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Genes to Cells (2005) 10, 381-392. doi:10.1111/j.1365-2443.2005.00845.x
© 2005 Blackwell Publishing or its licensors

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A novel function of WAVE in lamellipodia: WAVE1 is required for stabilization of lamellipodial protrusions during cell spreading

Daisuke Yamazaki1,2, Takashi Fujiwara3, Shiro Suetsugu1,2 and Tadaomi Takenawa1,2,*

1 Department of Biochemistry, Institute of Medical Science, University of Tokyo, Tokyo, Japan
2 CREST, Japan Science and Technology Corporation
3 Department of Biological Resources, Integrated Center for Sciences, Ehime University, Ehime, Japan


    Abstract
 Top
 Abstract
 Introduction
 Results
 Discussion
 Experimental procedures
 Supplementary material
 References
 
When a cell spreads and moves, reorganization of the actin cytoskeleton pushes the cell membrane, and the resulting membrane protrusions create new points of contact with the substrate and generate the locomotive force. Membrane extension and adhesion to a substrate must be tightly coordinated for effective cell movement, but little is known about the mechanisms underlying these processes. WAVEs are critical regulators of Rac-induced actin reorganization. WAVE2 is essential for formation of lamellipodial structures at the cell periphery stimulated by growth factors, but it is thought that WAVE1 is dispensable for such processes in mouse embryonic fibroblasts (MEFs). Here we show a novel function of WAVE in lamellipodial protrusions during cell spreading. During spreading on fibronectin (FN), MEFs with knockouts (KOs) of WAVE1 and WAVE2 showed different membrane dynamics, suggesting that these molecules have distinct roles in lamellipodium formation. Formation of lamellipodial structures on FN was inhibited in WAVE2 KO MEFs. In contrast, WAVE1 is not essential for extension of lamellipodial protrusions but is required for stabilization of such structures. WAVE1-deficiency decreased the density of actin filaments and increased the speed of membrane extension, causing deformation of focal complex at the tip of spreading edges. Thus, at the tip of the lamellipodial protrusion, WAVE2 generates the membrane protrusive structures containing actin filaments, and modification by WAVE1 stabilizes these structures through cell-substrate adhesion. Coordination of WAVE1 and WAVE2 activities appears to be necessary for formation of proper actin structures in stable lamellipodia.


    Introduction
 Top
 Abstract
 Introduction
 Results
 Discussion
 Experimental procedures
 Supplementary material
 References
 
Directed cell movement consists of cycles of four ordered processes: membrane protrusion at the leading edge, adhesion of the protrusion to the substrate, movement of the cell body, and retraction of the rear part of the cell (Pollard & Borisy 2003). During the first process, rapid actin polymerization, which is regulated by Rho family small GTPases Rac and Cdc42, causes protrusion of the membrane (Etienne-Manneville & Hall 2002). Wiskott–Aldrich syndrome protein (WASP) family members are key regulators that link such small GTPases to actin reorganization (Takenawa & Miki 2001; Miki & Takenawa 2003). Downstream of Rac and Cdc42, WASP family proteins activate the Arp2/3 complex through their C-terminal catalytic domains (VCA domains) and induce actin polymerization.

To generate the locomotive force, the protrusive membrane must adhere to the substrate. The molecular interaction underlying this adhesion remains unknown. Recently, interaction between the Arp2/3 complex and vinculin was found to be essential for lamellipodium formation (DeMali et al. 2002). Vinculin recruits Arp2/3 complex to focal complexes and nearby Arp2/3 activators at the leading edges. Formation of a vinculin-Arp2/3 complex might physically couple newly polymerized actin to sites of cell-substrate adhesion. These findings suggest the presence of mechanisms that coordinate actin reorganization and cell-substrate adhesion.

Giannone et al. (2004) proposed an attractive model to explain extension and adhesion of lamellipodia. In this model, a rearward actin wave (retrograde flow) arising at the back of the lamellipodial edge conveys the contractile signal, which involves myosin light chain kinase (MLCK), from the tip to the base of the lamellipodium. MLCK activates myosin-based contractility and causes contraction of actin structures in the lamellipodial protrusion. The rearward force applied to the tip of the lamellipodium enhances integrin binding to the extracellular matrix and initiates integrin-mediated signaling, thereby stabilizing the points of adhesion. Activated integrin signaling causes another round of MLCK release at the front of the lamellipodium. This positive feedback loop causes periodic interruptions in the process of extension of the membrane. However, it is still unclear how actin reorganization is regulated in such complex processes.

