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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Feb 13;64(Pt 3):o573. doi: 10.1107/S1600536808003887

1,3-Di-3-pyridyl-2,3-dihydro-1H-naphth[1,2-e][1,3]oxazine

Betül Şen a,*, Zuhal Turgut b, Emel Pelit b, Muhittin Aygün a
PMCID: PMC2960797  PMID: 21201915

Abstract

In the crystal structure of the title compound, C22H17N3O, the oxazine ring has a half-chair conformation. The dihedral angles between the best least-squares plane through the pyridine rings and the planar part (O–C–C–C–N) of the oxazine ring are 72.14 (6) and 35.44 (7)°, the smaller angle involving the pyridine ring adjacent to the oxazine O atom. The mol­ecule has two stereogenic centers at the oxazine carbons, RS and SR. The crystal packing reveals that symmetry-related mol­ecules are linked by inter­molecular N—H⋯N hydrogen bonds to form chains parallel to the b axis.

Related literature

For related literature, see: Kurz et al. (2005); Turgut et al. (2007); Szatmari et al. (2003, 2004); Bernstein et al. (1995); Cremer & Pople (1975).graphic file with name e-64-0o573-scheme1.jpg

Experimental

Crystal data

  • C22H17N3O

  • M r = 339.39

  • Monoclinic, Inline graphic

  • a = 12.1720 (8) Å

  • b = 8.0444 (6) Å

  • c = 18.7716 (15) Å

  • β = 112.615 (5)°

  • V = 1696.7 (2) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 293 (2) K

  • 0.28 × 0.22 × 0.12 mm

Data collection

  • Stoe IPDSII diffractometer

  • Absorption correction: none

  • 15207 measured reflections

  • 3703 independent reflections

  • 1786 reflections with I > 2σ(I)

  • R int = 0.124

Refinement

  • R[F 2 > 2σ(F 2)] = 0.041

  • wR(F 2) = 0.092

  • S = 0.80

  • 3703 reflections

  • 304 parameters

  • All H-atom parameters refined

  • Δρmax = 0.12 e Å−3

  • Δρmin = −0.13 e Å−3

Data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEPIII (Burnett & Johnson, 1996) and PLATON (Spek, 2003); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808003887/su2043sup1.cif

e-64-0o573-sup1.cif (20.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808003887/su2043Isup2.hkl

e-64-0o573-Isup2.hkl (221.2KB, 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
N1—H1⋯N3i 0.98 (2) 2.04 (2) 3.009 (2) 170.7 (17)

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors acknowledge the Faculty of Arts and Sciences, Ondokuz Mayıs University, Turkey, for the use of the Stoe IPDSII diffractometer (purchased under grant No. F.279 of the University Research Fund), and Dokuz Eylül University Research Funds (Project No. 04.KB.FEN.100).

supplementary crystallographic information

Comment

1,3-oxazine heterocycles are of interest because they constitute an important class of natural and non-natural products. Many of them exhibit biological activity such as analgesic, anticonvulsant, antitubercular, antibacterial and anticancer (Kurz et al., 2005; Turgut et al., 2007). In addition, they can be used as intermediates in the synthesis of N-substituted amino alcohols or in enantioselective synthesis of chiral amines. The tautomeric character of the 1,3-O,N-heterocycles offers a great number of synthetic possibilities (Szatmari et al., 2003; Szatmari et al., 2004).

Atoms (C11, C20, C21 and O1) of the oxazine six-membered ring are planar to within 0.014 Å. The oxazine ring adopts a half-chair conformation, with atom C22 and N1 deviating by -0.375 (3) Å and 0.308 (3) Å, respectively, from the mean plane formed by atoms (C11, C20, C21 and O1). The ring puckering parameters for the oxazine ring are Q = 0.451 (2) Å, θ = 126.2 (2)° and φ = 92.4 (3) ° (Cremer & Pople, 1975). The dihedral angles made by the best least-squares plane through all six atoms of the oxazine ring with the mean planes of the pyridine rings (N2/C1—C5) and (N3/C6—C10) are 79.62 (9)° and 36.40 (9)°, respectively. The sum of the angles at N1 of the oxazine ring is 334.1°, in accordance with sp3-hybridization. The H atoms bonded to atoms C22 and C21 of the oxazine ring are axial and trans to one another. The structure is centrosymmetric so the absolute configurations of the two stereogenic centres, C21 and C22, are RS and SR, respectively.

