The electrical breakdown of cell and lipid membranes: the similarity of phenomenologies

The current responses of human erythrocyte and L-cell membranes being subject to rectangular voltage pulses of 150-700 mV amplitude and 5 X 10(-3)-10 s duration were recorded by means of the patch-clamp method. The behaviour of planar lipid bilayer membranes of oxidized cholesterol and UO2(2+)-modified bilayers of azolectin in a high electric field was investigated for comparison. The gradual growth in the conductance (reversible electrical breakdown) was found for both the cell membranes and lipid bilayers of the compositions studied, with the application of voltage pulses of sufficient duration, to be completed by its drastic enhancement (irreversible breakdown). The time interval preceding the irreversible breakdown and the rate of increase in conductance during the reversible breakdown are determined by the amplitude of the voltage applied. The recovery of the initial properties of the membrane following the reversible breakdown consists of the two stages, the latter substantially differing by their characteristic times. The first very rapid stage (tau much less than 1 ms) reflects the lowering of the conductance of small pores with decreasing voltage across the membrane. The diminishing of the number and mean radii of the pores resulting in their complete disappearance occurs only at the second stage of membrane healing, which lasts several seconds or even minutes. The phenomenological similarity of the cell and lipid membrane breakdown indicates that pores developed during the electrical breakdown of biological membranes arise in their lipid matrices. The structure and the properties of the pores are discussed.     

The breakdown of cell membranes by electrical and mechanical stress.

We attempted to determine whether mechanical tension and electrical stress couple to cause membrane breakdown in cells. Using cell-attached patches from HEK293 cells, we estimated the mechanically produced tension from the applied pressure and geometry of the patch. Voltage pulses of increasing amplitude were applied until we observed a sudden increase in conductance and capacitance. For pulses of 50 micros duration, breakdown required >0.5 V and was dependent on the tension. For pulses of 50-100 ms duration, breakdown required 0.2-0.4 V and was independent of tension. Apparently two physically different processes can lead to membrane breakdown. We could explain the response to the short, high-voltage pulses if breakdown occurred in the lipid bilayer. The critical electromechanical energy per unit area for breakdown by short pulses was approximately 4 dyne/cm, in agreement with earlier results on bilayers. Our data suggest that, at least in a patch, the bilayer may hold a significant fraction (approximately 40%) of the mean tension. To be compatible with the large, nonlytic area changes of patches, the bilayer appears to be pulled toward the pipette tip, perhaps by hydrophobic forces wetting membrane proteins bound to the glass. Although breakdown voltages for long pulses were in agreement with earlier work on algae, the mechanism(s) for this breakdown remain unclear.     

Electrical breakdown of erythrocyte membranes during UV-radiation

The electric stability of erythrocyte membrane was shown to reduce under UV-radiation. The disturbing action of UV-radiation depends on the value of membrane potential difference.     

On the effect of prestin on the electrical breakdown of cell membranes

The voltage-dependent activity of prestin, the outer hair cell (OHC) motor protein essential for its electromotility, enhances the mammalian inner ear's auditory sensitivity. We investigated the effect of prestin's activity on the plasma membrane's (PM) susceptibility to electroporation (EP) via cell-attached patch-clamping. Guinea pig OHCs, TSA201 cells, and prestin-transfected TSA cells were subjected to incremental 50 mus and/or 50 ms voltage pulse trains, or ramps, at rates from 10 V/s to 1 kV/s, to a maximum transmembrane potential of +/-1000 mV. EP was determined by an increase in capacitance to whole-cell levels. OHCs were probed at the prestin-rich lateral PM or prestin-devoid basal portion; TSA cells were patched at random points. OHCs were consistently electroporated with 50 ms pulses, with significant resistance to depolarizing pulses. Although EP rarely occurred with 50 mus pulses, prior stimulation with this protocol had a significant effect on the sensitivity to EP with 50 ms pulses, regardless of polarity or PM domain. Consistent with these results, resistance to EP with depolarizing 10-V/s ramps was also found. Our findings with TSA cells were comparable, showing resistance to EP with both depolarizing 50-ms pulses and 10 V/s ramps. We conclude prestin significantly affects susceptibility to EP, possibly via known biophysical influences on specific membrane capacitance and/or membrane stiffness.     

