The cytotoxic properties of cytotoxins (CTs) from snake venom are mediated by their interaction with the cell membrane. The hydrophobic pattern containing the tips of loops I-III and flanked by polar residues is known to be a membrane-binding motif of CTs. However, this is not enough to explain the difference in activity among various CTs which are similar in sequence and in 3D structure. The mechanism of further CT-membrane interaction leading to pore formation and cell death still remains unknown. Published experimental data on the specific interaction between CT and low molecular weight anionic components (sulphatide) of the bilayer point to the existence of corresponding ligand binding sites on the surface of toxin molecules. In this work we study the membrane-lytic properties of CT I, CT II (Naja oxiana), and Ct 4 (Naja kaouthia), which belong to different structural and functional types (P- and S-type) of CTs, by measuring the intensity of a fluorescent dye, calcein released from liposomes containing a phosphatidylserine (PS) lipid as an anionic component. Using molecular docking simulations, we find and characterize three sites in CT molecules that can potentially bind the PS polar head. Based on the data obtained, we suggest a hypothesis that CTs can specifically interact with one or more of the anionic lipids (in particular, with PS) contained in the membrane, thus facilitating the interaction between CTs and the lipid bilayer of a cell membrane.
The cytotoxic properties of cytotoxins (CTs) from snake venom are mediated by their interaction with the cell membrane. The hydrophobic pattern containing the tips of loops I-III and flanked by polar residues is known to be a membrane-binding motif of CTs. However, this is not enough to explain the difference in activity among various CTs which are similar in sequence and in 3D structure. The mechanism of further CT-membrane interaction leading to pore formation and cell death still remains unknown. Published experimental data on the specific interaction between CT and low molecular weight anionic components (sulphatide) of the bilayer point to the existence of corresponding ligand binding sites on the surface of toxin molecules. In this work we study the membrane-lytic properties of CT I, CT II (Naja oxiana), and Ct 4 (Naja kaouthia), which belong to different structural and functional types (P- and S-type) of CTs, by measuring the intensity of a fluorescent dye, calcein released from liposomes containing a phosphatidylserine (PS)lipid as an anionic component. Using molecular docking simulations, we find and characterize three sites in CT molecules that can potentially bind the PS polar head. Based on the data obtained, we suggest a hypothesis that CTs can specifically interact with one or more of the anionic lipids (in particular, with PS) contained in the membrane, thus facilitating the interaction between CTs and the lipid bilayer of a cell membrane.
One of the features of cytotoxins (CTs, sometimes called cardiotoxins) from snake venom is
their toxicity to cells of various types [1]. CTs are
small basic proteins from the three–finger toxin group. The secondary structure of CTs
consists of two β –sheets that have 2 and 3 antiparallel β –strands and
is stabilized with 4 disulphide bonds. The major differences between the amino acid sequence
and the 3D structure of members of this large CT group occur in irregular loop
segments, primarily in loops I and II. Depending on the presence of the conservative residues
S28 (S–type) or P30 (P–type) in loop II, CTs exhibit different functional
activities [2]. For a long time, CTs were believed to
interact with the cell membrane in a nonspecific way. P–type CTs interact with the
bilayer more actively than S–type CTs due to the more hydrophobic loop II, resulting in
an extended hydrophobic region on the toxin ’ s surface formed by the hydrophobic tips of
the three loops. The amphiphilic properties of CT molecules (the hydrophobic
ends of loops I–III are flanked with cationic residues) enable their embedding into the
lipid bilayer, creating porous defects in the membrane [3-6] and leading to the cell death.
Several models of the mechanism of bilayer damage by CT and lysis have been
proposed [7]. It was shown later that some CTs, for
instance the CT А3 ( Naja atra ), can penetrate
inside the cell and interact with cell organelles, mitochondria [8], and lysosomes [9].The biological activity of CTs is very diverse. In particular, they can modify the function of
various membrane proteins, such as protein kinase C (PKC), Na+,
K+–ATPase , and integrins. Therefore, the hypotheses about the specific
CT targets and molecular mechanisms of toxin–membrane interaction are of
interest and have been actively discussed [7, 10–12].Based on NMR and X–ray data, a search for potential CT
targets revealed a series of anionic low molecular weight ligands (heparin–derived
oligosaccharides, ATP derivatives, and sulphatide) that interact with certain sites on the
toxin’s surface [13-17]. Fluorescent spectroscopy studies on liposomes of various composition
combined with in vivo experiments using monoclonal antibodies indicate a
specific CT target—a polar head of a glycolipid sulphatide
(hSGC)—located on the surface of a rat’s cardiomyocyte membrane, which mediates the
toxic activity of CT А3 [17].
