Actin filaments undergo limited subunit exchange in physiological salt conditions

The exchange of actin filament subunits for unpolymerized actin or for subunits in other filaments has been quantitated by three experimental techniques: fluorescence energy transfer, incorporation of 35S-labeled actin monomers into unlabeled actin filaments, and exchange of [14C]ATP with filament-bound ADP. In the fluorescence energy transfer experiments, actin labeled with 5-(iodoacetamidoethyl)aminonaphthalene- 1-sulfonic acid (IAENS) served as the fluorescent energy donor, and actin labeled with either fluorescein-5-isothiocyanate (FITC) or fluorescein-5-maleimide (FM) served as the energy acceptor. Fluorescent- labeled actins from Dictyostelium amoebae and rabbit skeletal muscle were very similar to their unlabeled counterparts with respect to critical actin concentration for filament assembly, assembly rate, ATP hydrolysis upon assembly, and steady-state ATPase. As evidenced by two different types of fluorescence energy transfer experiments, less than 5% of the actin filament subunits exchanged under a variety of buffer conditions at actin concentrations greater than 0.5 mg/ml. At all actin concentrations limited exchange to a plateau level occurred with a half- time of about 20 min. Nearly identical results were obtained when exchange was quantitated by incorporation of 35S-labeled Dictyostelium actin monomers into unlabeled muscle actin or Dictyostelium actin filaments. Furthermore, the proportion of filament-bound ADP which exchanged with [14C]-ATP was nearly the same as actin subunit exchange measured by fluorescence energy transfer and 35S-labeled actin incorporation. These experiments demonstrate that under approximately physiologic ionic conditions only a small percentage of subunits in highly purified skeletal muscle or Dictyostelium F-actin participate in exchange.     

Assembly and exchange of intermediate filament proteins of neurons: neurofilaments are dynamic structures

We have explored the dynamics of intermediate filament assembly and subunit exchange using fluorescently labeled neurofilament proteins and a fluorescence resonance energy transfer assay. Neurofilaments (NFs) are assembled from three highly phosphorylated proteins with molecular masses of 180 (NF-H), 130 (NF-M), and 66 kD (NF-L) of which NF-L forms the structural core. The core component, NF-L, was stoichiometrically labeled at cysteine 321 with fluorescein, coumarin, or biotin-maleimide to produce assembly-competent fluorescent or biotinylated derivatives, respectively. Using coumarin-labeled NF-L as fluorescence donor and fluorescein-labeled NF-L as the fluorescence acceptor, assembly of NF filaments was induced by rapidly raising the NaCl concentration to 170 mM, and the kinetics was followed by the decrease in the donor fluorescence. Assembly of NF-L subunits into filaments does not require nucleotide binding or hydrolysis but is strongly dependent on ionic strength, pH, and temperature. The critical concentration of NF-L, that concentration that remains unassembled at equilibrium with fully formed filaments, is 38 micrograms/ml or 0.6 microM. Under physiological salt conditions NF-L filaments also undergo extensive subunit exchange. Kinetic analysis and evaluation of several possible mechanisms indicate that subunit exchange is preceded by dissociation of subunits from the filament and generation of a kinetically active pool of soluble subunits. Given the concentration of NF-L found in nerve cells and the possibility of regulating this pool, these results provide the first information that intermediate filaments are dynamic structures and that NF-L within the NF complex is in dynamic equilibrium with a small but kinetically active pool of unassembled NF-L units.     