An investigation of electrical breakdown of bimolecular lipid membranes

The investigation is concerned with the irreversible electrical breakdown of bimolecular lipid membranes, depending on the velocity of linear voltage scanning. It was found that the membrane breakdown potential depended on the velocity of electric field variation. For instance, at voltage scanning velocities of up to 0.1 V/s, the rupture of membrane from glycerol monooleate occurs at 0.20–0.25 V and, at velocities higher than 1 V/s, at 0.5–0.6 V. Then the film breakdown depending on lipid phase transition was studied. At high velocities of imposed voltage scanning, the disruption of the bimolecular lipid membranes was shown not to depend on their phase states; at the same time, at low velocities, one could note a slight difference in the stability of the films at temperatures higher and lower than those of the phase transition. Whereas transition from gel to liquid-crystalline state involves transition from an ordered to a less ordered membrane structure with a sharp increase in the number of defects in the membrane, the authors, conclude that the film breakdown in the second case occurs by the ‘defect’ mechanism suggested earlier. It was also assumed that, in certain cases involving low velocities of voltage scanning, membrane breakdown may occur because of variation in the interfacial tension and in the contact angle between the film and torus. Possible mechanisms of the membrane irreversible electrical breakdown at high velocities of voltage variation are discussed. It was shown that breakdown should occur as a result of membrane compression in an electric field by a mechanism previously examined. The elastic moduli of a number of membranes were calculated by the breakdown criterion suggested earlier. They were found to coincide with the results of other investigators and, depending on the type of lipid, to equal 10⁵–10⁶ Pa.     

Reversible electrical breakdown of lipid bilayer membranes: A charge-pulse relaxation study

Summary Charge-pulse experiments were performed with lipid bilayer membranes from oxidized cholesterol/n-decane at relatively high voltages (several hundred mV). The membranes show an irreversible mechanical rupture if the membrane is charged to voltages on the order of 300 mV. In the case of the mechanical rupture, the voltage across the membrane needs about 50–200 sec to decay completely to zero. At much higher voltages, applied to the membrane by charge pulses of about 500 nsec duration, a decrease of the specific resistance of the membranes by nine orders of magnitude is observed (from 10⁸ to 0.1 cm²), which is correlated with the reversible electrical breakdown of the lipid bilayer membrane. Due to the high conductance increase (breakdown) of the bilayer it is not possible to charge the membrane to a larger value than the critical potential differenceV _c. For 1m alkali ion chloridesV _c was about 1 V. The temperature dependence of the electrical breakdown voltageV _c is comparable to that being observed with cell membranes.V _c decreases between 2 and 48°C from 1.5 to 0.6 V in the presence of 1m KCl.Breakdown experiments were also performed with lipid bilayer membranes composed of other lipids. The fast decay of the voltage (current) in the 100-nsec range after application of a charge pulse was very similar in these experiments compared with experiments with membranes made from oxidized cholesterol. However, the membranes made from other lipids show a mechanical breakdown after the electrical breakdown, whereas with one single membrane from oxidized cholesterol more than twenty reproducible breakdown experiments could be repeated without a visible disturbance of the membrane stability.The reversible electrical breakdown of the membrane is discussed in terms of both compression of the membrane (electromechanical model) and ion movement through the membrane induced by high electric field strength (Born energy).     