Taking into account the fact that CTs affect various cell types and that toxins effectively
lyse model membranes containing no glycolipids [5, 18, 19], one can expect
CT to be able to interact nonspecifically with other anionic membrane lipids,
including the most common one, phosphatidylserine (PS). Although this lipid is
normally localized in the inner leaflet of the cell membrane, when the bilayer is damaged in
certain pathologies, PS is present in the outer leaflet and can be accessible
to CT molecules. Some experimental data indirectly support the possibility
that there is competition for a site on the membrane’s surface between
CT and other PS–binding molecules
(PKC, thionin) [10, 20, 21].In this work we assumed that PS is a specific target mediating
CT cell toxicity and studied the interaction of S–type
(CT I from Naja oxiana) and P–type
(CT II from Naja oxiana and CT 4 from
Naja kaouthia) cytotoxins with palmitoyl oleyl phosphatidylcholine
(POPC) membranes, including those containing PS and
SGC. It should be noted that the primary structure of CT 4
(N. kaouthia) is identical to that of CT А3
(N. atra ). Using fluorescent spectroscopy, we studied the lytic activity of
the selected CTs on liposomes of various composition. In order to identify sites in a
CT molecule capable of binding PS, we performed molecular
docking simulations of the PS polar head using 3D models of toxins active with
respect to PS–containing liposomes. Based on the results obtained, we
hypothesized that toxins interact with the bilayer via a two–stage
specific mechanism, the molecular determinants of which are the polar heads of the anionic
lipids, which interact with specific CT sites.
EXPERIMENT
Fluorescent Spectroscopy: .
CT I and CT II were extracted from N. oxiana
venom following the technique described in [22;]. CT 4 was extracted from N. k
aouthia venom using the technique proposed in [23] and refined by reverse phase chromatography. The toxin’s structure
was confirmed by mass–spectrometry using peptide mapping after the trypsin hydrolysis of
the reduced pyridylethylated toxin derivative. Liposomes were prepared using
SGC and PS extracted from bovine brain in the Laboratory of
Lipid Chemistry, Institute of Bioorganic Chemistry, Russian Academy of Sciences (IBC RAS), and
synthetic POPC (Avanti Polar Lipids, United States). Liposomes of the
following composition were prepared: POPC, POPC /PS5 %, POPC
/PS2 0%, POPC /PS3 5%, POPC /PS50 %, POPC
/PS7 0%, POPC /SGC5 %, and POPC /SGC50 %. Lipid solutions in
chloroform/methanol (1:1) at appropriate concentrations were mixed, evaporated, and dried in
vacuum. The lipid films were hydrated with a buffer containing 5 0 m M
tris–НСl (pH 7.8), 30 mM NaCl, 4 mM EDTA, and 100 mM calcein. The suspension
was incubated for several hours, subjected to 10 freeze/thaw cycles, and then forced through a
100–nm polycarbonate filter (NucleoPore, USA) 20 times using a mini–extruder
(Avanti Polar Lipids, United States). The external dye was eliminated by gel filtration using a
Sepharose СL–4B column equilibrated with a buffer containing 50 mM
tris–НСl (pH 7.8), 11 0 mM NaCl, and 4 mM EDTA. In addition, the activity of
CT 4 with respect to SGC–containing liposomes
(POPC/SGC50%) was measured under the conditions described in [6] (buffer: 10 mM tris–НСl (p H 7 .4), 75 mM
NaCl; 50 mM 6–carboxyfluorescein (6–CF) as fluorophore;
lipid/protein ratio (L/P) ~62). The level of liposome membrane damage by CTs
was estimated from spectrophotometric measurements of the amount of fluorophore released from
inside the liposomes, I , upon adding an aliquot of the toxin solution into
the quartz cuvette with the liposome sample. The value of I (%) was
calculated using the following equation:I = 100 x ( F – F ) / (
F ),where F is the fluorescent signal from liposomes without the
toxin (background level); F is the fluorescent signal from liposomes in the
presence of the toxin; and F is the fluorescent signal after the
liposomes have been destroyed with a detergent (Triton X–100).The L/P ratio in all experiments was 100, unless otherwise stated. The
fluorescent signal was measured at 517 nm, with excitation at 494 nm, and the spectral slit
width for excitation and emission was 3 and 5 nm, respectively. For each experiment, the
kinetics of the fluorescent signal was monitored (for about 40 min) and the final measurements
were taken when I reached a plateau. For reproducibility control, all
measurements were repeated 2–3 times. All measurements were performed at room temperature
using HITACHI F4000 (Japan) spectrofluorimeter.Molecular Docking of . Molecular docking simulations using GOLD 2.0 software [24] were performed to identify PS binding
sites on the surface of CT molecules.In our simulations, we used a crystallographic model of the 3D structure of
CT А3 from N. atra venom (PDB code:
2BHI) [17] and NMR models of
CT II in hydrated state (PDB code: 1CB9, models 1, 14 and 18)
[25] and in the presence of dodecylphosphocholine
(DPC) micelles (PDB code: 1FFJ, models: 1 and 10) [4].In order to account for the receptor’s conformational mobility, we used a series of 3D
models representing the dynamic behavior of the toxins in media of different polarities.
