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The structure of methyl (6R)-6-(3'[beta]-acetoxy-5'-androsten-17'[beta]-yl)-2-phenyl-5,6-dihydro-4H-[1,3]oxazine, C31H41NO3, synthesized from an azidopregnene derivative, is reported. The di­hydro-1,3-oxazine ring is connected in the [beta] position to the sterane skeleton at C-17'. An R configuration was found at C-6.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100009628/qa0336sup1.cif
Contains datablocks global, I

sft

Structure factor file (SHELXL table format) https://doi.org/10.1107/S0108270100009628/qa0336Isup2.sft
Supplementary material

CCDC reference: 150402

Comment top

Over the last few decades, increasing attention has been paid to the synthesis of cardenolide and bufadienolide analogues which are expected to have better therapeutic indices (Megges et al., 1978) than the natural glycosteroids. Extensive investigations have shown that for cardiotonic activity, the presence of the 17β side chain containing cN double-bond moieties is more important than the presence of the unsaturated lactone ring (Thomas et al., 1974; Shiao, 1982; Wicha & Masnyk, 1985a,b). Paryzek & Blaszczyk (1999) recently published a novel approach to the synthesis of the butenolide ring of cardenolides.

3β-Acetoxy-5-pregnen-20-one with methyl formate in the presence of sodium methylate gave 3β-hydroxy-21-hydroxymethylene-5-pregnen-20-one. The reduction of this product with sodium borohydride yielded a trihydroxy compound. This was acetylated, and after selective deacetylation on alumina, we obtained the 21-hydroxymethyl derivative. The selective functionalization of the side chain produced the 21-azidomethyl-20-hydroxy compound. This steroid was treated under Schmidt reaction conditions (Bach & Wolber, 1982) with benzaldehyde in the presence of boron trifluoride diethyl etherate yielding the title compound, (I). The reaction sequence will be published elsewhere (Wölfling et al., 2000).

The crystal structure of (I) shows that the C atom attached to C-17' (C-6) has an R configuration, i.e. the reduction of the C-20 carbonyl of the basic steroid – according to earlier observations (Hirsch & Fujimoto, 1970; Fieser & Fieser, 1959) – ran stereoselectively. The B/C and the C/D ring fusions are trans. Rings A and C adopt chair conformations, while ring B shows a distorted half-chair conformation. Ring D and the 1,3-oxazine ring display slightly distorted half-chair conformations. The sterane skeleton is an equatorial substituent of the 1,3-oxazine ring. The phenyl ring lies nearly in the plane, determined by atoms O20, C70 and N. The total puckering amplitudes (Cremer & Pople, 1975) of the A, B, C, D, 1,3-oxazine and phenyl rings are Q = 0.552, 0.467, 0.573, 0.469, 0.462 and 0.002 Å, respectively.

Crystal structures of some other androstene derivatives have been reported: androst-8-ene (Drouin et al., 1991), androst-9(10)-ene (Ginderow et al., 1993) and androst-4-ene (Anthony et al., 1999). Compounds with the androst-5-ene skeleton were studied, among others, by Cox et al. (1990), Stankovic et al. (1994) and Lazar et al. (1998).

Experimental top

The starting material of our reaction sequence (5-pregnen-3β-ol-20-one) was obtained from the Sigma Chemical Co. (St. Louis, MO).

Refinement top

All starting positions of the H atoms were generated with idealized coordinates using SHELXL97 (Sheldrick, 1997). The CH3 groups were generated with idealized tetrahedral angles and after a structure-factor calculation, the torsion angle of the CH3 group was adjusted to maximize the sum of the electron density at the three calculated H-atom positions. All non-H atoms were refined anisotropically. The H atoms were refined using a riding model and their isotropic displacement parameters were constrained to be 1.2 times (1.5 times for CH3 groups) the equivalent displacement parameters of their parent atom. CH3 groups were also allowed to rotate around the C—X bond. Floating-origin restraints were generated automatically by SHELXL97, according to the method of Flack & Schwarzenbach (1988). The refinement was carried out against data with Friedel pairs merged.

