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Vol. 17, Issue 2, 862-875, February 2006
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* CNRS, UMR 5091, Institut Magendie de Neurosciences, Université Bordeaux 2, 33077 Bordeaux, France;
INSERM, U706, Institut du Fer à Moulin, Université Pierre et Marie Curie, 75005 Paris, France
Submitted April 21, 2005;
Revised October 7, 2005;
Accepted November 18, 2005
Monitoring Editor: Asma Nusrat
| ABSTRACT |
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| INTRODUCTION |
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Cadherins are single-pass transmembrane proteins forming homophilic calcium-dependent bonds by transassociations of their extracellular domains (Pertz et al., 1999
; Boggon et al., 2002
). Cadherin ectodomains are also able to form lateral oligomers (Iino et al., 2001
; Troyanovsky et al., 2003
), resulting in complex adhesive structures (He et al., 2003
). On the intracellular side, the cadherin cytoplasmic tail can couple to actin via the adaptor proteins
- and
-catenin (Yap et al., 1998
). Such mechanical coupling could represent the molecular basis for the strengthening of intercellular contacts (Adams et al., 1998
; Vasioukhin et al., 2000
; Chu et al., 2004
). Recent findings indicate that, in addition to their role as adhesive moieties, cadherins also behave as signaling receptors (Yap and Kovacs, 2003
). In particular, cadherin ligation has been shown to activate Rho family GTPases known to affect actin assembly (Noren et al., 2001
; Kovacs et al., 2002
). Conversely, these enzymes together with the catenin complex participate to the regulation of cadherin adhesiveness. For example, a dominant negative form of Rac inhibits the extension of cadherin-dependent contact zones (Ehrlich et al., 2002
; Gavard et al., 2004
) as well as the rapid linkage of N-cadherin to the actively moving actin network in lamellipodia (Lambert et al., 2002
).
Although the molecular components involved in the formation of cadherin contacts are beginning to be characterized, the issue of how cells control the strength of such adhesive zones and remodel them remains unclear. It is often difficult in these processes to distinguish the respective effects of ligand-receptor binding, receptor clustering, and receptor coupling to the cytoskeleton. To answer these questions, it is necessary to investigate the dynamics of formation and renewal of cadherin-mediated adhesive contacts. Biophysical approaches using purified fragments of cadherin extracellular domains and techniques such as atomic force microscopy (Sivasankar et al., 1999
), laminar flow chamber (Perret et al., 2002
), or single molecule fluorescence detection (Baumgartner et al., 2003
) have shed light on the kinetics and strength of the cadherin homophilic interactions at the individual molecular level. They showed that the lifetime of a single cadherin-cadherin bond, irrespective of the cadherin subtype, is about 1 s. It is intriguing that cadherin interactions, apparently so labile at the individual level, can support long-term adhesion between cells. Clearly, it seems important to extend such measurements to living cells, in which an active regulation of cadherin adhesiveness can take place.
To probe the dynamics of N-cadherin accumulation and turnover at neuronal adhesion sites, we essentially used microspheres coated with purified N-cadherin interacting with primary cultures of neurons transfected with N-cadherin fused to GFP. This biomimetic system allowed a precise control of the type and density of ligand molecules presented to the cells and of the time and duration of the interaction, which is not possible in natural contacts. Furthermore, it has the advantage over purely artificial systems that one can probe the dynamics of wild-type or mutated receptors in a living cellular environment. Using a series of optical microscopy techniques, we characterized the kinetics of recruitment of N-cadherin receptors, their anchoring to the actin cytoskeleton, and the turnover of N-cadherin bonds at equilibrium within both semiartificial and spontaneous contacts. Our results demonstrate that the formation and stabilization of N-cadherin bonds in neurons is critically regulated by interactions with catenins.
| MATERIALS AND METHODS |
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-catenin binding region and fused at its C-terminal end in frame with the GFP cDNA (Ncad
cat-GFP) was obtained by ligation of a 2633-base pair SacI-SacI fragment of pNA 18-53 (Matsuzaki et al., 1990
cyto-GFP), a 2265 base pairs SacI-SacI fragment encoding the ectodomain and the transmembrane region of chicken N-cadherin was inserted into the SacI site of pEGFP N1 (Clontech). Mouse Ncad-GFP was a gift of C. Gauthier-Rouvière (Causeret et al., 2005
Protein Expression and Cell Extracts
The mouse sarcoma cell line S180, the mouse L cell line and the stable N-cadherin expressing S180Ncad cell line (Matsuzaki et al., 1990
) were cultured at 37°C in 5-7.5% CO2 in DMEM medium containing 10% fetal calf serum (FCS). About 5 million cells were briefly trypsinized and resuspended in 400 µl DMEM, 10% FCS, 50 mM HEPES pH 7.4. After addition of 40 µg plasmid, cells were electroporated at 280 V and 1500 µF for 50 ms (Easyject, Equibio, Ashford, United Kingdom) and seeded in DMEM with 10% FCS and placed back in the incubator. Two days later, cells were lysed in Laemmli, scraped, and sonicated to disrupt high-molecular-weight DNA molecules. For Western Blot analysis, equivalent amounts of total protein were separated on 7.5% homemade polyacrylamide-SDS gels or NuPAGE 4-12% (Invitrogen, Carlsbad, CA) in reducing conditions, transferred to 0.45-µm nitrocellulose membranes, and immunoblotted as previously described (Lambert et al., 2000
) with either monoclonal anti-N-cadherin (1/2000, Transduction Laboratories, Lexington, KY), monoclonal anti-GFP (1/2000, Roche, Indianapolis, IN), or polyclonal anti-
-catenin (1/5000, Sigma, St. Louis, MO) antibodies. After extensive washing, membranes were probed with either HRP-conjugated anti-mouse or anti-rabbit immunoglobulin (Ig) antibodies (1/5000, Dako, Carpenteria, CA) and developed using the ECL method (Amersham, Indianapolis, IN). For Figure 1D, this step was performed using IRDye 800CW-conjugated antibodies (1/5000, Rockland, Gilbertsville, PA) and signal detection was performed at 800 nm (excitation wavelength: 774 nm) with the Odyssey Infrared Imaging System (Li-Cor Biotechnology, Lincoln, NE).
