Reversible Electropermeabilization of Mammalian Cells by High-Intensity, Ultra-Short Pulses of Submicrosecond Duration

Mouse myeloma cells were electropermeabilized by single square-wave electric pulses with amplitudes of up to ∼150 kV/cm and durations of 10–100 nsec. The effects of the field intensity, pulse duration and medium conductivity on cell viability and field-induced uptake of molecules were analyzed by quantitative flow cytometry using the membrane-impermeable fluorescent dye propidium iodide as indicator molecule. Despite the extremely large field strengths, the majority of cells survived the exposure to ultra-short field pulses. The electrically induced dye uptake increased markedly with decreasing conductivity of the suspending medium. We assigned this phenomenon to the transient electrodeformation (stretching) force that assumes its maximum value if cells are suspended in low-conductivity media, i.e., if the external conductivity σ_e is smaller than that of the cytosol σ_i. The stretching force vanishes when σ_e is equal to or larger than σ_i. Due to their capability of delivering extremely large electric fields, the pulse power systems used here appear to be a promising tool for the electropermeabilization of very small cells and vesicles (including intracellular organelles, liposomes, etc.). Received: 15 May 2001/Revised: 20 July 2001     

Treatment of Cells with Detergent Activates Caspases and Induces Apoptotic Cell Death

Due to their amphiphilic properties, detergents readily disrupt cellular membranes and cause rapid cytolysis. In this study we demonstrate that treatment of cells with sublytic concentrations of detergents such as Triton X-100, Nonidet P-40, n-octylglucoside and the bile salt sodium deoxycholate induce typical signs of apoptosis including DNA fragmentation and cleavage of poly(ADP-ribose) polymerase molecules. The detergent concentration required for apoptosis was below the critical micellar concentration. Induction of apoptosis was not restricted to human cells but similarly occurred in a variety of other vertebrate cell lines. Unstimulated peripheral blood mononuclear cells were susceptible to apoptosis induction by detergent suggesting that apoptosis in this circumstance is not mediated by CD95. Cell death was not due to influx of calcium from the medium. Apoptosis was blocked and cytolysis prevented by treatment with peptide inhibitors of caspases. These findings suggest a process of apoptosis that is initiated upon nonspecific alterations at the cell membrane level. Physiologic correlates of this process still have to be defined. Received: 12 November 1999/Revised: 6 March 2000     

Effect of actin cytoskeleton disruption on electric pulse‐induced apoptosis and electroporation in tumour cells

Electric pulses are known to affect the outer membrane and intracellular structures of tumour cells. By applying electrical pulses of 450 ns duration with electric field intensity of 8 kV/cm to HepG2 cells for 30 s, electric pulse‐induced changes in the integrity of the plasma membrane, apoptosis, viability and mitochondrial transmembrane potential were investigated. Results demonstrated that electric pulses induced cell apoptosis and necrosis accompanied with the decrease of mitochondrial transmembrane potential and the formation of pores in the membrane. The role of cytoskeleton in cellular response to electric pulses was investigated. We found that the apoptotic and necrosis percentages of cells in response to electric pulses decreased after cytoskeletal disruption. The electroporation of cell was not affected by cytoskeletal disruption. The results suggest that the disruption of actin skeleton is positive in protecting cells from killing by electric pulses, and the skeleton is not involved in the electroporation directly.     

Diverse effects of nanosecond pulsed electric fields on cells and tissues

The application of pulsed electric fields to cells is extended to include nonthermal pulses with shorter durations (10-300 ns), higher electric fields (< or =350 kV/cm), higher power (gigawatts), and distinct effects (nsPEF) compared to classical electroporation. Here we define effects and explore potential application for nsPEF in biology and medicine. As the pulse duration is decreased below the plasma membrane charging time constant, plasma membrane effects decrease and intracellular effects predominate. NsPEFs induced apoptosis and caspase activation that was calcium-dependent (Jurkat cells) and calcium-independent (HL-60 and Jurkat cells). In mouse B10-2 fibrosarcoma tumors, nsPEFs induced caspase activation and DNA fragmentation ex vivo, and reduced tumor size in vivo. With conditions below thresholds for classical electroporation and apoptosis, nsPEF induced calcium release from intracellular stores and subsequent calcium influx through store-operated channels in the plasma membrane that mimicked purinergic receptor-mediated calcium mobilization. When nsPEF were applied after classical electroporation pulses, GFP reporter gene expression was enhanced above that observed for classical electroporation. These findings indicate that nsPEF extend classical electroporation to include events that primarily affect intracellular structures and functions. Potential applications for nsPEF include inducing apoptosis in cells and tumors, probing signal transduction mechanisms that determine cell fate, and enhancing gene expression.     

