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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Feb 4;68(Pt 3):o625–o626. doi: 10.1107/S1600536812003054

9-(3-Fluoro­phen­oxy­carbon­yl)-10-methyl­acridinium trifluoro­methane­sulfonate monohydrate

Damian Trzybiński a, Agnieszka Ożóg a, Karol Krzymiński a, Jerzy Błażejowski a,*
PMCID: PMC3295421  PMID: 22412532

Abstract

In the crystal structure of the title mol­ecular salt, C21H15FNO2 +·CF3SO3 ·H2O, the cations form inversion dimers through π–π inter­actions between the acridine ring systems. These dimers are linked via C—H⋯O and C—F⋯π inter­actions to adjacent anions, and by C—H⋯π and C—F⋯π inter­actions to neighbouring cations. The water mol­ecule links two sites of the cation by C—H⋯O inter­actions and two adjacent anions by O—H⋯O hydrogen bonds. The mean planes of the acridine and benzene ring systems are oriented at a dihedral angle of 15.1 (1)°. The carboxyl group is twisted at an angle of 84.5 (1)° relative to the acridine skeleton. The mean planes of the acridine ring systems are parallel in the crystal.

Related literature  

For general background to the chemiluminogenic features of 9-phen­oxy­carbonyl-10-methyl­acridinium trifluoro­methane­sulfonates, see: King et al. (2007); Krzymiński et al. (2011); Roda et al. (2003). For related structures, see: Trzybiński et al. (2010). For inter­molecular inter­actions, see: Aakeröy et al. (1992); Dorn et al. (2005); Hunter et al. (2001); Novoa et al. (2006); Takahashi et al. (2001). For the synthesis, see: Sato (1996); Trzybiński et al. (2010).graphic file with name e-68-0o625-scheme1.jpg

Experimental  

Crystal data  

  • C21H15FNO2 +·CF3O3S·H2O

  • M r = 499.44

  • Triclinic, Inline graphic

  • a = 9.5144 (10) Å

  • b = 11.5654 (11) Å

  • c = 11.9680 (12) Å

  • α = 109.975 (9)°

  • β = 97.838 (8)°

  • γ = 113.197 (9)°

  • V = 1080.3 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.23 mm−1

  • T = 295 K

  • 0.40 × 0.15 × 0.10 mm

Data collection  

  • Oxford Gemini R Ultra Ruby CCD diffractometer

  • 9148 measured reflections

  • 3769 independent reflections

  • 1647 reflections with I > 2σ(I)

  • R int = 0.050

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.051

  • wR(F 2) = 0.129

  • S = 0.81

  • 3769 reflections

  • 314 parameters

  • 3 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.27 e Å−3

  • Δρmin = −0.28 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2008); cell refinement: CrysAlis RED (Oxford Diffraction, 2008); 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 (Farrugia, 1997); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812003054/xu5452sup1.cif

e-68-0o625-sup1.cif (29.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812003054/xu5452Isup2.hkl

e-68-0o625-Isup2.hkl (184.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812003054/xu5452Isup3.cml

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

Table 1. Hydrogen-bond geometry (Å, °).

Cg4 is the centroid of the C18–C23 ring.

D—H⋯A D—H H⋯A DA D—H⋯A
O1W—H1W⋯O29i 0.85 (3) 2.24 (3) 3.071 (5) 172 (4)
O1W—H2W⋯O28 0.89 (3) 1.99 (3) 2.873 (5) 176 (8)
C1—H1⋯O1W 0.93 2.51 3.365 (7) 152
C3—H3⋯O29ii 0.93 2.60 3.298 (5) 133
C19—H19⋯O1W 0.93 2.60 3.415 (7) 145
C25—H25A⋯O27iii 0.96 2.53 3.424 (5) 155
C25—H25CCg4ii 0.96 2.64 3.527 (4) 154

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

Table 2. C—F⋯π inter­actions (Å,°).

Cg1, Cg2 and Cg3 are the centroids of the C9/N10/C11–C14, C1–C4/C11/C12 and C5–C8/C13/C14 rings, respectively.

