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, C47H60O6·3CHCl3, is the first example of a lower-rim mono-ester calixarene derivative to be crystallographically characterized. The cone conformation adopted by the macrocycle is stabilized by three intramolecular hydrogen bonds. Self-inclusion of the methyl ester chain in the cavity of an adjacent mol­ecule gives rise to infinite chains parallel to the c axis. C-H...[pi] interactions involving the methyl group most imbedded in the cavity contribute to the stabilization of the system.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270104026356/sx1158sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270104026356/sx1158Isup2.hkl
Contains datablock I

CCDC reference: 259032

Comment top

Lower-rim ester derivatives of calixarenes (Thondorf, Shivanyuk & Böhmer, 2001) have been the subject of much attention, in particular for their ionophoric properties (Arnaud-Neu et al., 2001). Numerous di- and tetra-ester derivatives of R-calix[4]arene have been synthesized and characterized, but to the best of our knowledge, no crystal structure of a mono-ester derivative has been reported. The mono-ester (I) was prepared to be used in the synthesis of new dendrimers (Cheriaa et al., 2004). We have reported previously the syntheses and crystal structures of the related compound 5,11,17,23-tetra-tert-butyl-25,27-di(methoxycarbonylmethoxy)- 26,28-dimethoxycalix[4]arene and its complexes with Na+ and K+ (Oueslati et al., 2000); the absence of hydroxy groups in the former prevents stabilization of the cone conformation by intramolecular hydrogen bonding, as usual for calix[4]arene derivatives (Gutsche, 1998), and it crystallizes in the partial cone conformation. In contrast, the di-methylester derivative of calix[4]arene, unsubstituted at the para positions, 1,3-di(methoxycarbonylmethoxy)-2,4-dihydroxycalix[4]arene, is in the cone conformation (Coles et al., 2002) as is 5,11,17,23-tetra-tert-butyl-25,26,27,28- tetra(methoxycarbonylmethoxy)calix[4]arene and the corresponding tetra-ethyl ester derivative (Arnaud-Neu et al., 1989). A search of the Cambridge Structural Database (CSD; Version 5.25; Allen, 2002) identifies several crystal structures of diethyl ester derivatives, with tert-butyl or H substituents in the para positions (Creaven et al., 2001; Genorio et al., 2003; Bolte et al., 2003; Dudič et al., 2003), but only two triethyl ester compounds have been described (Cooper et al., 2000).

Compound (I) crystallizes as a chloroform trisolvate, with one complete molecule in the asymmetric unit (Fig. 1). The macrocycle adopts a cone conformation, as expected from the intramolecular homodromic hydrogen bonds (Steiner, 2002) involving the three phenol hydroxide groups and the substituted phenol O atom. The mean plane defined by the four methylene C-atom bridges (r.m.s. deviation 0.042 Å) was chosen as a reference plane. The plane defined by the four phenol O atoms (O1, O4, O5 and O6; r.m.s. deviation 0.007 Å) makes a dihedral angle of 2.82 (8)° with this reference plane, whereas the four aromatic rings make dihedral angles of 66.43 (8), 54.24 (10), 56.30 (10) and 62.23 (9)°. The cone conformation thus appears to be regular, but the aromatic ring that bears the ester substituent is more inclined with respect to the reference plane than the other three rings. Comparable conformations were found in diethyl ester derivatives (Creaven et al., 2001; Bolte et al., 2003), whereas the cone conformation is much more distorted in tetra-ester derivatives (Arnaud-Neu et al., 1989) as a result of increased steric interactions. The conformation of the ester chain in (I) is extended and roughly perpendicular to the reference plane. Atom C1 points towards the exterior of the macrocycle [the torsion angles around the Carom—O1 bond are −93.8 (4) and 87.7 (4)°], whereas the torsion angles around the O1—C1, C1—C2 and C2—O3 bonds do not deviate from syn or anti ideal values by more than 19°. An additional close interaction, possibly a weak hydrogen bond, between atoms O4 and O2 may stabilize this conformation of the chain, the H atom bound to atom O4 being thus involved in a dissymmetric bifurcated hydrogen bond.

