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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Nov 25;67(Pt 12):o3429–o3430. doi: 10.1107/S1600536811048768

N 2,N 2,N 6,N 6-Tetra­kis(2,3,4,5,6-penta­fluoro­benzo­yl)pyridine-2,6-diamine

Arto Valkonen a,*, Erkki Kolehmainen a, Borys Ośmiałowski b
PMCID: PMC3239063  PMID: 22199911

Abstract

The title compound, C33H3F20N3O4, is a highly fluorinated organic imide that was isolated as an unexpected product from the reaction of 2,6-diamino­pyridine with 2,3,4,5,6-penta­fluoro­benzoyl chloride in a 1:2 molar ratio. The mol­ecule is located on a twofold axis and one of its symmetry-independent 2,3,4,5,6-penta­fluoro­benzoyl groups is disordered over two sets of sites, the occupancy of the major component being 0.773 (3). In the major component, the dihedral angle between the perfluoro­phenyl groups is 63.64 (10)°, and these groups form dihedral angles of 67.14 (7) and 21.1 (2)° with the pyridine core. Short inter­molecular C—H⋯O and C—H⋯N contacts are found in the crystal structure.

Related literature

For preparation of 2-acyl­amino­pyridines and their structures, see: Ośmiałowski et al. (2010a ,b ). For related structures, see: Kovalevsky et al. (1999).graphic file with name e-67-o3429-scheme1.jpg

Experimental

Crystal data

  • C33H3F20N3O4

  • M r = 885.38

  • Monoclinic, Inline graphic

  • a = 21.2370 (5) Å

  • b = 6.3940 (1) Å

  • c = 23.1045 (5) Å

  • β = 100.585 (1)°

  • V = 3083.96 (11) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.21 mm−1

  • T = 123 K

  • 0.30 × 0.18 × 0.16 mm

Data collection

  • Bruker–Nonius KappaCCD with an APEXII detector diffractometer

  • 7138 measured reflections

  • 3785 independent reflections

  • 2526 reflections with I > 2σ(I)

  • R int = 0.039

Refinement

  • R[F 2 > 2σ(F 2)] = 0.057

  • wR(F 2) = 0.133

  • S = 1.05

  • 3785 reflections

  • 366 parameters

  • 97 restraints

  • H-atom parameters constrained

  • Δρmax = 0.35 e Å−3

  • Δρmin = −0.42 e Å−3

Data collection: COLLECT (Bruker, 2008); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN; program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811048768/gk2434sup1.cif

e-67-o3429-sup1.cif (33.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811048768/gk2434Isup2.hkl

e-67-o3429-Isup2.hkl (181.9KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811048768/gk2434Isup3.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⋯N1i 0.95 2.67 3.621 (5) 180
C3—H3⋯O1i 0.95 2.52 3.318 (3) 141

Symmetry code: (i) Inline graphic.

Acknowledgments

Academy Professor Kari Rissanen and the Academy of Finland (project No. 212588) are thanked for financial support to AV. The Polish Ministry of Science and Higher Education (grant No. N N204 174138 to BO) is also gratefully acknowledged.

supplementary crystallographic information

Comment

The title compound was accidentally obtained by reaction of 2,6-diaminopyridine with two equivalents of 2,3,4,5,6-pentafluorobenzoyl chloride, while the preparation of N,N'-bis(pentafluorobenzoyl)-2,6-diaminopyridine was attempted. The reaction was carried out analogously to our previously reported preparations of 2-acylaminopyridines (Ośmiałowski et al., 2010a). Previously we have structurally characterized two related secondary amides (Ośmiałowski et al., 2010b). This title imide has not been previously reported in the literature. The crystal structure of closely related imide, N,N'-(pyridine-2,6-diyl)-bis(naphthalenedicarboximide), has been reported (Kovalevsky et al., 1999).

In the crystal molecules are located on a twofold rotation axis and one of the symmetry independent perfluorobenzoyl group is disordered over two sets of sites with different occupancies (Fig.1). The perfluorophenyl groups are twisted out of the pyridine core by 67.14 (7) and 21.1 (2) ° in the major component whereas in the minor component these angles are 67.14 (7) and 63.4 (4)°. Furthermore, the dihedral angle between perfluorophenyl - group planes is 63.64 (10) ° [the minor component 67.9 (4) °]. Mercury (Macrae et al., 2008) helped us to find a motif along [0-10] direction (Fig. 2), where the molecule is connected to the translation related one by two C—H···O contacts (Table 1). Between these molecules there is also one rather long but linear C—H···N contact. A few F···CAr, F···F and F···O type contacts were found, which are only slightly shorter than the sum of van der Waals radii.

