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The title compound, C16H12N4O, was obtained through a two-step process. There are two mol­ecules in the asymmetric unit with essentially equal bond lengths. The phenyl and oxazole rings are essentially coplanar. Steric interactions between the two halves of the mol­ecule produce a wide angle at the central C atom.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536800018808/cf6013sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536800018808/cf6013Isup2.hkl
Contains datablock I

CCDC reference: 155878

Key indicators

  • Single-crystal X-ray study
  • T = 180 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.040
  • wR factor = 0.082
  • Data-to-parameter ratio = 8.3

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
PLAT_741 Alert C Bond Calc 1.390(2), Rep 1.39000 .... Missing s.u. C3 -C4 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(2), Rep 1.39000 .... Missing s.u. C3 -C8 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(3), Rep 1.39000 .... Missing s.u. C4 -C5 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(3), Rep 1.39000 .... Missing s.u. C5 -C6 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(3), Rep 1.39000 .... Missing s.u. C6 -C7 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(3), Rep 1.39000 .... Missing s.u. C7 -C8 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(2), Rep 1.39000 .... Missing s.u. C33 -C34 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(3), Rep 1.39000 .... Missing s.u. C33 -C38 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(3), Rep 1.39000 .... Missing s.u. C34 -C35 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(3), Rep 1.39000 .... Missing s.u. C35 -C36 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(3), Rep 1.39000 .... Missing s.u. C36 -C37 1.555 1.555 PLAT_741 Alert C Bond Calc 1.390(3), Rep 1.39000 .... Missing s.u. C37 -C38 1.555 1.555 PLAT_742 Alert C Angle Calc 119.99(16), Rep 120.00 .... Missing s.u. C4 -C3 -C8 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.00(16), Rep 120.00 .... Missing s.u. C5 -C4 -C3 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.00(15), Rep 120.00 .... Missing s.u. C4 -C5 -C6 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.00(18), Rep 120.00 .... Missing s.u. C7 -C6 -C5 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.01(17), Rep 120.00 .... Missing s.u. C8 -C7 -C6 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.01(14), Rep 120.00 .... Missing s.u. C7 -C8 -C3 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.00(17), Rep 120.00 .... Missing s.u. C34 -C33 -C38 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 119.99(17), Rep 120.00 .... Missing s.u. C35 -C34 -C33 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.00(15), Rep 120.00 .... Missing s.u. C36 -C35 -C34 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.00(19), Rep 120.00 .... Missing s.u. C35 -C36 -C37 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.00(17), Rep 120.00 .... Missing s.u. C38 -C37 -C36 1.555 1.555 1.555 PLAT_742 Alert C Angle Calc 120.00(15), Rep 120.00 .... Missing s.u. C37 -C38 -C33 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C8 -C3 -C4 -C5 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C3 -C4 -C5 -C6 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C4 -C5 -C6 -C7 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C5 -C6 -C7 -C8 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C6 -C7 -C8 -C3 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C4 -C3 -C8 -C7 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C38 -C33 -C34 -C35 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C33 -C34 -C35 -C36 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C34 -C35 -C36 -C37 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C35 -C36 -C37 -C38 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C36 -C37 -C38 -C33 1.555 1.555 1.555 1.555 PLAT_743 Alert C Torsion Calc 0.0(3), Rep 0.00 .... Missing s.u. C34 -C33 -C38 -C37 1.555 1.555 1.555 1.555 General Notes
REFLT_03 From the CIF: _diffrn_reflns_theta_max 25.90 From the CIF: _reflns_number_total 2943 Count of symmetry unique reflns 2982 Completeness (_total/calc) 98.69% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF.
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
36 Alert Level C = Please check

Comment top

The title compound, (I), was obtained through a two-step process. By reaction of 5-bromo-4-(bromomethyl)-2-phenyl-1,3-oxazole and a mixture of N-(1-cyanoethyl)benzenesulfonamide and benzotriazole in the presence of a base and small traces of DMSO, the N-alkylation took place with the more reactive benzotriazole. A halogen–lithium exchange reaction was conducted on the obtained product resulting in the formation of (I).

