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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jun 7;64(Pt 7):o1240–o1241. doi: 10.1107/S1600536808015857

rac-(1S,2R)-Diethyl 6-hydr­oxy-1-(4-methoxy­phen­yl)-3-oxo-2,3-di­hydro-1H-benzo[f]chromen-2-yl]­phospho­nate

Jakub Wojciechowski a, Henryk Krawczyk b, Łukasz Albrecht b, Wojciech M Wolf a,*
PMCID: PMC2961657  PMID: 21202876

Abstract

In the title compound, C24H25O7P, the δ-valerolactonyl ring exists in a distorted screw-boat conformation with the diethoxy­phosphoryl substituent occupying an axial position. The latter adopts an almost syn-periplanar conformation around the P—C bond. The mol­ecules form centrosymmetric dimers connected by O—H⋯O hydrogen bonds.

Related literature

For the biological activity of 4-aryl-3,4-dihydro­coumarins, see: Bailly et al. (2003); Roelens et al. (2005); Zhang et al. (2006). For their synthesis, see: Aoki et al. (2005); Krawczyk et al. (2007a ); Li et al. (2005); Rizzi et al. (2006). For a comparison structure, see: Krawczyk et al. (2007b ).

For the atomic charges fitted to electrostatic potential, see: Frisch et al. (2004); Breneman & Wiberg (1990). For repulsive interactions between O atoms, see: Gillespie & Popelier, (2001). For hydrogen-bond graph-set terminology, see: Bernstein et al. (1995); Etter (1990). For ring puckering analysis, see: Boeyens (1978); Cremer & Pople (1975); Frisch et al. (2004). For details of the Cambridge Structural Database, see: Allen (2002).graphic file with name e-64-o1240-scheme1.jpg

Experimental

Crystal data

  • C24H25O7P

  • M r = 456.41

  • Monoclinic, Inline graphic

  • a = 21.6231 (17) Å

  • b = 10.0018 (8) Å

  • c = 22.4011 (17) Å

  • β = 111.806 (1)°

  • V = 4498.0 (6) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.17 mm−1

  • T = 293 (2) K

  • 0.30 × 0.20 × 0.15 mm

Data collection

  • Bruker SMART APEX diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2003) T min = 0.951, T max = 0.976

  • 37601 measured reflections

  • 5076 independent reflections

  • 3585 reflections with I > 2σ(I)

  • R int = 0.043

Refinement

  • R[F 2 > 2σ(F 2)] = 0.045

  • wR(F 2) = 0.137

  • S = 1.05

  • 5076 reflections

  • 310 parameters

  • H-atom parameters constrained

  • Δρmax = 0.30 e Å−3

  • Δρmin = −0.36 e Å−3

Data collection: SMART (Bruker, 2003); cell refinement: SAINT-Plus (Bruker, 2003); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL and publCIF (Westrip, 2008).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808015857/ng2458sup1.cif

e-64-o1240-sup1.cif (23.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808015857/ng2458Isup2.hkl

e-64-o1240-Isup2.hkl (308.1KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O6—H6⋯O4i 0.83 1.87 2.701 (2) 178

Symmetry code: (i) Inline graphic.

Acknowledgments

Atomic charges were calculated in the ACK CYFRONET, Kraków, Poland; support through computational grants 055/1999 and 056/1999 is gratefully acknowledged.

supplementary crystallographic information

Comment

The 4-aryl-3,4-dihydrocoumarin (neoflavonoid) moiety is found in several natural compounds which show a wide range of biological activities. Among them, the anti-inflammatory, anti-oxidative and anti-aging properties are best recognized (Zhang et al., 2006). A number of neoflavonoids isolated from various plant sources revealed cytotoxic and chemopreventive activity against cancer (Bailly et al., 2003). Morever, some 4-aryl-3,4-dihydrocoumarin derivatives exhibit estrogenic activity (Roelens et al., 2005). The most common method for the synthesis of 4-aryl-3,4-dihydrocoumarins involves Michael type addition of electron-rich hydroxyarenes to cinnamic acids or their derivatives (Aoki et al., 2005; Li et al., 2005; Rizzi et al., 2006). Unfortunately this method is limited to the reactions of cinnamic acid bearing electron-donationg groups on the aromatic ring. Recently we developed a novel synthesis of the dihydrocoumarins based on CF3SO3H promoted Friedel Crafts reaction of electron-rich hydroxyarenes (Krawczyk et al., 2007a) with the (E)-3-aryl-2-(diethoxyphosphoryl)acrylic acids. The title compound (I) is a key product of that synthesis.

