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The crystal structure of tylophorine B (or 2,3,6-tri­methoxy­phen­an­thro­[9,10-f]­indol­izidine) as the benzene solvate, C23H25NO3·­C6H6, has been determined. The compound was isolated from albizzia julibrissin and this is the first definitive report of the steochemistry of tylo­phorine.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270199013499/ta1256sup1.cif
Contains datablocks (I), global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270199013499/ta1256Isup2.hkl
Contains datablock I

CCDC reference: 142749

Comment top

Phenanthroindolizidine (tylophorine) and autofine have been reported to have antitumor and antibiotic effects. We have, for the first time, isolated tylophorine B from albizzia julibrissin in a search for interesting bioactive drugs. The title compound, (I), was extracted from the dried bark of silk trees which grow widely in the northwest of China. In traditional Chinese medicine, tylophorine B is used for pain relief, invigorating the circulation of the blood, treating insomnia and asthma, and the removal of strains. The flowers of silk trees are used to make tea by country folk to treat sore throat.

The MS—IR and NMR data suggest that the structure is consistent with that reported by Li et al. (1989). Although the molecular formulae of some similar and closely related compounds have also been reported (Cave et al., 1989; Mitra et al., 1996; Wadhawan & Sikka, 1976), the three-dimensional structure of tylophorine has not been determined until now.

The structure of tylophorine B (Fig. 1) shows a conjunction of phenanthro and indolizidine moieties. The aromatic rings lie almost in the same plane, with dihedral angles of only 1.7 (2) (A/B), 2.8 (2) (B/C) and 2.2 (2)° (A/C). The observed bond lengths and angles are normal in their alternate single- and double-bond display. The D ring, consisting of atoms C19, C20, C13 and C14, forms a plane with N1 above [0.338 (10) Å] and C15 below [0.325 (12) Å]. The B ring is almost coplanar with ring D. The E ring takes an envelope conformation and makes a dihedral angle of 6.7 (3)° with ring D. The dihedral angle between the B and D rings is 7.3 (2)°.

The benzene molecules are held very loosely in the crystal structure with apparently no strong hydrogen-bond interactions.

Experimental top

The dry bark of albizzia julibrissin (2.3 kg) was powdered and extracted with EtOH (333–343 K) at room temperature. The extract was concentrated and then developed repeatedly by silica-gel chromatography using EtOAc as the developing solvent to yield tylophorine and a number of other known compounds. The dried tylophorine powder is yellow and crystallization in commonly used solvents is difficult. The sample used in this study was recrystallized from a benzene/acetone solution (2:8).

Refinement top

The intensities of higher θ angle reflections were very weak due to both the large thermal motion of benzene and the poor crystal quality. This is also reflected in the R value obtained using all the data. The benzene solvent was treated as a fixed planar hexagon with individual isotropic displacement parameters for the C atoms. Attempts to use anisotropic displacement parameters did not result in a chemically realistic model. The absolute configuration was based on related chemistry.

Computing details top

Data collection: CAD-4 Software (Enraf-Nonius, 1989); cell refinement: CAD-4 Software; data reduction: MolEN/PC (Fair, 1990); program(s) used to solve structure: SHELXS86 (Sheldrick, 1985); program(s) used to refine structure: SHELXL93 (Sheldrick, 1993); molecular graphics: SHELXTL/PC (Siemens, 1995).

