While semi-flexible polymers and fibres are an important class of material due to their rich mechanical properties, it remains unclear how these properties relate to the microscopic conformation of the polymers. Actin filaments constitute an ideal model polymer system due to their micron-sized length and relatively high stiffness that allow imaging at the single filament level. Here we study the effect of entanglements on the conformational dynamics of actin filaments in shear flow. We directly measure the full three-dimensional conformation of single actin filaments, using confocal microscopy in combination with a counter-rotating cone-plate shear cell. We show that initially entangled filaments form disentangled orientationally ordered hairpins, confined in the flow-vorticity plane. In addition, shear flow causes stretching and shear alignment of the hairpin tails, while the filament length distribution remains unchanged. These observations explain the strain-softening and shear-thinning behaviour of entangled F-actin solutions, which aids the understanding of the flow behaviour of complex fluids containing semi-flexible polymers.
Networks of semi-flexible polymers or fibres form the basis of many materials that we encounter in daily life. Concentrated dispersions of wormlike micelles are used to engineer the viscoelastic properties of industrial and consumer products1, while polysaccharides and self-assembled supra-molecular structures are used in tissue engineering2 and smart gels3. In biology, eukaryotic cells are mechanically supported by an internal cytoskeleton composed of protein filaments including filamentous (F-)actin. These filaments can form striking non-equilibrium patterns when they are subjected to cytoplasmic flows within plants4 and animal embryos5 generated by molecular motor activity. The basis of understanding these phenomena is knowledge of the conformational response of the stiff polymers constituting the materials to an applied flow.
Here, we directly visualize the full three-dimensional (3D) contour of labelled F-actin subjected to shear flow, to resolve the microscopic basis of the macroscopic non-Newtonian flow response. Our system lies in between the limiting cases of permanently cross-linked networks, where filaments do not relax, and of dilute non-interacting polymers, where filaments relax freely. Permanently cross-linked networks, which represent a model for cytoskeletal networks, show remarkable viscoelastic properties such as elasticity at low filament density and strong strain-stiffening behaviour, where the stress increases with increasing strain6,7,8. Theoretical models can capture this behaviour on the basis of microscopic properties of the filaments, such as the bending rigidity, length distribution and cross-link density9.
The rheology of F-actin solutions in the absence of cross-links10,11,12,13,14 is comparatively poorly understood. The complex behaviour of such solutions is due to entanglements between the filaments that form at concentrations above the overlap density, where diffusion takes place by reptation within tube-like confinement zones defined by the entanglements15. The tube itself is not a rigid object, but describes rather a confining potential with a varying tube radius16. The linear viscoelastic response of such entangled F-actin solutions to small deformations that leave the tubes unaffected have been described by wormlike chain models17,18. When starting up shear flow, entangled F-actin solutions first display strain-stiffening, followed by strain-softening, where stress decreases with increasing strain13,14,19. In addition, the viscosity of entangled F-actin decreases with increasing shear rate, known as shear-thinning10,19,20. These are key ingredients for the formation of flow instabilities, which often occur in concentrated semi-flexible polymers21 such as DNA22, wormlike micelles23 and also F-actin20. Though the connection between shear-thinning and flow instabilities is fairly well understood24,25, the microscopic mechanism of shear-thinning is still under debate mainly because real space information for nanoscopic systems like DNA and wormlike micelles is limited. F-actin is a particularly useful semi-flexible model polymer because the micron-sized lengths and relatively high stiffness allows imaging of the conformation at the single filament level by fluorescence microscopy15,26,27,28.
Two-dimensional filament tracking in microfluidic devices for dilute F-actin solutions, where the filaments do not interact, has shown that the conformational dynamics is dominated by the interplay between the Brownian motion of the filament ends and the shear flow26. Due to this competition, the filaments tumble in the gradient direction forming so-called hairpins, which contain highly curved segments between the stretched parts of the filaments. Here, the only relevant stress component is the shear stress, while reorientational motion takes place in the flow-gradient plane. The frequency of this tumbling motion in this direction was shown to decrease when the system is entangled29. However, since stress can develop in all directions for entangled systems22,30,31, knowledge of the 3D contour of the filament is crucial for a full understanding of the mechanical response of these systems.
