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).     

Fluorescence measurements of environmental relaxation at the lipid-water interface region of bilayer membranes

Nanosecond time-resolved emission spectroscopy is used to characterize the complex fluorescence behavior of the probe 2-p-toluidinonaphthalene 6-sulfonate (2,6 p-TNS) when adsorbed to several bilayer membrane system. These include egg phosphatidylcholine vesicles with and without added cholesterol as well as erythrocyte ghost membranes. In each case a nanosecond time-dependent shift of the fluorescence emission to lower energy follows pulsed photoexcitation. The properties of the time-resolved surfaces obtained are consistent with a non-exponential decay law which describes a continuous interaction process of 2,6 p-TNS with its local environment in the membrane. This environment consists in part of polar residues (water plus polar head region) undergoing nanosecond motions. The pure phosphatidylcholine bilayer system was studied at four temperatures and electronic and spectral relaxation contributions to the total fluorescence decay were separated. Temperature coefficients for empirical rate parameters derived for the separated processes were obtained. It appears that a treatment of the fluorescence behavior of amphiphilic probes such as 2,6 p-TNS adsorbed to bilayer membranes at temperatures near ambient in which a single lifetime and radiative decay channel have been assumed is inappropriate.     

A study of the inhomogeneity of bilayer lipid membranes by measurements of higher harmonics of transmembrane current

Higher harmonics of alternating current in bilayer lipid membranes caused by sinusoidal voltage applied to the membrane were measured. The bilayer lipid membranes were prepared from diphytanoylphosphatidylcholine in n-decane and n-tetradecane, and measurements were conducted with the aid of an analog-to-digital converter of 16th category. Sinusoidal voltage was formed using a digital-to-analog converter of the 16th category. The dynamic region of measurements was up 90 dB. The results of measurements were used to determine the alpha and beta coefficients of the expansion of membrane capacity C in terms of membrane voltage U C = C0 (1 + alphaU2 + betaU4). We showed in the framework of the electrostriction model that the relation between the alpha and beta coefficients characterizes the inhomogeneity of bilayer lipid membrane with respect to its thickness and Young modulus of elasticity.     

Interactions of proteins and cholesterol with lipids in bilayer membranes

Mixtures of lipids and proteins, the ATPase from rabbit sarcoplasmic reticulum, were studied by freeze-fracture electron microscopy and by measurement of the amount of fluid lipid with the spin label 2,2,6,6-tetramethylpiperidine-1-oxyl (TEMPO). In dimyristoyl phosphatidylcholine vesicles the protein molecules were randomly distributed above the transition temperature, $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$, of the lipid and aggregated below $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$. For mixtures af dimyristoyl and dipalmitoyl phosphatidylcholine the existence of fluid and solid domains was shown in the temperature interval predicted from earlier TEMPO measurements. When protein was incorporated into this lipid mixture, freeze-fracture particles were randomly distributed in fluid lipids, or aggregated when only solid lipids were present.In mixtures of dimyristoyl phosphatidylcholine with cholesterol the protein was distributed randomly above the transition temperature of the phosphatidylcholine. Below that transition temperature the protein was excluded from a banded phase of solid lipid in the case of 10 mol% cholesterol. In mixtures containing 20 mol% cholesterol, protein molecules formed linear arrays, 50–200 nm in length, around smooth patches of lipid.Phase diagrams for lipid/cholesterol and lipid/protein systems are proposed which account for many of the available data. A model for increasing solidification of lipid around protein molecules or cholesterol above the transition temperarture of the lipid is discussed.     

Photo-voltages of bilayer lipid membranes in the presence of cyanine dyes.

The transmembrane photo-voltage waveforms induced by 10 different cyanine dyes absorbed to one side of bilayer lipid membranes are described. The membranes were prepared from lecithin, oxidized cholesterol, and mixed lecithin and oxidized cholesterol. An 8-mus flash illumination was used. Three dyes induced a photo-voltage which developed in a few milliseconds, then discharged in less than the membranes' resistance-capacitance time. Five dyes induced a photo-voltage which increased for much longer than the membranes' resistance-capacitance time. Two dyes did not induce any photo-electric effects. Models are presented which correlate the dye structure with the type of photo-voltage waveform induced.     

