This journal is c The Royal Society of Chemistry 2011 Chem. Commun., 2011, 47, 9483–9485 9483
Cite this: Chem. Commun., 2011, 47, 9483–9485
AFM investigation of Pseudomonas aeruginosa lectin LecA (PA-IL)
filaments induced by multivalent glycoclustersw
Delphine Sicard,aSamy Cecioni,
bcMaksym Iazykov,
aYann Chevolot,
aSusan E. Matthews,
d
Jean-Pierre Praly,bEliane Souteyrand,
aAnne Imberty,
cSebastien Vidal*
band
Magali Phaner-Goutorbe*a
Received 26th May 2011, Accepted 13th July 2011
DOI: 10.1039/c1cc13097h
Atomic force microscopy reveals that Pseudomonas aeruginosa
LecA (PA-IL) and a tetra-galactosylated 1,3-alternate
calix[4]arene-based glycocluster self-assemble according to an
aggregative chelate binding mode to create monodimensional
filaments. Lectin oligomers are identified along the filaments and
defects in chelate binding generate branches and bifurcations. A
molecular model with alternate 908 orientation of LecA tetramers
is proposed to describe the organisation of lectins and glycoclusters
in the filaments.
The opportunistic bacterium Pseudomonas aeruginosa is a
major cause of lung infections for immuno-compromised
and cystic fibrosis patients.1 Since the appearance of several
multidrug resistant strains, new therapeutic approaches are
receiving much attention especially for the prevention of
pathogen adhesion to host epithelia surfaces.2 In their
infection strategy, microorganisms often use carbohydrate-
binding proteins called lectins, to recognize and bind to host
cells.3 Pseudomonas aeruginosa displays two soluble lectins
(LecA/PA-IL and LecB/PA-IIL) which are implicated in
binding and virulence events leading to lung infection.4 A
structural study of LecA showed a homotetrametric lectin with
specificity for galactosides with a calcium ion involved in the
binding site.5 The molecular size of the tetramer can be described
as parallel piped with 7.0 � 3.2 � 1.9 nm3 dimensions (Fig. 1a).
The design of high affinity ligands for bacterial lectins6
such as LecA represents a strategy for the development
of anti-bacterial drugs, able to block the infection process
at the early stage of binding to the host cell.7 The affinity
of LecA for galactose is in the submillimolar range and the
design of multivalent glycoconjugates takes advantage of the
so-called ‘‘glycoside cluster effect’’,8 through the concept of
multivalency.9 We have recently synthesized topologically
isomeric calix[4]arene glycoclusters and measured nanomolar
affinities by microcalorimetry (ITC) and surface plasmon
resonance (SPR) for LecA.7c The sugar–protein interaction
was shown to be strongly dependent on both the valency and
the topology of the glycoclusters. The 1,3-alternate
calix[4]arene-based glycocluster (Fig. 1b) displayed the best
affinity towards LecA and molecular modeling was performed
in order to rationalize the high affinity observed and indicated
an aggregative chelate binding mode (Fig. 1c).
In order to further characterize the interaction between
calix[4]arene-based glycoclusters and LecA, we performed an
atomic force microscope (AFM) study of the self-assembly of
these partners. AFM offers the opportunity to evaluate both the
size and shape of nano-assemblies formed between multimeric
lectins and multivalent ligands. However, only a few experiments
have been reported where lectins and glycoconjugates were
deposited on a surface and then studied in air by AFM to
obtain additional information concerning their self-assembly
properties.10 In these recent reports, the sugar-lectin arrangement
yielded thin and thick films on the surface, which could then
self-assembly into a network rather than discrete assemblies.
Fig. 1 (a) Three-dimensional structure of lectin LecA (pdb code:
1OKO). Blue spheres represent calcium ions in binding sites. Dimensions
are measured between calcium ions. (b) Structure of the galactosylated
1,3-alternate calix[4]arene-based glycocluster 1. (c) Molecular modeling
pictures of aggregative chelate arrangement between LecA and the
ligand.7c Dimensions of the glycocluster 1 were measured between the
O-4 oxygen atom of galactose residues.
