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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Aug 27;67(Pt 9):o2481. doi: 10.1107/S1600536811034143

Ethane-1,2-diaminium bis­{5-[4-(1H-tetra­zol-5-yl)phen­yl]tetra­zolide} dihydrate

Chun-Rong Li a, Zheng-Qiang Xia b,*
PMCID: PMC3200657  PMID: 22059036

Abstract

In the two anions of the title salt, C2H10N2 2+·2C8H5N8 ·2H2O, the central aromatic rings make dihedral angles of 13.53 (6) and 6.53 (7)° with the deprotonated tetra­zole rings, and 11.39 (6) and 10.41 (9)° with the other tetra­zole groups. In the crystal, the cations, anions and water mol­ecules are linked by an extensive O—H⋯N, N—H⋯O and N—H⋯N hydrogen-bond network into two-dimensional wave-like duplex sheets extending parallel to the bc plane. π–π stacking inter­actions between benzene rings [inter­centroid distances are 3.8482 (4) and 3.9621 (5) Å] and between tetra­zole rings [inter­centroid distances are 3.4350 (4) and 3.7169 (4) Å] further consolidate the crystal structure.

Related literature

For similar structures, see: Tao et al. (2004); Deng et al. (2010); He et al. (2008). For 5,5′-(1,4-phenyl­ene)bis­(1H-tetra­zole) applied in coordination chemistry, see: Liu et al. (2010); Ouellette et al. (2009); Dinca et al. (2006); Qiao et al. (2011).graphic file with name e-67-o2481-scheme1.jpg

Experimental

Crystal data

  • C2H10N2 2+·2C8H5N8 ·2H2O

  • M r = 524.55

  • Triclinic, Inline graphic

  • a = 7.3918 (9) Å

  • b = 12.4699 (16) Å

  • c = 13.6367 (17) Å

  • α = 89.774 (2)°

  • β = 78.556 (2)°

  • γ = 74.153 (2)°

  • V = 1183.5 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.11 mm−1

  • T = 296 K

  • 0.32 × 0.28 × 0.11 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2008) T min = 0.966, T max = 0.988

  • 5924 measured reflections

  • 4089 independent reflections

  • 3254 reflections with I > 2σ(I)

  • R int = 0.017

Refinement

  • R[F 2 > 2σ(F 2)] = 0.042

  • wR(F 2) = 0.122

  • S = 1.02

  • 4089 reflections

  • 345 parameters

  • H-atom parameters constrained

  • Δρmax = 0.19 e Å−3

  • Δρmin = −0.23 e Å−3

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811034143/yk2016sup1.cif

e-67-o2481-sup1.cif (21.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811034143/yk2016Isup2.hkl

e-67-o2481-Isup2.hkl (200.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811034143/yk2016Isup3.cml

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O2—H2B⋯N4Ai 0.82 2.02 2.843 (2) 177
O2—H2A⋯N13A 0.85 2.08 2.919 (2) 173
O1—H1A⋯N4B 0.84 2.02 2.857 (2) 179
O1—H1B⋯N13Bii 0.85 2.10 2.946 (2) 174
N10—H10E⋯N3Aiii 0.89 2.02 2.869 (2) 160
N10—H10D⋯N1Biv 0.89 2.00 2.848 (2) 159
N10—H10C⋯N14Av 0.89 2.08 2.938 (2) 163
N9—H9E⋯N1Avi 0.89 1.98 2.8517 (19) 165
N9—H9D⋯N14Bii 0.89 2.13 2.888 (2) 143
N9—H9C⋯N3B 0.89 2.01 2.856 (2) 159
N11B—H11B⋯O2 0.86 1.86 2.685 (2) 161
N11A—H11A⋯O1 0.86 1.87 2.6903 (19) 160

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic; (v) Inline graphic; (vi) Inline graphic.

