- Journal List
- Biophys J
- v.89(2); 2005 Aug
- PMC1366629

# The Physics of Filopodial Protrusion

## Abstract

Filopodium, a spike-like actin protrusion at the leading edge of migrating cells, functions as a sensor of the local environment and has a mechanical role in protrusion. We use modeling to examine mechanics and spatial-temporal dynamics of filopodia. We find that >10 actin filaments have to be bundled to overcome the membrane resistance and that the filopodial length is limited by buckling for 10–30 filaments and by G-actin diffusion for >30 filaments. There is an optimal number of bundled filaments, ∼30, at which the filopodial length can reach a few microns. The model explains characteristic interfilopodial distance of a few microns as a balance of initiation, lateral drift, and merging of the filopodia. The theory suggests that F-actin barbed ends have to be focused and protected from capping (the capping rate has to decrease one order of magnitude) once every hundred seconds per micron of the leading edge to initiate the observed number of filopodia. The model generates testable predictions about how filopodial length, rate of growth, and interfilopodial distance should depend on the number of bundled filaments, membrane resistance, lamellipodial protrusion rate, and G-actin diffusion coefficient.

## INTRODUCTION

The crawling motion of animal cells over a substrate has been described as the succession of protrusion, attachment, and retraction (1). The first step in this sequence, protrusion, is driven by actin polymerization at the leading edge of the cell (2). A common type of protrusive specialization of the leading edge of the cell is the lamellipodium—a flat, leaf-like extension filled with a dense branched network of short (tenths of micron long) actin filaments (Fig. 1). According to the dendritic nucleation model (3), nascent filaments branch from the sides or tips of existing filaments in a sterically precise way. Filaments' barbed ends are oriented forward at roughly ±35° to the direction of protrusion (4). The barbed ends elongate at tenths of micron per second and are capped within seconds. After capping, the filaments lag behind the leading edge and are replaced by the next generation of filaments.

The lamellipodial leading edge is interspersed with filopodia—bundles of actin filaments that are packed tightly together and protrude forward (5,6) (Fig. 1). Similar to the lamellipodial filaments, filopodial filaments are polarized with their barbed ends in the direction of protrusion, but in contrast, they are parallel, long, and turn over very slowly (7) (Fig. 1). Filopodial and lamellipodial protrusions rely on different mechanisms: filament treadmilling (8) and array (9) treadmilling, respectively. They are regulated by different signaling pathways (10,11), yet they are intimately connected, because the filopodial bundles emerge from the lamellipodial network (12,13).

Filopodial protrusions can be “guiding” devices probing space ahead of the lamellipodium. They can also be mechanical devices “penetrating” the environment and serving as a robust scaffold for the lamellipodial protrusion. The role of filopodia as the sensors of the local environment and as sites for adhesion and signaling is well documented (14). In some cells, filopodia are essential for navigation: when filopodia are suppressed, the nerve growth cones can advance but cannot navigate (15). However, fish keratocytes, for example, migrate without filopodia at all (16). It is also worth mentioning that three-dimensional (3D) cell migration through extracellular matrices or engineered scaffolds seems to rely more on the filopodial protrusions in contrast with two-dimensional (2D) cell crawling on flat surfaces (17,18).

There are two major questions about the filopodial protrusion: how is it maintained and how is it initiated? One possibility is that the filopodial filaments are initiated from the cell leading edge by specialized structures (19). Recent evidence, however, points out that the lamellipodial filaments themselves can bend together and “zipper” into parallel bundles of actin filaments (12,20). First, these bundles do not protrude much from the leading edge (such bundles are called Λ-precursors (12) because of their shape). Then, they either mature into the filopodia, or merge with other bundles. To initiate such bundles, the barbed ends have to be locally associated with each other and protected from capping. Protein VASP, elevated in the region of frequent filopodial emergence (12), inhibits capping (21). VASP also transiently binds the barbed ends (22), so association of VASP molecules with each other or some protein cluster could be sufficient to create the tip of the actin bundle. Bundling protein fascin, which is enriched near the tip of the bundle (12), assists VASP and likely other proteins in filopodial initiation. Emerged filopodia have to “outrun” the lamellipodial protrusion, so they have to overcome the membrane resistance, and the G-actin has to be delivered to the filopodial tips.

Available quantitative data (12,23,24) allow theoretical examination of the filopodial mechanics. In the next section, we investigate the restrictions that buckling, membrane resistance, and G-actin diffusion impose on the filopodial dynamics. Then, we find the connection between the spacing between adjacent filopodia and the rates of the filopodial initiation and lateral drift. Finally, we discuss the modeling implications for the biology of filopodial protrusions.

## MECHANICS AND MAINTENANCE OF FILOPODIA

Filopodial protrusions are a few tenths of micron in diameter (25), a few microns in length (7,12,13) (see Discussion for exceptions), and contain 10–30 bundled filaments (12,25) (Fig. 1). The distances between neighboring filopodia are in the micron range. In this article, we explain how these characteristic scales emerge from the physics of the actin bundle. Models' parameters and variables are listed in Tables 1 and and2,2, respectively.

### More than 10 bundled filaments are required for filopodia not to buckle

Membrane bending and tension result in the resistance force at the filopodial tip estimated theoretically as *F* ∼10–20 pN for a membrane cylinder of radius 50–100 nm (26). More detailed recent modeling results in a similar estimate (S. Sun, Johns Hopkins University, personal communication). Experiments with pulling membrane tethers the width and length of which are similar to characteristic filopodial dimensions also give the forces in similar range of 10–50 pN (27,28). Note that in these experiments both membrane bending force and breaking of membrane-cortex links contribute to the resistance, which is likely similar to the resistance to the filopodial protrusion.

