Adhesion-induced domain formation by interplay of long-range repulsion and short-range attraction force: a model membrane study.

We study the role of the interplay of specific and universal forces for the adhesion of giant vesicles on solid supported membranes. To model the situation of cell adhesion, we incorporated lipopolymers (phospholipids with polyethyleneoxide headgroups) as artificial glycocalix, whereas attractive lock-and-key forces are mimicked by incorporating biotinylated lipids into both membranes and by mediating the strong coupling through streptavidin. Adhesion is studied by quantitative reflection interference contrast microscopy (RICM), which enables visualization of the contact zone and reconstruction of the height profile of the membrane beyond the contact line (outside the contact zone) up to a height of 1 micron. We demonstrate that adhesion is accompanied by lateral phase separation, leading to the formation of domains of tight adhesion (adhesion plaques) separated by areas of weak adhesion exhibiting pronounced flickering. By analyzing the height profile S(x) near the contact line in terms of the tension equilibrium (Young equation) and the moment equilibrium, respectively, the adhesion energy and membrane tension can be approximately measured locally. We show that the adhesion energy is about three orders of magnitude larger for the adhesion plaques than for the weekly adhering regions. The adhesion is studied as a function of the excess area of the vesicle generated by temperature variation. A very remarkable finding is that increased excess area is not always stored in the contact area, but leads to the formation of microbuds (diameter approximately 2 microns).     

Axonin-1/TAG-1 mediates cell-cell adhesion by a cis-assisted trans-interaction.

The neural cell adhesion molecule axonin-1/TAG-1 mediates cell-cell interactions via homophilic and heterophilic contacts. It consists of six Ig and four fibronectin type III domains anchored to the membrane by glycosylphosphatidylinositol. The recently solved crystal structure indicates a module composed of the four N-terminal Ig domains as the contact site between trans-interacting axonin-1 molecules from apposed membranes. Here, we have tested domain-specific monoclonal antibodies for their capacity to interfere with homophilic binding in a cell aggregation assay. The results confirmed the existence of a binding region within the N-terminal Ig domains and identified a second region contributing to homophilic binding on the third and fourth fibronectin domains near the C terminus. The perturbation of each region alone resulted in a complete loss of cell aggregation, suggesting that axonin-1-mediated cell-cell contact results from a cooperative action of two homophilic binding regions. The data support that axonin-1-mediated cell-cell contact is formed by cis-assisted trans-binding. The N-terminal binding regions of axonin-1 establish a linear zipper-like string of trans-interacting axonin-1 molecules alternately provided by the two apposed membranes. The C-terminal binding regions strengthen the cell-cell contact by enhancing the expansion of the linear string into a two-dimensional array via cis-interactions. Cis-assisted trans-binding may be a basic binding mechanism common to many cell adhesion molecules.     

Avidin-biotin interactions at vesicle surfaces: adsorption and binding, cross-bridge formation, and lateral interactions.

Densely packed domains of membrane proteins are important structures in cellular processes that involve ligand-receptor binding, receptor-mediated adhesion, and macromolecule aggregation. We have used the biotin-avidin interaction at lipid vesicle surfaces to mimic these processes, including the influence of a surface grafted polymer, polyethyleneglycol (PEG). Single vesicles were manipulated by micropipette in solutions of fluorescently labeled avidin to measure the rate and give an estimate of the amount of avidin binding to a biotinylated vesicle as a function of surface biotin concentration and surface-grafted PEG as PEG-lipid. The rate of avidin adsorption was found to be four times less with 2 mol% PEG750 than for the unmodified surface, and 10 mol% PEG completely inhibited binding of avidin to biotin for a 2-min incubation. Using two micropipettes, an avidin-coated vesicle was presented to a biotinylated vesicle. In this vesicle-vesicle adhesion test, the accumulation of avidin in the contact zone was observed, again by using fluorescent avidin. More importantly, by controlling the vesicle membrane tension, this adhesion test provided a direct measure of the spreading pressure of the biotin-avidin-biotin cross-bridges confined in the contact zone. Assuming ideality, this spreading pressure gives the concentration of avidin cross-bridges in the contact zone. The rate of cross-bridge accumulation was consistent with the diffusion of the lipid-linked "receptors" into the contact zone. Once adherent, the membranes failed in tension before they could be peeled apart. PEG750 did not influence the mechanical equilibrium because it was not compressed in the contact zone, but it did perform an important function by eliminating all nonspecific adhesion. This vesicle-vesicle adhesion experiment, with a lower tension limit of 0.01 dyn/cm, now provides a new and useful method with which to measure the spreading pressures and therefore colligative properties of a range of membrane-bound macromolecules.     

