A-to-I RNA editing of Filamin A regulates cellular adhesion, migration and mechanical properties.

A-to-I RNA editing by ADARs is an abundant epitranscriptomic RNA-modification in metazoa. In mammals, Flna pre-mRNA harbours a single conserved A-to-I RNA editing site that introduces a Q-to-R amino acid change in Ig repeat 22 of the encoded protein. Previously, we showed that FLNA editing regulates smooth muscle contraction in the cardiovascular system and affects cardiac health. The present study investigates how ADAR2-mediated A-to-I RNA editing of Flna affects actin crosslinking, cell mechanics, cellular adhesion and cell migration. Cellular assays and AFM measurements demonstrate that the edited version of FLNA increases cellular stiffness and adhesion but impairs cell migration in both, mouse fibroblasts and human tumour cells. In vitro, edited FLNA leads to increased actin crosslinking, forming actin gels of higher stress resistance. Our study shows that Flna RNA editing is a novel regulator of cytoskeletal organisation, affecting the mechanical property and mechanotransduction of cells.

Comparison between 102k and 20k Poly(ethylene oxide) Depletants in Osmotic Pressure Measurements of Interfilament Forces in Cytoskeletal Systems.

The proliferation of successful, cell-free reconstitutions of cytoskeletal networks have prompted measurements of forces between network elements via induced osmotic pressure by the addition of depletants. Indeed, it was through osmotic pressurization that Tau, an intrinsically disordered protein found in neuronal axons, was recently discovered to mediate two distinct microtubule (MT) bundle states, one widely spaced and a second tightly packed, separated by an energy barrier due to polyelectrolyte repulsions between opposing Tau projection domains on neighboring MT surfaces. Here, we compare interfilament force measurements in Tau coated MT bundles using PEO20k (poly(ethylene oxide), Mw = 20000), a commonly used inert depletant, and recently published measurements with PEO102k. While force measurements with either depletant reveals the transition between the two bundled states, measurements with PEO20k cannot recapitulate the correct critical pressure (Pc) at which widely spaced MT bundles transition to tightly packed MT bundles due to depletant penetration into widely spaced bundles below Pc. Surprisingly, upon transitioning to the tightly packed bundle state data from both depletants are in quantitative agreement indicative of expulsion of the smaller PEO20k depletant, but only at distances comparable or less than the PEO20k radius of gyration, significantly smaller than the effective diameter of PEO20k. While PEO102k (with size larger than the wall-to-wall distance between MTs in bundles) can more accurately capture the force response behavior at low to intermediate pressures (<104 Pa), measurements with PEO20k, beyond the overlap regime with PEO102k, extend the achievable osmotic pressure range into the higher-pressure regime (∼5 × 104 Pa). The data underscores the importance of the use of polymeric depletants of different sizes to elucidate force response behavior of cytoskeletal filamentous networks over a more complete extended pressure range.

Tau mediates microtubule bundle architectures mimicking fascicles of microtubules found in the axon initial segment.

Tau, an intrinsically disordered protein confined to neuronal axons, binds to and regulates microtubule dynamics. Although there have been observations of string-like microtubule fascicles in the axon initial segment (AIS) and hexagonal bundles in neurite-like processes in non-neuronal cells overexpressing Tau, cell-free reconstitutions have not replicated either geometry. Here we map out the energy landscape of Tau-mediated, GTP-dependent 'active' microtubule bundles at 37 °C, as revealed by synchrotron SAXS and TEM. Widely spaced bundles (wall-to-wall distance Dw-w≈25-41 nm) with hexagonal and string-like symmetry are observed, the latter mimicking bundles found in the AIS. A second energy minimum (Dw-w≈16-23 nm) is revealed under osmotic pressure. The wide spacing results from a balance between repulsive forces, due to Tau's projection domain (PD), and a stabilizing sum of transient sub-kBT cationic/anionic charge-charge attractions mediated by weakly penetrating opposing PDs. This landscape would be significantly affected by charge-altering modifications of Tau associated with neurodegeneration.

Mechanics of soft epithelial keratin networks depend on modular filament assembly kinetics.

