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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2015 Oct 17;71(Pt 11):o867–o868. doi: 10.1107/S2056989015019040

Crystal and mol­ecular structure of aflatrem

Bruno N Lenta a,*, Jules Ngatchou b, Patrice T Kenfack c, Beate Neumann d, Hans-Georg Stammler d, Norbert Sewald d
PMCID: PMC4645010  PMID: 26594569

Abstract

The crystal structure of the title compound, C32H39NO4, confirms the absolute configuration of the seven chiral centres in the mol­ecule. The molecule has a 1,1-dimethylprop-2-enyl substituent on the indole nucleus and this nucleus shares one edge with the five-membered ring which is, in turn, connected to a sequence of three edge-shared fused rings. The skeleton is completed by the 7,7-trimethyl-6,8-dioxabi­cyclo­[3.2.1]oct-3-en-2-one group connected to the terminal cyclohexene ring. The two cyclohexane rings adopt chair and half-chair conformations, while in the dioxabi­cyclo­[3.2.1]oct-3-en-2-one unit, the six-membered ring has a half-chair conformation. The indole system of the mol­ecule exhibits a tilt of 2.02 (1)° between its two rings. In the crystal, O—H⋯O hydrogen bonds connect mol­ecules into chains along [010]. Weak N—H⋯π inter­actions connect these chains, forming sheets parallel to (10-1).

Keywords: crystal structure, aflatrem, indole-diterpenoid, fungal endophytes, Aspergillus species, N—H⋯Cg (indole), hydrogen bonding

Related literature  

For background to indole diterpenoids from endophytes, see: Strobel & Daisy (2003); Munday-Finch et al. (1996); Gallagher et al. (1980a ,b ); Lenta et al. (2007); Phongpaichit et al. (2007). For studies of Aspergillus sp, see: Nicholson et al. (2009); Duran et al. (2006). For the pharmacological basis of the behavioural effects of this mol­ecule, see: Tinao-Wooldridge et al. (1995). For the isolation of fungal endophytes from the stem of Symphonia globulifera, see: Petrini et al. (1992); Amin et al. (2014). For geometric details of indole compounds, see: Krishna et al. (1999). For circular dichroism experiments on the title compound, see: Sun et al. (2014). For information on the Cambridge Structural Database (CSD), see: Groom & Allen (2014).graphic file with name e-71-0o867-scheme1.jpg

Experimental  

Crystal data  

  • C32H39NO4

  • M r = 501.64

  • Monoclinic, Inline graphic

  • a = 12.8022 (5) Å

  • b = 6.4019 (2) Å

  • c = 15.9557 (6) Å

  • β = 98.821 (4)°

  • V = 1292.24 (9) Å3

  • Z = 2

  • Cu Kα radiation

  • μ = 0.66 mm−1

  • T = 100 K

  • 0.18 × 0.14 × 0.02 mm

Data collection  

  • Agilent SuperNova Dual Source diffractometer with an Atlas detector

  • Absorption correction: gaussian (CrysAlis PRO; Agilent, 2013) T min = 0.899, T max = 1.000

  • 19981 measured reflections

  • 4585 independent reflections

  • 4078 reflections with I > 2σ(I)

  • R int = 0.050

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.056

  • wR(F 2) = 0.150

  • S = 1.06

  • 4585 reflections

  • 341 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.35 e Å−3

  • Δρmin = −0.23 e Å−3

  • Absolute structure: Flack x determined using 1671 quotients [(I +)−(I )]/[(I +)+(I )] (Parsons & Flack, 2004)

  • Absolute structure parameter: 0.09 (14)

Data collection: CrysAlis PRO (Agilent, 2013); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S2056989015019040/lh5789sup1.cif

e-71-0o867-sup1.cif (28.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015019040/lh5789Isup2.hkl

e-71-0o867-Isup2.hkl (150.9KB, hkl)

. DOI: 10.1107/S2056989015019040/lh5789fig1.tif

The mol­ecular structure of aflatrem with the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level.

b x y z x y z x y z x y z . DOI: 10.1107/S2056989015019040/lh5789fig2.tif

Crystal packing of aflatrem showing O—H⋯O hydrogen-bonded (dashed lines) zigzag chains along the b axis in the (010) plane. Weak N—H⋯π inter­actions are also shown as dashed lines. Symmetry codes: (i) − x + 2, y − Inline graphic, −z + 2; (ii) −x + 1, y − Inline graphic, −z + 1; (iii) −x + 1, y + Inline graphic, −z + 1; (iv) −x + 2, y + Inline graphic, −z + 2.

b x y z x y z x y z x y z . DOI: 10.1107/S2056989015019040/lh5789fig3.tif

Crystal packing of aflatrem showing O—H⋯O hydrogen-bonded (dashed lines) zigzag chains along the b axis in the (001) plane. Weak N—H⋯π inter­actions are also shown as dashed lines. Symmetry codes: (i) −x + 2, y − Inline graphic, −z + 2; (ii) −x + 1, y − Inline graphic, −z + 1; (iii) −x + 1, y + Inline graphic, −z + 1 and (iv) −x + 2, y + Inline graphic, −z + 2.

