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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 May 15;69(Pt 6):o882. doi: 10.1107/S1600536813012336

4-(Adamantan-1-yl)-2-(4-fluoro­phen­yl)quinoline

Zuzana Kozubková a, Eva Babjaková a, Peter Bartoš b, Robert Vícha a,*
PMCID: PMC3685039  PMID: 23795058

Abstract

In the mol­ecule of the title compound, C25H24FN, the dihedral angle between the best planes of the quinoline fragment (rings A and B) and the benzene ring (C) is 9.51 (4)°. In the crystal, mol­ecules are linked into centrosymmetric dimers via pairs of weak C—H⋯F inter­actions. The mol­ecules are stacked into chains along the a axis by weak off-set π–π inter­actions between the A and C rings of translation-related mol­ecules with a centroid–centroid distance of 3.6440 (2) Å.

Related literature  

For the preparation and spectroscopic properties of the title compound, see: Kozubková et al. (2012). For related structures, see: Kozubková et al. (2012); Prabhuswamy et al. (2012). For the biological activity of related compounds, see: Nayyar et al. (2009).graphic file with name e-69-0o882-scheme1.jpg

Experimental  

Crystal data  

  • C25H24FN

  • M r = 357.45

  • Triclinic, Inline graphic

  • a = 6.4604 (3) Å

  • b = 10.9964 (4) Å

  • c = 12.9074 (5) Å

  • α = 93.205 (3)°

  • β = 96.446 (3)°

  • γ = 100.507 (3)°

  • V = 893.14 (6) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 120 K

  • 0.60 × 0.40 × 0.20 mm

Data collection  

  • Oxford Diffraction Xcalibur diffractometer

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) T min = 0.971, T max = 1.000

  • 9490 measured reflections

  • 3142 independent reflections

  • 2445 reflections with I > 2σ(I)

  • R int = 0.015

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.034

  • wR(F 2) = 0.099

  • S = 1.08

  • 3142 reflections

  • 244 parameters

  • H-atom parameters constrained

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.19 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2009); cell refinement: CrysAlis RED (Oxford Diffraction, 2009); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012) 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/S1600536813012336/fy2093sup1.cif

e-69-0o882-sup1.cif (23.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813012336/fy2093Isup2.hkl

e-69-0o882-Isup2.hkl (154.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813012336/fy2093Isup3.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
C12—H12⋯F1i 0.95 2.61 3.2955 (12) 129

Symmetry code: (i) Inline graphic.

Acknowledgments

The financial support of this work by the Inter­nal Founding Agency of Tomas Bata University in Zlin (project No. IGA/FT/2013/008) is gratefully acknowledged.

supplementary crystallographic information

Comment

Quinoline and its derivatives are very important compounds whose structures occur in a variety of natural alkaloids and therapeutics with interesting biological activities. As an example, derivatives of 4-(1-adamantyl)quinoline-2-carboxylic acid have been recently described as potent antituberculosis agents (Nayyar et al., 2009). The title compound was prepared as a part of our research aimed at the examination of novel convenient synthetic procedures toward 4-(1-adamantyl)quinoline derivatives (Kozubková et al., 2012).

The molecule of the title compound consists of three motifs – quinoline and benzene rings and adamantane cage (Figure 1). The quinoline and benzene rings are essentially planar with the respective r.m.s. deviations of 0.0303 and 0.0052 Å and the respective maximum deviations of -0.0477 (12) Å for C1 and 0.0067 (12) Å for C13. The dihedral angle between the planes of these rings is 9.51 (4)°. The adamantane cage consist of free fused cyclohexane rings in classical chairs conformations with C—C—C angles in the range 105.68 (10)–111.83 (11)°. The torsion angles describing the mutual orientation of the benzene, quinoline and adamantane moieties C2–C1–C10–C15 and C4–C3–C16–C17 are -10.62 (19) and 66.77 (15)°, respectively. Although the quinoline ring is essentially planar, it is markedly deformed in plane as it is usual for similar quinoline rings substituted with bulky adamantane at position 4 (Kozubková et al., 2012). The most affected valence angles N1–C9–C8, C2–C3–C4, N1–C9–C4 and C3–C4–C5 are 115.82 (11), 115.91 (11), 124.06 (12) and 125.91 (12)°, respectively. The packing of the molecules in the crystal is stabilized by a weak C—H···F interaction (Table 1, Figure 2). In addition, a weak π–π interaction (Figure 2) is observed between the benzene ring (C10–C15) and quinoline ring (C1–C9, N1), with the shortest centroid-to-centroid distance of 3.6440 (2) Å. Distances of C14, C15, and Cg1 from best plane of adjacent quinoline ring are -3.2742 (13), -3.2448 (13), and -3.4517 (13) Å.

