J. J. Kaminski et al. / Bioorg. Med. Chem. 7 (1999) 1413±1423
1423
recorded on an Enraf±Nonius CAD-4 diractometer
[Cu-Ka radiation, graphite monochromator; w-2q
scans, qmax=75ꢀ, scanwidths (1.15+0.14 tanq)ꢀ for 20,
(1.00+0.14 tanq)ꢀ for 5 and 9]; the intensities of four
reference re¯ections, remeasured every 2 h, showed no
signi®cant variation (<1%) throughout. Re®ned unit-
cell parameters were calculated in each case from the
diractometer setting angles for 25 re¯ections
(36ꢀ<q<40ꢀ for 20 and 9; 32ꢀ<q<36ꢀ for 5) widely
separated in reciprocal space. Intensity data were cor-
rected for the usual Lorentz and polarization eects. An
Crystallographic calculations were performed on
PDP11/44 and MicroVAX computers by use of the
Enraf±Nonius Structure Determination Package (SDP).
For all structure-factor calculations, neutral atom scat-
tering factors and their anomalous dispersion correc-
tions were taken from ref. 14.
Supplementary information available
ORTEP diagrams showing the crystallographic atom
numbering schemes, tables of fractional atomic coordi-
nates and temperature factor parameters, bond lengths,
bond angles, and torsion angles for 20, 5 and 9 (26
pages) are available from the authors.
empirical
absorption
correction
[Tmax:Tmin(rela-
tive)=1.00:0.80], based on the f-dependency of the inten-
sities of several re¯ections with c ca. 90ꢀ, was also applied
to the data for 5. Equivalent re¯ections for 5 and 9 were
averaged [Rmerge (on I)=0.03 for 5, 0.01 for 9] to yield 3973
and 3589 nonequivalent values. The structure analyses and
parameter re®nements were based on 1902, 1475, and 3289
re¯ections with I>3.0s(I) for 20, 5 and 9, respectively. All
three crystal structures were solved by direct methods. For
both 5 and 9, the centrosymmetric space group choices (P1
and C2/c, respectively) were assumed at the outset and
shown to be correct by the structure solutions and re®ne-
ments. E-maps yielded initial coordinates for all non-
hydrogen atoms in 20 and 9. For 20, the enantiomer was
selected to yield the known absolute stereochemistry of the
N-acetyl-d-leucyl anion. Approximate coordinates for the
non-hydrogen atoms of 5, other than those of the ethyl
moiety, were obtained from an E-map; positions for the
carbon atoms of the ethyl group, which was found to be
disordered over two orientations, were derived from a dif-
ference Fourier synthesis phased by the other atoms.
Atomic positional and thermal parameters (®rst isotropic
and then anisotropic) were adjusted by means of full-
matrix least-squares calculations during which SwD2
[w=1/s2(jFoj),d=(jFoj jFcj)] was minimized. Hydrogen
atoms in 5 and 9 (other than those of the disordered ethyl
group in 5) were located in dierence Fourier syntheses,
and their positional and isotropic thermal parameters
were re®ned in addition to the non-hydrogen atom para-
meters in the subsequent least-squares iterations. For 20
and the ethyl group of 5, hydrogen atoms were incorpo-
rated at their calculated positions. An extinction correc-
tion (g) was included as a variable during the later least-
squares cycles for 20 and 9. The parameter re®nements
converged at R(=SjjFoj jFcjj)/SjFoj)=0.049, {Rw=
[Sw(jFoj jFcj)2/Sw(jFoj2]1/2=0.066, GOF=[SwD2/(N
References
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Nparameters)]1/2=1.28, g=3.2 (5)Â10 6} for
observations
20; R=0.044 (Rw=0.055), GOF=1.41 for 5, R=0.038
5
(Rw=0.064), GOF=2.82, g=1.08(6)Â10 for 9. Final
dierence Fourier syntheses contained no unusual fea-
tures [Dr(eA 3) max, min: 0.45, 0.19 (2); 0.13, 0.12
(5), 0.30, 0.21 (9)].