Abstract
The title compound, [Ni(C60H52N4)], is an example of a meso tetrasubstituted nickel(II) porphyrin with both meso aryl and alkyl residues. The molecule exhibits a planar macrocycle with an average deviation of the 24 macrocycle atoms from their least-squares plane (Δ24) of 0.01 Å and an average Ni—N bond length of 1.960 (2) Å. The NiII atom lies on a center of inversion. The structure presents a rare example for a planar nickel(II) porphyrin, as meso-substituted nickel(II) porphyrins with either only meso-aryl or with meso-alkyl residues typically exhibit a ruffled conformation.
Related literature
For the conformation of porphyrins, see: Senge (2006 ▶). For porphyrins with mixed meso substituents, see: Senge et al. (2010 ▶). For Ni(II) porphyrin structures, see: Fleischer et al. (1964 ▶); Gallucci et al. (1982 ▶); Hoard (1973 ▶); Lee & Scheidt (1987 ▶); Senge et al. (1999 ▶, 2000 ▶) and Runge et al. (1999 ▶). For anthracenyl porphyrins see: Volz & Schäffer (1985 ▶); Davis et al. (2008 ▶); Sooambar et al. (2009 ▶). For the handling of the crystals, see: Hope (1994 ▶).
Experimental
Crystal data
[Ni(C60H52N4)]
M r = 887.77
Triclinic,
a = 7.797 (3) Å
b = 9.387 (3) Å
c = 15.285 (5) Å
α = 97.246 (6)°
β = 91.222 (4)°
γ = 91.402 (6)°
V = 1109.1 (7) Å3
Z = 1
Mo Kα radiation
μ = 0.48 mm−1
T = 118 K
0.50 × 0.20 × 0.05 mm
Data collection
Rigaku Saturn724 diffractometer
17330 measured reflections
3875 independent reflections
3233 reflections with I > 2σ(I)
R int = 0.070
Refinement
R[F 2 > 2σ(F 2)] = 0.039
wR(F 2) = 0.087
S = 1.00
3875 reflections
296 parameters
H-atom parameters constrained
Δρmax = 0.37 e Å−3
Δρmin = −0.40 e Å−3
Data collection: CrystalClear (Rigaku, 2008 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810021434/ng2783sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810021434/ng2783Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected bond lengths (Å).
| Ni—N22 | 1.9570 (17) |
| Ni—N21 | 1.9632 (17) |
Acknowledgments
This work was supported by a grant from Science Foundation Ireland (SFI P.I. 09/IN.1/B2650).
supplementary crystallographic information
Comment
In continuation of studies on the conformational flexibility of porphyrins (Senge, 2006) the structure of the title compound was determined as an example for a meso substituted porphyrin with both meso alkyl and meso aryl subsitutents (Senge et al., 2010) and in relation to current synthetic studies on anthracenyl porphyrins (Volz & Schäffer, 1985; Davis et al., 2008; Sooambar et al., 2009).
The structure of (I), is shown in Fig. 1. The molecule exhibits a completely planar macrocycle with an average deviation of the 24 macrocycle atoms from their least-squares-plane (Δ24) of 0.01 Å and an average Ni—N bond length of 1.960 (2) Å. All geometrical parameters are typical for a planar nickel(II) porphyrin (Senge et al., 2000). No individual macrocycle atom was displaced more then 0.015 Å from the mean plane. Likewise, differences in bond angles and lenghts between the meso aryl and meso alkyl quadrants are minimal. The anthracenyl residues are almost orthogonal to the plane of the four nitrogen atoms (96.2°) similarly to the situation found in related zinc(II) systems with meso aryl residues (Sooambar et al., 2009). In the crystal packing there are no close contacts (not shown). The anthracene residues prevent π-stacking of the porphyrins and the hexyl side chains are oriented between neighboring anthracenyl substituents and hinder π-stacking as well.