The methyl ester chain is included in the cavity of the neighbouring calixarene along the c axis, which gives rise to infinite chains of parallel calixarenes held together by weak interactions directed along this axis (Fig. 2). The chloroform solvent molecules are located in the voids between these chains. Such self-inclusion phenomena are not uncommon in calixarene structures, but very often they involve the para substituents and, as a consequence, the upper rims of adjacent molecules are facing each other and offset (Gallagher et al., 1994; Böhmer et al., 1996; Brouwer et al., 2001). Self-inclusion of an ethyl ester residue in 5,11,17,23-tetra-tert-butyl-25,27-di(ethoxycarbonylmethoxy)- 26,28-dihydroxycalix[4]arene has, however, also been reported recently (Bolte et al., 2003). The C3 methyl group in (I) is located near the centre of the cavity of the neighbouring molecule. Atom C3 is located 4.002 (6)–4.178 (6) Å from the four aromatic para C atoms of the host molecule and 0.416 (4) Å (on the outer side) from the mean plane defined by these four aromatic C atoms (r.m.s. deviation 0.042 Å). This methyl group is thus well imbedded in the cavity, as evidenced by the shortest C3···Carom distance, 3.657 (6) Å, which involves atom C26 in an ortho position with respect to O5. This value is comparable to that found in the diethyl ester derivative (Bolte et al., 2003), 3.685 (6) Å, but the latter involves a C atom bearing a phenol O atom. Apart from van der Waals contacts, CH–π interactions seem to play an important role in this self-inclusion phenomenon in (I). The three H atoms bound to atom C3 could not be found satisfactorily in difference Fourier maps, but refinement of this group as a rotating methyl group so as to maximize the sum of the electron density at the H-atom positions gave H atoms possibly involved in CH–π interactions with three aromatic rings [H3A···Cg1 = 2.91 Å and C3—H3A···Cg1 = 144°, H3B···Cg2 = 2.93 Å and C3—H3B···Cg2 = 149°, and H3C···Cg3 = 2.77 Å and C3—H3C···Cg3 = 144°, where Cg1, Cg2 and Cg3 are the centroids of the aromatic rings attached to atoms O4i, O1i and O5i, respectively; symmetry code (i) x, y, 1 + z]. In the case of host–guest complexes of calixarenes, it has been suggested that the CH–π interactions could be second to other interactions, such as packing forces (Brouwer, Enright & Ripmeester 1996; Brouwer, Ripmeester & Enright 1996). The relative contributions of such weak interactions cannot be separated on the basis of structural data alone (dipole–dipole interactions may also be present), but the arrangement observed in (I) supports the hypothesis that CH–π interactions are important components in the stabilization of the system.

Experimental top

p-tert-Butylcalix[4]arene was refluxed in acetonitrile with three equivalents of bromomethyl acetate and 0.5 equivalents of potassium carbonate for a period of 18 h. After acidification, two-phase extraction with chloroform and evaporation of the solvents, the crude mixture was precipitated with methanol to give the title compound in 55% yield. Mp > 421–422 K. Single crystals were obtained from methanol diffusion in a chloroform solution of (I).

Refinement top

Hydroxy H atoms were found in a difference Fourier map and were introduced as riding atoms, with Uiso(H) values of 1.2Ueq(O). All other H atoms were introduced at calculated positions as riding atoms, with C–H bond lengths of 0.93 (aromatic CH), 0.98 (aliphatic CH), 0.97 (CH2) and 0.96 Å (CH3), and with Uiso(H) values of 1.2Ueq(parent atom) for CH and CH2 H atoms and 1.5Ueq(parent atom) for CH3 Ha toms. The H atoms bound to atom C3, which are probably involved in CH–π interactions, could not be found satisfyingly, but this methyl group was treated as a rotating group and its position was calculated so as to maximize the sum of the electron density at the H-atom positions. The absolute structure was determined from the value of the Flack (1983) parameter [0.03 (5)].

Computing details top

Data collection: KappaCCD 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 (Bruker, 1999); software used to prepare material for publication: SHELXTL (Bruker, 1999) and PLATON (Spek, 2000).

Figures top
[Figure 1] Fig. 1. A view of (I), with the atom-numbering scheme. Displacement ellipsoids are drawn at the 40% probability level. H atoms have been omitted, except for those involved in hydrogen bonds, which are drawn as small spheres of arbitrary radii. Hydrogen bonds are shown as dashed lines.
[Figure 2] Fig. 2. A view showing the self-inclusion in (I). Displacement ellipsoids are drawn at the 30% probability level. H atoms have been omitted, except for those involved in hydrogen bonds and CH–π interactions, which are drawn as small spheres of arbitrary radii. Solvent molecules have been omitted. [Symmetry code: (') x, y, 1 + z.]
5,11,17,23-tetra-tert-butyl-25-methoxycarbonylmethoxy-26,27,28- trihydroxycalix[4]arene chloroform trisolvate top
Crystal data top
C47H60O6·3CHCl3Dx = 1.331 Mg m3
Mr = 1079.05Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pna21Cell parameters from 35034 reflections
a = 23.7595 (9) Åθ = 2.3–25.7°
b = 24.2234 (8) ŵ = 0.51 mm1
c = 9.3546 (3) ÅT = 100 K
V = 5383.9 (3) Å3Parallelepiped, colourless
Z = 40.26 × 0.14 × 0.12 mm
F(000) = 2256
Data collection top
Nonius KappaCCD
diffractometer
9864 independent reflections
Radiation source: fine-focus sealed tube7715 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.081
ϕ scansθmax = 25.7°, θmin = 2.3°
Absorption correction: part of the refinement model (ΔF)
(DELABS in PLATON; Spek, 2000)
h = 2827
Tmin = 0.891, Tmax = 0.936k = 2928
35034 measured reflectionsl = 1111
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)] = 0.048H-atom parameters constrained
wR(F2) = 0.125 w = 1/[σ2(Fo2) + (0.0582P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
9864 reflectionsΔρmax = 0.33 e Å3
600 parametersΔρmin = 0.43 e Å3
1 restraintAbsolute structure: Flack (1983), 4416 Friedel pairs?
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.03 (5)
Crystal data top
C47H60O6·3CHCl3V = 5383.9 (3) Å3
Mr = 1079.05Z = 4
Orthorhombic, Pna21Mo Kα radiation
a = 23.7595 (9) ŵ = 0.51 mm1
b = 24.2234 (8) ÅT = 100 K
c = 9.3546 (3) Å0.26 × 0.14 × 0.12 mm
Data collection top
Nonius KappaCCD
diffractometer
9864 independent reflections
Absorption correction: part of the refinement model (ΔF)
(DELABS in PLATON; Spek, 2000)
7715 reflections with I > 2σ(I)
Tmin = 0.891, Tmax = 0.936Rint = 0.081
35034 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.048H-atom parameters constrained
wR(F2) = 0.125Δρmax = 0.33 e Å3
S = 1.05Δρmin = 0.43 e Å3
9864 reflectionsAbsolute structure: Flack (1983), 4416 Friedel pairs?
600 parametersAbsolute structure parameter: 0.03 (5)
1 restraint
Special details top

