Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
The title compound, 7,13,21,27-tetra-tert-butyl-3,17-di­oxa­penta­cyclo­[23.3.1.15,9.111,15.19,23]ditriaconta-1(29),­5,­7,­9(30),11(31),­12,­14,­19(32),­20,­22,­25,­27-do­deca­ene-29,­30,­31,­32-tetraol, crystallizes as a solvate with one mol­ecule of chloro­form and one mol­ecule of tetra­hydro­furan, C46H60O6·CHCl3·C4H8O. The calixarene assumes a cone-like conformation stabilized by intramolecular hydrogen bonds involving both phenolic and ether O atoms. The two solvent mol­ecules are located in each of the two half-cone cavities of the calixarene.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100013329/na1482sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100013329/na1482Isup2.hkl
Contains datablock I

CCDC reference: 158253

Comment top

We have recently reported the first crystal structures of p-tert-butyltetrahomodioxacalix[4]arene as well as of its uranyl ion complex (Thuéry et al., 2000). Two forms presenting slightly different conformations have been found for the uncomplexed ligand, associated with some differences in the ether bridge conformations and intramolecular hydrogen-bond pattern. In each case, two solvent molecules (acetonitrile or pyridine) are included in the calixarene cavity. \sch

The main features of these structures are present in the case of the new solvate, (I), but the conformation is slightly different from the previous ones. The asymmetric unit in 1 is composed of one calixarene and two different solvent molecules. The calixarene symmetry was higher in one of the cases previously reported, in which the molecule was located around a binary axis, (II). If the plane defined by the four phenolic oxygen atoms is taken as a reference (highest deviation #from mean plane 0.324 (3) Å), the dihedral #angles made with it by the four phenyl rings are 124.5 (1), 126.4 (1), #157.5 (2) and 159.6 (1)° in 1, i.e. they span a wider range than those in the #more symmetrical and regular form 2 previously described #(132.8 (2)–141.2 (2)°). However, this from mean plane 0.459 (4) Å), the dihedral angles made with it by the four phenyl rings are 132.4 (1), 125.7 (1), 148.2 (2) and 156.2 (1)° in (I), i.e. they span a wider range than those in the more symmetrical and regular form (II) previously described [132.8 (2)–141.2 (2)°]. However, this range was even larger in the second form previously described (3) [109.4 (1)–157.3 (2)°]. The intramolecular hydrogen-bond pattern is different in the two previous forms: in 2, two phenolic units give bifurcated hydrogen bonds with the other phenolic units and the ether groups whereas in (III), one of those bifurcated bonds is replaced by a simple one (with the ether group). In (I), both hydrogen bonds are bifurcated, the phenol···phenol ones being seemingly somewhat less strong than in (II). The conformation around the ether bridges is identical to that in (II), the slight geometrical differences between those two compounds being possibly connected to the difference in the solvents included. By contrast with the parent calixarenes, in which the hydrogen-bond pattern is rather well defined and contributes to the rigidity of the molecule, the presence of the ether groups in oxacalixarenes makes this pattern more variable and the molecule more flexible.

The inclusion of two chemically different solvent molecules in a calixarene cavity is a somewhat uncommon feature, at least for small calixarenes [in both compounds (II) and (III), two identical molecules were included, acetonitrile in (II), pyridine in (III)]. It has been suggested that the ability of calixarenes to held two different species relatively close one to the other was indicative of their potential as 'enzyme mimics' (Asfari et al., 1991). The location of the choroform hydrogen atom is indicative of a possible hydrogen bond with the oxygen atom of tetrahydrofuran. Feeble interactions are thus present between the three species in this complex.

Experimental top

p-tert-Butyltetrahomodioxacalix[4]arene was synthesized as previously reported (Dhawan & Gutsche, 1983) and recrystallized from chloroform/tetrahydrofuran (1:1).

Refinement top

4517 Friedel pairs have been measured. Hydroxyl and chloroform protons were found on the Fourier-difference map and introduced as riding atoms with a displacement parameter equal to 1.2 times that of the parent atom. All other hydrogen atoms were introduced at calculated positions as riding atoms with a displacement parameter equal to 1.2 (CH, CH2) or 1.5 (CH3) times that of the parent atom. The tetrahydrofuran molecule bahaves badly on refinement and some restraints had to be applied to the displacement parameters. One of the C—C distances in this molecule is shorter than usual [1.425 (14) Å].