In the crystal structure, intermolecular N1—H1···N3i hydrogen bonds (Table 1) link the molecules to form an infinite one-dimensional polymeric chain. In this manner a C(6) chain (Bernstein et al., 1995) is formed and the axis of the polymeric chain runs co-linear with the crystallographic [010] direction of the monoclinic unit cell (Fig. 2).

Experimental

The title compound was prepared by cyclization reactions realised using 2-naphthol and pyridine-3-carbaldehyde in the presence of dry methanolic ammonia (Fig. 3). The structure of the title compound has been clarified by FTIR, MS and NMR techniques and confirmed by elemental analysis.

Pyridin-3-carbaldehyde (2 mmol; freshly distilled if liquid) and 25% methanolic ammonia solution (0.5 mL) were added to a solution of 2-naphthol (1 mmol) in absolute MeOH (0.5 ml). The mixture was left to stand at ambient temperature for 2 days, during which time a crystalline product separated out. The crude product was filtered off, washed with cold MeOH (2x2mL), then purified by column chromatography with ethyl acetate/n-hexane (3:1). Pale-yellow crystals of the title compound, suitable for X-ray analysis, were obtained by slow evaporation of this solution.

1H NMR (CDCl3, δ (p.p.m.)): 5.34 (s, 1H, CH); 5.89 (s, 1H, CH); 7.21–7.89 (m, 10H, ArH); 8.50–8.89 (m, 4H, pyridine)

13C NMR (CDCl3, δ (p.p.m.)): 56.23, 81.75, 124.37, 133.67, 139.76, 148.27, 150.52, 154.3

FTIR(KBr, cm-1, ν) 3335, 3056,3034, 1622,1596,1260,1233,1023,928

Refinement

All H atoms were located in difference Fourier maps and were freely refined: N—H = 0.97 (2), C—H = 0.95 (2) - 1.04 (2) Å

Figures

Fig. 1.

Fig. 1.

An ORTEPIII (Burnett & Johnson, 1996) view of the title compound with the atomic numbering scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are shown as spheres of arbitrary size.

Fig. 2.

Fig. 2.

The crystal packing diagram of the title compound showing the infinite zigzag chain along the b axis, formed through N—H···N hydrogen bonding (dashed lines) [Symmetry codes: (*) 1 - x,1/2 + y,1/2 - z].

Fig. 3.

Fig. 3.

The formation of the title compound.

Crystal data

C22H17N3O F000 = 712
Mr = 339.39 Dx = 1.329 Mg m3
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 10289 reflections
a = 12.1720 (8) Å θ = 1.7–27.2º
b = 8.0444 (6) Å µ = 0.08 mm1
c = 18.7716 (15) Å T = 293 (2) K
β = 112.615 (5)º Prism, pale yellow
V = 1696.7 (2) Å3 0.28 × 0.22 × 0.12 mm
Z = 4

Data collection

Stoe IPDSII diffractometer 3703 independent reflections
Radiation source: fine-focus sealed tube 1786 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.124
Detector resolution: 6.67 pixels mm-1 θmax = 27.2º
T = 293(2) K θmin = 2.4º
ω and φ scans h = −15→15
Absorption correction: none k = −10→10
15207 measured reflections l = −24→24

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full All H-atom parameters refined
R[F2 > 2σ(F2)] = 0.041   w = 1/[σ2(Fo2) + (0.0317P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.092 (Δ/σ)max < 0.001
S = 0.80 Δρmax = 0.12 e Å3
3703 reflections Δρmin = −0.13 e Å3
304 parameters Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0155 (15)
Secondary atom site location: difference Fourier map