Mechanism of potential-dependent light absorption changes of lipid bilayer membranes in the presence of cyanine and oxonol dyes

Summary The mechanism by which the light absorption of cyanine and oxonol dyes changes in response to changes in transmembrane electrical potential has been studied. Trains of membrane potential steps produce changes in the intensity of light passing through glycerylmonooleate (GMO) bilayer lipid membranes (BLM) in the presence of these dyes. The size of the signal-averaged absorbance change for one of the cyanine dyes diS-C₂-(5) is 10^–5. The response time for the absorbance change of all of the dyes was 10 sec. In order for an absorption signal to be observed, the concentration of dye on both sides of the membrane must be different. Since GMO bilayer membranes are permeable to the charged dyes that were studied, the dye concentration asymmetry necessary for the optical signal had to be maintained with a constant dc membrane potential, onto which the trains of potential steps were superimposed. The more hydrophobic dyes were the most permeant. Inclusion of cholesterol in the GMO bilayers decreased the permeance of the positively charged cyanine dyes, but increased the permeance of the negatively charged oxonol dyes. The magnitude and the size of the BLM absorbance change depended on the wavelength of illumination. Comparisons of the wavelength dependence of the BLM spectra with absorption difference spectra obtained with model membrane systems allow us to postulate a mechanism for a BLM absorbance change. For the cyanine and oxonol dyes, the data are consistent with an ON-OFF mechanism where a quantity of dye undergoes a rapid potential-dependent movement between a hydrocarbon-like binding site on the membrane and the aqueous salt solution near the membrane. For some dyes, which readily aggregate on the membrane, part of the absorbance change may possibly be explained by a potential dependent change in the state of aggregation of dye molecules localized on the membrane. Mechanisms involving a potential dependent change in the polarizability of the environment of membrane-localized dye molecules cannot be excluded, but seem unlikely.     

A comparative study of cell death using electrical capacitance measurements and dielectrophoresis

The changes in the dielectric properties of cells that occur during their exposure to various lethal environmental stresses were measured using both dielectric spectroscopy and dielectrophoresis. It is shown that the dielectric properties of both dying and dead yeast cells were strongly dependent on the method used to induce cell death. Methods which directly affected the membrane permeability, and consequently the membrane conductivity and internal conductivity, resulted in large changes in the suspension capacitance and dielectrophoretic behaviour, whilst methods which affected the cell interior but had little effect on the cell membrane resulted in few or no changes in the dielectric properties of the cells. The findings indicate that, depending on the method by which cell death is induced, dielectric spectroscopy may not always be able to observe differences between viable and non-viable cells, and that dielectrophoresis will not always be able to separate viable from non-viable cells.     

Viscoelastic relaxation of bilayer lipid membranes. Frequency-dependent tension and membrane viscosity.

Photon correlation spectroscopy has been used to study capillary waves on black lipid membranes of glycerol monooleate at temperatures above the lipid transition. For the first time the tension and viscosity of solvent-free bilayers have been observed to display a frequency dependence. The variations of both parameters can be accounted for by a Maxwell viscoelastic fluid model having a relaxation time of 37 microseconds. The equilibrium (omega = 0) tension is compatible with literature values. The present results do not suffice to precisely define the specific molecular processes involved, but relaxation times similar to the present are associated with certain phenomena in phospholipid vesicles. Bilayers containing hydrocarbon solvent do not show such relaxation, presumably due to their weaker intermolecular interactions.     

