Literature DB >> 29152337

Crystal structure and features of 3',8-di-benzyl-idene-4a,5,6,7,8,8a-hexa-hydro-2'H-spiro-[chromene-2,1'-cyclo-hexa-n]-2'-one.

Alexander Anis'kov1, Vyacheslav Grinev1, Irina Klochkova1.   

Abstract

The synthesis and crystal structure of the title compound, C28H28O2, are reported. The C=C-C-C torsion angles in the phenyl-methyl-idene units are 166.6 (3) and -48.0 (4)°. In the crystal, mol-ecules form a three-dimensional network by means of weak C-H⋯O hydrogen bonds. The most important contributions to the crystal structure are the H⋯H inter-actions (68.8%), while the H⋯O contacts account for 4.5%.

Entities:  

Keywords:  X-ray structural analysis; crystal structure; non-covalent inter­actions; spiro heterocycle

Year:  2017        PMID: 29152337      PMCID: PMC5683477          DOI: 10.1107/S2056989017014165

Source DB:  PubMed          Journal:  Acta Crystallogr E Crystallogr Commun


Chemical context

Spiro heterocycles are of great inter­est for the creation of new promising biologically active compounds. The spiro center causes a rigid, spatially oriented configuration, which makes the compounds containing them potentially more complementary to binding sites for biological targets (Mirzabekova et al., 2008 ▸; Abou-Elmagd & Hashem, 2016 ▸; Saraswat et al., 2016 ▸). A convenient way obtain heterocyclic compounds, including those with the spiro chromane moiety, is dimerization of Mannich ketones (Shchekina et al., 2017 ▸).

Structural commentary

The structure of the title compound is shown in Fig. 1 ▸. The pyran, cyclo­hexa­none and methyl­ene­cyclo­hexene units are each non-planar structures with the following puckering parameters: Q = 0.447 Å, θ = 128.1°, φ = 249.3°; Q = 0.517 Å, θ = 167.2°, φ = 12.9°; and Q = 0.460 Å, θ = 130.0°, φ = 39.9°, respectively. In the two phenyl­methyl­idene moieties, the corresponding σ-bonds are shortened [C6—C7 = 1.475 (4) and C23—C22 = 1.471 (4) Å], which allows us to speak of incomplete π–π conjugation of aromatic rings and double bonds. These values are slightly longer than the bond lengths characteristic for complete conjugation in similarly constructed moieties (Golikov et al., 2006 ▸); in particular, for di­benzyl­idene­cyclo­hexa­none it is 1.341 Å. The torsion angles C8=C7—C6—C5 and C18=C22—C23—C28 are similar [−38.5 (5) and −36.3 (5)°, respectively], and reflect the non-coplanarity of the phenyl­methyl­idene moiety, and therefore confirms incomplete conjugation of the phenyl and yl­idene moieties (Kriven’ko et al., 2005 ▸). The values noted above significantly exceed the corresponding ones for torsion angles in analogous moieties in di­benzyl­idene cyclo­hexa­nones (−28.70°; Jia et al., 1989 ▸). Such a significant deviation of the torsion angle from the expected value is probably due to van der Waals repulsion of hydrogen atoms on the cyclo­hexene atoms C9 and C19 and hydrogen atoms of the aromatic rings. Thus, the inter­atomic distance between the hydrogen atoms of the aromatic substituent at C5 and the methyl­ene group at C9 is 2.27 Å, close to the sum of the van der Waals radii for hydrogen atoms (2.2 Å). The C7=C8 bond is a little shorter than the C18=C22 bond [1.337 (4) and 1.346 (4) Å, respectively]. We believe that this is due to better conditions for π–π conjugation of the Ph–C22=C18C17=C16 unit compared to the Ph—C7=C8—C12=O1 unit. So, the value of the C22=C18C17=C16 torsion angle is 166.6 (3)° in comparison with 135.0 (3)° for C7=C8—C12=O1, allowing us to conclude a more pronounced flat structure for the former unit. The O2—C17 bond is noticeably shorter [1.391 (3) Å] than O2—C13 [1.446 (3) Å] due to conjugation of the endocyclic oxygen atom and a multiple bond. The bond lengths of the spiro center are within expected values, and are typical of those in similar moieties (Clark et al., 2005 ▸; Kia et al., 2012 ▸).
Figure 1

The mol­ecular structure of the title compound with atom-labeling scheme, with displacement ellipsoids drawn at the 50% probability level.