Electroporation and electrophoretic DNA transfer into cells. The effect of DNA interaction with electropores.

It has been shown recently that electrically induced DNA transfer into cells is a fast vectorial process with the same direction as DNA electrophoresis in an external electric field (Klenchin, V. A., S. I. Sukharev, S. M. Serov, L. V. Chernomordik, and Y. A. Chizmadzhev. 1991. Biophys. J. 60:804-811). Here we describe the effect of DNA interaction with membrane electropores and provide additional evidences for the key role of DNA electrophoresis in cell electrotransfection. The assay of electrically induced uptake of fluorescent dextrans (FDs) by cells shows that the presence of DNA in the medium during electroporation leads to a sharp increase in membrane permeability to FDs of M(r) < 20,000. The permeability increases with DNA concentration and the effect is seen even if FD is added to the cell suspension a few minutes after pulse application. The longer the DNA fragment, the greater the increase in permeability. The use of a two-pulse technique allows us to separate two effects provided by a pulsed electric field: membrane electroporation and DNA electrophoresis. The first pulse (6 kV/cm, 10 microseconds) creates pores efficiently, whereas transfection efficiency (TE) is low. The second pulse of much lower amplitude, but substantially longer (0.2 kV/cm, 10 ms), does not cause poration and transfection by itself but enhances TE by about one order of magnitude. In two-pulse experiments, TE rises monotonously with the increase of the second pulse duration. By varying the delay duration between the two pulses, we estimate the lifetime of electropores (which are DNA-permeable in conditions of low electric field) as tens of seconds.(ABSTRACT TRUNCATED AT 250 WORDS)     

In vivo electroporation of skeletal muscle: threshold, efficacy and relation to electric field distribution.

In vivo electroporation is increasingly being used to deliver small molecules as well as DNA to tissues. The aim of this study was to quantitatively investigate in vivo electroporation of skeletal muscle, and to determine the threshold for permeabilization. We designed a quantitative method to study in vivo electroporation, by measuring uptake of (51)Cr-EDTA. As electrode configuration influences electric field (E-field) distribution, we developed a method to calculate this. Electroporation of mouse muscle tissue was investigated using either external plate electrodes or internal needle electrodes placed 4 mm apart, and eight pulses of 99 micros duration at a frequency of 1 Hz. The applied voltage to electrode distance ratio was varied from 0 to 2.0 kV/cm. We found that: (1) the threshold for permeabilization of skeletal muscle tissue using short duration pulses was at an applied voltage to electrode distance ratio of 0.53 kV/cm (+/-0.03 kV/cm), corresponding to an E-field of 0.45 kV/cm; (2) there were two phases in the uptake of (51)Cr-EDTA, the first indicating increasing permeabilization and the second indicating beginning irreversible membrane damage; and (3) the calculated E-field distribution was more homogeneous for plate than for needle electrodes, which was reflected in the experimental results.     

The Effect of Electrical Deformation Forces on the Electropermeabilization of Erythrocyte Membranes in Low- and High-Conductivity Media

Electrical breakdown of erythrocytes induces hemoglobin release which increases markedly with decreasing conductivity of the pulse medium. This effect presumably results from the transient, conductivity-dependent deformation forces (elongation or compression) on the cell caused by Maxwell stress. The deformation force is exerted on the plasma membrane of the cell, which can be viewed as a transient dipole induced by an applied DC electric field pulse. The induced dipole arises from the free charges that accumulate at the cell interfaces via the Maxwell-Wagner polarization mechanism. The polarization response of erythrocytes to a DC field pulse was estimated from the experimental data obtained by using two complementary frequency-domain techniques. The response is very rapid, due to the highly conductive cytosol. Measurements of the electrorotation and electrodeformation spectra over a wide conductivity range yielded the information and data required for the calculation of the deformation force as a function of frequency and external conductivity and for the calculation of the transient development of the deformation forces during the application of a DC-field pulse. These calculations showed that (i) electric force precedes and accompanies membrane charging (up to the breakdown voltage) and (ii) that under low-conductivity conditions, the electric stretching force contributes significantly to the enlargement of ``electroleaks' in the plasma membrane generated by electric breakdown. Received: 12 December 1997/Revised: 13 March 1998     

