N. Aberle et al. / Tetrahedron Letters 48 (2007) 2199–2203
2201
Scheme 2. Model system for oxidative spirocyclisation.
or 15 (R = CH3), or mixtures thereof, were isolated,
casting further doubt on the ability to isolate such an
orthoamide functionality via hyper-valent iodine-medi-
ated oxidative cyclisation.
ment8 and, after their recent use to propose structural
revision of the natural product hexacyclinol,9 were used
here to support an alternative structure of spiroleucetta-
dine. The hybrid functional MPW1PW91 has been shown
to perform particularly well in this regard, especially
when employed with the 6-311+G(2d,p) basis set.10–13
Our experience with both the model system and the actual
precursor 10, along with the comments in both the Dani-
shefsky and Ciufolini papers, led us to examine the avail-
able spectroscopic data of spiroleucettadine in greater
detail. This highlighted several areas of concern with the
initial structure assignment, based around the observed
13C chemical shift values of C-4 (102.5 ppm) and C-5
(82.5 ppm) (and hence the regiochemistry of the oxygen
in the oxolane ring), and the interpretation of the
gHMBC and ROESY data. In particular, Ralifo and
Crews state that there is a gHMBC correlation observed
between H2-8 and C-6. Our analysis of the available
gHMBC data suggested that this correlation is in fact a
The minimum energy conformation of each structure
was located on the B3LYP/6-31G(d) potential energy
surface, and the nuclear shielding determined at the
MPW1PW91/6-311+G(2d,p) level upon these geo-
metries. The 13C chemical shifts were obtained by sub-
tracting the predicted nuclear shielding for each atom
from the predicted shielding for tetramethylsilane
(TMS). The nuclear shielding of the carbon nucleus in
TMS at this level, 186.49, compares very favourably
with the experimental value, 186.4.14 The calculated
shifts were corrected from a least-squares correlation
of the predicted and experimental shifts.9,15
1
coincidental correlation from H2-8 into the JC–H of
the 13C resonance of MeOH, the solvent in which
the two-dimensional NMR data were collected. Thus, in
the absence of any evidence linking C-6 and C-8, we con-
sidered the possibility that the actual structure of spiro-
leucettadine has C-6 and the oxygen in the oxolane ring
reversed (16, Fig. 2). This change in structure is consistent
with the absence of gHMBC correlations between C-8
and C-6, and was also expected to better explain the
observed 13C resonances for both C-4 and C-5.
The differences in experimental and calculated (cor-
rected) 13C chemical shifts for 1 and 16 are presented
in Figure 3. The mean absolute error (MAE) for 1 is
4.3, whereas for 16 the MAE is 3.4 ppm. The error in
13C shift for atoms C-4, -5, -6 and -7 of 1 are quite large,
between 7.8 and 14.0 ppm. The error in 13C shift for
three of these four atoms in 16 remains high, but C-5 is
within 0.6 ppm of the experimental value. Despite this,
16 appears to be a biosynthetically feasible alternative.
Density functional calculations of 13C NMR chemical
shifts generally show good agreement with the experi-
Performing the same calculations on various known
structures (Fig. 4)16–18 confirmed the accuracy of the
predictions (with the exception of brominated carbons,
due to the omission in the calculations of relativistic
and spin–orbit coupling effects19) to within about
5 ppm. These results also provided evidence that the pre-
viously unassigned rings of spirocalcaridines A and B
(17 and 18)16 are likely to be cis-fused (MAEs 2.4 and
2.7 ppm, respectively) rather than trans-fused (MAEs
3.9 and 4.3 ppm, respectively).
A range of structural and conformational variants of 1
and 16 were then modelled following the method outlined
Figure 2. Spiroleucettadine 1 and oxolane-inverted version 16.