The structure presents a rare example for a planar nickel(II) porphyrin. Typically, meso substituted nickel(II) porphyrins with only meso aryl residues (Fleischer et al., 1964; Hoard, 1973; Lee & Scheidt, 1987) and those with meso alkyl residues (Senge et al., 1999; Runge et al., 1999) exhibit a ruffled conformation. Only (5,10,15,20-tetramethylporphyrinato)nickel(II) exbihits an almost planar conformation as well (Gallucci et al., 1982).
Experimental
The compound was prepared via metallation of the respective free base porphyrin and crystallized via liquid diffusion of methanol into a solution of the porphyrin in methylene chloride. Crystals were handled as described by Hope (1994).
Refinement
Hydrogen atoms were located in difference maps and refined using a standard riding model.
Figures
Fig. 1.
: View of the molecular structure of I in the crystals. Thermal ellipsoids are drawn for 50% occupancy.
Crystal data
| [Ni(C60H52N4)] | Z = 1 |
| Mr = 887.77 | F(000) = 468 |
| Triclinic, P1 | Dx = 1.329 Mg m−3 |
| Hall symbol: -P 1 | Melting point: n/d K |
| a = 7.797 (3) Å | Mo Kα radiation, λ = 0.71075 Å |
| b = 9.387 (3) Å | Cell parameters from 3864 reflections |
| c = 15.285 (5) Å | θ = 2.4–31.2° |
| α = 97.246 (6)° | µ = 0.48 mm−1 |
| β = 91.222 (4)° | T = 118 K |
| γ = 91.402 (6)° | Prism, red |
| V = 1109.1 (7) Å3 | 0.50 × 0.20 × 0.05 mm |
Data collection
| Rigaku Saturn724 diffractometer | 3233 reflections with I > 2σ(I) |
| Radiation source: Sealed Tube | Rint = 0.070 |
| Graphite Monochromator | θmax = 25.0°, θmin = 3.0° |
| Detector resolution: 28.5714 pixels mm-1 | h = −9→9 |
| dtprofit.ref scans | k = −11→11 |
| 17330 measured reflections | l = −18→18 |
| 3875 independent reflections |
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)] = 0.039 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.087 | H-atom parameters constrained |
| S = 1.00 | w = 1/[σ2(Fo2) + (0.0371P)2] where P = (Fo2 + 2Fc2)/3 |
| 3875 reflections | (Δ/σ)max < 0.001 |
| 296 parameters | Δρmax = 0.37 e Å−3 |
| 0 restraints | Δρmin = −0.40 e Å−3 |
| 0 constraints |
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 | ||
| Ni | 0.0000 | 0.5000 | 0.0000 | 0.01798 (12) | |
| N21 | 0.1442 (2) | 0.47152 (16) | 0.10290 (10) | 0.0185 (4) | |
