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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Jan 17;65(Pt 2):o346. doi: 10.1107/S160053680900155X

1,4-Bis[(3,5-dimethoxy­phen­yl)ethyn­yl]benzene

Katsuhiko Ono a,*, Koki Nakagawa a, Masaaki Tomura b
PMCID: PMC2968219  PMID: 21581947

Abstract

The title compound, C26H22O4, is a derivative of 1,4-bis­(phenyl­ethyn­yl)benzene substituted by four meth­oxy groups on the terminal benzene rings. The mol­ecule is almost planar with an r.m.s. deviation of 0.266 Å. The dihedral angles between the two terminal benzene rings and the central benzene ring are 7.96 (6) and 13.32 (7)°. In the crystal structure, mol­ecules aggregate via C—H⋯O inter­actions, forming mol­ecular tapes along the a axis, which aggregate to form a herring-bone structure.

Related literature

For the crystal structure of 1,4-bis­[(2,6-dimethoxy­phen­yl)ethyn­yl]benzene, see: Ono et al. (2008). For related sructures, including a 1,4-bis­(phenyl­ethyn­yl)benzene system, see: Watt et al. (2004); Li et al. (1998); Filatov & Petrukhina (2005).graphic file with name e-65-0o346-scheme1.jpg

Experimental

Crystal data

  • C26H22O4

  • M r = 398.44

  • Monoclinic, Inline graphic

  • a = 8.8980 (5) Å

  • b = 19.4610 (8) Å

  • c = 12.2820 (5) Å

  • β = 100.607 (1)°

  • V = 2090.46 (17) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 173 (1) K

  • 0.30 × 0.25 × 0.15 mm

Data collection

  • Rigaku Mercury CCD diffractometer

  • Absorption correction: none

  • 15238 measured reflections

  • 4638 independent reflections

  • 3914 reflections with I > 2σ(I)

  • R int = 0.024

Refinement

  • R[F 2 > 2σ(F 2)] = 0.048

  • wR(F 2) = 0.140

  • S = 1.11

  • 4638 reflections

  • 271 parameters

  • H-atom parameters constrained

  • Δρmax = 0.26 e Å−3

  • Δρmin = −0.17 e Å−3

Data collection: CrystalClear (Rigaku, 2001); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SIR2002 (Burla et al., 2003); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2003) and Mercury (Macrae et al., 2006); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053680900155X/ci2753sup1.cif

e-65-0o346-sup1.cif (21KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680900155X/ci2753Isup2.hkl

e-65-0o346-Isup2.hkl (222.6KB, 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
C11—H11⋯O4i 0.95 2.42 3.3511 (17) 167
C14—H14⋯O2ii 0.95 2.37 3.2758 (16) 160

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

Acknowledgments

This work was supported by a Grant-in-Aid for Scientific Research (grant No. 19550034) from the Ministry of Education, Culture, Sports, Science and Technology, Japan. The authors thank the Instrument Center of the Institute for Molecular Science for the X-ray structure analysis.

supplementary crystallographic information

Comment

The synthetic research of ethynylated aromatic compounds has attracted considerable attention because of interests in their molecular structures, optical properties, and molecular electronics. Among these ethynylated aromatic compounds, 1,4-bis(phenylethynyl)benzene derivatives have been extensively studied. These compounds have stiff, linear molecular structures and are used as building blocks in the applications. Recently, we found that 1,4-bis[(2,6-dimethoxyphenyl)ethynyl]benzene, (II), formed a zigzag molecular network in the crystal (Ono et al., 2008). The crystal structure is different from those of 1,4-bis(phenylethynyl)benzene derivatives (Watt et al., 2004; Li et al., 1998; Filatov & Petrukhina, 2005). With regard to this, we investigated the molecular and crystal structure of the title compound, (I), which is a regioisomer of (II). The substitution effect of four methoxy groups at the terminal benzene rings was studied.

The molecular structure of (I) is shown in Fig. 1. The molecule is almost planar with an r.m.s deviation of 0.266 Å. The dihedral angles between the terminal benzene rings and the central benzene ring are 7.96 (6)° (C1–C6) and 13.32 (7)° (C17–C22). The methoxy groups are coplanar with the attached benzene rings.

