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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jul 19;64(Pt 8):o1537. doi: 10.1107/S1600536808022101

1,1,1,3,3,3-Hexafluoro-2,2-bis­[4-(4-nitro­phen­oxy)phen­yl]propane

H Nawaz a, Zareen Akhter a,*, Michael Bolte b, M S Butt a, Humaira M Siddiqi a
PMCID: PMC2962162  PMID: 21203242

Abstract

In the title compound, C27H16F6N2O6, the nitro groups are almost coplanar with the aromatic rings to which they are attached [dihedral angles = 3.5 (5) and 6.2 (3)°]. The dihedral angles between adjacent aromatic rings are 78.07 (8) and 71.11 (8)° for nitro­phen­yl/phenyl and 69.50 (8)° for phen­yl/phenyl. An inter­molecular C—H⋯π inter­action seems to be effective in the stabilization of the structure.

Related literature

For related literature, see: Liaw et al. (2005); Yang et al. (2003); Miyagawa et al. (2003); Leu et al. (2003); Zhou et al. (2001.graphic file with name e-64-o1537-scheme1.jpg

Experimental

Crystal data

  • C27H16F6N2O6

  • M r = 578.42

  • Monoclinic, Inline graphic

  • a = 25.523 (3) Å

  • b = 10.5530 (12) Å

  • c = 9.3869 (8) Å

  • β = 98.248 (8)°

  • V = 2502.2 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.14 mm−1

  • T = 173 (2) K

  • 0.23 × 0.10 × 0.10 mm

Data collection

  • Stoe IPDSII two-circle diffractometer

  • Absorption correction: none

  • 13020 measured reflections

  • 4653 independent reflections

  • 2651 reflections with I > 2σ(I)

  • R int = 0.076

Refinement

  • R[F 2 > 2σ(F 2)] = 0.044

  • wR(F 2) = 0.092

  • S = 0.91

  • 4653 reflections

  • 371 parameters

  • H-atom parameters constrained

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.21 e Å−3

Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808022101/bq2089sup1.cif

e-64-o1537-sup1.cif (24.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808022101/bq2089Isup2.hkl

e-64-o1537-Isup2.hkl (228KB, 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
C46—H46⋯Cg1i 0.95 3.04 3.710 129

Symmetry code: (i) Inline graphic. Cg1 is the centroid of the C31–C36 ring.

Acknowledgments

The authors are grateful to the Department of Chemistry, Quaid-I-Azam University, Islamabad, Pakistan, and to the Institute for Inorganic Chemistry, University of Frankfurt, Germany, for providing laboratory and analytical facilities.

supplementary crystallographic information

Comment

Aromatic polyimides have many useful properties, such as high glass transition temperature, excellent dimensional stability, low dielectric constant and outstanding thermal stability (Liaw et al. 2005). Polyimides also have many commercial applications but one of the problems with the polyimides is their poor solubility (Yang et al. 2003). Many efforts have been made to increase the solubility (Miyagawa et al. 2003) and processability of the polyimides. The common strategy that enhances the solubility is the introduction of flexible linkages, bulky substituents (Leu et al. 2003) and structurally unsymmetrical segment (Zhou et al. 2001) in to the polymer backbone. The present compound is the starting material for such types of polymers.

Geometric parameters of (I) are in the usual ranges. The nitro groups are almost coplanar with the aromatic rings to which they are attached [dihedral angles: 3.5 (5)128.52 and 6.2 (3)°], (Figure 1.). The dihedral angles between the adjacent aromatic rings are 78.07 (8)° and 71.11 (8)° for nitrophenyl/phenyl and 69.50 (8)° for phenyl/phenyl. The C46···H46-Cg1 intermolecular interaction seems to be effective in the stabilization of the structure. Cg1 is the center of the ring (C31-C36) at the symmetry of x, 1/2-y, 1/2+z (Table 1.)

