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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Nov 20;64(Pt 12):o2393. doi: 10.1107/S1600536808037811

3-Nitro-N-(8-quinol­yl)benzamide

Gang Lei a,*, Lin-Hai Jing a, Li Zhou a
PMCID: PMC2960006  PMID: 21581363

Abstract

The title compound, C16H11N3O3, crystallizes with two independent mol­ecules which are almost identical to each other in the asymmetric unit. The dihedral angle between the quinoline ring system and the nitro­benzene ring is 51.04 (9)° in one of the mol­ecules and 48.91 (9)° in the other. The crystal packing is stabilized by C—H⋯O hydrogen bonds and π–π inter­actions, with a centroid–centroid distance of 3.6010 (15) Å.

Related literature

For general background, see: Oku et al. (1998, 1999). For a related structure, see: Lei et al. (2008).graphic file with name e-64-o2393-scheme1.jpg

Experimental

Crystal data

  • C16H11N3O3

  • M r = 293.28

  • Monoclinic, Inline graphic

  • a = 7.3783 (14) Å

  • b = 23.878 (5) Å

  • c = 7.4371 (14) Å

  • β = 90.775 (3)°

  • V = 1310.2 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.11 mm−1

  • T = 93 (2) K

  • 0.40 × 0.30 × 0.23 mm

Data collection

  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: none

  • 10838 measured reflections

  • 3071 independent reflections

  • 2860 reflections with I > 2σ(I)

  • R int = 0.030

Refinement

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.075

  • S = 1.14

  • 3071 reflections

  • 397 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.19 e Å−3

  • Δρmin = −0.19 e Å−3

Data collection: RAPID-AUTO (Rigaku, 2004); cell refinement: RAPID-AUTO; data reduction: RAPID-AUTO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808037811/ci2717sup1.cif

e-64-o2393-sup1.cif (25.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808037811/ci2717Isup2.hkl

e-64-o2393-Isup2.hkl (150.7KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C2—H2⋯O2i 0.95 2.56 3.395 (3) 147
C2A—H2A⋯O2i 0.95 2.50 3.346 (3) 148
C4—H4⋯O2Ai 0.95 2.48 3.317 (3) 146
C16—H16⋯O3Aii 0.95 2.46 3.147 (3) 130
C16A—H16A⋯O1iii 0.95 2.50 3.198 (3) 130
C17—H17⋯O1Aiv 0.95 2.45 3.396 (3) 172

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic.

Acknowledgments

The authors thank the Centre for Testing and Analysis, Cheng Du Branch, Chinese Academy of Sciences, for analytical support.

supplementary crystallographic information

Comment

Quinoline derivatives are important compounds for the treatment of bone metabolic disorders (Oku et al., 1998) and as H+-ATPases inhibitors (Oku et al., 1999). Previously, we have reported the crystal structure of (2-nitrophenyl)-N-(8-quinolyl)carboxamide (Lei et al., 2008). Now, we report here the crystal structure of the title compound.

The asymmetric unit of the title compound contains two independent molecules (Fig. 1) almost identical to each other in structure. Bond lengths and angles of the two molecules agree with each other and are comparable to those observed for (2-nitrophenyl)-N-(8-quinolyl)carboxamide (Lei et al., 2008). The quinoline ring systems are planar, with a maximum deviation of 0.017 (5) Å for atom C8 and 0.008 (5) Å for atom C9A, respectively. As a result of steric effects, the amide groups are twisted away from the planes of the quinoline benzene rings and 2-nitro substituted benzene rings (Fig. 1). The C5-C10 and C12-C17 planes form dihedral angles of 18.67 (1) and 32.89 (1)°, respectively, with the O1/N2/C8/C11 plane. Similarly, the C5A—C10A and C12A—C17A planes form dihedral angles of 20.90 (1) and 28.46 (1)°, respectively, with the O1A/N2A/C8A/C11A plane. The dihedral angle between C12-C17 and O2/O3/N3/C14 planes is 1.07 (1)° and that between C12A—C17A and O2A/O3A/N3A/C14A planes is 2.28 (1)°. The dihedral angle between quinoline ring system and nitrobenzene ring is 51.04 (9)° in one of the molecules and 48.91 (9)° in the other (with suffix A).

