Transmembrane potential measurements on plant cells using the voltage-sensitive dye ANNINE-6

The charging of the plasma membrane is a necessary condition for the generation of an electric-field-induced permeability increase of the plasmalemma, which is usually explained by the creation and the growth of aqueous pores. For cells suspended in physiological buffers, the time domain of membrane charging is in the submicrosecond range. Systematic measurements using Nicotiana tabacum L. cv. Bright Yellow 2 (BY-2) protoplasts stained with the fast voltage-sensitive fluorescence dye ANNINE-6 have been performed using a pulsed laser fluorescence microscopy setup with a time resolution of 5 ns. A clear saturation of the membrane voltage could be measured, caused by a strong membrane permeability increase, commonly explained by enhanced pore formation, which prevents further membrane charging by external electric field exposure. The field strength dependence of the protoplast’s transmembrane potential V _M shows strong asymmetric saturation characteristics due to the high resting potential of the plants plasmalemma. At the pole of the hyperpolarized hemisphere of the cell, saturation starts at an external field strength of 0.3 kV/cm, resulting in a measured transmembrane voltage shift of ?V _M?=??150 mV, while on the cathodic (depolarized) cell pole, the threshold for enhanced pore formation is reached at a field strength of approximately 1.0 kV/cm and ?V _M?=?450 mV, respectively. From this asymmetry of the measured maximum membrane voltage shifts, the resting potential of BY-2 protoplasts at the given experimental conditions can be determined to V _R?=??150 mV. Consequently, a strong membrane permeability increase occurs when the membrane voltage diverges |V _M|?=?300 mV from the resting potential of the protoplast. The largest membrane voltage change at a given external electric field occurs at the cell poles. The azimuthal dependence of the transmembrane potential, measured in angular intervals of 10° along the circumference of the cell, shows a flattening and a slight decrease at higher fields at the pole region due to enhanced pore formation. Additionally, at the hyperpolarized cell pole, a polarization reversal could be observed at an external field range around 1.0 kV/cm. This behavior might be attributed to a fast charge transfer through the membrane at the hyperpolarized pole, e.g., by voltage-gated channels.     

Electropermeabilization of mammalian cells. Quantitative analysis of the phenomenon.

Transient membrane permeabilization by application of high electric field intensity pulses on cells (electropermeabilization) depends on several physical parameters associated with the technique (pulse intensity, number, and duration). In the present study, electropermeabilization is studied in terms of flow of diffusing molecules between cells and external medium. Direct quantification of the phenomenon shows that electric field intensity is a critical parameter in the induction of permeabilization. Electric field intensity must be higher than a critical threshold to make the membrane permeable. This critical threshold depends on the cell size. Extent of permeabilization (i.e., the flow rate across the membrane) is then controlled by both pulse number and duration. Increasing electric field intensity above the critical threshold needed for permeabilization results in an increase membrane area able to be permeabilized but not due to an increase in the specific permeability of the field alterated area. The electroinduced permeabilization is transient and disappears progressively after the application of the electric field pulses. Its life time is under the control of the electric field parameters. The rate constant of the annealing phase is shown to be dependent on both pulse duration and number, but is independent of electric field intensity which creates the permeabilization. The phenomenon is described in terms of membrane organization transition between the natural impermeable state and the electro-induced permeable state, phenomenon only locally induced for electric field intensities above a critical threshold and expanding in relation to both pulse number and duration.     

External electric fields stimulate the electrogenic calcium/sodium exchange in plant protoplasts

External electric fields of low intensity stimulated calcium influx in protoplasts isolated from carrot cell suspension cultures in field intensity dependent and frequency-dependent ways. The field-induced calcium uptake involved a temperature-dependent system that was saturable by external calcium. The induction process appeared mainly cumulative as long as the morphology of the protoplasts did not change (up to 10 min). The stimulation elicited by the electric fields was effective even after switching the field off; the influx increased for 5 min and then slowed down to its initial value 15 min later. During electrostimulation, an additional amount of ATP was accumulated; on removal of the stimulatory field, the extra amount of ATP was consumed, whereas the plasma membrane was hyperpolarized and sodium ions were expelled from the protoplasts. Inhibition of either ATP accumulation or consumption results in the inhibition of both calcium influx and sodium efflux, demonstrating that these processes are coupled. From the data obtained in this work, it may be concluded that the electric field stimulates an ATP synthase like activity; the consumption of the ATP thus formed elicits an electric potential (probably due to the efflux of cations and more specifically sodium) that drives the influx of calcium.     

