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The title compound, C50H60O6, is a new p-tert-butylcalix[4]arene derivative, adopting a 1,3-alternate conformation, with the complete mol­ecule generated by twofold rotation symmetry. In the crystal structure, the mol­ecules associate into layers in the ac plane. The three methyl groups of one tert-butyl group are disordered over two positions with site-occupancy factors approximately in the ratio 3:1.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807031996/hb2469sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807031996/hb2469Isup2.hkl
Contains datablock I

CCDC reference: 610039

Key indicators

  • Single-crystal X-ray study
  • T = 297 K
  • Mean [sigma](C-C) = 0.004 Å
  • Disorder in main residue
  • R factor = 0.058
  • wR factor = 0.153
  • Data-to-parameter ratio = 14.7

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT242_ALERT_2_B Check Low Ueq as Compared to Neighbors for C22 PLAT420_ALERT_2_B D-H Without Acceptor O3 - H3 ... ?
Alert level C RINTA01_ALERT_3_C The value of Rint is greater than 0.10 Rint given 0.131 PLAT020_ALERT_3_C The value of Rint is greater than 0.10 ......... 0.13 PLAT026_ALERT_3_C Ratio Observed / Unique Reflections too Low .... 46 Perc. PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 3.22 Ratio PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C11 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C15 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C16 PLAT301_ALERT_3_C Main Residue Disorder ......................... 10.00 Perc.
Alert level G PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 69
0 ALERT level A = In general: serious problem 2 ALERT level B = Potentially serious problem 8 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 6 ALERT type 2 Indicator that the structure model may be wrong or deficient 5 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

For the past 20 years the calixarenes, cavity-shaped macrocycles, have attracted much attention mainly in supramolecular and analytical chemistry, because they can form typical host–guest complexes with many neutral molecules and ions, like cyclodextrins and crown ethers (Gutsche & Alam, 1988; Gutsche, 1989). Owing to their nonplanar structure, calix[4]arenes can exist in one of the four conformations, and has been designated as cone, partial cone, 1,2-alternate, and 1,3-alternate [Andreetti et al., 1991; Casnati et al., 1995; Kim et al., 1999; Kim et al., 2000). By placing substituents at OH groups larger than methyl, conformation can be locked. Very often cone and partial cone conformes were synthesized by the alkylation (Iwamoto et al., 1991) and acylation (Gutsche & Lin, 1986) reaction at lover rim of calix[4]arene. But 1,2-alternate and 1,3-alternate conformers were observed only under certain reaction conditions.

As part of our work on substituted calix[4]arenes, we report herein the crystal structure of the title compound, (I), adopting a 1,3-alternate conformation. The two phenyl groups, A and D, lie above and the other two phenyl groups, B and C, below the least-squares plane defined by the four bridging methylene group, as illustrated in Fig. 1. The complete molecule is generated by 2-fold rotation symmetry. Bond angles involving the bridging methylene groups, i.e, C5—C7—C8 [116.2 (2)°] and C3—C18—C19 [116.4 (2)°], are significantly larger than the tetrahedral angle due to repulsion among the four phenyl groups. The dihedral angles of two pairs of facing rings, namely A and D, to which the OH group is bonded, and B and C, to which the acryloiloxy group is bonded, are 35.34 (10) and 20.01 (11)° respectively, so that rings A and D are splayed out upwards, and C and B are splayed out downwards from the central axis. Dihedral angles of adjacent phenyl rings in the calix[4]arene range from 85.13 (7) to 88.82 (7)°.

In the extended structure, there are no hydrogen bonding interactions and van der Waals interactions stabilize the extended structure (Fig. 2).

Related literature top

For related literature, see: Andreetti et al. (1991); Casnati et al. (1995); Gutsche (1989); Gutsche & Alam (1988); Gutsche & Lin (1986); Iwamoto et al. (1991); Kim et al. (1999, 2000).

Experimental top

The title compound was synthesized according to the literature method of Gutsche & Lin (1986) and colourless plates of (I) were recrystallized from toluene.

