Magnesium gating of cardiac gap junction channels

We aimed to study kinetics of modulation by intracellular Mg²⁺ of cardiac gap junction (Mg²⁺ gate). Paired myocytes of guinea-pig ventricle were superfused with solutions containing various concentrations of Mg²⁺. In order to rapidly apply Mg²⁺ to one aspect of the gap junction, the non-junctional membrane of one of the pair was perforated at nearly the connecting site by pulses of nitrogen laser beam. The gap junction conductance (G_j) was measured by clamping the membrane potential of the other cell using two-electrode voltage clamp method. The laser perforation immediately increased G_j, followed by slow G_j change with time constant of 3.5 s at 10 mM Mg²⁺. Mg²⁺ more than 1.0 mM attenuated dose-dependently the gap junction conductance and lower Mg²⁺ (0.6 mM) increased G_j with a Hill coefficient of 3.4 and a half-maximum effective concentration of 0.6 mM. The time course of G_j changes was fitted by single exponential function, and the relationship between the reciprocal of time constant and Mg²⁺ concentration was almost linear. Based on the experimental data, a mathematical model of Mg²⁺ gate with one open state and three closed states well reproduced experimental results. One-dimensional cable model of thirty ventricular myocytes connected to the Mg²⁺ gate model suggested a pivotal role of the Mg²⁺ gate of gap junction under pathological conditions.     

Bipolar nanosecond electric pulses are less efficient at electropermeabilization and killing cells than monopolar pulses

Multiple studies have shown that bipolar (BP) electric pulses in the microsecond range are more effective at permeabilizing cells while maintaining similar cell survival rates as compared to monopolar (MP) pulse equivalents. In this paper, we investigated whether the same advantage existed for BP nanosecond-pulsed electric fields (nsPEF) as compared to MP nsPEF. To study permeabilization effectiveness, MP or BP pulses were delivered to single Chinese hamster ovary (CHO) cells and the response of three dyes, Calcium Green-1, propidium iodide (PI), and FM1-43, was measured by confocal microscopy. Results show that BP pulses were less effective at increasing intracellular calcium concentration or PI uptake and cause less membrane reorganization (FM1-43) than MP pulses. Twenty-four hour survival was measured in three cell lines (Jurkat, U937, CHO) and over ten times more BP pulses were required to induce death as compared to MP pulses of similar magnitude and duration. Flow cytometry analysis of CHO cells after exposure (at 15 min) revealed that to achieve positive FITC-Annexin V and PI expression, ten times more BP pulses were required than MP pulses. Overall, unlike longer pulse exposures, BP nsPEF exposures proved far less effective at both membrane permeabilization and cell killing than MP nsPEF.     

Cardiac Myocyte Excitation by Ultrashort High-Field Pulses

In unexcitable, noncardiac cells, ultrashort (nanosecond) high-voltage (megavolt-per-meter) pulsed electrical fields (nsPEF) can mobilize intracellular Ca²⁺ and create transient nanopores in the plasmalemma. We studied Ca²⁺ responses to nsPEF in cardiac cells. Fluorescent Ca²⁺ or voltage signals were recorded from isolated adult rat ventricular myocytes deposited in an electrode microchamber and stimulated with conventional pulses (CPs; 0.5-2.4 kV/cm, 1 ms) or nsPEF (10-80 kV/cm, 4 ns). nsPEF induced Ca²⁺ transients in 68/104 cells. Repeating nsPEF increased the likelihood of Ca²⁺ transient induction (61.8% for <10 nsPEF vs. 80.6% for ≥10 nsPEF). Repetitive Ca²⁺ waves arising at the anodal side and Ca²⁺ destabilization occurred after repeated nsPEF (12/29) or during steady-state single nsPEF delivery at 2 Hz. Removing extracellular Ca²⁺ abolished responses to nsPEF. Verapamil did not affect nsPEF-induced Ca²⁺ transients, but decreased responses to CP. Tetrodotoxin and KB-R7943 increased the repetition threshold in response to nsPEF: 1-20 nsPEF caused local anodal Ca²⁺ waves without Ca²⁺ transients, and ≥20 nsPEF caused normal transients. Ryanodine-thapsigargin and caffeine protected against nsPEF-induced Ca²⁺ waves and showed less recovery of diastolic Ca²⁺ levels than CP. Voltage recordings demonstrated action potentials triggered by nsPEF, even in the presence of tetrodotoxin. nsPEF can mobilize intracellular Ca²⁺ in cardiac myocytes by inducing action potentials. Anodal Ca²⁺ waves and resistance to Na⁺ and Ca²⁺ channel blockade suggest nonselective ion channel transport via sarcolemmal nanopores as a triggering mechanism.     

