Abstract
In the title compound, C25H26ClN, the piperidine ring has a chair conformation with all ring substituents in equatorial positions. The dihedral angle formed between the chlorobenzene ring and the flanking phenyl rings are 74.91 (18) and 47.86 (17)°. The chloro substituent is anti to the piperidine N atom. In the crystal, centrosymmetrically related molecules aggregate via π–π interactions occurring between chlorobenzene rings [centroid–centroid distance = 3.778 (2) Å] and these are linked into linear supramolecular chains along the a axis by C—H⋯π interactions occurring between the phenyl rings.
Related literature
For the biological activity of piperidine derivatives, see: Ramalingan et al. (2004 ▶); Ramachandran et al. (2011 ▶). For a related structure, see: Ramalingan et al. (2012 ▶).
Experimental
Crystal data
C25H26ClN
M r = 375.92
Triclinic,
a = 10.0878 (7) Å
b = 10.2837 (5) Å
c = 11.3583 (7) Å
α = 94.150 (5)°
β = 107.713 (6)°
γ = 111.065 (5)°
V = 1025.32 (11) Å3
Z = 2
Mo Kα radiation
μ = 0.20 mm−1
T = 100 K
0.25 × 0.15 × 0.03 mm
Data collection
Agilent SuperNova Dual diffractometer with an Atlas detector
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2012 ▶) T min = 0.495, T max = 1.000
7033 measured reflections
4678 independent reflections
2850 reflections with I > 2σ(I)
R int = 0.034
Refinement
R[F 2 > 2σ(F 2)] = 0.074
wR(F 2) = 0.185
S = 1.03
4678 reflections
244 parameters
12 restraints
H-atom parameters constrained
Δρmax = 0.72 e Å−3
Δρmin = −0.47 e Å−3
Data collection: CrysAlis PRO (Agilent, 2012 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812029200/hb6872sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812029200/hb6872Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812029200/hb6872Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
Cg1 is the centroid of the C20–C25 ring.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C17—H17⋯Cg1i | 0.95 | 2.83 | 3.692 (4) | 151 |
Symmetry code: (i)
.
Acknowledgments
The authors are grateful for facilities provided by the Chairman/Management of Kalasalingam University, and thank the Ministry of Higher Education (Malaysia) for funding structural studies through the High-Impact Research scheme (UM.C/HIR/MOHE/SC/3).
supplementary crystallographic information
Comment
Piperidine derivatives are an important class of heterocyclic compounds with potential applications in medicinal chemistry as these can be frequently recognized in the structures of various synthetic targets as well as naturally occurring alkaloids (Ramalingan et al., 2004; Ramachandran et al., 2011). The title compound, (I), was designed and synthesized to evaluate its biological properties. The crystal structure determination was undertaken in order to establish conformational details.
In (I), Fig. 1, the piperidine ring has a chair conformation and all ring-substituents occupy equatorial positions. The dihedral angle formed between the C1–C6 benzene ring and the flanking C14–C19 and C20–C25 phenyl rings are 74.91 (18) and 47.86 (17)°, respectively; the dihedral angle between the phenyl rings is 58.93 (18)°. In a comparable molecule, having an extra C-bound methyl group (Ramalingan et al., 2012), these substituents were found to occupy the same positions. The chloro substituent is anti to the piperidine-N atom.
In the crystal packing, centrosymmetrically related molecules aggregate viaπ—π interactions occurring between chlorobenzene rings [inter-centroid distance = 3.778 (2) Å for symmetry operation 2 - x, 1 - y, 1 - z]. These are linked into linear supramolecular chains along the a axis by C—H···π interactions whereby a phenyl-H17 atom associates with the C20—C25 ring, Fig. 2 and Table 1. Chains aggregate into layers in the ab plane without specific intermolecular interactions between them, Fig. 3.