Detailed mechanics of membrane-membrane adhesion and separation. I. Continuum of molecular cross-bridges

The mechanics of membrane-membrane adhesion are developed for the approximation that the molecular cross-bridging forces are continuously distributed as a normal stress (force per unit area). The significance of the analysis is that the finite range of the cross-bridging forces and the microscopic contact angle are not assumed negligible. Since the cross-bridging and adhesion forces are finite range interactions, there are two membrane regions: a free zone where the membranes are not subject to attractive forces; and an adherent zone where the membranes are held together by attractive stresses. The membrane is treated as an elastic continuum. The approach is to analyze the mechanics for each zone separately and then to require continuity of the solutions at the interface between the zones. Final solution yields the membrane contour and stresses proximal to and within the contact zone as well as the microscopic contact angle at the edge of the contact zone. It is demonstrated that the classical Young equation is consistent with this model. The results show that the microscopic contact angle becomes appreciable when the strength of adhesion is large or the length of the cross-bridge is large; however, the microscopic contact angle approaches zero as the membrane elastic stiffness increases. The solution predicts the width of the contact zone over which molecular bonds are stretched. It is this boundary region where increased biochemical activity is expected. In the classical model presented here, the level of tension necessary to oppose spreading of the contact is equal to the minimal level of tension required to separate the adherent membranes. This behavior is in contrast with that derived for the case of discrete molecular cross-bridges where the possibility of different levels of tension associated with adhesion and separation is introduced. The discrete cross-bridge case is the subject of a companion paper.     

Functional incorporation of integrins into solid supported membranes on ultrathin films of cellulose: impact on adhesion

Biomimetic models of cell surfaces were designed to study the physical basis of cell adhesion. Vesicles bearing reconstituted blood platelet integrin receptors alpha(IIb)beta(3) were spread on ultrathin films of cellulose, forming continuous supported membranes. One fraction of the integrin receptors, which were facing their extracellular domain toward the aqueous phase, were mobile, exhibiting a diffusion constant of 0.6 micro m(2) s(-1). The functionality of receptors on bare glass and on cellulose cushions was compared by measuring adhesion strength to giant vesicles. The vesicles contained lipid-coupled cyclic hexapeptides that are specifically recognized by integrin alpha(IIb)beta(3). To mimic the steric repulsion forces of the cell glycocalix, lipids with polyethylene glycol headgroups were incorporated into the vesicles. The free adhesion energy per unit area deltag(ad) was determined by micro-interferometric analysis of the vesicle's contour near the membrane surface in terms of the equilibrium of the elastic forces. By accounting for the reduction of the adhesion strength by the repellers and from measuring the density of receptors one could estimate the specific receptor ligand binding energy. We estimate the receptor-ligand binding energy to be 10 k(B)T under bioanalogue conditions.     

Antagonist-induced deadhesion of specifically adhered vesicles

By use of a model system consisting of giant vesicles adhering to flat substrates, we identified, both experimentally and theoretically, two new control mechanisms for antagonist-induced deadhesion. Adhesion is established by specific binding of surface-grafted E-selectin and vesicle-carrying oligosaccharide Lewis(X). Deadhesion is achieved by controlled titration of monoclonal antibodies against E-selectin. The first mechanism is characterized by a considerable retraction of the contact zone resulting in a loss of contact area between the vesicle and the substrate. Within the developed theoretical framework, the observed equilibrium state is understood as a balance between the spreading pressure of the vesicle and the antagonist-induced lateral pressure at the edge of the contact zone. In the second mechanism, the antibodies induce unbinding by penetrating the contact zone without significantly affecting its size. This process reveals the decomposition of the adhesion zone into microdomains of tight binding separated by strongly fluctuating sections of the membrane. Both experiment and theory show a sigmoidal decrease of the number of bound ligands as a function of the logarithm of antagonist concentration. The work presented herein also provides a new method for the determination of the receptor binding affinity of either the surface-embedded ligands or the competing antagonist molecules.     

