Abstract
In the title compound, C19H13N5·3CH4O, the 2,6-bis(2-benzimidazolyl)pyridine molecule is essentially planar with an r.m.s. deviation for all non-H atoms of 0.185 Å. The crystal structure is stabilized by intermolecular O—H⋯O, O—H⋯N and N—H⋯O hydrogen bonds and weak π⋯π stacking interactions with centroid–centroid distances of 3.6675 (16) and 3.6891 (15) Å. The atoms of one of the methanol solvent molecules are disordered over two sites with refined occupancies of 0.606(8) and 0.394(8).
Related literature
For the crystal structures of the mono- and sesquihydrate analogs of 2,6-bis(2-benzimidazolyl)pyridine, see: Freire et al. (2003 ▶). For the synthesis of 2,6-bis(2-benzimidazolyl)pyridine, see: Addison & Burke (1981 ▶).
Experimental
Crystal data
C19H13N5·3CH4O
M r = 407.47
Monoclinic,
a = 11.2686 (9) Å
b = 15.0928 (13) Å
c = 13.0679 (11) Å
β = 107.391 (2)°
V = 2120.9 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.09 mm−1
T = 153 K
0.18 × 0.14 × 0.11 mm
Data collection
Rigaku R-AXIS Spider diffractometer
Absorption correction: multi-scan (Higashi, 1995 ▶) T min = 0.984, T max = 0.990
17035 measured reflections
3945 independent reflections
2527 reflections with I > 2σ(I)
R int = 0.071
Refinement
R[F 2 > 2σ(F 2)] = 0.077
wR(F 2) = 0.236
S = 1.04
3945 reflections
307 parameters
2 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.39 e Å−3
Δρmin = −0.40 e Å−3
Data collection: RAPID-AUTO (Rigaku/MSC 2004 ▶); cell refinement: RAPID-AUTO; data reduction: RAPID-AUTO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶) and PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809012574/lh2799sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809012574/lh2799Isup2.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 |
|---|---|---|---|---|
| O1—H1⋯O2i | 0.84 | 1.83 | 2.670 (3) | 176 |
| O2—H2⋯N4 | 0.84 | 1.91 | 2.741 (3) | 168 |
| N1—H1N⋯O1 | 0.866 (10) | 2.069 (12) | 2.927 (3) | 171 (3) |
| N3—H3N⋯O1 | 0.863 (10) | 2.069 (12) | 2.925 (3) | 171 (4) |
Symmetry code: (i)
.
Acknowledgments
The authors acknowledge financial support and a grant from ‘Qing Lan’ Talent Engineering Funds and Students’ Science and Technology Innovation Funds (grant No. DXS2008–040,041) of Lanzhou Jiaotong University. A grant from the Middle-Young Age Science Foundation (grant No. 3YS061-A25–023) and Long Yuan ‘Qing Nian’ of Gansu Province is also acknowledged.
supplementary crystallographic information
Comment
The synthesis of 2,6-bis(2-benzimidazolyl)pyridine has been reported in the literature (Addison & Burke 1981) and the crystal structures of the mono and sesqihydrates of this compound have been determined (Freire et al., 2003). During our studies of benzimidazole complexes involving a recrystallization of 2,6-bis(2-benzimidazolyl)pyridine from methanol we unexpectedly form the trimethanol solvate (I).
The molecular structure of the 2,6-bis(2-benzimidazolyl)pyridine molecule is shown in Fig. 1. The molecule is essentially planar with a rms deviation of all non-hydrogen fitted atoms = 0.185. The crystal structure is stabilized by intermolecular hydrogen bonds (see Table 1) and weak π···π stacking interactions (Fig. 2) with, centroid to centroid distances of 3.6675 (16) and 3.6891 (15)Å, between pryridine rings and benzimidazole rings of inversion related molecules.
Experimental
2,6-bis(2-benzimidazolyl)pyridine was prepared by the method of Addison & Burke (1981). After recrystallization from methanol, fine white needles were formed. The mother liquor was set aside for several days leading to the formation of crystals that were suitable for X-ray diffraction analysis.
