Abstract
In the title compound, C25H19N3O3, steric repulsion between the methine H atom and one of the anthryl H atoms seems to be concomitant with the considerable distortion of the anthryl fragment from planarity. The side rings of the anthryl subtend an angle of 9.57 (8)°, which is an extreme value among the known reliably determined structures. This angle correlates with the length of the bond by which the anthryl is attached to the rest of the molecule. In the anthryl fragment, the maximum deviation of one of the C atoms from the mean plane is 0.126 (3) Å and regards the carrier C atom involved in the repulsion between the anthryl and the methine H atoms. The interplanar angle between the pyrazoline ring and the anthryl fragment is 88.36 (5)° and that between the pyrazoline and 4-nitrophenyl rings is 8.80 (15)°. Weak intermolecular C—H⋯N, C—H⋯π and π–π interactions [centroid–centroid distances of 3.7659 (17), 3.9477 (15) and 3.8972 (15) Å] are pesent in the structure.
Related literature
For the related structure 1′,2′,3′,4′-tetrahydro-1,3-diphenyl-4-p-tolylspiro[2-pyrazoline-5,2′-naphthalen]-1′-one, see: Krishna et al. (1999 ▶). For examples of the synthetic utility applied in the case of the title compound, see: Akama et al. (1996 ▶); Fahrni et al. (2003 ▶); Wei et al. (2007 ▶). For a description of the Cambridge Structural Database, see: Allen (2002 ▶).
Experimental
Crystal data
C25H19N3O3
M r = 409.43
Orthorhombic,
a = 22.888 (5) Å
b = 9.4031 (19) Å
c = 8.9688 (18) Å
V = 1930.3 (7) Å3
Z = 4
Mo Kα radiation
μ = 0.09 mm−1
T = 293 K
0.30 × 0.20 × 0.20 mm
Data collection
Rigaku SCXmini diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.962, T max = 0.982
19272 measured reflections
2352 independent reflections
2131 reflections with I > 2σ(I)
R int = 0.062
Refinement
R[F 2 > 2σ(F 2)] = 0.039
wR(F 2) = 0.097
S = 1.07
2352 reflections
288 parameters
69 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.17 e Å−3
Δρmin = −0.18 e Å−3
Data collection: CrystalClear (Rigaku, 2005 ▶); 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/PC (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL/PC.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810053365/fb2230sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810053365/fb2230Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
Cg1, Cg2 and Cg3 are the centroids of the N1,N2,C15–C17, C5–C7,C12–C14 and C7–C12 rings, respectively.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C8—H8A⋯N1 | 0.93 | 2.47 | 3.047 (3) | 120 |
| C8—H8A⋯N2 | 0.93 | 2.54 | 3.391 (3) | 152 |
| C8—H8A⋯Cg1 | 0.93 | 2.29 | 2.979 (3) | 142 |
| C15—H15A⋯Cg2i | 0.99 | 2.90 (3) | 3.731 (3) | 142 |
| C4—H4A⋯Cg3i | 0.976 | 2.95 | 3.824 (3) | 150 |
Symmetry code: (i)
.
supplementary crystallographic information
Comment
Pyrazoline derivatives are widely studied compounds. Some of them are capable of prototropic tautomerism (Akama et al., 1996). Others show elevated fluorescence. Therefore they have been widely used as fluorescence probes in some elaborated chemosensors (Fahrni et al., 2003) as well as hole-transport materials in electrophotography and electroluminescence (Wei et al., 2007). Here we report the structure of the title compound, a new derivative of pyrazoline.
In the pyrazoline ring, all the atoms are coplanar with the maximum deviation of 0.0258 (14)° for atom N1. The bond length of N2═C17 [1.2865 (31) Å] agrees with normal C═N bond (1.28 Å). The bond distance of N1—N2 [1.3796 (25) Å] conforms to the expected value (Krishna et al., 1999), too. The mean plane of pyrazoline ring makes interplanar angles of 8.80 (15)° and 88.36 (5)° with 4-nitrophenyl ring and the anthryl fragment, respectively.