We use here concentrations just below and above the concentration where a confining tube can be defined32. We achieve 3D in situ imaging by employing a counter-rotating cone-plate shear cell (Supplementary Fig. 1) in combination with a fast confocal microscope33. The advantage of this shear cell is that it induces a simple shear flow with a linear velocity gradient, while the presence of a zero-velocity plane guarantees that the filaments stay sufficiently long in the field of view to obtain the full 3D contour. This approach allows us to test predictions on the structural origin of strain-softening of entangled semi-flexible polymers34,35. We quantitatively measure the effect of strain on the distribution of the local curvature. Moreover, a detailed analysis of the orientational distributions of the filaments reveals that entanglements are lost during strain deformation while hairpins are formed that are confined in the flow-vorticity plane. Thus we identify the mechanism for strain-softening and shear-thinning of entangled F-actin solutions.
Strain-softening and shear-thinning
We subjected F-actin solutions of 0.02 and 0.15 mg ml−1 to shear flow , increasing the shear rate from 0.075 to 0.3 s−1 in four steps of 5 min, while keeping track of the total acquired strain, see Methods section. The stress as a function of strain at 0.15 mg ml−1 is plotted in Fig. 1a. The stress decreases with increasing strain after start-up of the shear flow at the lowest shear rate. This behaviour is indicative for strain-softening. After about eight strain units, the stress stays constant and the viscosity of the system can be determined. In Fig. 1b, the viscosity is plotted as a function of shear rate for both concentrations. Both systems display a clear shear-thinning behaviour. Thus we observe both strain-softening and shear-thinning. The viscosity at 0.02 mg ml−1 is an order of magnitude less than that at 0.15 mg ml−1 and approaches for high shear rates the buffer viscosity, exemplifying the effect of entanglement. From now on we refer to these samples as chigh=0.15 mg ml−1 and clow=0.02 mg ml−1, where the indices refer to the viscosity of the samples.
Global and local information as obtained from imaging
To visualize shear-induced conformational transitions of entangled individual actin filaments, we embedded trace amounts of fluorescently labelled actin filaments in the host dispersion. For imaging we used a home-built counter-rotating cone-plate cell mounted on an inverted microscope (Fig. 1c) that was equipped with a multi-pinhole confocal scanning head, allowing frame rates of eight frames per second. We obtain the full 3D contour of on average 150 filaments per analysed dimensionless strain. Figure 1d shows several filaments, including one for which the contour is fitted. The coordinate system of this fitted contour, parametrized by rj (j is the index of the coordinates along the contour), is given by the velocity direction (along the shear direction), gradient direction (along the gap direction) and vorticity direction. From rj we can extract information about the global filament conformation, such as the filament contour length L and its end-to-end vector Ree. Figure 2a,b show the distribution of the ratio Ree/L for chigh, which is a measure for the degree of stretching. This distribution does not show a significant change with strain for the short filaments (<13 μm, Fig. 2a). For the long filaments (>21 μm, 2b), the distribution widens towards small Ree/L while a pronounced peak is formed for Ree/L→1. This means that the filaments become more stretched and at the same time more bent, which is indicative for the formation of hairpins. Figure 2c displays the length distribution at different dimensionless strain values for chigh. The distribution does not shift to lower values of filament lengths with increasing strain, so that we conclude that shear-softening and shear-thinning is not due to rupture of actin filaments.
We will characterize the filament conformations by extracting the local curvature, κj, tangent vector, , and binormal vector, , along the contour, see Fig. 3a. To calculate these values, we average over two neighbouring points in the contour. Thus, the contour is split up in segments of an average length of ‹Ln›=2.36 μm (Supplementary Note 1). Figure 3b,c display the projections of two typical examples of filaments strained at clow (b) and chigh (c). At clow, which corresponds to the onset of entanglements, we find filaments with highly curved segments (region I) and segments that are stretched and orientated with the flow direction (region II). At chigh, the filament has a hairpin conformation (region III), with two dangling ends which are stretched in the flow direction (region IV). Strikingly, for chigh the hairpin is confined to the flow/vorticity plane, with its binormal vectors (blue arrows) pointing in the gradient direction (Fig. 3c). This behaviour is markedly different from the behaviour observed for filaments in dilute solutions26, which tumble in the gradient direction. The behaviour at clow is intermediate.