The crystal structure is characterized by a molecular tape along the a axis formed by C—H···O interactions (Table 1 and Fig. 2). The molecular tapes aggregate to form a herring-bone-type structure, as shown in Fig.3. The crystal structure of (I) is different from that of (II). The crystal structures of (I) and (II) indicate that the methoxy groups at terminal benzene rings play an important role in the crystal packing.

Experimental

The title compound (I) was prepared as follows: Tetrakis(triphenylphosphine)palladium(0) [Pd(PPh3)4] (52 mg, 0.045 mmol) was added to a mixture of 1-ethynyl-3,5-dimethoxybenzene (0.39 g, 2.4 mmol), 1,4-diiodobenzene (0.39 g, 1.2 mmol) and copper(I) iodide (5 mg, 0.03 mmol) in dry triethylamine (7 ml) under nitrogen. The reaction mixture was stirred for 18 h at 353 K. After removal of the solvent, dichloromethane (20 ml) and aqueous disodium ethylenediaminetetraacetate (Na2edta) solution (5%, 20 ml) were added. The organic layer was separated and washed with water (20 ml). The organic solution was dried over Na2SO4 and concentrated. The residue was chromatographed on silica gel (CH2Cl2) to afford the title compound (0.23 g, 49%) as a yellow powder. Yellow crystals of the compound, suitable for X-ray analysis were grown from an ethanol solution.

Refinement

All H atoms were placed in geometrically calculated positions, with C-H = 0.95 (aromatic) and 0.98 Å (methyl) and Uiso(H) = 1.2Ueq(C) (aromatic) and 1.5Ueq(C) (methyl), and refined using a riding model.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I), with atom labels and 50% probability displacement ellipsoids for non-H atoms and H atoms are shown as small spheres of arbitrary radii.

Fig. 2.

Fig. 2.

Partial packing diagram of (I), showing a molecular tape along the a axis.

Fig. 3.

Fig. 3.

The packing diagram of (I), showing herringbone-type network on the bc plane.

Crystal data

C26H22O4 F(000) = 840
Mr = 398.44 Dx = 1.266 Mg m3
Monoclinic, P21/a Melting point: 431 K
Hall symbol: -P 2yab Mo Kα radiation, λ = 0.71073 Å
a = 8.8980 (5) Å Cell parameters from 5437 reflections
b = 19.4610 (8) Å θ = 3.1–27.5°
c = 12.2820 (5) Å µ = 0.09 mm1
β = 100.607 (1)° T = 173 K
V = 2090.46 (17) Å3 Block, yellow
Z = 4 0.30 × 0.25 × 0.15 mm

Data collection

Rigaku Mercury CCD diffractometer 3914 reflections with I > 2σ(I)
Radiation source: Rotating Anode Rint = 0.024
Graphite Monochromator θmax = 27.5°, θmin = 3.1°
Detector resolution: 14.7059 pixels mm-1 h = −11→10
φ and ω scans k = −22→25
15238 measured reflections l = −15→12
4638 independent reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.048 H-atom parameters constrained
wR(F2) = 0.140 w = 1/[σ2(Fo2) + (0.0818P)2 + 0.1522P] where P = (Fo2 + 2Fc2)/3
S = 1.11 (Δ/σ)max = 0.001
4638 reflections Δρmax = 0.26 e Å3
271 parameters Δρmin = −0.17 e Å3
0 restraints