The most interesting feature of the title structure is the distortion of the anthryl from planarity. The side rings of the anthryl fragment, i. e. the benzene rings C1\C2\C3\C4\C5\C14 and C7\C8\C9\C10\C11\C12, contain the angle 9.57 (8)°. In the anthryl fragment, the maximum deviation is 0.126 (3) Å from C4 atom to the mean plane of the ring. It can be related to the repulsion between the methine H15A and the anthryl H4A atoms (Fig. 1). The non-bonding distance between these two hydrogens equals to 1.95 Å. The attached atom H4A is also situated out of the plane of the ring.
Fig. 2 was obtained from the search on the Cambridge Crystallographic Structure Database (Allen, 2002; version CSD 5.31 with the last upgrade from Sept. 1 2010) carried out on the structures with R-factor < 0.05, with no disorder, no errors, with exclusion of the powder diffraction determinations and the polymeric structures or structures containing ions. This plot shows the correlation of the interplanar angle of the side anthryl rings with the C—C distance corresponding to C15—C6 (1.520 Å) in the title structure. It can be seen that the loss of planarity of the anthryl fragment is correlated to the lengthening of the bond by which is the anthryl attached to the the rest of the molecule. The present structure is situated at the extreme of the plot in Fig. 2.
There are present only weak intermolecular interactions in the structure: C—H···N, C—H···π- electron ring interactions (Tab. 1). Moreover, there are also π-electron ring -π-electron ring interactions present in the structure: Between the pyrazoline ring N1\N2\C17\C16\C15 and the benzene C1\C2\C3\C4\C5\C14 ring [symmetry code: -x,1-y,1/2+z] with the centroid-centroid distance equal to 3.7659 (17) Å; between the pyrazoline ring N1\N2\C17\C16\C15 and the benzene C5\C6\C7\C12\C13\C14 ring [symmetry code: x, y, z] with the centroid-centroid distance equal to 3.9477 (15) Å and between the pyrazoline ring N1\N2\C17\C16\C15 and the benzene C5\C6\C7\C12\C13\C14 ring [symmetry code: -x, 1-y, 1/2+z] with the centroid-centroid distance equal to 3.8972 (15) Å.
Experimental
3-(9-anthryl)-1-(4-nitrophenylprop)-2-en-1-one (3 mmol) and 0.6 g of hydrazine hydrate aqueous solution (1:1 w/w) were dissolved in 10 ml of glacial acetic acid. The mixture was stirred for 8 h at 391 K to give an orange solid. The product was then isolated and recrystallized from acetonitrile. The average size of light yellow single-crystals of the title structure equalled to 2.0 mm×1.0 mm×1.0 mm.
Refinement
All the H atoms were discernible in the difference electron density map. Nevertheless all the H atoms except the atoms H4A and H15A the coordinates of which have been freely refined were fully constrained. (The atoms H4A and H15A are involved in the repulsion that plausibly results in the deformation of the anthryl fragment - see the comment section.) The values of the used constraints were following: Caryl—Haryl = 0.93, Cmethyl—Hmethyl = 0.96, Cmethylene—Hmethylene = 0.97, Cmethine—Hmethine = 0.98 Å; UisoHaryl/methylene/methine = 1.2UeqCaryl/methylene/methine; UisoHmethyl = 1.5UeqCmethyl. As there have been present no significant atomic scatterers in the experiment, 2058 Friedel pairs were merged.
Figures
Fig. 1.
The title molecule, showing the atom-numbering scheme. The displacement ellipsoids are drawn at the 30% probability level.
Fig. 2.
The correlation between the interplanar angles of the side rings in the anthryl fragments retrieved from the Cambridge Crystallographic Database (Allen, 2002; version CSD 5.31 with the last upgrade from Sept. 1 2010) and the length of the bond by which the anthryl is attached to the rest of the molecule. (Cattached and Canthryl correspond to C15 and C6 atoms of the title molecule, respectively.) The title compound is indicated by a red large circle while the rest of the compounds by small black squares.