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Neuronal Culture and Transfection
Hippocampal neurons from E18 Sprague-Dawley rat embryos were seeded on 15-mm polylysine-coated glass coverslips at a density of 10,000 cells per cm2 and cultured on a layer of glial cells in Neurobasal medium supplemented with B27 (Invitrogen; Hemar et al., 1997
). Neurons were transfected 1 or 2 d after plating, using a phosphate calcium method with 30 µg DNA for five coverslips (Xia et al., 1996
) and processed 24 h later. Cells were placed in 1-ml culture medium supplemented with 1% BSA, 20 mM HEPES, and 10 µl of the bead solution, left at 37°C for 0.5 h and then rinsed three times in warm medium (except for optical tweezers experiments where cells were observed immediately). For live experiments, coverslips were mounted in a homemade aluminum chamber sealed with vacuum grease. GC4 antibody (1:50 from 10 mg/ml ascites fluid), EGTA (4 mM), cytochalasin D (1 µM), nocodazole (3 µM), or dimethylsulfoxide (DMSO; 1:2000) were added at this stage when indicated. For the characterization of spontaneous neuronal contacts, cells at 6 d in vitro (DIV) were transfected with Ncad-GFP using a lipofection kit (Effectene, Qiagen, Chatsworth, CA), and observed 24 h later.
Optical Tweezers and Epifluorescence
The optical tweezers setup consists of an inverted microscope (Olympus IX 70, Lake Success, NY) fed through its epifluorescence port by a Nd:YAG laser beam (Compass 1064 nm, Coherent, Palo Alto, CA) expanded by a 10x telescope. Fluorescence illumination comes from a Xenon lamp deported at 90° and reflected by a 750-nm cutoff dichroic mirror (Omega Optical, Brattleboro, VT). Both the infrared beam and the GFP excitation light (filter 480/20 nm, Chroma Technology, Brattleboro, VT) are reflected inside the microscope by a dual dichroic mirror (Chroma Technology) and focused by a 100x/1.40 NA oil objective. The laser power was 100 mW at the back of the objective. A set of two lenses in a near afocal configuration, with one lens on a three-dimensional (3D) translator were used for fine centering of the beam. Digital images were acquired using a cooled CCD camera (HQ Cool Snap, Roper Scientific, Tucson, AZ) driven by the Metamorph software (Universal Imaging, West Chester, PA). The temperature was maintained at 37°C with an air blower (World Precision Instruments, Sarasota, FL) and an objective heater (Bioptechs, Butler, PA). Using a motorized stage (MarzHauser, Wetzlar, Germany), microbeads were captured and maintained on neuronal growth cones for 10 s. In short-term experiments, the microsphere trajectory was monitored for 2 min by 10-Hz image acquisition in DIC illumination mode. The coordinates of the microspheres were tracked automatically through the Metamorph software, and the mean squared displacement over time was computed using a homemade algorithm (Serge et al., 2002
). In longer term experiments, images were taken every 10 s, alternating between bright field and fluorescence illumination (emission filter 525/50 nm) using shutters (Uniblitz, Vincent Associates, Rochester, NY). To estimate the force that could be applied on microspheres by optical tweezers, the stage was moved at increasing velocities until a trapped microsphere escaped. The maximal tarp force was taken as Stokes' drag on the sphere (6
a
v), where a is the radius of the microsphere (2 µm),
the viscosity of the medium (10-3 kg·m-1s-1), and v the critical velocity for escape (about 150 µm/s), leading to a value of 6 pN.