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 0.50525 (11) 0.70176 (16) 0.05782 (6) 0.0613 (3)
N1 0.34476 (13) 0.63357 (19) 0.09666 (7) 0.0530 (4)
N2 0.07931 (16) 0.2535 (2) 0.01583 (9) 0.0797 (5)
N3 0.61988 (16) 0.4333 (2) 0.30101 (8) 0.0708 (5)
C1 0.20165 (16) 0.4668 (2) −0.00607 (8) 0.0515 (4)
C2 0.22195 (18) 0.3658 (2) −0.05879 (10) 0.0624 (5)
C3 0.1718 (2) 0.2087 (3) −0.07310 (11) 0.0721 (6)
C4 0.1012 (2) 0.1592 (3) −0.03549 (11) 0.0750 (6)
C5 0.13038 (19) 0.4030 (3) 0.02947 (10) 0.0664 (5)
C6 0.55109 (16) 0.5779 (2) 0.17981 (8) 0.0518 (4)
C7 0.54203 (19) 0.4545 (2) 0.22813 (10) 0.0619 (5)
C8 0.7097 (2) 0.5402 (3) 0.32714 (11) 0.0717 (6)
C9 0.7258 (2) 0.6678 (3) 0.28396 (10) 0.0713 (6)
C10 0.64504 (18) 0.6866 (2) 0.20842 (9) 0.0621 (5)
C11 0.42404 (16) 0.7472 (2) −0.01352 (8) 0.0521 (4)
C12 0.4760 (2) 0.8298 (2) −0.05937 (10) 0.0581 (5)
C13 0.40609 (19) 0.8731 (2) −0.13285 (10) 0.0614 (5)
C14 0.28339 (18) 0.8404 (2) −0.16314 (9) 0.0571 (5)
C15 0.2110 (2) 0.8834 (3) −0.24001 (10) 0.0703 (6)
C16 0.0929 (2) 0.8602 (3) −0.26809 (12) 0.0854 (7)
C17 0.0389 (2) 0.7933 (3) −0.22063 (12) 0.0884 (7)
C18 0.10616 (19) 0.7473 (3) −0.14611 (10) 0.0703 (6)
C19 0.23078 (17) 0.7670 (2) −0.11493 (9) 0.0548 (5)
C20 0.30495 (16) 0.7173 (2) −0.03826 (8) 0.0506 (4)
C21 0.25461 (17) 0.6395 (2) 0.01656 (8) 0.0530 (4)
C22 0.45819 (16) 0.5869 (2) 0.09848 (8) 0.0526 (4)
H1 0.3522 (17) 0.738 (3) 0.1247 (10) 0.080 (6)*
H2 0.2726 (17) 0.408 (2) −0.0873 (9) 0.073 (5)*
H3 0.1834 (19) 0.141 (3) −0.1108 (12) 0.099 (7)*
H4 0.0621 (19) 0.051 (3) −0.0461 (11) 0.089 (7)*
H5 0.1146 (18) 0.475 (3) 0.0680 (10) 0.083 (6)*
H7 0.4767 (18) 0.367 (3) 0.2099 (10) 0.077 (6)*
H8 0.7714 (19) 0.522 (3) 0.3822 (11) 0.094 (7)*
H9 0.7932 (19) 0.744 (3) 0.3052 (10) 0.083 (6)*
H10 0.6560 (18) 0.777 (3) 0.1759 (10) 0.090 (6)*
H12 0.5600 (18) 0.853 (2) −0.0360 (9) 0.064 (5)*
H13 0.4472 (17) 0.928 (2) −0.1648 (9) 0.076 (5)*
H15 0.2541 (18) 0.935 (3) −0.2732 (10) 0.087 (6)*
H16 0.041 (2) 0.891 (3) −0.3203 (13) 0.113 (8)*
H17 −0.047 (2) 0.776 (3) −0.2404 (12) 0.107 (8)*
H18 0.0647 (16) 0.705 (2) −0.1138 (9) 0.066 (5)*
