Abstract
The crystal structure of the low-temperature form of the title compound, C4H10NO+·BF4 −, was determined at 80 K. Two reversible phase transitions, at 158/158 and 124/126 K (heating/cooling), were detected by differential scanning calorimetry for this compound, and the sequence of phase transitions was subsequently confirmed by single-crystal X-ray diffraction experiments. The asymmetric unit at 80 K consists of three BF4 − tetrahedral anions and three morpholinium cations (Z′ = 3). Hydrogen-bonded morpholinium cations form chains along the [100] direction. The BF4 − anions are connected to these chains by N—H⋯F hydrogen bonds. In the crystal structure, two different layers perpendicular to the [001] direction can be distinguished, which differ in the geometry of the hydrogen bonds between cationic and anionic species.
Related literature
For the crystal structures of morpholinium chlorate(VII) (isostructural with the title compound) and morpholinium hydrogensulfate, see: Grigoriev et al. (2008 ▶); Yin et al. (2006 ▶).
Experimental
Crystal data
C4H10NO+·BF4 −
M r = 174.94
Orthorhombic,
a = 8.106 (4) Å
b = 9.417 (4) Å
c = 28.572 (11) Å
V = 2181.0 (16) Å3
Z = 12
Mo Kα radiation
μ = 0.17 mm−1
T = 80 (2) K
0.5 × 0.5 × 0.4 mm
Data collection
Kuma KM-4 CCD κ-geometry diffractometer
Absorption correction: none
20616 measured reflections
4642 independent reflections
3913 reflections with I > 2σ(I)
R int = 0.033
Refinement
R[F 2 > 2σ(F 2)] = 0.037
wR(F 2) = 0.092
S = 1.13
4642 reflections
298 parameters
H-atom parameters constrained
Δρmax = 0.46 e Å−3
Δρmin = −0.31 e Å−3
Data collection: CrysAlis CCD (Oxford Diffraction, 2006 ▶); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2006 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg, 1998 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808004339/gk2132sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808004339/gk2132Isup2.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 |
|---|---|---|---|---|
| N1—H1C⋯F2 | 0.92 | 1.96 | 2.742 (2) | 142 |
| N1—H1D⋯O3i | 0.92 | 1.96 | 2.857 (2) | 164 |
| N2—H2C⋯F8 | 0.92 | 1.96 | 2.799 (2) | 151 |
| N2—H2D⋯O2ii | 0.92 | 1.95 | 2.842 (2) | 164 |
| N3—H3C⋯F9 | 0.92 | 1.96 | 2.742 (2) | 141 |
| N3—H3D⋯O1i | 0.92 | 1.96 | 2.856 (2) | 164 |
Symmetry codes: (i)
; (ii)
.
supplementary crystallographic information
Comment
The morpholinium tetrafluoroborate (I) undergoes two reversible phase transitions at 158/158 K and 124/126 K (heating/cooling). At the room temperature it crystallizes in the orthorhombic space group Pnma with Z'=1. The intermediate phase appeared to be incommensurately modulated. The structure of (I) in the low-temperature phase contains ordered BF4- tetrahedral units and morpholinium cations in the chair conformation. The bond distances and angles in the BF4- anions and morpholinium cations are in agreement with the expected values. The N–H morpholinium protons are involved in the hydrogen bonds N–H···O (morpholine-morpholine zigzag chains) and N—H···F with BF4- anions. The tetrahedral BF4- anions occupy voids between morpholinium chains.
The title compound I appeared to be isostructural with morpholinium chlorate(VII) at 100 K (Grigoriev et al., 2008). Both structures are characterized by two independent hydrogen bonded layers and only slight differences in geometry of hydrogen bonds between morpholinium and anionic species are observed.
The room-temperature phase of I is isostructural with the morpholinium hydrogensulfate (Yin et al., 2006). The tetrafluoroborate anions appear to be dynamically disordered in this phase. During the phase transition from modulated to the low temperature phase at 124 K threefold increase of the lattice parameter b is observed.
Experimental
The title compound was prepared by reaction of stoichiometric amounts of morpholine and concentrated tetrafluoroboric acid in water. The resulting solid was recrystallized from methanol at room temperature. The crystal for X-ray measurements was slowly cooled from room temperature to 80 K. During cooling, the crystal undergoes phase transition from centrosymmetric (Pnma), through modulated phase, to the non-centrosymmetric P212121 space group.