Expression of voltage-gated calcium channels augments cell susceptibility to membrane disruption by nanosecond pulsed electric field

We compared membrane permeabilization by nanosecond pulsed electric field (nsPEF) in HEK293 cells with and without assembled CaV1.3 L-type voltage-gated calcium channel (VGCC). Individual cells were subjected to one 300-ns pulse at 0 (sham exposure); 1.4; 1.8; or 2.3 kV/cm, and membrane permeabilization was evaluated by measuring whole-cell currents and by optical monitoring of cytosolic Ca²⁺. nsPEF had either no effect (0 and 1.4 kV/cm), or caused a lasting (>80 s) increase in the membrane conductance in about 50% of cells (1.8 kV/cm), or in all cells (2.3 kV/cm). The conductance pathway opened by nsPEF showed strong inward rectification, with maximum conductance increase for the inward current at the most negative membrane potentials. Although these potentials were below the depolarization threshold for VGCC activation, the increase in conductance in cells which expressed VGCC (VGCC+ cells) was about twofold greater than in cells which did not (VGCC− cells). Among VGCC+ cells, the nsPEF-induced increase in membrane conductance showed a positive correlation with the amplitude of VGCC current measured in the same cells prior to nsPEF exposure. These findings demonstrate that the expression of VGCC makes cells more susceptible to membrane permeabilization by nsPEF. Time-lapse imaging of nsPEF-induced Ca²⁺ transients confirmed permeabilization by a single 300-ns pulse at 1.8 or 2.3 kV/cm, but not at 1.4 kV/cm, and the transients were expectedly larger in VGCC+ cells. However, it remains to be established whether larger transients reflected additional Ca²⁺ entry through VGCC, or were a result of more severe electropermeabilization of VGCC+ cells.     

Two Modes of Cell Death Caused by Exposure to Nanosecond Pulsed Electric Field

High-amplitude electric pulses of nanosecond duration, also known as nanosecond pulsed electric field (nsPEF), are a novel modality with promising applications for cell stimulation and tissue ablation. However, key mechanisms responsible for the cytotoxicity of nsPEF have not been established. We show that the principal cause of cell death induced by 60- or 300-ns pulses in U937 cells is the loss of the plasma membrane integrity (“nanoelectroporation”), leading to water uptake, cell swelling, and eventual membrane rupture. Most of this early necrotic death occurs within 1–2 hr after nsPEF exposure. The uptake of water is driven by the presence of pore-impermeable solutes inside the cell, and can be counterbalanced by the presence of a pore-impermeable solute such as sucrose in the medium. Sucrose blocks swelling and prevents the early necrotic death; however the long-term cell survival (24 and 48 hr) does not significantly change. Cells protected with sucrose demonstrate higher incidence of the delayed death (6–24 hr post nsPEF). These cells are more often positive for the uptake of an early apoptotic marker dye YO-PRO-1 while remaining impermeable to propidium iodide. Instead of swelling, these cells often develop apoptotic fragmentation of the cytoplasm. Caspase 3/7 activity increases already in 1 hr after nsPEF and poly-ADP ribose polymerase (PARP) cleavage is detected in 2 hr. Staurosporin-treated positive control cells develop these apoptotic signs only in 3 and 4 hr, respectively. We conclude that nsPEF exposure triggers both necrotic and apoptotic pathways. The early necrotic death prevails under standard cell culture conditions, but cells rescued from the necrosis nonetheless die later on by apoptosis. The balance between the two modes of cell death can be controlled by enabling or blocking cell swelling.     

