Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
Dibothrioclinin I and II, namely (+)-(11R,12S,25R,27S)- and (±)-­(11RS,12RS,25RS,27SR)-3,3,7,17,21-penta­methyl-4,12,18,26-tetraoxahepta­cyclo­[15.11.1.02,15.05,14.06,11.019,28.020,25]­nona­cosa-5(14),6,8,10,19(28),20,22,24-octaene-13,27-dione, respectively, are C30H28O6 epimers which are derived from two bothrioclinin moieties joined so as to create an additional six-membered ring. Structurally, the epimers differ only by inversion at one C atom of a central ring junction and the corresponding six-membered rings have similar conformations in each mol­ecule, except for one ring adjacent to this inversion site.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S010827010301864X/ln1173sup1.cif
Contains datablocks global, I, II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S010827010301864X/ln1173Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S010827010301864X/ln1173IIsup3.hkl
Contains datablock II

CCDC references: 224670; 224671

Comment top

Most coumarins are widely distributed among higher plants, while only a few occur in animals and microorganisms, e.g. aflatoxin from Aspergillus and armillarisin from Armillarialla tabescens. Coumarins and their derivatives are active natural products which have many biological activities, such as anticoagulant, antimicrobial (Kwon et al., 2002) and non-specific spasmolytic action (Oliveira et al., 2001). In recent years, further investigations have indicated that they have anti-HIV activity (Yang, 2001). Therefore, these compounds are widely applied in food, chemical engineering and medical fields and extensive future research into cumarin derivatives is likely.

Gerbera piloselloides (L.) Cass has been used as an antipyretic and alexipharmic agent, and for regulating the flow of vital energy and the condition of the blood in traditional Chinese medicine (Jiangsu New Medical College, 1977). Besides 15 known compounds (Xiao et al.,. 2002), two novel coumarin dimers, dibothrioclinin I and II, hereinafter (I) and (II), respectively, have been isolated from Gerbera piloselloides (L.) Cass. The structures and relative stereochemistry of these two compounds have been established by spectroscopy. The present study reports their crystal structures, which confirms the relative stereochemistry and establishes the conformations of all rings in the molecules. \sch

Dibothrioclinin I, (I) (Fig. 1a), is enantiopure ([α]D = 24°, c 0.05, CHCl3), although the absolute configuration has not been established, while dibothrioclinin II, (II) (Fig. 1 b), is racemic. The compounds are epimers and their skeletons differ only by inversion of the configuration at C12, so that the stereochemistry of the ring C/D junction is cis in (I) and trans in (II). Each compound incorporates two structural units of bothrioclinin (Ferdinand & Christa, 1977) at opposite ends of the molecule. These units are dimerized by the formation of two single bonds, one of which is a direct connection between rings C and E via C11—C27, while the second connects ring C, via C12—C29, to one of the methyl substituents on ring E, thereby building a seventh six-membered ring, D.

The two coumarin skeletons in each structure, rings A/B and F/G, are each almost planar, with a mean deviation of 0.014 (3) Å in (I) and 0.019 (2) Å in (II). The dihedral angles between rings A and B, and between rings F and G, are 2.1 (1) and 3.7 (1)°, respectively, for (I), and 4.1 (1) and 3.7 (1)°, respectively, for (II). These properties are similar to those observed in the structure of ethuliacoumarin A (Larsen et al., 1992).

The corresponding six-membered rings in each compound have similar conformations, except for differences in the conformations of rings C, D and E because of the effect of the inversion at C12. The 2H-dihydropyran ring C adopts a half-chair conformation in (I), with puckering parameters (Cremer & Pople, 1975) Q = 0.444 (3) Å, θ = 128.1 (4)° and ϕ = 98.9 (5)° for the atom sequence O3, C3, C2, C12, C11, C10. In (II), ring C adopts a distorted envelope conformation, with puckering parameters for the corresponding atom sequence Q = 0.525 (3) Å, θ = 122.1 (3)° and ϕ = 46.5 (3)°. The 2H-dihydropyran ring E has an almost ideal envelope form in (I), with puckering parameters Q = 0.544 (3) Å, θ = 55.1 (3)° and ϕ = 240.0 (4)° for the atom sequence O6, C18, C17, C27, C26, C25. In (II), this ring is halfway between an envelope and a half-chair conformation, with puckering parameters for the corresponding atom sequence Q = 0.574 (3) Å, θ = 53.9 (3)° and ϕ = 259.8 (3)°.

The greatest difference between the two compounds lies in the conformation of ring D. In dibothrioclinin I, ring D has a slightly twisted chair conformation owing to the cis fusion with ring C. The puckering parameters are Q = 0.537 (3) Å, θ = 13.5 (4)° and ϕ =241 (2)° for the atom sequence C11, C12, C29, C25, C26, C27. This is also indicated by the smaller C27—C11—C12—C29 and C11—C12—C29—C25 torsion angles of −41.7 (3) and 43.8 (4)°, respectively. The mean of the other four torsion angles is 55.7 (5)° (the torsion angle of the normal chair form of cyclohexane is 56°). In (II), the trans C/D ring junction imposes a conformation on ring D that is halfway between a boat and a twisted boat. The puckering parameters are Q = 0.815 (3) Å, θ = 87.4 (2)° and ϕ = 255.5 (2)°, for the same atom sequence as in (I). This is supported by the C12—C11—C27—C26 and C26—C25—C29—C12 torsion angles of 20.8 (3) and 13.6 (3)°, repsectively. The mean of the other four torsion angles is 55.6 (4)° (the torsion angles of the normal boat form of cyclohexane are 0 and 56°).

Compounds (I) and (II) also exhibit different molecular stereo structures. The dihedral angle between the plane of rings A/B and the least-squares plane through ring C (including puckered atoms) is 4.8 (1)° for (I) and 16.8 (1)° for (II). The dihedral angle between the least-squares planes through rings A/B/C and E/F/G is 72.4 (1)° for (I) and 80.4 (1)° for (II). However, while the inversion at C12 influences the stereochemistry of the ring C/D junction, the stereo structure of rings E, F and G remains unaffected. This can be inferred from the dihedral angle between the plane of rings F/G and the least-squares plane through ring E (including puckered atoms), which is 8.9 (1)° for (I) and 10.9 (1)° for (II).

Experimental top

The roots and rhizomes of Gerbera piloselloides (L.) Cass were collected from DALI, Yunnan Province, China. The air-dried roots and rhizomes (1 kg) were ground to a fine powder and extracted with ethanol, and the ethanol extract was partitioned between an aqueous solution and petroleum ether. The petroleum ether fraction was chromatographed repeatedly on silica gel, eluted with petroleum ether-acetylacetate (9:1), and gave colourless crystals. Purification of the crystals on a preparative high-performance liquid chromatography column afforded compounds (I) (18 mg) and (II) (30 mg). Compound (I) was dissolved in methanol and chloroform (1:1) and stored at room temperature, and transparent block-shaped crystals were obtained after 4 d. Compound (II) was dissolved in chloroform and stored at room temperature, and transparent plate-like crystals were obtained after 7 d.

