800
C9A—H9AB0.9801C9B—H9BB0.9800
C9A—H9AC0.9801C9B—H9BC0.9800
O1A'—C7A'1.358 (3)O1B'—C7B'1.337 (4)
O1A'—C3A'1.404 (3)O1B'—C3B'1.407 (3)
O2A'—C7A'1.200 (4)O2B'—C7B'1.186 (5)
O3A'—C4A'1.362 (3)O3B'—C4B'1.351 (3)
O3A'—C9A'1.417 (4)O3B'—C9B'1.439 (4)
C1A'—C2A'1.394 (4)C1B'—C2B'1.389 (4)
C1A'—C6A'1.406 (4)C1B'—C6B'1.401 (5)
C1A'—H1AB0.9500C1B'—H1BB0.9500
C2A'—C3A'1.376 (4)C2B'—C3B'1.388 (4)
C2A'—H2AB0.9500C2B'—H2BB0.9500
C3A'—C4A'1.400 (4)C3B'—C4B'1.393 (4)
C4A'—C5A'1.388 (3)C4B'—C5B'1.387 (3)
C5A'—C6A'1.394 (3)C5B'—C6B'1.400 (4)
C5A'—H5AB0.9500C5B'—H5BB0.9500
C7A'—C8A'1.489 (4)C7B'—C8B'1.497 (5)
C8A'—H8AD0.9801C8B'—H8BD0.9801
C8A'—H8AE0.9801C8B'—H8BE0.9801
C8A'—H8AF0.9801C8B'—H8BF0.9801
C9A'—H9AD0.9801C9B'—H9BD0.9801
C9A'—H9AE0.9801C9B'—H9BE0.9801
C9A'—H9AF0.9801C9B'—H9BF0.9801
C7A—O1A—C3A118.5 (3)C7B—O1B—C3B118.0 (3)
C4A—O3A—C9A116.0 (2)C4B—O3B—C9B118.0 (4)
C2A—C1A—C6A122.0 (3)C6B—C1B—C2B119.5 (4)
C2A—C1A—H1AA119.0C6B—C1B—H1BA120.3
C6A—C1A—H1AA119.0C2B—C1B—H1BA120.3
C3A—C2A—C1A117.4 (3)C3B—C2B—C1B119.4 (4)
C3A—C2A—H2AA121.3C3B—C2B—H2BA120.3
C1A—C2A—H2AA121.3C1B—C2B—H2BA120.3
C2A—C3A—C4A121.8 (3)C4B—C3B—C2B122.5 (4)
C2A—C3A—O1A117.6 (3)C4B—C3B—O1B116.2 (5)
C4A—C3A—O1A120.7 (3)C2B—C3B—O1B121.2 (5)
O3A—C4A—C5A124.5 (3)C3B—C4B—O3B117.5 (4)
O3A—C4A—C3A115.8 (2)C3B—C4B—C5B117.9 (4)
C5A—C4A—C3A119.6 (3)O3B—C4B—C5B124.5 (5)
C4A—C5A—C6A120.7 (2)C6B—C5B—C4B121.1 (4)
C4A—C5A—H5AA119.7C6B—C5B—H5BA119.4
C6A—C5A—H5AA119.7C4B—C5B—H5BA119.4
C5A—C6A—C1A117.7 (2)C1B—C6B—C5B119.4 (3)
C5A—C6A—C6A'120.7 (2)C1B—C6B—C6B'120.0 (3)
C1A—C6A—C6A'121.4 (2)C5B—C6B—C6B'120.4 (3)
O2A—C7A—O1A124.1 (3)O2B—C7B—O1B122.6 (3)
O2A—C7A—C8A125.4 (4)O2B—C7B—C8B128.0 (4)
O1A—C7A—C8A110.4 (4)O1B—C7B—C8B109.3 (3)
C7A—C8A—H8AA109.5C7B—C8B—H8BA109.5
C7A—C8A—H8AB109.5C7B—C8B—H8BB109.5
H8AA—C8A—H8AB109.5H8BA—C8B—H8BB109.5
C7A—C8A—H8AC109.5C7B—C8B—H8BC109.5
H8AA—C8A—H8AC109.5H8BA—C8B—H8BC109.5
H8AB—C8A—H8AC109.5H8BB—C8B—H8BC109.5
O3A—C9A—H9AA109.5O3B—C9B—H9BA109.8
O3A—C9A—H9AB109.5O3B—C9B—H9BB110.9
H9AA—C9A—H9AB109.5H9BA—C9B—H9BB109.4