The mechanism of electrical breakdown in the membranes ofValonia utricularis

Summary The dielectric breakdown in the membranes of cells ofValonia utricularis was investigated using intracellular electrodes and 500-sec current pulses. Electrical breakdown, which occurs when the membrane potential reaches a well-defined critical value, is not associated with global damage to the cell or its membranes (the membrane reseals in <5 sec). It was thus possible to investigate the effect of temperature on dielectric breakdown in single cells. It was found that the critical potential for breakdown was strongly dependent on temperature, decreasing from 1000 mV at 4°C to 640 mV at 30°C. The decrease in the breakdown potential with increasing temperature and the very short rise-time of the breakdown current (1 sec) suggests that the Wien field dissociation does not play a major role in the breakdown process. It is shown that the nonlinearI–V characteristics observed at different temperatures can be accurately accounted for with no adjustable parameters, by considerations of the mechanical compression of the membrane due to stresses induced by the electric field. Electrical breakdown on this scheme results from an electromechanical instability in the membrane. On this basis the present results indicate that the elastic modulus of the region of the membrane where breakdown occurs, decreases by a factor of 2 with increasing temperature from 4 to 30°C. On the assumption of a thickness of 4.0 nm and a dielectric constant of 5, the elastic modulus is estimated to have a value of 5×10⁶ Nm^–2 at 20°C.     

Pulse-length dependence of the electrical breakdown in lipid bilayer membranes

Charge-pulse experiments were performed on artificial lipid bilayer membranes with charging times in the range between 10 ns and 10 μs. If the membranes are charged to voltages in the order of 100 mV, the membrane voltage at the end of the charge pulse is a linear function of the injected charge. However, if the membranes are charged to voltages in the range of 1 V, this relationship no longer holds and a reversible high conductance state occurs. This state is defined as an electrical breakdown and it does not allow the membranes to charge to higher voltages than the breakdown voltage, $\text{V}{}_{\mathrm{<mtext>c</mtext>}}$. Between charging times of 300 ns and 5 μs at 25°C and between 100 ns and 2 μs at 40°C, $\text{V}{}_{\mathrm{<mtext>c</mtext>}}$ showed a strong dependence on the charging time of the membrane and decreased from 1.2 to 0.5 V (25°C) and from 1 to 0.4 V (40°C). For other charging times below and above these ranges, the breakdown voltage seemed to be constant. The results indicate that the breakdown phenomenon occurs in less than 10 ns.The pulse-length dependence of the breakdown voltage is consistent with the interpretation of the electrical breakdown mechanism in terms of the electromechanical model. However, it seems possible that below a charging time of the membrane of 300 ns (25°C) and 100 ns (40°C) other processes (such as the Born energy) become possible.     

Electrical injury mechanisms: dynamics of the thermal response

The thermal response of the human upper extremity to large electric currents was examined using an axisymmetric unidimensional model containing bone, skeletal muscle, fat, and skin in coaxial cylindrical geometry. Appropriate thermal and electrical properties were assigned to each tissue, and the tissue response to joule heating was determined by a finite-element numerical technique. We found that when the tissues are electrically in parallel, skeletal muscle sustained the largest temperature rise and then heated adjacent tissues. Thus, when bone is not in series with other tissues, joule heating of bone is unlikely to be responsible for thermal damage to adjacent tissue. In addition, the effect of tissue perfusion on the thermal response was found to be essential for rapid cooling of the centrally located tissues.     

Kinetics of pore size during irreversible electrical breakdown of lipid bilayer membranes.

The kinetics of pore formation followed by mechanical rupture of lipid bilayer membranes were investigated in detail by using the charge-pulse method. Membranes of various compositions were charged to a sufficiently high voltage to induce mechanical breakdown. The subsequent decrease of membrane voltage was used to calculate the conductance. During mechanical breakdown, which was probably caused by the widening of one single pore, the membrane conductance was a linear and not exponential function of time after the initial starting process. In a large number of experiments using various lipids and electrolytes, the characteristic opening process of the pore turned out to be independent of the actual membrane potential and electrolyte concentration. Our theoretical analysis of the pore formation suggested that the voltage-induced irreversible breakdown is due to a decrease in edge energy when the pore had formed. After initiation of the pore, the electrical contribution to surface tension is negligible. The time course of the increase of pore size shows that our model of the irreversible breakdown is in good agreement with mechanical properties of membranes reported elsewhere.     