Experimental

The title compound was prepared via a Friedländer reaction from the corresponding 1-adamantyl aminophenyl ketone and 4-fluoroacetophenone as it has been described previously (Kozubková et al., 2012). A single-crystal usable for X-ray analysis was obtained by slow spontaneous evaporation from deuterochloloform at room temperature.

Refinement

All H atoms were placed at calculated positions and were refined as riding with their Uiso set to 1.2Ueq of the respective carrier atoms. C—H distances are 0.9500 Å for aromatic H atoms, 0.9900 Å for H atoms of secondary carbon atoms and 1.0000 Å for H atoms of tertiary carbon atoms.

Figures

Fig. 1.

Fig. 1.

ORTEP view of the asymmetric unit with atoms represented as 50% probability ellipsoids. H-atoms are shown as small spheres at arbitrary radii.

Fig. 2.

Fig. 2.

Part of the crystal structure of the title compound showing the intermolecular π–π and C–H···F interactions as dotted lines. H-atoms have been omitted for clarity (except for those participating in H-bonds). Cg1 and Cg2 are the respective centers of gravity of the C10–C15 and C1–C4,C9,N1 rings. Symmetry codes: (i) -x + 1, -y + 1, -z + 1; (ii) x - 1, y, z.

Crystal data

C25H24FN Z = 2
Mr = 357.45 F(000) = 380
Triclinic, P1 Dx = 1.329 Mg m3
Hall symbol: -P 1 Melting point: 435 K
a = 6.4604 (3) Å Mo Kα radiation, λ = 0.71073 Å
b = 10.9964 (4) Å Cell parameters from 5109 reflections
c = 12.9074 (5) Å θ = 3.2–27.2°
α = 93.205 (3)° µ = 0.08 mm1
β = 96.446 (3)° T = 120 K
γ = 100.507 (3)° Block, colourless
V = 893.14 (6) Å3 0.60 × 0.40 × 0.20 mm

Data collection

Oxford Diffraction Xcalibur diffractometer 3142 independent reflections
Radiation source: Enhance (Mo) X-ray Source 2445 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.015
Detector resolution: 8.4353 pixels mm-1 θmax = 25.0°, θmin = 3.2°
ω scan h = −7→7
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) k = −8→13
Tmin = 0.971, Tmax = 1.000 l = −15→15
9490 measured reflections

Refinement

Refinement on F2 0 restraints
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.034 w = 1/[σ2(Fo2) + (0.0613P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.099 (Δ/σ)max < 0.001
S = 1.08 Δρmax = 0.20 e Å3
3142 reflections Δρmin = −0.19 e Å3
244 parameters