O3A—C9A—H9AC109.5O3B—C9B—H9BC107.8
H9AA—C9A—H9AC109.5H9BA—C9B—H9BC109.4
H9AB—C9A—H9AC109.5H9BB—C9B—H9BC109.4
C7A'—O1A'—C3A'117.3 (2)C7B'—O1B'—C3B'117.2 (3)
C4A'—O3A'—C9A'116.7 (2)C4B'—O3B'—C9B'115.7 (2)
C2A'—C1A'—C6A'120.5 (2)C2B'—C1B'—C6B'120.9 (3)
C2A'—C1A'—H1AB119.8C2B'—C1B'—H1BB119.6
C6A'—C1A'—H1AB119.8C6B'—C1B'—H1BB119.6
C3A'—C2A'—C1A'119.8 (2)C3B'—C2B'—C1B'118.7 (3)
C3A'—C2A'—H2AB120.1C3B'—C2B'—H2BB120.7
C1A'—C2A'—H2AB120.1C1B'—C2B'—H2BB120.7
C2A'—C3A'—C4A'120.8 (2)C2B'—C3B'—C4B'121.8 (3)
C2A'—C3A'—O1A'119.2 (2)C2B'—C3B'—O1B'118.0 (3)
C4A'—C3A'—O1A'119.7 (2)C4B'—C3B'—O1B'120.0 (3)
O3A'—C4A'—C5A'124.6 (2)O3B'—C4B'—C5B'126.0 (3)
O3A'—C4A'—C3A'116.2 (2)O3B'—C4B'—C3B'115.3 (2)
C5A'—C4A'—C3A'119.2 (2)C5B'—C4B'—C3B'118.7 (3)
C4A'—C5A'—C6A'121.1 (2)C4B'—C5B'—C6B'120.9 (3)
C4A'—C5A'—H5AB119.4C4B'—C5B'—H5BB119.6
C6A'—C5A'—H5AB119.4C6B'—C5B'—H5BB119.6
C5A'—C6A'—C1A'118.6 (2)C5B'—C6B'—C1B'118.9 (3)
C5A'—C6A'—C6A120.3 (2)C5B'—C6B'—C6B120.7 (3)
C1A'—C6A'—C6A121.0 (2)C1B'—C6B'—C6B120.2 (3)
O2A'—C7A'—O1A'123.4 (3)O2B'—C7B'—O1B'123.8 (3)
O2A'—C7A'—C8A'126.9 (3)O2B'—C7B'—C8B'125.2 (4)
O1A'—C7A'—C8A'109.6 (3)O1B'—C7B'—C8B'110.9 (4)
C7A'—C8A'—H8AD109.5C7B'—C8B'—H8BD109.5
C7A'—C8A'—H8AE109.5C7B'—C8B'—H8BE109.5
H8AD—C8A'—H8AE109.5H8BD—C8B'—H8BE109.5
C7A'—C8A'—H8AF109.5C7B'—C8B'—H8BF109.5
H8AD—C8A'—H8AF109.5H8BD—C8B'—H8BF109.5
H8AE—C8A'—H8AF109.5H8BE—C8B'—H8BF109.5
O3A'—C9A'—H9AD109.5O3B'—C9B'—H9BD109.5
O3A'—C9A'—H9AE109.5O3B'—C9B'—H9BE109.5
H9AD—C9A'—H9AE109.5H9BD—C9B'—H9BE109.5
O3A'—C9A'—H9AF109.5O3B'—C9B'—H9BF109.5
H9AD—C9A'—H9AF109.5H9BD—C9B'—H9BF109.5
H9AE—C9A'—H9AF109.5H9BE—C9B'—H9BF109.5
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2A—H2AA···O3Ai0.952.593.506 (5)162
C5A—H5AA···O2B0.952.663.592 (4)167
C2A—H2AB···O3Bii0.952.613.512 (4)160
C9A—H9AF···O1Bi0.982.543.485 (4)162
C2B—H2BA···O3Biii0.952.513.240 (6)134
C8B—H8BC···O2Aiv0.982.393.366 (6)172
C9B—H9BB···O1Biv0.982.613.401 (11)138
C9B—H9BF···O1Aiv0.982.553.421 (4)148
Symmetry codes: (i) x+2, y+1/2, z+1; (ii) x, y, z+1; (iii) x+1, y+1/2, z+1; (iv) x+1, y1/2, z+1.