Resistivity of Red Blood Cells Against High-Intensity, Short-Duration Electric Field Pulses Induced by Chelating Agents

The interaction of human red blood cells (RBCs) with diethylenetriamine-pentaacetic acid (DTPA) or its Gd-complex (Magnevist, a widely used clinical magnetic resonance contrast agent containing free DTPA ligands) led to the following, obviously interrelated phenomena. (i) Both compounds protected erythrocytes against electrohemolysis in isotonic solutions caused by a high-intensity DC electric field pulse. (ii) The inhibition of electrohemolysis was observed only when cells were electropulsed in low-conductivity solutions. (iii) The uptake of Gd-DTPA by electropulsed RBCs was relatively low. (iv) (Gd-) DTPA reduced markedly deformability of erythrocytes, as revealed by the electrodeformation experiments using high-frequency electric fields. Taken together, the results indicate that (Gd-) DTPA produce stiffer erythrocytes that are more resistant to electric field exposure. The observed effects of the chelating agents on the mechanical properties and the electropermeabilization of RBCs must have an origin in molecular changes of the bilayer or membrane-coupled cytoskeleton, which, in turn, appear to result from an alteration of the ionic equilibrium (e.g., Ca²⁺ sequestration) in the vicinity of the cell membrane. Received: 19 January 1999/Revised: 1 April 1999     

Permeabilization of tumor cells induced by pulsed electric fields in vitro

The permeabilization of tumor cells in vitro under the action of pulsed electric fields with a duration of 6 mks in the range of amplitudes 1-7 kV/cm was studied. In the mode of excitation in the ambience of localized plasma discharge in a chamber of special design, an enhanced damage to cells in suspension was observed. It is assumed that the enhancement is due to the synchronous action of the electric field and acoustic shock wave pulses. In the mode without the plasma breakdown of ambience, when the pulse duration of electric field of intensity of 1-2 kV/cm was increased to 60 mks, the efficiency of permeabilization increases nearly by one order. The experimental results are compared with the known theoretical models of cell membrane electroporation.     

The Transient Outward Current of Isolated Bovine Adrenal Zona Fasciculata Cells: Comparison between Standard and Perforated Patch Recording Methods

Voltage-clamp experiments were performed on single bovine adrenal fasciculata cells in short-term primary culture using either standard (broken membrane) or perforated whole-cell patch clamp recording. The membrane current measured with the perforated method was dominated by a very stable transient outward current. By contrast, the transient outward current recorded using the standard method was unstable. The reversal potential of the transient outward current varied linearly with the logarithm of [K⁺] _e with a slope of 47 mV per decade. The onset of activation was sigmoidal and was fitted with a power function where n= 4. Time constants ranged from 1 to 4 msec with a maximum at −25 mV. The steady-state activation curve spanned the voltage range −50 to +80 mV without reaching a clear maximum. During a pulse, the current decayed in a biexponential manner. Time constants τ₁ and τ₂ were voltage-dependent and ranged from 50 to 200 msec respectively for a voltage step at +50 mV. The steady-state inactivation was dependent on the conditioning pulse duration. Using short conditioning pulses (1.2 sec), the curve which spanned the voltage range −40 to −20 mV, was 15 mV more positive than that obtained with longer conditioning pulses (60 sec). Time constants of this ``very slow inactivation' process (τ<sub>vs</sub>) determined for voltage steps at −60 and −50 mV were 15 and 10 sec respectively. A ``facilitation process' of the peak current was observed when the duration or the amplitude of conditioning pulses were increased in the voltage range −100 to −50 mV. Recovery from inactivation followed a biexponential time course which seemed a mixture of both inactivation processes. In some experimental conditions, isolated cells were able to produce overshooting action potentials. These results are discussed in relation with the membrane electrogenesis of this cell type. Received: 14 November 1994/Revised: 24 October 1995     