Direct Observation of Subunit Exchange along Mature Vimentin Intermediate Filaments

Actin filaments, microtubules, and intermediate filaments (IFs) are central elements of the metazoan cytoskeleton. At the molecular level, the assembly mechanism for actin filaments and microtubules is fundamentally different from that of IFs. The former two types of filaments assemble from globular proteins. By contrast, IFs assemble from tetrameric complexes of extended, half-staggered, and antiparallel oriented coiled-coils. These tetramers laterally associate into unit-length filaments; subsequent longitudinal annealing of unit-length filaments yields mature IFs. In vitro, IFs form open structures without a fixed number of tetramers per cross-section along the filament. Therefore, a central question for the structural biology of IFs is whether individual subunits can dissociate from assembled filaments and rebind at other sites. Using the fluorescently labeled IF-protein vimentin for assembly, we directly observe and quantitatively determine subunit exchange events between filaments as well as with soluble vimentin pools. Thereby we demonstrate that the cross-sectional polymorphism of donor and acceptor filaments plays an important role. We propose that in segments of donor filaments with more than the standard 32 molecules per cross-section, subunits are not as tightly bound and are predisposed to be released from the filament.     

Fluorescence energy transfer between subfragment-1 and actin points in the rigor complex of actosubfragment-1.

The fast-reacting thiol (SH1) of myosin subfragment-1 (S-1) was covalently and specifically labeled with (iodoacetamido)fluorescein (IAF), while Cys-373 of actin was also covalently and preferentially labeled with N-(iodoacetyl)-N'-(1-sulfo-5-naphthyl)ethylenediamine (1,5-IAEDANS). The method of fluorescence energy transfer was used to examine the spatial proximity between the two sites, i.e., SH1 and Cys-373, in the rigor complex of acto-S-1. Approximately 30% fluorescence energy transfer was observed from the 1,5-IAEDANS on actin as a donor to the IAF on S-1 as an acceptor in their rigor complex; under certain assumptions this corresponds to a distance of ca. 6.0 nm.     

Actin filament uncapping localizes to ruffling lamellae and rocketing vesicles

Regulated actin filament assembly is critical for eukaryotic cell physiology. Actin filaments are polar structures, and those with free high affinity or barbed ends are crucial for actin dynamics and cell motility. Actin filament barbed-end-capping proteins inhibit filament elongation after binding, and their regulated disassociation is proposed to provide a source of free filament ends to drive processes dependent on actin polymerization. To examine whether dissociation of actin filament capping proteins occurs with the correct spatio-temporal constraints to contribute to regulated actin assembly in live cells, I measured the dissociation of an actin capping protein, gelsolin, from actin in cells using a variation of fluorescence resonance energy transfer (FRET). Uncapping was found to occur in cells at sites of active actin assembly, including protruding lamellae and rocketing vesicles, with the correct spatio-temporal properties to provide sites of actin filament polymerization during protrusion. These observations are consistent with models where uncapping of existing filaments provides sites of actin filament elongation.     

Conformational and dynamic differences between actin filaments polymerized from ATP- or ADP-actin monomers

Conformational and dynamic properties of actin filaments polymerized from ATP- or ADP-actin monomers were compared by using fluorescence spectroscopic methods. The fluorescence intensity of IAEDANS attached to the Cys(374) residue of actin was smaller in filaments from ADP-actin than in filaments from ATP-actin monomers, which reflected a nucleotide-induced conformational difference in subdomain 1 of the monomer. Radial coordinate calculations revealed that this conformational difference did not modify the distance of Cys(374) from the longitudinal filament axis. Temperature-dependent fluorescence resonance energy transfer measurements between donor and acceptor molecules on Cys(374) of neighboring actin protomers revealed that the inter-monomer flexibility of filaments assembled from ADP-actin monomers were substantially greater than the one of filaments from ATP-actin monomers. Flexibility was reduced by phalloidin in both types of filaments.     

Intermonomer flexibility of Ca- and Mg-actin filaments at different pH values.