Refinement top

The H atoms were placed at calculated positions (O—H = 0.82 Å, C—H = 0.93–0.96 Å) and refined as riding with Uiso(H) = 1.2eq(C) or 1.5Ueq(O, methyl C).

The disordered tetra-tert-butyl moiety [site-occupancy factors of 0.753 (9) for C44A/C88A/C99A and 0.247 (9) for C44B/C88B/C99B] was refined anisotropically, with constraints and restraints imposed on the anisotropic displacement parameters of C atoms.

Structure description top

For the past 20 years the calixarenes, cavity-shaped macrocycles, have attracted much attention mainly in supramolecular and analytical chemistry, because they can form typical host–guest complexes with many neutral molecules and ions, like cyclodextrins and crown ethers (Gutsche & Alam, 1988; Gutsche, 1989). Owing to their nonplanar structure, calix[4]arenes can exist in one of the four conformations, and has been designated as cone, partial cone, 1,2-alternate, and 1,3-alternate [Andreetti et al., 1991; Casnati et al., 1995; Kim et al., 1999; Kim et al., 2000). By placing substituents at OH groups larger than methyl, conformation can be locked. Very often cone and partial cone conformes were synthesized by the alkylation (Iwamoto et al., 1991) and acylation (Gutsche & Lin, 1986) reaction at lover rim of calix[4]arene. But 1,2-alternate and 1,3-alternate conformers were observed only under certain reaction conditions.

As part of our work on substituted calix[4]arenes, we report herein the crystal structure of the title compound, (I), adopting a 1,3-alternate conformation. The two phenyl groups, A and D, lie above and the other two phenyl groups, B and C, below the least-squares plane defined by the four bridging methylene group, as illustrated in Fig. 1. The complete molecule is generated by 2-fold rotation symmetry. Bond angles involving the bridging methylene groups, i.e, C5—C7—C8 [116.2 (2)°] and C3—C18—C19 [116.4 (2)°], are significantly larger than the tetrahedral angle due to repulsion among the four phenyl groups. The dihedral angles of two pairs of facing rings, namely A and D, to which the OH group is bonded, and B and C, to which the acryloiloxy group is bonded, are 35.34 (10) and 20.01 (11)° respectively, so that rings A and D are splayed out upwards, and C and B are splayed out downwards from the central axis. Dihedral angles of adjacent phenyl rings in the calix[4]arene range from 85.13 (7) to 88.82 (7)°.

In the extended structure, there are no hydrogen bonding interactions and van der Waals interactions stabilize the extended structure (Fig. 2).

For related literature, see: Andreetti et al. (1991); Casnati et al. (1995); Gutsche (1989); Gutsche & Alam (1988); Gutsche & Lin (1986); Iwamoto et al. (1991); Kim et al. (1999, 2000).