Experimental

A mixture containing 2 g (5.94 mmol) of 4,4'-(hexafluoroisopropylidene)-diphenol, 2.25 g (11.88 mmol) of anhydrous potassium carbonate, and 1.87 g (11.88 mmoles) of p-nitrochlorobenzene, in 70 mL of DMF was heated at 120° C for 18 h in nitrogen atmosphere. After cooling to room temperature, the reaction mixture was poured into 500 mL of water to form precipitates and washed thoroughly with water and then collected by filtration. The crude product was recrystallized from ethanol. m.p.352 K.

Refinement

H atoms could be located by difference Fourier synthesis. They were refined with fixed individual displacement parameters [U(H) = 1.2 Ueq(C)] using a riding model with C—H = 0.95 Å.

Figures

Fig. 1.

Fig. 1.

Perspective view of the title compound with the atom numbering; displacement ellipsoids are at the 50% probability level.

Crystal data

C27H16F6N2O6 F000 = 1176
Mr = 578.42 Dx = 1.535 Mg m3
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 6504 reflections
a = 25.523 (3) Å θ = 3.5–25.6º
b = 10.5530 (12) Å µ = 0.14 mm1
c = 9.3869 (8) Å T = 173 (2) K
β = 98.248 (8)º Rod, colourless
V = 2502.2 (5) Å3 0.23 × 0.10 × 0.10 mm
Z = 4

Data collection

Stoe IPDSII two-circle diffractometer 2651 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.076
Monochromator: graphite θmax = 25.6º
T = 173(2) K θmin = 3.5º
ω scans h = −30→31
Absorption correction: none k = −12→12
13020 measured reflections l = −11→9
4653 independent reflections

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.044   w = 1/[σ2(Fo2) + (0.0358P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.092 (Δ/σ)max < 0.001
S = 0.91 Δρmax = 0.20 e Å3
4653 reflections Δρmin = −0.21 e Å3
371 parameters Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0055 (6)
Secondary atom site location: difference Fourier map