Refinement
In the absence of signifiant anomalous scattering effects, Friedel pairs were averaged. All H atoms were found in difference-Fourier maps. In the final refinement, all H atoms were positioned geometrically and treated as riding on their parent atoms, with C–H distances of 0.99 Å and N–H distances of 0.92 Å, and with Uiso(H) values of 1.2Ueq(C) and 1.2Ueq(N).
Figures
Fig. 1.
Asymmetric unit of the title compound with atom labelling scheme. The displacement ellipsoids were drawn at the 50% probability level.
Fig. 2.
Projection of the crystal packing along [100].
Fig. 3.
Two types of chains in the crystal structure of (I). Symmetry codes: (v) 1/2 + x, 1/2 - y, 1 - z; (x) 1 + x, y, z; (xi) 3/2 + x, 1/2 - y,1 - z; (xii) -1/2 + x, 3/2 - y,1 - z; (xiii) -1 + x, y, z; (xiv) -3/2 + x, 3/2 - y, 1 - z.
Crystal data
| C4H10NO+·BF4– | F000 = 1080 |
| Mr = 174.94 | Dx = 1.598 Mg m−3 |
| Orthorhombic, P212121 | Mo Kα radiation λ = 0.71073 Å |
| Hall symbol: P 2ac 2ab | Cell parameters from 14871 reflections |
| a = 8.106 (4) Å | θ = 5–34º |
| b = 9.417 (4) Å | µ = 0.17 mm−1 |
| c = 28.572 (11) Å | T = 80 (2) K |
| V = 2181.0 (16) Å3 | Block, colorless |
| Z = 12 | 0.5 × 0.5 × 0.4 mm |
Data collection
| Kuma KM-4 CCD κ-geometry diffractometer | 3913 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.033 |
| Monochromator: graphite | θmax = 34.3º |
| T = 80(2) K | θmin = 4.8º |
| ω scans | h = −12→9 |
| Absorption correction: none | k = −14→14 |
| 20616 measured reflections | l = −44→32 |
| 4642 independent reflections |
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)] = 0.037 | H-atom parameters constrained |
| wR(F2) = 0.092 | w = 1/[σ2(Fo2) + (0.052P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 1.13 | (Δ/σ)max = 0.001 |
| 4642 reflections | Δρmax = 0.46 e Å−3 |
| 298 parameters | Δρmin = −0.31 e Å−3 |
| Primary atom site location: structure-invariant direct methods | Extinction correction: none |
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 | ||
| B1 | 0.5748 (2) | −0.38148 (19) | 0.66006 (6) | 0.0138 (3) | |
| B2 | 0.38324 (17) | 0.16152 (18) | 0.50547 (6) | 0.0145 (3) | |
| B3 | 0.5721 (2) | −0.36435 (19) | 0.33817 (6) | 0.0137 (3) | |
| F1 | 0.67871 (11) | −0.36736 (13) | 0.69879 (3) | 0.0272 (2) | |
| F2 | 0.52308 (13) | −0.24786 (11) | 0.64441 (4) | 0.0285 (2) | |
| F3 | 0.43715 (11) | −0.46227 (11) | 0.67231 (3) | 0.0207 (2) | |
| F4 | 0.66156 (10) | −0.44725 (10) | 0.62384 (3) | 0.01512 (17) | |