The fluorescence resonance energy transfer parameter, f, is defined as the efficiency of the energy transfer normalized by the quantum yield of the donor in the presence of acceptor. It is possible to characterize the flexibility of the protein matrix between the appropriate fluorescent probes by monitoring the temperature dependence of f. The intermonomer flexibility of the Ca-actin and Mg-actin filaments was characterized by using this method at pH values of 6.5 and 7.4. The protomers were labeled on Cys374 with donor [N-(((iodoacetyl)amino)ethyl)-5-naphthylamine-1-sulfonate; IAEDANS] or acceptor [5-(iodoacetamido)fluorescein; IAF] molecules. The temperature profile of f suggested that the intermonomer flexibility of actin filaments was larger at pH 7.4 than pH 6.5 in the case of Mg-F-actin while this difference was absent in the case of Ca-F-actin. More rigid intermonomer connection was identified at both pH values between the protomers of Mg-F-actin compared to the Ca-F-actin. The results were further supported by time dependent fluorescence measurements made on IAEDANS and IAF labeled Mg- and Ca-actin filaments at pH 6.5 and 7.4. Our spectroscopic results may suggest that the altered function of muscle following the change of pH within the muscle cells under physiological or pathological conditions might be affected by the modified dynamic properties of the magnesium saturated actin filaments. The change of the intracellular pH does not have an effect on the intermonomer flexibility of the Ca-actin filaments.     

Distances between tropomyosin sites across the muscle thin filament using luminescence resonance energy transfer: evidence for tropomyosin flexibility

To obtain information about the interaction of tropomyosin (Tm) with actin associated with the regulatory states of the muscle thin filament, we used luminescence resonance energy transfer (LRET) between Tb(3+) as a donor and rhodamine as an acceptor. A novel Tb(3+) chelator, S-(2-nitro-5-thiobenzoate)cysteaminyl-DTPA-Cs124, was synthesized, which specifically labels Cys groups in proteins. With the Tb chelate as the donor and tetramethylrhodamine-5-maleimide as the acceptor, both bound to specific Cys groups of Tm, we obtained 67 A as the distance between Tm's across the actin filament, a much shorter value than that obtained from structural studies (72-86 A). The difference appears to be due to submillisecond motion associated with Tm flexibility, which brings the probes closer during the millisecond lifetime of the donor. Ca(2+) did not change the energy transfer with the reconstituted thin filament, but myosin subfragment 1 decreased the transfer, consistent with either a 5-6 A increase in distance or, more likely, a decrease in flexibility.     

Mechanism of interaction of Dictyostelium severin with actin filaments

Severin, a 40,000-dalton protein from Dictyostelium that disassembles actin filaments in a Ca2+ -dependent manner, was purified 500-fold to greater than 99% homogeneity by modifications of the procedure reported by Brown, Yamamoto, and Spudich (1982. J. Cell Biol. 93:205-210). Severin has a Stokes radius of 29 A and consists of a single polypeptide chain. It contains a single methionyl and five cysteinyl residues. We studied the action of severin on actin filaments by electron microscopy, viscometry, sedimentation, nanosecond emission anisotropy, and fluorescence energy transfer spectroscopy. Nanosecond emission anisotropy of fluoresence-labeled severin shows that this protein changes its conformation on binding Ca2+. Actin filaments are rapidly fragmented on addition of severin and Ca2+, but severin does not interact with actin filaments in the absence of Ca2+. Fluorescence energy transfer measurements indicate that fragmentation of actin filaments by severin leads to a partial depolymerization (t1/2 approximately equal to 30 s). Depolymerization is followed by exchange of a limited number of subunits in the filament fragments with the disassembled actin pool (t1/2 approximately equal to 5 min). Disassembly and exchange are probably restricted to the ends of the filament fragments since only a few subunits in each fragment participate in the disassembly or exchange process. Steady state hydrolysis of ATP by actin in the presence of Ca2+-severin is maximal at an actin: severin molar ratio of approximately 10:1, which further supports the inference that subunit exchange is limited to the ends of actin filaments. The observation of sequential depolymerization and subunit exchange following the fragmentation of actin by severin suggests that severin may regulate site-specific disassembly and turnover of actin filament arrays in vivo.     

Ca(2+)-dependent, myosin subfragment 1-induced proximity changes between actin and the inhibitory region of troponin I.