Effects on capacitance by overexpression of membrane proteins

Functional Channelrhodopsin-2 (ChR2) overexpression of about 10⁴ channels/μm² in the plasma membrane of HEK293 cells was studied by patch-clamp and freeze-fracture electron microscopy. Simultaneous electrorotation measurements revealed that ChR2 expression was accompanied by a marked increase of the area-specific membrane capacitance (C_m). The C_m increase apparently resulted partly from an enlargement of the size and/or number of microvilli. This is suggested by a relatively large C_m of 1.15 ± 0.08 μF/cm² in ChR2-expressing cells measured under isotonic conditions. This value was much higher than that of the control HEK293 cells (0.79 ± 0.02 μF/cm²). However, even after complete loss of microvilli under strong hypoosmolar conditions (100 mOsm), the ChR2-expressing cells still exhibited a significantly larger C_m (0.85 ± 0.07 μF/cm²) as compared to non-expressing control cells (0.70 ± 0.03 μF/cm²). Therefore, a second mechanism of capacitance increase may involve changes in the membrane permittivity and/or thickness due to the embedded ChR2 proteins.     

Nanosecond pulse electric field (nanopulse): a novel non-ligand agonist for platelet activation

Nanosecond pulse stimulation of a variety of cells produces a wide range of physiological responses (e.g., apoptosis, stimulation of calcium (Ca²⁺) fluxes, changes in membrane potential). In this study, we investigated the effect of nanosecond pulses, which generate intense electric fields (nsPEFs), on human platelet aggregation, intracellular free Ca²⁺ ion concentration ([Ca²⁺]_i) and platelet-derived growth factor release. When platelet rich plasma was pulsed with one 300 ns pulse with an electric field of 30 kV/cm, platelets aggregated and a platelet gel was produced. Platelet aggregation was observed with pulses as low as 7 kV/cm with maximum effects seen with approximately 30 kV/cm. The increases in intracellular Ca²⁺ release and Ca²⁺ influx were dose dependent on the electrical energy density and were maximally stimulated with approximately 30 kV/cm. The increases in [Ca²⁺]_i induced by nsPEF were similar to those seen with thapsigargin but not thrombin. We postulate that nsPEF caused Ca²⁺ to leak out of intracellular Ca²⁺ stores by a process involving the formation of nanopores in organelle membranes and also caused Ca²⁺ influx through plasma membrane nanopores. We conclude that nsPEFs dose-dependently cause platelets to rapidly aggregate, like other platelet agonists, and this is most likely initiated by the nsPEFs increasing [Ca²⁺]_i, however by a different mechanism.     

Role of the Transmembrane Potential in the Membrane Proton Leak

The molecular mechanism responsible for the regulation of the mitochondrial membrane proton conductance (G) is not clearly understood. This study investigates the role of the transmembrane potential (ΔΨ_m) using planar membranes, reconstituted with purified uncoupling proteins (UCP1 and UCP2) and/or unsaturated FA. We show that high ΔΨ_m (similar to ΔΨ_m in mitochondrial State IV) significantly activates the protonophoric function of UCPs in the presence of FA. The proton conductance increases nonlinearly with ΔΨ_m. The application of ΔΨ_m up to 220 mV leads to the overriding of the protein inhibition at a constant ATP concentration. Both, the exposure of FA-containing bilayers to high ΔΨ_m and the increase of FA membrane concentration bring about the significant exponential G_m increase, implying the contribution of FA in proton leak. Quantitative analysis of the energy barrier for the transport of FA anions in the presence and absence of protein suggests that FA⁻ remain exposed to membrane lipids while crossing the UCP-containing membrane. We believe this study shows that UCPs and FA decrease ΔΨ_m more effectively if it is sufficiently high. Thus, the tight regulation of proton conductance and/or FA concentration by ΔΨ_m may be key in mitochondrial respiration and metabolism.     

Cutaneous Papilloma and Squamous Cell Carcinoma Therapy Utilizing Nanosecond Pulsed Electric Fields (nsPEF)

