Nonideality of volume flows and phase transitions of F-actin solutions in response to osmotic stress.

Ovalbumin and G-actin solutions decreased their volume in a concentration-dependent manner in response to an osmotic stress, arising from an osmotic pressure gradient of 5-20 cm H2O at 25 degrees C, at protein concentrations as high as 20 mg/ml. In contrast, solutions of F-actin exhibited a concentration-dependent decrease in their rate of volume change in response to the osmotic stress. Shortening of F-actin by gelsolin did not affect this decrease, suggesting that the elastic response of the filaments underlies the osmotically nonideal behavior. However, above a critical actin concentration of approximately 7 mg/ml, no volume change occurred in response to osmotic gradients as high as 20 cm H2O. The concentration at which this critical phenomenon occurred and its abolition by shortening of F-actin by gelsolin suggest that a transition of diffusible rods to a glassy state is the cause of this critical phenomenon. Above the critical concentration, an increase in the osmotic pressure applied to an F-actin solution to greater than 20 cm H2O produced a transient increase in flow rate to that expected for a solution containing no polymer. This finding may represent a transition from an isotropic glassy state to an anisotropic and heterogeneous one wherein regions of pure solvent coexist with domains of pure polymer.     

Cell cycle-dependence of HL-60 cell deformability.

In this study, the role of cytoskeleton in HL-60 deformability during the cell cycle was investigated. G1, S, and G2/M cell fractions were separated by centrifugal elutriation. Cell deformability was evaluated by pipette aspiration. Tested at the same aspiration pressures, S cells were found to be less deformable than G1 cells. Moreover, HL-60 cells exhibited power-law fluid behavior: mu = mu c(gamma m/ gamma c)-b, where mu is cytoplasmic viscosity, gamma m is mean shear rate, mu c is the characteristic viscosity at the characteristic shear rate gamma c, and b is a material constant. At a given shear rate, S cells (mu c = 276 +/- 14 Pa.s, b = 0.51 +/- 0.03) were more viscous than G1 cells (mu c = 197 +/- 25, b = 0.53 +/- 0.02). To evaluate the relative importance of different cytoskeletal components in these cell cycle-dependent properties, HL-60 cells were treated with 30 microM dihydrocytochalasin B (DHB) to disrupt F-actin or 100 microM colchicine to collapse microtubules. DHB dramatically softened both G1 and S cells, which reduced the material constants mu c by approximately 65% and b by 20-30%. Colchicine had a limited effect on G1 cells but significantly reduced mu c of S cells (approximately 25%). Thus, F-actin plays the predominate role in determining cell mechanical properties, but disruption of microtubules may also influence the behavior of proliferating cells in a cell cycle-dependent fashion.     

Regional bioelectric properties of porcine airway epithelium.

Ion transport properties of pulmonary small airway epithelia are poorly understood. To characterize these properties, airways were excised from anesthetized pigs. Transepithelial potential difference (PD) and conductance were measured in five airway regions: trachea (T, 7.9 +/- 0.2 mm diam), mainstem bronchi (MB, 5.5 +/- 0.2 mm diam), large bronchi (LB, 1.69 +/- 0.12 mm diam), small bronchi (SB, 0.70 +/- 0.06 mm diam), and bronchioles (BR, 0.25 +/- 0.05 mm diam). T and MB were mounted in Ussing-type chambers, and LB, SB, and BR were cannulated with pipettes and perfused. PDs of control tissues were -9.7 +/- 0.8 mV (T), -4.0 +/- 0.5 mV (MB), -4.3 +/- 1.0 mV (LB), -4.5 +/- 0.4 mV (SB), and -1.5 +/- 0.4 mV (BR), lumen negative. Amiloride significantly (P < 0.05) inhibited PDs by 25-70% in all airway regions and decreased conductance 17-33% in all regions except LB where a 10% increase was observed. Bumetanide significantly reduced the amiloride-insensitive PD 54-62% in all regions except BR. Bumetanide had little effect on conductance in T, SB, and BR, but conductance was increased in MB and LB. All airways except the smallest BR significantly hyperpolarized when the solution that bathed the lumen was replaced with Cl(-)-free solution. In bronchioles, hyperpolarization by luminal Cl(-)-free solution was inversely related to fractional inhibition of PD with amiloride but directly related to lumen diameter. These results suggest that 1) porcine tracheas, bronchi, and bronchioles actively absorb Na+, and 2) secretion of Cl- may occur in all airway regions except small bronchioles.     