Starting from experimental toxin models, we obtained representative sets of corresponding 3D
models of CT 4 and CT II by molecular dynamics simulations in
aqueous media and by Monte Carlo conformational search for finding low–energy states in
the presence of the implicit membrane (data not published).The phosphatidylserine polar head (hPS) used in the simulations included all
atoms of this lipid’s polar head group with СН3 groups, instead of
fatty acid residues (Fig. 1A). hPS
docking simulations were performed for 16 and 15 spatial models of CT 4 and
CT II, respectively.
Fig. 1
(a) 3D model of the PS polar
head (hPS) used in molecular dock-
ing simulations. Functional groups are
indicated. (b–h): Molecular docking
solutions for hPS bound in the M site
of (b, d) CT 4 and (c) CT II, in the L3
site of (e) CT II and (f) CT 4, and in the
L1 site of (g) CT II and (h) CT 4. 3D
models of the toxins are shown in a
ribbon representation. The membrane
binding hydrophobic residues of loops
I–III (designated with roman numbers),
backbone and/or side chain atoms
of the site-forming residues, and one
of the preferred conformations of hPS
in the related sites are displayed as
stick diagrams. To demonstrate the
diversity of hPS positions in the sites,
the corresponding locations of the hPS
phosphate group are also shown in
stick representation for other docking
solutions from the TOP10 set. Amino
acid residues forming the sites are
marked with a one-letter code, with a
residue number and a standard color-
ing scheme for the atom types. The
phosphate group and carbon atoms of
hPS are pink and cyan, respectively.
(b) Different positions of hPS in the
site M_Y51 of CT 4 found among the
TOP10 docking solutions. A hypotheti-
cal migration path of hPS from the M_
Y51 site towards the M site is shown
by arrows. The phospholipid bilayer is
depicted as the shadow region under
the horizontal line. The location of CT
4 relative to the membrane’s interface
(the horizontal line) corresponds to the
proposed mode of CT binding to the
lipid membrane.
(a) 3D model of the PS polar
head (hPS) used in molecular dock-
ing simulations. Functional groups are
indicated. (b–h): Molecular docking
solutions for hPS bound in the M site
of (b, d) CT 4 and (c) CT II, in the L3
site of (e) CT II and (f) CT 4, and in the
L1 site of (g) CT II and (h) CT 4. 3D
models of the toxins are shown in a
ribbon representation. The membrane
binding hydrophobic residues of loops
I–III (designated with roman numbers),
backbone and/or side chain atoms
of the site-forming residues, and one
of the preferred conformations of hPS
in the related sites are displayed as
stick diagrams. To demonstrate the
diversity of hPS positions in the sites,
the corresponding locations of the hPSphosphate group are also shown in
stick representation for other docking
solutions from the TOP10 set. Amino
acid residues forming the sites are
marked with a one-letter code, with a
residue number and a standard color-
ing scheme for the atom types. The
phosphate group and carbon atoms of
hPS are pink and cyan, respectively.