CCDC reference: 1430332

Additional supporting information: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (, ).

Cg is the centroid of the C17C22 ring.

DHA DH HA D A DHA
O4H4O3i 0.82 2.03 2.757(3) 148
N1H1Cg ii 0.86 2.78 3.527(1) 146

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The authors wish to acknowledge the Alexander von Humboldt Foundation for providing a fellowship to B. N. Lenta at Bielefeld University

supplementary crystallographic information

S1. Comment

The search of compounds from plant endophytes has been the subject of research interest (Strobel & Daisy 2003). They produce a plethora of substances with potential applications in agriculture, medicine, pharmaceutical and for industry (Petrini et al. 1992; Strobel & Daisy, 2003; Phongpaichit et al., 2007). We are interested in the isolation and the structural study of compounds produced by endophytes from Cameroonian medicinal plants with pharmacological properties (Lenta et al., 2007) and one of the compounds that we have isolated from the fungal endophyte of the stem of Symphonia globulifera was aflatrem. Some authors have identified the biosynthetic genes of this molecule in Aspergilius sp (Nicholson et al., 2009; Duran et al., 2006). We report herein the study of its molecular and crystal structure.

Aflatrem crystallizes in the non-centrosymmetric space group P21 and its asymmetric unit consists of a single molecule as shown in Figure 1. As known in the literature, the molecule has a 1,l-dimethyl-2-propenyl substituent on the indole nucleus at position C18 and this nucleus shares one edge with the 5-membered ring (A) belonging to a group of three fused rings like an anthracene system (see Fig.1). The two others rings (6-membered, B and C) also share one edge with the 7, 7-trimethyl-6,8- dioxabicyclo[3.2.1]oct-3-en-2-one group. All the bond distances observed in the compounds are in agreement with the bonds distance of the Cambridge Structural Database (CSD, Groom & Allen, 2014). In the indole ring system, a small tilt of 2.02 (1)° is observed between the 6 and 5-membered rings. This value as well as the values of the bond angles is near the values always obtained in the indole based compounds (Krishna et al., 1999). The ring A (C1/C16/C15/C14/C2) adopts a dihedral angle of 3.12 (1)° with the 5-membered ring of indole system. With the exception of the C1–C2–C14 angle (96.9 (1)°),the values of the bond angles in this ring are in the range between 100 and 112° and they are in good agreement with the ideal conformation for which the angle is 107°. The lower value observed could be favored by the chair conformation of the B ring which shares one edge (C2 and C14) with ring A. This conformation is close to the ideal chair conformation since the bond angles range from 107 to 113° compared to an ideal value of 109°. The ring C assumes a half-chair conformation. The bicyclo[3.2.1]oct-3-en-2-one system is composed by a 6-membered ring named D (C6/C10/C9/C8/C7/O1) sharing one edge (C6 –C7) with a 5-membered ring called E (O1/C7/C6/O2/C25). The carbon atoms of ring D lie in the same plane and the O1 atom is located at 0.80 (1) Å from this plane. This atom is also located at 0.656 (1) Å from the plane which contains the carbon atoms of ring E and the dihedral angle between the two planes is 69.07 (1)°. The methyl and hydroxyl groups linked to the fused ring give the absolute configuration of 1S,3R,6S,7S,11R,12S,13S determined by Cu KαX-radiation with the Flack parameter being refined to 0.09 (14) and this configuration is in agreement with the previous circular dichroism assignment reported by Sun et al. (2014).

The crystal packing of the aflatrem molecules is illustrated in Figs. 2 and 3. In the crystal, molecules are connected along the b axis via O—H···O hydrogen bonds. In addition, weak N—H···π(indole) interactions connect these chains forming planes parallel to (10-1). This N—H···π(indole) interaction is typical of indole-based molecules as reported by Krishna et al. (1999).

S2. Experimental

The isolation of fungal endophytes from the stem of Symphonia globulifera was carried out aat the University of Yaoundé 1 (Cameroon) and was based on the method described by Petrini et al. (1992). One of the fungi was identified to Aspergillus sp. according to the method described by Amin et al. (2014) and cultured in solid medium prepared from 1 kg of rice distributed in the glass flask (total capacity of 2.5 L) at a rate of 200 g of rice in 200 ml of distilled water. After one month of incubation at 301K in the same laboratory, the culture medium was extracted with EtOAc and the extract concentrated on a rotary evaporator under vacuum at a temperature of 313K to yield 20.1 g of extract. This extract was subjected to column chromatography (CC) over silica gel (0.023–0.20 mesh, Merck) and eluted with a gradient system of petroleum ether /ethyl acetate to afford aflatrem (7.5 mg). The colourless crystals obtained were sent to the Laboratory of Inorganic and Structural Chemistry at Bielefeld University (Germany) for X-ray diffraction measurements.

S3. Refinement

H atoms were placed in calculated positions with C–H = 0.93-0.98Å, N—H = 0.86Å and O—H = 0.82Å. They were included in calculated positions with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(Cmethyl,O).

Figures

Fig. 1.

Fig. 1.