Experimental
A starting material, 3-methyl-2,6-diphenylpiperidine, was synthesized from benzaldehyde, 2-butanone and ammonium acetate through a Mannich-type reaction (for a typical synthesis, see Ramalingan et al. (2004)) followed by standard Wolff-Kishner reduction using hydrazine hydrate in diethylene glycol. 1-(2-Chlorobenzyl)-3-methyl-2,6-diphenylpiperidine was then synthesized as follows. To a DMF solution (15 ml) of 3-methyl-2,6-diphenylpiperidine (1.26 g, 0.005 mol) was added potassium tert-butoxide (0.67 g, 0.006 mol). The mixture was stirred for 30 minutes and 2-chlorobenzyl bromide (0.78 ml, 0.006 mol) was added drop-wise. Stirring was continued overnight before aqueous work-up. Extraction with diethyl ether followed by column chromatography separation using n-hexane/ethyl acetate (100:4) as an eluent eventually provided the pure title compound as a white solid. Re-crystallization was performed by slow evaporation of its ethanolic solution which afforded colourless plates. M.pt: 352–353 K. Yield: 83%.
Refinement
Carbon-bound H-atoms were placed in calculated positions [C—H = 0.95–1.00 Å, Uiso(H) = 1.2–1.5Ueq(C)] and were included in the refinement in the riding model approximation. The anisotropic displacement parameters for the C3 and C4 atoms were constrained to be nearly isotropic.
Figures
Fig. 1.
The molecular structure of (I) showing displacement ellipsoids at the 50% probability level.
Fig. 2.
A view of the supramolecular chain in (I) sustained by C—H···π and π—π interactions which are shown as orange and purple dashed lines, respectively
Fig. 3.
A view in projection down the a axis of the unit-cell contents for (I). The C—H···π and π—π interactions are shown as orange and purple dashed lines, respectively.
Crystal data
| C25H26ClN | Z = 2 |
| Mr = 375.92 | F(000) = 400 |
| Triclinic, P1 | Dx = 1.218 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 10.0878 (7) Å | Cell parameters from 1908 reflections |
| b = 10.2837 (5) Å | θ = 2.4–27.5° |
| c = 11.3583 (7) Å | µ = 0.20 mm−1 |
| α = 94.150 (5)° | T = 100 K |
| β = 107.713 (6)° | Plate, colourless |
| γ = 111.065 (5)° | 0.25 × 0.15 × 0.03 mm |
| V = 1025.32 (11) Å3 |
Data collection
| Agilent SuperNova Dual diffractometer with an Atlas detector | 4678 independent reflections |
| Radiation source: SuperNova (Mo) X-ray Source | 2850 reflections with I > 2σ(I) |