| N22 | 0.1822 (2) | 0.62389 (16) | −0.03788 (10) | 0.0192 (4) | |
| C5 | −0.0499 (3) | 0.31349 (19) | 0.17545 (13) | 0.0185 (4) | |
| C6 | 0.1022 (3) | 0.3901 (2) | 0.16960 (13) | 0.0198 (5) | |
| C7 | 0.2375 (3) | 0.3969 (2) | 0.23403 (13) | 0.0247 (5) | |
| H7A | 0.2383 | 0.3500 | 0.2856 | 0.030* | |
| C8 | 0.3643 (3) | 0.4817 (2) | 0.20886 (14) | 0.0243 (5) | |
| H8A | 0.4707 | 0.5059 | 0.2391 | 0.029* | |
| C9 | 0.3069 (3) | 0.5284 (2) | 0.12716 (13) | 0.0194 (5) | |
| C10 | 0.4031 (3) | 0.6194 (2) | 0.08102 (13) | 0.0204 (5) | |
| C11 | 0.3407 (3) | 0.6617 (2) | 0.00254 (13) | 0.0197 (5) | |
| C12 | 0.4362 (3) | 0.7542 (2) | −0.04785 (14) | 0.0244 (5) | |
| H12A | 0.5476 | 0.7949 | −0.0337 | 0.029* | |
| C13 | 0.3384 (3) | 0.7725 (2) | −0.11872 (14) | 0.0248 (5) | |
| H13A | 0.3677 | 0.8283 | −0.1642 | 0.030* | |
| C14 | 0.1820 (3) | 0.69232 (19) | −0.11298 (13) | 0.0190 (5) | |
| C5A | −0.0738 (3) | 0.2335 (2) | 0.25355 (13) | 0.0205 (5) | |
| C5B | −0.0381 (3) | 0.0855 (2) | 0.24777 (14) | 0.0230 (5) | |
| C5C | 0.0207 (3) | 0.0055 (2) | 0.16833 (15) | 0.0263 (5) | |
| H5CA | 0.0405 | 0.0534 | 0.1181 | 0.032* | |
| C5D | 0.0488 (3) | −0.1376 (2) | 0.16363 (16) | 0.0334 (6) | |
| H5DA | 0.0880 | −0.1884 | 0.1104 | 0.040* | |
| C5E | 0.0197 (3) | −0.2119 (2) | 0.23800 (17) | 0.0360 (6) | |
| H5EA | 0.0382 | −0.3122 | 0.2338 | 0.043* | |
| C5F | −0.0339 (3) | −0.1403 (2) | 0.31441 (16) | 0.0321 (6) | |
| H5FA | −0.0517 | −0.1913 | 0.3635 | 0.038* | |
| C5G | −0.0645 (3) | 0.0104 (2) | 0.32312 (14) | 0.0255 (5) | |
| C5H | −0.1190 (3) | 0.0864 (2) | 0.40177 (14) | 0.0276 (5) | |
| H5HA | −0.1338 | 0.0367 | 0.4516 | 0.033* | |
| C5I | −0.1523 (3) | 0.2321 (2) | 0.40970 (13) | 0.0230 (5) | |
| C5J | −0.2098 (3) | 0.3101 (2) | 0.48906 (14) | 0.0318 (6) | |
| H5JA | −0.2196 | 0.2628 | 0.5402 | 0.038* | |
| C5K | −0.2508 (3) | 0.4502 (2) | 0.49355 (15) | 0.0393 (6) | |
| H5KA | −0.2877 | 0.5003 | 0.5475 | 0.047* | |
| C5L | −0.2383 (3) | 0.5230 (2) | 0.41624 (15) | 0.0347 (6) | |
| H5LA | −0.2719 | 0.6200 | 0.4186 | 0.042* | |
| C5M | −0.1797 (3) | 0.4549 (2) | 0.34139 (15) | 0.0298 (5) | |
| H5MA | −0.1677 | 0.5061 | 0.2920 | 0.036* | |
| C5N | −0.1344 (3) | 0.3070 (2) | 0.33320 (13) | 0.0230 (5) | |
| C10A | 0.5771 (3) | 0.6803 (2) | 0.11646 (13) | 0.0235 (5) | |