The crystal packing is stabilized by C—H···O hydrogen bonds (Table 1) and π-π interactionS involving C5A—C10A (centroid Cg1) and C12—C17 (centroid Cg2) benzene rings, with a Cg1···Cg2 distance of 3.6010 (15) Å.

Experimental

m-Nitrobenzoic acid (2 mmol) and an excess of thionyl chloride (3 mmol) in dioxane (20 ml) were boiled under reflux for 6 h. The solution was distilled under reduced pressure and a yellow solid was obtained. 8-Aminoquinoline (2 mmol) in tetrahydrofuran (20 ml) was added to the yellow solid and boiled under reflux for 6 h. The solution was then cooled to ambient temperature and filtered to remove the tetrahydrofuran. The precipitate was dissolved in dimethyl sulfoxide and the solution was allowed to stand for one month at ambient temperature, after which time white single crystals of the title compound suitable for X-ray diffraction were obtained.

Refinement

All H atoms were placed in calculated positions, with C-H = 0.95 Å and N-H = 0.88 Å, and refined using a riding model, with Uiso(H) = 1.2Ueq(C,N). In the absence of significant anomalous scattering, Friedel pairs were merged prior to the final refinement.

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of the title compound, showing two independent molecules. Displacement ellipsoids are drawn at the 50% probability level. H atoms have been omitted for clarity.

Crystal data

C16H11N3O3 F000 = 608
Mr = 293.28 Dx = 1.487 Mg m3
Monoclinic, P21 Mo Kα radiation λ = 0.71073 Å
Hall symbol: P 2yb Cell parameters from 4482 reflections
a = 7.3783 (14) Å θ = 3.2–27.5º
b = 23.878 (5) Å µ = 0.11 mm1
c = 7.4371 (14) Å T = 93 (2) K
β = 90.775 (3)º Block, white
V = 1310.2 (4) Å3 0.40 × 0.30 × 0.23 mm
Z = 4

Data collection

Rigaku R-AXIS RAPID diffractometer 2860 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.030
Monochromator: graphite θmax = 27.5º
T = 93(2) K θmin = 3.2º
ω scans h = −9→9
Absorption correction: none k = −31→30
10838 measured reflections l = −9→9
3071 independent reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.037 H-atom parameters constrained
wR(F2) = 0.075   w = 1/[σ2(Fo2) + (0.0354P)2] where P = (Fo2 + 2Fc2)/3
S = 1.14 (Δ/σ)max = 0.001
3071 reflections Δρmax = 0.19 e Å3
397 parameters Δρmin = −0.19 e Å3
1 restraint Extinction correction: none
Primary atom site location: structure-invariant direct methods