Refinement top

Due to the absence of any significant anomalous scatterers in (I), attempts to confirm the absolute structure by refinement of the Flack parameter (Flack, 1983) led to an inconclusive value (Flack & Bernardinelli, 2000) for this parameter. Therefore, the enantiomer used in the model was chosen arbitrarily and the Friedel pairs were merged before the final refinement. For both compounds, the methyl H atoms were constrained to an ideal geometry, with Uiso(H) = 1.5Ueq(C), but were allowed to rotate freely about the C—C bonds. All other H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C).

Computing details top

For both compounds, data collection: DENZO (Otwinowski & Minor, 1997); cell refinement: SCALE (Otwinowski & Minor, 1997); data reduction: SCALE; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEPII (Johnson, 1976) and PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97 and PLATON.

Figures top
[Figure 1] Fig. 1. The molecular structures and atomic numbering schemes for (a) (I) and (b) (II). Displacement ellipsoids are drawn at the 30% probability level and H atoms have been omitted for clarity.
(I) (+)-(11R,12S,25R,27S)-3,3,7,17,21-pentamethyl-4,12,18,26- tetraoxaheptacyclo[15.11.1.02,15.05,14.06,11.019,28.020,25] nonacosa-5(14),6,8,10,19 (28),20,22,24-octaene-13,27-dione top
Crystal data top
C30H28O6F(000) = 512
Mr = 484.52Dx = 1.321 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 5888 reflections
a = 11.001 (2) Åθ = 2.4–27.3°
b = 8.307 (2) ŵ = 0.09 mm1
c = 13.332 (3) ÅT = 296 K
β = 90.39 (3)°Block, colourless
V = 1218.3 (4) Å30.4 × 0.2 × 0.1 mm
Z = 2
Data collection top
MAC DIP 2030K area-detector
diffractometer
2715 reflections with I > 2σ(I)
Radiation source: rotating anodeRint = 0.024
Graphite monochromatorθmax = 27.3°, θmin = 2.4°
ω scansh = 014
5888 measured reflectionsk = 010
2725 independent reflectionsl = 1717
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)] = 0.054Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.138H-atom parameters constrained
S = 1.23 w = 1/[σ2(Fo2) + (0.0589P)2 + 0.4086P]
where P = (Fo2 + 2Fc2)/3
2725 reflections(Δ/σ)max = 0.014
325 parametersΔρmax = 0.17 e Å3
1 restraintΔρmin = 0.26 e Å3
Crystal data top
C30H28O6V = 1218.3 (4) Å3
Mr = 484.52Z = 2
Monoclinic, P21Mo Kα radiation
a = 11.001 (2) ŵ = 0.09 mm1
b = 8.307 (2) ÅT = 296 K
c = 13.332 (3) Å0.4 × 0.2 × 0.1 mm
β = 90.39 (3)°
Data collection top
MAC DIP 2030K area-detector
diffractometer
2715 reflections with I > 2σ(I)
5888 measured reflectionsRint = 0.024
2725 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0541 restraint
wR(F2) = 0.138H-atom parameters constrained
S = 1.23Δρmax = 0.17 e Å3
2725 reflectionsΔρmin = 0.26 e Å3
325 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.7355 (3)0.2776 (4)0.14454 (18)0.0643 (8)
O20.8216 (3)0.1374 (4)0.0228 (2)0.0693 (8)
O30.6770 (2)0.6634 (3)0.04218 (18)0.0505 (6)
O40.6584 (2)0.2453 (4)0.45755 (18)0.0531 (6)
O50.6168 (2)0.4948 (4)0.4124 (2)0.0649 (8)
O60.9704 (2)0.2404 (3)0.29082 (16)0.0428 (5)
C10.7763 (4)0.2653 (5)0.0467 (2)0.0530 (9)
C20.7620 (3)0.4032 (4)0.0175 (2)0.0402 (7)
C30.6996 (3)0.5345 (5)0.0158 (2)0.0430 (7)
C40.6504 (3)0.5440 (5)0.1176 (2)0.0491 (8)
C50.5853 (3)0.6767 (6)0.1592 (3)0.0615 (11)
C60.5506 (4)0.6651 (8)0.2605 (3)0.0756 (15)
H6A0.50780.75000.28930.091*
C70.5773 (4)0.5335 (9)0.3187 (3)0.0811 (17)
H7A0.55330.53180.38570.097*
C80.6390 (4)0.4043 (8)0.2791 (3)0.0715 (13)
H8A0.65680.31480.31820.086*
C90.6741 (3)0.4114 (6)0.1787 (3)0.0569 (10)
C100.7515 (3)0.6904 (4)0.1339 (2)0.0434 (7)
C110.7614 (3)0.5278 (4)0.1887 (2)0.0366 (6)
H11A0.67760.49800.20520.044*
C120.8097 (3)0.3885 (4)0.1239 (2)0.0372 (6)
H12A0.77510.28930.15140.045*
C130.5560 (5)0.8283 (8)0.1029 (4)0.0867 (17)
H13A0.51090.89980.14580.130*
H13B0.63010.87950.08190.130*
H13C0.50830.80230.04510.130*
C140.8674 (4)0.7694 (5)0.0978 (3)0.0600 (10)
H14A0.84800.86910.06500.090*
H14B0.90770.69910.05150.090*
H14C0.92000.79000.15410.090*
C150.6741 (5)0.8099 (6)0.1928 (3)0.0711 (13)
H15A0.66980.91000.15700.107*
H15B0.71020.82750.25760.107*
H15C0.59370.76710.20080.107*
C160.6883 (3)0.3854 (5)0.4071 (2)0.0472 (8)
C170.7993 (3)0.3854 (4)0.3504 (2)0.0394 (6)
C180.8705 (3)0.2522 (4)0.3484 (2)0.0368 (6)
C190.8438 (3)0.1088 (4)0.4075 (2)0.0409 (7)
C200.9172 (3)0.0313 (4)0.4168 (2)0.0460 (7)