| H10A | 0.6577 | 0.6781 | 0.0671 | 0.028* | |
| H10B | 0.6232 | 0.6189 | 0.1591 | 0.028* | |
| C10B | 0.5667 (3) | 0.8359 (2) | 0.16236 (13) | 0.0265 (5) | |
| H10C | 0.6835 | 0.8805 | 0.1670 | 0.032* | |
| H10D | 0.4955 | 0.8913 | 0.1250 | 0.032* | |
| C10C | 0.4915 (3) | 0.8477 (2) | 0.25444 (14) | 0.0279 (5) | |
| H10E | 0.5718 | 0.8051 | 0.2943 | 0.033* | |
| H10F | 0.3823 | 0.7909 | 0.2514 | 0.033* | |
| C10D | 0.4574 (3) | 1.0030 (2) | 0.29382 (14) | 0.0287 (5) | |
| H10G | 0.5637 | 1.0622 | 0.2916 | 0.034* | |
| H10H | 0.3681 | 1.0425 | 0.2574 | 0.034* | |
| C10E | 0.4000 (3) | 1.0138 (2) | 0.38747 (15) | 0.0356 (6) | |
| H10I | 0.4938 | 0.9824 | 0.4246 | 0.043* | |
| H10J | 0.3004 | 0.9473 | 0.3904 | 0.043* | |
| C10F | 0.3500 (3) | 1.1641 (2) | 0.42523 (14) | 0.0316 (6) | |
| H10K | 0.3292 | 1.1666 | 0.4884 | 0.047* | |
| H10L | 0.2453 | 1.1900 | 0.3950 | 0.047* | |
| H10M | 0.4430 | 1.2326 | 0.4166 | 0.047* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Ni | 0.0227 (2) | 0.0162 (2) | 0.0154 (2) | −0.00037 (16) | 0.00200 (15) | 0.00351 (15) |
| N21 | 0.0227 (10) | 0.0156 (8) | 0.0174 (9) | −0.0013 (7) | 0.0034 (7) | 0.0021 (7) |
| N22 | 0.0240 (10) | 0.0184 (9) | 0.0155 (9) | 0.0016 (8) | 0.0008 (7) | 0.0030 (7) |
| C5 | 0.0243 (12) | 0.0137 (10) | 0.0171 (10) | −0.0003 (9) | 0.0026 (9) | 0.0004 (8) |
| C6 | 0.0279 (13) | 0.0145 (10) | 0.0170 (11) | 0.0015 (9) | 0.0004 (9) | 0.0020 (8) |
| C7 | 0.0307 (13) | 0.0231 (11) | 0.0212 (11) | −0.0003 (10) | −0.0011 (10) | 0.0069 (9) |
| C8 | 0.0244 (12) | 0.0235 (11) | 0.0252 (12) | −0.0005 (9) | −0.0043 (9) | 0.0048 (9) |
| C9 | 0.0219 (12) | 0.0161 (10) | 0.0198 (11) | 0.0005 (9) | 0.0000 (9) | 0.0005 (9) |
| C10 | 0.0215 (12) | 0.0177 (10) | 0.0211 (11) | 0.0032 (9) | 0.0025 (9) | −0.0015 (9) |
| C11 | 0.0208 (12) | 0.0171 (10) | 0.0204 (11) | −0.0007 (9) | 0.0021 (9) | −0.0005 (9) |
| C12 | 0.0243 (12) | 0.0245 (11) | 0.0246 (12) | −0.0043 (9) | 0.0021 (9) | 0.0047 (9) |
| C13 | 0.0282 (13) | 0.0248 (11) | 0.0221 (11) | −0.0045 (10) | 0.0024 (9) | 0.0061 (9) |
| C14 | 0.0249 (12) | 0.0138 (10) | 0.0184 (10) | −0.0005 (9) | 0.0027 (9) | 0.0028 (8) |
| C5A | 0.0206 (12) | 0.0199 (11) | 0.0209 (11) | −0.0033 (9) | −0.0013 (9) | 0.0036 (9) |
