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The NNO2 group of the title compound is significantly less twisted with respect to the aromatic ring in comparison to a typical secondary nitramine. The amide nitrogen is trigonally hybridized. The nitramino group is almost planar. The C-C-N-N torsion angles vary between ca 13 and 42°, whereas the twist along the N-N bond is much smaller and amounts to between ca 1 and 15°. Those twist angles are governed by a crystal packing and are much larger in the case of crystals of pure N,4-dinitroaniline in comparison to that of its complex with sulfolane. The deviations of the internal angles of the aromatic ring from 120° do not exceed 3°. The presence of the nitro group increases the C-C-C valence angle of ca 2.0-2.6°, whereas an analogous effect associated with the nitramino group is much smaller (ca 0.3-1.3°), pointing to its weak electron-withdrawing properties. The nitramino group displays no tendency to conjugate with an electron-demanding substituent across the ring. It participates in hydrogen bonding only as a hydrogen-bonding donor. It does not act as a proton acceptor, despite the fact that nitramine rearrangement is catalysed by acids.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768101016548/lc0040sup1.cif
Contains datablocks global, 1, 2

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S0108768101016548/lc00401sup2.fcf
Contains datablock 1

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S0108768101016548/lc00402sup3.fcf
Contains datablock 2

CCDC references: 180196; 180197

Computing details top

For both compounds, cell refinement: KUMA Diffraction Software, ver. KM4b8 (KUMA, 1997); data reduction: KUMA Diffraction Software, DATARED9 (KUMA, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Sheldrick, 1990); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

(1) 'N,4-Dinitroaniline-sulpholane complex' top
Crystal data top
C16H18N6O10SF(000) = 1008
Mr = 486.42Dx = 1.605 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 10.043 (3) ÅCell parameters from 24 reflections
b = 17.131 (4) Åθ = 16–23°
c = 12.299 (4) ŵ = 0.23 mm1
β = 107.95 (3)°T = 85 K
V = 2013.1 (10) Å3Plates, yellow
Z = 40.5 × 0.3 × 0.25 mm
Data collection top
KUMA KM4
diffractometer
Rint = 0.061
Radiation source: fine-focus sealed tubeθmax = 27.0°, θmin = 2.1°
Graphite monochromatorh = 120
ω scansk = 210
4440 measured reflectionsl = 1414
4200 independent reflections2 standard reflections every 50 reflections