C210.8725 (4)0.1588 (5)0.4723 (3)0.0560 (9)
H21A0.92060.25000.48040.067*
C220.7584 (4)0.1556 (5)0.5163 (3)0.0619 (11)
H22A0.72970.24600.54980.074*
C230.6882 (4)0.0202 (6)0.5106 (3)0.0598 (10)
H23A0.61250.01630.54130.072*
C240.7323 (3)0.1118 (5)0.4580 (2)0.0473 (8)
C251.0080 (3)0.3801 (4)0.2292 (2)0.0405 (7)
C260.9692 (3)0.5335 (4)0.2813 (2)0.0424 (7)
H26A0.99520.62630.24280.051*
H26B1.00650.53960.34730.051*
C270.8302 (3)0.5333 (4)0.2907 (2)0.0398 (7)
H27A0.80470.62910.32800.048*
C281.0431 (4)0.0474 (5)0.3722 (3)0.0549 (9)
H28A1.07550.15180.38780.082*
H28B1.09530.03420.39980.082*
H28C1.03810.03480.30070.082*
C290.9487 (3)0.3673 (4)0.1257 (2)0.0406 (7)
H29A0.96800.26270.09760.049*
H29B0.98430.44820.08240.049*
C301.1448 (3)0.3621 (6)0.2214 (3)0.0552 (9)
H30A1.18080.37100.28690.083*
H30B1.17640.44530.17890.083*
H30C1.16380.25880.19330.083*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0834 (19)0.0721 (19)0.0375 (12)0.0012 (17)0.0058 (12)0.0085 (13)
O20.102 (2)0.0495 (16)0.0560 (15)0.0131 (16)0.0114 (15)0.0132 (13)
O30.0520 (13)0.0516 (15)0.0478 (12)0.0145 (12)0.0099 (10)0.0030 (11)
O40.0447 (12)0.0690 (17)0.0458 (12)0.0008 (13)0.0114 (10)0.0099 (12)
O50.0554 (15)0.074 (2)0.0653 (16)0.0142 (15)0.0178 (12)0.0005 (15)
O60.0416 (11)0.0459 (13)0.0410 (11)0.0060 (10)0.0097 (9)0.0082 (10)
C10.066 (2)0.057 (2)0.0369 (15)0.0011 (19)0.0031 (14)0.0067 (16)
C20.0416 (14)0.0441 (17)0.0347 (14)0.0015 (14)0.0004 (11)0.0002 (13)
C30.0380 (14)0.0526 (19)0.0385 (14)0.0010 (14)0.0024 (11)0.0016 (14)
C40.0349 (14)0.072 (2)0.0401 (15)0.0041 (16)0.0005 (12)0.0096 (17)
C50.0353 (15)0.095 (3)0.0542 (19)0.0025 (19)0.0031 (14)0.025 (2)
C60.0463 (19)0.122 (4)0.058 (2)0.001 (2)0.0114 (17)0.034 (3)
C70.054 (2)0.147 (5)0.0418 (18)0.019 (3)0.0100 (16)0.020 (3)
C80.064 (2)0.112 (4)0.0389 (17)0.019 (3)0.0048 (16)0.000 (2)
C90.0471 (18)0.083 (3)0.0407 (16)0.011 (2)0.0017 (13)0.0060 (18)
C100.0494 (17)0.0422 (17)0.0387 (15)0.0101 (14)0.0012 (12)0.0009 (13)
C110.0341 (12)0.0411 (16)0.0345 (13)0.0047 (12)0.0023 (10)0.0012 (12)
C120.0389 (14)0.0399 (15)0.0329 (13)0.0027 (13)0.0031 (10)0.0017 (12)
C130.074 (3)0.107 (4)0.078 (3)0.043 (3)0.007 (2)0.024 (3)
C140.061 (2)0.047 (2)0.072 (2)0.0025 (18)0.0037 (18)0.0141 (19)
C150.091 (3)0.058 (3)0.064 (2)0.039 (2)0.001 (2)0.0062 (19)
C160.0432 (16)0.063 (2)0.0356 (14)0.0014 (17)0.0065 (12)0.0004 (16)
C170.0421 (15)0.0465 (17)0.0295 (12)0.0019 (15)0.0035 (11)0.0021 (13)
C180.0370 (13)0.0433 (16)0.0302 (12)0.0047 (13)0.0016 (10)0.0033 (12)
C190.0466 (16)0.0460 (18)0.0301 (13)0.0047 (14)0.0012 (11)0.0021 (12)
C200.0574 (18)0.0438 (18)0.0368 (15)0.0058 (16)0.0084 (13)0.0015 (14)
C210.074 (2)0.049 (2)0.0451 (18)0.0082 (19)0.0086 (16)0.0045 (16)
C220.079 (3)0.058 (2)0.0483 (19)0.022 (2)0.0058 (18)0.0136 (17)
C230.056 (2)0.079 (3)0.0441 (17)0.021 (2)0.0030 (15)0.0102 (19)
C240.0467 (16)0.060 (2)0.0353 (14)0.0066 (16)0.0005 (13)0.0051 (15)
C250.0366 (14)0.0464 (17)0.0385 (14)0.0014 (14)0.0042 (11)0.0071 (14)
C260.0417 (15)0.0445 (17)0.0411 (15)0.0029 (14)0.0009 (12)0.0035 (14)
C270.0420 (15)0.0423 (17)0.0349 (14)0.0025 (14)0.0000 (11)0.0024 (13)
C280.061 (2)0.046 (2)0.057 (2)0.0079 (17)0.0001 (16)0.0012 (16)
C290.0397 (14)0.0477 (18)0.0344 (13)0.0071 (14)0.0071 (11)0.0041 (13)
C300.0347 (15)0.074 (3)0.0568 (19)0.0051 (17)0.0041 (13)0.0174 (19)
Geometric parameters (Å, º) top
O1—C91.376 (6)C14—H14A0.9600
O1—C11.380 (4)C14—H14B0.9600
O2—C11.215 (5)C14—H14C0.9600
O3—C31.344 (4)C15—H15A0.9600
O3—C101.484 (4)C15—H15B0.9600
O4—C241.375 (5)C15—H15C0.9600
O4—C161.385 (5)C16—C171.440 (4)
O5—C161.205 (5)C17—C181.356 (5)
O6—C181.348 (3)C17—C271.505 (5)
O6—C251.482 (4)C18—C191.460 (4)
C1—C21.440 (5)C19—C241.403 (5)
C2—C31.362 (5)C19—C201.421 (5)
C2—C121.514 (4)C20—C211.384 (5)
C3—C41.461 (4)C20—C281.517 (5)
C4—C91.395 (6)C21—C221.389 (6)
C4—C51.425 (6)C21—H21A0.9300
C5—C61.404 (6)C22—C231.367 (7)
C5—C131.502 (8)C22—H22A0.9300
C6—C71.374 (8)C23—C241.391 (5)
C6—H6A0.9300C23—H23A0.9300
C7—C81.373 (8)C25—C261.514 (5)
C7—H7A0.9300C25—C301.517 (4)
C8—C91.392 (5)C25—C291.526 (4)
C8—H8A0.9300C26—C271.535 (4)
C10—C141.516 (5)C26—H26A0.9700
C10—C151.529 (5)C26—H26B0.9700
C10—C111.539 (4)C27—H27A0.9800
C11—C121.540 (4)C28—H28A0.9600
C11—C271.552 (4)C28—H28B0.9600
C11—H11A0.9800C28—H28C0.9600
C12—C291.539 (4)C29—H29A0.9700
C12—H12A0.9800C29—H29B0.9700