X I J IJ XJ XIJ
C20 F24 Cg2iv 3.743 (3) 4.139 (5) 97.6 (2)
C20 F24 Cg2v 3.854 (4) 4.188 (5) 94.9 (3)
C30 F31 Cg1v 3.665 (4) 4.519 (6) 123.6 (3)
C30 F31 Cg3v 3.910 (4) 4.049 (6) 86.7 (3)
C30 F33 Cg3v 3.654 (4) 4.049 (6) 97.7 (3)

Symmetry codes: (iv) x − 1, y, z; (v) −x + 1, −y + 2, −z + 1.

Table 3. π–π inter­actions (Å,°).

Cg1, Cg2 and Cg3 are as defined in Table 2. CgICgJ is the distance between ring centroids. The dihedral angle is that between the planes of the rings I and J. CgI Perp is the perpendicular distance of CgI from ring J. CgI Offset is the distance between CgI and the perpendicular projection of CgJ on ring I.

I J CgICgJ Dihedral angle CgIPerp CgIOffset
1 1vi 3.990 (2)   3.591 (2) 1.739 (2)
1 3vi 3.645 (2) 2.08 (17) 3.557 (2) 0.796 (2)
2 3vi 3.907 (2) 3.85 (19) 3.431 (2) 1.863 (2)
3 1vi 3.645 (2) 2.08 (17) 3.546 (2) 0.844 (2)
3 2vi 3.907 (2) 3.85 (19) 3.548 (2) 1.629 (2)

Symmetry code: (vi) −x + 1, −y + 1, −z.

Acknowledgments

This study was financed by the State Funds for Scientific Research through National Center for Science grant No. N N204 375 740 (contract No. 3757/B/H03/2011/40). DT acknowledges financial support from the European Social Fund within the project ‘Educators for the elite – integrated training program for PhD students, post-docs and professors as academic teachers at the University of Gdansk’ and the Human Capital Operational Program Action 4.1.1, ‘Improving the quality on offer at tertiary educational institutions’. This publication reflects the views only of the authors: the sponsors cannot be held responsible for any use which may be made of the information contained therein.

supplementary crystallographic information

Comment

9-Phenoxycarbonyl-10-methylacridinium cations react with oxidants (e.g. H2O2) in alkaline media, as a result of which electronically excited 10-methyl-9-acridinone molecules are generated (Krzymiński et al., 2011). This phenomenon forms the basis for the use of these entities as chemiluminogenic indicators or fragments of chemiluminescent labels (Roda et al., 2003; King et al., 2007; Krzymiński et al., 2011). It has been noted that the conversion efficiency of the above-mentioned cations to 10-methyl-9-acridinone molecules, and consequently the chemiluminescence quantum yield, crucial in analytical applications, depends on the structure of the phenoxycarbonyl fragment (Krzymiński et al., 2011). For these reasons we have been synthesizing 9-phenoxycarbonyl-10-methylacridinium trifluoromethanesulfonates variously substituted in the phenyl fragment in order to select derivatives optimal for analytical applications. Here we present the structure of one of the compounds of this series.

In the cation of the title compound (Fig. 1), the bond lengths and angles characterizing the geometry of the acridinium and phenyl moieties are typical of 9-phenoxycarbonyl-10-methylacridinium derivatives (Trzybiński et al., 2010). With respective average deviations from planarity of 0.0397 (3) Å and 0.0066 (3) Å, the acridine and benzene ring systems are oriented at a dihedral angle of 15.1 (1)° [in 9-(4-fluorophenoxycarbonyl)-10-methylacridinium trifluoromethanesulfonate this angle is equal to 74.1 (1)° (Trzybiński et al., 2010)]. The carboxyl group is twisted at an angle of 84.5 (1)° relative to the acridine skeleton [in 9-(4-fluorophenoxycarbonyl)-10-methylacridinium trifluoromethanesulfonate this angle is 4.4 (1)° (Trzybiński et al., 2010)]. The mean planes of the adjacent acridine moieties are parallel [remain at an angle of 0.0 (1)°)] in the lattice.