The title compound (I) represents a novel dihydrocoumarine analog in which the δ-valerolactone ring bears the P—C bond. A related compound (II) in which the electron-donating para-methoxy substituent was replaced by the electron-withdrawing Br atom has been published by us recently (Krawczyk et al., 2007b). A search of the Cambridge Structural Database (Version 5.29; Allen, 2002) showed that crystal structures of the related compounds have not been reported so far.

A view of (I), with atom numbering scheme is shown in Fig. 1. The δ-valerolactone and naphtalene moieties are almost coplanar with one another. The former ring adopts conformation close to a 4S3 screw-boat (Boeyens, 1978), with O1, C1, C3, C4 and C9 almost coplanar (the average r.m.s. deviation from the mean plane is 0.09 Å) and C2 situated at the flap. The Cremer & Pople (1975) puckering parameters for the ring atom sequence O1/C1/C2/C3/C4/C9 are: Q = 0.489 (2) Å, θ = 113.6 (2)° and φ = 327.5 (3)°. Both exocyclic substituents, namely the diethoxyphosphoryl and phenyl groups occupy axial positions in respect to the δ-valerolactone ring.

The former group adopts an almost synperiplanar conformation along the P—C2 bond (Fig. 2). This arrangement is stabilized by electrostatic interactions of the oppositely charged phosphoryl O4 (-0.70 e) with the carbonyl C1 (0.79 e) atoms [the C1···O2 distance is 2.966 (2) Å] Atomic charges derived from electrostatic potentials were calculated using GAUSSIAN03 (Frisch et al., 2004) at the MP2/6-311++G(d,p) level for the X-ray determined coordinates. Grid points were selected according to the CHELPG procedure of Breneman & Wiberg (1990).

The phosphorus atom is located within the center of distorted tetrahedron with valency angles ranging in value from 99.90 (9) to 115.74 (11)°. On average the O—P—O type angles [111.6 (2)°] are larger then O—P—C [106.9 (2)°]. This is a general feature, often encountered in phosphorus compounds, indicating a significance of repulsive Coulombic type interactions between the oxygen atoms bearing the negative charge (Gillespie & Popelier, 2001).

A superposition of structures (I) and (II), as presented in Fig. 3, clearly shows similarity of the neoflavonoid fragments. The major difference is position of the O5—C22—C23 diethoxy group. In (I) this group points away from the naphtalene fragment while in (II) it is almost paralel and involved in the C—H—π(arom) interaction. The latter stabilizes a virtual eclipsed conformation along the axial P—C bond as was found in (II).

In the crystal molecules form centrosymmetric dimers connected by strong, practically linear hydrogen bonds linking phosphoryl and hydroxyl groups of both monomers. In terms of Etter's graph-set terminology (Etter, 1990; Bernstein, et al., 1995) this system can be described as R22(20).

Experimental

The solution 1,3-dihydroxynaphtalene in CH2Cl2, trifluoromethanesulfonic acid and (E)-2-diethoxyphosphoryl-3-(4-methoxyphenyl)acrylic acid were added and a resulting mixture was left at room temperature for 1 day. After the acrylic acid was completely reacted, saturated NaHCO3 solution was added. The organic layer was separated, washed with water and dried over MgSO4. Evaporation of the solvent under reduced preasure gave a crude product which was purified by column chromatography and recrystalized from diethyl ether.

Refinement

H atoms were located on difference Fourier maps and refined as riding on their carrier O or C atoms with Uiso(H) = 1.2Ueq(O or C). The methyl groups were allowed to rotate about their local threefold axis. AFIX 84, AFIX 14, AFIX 24, AFIX 44 and AFIX 138 procedures as in SHELXTL (Sheldrick, 2008) were applied.

Figures

Fig. 1.

Fig. 1.