C13—H13A0.9600C30—H30A0.9600
C13—H13B0.9600C30—H30B0.9600
C13—H13C0.9600C30—H30C0.9600
C9—O1—C1121.9 (3)H15A—C15—H15C109.5
C3—O3—C10119.3 (2)H15B—C15—H15C109.5
C24—O4—C16122.5 (2)O5—C16—O4116.6 (3)
C18—O6—C25119.3 (2)O5—C16—C17126.0 (4)
O2—C1—O1116.3 (3)O4—C16—C17117.4 (3)
O2—C1—C2125.9 (3)C18—C17—C16120.2 (3)
O1—C1—C2117.8 (3)C18—C17—C27121.5 (2)
C3—C2—C1120.1 (3)C16—C17—C27118.2 (3)
C3—C2—C12122.7 (3)O6—C18—C17123.0 (3)
C1—C2—C12117.0 (3)O6—C18—C19114.6 (3)
O3—C3—C2123.1 (3)C17—C18—C19122.5 (3)
O3—C3—C4115.0 (3)C24—C19—C20118.1 (3)
C2—C3—C4121.9 (3)C24—C19—C18115.1 (3)
C9—C4—C5118.6 (3)C20—C19—C18126.8 (3)
C9—C4—C3115.5 (3)C21—C20—C19118.0 (3)
C5—C4—C3125.8 (4)C21—C20—C28118.1 (3)
C6—C5—C4117.0 (5)C19—C20—C28123.9 (3)
C6—C5—C13118.7 (4)C20—C21—C22122.5 (4)
C4—C5—C13124.3 (3)C20—C21—H21A118.8
C7—C6—C5122.7 (5)C22—C21—H21A118.8
C7—C6—H6A118.7C23—C22—C21120.3 (4)
C5—C6—H6A118.7C23—C22—H22A119.9
C8—C7—C6120.8 (4)C21—C22—H22A119.9
C8—C7—H7A119.6C22—C23—C24118.5 (3)
C6—C7—H7A119.6C22—C23—H23A120.7
C7—C8—C9118.0 (5)C24—C23—H23A120.7
C7—C8—H8A121.0O4—C24—C23115.4 (3)
C9—C8—H8A121.0O4—C24—C19122.1 (3)
O1—C9—C8114.6 (4)C23—C24—C19122.5 (4)
O1—C9—C4122.5 (3)O6—C25—C26108.9 (2)
C8—C9—C4122.9 (4)O6—C25—C30104.0 (3)
O3—C10—C14105.4 (3)C26—C25—C30113.4 (3)
O3—C10—C15102.4 (3)O6—C25—C29109.1 (3)
C14—C10—C15110.8 (4)C26—C25—C29110.7 (3)
O3—C10—C11107.2 (3)C30—C25—C29110.5 (3)
C14—C10—C11118.3 (3)C25—C26—C27108.7 (3)
C15—C10—C11111.3 (3)C25—C26—H26A110.0
C10—C11—C12114.6 (2)C27—C26—H26A110.0
C10—C11—C27115.0 (3)C25—C26—H26B110.0
C12—C11—C27110.2 (2)C27—C26—H26B110.0
C10—C11—H11A105.3H26A—C26—H26B108.3
C12—C11—H11A105.3C17—C27—C26105.8 (3)
C27—C11—H11A105.3C17—C27—C11109.2 (3)
C2—C12—C29111.2 (2)C26—C27—C11114.1 (2)
C2—C12—C11110.3 (3)C17—C27—H27A109.2
C29—C12—C11115.1 (3)C26—C27—H27A109.2
C2—C12—H12A106.6C11—C27—H27A109.2
C29—C12—H12A106.6C20—C28—H28A109.5
C11—C12—H12A106.6C20—C28—H28B109.5
C5—C13—H13A109.5H28A—C28—H28B109.5
C5—C13—H13B109.5C20—C28—H28C109.5
H13A—C13—H13B109.5H28A—C28—H28C109.5
C5—C13—H13C109.5H28B—C28—H28C109.5
H13A—C13—H13C109.5C25—C29—C12115.1 (2)
H13B—C13—H13C109.5C25—C29—H29A108.5
C10—C14—H14A109.5C12—C29—H29A108.5
C10—C14—H14B109.5C25—C29—H29B108.5
H14A—C14—H14B109.5C12—C29—H29B108.5
C10—C14—H14C109.5H29A—C29—H29B107.5
H14A—C14—H14C109.5C25—C30—H30A109.5
H14B—C14—H14C109.5C25—C30—H30B109.5
C10—C15—H15A109.5H30A—C30—H30B109.5
C10—C15—H15B109.5C25—C30—H30C109.5
H15A—C15—H15B109.5H30A—C30—H30C109.5
C10—C15—H15C109.5H30B—C30—H30C109.5
C9—O1—C1—O2174.9 (4)O5—C16—C17—C18178.1 (3)
C9—O1—C1—C25.1 (5)O4—C16—C17—C180.5 (4)
O2—C1—C2—C3173.9 (4)O5—C16—C17—C270.7 (5)
O1—C1—C2—C36.1 (5)O4—C16—C17—C27176.9 (3)
O2—C1—C2—C121.2 (6)C25—O6—C18—C172.3 (4)
O1—C1—C2—C12178.8 (3)C25—O6—C18—C19178.6 (3)
C10—O3—C3—C219.3 (5)C16—C17—C18—O6174.8 (3)
C10—O3—C3—C4161.6 (3)C27—C17—C18—O62.5 (5)
C1—C2—C3—O3176.1 (3)C16—C17—C18—C194.2 (4)
C12—C2—C3—O31.3 (5)C27—C17—C18—C19178.5 (3)
C1—C2—C3—C42.9 (5)O6—C18—C19—C24172.4 (3)
C12—C2—C3—C4177.7 (3)C17—C18—C19—C246.7 (4)
O3—C3—C4—C9179.6 (3)O6—C18—C19—C206.2 (4)
C2—C3—C4—C91.4 (5)C17—C18—C19—C20174.7 (3)
O3—C3—C4—C51.6 (5)C24—C19—C20—C212.2 (4)
C2—C3—C4—C5179.3 (3)C18—C19—C20—C21176.4 (3)
C9—C4—C5—C60.9 (5)C24—C19—C20—C28175.9 (3)
C3—C4—C5—C6177.0 (3)C18—C19—C20—C285.5 (5)
C9—C4—C5—C13178.6 (4)C19—C20—C21—C221.7 (5)
C3—C4—C5—C130.7 (6)C28—C20—C21—C22179.9 (3)
C4—C5—C6—C70.2 (6)C20—C21—C22—C233.6 (6)
C13—C5—C6—C7177.7 (4)C21—C22—C23—C241.5 (6)
C5—C6—C7—C80.8 (7)C16—O4—C24—C23178.9 (3)
C6—C7—C8—C90.4 (6)C16—O4—C24—C190.3 (5)
C1—O1—C9—C8179.9 (3)C22—C23—C24—O4178.3 (3)
C1—O1—C9—C40.8 (5)C22—C23—C24—C192.4 (5)
C7—C8—C9—O1180.0 (4)C20—C19—C24—O4176.5 (3)
C7—C8—C9—C40.7 (6)C18—C19—C24—O44.7 (4)
C5—C4—C9—O1179.4 (3)C20—C19—C24—C234.3 (5)
C3—C4—C9—O12.5 (5)C18—C19—C24—C23174.4 (3)
C5—C4—C9—C81.3 (5)C18—O6—C25—C2629.9 (3)
C3—C4—C9—C8176.8 (3)C18—O6—C25—C30151.1 (3)
C3—O3—C10—C1481.3 (4)C18—O6—C25—C2991.0 (3)
C3—O3—C10—C15162.8 (3)O6—C25—C26—C2761.2 (3)
C3—O3—C10—C1145.5 (4)C30—C25—C26—C27176.4 (3)
O3—C10—C11—C1254.3 (3)C29—C25—C26—C2758.8 (3)
C14—C10—C11—C1264.6 (4)C18—C17—C27—C2628.6 (4)
C15—C10—C11—C12165.5 (3)C16—C17—C27—C26154.0 (3)
O3—C10—C11—C27176.5 (2)C18—C17—C27—C1194.6 (3)
C14—C10—C11—C2764.6 (4)C16—C17—C27—C1182.7 (3)
C15—C10—C11—C2765.3 (4)C25—C26—C27—C1759.2 (3)
C3—C2—C12—C29120.7 (3)C25—C26—C27—C1160.9 (4)
