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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2007 Dec 6;64(Pt 1):o77. doi: 10.1107/S1600536807057455

N,N′-(Oxydi-p-phenyl­ene)diphthalimide

Yi-Tao Li a,*, Zhiguo Wang b
PMCID: PMC2915034  PMID: 21200954

Abstract

The title compound, C28H16N2O5, is a bis-imide derivative in which two phthalimide units are linked by an oxydi-p-phenyl­ene bridge. The dihedral angle between the planes of the two central benzene rings is 86.1 (4)°. The isoindole groups make dihedral angles of 46.0 (14) and 77.5 (13)° with the attached benzene rings. Inter­molecular C—H⋯O hydrogen bonds contribute to the stability of the structure.

Related literature

For details of the biological activity and uses of bis-imide derivatives, see: Rich et al. (1975); Degenhardt et al. (2002); Mallakpour & Kowsari (2004); Zhang et al. (1999); Langhals & Kirner (2000); Yakimov & Forrest (2002). For a related structure, see: Li et al. (2007).graphic file with name e-64-00o77-scheme1.jpg

Experimental

Crystal data

  • C28H16N2O5

  • M r = 460.43

  • Orthorhombic, Inline graphic

  • a = 7.5059 (11) Å

  • b = 16.480 (3) Å

  • c = 17.551 (3) Å

  • V = 2171.0 (6) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 292 (2) K

  • 0.30 × 0.30 × 0.30 mm

Data collection

  • Bruker SMART 4K CCD area-detector diffractometer

  • Absorption correction: none

  • 13091 measured reflections

  • 2925 independent reflections

  • 2644 reflections with I > 2σ(I)

  • R int = 0.027

Refinement

  • R[F 2 > 2σ(F 2)] = 0.046

  • wR(F 2) = 0.118

  • S = 1.23

  • 2925 reflections

  • 316 parameters

  • H-atom parameters constrained

  • Δρmax = 0.16 e Å−3

  • Δρmin = −0.26 e Å−3

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536807057455/wn2220sup1.cif

e-64-00o77-sup1.cif (22.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807057455/wn2220Isup2.hkl

e-64-00o77-Isup2.hkl (143.6KB, 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⋯O5i 0.93 2.47 3.222 (4) 138
C19—H19⋯O5ii 0.93 2.56 3.298 (4) 136

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

Acknowledgments

The authors thank Dr Xiang-Gao Meng for the data collection.

supplementary crystallographic information

Comment

Bisimides are heterocyclic compounds, some of which have biological activity (Rich et al., 1975). Moreover, they are synthetic precursors with applications in organic synthesis (Degenhardt et al., 2002), polymer synthesis (Mallakpour & Kowsari, 2004), supramolecular chemistry (Zhang et al., 1999), and for the development of new materials (Langhals & Kirner, 2000) and molecular electronic devices (Yakimov & Forrest, 2002).

Following our studies on the synthesis of bisimide derivatives (Li et al., 2007), we report here the structure of the title compound (Fig. 1). The two phthalimide units are linked by a (phenoxy)phenylene bridge. The dihedral angle between the planes of the two central benzene rings is 86.1 (4)° The isoindole groups make dihedral angles of 46.0 (14)° and 77.5 (13)° with the attached benzene rings. Compared to a similar structure, N,N'-(methylenedi-p-phenylene)diphthalimide (Li et al., 2007), the packing pattern is different; this may be due to the bridging methylene group being replaced by the bridging O atom. Intermolecular C—H···O hydrogen bonds contribute to the stability of the structure (Table 1).

Experimental

A solution of phthaloyl dichoride (420 mg, 2 mmol) was added slowly over a period of 10 min to a solution of 4-aminophenyl ether (400 mg, 2 mmol) in dichloromethane (25 ml) at 273 K to yield a light yellow precipitate. Triethylamine (5 ml) was then added to dissolve the precipitate which became a yellow suspension after stirring for 12 h. The compound was filtered and dried (yield 510 mg, 70%). Single crystals of the title compound were obtained by recrystallization from dimethylformamide at room temperature.

