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 ▶).
Experimental
Crystal data
C21H15FNO2 +·CF3O3S−·H2O
M r = 499.44
Triclinic,
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
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812003054/xu5452Isup2.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 | 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)
; (ii)
; (iii)
.
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 | I⋯J | X⋯J | X—I⋯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.
Table 3. π–π interactions (Å,°).
Cg1, Cg2 and Cg3 are as defined in Table 2. CgI⋯CgJ 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 | CgI⋯CgJ | 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.
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.
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 m−3 |
| 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 mm−1 |
| 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 Å−3 |
| 3 restraints | Δρmin = −0.28 e Å−3 |
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 | X—I···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).
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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
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812003054/xu5452Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812003054/xu5452Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