In the crystal structure, the inversely oriented cations form dimers through π–π contacts involving all three rings of the acridine aromatic system (Table 3, Fig. 2). These dimers are linked by C—H···O (Table 1, Fig. 2) and C—F···π (Table 2, Fig. 2) interactions to adjacent anions and by C—H···π (Table 1, Fig. 2) and C—F···π (Table 2, Fig. 2) interactions to neighbouring cations. Each cation is involved in two C—H···O interactions with a water molecule, which in turn is engaged in O—H···O hydrogen bonds involving O atoms of two adjacent anions (Table 1, Figs. 1 and 2). The O—H···O (Aakeröy et al., 1992) and C—H···O (Novoa et al., 2006) interactions are of the hydrogen bond type. The C—H···π interactions should be of an attractive nature (Takahashi et al., 2001), like the C—F···π (Dorn et al., 2005) and the π–π (Hunter et al., 2001) interactions. The crystal structure is stabilized by a network of these short-range specific interactions and by long-range electrostatic interactions between ions.

Experimental

3-Fluorophenylacridine-9-carboxylate was obtained by esterification of 9-(chlorocarbonyl)acridine (synthesized in the reaction of acridine-9-carboxylic acid with a tenfold excess of thionyl chloride) with 3-fluorophenol in anhydrous dichloromethane in the presence of N,N-diethylethanamine and a catalytic amount of N,N-dimethyl-4-pyridinamine (room temperature, 15 h) (Sato, 1996). The product was purified chromatographically (SiO2, cyclohexane/ethyl acetate, 1/1 v/v) and subsequently quaternarized with a fivefold molar excess of methyl trifluoromethanesulfonate dissolved in anhydrous dichloromethane. The crude 3-(fluorophenoxycarbonyl)-10-methylacridinium trifluoromethanesulfonate was dissolved in a small amount of ethanol, filtered and precipitated with a 20 v/v excess of diethyl ether (Trzybiński et al., 2010). Light-yellow crystals suitable for X-ray investigations were grown from methanol/water solution (1/1 v/v) (m.p. 497–498 K).

Refinement

The H atoms of the water molecule were located on a Fourier difference map, restrained by DFIX command 0.85 for O—H distances and by DFIX 1.39 for H···H distance, and refined as riding with Uiso(H) = 1.5Ueq(O). Other H atoms were positioned geometrically, with C—H = 0.93 Å and 0.96 Å for the aromatic and methyl H atoms, respectively, and constrained to ride on their parent atoms with Uiso(H) = xUeq(C), where x = 1.2 for the aromatic H atoms and x = 1.5 for the methyl H atoms.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound showing the atom labeling scheme. Displacement ellipsoids are drawn at the 25% probability level and H atoms are shown as small spheres of arbitrary radius. Cg1, Cg2, Cg3 and Cg4 denote the ring centroids. The O—H···O and C—H···O hydrogen bonds are represented by dashed lines.

Fig. 2.

Fig. 2.

The arrangement of the ions and H2O molecules in the crystal structure, viewed along b-direction. The O—H···O and C—H···O interactions are represented by dashed lines, the C—H···π, C—F···π and π—π contacts by dotted lines. H atoms not involved in interactions have been omitted. [Symmetry codes: (i) -x, -y + 1, -z + 1; (ii) x + 1, y, z; (iii) x + 1, y, z - 1; (iv) x - 1, y, z; (v) -x + 1, -y + 2, -z + 1; (vi) -x + 1, -y + 1, -z.]

Crystal data

C21H15FNO2+·CF3O3S·H2O Z = 2
Mr = 499.44 F(000) = 512
Triclinic, P1 Dx = 1.535 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.5144 (10) Å Cell parameters from 2551 reflections
b = 11.5654 (11) Å θ = 3.1–29.0°
c = 11.9680 (12) Å µ = 0.23 mm1
α = 109.975 (9)° T = 295 K
β = 97.838 (8)° Prism, light yellow
γ = 113.197 (9)° 0.40 × 0.15 × 0.10 mm
V = 1080.3 (2) Å3