Refinement

All H atoms were initially located in a difference Fourier map; they were then placed in calculated positions and constrained to ride on their parent atoms, with C—-H = 0.93 Å and Uiso(H) = 1.2Ueq(C). In the absence of significant anomalous scattering effects, Friedel pairs were merged.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, with 50% probability displacement ellipsoids. H atoms have been omitted.

Crystal data

C28H16N2O5 F000 = 952
Mr = 460.43 Dx = 1.409 Mg m3
Orthorhombic, P212121 Mo Kα radiation λ = 0.71073 Å
Hall symbol: P 2ac 2ab Cell parameters from 5562 reflections
a = 7.5059 (11) Å θ = 2.3–25.9º
b = 16.480 (3) Å µ = 0.10 mm1
c = 17.551 (3) Å T = 292 (2) K
V = 2171.0 (6) Å3 Block, colourless
Z = 4 0.30 × 0.30 × 0.30 mm

Data collection

Bruker SMART 4K CCD area-detector diffractometer 2644 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.027
Monochromator: graphite θmax = 28.0º
T = 292(2) K θmin = 2.3º
φ and ω scans h = −8→9
Absorption correction: none k = −21→17
13091 measured reflections l = −22→22
2925 independent reflections

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)] = 0.046 H-atom parameters constrained
wR(F2) = 0.118   w = 1/[σ2(Fo2) + (0.06P)2 + 0.1294P] where P = (Fo2 + 2Fc2)/3
S = 1.23 (Δ/σ)max = 0.017
2925 reflections Δρmax = 0.16 e Å3
316 parameters Δρmin = −0.26 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
C1 0.8558 (3) 0.62700 (13) 1.04648 (13) 0.0449 (5)
C2 0.9322 (4) 0.70185 (14) 1.05712 (13) 0.0492 (5)
H2 0.9588 0.7202 1.1059 0.059*
C3 0.9691 (4) 0.74958 (14) 0.99444 (15) 0.0492 (6)
H3 1.0231 0.7999 1.0009 0.059*
C4 0.9259 (3) 0.72283 (12) 0.92192 (12) 0.0432 (5)
C5 0.8447 (4) 0.64854 (13) 0.91224 (12) 0.0474 (5)
H5 0.8124 0.6313 0.8637 0.057*
C6 0.8115 (4) 0.59984 (13) 0.97454 (13) 0.0485 (5)
H6 0.7595 0.5491 0.9681 0.058*
C7 0.9251 (4) 0.85440 (13) 0.84975 (13) 0.0474 (5)
C8 1.0414 (4) 0.74006 (15) 0.78915 (14) 0.0506 (6)
C9 0.9801 (3) 0.87704 (15) 0.77128 (14) 0.0491 (5)
C10 1.0480 (3) 0.80952 (15) 0.73544 (13) 0.0494 (5)
C11 1.1046 (4) 0.81216 (19) 0.66035 (15) 0.0616 (7)
H11 1.1511 0.7665 0.6363 0.074*