The molecular structure of aflatrem with the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Crystal packing of aflatrem showing O—H···O hydrogen-bonded (dashed lines) zigzag chains along the b axis in the (010) plane . Weak N—H···π interactions are also shown as dashed lines. Symmetry codes: (i) - x+ 2, y - 1/2, -z + 2; (ii) -x + 1, y - 1/2, -z + 1; (iii) -x + 1, y + 1/2, -z + 1; (iv) -x + 2, y + 1/2, -z + 2.

Fig. 3.

Fig. 3.

Crystal packing of aflatrem showing O—H···O hydrogen-bonded (dashed lines) zigzag chains along the b axis in the (001) plane. Weak N—H···π interactions are also shown as dashed lines. Symmetry codes: (i) -x + 2, y - 1/2, -z +2; (ii) -x + 1, y - 1/2, -z + 1; (iii) -x + 1, y + 1/2, -z + 1 and (iv) -x + 2, y + 1/2, -z + 2.

Crystal data

C32H39NO4 F(000) = 540
Mr = 501.64 Dx = 1.289 Mg m3
Monoclinic, P21 Cu Kα radiation, λ = 1.5418 Å
a = 12.8022 (5) Å Cell parameters from 6775 reflections
b = 6.4019 (2) Å θ = 4.8–66.4°
c = 15.9557 (6) Å µ = 0.66 mm1
β = 98.821 (4)° T = 100 K
V = 1292.24 (9) Å3 Plate, colourless
Z = 2 0.18 × 0.14 × 0.02 mm

Data collection

Agilent SuperNova Dual Source diffractometer with an Atlas detector 4585 independent reflections
Radiation source: SuperNova (Cu) X-ray Source 4078 reflections with I > 2σ(I)
Mirror monochromator Rint = 0.050
Detector resolution: 5.3114 pixels mm-1 θmax = 66.9°, θmin = 2.8°
ω scans h = −15→15
Absorption correction: gaussian (CrysAlis PRO; Agilent, 2013) k = −7→7
Tmin = 0.899, Tmax = 1.000 l = −18→18
19981 measured reflections

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.056 w = 1/[σ2(Fo2) + (0.0948P)2 + 0.4383P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.150 (Δ/σ)max < 0.001
S = 1.06 Δρmax = 0.35 e Å3
4585 reflections Δρmin = −0.23 e Å3
341 parameters Absolute structure: Flack x determined using 1671 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons & Flack, 2004)
1 restraint Absolute structure parameter: 0.09 (14)
Primary atom site location: structure-invariant direct methods

Special details

Experimental. Numerical absorption correction based on gaussian integration over a multifaceted crystal model
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)