| F5 | 0.35554 (13) | 0.23160 (12) | 0.46328 (3) | 0.0258 (2) | |
| F6 | 0.24001 (11) | 0.09601 (11) | 0.52149 (4) | 0.0257 (2) | |
| F7 | 0.50716 (11) | 0.06012 (10) | 0.50017 (4) | 0.0244 (2) | |
| F8 | 0.43192 (12) | 0.26312 (10) | 0.53898 (3) | 0.01994 (19) | |
| F9 | 0.52566 (14) | −0.23018 (12) | 0.35451 (4) | 0.0333 (3) | |
| F10 | 0.67387 (11) | −0.35204 (14) | 0.29913 (3) | 0.0306 (3) | |
| F11 | 0.43177 (11) | −0.44221 (11) | 0.32671 (3) | 0.0222 (2) | |
| F12 | 0.65993 (10) | −0.43246 (10) | 0.37371 (3) | 0.01573 (18) | |
| O1 | 0.69421 (11) | 0.25053 (12) | 0.67290 (4) | 0.0142 (2) | |
| O2 | 0.23260 (11) | 0.76931 (12) | 0.49397 (4) | 0.0166 (2) | |
| O3 | 0.69339 (11) | 0.26920 (12) | 0.32955 (4) | 0.0151 (2) | |
| N1 | 0.45612 (14) | 0.02870 (13) | 0.66772 (4) | 0.0111 (2) | |
| H1C | 0.4314 | −0.0664 | 0.6654 | 0.013* | |
| H1D | 0.3585 | 0.0784 | 0.6690 | 0.013* | |
| N2 | 0.45949 (13) | 0.54141 (13) | 0.50542 (4) | 0.0130 (2) | |
| H2C | 0.4778 | 0.4455 | 0.5086 | 0.016* | |
| H2D | 0.5599 | 0.5868 | 0.5063 | 0.016* | |
| N3 | 0.45585 (14) | 0.04709 (13) | 0.33294 (4) | 0.0113 (2) | |
| H3C | 0.4306 | −0.0480 | 0.3350 | 0.014* | |
| H3D | 0.3586 | 0.0971 | 0.3311 | 0.014* | |
| C1 | 0.55316 (17) | 0.05500 (16) | 0.71154 (5) | 0.0133 (3) | |
| H1A | 0.6538 | −0.0046 | 0.7117 | 0.016* | |
| H1B | 0.4861 | 0.0300 | 0.7393 | 0.016* | |
| C2 | 0.60018 (17) | 0.21069 (18) | 0.71332 (5) | 0.0154 (3) | |
| H2A | 0.4989 | 0.2693 | 0.7149 | 0.018* | |
| H2B | 0.6659 | 0.2291 | 0.7419 | 0.018* | |
| C3 | 0.59955 (16) | 0.22934 (17) | 0.63068 (5) | 0.0139 (3) | |
| H3A | 0.6654 | 0.2594 | 0.6032 | 0.017* | |
| H3B | 0.4985 | 0.2883 | 0.6318 | 0.017* | |
| C4 | 0.55267 (18) | 0.07415 (16) | 0.62565 (5) | 0.0137 (3) | |
| H4A | 0.4855 | 0.0607 | 0.5970 | 0.016* | |
| H4B | 0.6535 | 0.0155 | 0.6228 | 0.016* | |
| C5 | 0.35391 (17) | 0.59281 (18) | 0.54488 (5) | 0.0160 (3) | |
| H5A | 0.4122 | 0.5791 | 0.5750 | 0.019* | |
| H5B | 0.2498 | 0.5379 | 0.5459 | 0.019* | |
| C6 | 0.31647 (17) | 0.74878 (17) | 0.53769 (5) | 0.0179 (3) | |
| H6A | 0.2465 | 0.7838 | 0.5636 | 0.022* | |
| H6B | 0.4206 | 0.8038 | 0.5378 | 0.022* | |
| C7 | 0.33543 (18) | 0.72648 (17) | 0.45575 (5) | 0.0166 (3) | |
| H7A | 0.4384 | 0.7830 | 0.4560 | 0.020* | |
| H7B | 0.2777 | 0.7450 | 0.4258 | 0.020* | |
| C8 | 0.37715 (17) | 0.56993 (17) | 0.45929 (5) | 0.0149 (3) | |
| H8A | 0.2751 | 0.5126 | 0.4567 | 0.018* | |
