´
73
A. Huczynski et al. / Journal of Molecular Structure 1032 (2013) 69–77
extracted with 10 mM TRIS base (Sigma–Aldrich, Germany) for
optical density reading of each well in Multiskan RC photometer
(Labsystems, Helsinki, Finland) at 540 nm wavelength.
The results are presented as the IC50 values: the concentration
of the agent tested which inhibits proliferation of 50% of cells pop-
ulation. IC50 values were calculated in Cheburator 0.4, Dmitry Nev-
ozhay software for each experiment and the results are presented
as a mean IC50 standard deviation calculated from each experi-
ments performed. The results are summarized in Table 5.
In the spectrum of LAS–BuA complex, the bands with maxima at
3379 cmꢀ1 and 3166 cmꢀ1 can be assigned to O(8)AHꢂ ꢂ ꢂO(1)ꢀ and
O(4)AHꢂ ꢂ ꢂO(2)ꢀ intramolecular hydrogen bonds on the basis of the
hydrogen bonds parameters collected in Table 2.
The most important information provided by the FT-IR spectra
concerning the structures of LAS–PhA and LAS–BuA complexes is
included in the region 1750–1500 cmꢀ1 (Fig. 3c). In the spectrum
of Lasalocid acid (dashed line) the band assigned to the
m(C@O)
vibrations of the carboxylic group is observed at 1652 cmꢀ1. In
the spectra of both complexes (solid and dashed-dotted lines,
respectively) this band is no longer observed and instead a new
complex band arises in the region below 1600 cmꢀ1 with maxima
at 1587 cmꢀ1 and 1571 cmꢀ1. This new composite band is a super-
3. Results and discussion
À
þÁ
position of the
m
as(COOꢀ), d NH3 and
m
(C@C) vibrations and its
3.1. Crystal structure of the Lasalocid–Phenylamine (LAS–PhA) and
Lasalocid–Butylamine (LAS–BuA) complexes
presence indicates a proton transfer from the carboxylic group of
LAS to the NH2 group of the respective amines within the complex.
The band assigned to the m(C@O) vibrations of the ketone group
The crystals of Lasalocid–Phenylamine (LAS–PhA) and Lasalo-
cid–Butylamine (LAS–BuA) complexes are isostructural. Both com-
plexes crystallise in the same space group and the crystals have
very similar unit-cell dimensions (Table 1). The unit-cell dimen-
sion a is longer by about 0.5 Å in LAS–PhA, but parameter c is more
than 1 Å longer in LAS–BuA, and the unit-cell volumes of both com-
pounds differ in only 5 Å3. It is characteristic that LAS anions as-
sume very similar pseudo-cyclic conformations, with the same
system of hydrogen bonds OAHꢂ ꢂ ꢂO, as illustrated in Fig. 1 and in
Table 2. The shortest of OAHꢂ ꢂ ꢂO bonds links hydroxyl group
O(3)AH and carboxylate oxygen O(1) (Table 2). The other two
O(8)AHꢂ ꢂ ꢂO(1) and O(4)AHꢂ ꢂ ꢂO(2) intramolecular hydrogen bonds,
are similar in length in LAS–PhA and in LAS–BuA complexes, too.
Likewise, the complexes host the PhA and BuA cations in a similar
manner (see Table S1, Supplementary material). They are included
in the void inside the pseudo-cyclic structure, with practically
identical position of the nitrogen atom. The location of the N-atoms
is fixed by intermolecular NAHꢂ ꢂ ꢂO hydrogen bonds to LAS oxygen
atoms O(2), O(6) and O(8) (Fig. 1 and Table 2). These host-guest
NAHꢂ ꢂ ꢂO hydrogen bonds additionally stabilize the LAS conforma-
tion. The crystal packing of LAS–PhA and LAS–BuA is similar
(Fig. 2), and dominated by van der Waals interactions.
in Lasalocid and its both complexes is observed at ca. 1712 cmꢀ1
indicating that this group is not involved in any hydrogen bond.
Formation of protonated 1:1 LAS–BuA and LAS–PhA complexes
in chloroform solution is indicated by their ESI-MS spectra (Fig. S1,
supplementary data) in which at cv = 10 V only one signal at m/
z = 664 and 684 respectively, characteristic of such complexes, is
observed.