Nanosecond pulsed electric fields (nsPEF) induce apoptotic pathways in human cancer cells. The potential therapeutic effective of nsPEF has been reported in cell lines and in xenograft animal tumor model. The present study investigated the ability of nsPEF to cause cancer cell death in vivo using carcinogen-induced animal tumor model, and the pulse duration of nsPEF was only 7 and 14 nano second (ns). An nsPEF generator as a prototype medical device was used in our studies, which is capable of delivering 7–30 nanosecond pulses at various programmable amplitudes and frequencies. Seven cutaneous squamous cell carcinoma cell lines and five other types of cancer cell lines were used to detect the effect of nsPEF in vitro. Rate of cell death in these 12 different cancer cell lines was dependent on nsPEF voltage and pulse number. To examine the effect of nsPEF in vivo, carcinogen-induced cutaneous papillomas and squamous cell carcinomas in mice were exposed to nsPEF with three pulse numbers (50, 200, and 400 pulses), two nominal electric fields (40 KV/cm and 31 KV/cm), and two pulse durations (7 ns and 14 ns). Carcinogen-induced cutaneous papillomas and squamous carcinomas were eliminated efficiently using one treatment of nsPEF with 14 ns duration pulses (33/39 = 85%), and all remaining lesions were eliminated after a 2nd treatment (6/39 = 15%). 13.5% of carcinogen-induced tumors (5 of 37) were eliminated using 7 ns duration pulses after one treatment of nsPEF. Associated with tumor lysis, expression of the anti-apoptotic proteins Bcl-xl and Bcl-2 were markedly reduced and apoptosis increased (TUNEL assay) after nsPEF treatment. nsPEF efficiently causes cell death in vitro and removes papillomas and squamous cell carcinoma in vivo from skin of mice. nsPEF has the therapeutic potential to remove human squamous carcinoma.     

Single-channel analysis of the anion channel-forming protein from the plant pathogenic bacterium Clavibacter michiganense ssp. nebraskense

The anion channel protein from Clavibacter michiganense ssp. nebraskense (Schürholz, Th. et al. 1991, J. Membrane Biol. 123: 1-8) was analyzed at different concentrations of KCl and KF. At 0.8 M KCl the conductance G(V_m) increases exponentially from 21 pS at 50 mV up to 53 pS at V_m = 200 mV, 20°C. The concentration dependence of G(V_m) corresponds to a Michaelis-Menten type saturation function at all membrane voltage values applied (0-200 mV). The anion concentration K_0.5, where G(V_m) has its half-maximum value, increases from 0.12 M at 50 mV to 0.24 M at 175 mV for channels in a soybean phospholipid bilayer. The voltage dependence of the single channel conductance, which is different for charged and neutral lipid bilayers, can be described either by a two-state flicker (2SF) model and the Nernst-Planck continuum theory, or by a two barrier, one-site (2B1S) model with asymmetric barriers. The increase in the number of open channels after a voltage jump from 50 mV to 150 mV has a time constant of 0.8 s. The changes of the single-channel conductance are much faster (<1 ms). The electric part of the gating process is characterized by the (reversible) molar electrical work ΔG^θ_el = ρZ_gFV_m ≈ -1.3 RT, which corresponds to the movement of one charge of the gating charge number |Z_g| = 1 across the fraction ρ = ΔV_m/V_m = 0.15 of the membrane voltage V_m = 200 mV. Unlike with chloride, the single channel conductance of fluoride has a maximum at about 150 mV in the presence of the buffer PIPES (≥5 mM, pH 6.8) with K_0.5 ≈ 1 M. It is shown that the decrease in conductance is due to a blocking of the channel by the PIPES anion. In summary, the results indicate that the anion transport by the Clavibacter anion channel (CAC) does not require a voltage dependent conformation change of the CAC.     

Stability of the Shab K+ channel conductance in 0 K+ solutions: the role of the membrane potential

Shab channels are fairly stable with K⁺ present on only one side of the membrane. However, on exposure to 0 K⁺ solutions on both sides of the membrane, the Shab K⁺ conductance (G_K) irreversibly drops while the channels are maintained undisturbed at the holding potential. Herein it is reported that the drop of G_K follows first-order kinetics, with a voltage-dependent decay rate r. Hyperpolarized potentials drastically inhibit the drop of G_K. The G_K drop at negative potentials cannot be explained by a shift in the voltage dependence of activation. At depolarized potentials, where the channels undergo a slow inactivation process, G_K drops in 0 K⁺ with rates slower than those predicted based on the behavior of r at negative potentials, endowing the r-V_m relationship with a maximum. Regardless of voltage, r is very small compared with the rate of ion permeation. Observations support the hypothesized presence of a stabilizing K⁺ site (or sites) located either within the pore itself or in its external vestibule, at an inactivation-sensitive location. It is argued that part of the G_K stabilization achieved at hyperpolarized potentials could be the result of a conformational change in the pore itself.     

