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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Jan 9;69(Pt 2):o212. doi: 10.1107/S1600536813000214

4-(Oct­yloxy)phenyl 2-oxo-2H-chromene-3-carboxyl­ate

B S Palakshamurthy a, S Sreenivasa b, H T Srinivasa c, K R Roopashree a, H C Devarajegowda a,*
PMCID: PMC3569748  PMID: 23424494

Abstract

In the title compound, C24H26O5, the 2H-chromene ring system is essentially planar, with a maximum deviation of 0.029 (2) Å from the best-fit mean plane incorporating both rings. The dihedral angle between the 2H-chromene ring system and the benzene ring is 21.00 (1)°. In the crystal, pairs of C—H⋯O hydrogen bonds generate an R 2 2(8) ring pattern. These contacts are bolstered by weaker bifurcated C—H⋯O hydrogen bonds.

Related literature  

For general background to coumarin derivatives and their biological and technological applications, see: Georgieva et al. (2004); Creaven et al. (2005); Morita et al. (2005); Tian et al. (2003); Iliopoulos et al. (2010); Hejchman et al. (2011). For hydrogen-bond motifs, see: Bernstein et al. (1995).graphic file with name e-69-0o212-scheme1.jpg

Experimental  

Crystal data  

  • C24H26O5

  • M r = 394.45

  • Monoclinic, Inline graphic

  • a = 14.464 (3) Å

  • b = 6.7548 (15) Å

  • c = 21.381 (5) Å

  • β = 91.663 (8)°

  • V = 2088.0 (8) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 293 K

  • 0.29 × 0.25 × 0.21 mm

Data collection  

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2007) T min = 0.975, T max = 0.982

  • 22609 measured reflections

  • 3615 independent reflections

  • 1926 reflections with I > 2σ(I)

  • R int = 0.084

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.058

  • wR(F 2) = 0.146

  • S = 0.94

  • 3615 reflections

  • 264 parameters

  • H-atom parameters constrained

  • Δρmax = 0.18 e Å−3

  • Δρmin = −0.14 e Å−3

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 2012); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813000214/sj5291sup1.cif

e-69-0o212-sup1.cif (29.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813000214/sj5291Isup2.hkl

e-69-0o212-Isup2.hkl (173.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813000214/sj5291Isup3.cml

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
C4—H4⋯O1i 0.93 2.59 3.513 (4) 174
C9—H9⋯O2i 0.93 2.51 3.420 (3) 167
C16—H16⋯O2i 0.93 2.71 3.551 (3) 151
C16—H16⋯O3i 0.93 2.63 3.338 (3) 133

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank Professor T. N. Guru Row, Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore, and P. A. Suchetan, Department of Studies and Research in Chemistry, U·C.S. Tumkur University, Tumkur, for their help and suggestions.

supplementary crystallographic information

Comment

Coumarin derivatives have been attracted increasing attention due to their extensive biological applications, such as anticancer, anti-inflammatory and anticoagulant agents (Georgieva et al., 2004; Creaven et al., 2005). The coumarin nucleus has been the focus of our recent research concerning the design, synthesis and characterization to investigate their liquid crystal properties together with crystal structure studies (Morita et al., 2005; Tian et al., 2003). Coumarins are interesting class of heterocycles because of their dipolar moment increases by external stimulus such as light, temperature, electric current and chemical reaction (Iliopoulos et al., 2010). The excitation of the coumarin chromophore increases the electron density of its carbonyl groups owing to excited photochemical and photophysical properties such as molecular fluorescent sensors, laser dyes and many industrial applications (Hejchman et al., 2011).

The asymmetric unit of 4-(octyloxy)phenyl 2-oxo-2H-chromene-3 -carboxylate is shown in Fig. 1. The 2H-chromene ring (O1/C1–C9) system is planar, with a maximum deviation of 0.028 (2) Å for atom C8. The dihedral angle between 2H-chromene ring (O1/C1–C9) and benzene ring (C11–C16) is 21.11 (1)°. The crystal structure is characterized by intermolecular C4—H4···O1 and C9—H9···O2 hydrogen bonding generating an R22(8) ring pattern (Bernstein et al., 1995). Bifurcated C16—H16···O2 and C16—H16···O3 contacts further strengthen the packing, Fig. 2.

