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Cytosolic pressure provides a propulsive force comparable to actin polymerization during lamellipod protrusion

Does cytosolic pressure facilitate f-actin polymerization to push the leading edge of a cell forward during self-propelled motion? AFM force-distance (f-d) curves obtained from lamellipodia of live cells often exhibit a signal from which the tension, bending modulus, elastic modulus and thickness in the membrane-cortex complex can be estimated close to the contact point. These measurements permit an estimate of the cytosolic pressure via the canonical Laplace force balance. The deeper portion of the f-d curve allows estimation of the bulk modulus of the cytoskeleton after removal of the bottom effect artifact. These estimates of tension, pressure, cortex thickness and elastic moduli imply that cytosolic pressure both pushes the membrane forward and compresses the actin cortex rearward to facilitate f-actin polymerization. We also estimate that cytosolic pressure fluctuations, most likely induced by myosin, provide a propulsive force comparable to that provided by f-actin polymerization in a lamellipod.

The canonical view in cell mechanics is that an f-actin polymerization force pushes against the leading edge membrane of a lamellipod and causes protrusion 1 . The theoretical basis for the polymerization force is due to Hill & Kirschner 2 , who predicted that actin or microtubules could either push or pull against a load depending on whether the local monomer concentration is greater or less than a critical concentration, a quantity that is unknown and may not apply inside a cell because of capping and monomer sequestration. In any case, it is difficult to separate cytoplasmic pressure from polymerization as the origin of the pushing force since both types of pushing forces can coexist. While the actin polymerization force has been directly measured outside of a cell 3 , until recently there have been no such measurements inside a cell 4 . Farrell et al. 5 recently reported an assay that involved pulling actin-filled tethers with an optical trap and interpreted the data using the Hill formalism. A conceptual difficulty with f-actin pushing the membrane is that it must detach from the cell membrane to enable a g-actin monomer to intercalate. A way around the difficulty has been to argue that statistical fluctuations in either the membrane position or the f-actin location will permit intercalation. These are the two forms of the Brownian ratchet mechanism 6,7 . However, there is a growing body of evidence that f-actin may not be in full contact with the leading edge and protrusion still occurs. For example, rapidly assembling f-actin dynamics occurs throughout a domain that is hundreds of nanometers wide as measured by qFSM 8 . Since polymerization can only occur at the end of an f-actin filament, filament ends should also be distributed over a domain that is hundreds of nanometers wide. If a filament end is not in contact with the leading edge, then it cannot exert a pushing force. Instead cytosolic pressure must do the pushing. Indeed a reduced number filament ends near the membrane was measured using cryo-EM 9 . Furthermore a rearward shift away from the membrane of a dorsal layer of f-actin was seen using dual-objective STORM 10 , which further reduces the number of f-actin ends in contact with the membrane. We also mention the absence of f-actin in contact with the membrane during bleb formation where it is clear that cytosolic pressure is dominant 11 . In what follows, we will analyse our data keeping in mind the model lamellipod having a ventral and dorsal cortical layer separated by a gap shown in Fig. 1, which is suggested by the images obtained by dual-objective STORM 10 .