HDLs induce raft domain vanishing in heterogeneous giant vesicles

Cholesterol efflux from the plasma membrane to HDLs is essential for cell cholesterol homeostasis. Recently, cholesterol-enriched ordered membrane domains, i.e. lipid rafts have been proposed to play an important role in this process. Here we introduce a new method to investigate the role of HDL interactions with the raft lipid phase and to directly visualize the effects of HDL-induced cholesterol efflux on rafts in model membranes. Addition of HDLs to giant lipid vesicles containing raft-type domains promoted decrease in size and disappearance of such domains as visualized by fluorescence microscopy. This was interpreted as resulting from cholesterol efflux from the vesicles to the HDLs. The raft vanishing rate was directly related to the HDL concentration. Evidence for a direct interaction of HDLs with the membrane was obtained by observing mutual adhesion of vesicles. It is suggested that the present method can be used to study the selective role of the bilayer lipid phase (raft and non-raft) in cholesterol efflux and membrane-HDL interaction and their underlying mechanisms. Such mechanisms may contribute to cholesterol efflux in vivo.     

Galactosylceramide domain microstructure: impact of cholesterol and nucleation/growth conditions

Galactosylceramide (GalCer), a glycosphingolipid, is believed to exist in the extracellular leaflet of cell membranes in nanometer-sized domains or rafts. The local clustering of GalCer within rafts is thought to facilitate the initial adhesion of certain viruses, including HIV-1, and bacteria to cells through multivalent interactions between receptor proteins (gp120 for HIV-1) and GalCer. Here we use atomic force microscopy (AFM) to study the effects of cholesterol on solid-phase GalCer domain microstructure and miscibility with a fluid lipid 1,2-dilauroyl-sn-glycero-3-phosphocholine (DLPC) in supported lipid bilayers. Using "slow-cooled vesicle fusion" to prepare the supported lipid bilayers, we were able to overcome the nonequilibrium effects of the substrate (verified by comparison to results for giant unilamellar vesicles) and accurately quantify the dramatic effect of cholesterol on the GalCer domain surface area/perimeter ratio (A(D)/P) and DLPC-GalCer miscibility. We compare these results to a supported lipid bilayer system in which the bilayer is rapidly cooled (nonequilibrium conditions), "quenched vesicle fusion", and find that the microstructures are remarkably similar above a cholesterol mol fraction of approximately 0.06. We determined that GalCer domains were contained in one leaflet distal to the mica substrate through qualitative binding experiments with Trichosanthes kirilowii agglutinin (TKA), a galactose-specific lectin, and AFM of Langmuir-Blodgett deposited GalCer/DLPC supported lipid bilayers. In addition, GalCer domains in bilayers containing cholesterol rearranged upon tip-sample contact. Our results further serve to clarify why discrepancies exist between different model membrane systems and between model membranes and cell membranes. In addition, these results offer new insight into the effect of cholesterol and surrounding lipid on domain microstructure and behavior. Finally, our observations may be pertinent to cell membrane structure, dynamics, and HIV infection.     

A numerical analysis of forces exerted by laminar flow on spreading cells in a parallel plate flow chamber assay

Exposure of spreading anchorage-dependent cells to laminar flow is a common technique to measure the strength of cell adhesion. Since cells protrude into the flow stream, the force exerted by the fluid on the cells is a function of cell shape. To assess the relationship between cell shape and the hydrodynamic force on adherent cells, we obtained numerical solutions of the velocity and stress fields around bovine aortic endothelial cells during various stages of spreading and calculated the force required to detach the cells. Morphometric parameters were obtained from light and scanning electron microscopy measurements. Cells were assumed to have a constant volume, but the surface area increased during spreading until the membrane was stretched taut. Two-dimensional models of steady flow were generated using the software packages ANSYS (mesh generation) and FIDAP (problem solution). The validity of the numerical results was tested by comparison with published results for a semicircle in contact with the surface. The drag force and torque were greatest for round cells making initial contact with the surface. During spreading, the drag force and torque declined by factors of 2 and 20, respectively. The calculated forces and moments were used in adhesion models to predict the wall shear stress at which the cells detached. Based upon published values for the bond force and receptor number, round cells should detach at shear stresses between 2.5 and 6 dyn/cm(2), whereas substantially higher stresses are needed to detach spreading and fully spread cells. Results from the simulations indicate that (1) the drag force varies little with cell shape whereas the torque is very sensitive to cell shape, and (2) the increase in the strength of adhesion during spreading is due to increased contact area and receptor densities within the contact area. (c) 1993 John Wiley & Sons, Inc.     

