Abstract:The distribution of spectrin and band 3 in deoxygenated reversibly sickled cells was visualized by immunofluorescence and immunoelectron microscopy. Antibodies against band 3, the major lipid-associated transmembrane protein, labeled the entire cell body, including the entire length of the long protruding spicule, whereas antibodies against spectrin labeled only the cell body and the base region of the spicules. The results suggest that the formation of long spicules during sickling is associated with a contin… Show more
“…In other words, integral proteins are torn out and dragged into the tube upon extrusion. Although never observed directly in tethers, such a phenomenon has already been evidenced in RBC vesiculation (25) and in membrane spicules of sickled RBCs (26). The description of the slipping contribution to the dynamics of tether growth is beyond the scope of the present paper.…”
Section: Proposed Reinterpretation Of Experimental Resultsmentioning
We discuss the pulling force f required to extrude a lipid tube from a living cell as a function of the extrusion velocity L . The main feature is membrane friction on the cytoskeleton. As recently observed for neutrophils, the tether force exhibits a ''shear thinning'' response over a large range of pulling velocities, which was previously interpreted by assuming viscoelastic flows of the sliding membrane. Here, we propose an alternative explanation based on purely Newtonian flow: The diameter of the tether decreases concomitantly with the increase of the membrane tension in the lipid tube. The pulling force is found to vary as L 1/3 , which is consistent with reported experimental data for various types of cells.cytoskeleton ͉ dynamics ͉ membrane tethers M any cellular processes [such as intracellular trafficking (1) or intercellular organelle transport (2)] involve the formation of thin tubular structures known as tethers. Membranous tails also are observed to be left by migrating cells in culture dishes (3). Tethers can be extracted from synthetic vesicles or living cells by the application of an external point force [using a fluid drag (4, 5) or pipette-tweezer system (6, 7)]. In the case of living cells, where the lipidic membrane is coupled to a cytoskeleton, tethers can be used as membrane sensors to measure the membrane-cytoskeleton adhesion energy W 0 (8-12).Our aim here is to describe the formation of a tether and to derive the required pulling force as a function of the extrusion velocity. Pulling a tube from a cell membrane implies a surface flow of lipid from the cell body to the tether through the membranecytoskeleton binders. This viscous drag gives rise to an increase of the membrane tension in the tube and a decrease of its radius.
Statics of ExtrusionWe follow the thermodynamic analysis of tether formation proposed by Waugh and coworkers (7,13,14), Evans and Yeung (15), and Derényi and coworkers (16) for lipidic bilayers and extended to cell membranes by Sheetz and coworkers (10, 12). As shown in Fig. 1, the cell is usually held by micropipette suction (pressure Ϫ⌬P) that sets the membrane tension of the cell : 2 Ӎ R p ⌬P, where R p is the radius of the micropipette. The length of the tongue in the pipette is L p . Another case of experimental interest is found when cells are spread onto an adhesive surface, which ensures that the membrane tension remains weak or constant during the time course of the experiment. The tube is then either extruded by pulling out a small bead adhering to the membrane via micromanipulation if the cell is firmly adhered or, more simply, by applying a hydrodynamic flow over the cell in case of a discrete and sparse adhesion site. The length of the tube is L, the membrane tension of the tube is t , and its radius is r t . We want to relate r t and t to , the tension of the cell body, and to W 0 , the adhesion energy of the membrane to the cytoskeleton. The pulling force f 0 is deduced from the following four equations.
The distribution of areas:2 r t dL ϭ 2 R p dL p...