x y z Uiso*/Ueq
O1 0.77480 (17) 0.1640 (3) 1.04104 (13) 0.0330 (5)
O2 0.64687 (16) 0.3772 (3) 0.97693 (13) 0.0307 (5)
O3 0.88440 (18) 0.5994 (4) 1.15707 (14) 0.0414 (6)
O4 0.91050 (17) 0.2056 (3) 0.85758 (13) 0.0316 (5)
H4 0.9698 0.2203 0.8449 0.047*
N1 0.61755 (19) 0.3716 (4) 0.58123 (15) 0.0267 (5)
H1 0.5782 0.2885 0.6050 0.032*
C1 0.7110 (2) 0.4610 (4) 0.61906 (19) 0.0260 (6)
C2 0.7906 (2) 0.4099 (4) 0.69719 (18) 0.0252 (6)
C3 0.7579 (2) 0.4000 (5) 0.78767 (18) 0.0264 (6)
C4 0.6942 (2) 0.1981 (4) 0.80235 (19) 0.0279 (6)
H4A 0.6195 0.2288 0.7870 0.033*
H4B 0.7117 0.0912 0.7637 0.033*
C5 0.7119 (2) 0.1065 (5) 0.89279 (19) 0.0301 (6)
H5A 0.6482 0.0338 0.9021 0.036*
H5B 0.7684 0.0044 0.8968 0.036*
C6 0.7394 (2) 0.2648 (5) 0.96202 (19) 0.0293 (7)
C7 0.7658 (3) 0.3273 (5) 1.10039 (19) 0.0327 (7)
H7 0.7714 0.2729 1.1583 0.039*
C8 0.8486 (2) 0.4967 (5) 1.0940 (2) 0.0338 (7)
C9 0.8771 (2) 0.5268 (5) 1.0107 (2) 0.0328 (7)
H9 0.9297 0.6218 1.0028 0.039*
C10 0.8270 (2) 0.4165 (5) 0.94420 (19) 0.0287 (6)
C11 0.8592 (2) 0.4071 (5) 0.85721 (18) 0.0270 (6)
C12 0.9380 (2) 0.5804 (5) 0.8432 (2) 0.0316 (7)
H12A 0.9080 0.7144 0.8551 0.038*
H12B 1.0022 0.5614 0.8834 0.038*
C13 0.9661 (2) 0.5851 (5) 0.75408 (19) 0.0326 (7)
H13A 1.0117 0.7032 0.7477 0.039*
H13B 1.0029 0.4580 0.7430 0.039*
C14 0.8634 (2) 0.6041 (5) 0.69266 (19) 0.0277 (6)
H14 0.8256 0.7216 0.7135 0.033*
C15 0.8636 (2) 0.6488 (5) 0.59791 (19) 0.0313 (7)
H15A 0.8759 0.7955 0.5876 0.038*
H15B 0.9157 0.5649 0.5751 0.038*
C16 0.7522 (2) 0.5841 (4) 0.56234 (19) 0.0276 (6)
C17 0.6812 (2) 0.5766 (4) 0.48313 (18) 0.0262 (6)
C18 0.6770 (2) 0.6725 (4) 0.40181 (18) 0.0267 (6)
C19 0.5951 (2) 0.6126 (5) 0.33970 (19) 0.0310 (7)
H19 0.5918 0.6687 0.2856 0.037*
C20 0.5165 (2) 0.4704 (5) 0.35503 (19) 0.0308 (7)
H20 0.4644 0.4318 0.3105 0.037*
C21 0.5147 (2) 0.3863 (5) 0.43453 (19) 0.0279 (6)
H21 0.4605 0.2986 0.4455 0.033*
C22 0.5987 (2) 0.4402 (4) 0.49762 (18) 0.0262 (6)
C23 0.8453 (3) 0.2072 (5) 0.6718 (2) 0.0308 (7)
H23A 0.7937 0.0983 0.6598 0.046*
H23B 0.8987 0.1648 0.7176 0.046*
H23C 0.8774 0.2338 0.6223 0.046*
C24 0.6862 (2) 0.5888 (4) 0.80049 (19) 0.0281 (6)
H24A 0.7270 0.7150 0.8035 0.042*
H24B 0.6576 0.5712 0.8523 0.042*
H24C 0.6294 0.5971 0.7537 0.042*
C25 0.6530 (2) 0.4108 (6) 1.06813 (19) 0.0336 (7)
C26 0.6353 (3) 0.6379 (5) 1.0847 (2) 0.0384 (8)
H26A 0.6817 0.7211 1.0565 0.058*
H26B 0.6497 0.6639 1.1447 0.058*
H26C 0.5633 0.6738 1.0637 0.058*
C27 0.5722 (3) 0.2731 (6) 1.1015 (2) 0.0376 (8)
H27A 0.5028 0.3075 1.0731 0.056*
H27B 0.5757 0.2954 1.1614 0.056*
H27C 0.5872 0.1292 1.0912 0.056*
C28 0.7593 (2) 0.8372 (4) 0.38782 (18) 0.0295 (7)
C29 0.7411 (3) 0.9297 (5) 0.2981 (2) 0.0381 (8)
H29A 0.7483 0.8217 0.2576 0.057*
H29B 0.7924 1.0372 0.2940 0.057*
H29C 0.6714 0.9881 0.2866 0.057*
C30 0.7512 (3) 1.0194 (5) 0.4492 (2) 0.0351 (7)
H30A 0.6870 1.0954 0.4313 0.053*
H30B 0.8106 1.1109 0.4494 0.053*
H30C 0.7508 0.9657 0.5054 0.053*
C31 0.8695 (3) 0.7438 (5) 0.4004 (2) 0.0340 (7)
H31 0.9255 0.8328 0.4195 0.041*
