Dielectric breakdown measurements of human and bovine erythrocyte membranes using benzyl alcohol as a probe molecule

Cryopreservation of human erythrocytes through high intracellular trehalose with membrane stabilization of maltotriose-grafted ε-poly(L-lysine)

Cryopreservation of human erythrocytes via suitable cryoprotectants is essential for transfusion at emergency, but the conventional glycerolization method requires a tedious thawing-deglycerolization process. Alternatively, trehalose, a nonreducing disaccharide, has gained...

Cell electropermeabilization: a new tool for biochemical and pharmacological studies

Cell electropermeabilization is the transient permeabilization of the plasma membrane by means of short and intense electric pulses. Under optimized conditions, electropermeabilization is compatible with cell survival. It provides a direct access into the cytosol to ions, small molecules, exogenous drugs and macromolecules. As cells remain functional, a large variety of cell biology questions can be addressed. Such 'in situ biochemistry' opens new possibilities beside the more classical studies dealing with unpermeabilized cells or subcellular extracts. Electropermeabilization also allows pharmacological studies with cells, cultured monolayers and in vivo tissues as well as the design of drug controlled-release systems.

Chromate effects on red cells membranes

The modification of human erythrocyte membrane proteins by chromate previously had been investigated by kinetic (4) and electrophoretic techniques (5). In the Coulter Counter we now observed that chromate (10 mM) caused an increase in the intracellular resistivity but also an augmentation of the critical voltage where the membrane resistance breaks down owing to electroporation. Furthermore, a slight chromate-induced augmentation of echinocyte shape was observed. Also, chromate causes the intracellular pH to shift to higher values.

Kinetics of ultrastructural changes during electrically induced fusion of human erythrocytes

The sequence of events during the electrically induced fusion of human erythrocytes was studied by rapid quench freeze-fracture electron microscopy. A single electric field pulse was used to induce fusion of human erythrocytes treated with pronase and closely positioned by dielectrophoresis. The electronic circuit was coupled to a rapid freezing mechanism so that ultrastructural changes of the membrane could be preserved at given time points. Pronase treatment enabled adjacent cells to approach each other within 15 nm during dielectrophoresis. The pulse caused a brief disruption of the aqueous boundaries which separated the cells. Within 100 msec following pulse application, the fracture faces exhibited discontinuous areas which were predominantly free of intramembranous particles. At 2 sec after the pulse, transient point defects attributed to intercellular contact appeared in the same membrane areas and replaced the discontinuous areas as the predominant membrane perturbation. At 10 sec after the pulse, the majority of the discontinuous areas and point defects disappeared as the intercellular distance returned to approximately 15 to 25 nm, except at sites of cytoplasmic bridge formation. Intramembranous particle clearing was observed at 60 sec following pulse application in discrete zones of membrane fusion.

Permeability of membrane of Babesia canis infected erythrocytes--influence of an external electric field

The erythrocytes infection by a parasite (Babesia canis) induced a modification of the biological membrane which was studied using the effect of electric pulses of short duration. This process induces the formation of pores and during the opening hemoglobin and other cytoplasmic proteins diffuse out of the cells and are recovered in the external medium. The rate of molecular permeation across the electrically perforated membranes depends on several factors: electric-field strength, pulses number, pulse duration, temperature and cellular concentration. Even for low parasitemia, differences in the effect of these parameters were observed between infected and non-infected erythrocytes.

Effects of benzyl alcohol on erythrocyte shape, membrane hemileaflet fluidity and membrane viscoelasticity

The effects of benzyl alcohol on cell shape, hemileaflet lipid fluidity and membrane rheology of human red blood cells were studied. Membrane fluidity was assessed by determining the fluorescence anisotropy of permeant probes (1,6-diphenyl-1,3,5-hexatriene,12-(9-anthroyloxy)stearate, 2-(9-anthroyloxy)stearate) and a new impermeant probe (N-stachyosylsuccinic acid dihydrazide-2-(9-anthroyloxy)stearate). Measurements made on intact red blood cells reflected primarily the outer leaflet fluidity while measurements made on red blood cells ghosts reflected the fluidity of both leaflets. Membrane viscoelasticity was determined by micropipette aspiration. Treatment of intact red blood cells with benzyl alcohol up to 50 mM caused progressive stomatocytic shape change but no change in membrane viscoelasticity, 1,6-diphenyl-1,3,5-hexatriene anisotropy or stachyosyldihydrazide-2(9-anthroyloxy)stearate correlation time; similar treatment of leaky ghosts yielded decreases in 1,6-diphenyl-1,3,5-hexatriene anisotropy and stachyosyldihydrazide-2(9-anthroyloxy)stearate correlation time. With benzyl alcohol above 50-60 mM, intact red blood cells became echinocytic, and decreases in 1,6-diphenyl-1,3,5-hexatriene anisotropy and stachyosyldihydrazide-2(9-anthroyloxy)stearate correlation time occurred in both intact cells and ghosts; there was no change in membrane viscoelasticity. These results indicate that benzyl alcohol up to 50 mM affects primarily the inner leaflet of the red blood cell membrane and that higher concentrations affect both leaflets. These increases in membrane fluidity are not associated with changes in membrane viscoelasticity. This study illustrates the use of fluorescence techniques to monitor specifically the lipid fluidity of each hemileaflet of the erythrocyte membrane.