WASP family Verproline-homologous proteins (WAVEs) are crucial for Rac-induced membrane ruffling (Miki et al. 1998). Three WAVE proteins (WAVE1-3) have been identified in mammals (Suetsugu et al. 1999). These WAVEs have distinct tissue distributions, and their actin polymerization activities are regulated differentially by associations with various molecules (Miki et al. 2000; Westphal et al. 2000; Eden et al. 2002; Miki & Takenawa 2002; Soderling et al. 2002; Blagg et al. 2003; Bogdan & Klambt 2003). In a previous study, we established cultures of mouse embryonic fibroblasts (MEFs) from WAVE1 knockout (KO) and WAVE2 KO embryos and showed that WAVE1 and WAVE2 have distinct roles in different membrane ruffling structures in response to platelet-derived growth factor (PDGF) (Suetsugu et al. 2003). WAVE1 is essential for formation of membrane protrusions at the dorsal cell surface (dorsal ruffles) and is localized to the upper part of membrane ruffles. WAVE2 is required for formation of membrane ruffles at the cell periphery (peripheral ruffles) and is localized to the extreme edge of such ruffles; however, WAVE1-deficiency causes no defect during such processes. Thus, WAVE1 and WAVE2 appear to induce actin polymerization in different directions according to their localization and to promote formation of different membrane structures.

Here we show a novel function of WAVE1 in lamellipodia. WAVE1-deficiency increases the extension speed of lamellipodial protrusions, causing deformation transient cell-substrate adhesive structures in lamellipodia. It is suggested that WAVE1 is required for formation of stable lamellipodial protrusions with adhesions to a substrate.


    Results
 Top
 Abstract
 Introduction
 Results
 Discussion
 Experimental procedures
 Supplementary material
 References
 
WAVE1 stabilizes lamellipodial protrusion at the cell periphery

To investigate the relation between membrane-protrusive actin reorganization and the formation of cell-substrate adhesions in lamellipodia, we prepared WAVE-deficient MEFs as previously described (Fig. 1A) (Suetsugu et al. 2003). Of the WAVE family of proteins, only WAVE1 and WAVE2 are expressed in wild-type (WT) MEFs. To observe the process of coordination of membrane extension and cell-substrate adhesion, we observed cell spreading on glasses coated with fibronectin (FN). FN induces integrin-mediated activation of Rac and Cdc42 and subsequent formation of membrane protrusions (Price et al. 1998).




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Figure 1  Cell spreading of WAVE KO MEFs on FN. (A) Western blot analysis. Extracts of MEFs were probed with antibodies to WAVE1, WAVE2, or actin. The upper bands in the upper panel depict phosphorylated WAVEs. (B-H) Phase-contrast sequence of the spreading MEFs. (B) Wild-type (WT) MEFs. (C) WAVE1 KO MEFs. (D) WAVE1 KO MEFs transfected with vector alone. (E) WAVE1 KO MEFs expressing exogeneous WAVE1 (rescued WAVE1 KO MEFs). (F) WAVE2 KO MEFs. (G) WAVE2 KO MEFs transfected with vector alone. (H) WAVE2 KO MEFs expressing exogeneous WAVE2 (rescued WAVE2 KO MEFs) were plated on FN. Interval between sequential frames is 300 s. Arrows in C and D indicate curling of spreading edges. (F-H) High magnifications of the boxed regions are shown in right-hand corner. Arrows in F and G indicate the web-like membrane protrusions. Bar: 5 µm. (I) Classification of the membrane structures of WAVE1 KO MEFs during spreading on FN. Lamellipodia, cells with lamellipodial protrusions across 75% of the cell periphery. Curl up, cells with curling membranes across over (L) or below (S) 10% of the cell periphery. Ruffle, cells with ruffled membranes that did not curl up. Others, other cells. Values are given as means of counted cells and standard errors from three independent quantifications. n: total numbers of analyzed cells. (J) Classification of the membrane structures of WAVE2 KO MEFs during spreading on FN. Lamellipodia, cells with lamellipodial protrusions (including ruffled membranes) across 75% of the cell periphery. Curl up, cells with curling membranes across over 10% of the cell periphery. Irregular, cells spreading irregularly with finger-like projections. Others, other cells. Values are given as means of counted cells and standard errors from three independent quantification. n: total numbers of analyzed cells.