Filament stretching and bending in shear flow
The typical configuration of a sheared filament as displayed in Fig. 3a shows a hairpin, which is characterized by two stretched tails connected by a bent part. The formation of these hairpins suggests that the distribution of the curvature of the segments changes when entangled semi-flexible polymers are sheared. Stretching and bending of filaments both contribute to the free energy of a filament. Usually this is connected to Ree, which measures the stretching of a filament36. Ree, however, can be small for hairpins, which can thus be incorrectly taken to suggest that the entropic contribution to the energy is low. This is clearly a flaw because the main part of the filament is stretched. One therefore needs to analyse the filaments at smaller length scales. We do this by using the local curvature κj, which is related to the scaled end-to-end vector xj=Rj/‹Ln› (Fig. 3a). In this analysis we only used filaments with length L>21 μm to assure good statistics and sufficient flexibility (L/lp>1). On average we analysed about 1,200 segments per image stack, allowing us to obtain distributions for the curvature P(κj).
The distribution of κj are plotted in Fig. 4 for zero shear strain and high strain (γ=215±12). For both concentrations, the equilibrium curvature distribution is well-described by a Gaussian distribution. The distribution in equilibrium deviates from earlier studies of unsheared F-actin37, probably due to the different sample environment and relatively high concentrations of filaments that are used in this study. For the low concentration the distribution remains unchanged when straining the system. In contrast, at the high concentration we observe that the distribution takes the form of a log-normal distribution. Compared with the unsheared situation, the peak of the distribution shifts towards smaller values of κj, showing that the majority of segments are more stretched. In addition the distribution also has a long tail with a power law form, showing that strain induces curvature in the system. These observations hint that at chigh energy is stored in the system, but not at clow. This is consistent with the presence of entanglements at chigh. However, these observations do not yet explain the strain-softening behaviour.
Orientation of shear-induced hairpins
To quantify the orientations of the filaments, we collected all local tangent and binormal vectors along the filament contour, as plotted in Fig. 5a,d on a unit sphere, and calculated the corresponding two-dimensional angular orientational distribution functions which are best fitted with a two-dimensional Lorentzian given by . Here the angles φ and θ, which set up the vectors and , are defined as shown in Fig. 3a right. As examples we show in Fig. 5 the distribution for chigh after straining the sample to γ=215±12, separating the orientation of the stretched segments, using all segments with κj<0.1 μm−1 (top) and bent segments, using all segments with κj>0.2 μm−1 (bottom).
The stretched segments display a strong shear alignment of the tangent: Figure 5a,b shows that the segments all point in the flow direction. Note however that the distributions are slightly biaxial, that is, not symmetric around the maximum. The binormal distribution has a low degree of order and is strongly biaxial, Fig. 5c. This can be rationalized as follows. When the tangent is well aligned, then there is no clearly defined plane that is spanned by two sequential segments. Thus the binormal is ill-defined though per definition in the plane perpendicular to the tangent: the distribution in Fig. 5c is very sharp with respect to φB and very broad with respect to θB. On the contrary, the bent segments have a pronounced uniaxial ordering of the binormal pointing in the gradient direction (Fig. 5d,f), while the distribution of the tangent is biaxial (Fig. 5e), which is to be expected for hairpins, see for example region I in Fig. 3b.
To quantify separately the orientational behaviour of the stretched and bent parts of the filaments, we use the distribution functions f(θ,φ) to calculate the orientational order tensors and similarly . For our purpose the traceless diagonalized form is particularly useful since Fig. 3 and Fig. 5b both suggest that the orientational distributions can be biaxial. may be written as
where λT,B is the orientational order parameter of the main orientation axis and ηT,B parametrizes the biaxiality of the system.
We will now discuss the behaviour of these parameters for the four features that we indicated in Fig. 3b,c: segments with high curvatures of κj>0.2 μm−1 for clow (I) and chigh (III), and segments with low curvatures of κj <0.1 μm−1 for clow (II) and chigh (IV). The stretched segments at chigh (IV in Fig. 3) clearly display a high degree of ordering of the tangent with λT → 1 (solid symbols in Fig. 6b). The ordering is uniaxial (solid symbols in Fig. 6f) and almost along the flow direction, as expected (solid symbols in Fig. 7c,f). λT is higher for chigh than for clow (compare Fig. 6a,b, II and IV), which shows that entanglements enhance ordering when the sample is sheared. Interestingly, λT jumps immediately to a high value when strain is applied for chigh. On the contrary, λT displays a moderate increase with increasing strain for clow, while the corresponding eigenvector tilts towards the flow direction (solid symbols in Fig. 7a,e). This complies with measurements on wormlike micelles38. Thus, the entanglements not only cause stretching of parts of the filaments, as seen from Fig. 4, but also strong shear alignment of these stretched segments along the flow direction.