Computing details top

Data collection: Kappa-CCD Software (Nonius, 1997); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Sheldrick, 1999); software used to prepare material for publication: SHELXTL (Sheldrick, 1999) and PARST97 (Nardelli, 1995).

Figures top
[Figure 1] Fig. 1. The title molecule with atomic numbering scheme. Hydrogen atoms omitted for clarity unless those involved in hydrogen bonds, which are drawn as small spheres of arbitrary radii. Hydrogen bonds are shown as dashed lines. Displacement ellipsoids are drawn at the 30% probability level.
(I) top
Crystal data top
C46H60O6·CHCl3·C4H8ODx = 1.213 Mg m3
Mr = 900.41Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, P212121Cell parameters from 35687 reflections
a = 9.2248 (5) Åθ = 2.7–25.7°
b = 17.6451 (15) ŵ = 0.24 mm1
c = 30.282 (3) ÅT = 100 K
V = 4929.1 (7) Å3Parallelepipedic, colourless
Z = 40.28 × 0.28 × 0.25 mm
F(000) = 1928
Data collection top
Nonius Kappa-CCD
diffractometer
5464 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.084
Graphite monochromatorθmax = 25.7°, θmin = 2.7°
Detector resolution: 18 pixels mm-1h = 010
ϕ scansk = 2121
35687 measured reflectionsl = 3636
9064 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.078H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.213 w = 1/[σ2(Fo2) + (0.1216P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.96(Δ/σ)max = 0.001
9064 reflectionsΔρmax = 0.71 e Å3
562 parametersΔρmin = 0.39 e Å3
42 restraintsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.00
Crystal data top
C46H60O6·CHCl3·C4H8OV = 4929.1 (7) Å3
Mr = 900.41Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 9.2248 (5) ŵ = 0.24 mm1
b = 17.6451 (15) ÅT = 100 K
c = 30.282 (3) Å0.28 × 0.28 × 0.25 mm
Data collection top
Nonius Kappa-CCD
diffractometer
5464 reflections with I > 2σ(I)
35687 measured reflectionsRint = 0.084
9064 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.078H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.213Δρmax = 0.71 e Å3
S = 0.96Δρmin = 0.39 e Å3
9064 reflectionsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
562 parametersAbsolute structure parameter: 0.00
42 restraints
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.