3360 reflections with I > 2σ(I) intensity decay: 0.5%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.053Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.165H atoms treated by a mixture of independent and constrained refinement
S = 1.19 w = 1/[σ2(Fo2) + (0.0489P)2 + 7.0136P]
where P = (Fo2 + 2Fc2)/3
4200 reflections(Δ/σ)max = 0.033
298 parametersΔρmax = 0.61 e Å3
0 restraintsΔρmin = 0.41 e Å3
Special details top

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) top
xyzUiso*/Ueq
S10.65278 (8)0.01688 (4)0.80618 (7)0.0157 (2)
O10.6048 (3)0.05541 (14)0.8433 (2)0.0223 (5)
O20.5821 (2)0.08743 (13)0.8226 (2)0.0214 (5)
C10.8364 (3)0.02269 (19)0.8692 (3)0.0189 (7)
H110.86590.00560.94260.023*
H120.87170.07450.86660.023*
C20.8871 (4)0.0359 (2)0.7970 (3)0.0207 (7)
H210.86950.08840.81420.025*
H220.98910.03020.81280.025*
C30.8024 (4)0.0203 (2)0.6703 (3)0.0251 (8)
H310.79770.06720.62970.030*
H320.85020.01920.64410.030*
C40.6538 (4)0.0056 (2)0.6619 (3)0.0202 (7)
H410.63110.05450.62440.024*
H420.58330.03220.62300.024*
C1A1.1712 (3)0.29214 (18)0.6125 (3)0.0144 (6)
C2A1.0785 (3)0.24838 (18)0.6525 (3)0.0152 (6)
H2A1.01150.27440.67890.018*
C3A1.0862 (3)0.16805 (19)0.6527 (3)0.0159 (6)
H3A1.02410.13700.67830.019*
C4A1.1875 (3)0.13295 (18)0.6148 (3)0.0160 (6)
C5A1.2795 (3)0.17510 (19)0.5740 (3)0.0158 (6)
H5A1.34640.14850.54820.019*
C6A1.2710 (3)0.25614 (19)0.5717 (3)0.0157 (6)
H6A1.33100.28680.54360.019*
N11A1.1999 (3)0.04765 (16)0.6187 (2)0.0184 (6)
O12A1.1064 (3)0.00980 (14)0.6383 (2)0.0263 (6)
O13A1.3040 (3)0.01820 (14)0.6027 (2)0.0250 (6)
N7A1.1520 (3)0.37359 (16)0.6142 (2)0.0175 (6)
H7A1.06940.39020.62140.021*
N8A1.2441 (3)0.42869 (16)0.6061 (2)0.0167 (6)
O9A1.3564 (2)0.40954 (14)0.5942 (2)0.0224 (5)
O10A1.2065 (3)0.49686 (13)0.6103 (2)0.0233 (5)
C1B1.9499 (3)0.26226 (19)0.3552 (3)0.0153 (6)
C2B1.8840 (3)0.32530 (18)0.3899 (3)0.0166 (6)
H2B1.91460.37760.38330.020*
C3B1.7752 (3)0.31299 (18)0.4335 (3)0.0162 (6)
H3B1.73100.35610.45640.019*
C4B1.7329 (3)0.23653 (19)0.4426 (3)0.0154 (6)
C5B1.7961 (3)0.17351 (19)0.4083 (3)0.0166 (6)
H5B1.76480.12140.41480.020*
C6B1.9054 (3)0.18586 (19)0.3644 (3)0.0162 (6)
H6B1.94860.14260.34110.019*
N11B1.6158 (3)0.22361 (17)0.4873 (2)0.0204 (6)
O13B1.5785 (3)0.15586 (15)0.4957 (2)0.0263 (6)
O12B1.5595 (3)0.28042 (16)0.5148 (3)0.0310 (6)
N7B2.0568 (3)0.28484 (16)0.3103 (2)0.0186 (6)
H7B2.05880.33580.29480.022*
N8B2.1553 (3)0.23913 (17)0.2881 (2)0.0199 (6)
O9B2.1476 (3)0.16799 (14)0.2972 (2)0.0239 (6)
O10B2.2467 (3)0.27356 (15)0.2595 (2)0.0273 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0167 (4)0.0109 (4)0.0227 (4)0.0013 (3)0.0107 (3)0.0020 (3)