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
O1 0.3802 (2) 0.19096 (7) 0.4467 (2) 0.0229 (4)
O2 0.1871 (3) 0.35241 (8) 0.0594 (2) 0.0334 (4)
O3 0.1573 (2) 0.43422 (7) 0.1784 (2) 0.0308 (4)
N1 0.9400 (3) 0.22508 (8) 0.7724 (3) 0.0202 (4)
N2 0.6102 (3) 0.21775 (8) 0.6364 (3) 0.0195 (4)
H2N 0.6600 0.2477 0.6850 0.023*
N3 0.2028 (3) 0.38491 (8) 0.1864 (3) 0.0220 (4)
C2 1.1064 (3) 0.23028 (11) 0.8387 (3) 0.0233 (5)
H2 1.1537 0.2670 0.8546 0.028*
C3 1.2169 (3) 0.18492 (11) 0.8868 (3) 0.0263 (5)
H3 1.3365 0.1910 0.9315 0.032*
C4 1.1508 (3) 0.13180 (11) 0.8688 (3) 0.0255 (5)
H4 1.2237 0.1006 0.9024 0.031*
C5 0.8918 (3) 0.07037 (10) 0.7766 (3) 0.0224 (5)
H5 0.9567 0.0374 0.8082 0.027*
C6 0.7193 (3) 0.06662 (10) 0.7085 (3) 0.0237 (5)
H6 0.6655 0.0307 0.6949 0.028*
C7 0.6189 (3) 0.11439 (10) 0.6579 (3) 0.0218 (5)
H7 0.4997 0.1105 0.6097 0.026*
C8 0.6946 (3) 0.16665 (9) 0.6785 (3) 0.0181 (5)
C9 0.8739 (3) 0.17209 (9) 0.7526 (3) 0.0181 (5)
C10 0.9734 (3) 0.12345 (10) 0.7999 (3) 0.0206 (5)
C11 0.4622 (3) 0.22707 (10) 0.5310 (3) 0.0184 (5)
C12 0.4060 (3) 0.28758 (9) 0.5227 (3) 0.0165 (5)
C13 0.3286 (3) 0.30764 (9) 0.3644 (3) 0.0178 (5)
H13 0.3102 0.2836 0.2640 0.021*
C14 0.2792 (3) 0.36325 (9) 0.3560 (3) 0.0169 (4)
C15 0.3002 (3) 0.39973 (10) 0.4987 (3) 0.0205 (5)
H15 0.2654 0.4379 0.4883 0.025*
C16 0.3735 (3) 0.37886 (10) 0.6575 (3) 0.0207 (5)
H16 0.3869 0.4027 0.7591 0.025*
C17 0.4276 (3) 0.32341 (10) 0.6691 (3) 0.0188 (5)
H17 0.4798 0.3097 0.7779 0.023*
O1A 0.6075 (2) 0.26160 (7) 0.0420 (2) 0.0221 (4)
O2A 0.4490 (2) 0.06211 (8) 0.1206 (3) 0.0371 (5)
O3A 0.6518 (3) 0.00459 (8) 0.2183 (3) 0.0488 (6)
N1A 0.8655 (3) 0.35147 (8) 0.5612 (2) 0.0213 (4)
N2A 0.7920 (3) 0.29510 (8) 0.2650 (3) 0.0189 (4)
H2NA 0.8755 0.2849 0.3440 0.023*
N3A 0.6014 (3) 0.05199 (8) 0.1811 (3) 0.0268 (5)
C2A 0.9074 (3) 0.37849 (11) 0.7114 (3) 0.0267 (6)
H2A 0.9586 0.3578 0.8086 0.032*
C3A 0.8798 (3) 0.43636 (12) 0.7346 (3) 0.0299 (6)
H3A 0.9132 0.4540 0.8446 0.036*
C4A 0.8049 (3) 0.46662 (11) 0.5980 (3) 0.0273 (6)
H4A 0.7831 0.5055 0.6130 0.033*
C5A 0.6826 (3) 0.46776 (10) 0.2831 (3) 0.0241 (5)