UNLABELLED: Structural adaptability is a pivotal requirement of cytoskeletal structures, enabling their reorganization to meet the cellular needs. Shear stress, for instance, results in large morphological network changes of the human soft epithelial keratin pair K8:K18, and is accompanied by an increase in keratin phosphorylation levels. Yet the mechanisms responsible for the disruption of the network structure in vivo remain poorly understood. To understand the effect of the stress-related site-specific phosphorylation of the K8:K18 pair, we created phosphomimicry mutants - K8(S431E), K8(S73E), K18(S52E) - in vitro, and investigated the various steps of keratin assembly from monomer to network structure using fluorescence and electron microscopy, and using rheology characterized their network mechanical properties. We find that the addition of a charged group produces networks with depleted intra-connectivity, which translates to a mechanically weaker and more deformable network. This large variation in network structure is achieved by the formation of shorter mutant filaments, which exhibit differing assembly kinetics and a manifestly reduced capacity to form the extended structures characteristic of the wild-type system. The similarity in outcome for all the phosphomimicry mutants explored points to a more general mechanism of structural modulation of intermediate filaments via phosphorylation. Understanding the role of kinetic effects in the construction of these cytoskeletal biopolymer networks is critical to elucidating their structure-function properties, providing new insight for the design of keratin-inspired biomaterials. STATEMENT OF SIGNIFICANCE: Structural remodeling of cytoskeletal networks accompanies many cellular processes. Interestingly, levels of phosphorylation of the human soft epithelial keratin pair K8:K18 increase during their stress-related structural remodeling. Our multi-scale study sheds light on the poorly understood mechanism with which site-specific phosphorylation induces disruption of the keratin network structure in vivo. We show how phosphorylation reduces keratin filament length, an effect that propagates through to the mesoscopic structure, resulting in the formation of connectivity-depleted and mechanically weaker networks. We determine that the intrinsically-set filament-to-filament attractions that drive bundle assembly give rise to the structural variability by enabling the formation of kinetically-arrested structures. Overall, our results shed light on how self-assembled intermediate filament structures can be tailored to exhibit different structural functionalities.

Neurofilament networks: Salt-responsive hydrogels with sidearm-dependent phase behavior.

BACKGROUND: Neurofilaments (NFs) - the neuron-specific intermediate filament proteins - are assembled into 10nm wide filaments in a tightly controlled ratio of three different monomer types: NF-Low (NF-L), NF-Medium (NF-M), and NF-High (NF-H). Previous work on reconstituted bovine NF hydrogels has shown the dependence of network properties, including filament alignment and spacing, on the subunit composition. METHODS: We use polarized optical microscopy and SAXS to explore the full salt-dependent phase behavior of reconstituted bovine NF networks as a function of various binary and ternary subunit ratios. RESULTS: We observe three salt-induced liquid crystalline phases: the liquid-ordered B(G) and N(G) phases, and the disordered I(G) phase. We note the emergent sidearm roles, particularly that of NF-H in driving the parallel to cross-filament transition, and the counter-role of NF-M in suppressing the I(G) phase. CONCLUSIONS: In copolymers of NF-LH, NF-H shifts the I(G) to N(G) transition to nearer physiological salt concentrations, as compared to NF-M in copolymers of NF-LM. For ternary mixtures, the role of NF-H is modulated by the ratio of NF-M, where beneath 10wt.% NF-M, NF-H drives the transition to the disordered phase, and above which NF-H increases interfilament spacing. GENERAL SIGNIFICANCE: Understanding the role of individual subunits in regulating the network structure will enable us to understand the mechanisms that drive the dysfunction of these networks, as observed in diseased conditions.

Neurofilament sidearms modulate parallel and crossed-filament orientations inducing nematic to isotropic and re-entrant birefringent hydrogels.

Neurofilaments are intermediate filaments assembled from the subunits neurofilament-low, neurofilament-medium and neurofilament-high. In axons, parallel neurofilaments form a nematic liquid-crystal hydrogel with network structure arising from interactions between the neurofilaments' C-terminal sidearms. Here we report, using small-angle X-ray-scattering, polarized-microscopy and rheometry, that with decreasing ionic strength, neurofilament-low-high, neurofilament-low-medium and neurofilament-low-medium-high hydrogels transition from the nematic hydrogel to an isotropic hydrogel (with random, crossed-filament orientation) and to an unexpected new re-entrant liquid-crystal hydrogel with parallel filaments--the bluish-opaque hydrogel--with notable mechanical and water retention properties reminiscent of crosslinked hydrogels. Significantly, the isotropic gel phase stability is sidearm-dependent: neurofilament-low-high hydrogels exhibit a wide ionic strength range, neurofilament-low-medium hydrogels a narrow ionic strength range, whereas neurofilament-low hydrogels lack the isotropic gel phase. This suggests a dominant regulatory role for neurofilament-high sidearms in filament reorientation plasticity, facilitating organelle transport in axons. Neurofilament-inspired biomimetic hydrogels should therefore exhibit remarkable structure-dependent moduli and slow and fast water-release properties.