Refinement
All H atoms were found in difference electron maps and were subsequently refined in a riding-model approximation with C—H distances ranging from 0.95 to 0.98 Å and with Uiso(H) = 1.2 Ueq(C) for CH and Uiso(H) = 1.2 Ueq(O) for OH. H atoms bonded to N atoms were refined independently with isotropic displacement parameters. The atoms of one methanol solvent molecule is disordered over two sites with refined occupancies of 0.606 (8) and 0.394 (8).
Figures
Fig. 1.
The molecular structure of the title compound. Displacement ellipsoids are drawn at the 30% probability level. H atoms and solvent molecules have been omitted for clarity.
Fig. 2.
Part of the crystal structure showing weak π···π stacking interactions. The solvent molecules are not shown
Crystal data
| C19H13N5·3CH4O | F(000) = 864 |
| Mr = 407.47 | Dx = 1.276 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 3945 reflections |
| a = 11.2686 (9) Å | θ = 3.2–25.5° |
| b = 15.0928 (13) Å | µ = 0.09 mm−1 |
| c = 13.0679 (11) Å | T = 153 K |
| β = 107.391 (2)° | Block, colorless |
| V = 2120.9 (3) Å3 | 0.18 × 0.14 × 0.11 mm |
| Z = 4 |
Data collection
| Rigaku R-AXIS Spider diffractometer | 3945 independent reflections |
| Radiation source: fine-focus sealed tube | 2527 reflections with I > 2σ(I) |
| graphite | Rint = 0.071 |
| φ and ω scans | θmax = 25.5°, θmin = 3.2° |
| Absorption correction: multi-scan (Higashi, 1995) | h = −13→11 |
| Tmin = 0.984, Tmax = 0.990 | k = −18→18 |
| 17035 measured reflections | l = −15→15 |
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)] = 0.077 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.236 | w = 1/[σ2(Fo2) + (0.1505P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 1.04 | (Δ/σ)max = 0.002 |
| 3945 reflections | Δρmax = 0.39 e Å−3 |
| 307 parameters | Δρmin = −0.40 e Å−3 |
| 2 restraints | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.040 (6) |
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 | Occ. (<1) | |
| O1 | 0.20534 (18) | 0.61337 (13) | 0.36351 (15) | 0.0631 (6) | |
| H1 | 0.2509 | 0.6582 | 0.3816 | 0.076* | |
| O2 | 0.65988 (19) | 0.23950 (14) | 0.57774 (17) | 0.0704 (6) | |
| H2 | 0.6009 | 0.2626 | 0.5299 | 0.084* | |
| N1 | 0.11042 (19) | 0.58598 (15) | 0.54657 (17) | 0.0477 (6) | |
| N2 | 0.0754 (2) | 0.53929 (15) | 0.69788 (17) | 0.0517 (6) | |
| N3 | 0.3694 (2) | 0.46017 (15) | 0.38227 (18) | 0.0510 (6) | |