Mechanically, the cross-linked filopodial bundle is an effective elastic rod, to which tip the membrane resistance force is applied. The critical force that buckles such rod is equal to:

where *k*_{B}*T* ≈ 4.1 pN nm is the thermal energy (26), *L*_{p} ∼ 10 *μ*m is the F-actin persistence length (29,30), and *L* is the length of the filopodial protrusion. Here *π*^{2}*k*_{B}*TL*_{p}/4*L*^{2} is the buckling force for one filament (31), and *I*(*N*) is the nondimensional factor, which is responsible for the dependence of the bundle stiffness on the number of the bundled filaments, *N*. There are two limiting cases: if the filaments are bundled weakly (for example, the distance between the cross-links along the filaments is large and bundling protein is very flexible), then the filaments buckle independently, and *I*(*N*) = *N*. If, in the opposite limit, the bundling is so frequent and tight that the filaments are effectively “glued” to each other, then the bundle can be considered as a single thick rod. The cross-section area of such rod is equal to the number of the filaments times one filament's cross-section area, and the rod's effective radius is proportional to the square root of the number of the filaments. The stiffness is proportional to the radius in power four (31), so in this case *I*(*N*) ∼ *N*^{2}. Numerical simulations described below suggest that *I*(*N*) ≈ 0.5 × *N*^{2}.

Using Eq. 1, we can estimate the critical length at which the membrane resistance force buckles the filopodial bundle:

We plotted as function of *N* in two limiting cases (*I*(*N*) = *N* and ) in Fig. 2. The plot demonstrates that the weakly cross-linked bundle of 10–30 filaments would buckle at length below 0.5 *μ*m. Strong bundling can support the length in micron range, in agreement with numerous observations.

We used computer simulations to derive the function *I*(*N*) in biologically relevant situation. In the filopodial bundle, the filaments are not packed densely (the cross-section area of the protrusion is ∼0.01 *μ*m^{2}, whereas the total cross-section area of the 25 filopodial filaments is ∼0.001 *μ*m^{2}), so it is likely that each filament is cross-linked with only a few neighbors. We considered variable number (3–15) of elastic rods, 2 *μ*m in length, with the same mechanical characteristics as those of F-actin. The rods were arranged in a parallel stack, and each rod was connected by elastic cross-links to 2–4 nearest neighbors. The bundling protein, fascin, has length between 10 and 15 nm (32), and its stiffness is likely to be similar to that of F-actin (33). We varied both the length of the cross-links from 10 to 50 nm, and their stiffness from 10 times less to 10 times more than that of F-actin. The electron microscopy (EM) data (12) indicate that the interfascin distance along a filament in the filopodia is of the order of tens of nanometers, so we varied the average corresponding distance from 20 to 500 nm. (In the Appendix, we consider a model of fascin distribution along the bundle.)

We used FEMLAB to solve the buckling problem of elasticity theory (the “Structural Mechanics” module solves an eigenvalue problem, such that the lowest eigenvalue corresponds to the buckling force, whereas the corresponding eigenfunction gives the shape of the buckled bundle). The shape of the buckled actin bundle in a sample simulation is shown in Fig. 3 *A*. (Filaments were arranged in parallel in 2D; general principles of the linear elasticity theory suggest that the 3D bundle would buckle at similar forces.) The simulation results showed that if the average distance between the neighboring cross-links along an actin filament in the bundle is of the order of 1 *μ*m, then the stiffness of the bundle scaled as ≈*N* (Fig. 3, *B* and *C*), in agreement with simple physical arguments above. Also in agreement with these qualitative arguments, at small average distance between the neighboring cross-links ≈0.1 *μ*m, the stiffness of the bundle scaled as ≈0.5 × *N*^{2} (Fig. 3, *B* and *C*). We conclude that the observed bundling is tight and in the biologically relevant regime the stiffness of the filopodial bundle increases with the number of the bundled filaments approximately as ≈0.5 × *N*^{2}. The observed number of the filaments can support the bundle of 1–1.5-*μ*m long against buckling (Fig. 2).

*A*) Computed shape of the actin filaments bundled by short elastic links. (

*B*) The computed buckling force (scaled by the buckling force for one 2-

*μ*m-long filament) is plotted as the function of the number of bundled filaments

*N*for the average

**...**

D. Mullins (University of California, San Francisco, personal communication) observed recently that a filopodial bundle of 25 filaments has effective persistence length of 14 mm. This agrees with our simulations, according to which In this observation, bundle grew to be 40-*μ*m long, an order of magnitude greater than predicted by the model. We discuss the difference in the Discussion.

### G-actin diffusion limits the length of thick bundles; membrane resistance limits the length of thin bundles

G-actin diffusion, in addition to the membrane resistance, limits the length of the filopodium. In this article, by G-actin we mean a part of the G-actin pool that can assemble onto the barbed ends (GTP-G-actin not sequestered by thymosin; see Mogilner and Edelstein-Keshet (34)). Let *L*(*t*) be the time-dependent length of the *N*-filament bundle, and *a*(*x*, *t*) be the concentration of the G-actin along the filopodial length (Fig. 4 *A*). The *x* axis is oriented forward, and its origin is at the base of the filopodium at the leading edge (Fig. 4 *A*). In the filopodium, G-actin diffuses and drifts with the cytoplasmic fluid. This drift rate is roughly equal to the rate of the filopodial protrusion *dL*/*dt*, because on the relevant timescale the membrane is impermeable to water (35), and due to incompressibility, the cytoplasm has to fill the filopodium at the rate of protrusion. Equation for the G-actin concentration has the form:

*A*) Results of computer simulations of the 2-D G-actin distribution (

*a*(

*x*,

*t*)) in the filopodium and the small adjacent part of the lamellipodium (distance is in microns; G-actin concentration illustrated with

*shading*is in nondimensional units, see Appendix

**...**

Here *D* is the effective G-actin diffusion coefficient. The boundary condition at the filopodial base (*x* = 0) is that the G-actin concentration there is equal to that at the leading lamellipodial edge, *a*_{0}. (In the Appendix, we examine this assumption by simulating a two-dimensional G-actin distribution (shown in Fig. 4 *A*) in the filopodium and adjacent part of the lamellipodium.) The boundary condition at the filopodial tip (*x* = *L*(*t*)), which is similar to that at the lamellipodial leading edge (34), is that the G-actin diffusive flux there, −*D*(∂*a*/∂*x*)(*L*), is equal to the number of monomers assembling per second onto the tips of *N* filaments. This number is equal to the number of the filaments times the rate of elongation of the filopodial filaments *V*_{f} and divided by the half-monomer size *δ*; *η* is the geometric coefficient converting the number of monomers into micromolar units (see the Appendix). The drift part of the G-actin flux is not included into the boundary condition, because the filopodial tip and the cytoplasm move together.

The rate of the filopodial extension, *dL*/*dt*, is equal to the difference between the rates of the filopodial filaments' elongation *V*_{f} and of the lamellipodial filaments' extension in the direction of protrusion, *V*_{l}: *dL*/*dt* = *V*_{f} − *V*_{l}. Neglecting small rate of filaments' disassembly, *V*_{f} ≈ *k*_{on}*δa*(*L*) exp(−*Fδ*/*k*_{B}*TN*) (34). Here *V*_{0} = *k*_{on}*δa*(*L*) is the free polymerization rate proportional to the G-actin concentration at the filopodial tip (*k*_{on} is the assembly rate); *F*/*N* is the membrane resistance load force per filament. The exponential factor is responsible for slowing the protrusion rate by the membrane resistance (34). It is convenient to introduce the effective number of filaments that can support the filopodial protrusion, *N*_{0} = *Fδ*/*k*_{B}*T* ≈ 13, then *V*_{f} ≈ *k*_{on}*δa*(*L*) exp(−*N*_{0}/*N*).

In the lamellipodium, the leading edge filaments are distributed over a wide range of angles (4). Those elongating at acute angles to the direction of protrusion grow slower, than those elongating at greater angles, simply because the filaments' elongation rate is the increasing function of the angle, *V*_{elong} = *V*_{l}/ cos *θ*, where *V*_{l} is the same for all filaments (Fig. 4 *A*). This means that slower growing filaments at small angles are generating disproportionately large force, whereas the filaments at greater angles are “free-loaders” growing faster against smaller force. This also means that a large “critical angle” *θ*_{c} exists, such that filaments growing at this angle elongate against zero force at free polymerization rate *V*_{0} = *k*_{on}*δa*_{0}, whereas filaments growing at even greater angles simply cannot keep up with the leading edge and lag behind it (36,24). Then, *V*_{l} = *k*_{on}*δa*_{0} cos *θ*_{c}, and

Equations 3 and 4 together represent a difficult free boundary problem. Fortunately, the timescale separation (G-actin diffusion is much faster than the filopodial growth and cytoplasmic drift) allows approximate analytical solution of the problem, which is sketched in the Appendix. The result is that the G-actin concentration decreases linearly from the base to the tip of the filopodium (Fig. 4 *A*), so that the concentration gradient is the function of the filopodial length:

This gradient induces the G-actin flux, which is “consumed” at the tip and makes it grow, but the longer the filopodium becomes, the smaller is the G-actin concentration at the tip, and the slower is the rate of growth. Solution of Eqs. 3 and 4 (see the Appendix) is plotted in Fig. 4 *B* for *N* = 20, *θ*_{c} = 80°. It has the following asymptotics:

Thus, for the first few seconds, when the filopodium is short, the G-actin concentration at its tip is almost equal to that at the lamellipodial leading edge, and the filopodial filaments grow in the direction of protrusion much faster than tilted lamellipodial filaments. Then, the G-actin concentration decreases, and the filopodial growth slows down exponentially at great (over micron) lengths. The maximal length of the filopodium, when its elongation slows down to match the lamellipodial expansion rate, is given by the formula:

In Fig. 4 *C*, we plotted the stationary filopodial length *L*_{max} as a function of *N* at three different values of the critical angle, *θ*_{c} = 60°, 75°, 80°. The data (4) indicate that the critical angle in rapidly moving cells is likely to be not <60°.

The greater the critical angle is, the slower the lamellipodial protrusion, and the farther the filopodium can extend (Fig. 4 *C*). This is in agreement with the observation that in the rapidly and steadily moving keratocyte cells the filopodia are absent (16). Another prediction is that the filopodial length is linearly proportional to the G-actin diffusion coefficient.

Dependence of the filopodial length on the number of the bundled filaments is biphasic. At great *N*, the factor exp(*N*_{0}/*N*) ≈ 1 (many filaments easily overcome the membrane resistance), and the length is inversely proportional to the filament number, because many growing filament tips deplete the actin monomeric pool. When *N* is small, the exponential factor exp(*N*_{0}/*N*) increases rapidly, and the filopodial length dramatically decreases. In fact, if the filament number is less than:

the bundle cannot protrude at all. These results are similar to effects of the membrane resistance and G-actin diffusion in lamellipodial protrusion (35,34).