 
When plated on FN, most of WT MEFs spread uniformly with lamellipodia around the cell periphery (Fig. 1B,I; Supplemental Fig. S1).

WAVE1 KO MEFs also showed smooth, sheet-like protrusions at the cell periphery similar to those in WT MEFs. However, the spreading edges tended to curl up and retract, followed by formation of new protrusions (Fig. 1C, arrows; Supplemental Fig. S2). These processes occurred repeatedly even after the cells had spread fully. Such curling up of the spreading edges was not observed in WT MEFs, though some WT MEFs had ruffled edges that did not curl up (Fig. 1I, ruffle). When observed by scanning electron microscopy, curling up of the spreading edges was confirmed in WAVE1 KO MEFs (Fig. 2B).



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Figure 2  Electron microscopy. Scanning electron photomicrographs of (A) WT, (B, C) WAVE1 KO, and (D, E) WAVE2 KO MEFs plated on FN. (C, E) High magnification of the regions indicated by arrows in B and D, respectively. Arrows in C indicate the remaining adhesion. Arrowhead in E indicates finger-like protrusions. Arrow in E indicates the tip of a web-like protrusion. Bar: (A) 7.5 µm; (B) 7.5 µm; (C) 3 µm; (D) 10 µm; (E) 1 µm.

 
In contrast to WT MEFs, most WAVE2 KO MEFs spread non-uniformly with finger-like projections (Fig. 1F). In peripheral areas of WAVE2 KO MEFs, finger-like projections were observed first, and narrow web-like membrane protrusions (arrows in Fig. 1F) then developed somewhat irregularly between these projections (Supplemental Fig. S3). These protrusive membrane structures were unstable and soon disappeared. When observed by electron microscopy, the spreading edges did not adhere to the substrate and aberrant filopodia-like structures were confirmed (Fig. 2D,E). Thus, WAVE2-deficiency disturbed the structure of smooth lamellipodial protrusions as well as peripheral ruffle formation induced by growth factors (Suetsugu et al. 2003; Yamazaki et al. 2003).

We next examined whether expression of exogeneous WAVE1 and WAVE2 could restore formation of normal lamellipodial protrusions in WAVE1 and WAVE2 KO MEFs, respectively. WAVE1 KO MEFs expressing only vector showed features similar to those of untransfected WAVE1 KO MEFs (Fig. 1D). However, WAVE1 KO MEFs expressing exogeneous WAVE1 (rescued WAVE1 KO MEFs) generated lamellipodial membrane protrusions similar to those in WT MEFs (Fig. 1E). The percentage of WAVE1 KO MEFs with lamellipodia after expression of exogeneous WAVE1 (74.1 ± 7.9%) was similar to that in WT MEFs (81.3 ± 5.0%) (Fig. 1I). Thus, WAVE1 is not essential for formation of lamellipodial membrane protrusions but is required for their stabilization.

WAVE2KO MEFs expressing only vector showed features similar to those of untransfected WAVE2 KO MEFs (Fig. 1G). Uniform cell spreading with lamellipodia was partially restored in WAVE2 KO MEFs expressing exogeneousWAVE2 (rescued WAVE2 KO MEFs) (55.2 ± 11.2%) compared with WT MEFs (88.6 ± 3.2%) (Fig. 1H,J). This partial restoration may reflect differential levels and/or regulation of exogeneous WAVE2 expression in WAVE2 KO MEFs. Interestingly, some rescued WAVE2 KO MEFs (10.0 ± 4.2%) showed curling up of the spreading edges observed in WAVE1 KO MEFs (Fig. 1J). Thus, in contrast to WAVE1, WAVE2 is essential for formation of lamellipodial structures.