| Mirror monochromator | Rint = 0.034 |
| Detector resolution: 10.4041 pixels mm-1 | θmax = 27.6°, θmin = 2.4° |
| ω scan | h = −13→9 |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2012) | k = −13→13 |
| Tmin = 0.495, Tmax = 1.000 | l = −13→14 |
| 7033 measured reflections |
Refinement
| Refinement on F2 | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.074 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.185 | H-atom parameters constrained |
| S = 1.03 | w = 1/[σ2(Fo2) + (0.0541P)2 + 1.0947P] where P = (Fo2 + 2Fc2)/3 |
| 4678 reflections | (Δ/σ)max < 0.001 |
| 244 parameters | Δρmax = 0.72 e Å−3 |
| 12 restraints | Δρmin = −0.47 e Å−3 |
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 | ||
| Cl1 | 0.71459 (12) | 0.30264 (9) | 0.23928 (9) | 0.0512 (3) | |
| C1 | 0.8802 (4) | 0.4580 (4) | 0.3038 (3) | 0.0395 (8) | |
| C2 | 1.0149 (5) | 0.4438 (5) | 0.3581 (3) | 0.0522 (10) | |
| H2 | 1.0170 | 0.3523 | 0.3591 | 0.063* | |
| C3 | 1.1464 (5) | 0.5651 (6) | 0.4110 (4) | 0.0622 (12) | |
| H3 | 1.2396 | 0.5560 | 0.4494 | 0.075* | |
| C4 | 1.1470 (4) | 0.7006 (5) | 0.4099 (3) | 0.0482 (10) | |
| H4 | 1.2386 | 0.7836 | 0.4462 | 0.058* | |
| C5 | 1.0061 (4) | 0.7099 (4) | 0.3528 (3) | 0.0395 (8) | |
| H5 | 1.0039 | 0.8013 | 0.3505 | 0.047* | |
| C6 | 0.8716 (3) | 0.5909 (3) | 0.3004 (3) | 0.0284 (7) | |
| N1 | 0.7224 (3) | 0.7408 (2) | 0.2310 (2) | 0.0260 (6) | |
| C7 | 0.7188 (3) | 0.5974 (3) | 0.2470 (3) | 0.0287 (7) | |
| H7A | 0.6623 | 0.5315 | 0.1637 | 0.034* | |
| H7B | 0.6614 | 0.5625 | 0.3032 | 0.034* | |
| C8 | 0.6816 (4) | 0.7457 (3) | 0.0938 (3) | 0.0308 (7) | |
| H8 | 0.5797 | 0.6671 | 0.0471 | 0.037* | |
| C9 | 0.6704 (4) | 0.8861 (3) | 0.0710 (3) | 0.0390 (8) | |
| H9A | 0.6383 | 0.8849 | −0.0207 | 0.047* | |
| H9B | 0.7715 | 0.9652 | 0.1128 | 0.047* | |
| C10 | 0.5567 (4) | 0.9107 (4) | 0.1226 (3) | 0.0386 (8) | |
| H10A | 0.5526 | 1.0033 | 0.1086 | 0.046* | |
| H10B | 0.4542 | 0.8349 | 0.0773 | 0.046* | |
| C11 | 0.6033 (4) | 0.9101 (3) | 0.2629 (3) | 0.0367 (8) | |
| H11 | 0.7050 | 0.9898 | 0.3071 | 0.044* | |
| C12 | 0.6174 (4) | 0.7696 (3) | 0.2865 (3) | 0.0289 (7) | |
| H12 | 0.5145 | 0.6903 | 0.2462 | 0.035* | |
| C13 | 0.4882 (5) | 0.9353 (4) | 0.3160 (3) | 0.0508 (10) | |
| H13A | 0.4819 | 1.0256 | 0.2998 | 0.076* | |
| H13B | 0.5220 | 0.9390 | 0.4072 | 0.076* | |