Supra­molecular features

In the crystal, the mol­ecules are linked into a complex three-dimensional network by means of weak C20—H20B⋯O1i and C11—H11B⋯O1i hydrogen bonds between (Figs. 2 ▸–4 ▸ ▸ and Table 1 ▸).
Figure 2

Graphical representation of the hydrogen bonds (dashed lines) along the a axis.

Figure 3

Graphical representation of the hydrogen bonds (dashed lines) along the c axis.

Figure 4

Graphical representation of the hydrogen bonds.

Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
C20—H20B⋯O1i 0.992.643.630175
C11—H11B⋯O1i 0.992.613.521153

Symmetry code: (i) .

Analysis of the Hirshfeld Surfaces

The C11—H11B⋯O1i and C20—H20B⋯O1i inter­actions are visualized as bright-red spots between the corresponding donor and acceptor atoms on the Hirshfeld surfaces, mapped by d norm (Fig. 5 ▸). This is confirmed by the Hirshfeld surfaces, displayed as the electrostatic potential (Fig. 6 ▸), showing a negative potential around the oxygen atoms in the form of light-red clouds and a positive potential around the H atoms in the form of bluish clouds. The H⋯O contacts account for about 4.5% of the Hirshfeld surface displayed on the fingerprint plots with a curved surface with d + d ∼2.2 Å (Fig. 7 ▸). The largest proportion, 68.8%, is for H⋯H contacts, with a bright splash on the fingerprint plot corresponding to d + d ∼2.2 Å. The C⋯H inter­action corresponds to 12.2% d + d ∼2.4 Å with peaks in the region of the aromatic rings (Fig. 7 ▸). The presence of π–π stacking reflects the presence of CC contacts, which account for only 1.0% of the Hirschfield surface with d + d ∼2.2 Å.
Figure 5

Graphical representation of the Hirshfeld surface mapped over d norm. The highlighted red spots on the top face of the surfaces indicate contact points with the atoms participating in the C—H⋯O inter­molecular inter­actions.

Figure 6

Graphical representation of the electrostatic potential surfaces.

Figure 7

Graphical representation of the Hirshfeld surface two-dimensional fingerprint plot for the title compound (a) showing the: (b) H⋯O, (c) C⋯H, (d) H⋯H, (e) C⋯C inter­actions.

Database survey

The structure and configuration of the mol­ecule is complex and includes a spiro node and aryl­methyl­idene moieties. A similar spiro ring based on the Mannich ketone was described earlier (Siaka et al., 2012 ▸). The tetra­hydro­pyridine ring is in an unsymmetrical half-chair conformation, while the cyclo­hexa­diene and cyclo­hexene rings display semi-boat conformations.

Synthesis and crystallization

A 5% solution of potassium tert-butoxide in i-iso­propanol (5 mL) was added to a 2-[(di­methyl­amino)­meth­yl)]-6-(phenyl­methyl­idene)cyclo­hexa­none solution (1.396 g, 5 mmol) in i-iso­propanol. The mixture was refluxed for two h, then cooled. The precipitated crystalline substance was washed with a 2% aqueous solution of acetic acid, recrystallized from i-iso­propanol, yielding colourless crystals (1.47 g, 74%), m.p. 413–414 K (i-PrOH). 1H NMR (CDCl3): δ 1.56–1.83 (m, 4H, CH2), 1.90–2.30 (m, 1H, CH2), 2.61 (tt, 2H, J = 15.4, 7.8 Hz, CH2), 2.76–2.88 (m, 1H, CH2), 2.91–3.01 (m,1H, CH2), 6.81 (s, 1H, =CH), 7.10–7.41 (m, 11H, Ar, =CH). 13C NMR (CDCl3): δ 19.6, 22.9 23.8, 27.4, 27.8, 28.7, 29.6, 34.8, 78.9 (spiro C), 111.7, 120.3, 125.8, 127.8, 128.3, 129.3, 129.9, 130.1, 132.7, 134.7, 135.8, 138.0, 138.2, 143.2, 201.2 (C=O). Analysis calculated for C28H28O2 (396.2): C 73.23; H 5.23; N 6.32. Found: C 73.68; H 5.09; N 6.27.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2 ▸.
Table 2