Experimental. The unit-cell parameters have been determined from 10 frames, then refined on all data. The crystal-to-detector distance was fixed to 30 mm. One-half of the diffraction sphere was scanned (90 frames, ϕ scans, 2° by frame).

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 subsequent Fourier-difference synthesis. All non-hydrogen atoms were refined with anisotropic displacement parameters. The H atoms bound to O atoms were found on a Fourier-difference map and all the other ones were introduced at calculated positions. All H atoms were treated as riding atoms with an isotropic displacement parameter equal to 1.2 (OH, CH, CH2) or 1.5 (CH3) times that of the parent atom. 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
O10.84998 (11)0.37195 (11)1.0158 (2)0.0261 (6)
O20.78661 (12)0.34530 (13)1.2415 (3)0.0393 (7)
O30.85779 (12)0.36756 (11)1.3917 (3)0.0315 (6)
O40.74012 (11)0.34386 (10)0.9239 (3)0.0287 (6)
H40.76790.35440.98170.034*
O50.76656 (11)0.24116 (11)0.8486 (3)0.0282 (6)
H50.75220.27520.88640.034*
O60.87691 (11)0.25542 (10)0.9253 (3)0.0279 (6)
H60.83850.24710.92390.033*
C10.86951 (18)0.39005 (17)1.1525 (4)0.0296 (9)
H1A0.86750.43001.15880.036*
H1B0.90830.37891.16660.036*
C20.83246 (16)0.36409 (15)1.2646 (4)0.0257 (8)
C30.82578 (19)0.34695 (19)1.5119 (4)0.0370 (10)
H3A0.78960.36461.51410.055*
H3B0.84560.35481.59890.055*
H3C0.82080.30781.50240.055*
C40.84143 (15)0.44835 (15)0.8555 (4)0.0237 (8)
C50.87297 (16)0.40331 (15)0.9042 (4)0.0258 (8)
C60.92450 (16)0.38912 (15)0.8424 (4)0.0235 (8)
C70.94548 (16)0.42335 (15)0.7358 (4)0.0274 (8)
H70.98010.41470.69510.033*
C80.91715 (16)0.46973 (15)0.6874 (4)0.0248 (8)
C90.86455 (16)0.48097 (15)0.7482 (4)0.0271 (8)
H90.84430.51130.71560.032*
C100.94119 (17)0.50817 (17)0.5738 (4)0.0315 (9)
C110.9021 (2)0.5089 (2)0.4439 (5)0.0562 (14)
H11A0.89680.47190.40970.084*
H11B0.91850.53100.36980.084*
H11C0.86630.52420.47090.084*
C120.9995 (2)0.4910 (2)0.5274 (6)0.0569 (15)
H12A1.02310.48690.61000.085*
H12B1.01500.51870.46550.085*
H12C0.99740.45650.47730.085*
C130.9456 (2)0.56757 (18)0.6334 (5)0.0463 (12)
H13A0.90920.57970.66470.069*
H13B0.95920.59180.55980.069*
H13C0.97130.56810.71260.069*
C140.78198 (15)0.45866 (16)0.9077 (4)0.0289 (9)
H14A0.77730.44251.00190.035*
H14B0.77550.49810.91550.035*
C150.73955 (16)0.43375 (15)0.8059 (4)0.0253 (8)
C160.72352 (16)0.37851 (16)0.8138 (4)0.0264 (8)
C170.68808 (15)0.35511 (15)0.7097 (4)0.0256 (8)
C180.66887 (16)0.38882 (16)0.5989 (4)0.0280 (9)
H180.64530.37370.52990.034*
C190.68380 (16)0.44453 (16)0.5877 (4)0.0272 (8)
C200.71893 (16)0.46534 (16)0.6930 (4)0.0280 (8)
H200.72930.50230.68800.034*
C210.66268 (17)0.47833 (16)0.4605 (4)0.0325 (9)
C220.6933 (2)0.45768 (19)0.3238 (5)0.0438 (11)
H22A0.73320.46190.33560.066*
H22B0.68100.47890.24300.066*
H22C0.68460.41940.30840.066*
C230.67517 (19)0.53989 (17)0.4793 (5)0.0404 (10)
H23A0.65800.55280.56590.061*
H23B0.66020.56000.39950.061*
H23C0.71510.54540.48440.061*
C240.59894 (18)0.47107 (18)0.4403 (5)0.0405 (10)
H24A0.59060.43280.42350.061*
H24B0.58670.49260.35990.061*
H24C0.57970.48330.52480.061*
C250.67126 (15)0.29458 (15)0.7125 (4)0.0252 (8)
H25A0.66890.28260.81120.030*
H25B0.63410.29090.67070.030*
C260.71144 (16)0.25691 (15)0.6335 (4)0.0246 (8)