The effect of the 540-kilodalton actin cross-linking protein, actin-binding protein, on the mechanical properties of F-actin

This study describes the effect of actin-binding protein derived from rabbit lung macrophages on the mechanical properties of F-actin. The dynamic storage modulus, G'(omega), and loss modulus, G"(omega) of F-actin, at concentrations from 1 to 4 mg/ml, in the absence or presence of actin-binding protein at molar ratios to actin of 1:1000 to 1:125, were measured at frequencies ranging from 3 X 10(-3) to 0.5 Hz. Actin-binding protein increased the dynamic moduli of F-actin, but this increase was much greater as either the actin-binding protein/actin ratio or the total protein concentration increased. Moreover, there was a convergence of the values of G' and G" at high frequencies for F-actin which became more prominent upon the addition of actin-binding protein. The value of the modulus obtained by an extrapolation of these data to actin concentrations similar to that found in the cell cortex was close to values which have been obtained by direct measurements. The addition of actin-binding protein to an F-actin solution enabled it to reach an equilibrium strain following the application of a stress, in contrast to pure F-actin. These data allow a more rigorous definition of the "sol" to "gel" transition and suggest that the cross-linking of actin filaments by actin-binding protein leads to the formation of a network structure whose underlying mechanism of mechanical behavior is short range intrafilament bending in contrast to the classical rubber network.     

Pressure regulation of the electrical properties of growing Arabidopsis thaliana L. root hairs.

Actively growing Arabidopsis thaliana L. (Columbia wild type) root hairs were used to examine the interplay between cell turgor pressure and electrical properties of the cell: membrane potential, conductance, cell-to-cell coupling, and input resistance. Pressure was directly modulated using a pressure probe or indirectly by changing the extracellular osmolarity. Direct modulation of pressure in the range of 0 to about 15 x 10(5) Pa (normal turgor pressure was 6.8 +/- 2.0 x 10(5) Pa, n = 29) did not affect the membrane potential, conductance, coupling, or input resistance. Indirect modulation of turgor pressure by adding (hyperosmotic) or removing (hypo-osmotic) 200 mM mannitol/sorbitol affected the potential and conductance but not cell-to-cell coupling. Hypo-osmotic treatment depolarized the potential about 40 mV from an initial potential of about -190 mV and increased membrane conductance, consistent with an increase in anion efflux from the cell. Hyperosmotic treatment hyperpolarized the cell about 25 mV from the same initial potential and decreased conductance, consistent with a decline in cation influx. The results are likely due to the presence of an "osmo-sensor," rather than a "turgor-sensor," regulating the cell's response to osmotic stress.     

Correlation among endothelial cell shape, F-actin arrangement, and prostacyclin synthesis

Though many factors have been identified which modulate prostacyclin (PGI2) synthesis, there is little information on cellular mechanisms whereby endothelial cells (EC) regulate their basal eicosanoid metabolism. Using substrates of various adhesive capacities, bovine and porcine aortic EC shape and cytoskeletal F-actin arrangement could be modulated. Staining with rhodamine-phalloidin (R-P) permitted analysis of F-actin arrangement, while differences in cell shape were determined by measurement of cell perimeter surface area (CPSA). Spectrophotoflurometric measurements were used to quantitate the R-P binding capacity of the cultures. Cultures of reduced CPSA (225.2 +/- 13.5 mu2) generated the highest levels of basal PGl2 (6.14 +/- 0.51 pg/ug cell protein); had a diffuse arrangement of F-actin and an increased binding capacity for R-P (463.55 +/- 50.58 nmoles/ug cell protein). Cultures of enlarged CPSA (1399.3 +/- 148.3 mu2), with many actin cables and a significantly reduced (p less than 0.001) R-P binding capacity (74.941 +/- 11.79 nmoles/ug of cell protein) produced significantly smaller (p less than 0.001) basal quantities of PGl2 (1.33 +/- 0.14 pg/ug cell protein). Similarly, arachidonic acid stimulation of cultures of reduced CPSA resulted in an increased synthesis of PGl2 when compared to stimulated cultures of enlarged cells. These findings suggest a role for cell shape and the cytoskeleton in the mechanism controlling PGl2 production and indicate that alteration of the arrangement of F-actin may be of importance in regulation of EC eicosanoid metabolism.     