Data collection

Oxford Gemini R Ultra Ruby CCD diffractometer 1647 reflections with I > 2σ(I)
Radiation source: Enhanced (Mo) X-ray Source Rint = 0.050
Graphite monochromator θmax = 25.1°, θmin = 3.1°
Detector resolution: 10.4002 pixels mm-1 h = −11→11
ω scans k = −13→13
9148 measured reflections l = −13→14
3769 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)] = 0.051 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.129 H atoms treated by a mixture of independent and constrained refinement
S = 0.81 w = 1/[σ2(Fo2) + (0.0706P)2] where P = (Fo2 + 2Fc2)/3
3769 reflections (Δ/σ)max = 0.003
314 parameters Δρmax = 0.27 e Å3
3 restraints Δρmin = −0.28 e Å3

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
C1 0.6064 (4) 0.6768 (4) 0.3644 (3) 0.0694 (10)
H1 0.5226 0.6930 0.3842 0.083*
O1W 0.2866 (5) 0.6414 (4) 0.4672 (4) 0.1503 (14)
H1W 0.229 (7) 0.553 (3) 0.420 (5) 0.225*
H2W 0.258 (8) 0.655 (6) 0.535 (4) 0.225*
C2 0.6940 (5) 0.6521 (4) 0.4419 (3) 0.0774 (11)
H2 0.6694 0.6494 0.5139 0.093*
C3 0.8221 (5) 0.6303 (4) 0.4147 (4) 0.0780 (11)
H3 0.8836 0.6155 0.4703 0.094*
C4 0.8587 (4) 0.6302 (4) 0.3100 (3) 0.0669 (9)
H4 0.9441 0.6147 0.2938 0.080*
C5 0.7416 (4) 0.6647 (3) −0.0808 (3) 0.0610 (9)
H5 0.8279 0.6514 −0.0982 0.073*
C6 0.6469 (5) 0.6792 (4) −0.1633 (3) 0.0701 (10)
H6 0.6688 0.6748 −0.2376 0.084*
C7 0.5172 (4) 0.7005 (4) −0.1417 (3) 0.0712 (10)
H7 0.4535 0.7095 −0.2011 0.085*
C8 0.4848 (4) 0.7081 (3) −0.0346 (3) 0.0619 (9)
H8 0.3984 0.7228 −0.0200 0.074*
C9 0.5504 (4) 0.7021 (3) 0.1689 (3) 0.0519 (8)
N10 0.8010 (3) 0.6524 (3) 0.1173 (2) 0.0524 (7)
C11 0.6393 (4) 0.6788 (3) 0.2530 (3) 0.0539 (8)
C12 0.7684 (4) 0.6534 (3) 0.2251 (3) 0.0521 (8)
C13 0.5797 (3) 0.6941 (3) 0.0564 (3) 0.0502 (8)
C14 0.7103 (4) 0.6698 (3) 0.0315 (3) 0.0501 (8)
C15 0.4158 (5) 0.7316 (4) 0.1978 (3) 0.0609 (9)
O16 0.4730 (3) 0.8678 (2) 0.2685 (2) 0.0703 (7)
O17 0.2782 (3) 0.6459 (3) 0.1585 (3) 0.0872 (8)
C18 0.3576 (4) 0.9124 (3) 0.2952 (3) 0.0613 (9)
C19 0.3045 (4) 0.9060 (4) 0.3932 (3) 0.0672 (9)
H19 0.3389 0.8693 0.4426 0.081*
C20 0.1975 (4) 0.9564 (4) 0.4164 (4) 0.0749 (10)
C21 0.1428 (5) 1.0080 (4) 0.3448 (4) 0.0842 (12)
H21 0.0687 1.0395 0.3624 0.101*
C22 0.1981 (5) 1.0130 (4) 0.2468 (4) 0.0915 (13)
H22 0.1613 1.0478 0.1966 0.110*
C23 0.3089 (5) 0.9664 (4) 0.2211 (4) 0.0816 (11)
H23 0.3492 0.9716 0.1554 0.098*
F24 0.1452 (3) 0.9541 (3) 0.5144 (2) 0.1166 (9)
C25 0.9405 (4) 0.6317 (4) 0.0943 (3) 0.0695 (10)
H25A 0.9560 0.6413 0.0197 0.104*
H25B 0.9204 0.5401 0.0843 0.104*
H25C 1.0355 0.7005 0.1642 0.104*
S26 0.08915 (12) 0.70895 (10) 0.76540 (9) 0.0699 (3)
O27 0.1099 (3) 0.6733 (3) 0.8669 (2) 0.0903 (8)
