Abstract
The title compound, C21H19ClF3N3O2, has a structure related to other coumarin derivatives that have been used as fluorescent probes of metal ions. The dihedral angle between the coumarin ring system and the chlorobenzene ring is 42.99 (9)°. Intramolecular hydrogen bonding occurs via N—H⋯O and N—H⋯Cl interactions, generating S(7) and S(5) rings, respectively. The crystal packing is stabilized by weak C—H⋯O hydrogen bonds.
Related literature
For applications of coumarins and coumarin derivatives, see: Trenor et al. (2004 ▶); Starcevic et al. (2011 ▶); Danko et al. (2011 ▶). For the synthesis of the title compound and related structures, see: Li et al. (2011 ▶).
Experimental
Crystal data
C21H19ClF3N3O2
M r = 437.84
Orthorhombic,
a = 7.940 (6) Å
b = 12.602 (9) Å
c = 20.233 (15) Å
V = 2025 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.24 mm−1
T = 296 K
0.20 × 0.20 × 0.18 mm
Data collection
Bruker APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2001 ▶) T min = 0.954, T max = 0.958
10369 measured reflections
3576 independent reflections
3162 reflections with I > 2σ(I)
R int = 0.023
Refinement
R[F 2 > 2σ(F 2)] = 0.032
wR(F 2) = 0.078
S = 1.03
3576 reflections
273 parameters
H-atom parameters constrained
Δρmax = 0.15 e Å−3
Δρmin = −0.21 e Å−3
Absolute structure: Flack (1983 ▶), 1511 Friedel pairs
Flack parameter: −0.09 (6)
Data collection: APEX2 (Bruker, 2003 ▶); cell refinement: SAINT-Plus (Bruker, 2003 ▶); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811031916/lr2022sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811031916/lr2022Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811031916/lr2022Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N3—H3A⋯Cl1 | 0.86 | 2.57 | 2.960 (2) | 109 |
| N3—H3A⋯O2 | 0.86 | 2.22 | 2.761 (3) | 121 |
| C14—H14⋯O2i | 0.93 | 2.55 | 3.316 (3) | 140 |
Symmetry code: (i)
.
Acknowledgments
Financial support by the Fundamental Research Funds for the Central Universities was acknowledged.
supplementary crystallographic information
Comment
Because the structure of benzopyrone has many advantages including high fluorescence quantum yield, large Stokes shift, excellent light stability, and less toxicity coumairns have been widely used in the fields of biology, medicine (Starcevic et al., 2011), perfumes, cosmetics (Trenor et al., 2004), and fluorescent dyes (Danko et al., 2011). We have synthesized a series of novel coumarin derivatives and found that one of them 3-(2-benzoylhydrazonotrifluoroethyl)-7- (N,N-diethylamino)coumarin can be used as fluorescent probes of Cu(II) and Ni(II) (Li et al., 2011). Herein we report the single-crystal structure of 3-(2-Chlorophenylhydrazonotrifluoroethyl)-7-(N,N- diethylamino)coumarin, which may be a good candidate for fluorescent probe of metal ions.
Experimental
The title compound was prepared as reported in the literature (Li et al., 2011). Red orange single crystals suitable for X-ray diffraction analysis were obtained by slow evaporation from a 1:1 petroleum ether and ethyl acetate mixture.
Refinement
All H atoms were placed at calculated positions and refined using a riding model approximation, with C—H = 0.93–0.97 Å and with Uiso(H)=1.2 (1.5 for methyl groups) times Ueq(C). A distance of 0.86 Å was assumed for the N3—H3A bond.
Figures
Fig. 1.
ORTEP plot of the title compound with displacement ellipsoids at the 30% probability level. H atoms are omitted for clarity.