There are two molecules in the asymmetric unit. All corresponding bond lengths are equal within 2σ and in accordance with the chemical diagram. In both molecules, the dihedral angle between the phenyl and oxazole rings (less than 5°) indicates communicating π systems. The steric demand of the ring systems on the two sides of the molecule seems to have the effects (i) that the tetrahedral angle at the centre of the molecule formed by the non-H atoms is significantly enlarged to 112.0 (3) and 111.0 (3)° in the two molecules, respectively, and (ii) that the halves of the molecule are inclined to each other by about 43 and 33° in the two molecules.

Experimental top

Following the method of Lesbosquain & Decruix (1993), 5-bromo-4(bromomethyl)-2-phenyl-1,3-oxazole, K2CO3 and a mixture of N-(1-cyanoethyl)benzenesulfonamide and benzotriazole in the presence of traces of DMSO were refluxed in acetonitrile for 1 h. The resulting suspension was cooled, filtered and concentrated under reduced pressure, and the obtained compound was purified by column chromatography. Br–Li exchange reaction was further carried out on the purified compound at 173 K for 2 h, as already described by Swaleh & Liebscher (1999). The compound isolated by subsequent column chromatography was recrystallized from absolute ethanol, affording (I).

Refinement top

To save variable parameters, both monosubstituted benzene rings were refined as rigid ideal hexagons. This seems to be justified, because every ring is bonded to a C atom; and in such a case, according to Domenicano et al. (1975), the ideal symmetry of the C6-hexagon is maintained. 2235 Friedel pairs were measured, i.e. 75.2% of those possible, and they were merged in the data set.

Computing details top

Data collection: IPDS2.87 (Stoe & Cie, 1997); cell refinement: IPDS2.87; data reduction: IPDS2.87; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: OPTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The structure of one molecule OF (I) showing 50% probability ellipsoids.
1-[(2-phenyl-1,3-oxazol-4-yl)methyl]-1H-1,2,3-benzotriazole top
Crystal data top
C16H12N4ODx = 1.355 Mg m3
Mr = 276.30Melting point: 376(1) K
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 14.880 (2) ÅCell parameters from 4003 reflections
b = 4.6251 (5) Åθ = 3.1–24.3°
c = 20.043 (3) ŵ = 0.09 mm1
β = 100.963 (19)°T = 180 K
V = 1354.2 (3) Å3Prism, colorless
Z = 40.52 × 0.24 × 0.12 mm
F(000) = 576
Data collection top
Stoe IPDS
diffractometer
2202 reflections with I > 2σ(I)
Radiation source: fine-focus sealed X-ray tubeRint = 0.068
Planar graphite monochromatorθmax = 25.9°, θmin = 2.3°
Detector resolution: 6.667 pixels mm-1h = 1818
ϕ–rotation, ϕ–incr. = 1.2°, 183 exposures scansk = 55
9269 measured reflectionsl = 2424
2943 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H-atom parameters not refined
wR(F2) = 0.082 w = 1/[σ2(Fo2) + (0.0401P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.95(Δ/σ)max = 0.001
2943 reflectionsΔρmax = 0.17 e Å3
356 parametersΔρmin = 0.16 e Å3
1 restraintExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.009 (2)
Crystal data top
C16H12N4OV = 1354.2 (3) Å3
Mr = 276.30Z = 4
Monoclinic, P21Mo Kα radiation
a = 14.880 (2) ŵ = 0.09 mm1
b = 4.6251 (5) ÅT = 180 K
c = 20.043 (3) Å0.52 × 0.24 × 0.12 mm
β = 100.963 (19)°
Data collection top
Stoe IPDS
diffractometer
2202 reflections with I > 2σ(I)
9269 measured reflectionsRint = 0.068
2943 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0401 restraint
wR(F2) = 0.082H-atom parameters not refined
S = 0.95Δρmax = 0.17 e Å3
2943 reflectionsΔρmin = 0.16 e Å3
356 parameters
Special details top

Experimental. Recrystallized from ethanol. During data collection the crystal was in cold N2 gas of the Cryostream Cooler (Oxford Cryosystems, 1992) mounted on a ϕ-axis diffractometer supplied with an area detector.

