organic compounds
1,1′-[(2,3,5,6-Tetramethyl-1,4-phenylene)bis(methylene)]dipiperidine
aDepartment of Chemistry, Popes College affiliated to Manonmaniam Sundaranar University, Tirunelveli, Tamil Nadu 627 012, India, bDepartment of Chemistry, Ponnaiyah Ramajayam Institute of Science and Technology, Vallam, Thanjavur 613 403, TamilNadu, India, and cUniversity of Mainz, Institut of Organic Chemistry, Duesbergweg 10-14, 55128 Mainz, Germany
*Correspondence e-mail: bravidurai@gmail.com
The 22H36N2, comprises one half-molecule, the other half being generated by a center of inversion. The piperidine ring adopts a chair conformation, with the exocyclic N—C bond in an equatorial orientation. A short intramolecular C—H⋯N hydrogen bond occurs and forms an S(6) motif. No directional interactions beyond van der Waals contacts are observed between the molecules, which form a wave-like supramolecular architecture.
of the title compound, CCCDC reference: 943697
Structure description
Some piperidine derivatives possess significant biological and medicinal properties including insulin normalization, addiction therapeutics (Kozikowski et al., 1998) and local anaesthesia (McElvain & Carney, 1946). Here we report the synthesis and of a new piperidine-substituted durene.
The x,1 − y,1 − z; see Fig. 1). The piperidine rings adopt a chair conformation with puckering parameters Q = 0.5765 (16) Å, Θ =178.20 (15)° φ = 181 (5)°. The dihedral angle between the phenyl (C8/C9/C11/C8a/C9a/C11a) and piperidine (N1/C2–C6) rings is 73.66 (7)°. The weak intramolecular C12—H12B⋯N1 hydrogen bond (Table 1) forms an S(6) motif. In the crystal, adjacent molecules are aggregated by weak van der Waals interactions, leading to a wave-like supramolecular architecture (Fig. 2) extending along b-axis direction.
is made up of one half-molecule, the other half being generated by inversion (symmetry code: 1 −
|
Synthesis and crystallization
A mixture of piperidine hydrochloride (0.242 g, 2 mmol) in sodium ethoxide solution and 1,4-bis(bromomethyl)durene (0.320 g, 1 mmol) in ethanol and water (15 ml) were heated at 333 K with continuous stirring for about 4 h. The mixture was kept aside for slow evaporation. After two weeks, colourless block-shaped crystals (m.p. 462 K) suitable for single-crystal X-ray diffraction were formed.
Refinement
Crystal data, data collection and structure .
details are summarized in Table 2Structural data
CCDC reference: 943697
https://doi.org/10.1107/S2414314618012373/bv4021sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314618012373/bv4021Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314618012373/bv4021Isup3.cml
Data collection: APEX2 (Bruker, 2004); cell
SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004); program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015); software used to prepare material for publication: SHELXL2018 (Sheldrick, 2015).C22H36N2 | F(000) = 364 |
Mr = 328.53 | Dx = 1.150 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 5.6271 (4) Å | Cell parameters from 1751 reflections |
b = 21.1764 (14) Å | θ = 2.7–27.7° |
c = 8.2787 (5) Å | µ = 0.07 mm−1 |
β = 105.860 (2)° | T = 173 K |
V = 948.95 (11) Å3 | Block, colourless |
Z = 2 | 0.45 × 0.17 × 0.15 mm |
Bruker SMART APEXII diffractometer | 1779 reflections with I > 2σ(I) |
Radiation source: sealed Tube | Rint = 0.027 |
Graphite monochromator | θmax = 27.7°, θmin = 1.9° |
CCD scan | h = −7→6 |
6578 measured reflections | k = −27→16 |
2237 independent reflections | l = −9→10 |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.045 | All H-atom parameters refined |
wR(F2) = 0.118 | w = 1/[σ2(Fo2) + (0.0555P)2 + 0.2324P] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max < 0.001 |
2237 reflections | Δρmax = 0.28 e Å−3 |
172 parameters | Δρmin = −0.16 e Å−3 |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
Refinement. The H atoms were added at positions obtained from difference Fourier maps and refined isotropically. |
x | y | z | Uiso*/Ueq | ||
N1 | 0.48878 (19) | 0.63789 (5) | 0.20943 (13) | 0.0239 (3) | |
C2 | 0.4075 (2) | 0.59637 (6) | 0.06304 (16) | 0.0268 (3) | |
H2A | 0.221 (3) | 0.6020 (6) | 0.0122 (18) | 0.029 (3)* | |
H2B | 0.434 (3) | 0.5516 (7) | 0.1021 (18) | 0.029 (3)* | |
C3 | 0.5439 (3) | 0.61062 (6) | −0.06807 (17) | 0.0305 (3) | |
H3A | 0.487 (3) | 0.5819 (8) | −0.166 (2) | 0.039 (3)* | |
H3B | 0.725 (3) | 0.6027 (7) | −0.018 (2) | 0.039 (3)* | |
C4 | 0.5071 (3) | 0.67927 (7) | −0.12320 (19) | 0.0363 (3) | |
H4A | 0.331 (3) | 0.6873 (8) | −0.179 (2) | 0.048 (3)* | |
H4B | 0.605 (3) | 0.6902 (8) | −0.201 (2) | 0.048 (3)* | |
C5 | 0.5808 (3) | 0.72219 (7) | 0.0303 (2) | 0.0380 (4) | |
H5A | 0.765 (3) | 0.7182 (8) | 0.083 (2) | 0.047 (3)* | |
H5B | 0.549 (3) | 0.7677 (9) | −0.003 (2) | 0.047 (3)* | |
C6 | 0.4436 (3) | 0.70403 (6) | 0.15832 (18) | 0.0320 (3) | |
H6A | 0.497 (3) | 0.7317 (7) | 0.262 (2) | 0.037 (3)* | |
H6B | 0.258 (3) | 0.7116 (7) | 0.1108 (19) | 0.037 (3)* | |
C7 | 0.3611 (2) | 0.62262 (6) | 0.33824 (16) | 0.0267 (3) | |
H7A | 0.178 (3) | 0.6271 (6) | 0.2908 (18) | 0.028 (2)* | |
H7B | 0.407 (3) | 0.6563 (7) | 0.4244 (18) | 0.028 (2)* | |
C8 | 0.4317 (2) | 0.55846 (6) | 0.41941 (15) | 0.0227 (3) | |
C9 | 0.2674 (2) | 0.50691 (6) | 0.38251 (14) | 0.0232 (3) | |
C10 | 0.0179 (3) | 0.51192 (7) | 0.25473 (18) | 0.0312 (3) | |
H10A | 0.015 (4) | 0.4889 (11) | 0.152 (3) | 0.088 (4)* | |
H10B | −0.024 (4) | 0.5535 (12) | 0.220 (3) | 0.088 (4)* | |
H10C | −0.114 (5) | 0.4943 (10) | 0.296 (3) | 0.088 (4)* | |
C11 | 0.6640 (2) | 0.55124 (6) | 0.53631 (15) | 0.0231 (3) | |