Experimental

A mixture of 2-oxo-2H-chromene-3-carboxylic acid (19 mg,1 mmol), 4-(octyloxy)phenol (22.2 mg,1 mmol), N,N -dicyclohexylcarbodiimide (23 mg,1.2 mmol) and a catalytic quantity of N,N-dimethylaminopyrimidine was stirred in 5 ml of dry dichloromethane for 24 h at room temperature. The residue obtained on removal of solvent was chromatographed on silica gel and eluted with chloroform. Removal of solvent from the eluate afforded a colorless solid, which was re-crystallized from absolute ethanol to obtain needle like crystals of the title compound for X-ray diffraction analysis.

Refinement

All H atoms were positioned geometrically, with C—H = 0.93 Å for aromatic H, C—H = 0.97 Å for methylene H and C—H = 0.96 Å for methyl H, and refined using a riding model with Uiso(H) = 1.5Ueq(C) for methyl H and Uiso(H) = 1.2Ueq(C) for all other H.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound. Displacement ellipsoids are drawn at the 50% probability level. Hydrogen atoms are shown as spheres of arbitrary radius.

Fig. 2.

Fig. 2.

Crystal packing for the title compound with hydrogen bonds drawn as dashed lines.

Crystal data

C24H26O5 F(000) = 840
Mr = 394.45 Dx = 1.255 Mg m3
Monoclinic, P21/n Melting point: 580 K
Hall symbol: -P 2yn Mo Kα radiation, λ = 0.71073 Å
a = 14.464 (3) Å Cell parameters from 3615 reflections
b = 6.7548 (15) Å θ = 3.2–25.0°
c = 21.381 (5) Å µ = 0.09 mm1
β = 91.663 (8)° T = 293 K
V = 2088.0 (8) Å3 Needles, colourless
Z = 4 0.29 × 0.25 × 0.21 mm

Data collection

Bruker SMART CCD area-detector diffractometer 3615 independent reflections
Radiation source: fine-focus sealed tube 1926 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.084
ω and φ scans θmax = 25.0°, θmin = 3.2°
Absorption correction: multi-scan (SADABS; Sheldrick, 2007) h = −17→16
Tmin = 0.975, Tmax = 0.982 k = −8→5
22609 measured reflections l = −25→25

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.058 H-atom parameters constrained
wR(F2) = 0.146 w = 1/[σ2(Fo2) + (0.077P)2] where P = (Fo2 + 2Fc2)/3
S = 0.94 (Δ/σ)max < 0.001
3615 reflections Δρmax = 0.18 e Å3
264 parameters Δρmin = −0.14 e Å3
0 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0019 (7)