| H8B | 0.4517 | 0.5426 | 0.4334 | 0.018* | |
| C9 | 0.54945 (18) | 0.09205 (16) | 0.37573 (5) | 0.0140 (3) | |
| H9A | 0.6502 | 0.0335 | 0.3791 | 0.017* | |
| H9B | 0.4803 | 0.0782 | 0.4039 | 0.017* | |
| C10 | 0.59621 (16) | 0.24721 (16) | 0.37110 (5) | 0.0147 (3) | |
| H10A | 0.4950 | 0.3059 | 0.3695 | 0.018* | |
| H10B | 0.6601 | 0.2771 | 0.3989 | 0.018* | |
| C11 | 0.60280 (17) | 0.22966 (17) | 0.28841 (5) | 0.0153 (3) | |
| H11A | 0.6707 | 0.2484 | 0.2603 | 0.018* | |
| H11B | 0.5014 | 0.2878 | 0.2862 | 0.018* | |
| C12 | 0.55689 (17) | 0.07375 (16) | 0.29006 (5) | 0.0132 (3) | |
| H12A | 0.4929 | 0.0480 | 0.2618 | 0.016* | |
| H12B | 0.6580 | 0.0148 | 0.2908 | 0.016* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| B1 | 0.0138 (6) | 0.0131 (8) | 0.0143 (7) | −0.0009 (6) | −0.0009 (5) | −0.0013 (6) |
| B2 | 0.0134 (5) | 0.0142 (7) | 0.0158 (7) | 0.0010 (5) | −0.0013 (5) | −0.0011 (7) |
| B3 | 0.0145 (6) | 0.0128 (8) | 0.0139 (7) | −0.0011 (6) | −0.0002 (5) | 0.0014 (6) |
| F1 | 0.0194 (4) | 0.0478 (7) | 0.0145 (4) | −0.0065 (5) | −0.0016 (3) | −0.0079 (5) |
| F2 | 0.0373 (5) | 0.0128 (5) | 0.0353 (6) | 0.0082 (4) | 0.0082 (4) | 0.0009 (4) |
| F3 | 0.0151 (4) | 0.0218 (5) | 0.0251 (4) | −0.0049 (4) | 0.0030 (4) | 0.0001 (4) |
| F4 | 0.0160 (4) | 0.0152 (4) | 0.0142 (4) | 0.0024 (3) | 0.0004 (3) | −0.0005 (4) |
| F5 | 0.0338 (5) | 0.0305 (6) | 0.0131 (4) | 0.0110 (5) | −0.0033 (4) | 0.0005 (4) |
| F6 | 0.0173 (4) | 0.0230 (5) | 0.0369 (5) | −0.0078 (4) | 0.0042 (4) | −0.0056 (5) |
| F7 | 0.0200 (4) | 0.0197 (5) | 0.0334 (5) | 0.0079 (3) | 0.0017 (4) | 0.0011 (5) |
| F8 | 0.0288 (4) | 0.0143 (5) | 0.0167 (4) | −0.0052 (4) | −0.0058 (3) | 0.0007 (4) |
| F9 | 0.0418 (6) | 0.0122 (5) | 0.0458 (6) | 0.0099 (5) | −0.0112 (5) | −0.0032 (5) |
| F10 | 0.0210 (5) | 0.0571 (8) | 0.0137 (4) | −0.0115 (5) | 0.0012 (3) | 0.0090 (5) |
| F11 | 0.0148 (4) | 0.0249 (5) | 0.0270 (5) | −0.0056 (4) | −0.0027 (4) | 0.0019 (5) |
| F12 | 0.0179 (4) | 0.0160 (4) | 0.0133 (4) | 0.0026 (3) | −0.0011 (3) | 0.0001 (4) |
| O1 | 0.0122 (4) | 0.0166 (5) | 0.0138 (4) | −0.0041 (4) | −0.0018 (3) | 0.0007 (4) |
| O2 | 0.0128 (3) | 0.0165 (5) | 0.0205 (5) | 0.0050 (4) | −0.0019 (4) | −0.0021 (5) |
| O3 | 0.0126 (4) | 0.0160 (5) | 0.0166 (5) | −0.0042 (4) | 0.0008 (3) | −0.0005 (4) |
| N1 | 0.0105 (5) | 0.0092 (5) | 0.0136 (5) | −0.0006 (4) | −0.0003 (4) | −0.0004 (5) |
| N2 | 0.0112 (4) | 0.0094 (5) | 0.0185 (6) | 0.0002 (4) | −0.0001 (4) | 0.0012 (5) |