Results
Indentation of the membrane/actin cortex by a paraboloid. The dorsal cell surface is assumed to be a flat horizontal surface indented by the AFM cantilever whose tip has the local shape of a paraboloid, as shown in Fig. 2. The paraboloid shape is used as the simplest model of an axisymmetric shape with finite radius of curvature R. We assume that both tension and bending curvature elastically resist the probe tip. The contact mechanics is therefore governed by the membrane-plate equation where D (N-m) is the bending modulus, γ (N/m) is the tension, and w is the vertical displacement induced by the probe. It is easy to show that this contact problem can be reduced to the superposition of two previously solved problems: the indentation of an elastic half-space by a cone 12 and the indentation of an elastic half-space by a flat-ended circular cylinder 13 . The mechanics problem is to determine the force F required to indent a membrane having tension γ (N/m) and bending modulus D (N-m) when the indentation distance is δ. The radial distribution of contact pressure p(r) and the contact radius a are auxiliary unknowns. The paraboloid δ ( ) = − + /( ) z r r R 2 2 describes the shape of the tip in contact with the membrane as a function of the radial distance r when it is at distance δ lower than the upper cell surface before indentation. The same shape can be calculated as a result from a distribution of point forces acting over the contact area πa 2 , resulting from an unknown pressure distribution p(ρ). The resulting integral equation for the pressure-resulting indentation is The log term is the axisymmetric point force solution of the plate-membrane equation, which governs the transverse displacement. We differentiate equation (2) with respect to r to obtain  The right-hand side can be viewed as the superposition of the indentation by two shapes: a cone having a half-opening angle of π/4 (the − δ + r term) plus the pulling upward by a flat-ended cylinder (the δ term). The term ρ / − r 1 is the Green's function for an elastic half-space. The pressure distribution is known for the cone and flat-ended cylinder problems in terms of the modulus of elasticity E of the half-space. By looking at the integral equations for the half-space problems we can make the identifica- 2 for an incompressible material. We then find the contact pressure acting on the membrane is (cf. ref. Johnson 14 ).
The net downward force acting on the membrane is From classical contact mechanics 15 the contact radius a can be found by setting = Finding the cortical tension, bending modulus, elastic modulus and thickness from the AFM force-distance curve. The upward pushing force of the membrane tension acting on the tip must be balanced by the cantilever restoring force kd, where k is the spring constant of the cantilever and d is the deflection of the cantilever measured by the AFM laser signal. The vertical component of the tension force is 2πrγ cosα , where α is the angle between the tangent to the tip surface at the contact radius and the vertical direction. Thus For the AFM piezo signal we need to relate z at the contact radius a to the distance below the horizontal line (original contact location) in Fig. 2, where we have used equation (6) to eliminate a in terms of δ. The force -indentation curve has an inflection at where the force is The ventral and dorsal cortices come together at this point to induce the curvature change. The membrane tension γ can be determined from equation (10) and the AFM measurements of (k, d * , δ * ) (see Fig. 3). Note the probe radius R could not be measured directly, but was eliminated using equation (9).
The bending modulus can also be determined from δ * and d * as follows. Outside the contact region (r > a), we note that the axisymmetric solution Eq. 1 of is where K 0 is the decaying modified Bessel function and κ γ = /D . The two constants C 0 and C 1 can be found by matching the known displacement and slope of the probe at = r a. Since we require = →∞ w lim 0 r , we must set = C 0 0 , which yields the transcendental equation which has the root κa = 1.555265. This relation allows one to determine D in terms of γ and a. Once D and γ are determined we can estimate the cortex elastic modulus E c and thickness h c by combining Hooke's law and elementary bending theory to obtain: where the strain ε = 0.081 is calculated from the shape of the deformed surface.
Comparison of AFM -determined membrane/cortex properties with other methods. PtK-1 rat-kangaroo kidney epithelial cells were plated on fibronectin coated glass bottom dishes and subjected to contact mode AFM indentation using gold coated silicon nitride four-sided pyramidal tip cantilevers using 5-μm ramps with up to 150 nm indentations at 1 Hz. This resulted in a stereotypical force-distance curve with a characteristic bump in the low force-distance regime when the cantilever tip was just coming in contact with the cell surface. Following the "bump" upon further distance indentation, a sharp rise in force was observed with increasing distance of indentation that is typical of cell indentation observed by others 16,17 . The values of tension shown for cells 1-5 in Table 1 are comparable to values obtained from keratocytes using the tether method 18 and from fibroblasts using micropipette aspiration 11 . A kinematic method developed for bleb dynamics and based on plasma membrane viscosity yielded values 2 orders of magnitude smaller 19 . This may reflect the contribution of the cortex to membrane tension, which is periodically disrupted in blebbing cells. The substantially larger values of our bending modulus compared to others 5 is most probably due to the fact that our experimental method is relatively gentle and determines the modulus of the combined membrane/cortex structure, instead of the membrane alone. It may be that the other methods that pull tethers using an optical trap or aspirate a cell into a micropipette disrupt the membrane cortex bonds.