Acknowledgments

We gratefully acknowledge the National Science Foundation of China (grant No. 20873100) and Natural Science Foundation of Shaanxi Province (grant No. FF10091).

supplementary crystallographic information

Comment

Recently, 5,5'-(1,4-phenylene)-bis(1H-tetrazole) has been widely employed in the construction of many useful metal-organic frameworks (Liu et al., 2010; Ouellette et al., 2009; Dinca et al., 2006). This compound attracted our attention and our recent investigation on it (Qiao et al., 2011) has revealed its potential applications in energetic materials as the additives for the propellant. However, reports on its use in the construction of co-crystals are very scarce. Here, in the reaction of ethylenediamine, 5,5'-(1,4-phenylene)bis(1H-tetrazole) and PbCl2 under hydrothermal conditions, we have unexpectedly obtained the title compound, C2H10N22+.2C8H5N8-.2H2O, and determined its crystal structure.

The asymmetric unit of the title salt is composed of one ethylenediaminium cation, two 5-[4-(1H-tetrazol-5-yl)phenyl]tetrazolide monoanions and two water molecules (Fig.1). Both the amine N atoms of the ethylenediaminium cation are protonated. The geometric parameters are within the normal ranges.

In the crystal structure, the two terminal tetrazole rings of the anions are nearly coplanar with the dihedral angles of 5.03 (7) or 6.37 (10)°. It is noteworthy that there are two types of π-π stacking interactions: one occurs between benzene rings with centroid-centroid distances of 3.8482 (4) and 3.9621 (5) Å, the other occurs between tetrazole rings with centroid-centroid distances of 3.4350 (4) and 3.7169 (4) Å. Thus, a wide range of hydrogen bonds (O—H···N, N—H···O and N—H···N) (Table 1) and π-π stacking interactions contribute to the formation of the supramolecular network (Fig. 2).

Experimental

Lead chloride (0.0278 g, 0.1 mmol) and 5,5'-(1,4-phenylene)-bis(1H-tetrazole) (0.0215 g, 0.1 mmol) were added to water (6 ml). The pH of this solution was adjusted to neutral with ethylenediamine solution. The solution was sealed in a 10-ml Teflon-lined stainless reactor at 393 K for 3 days. After the sample was cooled to room temperature at a rate of 5 K/h, the colorless block crystals suitable for X-ray analysis were obtained.

Refinement

All H atoms attached to C atoms were fixed geometrically and treated as riding with C—H = 0.97 (methylene) and 0.93 Å (aromatic), Uiso(H) = 1.2Ueq(C). The H atoms bonded to N atoms were placed in calculated positions and refined in riding mode with N—H = 0.86 (tetrazole) and 0.89 Å (amine), Uiso(H) = 1.2Ueq(N of tetrazole), Uiso(H) = 1.5Ueq(N of amine). The water H atoms were located in difference Fourier maps, with distance restraints of O—H = 0.84±0.02 Å, and then refined with isotropic thermal parameters 1.5 times those of O atoms.

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound, showing the atom labeling scheme and displacement ellipsoids drawn at the 30% probalility level.

Fig. 2.

Fig. 2.

A view of the crystal packing of the title compound, showing the O—H···N, N—H···O and N—H···N hydrogen bonds interactions. Symmetry operators: ix, y + 1, z; iix, y - 1, z; iii -x, -y, -z + 1; iv -x, -y + 1, -z + 2; v -x, -y + 1, -z + 1; vix, y, z + 1.