C12 | 0.8452 (3) | 0.60566 (7) | 0.57599 (18) | 0.0307 (3) | |
H12A | 0.882 (3) | 0.6199 (8) | 0.695 (2) | 0.056 (3)* | |
H12B | 0.791 (4) | 0.6411 (9) | 0.508 (2) | 0.056 (3)* | |
H12C | 1.002 (4) | 0.5941 (9) | 0.561 (2) | 0.056 (3)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0289 (5) | 0.0205 (5) | 0.0239 (5) | 0.0011 (4) | 0.0102 (4) | 0.0009 (4) |
C2 | 0.0328 (7) | 0.0242 (6) | 0.0244 (6) | −0.0008 (5) | 0.0095 (5) | 0.0001 (5) |
C3 | 0.0380 (7) | 0.0309 (7) | 0.0255 (7) | 0.0034 (6) | 0.0136 (6) | 0.0014 (5) |
C4 | 0.0427 (8) | 0.0372 (8) | 0.0339 (8) | 0.0082 (6) | 0.0187 (7) | 0.0127 (6) |
C5 | 0.0491 (9) | 0.0247 (7) | 0.0477 (9) | 0.0014 (6) | 0.0256 (7) | 0.0074 (6) |
C6 | 0.0409 (8) | 0.0208 (6) | 0.0375 (8) | 0.0032 (5) | 0.0164 (6) | 0.0021 (5) |
C7 | 0.0316 (7) | 0.0248 (6) | 0.0269 (7) | 0.0036 (5) | 0.0134 (5) | 0.0009 (5) |
C8 | 0.0275 (6) | 0.0243 (6) | 0.0194 (6) | 0.0005 (5) | 0.0117 (5) | −0.0014 (4) |
C9 | 0.0255 (6) | 0.0283 (6) | 0.0180 (6) | 0.0004 (5) | 0.0098 (5) | −0.0016 (5) |
C10 | 0.0286 (7) | 0.0359 (7) | 0.0274 (7) | −0.0018 (5) | 0.0049 (5) | 0.0015 (6) |
C11 | 0.0282 (6) | 0.0249 (6) | 0.0194 (6) | −0.0024 (5) | 0.0117 (5) | −0.0036 (4) |
C12 | 0.0337 (7) | 0.0290 (7) | 0.0294 (7) | −0.0073 (5) | 0.0085 (6) | −0.0030 (5) |
N1—C6 | 1.4652 (16) | C6—H6B | 1.024 (16) |
N1—C2 | 1.4655 (16) | C7—C8 | 1.5198 (17) |
N1—C7 | 1.4753 (16) | C7—H7A | 1.003 (15) |
C2—C3 | 1.5207 (18) | C7—H7B | 0.991 (15) |
C2—H2A | 1.026 (15) | C8—C11 | 1.4060 (17) |
C2—H2B | 1.000 (14) | C8—C9 | 1.4090 (17) |
C3—C4 | 1.5209 (19) | C9—C11i | 1.4055 (17) |
C3—H3A | 0.991 (17) | C9—C10 | 1.5131 (18) |
C3—H3B | 1.003 (17) | C10—H10A | 0.98 (2) |
C4—C5 | 1.525 (2) | C10—H10B | 0.94 (2) |
C4—H4A | 0.987 (18) | C10—H10C | 0.97 (2) |
C4—H4B | 0.984 (18) | C11—C12 | 1.5143 (17) |
C5—C6 | 1.521 (2) | C12—H12A | 0.996 (19) |
C5—H5A | 1.013 (18) | C12—H12B | 0.94 (2) |
C5—H5B | 1.003 (18) | C12—H12C | 0.957 (19) |
C6—H6A | 1.017 (16) | ||
C6—N1—C2 | 110.14 (10) | N1—C6—H6B | 109.9 (9) |
C6—N1—C7 | 109.74 (10) | C5—C6—H6B | 110.6 (9) |
C2—N1—C7 | 111.27 (10) | H6A—C6—H6B | 105.6 (12) |
N1—C2—C3 | 111.53 (11) | N1—C7—C8 | 113.30 (10) |
N1—C2—H2A | 108.8 (8) | N1—C7—H7A | 110.4 (8) |
C3—C2—H2A | 110.1 (8) | C8—C7—H7A | 112.0 (8) |
N1—C2—H2B | 108.5 (8) | N1—C7—H7B | 106.3 (8) |
C3—C2—H2B | 111.0 (8) | C8—C7—H7B | 109.8 (8) |
H2A—C2—H2B | 106.7 (11) | H7A—C7—H7B | 104.5 (11) |
C2—C3—C4 | 110.49 (11) | C11—C8—C9 | 119.77 (11) |
C2—C3—H3A | 110.2 (9) | C11—C8—C7 | 118.88 (11) |
C4—C3—H3A | 110.8 (9) | C9—C8—C7 | 121.33 (11) |
C2—C3—H3B | 109.0 (9) | C11i—C9—C8 | 119.79 (11) |
C4—C3—H3B | 108.9 (9) | C11i—C9—C10 | 118.48 (11) |
H3A—C3—H3B | 107.5 (13) | C8—C9—C10 | 121.73 (11) |