Refinement. Structure solved by direct methods and expanded by subsequent Fourier-difference synthesis. All non-hydrogen atoms have been refined anisotropically. The structure has been refined as corresponding to a racemic twin. 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
O10.8511 (3)0.41297 (18)0.05789 (11)0.0224 (8)
H10.89440.42410.03440.027*
O20.9551 (3)0.5157 (2)0.00001 (11)0.0258 (8)
O30.7592 (4)0.4037 (2)0.03249 (12)0.0350 (9)
H30.70700.35780.03420.042*
O40.5418 (3)0.30084 (19)0.03874 (11)0.0233 (8)
H40.48260.29920.00930.028*
O50.3058 (3)0.30112 (19)0.01185 (11)0.0242 (8)
O60.5522 (3)0.38272 (19)0.04573 (10)0.0213 (7)
H60.64900.39390.05060.026*
C10.8370 (4)0.4743 (3)0.08699 (16)0.0195 (10)
C20.7533 (4)0.4645 (3)0.12435 (15)0.0179 (10)
C30.7346 (5)0.5263 (3)0.15212 (16)0.0217 (10)
H3A0.67720.52020.17710.026*
C40.7976 (5)0.5974 (3)0.14454 (16)0.0228 (11)
C50.8830 (5)0.6040 (3)0.10650 (16)0.0214 (10)
H50.92570.65050.10010.026*
C60.9060 (4)0.5433 (3)0.07784 (16)0.0197 (10)
C70.7738 (6)0.6632 (3)0.17627 (19)0.0316 (12)
C80.8539 (10)0.6492 (4)0.2188 (3)0.067 (2)
H8A0.83300.59900.22920.100*
H8B0.82360.68560.24050.100*
H8C0.95620.65420.21380.100*
C90.6100 (7)0.6699 (4)0.1870 (3)0.058 (2)
H9A0.55700.67930.16020.086*
H9B0.59480.71100.20720.086*
H9C0.57670.62350.20000.086*
C100.8140 (9)0.7389 (3)0.1562 (2)0.0534 (19)
H10A0.91700.74110.15180.080*
H10B0.78470.77900.17570.080*
H10C0.76590.74470.12830.080*
C111.0082 (5)0.5516 (3)0.03893 (15)0.0241 (11)
H11A1.02310.60500.03300.029*
H11B1.10130.52970.04660.029*
C120.8357 (6)0.5522 (3)0.01916 (18)0.0325 (12)
H12A0.85430.60620.02080.039*
H12B0.75080.54450.00080.039*
C130.8066 (5)0.5223 (3)0.06456 (19)0.0331 (13)
C140.7659 (5)0.4457 (3)0.06974 (18)0.0298 (12)
C150.7326 (4)0.4179 (3)0.11206 (17)0.0224 (10)
C160.7407 (5)0.4668 (3)0.14761 (17)0.0213 (10)
H160.71200.44920.17520.026*
C170.7899 (5)0.5413 (3)0.14414 (18)0.0270 (11)
C180.8173 (6)0.5681 (3)0.10158 (18)0.0341 (13)
H180.84370.61860.09790.041*
C190.7949 (5)0.5958 (3)0.18339 (17)0.0248 (11)
C200.6714 (6)0.6530 (4)0.1800 (2)0.0394 (14)
H20A0.67610.68750.20450.059*
H20B0.68000.68080.15290.059*
H20C0.58020.62670.18050.059*
C210.7839 (6)0.5554 (3)0.22760 (18)0.0362 (13)
H21A0.86010.51860.22990.054*
H21B0.79300.59170.25100.054*
H21C0.69170.53050.22970.054*
C220.9406 (6)0.6384 (4)0.1838 (2)0.0409 (15)
H22A1.01870.60260.18160.061*
H22B0.94440.67270.15920.061*
H22C0.94950.66640.21090.061*
C230.6772 (5)0.3363 (3)0.11966 (17)0.0219 (11)
H23A0.70440.31980.14910.026*
H23B0.72290.30250.09860.026*
C240.5149 (4)0.3311 (3)0.11476 (17)0.0193 (10)
C250.4507 (5)0.3134 (3)0.07492 (16)0.0192 (10)
C260.3010 (5)0.3069 (3)0.06974 (16)0.0217 (11)
C270.2140 (5)0.3194 (3)0.10703 (16)0.0212 (11)
H270.11380.31710.10390.025*
C280.2714 (5)0.3352 (3)0.14866 (16)0.0189 (10)
C290.4241 (5)0.3412 (3)0.15117 (16)0.0183 (10)
H290.46600.35240.17830.022*
C300.1784 (5)0.3469 (3)0.18981 (16)0.0208 (10)
C310.1912 (7)0.4284 (3)0.2056 (2)0.0431 (15)
H31A0.13530.43490.23200.065*
H31B0.29100.43990.21150.065*