| H13C | 0.3880 | 0.8573 | 0.2747 | 0.076* | |
| C14 | 0.6717 (3) | 0.7731 (3) | 0.4273 (3) | 0.0257 (6) | |
| C15 | 0.8186 (4) | 0.8583 (3) | 0.5027 (3) | 0.0373 (8) | |
| H15 | 0.8873 | 0.9119 | 0.4653 | 0.045* | |
| C16 | 0.8687 (4) | 0.8678 (4) | 0.6320 (3) | 0.0425 (9) | |
| H16 | 0.9714 | 0.9261 | 0.6822 | 0.051* | |
| C17 | 0.7699 (4) | 0.7930 (4) | 0.6883 (3) | 0.0430 (9) | |
| H17 | 0.8030 | 0.8017 | 0.7773 | 0.052* | |
| C18 | 0.6248 (5) | 0.7071 (4) | 0.6151 (3) | 0.0537 (11) | |
| H18 | 0.5566 | 0.6544 | 0.6532 | 0.064* | |
| C19 | 0.5744 (4) | 0.6950 (4) | 0.4837 (3) | 0.0443 (9) | |
| H19 | 0.4730 | 0.6330 | 0.4333 | 0.053* | |
| C20 | 0.7954 (4) | 0.7211 (3) | 0.0442 (3) | 0.0299 (7) | |
| C21 | 0.7525 (4) | 0.5955 (3) | −0.0406 (3) | 0.0367 (8) | |
| H21 | 0.6511 | 0.5262 | −0.0672 | 0.044* | |
| C22 | 0.8556 (5) | 0.5702 (4) | −0.0870 (3) | 0.0459 (9) | |
| H22 | 0.8247 | 0.4838 | −0.1441 | 0.055* | |
| C23 | 1.0022 (5) | 0.6704 (4) | −0.0500 (3) | 0.0488 (10) | |
| H23 | 1.0730 | 0.6536 | −0.0814 | 0.059* | |
| C24 | 1.0459 (4) | 0.7955 (4) | 0.0331 (3) | 0.0488 (10) | |
| H24 | 1.1470 | 0.8651 | 0.0587 | 0.059* | |
| C25 | 0.9436 (4) | 0.8202 (4) | 0.0791 (3) | 0.0412 (9) | |
| H25 | 0.9754 | 0.9071 | 0.1360 | 0.049* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl1 | 0.0784 (7) | 0.0327 (4) | 0.0474 (5) | 0.0239 (5) | 0.0270 (5) | 0.0073 (4) |
| C1 | 0.053 (2) | 0.053 (2) | 0.0308 (16) | 0.0303 (18) | 0.0270 (16) | 0.0130 (15) |
| C2 | 0.069 (3) | 0.083 (3) | 0.039 (2) | 0.054 (3) | 0.035 (2) | 0.023 (2) |
| C3 | 0.047 (2) | 0.119 (4) | 0.042 (2) | 0.047 (3) | 0.0269 (19) | 0.024 (2) |
| C4 | 0.0341 (19) | 0.082 (3) | 0.0307 (18) | 0.0177 (19) | 0.0204 (15) | 0.0145 (18) |
| C5 | 0.0325 (18) | 0.052 (2) | 0.0270 (16) | 0.0060 (16) | 0.0147 (15) | 0.0051 (15) |
| C6 | 0.0312 (16) | 0.0384 (17) | 0.0195 (14) | 0.0126 (14) | 0.0158 (13) | 0.0069 (12) |
| N1 | 0.0342 (14) | 0.0246 (12) | 0.0213 (12) | 0.0102 (11) | 0.0147 (11) | 0.0053 (10) |
| C7 | 0.0316 (17) | 0.0235 (14) | 0.0290 (15) | 0.0065 (13) | 0.0140 (13) | 0.0037 (12) |
| C8 | 0.0398 (18) | 0.0295 (15) | 0.0222 (14) | 0.0105 (14) | 0.0145 (14) | 0.0025 (12) |
| C9 | 0.062 (2) | 0.0353 (17) | 0.0218 (15) | 0.0190 (17) | 0.0173 (16) | 0.0092 (13) |
| C10 | 0.060 (2) | 0.0386 (18) | 0.0266 (16) | 0.0283 (17) | 0.0165 (16) | 0.0123 (14) |