Although this shear alignment is a well-known phenomenon, the orientational behaviour of segments with high curvature (I and III in Fig. 3) is a priori not obvious. The binormal is a particularly informative parameter as it is oriented along the normal of the plane spanned by a curved segment. When there is a train of segments with similar curvature, which is the case in the bent part of a hairpin, then binormal vectors point in the same direction. This can be seen for chigh, where the blue arrows in region III of Fig. 3c on the right all point in the gradient direction. The behaviour of the binormal order parameter λB confirms this observation. Indeed λB is higher for the highly curved than for the stretched segments; compare open and solid symbols in Fig. 6d. The eigenvectors belonging to λB point along the gradient direction (Fig. 5f and open symbols in Fig. 7d,h) and therefore also the plane spanned by the highly curved segments. The fact that the binormal is well defined for κj>0.2 μm−1 implies that the ordering of the tangent is low and biaxial. This is indeed confirmed by Fig. 6f, where the biaxiality of the tangent ηT is plotted: for chigh the biaxiality of the tangent ηT increases with strain when κ>0.2 μm−1. We therefore conclude that the plane spanned by the bent part of the hairpin, which we labelled III in Fig. 3c, indeed is located in the flow-vorticity plane, with its normal pointing in the gradient direction.
The behaviour of the binormal and biaxiality is distinctively different for clow. No increase in λB nor in ηT is observed with increasing strain (Fig. 6c,e). Thus, there is no well-defined orientation of hairpins at the low concentration, as is exemplified in region I of Fig. 3b. In Fig. 6, we also plot the points measured about 150 s after cessation of shear flow. We note a clear difference between the relaxation times at low and high concentration: for clow the orientation is partly lost, whereas for chigh the orientations remain unchanged. This indicates that the relaxation time at chigh is indeed much longer than for clow. A time series after cessation of flow confirms these observations: the shape is mainly lost for clow (Fig. 6g), whereas at chigh the filament conserves its shape (Fig. 6h).
By directly visualizing the full 3D conformation of individual actin filaments within entangled F-actin solutions, we can show how entanglements influence the conformation of the filaments in response to shear flow. First, the distribution of curvature for clow, at the onset of the entangled regime, remains unchanged when applying shear flow, while the number of stretched as well as bent segments increases for chigh when applying shear, see Fig. 4. This explains the much higher viscosity for chigh. Second, we observe at chigh that hairpins form in shear flow, which tilt into the flow-vorticity plane. The behaviour of entangled filaments is in marked contrast with the dynamics of filaments in dilute solutions which tumble in the gradient direction26. Our observations also explain why tumbling was previously shown to be strongly reduced at concentrations three times higher than chigh (ref. 29), although the shear rates used in this reference were (102) higher. We find that the response at clow lies between these two extremes, as there is no well-defined plane into which the filaments turn. In this case we find shear-thinning which is purely due to increased alignment of the filaments, as we conclude from Fig. 6a,e.
We will now try to relate the formation of the strongly aligned hairpins with the strain-softening in entangled solutions. Hairpins are generally viewed as a signature of an entanglement. Two entangled filaments will strongly bend around the point where they are entangled when they are moved in opposite directions faster than the time they need to relax. Mechanically this leads to strain-stiffening, while pairs of hairpins with the orientations of the bent segments roughly perpendicular to each other result in a very flat distribution of the binormal of the bent segments. We observe, however, exactly the opposite: the binormal of the bent segments is highly aligned when straining the system at chigh. Moreover, there is a strong increase in the number of stretched segments and a marginal increase in the number of bent segments and we predominantly find only one hairpin per filament, see Fig. 4b. These observations strongly hint that entanglements disappear as the system is strained. Since the hairpins and their stretched tails are strictly located in the flow-vorticity plane, they have no components in the gradient direction that cause the shear stress, which results in strain softening. The filaments slide over each other facilitating lamellar flow. These findings are contrary to theoretical predictions that hairpins cause strain-stiffening. However, the theory considered the contour lengths to be much longer than the persistence length34,35, while in our experiments they are of the same order. Theory does predict an instability where shear deformation pushes out contacts between filaments causing strain-softening35. This strain-induced loss of entanglements, very similar to the convective constraint release39, is exactly what we find.