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
F1 0.22322 (6) 0.68466 (15) 0.12465 (17) 0.0501 (5)
F2 0.20394 (6) 0.68591 (13) 0.33963 (17) 0.0410 (4)
F3 0.28426 (6) 0.71700 (14) 0.30377 (18) 0.0506 (5)
F4 0.30099 (6) 0.34542 (16) 0.17262 (18) 0.0535 (5)
F5 0.25025 (6) 0.46271 (18) 0.02529 (16) 0.0551 (5)
F6 0.32280 (6) 0.54001 (17) 0.13798 (17) 0.0552 (5)
O1 0.36452 (7) 0.43650 (18) 0.8434 (2) 0.0482 (5)
O2 0.06515 (6) 0.19665 (15) 0.2107 (2) 0.0379 (5)
N1 0.50826 (10) 0.7761 (3) 1.1374 (3) 0.0511 (7)
O11 0.51204 (11) 0.8833 (2) 1.0897 (3) 0.0842 (9)
O12 0.53558 (8) 0.7378 (2) 1.2468 (2) 0.0641 (7)
N2 0.06342 (9) −0.2973 (2) 0.0006 (2) 0.0366 (5)
O21 0.09940 (8) −0.33014 (17) −0.0658 (2) 0.0467 (5)
O22 0.02828 (8) −0.36920 (18) 0.0283 (2) 0.0544 (6)
C1 0.25201 (9) 0.5041 (2) 0.2760 (2) 0.0282 (5)
C2 0.24075 (10) 0.6489 (2) 0.2604 (3) 0.0352 (6)
C3 0.28207 (10) 0.4635 (3) 0.1534 (3) 0.0414 (7)
C11 0.28502 (9) 0.4859 (2) 0.4265 (3) 0.0264 (5)
C12 0.25853 (9) 0.4963 (2) 0.5458 (3) 0.0285 (6)
H12 0.2216 0.5127 0.5325 0.034*
C13 0.28577 (10) 0.4830 (2) 0.6843 (3) 0.0340 (6)
H13 0.2676 0.4903 0.7655 0.041*
C14 0.33916 (10) 0.4592 (2) 0.7024 (3) 0.0358 (6)
C15 0.36642 (10) 0.4496 (3) 0.5880 (3) 0.0449 (7)
H15 0.4034 0.4337 0.6030 0.054*
C16 0.33941 (9) 0.4632 (3) 0.4487 (3) 0.0383 (7)
H16 0.3582 0.4570 0.3686 0.046*
C21 0.39889 (9) 0.5259 (2) 0.9095 (3) 0.0328 (6)
C22 0.40440 (10) 0.6473 (3) 0.8560 (3) 0.0379 (7)
H22 0.3842 0.6729 0.7678 0.045*
C23 0.43979 (10) 0.7308 (3) 0.9330 (3) 0.0400 (7)
H23 0.4439 0.8143 0.8986 0.048*
C24 0.46891 (10) 0.6905 (3) 1.0604 (3) 0.0353 (6)
C25 0.46318 (10) 0.5707 (3) 1.1147 (3) 0.0355 (6)
H25 0.4834 0.5455 1.2030 0.043*
C26 0.42775 (9) 0.4881 (3) 1.0393 (3) 0.0343 (6)
H26 0.4231 0.4056 1.0759 0.041*
C31 0.20057 (9) 0.4246 (2) 0.2604 (2) 0.0253 (5)
C32 0.15356 (9) 0.4636 (2) 0.1781 (3) 0.0287 (6)
H32 0.1520 0.5445 0.1332 0.034*
C33 0.10890 (9) 0.3865 (2) 0.1602 (3) 0.0312 (6)
