Abstract
The title compound, C15H20N2O2 2+·2PF6 −, was prepared by anion exchange of two bromide ions in the ionic liquid 2,2′-bis-(pyridinium-1-ylmethyl)-propane-1,3-diol dibromide with potassium hexafluorophosphate. The two pyridine rings are planar (r.m.s. deviations = 0.008 and 0.00440 Å) and make a dihedral angle of 44.0 (2)°. Intermolecular O—H⋯F and C—H⋯F interactions occur. The four F atoms in each anion were refined as disordered over two sets of sites with an occupancy ration of 0.700 (19):0.300 (19).
Related literature
For properties and applications of ionic liquids, see: Welton (1999 ▶). For dicationic ionic liquids, see: Liang et al. (2008 ▶); Geng et al. (2010 ▶); Yuan et al. (2010 ▶); Yang et al. (2010 ▶). For the synthesis of dicationic ionic liquids, see: Yuan et al. (2010 ▶). For bond-length data, see: Allen et al. (1987 ▶).
Experimental
Crystal data
C15H20N2O2 2+·2PF6 −
M r = 550.27
Monoclinic,
a = 11.955 (2) Å
b = 13.796 (3) Å
c = 12.707 (3) Å
β = 95.17 (3)°
V = 2087.3 (7) Å3
Z = 4
Mo Kα radiation
μ = 0.33 mm−1
T = 293 K
0.30 × 0.20 × 0.10 mm
Data collection
Enraf–Nonius CAD-4 diffractometer
Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.907, T max = 0.968
4027 measured reflections
3835 independent reflections
2564 reflections with I > 2σ(I)
R int = 0.031
3 standard reflections every 200 reflections intensity decay: 1%
Refinement
R[F 2 > 2σ(F 2)] = 0.053
wR(F 2) = 0.141
S = 1.04
3835 reflections
372 parameters
H-atom parameters constrained
Δρmax = 0.36 e Å−3
Δρmin = −0.26 e Å−3
Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1994 ▶); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo,1995 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811013080/im2266sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013080/im2266Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C6—H6B⋯O1 | 0.97 | 2.47 | 2.831 (5) | 102 |
| C10—H10B⋯O2 | 0.97 | 2.44 | 2.796 (5) | 102 |
| O1—H1A⋯F8i | 0.82 | 2.29 | 2.898 (8) | 131 |
| O2—H2A⋯F1 | 0.82 | 2.49 | 2.973 (11) | 119 |
| C1—H1B⋯F6 | 0.93 | 2.40 | 3.280 (4) | 158 |
| C11—H11A⋯F10i | 0.93 | 2.31 | 3.087 (7) | 141 |
Symmetry code: (i)
.
Acknowledgments
We acknowledge the National Natural Science Foundation of China (No. 51003047) and the Foundation for Young Teachers Scholarship of Nanjing University of Technology, Jiangsu, China (No. 39729005) for financial support. The authors thank the Centre of Testing and Analysis, Nanjing University, for the data collection.
supplementary crystallographic information
Comment
Ionic liquids (ILs) have enjoyed vast research interests in recent years because of their unique physicochemical properties (Welton, 1999). Geminal dicationic ionic liquids have been shown to possess superior properties in terms of thermal stability and volatility compared to traditional ionic liquids (ILs) (Liang et al., 2008). Consequently, they have been proposed as solvents in high-temperature reactions, as novel high-temperature lubricants or ultrastable separation phases (Yang et al., 2010).
As part of our ongoing studies on new geminal dicationic ionic liquids (Geng et al., 2010; Yuan et al., 2010), we here report the crystal structure of the title compound (I).
The atom-numbering scheme of (I) is shown in Fig.1. Intramolecular C—H···O hydrogen bonds are observed between the methylene groups next to the pyridine N atoms ans the hydroxy groups. All bond lengths are within normal ranges (Allen et al., 1987). The two pyridine rings are planar (r.m.s. deviations = 0.008 and 0.004 Å) and make a dihedral angle of 44.0 (2)°. (Table 1, Fig. 1).
