Abstract
The title compound, C22H19NO2, has potential for use as a new nonlinear optical material. Molecules are almost planar. One C atom of the heterocyclic ring system is disordered over two positions; the site occupancy factors are 0.6 and 0.4.
Related literature
For related literature, see: Honda et al. (1996 ▶); Allen (2002 ▶).
Experimental
Crystal data
C22H19NO2
M r = 329.38
Monoclinic,
a = 8.5125 (2) Å
b = 19.2973 (5) Å
c = 10.4969 (3) Å
β = 109.5301 (10)°
V = 1625.10 (7) Å3
Z = 4
Mo Kα radiation
μ = 0.09 mm−1
T = 293 (2) K
0.26 × 0.19 × 0.04 mm
Data collection
Nonius KappaCCD diffractometer
Absorption correction: none
6190 measured reflections
3685 independent reflections
2852 reflections with I > 2σ(I)
R int = 0.021
Refinement
R[F 2 > 2σ(F 2)] = 0.055
wR(F 2) = 0.155
S = 1.01
3685 reflections
255 parameters
H-atom parameters constrained
Δρmax = 0.27 e Å−3
Δρmin = −0.39 e Å−3
Data collection: KappaCCD Server Software (Nonius, 1999 ▶); cell refinement: KappaCCD Server Software; data reduction: DENZO and SCALEPACK (Otwinowski & Minor, 1997 ▶); program(s) used to solve structure: maXus (Mackay et al., 1999 ▶) and SIR92 (Altomare et al., 1994 ▶); program(s) used to refine structure: maXus and SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808016346/rk2090sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808016346/rk2090Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Acknowledgments
The authors acknowledge financial support from the Latvian Council of Science.
supplementary crystallographic information
Comment
The molecular structure of the title compound, C22H19NO2, (I), with atomic numbering scheme and thermal ellipsoids is presented in Fig. 1. The indandione fragment geometry is usual. The aromatic C14-C15 and C23-C24 bonds are shorter than other aromatic bonds in yulolidine system, indicating the quinoid character. Thus, presenting schematically the structure of I as two mesomeric forms (A or B) one can infer that the specific weight of the ionic form of B is increased (see Fig. 2). Therefore, the deep coloration occurs for the crystals I. A search of the Cambridge Structural Database (CSD, Version 5.29, November 2007; Allen, 2002) indicates that there are only 26 entries containing yulolidine fragments. For the title compound there is the disorder of crystal structure analogously to the crystal structure of "Coumarin 106" (Honda et al., 1996). In the yulolidine system the C17 atom is disordered and the site occupancies were initially refined then fixed at 0.6 and 0.4 for C17 and C17', respectively, in the final refinement. Atoms C17 and C17' are located on the opposite sides of the least-squares plane of the molecule. The atoms C17, C17' and C21 deviate from the molecule plane on 0.597 (4), -0.288 (6) and -0.527 (2)Å, respectively.
The packing diagram of the molecules is given in Fig. 3. The moderate π-π-stacking interaction in the crystal structure of (I) is between paris of inversion-related indandione systems. The five-membered cycle overlaps with the benzene ring of indandione; the centroids of these rings are separated by 3.509 (3)Å, but the distance between planes of these indandione systems is 3.435 (3)Å.
Experimental
A mixture of indan-1,3-dione, (0.44 g, 3.0 mmole), yulolidine-9-carbaldehyde (0.62 g, 3.1 mmole) of and 30 ml of absolute ethanol was boiled for 15 minutes, cooled to room temperature and filtered. Deep red crystals of I with metallic sheen were obtained after recrystallyzation from ethanol. M.p. is 504 K (decomp.); Yield 83%. Analysis calculated for C22H19NO2: C 80.22, H 5.81, N 4.25%; found: C 80.07, H 5.43, N 4.30%.
Refinement
The H atoms were place in geometrically idealized positions, with C–H distances of 0.93Å for aromatic H atoms and 0.96Å for other H-atoms. All H atoms were refined riding on their attached C atoms, with Uiso values equal to 1.2 times the Ueq values of the parent atoms.
Figures
Fig. 1.
The molecular structure of (I) with the atom numbering scheme. The displacement ellipsoids are showed at 50% probability level. H atoms are represented by spheres of arbitrary radii. Only major fragnent are presented for clarity.
Fig. 2.
Two mesomeric forms for molecular structure of I.