Special details

Experimental. IR (KBr, cm-1): 1605, 1580, 1345, 1254, 1202, 1161, 1065, 841; 1H NMR (CDCl3, δ p.p.m.): 3.81 (s, 12H), 6.48 (t, J = 2.3 Hz, 2H), 6.70 (d, J = 2.3 Hz, 4H), 7.51 (s, 4H); 13C NMR (CDCl3, δ p.p.m.): 55.3, 88.6, 91.3, 102.0, 109.4, 123.0, 124.3, 131.6, 160.6; MS (EI): m/z 398 (M+), 199.
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
C1 0.04347 (14) 0.17522 (6) 0.71287 (10) 0.0266 (3)
C2 −0.11459 (14) 0.17481 (6) 0.67760 (11) 0.0266 (3)
H2 −0.1799 0.1980 0.7185 0.032*
C3 −0.17430 (13) 0.13932 (6) 0.58033 (11) 0.0265 (3)
C4 −0.07979 (14) 0.10623 (6) 0.51948 (11) 0.0277 (3)
H4 −0.1225 0.0824 0.4535 0.033*
C5 0.07839 (14) 0.10787 (6) 0.55512 (10) 0.0261 (3)
C6 0.14059 (14) 0.14194 (6) 0.65309 (11) 0.0283 (3)
H6 0.2480 0.1424 0.6787 0.034*
C7 0.17340 (14) 0.07642 (6) 0.48619 (11) 0.0288 (3)
C8 0.24292 (14) 0.05168 (7) 0.42138 (11) 0.0288 (3)
C9 0.32492 (14) 0.02180 (6) 0.34289 (10) 0.0262 (3)
C10 0.24597 (14) −0.01164 (7) 0.24864 (11) 0.0286 (3)
H10 0.1377 −0.0150 0.2371 0.034*
C11 0.32439 (14) −0.03986 (7) 0.17214 (11) 0.0303 (3)
H11 0.2695 −0.0621 0.1081 0.036*
C12 0.48372 (14) −0.03594 (6) 0.18839 (10) 0.0273 (3)
C13 0.56275 (14) −0.00329 (6) 0.28348 (11) 0.0297 (3)
H13 0.6712 −0.0009 0.2959 0.036*
C14 0.48439 (14) 0.02550 (7) 0.35943 (11) 0.0295 (3)
H14 0.5392 0.0479 0.4233 0.035*
C15 0.56748 (14) −0.06453 (7) 0.10994 (11) 0.0305 (3)
C16 0.64138 (15) −0.08764 (7) 0.04662 (11) 0.0313 (3)
C17 0.73414 (14) −0.11338 (6) −0.02860 (11) 0.0289 (3)
C18 0.67256 (14) −0.15780 (7) −0.11433 (11) 0.0309 (3)
H18 0.5689 −0.1720 −0.1231 0.037*
C19 0.76419 (14) −0.18118 (7) −0.18695 (11) 0.0289 (3)
C20 0.91672 (14) −0.16179 (7) −0.17484 (11) 0.0289 (3)
H20 0.9792 −0.1787 −0.2238 0.035*
C21 0.97568 (14) −0.11696 (7) −0.08931 (11) 0.0310 (3)
C22 0.88622 (14) −0.09254 (7) −0.01627 (11) 0.0316 (3)
H22 0.9283 −0.0619 0.0416 0.038*
C23 0.02302 (18) 0.24526 (8) 0.87014 (12) 0.0434 (4)
H23A 0.0889 0.2677 0.9328 0.065*
H23B −0.0440 0.2122 0.8980 0.065*
H23C −0.0392 0.2800 0.8247 0.065*
C24 −0.43253 (15) 0.17035 (8) 0.58918 (13) 0.0409 (4)
H24A −0.5365 0.1618 0.5488 0.061*
H24B −0.4108 0.2197 0.5890 0.061*
H24C −0.4236 0.1543 0.6657 0.061*
C25 0.77935 (17) −0.24753 (8) −0.34851 (12) 0.0398 (3)
H25A 0.7151 −0.2772 −0.4025 0.060*
H25B 0.8679 −0.2737 −0.3107 0.060*
H25C 0.8146 −0.2082 −0.3868 0.060*
C26 1.22202 (17) −0.11600 (9) −0.14105 (15) 0.0506 (4)
H26A 1.3229 −0.0950 −0.1178 0.076*
