organic compounds
Closely associated with the ring disorder in (I) is the posi-
tional disorder of the entire 3,4,5-trimethoxyphenyl unit,
where the two components occupy similar regions of space
(Fig. 1). For example, the dihedral angle between the planes of
the two rings C111–C116 and C211–C216 is only 3.6 (9)ꢁ, and
having different configurations, S at C16 in the major
component and R at C26 in the minor component. The
enantiomeric nature of the two components is further illu-
strated by the ring puckering angles for the same atom
sequences as in (I) [ꢁ = 54.8 (5)ꢁ and ’ = 298.5 (6)ꢁ for the
major form, and ꢁ = 126 (4)ꢁ and ’ = 114 (4)ꢁ for the minor
form], indicating an almost perfect half-chair form in both
components of (II).
The observed disorder in (I) and (II) has prompted us to re-
examine compound (III) using the original diffraction data,
and this has confirmed that, as originally reported (Low, Cobo,
Cuervo et al., 2004), the molecules in (III) are fully ordered,
with only a single enantiomer occupying each molecular site in
the space group P21/c. The ring-puckering angles in (III)
correspond almost exactly to an envelope conformation for
the nitrogen-containing ring, so that the six-membered ring
conformations in (I)–(III) are all slightly different.
˚
while the C16ꢀ ꢀ ꢀC26 distance is 0.855 (9) A, the O144ꢀ ꢀ ꢀO214
˚
distance, at the far end of this substituent, is only 0.17 (3) A.
For each conformation of the nitrogen-containing ring, the
3,4,5-trimethoxyphenyl substituent occupies an equatorial site,
and it seems probable therefore that the conformational
disorder of the nitrogen-containing ring is a direct conse-
quence of the statistical occurrence of two enantiomeric forms
at each molecular site in an orientation dominated by the bulk
of the 3,4,5-trimethoxyphenyl substituent.
Rather similar disorder was found in (II), but it was found
necessary to treat the entire molecule as disordered over two
sets of sites, again with the major and minor components
The crystallization of (I)–(III) as racemates is wholly to be
expected, as their syntheses utilized no reagents capable of
imparting enantiomeric bias. What is unexpected, however, is
the site occupancy in (I) and (II) by a mixture of enantiomeric
forms. Possibly, the larger the steric bulk of the peripheral
substituents, the more likely the observation of such behaviour
becomes.
Within the fused tricyclic component of (I) there are some
unusual bond distances (Table 1) which provide evidence for
polarization of the electronic structure. In the central carbo-
cyclic ring of this unit, the distances C3A—C4 and C9—C9A
are both significantly shorter than the remaining C—C
distances. In addition, the exocyclic bonds C4A—N15 and
C18—C8A are both short for their types [mean values (Allen
˚
et al., 1987) 1.419 and 1.485 A, respectively; lower-quartile
˚
values 1.412 and 1.478 A], while the ketonic C18—O8 bond is
˚
long for its type (mean value 1.230 A; upper-quartile value
˚
1.215 A). These observations indicate that the polarized form
Figure 1
The molecular structure of (I), showing the two disorder components and
the atom-labelling scheme. Displacement ellipsoids are drawn at the 30%
probability level. The disordered atom sites O18 and O28 are almost
coincident, so that it is not possible to distinguish them in this figure.
(Ia) (see scheme) is a significant contributor to the overall
electronic structure, so that hydrogen bonds (see below and
Table 2) involving either N15 as donor or O18 as acceptor can
be regarded as charge-assisted hydrogen bonds (Gilli et al.,
1994). Entirely similar patterns of distances are found both in
(II) (Table 3) and in (III) (Low, Cobo, Cuervo et al., 2004), and
it is possible that such polarization is typical of compounds
containing this quinolinone ring system. For example, a
comparable pattern is evident in N-acetyl derivative (IV)
´
(Low, Cobo, Ortız et al., 2004).
The methyl C atoms in two of the three methoxy groups in
(I) lie very close to the plane of the adjacent ring, as indicated
by the relevant torsion angles (Table 1), while the plane of the
central methoxy C—O—C fragment containing C118 is almost
orthogonal to the ring plane. The displacements of atoms
C117, C118 and C119 from the mean plane of the adjacent ring
˚
are 0.147 (3), 1.249 (6) and ꢂ0.047 (3) A, respectively. Asso-
ciated with these substituent conformations, the two exocyclic
C—C—O angles at C114 are almost identical, while the pairs
of angles at C113 and C115 differ, as usual, by ca 10ꢁ (Table 1).
The C—O—C angles at O113 and O115 are both significantly
larger than the ideal tetrahedral value.
Figure 2
The molecular structure of (II), showing the two disorder components
and the atom-labelling scheme. Displacement ellipsoids are drawn at the
30% probability level. The atom numbers in the major component all
begin with 1 and those in the minor component all begin with 2.
ꢃ
Acta Cryst. (2009). C65, o326–o330
Cuervo et al. C19H19NO6 and C17H13NO5 o327