Crystal data
| C21H19ClF3N3O2 | Dx = 1.436 Mg m−3 |
| Mr = 437.84 | Melting point = 423–425 K |
| Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
| a = 7.940 (6) Å | Cell parameters from 3770 reflections |
| b = 12.602 (9) Å | θ = 2.6–24.7° |
| c = 20.233 (15) Å | µ = 0.24 mm−1 |
| V = 2025 (3) Å3 | T = 296 K |
| Z = 4 | Block, orange |
| F(000) = 904 | 0.20 × 0.20 × 0.18 mm |
Data collection
| Bruker APEXII CCD diffractometer | 3576 independent reflections |
| Radiation source: fine-focus sealed tube | 3162 reflections with I > 2σ(I) |
| graphite | Rint = 0.023 |
| φ and ω scans | θmax = 25.1°, θmin = 1.9° |
| Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −9→9 |
| Tmin = 0.954, Tmax = 0.958 | k = −15→9 |
| 10369 measured reflections | l = −24→24 |
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)] = 0.032 | H-atom parameters constrained |
| wR(F2) = 0.078 | w = 1/[σ2(Fo2) + (0.0416P)2 + 0.1045P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.03 | (Δ/σ)max = 0.001 |
| 3576 reflections | Δρmax = 0.15 e Å−3 |
| 273 parameters | Δρmin = −0.21 e Å−3 |
| 0 restraints | Absolute structure: Flack (1983), 1511 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: −0.09 (6) |
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 | ||
| C1 | −0.0571 (3) | 0.51038 (15) | 0.15673 (9) | 0.0426 (5) | |
| C2 | −0.0012 (3) | 0.46256 (15) | 0.09683 (10) | 0.0479 (5) | |
| H2 | 0.0292 | 0.3913 | 0.0970 | 0.058* | |
| C3 | 0.0088 (3) | 0.51828 (14) | 0.03965 (10) | 0.0450 (5) | |
| H3 | 0.0447 | 0.4842 | 0.0014 | 0.054* | |
| C4 | −0.0343 (2) | 0.62689 (14) | 0.03692 (9) | 0.0382 (4) | |
| C5 | −0.0249 (2) | 0.69109 (14) | −0.01980 (10) | 0.0391 (4) | |
| H5 | 0.0082 | 0.6604 | −0.0595 | 0.047* | |
| C6 | −0.0629 (2) | 0.79729 (14) | −0.01872 (9) | 0.0358 (4) | |
| C7 | −0.1134 (3) | 0.84426 (14) | 0.04343 (9) | 0.0392 (4) | |
| C8 | −0.0900 (2) | 0.67227 (13) | 0.09569 (9) | 0.0366 (4) | |
| C9 | −0.1056 (3) | 0.61729 (14) | 0.15382 (9) | 0.0415 (5) | |
| H9 | −0.1481 | 0.6508 | 0.1912 | 0.050* | |
| C10 | −0.0636 (2) | 0.86150 (14) | −0.08005 (8) | 0.0363 (4) | |
| C11 | 0.1033 (2) | 1.12141 (14) | −0.06355 (9) | 0.0382 (4) | |
| C12 | 0.1722 (3) | 1.18859 (16) | −0.01670 (10) | 0.0471 (5) | |
| C13 | 0.2242 (3) | 1.29033 (17) | −0.03257 (12) | 0.0564 (6) | |
| H13 | 0.2701 | 1.3341 | −0.0003 | 0.068* | |
| C14 | 0.2075 (3) | 1.32630 (17) | −0.09657 (12) | 0.0613 (6) | |
| H14 | 0.2430 | 1.3942 | −0.1080 | 0.074* | |