| N4 | 0.4825 (2) | 0.33787 (15) | 0.43304 (18) | 0.0536 (6) | |
| N5 | 0.27120 (19) | 0.45211 (14) | 0.54781 (16) | 0.0492 (6) | |
| C1 | 0.0280 (2) | 0.64631 (18) | 0.5671 (2) | 0.0498 (7) | |
| C2 | −0.0274 (2) | 0.72243 (19) | 0.5148 (2) | 0.0558 (7) | |
| H2A | −0.0109 | 0.7432 | 0.4518 | 0.067* | |
| C3 | −0.1076 (3) | 0.7667 (2) | 0.5589 (2) | 0.0609 (8) | |
| H3 | −0.1476 | 0.8191 | 0.5254 | 0.073* | |
| C4 | −0.1313 (3) | 0.7359 (2) | 0.6519 (2) | 0.0615 (8) | |
| H4 | −0.1875 | 0.7680 | 0.6795 | 0.074* | |
| C5 | −0.0761 (2) | 0.6613 (2) | 0.7043 (2) | 0.0558 (7) | |
| H5 | −0.0930 | 0.6411 | 0.7674 | 0.067* | |
| C6 | 0.0060 (2) | 0.61602 (18) | 0.6613 (2) | 0.0500 (7) | |
| C7 | 0.1350 (2) | 0.52423 (17) | 0.6263 (2) | 0.0479 (6) | |
| C8 | 0.2211 (2) | 0.45155 (17) | 0.62863 (19) | 0.0467 (7) | |
| C9 | 0.2477 (2) | 0.38735 (18) | 0.7084 (2) | 0.0513 (7) | |
| H9 | 0.2096 | 0.3888 | 0.7641 | 0.062* | |
| C10 | 0.3312 (2) | 0.32126 (18) | 0.7045 (2) | 0.0536 (7) | |
| H10 | 0.3520 | 0.2767 | 0.7582 | 0.064* | |
| C11 | 0.3837 (2) | 0.32049 (18) | 0.6221 (2) | 0.0529 (7) | |
| H11 | 0.4411 | 0.2755 | 0.6181 | 0.063* | |
| C12 | 0.3512 (2) | 0.38721 (17) | 0.5444 (2) | 0.0471 (7) | |
| C13 | 0.4022 (2) | 0.39322 (17) | 0.4542 (2) | 0.0480 (7) | |
| C14 | 0.5051 (2) | 0.37188 (19) | 0.3421 (2) | 0.0539 (7) | |
| C15 | 0.5848 (3) | 0.3422 (2) | 0.2854 (2) | 0.0656 (8) | |
| H15 | 0.6334 | 0.2901 | 0.3066 | 0.079* | |
| C16 | 0.5905 (3) | 0.3906 (2) | 0.1981 (3) | 0.0695 (9) | |
| H16 | 0.6442 | 0.3717 | 0.1584 | 0.083* | |
| C17 | 0.5188 (3) | 0.4674 (2) | 0.1662 (2) | 0.0713 (9) | |
| H17 | 0.5244 | 0.4990 | 0.1049 | 0.086* | |
| C18 | 0.4406 (3) | 0.4980 (2) | 0.2211 (2) | 0.0616 (8) | |
| H18 | 0.3930 | 0.5504 | 0.1999 | 0.074* | |
| C19 | 0.4344 (2) | 0.44882 (18) | 0.3089 (2) | 0.0531 (7) | |
| C20 | 0.1118 (3) | 0.6305 (3) | 0.2645 (3) | 0.0789 (10) | |
| H20A | 0.0453 | 0.6661 | 0.2780 | 0.095* | |
| H20B | 0.0773 | 0.5742 | 0.2312 | 0.095* | |
| H20C | 0.1484 | 0.6628 | 0.2163 | 0.095* | |
| C21 | 0.7174 (4) | 0.1739 (3) | 0.5314 (4) | 0.0958 (12) | |
| H21A | 0.7639 | 0.2025 | 0.4879 | 0.115* | |
| H21B | 0.6536 | 0.1350 | 0.4858 | 0.115* | |
| H21C | 0.7745 | 0.1389 | 0.5883 | 0.115* | |
| O3 | 0.1278 (5) | 0.5658 (3) | 0.9743 (4) | 0.094 (2) | 0.606 (8) |
| H3A | 0.1412 | 0.5425 | 1.0350 | 0.112* | 0.606 (8) |