O10.0234 (13)0.0129 (11)0.0349 (14)0.0030 (9)0.0152 (11)0.0002 (10)
O20.0231 (12)0.0126 (11)0.0343 (14)0.0004 (9)0.0173 (11)0.0039 (10)
C10.0171 (16)0.0173 (16)0.0230 (17)0.0026 (12)0.0073 (13)0.0021 (13)
C20.0169 (16)0.0168 (16)0.0285 (19)0.0007 (12)0.0070 (14)0.0045 (13)
C30.0221 (18)0.0264 (18)0.030 (2)0.0009 (14)0.0136 (15)0.0088 (15)
C40.0200 (17)0.0228 (17)0.0186 (16)0.0011 (13)0.0071 (13)0.0016 (13)
C1A0.0154 (15)0.0137 (15)0.0144 (15)0.0022 (12)0.0049 (12)0.0000 (12)
C2A0.0146 (15)0.0143 (15)0.0162 (15)0.0006 (12)0.0041 (12)0.0009 (12)
C3A0.0158 (15)0.0151 (15)0.0162 (15)0.0035 (12)0.0040 (12)0.0011 (12)
C4A0.0192 (16)0.0127 (15)0.0149 (15)0.0018 (12)0.0034 (13)0.0011 (12)
C5A0.0161 (15)0.0147 (15)0.0166 (15)0.0017 (12)0.0050 (12)0.0026 (12)
C6A0.0149 (15)0.0155 (15)0.0175 (16)0.0018 (12)0.0063 (13)0.0005 (12)
N11A0.0199 (14)0.0148 (13)0.0204 (14)0.0011 (11)0.0061 (12)0.0038 (11)
O12A0.0299 (14)0.0158 (12)0.0391 (16)0.0024 (10)0.0194 (12)0.0006 (11)
O13A0.0257 (13)0.0177 (12)0.0353 (15)0.0030 (10)0.0148 (11)0.0028 (10)
N7A0.0149 (13)0.0107 (13)0.0278 (15)0.0003 (10)0.0080 (11)0.0003 (11)
N8A0.0168 (14)0.0146 (13)0.0190 (14)0.0020 (10)0.0056 (11)0.0003 (11)
O9A0.0168 (12)0.0179 (12)0.0355 (14)0.0017 (9)0.0124 (10)0.0001 (10)
O10A0.0281 (13)0.0108 (11)0.0331 (14)0.0012 (9)0.0124 (11)0.0012 (10)
C1B0.0156 (15)0.0167 (16)0.0127 (15)0.0005 (12)0.0031 (12)0.0007 (11)
C2B0.0194 (16)0.0103 (14)0.0173 (16)0.0001 (12)0.0017 (13)0.0012 (12)
C3B0.0164 (15)0.0128 (15)0.0173 (16)0.0018 (12)0.0023 (13)0.0015 (12)
C4B0.0153 (15)0.0167 (16)0.0149 (15)0.0008 (12)0.0055 (13)0.0019 (12)
C5B0.0202 (16)0.0123 (14)0.0152 (15)0.0018 (12)0.0025 (13)0.0003 (12)
C6B0.0198 (16)0.0128 (15)0.0152 (15)0.0010 (12)0.0040 (13)0.0001 (12)
N11B0.0201 (14)0.0202 (14)0.0220 (15)0.0006 (11)0.0079 (12)0.0029 (12)
O13B0.0263 (13)0.0208 (13)0.0364 (15)0.0038 (10)0.0162 (12)0.0042 (11)
O12B0.0278 (14)0.0239 (13)0.0478 (17)0.0016 (11)0.0212 (13)0.0032 (12)
N7B0.0230 (15)0.0119 (13)0.0236 (15)0.0005 (11)0.0110 (12)0.0002 (11)
N8B0.0211 (15)0.0191 (14)0.0199 (14)0.0015 (11)0.0072 (12)0.0029 (11)
O9B0.0301 (14)0.0137 (12)0.0330 (14)0.0001 (10)0.0174 (11)0.0037 (10)
O10B0.0264 (13)0.0247 (13)0.0373 (15)0.0068 (11)0.0194 (12)0.0057 (11)
Geometric parameters (Å, º) top
S1—O21.447 (2)N7A—N8A1.346 (4)
S1—O11.453 (2)N8A—O9A1.226 (4)
S1—C11.769 (3)N8A—O10A1.233 (4)
S1—C41.788 (3)C1B—C6B1.399 (4)
C1—C21.528 (5)C1B—C2B1.400 (4)
C2—C31.551 (5)C1B—N7B1.404 (4)
C3—C41.530 (5)C2B—C3B1.375 (5)
C1A—C6A1.395 (4)C3B—C4B1.392 (4)
C1A—C2A1.398 (4)C4B—C5B1.382 (4)