| C11 | 0.055 (2) | 0.0365 (17) | 0.0253 (15) | 0.0243 (16) | 0.0160 (15) | 0.0082 (13) |
| C12 | 0.0338 (17) | 0.0297 (15) | 0.0243 (15) | 0.0112 (13) | 0.0136 (13) | 0.0049 (12) |
| C13 | 0.070 (3) | 0.058 (2) | 0.042 (2) | 0.038 (2) | 0.026 (2) | 0.0164 (18) |
| C14 | 0.0306 (16) | 0.0254 (14) | 0.0227 (14) | 0.0107 (13) | 0.0124 (13) | 0.0040 (12) |
| C15 | 0.0389 (19) | 0.0342 (17) | 0.0284 (16) | 0.0018 (15) | 0.0147 (15) | 0.0005 (14) |
| C16 | 0.042 (2) | 0.046 (2) | 0.0263 (16) | 0.0095 (17) | 0.0070 (16) | −0.0050 (15) |
| C17 | 0.062 (2) | 0.0429 (19) | 0.0227 (15) | 0.0210 (18) | 0.0136 (17) | 0.0072 (14) |
| C18 | 0.059 (2) | 0.060 (2) | 0.038 (2) | 0.009 (2) | 0.0293 (19) | 0.0197 (18) |
| C19 | 0.0365 (19) | 0.050 (2) | 0.0355 (18) | 0.0038 (17) | 0.0154 (16) | 0.0078 (16) |
| C20 | 0.0413 (18) | 0.0320 (16) | 0.0189 (13) | 0.0133 (14) | 0.0157 (13) | 0.0065 (12) |
| C21 | 0.045 (2) | 0.0311 (16) | 0.0293 (16) | 0.0087 (15) | 0.0151 (15) | 0.0039 (13) |
| C22 | 0.072 (3) | 0.046 (2) | 0.0320 (18) | 0.031 (2) | 0.0261 (19) | 0.0075 (16) |
| C23 | 0.059 (2) | 0.076 (3) | 0.0330 (18) | 0.037 (2) | 0.0304 (18) | 0.0223 (19) |
| C24 | 0.045 (2) | 0.065 (2) | 0.0323 (18) | 0.0119 (19) | 0.0200 (17) | 0.0140 (18) |
| C25 | 0.047 (2) | 0.0412 (19) | 0.0279 (16) | 0.0066 (17) | 0.0176 (16) | 0.0005 (14) |
Geometric parameters (Å, º)
| Cl1—C1 | 1.746 (4) | C11—H11 | 1.0000 |
| C1—C2 | 1.376 (5) | C12—C14 | 1.518 (4) |
| C1—C6 | 1.402 (5) | C12—H12 | 1.0000 |
| C2—C3 | 1.376 (6) | C13—H13A | 0.9800 |
| C2—H2 | 0.9500 | C13—H13B | 0.9800 |
| C3—C4 | 1.393 (6) | C13—H13C | 0.9800 |
| C3—H3 | 0.9500 | C14—C15 | 1.372 (4) |
| C4—C5 | 1.413 (5) | C14—C19 | 1.381 (4) |
| C4—H4 | 0.9500 | C15—C16 | 1.384 (4) |
| C5—C6 | 1.379 (4) | C15—H15 | 0.9500 |
| C5—H5 | 0.9500 | C16—C17 | 1.379 (5) |
| C6—C7 | 1.504 (4) | C16—H16 | 0.9500 |
| N1—C12 | 1.487 (4) | C17—C18 | 1.355 (5) |
| N1—C7 | 1.488 (4) | C17—H17 | 0.9500 |
| N1—C8 | 1.496 (4) | C18—C19 | 1.402 (5) |
| C7—H7A | 0.9900 | C18—H18 | 0.9500 |
| C7—H7B | 0.9900 | C19—H19 | 0.9500 |
| C8—C20 | 1.511 (4) | C20—C25 | 1.384 (4) |
| C8—C9 | 1.523 (4) | C20—C21 | 1.395 (4) |
| C8—H8 | 1.0000 | C21—C22 | 1.391 (5) |
| C9—C10 | 1.523 (5) | C21—H21 | 0.9500 |
| C9—H9A | 0.9900 | C22—C23 | 1.374 (5) |
| C9—H9B | 0.9900 | C22—H22 | 0.9500 |
| C10—C11 | 1.520 (4) | C23—C24 | 1.380 (5) |