Fig. 3.
Perspective view of the molecular packing for I, showing the stacking interactions betwee indandione systems.
Crystal data
| C22H19NO2 | F000 = 696 |
| Mr = 329.38 | Dx = 1.346 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 6190 reflections |
| a = 8.5125 (2) Å | θ = 2.1–27.5º |
| b = 19.2973 (5) Å | µ = 0.09 mm−1 |
| c = 10.4969 (3) Å | T = 293 (2) K |
| β = 109.5301 (10)º | Plate, red |
| V = 1625.10 (7) Å3 | 0.26 × 0.19 × 0.04 mm |
| Z = 4 |
Data collection
| Nonius KappaCCD diffractometer | 2852 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.021 |
| Monochromator: graphite | θmax = 27.5º |
| T = 293(2) K | θmin = 2.1º |
| φ and ω scans | h = −11→11 |
| Absorption correction: none | k = −24→23 |
| 6190 measured reflections | l = −13→13 |
| 3685 independent reflections |
Refinement
| Refinement on F2 | Secondary atom site location: Difmap |
| Least-squares matrix: full | Hydrogen site location: Geom |
| R[F2 > 2σ(F2)] = 0.055 | H-atom parameters constrained |
| wR(F2) = 0.155 | Calculated w = 1/[σ2(Fo2) + (0.0792P)2 + 0.4361P] where P = (Fo2 + 2Fc2)/3 ? |
| S = 1.01 | (Δ/σ)max = 0.008 |
| 3685 reflections | Δρmax = 0.27 e Å−3 |
| 255 parameters | Δρmin = −0.39 e Å−3 |
| Primary atom site location: Direct | Extinction correction: none |
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 beeven larger. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | Occ. (<1) | |
| C1 | 1.0787 (2) | 0.02825 (8) | 0.26816 (16) | 0.0432 (4) | |
| C2 | 0.9234 (2) | −0.00221 (8) | 0.27606 (15) | 0.0423 (4) | |
| C3 | 0.8928 (2) | −0.06707 (8) | 0.19540 (17) | 0.0475 (4) | |
| C4 | 1.0528 (2) | −0.12254 (9) | 0.04817 (18) | 0.0539 (4) | |
| H4 | 0.9807 | −0.1600 | 0.0197 | 0.065* | |
| C5 | 1.1874 (2) | −0.11410 (10) | 0.00365 (19) | 0.0579 (5) | |
| H5 | 1.2054 | −0.1463 | −0.0560 | 0.069* | |
| C6 | 1.2957 (2) | −0.05867 (10) | 0.04616 (19) | 0.0585 (5) | |
| H6 | 1.3854 | −0.0542 | 0.0149 | 0.070* | |
| C7 | 1.2720 (2) | −0.00962 (9) | 0.13495 (18) | 0.0526 (4) | |
| H7 | 1.3447 | 0.0276 | 0.1640 | 0.063* | |
| C8 | 1.1372 (2) | −0.01783 (8) | 0.17868 (15) | 0.0432 (4) | |
| C9 | 1.0285 (2) | −0.07358 (8) | 0.13643 (16) | 0.0447 (4) | |
| O10 | 1.15210 (15) | 0.08098 (6) | 0.32016 (13) | 0.0576 (4) | |
| O11 | 0.77589 (18) | −0.10689 (7) | 0.17663 (15) | 0.0686 (4) | |
| C12 | 0.8117 (2) | 0.01796 (8) | 0.33618 (15) | 0.0439 (4) | |
| H12 | 0.7261 | −0.0140 | 0.3238 | 0.053* | |
| C13 | 0.79509 (19) | 0.07662 (8) | 0.41372 (15) | 0.0411 (4) | |