Computing details top

Data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 20% probability level and H atoms are omitted for the clarity. Symmetry code: (i) 1 - x, y, 0.5 - z.
[Figure 2] Fig. 2. The extended structure of (I).
25,27-Bis(acryloyloxy)-5,11,17,23-tetra-tert-butyl-26,28-dihydroxycalix[4]arene top
Crystal data top
C50H60O6F(000) = 1632
Mr = 756.98Dx = 1.158 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71069 Å
Hall symbol: -C 2ycCell parameters from 2487 reflections
a = 15.8896 (11) Åθ = 2.0–28.1°
b = 26.482 (2) ŵ = 0.07 mm1
c = 10.3522 (7) ÅT = 297 K
β = 95.047 (6)°Plate, colorless
V = 4339.2 (5) Å30.41 × 0.24 × 0.09 mm
Z = 4
Data collection top
Stoe IPDS2
diffractometer
4277 independent reflections
Radiation source: fine-focus sealed tube1985 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.131
Detector resolution: 6.67 pixels mm-1θmax = 26.0°, θmin = 2.4°
ω scansh = 1919
Absorption correction: integration
(X-RED32; Stoe & Cie, 2002)
k = 3232
Tmin = 0.940, Tmax = 0.983l = 1212
28360 measured 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)] = 0.058H-atom parameters constrained
wR(F2) = 0.153 w = 1/[σ2(Fo2) + (0.0732P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.89(Δ/σ)max < 0.001
4277 reflectionsΔρmax = 0.28 e Å3
291 parametersΔρmin = 0.25 e Å3
69 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0017 (3)
Crystal data top
C50H60O6V = 4339.2 (5) Å3
Mr = 756.98Z = 4
Monoclinic, C2/cMo Kα radiation
a = 15.8896 (11) ŵ = 0.07 mm1
b = 26.482 (2) ÅT = 297 K
c = 10.3522 (7) Å0.41 × 0.24 × 0.09 mm
β = 95.047 (6)°
Data collection top
Stoe IPDS2
diffractometer
4277 independent reflections
Absorption correction: integration
(X-RED32; Stoe & Cie, 2002)
1985 reflections with I > 2σ(I)
Tmin = 0.940, Tmax = 0.983Rint = 0.131
28360 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.05869 restraints
wR(F2) = 0.153H-atom parameters constrained
S = 0.89Δρmax = 0.28 e Å3
4277 reflectionsΔρmin = 0.25 e Å3
291 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.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C10.39759 (18)0.14689 (10)0.4886 (3)0.0489 (7)
C20.33804 (18)0.17650 (10)0.4175 (3)0.0516 (7)
H20.28920.16120.38020.062*
C30.34844 (17)0.22828 (10)0.3998 (3)0.0502 (7)
C40.42153 (18)0.24978 (10)0.4597 (2)0.0488 (7)
C50.48335 (17)0.22247 (10)0.5324 (2)0.0484 (7)
C60.46870 (18)0.17095 (11)0.5453 (3)0.0511 (7)
H60.50870.15180.59450.061*
C70.56389 (18)0.24571 (11)0.5930 (3)0.0556 (7)
H7A0.59940.21890.63110.067*
H7B0.54990.26760.66300.067*
C80.61498 (17)0.27597 (10)0.5029 (2)0.0477 (7)