Fluorescence Recovery after Photobleaching
The same microscope was used for photobleaching experiments, except that the long-pass dichroic mirror was replaced by a 70/30 beam splitter (Chroma Technology), allowing illumination with the 488- and 514-nm lines of an Argon laser (Innova 300, Coherent) together with that of the Xenon lamp. The laser beam was also expanded 10 times to fill the back aperture of the objective, and the movable lens was adjusted to yield a diffraction-limited spot on the focal plane. The laser power was 2.5 mW at the back of the objective, either with GFP or YFP filter sets. Both wide-field and laser illuminations were controlled by shutters. A region of interest on a neuron expressing Ncad-GFP was brought to the position of the laser spot and the fluorescence recovery after photobleaching (FRAP) sequence was started: five reference images were acquired first and then the sample was bleached by the laser for 0.3 s, and fluorescence recovery was recorded for 12 min. Images were acquired in full-field illumination with exposure times of 50-200 ms. The whole sequence was driven by a journal written in the Metamorph software. Three FRAP sequences were run per coverslip, bringing the experiment duration to
45 min. Using Ncad-GFP-positive cells fixed with paraformaldehyde, we measured the diameter of the bleached area (2r = 4 µm) and the photobleaching due to the illumination sequence itself, which was <5%.
Photoactivation of Fluorescence
Cells transfected for Ncad-PAGFP and incubated with Ncad-Fc beads were mounted on a confocal microscope (Leica TCS, Deerfield, IL) equipped with a pulsed laser (Mira 900, Coherent) set at 800 nm, whose power was controlled by an electro-optic modulator (Linos Photonics, Milford, MA). The sample was scanned at 800 Hz by the 488-nm laser line and the fluorescence between 500 and 600 nm was collected by a photomultiplier, using a 60x/1.3 objective and a pinhole open to three times the Airy disk (180 µm). To select cells expressing Ncad-PAGFP, we superimposed illumination with the 800-nm biphoton light at low power (
3 mW at the front of the objective), until a cell lighted up (only the cell body, where most of the fluorescence is concentrated was activated during this process). Alternatively, neurons were cotransfected with DsRed, allowing the identification of Ncad-PAGFP-positive cells. Then, a photoactivation sequence was run using the FRAP module on the Leica software: a few reference images were acquired and then an area of 6 x 6 µm around a bead was illuminated with the 800-nm biphoton laser at high power (30 mW) for one scan of 600 ms, and the fluorescence decay was recorded for 10 min with no further photoactivation. Measurements were also made on cell bodies for comparison.
Immunocytochemistry
Cells were fixed for 10 min in warm paraformaldehyde (4% in phosphate-buffered saline [PBS]), and remaining active sites were saturated with 50 mM NH4Cl in PBS for 5 min. For staining of intracellular epitopes, cells were permeabilized with 0.1% Triton X-100 in PBS for 5 min, and nonspecific binding sites were blocked with 1% BSA in PBS for 30 min. Cells were incubated in PBS-BSA with 1:400 rabbit anti-GFP (Molecular Probes, Eugene, OR), 1:100 anti-N-cadherin (Transduction Laboratories), 1:400 anti-
-catenin (Sigma), or 1:500 anti-
-tubulin (Sigma) for 2 h, rinsed extensively, and incubated with 1:800 Alexa568-conjugated goat anti-rabbit antibody (2 mg/ml, Molecular Probes) for 1 h. For F-actin labeling, cells were incubated with 1:500 Alexa488-phalloidin (Molecular Probes) in place of the secondary antibody. After rinsing, coverslips were mounted with Moviol and observed under the Olympus microscope with a 100x objective and appropriate filter sets (Chroma). For surface staining, neurons transfected for Ncad-GFP were incubated in 50 µl culture medium containing 1% BSA and 5 µl GC4 antibody for 20 min at room temperature, then rinsed, and processed as above without the permeabilization step. To estimate the surface versus total density of exogenous N-cadherin receptors, Ncad-GFP transfected cells were labeled using GC4 as a primary antibody under permeabilized or nonpermeabilized conditions, respectively, and the fluorescent signals on neurites and growth cones were compared with those of latex microspheres coated with known amounts of Ncad-Fc and stained identically.
Model of Diffusion-Reaction for Membrane N-Cadherin
Transient Phase: Recruitment of N-Cadherin Receptors. The interaction between Ncad-Fc ligands on the microspheres and Ncad-GFP receptors on the cell surface was treated as a first-order chemical reaction, with association rate kon (µm2 s-1) and dissociation rate koff (s-1), in agreement with measurements on individual bonds (Perret et al., 2002
). The formation of a ligand-receptor bond depends on the diffusion of free receptors to the vicinity of ligand molecules, followed by the reaction step itself (Bell, 1978
). Here, we assumed that the process was reaction-limited, so that the density of homophilic bonds at the microsphere-to-cell interface, C(t), was given by dC/dt = kon (L - C)R - koff C, where L is the ligand density on the microspheres and R is the receptor density on cell surface (both in µm-2). In the binding term, we assumed that the pool of surface receptors was sufficiently large so as to neglect receptor depletion, consistent with the fact that there was no decrease in fluorescence over time in areas outside bead-to-cell contacts. Given the initial condition of no bond and after introducing the pooled parameters K = koff/konR, k = konR + koff, and C
= L/(1 + K), the solution of this differential equation is: C(t) = C
[1 -exp(-kt)]. The fluorescence level around beads that were placed on growth cones at time zero using optical tweezers was normalized by a control level on regions containing no-bead, and the data were fit by the expression 1 + C(t)/(R
), where
is the ratio between total and surface receptors. The measurements of L/R and
allowed us to compute the intrinsic rates kon and koff (Table 1).