Absent effect of zinc deficiency on the oxidative stress of erythrocytes in chronic uremic rats

Both anemia and zinc deficiency are commonly observed in patients with chronic uremia. Oxidative stress of red blood cells (RBC) has been suggested to participate in the development of anemia in these patients with chronic uremia due to reduced life span of RBC. Whether zinc deficiency aggravates the effect of oxidative stress on RBC of chronic uremia is still not understood. We thus performed the study to determine the influence of zinc deficiency on the oxidative stress of RBC in uremic rats. Zinc deficiency was induced by long-term dietary zinc deficiency. Five-sixth nephrectomy (5/6 Nx) was used to produce chronic uremia. Experiment was carried out in the following five groups: normal control (NL), chronic uremia (Nx), chronic uremia + dietary zinc deficiency (Nx-D), Nx-D + zinc supplement (Nx-DZ) and Chronic uremia + pair-fed (Nx-PF). Osmotic fragility and lipid peroxidation of RBC were used to evaluate the oxidative stress of RBC. Five weeks after 5/6 nephrectomy (Nx), 5/6 Nx rats present a syndrome of uremia to elevate the levels of plasma creatinine and urea, and reduce the level of plasma zinc (1.12 +/- 0.08 vs 1.35 +/- 0.05 ug/ml). But they does not find to produce anemia and to increase osmotic fragility and lipid peroxidation in RBC. Dietary zinc deficiency in Nx-D group produced severe anorexia and reduced plasma zinc and selenium levels and the activity of RBC-GPX. Yet in Nx-D rats, osmotic fragility and susceptibility of lipid peroxidation in red cells did not increase, because of the increase of plasma copper level (1.85 +/- 0.3 vs 1.41 +/- 0.05 microg/ml) and RBC-SOD activity (1.95 +/- 0.27 vs 0.78 +/- 0.05 unit/g Hb). Zinc supplement in Nx-D rats (Nx-DZ group) recovered the appetite and normalized the levels of plasma zinc, copper and selenium. Food restriction in 5/6 Nx rats (Nx-PF group) decreased plasma copper level and increased osmotic fragility of RBC and elevated the susceptibility of lipid peroxidation after stressing RBC with H2O2 Because Nx-PF rats presented a lower RBC-SOD activity (0.44 +/- 0.11 vs 0.78 +/- 0.05 unit/g Hb) and a lower plasma copper level. We further found a positive relationship (r=0. 802,p<0.01) between plasma copper level and RBC-SOD activity in normal and uremic rats. This study suggests that RBC-SOD activity may play an important role in preventing RBC oxidative stress. Plasma copper level may be a marker of RBC-SOD activity. We conclude, in chronic uremia, zinc deficiency doses not result in RBC oxidative stress as plasma copper level is normal, but may affect the absorption of intestinal nutrition.     

Junctional permeability in heart muscle is independent upon the non-junctional membrane potential

The influence of high K solution on the longitudinal movement of Lucifer Yellow CH along dog atrial trabeculae was investigated. It was found that in normal heart muscle the dye diffused from cell-to-cell and the average diffusion coefficient (D) was 4.3 +/- 1.3 X 10(-7) cm2/s. In muscles exposed to 20, 40 or 60 mM K solution the resting potential was reduced from -78 mV (S.E. +/- 0.71) (control) to -41 mV (S.E. +/- 0.95), -30 mV (S.E. +/- 0.64) and -22.5 mV (S.E. +/- 0.64), respectively. Despite the maintained depolarization the cell-to-cell diffusion of Lucifer Yellow CH did not change. These findings indicate that the junctional permeability in heart muscle is not influenced by the non-junctional membrane potential.     