| C15 | 0.1377 (3) | 1.26061 (16) | −0.14320 (11) | 0.0559 (6) | |
| H15 | 0.1242 | 1.2851 | −0.1862 | 0.067* | |
| C16 | 0.0874 (3) | 1.15921 (15) | −0.12760 (10) | 0.0456 (5) | |
| H16 | 0.0424 | 1.1157 | −0.1603 | 0.055* | |
| C17 | −0.1226 (3) | 0.80735 (15) | −0.14206 (10) | 0.0434 (5) | |
| C18 | 0.0107 (3) | 0.34867 (17) | 0.21991 (12) | 0.0607 (6) | |
| H18A | −0.0171 | 0.3080 | 0.1807 | 0.073* | |
| H18B | −0.0374 | 0.3124 | 0.2578 | 0.073* | |
| C19 | 0.1987 (3) | 0.3531 (2) | 0.22744 (16) | 0.0921 (9) | |
| H19A | 0.2465 | 0.3907 | 0.1907 | 0.138* | |
| H19B | 0.2431 | 0.2823 | 0.2287 | 0.138* | |
| H19C | 0.2266 | 0.3892 | 0.2678 | 0.138* | |
| C20 | −0.1199 (3) | 0.50530 (18) | 0.27618 (10) | 0.0596 (6) | |
| H20A | −0.0763 | 0.5772 | 0.2778 | 0.071* | |
| H20B | −0.0738 | 0.4667 | 0.3135 | 0.071* | |
| C21 | −0.3098 (3) | 0.50846 (19) | 0.28210 (12) | 0.0698 (7) | |
| H21A | −0.3558 | 0.5489 | 0.2462 | 0.105* | |
| H21B | −0.3405 | 0.5411 | 0.3233 | 0.105* | |
| H21C | −0.3535 | 0.4375 | 0.2807 | 0.105* | |
| Cl1 | 0.19498 (10) | 1.14505 (5) | 0.06447 (3) | 0.0753 (2) | |
| F1 | −0.24651 (16) | 0.73715 (9) | −0.13101 (6) | 0.0567 (3) | |
| F2 | 0.00093 (17) | 0.75115 (10) | −0.17132 (6) | 0.0632 (4) | |
| F3 | −0.17985 (19) | 0.87363 (10) | −0.18810 (5) | 0.0661 (4) | |
| N1 | −0.0641 (2) | 0.45457 (13) | 0.21455 (9) | 0.0514 (4) | |
| N2 | −0.0139 (2) | 0.95674 (12) | −0.09268 (8) | 0.0397 (4) | |
| N3 | 0.0552 (2) | 1.01831 (12) | −0.04584 (8) | 0.0437 (4) | |
| H3A | 0.0694 | 0.9952 | −0.0062 | 0.052* | |
| O1 | −0.12920 (18) | 0.77888 (9) | 0.09745 (6) | 0.0415 (3) | |
| O2 | −0.1471 (2) | 0.93702 (10) | 0.05297 (6) | 0.0522 (4) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0369 (11) | 0.0411 (11) | 0.0499 (11) | −0.0028 (9) | −0.0021 (9) | 0.0060 (9) |
| C2 | 0.0502 (13) | 0.0323 (10) | 0.0613 (12) | 0.0059 (10) | 0.0028 (11) | 0.0016 (9) |
| C3 | 0.0496 (12) | 0.0335 (10) | 0.0520 (11) | 0.0050 (9) | 0.0082 (10) | −0.0049 (9) |
| C4 | 0.0382 (11) | 0.0322 (9) | 0.0441 (10) | 0.0007 (8) | 0.0012 (8) | −0.0024 (8) |
| C5 | 0.0382 (11) | 0.0361 (10) | 0.0430 (10) | 0.0023 (8) | 0.0020 (9) | −0.0069 (8) |
| C6 | 0.0337 (10) | 0.0334 (9) | 0.0404 (10) | −0.0007 (8) | 0.0015 (8) | −0.0041 (8) |
| C7 | 0.0395 (11) | 0.0338 (10) | 0.0441 (10) | 0.0006 (9) | 0.0034 (9) | −0.0006 (8) |
| C8 | 0.0356 (11) | 0.0283 (9) | 0.0458 (11) | 0.0003 (8) | −0.0020 (9) | −0.0039 (8) |
| C9 | 0.0448 (12) | 0.0373 (10) | 0.0423 (11) | −0.0002 (9) | 0.0035 (9) | −0.0008 (8) |