Determination of cell height and cytoskeletal bulk elasticity.
With the ability to measure membrane tension at the leading edge, we then sought to determine if distinct actin structures within the leading edge exhibited distinct mechanical properties, and how the mechanical properties contribute to the overall balance of forces. To visualize we transfected PTK1 cells with GFP-tagged F-tractin (provided by Mike Schell, Uniformed Services University of the Heath Sciences, Bethesda, MD, USA) as a marker of actin cytoskeletal filaments and mCherry paxillin as a marker of integrin-based focal adhesions. Simultaneous live-cell fluorescence microscopy and AFM allowed us to choose specific cytoskeletal structures in the leading edge for AFM analysis. In order to analyze our data, we derived additional parameters to allow us to test this hypothesis. The parameters required for the balance of forces at the leading edge are membrane tension, cortical elastic modulus, cortex thickness, bulk cytoskeletal elastic modulus, cell height, cytosolic pressure, and the distance between the leading edge and a focal adhesion. Cell height and bulk modulus are obtained by fitting the deeper region of the force-distance curve (red portion of Fig. 3) to the BECC model of contact mechanics 16 . Cytosolic pressure, membrane thermal fluctuation mean amplitude, dendritic actin network bending thermal fluctuation mean amplitude, and dorsal and ventral actin polymerization zone width are estimated in the following subsections. We also calculate the probability that a peak fluctuation amplitude will exceed the size of a G-actin monomer. Fig. 1, the protrusion forces acting at the edge to the right are the cytosolic pressure p and the effective pressure due to actin polymerization p f . The resisting force acting to the left is due the membrane cortex tension γ.

Estimation of cytosolic and polymerization pressures. Considering the model in
The force balance requires ( ) where h e is thickness of the lamellipod at its edge. We estimate p f from the optical trap assay of Cojoc et al. 4 who measured a net propulsive force of 3pN in filopodia with a diameter of 100 nm. The polymerization force is the sum of the net propulsive 3 pN and the 15 pN membrane resistance force measured in a retracting filopod by Bornschloegl et al. 20 . We can achieve independent estimates of the polymerization pressure and the cytosolic pressure by using a filopod model based on EM images of Medalia et al. 21 , where it is clear that all the actin is polymerized in its tightly packed bundled core, i.e. there is no cortex layer and no space for fluid to generate a cytosolic pressure compared to the relatively sparce distribution of polymerized actin in a lamellipod. Therefore the effective polymerization pressure in the filopod measurement of Cojoc et al. is (15 + 3)pN/ (π/4 ⋅ 100 nm 2 ) ≈ 2.29 kPa.
However, in the lamellipod model ( Fig. 1) only the ventral cortex is in contact with the membrane. The effective polymerization pressure in a lamellipod is therefore p f ∼ 2.29 h c /h e kPa. To estimate h e ∼ 300 nm we solved Eq. 1 with pressure loading with clamped conditions at the lamella end and free conditions at the edge. We assumed an unpressurized tapered shape seen by cryo EM 9 with the height reduced from 200 nm to 100 nm at the edge over a distance of 1 μm. Values of cytosolic and polymerization pressure are computed for each cell in Table 1.

Estimation of membrane mean fluctuation amplitude.
Here we retrace the calculations of Mogilner & Oster 6 but incorporate the AFM measurement of membrane tension reported in this study (Table 1) and cytoskeletal elastic modulus and cell height (Fig. 4B). These authors use the membrane fluctuation theory of Sackmann 22 Table 1 based on a factor of 10 smaller D, which is intended to mimic a membrane stripped of its cortex.  Table 1. Data collected from 5 live PtK-1 cells using a cantilever with stiffness k = 0.0365 N/m. Membrane tension determined using equation (10). Bending modulus can be calculated from the κ root (see text above), the membrane tension and equation (6). Calculation of all of other entries are described in text.
Scientific and listed in Table 1. The persistence length metric is often used in the analysis of in vitro images of filaments 23 .
Estimation of polymerization zone width generated by cytosolic pressure. Consider the ventral cortex modeled as a poroelastic gel having length l fixed at one end by focal adhesions and initially in contact with the membrane at the leading edge. We assume that cytosolic pressure p acts on all faces of the gel region except at the focal adhesion end which fixes that end, and we also assume that any membrane attachments are weak so that separation can occur at the leading edge. On the timescale of the edge protrusion or retraction cycle (∼ 10 sec) pressure does not have time to equalize inside the gel with the pressure on its boundaries due the hindered percolation of the cytosol through the gel. Indeed, such permeability-limited percolation leading to pressure non-equilibration has been previously noted as being likely to contribute to leading edge protrusion 24 . From elasticity theory, the compression of the cytoskeletal gel network having an elastic modulus E c , will create a gap between the membrane and actin allowing polymerization to take place in a zone having a width Δ v given by The calculated values for each cell are given in Table 1. A similar formula can be obtained for the dorsal actin cortex which we assume to be in series with the bulk cytoskeleton and have elasticity E b . The larger dorsal gap Δ d results from the softer bulk cytoskeletal spring having an E b = 5 kPa. The probability of membrane amplitude fluctuation peaks exceeding the monomer size. The amplitude probability density distribution function is classically known for the Brownian motion of a damped oscillator 25 . At long times, the probability density function is a Gaussian, so the probability P that a fluctuation amplitude is greater than or equal to x if the equipartition value is a is given by Erfc denotes the complimentary error function. The formula predicts that a g-actin monomer larger than the mean gap predicted by thermal equilibrium can still intercalate with a finite probability. The maximal dimension of an ellipsoidal model of a g-actin monomer can be estimated form its crystal structure to be . 6 7 nm, while the same dimension is estimated as . 8 4 nm in solution using dynamic light scattering 26 . Taking x = 7 nm, recognizing that the solution monomer maximal dimension may be slightly larger than its crystallized value, but substantially larger than the usual value of 2.7 nm used in the Brownian ratchet literature 6 based on the assembled helix repeat, and a = 7.3 nm for the mean value of membrane fluctuation amplitude given by the mean value of δ m in Table 1 gives P = 0.169.
Other probabilities based on the means of δ f , Δ v , and Δ d are 0.288, 0.381, and 0.481 respectively. We take notice that / = . ⟨ ⟩ ⟨ ⟩ p p 2 78 f is close to the ratio of probability of intercalation into the mean ventral gap caused by cytosolic pressure, to the probabilty of intercalation into the mean gap caused by membrane fluctuations.