C270.75663 (16)0.23207 (15)0.7039 (4)0.0244 (8)
C280.79347 (16)0.19611 (16)0.6336 (4)0.0256 (8)
C290.78374 (15)0.18547 (15)0.4903 (4)0.0257 (8)
H290.80750.16100.44310.031*
C300.73967 (15)0.20996 (15)0.4131 (4)0.0245 (8)
C310.70470 (16)0.24568 (15)0.4879 (4)0.0259 (8)
H310.67550.26290.43900.031*
C320.73149 (16)0.19458 (16)0.2554 (4)0.0294 (9)
C330.78782 (17)0.19568 (19)0.1762 (4)0.0348 (10)
H33A0.80360.23210.18120.052*
H33B0.78200.18570.07800.052*
H33C0.81320.16990.21980.052*
C340.69181 (18)0.23457 (19)0.1790 (4)0.0355 (10)
H34A0.65510.23260.22170.053*
H34B0.68930.22470.07980.053*
H34C0.70610.27150.18740.053*
C350.7075 (2)0.13616 (17)0.2471 (5)0.0414 (11)
H35A0.73330.11080.29120.062*
H35B0.70210.12610.14880.062*
H35C0.67200.13490.29620.062*
C360.84456 (15)0.17306 (15)0.7085 (4)0.0263 (8)
H36A0.85460.13770.66680.032*
H36B0.83620.16730.80890.032*
C370.89356 (15)0.21324 (15)0.6935 (4)0.0246 (8)
C380.90523 (16)0.25303 (15)0.7985 (4)0.0261 (8)
C390.94807 (16)0.29137 (15)0.7771 (4)0.0250 (8)
C400.97927 (16)0.28966 (15)0.6502 (4)0.0284 (9)
H401.00800.31520.63690.034*
C410.96875 (16)0.25091 (16)0.5430 (4)0.0267 (8)
C420.92524 (15)0.21300 (16)0.5689 (4)0.0262 (8)
H420.91730.18660.49960.031*
C431.00031 (16)0.24939 (17)0.4011 (4)0.0297 (9)
C441.0390 (2)0.29940 (19)0.3823 (6)0.0519 (13)
H44A1.01730.33270.39010.078*
H44B1.05650.29790.28990.078*
H44C1.06750.29900.45510.078*
C451.03587 (19)0.19695 (18)0.3916 (5)0.0383 (10)
H45A1.06330.19690.46690.057*
H45B1.05460.19580.30080.057*
H45C1.01200.16520.40120.057*
C460.95818 (19)0.2497 (2)0.2756 (4)0.0427 (11)
H46A0.93490.21740.28060.064*
H46B0.97840.24980.18680.064*
H46C0.93500.28210.28140.064*
C470.95712 (16)0.33717 (15)0.8855 (4)0.0270 (8)
H47A0.99690.34570.89170.032*
H47B0.94460.32490.97890.032*
Cl10.87051 (6)0.65385 (5)0.29993 (16)0.0611 (4)
Cl20.78031 (5)0.57748 (6)0.23818 (19)0.0680 (4)
Cl30.87814 (6)0.58005 (6)0.06059 (14)0.0575 (3)
C480.83252 (18)0.61951 (17)0.1667 (5)0.0350 (10)
H480.81450.64730.10570.042*
Cl40.44406 (6)0.51353 (6)0.54680 (14)0.0585 (4)
Cl50.44283 (6)0.44421 (6)0.29698 (14)0.0597 (4)
Cl60.34256 (4)0.45547 (5)0.46941 (13)0.0435 (3)
C490.40308 (19)0.48882 (18)0.4040 (4)0.0390 (10)
H490.39120.52030.34560.047*
Cl70.56806 (6)0.32987 (7)0.96994 (16)0.0691 (4)
Cl80.52589 (7)0.39355 (5)0.73349 (14)0.0613 (4)
Cl90.45409 (5)0.36963 (5)0.97551 (14)0.0480 (3)
C500.50905 (18)0.34566 (19)0.8669 (5)0.0373 (10)
H500.49640.31160.82020.045*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0315 (14)0.0283 (14)0.0186 (12)0.0043 (11)0.0006 (11)0.0002 (10)
O20.0339 (16)0.0517 (18)0.0323 (15)0.0093 (14)0.0004 (13)0.0006 (14)
O30.0338 (15)0.0390 (17)0.0219 (13)0.0076 (13)0.0009 (12)0.0028 (12)
O40.0328 (15)0.0274 (14)0.0260 (14)0.0023 (11)0.0047 (12)0.0001 (11)
O50.0356 (15)0.0296 (15)0.0194 (12)0.0000 (12)0.0013 (11)0.0017 (10)
O60.0286 (14)0.0300 (15)0.0251 (13)0.0039 (11)0.0051 (11)0.0034 (11)
C10.036 (2)0.036 (2)0.0166 (18)0.0069 (18)0.0004 (17)0.0001 (16)
C20.031 (2)0.0241 (19)0.0215 (19)0.0009 (16)0.0002 (17)0.0031 (14)
C30.044 (2)0.047 (3)0.0200 (19)0.008 (2)0.0042 (18)0.0046 (17)
C40.0245 (19)0.0205 (19)0.0261 (18)0.0016 (15)0.0020 (16)0.0048 (15)
C50.030 (2)0.0232 (19)0.0245 (19)0.0058 (16)0.0001 (17)0.0001 (15)
C60.027 (2)0.0215 (19)0.0221 (18)0.0006 (15)0.0052 (16)0.0017 (14)
