Interactions between biological surfaces

Nano-mechanical exploration of the surface and sub-surface of hydrated cells of Staphylococcus epidermidis

The surface of hydrated cells of Staphylococcus epidermidis has been probed using an atomic force microscope. While local force measurements over the surface of bacteria reveal a heterogeneous chemical surface, with heterogeneous mechanical properties, different kinds of force curves appear with high frequency, and are thought to provide information on features contributing strongly to the overall mechanical and surface behaviour of the cell. Force curves often present two different mechanical regimes, being the first one (outer) of about 48 nm thick, and presenting a local relative elasticity of about 0.08 N/m, which is about a third of the relative elasticity of the inner part of the cell wall, harder, with a relative elasticity of about 0.24 N/m, in water. Both regimes appears as straight lines in the force versus distance curves (the 'corresponding' stress-strain curves in contact mechanics), but hysteresis is observed between the approach and the retraction line in the inner regime, indicating a degree of viscoelasticity. No viscoelasticity is observed in the outer regime, however, which presents quite linear and juxtaposed approach-retraction lines. These kinds of force curves do not present measurable pull-off forces nor snap-in forces, which indicates an almost null interaction between tip and bacterial surface, which could be in agreement with the measured very high hydrophobicity of this strain. Another kind of force curve has been observed recurrently, showing peaks in the retraction curves. Adhesive pull-off forces were measured giving an average of about 2 nN. Interestingly, however, these force curves appear only when quite irregular and wavy retraction curves are present, from the very beginning of its trace (maximum indentation). This leads us to think that these pull-off forces measured by our AFM do not give information on surface forces-unbinding events at the surface of the bacteria, but could be related to events at the sub-surface of the cell surface. Oscillations seen in the retraction curve in the portion corresponding to the contact with the bacteria surface could be due to rupture phenomena within the multilayered cell wall architecture expected in Gram-positive bacteria as Staphylococcus epidermidis, which could result in local irreversible deformations of the cell surface. Imaging with a sharp tip in contact mode sometimes leads to surface damage. Force curves recorded over damaged parts of the cell surface showed a completely different behaviour, in many cases with two well-defined high-adhesion peaks, and also interestingly, with snap-in forces of about 0-2 nN, which seems to indicate a completely different electrical/hydrophobicity state only a few nanometers down from the surface. Similar indentation effects can occur in the contact of a bacterial cell with a solid surface, even when showing only atomic-molecular-scale roughness, thus interacting not only with the very surface of the cell, especially when soft layers are present in the outer. Our results highlight the importance of the cell surface mechanical properties and their interplay with purely surface properties when analyzing cell-material interaction, and show the AFM as a useful method for investigating this.

Molecular bond formation between surfaces: anchoring and shearing effects

Specific molecular bonds between apposing surfaces play a central role in many biological structures and functions. They display a widely varying anchoring to the cell surface, and they are subject to forces that affect their binding characteristics due to their hydrodynamic environments. Here, we examine both anchoring and shearing aspects using simplified model systems aimed at gaining insight into the formation of a 2D bond collection under stress using two different surface anchors. The highly specific streptavidin-biotin molecular bond was chosen as the model receptor-ligand pair, and grafted colloids were used as model surfaces. To explore the role of the surface anchor, we grafted biotin onto the particle surface following two different approaches: first, the grafting was performed directly on the particle amine functions; second, a 35-nm-long PEG spacer was used. Hybrid particle classes were brought into contact in a homogeneous shear (between 200 s(-)(1) and 1200 s(-)(1)) using a cone plate geometry. The bond association and dissociation kinetics were given by the time course assemblage of hybrid particles into doublets. We observed saturating kinetics profiles that we interpreted as a linkage-breakage equilibrium, which yielded the on and off rates. We found that the biotin-PEG spacer was needed in order to observe significant binding at any shear rate. We also showed that only the number of collisions per unit time, generated by the shear, affected the on rate of the binding. Neither the exerted forces nor the collision lifetime had any effect. The off rate decreased with shear, possibly because of the shortening of the force duration, which results from the increasing shear rate.

Diffusion of microspheres in shear flow near a wall: use to measure binding rates between attached molecules

The rate and distance-dependence of association between surface-attached molecules may be determined by monitoring the motion of receptor-bearing spheres along ligand-coated surfaces in a flow chamber (Pierres et al., Proc. Natl. Acad. Sci. U.S.A. 95:9256-9261, 1998). Particle arrests reveal bond formation, and the particle-to-surface distance may be estimated from the ratio between the velocity and the wall shear rate. However, several problems are raised. First, data interpretation requires extensive computer simulations. Second, the relevance of standard results from fluid mechanics to micrometer-size particles separated from surfaces by nanometer distances is not fully demonstrated. Third, the wall shear rate must be known with high accuracy. Here we present a simple derivation of an algorithm permitting one to simulate the motion of spheres near a plane in shear flow. We check that theoretical predictions are consistent with the experimental dependence of motion on medium viscosity or particle size, and the requirement for equilibrium particle height distribution to follow Boltzman's law. The determination of the statistical relationship between particle velocity and acceleration allows one to derive the wall shear rate with 1-s(-1) accuracy and the Hamaker constant of interaction between the particle and the wall with a sensitivity better than 10(-21) J. It is demonstrated that the correlation between particle height and mean velocity during a time interval Deltat is maximal when Deltat is about 0.1-0.2 s for a particle of 1.4-microm radius. When the particle-to-surface distance ranges between 10 and 40 nm, the particle height distribution may be obtained with a standard deviation ranging between 8 and 25 nm, provided the average velocity during a 160-ms period of time is determined with 10% accuracy. It is concluded that the flow chamber allows one to detect the formation of individual bonds with a minimal lifetime of 40 ms in presence of a disruptive force of approximately 5 pN and to assess the distance dependence within the tens of nanometer range.

[Adhesion molecules and cancer]

INTRODUCTION

This review was aimed at summarizing recent advances in the understanding of cell adhesion in order to discuss the possible relevance of new knowledge to the exploration of cancer patients and elaboration of therapeutic strategies.

CURRENT KNOWLEDGE AND KEY POINTS

During the last 10 years, many adhesion molecules were identified, thus allowing to determine their tissue distribution and functional regulation. The concept of adhesiveness was refined. It is now well known that adhesive rate (i.e., the minimal contact time required for bond formation) and binding strength (i.e., the minimal force required to detach bound cells) are distinct parameters. They may be regulated independently, and influence the cell behavior in different ways. It is now possible to achieve accurate control of tumor cell adhesiveness, either by inhibiting an adhesive mechanism (through monoclonal antibodies, competitive ligands, or inhibition of receptor expression with antisense strategy or gene knock-out) or by promoting a binding mechanism (with receptor transfection or pro-inflammatory stimulation).

FUTURE PROSPECTS AND PROJECTS

Recent progress opens new possibilities for diagnosis and treatment. First, the interpretation of experimental data may be improved. Cell adhesive behavior is not entirely accounted for by the density of membrane adhesion receptors. Indeed, adhesion is influenced by receptor connection to the cytoskeleton and structure of the cell coat. An adhesion receptor may be anti-metastatic through an increase in tumor cohesion and cell differentiation, or pro-metastatic, through facilitation of cell migration towards a target tissue. New therapeutic strategies may include anti-adhesive procedure aimed at preventing metastasis formation. The potential importance of a better control of inflammatory processes is also emphasized in view of the influence of these processes on the expression of adhesion molecules.