We describe here the properties of mAb GK1.5, which recognizes a cell surface molecule designated L3T4; the determinant on L3T4 recognized by mAb GK1.5 is designated L3T4a. We present evidence here that: i) the expression of L3T4a by murine T cell clones correlates primarily with class II MHC antigen-reactivity; ii) mAb GK1.5 blocks all class II MHC antigen-specific functions (cytolysis, proliferation, release of lymphokines) by murine class II MHC antigen-reactive T cell clones, although there appears to be clonal heterogeneity in the degree to which these functions are blocked by mAb GK1.5; iii) mAb GK1.5 blocks class II MHC antigen-specific release of IL-2 from cloned T cell hybridomas by blocking class II MHC antigen-specific binding; and iv) L3T4 is very similar to the human Leu3/T4 antigen. The properties of mAb GK1.5 (complement fixation, reactivity with all mouse strains tested, profound blocking of all class II MHC antigen-specific functions by murine T cells, usefulness for FACS analyses, and usefulness for immuno-precipitation/SDS-PAGE analyses) make it suitable for investigating both the role of class II MHC antigen-reactive T cells in various immunological phenomena and the mechanistic basis, at the molecular level, of class II MHC antigen-reactivity by murine T cells.

The adhesion of moving cells to receptor-bearing surfaces is a key step to many important biological processes. Attachment was subjected to extensive modeling. However, the numerical values of kinetic bonding parameters relevant to realistic models of cell adhesion remain poorly known. In this report, we describe the motion of human granulocytes to interleukin-1-activated endothelial cells in presence of a low hydrodynamic drag (a few piconewtons) estimated to be much weaker than a standard ligand-receptor bond. It was thus expected to visualize the formation and rupture of individual bonds. We observed multiple short-time cell arrests with a median duration of 2.43 s. Stop frequency, not duration, was significantly inhibited by anti-E-selectin antibodies. Binding efficiency exhibited an almost linear relationship with the inverse of cell velocity. The distribution of arrest duration was determined: results were consistent with the view that these arrests reflected the formation/dissociation of single ligand-receptor bonds with a spontaneous dissociation rate of 0.5 s-1. The rate of bond formation was on the order of 0.04 s-1 when cells were freely rolling (mean velocity: 19 microns/s) and it exhibited an approximately 10-fold increase after the formation of a first adhesion.

First case of a human RASGRP2 mutation affecting Rap1 activation in platelets and causing severe bleeding.

A laminar flow chamber was used to study single molecule interactions between biotinylated surfaces and streptavidin-coated spheres subjected to a hydrodynamic drag lower than a piconewton. Spheres were tracked with 20 ms and 40 nm resolution. They displayed multiple arrests lasting between a few tens of milliseconds and several minutes or more. Analysis of about 500,000 positions revealed that streptavidin-biotin interaction was multiphasic: transient bound states displayed a rupture frequency of 5.3 s(-1) and a rate of transition toward a more stable configuration of 1.3 s(-1). These parameters did not display any significant change when the force exerted on bonds varied between 3.5 and 11 pN. However, the apparent rate of streptavidin-biotin association exhibited about 10-fold decrease when the wall shear rate was increased from 7 to 22 s(-1), which supports the existence of an energy barrier opposing the formation of the transient binding state. It is concluded that a laminar flow chamber can yield new and useful information on the formation of molecular bonds, and especially on the structure of the external part of the energy landscape of ligand-receptor complexes.

Cell membranes are studded with protrusions that were thoroughly analyzed with electron microscopy. However, the nanometer-scale three-dimensional motions generated by cell membranes to fit the topography of foreign surfaces and initiate adhesion remain poorly understood. Here, we describe the dynamics of surface deformations displayed by monocytic cells bumping against fibronectin-coated surfaces. We observed membrane undulations with typically 5 nm amplitude and 5-10 s lifetime. Cell membranes behaved as independent units of micrometer size. Cells detected the presence of foreign surfaces at 50 nm separation, resulting in time-dependent amplification of membrane undulations. Molecular contact then ensued with apparent cell-membrane separation of 30-40 nm, and this distance steadily decreased during the following tens of seconds. Contact maturation was associated with in-plane egress of bulky molecules and robust membrane fluctuations. Thus, membrane undulations may be the major determinant of cell sensitivity to substrate topography, outcome of interaction, and initial kinetics of contact extension.

It is not well known how the kinetic constants of association between soluble receptors and ligands may be used to predict the behavior of these molecules when they are bound to cell surfaces. Spherical beads were coated with varying densities of anti-rabbit immunoglobulin monoclonal antibodies and driven along glass surfaces derivatized with rabbit anti-dinitrophenol. Particle motion was analyzed. The velocity, attachment frequency, and duration of binding events were determined on individual particles. It was found that i) beads exhibited frequent arrests lasting between a few tenths of a second and more than one minute; ii) when antibodies were diluted, the median arrest duration remained fairly constant (Ϸ1 s) whereas binding frequency varied as the first power of the antibody concentration, suggesting that most particle arrests were due to the formation of a single bond; iii) when the shear rate was increased 7-fold, the duration of transient binding events remained constant. The disruptive force exerted on attachment points was estimated to range between about 6 and 37 piconewtons; and iv) the distribution of arrest durations suggested that binding was not a monophasic reaction but involved at least one intermediate step. Therefore, transient binding events reflected the formation of unstable associations that are not detected with standard techniques.An obvious requirement for a molecular understanding of cell adhesion would be to obtain a precise knowledge of the rates of bond formation and dissociation between membraneassociated receptors and ligands. Indeed, it was recently emphasized that the outcome of an intercellular contact might be more dependent on the kinetics than the affinity of interaction between ligands and receptors (1-3). Thus, the capacity of adhesion molecules such as selectins to allow the rolling of leukocytes along endothelial cells in flowing blood was suggested to rely on a particularly high value of kinetic constants (3). Also, when a first bond occurred between a cell and another cell or surface, a critical parameter of adhesion is the ratio between the rates of dissociation of the first bond and formation of additional interactions (4).However, to our knowledge, no previously reported methodology allowed a direct measurement of the lifetime of interactions between particle-bound molecules (5). Tha et al. (6) used a travelling microtube to study the time and force dependence of rupture of antibody-mediated erythrocyte doublets. However, they did not study very transient attachments. Wattenbarger et al. (7) studied the adhesion of glycophorin-containing liposomes to a lectin-coated surface in shear flow. Although they studied the motion of individual particles, they did not present quantitative data on short-term arrests. Other experiments done with the parallel plate flow chamber yielded direct information on binding efficiency and binding strength rather than binding kinetics (8, 9). Also, Evans et al. (10) performed micromanipulation to determine the mechanical resistance of ...

E-cadherin is the predominant adhesion molecule of epithelia. The interaction between extracellular segments of E-cadherin in the membrane of opposing cells is homophilic and calcium dependent. Whereas it is widely accepted that the speci®city of the adhesive interaction is localized to the N-terminal domain, the kinetics of the recognition process are unknown. We report the ®rst quantitative data describing the dissociation kinetics of individual E-cadherin interactions. Aggregation assays indicate that the two outermost domains of E-cadherin (E/EC1±2) retain biological activity when chemically immobilized on glass beads. Cadherin fragment trans-interaction was analysed using a¯ow chamber technique. Transient tethers had ®rst-order kinetics, suggesting a unimolecular interaction. The unstressed lifetime of individual E-cadherin interactions was as brief as 2 s. A fast off rate and the low tensile strength of the E-cadherin bond may be necessary to support the high selectivity and plasticity of epithelial cell interactions.

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.