Figures top
[Figure 1] Fig. 1. A view of tylophorine B showing the labelling of the non-H atoms. Displacement ellipsoids are shown at 50% probability levels and H atoms are drawn as small circles of arbitrary radii.
2,3,6 trimethoxy phenanthro [9,10:6',7'] indolizedine top
Crystal data top
C23H25NO3·C6H6Z = 1
Mr = 441.55F(000) = 236
Triclinic, P1Dx = 1.273 Mg m3
a = 5.393 (1) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.130 (2) ÅCell parameters from 25 reflections
c = 11.963 (2) Åθ = 10–20°
α = 92.67 (3)°µ = 0.08 mm1
β = 95.02 (3)°T = 293 K
γ = 100.45 (3)°Block, pale yellow
V = 575.8 (2) Å30.5 × 0.4 × 0.3 mm
Data collection top
Enraf-Nonius CAD-4
diffractometer
θmax = 27.8°, θmin = 1.7°
Radiation source: fine-focus sealed tubeh = 06
Graphite monochromatork = 1111
θ/2θ scansl = 1414
2510 measured reflections3 standard reflections every 60 min
2510 independent reflections intensity decay: <0.1%
1992 reflections with I > 2σ(I)
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.062Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.193H-atom parameters constrained
S = 1.13Calculated w = 1/[σ2(Fo2) + (0.1522P)2 + 0.0106P]
where P = (Fo2 + 2Fc2)/3
2510 reflections(Δ/σ)max = 0.028
281 parametersΔρmax = 0.48 e Å3
3 restraintsΔρmin = 0.36 e Å3
Crystal data top
C23H25NO3·C6H6γ = 100.45 (3)°
Mr = 441.55V = 575.8 (2) Å3
Triclinic, P1Z = 1
a = 5.393 (1) ÅMo Kα radiation
b = 9.130 (2) ŵ = 0.08 mm1
c = 11.963 (2) ÅT = 293 K
α = 92.67 (3)°0.5 × 0.4 × 0.3 mm
β = 95.02 (3)°
Data collection top
Enraf-Nonius CAD-4
diffractometer
1992 reflections with I > 2σ(I)
2510 measured reflections3 standard reflections every 60 min
2510 independent reflections intensity decay: <0.1%
Refinement top
R[F2 > 2σ(F2)] = 0.0623 restraints
wR(F2) = 0.193H-atom parameters constrained
S = 1.13Δρmax = 0.48 e Å3
2510 reflectionsΔρmin = 0.36 e Å3
281 parameters
Special details top