Note that we made the estimates assuming that the filaments are not moving relative to the substratum. In fact, the model is also valid in the presence of retrograde flow of actin, which is almost always the case (37). Indeed, let *V*_{e} be the elongation rate of the lamellipodial filaments in the direction of protrusion, and *V*_{r} be the rate of lamellipodial network's retrograde movement. Then, the lamellipodial extension rate would be *V*_{e} = *V*_{l} − *V*_{r}. The filopodial bundles are embedded into the lamellipodial network and move rearward with the same rate (7,24), so the rate of the filopodial extension is *V*_{f} − *V*_{r}, where *V*_{f} is the rate of growth of the filopodial filaments. Then, the filopodial length changes with the rate (*V*_{l} − *V*_{r}) − (*V*_{f} − *V*_{r}), same as in Eq. 4. The G-actin diffusion and drift are unaffected by the retrograde flow. Note also, that our theory is not applicable to the acrosomal protrusion of Thyone (38,39), where the physics and biology is different, and length, rate of extension, and actin concentration are many times greater. Finally, there is a possibility that filopodial tip complex proteins, such as formins, change the polymerization kinetics, in which case the estimates would change.

### Length of 10–30-filament bundle is limited by buckling; length of >30-filament bundle is limited by G-actin diffusion

Equations 2 and 8 give the maximal attainable filopodial lengths limited by buckling and diffusion, respectively, as functions of the number of the bundled filaments. The resulting observed length is the minimum of these two lengths, if at given *N* the filopodium buckles at shorter length than that allowed by diffusion, then the growth would be stopped by buckling, and vice versa. We plotted the function *L*_{max}(*N*) in Fig. 5 *A*. Our model predicts that >7–8 bundled filaments can maintain the filopodial protrusion. When the filament number is <10, the membrane resistance limits the filopodial length to submicron range. The length of the bundle of 10–30 filaments is limited by buckling, and is proportional to the filament number. The length of the optimal, 30-filament bundle, reaches 1.5 *μ*m. The length of the thicker bundle decreases inversely proportionally to the filament number, because more filament tips deplete G-actin.

*A*) Predicted filopodial length limited by the membrane resistance, buckling, and G-actin diffusion as a function of the number of bundled filaments (

*θ*

_{c}= 80°). (

*B*) Length distribution for 26 filopodial protrusions gleaned from

**...**

Quantitative observations reported in Argiro et al. (23) partially corroborate our theoretical findings. The maximal length of the observed filopodia was 2–10 *μ*m, which is greater, but the same order of magnitude as predicted. In the Discussion, we speculate on the factors that can explain the difference. The observed rate of the filopodial extension, ≈0.12 *μ*m/s, in agreement with Eq. 6, was maximal just after filopodial initiation and declined thereafter, similar to the predicted time series in Fig. 4 *B*. The growth did not end with asymptotic slowing down, rather, the filopodia collapsed pivoting or buckling when the maximal length was reached. The initial rate of extension directly correlated with the eventual length of the filopodium (23). This is explained by Eq. 6: greater *N* means faster initial extension rate (more filaments are less affected by the membrane resistance), and also greater final length when the bundle buckles. Interesting model prediction is that for thicker bundles, length of which is limited by the diffusion, the initial extension rate should be correlated negatively with the final filopodial length. Also, we measured the lengths of 26 adjacent filopodial protrusions in Fig. 2 of Oldenbourg et al. (24) (plotted in Fig. 5 *B*). Most of the filopodia observed have lengths of 2 *μ*m, in agreement with our estimates.

## BALANCE OF LATERAL DRIFT AND EMERGENCE RATE OF Λ-PRECURSORS REGULATES INTERFILOPODIAL SPACING

The data on molecular mechanisms are too sketchy to attempt detailed quantitative modeling of the filopodial initiation. Here we address the easier question of spacing of the filopodial protrusions along the lamellipodial leading edge. In the next section we also discuss the implications of the estimates that we derive below for the “convergence-elongation” model (12) of the actin bundle initiation. In the Appendix, we consider a simple model that explains fascin-mediated bundling near the tip of the bundle.

Growing lamellipodial barbed end tilted at angle *θ* relative to the direction of protrusion drifts with velocity *V*_{l} tan *θ* relative to the leading edge protruding with the rate *V*_{l} (8) (Figs. 4 *A* and 6 *A*). Convergence, “zippering”, and elongation of a few such lamellipodial filaments would produce an actin bundle, either remaining embedded into the lamellipodium, or making filopodial protrusion (Fig. 6 *A*). Such bundle would be also tilted at some smaller angle and undergo the lateral drift (24). When two such bundles “collide” at the leading edge, their filaments align with each other and the bundles merge (12). As a result, the number of the bundles decreases. Here we show that the interfilopodial spacing can be explained by the balance between the bundle initiation and merging caused by the lateral drift. We neglect simple disappearance of filipodia, because filaments in a filopodium are stable for >1000 s (11).