H26B 1.1803 −0.1025 −0.2175 0.076*
H26C 1.2316 −0.1661 −0.1366 0.076*
O1 0.11541 (10) 0.21008 (5) 0.80454 (8) 0.0360 (2)
O2 −0.32622 (10) 0.13442 (5) 0.53688 (8) 0.0352 (2)
O3 0.69301 (10) −0.22363 (5) −0.26936 (9) 0.0396 (3)
O4 1.12292 (11) −0.09341 (6) −0.07075 (9) 0.0477 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0340 (6) 0.0247 (6) 0.0213 (6) 0.0006 (5) 0.0059 (5) −0.0006 (5)
C2 0.0318 (6) 0.0241 (6) 0.0263 (7) 0.0011 (5) 0.0113 (5) −0.0004 (5)
C3 0.0273 (6) 0.0244 (6) 0.0287 (7) −0.0013 (4) 0.0073 (5) 0.0015 (5)
C4 0.0345 (6) 0.0257 (6) 0.0235 (6) −0.0007 (5) 0.0068 (5) −0.0036 (5)
C5 0.0322 (6) 0.0232 (6) 0.0249 (6) 0.0034 (5) 0.0106 (5) 0.0016 (5)
C6 0.0280 (6) 0.0281 (6) 0.0291 (7) 0.0025 (5) 0.0058 (5) −0.0005 (5)
C7 0.0314 (6) 0.0279 (6) 0.0277 (7) 0.0016 (5) 0.0071 (5) −0.0007 (5)
C8 0.0324 (6) 0.0280 (6) 0.0266 (7) 0.0020 (5) 0.0069 (5) −0.0004 (5)
C9 0.0309 (6) 0.0248 (6) 0.0243 (6) 0.0033 (5) 0.0089 (5) 0.0012 (5)
C10 0.0266 (6) 0.0331 (7) 0.0265 (7) 0.0027 (5) 0.0061 (5) −0.0005 (5)
C11 0.0340 (6) 0.0338 (7) 0.0226 (6) 0.0014 (5) 0.0042 (5) −0.0045 (5)
C12 0.0330 (6) 0.0269 (6) 0.0238 (6) 0.0043 (5) 0.0103 (5) 0.0000 (5)
C13 0.0277 (6) 0.0333 (7) 0.0293 (7) 0.0007 (5) 0.0083 (5) −0.0012 (5)
C14 0.0325 (6) 0.0316 (6) 0.0248 (7) −0.0015 (5) 0.0064 (5) −0.0051 (5)
C15 0.0346 (6) 0.0303 (7) 0.0278 (7) 0.0033 (5) 0.0086 (5) −0.0006 (5)
C16 0.0358 (6) 0.0316 (7) 0.0278 (7) 0.0036 (5) 0.0092 (5) −0.0007 (5)
C17 0.0344 (6) 0.0299 (6) 0.0238 (6) 0.0062 (5) 0.0089 (5) 0.0002 (5)
C18 0.0286 (6) 0.0338 (7) 0.0322 (7) −0.0007 (5) 0.0109 (5) −0.0034 (6)
C19 0.0317 (6) 0.0294 (6) 0.0259 (7) −0.0011 (5) 0.0065 (5) −0.0044 (5)
C20 0.0296 (6) 0.0330 (7) 0.0255 (7) 0.0018 (5) 0.0091 (5) −0.0038 (5)
C21 0.0286 (6) 0.0363 (7) 0.0285 (7) −0.0008 (5) 0.0057 (5) −0.0029 (5)
C22 0.0356 (7) 0.0348 (7) 0.0244 (7) 0.0003 (5) 0.0057 (5) −0.0071 (5)
C23 0.0512 (8) 0.0486 (9) 0.0291 (8) 0.0112 (7) 0.0037 (6) −0.0135 (7)
C24 0.0286 (6) 0.0471 (9) 0.0487 (9) 0.0001 (6) 0.0112 (6) −0.0110 (7)
C25 0.0459 (8) 0.0429 (8) 0.0324 (8) −0.0052 (6) 0.0121 (6) −0.0150 (6)
C26 0.0339 (7) 0.0718 (12) 0.0499 (10) −0.0131 (7) 0.0179 (7) −0.0190 (8)
O1 0.0364 (5) 0.0429 (6) 0.0274 (5) 0.0056 (4) 0.0023 (4) −0.0123 (4)
O2 0.0271 (4) 0.0380 (5) 0.0403 (6) −0.0022 (4) 0.0062 (4) −0.0102 (4)
O3 0.0361 (5) 0.0459 (6) 0.0390 (6) −0.0091 (4) 0.0123 (4) −0.0198 (5)
O4 0.0302 (5) 0.0698 (7) 0.0446 (7) −0.0122 (5) 0.0112 (4) −0.0260 (6)