The molecule of the title compound (I). Displacement elipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Newman projection along the C2—P bond.

Fig. 3.

Fig. 3.

A superposition of structures (I) and (II). The latter is indicated in the dashed line. The least-squares fit was based on all common non-H atoms of the 3,4-dihydrocoumarin moiety; the r.m.s. deviation was 0.10 Å.

Fig. 4.

Fig. 4.

Supplementary figure.

Crystal data

C24H25O7P Dx = 1.348 Mg m3
Mr = 456.41 Melting point = 396–398 K
Monoclinic, C2/c Mo Kα radiation λ = 0.71073 Å
a = 21.6231 (17) Å Cell parameters from 8721 reflections
b = 10.0018 (8) Å θ = 2.2–23.3º
c = 22.4011 (17) Å µ = 0.17 mm1
β = 111.8060 (10)º T = 293 (2) K
V = 4498.0 (6) Å3 Prism, colourless
Z = 8 0.30 × 0.20 × 0.15 mm
F000 = 1920

Data collection

Bruker SMART APEX diffractometer 5076 independent reflections
Radiation source: fine-focus sealed tube 3585 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.044
T = 293(2) K θmax = 27.4º
ω scans θmin = 2.0º
Absorption correction: multi-scan(SADABS; Bruker, 2003) h = −27→27
Tmin = 0.951, Tmax = 0.976 k = −12→12
37601 measured reflections l = −28→28

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045 H-atom parameters constrained
wR(F2) = 0.137   w = 1/[σ2(Fo2) + (0.0691P)2 + 2.0425P] where P = (Fo2 + 2Fc2)/3
S = 1.05 (Δ/σ)max = 0.001
5076 reflections Δρmax = 0.30 e Å3
310 parameters Δρmin = −0.36 e Å3
Primary atom site location: structure-invariant direct methods Extinction correction: none

Special details

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)