Experimental
A mixture of pyridine (1.98 g, 25 mmol) and 2,2-bis-(bromomethyl)-propane-1,3-diol (2.60 g, 10 mmol) was stirred vigorously at 387 K for 16 h. After cooling to room temperature, the crude product was washed with acetonitrile. The resulting solid collected by filtration was treated with water (20 ml) as well as KPF6 (3.68 g, 20 mmol) and the reaction mixture was stirred at room temperature for 1 h. After filtration, the white solid was washed with ethanol and dried in vacuo to give the title compound (I) (4.82 g, 88%). M.p. 508–510 K. Crystals of (I) suitable for X-ray diffraction were obtained by slow evaporation of a methanolic solution. 1H NMR (DMSO, δ, p.p.m.) 8.92 (t, 4 H), 8.68 (m, 2 H), 8.20 (m, 4 H), 5.57 (s, 2 H) 4.79 (s, 4 H), 3.16 (s, 4 H).
Refinement
In both hexafluorophosphate groups fluorine atoms have strong oscillations, while central P atoms are fixed. Four fluorine positions in each anion have therefore been split over two positions each. All H atoms were positioned geometrically, with C—H = 0.93, 0.96 and 0.97 Å for methine, methyl, methylene H, respectively, and constrained to ride on their parent atoms, with Uiso(H) = xUeq(C), where x= 1.5 for methyl H and x = 1.2 for methylene H atoms.
Figures
Fig. 1.
A view of the molecular structure of (I) showing the atom-numbering scheme and 30% displacement ellipsoids. Dashed lines indicte hydrogen bonds.
Crystal data
| C15H20N2O22+·2PF6− | F(000) = 1112 |
| Mr = 550.27 | Dx = 1.751 Mg m−3 |
| Monoclinic, P21/n | Melting point = 508–510 K |
| Hall symbol: -P 2yn | Mo Kα radiation, λ = 0.71073 Å |
| a = 11.955 (2) Å | Cell parameters from 25 reflections |
| b = 13.796 (3) Å | θ = 9–13° |
| c = 12.707 (3) Å | µ = 0.33 mm−1 |
| β = 95.17 (3)° | T = 293 K |
| V = 2087.3 (7) Å3 | Block, colorless |
| Z = 4 | 0.30 × 0.20 × 0.10 mm |
Data collection
| Enraf–Nonius CAD-4 diffractometer | 2564 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.031 |
| graphite | θmax = 25.4°, θmin = 2.2° |
| ω/2θ scans | h = 0→14 |
| Absorption correction: ψ scan (North et al., 1968) | k = 0→16 |
| Tmin = 0.907, Tmax = 0.968 | l = −15→15 |
| 4027 measured reflections | 3 standard reflections every 200 reflections |
