organic compounds
1-Chloromethyl-4-aza-1-azoniabicyclo[2.2.2]octane tetrafluoroborate deuterochloroform solvate
aDepartment of Chemistry, University of Durham, South Road, Durham DH1 3LE, England
*Correspondence e-mail: a.s.batsanov@durham.ac.uk
The title structure, C7H14ClN2+·BF4−·CDCl3, comprises 1-chloromethyl-4-aza-1-azoniabicyclo[2.2.2]octane cations, BF4− anions and CDCl3 solvent molecules, each having Cs The cation has a and the anion and solvent molecule are connected via a C—D⋯F interaction.
Comment
In the course of our studies of electrophilic fluorination methodology (Chambers et al., 2004), 1-chloromethyl-4-aza-1-azoniabicyclo[2.2.2]octane tetrafluoroborate deuterochloroform solvate, (I), was obtained as a by-product in the reaction of `Selectfluor', (II), with N-ethylpiperidine. Compound (I) was obtained by recrystallization from deuterochloroform. The of solvent-free 1-chloromethyl-4-aza-1-azoniabicyclo[2.2.2]octane tetrafluoroborate has been reported previously by Banks et al. (1993).
The cation, anion and solvent molecule (Fig. 1 and Table 1) all lie on a crystallographic mirror plane, which passes through atoms Cl1/N1/N2/C1–C3 of the cation (which, therefore, has a around the N1—C1 bond), atoms B, F1 and F2 of the anion, and atoms C6, Cl3 and D of the deuterochloroform molecule. The solvent molecule and the anion are linked by a C6—D⋯F1 hydrogen bond (Table 2) The N—C bonds at quaternized atom N1 are longer by 0.047 (4) Å than at N2.
Experimental
A mixture comprising (II) (3.5 g, 12.1 mmol) and N-ethylpiperidine (1.0 g, 11.1 mmol) in acetonitrile was heated at reflux temperature 355 K for 18 h. The reaction mixture appeared dark red in colour. On completion of the reaction, the mixture was poured into water and extracted with dichloromethane (3 × 100 ml). The organic phase was dried with magnesium sulfate. After evaporation, the crude product was purified by distillation on a Kugelrohr apparatus. Crystals of X-ray quality were grown from a deuterochloroform solution of the non-volatile residue at room temperature.
Crystal data
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Refinement
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All H and D atoms were refined isotropically with C—H bond distances in the range 0.93 (3)–0.99 (3) Å and C—D distances of 0.90 (4) Å.
Data collection: SMART (Bruker, 1999); cell SMART; data reduction: SAINT (Bruker, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1998); software used to prepare material for publication: SHELXTL.
Supporting information
https://doi.org/10.1107/S1600536805004411/tk6209sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536805004411/tk6209Isup2.hkl
Data collection: SMART (Bruker, 1999); cell
SMART; data reduction: SAINT (Bruker, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1998); software used to prepare material for publication: SHELXTL.C7H14ClN2+·BF4−·CDCl3 | F(000) = 744 |
Mr = 368.84 | Dx = 1.725 Mg m−3 |
Orthorhombic, Pnma | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ac 2n | Cell parameters from 884 reflections |