Liquid crystal assemblies in biologically inspired systems.

In this paper, which is part of a collection in honor of Noel Clark's remarkable career on liquid crystal and soft matter research, we present examples of biologically inspired systems, which form liquid crystal (LC) phases with their LC nature impacting biological function in cells or being important in biomedical applications. One area focuses on understanding network and bundle formation of cytoskeletal polyampholytes (filamentous-actin, microtubules, and neurofilaments). Here, we describe studies on neurofilaments (NFs), the intermediate filaments of neurons, which form open network nematic liquid crystal hydrogels in axons. Synchrotron small-angle-x-ray scattering studies of NF-protein dilution experiments and NF hydrogels subjected to osmotic stress show that neurofilament networks are stabilized by competing long-range repulsion and attractions mediated by the neurofilament's polyampholytic sidearms. The attractions are present both at very large interfilament spacings, in the weak sidearm-interpenetrating regime, and at smaller interfilament spacings, in the strong sidearm-interpenetrating regime. A second series of experiments will describe the structure and properties of cationic liposomes (CLs) complexed with nucleic acids (NAs). CL-NA complexes form liquid crystalline phases, which interact in a structure-dependent manner with cellular membranes enabling the design of complexes for efficient delivery of nucleic acid (DNA, RNA) in therapeutic applications.

Structures and interactions in 'bottlebrush' neurofilaments: the role of charged disordered proteins in forming hydrogel networks.

NFs (neurofilaments), the major cytoskeletal constituent of myelinated axons in vertebrates, consist of three different molecular-mass subunit proteins, NF-L (low), NF-M (medium) and NF-H (high), assembled to form mature filaments with protruding intrinsically disordered C-terminal side-arms. Liquid crystal gel networks of side-arm-mediated NF assemblies play a key role in the mechanical stability of neuronal processes. Disruptions of the NF network, due to NF overaccumulation or incorrect side-arm interactions, are a hallmark of motor neuron diseases including amyotrophic lateral sclerosis. Using synchrotron small-angle X-ray scattering and various microscopy techniques, we have investigated the role of the peptide charges in the subunit side-arms on the structure and interaction of NFs. Our findings, which delineate the distinct roles of NF-M and NF-H in regulating NF interactions, shed light on possible mechanisms of disruption of optimal mechanical network properties.

Unconventional salt trend from soft to stiff in single neurofilament biopolymers.

We present persistence length measurements on neurofilaments (NFs), an intermediate filament with protruding side arms, of the neuronal cytoskeleton. Tapping mode atomic force microscopy enabled us to visualize and trace at subpixel resolution photoimmobilized NFs, assembled at various subunit protein ratios, thereby modifying the side-arm length and chain density charge distribution. We show that specific polyampholyte sequences of the side arms can form salt-switchable intrafilament attractions that compete with the net electrostatic and steric repulsion and can reduce the total persistence length by half. The results are in agreement with present X-ray and microscopy data yet present a theoretical challenge for polyampholyte interchain interactions.

Gel-expanded to gel-condensed transition in neurofilament networks revealed by direct force measurements.

Neurofilaments (NF)--the principal cytoskeletal constituent of myelinated axons in vertebrates--consist of three molecular-weight subunit proteins NF-L (low), NF-M (medium) and NF-H (high), assembled to form mature filaments with protruding unstructured C-terminus side arms. Liquid-crystal gel networks of side-arm-mediated neurofilament assemblies have a key role in the mechanical stability of neuronal processes. Disruptions of the neurofilament network, owing to neurofilament over-accumulation or incorrect side-arm interactions, are a hallmark of motor-neuron diseases including amyotrophic lateral sclerosis. Using synchrotron X-ray scattering, we report on a direct measurement of forces in reconstituted neurofilament gels under osmotic pressure (P). With increasing pressure near physiological salt and average phosphorylation conditions, NF-LMH, comprising the three subunits near in vivo composition, or NF-LH gels, undergo for P > P(c) approximately 10 kPa, an abrupt non-reversible gel-expanded to gel-condensed transition. The transition indicates side-arm-mediated attractions between neurofilaments consistent with an electrostatic model of interpenetrating chains. In contrast, NF-LM gels remain in a collapsed state for P < P(c) and transition to the gel-condensed state at P > P(c). These findings, which delineate the distinct roles of NF-M and NF-H in regulating neurofilament interactions, shed light on possible mechanisms for disruptions of optimal mechanical network properties.