H31C0.15520.46190.18310.065*
C320.0196 (5)0.3289 (4)0.1811 (2)0.0383 (14)
H32A0.01320.35700.15590.057*
H32B0.00900.27560.17560.057*
H32C0.03710.34280.20650.057*
C330.2310 (6)0.2940 (4)0.22643 (18)0.0367 (13)
H33A0.17950.30490.25320.055*
H33B0.21350.24240.21800.055*
H33C0.33290.30140.23110.055*
C340.2330 (5)0.2775 (3)0.02779 (16)0.0261 (11)
H34A0.13310.29450.02650.031*
H34B0.23200.22250.02880.031*
C350.2599 (5)0.3735 (3)0.02840 (16)0.0231 (11)
H35A0.15490.37690.02800.028*
H35B0.29870.41390.01010.028*
C360.3156 (4)0.3808 (3)0.07508 (16)0.0205 (10)
C370.4671 (5)0.3848 (3)0.08268 (16)0.0200 (10)
C380.5191 (4)0.3881 (3)0.12493 (16)0.0182 (10)
C390.4223 (5)0.3924 (3)0.16034 (17)0.0208 (10)
H390.45920.39650.18880.025*
C400.2698 (5)0.3907 (3)0.15439 (15)0.0195 (10)
C410.2207 (5)0.3855 (3)0.11068 (16)0.0225 (10)
H410.12140.38530.10530.027*
C420.1647 (5)0.4005 (3)0.19308 (16)0.0228 (11)
C430.1035 (5)0.4799 (3)0.1916 (2)0.0311 (13)
H43A0.02830.48480.21330.047*
H43B0.06430.48960.16280.047*
H43C0.17920.51570.19780.047*
C440.2381 (5)0.3865 (3)0.23702 (15)0.0253 (11)
H44A0.28140.33700.23700.038*
H44B0.16760.38950.26030.038*
H44C0.31180.42400.24170.038*
C450.0403 (5)0.3421 (3)0.18882 (19)0.0322 (12)
H45A0.07960.29170.19000.048*
H45B0.00870.34930.16120.048*
H45C0.02710.34900.21260.048*
C460.6821 (5)0.3889 (3)0.13465 (17)0.0212 (10)
H46A0.69720.37710.16560.025*
H46B0.72870.34960.11730.025*
C470.4073 (9)0.6656 (5)0.0445 (3)0.073 (2)
H470.36650.66320.01470.087*
Cl10.2803 (3)0.70978 (15)0.07854 (10)0.1005 (9)
Cl20.5685 (3)0.71738 (15)0.04176 (9)0.0934 (8)
Cl30.4431 (3)0.57232 (12)0.06175 (9)0.0862 (7)
O70.3201 (5)0.6469 (3)0.05420 (16)0.0573 (13)
C480.1989 (8)0.6047 (4)0.0688 (3)0.067 (2)
H48A0.14810.63280.09160.080*
H48B0.13260.59690.04430.080*
C490.2451 (12)0.5324 (7)0.0860 (4)0.109 (3)
H49A0.21640.49160.06640.131*
H49B0.20380.52340.11500.131*
C500.3989 (12)0.5381 (7)0.0884 (5)0.118 (3)
H50A0.42940.53230.11890.141*
H50B0.44220.49740.07140.141*
C510.4506 (10)0.6109 (6)0.0715 (4)0.091 (3)
H51A0.52200.60360.04840.110*
H51B0.49310.64110.09500.110*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0215 (15)0.0262 (18)0.0196 (19)0.0027 (13)0.0050 (13)0.0064 (15)
O20.0301 (17)0.0293 (19)0.0182 (19)0.0059 (15)0.0014 (15)0.0016 (15)
O30.0424 (19)0.033 (2)0.030 (2)0.0093 (16)0.0027 (17)0.0054 (17)
O40.0239 (16)0.0267 (19)0.0192 (19)0.0036 (14)0.0009 (14)0.0009 (15)
O50.0297 (17)0.0235 (18)0.0195 (19)0.0008 (14)0.0031 (14)0.0058 (15)
O60.0208 (15)0.0293 (19)0.0139 (17)0.0055 (14)0.0002 (13)0.0005 (15)
C10.015 (2)0.017 (2)0.026 (3)0.0002 (17)0.0071 (19)0.003 (2)
C20.0132 (19)0.024 (3)0.017 (2)0.0007 (18)0.0046 (18)0.001 (2)
C30.019 (2)0.024 (3)0.022 (3)0.0026 (19)0.0044 (19)0.001 (2)
C40.028 (2)0.024 (3)0.017 (3)0.0006 (19)0.001 (2)0.004 (2)
C50.027 (2)0.017 (2)0.020 (3)0.0090 (18)0.001 (2)0.001 (2)
C60.017 (2)0.026 (3)0.017 (3)0.0030 (18)0.0003 (18)0.002 (2)
C70.037 (3)0.025 (3)0.032 (3)0.002 (2)0.003 (2)0.002 (2)
C80.100 (6)0.050 (4)0.050 (5)0.020 (4)0.036 (4)0.019 (4)