Experimental

2,3,4,5,6-Pentafluorobenzoyl chloride (2.28 g, 10 mmol) was added dropwise to a magnetically stirred solution of 2,6-diaminopyridine (0.54 g, 5 mmol) and triethylamine (1 ml) in dry methylene chloride (6 ml) at 0 °C. Subsequently the reaction mixture was refluxed for 4 h and the solution was treated with water and extracted with CH2Cl2. The organic solvent of the extract was evaporated under reduced pressure and the product recrystallized from hexane/ethyl acetate (10:1) mixture. 1H NMR (CDCl3): δ (p.p.m.) = 8.00 (t, 1H, H4), 7.45 (d, 2H, H3). Single crystals suitable for X-ray diffraction were obtained by very slow evaporation of analytical sample from NMR-tube, where CDCl3 was used as a solvent.

Refinement

All H atoms were visible in electron density maps, but were calculated at their idealized positions and allowed to ride on their parent atoms at C—H distances of 0.95 Å with Uiso(H) of 1.2 times Ueq(C). A large number of restraints was needed to rationalize the disorder in perfluorobenzoyl group. FLAT (2 restraints, s=0.1) was applied to amide groups of both components to make them more planar. SADI (3 restraints, s=0.02) was applied for amide groups of both components to equalize the bond distances. DELU (2 restraints, s1=s2=0.01) was applied for one C—C and one C—F bond of the major component to equalize the anisotropic displacement parameters. SIMU (84 restraints, s=0.01, st=0.02, dmax=1.7) was applied to carbons of the disordered perfluorophenyl ring and carbonyl group of both components to equalize the anisotropic displacement parameters. ISOR (6 restraints, s=0.01, st=0.02) was applied to carbonyl oxygen atom of the minor component to prevent the atom to appear as non-positive definite.

Figures

Fig. 1.

Fig. 1.

The structures of the major (top) and the minor (bottom) components of the disordered title molecule showing the atom-labeling scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are represented by circles of arbitrary size.

Fig. 2.

Fig. 2.

The short C—H···O/N contacts (blue dashed lines) organizing the molecules in the [0 1 0] direction. The minor component of disordered part of the molecule was removed for clarity.

Crystal data

C33H3F20N3O4 F(000) = 1736
Mr = 885.38 Dx = 1.907 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yc Cell parameters from 4030 reflections
a = 21.2370 (5) Å θ = 0.4–28.3°
b = 6.3940 (1) Å µ = 0.21 mm1
c = 23.1045 (5) Å T = 123 K
β = 100.585 (1)° Block, colourless
V = 3083.96 (11) Å3 0.30 × 0.18 × 0.16 mm
Z = 4

Data collection

Bruker–Nonius KappaCCD with an APEXII detector diffractometer 2526 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.039
graphite θmax = 28.2°, θmin = 1.8°
Detector resolution: 9 pixels mm-1 h = −27→28
φ and ω scans k = −8→8
7138 measured reflections l = −30→30
3785 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)] = 0.057 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.133 H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0381P)2 + 7.2159P] where P = (Fo2 + 2Fc2)/3
3785 reflections (Δ/σ)max < 0.001
366 parameters Δρmax = 0.35 e Å3
97 restraints Δρmin = −0.42 e Å3