Special details

Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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
O1 0.11082 (14) 0.0294 (3) −0.01675 (8) 0.0705 (6)
O2 0.11756 (15) −0.1104 (3) 0.07552 (9) 0.0826 (7)
O3 0.06844 (14) 0.1538 (3) 0.17685 (9) 0.0744 (6)
O4 0.14523 (12) 0.4373 (2) 0.16091 (7) 0.0610 (5)
O5 0.14206 (14) 0.7392 (3) 0.40100 (8) 0.0730 (6)
C1 0.1075 (2) 0.1595 (5) −0.11861 (13) 0.0755 (9)
H1 0.1043 0.0314 −0.1345 0.091*
C2 0.1090 (2) 0.3196 (5) −0.15818 (14) 0.0827 (9)
H2 0.1062 0.2995 −0.2012 0.099*
C3 0.1146 (2) 0.5101 (5) −0.13485 (14) 0.0775 (9)
H3 0.1165 0.6174 −0.1620 0.093*
C4 0.11723 (19) 0.5398 (4) −0.07203 (13) 0.0682 (8)
H4 0.1203 0.6682 −0.0564 0.082*
C5 0.11538 (17) 0.3810 (4) −0.03071 (11) 0.0509 (6)
C6 0.11088 (18) 0.1917 (4) −0.05564 (12) 0.0557 (7)
C7 0.11337 (19) 0.0428 (4) 0.04771 (12) 0.0603 (7)
C8 0.11338 (17) 0.2423 (3) 0.07410 (11) 0.0497 (6)
C9 0.11632 (16) 0.3995 (4) 0.03580 (11) 0.0524 (7)
H9 0.1191 0.5255 0.0533 0.063*
C10 0.10603 (18) 0.2654 (4) 0.14224 (12) 0.0531 (7)
C11 0.13845 (18) 0.5046 (4) 0.22323 (11) 0.0535 (7)
C12 0.16625 (19) 0.3932 (4) 0.27383 (12) 0.0639 (8)
H12 0.1845 0.2623 0.2686 0.077*
C13 0.16691 (19) 0.4769 (4) 0.33248 (12) 0.0650 (8)
H13 0.1863 0.4028 0.3671 0.078*
C14 0.13875 (19) 0.6712 (4) 0.34023 (11) 0.0567 (7)
C15 0.11116 (19) 0.7799 (4) 0.28884 (11) 0.0619 (7)
H15 0.0923 0.9104 0.2938 0.074*
C16 0.11120 (19) 0.6972 (4) 0.22990 (11) 0.0591 (7)
H16 0.0929 0.7715 0.1951 0.071*
C17 0.1323 (2) 0.9462 (4) 0.41084 (12) 0.0645 (7)
H17A 0.0739 0.9916 0.3926 0.077*
H17B 0.1819 1.0168 0.3909 0.077*
C18 0.1356 (2) 0.9869 (4) 0.47999 (11) 0.0675 (8)
H18A 0.1914 0.9287 0.4984 0.081*
H18B 0.0831 0.9239 0.4989 0.081*
C19 0.1343 (2) 1.2047 (4) 0.49476 (12) 0.0707 (8)
H19A 0.0812 1.2634 0.4731 0.085*
H19B 0.1893 1.2646 0.4780 0.085*
C20 0.1304 (2) 1.2574 (4) 0.56327 (12) 0.0723 (8)
H20A 0.0761 1.1960 0.5806 0.087*
H20B 0.1843 1.2027 0.5850 0.087*
C21 0.1269 (2) 1.4752 (5) 0.57543 (13) 0.0831 (9)
H21A 0.0717 1.5278 0.5546 0.100*
H21B 0.1797 1.5360 0.5562 0.100*
C22 0.1265 (2) 1.5383 (5) 0.64278 (13) 0.0839 (9)
H22A 0.1818 1.4883 0.6641 0.101*
H22B 0.0734 1.4801 0.6625 0.101*
C23 0.1229 (3) 1.7629 (5) 0.65022 (15) 0.1031 (12)
H23A 0.1746 1.8199 0.6287 0.124*
H23B 0.0666 1.8108 0.6295 0.124*
C24 0.1255 (3) 1.8364 (6) 0.71544 (16) 0.1332 (16)