| C14 | 0.9044 (2) | 0.13387 (8) | 0.44714 (17) | 0.0462 (4) | |
| H14 | 0.9949 | 0.1349 | 0.4163 | 0.055* | |
| C15 | 0.8815 (2) | 0.18804 (8) | 0.52349 (18) | 0.0471 (4) | |
| C16 | 0.9979 (3) | 0.24908 (11) | 0.5566 (3) | 0.0806 (7) | |
| H16A | 1.1051 | 0.2352 | 0.5539 | 0.097* | 0.60 |
| H16B | 0.9532 | 0.2850 | 0.4912 | 0.097* | 0.60 |
| H16C | 1.1060 | 0.2347 | 0.6147 | 0.097* | 0.40 |
| H16D | 1.0066 | 0.2676 | 0.4744 | 0.097* | 0.40 |
| C17 | 1.0199 (4) | 0.27643 (19) | 0.6845 (4) | 0.0554 (7) | 0.60 |
| H17A | 1.0823 | 0.2443 | 0.7524 | 0.067* | 0.60 |
| H17B | 1.0798 | 0.3194 | 0.6949 | 0.067* | 0.60 |
| C17' | 0.9495 (7) | 0.3072 (3) | 0.6257 (6) | 0.0557 (11) | 0.40 |
| H17C | 1.0477 | 0.3309 | 0.6812 | 0.067* | 0.40 |
| H17D | 0.8808 | 0.3388 | 0.5597 | 0.067* | 0.40 |
| C18 | 0.8574 (2) | 0.29182 (10) | 0.7109 (2) | 0.0615 (5) | |
| H18A | 0.8169 | 0.3357 | 0.6700 | 0.074* | 0.60 |
| H18B | 0.8839 | 0.2952 | 0.8071 | 0.074* | 0.60 |
| H18C | 0.8064 | 0.3340 | 0.7258 | 0.074* | 0.40 |
| H18D | 0.9360 | 0.2761 | 0.7949 | 0.074* | 0.40 |
| N19 | 0.72946 (17) | 0.23902 (7) | 0.65742 (14) | 0.0466 (3) | |
| C20 | 0.5980 (2) | 0.23753 (10) | 0.71759 (18) | 0.0531 (4) | |
| H20A | 0.5683 | 0.2842 | 0.7317 | 0.064* | |
| H20B | 0.6392 | 0.2152 | 0.8042 | 0.064* | |
| C21 | 0.4455 (2) | 0.19991 (10) | 0.6302 (2) | 0.0557 (5) | |
| H21A | 0.3947 | 0.2258 | 0.5486 | 0.067* | |
| H21B | 0.3663 | 0.1964 | 0.6771 | 0.067* | |
| C22 | 0.4894 (2) | 0.12830 (9) | 0.59526 (18) | 0.0505 (4) | |
| H22A | 0.5184 | 0.0996 | 0.6744 | 0.061* | |
| H22B | 0.3941 | 0.1081 | 0.5283 | 0.061* | |
| C23 | 0.63360 (19) | 0.13043 (8) | 0.54173 (15) | 0.0405 (3) | |
| C24 | 0.65899 (19) | 0.07823 (8) | 0.46198 (16) | 0.0429 (4) | |
| H24 | 0.5825 | 0.0420 | 0.4385 | 0.051* | |
| C25 | 0.74777 (18) | 0.18666 (8) | 0.57636 (15) | 0.0386 (3) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0486 (8) | 0.0375 (8) | 0.0416 (8) | 0.0002 (6) | 0.0127 (6) | −0.0002 (6) |
| C2 | 0.0505 (9) | 0.0344 (7) | 0.0408 (7) | −0.0031 (6) | 0.0134 (7) | −0.0001 (6) |
| C3 | 0.0559 (9) | 0.0382 (8) | 0.0465 (9) | −0.0039 (7) | 0.0148 (7) | −0.0019 (7) |
| C4 | 0.0628 (11) | 0.0430 (9) | 0.0532 (10) | 0.0064 (8) | 0.0158 (8) | −0.0053 (7) |
| C5 | 0.0709 (12) | 0.0508 (10) | 0.0529 (10) | 0.0159 (9) | 0.0218 (9) | −0.0032 (8) |
| C6 | 0.0605 (11) | 0.0585 (11) | 0.0620 (11) | 0.0167 (9) | 0.0278 (9) | 0.0065 (9) |
| C7 | 0.0525 (10) | 0.0480 (9) | 0.0580 (10) | 0.0035 (7) | 0.0194 (8) | 0.0029 (8) |