*A*) Illustration of the lateral drift. Dashed lines represent the lamellipodial leading edge at four consecutive moments of time. Barbed ends of the individual filaments and the Λ-precursor change their position along the leading edge as the edge

**...**

We investigate the spacing between filopodia using first a continuous deterministic model that reveals important biological scales, and then performing realistic stochastic simulations. In the continuous model, we introduce densities (numbers per micron) of Λ-precursors, *λ*(*x*, *t*), and of filopodial protrusions, *f*(*x*, *t*), along the lamellipodial leading edge. These densities change according to the following dynamics:

(Fig. 6 *A*). Here *b* is the rate of initiation of Λ-precursors (bundling), and *m* is the rate of “maturation” of the Λ-precursors into the filopodial protrusions; *r*_{1} is the effective rate of “collision” of the Λ-precursors, as a result of which two colliding Λ-precursors merge into one filopodial protrusion due to the increase of the number of filaments in the merged bundle; *r*_{2} is the effective rate of “collision” of a Λ-precursor with a filopodial protrusion, as a result of which the Λ-precursor disappears merging with the filopodial protrusion. Finally, *r*_{3} is the effective rate of “collision” of two filopodia that merge into one. This simple model can be made more sophisticated by making the number of filaments in actin bundles the independent model variable and assuming some rules of when merging of Λ-precursors results in a thicker Λ-precursor, and when it results in a filopodial protrusion depending on the numbers of bundled filaments. However, this does not change qualitatively simple results derived below.

Order of magnitude of the rate *r*_{1} can be estimated as average inverse time before collision of two Λ-precursors, which is equal to the average distance between the precursors, 1/*λ*, divided by the average rate of the lateral drift, *v*_{d}: *r*_{1} ≈ *v*_{d}*λ*. Similarly, *r*_{2} ≈ *v*_{d}*f*, *r*_{3} ≈ *v*_{d}*f*. Thus, we obtain the system of equations (in the mean field approximation neglecting correlations between filopodia) for the actin bundle densities:

These equations can be nondimensionalized by scaling the densities using the balance between the bundling rate and merging rate: *v*_{d}*λ*^{2} ∼ *b*, so the density scale is Timescale is equal to the characteristic life time of an individual *λ*-precursor before it merges with another, Equations for nondimensional variables have the form:

Here is the dimensionless ratio of the maturation rate to the effective rate of merging of actin bundles.

Phase plane analysis of nonlinear Eq. 11 shows that there is a unique stable biologically relevant stationary solution. It can be found analytically in two limits. First, when the maturation rate is very slow, the average precursor and filopodial densities are almost equal: On the other hand, when the *λ*-precursors mature fast, the *λ*-precursors density is low, *λ*′ ≈ 1/*ε*, while *f*′ ≈ 1. For intermediate values of *ε*, *f*′ ∼ 1. The important conclusion is that the order of magnitude of the stationary filopodial density is (in dimensional variables).

We measured the distances between 26 adjacent filopodia in Fig. 2 of Oldenbourg et al. (24) and plotted the results in Fig. 6 *B*. The average interfilopodial distance is ∼2 *μ*m, and *f* ∼ 0.5/*μ*m. The average angle at which the actin bundles are tilted relative to the direction of protrusion is <30°, and the average lateral drift rate is a few fold less than the rate of protrusion, *v*_{d} ∼ 0.01*μ*m/s. We can estimate the rate of emergence of the Λ-precursors as *b* ∼ *v*_{d}f^{2} ∼ 0.001–0.01 *μ*m^{−1}s^{−1}. Thus, a new Λ-precursor has to appear once every few hundreds of seconds per micron of the leading edge. There are no measurements of this rate available, but this estimate seems to compare well with observations reported in Svitkina et al. (12).

Also, the micrographs in Svitkina et al. (12) indicate that the densities of Λ-precursors and filopodial protrusions are comparable, so, according to our analysis, the rate of precursors' maturation cannot be faster than s. In other words, on the average, individual Λ-precursors can be observed for ∼100 s before merging or maturing into a filopodium.

This analysis is supported by the following stochastic simulations, which are essential because of the dispersal of the actin bundles' orientations, correlations between the bundles and large fluctuations of the bundles' number. Each actin bundle (either Λ-precursor, or filopodium) is characterized by its position along the lamellipodial leading edge, *x*_{i}(*t*), rate of lateral movement, *v*_{i}(*t*), and maturity index, *m*_{i}, equal to zero for a precursor and to unity for a filopodium. We consider a 30-*μ*m-long segment of the leading edge (Fig. 6 *C*) and generate new precursors on it at random location with the rate *b* = 0.01 *μ*m^{−1}s^{−1}. Each nascent precursor is tilted to the protrusion direction at a random angle uniformly distributed in the interval −30° < *θ*_{i} < 30°, and *v*_{i}(*t*) = *v* × tan(*θ*_{i}), where *v* = 0.05 *μ*m/s is the protrusion rate. The precursors mature (*m*_{i} switches from 0 to 1) into the filopodia with the constant rate *m* = 0.01/s. The trajectories of the precursors (*light gray*) and filopodia (*dark gray*) from a sample simulation are shown in Fig. 6 *C*, where time in seconds is shown on the *y* axis. In the simulations, we update the positions of the tips of the precursors and bases of the filopodia along the leading edge each time step (5 s). Actin bundles that run into the edges of the segment “disappear”.

We consider “collision events” of pairs of the actin bundle, when the distance between them is smaller than 30 nm. Each collision results in the merger of the pair. When two precursors collide, the resulting actin bundle becomes another precursor, or changes into a filopodium with equal probability. (Numerical experiments show that assigning weighed probabilities does not change the results qualitatively.) When either a precursor collides with a filopodium, or two filopodia collide, a single filopodium results. The lateral movement rate of the resulting bundle is equal to that of one of the colliding pair having minimal absolute value, if either two precursors, or two filopodia collide. If a precursor and a filopodium collide, then the lateral movement rates of “mother” and “daughter” filopodia are the same.