Experimental details

Crystal data
Chemical formulaC28H28O2
M r 396.50
Crystal system, space groupOrthorhombic, P n a21
Temperature (K)100
a, b, c (Å)8.5797 (7), 14.7450 (13), 16.7720 (14)
V3)2121.8 (3)
Z 4
Radiation typeMo Kα
μ (mm−1)0.08
Crystal size (mm)0.24 × 0.22 × 0.21
 
Data collection
DiffractometerBruker SMART CCD 1K area detector
Absorption correctionMulti-scan (SADABS; Bruker, 2008)
T min, T max 0.917, 0.984
No. of measured, independent and observed [I > 2σ(I)] reflections23380, 6113, 4907
R int 0.050
(sin θ/λ)max−1)0.703
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.056, 0.132, 1.05
No. of reflections6113
No. of parameters271
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å−3)0.33, −0.24

Computer programs: SMART (Bruker, 2001 ▸), SAINT (Bruker, 2009 ▸), SHELXS97 (Sheldrick, 2008 ▸), SHELXL2014 (Sheldrick, 2015 ▸), PLATON (Spek, 2009 ▸), publCIF (Westrip, 2010 ▸).

Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989017014165/rk2438sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989017014165/rk2438Isup2.hkl CCDC reference: 1577738 Additional supporting information: crystallographic information; 3D view; checkCIF report
C28H28O2Dx = 1.241 Mg m3
Mr = 396.50Melting point = 413–414 K
Orthorhombic, Pna21Mo Kα radiation, λ = 0.71073 Å
a = 8.5797 (7) ÅCell parameters from 3830 reflections
b = 14.7450 (13) Åθ = 2.4–24.5°
c = 16.7720 (14) ŵ = 0.08 mm1
V = 2121.8 (3) Å3T = 100 K
Z = 4Prism, colourless
F(000) = 8480.24 × 0.22 × 0.21 mm
Bruker SMART CCD 1K area detector diffractometer4907 reflections with I > 2σ(I)
Radiation source: sealed X-ray tubeRint = 0.050
ω scansθmax = 30.0°, θmin = 1.8°
Absorption correction: multi-scan (SADABS; Bruker, 2008)h = −11→12
Tmin = 0.917, Tmax = 0.984k = −20→20
23380 measured reflectionsl = −23→23
6113 independent reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.056Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.132H-atom parameters constrained
S = 1.05w = 1/[σ2(Fo2) + (0.0522P)2 + 1.0029P] where P = (Fo2 + 2Fc2)/3
6113 reflections(Δ/σ)max < 0.001
271 parametersΔρmax = 0.33 e Å3
1 restraintΔρmin = −0.24 e Å3
Geometry. All s.u.'s (except the s.u.in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'s involving l.s. planes.
xyzUiso*/Ueq
O20.1174 (2)0.52918 (13)0.16577 (13)0.0218 (4)
O10.1183 (3)0.75243 (15)0.14425 (13)0.0280 (5)