| C8 | 0.0482 (8) | 0.0375 (8) | 0.0405 (8) | 0.0063 (6) | 0.0104 (7) | 0.0032 (6) |
| C9 | 0.0530 (9) | 0.0365 (8) | 0.0400 (8) | 0.0052 (7) | 0.0093 (7) | 0.0008 (6) |
| O10 | 0.0591 (7) | 0.0499 (7) | 0.0697 (8) | −0.0157 (6) | 0.0291 (6) | −0.0182 (6) |
| O11 | 0.0757 (9) | 0.0525 (8) | 0.0845 (10) | −0.0240 (7) | 0.0358 (7) | −0.0233 (7) |
| C12 | 0.0513 (9) | 0.0370 (8) | 0.0427 (8) | −0.0083 (6) | 0.0146 (7) | −0.0002 (6) |
| C13 | 0.0462 (8) | 0.0368 (7) | 0.0406 (8) | −0.0024 (6) | 0.0148 (6) | 0.0013 (6) |
| C14 | 0.0438 (8) | 0.0418 (8) | 0.0577 (10) | −0.0031 (7) | 0.0235 (7) | −0.0059 (7) |
| C15 | 0.0416 (8) | 0.0404 (8) | 0.0630 (10) | −0.0048 (6) | 0.0225 (7) | −0.0073 (7) |
| C16 | 0.0712 (13) | 0.0601 (12) | 0.135 (2) | −0.0293 (10) | 0.0664 (14) | −0.0441 (13) |
| C17 | 0.0490 (16) | 0.0517 (18) | 0.0645 (19) | −0.0096 (14) | 0.0176 (15) | −0.0153 (16) |
| C17' | 0.058 (3) | 0.044 (3) | 0.068 (3) | −0.010 (2) | 0.025 (2) | −0.007 (2) |
| C18 | 0.0574 (10) | 0.0550 (11) | 0.0747 (12) | −0.0070 (8) | 0.0258 (9) | −0.0237 (9) |
| N19 | 0.0465 (7) | 0.0460 (8) | 0.0511 (8) | −0.0001 (6) | 0.0211 (6) | −0.0054 (6) |
| C20 | 0.0578 (10) | 0.0537 (10) | 0.0554 (10) | 0.0087 (8) | 0.0291 (8) | 0.0006 (8) |
| C21 | 0.0482 (9) | 0.0641 (11) | 0.0634 (11) | 0.0081 (8) | 0.0299 (8) | 0.0103 (9) |
| C22 | 0.0479 (9) | 0.0550 (10) | 0.0527 (9) | −0.0050 (7) | 0.0223 (7) | 0.0063 (8) |
| C23 | 0.0393 (7) | 0.0432 (8) | 0.0384 (7) | −0.0009 (6) | 0.0122 (6) | 0.0073 (6) |
| C24 | 0.0455 (8) | 0.0393 (8) | 0.0433 (8) | −0.0078 (6) | 0.0140 (7) | 0.0023 (6) |
| C25 | 0.0380 (7) | 0.0376 (7) | 0.0390 (7) | 0.0029 (6) | 0.0113 (6) | 0.0033 (6) |
Geometric parameters (Å, °)
| C1—O10 | 1.2231 (19) | C17—C18 | 1.528 (4) |
| C1—C2 | 1.474 (2) | C17—H16C | 1.4431 |
| C1—C8 | 1.494 (2) | C17—H17A | 0.9600 |
| C2—C12 | 1.362 (2) | C17—H17B | 0.9600 |
| C2—C3 | 1.485 (2) | C17—H17C | 1.0804 |
| C3—O11 | 1.220 (2) | C17—H18D | 1.5509 |
| C3—C9 | 1.487 (2) | C17'—C18 | 1.405 (5) |
| C4—C5 | 1.384 (3) | C17'—H16B | 1.4854 |
| C4—C9 | 1.386 (2) | C17'—H17B | 1.1288 |
| C4—H4 | 0.9300 | C17'—H17C | 0.9599 |
| C5—C6 | 1.385 (3) | C17'—H17D | 0.9600 |
| C5—H5 | 0.9300 | C17'—H18A | 1.4642 |
| C6—C7 | 1.390 (3) | C18—N19 | 1.460 (2) |
| C6—H6 | 0.9300 | C18—H18A | 0.9600 |
| C7—C8 | 1.380 (2) | C18—H18B | 0.9600 |
| C7—H7 | 0.9300 | C18—H18C | 0.9600 |
| C8—C9 | 1.391 (2) | C18—H18D | 0.9600 |
| C12—C13 | 1.429 (2) | N19—C25 | 1.363 (2) |
| C12—H12 | 0.9300 | N19—C20 | 1.458 (2) |
| C13—C14 | 1.411 (2) | C20—C21 | 1.503 (3) |