Repeating simulations like those shown in Fig. 6 *C*, we plotted the histogram of the interfilopodial distances (Fig. 6 *D*). We chose the rate of initiation of Λ-precursors so that the observed and calculated mean interfilopodial distances are the same order of magnitude. Simulations demonstrate that the observed and calculated variances of these distances are also similar (Fig. 6, *B* and *D*). We also tested numerically the predicted dependence of the analytical model. The stochastic simulations confirm that the density of filopodia along the leading edge is proportional to the square root of the rate of initiation of Λ-precursors and inversely proportional to the square root of the drift rate (Fig. 6, *E* and *F*).

## DISCUSSION

### Filopodial length

Estimates in this article show that to overcome the membrane resistance, >10 actin filaments have to be bundled in filopodia. The length of the filopodial bundle of 10–25 filaments is limited to 1–2 *μ*m due to buckling of the bundle by the membrane resistance force. Thicker bundles are stronger, but growth of >30 filaments bundled together is limited by G-actin diffusion: more barbed ends consume so many monomers that diffusion cannot maintain bundles longer than 2 *μ*m. This analysis explains the observed number (tens) of actin filaments in filopodia and their length (microns): in fibroblasts, macrophages, and nerve growth cones the filopodial length rarely exceeds 10 *μ*m. Our findings can also explain the experimental observations (23) of the rate of the filopodial growth of the order of 0.1 *μ*m/s and its correlation with the final filopodial length.

However, filopodia sometimes grow longer: in sea urchin embryo, where filopodia were first seen live in 1961 (40), they were 5–35-*μ*m long. R. D. Mullins (University of California, San Francisco, personal communication cited above) observed recently the filopodial bundle 40-*μ*m long. Also, some observations indicate that the rate of filopodial elongation does not slow down with filopodial length as fast as predicted by our theory (7). These discrepancies point out that simple G-actin diffusion and linear elastic stability of the cross-linked filament bundle cannot fully explain the observed filopodial behavior. Thus, perhaps the most valuable lesson from our model is that additional mechanisms have to be at work in filopodia.

There are few possible explanations for these discrepancies between theory and experiment. First, decreasing membrane resistance by two orders of magnitude increases the filopodial length limited by buckling by one order of magnitude, from a few microns to a few tens of microns (buckling length is proportional to the square root of the force). This can be accomplished by regulation of the membrane tension (41). Second, adhesion of the filopodia to the substratum, which we did not consider, can strengthen the filopodia significantly: long filopodia adheres to the surface, whereas filopodia without adhesions bends laterally (13). Third, as far as the diffusion-limited growth is concerned, our estimates were made for the steadily protruding lamellipodial leading edge. In fact, this protrusion in most cells consists of irregular cycles of protrusion and retraction (21). Filopodial growth can continue past the micron range, with slowing speed, if the lamellipodial leading edge is stalled. Finally, other means of transport not considered here, for example those mediated by unconventional myosin motors (42), can contribute to filopodial elongation. Indeed, there are indications that unconventional myosin motors are responsible for transport of adhesion molecules (14) and of Mena/VASP proteins (43).

### Note about protrusion force generation

The polymerization ratchet mechanism of force generation (44) requires frequent bending of either filament tips, or membrane, or both, so that the transient gap between the filaments' tips and membrane is >*δ* ≈ 2.7 nm. Unlike the tilted lamellipodial filaments, the filopodial filaments are perpendicular to the resisting membrane, and the transient gap due to their thermal bending is smaller. Its magnitude can be estimated as the shortening of the end-to-end distance for elastic rod of length *l*_{c} and persistence length *L*_{p} due to the thermal bending: (45). For actin, *L*_{p} ∼ 10 *μ*m, and *l*_{c} ∼ 20–30 nm is of the order of the average distance between the fascin cross-links. The value of *δ*_{1} is <1 nm at these parameters, so filament bending is not sufficient. However, the membrane bending is sufficient: in Mogilner and Oster (44) we derived the formula: for the corresponding gap. Substituting the values of the membrane bending modulus, *B* ∼ 50 *k*_{B}*T*, the membrane resistance force, *F* ∼ 20 pN, and the area of the filopodial tip, *A* ∼ 0.01 *μ*m^{2} we estimate the corresponding gap as ∼10 nm.

More thorough stochastic simulations taking into account detailed membrane dynamics and polymerization kinetics confirm this conclusion (S. Sun, Johns Hopkins University, personal communication). However, future modeling is needed because the filopodial tip is loaded with proteins and its mechanical properties are unknown. Also, abundance of VASP at the tip could lead to frequent attachment of the filaments to the membrane (46). It is possible that other models of force generation based on complex mechanochemical cycles of barbed ends associated with auxiliary proteins are relevant for the filopodial protrusion (47,48). If this is the case, then the exact values for the generated polymerization force and G-actin kinetics rates at the filopodial tip would change, but their orders of magnitude would not, so the order of magnitude estimates in this article would remain valid.

### Model implications for molecular mechanisms of filopodia initiation

The model explains the characteristic distance between adjacent filopodia in micron range as the balance of initiation and lateral drift and merging of the actin bundles. The theory suggests that F-actin barbed ends have to be locally focused and protected from capping approximately once every hundred seconds per micron of the lamellipodial leading edge to initiate the observed number of filopodia.