a = 22.368 (3) Å | θ = 12.2–25.4° |
b = 8.4961 (11) Å | µ = 0.86 mm−1 |
c = 7.4726 (10) Å | T = 120 K |
V = 1420.1 (3) Å3 | Plate, colourless |
Z = 4 | 0.50 × 0.20 × 0.06 mm |
Bruker SMART 1K CCD area-detector diffractometer | 2037 independent reflections |
Radiation source: fine-focus sealed tube | 1760 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.045 |
Detector resolution: 8 pixels mm-1 | θmax = 29.1°, θmin = 1.8° |
ω scans | h = −30→30 |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | k = −11→11 |
Tmin = 0.672, Tmax = 0.950 | l = −10→10 |
16850 measured reflections |
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)] = 0.040 | Hydrogen site location: difference Fourier map |
wR(F2) = 0.095 | All H-atom parameters refined |
S = 1.21 | w = 1/[σ2(Fo2) + (0.0364P)2 + 1.1232P] where P = (Fo2 + 2Fc2)/3 |
2037 reflections | (Δ/σ)max = 0.001 |
134 parameters | Δρmax = 0.73 e Å−3 |
0 restraints | Δρmin = −0.46 e Å−3 |
Experimental. The data collection nominally covered full sphere of reciprocal space, by a combination of 5 sets of ω scans; each set at different φ and/or 2θ angles and each scan (20 sec exposure) covering 0.3° in ω. Crystal to detector distance 4.41 cm. |
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. |
x | y | z | Uiso*/Ueq | ||
Cl1 | 0.25564 (3) | 0.2500 | 0.34874 (9) | 0.01955 (16) | |
N1 | 0.33556 (10) | 0.2500 | 0.6221 (3) | 0.0139 (4) | |
N2 | 0.35116 (11) | 0.2500 | 0.9627 (3) | 0.0189 (5) | |
C1 | 0.33068 (12) | 0.2500 | 0.4210 (4) | 0.0180 (5) | |
H1 | 0.3499 (9) | 0.157 (3) | 0.379 (3) | 0.014 (5)* | |
C2 | 0.40138 (13) | 0.2500 | 0.6669 (4) | 0.0305 (8) | |
H2 | 0.4162 (12) | 0.151 (4) | 0.617 (4) | 0.046 (9)* | |
C3 | 0.40859 (14) | 0.2500 | 0.8711 (4) | 0.0254 (6) | |
H3 | 0.4297 (10) | 0.160 (3) | 0.904 (4) | 0.027 (7)* | |
C4 | 0.30739 (11) | 0.1057 (2) | 0.7039 (3) | 0.0234 (4) | |
H41 | 0.2661 (12) | 0.113 (3) | 0.677 (4) | 0.028 (7)* | |
H42 | 0.3276 (12) | 0.018 (4) | 0.651 (4) | 0.042 (8)* | |
C5 | 0.31737 (10) | 0.1104 (2) | 0.9081 (3) | 0.0218 (4) | |
H51 | 0.2774 (11) | 0.111 (3) | 0.964 (4) | 0.027 (7)* | |
H52 | 0.3387 (11) | 0.022 (3) | 0.943 (4) | 0.031 (7)* | |
F1 | 0.57683 (8) | 0.2500 | 0.6439 (3) | 0.0376 (5) | |
F2 | 0.65427 (8) | 0.2500 | 0.4503 (3) | 0.0317 (4) | |
F3 | 0.66116 (7) | 0.11659 (19) | 0.7124 (2) | 0.0437 (4) | |
B | 0.63872 (15) | 0.2500 | 0.6307 (4) | 0.0205 (6) | |
Cl2 | 0.48099 (2) | 0.07856 (6) | 0.26682 (7) | 0.02478 (14) | |
Cl3 | 0.56793 (4) | 0.2500 | 0.05699 (11) | 0.0326 (2) | |
C6 | 0.52554 (13) | 0.2500 | 0.2552 (4) | 0.0216 (5) | |
D6 | 0.5509 (15) | 0.2500 | 0.349 (5) | 0.019 (8)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0222 (3) | 0.0214 (3) | 0.0150 (3) | 0 | −0.0041 (2) | 0 |
N1 | 0.0171 (10) | 0.0161 (10) | 0.0086 (9) | 0 | −0.0007 (8) | 0 |
N2 | 0.0243 (11) | 0.0173 (11) | 0.0152 (10) | 0 | −0.0005 (9) | 0 |
C1 | 0.0187 (12) | 0.0241 (14) | 0.0112 (11) | 0 | 0.0005 (10) | 0 |
C2 | 0.0164 (13) | 0.060 (2) | 0.0147 (13) | 0 | −0.0011 (11) | 0 |