C1A—N7A1.410 (4)C4B—N11B1.460 (4)
C2A—C3A1.378 (4)C5B—C6B1.381 (5)
C3A—C4A1.380 (5)N11B—O12B1.225 (4)
C4A—C5A1.383 (5)N11B—O13B1.234 (4)
C4A—N11A1.466 (4)N7B—N8B1.355 (4)
C5A—C6A1.391 (4)N8B—O9B1.229 (4)
N11A—O12A1.225 (4)N8B—O10B1.230 (4)
N11A—O13A1.230 (4)
O2—S1—O1116.32 (14)O13A—N11A—C4A118.1 (3)
O2—S1—C1112.43 (15)N8A—N7A—C1A126.3 (3)
O1—S1—C1108.20 (16)O9A—N8A—O10A124.3 (3)
O2—S1—C4112.44 (16)O9A—N8A—N7A120.0 (3)
O1—S1—C4108.93 (16)O10A—N8A—N7A115.8 (3)
C1—S1—C496.70 (16)C6B—C1B—C2B120.3 (3)
C2—C1—S1101.4 (2)C6B—C1B—N7B126.3 (3)
C1—C2—C3107.0 (3)C2B—C1B—N7B113.4 (3)
C4—C3—C2109.9 (3)C3B—C2B—C1B120.5 (3)
C3—C4—S1105.5 (2)C2B—C3B—C4B118.3 (3)
C6A—C1A—C2A121.3 (3)C5B—C4B—C3B122.0 (3)
C6A—C1A—N7A124.1 (3)C5B—C4B—N11B119.7 (3)
C2A—C1A—N7A114.6 (3)C3B—C4B—N11B118.3 (3)
C3A—C2A—C1A119.5 (3)C6B—C5B—C4B119.6 (3)
C2A—C3A—C4A118.8 (3)C5B—C6B—C1B119.2 (3)
C3A—C4A—C5A122.6 (3)O12B—N11B—O13B123.1 (3)
C3A—C4A—N11A119.2 (3)O12B—N11B—C4B118.6 (3)
C5A—C4A—N11A118.2 (3)O13B—N11B—C4B118.3 (3)
C4A—C5A—C6A119.0 (3)N8B—N7B—C1B127.9 (3)
C5A—C6A—C1A118.7 (3)O9B—N8B—O10B125.2 (3)
O12A—N11A—O13A123.7 (3)O9B—N8B—N7B118.9 (3)
O12A—N11A—C4A118.1 (3)O10B—N8B—N7B115.9 (3)
O2—S1—C1—C2154.9 (2)C6A—C1A—N7A—N8A18.1 (5)
O1—S1—C1—C275.3 (2)C2A—C1A—N7A—N8A163.6 (3)
C4—S1—C1—C237.2 (2)C1A—N7A—N8A—O9A1.2 (5)
S1—C1—C2—C344.9 (3)C1A—N7A—N8A—O10A179.5 (3)
C1—C2—C3—C434.1 (4)C6B—C1B—C2B—C3B0.2 (5)
C2—C3—C4—S16.5 (3)N7B—C1B—C2B—C3B178.6 (3)
O2—S1—C4—C3136.1 (2)C1B—C2B—C3B—C4B0.2 (5)
O1—S1—C4—C393.5 (3)C2B—C3B—C4B—C5B0.6 (5)
C1—S1—C4—C318.4 (3)C2B—C3B—C4B—N11B179.0 (3)
C6A—C1A—C2A—C3A0.5 (5)C3B—C4B—C5B—C6B0.5 (5)
N7A—C1A—C2A—C3A178.9 (3)N11B—C4B—C5B—C6B179.0 (3)
C1A—C2A—C3A—C4A1.0 (5)C4B—C5B—C6B—C1B0.1 (5)
C2A—C3A—C4A—C5A1.6 (5)C2B—C1B—C6B—C5B0.2 (5)
C2A—C3A—C4A—N11A177.8 (3)N7B—C1B—C6B—C5B178.4 (3)
C3A—C4A—C5A—C6A0.6 (5)C5B—C4B—N11B—O12B178.4 (3)
N11A—C4A—C5A—C6A178.8 (3)C3B—C4B—N11B—O12B0.1 (5)
C4A—C5A—C6A—C1A1.0 (5)C5B—C4B—N11B—O13B1.7 (5)
C2A—C1A—C6A—C5A1.6 (5)C3B—C4B—N11B—O13B179.8 (3)
N7A—C1A—C6A—C5A179.7 (3)C6B—C1B—N7B—N8B14.2 (5)
C3A—C4A—N11A—O12A11.3 (5)C2B—C1B—N7B—N8B167.5 (3)
C5A—C4A—N11A—O12A169.3 (3)C1B—N7B—N8B—O9B7.3 (5)
C3A—C4A—N11A—O13A168.3 (3)C1B—N7B—N8B—O10B172.9 (3)
C5A—C4A—N11A—O13A11.1 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2B—H2B···O1i0.962.413.194 (4)139
C2B—H2B···O10Aii0.962.483.179 (4)129
C5B—H5B···O13Aiii0.962.483.425 (4)169
N7A—H7A···O2iv0.911.892.776 (4)164
N7B—H7B···O1i0.891.972.787 (4)151
C2A—H2A···O2iv0.942.553.303 (4)138
Symmetry codes: (i) x+3/2, y1/2, z1/2; (ii) x+3, y1, z+1; (iii) x+3, y, z+1; (iv) x+3/2, y1/2, z+3/2.