Discussion
Novel analysis of AFM force-indentation curves presented here has allowed us to measure membrane/ cortex tension, cortical membrane bending rigidity, cortical elastic modulus and cortical thickness at the leading edge of a lamellipod without the need for pulling tethers using an optical trap set-up or by micropipette suction. Both these previous methods are much harsher perturbations to the cell. The determination of tension at the same spatial location as the measurement of cytoskeletal bulk elasticity was achieved using a hybrid spinning disk/AFM set-up. Our microscope permitted us to examine the relationship between measured tension, calculated cytosolic pressure, and elastic moduli via a force balance. Although our measurements were made by probing the cell in a direction perpendicular to its protrusion direction we believe this is still meaningful to determine the local isotropic cytosolic pressure at the leading edge that provides the protrusive force. We could also estimate the effective actin polymerization pressure at the leading edge of a lamellipod based on the model shown in Fig. 1 and previous optical trap measurements by others 4 on filipodia. We found that these two sources of propulsive force are comparable in a lamellipod. Our results also suggest that cytosolic pressure fluctuations facilitate actin polymerization by increasing the width of the polymerization zone. Our estimated zone of polymerization is consistent with previous actin dynamics imaging, as well as tomographic cryo -EM images showing a decreasing number of f-actin ends as the membrane is approached. Thus we conclude that pressure fluctuations provide a propulsive force comparable to actin polymerization, while also increasing the probability that g-actin intercalation can occur.

Materials and Methods
Imaging. The base plate of an AFM (Bioscope II, Bruker Instruments) was placed on an inverted microscope (Ti-E, Nikon). 488 nm and 561 nm excitation wavelength from a laser source (MLC 400, Agilent Technologies) was directed via fiber optics to a spinning disk confocal (CSU-X1, Yokogawa). Images were collected using a Plan APO VC 100 × 1.40 NA Phase objective on a high speed camera (Neo sCMOS, Andor Technology). Camera and peripherals were controlled through Metamorph software (Downingtown, PA). To minimize vibration induced from the disk rotation of the Yokogawa scan head, the CSU-X1 was mounted and aligned such that the scan head and microscope were not in direct contact. The placement of the AFM on the microscope was such that the AFM cantilever was in the microscope light path.
Atomic Force Microscopy. Sharp tip contact mode AFM was used with BECC bottom correction 16 for Young's modulus and cell height determination. A new AFM model for membrane/cortex mechanical properties determination is presented here for indentation by a sharp tip with finite radius of curvature. Gold coated silicon nitride pyramidal tip MLTC cantilevers (Bruker Nano) were used with a spring constant 0.0365 N/m, determined by thermal fluctuation method. Ten ramps were averaged at a given location on the cell. The ramp rate was 1/sec.