| C22 | 0.2186 (8) | 0.5366 (7) | 0.9269 (9) | 0.0521 (19) | 0.606 (8) |
| H22A | 0.2730 | 0.5862 | 0.9227 | 0.062* | 0.606 (8) |
| H22B | 0.1774 | 0.5142 | 0.8547 | 0.062* | 0.606 (8) |
| H22C | 0.2681 | 0.4892 | 0.9707 | 0.062* | 0.606 (8) |
| O3' | 0.0859 (9) | 0.4916 (6) | 0.8986 (6) | 0.118 (4) | 0.394 (8) |
| H3' | 0.0325 | 0.5092 | 0.9272 | 0.141* | 0.394 (8) |
| C22' | 0.1816 (12) | 0.5468 (13) | 0.9232 (18) | 0.078 (5) | 0.394 (8) |
| H22D | 0.1522 | 0.6072 | 0.9022 | 0.094* | 0.394 (8) |
| H22E | 0.2405 | 0.5293 | 0.8848 | 0.094* | 0.394 (8) |
| H22F | 0.2230 | 0.5449 | 1.0006 | 0.094* | 0.394 (8) |
| H1N | 0.144 (3) | 0.589 (2) | 0.4954 (17) | 0.075 (10)* | |
| H3N | 0.316 (3) | 0.5018 (17) | 0.380 (3) | 0.095 (12)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0689 (13) | 0.0565 (13) | 0.0638 (13) | 0.0040 (9) | 0.0197 (10) | 0.0078 (9) |
| O2 | 0.0655 (13) | 0.0665 (14) | 0.0811 (15) | 0.0113 (10) | 0.0249 (11) | 0.0109 (11) |
| N1 | 0.0473 (12) | 0.0518 (13) | 0.0463 (12) | 0.0027 (10) | 0.0175 (10) | 0.0002 (10) |
| N2 | 0.0524 (12) | 0.0558 (14) | 0.0479 (12) | −0.0030 (10) | 0.0164 (10) | −0.0030 (10) |
| N3 | 0.0535 (13) | 0.0505 (14) | 0.0516 (13) | −0.0013 (10) | 0.0196 (10) | −0.0001 (10) |
| N4 | 0.0559 (13) | 0.0514 (14) | 0.0553 (13) | −0.0005 (10) | 0.0194 (10) | −0.0041 (10) |
| N5 | 0.0515 (12) | 0.0491 (13) | 0.0443 (12) | −0.0018 (10) | 0.0104 (10) | −0.0040 (9) |
| C1 | 0.0490 (14) | 0.0486 (15) | 0.0505 (14) | −0.0026 (12) | 0.0130 (11) | −0.0065 (12) |
| C2 | 0.0579 (15) | 0.0553 (17) | 0.0534 (15) | 0.0034 (13) | 0.0154 (13) | 0.0005 (13) |
| C3 | 0.0564 (16) | 0.0600 (18) | 0.0634 (17) | 0.0060 (13) | 0.0134 (14) | −0.0076 (14) |
| C4 | 0.0529 (15) | 0.067 (2) | 0.0655 (18) | 0.0034 (14) | 0.0188 (14) | −0.0138 (15) |
| C5 | 0.0523 (15) | 0.0639 (19) | 0.0538 (15) | −0.0056 (13) | 0.0195 (12) | −0.0095 (13) |
| C6 | 0.0464 (13) | 0.0524 (16) | 0.0508 (14) | −0.0025 (12) | 0.0140 (11) | −0.0058 (12) |
| C7 | 0.0495 (14) | 0.0462 (15) | 0.0470 (14) | −0.0030 (11) | 0.0130 (11) | −0.0019 (11) |
| C8 | 0.0474 (14) | 0.0469 (15) | 0.0446 (13) | −0.0029 (11) | 0.0119 (11) | −0.0032 (11) |
| C9 | 0.0551 (15) | 0.0542 (17) | 0.0440 (14) | −0.0031 (12) | 0.0136 (12) | 0.0031 (11) |
| C10 | 0.0587 (16) | 0.0499 (16) | 0.0518 (15) | 0.0000 (12) | 0.0159 (13) | 0.0066 (12) |
| C11 | 0.0517 (15) | 0.0486 (16) | 0.0548 (15) | 0.0031 (12) | 0.0106 (12) | 0.0008 (12) |