aUniversite de Lyon, Institut des Nanotechnologies de Lyon (INL), UMRCNRS 5270, site Ecole Centrale de Lyon, 36, avenue Guy de Collongue,69134 Ecully cedex, France. E-mail: [email protected]
b Institut de Chimie et Biochimie Moleculaires et Supramoleculaires(ICBMS, UMR 5246), Laboratoire de Chimie Organique 2 –Glycochimie, CNRS, Universite de Lyon, 43 Boulevard du 11Novembre 1918, 69622 Villeurbanne, France.E-mail: [email protected]
cCERMAV – CNRS, UPR5301, affiliated with Universite Joseph Fourierand ICMG, BP 53, 38041, Grenoble, France
dUniversity of East Anglia, School of Pharmacy, Norwich, NR4 7TJ, UKw Electronic supplementary information (ESI) available. See DOI:10.1039/c1cc13097h
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9484 Chem. Commun., 2011, 47, 9483–9485 This journal is c The Royal Society of Chemistry 2011
Here we report the formation of supramolecular structures
through self-assembly of proteins mediated by small molecules.
In a typical AFM experiment, solutions containing 20 mL of
CaCl2 (0.3 mM in final concentration) and 10 mL of recombi-
nant LecA5b (25 pM final concentration) and 10 mL of tetra-
galactosylated glycocluster 1 (25 pM final concentration) were
mixed and incubated during 1 h, at room temperature, so that
the lectin and glycocluster could bind and equilibrate in
solution. The presence of calcium cation is required for an
active lectin binding site.5a The solution was then deposited on
a freshly cleaved mica surface and the sample dried overnight
in a desiccator, at ambient pressure, with silica gel as a desiccant.
Topography images were taken in air, at room temperature,
using a Di-Cp-II (Bruker) AFM microscope in the Amplitude
Modulation (AM) AFM mode with MikroMasch NSC 21 tips
(see ESIw). The data analysis was performed with Gwyddion
Software.
The AFM image of the complex between LecA and the
galactosylated glycocluster 1 displayed small filaments on the
surface (Fig. 2a). Negative controls performed for LecA incubated
with the corresponding tetra-mannosylated glycocluster7c did
not reveal the presence of any filaments (see ESIw). For LecA/
1 complexes, the images showed linear segments interrupted
by bifurcations and branching points. The length of the linear
segments varies between 90 and 500 nm � 5 nm. Branching
occurs mostly in linear regions with only one defect at a time
on a filament. The average height of these structures is estimated
at 1.7 � 0.5 nm which is in agreement with the thickness of the
dried protein (i.e. slightly less than 1.9 nm, vide supra) (Fig. 2b).
The average width of these monodimensional filaments is of
36.4 � 8.5 nm, which is 5- to 10-times more than the length
and width of the lectin as measured by X-ray crystallography.
This difference is believed to be a consequence of both the
curvature radius of the tip, which is known to enlarge features
in AFM, and the experimental adsorption conditions. In fact,
the lateral dimensions measured in AFM are obtained by a
convolution of the tip shape with the real size of the features.11
In addition, it is well known that biological objects adsorbed
on a substrate are spread over the surface to promote a better
binding.12 Our drying (one night in a desiccator) and imaging
conditions (in air) could also increase this spreading-out of the
biomolecules. The mica structure is hexagonal, its influence
would induce preferentially angles of 601, 1201. . .. However, a
statistical analysis of the angle distribution was performed on
all the images and no preferential angle was identified (distribu-
tion on 130 angles). This indicates that no influence of the mica
structure was observed confirming that filaments were formed
in the solution before deposition and evaporation.
We have previously shown7c that in terms of topology the
best molecular model of the interaction between LecA and the
1,3-alternate glycocluster 1 would be the aggregative chelate
binding mode (Fig. 1c). Two 1,3-alternate galactose epitopes
of the glycocluster 1 can chelate the two adjacent binding sites
of a lectin tetramer on the width side (3.2 nm). The two other
monosaccharides can have the same interaction with another
lectin tetramer. The repetition of this particular structure, by
self-assembly, which would lead to the formation of a mono-
dimensional filament is consistent with our AFM images
(Fig. 2a). The length of linear segments is in agreement with
a repeat of 10 to 50 LecA tetramers, based on the dimensions
of the modelled filament (Fig. 3c and ESIw).The branches observed between filaments can be rationalised
by a defect in the symmetry of the glycocluster. One of the four
galactose residues can then bind to a third lectin tetramer on
the side of the filament, generating a branching point (Fig. 2c).
A model was generated using the Sybyl software (Tripos, St.
Louis) by exploring the available conformational flexibility,
the length of the triethyleneglycol linker, and ensuring the
absence of steric conflict between adjacent proteins (see ESIw).The model demonstrated that such a branching point to
generate the formation of another filament binding to the first
one is possible, even though no predominant angle could be
clearly identified.
