Abstract:Changes in the cytoskeletal organization within cells can be characterized by large spatial and temporal variations in rheological properties of the cell (e.g., the complex shear modulus G). Although the ensemble variation in G of single cells has been elucidated, the detailed temporal variation of G remains unknown. In this study, we investigated how the rheological properties of individual fibroblast cells change under a spatially confined environment in which the cell translational motion is highly restrict… Show more
“…Previous studies have reported that the number distribution of cell mechanical properties exhibits a large variation in single cells 41 , 42 and the cell stiffness and tension are very broadly varied over a long intercellular distance in a cell monolayer 43 – 46 . In contrast, the embryonic cells in the vegetal hemisphere exhibited broad spatiotemporal heterogeneity occurring at the single-cell level.…”
During the developmental processes of embryos, cells undergo massive deformation and division that are regulated by mechanical cues. However, little is known about how embryonic cells change their mechanical properties during different cleavage stages. Here, using atomic force microscopy, we investigated the stiffness of cells in ascidian embryos from the fertilised egg to the stage before gastrulation. In both animal and vegetal hemispheres, we observed a Rho kinase (ROCK)-independent cell stiffening that the cell stiffness exhibited a remarkable increase at the timing of cell division where cortical actin filaments were organized. Furthermore, in the vegetal hemisphere, we observed another mechanical behaviour, i.e., a ROCK-associated cell stiffening, which was retained even after cell division or occurred without division and propagated sequentially toward adjacent cells, displaying a characteristic cell-to-cell mechanical variation. The results indicate that the mechanical properties of embryonic cells are regulated at the single cell level in different germ layers.
“…Previous studies have reported that the number distribution of cell mechanical properties exhibits a large variation in single cells 41 , 42 and the cell stiffness and tension are very broadly varied over a long intercellular distance in a cell monolayer 43 – 46 . In contrast, the embryonic cells in the vegetal hemisphere exhibited broad spatiotemporal heterogeneity occurring at the single-cell level.…”
During the developmental processes of embryos, cells undergo massive deformation and division that are regulated by mechanical cues. However, little is known about how embryonic cells change their mechanical properties during different cleavage stages. Here, using atomic force microscopy, we investigated the stiffness of cells in ascidian embryos from the fertilised egg to the stage before gastrulation. In both animal and vegetal hemispheres, we observed a Rho kinase (ROCK)-independent cell stiffening that the cell stiffness exhibited a remarkable increase at the timing of cell division where cortical actin filaments were organized. Furthermore, in the vegetal hemisphere, we observed another mechanical behaviour, i.e., a ROCK-associated cell stiffening, which was retained even after cell division or occurred without division and propagated sequentially toward adjacent cells, displaying a characteristic cell-to-cell mechanical variation. The results indicate that the mechanical properties of embryonic cells are regulated at the single cell level in different germ layers.
“…with an empirically derived model known as the structural damping (or hysteretic damping) model 33,[137][138][139][140][141][142] whose complex modulus is given by:…”
Section: Structural Damping Model a Number Of Dynamic (Oscillatory) mentioning
“…where F is the loading force, d is the indentation depth, and n is the Poisson's ratio of the cell, assumed here to be 0.5 (16,(18)(19)(20)34), which corresponds to a perfectly incompressible material (33). We estimated E from the force-indentation curve in the region of d < 0.6 mm (see Fig.…”
Section: Afm Measurementsmentioning
confidence: 99%
“…The intracellular stiffness is a fundamental cell mechanical property. Previous studies of isolated single cells adhered to a substrate revealed that the intracellular stiffness-that is, the Young's modulus, E-measured by atomic force microscopy (AFM) is mainly dominated by actin cytoskeletal structures (16)(17)(18)(19) and can change in response to the rigidity of the substrate to which the cells adhere (20,21); specifically, the intracellular stiffness increases with increasing substrate rigidity. However, little is known about how the intracellular stiffness changes in response to neighboring cells in a cell monolayer system.…”
Section: Introductionmentioning
confidence: 99%
“…However, little is known about how the intracellular stiffness changes in response to neighboring cells in a cell monolayer system. Furthermore, although single cells are known to exhibit large cell-tocell variations in the cell stiffness (18,19), the cell-to-cell variation in the intracellular stiffness in a cell monolayer system is not well understood.…”
For isolated single cells on a substrate, the intracellular stiffness, which is often measured as the Young's modulus, E, by atomic force microscopy (AFM), depends on the substrate rigidity. However, little is known about how the E of cells is influenced by the surrounding cells in a cell population system in which cells physically and tightly contact adjacent cells. In this study, we investigated the spatial heterogeneities of E in a jammed epithelial monolayer in which cell migration was highly inhibited, allowing us to precisely measure the spatial distribution of E in large-scale regions by AFM. The AFM measurements showed that E can be characterized using two spatial correlation lengths: the shorter correlation length, l S , is within the single cell size, whereas the longer correlation length, l L , is longer than the distance between adjacent cells and corresponds to the intercellular correlation of E. We found that l L decreased significantly when the actin filaments were disrupted or calcium ions were chelated using chemical treatments, and the decreased l L recovered to the value in the control condition after the treatments were washed out. Moreover, we found that l L decreased significantly when E-cadherin was knocked down. These results indicate that the observed long-range correlation of E is not fixed within the jammed state but inherently arises from the formation of a large-scale actin filament structure via E-cadherin-dependent cell-cell junctions.
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