| 3835 independent reflections | intensity decay: 1% |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.053 | H-atom parameters constrained |
| wR(F2) = 0.141 | w = 1/[σ2(Fo2) + (0.0676P)2 + 0.894P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.04 | (Δ/σ)max < 0.001 |
| 3835 reflections | Δρmax = 0.36 e Å−3 |
| 372 parameters | Δρmin = −0.26 e Å−3 |
| 0 restraints | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0115 (12) |
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 | Occ. (<1) | |
| C1 | 0.7687 (3) | 0.3662 (2) | 0.7039 (3) | 0.0524 (8) | |
| H1B | 0.8189 | 0.3301 | 0.6679 | 0.063* | |
| C2 | 0.6564 (3) | 0.3615 (3) | 0.6737 (3) | 0.0634 (10) | |
| H2B | 0.6302 | 0.3240 | 0.6158 | 0.076* | |
| C3 | 0.5825 (3) | 0.4116 (3) | 0.7286 (3) | 0.0684 (11) | |
| H3A | 0.5056 | 0.4069 | 0.7100 | 0.082* | |
| C4 | 0.6229 (3) | 0.4692 (3) | 0.8114 (3) | 0.0659 (10) | |
| H4A | 0.5738 | 0.5046 | 0.8492 | 0.079* | |
| C5 | 0.7352 (3) | 0.4739 (3) | 0.8378 (3) | 0.0523 (8) | |
| H5A | 0.7630 | 0.5135 | 0.8934 | 0.063* | |
| C6 | 0.9277 (3) | 0.4206 (2) | 0.8207 (2) | 0.0443 (7) | |
| H6A | 0.9569 | 0.3568 | 0.8060 | 0.053* | |
| H6B | 0.9362 | 0.4296 | 0.8967 | 0.053* | |
| C7 | 0.9999 (2) | 0.4972 (2) | 0.7698 (2) | 0.0366 (7) | |
| C8 | 0.9657 (3) | 0.5992 (2) | 0.7975 (3) | 0.0491 (8) | |
| H8A | 1.0165 | 0.6459 | 0.7703 | 0.059* | |
| H8B | 0.8903 | 0.6127 | 0.7662 | 0.059* | |
| C9 | 0.9929 (3) | 0.4856 (2) | 0.6495 (2) | 0.0457 (8) | |
| H9A | 0.9157 | 0.4930 | 0.6198 | 0.055* | |
| H9B | 1.0380 | 0.5349 | 0.6191 | 0.055* | |
| C10 | 1.1185 (2) | 0.4719 (2) | 0.8195 (2) | 0.0416 (7) | |
| H10A | 1.1182 | 0.4741 | 0.8958 | 0.050* | |
| H10B | 1.1355 | 0.4058 | 0.8004 | 0.050* | |
| C11 | 1.2419 (3) | 0.6103 (2) | 0.8503 (3) | 0.0504 (8) | |
| H11A | 1.2049 | 0.6237 | 0.9100 | 0.060* | |
| C12 | 1.3296 (3) | 0.6672 (3) | 0.8268 (3) | 0.0621 (10) | |
| H12A | 1.3531 | 0.7187 | 0.8706 | 0.074* | |
| C13 | 1.3824 (3) | 0.6479 (3) | 0.7383 (3) | 0.0649 (10) | |
| H13A | 1.4421 | 0.6862 | 0.7213 | 0.078* | |
| C14 | 1.3471 (3) | 0.5719 (3) | 0.6748 (3) | 0.0609 (10) | |
| H14A | 1.3821 | 0.5587 | 0.6140 | 0.073* | |
| C15 | 1.2606 (3) | 0.5161 (2) | 0.7011 (3) | 0.0496 (8) | |