H5A 0.6603 0.5069 0.2881 0.029*
C6A 0.6403 (3) 0.43863 (10) 0.1308 (3) 0.0235 (5)
H6A 0.5880 0.4578 0.0309 0.028*
C7A 0.6729 (3) 0.38034 (10) 0.1186 (3) 0.0217 (5)
H7A 0.6420 0.3606 0.0115 0.026*
C8A 0.7486 (3) 0.35259 (9) 0.2608 (3) 0.0174 (5)
C9A 0.7935 (3) 0.38198 (10) 0.4228 (3) 0.0185 (5)
C10A 0.7595 (3) 0.44004 (10) 0.4334 (3) 0.0211 (5)
C11A 0.7202 (3) 0.25366 (10) 0.1617 (3) 0.0185 (5)
C12A 0.7870 (3) 0.19612 (10) 0.2061 (3) 0.0174 (5)
C13A 0.6706 (3) 0.15156 (10) 0.1700 (3) 0.0189 (5)
H13A 0.5544 0.1578 0.1174 0.023*
C14A 0.7274 (3) 0.09834 (10) 0.2121 (3) 0.0194 (5)
C15A 0.8969 (3) 0.08665 (10) 0.2844 (3) 0.0231 (5)
H15A 0.9326 0.0492 0.3099 0.028*
C16A 1.0131 (3) 0.13095 (10) 0.3186 (3) 0.0226 (5)
H16A 1.1307 0.1242 0.3674 0.027*
C17A 0.9574 (3) 0.18545 (10) 0.2814 (3) 0.0204 (5)
H17A 1.0366 0.2158 0.3077 0.025*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0230 (9) 0.0215 (9) 0.0242 (9) 0.0012 (7) −0.0047 (7) −0.0039 (7)
O2 0.0457 (11) 0.0319 (10) 0.0223 (9) 0.0074 (9) −0.0102 (8) −0.0034 (8)
O3 0.0382 (11) 0.0207 (9) 0.0333 (10) 0.0058 (8) −0.0072 (8) 0.0065 (8)
N1 0.0173 (10) 0.0224 (10) 0.0209 (10) −0.0028 (8) 0.0014 (8) 0.0017 (9)
N2 0.0215 (10) 0.0154 (10) 0.0214 (10) 0.0025 (8) −0.0044 (8) −0.0030 (8)
N3 0.0189 (10) 0.0249 (11) 0.0222 (10) 0.0011 (8) −0.0008 (8) 0.0029 (9)
C2 0.0187 (11) 0.0264 (14) 0.0247 (13) −0.0039 (10) 0.0010 (10) 0.0014 (11)
C3 0.0187 (12) 0.0359 (14) 0.0242 (13) −0.0010 (11) −0.0007 (10) 0.0016 (11)
C4 0.0209 (12) 0.0329 (14) 0.0228 (12) 0.0065 (11) 0.0003 (10) 0.0021 (11)
C5 0.0242 (12) 0.0197 (12) 0.0233 (12) 0.0043 (10) 0.0008 (10) 0.0020 (10)
C6 0.0298 (13) 0.0166 (12) 0.0248 (12) −0.0005 (10) 0.0026 (10) −0.0013 (10)
C7 0.0222 (12) 0.0198 (12) 0.0233 (12) −0.0008 (9) −0.0003 (10) −0.0022 (10)
C8 0.0201 (11) 0.0178 (11) 0.0165 (11) 0.0016 (9) 0.0027 (9) 0.0005 (9)
C9 0.0206 (11) 0.0185 (12) 0.0152 (11) 0.0017 (9) 0.0038 (9) 0.0004 (9)
C10 0.0212 (12) 0.0233 (12) 0.0175 (12) 0.0029 (10) 0.0023 (9) 0.0014 (10)
C11 0.0191 (11) 0.0190 (11) 0.0170 (11) −0.0009 (9) 0.0010 (9) −0.0002 (10)
