+
+
Stereochemical Analysis of Strictosidine
Ta ble 4. Through-Space Distances of Protons in Strictosidine
J ournal of Natural Products, 1997, Vol. 60, No. 2 71
Ta ble 6. Calculated Coupling Constants in the Three
Staggered Conformations Across the C-3-C-14, C-14-C-15,
C-1-O, and O-C-1′ Bonds and the Measured Values for
Strictosidine (1)
a
(1) and the Intensity of the Corresponding Cross Peaks from
the NOESY Spectrum
neighboring protons,
inter-proton distances (Å),
calculated coupling constant (Hz)
hydrogen
and NOESY cross peaks intensityb
assignment æ ) 60°
æ ) 180°
æ ) 300° measured (Hz)
H-3
H-14proS 2.4 w; H-5R 2.6 w; H-14proR 3.1 n
J H-3,H-14S
J H-3,H-14R
J H-14S,H-15
J H-14R,H-15
J C-2,H-14S
J C-2,H-14R
J C-3,H-15
J C-14,H-20
J C-16,H-14S
J C-16,H-14R
J C-20,H-14S
J C-20,H-14R
J C-21,H-1’
J C-1’,H-21
3.4
3.6
3.2
3.0
2.1
2.1
2.1
2.1
0.1
0.1
2.1
2.1
1.6
1.6
11.8
11.8
12.4
12.4
8.5
8.5
7.7
6.8
6.5
6.5
8.5
8.5
6.8
2.9
2.6
3.0
3.2
2.1
2.1
2.1
2.1
0.1
0.1
2.1
2.1
1.6
1.6
3.2
11.8
12.3
2.9
3
2
2
6
<2
6.5
<2
2.5
2.7
3.2
c
H-5R
H-5â
H-6R
H-6â
H-9
H-5â 1.8 s; H-6R 2.5 n ; H-3 2.6 w; H-6â 3.1 n
H-5R 1.8 s; H-6â 2.5 n
H-6â 1.8 s; H-5R 2.5 n
H-6R 1.8 s; H-5â 2.5 n
H-10 2.6 s; H-6R 3.0 n
H-10
H-9 2.6 s; H-11 2.6 s; H-12 4.5 n
H-10 2.6 s; H-12 2.6 s; H-9 4.5 n
H-11 2.6 s; H-10 4.5 n
1
H-1
H-12
H-14proR
H-14proS
H-15
H-18Z
H-18E
H-19
H-14proS 1.8 s; H-19 2.4 w; H-15 2.5 w; H-3 3.1 n
H-14proR 1.8 s; H-21 2.2 s; H-3 2.4 w; H-15 3.1 n
H-20 2.4 s; H-14proR 2.5 w; H-14proS 3.1 n
H-18E 1.9 s; H-20 2.4 m; H-19 3.1 w; H-15 3.6 n
H-18Z 1.9 s; H-19 2.4 m; H-20 3.7 n
6.8
d
H-14proR 2.4 s; H-18E 2.4 m; H-21 2.7 ? ;
H-18Z 3.1 n
H-20
H-15 2.4 s; H-18Z 2.4 m; H-21 3.1 w; H-19 3.1 w;
H-14proR 3.8 n
H-14proS 2.2 s; H-19 2.7 ? ; H-1′ 3.0 s; H-20 3.1 n
droxy groups to the rings were not investigated because
of the lack of NMR data. According to these restrictions,
two series of configurational isomers based on C-3 can
be expected, each having 324 conformers.
c
H-21
H-1′
H-5′ 2.5 s; H-3′ 2.6 s; H-21 3.0 s; Ha-6′ 4.2 n
a
Corresponding to the structure shown in Figure 4.
The conformations around the single bonds were
determined from vicinal proton-proton and carbon-
proton coupling constants. The measured values were
compared with calculated coupling constants of the
three staggered conformations. The vicinal proton-
proton coupling constants were calculated using the
parametrized Karplus type of equation of Haasnoot et
b
Abbreviationsss: strong; m: medium; w: weak; n: cross peak
not detected. The cross peak was missing due to a coupling
interaction between the two protons. No cross peak could be
observed because the two corresponding signals were overlapping.
c
d
Ta ble 5. Measured and Calculated 13C-1H Coupling
Constants of Strictosidine (1) in Hz
2
8
measureda
calculatedb
al. The vicinal carbon-proton coupling constants of
the CR-Câ-Cγ-H fragments were calculated using the
assignment
J C-2,H-14R
J C-2,H-14S
J C-3,H-15
2
3
2
2.6
1.9
2.3
6.7
1.9
6.5
2.3
0.6
1.4
0
2
9
equation of Aydin and G u¨ nther. In the calculation of
torsion angles larger than 90°, these authors applied
-0.9 and -1.7 Hz correctional terms for carbon sub-
stituents at â- and γ-carbons, respectively; no correction
was needed for carbon substituents at the R-carbon.
