Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768105006075/ws5016sup1.cif | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768105006075/ws50161Asup2.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768105006075/ws50161Bsup3.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768105006075/ws50161Csup4.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768105006075/ws50161Dsup5.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768105006075/ws50161Esup6.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768105006075/ws50161Fsup7.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768105006075/ws50162Asup8.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768105006075/ws50162ASsup9.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768105006075/ws50162Esup10.rtv |
CCDC reference: 268176
Data collection: Johannson LS18 linescanner data collection program; cell refinement: LSPAID (Visser et al., 1986); data reduction: local program; program(s) used to solve structure: MRIA (Chernyshev & Zlokazov, 1992); program(s) used to refine structure: MRIA; molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: MRIA, SHELXL93 (Sheldrick, 1997), PARST (Nardelli, 1995).
C17H13N3O2 | Dx = 1.395 Mg m−3 |
Mr = 291.30 | Melting point: 282-283 C K |
Orthorhombic, P212121 | Cu Kα1 radiation, λ = 1.54059 Å |
a = 23.97 (2) Å | µ = 0.77 mm−1 |
b = 10.609 (8) Å | T = 295 K |
c = 5.457 (3) Å | Particle morphology: needles |
V = 1387.0 (17) Å3 | pale yellow |
Z = 4 | flat_sheet, 7 × 7 mm |
F(000) = 608 |
Enraf-Nonius Guinier Johannson camera FR 552 diffractometer | Specimen mounting: pressed as a thin layer in the specimen holder of the camera |
Radiation source: Fine focus X-ray tube, Nonius 3502.223 | Data collection mode: transmission |
Quartz monochromator | Scan method: Stationary detector |
Refinement on Inet | 120 parameters |
Least-squares matrix: full with fixed elements per cycle | 95 restraints |
Rp = 0.088 | 21 constraints |
Rwp = 0.118 | H atoms treated by a mixture of independent and constrained refinement |
Rexp = 0.040 | Weighting scheme based on measured s.u.'s |
χ2 = 8.679 | (Δ/σ)max = 0.032 |
6901 data points | Background function: Chebyshev polynomial up to the 5th order |
Profile function: split-type pseudo-Voigt (Toraya, 1986) | Preferred orientation correction: Symmetrized harmonics expansion up to the 6th order (Ahtee et al., 1989, (Jarvinen, 1993) |
C17H13N3O2 | V = 1387.0 (17) Å3 |
Mr = 291.30 | Z = 4 |
Orthorhombic, P212121 | Cu Kα1 radiation, λ = 1.54059 Å |
a = 23.97 (2) Å | µ = 0.77 mm−1 |
b = 10.609 (8) Å | T = 295 K |
c = 5.457 (3) Å | flat_sheet, 7 × 7 mm |
Enraf-Nonius Guinier Johannson camera FR 552 diffractometer | Data collection mode: transmission |