Kv4.2通道电流与大鼠海马神经元瞬间外向钾电流特性的比较

本研究比较了转染的Kv4.2钾电流与原代培养大鼠海马神经元上瞬间外向钾电流(IA)动力学特征。实验采用瞬时转染,细胞培养和全细胞膜片钳记录等方法。结果表明:转染的Kv4.2通道电流和海马神经元上IA均具有明显的A型电流特征。海马神经元IA的半数最大激活电位和斜率因子分别为-10.0±3.3 mV和13.9±2.6 mV;半数最大失活电位和斜率因子分别为-93.0±11.4 mV和-9.0±1.5 mV;失活后再激活恢复时间常数(T)为27.9±14.1 ms。Kv4.2的半数最大激活电位和斜率因子分别为-9.7±4.1 mV和15.8±5.7 mV;半数最大失活电位和斜率因子分别为-59.4±12.2 mV和8.0±3.1 mV;Kv4.2的灭活后再激活的恢复时间常数τ为172.8±10.0 ms。结果提示:Kv4.2通道电流可能是海马神经元上的IA电流的主要成分,但不是唯一成分。     

The effects of osmotic stress on the viscoelastic and physical properties of articular chondrocytes.

The metabolic activity of chondrocytes in articular cartilage is influenced by alterations in the osmotic environment of the tissue, which occur secondary to mechanical compression. The mechanism by which osmotic stress modulates cell physiology is not fully understood and may involve changes in the physical properties of the membrane or the cytoskeleton. The goal of this study was to determine the effect of the osmotic environment on the mechanical and physical properties of chondrocytes. In isoosmotic medium, chondrocytes exhibited a spherical shape with numerous membrane ruffles. Normalized cell volume was found to be linearly related to the reciprocal of the extracellular osmolality (Boyle van't Hoff relationship) with an osmotically active intracellular water fraction of 61%. In deionized water, chondrocytes swelled monotonically until lysis at a mean apparent membrane area 234 +/- 49% of the initial area. Biomechanically, chondrocytes exhibited viscoelastic solid behavior. The instantaneous and equilibrium elastic moduli and the apparent viscosity of the cell were significantly decreased by hypoosmotic stress, but were unchanged by hyperosmotic stress. Changes in the viscoelastic properties were paralleled by the rapid dissociation and remodeling of cortical actin in response to hypoosmotic stress. These findings indicate that the physicochemical environment has a strong influence on the viscoelastic and physical properties of the chondrocyte, potentially through alterations in the actin cytoskeleton.     

Hydration changes in the association of Hoechst 33258 with DNA

The role of water in the interaction of Hoechst 33258 with the minor groove binding site of the (AATT)2 sequence was investigated using calorimetric and equilibrium constant measurements. Using isothermal titration calorimetry measurements, the heat capacity change for the reaction is -256 +/- 10 cal/(K mol of Hoechst). Comparison with the heat capacity changes based on area models supports the expulsion of water from the interface of the Hoechst-DNA complex. To further consider the role of water, the osmotic stress method was used to determine if the Hoechst association with DNA was coupled with hydration changes. Using four osmolytes with varying molecular weights and chemical properties, the Hoechst affinity for DNA decreases with increasing osmolyte concentration. From the dependence of the equilibrium constant on the solution osmolality, 60 +/- 13 waters are acquired in the complex relative to the reactants. It is proposed that the osmotic stress technique is measuring weakly bound waters that are not measured via the heat capacity changes.     