H33 0.0770 0.4149 0.1049 0.037*
C34 0.11153 (9) 0.2691 (2) 0.2234 (3) 0.0301 (6)
C35 0.15786 (9) 0.2261 (2) 0.3063 (3) 0.0320 (6)
H35 0.1591 0.1449 0.3504 0.038*
C36 0.20206 (9) 0.3040 (2) 0.3230 (3) 0.0309 (6)
H36 0.2340 0.2750 0.3780 0.037*
C41 0.06640 (9) 0.0749 (2) 0.1551 (3) 0.0282 (6)
C42 0.02822 (9) −0.0074 (2) 0.1911 (3) 0.0305 (6)
H42 0.0035 0.0201 0.2513 0.037*
C43 0.02635 (9) −0.1297 (2) 0.1388 (3) 0.0323 (6)
H43 0.0005 −0.1878 0.1621 0.039*
C44 0.06299 (9) −0.1656 (2) 0.0517 (3) 0.0288 (6)
C45 0.10087 (9) −0.0837 (2) 0.0139 (3) 0.0311 (6)
H45 0.1255 −0.1112 −0.0464 0.037*
C46 0.10214 (9) 0.0389 (2) 0.0653 (3) 0.0316 (6)
H46 0.1273 0.0978 0.0393 0.038*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
F1 0.0590 (10) 0.0512 (10) 0.0374 (10) −0.0124 (8) −0.0025 (8) 0.0207 (8)
F2 0.0454 (9) 0.0307 (8) 0.0468 (10) 0.0004 (7) 0.0066 (7) −0.0023 (7)
F3 0.0459 (9) 0.0431 (9) 0.0595 (11) −0.0219 (8) −0.0034 (8) 0.0081 (8)
F4 0.0509 (10) 0.0638 (12) 0.0482 (11) 0.0104 (9) 0.0159 (8) −0.0167 (9)
F5 0.0504 (9) 0.0941 (13) 0.0215 (8) −0.0100 (9) 0.0076 (7) −0.0080 (9)
F6 0.0388 (9) 0.0910 (13) 0.0392 (9) −0.0180 (9) 0.0170 (7) −0.0004 (9)
O1 0.0504 (11) 0.0580 (13) 0.0309 (11) −0.0141 (10) −0.0124 (9) 0.0125 (9)
O2 0.0260 (9) 0.0301 (10) 0.0598 (13) −0.0036 (7) 0.0138 (8) −0.0111 (9)
N1 0.0596 (16) 0.0552 (17) 0.0381 (16) −0.0014 (13) 0.0055 (13) −0.0132 (13)
O11 0.128 (2) 0.0599 (16) 0.0584 (17) −0.0334 (15) −0.0091 (15) −0.0057 (14)
O12 0.0604 (14) 0.0735 (16) 0.0505 (14) 0.0013 (12) −0.0196 (12) −0.0135 (12)
N2 0.0397 (13) 0.0312 (13) 0.0348 (13) −0.0035 (11) −0.0083 (11) 0.0009 (10)
O21 0.0453 (11) 0.0416 (11) 0.0513 (13) 0.0043 (9) 0.0009 (10) −0.0124 (10)
O22 0.0651 (13) 0.0338 (11) 0.0642 (15) −0.0196 (10) 0.0084 (11) 0.0007 (10)
C1 0.0258 (11) 0.0381 (14) 0.0207 (13) −0.0041 (11) 0.0036 (9) −0.0011 (11)
C2 0.0346 (14) 0.0388 (16) 0.0317 (16) −0.0140 (12) 0.0027 (12) 0.0071 (13)