Special details

Experimental. 13C NMR (CDCl3): δ (ppm) = 159.4, 149.1, 144.5, 142.4, 141.7, 138.7, 136.6, 123.8, 110.5.
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 Occ. (<1)
F1 0.86727 (7) 0.9378 (2) 0.69841 (7) 0.0376 (4)
F2 0.78577 (10) 0.8370 (3) 0.59909 (7) 0.0616 (5)
F3 0.72661 (9) 0.4583 (3) 0.58930 (7) 0.0579 (5)
F4 0.75118 (6) 0.1782 (2) 0.67885 (7) 0.0362 (4)
F5 0.82680 (7) 0.2875 (2) 0.78079 (6) 0.0345 (4)
O1 0.87489 (9) 0.8475 (3) 0.82339 (8) 0.0380 (4)
N7 0.93905 (9) 0.5589 (3) 0.82488 (9) 0.0330 (5)
N1 1.0000 0.5463 (4) 0.7500 0.0278 (6)
C2 0.97130 (10) 0.4368 (4) 0.78664 (11) 0.0303 (5)
C3 0.97017 (12) 0.2207 (4) 0.78901 (14) 0.0392 (7)
H3 0.9496 0.1495 0.8165 0.047*
C4 1.0000 0.1126 (6) 0.7500 0.0450 (11)
H4 1.0000 −0.0360 0.7500 0.054*
C8 0.88798 (11) 0.6875 (4) 0.80002 (11) 0.0295 (5)
C9 0.84960 (10) 0.6158 (4) 0.74248 (10) 0.0253 (5)
C10 0.83779 (11) 0.7515 (4) 0.69504 (11) 0.0293 (5)
C11 0.79688 (13) 0.6999 (4) 0.64361 (11) 0.0373 (6)
C12 0.76727 (13) 0.5075 (4) 0.63878 (11) 0.0368 (6)
C13 0.77919 (11) 0.3668 (4) 0.68450 (11) 0.0294 (5)
C14 0.81941 (10) 0.4222 (4) 0.73576 (10) 0.0257 (5)
O2 1.02137 (19) 0.5421 (8) 0.9007 (2) 0.0851 (16) 0.773 (2)
C15 0.9663 (3) 0.5901 (8) 0.8850 (2) 0.0484 (16) 0.773 (2)
F6 0.96821 (11) 0.9929 (4) 0.93716 (10) 0.0545 (6) 0.773 (2)
F7 0.90327 (13) 1.0815 (4) 1.02541 (11) 0.0641 (8) 0.773 (2)
F8 0.82644 (14) 0.7899 (4) 1.06022 (10) 0.0548 (7) 0.773 (2)
F9 0.81043 (14) 0.4137 (4) 1.00624 (12) 0.0565 (7) 0.773 (2)
F10 0.87435 (13) 0.3237 (4) 0.91753 (12) 0.0533 (7) 0.773 (2)
C16 0.92394 (13) 0.6546 (4) 0.92708 (10) 0.0413 (10) 0.773 (2)
C17 0.93101 (11) 0.8490 (4) 0.95442 (11) 0.0429 (9) 0.773 (2)
C18 0.89756 (12) 0.8949 (3) 0.99922 (10) 0.0451 (9) 0.773 (2)
C19 0.85705 (12) 0.7464 (4) 1.01668 (10) 0.0432 (9) 0.773 (2)
C20 0.84999 (14) 0.5520 (4) 0.98934 (13) 0.0407 (11) 0.773 (2)
C21 0.88343 (15) 0.5061 (3) 0.94454 (13) 0.0381 (12) 0.773 (2)
O2B 1.0322 (5) 0.4514 (16) 0.8935 (5) 0.041 (3) 0.227 (2)
C15B 0.9785 (6) 0.524 (2) 0.8821 (5) 0.027 (4) 0.227 (2)
F6B 1.0454 (3) 0.7631 (12) 0.9763 (3) 0.048 (2) 0.227 (2)
F7B 0.9953 (4) 0.8597 (13) 1.0711 (3) 0.060 (2) 0.227 (2)
F8B 0.8734 (5) 0.7549 (14) 1.0761 (3) 0.059 (2) 0.227 (2)
F9B 0.8023 (5) 0.5329 (19) 0.9872 (4) 0.058 (3) 0.227 (2)
F10B 0.8522 (4) 0.4215 (13) 0.8935 (3) 0.0397 (18) 0.227 (2)
C16B 0.9465 (4) 0.6015 (14) 0.9305 (3) 0.029 (3) 0.227 (2)
C17B 0.9844 (3) 0.7046 (14) 0.9773 (3) 0.040 (2) 0.227 (2)
C18B 0.9591 (4) 0.7582 (14) 1.0267 (3) 0.043 (3) 0.227 (2)
C19B 0.8959 (4) 0.7086 (15) 1.0293 (3) 0.042 (3) 0.227 (2)
C20B 0.8581 (3) 0.6055 (17) 0.9825 (4) 0.034 (3) 0.227 (2)
C21B 0.8833 (4) 0.5519 (16) 0.9331 (4) 0.025 (3) 0.227 (2)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
F1 0.0398 (8) 0.0247 (7) 0.0498 (9) −0.0086 (6) 0.0121 (7) 0.0033 (7)
F2 0.0912 (14) 0.0489 (11) 0.0402 (9) −0.0188 (10) 0.0006 (9) 0.0136 (8)
F3 0.0692 (12) 0.0568 (12) 0.0403 (9) −0.0210 (10) −0.0093 (8) −0.0015 (9)