CFTR involvement in nasal potential differences in mice and pigs studied using a thiazolidinone CFTR inhibitor

Nasal potential difference (PD) measurements have been used to demonstrate defective CFTR function in cystic fibrosis (CF) and to evaluate potential CF therapies. We used the selective thiazolidinone CFTR inhibitor CFTR(inh)-172 to define the involvement of CFTR in nasal PD changes in mice and pigs. In normal mice infused intranasally with a physiological saline solution containing amiloride, nasal PD was -4.7 +/- 0.7 mV, hyperpolarizing by 15 +/- 1 mV after a low-Cl- solution, and a further 3.9 +/- 0.5 mV after forskolin. CFTR(inh)-172 produced 1.1 +/- 0.9- and 4.3 +/- 0.7-mV depolarizations when added after low Cl- and forskolin, respectively. Systemically administered CFTR(inh)-172 reduced the forskolin-induced hyperpolarization from 4.7 +/- 0.4 to 0.9 +/- 0.1 mV but did not reduce the low Cl(-)-induced hyperpolarization. Nasal PD was -12 +/- 1 mV in CF mice after amiloride, changing by <0.5 mV after low Cl- or forskolin. In pigs, nasal PD was -14 +/- 3 mV after amiloride, hyperpolarizing by 13 +/- 2 mV after low Cl- and a further 9 +/- 1 mV after forskolin. CFTR(inh)-172 and glibenclamide did not affect nasal PD in pigs. Our results suggest that cAMP-dependent nasal PDs in mice primarily involve CFTR-mediated Cl- conductance, whereas cAMP-independent PDs are produced by a different, but CFTR-dependent, Cl- channel. In pigs, CFTR may not be responsible for Cl- channel-dependent nasal PDs. These results have important implications for interpreting nasal PDs in terms of CFTR function in animal models of CFTR activation and inhibition.     

Measurement of mitochondrial transmembrane electric potential using the fluorescent probe DSM]

The measurement of transmembrane electric potential of rat liver mitochondria was performed with fluorescent probe DSM. In the incubation medium with succinate the electric potential was -190 +/- 5 mV. Complete uncoupling caused by CCCP in the concentration 0.5 microM decreased the potential to -142 +/- 3 mV. In the partial uncoupling with a half of the mentioned CCCP concentration the potential was -158 +/- 6 mV. DSM influence on oxidation and phosphorylation was not detected.     

Solute inaccessible aqueous volume changes during opening of the potassium channel of the squid giant axon.

We have applied solutions with varying osmotic pressures symmetrically to the inside and outside of perfused, TTX-treated, giant axons. The potassium conductance G decreased with increasing osmotic stress, but there was no effect on either the shape or the position of the voltage-current curve. One must distinguish three possible actions of the osmotic agent: osmotic stress, channel blocking, and lowered solution conductivity. To do so, we compared results obtained working with pairs of internal and external solutions of either (a) equal osmotic stress, (b) equal conductivity, or (c) the same blocking agent. There was the same change in G irrespective of the type of stressing species (sorbitol or sucrose); this provides some evidence against a blocking mechanism. The conductivity of the external solution had a small effect on K currents; internal solution conductivity had none. A change in series resistance of the Schwann cell layer could account for the small effect of external solution conductivity. The primary cause of G depression appears, then, to be the applied osmotic stress. Using this result, we have developed models in which the channel has a transition between closed states under voltage control but osmotically insensitive and a closed/open step that is voltage-independent but osmotically sensitive. We have assumed that the conductance of this open state does not change with osmotic stress. In this way, we estimate that an additional 1,350 +/- 200 A3 or 40-50 molecules of solute-inaccessible water appear to associate with the average delayed rectifier potassium channel of the squid axon when it opens.     

Calmodulin transit via gap junctions is reduced in the absence of an electric field

Gap junctional transport of Calmodulin (CaM) from epithelial cells to insect oocytes is enhanced by alignment of the molecules via an electric field. It has recently been shown that CaM is needed for uptake of vitellogenins, is produced in the epithelial cells and reaches oocytes via gap junctions. For CaM to transit the gap junctions something must align these elongated molecules with the lumina of the gap junctions. This might be accomplished by the electric field that exists at the membrane of any cell with an Em of >0 mV. Fluorescently labeled CaM was injected into oocytes. At t=0, the epithelial cell/oocyte "fluorescence" ratio showed epithelial cells to be 24%+/-1.5% as bright as the injected oocyte. In follicles which maintained an electric field for one hour the epithelial cell/oocyte fluorescence ratio had risen to 79%+/-1.4%, while for follicles in which the field was cancelled by holding Em at 0 mV the ratio was only 45%+/-1.7%. After termination of the holding current follicles regained their original Em and their original electric field. At the end of a second hour of incubation the ratio had risen to 76%+/-1.2%, very close to what was observed in the untreated control follicles.     