Photosynthetic electron transport activity in heat-treated barley leaves: The role of internal alternative electron donors to photosystem II

Electron transport processes were investigated in barley leaves in which the oxygen-evolution was fully inhibited by a heat pulse (48 °C, 40 s). Under these circumstances, the K peak (∼ F_400 μs) appears in the chl a fluorescence (OJIP) transient reflecting partial Q_A reduction, which is due to a stable charge separation resulting from the donation of one electron by tyrozine Z. Following the K peak additional fluorescence increase (indicating Q_A⁻ accumulation) occurs in the 0.2-2 s time range. Using simultaneous chl a fluorescence and 820 nm transmission measurements it is demonstrated that this Q_A⁻ accumulation is due to naturally occurring alternative electron sources that donate electrons to the donor side of photosystem II. Chl a fluorescence data obtained with 5-ms light pulses (double flashes spaced 2.3-500 ms apart, and trains of several hundred flashes spaced by 100 or 200 ms) show that the electron donation occurs from a large pool with t_1/2 ∼ 30 ms. This alternative electron donor is most probably ascorbate.     

Simultaneous Measurements of Cytoplasmic K Concentration and the Plasma Membrane Electrical Parameters in Single Membrane Samples of Chara corallina

The electrophysiological properties of cytoplasm-rich fragments (single membrane samples) prepared from internodal cells of Chara corallina were explored in conjunction with K⁺-sensitive microelectrode and current-voltage (I-V) measurements. This system eliminated the problem of the inaccessible cytoplasmic layer, while preserving many of the electrical characteristics of the intact cells. In 0.1 millimolar external K concentration (K_o⁺), the resting conductance (membrane conductance G_m, 0.85 ± 0.25 Siemens per square meter (±standard error)) of the single membrane samples, was dominated by the proton pump, as suggested by the response of the near-linear I-V characteristic to changes in external pH. Initial cytoplasmic K⁺ activities (a_K+), judged most reliable, gave values of 117 ± 67 millimolar; stable a_K+ values were 77 ± 31 millimolar. Equilibrium potentials for K⁺ (Nernst equilibrium potential) (E_K) calculated, using either of these data sets, were near the mean membrane potential (V_m). On a cell-to-cell basis, however, E_K was generally negative of the V_m, despite an electrogenic contribution from the Chara proton pump. When K_o⁺ was increased to 1.0 millimolar or above, G_m rose (by 8- to 10-fold in 10 millimolar K_o⁺), the steady state I-V characteristics showed a region of negative slope conductance, and V_m followed E_K. These results confirm previous studies which implicated a K_o⁺-induced and voltage-dependent permeability to K⁺ at the Chara plasma membrane. They provide an explanation for transitions between apparent K_o⁺-insensitive and K_o⁺-sensitive (`K⁺ electrode') behavior displayed by the membrane potential, as recorded in many algae and higher plant cells.     

Selective cytotoxicity of intense nanosecond-duration electric pulses in mammalian cells

Background

Nanosecond electric pulses (EP) disrupt cell membrane and organelles and cause cell death in a manner different from the conventional irreversible electroporation. We explored the cytotoxic effect of 10-ns EP (quantitation, mechanisms, efficiency, and specificity) in comparison with 300-ns, 1.8- and 9-μs EP.

Methods

Effects in Jurkat and U937 cells were characterized by survival assays, DNA electrophoresis and flow cytometry.

Results

10-ns EP caused apoptotic or necrotic death within 2–20 h. Survival (S, %) followed the absorbed dose (D, J/g) as: S = αD^(−K), where coefficients K and α determined the slope and the “shoulder” of the survival curve. K was similar in all groups, whereas α was cell type- and pulse duration-dependent. Long pulses caused immediate propidium uptake and phosphatidylserine (PS) externalization, whereas 10-ns pulses caused PS externalization only.

Conclusions

1.8- and 9-μs EP cause cell death efficiently and indiscriminately (LD₅₀ 1–3 J/g in both cell lines); 10-ns EP are less efficient, but very selective (LD₅₀ 50–80 J/g for Jurkat and 400–500 J/g for U937); 300-ns EP show intermediate effects. Shorter EP open propidium-impermeable, small membrane pores (”nanopores”), triggering different cell death mechanisms.

General significance

Nanosecond EP can selectively target certain cells in medical applications like tumor ablation.     

Are Orai1 and Orai3 channels more important than calcium influx for cell proliferation?