F4 0.0296 (7) 0.0285 (8) 0.0512 (9) −0.0101 (6) 0.0095 (6) −0.0078 (7)
F5 0.0346 (7) 0.0277 (8) 0.0409 (8) −0.0072 (6) 0.0062 (6) 0.0061 (6)
O1 0.0464 (11) 0.0271 (9) 0.0434 (10) −0.0083 (8) 0.0159 (8) −0.0102 (8)
N7 0.0269 (10) 0.0343 (12) 0.0373 (11) −0.0054 (9) 0.0049 (9) −0.0024 (10)
N1 0.0174 (12) 0.0214 (14) 0.0433 (17) 0.000 0.0021 (12) 0.000
C2 0.0179 (10) 0.0263 (12) 0.0447 (14) −0.0012 (10) 0.0000 (10) 0.0012 (11)
C3 0.0236 (12) 0.0271 (13) 0.0656 (19) −0.0033 (10) 0.0042 (12) 0.0084 (13)
C4 0.0240 (17) 0.0192 (17) 0.089 (3) 0.000 0.0020 (19) 0.000
C8 0.0276 (11) 0.0245 (12) 0.0386 (13) −0.0081 (10) 0.0118 (10) −0.0014 (11)
C9 0.0219 (10) 0.0237 (11) 0.0331 (12) −0.0003 (9) 0.0118 (9) −0.0031 (10)
C10 0.0304 (12) 0.0201 (11) 0.0400 (14) −0.0056 (10) 0.0140 (11) −0.0031 (11)
C11 0.0457 (15) 0.0356 (15) 0.0319 (13) −0.0049 (12) 0.0105 (11) 0.0059 (12)
C12 0.0383 (14) 0.0381 (15) 0.0329 (13) −0.0081 (12) 0.0033 (11) −0.0051 (12)
C13 0.0256 (11) 0.0241 (12) 0.0408 (14) −0.0059 (10) 0.0121 (10) −0.0057 (11)
C14 0.0228 (10) 0.0230 (12) 0.0330 (12) 0.0016 (9) 0.0095 (9) −0.0003 (10)
O2 0.040 (2) 0.106 (4) 0.094 (3) 0.032 (2) −0.0279 (18) −0.061 (3)
C15 0.035 (2) 0.041 (3) 0.062 (3) 0.009 (2) −0.011 (2) −0.026 (2)
F6 0.0586 (14) 0.0444 (14) 0.0607 (15) −0.0048 (12) 0.0116 (12) −0.0191 (12)
F7 0.0776 (17) 0.0436 (14) 0.0734 (17) −0.0001 (13) 0.0204 (13) −0.0319 (13)
F8 0.0691 (17) 0.0515 (15) 0.0451 (13) 0.0136 (13) 0.0142 (12) −0.0149 (11)
F9 0.0761 (18) 0.0438 (16) 0.0508 (16) 0.0007 (15) 0.0151 (14) −0.0041 (13)
F10 0.0680 (17) 0.0360 (14) 0.0561 (16) 0.0013 (12) 0.0117 (13) −0.0186 (12)
C16 0.038 (2) 0.036 (2) 0.043 (2) 0.0126 (18) −0.0102 (16) −0.0140 (17)
C17 0.0409 (18) 0.0379 (19) 0.045 (2) 0.0075 (16) −0.0048 (16) −0.0116 (17)
C18 0.050 (2) 0.0365 (19) 0.044 (2) 0.0138 (17) −0.0044 (16) −0.0166 (17)
C19 0.047 (2) 0.044 (2) 0.0341 (18) 0.0151 (18) −0.0019 (16) −0.0082 (17)
C20 0.055 (3) 0.029 (2) 0.033 (2) 0.0114 (19) −0.006 (2) −0.0009 (18)
C21 0.048 (2) 0.023 (2) 0.037 (2) 0.0125 (17) −0.0080 (18) −0.0023 (18)
O2B 0.040 (5) 0.030 (5) 0.044 (5) 0.004 (4) −0.016 (4) 0.017 (4)
C15B 0.030 (8) 0.027 (8) 0.024 (6) −0.005 (6) 0.005 (5) 0.009 (6)
F6B 0.048 (4) 0.050 (5) 0.040 (4) −0.003 (4) −0.007 (3) 0.011 (4)
F7B 0.083 (6) 0.049 (5) 0.038 (4) 0.001 (5) −0.012 (4) −0.003 (4)
F8B 0.077 (6) 0.065 (6) 0.038 (4) 0.022 (5) 0.020 (4) −0.007 (4)
F9B 0.067 (6) 0.076 (7) 0.036 (5) −0.012 (6) 0.018 (4) −0.005 (5)
F10B 0.055 (5) 0.038 (4) 0.025 (3) −0.013 (4) 0.004 (3) −0.006 (3)
C16B 0.042 (6) 0.023 (5) 0.020 (4) 0.001 (5) 0.002 (4) 0.000 (4)
C17B 0.053 (6) 0.031 (5) 0.032 (5) −0.001 (5) 0.000 (4) 0.003 (4)
C18B 0.060 (6) 0.039 (5) 0.027 (5) 0.007 (5) −0.001 (5) −0.002 (4)
C19B 0.059 (6) 0.045 (6) 0.024 (5) 0.006 (5) 0.015 (5) −0.001 (4)
C20B 0.046 (6) 0.021 (5) 0.037 (5) 0.005 (5) 0.009 (5) 0.014 (5)
C21B 0.044 (6) 0.009 (4) 0.020 (5) 0.003 (4) 0.001 (4) 0.002 (4)