C1—C2—C12—C2964.4 (4)C10—C11—C27—C17161.9 (2)
C3—C2—C12—C118.2 (4)C12—C11—C27—C1766.7 (3)
C1—C2—C12—C11166.7 (3)C10—C11—C27—C2679.9 (3)
C10—C11—C12—C236.9 (4)C12—C11—C27—C2651.4 (4)
C27—C11—C12—C2168.4 (2)O6—C25—C29—C1267.9 (4)
C10—C11—C12—C2989.9 (3)C26—C25—C29—C1251.9 (4)
C27—C11—C12—C2941.7 (3)C30—C25—C29—C12178.3 (3)
C24—O4—C16—O5179.7 (3)C2—C12—C29—C25170.0 (3)
C24—O4—C16—C172.5 (5)C11—C12—C29—C2543.8 (4)
(II) (±)-(11RS,12RS,25RS,27SR)-3,3,7,17,21-pentamethyl-4,12,18,26- tetraoxaheptacyclo[15.11.1.02,15.05,14.06,11.019,28.020,25] nonacosa-5(14),6,8,10,19 (28),20,22,24-octaene-13,27-dione top
Crystal data top
C30H28O6F(000) = 1024
Mr = 484.52Dx = 1.377 Mg m3
Monoclinic, P121/c1Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 15334 reflections
a = 15.517 (3) Åθ = 2.5–27.4°
b = 19.411 (4) ŵ = 0.10 mm1
c = 7.963 (2) ÅT = 296 K
β = 102.90 (3)°Block, colourless
V = 2337.9 (9) Å30.5 × 0.3 × 0.1 mm
Z = 4
Data collection top
Rigaku RAXIS-RAPID area-detector
diffractometer
2479 reflections with I > 2σ(I)
Radiation source: rotating anodeRint = 0.070
Graphite monochromatorθmax = 27.4°, θmin = 1.4°
ω scansh = 2019
15334 measured reflectionsk = 250
5186 independent reflectionsl = 010
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)] = 0.057Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.161H-atom parameters constrained
S = 0.84 w = 1/[σ2(Fo2) + (0.0719P)2]
where P = (Fo2 + 2Fc2)/3
5186 reflections(Δ/σ)max = 0.001
325 parametersΔρmax = 0.28 e Å3
0 restraintsΔρmin = 0.30 e Å3
Crystal data top
C30H28O6V = 2337.9 (9) Å3
Mr = 484.52Z = 4
Monoclinic, P121/c1Mo Kα radiation
a = 15.517 (3) ŵ = 0.10 mm1
b = 19.411 (4) ÅT = 296 K
c = 7.963 (2) Å0.5 × 0.3 × 0.1 mm
β = 102.90 (3)°
Data collection top
Rigaku RAXIS-RAPID area-detector
diffractometer
2479 reflections with I > 2σ(I)
15334 measured reflectionsRint = 0.070
5186 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0570 restraints
wR(F2) = 0.161H-atom parameters constrained
S = 0.84Δρmax = 0.28 e Å3
5186 reflectionsΔρmin = 0.30 e Å3
325 parameters
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.03621 (11)0.47239 (9)0.7275 (2)0.0259 (4)
O20.15966 (12)0.52699 (10)0.8351 (2)0.0386 (5)
O30.05187 (11)0.35392 (9)1.1577 (2)0.0313 (5)
O40.43745 (11)0.22477 (9)1.1862 (2)0.0263 (4)
O50.31980 (13)0.21359 (9)1.2955 (3)0.0361 (5)
O60.43873 (11)0.43504 (9)1.2440 (2)0.0228 (4)
C10.10974 (17)0.48231 (14)0.8602 (3)0.0261 (6)
C20.11841 (16)0.43835 (13)1.0101 (3)0.0204 (6)
C30.05082 (16)0.39516 (13)1.0219 (3)0.0212 (6)
C40.02983 (16)0.38913 (13)0.8876 (3)0.0211 (6)
C50.10339 (17)0.34695 (13)0.8915 (3)0.0261 (6)
C60.17184 (17)0.34547 (14)0.7468 (4)0.0312 (7)
H6A0.22160.31900.74910.037*
C70.16915 (18)0.38181 (14)0.5988 (4)0.0308 (7)
H7A0.21560.37820.50260.037*
C80.09805 (17)0.42330 (14)0.5931 (3)0.0263 (6)
H8A0.09550.44790.49410.032*
C90.03088 (16)0.42733 (13)0.7378 (3)0.0220 (6)
C100.13262 (16)0.34270 (13)1.2957 (3)0.0217 (6)
C110.21214 (15)0.36568 (12)1.2283 (3)0.0189 (6)
H11A0.21490.33551.13100.023*
C120.19930 (15)0.43949 (12)1.1563 (3)0.0197 (6)
H12A0.18580.46901.24700.024*
C130.11279 (18)0.30387 (14)1.0449 (4)0.0384 (8)
H13A0.16770.27911.01750.058*
H13B0.11190.33341.14200.058*
H13C0.06470.27171.07250.058*
C140.11824 (19)0.38248 (14)1.4530 (3)0.0318 (7)
H14A0.06700.36481.48720.048*
H14B0.10960.43041.42440.048*
H14C0.16910.37721.54610.048*
C150.13023 (18)0.26571 (13)1.3266 (3)0.0277 (6)
H15A0.13940.24161.22680.042*
H15B0.07380.25331.34810.042*
H15C0.17610.25361.42460.042*
C160.37286 (17)0.25337 (14)1.2595 (3)0.0249 (6)
C170.37308 (16)0.32691 (13)1.2810 (3)0.0198 (6)
C180.43707 (16)0.36570 (13)1.2355 (3)0.0213 (6)
C190.51009 (16)0.33507 (14)1.1732 (3)0.0214 (6)
C200.58517 (17)0.36972 (14)1.1419 (3)0.0260 (6)
C210.64612 (18)0.33189 (15)1.0763 (3)0.0296 (7)
H21A0.69510.35431.05290.036*
C220.63622 (18)0.26188 (15)1.0448 (3)0.0312 (7)
H22A0.67740.23840.99750.037*
C230.56672 (17)0.22700 (14)1.0823 (3)0.0277 (7)
H23A0.56080.17971.06400.033*
C240.50492 (17)0.26356 (14)1.1483 (3)0.0230 (6)
C250.36000 (16)0.46824 (13)1.2812 (3)0.0207 (6)
C260.33610 (16)0.42898 (12)1.4302 (3)0.0214 (6)
H26A0.29050.45331.47230.026*
H26B0.38760.42411.52430.026*
C270.30265 (16)0.35833 (12)1.3606 (3)0.0209 (6)
H27A0.29460.32931.45660.025*
C280.60413 (18)0.44519 (14)1.1780 (4)0.0330 (7)
H28A0.65820.45741.14580.050*