| C10—H10A | 0.9900 | C23—H23 | 0.9500 |
| C10—H10B | 0.9900 | C24—C25 | 1.378 (5) |
| C11—C12 | 1.536 (4) | C24—H24 | 0.9500 |
| C11—C13 | 1.549 (5) | C25—H25 | 0.9500 |
| C2—C1—C6 | 122.7 (4) | C13—C11—H11 | 108.3 |
| C2—C1—Cl1 | 117.7 (3) | N1—C12—C14 | 109.9 (2) |
| C6—C1—Cl1 | 119.6 (3) | N1—C12—C11 | 112.0 (2) |
| C1—C2—C3 | 118.6 (4) | C14—C12—C11 | 109.8 (2) |
| C1—C2—H2 | 120.7 | N1—C12—H12 | 108.3 |
| C3—C2—H2 | 120.7 | C14—C12—H12 | 108.3 |
| C2—C3—C4 | 122.0 (4) | C11—C12—H12 | 108.3 |
| C2—C3—H3 | 119.0 | C11—C13—H13A | 109.5 |
| C4—C3—H3 | 119.0 | C11—C13—H13B | 109.5 |
| C3—C4—C5 | 117.4 (4) | H13A—C13—H13B | 109.5 |
| C3—C4—H4 | 121.3 | C11—C13—H13C | 109.5 |
| C5—C4—H4 | 121.3 | H13A—C13—H13C | 109.5 |
| C6—C5—C4 | 122.2 (4) | H13B—C13—H13C | 109.5 |
| C6—C5—H5 | 118.9 | C15—C14—C19 | 118.2 (3) |
| C4—C5—H5 | 118.9 | C15—C14—C12 | 120.4 (3) |
| C5—C6—C1 | 117.1 (3) | C19—C14—C12 | 121.4 (3) |
| C5—C6—C7 | 123.5 (3) | C14—C15—C16 | 121.3 (3) |
| C1—C6—C7 | 119.4 (3) | C14—C15—H15 | 119.3 |
| C12—N1—C7 | 108.8 (2) | C16—C15—H15 | 119.3 |
| C12—N1—C8 | 112.7 (2) | C17—C16—C15 | 120.2 (3) |
| C7—N1—C8 | 108.9 (2) | C17—C16—H16 | 119.9 |
| N1—C7—C6 | 115.3 (2) | C15—C16—H16 | 119.9 |
| N1—C7—H7A | 108.4 | C18—C17—C16 | 119.3 (3) |
| C6—C7—H7A | 108.4 | C18—C17—H17 | 120.4 |
| N1—C7—H7B | 108.4 | C16—C17—H17 | 120.4 |
| C6—C7—H7B | 108.4 | C17—C18—C19 | 120.7 (3) |
| H7A—C7—H7B | 107.5 | C17—C18—H18 | 119.6 |
| N1—C8—C20 | 110.2 (3) | C19—C18—H18 | 119.6 |
| N1—C8—C9 | 111.0 (2) | C14—C19—C18 | 120.2 (3) |
| C20—C8—C9 | 111.2 (3) | C14—C19—H19 | 119.9 |
| N1—C8—H8 | 108.1 | C18—C19—H19 | 119.9 |
| C20—C8—H8 | 108.1 | C25—C20—C21 | 117.6 (3) |
| C9—C8—H8 | 108.1 | C25—C20—C8 | 122.3 (3) |
| C8—C9—C10 | 110.8 (3) | C21—C20—C8 | 120.1 (3) |
| C8—C9—H9A | 109.5 | C22—C21—C20 | 121.1 (3) |
| C10—C9—H9A | 109.5 | C22—C21—H21 | 119.4 |
| C8—C9—H9B | 109.5 | C20—C21—H21 | 119.4 |
| C10—C9—H9B | 109.5 | C23—C22—C21 | 119.9 (3) |
| H9A—C9—H9B | 108.1 | C23—C22—H22 | 120.1 |
| C11—C10—C9 | 110.0 (3) | C21—C22—H22 | 120.1 |
| C11—C10—H10A | 109.7 | C22—C23—C24 | 119.6 (4) |
| C9—C10—H10A | 109.7 | C22—C23—H23 | 120.2 |
| C11—C10—H10B | 109.7 | C24—C23—H23 | 120.2 |
| C9—C10—H10B | 109.7 | C25—C24—C23 | 120.4 (3) |
| H10A—C10—H10B | 108.2 | C25—C24—H24 | 119.8 |
| C10—C11—C12 | 110.2 (2) | C23—C24—H24 | 119.8 |