C12 0.0125 (10) 0.0180 (11) 0.0188 (11) −0.0009 (9) −0.0006 (9) −0.0001 (9)
C13 0.0144 (10) 0.0196 (11) 0.0195 (11) −0.0028 (9) 0.0003 (9) −0.0022 (9)
C14 0.0135 (10) 0.0207 (11) 0.0166 (11) −0.0022 (8) −0.0011 (8) 0.0043 (9)
C15 0.0185 (11) 0.0177 (12) 0.0252 (13) 0.0001 (9) 0.0023 (10) 0.0009 (10)
C16 0.0224 (12) 0.0186 (12) 0.0212 (12) −0.0022 (9) 0.0009 (10) −0.0022 (10)
C17 0.0164 (11) 0.0219 (12) 0.0181 (12) −0.0006 (9) 0.0000 (9) 0.0002 (9)
O1A 0.0235 (8) 0.0199 (8) 0.0229 (9) 0.0015 (7) −0.0048 (7) 0.0002 (7)
O2A 0.0302 (11) 0.0256 (10) 0.0551 (12) −0.0065 (8) −0.0173 (9) 0.0057 (9)
O3A 0.0509 (14) 0.0158 (9) 0.0787 (15) −0.0034 (9) −0.0272 (12) 0.0107 (10)
N1A 0.0175 (10) 0.0261 (11) 0.0203 (10) −0.0014 (8) −0.0005 (8) 0.0019 (8)
N2A 0.0182 (10) 0.0166 (10) 0.0216 (10) 0.0010 (8) −0.0046 (8) 0.0015 (8)
N3A 0.0304 (12) 0.0208 (11) 0.0290 (12) −0.0007 (9) −0.0063 (10) 0.0023 (9)
C2A 0.0210 (12) 0.0384 (15) 0.0206 (12) −0.0023 (11) −0.0020 (10) −0.0013 (11)
C3A 0.0277 (14) 0.0364 (15) 0.0257 (13) −0.0091 (12) 0.0030 (11) −0.0106 (12)
C4A 0.0229 (13) 0.0242 (13) 0.0347 (14) −0.0054 (10) 0.0047 (11) −0.0061 (11)
C5A 0.0189 (11) 0.0170 (12) 0.0365 (14) −0.0011 (9) 0.0040 (10) 0.0045 (10)
C6A 0.0217 (12) 0.0204 (12) 0.0284 (13) 0.0013 (10) −0.0020 (10) 0.0076 (11)
C7A 0.0214 (11) 0.0214 (12) 0.0224 (12) −0.0009 (9) 0.0001 (10) 0.0022 (10)
C8A 0.0158 (10) 0.0154 (11) 0.0210 (12) −0.0009 (9) 0.0019 (9) 0.0012 (9)
C9A 0.0144 (10) 0.0198 (11) 0.0214 (11) −0.0024 (9) 0.0027 (9) 0.0017 (9)
C10A 0.0171 (11) 0.0203 (12) 0.0260 (12) −0.0032 (9) 0.0029 (9) −0.0026 (10)
C11A 0.0173 (11) 0.0199 (12) 0.0183 (12) 0.0005 (9) 0.0012 (10) −0.0001 (10)
C12A 0.0192 (11) 0.0165 (11) 0.0164 (11) 0.0001 (9) 0.0015 (9) 0.0005 (9)
C13A 0.0224 (12) 0.0203 (12) 0.0138 (11) 0.0016 (9) −0.0022 (9) 0.0010 (9)
C14A 0.0206 (11) 0.0188 (12) 0.0188 (11) −0.0016 (9) −0.0018 (9) 0.0003 (9)
C15A 0.0258 (12) 0.0196 (12) 0.0236 (13) 0.0023 (10) −0.0026 (10) −0.0004 (10)
C16A 0.0184 (12) 0.0242 (13) 0.0251 (12) 0.0030 (10) −0.0038 (10) 0.0006 (10)
C17A 0.0184 (11) 0.0218 (12) 0.0211 (11) −0.0010 (9) 0.0001 (9) −0.0006 (10)