H28B0.60980.45401.29860.050*
H28C0.55650.47221.11250.050*
C290.28511 (16)0.46543 (13)1.1169 (3)0.0218 (6)
H29A0.27580.51111.06670.026*
H29B0.30250.43521.03330.026*
C300.38962 (17)0.54159 (13)1.3277 (3)0.0285 (7)
H30A0.43570.54151.43080.043*
H30B0.34040.56811.34670.043*
H30C0.41150.56171.23520.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0253 (10)0.0285 (11)0.0227 (10)0.0034 (8)0.0029 (8)0.0051 (8)
O20.0364 (12)0.0387 (13)0.0368 (12)0.0130 (10)0.0001 (10)0.0183 (10)
O30.0210 (10)0.0423 (13)0.0296 (11)0.0046 (9)0.0037 (8)0.0168 (9)
O40.0249 (10)0.0233 (10)0.0305 (10)0.0026 (8)0.0057 (9)0.0056 (8)
O50.0371 (12)0.0228 (11)0.0523 (13)0.0039 (9)0.0185 (10)0.0036 (10)
O60.0196 (9)0.0197 (10)0.0310 (10)0.0005 (8)0.0098 (8)0.0011 (8)
C10.0247 (15)0.0248 (15)0.0288 (15)0.0023 (12)0.0062 (13)0.0018 (12)
C20.0221 (14)0.0182 (14)0.0231 (14)0.0012 (11)0.0092 (11)0.0009 (11)
C30.0223 (14)0.0207 (14)0.0228 (14)0.0045 (11)0.0094 (12)0.0024 (11)
C40.0200 (14)0.0210 (15)0.0223 (14)0.0030 (11)0.0045 (12)0.0014 (11)
C50.0232 (15)0.0232 (15)0.0326 (16)0.0020 (12)0.0079 (13)0.0009 (12)
C60.0171 (14)0.0272 (16)0.0501 (19)0.0042 (12)0.0090 (14)0.0021 (14)
C70.0244 (15)0.0310 (16)0.0334 (16)0.0018 (12)0.0014 (13)0.0063 (13)
C80.0265 (15)0.0280 (16)0.0241 (15)0.0055 (12)0.0055 (13)0.0006 (12)
C90.0221 (14)0.0215 (14)0.0213 (14)0.0014 (11)0.0029 (11)0.0039 (11)
C100.0194 (14)0.0223 (14)0.0225 (14)0.0005 (11)0.0031 (12)0.0042 (11)
C110.0231 (14)0.0170 (14)0.0175 (13)0.0005 (11)0.0062 (11)0.0013 (10)
C120.0212 (14)0.0192 (14)0.0179 (13)0.0003 (11)0.0027 (11)0.0004 (11)
C130.0237 (16)0.0418 (19)0.0486 (19)0.0081 (14)0.0059 (14)0.0150 (16)
C140.0380 (17)0.0322 (17)0.0306 (16)0.0005 (14)0.0192 (14)0.0004 (13)
C150.0323 (16)0.0249 (15)0.0275 (15)0.0031 (12)0.0102 (13)0.0048 (12)
C160.0240 (15)0.0287 (16)0.0203 (14)0.0022 (13)0.0013 (12)0.0015 (12)
C170.0216 (14)0.0206 (14)0.0160 (13)0.0019 (11)0.0016 (11)0.0014 (11)
C180.0214 (14)0.0225 (15)0.0185 (13)0.0027 (12)0.0011 (11)0.0018 (11)
C190.0195 (14)0.0277 (15)0.0154 (13)0.0028 (12)0.0005 (11)0.0006 (11)
C200.0236 (15)0.0321 (16)0.0219 (14)0.0012 (12)0.0043 (12)0.0032 (12)
C210.0272 (16)0.0394 (18)0.0239 (14)0.0046 (13)0.0094 (13)0.0055 (13)
C220.0264 (16)0.0425 (19)0.0245 (15)0.0139 (14)0.0052 (13)0.0000 (13)
C230.0273 (15)0.0283 (16)0.0243 (15)0.0085 (13)0.0009 (12)0.0028 (12)
C240.0225 (14)0.0279 (16)0.0173 (13)0.0026 (12)0.0018 (11)0.0003 (11)
C250.0167 (13)0.0201 (14)0.0266 (14)0.0012 (11)0.0072 (12)0.0017 (11)
C260.0188 (13)0.0233 (14)0.0222 (14)0.0004 (11)0.0044 (11)0.0039 (11)
C270.0233 (14)0.0196 (14)0.0198 (13)0.0005 (11)0.0053 (11)0.0027 (11)
C280.0286 (16)0.0366 (18)0.0372 (17)0.0033 (13)0.0147 (13)0.0014 (14)
C290.0227 (14)0.0224 (14)0.0203 (13)0.0025 (11)0.0047 (11)0.0027 (11)
C300.0286 (16)0.0258 (15)0.0308 (15)0.0010 (12)0.0058 (13)0.0018 (12)
Geometric parameters (Å, º) top
O1—C91.376 (3)C14—H14A0.9600
O1—C11.385 (3)C14—H14B0.9600
O2—C11.209 (3)C14—H14C0.9600
O3—C31.343 (3)C15—H15A0.9600
O3—C101.486 (3)C15—H15B0.9600
O4—C241.377 (3)C15—H15C0.9600
O4—C161.384 (3)C16—C171.438 (4)
O5—C161.209 (3)C17—C181.358 (3)
O6—C181.348 (3)C17—C271.509 (3)
O6—C251.469 (3)C18—C191.461 (4)
C1—C21.449 (3)C19—C241.402 (3)
C2—C31.362 (3)C19—C201.415 (4)
C2—C121.509 (3)C20—C211.388 (4)
C3—C41.458 (3)C20—C281.509 (4)
C4—C91.401 (3)C21—C221.384 (4)
C4—C51.411 (3)C21—H21A0.9300
C5—C61.382 (4)C22—C231.362 (4)
C5—C131.514 (4)C22—H22A0.9300
C6—C71.382 (4)C23—C241.387 (3)
C6—H6A0.9300C23—H23A0.9300
C7—C81.375 (4)C25—C301.517 (3)
C7—H7A0.9300C25—C261.524 (3)
C8—C91.372 (3)C25—C291.545 (3)
C8—H8A0.9300C26—C271.526 (3)
C10—C151.516 (4)C26—H26A0.9700
C10—C111.518 (3)C26—H26B0.9700
C10—C141.530 (3)C27—H27A0.9800
C11—C121.540 (3)C28—H28A0.9600
C11—C271.563 (3)C28—H28B0.9600
C11—H11A0.9800C28—H28C0.9600
C12—C291.520 (3)C29—H29A0.9700
C12—H12A0.9800C29—H29B0.9700
C13—H13A0.9600C30—H30A0.9600
C13—H13B0.9600C30—H30B0.9600
C13—H13C0.9600C30—H30C0.9600
C9—O1—C1123.2 (2)H15A—C15—H15C109.5
C3—O3—C10122.63 (19)H15B—C15—H15C109.5
C24—O4—C16122.1 (2)O5—C16—O4116.1 (2)
C18—O6—C25116.16 (19)O5—C16—C17126.1 (3)
O2—C1—O1115.0 (2)O4—C16—C17117.8 (2)
O2—C1—C2127.9 (2)C18—C17—C16120.1 (2)
O1—C1—C2117.1 (2)C18—C17—C27121.9 (2)
C3—C2—C1119.2 (2)C16—C17—C27117.9 (2)
C3—C2—C12118.5 (2)O6—C18—C17123.2 (2)
C1—C2—C12122.3 (2)O6—C18—C19114.6 (2)