O28 0.1777 (3) 0.6826 (3) 0.6828 (2) 0.1036 (9)
O29 −0.0729 (3) 0.6712 (3) 0.7054 (2) 0.0931 (8)
C30 0.1857 (6) 0.8973 (5) 0.8431 (4) 0.0860 (12)
F31 0.1788 (4) 0.9507 (3) 0.7638 (3) 0.1385 (10)
F32 0.3375 (3) 0.9479 (3) 0.9058 (3) 0.1292 (9)
F33 0.1148 (4) 0.9392 (3) 0.9240 (3) 0.1307 (10)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.066 (3) 0.071 (3) 0.065 (2) 0.030 (2) 0.023 (2) 0.025 (2)
O1W 0.182 (4) 0.113 (3) 0.147 (3) 0.046 (3) 0.105 (3) 0.056 (3)
C2 0.093 (3) 0.077 (3) 0.058 (2) 0.037 (3) 0.021 (2) 0.029 (2)
C3 0.084 (3) 0.074 (3) 0.070 (3) 0.039 (2) 0.009 (2) 0.030 (2)
C4 0.062 (2) 0.070 (3) 0.068 (2) 0.034 (2) 0.015 (2) 0.028 (2)
C5 0.056 (2) 0.059 (2) 0.063 (2) 0.023 (2) 0.021 (2) 0.0251 (19)
C6 0.075 (3) 0.069 (3) 0.066 (2) 0.029 (2) 0.024 (2) 0.034 (2)
C7 0.069 (3) 0.073 (3) 0.074 (3) 0.033 (2) 0.013 (2) 0.039 (2)
C8 0.054 (2) 0.063 (2) 0.073 (2) 0.030 (2) 0.018 (2) 0.031 (2)
C9 0.0383 (19) 0.041 (2) 0.063 (2) 0.0149 (17) 0.0100 (18) 0.0155 (17)
N10 0.0393 (16) 0.0494 (17) 0.0600 (17) 0.0198 (14) 0.0128 (14) 0.0170 (14)
C11 0.049 (2) 0.047 (2) 0.055 (2) 0.0186 (18) 0.0146 (18) 0.0156 (17)
C12 0.046 (2) 0.047 (2) 0.053 (2) 0.0194 (18) 0.0093 (17) 0.0160 (17)
C13 0.0399 (19) 0.046 (2) 0.058 (2) 0.0177 (17) 0.0096 (17) 0.0199 (17)
C14 0.0427 (19) 0.043 (2) 0.057 (2) 0.0176 (17) 0.0115 (17) 0.0187 (17)
C15 0.052 (2) 0.062 (3) 0.069 (2) 0.029 (2) 0.019 (2) 0.026 (2)
O16 0.0491 (15) 0.0527 (17) 0.0950 (18) 0.0241 (14) 0.0246 (14) 0.0159 (14)
O17 0.0458 (17) 0.0675 (18) 0.120 (2) 0.0229 (16) 0.0242 (16) 0.0149 (16)
C18 0.047 (2) 0.050 (2) 0.075 (2) 0.0228 (19) 0.019 (2) 0.0160 (19)
C19 0.053 (2) 0.062 (2) 0.070 (2) 0.023 (2) 0.017 (2) 0.017 (2)
C20 0.063 (2) 0.078 (3) 0.067 (3) 0.029 (2) 0.029 (2) 0.015 (2)
C21 0.076 (3) 0.075 (3) 0.101 (3) 0.047 (3) 0.030 (3) 0.024 (3)
C22 0.088 (3) 0.091 (3) 0.115 (4) 0.054 (3) 0.042 (3) 0.049 (3)
C23 0.084 (3) 0.079 (3) 0.099 (3) 0.043 (3) 0.050 (3) 0.044 (3)
F24 0.1057 (19) 0.148 (2) 0.0961 (18) 0.0634 (18) 0.0560 (16) 0.0400 (16)
C25 0.053 (2) 0.084 (3) 0.077 (2) 0.042 (2) 0.023 (2) 0.029 (2)
S26 0.0717 (7) 0.0774 (7) 0.0647 (6) 0.0376 (6) 0.0255 (6) 0.0312 (5)
O27 0.104 (2) 0.111 (2) 0.0891 (19) 0.0613 (19) 0.0385 (17) 0.0646 (18)
O28 0.124 (2) 0.117 (2) 0.099 (2) 0.073 (2) 0.067 (2) 0.0466 (18)
O29 0.0619 (18) 0.116 (2) 0.0755 (18) 0.0298 (17) 0.0063 (14) 0.0341 (17)
C30 0.084 (3) 0.096 (3) 0.093 (3) 0.050 (3) 0.028 (3) 0.048 (3)
F31 0.149 (3) 0.122 (2) 0.169 (3) 0.059 (2) 0.039 (2) 0.101 (2)
F32 0.0778 (19) 0.102 (2) 0.152 (2) 0.0157 (16) −0.0044 (17) 0.0420 (18)
F33 0.152 (3) 0.104 (2) 0.129 (2) 0.077 (2) 0.047 (2) 0.0220 (17)