(b) Different positions of hPS in the
site M_Y51 of CT 4 found among the
TOP10 docking solutions. A hypotheti-
cal migration path of hPS from the M_
Y51 site towards the M site is shown
by arrows. The phospholipid bilayer is
depicted as the shadow region under
the horizontal line. The location of CT
4 relative to the membrane’s interface
(the horizontal line) corresponds to the
proposed mode of CT binding to the
lipid membrane.For each CT model, 50 complexes (docking solutions) were obtained, among
which 10 with the best “gold score” criterion [26] (TOP10) were used for further analysis. Thus, for CT 4
and CT II, 160 and 150 ТОР10 solutions in total were
selected, respectively. We made decisions about hPS binding sites at
CT by analyzing the localization of hPS on the toxins
molecule’s surface and the frequency of occurrence of corresponding complexes in the
ТОР10 solutions. The hPS surface is polar; therefore,
hydrogen bonds and electrostatic forces contribute most to the lipid–toxin complex
energy. The docking solution sets were analyzed with respect to the number and distribution of
hydrogen bonds and ionic contacts (those with distances between ionic groups below 6 Å ) in
order to identify the key residues involved in the interaction with hPS in
most of the complexes.The presence of hydrogen bonds and ionic interactions was estimated using the PLATINUM [27] and GROMACS 3.3.1 [28] software packages.
RESULTS
Fluorescence Measurements: .Dependence of . In this work, we estimated the lytic
activity of P– and S–type toxins, namely CT II ( N.
oxiana ; ), CT 4 ( N. ka
outhia
), and CT I ( N. oxiana ) by the amount of organic dye
calcein released from POPC, POPC/PS5%, and POPC/SGC5%
liposomes. CT I (S–type) shows almost no activity with respect to both
neutral liposomes (POPC) and those containing minor quantities of anionic
lipids (PS, SGC) (Fig. 2): in all cases
intensity of the released calcein, I , was below 5%. In experiments with
CT II (Р–type), the release intensity of dye was higher (compared
to the results obtained with CT I), average I values being
below 10% regardless of the liposome composition (Fig. 2).
Fig. 2
CT-induced release of fluorescent dye calcein from liposomes of different compositions: (a) pure POPC; (b) POPC/PS5%,
and (d) POPC/SGC5% after addition of CT I, CT II (Naja oxiana), and CT 4 (Naja kaouthia). (c) Kinetics of 6-CF fluorescence during
the initial few minutes after addition of CT II and CT 4. For this measurement, (c) the experimental conditions, such as buffer composi-
tion, fluorophore and lipid/protein concentrations (10/0.16 µM) in the sample correspond to those in [6]. The data for 6-CF release
induced by CT A3 (Naja atra) reported in [6] are shown as (_ .. _).
CT-induced release of fluorescent dye calcein from liposomes of different compositions: (a) pure POPC; (b) POPC/PS5%,
and (d) POPC/SGC5% after addition of CT I, CT II (Naja oxiana), and CT 4 (Naja kaouthia). (c) Kinetics of 6-CF fluorescence during
the initial few minutes after addition of CT II and CT 4. For this measurement, (c) the experimental conditions, such as buffer composi-
tion, fluorophore and lipid/protein concentrations (10/0.16 µM) in the sample correspond to those in [6]. The data for 6-CF release
induced by CT A3 (Naja atra) reported in [6] are shown as (_ .. _).Fluorescence measurements showed that CT 4 had the strongest damaging effect
on all the liposome types studied (Fig. 2). With this
toxin, a clear trend is visible: its activity depends on the presence and type of the anionic
component in the liposome. Thus, the value of I for neutral liposomes was
only ~10%, whereas for SGC–containing vesicles it was 30%. The highest
CT 4 activity was measured for POPC/PS5% liposomes, with dye
release reaching 50%. It should be noted that there was also a significant difference in the
activity of individual toxins with respect to the anionic lipids in liposomes. For instance,
CT II does not differentiate between PS– and
SGC–containing liposomes, while the lytic activity of
CT 4 with respect to POPC/PS vesicles is almost twice as high
as that with respect to SGC–containing ones (Figs. 2B, D).It is interesting that we did not find a specific interaction between SGC
molecules and CT 4 (which is identical to CT А3 from
N. atra venom). Moreover, when we reproduced the experimental conditions
described in [6] (see the Experiment section), the value
of I after a few minutes of incubation was less than 10%, unlike the >70%
reported in [6] (Fig.