These calculations were supported also by those of van
J C-14,H-20
J C-15,H-21
J C-16,H-14R
J C-16,H-14S
J C-17,H-21
J C-19,H-15
J C-19,H-21
J C-20,H-14R
J C-20,H-14S
J C-21,H-15
J C-21,H-17
J C-21,H-1′
J C-22,H-15
J C-1′,H-21
6
2.7
6.5
<2
2
2.8
2
3
0
31
Beuzekom et al. However, Parella et al. reported a
negative contribution of the carbonyl substituent on the
R-carbon. Therefore, in the calculation of J C-16,H-14S
and J C-16,H-14R, we applied a correctional term of -2
Hz to the equation of Aydin and G u¨ nther.28 The vicinal
carbon-proton coupling constants of C-O-C-H frag-
ments were calculated by the Karplus type of equation
2.5
<2
8
7.0
2.7
3
3.0
1.7
8.0
6.7
1.5
4.8
1.8
3.2
3
2
described by Mulloy et al.
The calculated coupling
a
Further 13C- H coupling constants in Hz: J C-2,H-3 ) 6.5,
1
2
constants of the three staggered conformations across
bonds C-3-C-14, C-14-C-15, C-21-O, and O-C-1′ are
summarized in Table 6.
1
3
1
3
2
2
3
J C-3,H-3 ) 144, J C-3,H-14R < 1, J C-3,H-14S ) 4.2, J C-7,H-9 ) 3.4,
2
1
3
J C-8,H-12 ) 4.9, J C-8,H-9 ) 3, J C-9,H ) 157.5, J C-10,H-12- ) 6.5,
2
2
2
J C-12,H ) 58.6, J C-14,H-3 ) 7, J C-15,H-14R ) 3, J C-15,H-14S < 1,
2
3
1
There were nine conformations resulting from the
rotation around C-3-C-14 and C-14-C-15 bonds in each
of the two configurational series. One of the protons at
C-14 had a large coupling constant (11.4 Hz) at H-3 and
a small one (3.9 Hz) at H-15, whereas the other proton
had a large coupling constant (11.5 Hz) at H-15 and a
small one (3.0 Hz) at H-3. According to the calculated
coupling constants in Table 6, this means that, in the
dominant conformation, one of the H-14 atoms is
antiperiplanar (æ ) 180°) to H-3 and the other to H-15.
Such an arrangement can be found only in two confor-
mations in each (H-3R and H-3â) series: S11 and S22
as well as V11 and V22 (shown in Figure 1). In these
conformers neither of the big ligands of C-3 and C-15
(C-2, N-4, C-16, C-20) interfere each other. Conse-
quently, 14 of the 18 structures in which such interfer-
ences exist may be disregarded. Moreover, the coupling
J C-15,H-17 ) 5.8, J C-16,H-17 ) 6.0, J C-17,H-15 ) 4.0, J C-17,H-17
1
1
3
)
193.3, J C-18,H-18Z ) 155.0, J C-18,H-18E ) 158.2, J C-18,H-20 )
5
.4, J C-19,H-18Z ) 3.9, J C-19,H-18E ) 2.6, 1J C-19,H-19 ) 156,
2
2
2
2
3
3
J C-19,H-20 ) 6, J C-20,H-15 ) 6.0, J C-20,H-18Z ) 3.1, J C-20,H-18E )
2
1
2
1
1.8, J C-20,H-19 ) 1.1, J C-20,H-20 ) 133, J C-21,H-20 ) 7.5,
3 2 1
1
J C-21,H-21 ) 172.9, J C-22,H-17 ) 3.4, J C-22,OMe ) 3.9, J OMe,H )
b
1
47.3. Values are for the structure shown in Figure 4.
the secologanin unit in N-4-(p-bromobenzyl)-O,O,O,O-
tetraacetyl vincoside.
The stereogenic elements and the number of possible
stereoisomers of strictosidine (1) are shown in Table 1.
In our work only staggered conformations around C-14
and the glycosidic oxygen bridge, as well as the two half-
chair conformations of the two partially saturated
heterocycles, were considered. The less stable config-
uration of N-1 and N-4 and the rotational position of
the methoxycarbonyl, vinyl, hydroxymethyl, and hy-