Geometric parameters (Å, º)

C1—C2 1.340 (4) C11—C12 1.427 (4)
C1—C11 1.416 (4) C13—C14 1.425 (4)
C1—H1 0.9300 C15—O17 1.187 (4)
O1W—H1W 0.86 (2) C15—O16 1.335 (4)
O1W—H2W 0.874 (19) O16—C18 1.415 (3)
C2—C3 1.396 (5) C18—C19 1.352 (4)
C2—H2 0.9300 C18—C23 1.373 (5)
C3—C4 1.345 (4) C19—C20 1.375 (4)
C3—H3 0.9300 C19—H19 0.9300
C4—C12 1.404 (4) C20—F24 1.339 (4)
C4—H4 0.9300 C20—C21 1.354 (5)
C5—C6 1.343 (4) C21—C22 1.359 (5)
C5—C14 1.404 (4) C21—H21 0.9300
C5—H5 0.9300 C22—C23 1.385 (5)
C6—C7 1.390 (4) C22—H22 0.9300
C6—H6 0.9300 C23—H23 0.9300
C7—C8 1.342 (4) C25—H25A 0.9600
C7—H7 0.9300 C25—H25B 0.9600
C8—C13 1.412 (4) C25—H25C 0.9600
C8—H8 0.9300 S26—O28 1.415 (2)
C9—C13 1.391 (4) S26—O27 1.423 (2)
C9—C11 1.391 (4) S26—O29 1.427 (2)
C9—C15 1.504 (4) S26—C30 1.806 (5)
N10—C12 1.365 (4) C30—F31 1.304 (4)
N10—C14 1.369 (4) C30—F32 1.315 (4)
N10—C25 1.484 (3) C30—F33 1.320 (4)
C2—C1—C11 121.1 (3) C5—C14—C13 118.5 (3)
C2—C1—H1 119.4 O17—C15—O16 125.6 (3)
C11—C1—H1 119.4 O17—C15—C9 124.2 (3)
H1W—O1W—H2W 105 (3) O16—C15—C9 110.2 (3)
C1—C2—C3 120.1 (3) C15—O16—C18 116.3 (3)
C1—C2—H2 120.0 C19—C18—C23 122.6 (3)
C3—C2—H2 120.0 C19—C18—O16 120.1 (3)
C4—C3—C2 121.6 (3) C23—C18—O16 117.2 (3)
C4—C3—H3 119.2 C18—C19—C20 116.8 (3)
C2—C3—H3 119.2 C18—C19—H19 121.6
C3—C4—C12 120.3 (3) C20—C19—H19 121.6
C3—C4—H4 119.8 F24—C20—C21 118.8 (3)
C12—C4—H4 119.8 F24—C20—C19 118.2 (4)
C6—C5—C14 119.9 (3) C21—C20—C19 123.0 (4)
C6—C5—H5 120.0 C20—C21—C22 118.8 (3)
C14—C5—H5 120.0 C20—C21—H21 120.6
C5—C6—C7 122.4 (3) C22—C21—H21 120.6
C5—C6—H6 118.8 C21—C22—C23 120.4 (4)
C7—C6—H6 118.8 C21—C22—H22 119.8
C8—C7—C6 119.4 (3) C23—C22—H22 119.8
C8—C7—H7 120.3 C18—C23—C22 118.2 (4)
C6—C7—H7 120.3 C18—C23—H23 120.9
C7—C8—C13 121.2 (3) C22—C23—H23 120.9
C7—C8—H8 119.4 N10—C25—H25A 109.5
C13—C8—H8 119.4 N10—C25—H25B 109.5
C13—C9—C11 121.5 (3) H25A—C25—H25B 109.5
C13—C9—C15 119.1 (3) N10—C25—H25C 109.5
C11—C9—C15 119.4 (3) H25A—C25—H25C 109.5
C12—N10—C14 122.5 (2) H25B—C25—H25C 109.5
C12—N10—C25 117.7 (2) O28—S26—O27 115.73 (15)
C14—N10—C25 119.8 (3) O28—S26—O29 114.66 (17)