C18−0.1447 (3)0.48947 (19)0.19621 (18)0.0196 (5)
C6−0.1400 (3)0.65682 (19)−0.06165 (19)0.0225 (6)
C150.1452 (3)0.6535 (2)0.29827 (19)0.0244 (6)
H15A0.17630.64160.35410.029*
H15B0.12110.71890.29350.029*
C21−0.1350 (4)0.6132 (2)0.33496 (19)0.0255 (6)
H21A−0.14340.67820.34920.031*
H21B−0.11680.57870.38470.031*
C22−0.1532 (3)0.44888 (19)0.12445 (18)0.0214 (6)
H22−0.06580.45720.09040.026*
C24−0.3097 (4)0.3970 (2)0.01014 (18)0.0232 (6)
H24−0.24830.4358−0.02240.028*
C120.1424 (3)0.67807 (19)0.11548 (18)0.0202 (5)
C110.3598 (3)0.5667 (2)0.1080 (2)0.0245 (6)
H11A0.41350.51660.13600.029*
H11B0.43680.61550.09850.029*
C28−0.3708 (3)0.3333 (2)0.1377 (2)0.0252 (6)
H28−0.35090.32740.19320.030*
C90.2076 (4)0.6050 (2)−0.01768 (19)0.0245 (6)
H9A0.28220.6499−0.03950.029*
H9B0.15350.5762−0.06320.029*
C2−0.3786 (4)0.6144 (2)−0.1291 (2)0.0300 (7)
H2−0.48500.5966−0.12670.036*
C19−0.2720 (3)0.4892 (2)0.25860 (18)0.0231 (6)
H19A−0.24740.44350.30000.028*
H19B−0.37220.47210.23350.028*
C100.2982 (4)0.5323 (2)0.02809 (19)0.0252 (6)
H10A0.22920.47960.03750.030*
H10B0.38700.5116−0.00490.030*
C23−0.2807 (3)0.39322 (19)0.09204 (18)0.0219 (6)
C130.2283 (3)0.60278 (19)0.16023 (18)0.0212 (6)
C80.0891 (4)0.65388 (19)0.03317 (18)0.0218 (6)
C17−0.0070 (3)0.54326 (19)0.21749 (17)0.0204 (6)
C1−0.2972 (4)0.6319 (2)−0.05929 (19)0.0271 (6)
H1−0.34870.6269−0.00940.033*
C140.2827 (4)0.6308 (2)0.24302 (19)0.0257 (6)
H14A0.35140.68440.23850.031*
H14B0.34420.58080.26680.031*
C25−0.4265 (4)0.3451 (2)−0.0247 (2)0.0279 (7)
H25−0.44400.3486−0.08060.033*
C5−0.0683 (4)0.6665 (2)−0.1359 (2)0.0264 (6)
H50.03740.6853−0.13870.032*
C4−0.1497 (4)0.6491 (2)−0.2057 (2)0.0286 (7)
H4−0.09920.6553−0.25580.034*
C3−0.3049 (4)0.6227 (2)−0.2025 (2)0.0307 (7)
H3−0.36040.6104−0.25030.037*
C7−0.0583 (4)0.67387 (19)0.01428 (18)0.0232 (6)
H7−0.11790.70260.05480.028*
C27−0.4889 (4)0.2823 (2)0.1028 (2)0.0316 (7)
H27−0.55060.24310.13480.038*
C160.0016 (3)0.6001 (2)0.27985 (19)0.0230 (6)
C20−0.2876 (4)0.5820 (2)0.2972 (2)0.0283 (7)
H20A−0.36960.57960.33870.034*
H20B−0.32030.62670.25640.034*
C26−0.5171 (4)0.2885 (2)0.0216 (2)0.0336 (7)
H26−0.59840.2539−0.00200.040*
U11U22U33U12U13U23
O20.0196 (9)0.0200 (10)0.0259 (10)−0.0023 (8)0.0012 (8)0.0002 (8)
O10.0335 (12)0.0230 (10)0.0274 (12)0.0018 (9)−0.0003 (9)−0.0023 (9)
C180.0196 (12)0.0177 (12)0.0215 (13)0.0005 (10)−0.0010 (11)0.0022 (10)