(Vb) top
Crystal data top
C16H18O4F(000) = 584
Mr = 274.30Dx = 1.264 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 13.1000 (7) ÅCell parameters from 2116 reflections
b = 7.6709 (3) Åθ = 4.1–26.7°
c = 15.2881 (7) ŵ = 0.09 mm1
β = 110.181 (5)°T = 294 K
V = 1441.97 (12) Å3Fragment, colourless
Z = 40.48 × 0.18 × 0.14 mm
Data collection top
Oxford Diffraction Gemini CCD S Ultra
diffractometer
2334 reflections with I > 2σ(I)
ω scans, thick slicesRint = 0.055
Absorption correction: multi-scan
CrysAlisPro 1.171.38.46 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
θmax = 29.5°, θmin = 3.8°
Tmin = 0.92, Tmax = 0.99h = 1717
42671 measured reflectionsk = 1010
3773 independent reflectionsl = 2019
Refinement top
Refinement on F2Primary atom site location: direct methods
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.050H-atom parameters constrained
wR(F2) = 0.132 w = 1/[σ2(Fo2) + (0.0543P)2 + 0.2499P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
3773 reflectionsΔρmax = 0.17 e Å3
185 parametersΔρmin = 0.17 e Å3
0 restraints
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O11.08189 (8)0.39901 (16)0.36020 (8)0.0599 (3)
O20.96587 (9)0.26155 (18)0.44747 (8)0.0683 (4)
O1'0.28686 (8)0.38500 (17)0.07344 (9)0.0679 (4)
O2'0.38943 (9)0.65661 (15)0.05161 (8)0.0582 (3)
C10.80803 (12)0.4743 (2)0.18792 (10)0.0483 (4)
H1A0.7740020.5248080.1281660.058*
C20.92069 (12)0.4789 (2)0.22853 (11)0.0495 (4)
H2A0.9627110.5329510.1964150.059*
C30.97181 (11)0.40596 (19)0.31468 (10)0.0460 (4)
C40.90877 (12)0.3293 (2)0.36221 (10)0.0469 (4)
C50.79721 (11)0.3254 (2)0.32164 (10)0.0444 (3)
H5A0.7550640.2730510.3541610.053*
C60.74482 (11)0.39729 (19)0.23318 (9)0.0421 (3)
C71.14949 (14)0.4649 (3)0.31293 (15)0.0749 (6)
H7A1.2259080.4463810.3512060.112*
H7B1.1359310.5899890.3015450.112*
H7C1.1334350.4040890.2533080.112*
C80.90805 (15)0.2138 (3)0.50611 (12)0.0756 (6)
H8A0.9594120.1790150.5671200.113*
H8B0.8596410.1158590.4783160.113*
H8C0.8648140.3131000.5137420.113*
C1'0.56716 (12)0.24702 (19)0.20493 (10)0.0471 (4)