C90.63760 (17)0.32534 (10)0.5299 (3)0.0522 (7)
H90.62150.33990.60570.063*
C100.68349 (18)0.35436 (10)0.4487 (3)0.0522 (7)
C110.7106 (2)0.40896 (11)0.4792 (3)0.0611 (8)
C120.8071 (2)0.41237 (13)0.4860 (4)0.0823 (11)
H12A0.82450.44630.50760.123*
H12B0.82590.40340.40340.123*
H12C0.83130.38960.55120.123*
C130.6815 (3)0.42761 (13)0.6066 (4)0.0915 (12)
H13A0.62090.42650.60250.137*
H13B0.70040.46170.62180.137*
H13C0.70470.40640.67600.137*
C140.6726 (2)0.44401 (12)0.3718 (4)0.0833 (11)
H14A0.61210.44330.37000.125*
H14B0.68940.43280.28970.125*
H14C0.69240.47780.38840.125*
C150.41891 (19)0.33598 (11)0.5224 (3)0.0613 (8)
C160.4375 (2)0.38666 (13)0.4723 (5)0.0894 (12)
H160.45490.38960.38910.107*
C170.4307 (3)0.4257 (2)0.5384 (7)0.153 (2)
H17A0.41340.42340.62180.183*
H17B0.44290.45710.50430.183*
C180.28391 (17)0.25805 (11)0.3157 (3)0.0549 (7)
H18A0.26280.28490.36790.066*
H18B0.23670.23590.29000.066*
C190.31394 (16)0.28140 (10)0.1945 (2)0.0477 (7)
C200.35920 (17)0.25403 (10)0.1088 (3)0.0475 (6)
C210.29447 (17)0.33092 (10)0.1629 (3)0.0509 (7)
H210.26480.34960.22000.061*
C220.38507 (18)0.08963 (11)0.4972 (3)0.0563 (7)
O10.43527 (12)0.30121 (7)0.43395 (18)0.0581 (5)
O20.39125 (18)0.32601 (9)0.6231 (3)0.0931 (8)
O30.37741 (13)0.20369 (7)0.1318 (2)0.0658 (6)
H30.40290.19240.07260.099*
C88A0.2920 (3)0.07769 (17)0.5133 (7)0.088 (2)0.753 (9)
H88A0.28570.04210.52750.133*0.753 (9)
H88B0.25790.08750.43620.133*0.753 (9)
H88C0.27430.09600.58620.133*0.753 (9)
C99A0.4087 (6)0.0663 (2)0.3724 (6)0.101 (3)0.753 (9)
H99A0.46780.07150.36440.152*0.753 (9)
H99B0.37630.08180.30040.152*0.753 (9)
H99C0.39690.03080.37290.152*0.753 (9)
C44A0.4365 (4)0.06675 (19)0.6111 (6)0.099 (3)0.753 (9)
H44A0.42340.03150.61670.148*0.753 (9)
H44B0.42350.08340.68930.148*0.753 (9)
H44C0.49550.07070.60030.148*0.753 (9)
C44B0.4719 (9)0.0619 (5)0.505 (2)0.095 (7)0.247 (9)
H44D0.50500.07180.58320.142*0.247 (9)
H44E0.50140.07080.43140.142*0.247 (9)
H44F0.46280.02610.50610.142*0.247 (9)
C88B0.3461 (16)0.0783 (6)0.6233 (19)0.105 (8)0.247 (9)
H88D0.34070.04240.63320.157*0.247 (9)
H88E0.29130.09370.62130.157*0.247 (9)
H88F0.38180.09160.69500.157*0.247 (9)
C99B0.3324 (15)0.0678 (6)0.3805 (18)0.102 (7)0.247 (9)
H99D0.33770.03170.38090.153*0.247 (9)
H99E0.35220.08100.30230.153*0.247 (9)
H99F0.27430.07690.38460.153*0.247 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0487 (16)0.0494 (17)0.0488 (15)0.0049 (13)0.0054 (13)0.0044 (13)
C20.0460 (16)0.0515 (17)0.0573 (17)0.0068 (13)0.0054 (14)0.0032 (13)
C30.0496 (16)0.0519 (17)0.0507 (16)0.0022 (13)0.0127 (14)0.0065 (13)