Properties of the conductance induced in lecithin bilayer membranes by alamethicin

Current-voltage relations have been measured across lecithin bilayers doped with alamethicin molecules. The results show that there are two aspects of the induced conductances, a voltage-dependent and a voltage-independent conductance. Both have been characterized as a function of alamethicin and KCl concentration. The two aspects of the conductances do not show the same changes with those two variables. The voltage-independent conductance is affected very little by changes in KCl concentration, and its dependance on alamethicin concentration reveals that it is produced by two or three alamethicin molecules. The voltage-dependent conductance is shifted by the changes in KCl concentration only when the concentrations are greater than or equal to 100 mM; below 100 mM KCl the slope of the log conductance-voltage curve is also reduced. The effect of changing alamethicin concentration reveals that nine or ten molecules are involved for KCl concentrations larger than 100 mM; if the KCl concentration is less than 100 mM, the effect of changing the alamethicin concentration is reduced. Time-dependent measurements have also been performed; only one time constant was found and it is strongly voltage-dependent. Also a very slow voltage-dependent absorption process is found. These results can be explained if it is assumed that pores are formed of a mixture of charged and uncharged alamethicin molecules when a voltage is applied and that uncharged alamethicin can also form pores without applying a voltage, once the absorption process has been started by previously applied voltages. The voltage dependence of the time constant seems to indicate that the voltage-dependent pore formation is produced by aggregates of charged alamethicin rather than independent molecules.     

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.     

Properties of bilayer lipid membranes with different surface charges in the presence of tetraalkylammonium salts]

It is shown that with the growth of the radius of tetraalkylammonium ions the conductivity of the membrane increases. With an increase of the dimensions of penetrating ions the maximum cation selectivity reached in the beginning decreases with a further growth of cation radius. A negative charge on the membrane surface results in a higher cation selectivity and conductance mechanism is observed at the transition to the cations with a large radius at their high enough concentration in the aqueous solution. It can be explaind by the formation of triplet in the membrane phase which aid in the penetration of C1-.     

Properties of ganglioside GM1 in phosphatidylcholine bilayer membranes.

Gangliosides have been shown to function as cell surface receptors, as well as participating in cell growth, differentiation, and transformation. In spite of their multiple biological functions, relatively little is known about their structure and physical properties in membrane systems. The thermotropic and structural properties of ganglioside GM1 alone and in a binary system with 1,2-dipalmitoyl phosphatidylcholine (DPPC) have been investigated by differential scanning calorimetry (DSC) and x-ray diffraction. By DSC hydrated GM1 undergoes a broad endothermic transition TM = 26 degrees C (delta H = 1.7 kcal/mol GM1). X-ray diffraction below (-2 degrees C) and above (51 degrees C) this transition indicates a micellar structure with changes occurring only in the wide angle region of the diffraction pattern (relatively sharp reflection at 1/4.12 A-1 at -2 degrees C; more diffuse reflection at 1/4.41 A-1 at 51 degrees C). In hydrated binary mixtures with DPPC, incorporation of GM1 (0-30 mol%; zone 1) decreases the enthalpy of the DPPC pretransition at low molar compositions while increasing the TM of both the pre- and main transitions (limiting values, 39 and 44 degrees C, respectively). X-ray diffraction studies indicate the presence of a single bilayer gel phase in zone 1 that can undergo chain melting to an L alpha bilayer phase. A detailed hydration study of GM1 (5.7 mol %)/DPPC indicated a conversion of the DPPC bilayer gel phase to an infinite swelling system in zone 1 due to the presence of the negatively charged sialic acid moiety of GM1. At 30-61 mol % GM1 (zone 2), two calorimetric transitions are observed at 44 and 47 degrees C, suggesting the presence of two phases. The lower transition reflects the bilayer gel --> L alpha transition (zone 1), whereas the upper transition appears to be a consequence of the formation of a nonbilayer, micellar or hexagonal phase, although the structure of this phase has not been defined by x-ray diffraction. At > 61 mol % GM1 (zone 3) the calorimetric and phase behavior is dominated by the micelle-forming properties of GM1; the presence of mixed GM1/DPPC micellar phases is predicted.     

Lateral electrical conductivity of mica-supported lipid bilayer membranes measured by scanning tunneling microscopy.