Computing details top

Data collection: SMART (Bruker 1998); cell refinement: SAINT (Bruker 1998); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); software used to prepare material for publication: SHELXTL.

(6R)-6-(3'β-acetoxy-5'-androsten-17'β-yl)-2-phenyl- 5,6-dihydro-4H-[1,3]oxazine top
Crystal data top
C31H41NO3Dx = 1.202 Mg m3
Mr = 475.65Melting point = 183–186 K
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 9.438 (2) ÅCell parameters from 8192 reflections
b = 8.529 (2) Åθ = 2.4–25.0°
c = 16.503 (3) ŵ = 0.08 mm1
β = 98.38 (3)°T = 133 K
V = 1314.3 (5) Å3Block, colourless
Z = 20.48 × 0.48 × 0.25 mm
F(000) = 516
Data collection top
STOE-Siemens-Huber four circle
diffractometer
2416 independent reflections
Radiation source: fine-focus sealed tube2177 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.049
Detector resolution: 8.192 pixels mm-1 pixels mm-1θmax = 25.0°, θmin = 2.4°
ϕ and ω scansh = 1110
Absorption correction: semi-empirical (using intensity measurements)
(SADABS; Sheldrick, 1999)
k = 010
Tmin = 0.964, Tmax = 0.981l = 019
14574 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.035H-atom parameters constrained
wR(F2) = 0.083 w = 1/[σ2(Fo2) + (0.0458P)2 + 0.2578P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
2416 reflectionsΔρmax = 0.17 e Å3
316 parametersΔρmin = 0.14 e Å3
1 restraintExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.015 (2)
Crystal data top
C31H41NO3V = 1314.3 (5) Å3
Mr = 475.65Z = 2
Monoclinic, P21Mo Kα radiation
a = 9.438 (2) ŵ = 0.08 mm1
b = 8.529 (2) ÅT = 133 K
c = 16.503 (3) Å0.48 × 0.48 × 0.25 mm
β = 98.38 (3)°
Data collection top
STOE-Siemens-Huber four circle
diffractometer
2416 independent reflections
Absorption correction: semi-empirical (using intensity measurements)
(SADABS; Sheldrick, 1999)
2177 reflections with I > 2σ(I)
Tmin = 0.964, Tmax = 0.981Rint = 0.049
14574 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0351 restraint
wR(F2) = 0.083H-atom parameters constrained
S = 1.08Δρmax = 0.17 e Å3
2416 reflectionsΔρmin = 0.14 e Å3
316 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*/UeqOcc. (<1)
C700.7192 (3)0.4472 (3)0.08344 (15)0.0286 (6)*
O200.59838 (17)0.4167 (2)0.11841 (10)0.0258 (4)
N0.7778 (2)0.3579 (3)0.03618 (13)0.0339 (6)
C560.8996 (3)0.6564 (4)0.07191 (16)0.0359 (7)
H560.94550.58690.03900.043*
C510.7775 (3)0.6058 (3)0.10421 (14)0.0268 (6)
C200.5544 (3)0.2527 (3)0.11728 (15)0.0261 (6)
H200.62220.19300.15830.031*
C520.7129 (3)0.7101 (3)0.15241 (14)0.0268 (6)
H520.63040.67850.17500.032*
C540.8882 (3)0.9072 (4)0.13517 (15)0.0334 (6)