Geometric parameters (Å, °)

O1—C11 1.222 (3) O1A—C11A 1.224 (3)
O2—N3 1.227 (2) O2A—N3A 1.230 (3)
O3—N3 1.225 (3) O3A—N3A 1.222 (3)
N1—C2 1.323 (3) N1A—C2A 1.323 (3)
N1—C9 1.363 (3) N1A—C9A 1.363 (3)
N2—C11 1.354 (3) N2A—C11A 1.356 (3)
N2—C8 1.403 (3) N2A—C8A 1.410 (3)
N2—H2N 0.88 N2A—H2NA 0.88
N3—C14 1.469 (3) N3A—C14A 1.462 (3)
C2—C3 1.399 (3) C2A—C3A 1.408 (4)
C2—H2 0.95 C2A—H2A 0.95
C3—C4 1.365 (3) C3A—C4A 1.358 (4)
C3—H3 0.95 C3A—H3A 0.95
C4—C10 1.414 (3) C4A—C10A 1.415 (3)
C4—H4 0.95 C4A—H4A 0.95
C5—C6 1.366 (3) C5A—C6A 1.362 (3)
C5—C10 1.413 (3) C5A—C10A 1.412 (3)
C5—H5 0.95 C5A—H5A 0.95
C6—C7 1.409 (3) C6A—C7A 1.416 (3)
C6—H6 0.95 C6A—H6A 0.95
C7—C8 1.375 (3) C7A—C8A 1.361 (3)
C7—H7 0.95 C7A—H7A 0.95
C8—C9 1.432 (3) C8A—C9A 1.429 (3)
C9—C10 1.416 (3) C9A—C10A 1.411 (3)
C11—C12 1.504 (3) C11A—C12A 1.495 (3)
C12—C13 1.387 (3) C12A—C13A 1.391 (3)
C12—C17 1.392 (3) C12A—C17A 1.393 (3)
C13—C14 1.378 (3) C13A—C14A 1.373 (3)
C13—H13 0.95 C13A—H13A 0.95
C14—C15 1.380 (3) C14A—C15A 1.383 (3)
C15—C16 1.385 (3) C15A—C16A 1.383 (3)
C15—H15 0.95 C15A—H15A 0.95
C16—C17 1.385 (3) C16A—C17A 1.391 (3)
C16—H16 0.95 C16A—H16A 0.95
C17—H17 0.95 C17A—H17A 0.95
C2—N1—C9 117.2 (2) C2A—N1A—C9A 117.5 (2)
C11—N2—C8 128.63 (19) C11A—N2A—C8A 127.67 (18)
C11—N2—H2N 115.7 C11A—N2A—H2NA 116.2
C8—N2—H2N 115.7 C8A—N2A—H2NA 116.2
O3—N3—O2 123.2 (2) O3A—N3A—O2A 122.6 (2)
O3—N3—C14 118.80 (19) O3A—N3A—C14A 118.3 (2)
O2—N3—C14 118.03 (19) O2A—N3A—C14A 119.05 (19)
N1—C2—C3 123.9 (2) N1A—C2A—C3A 123.3 (2)
N1—C2—H2 118.1 N1A—C2A—H2A 118.3
C3—C2—H2 118.1 C3A—C2A—H2A 118.3
C4—C3—C2 119.2 (2) C4A—C3A—C2A 119.2 (2)
C4—C3—H3 120.4 C4A—C3A—H3A 120.4
C2—C3—H3 120.4 C2A—C3A—H3A 120.4
C3—C4—C10 119.6 (2) C3A—C4A—C10A 119.8 (2)
C3—C4—H4 120.2 C3A—C4A—H4A 120.1
C10—C4—H4 120.2 C10A—C4A—H4A 120.1
C6—C5—C10 119.8 (2) C6A—C5A—C10A 120.3 (2)
C6—C5—H5 120.1 C6A—C5A—H5A 119.9
C10—C5—H5 120.1 C10A—C5A—H5A 119.9
C5—C6—C7 122.0 (2) C5A—C6A—C7A 121.2 (2)
C5—C6—H6 119.0 C5A—C6A—H6A 119.4
C7—C6—H6 119.0 C7A—C6A—H6A 119.4
C8—C7—C6 119.6 (2) C8A—C7A—C6A 119.8 (2)
C8—C7—H7 120.2 C8A—C7A—H7A 120.1
C6—C7—H7 120.2 C6A—C7A—H7A 120.1
C7—C8—N2 125.8 (2) C7A—C8A—N2A 125.6 (2)
C7—C8—C9 119.8 (2) C7A—C8A—C9A 120.2 (2)
N2—C8—C9 114.33 (19) N2A—C8A—C9A 114.17 (18)