There are no predictions of the shape of the filaments at high strains after strain softening. We find experimentally that the effect of the surrounding filaments is to confine the hairpins in the flow-vorticity plane. Instead of a confining tube as can be defined in equilibrium, there are now confining planes, without entanglements. This can also be appreciated from the movie (Supplementary Movie 1), where fluctuations in the vorticity directions are observed, but not in the gradient direction, in contrast to the movie of a filament at clow (Supplementary Movie 2). While the hairpins immediately form and can be related to the strain-softening, we also observe shear thinning, see Fig. 1b. This behaviour is likely to relate to the small but significant increase in the orientational ordering of the stretched segments (solid symbols in Fig. 6b) and decrease in the biaxiality (solid symbols in Fig. 6f) parameterizing the flow alignment of the segments. These new scenarios for strain-softening and shear-thinning exclude the need for scission of the F-actin filaments as a pathway to explain nonlinear rheology, which is known for living polymers such as wormlike micelles23. Indeed, we observe in Fig. 2b no change in the filament length distribution over the full measured range of strain.
The mechanism for stress release by the formation of disentangled sliding hairpins could be a precursor for the formation of flow instabilities, which is often related with local reorganization of the constituting particles23. The distinct orientation of the hairpins also suggests that a normal stress builds up which could lead to flow instabilities. Polymer solutions22,30,31, polymer melts40 and sticky carbon nanotubes41 are all systems that display pronounced normal stresses as well as flow instabilities. Flow instabilities have also been observed for actin dispersions at higher concentrations than we used20. We did not find any signature of such a behaviour, scanning a significant part of the gap of the shear cell at a fixed position from the centre of the shear cell. This could be due to the limited strain applied to the system as well as the relatively low filament concentration as compared with ref. 20.
In conclusion, we expect that the mechanism of stress release we identified here may be generally valid for solutions of semi-flexible polymers, including supramolecular systems23,42,43,44. Thus, our findings will aid to the understanding of the complex flow behaviour of such systems. Likewise, this mechanism could impact the self-organization of cytoskeletal filaments in response to intracellular shear flows created by processes like cytoplasmic streaming4,5.
Protein purification and sample preparation
G-actin was isolated from rabbit skeletal muscle45, stored in G-buffer solution (5.0 mM Tris, 0.2 mM CaCl2, 0.2 mM ATP, 0.2 mM DTT, pH 7.4, 21 °C) at 4 °C. Fluorescently labelled filaments were obtained by polymerizing G-actin (0.2 mg ml−1) for 1 h at 21 °C by adding 10 vol% 10 × F-buffer solution (20 mM Tris, 2.0 mM CaCl2, 1.0 M KCl, 20 mM MgCl2, pH 8.5, 21 °C, 5.0 mM ATP, 2.0 mM DTT) in the presence of an equimolar amount of Atto647N-Phalloidin (Atto-Tec). Unlabelled G-actin (0.2–0.3 mg ml−1) was similarly polymerized, but in the presence of unlabelled phalloidin (Sigma/P2141). These filaments have a persistence length of lp 9–18 μm (ref. 46, 47, 48, 49). Samples were prepared by diluting labelled filaments in a 1:2,000 ratio with GFS-buffer solution (10% 10 × F-buffer, 60% sucrose in G-buffer) and mixing this solution in equal volume with unlabelled F-actin to reach final concentrations of 0.02 and 0.15 mg ml−1. The final buffer solution thus contained 30% sucrose, which reduced the off-rate of labelled phalloidin50, improving the signal-to-noise ratio during image acquisition. All measurements were done at 21 °C.