H540.92561.00970.14580.040*
C550.9536 (3)0.8054 (4)0.08726 (17)0.0382 (7)
H551.03590.83800.06480.046*
C530.7680 (3)0.8599 (3)0.16783 (15)0.0300 (6)
H530.72320.93010.20090.036*
C220.7098 (3)0.2108 (4)0.00949 (16)0.0359 (7)
H22A0.77210.12400.03320.043*
H22B0.70310.20410.05080.043*
C210.5610 (3)0.1867 (3)0.03245 (15)0.0335 (6)
H21A0.48920.23980.00800.040*
H21B0.53820.07330.03160.040*
O30.33413 (17)0.7318 (2)0.43649 (10)0.0278 (4)
C50.0646 (3)0.4429 (3)0.37972 (15)0.0271 (6)
C150.2669 (3)0.0691 (3)0.22244 (16)0.0288 (6)
H15A0.17880.00670.20660.035*
H15B0.31910.02740.27430.035*
C80.1630 (2)0.2993 (3)0.30338 (14)0.0235 (6)
H80.22930.27840.35520.028*
C170.4048 (3)0.2420 (3)0.14046 (14)0.0257 (6)
H170.33670.28340.09320.031*
C30.2273 (2)0.6689 (3)0.38872 (15)0.0255 (6)
H30.27320.65050.33100.031*
C100.0616 (3)0.5470 (3)0.36497 (15)0.0235 (5)
C110.2711 (3)0.5674 (3)0.28079 (17)0.0309 (6)
H11A0.24720.67940.27080.037*
H11B0.34230.56060.33110.037*
O100.4280 (2)0.8770 (3)0.32815 (12)0.0487 (6)
C90.1343 (3)0.4778 (3)0.29465 (15)0.0226 (5)
H90.06450.49160.24340.027*
C40.1747 (3)0.5147 (3)0.42715 (15)0.0278 (6)
H4A0.25640.44190.42690.033*
H4B0.13120.53220.48470.033*
C60.0776 (3)0.2949 (3)0.35502 (16)0.0290 (6)
H60.15560.23640.36990.035*
C600.4264 (3)0.8371 (3)0.39826 (15)0.0296 (6)
C140.2320 (2)0.2434 (3)0.23029 (15)0.0235 (5)
H140.16180.26920.18070.028*
C20.1030 (3)0.7819 (3)0.38934 (16)0.0280 (6)
H2A0.05620.79940.44630.034*
H2B0.13830.88400.36610.034*
C800.5268 (3)0.8983 (4)0.45336 (17)0.0364 (7)
H810.53710.82030.49570.055*0.68 (3)
H820.62060.91880.42110.055*0.68 (3)
H830.48840.99570.47930.055*0.68 (3)
H840.56041.00150.43580.055*0.32 (3)
H850.47820.90460.50890.055*0.32 (3)
H860.60820.82910.45190.055*0.32 (3)
C190.1658 (3)0.5600 (3)0.44587 (15)0.0316 (6)
H19A0.21090.45800.45930.047*
H19B0.11290.59240.48990.047*
H19C0.23980.63790.43970.047*
C70.0210 (3)0.2128 (3)0.30549 (17)0.0313 (6)
H7A0.02840.20020.24870.038*
H7B0.04190.10670.32850.038*
C130.3722 (2)0.3282 (3)0.21826 (14)0.0239 (6)
C160.3628 (3)0.0681 (3)0.15367 (16)0.0314 (6)
H16A0.30970.02410.10260.038*
H16B0.44950.00380.17010.038*
C10.0050 (3)0.7128 (3)0.33843 (15)0.0269 (6)
H1A0.08760.78500.34130.032*
H1B0.04050.70780.28050.032*
C180.4940 (3)0.3005 (3)0.28983 (14)0.0282 (6)
H18A0.57840.36110.28070.042*
H18B0.51820.18870.29310.042*
H18C0.46280.33400.34120.042*
C120.3379 (3)0.5028 (3)0.20834 (16)0.0304 (6)
H12A0.27070.51930.15710.036*
H12B0.42700.56120.20370.036*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O200.0251 (9)0.0265 (10)0.0282 (9)0.0006 (8)0.0123 (7)0.0017 (8)