C70.030 (2)0.025 (2)0.0272 (19)0.0017 (16)0.0021 (17)0.0006 (16)
C80.029 (2)0.0211 (19)0.0240 (19)0.0020 (15)0.0017 (17)0.0008 (14)
C90.030 (2)0.0228 (19)0.0285 (19)0.0002 (16)0.0008 (17)0.0019 (15)
C100.037 (2)0.031 (2)0.027 (2)0.0011 (18)0.0050 (19)0.0039 (16)
C110.081 (4)0.056 (3)0.031 (2)0.020 (3)0.011 (3)0.015 (2)
C120.064 (3)0.049 (3)0.057 (3)0.014 (3)0.031 (3)0.025 (2)
C130.057 (3)0.036 (3)0.046 (3)0.015 (2)0.005 (2)0.003 (2)
C140.029 (2)0.026 (2)0.032 (2)0.0038 (16)0.0021 (17)0.0042 (16)
C150.0233 (19)0.024 (2)0.0283 (19)0.0014 (15)0.0040 (16)0.0046 (15)
C160.0256 (19)0.028 (2)0.0259 (19)0.0012 (16)0.0029 (17)0.0002 (15)
C170.0221 (18)0.023 (2)0.031 (2)0.0026 (14)0.0030 (17)0.0020 (16)
C180.028 (2)0.029 (2)0.028 (2)0.0014 (17)0.0034 (17)0.0010 (16)
C190.0258 (19)0.023 (2)0.032 (2)0.0012 (16)0.0052 (18)0.0024 (16)
C200.027 (2)0.024 (2)0.034 (2)0.0009 (16)0.0022 (18)0.0007 (16)
C210.036 (2)0.029 (2)0.032 (2)0.0036 (17)0.0001 (19)0.0045 (18)
C220.054 (3)0.042 (3)0.036 (2)0.007 (2)0.008 (2)0.007 (2)
C230.043 (2)0.033 (2)0.045 (2)0.0009 (19)0.005 (2)0.013 (2)
C240.039 (2)0.037 (3)0.045 (3)0.0007 (19)0.004 (2)0.0125 (19)
C250.0206 (18)0.028 (2)0.028 (2)0.0031 (15)0.0000 (16)0.0019 (15)
C260.028 (2)0.0188 (19)0.0275 (19)0.0047 (16)0.0032 (16)0.0006 (15)
C270.030 (2)0.0198 (18)0.0229 (18)0.0054 (16)0.0005 (17)0.0017 (14)
C280.0243 (19)0.0239 (19)0.0287 (19)0.0031 (16)0.0020 (16)0.0033 (16)
C290.0253 (18)0.027 (2)0.0249 (19)0.0060 (15)0.0004 (17)0.0018 (15)
C300.0254 (19)0.0214 (19)0.027 (2)0.0046 (15)0.0012 (16)0.0026 (15)
C310.0246 (18)0.026 (2)0.0266 (19)0.0041 (15)0.0021 (16)0.0038 (16)
C320.031 (2)0.030 (2)0.027 (2)0.0042 (17)0.0000 (17)0.0012 (16)
C330.037 (2)0.046 (3)0.022 (2)0.0037 (19)0.0011 (18)0.0018 (17)
C340.031 (2)0.045 (3)0.030 (2)0.0011 (19)0.0031 (18)0.0008 (18)
C350.060 (3)0.034 (2)0.030 (2)0.012 (2)0.001 (2)0.0034 (18)
C360.0275 (19)0.0216 (19)0.030 (2)0.0015 (15)0.0024 (17)0.0002 (15)
C370.0243 (19)0.026 (2)0.0240 (19)0.0003 (15)0.0025 (16)0.0009 (15)
C380.029 (2)0.026 (2)0.0234 (18)0.0007 (16)0.0003 (17)0.0046 (15)
C390.0270 (19)0.0218 (19)0.026 (2)0.0038 (15)0.0027 (17)0.0008 (15)
C400.023 (2)0.025 (2)0.037 (2)0.0009 (16)0.0021 (17)0.0007 (17)
C410.0283 (19)0.024 (2)0.0275 (19)0.0016 (16)0.0005 (17)0.0035 (15)
C420.0250 (19)0.027 (2)0.0261 (19)0.0024 (16)0.0011 (17)0.0014 (16)
C430.029 (2)0.030 (2)0.030 (2)0.0027 (17)0.0064 (17)0.0003 (17)
C440.061 (3)0.041 (3)0.054 (3)0.015 (2)0.034 (3)0.006 (2)
C450.040 (2)0.039 (2)0.036 (2)0.006 (2)0.002 (2)0.0051 (19)
C460.041 (3)0.057 (3)0.030 (2)0.014 (2)0.004 (2)0.009 (2)
C470.0238 (19)0.029 (2)0.029 (2)0.0009 (16)0.0037 (16)0.0016 (16)
Cl10.0713 (9)0.0439 (7)0.0681 (8)0.0131 (6)0.0327 (7)0.0081 (6)
Cl20.0369 (6)0.0669 (9)0.1003 (11)0.0027 (6)0.0029 (7)0.0479 (8)
Cl30.0652 (8)0.0591 (8)0.0481 (7)0.0307 (7)0.0085 (6)0.0072 (6)
C480.035 (2)0.031 (2)0.039 (2)0.0063 (18)0.0001 (19)0.0023 (18)
Cl40.0599 (8)0.0709 (9)0.0447 (7)0.0218 (7)0.0042 (6)0.0023 (6)
Cl50.0596 (8)0.0692 (9)0.0502 (7)0.0142 (7)0.0065 (6)0.0076 (6)
Cl60.0392 (6)0.0401 (6)0.0513 (6)0.0048 (5)0.0035 (5)0.0119 (5)
C490.046 (3)0.037 (3)0.035 (2)0.006 (2)0.001 (2)0.0055 (19)
Cl70.0463 (7)0.1094 (12)0.0517 (7)0.0234 (7)0.0010 (7)0.0079 (8)
Cl80.0898 (10)0.0547 (8)0.0394 (6)0.0283 (7)0.0045 (7)0.0010 (6)