Water permeability in different epithelial barriers

The water permeability properties of a series of epithelial barriers (the toad urinary bladder [TUB], the rat caecum [RC], the distal human colon [DHC], and the human amnion [HA] were studied in different experimental conditions. Three parameters were simultaneously determined: the water permeability coefficient in the presence of a transepithelial hydrostatic gradient (Phydr); the water permeability coefficient in the presence of an osmotic gradient (Posm); and the transepithelial potential difference (dV). All experiments were performed with the same experimental device, allowing comparison of the permeability properties of the barriers tested. The results obtained were: (1) TUB (N = 8): Phydr = 0.079 +/- 0.008 cm/s; Posm = 0.0004 +/- 0.0002 cm/s; dV = 31 +/- 5 mV; (2) TUB after ADH (N = 8): Phydr = 0.093 +/- 0.012 cm/s; Posm = 0.0065 +/- 0.0011 cm/s; dV = 52 +/- 8; (3) RC (N = 10): Phydr = 0.18 +/- 0.02 cm/s; Posm = 0.0019 +/- 0.0004 cm/s; dV = 3.9 +/- 0.1 mV; (4) RC adapted to a high K diet (N = 10): Phydr = 0.21 +/- 0.02 cm/s; Posm = 0.0018 +/- 0.0006 cm/s; dV = 4.5 +/- 0.5 mV; (5) DHC (N = 6): Phydr = 0.22 +/- 0.03 cm/s; Posm = 0.002 +/- 0.05 cm/s; dV = 15 +/- 3 mV; (6) HA (N = 10): Phydr = 0.32 +/- 0.05 cm/s; Posm = 0.0154 +/- 0.0015; dV = 0. The results show a good correlation between Phydr and dV, but not between dV and Posm or between Posm and Phydr.     

Transepithelial potential in mesonephric nephrons of 7-day-old chick embryos in relation to the histochemically detected sodium pump

In order to obtain basic information on the transport properties of differentiating embryonic nephrons, we examined the 7-day-old chick mesonephros by measuring the transtubular epithelial potential difference (TPD) and by histochemical detection of Na,K-ATPase activity. TPD as an indicator of the electrogenic transport was measured in individual segments of superficial nephrons in vivo. Their electric polarity was always lumen-negative. TPD was reduced by addition of 10 mM KCN applied to the mesonephric nephrons from the outside. In the proximal tubules, TPD was significantly lower (mean+/-SD: -1.0+/-0.5 mV) than in the distal and collecting tubules (-2.2+/-1.0 mV, p< or =0.05). Activity of the sodium pump was evaluated histochemically by detection of ouabain-sensitive potassium-dependent p-nitrophenyl phosphatase in cryostat sections of the mesonephros. The enzyme activity was demonstrated only in distal tubules and in the collecting ducts, but not in the proximal tubules. These findings have revealed significant differences between embryonic nephron segments: the distal tubule, in contrast to the proximal one, is supplied by the sodium pump and is able to generate higher TPD. Therefore, we consider that it is only the distal nephron, which possesses the ability of active transport.     

Diphasic transformations of F-actin. Effects of urea and MgCl2 on F-actin.