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 > 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
F1 0.34394 (12) 0.33553 (7) 0.56712 (6) 0.0332 (2)
N1 1.06928 (16) 0.26583 (10) 0.29611 (8) 0.0214 (3)
C1 0.92455 (19) 0.17633 (12) 0.32331 (9) 0.0198 (3)
C2 0.91382 (19) 0.05025 (12) 0.29032 (9) 0.0200 (3)
H2 0.8044 −0.0101 0.3110 0.024*
C3 1.05410 (19) 0.01109 (12) 0.22984 (9) 0.0187 (3)
C4 1.21873 (19) 0.10663 (12) 0.20249 (9) 0.0194 (3)
C5 1.39056 (19) 0.08736 (13) 0.14764 (9) 0.0213 (3)
H5 1.4001 0.0052 0.1247 0.026*
C6 1.5421 (2) 0.18375 (13) 0.12701 (9) 0.0243 (3)
H6 1.6546 0.1674 0.0902 0.029*
C7 1.5339 (2) 0.30672 (13) 0.15946 (10) 0.0261 (3)
H7 1.6392 0.3733 0.1441 0.031*
C8 1.3735 (2) 0.32951 (13) 0.21319 (10) 0.0244 (3)
H8 1.3678 0.4126 0.2351 0.029*
C9 1.21530 (19) 0.23188 (12) 0.23691 (9) 0.0202 (3)
C10 0.77164 (19) 0.21533 (12) 0.39064 (9) 0.0195 (3)
C11 0.8057 (2) 0.33784 (12) 0.43399 (10) 0.0236 (3)
H11 0.9288 0.3944 0.4218 0.028*
C12 0.6640 (2) 0.37833 (13) 0.49428 (10) 0.0250 (3)
H12 0.6889 0.4615 0.5240 0.030*
C13 0.4865 (2) 0.29515 (13) 0.51007 (9) 0.0236 (3)
C14 0.4466 (2) 0.17378 (13) 0.47036 (9) 0.0237 (3)
H14 0.3231 0.1181 0.4834 0.028*
C15 0.59069 (19) 0.13429 (12) 0.41086 (9) 0.0216 (3)
H15 0.5658 0.0503 0.3832 0.026*
C16 1.03604 (19) −0.12759 (12) 0.19886 (9) 0.0180 (3)
C17 1.22648 (19) −0.17477 (12) 0.25635 (9) 0.0197 (3)
H17A 1.3607 −0.1264 0.2383 0.024*
H17B 1.2260 −0.1621 0.3329 0.024*
C18 1.2147 (2) −0.31265 (12) 0.22571 (9) 0.0218 (3)
H18 1.3411 −0.3403 0.2620 0.026*
C19 1.0124 (2) −0.38832 (12) 0.25789 (9) 0.0230 (3)
H19A 1.0050 −0.4776 0.2390 0.028*
H19B 1.0131 −0.3763 0.3345 0.028*
C20 0.82066 (19) −0.34565 (12) 0.20168 (9) 0.0214 (3)
H20 0.6879 −0.3938 0.2235 0.026*
C21 0.83436 (19) −0.20723 (12) 0.23111 (9) 0.0203 (3)
H21A 0.8346 −0.1938 0.3076 0.024*
H21B 0.7076 −0.1804 0.1963 0.024*
C22 1.0223 (2) −0.15445 (12) 0.07863 (9) 0.0207 (3)
H22A 0.8924 −0.1307 0.0441 0.025*
H22B 1.1463 −0.1039 0.0528 0.025*
C23 1.0176 (2) −0.29224 (12) 0.05047 (9) 0.0220 (3)
H23 1.0164 −0.3067 −0.0268 0.026*
C24 0.8172 (2) −0.36869 (13) 0.08344 (9) 0.0238 (3)