Cl90.0381 (6)0.0479 (7)0.0580 (7)0.0012 (5)0.0093 (6)0.0130 (6)
C500.033 (2)0.040 (3)0.040 (2)0.0040 (19)0.004 (2)0.0041 (19)
Geometric parameters (Å, º) top
O1—C51.402 (4)C25—C261.513 (5)
O1—C11.429 (4)C25—H25A0.9700
O2—C21.200 (5)C25—H25B0.9700
O3—C21.335 (5)C26—C271.396 (5)
O3—C31.446 (4)C26—C311.398 (5)
O4—C161.386 (5)C27—C281.399 (5)
O4—H40.8901C28—C291.384 (5)
O5—C271.392 (4)C28—C361.509 (5)
O5—H50.9594C29—C301.404 (5)
O6—C381.365 (4)C29—H290.9300
O6—H60.9345C30—C311.389 (5)
C1—C21.507 (5)C30—C321.533 (5)
C1—H1A0.9700C31—H310.9300
C1—H1B0.9700C32—C341.529 (6)
C3—H3A0.9600C32—C351.528 (6)
C3—H3B0.9600C32—C331.530 (6)
C3—H3C0.9600C33—H33A0.9600
C4—C91.391 (5)C33—H33B0.9600
C4—C51.399 (5)C33—H33C0.9600
C4—C141.515 (5)C34—H34A0.9600
C5—C61.397 (5)C34—H34B0.9600
C6—C71.390 (5)C34—H34C0.9600
C6—C471.532 (5)C35—H35A0.9600
C7—C81.386 (5)C35—H35B0.9600
C7—H70.9300C35—H35C0.9600
C8—C91.399 (5)C36—C371.524 (5)
C8—C101.524 (5)C36—H36A0.9700
C9—H90.9300C36—H36B0.9700
C10—C121.511 (6)C37—C421.388 (5)
C10—C111.530 (6)C37—C381.403 (5)
C10—C131.547 (6)C38—C391.392 (5)
C11—H11A0.9600C39—C401.400 (5)
C11—H11B0.9600C39—C471.518 (5)
C11—H11C0.9600C40—C411.396 (5)
C12—H12A0.9600C40—H400.9300
C12—H12B0.9600C41—C421.404 (5)
C12—H12C0.9600C41—C431.525 (5)
C13—H13A0.9600C42—H420.9300
C13—H13B0.9600C43—C451.528 (6)
C13—H13C0.9600C43—C441.531 (6)
C14—C151.513 (5)C43—C461.543 (6)
C14—H14A0.9700C44—H44A0.9600
C14—H14B0.9700C44—H44B0.9600
C15—C161.393 (5)C44—H44C0.9600
C15—C201.393 (5)C45—H45A0.9600
C16—C171.406 (5)C45—H45B0.9600
C17—C181.396 (5)C45—H45C0.9600
C17—C251.520 (5)C46—H46A0.9600
C18—C191.399 (5)C46—H46B0.9600
C18—H180.9300C46—H46C0.9600
C19—C201.386 (6)C47—H47A0.9700
C19—C211.529 (6)C47—H47B0.9700
C20—H200.9300Cl1—C481.749 (4)
C21—C231.531 (6)Cl2—C481.739 (4)
C21—C241.536 (6)Cl3—C481.753 (4)
C21—C221.554 (6)C48—H480.9800
C22—H22A0.9600Cl4—C491.758 (4)
C22—H22B0.9600Cl5—C491.750 (5)
C22—H22C0.9600Cl6—C491.759 (4)
C23—H23A0.9600C49—H490.9800
C23—H23B0.9600Cl7—C501.744 (5)
C23—H23C0.9600Cl8—C501.750 (5)
C24—H24A0.9600Cl9—C501.753 (4)
C24—H24B0.9600C50—H500.9800
C24—H24C0.9600
C5—O1—C1112.0 (3)H25A—C25—H25B107.6
C2—O3—C3115.7 (3)C27—C26—C31117.6 (3)
C16—O4—H4119.2C27—C26—C25121.0 (3)
C27—O5—H5115.7C31—C26—C25121.4 (3)
C38—O6—H6117.4O5—C27—C26121.4 (3)
O1—C1—C2107.8 (3)O5—C27—C28116.7 (3)
O1—C1—H1A110.2C26—C27—C28121.9 (3)
C2—C1—H1A110.2C29—C28—C27117.8 (4)
O1—C1—H1B110.2C29—C28—C36121.0 (3)
C2—C1—H1B110.2C27—C28—C36121.0 (3)
H1A—C1—H1B108.5C28—C29—C30123.0 (4)
O2—C2—O3126.4 (4)C28—C29—H29118.5
O2—C2—C1124.3 (3)C30—C29—H29118.5
O3—C2—C1109.3 (3)C31—C30—C29116.7 (3)
O3—C3—H3A109.5C31—C30—C32124.1 (3)
O3—C3—H3B109.5C29—C30—C32119.2 (3)
H3A—C3—H3B109.5C30—C31—C26122.9 (4)
O3—C3—H3C109.5C30—C31—H31118.5
H3A—C3—H3C109.5C26—C31—H31118.5
H3B—C3—H3C109.5C34—C32—C35109.5 (3)
C9—C4—C5117.8 (3)C34—C32—C33107.6 (3)
C9—C4—C14120.5 (3)C35—C32—C33108.5 (4)
C5—C4—C14121.5 (3)C34—C32—C30112.0 (3)
C6—C5—C4121.8 (3)C35—C32—C30108.7 (3)
C6—C5—O1121.1 (3)C33—C32—C30110.5 (3)
C4—C5—O1117.1 (3)C32—C33—H33A109.5
C7—C6—C5117.7 (3)C32—C33—H33B109.5
C7—C6—C47119.8 (3)H33A—C33—H33B109.5
C5—C6—C47122.5 (3)C32—C33—H33C109.5
C8—C7—C6123.0 (4)H33A—C33—H33C109.5
C8—C7—H7118.5H33B—C33—H33C109.5
C6—C7—H7118.5C32—C34—H34A109.5