Asakura, Taniguchi and Oosawa [1]proposed that muscle actin polymer under sonic vibration is in a different state from that of the ordinary double stranded helical structure (F-actin), characterised by partially interrupted structures of F-actin, a state of "f-actin". In order to confirm different states for actin polymers [1, 2], physicochemical studies were made by measurements of viscosity, flow birefringence, electric birefringence, fluorescence, electron microscopy, quasielastic light scattering and ATP splitting. The following results were obtained. (1) F-actin polymers can undergo two processes of depolymerization upon treatment with urea and various salts as judged by measurements of flow birefringence and viscosity: one is a rapid process in a solution containing K+ or Ca2+ and urea; the other is a slow process following a brief rapid one in a solution containing Mg2+ and urea. (2) In the presence of Mg2+ and a suitable concentration of urea, F-actin (FMU-actin) appeared to exhibit different properties than ordinary F-actin; it had lower viscosity and lower flow birefringence and it had on the whole a more flexible polymer structure, also judging from experiments of quasielastic light scattering, electric birefringence. The different structure was confirmed directly be electron microscopic observation. The aromatic side chains of FMU-actin were also more mobile than those of F-actin judging from fluorescence measurements. The transformation between F-actin and FMU-actin was reversible. (3) The state of FMU-actin polymers was also characterized by ATP splitting; FMU-actin split about one mole of ATP into ADP and inorganic phosphate per mole of actin monomer at room temperature, where F-actin did not. A molar excess of Mg2+ with respect to actin monomer at room temperature, where F-actin did not. A molar excess of Mg2+ with respect to actin monomer is required for ATP splitting. F-actin in solutions containing K+ or Ca2+ and urea did not split ATP. FMU-actin activated on Mg-ATP-ase of myosin at nearly the same rate as that of F-actin. (4) We have postulated a flexible filament model (f-actin). The relationships between the structure of f-actin and its functional role for force generation during contraction are discussed.     

UV microirradiation implicates F-actin in reinforcing growing hyphal tips

Summary The cell walls of plants and fungi are thought to provide the strength required to resist turgor and thus maintain the integrity and morphology of these cells. However, during growth, walls must undergo rapid expansion which requires them to be plastic and therefore weak. In most tip-growing cells there is an apical concentration of F-actin associated with the rapidly expanding cell wall. Disruption of F-actin in the growing tips of hyphae ofSaprolegnia ferax by a localized irradiation, beginning 2–6 m behind the apex, with actin-selective 270 nm uv light caused the hyphae to burst, suggesting that actin supports the weak apical wall against turgor pressure. Bursting was pH dependent and Ca²⁺ independent at neutral pH. Hyphae burst in the very tip, where the cell wall is expected to be weakest and actin is most concentrated, as opposed to the lower part of the apical taper where osmotic shock induces bursting when actin is intact. When hyphae were irradiated with a wavelength of light that is less effective at disrupting actin, growth was slowed but they failed to burst, demonstrating that bursting was most likely due to F-actin damage. We conclude that F-actin reinforces the expanding apical wall in growing hyphae and may be the prime stress bearing structure resisting turgor pressure in tip growing cells.Abbreviations RP rhodamine phalloidin - F-actin filamentous actin - EGTA ethylene-glycol-bis-(-amino-ethyl ether) N,N-tetra-acetic acid - PIPES piperazine-N,N-bis-(2-ethanesulfonic acid) - uv ultraviolet     

Calcium channel currents in isolated smooth muscle cells from human bronchus

An electrophysiological study was carried out on smooth muscle cells that were enzymatically dissociated from bundles of muscle fibers dissected out of human bronchi obtained at thoracotomy. These cells that retain the contractile properties of intact bundles were voltage-clamped by means of the whole-cell patch-clamp technique. Upon voltage steps from a holding potential of -60 mV to more positive levels, the initial inward current was followed by large outward currents that inactivated slowly. These were subsequently reduced by substituting Cs+ for K+ in the internal solution and by using Ba2+ instead of Ca2+ as a charge carrier in the external solution. Under these conditions, the inward current did not completely inactivate in the course of 300-ms voltage steps. Inward current measured after leak subtraction was activated at a membrane potential of -25.8 +/- 5 mV, was maximum at +18 +/- 4 mV, and had an apparent reversal potential of +52.5 +/- 5.5 mV (n = 5). The potential at which steady-state inactivation was half-maximum was -28 mV (n = 5). This inward current was identified as a calcium current on the following basis: 1) it was not altered by 10 microM tetrodotoxin (TTX) or by lowering to 10 mM external Na+ concentration; 2) it was blocked by 2.5 mM Co2+ or 1 microM PN 200-110; 3) it was enhanced by 1 microM BAY K 8644, which in addition suppressed the PN 200-110 blockade.(ABSTRACT TRUNCATED AT 250 WORDS)