| C5B | 0.0215 (12) | 0.0224 (11) | 0.0254 (12) | −0.0028 (9) | −0.0011 (9) | 0.0050 (9) |
| C5C | 0.0235 (12) | 0.0243 (12) | 0.0312 (13) | −0.0006 (10) | 0.0029 (10) | 0.0029 (10) |
| C5D | 0.0297 (14) | 0.0295 (13) | 0.0400 (14) | 0.0025 (11) | 0.0049 (11) | 0.0001 (11) |
| C5E | 0.0338 (15) | 0.0204 (12) | 0.0548 (17) | 0.0030 (10) | 0.0046 (12) | 0.0073 (11) |
| C5F | 0.0275 (14) | 0.0275 (12) | 0.0445 (15) | 0.0023 (10) | 0.0012 (11) | 0.0166 (11) |
| C5G | 0.0227 (12) | 0.0242 (12) | 0.0308 (12) | −0.0018 (9) | −0.0011 (10) | 0.0088 (10) |
| C5H | 0.0259 (13) | 0.0333 (13) | 0.0259 (12) | −0.0043 (10) | −0.0008 (10) | 0.0135 (10) |
| C5I | 0.0234 (12) | 0.0244 (11) | 0.0218 (11) | −0.0032 (9) | 0.0020 (9) | 0.0056 (9) |
| C5J | 0.0353 (14) | 0.0375 (14) | 0.0232 (12) | −0.0075 (11) | 0.0003 (10) | 0.0075 (10) |
| C5K | 0.0509 (17) | 0.0376 (14) | 0.0268 (13) | −0.0036 (12) | 0.0092 (12) | −0.0069 (11) |
| C5L | 0.0490 (17) | 0.0188 (11) | 0.0359 (14) | 0.0024 (11) | 0.0132 (12) | −0.0006 (10) |
| C5M | 0.0370 (14) | 0.0257 (12) | 0.0282 (13) | −0.0016 (10) | 0.0020 (10) | 0.0090 (10) |
| C5N | 0.0238 (12) | 0.0220 (11) | 0.0234 (11) | −0.0015 (9) | 0.0003 (9) | 0.0035 (9) |
| C10A | 0.0212 (12) | 0.0290 (12) | 0.0209 (11) | −0.0013 (9) | 0.0002 (9) | 0.0059 (9) |
| C10B | 0.0222 (12) | 0.0306 (12) | 0.0262 (12) | −0.0058 (10) | −0.0007 (10) | 0.0035 (10) |
| C10C | 0.0286 (13) | 0.0284 (12) | 0.0269 (12) | −0.0013 (10) | −0.0015 (10) | 0.0048 (10) |
| C10D | 0.0265 (13) | 0.0316 (12) | 0.0282 (12) | −0.0031 (10) | −0.0030 (10) | 0.0057 (10) |
| C10E | 0.0428 (16) | 0.0354 (13) | 0.0285 (13) | 0.0020 (11) | 0.0001 (11) | 0.0033 (11) |
| C10F | 0.0368 (15) | 0.0288 (12) | 0.0289 (13) | 0.0039 (11) | 0.0004 (11) | 0.0019 (10) |
Geometric parameters (Å, °)
| Ni—N22 | 1.9570 (17) | C5E—H5EA | 0.9500 |
| Ni—N22i | 1.9570 (17) | C5F—C5G | 1.430 (3) |
| Ni—N21i | 1.9632 (17) | C5F—H5FA | 0.9500 |
| Ni—N21 | 1.9632 (17) | C5G—C5H | 1.399 (3) |
| N21—C6 | 1.389 (2) | C5H—C5I | 1.389 (3) |
| N21—C9 | 1.389 (3) | C5H—H5HA | 0.9500 |
| N22—C14 | 1.384 (2) | C5I—C5J | 1.423 (3) |
| N22—C11 | 1.388 (3) | C5I—C5N | 1.446 (3) |
| C5—C6 | 1.382 (3) | C5J—C5K | 1.354 (3) |
| C5—C14i | 1.385 (3) | C5J—H5JA | 0.9500 |
| C5—C5A | 1.501 (3) | C5K—C5L | 1.442 (3) |
| C6—C7 | 1.423 (3) | C5K—H5KA | 0.9500 |