| H15A | 1.2369 | 0.4639 | 0.6584 | 0.060* | |
| F1 | 0.8561 (10) | 0.3151 (7) | 0.4690 (8) | 0.077 (2) | 0.700 (19) |
| F2 | 0.8566 (7) | 0.0817 (6) | 0.4416 (8) | 0.095 (2) | 0.700 (19) |
| F3 | 0.7337 (10) | 0.1917 (9) | 0.4717 (10) | 0.111 (4) | 0.700 (19) |
| F4 | 0.9805 (9) | 0.2016 (13) | 0.4446 (10) | 0.156 (5) | 0.700 (19) |
| F1' | 0.886 (3) | 0.3061 (18) | 0.448 (2) | 0.107 (10) | 0.300 (19) |
| F2' | 0.867 (3) | 0.0966 (17) | 0.4638 (19) | 0.174 (13) | 0.300 (19) |
| F3' | 0.742 (2) | 0.2191 (19) | 0.455 (3) | 0.111 (8) | 0.300 (19) |
| F4' | 1.0133 (16) | 0.1966 (19) | 0.4436 (13) | 0.083 (4) | 0.300 (19) |
| F5 | 0.8379 (3) | 0.2040 (2) | 0.33183 (18) | 0.1135 (10) | |
| F6 | 0.8902 (3) | 0.19322 (18) | 0.57857 (18) | 0.1019 (9) | |
| F7 | 0.7615 (12) | 0.6122 (8) | 0.5469 (9) | 0.134 (4) | 0.700 (19) |
| F8 | 0.5398 (6) | 0.7270 (5) | 0.5386 (7) | 0.087 (2) | 0.700 (19) |
| F9 | 0.5816 (5) | 0.5722 (6) | 0.5350 (8) | 0.079 (2) | 0.700 (19) |
| F10 | 0.7152 (4) | 0.7742 (5) | 0.5546 (4) | 0.0600 (16) | 0.700 (19) |
| F7' | 0.783 (3) | 0.620 (3) | 0.5484 (16) | 0.144 (13) | 0.300 (19) |
| F8' | 0.5348 (13) | 0.701 (2) | 0.5434 (19) | 0.152 (11) | 0.300 (19) |
| F9' | 0.631 (4) | 0.558 (2) | 0.535 (2) | 0.211 (15) | 0.300 (19) |
| F10' | 0.710 (2) | 0.7468 (16) | 0.5498 (16) | 0.178 (15) | 0.300 (19) |
| F11 | 0.6508 (2) | 0.67341 (18) | 0.41995 (16) | 0.0884 (8) | |
| F12 | 0.6571 (2) | 0.6637 (2) | 0.66872 (17) | 0.0994 (9) | |
| N1 | 0.8068 (2) | 0.42241 (18) | 0.78490 (19) | 0.0401 (6) | |
| N2 | 1.2088 (2) | 0.53542 (17) | 0.78851 (19) | 0.0391 (6) | |
| O1 | 0.9697 (2) | 0.60654 (18) | 0.91006 (18) | 0.0683 (7) | |
| H1A | 0.9511 | 0.6613 | 0.9264 | 0.102* | |
| O2 | 1.0330 (2) | 0.39234 (18) | 0.62617 (18) | 0.0614 (7) | |
| H2A | 1.0300 | 0.3852 | 0.5619 | 0.092* | |
| P1 | 0.86380 (8) | 0.19842 (7) | 0.45439 (7) | 0.0540 (3) | |
| P2 | 0.65577 (8) | 0.66706 (6) | 0.54479 (6) | 0.0474 (3) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.061 (2) | 0.0469 (19) | 0.050 (2) | −0.0083 (17) | 0.0084 (16) | −0.0058 (16) |
| C2 | 0.065 (3) | 0.060 (2) | 0.063 (2) | −0.017 (2) | −0.0047 (19) | −0.0065 (19) |