Crystal data
| C25H19N3O3 | F(000) = 856 |
| Mr = 409.43 | Dx = 1.409 Mg m−3 |
| Orthorhombic, Pca21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2c -2ac | Cell parameters from 3824 reflections |
| a = 22.888 (5) Å | θ = 2.6–25.0° |
| b = 9.4031 (19) Å | µ = 0.09 mm−1 |
| c = 8.9688 (18) Å | T = 293 K |
| V = 1930.3 (7) Å3 | Prism, yellow |
| Z = 4 | 0.30 × 0.20 × 0.20 mm |
Data collection
| Rigaku SCXmini diffractometer | 2352 independent reflections |
| Radiation source: fine-focus sealed tube | 2131 reflections with I > 2σ(I) |
| graphite | Rint = 0.062 |
| φ and ω scans | θmax = 27.5°, θmin = 3.3° |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | h = −29→29 |
| Tmin = 0.962, Tmax = 0.982 | k = −12→12 |
| 19272 measured reflections | l = −11→11 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.039 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.097 | w = 1/[σ2(Fo2) + (0.0488P)2 + 0.2241P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.07 | (Δ/σ)max < 0.001 |
| 2352 reflections | Δρmax = 0.17 e Å−3 |
| 288 parameters | Δρmin = −0.18 e Å−3 |
| 69 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.018 (2) |
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 | ||
| N1 | 0.09343 (7) | 0.5404 (2) | 0.2678 (2) | 0.0364 (4) | |
| C5 | −0.06548 (9) | 0.5860 (2) | 0.2243 (2) | 0.0319 (5) | |
| C6 | −0.00794 (9) | 0.6399 (2) | 0.2175 (2) | 0.0316 (4) | |
| N2 | 0.14083 (8) | 0.6030 (2) | 0.3366 (2) | 0.0360 (4) | |
| C13 | −0.09433 (10) | 0.7481 (2) | 0.0248 (3) | 0.0410 (5) | |
| H13A | −0.1228 | 0.7832 | −0.0394 | 0.049* | |
| C8 | 0.06219 (10) | 0.8147 (2) | 0.1055 (3) | 0.0390 (5) | |
| H8A | 0.0915 | 0.7868 | 0.1711 | 0.047* | |
| C17 | 0.12204 (9) | 0.6934 (2) | 0.4330 (3) | 0.0335 (5) | |
| C15 | 0.03652 (9) | 0.5881 (2) | 0.3311 (3) | 0.0337 (5) | |
| H15A | 0.0208 (10) | 0.506 (3) | 0.387 (3) | 0.040* | |
| C7 | 0.00641 (9) | 0.7476 (2) | 0.1140 (2) | 0.0326 (5) | |
| C25 | 0.22213 (9) | 0.7571 (3) | 0.5197 (3) | 0.0416 (5) | |
| H25A | 0.2374 | 0.6845 | 0.4611 | 0.050* | |
| C12 | −0.03748 (10) | 0.7977 (2) | 0.0123 (3) | 0.0355 (5) | |
| C23 | 0.23569 (10) | 0.9475 (2) | 0.6891 (3) | 0.0405 (5) | |
| C20 | 0.16176 (9) | 0.7811 (2) | 0.5216 (3) | 0.0344 (5) | |
| C1 | −0.16961 (10) | 0.6046 (3) | 0.1484 (3) | 0.0454 (6) | |
| H1A | −0.1985 | 0.6480 | 0.0915 | 0.054* | |