| C7—C8 | 1.346 (3) | C5L—C5M | 1.333 (3) |
| C7—H7A | 0.9500 | C5L—H5LA | 0.9500 |
| C8—C9 | 1.441 (3) | C5M—C5N | 1.433 (3) |
| C8—H8A | 0.9500 | C5M—H5MA | 0.9500 |
| C9—C10 | 1.390 (3) | C10A—C10B | 1.544 (3) |
| C10—C11 | 1.392 (3) | C10A—H10A | 0.9900 |
| C10—C10A | 1.521 (3) | C10A—H10B | 0.9900 |
| C11—C12 | 1.436 (3) | C10B—C10C | 1.529 (3) |
| C12—C13 | 1.343 (3) | C10B—H10C | 0.9900 |
| C12—H12A | 0.9500 | C10B—H10D | 0.9900 |
| C13—C14 | 1.427 (3) | C10C—C10D | 1.538 (3) |
| C13—H13A | 0.9500 | C10C—H10E | 0.9900 |
| C14—C5i | 1.385 (3) | C10C—H10F | 0.9900 |
| C5A—C5B | 1.416 (3) | C10D—C10E | 1.501 (3) |
| C5A—C5N | 1.417 (3) | C10D—H10G | 0.9900 |
| C5B—C5C | 1.435 (3) | C10D—H10H | 0.9900 |
| C5B—C5G | 1.440 (3) | C10E—C10F | 1.518 (3) |
| C5C—C5D | 1.359 (3) | C10E—H10I | 0.9900 |
| C5C—H5CA | 0.9500 | C10E—H10J | 0.9900 |
| C5D—C5E | 1.426 (3) | C10F—H10K | 0.9800 |
| C5D—H5DA | 0.9500 | C10F—H10L | 0.9800 |
| C5E—C5F | 1.352 (3) | C10F—H10M | 0.9800 |
| N22—Ni—N22i | 180.00 (8) | C5H—C5G—C5F | 122.4 (2) |
| N22—Ni—N21i | 91.02 (7) | C5H—C5G—C5B | 119.23 (19) |
| N22i—Ni—N21i | 88.98 (7) | C5F—C5G—C5B | 118.4 (2) |
| N22—Ni—N21 | 88.98 (7) | C5I—C5H—C5G | 122.40 (19) |
| N22i—Ni—N21 | 91.02 (7) | C5I—C5H—H5HA | 118.8 |
| N21i—Ni—N21 | 180.00 (9) | C5G—C5H—H5HA | 118.8 |
| C6—N21—C9 | 104.27 (16) | C5H—C5I—C5J | 122.86 (19) |
| C6—N21—Ni | 126.74 (14) | C5H—C5I—C5N | 118.78 (19) |
| C9—N21—Ni | 128.98 (13) | C5J—C5I—C5N | 118.31 (19) |
| C14—N22—C11 | 104.18 (16) | C5K—C5J—C5I | 121.6 (2) |
| C14—N22—Ni | 127.19 (14) | C5K—C5J—H5JA | 119.2 |
| C11—N22—Ni | 128.63 (13) | C5I—C5J—H5JA | 119.2 |
| C6—C5—C14i | 123.17 (18) | C5J—C5K—C5L | 119.8 (2) |
| C6—C5—C5A | 118.53 (18) | C5J—C5K—H5KA | 120.1 |
| C14i—C5—C5A | 118.30 (18) | C5L—C5K—H5KA | 120.1 |
| C5—C6—N21 | 126.01 (18) | C5M—C5L—C5K | 120.3 (2) |
| C5—C6—C7 | 123.21 (18) | C5M—C5L—H5LA | 119.8 |
| N21—C6—C7 | 110.77 (18) | C5K—C5L—H5LA | 119.8 |
| C8—C7—C6 | 107.78 (19) | C5L—C5M—C5N | 122.0 (2) |
| C8—C7—H7A | 126.1 | C5L—C5M—H5MA | 119.0 |
| C6—C7—H7A | 126.1 | C5N—C5M—H5MA | 119.0 |
| C7—C8—C9 | 106.63 (19) | C5A—C5N—C5M | 122.31 (19) |
| C7—C8—H8A | 126.7 | C5A—C5N—C5I | 119.88 (18) |
| C9—C8—H8A | 126.7 | C5M—C5N—C5I | 117.81 (18) |