Transformed and tumoral cells share the characteristic of being able to proliferate even when external calcium concentration is very low. We have investigated whether Human Embryonic Kidney 293 cells, human hepatoma cell Huh-7 and HeLa cells were able to proliferate when kept 72 h in complete culture medium without external calcium. Our data showed that cell proliferation rate was similar over a range of external calcium concentration (2 μM to 1.8 mM). Incubation in the absence of external calcium for 72 h had no significant effect on endoplasmic reticulum (ER) Ca^2 + contents but resulted in a significant decrease in cytosolic free calcium concentration in all 3 cell types. Cell proliferation rates were dependent on Orai1 and Orai3 expression levels in HEK293 and HeLa cells. Silencing Orai1 or Orai3 resulted in a 50% reduction in cell proliferation rate. Flow cytometry analysis showed that Orai3 induced a small but significant increase in cell number in G₂/M phase. RO-3306, a cdk-1 inhibitor, induced a 90% arrest in G₂/M reversible in less than 15 min. Our data showed that progression through G₂/M phase after release from RO-3306-induced cell cycle arrest was slower in both Orai1 and Orai3 knock-downs. Overexpressing Orai1, Orai3 and the dominant negative non-permeant mutants E106Q-Orai1 and E81Q-Orai3 induced a 50% increase in cell proliferation rate in HEK293 cells. Our data clearly demonstrated that Orai1 and Orai3 proteins are more important than calcium influx to control cell proliferation in some cell lines and that this process is probably independent of I_CRAC and I_arc.     

Calcium effects on electrogenic pump and passive permeability of the plasma membrane ofChara corallina

Summary Removal of Ca²⁺ from the medium results in depolarization of theChara internodal cell and an increase in membrane conductance (G _m). The increase in conductance is associated with an increase in K⁺ conductance, as judged by Ca²⁺ effects on the K⁺ dependence of clamp current. The voltage dependence ofG _m is also affected by Ca²⁺, as is the time course of the response of clamp current to a step change in voltage. Mg²⁺ restores the low conductance and the fast response to a voltage change, but not hyperpolarization at neutral pH, suggesting that there is an additional, independent effect on the electrogenic pump. The membrane does not show the normal ability to increase proton conductance at high pH in the absence of Ca²⁺; this is also restored by Mg²⁺ as well as by Ca²⁺.     

Effects of cell culture density on phagocytosis parameters in IC-21 macrophages

Cell culture density is shown to alter the parameters characterizing phagocytic activity of cells in vitro. Phagocytosis index (PI, mean number of beads per cell in the bead-containing population) and phagocytosis percent (PP, percentage of bead-containing cells in cell population under study) for IC-21 macrophages incubated in the presence of non-opsonized 2-μm fluorescent latex beads were determined using fluorescent microscopy and ImageJ software specially adapted for the purpose. Under control conditions (DMEM without serum), increase in cell culture density was accompanied with a decrease of both parameters of the phagocytic activity. At a mean density of 4 cells/10⁵ μm² (9 cells per a viewfield) PI was 7.1 ± 0.2 beads/cell and at 20 cells/10⁵ μm² (40 cells per a viewfield) PI dropped to 4.6 ± 0.1 beads/cell. PP was less sensitive, varied in the range of 95–100% but also decreased as the cell density grew. At any density, PI was 1.5–2 times higher than the expected value (number of beads per μm² × cell contour area); apparently this divergence can be accounted for by cell locomotion and capture of a larger number of beads than could drop onto a motionless cell with a constant contour area. Increase in cell density was also accompanied by a decrease of the cell contour area (S _c), which amounted to 750 ± 16 μm² at a density of 4 cells/10⁵ μm² and 346 ± 4 μm² at a density of 20 cells/10⁵ μm². As the bead concentration was the same in all experiments, density-dependent decrease in PI and PP may be related with the observed decrease in cell contour area. Yet, the bead number per cell area unit (PI/S _c) was bigger at higher density and PI/S _c was higher in cells with smaller S _c. Thus, individual (specific) activity of the cells did not lessen with an increase of the cell culture density in the range studied (4–20 cells/10⁵ μm²). Reduction of the cell contour area may reflect alteration in cell adhesion to the substrate as well as competitive relations between adhesion and phagocytic processes. The data obtained imply that cell culture density has to be controlled as a factor notably altering the phagocytic activity parameters. The effects of serum, methyl-β-cyclodextrin, and carbenoxolon reported earlier [Golovkina et al. 2009. Biol membrany. 26 (5), 379–386] are re-evaluated and confirmed here.     

