Abstract:Plasma membranes are subject to continuous deformations. Strikingly, some of these transient membrane undulations yield membrane-associated signaling hubs that differ in composition and function, depending on membrane geometry and the availability of co-factors. Here, recent advancements on this ubiquitous type of receptor-independent signaling are reviewed, with a special focus on emerging concepts and technical challenges associated with studying these elusive signaling sites.
“…The burst in actin polymerization at the evaginated PM and the simultaneous reattachment to the cortex suggest that the local topography generated by compression may act as the mechanical input triggering the subsequent polymerization event. Indeed, membrane curvature can recruit different signaling molecules (19,(34)(35)(36)(37), chief among them curvature-sensing BAR proteins (38)(39)(40)(41). The superfamily of BAR proteins includes molecules containing different curvature sensing and generating BAR domains: The N-BAR and F-BAR domains, which interact with positively curved membranes (invaginations), and the I-BAR domain for the opposite type of curvature (negatively curved membranes or evaginations).…”
As cells migrate and experience forces from their surroundings, they constantly undergo mechanical deformations which reshape their plasma membrane (PM). To maintain homeostasis, cells need to detect and restore such changes, not only in terms of overall PM area and tension as previously described, but also in terms of local, nano-scale topography. Here we describe a novel phenomenon, by which cells sense and restore mechanically induced PM nano-scale deformations. We show that cell stretch and subsequent compression reshape the PM in a way that generates local membrane evaginations in the 100 nm scale. These evaginations are recognized by the I-BAR protein IRSp53, which triggers a burst of actin polymerization mediated by Rac1 and Arp2/3. The actin polymerization burst subsequently re-flattens the evagination, completing the mechanochemical feedback loop. Our results demonstrate a new mechanosensing mechanism for PM shape homeostasis, with potential applicability in different physiological scenarios.
“…The burst in actin polymerization at the evaginated PM and the simultaneous reattachment to the cortex suggest that the local topography generated by compression may act as the mechanical input triggering the subsequent polymerization event. Indeed, membrane curvature can recruit different signaling molecules (19,(34)(35)(36)(37), chief among them curvature-sensing BAR proteins (38)(39)(40)(41). The superfamily of BAR proteins includes molecules containing different curvature sensing and generating BAR domains: The N-BAR and F-BAR domains, which interact with positively curved membranes (invaginations), and the I-BAR domain for the opposite type of curvature (negatively curved membranes or evaginations).…”
As cells migrate and experience forces from their surroundings, they constantly undergo mechanical deformations which reshape their plasma membrane (PM). To maintain homeostasis, cells need to detect and restore such changes, not only in terms of overall PM area and tension as previously described, but also in terms of local, nano-scale topography. Here we describe a novel phenomenon, by which cells sense and restore mechanically induced PM nano-scale deformations. We show that cell stretch and subsequent compression reshape the PM in a way that generates local membrane evaginations in the 100 nm scale. These evaginations are recognized by the I-BAR protein IRSp53, which triggers a burst of actin polymerization mediated by Rac1 and Arp2/3. The actin polymerization burst subsequently re-flattens the evagination, completing the mechanochemical feedback loop. Our results demonstrate a new mechanosensing mechanism for PM shape homeostasis, with potential applicability in different physiological scenarios.
“…This principle was first identified for the case of STxB and represents an example of a broader mechanism whereby lectins generate membrane curvature to drive endocytosis by binding to multiple glycolipids or glycoproteins (the GL-Lect hypothesis) [ 146 ]. Membrane curvature created by the extracellular CTxB could potentially lead to the recruitment of intracellular curvature-sensing proteins, in turn controlling the local membrane composition [ 147 , 148 ]. However, CTxB mutants capable of binding to only a single copy of GM1 can sort into preformed clathrin-independent endocytic structures, suggesting glycolipid clustering-induced curvature generation is dispensable for its uptake into at least a subset of CIE carriers [ 141 ].…”
Section: Ctxb As a Reporter Of Clathrin-independent Endocytosismentioning
Cholera toxin B-subunit (CTxB) has emerged as one of the most widely utilized tools in membrane biology and biophysics. CTxB is a homopentameric stable protein that binds tightly to up to five GM1 glycosphingolipids. This provides a robust and tractable model for exploring membrane structure and its dynamics including vesicular trafficking and nanodomain assembly. Here, we review important advances in these fields enabled by use of CTxB and its lipid receptor GM1.
“…2.2 in Box 1 ). Adding hydrophobic heads with varying size further renders lipids curvature-sensitive, while differences in charge will influence protein-lipid interactions with peripheral cytosolic proteins ( Ebrahimkutty and Galic, 2019 ; Bassereau et al, 2018 ). The bending stiffness of the cell cortex, which is relevant in the μm regime, can be influenced by changes to the actin mesh size (depicted by the density of cortex linker proteins) or the thickness of the cortex itself.…”
Section: Engineering a Hypothetical Biomimetic Membranementioning
Cellular membranes belong to the most vital yet least understood biomaterials of live matter. For instance, its biomechanical requirements substantially vary across species and subcellular sites, raising the question how membranes manage to adjust to such dramatic changes. Central to its adaptability at the cell surface is the interplay between the plasma membrane and the adjacent cell cortex, forming an adaptive composite material that dynamically adjusts its mechanical properties. Using a hypothetical composite material, we identify core challenges, and discuss how cellular membranes solved these tasks. We further muse how pathological changes in material properties affect membrane mechanics and cell function, before closing with open questions and future challenges arising when studying cellular membranes.
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