H21 0.1904 (15) 0.710 (2) 0.0184 (8) 0.055 (5)*
H22 0.4510 (15) 0.472 (2) 0.0725 (8) 0.057 (5)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0548 (8) 0.0777 (9) 0.0510 (6) −0.0024 (6) 0.0199 (6) 0.0111 (6)
N1 0.0553 (10) 0.0593 (10) 0.0451 (7) −0.0015 (7) 0.0201 (7) −0.0059 (6)
N2 0.0853 (14) 0.0791 (13) 0.0802 (10) −0.0210 (10) 0.0380 (10) −0.0002 (9)
N3 0.0791 (13) 0.0742 (12) 0.0544 (9) −0.0034 (10) 0.0205 (8) 0.0110 (7)
C1 0.0464 (11) 0.0572 (11) 0.0479 (8) −0.0006 (8) 0.0147 (8) 0.0004 (7)
C2 0.0677 (14) 0.0614 (12) 0.0625 (10) −0.0053 (10) 0.0296 (10) −0.0082 (9)
C3 0.0791 (16) 0.0637 (13) 0.0711 (12) −0.0062 (11) 0.0261 (11) −0.0124 (10)
C4 0.0768 (16) 0.0669 (14) 0.0712 (12) −0.0135 (12) 0.0172 (11) 0.0009 (11)
C5 0.0717 (15) 0.0705 (13) 0.0615 (10) −0.0078 (11) 0.0305 (10) −0.0007 (10)
C6 0.0556 (12) 0.0525 (10) 0.0492 (9) 0.0008 (9) 0.0223 (8) −0.0024 (7)
C7 0.0701 (15) 0.0624 (12) 0.0539 (10) −0.0053 (10) 0.0246 (10) 0.0031 (9)
C8 0.0690 (16) 0.0815 (15) 0.0561 (11) −0.0004 (12) 0.0146 (10) 0.0068 (10)
C9 0.0666 (15) 0.0794 (15) 0.0596 (11) −0.0132 (12) 0.0152 (10) 0.0003 (10)
C10 0.0683 (14) 0.0639 (12) 0.0529 (10) −0.0049 (10) 0.0217 (9) 0.0019 (9)
C11 0.0582 (13) 0.0539 (10) 0.0433 (8) 0.0026 (9) 0.0183 (8) 0.0005 (7)
C12 0.0592 (14) 0.0595 (11) 0.0568 (10) −0.0026 (10) 0.0236 (9) 0.0017 (8)
C13 0.0733 (15) 0.0580 (11) 0.0573 (10) −0.0009 (10) 0.0301 (10) 0.0073 (8)
C14 0.0625 (14) 0.0563 (11) 0.0516 (9) 0.0025 (9) 0.0209 (9) 0.0041 (8)
C15 0.0777 (18) 0.0720 (13) 0.0576 (11) 0.0021 (11) 0.0219 (11) 0.0106 (9)
C16 0.0798 (19) 0.1046 (18) 0.0596 (12) −0.0013 (14) 0.0131 (12) 0.0173 (12)
C17 0.0630 (18) 0.119 (2) 0.0697 (13) 0.0006 (14) 0.0104 (11) 0.0228 (12)
C18 0.0620 (15) 0.0829 (14) 0.0636 (11) −0.0025 (11) 0.0214 (10) 0.0088 (10)
C19 0.0585 (14) 0.0518 (10) 0.0526 (9) 0.0029 (9) 0.0196 (8) 0.0003 (8)
C20 0.0554 (13) 0.0495 (10) 0.0484 (8) 0.0016 (8) 0.0215 (8) −0.0003 (7)
C21 0.0542 (12) 0.0591 (11) 0.0475 (9) 0.0053 (9) 0.0217 (8) 0.0007 (8)
C22 0.0566 (13) 0.0551 (11) 0.0480 (9) 0.0021 (9) 0.0222 (8) 0.0009 (8)