From the EM data reported in Svitkina et al. (12) we can glean ∼100 barbed ends per micron of the leading edge (this estimate compares well with 250 ends per micron reported in (49)). At protrusion rate *v* = 0.05 *μ*m/s and average angle between filament growth and leading edge protrusion *θ* = 35°, the average lateral drift rate is *v* × tan(*θ*) ≈ 0.035 *μ*m/s, so barbed ends tilted to the right/left converge at the rate 0.07 *μ*m/s. Total height of the lamellipod is ∼0.2 *μ*m (49), so each filament (which is ∼0.005 *μ*m in diameter) would, on the average, “collide” due to the lateral drift with another filament at the rate (∼50 filaments/*μ*m) × (0.07 *μ*m/s) × (0.005 / 0.2 *μ*m) ∼ 0.1/s. Filaments are tenths of microns long, so the capping rate at the leading edge is of the order of 0.1/s, so there is a significant probability that any growing filament would “collide” with an oppositely tilted filament. If the barbed ends of such pair of filaments are kept together either by a dynamic cross-linker that stays close to the growing filament tips, or by a “processive capper”, such as formin (50), which in turn is associated with a nascent “filopodial tip complex” (reviewed in Small et al. (51)), then the filaments would bend into parallel configuration and start to grow almost in the direction of protrusion. The corresponding bending force is in subpiconewton range and can be easily generated by the polymerization ratchet mechanism (44,50).

Other filament tips would collide with the pair and could be trapped in the growing bundle creating a nascent Λ-precursor. In order for this precursor to assemble a bundle of ∼10 filaments, the effective capping rate in the vicinity of the precursor tip has to decrease to ∼0.01/s. Indeed, the average stationary number of the growing tips in the bundle can be estimated as the ratio of the rate of collisions of the bundle with lamellipodial barbed ends, ∼0.1/s, to the capping rate, so the latter can be estimated as ∼(0.1/s) / 10 = 0.01/s. It would take ∼10 / (0.1/s) = 100 s to assemble the actin bundle.

Such a low capping rate cannot be maintained along the whole leading edge, because the filaments would grow a few microns long and buckle (21). Therefore, our estimates suggest that once every hundred seconds per micron of the lamellipodial leading edge, a nascent filopodial tip complex (or part of it) self-assembles, such that its components both associate with the filament tips physically, and protect them from capping. Then, in hundred seconds, a Λ-precursor develops and matures into a filopodium or merges with other actin bundles. Likely, some positive feedbacks are involved in this process. For example, transient changes in membrane curvature have been shown to cause filopodia perhaps by activating pathways that trigger actin polymerization (52), and in turn concentration of filaments in actin bundles curves the membrane locally. It is premature to speculate about specific pathways of the filopodial initiation. The value of our model is that it predicts the rate of filopodial precursors initiation and the local capping rate posing quantitative constraints for future models.

### Model predictions

The model generates the following testable predictions:

- There is an “optimal” filament number at which the maximal filopodial length is achieved.
- Decreasing membrane stiffness would lead to increasing of the filopodial lengths for actin bundles with small filament numbers (the length of which is limited by the membrane resistance), whereas the length of thicker filament bundles (the length of which is limited by the G-actin diffusion) would not change.
- Faster lamellipodial protrusion correlates with shorter average filopodial lengths.
- Faster lamellipodial protrusion correlates with greater average distance between adjacent filopodia.
- Initial growth rate of thin (thick) filopodial bundles is an increasing (decreasing) function of the filament number and correlates positively (negatively) with the final filopodial length.

From the physical point of view, it is tempting to compare the filopodial and lamellipodial protrusions. In terms of G-actin “consumption”, the lamellipodial filaments (hundreds per micron of the leading edge (49)) deplete G-actin pool equally with the filopodial bundle (tens of filaments per one-tenth of micron of the leading edge). On smooth surfaces, lamellipodial organization of actin filaments is optimal for the elastic polymerization ratchet mechanism of protrusion force generation, because in the lamellipodium the filaments are cross-linked neither too heavily, nor too lightly, so they do not buckle, yet are flexible enough (46). However, filopodial protrusions would be more efficient for crawling through extracellular matrix and on surfaces of other cells. Another possible role of relatively rigid actin bundles embedded into the lamellipodial actin sheet is to strengthen the lamellipodium against buckling, by analogy with engineered macroscopic structures (53). Future modeling efforts can help to elucidate other filopodial important functions, such as being guides for microtubules (54).

## Acknowledgments

We are grateful to G. G. Borisy, T. Schaus, R. Cheney, T. Switkina, and K. Tosney for fruitful discussions, and to R. D. Mullins, G. G. Borisy, and S. Sun for sharing unpublished data.

The work is supported by National Institutes of Health GLUE grant “Cell Migration Consortium” (NIGMS U54 GM64346) and National Science Foundation grant DMS-0315782.

## APPENDIX I: ANALYSIS OF THE G-ACTIN DIFFUSION AND THE GROWTH OF THE FILOPODIUM

The factor *η* [*μ*M^{−1}*μ*m^{−1}] converts *μ*M concentration units into the number of molecules per unit length of the filopodium, given that the filopodial radius is ∼0.1 *μ*m. As noted above, most of the volume inside the filopodium is free for the monomers to diffuse in. A concentration of 1 *μ*M corresponds to molecules per *μ*m^{3}, and this figure corresponds to *π* × (0.1 *μ*m)^{2} × 600/*μ*m molecules per 1 *μ*m of the filopodium. Thus, .