Distribution of actin filaments in WAVE-deficient MEFs

To examine whether WAVE-deficiency affects distribution of actin filaments at the spreading edges, we examined spreading MEFs with phalloidin staining. Lamellipodial protrusions contain a highly branched actin-filament meshwork (Svitkina & Borisy 1999). During spreading on FN, lamellipodial protrusions were supported by high-density actin filaments at the spreading edges of WT MEFs (Fig. 3A). Actin structures at the peripheral areas in WT MEFs could be divided into two zones: a first actin-dense zone at the extreme periphery of the cells (indicated by arrows in Fig. 3B) and a second central zone of lower actin density. However, in WAVE1 KO MEFs with curling edges, density of actin filaments at the extreme periphery decreased and a boundary between two zones was ambiguous as compared with WT MEFs (compare Fig. 3A,B with I, J, respectively). Thus, actin filaments at the spreading edges were not properly organized in WAVE1 KO MEFs. Because expression of exogeneous WAVE1 in WAVE1 KO MEFs corrected the distribution of actin filaments, WAVE1 appears to be essential for formation of normal actin structures in lamellipodia (Fig. 3R).



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Figure 3  The spreading edges of WAVE KO MEFs. Spreading MEFs were fixed and stained for actin filaments (A,B, D–F, H–J, L–N, and P–T), WAVE1 (C, D, and O–Q), and WAVE2 (G, H, K, L, and S). (B–D, F–H, J–L, and N–P). High magnification of the boxed regions in A, E, I, and M, respectively. (A–H) WT MEFs. (I–L) WAVE1 KO MEF. (M–P) WAVE2 KO MEF. (Q, R) rescued WAVE1 KO MEF, and (S, T) rescued WAVE2 KO MEF with lamellipodial protrusions. (I) In WAVE1 KO MEFs, the spreading edges curl up (arrows) but new spreading edges emerge (arrowheads). (B, F, J, R, and T) Accumulation of actin filaments at the extreme periphery (indicated by arrows) was decreased in WAVE1 KO MEFs as compared with WT and rescued WAVE KO MEFs. (C, D, and Q) The localization of WAVE1 at the spreading edges was discontinuous as indicated by arrowheads. (D, H, L, P, Q, and S) Merged images of the signals for actin filaments (red) and WAVE (green) are shown. Arrowheads in O and P indicate localization of WAVE1 at the actin bundles. Bar: (A, E, I, and M) 5 µm; (B–D, F–H, J–L, and N–T) 1.3 µm.

 
When the spreading edges of WAVE2 KO MEFs were stained for actin filaments, the aberrant long bundles of actin filaments were visible and the web-like membrane protrusions were scarcely supported by actin filaments (Fig. 3M,N). This finding suggests that lamellipodial structures are almost absent in WAVE2 KO MEFs. The accumulation of actin filaments at the spreading edges in uniformly spreading, rescued WAVE2 KO cells was comparable to that in WT MEFs (Fig. 3T). These results suggest that WAVE2 is required to generate the membrane protrusive structures of actin filaments in lamellipodia. Thus, at the lamellipodial edges, WAVE2 forms frameworks of actin filaments that protrude the membrane parallel to the substrate, and sequential modification by WAVE1 organizes the actin structures.

Localization of WAVEs during cell spreading on FN

To define the role of WAVEs at the spreading edges, we investigated the localization of these proteins in spreading WT MEFs. When stimulated by PDGF, WAVE1 was scarcely detected at the tip of peripheral ruffles (Suetsugu et al. 2003). However, while spreading on FN, WAVE1 showed a punctate pattern throughout the cytoplasm, and some WAVE1 was localized at the edges of lamellipodial protrusions (Fig. 3C,D). This localization of WAVE1 at the lamellipodial edge often appeared discontinuous (Fig. 3C, arrowheads). Exogeneously expressed WAVE1 showed similar localization in rescued WAVE1 KO MEFs (Fig. 3Q). Thus, WAVE1 was localized at the tips of spreading edges different from peripheral ruffles induced by PDGF. In contrast, WAVE2 was clearly and continuously localized at the extreme edges of lamellipodial protrusions (Fig. 3G,H). Thus, WAVE1 and WAVE2 show different localization patterns in lamellipodia.

Localization of WAVE1 at the web-like protrusions in WAVE2 KO MEFs was continuous and clearer than that at the lamellipodial edges in WT MEFs (compare Fig. 3C,D with 3O, P, respectively). Despite strong WAVE1 expression, defective lamellipodium formation was not compensated in WAVE2 KO MEFs. Similarly, at the spreading edges in WAVE1 KO MEFs, the localization of WAVE2 was confirmed. These results suggest that WAVE1 and WAVE2 cannot compensate for each other's deficiencies.

