3
18
Caignan and Holt
X-ray crystallographic study
For IV, the average plane of the cyclohex-
ane ring subtends an angle of 81.9 with the base
�
The collection of diffraction data using suit-
able crystals was accomplished using a Siemens
P4 automated single crystal x-ray diffractometer
equipped with monochromatized Mo K� radia-
of the dihydropyridine ring (atoms C2, C3, C5,
and C6). The fused and hetero B rings are seen in
orientations closer to orthogonality with the basal
�
�
�
plane of the boat: 93.3 (I), 88.5 (II), and 88.5
1
7
˚
tion (0.71073 A) and a �–2� scan. Cell constants
were determined using the least-squares fit of the
four diffractometer angles for an appropriate num-
ber of reflections (Table 1). The intensities of three
standard reflections were monitored after every 97
reflections. Crystaldecompositionwasfoundtobe
insignificant. The structures were solved and re-
fined using the programs SHELXS and SHELXL
(III), suggesting that B ring bulk or the presence of
hetero atoms in the B ring leads to more rigorous
orthogonality.
The conformations of carbonyl groups sub-
stituted at C5 and C3 may be quantified by the
0
0
0
0
C6---C5---C5 ---O5 and C2---C3---C3 ---O3 tor-
sion angles, respectively. Values close to 0 in-
dicate sp conformation, whereas those close to
1
8
�
of the SHELX package. Refinement of an ex-
tinction coefficient showed it to be insignificant.
180 denote ap conformation. Delocalization of
charge over the conjugated C---C---C---O sys-
0
The hydrogen atoms of methyl groups C2 and
tem normally insures that these angles remain
close to their theoretical values. The absolute
0
0
00
00
0
0
C6 of I; C2 , C3 , C5 , and C6 of II; and C2 ,
0
0
00
0
C3 , C5 , and C6 of III showed a rotational dis-
order. The two sets of hydrogen positions associ-
ated with each methyl group, which were apparent
from a difference Fourier synthesis, were refined
with 50% occupancy factors in the final cycles of
refinement.
Table 2. Atomic Coordinates and Equivalent Isotropic Displacment
˚
Coefficients (A) for Compound I
Atom
x
y
z
Ueqa
N(1)
C(2)
C(2 )
0.7867(5)
0.6539(6)
0.7325(7)
0.4759(6)
0.3252(6)
0.2241(7)
0.1698(4)
0.3703(5)
0.4167(6)
0.5804(6)
0.5417(7)
0.3069(9)
0.6517(5)
0.3591(5)
0.7551(6)
0.9301(7)
0.3324(6)
0.1401(6)
0.2921(4) 0.4190(3) 0.055(1)
0.2438(5) 0.4810(4) 0.050(1)
0.1880(6) 0.5782(4) 0.062(1)
0.2521(4) 0.4465(3) 0.045(1)
0.2203(5) 0.5104(4) 0.048(1)
0.1214(6) 0.6595(5) 0.074(2)
0.2428(4) 0.4857(3) 0.063(1)
0.1613(4) 0.5978(3) 0.069(1)
0.2917(5) 0.3350(3) 0.047(1)
0.3830(5) 0.3015(4) 0.048(1)
0.4749(5) 0.2224(4) 0.055(1)
0.5693(6) 0.1274(5) 0.078(2)
0.5397(4) 0.1762(3) 0.084(1)
0.4776(4) 0.2013(3) 0.066(1)
0.3742(5) 0.3400(4) 0.051(1)
0.4466(5) 0.3078(5) 0.068(2)
0.1548(4) 0.2449(3) 0.045(1)
0.1039(4) 0.2254(4) 0.050(1)
Results and discussion
0
C(3)
Projection drawings of the four structures are
given in Fig. 2 on the basis of positional parame-
ters of Tables 2, 4, 6, and 8. Tables 3, 5, 7, and 9
display selected bond angles and distances based
on the final positional parameters.
0
C(3 )
0
0
C(3 )
0
O(3 )
0
0
O(3 )
C(4)
C(5)
0
C(5 )
In molecule IV, with a six-membered B ring
in chair conformation containing no hetero atoms,
the sum of the torsion angles of ring A (boat
0
0
C(5 )
0
O(5 )
00
O(5 )
�
conformation) is 114.5 . The two structures with
C(6)
0
C(6 )
bulky fused rings substituted at C4, i.e. I and III,
are seen with flatter boat conformations of the
C(7)
C(8)
C(9)
O(10)
C(11)
O(12)
C(13)
C(14)
C(15)
�
A ring (torsion angle sum = 0 for a totally flat
0.0703(7) � 0.0204(5) 0.1464(4) 0.055(1)
� 0.1129(5) � 0.0871(4) 0.1096(3) 0.075(1)
� 0.1098(9) � 0.2210(6) 0.0371(5) 0.081(2)
0.0746(6) � 0.2170(4) 0.0128(3) 0.078(1)
0.1813(8) � 0.0977(5) 0.0883(4) 0.058(1)
0.3697(7) � 0.0499(5) 0.1048(4) 0.062(1)
�
ring and 240 for a boat of idealized conforma-
�
tion). Their torsion angle sums are 94.8 (I) and
�
1
08.1 (III). Structure II, in which the aromatic
B ring has an unshared pair localized on the ni-
trogen atom in the meta position, is the most dis-
torted from idealized boat geometry: torsion angle
0.4433(7)
0.0775(5) 0.1837(4) 0.054(1)
a
Equivalent isotropic U defined as one third of the trace of the or-
thogonalized Ui j tensor.
�
sum = 78.6 .