
Supporting information
![]() | Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807022805/om2123sup1.cif |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S1600536807022805/om2123Isup2.hkl |
CCDC reference: 643464
1,4-Diazabicyclo[2.2.2]octane and concentrated nitric acid were obtained from Sigma-Aldrich. All reagents were used without further purification. 1,4-diazabicyclo[2.2.2]octane (0.098 g, 0.87 mmol) and distilled water (5 g, 278 mmol) were placed into a 23 ml Teflon-lined Parr bomb in the molar ratios of 1.0:320 respectively. The pH was adjusted to 1.5 using concentrated HNO3. The reaction vessel was then sealed and heated statically at 120 °C for 10 days. Upon cooling to room temperature, a clear colorless solution was obtained. The solvent was allowed to evaporate at room temperature resulting in colourless crystals of the title compound.
All H atoms of the DABCO carbons were placed in calculated positions whereas those of the DABCO nitrogen were located in a difference Fourier map. The bond distances to H were fixed at 0.97 Å for the carbon atoms and the H atoms were allowed to ride on their bonded C atoms with Uiso = 1.2Ueq(C). Those of the nitrogen atoms were freely refined with a distance restraint of 0.8 Å.
As the field of inorganic organic coordination polymers and metal organic frameworks has developed, it has become increasingly important to explore the oxidation or reduction of organic molecules utlilized in the syntheses of such materials. Consequently the title compound was synthesized as part of an investigation to understand the stability of DABCO under hydrothermal conditions, in the presence of nitrate groups.
Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: CrystalMaker (CrystalMaker Software, 2003) and ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).
C6H14N22+·2NO3− | F(000) = 504 |
Mr = 238.21 | Dx = 1.578 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 2891 reflections |
a = 11.4887 (4) Å | θ = 2.4–30.4° |
b = 6.8821 (2) Å | µ = 0.14 mm−1 |
c = 12.6838 (5) Å | T = 293 K |
β = 91.247 (5)° | Block, colourless |
V = 1002.62 (6) Å3 | 0.2 × 0.2 × 0.1 mm |
Z = 4 |
Bruker APEX II CCD diffractometer | 2891 independent reflections |
Radiation source: fine-focus sealed tube | 1701 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.046 |
ω and φ scans | θmax = 30.4°, θmin = 2.4° |
Absorption correction: multi-scan (SADABS; Sheldrick, 2002) | h = −16→16 |
Tmin = 0.972, Tmax = 0.986 | k = −9→9 |
18932 measured reflections | l = −18→18 |
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)] = 0.052 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.156 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | w = 1/[σ2(Fo2) + (0.0711P)2 + 0.2134P] where P = (Fo2 + 2Fc2)/3 |
2891 reflections | (Δ/σ)max < 0.001 |
153 parameters | Δρmax = 0.33 e Å−3 |
2 restraints | Δρmin = −0.21 e Å−3 |
C6H14N22+·2NO3− | V = 1002.62 (6) Å3 |
Mr = 238.21 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 11.4887 (4) Å | µ = 0.14 mm−1 |
b = 6.8821 (2) Å | T = 293 K |
c = 12.6838 (5) Å | 0.2 × 0.2 × 0.1 mm |
β = 91.247 (5)° |
Bruker APEX II CCD diffractometer | 2891 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2002) | 1701 reflections with I > 2σ(I) |
Tmin = 0.972, Tmax = 0.986 | Rint = 0.046 |
18932 measured reflections |
R[F2 > 2σ(F2)] = 0.052 | 2 restraints |
wR(F2) = 0.156 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | Δρmax = 0.33 e Å−3 |
2891 reflections | Δρmin = −0.21 e Å−3 |