| C10 | 0.0359 (11) | 0.0332 (10) | 0.0398 (10) | 0.0001 (8) | −0.0001 (8) | −0.0045 (8) |
| C11 | 0.0341 (11) | 0.0338 (9) | 0.0467 (10) | 0.0001 (8) | 0.0010 (9) | −0.0045 (9) |
| C12 | 0.0439 (12) | 0.0480 (12) | 0.0493 (11) | −0.0006 (9) | −0.0033 (10) | −0.0109 (9) |
| C13 | 0.0489 (14) | 0.0448 (12) | 0.0755 (15) | −0.0057 (11) | 0.0002 (12) | −0.0199 (11) |
| C14 | 0.0652 (17) | 0.0379 (11) | 0.0809 (16) | −0.0099 (11) | 0.0106 (14) | −0.0033 (12) |
| C15 | 0.0653 (15) | 0.0442 (12) | 0.0584 (12) | −0.0021 (11) | 0.0072 (12) | 0.0072 (11) |
| C16 | 0.0494 (12) | 0.0402 (11) | 0.0470 (11) | −0.0022 (9) | 0.0002 (10) | −0.0045 (9) |
| C17 | 0.0439 (12) | 0.0416 (10) | 0.0448 (11) | 0.0006 (10) | 0.0007 (10) | −0.0035 (9) |
| C18 | 0.0596 (15) | 0.0501 (13) | 0.0723 (14) | 0.0051 (12) | 0.0076 (13) | 0.0251 (12) |
| C19 | 0.0581 (18) | 0.098 (2) | 0.120 (2) | 0.0182 (16) | 0.0011 (17) | 0.0512 (19) |
| C20 | 0.0794 (18) | 0.0557 (13) | 0.0437 (12) | 0.0008 (13) | −0.0060 (11) | 0.0080 (10) |
| C21 | 0.0807 (19) | 0.0722 (16) | 0.0566 (14) | 0.0012 (15) | 0.0098 (13) | 0.0013 (12) |
| Cl1 | 0.0938 (5) | 0.0819 (4) | 0.0501 (3) | −0.0075 (4) | −0.0206 (3) | −0.0080 (3) |
| F1 | 0.0522 (7) | 0.0562 (7) | 0.0616 (7) | −0.0130 (6) | −0.0040 (6) | −0.0129 (6) |
| F2 | 0.0581 (8) | 0.0710 (8) | 0.0604 (7) | 0.0048 (7) | 0.0106 (6) | −0.0272 (6) |
| F3 | 0.0926 (11) | 0.0582 (8) | 0.0474 (7) | 0.0008 (7) | −0.0190 (7) | −0.0007 (6) |
| N1 | 0.0567 (12) | 0.0434 (9) | 0.0542 (10) | 0.0047 (9) | 0.0003 (9) | 0.0121 (8) |
| N2 | 0.0408 (10) | 0.0356 (9) | 0.0429 (8) | 0.0006 (7) | 0.0006 (7) | −0.0048 (7) |
| N3 | 0.0537 (11) | 0.0375 (8) | 0.0398 (9) | −0.0064 (8) | −0.0056 (7) | −0.0017 (7) |
| O1 | 0.0534 (9) | 0.0311 (6) | 0.0401 (7) | 0.0056 (6) | 0.0076 (6) | −0.0014 (6) |
| O2 | 0.0747 (11) | 0.0300 (7) | 0.0519 (8) | 0.0090 (7) | 0.0138 (8) | −0.0026 (6) |
Geometric parameters (Å, °)
| C1—N1 | 1.366 (3) | C13—H13 | 0.9300 |
| C1—C9 | 1.402 (3) | C14—C15 | 1.372 (3) |
| C1—C2 | 1.424 (3) | C14—H14 | 0.9300 |
| C2—C3 | 1.356 (3) | C15—C16 | 1.376 (3) |
| C2—H2 | 0.9300 | C15—H15 | 0.9300 |
| C3—C4 | 1.412 (3) | C16—H16 | 0.9300 |
| C3—H3 | 0.9300 | C17—F3 | 1.331 (2) |
| C4—C8 | 1.392 (3) | C17—F1 | 1.342 (2) |
| C4—C5 | 1.406 (3) | C17—F2 | 1.347 (2) |
| C5—C6 | 1.372 (3) | C18—N1 | 1.465 (3) |
| C5—H5 | 0.9300 | C18—C19 | 1.501 (4) |
| C6—C7 | 1.447 (3) | C18—H18A | 0.9700 |
| C6—C10 | 1.481 (3) | C18—H18B | 0.9700 |