2C). The authors of [6] used
6–CF fluorofore, which, due to its lower molecular charge, is prone to
spontaneously releasing from liposomes (A.V. Feofanov, private communication).We measured I for the
interaction of CT I, CT II, and CT 4 with
POPC liposomes containing varying amounts of PS (20, 35, 50,
and 70%) and studied the dependence of the lytic efficiency on the anionic lipid concentration.
The latter turned out to be similar for all three toxins; in particular, there was a maximum in
I at 20% PS (Fig. 3)
for all CTs. The toxicity trend CT 4 >; CT II >;
CT I stays the same for all liposome types at the given lipid/protein ratio
(L/P = 100). The lytic effect of CT 4 and, especially,
CT II increases drastically for liposomes POPC/PS20% (over 90
and 70%, respectively). At lower (5%) and higher (35% and more) PS contents,
the drop in the activity curve I is more pronounced for CT
II than for CT 4. CT I shows low lytic activity in the entire
range of PS contents in the liposomes, with a weak maximum at PS20% (Fig. 3).
Fig. 3
Dependence of the CT-induced calcein release, I (%), on
the PS content (in %) in the POPC liposomes. The fluorescence
measurements were performed 10 min after the addition of the
toxins. The values of I are calculated (see the Experiment sec-
tion) and averaged for 2–3 measurements.
Dependence of the CT-induced calcein release, I (%), on
the PS content (in %) in the POPC liposomes. The fluorescence
measurements were performed 10 min after the addition of the
toxins. The values of I are calculated (see the Experiment sec-
tion) and averaged for 2–3 measurements.To explain the observed effects, we assumed a uniform distribution of PS in
the liposomes and calculated the number of PS molecules per toxin molecule in
liposomes of various composition that were 100 0 Å in diameter . It appeared that the number of
PS molecules for liposomes, with respect to which CTs show the maximum
activity, is the same as the number of potential binding sites for the lipid head found in
molecular docking simulations. In the case of complete toxin binding at L/P =
100, the liposome charge is compensated in the POPC/PS20% liposomes. Thus,
there are 10–12 PS molecules (on average, 3.5 PS at the
toxin’s binding site) per each toxin molecule. There are 50–60 lipids in total per
each toxin, and 16–18 lipids are located in direct proximity to the contact region with
toxin.For comparison, in the POPC/PS5% liposomes, charge compensation occurs at
very low CT concentrations (L/P ~300); therefore, at a higher
toxin content (L/P = 100), some CT molecules may not bind to
the membrane. However, even if there is complete CT binding to the
POPC/PS5% liposome surface, there may not be a single PS
molecule at the toxin/lipid contact region (on average, there are 0.8 PS
molecules per surface area in contact with a toxin molecule).Molecular Docking. As a result of molecular docking simulations of
hPS into 3D models of CT 4 and CT II, three
hPS binding sites (referred to further as М, L3, and L1) consisting
mainly of conservative residues were found on the surfaces of both toxins. One feature of the
complexes that were formed is the multivariant positioning of the ligand in the sites (Fig. 1), which is due to the presence of several
donor–acceptor groups capable of forming hydrogen bonds in both the ligand and the
receptor.The M site. The M site is the most frequently occurring one among the
ТОР10 docking solutions; it is present in 75 and 60% of solutions for
CT 4 and CT II, respectively (Fig. 4). The site M includes a “lysine” cluster (K5, K12, K18, K35)
surrounding the polar surface (the site’s bed), which is formed by the backbone atoms of
the residues L6, R36, G37, C38 and Y22 OH–group (Figs. 1C,
D). In more than 60% of solutions for both toxins, there are three or more hydrogen
bonds between key residues of the site М (K12, Y22, R36, and C38) and
hPS and, usually, several ionic contacts.
Fig. 4
Distribution histogram of docking solutions for the hPS
binding sites (М, М_Y51, L3, L1) in CT II (grey) and CT 4 (black)
molecules. The best scoring solutions (TOP10) for both toxins
are presented.