C12 1.0891 (5) 0.8850 (2) 0.62283 (15) 0.0712 (9)
H12 1.1250 0.8886 0.5722 0.085*
C13 1.0219 (4) 0.9526 (2) 0.65846 (17) 0.0706 (9)
H13 1.0131 1.0009 0.6313 0.085*
C14 0.9667 (4) 0.95066 (17) 0.73407 (16) 0.0598 (7)
H14 0.9228 0.9966 0.7584 0.072*
C15 0.8345 (4) 0.49870 (14) 1.10677 (13) 0.0493 (6)
C16 0.6860 (4) 0.45102 (17) 1.11019 (18) 0.0634 (7)
H16 0.5730 0.4742 1.1105 0.076*
C17 0.7065 (4) 0.36759 (17) 1.11325 (19) 0.0649 (7)
H17 0.6066 0.3343 1.1156 0.078*
C18 0.8727 (4) 0.33395 (13) 1.11278 (13) 0.0484 (6)
C19 1.0208 (4) 0.38264 (17) 1.1071 (2) 0.0687 (8)
H19 1.1340 0.3598 1.1052 0.082*
C20 0.9999 (4) 0.46591 (17) 1.1043 (2) 0.0693 (8)
H20 1.0993 0.4994 1.1006 0.083*
C21 0.9359 (4) 0.20766 (15) 1.18659 (14) 0.0559 (6)
C22 0.8648 (4) 0.19351 (15) 1.05848 (15) 0.0577 (7)
C23 0.9404 (4) 0.12045 (15) 1.16640 (15) 0.0556 (6)
C24 0.8952 (4) 0.11189 (15) 1.09096 (15) 0.0563 (6)
C25 0.8777 (5) 0.03623 (17) 1.0583 (2) 0.0741 (9)
H25 0.8460 0.0300 1.0074 0.089*
C26 0.9095 (6) −0.03000 (18) 1.1046 (3) 0.0897 (12)
H26 0.8972 −0.0819 1.0844 0.108*
C27 0.9587 (6) −0.0216 (2) 1.1793 (3) 0.0890 (12)
H27 0.9808 −0.0676 1.2085 0.107*
C28 0.9758 (5) 0.05402 (19) 1.2116 (2) 0.0757 (9)
H28 1.0101 0.0601 1.2622 0.091*
N1 0.9654 (3) 0.77149 (11) 0.85670 (10) 0.0471 (5)
N2 0.8933 (3) 0.24810 (11) 1.11843 (11) 0.0533 (5)
O1 0.8144 (3) 0.58251 (10) 1.11128 (10) 0.0597 (5)
O2 0.8594 (3) 0.89603 (10) 0.89869 (11) 0.0626 (5)
O3 1.0881 (3) 0.67169 (11) 0.77944 (11) 0.0703 (6)
O4 0.9586 (4) 0.24056 (13) 1.24656 (11) 0.0848 (8)
O5 0.8234 (4) 0.21334 (12) 0.99506 (11) 0.0835 (7)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0544 (13) 0.0353 (10) 0.0449 (11) 0.0030 (10) 0.0066 (10) 0.0026 (9)
C2 0.0603 (14) 0.0456 (12) 0.0416 (10) −0.0062 (11) −0.0017 (11) −0.0034 (9)
C3 0.0631 (15) 0.0353 (9) 0.0491 (11) −0.0105 (10) −0.0011 (11) −0.0034 (9)
C4 0.0522 (12) 0.0335 (9) 0.0437 (10) 0.0012 (9) 0.0038 (10) 0.0009 (9)
C5 0.0631 (14) 0.0363 (11) 0.0427 (11) 0.0000 (10) −0.0001 (11) −0.0062 (9)
C6 0.0644 (14) 0.0298 (9) 0.0515 (12) −0.0061 (10) 0.0062 (11) −0.0041 (9)
C7 0.0549 (13) 0.0344 (10) 0.0528 (13) −0.0017 (10) 0.0010 (11) 0.0026 (9)