H24A 0.0720 1.7894 0.7365 0.200*
H24B 0.1256 1.9785 0.7153 0.200*
H24C 0.1804 1.7889 0.7368 0.200*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.1120 (16) 0.0356 (11) 0.0641 (12) −0.0062 (10) 0.0039 (10) −0.0070 (9)
O2 0.1353 (19) 0.0309 (12) 0.0816 (14) −0.0007 (11) 0.0057 (12) 0.0064 (10)
O3 0.1055 (16) 0.0459 (12) 0.0723 (12) −0.0202 (11) 0.0096 (11) 0.0020 (10)
O4 0.0867 (14) 0.0398 (11) 0.0564 (11) −0.0166 (9) 0.0003 (9) −0.0004 (9)
O5 0.1129 (17) 0.0487 (13) 0.0570 (12) 0.0036 (10) −0.0023 (10) −0.0017 (9)
C1 0.103 (2) 0.059 (2) 0.0653 (19) −0.0103 (16) 0.0005 (16) −0.0075 (16)
C2 0.098 (3) 0.090 (3) 0.0596 (18) −0.0053 (19) −0.0046 (16) 0.0027 (19)
C3 0.097 (3) 0.066 (2) 0.069 (2) 0.0052 (17) 0.0010 (16) 0.0184 (17)
C4 0.082 (2) 0.0507 (18) 0.0718 (19) 0.0039 (15) 0.0006 (15) 0.0067 (16)
C5 0.0562 (17) 0.0401 (16) 0.0562 (15) 0.0004 (12) −0.0026 (12) 0.0034 (13)
C6 0.0659 (19) 0.0445 (17) 0.0566 (16) −0.0040 (13) −0.0021 (13) −0.0030 (14)
C7 0.075 (2) 0.0386 (17) 0.0672 (18) −0.0039 (13) 0.0036 (14) −0.0036 (15)
C8 0.0573 (17) 0.0307 (14) 0.0608 (16) −0.0013 (11) −0.0018 (12) 0.0018 (13)
C9 0.0623 (18) 0.0326 (15) 0.0622 (16) 0.0006 (12) −0.0020 (12) −0.0042 (12)
C10 0.0590 (17) 0.0361 (16) 0.0639 (17) −0.0016 (13) −0.0025 (13) 0.0025 (14)
C11 0.0697 (19) 0.0365 (15) 0.0542 (15) −0.0078 (12) 0.0018 (12) 0.0008 (13)
C12 0.087 (2) 0.0373 (15) 0.0670 (18) 0.0048 (14) −0.0062 (15) 0.0005 (14)
C13 0.092 (2) 0.0435 (17) 0.0588 (17) 0.0071 (14) −0.0091 (14) 0.0103 (14)
C14 0.0749 (19) 0.0434 (17) 0.0515 (16) −0.0048 (13) −0.0026 (13) 0.0046 (13)
C15 0.088 (2) 0.0377 (15) 0.0599 (17) 0.0002 (14) −0.0029 (14) 0.0023 (13)
C16 0.081 (2) 0.0369 (16) 0.0588 (17) −0.0038 (13) −0.0064 (14) 0.0094 (13)
C17 0.077 (2) 0.0548 (19) 0.0615 (17) 0.0054 (14) 0.0026 (13) −0.0055 (14)
C18 0.069 (2) 0.070 (2) 0.0638 (17) 0.0044 (15) 0.0027 (13) −0.0025 (15)
C19 0.090 (2) 0.0596 (19) 0.0627 (17) −0.0049 (16) 0.0010 (15) −0.0041 (15)
C20 0.086 (2) 0.060 (2) 0.0706 (19) −0.0015 (15) 0.0053 (15) −0.0064 (15)
C21 0.106 (3) 0.067 (2) 0.076 (2) 0.0033 (18) −0.0015 (17) −0.0039 (17)
C22 0.102 (3) 0.074 (2) 0.077 (2) 0.0031 (18) 0.0093 (17) −0.0084 (18)
C23 0.152 (3) 0.077 (3) 0.080 (2) 0.015 (2) 0.004 (2) −0.0115 (19)
C24 0.204 (5) 0.110 (3) 0.088 (3) 0.014 (3) 0.028 (3) −0.014 (2)