Single-molecule force spectroscopy of mycobacterial adhesin-adhesin interactions

The heparin-binding hemagglutinin (HBHA) is one of the few virulence factors identified for Mycobacterium tuberculosis. It is a surface-associated adhesin that expresses a number of different activities, including mycobacterial adhesion to nonphagocytic cells and microbial aggregation. Previous evidence indicated that HBHA is likely to form homodimers or homopolymers via a predicted coiled-coil region located within the N-terminal portion of the molecule. Here, we used single-molecule atomic-force microscopy to measure individual homophilic HBHA-HBHA interaction forces. Force curves recorded between tips and supports derivatized with HBHA proteins exposing their N-terminal domains showed a bimodal distribution of binding forces reflecting the formation of dimers or multimers. Moreover, the binding peaks showed elongation forces that were consistent with the unfolding of α-helical coiled-coil structures. By contrast, force curves obtained for proteins exposing their lysine-rich C-terminal domains showed a broader distribution of binding events, suggesting that they originate primarily from intermolecular electrostatic bridges between cationic and anionic residues rather than from specific coiled-coil interactions. Notably, similar homophilic HBHA-HBHA interactions were demonstrated on live mycobacteria producing HBHA, while they were not observed on an HBHA-deficient mutant. Together with the fact that HBHA mediates bacterial aggregation, these observations suggest that the single homophilic HBHA interactions measured here reflect the formation of multimers that may promote mycobacterial aggregation.     

Reconstitution of the rat liver vasopressin receptor coupled to guanine nucleotide-binding proteins

The V1 vasopressin receptor has been solubilized from rat liver membranes with the zwitterionic detergent 3-[(3-cholamidopropyl)dimethylammoniol]-1-propanesulfonate (CHAPS) and reconstituted into phospholipid vesicles. There is essentially complete solubilization of the receptor by 3% CHAPS at a protein concentration of 15 mg/ml. Reconstitution into soybean phospholipid vesicles is readily achieved either by gel filtration chromatography or by membrane dialysis. The binding of [3H]vasopressin to proteoliposomes is specific, saturable, reversible, and magnesium-dependent. In contrast, the detergent-soluble vasopressin receptor does not display specific binding. The apparent affinity of the reconstituted receptor for [3H]vasopressin is approximately 4-fold lower than that of the receptor in native membranes. In addition, the binding of [3H]vasopressin to reconstituted vesicles is not sensitive to 100 microM guanosine 5'-O-thiotriphosphate (GTP gamma S) as it is in native membranes. However, the apparent affinity of the reconstituted receptor for ligand approximates that of native membranes when membranes are prebound with vasopressin prior to solubilization and reconstitution into vesicles. Furthermore, vesicles reconstituted from membranes prebound with vasopressin show GTP gamma S sensitivity of [3H] vasopressin binding. This finding strongly suggests that vasopressin stabilizes a receptor-G-protein complex during solubilization. The rat liver vasopressin receptor is a glycoprotein, as shown by its specific binding to the lectin "wheat germ agglutinin." The vasopressin receptor can be reconstituted from the N-acetylglucosamine-eluted peak of a wheat germ agglutinin-Sepharose column, and [3H] vasopressin binding activity is purified 5-6-fold from membranes by this chromatographic procedure. The functionality of the partially purified receptor is indicated by its ability to bind ligand with high affinity and by its ability to functionally interact with a G-protein when vasopressin is bound prior to solubilization.     

Liquid domains in vesicles investigated by NMR and fluorescence microscopy

We use (2)H-NMR, (1)H-MAS NMR, and fluorescence microscopy to detect immiscibility in three particular phospholipid ratios mixed with 30% cholesterol: 2:1 DOPC/DPPC, 1:1 DOPC/DPPC, and 1:2 DOPC/DPPC. Large-scale (>160 nm) phase separation into liquid-ordered (L(o)) and liquid-crystalline (L(alpha)) phases is observed by both NMR and fluorescence microscopy. By fitting superimposed (2)H-NMR spectra, we quantitatively determine that the L(o) phase is strongly enriched in DPPC and moderately enriched in cholesterol. Tie-lines estimated at different temperatures and membrane compositions are based on both (2)H-NMR observations and a previously published ternary phase diagram. (2)H- and (1)H-MAS NMR techniques probe significantly smaller length scales than microscopy experiments (submicron versus micron-scalp), and complex behavior is observed near the miscibility transition. Fluorescence microscopy of giant unilamellar vesicles shows micrometer-scale domains below the miscibility transition. In contrast, NMR of multilamellar vesicles gives evidence for smaller ( approximately 80 nm) domains just below the miscibility transition, whereas large-scale demixing occurs at a lower temperature, T(low). A transition at T(low) is also evident in fluorescence microscopy measurements of the surface area fraction of ordered phase in giant unilamellar vesicles. Our results reemphasize the complex phase behavior of cholesterol-containing membranes and provide a framework for interpreting (2)H-NMR experiments in similar membranes.     

