J. Ba´lint et al. / Tetrahedron: Asymmetry 12 (2001) 1511–1518
1517
bined organic phase was dried over Na2SO4 and the
solvent was evaporated, yielding (S)-1-phenylethyl-
amine as an oil (0.18 g), [h]2D0=−19.8 (c 10, ethanol).
crystal decay of 3% (the data were corrected for decay).
A total of 6873 reflections were collected of which 5975
were unique [Rint=0.0231, R(|)=0.0539]; intensities of
3386 reflections were greater than 2|(I). Completeness
to 2q=0.998. An empirical absorption correction was
applied to the data (the minimum and maximum trans-
mission factors were 0.934 and 1.00). The structure was
solved by direct methods. Anisotropic full-matrix least-
squares refinement on F2 for all non-hydrogen atoms
yielded R1=0.0473 and wR2=0.1113 for 3386 [I>2|(I)]
and R1=0.0937 and wR2=0.1212 for all (5975) inten-
sity data (goodness-of fit=0.941; the maximum and
mean shift/e.s.d. 0.002 and 0.000). The maximum and
3.6. X-Ray crystallography
Single crystals were obtained from their optically pure
components by crystallization from acetone.
Compound 1a. Crystal data: C18H22N2O3, Fw 314.38,
colorless block, size: 0.40×0.35×0.15 mm, monoclinic,
space group P21, a=9.869(1), b=6.750(1), c=13.548(1)
3
,
,
A, i=101.38(1)°, V=884.77(17) A , T=566(2) K, Z=
2, F(000)=336, Dcalcd=1.180 Mg m−3, v=0.081 mm−1.
A crystal of 1a was mounted on a glass fiber. Cell
parameters were determined by least-squares of the
setting angles of 25 (14.595q516.70°) reflections.
Intensity data were collected on an Enraf–Nonius
CAD4 diffractometer (graphite monochromator; Mo
minimum residual electron density in the final differ-
−3
,
ence map was 0.224 and −0.133 e A . Hydrogen
atomic positions were calculated from assumed
geometries. Hydrogen atoms were included in structure-
factor calculations but they were not refined. The
isotropic displacement parameters of the hydrogen
atoms were approximated from the U(eq.) value of the
atom they were bonded to.
,
Ka radiation, u=0.710730 A) at 293(2) K in the range
2.355q531.97° using ꢀ–2q scans. The scan width was
0.54+0.54tg(q)° in ꢀ. Backgrounds were measured 1/2
the total time of the peak scans. The intensities of three
standard reflections were monitored regularly (every 60
min). The intensities of the standard reflections indi-
cated a crystal decay of 8% (the data were corrected for
decay). A total of 6973 reflections15 were collected of
which 6117 were unique [Rint=0.0110, R(|)=0.0402];
intensities of 3576 reflections were greater than 2|(I).
Completeness to 2q=0.998. Empirical absorption
correction16 was applied. The structure was solved by
direct methods17 and subsequent difference syntheses.
Anisotropic full-matrix least-squares refinement18 on F2
for all non-hydrogen atoms yielded R1=0.0411 and
wR2=0.1042 for 3576 [I>2|(I)] and R1=0.0843 and
wR2=0.1126 for all (6117) intensity data (goodness-of-
fit=0.977; the maximum and mean shift/e.s.d. 0.000
and 0.000; extinction coefficient=0.013(5)). The maxi-
Acknowledgements
The Hungarian OTKA Foundation (Project No.
T29251) is gratefully acknowledged for financial sup-
port. J.B. and G.E. would like to thank the OTKA
(D32705 and D 29445, respectively) for Postdoctoral
Fellowships. M.C. would also like to thank the OTKA
(T25910) for partial support with the X-ray crystallog-
raphy measurements.
References
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´
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time of the peak scans. The intensities of 3 standard
reflections were monitored regularly (every 60 min).
The intensities of the standard reflections indicated a
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