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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 13;67(Pt 5):o1104. doi: 10.1107/S1600536811013080

1,1′-[(1,3-Dihydroxypropane-2,2-diyl)dimethylene]dipyridinium bis­(hexa­fluoro­phosphate)

Ai-lin Yuan a, Chun-ling Zheng a, Ling-hua Zhuang b, Chang-sheng Wang a, Guo-wei Wang a,*
PMCID: PMC3089249  PMID: 21754422

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 ▶).graphic file with name e-67-o1104-scheme1.jpg

Experimental

Crystal data

  • C15H20N2O2 2+·2PF6 −

  • M r = 550.27

  • Monoclinic, Inline graphic

  • 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

e-67-o1104-sup1.cif (23.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013080/im2266Isup2.hkl

e-67-o1104-Isup2.hkl (188KB, 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) Inline graphic.

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.

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

e-67-o1104-sup1.cif (23.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013080/im2266Isup2.hkl

e-67-o1104-Isup2.hkl (188KB, hkl)

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


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