Crystal data

C2H10N22+·2C8H5N8·2H2O Z = 2
Mr = 524.55 F(000) = 548
Triclinic, P1 Dx = 1.472 Mg m3Dm = 1.472 Mg m3Dm measured by not measured
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 7.3918 (9) Å Cell parameters from 2314 reflections
b = 12.4699 (16) Å θ = 2.9–25.8°
c = 13.6367 (17) Å µ = 0.11 mm1
α = 89.774 (2)° T = 296 K
β = 78.556 (2)° Block, colorless
γ = 74.153 (2)° 0.32 × 0.28 × 0.11 mm
V = 1183.5 (3) Å3

Data collection

Bruker APEXII CCD diffractometer 4089 independent reflections
Radiation source: fine-focus sealed tube 3254 reflections with I > 2σ(I)
graphite Rint = 0.017
φ and ω scans θmax = 25.0°, θmin = 1.5°
Absorption correction: multi-scan (SADABS; Bruker, 2008) h = −8→8
Tmin = 0.966, Tmax = 0.988 k = −14→11
5924 measured reflections l = −16→16

Refinement

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)] = 0.042 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.122 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0641P)2 + 0.2582P] where P = (Fo2 + 2Fc2)/3
4089 reflections (Δ/σ)max < 0.001
345 parameters Δρmax = 0.19 e Å3
0 restraints Δρmin = −0.23 e Å3