Specimen mounting: pressed as a thin layer in the specimen holder of the camera | Scan method: Stationary detector |
Rp = 0.088 | 6901 data points |
Rwp = 0.118 | 120 parameters |
Rexp = 0.040 | 95 restraints |
χ2 = 8.679 | H atoms treated by a mixture of independent and constrained refinement |
Experimental. specimen was rotated in its plane |
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. |
x | y | z | Uiso*/Ueq | ||
C11 | 0.8705 (4) | 0.7791 (8) | 0.8016 (16) | 0.053 (2)* | |
C9 | 0.8031 (3) | 0.8642 (9) | 1.0901 (13) | 0.053 (2)* | |
C7 | 0.8374 (4) | 1.0002 (7) | 0.7592 (16) | 0.053 (2)* | |
C10 | 0.8358 (4) | 0.7651 (8) | 1.0135 (17) | 0.053 (2)* | |
C8 | 0.8034 (3) | 0.9817 (8) | 0.9645 (18) | 0.053 (2)* | |
C13 | 0.8713 (3) | 0.8972 (8) | 0.6837 (15) | 0.053 (2)* | |
C12 | 0.9096 (4) | 0.6984 (7) | 0.6746 (16) | 0.053 (2)* | |
C14 | 0.9300 (3) | 0.7683 (8) | 0.4714 (15) | 0.053 (2)* | |
N6 | 0.9067 (3) | 0.8895 (6) | 0.4825 (13) | 0.053 (2)* | |
N1 | 0.9227 (3) | 0.5715 (6) | 0.7259 (14) | 0.053 (2)* | |
C5 | 0.9694 (4) | 0.7336 (7) | 0.2886 (17) | 0.053 (2)* | |
N4 | 1.0126 (3) | 0.6574 (6) | 0.3393 (12) | 0.053 (2)* | |
C2 | 0.9748 (4) | 0.5142 (7) | 0.6674 (15) | 0.053 (2)* | |
C3 | 1.0197 (4) | 0.6060 (9) | 0.5915 (15) | 0.053 (2)* | |
O15 | 1.0475 (2) | 0.6164 (4) | 0.1744 (9) | 0.053 (2)* | |
O16 | 0.9802 (2) | 0.3977 (5) | 0.6573 (9) | 0.053 (2)* | |
C17 | 0.8804 (4) | 0.4883 (7) | 0.8345 (18) | 0.053 (2)* | |
C18 | 0.8927 (4) | 0.4171 (9) | 1.0478 (16) | 0.053 (2)* | |
C19 | 0.8528 (4) | 0.3386 (8) | 1.1426 (16) | 0.053 (2)* | |
C20 | 0.7974 (4) | 0.3382 (9) | 1.0478 (17) | 0.053 (2)* | |
C21 | 0.7857 (4) | 0.4095 (9) | 0.8375 (16) | 0.053 (2)* | |
C22 | 0.8266 (4) | 0.4854 (8) | 0.7333 (18) | 0.053 (2)* | |
H9 | 0.7803 | 0.8538 | 1.2264 | 0.050* | |
H7 | 0.8378 | 1.0769 | 0.6761 | 0.050* | |
H10 | 0.8353 | 0.6896 | 1.1000 | 0.050* | |
H8 | 0.7807 | 1.0466 | 1.0189 | 0.050* | |
H6 | 0.9132 | 0.9495 | 0.3803 | 0.050* | |
H5 | 0.9651 | 0.7648 | 0.1307 | 0.050* | |
H31 | 1.0556 | 0.5640 | 0.6015 | 0.050* | |
H32 | 1.0201 | 0.6756 | 0.7067 | 0.050* | |
H18 | 0.9274 | 0.4236 | 1.1224 | 0.050* | |
H19 | 0.8620 | 0.2847 | 1.2708 | 0.050* | |
H20 | 0.7695 | 0.2915 | 1.1239 | 0.050* | |
H21 | 0.7503 | 0.4059 | 0.7673 | 0.050* | |
H22 | 0.8183 | 0.5342 | 0.5965 | 0.050* |
C11—C13 | 1.411 (14) | C5—N4 | 1.343 (12) |
C11—C10 | 1.428 (14) | C5—H5 | 0.93 |
C11—C12 | 1.446 (14) | N4—O15 | 1.303 (10) |
C9—C10 | 1.376 (14) | N4—C3 | 1.492 (12) |
C9—C8 | 1.423 (14) | C2—O16 | 1.242 (12) |
C9—H9 | 0.93 | C2—C3 | 1.514 (14) |
C7—C8 | 1.403 (14) | C3—H31 | 0.97 |
C7—C13 | 1.419 (14) | C3—H32 | 0.97 |
C7—H7 | 0.93 | C17—C22 | 1.394 (14) |
C10—H10 | 0.93 | C17—C18 | 1.418 (14) |
C8—H8 | 0.93 | C18—C19 | 1.377 (14) |
C13—N6 | 1.398 (12) | C18—H18 | 0.93 |