N0.0375 (13)0.0369 (14)0.0304 (11)0.0010 (11)0.0152 (10)0.0070 (10)
C560.0333 (15)0.0424 (17)0.0348 (14)0.0017 (14)0.0138 (12)0.0063 (13)
C510.0230 (13)0.0358 (16)0.0221 (12)0.0005 (11)0.0054 (10)0.0009 (11)
C200.0275 (13)0.0237 (15)0.0278 (12)0.0002 (11)0.0060 (10)0.0026 (11)
C520.0227 (12)0.0354 (16)0.0224 (11)0.0018 (12)0.0036 (10)0.0013 (11)
C540.0341 (15)0.0332 (16)0.0330 (14)0.0055 (13)0.0049 (11)0.0027 (13)
C550.0357 (16)0.0426 (18)0.0392 (15)0.0085 (14)0.0152 (12)0.0007 (14)
C530.0293 (14)0.0304 (16)0.0299 (13)0.0035 (12)0.0032 (11)0.0031 (11)
C220.0437 (16)0.0350 (17)0.0315 (13)0.0037 (13)0.0139 (12)0.0058 (12)
C210.0389 (15)0.0324 (17)0.0306 (13)0.0017 (13)0.0098 (11)0.0072 (12)
O30.0235 (8)0.0316 (10)0.0303 (9)0.0029 (8)0.0103 (7)0.0009 (8)
C50.0216 (13)0.0258 (16)0.0353 (14)0.0002 (11)0.0085 (11)0.0069 (12)
C150.0241 (14)0.0274 (15)0.0357 (14)0.0020 (12)0.0066 (11)0.0028 (12)
C80.0198 (12)0.0211 (13)0.0300 (13)0.0002 (11)0.0053 (10)0.0009 (11)
C170.0240 (12)0.0276 (14)0.0253 (12)0.0021 (12)0.0024 (10)0.0020 (11)
C30.0205 (12)0.0305 (15)0.0270 (12)0.0040 (12)0.0092 (10)0.0004 (12)
C100.0210 (12)0.0216 (14)0.0287 (12)0.0003 (11)0.0064 (10)0.0009 (11)
C110.0298 (14)0.0196 (14)0.0474 (16)0.0018 (12)0.0192 (12)0.0001 (12)
O100.0466 (12)0.0621 (16)0.0410 (11)0.0260 (12)0.0186 (9)0.0174 (11)
C90.0194 (12)0.0206 (14)0.0282 (12)0.0007 (10)0.0047 (10)0.0023 (10)
C40.0270 (14)0.0243 (14)0.0337 (14)0.0031 (11)0.0103 (11)0.0036 (11)
C60.0253 (13)0.0272 (15)0.0366 (14)0.0052 (12)0.0117 (11)0.0016 (12)
C600.0240 (13)0.0310 (15)0.0345 (14)0.0036 (12)0.0065 (11)0.0000 (12)
C140.0195 (12)0.0241 (14)0.0267 (12)0.0006 (11)0.0030 (9)0.0021 (11)
C20.0265 (13)0.0219 (14)0.0371 (14)0.0029 (11)0.0096 (11)0.0032 (11)
C800.0273 (14)0.0401 (17)0.0427 (15)0.0059 (13)0.0086 (11)0.0070 (14)
C190.0262 (13)0.0378 (16)0.0313 (13)0.0001 (13)0.0055 (11)0.0002 (12)
C70.0279 (13)0.0230 (15)0.0458 (15)0.0048 (12)0.0145 (12)0.0037 (12)
C130.0203 (12)0.0251 (14)0.0274 (12)0.0001 (11)0.0067 (10)0.0006 (11)
C160.0300 (14)0.0284 (15)0.0363 (14)0.0018 (12)0.0071 (11)0.0070 (12)
C10.0249 (12)0.0226 (14)0.0353 (13)0.0016 (11)0.0110 (11)0.0044 (11)
C180.0239 (13)0.0321 (15)0.0294 (12)0.0031 (11)0.0061 (10)0.0053 (11)
C120.0319 (14)0.0242 (15)0.0387 (15)0.0020 (11)0.0173 (12)0.0045 (12)
Geometric parameters (Å, º) top
C70—N1.273 (3)C15—C161.551 (3)
C70—O201.375 (3)C8—C141.528 (3)
C70—C511.482 (4)C8—C71.535 (3)
O20—C201.459 (3)C8—C91.550 (3)
N—C221.448 (4)C17—C131.549 (3)
C56—C551.379 (4)C17—C161.559 (4)
C56—C511.406 (4)C3—C41.512 (4)
C51—C521.391 (3)C3—C21.517 (4)
C20—C171.519 (3)C10—C191.542 (3)
C20—C211.519 (3)C10—C91.549 (3)
C52—C531.389 (4)C10—C11.552 (4)
C54—C551.379 (4)C11—C121.533 (3)
C54—C531.385 (4)C11—C91.546 (3)
C22—C211.521 (4)O10—C601.204 (3)
O3—C601.343 (3)C6—C71.499 (4)
O3—C31.469 (3)C60—C801.499 (3)
C5—C61.327 (4)C14—C131.546 (3)
C5—C41.518 (3)C2—C11.530 (3)
C5—C101.533 (3)C13—C121.527 (4)
C15—C141.532 (4)C13—C181.542 (3)
N—C70—O20127.2 (2)C4—C3—C2110.1 (2)
N—C70—C51120.5 (2)C5—C10—C19108.4 (2)
O20—C70—C51112.2 (2)C5—C10—C9109.7 (2)
C70—O20—C20115.31 (19)C19—C10—C9112.3 (2)
C70—N—C22119.4 (2)C5—C10—C1109.2 (2)
C55—C56—C51120.9 (3)C19—C10—C1109.2 (2)
C52—C51—C56118.2 (3)C9—C10—C1107.91 (19)
C52—C51—C70122.5 (2)C12—C11—C9112.6 (2)
C56—C51—C70119.3 (2)C11—C9—C10113.2 (2)
O20—C20—C17109.1 (2)C11—C9—C8111.1 (2)
O20—C20—C21108.5 (2)C10—C9—C8113.3 (2)
C17—C20—C21112.0 (2)C3—C4—C5110.0 (2)
C53—C52—C51120.6 (2)C5—C6—C7125.1 (2)
C55—C54—C53120.0 (3)O10—C60—O3123.8 (2)
C54—C55—C56120.1 (3)O10—C60—C80124.4 (3)
C54—C53—C52120.2 (3)O3—C60—C80111.8 (2)
N—C22—C21115.2 (2)C8—C14—C15119.4 (2)
C20—C21—C22110.1 (2)C8—C14—C13115.2 (2)
C60—O3—C3116.18 (18)C15—C14—C13104.2 (2)
C6—C5—C4120.2 (2)C3—C2—C1109.1 (2)
C6—C5—C10122.8 (2)C6—C7—C8113.7 (2)
C4—C5—C10117.0 (2)C12—C13—C18110.8 (2)
C14—C15—C16102.9 (2)C12—C13—C14107.4 (2)
C14—C8—C7110.0 (2)C18—C13—C14112.7 (2)
C14—C8—C9108.8 (2)C12—C13—C17116.0 (2)
C7—C8—C9109.5 (2)C18—C13—C17110.3 (2)
C20—C17—C13119.0 (2)C14—C13—C1799.28 (19)
C20—C17—C16110.9 (2)C15—C16—C17106.5 (2)
C13—C17—C16104.5 (2)C2—C1—C10115.2 (2)
O3—C3—C4107.57 (19)C13—C12—C11111.8 (2)
O3—C3—C2110.8 (2)

Experimental details

Crystal data
Chemical formulaC31H41NO3
Mr475.65
Crystal system, space groupMonoclinic, P21
Temperature (K)133
a, b, c (Å)9.438 (2), 8.529 (2), 16.503 (3)
β (°) 98.38 (3)
V3)1314.3 (5)
Z2
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.48 × 0.48 × 0.25
Data collection
DiffractometerSTOE-Siemens-Huber four circle
diffractometer
Absorption correctionSemi-empirical (using intensity measurements)
(SADABS; Sheldrick, 1999)
Tmin, Tmax0.964, 0.981
No. of measured, independent and
observed [I > 2σ(I)] reflections
14574, 2416, 2177
Rint0.049
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.035, 0.083, 1.08
No. of reflections2416
No. of parameters316
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.17, 0.14

Computer programs: SMART (Bruker 1998), SAINT (Bruker 1998), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL.

 

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