H24A 0.8113 −0.4579 0.0648 0.029*
H24B 0.6901 −0.3444 0.0465 0.029*
C25 1.2133 (2) −0.33189 (13) 0.10712 (9) 0.0235 (3)
H25A 1.2110 −0.4204 0.0871 0.028*
H25B 1.3437 −0.2822 0.0862 0.028*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
F1 0.0378 (5) 0.0358 (5) 0.0331 (4) 0.0163 (4) 0.0192 (4) 0.0045 (4)
N1 0.0203 (6) 0.0218 (7) 0.0228 (5) 0.0056 (5) 0.0024 (4) 0.0036 (5)
C1 0.0184 (7) 0.0214 (8) 0.0192 (6) 0.0043 (6) −0.0010 (5) 0.0032 (6)
C2 0.0183 (6) 0.0196 (8) 0.0221 (6) 0.0028 (6) 0.0040 (5) 0.0026 (6)
C3 0.0176 (6) 0.0214 (8) 0.0165 (6) 0.0034 (6) 0.0001 (5) 0.0022 (5)
C4 0.0194 (6) 0.0233 (8) 0.0154 (6) 0.0043 (6) 0.0000 (5) 0.0031 (5)
C5 0.0212 (7) 0.0244 (8) 0.0180 (6) 0.0034 (6) 0.0026 (5) 0.0015 (5)
C6 0.0208 (7) 0.0325 (9) 0.0195 (6) 0.0029 (6) 0.0051 (5) 0.0041 (6)
C7 0.0235 (7) 0.0271 (9) 0.0265 (7) −0.0007 (6) 0.0051 (6) 0.0076 (6)
C8 0.0270 (7) 0.0185 (8) 0.0271 (7) 0.0020 (6) 0.0035 (6) 0.0049 (6)
C9 0.0192 (6) 0.0230 (8) 0.0187 (6) 0.0048 (6) 0.0008 (5) 0.0041 (6)
C10 0.0204 (7) 0.0202 (8) 0.0186 (6) 0.0065 (6) 0.0007 (5) 0.0017 (5)
C11 0.0229 (7) 0.0218 (8) 0.0261 (7) 0.0034 (6) 0.0035 (5) 0.0022 (6)
C12 0.0309 (8) 0.0217 (8) 0.0235 (7) 0.0087 (6) 0.0036 (6) −0.0004 (6)
C13 0.0268 (7) 0.0306 (9) 0.0179 (6) 0.0139 (7) 0.0068 (5) 0.0040 (6)
C14 0.0226 (7) 0.0268 (9) 0.0230 (6) 0.0052 (6) 0.0056 (5) 0.0062 (6)
C15 0.0230 (7) 0.0202 (8) 0.0219 (6) 0.0056 (6) 0.0020 (5) 0.0012 (6)
C16 0.0172 (6) 0.0187 (8) 0.0183 (6) 0.0033 (6) 0.0044 (5) 0.0010 (5)
C17 0.0174 (6) 0.0236 (8) 0.0179 (6) 0.0033 (6) 0.0030 (5) 0.0003 (5)
C18 0.0220 (7) 0.0229 (8) 0.0222 (6) 0.0086 (6) 0.0029 (5) 0.0013 (6)
C19 0.0313 (7) 0.0183 (8) 0.0212 (6) 0.0068 (6) 0.0075 (5) 0.0008 (6)
C20 0.0194 (7) 0.0209 (8) 0.0236 (6) 0.0006 (6) 0.0077 (5) 0.0005 (6)
C21 0.0178 (6) 0.0224 (8) 0.0212 (6) 0.0043 (6) 0.0048 (5) 0.0005 (6)
C22 0.0188 (6) 0.0249 (8) 0.0179 (6) 0.0022 (6) 0.0026 (5) 0.0023 (5)
C23 0.0247 (7) 0.0253 (8) 0.0155 (6) 0.0033 (6) 0.0043 (5) −0.0023 (5)
C24 0.0230 (7) 0.0240 (8) 0.0227 (7) 0.0017 (6) 0.0019 (5) −0.0026 (6)
C25 0.0238 (7) 0.0222 (8) 0.0256 (7) 0.0052 (6) 0.0076 (5) −0.0018 (6)

