ꢀ
A. Sikorski, D. Trzybinski / Tetrahedron 67 (2011) 2839e2843
2842
acridine skeletons are linked by
rangement forming alternately aligned columns of molecules A and
B (Figs. 3a and 4).
p
e
p
interactions in the ABA ar-
of 3, there are networks of chains forming columns (Fig. 3c). The
presence of chains in the crystal packing is the reason of lack of
-stacking interactions between the aromatic rings in the anions.
p
3. Conclusion
In summary, as a continuation of our recent work, we discuss the
crystal structures of a series of salts with the 9-aminoacridinium
cation and the 3-chlorobenzoate (1), 4-chlorobenzoate (2), and 3-
hydroxybenzoate (3) anions. The structure of 3 is the first of all the
known 9-aminoacridinium salts where mixed salts were obtained.
Conformational analysis of the 9-aminoacridinium skeleton sug-
gests that the aromatic carboxylic acid anions affect the planarity of
the 9-AA skeleton, especially in compound 3, which adopts an evi-
dent butterfly conformation. Analysis of the hydrogen bonds in the
crystal lattices of the title compounds shows that the cations and
anions form tetramers (1 and 2) or chains (3). In the tetramers, the
ions are linked via N(amino)eH/O(carboxy) hydrogen bonds
forming R22(8) (1) or R42(16) (2) hydrogen bond ring motifs. In the
packing of 3, there are two kinds of hydrogen bond chain motif. The
first, C24(16), in which 9-AA cations, a Clꢀ anion and a water molecule
are interlinked, and the second, C(7), in which aromatic carboxylic
acid anions are connected directly. We also observed the influence of
the different anions on the packing of the acridine skeletons in the
crystal lattice. The 9-AA cations are
pep stacked in the AB (1) or ABA
(2 and 3) arrangement to form a two-fold helical arrangement (1) or
columns (2 and 3). Analysis of the
aromatic rings of anions indicates that
p
e
p
p
interactions between the
-stacking interactions are
observed only in the packing of molecules 2.
4. Experimental
4.1. General
The synthesis of compounds 1, 2, and 3 is described in
Supplementary data. Single crystals of 1e3 were grown by slow
evaporation of an ethanol solution.
4.2. Crystal structure determination
Good-quality single-crystal specimens of 1, 2, and 3 were se-
lected for the X-ray diffraction experiments at T¼295(2) K. They
were mounted with epoxy glue at the tip of glass capillaries Dif-
Fig. 4. Geometry of the
pep interactions in 3.
fraction data were collected on an Oxford Diffraction Gemini R
ꢁ
ULTRA Ruby CCD diffractometer with CuK
a
(
l
¼1.54184 A) (for 1)
ꢁ
In the ABA arrangement of molecules A, all the aromatic rings
from the acridine skeletons participate in interactions, form-
ing a zigzag motif with centroid/centroid distances from 3.573 to
and Mo K
a
(l
¼0.71073 A) (for 2 and 3) radiation. In all cases, lattice
pep
parameters were obtained by least-squares fit to the optimized
setting angles of the collected reflections by means of CrysAlis CCD9
Data were reduced by using CrysAlis RED software with applying
multi-scan absorption corrections (Empirical absorption correction
using spherical harmonics, implemented in SCALE3 ABSPACK
scaling algorithm). The structural resolution procedure was made
using the SHELXS-97 package solving the structures by direct
methods and carrying out refinements by full-matrix least-squares
on F2 using SHELXL-97 program.10 All H-atoms bound with aromatic
C-atoms were placed geometrically and refined using a riding
ꢁ
ꢁ
4.182 A and a distance of 3.450 A between the mean planes of the
neighboring acridine skeleton. In this arrangement, the over-
lapping mode of the neighboring cations shows that they are al-
ꢁ
ternately shifted toward each other for a distance of w1.4 A and
w1.2 A along the shortest and longest axis of the acridine skeletons,
respectively, in the AB sequence and shifted for a distance of w1.4 A
and w1.8 A along the shortest and longest axis of the acridine
ꢁ
ꢁ
ꢁ
skeletons, respectively, in the BA sequence. Molecules of B are also
packed in the ABA arrangement with centroid/centroid distances
ꢁ
model with CeH¼0.93 A and Uiso(H)¼1.2 Ueq(C). All H-atoms
ꢁ
ꢁ
from 3.602 to 4.364 A and a distance of 3.520 A between the mean
planes of the neighboring acridine skeleton. However, there are
differences between the overlapping modes of the neighboring
cations. In the AB sequence, the adjacent cations are alternately
shifted along the longest axis of the acridine skeletons for a dis-
bound with N-atoms were placed geometrically and refined using
ꢁ
a riding model with NeH¼0.86 A and Uiso(H)¼1.5 Ueq(N). The all
amino eNH2 groups were assumed to be planar-trigonal and co-
planar with the mean planes of acridinium skeleton. All H-atoms
from the water molecules were located in a difference Fourier map
and refined freely with Uiso(H)¼1.5 Ueq(O). All interactions dem-
onstrated were found by PLATON program.11
ꢁ
tance of w1.2 A, whereas in the BA sequence, the overlapping mode
of neighboring cations shows that they are alternately shifted along
the shorter axis by a distance of w0.7 A and along the longer axis of
the acridine skeleton by a distance of w2.4 A. In the crystal lattice
ꢁ
Crystallographic data for the structures reported in this paper
have been deposited with the Cambridge Crystallographic Data
ꢁ