x y z Uiso*/Ueq
P 0.85826 (2) 0.18689 (5) 0.93687 (3) 0.04719 (16)
O1 0.86909 (7) 0.50338 (13) 0.99316 (6) 0.0501 (3)
O2 0.82123 (8) 0.38041 (16) 1.04447 (7) 0.0612 (4)
O3 0.82989 (9) 0.07064 (16) 0.96515 (11) 0.0843 (6)
O4 0.92748 (7) 0.22132 (16) 0.97264 (8) 0.0645 (4)
O5 0.84281 (8) 0.14572 (19) 0.86632 (8) 0.0751 (5)
O6 1.00680 (7) 0.72224 (17) 0.90165 (8) 0.0694 (5)
O7 0.54354 (8) 0.70103 (17) 0.84382 (11) 0.0838 (6)
C1 0.82904 (10) 0.40053 (19) 0.99520 (10) 0.0464 (4)
C2 0.79907 (9) 0.31862 (18) 0.93467 (9) 0.0445 (4)
C3 0.77848 (9) 0.40694 (18) 0.87347 (9) 0.0433 (4)
C4 0.83847 (9) 0.49031 (17) 0.87772 (9) 0.0411 (4)
C5 0.85316 (9) 0.53228 (18) 0.82352 (9) 0.0432 (4)
C6 0.91093 (9) 0.60975 (19) 0.83255 (9) 0.0457 (4)
C7 0.95280 (9) 0.6475 (2) 0.89610 (10) 0.0492 (5)
C8 0.93774 (10) 0.60900 (19) 0.94736 (10) 0.0484 (5)
C9 0.88100 (9) 0.53133 (18) 0.93693 (9) 0.0435 (4)
C10 0.81079 (11) 0.5026 (2) 0.75920 (10) 0.0540 (5)
C11 0.82642 (13) 0.5444 (2) 0.70810 (11) 0.0616 (6)
C12 0.88486 (13) 0.6152 (2) 0.71814 (12) 0.0636 (6)
C13 0.92573 (12) 0.6490 (2) 0.77862 (11) 0.0567 (5)
C14 0.71632 (9) 0.48976 (18) 0.86470 (9) 0.0436 (4)
C15 0.65938 (10) 0.4277 (2) 0.86667 (12) 0.0596 (6)
C16 0.60208 (11) 0.4993 (2) 0.85812 (13) 0.0667 (6)
C17 0.60088 (11) 0.6368 (2) 0.84824 (11) 0.0589 (5)
C18 0.65601 (11) 0.6988 (2) 0.84519 (11) 0.0586 (5)
C19 0.71301 (11) 0.6250 (2) 0.85320 (10) 0.0525 (5)
C20 0.85865 (19) −0.0622 (3) 0.97519 (18) 0.0957 (10)
C21 0.80938 (19) −0.1530 (3) 0.98260 (16) 0.0963 (10)
C22 0.89018 (18) 0.1465 (3) 0.83444 (15) 0.0930 (9)
C23 0.90252 (16) 0.0103 (4) 0.81830 (16) 0.0989 (10)
C24 0.54361 (16) 0.8430 (3) 0.84361 (19) 0.1038 (12)
H6 1.0276 0.7404 0.9401 0.083*
H21 0.7610 0.2782 0.9357 0.053*
H31 0.7679 0.3463 0.8355 0.049*
H81 0.9632 0.6325 0.9862 0.058*
H101 0.7706 0.4525 0.7514 0.065*
H111 0.7983 0.5257 0.6674 0.074*
H121 0.8960 0.6395 0.6832 0.076*
H131 0.9646 0.6994 0.7848 0.068*
H151 0.6601 0.3230 0.8750 0.071*
H161 0.5596 0.4502 0.8591 0.080*
H181 0.6553 0.7910 0.8377 0.070*
H191 0.7487 0.6669 0.8508 0.063*
H201 0.9030 −0.0639 1.0173 0.115*
H202 0.8708 −0.0913 0.9351 0.115*
H211 0.7686 −0.1586 0.9396 0.116*
H212 0.7941 −0.1177 1.0185 0.116*
H213 0.8303 −0.2473 0.9950 0.116*
H221 0.9333 0.1881 0.8636 0.112*
H222 0.8721 0.2019 0.7940 0.112*
H231 0.8583 −0.0365 0.7950 0.119*
H232 0.9286 −0.0405 0.8593 0.119*
H233 0.9293 0.0130 0.7894 0.119*
H241 0.5474 0.8736 0.8060 0.125*