Geometric parameters (Å, º)

O1—C6 1.376 (3) C14—C15 1.371 (3)
O1—C7 1.381 (3) C15—C16 1.379 (3)
O2—C7 1.194 (3) C15—H15 0.9300
O3—C10 1.198 (3) C16—H16 0.9300
O4—C10 1.347 (3) C17—C18 1.503 (3)
O4—C11 1.414 (3) C17—H17A 0.9700
O5—C14 1.378 (3) C17—H17B 0.9700
O5—C17 1.422 (3) C18—C19 1.505 (4)
C1—C6 1.363 (3) C18—H18A 0.9700
C1—C2 1.374 (4) C18—H18B 0.9700
C1—H1 0.9300 C19—C20 1.510 (3)
C2—C3 1.381 (4) C19—H19A 0.9700
C2—H2 0.9300 C19—H19B 0.9700
C3—C4 1.357 (3) C20—C21 1.496 (4)
C3—H3 0.9300 C20—H20A 0.9700
C4—C5 1.390 (3) C20—H20B 0.9700
C4—H4 0.9300 C21—C22 1.502 (4)
C5—C6 1.386 (3) C21—H21A 0.9700
C5—C9 1.427 (3) C21—H21B 0.9700
C7—C8 1.461 (3) C22—C23 1.527 (4)
C8—C9 1.342 (3) C22—H22A 0.9700
C8—C10 1.472 (3) C22—H22B 0.9700
C9—H9 0.9300 C23—C24 1.479 (4)
C11—C16 1.368 (4) C23—H23A 0.9700
C11—C12 1.369 (3) C23—H23B 0.9700
C12—C13 1.375 (3) C24—H24A 0.9600
C12—H12 0.9300 C24—H24B 0.9600
C13—C14 1.386 (4) C24—H24C 0.9600
C13—H13 0.9300
C6—O1—C7 123.4 (2) C15—C16—H16 120.4
C10—O4—C11 121.06 (19) O5—C17—C18 109.0 (2)
C14—O5—C17 117.82 (19) O5—C17—H17A 109.9
C6—C1—C2 118.8 (3) C18—C17—H17A 109.9
C6—C1—H1 120.6 O5—C17—H17B 109.9
C2—C1—H1 120.6 C18—C17—H17B 109.9
C1—C2—C3 120.8 (3) H17A—C17—H17B 108.3
C1—C2—H2 119.6 C17—C18—C19 112.6 (2)
C3—C2—H2 119.6 C17—C18—H18A 109.1
C4—C3—C2 119.6 (3) C19—C18—H18A 109.1
C4—C3—H3 120.2 C17—C18—H18B 109.1
C2—C3—H3 120.2 C19—C18—H18B 109.1
C3—C4—C5 120.9 (3) H18A—C18—H18B 107.8
C3—C4—H4 119.5 C18—C19—C20 115.8 (2)
C5—C4—H4 119.5 C18—C19—H19A 108.3
C6—C5—C4 117.9 (2) C20—C19—H19A 108.3
C6—C5—C9 117.6 (2) C18—C19—H19B 108.3
C4—C5—C9 124.5 (2) C20—C19—H19B 108.3
C1—C6—O1 118.0 (2) H19A—C19—H19B 107.4
C1—C6—C5 121.8 (2) C21—C20—C19 113.8 (2)
O1—C6—C5 120.2 (2) C21—C20—H20A 108.8
O2—C7—O1 116.1 (2) C19—C20—H20A 108.8
O2—C7—C8 127.4 (2) C21—C20—H20B 108.8
O1—C7—C8 116.5 (2) C19—C20—H20B 108.8
C9—C8—C7 119.6 (2) H20A—C20—H20B 107.7
C9—C8—C10 121.6 (2) C20—C21—C22 116.5 (3)
C7—C8—C10 118.7 (2) C20—C21—H21A 108.2
C8—C9—C5 122.6 (2) C22—C21—H21A 108.2
C8—C9—H9 118.7 C20—C21—H21B 108.2
C5—C9—H9 118.7 C22—C21—H21B 108.2
O3—C10—O4 123.6 (2) H21A—C21—H21B 107.3
O3—C10—C8 126.3 (2) C21—C22—C23 112.5 (3)
O4—C10—C8 110.0 (2) C21—C22—H22A 109.1
C16—C11—C12 121.3 (2) C23—C22—H22A 109.1
C16—C11—O4 115.6 (2) C21—C22—H22B 109.1
C12—C11—O4 122.8 (2) C23—C22—H22B 109.1
C11—C12—C13 119.3 (2) H22A—C22—H22B 107.8
C11—C12—H12 120.4 C24—C23—C22 115.6 (3)