| C12 | 0.0474 (14) | 0.0437 (15) | 0.0480 (14) | −0.0022 (11) | 0.0108 (11) | −0.0047 (11) |
| C13 | 0.0478 (14) | 0.0440 (15) | 0.0515 (14) | −0.0022 (11) | 0.0140 (11) | −0.0038 (11) |
| C14 | 0.0536 (15) | 0.0539 (17) | 0.0570 (16) | −0.0096 (12) | 0.0211 (13) | −0.0116 (13) |
| C15 | 0.0624 (17) | 0.068 (2) | 0.0706 (19) | −0.0118 (15) | 0.0260 (15) | −0.0182 (16) |
| C16 | 0.0716 (19) | 0.076 (2) | 0.070 (2) | −0.0209 (17) | 0.0358 (16) | −0.0247 (17) |
| C17 | 0.081 (2) | 0.082 (2) | 0.0552 (17) | −0.0275 (18) | 0.0271 (16) | −0.0105 (16) |
| C18 | 0.0663 (17) | 0.0607 (19) | 0.0588 (16) | −0.0094 (14) | 0.0202 (14) | −0.0025 (14) |
| C19 | 0.0548 (15) | 0.0552 (17) | 0.0486 (15) | −0.0087 (12) | 0.0145 (12) | −0.0072 (12) |
| C20 | 0.073 (2) | 0.091 (3) | 0.070 (2) | −0.0099 (18) | 0.0166 (17) | 0.0182 (18) |
| C21 | 0.087 (2) | 0.073 (3) | 0.131 (3) | 0.0229 (19) | 0.037 (2) | 0.005 (2) |
| O3 | 0.106 (4) | 0.102 (4) | 0.070 (3) | −0.012 (3) | 0.021 (3) | 0.001 (2) |
| C22 | 0.024 (4) | 0.086 (5) | 0.050 (3) | 0.011 (3) | 0.016 (4) | 0.010 (3) |
| O3' | 0.130 (8) | 0.127 (7) | 0.088 (5) | −0.044 (6) | 0.020 (5) | 0.001 (5) |
| C22' | 0.021 (7) | 0.147 (13) | 0.070 (7) | 0.039 (7) | 0.019 (6) | 0.000 (6) |
Geometric parameters (Å, °)
| O1—C20 | 1.427 (3) | C10—H10 | 0.9500 |
| O1—H1 | 0.8400 | C11—C12 | 1.399 (4) |
| O2—C21 | 1.415 (4) | C11—H11 | 0.9500 |
| O2—H2 | 0.8400 | C12—C13 | 1.460 (4) |
| N1—C7 | 1.363 (3) | C14—C15 | 1.398 (4) |
| N1—C1 | 1.383 (3) | C14—C19 | 1.402 (4) |
| N1—H1N | 0.866 (10) | C15—C16 | 1.372 (5) |
| N2—C7 | 1.324 (3) | C15—H15 | 0.9500 |
| N2—C6 | 1.399 (3) | C16—C17 | 1.404 (5) |
| N3—C13 | 1.354 (3) | C16—H16 | 0.9500 |
| N3—C19 | 1.381 (4) | C17—C18 | 1.372 (4) |
| N3—H3N | 0.863 (10) | C17—H17 | 0.9500 |
| N4—C13 | 1.321 (3) | C18—C19 | 1.385 (4) |
| N4—C14 | 1.386 (4) | C18—H18 | 0.9500 |
| N5—C8 | 1.338 (3) | C20—H20A | 0.9800 |
| N5—C12 | 1.341 (3) | C20—H20B | 0.9800 |
| C1—C2 | 1.386 (4) | C20—H20C | 0.9800 |
| C1—C6 | 1.402 (4) | C21—H21A | 0.9800 |
| C2—C3 | 1.381 (4) | C21—H21B | 0.9800 |
| C2—H2A | 0.9500 | C21—H21C | 0.9800 |
| C3—C4 | 1.398 (4) | O3—C22 | 1.414 (10) |
| C3—H3 | 0.9500 | O3—H3A | 0.8400 |
| C4—C5 | 1.367 (4) | C22—H22A | 0.9800 |
| C4—H4 | 0.9500 | C22—H22B | 0.9800 |
| C5—C6 | 1.397 (4) | C22—H22C | 0.9800 |
| C5—H5 | 0.9500 | O3'—C22' | 1.324 (19) |