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Dynamic Equilibrium: Continuous Exchange of Receptors. At steady state (dC/dt = 0), the bond density reaches the value C
, and there is a continuous exchange between free and bound receptors at a rate koff C
. FRAP experiments in areas outside bead contacts were interpreted using a 1D model of unrestricted diffusion with infinite boundaries, consistent with the geometry of neurites and with the fact that the bleached zone was small compared with the total neuronal surface area. Accordingly, the recovered fluorescence intensity was fit by the expression 1 - erf[1/2(Dt/r2)1/2], where erf is the error function, t is the time and r = 2 µm the radius of the area bleached at time zero (Crank, 1975
). Because it takes on average a time
= d2/2D = 20 s to diffuse across the bead diameter d, whereas the accumulation of fluorescence under beads occurs in several minutes, our hypothesis that diffusion was much faster than reaction seems valid. At bead contacts, the recovery of fluorescence should then occur in two steps: a fast one due to diffusion of unbound receptors and a slower phase due to replacement of bound receptors by unbleached Ncad-GFP molecules. The diffusion term was fit as above by the error function. To obtain the reaction term, we assumed that the rate at which bleached receptors leave the contact was proportional to the density of bleached receptors at time t, as in a Poisson process. The recovered intensity due to ligand-receptor exchange was then (C
- R)[1 - exp(-kofft)]. Normalized fluorescence data were fit by the sum of these two expressions, yielding the two parameters kdiff = D/r2 and koff.
| RESULTS |
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-catenin was barely expressed in S180 cells that do not express any cadherin (Papkoff, 1997
-catenin levels (Figure 1B). Therefore, despite the presence of GFP and PAGFP sequences close to their
-catenin binding site, N-cadherin GFP/PAGFP fusion proteins conserve the ability to interact with and stabilize
-catenin.
Mutants deleted either in the
-catenin binding site (Ncad
cat-GFP) or in the whole cytoplasmic domain (NcadDcyto-GFP), or mutated in the p120ctn interacting region (NcadAAA-YFP; Chen et al., 2003
) were used to investigate the respective roles of N-cadherin intracytoplasmic regions (Figure 1A). Western blots analysis after transient expression of these mutants into S180 or L cells showed that each fusion protein migrates as a double band with expected molecular weights (Figures 1, C and D). Moreover, in contrast to NcadAAA-YFP, which recruited
-catenin as much as wild-type Ncad-GFP, neither Ncad
cat-GFP nor Ncad
cyto-GFP were able to stabilize
-catenin (Figure 1C), which was expected because both mutants lack the
-catenin interacting domain.
N-Cadherin-GFP Proteins Are Expressed at the Neuronal Surface and Present in Growth Cones
We transfected these Ncad-GFP constructs in rat hippocampal neurons at 2-3 DIV and compared their distribution with that of native N-cadherin. All constructs were of chicken origin (except NcadAAA-YFP of mouse origin), allowing in subsequent experiments the use of a chicken-specific antibody directed against the N-cadherin ectodomain (clone GC4) and were used as surrogates of endogenous rat N-cadherin. Both endogenous and transfected N-cadherin were recognized by another mAb directed against the cytoplasmic tail of mouse N-cadherin (immunogen 638-655 of the mature protein that bears 100% sequence homology between rat, mouse, and chicken). In agreement with such homology, the staining intensities for cells transfected for chicken or mouse Ncad-GFP were very similar (Figure 2A). This allowed us to quantify the relative expression levels of Ncad-GFP versus native N-cadherin, which we found to be moderately overexpressed with a ratio of 1.9 ± 0.7 (mean ± SEM, n = 15 cells).
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N-Cadherin-coated Microspheres Adhere Specifically to N-Cadherin-expressing Neurons
We used a recombinant dimeric N-cadherin-Fc fusion molecule, hereafter abbreviated Ncad-Fc, whose functional properties were described previously (Lambert et al., 2000
). Microspheres coated with Ncad-Fc adhered stably to the surface of untransfected cells (Figure 3, A and E). Such adhesion was specific of N-cadherin homophilic interaction because beads coated with Fc fragment, or Ncad-Fc-coated beads in the presence of EGTA (4 mM) or of a function blocking antibody (GC4, dilution 1:50) did not bind to neurons (Figure 3, B and E). Neither treatment was found to particularly affect cell morphology or motility (unpublished data). Neurons transfected with either Ncad-GFP, NcadAAA-YFP, Ncad
cat-GFP, or Ncad
cyto-GFP bound about two times more Ncad-Fc-coated microspheres than untransfected cells or cells transfected with GFP alone (Figure 3E). Moreover, microspheres coated with the GC4 antibody adhered only to cells expressing the chicken Ncad-GFP sequence and not to untransfected cells or GFP-expressing cells (Figure 3, C-E). Taken together, these data show that hippocampal neurons express endogenous N-cadherin, which binds Ncad-Fc ligands on microspheres and that transfection for Ncad-GFP increases the number of functional receptors at the cell surface. Furthermore, we detected strong immunofluorescent signals around Ncad-Fc-coated beads for endogenous N-cadherin,
-catenin (unpublished data),
-catenin, and F-actin (see Figure 5A), all usual markers of cadherin-dependent adhesions (Lambert et al., 2000
, 2002
).