The mobility of side chains of lysine residues makes site M compatible with different
hPS conformations (Figs. 1C, D). This
site is present in the ТОР10 docking solutions for most CT 4
and CT II models, including the toxin structures determined experimentally.In contrast to CT II, in the ТОР10 set for
CT 4, there is a group of solutions (further referred to as М_Y51) in
which the Y51 residue’s hydroxyl group is involved in binding of the lipid head (Figs. 1B, 2D). In most
М_Y51 solutions (10 out of 16 complexes), the hPS tail is oriented
towards the tip of loop III (Fig. 1B). In the other
М_Y51 solutions, the hPSglycerine group is oriented towards loop I with
fewer hydrogen bonds with the ligand. Therefore, in this group of solutions, the ligand’s
position is intermediate between those in the M_Y51 and М sites. In this case, Y22 is a
key residue with which the ligand interacts ( via the hydrogen bond) during
the supposed migration from the М_Y51 to the М site (Fig. 1B).The L3 and L1 sites.
In addition to the major (in the number
of solutions) site М, there are two sites in the ТОР10 set, L1 and L3,
located on the concave side of the CT molecule surface near loops I and III,
respectively. The frequency at which these sites occur among the TOP10 docking solutions is
different for CT II and CT 4 (Fig. 4).Distribution histogram of docking solutions for the hPS
binding sites (М, М_Y51, L3, L1) in CT II (grey) and CT 4 (black)
molecules. The best scoring solutions (TOP10) for both toxins
are presented.The L3 site is formed by the bakbone atoms of the P43, Y51, C53, and S45 conservative
residues, as well as by the side chain of the S45 residue. In most of the
CT–hPS complexes, P43 and Y51 carbonyl groups and the S45
ОН–group fix the position of the ligand’s NH3+
group by forming a hydrogen bond (Figs. 1E, 1). In some solutions, the hPSglycerine
residue is oriented towards the tips of loops I–III and the K44 and K50 side chains are
near the hPSphosphate group (Fig. 1F).The site L1 and CT 4/CT II represents a region with high
electrostatic potential containing side chains of the N4/K4, K23, R36, R58/K58, and N60
residues, which form favorable electrostatic contacts with hPS. In most
docking solutions obtained for CT II and CT, the
hPS NH3+ group is located near the N60 residue, forming
a hydrogen bond with the side chain carboxyl or carbonyl group (Figs. 1G, 1H). The hPS molecule accommodates various
orientations with respect to the toxin molecule and suggested bilayer, including those
corresponding to the lipid position in the bilayer (Fig.
1G).
DISCUSSION
The functional activity of cytotoxins arises from their interaction with the cell membrane;
however, the mechanism of this interaction at the molecular level is still unknown. The
oligomerisation of CTs necessary for forming pores in the membrane [5, 6] takes place not in solution, but
apparently in the vicinity of the membrane; the details of this process and the geometry of the
supramolecular complex are unclear. Understanding the initial stages of the
toxin–membrane interaction is extremely important for understanding the entire mechanism
of cytotoxic activity.The data obtained in this study on the release of calcein from the POPC,
POPC/PS5%, and POPC/SGC5% liposomes, depending on the CT type
(Р– or S–), correlate with the hypothesis that the properties of the
membrane–binding motif (tips of loops I–III) influence the CT
lytic activity with respect to the cell membranes. P–type CTs are known to more actively
interact with the bilayer [2, 29, 30]. Indeed, both of the
Р–type CTs studied, CT II and CT 4, demonstrated
more pronounced lipolytic behavior (on POPC/PS5% and
POPC/SGC5%) than CT I, for which intensity of the released
dye did not exceed 5%. It has been suggested that, due to the presence of polar residues in
loop II (S28 and D29 in CT I) of the S–type CTs, their interaction with
the bilayer involves fewer residues, primarily those of loop I [2, 31]. For identical bilayer embedding
geometry, the calculated free energy of binding is higher for CT I than for
CT II [30].The experiments also showed that all the toxins studied were most active with respect to
PS–containing liposomal membranes, and that the dye–release
dependencies on the PS content were of dome shape and with the highest lysis
intensity for the POPC/PS20% liposomes. An estimation of the number of
PS molecules in 1000– Å diameter liposomes at L/P = 100
suggests that the lysis intensity peak can be reached when there are no less than three
PS molecules on the surface of the bilayer in contact with the toxin during
embedding. Under such conditions, the difference in the intensity of the released dye for
CT 4 and the significantly less active CT II is minimal (90
and ~70%) compared to the case of liposomes with a PS content other than 20%.