Cell-substrate adhesion in WAVE1 KO MEFs

To investigate the role of WAVE1 in stabilization of lamellipodia, we examined whether cell-substrate adhesions formed properly at the spreading edges in WAVE1 KO MEFs. At the spreading edges in WT MEFs, focal complexes were localized just behind the extreme edges in the lamellipodial protrusions (Fig. 4A–D). WAVE1 and WAVE2 were localized at more forward position in the lamellipodial protrusions compared with focal complexes (Fig. 4D,I). Intensity profiles reveal that there was no co-localization of vinculin and WAVEs (Fig. 4J,K). In contrast, Arp2 and vinculin were partially co-localized at the spreading edges (Fig. 4L,M).



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Figure 4  Cell-substrate adhesion of spreading WAVE1 KO MEFs. Spreading WT (A–D, I and L) or WAVE1 KO (E–H) MEFs on FN were fixed and stained for vinculin (A, B, D–F, H, I, and L), WAVE2 (A, C–E, and G–H), and Arp2 (L). (A, D, E, H, I, and L) Merged images of the signals for vinculin (red) and WAVE or Arp2 (green) are shown. (B–D and F–H) High magnification of the boxed regions in A and E, respectively. (E) Arrowheads in E indicate the beginning of curling up. Bar: (A, E) 10 µm; (B–D, F–I, and L) 2.5 µm. Asterisks in D, I and L indicate direction of intensity profiles in J and K, respectively. (J, K and M) Intensity profiles were made along the lines in D, I, and L, respectively.

 
When WAVE1 KO MEFs spread to some extent, part of WAVE2 at the tip of spreading edges transited from the basal level to the upper level (Fig. 4E, large arrowheads), indicating that the spreading edges were beginning to curl up in this cell. In such WAVE1 KO MEFs, focal complexes were absent at the tips although focal adhesions were observed in WAVE1 KO MEFs (Fig. 4E–H). When observed by scanning electron microscopy, although the spreading edge curled up, part of membranes adhered to the substrate and did not curl up (Fig. 2C, arrows). These observations suggest that formation of adhesive structures was inhibited only at the spreading edges in WAVE1 KO MEFs. Thus, transient formation of focal complexes was inhibited in WAVE1 KO MEFs, resulting in destabilization of lamellipodial protrusions.

Membrane dynamics of WAVE1KO MEFs during spreading on FN

Recently, it was shown that there was a close relation between membrane extension and adhesion to a substrate in lamellipodia during cell spreading on FN (Giannone et al. 2004). To better understand the membrane dynamics of WAVE1 KO MEFs, we made kymographs of WT and WAVE1 KO MEFs during cell spreading on FN. Kymographs show membrane activity at spreading edges (Bear et al. 2002). When WT MEFs spread, periodic interruptions of membrane extension were observed at the spreading edges (Fig. 5A, boxed region in the far right panel). The extension speed of the spreading edges decreased gradually when periodic interruptions were observed (compare the neighboring phases in Fig. 5A). In contrast, there was no interruption of membrane extension in WAVE1 KO MEFs until the spreading edges curled up (Fig. 5B, boxed region in the right most panel). The speed of membrane extension in WAVE1 KO MEFs before curling was relatively constant and was approximately 2.5 times faster than that of WT MEFs before periodic interruptions (Fig. 5C). When exogeneous WAVE1 was expressed in WAVE1 KO MEFs, membrane extension speed decreased to that observed in WT MEFs. Thus, WAVE1 KO MEFs showed different membrane dynamics from WT MEFs before curling up of spreading edges.




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Figure 5  Membrane dynamics of WAVE1 KO MEFs. (A, B) Left four panels are the first and the last frames of time-lapse movies of WT (A) or WAVE1 KO (B) MEFs for kymographs, respectively. Elapsed time: s. Right two panels are kymographs of spreading MEFs on FN of 600 s. Kymographs show membrane activity along the lines in the left panels. High magnification images of the boxed regions in kymographs are shown in the left-hand corner. Arrows indicate periodic interruptions of lamellipodial membrane protrusions. Bar: 5 µm. (C) Quantification of membrane extension speed at spreading edges as described in Experimental procedures. *P < 0.0001. P-values were calculated using 2-tailed Student t-tests. n: total numbers of analyzed protrusions. (D, E) Time-lapse sequences of the tips of spreading edges of WT (D) or WAVE1 KO (E) MEFs shown in A and B, respectively. Larger panels show the beginning and the end of the time-lapse sequences shown in the smaller panels. High magnification images of the boxed regions in the larger panels are shown in the smaller panels. *rearward actin wave. Bar: (large panels) 5 µm; (small panels) 1.7 µm.