| O3 | 0.25365 (12) | 1.1255 (2) | 0.8605 (3) | 0.0729 (7) | |
| C14 | −0.10970 (9) | 0.6478 (2) | 0.1304 (3) | 0.0368 (5) | |
| O1 | 0.05499 (8) | 0.3576 (2) | 0.1437 (3) | 0.0563 (5) | |
| C22 | 0.17679 (11) | 0.9742 (3) | 0.6936 (3) | 0.0453 (6) | |
| H22A | 0.1620 | 1.0473 | 0.7523 | 0.054* | |
| C4 | −0.08379 (10) | 0.4732 (3) | 0.3199 (3) | 0.0400 (5) | |
| H4A | −0.0558 (12) | 0.417 (3) | 0.377 (3) | 0.048* | |
| C9 | 0.07371 (11) | 0.9182 (3) | 0.0041 (3) | 0.0467 (6) | |
| H9A | 0.1101 | 0.9621 | 0.0041 | 0.056* | |
| C21 | 0.13977 (10) | 0.8900 (3) | 0.6090 (3) | 0.0421 (6) | |
| H21A | 0.0997 | 0.9068 | 0.6110 | 0.051* | |
| C16 | 0.05649 (9) | 0.7025 (3) | 0.4436 (3) | 0.0371 (5) | |
| H16A | 0.0425 | 0.7960 | 0.4152 | 0.045* | |
| H16B | 0.0430 | 0.6808 | 0.5435 | 0.045* | |
| C3 | −0.14067 (10) | 0.4332 (3) | 0.3298 (3) | 0.0463 (6) | |
| H3A | −0.1510 | 0.3589 | 0.3929 | 0.056* | |
| C11 | −0.02261 (12) | 0.9016 (3) | −0.0966 (3) | 0.0474 (6) | |
| H11A | −0.0506 | 0.9297 | −0.1659 | 0.057* | |
| N3 | 0.27495 (10) | 1.0378 (2) | 0.7773 (3) | 0.0515 (6) | |
| C24 | 0.25901 (10) | 0.8402 (3) | 0.6037 (3) | 0.0449 (6) | |
| H24A | 0.2991 | 0.8241 | 0.6027 | 0.054* | |
| O2 | 0.32753 (9) | 1.0208 (2) | 0.7630 (3) | 0.0698 (7) | |
| C18 | 0.09882 (10) | 0.4194 (2) | 0.1846 (3) | 0.0397 (5) | |
| C2 | −0.18442 (10) | 0.5023 (3) | 0.2462 (4) | 0.0497 (6) | |
| H29A | −0.2234 | 0.4772 | 0.2587 | 0.060* | |
| C19 | 0.15940 (11) | 0.3706 (3) | 0.1485 (4) | 0.0528 (7) | |
| H19A | 0.1576 | 0.2937 | 0.0783 | 0.079* | |
| H19B | 0.1784 | 0.3389 | 0.2380 | 0.079* | |
| H19C | 0.1811 | 0.4480 | 0.1061 | 0.079* | |
| C10 | 0.03117 (11) | 0.9604 (3) | −0.1016 (3) | 0.0515 (7) | |
| H10A | 0.0402 | 1.0280 | −0.1737 | 0.062* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N1 | 0.0253 (8) | 0.0385 (10) | 0.0455 (11) | 0.0019 (7) | −0.0063 (8) | 0.0004 (9) |
| C5 | 0.0279 (10) | 0.0329 (10) | 0.0349 (12) | 0.0039 (8) | −0.0028 (9) | −0.0064 (9) |
| C6 | 0.0271 (9) | 0.0328 (10) | 0.0348 (11) | 0.0048 (8) | −0.0054 (9) | −0.0017 (9) |
| N2 | 0.0266 (9) | 0.0383 (10) | 0.0430 (10) | −0.0011 (7) | −0.0073 (8) | 0.0041 (9) |
| C13 | 0.0389 (12) | 0.0428 (12) | 0.0412 (13) | 0.0136 (10) | −0.0119 (11) | −0.0007 (11) |
| C8 | 0.0350 (11) | 0.0412 (11) | 0.0408 (13) | 0.0055 (9) | 0.0004 (10) | 0.0055 (10) |