| C3 | 0.049 (2) | 0.069 (3) | 0.085 (3) | −0.007 (2) | −0.005 (2) | 0.012 (2) |
| C4 | 0.055 (2) | 0.071 (3) | 0.073 (3) | 0.006 (2) | 0.0133 (19) | 0.003 (2) |
| C5 | 0.056 (2) | 0.055 (2) | 0.0466 (19) | 0.0023 (17) | 0.0099 (16) | 0.0003 (16) |
| C6 | 0.0475 (19) | 0.0442 (18) | 0.0407 (17) | 0.0027 (15) | 0.0015 (14) | 0.0090 (14) |
| C7 | 0.0403 (17) | 0.0352 (16) | 0.0338 (15) | −0.0004 (13) | 0.0009 (12) | 0.0023 (12) |
| C8 | 0.053 (2) | 0.0432 (19) | 0.050 (2) | 0.0045 (15) | 0.0001 (15) | 0.0020 (15) |
| C9 | 0.0509 (19) | 0.051 (2) | 0.0345 (16) | −0.0036 (15) | −0.0014 (14) | 0.0063 (14) |
| C10 | 0.0473 (18) | 0.0388 (17) | 0.0377 (16) | −0.0003 (14) | −0.0014 (13) | 0.0045 (13) |
| C11 | 0.054 (2) | 0.052 (2) | 0.0449 (19) | −0.0033 (16) | 0.0038 (15) | −0.0099 (15) |
| C12 | 0.055 (2) | 0.060 (2) | 0.071 (3) | −0.0092 (18) | 0.0026 (19) | −0.0154 (19) |
| C13 | 0.049 (2) | 0.058 (2) | 0.089 (3) | −0.0039 (18) | 0.015 (2) | 0.006 (2) |
| C14 | 0.051 (2) | 0.071 (3) | 0.063 (2) | 0.0043 (19) | 0.0186 (18) | −0.001 (2) |
| C15 | 0.048 (2) | 0.054 (2) | 0.0475 (19) | 0.0074 (16) | 0.0065 (15) | −0.0106 (16) |
| F1 | 0.109 (5) | 0.053 (3) | 0.066 (4) | 0.004 (3) | −0.012 (4) | 0.003 (2) |
| F2 | 0.141 (5) | 0.050 (3) | 0.088 (5) | 0.010 (3) | −0.032 (3) | −0.037 (3) |
| F3 | 0.079 (4) | 0.123 (8) | 0.137 (6) | −0.047 (5) | 0.039 (4) | −0.036 (6) |
| F4 | 0.027 (5) | 0.255 (9) | 0.188 (7) | 0.012 (5) | 0.012 (4) | −0.044 (6) |
| F1' | 0.15 (2) | 0.068 (11) | 0.107 (14) | −0.060 (13) | 0.004 (11) | −0.009 (8) |
| F2' | 0.40 (3) | 0.052 (9) | 0.055 (8) | −0.032 (11) | −0.054 (11) | −0.024 (7) |
| F3' | 0.058 (11) | 0.084 (11) | 0.194 (18) | 0.014 (10) | 0.019 (10) | 0.027 (10) |
| F4' | 0.014 (8) | 0.159 (11) | 0.076 (7) | 0.005 (7) | 0.009 (5) | −0.018 (6) |
| F5 | 0.157 (3) | 0.137 (3) | 0.0422 (14) | 0.001 (2) | −0.0148 (15) | −0.0030 (14) |
| F6 | 0.180 (3) | 0.0738 (16) | 0.0473 (14) | 0.0147 (17) | −0.0141 (15) | −0.0025 (11) |
| F7 | 0.088 (6) | 0.116 (6) | 0.196 (9) | 0.047 (4) | −0.005 (5) | −0.029 (5) |
| F8 | 0.100 (6) | 0.066 (3) | 0.094 (4) | 0.035 (3) | 0.009 (3) | −0.011 (2) |
| F9 | 0.095 (4) | 0.056 (4) | 0.087 (4) | −0.028 (2) | 0.010 (2) | −0.005 (3) |