Geometric parameters (Å, °)

O1—C11 1.3732 (19) C9—C10 1.389 (3)
O1—C22 1.4492 (19) C9—H9 0.98 (2)
N1—C22 1.419 (2) C10—H10 0.99 (2)
N1—C21 1.483 (2) C11—C20 1.363 (2)
N1—H1 0.97 (2) C11—C12 1.415 (2)
N2—C4 1.331 (3) C12—C13 1.359 (3)
N2—C5 1.332 (2) C12—H12 0.962 (19)
N3—C8 1.328 (3) C13—C14 1.404 (3)
N3—C7 1.342 (2) C13—H13 1.017 (18)
C1—C2 1.374 (2) C14—C15 1.414 (2)
C1—C5 1.381 (2) C14—C19 1.422 (2)
C1—C21 1.522 (2) C15—C16 1.341 (3)
C2—C3 1.384 (3) C15—H15 1.040 (19)
C2—H2 1.017 (17) C16—C17 1.402 (3)
C3—C4 1.365 (3) C16—H16 0.97 (2)
C3—H3 0.95 (2) C17—C18 1.372 (3)
C4—H4 0.98 (2) C17—H17 0.98 (2)
C5—H5 1.002 (19) C18—C19 1.409 (3)
C6—C10 1.374 (2) C18—H18 0.988 (17)
C6—C7 1.378 (2) C19—C20 1.431 (2)
C6—C22 1.512 (2) C20—C21 1.520 (2)
C7—H7 1.02 (2) C21—H21 0.975 (16)
C8—C9 1.368 (3) C22—H22 1.032 (17)
C8—H8 1.03 (2)
C11—O1—C22 113.65 (13) C13—C12—C11 119.1 (2)
C22—N1—C21 111.52 (12) C13—C12—H12 123.7 (10)
C22—N1—H1 109.1 (11) C11—C12—H12 117.2 (10)
C21—N1—H1 113.5 (11) C12—C13—C14 121.13 (17)
C4—N2—C5 116.46 (18) C12—C13—H13 116.8 (11)
C8—N3—C7 116.90 (17) C14—C13—H13 122.0 (10)
C2—C1—C5 116.69 (17) C13—C14—C15 121.03 (17)
C2—C1—C21 124.50 (16) C13—C14—C19 119.30 (15)
C5—C1—C21 118.79 (15) C15—C14—C19 119.65 (19)
C1—C2—C3 119.44 (18) C16—C15—C14 121.3 (2)
C1—C2—H2 119.6 (10) C16—C15—H15 122.1 (11)
C3—C2—H2 120.9 (10) C14—C15—H15 116.6 (11)
C4—C3—C2 119.0 (2) C15—C16—C17 119.8 (2)
C4—C3—H3 121.6 (14) C15—C16—H16 123.2 (14)
C2—C3—H3 119.3 (13) C17—C16—H16 116.9 (14)
N2—C4—C3 123.3 (2) C18—C17—C16 120.6 (2)
N2—C4—H4 116.1 (12) C18—C17—H17 118.8 (13)
C3—C4—H4 120.6 (12) C16—C17—H17 120.5 (12)
N2—C5—C1 125.15 (18) C17—C18—C19 121.2 (2)
N2—C5—H5 117.1 (11) C17—C18—H18 118.3 (10)
C1—C5—H5 117.7 (11) C19—C18—H18 120.5 (10)
C10—C6—C7 117.81 (16) C18—C19—C14 117.29 (16)
C10—C6—C22 123.44 (15) C18—C19—C20 123.26 (16)
C7—C6—C22 118.75 (17) C14—C19—C20 119.45 (17)
N3—C7—C6 124.0 (2) C11—C20—C19 118.07 (14)
N3—C7—H7 114.2 (10) C11—C20—C21 119.66 (14)
C6—C7—H7 121.8 (10) C19—C20—C21 122.23 (17)
N3—C8—C9 123.56 (19) N1—C21—C20 111.47 (15)
N3—C8—H8 117.4 (12) N1—C21—C1 108.81 (14)
C9—C8—H8 119.0 (12) C20—C21—C1 115.12 (13)
C8—C9—C10 118.7 (2) N1—C21—H21 105.9 (9)
C8—C9—H9 121.3 (11) C20—C21—H21 108.8 (9)
C10—C9—H9 120.0 (11) C1—C21—H21 106.2 (10)