| C17 | 0.0275 (10) | 0.0370 (11) | 0.0361 (12) | 0.0006 (8) | −0.0023 (9) | 0.0063 (10) |
| C15 | 0.0259 (10) | 0.0389 (11) | 0.0362 (11) | −0.0015 (9) | −0.0042 (9) | 0.0071 (10) |
| C7 | 0.0335 (11) | 0.0330 (10) | 0.0312 (11) | 0.0063 (8) | −0.0004 (9) | −0.0024 (9) |
| C25 | 0.0313 (11) | 0.0448 (13) | 0.0486 (14) | 0.0004 (9) | −0.0041 (11) | −0.0027 (12) |
| C12 | 0.0376 (11) | 0.0352 (10) | 0.0336 (11) | 0.0087 (9) | −0.0035 (10) | −0.0003 (10) |
| C23 | 0.0437 (13) | 0.0394 (11) | 0.0382 (13) | −0.0085 (10) | −0.0099 (11) | 0.0081 (10) |
| C20 | 0.0305 (10) | 0.0387 (11) | 0.0340 (11) | −0.0038 (8) | −0.0028 (9) | 0.0065 (10) |
| C1 | 0.0283 (11) | 0.0526 (14) | 0.0553 (15) | 0.0067 (10) | −0.0114 (11) | −0.0095 (13) |
| O3 | 0.0843 (15) | 0.0646 (12) | 0.0698 (16) | −0.0126 (13) | −0.0163 (12) | −0.0162 (13) |
| C14 | 0.0304 (10) | 0.0378 (11) | 0.0421 (12) | 0.0058 (9) | −0.0055 (10) | −0.0091 (10) |
| O1 | 0.0478 (10) | 0.0497 (10) | 0.0713 (13) | −0.0029 (8) | −0.0149 (10) | −0.0094 (10) |
| C22 | 0.0483 (14) | 0.0478 (13) | 0.0399 (13) | 0.0014 (11) | −0.0015 (11) | −0.0043 (11) |
| C4 | 0.0316 (12) | 0.0417 (13) | 0.0468 (14) | −0.0006 (9) | −0.0033 (10) | 0.0026 (11) |
| C9 | 0.0414 (13) | 0.0461 (13) | 0.0527 (15) | 0.0033 (10) | 0.0076 (12) | 0.0102 (12) |
| C21 | 0.0316 (11) | 0.0502 (13) | 0.0445 (14) | 0.0019 (10) | −0.0047 (10) | −0.0013 (11) |
| C16 | 0.0287 (10) | 0.0493 (13) | 0.0333 (12) | 0.0008 (9) | −0.0025 (9) | 0.0014 (10) |
| C3 | 0.0358 (12) | 0.0499 (14) | 0.0531 (15) | −0.0074 (10) | 0.0019 (11) | −0.0012 (12) |
| C11 | 0.0510 (14) | 0.0498 (13) | 0.0413 (13) | 0.0145 (11) | −0.0051 (12) | 0.0072 (11) |
| N3 | 0.0599 (14) | 0.0461 (12) | 0.0487 (13) | −0.0135 (10) | −0.0163 (12) | 0.0074 (11) |
| C24 | 0.0304 (11) | 0.0498 (13) | 0.0546 (16) | −0.0033 (10) | −0.0073 (11) | 0.0050 (12) |
| O2 | 0.0491 (11) | 0.0722 (13) | 0.0881 (17) | −0.0182 (10) | −0.0255 (12) | −0.0016 (13) |
| C18 | 0.0392 (12) | 0.0353 (11) | 0.0446 (13) | 0.0029 (9) | −0.0087 (10) | 0.0026 (11) |
| C2 | 0.0269 (10) | 0.0579 (15) | 0.0642 (17) | −0.0043 (10) | −0.0019 (12) | −0.0107 (14) |
| C19 | 0.0482 (14) | 0.0493 (14) | 0.0609 (17) | 0.0122 (11) | −0.0046 (13) | −0.0073 (14) |
| C10 | 0.0572 (16) | 0.0498 (14) | 0.0476 (15) | 0.0119 (12) | 0.0084 (13) | 0.0191 (12) |
Geometric parameters (Å, °)
