Orientation of apical and basal actin stress fibers in isolated and subconfluent endothelial cells as an early response to cyclic stretching

We investigated the response of apical and basal actin stress fibers (SFs) and its dependency on cell confluency for endothelial cells subjected to cyclic stretching. Porcine aortic endothelial cells from the 2nd and 5th passages were transferred to a fibronectin-coated silicone chamber with 5000-8000 cells/cm2 (isolated condition), positioning the cells apart, or with 25,000-27,000 cells/cm2 (subconfluent condition), allowing cell-to-cell contact. The substrate was stretched cyclically by 0.5 Hz for 2 h with a peak strain on the substrate that was 15% in the stretch direction and -4% in the transverse direction. The actin filaments (AFs) were stained with rhodamine phalloidin and their orientations were examined under a confocal laser scanning microscope. In the basal region, SFs formed in all of the cells under both the isolated and subconfluent conditions. We observed an average of 5 and 9 SFs per cell under the isolated and subconfluent conditions, respectively, in the fluorescent images of the apical region. We also observed cells that were bush-like without apical AFs or apical SFs. On average, the SFs in the subconfluent cells oriented in the direction of minimal strain, while the SFs in the isolated cells oriented in the direction of a 2% compressive strain. These results suggest that such differential response may be due to differences in the transmission of mechanical stretching to the central and apical regions of the cell through the SFs. We also speculate that cell-to-cell contact might change the strength, orientation, and anchorage of apical AFs and play a critical role in mechanical signal transduction.     

Intracellular stress transmission through actin stress fiber network in adherent vascular cells

Intracellular stress transmission through subcellular structural components has been proposed to affect activation of localized mechano-sensing sites such as focal adhesions in adherent cells. Previous studies reported that physiological extracellular forces produced heterogeneous spatial distributions of cytoplasmic strain. However, mechanical signaling pathway involved in intracellular force transmission through basal actin stress fibers (SFs), a mechano-responsive cytoskeletal structure, remains elusive. In the present study, we investigated force balance within the basal SFs of cultured smooth muscle cells and endothelial cells by (i) removing the cell membrane and cytoplasmic constituents except for materials physically attaching to the substrate (i.e., SF-focal adhesion complexities) or (ii) dislodging either mechanically or chemically the cell processes of the cells expressing fluorescent proteins-labeled actin and focal adhesions in order, to examine stress-release-induced deformation of the basal SFs. The result showed that a removal of mechanical restrictions for SFs resulted in a decrease in the length of the remaining SFs, which means SFs bear tension. In addition, a release of the preexisting tension in a single SF was transmitted to another SF physically linked to the former, but not transmitted to the other ones physically independent of the former, suggesting that the prestress is balanced in tensed SF networks. These results support a hypothesis regarding cell structural architecture that physiological extracellular forces can produce in the basal SF network a directional intracellular stress or strain distribution. Therefore, consideration of the coexistence of the directional stretching strain along the axial direction of SFs and the heterogeneous strain in the other cytoplasmic region will be essential for understanding intracellular stress transmission in the adherent cells.     

Role of marginal stress fibers formed in the rat vascular endothelial cells

Fluorescence cytochemistry using en face preparations of rat vascular endothelial cells (ECs) revealed the localization of actin, fibronectin (FN) and fibronectin receptor (FNR) along not only central stress fibers (SFs) but also the cell margins. Electron microscopy showed very close proximity between the topographical distribution of intracellular microfilament bundles and that of subendothelial FN in the EC margins. Therefore, these basal and marginal actin cables may be comparable to the well-established central SFs present in ECs. Formation of the central SFs was induced in ECs or mesothelial cells in response to tension, by which their cellular integrity seems to be effectively maintained. However, even when central SF formation was inhibited by cytochalasin D, the ECs with marginal SFs showed high resistance to mechanical tension, whereas mesenteric mesothelial cells having no such fibers easily lost their integrity. Thus, together with central SFs, the marginal SFs characteristic of rat vascular ECs may play an essential role in strengthening cell-matrix adhesion.     