C40.0568 (17)0.0441 (16)0.0476 (15)0.0075 (13)0.0160 (14)0.0049 (13)
C50.0516 (17)0.0543 (18)0.0401 (14)0.0081 (13)0.0078 (13)0.0046 (13)
C60.0524 (17)0.0537 (18)0.0468 (15)0.0035 (13)0.0011 (14)0.0086 (13)
C70.0596 (18)0.0583 (18)0.0482 (16)0.0138 (15)0.0006 (14)0.0008 (13)
C80.0477 (16)0.0484 (17)0.0461 (15)0.0067 (13)0.0016 (13)0.0013 (13)
C90.0520 (17)0.0531 (18)0.0508 (16)0.0078 (13)0.0014 (14)0.0068 (13)
C100.0538 (17)0.0466 (16)0.0563 (17)0.0097 (13)0.0051 (14)0.0070 (13)
C110.070 (2)0.0463 (17)0.0679 (19)0.0130 (14)0.0108 (17)0.0066 (14)
C120.076 (2)0.057 (2)0.113 (3)0.0241 (17)0.004 (2)0.0104 (19)
C130.120 (3)0.068 (2)0.089 (3)0.032 (2)0.027 (2)0.0326 (19)
C140.103 (3)0.047 (2)0.099 (3)0.0034 (18)0.002 (2)0.0021 (18)
C150.0581 (19)0.0485 (19)0.078 (2)0.0042 (14)0.0078 (17)0.0011 (16)
C160.076 (2)0.046 (2)0.144 (4)0.0032 (17)0.003 (2)0.018 (2)
C170.116 (4)0.098 (4)0.248 (7)0.001 (3)0.037 (4)0.009 (4)
C180.0484 (17)0.0525 (17)0.0646 (18)0.0048 (13)0.0103 (15)0.0075 (14)
C190.0418 (15)0.0505 (17)0.0508 (16)0.0034 (12)0.0050 (13)0.0027 (13)
C200.0485 (15)0.0397 (15)0.0537 (16)0.0064 (12)0.0014 (13)0.0001 (12)
C210.0534 (17)0.0448 (17)0.0551 (16)0.0116 (12)0.0081 (14)0.0003 (13)
C220.0590 (18)0.0488 (17)0.0605 (17)0.0030 (13)0.0028 (15)0.0060 (14)
O10.0704 (13)0.0460 (12)0.0593 (12)0.0106 (9)0.0126 (10)0.0055 (9)
O20.122 (2)0.0752 (16)0.0875 (18)0.0008 (14)0.0381 (17)0.0087 (13)
O30.0848 (15)0.0450 (12)0.0699 (13)0.0151 (10)0.0190 (12)0.0017 (10)
C88A0.081 (3)0.050 (3)0.137 (6)0.020 (2)0.025 (4)0.008 (3)
C99A0.154 (7)0.065 (3)0.088 (4)0.014 (4)0.036 (4)0.009 (3)
C44A0.117 (6)0.064 (3)0.107 (5)0.016 (3)0.032 (4)0.026 (3)
C44B0.079 (8)0.053 (9)0.15 (2)0.003 (7)0.007 (8)0.029 (10)
C88B0.15 (2)0.060 (10)0.112 (11)0.009 (10)0.069 (14)0.018 (9)
C99B0.127 (16)0.049 (8)0.121 (11)0.015 (10)0.039 (12)0.016 (9)
Geometric parameters (Å, º) top
C1—C61.382 (4)C16—H160.9300
C1—C21.389 (4)C17—H17A0.9300
C1—C221.533 (4)C17—H17B0.9300
C2—C31.395 (4)C18—C191.513 (4)
C2—H20.9300C18—H18A0.9700
C3—C41.389 (4)C18—H18B0.9700
C3—C181.508 (4)C19—C211.380 (4)
C4—C51.388 (4)C19—C201.394 (3)
C4—O11.409 (3)C20—O31.380 (3)
C5—C61.393 (4)C20—C8i1.388 (4)
C5—C71.506 (4)C21—C10i1.383 (4)
C6—H60.9300C21—H210.9300
C7—C81.518 (4)C22—C44A1.502 (5)
C7—H7A0.9700C22—C99A1.509 (5)
C7—H7B0.9700C22—C99B1.522 (13)
C8—C91.378 (4)C22—C88B1.523 (12)
C8—C20i1.388 (4)C22—C88A1.535 (5)
C9—C101.392 (4)C22—C44B1.558 (12)
C9—H90.9300O3—H30.8200
C10—C21i1.383 (4)C88A—H88A0.9600
C10—C111.534 (4)C88A—H88B0.9600
C11—C131.518 (4)C88A—H88C0.9600
C11—C141.531 (5)C99A—H99A0.9600