C32 0.8925 (3) 0.5482 (6) 0.3866 (2) 0.0426 (8)
H32A 0.8388 0.4540 0.3675 0.051*
H32B 0.9625 0.5039 0.3960 0.051*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0397 (12) 0.0260 (10) 0.0297 (11) 0.0012 (9) −0.0062 (9) 0.0028 (9)
O2 0.0311 (10) 0.0307 (11) 0.0269 (10) −0.0007 (9) −0.0065 (8) −0.0031 (9)
O3 0.0390 (12) 0.0489 (14) 0.0317 (12) −0.0085 (11) −0.0090 (10) −0.0092 (11)
O4 0.0329 (11) 0.0272 (11) 0.0327 (11) 0.0059 (9) −0.0019 (9) 0.0019 (9)
N1 0.0308 (12) 0.0218 (12) 0.0254 (12) −0.0015 (10) −0.0027 (10) 0.0024 (10)
C1 0.0273 (14) 0.0188 (13) 0.0298 (15) 0.0013 (11) −0.0018 (12) −0.0022 (11)
C2 0.0296 (14) 0.0163 (12) 0.0270 (14) 0.0012 (12) −0.0037 (11) −0.0015 (11)
C3 0.0304 (14) 0.0177 (13) 0.0276 (15) 0.0005 (12) −0.0062 (12) −0.0004 (11)
C4 0.0310 (15) 0.0198 (14) 0.0303 (14) −0.0030 (12) −0.0031 (12) −0.0014 (11)
C5 0.0368 (16) 0.0186 (13) 0.0330 (16) −0.0041 (12) −0.0006 (13) −0.0036 (12)
C6 0.0351 (16) 0.0229 (15) 0.0268 (15) 0.0005 (12) −0.0055 (12) −0.0014 (11)
C7 0.0348 (16) 0.0349 (16) 0.0250 (15) −0.0017 (13) −0.0065 (12) 0.0008 (13)
C8 0.0299 (15) 0.0364 (17) 0.0325 (16) 0.0013 (13) −0.0034 (13) −0.0014 (13)
C9 0.0330 (15) 0.0330 (16) 0.0296 (15) −0.0062 (13) −0.0044 (12) −0.0008 (13)
C10 0.0307 (14) 0.0212 (14) 0.0314 (15) 0.0026 (12) −0.0038 (12) 0.0015 (12)
C11 0.0281 (14) 0.0216 (13) 0.0286 (15) 0.0006 (12) −0.0044 (12) −0.0014 (12)
C12 0.0316 (15) 0.0278 (15) 0.0325 (16) −0.0030 (13) −0.0047 (12) −0.0014 (13)
C13 0.0306 (15) 0.0311 (15) 0.0330 (16) −0.0027 (13) −0.0055 (13) −0.0035 (13)
C14 0.0285 (14) 0.0231 (14) 0.0290 (15) −0.0015 (12) −0.0037 (12) 0.0008 (12)
C15 0.0386 (17) 0.0234 (14) 0.0283 (15) −0.0022 (12) −0.0056 (13) 0.0026 (12)
C16 0.0322 (14) 0.0193 (13) 0.0292 (15) 0.0002 (12) −0.0021 (12) −0.0022 (12)
C17 0.0307 (14) 0.0206 (13) 0.0260 (14) 0.0018 (12) −0.0001 (12) −0.0008 (11)
C18 0.0329 (15) 0.0207 (13) 0.0247 (14) −0.0001 (12) −0.0007 (11) 0.0007 (11)
C19 0.0353 (15) 0.0265 (15) 0.0287 (15) 0.0036 (13) −0.0034 (13) 0.0026 (12)
C20 0.0329 (15) 0.0247 (14) 0.0300 (15) 0.0019 (12) −0.0099 (13) −0.0009 (12)
C21 0.0293 (14) 0.0200 (13) 0.0318 (15) −0.0002 (12) −0.0032 (12) 0.0019 (12)
C22 0.0327 (15) 0.0190 (14) 0.0254 (14) 0.0028 (11) −0.0006 (12) −0.0004 (11)
C23 0.0365 (16) 0.0212 (15) 0.0326 (15) 0.0024 (12) −0.0016 (13) −0.0028 (12)
C24 0.0362 (16) 0.0183 (13) 0.0280 (14) 0.0027 (12) −0.0013 (12) −0.0020 (11)
C25 0.0339 (16) 0.0382 (17) 0.0255 (15) −0.0009 (14) −0.0059 (12) −0.0034 (13)
C26 0.0408 (17) 0.0387 (18) 0.0317 (16) 0.0011 (14) −0.0074 (13) −0.0077 (14)
C27 0.0336 (17) 0.0419 (19) 0.0354 (17) −0.0041 (14) −0.0010 (14) −0.0025 (14)
C28 0.0384 (16) 0.0222 (15) 0.0262 (15) −0.0027 (12) −0.0007 (12) 0.0031 (12)
C29 0.0478 (19) 0.0319 (17) 0.0310 (16) −0.0070 (14) −0.0054 (14) 0.0056 (13)
C30 0.0453 (18) 0.0211 (15) 0.0359 (17) −0.0015 (13) −0.0034 (14) 0.0009 (13)
C31 0.0332 (16) 0.0319 (16) 0.0349 (16) −0.0061 (13) −0.0013 (13) 0.0006 (13)
C32 0.0397 (18) 0.0356 (18) 0.052 (2) 0.0042 (15) 0.0068 (16) 0.0025 (15)