C9—C11—C1 123.2 (3) O27—S26—O29 115.01 (16)
C9—C11—C12 118.6 (3) O28—S26—C30 102.91 (19)
C1—C11—C12 118.2 (3) O27—S26—C30 102.55 (19)
N10—C12—C4 121.9 (3) O29—S26—C30 103.36 (18)
N10—C12—C11 119.4 (3) F31—C30—F32 109.0 (4)
C4—C12—C11 118.7 (3) F31—C30—F33 107.7 (3)
C9—C13—C8 122.8 (3) F32—C30—F33 107.5 (4)
C9—C13—C14 118.6 (3) F31—C30—S26 111.8 (3)
C8—C13—C14 118.6 (3) F32—C30—S26 110.4 (3)
N10—C14—C5 122.2 (3) F33—C30—S26 110.3 (3)
N10—C14—C13 119.3 (3)
C11—C1—C2—C3 1.2 (6) C6—C5—C14—C13 −1.7 (5)
C1—C2—C3—C4 −1.6 (6) C9—C13—C14—N10 1.2 (4)
C2—C3—C4—C12 0.5 (6) C8—C13—C14—N10 −178.4 (3)
C14—C5—C6—C7 0.6 (5) C9—C13—C14—C5 −178.6 (3)
C5—C6—C7—C8 0.4 (5) C8—C13—C14—C5 1.8 (4)
C6—C7—C8—C13 −0.3 (5) C13—C9—C15—O17 81.3 (5)
C13—C9—C11—C1 −175.7 (3) C11—C9—C15—O17 −96.5 (4)
C15—C9—C11—C1 2.1 (5) C13—C9—C15—O16 −95.9 (3)
C13—C9—C11—C12 3.3 (5) C11—C9—C15—O16 86.3 (4)
C15—C9—C11—C12 −178.9 (3) O17—C15—O16—C18 −1.8 (5)
C2—C1—C11—C9 179.1 (3) C9—C15—O16—C18 175.4 (3)
C2—C1—C11—C12 0.1 (5) C15—O16—C18—C19 85.5 (4)
C14—N10—C12—C4 177.5 (3) C15—O16—C18—C23 −97.1 (4)
C25—N10—C12—C4 −2.5 (4) C23—C18—C19—C20 0.1 (5)
C14—N10—C12—C11 −2.5 (4) O16—C18—C19—C20 177.4 (3)
C25—N10—C12—C11 177.4 (3) C18—C19—C20—F24 −178.7 (3)
C3—C4—C12—N10 −179.2 (3) C18—C19—C20—C21 1.3 (6)
C3—C4—C12—C11 0.8 (5) F24—C20—C21—C22 178.7 (3)
C9—C11—C12—N10 −0.1 (4) C19—C20—C21—C22 −1.3 (6)
C1—C11—C12—N10 178.9 (3) C20—C21—C22—C23 −0.2 (6)
C9—C11—C12—C4 179.8 (3) C19—C18—C23—C22 −1.5 (6)
C1—C11—C12—C4 −1.1 (4) O16—C18—C23—C22 −178.9 (3)
C11—C9—C13—C8 175.7 (3) C21—C22—C23—C18 1.6 (6)
C15—C9—C13—C8 −2.0 (5) O28—S26—C30—F31 59.7 (3)
C11—C9—C13—C14 −3.9 (4) O27—S26—C30—F31 −179.8 (3)
C15—C9—C13—C14 178.4 (3) O29—S26—C30—F31 −60.0 (3)
C7—C8—C13—C9 179.6 (3) O28—S26—C30—F32 −61.8 (3)
C7—C8—C13—C14 −0.8 (5) O27—S26—C30—F32 58.7 (3)
C12—N10—C14—C5 −178.2 (3) O29—S26—C30—F32 178.6 (3)
C25—N10—C14—C5 1.9 (4) O28—S26—C30—F33 179.5 (3)
C12—N10—C14—C13 2.0 (4) O27—S26—C30—F33 −60.0 (3)
C25—N10—C14—C13 −178.0 (3) O29—S26—C30—F33 59.8 (3)
C6—C5—C14—N10 178.5 (3)