C11—C121.531 (4)C99A—H99B0.9600
C12—H12A0.9600C99A—H99C0.9600
C12—H12B0.9600C44A—H44A0.9600
C12—H12C0.9600C44A—H44B0.9600
C13—H13A0.9600C44A—H44C0.9600
C13—H13B0.9600C44B—H44D0.9600
C13—H13C0.9600C44B—H44E0.9600
C14—H14A0.9600C44B—H44F0.9600
C14—H14B0.9600C88B—H88D0.9600
C14—H14C0.9600C88B—H88E0.9600
C15—O21.195 (3)C88B—H88F0.9600
C15—O11.340 (4)C99B—H99D0.9600
C15—C161.478 (5)C99B—H99E0.9600
C16—C171.250 (6)C99B—H99F0.9600
C6—C1—C2117.3 (3)C3—C18—C19116.4 (2)
C6—C1—C22122.5 (3)C3—C18—H18A108.2
C2—C1—C22120.2 (3)C19—C18—H18A108.2
C1—C2—C3122.8 (3)C3—C18—H18B108.2
C1—C2—H2118.6C19—C18—H18B108.2
C3—C2—H2118.6H18A—C18—H18B107.3
C4—C3—C2116.6 (3)C21—C19—C20117.4 (2)
C4—C3—C18122.9 (2)C21—C19—C18120.3 (2)
C2—C3—C18120.5 (3)C20—C19—C18122.2 (2)
C5—C4—C3123.6 (2)O3—C20—C8i118.4 (2)
C5—C4—O1119.5 (2)O3—C20—C19120.3 (2)
C3—C4—O1116.7 (2)C8i—C20—C19121.3 (2)
C4—C5—C6116.5 (3)C19—C21—C10i123.8 (2)
C4—C5—C7123.2 (3)C19—C21—H21118.1
C6—C5—C7120.2 (3)C10i—C21—H21118.1
C1—C6—C5123.2 (3)C44A—C22—C99A110.4 (4)
C1—C6—H6118.4C44A—C22—C99B133.9 (7)
C5—C6—H6118.4C99A—C22—C99B47.6 (9)
C5—C7—C8116.2 (2)C44A—C22—C88B58.7 (9)
C5—C7—H7A108.2C99A—C22—C88B143.5 (7)
C8—C7—H7A108.2C99B—C22—C88B111.7 (13)
C5—C7—H7B108.2C44A—C22—C1112.3 (3)
C8—C7—H7B108.2C99A—C22—C1108.2 (3)
H7A—C7—H7B107.4C99B—C22—C1113.3 (7)
C9—C8—C20i118.4 (2)C88B—C22—C1108.0 (6)
C9—C8—C7121.4 (2)C44A—C22—C88A107.1 (4)
C20i—C8—C7120.3 (2)C99A—C22—C88A108.8 (4)
C8—C9—C10122.9 (3)C99B—C22—C88A62.7 (10)
C8—C9—H9118.6C88B—C22—C88A53.0 (10)
C10—C9—H9118.6C1—C22—C88A109.9 (3)
C21i—C10—C9116.2 (2)C44A—C22—C44B49.5 (8)
C21i—C10—C11120.5 (2)C99A—C22—C44B64.4 (8)
C9—C10—C11123.3 (2)C99B—C22—C44B106.6 (11)
C13—C11—C14107.6 (3)C88B—C22—C44B106.6 (12)
C13—C11—C12108.7 (3)C1—C22—C44B110.5 (6)
C14—C11—C12109.1 (3)C88A—C22—C44B138.9 (7)
C13—C11—C10112.6 (2)C15—O1—C4119.5 (2)
C14—C11—C10109.7 (3)C20—O3—H3109.5
C12—C11—C10109.1 (2)C22—C88A—H88A109.5
C11—C12—H12A109.5C22—C88A—H88B109.5
C11—C12—H12B109.5C22—C88A—H88C109.5
H12A—C12—H12B109.5C22—C99A—H99A109.5
C11—C12—H12C109.5C22—C99A—H99B109.5
H12A—C12—H12C109.5C22—C99A—H99C109.5
H12B—C12—H12C109.5C22—C44A—H44A109.5
C11—C13—H13A109.5C22—C44A—H44B109.5
C11—C13—H13B109.5C22—C44A—H44C109.5
H13A—C13—H13B109.5C22—C44B—H44D109.5
C11—C13—H13C109.5C22—C44B—H44E109.5
H13A—C13—H13C109.5H44D—C44B—H44E109.5
H13B—C13—H13C109.5C22—C44B—H44F109.5
C11—C14—H14A109.5H44D—C44B—H44F109.5
C11—C14—H14B109.5H44E—C44B—H44F109.5
H14A—C14—H14B109.5C22—C88B—H88D109.5
C11—C14—H14C109.5C22—C88B—H88E109.5
H14A—C14—H14C109.5H88D—C88B—H88E109.5
H14B—C14—H14C109.5C22—C88B—H88F109.5