C60.0246 (14)0.0194 (13)0.0236 (14)0.0048 (11)−0.0015 (12)−0.0011 (11)
C150.0267 (15)0.0250 (14)0.0214 (14)−0.0048 (11)−0.0046 (12)−0.0012 (11)
C210.0286 (16)0.0253 (14)0.0227 (14)−0.0022 (12)0.0023 (12)−0.0006 (12)
C220.0202 (12)0.0200 (13)0.0239 (15)−0.0012 (11)0.0012 (11)−0.0004 (11)
C240.0225 (14)0.0208 (14)0.0263 (15)0.0005 (11)0.0009 (12)−0.0011 (11)
C120.0188 (12)0.0195 (13)0.0222 (14)−0.0012 (10)0.0022 (11)−0.0008 (11)
C110.0185 (13)0.0235 (14)0.0315 (16)0.0011 (11)0.0010 (12)0.0008 (12)
C280.0253 (14)0.0239 (14)0.0264 (15)−0.0033 (11)−0.0012 (12)−0.0001 (12)
C90.0238 (14)0.0231 (14)0.0265 (15)0.0022 (11)0.0050 (12)−0.0028 (12)
C20.0276 (15)0.0295 (16)0.0328 (17)0.0010 (12)−0.0025 (14)−0.0012 (13)
C190.0204 (13)0.0266 (14)0.0223 (15)−0.0027 (11)0.0006 (11)0.0001 (12)
C100.0212 (13)0.0245 (14)0.0300 (16)0.0024 (11)0.0051 (12)−0.0009 (12)
C230.0198 (13)0.0197 (13)0.0263 (15)0.0012 (11)−0.0009 (12)−0.0025 (11)
C130.0172 (12)0.0205 (13)0.0258 (14)−0.0012 (10)−0.0009 (11)0.0015 (11)
C80.0247 (14)0.0172 (12)0.0237 (15)−0.0010 (10)0.0035 (12)−0.0007 (11)
C170.0211 (13)0.0189 (13)0.0212 (14)0.0007 (11)0.0002 (10)0.0013 (10)
C10.0272 (15)0.0285 (15)0.0257 (16)0.0037 (12)0.0031 (13)−0.0001 (12)
C140.0239 (14)0.0270 (15)0.0261 (16)−0.0051 (12)−0.0067 (13)0.0010 (12)
C250.0261 (15)0.0297 (16)0.0279 (16)0.0045 (13)−0.0053 (13)−0.0045 (13)
C50.0290 (16)0.0228 (14)0.0275 (15)0.0017 (11)0.0023 (13)0.0002 (12)
C40.0361 (17)0.0271 (15)0.0228 (15)0.0056 (13)0.0028 (13)0.0018 (12)
C30.0377 (18)0.0276 (16)0.0267 (16)0.0051 (13)−0.0065 (14)−0.0038 (13)
C70.0262 (14)0.0201 (13)0.0232 (14)0.0028 (11)0.0040 (12)−0.0018 (11)
C270.0294 (15)0.0269 (15)0.0386 (19)−0.0097 (13)−0.0001 (14)0.0017 (14)
C160.0230 (13)0.0236 (14)0.0224 (14)−0.0011 (11)−0.0007 (11)0.0018 (11)
C200.0243 (15)0.0327 (16)0.0280 (16)0.0013 (13)0.0021 (13)−0.0039 (13)
C260.0295 (16)0.0311 (16)0.0401 (18)−0.0068 (13)−0.0074 (15)−0.0060 (14)
O2—C171.391 (3)C9—C81.510 (4)
O2—C131.446 (3)C9—C101.531 (4)
O1—C121.216 (4)C9—H9A0.9900
C18—C221.346 (4)C9—H9B0.9900
C18—C171.467 (4)C2—C11.387 (5)
C18—C191.512 (4)C2—C31.390 (5)
C6—C51.396 (4)C2—H20.9500
C6—C11.398 (4)C19—C201.520 (4)
C6—C71.475 (4)C19—H19A0.9900
C15—C161.494 (4)C19—H19B0.9900
C15—C141.537 (4)C10—H10A0.9900
C15—H15A0.9900C10—H10B0.9900
C15—H15B0.9900C13—C141.522 (4)
C21—C161.505 (4)C8—C71.337 (4)
C21—C201.526 (4)C17—C161.342 (4)
C21—H21A0.9900C1—H10.9500