Ultraweak sugar-sugar interactions for transient cell adhesion

Carbohydrate-carbohydrate interactions are rarely considered in biologically relevant situations such as cell recognition and adhesion. One Ca(2+)-mediated homotypic interaction between two Lewis(x) determinants (Le(x)) has been proposed to drive cell adhesion in murine embryogenesis. Here, we confirm the existence of this specific interaction by reporting the first direct quantitative measurements in an environment akin to that provided by membranes. The adhesion between giant vesicles functionalized with Le(x) was obtained by micropipette aspiration and contact angle measurements. This interaction is below the thermal energy, and cell-cell adhesion will require a large number of molecules, as illustrated by the Le(x) concentration peak observed at the cell membranes during the morula stage of the embryo. This adhesion is ultralow and therefore difficult to measure. Such small interactions explain why the concept of specific interactions between carbohydrates is often neglected.     

Phosphatidylserine membrane domain clustering induced by annexin A2/S100A10 heterotetramer

By means of scanning force and fluorescence microscopy of artificial membranes immobilized on mica surfaces, the lateral organization of the annexin A2/S100A10 heterotetramer (annexin A2t) and its influence on the lateral organization of the lipids within the membrane have been elucidated. Planar lipid bilayers composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC)/1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoserine (POPS) were prepared on atomically flat mica surfaces by the spreading of unilamellar vesicles. Fluorescence images of fluorescently labeled annexin A2t and scanning force microscopy images of nonlabeled protein bound to POPC/POPS bilayers show the formation of micrometer-sized lateral protein domains in the presence of 1 mM CaCl2. By means of scanning force microscopy, not only protein domains became discernible but also small membrane domains, which were attributed to POPS-enriched areas. A depletion of these POPS domains was observed in the vicinity of annexin A2t protein domains. These results indicate that annexin A2t is a peripheral membrane-binding complex capable of inducing lipid segregation.     

Adhesion energy of receptor-mediated interaction measured by elastic deformation

We investigated the role of receptor binding affinity in surface adhesion. A sensitive technique was developed to measure the surface energy of receptor-mediated adhesion. The experimental system involved a functionalized elastic agarose bead resting on a functionalized glass coverslip. Attractive intersurface forces pulled the two surfaces together, deforming the bead to produce an enlarged contact area. The Johnson-Kendall-Roberts (JKR) model was used to relate the surface energy of the interaction to the elasticity of the bead and the area of contact. The surface energies for different combinations of modified surfaces in solution were obtained from reflection interference contrast microscopy (RICM) measurements of the contact area formed by the bead and the coverslip. Studies with surfaces functionalized with ligand-receptor pairs showed that the relationship between surface energy and the association constant of the ligand binding has two regimes. At low binding affinity, surface energy increased linearly with the association constant, while surface energy increased logarithmically with the association constant in the high affinity regime.     

Intracellular site of asialoglycoprotein receptor-ligand uncoupling: Double-label immunoelectron microscopy during receptor-mediated endocytosis

In rats infused with asialoglycoprotein for 60 min, receptor-mediated endocytosis of the ligand occurred exclusively in hepatic parenchymal cells. We have used double-label immunoelectron microscopy on ultrathin cryosections of rat liver to identify the site at which the asialoglycoprotein receptor and its ligand dissociate following their common endocytosis. Asialoglycoprotein receptor, ligand and clathrin were identified and quantitated by the use of monospecific antibodies followed by gold-protein A complexes. Both receptor and ligand were found associated with the membrane of clathrin-coated vesicles close to the cell surface. We identified other vesicles that contained ligand accumulated within the lumen. The membranes of these latter vesicles contained little receptor, but receptor was concentrated in tubular extensions that were largely free of ligand. We call this organelle CURL (compartment of uncoupling of receptor and ligand). CURL vesicles appear to transform into secondary lysosomes, wherein the ligand is degraded. The tubular vesicles are, we propose, an intermediate in recycling the receptor to the cell surface.     