| N3 | 0.0113 (5) | 0.0096 (5) | 0.0130 (5) | −0.0005 (4) | 0.0011 (4) | 0.0011 (5) |
| C1 | 0.0156 (6) | 0.0139 (7) | 0.0105 (5) | −0.0015 (5) | −0.0007 (5) | −0.0001 (6) |
| C2 | 0.0165 (6) | 0.0172 (7) | 0.0124 (6) | −0.0027 (5) | −0.0005 (4) | −0.0031 (6) |
| C3 | 0.0152 (6) | 0.0147 (7) | 0.0116 (6) | −0.0018 (5) | −0.0009 (4) | 0.0012 (6) |
| C4 | 0.0176 (6) | 0.0129 (7) | 0.0105 (5) | −0.0011 (5) | 0.0009 (5) | −0.0016 (6) |
| C5 | 0.0139 (5) | 0.0237 (8) | 0.0104 (5) | −0.0020 (6) | −0.0014 (5) | −0.0003 (6) |
| C6 | 0.0158 (6) | 0.0199 (8) | 0.0182 (6) | 0.0020 (6) | −0.0018 (5) | −0.0080 (6) |
| C7 | 0.0170 (6) | 0.0169 (7) | 0.0159 (6) | 0.0017 (5) | 0.0001 (5) | 0.0053 (6) |
| C8 | 0.0175 (6) | 0.0152 (7) | 0.0120 (6) | 0.0014 (5) | 0.0019 (5) | −0.0019 (6) |
| C9 | 0.0167 (6) | 0.0144 (7) | 0.0109 (5) | 0.0009 (5) | −0.0001 (5) | 0.0012 (6) |
| C10 | 0.0157 (6) | 0.0141 (7) | 0.0144 (6) | −0.0009 (5) | 0.0004 (4) | −0.0019 (6) |
| C11 | 0.0161 (6) | 0.0162 (7) | 0.0135 (6) | −0.0027 (5) | 0.0014 (4) | 0.0019 (6) |
| C12 | 0.0140 (5) | 0.0153 (7) | 0.0103 (5) | −0.0011 (5) | 0.0008 (5) | −0.0010 (6) |
Geometric parameters (Å, °)
| B1—F3 | 1.3950 (19) | C1—C2 | 1.516 (2) |
| B1—F4 | 1.3964 (19) | C1—H1A | 0.9900 |
| B1—F1 | 1.3971 (18) | C1—H1B | 0.9900 |
| B1—F2 | 1.400 (2) | C2—H2A | 0.9900 |
| B2—F6 | 1.3921 (18) | C2—H2B | 0.9900 |
| B2—F5 | 1.3926 (19) | C3—C4 | 1.517 (2) |
| B2—F7 | 1.3942 (18) | C3—H3A | 0.9900 |
| B2—F8 | 1.4098 (19) | C3—H3B | 0.9900 |
| B3—F10 | 1.3919 (18) | C4—H4A | 0.9900 |
| B3—F11 | 1.3926 (19) | C4—H4B | 0.9900 |
| B3—F12 | 1.3962 (19) | C5—C6 | 1.514 (2) |
| B3—F9 | 1.399 (2) | C5—H5A | 0.9900 |
| O1—C2 | 1.4338 (18) | C5—H5B | 0.9900 |
| O1—C3 | 1.4435 (17) | C6—H6A | 0.9900 |
| O2—C7 | 1.4318 (18) | C6—H6B | 0.9900 |
| O2—C6 | 1.4354 (18) | C7—C8 | 1.516 (2) |
| O3—C11 | 1.4350 (18) | C7—H7A | 0.9900 |
| O3—C10 | 1.4397 (18) | C7—H7B | 0.9900 |
| N1—C4 | 1.4968 (18) | C8—H8A | 0.9900 |
| N1—C1 | 1.4992 (17) | C8—H8B | 0.9900 |
| N1—H1C | 0.9200 | C9—C10 | 1.515 (2) |
| N1—H1D | 0.9200 | C9—H9A | 0.9900 |
| N2—C5 | 1.4960 (18) | C9—H9B | 0.9900 |
| N2—C8 | 1.5014 (18) | C10—H10A | 0.9900 |
| N2—H2C | 0.9200 | C10—H10B | 0.9900 |
| N2—H2D | 0.9200 | C11—C12 | 1.515 (2) |
| N3—C12 | 1.4950 (17) | C11—H11A | 0.9900 |
| N3—C9 | 1.4998 (18) | C11—H11B | 0.9900 |
| N3—H3C | 0.9200 | C12—H12A | 0.9900 |
| N3—H3D | 0.9200 | C12—H12B | 0.9900 |
| F3—B1—F4 | 110.30 (13) | H3A—C3—H3B | 108.1 |