| C13—C24 | 1.412 (2) | C20—H20A | 0.9600 |
| C14—C15 | 1.370 (2) | C20—H20B | 0.9600 |
| C14—H14 | 0.9300 | C21—C22 | 1.509 (3) |
| C15—C25 | 1.423 (2) | C21—H21A | 0.9600 |
| C15—C16 | 1.503 (2) | C21—H21B | 0.9600 |
| C16—C17 | 1.396 (4) | C22—C23 | 1.512 (2) |
| C16—C17' | 1.468 (5) | C22—H22A | 0.9600 |
| C16—H16A | 0.9600 | C22—H22B | 0.9600 |
| C16—H16B | 0.9601 | C23—C24 | 1.372 (2) |
| C16—H16C | 0.9600 | C23—C25 | 1.420 (2) |
| C16—H16D | 0.9600 | C24—H24 | 0.9300 |
| C17—C17' | 0.920 (6) | ||
| O10—C1—C2 | 129.84 (15) | H16C—C17—H18D | 144.7 |
| O10—C1—C8 | 123.21 (15) | H17A—C17—H18D | 73.8 |
| C2—C1—C8 | 106.95 (13) | H17B—C17—H18D | 106.2 |
| C12—C2—C1 | 133.65 (15) | H17C—C17—H18D | 100.9 |
| C12—C2—C3 | 119.24 (14) | C17—C17'—C18 | 79.2 (4) |
| C1—C2—C3 | 107.09 (14) | C17—C17'—C16 | 67.1 (4) |
| O11—C3—C9 | 125.77 (15) | C18—C17'—C16 | 117.5 (4) |
| O11—C3—C2 | 126.97 (17) | C17—C17'—H16B | 103.6 |
| C9—C3—C2 | 107.21 (13) | C18—C17'—H16B | 137.5 |
| C5—C4—C9 | 118.09 (17) | C16—C17'—H16B | 37.9 |
| C5—C4—H4 | 121.0 | C17—C17'—H17B | 54.7 |
| C9—C4—H4 | 121.0 | C18—C17'—H17B | 105.8 |
| C6—C5—C4 | 121.28 (17) | C16—C17'—H17B | 95.7 |
| C6—C5—H5 | 119.4 | H16B—C17'—H17B | 110.1 |
| C4—C5—H5 | 119.4 | C17—C17'—H17C | 70.1 |
| C5—C6—C7 | 120.78 (18) | C18—C17'—H17C | 105.8 |
| C5—C6—H6 | 119.6 | C16—C17'—H17C | 109.4 |
| C7—C6—H6 | 119.6 | H16B—C17'—H17C | 115.0 |
| C8—C7—C6 | 117.91 (17) | H17B—C17'—H17C | 16.5 |
| C8—C7—H7 | 121.0 | C17—C17'—H17D | 175.6 |
| C6—C7—H7 | 121.0 | C18—C17'—H17D | 105.0 |
| C7—C8—C9 | 121.41 (15) | C16—C17'—H17D | 109.4 |
| C7—C8—C1 | 129.00 (15) | H16B—C17'—H17D | 72.4 |
| C9—C8—C1 | 109.55 (14) | H17B—C17'—H17D | 124.3 |
| C8—C9—C4 | 120.53 (17) | H17C—C17'—H17D | 109.5 |
| C8—C9—C3 | 109.16 (14) | C17—C17'—H18A | 115.3 |
| C4—C9—C3 | 130.25 (16) | C18—C17'—H18A | 39.0 |
| C2—C12—C13 | 135.06 (15) | C16—C17'—H18A | 144.8 |
| C2—C12—H12 | 112.5 | H16B—C17'—H18A | 132.4 |
| C13—C12—H12 | 112.5 | H17B—C17'—H18A | 114.4 |
| C14—C13—C24 | 116.46 (14) | H17C—C17'—H18A | 103.7 |
| C14—C13—C12 | 125.41 (14) | H17D—C17'—H18A | 69.1 |
| C24—C13—C12 | 118.14 (14) | C17'—C18—N19 | 114.0 (2) |
| C15—C14—C13 | 122.13 (15) | C17'—C18—C17 | 36.3 (2) |
| C15—C14—H14 | 118.9 | N19—C18—C17 | 113.50 (17) |
| C13—C14—H14 | 118.9 | C17'—C18—H18A | 73.8 |
| C14—C15—C25 | 120.17 (14) | N19—C18—H18A | 109.5 |
| C14—C15—C16 | 121.40 (16) | C17—C18—H18A | 107.6 |
| C25—C15—C16 | 118.42 (15) | C17'—C18—H18B | 132.1 |