| C7—C8 | 1.459 (4) | O3'—H3' | 0.8400 |
| C8—C9 | 1.389 (3) | C22'—H22D | 0.9800 |
| C9—C10 | 1.383 (4) | C22'—H22E | 0.9800 |
| C9—H9 | 0.9500 | C22'—H22F | 0.9800 |
| C10—C11 | 1.374 (4) | ||
| C20—O1—H1 | 109.5 | N5—C12—C11 | 122.3 (3) |
| C21—O2—H2 | 109.5 | N5—C12—C13 | 114.4 (2) |
| C7—N1—C1 | 107.3 (2) | C11—C12—C13 | 123.4 (2) |
| C7—N1—H1N | 126 (2) | N4—C13—N3 | 112.8 (2) |
| C1—N1—H1N | 126 (2) | N4—C13—C12 | 126.1 (2) |
| C7—N2—C6 | 104.5 (2) | N3—C13—C12 | 121.0 (2) |
| C13—N3—C19 | 107.4 (2) | N4—C14—C15 | 130.3 (3) |
| C13—N3—H3N | 128 (3) | N4—C14—C19 | 109.9 (2) |
| C19—N3—H3N | 125 (3) | C15—C14—C19 | 119.8 (3) |
| C13—N4—C14 | 105.0 (2) | C16—C15—C14 | 117.8 (3) |
| C8—N5—C12 | 117.9 (2) | C16—C15—H15 | 121.1 |
| N1—C1—C2 | 132.8 (3) | C14—C15—H15 | 121.1 |
| N1—C1—C6 | 105.1 (2) | C15—C16—C17 | 121.4 (3) |
| C2—C1—C6 | 122.1 (3) | C15—C16—H16 | 119.3 |
| C3—C2—C1 | 116.7 (3) | C17—C16—H16 | 119.3 |
| C3—C2—H2A | 121.6 | C18—C17—C16 | 121.7 (3) |
| C1—C2—H2A | 121.6 | C18—C17—H17 | 119.1 |
| C2—C3—C4 | 121.4 (3) | C16—C17—H17 | 119.1 |
| C2—C3—H3 | 119.3 | C17—C18—C19 | 116.9 (3) |
| C4—C3—H3 | 119.3 | C17—C18—H18 | 121.6 |
| C5—C4—C3 | 122.2 (3) | C19—C18—H18 | 121.6 |
| C5—C4—H4 | 118.9 | N3—C19—C18 | 132.6 (3) |
| C3—C4—H4 | 118.9 | N3—C19—C14 | 104.9 (2) |
| C4—C5—C6 | 117.3 (3) | C18—C19—C14 | 122.4 (3) |
| C4—C5—H5 | 121.4 | O1—C20—H20A | 109.5 |
| C6—C5—H5 | 121.4 | O1—C20—H20B | 109.5 |
| C5—C6—N2 | 129.6 (3) | H20A—C20—H20B | 109.5 |
| C5—C6—C1 | 120.4 (3) | O1—C20—H20C | 109.5 |
| N2—C6—C1 | 110.1 (2) | H20A—C20—H20C | 109.5 |
| N2—C7—N1 | 113.1 (2) | H20B—C20—H20C | 109.5 |
| N2—C7—C8 | 126.1 (2) | O2—C21—H21A | 109.5 |
| N1—C7—C8 | 120.8 (2) | O2—C21—H21B | 109.5 |
| N5—C8—C9 | 123.3 (2) | H21A—C21—H21B | 109.5 |
| N5—C8—C7 | 114.4 (2) | O2—C21—H21C | 109.5 |
| C9—C8—C7 | 122.2 (2) | H21A—C21—H21C | 109.5 |
| C10—C9—C8 | 118.2 (3) | H21B—C21—H21C | 109.5 |
| C10—C9—H9 | 120.9 | C22'—O3'—H3' | 109.5 |
| C8—C9—H9 | 120.9 | O3'—C22'—H22D | 109.5 |
| C11—C10—C9 | 119.5 (2) | O3'—C22'—H22E | 109.5 |
| C11—C10—H10 | 120.3 | H22D—C22'—H22E | 109.5 |
| C9—C10—H10 | 120.3 | O3'—C22'—H22F | 109.5 |
| C10—C11—C12 | 118.8 (2) | H22D—C22'—H22F | 109.5 |
| C10—C11—H11 | 120.6 | H22E—C22'—H22F | 109.5 |
| C12—C11—H11 | 120.6 | ||
| C7—N1—C1—C2 | 179.1 (3) | C9—C10—C11—C12 | 0.2 (4) |
| C7—N1—C1—C6 | −0.4 (3) | C8—N5—C12—C11 | −0.5 (3) |