In order to help understand the spatial rearrangements of thin filament proteins during the regulation of muscle contraction, we used fluorescence resonance energy transfer (FRET) to measure Ca(2+)-dependent, myosin-induced changes in distances and fluorescence energy transfer efficiencies between actin and the inhibitory region of troponin I (TnI). We labeled the single Cys-117 of a mutant TnI with N-(iodoacetyl)-N'-(1-sulfo-5-naphthyl)ethylenediamine (IAEDANS) and Cys-374 of actin with 4-dimethylaminophenylazophenyl-4'-maleimide (DABmal). These fluorescent probes were used as donor and acceptor, respectively, for the FRET measurements. We reconstituted a troponin-tropomyosin (Tn-Tm) complex which contained the AEDANS-labeled mutant TnI, together with natural troponin T (TnT), troponin C (TnC) and tropomyosin (Tm) from rabbit fast skeletal muscle. Fluorescence titration of the AEDANS-labeled Tn-Tm complex with DABmal-labeled actin, in the presence and absence of Ca(2+), resulted in proportional, linear increases in energy transfer efficiency up to a 7:1 molar excess of actin over Tn-Tm. The distance between AEDANS on TnI Cys-117 and DABmal on actin Cys-374 increased from 37.9 A to 44.1 A when Ca(2+) bound to the regulatory sites of TnC. Titration of reconstituted thin filaments, containing AEDANS-labeled Tn-Tm and DABmal-labeled actin, with myosin subfragment 1 (S1) decreased the energy transfer efficiency, in both the presence and absence of Ca(2+). The maximum decrease occurred at well below stoichiometric levels of S1 binding to actin, showing a cooperative effect of S1 on the state of the thin filaments. S1:actin molar ratios of approximately 0.1 in the presence of Ca(2+), and approximately 0.3 in the absence of Ca(2+), were sufficient to cause a 50% reduction in normalized transfer efficiency. The distance between AEDANS on TnI Cys-117 and DABmal on actin Cys-374 increased by approximately 7 A in the presence of Ca(2+) and by approximately 2 A in the absence of Ca(2+) when S1 bound to actin. Our results suggest that TnI's interaction with actin inhibits actomyosin ATPase activity by modulating the equilibria among active and inactive states of the thin filament. Structural rearrangements caused by myosin S1 binding to the thin filament, as detected by FRET measurements, are consistent with the cooperative behavior of the thin filament proteins.     

Effect of tropomyosin on formin-bound actin filaments

Formins are conservative proteins with important roles in the regulation of the microfilament system in eukaryotic cells. Previous studies showed that the binding of formins to actin made the structure of actin filaments more flexible. Here, the effects of tropomyosin on formin-induced changes in actin filaments were investigated using fluorescence spectroscopic methods. The temperature dependence of the Förster-type resonance energy transfer showed that the formin-induced increase of flexibility of actin filaments was diminished by the binding of tropomyosin to actin. Fluorescence anisotropy decay measurements also revealed that the structure of flexible formin-bound actin filaments was stabilized by the binding of tropomyosin. The stabilizing effect reached its maximum when all binding sites on actin were occupied by tropomyosin. The effect of tropomyosin on actin filaments was independent of ionic strength, but became stronger as the magnesium concentration increased. Based on these observations, we propose that in cells there is a molecular mechanism in which tropomyosin binding to actin plays an important role in forming mechanically stable actin filaments, even in the case of formin-induced rapid filament assembly.     