Lateral electric conductivity of mica-supported lipid monolayers and of the corresponding lipid bilayers has been studied by means of scanning tunneling microscopy (STM). The surface of freshly cleaved mica itself was found to be conductive when exposed to humid air. Lipid monolayers were transferred onto such a surface by means of the Langmuir-Blodgett technique, which makes the mica surface hydrophobic and suppresses the electric current along the surface in the experimentally accessible humidity (5-80%) and applied voltage (0-10 V) range. This is true for dipalmitoylphosphatidylethanolamine (DPPE) as well as dipalmitoylphosphatidylcholine (DPPC) monolayers. Repeated deposition of DPPC layers by means of the Langmuir-Blodgett LB technique does not lead to the formation of a stable surface-supported bilayer because of the high hydrophilicity of the phosphatidylcholine headgroups that causes DPPC/DPPC bilayers to peel off the supporting surface during the sample preparation. In contrast to this, a DPPE or a DPPC monolayer on top of a DPPE monolayer gives rise to a rather stable mica-supported bilayer that can be studied by STM. Electric currents between 10 and 100 fA, depending on the ambient humidity, flow along the DPPE bilayer surface, in the humidity range between 35 and 60%. The DPPC surface, which is more hydrophilic, is up to 100 times more conductive under comparable conditions. Anomalous high lateral conductivity thus depends on, and probably proceeds via, the surface-adsorbed water layers. The prominence of ambient humidity and surface hydrophilicity on the measured lateral currents suggests this.(ABSTRACT TRUNCATED AT 250 WORDS)     

Changes in the electrical characteristics of bilayer lipid membranes during adsorption of heparin in the presence of Ca2+

It was shown that a change in conductance and capacitance of BLM can be explained by Ca++ BLM--heparin complex organization.     

Photo-voltages of bilayer lipid membranes in the presence of cyanine dyes

The transmembrane photo-voltage waveforms induced by 10 different cyanine dyes absorbed to one side of bilayer lipid membranes are described. The membranes were prepared from lecithin, oxidized cholesterol, and mixed lecithin and oxidized cholesterol. An 8-μs flash illumination was used. Three dyes induced a photo-voltage which developed in a few milliseconds, then discharged in less than the membranes' resistance-capacitance time. Five dyes induced a photo-voltage which increased for much longer than the membranes' resistance-capacitance time. Two dyes did not induce any photo-electric effects. Models are presented which correlate the dye structure with the type of photo-voltage waveform induced.     

Anisotropic 2H-nuclear magnetic resonance spin-lattice relaxation in cerebroside- and phospholipid-cholesterol bilayer membranes.

The axially symmetric powder pattern 2H-nuclear magnetic resonance (NMR) lineshapes observed in the liquid crystalline phase of pure lipid or lipid/cholesterol bilayers are essentially invariant to temperature, or, equivalently, to variations in the correlation times characterizing C-2H bond reorientations. In either of these melted phases, where correlation times for C-2H bond motions are shorter than 10(-7) s, information on the molecular dynamics of the saturated hydrocarbon chain would be difficult to obtain using lineshape analyses alone, and one must resort to other methods, such as the measurement of 2H spin-lattice relaxation rates, in order to obtain dynamic information. In pure lipid bilayers, the full power of the spin-lattice relaxation technique has yet to be realized, since an important piece of information, namely the orientation dependence of the 2H spin-lattice relaxation rates is usually lost due to orientational averaging of T1 by rapid lateral diffusion. Under more favorable circumstances, such as those encountered in the lipid/cholesterol mixtures of this study, the effects of orientational averaging by lateral diffusion are nullified, due to either a marked reduction (by at least an order of magnitude) in the diffusion rate, or a marked increase in the radii of curvature of the liposomes. In either case, the angular dependence of 2H spin-lattice relaxation is accessible to experimental study, and can be used to test models of molecular dynamics in these systems. Simulations of the partially recovered lineshapes indicate that the observed T1 anisotropies are consistent with large amplitude molecular reorientation of the C-2H bond among a finite number of sites.(ABSTRACT TRUNCATED AT 250 WORDS)