Special details

Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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
C11A 0.2135 (2) 0.47786 (13) 0.31175 (12) 0.0301 (4)
C12A 0.2209 (2) 0.37261 (13) 0.26227 (12) 0.0297 (4)
C13A 0.2551 (3) 0.36244 (14) 0.15792 (12) 0.0333 (4)
H13A 0.2671 0.4237 0.1207 0.040*
C14A 0.2017 (3) 0.28026 (14) 0.31627 (13) 0.0367 (4)
H14A 0.1790 0.2857 0.3859 0.044*
C11B 0.2752 (3) 0.96745 (14) 0.60365 (12) 0.0333 (4)
C12B 0.2807 (3) 0.86208 (14) 0.65171 (12) 0.0321 (4)
C13B 0.2756 (3) 0.85759 (14) 0.75418 (13) 0.0352 (4)
H13B 0.2664 0.9219 0.7914 0.042*
C14B 0.2936 (3) 0.76531 (15) 0.59755 (13) 0.0394 (5)
H14B 0.2969 0.7672 0.5290 0.047*
C9 0.0711 (3) 0.20961 (15) 0.83423 (13) 0.0378 (4)
H9A 0.0183 0.1467 0.8323 0.045*
H9B 0.0523 0.2512 0.7751 0.045*
C10 −0.0329 (3) 0.28374 (15) 0.92698 (13) 0.0370 (4)
H10A −0.0148 0.2421 0.9862 0.044*
H10B 0.0201 0.3466 0.9290 0.044*
C1A 0.2689 (2) 0.06357 (13) 0.11169 (12) 0.0285 (4)
C2A 0.2516 (2) 0.16970 (13) 0.16380 (12) 0.0289 (4)
C3A 0.2159 (3) 0.18057 (14) 0.26764 (13) 0.0357 (4)
H3A 0.2012 0.1198 0.3050 0.043*
C4A 0.2713 (3) 0.26267 (14) 0.10956 (12) 0.0325 (4)
H4A 0.2956 0.2570 0.0399 0.039*
C1B 0.3137 (2) 0.55566 (14) 0.79614 (12) 0.0294 (4)
C2B 0.2975 (2) 0.66181 (14) 0.74691 (12) 0.0308 (4)
C3B 0.3016 (3) 0.66656 (15) 0.64432 (13) 0.0391 (4)
H3B 0.3099 0.6024 0.6071 0.047*
C4B 0.2841 (3) 0.75917 (14) 0.80075 (12) 0.0343 (4)
H4B 0.2808 0.7575 0.8693 0.041*
N11A 0.2160 (2) 0.49535 (11) 0.40801 (10) 0.0373 (4)
H11A 0.2204 0.4457 0.4521 0.045*
N12A 0.2104 (3) 0.60166 (12) 0.42518 (11) 0.0446 (4)
N13A 0.2043 (3) 0.64840 (12) 0.34094 (11) 0.0426 (4)
N14A 0.2065 (2) 0.57367 (12) 0.26830 (10) 0.0355 (4)
N11B 0.2501 (3) 0.98954 (12) 0.51052 (11) 0.0436 (4)
H11B 0.2368 0.9431 0.4679 0.052*
N12B 0.2491 (3) 1.09568 (13) 0.49410 (12) 0.0527 (5)
N13B 0.2731 (3) 1.13653 (13) 0.57554 (12) 0.0506 (5)
N14B 0.2906 (3) 1.05895 (12) 0.64532 (11) 0.0417 (4)
N9 0.2778 (2) 0.16876 (11) 0.83363 (10) 0.0322 (3)
H9C 0.3286 0.2261 0.8290 0.048*
H9D 0.3353 0.1206 0.7815 0.048*
H9E 0.2945 0.1350 0.8901 0.048*
N10 −0.2399 (2) 0.32474 (11) 0.92681 (10) 0.0315 (3)
H10C −0.2562 0.3631 0.8726 0.047*
H10D −0.2994 0.3688 0.9814 0.047*
H10E −0.2888 0.2670 0.9263 0.047*
N1A 0.2669 (2) 0.05241 (11) 0.01421 (10) 0.0339 (4)
N2A 0.2887 (2) −0.05668 (12) −0.00421 (11) 0.0381 (4)
N3A 0.3040 (2) −0.10827 (12) 0.07894 (11) 0.0392 (4)
N4A 0.2908 (2) −0.03469 (12) 0.15402 (10) 0.0351 (4)
N1B 0.3320 (2) 0.54178 (11) 0.89155 (10) 0.0346 (4)
N2B 0.3495 (2) 0.43315 (12) 0.90616 (11) 0.0385 (4)
N3B 0.3432 (2) 0.38426 (12) 0.82212 (11) 0.0404 (4)
N4B 0.3198 (2) 0.45938 (12) 0.75156 (11) 0.0376 (4)
O1 0.2556 (2) 0.37535 (11) 0.57068 (10) 0.0567 (4)
H1B 0.2661 0.3062 0.5750 0.085*
H1A 0.2766 0.4000 0.6234 0.085*
O2 0.2347 (3) 0.87668 (13) 0.34653 (11) 0.0842 (7)
H2A 0.2303 0.8101 0.3399 0.126*