Effects of PKA phosphorylation of cardiac troponin I and strong crossbridge on conformational transitions of the N-domain of cardiac troponin C in regulated thin filaments

Regulation of cardiac muscle function is initiated by binding of Ca2+ to troponin C (cTnC) which induces a series of structural changes in cTnC and other thin filament proteins. These structural changes are further modulated by crossbridge formation and fine-tuned by phosphorylation of cTnI. The objective of the present study is to use a new F?rster resonance energy transfer-based structural marker to distinguish structural and kinetic effects of Ca2+ binding, crossbridge interaction, and protein kinase A phosphorylation of cTnI on the conformational changes of the cTnC N-domain. The FRET-based structural marker was generated by attaching AEDANS to one cysteine of a double-cysteine mutant cTnC(13C/51C) as a FRET donor and attaching DDPM to the other cysteine as the acceptor. The doubly labeled cTnC mutant was reconstituted into the thin filament by adding cTnI, cTnT, tropomyosin, and actin. Changes in the distance between Cys13 and Cys51 induced by Ca2+ binding/dissociation were determined by FRET-sensed Ca2+ titration and stopped-flow studies, and time-resolved fluorescence measurements. The results showed that the presence of both Ca2+ and strong binding of myosin head to actin was required to achieve a fully open structure of the cTnC N-domain in regulated thin filaments. Equilibrium and stopped-flow studies suggested that strongly bound myosin head significantly increased the Ca2+ sensitivity and changed the kinetics of the structural transition of the cTnC N-domain. PKA phosphorylation of cTnI impacted the Ca2+ sensitivity and kinetics of the structural transition of the cTnC N-domain but showed no global structural effect on cTnC opening. These results provide an insight into the modulation mechanism of strong crossbridge and cTnI phosphorylation in cardiac thin filament activation/relaxation processes.     

Aggregation, lipid exchange, and metastable phases of dimyristoylphosphatidylethanolamine vesicles

A new fluorescent lipid analogue, bimanephosphatidylcholine, has been synthesized for use in lipid bilayers. This probe is well suited as an energy-transfer donor with N-(7-nitro-2,1,3-benzoxadiazol-4-yl)phosphatidylethanolamine as the acceptor. Dimyristoylphosphatidylethanolamine vesicles are prepared by sonication at pH 9 and characterized by electron microscopy and other methods. Resonance energy transfer between separately labeled donor and acceptor vesicles is monitored during HCl-induced aggregation to determine the kinetics of lipid randomization. Light scattering is also monitored to measure the kinetics of aggregation. The light scattering shows a marked reversal with NaOH while the energy transfer does not, indicating lipid exchange during a reversibly aggregated state; the extent of energy transfer suggests that only lipids in the outer monolayers exchange. The gel to liquid-crystalline phase transition temperature in HCl-treated vesicles is found to be 47 degrees C with diphenylhexatriene. The initial sonicated dispersion does not show a sharp phase transition. In vesicles labeled with both donor and acceptor probes, a small, irreversible increase in energy transfer is obtained upon lowering and then restoring the pH. These results suggest a metastable phase in the sonicated vesicles containing a randomized distribution of lipid and probes within the bilayers; the thermodynamically favored phase, whose formation is triggered by the pH shock, contains domains within which the probe lipids are more highly concentrated.     

Actin and myosin: control of filament assembly

Actin filaments, assembled from highly purified actin from either skeletal muscle or Dictyostelium amoebae, are very stable under physiological ionic conditions. A small and limited amount of exchange of actin filament subunits for unpolymerized actin or subunits in other filaments has been measured by three techniques: fluorescence energy transfer, incorporation of 35S-labelled actin monomers into unlabelled actin filaments, and exchange of [14C]ATP with filament-bound ADP. A 40 kDa protein purified from amoebae destabilizes these otherwise stable filaments in a Ca2+-dependent manner. Myosin purified from Dictyostelium amoebae is phosphorylated both in the tail region of the heavy chain and in one of the light chains. Phosphorylation appears to regulate myosin thick-filament formation.     