 
Rearward actin waves are thought to convey the contractile signal that causes interruptions of membrane extension (Giannone et al. 2004). In our experiments, black shadows moved radially inward from the tip of the extending membrane in spreading WT MEFs (Fig. 5D, asterisks). These shadows occurred periodically and repeatedly at the tip of the spreading edge and disappeared at the base of lamellipodia. Therefore, these shadows correspond to the rearward actin waves described by Giannone et al. At the rapidly spreading edges of WAVE1 KO MEFs, no rearward actin wave was observed (Fig. 5E). Such a defect in the rearward actin wave in WAVE1 KO MEFs may underlie the lack of interruption in formation of lamellipodial protrusion.


    Discussion
 Top
 Abstract
 Introduction
 Results
 Discussion
 Experimental procedures
 Supplementary material
 References
 
In the present study, we show a novel function of WAVE1 in lamellipodiun formation. It has been shown that WAVE is crucial for formation of lamellipodial structures in various cell types. This is the first report about WAVE's function in adhesion of lamellipodial protrusions. Different from peripheral ruffles induced by PDGF, not only WAVE2 but also WAVE1 is essential for formation of stable lamellipodia during spreading on FN. WAVE1 is required for stabilization of lamellipodial protrusions. WAVE1 and WAVE2 work cooperatively at the spreading edges, resulting in efficient cell spreading.

WAVE1 KO and WAVE2 KO MEFs showed different phenotypes for lamellipodium formation and WAVE1 and WAVE2 can not compensate for each other's deficiencies. We further speculate the function of each WAVE from phenotypes of WAVE KO MEFs. In the case of WAVE2 KO MEFs, lamellipodial actin structure is absent. Also in the other situations (stimulation by growth factors) and cell types (endothelial cells), it was shown that WAVE2 is essential for lamellipodial structure formation (Suetsugu et al. 2003; Yamazaki et al. 2003). Thus, WAVE2 mainly forms membrane protrusive structures when membrane protrudes parallel to a substrate.

In the case of WAVE1 KO MEFs, lamellipodial membrane protrusions develop but are not stabilized by adhesive structures. WAVE1 may function directly or indirectly in the formation of cell-substrate adhesions.

One possibility is that WAVE1 indirectly affects the formation of adhesive structures in the lamellipodium by regulating actin reorganization. Recently, a model concerning the formation of adhesive structures in lamellipodium was proposed (Giannone et al. 2004) (see Introduction). This model is very attractive, but it is unclear how the rearward actin wave is generated. According to this model, the lack of a rearward actin wave in lamellipodia of WAVE1 KO MEFs appears to cause defects in formation of adhesive structures. If WAVE1 is involved in the generation of the rearward actin wave, we propose two possible roles of WAVE1 in the process. One possible role is that in response to lamellipodial contraction, WAVE1 directly creates a new actin structure by inducing actin polymerization at the back of the lamellipodium, which generates the rearward actin wave. During spreading on FN, contact with FN activates Rac and Cdc42 via integrin signaling (Price et al. 1998). Activated integrin signaling by lamellipodial contraction may induce WAVE1-mediated actin reorganization. The other possible role is that WAVE1 influences the highly organized mesh-like structure of actin filaments by modifying the actin framework structure formed by WAVE2. Normal actin structures may be required to produce the rearward actin wave. In cells treated with cytochalasin D, which decreases the concentration of actin filaments in lamellipodia, periodic interruptions of extension of the membrane were rare (Giannone et al. 2004). In WAVE1 KO MEFs with curling spreading edges, the accumulation of actin filaments was not uniform and decreased at the spreading edges. These two possibilities are not exclusive, and WAVE1 may be involved in both processes.