C12—N1 | 1.411 (12) | C19—C20 | 1.423 (14) |
C12—C14 | 1.422 (14) | C19—H19 | 0.93 |
C14—N6 | 1.403 (13) | C20—C21 | 1.399 (14) |
C14—C5 | 1.419 (14) | C20—H20 | 0.93 |
N6—H6 | 0.86 | C21—C22 | 1.401 (14) |
N1—C2 | 1.426 (12) | C21—H21 | 0.93 |
N1—C17 | 1.464 (12) | C22—H22 | 0.93 |
C13—C11—C10 | 118.0 (9) | C14—C5—H5 | 119 |
C13—C11—C12 | 107.4 (8) | O15—N4—C5 | 123.9 (8) |
C10—C11—C12 | 134.6 (9) | O15—N4—C3 | 116.1 (7) |
C10—C9—C8 | 121.2 (9) | C5—N4—C3 | 119.8 (8) |
C10—C9—H9 | 119 | O16—C2—N1 | 121.8 (9) |
C8—C9—H9 | 119 | O16—C2—C3 | 123.4 (9) |
C8—C7—C13 | 116.9 (9) | N1—C2—C3 | 114.5 (8) |
C8—C7—H7 | 122 | N4—C3—C2 | 114.0 (8) |
C13—C7—H7 | 121 | N4—C3—H31 | 109 |
C9—C10—C11 | 119.9 (9) | C2—C3—H31 | 109 |
C9—C10—H10 | 120 | N4—C3—H32 | 109 |
C11—C10—H10 | 120 | C2—C3—H32 | 109 |
C7—C8—C9 | 120.9 (9) | H31—C3—H32 | 108 |
C7—C8—H8 | 120 | C22—C17—C18 | 120.2 (9) |
C9—C8—H8 | 120 | C22—C17—N1 | 119.3 (8) |
N6—C13—C11 | 108.4 (8) | C18—C17—N1 | 120.4 (8) |
N6—C13—C7 | 128.5 (9) | C19—C18—C17 | 119.1 (9) |
C11—C13—C7 | 123.0 (9) | C19—C18—H18 | 120 |
N1—C12—C14 | 125.0 (8) | C17—C18—H18 | 120 |
N1—C12—C11 | 128.0 (8) | C18—C19—C20 | 121.0 (9) |
C14—C12—C11 | 106.9 (8) | C18—C19—H19 | 119 |
N6—C14—C5 | 121.7 (9) | C20—C19—H19 | 120 |
N6—C14—C12 | 108.0 (8) | C21—C20—C19 | 119.0 (9) |
C5—C14—C12 | 130.2 (9) | C21—C20—H20 | 121 |
C13—N6—C14 | 109.2 (7) | C19—C20—H20 | 121 |
C13—N6—H6 | 125 | C20—C21—C22 | 120.0 (9) |
C14—N6—H6 | 125 | C20—C21—H21 | 120 |
C12—N1—C2 | 123.9 (8) | C22—C21—H21 | 120 |
C12—N1—C17 | 119.9 (8) | C17—C22—C21 | 120.3 (9) |
C2—N1—C17 | 116.2 (7) | C17—C22—H22 | 120 |
N4—C5—C14 | 121.5 (9) | C21—C22—H22 | 120 |
N4—C5—H5 | 119 |
Experimental details
Crystal data | |
Chemical formula | C17H13N3O2 |
Mr | 291.30 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 295 |
a, b, c (Å) | 23.97 (2), 10.609 (8), 5.457 (3) |
V (Å3) | 1387.0 (17) |
Z | 4 |
Radiation type | Cu Kα1, λ = 1.54059 Å |
µ (mm−1) | 0.77 |
Specimen shape, size (mm) | Flat_sheet, 7 × 7 |
Data collection | |
Diffractometer | Enraf-Nonius Guinier Johannson camera FR 552 diffractometer |
Specimen mounting | Pressed as a thin layer in the specimen holder of the camera |
Data collection mode | Transmission |
Scan method | Stationary detector |
2θ values (°) | 2θfixed = ? |
Refinement | |
R factors and goodness of fit | Rp = 0.088, Rwp = 0.118, Rexp = 0.040, χ2 = 8.679 |
No. of data points | 6901 |
No. of parameters | 120 |
No. of restraints | 95 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Computer programs: Johannson LS18 linescanner data collection program, LSPAID (Visser et al., 1986), local program, MRIA (Chernyshev & Zlokazov, 1992), PLATON (Spek, 2003), MRIA, SHELXL93 (Sheldrick, 1997), PARST (Nardelli, 1995).