153 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.93691 (19) | 0.7655 (3) | 0.25071 (15) | 0.0463 (5) | |
H1A | 0.9694 | 0.6490 | 0.2827 | 0.056* | |
H1B | 0.8701 | 0.7286 | 0.2072 | 0.056* | |
C2 | 0.90005 (17) | 0.9055 (3) | 0.33541 (16) | 0.0421 (5) | |
H2A | 0.8164 | 0.9245 | 0.3313 | 0.051* | |
H2B | 0.9200 | 0.8530 | 0.4044 | 0.051* | |
C3 | 1.08900 (18) | 1.0677 (3) | 0.33089 (16) | 0.0457 (5) | |
H3A | 1.1094 | 1.0248 | 0.4018 | 0.055* | |
H3B | 1.1280 | 1.1903 | 0.3183 | 0.055* | |
C4 | 1.12770 (17) | 0.9181 (3) | 0.25179 (16) | 0.0463 (5) | |
H4A | 1.1883 | 0.9719 | 0.2084 | 0.056* | |
H4B | 1.1588 | 0.8049 | 0.2882 | 0.056* | |
C5 | 0.9751 (2) | 1.0361 (3) | 0.13096 (14) | 0.0422 (5) | |
H5A | 0.9122 | 0.9972 | 0.0833 | 0.051* | |
H5B | 1.0342 | 1.1006 | 0.0902 | 0.051* | |
C6 | 0.9296 (2) | 1.1734 (3) | 0.21419 (16) | 0.0491 (5) | |
H6A | 0.9641 | 1.3010 | 0.2060 | 0.059* | |
H6B | 0.8458 | 1.1861 | 0.2064 | 0.059* | |
N1 | 0.84994 (15) | 0.4322 (2) | 0.48142 (13) | 0.0409 (4) | |
N2 | 0.96035 (14) | 1.0939 (2) | 0.32027 (12) | 0.0350 (4) | |
N3 | 1.02573 (14) | 0.8620 (2) | 0.18482 (11) | 0.0333 (4) | |
N4 | 0.63928 (13) | 0.0013 (2) | 0.54168 (14) | 0.0405 (4) | |
O1 | 0.92260 (13) | 0.2997 (2) | 0.50023 (11) | 0.0527 (4) | |
O2 | 0.81216 (19) | 0.5294 (3) | 0.55311 (17) | 0.0858 (7) | |
O3 | 0.81960 (15) | 0.4576 (2) | 0.38782 (13) | 0.0601 (5) | |
O4 | 0.59975 (15) | −0.1572 (2) | 0.50989 (12) | 0.0583 (5) | |
O5 | 0.64042 (15) | 0.0298 (3) | 0.63862 (13) | 0.0630 (5) | |
O6 | 0.67368 (18) | 0.1223 (3) | 0.47992 (16) | 0.0897 (7) | |
H30 | 1.0467 (19) | 0.785 (3) | 0.1429 (15) | 0.049 (7)* | |
H20 | 0.9441 (19) | 1.169 (3) | 0.3691 (15) | 0.051 (6)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0612 (13) | 0.0367 (10) | 0.0413 (11) | −0.0152 (9) | 0.0087 (9) | −0.0028 (9) |
C2 | 0.0408 (11) | 0.0442 (11) | 0.0418 (10) | −0.0041 (9) | 0.0109 (8) | 0.0018 (9) |
C3 | 0.0417 (11) | 0.0502 (12) | 0.0452 (11) | −0.0082 (9) | −0.0008 (8) | −0.0153 (9) |
C4 | 0.0377 (10) | 0.0580 (13) | 0.0433 (11) | 0.0053 (9) | 0.0032 (8) | −0.0100 (10) |
C5 | 0.0625 (13) | 0.0363 (10) | 0.0278 (9) | 0.0065 (9) | 0.0019 (8) | 0.0027 (8) |
C6 | 0.0726 (15) | 0.0342 (10) | 0.0407 (11) | 0.0165 (10) | 0.0049 (10) | 0.0040 (8) |
N1 | 0.0438 (9) | 0.0361 (9) | 0.0432 (10) | −0.0021 (7) | 0.0114 (7) | −0.0060 (7) |
N2 | 0.0460 (9) | 0.0304 (8) | 0.0288 (8) | 0.0037 (7) | 0.0061 (6) | −0.0078 (6) |
N3 | 0.0435 (9) | 0.0272 (8) | 0.0292 (8) | 0.0038 (6) | 0.0051 (6) | −0.0065 (6) |
N4 | 0.0344 (8) | 0.0420 (9) | 0.0448 (9) | −0.0061 (7) | −0.0030 (7) | 0.0090 (8) |
O1 | 0.0566 (9) | 0.0528 (9) | 0.0486 (9) | 0.0135 (8) | −0.0027 (7) | −0.0027 (7) |
O2 | 0.0961 (15) | 0.0754 (13) | 0.0876 (14) | 0.0042 (11) | 0.0411 (11) | −0.0400 (11) |
O3 | 0.0643 (10) | 0.0609 (10) | 0.0551 (10) | −0.0022 (8) | −0.0001 (8) | 0.0195 (8) |
O4 | 0.0795 (12) | 0.0405 (9) | 0.0549 (10) | −0.0036 (8) | −0.0013 (8) | −0.0062 (7) |
O5 | 0.0695 (11) | 0.0744 (12) | 0.0444 (9) | −0.0063 (9) | −0.0102 (7) | −0.0050 (8) |
O6 | 0.0924 (15) | 0.0900 (15) | 0.0867 (14) | −0.0397 (12) | 0.0023 (11) | 0.0444 (12) |
C1—N3 | 1.489 (2) | C5—C6 | 1.518 (3) |
C1—C2 | 1.510 (3) | C5—H5A | 0.9700 |
C1—H1A | 0.9700 | C5—H5B | 0.9700 |
C1—H1B | 0.9700 | C6—N2 | 1.488 (3) |
C2—N2 | 1.484 (3) | C6—H6A | 0.9700 |
C2—H2A | 0.9700 | C6—H6B | 0.9700 |
C2—H2B | 0.9700 | N1—O2 | 1.217 (2) |
C3—N2 | 1.492 (3) | N1—O3 | 1.242 (2) |
C3—C4 | 1.511 (3) | N1—O1 | 1.255 (2) |
C3—H3A | 0.9700 | N2—H20 | 0.832 (15) |