| F3—B1—F1 | 109.61 (13) | N1—C4—C3 | 109.29 (11) |
| F4—B1—F1 | 109.00 (12) | N1—C4—H4A | 109.8 |
| F3—B1—F2 | 109.32 (13) | C3—C4—H4A | 109.8 |
| F4—B1—F2 | 108.22 (13) | N1—C4—H4B | 109.8 |
| F1—B1—F2 | 110.37 (14) | C3—C4—H4B | 109.8 |
| F6—B2—F5 | 111.11 (12) | H4A—C4—H4B | 108.3 |
| F6—B2—F7 | 109.46 (13) | N2—C5—C6 | 109.05 (12) |
| F5—B2—F7 | 110.28 (12) | N2—C5—H5A | 109.9 |
| F6—B2—F8 | 108.12 (12) | C6—C5—H5A | 109.9 |
| F5—B2—F8 | 108.14 (13) | N2—C5—H5B | 109.9 |
| F7—B2—F8 | 109.69 (11) | C6—C5—H5B | 109.9 |
| F10—B3—F11 | 109.85 (13) | H5A—C5—H5B | 108.3 |
| F10—B3—F12 | 108.61 (13) | O2—C6—C5 | 110.10 (12) |
| F11—B3—F12 | 110.21 (13) | O2—C6—H6A | 109.6 |
| F10—B3—F9 | 110.60 (14) | C5—C6—H6A | 109.6 |
| F11—B3—F9 | 109.52 (13) | O2—C6—H6B | 109.6 |
| F12—B3—F9 | 108.03 (13) | C5—C6—H6B | 109.6 |
| C2—O1—C3 | 110.75 (10) | H6A—C6—H6B | 108.2 |
| C7—O2—C6 | 110.50 (10) | O2—C7—C8 | 110.66 (12) |
| C11—O3—C10 | 110.98 (10) | O2—C7—H7A | 109.5 |
| C4—N1—C1 | 110.43 (11) | C8—C7—H7A | 109.5 |
| C4—N1—H1C | 109.6 | O2—C7—H7B | 109.5 |
| C1—N1—H1C | 109.6 | C8—C7—H7B | 109.5 |
| C4—N1—H1D | 109.6 | H7A—C7—H7B | 108.1 |
| C1—N1—H1D | 109.6 | N2—C8—C7 | 109.38 (12) |
| H1C—N1—H1D | 108.1 | N2—C8—H8A | 109.8 |
| C5—N2—C8 | 110.45 (10) | C7—C8—H8A | 109.8 |
| C5—N2—H2C | 109.6 | N2—C8—H8B | 109.8 |
| C8—N2—H2C | 109.6 | C7—C8—H8B | 109.8 |
| C5—N2—H2D | 109.6 | H8A—C8—H8B | 108.2 |
| C8—N2—H2D | 109.6 | N3—C9—C10 | 109.12 (12) |
| H2C—N2—H2D | 108.1 | N3—C9—H9A | 109.9 |
| C12—N3—C9 | 110.09 (11) | C10—C9—H9A | 109.9 |
| C12—N3—H3C | 109.6 | N3—C9—H9B | 109.9 |
| C9—N3—H3C | 109.6 | C10—C9—H9B | 109.9 |
| C12—N3—H3D | 109.6 | H9A—C9—H9B | 108.3 |
| C9—N3—H3D | 109.6 | O3—C10—C9 | 110.34 (12) |
| H3C—N3—H3D | 108.2 | O3—C10—H10A | 109.6 |
| N1—C1—C2 | 108.65 (11) | C9—C10—H10A | 109.6 |
| N1—C1—H1A | 110.0 | O3—C10—H10B | 109.6 |
| C2—C1—H1A | 110.0 | C9—C10—H10B | 109.6 |
| N1—C1—H1B | 110.0 | H10A—C10—H10B | 108.1 |
| C2—C1—H1B | 110.0 | O3—C11—C12 | 110.59 (12) |
| H1A—C1—H1B | 108.3 | O3—C11—H11A | 109.5 |
| O1—C2—C1 | 111.08 (12) | C12—C11—H11A | 109.5 |
| O1—C2—H2A | 109.4 | O3—C11—H11B | 109.5 |
| C1—C2—H2A | 109.4 | C12—C11—H11B | 109.5 |
| O1—C2—H2B | 109.4 | H11A—C11—H11B | 108.1 |
| C1—C2—H2B | 109.4 | N3—C12—C11 | 108.82 (11) |
| H2A—C2—H2B | 108.0 | N3—C12—H12A | 109.9 |
| O1—C3—C4 | 110.22 (12) | C11—C12—H12A | 109.9 |
| O1—C3—H3A | 109.6 | N3—C12—H12B | 109.9 |