C90.058 (4)0.041 (4)0.073 (5)0.001 (3)0.038 (4)0.015 (4)
C100.091 (5)0.025 (3)0.044 (4)0.006 (3)0.022 (4)0.007 (3)
C110.027 (2)0.033 (3)0.013 (3)0.010 (2)0.0002 (19)0.002 (2)
C120.038 (3)0.033 (3)0.026 (3)0.003 (2)0.004 (2)0.006 (2)
C130.031 (3)0.036 (3)0.032 (3)0.001 (2)0.000 (2)0.001 (3)
C140.030 (3)0.032 (3)0.027 (3)0.003 (2)0.001 (2)0.002 (2)
C150.017 (2)0.025 (3)0.025 (3)0.0045 (19)0.0021 (19)0.002 (2)
C160.015 (2)0.025 (3)0.023 (3)0.0005 (19)0.0002 (19)0.000 (2)
C170.028 (3)0.028 (3)0.025 (3)0.004 (2)0.006 (2)0.002 (2)
C180.042 (3)0.034 (3)0.026 (3)0.007 (2)0.001 (2)0.011 (2)
C190.028 (2)0.023 (3)0.023 (3)0.002 (2)0.001 (2)0.004 (2)
C200.035 (3)0.052 (4)0.031 (3)0.016 (3)0.001 (3)0.008 (3)
C210.053 (3)0.035 (3)0.020 (3)0.003 (3)0.002 (3)0.003 (2)
C220.040 (3)0.049 (4)0.034 (4)0.011 (3)0.001 (3)0.008 (3)
C230.022 (2)0.018 (2)0.026 (3)0.0032 (19)0.000 (2)0.002 (2)
C240.021 (2)0.010 (2)0.027 (3)0.0019 (17)0.002 (2)0.001 (2)
C250.023 (2)0.016 (2)0.018 (3)0.0026 (18)0.004 (2)0.0004 (19)
C260.023 (2)0.023 (3)0.019 (3)0.0059 (19)0.001 (2)0.002 (2)
C270.022 (2)0.022 (3)0.020 (3)0.0015 (18)0.0025 (19)0.004 (2)
C280.022 (2)0.017 (2)0.018 (3)0.0029 (19)0.0029 (19)0.001 (2)
C290.020 (2)0.019 (2)0.015 (3)0.0033 (18)0.0041 (18)0.002 (2)
C300.018 (2)0.022 (3)0.022 (3)0.0009 (18)0.0019 (19)0.000 (2)
C310.052 (3)0.033 (3)0.045 (4)0.004 (3)0.013 (3)0.006 (3)
C320.029 (3)0.057 (4)0.029 (3)0.009 (2)0.006 (2)0.012 (3)
C330.040 (3)0.047 (3)0.022 (3)0.006 (3)0.011 (2)0.008 (3)
C340.027 (2)0.031 (3)0.020 (3)0.008 (2)0.003 (2)0.001 (2)
C350.019 (2)0.031 (3)0.019 (3)0.004 (2)0.004 (2)0.006 (2)
C360.017 (2)0.022 (3)0.022 (3)0.0018 (19)0.0039 (19)0.004 (2)
C370.019 (2)0.018 (2)0.023 (3)0.0002 (19)0.0040 (19)0.003 (2)
C380.017 (2)0.019 (3)0.018 (3)0.0014 (18)0.0019 (18)0.005 (2)
C390.026 (2)0.016 (2)0.020 (3)0.0013 (19)0.006 (2)0.000 (2)
C400.019 (2)0.019 (2)0.021 (3)0.0060 (18)0.0015 (18)0.002 (2)
C410.020 (2)0.025 (3)0.023 (3)0.0010 (19)0.0008 (19)0.001 (2)
C420.022 (2)0.024 (3)0.021 (3)0.0059 (19)0.0011 (19)0.006 (2)
C430.022 (2)0.035 (3)0.036 (3)0.007 (2)0.002 (2)0.009 (3)
C440.028 (2)0.031 (3)0.017 (3)0.003 (2)0.004 (2)0.003 (2)
C450.028 (2)0.039 (3)0.030 (3)0.013 (2)0.006 (2)0.007 (3)
C460.017 (2)0.022 (3)0.024 (3)0.0003 (19)0.0051 (19)0.001 (2)
C470.082 (5)0.053 (5)0.082 (6)0.002 (4)0.030 (5)0.002 (4)
Cl10.0882 (15)0.0866 (16)0.127 (2)0.0010 (13)0.0001 (14)0.0468 (16)
Cl20.0961 (16)0.0803 (16)0.1037 (19)0.0264 (13)0.0120 (14)0.0019 (14)
Cl30.0915 (14)0.0536 (12)0.113 (2)0.0001 (10)0.0220 (14)0.0112 (12)
O70.041 (2)0.067 (3)0.064 (3)0.006 (2)0.002 (2)0.013 (3)
C480.065 (3)0.063 (3)0.073 (4)0.007 (3)0.007 (3)0.005 (3)
C490.108 (4)0.106 (4)0.114 (4)0.007 (4)0.004 (4)0.014 (4)
C500.113 (4)0.115 (4)0.125 (5)0.011 (4)0.020 (4)0.009 (4)
C510.077 (4)0.106 (4)0.091 (4)0.003 (4)0.008 (3)0.007 (4)
Geometric parameters (Å, º) top
O1—C11.402 (6)C23—C241.507 (6)
O2—C121.401 (6)C24—C251.380 (7)
O2—C111.425 (6)C24—C291.396 (7)
O3—C141.352 (6)C25—C261.394 (6)
O4—C251.398 (6)C26—C271.403 (7)
O5—C351.436 (6)C26—C341.509 (7)