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) top
xyzUiso*/Ueq
O10.0884 (6)0.9618 (4)0.2243 (2)0.0576 (8)
O20.3198 (6)0.8107 (3)0.1176 (2)0.0537 (8)
O30.4947 (6)0.8094 (4)0.4897 (3)0.0570 (8)
N10.6663 (6)1.4005 (3)0.2286 (3)0.0389 (7)
C10.1242 (6)1.0782 (4)0.3012 (3)0.0361 (8)
C20.0864 (7)1.0732 (5)0.4199 (3)0.0440 (9)
H20.20871.13820.47330.042 (11)*
C30.1181 (8)0.9848 (5)0.4798 (3)0.0484 (10)
H30.12380.97070.55630.037 (10)*
C40.2998 (7)0.8934 (4)0.4224 (3)0.0425 (9)
C50.2660 (7)0.8914 (4)0.3081 (3)0.0413 (9)
H50.37540.83280.27870.028 (9)*
C60.0535 (7)0.9817 (4)0.2456 (3)0.0343 (8)
C70.0160 (6)0.9817 (4)0.1238 (3)0.0361 (8)
C80.1953 (7)0.8936 (4)0.0623 (3)0.0386 (9)
H80.33420.83230.11180.056 (13)*
C90.1579 (7)0.8929 (4)0.0520 (3)0.0413 (9)
C100.0664 (7)0.9794 (4)0.1118 (3)0.0391 (9)
C110.2314 (7)1.0672 (4)0.0527 (3)0.0402 (9)
H110.37171.13900.10930.078 (17)*
C120.1976 (6)1.0718 (4)0.0656 (3)0.0341 (8)
C130.3750 (7)1.1698 (4)0.1244 (3)0.0356 (8)
C140.6031 (7)1.2683 (4)0.0584 (3)0.0376 (8)
H14B0.54321.35940.00030.041 (10)*
H14A0.66821.22070.00030.044 (11)*
C150.7922 (6)1.3379 (4)0.1342 (3)0.0380 (8)
H150.89941.26830.15740.090 (19)*
C160.9925 (7)1.4726 (4)0.0826 (4)0.0468 (10)
H16B0.91651.52720.02910.031 (9)*
H16A1.12551.41590.02910.068 (14)*
C171.0685 (8)1.5581 (5)0.1848 (5)0.0561 (11)
H17B1.25151.52670.19430.042 (10)*
H17A1.04251.66540.16700.083 (17)*
C180.8754 (8)1.4872 (5)0.2824 (4)0.0506 (10)
H18B0.95561.41510.33490.085 (18)*
H18A0.83061.55380.33490.048 (11)*
C190.5085 (7)1.2830 (5)0.3023 (4)0.0431 (9)
H19B0.41751.33160.36140.043 (10)*
H19A0.58361.22030.36140.069 (15)*
C200.3342 (6)1.1751 (4)0.2383 (3)0.0341 (8)
C210.3250 (10)1.0213 (8)0.2835 (4)0.0719 (15)
H21C0.49920.97070.24980.073 (15)*
H21B0.33121.02730.35920.11 (2)*
H21A0.34941.12520.26970.17 (5)*
C220.5297 (9)0.7136 (5)0.0623 (4)0.0580 (12)
H22C0.62320.75030.00020.09 (2)*
H22B0.49820.63900.00020.079 (17)*
H22A0.62930.65960.11330.13 (3)*
C230.6888 (9)0.7183 (6)0.4352 (5)0.0604 (12)
H23C0.58710.63800.39100.058 (13)*
H23B0.79610.77670.39100.076 (17)*
H23A0.83710.69270.47310.071 (16)*
C240.9273 (12)0.3092 (5)0.3246 (5)0.120 (3)*
H240.98190.21830.32490.144*
C250.7650 (12)0.3429 (6)0.4021 (5)0.102 (2)*
H250.71110.27450.45420.123*
C260.6834 (10)0.4788 (6)0.4017 (4)0.108 (2)*
H260.57490.50140.45360.130*
C270.7640 (11)0.5811 (5)0.3239 (5)0.108 (2)*
H270.70940.67200.32360.130*
C280.9263 (13)0.5474 (6)0.2464 (5)0.128 (3)*
H280.98020.61580.19430.153*
C291.0079 (12)0.4115 (7)0.2468 (5)0.134 (3)*
H291.11650.38900.19490.160*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0506 (17)0.0754 (19)0.0402 (14)0.0072 (15)0.0018 (13)0.0164 (13)
O20.0478 (17)0.0615 (18)0.0478 (15)0.0077 (14)0.0129 (13)0.0175 (13)
O30.0468 (16)0.067 (2)0.0481 (15)0.0104 (14)0.0036 (13)0.0069 (13)
N10.0283 (14)0.0322 (14)0.0572 (17)0.0037 (11)0.0082 (13)0.0124 (12)
C10.0318 (19)0.0352 (17)0.0423 (19)0.0054 (15)0.0092 (15)0.0069 (14)
C20.041 (2)0.050 (2)0.0407 (19)0.0034 (17)0.0096 (16)0.0051 (15)
C30.054 (2)0.052 (2)0.0355 (17)0.0023 (19)0.0069 (17)0.0083 (16)
C40.037 (2)0.045 (2)0.0429 (19)0.0034 (17)0.0010 (16)0.0004 (16)
C50.039 (2)0.0389 (19)0.0445 (19)0.0011 (17)0.0075 (16)0.0108 (15)
C60.0315 (18)0.0331 (17)0.0382 (16)0.0055 (14)0.0040 (14)0.0026 (13)
C70.0323 (19)0.0339 (18)0.0443 (19)0.0069 (15)0.0095 (16)0.0130 (14)
C80.0343 (19)0.0356 (18)0.044 (2)0.0003 (16)0.0074 (16)0.0066 (15)