C3—H3B | 0.9700 | N3—H30 | 0.793 (16) |
C4—N3 | 1.483 (3) | N4—O6 | 1.215 (2) |
C4—H4A | 0.9700 | N4—O5 | 1.245 (2) |
C4—H4B | 0.9700 | N4—O4 | 1.245 (2) |
C5—N3 | 1.491 (2) | ||
N3—C1—C2 | 108.72 (15) | N3—C5—H5B | 110.0 |
N3—C1—H1A | 109.9 | C6—C5—H5B | 110.0 |
C2—C1—H1A | 109.9 | H5A—C5—H5B | 108.4 |
N3—C1—H1B | 109.9 | N2—C6—C5 | 108.74 (15) |
C2—C1—H1B | 109.9 | N2—C6—H6A | 109.9 |
H1A—C1—H1B | 108.3 | C5—C6—H6A | 109.9 |
N2—C2—C1 | 109.03 (14) | N2—C6—H6B | 109.9 |
N2—C2—H2A | 109.9 | C5—C6—H6B | 109.9 |
C1—C2—H2A | 109.9 | H6A—C6—H6B | 108.3 |
N2—C2—H2B | 109.9 | O2—N1—O3 | 122.6 (2) |
C1—C2—H2B | 109.9 | O2—N1—O1 | 120.3 (2) |
H2A—C2—H2B | 108.3 | O3—N1—O1 | 117.11 (16) |
N2—C3—C4 | 109.12 (15) | C2—N2—C6 | 109.64 (16) |
N2—C3—H3A | 109.9 | C2—N2—C3 | 110.30 (15) |
C4—C3—H3A | 109.9 | C6—N2—C3 | 109.95 (16) |
N2—C3—H3B | 109.9 | C2—N2—H20 | 109.6 (16) |
C4—C3—H3B | 109.9 | C6—N2—H20 | 113.0 (16) |
H3A—C3—H3B | 108.3 | C3—N2—H20 | 104.3 (16) |
N3—C4—C3 | 108.51 (15) | C4—N3—C1 | 109.69 (15) |
N3—C4—H4A | 110.0 | C4—N3—C5 | 110.40 (16) |
C3—C4—H4A | 110.0 | C1—N3—C5 | 110.50 (16) |
N3—C4—H4B | 110.0 | C4—N3—H30 | 108.1 (16) |
C3—C4—H4B | 110.0 | C1—N3—H30 | 107.4 (17) |
H4A—C4—H4B | 108.4 | C5—N3—H30 | 110.7 (16) |
N3—C5—C6 | 108.56 (15) | O6—N4—O5 | 122.1 (2) |
N3—C5—H5A | 110.0 | O6—N4—O4 | 120.9 (2) |
C6—C5—H5A | 110.0 | O5—N4—O4 | 116.99 (17) |
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H30···O4i | 0.79 (2) | 2.01 (2) | 2.778 (2) | 163 (2) |
N3—H30···O5i | 0.79 (2) | 2.42 (2) | 3.063 (2) | 139 (2) |
N2—H20···O1ii | 0.83 (2) | 1.91 (2) | 2.729 (2) | 167 (2) |
N2—H20···O3ii | 0.83 (2) | 2.46 (2) | 3.111 (2) | 136 (2) |
Symmetry codes: (i) x+1/2, −y+1/2, z−1/2; (ii) x, y+1, z. |
Experimental details
Crystal data | |
Chemical formula | C6H14N22+·2NO3− |
Mr | 238.21 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 293 |
a, b, c (Å) | 11.4887 (4), 6.8821 (2), 12.6838 (5) |
β (°) | 91.247 (5) |
V (Å3) | 1002.62 (6) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.14 |
Crystal size (mm) | 0.2 × 0.2 × 0.1 |
Data collection | |
Diffractometer | Bruker APEX II CCD |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2002) |
Tmin, Tmax | 0.972, 0.986 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 18932, 2891, 1701 |
Rint | 0.046 |
(sin θ/λ)max (Å−1) | 0.711 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.052, 0.156, 1.04 |
No. of reflections | 2891 |
No. of parameters | 153 |
No. of restraints | 2 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.33, −0.21 |
Computer programs: APEX2 (Bruker, 2005), SAINT (Bruker, 2005), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), CrystalMaker (CrystalMaker Software, 2003) and ORTEP-3 (Farrugia, 1997), WinGX (Farrugia, 1999).
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H30···O4i | 0.793 (16) | 2.009 (16) | 2.778 (2) | 163 (2) |
N3—H30···O5i | 0.793 (16) | 2.419 (19) | 3.063 (2) | 139 (2) |
N2—H20···O1ii | 0.832 (15) | 1.911 (16) | 2.729 (2) | 167 (2) |
N2—H20···O3ii | 0.832 (15) | 2.46 (2) | 3.111 (2) | 136 (2) |
Symmetry codes: (i) x+1/2, −y+1/2, z−1/2; (ii) x, y+1, z. |
As the field of inorganic organic coordination polymers and metal organic frameworks has developed, it has become increasingly important to explore the oxidation or reduction of organic molecules utlilized in the syntheses of such materials. Consequently the title compound was synthesized as part of an investigation to understand the stability of DABCO under hydrothermal conditions, in the presence of nitrate groups.