C3 | 0.0239 (14) | 0.0385 (18) | 0.0140 (13) | 0 | −0.0032 (11) | 0 |
C4 | 0.0417 (12) | 0.0143 (9) | 0.0142 (9) | −0.0067 (9) | −0.0015 (8) | 0.0001 (7) |
C5 | 0.0322 (10) | 0.0181 (9) | 0.0150 (8) | −0.0039 (8) | −0.0018 (8) | 0.0046 (7) |
F1 | 0.0254 (9) | 0.0646 (15) | 0.0228 (9) | 0 | 0.0009 (8) | 0 |
F2 | 0.0347 (10) | 0.0394 (11) | 0.0210 (9) | 0 | 0.0080 (8) | 0 |
F3 | 0.0573 (10) | 0.0285 (8) | 0.0452 (9) | 0.0129 (7) | −0.0061 (7) | 0.0111 (7) |
B | 0.0247 (15) | 0.0180 (14) | 0.0187 (14) | 0 | −0.0002 (12) | 0 |
Cl2 | 0.0308 (3) | 0.0220 (2) | 0.0216 (2) | 0.00027 (19) | 0.00304 (19) | 0.00215 (19) |
Cl3 | 0.0323 (4) | 0.0371 (4) | 0.0285 (4) | 0.000 | 0.0129 (3) | 0 |
C6 | 0.0236 (13) | 0.0245 (14) | 0.0166 (12) | 0 | −0.0011 (11) | 0 |
Cl1—C1 | 1.763 (3) | C4—H42 | 0.96 (3) |
N1—C1 | 1.507 (3) | C4—C5 | 1.543 (3) |
N1—C4 | 1.507 (2) | C5—H52 | 0.93 (3) |
N1—C2 | 1.510 (4) | C5—H51 | 0.99 (3) |
N2—C3 | 1.456 (4) | F1—B | 1.388 (4) |
N2—C5 | 1.464 (2) | F2—B | 1.393 (4) |
C1—H1 | 0.95 (2) | F3—B | 1.381 (2) |
C2—H2 | 0.98 (3) | Cl2—C6 | 1.767 (2) |
C2—C3 | 1.535 (4) | Cl3—C6 | 1.759 (3) |
C3—H3 | 0.93 (3) | C6—D6 | 0.90 (4) |
C4—H41 | 0.95 (3) | ||
C1—N1—C4 | 111.96 (13) | H41—C4—N1 | 105.3 (17) |
C4i—N1—C4 | 108.8 (2) | H42—C4—N1 | 105.6 (18) |
C1—N1—C2 | 107.0 (2) | H41—C4—C5 | 110.6 (17) |
C4—N1—C2 | 108.54 (14) | H42—C4—C5 | 111.1 (19) |
C3—N2—C5 | 108.94 (15) | N1—C4—C5 | 108.63 (17) |
C5—N2—C5i | 108.2 (2) | H52—C5—H51 | 110 (2) |
H1i—C1—H1 | 112 (3) | H52—C5—N2 | 108.0 (17) |
H1—C1—N1 | 107.2 (14) | H51—C5—N2 | 110.3 (16) |
H1—C1—Cl1 | 109.3 (13) | H52—C5—C4 | 109.5 (17) |
N1—C1—Cl1 | 111.99 (18) | H51—C5—C4 | 106.8 (15) |
H2i—C2—H2 | 119 (4) | N2—C5—C4 | 111.79 (17) |
H2—C2—N1 | 104.2 (17) | F3i—B—F3 | 110.3 (3) |
H2—C2—C3 | 110.2 (19) | F3—B—F1 | 109.34 (18) |
N1—C2—C3 | 108.8 (2) | F3—B—F2 | 109.68 (18) |
H3i—C3—H3 | 110 (3) | F1—B—F2 | 108.5 (2) |
H3—C3—N2 | 108.8 (15) | Cl3—C6—Cl2 | 110.21 (11) |
H3—C3—C2 | 108.5 (16) | Cl2i—C6—Cl2 | 111.04 (16) |
N2—C3—C2 | 112.0 (2) | Cl3—C6—D6 | 109 (2) |
H41—C4—H42 | 115 (2) | Cl2—C6—D6 | 108.4 (11) |
C2—N1—C1—Cl1 | 180.0 |
Symmetry code: (i) x, −y+1/2, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C6—D6···F1 | 0.90 (4) | 2.28 (4) | 3.123 (4) | 156 (3) |
Acknowledgements
We thank the Asahi Glass Co. (Japan) for funding (studentship to JT).
References
Banks, R. E., Sharif, I. & Pritchard, R. G. (1993). Acta Cryst. C49, 492–495. CSD CrossRef CAS Web of Science IUCr Journals Google Scholar
Bruker (1998). SHELXTL. Version 5.10. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Bruker (1999). SMART (Version 5.060) and SAINT (Version 6.02A), Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Bruker (2001). SADABS. Version 2.03. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Chambers, R. D., Holling, D., Sandford, G., Batsanov, A. S. & Howard, J. A. K. (2004). J. Fluorine Chem. 125, 661–671. Web of Science CSD CrossRef CAS Google Scholar
Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany. Google Scholar
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