O5—C341.438 (6)C27—C281.396 (7)
O6—C371.367 (6)C28—C291.415 (6)
C1—C21.381 (6)C28—C301.527 (7)
C1—C61.402 (7)C30—C311.519 (8)
C2—C31.387 (7)C30—C331.529 (7)
C2—C461.519 (7)C30—C321.521 (7)
C3—C41.401 (7)C35—C361.510 (7)
C4—C51.401 (7)C36—C411.392 (7)
C4—C71.523 (7)C36—C371.418 (6)
C5—C61.395 (7)C37—C381.367 (7)
C6—C111.516 (6)C38—C391.397 (7)
C7—C81.505 (9)C38—C461.532 (6)
C7—C101.515 (8)C39—C401.418 (6)
C7—C91.550 (8)C40—C411.402 (7)
C12—C131.497 (8)C40—C421.531 (7)
C13—C181.386 (8)C42—C431.511 (7)
C13—C141.410 (8)C42—C441.513 (7)
C14—C151.407 (7)C42—C451.547 (7)
C15—C161.382 (7)C47—Cl11.744 (9)
C15—C231.545 (7)C47—Cl21.748 (9)
C16—C171.394 (7)C47—Cl31.758 (8)
C17—C181.396 (8)O7—C481.413 (9)
C17—C191.529 (7)O7—C511.458 (10)
C19—C211.519 (7)C48—C491.442 (14)
C19—C201.526 (7)C49—C501.425 (14)
C19—C221.540 (7)C50—C511.462 (16)
C12—O2—C11114.2 (4)C24—C25—C26122.8 (4)
C35—O5—C34114.3 (3)C24—C25—O4117.6 (4)
C2—C1—C6121.7 (4)C26—C25—O4119.6 (4)
C2—C1—O1118.0 (4)C25—C26—C27117.6 (4)
C6—C1—O1120.3 (4)C25—C26—C34122.3 (4)
C1—C2—C3117.9 (4)C27—C26—C34119.6 (4)
C1—C2—C46121.3 (4)C28—C27—C26122.8 (4)
C3—C2—C46120.8 (4)C27—C28—C29116.2 (4)
C2—C3—C4123.5 (4)C27—C28—C30123.5 (4)
C3—C4—C5116.3 (4)C29—C28—C30120.4 (4)
C3—C4—C7121.3 (4)C24—C29—C28123.0 (4)
C5—C4—C7122.4 (4)C31—C30—C33109.0 (5)
C6—C5—C4122.2 (4)C31—C30—C32109.1 (4)
C5—C6—C1118.3 (4)C33—C30—C32107.6 (4)
C5—C6—C11120.3 (4)C31—C30—C28109.9 (4)
C1—C6—C11121.3 (4)C33—C30—C28109.3 (4)
C8—C7—C10111.6 (5)C32—C30—C28111.8 (4)
C8—C7—C4110.1 (5)O5—C34—C26114.1 (4)
C10—C7—C4112.6 (5)O5—C35—C36107.6 (4)
C8—C7—C9108.2 (6)C41—C36—C37119.4 (4)
C10—C7—C9104.8 (5)C41—C36—C35121.1 (4)
C4—C7—C9109.3 (5)C37—C36—C35119.5 (4)
O2—C11—C6112.7 (4)C38—C37—O6124.4 (4)
O2—C12—C13111.0 (4)C38—C37—C36120.0 (4)
C18—C13—C14119.2 (5)O6—C37—C36115.6 (4)
C18—C13—C12121.6 (5)C37—C38—C39119.7 (4)
C14—C13—C12119.2 (5)C37—C38—C46121.6 (4)
O3—C14—C15123.9 (5)C39—C38—C46118.6 (4)
O3—C14—C13116.4 (5)C38—C39—C40122.3 (5)
C15—C14—C13119.6 (5)C41—C40—C39116.2 (4)
C16—C15—C14118.6 (4)C41—C40—C42121.6 (4)
C16—C15—C23118.9 (4)C39—C40—C42121.9 (4)
C14—C15—C23122.3 (4)C40—C41—C36122.1 (4)
C15—C16—C17123.2 (5)C43—C42—C44110.1 (4)
C16—C17—C18116.6 (5)C43—C42—C40108.6 (4)
C16—C17—C19122.9 (5)C44—C42—C40111.8 (4)
C18—C17—C19119.9 (5)C43—C42—C45109.8 (4)
C13—C18—C17122.4 (5)C44—C42—C45107.2 (4)
C17—C19—C21112.9 (4)C40—C42—C45109.3 (4)
C17—C19—C20109.9 (4)C2—C46—C38113.2 (4)
C21—C19—C20108.6 (4)Cl1—C47—Cl2111.5 (5)
C17—C19—C22109.9 (4)Cl1—C47—Cl3111.7 (5)
C21—C19—C22106.2 (4)Cl2—C47—Cl3110.1 (4)
C20—C19—C22109.2 (4)C48—O7—C51108.2 (6)
C24—C23—C15111.7 (4)O7—C48—C49110.1 (7)
C25—C24—C29117.5 (4)C50—C49—C48104.5 (10)
C25—C24—C23121.8 (4)C49—C50—C51111.6 (10)
C29—C24—C23120.7 (4)O7—C51—C50103.8 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O20.842.002.699 (8)140
O1—H1···O30.842.412.870 (8)116
O3—H3···O40.941.832.712 (8)154
O4—H4···O51.051.752.662 (8)143
O4—H4···O61.052.322.939 (8)117
O6—H6···O10.931.912.833 (8)177
C47—H47···O70.982.153.113 (10)168