| F10 | 0.088 (3) | 0.043 (3) | 0.050 (2) | −0.032 (2) | 0.0108 (17) | −0.0115 (18) |
| F7' | 0.085 (12) | 0.27 (3) | 0.083 (11) | 0.101 (15) | 0.022 (8) | 0.049 (13) |
| F8' | 0.034 (8) | 0.29 (3) | 0.130 (14) | −0.055 (12) | 0.014 (7) | 0.024 (15) |
| F9' | 0.47 (5) | 0.050 (9) | 0.121 (15) | −0.05 (2) | 0.08 (3) | −0.008 (8) |
| F10' | 0.35 (4) | 0.089 (12) | 0.075 (8) | −0.151 (17) | 0.050 (11) | −0.032 (7) |
| F11 | 0.131 (2) | 0.0975 (18) | 0.0378 (12) | −0.0269 (16) | 0.0152 (12) | −0.0127 (11) |
| F12 | 0.151 (2) | 0.109 (2) | 0.0386 (13) | −0.0268 (18) | 0.0083 (13) | 0.0125 (12) |
| N1 | 0.0438 (15) | 0.0395 (14) | 0.0369 (13) | −0.0014 (12) | 0.0040 (11) | 0.0062 (11) |
| N2 | 0.0394 (14) | 0.0395 (14) | 0.0378 (14) | 0.0011 (11) | −0.0003 (11) | −0.0022 (11) |
| O1 | 0.094 (2) | 0.0608 (16) | 0.0497 (15) | 0.0114 (14) | 0.0054 (13) | −0.0156 (12) |
| O2 | 0.0687 (16) | 0.0663 (17) | 0.0485 (14) | 0.0037 (13) | 0.0019 (12) | −0.0185 (12) |
| P1 | 0.0626 (7) | 0.0553 (6) | 0.0426 (5) | −0.0065 (5) | −0.0043 (4) | −0.0053 (4) |
| P2 | 0.0626 (6) | 0.0428 (5) | 0.0374 (5) | −0.0009 (4) | 0.0071 (4) | −0.0009 (4) |
Geometric parameters (Å, °)
| C1—N1 | 1.336 (4) | C12—C13 | 1.365 (5) |
| C1—C2 | 1.364 (5) | C12—H12A | 0.9300 |
| C1—H1B | 0.9300 | C13—C14 | 1.365 (5) |
| C2—C3 | 1.362 (6) | C13—H13A | 0.9300 |
| C2—H2B | 0.9300 | C14—C15 | 1.355 (5) |
| C3—C4 | 1.372 (6) | C14—H14A | 0.9300 |
| C3—H3A | 0.9300 | C15—N2 | 1.346 (4) |
| C4—C5 | 1.356 (5) | C15—H15A | 0.9300 |
| C4—H4A | 0.9300 | F1—P1 | 1.624 (10) |
| C5—N1 | 1.339 (4) | F2—P1 | 1.620 (9) |
| C5—H5A | 0.9300 | F3—P1 | 1.593 (12) |
| C6—N1 | 1.476 (4) | F4—P1 | 1.412 (10) |
| C6—C7 | 1.542 (4) | F1'—P1 | 1.51 (2) |
| C6—H6A | 0.9700 | F2'—P1 | 1.41 (2) |
| C6—H6B | 0.9700 | F3'—P1 | 1.49 (2) |
| C7—C8 | 1.516 (4) | F4'—P1 | 1.805 (18) |
| C7—C9 | 1.532 (4) | F5—P1 | 1.562 (2) |
| C7—C10 | 1.539 (4) | F6—P1 | 1.583 (2) |
| C8—O1 | 1.430 (4) | F7—P2 | 1.471 (12) |
| C8—H8A | 0.9700 | F8—P2 | 1.610 (6) |
| C8—H8B | 0.9700 | F9—P2 | 1.580 (8) |
| C9—O2 | 1.414 (4) | F10—P2 | 1.639 (7) |
| C9—H9A | 0.9700 | F7'—P2 | 1.65 (3) |
| C9—H9B | 0.9700 | F8'—P2 | 1.517 (19) |
| C10—N2 | 1.472 (4) | F9'—P2 | 1.54 (3) |