C3 0.0348 (14) 0.065 (2) 0.0256 (15) −0.0094 (14) 0.0080 (12) −0.0032 (14)
C11 0.0261 (12) 0.0291 (13) 0.0235 (13) −0.0040 (10) 0.0019 (10) −0.0018 (11)
C12 0.0246 (12) 0.0343 (14) 0.0264 (14) −0.0007 (11) 0.0030 (10) −0.0018 (12)
C13 0.0421 (14) 0.0374 (15) 0.0227 (14) −0.0072 (12) 0.0056 (11) −0.0009 (12)
C14 0.0368 (14) 0.0404 (16) 0.0272 (15) −0.0054 (12) −0.0058 (12) 0.0057 (12)
C15 0.0272 (13) 0.067 (2) 0.0388 (17) 0.0009 (13) −0.0022 (13) 0.0059 (15)
C16 0.0283 (13) 0.0540 (17) 0.0328 (15) −0.0025 (12) 0.0053 (11) 0.0000 (13)
C21 0.0257 (12) 0.0460 (16) 0.0258 (14) 0.0010 (12) 0.0008 (10) 0.0019 (13)
C22 0.0376 (14) 0.0480 (17) 0.0271 (15) 0.0060 (13) 0.0012 (11) 0.0040 (13)
C23 0.0468 (16) 0.0416 (16) 0.0324 (16) 0.0035 (13) 0.0087 (13) 0.0034 (13)
C24 0.0336 (14) 0.0450 (16) 0.0269 (15) 0.0042 (12) 0.0033 (11) −0.0077 (13)
C25 0.0328 (14) 0.0489 (17) 0.0239 (14) 0.0120 (12) 0.0012 (11) 0.0002 (13)
C26 0.0316 (13) 0.0447 (16) 0.0264 (14) 0.0088 (12) 0.0034 (11) 0.0035 (13)
C31 0.0277 (13) 0.0294 (13) 0.0195 (13) −0.0023 (10) 0.0058 (10) −0.0029 (11)
C32 0.0299 (13) 0.0282 (13) 0.0277 (14) 0.0004 (11) 0.0030 (10) 0.0022 (11)
C33 0.0246 (12) 0.0334 (15) 0.0347 (15) 0.0044 (11) 0.0011 (11) −0.0033 (12)
C34 0.0259 (12) 0.0273 (13) 0.0387 (15) −0.0022 (10) 0.0097 (11) −0.0089 (12)
C35 0.0339 (13) 0.0236 (13) 0.0382 (16) −0.0018 (11) 0.0043 (11) 0.0004 (12)
C36 0.0280 (13) 0.0319 (14) 0.0321 (15) 0.0030 (11) 0.0022 (11) −0.0012 (12)
C41 0.0246 (12) 0.0278 (14) 0.0312 (15) 0.0012 (10) 0.0003 (11) −0.0016 (11)
C42 0.0253 (12) 0.0380 (15) 0.0287 (14) −0.0012 (11) 0.0058 (10) 0.0022 (12)
C43 0.0286 (13) 0.0361 (15) 0.0312 (15) −0.0083 (11) 0.0012 (11) 0.0084 (12)
C44 0.0317 (13) 0.0250 (13) 0.0272 (14) −0.0004 (11) −0.0039 (11) 0.0026 (11)
C45 0.0279 (13) 0.0343 (15) 0.0318 (15) 0.0000 (11) 0.0070 (11) −0.0008 (12)
C46 0.0255 (12) 0.0312 (14) 0.0393 (16) −0.0060 (10) 0.0091 (11) 0.0009 (12)