Comparison of the FT-IR spectra of LAS–BuA complex in chloro-
form and in the solid state (Fig. 4) shows small changes associated
only with changes in hydrogen bond strength, indicating that in
the solution the crystal structure is practically conserved. Protonic
vibrations within the O(8)AHꢂ ꢂ ꢂO(1)ꢀ and O(4)–Hꢂ ꢂ ꢂO(2)ꢀ hydro-
gen bonds are indicated by a broad band in the same region in
which the respective vibrations in the spectrum of the crystalline
LAS–BuA complex are found.
In Fig. 5 the spectra of LAS–PhA complex in chloroform and in
the solid state and the spectrum of LAS in solution are compared
showing very strong changes. The spectral features of the complex
in solution compared with those in the spectrum of LAS indicate
clearly a partial dissociation of the complex with formation of
Lasalocid acid. This statement is proved by the appearance of a
band at 1653 cmꢀ1, 3597 cmꢀ1 and a shoulder at 3430 cmꢀ1 as well
as by the 1H and 13C NMR data of LAS and its complexes given in
Table 3. Most informative are the signals of the C(1) atom of the
carboxylic group and its C(2) neighbouring atom. In the 13C NMR
spectrum of LAS the signal of C(1) atom is found at 173.2 ppm
and in the spectrum of LAS–BuA at 175.4 ppm due to the proton
transfer from the carboxylic group to the amine group. In the spec-
trum of LAS–PhA the respective signal is observed at 174.4 ppm
indicating that the proton transfer process is incomplete. The same
conclusion follows from a comparison of the chemical shifts of C(2)
carbon atom.
3.2. Spectroscopic studies
In Fig. 3 the FT-IR spectra of crystalline Lasalocid acid (dashed
line) and its crystalline complexes with phenylamine (LAS–PhA)
(solid line) and butylamine (LAS–BuA) (dashed-dotted line) are
compared. We observe clear differences between these structures,
especially regarding the formation of hydrogen bonds (Fig. 3b).
According to the X-ray data, in the spectrum of the LAS–PhA
and LAS–BuA complexes, the bands labelled in Fig. 3b should be as-
signed to the inter- and intramolecular hydrogen bonds of different
strength that exist within the structure of these complexes. The
hydrogen bonds and their parameters are given in Table 2. The
strongest hydrogen bond observed in both complexes is formed
between the O(3)AH group and the O(1) atom of the carboxylic
group, in LAS–BuA it is more symmetrical than in the LAS–PhA
structure. These intramolecular hydrogen bonds belong to the so
called quasi-aromatic hydrogen bonds [28] characterized by very
low intensity and limited shape of the band assigned to the
stretching protonic vibrations occurring usually in the region ca.
2200–3000 cmꢀ1 [29,30]. Thus, the broad band with maxima at
The analysis of the shift of the 13C NMR signal assigned to the
carbon atom of ketone group from 214.4 ppm (LAS) to 217.8 ppm
(LAS–BuA complex) or 216.3 ppm (LAS–BuA complex) can indicate
that oxygen atom of carbonyl group interacts with the hydrogen
atoms of protonated amines by weak hydrogen bond. On the other
hand, the band assigned to the C@O stretching vibrations in the FT-
IR spectra of both complexes shifts very slightly toward lower
wave numbers in comparison with the position of this band in
the FT-IR spectrum of LAS. Thus, it seems that carbonyl group is
À
Á
not engaged in the hydrogen bond formation with NHþ3 group
and the shifts of the 13C NMR signal carbonyl carbon atom is con-
nected with conformational changes of LAS molecule after com-
plexation of the respective amines.
À
Á
2595 cmꢀ1 and 2310 cmꢀ1 should be assigned to the
m
NHþ3 vibra-
tions of the protonated and hydrogen bonded amine group.
According to the crystal data (Table 2) in the spectrum of the
LAS–PhA complex, the bands with maxima at 3394 cmꢀ1 and
3062 cmꢀ1 are assigned to O(4)AHꢂ ꢂ ꢂO(2)ꢀ and O(8)AHꢂ ꢂ ꢂO(1)ꢀ
intramolecular hydrogen bonds, respectively.
The dissociation of LAS–PhA complex in solution is also con-
À
Á
firmed by the proton signals assigned to NHþ3 in the spectrum
of the complex at 9.34 ppm and of the free, non-hydrogen-bonded
NH2 protons of the aniline molecule at 3.80 ppm. The dissociation