| N1—C1—C2—C3 | 179.4 (3) | C8—N5—C12—C13 | −179.5 (2) |
| C6—C1—C2—C3 | −1.1 (4) | C10—C11—C12—N5 | 0.4 (4) |
| C1—C2—C3—C4 | 0.1 (4) | C10—C11—C12—C13 | 179.4 (2) |
| C2—C3—C4—C5 | 0.4 (4) | C14—N4—C13—N3 | 1.0 (3) |
| C3—C4—C5—C6 | 0.0 (4) | C14—N4—C13—C12 | −178.6 (2) |
| C4—C5—C6—N2 | 179.5 (2) | C19—N3—C13—N4 | −0.9 (3) |
| C4—C5—C6—C1 | −1.0 (4) | C19—N3—C13—C12 | 178.7 (2) |
| C7—N2—C6—C5 | 178.7 (3) | N5—C12—C13—N4 | 179.9 (2) |
| C7—N2—C6—C1 | −0.9 (3) | C11—C12—C13—N4 | 0.8 (4) |
| N1—C1—C6—C5 | −178.8 (2) | N5—C12—C13—N3 | 0.3 (3) |
| C2—C1—C6—C5 | 1.6 (4) | C11—C12—C13—N3 | −178.7 (2) |
| N1—C1—C6—N2 | 0.8 (3) | C13—N4—C14—C15 | 178.1 (3) |
| C2—C1—C6—N2 | −178.8 (2) | C13—N4—C14—C19 | −0.7 (3) |
| C6—N2—C7—N1 | 0.6 (3) | N4—C14—C15—C16 | −178.7 (3) |
| C6—N2—C7—C8 | 179.5 (2) | C19—C14—C15—C16 | 0.1 (4) |
| C1—N1—C7—N2 | −0.1 (3) | C14—C15—C16—C17 | −0.2 (4) |
| C1—N1—C7—C8 | −179.1 (2) | C15—C16—C17—C18 | 0.6 (5) |
| C12—N5—C8—C9 | −0.1 (3) | C16—C17—C18—C19 | −0.9 (4) |
| C12—N5—C8—C7 | −179.9 (2) | C13—N3—C19—C18 | −177.7 (3) |
| N2—C7—C8—N5 | −178.7 (2) | C13—N3—C19—C14 | 0.4 (3) |
| N1—C7—C8—N5 | 0.1 (3) | C17—C18—C19—N3 | 178.6 (3) |
| N2—C7—C8—C9 | 1.5 (4) | C17—C18—C19—C14 | 0.8 (4) |
| N1—C7—C8—C9 | −179.7 (2) | N4—C14—C19—N3 | 0.2 (3) |
| N5—C8—C9—C10 | 0.7 (4) | C15—C14—C19—N3 | −178.7 (2) |
| C7—C8—C9—C10 | −179.6 (2) | N4—C14—C19—C18 | 178.6 (2) |
| C8—C9—C10—C11 | −0.7 (4) | C15—C14—C19—C18 | −0.4 (4) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1—H1···O2i | 0.84 | 1.83 | 2.670 (3) | 176 |
| O2—H2···N4 | 0.84 | 1.91 | 2.741 (3) | 168 |
| N1—H1N···O1 | 0.87 (1) | 2.07 (1) | 2.927 (3) | 171 (3) |
| N3—H3N···O1 | 0.86 (1) | 2.07 (1) | 2.925 (3) | 171 (4) |
Symmetry codes: (i) −x+1, −y+1, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH2799).
References
- Addison, A. W. & Burke, P. J. (1981). J. Heterocycl. Chem 18, 803–805.
- Freire, E., Baggio, S., Muñoz, J. C. & Baggio, R. (2003). Acta Cryst. C59, o259–o262. [DOI] [PubMed]
- Higashi, T. (1995). Rigaku Corporation, Tokyo, Japan.
- Rigaku/MSC (2004). RAPID-AUTO Rigaku/MSC, The Woodlans, Texas, USA.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst D65, 148–155. [DOI] [PMC free article] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809012574/lh2799sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809012574/lh2799Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