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On Ligation, N-Cadherin Receptors at Growth Cones Rapidly Couple to the Actin Cytoskeleton
We next examined the early steps of N-cadherin dependent contact formation by placing Ncad-Fc- or GC4-coated microspheres on neuronal growth cones with optical tweezers. We chose growth cones exhibiting active lamellipodial and filopodial movements. After maintaining a bead in contact for 10 s, the bead trajectory was followed for 2 min (Figure 4A). Ncad-Fc-coated microspheres displayed a characteristic behavior: 1) they adhered quickly and firmly to the cell surface and could not be subsequently displaced by the optical trap, whose maximal force was around 6 pN; 2) they exhibited a low lateral diffusion coefficient and moved backward, with velocities in the range of 1.5-4 µm/min (Figure 4, B and E). These observations suggested that microspheres were coupled to the continuous retrograde actin flow underlying growth cone motility (Suter et al., 1998
). Indeed, an inhibitor of actin polymerization (cytochalasin D) which dramatically affected the distribution of F-actin and reduced the motility of growth cones (unpublished data), blocked the retrograde motion of the beads, whereas an inhibitor of microtubule polymerization (nocodazole), which efficiently depolymerized microtubules (unpublished data), did not affect bead velocity (Figure 4, B-E). Coupling to the actin flow was independent of bead size, because microspheres of 1 or 4 µm diameter had an equal probability of moving rearward (
90% of the trials) and showed similar velocities (3.2 ± 0.7 µm/min, n = 7 for 1-µm beads vs. 2.7 ± 0.3 µm/min, n = 13 for 4-µm beads). In the presence of blocking antibodies or EGTA, Ncad-Fc-coated microspheres interacted loosely with the cell surface and often detached, as did control microspheres coated with Fc alone, further demonstrating the specificity of the cadherin-cadherin interaction (unpublished data). Moreover, Ncad-Fc-coated beads placed on neurites showed random motion with a high diffusion coefficient (Figure 4, B and C), indicating that the robust coupling was specific to growth cones. Microspheres coated with GC4 antibodies also moved rearward on the growth cones of Ncad-GFP-transfected cells, suggesting that cross-linking of receptors alone was sufficient to induce such coupling to the actin flow (Figure 4, B-E).
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cat-GFP, or Ncad
cyto-GFP. Transfection per se did not affect the motile activity of growth cones. We reasoned that these mutant molecules should compete with endogenous N-cadherin receptors for ligand sites on microspheres and thus reduce the coupling because of their inability to bind cytoplasmic partners. Indeed, the velocity of Ncad-Fc-coated beads was reduced for all three mutants (40% inhibition for Ncad
cyto-GFP, 55% for NcadAAA-YFP, and 16% for Ncad
cat-GFP), compared with cells transfected with wild-type Ncad-GFP (Figure 4, C-E), suggesting that interactions with catenins are critical for the coupling of ligated receptors to the actin flow.
N-Cadherin Receptors Slowly Accumulate around Ncad-Fc-coated Microspheres
We then asked if the coupling between microspheres and the actin cytoskeleton was related to the recruitment of N-cadherin receptors by ligands exposed on microspheres. We thus monitored the fluorescence distribution of Ncad-GFP during 15 min after placing Ncad-Fc- or GC4-coated microspheres on neuronal growth cones by optical tweezers and in parallel measured the microsphere movement. Transfected cells with moderate levels of fluorescence and showing active growth cone motion were selected. We observed a progressive accumulation of fluorescence signal around beads, usually reaching a plateau in
15 min (Figure 5B). In few cases, fluorescent packets came directly to the proximity of the beads, possibly corresponding to N-cadherin-rich vesicles or clusters, but most of the time a monotonous increase in fluorescence around beads was observed, supporting the idea that N-cadherin accumulates around beads via ligand-receptor binding. All beads did not recruit N-cadherin to the same extent (Figure 5A), showing that this effect was specific and not resulting from optical artifacts.
In the same time as they accumulated Ncad-GFP signal, microspheres still moved rearward on growth cones, but with a velocity that decreased in a few minutes, independently of bead coating and mutations in the receptor (Figure 5D). Such tendency of microspheres to progressively slow down was already apparent as a downward deflection of the displacement curves at short term (Figure 4C). Therefore, bead coupling to the retrograde flow and recruitment of receptors occur on two separate time scales.
Fluorescence levels at bead-to-cell contacts were quantified and the data were fit by an equation derived from first-order chemical kinetics (Figure 5C), giving the intrinsic reaction rates of the adhesive interactions and the equilibrium values (Table 1). The accumulation of Ncad-GFP was higher for GC4- than for Ncad-Fc-coated beads, owing to the different affinities of GC4 and Ncad-Fc for Ncad-GFP receptors (Table 1) and also to a competition between endogenous N-cadherin and exogenous Ncad-GFP in the case of Ncad-Fc ligands (the GC4 antibody recognizes only Ncad-GFP). The truncated molecule Ncad
cyto-GFP reached equilibrium later than its wild-type counterpart, reflecting slower kinetics both in the association and the dissociation steps (Figure 5C; Table 1). In contrast, the NcadAAA-YFP mutant reached equilibrium faster than both Ncad-GFP and Ncad
cyto-GFP, indicating a higher association rate and/or lower dissociation rate, although we could not distinguish between these possibilities (Figure 5C; Table 1). Finally, Ncad
cat-GFP was characterized by a lower association rate and a higher dissociation rate than the wild-type molecule (Figure 5C; Table 1). These data thus indicated subtle differences in the dynamic behavior of the different receptor constructs. However, this approach required the quantification of several parameters (ligand and receptor densities, surface vs. total receptor expression, and kinetic rates), which had a high variance. We therefore performed more direct measurements of receptor turnover in areas of bead contact at equilibrium, using a photobleaching technique.