H242 0.5793 0.8740 0.8787 0.125*
H243 0.5042 0.8741 0.8460 0.125*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
P 0.0439 (3) 0.0381 (3) 0.0599 (3) −0.0019 (2) 0.0197 (2) −0.0012 (2)
O1 0.0655 (8) 0.0447 (7) 0.0433 (7) −0.0119 (6) 0.0239 (6) −0.0030 (6)
O2 0.0725 (10) 0.0645 (9) 0.0561 (9) −0.0060 (7) 0.0350 (8) 0.0033 (7)
O3 0.0837 (12) 0.0446 (9) 0.1457 (18) 0.0093 (8) 0.0673 (12) 0.0225 (10)
O4 0.0446 (8) 0.0607 (9) 0.0785 (11) −0.0006 (7) 0.0117 (7) −0.0075 (8)
O5 0.0616 (9) 0.0879 (12) 0.0692 (11) 0.0157 (8) 0.0167 (8) −0.0224 (9)
O6 0.0543 (9) 0.0794 (11) 0.0696 (10) −0.0216 (8) 0.0174 (7) 0.0139 (8)
O7 0.0596 (10) 0.0626 (11) 0.1338 (17) 0.0164 (8) 0.0414 (10) 0.0119 (10)
C1 0.0509 (10) 0.0410 (9) 0.0514 (11) 0.0028 (8) 0.0236 (9) 0.0050 (8)
C2 0.0418 (9) 0.0380 (9) 0.0562 (11) −0.0040 (8) 0.0213 (8) 0.0010 (8)
C3 0.0451 (10) 0.0381 (9) 0.0464 (10) −0.0037 (7) 0.0169 (8) −0.0037 (8)
C4 0.0412 (9) 0.0383 (9) 0.0445 (10) −0.0008 (7) 0.0170 (8) 0.0002 (7)
C5 0.0448 (10) 0.0414 (9) 0.0437 (10) 0.0087 (8) 0.0169 (8) 0.0033 (8)
C6 0.0461 (10) 0.0426 (10) 0.0511 (11) 0.0087 (8) 0.0214 (8) 0.0098 (8)
C7 0.0418 (10) 0.0459 (10) 0.0584 (12) −0.0003 (8) 0.0169 (9) 0.0101 (9)
C8 0.0493 (11) 0.0459 (10) 0.0443 (11) −0.0060 (8) 0.0106 (8) 0.0032 (8)
C9 0.0514 (10) 0.0378 (9) 0.0433 (10) −0.0006 (8) 0.0198 (8) 0.0018 (7)
C10 0.0553 (12) 0.0562 (12) 0.0483 (12) 0.0062 (9) 0.0167 (9) −0.0012 (9)
C11 0.0753 (15) 0.0636 (14) 0.0431 (11) 0.0190 (11) 0.0189 (10) 0.0050 (10)
C12 0.0793 (16) 0.0655 (14) 0.0563 (13) 0.0187 (12) 0.0371 (12) 0.0177 (11)
C13 0.0600 (12) 0.0579 (12) 0.0601 (14) 0.0096 (10) 0.0316 (11) 0.0160 (10)
C14 0.0445 (10) 0.0403 (9) 0.0432 (10) −0.0030 (8) 0.0129 (8) −0.0045 (8)
C15 0.0497 (12) 0.0424 (11) 0.0826 (16) −0.0040 (9) 0.0200 (11) −0.0020 (10)
C16 0.0469 (12) 0.0520 (12) 0.0978 (19) −0.0041 (10) 0.0231 (12) −0.0002 (12)
C17 0.0513 (12) 0.0538 (12) 0.0698 (14) 0.0071 (9) 0.0204 (10) 0.0034 (10)
C18 0.0631 (13) 0.0425 (11) 0.0710 (14) 0.0055 (9) 0.0262 (11) 0.0090 (10)
C19 0.0526 (11) 0.0445 (10) 0.0634 (13) −0.0034 (9) 0.0248 (10) 0.0045 (9)
C20 0.134 (3) 0.0501 (14) 0.134 (3) 0.0191 (15) 0.085 (2) 0.0209 (15)
C21 0.150 (3) 0.0501 (14) 0.093 (2) −0.0089 (17) 0.050 (2) −0.0010 (14)
C22 0.128 (3) 0.091 (2) 0.0795 (19) 0.0193 (19) 0.0617 (19) 0.0055 (16)
C23 0.093 (2) 0.109 (2) 0.102 (2) 0.0270 (19) 0.0449 (18) −0.0189 (19)
C24 0.084 (2) 0.0640 (17) 0.169 (4) 0.0255 (15) 0.053 (2) 0.0175 (19)