Geometric parameters (Å, °)

C1—O1 1.3684 (15) C17—C22 1.3940 (18)
C1—C6 1.3924 (16) C17—C18 1.3942 (18)
C1—C2 1.3933 (17) C18—C19 1.3911 (16)
C2—C3 1.3975 (18) C18—H18 0.95
C2—H2 0.95 C19—O3 1.3683 (15)
C3—O2 1.3622 (15) C19—C20 1.3900 (17)
C3—C4 1.3826 (16) C20—C21 1.3917 (18)
C4—C5 1.3953 (17) C20—H20 0.95
C4—H4 0.95 C21—O4 1.3670 (15)
C5—C6 1.3960 (18) C21—C22 1.3882 (17)
C5—C7 1.4386 (16) C22—H22 0.95
C6—H6 0.95 C23—O1 1.4274 (16)
C7—C8 1.1956 (17) C23—H23A 0.98
C8—C9 1.4348 (16) C23—H23B 0.98
C9—C14 1.3977 (17) C23—H23C 0.98
C9—C10 1.3991 (18) C24—O2 1.4213 (15)
C10—C11 1.3831 (17) C24—H24A 0.98
C10—H10 0.95 C24—H24B 0.98
C11—C12 1.3969 (17) C24—H24C 0.98
C11—H11 0.95 C25—O3 1.4236 (16)
C12—C13 1.3999 (18) C25—H25A 0.98
C12—C15 1.4345 (16) C25—H25B 0.98
C13—C14 1.3820 (17) C25—H25C 0.98
C13—H13 0.95 C26—O4 1.4130 (17)
C14—H14 0.95 C26—H26A 0.98
C15—C16 1.1949 (18) C26—H26B 0.98
C16—C17 1.4375 (17) C26—H26C 0.98
O1—C1—C6 115.01 (10) C19—C18—C17 119.46 (11)
O1—C1—C2 123.44 (11) C19—C18—H18 120.3
C6—C1—C2 121.49 (11) C17—C18—H18 120.3
C1—C2—C3 118.14 (11) O3—C19—C20 123.57 (11)
C1—C2—H2 120.9 O3—C19—C18 115.19 (11)
C3—C2—H2 120.9 C20—C19—C18 121.24 (12)
O2—C3—C4 114.46 (11) C19—C20—C21 118.42 (11)
O2—C3—C2 124.28 (11) C19—C20—H20 120.8
C4—C3—C2 121.26 (11) C21—C20—H20 120.8
C3—C4—C5 119.91 (11) O4—C21—C22 115.05 (12)
C3—C4—H4 120.0 O4—C21—C20 123.55 (11)
C5—C4—H4 120.0 C22—C21—C20 121.40 (11)
C4—C5—C6 119.88 (11) C21—C22—C17 119.40 (12)
C4—C5—C7 118.29 (11) C21—C22—H22 120.3
C6—C5—C7 121.78 (11) C17—C22—H22 120.3
C1—C6—C5 119.30 (11) O1—C23—H23A 109.5
C1—C6—H6 120.4 O1—C23—H23B 109.5
C5—C6—H6 120.4 H23A—C23—H23B 109.5
C8—C7—C5 174.44 (14) O1—C23—H23C 109.5
C7—C8—C9 179.42 (15) H23A—C23—H23C 109.5
C14—C9—C10 119.07 (11) H23B—C23—H23C 109.5
C14—C9—C8 120.64 (11) O2—C24—H24A 109.5
C10—C9—C8 120.29 (11) O2—C24—H24B 109.5
C11—C10—C9 120.50 (11) H24A—C24—H24B 109.5
C11—C10—H10 119.8 O2—C24—H24C 109.5
C9—C10—H10 119.8 H24A—C24—H24C 109.5
C10—C11—C12 120.45 (11) H24B—C24—H24C 109.5
C10—C11—H11 119.8 O3—C25—H25A 109.5
C12—C11—H11 119.8 O3—C25—H25B 109.5
C11—C12—C13 119.00 (11) H25A—C25—H25B 109.5
C11—C12—C15 121.46 (11) O3—C25—H25C 109.5