| C10—H10A | 0.9700 | F10'—P2 | 1.276 (19) |
| C10—H10B | 0.9700 | F11—P2 | 1.585 (2) |
| C11—N2 | 1.336 (4) | F12—P2 | 1.574 (2) |
| C11—C12 | 1.364 (5) | O1—H1A | 0.8200 |
| C11—H11A | 0.9300 | O2—H2A | 0.8200 |
| N1—C1—C2 | 120.2 (3) | C13—C14—H14A | 120.2 |
| N1—C1—H1B | 119.9 | N2—C15—C14 | 120.6 (3) |
| C2—C1—H1B | 119.9 | N2—C15—H15A | 119.7 |
| C3—C2—C1 | 119.9 (4) | C14—C15—H15A | 119.7 |
| C3—C2—H2B | 120.0 | C1—N1—C5 | 120.4 (3) |
| C1—C2—H2B | 120.0 | C1—N1—C6 | 118.9 (3) |
| C2—C3—C4 | 119.2 (4) | C5—N1—C6 | 120.5 (3) |
| C2—C3—H3A | 120.4 | C11—N2—C15 | 120.3 (3) |
| C4—C3—H3A | 120.4 | C11—N2—C10 | 119.3 (3) |
| C5—C4—C3 | 119.4 (4) | C15—N2—C10 | 120.4 (3) |
| C5—C4—H4A | 120.3 | C8—O1—H1A | 109.5 |
| C3—C4—H4A | 120.3 | C9—O2—H2A | 109.5 |
| N1—C5—C4 | 120.9 (3) | F2'—P1—F3' | 102.4 (17) |
| N1—C5—H5A | 119.5 | F2'—P1—F1' | 168.1 (19) |
| C4—C5—H5A | 119.5 | F3'—P1—F1' | 89.3 (15) |
| N1—C6—C7 | 115.4 (2) | F2'—P1—F5 | 97.8 (10) |
| N1—C6—H6A | 108.4 | F4—P1—F5 | 91.1 (5) |
| C7—C6—H6A | 108.4 | F4—P1—F6 | 88.8 (5) |
| N1—C6—H6B | 108.4 | F5—P1—F6 | 179.74 (18) |
| C7—C6—H6B | 108.4 | F4—P1—F3 | 176.7 (8) |
| H6A—C6—H6B | 107.5 | F5—P1—F3 | 91.9 (5) |
| C8—C7—C9 | 109.6 (2) | F6—P1—F3 | 88.2 (5) |
| C8—C7—C10 | 111.9 (2) | F4—P1—F2 | 93.8 (8) |
| C9—C7—C10 | 110.6 (2) | F5—P1—F2 | 86.9 (4) |
| C8—C7—C6 | 111.5 (3) | F6—P1—F2 | 93.4 (4) |
| C9—C7—C6 | 111.3 (2) | F3—P1—F2 | 85.0 (5) |
| C10—C7—C6 | 101.7 (2) | F4—P1—F1 | 92.6 (8) |
| O1—C8—C7 | 108.2 (2) | F5—P1—F1 | 93.2 (4) |
| O1—C8—H8A | 110.1 | F6—P1—F1 | 86.5 (4) |
| C7—C8—H8A | 110.1 | F3—P1—F1 | 88.6 (6) |
| O1—C8—H8B | 110.1 | F2—P1—F1 | 173.6 (5) |
| C7—C8—H8B | 110.1 | F2'—P1—F4' | 88.2 (16) |
| H8A—C8—H8B | 108.4 | F3'—P1—F4' | 168.9 (13) |
| O2—C9—C7 | 108.4 (2) | F1'—P1—F4' | 80.2 (15) |
| O2—C9—H9A | 110.0 | F10'—P2—F8' | 102.6 (19) |
| C7—C9—H9A | 110.0 | F10'—P2—F9' | 160 (3) |
| O2—C9—H9B | 110.0 | F8'—P2—F9' | 96.8 (16) |
| C7—C9—H9B | 110.0 | F7—P2—F12 | 92.0 (5) |
| H9A—C9—H9B | 108.4 | F7—P2—F9 | 92.9 (7) |
| N2—C10—C7 | 115.2 (2) | F12—P2—F9 | 90.6 (4) |
| N2—C10—H10A | 108.5 | F7—P2—F11 | 90.1 (5) |
| C7—C10—H10A | 108.5 | F12—P2—F11 | 177.84 (16) |