C8 0.0596 (15) 0.0459 (13) 0.0464 (12) −0.0013 (11) 0.0034 (11) −0.0033 (10)
C9 0.0511 (13) 0.0459 (12) 0.0502 (12) −0.0065 (10) −0.0071 (11) 0.0058 (10)
C10 0.0522 (13) 0.0511 (13) 0.0449 (12) −0.0085 (11) −0.0035 (10) 0.0019 (10)
C11 0.0655 (17) 0.0728 (17) 0.0467 (12) −0.0166 (14) −0.0006 (12) −0.0007 (12)
C12 0.0768 (19) 0.090 (2) 0.0469 (13) −0.0275 (18) −0.0038 (13) 0.0141 (15)
C13 0.0731 (19) 0.0712 (18) 0.0674 (17) −0.0239 (16) −0.0144 (15) 0.0306 (16)
C14 0.0633 (16) 0.0489 (13) 0.0673 (16) −0.0089 (12) −0.0110 (14) 0.0154 (12)
C15 0.0711 (16) 0.0379 (11) 0.0387 (10) −0.0051 (11) 0.0079 (11) 0.0024 (9)
C16 0.0620 (16) 0.0486 (13) 0.0797 (18) 0.0008 (12) −0.0009 (15) 0.0064 (13)
C17 0.0617 (16) 0.0456 (13) 0.087 (2) −0.0137 (12) 0.0021 (15) 0.0080 (14)
C18 0.0660 (15) 0.0370 (10) 0.0423 (11) −0.0051 (11) 0.0033 (11) 0.0042 (9)
C19 0.0567 (15) 0.0478 (14) 0.102 (2) −0.0010 (12) 0.0124 (16) −0.0028 (15)
C20 0.0626 (17) 0.0446 (13) 0.101 (2) −0.0120 (13) 0.0191 (16) −0.0048 (15)
C21 0.0687 (17) 0.0492 (14) 0.0496 (13) −0.0032 (13) 0.0003 (12) 0.0084 (11)
C22 0.0773 (18) 0.0470 (13) 0.0489 (13) −0.0085 (13) 0.0083 (13) −0.0022 (10)
C23 0.0586 (14) 0.0461 (12) 0.0622 (14) 0.0027 (12) 0.0086 (12) 0.0093 (11)
C24 0.0628 (15) 0.0429 (12) 0.0633 (14) −0.0016 (11) 0.0173 (13) −0.0003 (11)
C25 0.088 (2) 0.0525 (15) 0.0818 (19) −0.0029 (16) 0.0251 (18) −0.0115 (15)
C26 0.099 (3) 0.0418 (14) 0.128 (3) 0.0071 (16) 0.044 (3) −0.0095 (18)
C27 0.094 (3) 0.0545 (17) 0.118 (3) 0.0193 (18) 0.030 (2) 0.0254 (19)
C28 0.083 (2) 0.0565 (17) 0.088 (2) 0.0114 (15) 0.0092 (18) 0.0242 (16)
N1 0.0628 (12) 0.0349 (9) 0.0436 (9) −0.0002 (9) 0.0033 (9) 0.0016 (8)
N2 0.0771 (14) 0.0392 (9) 0.0437 (10) −0.0040 (10) −0.0006 (10) 0.0045 (8)
O1 0.0951 (14) 0.0372 (8) 0.0470 (9) −0.0010 (9) 0.0187 (10) 0.0013 (7)
O2 0.0824 (13) 0.0389 (9) 0.0666 (11) 0.0050 (9) 0.0175 (10) −0.0008 (8)
O3 0.1010 (15) 0.0449 (9) 0.0649 (10) 0.0095 (10) 0.0192 (12) −0.0044 (8)
O4 0.138 (2) 0.0649 (12) 0.0520 (11) −0.0018 (14) −0.0199 (13) 0.0008 (9)
O5 0.142 (2) 0.0636 (12) 0.0452 (10) −0.0148 (14) −0.0081 (12) 0.0031 (9)