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) top
xyzUiso*/Ueq
C20.06870 (17)0.0245 (7)0.15417 (12)0.0290 (7)
C30.05480 (11)0.1832 (4)0.20681 (8)0.0299 (7)
C40.03202 (10)0.2286 (5)0.22091 (9)0.0388 (8)
H40.08320.12950.19550.047*
C50.04392 (10)0.4190 (5)0.27219 (9)0.0428 (8)
H50.10330.45000.28180.051*
C60.03101 (13)0.5640 (5)0.30936 (8)0.0428 (8)
H60.02290.69410.34440.051*
C70.11784 (11)0.5186 (5)0.29525 (9)0.0442 (9)
H70.16900.61770.32070.053*
C80.12973 (9)0.3283 (5)0.24398 (9)0.0365 (8)
H80.18910.29730.23430.044*
C100.11906 (17)0.3114 (7)0.08632 (12)0.0289 (7)
C110.02861 (19)0.3590 (8)0.07827 (13)0.0341 (7)
H110.00560.49530.04820.041*
C120.18829 (19)0.4713 (8)0.05463 (13)0.0338 (7)
H12A0.15770.63420.02730.041*
H12B0.23600.55270.09100.041*
C150.33320 (17)0.0634 (7)0.02953 (12)0.0276 (7)
C160.41368 (18)0.0574 (8)0.04677 (13)0.0365 (8)
H160.47290.00910.02220.044*
C170.40213 (19)0.2448 (8)0.09988 (13)0.0375 (8)
H170.45470.33060.11220.045*
C180.3142 (2)0.3174 (9)0.13784 (14)0.0429 (9)
H180.30960.45040.17440.051*
C190.23539 (19)0.1991 (8)0.12267 (13)0.0409 (9)
H190.17670.24560.14840.049*
C200.24579 (17)0.0055 (7)0.06717 (12)0.0293 (7)
C320.28777 (18)0.1186 (7)0.50472 (13)0.0311 (7)
C330.22925 (12)0.0908 (4)0.53084 (8)0.0339 (7)
C340.24384 (13)0.1601 (5)0.59954 (8)0.0446 (9)
H340.29310.07410.63020.054*
C350.18629 (15)0.3553 (5)0.62338 (7)0.0502 (9)
H350.19630.40270.67030.060*
C360.11415 (14)0.4811 (5)0.57853 (10)0.0525 (10)
H360.07480.61450.59480.063*
C370.09956 (12)0.4118 (5)0.50984 (9)0.0493 (9)
H370.05020.49780.47920.059*
C380.15710 (13)0.2166 (5)0.48599 (7)0.0402 (8)
H380.14710.16920.43900.048*
C400.35437 (17)0.4084 (8)0.44633 (13)0.0301 (7)
C410.39498 (19)0.4419 (8)0.51185 (13)0.0365 (8)
H410.44380.57090.52840.044*
C420.37294 (19)0.5678 (8)0.38533 (12)0.0339 (7)
H42A0.31680.67070.36310.041*
H42B0.42140.71360.39980.041*
C450.39843 (17)0.1057 (7)0.25065 (13)0.0289 (7)
C460.37797 (18)0.0470 (8)0.18831 (13)0.0347 (8)
H460.32140.02140.15770.042*
C470.44326 (19)0.2325 (8)0.17417 (13)0.0371 (8)
H470.43170.33810.13280.045*
C480.5284 (2)0.2719 (8)0.21994 (13)0.0390 (8)
H480.57170.40500.20840.047*
C490.54947 (19)0.1230 (8)0.28005 (13)0.0359 (8)
H490.60670.14780.30990.043*
C500.48256 (18)0.0686 (7)0.29570 (12)0.0289 (7)
O10.00585 (11)0.1743 (5)0.12147 (8)0.0339 (5)