A higher resolution image showed the discrete LecA tetramers
along the linear filament (Fig. 3a) as rectangular patterns
positioned one next to each other. Profile measurements indicated
that a segment of 102 nm contains six of these patterns with
Fig. 2 (a) AM-AFM image of the filaments of lectin LecA and
glycocluster 1 on the mica substrate. Image size is of 850 � 850 nm2.
(b) Height of the filament on the profile (black bar in (a)). (c) Molecular
modeling of 12 lectin tetramers (cyan) connected by galactosylated
glycoclusters (dark blue). 8 tetramers have been modeled in lines, and
4 from a branching point.
Fig. 3 (a) High resolution AM-AFM image of the LecA/1 filament at
a 400 nm scan range on the mica surface. (b) Profile of six portions on
a filament (black line) and on a mica substrate (cyan line). Height of
the filament is not calibrated with the mica surface. (c) Details of the
molecular model of LecA tetramers linked by glycocluster 1 with the
corresponding schematic representation.
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This journal is c The Royal Society of Chemistry 2011 Chem. Commun., 2011, 47, 9483–9485 9485
an average size of around 17 � 3.3 nm per pattern (Fig. 3b).
This value is 2 times greater than the theoretical length (9 nm,
longitudinal dimensions of LecA and glycocluster 1). Again,
the lateral size of each repeated tetramer cannot be precisely
estimated because of the limitations of the AFM method.
However, the enlargement of the pattern is less along the
filament than perpendicularly (36.4 � 8.5 nm) and cannot be
just attributed to a different geometry of the tip in both
directions but mostly to the spreading-out of the molecules
limited by the proximity of the neighboring molecules along
the filament.12 These values would suggest that the lectins are
arranged perpendicularly to the growth of the filament, this is
in contrast to the result obtained from models in which bridging
occurs on the shorter face of the lectin. This discrepancy is a
consequence of the imaging technique. The calculated arrange-
ment is believed to be the most probable, the binding sites are
too far away on the long side to allow perpendicular growth
(Fig. 3c). A difference in contrast was observed between the
patterns, some of them are brighter than the others, which
indicates a variation in the height value. A statistical measure-
ment on different patterns revealed an average height shift of
1.7 � 0.5 nm. This is consistent with our current model of the
LecA/1 complex7c which proposes that the cobblestone-shaped
tetramers are maintained in a 901 orientation one to the other,
due to the geometry of the calixarene-based glycocluster 1 in
which the galactose pairs on the top and bottom sides of the
calix[4]arene are in perpendicular planes (Fig. 1c). This topology
would result in a difference in height between neighbouring
tetramers as seen with the height shift of the AFM patterns.
However, the alternance of bright and dark patterns was not
systematic on the AFM image and one should also consider the
roughness of the mica surface underneath which could generate a
small variation of contrast (Fig. 3b).
In conclusion, the calixarene-based glycocluster previously
studied through bioanalytical techniques (HIA, ELLA, ITC
and SPR) for its binding properties towards the LecA was
further investigated by means of AFM to gain a more complete
understanding of its specific mode of binding. This AFM study
revealed that the aggregative chelate binding mode was most
probably adopted in the self-assembly of the glycocluster with
the lectin. A network of monodimensional filaments was
formed, with branching points and rare defects, attributed to
conformational changes in the glycosylated ligand. High
resolution images revealed each discrete lectin tetrameric unit
along the filament. Generally, the interaction between multimeric
lectins and multivalent ligands yields to the formation of aggre-
gates, or eventually organized 2D-networks.10a,13 Filament-like
association has been observed previously only for dimeric
bacterial BclA lectin interacting with bivalent mannosides.10b
The regular self-assembly through building blocks, observed
here, points to applications in nanotechnology. Further AFM
investigations are ongoing in our laboratories to describe more
precisely these self-assembly processes with various concentrations
of bio-materials, various lectin/glycocluster ratios, both in air
and in solution.
This work was financially supported by the CNRS, the
French Research Ministry with the ANR-08-BLAN-0114-01
programme, the LyonBioPole consortium and the French
Association ‘‘Vaincre laMucoviscidose’’ (against Cystic Fibrosis).
We also acknowledge University Claude Bernard Lyon 1, the
CNRS and University of East Anglia. S.C. thanks the Region
Rhone-Alpes for additional funding (Cluster de Recherche
Chimie).
Notes and references
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