Geometric parameters (Å, º)

F1—C13 1.3610 (14) C15—H15 0.9500
N1—C1 1.3201 (16) C16—C21 1.5441 (16)
N1—C9 1.3681 (16) C16—C17 1.5506 (16)
C1—C2 1.4144 (17) C16—C22 1.5530 (15)
C1—C10 1.4901 (17) C17—C18 1.5313 (17)
C2—C3 1.3710 (16) C17—H17A 0.9900
C2—H2 0.9500 C17—H17B 0.9900
C3—C4 1.4414 (17) C18—C19 1.5287 (17)
C3—C16 1.5348 (17) C18—C25 1.5322 (16)
C4—C5 1.4227 (17) C18—H18 1.0000
C4—C9 1.4282 (18) C19—C20 1.5262 (17)
C5—C6 1.3654 (18) C19—H19A 0.9900
C5—H5 0.9500 C19—H19B 0.9900
C6—C7 1.4051 (18) C20—C24 1.5300 (16)
C6—H6 0.9500 C20—C21 1.5322 (17)
C7—C8 1.3617 (18) C20—H20 1.0000
C7—H7 0.9500 C21—H21A 0.9900
C8—C9 1.4134 (18) C21—H21B 0.9900
C8—H8 0.9500 C22—C23 1.5324 (17)
C10—C15 1.3941 (17) C22—H22A 0.9900
C10—C11 1.3986 (18) C22—H22B 0.9900
C11—C12 1.3826 (17) C23—C24 1.5264 (17)
C11—H11 0.9500 C23—C25 1.5337 (17)
C12—C13 1.3727 (19) C23—H23 1.0000
C12—H12 0.9500 C24—H24A 0.9900
C13—C14 1.3708 (18) C24—H24B 0.9900
C14—C15 1.3838 (17) C25—H25A 0.9900
C14—H14 0.9500 C25—H25B 0.9900
C1—N1—C9 117.34 (11) C18—C17—H17A 109.5
N1—C1—C2 122.11 (11) C16—C17—H17A 109.5
N1—C1—C10 116.32 (12) C18—C17—H17B 109.5
C2—C1—C10 121.57 (11) C16—C17—H17B 109.5
C3—C2—C1 123.02 (12) H17A—C17—H17B 108.1
C3—C2—H2 118.5 C19—C18—C17 109.63 (10)
C1—C2—H2 118.5 C19—C18—C25 109.72 (10)
C2—C3—C4 115.91 (12) C17—C18—C25 109.25 (10)
C2—C3—C16 120.26 (11) C19—C18—H18 109.4
C4—C3—C16 123.79 (11) C17—C18—H18 109.4
C5—C4—C9 116.54 (12) C25—C18—H18 109.4
C5—C4—C3 125.90 (12) C20—C19—C18 108.95 (10)
C9—C4—C3 117.51 (11) C20—C19—H19A 109.9
C6—C5—C4 121.80 (13) C18—C19—H19A 109.9
C6—C5—H5 119.1 C20—C19—H19B 109.9
C4—C5—H5 119.1 C18—C19—H19B 109.9
C5—C6—C7 120.96 (12) H19A—C19—H19B 108.3
C5—C6—H6 119.5 C19—C20—C24 109.41 (10)
C7—C6—H6 119.5 C19—C20—C21 109.41 (10)
C8—C7—C6 119.30 (13) C24—C20—C21 110.10 (10)
C8—C7—H7 120.4 C19—C20—H20 109.3
C6—C7—H7 120.4 C24—C20—H20 109.3
C7—C8—C9 121.27 (13) C21—C20—H20 109.3
C7—C8—H8 119.4 C20—C21—C16 111.83 (10)
C9—C8—H8 119.4 C20—C21—H21A 109.3
N1—C9—C8 115.81 (12) C16—C21—H21A 109.3
N1—C9—C4 124.04 (12) C20—C21—H21B 109.3
C8—C9—C4 120.11 (11) C16—C21—H21B 109.3
C15—C10—C11 117.95 (12) H21A—C21—H21B 107.9
C15—C10—C1 122.31 (12) C23—C22—C16 110.71 (10)
C11—C10—C1 119.73 (11) C23—C22—H22A 109.5
C12—C11—C10 121.36 (12) C16—C22—H22A 109.5
C12—C11—H11 119.3 C23—C22—H22B 109.5
C10—C11—H11 119.3 C16—C22—H22B 109.5
C13—C12—C11 118.23 (13) H22A—C22—H22B 108.1
C13—C12—H12 120.9 C24—C23—C22 109.06 (10)
C11—C12—H12 120.9 C24—C23—C25 109.39 (10)
F1—C13—C14 118.85 (12) C22—C23—C25 110.17 (10)
F1—C13—C12 118.38 (12) C24—C23—H23 109.4
C14—C13—C12 122.77 (12) C22—C23—H23 109.4
C13—C14—C15 118.37 (12) C25—C23—H23 109.4
C13—C14—H14 120.8 C23—C24—C20 108.93 (10)
C15—C14—H14 120.8 C23—C24—H24A 109.9
C14—C15—C10 121.32 (13) C20—C24—H24A 109.9
C14—C15—H15 119.3 C23—C24—H24B 109.9
C10—C15—H15 119.3 C20—C24—H24B 109.9
C3—C16—C21 112.40 (10) H24A—C24—H24B 108.3
C3—C16—C17 109.61 (10) C18—C25—C23 109.93 (10)
C21—C16—C17 106.18 (10) C18—C25—H25A 109.7