Studies on the relationship between pulsed UV light irradiation and the simultaneous occurrence of molecular and cellular damage in clinically-relevant Candida albicans

This constitutes the first study to report on the relationship between pulsed UV light (PL) irradiation and the simultaneous occurrence of molecular and cellular damage in clinical strains of Candida albicans. Microbial protein leakage and propidium iodide (PI) uptake assays demonstrated significant increases in cell membrane permeability in PL-treated yeast that depended on the amount of UV pulses applied. This finding correlated well with the measurement of increased levels of lipid hydroperoxidation in the cell membrane of PL-treated yeast. PL-treated yeast cells also displayed a specific pattern of intracellular reactive oxygen species (ROS) generation, where ROS were initially localised in the mitochondria after low levels of pulsing (UV dose 0.82 μJ/cm²) before more wide-spread cytosolic ROS production occurred with enhanced pulsing. Intracellular ROS levels were measured using the specific mitochondrial peroxide stain dihydrorhodamine 123 and the cytosolic oxidation stain dichloroflurescin diacetate. Use of the dihydroethidium stain also revealed increased levels of intracellular superoxide as a consequence of augmented pulsing. The ROS bursts observed during the initial phases of PL treatment was consistent with the occurrence of apoptotic cells as confirmed by detection of specific apoptotic markers, abnormal chromatin condensation and externalisation of cell membrane lipid phosphatidylserine. Increased amount of PL-irradiation (ca. UV does 1.24-1.65 μJ/cm²) also resulted in the occurrence of late apoptotic and necrotic yeast phenotypes, which coincided with the transition from mitochondrial to cytosolic localisation of ROS and with irreversible cell membrane leakage. Use of the comet assay also revealed significant nuclear damage in similarly treated PL samples. Although some level of cellular repair was observed in all test strains during sub-lethal exposure to PL-treatments (≤ 20 pulses or UV dose 0.55 μJ/cm²), this was absent in similar samples exposed to increased amounts of pulsing. This study showed that PL-irradiation inactivates C. albicans test strains through a multi-targeted process with no evidence of microbial ability to support cell growth after ≤ 20 pulses. Implications of our findings in terms of application of PL for contact-surface disinfection are discussed.     

Effect of adherence,cell morphology,and lipopolysaccharide on potassium conductance and passive membrane properties of murine macrophage J774.1 cells

Summary The effects of adherence, cell morphology, and lipopolysaccharide on electrical membrane properties and on the expression of the inwardly rectifying K conductance in J774.1 cells were investigated. Whole-cell inwardly rectifying K currents (K _i), membrane capacitance (C _m), and membrane potential (V _m) were measured using the patch-clamp technique. SpecificK _i conductance (G _K i, whole-cell Ki conductance corrected for leak and normalized to membrane capacitance) was measured as a function of time after adherence, and was found to increase almost twofold one day after plating. Membrane potential (V _m) also increased from –42±4 mV (n=32) to –58±2 mV (n=47) over the same time period.G _K i andV _m were correlated with each other;G _L (leak conductance normalized to membrane capacitance) andV _m were not. The magnitudes ofG _K i andV _m 15 min to 2 hr after adherence were unaffected by the presence of 100 m cycloheximide, but the increase inG _K iandV _m that normally occurred between 2 and 8 hr after adherence was abolished by cycloheximide treatment. Membrane properties were analyzed as a function of cell morphology, by dividing cells into three categories ranging from small round cells to large, extremely spread cells. The capacitance of spread cells increased more than twofold within one day after adherence, which indicates that spread cells inserted new membrane. Spread cells had more negative resting membrane potentials than round cells, butG _K i andG _L were not significantly different. Lipopolysaccharide-(LPS; 1 or 10 g/ml) treated cells showed increasedC _m compared to control cells plated for comparable times. In contrast to the effect of adherence, LPS-treated cells exhibited a significantly lowerG _K i than control cells, indicating that the additional membrane did not have as high a density of functionalG _K i channels. We conclude that both adherence and LPS treatment increase the total surface membrane area of J774 cells and change the density of Ki channels. In addition, this study demonstrates that membrane area and density of Ki channels can vary independently of one another.