Geometric parameters (Å, °)

F1—C10 1.341 (3) C15—C16 1.498 (6)
F2—C11 1.339 (3) F6—C17 1.321 (3)
F3—C12 1.338 (3) F7—C18 1.333 (3)
F4—C13 1.340 (3) F8—C19 1.324 (3)
F5—C14 1.338 (3) F9—C20 1.327 (4)
O1—C8 1.213 (3) F10—C21 1.320 (3)
N7—C8 1.398 (3) C16—C17 1.3900
N7—C15 1.417 (6) C16—C21 1.3900
N7—C2 1.443 (3) C17—C18 1.3900
N7—C15B 1.446 (12) C18—C19 1.3900
N1—C2i 1.330 (3) C19—C20 1.3900
N1—C2 1.330 (3) C20—C21 1.3900
C2—C3 1.383 (4) O2B—C15B 1.215 (14)
C3—C4 1.379 (3) C15B—C16B 1.497 (13)
C3—H3 0.9500 F6B—C17B 1.353 (9)
C4—C3i 1.379 (3) F7B—C18B 1.332 (10)
C4—H4 0.9500 F8B—C19B 1.294 (9)
C8—C9 1.498 (3) F9B—C20B 1.294 (12)
C9—C10 1.384 (3) F10B—C21B 1.321 (9)
C9—C14 1.389 (3) C16B—C17B 1.3900
C10—C11 1.377 (4) C16B—C21B 1.3900
C11—C12 1.377 (4) C17B—C18B 1.3900
C12—C13 1.375 (4) C18B—C19B 1.3900
C13—C14 1.374 (3) C19B—C20B 1.3900
O2—C15 1.200 (6) C20B—C21B 1.3900
C8—N7—C15 117.8 (3) C17—C16—C21 120.0
C8—N7—C2 119.1 (2) C17—C16—C15 120.9 (3)
C15—N7—C2 121.5 (3) C21—C16—C15 118.5 (3)
C8—N7—C15B 138.0 (6) F6—C17—C16 120.4 (2)
C2—N7—C15B 102.4 (6) F6—C17—C18 119.6 (2)
C2i—N1—C2 116.5 (3) C16—C17—C18 120.0
N1—C2—C3 124.4 (3) F7—C18—C19 119.3 (2)
N1—C2—N7 115.5 (2) F7—C18—C17 120.7 (2)
C3—C2—N7 120.2 (2) C19—C18—C17 120.0
C4—C3—C2 117.5 (3) F8—C19—C18 119.6 (2)
C4—C3—H3 121.3 F8—C19—C20 120.4 (2)
C2—C3—H3 121.3 C18—C19—C20 120.0
C3—C4—C3i 119.8 (4) F9—C20—C21 121.1 (2)
C3—C4—H4 120.1 F9—C20—C19 118.9 (2)
C3i—C4—H4 120.1 C21—C20—C19 120.0
O1—C8—N7 122.5 (2) F10—C21—C20 119.2 (2)
O1—C8—C9 121.4 (2) F10—C21—C16 120.7 (2)
N7—C8—C9 116.1 (2) C20—C21—C16 120.0
C10—C9—C14 117.2 (2) O2B—C15B—N7 128.4 (11)
C10—C9—C8 120.1 (2) O2B—C15B—C16B 120.1 (11)
C14—C9—C8 122.4 (2) N7—C15B—C16B 111.4 (9)
F1—C10—C11 118.5 (2) C17B—C16B—C21B 120.0
F1—C10—C9 119.7 (2) C17B—C16B—C15B 117.5 (7)
C11—C10—C9 121.8 (2) C21B—C16B—C15B 122.0 (7)
F2—C11—C12 120.6 (2) F6B—C17B—C18B 117.5 (6)
F2—C11—C10 120.0 (2) F6B—C17B—C16B 122.5 (6)
C12—C11—C10 119.4 (2) C18B—C17B—C16B 120.0
F3—C12—C13 120.1 (2) F7B—C18B—C17B 119.8 (7)
F3—C12—C11 119.5 (2) F7B—C18B—C19B 120.2 (7)
C13—C12—C11 120.4 (2) C17B—C18B—C19B 120.0
F4—C13—C14 120.7 (2) F8B—C19B—C20B 120.6 (8)
F4—C13—C12 119.9 (2) F8B—C19B—C18B 119.4 (8)