FRAP Experiments Reveal the Slow Turnover of N-Cadherin Receptors at Cell-Microsphere Contacts
We photobleached bead-to-cell contacts exhibiting Ncad-GFP recruitment, with the idea that if bleached receptors could dissociate from their ligands on the bead and be replaced by unbleached receptors, the fluorescent signal should increase over time and reveal such exchange. To first evaluate the diffusion properties of Ncad-GFP receptors, we carried out photobleaching experiments on control regions of neurites and growth cones (Figure 6A). The fluorescence recovery was well described by a model of unbiased diffusion (Figure 6C), indicating that most N-cadherin receptors were freely mobile with a diffusion coefficient of 0.1 µm2/s. This value is slightly higher than that reported for E-cadherin using single particle tracking (Sako et al., 1998
) and can be attributed to differences in the measurement methods (Kucik et al., 1999
) or to a fraction of intracellular Ncad-GFP, which diffuses more quickly.
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1.2 in 12 min. In its initial phase, the recovery curve was superimposable to that obtained from control experiments on neurites or growth cones (no bead), suggesting that the gain of fluorescence was due to the diffusion of unbound receptors (Figure 6C). However, the fluorescent ratio around beads finally reached higher levels than on control areas, suggesting that a fraction of the fluorescence on the beads corresponding to trapped receptors recovered with a slow turnover. The data were well described by a diffusion-reaction model (Figure 6C), allowing the characterization of the turnover rate of ligand-receptor bonds koff = 2.3 ± 0.4 h-1 (n = 31), which was in the same range as that obtained by quantifying the kinetics of Ncad-GFP recruitment (Table 1). Such value means that the whole population of receptors trapped beneath a microsphere exchanges within 45 min (30% in 12 min). This turnover was insensitive to bead size, because FRAP experiments on Ncad-GFP receptors using 1-µm microspheres coated with Ncad-Fc gave a similar turnover rate (koff = 3.6 ± 1.8 h-1, n = 7). Thereafter, we used 4-µm beads, which provide a higher signal-to-noise ratio in fluorescence.
The Exchange Regime Is Characteristic of the N-Cadherin Homophilic Interaction
To further validate the hypothesis that fluorescence recovery originates from turnover of N-cadherin homophilic bonds at the bead-to-cell interface, we carried out a series of control experiments. We first blocked N-cadherin homophilic adhesion by adding 4 mM EGTA at the beginning of the FRAP experiment and observed a disappearance of the slow recovery regime (Figure 6C). This came in agreement with the hypothesis that bonds which dissociate cannot be replaced by new bonds, because free receptors and free ligands are unable to bind again. At higher concentrations of EGTA (10 mM), we observed a progressive disappearance of Ncad-GFP signal at N-cadherin contacts (unpublished data). In addition, when the GC4 antibody was used in place of Ncad-Fc as a ligand on the microspheres, fluorescence recovery was significantly inhibited (Figures 6D). This was likely due to the fact that the antibody-antigen bond is more stable than the natural N-cadherin/N-cadherin bond, such that bleached receptors stay longer in the contact. As the reverse control, we studied the mobility of NrCAM, a member of the IgCAM family not reported to interact with cadherins (Falk et al., 2004
), at contacts with Ncad-Fc microspheres. Transfected NrCAM-GFP receptors were expressed at the neuronal surface, as revealed by live staining with anti-GFP (unpublished data) and, as expected, showed little accumulation around Ncad-Fc-coated beads (baseline, Figure 6D). More precisely, in neurons cotransfected for Ncad-DsRed (Lambert et al., unpublished results) and NrCAM-GFP, the enrichment factor around Ncad-Fc or GC4 microspheres was 2.6 ± 0.2 for the Ncad-DsRed signal versus 1.3 ± 0.1 in the NrCAM-GFP channel, as measured on the same beads (n = 33, p < 0.0001). This experiment demonstrated the specificity of fluorescence accumulation around microspheres and ruled out potential optical artifacts, owing for example to membrane wrapping of microspheres within partial phagocytosis (Lambert et al., 2000
). The recovery of fluorescence for NrCAM-GFP was analogous to that on control neurites with an absence of long-term recovery, showing that the exchange regime was indeed a specific feature of Ncad-GFP receptors (Figure 6D). Finally, to rule out possible photodamage, we bleached the whole Ncad-GFP signal of several neurons using the laser then incubated cells with Ncad-Fc-coated beads, and stained the receptors with anti-GFP. Beads were found to recruit immunoreactive GFP (unpublished data), indicating that photobleached Ncad-GFP receptors were still functional.