O3—C3—C2123.5 (2)C17—C18—C19122.2 (2)
O3—C3—C4113.4 (2)C24—C19—C20118.0 (2)
C2—C3—C4123.1 (2)C24—C19—C18115.3 (2)
C9—C4—C5118.1 (2)C20—C19—C18126.7 (2)
C9—C4—C3115.3 (2)C21—C20—C19118.1 (3)
C5—C4—C3126.6 (2)C21—C20—C28117.7 (3)
C6—C5—C4117.9 (2)C19—C20—C28124.1 (2)
C6—C5—C13117.8 (2)C22—C21—C20122.0 (3)
C4—C5—C13124.3 (2)C22—C21—H21A119.0
C7—C6—C5122.4 (3)C20—C21—H21A119.0
C7—C6—H6A118.8C23—C22—C21120.6 (3)
C5—C6—H6A118.8C23—C22—H22A119.7
C8—C7—C6120.3 (3)C21—C22—H22A119.7
C8—C7—H7A119.9C22—C23—C24118.5 (3)
C6—C7—H7A119.9C22—C23—H23A120.8
C9—C8—C7118.1 (3)C24—C23—H23A120.8
C9—C8—H8A121.0O4—C24—C23115.3 (2)
C7—C8—H8A121.0O4—C24—C19122.2 (2)
C8—C9—O1115.4 (2)C23—C24—C19122.5 (3)
C8—C9—C4123.1 (3)O6—C25—C30103.93 (19)
O1—C9—C4121.5 (2)O6—C25—C26107.21 (19)
O3—C10—C15102.56 (19)C30—C25—C26113.1 (2)
O3—C10—C11108.26 (18)O6—C25—C29108.41 (19)
C15—C10—C11113.5 (2)C30—C25—C29111.7 (2)
O3—C10—C14106.1 (2)C26—C25—C29112.0 (2)
C15—C10—C14110.6 (2)C25—C26—C27106.8 (2)
C11—C10—C14114.8 (2)C25—C26—H26A110.4
C10—C11—C12110.9 (2)C27—C26—H26A110.4
C10—C11—C27114.45 (19)C25—C26—H26B110.4
C12—C11—C27110.99 (19)C27—C26—H26B110.4
C10—C11—H11A106.7H26A—C26—H26B108.6
C12—C11—H11A106.7C17—C27—C26107.2 (2)
C27—C11—H11A106.7C17—C27—C11112.3 (2)
C2—C12—C29117.5 (2)C26—C27—C11110.1 (2)
C2—C12—C11106.84 (19)C17—C27—H27A109.0
C29—C12—C11109.8 (2)C26—C27—H27A109.0
C2—C12—H12A107.4C11—C27—H27A109.0
C29—C12—H12A107.4C20—C28—H28A109.5
C11—C12—H12A107.4C20—C28—H28B109.5
C5—C13—H13A109.5H28A—C28—H28B109.5
C5—C13—H13B109.5C20—C28—H28C109.5
H13A—C13—H13B109.5H28A—C28—H28C109.5
C5—C13—H13C109.5H28B—C28—H28C109.5
H13A—C13—H13C109.5C12—C29—C25111.4 (2)
H13B—C13—H13C109.5C12—C29—H29A109.3
C10—C14—H14A109.5C25—C29—H29A109.3
C10—C14—H14B109.5C12—C29—H29B109.3
H14A—C14—H14B109.5C25—C29—H29B109.3
C10—C14—H14C109.5H29A—C29—H29B108.0
H14A—C14—H14C109.5C25—C30—H30A109.5
H14B—C14—H14C109.5C25—C30—H30B109.5
C10—C15—H15A109.5H30A—C30—H30B109.5
C10—C15—H15B109.5C25—C30—H30C109.5
H15A—C15—H15B109.5H30A—C30—H30C109.5
C10—C15—H15C109.5H30B—C30—H30C109.5
C9—O1—C1—O2175.3 (2)O5—C16—C17—C18179.8 (2)
C9—O1—C1—C25.3 (3)O4—C16—C17—C182.2 (3)
O2—C1—C2—C3173.8 (3)O5—C16—C17—C272.0 (4)
O1—C1—C2—C36.8 (4)O4—C16—C17—C27179.9 (2)
O2—C1—C2—C125.1 (4)C25—O6—C18—C178.8 (3)
O1—C1—C2—C12174.3 (2)C25—O6—C18—C19171.27 (19)
C10—O3—C3—C210.4 (4)C16—C17—C18—O6176.6 (2)
C10—O3—C3—C4169.5 (2)C27—C17—C18—O65.7 (4)
C1—C2—C3—O3178.2 (2)C16—C17—C18—C193.5 (4)
C12—C2—C3—O30.7 (4)C27—C17—C18—C19174.2 (2)
C1—C2—C3—C41.9 (4)O6—C18—C19—C24174.3 (2)
C12—C2—C3—C4179.1 (2)C17—C18—C19—C245.8 (3)
O3—C3—C4—C9175.3 (2)O6—C18—C19—C207.9 (3)
C2—C3—C4—C94.5 (4)C17—C18—C19—C20172.0 (2)
O3—C3—C4—C51.6 (4)C24—C19—C20—C214.7 (3)
C2—C3—C4—C5178.5 (3)C18—C19—C20—C21177.6 (2)
C9—C4—C5—C60.5 (4)C24—C19—C20—C28174.3 (2)
C3—C4—C5—C6176.4 (2)C18—C19—C20—C283.4 (4)
C9—C4—C5—C13178.7 (2)C19—C20—C21—C221.4 (4)
C3—C4—C5—C134.4 (4)C28—C20—C21—C22177.7 (2)
C4—C5—C6—C72.0 (4)C20—C21—C22—C231.9 (4)
C13—C5—C6—C7178.7 (3)C21—C22—C23—C241.7 (4)
C5—C6—C7—C82.3 (4)C16—O4—C24—C23177.3 (2)
C6—C7—C8—C90.1 (4)C16—O4—C24—C193.3 (3)
C7—C8—C9—O1176.7 (2)C22—C23—C24—O4178.8 (2)
C7—C8—C9—C42.7 (4)C22—C23—C24—C191.8 (4)
C1—O1—C9—C8179.1 (2)C20—C19—C24—O4175.6 (2)
C1—O1—C9—C41.5 (4)C18—C19—C24—O42.4 (3)
C5—C4—C9—C82.9 (4)C20—C19—C24—C235.0 (4)
C3—C4—C9—C8174.3 (2)C18—C19—C24—C23177.0 (2)
C5—C4—C9—O1176.5 (2)C18—O6—C25—C30165.99 (19)
C3—C4—C9—O16.3 (3)C18—O6—C25—C2646.0 (3)
C3—O3—C10—C15137.4 (2)C18—O6—C25—C2975.1 (2)
C3—O3—C10—C1117.2 (3)O6—C25—C26—C2769.4 (2)
C3—O3—C10—C14106.6 (2)C30—C25—C26—C27176.7 (2)
O3—C10—C11—C1252.4 (3)C29—C25—C26—C2749.4 (3)
C15—C10—C11—C12165.5 (2)C18—C17—C27—C2618.7 (3)
C14—C10—C11—C1266.0 (3)C16—C17—C27—C26159.1 (2)
O3—C10—C11—C27178.91 (19)C18—C17—C27—C11102.5 (3)
C15—C10—C11—C2768.0 (3)C16—C17—C27—C1179.8 (3)
C14—C10—C11—C2760.5 (3)C25—C26—C27—C1754.1 (2)
C3—C2—C12—C29157.7 (2)C25—C26—C27—C1168.3 (2)
C1—C2—C12—C2923.5 (3)C10—C11—C27—C17134.9 (2)
C3—C2—C12—C1133.8 (3)C12—C11—C27—C1798.6 (2)
C1—C2—C12—C11147.3 (2)C10—C11—C27—C26105.6 (2)
C10—C11—C12—C260.7 (2)C12—C11—C27—C2620.8 (3)
C27—C11—C12—C2170.86 (19)C2—C12—C29—C25176.1 (2)
C10—C11—C12—C29170.81 (19)C11—C12—C29—C2561.6 (3)
C27—C11—C12—C2942.4 (3)O6—C25—C29—C12131.7 (2)
C24—O4—C16—O5176.1 (2)C30—C25—C29—C12114.4 (2)
C24—O4—C16—C175.7 (3)C26—C25—C29—C1213.6 (3)