C90.038 (2)0.0362 (18)0.049 (2)0.0008 (16)0.0136 (17)0.0107 (15)
C100.0331 (18)0.045 (2)0.0379 (18)0.0035 (16)0.0001 (15)0.0062 (15)
C110.0335 (19)0.0397 (19)0.0430 (19)0.0029 (16)0.0002 (16)0.0029 (15)
C120.0265 (17)0.0343 (17)0.0412 (18)0.0056 (15)0.0012 (15)0.0034 (14)
C130.0320 (19)0.0300 (16)0.0451 (19)0.0043 (15)0.0072 (15)0.0056 (14)
C140.0267 (17)0.0415 (18)0.0427 (19)0.0016 (15)0.0005 (15)0.0064 (14)
C150.0274 (17)0.0333 (16)0.0515 (19)0.0010 (14)0.0028 (15)0.0050 (14)
C160.0281 (17)0.0402 (19)0.067 (2)0.0067 (15)0.0026 (17)0.0060 (18)
C170.041 (2)0.041 (2)0.085 (3)0.0027 (17)0.015 (2)0.014 (2)
C180.041 (2)0.045 (2)0.063 (2)0.0044 (18)0.0109 (18)0.0150 (18)
C190.0353 (19)0.046 (2)0.0479 (19)0.0009 (16)0.0121 (16)0.0124 (15)
C200.0259 (16)0.0310 (16)0.0445 (18)0.0015 (14)0.0062 (14)0.0039 (14)
C210.062 (3)0.104 (4)0.043 (2)0.001 (3)0.003 (2)0.002 (2)
C220.049 (2)0.054 (2)0.066 (3)0.013 (2)0.015 (2)0.016 (2)
C230.042 (2)0.058 (2)0.071 (3)0.013 (2)0.004 (2)0.004 (2)
Geometric parameters (Å, º) top
O1—C101.361 (5)C8—C91.365 (6)
O1—C211.407 (5)C9—C101.431 (5)
O2—C91.370 (4)C10—C111.356 (6)
O2—C221.399 (5)C11—C121.415 (5)
O3—C41.357 (5)C12—C131.441 (5)
O3—C231.437 (5)C13—C201.366 (5)
N1—C191.450 (5)C13—C141.520 (5)
N1—C151.459 (5)C14—C151.499 (5)
N1—C181.470 (5)C15—C161.547 (5)
C1—C61.414 (5)C16—C171.528 (6)
C1—C21.414 (5)C17—C181.529 (7)
C1—C201.434 (5)C19—C201.516 (5)
C2—C31.366 (6)C24—C251.3900
C3—C41.415 (5)C24—C291.3900
C4—C51.364 (6)C25—C261.3900
C5—C61.415 (5)C26—C271.3900
C6—C71.453 (5)C27—C281.3900
C7—C121.397 (5)C28—C291.3900
C7—C81.422 (5)
C10—O1—C21116.6 (3)C11—C10—C9118.3 (3)
C9—O2—C22117.2 (3)O1—C10—C9114.4 (3)
C4—O3—C23117.1 (3)C10—C11—C12123.0 (3)
C19—N1—C15110.7 (3)C7—C12—C11118.3 (3)
C19—N1—C18113.8 (3)C7—C12—C13120.7 (3)
C15—N1—C18104.2 (3)C11—C12—C13121.0 (3)
C6—C1—C2117.2 (3)C20—C13—C12119.8 (3)
C6—C1—C20120.5 (3)C20—C13—C14120.7 (3)
C2—C1—C20122.3 (3)C12—C13—C14119.4 (3)
C3—C2—C1122.4 (4)C15—C14—C13111.7 (3)
C2—C3—C4119.6 (3)N1—C15—C14110.7 (3)
O3—C4—C5125.3 (4)N1—C15—C16102.7 (3)
O3—C4—C3114.9 (3)C14—C15—C16116.5 (3)
C5—C4—C3119.8 (3)C17—C16—C15103.3 (3)
C4—C5—C6120.9 (3)C16—C17—C18105.5 (3)
C5—C6—C1120.0 (3)N1—C18—C17104.8 (3)
C5—C6—C7121.6 (3)N1—C19—C20112.2 (3)
C1—C6—C7118.4 (3)C13—C20—C1120.8 (3)
C12—C7—C8119.2 (3)C13—C20—C19121.3 (3)
C12—C7—C6119.6 (3)C1—C20—C19117.9 (3)
C8—C7—C6121.2 (3)C25—C24—C29120.0
C9—C8—C7121.0 (3)C26—C25—C24120.0
O2—C9—C8124.8 (4)C27—C26—C25120.0
O2—C9—C10115.0 (3)C26—C27—C28120.0
C8—C9—C10120.2 (3)C29—C28—C27120.0
C11—C10—O1127.4 (3)C28—C29—C24120.0

Experimental details

Crystal data
Chemical formulaC23H25NO3·C6H6
Mr441.55
Crystal system, space groupTriclinic, P1
Temperature (K)293
a, b, c (Å)5.393 (1), 9.130 (2), 11.963 (2)
α, β, γ (°)92.67 (3), 95.02 (3), 100.45 (3)
V3)575.8 (2)
Z1
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.5 × 0.4 × 0.3
Data collection
DiffractometerEnraf-Nonius CAD-4
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
2510, 2510, 1992
Rint?
(sin θ/λ)max1)0.656
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.062, 0.193, 1.13
No. of reflections2510
No. of parameters281
No. of restraints3
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.48, 0.36

Computer programs: CAD-4 Software (Enraf-Nonius, 1989), CAD-4 Software, MolEN/PC (Fair, 1990), SHELXS86 (Sheldrick, 1985), SHELXL93 (Sheldrick, 1993), SHELXTL/PC (Siemens, 1995).

 

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