O2—C15—O1123.5 (3)H88D—C88B—H88F109.5
O2—C15—C16127.3 (3)H88E—C88B—H88F109.5
O1—C15—C16109.1 (3)C22—C99B—H99D109.5
C17—C16—C15122.0 (5)C22—C99B—H99E109.5
C17—C16—H16119.0H99D—C99B—H99E109.5
C15—C16—H16119.0C22—C99B—H99F109.5
C16—C17—H17A120.0H99D—C99B—H99F109.5
C16—C17—H17B120.0H99E—C99B—H99F109.5
H17A—C17—H17B120.0
C6—C1—C2—C31.4 (4)C9—C10—C11—C12120.5 (3)
C22—C1—C2—C3176.0 (2)O2—C15—C16—C175.0 (6)
C1—C2—C3—C41.4 (4)O1—C15—C16—C17177.2 (4)
C1—C2—C3—C18176.7 (2)C4—C3—C18—C1962.2 (3)
C2—C3—C4—C51.1 (4)C2—C3—C18—C19115.7 (3)
C18—C3—C4—C5176.9 (2)C3—C18—C19—C21133.9 (3)
C2—C3—C4—O1175.4 (2)C3—C18—C19—C2048.3 (4)
C18—C3—C4—O12.6 (3)C21—C19—C20—O3177.1 (3)
C3—C4—C5—C60.8 (4)C18—C19—C20—O30.8 (4)
O1—C4—C5—C6174.9 (2)C21—C19—C20—C8i1.1 (4)
C3—C4—C5—C7177.7 (2)C18—C19—C20—C8i179.0 (3)
O1—C4—C5—C73.5 (4)C20—C19—C21—C10i0.7 (4)
C2—C1—C6—C51.1 (4)C18—C19—C21—C10i177.2 (3)
C22—C1—C6—C5176.3 (2)C6—C1—C22—C44A22.8 (5)
C4—C5—C6—C10.8 (4)C2—C1—C22—C44A159.9 (4)
C7—C5—C6—C1177.7 (2)C6—C1—C22—C99A99.3 (5)
C4—C5—C7—C852.3 (4)C2—C1—C22—C99A78.0 (5)
C6—C5—C7—C8126.1 (3)C6—C1—C22—C99B150.1 (12)
C5—C7—C8—C9125.0 (3)C2—C1—C22—C99B27.2 (12)
C5—C7—C8—C20i55.7 (4)C6—C1—C22—C88B85.7 (12)
C20i—C8—C9—C101.5 (4)C2—C1—C22—C88B97.0 (12)
C7—C8—C9—C10179.2 (3)C6—C1—C22—C88A142.0 (4)
C8—C9—C10—C21i0.2 (4)C2—C1—C22—C88A40.7 (4)
C8—C9—C10—C11178.7 (3)C6—C1—C22—C44B30.6 (10)
C21i—C10—C11—C13179.1 (3)C2—C1—C22—C44B146.7 (10)
C9—C10—C11—C130.3 (4)O2—C15—O1—C41.5 (5)
C21i—C10—C11—C1461.0 (4)C16—C15—O1—C4179.5 (3)
C9—C10—C11—C14120.1 (3)C5—C4—O1—C1583.6 (3)
C21i—C10—C11—C1258.4 (4)C3—C4—O1—C15101.9 (3)
Symmetry code: (i) x+1, y, z+1/2.

Experimental details

Crystal data
Chemical formulaC50H60O6
Mr756.98
Crystal system, space groupMonoclinic, C2/c
Temperature (K)297
a, b, c (Å)15.8896 (11), 26.482 (2), 10.3522 (7)
β (°) 95.047 (6)
V3)4339.2 (5)
Z4
Radiation typeMo Kα
µ (mm1)0.07
Crystal size (mm)0.41 × 0.24 × 0.09
Data collection
DiffractometerStoe IPDS2
Absorption correctionIntegration
(X-RED32; Stoe & Cie, 2002)
Tmin, Tmax0.940, 0.983
No. of measured, independent and
observed [I > 2σ(I)] reflections
28360, 4277, 1985
Rint0.131
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.058, 0.153, 0.89
No. of reflections4277
No. of parameters291
No. of restraints69
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.28, 0.25

Computer programs: X-AREA (Stoe & Cie, 2002), X-AREA, X-RED32 (Stoe & Cie, 2002), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 (Farrugia, 1997), WinGX (Farrugia, 1999).

 

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