(2) N,4-Dinitroaniline top
Crystal data top
C6H5N3O4Z = 4
Mr = 183.13F(000) = 376
Triclinic, P1Dx = 1.679 Mg m3
a = 6.947 (1) ÅMo Kα radiation, λ = 0.71073 Å
b = 7.773 (2) ÅCell parameters from 28 reflections
c = 13.836 (3) Åθ = 17–24°
α = 84.25 (3)°µ = 0.14 mm1
β = 79.77 (3)°T = 85 K
γ = 81.27 (3)°Plates, yellow
V = 724.7 (3) Å30.5 × 0.45 × 0.4 mm
Data collection top
KUMA KM4
diffractometer
Rint = 0.018
Radiation source: fine-focus sealed tubeθmax = 28.1°, θmin = 1.5°
Graphite monochromatorh = 90
ω scansk = 99
3500 measured reflectionsl = 1818
3255 independent reflections2 standard reflections every 50 reflections
2972 reflections with I > 2σ(I) intensity decay: 0.5%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.031Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.090All H-atom parameters refined
S = 1.05 w = 1/[σ2(Fo2) + (0.0488P)2 + 0.318P]
where P = (Fo2 + 2Fc2)/3
3255 reflections(Δ/σ)max = 0.009
265 parametersΔρmax = 0.33 e Å3
2 restraintsΔρmin = 0.25 e Å3
Special details top

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) top
xyzUiso*/Ueq
C1A0.26811 (16)0.31451 (15)0.35902 (8)0.0142 (2)
C2A0.24181 (16)0.28904 (15)0.26047 (8)0.0142 (2)
C3A0.18037 (16)0.12358 (16)0.22120 (8)0.0144 (2)
C4A0.14768 (16)0.01378 (15)0.28144 (8)0.0142 (2)
C5A0.17609 (17)0.00885 (16)0.37901 (8)0.0160 (2)
C6A0.23772 (17)0.17429 (16)0.41815 (8)0.0164 (2)
N7A0.34002 (15)0.48561 (13)0.39180 (7)0.0169 (2)
H7A0.383 (2)0.5656 (17)0.3501 (10)0.024*
N8A0.27305 (15)0.56295 (13)0.48208 (7)0.0166 (2)
O9A0.33747 (13)0.58521 (12)0.05994 (6)0.02013 (19)
O10A0.32033 (14)0.72185 (11)0.49187 (6)0.0219 (2)
N11A0.07702 (14)0.18810 (13)0.24168 (7)0.0150 (2)
O12A0.01170 (12)0.20082 (11)0.16300 (6)0.01833 (19)
O13A0.08106 (13)0.31379 (11)0.28740 (7)0.02034 (19)
C1B0.25805 (16)0.67362 (15)0.11991 (8)0.0140 (2)
C2B0.24633 (16)0.66383 (15)0.22035 (8)0.0140 (2)
C3B0.28485 (16)0.81371 (16)0.27012 (8)0.0147 (2)
C4B0.33955 (16)0.97061 (15)0.21920 (8)0.0139 (2)
C5B0.35205 (17)0.98318 (16)0.11969 (8)0.0160 (2)
C6B0.30861 (18)0.83405 (16)0.06899 (8)0.0167 (2)
N7B0.20445 (15)0.51396 (13)0.07679 (7)0.0164 (2)
H7B0.155 (2)0.4194 (16)0.1115 (11)0.026*
N8B0.25262 (14)0.47271 (13)0.00817 (7)0.0155 (2)
O9B0.17861 (16)0.47260 (13)0.54623 (7)0.0283 (2)
O10B0.20143 (13)0.31906 (11)0.02665 (6)0.02079 (19)
N11B0.37953 (14)1.12878 (13)0.27200 (7)0.0153 (2)