Movement of stress fibers away from focal adhesions identifies focal adhesions as sites of stress fiber assembly in stationary cells

Force generated in contractile actin filament bundles (stress fibers-SFs) is transmitted to the extracellular matrix (ECM) via linker proteins and transmembrane integrins at focal adhesions (FAs). Though it has long been known that actin is rapidly exchanged in FAs, the connection between SFs and FAs has not been studied in detail. We introduced fiduciary marks on SFs by expressing GFP-palladin or GFP-alpha-actinin-1, which are both FA and dense body proteins, and by pattern bleaching of GFP-actin. Following fiduciary marks on SFs over time by time-lapse fluorescence microscopy, we detected assembly of SFs at FAs in stationary cells resulting in movement of SFs away from FAs with a velocity of 0.2-0.4 microm/min. Visualization of FAs in GFP-palladin/DsRed-paxillin double transfected cells showed that SF elongation was not accompanied by a change in FA length. SF elongation at FAs depended on actin polymerization and force as demonstrated by inhibitors of actin polymerization (cytochalasin D, jasplakinolide) and inhibitors of myosin-dependent contraction (blebbistatin, Y-27632), respectively. Our finding of SF assembly at FAs has important implications for SF formation, force transmission, and tension distribution within the actin cytoskeletal network of stationary cells.     

Estimation of the mechanical connection between apical stress fibers and the nucleus in vascular smooth muscle cells cultured on a substrate

Actin stress fibers (SFs) generate intercellular tension and play important roles in cellular mechanotransduction processes and the regulation of various cellular functions. We recently found, in vascular smooth muscle cells (SMCs) cultured on a substrate, that the apical SFs running across the top surface of the nucleus have a mechanical connection with the cell nucleus and that their internal tension is transmitted directly to the nucleus. However, the effects of the connecting conditions and binding forces between SFs and the nucleus on force transmission processes are unclear at this stage. Here, we estimated the mechanical connection between apical SFs and the nucleus in SMCs, taking into account differences in the contractility of individual SFs, using experimental and numerical approaches. First, we classified apical SFs in SMCs according to their morphological characteristics: one subset appeared pressed onto the apical surface of the nucleus (pressed SFs), and the other appeared to be smoothly attached to the nuclear surface (attached SFs). We then dissected these SFs by laser irradiation to release the pretension, observed the dynamic behavior of the dissected SFs and the nucleus, and estimated the pretension of the SFs and the connection strength between the SFs and the nucleus by using a simple viscoelastic model. We found that pressed SFs generated greater contractile force and were more firmly connected to the nuclear surface than were attached SFs. We also observed line-like concentration of the nuclear membrane protein nesprin 1 and perinuclear DNA that was significantly located along the pressed SFs. These results indicate that the internal tension of pressed SFs is transmitted to the nucleus more efficiently than that of attached SFs, and that pressed SFs have significant roles in the regulation of the nuclear morphology and rearrangement of intranuclear DNA.     

Stress fibers of the aortic smooth muscle cells in tissues do not align with the principal strain direction during intraluminal pressurization

Stress fibers (SFs) in cells transmit external forces to cell nuclei, altering the DNA structure, gene expression, and cell activity. To determine whether SFs are involved in mechanosignal transduction upon intraluminal pressure, this study investigated the SF direction in smooth muscle cells (SMCs) in aortic tissue and strain in the SF direction. Aortic tissues were fixed under physiological pressure of 120 mmHg. First, we observed fluorescently labeled SFs using two-photon microscopy. It was revealed that SFs in the same smooth muscle layers were aligned in almost the same direction, and the absolute value of the alignment angle from the circumferential direction was 16.8° ± 5.2° (n = 96, mean ± SD). Second, we quantified the strain field in the aortic tissue in reference to photo-bleached markers. It was found in the radial-circumferential plane that the largest strain direction was − 21.3° ± 11.1°, and the zero normal strain direction was 28.1° ± 10.2°. Thus, the SFs in aortic SMCs were not in line with neither the largest strain direction nor the zero strain direction, although their orientation was relatively close to the zero strain direction. These results suggest that SFs in aortic SMCs undergo stretch, but not maximal and transmit the force to nuclei under intraluminal pressure.

     

Strain waveform dependence of stress fiber reorientation in cyclically stretched osteoblastic cells: effects of viscoelastic compression of stress fibers