H1A'0.6054210.1517100.2412860.057*
C2'0.45432 (12)0.2410 (2)0.16667 (10)0.0498 (4)
H2A'0.4164810.1417480.1767970.060*
C3'0.39705 (12)0.3781 (2)0.11418 (10)0.0472 (4)
C4'0.45376 (12)0.52447 (19)0.10073 (9)0.0440 (3)
C5'0.56553 (12)0.52812 (19)0.13789 (9)0.0432 (3)
H5A'0.6033990.6269520.1273040.052*
C6'0.62470 (11)0.38892 (18)0.19108 (9)0.0415 (3)
C7'0.22693 (15)0.2363 (3)0.08319 (17)0.0845 (7)
H7A'0.1497580.2530810.0467170.127*
H7B'0.2357430.2204600.1490150.127*
H7C'0.2539830.1327390.0605550.127*
C8'0.44236 (15)0.8102 (2)0.03905 (14)0.0682 (5)
H8A'0.3880870.8943780.0024350.102*
H8B'0.4924430.7821160.0060130.102*
H8C'0.4832490.8607760.0999830.102*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0405 (6)0.0703 (8)0.0650 (7)0.0062 (5)0.0133 (5)0.0046 (6)
O20.0438 (6)0.1016 (10)0.0524 (6)0.0013 (6)0.0074 (5)0.0265 (6)
O1'0.0390 (6)0.0774 (8)0.0770 (8)0.0020 (6)0.0071 (6)0.0186 (6)
O2'0.0542 (7)0.0550 (7)0.0608 (7)0.0140 (5)0.0140 (5)0.0149 (5)
C10.0518 (9)0.0499 (9)0.0414 (8)0.0026 (7)0.0137 (7)0.0053 (6)
C20.0506 (9)0.0503 (9)0.0504 (8)0.0057 (7)0.0208 (7)0.0015 (7)
C30.0384 (8)0.0467 (8)0.0507 (8)0.0019 (6)0.0125 (6)0.0029 (6)
C40.0427 (8)0.0522 (9)0.0417 (8)0.0023 (6)0.0094 (6)0.0034 (6)
C50.0413 (8)0.0514 (8)0.0411 (8)0.0015 (6)0.0149 (6)0.0030 (6)
C60.0417 (8)0.0435 (8)0.0386 (7)0.0031 (6)0.0107 (6)0.0011 (6)
C70.0509 (10)0.0881 (14)0.0892 (14)0.0103 (9)0.0288 (10)0.0068 (11)
C80.0613 (11)0.1097 (16)0.0494 (10)0.0029 (11)0.0111 (9)0.0236 (10)
C1'0.0476 (9)0.0471 (8)0.0418 (7)0.0052 (6)0.0093 (7)0.0083 (6)
C2'0.0485 (9)0.0522 (9)0.0464 (8)0.0028 (7)0.0136 (7)0.0067 (7)
C3'0.0403 (8)0.0576 (9)0.0403 (7)0.0037 (7)0.0096 (6)0.0021 (7)
C4'0.0458 (8)0.0474 (8)0.0365 (7)0.0090 (6)0.0115 (6)0.0031 (6)
C5'0.0470 (8)0.0423 (7)0.0398 (7)0.0017 (6)0.0144 (6)0.0009 (6)
C6'0.0421 (8)0.0461 (8)0.0344 (7)0.0035 (6)0.0109 (6)0.0008 (6)
C7'0.0482 (10)0.0937 (16)0.1006 (16)0.0128 (10)0.0118 (10)0.0129 (12)
C8'0.0758 (12)0.0496 (10)0.0760 (12)0.0140 (9)0.0223 (10)0.0168 (9)