Membrane stability

Rupture and buckling of artificial and biological membranes is an important part of many biological processes. In this review, we present some of the main experimental facts and their analysis. Recent theoretical work, in particular thin film models and nucleation mechanisms of membrane instability, are discussed in detail. Possible applications to membrane adhesion and fusion are pointed out. Attempts are made to explain biological phenomena and experimental results for biological membranes based on a rigorous physicochemical approach developed previously for thin films in colloid systems.

Studies on erythrocyte membranes of patients with Huntington's disease

Several red cell membrane properties and activities of membrane-bound enzymes were investigated in blood samples of patients with Huntington's disease. (Na(+)+K(+)) ATPase activity and cell deformability appeared to be normal, in contradiction to preceding reports from other laboratories. With other techniques sensitive to relatively small changes in membrane structure, no abnormalities were found in Huntington's disease red cell membranes. These investigations do not support the concept that a generalised membrane abnormality is present in Huntington's disease.

Electro-mechanical properties of human erythrocyte membranes: the pressure-dependence of potassium permeability

Electrical breakdown of cell membranes is interpreted in terms of an electro-mechanical model. It postulates for certain finite membrane areas that the actual membrane thickness depends on the voltage across the membrane and the applied pressure. The magnitude of the membrane compression depends both on the dielectric constant and the compressive, elastic modulus transverse to the membrane plane. The theory predicts the existence of a critical absolute hydrostatic pressure at which the intrinsic membrane potential is sufficiently high to induce "mechanical" breakdown of the membrane. The theoretically expected value for the critical pressure depends on the assumption made both for the pressure-dependence of the elastic modulus of the membrane and of the intrinsic membrane potential. It is shown that the critical pressure is expected at about 65 M Pa. The prediction of a critical pressure could be verified by subjecting human erythrocytes to high pressures (up to 100 M Pa) in a hyperbaric chamber. The net potassium efflux in dependence on pressure was used as an criterion for breakdown. Whereas the potassium net efflux was linearly dependent on pressure up to 60 M Pa, a significant increase in potassium permeability was observed towards higher pressure in agreement with the theory. The increase in the net potassium efflux above 60 M Pa was reversible, as indicated by measurements in which the same erythrocyte sample was subjected to several consecutive pressure pulses. Temperature changes in the erythrocyte suspension during compression and decompression were so small (less than 2 degrees C) that they could not account for the observed effects.

Electrical field effects induced in membranes of developing chloroplasts

Etioplasts, etiochloroplasts, and chloroplasts of Avena sativa L. purified on a Percoll gradient were subjected to increasing electric field strengths in the orifice of a hydrodynamically focussing Coulter Counter. The change in resistance of the orifice when an organelle is present correlates well with the size of the plastid for field strengths up to about 3.5 kV cm(-1). Beyond this field strength, depending on the size of the organelle, the size is underestimated. The underestimation of the size is caused by the dielectric breakdown of the envelope membranes once a critical membrane potential has been exceeded. Beyond breakdown the signal of the particle is predominately determined both by the internal conductivity and the increased membrane conductivity. Measurements of the breakdown voltage of different developmental stages of the plastids reveal that the breakdown voltage decreases from 1.2 V in etioplasts to about 0.9 V in chloroplasts after 48 h illumination. The decrease in breakdown voltage can be explained in terms of increasing incorporation of proteins into the inner envelope membrane during development.This view is consistent with conclusions drawn by other authors from transport and biochemical studies. The underestimation of the size beyond breakdown is about 20% and increases to a constant value of about 40% during the first 3 h of illumination. The underestimation decreases again to about 10% when the chloroplast stage is reached. This result is consistent with the current view of chloroplast development. Mobilisation of glucans, the transformation of the prolamellar body of etioplasts into thylacoid membranes as well as an intensive synthesis of pigments and enhanced rates of ions transport in the first hour of illumination gives rise to an increased pool of ionic compounds within the plastid stroma.It should be noted that purification of the plastids on Percoll gradient leads to size distributions which are almost normally distributed over the whole field range, suggesting that the preparations are also electrically homogeneous (U. Zimmermann, F. Riemann and G. Pilwat: Biochim. Biophys. Acta 436, 460-474 (1976)). In contrast with results of Lürssen, K., Z. Naturforsch. 25b, 1113-1119 (1970) only a slight increase of the modal volume from the etioplast stage to the chloroplast stage is observed.