O310.35385 (12)0.2580 (5)0.55065 (8)0.0370 (5)
N90.14449 (14)0.0937 (6)0.13455 (10)0.0312 (6)
N130.23177 (14)0.2829 (6)0.01091 (10)0.0297 (6)
N140.32274 (14)0.2526 (6)0.02065 (10)0.0324 (6)
N210.18141 (15)0.1361 (6)0.04007 (11)0.0353 (7)
N390.28587 (15)0.1994 (6)0.44192 (10)0.0316 (6)
N430.40198 (14)0.3690 (6)0.33659 (10)0.0295 (6)
N440.34733 (14)0.3007 (6)0.27797 (10)0.0323 (6)
N510.48369 (14)0.2369 (6)0.35103 (10)0.0316 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C20.0254 (14)0.031 (2)0.0306 (14)0.0006 (13)0.0058 (11)0.0050 (13)
C30.0315 (14)0.032 (2)0.0276 (13)0.0026 (14)0.0091 (11)0.0060 (13)
C40.0351 (15)0.039 (2)0.0460 (16)0.0047 (15)0.0175 (13)0.0017 (16)
C50.0453 (18)0.045 (2)0.0445 (16)0.0048 (17)0.0237 (14)0.0016 (17)
C60.058 (2)0.041 (2)0.0314 (14)0.0082 (18)0.0134 (14)0.0012 (15)
C70.0414 (17)0.052 (3)0.0361 (16)0.0041 (17)0.0010 (13)0.0039 (16)
C80.0362 (16)0.041 (2)0.0338 (14)0.0053 (15)0.0099 (12)0.0031 (14)
C100.0310 (15)0.030 (2)0.0270 (13)0.0003 (14)0.0086 (11)0.0068 (13)
C110.0368 (16)0.038 (2)0.0301 (13)0.0038 (15)0.0117 (11)0.0022 (14)
C120.0383 (16)0.027 (2)0.0396 (15)0.0052 (15)0.0166 (12)0.0043 (14)
C150.0295 (14)0.0276 (19)0.0266 (13)0.0030 (13)0.0077 (11)0.0028 (13)
C160.0268 (14)0.046 (2)0.0372 (15)0.0009 (15)0.0063 (11)0.0022 (15)
C170.0365 (16)0.040 (2)0.0407 (15)0.0038 (16)0.0182 (12)0.0041 (16)
C180.0443 (18)0.051 (3)0.0368 (15)0.0085 (17)0.0171 (13)0.0099 (15)
C190.0341 (16)0.053 (3)0.0375 (15)0.0121 (16)0.0112 (12)0.0099 (16)
C200.0278 (14)0.034 (2)0.0287 (13)0.0053 (13)0.0120 (11)0.0008 (13)
C320.0321 (15)0.028 (2)0.0340 (14)0.0076 (14)0.0084 (12)0.0020 (13)
C330.0370 (16)0.032 (2)0.0370 (14)0.0093 (15)0.0179 (12)0.0029 (14)
C340.0557 (19)0.042 (3)0.0400 (16)0.0029 (18)0.0196 (14)0.0038 (16)
C350.066 (2)0.047 (3)0.0452 (17)0.009 (2)0.0301 (17)0.0077 (17)
C360.058 (2)0.039 (3)0.073 (2)0.0071 (18)0.0421 (18)0.0106 (19)
C370.0434 (18)0.044 (3)0.065 (2)0.0016 (17)0.0224 (16)0.0014 (19)
C380.0408 (16)0.038 (2)0.0456 (16)0.0040 (16)0.0184 (13)0.0029 (16)
C400.0254 (14)0.031 (2)0.0345 (15)0.0036 (13)0.0064 (11)0.0049 (13)
C410.0332 (15)0.039 (2)0.0384 (16)0.0007 (15)0.0101 (12)0.0038 (15)
C420.0373 (16)0.031 (2)0.0346 (14)0.0017 (15)0.0099 (12)0.0015 (14)
C450.0262 (14)0.033 (2)0.0297 (13)0.0001 (14)0.0111 (11)0.0062 (13)