Geometric parameters (Å, º) top
O1—C31.3689 (17)C7—H7C0.9801
O1—C71.416 (2)C8—H8A0.9801
O2—C41.3625 (17)C8—H8B0.9801
O2—C81.407 (2)C8—H8C0.9801
O1'—C3'1.3616 (17)C1'—C6'1.381 (2)
O1'—C7'1.422 (2)C1'—C2'1.390 (2)
O2'—C4'1.3656 (17)C1'—H1A'0.9500
O2'—C8'1.414 (2)C2'—C3'1.377 (2)
C1—C61.381 (2)C2'—H2A'0.9500
C1—C21.390 (2)C3'—C4'1.400 (2)
C1—H1A0.9500C4'—C5'1.376 (2)
C2—C31.374 (2)C5'—C6'1.4026 (19)
C2—H2A0.9500C5'—H5A'0.9500
C3—C41.403 (2)C7'—H7A'0.9801
C4—C51.3770 (19)C7'—H7B'0.9801
C5—C61.4014 (19)C7'—H7C'0.9801
C5—H5A0.9500C8'—H8A'0.9801
C6—C6'1.4818 (19)C8'—H8B'0.9801
C7—H7A0.9801C8'—H8C'0.9801
C7—H7B0.9801
C3—O1—C7117.48 (13)H8A—C8—H8C109.5
C4—O2—C8118.06 (12)H8B—C8—H8C109.5
C3'—O1'—C7'117.22 (13)C6'—C1'—C2'121.26 (13)
C4'—O2'—C8'117.06 (12)C6'—C1'—H1A'119.4
C6—C1—C2120.97 (13)C2'—C1'—H1A'119.4
C6—C1—H1A119.5C3'—C2'—C1'120.41 (14)
C2—C1—H1A119.5C3'—C2'—H2A'119.8
C3—C2—C1120.60 (14)C1'—C2'—H2A'119.8
C3—C2—H2A119.7O1'—C3'—C2'125.07 (14)
C1—C2—H2A119.7O1'—C3'—C4'115.73 (13)
O1—C3—C2125.64 (14)C2'—C3'—C4'119.20 (13)
O1—C3—C4115.17 (13)O2'—C4'—C5'125.37 (14)
C2—C3—C4119.18 (13)O2'—C4'—C3'114.71 (13)
O2—C4—C5124.71 (14)C5'—C4'—C3'119.91 (13)
O2—C4—C3115.36 (13)C4'—C5'—C6'121.36 (14)
C5—C4—C3119.92 (13)C4'—C5'—H5A'119.3
C4—C5—C6121.08 (14)C6'—C5'—H5A'119.3
C4—C5—H5A119.5C1'—C6'—C5'117.85 (13)
C6—C5—H5A119.5C1'—C6'—C6121.43 (12)
C1—C6—C5118.23 (13)C5'—C6'—C6120.70 (13)
C1—C6—C6'122.08 (12)O1'—C7'—H7A'109.5
C5—C6—C6'119.69 (13)O1'—C7'—H7B'109.5
O1—C7—H7A109.5H7A'—C7'—H7B'109.5
O1—C7—H7B109.5O1'—C7'—H7C'109.5
H7A—C7—H7B109.5H7A'—C7'—H7C'109.5
O1—C7—H7C109.5H7B'—C7'—H7C'109.5
H7A—C7—H7C109.5O2'—C8'—H8A'109.5
H7B—C7—H7C109.5O2'—C8'—H8B'109.5
O2—C8—H8A109.5H8A'—C8'—H8B'109.5
O2—C8—H8B109.5O2'—C8'—H8C'109.5
H8A—C8—H8B109.5H8A'—C8'—H8C'109.5
O2—C8—H8C109.5H8B'—C8'—H8C'109.5
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8B···O1i0.982.533.495 (2)168
C7—H7A···O2ii0.982.373.332 (2)169
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x1, y+1/2, z1/2.
 

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