Cofilin tunes the nucleotide state of actin filaments and severs at bare and decorated segment boundaries

Actin-based motility demands the spatial and temporal coordination of numerous regulatory actin-binding proteins (ABPs), many of which bind with affinities that depend on the nucleotide state of actin filament. Cofilin, one of three ABPs that precisely choreograph actin assembly and organization into comet tails that drive motility in vitro, binds and stochastically severs aged ADP actin filament segments of de novo growing actin filaments. Deficiencies in methodologies to track in real time the nucleotide state of actin filaments, as well as cofilin severing, limit the molecular understanding of coupling between actin filament chemical and mechanical states and severing. We engineered a fluorescently labeled cofilin that retains actin filament binding and severing activities. Because cofilin binding depends strongly on the actin-bound nucleotide, direct visualization of fluorescent cofilin binding serves as a marker of the actin filament nucleotide state during assembly. Bound cofilin allosterically accelerates P(i) release from unoccupied filament subunits, which shortens the filament ATP/ADP-P(i) cap length by nearly an order of magnitude. Real-time visualization of filament severing indicates that fragmentation scales with and occurs preferentially at boundaries between bare and cofilin-decorated filament segments, thereby controlling the overall filament length, depending on cofilin binding density.     

Fluorescence energy transfer measurements between the nucleotide binding site and Cys-373 in actin and their application to the kinetics of actin polymerization

Intramonomer fluorescence energy transfer between the donor epsilon-ATP bound to the nucleotide-binding site and the acceptor 7-chloro-4-nitrobenzo-2-oxa-1,3-diazole bound to Cys-373 in G-actin was measured by steady-state fluorimetry. Assuming for the orientation factor its dynamic limit K2 = 2/3, the donor and acceptor distance in a G-actin molecule was calculated to be about 3 nm. The intermonomer energy transfer in F-actin occurring between the donor bound to an actin monomer and the acceptor bound to the nearest-neighbour actin monomer was also measured and the distance was calculated to be about 4 nm. The kinetics of the actin polymerization process was studied by following the decrease in fluorescence intensity upon addition of salts to G-actin solution. The initial velocity of the fluorescence intensity change was proportional to the square of the initial G-actin concentration. The temperature dependence of the velocity was proportional to the square of the initial G-actin concentration. The temperature dependence of the velocity was proportional to exp(-10/RT). These results indicated that the initial fluorescence intensity change corresponds to monomer-dimer transformation and its activation enthalpy was 10 kcal/mol.     

Polymerization and depolymerization of actin with nucleotide states at filament ends

Polymerization induces hydrolysis of ATP bound to actin, followed by γ-phosphate release, which helps advance the disassembly of actin filaments into ADP-G-actin. Mechanical understanding of this correlation between actin assembly and ATP hydrolysis has been an object of intensive studies in biochemistry and structural biology for many decades. Although actin polymerization and depolymerization occur only at either the barbed or pointed ends and the kinetic and equilibrium properties are substantially different from each other, characterizing their properties is difficult to do by bulk assays, as these assays report the average of all actin filaments in solution and are therefore not able to discern the properties of individual actin filaments. Biochemical studies of actin polymerization and hydrolysis were hampered by these inherent properties of actin filaments. Total internal reflection fluorescence (TIRF) microscopy overcame this problem by observing single actin filaments. With TIRF, we now know not only that each end has distinct properties, but also that the rate of γ-phosphate release is much faster from the terminals than from the interior of actin filaments. The rate of γ-phosphate release from actin filament ends is even more accelerated when latrunculin A is bound. These findings highlight the importance of resolving structural differences between actin molecules in the interior of the filament and those at either filament end. This review provides a history of observing actin filaments under light microscopy, an overview of dynamic properties of ATP hydrolysis at the end of actin filament, and structural views of γ-phosphate release.     