H2B 0.2537 0.9038 0.2915 0.126*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C11A 0.0383 (10) 0.0262 (9) 0.0257 (8) −0.0075 (7) −0.0084 (7) 0.0014 (7)
C12A 0.0370 (10) 0.0251 (9) 0.0269 (9) −0.0077 (7) −0.0081 (7) 0.0007 (7)
C13A 0.0496 (11) 0.0261 (9) 0.0284 (9) −0.0146 (8) −0.0120 (8) 0.0040 (7)
C14A 0.0569 (12) 0.0319 (10) 0.0227 (8) −0.0146 (8) −0.0084 (8) 0.0012 (7)
C11B 0.0463 (11) 0.0281 (9) 0.0252 (9) −0.0100 (8) −0.0069 (7) 0.0005 (7)
C12B 0.0423 (11) 0.0261 (9) 0.0287 (9) −0.0099 (7) −0.0087 (7) 0.0024 (7)
C13B 0.0513 (12) 0.0265 (9) 0.0292 (9) −0.0122 (8) −0.0096 (8) 0.0003 (7)
C14B 0.0643 (13) 0.0319 (10) 0.0253 (9) −0.0141 (9) −0.0157 (8) 0.0038 (7)
C9 0.0398 (11) 0.0394 (10) 0.0331 (10) −0.0069 (8) −0.0104 (8) −0.0061 (8)
C10 0.0381 (11) 0.0406 (10) 0.0323 (9) −0.0104 (8) −0.0083 (8) −0.0046 (8)
C1A 0.0347 (10) 0.0261 (9) 0.0266 (8) −0.0115 (7) −0.0069 (7) 0.0029 (7)
C2A 0.0351 (10) 0.0244 (8) 0.0292 (9) −0.0092 (7) −0.0099 (7) 0.0010 (7)
C3A 0.0563 (12) 0.0252 (9) 0.0284 (9) −0.0167 (8) −0.0077 (8) 0.0050 (7)
C4A 0.0459 (11) 0.0307 (9) 0.0240 (8) −0.0135 (8) −0.0103 (7) 0.0029 (7)
C1B 0.0352 (10) 0.0272 (9) 0.0279 (9) −0.0107 (7) −0.0083 (7) 0.0014 (7)
C2B 0.0368 (10) 0.0292 (9) 0.0279 (9) −0.0109 (7) −0.0081 (7) 0.0020 (7)
C3B 0.0630 (13) 0.0266 (9) 0.0304 (9) −0.0137 (9) −0.0142 (9) −0.0006 (7)
C4B 0.0496 (11) 0.0312 (9) 0.0230 (8) −0.0126 (8) −0.0074 (8) 0.0014 (7)
N11A 0.0625 (11) 0.0240 (8) 0.0287 (8) −0.0130 (7) −0.0160 (7) 0.0025 (6)
N12A 0.0762 (12) 0.0290 (8) 0.0331 (8) −0.0175 (8) −0.0179 (8) 0.0004 (7)
N13A 0.0665 (12) 0.0287 (8) 0.0354 (9) −0.0157 (7) −0.0134 (8) −0.0017 (7)
N14A 0.0526 (10) 0.0267 (8) 0.0292 (8) −0.0123 (7) −0.0116 (7) 0.0017 (6)
N11B 0.0780 (13) 0.0284 (8) 0.0289 (8) −0.0186 (8) −0.0163 (8) 0.0032 (6)
N12B 0.0961 (15) 0.0315 (9) 0.0346 (9) −0.0219 (9) −0.0170 (9) 0.0077 (7)
N13B 0.0888 (14) 0.0299 (9) 0.0341 (9) −0.0189 (9) −0.0116 (9) 0.0036 (7)
N14B 0.0689 (12) 0.0283 (8) 0.0296 (8) −0.0165 (7) −0.0098 (7) 0.0032 (6)
N9 0.0397 (9) 0.0283 (8) 0.0284 (7) −0.0087 (6) −0.0074 (6) −0.0002 (6)
N10 0.0387 (9) 0.0260 (7) 0.0297 (8) −0.0083 (6) −0.0078 (6) 0.0008 (6)
N1A 0.0479 (9) 0.0276 (8) 0.0287 (8) −0.0122 (7) −0.0111 (7) 0.0003 (6)
N2A 0.0535 (10) 0.0304 (8) 0.0324 (8) −0.0151 (7) −0.0086 (7) −0.0019 (6)
N3A 0.0553 (10) 0.0283 (8) 0.0365 (9) −0.0177 (7) −0.0064 (7) −0.0013 (7)
N4A 0.0505 (10) 0.0274 (8) 0.0303 (8) −0.0153 (7) −0.0083 (7) 0.0024 (6)
N1B 0.0485 (10) 0.0287 (8) 0.0281 (8) −0.0123 (7) −0.0092 (7) 0.0045 (6)
N2B 0.0539 (10) 0.0309 (8) 0.0347 (8) −0.0161 (7) −0.0122 (7) 0.0074 (6)
N3B 0.0562 (10) 0.0301 (8) 0.0379 (9) −0.0161 (7) −0.0106 (7) 0.0042 (7)
N4B 0.0576 (10) 0.0281 (8) 0.0320 (8) −0.0170 (7) −0.0135 (7) 0.0039 (6)
O1 0.1072 (13) 0.0371 (8) 0.0373 (7) −0.0283 (8) −0.0303 (8) 0.0085 (6)
O2 0.190 (2) 0.0513 (10) 0.0361 (8) −0.0628 (12) −0.0398 (11) 0.0109 (7)