C460.0331 (15)0.041 (2)0.0313 (14)0.0033 (15)0.0087 (12)0.0036 (14)
C470.0421 (16)0.043 (2)0.0301 (13)0.0053 (17)0.0154 (12)0.0013 (15)
C480.0434 (17)0.040 (2)0.0388 (15)0.0059 (16)0.0213 (13)0.0069 (16)
C490.0341 (15)0.042 (2)0.0330 (14)0.0048 (15)0.0098 (12)0.0063 (15)
C500.0292 (14)0.0314 (19)0.0276 (13)0.0003 (14)0.0096 (11)0.0071 (13)
O10.0243 (10)0.0412 (16)0.0376 (10)0.0033 (9)0.0099 (8)0.0029 (10)
O310.0407 (11)0.0414 (15)0.0288 (9)0.0010 (11)0.0067 (8)0.0010 (10)
N90.0256 (11)0.0378 (18)0.0312 (12)0.0016 (12)0.0079 (9)0.0030 (12)
N130.0305 (12)0.0317 (17)0.0291 (11)0.0044 (12)0.0117 (9)0.0013 (11)
N140.0279 (12)0.0392 (18)0.0309 (11)0.0016 (12)0.0074 (9)0.0018 (12)
N210.0292 (12)0.042 (2)0.0362 (12)0.0055 (12)0.0107 (10)0.0055 (12)
N390.0330 (13)0.0344 (18)0.0283 (11)0.0033 (12)0.0079 (9)0.0016 (11)
N430.0293 (12)0.0318 (17)0.0288 (11)0.0019 (11)0.0090 (9)0.0036 (11)
N440.0273 (12)0.0398 (19)0.0297 (11)0.0029 (12)0.0049 (9)0.0046 (11)
N510.0316 (12)0.0348 (17)0.0289 (11)0.0045 (12)0.0072 (9)0.0039 (12)
Geometric parameters (Å, º) top
C2—N91.303 (3)C32—C331.464 (3)
C2—O11.365 (3)C33—C341.390
C2—C31.470 (3)C33—C381.390
C3—C41.390C34—C351.390
C3—C81.390C34—H340.950
C4—C51.390C35—C361.390
C4—H40.950C35—H350.950
C5—C61.390C36—C371.390
C5—H50.950C36—H360.950
C6—C71.390C37—C381.390
C6—H60.950C37—H370.950
C7—C81.390C38—H380.950
C7—H70.950C40—C411.346 (4)
C8—H80.950C40—N391.395 (4)
C10—C111.343 (4)C40—C421.498 (4)
C10—N91.397 (4)C41—O311.372 (4)
C10—C121.504 (4)C41—H410.950
C11—O11.382 (3)C42—N431.465 (4)
C11—H110.950C42—H42A0.990
C12—N131.470 (4)C42—H42B0.990
C12—H12A0.990C45—N441.360 (4)
C12—H12B0.990C45—C501.408 (4)
C15—N141.364 (4)C45—C461.417 (4)
C15—C201.410 (4)C46—C471.366 (4)
C15—C161.422 (4)C46—H460.950
C16—C171.358 (4)C47—C481.428 (4)
C16—H160.950C47—H470.950
C17—C181.423 (4)C48—C491.371 (4)
C17—H170.950C48—H480.950
C18—C191.379 (4)C49—C501.412 (4)
C18—H180.950C49—H490.950
C19—C201.413 (4)C50—N511.352 (4)
C19—H190.950N13—N211.332 (3)
C20—N211.356 (4)N13—N141.338 (3)
C32—N391.308 (3)N43—N441.333 (3)
C32—O311.373 (3)N43—N511.342 (3)
N9—C2—O1113.7 (3)C35—C34—H34120.0
N9—C2—C3128.7 (2)C33—C34—H34120.0
O1—C2—C3117.6 (2)C36—C35—C34120.0
C4—C3—C8120.0C36—C35—H35120.0
C4—C3—C2120.50 (15)C34—C35—H35120.0
C8—C3—C2119.47 (15)C35—C36—C37120.0
C5—C4—C3120.0C35—C36—H36120.0
