ring and a negative 1Lb band were observed for schulzeine B
(Figure S23). It is well documented that the sign of the 1Lb
band of the fused benzene system is basically determined by
the helicity of the cyclohexene, tetrahydropyridine, or dihy-
dropyran ring (Figure 3), but the sign could be reversed by
factors such as (1) polar substituent(s) of the benzene ring
and (2) an axial substituent at the benzylic position.14 Judging
Scheme 1. Chemical Degradation of Jasisoquinoline A (1)
1
from the signs of Lb bands in schulzeines, it was demon-
strated that substitution of the benzene ring by two OH
groups did not reverse the relationship between the helicity
and the sign of the 1Lb band in isoquinolines: P- orM-helicity
corresponds to a positive or negative 1Lb band, respectively.15
We were able to assign the conformation of the tetrahydro-
pyridine ring of jasisoquinoline A (1) on the basis of the
ROESY data (Figure 1c) and observed a positive 1Lb band.
1
However, the sign of the Lb band is variable due to the
presence of an axial substituent at the benzylic position.
Because of the lack of suitable examples, it is not possible
to assess the effect of quaternalization of the benzylic position
1
toward the sign of the Lb band. Therefore, we tentatively
draw the structure of 1by taking into account the positive 1Lb
band and by presuming that its sign was not reversed by
substituents at C-1 (Figure 3).
converting to the (R)-MTPA ester 8 (Scheme 1b).11 The 1H
NMR spectra of the (S)- and (R)-MTPA esters of 3-methyl-
1-alkanols give charasteristic patterns for the oxygenated
methylene protons by reflecting the configuration of the
methyl branch.7,12 The 1H NMR data of 8 were consistent
with the corresponding ester of the 3R-alkanols, indicating
the 27R configuration. Because the relative configuration of
the C-21 to C-27 portion was suggested to be identical with
that of the corresponding portion of 3, configurations at
C-21, C-24, and C-25 were deduced to be all S.
We initially anticipated determining the absolute config-
uration of the C-1 quaternary carbon by applying the exciton
chirality method13 because of the presence of two chromo-
phoric resorcinol moieties. However, in the CD spectrum of 1
(Figure 2), no exciton split was observed near the absorption
maximum of resorcinol rings (280 nm). Instead a positive 1Lb
transition was observed at 280 nm.14 The conformation of
the tetrahydropyridine ring in schulzeine A had been assigned
on the basis of the ROESY data, and its absolute configura-
tion had been determined by the modified Mosher analysis.7
A positive 1Lb band of schulzeine A (Figure S23) was consis-
tent with the P-helicity of the tetrahydropyridine ring. On
the other hand the M-helicity of the tetrahydropyridine
Figure 2. CD spectrum of jasisoquinoline A (1).
(12) (a) Oikawa, H.; Matsuda, I.; Kagawa, T.; Ichikawa, A.; Kohmoto,
K. Tetrahedron 1994, 50, 13347–13368. (b) Eguchi, T.; Kobayashi, K.;
Uesaka, H.; Ohashi, Y.; Mizoue, K.; Matsushima, Y.; Kakinuma, K. Org.
Lett. 2002, 4, 3383–3386.
(13) Nakanishi, K.; Berova, N. In Circular Dichroism, Principles and
applications; Nakanishi, K., Berova, N., Woody, R. W., Eds; VCH Publish-
ers, Inc.: New York, 1994; Chapter 13.
(14) (a) Snatzke, G.; Ho, P. C. Tetrahedron 1971, 27, 3645–3653. (b)
ꢀ
Snatzke, G.; Kajtar, M.; Werner-Zamojska, F. Tetrahedron 1972, 28, 281–
ꢀ
288. (c) Snatzke, G.; Kajtar, M.; Snatzke, F. In Fundamental Aspects and
Figure 3. Helicity of the tetrahydropyridine ring of jasisoquino-
line A (1). The bold lines represent the benzene rings.
Recent Developments in Optical Rotatory Dispersion and Circular Dichroism;
Ciardelli, F., Salvadori, P., Eds; Heyden: London, 1973; Chapter 3.4. (d) Toda, J.;
Matsumoto, S.; Saitoh, T.; Sano, T. Chem. Pharm. Bull. 2000, 48, 91–98.
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