Geometric parameters (Å, °)

C11A—N14A 1.324 (2) C1B—N4B 1.334 (2)
C11A—N11A 1.336 (2) C1B—N1B 1.340 (2)
C11A—C12A 1.461 (2) C1B—C2B 1.468 (2)
C12A—C14A 1.389 (2) C2B—C4B 1.391 (2)
C12A—C13A 1.395 (2) C2B—C3B 1.395 (2)
C13A—C4A 1.375 (2) C3B—H3B 0.9300
C13A—H13A 0.9300 C4B—H4B 0.9300
C14A—C3A 1.380 (2) N11A—N12A 1.335 (2)
C14A—H14A 0.9300 N11A—H11A 0.8600
C11B—N14B 1.319 (2) N12A—N13A 1.289 (2)
C11B—N11B 1.336 (2) N13A—N14A 1.3574 (19)
C11B—C12B 1.460 (2) N11B—N12B 1.340 (2)
C12B—C14B 1.388 (2) N11B—H11B 0.8600
C12B—C13B 1.392 (2) N12B—N13B 1.287 (2)
C13B—C4B 1.372 (2) N13B—N14B 1.353 (2)
C13B—H13B 0.9300 N9—H9C 0.8900
C14B—C3B 1.377 (2) N9—H9D 0.8900
C14B—H14B 0.9300 N9—H9E 0.8900
C9—N9 1.471 (2) N10—H10C 0.8900
C9—C10 1.510 (2) N10—H10D 0.8900
C9—H9A 0.9700 N10—H10E 0.8900
C9—H9B 0.9700 N1A—N2A 1.3440 (19)
C10—N10 1.475 (2) N2A—N3A 1.311 (2)
C10—H10A 0.9700 N3A—N4A 1.349 (2)
C10—H10B 0.9700 N1B—N2B 1.3430 (19)
C1A—N4A 1.336 (2) N2B—N3B 1.315 (2)
C1A—N1A 1.340 (2) N3B—N4B 1.3431 (19)
C1A—C2A 1.467 (2) O1—H1B 0.8477
C2A—C3A 1.388 (2) O1—H1A 0.8408
C2A—C4A 1.398 (2) O2—H2A 0.8464
C3A—H3A 0.9300 O2—H2B 0.8243
C4A—H4A 0.9300
N14A—C11A—N11A 107.27 (14) C2A—C4A—H4A 119.6
N14A—C11A—C12A 125.89 (14) N4B—C1B—N1B 110.77 (14)
N11A—C11A—C12A 126.82 (15) N4B—C1B—C2B 124.99 (14)
C14A—C12A—C13A 118.65 (15) N1B—C1B—C2B 124.19 (15)
C14A—C12A—C11A 121.72 (15) C4B—C2B—C3B 118.44 (15)
C13A—C12A—C11A 119.58 (14) C4B—C2B—C1B 120.84 (15)
C4A—C13A—C12A 120.61 (15) C3B—C2B—C1B 120.68 (15)
C4A—C13A—H13A 119.7 C14B—C3B—C2B 120.64 (16)
C12A—C13A—H13A 119.7 C14B—C3B—H3B 119.7
C3A—C14A—C12A 120.65 (16) C2B—C3B—H3B 119.7
C3A—C14A—H14A 119.7 C13B—C4B—C2B 120.90 (15)
C12A—C14A—H14A 119.7 C13B—C4B—H4B 119.5
N14B—C11B—N11B 107.58 (15) C2B—C4B—H4B 119.5
N14B—C11B—C12B 125.96 (15) N12A—N11A—C11A 109.55 (14)
N11B—C11B—C12B 126.46 (15) N12A—N11A—H11A 125.2
C14B—C12B—C13B 118.83 (15) C11A—N11A—H11A 125.2
C14B—C12B—C11B 121.69 (15) N13A—N12A—N11A 106.35 (14)
C13B—C12B—C11B 119.47 (15) N12A—N13A—N14A 110.58 (14)
C4B—C13B—C12B 120.58 (16) C11A—N14A—N13A 106.25 (13)
C4B—C13B—H13B 119.7 C11B—N11B—N12B 109.11 (14)
C12B—C13B—H13B 119.7 C11B—N11B—H11B 125.4
C3B—C14B—C12B 120.60 (16) N12B—N11B—H11B 125.4
C3B—C14B—H14B 119.7 N13B—N12B—N11B 106.27 (14)
C12B—C14B—H14B 119.7 N12B—N13B—N14B 110.78 (14)
N9—C9—C10 110.58 (14) C11B—N14B—N13B 106.26 (14)
N9—C9—H9A 109.5 C9—N9—H9C 109.5
C10—C9—H9A 109.5 C9—N9—H9D 109.5
N9—C9—H9B 109.5 H9C—N9—H9D 109.5
C10—C9—H9B 109.5 C9—N9—H9E 109.5
H9A—C9—H9B 108.1 H9C—N9—H9E 109.5
N10—C10—C9 110.26 (14) H9D—N9—H9E 109.5
N10—C10—H10A 109.6 C10—N10—H10C 109.5
C9—C10—H10A 109.6 C10—N10—H10D 109.5
N10—C10—H10B 109.6 H10C—N10—H10D 109.5
C9—C10—H10B 109.6 C10—N10—H10E 109.5
H10A—C10—H10B 108.1 H10C—N10—H10E 109.5
N4A—C1A—N1A 110.91 (14) H10D—N10—H10E 109.5
N4A—C1A—C2A 124.96 (14) C1A—N1A—N2A 105.64 (13)
N1A—C1A—C2A 124.13 (14) N3A—N2A—N1A 108.65 (13)
C3A—C2A—C4A 118.34 (15) N2A—N3A—N4A 110.11 (13)
C3A—C2A—C1A 121.17 (14) C1A—N4A—N3A 104.69 (13)
C4A—C2A—C1A 120.49 (15) C1B—N1B—N2B 105.69 (13)
C14A—C3A—C2A 120.94 (16) N3B—N2B—N1B 108.54 (13)
C14A—C3A—H3A 119.5 N2B—N3B—N4B 109.96 (13)
C2A—C3A—H3A 119.5 C1B—N4B—N3B 105.03 (13)
C13A—C4A—C2A 120.80 (15) H1B—O1—H1A 108.9
C13A—C4A—H4A 119.6 H2A—O2—H2B 110.7