Geometric parameters (Å, °)

C1—C2 1.373 (3) C15—C20 1.354 (4)
C1—C6 1.380 (3) C15—C16 1.365 (4)
C1—O1 1.388 (3) C15—O1 1.392 (3)
C2—C3 1.380 (3) C16—C17 1.385 (4)
C2—H2 0.9300 C16—H16 0.9300
C3—C4 1.385 (3) C17—C18 1.365 (4)
C3—H3 0.9300 C17—H17 0.9300
C4—C5 1.378 (3) C18—C19 1.374 (4)
C4—N1 1.429 (3) C18—N2 1.427 (3)
C5—C6 1.379 (3) C19—C20 1.382 (4)
C5—H5 0.9300 C19—H19 0.9300
C6—H6 0.9300 C20—H20 0.9300
C7—O2 1.205 (3) C21—O4 1.196 (3)
C7—N1 1.405 (3) C21—N2 1.406 (3)
C7—C9 1.485 (3) C21—C23 1.481 (4)
C8—O3 1.192 (3) C22—O5 1.201 (3)
C8—N1 1.414 (3) C22—N2 1.401 (3)
C8—C10 1.484 (3) C22—C24 1.478 (4)
C9—C10 1.376 (4) C23—C24 1.374 (4)
C9—C14 1.382 (3) C23—C28 1.378 (4)
C10—C11 1.385 (4) C24—C25 1.378 (4)
C11—C12 1.374 (4) C25—C26 1.381 (5)
C11—H11 0.9300 C25—H25 0.9300
C12—C13 1.374 (5) C26—C27 1.368 (6)
C12—H12 0.9300 C26—H26 0.9300
C13—C14 1.391 (4) C27—C28 1.375 (5)
C13—H13 0.9300 C27—H27 0.9300
C14—H14 0.9300 C28—H28 0.9300
C2—C1—C6 121.1 (2) C15—C16—H16 120.6
C2—C1—O1 117.2 (2) C17—C16—H16 120.6
C6—C1—O1 121.6 (2) C18—C17—C16 120.3 (3)
C1—C2—C3 119.2 (2) C18—C17—H17 119.8
C1—C2—H2 120.4 C16—C17—H17 119.8
C3—C2—H2 120.4 C17—C18—C19 120.2 (2)
C2—C3—C4 120.3 (2) C17—C18—N2 120.1 (2)
C2—C3—H3 119.9 C19—C18—N2 119.8 (3)
C4—C3—H3 119.9 C18—C19—C20 119.4 (3)
C5—C4—C3 120.0 (2) C18—C19—H19 120.3
C5—C4—N1 119.44 (19) C20—C19—H19 120.3
C3—C4—N1 120.60 (19) C15—C20—C19 119.9 (3)
C4—C5—C6 119.9 (2) C15—C20—H20 120.0
C4—C5—H5 120.0 C19—C20—H20 120.0
C6—C5—H5 120.0 O4—C21—N2 124.5 (2)
C1—C6—C5 119.5 (2) O4—C21—C23 130.3 (2)
C1—C6—H6 120.2 N2—C21—C23 105.2 (2)
C5—C6—H6 120.2 O5—C22—N2 124.1 (2)
O2—C7—N1 125.5 (2) O5—C22—C24 130.1 (2)
O2—C7—C9 129.2 (2) N2—C22—C24 105.7 (2)
N1—C7—C9 105.4 (2) C24—C23—C28 121.4 (3)
O3—C8—N1 125.8 (2) C24—C23—C21 108.9 (2)
O3—C8—C10 128.9 (2) C28—C23—C21 129.6 (3)
N1—C8—C10 105.29 (19) C23—C24—C25 121.1 (3)
C10—C9—C14 121.4 (2) C23—C24—C22 108.4 (2)
C10—C9—C7 108.9 (2) C25—C24—C22 130.4 (3)
C14—C9—C7 129.7 (3) C24—C25—C26 117.0 (3)
C9—C10—C11 121.5 (2) C24—C25—H25 121.5
C9—C10—C8 108.7 (2) C26—C25—H25 121.5
C11—C10—C8 129.7 (2) C27—C26—C25 122.0 (3)
C12—C11—C10 117.2 (3) C27—C26—H26 119.0
C12—C11—H11 121.4 C25—C26—H26 119.0
C10—C11—H11 121.4 C26—C27—C28 120.8 (3)
C11—C12—C13 121.4 (3) C26—C27—H27 119.6
C11—C12—H12 119.3 C28—C27—H27 119.6
C13—C12—H12 119.3 C27—C28—C23 117.6 (3)
C12—C13—C14 121.6 (3) C27—C28—H28 121.2
C12—C13—H13 119.2 C23—C28—H28 121.2
C14—C13—H13 119.2 C7—N1—C8 111.74 (19)
C9—C14—C13 116.7 (3) C7—N1—C4 124.81 (19)
C9—C14—H14 121.6 C8—N1—C4 123.36 (18)
C13—C14—H14 121.6 C22—N2—C21 111.7 (2)
C20—C15—C16 121.3 (2) C22—N2—C18 124.6 (2)
C20—C15—O1 119.8 (2) C21—N2—C18 123.6 (2)