| C10—C11—C13 | 110.3 (3) | C24—C25—C20 | 121.4 (3) |
| C12—C11—C13 | 111.4 (3) | C24—C25—H25 | 119.3 |
| C10—C11—H11 | 108.3 | C20—C25—H25 | 119.3 |
| C12—C11—H11 | 108.3 | ||
| C6—C1—C2—C3 | −0.2 (5) | C10—C11—C12—N1 | 54.7 (4) |
| Cl1—C1—C2—C3 | −179.1 (3) | C13—C11—C12—N1 | 177.5 (3) |
| C1—C2—C3—C4 | −0.6 (5) | C10—C11—C12—C14 | 177.1 (3) |
| C2—C3—C4—C5 | 0.5 (5) | C13—C11—C12—C14 | −60.1 (3) |
| C3—C4—C5—C6 | 0.5 (5) | N1—C12—C14—C15 | 52.4 (4) |
| C4—C5—C6—C1 | −1.2 (4) | C11—C12—C14—C15 | −71.3 (4) |
| C4—C5—C6—C7 | 175.6 (3) | N1—C12—C14—C19 | −129.9 (3) |
| C2—C1—C6—C5 | 1.0 (4) | C11—C12—C14—C19 | 106.5 (4) |
| Cl1—C1—C6—C5 | 179.9 (2) | C19—C14—C15—C16 | −0.7 (5) |
| C2—C1—C6—C7 | −175.9 (3) | C12—C14—C15—C16 | 177.1 (3) |
| Cl1—C1—C6—C7 | 3.0 (4) | C14—C15—C16—C17 | −1.3 (6) |
| C12—N1—C7—C6 | −131.3 (2) | C15—C16—C17—C18 | 2.0 (6) |
| C8—N1—C7—C6 | 105.4 (3) | C16—C17—C18—C19 | −0.8 (6) |
| C5—C6—C7—N1 | 11.4 (4) | C15—C14—C19—C18 | 1.9 (5) |
| C1—C6—C7—N1 | −171.9 (3) | C12—C14—C19—C18 | −175.9 (3) |
| C12—N1—C8—C20 | 177.9 (2) | C17—C18—C19—C14 | −1.2 (6) |
| C7—N1—C8—C20 | −61.2 (3) | N1—C8—C20—C25 | −69.8 (4) |
| C12—N1—C8—C9 | 54.3 (3) | C9—C8—C20—C25 | 53.7 (4) |
| C7—N1—C8—C9 | 175.2 (3) | N1—C8—C20—C21 | 110.8 (3) |
| N1—C8—C9—C10 | −56.3 (3) | C9—C8—C20—C21 | −125.7 (3) |
| C20—C8—C9—C10 | −179.4 (2) | C25—C20—C21—C22 | 0.9 (5) |
| C8—C9—C10—C11 | 58.1 (3) | C8—C20—C21—C22 | −179.6 (3) |
| C9—C10—C11—C12 | −56.7 (4) | C20—C21—C22—C23 | −0.6 (5) |
| C9—C10—C11—C13 | 179.9 (3) | C21—C22—C23—C24 | 0.1 (5) |
| C7—N1—C12—C14 | 62.9 (3) | C22—C23—C24—C25 | 0.1 (5) |
| C8—N1—C12—C14 | −176.1 (2) | C23—C24—C25—C20 | 0.2 (5) |
| C7—N1—C12—C11 | −174.7 (2) | C21—C20—C25—C24 | −0.8 (5) |
| C8—N1—C12—C11 | −53.7 (3) | C8—C20—C25—C24 | 179.8 (3) |
Hydrogen-bond geometry (Å, º)
Cg1 is the centroid of the C20–C25 ring.
| D—H···A | D—H | H···A | D···A | D—H···A |
| C17—H17···Cg1i | 0.95 | 2.83 | 3.692 (4) | 151 |
Symmetry code: (i) x, y, z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB6872).
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) I, global. DOI: 10.1107/S1600536812029200/hb6872sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812029200/hb6872Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812029200/hb6872Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