| N21—C9—C10 | 125.85 (19) | C10—C10A—C10B | 112.21 (17) |
| N21—C9—C8 | 110.55 (17) | C10—C10A—H10A | 109.2 |
| C10—C9—C8 | 123.6 (2) | C10B—C10A—H10A | 109.2 |
| C9—C10—C11 | 121.1 (2) | C10—C10A—H10B | 109.2 |
| C9—C10—C10A | 121.00 (19) | C10B—C10A—H10B | 109.2 |
| C11—C10—C10A | 117.87 (18) | H10A—C10A—H10B | 107.9 |
| N22—C11—C10 | 126.47 (18) | C10C—C10B—C10A | 113.98 (17) |
| N22—C11—C12 | 110.47 (18) | C10C—C10B—H10C | 108.8 |
| C10—C11—C12 | 123.1 (2) | C10A—C10B—H10C | 108.8 |
| C13—C12—C11 | 107.1 (2) | C10C—C10B—H10D | 108.8 |
| C13—C12—H12A | 126.4 | C10A—C10B—H10D | 108.8 |
| C11—C12—H12A | 126.4 | H10C—C10B—H10D | 107.7 |
| C12—C13—C14 | 107.17 (19) | C10B—C10C—C10D | 113.40 (17) |
| C12—C13—H13A | 126.4 | C10B—C10C—H10E | 108.9 |
| C14—C13—H13A | 126.4 | C10D—C10C—H10E | 108.9 |
| N22—C14—C5i | 125.85 (19) | C10B—C10C—H10F | 108.9 |
| N22—C14—C13 | 111.04 (18) | C10D—C10C—H10F | 108.9 |
| C5i—C14—C13 | 123.11 (18) | H10E—C10C—H10F | 107.7 |
| C5B—C5A—C5N | 120.05 (18) | C10E—C10D—C10C | 112.63 (18) |
| C5B—C5A—C5 | 120.47 (18) | C10E—C10D—H10G | 109.1 |
| C5N—C5A—C5 | 119.47 (17) | C10C—C10D—H10G | 109.1 |
| C5A—C5B—C5C | 122.32 (19) | C10E—C10D—H10H | 109.1 |
| C5A—C5B—C5G | 119.53 (19) | C10C—C10D—H10H | 109.1 |
| C5C—C5B—C5G | 118.13 (18) | H10G—C10D—H10H | 107.8 |
| C5D—C5C—C5B | 121.2 (2) | C10D—C10E—C10F | 113.70 (18) |
| C5D—C5C—H5CA | 119.4 | C10D—C10E—H10I | 108.8 |
| C5B—C5C—H5CA | 119.4 | C10F—C10E—H10I | 108.8 |
| C5C—C5D—C5E | 120.5 (2) | C10D—C10E—H10J | 108.8 |
| C5C—C5D—H5DA | 119.8 | C10F—C10E—H10J | 108.8 |
| C5E—C5D—H5DA | 119.8 | H10I—C10E—H10J | 107.7 |
| C5F—C5E—C5D | 120.3 (2) | C10E—C10F—H10K | 109.5 |
| C5F—C5E—H5EA | 119.9 | C10E—C10F—H10L | 109.5 |
| C5D—C5E—H5EA | 119.9 | H10K—C10F—H10L | 109.5 |
| C5E—C5F—C5G | 121.6 (2) | C10E—C10F—H10M | 109.5 |
| C5E—C5F—H5FA | 119.2 | H10K—C10F—H10M | 109.5 |
| C5G—C5F—H5FA | 119.2 | H10L—C10F—H10M | 109.5 |
Symmetry codes: (i) −x, −y+1, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG2783).
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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 datablocks I, global. DOI: 10.1107/S1600536810021434/ng2783sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810021434/ng2783Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