O12B0.31808 (13)1.12592 (12)0.34980 (6)0.0211 (2)
O13B0.47274 (13)1.25969 (11)0.23512 (6)0.0212 (2)
H2A0.262 (2)0.384 (2)0.2209 (12)0.021*
H3A0.160 (2)0.103 (2)0.1552 (12)0.022*
H5A0.157 (2)0.088 (2)0.4181 (12)0.023*
H6A0.262 (2)0.196 (2)0.4836 (13)0.028*
H2B0.217 (2)0.555 (2)0.2566 (12)0.023*
H3B0.279 (3)0.809 (2)0.3407 (13)0.030*
H5B0.383 (2)1.094 (2)0.0857 (13)0.027*
H6B0.309 (2)0.840 (2)0.0010 (12)0.022*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1A0.0129 (5)0.0140 (5)0.0154 (5)0.0001 (4)0.0027 (4)0.0020 (4)
C2A0.0139 (5)0.0142 (5)0.0148 (5)0.0008 (4)0.0022 (4)0.0053 (4)
C3A0.0135 (5)0.0164 (6)0.0137 (5)0.0009 (4)0.0034 (4)0.0028 (4)
C4A0.0119 (5)0.0133 (6)0.0172 (5)0.0002 (4)0.0031 (4)0.0020 (4)
C5A0.0163 (5)0.0153 (6)0.0164 (5)0.0001 (4)0.0023 (4)0.0065 (4)
C6A0.0183 (5)0.0172 (6)0.0144 (5)0.0003 (4)0.0046 (4)0.0043 (4)
N7A0.0219 (5)0.0136 (5)0.0133 (4)0.0030 (4)0.0012 (4)0.0034 (4)
N8A0.0201 (5)0.0160 (5)0.0145 (4)0.0008 (4)0.0059 (4)0.0016 (4)
O9A0.0260 (4)0.0185 (4)0.0171 (4)0.0026 (4)0.0080 (3)0.0001 (3)
O10A0.0318 (5)0.0142 (4)0.0194 (4)0.0008 (4)0.0081 (4)0.0007 (3)
N11A0.0121 (4)0.0142 (5)0.0179 (4)0.0001 (4)0.0017 (3)0.0026 (4)
O12A0.0199 (4)0.0171 (4)0.0179 (4)0.0008 (3)0.0064 (3)0.0006 (3)
O13A0.0237 (4)0.0132 (4)0.0245 (4)0.0016 (3)0.0056 (3)0.0069 (3)
C1B0.0127 (5)0.0148 (6)0.0143 (5)0.0007 (4)0.0016 (4)0.0037 (4)
C2B0.0136 (5)0.0142 (6)0.0137 (5)0.0009 (4)0.0033 (4)0.0006 (4)
C3B0.0135 (5)0.0179 (6)0.0126 (5)0.0003 (4)0.0033 (4)0.0016 (4)
C4B0.0121 (5)0.0142 (6)0.0155 (5)0.0003 (4)0.0018 (4)0.0043 (4)
C5B0.0182 (5)0.0146 (6)0.0148 (5)0.0006 (4)0.0037 (4)0.0002 (4)
C6B0.0206 (5)0.0164 (6)0.0127 (5)0.0008 (4)0.0031 (4)0.0010 (4)
N7B0.0216 (5)0.0133 (5)0.0143 (4)0.0023 (4)0.0063 (4)0.0029 (4)
N8B0.0160 (4)0.0172 (5)0.0135 (4)0.0034 (4)0.0008 (3)0.0041 (4)
O9B0.0437 (6)0.0218 (5)0.0148 (4)0.0018 (4)0.0035 (4)0.0042 (4)
O10B0.0256 (4)0.0160 (4)0.0210 (4)0.0006 (3)0.0032 (3)0.0071 (3)
N11B0.0136 (4)0.0156 (5)0.0166 (4)0.0012 (4)0.0013 (3)0.0041 (4)
O12B0.0229 (4)0.0235 (5)0.0185 (4)0.0001 (4)0.0071 (3)0.0076 (3)
O13B0.0257 (5)0.0141 (4)0.0225 (4)0.0044 (3)0.0057 (3)0.0025 (3)
Geometric parameters (Å, º) top
C1A—C6A1.396 (2)N11A—O12A1.241 (1)
C1A—C2A1.398 (2)C1B—C6B1.398 (2)
C1A—N7A1.408 (2)C1B—C2B1.400 (2)
C2A—C3A1.381 (2)C1B—N7B1.401 (2)
C3A—C4A1.387 (2)C2B—C3B1.380 (2)
C4A—C5A1.389 (2)C3B—C4B1.382 (2)
C4A—N11A1.457 (2)C4B—C5B1.388 (2)