| C7—O2 | 1.215 (2) | C19—H19A | 0.9600 |
| C7—O1 | 1.374 (2) | C19—H19B | 0.9600 |
| C8—C9 | 1.371 (3) | C19—H19C | 0.9600 |
| C8—O1 | 1.380 (2) | C20—N1 | 1.470 (3) |
| C9—H9 | 0.9300 | C20—C21 | 1.513 (4) |
| C10—N2 | 1.289 (2) | C20—H20A | 0.9700 |
| C10—C17 | 1.503 (3) | C20—H20B | 0.9700 |
| C11—C12 | 1.384 (3) | C21—H21A | 0.9600 |
| C11—C16 | 1.387 (3) | C21—H21B | 0.9600 |
| C11—N3 | 1.401 (2) | C21—H21C | 0.9600 |
| C12—C13 | 1.385 (3) | N2—N3 | 1.342 (2) |
| C12—Cl1 | 1.741 (2) | N3—H3A | 0.8600 |
| C13—C14 | 1.378 (3) | ||
| N1—C1—C9 | 121.30 (18) | C14—C15—H15 | 119.3 |
| N1—C1—C2 | 121.56 (18) | C16—C15—H15 | 119.3 |
| C9—C1—C2 | 117.14 (17) | C15—C16—C11 | 120.48 (19) |
| C3—C2—C1 | 121.68 (18) | C15—C16—H16 | 119.8 |
| C3—C2—H2 | 119.2 | C11—C16—H16 | 119.8 |
| C1—C2—H2 | 119.2 | F3—C17—F1 | 106.26 (17) |
| C2—C3—C4 | 121.42 (17) | F3—C17—F2 | 105.71 (17) |
| C2—C3—H3 | 119.3 | F1—C17—F2 | 105.10 (15) |
| C4—C3—H3 | 119.3 | F3—C17—C10 | 113.93 (16) |
| C8—C4—C5 | 118.53 (16) | F1—C17—C10 | 112.88 (16) |
| C8—C4—C3 | 116.23 (16) | F2—C17—C10 | 112.26 (17) |
| C5—C4—C3 | 125.24 (17) | N1—C18—C19 | 112.1 (2) |
| C6—C5—C4 | 122.46 (18) | N1—C18—H18A | 109.2 |
| C6—C5—H5 | 118.8 | C19—C18—H18A | 109.2 |
| C4—C5—H5 | 118.8 | N1—C18—H18B | 109.2 |
| C5—C6—C7 | 118.29 (18) | C19—C18—H18B | 109.2 |
| C5—C6—C10 | 121.36 (17) | H18A—C18—H18B | 107.9 |
| C7—C6—C10 | 120.22 (16) | C18—C19—H19A | 109.5 |
| O2—C7—O1 | 115.49 (16) | C18—C19—H19B | 109.5 |
| O2—C7—C6 | 126.37 (17) | H19A—C19—H19B | 109.5 |
| O1—C7—C6 | 118.12 (15) | C18—C19—H19C | 109.5 |
| C9—C8—O1 | 116.72 (16) | H19A—C19—H19C | 109.5 |
| C9—C8—C4 | 123.65 (17) | H19B—C19—H19C | 109.5 |
| O1—C8—C4 | 119.61 (16) | N1—C20—C21 | 112.3 (2) |
| C8—C9—C1 | 119.79 (17) | N1—C20—H20A | 109.1 |
| C8—C9—H9 | 120.1 | C21—C20—H20A | 109.1 |
| C1—C9—H9 | 120.1 | N1—C20—H20B | 109.1 |
| N2—C10—C6 | 132.33 (16) | C21—C20—H20B | 109.1 |
| N2—C10—C17 | 110.65 (16) | H20A—C20—H20B | 107.9 |
| C6—C10—C17 | 116.90 (16) | C20—C21—H21A | 109.5 |
| C12—C11—C16 | 117.78 (18) | C20—C21—H21B | 109.5 |
| C12—C11—N3 | 120.01 (18) | H21A—C21—H21B | 109.5 |
| C16—C11—N3 | 122.20 (17) | C20—C21—H21C | 109.5 |
| C11—C12—C13 | 121.7 (2) | H21A—C21—H21C | 109.5 |
| C11—C12—Cl1 | 119.64 (16) | H21B—C21—H21C | 109.5 |
| C13—C12—Cl1 | 118.65 (17) | C1—N1—C18 | 121.08 (18) |
| C14—C13—C12 | 119.6 (2) | C1—N1—C20 | 120.98 (17) |
| C14—C13—H13 | 120.2 | C18—N1—C20 | 117.11 (18) |