Another possibility is that WAVE1 directly recruits adhesion proteins such as vinculin to sites of cell-substrate adhesion. However, we did not observe localization of WAVE proteins at cell-substrate adhesion sites in MEFs in contrast to Arp2/3 complex. In addition, we did not observe any interaction between WAVE proteins and vinculin (data not shown). On the basis of these findings, we believe that WAVEs are not involved directly in adhesion of the cell membrane to a substrate. However, in a previous study, WAVE1 was shown to be localized at focal adhesions in NIH3T3 cells (Westphal et al. 2000); this discrepancy may be due to the differences in the types of cells used for the experiments.

At the lamellipodial edges, WAVE1 and WAVE2 induce actin polymerization in different directions and the balance of these activities influences the direction and the extension speed of membrane protrusions. When relative activity of WAVE1 increases as compared with that of WAVE2 (WAVE2 KO MEFs), strong localization of WAVE1 at the peripheral area causes upward protrusions of the membrane. In contrast, when relative activity of WAVE2 is high (WAVE1 KO MEFs), membrane extension speed parallel to a substrate increases. Interestingly, some of rescued WAVE2 KO MEFs showed membrane dynamics similar to WAVE1 KO MEFs (Fig. 1J). In these cells, excessive WAVE2 activity may break the balance of actin polymerization.

The difference between the directions of WAVE1- and WAVE2-mediated actin polymerization is thought to be the result of their distinct localization patterns. WAVE1 was shown to localize to the dorsal part of membrane protrusions in dorsal ruffles (Suetsugu et al. 2003). WAVE1 may function at the back of a lamellipodium. Because lamellipodia are thin structures and can be observed only within a single phase, we could not confirm the apical distribution of WAVE1 in lamellipodia (data not shown). Further analysis with immuno-electron microscopy should resolve this problem. In contrast to WAVE1, WAVE2 is clearly localized at the tips of lamellipodial protrusions and therefore induces actin polymerization parallel to the substrate during lamellipodium formation. The mechanism underlying localization of WAVEs is not known. WAVE1 and WAVE2 interact with distinct molecules, and such molecules and interactions may influence localization (Stradal et al. 2004; Vartiainen & Machesky 2004).

In the present study, we observed a novel relation between WAVEs-dependent actin polymerization and cell-substrate adhesion during lamellipodium formation. Formation of cell-substrate adhesions is a critical step in cell migration. Further study of the regulation of WAVEs will bring new insights into our understanding of cell migration.


    Experimental procedures
 Top
 Abstract
 Introduction
 Results
 Discussion
 Experimental procedures
 Supplementary material
 References
 
Cell culture

All cells in this study were maintained in Dulbecco's modified Eagle medium (DMEM) supplemented with 10% foetal calf serum (FCS). WT, WAVE1 KO and WAVE2 KO MEFs were established from embryonic day (E) 9.5 embryos from heterozygous crosses (Suetsugu et al. 2003). E9.5 embryos were incubated in 0.25% trypsin and 0.5 mM EDTA in phosphate-buffered saline (PBS) for 30 min at 37 °C and then dispersed with a micropipette. Cells were cultured in DMEM supplemented with 10% FCS for 3 months and became spontaneously immortalized lines. Experiments were performed with two independently established lines.

Expression of exogeneous WAVEs

Full-length WAVE1- and WAVE2-expression plasmids were constructed in pEF-BOS plasmid vectors (Miki et al. 1998; Suetsugu et al. 1999). Recombinant plasmids and pTK-Hyg, which contains the hygromycin-resistance gene, were co-transfected into MEFs with Lipofectamine 2000 (Invitrogen, Carlsbad, CA, USA) according to the manufacturer's instructions. Single colonies were isolated after 1 month of hygromycin selection (50 µg/mL). Protein expression was confirmed by immunoblotting of cell lysates with appropriate antibodies. Stable rescued cell lines were used in the spreading assays.

Video microscopy

Sub-confluent cells were trypsinized, centrifuged, and dispersed as single-cell suspensions in DMEM supplemented with 10% FCS. Glass-bottomed culture dishes were coated with FN (25 µg/mL; Sigma, St. Louis, MO, USA) for 1 h at room temperature. Single-cell suspensions (50 cells/µL) were plated on FN-coated culture dishes, and observed with phase-contrast microscopy at 2-s intervals.