C5—C4—H4120.0C37—C36—H36120.0
C3—C4—H4120.0C38—C37—C36120.0
C4—C5—C6120.0C38—C37—H37120.0
C4—C5—H5120.0C36—C37—H37120.0
C6—C5—H5120.0C37—C38—C33120.0
C7—C6—C5120.0C37—C38—H38120.0
C7—C6—H6120.0C33—C38—H38120.0
C5—C6—H6120.0C41—C40—N39109.2 (3)
C8—C7—C6120.0C41—C40—C42128.4 (3)
C8—C7—H7120.0N39—C40—C42122.4 (2)
C6—C7—H7120.0C40—C41—O31108.4 (3)
C7—C8—C3120.0C40—C41—H41125.8
C7—C8—H8120.0O31—C41—H41125.8
C3—C8—H8120.0N43—C42—C40111.0 (3)
C11—C10—N9109.6 (2)N43—C42—H42A109.4
C11—C10—C12128.3 (3)C40—C42—H42A109.4
N9—C10—C12122.0 (2)N43—C42—H42B109.4
C10—C11—O1107.8 (3)C40—C42—H42B109.4
C10—C11—H11126.1H42A—C42—H42B108.0
O1—C11—H11126.1N44—C45—C50108.6 (2)
N13—C12—C10112.0 (3)N44—C45—C46130.0 (2)
N13—C12—H12A109.2C50—C45—C46121.4 (3)
C10—C12—H12A109.2C47—C46—C45117.0 (2)
N13—C12—H12B109.2C47—C46—H46121.5
C10—C12—H12B109.2C45—C46—H46121.5
H12A—C12—H12B107.9C46—C47—C48121.8 (3)
N14—C15—C20108.4 (2)C46—C47—H47119.1
N14—C15—C16130.6 (2)C48—C47—H47119.1
C20—C15—C16121.0 (3)C49—C48—C47121.8 (3)
C17—C16—C15117.0 (3)C49—C48—H48119.1
C17—C16—H16121.5C47—C48—H48119.1
C15—C16—H16121.5C48—C49—C50117.2 (3)
C16—C17—C18122.4 (3)C48—C49—H49121.4
C16—C17—H17118.8C50—C49—H49121.4
C18—C17—H17118.8N51—C50—C45109.1 (2)
C19—C18—C17121.5 (3)N51—C50—C49130.1 (2)
C19—C18—H18119.3C45—C50—C49120.8 (3)
C17—C18—H18119.3C2—O1—C11104.5 (2)
C18—C19—C20117.0 (3)C41—O31—C32104.5 (2)
C18—C19—H19121.5C2—N9—C10104.5 (2)
C20—C19—H19121.5N21—N13—N14117.7 (2)
N21—C20—C15109.1 (2)N21—N13—C12120.8 (2)
N21—C20—C19129.9 (2)N14—N13—C12121.5 (2)
C15—C20—C19121.1 (2)N13—N14—C15102.3 (2)
N39—C32—O31113.1 (3)N13—N21—C20102.5 (2)
N39—C32—C33128.9 (2)C32—N39—C40104.8 (2)
O31—C32—C33118.0 (2)N44—N43—N51117.3 (2)
C34—C33—C38120.0N44—N43—C42121.9 (2)
C34—C33—C32121.02 (16)N51—N43—C42120.8 (2)
C38—C33—C32118.97 (15)N43—N44—C45102.6 (2)
C35—C34—C33120.0N43—N51—C50102.5 (2)
N9—C2—C3—C4179.9 (2)C50—C45—C46—C470.4 (4)
O1—C2—C3—C41.7 (3)C45—C46—C47—C480.0 (5)
N9—C2—C3—C81.8 (4)C46—C47—C48—C490.8 (5)
O1—C2—C3—C8176.40 (18)C47—C48—C49—C501.1 (5)
C8—C3—C4—C50.0N44—C45—C50—N510.6 (3)
C2—C3—C4—C5178.1 (2)C46—C45—C50—N51179.5 (3)
C3—C4—C5—C60.0N44—C45—C50—C49180.0 (3)
C4—C5—C6—C70.0C46—C45—C50—C490.0 (4)
C5—C6—C7—C80.0C48—C49—C50—N51178.6 (3)
C6—C7—C8—C30.0C48—C49—C50—C450.7 (4)
C4—C3—C8—C70.0N9—C2—O1—C111.4 (3)
C2—C3—C8—C7178.1 (2)C3—C2—O1—C11177.1 (2)