Actin stress fibers (SFs) of cells cultured on cyclically stretched substrate tend to reorient in the direction in which a normal strain of substrate becomes zero. However, little is known about the mechanism of this reorientation. Here we investigated the effects of cyclic stretch waveform on SF reorientation in osteoblastic cells. Cells adhering to silicone membranes were subjected to cyclic uniaxial stretch, having one of the following waveforms with an amplitude of 8% for 24 h: triangular, trapezoid, bottom hold, or peak hold. SF reorientation of these cells was then analyzed. No preferential orientation was observed for the triangular and the peak-hold waveforms, whereas SFs aligned mostly in the direction with zero normal strain (~55°) with other waveforms, especially the trapezoid waveform, which had a hold time both at loaded and unloaded states. Viscoelastic properties of SFs were estimated in a quasi-in situ stress relaxation test using intact and SF-disrupted cells that maintained their shape on the substrate. The dynamics of tension F(SFs) acting on SFs during cyclic stretching were simulated using these properties. The simulation demonstrated that F(SFs) decreased gradually during cyclic stretching and exhibited a compressive value (F(SFs) < 0). The magnitude and duration time of the compressive forces were relatively larger in the group with a trapezoid waveform. The frequency of SF orientation had a significant negative correlation with the applied compressive forces integrated with time in a strain cycle, and the integrated value was largest with the trapezoid waveform. These results may indicate that the applied compressive forces on SFs have a significant effect on the stretch-induced reorientation of SFs, and that SFs realigned to avoid their compression. Stress relaxation of SFs might be facilitated during the holding period in the trapezoid waveform, and depolymerization and reorientation of SFs were significantly accelerated by their viscoelastic compression.     

Probing elasticity and adhesion of live cells by atomic force microscopy indentation

Atomic force microscopy (AFM) indentation has become an important technique for quantifying the mechanical properties of live cells at nanoscale. However, determination of cell elasticity modulus from the force–displacement curves measured in the AFM indentations is not a trivial task. The present work shows that these force–displacement curves are affected by indenter-cell adhesion force, while the use of an appropriate indentation model may provide information on the cell elasticity and the work of adhesion of the cell membrane to the surface of the AFM probes. A recently proposed indentation model (Sirghi, Rossi in Appl Phys Lett 89:243118, 2006), which accounts for the effect of the adhesion force in nanoscale indentation, is applied to the AFM indentation experiments performed on live cells with pyramidal indenters. The model considers that the indentation force equilibrates the elastic force of the cell cytoskeleton and the adhesion force of the cell membrane. It is assumed that the indenter-cell contact area and the adhesion force decrease continuously during the unloading part of the indentation (peeling model). Force–displacement curves measured in indentation experiments performed with silicon nitride AFM probes with pyramidal tips on live cells (mouse fibroblast Balb/c3T3 clone A31-1-1) in physiological medium at 37°C agree well with the theoretical prediction and are used to determine the cell elasticity modulus and indenter-cell work of adhesion. Electronic supplementary material  The online version of this article (doi:) contains supplementary material, which is available to authorized users.     

Mechanical properties of actin stress fibers in living cells

Actin stress fibers (SFs) play an important role in many cellular functions, including morphological stability, adhesion, and motility. Because of their central role in force transmission, it is important to characterize the mechanical properties of SFs. However, most of the existing studies focus on properties of whole cells or of actin filaments isolated outside cells. In this study, we explored the mechanical properties of individual SFs in living endothelial cells by nanoindentation using an atomic force microscope. Our results demonstrate the pivotal role of SF actomyosin contractile level on mechanical properties. In the same SF, decreasing contractile level with 10 μM blebbistatin decreased stiffness, whereas increasing contractile level with 2 nM calyculin A increased stiffness. Incrementally stretching and indenting SFs made it possible to determine stiffness as a function of strain level and demonstrated that SFs have nearly linear stress-stain properties in the baseline state but nonlinear properties at a lower contractile level. The stiffnesses of peripheral and central portions of the same SF, which were nearly the same in the baseline state, became markedly different after contractile level was increased with calyculin A. Because these results pertain to effects of interventions in the same SF in a living cell, they provide important new understanding about cell mechanics.     

Microfilament Orientation Constrains Vesicle Flow and Spatial Distribution in Growing Pollen Tubes

The dynamics of cellular organelles reveals important information about their functioning. The spatio-temporal movement patterns of vesicles in growing pollen tubes are controlled by the actin cytoskeleton. Vesicle flow is crucial for morphogenesis in these cells as it ensures targeted delivery of cell wall polysaccharides. Remarkably, the target region does not contain much filamentous actin. We model the vesicular trafficking in this area using as boundary conditions the expanding cell wall and the actin array forming the apical actin fringe. The shape of the fringe was obtained by imposing a steady state and constant polymerization rate of the actin filaments. Letting vesicle flux into and out of the apical region be determined by the orientation of the actin microfilaments and by exocytosis was sufficient to generate a flux that corresponds in magnitude and orientation to that observed experimentally. This model explains how the cytoplasmic streaming pattern in the apical region of the pollen tube can be generated without the presence of actin microfilaments.     