Geometric parameters (Å, º)

O1—C7 1.427 (4) C15—C16 1.509 (4)
O1—C6 1.427 (4) C15—H15A 0.9700
O2—C6 1.437 (4) C15—H15B 0.9700
O2—C25 1.461 (4) C16—C17 1.440 (4)
O3—C8 1.231 (4) C17—C22 1.417 (4)
O4—C11 1.447 (4) C17—C18 1.429 (4)
O4—H4 0.8200 C18—C19 1.382 (4)
N1—C1 1.379 (4) C18—C28 1.532 (4)
N1—C22 1.390 (4) C19—C20 1.406 (5)
N1—H1 0.8600 C19—H19 0.9300
C1—C16 1.366 (4) C20—C21 1.381 (4)
C1—C2 1.520 (4) C20—H20 0.9300
C2—C23 1.557 (4) C21—C22 1.399 (4)
C2—C14 1.562 (4) C21—H21 0.9300
C2—C3 1.565 (4) C23—H23A 0.9600
C3—C24 1.550 (4) C23—H23B 0.9600
C3—C4 1.565 (4) C23—H23C 0.9600
C3—C11 1.573 (4) C24—H24A 0.9600
C4—C5 1.542 (4) C24—H24B 0.9600
C4—H4A 0.9700 C24—H24C 0.9600
C4—H4B 0.9700 C25—C26 1.501 (5)
C5—C6 1.500 (4) C25—C27 1.517 (5)
C5—H5A 0.9700 C26—H26A 0.9600
C5—H5B 0.9700 C26—H26B 0.9600
C6—C10 1.543 (4) C26—H26C 0.9600
C7—C8 1.531 (5) C27—H27A 0.9600
C7—C25 1.552 (4) C27—H27B 0.9600
C7—H7 0.9800 C27—H27C 0.9600
C8—C9 1.443 (5) C28—C31 1.516 (4)
C9—C10 1.351 (4) C28—C29 1.533 (4)
C9—H9 0.9300 C28—C30 1.537 (4)
C10—C11 1.508 (4) C29—H29A 0.9600
C11—C12 1.538 (4) C29—H29B 0.9600
C12—C13 1.521 (4) C29—H29C 0.9600
C12—H12A 0.9700 C30—H30A 0.9600
C12—H12B 0.9700 C30—H30B 0.9600
C13—C14 1.520 (4) C30—H30C 0.9600
C13—H13A 0.9700 C31—C32 1.313 (5)
C13—H13B 0.9700 C31—H31 0.9300
C14—C15 1.539 (4) C32—H32A 0.9300
C14—H14 0.9800 C32—H32B 0.9300
C7—O1—C6 102.0 (2) C14—C15—H15A 111.8
C6—O2—C25 108.6 (2) C16—C15—H15B 111.8
C11—O4—H4 109.5 C14—C15—H15B 111.8
C1—N1—C22 107.5 (2) H15A—C15—H15B 109.5
C1—N1—H1 126.3 C1—C16—C17 107.9 (3)
C22—N1—H1 126.3 C1—C16—C15 110.4 (3)
C16—C1—N1 110.3 (2) C17—C16—C15 140.5 (3)
C16—C1—C2 112.9 (2) C22—C17—C18 119.1 (3)
N1—C1—C2 134.2 (3) C22—C17—C16 105.3 (2)
C1—C2—C23 103.7 (2) C18—C17—C16 135.6 (3)
C1—C2—C14 96.9 (2) C19—C18—C17 116.8 (3)
C23—C2—C14 110.8 (2) C19—C18—C28 123.4 (3)
C1—C2—C3 121.6 (2) C17—C18—C28 119.8 (2)
C23—C2—C3 113.7 (2) C18—C19—C20 122.6 (3)
C14—C2—C3 108.7 (2) C18—C19—H19 118.7
C24—C3—C2 109.7 (2) C20—C19—H19 118.7
C24—C3—C4 106.9 (2) C21—C20—C19 121.7 (3)
C2—C3—C4 113.0 (2) C21—C20—H20 119.2
C24—C3—C11 109.0 (2) C19—C20—H20 119.2
C2—C3—C11 109.9 (2) C20—C21—C22 116.5 (3)
C4—C3—C11 108.1 (2) C20—C21—H21 121.8
C5—C4—C3 116.7 (2) C22—C21—H21 121.8
C5—C4—H4A 108.1 N1—C22—C21 127.9 (3)
C3—C4—H4A 108.1 N1—C22—C17 109.1 (2)
C5—C4—H4B 108.1 C21—C22—C17 123.0 (3)
C3—C4—H4B 108.1 C2—C23—H23A 109.5
H4A—C4—H4B 107.3 C2—C23—H23B 109.5
C6—C5—C4 114.6 (2) H23A—C23—H23B 109.5
C6—C5—H5A 108.6 C2—C23—H23C 109.5
C4—C5—H5A 108.6 H23A—C23—H23C 109.5
C6—C5—H5B 108.6 H23B—C23—H23C 109.5
C4—C5—H5B 108.6 C3—C24—H24A 109.5
H5A—C5—H5B 107.6 C3—C24—H24B 109.5
O1—C6—O2 103.8 (2) H24A—C24—H24B 109.5
O1—C6—C5 110.6 (2) C3—C24—H24C 109.5
O2—C6—C5 110.7 (2) H24A—C24—H24C 109.5
O1—C6—C10 107.8 (2) H24B—C24—H24C 109.5
O2—C6—C10 110.9 (2) O2—C25—C26 109.4 (3)
C5—C6—C10 112.6 (3) O2—C25—C27 109.2 (3)
O1—C7—C8 110.3 (3) C26—C25—C27 111.8 (3)
O1—C7—C25 101.4 (2) O2—C25—C7 100.7 (2)
C8—C7—C25 110.6 (3) C26—C25—C7 115.7 (3)
O1—C7—H7 111.4 C27—C25—C7 109.5 (3)
C8—C7—H7 111.4 C25—C26—H26A 109.5
C25—C7—H7 111.4 C25—C26—H26B 109.5
O3—C8—C9 124.6 (3) H26A—C26—H26B 109.5
O3—C8—C7 119.9 (3) C25—C26—H26C 109.5
C9—C8—C7 115.5 (3) H26A—C26—H26C 109.5
C10—C9—C8 119.8 (3) H26B—C26—H26C 109.5
C10—C9—H9 120.1 C25—C27—H27A 109.5
C8—C9—H9 120.1 C25—C27—H27B 109.5
C9—C10—C11 125.4 (3) H27A—C27—H27B 109.5
C9—C10—C6 117.1 (3) C25—C27—H27C 109.5
C11—C10—C6 116.9 (3) H27A—C27—H27C 109.5
O4—C11—C10 102.7 (2) H27B—C27—H27C 109.5
O4—C11—C12 109.6 (2) C31—C28—C18 110.9 (2)
C10—C11—C12 112.5 (2) C31—C28—C29 106.3 (3)
O4—C11—C3 107.6 (2) C18—C28—C29 113.1 (3)
C10—C11—C3 109.8 (2) C31—C28—C30 111.6 (3)