C3—C4—C5 | 109.63 (12) | C9—C10—H10A | 111.6 (14) |
C3—C4—H4A | 109.9 (10) | C9—C10—H10B | 112.8 (15) |
C5—C4—H4A | 107.2 (10) | H10A—C10—H10B | 104.8 (19) |
C3—C4—H4B | 111.5 (10) | C9—C10—H10C | 112.3 (14) |
C5—C4—H4B | 109.5 (10) | H10A—C10—H10C | 106.1 (19) |
H4A—C4—H4B | 109.0 (14) | H10B—C10—H10C | 108.6 (19) |
C6—C5—C4 | 110.83 (12) | C9i—C11—C8 | 120.44 (11) |
C6—C5—H5A | 109.3 (9) | C9i—C11—C12 | 118.84 (11) |
C4—C5—H5A | 109.0 (9) | C8—C11—C12 | 120.72 (11) |
C6—C5—H5B | 110.2 (10) | C11—C12—H12A | 113.1 (10) |
C4—C5—H5B | 111.0 (10) | C11—C12—H12B | 113.0 (12) |
H5A—C5—H5B | 106.5 (13) | H12A—C12—H12B | 107.0 (15) |
N1—C6—C5 | 111.19 (11) | C11—C12—H12C | 111.5 (11) |
N1—C6—H6A | 108.6 (9) | H12A—C12—H12C | 104.8 (15) |
C5—C6—H6A | 110.8 (9) | H12B—C12—H12C | 106.8 (16) |
C6—N1—C2—C3 | 59.72 (14) | N1—C7—C8—C11 | 74.54 (14) |
C7—N1—C2—C3 | −178.35 (10) | N1—C7—C8—C9 | −106.87 (13) |
N1—C2—C3—C4 | −57.54 (15) | C11—C8—C9—C11i | 0.46 (18) |
C2—C3—C4—C5 | 53.97 (16) | C7—C8—C9—C11i | −178.11 (10) |
C3—C4—C5—C6 | −54.05 (17) | C11—C8—C9—C10 | −178.56 (11) |
C2—N1—C6—C5 | −59.38 (15) | C7—C8—C9—C10 | 2.87 (18) |
C7—N1—C6—C5 | 177.78 (12) | C9—C8—C11—C9i | −0.46 (18) |
C4—C5—C6—N1 | 57.25 (16) | C7—C8—C11—C9i | 178.14 (10) |
C6—N1—C7—C8 | −170.47 (11) | C9—C8—C11—C12 | 179.05 (11) |
C2—N1—C7—C8 | 67.37 (14) | C7—C8—C11—C12 | −2.34 (17) |
Symmetry code: (i) −x+1, −y+1, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
C12—H12B···N1 | 0.94 (2) | 2.59 (2) | 3.2204 (18) | 124.8 (14) |
References
Bruker (2004). APEX2. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Burla, M. C., Caliandro, R., Camalli, M., Carrozzini, B., Cascarano, G. L., De Caro, L., Giacovazzo, C., Polidori, G. & Spagna, R. (2005). J. Appl. Cryst. 38, 381–388. Web of Science CrossRef CAS IUCr Journals Google Scholar
Cason, C. J. (2004). POV-RAY for Windows. Persistence of Vision, Raytracer Pty. Ltd, Victoria, Australia. https://www.povray.org. Google Scholar
Johnson, C. K. (1976). ORTEPII. Report ORNL-5138. Oak Ridge National Laboratory, Tennessee, USA. Google Scholar
Kozikowski, A. P., Araldi, G. L., Boja, J., Meil, W. M., Johnson, K. M., Flippen-Anderson, J. L., George, C. & Saiah, E. (1998). J. Med. Chem. 41, 1962–1969. Web of Science CSD CrossRef CAS PubMed Google Scholar
Macrae, C. F., Bruno, I. J., Chisholm, J. A., Edgington, P. R., McCabe, P., Pidcock, E., Rodriguez-Monge, L., Taylor, R., van de Streek, J. & Wood, P. A. (2008). J. Appl. Cryst. 41, 466–470. Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
McElvain, S. M. & Carney, T. P. (1946). J. Am. Chem. Soc. 68, 2592–2600. CrossRef Web of Science Google Scholar
Sheldrick, G. M. (2015). Acta Cryst. C71, 3–8. Web of Science CrossRef IUCr Journals Google Scholar
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