Voltage-independent Adaptation of Mechanosensitive Channels in Escherichia coli Protoplasts

Mechanosensitive (MS) ion channels, with 560 pS conductance, opened transiently by rapid application of suction pulses to patches of E. coli protoplast membrane. The adaptation phase of the response was voltage-independent. Application of strong suction pulses, which were sufficient to cause saturation of the MS current, did not abolish the adaptation. Multiple-pulse experimental protocols revealed that once MS channels had fully adapted, they could be reactivated by a second suction pulse of similar amplitude, providing the time between pulses was long enough and suction had been released between pulses. Limited proteolysis (0.2 mg/ml pronase applied to the cytoplasmic side of the membrane patch) reduced the number of open channels without affecting the adaptation. Exposing patches to higher levels of pronase (1 mg/ml) removed responsiveness of the channel to suction and abolished adaptation consistent with disruption of the tension transmission mechanism responsible for activating the MS channel. Based on these data we discuss a mechanism for mechanosensitivity mediated by a cytoplasmic domain of the MS channel molecule or associated protein. Received: 29 January 1998/Revised: 16 April 1998     

The effects of intense submicrosecond electrical pulses on cells

A simple electrical model for living cells predicts an increasing probability for electric field interactions with intracellular substructures of both prokaryotic and eukaryotic cells when the electric pulse duration is reduced into the sub-microsecond range. The validity of this hypothesis was verified experimentally by applying electrical pulses (durations 100 micros-60 ns, electric field intensities 3-150 kV/cm) to Jurkat cells suspended in physiologic buffer containing propidium iodide. Effects on Jurkat cells were assessed by means of temporally resolved fluorescence and light microscopy. For the longest applied pulses, immediate uptake of propidium iodide occurred consistent with electroporation as the cause of increased surface membrane permeability. For nanosecond pulses, more delayed propidium iodide uptake occurred with significantly later uptake of propidium iodide occurring after 60 ns pulses compared to 300 ns pulses. Cellular swelling occurred rapidly following 300 ns pulses, but was minimal following 60 ns pulses. These data indicate that submicrosecond pulses achieve temporally distinct effects on living cells compared to microsecond pulses. The longer pulses result in rapid permeability changes in the surface membrane that are relatively homogeneous across the cell population, consistent with electroporation, while shorter pulses cause surface membrane permeability changes that are temporally delayed and heterogeneous in their magnitude.     

Effects of pulsed electric fields on mouse spleen lymphocytes in vitro

The effects of pulsed electric fields on cell membranes were investigated. In vitro exposure of mouse splenocytes to a single high-voltage pulse resulted in an increase in membrane permeability that was dependent on both the electric field strength and the pulse duration. Exposure to a 2 μs, 3.0 kV/cm pulse resulted in the induction of a 1.26 V transmembrane potential, and elicited a 50% loss of intracellular K⁺. These results are in agreement with previous studies of the effects of pulsed electric fields on erythrocytes and microorganisms. The effect of pulsed electric fields on the functional integrity of lymphocytes was i vestigated by measuring [³H]thymidine incorporation by cells cultured in the presence and absence of various mitogens following exposure to an electrical pulse. No statistically significant effects on the response of mouse spleen lymphocytes to concanavalin A, phytohemagglutinin or lipopolysaccharide were observed following exposure to 2 μs electric pulses at amplitudes of up to 3.5 kV/cm. Exposure to a single 10 μs pulse of 2.4–3.5 kV/cm produced a statistically significant reduction in the response of lymphocytes to lipopolysaccharide stimulation that was attributed to cell death.     