C12—C11—C3 114.0 (2) C18—C28—C30 108.3 (2)
C13—C12—C11 113.9 (2) C29—C28—C30 106.7 (3)
C13—C12—H12A 108.8 C28—C29—H29A 109.5
C11—C12—H12A 108.8 C28—C29—H29B 109.5
C13—C12—H12B 108.8 H29A—C29—H29B 109.5
C11—C12—H12B 108.8 C28—C29—H29C 109.5
H12A—C12—H12B 107.7 H29A—C29—H29C 109.5
C14—C13—C12 107.4 (2) H29B—C29—H29C 109.5
C14—C13—H13A 110.2 C28—C30—H30A 109.5
C12—C13—H13A 110.2 C28—C30—H30B 109.5
C14—C13—H13B 110.2 H30A—C30—H30B 109.5
C12—C13—H13B 110.2 C28—C30—H30C 109.5
H13A—C13—H13B 108.5 H30A—C30—H30C 109.5
C13—C14—C15 121.1 (3) H30B—C30—H30C 109.5
C13—C14—C2 111.7 (2) C32—C31—C28 125.6 (3)
C15—C14—C2 106.5 (2) C32—C31—H31 117.2
C13—C14—H14 105.4 C28—C31—H31 117.2
C15—C14—H14 105.4 C31—C32—H32A 120.0
C2—C14—H14 105.4 C31—C32—H32B 120.0
C16—C15—C14 100.1 (2) H32A—C32—H32B 120.0
C16—C15—H15A 111.8
C22—N1—C1—C16 0.0 (3) C4—C3—C11—C12 171.7 (2)
C22—N1—C1—C2 −159.8 (3) O4—C11—C12—C13 70.5 (3)
C16—C1—C2—C23 −88.8 (3) C10—C11—C12—C13 −175.9 (2)
N1—C1—C2—C23 70.7 (4) C3—C11—C12—C13 −50.1 (3)
C16—C1—C2—C14 24.7 (3) C11—C12—C13—C14 55.7 (3)
N1—C1—C2—C14 −175.9 (3) C12—C13—C14—C15 170.0 (3)
C16—C1—C2—C3 141.7 (3) C12—C13—C14—C2 −63.3 (3)
N1—C1—C2—C3 −58.8 (4) C1—C2—C14—C13 −169.4 (2)
C1—C2—C3—C24 −44.3 (3) C23—C2—C14—C13 −61.8 (3)
C23—C2—C3—C24 −169.4 (2) C3—C2—C14—C13 63.8 (3)
C14—C2—C3—C24 66.6 (3) C1—C2—C14—C15 −35.2 (3)
C1—C2—C3—C4 74.9 (3) C23—C2—C14—C15 72.4 (3)
C23—C2—C3—C4 −50.1 (3) C3—C2—C14—C15 −162.0 (2)
C14—C2—C3—C4 −174.1 (2) C13—C14—C15—C16 162.6 (3)
C1—C2—C3—C11 −164.2 (2) C2—C14—C15—C16 33.6 (3)
C23—C2—C3—C11 70.7 (3) N1—C1—C16—C17 0.6 (3)
C14—C2—C3—C11 −53.2 (3) C2—C1—C16—C17 165.0 (2)
C24—C3—C4—C5 −93.2 (3) N1—C1—C16—C15 −169.2 (2)
C2—C3—C4—C5 145.9 (3) C2—C1—C16—C15 −4.8 (3)
C11—C3—C4—C5 24.0 (3) C14—C15—C16—C1 −18.0 (3)
C3—C4—C5—C6 30.1 (4) C14—C15—C16—C17 177.3 (4)
C7—O1—C6—O2 −44.4 (3) C1—C16—C17—C22 −0.9 (3)
C7—O1—C6—C5 −163.2 (3) C15—C16—C17—C22 164.0 (4)
C7—O1—C6—C10 73.3 (3) C1—C16—C17—C18 177.8 (3)
C25—O2—C6—O1 22.5 (3) C15—C16—C17—C18 −17.3 (6)
C25—O2—C6—C5 141.2 (2) C22—C17—C18—C19 −4.7 (4)
C25—O2—C6—C10 −93.0 (3) C16—C17—C18—C19 176.7 (3)
C4—C5—C6—O1 −168.4 (2) C22—C17—C18—C28 173.7 (3)
C4—C5—C6—O2 77.1 (3) C16—C17—C18—C28 −4.8 (5)
C4—C5—C6—C10 −47.7 (3) C17—C18—C19—C20 2.3 (4)
C6—O1—C7—C8 −69.4 (3) C28—C18—C19—C20 −176.1 (3)
C6—O1—C7—C25 47.9 (3) C18—C19—C20—C21 2.1 (5)
O1—C7—C8—O3 −149.9 (3) C19—C20—C21—C22 −3.8 (4)
C25—C7—C8—O3 98.7 (3) C1—N1—C22—C21 178.2 (3)
O1—C7—C8—C9 31.6 (4) C1—N1—C22—C17 −0.6 (3)
C25—C7—C8—C9 −79.8 (3) C20—C21—C22—N1 −177.4 (3)
O3—C8—C9—C10 −174.8 (3) C20—C21—C22—C17 1.2 (4)
C7—C8—C9—C10 3.5 (4) C18—C17—C22—N1 −178.0 (3)
C8—C9—C10—C11 −170.2 (3) C16—C17—C22—N1 0.9 (3)
C8—C9—C10—C6 1.0 (4) C18—C17—C22—C21 3.1 (4)
O1—C6—C10—C9 −40.5 (4) C16—C17—C22—C21 −178.0 (3)
O2—C6—C10—C9 72.5 (3) C6—O2—C25—C26 128.7 (3)
C5—C6—C10—C9 −162.8 (3) C6—O2—C25—C27 −108.7 (3)
O1—C6—C10—C11 131.5 (3) C6—O2—C25—C7 6.5 (3)
O2—C6—C10—C11 −115.5 (3) O1—C7—C25—O2 −33.0 (3)
C5—C6—C10—C11 9.2 (4) C8—C7—C25—O2 84.1 (3)
C9—C10—C11—O4 102.7 (3) O1—C7—C25—C26 −150.7 (3)
C6—C10—C11—O4 −68.5 (3) C8—C7—C25—C26 −33.7 (4)
C9—C10—C11—C12 −15.1 (4) O1—C7—C25—C27 81.9 (3)
C6—C10—C11—C12 173.7 (2) C8—C7—C25—C27 −161.0 (3)
C9—C10—C11—C3 −143.1 (3) C19—C18—C28—C31 −118.9 (3)
C6—C10—C11—C3 45.7 (3) C17—C18—C28—C31 62.7 (3)
C24—C3—C11—O4 165.8 (2) C19—C18—C28—C29 0.4 (4)
C2—C3—C11—O4 −73.9 (3) C17—C18—C28—C29 −178.0 (3)
C4—C3—C11—O4 49.9 (3) C19—C18—C28—C30 118.4 (3)
C24—C3—C11—C10 54.8 (3) C17—C18—C28—C30 −60.0 (3)
C2—C3—C11—C10 175.1 (2) C18—C28—C31—C32 29.3 (4)
C4—C3—C11—C10 −61.1 (3) C29—C28—C31—C32 −94.0 (4)
C24—C3—C11—C12 −72.4 (3) C30—C28—C31—C32 150.1 (3)
C2—C3—C11—C12 47.9 (3)