Fusion of Avena sativa mesophyll cell protoplasts by electrical breakdown

Studies with the light microscope were carried out on mesophyll cell protoplasts of Avena sativa which had been made to undergo fusion by reversible electrical breakdown of the cell membrane. In order to establish close membrane contact between the cells, an important prerequisite for fusion, a method known as dielectrophoresis was used. In an inhomogeneous alternating electrical field the protoplasts adhere to the electrodes and to each other in the direction of the field lines. The cells which were thus brought into close contact with each other could be made to fuse by the application of a field pulse of high amplitude (about 750 V/cm) and short duration (20–50 μs). The field strength required for fusion exceeds the value necessary for the electrical breakdown of the cell membrane. Fusion took place within some minutes and led to a high yield of fused protoplasts. The fusion of cells being in the electric field occured in a synchronous manner. In some of the fusion experiments part of the protoplasts of A. sativa were stained with neutral red. When these cells were fused with unstained protoplasts, the vacuoles from the different cells within the fused aggregate could be shown to remain separate for quite some time.     

Electric field-induced breakdown of lipid bilayers and cell membranes: A thin viscoelastic film model

Summary A simple viscoelastic film model is presented, which predicts a breakdown electric potential having a dependence on the electric pulse length which approximates the available experimental data for the electric breakdown of lipid bilayers and cell membranes (summarized in the reviews of U. Zimmermann and J. Vienken, 1982,J. Membrane Biol. 67:165 and U. Zimmermann, 1982,Biochim. Biophys. Acta 694:227). The basic result is a formula for the time of membrane breakdown (up to the formation of pores): =(/C)/( _m ² ₀ ² U ⁴/24Gh ³+T ²/Gh–1), where is a proportionality coefficient approximately equal to ln(h/2₀),h being the membrane thickness and ₀ the amplitude of the initial membrane surface shape fluctuation ( is usually of the order of unity), represents the membrane shear viscosity,G the membranes shear elasticity modules, _m the membrane relative permittivity, ₀=8.85×10^–12 Fm,U the electric potential across the membrane, the membrane surface tension andT the membrane tension. This formula predicts a critical potentialU _c ;U _c =(24Gh ³/ _m ² ₀ ² )^1/4 (for = andT=0). It is proposed that the time course of the electric field-induced membrane breakdown can be divided into three stages: (i) growth of the membrane surface fluctuations, (ii) molecular rearrangements leading to membrane discontinuities, and (iii) expansion of the pores, resulting in the mechanical breakdown of the membrane.     

The effect of pressure on the electrical breakdown in the membranes of Valonia utricularis

The interpretation of electrical breakdown in terms of electro-mechanical instabilities, predicts that the breakdown potential should decrease with increasing cell turgor pressure.Experiments were conducted to test this hypothesis on cells of Valonia utricularis over a turgor pressure range of 0.5 · 10⁵–5.0 · 10⁵ N/m². Electrical breakdown was measured using intracellular electrodes and 500 μs current pulses. The pressure was monitored by an intracellular micropipette pressure transducer. The results obtained show a linear decrease in the critical breakdown potential with pressure. The effective compressive modulus of the cell membrane, γ, is calculated from the slope of this line to 69 ± 10 · 10⁵N/m² (average value of seven measurements). This is consistent with the theoretical prediction of the electromechanical model using our previously determined values of the elastic modulus of the membrane.A theoretical analysis is given of the effects of pressure on the breakdown. This includes also considerations of the indirect effect of pressure on the membrane via stretching of the cell wall with a possible coupling of such strains to the cell membrane. The results and analysis presented allow us to conclude on the basis of the experimentally determined breakdown P.D. of 959 mV that the region of membrane where electrical breakdown occurs is a dielectric with one of the following combinations of parameters: (A) a thickness δ = 7–9 nm with a dielectric constant ? = >10, e.g. a hydrated protein spanning the whole membrane. (B) δ = 4–5 nm with ? = 3–8, e.g. a lipoprotein of lipid bilayer dimensions. (C) δ ≈ 2 nm with ? = 2–3, e.g. a half lipid bilayer.If we assume that the breakdown P.D. of the tonoplast and plasmalemma are identical, that is 480 mV, then there is only one reasonable choice for the membrane thickness and the dielectric constant: δ = 2nm, ? = 3–8, e.g. a (lipo-)proteinaceous module facing a half lipid bilayer.     