We can speculate that the optimum PS content for lysis that ensures the
involvement of all three toxin sites is very important for the efficiency of
toxin–membrane interaction. The weak response observed for the nearly inactive
CT I is, perhaps, due to the fact that that this toxin does not embed deep
enough into the bilayer and/or because of the different binding geometry involving only one or
two loops, resulting in a lower availability of sites for binding with PS.The drastic decrease of the POPC/PS5% lysis efficiency indicates that the
mechanism that binds the highly basic toxin with the anionic membrane includes nonspecific
electrostatic attraction. As a result, due to the low membrane charge density and too few
PS molecules as potential ligands (less than one per toxin–membrane
contact region), the CT does not embed into the bilayer efficiently.The observed decrease in CT 4 and CT II activity with
respect to liposomes with PS contents of 35% and higher is most likely caused
by a change in the bilayer’s properties, in particular, by an increase in the lipid
packing density near the interface. For instance, the formation of mini–clusters of
PS molecules becomes more probable. According to the data of molecular
dynamics simulations for bilayers containing 20 and 50% PS, in the latter case
there are twice as many hydrogen bonds between PS polar heads near the
interface (data not published).The estimated number of PS molecules in the POPC/PS20%
liposomes interacting with CTs is the same as the number of the toxin
PS–binding sites predicted by molecular docking simulations. It should
be also noted that the embedding of the hydrophobic tips of loops I–III of the toxins
studied into the lipid bilayer has been confirmed by NMR data on
CT II [4] and CT
А3 ( N. atra ) [6] in micelles.The M site (residues K5, K12, K18, Y22, R36, and C38), presents in most docking solutions, is
identical to the sulphatide–binding pocket located on the convex side of the toxin
molecule [17]. Indeed, the results of a chemical
modification of lysine and tyrosine residues suggest that the site’s key residues, such
as Y22 and K12, significantly influence the functional activity of CTs [32, 33]. Judging by the number of
intermolecular hydrogen bonds and ionic contacts in the docking solutions, the M site has the
best potential for forming a stable complex with the ligand. Formation of the
CT A3–SGC complex in of a membrane–mimicking
environment [17] indicates that other anionic components
in the membrane can bind to the M site. At the same time, the superimposition of
CT docking models, according to the mode by which they are embedded into the
bilayer, indicates different availabilities of the sites for the PS head. For
instance, the M site residues do not directly interact with the bilayer. In order to reach the
M site, the lipid molecule must overcome the energy barrier so that the acyl part of the lipid
will penetrate the polar interfacial zone.It is interesting that, in the М_Y51 docking models for CT 4, the lipid
binding site assumes a hydrogen bond between the lipid NH3+ group and
ОН groups of both tyrosine residues, Y22 and Y51, the phosphate group being near
the membrane’s surface. Therefore, we can expect that lipids reach the М_Y51 site
faster than they reach the M site. Moreover, the existence of M_Y51 solutions differing in the
involvement of the M site’s key residues and the orientation of the lipid’s
glycerin residue can indicate a possible migration path of the lipid head from the М_Y51
site to the M site.There is no direct experimental evidence of the existence of the L3 and L1 sites revealed by
docking simulations. On the other hand, the L3 site located near loop III has a structure
similar to that of the M site: the backbone atoms of this site’s residues (P43, Y51, and
C53) form hydrogen bonds with the lipid’s polar head, which is additionally supported by
an electrostatic interaction with the ionic groups of lysine residues (K44 and K50). Recently,
a consensus sequence L/PKSSLL based on a peptide sequence alignment (related to antibodies
neutralizing N. atra venom) revealed by phage display has been proposed as
an epitope involved in the action of CT A3 from N. atra
venom [34]. This epitope corresponds to a fragment of
the loop III sequence and contains the L3 site residues (P43–S45). The L3 site is the
least available for PS in the bilayer, taking into account the
CT–membrane binding mode. It is possible that, during later stages of
embedding, when CT penetrates deeper and this site becomes more available,
binding an additional lipid strengthens the CT–membrane interaction.In contrast, among docking solutions for the L1 site (a polar cluster comprised mainly of
charged residues at the base of loops I and II) there are models of complexes with
hPS in the membrane–water interfacial zone (in case CT
loops embed into the membrane). This indicates the availability of this site for the bilayer
hPS. There have been reports of NMR studies showing that some
L1 site residues take part in dATP binding [16].It is interesting to note that just five amino acid substitutions turn CT II
into the much more lytically active CT 4 (Fig.