C14—C13—C12 119.4 (2) C20B—C19B—C18B 120.0
F5—C14—C13 118.0 (2) F9B—C20B—C19B 120.8 (8)
F5—C14—C9 120.1 (2) F9B—C20B—C21B 118.5 (8)
C13—C14—C9 121.8 (2) C19B—C20B—C21B 120.0
O2—C15—N7 117.4 (5) F10B—C21B—C20B 120.3 (7)
O2—C15—C16 122.8 (5) F10B—C21B—C16B 118.6 (7)
N7—C15—C16 119.3 (4) C20B—C21B—C16B 120.0
C2i—N1—C2—C3 0.57 (19) C21—C16—C17—C18 0.0
C2i—N1—C2—N7 −178.4 (2) C15—C16—C17—C18 −171.1 (3)
C8—N7—C2—N1 62.2 (3) F6—C17—C18—F7 −0.9 (3)
C15—N7—C2—N1 −103.0 (4) C16—C17—C18—F7 −179.2 (3)
C15B—N7—C2—N1 −111.0 (6) F6—C17—C18—C19 178.4 (3)
C8—N7—C2—C3 −116.9 (3) C16—C17—C18—C19 0.0
C15—N7—C2—C3 78.0 (4) F7—C18—C19—F8 −2.2 (3)
C15B—N7—C2—C3 70.0 (6) C17—C18—C19—F8 178.6 (3)
N1—C2—C3—C4 −1.1 (4) F7—C18—C19—C20 179.3 (3)
N7—C2—C3—C4 177.85 (18) C17—C18—C19—C20 0.0
C2—C3—C4—C3i 0.50 (17) F8—C19—C20—F9 2.3 (3)
C15—N7—C8—O1 15.2 (4) C18—C19—C20—F9 −179.1 (3)
C2—N7—C8—O1 −150.5 (2) F8—C19—C20—C21 −178.6 (3)
C15B—N7—C8—O1 19.5 (9) C18—C19—C20—C21 0.0
C15—N7—C8—C9 −164.5 (3) F9—C20—C21—F10 1.7 (3)
C2—N7—C8—C9 29.8 (3) C19—C20—C21—F10 −177.5 (3)
C15B—N7—C8—C9 −160.2 (8) F9—C20—C21—C16 179.1 (3)
O1—C8—C9—C10 51.4 (3) C19—C20—C21—C16 0.0
N7—C8—C9—C10 −128.9 (2) C17—C16—C21—F10 177.4 (3)
O1—C8—C9—C14 −122.1 (3) C15—C16—C21—F10 −11.2 (4)
N7—C8—C9—C14 57.6 (3) C17—C16—C21—C20 0.0
C14—C9—C10—F1 −177.86 (19) C15—C16—C21—C20 171.3 (3)
C8—C9—C10—F1 8.3 (3) C8—N7—C15B—O2B −155.9 (9)
C14—C9—C10—C11 1.3 (4) C2—N7—C15B—O2B 15.1 (14)
C8—C9—C10—C11 −172.6 (2) C8—N7—C15B—C16B 20.5 (14)
F1—C10—C11—F2 −2.1 (4) C2—N7—C15B—C16B −168.5 (7)
C9—C10—C11—F2 178.8 (2) O2B—C15B—C16B—C17B 37.7 (14)
F1—C10—C11—C12 178.5 (2) N7—C15B—C16B—C17B −139.0 (8)
C9—C10—C11—C12 −0.6 (4) O2B—C15B—C16B—C21B −134.5 (10)
F2—C11—C12—F3 −0.6 (4) N7—C15B—C16B—C21B 48.8 (11)
C10—C11—C12—F3 178.8 (3) C21B—C16B—C17B—F6B −177.6 (9)
F2—C11—C12—C13 179.6 (2) C15B—C16B—C17B—F6B 10.0 (10)
C10—C11—C12—C13 −1.1 (4) C21B—C16B—C17B—C18B 0.0
F3—C12—C13—F4 1.6 (4) C15B—C16B—C17B—C18B −172.3 (9)
C11—C12—C13—F4 −178.6 (2) F6B—C17B—C18B—F7B −1.2 (9)
F3—C12—C13—C14 −177.9 (2) C16B—C17B—C18B—F7B −179.0 (9)
C11—C12—C13—C14 2.0 (4) F6B—C17B—C18B—C19B 177.8 (9)
F4—C13—C14—F5 −3.7 (3) C16B—C17B—C18B—C19B 0.0