In vitro clustering and multiple fusion among macrophage endosomes

Early steps of receptor-mediated endocytosis appear to require the fusion of endosomes with each other. Recently, these fusion events have been reconstituted in vitro using vesicle preparations from J774 macrophages which have internalized ligands via the mannose receptor (Diaz, R., Mayorga, L., and Stahl, P. (1988) J. Biol. Chem. 263, 6093-6100). The present studies indicate that endosomes first form clusters when incubated under fusogenic conditions. Aggregation state was determined by electron microscopy using vesicles containing ligand-coated colloidal gold of different sizes previously internalized via the mannose receptor. Aggregation required cytosol and ATP. Afterwards, the limiting membranes of the vesicles composing these aggregates undergo multiple fusion and bring about the formation of large diameter vesicles that maintained the same density as endosomes when analyzed by Percoll gradient sedimentation. These large diameter vesicles were no longer fusogenic in the fusion assay. Multiple fusion was determined morphologically by the co-localization of three different size colloidal gold vesicles inside endocytic vesicles and biochemically by the fusion-dependent formation of triple immune complexes between three endocytic ligands internalized by receptor-mediated endocytosis: anti-dinitrophenol mouse IgG and dinitrophenol-derivatized beta-glucuronidase, ligands for the mannose receptor, and aggregated rabbit anti-mouse IgG, a ligand for the macrophage Fc receptor.     

Recurrent dynamics of rupture transitions of giant lipid vesicles at solid surfaces

Single giant unilamellar vesicles (GUVs) rupture spontaneously from their salt-laden suspension onto solid surfaces. At hydrophobic surfaces, the GUVs rupture via a recurrent, bouncing ball rhythm. During each contact, the GUVs, rendered tense by the substrate interactions, porate, and spread a molecularly transformed motif of a monomolecular layer on the hydrophobic surface from the point of contact in a symmetric manner. The competition from pore closure, however, limits the spreading and produces a daughter vesicle, which re-engages with the substrate. At solid hydrophilic surfaces, by contrast, GUVs rupture via a distinctly different recurrent burst-heal dynamics; during burst, single pores nucleate at the contact boundary of the adhering vesicles, facilitating asymmetric spreading and producing a “heart”-shaped membrane patch. During the healing phase, the competing pore closure produces a daughter vesicle. In both cases, the pattern of burst-reseal events repeats multiple times, splashing and spreading the vesicular fragments as bilayer patches at the solid surface in a pulsatory manner. These remarkable recurrent dynamics arise, not because of the elastic properties of the solid surface, but because the competition between membrane spreading and pore healing, prompted by the surface-energy-dependent adhesion, determine the course of the topological transition.     

Studies on nucleotide and receptor regulation of Gi proteins: effects of pertussis toxin

In intact membranes as well as after reconstitution into phospholipid vesicles, pertussis toxin (PT)-mediated ADP-ribosylation of G proteins causes loss of receptor-mediated regulation of effectors and/or G protein-mediated regulation of receptor binding. Studies were carried out to test which of several discrete steps known to constitute the basal and receptor-stimulated regulatory cycles of Gi proteins are affected by PT. Experiments with the Gs-deficient Gi-regulated adenylyl cyclase of cyc- S49 cell membranes indicated that PT blocks Gi activation by GTP without affecting GDP dissociation or GTP binding to a major extent. This suggested that the block lies in the transition of inactive GTP-Gi to active GTP-Gi (G to G* transition). Experiments with purified Gi in solution and after incorporation into phospholipid vesicles showed that PT does not increase or decrease the intrinsic GTPase activity of Gi. Experiments in which Gi was incorporated into phospholipid vesicles with rhodopsin, a receptor that interacts with Gi to stimulate the rate of guanosine 5'-O-(3-thio)triphosphate binding and GTP hydrolysis, indicated that PT does not affect the basal GTPase activity of Gi, but blocks its activation by the photoreceptor. Taken together the results indicate that PT-mediated ADP ribosylation has two separate effects, one to block the interaction of receptor with Gi and another to impede the GTP-induced activation reaction from occurring, or that PT has only one effect, that of blocking interaction with receptors. In this latter case the present results add to a mounting series of data that are consistent with the hypothesis that unoccupied receptors are not inactive, but exhibit a basal agonist-independent activity responsible for the various effects of GTP observed on G protein-coupled effector functions in intact membranes.