Plasma membrane permeabilization by 60- and 600-ns electric pulses is determined by the absorbed dose

We explored how the effect of plasma membrane permeabilization by nanosecond-duration electric pulses (nsEP) depends on the physical characteristics of exposure. The resting membrane resistance (R(m)) and membrane potential (MP) were measured in cultured GH3 and CHO cells by conventional whole-cell patch-clamp technique. Intact cells were exposed to a single nsEP (60 or 600 ns duration, 0-22 kV/cm), followed by patch-clamp measurements after a 2-3 min delay. Consistent with earlier findings, nsEP caused long-lasting R(m) decrease, accompanied by the loss of MP. The threshold for these effects was about 6 kV/cm for 60 ns pulses, and about 1 kV/cm for 600 ns pulses. Further analysis established that it was neither pulse duration nor the E-field amplitude per se, but the absorbed dose that determined the magnitude of the biological effect. In other words, exposure to nsEP at either pulse duration caused equal effects if the absorbed doses were equal. The threshold absorbed dose to produce plasma membrane effects in either GH3 or CHO cells at either pulse duration was found to be at or below 10 mJ/g. Despite being determined by the dose, the nsEP effect clearly is not thermal, as the maximum heating at the threshold dose is less than 0.01 degrees C. The use of the absorbed dose as a universal exposure metric may help to compare and quantify nsEP sensitivity of different cell types and of cells in different physiological conditions. The absorbed dose may also prove to be a more useful metric than the incident E-field in determining safety limits for high peak, low average power EMF emissions.     

Inactivation and injury of Escherichia coli O157:H7 and Staphylococcus aureus by pulsed electric fields

Two pathogenic microorganisms Escherichia coli O157:H7 and Staphylococcus aureus, suspended in peptone solution (0.1% w/v) were treated with 12, 14, 16 and 20 kV/cm electric field strengths with different pulse numbers up to 60 pulses. Pulsed electric field (PEF) treatment at 20 kV/cm with 60 pulses provided nearly 2 log reduction in viable cell counts of E. coli O157:H7 and S. aureus. S. aureus cells were slightly more resistant than E.coli O157:H7 cells. The results related to the effect of initial cell concentration of E. coli O157:H7 on the PEF inactivation showed that more inactivation was obtained by decreasing initial cell concentration. Any possible injury by PEF was also investigated after applying 20 kV/cm electric field to the microorganisms. As a result, it was determined that there was 35.92 to 43.36% injury in E. coli O157:H7 cells, and 17.26 to 30.86% injury in S. aureus cells depending on pulse number. The inactivation results were also described by a kinetic model.     

Electrorotation of Erythrocytes Treated with Dipicrylamine: Mobile Charges within the Membrane Show their ``Signature' in Rotational Spectra

In this study, electrorotation spectra of individual cells (that is, frequency dependence of cell rotation speed) have been proved to yield information not only about the passive electric properties of cell constituents, but also about the presence of mobile charges within the plasma membrane being part of ion carrier transport systems. Experiments on human erythrocytes pretreated with the lipophilic anion dipicrylamine (DPA) gave convincing evidence that these artificial mobile charges adsorbed to the plasma membrane contributed significantly to the rotational spectrum at relatively low conductivity of the external medium (2–5 mS m⁻¹). Theoretical integration of the mobile charge concept into the single-shell model (viewing the cell as a homogenous sphere surrounded by a membrane) led to a set of equations which predicted electrorotational behavior of DPA-treated cells in dependence on medium conductivity. The quantitative data on the partition and the transmembrane translocation rate of the DPA anion extracted from the experimental rotational spectra agreed well with the corresponding literature values. Received: 14 February 1996/Revised: 29 May 1996     

Electro-fusion of haploid Saccharomyces yeast cells of identical mating type

Yeast protoplasts from the haploid strains 21 a and 111a were exposed to an inhomogeneous alternating field (about 1 kV/cm, 2 MHz). Due to dielectrophoretic aggregation two or more cells with close membrane contact are formed between the electrodes. Cell fusion was observed by application of two field pulses (11 kV/cm, 7 s duration) applied at an interval of 1 s. The intensity of the field pulses is sufficiently high to induce reversible electrical breakdown at membrane sites oriented in the field direction. After a 8 to 14 days incubation period on selection medium two types of fusion products could be isolated: 1) Hybrids with a haploid constitution, respiratory-competent and auxotrophic for histidine. 2) Cells with a diploid cell size and prototrophic for histidine. The genetic analysis for mating types and auxotrophic markers show that in the second case plasmogamy followed by karyogamy had occurred.     