C21—H21B0.9900C14—H14A0.9900
C22—C231.471 (4)C14—H14B0.9900
C22—H220.9500C25—C261.380 (5)
C24—C251.390 (4)C25—H250.9500
C24—C231.397 (4)C5—C41.387 (5)
C24—H240.9500C5—H50.9500
C12—C81.497 (4)C4—C31.388 (5)
C12—C131.529 (4)C4—H40.9500
C11—C131.525 (4)C3—H30.9500
C11—C101.526 (4)C7—H70.9500
C11—H11A0.9900C27—C261.386 (5)
C11—H11B0.9900C27—H270.9500
C28—C271.391 (4)C20—H20A0.9900
C28—C231.402 (4)C20—H20B0.9900
C28—H280.9500C26—H260.9500
C17—O2—C13115.6 (2)C9—C10—H10B109.1
C22—C18—C17120.1 (3)H10A—C10—H10B107.8
C22—C18—C19125.3 (3)C24—C23—C28117.6 (3)
C17—C18—C19114.5 (3)C24—C23—C22118.3 (3)
C5—C6—C1118.5 (3)C28—C23—C22124.0 (3)
C5—C6—C7122.9 (3)O2—C13—C14110.3 (2)
C1—C6—C7118.6 (3)O2—C13—C11105.2 (2)
C16—C15—C14113.2 (3)C14—C13—C11113.1 (2)
C16—C15—H15A108.9O2—C13—C12105.0 (2)
C14—C15—H15A108.9C14—C13—C12113.5 (2)
C16—C15—H15B108.9C11—C13—C12109.1 (2)
C14—C15—H15B108.9C7—C8—C12117.1 (3)
H15A—C15—H15B107.8C7—C8—C9127.5 (3)
C16—C21—C20112.0 (3)C12—C8—C9115.4 (3)
C16—C21—H21A109.2C16—C17—O2122.5 (3)
C20—C21—H21A109.2C16—C17—C18124.8 (3)
C16—C21—H21B109.2O2—C17—C18112.7 (2)
C20—C21—H21B109.2C2—C1—C6120.7 (3)
H21A—C21—H21B107.9C2—C1—H1119.6
C18—C22—C23128.2 (3)C6—C1—H1119.6
C18—C22—H22115.9C13—C14—C15112.0 (2)
C23—C22—H22115.9C13—C14—H14A109.2
C25—C24—C23121.3 (3)C15—C14—H14A109.2
C25—C24—H24119.3C13—C14—H14B109.2
C23—C24—H24119.3C15—C14—H14B109.2
O1—C12—C8121.9 (3)H14A—C14—H14B107.9
O1—C12—C13122.8 (3)C26—C25—C24120.2 (3)
C8—C12—C13115.3 (2)C26—C25—H25119.9
C13—C11—C10111.3 (2)C24—C25—H25119.9
C13—C11—H11A109.4C4—C5—C6120.8 (3)
C10—C11—H11A109.4C4—C5—H5119.6
C13—C11—H11B109.4C6—C5—H5119.6
C10—C11—H11B109.4C5—C4—C3120.2 (3)
H11A—C11—H11B108.0C5—C4—H4119.9
C27—C28—C23120.8 (3)C3—C4—H4119.9
C27—C28—H28119.6C2—C3—C4119.7 (3)
C23—C28—H28119.6C2—C3—H3120.1
C8—C9—C10113.1 (3)C4—C3—H3120.1
C8—C9—H9A109.0C8—C7—C6128.1 (3)
C10—C9—H9A109.0C8—C7—H7116.0
C8—C9—H9B109.0C6—C7—H7116.0
C10—C9—H9B109.0C26—C27—C28120.4 (3)
H9A—C9—H9B107.8C26—C27—H27119.8
C1—C2—C3120.1 (3)C28—C27—H27119.8
C1—C2—H2120.0C17—C16—C15122.4 (3)
C3—C2—H2120.0C17—C16—C21121.1 (3)
C18—C19—C20110.8 (3)C15—C16—C21116.6 (3)
C18—C19—H19A109.5C19—C20—C21111.9 (3)
C20—C19—H19A109.5C19—C20—H20A109.2
C18—C19—H19B109.5C21—C20—H20A109.2
C20—C19—H19B109.5C19—C20—H20B109.2
H19A—C19—H19B108.1C21—C20—H20B109.2
C11—C10—C9112.6 (2)H20A—C20—H20B107.9
C11—C10—H10A109.1C25—C26—C27119.6 (3)
