For the elucidation of the absolute configuration of the
nudicaulins 3a/b, electronic circular-dichroism (ECD) spec-
troscopy in combination with quantum-chemical ECD
calculations5 was the method of choice. A first analysis of
the experimental UV absorptions of 3a and 3b measured
in two different solvent systems revealed a strong solvent
dependence of the first UV band. In the MeCNꢀH2O
mixture, this absorption appeared with high intensity
around 460 nm, possessing a broad blue-shifted shoulder,
while two signals of low intensity around 460 and 385 nm
were observed in MeOH (Figure S43).
First excited-state calculations for the cis-configured
nudicaulins I and II were performed with time-dependent
(TD) CAM-B3LYP, including CPCM for solvent effects
of MeOH. However, the calculated spectra did not show
sufficiently good agreement with the experimental ones
(Figure S46). A reason for this could be interactions be-
tween the solvent and the glucose moieties that might
influence the chiroptical properties.
Figure 2. Modification of nudicaulins I and II (3a/b) and ‘new’
HMBC interactions (in red). (a) Catalytic hydrogenation.
(b) Permethylation. (c) Enzymatic hydrolysis by a pectinase.
Therefore, an arbitrarily chosen number of water mole-
cules (12) were added to the structure of the two cis-
diastereomers, (3S,11R)-3 and (3R,11S)-3, using the
CAST program.6 The conformations thus identified were
further optimized with B97-D/SVP and then submitted to
semiempirical ZINDO/S-CI UV calculations. The results
were compared with the UV curves calculated for identical
conformations, without water molecules. The ones includ-
ing water possessed a red-shifted, intensified first absorp-
tion band, thus corroborating the substantial effect of the
solvent (Figure S45, Table S5). These findings showed that
within TDDFT the CPCM approach alone would possibly
not be sufficient to describe the excited-state properties of
the authentic nudicaulins I and II properly, even though
the effects seemed smaller in the experiment when using
methanol. In addition to the ZINDO/S-CI tests, the
analysis of the excited states of the TDDFT computations
showed that within the aglycon core electronic transitions
with charge-transfer (CT) character occurred within the
same wavelength region that was affected by the solvent.
Since more advanced methods to correctly account for
these properties would have led to an immense increase in
computational costs, the compound had to be simplified
synthetically, at least to minimize the solvent effects.
Attempts to remove all three glucose units were unsuc-
cessful, since, apparently, Glc A is needed to prevent de-
composition of the chemically unstable aglycon core.
Therefore, nudicaulins I and II could only be partially
deglucosylated to give their monoglucosidic forms 6a/b
(Figure 2c), using a commercial pectinase. Compared to
the nudicaulins I and II, the NMR spectra of the mono-
glucosides 6a and 6b (Figures S22, S23, S25) were con-
siderably simplified in the carbohydrate regions. The
ROESY spectra of the two diastereomeric monoglucosides
(Figures S24, S26) confirmed the results that had been
obtained for nudicaulins I (3a) and II (3b), indicating an
unchanged aglycon structure after hydrolysis.
same side of the aglycon skeleton, i.e., cis to each other
(Figure 1). Interestingly, nudicaulin II (3b) (Figure S20)
showed such a ROESY cross signal, too, which was also in
agreement with a relative cis-configuration, but it was far
less intense. Relative to the integral intensities of the ROE
signals between H-20/60 and H-30/50, which were used as a
reference (100%), the integral intensity of the H-3 ꢀ H-100
cross signal of nudicaulin I (3a) was 32% and that of
nudicaulin II (3b) was 19%. A conformational search with
B97D/SVP resultedin a minimumstructurewithadistance
00
˚
d(H-3,H-1 ) of 2.4 A for the (3S,11R)-3 diastereomer (cis),
which was consistent with the strong ROE of nudicaulin I
00
˚
(3a), while the longer distance d(H-3,H-1 ), 3.8 A, for the
lowest-energy conformer of the (3R,11S)-3 diastereomer
(also cis) was in accordance with the weaker ROE of
nudicaulin II (3b). For (3R,11R)-3 a0s0 a likewise imaginable
˚
trans-isomer, a distance d(H-3,H-1 ) of about 4.5 A was
predicted, from which no ROE signal would be expected,
because the aglycon core was in between and, therefore,
could be excluded (Figure S42).
In the ROESY spectra of dihydronudicaulins I (4a) and
II (4b) (Figures S31 and S36), ROE signals were observed
between H-3 and H-100 of glucose A, between H-12 and
H-100 of glucose A, between H-12 and H-20/60, and between
H-3 and H-20/60. No ROE signal was observed between
H-3 and H-12 suggesting an opposite orientation with
respect to the plane formed by the indole moiety and ring e
(corresponds to trans-orientation of Glc A and H-12 and
trans-orientation of the p-hydroxyphenyl ring and the ben-
zofuran moiety). According to these data, the hydrogenation
had occurred with a high degree of stereoselectivity.
(5) For selected reviews, see: (a) Warnke, I.; Furche, F. WIREs
Comp. Mol. Sc. 2012, 2, 150–166. (b) Pescitelli, G.; Di Bari, L.; Berova,
N. Chem. Soc. Rev. 2011, 40, 4603–4625. (c) Autschbach, J. Chirality
2009, 21, E116–E152. (d) Bringmann, G.; Bruhn, T.; Maksimenka, K.;
Hemberger, Y. Eur. J. Org. Chem. 2009, 2717–2727.
(6) Grebner, C.; Becker, J.; Stepanenko, S.; Engels, B. J. Comput.
Chem. 2011, 32, 2245–2253.
Org. Lett., Vol. XX, No. XX, XXXX
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