Shear cell and microscopy
To produce shear flows with a well-defined linear velocity gradient, we used an adapted version of the counter-rotating cone-plane shear cell used in ref.51 (Supplementary Fig. 1). It consists of a bottom glass plate (diameter 80 mm, thickness 170 μm, Menzel) which is fixed by two Teflon rings that are pressed together between a titanium plate at the bottom and a stainless steel block at the top. In this block there is a hole where the top cone is inserted, which is also made out of stainless steel. Both the glass plate and steel cone can move independently and are in our experiments moved counter clockwise. We used an Epiplan-Neofluar × 50/1.0 Pol objective (Zeiss). The shear cell was mounted on an inverted microscope (Zeiss/Axiovert 200 M), equipped with a multi-pinhole confocal system (VisiTech/VT-Infinity-I) and an Epiplan-Neofluar × 50/1.0 Oil Pol Objektiv (Zeiss). An Argon/Krypton laser (Spectra Physics/Stabilite 2250) operating at 647 nm was used for excitation of the fluorescent dye. An observation area of 151 μm × 151 μm was imaged onto an EMCCD-camera (Andor/iXon DU-897) operated with IQ software. Confocal stacks consisted of 51 frames taken at 1-μm intervals at a rate of 7.2 s per stack. The difference in the geometrical and the optical path length, due to the different refractive indices of the immersion oil (noil=1.518) objective and the actin solution (≈ nwater=1.33) was determined by two independent methods. First we measured the refractive indices of the immersion oil and the actin solution and calculated the correction factor nk on the basis of the ratio of those indices. Second we filled a glass capillary of known thickness (10 μm±10%) with a solution of fluorescent beads (Ø 0.5 μm, Latex beads, Sigma) and measured the geometrical path length, by the use of a calibrated piezo element, calculating the correction factor nk on the basis of the difference of the capillary and geometrical length: . Both methods gave equivalent results. Data were taken 30–80 μm into the sample to reduce wall effects.
Our shear protocol consists of four blocks of 5 min where a shear rate of 0.075, 0.15, 0.225, 0.3 s−1, respectively, is applied. The reason for the shear protocol is that after sample loading and inserting the cone, the orientation of the filaments for chigh is not well defined, while it does not relax. This is a fact that cannot be avoided. Thus quite some strain units are needed to remove this memory effect. For clow the sample does relax before we start the experiment and indeed we can follow trends with increasing strain.
Rheology data are taken with an Anton Paar MCR501, using a cone-plate geometry with 30 mm diameter and 1 degree angle.
The 3D filament contours were tracked with the autodepth-function of the visualization and analysis software Imaris (Bitplane/ Imaris 6.1), and subsequent filament position analysis was done using Matlab (Version, Mathworks). As a control for the conformation of the filaments before the shear experiment (γ=0), one frame was taken before placing the cone. This frame contained about 50 tracer filaments that were tracked with Imaris. For the analysis of the filament conformation at a certain strain value, three statistically independent stacks (circa 30 s apart) before changing the shear rate, were analysed, containing also about 50 tracer filaments each, corresponding to a strain of γ=21±3, 59±6, 126±7 and 215±12. For the last data point three frames, 120, 150 and 180 s after cessation, were analysed.
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G.H.K. was supported by the Foundation for Fundamental Research on Matter (FOM), which is part of NWO, and N.A.K. acknowledges support by a Marie Curie FP7 IIF Fellowship. D.G. was supported by the International Helmholtz Research School (BioSoft). We thank F. MacKintosh, R. Winkler, J. Dhont, M. Giesen and R. Merkel for fruitful discussions and Y. Jia for help with the data analysis.
The authors declare no competing financial interests.
Supplementary Figure 1 and Supplementary Note 1 (PDF 271 kb)
Projections of a labeled F-actin filament in the flow-vorticity plane (left) and flow-gradient plane (right) at a low concentration clow. The flow direction is in the z-direction. For clow the fluctuation in the gradient direction is prominent. The movie is taken at a strain of γ=203–219 and shear rate of 0.3 and consist of a series of stacks of 51 frames taken in 7.1 s; scale bar is 10 μm. (AVI 267 kb)
Projections of a labeled F-actin filament in the flow-vorticity plane (left) and flow-gradient plane (right) at a high concentration chigh. The flow direction is in the z-direction. Clearly, for chigh the fluctuations in the gradient direction are negligible. The movie is taken at a strain of γ=203–219 and shear rate of 0.3 and consist of a series of stacks of 51 frames taken in 7.1 s; scale bar is 10 μm. (AVI 285 kb)
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Kirchenbuechler, I., Guu, D., Kurniawan, N. et al. Direct visualization of flow-induced conformational transitions of single actin filaments in entangled solutions. Nat Commun 5, 5060 (2014). https://doi.org/10.1038/ncomms6060
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