Geometric parameters (Å, °)

P—O4 1.4524 (15) C11—C12 1.392 (3)
P—O5 1.5449 (17) C11—H111 0.9082
P—O3 1.5551 (16) C12—C13 1.357 (3)
P—C2 1.8248 (19) C12—H121 0.9322
O1—C1 1.356 (2) C13—H131 0.9462
O1—C9 1.404 (2) C14—C19 1.374 (3)
O2—C1 1.194 (2) C14—C15 1.394 (3)
O3—C20 1.449 (3) C15—C16 1.381 (3)
O5—C22 1.450 (3) C15—H151 1.0672
O6—C7 1.352 (2) C16—C17 1.391 (3)
O6—H6 0.8309 C16—H161 1.0483
O7—C17 1.367 (3) C17—C18 1.368 (3)
O7—C24 1.420 (3) C18—C19 1.390 (3)
C1—C2 1.509 (3) C18—H181 0.9346
C2—C3 1.551 (3) C19—H191 0.8967
C2—H21 0.9241 C20—C21 1.455 (4)
C3—C4 1.515 (2) C20—H201 1.0668
C3—C14 1.528 (3) C20—H202 1.0668
C3—H31 1.0001 C21—H211 1.0385
C4—C9 1.366 (3) C21—H212 1.0385
C4—C5 1.428 (3) C21—H213 1.0385
C5—C6 1.419 (3) C22—C23 1.459 (4)
C5—C10 1.422 (3) C22—H221 1.0092
C6—C13 1.415 (3) C22—H222 1.0092
C6—C7 1.425 (3) C23—H231 1.0166
C7—C8 1.360 (3) C23—H232 1.0166
C8—C9 1.397 (3) C23—H233 1.0166
C8—H81 0.8711 C24—H241 0.9270
C10—C11 1.374 (3) C24—H242 0.9270
C10—H101 0.9613 C24—H243 0.9270
O4—P—O5 114.48 (10) C11—C12—H121 119.9
O4—P—O3 115.74 (11) C12—C13—C6 120.9 (2)
O5—P—O3 104.43 (11) C12—C13—H131 119.6
O4—P—C2 114.36 (9) C6—C13—H131 119.6
O5—P—C2 106.37 (9) C19—C14—C15 117.34 (18)
O3—P—C2 99.90 (9) C19—C14—C3 122.67 (17)
C1—O1—C9 120.89 (15) C15—C14—C3 119.98 (17)
C20—O3—P 122.52 (17) C16—C15—C14 121.5 (2)
C22—O5—P 125.35 (18) C16—C15—H151 119.3
C7—O6—H6 109.5 C14—C15—H151 119.3
C17—O7—C24 117.9 (2) C15—C16—C17 119.8 (2)
O2—C1—O1 118.05 (18) C15—C16—H161 120.1
O2—C1—C2 125.32 (18) C17—C16—H161 120.1
O1—C1—C2 116.61 (16) O7—C17—C18 124.5 (2)
C1—C2—C3 111.81 (15) O7—C17—C16 116.0 (2)
C1—C2—P 107.75 (13) C18—C17—C16 119.4 (2)
C3—C2—P 113.78 (13) C17—C18—C19 120.0 (2)
C1—C2—H21 107.8 C17—C18—H181 120.0
C3—C2—H21 107.8 C19—C18—H181 120.0
P—C2—H21 107.8 C14—C19—C18 121.9 (2)
C4—C3—C14 113.67 (15) C14—C19—H191 119.0
C4—C3—C2 107.47 (15) C18—C19—H191 119.0
C14—C3—C2 111.86 (15) O3—C20—C21 107.4 (3)
C4—C3—H31 107.9 O3—C20—H201 110.2
C14—C3—H31 107.9 C21—C20—H201 110.2
C2—C3—H31 107.9 O3—C20—H202 110.2
C9—C4—C5 117.07 (17) C21—C20—H202 110.2
C9—C4—C3 118.56 (16) H201—C20—H202 108.5
C5—C4—C3 124.35 (16) C20—C21—H211 109.5
C6—C5—C10 117.40 (18) C20—C21—H212 109.5
C6—C5—C4 120.10 (17) H211—C21—H212 109.5
C10—C5—C4 122.48 (18) C20—C21—H213 109.5
C13—C6—C5 119.73 (19) H211—C21—H213 109.5
C13—C6—C7 121.19 (19) H212—C21—H213 109.5
C5—C6—C7 119.08 (17) O5—C22—C23 110.2 (3)
O6—C7—C8 123.23 (19) O5—C22—H221 109.6
O6—C7—C6 116.41 (18) C23—C22—H221 109.6
C8—C7—C6 120.37 (18) O5—C22—H222 109.6
C7—C8—C9 119.15 (19) C23—C22—H222 109.6
C7—C8—H81 120.4 H221—C22—H222 108.1
C9—C8—H81 120.4 C22—C23—H231 109.5
C4—C9—C8 124.20 (17) C22—C23—H232 109.5