Optimum Conditions for Electric Pulse-mediated Gene Transfer to Bacillus subtilis Cells

It was found that plasmid DNA (pUB 110) can be introduced into not only protoplasts but also intact cells of Bacillus subtilis by electric field pulses. The transformation of, B. subtilis using protoplasts results in an efficiency of 2.5 × 10⁴ transformants per μg of DNA, with a single pulse of 50 jisec with an initial electric field strength of 7kV/cm. Even transformation of intact B. subtilis cells results in a maximum efficiency of 1.5 × 10³ transformants per μg DNA, with a single pulse of 400 μsec with an initial electric field strength of 16kV/cm. The cell survival of protoplasts and intact cells was approximately 100% and 30%, respectively, under the conditions found to be optimal for the transformation process. Plasmid DNA isolated from pUB 110 containing transformants was indistinguishable from authentic preparations of pBU 110 on gel electrophoretic analysis.     

Chloride Currents in Skeletal Muscles of Bufo arenarum

Cl⁻ currents (I _Cl) were measured in short fibers (1–2 mm) from the lumbricalis muscle of toads (Bufo arenarum) with two microelectrodes (15°C). Initially the fibers were equilibrated in a high K⁺-containing solution: (mm) K₂SO₄ 68; Na₂SO₄ 20; KCl 60; CaSO₄ 8; MgSO₄ 1; HEPES 2.5. Constant pulses were applied when all the external K⁺ was replaced by Cs⁺: Cs₂SO₄ 68; Na₂SO₄ 20; CsCl 60; CaSO₄ 8; HEPES 2.5 (pH 7.5). Under these conditions about 80–90% of the current is carried by Cl⁻. The current-voltage relation is almost linear implying constant conductance and hence voltage-independent permeability. The voltage dependence of the net Cl⁻ current could be fitted by constant field equation with a P _Cl of 3.3 × 10⁻⁶ cm/sec. In a separate group of experiments a two-pulse technique was used to estimate the availability and the inactivation of the initial I _Cl during a test pulse. After returning the potential to the holding potential for various times, test pulses of the same amplitude and duration of the prepulses were applied. The initial current during the test pulse was 70% of the initial current during the prepulse and the recovery was complete in less than 300 msec with a linear relationship between the current during the test pulse and the amplitude of the preceding prepulse. When the test pulses were preceded by a positive prepulse, the initial current for any given test pulse was larger than with a negative prepulse. If we assumed that the initial current during the test pulse is a measure of the number of channels open at the end of the prepulse, these results suggest that hyperpolarizing pulses inactivate and depolarizing prepulses activate the I _Cl. Received: 31 March 1995/Revised: 27 October 1995     

Nanoelectroablation therapy for murine basal cell carcinoma

When skin tumors are exposed to non-thermal, low energy, nanosecond pulsed electric fields (nsPEF), apoptosis is initiated both in vitro and in vivo. This nanoelectroablation therapy has already been proven effective in treating subdermal murine allograft tumors. We wanted to determine if this therapy would be equally effective in the treatment of autochthonous BCC tumors in Ptch1(+/-)K14-Cre-ER p53 fl/fl mice. These tumors are similar to human BCCs in histology [2,20] and in response to drug therapy [19]. We have treated 27 BCCs across 8 mice with either 300 pulses of 300ns duration or 2700 pulses of 100ns duration, all at 30kV/cm and 5-7 pulses per second. Every nsPEF-treated BCC began to shrink within a day after treatment and their initial mean volume of 36±5 (SEM) mm(3) shrunk by 76±3% over the ensuing two weeks. After four weeks, they were 99.8% ablated if the size of the treatment electrode matched the tumor size. If the tumor was larger than the 4mm wide electrode, multiple treatments were needed for complete ablation. Treated tumors were harvested for histological analysis at various times after treatment and exhibited apoptosis markers. Specifically, pyknosis of nuclei was evident as soon as 2days after nsPEF treatment, and DNA fragmentation as detected via TUNEL staining was also evident post treatment. Nanoelectroablation is effective in triggering apoptosis and remission of radiation-induced BCCs with a single 6min-long treatment of 2700 pulses.