| C12—C13—H13 | 120.2 | C10—N2—N3 | 121.57 (16) |
| C15—C14—C13 | 119.1 (2) | N2—N3—C11 | 117.85 (16) |
| C15—C14—H14 | 120.4 | N2—N3—H3A | 121.1 |
| C13—C14—H14 | 120.4 | C11—N3—H3A | 121.1 |
| C14—C15—C16 | 121.3 (2) | C7—O1—C8 | 122.86 (14) |
| N1—C1—C2—C3 | −178.8 (2) | Cl1—C12—C13—C14 | 179.90 (18) |
| C9—C1—C2—C3 | 1.5 (3) | C12—C13—C14—C15 | 0.7 (4) |
| C1—C2—C3—C4 | 0.7 (3) | C13—C14—C15—C16 | −1.3 (4) |
| C2—C3—C4—C8 | −1.1 (3) | C14—C15—C16—C11 | 1.2 (3) |
| C2—C3—C4—C5 | 178.8 (2) | C12—C11—C16—C15 | −0.5 (3) |
| C8—C4—C5—C6 | 2.4 (3) | N3—C11—C16—C15 | −179.3 (2) |
| C3—C4—C5—C6 | −177.6 (2) | N2—C10—C17—F3 | −27.1 (2) |
| C4—C5—C6—C7 | 0.3 (3) | C6—C10—C17—F3 | 156.38 (17) |
| C4—C5—C6—C10 | −175.63 (17) | N2—C10—C17—F1 | −148.43 (17) |
| C5—C6—C7—O2 | 178.2 (2) | C6—C10—C17—F1 | 35.1 (2) |
| C10—C6—C7—O2 | −5.8 (3) | N2—C10—C17—F2 | 93.0 (2) |
| C5—C6—C7—O1 | −3.3 (3) | C6—C10—C17—F2 | −83.5 (2) |
| C10—C6—C7—O1 | 172.71 (16) | C9—C1—N1—C18 | −170.4 (2) |
| C5—C4—C8—C9 | 179.41 (19) | C2—C1—N1—C18 | 9.9 (3) |
| C3—C4—C8—C9 | −0.6 (3) | C9—C1—N1—C20 | −1.1 (3) |
| C5—C4—C8—O1 | −2.0 (3) | C2—C1—N1—C20 | 179.2 (2) |
| C3—C4—C8—O1 | 177.93 (18) | C19—C18—N1—C1 | 77.9 (3) |
| O1—C8—C9—C1 | −175.76 (18) | C19—C18—N1—C20 | −91.8 (3) |
| C4—C8—C9—C1 | 2.8 (3) | C21—C20—N1—C1 | 82.7 (3) |
| N1—C1—C9—C8 | 177.09 (18) | C21—C20—N1—C18 | −107.6 (2) |
| C2—C1—C9—C8 | −3.2 (3) | C6—C10—N2—N3 | 0.4 (3) |
| C5—C6—C10—N2 | −140.5 (2) | C17—C10—N2—N3 | −175.39 (17) |
| C7—C6—C10—N2 | 43.6 (3) | C10—N2—N3—C11 | −178.98 (17) |
| C5—C6—C10—C17 | 35.1 (3) | C12—C11—N3—N2 | 178.80 (17) |
| C7—C6—C10—C17 | −140.80 (19) | C16—C11—N3—N2 | −2.4 (3) |
| C16—C11—C12—C13 | −0.1 (3) | O2—C7—O1—C8 | −177.57 (17) |
| N3—C11—C12—C13 | 178.75 (19) | C6—C7—O1—C8 | 3.7 (3) |
| C16—C11—C12—Cl1 | −179.98 (15) | C9—C8—O1—C7 | 177.61 (18) |
| N3—C11—C12—Cl1 | −1.2 (3) | C4—C8—O1—C7 | −1.1 (3) |
| C11—C12—C13—C14 | 0.0 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N3—H3A···Cl1 | 0.86 | 2.57 | 2.960 (2) | 109. |
| N3—H3A···O2 | 0.86 | 2.22 | 2.761 (3) | 121. |
| C14—H14···O2i | 0.93 | 2.55 | 3.316 (3) | 140. |
Symmetry codes: (i) x+1/2, −y+5/2, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LR2022).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811031916/lr2022sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811031916/lr2022Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811031916/lr2022Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