Hydrogen-bond geometry (Å, º)

Cg4 is the centroid of the C18–C23 ring.

D—H···A D—H H···A D···A D—H···A
O1W—H1W···O29i 0.85 (3) 2.24 (3) 3.071 (5) 172 (4)
O1W—H2W···O28 0.89 (3) 1.99 (3) 2.873 (5) 176 (8)
C1—H1···O1W 0.93 2.51 3.365 (7) 152
C3—H3···O29ii 0.93 2.60 3.298 (5) 133
C19—H19···O1W 0.93 2.60 3.415 (7) 145
C25—H25A···O27iii 0.96 2.53 3.424 (5) 155
C25—H25C···Cg4ii 0.96 2.64 3.527 (4) 154

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

C—F···π interactions (Å,°)

X I J I···J X···J XI···J
C20 F24 Cg2iv 3.743 (3) 4.139 (5) 97.6 (2)
C20 F24 Cg2v 3.854 (4) 4.188 (5) 94.9 (3)
C30 F31 Cg1v 3.665 (4) 4.519 (6) 123.6 (3)
C30 F31 Cg3v 3.910 (4) 4.049 (6) 86.7 (3)
C30 F33 Cg3v 3.654 (4) 4.049 (6) 97.7 (3)

Symmetry codes: (iv) x - 1, y, z; (v) -x + 1, -y + 2, -z + 1. Cg1, Cg2 and Cg3 are the centroids of the C9/N10/C11–C14, C1–C4/C11/C12 and C5–C8/C13/C14 rings, respectively.

π–π interactions (Å,°)

I J CgI···CgJ Dihedral angle CgIPerp CgIOffset
1 1vi 3.990 (2) 0 3.591 (2) 1.739 (2)
1 3vi 3.645 (2) 2.08 (17) 3.557 (2) 0.796 (2)
2 3vi 3.907 (2) 3.85 (19) 3.431 (2) 1.863 (2)
3 1vi 3.645 (2) 2.08 (17) 3.546 (2) 0.844 (2)
3 2vi 3.907 (2) 3.85 (19) 3.548 (2) 1.629 (2)

Symmetry codes: (vi) -x + 1, -y + 1, -z. Notes: Cg1, Cg2 and Cg3 are the centroids of the C9/N10/C11–C14, C1–C4/C11/C12 and C5–C8/C13/C14 rings, respectively. CgI···CgJ is the distance between ring centroids. The dihedral angle is that between the planes of the rings I and J. CgIPerp is the perpendicular distance of CgI from ring J. CgIOffset is the distance between CgI and the perpendicular projection of CgJ on ring I.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5452).

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 datablock(s) global, I. DOI: 10.1107/S1600536812003054/xu5452sup1.cif

e-68-0o625-sup1.cif (29.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812003054/xu5452Isup2.hkl

e-68-0o625-Isup2.hkl (184.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812003054/xu5452Isup3.cml

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


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