M. J. Potrzebowski et al.
FULL PAPER
gel, 230Ϫ400 mesh, 5.0 g: eluted with a gradient of 0Ϫ10% meth-
anol in chloroform to provide SP-1 (55 mg, 72%): Rf 0.22 (chloro-
form, ethanol 19:1, v/v). Ϫ δP 67.7. Ϫ MS: FAB, ϩve, m/z ϭ 658
bis(dineopentoxyphosphorothioyl) disulfide set at 84.0 ppm. The
principal elements of the 31P chemical shift tensor and shielding
parameters were calculated employing the WINMAS program. The
[M ϩ 1]ϩ. Ϫ C25H32N5O12PS: calcd. C 45.66, H 4.90, N 10.65, S details describing the method and accuracy of calculations are dis-
4.88; found C 45.58, H 4.90 N 10.34 , S 4.65. SP-1 was crystallized cussed elsewhere in detail.[19,20]
from ethanol/chloroform/ hexane (1:1:1, v/v/v) to provide crystals,
X-ray Analysis: The crystal and molecular structure of SP-1 was
m.p. 189Ϫ190° C.
determined using data collected at room temperature on a CAD4
diffractometer with graphite monochromated Cu-Kα radiation.[26]
The compound crystallizes in a monoclinic system, in the space
group P21, with the unit cell consisting of two molecules. The lat-
tice constants were refined by a least-squares fit of 25 reflections
in the θ range 19.01°Ϫ28.87°. The decline in the intensity of three
control reflections (3, Ϫ5, 4; 1, Ϫ7, Ϫ2; Ϫ3, Ϫ4, 1) was 1.7% dur-
ing 94.0 h of exposure time. An empirical absorption correction
Starting from slow-eluted diastereomer RP-5 and using the same
procedure, RP-1 was obtained in 68% yield: Rf 0.18 (chloroform,
ethanol 19:1, v/v). Ϫ 31P NMR: δ ϭ 66.8. Ϫ C25H32N5O12PS:
calcd. C 45.66, H 4.90, N 10.65, S 4.88; found C 45.36, H 4.83, N
10.30, S 4.55. Attempts to crystallize RP-1 from several solvents
failed.
NMR Measurements in Solutions: The samples of SP-1 or RP-1
(5 mg) were dissolved in [D6]DMSO (0.5 mL). All spectra were re-
corded on a Bruker Avance DRX 500 spectrometer, operating at
500.1300 MHz for 1H, 125.2578 MHz for 13C, and 202.46 MHz for
31P. For all experiments, original Bruker pulse programs were used.
The chemical shift of the DMSO signal was used as a reference
(δ ϭ 2.49 for 1H and δ ϭ 39.5 for 13C). Phosphoric acid (85%) was
used as an external standard for 31P spectra. The spectrometer was
equipped with a Pulse Field Gradient Unit (50 G/cm). The inverse
broadband probe-head was used. The COSY90 spectra were ob-
tained from 1024 experiments, each with 4 scans. The relaxation
delay was 1.5 sec. The spectral width was 10 ppm (5000 Hz) in both
dimensions. The data size in F2 was 4 K. Digital quadrature detec-
tion (DQD) was applied. Two 10 µs length z-gradient pulses, with
a strength of approximately 5 G/cm each, were applied with a 1-ms
delay for gradient recovery. The FID were apodized with a sine-
bell function in both dimensions. Final data were zero filled twice
in both dimensions and symmetrized about the diagonal. The
ROESY spectra were recorded in a 2 K ϫ 1 K (F2 ϫ F1) data
matrix. Digital quadrature detection was applied and 32 scans were
accumulated in each experiment. The experiment was run in the
phase-sensitive mode with a 3650 ms cw pulse for ROESY spin
lock. The spectral width was 4500 Hz (9 ppm) in both dimensions.
Data were processed with a sine bell shaped apodization function
in both directions and TPPI in F1. No zero filling was applied. The
PFG-HMQC spectra were acquired in a 1 K ϫ 4 K [F1(13C) ϫ
F2(1 H)] data matrix. Three 1 ms length z-gradient pulses, with
strengths of approximately 25 G/cm, 15 G/cm, and 20 G/cm, in se-
quence were applied with 1 ms delay for gradient recovery. The
spectral width was 4000 Hz (8 ppm) in F2 (1 H) and 25 kHz
(200 ppm) in F1 (13C). A Garp decoupling sequence was employed.
Final data were processed with a sine function in F1 and qsine in
the F2 dimension. The PFG-HMBC experiment was acquired in
0.5 K ϫ 4 K (F1 ϫ F2) data matrix and 8 scans for each experi-
ment. Three 1-ms length z-gradient pulses, strength of about 25 G/
cm, 15 G/cm and 20 G/cm, in sequence were applied with 50 µs
delay for gradient recovery. Final data were processed with sine-
bell and qsine-bell functions in F1 and F2 dimensions respectively.
was applied by the use of the ψ-scan method (EAC program).[27]
A
total of 6279 reflections with I Ն 2σ(I) were used to solve the struc-
ture by direct methods and to refine it by full-matrix least-squares
using
F2.
Hydrogen
atoms
at
the
disordered
ϪOϪCH2ϪCH2ϪCϵN group with gof ϭ 0.26(2) were placed
geometrically, and allowed to ride on the preceding C atom with a
CϪH distance free to refine and fixed thermal parameters equal to
1.3 times the equivalent isotropic thermal parameter of the parent-
atom. All other hydrogen atoms were found on a difference-Fourier
map and refined isotropically. Anisotropic thermal parameters were
applied for all non-hydrogen atoms. The final refinement converged
to R ϭ 0.0355 for 6053 reflections with I Ն 2σ(I). The absolute
configuration at the chiral atoms were established as SP1, RC1Ј, SC3Ј
,
RC4Ј, RC1Јa, RC3Јa, RC4Јa. The absolute structure was determined by
the Flack method,[27] with the resulting χ ϭ Ϫ0.017(12).
Data Collection and Cell Refinement: Absorption correction:
EAC.[28] Structure solution: SHELXS-86.[29] Structure refinement:
SHELXL-93.[30]
Acknowledgments
This project was financially assisted by the State Committee for
Scientific Research, grants 3 T09A 026 19 (to M.J.P.) and 4 P05F
006 17 (to W.J.S.).
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