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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jan 15;67(Pt 2):o386. doi: 10.1107/S1600536810053365

1-[5-(Anthracen-9-yl)-3-(4-nitro­phen­yl)-4,5-dihydro-1H-pyrazol-1-yl]ethan-1-one

Bao-Li Dong a, Ming-Liang Wang a,*, Yong-Hua Li a
PMCID: PMC3051795  PMID: 21523061

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 ▶).graphic file with name e-67-0o386-scheme1.jpg

Experimental

Crystal data

  • C25H19N3O3

  • M r = 409.43

  • Orthorhombic, Inline graphic

  • 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

e-67-0o386-sup1.cif (19.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810053365/fb2230Isup2.hkl

e-67-0o386-Isup2.hkl (115.6KB, 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) Inline graphic.

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.

Fig. 1.

The title molecule, showing the atom-numbering scheme. The displacement ellipsoids are drawn at the 30% probability level.

Fig. 2.

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

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  3. Fahrni, C. J., Yang, L. C. & VanDerveer, D. G. (2003). J. Am. Chem. Soc. 125, 3799–3812. [DOI] [PubMed]
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  5. Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
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  7. 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

e-67-0o386-sup1.cif (19.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810053365/fb2230Isup2.hkl

e-67-0o386-Isup2.hkl (115.6KB, hkl)

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


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