| N1—C18 | 1.367 (3) | C20—C21 | 1.384 (3) |
| N1—N2 | 1.380 (3) | C1—C2 | 1.345 (4) |
| N1—C15 | 1.490 (3) | C1—C14 | 1.439 (3) |
| C5—C6 | 1.412 (3) | C1—H1A | 0.9300 |
| C5—C4 | 1.427 (3) | O3—N3 | 1.214 (3) |
| C5—C14 | 1.440 (3) | O1—C18 | 1.216 (3) |
| C6—C7 | 1.413 (3) | C22—C21 | 1.386 (3) |
| C6—C15 | 1.520 (3) | C22—H22A | 0.9300 |
| N2—C17 | 1.287 (3) | C4—C3 | 1.358 (3) |
| C13—C14 | 1.382 (4) | C4—H4A | 0.97 (3) |
| C13—C12 | 1.387 (3) | C9—C10 | 1.416 (4) |
| C13—H13A | 0.9300 | C9—H9A | 0.9300 |
| C8—C9 | 1.358 (3) | C21—H21A | 0.9300 |
| C8—C7 | 1.426 (3) | C16—H16A | 0.9700 |
| C8—H8A | 0.9300 | C16—H16B | 0.9700 |
| C17—C20 | 1.462 (3) | C3—C2 | 1.409 (4) |
| C17—C16 | 1.506 (3) | C3—H3A | 0.9300 |
| C15—C16 | 1.544 (3) | C11—C10 | 1.350 (4) |
| C15—H15A | 0.99 (3) | C11—H11A | 0.9300 |
| C7—C12 | 1.436 (3) | N3—O2 | 1.221 (3) |
| C25—C24 | 1.375 (3) | C24—H24A | 0.9300 |
| C25—C20 | 1.400 (3) | C18—C19 | 1.496 (3) |
| C25—H25A | 0.9300 | C2—H29A | 0.9300 |
| C12—C11 | 1.423 (4) | C19—H19A | 0.9600 |
| C23—C22 | 1.372 (3) | C19—H19B | 0.9600 |
| C23—C24 | 1.374 (4) | C19—H19C | 0.9600 |
| C23—N3 | 1.468 (3) | C10—H10A | 0.9300 |
| C18—N1—N2 | 121.89 (18) | C23—C22—C21 | 118.7 (2) |
| C18—N1—C15 | 122.51 (18) | C23—C22—H22A | 120.6 |
| N2—N1—C15 | 112.89 (18) | C21—C22—H22A | 120.6 |
| C6—C5—C4 | 124.50 (19) | C3—C4—C5 | 121.8 (2) |
| C6—C5—C14 | 119.1 (2) | C3—C4—H4A | 116.5 (16) |
| C4—C5—C14 | 116.45 (19) | C5—C4—H4A | 121.6 (16) |
| C5—C6—C7 | 120.14 (18) | C8—C9—C10 | 121.0 (2) |
| C5—C6—C15 | 118.71 (19) | C8—C9—H9A | 119.5 |
| C7—C6—C15 | 120.98 (18) | C10—C9—H9A | 119.5 |
| C17—N2—N1 | 108.61 (17) | C20—C21—C22 | 120.7 (2) |
| C14—C13—C12 | 121.6 (2) | C20—C21—H21A | 119.7 |
| C14—C13—H13A | 119.2 | C22—C21—H21A | 119.7 |
| C12—C13—H13A | 119.2 | C17—C16—C15 | 102.38 (18) |
| C9—C8—C7 | 121.8 (2) | C17—C16—H16A | 111.3 |
| C9—C8—H8A | 119.1 | C15—C16—H16A | 111.3 |
| C7—C8—H8A | 119.1 | C17—C16—H16B | 111.3 |
| N2—C17—C20 | 122.01 (19) | C15—C16—H16B | 111.3 |
| N2—C17—C16 | 114.39 (19) | H16A—C16—H16B | 109.2 |
| C20—C17—C16 | 123.6 (2) | C4—C3—C2 | 121.3 (3) |
| N1—C15—C6 | 115.24 (19) | C4—C3—H3A | 119.4 |
| N1—C15—C16 | 101.51 (16) | C2—C3—H3A | 119.4 |
| C6—C15—C16 | 114.36 (18) | C10—C11—C12 | 121.4 (2) |
| N1—C15—H15A | 106.1 (14) | C10—C11—H11A | 119.3 |
| C6—C15—H15A | 110.3 (15) | C12—C11—H11A | 119.3 |
| C16—C15—H15A | 108.6 (16) | O3—N3—O2 | 123.3 (2) |
| C6—C7—C8 | 124.09 (19) | O3—N3—C23 | 118.6 (2) |
| C6—C7—C12 | 119.35 (19) | O2—N3—C23 | 118.1 (2) |
| C8—C7—C12 | 116.5 (2) | C23—C24—C25 | 118.9 (2) |
| C24—C25—C20 | 120.5 (2) | C23—C24—H24A | 120.5 |
| C24—C25—H25A | 119.7 | C25—C24—H24A | 120.5 |
| C20—C25—H25A | 119.7 | O1—C18—N1 | 119.2 (2) |
| C13—C12—C11 | 120.7 (2) | O1—C18—C19 | 123.6 (2) |
| C13—C12—C7 | 119.6 (2) | N1—C18—C19 | 117.2 (2) |
| C11—C12—C7 | 119.6 (2) | C1—C2—C3 | 119.8 (2) |
| C22—C23—C24 | 122.2 (2) | C1—C2—H29A | 120.1 |
| C22—C23—N3 | 118.7 (2) | C3—C2—H29A | 120.1 |
| C24—C23—N3 | 119.2 (2) | C18—C19—H19A | 109.5 |
| C21—C20—C25 | 119.0 (2) | C18—C19—H19B | 109.5 |
| C21—C20—C17 | 119.93 (19) | H19A—C19—H19B | 109.5 |
| C25—C20—C17 | 121.1 (2) | C18—C19—H19C | 109.5 |
| C2—C1—C14 | 121.0 (2) | H19A—C19—H19C | 109.5 |
| C2—C1—H1A | 119.5 | H19B—C19—H19C | 109.5 |
| C14—C1—H1A | 119.5 | C11—C10—C9 | 119.4 (2) |
| C13—C14—C1 | 120.8 (2) | C11—C10—H10A | 120.3 |
| C13—C14—C5 | 119.8 (2) | C9—C10—H10A | 120.3 |
| C1—C14—C5 | 119.3 (2) |
Hydrogen-bond geometry (Å, °)
| Cg1, Cg2 and Cg3 are the centroids of the N1,N2,C15–C17, C5–C7,C12–C14 and C7–C12 rings, respectively. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| C8—H8A···N1 | 0.93 | 2.47 | 3.047 (3) | 120. |
| C8—H8A···N2 | 0.93 | 2.54 | 3.391 (3) | 152. |
| C8—H8A···Cg1 | 0.93 | 2.29 | 2.979 (3) | 142 |
| C15—H15A···Cg2i | 0.99 | 2.90 (3) | 3.731 (3) | 142 |
| C4—H4A···Cg3i | 0.976 | 2.95 | 3.824 (3) | 150 |
Symmetry codes: (i) −x, −y+1, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FB2230).
References
- Akama, Y. & Tong, A. (1996). Microchem. J. 53, 34–41.
- Allen, F. H. (2002). Acta Cryst. B58, 380–388. [DOI] [PubMed]
- Fahrni, C. J., Yang, L. C. & VanDerveer, D. G. (2003). J. Am. Chem. Soc. 125, 3799–3812. [DOI] [PubMed]
- Krishna, R., Velmurugan, D., Murugesan, R., Shanmuga Sundaram, M. & Raghunathan, R. (1999). Acta Cryst. C55, 1676–1677.
- Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Wei, X., Yang, G., Cheng, J., Lu, Z. & Xie, M. (2007). Opt. Mater. 29, 936–940.
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/S1600536810053365/fb2230sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810053365/fb2230Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