C3—C16—C22 111.85 (10) C23—C25—H25A 109.7
C21—C16—C22 105.68 (10) C18—C25—H25B 109.7
C17—C16—C22 110.94 (10) C23—C25—H25B 109.7
C18—C17—C16 110.84 (10) H25A—C25—H25B 108.2
C9—N1—C1—C2 −2.15 (17) C11—C10—C15—C14 1.14 (18)
C9—N1—C1—C10 178.09 (10) C1—C10—C15—C14 −177.50 (11)
N1—C1—C2—C3 1.36 (18) C2—C3—C16—C21 7.19 (15)
C10—C1—C2—C3 −178.88 (11) C4—C3—C16—C21 −175.40 (10)
C1—C2—C3—C4 1.05 (17) C2—C3—C16—C17 −110.64 (12)
C1—C2—C3—C16 178.66 (10) C4—C3—C16—C17 66.78 (13)
C2—C3—C4—C5 174.85 (11) C2—C3—C16—C22 125.88 (12)
C16—C3—C4—C5 −2.67 (18) C4—C3—C16—C22 −56.70 (14)
C2—C3—C4—C9 −2.43 (15) C3—C16—C17—C18 −179.14 (9)
C16—C3—C4—C9 −179.94 (10) C21—C16—C17—C18 59.23 (12)
C9—C4—C5—C6 −1.31 (17) C22—C16—C17—C18 −55.13 (13)
C3—C4—C5—C6 −178.61 (11) C16—C17—C18—C19 −61.68 (12)
C4—C5—C6—C7 −0.01 (18) C16—C17—C18—C25 58.58 (12)
C5—C6—C7—C8 0.69 (18) C17—C18—C19—C20 60.25 (12)
C6—C7—C8—C9 0.01 (18) C25—C18—C19—C20 −59.73 (13)
C1—N1—C9—C8 −177.26 (10) C18—C19—C20—C24 61.41 (13)
C1—N1—C9—C4 0.59 (17) C18—C19—C20—C21 −59.29 (12)
C7—C8—C9—N1 176.56 (11) C19—C20—C21—C16 60.65 (12)
C7—C8—C9—C4 −1.39 (18) C24—C20—C21—C16 −59.63 (13)
C5—C4—C9—N1 −175.79 (10) C3—C16—C21—C20 −178.86 (9)
C3—C4—C9—N1 1.74 (17) C17—C16—C21—C20 −59.02 (12)
C5—C4—C9—C8 1.98 (16) C22—C16—C21—C20 58.88 (12)
C3—C4—C9—C8 179.51 (10) C3—C16—C22—C23 176.68 (10)
N1—C1—C10—C15 169.13 (10) C21—C16—C22—C23 −60.71 (12)
C2—C1—C10—C15 −10.64 (18) C17—C16—C22—C23 53.95 (13)
N1—C1—C10—C11 −9.49 (16) C16—C22—C23—C24 63.30 (12)
C2—C1—C10—C11 170.75 (10) C16—C22—C23—C25 −56.77 (13)
C15—C10—C11—C12 −0.61 (18) C22—C23—C24—C20 −60.27 (13)
C1—C10—C11—C12 178.06 (11) C25—C23—C24—C20 60.28 (14)
C10—C11—C12—C13 −0.57 (19) C19—C20—C24—C23 −61.85 (14)
C11—C12—C13—F1 −178.33 (11) C21—C20—C24—C23 58.43 (13)
C11—C12—C13—C14 1.30 (19) C19—C18—C25—C23 58.80 (14)
F1—C13—C14—C15 178.84 (11) C17—C18—C25—C23 −61.41 (13)
C12—C13—C14—C15 −0.79 (19) C24—C23—C25—C18 −59.05 (14)
C13—C14—C15—C10 −0.47 (18) C22—C23—C25—C18 60.83 (13)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C12—H12···F1i 0.95 2.61 3.2955 (12) 129

Symmetry code: (i) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FY2093).

References

  1. Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
  2. Kozubková, Z., Rouchal, M., Nečas, M. & Vícha, R. (2012). Helv. Chim. Acta, 95, 1003–1017.
  3. Macrae, C. F., Bruno, I. J., Chisholm, J. A., Edgington, P. R., McCabe, P., Pidcock, E., Rodriguez-Monge, L., Taylor, R., van de Streek, J. & Wood, P. A. (2008). J. Appl. Cryst. 41, 466–470.
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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/S1600536813012336/fy2093sup1.cif

e-69-0o882-sup1.cif (23.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813012336/fy2093Isup2.hkl

e-69-0o882-Isup2.hkl (154.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813012336/fy2093Isup3.cml

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


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