Experimental details

(I)(II)
Crystal data
Chemical formulaC30H28O6C30H28O6
Mr484.52484.52
Crystal system, space groupMonoclinic, P21Monoclinic, P121/c1
Temperature (K)296296
a, b, c (Å)11.001 (2), 8.307 (2), 13.332 (3)15.517 (3), 19.411 (4), 7.963 (2)
β (°) 90.39 (3) 102.90 (3)
V3)1218.3 (4)2337.9 (9)
Z24
Radiation typeMo KαMo Kα
µ (mm1)0.090.10
Crystal size (mm)0.4 × 0.2 × 0.10.5 × 0.3 × 0.1
Data collection
DiffractometerMAC DIP 2030K area-detector
diffractometer
Rigaku RAXIS-RAPID area-detector
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
5888, 2725, 2715 15334, 5186, 2479
Rint0.0240.070
(sin θ/λ)max1)0.6440.647
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.054, 0.138, 1.23 0.057, 0.161, 0.84
No. of reflections27255186
No. of parameters325325
No. of restraints10
H-atom treatmentH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.17, 0.260.28, 0.30

Computer programs: DENZO (Otwinowski & Minor, 1997), SCALE (Otwinowski & Minor, 1997), SCALE, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEPII (Johnson, 1976) and PLATON (Spek, 2003), SHELXL97 and PLATON.

 

Subscribe to Acta Crystallographica Section C: Structural Chemistry

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. C
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds