P. Bisel et al. / Tetrahedron: Asymmetry 9 (1998) 4027–4034
4033
30
[α]D +55.0 and −56.2, respectively. A single recrystallization from cyclohexane yielded (2S)-(+)-6
and (2R)-(−)-6 (435 mg, 56%), respectively: [α]D30 +105.4 (c=1.0, CHCl3) and −106.2 (c=1.0, CHCl3),
respectively.
1H NMR (300 MHz, CDCl3): δ 1.69 (m, 2H, H-5ax, H-3eq), 1.87 (m, 2H, H-4), 2.2 (m, 2H, H-5eq,
H-3ax), 2.54 (m, 1H, H-6eq), 2.70 (ddd, J=13.5, 13.5, 6.5 Hz, 1H, H-6ax), 2.97 (d, Jab=13.5 Hz, 1H,
H-benzyl), 3.14 (d, Jab=13.5 Hz, 1H, H-benzyl), 3.9 (s, 1H, OH), 7.25 (m, 5H, H-arom); 13C NMR (75
MHz, CDCl3): δ 22.7 (t), 27.3 (t), 38.5 (t), 40.3 (t), 43.2 (t), 79.2 (s), 126.9 (d), 128.1 (d), 130.0 (d),
135.3 (s), 213.1 (s).
3.7. (2R,3R,6R)- and (2R,3R,6S)-1,4-Dioxa-6-benzyl-6-hydroxy-2,3-dimethyl-spiro[4,5]-decan ((6R)-7
and (6S)-7)
A solution of 102 mg (0.5 mmol) (−)-(2R)-6 and (+)-(2S)-6, respectively, and 90 mg (1 mmol) (2R,3R)-
2,3-butandiol in 7 ml toluene was refluxed for 14 h in the presence of a catalytic amount of p-TsOH. The
solvent was removed and the residue chromatographed with cyclohexane:ethyl acetate (9:1) to give 119
1
mg (0.033 mmol, 66%) of (6R)-7 and (6S)-7, respectively: mp 86°C; H NMR (300 MHz, CDCl3): δ
1.26 (d, J=6.0 Hz, 3H, CH3), 1.30 (d, J=6.0 Hz, 3H, CH3), 1.3–2.0 (m, 8H, -CH2-), 1.78 (s, 1H, OH),
2.89 (s, 2H, H-benzyl), 3.66 (dq, J=8.5, 6.0 Hz, 1H, H-2), 3.79 (dq, J=8.5, 6.0 Hz, 1H, H-3), 7.25 (m,
5H, H-arom); 13C NMR (75 MHz, CDCl3): δ 16.1 (q), 17.7 (q), 20.3 (t), 22.9 (t), 32.8 (t), 33.4 (t), 39.3
(t), 75.2 (d), 77.9 (d), 79.8 (d), 109.9 (s), 125.4 (d), 127.8 (d), 130.8 (d), 137.2 (s) and, 16.2 (q), 17.7 (q),
20.3 (t), 23.1 (t), 32.4 (t), 32.8 (t), 40.4 (t), 75.3 (d), 78.4 (d), 79.6 (d), 110.1 (s), 126.0 (d), 127.8 (d),
130.9 (d), 137.4 (s), respectively.
3.8. X-Ray structure of (αR,2S)-5
C21H25ON·HCl, Mr=343.90, transparent crystal of size 0.25×0.4×0.6 mm3, orthorhombic, space
group P2,2,2 (No. 19 of IT16). Lattice parameters are a=8.535 (2) Å, b=11.628 (3) Å, c=18.018 (5)
Å and V=1788.2 (8) Å3 (determined from 13 211 reflections, 3°<θ<27°), Z=4, dcalc=1.277 g cm−3 and
µx (MoKα radiation, λ=0.7107 Å)=2.18 cm−1. Intensity data were collected with an image plate detector
system (MarResearch) using MoKα radiation and a graphite monochromator at T=150 K. Data collection
was carried out in the range −9≤h≤9, −14≤k≤14, −22≤l≤22 with (sinθ/λ)max=0.639. The total number
of reflections measured is 13 497, from which 3270 are unique (Rmerged=1.91%, completeness: 94%).
Data were integrated, reduced and scaled using XDS.17 3187 reflections have I(h)>3σ (I(h)) and were
retained for further analysis. The structure was solved by Direct Methods.18 All non-hydrogen atoms
were refined anisotropically using full-matrix least-squares19 based on |F| with weights 1/(σ(|F|)2 +0.1).
H-1 to H-3 were refined isotropically. The positions of all other H atoms were calculated with a C–H
distance of 0.97 Å and a hydrogen displacement parameter of 1.1 times that of the corresponding
C atoms. The shifts (∆/σ)max of the final least-square cycle were smaller than 0.01. R-values were
Rw=0.037 and R=0.028 for refined parameters. Goodness of the fit is 1.51. The final difference Fourier
is featureless (∆ρmin=−0.33, ∆ρmax=0.44 c/Å). The absolute configuration was determined by refining
an enantiomorph sensitive parameter (χ=0.02 (4)) according to Flack,20 including all Friedel related
reflections. Anomalous dispersion corrections were taken from IT Vol. IV, Table 2.3.1.16 The Cl ion is
weakly bound by a hydrogen bridge N1–H1. . .Cl1–N1, the N1–Cl1 distance is 3.118 (1) Å and the bond
angle at the H atom is 171 (2)°.
Under consideration of the measurements errors, all distances and angles are within the expected
values.21