5); the total charge of the molecule (+9) is the same for both CTs. It is not surprising
therefore that, along with a high sequence homology and similar 3D structure, the docking
results for the two CTs are also very similar, differing only in the frequency at which the
sites occur among the docking solutions. Four out of five amino acid substitutions are
localized near the L1 site (more frequently in the case of CT II), and three
of them—in the areas most important for the toxin—are in loops I and II. Thus, the
positive charge in CT II (K4/N4 in CT II/CT
4) is transferred to loop II (H31/K31 in CT II/CT 4) in
CT 4. On the one hand, this disturbs the hydrophobic pattern of loop II; on
the other hand, lysine residues are known to anchor at the interface by interacting with the
lipid phosphate groups [35], which may reduce the
protein dissociation constant. A correlation has been found between the presence of a positive
charge at the tip of loop II and CT hemolytic activity [36]. Although the K4/N4 and K58/R58 substitutions in toxins are localized
relatively far from the membrane surface (assuming that the CT embeds with the
tips of loops I–III), both residues are parts of the L1 site and form a hydrogen bond
and/or ionic contact with the lipid’s serine head in the docking solutions. The S11/Y11
substitution increases the hydrophobicity of the CT 4’s loop I by
enabling the coupling of the F10 and Y11 aromatic residues, which can act as a good hydrophobic
anchor. We can speculate that, due to the less favorable binding conditions in the M_Y51 site
(manifested by the absence of this site among the ТОР10 solutions for
CT II), the availability of the M site for the anionic lipid head is less for
CT II. The local conformational differences between CT II and
CT 4 can also contribute to the rearrangement of the hPS
binding locations for the L1 and L3 sites. At the same time, it is obvious that the simulation
data are not sufficient for a qualitative estimation of the possible changes of the lipid
binding constants for the predicted sites and, therefore, for a detailed explanation of the
differences in the CT II and CT 4 activities.
Fig. 5
Sequence alignment for CT I, CT II, CT 4, and CT A3. The β-strands are indicated by b. Amino acid substitutions between CT
A3 and CT 4 are underlined.
Sequence alignment for CT I, CT II, CT 4, and CT A3. The β-strands are indicated by b. Amino acid substitutions between CT
A3 and CT 4 are underlined.Also, we would like to note that our experiments on the release of calcein from the
POPC/SGC5% liposomes and reproducing the experimental conditions described in
[6], where 6–CF was used as
fluorophore, did not reveal any high affinity of CTs (in particular, CT 4)
with respect to SGC, which was in disagreement with the data published in
[6]. At the same time, the existence of the X–ray
CT A3–SGC complex confirms that various anionic
components in the membrane can bind to the M site, and experiments with
SGC–specific antibodies and enzymes reveal a dependence between the
CT A3 functional activity and the presence of SGC in the
membrane [17]. This glycolipid is present in low
concentration in the outer membrane leaflet of rat cardiomyocytes, hence the big interest in
SGC as a potential CT target. The low reproducibility of the
results achieved on model membranes, in addition to the importance of technical details (e.g.,
the nature of dye), emphasizes the need to exercise caution when extrapolating to cells the
results obtained using model systems. The functional activity of a toxin is likely to arise due
to a number of factors that are not at all limited to the affinity to various membrane
components.In conclusion, based on the data on fluorescence intensity of a due released from anionic
liposomes with a varying content of an anionic lipid as a measure of CT 4,
CT I, and CT II activity, as well as the results of molecular
docking of hPS into CT 4 and CT II, our
hypothesis is that there are specific lipid binding sites of various affinities on the toxin
surface. The concept of a CT binding to the membrane surface in two stages
(initially via electrostatic and then via hydrophobic interaction), specific
complexes of toxin with the anionic lipid’s polar heads being the determinants of the
process, provides qualitative insight into the dependence that the fluorescent dye release has
on the PS content in the POPC liposomes.
Authors: Sardar E Gasanov; Indira H Shrivastava; Firuz S Israilov; Aleksandr A Kim; Kamila A Rylova; Boris Zhang; Ruben K Dagda Journal: PLoS One Date: 2015-06-19 Impact factor: 3.240