Experimental details

Crystal data
Chemical formulaC46H60O6·CHCl3·C4H8O
Mr900.41
Crystal system, space groupOrthorhombic, P212121
Temperature (K)100
a, b, c (Å)9.2248 (5), 17.6451 (15), 30.282 (3)
V3)4929.1 (7)
Z4
Radiation typeMo Kα
µ (mm1)0.24
Crystal size (mm)0.28 × 0.28 × 0.25
Data collection
DiffractometerNonius Kappa-CCD
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
35687, 9064, 5464
Rint0.084
(sin θ/λ)max1)0.610
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.078, 0.213, 0.96
No. of reflections9064
No. of parameters562
No. of restraints42
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.71, 0.39
Absolute structureFlack H D (1983), Acta Cryst. A39, 876-881
Absolute structure parameter0.00

Computer programs: Kappa-CCD Software (Nonius, 1997), DENZO-SMN (Otwinowski & Minor, 1997), DENZO-SMN, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Sheldrick, 1999) and PARST97 (Nardelli, 1995).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O20.842.002.699 (8)140
O1—H1···O30.842.412.870 (8)116
O3—H3···O40.941.832.712 (8)154
O4—H4···O51.051.752.662 (8)143
O4—H4···O61.052.322.939 (8)117
O6—H6···O10.931.912.833 (8)177
C47—H47···O70.982.153.113 (10)168
 

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