“…In other words, integral proteins are torn out and dragged into the tube upon extrusion. Although never observed directly in tethers, such a phenomenon has already been evidenced in RBC vesiculation (25) and in membrane spicules of sickled RBCs (26). The description of the slipping contribution to the dynamics of tether growth is beyond the scope of the present paper.…”
Section: Proposed Reinterpretation Of Experimental Resultsmentioning
We discuss the pulling force f required to extrude a lipid tube from a living cell as a function of the extrusion velocity L . The main feature is membrane friction on the cytoskeleton. As recently observed for neutrophils, the tether force exhibits a ''shear thinning'' response over a large range of pulling velocities, which was previously interpreted by assuming viscoelastic flows of the sliding membrane. Here, we propose an alternative explanation based on purely Newtonian flow: The diameter of the tether decreases concomitantly with the increase of the membrane tension in the lipid tube. The pulling force is found to vary as L 1/3 , which is consistent with reported experimental data for various types of cells.cytoskeleton ͉ dynamics ͉ membrane tethers M any cellular processes [such as intracellular trafficking (1) or intercellular organelle transport (2)] involve the formation of thin tubular structures known as tethers. Membranous tails also are observed to be left by migrating cells in culture dishes (3). Tethers can be extracted from synthetic vesicles or living cells by the application of an external point force [using a fluid drag (4, 5) or pipette-tweezer system (6, 7)]. In the case of living cells, where the lipidic membrane is coupled to a cytoskeleton, tethers can be used as membrane sensors to measure the membrane-cytoskeleton adhesion energy W 0 (8-12).Our aim here is to describe the formation of a tether and to derive the required pulling force as a function of the extrusion velocity. Pulling a tube from a cell membrane implies a surface flow of lipid from the cell body to the tether through the membranecytoskeleton binders. This viscous drag gives rise to an increase of the membrane tension in the tube and a decrease of its radius.
Statics of ExtrusionWe follow the thermodynamic analysis of tether formation proposed by Waugh and coworkers (7,13,14), Evans and Yeung (15), and Derényi and coworkers (16) for lipidic bilayers and extended to cell membranes by Sheetz and coworkers (10, 12). As shown in Fig. 1, the cell is usually held by micropipette suction (pressure Ϫ⌬P) that sets the membrane tension of the cell : 2 Ӎ R p ⌬P, where R p is the radius of the micropipette. The length of the tongue in the pipette is L p . Another case of experimental interest is found when cells are spread onto an adhesive surface, which ensures that the membrane tension remains weak or constant during the time course of the experiment. The tube is then either extruded by pulling out a small bead adhering to the membrane via micromanipulation if the cell is firmly adhered or, more simply, by applying a hydrodynamic flow over the cell in case of a discrete and sparse adhesion site. The length of the tube is L, the membrane tension of the tube is t , and its radius is r t . We want to relate r t and t to , the tension of the cell body, and to W 0 , the adhesion energy of the membrane to the cytoskeleton. The pulling force f 0 is deduced from the following four equations.
The distribution of areas:2 r t dL ϭ 2 R p dL p...
“…For example, it has been hypothesized that the pathogenesis of hereditary spherocytosis is related to the weakened bilayercytoskeletal interaction strength, which leads to reduced spectrin density, and the loss of bilayer membrane resulting in reduced surface area (4). In addition, in sickle cell disease, the detachment of the RBC lipid bilayer from the spectrin network owing to hemoglobin polymerization also causes "budding off" of the bilayer, which in turn results in reduced cell deformability (1). Furthermore, when the RBCs pass through the interendothelial slits in the spleen, they undergo severe deformation.…”
mentioning
confidence: 99%
“…Under normal conditions, the cytoskeleton is tightly attached to the lipid bilayer from the cytoplasmic side. However, under certain pathological conditions, e.g., in sickle cell disease, the cytoskeleton may become dissociated from the lipid bilayer (1). Although the biomechanics of the two-component erythrocyte membrane have been studied extensively for decades (2), the mechanical properties of the interactions between the lipid bilayer and the cytoskeleton (such as elastic stiffness, viscous friction, and strength) via the pinning connections of transmembrane proteins are still largely unknown.…”
mentioning
confidence: 99%