C9—C10—H10A109.1C25—C26—H26120.2
C11—C10—H10B109.1C27—C26—H26120.2
C17—C18—C22—C23−179.5 (3)C19—C18—C17—C16−10.4 (4)
C19—C18—C22—C23−2.9 (5)C22—C18—C17—O2−13.6 (4)
C22—C18—C19—C20−138.5 (3)C19—C18—C17—O2169.4 (2)
C17—C18—C19—C2038.4 (3)C3—C2—C1—C6−0.9 (5)
C13—C11—C10—C956.7 (3)C5—C6—C1—C22.1 (5)
C8—C9—C10—C11−47.7 (3)C7—C6—C1—C2−179.4 (3)
C25—C24—C23—C281.7 (4)O2—C13—C14—C15−54.1 (3)
C25—C24—C23—C22178.9 (3)C11—C13—C14—C15−171.6 (2)
C27—C28—C23—C24−2.5 (4)C12—C13—C14—C1563.4 (3)
C27—C28—C23—C22−179.6 (3)C16—C15—C14—C1331.0 (4)
C18—C22—C23—C24146.7 (3)C23—C24—C25—C260.2 (5)
C18—C22—C23—C28−36.3 (5)C1—C6—C5—C4−2.0 (4)
C17—O2—C13—C1451.7 (3)C7—C6—C5—C4179.6 (3)
C17—O2—C13—C11173.9 (2)C6—C5—C4—C30.8 (5)
C17—O2—C13—C12−70.9 (3)C1—C2—C3—C4−0.3 (5)
C10—C11—C13—O255.0 (3)C5—C4—C3—C20.4 (5)
C10—C11—C13—C14175.4 (2)C12—C8—C7—C6−179.4 (3)
C10—C11—C13—C12−57.2 (3)C9—C8—C7—C6−2.8 (5)
O1—C12—C13—O2119.4 (3)C5—C6—C7—C8−38.5 (5)
C8—C12—C13—O2−60.5 (3)C1—C6—C7—C8143.1 (3)
O1—C12—C13—C14−1.1 (4)C23—C28—C27—C261.5 (5)
C8—C12—C13—C14179.0 (3)O2—C17—C16—C150.6 (4)
O1—C12—C13—C11−128.2 (3)C18—C17—C16—C15−179.7 (3)
C8—C12—C13—C1151.9 (3)O2—C17—C16—C21−179.6 (3)
O1—C12—C8—C7−48.0 (4)C18—C17—C16—C210.2 (5)
C13—C12—C8—C7131.9 (3)C14—C15—C16—C17−4.5 (4)
O1—C12—C8—C9135.0 (3)C14—C15—C16—C21175.6 (3)
C13—C12—C8—C9−45.1 (3)C20—C21—C16—C17−18.7 (4)
C10—C9—C8—C7−134.9 (3)C20—C21—C16—C15161.2 (3)
C10—C9—C8—C1241.8 (3)C18—C19—C20—C21−57.5 (3)
C13—O2—C17—C16−25.4 (4)C16—C21—C20—C1947.1 (4)
C13—O2—C17—C18154.9 (2)C24—C25—C26—C27−1.3 (5)
C22—C18—C17—C16166.6 (3)C28—C27—C26—C250.4 (5)
D—H···AD—HH···AD···AD—H···A
C20—H20B···O1i0.992.643.630175
C11—H11B···O1i0.992.613.521153
  4 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  Crystal structure refinement with SHELXL.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr C Struct Chem       Date:  2015-01-01       Impact factor: 1.172

3.  (3E,5E)-3,5-Bis(4-methyl-benzyl-idene)-1-[3-(piperidin-1-yl)propano-yl]piperidin-4-one.

Authors:  Yalda Kia; Hasnah Osman; Vikneswaran Murugaiyah; Suhana Arshad; Ibrahim Abdul Razak
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2012-07-18

4.  Structure validation in chemical crystallography.

Authors:  Anthony L Spek
Journal:  Acta Crystallogr D Biol Crystallogr       Date:  2009-01-20
  4 in total

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