Phenotypes of WAVE1 KO MEFs in Fig. 1I were classified on the basis of sequential images as follows. Lamellipodia, cells with lamellipodial protrusions across 75% of the cell periphery. Curl up, cells with curling membranes across over (L) or below (S) 10% of the cell periphery. Ruffle, cells with ruffled membranes that did not curl up. Others, other cells.

Phenotypes of WAVE2 KO MEFs in Fig. 1J were classified on the basis of sequential images as follows. Lamellipodia, cells with lamellipodial protrusions (including ruffled membranes) across 75% of the cell periphery. Curl up, cells with curling membranes across over 10% of the cell periphery. Irregular, cells spreading irregularly with finger-like projections. Others, other cells.

For kymography, phase-contrast time-lapse sequences were obtained using IP labs software using 40x objective. Video clips were 10 min long with frames taken every 2 s. Kymographs were produced and analyzed with ImageJ software (the United States National Institutes of Health). For quantitative analysis, kymographs illustrating the lamellipodial activity during 10-min time-lapse videos were made at four places around the edge of the cells. Straight lines were drawn on kymographs before periodic interruptions (in the case of cells with lamellipodia) or curling up (in the case of cells with curling membranes). Slopes of these lines were used to calculate the membrane extension speed. The speed of membrane extension was calculated with each kymograph of 100 s.

Antibodies

Polyclonal anti-WAVE1 and anti-WAVE2 antibodies were prepared as previously described (Yamazaki et al. 2003). Polyclonal anti-Arp2 antibody was generated in rabbits immunized with the CEKGVRVLEKLGVTVR peptide and affinity-purified with CNBr-activated Sepharose 4B (Amersham Pharmacia Biotech, Uppsala, Sweden) according to the manufacturer's instructions. Monoclonal anti-vinculin antibody was purchased from Sigma. Monoclonal anti-actin antibody was from Chemicon (Temecula, CA, USA). Rhodamine- and Alexa 647-conjugated phalloidin were from Molecular Probes (Eugene, OR, USA).

Immunofluorescence microscopy

Sub-confluent cells were trypsinized, centrifuged, and then resuspended as single-cell suspensions in DMEM supplemented with 10% FCS. Coverslips were coated with FN (25 µg/mL) for 1 h at room temperature. Suspended cells (100 cells/µL) were replated on FN-coated coverslips at 37 °C. Every 5 min, cells were fixed with 3.7% formaldehyde in PBS for 10 min. Cells were permeabilized with 0.5% Triton X-100 in PBS for 5 min and then incubated with primary antibodies at 1 : 100 dilution for 1 h. Cells were then incubated for 30 min with secondary antibodies conjugated to Alexa 488 or Alexa 568 (Molecular Probes). Coverslips were mounted on glass slides and observed by confocal microscopy. Intensity profiles in Fig. 4 were produced and analyzed with ImageJ software.

Scanning electron microscopy

Spreading MEFs were fixed with 1% glutaraldehyde in 0.1 M phosphate buffer at pH 7.3. Observation with a scanning electron microscope was performed as previously described (Yamazaki et al. 2003).


    Supplementary material
 Top
 Abstract
 Introduction
 Results
 Discussion
 Experimental procedures
 Supplementary material
 References
 
The following supplementary material is available from:

http://www.blackwellpublishing.com/products/journals/suppmat/GTC/GTC845/GTC845.htm.

Figure S1 Video of spreading WT MEF in Figs 1B and 5A,1. Time series acquired at the interval of 2 s are shown.

Figure S2 Video of WAVE1 KO MEF in Figs 1C and 5B,2. Time series acquired at the interval of 2 s are shown.

Figure S3 Video of WAVE2 KO MEF in Fig. 1F,3 on FN are shown, respectively. Time series acquired at the interval of 2 s are shown.


    Acknowledgements
 
We thank Dr H. Yamaguchi, T. Nakamichi, O. Nakanishi, and S. Kurisu for technical support. This work was supported by grants-in-aid from the Ministry of Education, Culture, Sports, Science, and Technology of Japan and from the Japan Science and Technology Corporation (JST).


    Footnotes
 
Communicated by: Eisuke Nishida

* Correspondence: E-mail: takenawa{at}ims.u-tokyo.ac.jp


    References
 Top
 Abstract
 Introduction
 Results
 Discussion
 Experimental procedures
 Supplementary material
 References
 
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Received: 26 December 2004
Accepted: 17 January 2005




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