| N2—C10—H10B | 108.5 | F9—P2—F11 | 89.8 (4) |
| C7—C10—H10B | 108.5 | F7—P2—F8 | 178.3 (6) |
| H10A—C10—H10B | 107.5 | F12—P2—F8 | 89.7 (3) |
| N2—C11—C12 | 120.6 (3) | F9—P2—F8 | 86.9 (4) |
| N2—C11—H11A | 119.7 | F11—P2—F8 | 88.2 (3) |
| C12—C11—H11A | 119.7 | F7—P2—F10 | 95.5 (6) |
| C11—C12—C13 | 119.3 (3) | F12—P2—F10 | 89.1 (2) |
| C11—C12—H12A | 120.4 | F9—P2—F10 | 171.5 (3) |
| C13—C12—H12A | 120.4 | F11—P2—F10 | 90.2 (2) |
| C14—C13—C12 | 119.7 (3) | F8—P2—F10 | 84.6 (3) |
| C14—C13—H13A | 120.1 | F10'—P2—F7' | 82.6 (18) |
| C12—C13—H13A | 120.1 | F8'—P2—F7' | 174.6 (16) |
| C15—C14—C13 | 119.5 (3) | F9'—P2—F7' | 78 (2) |
| C15—C14—H14A | 120.2 | ||
| N1—C1—C2—C3 | −2.2 (6) | N2—C11—C12—C13 | 1.0 (5) |
| C1—C2—C3—C4 | 2.3 (6) | C11—C12—C13—C14 | −0.1 (6) |
| C2—C3—C4—C5 | −0.8 (6) | C12—C13—C14—C15 | −0.6 (6) |
| C3—C4—C5—N1 | −0.8 (6) | C13—C14—C15—N2 | 0.6 (5) |
| N1—C6—C7—C8 | 63.2 (3) | C2—C1—N1—C5 | 0.6 (5) |
| N1—C6—C7—C9 | −59.6 (3) | C2—C1—N1—C6 | 175.6 (3) |
| N1—C6—C7—C10 | −177.4 (2) | C4—C5—N1—C1 | 0.9 (5) |
| C9—C7—C8—O1 | 178.2 (2) | C4—C5—N1—C6 | −174.0 (3) |
| C10—C7—C8—O1 | −58.7 (3) | C7—C6—N1—C1 | 92.4 (3) |
| C6—C7—C8—O1 | 54.4 (3) | C7—C6—N1—C5 | −92.7 (3) |
| C8—C7—C9—O2 | 175.8 (2) | C12—C11—N2—C15 | −1.0 (5) |
| C10—C7—C9—O2 | 51.9 (3) | C12—C11—N2—C10 | 176.3 (3) |
| C6—C7—C9—O2 | −60.4 (3) | C14—C15—N2—C11 | 0.2 (5) |
| C8—C7—C10—N2 | −59.2 (3) | C14—C15—N2—C10 | −177.1 (3) |
| C9—C7—C10—N2 | 63.4 (3) | C7—C10—N2—C11 | 95.2 (3) |
| C6—C7—C10—N2 | −178.3 (2) | C7—C10—N2—C15 | −87.5 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C6—H6B···O1 | 0.97 | 2.47 | 2.831 (5) | 102 |
| C10—H10B···O2 | 0.97 | 2.44 | 2.796 (5) | 102 |
| O1—H1A···F8i | 0.82 | 2.29 | 2.898 (8) | 131 |
| O2—H2A···F1 | 0.82 | 2.49 | 2.973 (11) | 119 |
| C1—H1B···F6 | 0.93 | 2.40 | 3.280 (4) | 158 |
| C11—H11A···F10i | 0.93 | 2.31 | 3.087 (7) | 141 |
Symmetry codes: (i) x+1/2, −y+3/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IM2266).
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 datablocks global, I. DOI: 10.1107/S1600536811013080/im2266sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013080/im2266Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