Geometric parameters (Å, °)

F1—C2 1.342 (3) C21—C26 1.388 (3)
F2—C2 1.338 (3) C21—C22 1.391 (4)
F3—C2 1.336 (3) C22—C23 1.388 (4)
F4—C3 1.339 (3) C22—H22 0.9500
F5—C3 1.351 (3) C23—C24 1.381 (4)
F6—C3 1.340 (3) C23—H23 0.9500
O1—C21 1.374 (3) C24—C25 1.379 (4)
O1—C14 1.408 (3) C25—C26 1.376 (4)
O2—C41 1.389 (3) C25—H25 0.9500
O2—C34 1.400 (3) C26—H26 0.9500
N1—O12 1.224 (3) C31—C32 1.393 (3)
N1—O11 1.226 (3) C31—C36 1.400 (3)
N1—C24 1.463 (3) C32—C33 1.391 (3)
N2—O22 1.230 (3) C32—H32 0.9500
N2—O21 1.231 (3) C33—C34 1.371 (3)
N2—C44 1.471 (3) C33—H33 0.9500
C1—C3 1.533 (4) C34—C35 1.395 (3)
C1—C31 1.547 (3) C35—C36 1.387 (3)
C1—C11 1.550 (3) C35—H35 0.9500
C1—C2 1.557 (4) C36—H36 0.9500
C11—C12 1.393 (3) C41—C46 1.381 (3)
C11—C16 1.394 (3) C41—C42 1.383 (3)
C12—C13 1.391 (3) C42—C43 1.380 (3)
C12—H12 0.9500 C42—H42 0.9500
C13—C14 1.372 (4) C43—C44 1.380 (4)
C13—H13 0.9500 C43—H43 0.9500
C14—C15 1.365 (4) C44—C45 1.381 (3)
C15—C16 1.395 (4) C45—C46 1.380 (3)
C15—H15 0.9500 C45—H45 0.9500
C16—H16 0.9500 C46—H46 0.9500
C21—O1—C14 119.1 (2) C21—C22—H22 120.4
C41—O2—C34 118.21 (18) C24—C23—C22 119.0 (3)
O12—N1—O11 123.1 (3) C24—C23—H23 120.5
O12—N1—C24 118.6 (3) C22—C23—H23 120.5
O11—N1—C24 118.3 (3) C25—C24—C23 122.0 (2)
O22—N2—O21 123.6 (2) C25—C24—N1 119.0 (2)
O22—N2—C44 118.3 (2) C23—C24—N1 119.0 (3)
O21—N2—C44 118.1 (2) C26—C25—C24 119.2 (2)
C3—C1—C31 106.68 (19) C26—C25—H25 120.4
C3—C1—C11 112.6 (2) C24—C25—H25 120.4
C31—C1—C11 111.18 (19) C25—C26—C21 119.7 (2)
C3—C1—C2 108.0 (2) C25—C26—H26 120.1
C31—C1—C2 112.37 (19) C21—C26—H26 120.1
C11—C1—C2 106.06 (19) C32—C31—C36 118.1 (2)
F3—C2—F2 107.0 (2) C32—C31—C1 122.9 (2)
F3—C2—F1 106.70 (19) C36—C31—C1 118.8 (2)
F2—C2—F1 106.3 (2) C33—C32—C31 121.3 (2)
F3—C2—C1 111.4 (2) C33—C32—H32 119.3
F2—C2—C1 111.7 (2) C31—C32—H32 119.3
F1—C2—C1 113.4 (2) C34—C33—C32 119.2 (2)
F4—C3—F6 107.7 (2) C34—C33—H33 120.4
F4—C3—F5 105.8 (2) C32—C33—H33 120.4
F6—C3—F5 106.5 (2) C33—C34—C35 121.4 (2)
F4—C3—C1 111.7 (2) C33—C34—O2 117.9 (2)
F6—C3—C1 113.1 (2) C35—C34—O2 120.5 (2)
F5—C3—C1 111.6 (2) C36—C35—C34 118.7 (2)
C12—C11—C16 118.7 (2) C36—C35—H35 120.6
C12—C11—C1 117.4 (2) C34—C35—H35 120.6
C16—C11—C1 123.9 (2) C35—C36—C31 121.3 (2)
C13—C12—C11 120.5 (2) C35—C36—H36 119.4
C13—C12—H12 119.7 C31—C36—H36 119.4
C11—C12—H12 119.7 C46—C41—C42 121.8 (2)
C14—C13—C12 119.3 (3) C46—C41—O2 122.4 (2)
C14—C13—H13 120.4 C42—C41—O2 115.7 (2)
C12—C13—H13 120.4 C43—C42—C41 119.3 (2)
C15—C14—C13 121.7 (2) C43—C42—H42 120.3
C15—C14—O1 120.6 (2) C41—C42—H42 120.3
C13—C14—O1 117.5 (2) C42—C43—C44 118.4 (2)
C14—C15—C16 119.4 (2) C42—C43—H43 120.8
C14—C15—H15 120.3 C44—C43—H43 120.8
C16—C15—H15 120.3 C43—C44—C45 122.6 (2)
C11—C16—C15 120.4 (3) C43—C44—N2 119.4 (2)
C11—C16—H16 119.8 C45—C44—N2 118.0 (2)
C15—C16—H16 119.8 C46—C45—C44 118.7 (2)
O1—C21—C26 115.0 (2) C46—C45—H45 120.7
O1—C21—C22 124.1 (2) C44—C45—H45 120.7