N1—C9—C10 123.4 (2) N1A—C9A—C10A 123.4 (2)
N1—C9—C8 116.94 (19) N1A—C9A—C8A 117.2 (2)
C10—C9—C8 119.6 (2) C10A—C9A—C8A 119.3 (2)
C5—C10—C4 124.2 (2) C9A—C10A—C5A 119.1 (2)
C5—C10—C9 119.1 (2) C9A—C10A—C4A 116.7 (2)
C4—C10—C9 116.7 (2) C5A—C10A—C4A 124.3 (2)
O1—C11—N2 124.8 (2) O1A—C11A—N2A 123.7 (2)
O1—C11—C12 121.5 (2) O1A—C11A—C12A 121.4 (2)
N2—C11—C12 113.66 (19) N2A—C11A—C12A 114.84 (19)
C13—C12—C17 119.5 (2) C13A—C12A—C17A 119.3 (2)
C13—C12—C11 118.46 (19) C13A—C12A—C11A 117.4 (2)
C17—C12—C11 122.01 (19) C17A—C12A—C11A 123.4 (2)
C14—C13—C12 118.5 (2) C14A—C13A—C12A 118.6 (2)
C14—C13—H13 120.8 C14A—C13A—H13A 120.7
C12—C13—H13 120.8 C12A—C13A—H13A 120.7
C15—C14—C13 123.1 (2) C13A—C14A—C15A 123.2 (2)
C15—C14—N3 118.4 (2) C13A—C14A—N3A 118.3 (2)
C13—C14—N3 118.4 (2) C15A—C14A—N3A 118.6 (2)
C14—C15—C16 117.8 (2) C14A—C15A—C16A 118.2 (2)
C14—C15—H15 121.1 C14A—C15A—H15A 120.9
C16—C15—H15 121.1 C16A—C15A—H15A 120.9
C17—C16—C15 120.4 (2) C15A—C16A—C17A 119.9 (2)
C17—C16—H16 119.8 C15A—C16A—H16A 120.1
C15—C16—H16 119.8 C17A—C16A—H16A 120.1
C16—C17—C12 120.6 (2) C16A—C17A—C12A 120.9 (2)
C16—C17—H17 119.7 C16A—C17A—H17A 119.5
C12—C17—H17 119.7 C12A—C17A—H17A 119.5
C9—N1—C2—C3 0.7 (3) C9A—N1A—C2A—C3A 0.5 (3)
N1—C2—C3—C4 −1.3 (4) N1A—C2A—C3A—C4A 0.7 (4)
C2—C3—C4—C10 0.8 (3) C2A—C3A—C4A—C10A −1.4 (4)
C10—C5—C6—C7 0.8 (4) C10A—C5A—C6A—C7A −0.4 (4)
C5—C6—C7—C8 −0.6 (4) C5A—C6A—C7A—C8A −0.3 (4)
C6—C7—C8—N2 −179.1 (2) C6A—C7A—C8A—N2A −178.4 (2)
C6—C7—C8—C9 −0.5 (3) C6A—C7A—C8A—C9A 0.7 (3)
C11—N2—C8—C7 −17.4 (4) C11A—N2A—C8A—C7A −22.8 (4)
C11—N2—C8—C9 164.0 (2) C11A—N2A—C8A—C9A 158.1 (2)
C2—N1—C9—C10 0.4 (3) C2A—N1A—C9A—C10A −1.0 (3)
C2—N1—C9—C8 −179.2 (2) C2A—N1A—C9A—C8A 180.0 (2)
C7—C8—C9—N1 −178.9 (2) C7A—C8A—C9A—N1A 178.7 (2)
N2—C8—C9—N1 −0.2 (3) N2A—C8A—C9A—N1A −2.1 (3)
C7—C8—C9—C10 1.5 (3) C7A—C8A—C9A—C10A −0.4 (3)
N2—C8—C9—C10 −179.8 (2) N2A—C8A—C9A—C10A 178.8 (2)
C6—C5—C10—C4 −179.9 (2) N1A—C9A—C10A—C5A −179.3 (2)
C6—C5—C10—C9 0.2 (3) C8A—C9A—C10A—C5A −0.3 (3)
C3—C4—C10—C5 −179.7 (2) N1A—C9A—C10A—C4A 0.3 (3)
C3—C4—C10—C9 0.2 (3) C8A—C9A—C10A—C4A 179.3 (2)
N1—C9—C10—C5 179.1 (2) C6A—C5A—C10A—C9A 0.7 (3)
C8—C9—C10—C5 −1.4 (3) C6A—C5A—C10A—C4A −178.9 (2)
N1—C9—C10—C4 −0.8 (3) C3A—C4A—C10A—C9A 1.0 (3)
C8—C9—C10—C4 178.7 (2) C3A—C4A—C10A—C5A −179.5 (2)