Estimation of single stress fiber stiffness in cultured aortic smooth muscle cells under relaxed and contracted states: Its relation to dynamic rearrangement of stress fibers

For a quantitative analysis of intracellular mechanotransduction, it is crucial to know the mechanical properties of actin stress fibers in situ. Here we measured tensile properties of cultured aortic smooth muscle cells (SMCs) in a quasi-in situ tensile test in relaxed and activated states to estimate stiffness of their single stress fibers (SFs). An SMC cultured on substrates was held using a pair of micropipettes and detached from the substrate while maintaining its in situ cell shape and cytoskeletal integrity. Stretching up to ～15% followed by unloading was repeated three times to stabilize their tension–strain curves in the untreated (relaxed) and 10 μM-serotonin-treated (activated) condition. Cell stiffness defined as the average slope of the loading limb of the stable loops was ～25 and ～40 nN/% in relaxed and activated states, respectively. It decreased to ～10 nN/% following SF disruption with cytochalasin D in both states. The number of SFs in each cell measured with confocal microscopy decreased significantly upon serotonin activation from 21.5±3.8 (mean±SD, n=80) to 17.5±3.9 (n=77). The dynamics of focal adhesions (FAs) were observed in adherent cells using surface reflective interference contrast microscopy. FAs aligned and elongated along the cell major axis following activation and then merged with each other, suggesting that the decrease in SFs was caused by their fusion. Average stiffness of single SFs estimated by the average decrease in whole-cell stiffness following SF disruption divided by the average number of SFs in each cell was ～0.7 and ～1.6 nN/% in the relaxed and activated states, respectively. Stiffening of single SFs following SF activation was remarkably higher than stiffening at the whole-cell level. Results indicate that SFs stiffen not only due to activation of the actomyosin interaction, but also due to their fusion, a finding which would not be obtained from analysis of isolated SFs.     

Simultaneous contraction and buckling of stress fibers in individual cells

It has been proposed that buckling of actin stress fibers (SFs) may be associated with their disassembly. However, much of the detail remains unknown partly because the use of an elastic membrane sheet, conventionally necessary for inducing SF buckling with a mechanical compression to adherent cells, may limit high quality and quick imaging of the dynamic cellular events. Here, we present an alternate approach to induce buckling behavior of SFs on a readily observable glass plate. Actin SFs were extracted from cells, and constituent myosin II (MII) molecules were partially photo-inactivated in contractility. An addition of Mg-ATP allowed actin-myosin cross-bridge cycling and resultant contraction of only thick SFs that still contained active MII in the large volume. Meanwhile, thin SFs with virtually no active motor protein in the small volume had no choice but to buckle with the shortening movement of nearby thick SFs functioning as a compression-inducing element. This novel technique, thus allowing for selective inductions of contraction and buckling of SFs and measurements of the cellular prestress, may be applicable to not only investigations on their disassembly mechanisms but also to measurements of the relative thickness of individual SFs in each cell.     

The protocerebral neurosecretory system and associated cerebral neurohemal area of Acheta domesticus

Summary A comparison of rectal morphology and ultrastructure is made between a freshwater (A. aegypti) and salt water (A. campestris) species of mosquito larvae, and between A. campestris larvae producing hyper- and hyposmotic urine.The epithelium of A. aegypti contains one cell type characterized by infolding of both the apical and basal membranes, straight lateral borders, and evenly distributed mitochondria.The rectum of A. campestris contains distinct anterior and posterior regions, each made up of a single cell type. These two regions can be distinguished on the basis of cell thickness, depth of apical infolding and distribution of mitochondria. The anterior region is similar to the rectum of A. aegypti, while the posterior region is considered unique to the salt-water species and hence probably is associated with the formation of hyperosmotic urine.In A. campestris, the apical (rather than lateral or basal) membranes are probably the site of hyperosmotic urine production. Two possible mechanisms for this process are discussed.This work was supported by operating grants from the National Research Council of Canada.     