C26—C21—C22 120.9 (2) C45—C46—C41 119.1 (2)
C23—C22—C21 119.2 (2) C45—C46—H46 120.4
C23—C22—H22 120.4 C41—C46—H46 120.4
C3—C1—C2—F3 −75.8 (3) O12—N1—C24—C25 1.2 (4)
C31—C1—C2—F3 166.8 (2) O11—N1—C24—C25 −178.3 (3)
C11—C1—C2—F3 45.1 (3) O12—N1—C24—C23 −176.7 (3)
C3—C1—C2—F2 164.62 (19) O11—N1—C24—C23 3.7 (4)
C31—C1—C2—F2 47.2 (3) C23—C24—C25—C26 0.6 (4)
C11—C1—C2—F2 −74.5 (2) N1—C24—C25—C26 −177.3 (2)
C3—C1—C2—F1 44.6 (3) C24—C25—C26—C21 0.8 (4)
C31—C1—C2—F1 −72.8 (3) O1—C21—C26—C25 −179.8 (2)
C11—C1—C2—F1 165.5 (2) C22—C21—C26—C25 −1.5 (4)
C31—C1—C3—F4 −69.4 (2) C3—C1—C31—C32 −89.6 (3)
C11—C1—C3—F4 52.8 (3) C11—C1—C31—C32 147.3 (2)
C2—C1—C3—F4 169.59 (19) C2—C1—C31—C32 28.6 (3)
C31—C1—C3—F6 168.9 (2) C3—C1—C31—C36 85.6 (3)
C11—C1—C3—F6 −68.9 (3) C11—C1—C31—C36 −37.5 (3)
C2—C1—C3—F6 47.9 (3) C2—C1—C31—C36 −156.2 (2)
C31—C1—C3—F5 48.8 (3) C36—C31—C32—C33 1.2 (4)
C11—C1—C3—F5 171.1 (2) C1—C31—C32—C33 176.4 (2)
C2—C1—C3—F5 −72.2 (3) C31—C32—C33—C34 −0.9 (4)
C3—C1—C11—C12 −168.0 (2) C32—C33—C34—C35 0.6 (4)
C31—C1—C11—C12 −48.3 (3) C32—C33—C34—O2 176.3 (2)
C2—C1—C11—C12 74.1 (3) C41—O2—C34—C33 125.7 (2)
C3—C1—C11—C16 13.8 (3) C41—O2—C34—C35 −58.6 (3)
C31—C1—C11—C16 133.5 (2) C33—C34—C35—C36 −0.7 (4)
C2—C1—C11—C16 −104.1 (3) O2—C34—C35—C36 −176.2 (2)
C16—C11—C12—C13 −0.7 (4) C34—C35—C36—C31 1.0 (4)
C1—C11—C12—C13 −179.0 (2) C32—C31—C36—C35 −1.2 (4)
C11—C12—C13—C14 −0.1 (4) C1—C31—C36—C35 −176.7 (2)
C12—C13—C14—C15 0.7 (4) C34—O2—C41—C46 −24.7 (3)
C12—C13—C14—O1 −175.2 (2) C34—O2—C41—C42 157.6 (2)
C21—O1—C14—C15 74.2 (3) C46—C41—C42—C43 1.5 (4)
C21—O1—C14—C13 −109.9 (3) O2—C41—C42—C43 179.2 (2)
C13—C14—C15—C16 −0.6 (4) C41—C42—C43—C44 0.0 (3)
O1—C14—C15—C16 175.2 (2) C42—C43—C44—C45 −0.8 (4)
C12—C11—C16—C15 0.9 (4) C42—C43—C44—N2 177.0 (2)
C1—C11—C16—C15 179.1 (2) O22—N2—C44—C43 5.5 (3)
C14—C15—C16—C11 −0.3 (4) O21—N2—C44—C43 −173.5 (2)
C14—O1—C21—C26 −171.1 (2) O22—N2—C44—C45 −176.7 (2)
C14—O1—C21—C22 10.6 (4) O21—N2—C44—C45 4.4 (3)
O1—C21—C22—C23 179.0 (2) C43—C44—C45—C46 0.1 (4)
C26—C21—C22—C23 0.8 (4) N2—C44—C45—C46 −177.7 (2)
C21—C22—C23—C24 0.5 (4) C44—C45—C46—C41 1.4 (3)
C22—C23—C24—C25 −1.2 (4) C42—C41—C46—C45 −2.2 (4)
C22—C23—C24—N1 176.7 (2) O2—C41—C46—C45 −179.8 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C46—H46···Cg1i 0.95 3.04 3.710 129

Symmetry codes: (i) x, −y+1/2, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BQ2089).

References

  1. Leu, C. M., Chang, Y. T. & Wei, K. H. (2003). Chem Mater 15, 3721–3727.
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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/S1600536808022101/bq2089sup1.cif

e-64-o1537-sup1.cif (24.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808022101/bq2089Isup2.hkl

e-64-o1537-Isup2.hkl (228KB, hkl)

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


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