The following scales are characteristic for the filopodial protrusion: *a*_{0} ≈ 10 *μ*M for the G-actin concentration, for the lamellipodial length, and s for time. Rescaling Eqs. 3 and 4, we obtain the nondimensionalized equations for variables (we keep the same notations for the rescaled variables):

Here On the relevant scale, the G-actin diffusion is much faster than the cytoplasmic drift and filopodial growth, and the left-hand side and the second term on the right-hand side in Eq. 12 can be neglected: over seconds, the diffusion establishes a quasistationary gradient of the G-actin concentration, which slowly follows changes of the filopodial length over tens of seconds. So, and using the boundary conditions, we obtain: *a*(*x*, *t*) ≈ 1 − *α*(*L*(*t*))*x*, where *α* ≈ 1/(1 + *L*(*t*)). Corresponding dimensional formula is Eq. 5. Substituting these expressions into Eq. 13 gives:

Integrating this first order ordinary differential equation (*L*(0) = 0), we find the solution implicitly:

This formula can be used to plot the solution numerically (Fig. 4 *B*) and to find the asymptotic behavior of the filopodial length:

## APPENDIX II: G-ACTIN GRADIENT IN THE FILOPODIUM “SEAMLESSLY” MATCHES THAT IN THE LAMELLIPODIUM

The boundary condition *a*(0) = *a*_{0} for the G-actin concentration at the base of the filopodium (Fig. 4 *A*), where *a*_{0} is the concentration at the lamellipodial leading edge, is nontrivial, because the “consumption” of the G-actin at the filopodial tip and corresponding diffusive flux can, in principle, locally deplete the G-actin concentration at the leading edge. To examine this boundary condition, we used FEMLAB to solve the following 2D (the lamellipodium is flat) diffusion problem. We considered the 0.1-*μ*m-wide and 1-*μ*m-long filopodium and 1-*μ*m-wide and 0.8-*μ*m-long adjacent part of the lamellipodium (Fig. 4 *A*). We solved the G-actin diffusion equation on this combined domain using the parameters described above and the following boundary conditions: i), the G-actin concentration at the “back” of the lamellipodial part of the domain is 1.2 (in the units of *a*_{0}); ii), the G-actin concentration at the “front” of the lamellipodial part of the domain is 1; iii), the G-actin flux at the tip of the filopodial part of the domain is given by Eq. 12; iv), the G-actin flux at the sides of both lamellipodial and filopodial parts of the domain is zero. Conditions i and ii are chosen so that the G-actin flux at the lamellipodial leading edge matches the “consumption” of the G-actin at the edge at characteristic protrusion rate and F-actin density at the edge (34). The stationary solution of this diffusion problem illustrated with shading in Fig. 4 *A* shows that the G-actin gradients at the lamellipodium and filopodium “seamlessly” match each other, and that the G-actin concentration at the base of the filopodium is, indeed, *a*_{0}. This is the consequence of the fact that the characteristic number of the filopodial filaments per filopodial size, ∼20/0.1 *μ*m, is the same as the characteristic number of the lamellipodial filaments per leading edge length, ∼200/1 *μ*m (49), so the filopodium “consumes” proportional share of G-actin and does not deplete the lamellipodial G-actin pool.

## APPENDIX III: DYNAMIC MODEL OF FASCIN DISTRIBUTION IN THE FILOPODIUM

The bundling protein fascin is turned on and off by regulated phosphorylation (32). It is likely that this regulation takes place at the filopodial tip complex (G. G. Borisy, Northwestern University, personal communication). This suggests the following model that explains the observed increased fascin presence near the tips of actin bundles. Let us consider the (*L* = 2 *μ*m)-long filopodium, place the *x* axis directed backward with the origin at the tip, and consider the linear densities of fascin bound to the actin filaments, *f*_{b}(*x*, *t*), diffusing “inactive” fascin dissociated from the actin filaments, *f*_{i}(*x*, *t*), and diffusing “active” fascin dissociated from the actin filaments, *f*_{a}(*x*, *t*). The dynamics of fascin is described by the following system of equations:

The first term in the right-hand side of Eq. 14 is responsible for the kinematic drift of the bound fascin with the protrusion rate *v*, due to treadmilling together with F-actin, away from the filopodial tip. The first terms in the right-hand side of Eqs. 15 and 16 describes the fascin diffusion. We use the value of the diffusion coefficient *D*_{f} = 2 *μ*m^{2}/s, scaled proportionally to length from the known value of the G-actin diffusivity. The second terms in the right-hand side of Eqs. 14 and 15 describe the inactivation and dissociation of fascin from F-actin with the rate *k*_{1}. The second term in the right-hand side of Eq. 16 and the third term in the right-hand side of Eq. 14 are responsible for association of activated fascin with F-actin with the rate *k*_{2}. We use the values *k*_{1} = *k*_{2} = 1/s, which are characteristic for the kinetics of actin-binding proteins (33). Equation 17 gives the boundary conditions: due to the drift, there is no bound fascin at the tip, *f*_{b}(0) = 0. All inactivated fascin is activated at the tip, so *f*_{i}(0) = 0, and the fluxes of the inactivated and activated fascin balance (last formula in Eq. 17). We assume that at the base of the filopodium there is no activated fascin (like in the lamellipodium), and the concentration of the inactivated fascin is equal to that in the lamellipodium, *f*_{0}.

We used FEMLAB to solve Eqs. 14–17. The solutions are plotted in Fig. 7. The model predicts that the bundling fascin concentration is maximal at approximately 300 nm from the filopodial tip, much closer to the tip, than to the base of the filopodium. Near the base, the cross-linking density decreases. This is unlikely to affect the buckling force. Finally, we repeated the simulations for the Λ-precursor (allowing the diffusion to be two-dimensional). The corresponding bound fascin density is shown with the dotted curve in Fig. 7. Again, the fascin density is maximal near the bundle's tip.

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**The Biophysical Society**

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