Immunofluorescence study of mitosis and cytokinesis in Acrosiphonia duriuscula (Acrosiphoniales,Chlorophyta)*

The behaviors of nuclei and microtubules (MT) in Acrosiphonia duriuscula (Ruprecht) Collins were observed in detail using fluorescence and electron microscopy. Numerous nuclei exist in cells of A. duriuscula (multinucleate cells). Cortical MT radiate from the apex of the tip cell and run parallel to its long axis. Between 30 and 40% of nuclei in the upper part of cytoplasm migrate downward to the region where cytokinesis will take place, and these numerous nuclei form a ‘nuclear ring’ before mitosis. The parallel array of the cortical MT changes to a transverse orientation at the region where cytokinesis will take place, and finally forms a characteristic circumferential band. Mitosis starts from the nuclei in the ring. Cortical MT disappear in the region of the nuclear ring and many mitotic spindles form. The band-shaped array of MT remains. Mitosis spreads in an apparent wave to the other nuclei. After mitosis, daughter nuclei that formed a nuclear ring migrate apically and repopulate the apical daughter cell. When the numerous daughter nuclei have relocated, a rearrangement of the cortical MT occurs. They are randomly arranged at first, but finally become parallel to the long axis of the cell. Cytokinesis occurs by furrowing of the cell, and the band-shaped array of MT could be detected at the leading edge of the furrow.     

Ultrastructure of the colon of Locusta migratoria

The ultrastructure of the colon of Locusta migratoria is described. The colon is lined by a thick cuticle that, for the most part, adheres to the underlying epithelium. The cuboid epithelial cells are characterized by moderate invaginations of the apical and, to a lesser extent, basal plasma membranes; the lateral plasma membranes are relatively flat. The bulk of the mitochondria are located in the apical region of the cell and are not particularly associated with any of the plasma membranes. The basal region of the cells contains much rough endoplasmic reticulum, glycogenlike granules, and a predominance of spherical, electron-dense bodies of various sizes. Where muscle fibers make contact with the epithelium, the cells are much reduced; the cytoplasm is usually less electron-dense, and, typically, the nucleus has a thick layer of granular material associated with the inner nuclear membrane. The apical and basal plasma membranes of the reduced epithelial cells contain numerous hemidesmosomes. The apical hemidesmosomes occur in pairs around an extracellular space that contains electron-opaque material. The latter forms tonofibrillae that extend into the endocuticle. Bundles of microtubules are associated with the hemidesmosomes. The tubules traverse the cell from the apical to the basal region. The possible significance of these findings is discussed.     

Measurements of strain on single stress fibers in living endothelial cells induced by fluid shear stress

Fluid shear stress (FSS) acting on the apical surface of endothelial cells (ECs) can be sensed by mechano-sensors in adhesive protein complexes found in focal adhesions and intercellular junctions. This sensing occurs via force transmission through cytoskeletal networks. This study quantitatively evaluated the force transmitted through cytoskeletons to the mechano-sensors by measuring the FSS-induced strain on SFs using live-cell imaging for actin stress fibers (SFs). FSS-induced bending of SFs caused the SFs to align perpendicular to the direction of the flow. In addition, the displacement vectors of the SFs were detected using image correlation and the FSS-induced axial strain of the SFs was calculated. The results indicated that FSS-induced strain on SFs spanned the range 0.01-0.1% at FSSs ranging from 2 to 10 Pa. Together with the tensile property of SFs reported in a previous study, the force exerted on SFs was estimated to range from several to several tens of pN.     

Actin stress fiber pre-extension in human aortic endothelial cells

Actin stress fibers (SFs) enable cells to sense and respond to mechanical stimuli and affect adhesion, motility and apoptosis. We and others have demonstrated that cultured human aortic endothelial cells (HAECs) are internally stressed so that SFs are pre-extended beyond their unloaded lengths. The present study explores factors affecting SF pre-extension. In HAECs cultured overnight the baseline pre-extension was 1.10 and independent of the amount of cell shortening. Decreasing contractility with 30 mM BDM or 10 microM blebbistatin decreased pre-extension to 1.05 whereas increasing contractility with 2 nM calyculin A increased pre-extension to 1.26. Knockdown of alpha-actinin-1 with an interfering RNA increased pre-extension to 1.28. None of these affected the wavelength of the buckled SFs. Pre-extension was the same in unperturbed cells as in those in which the actin cytoskeleton was disrupted by both chemical and mechanical means and then allowed to reassemble. Finally, disrupting MTs or IFs did not affect pre-extension but increased the wavelength. Taken together, these results suggest that pre-extension of SFs is determined primarily by intrinsic factors, i.e. the level of actin-myosin interaction. This intrinsic control of pre-extension is sufficiently robust that pre-extension is the same even after the actin cytoskeleton has been disrupted and reorganized. Unlike pre-extension, the morphology of the compressed SFs is partially determined by MTs and IFs which appear to support the SFs along their lengths.