C5A—C6A1.381 (2)C4B—N11B1.458 (2)
N7A—N8A1.366 (1)C5B—C6B1.381 (2)
N8A—O9B1.221 (1)N7B—N8B1.358 (1)
N8A—O10A1.229 (1)N8B—O10B1.232 (1)
O9A—N8B1.222 (1)N11B—O12B1.224 (1)
N11A—O13A1.222 (1)N11B—O13B1.236 (1)
C6A—C1A—C2A121.0 (1)C6B—C1B—C2B120.8 (1)
C6A—C1A—N7A122.7 (1)C6B—C1B—N7B124.8 (1)
C2A—C1A—N7A116.1 (1)C2B—C1B—N7B114.4 (1)
C3A—C2A—C1A119.8 (1)C3B—C2B—C1B120.0 (1)
C2A—C3A—C4A118.4 (1)C2B—C3B—C4B118.5 (1)
C3A—C4A—C5A122.5 (1)C3B—C4B—C5B122.5 (1)
C3A—C4A—N11A118.9 (1)C3B—C4B—N11B118.3 (1)
C5A—C4A—N11A118.6 (1)C5B—C4B—N11B119.2 (1)
C6A—C5A—C4A119.0 (1)C6B—C5B—C4B119.2 (1)
C5A—C6A—C1A119.2 (1)C5B—C6B—C1B119.1 (1)
N8A—N7A—C1A123.5 (1)N8B—N7B—C1B126.9 (1)
O9B—N8A—O10A125.4 (1)O9A—N8B—O10B125.4 (1)
O9B—N8A—N7A119.4 (1)O9A—N8B—N7B120.0 (1)
O10A—N8A—N7A115.2 (1)O10B—N8B—N7B114.6 (1)
O13A—N11A—O12A123.1 (1)O12B—N11B—O13B123.4 (1)
O13A—N11A—C4A119.2 (1)O12B—N11B—C4B118.6 (1)
O12A—N11A—C4A117.7 (1)O13B—N11B—C4B118.0 (1)
C6A—C1A—C2A—C3A1.54 (16)C6B—C1B—C2B—C3B0.02 (17)
N7A—C1A—C2A—C3A177.06 (10)N7B—C1B—C2B—C3B176.47 (10)
C1A—C2A—C3A—C4A0.44 (16)C1B—C2B—C3B—C4B1.66 (16)
C2A—C3A—C4A—C5A0.59 (17)C2B—C3B—C4B—C5B1.70 (17)
C2A—C3A—C4A—N11A178.15 (9)C2B—C3B—C4B—N11B179.81 (9)
C3A—C4A—C5A—C6A0.52 (17)C3B—C4B—C5B—C6B0.04 (17)
N11A—C4A—C5A—C6A178.22 (10)N11B—C4B—C5B—C6B178.13 (10)
C4A—C5A—C6A—C1A0.58 (17)C4B—C5B—C6B—C1B1.62 (17)
C2A—C1A—C6A—C5A1.60 (17)C2B—C1B—C6B—C5B1.64 (17)
N7A—C1A—C6A—C5A176.82 (10)N7B—C1B—C6B—C5B177.75 (10)
C6A—C1A—N7A—N8A44.8 (2)C6B—C1B—N7B—N8B23.8 (2)
C2A—C1A—N7A—N8A139.7 (1)C2B—C1B—N7B—N8B159.9 (1)
C1A—N7A—N8A—O9B16.2 (2)C1B—N7B—N8B—O9A6.7 (2)
C1A—N7A—N8A—O10A165.8 (1)C1B—N7B—N8B—O10B174.3 (1)
C3A—C4A—N11A—O13A167.2 (1)C3B—C4B—N11B—O12B17.8 (2)
C5A—C4A—N11A—O13A14.1 (2)C5B—C4B—N11B—O12B160.4 (1)
C3A—C4A—N11A—O12A14.2 (2)C3B—C4B—N11B—O13B162.8 (1)
C5A—C4A—N11A—O12A164.6 (1)C5B—C4B—N11B—O13B19.0 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3A—H3A···O10Bi0.94 (2)2.52 (2)3.192 (2)128 (1)
C3B—H3B···O10Aii0.98 (2)2.33 (2)3.272 (2)161 (1)
C5A—H5A···O10Aiii0.95 (2)2.40 (2)3.217 (2)145 (1)
C5B—H5B···O10Biii0.95 (2)2.55 (2)3.321 (2)138 (1)
C6A—H6A···O12Biv0.94 (2)2.53 (2)3.421 (2)157 (1)
N7A—H7A···O13Bv0.87 (1)2.20 (1)3.064 (2)171 (2)
N7B—H7B···O12A0.90 (1)2.05 (1)2.924 (2)167 (2)
Symmetry codes: (i) x, y, z; (ii) x, y, z+1; (iii) x, y+1, z; (iv) x, y+1, z+1; (v) x+1, y2, z.
 

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