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E
(18)(1'8')
(18)
(1'8')
1'
1'
1'
1'
1
1
1
1
Z-RR'
Z-SS'
E-SR'
E-RS'
(11')(88')(99')
1
1'
(18')(81')(99')
1
(11'88')(99')
(18'81')(99')
1
1
1'
1'
1'
Z-RR'
Z-SS'
E-SR'
E-RS'
E*
(18)(1'8')*
1
(18)*
(1'8')*
1
1
1
1'
1'
1'
1'
Z-RR'
E-RS'
E-SR'
Z-SS'
(11')(88')(99')*
(18')(81')(99')*
(11'88')(99')*
1'
(18'81')(99')*
1'
1'
1'
1
1
1
1
Z-SS'
Z-RR'
E-RS'
E-SR'
Fig. 22 Effect of the permutation-inversion operators on the anti -folded conformation a- C 2h ( y )
Table 8 Effect of permutation-inversion operators on the anti -folded conformation a- C 2h ( y )
Permutation-inversion operators Effect on the conformation a- C 2h ( y )
E , (11 0 )(88 0 )(99 0 ), (18)(1 0 8 0 )*, (18 0 )(81 0 )(99 0 )* None a
(18)(1 0 8 0 ), (18 0 )(81 0 )(99 0 ), E *, (11 0 )(88 0 )(99 0 )* Inversion of both moieties
(18), (11 0 88 0 )(99 0 ), (1 0 8 0 )*, (18 0 81 0 )(99 0 )* E , Z -isomerization and inversion of first
moiety
(1 0 8 0 ), (18 0 81 0 )(99 0 ), (18)*, (11 0 88 0 )(99 0 )* E , Z -isomerization and inversion of second
moiety
a E , (11 0 )(88 0 )(99 0 ), (18)(1 0 8 0 )*, (18 0 )(81 0 )(99 0 )* correspond to the point group symmetry operators,
E , C 2 ( y ),
˃
( xz ), and i of a- C 2h ( y ), respectively
the symmetry operators of the conformation. Each of the cosets contains at least one
self-inverse operator. Thus all three dynamic processes are self-inverse and the
corresponding transition states may include the permutation-operators of the coset
as symmetry operators of their respective point groups [ 271 ].
In homomerous BAEs, the two tricyclic moieties are equivalent. Thus, the
processes (2) and (3), i.e., E , Z -isomerization with inversion of either the first or
the second moiety, respectively, cannot be distinguished. They will be discussed
together as one dynamic process: E , Z -isomerization with inversion of one moiety.
Note that the combined mechanism has a connectivity of C
2. Each conforma-
tion may be converted into two distinct versions by inverting either the first or the
second moiety.
¼
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