ꢀ
A. Sikorski, D. Trzybinski / Tetrahedron 67 (2011) 1479e1484
1483
asymmetric unit are present, and the second only when B ions
that form separate monolayers in
Supplementary data).
a
zigzag motif (Fig. S6,
aggregate in the tetramers. In both tetramers, only one O-atom
from the carboxy group is engaged in the hydrogen bond ring motif.
This atom is also involved in weak C(acridine)eH/O(carboxy)
hydrogen bonds, which stabilize the tetramers. The second O-atom
from the carboxy group is involved in an intramolecular OeH/O
hydrogen bond, where the hydroxyl groups are donors of H-atoms.
Despite the fact that there is no water molecule in the structure of
3, in contrast to the other compounds, this O-atom is involved in
the N(acridine)eH/O(carboxy) hydrogen bonds that link the tet-
ramers. In the crystal lattice of 3, the neighboring acridine skeletons
In comparison to the title compounds, in the crystal structure of
9-aminoacridine, which crystallizes as a hemihydrate,5 the mole-
cules are aggregated in tetramers via N(amino)eH/N(acridine)
hydrogen bond, forming the R22(8) hydrogen bond ring motif, as in 1
and 3 (Fig. 7a). The water molecule connects the tetramers to one
another by means of an O(water)eH/N(acridine) hydrogen bond.
It is interesting that there are no
pep interactions between the
acridine skeletons in the structure of the 9-aminoacridine mono-
hydrate. However, the acridine skeletons rotating around the center
are linked by
p
ep
interactions in the ABA arrangement forming
of symmetry interact through CeH/p interactions. In the crystal
chains (Fig. 6). This is caused by the fact that the adjacent acridine
skeletons are not shifted but rotated in-plane with respect to one
packing of the 9-aminoacridine monohydrate we can observe the
supramolecular helical tubes, which are not present in the lattices
of the title compounds (Fig. 7b).
another by approximately 130ꢁ. As a result of this rotation, the
pep
interactions between the acridine skeletons form a zigzag motif
ꢁ
with centroid/centroid distances in the 3.545e4.076 A range and
3. Conclusion
distance between mean planes of the neighboring acridine skeleton
ꢁ
3.405 A. In this arrangement, however, only two aromatic rings of
To conclude: we report on the structures of a series of 9-amino-
acridinium salts with aromatic carboxylic acids. Conformational
Analysis of the hydrogen bonds in the crystal lattices of the title
compounds shows that the cations and anions form tetramers and
that the building of anions influences the geometry of the hydrogen
bond ring motifs, which are observed in the crystal packing of all
compounds. The ions in these tetramers are linked via N(amino)e
H/O(carboxy) hydrogen bonds forming R22(8) (1 and 3) or R42(15) (2)
hydrogen bond ring motifs. We also observe that the presence of
different kinds of anion determines how acridine skeletons interact
between themselves in the crystal packing. The 9-AA cations interact
cation A are involved in the
neighboring B and A cations. Analysis of the centroid/centroid
distances in this sequence shows that the distance between one
pair of the lateral aromatic rings, equal to 4.325 A, is too long to be
classed as a pep interaction. Analysis of pep interactions between
the aromatic rings in the acid anions in 3 show that the shortest
centroid/centroid distances is 4.326 A. This indicates that the
-stacking interactions between benzene ring from the acid anions
p-stack interactions between the
ꢁ
ꢁ
p
are absent. In the supramolecular architecture of 2, there are chains
only through
rangementto formcolumns(1 and 2)orchains(3). Ontheotherhand,
analysis of interactions between the aromatic rings in the acid
pep interactions in the ABBA (1), AB (2) or ABA (3) ar-
pep
anions indicates that the shortest centroid/centroid distances are
ꢁ
4.521, 4.034, and 4.326 A in 1, 2, and 3, respectively. This shows that
the p-stacking interactions are either very weak (2) or absent alto-
gether (1 and 3).
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-
fraction data were collected on a Oxford Diffraction Gemini R ULTRA
ꢁ
Ruby CCD diffractometer with Mo K
a
radiation (
l
¼0.71073 A). In all
cases, lattice parameters were obtained by least-squares fit to the
optimized setting angles of the collected reflections by means of
CrysAlis CCD6 Datawere 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.7 All interactions demon-
strated were found by PLATON program.8
Crystallographic data for the structures reported in this paper
have been deposited with the Cambridge Crystallographic Data
Centre as supplementary publication no. CCDC-770732 (1), CCDC-
770733 (2), and CCDC-770734 (3). Copies of the data can be obtained
Fig. 7. Network of the intermolecular interactions in the crystal structure of 9-ami-
noacridine monohydrate: hydrogen bonds (a) and crystal packing (b).