C13—C12—C15 119.54 (11) H25A—C25—H25C 109.5
C14—C13—C12 120.58 (11) H25B—C25—H25C 109.5
C14—C13—H13 119.7 O4—C26—H26A 109.5
C12—C13—H13 119.7 O4—C26—H26B 109.5
C13—C14—C9 120.39 (12) H26A—C26—H26B 109.5
C13—C14—H14 119.8 O4—C26—H26C 109.5
C9—C14—H14 119.8 H26A—C26—H26C 109.5
C16—C15—C12 177.95 (14) H26B—C26—H26C 109.5
C15—C16—C17 177.90 (14) C1—O1—C23 118.13 (10)
C22—C17—C18 120.08 (11) C3—O2—C24 118.91 (10)
C22—C17—C16 119.31 (12) C19—O3—C25 117.90 (10)
C18—C17—C16 120.60 (11) C21—O4—C26 118.72 (11)
O1—C1—C2—C3 177.69 (11) C8—C9—C14—C13 −179.92 (12)
C6—C1—C2—C3 0.59 (18) C22—C17—C18—C19 0.2 (2)
C1—C2—C3—O2 179.60 (11) C16—C17—C18—C19 179.07 (12)
C1—C2—C3—C4 −0.90 (18) C17—C18—C19—O3 −178.99 (12)
O2—C3—C4—C5 179.63 (11) C17—C18—C19—C20 0.8 (2)
C2—C3—C4—C5 0.08 (18) O3—C19—C20—C21 178.44 (12)
C3—C4—C5—C6 1.06 (18) C18—C19—C20—C21 −1.4 (2)
C3—C4—C5—C7 −176.30 (11) C19—C20—C21—O4 −178.72 (13)
O1—C1—C6—C5 −176.80 (11) C19—C20—C21—C22 0.9 (2)
C2—C1—C6—C5 0.53 (19) O4—C21—C22—C17 179.75 (12)
C4—C5—C6—C1 −1.36 (18) C20—C21—C22—C17 0.1 (2)
C7—C5—C6—C1 175.90 (11) C18—C17—C22—C21 −0.6 (2)
C14—C9—C10—C11 −0.84 (19) C16—C17—C22—C21 −179.55 (12)
C8—C9—C10—C11 179.30 (12) C6—C1—O1—C23 −179.78 (12)
C9—C10—C11—C12 0.59 (19) C2—C1—O1—C23 2.94 (18)
C10—C11—C12—C13 0.28 (19) C4—C3—O2—C24 −175.99 (12)
C10—C11—C12—C15 −179.69 (12) C2—C3—O2—C24 3.55 (18)
C11—C12—C13—C14 −0.90 (19) C20—C19—O3—C25 −1.8 (2)
C15—C12—C13—C14 179.07 (12) C18—C19—O3—C25 178.03 (12)
C12—C13—C14—C9 0.65 (19) C22—C21—O4—C26 179.71 (14)
C10—C9—C14—C13 0.22 (19) C20—C21—O4—C26 −0.6 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C11—H11···O4i 0.95 2.42 3.3511 (17) 167
C14—H14···O2ii 0.95 2.37 3.2758 (16) 160

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CI2753).

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 datablocks I, global. DOI: 10.1107/S160053680900155X/ci2753sup1.cif

e-65-0o346-sup1.cif (21KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680900155X/ci2753Isup2.hkl

e-65-0o346-Isup2.hkl (222.6KB, hkl)

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


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