C4—C9—O1 121.96 (17) H231—C23—H232 109.5
C8—C9—O1 113.77 (16) C22—C23—H233 109.5
C11—C10—C5 121.0 (2) H231—C23—H233 109.5
C11—C10—H101 119.5 H232—C23—H233 109.5
C5—C10—H101 119.5 O7—C24—H241 109.5
C10—C11—C12 120.7 (2) O7—C24—H242 109.5
C10—C11—H111 119.7 H241—C24—H242 109.5
C12—C11—H111 119.7 O7—C24—H243 109.5
C13—C12—C11 120.2 (2) H241—C24—H243 109.5
C13—C12—H121 119.9 H242—C24—H243 109.5
O4—P—C2—C1 −28.73 (16) C13—C6—C7—C8 179.94 (18)
O5—P—C2—C3 −31.54 (16) C5—C6—C7—C8 0.4 (3)
O4—P—O3—C20 −58.5 (3) O6—C7—C8—C9 −179.72 (18)
O5—P—O3—C20 68.3 (3) C6—C7—C8—C9 0.4 (3)
C2—P—O3—C20 178.2 (2) C5—C4—C9—C8 −1.1 (3)
O4—P—O5—C22 −3.4 (3) C3—C4—C9—C8 −179.64 (17)
O3—P—O5—C22 −131.0 (2) C5—C4—C9—O1 175.78 (15)
C2—P—O5—C22 123.9 (2) C3—C4—C9—O1 −2.8 (3)
C9—O1—C1—O2 179.21 (17) C7—C8—C9—C4 −0.1 (3)
C9—O1—C1—C2 0.5 (2) C7—C8—C9—O1 −177.13 (17)
O2—C1—C2—C3 143.09 (19) C1—O1—C9—C4 22.1 (3)
O1—C1—C2—C3 −38.3 (2) C1—O1—C9—C8 −160.77 (17)
O2—C1—C2—P −91.2 (2) C6—C5—C10—C11 1.8 (3)
O1—C1—C2—P 87.41 (17) C4—C5—C10—C11 −179.95 (18)
O5—P—C2—C1 −156.12 (13) C5—C10—C11—C12 1.1 (3)
O3—P—C2—C1 95.53 (15) C10—C11—C12—C13 −3.0 (3)
O4—P—C2—C3 95.84 (15) C11—C12—C13—C6 1.9 (3)
O5—P—C2—C3 −31.54 (16) C5—C6—C13—C12 1.0 (3)
O3—P—C2—C3 −139.90 (15) C7—C6—C13—C12 −178.5 (2)
C1—C2—C3—C4 52.53 (19) C4—C3—C14—C19 8.2 (3)
P—C2—C3—C4 −69.83 (17) C2—C3—C14—C19 130.13 (19)
C1—C2—C3—C14 −72.89 (19) C4—C3—C14—C15 −173.41 (18)
P—C2—C3—C14 164.74 (12) C2—C3—C14—C15 −51.5 (2)
C14—C3—C4—C9 90.9 (2) C19—C14—C15—C16 −0.7 (3)
C2—C3—C4—C9 −33.4 (2) C3—C14—C15—C16 −179.2 (2)
C14—C3—C4—C5 −87.6 (2) C14—C15—C16—C17 −1.0 (4)
C2—C3—C4—C5 148.11 (17) C24—O7—C17—C18 −7.7 (4)
C9—C4—C5—C6 1.9 (3) C24—O7—C17—C16 170.6 (3)
C3—C4—C5—C6 −179.65 (16) C15—C16—C17—O7 −176.4 (2)
C9—C4—C5—C10 −176.39 (17) C15—C16—C17—C18 2.0 (4)
C3—C4—C5—C10 2.1 (3) O7—C17—C18—C19 177.0 (2)
C10—C5—C6—C13 −2.8 (3) C16—C17—C18—C19 −1.3 (4)
C4—C5—C6—C13 178.90 (17) C15—C14—C19—C18 1.4 (3)
C10—C5—C6—C7 176.76 (17) C3—C14—C19—C18 179.84 (19)
C4—C5—C6—C7 −1.6 (3) C17—C18—C19—C14 −0.4 (3)
C13—C6—C7—O6 0.0 (3) P—O3—C20—C21 −162.7 (2)
C5—C6—C7—O6 −179.46 (17) P—O5—C22—C23 114.1 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O6—H6···O4i 0.83 1.87 2.701 (2) 178

Symmetry codes: (i) −x+2, −y+1, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG2458).

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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 datablocks global, I. DOI: 10.1107/S1600536808015857/ng2458sup1.cif

e-64-o1240-sup1.cif (23.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808015857/ng2458Isup2.hkl

e-64-o1240-Isup2.hkl (308.1KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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