C7—C8—C9117.3 (3)C32—C34—H34B109.5
C7—C8—C10122.8 (3)H34A—C34—H34B109.5
C9—C8—C10119.9 (3)C32—C34—H34C109.5
C4—C9—C8122.4 (3)H34A—C34—H34C109.5
C4—C9—H9118.8H34B—C34—H34C109.5
C8—C9—H9118.8C32—C35—H35A109.5
C12—C10—C8112.1 (3)C32—C35—H35B109.5
C12—C10—C11109.4 (4)H35A—C35—H35B109.5
C8—C10—C11109.5 (3)C32—C35—H35C109.5
C12—C10—C13107.3 (4)H35A—C35—H35C109.5
C8—C10—C13110.0 (3)H35B—C35—H35C109.5
C11—C10—C13108.5 (4)C28—C36—C37109.6 (3)
C10—C11—H11A109.5C28—C36—H36A109.7
C10—C11—H11B109.5C37—C36—H36A109.7
H11A—C11—H11B109.5C28—C36—H36B109.7
C10—C11—H11C109.5C37—C36—H36B109.7
H11A—C11—H11C109.5H36A—C36—H36B108.2
H11B—C11—H11C109.5C42—C37—C38118.9 (3)
C10—C12—H12A109.5C42—C37—C36119.3 (3)
C10—C12—H12B109.5C38—C37—C36121.7 (3)
H12A—C12—H12B109.5O6—C38—C39117.2 (3)
C10—C12—H12C109.5O6—C38—C37122.7 (3)
H12A—C12—H12C109.5C39—C38—C37120.1 (3)
H12B—C12—H12C109.5C38—C39—C40119.3 (3)
C10—C13—H13A109.5C38—C39—C47119.7 (3)
C10—C13—H13B109.5C40—C39—C47120.8 (3)
H13A—C13—H13B109.5C41—C40—C39122.3 (4)
C10—C13—H13C109.5C41—C40—H40118.9
H13A—C13—H13C109.5C39—C40—H40118.9
H13B—C13—H13C109.5C40—C41—C42116.6 (4)
C15—C14—C4110.6 (3)C40—C41—C43123.6 (4)
C15—C14—H14A109.5C42—C41—C43119.8 (3)
C4—C14—H14A109.5C37—C42—C41122.8 (4)
C15—C14—H14B109.5C37—C42—H42118.6
C4—C14—H14B109.5C41—C42—H42118.6
H14A—C14—H14B108.1C41—C43—C45110.0 (3)
C16—C15—C20118.1 (3)C41—C43—C44112.1 (3)
C16—C15—C14122.1 (4)C45—C43—C44108.6 (4)
C20—C15—C14119.5 (3)C41—C43—C46110.1 (3)
O4—C16—C15122.9 (3)C45—C43—C46108.6 (3)
O4—C16—C17116.2 (3)C44—C43—C46107.4 (4)
C15—C16—C17120.9 (4)C43—C44—H44A109.5
C18—C17—C16118.3 (3)C43—C44—H44B109.5
C18—C17—C25119.4 (3)H44A—C44—H44B109.5
C16—C17—C25122.3 (3)C43—C44—H44C109.5
C17—C18—C19122.4 (4)H44A—C44—H44C109.5
C17—C18—H18118.8H44B—C44—H44C109.5
C19—C18—H18118.8C43—C45—H45A109.5
C20—C19—C18116.8 (4)C43—C45—H45B109.5
C20—C19—C21123.8 (3)H45A—C45—H45B109.5
C18—C19—C21119.4 (4)C43—C45—H45C109.5
C19—C20—C15123.4 (4)H45A—C45—H45C109.5
C19—C20—H20118.3H45B—C45—H45C109.5
C15—C20—H20118.3C43—C46—H46A109.5
C19—C21—C23111.6 (3)C43—C46—H46B109.5
C19—C21—C24111.0 (3)H46A—C46—H46B109.5
C23—C21—C24108.5 (3)C43—C46—H46C109.5
C19—C21—C22108.3 (3)H46A—C46—H46C109.5
C23—C21—C22108.5 (4)H46B—C46—H46C109.5
C24—C21—C22108.9 (4)C39—C47—C6110.7 (3)
C21—C22—H22A109.5C39—C47—H47A109.5
C21—C22—H22B109.5C6—C47—H47A109.5
H22A—C22—H22B109.5C39—C47—H47B109.5
C21—C22—H22C109.5C6—C47—H47B109.5
H22A—C22—H22C109.5H47A—C47—H47B108.1
H22B—C22—H22C109.5Cl2—C48—Cl1111.9 (2)
C21—C23—H23A109.5Cl2—C48—Cl3109.9 (2)
C21—C23—H23B109.5Cl1—C48—Cl3110.1 (2)
H23A—C23—H23B109.5Cl2—C48—H48108.3
C21—C23—H23C109.5Cl1—C48—H48108.3
H23A—C23—H23C109.5Cl3—C48—H48108.3
H23B—C23—H23C109.5Cl5—C49—Cl4110.2 (3)
C21—C24—H24A109.5Cl5—C49—Cl6110.9 (2)
C21—C24—H24B109.5Cl4—C49—Cl6110.2 (2)
H24A—C24—H24B109.5Cl5—C49—H49108.5
C21—C24—H24C109.5Cl4—C49—H49108.5
H24A—C24—H24C109.5Cl6—C49—H49108.5
H24B—C24—H24C109.5Cl7—C50—Cl8110.8 (2)
C26—C25—C17114.1 (3)Cl7—C50—Cl9110.6 (2)
C26—C25—H25A108.7Cl8—C50—Cl9111.3 (3)
C17—C25—H25A108.7Cl7—C50—H50108.0
C26—C25—H25B108.7Cl8—C50—H50108.0
C17—C25—H25B108.7Cl9—C50—H50108.0
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O4—H4···O10.892.022.831 (4)151
O4—H4···O20.892.483.170 (4)135
O5—H5···O40.961.722.661 (4)164
O6—H6···O50.931.852.740 (4)157