Fluorescence resonance energy transfer between points on actin and the C-terminal region of tropomyosin in skeletal muscle thin filaments

Fluorescence resonance energy transfer between points on tropomyosin (positions 87 and 190) and actin (Gln-41, Lys-61, Cys-374, and the ATP-binding site) showed no positional change of tropomyosin relative to actin on the thin filament in response to changes in Ca2+ concentration (Miki et al. (1998) J. Biochem. 123, 1104-1111). This is consistent with recent electron cryo-microscopy analysis, which showed that the C-terminal one-third of tropomyosin shifted significantly towards the outer domain of actin, while the N-terminal half of tropomyosin shifted only a little (Narita et al. (2001) J. Mol. Biol. 308, 241-261). In order to detect any significant positional change of the C-terminal region of tropomyosin relative to actin, we generated mutant tropomyosin molecules with a unique cysteine residue at position 237, 245, 247, or 252 in the C-terminal region. The energy donor probe was attached to these positions on tropomyosin and the acceptor probe was attached to Cys-374 or Gln-41 of actin. These probe-labeled mutant tropomyosin molecules retain the ability to regulate the acto-S1 ATPase activity in conjunction with troponin and Ca2+. Fluorescence resonance energy transfer between these points of tropomyosin and actin showed a high transfer efficiency, which should be very sensitive to changes in distance between probes attached to actin and tropomyosin. However, the transfer efficiency did not change appreciably upon removal of Ca2+ ions, suggesting that the C-terminal region of tropomyosin did not shift significantly relative to actin on the reconstituted thin filament in response to the change of Ca2+ concentration.     

A Highlights from MBoC Selection: Dynamic actin filaments control the mechanical behavior of the human red blood cell membrane

Short, uniform-length actin filaments function as structural nodes in the spectrin-actin membrane skeleton to optimize the biomechanical properties of red blood cells (RBCs). Despite the widespread assumption that RBC actin filaments are not dynamic (i.e., do not exchange subunits with G-actin in the cytosol), this assumption has never been rigorously tested. Here we show that a subpopulation of human RBC actin filaments is indeed dynamic, based on rhodamine-actin incorporation into filaments in resealed ghosts and fluorescence recovery after photobleaching (FRAP) analysis of actin filament mobility in intact RBCs (∼25–30% of total filaments). Cytochalasin-D inhibition of barbed-end exchange reduces rhodamine-actin incorporation and partially attenuates FRAP recovery, indicating functional interaction between actin subunit turnover at the single-filament level and mobility at the membrane-skeleton level. Moreover, perturbation of RBC actin filament assembly/disassembly with latrunculin-A or jasplakinolide induces an approximately twofold increase or ∼60% decrease, respectively, in soluble actin, resulting in altered membrane deformability, as determined by alterations in RBC transit time in a microfluidic channel assay, as well as by abnormalities in spontaneous membrane oscillations (flickering). These experiments identify a heretofore-unrecognized but functionally important subpopulation of RBC actin filaments, whose properties and architecture directly control the biomechanical properties of the RBC membrane.     

Origin of Twist-Bend Coupling in Actin Filaments

Actin filaments are semiflexible polymers that display large-scale conformational twisting and bending motions. Modulation of filament bending and twisting dynamics has been linked to regulatory actin-binding protein function, filament assembly and fragmentation, and overall cell motility. The relationship between actin filament bending and twisting dynamics has not been evaluated. The numerical and analytical experiments presented here reveal that actin filaments have a strong intrinsic twist-bend coupling that obligates the reciprocal interconversion of bending energy and twisting stress. We developed a mesoscopic model of actin filaments that captures key documented features, including the subunit dimensions, interaction energies, helicity, and geometrical constraints coming from the double-stranded structure. The filament bending and torsional rigidities predicted by the model are comparable to experimental values, demonstrating the capacity of the model to assess the mechanical properties of actin filaments, including the coupling between twisting and bending motions. The predicted actin filament twist-bend coupling is strong, with a persistence length of 0.15-0.4 μm depending on the actin-bound nucleotide. Twist-bend coupling is an emergent property that introduces local asymmetry to actin filaments and contributes to their overall elasticity. Up to 60% of the filament subunit elastic free energy originates from twist-bend coupling, with the largest contributions resulting under relatively small deformations. A comparison of filaments with different architectures indicates that twist-bend coupling in actin filaments originates from their double protofilament and helical structure.