C12—C13—C14—F5 175.7 (2) F7B—C18B—C19B—F8B −2.6 (11)
F4—C13—C14—C9 179.26 (19) C17B—C18B—C19B—F8B 178.4 (10)
C12—C13—C14—C9 −1.3 (4) F7B—C18B—C19B—C20B 179.0 (9)
C10—C9—C14—F5 −177.3 (2) C17B—C18B—C19B—C20B 0.0
C8—C9—C14—F5 −3.6 (3) F8B—C19B—C20B—F9B −7.9 (12)
C10—C9—C14—C13 −0.3 (3) C18B—C19B—C20B—F9B 170.5 (12)
C8—C9—C14—C13 173.4 (2) F8B—C19B—C20B—C21B −178.4 (10)
C8—N7—C15—O2 −153.1 (5) C18B—C19B—C20B—C21B 0.0
C2—N7—C15—O2 12.2 (7) F9B—C20B—C21B—F10B −3.3 (10)
C8—N7—C15—C16 34.5 (6) C19B—C20B—C21B—F10B 167.5 (10)
C2—N7—C15—C16 −160.2 (3) F9B—C20B—C21B—C16B −170.7 (11)
O2—C15—C16—C17 73.5 (6) C19B—C20B—C21B—C16B 0.0
N7—C15—C16—C17 −114.5 (4) C17B—C16B—C21B—F10B −167.7 (10)
O2—C15—C16—C21 −97.7 (6) C15B—C16B—C21B—F10B 4.3 (11)
N7—C15—C16—C21 74.2 (5) C17B—C16B—C21B—C20B 0.0
C21—C16—C17—F6 −178.4 (3) C15B—C16B—C21B—C20B 172.0 (9)
C15—C16—C17—F6 10.5 (4)

Symmetry codes: (i) −x+2, y, −z+3/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C4—H4···N1ii 0.95 2.67 3.621 (5) 180
C3—H3···O1ii 0.95 2.52 3.318 (3) 141

Symmetry codes: (ii) x, y−1, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: GK2434).

References

  1. Bruker (2008). COLLECT Bruker AXS, Delft, The Netherlands.
  2. Burla, M. C., Caliandro, R., Camalli, M., Carrozzini, B., Cascarano, G. L., De Caro, L., Giacovazzo, C., Polidori, G. & Spagna, R. (2005). J. Appl. Cryst. 38, 381–388.
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  6. Ośmiałowski, B., Kolehmainen, E., Dobosz, R., Gawinecki, R., Kauppinen, R., Valkonen, A., Koivukorpi, J. & Rissanen, K. (2010a). J. Phys. Chem. A, 114, 10421–10426. [DOI] [PubMed]
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  8. Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press.
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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) global, I. DOI: 10.1107/S1600536811048768/gk2434sup1.cif

e-67-o3429-sup1.cif (33.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811048768/gk2434Isup2.hkl

e-67-o3429-Isup2.hkl (181.9KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811048768/gk2434Isup3.cml

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


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