| C17—C16—C17' | 37.4 (2) | N19—C18—H18B | 109.5 |
| C17—C16—C15 | 112.6 (2) | C17—C18—H18B | 107.2 |
| C17'—C16—C15 | 116.2 (2) | H18A—C18—H18B | 109.5 |
| C17—C16—H16A | 108.1 | C17'—C18—H18C | 107.7 |
| C17'—C16—H16A | 130.8 | N19—C18—H18C | 109.5 |
| C15—C16—H16A | 109.6 | C17—C18—H18C | 132.9 |
| C17—C16—H16B | 107.9 | H18A—C18—H18C | 37.8 |
| C17'—C16—H16B | 72.0 | H18B—C18—H18C | 74.4 |
| C15—C16—H16B | 109.1 | C17'—C18—H18D | 106.6 |
| H16A—C16—H16B | 109.5 | N19—C18—H18D | 109.5 |
| C17—C16—H16C | 72.9 | C17—C18—H18D | 73.1 |
| C17'—C16—H16C | 106.0 | H18A—C18—H18D | 136.5 |
| C15—C16—H16C | 109.8 | H18B—C18—H18D | 37.8 |
| H16A—C16—H16C | 38.7 | H18C—C18—H18D | 109.5 |
| H16B—C16—H16C | 136.9 | C25—N19—C20 | 121.36 (14) |
| C17—C16—H16D | 134.2 | C25—N19—C18 | 122.09 (14) |
| C17'—C16—H16D | 106.1 | C20—N19—C18 | 115.42 (14) |
| C15—C16—H16D | 109.2 | N19—C20—C21 | 112.15 (14) |
| H16A—C16—H16D | 73.6 | N19—C20—H20A | 109.2 |
| H16B—C16—H16D | 38.7 | C21—C20—H20A | 109.2 |
| H16C—C16—H16D | 109.5 | N19—C20—H20B | 109.2 |
| C17'—C17—C16 | 75.6 (4) | C21—C20—H20B | 109.2 |
| C17'—C17—C18 | 64.5 (4) | H20A—C20—H20B | 107.9 |
| C16—C17—C18 | 114.2 (2) | C20—C21—C22 | 110.93 (14) |
| C17'—C17—H16C | 110.3 | C20—C21—H21A | 109.5 |
| C16—C17—H16C | 39.5 | C22—C21—H21A | 109.5 |
| C18—C17—H16C | 147.7 | C20—C21—H21B | 109.5 |
| C17'—C17—H17A | 172.0 | C22—C21—H21B | 109.5 |
| C16—C17—H17A | 109.5 | H21A—C21—H21B | 108.0 |
| C18—C17—H17A | 107.5 | C23—C22—C21 | 111.32 (14) |
| H16C—C17—H17A | 76.6 | C23—C22—H22A | 109.4 |
| C17'—C17—H17B | 73.7 | C21—C22—H22A | 109.4 |
| C16—C17—H17B | 109.3 | C23—C22—H22B | 109.4 |
| C18—C17—H17B | 106.9 | C21—C22—H22B | 109.4 |
| H16C—C17—H17B | 101.5 | H22A—C22—H22B | 108.0 |
| H17A—C17—H17B | 109.5 | C24—C23—C25 | 118.88 (14) |
| C17'—C17—H17C | 56.7 | C24—C23—C22 | 121.31 (14) |
| C16—C17—H17C | 107.3 | C25—C23—C22 | 119.79 (14) |
| C18—C17—H17C | 92.2 | C23—C24—C13 | 123.41 (14) |
| H16C—C17—H17C | 111.9 | C23—C24—H24 | 118.3 |
| H17A—C17—H17C | 125.4 | C13—C24—H24 | 118.3 |
| H17B—C17—H17C | 18.2 | N19—C25—C15 | 120.18 (14) |
| C17'—C17—H18D | 98.3 | N19—C25—C23 | 120.98 (14) |
| C16—C17—H18D | 140.3 | C15—C25—C23 | 118.83 (14) |
| C18—C17—H18D | 36.3 |
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RK2090).
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 datablocks global, I. DOI: 10.1107/S1600536808016346/rk2090sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808016346/rk2090Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