Photoactivation Experiments Confirm that N-Cadherin Receptors Slowly Leave Adhesive Contacts
To show unambiguously that N-cadherin receptors could leave the adhesive contact and diffuse away, we carried out experiments using neurons transfected with Ncad-PAGFP. The fluorescence was briefly activated in areas of contact with Ncad-Fc-coated beads, and the fluorescence level was monitored over time (Figure 7A). A significant decay of fluorescence was observed in areas of bead contacts, which was not due to photobleaching because control experiments on cell bodies showed no decrease of fluorescence under the same conditions (Figure 7B). The curves were not the exact mirror images of FRAP experiments, in that they lacked the fast initial phase that was expected from the presence of free receptors. This was somewhat expected because photoactivation was carried out using a confocal microscope in biphoton mode, so that Ncad-PAGFP was excited in a narrow zone and fast diffusion of out-of-focus components was not detected. Indeed, FRAP experiments carried out with a confocal microscope also showed a reduction of the fast regime fraction (unpublished data). Furthermore, because of the low efficiency of the photoactivation process, we were selecting beads with a high Ncad-GFP signal, where the density of bound receptors was much higher than that of free receptors. Accordingly, we found it quite difficult to photoactivate Ncad-PAGFP on neurites or growth cones alone. Nevertheless, the fit with a monoexponential decay gave a turnover rate of 5.7 ± 0.9 h-1 (n = 9) in relative agreement with that obtained from FRAP experiments.
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To more specifically probe the molecular interactions involved in this process, we carried out FRAP experiments on mature contacts between Ncad-Fc-coated beads and neurons transfected for the mutated receptors Ncad
cyto-GFP, Ncad
cat-GFP, or NcadAAA-YFP. The initial phase of the recovery curve were indistinguishable for all constructs (Figure 8, B and C), indicating that the diffusion properties of the truncated molecules were similar to those of the wild type. However, the second phase of the fluorescence recovery was markedly different. For the constructs Ncad
cyto-GFP and NcadAAA-YFP, which were as enriched as Ncad-GFP at bead contacts (ratio bead/neurite about 2), the exchange regime was abolished (Figure 8, B and C) and characterized by significantly smaller koff values (Figure 8D). In contrast, Ncad
cat-GFP receptors were recruited less than Ncad-GFP receptors at bead contacts (ratio bead/neurite 1.7) and recycled more rapidly, as revealed by a higher koff (Figure 8D). These data validated the measurements obtained from recruitment experiments (Table 1) and demonstrated that the turnover of N-cadherin receptors at N-cadherin contacts is finely regulated by catenin partners.
Bond Exchange Occurs at Similar Rates in Natural Neuronal and Glial Contacts
Finally, to show that microsphere adhesion mimicked natural contacts quite well, we carried out similar FRAP experiments on spontaneous neuronal and glial contacts also showing Ncad-GFP accumulation (Figure 9, A and B). The ratio between the fluorescence level in the contacts and that on glial lamellipodia or adjacent regions on neurites was also about 2 (Figure 9C), as reported in other studies (Chen et al., 2003
). Strikingly, the recovery curve obtained for these contacts followed closely that obtained for contacts between Ncad-Fc-coated microspheres and neurons (Figure 9C), with very similar exchange rates (Figure 8D).
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| DISCUSSION |
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The expression of NcadAAA-YFP, Ncad
cat-GFP, or Ncad
cyto-GFP mutants all diminished the rearward motion of Ncad-Fc-coated beads on growth cones, albeit to varying degrees. Although we cannot totally exclude the possibility that the expression of mutated receptors may affect actin motility itself, the fact that NcadAAA-YFP and Ncad
cyto-GFP were more potent inhibitors than Ncad
cat-GFP suggests that the juxtamembrane domain, rather than the
-catenin binding region, is implicated in the coupling of N-cadherin to the actin flow. This may involve a direct physical linkage, for example, via p120, which has recently been shown to bind cortactin (Martinez et al., 2003
), a protein that interacts with filamentous actin and is closely associated with cadherin contacts (El Sayegh et al., 2004
; Helwani et al., 2004
). It may also involve signaling molecules such as the nonreceptor kinase FER and its downstream target cortactin, which regulates the actin nucleating complex Arp 2/3, or a Rac1 pathway (El Sayegh et al., 2005
; Kovacs et al., 2002
; Lambert et al., 2002
). Alternatively, the ability of mutant molecules to compete with endogenous N-cadherin for the coupling to the actin flow also depends on their ligand-binding affinity, which varies among mutants and is particularly low for Ncad
cat-GFP (see below). Beads coated with GC4 antibody on cells transfected for Ncad-GFP moved rearward as fast as beads coated with Ncad-Fc, suggesting that the lateral clustering of N-cadherin receptors is alone responsible for the efficient coupling to the actin flow. It is not excluded that the antibody, whose epitope lies close to the ligand-binding site, also activates the receptor (Harrison et al., 2005
). The clustering effect was also observed for L1-myc receptors bound to anti-myc-coated beads (Gil et al., 2003
) and at variance with the behavior of integrins, whose coupling to the actin flow specifically requires ligand binding (Choquet et al., 1997
). Altogether, these data show that neuronal N-cadherin mobilization in the growth cone is strongly coupled to the anchoring of this receptor to rearward moving actin, an event that was never observed along neurite shafts. This process may be important for both axonal elongation and neuronal contact formation requiring extensive actin cytoskeleton reorganization.