C8—N2—C11—O1 −3.3 (4) C8A—N2A—C11A—O1A 2.6 (4)
C8—N2—C11—C12 177.7 (2) C8A—N2A—C11A—C12A −176.5 (2)
O1—C11—C12—C13 −31.9 (3) O1A—C11A—C12A—C13A −27.5 (3)
N2—C11—C12—C13 147.2 (2) N2A—C11A—C12A—C13A 151.7 (2)
O1—C11—C12—C17 147.3 (2) O1A—C11A—C12A—C17A 152.8 (2)
N2—C11—C12—C17 −33.6 (3) N2A—C11A—C12A—C17A −28.0 (3)
C17—C12—C13—C14 1.5 (3) C17A—C12A—C13A—C14A 0.7 (3)
C11—C12—C13—C14 −179.2 (2) C11A—C12A—C13A—C14A −179.0 (2)
C12—C13—C14—C15 −1.1 (3) C12A—C13A—C14A—C15A −1.8 (3)
C12—C13—C14—N3 178.03 (19) C12A—C13A—C14A—N3A 177.4 (2)
O3—N3—C14—C15 −1.3 (3) O3A—N3A—C14A—C13A 179.9 (2)
O2—N3—C14—C15 178.9 (2) O2A—N3A—C14A—C13A −0.8 (3)
O3—N3—C14—C13 179.5 (2) O3A—N3A—C14A—C15A −0.9 (3)
O2—N3—C14—C13 −0.2 (3) O2A—N3A—C14A—C15A 178.4 (2)
C13—C14—C15—C16 −0.4 (3) C13A—C14A—C15A—C16A 1.2 (4)
N3—C14—C15—C16 −179.57 (19) N3A—C14A—C15A—C16A −178.0 (2)
C14—C15—C16—C17 1.6 (3) C14A—C15A—C16A—C17A 0.4 (3)
C15—C16—C17—C12 −1.2 (3) C15A—C16A—C17A—C12A −1.4 (3)
C13—C12—C17—C16 −0.4 (3) C13A—C12A—C17A—C16A 0.8 (3)
C11—C12—C17—C16 −179.7 (2) C11A—C12A—C17A—C16A −179.5 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C2—H2···O2i 0.95 2.56 3.395 (3) 147
C2A—H2A···O2i 0.95 2.50 3.346 (3) 148
C4—H4···O2Ai 0.95 2.48 3.317 (3) 146
C16—H16···O3Aii 0.95 2.46 3.147 (3) 130
C16A—H16A···O1iii 0.95 2.50 3.198 (3) 130
C17—H17···O1Aiv 0.95 2.45 3.396 (3) 172

Symmetry codes: (i) x+1, y, z+1; (ii) −x+1, y+1/2, −z+1; (iii) x+1, y, z; (iv) x, y, z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CI2717).

References

  1. Lei, G., Jing, L.-H. & Zhou, L. (2008). Acta Cryst. E64, o2392. [DOI] [PMC free article] [PubMed] [Google Scholar]
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  3. Oku, T., Sato, S., Inoue, T., Urano, Y., Yoshimitsu, T. & Yoshida, N. (1998). Jpn Patent 10 291 988.
  4. Rigaku (2004). RAPID-AUTO Rigaku/MSC Inc., The Woodlands, Texas, USA.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

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/S1600536808037811/ci2717sup1.cif

e-64-o2393-sup1.cif (25.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808037811/ci2717Isup2.hkl

e-64-o2393-Isup2.hkl (150.7KB, hkl)

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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