N9—C10—C11—O10.4 (3)C10—C11—O1—C20.5 (3)
C12—C10—C11—O1175.3 (3)C40—C41—O31—C320.2 (3)
C11—C10—C12—N13117.7 (3)N39—C32—O31—C410.6 (3)
N9—C10—C12—N1367.2 (3)C33—C32—O31—C41178.5 (2)
N14—C15—C16—C17179.4 (3)O1—C2—N9—C101.6 (3)
C20—C15—C16—C171.3 (5)C3—C2—N9—C10176.7 (3)
C15—C16—C17—C180.8 (5)C11—C10—N9—C21.2 (3)
C16—C17—C18—C190.3 (5)C12—C10—N9—C2174.8 (3)
C17—C18—C19—C200.8 (5)C10—C12—N13—N2155.7 (3)
N14—C15—C20—N210.9 (3)C10—C12—N13—N14124.4 (3)
C16—C15—C20—N21179.6 (3)N21—N13—N14—C150.2 (3)
N14—C15—C20—C19179.8 (3)C12—N13—N14—C15179.8 (2)
C16—C15—C20—C190.7 (5)C20—C15—N14—N130.7 (3)
C18—C19—C20—N21178.3 (3)C16—C15—N14—N13179.9 (3)
C18—C19—C20—C150.3 (5)N14—N13—N21—C200.3 (3)
N39—C32—C33—C34177.1 (2)C12—N13—N21—C20179.7 (2)
O31—C32—C33—C344.0 (3)C15—C20—N21—N130.7 (3)
N39—C32—C33—C384.2 (4)C19—C20—N21—N13179.5 (3)
O31—C32—C33—C38174.7 (2)O31—C32—N39—C400.7 (3)
C38—C33—C34—C350.0C33—C32—N39—C40178.3 (3)
C32—C33—C34—C35178.7 (2)C41—C40—N39—C320.5 (3)
C33—C34—C35—C360.0C42—C40—N39—C32177.5 (3)
C34—C35—C36—C370.0C40—C42—N43—N44107.4 (3)
C35—C36—C37—C380.0C40—C42—N43—N5169.3 (3)
C36—C37—C38—C330.0N51—N43—N44—C450.6 (3)
C34—C33—C38—C370.0C42—N43—N44—C45177.4 (3)
C32—C33—C38—C37178.8 (2)C50—C45—N44—N430.0 (3)
N39—C40—C41—O310.2 (3)C46—C45—N44—N43180.0 (3)
C42—C40—C41—O31177.7 (3)N44—N43—N51—C500.9 (3)
C41—C40—C42—N43120.0 (3)C42—N43—N51—C50177.8 (2)
N39—C40—C42—N4362.4 (3)C45—C50—N51—N430.8 (3)
N44—C45—C46—C47179.7 (3)C49—C50—N51—N43179.8 (3)

Experimental details

Crystal data
Chemical formulaC16H12N4O
Mr276.30
Crystal system, space groupMonoclinic, P21
Temperature (K)180
a, b, c (Å)14.880 (2), 4.6251 (5), 20.043 (3)
β (°) 100.963 (19)
V3)1354.2 (3)
Z4
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.52 × 0.24 × 0.12
Data collection
DiffractometerStoe IPDS
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
9269, 2943, 2202
Rint0.068
(sin θ/λ)max1)0.615
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.040, 0.082, 0.95
No. of reflections2943
No. of parameters356
No. of restraints1
H-atom treatmentH-atom parameters not refined
Δρmax, Δρmin (e Å3)0.17, 0.16

Computer programs: IPDS2.87 (Stoe & Cie, 1997), IPDS2.87, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), OPTEP-3 (Farrugia, 1997), SHELXL97.

 

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