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

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 musec 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 10(8) to 0.1 omega 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 difference Vc. For 1 M alkali ion chlorides Vc was about 1 V. The temperature dependence of the electrical breakdown voltage Vc is comparable to that being observed with cell membranes. Vc decreases between 2 and 48 degrees C from 1.5 to 0.6 V in the presence of 1 M KCl. Breakdown experiments were also performed with lipid bilayer membrane 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 anaesthesia: a new hypothesis based on the effects on electrical properties of a model membrane: preliminary studies

Changes induced by inhalational anaesthetic agents were investigated in a simple membrane model. All the agents tested increased the membrane's electrical capacitance and conductance linearly, proportional to concentration and potency, and decreased its dialectric strength independently of concentration. When protein was substituted for lipid, the same agents had no significant effect on capacitance, conductance, or dielectric strength. Based on these findings, the following hypothesis is presented. Anaesthetic agents exert their influence on the lipid portion of nerve membranes. They enhance excitability by reducing the dielectric strength of the membrane and depress excitability by increasing the membrane's dielectric constant and passive conductance. The degree of excitability or narcosis at any instant depends upon the relative magnitude of these opposing effects.

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 0.5-10(5)-5.0-10(5) N/m2. Electrical breakdown was measured using intracellular electrodes and 500 mus 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, gamma, is calculated from the slope of this line to 69+/-10-10(5) N/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.K. 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 delta=7-9 nm with a dielectric constant epsilon=greater than 10, e.g. a hydrated protein spanning the whole membrane. (B) delta=4-5 nm with epsilon=3-8, e.g. a lipoprotein of lipid bilayer dimensions. (C) delta approximately 2 nm with epsilon=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: delta=2 nm, epsilon=3-8, e.g. a (lipo) proteinaceous module facing a half life lipid bilayer.

Electrical hemolysis of human and bovine red blood cells

The external electric field strength required for electrical hemolysis of human red blood cells depends sensitively on the composition of the external medium. In isotonic NaCl und KCl solutions the onset of electrical hemolysis is observed at 4 kV per cm and 50 per cent hemolysis at 6 kV per cm, whereas increasing concentrations of phosphate, sulphate, sucrose, inulin and EDTA shift the onset and the 50 per cent hemolysis-value to higher field strengths. The most pronounced effect is observed for inulin and EDTA. In the presence of these substances the threshold value of the electric field strength is shifted to 14 kV per cm. This is in contrast to the dielectric breakdown voltage of human red blood cells which is unaltered by these substances and was measured to be approximately 1 V corresponding in the electrolytical discharge chamber to an external electric field strength of 2 to 3 kV per cm. On the other hand, dielectric breakdown of bovine red blood cell membranes occurs in NaCl solution at 4 to 5 kV per cm and is coupled directly with hemoglobin release. The electrical hemolysis of cells of this species is unaffected by the above substances with exception of inulin. Inulin suppressed the electrical hemolysis up to 15 kV per cm. The data can be explained by the assumption that the reflection coefficients of the membranes of these two species to bivalent anions and uncharged molecules are field-dependent to a different extent. This explanation implies that electrical hemolysis is a secondary process of osmotic nature induced by the reversible permeability change of the membrane (dielectric breakdown) in response to an electric field. This view is supported by the observation that the mean volumes of ghost cells obtained by electrical hemolysis can be changed by changing the external phosphate concentration during hemolysis and resealing, or by subjecting the cells to a transient osmotic stress immediately after the electrical hemolysis step. An interesting finding is that the breakdown voltage, although constant throughout each normally distributed ghost size distribution, increases with increasing mean volume of the ghost populations.