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O2—H2B···N4Ai 0.82 2.02 2.843 (2) 177.
O2—H2A···N13A 0.85 2.08 2.919 (2) 173.
O1—H1A···N4B 0.84 2.02 2.857 (2) 179.
O1—H1B···N13Bii 0.85 2.10 2.946 (2) 174.
N10—H10E···N3Aiii 0.89 2.02 2.869 (2) 160.
N10—H10D···N1Biv 0.89 2.00 2.848 (2) 159.
N10—H10C···N14Av 0.89 2.08 2.938 (2) 163.
N9—H9E···N1Avi 0.89 1.98 2.8517 (19) 165.
N9—H9D···N14Bii 0.89 2.13 2.888 (2) 143.
N9—H9C···N3B 0.89 2.01 2.856 (2) 159.
N11B—H11B···O2 0.86 1.86 2.685 (2) 161.
N11A—H11A···O1 0.86 1.87 2.6903 (19) 160.

Symmetry codes: (i) x, y+1, z; (ii) x, y−1, z; (iii) −x, −y, −z+1; (iv) −x, −y+1, −z+2; (v) −x, −y+1, −z+1; (vi) x, y, z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: YK2016).

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 datablock(s) global, I. DOI: 10.1107/S1600536811034143/yk2016sup1.cif

e-67-o2481-sup1.cif (21.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811034143/yk2016Isup2.hkl

e-67-o2481-Isup2.hkl (200.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811034143/yk2016Isup3.cml

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


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