| C4—C3—H3A | 109.6 | C11—C12—H12B | 109.9 |
| O1—C3—H3B | 109.6 | H12A—C12—H12B | 108.3 |
| C4—C3—H3B | 109.6 | ||
| C4—N1—C1—C2 | 56.30 (14) | C6—O2—C7—C8 | 61.49 (15) |
| C3—O1—C2—C1 | 61.00 (14) | C5—N2—C8—C7 | 54.94 (14) |
| N1—C1—C2—O1 | −58.22 (14) | O2—C7—C8—N2 | −57.26 (14) |
| C2—O1—C3—C4 | −60.55 (14) | C12—N3—C9—C10 | 57.02 (14) |
| C1—N1—C4—C3 | −56.75 (15) | C11—O3—C10—C9 | 60.49 (15) |
| O1—C3—C4—N1 | 58.12 (14) | N3—C9—C10—O3 | −58.07 (14) |
| C8—N2—C5—C6 | −55.96 (14) | C10—O3—C11—C12 | −60.89 (14) |
| C7—O2—C6—C5 | −62.45 (15) | C9—N3—C12—C11 | −57.07 (14) |
| N2—C5—C6—O2 | 59.27 (14) | O3—C11—C12—N3 | 58.66 (14) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1C···F2 | 0.92 | 1.96 | 2.742 (2) | 142 |
| N1—H1D···O3i | 0.92 | 1.96 | 2.857 (2) | 164 |
| N2—H2C···F8 | 0.92 | 1.96 | 2.799 (2) | 151 |
| N2—H2D···O2ii | 0.92 | 1.95 | 2.842 (2) | 164 |
| N3—H3C···F9 | 0.92 | 1.96 | 2.742 (2) | 141 |
| N3—H3D···O1i | 0.92 | 1.96 | 2.856 (2) | 164 |
| C1—H1B···F1iii | 0.99 | 2.42 | 3.261 (2) | 143 |
| C2—H2B···F10iv | 0.99 | 2.39 | 3.337 (2) | 160 |
| C3—H3A···F5v | 0.99 | 2.45 | 3.413 (2) | 165 |
| C5—H5A···F4vi | 0.99 | 2.47 | 3.384 (2) | 154 |
| C5—H5B···F7i | 0.99 | 2.54 | 3.410 (2) | 147 |
| C6—H6A···F12i | 0.99 | 2.38 | 3.318 (2) | 158 |
| C8—H8B···F12vi | 0.99 | 2.41 | 3.352 (2) | 159 |
| C9—H9B···F5 | 0.99 | 2.45 | 3.233 (2) | 136 |
| C11—H11A···F1vii | 0.99 | 2.41 | 3.373 (2) | 163 |
| C12—H12A···F10viii | 0.99 | 2.40 | 3.237 (2) | 142 |
| C12—H12B···F3ix | 0.99 | 2.54 | 3.429 (2) | 149 |
Symmetry codes: (i) x−1/2, −y+1/2, −z+1; (ii) x+1/2, −y+3/2, −z+1; (iii) −x+1, y+1/2, −z+3/2; (iv) −x+3/2, −y, z+1/2; (v) x+1/2, −y+1/2, −z+1; (vi) x, y+1, z; (vii) −x+3/2, −y, z−1/2; (viii) −x+1, y+1/2, −z+1/2; (ix) x+1/2, −y−1/2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: GK2132).
References
- Brandenburg, K. (1998). DIAMOND University of Bonn, Germany.
- Grigoriev, M. S., German, K. E. & Maruk, A. Y. (2008). Acta Cryst. E64, o390. [DOI] [PMC free article] [PubMed]
- Oxford Diffraction (2006). CrysAlis CCD and CrysAlis RED Versions 1.171. Oxford Diffraction, Abingdon, Oxfordshire, England.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Yin, C.-X., Huo, F.-J. & Yang, P. (2006). Acta Cryst. E62, o2084–o2085.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808004339/gk2132sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808004339/gk2132Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