“…The potential of the RBC membrane including these two different components is written as U = U s + U b + U a+v + U int ; [1] where U s is the spectrin's potential energy from the cytoskeleton, U b is the bending energy from the lipid bilayer, U a+v corresponds to the area and volume conservation constraints from the lipid bilayer, and U int is the potential energy of the interaction between the lipid bilayer and the cytoskeleton. The detailed expressions of U s , U b , and U a+v can be found in SI Text.…”
We study the biomechanical interactions between the lipid bilayer and the cytoskeleton in a red blood cell (RBC) by developing a general framework for mesoscopic simulations. We treated the lipid bilayer and the cytoskeleton as two distinct components and developed a unique whole-cell model of the RBC, using dissipative particle dynamics (DPD). The model is validated by comparing the predicted results with measurements from four different and independent experiments. First, we simulated the micropipette aspiration and quantified the cytoskeletal deformation. Second, we studied the membrane fluctuations of healthy RBCs and RBCs parasitized to different intraerythrocytic stages by the malaria-inducing parasite Plasmodium falciparum. Third, we subjected the RBC to shear flow and investigated the dependence of its tank-treading frequency on shear rate. Finally, we simulated the bilayer-cytoskeletal detachment in channel flow to quantify the strength of such interactions when the corresponding bonds break. Taken together, these experiments and corresponding systematic DPD simulations probe the governing constitutive response of the cytoskeleton, elastic stiffness, viscous friction, and strength of bilayer-cytoskeletal interactions as well as membrane viscosities. Hence, the DPD simulations and comparisons with available independent experiments serve as validation of the unique two-component model and lead to useful insights into the biomechanical interactions between the lipid bilayer and the cytoskeleton of the RBC. Furthermore, they provide a basis for further studies to probe cell mechanistic processes in health and disease in a manner that guides the design and interpretation of experiments and to develop simulations of phenomena that cannot be studied systematically by experiments alone.coarse graining | worm-like chain | multiscale modeling | adhesion energy | erythrocyte T he red blood cell (RBC) membrane consists of two components: a lipid bilayer and an attached 2D spectrin network that acts as the cytoskeleton. The resistance of the lipid bilayer to bending is controlled by the bending rigidity, k c , whereas the spectrin network's resistance to shear strain is characterized by the in-plane shear modulus, μ s . Under normal conditions, the cytoskeleton is tightly attached to the lipid bilayer from the cytoplasmic side. However, under certain pathological conditions, e.g., in sickle cell disease, the cytoskeleton may become dissociated from the lipid bilayer (1). Although the biomechanics of the two-component erythrocyte membrane have been studied extensively for decades (2), the mechanical properties of the interactions between the lipid bilayer and the cytoskeleton (such as elastic stiffness, viscous friction, and strength) via the pinning connections of transmembrane proteins are still largely unknown. This is at least in part ascribed to the fact that it is difficult to measure these interactions directly from experiments, because the length scale of these connections is too small compared with the chara...
“…In animal cells, the spectrin-based membrane skeleton (MS) is a topographically distinct cytoskeletal structure which, depending on the cell type, can be physically related to various other intercellular cytoskeletal systems [4,.5]. The MS is known to interact with various cytoplasmic and membrane proteins [6,7]. For example, spectrin, the major component of the MS binds to actin, a process which may be mediated by a minor MS protein now referred to as adducin [S].…”
Section: Introduction 2 Materials and Methodsmentioning
Electrophoretic analysis of low ionic strength extracts of tomato plant leaves revealed the presence of two proteins of apparent molecular weights of 240 kDa and 220 kDa which co-migrated with purified human erythrocyte a-and /I-spectrin subunits. Immunochemical analyses employing an affinity-purified polyclonal antibody to human erythrocyte /?-spectrin reacted specifically with the 220 kDa plant cell protein. Immunofluoresccncc microscopy indicated that the ,/?-spectrin antibody recognized an antigen which was primarily restricted to the peripheral areas of the cells. Collectively, these results suggest that the cells of higher plants contain polypeptides related to the spectrin family of proteins. It is proposed that the plant cell possesses a membrane skeleton which is structurally and perhaps functionally analogous to that of the animal cell.
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