C13—C12—H12 120.4 C24—C23—H23A 108.4
C12—C13—C14 120.3 (2) C22—C23—H23A 108.4
C12—C13—H13 119.9 C24—C23—H23B 108.4
C14—C13—H13 119.9 C22—C23—H23B 108.4
C15—C14—O5 125.3 (2) H23A—C23—H23B 107.4
C15—C14—C13 119.4 (2) C23—C24—H24A 109.5
O5—C14—C13 115.2 (2) C23—C24—H24B 109.5
C14—C15—C16 120.5 (3) H24A—C24—H24B 109.5
C14—C15—H15 119.7 C23—C24—H24C 109.5
C16—C15—H15 119.7 H24A—C24—H24C 109.5
C11—C16—C15 119.2 (2) H24B—C24—H24C 109.5
C11—C16—H16 120.4
C6—C1—C2—C3 0.6 (5) C9—C8—C10—O3 148.8 (3)
C1—C2—C3—C4 −1.0 (5) C7—C8—C10—O3 −28.5 (4)
C2—C3—C4—C5 0.7 (4) C9—C8—C10—O4 −28.8 (3)
C3—C4—C5—C6 0.1 (4) C7—C8—C10—O4 153.9 (2)
C3—C4—C5—C9 −178.9 (2) C10—O4—C11—C16 −131.1 (3)
C2—C1—C6—O1 −179.0 (3) C10—O4—C11—C12 55.5 (3)
C2—C1—C6—C5 0.2 (4) C16—C11—C12—C13 −0.1 (4)
C7—O1—C6—C1 −179.5 (2) O4—C11—C12—C13 172.9 (2)
C7—O1—C6—C5 1.2 (4) C11—C12—C13—C14 0.7 (4)
C4—C5—C6—C1 −0.6 (4) C17—O5—C14—C15 −11.9 (4)
C9—C5—C6—C1 178.5 (2) C17—O5—C14—C13 167.5 (2)
C4—C5—C6—O1 178.7 (2) C12—C13—C14—C15 −0.7 (4)
C9—C5—C6—O1 −2.3 (4) C12—C13—C14—O5 179.8 (2)
C6—O1—C7—O2 −176.5 (2) O5—C14—C15—C16 179.5 (2)
C6—O1—C7—C8 1.8 (4) C13—C14—C15—C16 0.1 (4)
O2—C7—C8—C9 174.3 (3) C12—C11—C16—C15 −0.5 (4)
O1—C7—C8—C9 −3.8 (4) O4—C11—C16—C15 −174.0 (2)
O2—C7—C8—C10 −8.4 (4) C14—C15—C16—C11 0.5 (4)
O1—C7—C8—C10 173.6 (2) C14—O5—C17—C18 178.6 (2)
C7—C8—C9—C5 2.8 (4) O5—C17—C18—C19 174.9 (2)
C10—C8—C9—C5 −174.5 (2) C17—C18—C19—C20 175.7 (2)
C6—C5—C9—C8 0.3 (4) C18—C19—C20—C21 −178.6 (3)
C4—C5—C9—C8 179.2 (3) C19—C20—C21—C22 −177.7 (3)
C11—O4—C10—O3 −4.6 (4) C20—C21—C22—C23 180.0 (3)
C11—O4—C10—C8 173.1 (2) C21—C22—C23—C24 −178.1 (3)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C4—H4···O1i 0.93 2.59 3.513 (4) 174
C9—H9···O2i 0.93 2.51 3.420 (3) 167
C16—H16···O2ii 0.93 2.71 3.551 (3) 151
C16—H16···O3ii 0.93 2.63 3.338 (3) 133

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SJ5291).

References

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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) I, global. DOI: 10.1107/S1600536813000214/sj5291sup1.cif

e-69-0o212-sup1.cif (29.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813000214/sj5291Isup2.hkl

e-69-0o212-Isup2.hkl (173.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813000214/sj5291Isup3.cml

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


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