C16—C15—O1 118.7 (3) C1—O1—C15 116.95 (18)
C15—C16—C17 118.8 (3)
C6—C1—C2—C3 −1.7 (4) C28—C23—C24—C25 2.2 (5)
O1—C1—C2—C3 −177.4 (2) C21—C23—C24—C25 −175.8 (3)
C1—C2—C3—C4 1.4 (4) C28—C23—C24—C22 179.7 (3)
C2—C3—C4—C5 0.5 (4) C21—C23—C24—C22 1.7 (3)
C2—C3—C4—N1 −179.3 (2) O5—C22—C24—C23 −180.0 (3)
C3—C4—C5—C6 −2.0 (4) N2—C22—C24—C23 −0.4 (3)
N1—C4—C5—C6 177.8 (2) O5—C22—C24—C25 −2.8 (6)
C2—C1—C6—C5 0.2 (4) N2—C22—C24—C25 176.8 (3)
O1—C1—C6—C5 175.7 (2) C23—C24—C25—C26 −0.7 (5)
C4—C5—C6—C1 1.7 (4) C22—C24—C25—C26 −177.6 (4)
O2—C7—C9—C10 −179.7 (3) C24—C25—C26—C27 −0.9 (6)
N1—C7—C9—C10 0.2 (3) C25—C26—C27—C28 1.0 (6)
O2—C7—C9—C14 −1.5 (5) C26—C27—C28—C23 0.5 (6)
N1—C7—C9—C14 178.4 (3) C24—C23—C28—C27 −2.1 (5)
C14—C9—C10—C11 −0.5 (4) C21—C23—C28—C27 175.5 (3)
C7—C9—C10—C11 177.8 (2) O2—C7—N1—C8 179.9 (3)
C14—C9—C10—C8 −178.7 (2) C9—C7—N1—C8 0.1 (3)
C7—C9—C10—C8 −0.4 (3) O2—C7—N1—C4 3.4 (4)
O3—C8—C10—C9 −179.8 (3) C9—C7—N1—C4 −176.5 (2)
N1—C8—C10—C9 0.4 (3) O3—C8—N1—C7 179.9 (3)
O3—C8—C10—C11 2.2 (5) C10—C8—N1—C7 −0.3 (3)
N1—C8—C10—C11 −177.6 (3) O3—C8—N1—C4 −3.4 (4)
C9—C10—C11—C12 −0.4 (4) C10—C8—N1—C4 176.4 (2)
C8—C10—C11—C12 177.4 (3) C5—C4—N1—C7 131.9 (3)
C10—C11—C12—C13 0.6 (5) C3—C4—N1—C7 −48.3 (4)
C11—C12—C13—C14 0.1 (5) C5—C4—N1—C8 −44.3 (3)
C10—C9—C14—C13 1.2 (4) C3—C4—N1—C8 135.5 (3)
C7—C9—C14—C13 −176.8 (3) O5—C22—N2—C21 178.5 (3)
C12—C13—C14—C9 −1.0 (4) C24—C22—N2—C21 −1.1 (3)
C20—C15—C16—C17 1.8 (4) O5—C22—N2—C18 1.6 (5)
O1—C15—C16—C17 −173.8 (3) C24—C22—N2—C18 −178.0 (3)
C15—C16—C17—C18 0.0 (5) O4—C21—N2—C22 −176.6 (3)
C16—C17—C18—C19 −1.8 (4) C23—C21—N2—C22 2.1 (3)
C16—C17—C18—N2 178.0 (3) O4—C21—N2—C18 0.3 (5)
C17—C18—C19—C20 2.0 (5) C23—C21—N2—C18 179.0 (3)
N2—C18—C19—C20 −177.8 (3) C17—C18—N2—C22 77.1 (4)
C16—C15—C20—C19 −1.7 (5) C19—C18—N2—C22 −103.1 (3)
O1—C15—C20—C19 173.8 (3) C17—C18—N2—C21 −99.4 (3)
C18—C19—C20—C15 −0.2 (5) C19—C18—N2—C21 80.4 (4)
O4—C21—C23—C24 176.3 (4) C2—C1—O1—C15 −144.7 (3)
N2—C21—C23—C24 −2.3 (3) C6—C1—O1—C15 39.6 (4)
O4—C21—C23—C28 −1.5 (6) C20—C15—O1—C1 71.4 (3)
N2—C21—C23—C28 179.9 (3) C16—C15—O1—C1 −113.0 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C11—H11···O5i 0.93 2.47 3.222 (4) 138
C19—H19···O5ii 0.93 2.56 3.298 (4) 136

Symmetry codes: (i) −x+2, y+1/2, −z+3/2; (ii) x+1/2, −y+1/2, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WN2220).

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/S1600536807057455/wn2220sup1.cif

e-64-00o77-sup1.cif (22.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807057455/wn2220Isup2.hkl

e-64-00o77-Isup2.hkl (143.6KB, hkl)

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


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