Hydrogen-bond geometry (Å, º)

Cg is the centroid of the C17–C22 ring.

D—H···A D—H H···A D···A D—H···A
O4—H4···O3i 0.82 2.03 2.757 (3) 148
N1—H1···Cgii 0.86 2.78 3.527 (1) 146

Symmetry codes: (i) −x+2, y−1/2, −z+2; (ii) −x+1, y−1/2, −z+1.

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: LH5789).

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S2056989015019040/lh5789sup1.cif

e-71-0o867-sup1.cif (28.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015019040/lh5789Isup2.hkl

e-71-0o867-Isup2.hkl (150.9KB, hkl)

. DOI: 10.1107/S2056989015019040/lh5789fig1.tif

The mol­ecular structure of aflatrem with the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level.

b x y z x y z x y z x y z . DOI: 10.1107/S2056989015019040/lh5789fig2.tif

Crystal packing of aflatrem showing O—H⋯O hydrogen-bonded (dashed lines) zigzag chains along the b axis in the (010) plane. Weak N—H⋯π inter­actions are also shown as dashed lines. Symmetry codes: (i) − x + 2, y − Inline graphic, −z + 2; (ii) −x + 1, y − Inline graphic, −z + 1; (iii) −x + 1, y + Inline graphic, −z + 1; (iv) −x + 2, y + Inline graphic, −z + 2.

b x y z x y z x y z x y z . DOI: 10.1107/S2056989015019040/lh5789fig3.tif

Crystal packing of aflatrem showing O—H⋯O hydrogen-bonded (dashed lines) zigzag chains along the b axis in the (001) plane. Weak N—H⋯π inter­actions are also shown as dashed lines. Symmetry codes: (i) −x + 2, y − Inline graphic, −z + 2; (ii) −x + 1, y − Inline graphic, −z + 1; (iii) −x + 1, y + Inline graphic, −z + 1 and (iv) −x + 2, y + Inline graphic, −z + 2.

CCDC reference: 1430332

Additional supporting information: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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