When monitoring the fluorescence distribution around microspheres, both Ncad-Fc- and GC4-coated beads recruited Ncad-GFP in a time course of several minutes. This process was much slower than the rapid coupling to the actin flow, suggesting that the retrograde motion of beads required only a limited number of bonds not detectable from the GFP signal at early time points. Conversely, the decrease of microsphere velocity on growth cones may be related to the accumulation of receptors beneath the beads, tending to increase lateral friction, possibly through connection to immobile components of the cytoskeleton. Likewise, in cells transfected with full-length E-cadherin, anti-E-cadherin-coated beads can be displaced over very limited distances by an optical trap due to strong connection of the receptor to the cytoskeleton (Sako et al., 1998
). At equilibrium, the recruitment of N-cadherin-GFP beneath Ncad-Fc beads remained moderate (ratio bead/neurite about 2.3), suggesting that it may be limited either by the availability of N-cadherin receptors or the affinity of N-cadherin bonds. The fast and unrestrained mobility of unbound N-cadherin receptors measured by FRAP on growth cones and neurites indicated that recruitment was not limited by receptor diffusion, but rather by the reaction itself, in agreement with a recent study showing a weak effect of lateral mobility on the rate of IgCAM recruitment at neuronal contacts (Thoumine et al., 2005
). Indeed, the kinetic analysis showed that the recruitment of N-cadherin around beads corresponded to a dynamic equilibrium with continuous bond association and dissociation, which we explored in more detail using photobleaching experiments at bead-to-cell contacts.
After previous FRAP studies on E-cadherin (Adams et al., 1998
), VE-cadherin (Delanoe-Ayari et al., 2004
), N-cadherin (Causeret et al., 2005
), or NCAM receptors (Jacobson et al., 1997
) at cell-cell contacts, we initially carried out a conventional analysis, normalizing all the recovery curves by their initial values. When we did so, the fluorescence intensity in contact areas reached a plateau about 50% of the initial value (in agreement with the reports cited above), revealing the presence of an immobile fraction of receptors. This suggested that the various receptors were trapped almost irreversibly by long-lasting interactions with their counterreceptors. However, a careful analysis based on diffusion and trapping, longer observations, and normalization against initial fluorescent intensities in control areas where N-cadherin remained unbound made possible the identification of a slow turnover of receptors. The recovery curves were strikingly similar for bead-cell contacts, where ligands are immobilized, and for cell-cell contacts, where receptors are freely moving within the two apposed cell membranes. In that case, bonds can a priori slide as individual pairs, although in practice they may be stabilized by interactions with cytoplasmic partners (Sako et al., 1998
; Nishimura et al., 2003
). Because similar recovery curves were obtained for these two situations, it seems again that diffusion is not a limiting step in the renewal of N-cadherin adhesions. Recycling of cadherins through endo-exocytosis has been documented (Chen et al., 2003
), but involves a relatively small fraction of membrane receptors, i.e., only 15% in the case of E-cadherin under basal conditions (Le et al., 1999
). Furthermore, depolymerization of microtubules did not significantly affect the recovery of fluorescence, so it is unlikely that the receptor turnover observed here comes from trafficking events from and to intracellular compartments, but rather involves molecules already present at the cell surface.
Analogous photobleaching experiments on contacts between TAG-1-coated beads and NrCAM-GFP-expressing cells showed an absence of exchange regime (Falk et al., 2004
), suggesting that the linkage between NrCAM and TAG-1 is rather stable. Similarly, the recovery of Ncad-GFP signal around GC4-coated beads was very slow, giving a lifetime of several hours typical of an antibody-antigen bond (Pierres et al., 1998
). Furthermore, FRAP experiments carried out on Ncad-GFP-rich adhesion sites formed between myogenic cells and a flat substrate coated with Ncad-Fc (Gavard et al., 2004
) gave turnover rates similar to those obtained for contacts between Ncad-Fc beads and neurons, showing that the particular geometry of microspheres does not perturb the measurements (Lambert et al., unpublished results). Thus, the data allowed to unravel the existence of long-lasting N-cadherin adhesive bonds compatible with the maintenance and the plasticity of cellular contacts needed during initiation and maturation of contacts between growth cones and neighboring neuronal or glial cell surfaces.
The lifetime of about 1 h for the N-cadherin bond obtained here is much longer than the values reported earlier for other cadherins in single molecule studies, i.e., on the order of 1 s (Perret et al., 2002
; Baumgartner et al., 2003
). Several differences can explain this apparent discrepancy. First, in laminar flow chamber studies, the authors used EC1-EC2 fragments grafted to microspheres or flat surfaces. The other domains EC3-5 might affect the adhesive capabilities, as shown by the unbinding force profile obtained by AFM (Sivasankar et al., 1999
). Recent measurements on entire extracellular domains using the bioforce probe apparatus suggest indeed that E-cadherin bonds can show