Electrical properties of parenchymal cell membranes in the oat coleoptile

Summary Parenchymal cells of oat (Avena sativa) coleoptiles had an osmotic concentration of 410 mM (determined by plasmolysis); of this only 22 mM was K⁺ and 1 mM Na⁺ (flame photometry). Cells were impaled with micropipette electrodes. Iontophoretic injection of the dye Niagara sky-blue from the micropipette showed that the tip of the electrode penetrated the vacuole. When sections of tissue were immersed in a solution of 22 mM KCl, 1 mM CaCl₂, and 50 mM glucose, average membrane potential was found to be 38.5 mV inside negative specific membrane resistance was 510 cm², and specific membrane capacitance, 2 f cm^-2. The cell membranes showed <25% retification and no electrical excitability. Electrotonic coupling of adjacent cells could not be demonstrated.     

Lipopolysaccharides in liver injury: molecular mechanisms of Kupffer cell activation

Endogenous gut-derived bacterial lipopolysaccharides have been implicated as important cofactors in the pathogenesis of liver injury. However, the molecular mechanisms by which lipopolysaccharides exert their effect are not entirely clear. Recent studies have pointed to proinflammatory cytokines such as tumor necrosis factor-alpha as mediators of hepatocyte injury. Within the liver, Kupffer cells are major sources of proinflammatory cytokines that are produced in response to lipopolysaccharides. This review will focus on three important molecular components of the pathway by which lipopolysaccharides activate Kupffer cells: CD14, Toll-like receptor 4, and lipopolysaccharide binding protein. Within the liver, lipopolysaccharides bind to lipopolysaccharide binding protein, which then facilitates its transfer to membrane CD14 on the surface of Kupffer cells. Signaling of lipopolysaccharide through CD14 is mediated by the downstream receptor Toll-like receptor 4 and results in activation of Kupffer cells. The role played by these molecules in liver injury will be examined.     

Theoretical study on the mechanisms of polyethylene electrical breakdown strength increment by the addition of voltage stabilizers

Journal of Molecular Modeling - Glycoprotein D (gD) is an essential protein of herpes simplex virus-1 (HSV-1) that targets the structurally unrelated receptors HVEM and nectin-1. Receptor binding...     

Electrical resistance of rabbit submaxillary main duct: A tight epithelium with leaky cell membranes

Summary The electrical resistance of rabbit salivary main duct epithelium has been measured. A small axial electrode, which passed current and measured potential simultaneously, was placed inside the ductal lumen. A cylindrical spiral was wound around the main duct and served as outside current electrode. The instantaneous current voltage relations were linearly up to current densities of 1.5 mA/cm², independently of the Cl concentration in the bathing solutions. Strong polarization effects were observed in low Cl solutions. There was a significant inverse correlation between the spontaneous potential difference across the epithelium and the epithelial resistance in solutions with either high or low Cl concentrations. In high Cl solutions the epithelial resistance was 12.2±1.8 (n=7) cm². The resistance increased when the mucosal Na and Cl concentrations decreased. After addition of ouabain the resistance always decreased. The temperature dependence of the resistance was determined, and apparent activation energies were calculated. Values for activation energies ranged from 3.2 to 6.5 kcal/mol, depending on the ionic composition of the bathing solutions. Addition of amiloride to the mucosal solution led to an increase in resistance by a factor of 2.1 in high Cl solutions and of 4.1 in low Cl solutions. When ouabain was applied before amiloride, there was no effect on the resistance in high Cl solutions and a smaller increase in the resistance in low Cl solutions. The results of this study support the conclusion that the low resistance of main duct epithelium resides in the cell membranes and is not due to a paracellular pathway.