C6—C10—C9 119.09 (18) N1—C22—O1 113.38 (14)
C6—C10—H10 121.0 (11) N1—C22—C6 112.33 (12)
C9—C10—H10 119.9 (12) O1—C22—C6 105.59 (14)
C20—C11—O1 123.91 (14) N1—C22—H22 108.7 (9)
C20—C11—C12 122.79 (15) O1—C22—H22 107.5 (8)
O1—C11—C12 113.30 (17) C6—C22—H22 109.2 (9)
C5—C1—C2—C3 −0.3 (3) C13—C14—C19—C18 175.59 (17)
C21—C1—C2—C3 178.03 (18) C15—C14—C19—C18 −2.6 (3)
C1—C2—C3—C4 1.4 (3) C13—C14—C19—C20 −4.4 (2)
C5—N2—C4—C3 0.1 (3) C15—C14—C19—C20 177.40 (16)
C2—C3—C4—N2 −1.3 (3) O1—C11—C20—C19 −178.17 (14)
C4—N2—C5—C1 1.0 (3) C12—C11—C20—C19 2.2 (2)
C2—C1—C5—N2 −0.9 (3) O1—C11—C20—C21 4.2 (2)
C21—C1—C5—N2 −179.35 (18) C12—C11—C20—C21 −175.39 (15)
C8—N3—C7—C6 0.7 (3) C18—C19—C20—C11 −178.01 (17)
C10—C6—C7—N3 −0.6 (3) C14—C19—C20—C11 1.9 (2)
C22—C6—C7—N3 179.19 (17) C18—C19—C20—C21 −0.5 (3)
C7—N3—C8—C9 −0.1 (3) C14—C19—C20—C21 179.47 (16)
N3—C8—C9—C10 −0.6 (3) C22—N1—C21—C20 −41.2 (2)
C7—C6—C10—C9 −0.1 (3) C22—N1—C21—C1 86.79 (17)
C22—C6—C10—C9 −179.90 (17) C11—C20—C21—N1 10.0 (2)
C8—C9—C10—C6 0.7 (3) C19—C20—C21—N1 −167.51 (15)
C22—O1—C11—C20 13.0 (2) C11—C20—C21—C1 −114.56 (18)
C22—O1—C11—C12 −167.37 (14) C19—C20—C21—C1 67.9 (2)
C20—C11—C12—C13 −3.9 (3) C2—C1—C21—N1 −109.53 (19)
O1—C11—C12—C13 176.41 (15) C5—C1—C21—N1 68.8 (2)
C11—C12—C13—C14 1.3 (3) C2—C1—C21—C20 16.4 (3)
C12—C13—C14—C15 −179.09 (18) C5—C1—C21—C20 −165.26 (17)
C12—C13—C14—C19 2.7 (3) C21—N1—C22—O1 61.15 (19)
C13—C14—C15—C16 −176.6 (2) C21—N1—C22—C6 −179.25 (14)
C19—C14—C15—C16 1.6 (3) C11—O1—C22—N1 −46.19 (18)
C14—C15—C16—C17 0.5 (4) C11—O1—C22—C6 −169.58 (13)
C15—C16—C17—C18 −1.6 (4) C10—C6—C22—N1 −111.91 (19)
C16—C17—C18—C19 0.5 (4) C7—C6—C22—N1 68.3 (2)
C17—C18—C19—C14 1.6 (3) C10—C6—C22—O1 12.1 (2)
C17—C18—C19—C20 −178.5 (2) C7—C6—C22—O1 −167.64 (15)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···N3i 0.98 (2) 2.04 (2) 3.009 (2) 170.7 (17)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2043).

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 datablocks I, global. DOI: 10.1107/S1600536808003887/su2043sup1.cif

e-64-0o573-sup1.cif (20.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808003887/su2043Isup2.hkl

e-64-0o573-Isup2.hkl (221.2KB, hkl)

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


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