Experimental details

Crystal data
Chemical formulaC47H60O6·3CHCl3
Mr1079.05
Crystal system, space groupOrthorhombic, Pna21
Temperature (K)100
a, b, c (Å)23.7595 (9), 24.2234 (8), 9.3546 (3)
V3)5383.9 (3)
Z4
Radiation typeMo Kα
µ (mm1)0.51
Crystal size (mm)0.26 × 0.14 × 0.12
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correctionPart of the refinement model (ΔF)
(DELABS in PLATON; Spek, 2000)
Tmin, Tmax0.891, 0.936
No. of measured, independent and
observed [I > 2σ(I)] reflections
35034, 9864, 7715
Rint0.081
(sin θ/λ)max1)0.610
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.048, 0.125, 1.05
No. of reflections9864
No. of parameters600
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.33, 0.43
Absolute structureFlack (1983), 4416 Friedel pairs?
Absolute structure parameter0.03 (5)

Computer programs: KappaCCD Software (Nonius, 1997), DENZO–SMN (Otwinowski & Minor, 1997), DENZO–SMN, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1999) and PLATON (Spek, 2000).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O4—H4···O10.892.022.831 (4)151
O4—H4···O20.892.483.170 (4)135
O5—H5···O40.961.722.661 (4)164
O6—H6···O50.931.852.740 (4)157
 

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