Electro-permeabilization of cell membranes: effect of the resting membrane potential

Electric field induced permeabilization of cell membranes is an important technique for gene transfection and cell hybridization. Mechanistic studies of this process revealed that the uptake of fluorescent indicator by plant protoplasts occurs predominantly on the hemisphere facing the positive electrode, while in erythrocyte ghosts the probes exit through the hemisphere facing the negative electrode. To reconcile these observations symmetrical pore formation and a mechanism of molecular exchange by electroosmosis has been proposed. In light of these controversial observations, we conducted a systematic study of electroporation of NIH3T3 cells with varying electric field strength, waveform and frequency. Our data revealed that (i) symmetrical permeabilization of the cell membrane occurs only with bipolar a.c. fields. (ii) When a critical membrane breakdown potential, Vc, is applied using either an unipolar a.c. fields or a single d.c. square pulse, the cell membrane becomes permeabilized only at the hemisphere facing the positive electrode. (iii) When the pulse-induced membrane potential, Vm, is approximately equal to or larger than the intrinsic membrane potential (i.e. using d.c. or unipolar a.c. field), asymmetric permeabilization was observed with the hemisphere facing the positive electrode being most permeable. (iv) The rate of fluorescent indicator uptake is dependent on the concentration of the indicator. These results indicate that electro-permeabilization of cell membranes is affected by its resting potential and that electroosmosis is not the dominant mechanism for the cellular uptake of foreign molecules in electroporation.     

Electrically Stimulated Fusion of Different Plant Cell Protoplasts : MESOPHYLL CELL AND GUARD CELL PROTOPLASTS OF VICIA FABA

Cell fusion is induced between guard cell and mesophyll cell protoplasts of Vicia faba by electrical field application. The process of fusion is initiated by electrical breakdown of the cell membrane. Prior to the application of an external electrical field pulse which brings about reversible breakdown of the membrane, the cells (suspended in a low-conducting medium) are brought into close contact with one another by exposing them to an external alternating, nonuniform field (5 volts, electrode distance, 200 micrometers; 500 kiloHertz). During this process, they form “pearl chains” which may become sufficiently long to form bridges between the electrodes. The process is reversible as long as this voltage is not exceeded. Cell fusion is initiated as a result of an electrical field pulse of 50 microseconds duration and of sufficiently high intensity to induce reversible electrical breakdown of the membranes. The process of fusion is completed within 40 minutes or less in the case of guard cell protoplasts, as well as in the case of fusion between guard cell and mesophyll cell protoplasts. The fused cells are spherical in shape, if the fusion product consists only of two or three cells.     

Electrofused giant protoplasts of Saccharomyces cerevisiae as a novel system for electrophysiological studies on membrane proteins

Giant protoplasts of Saccharomyces cerevisiae of 10-35 µm in diameter were generated by multi-cell electrofusion. Thereby two different preparation strategies were evaluated with a focus on size distribution and “patchability” of electrofused protoplasts. In general, parental protoplasts were suitable for electrofusion 1-12 h after isolation. The electrophysiological properties of electrofused giant protoplasts could be analyzed by the whole-cell patch clamp technique. The area-specific membrane capacitance (0.66 ± 0.07 µF/cm²) and conductance (23-44 µS/cm²) of giant protoplasts were consistent with the corresponding data for parental protoplasts. Measurements with fluorescein-filled patch pipettes allowed to exclude any internal compartmentalisation of giant protoplasts by plasma membranes, since uniform (diffusion-controlled) dye uptake was only observed in the whole-cell configuration, but not in the cell-attached formation. The homogeneous structure of giant protoplasts was further confirmed by the observation that no plasma membrane associated fluorescence was seen in the interior of giant cells after electrofusion of protoplasts expressing the light-activated cation channel Channelrhodopsin-2 (ChR2) linked to yellow fluorescent protein (YFP). Patch clamp analysis of the heterologously expressed ChR2-YFP showed typical blue light dependent, inwardly-directed currents for both electrofused giant and parental protoplasts. Most importantly, neither channel characteristics nor channel expression density was altered by electric field treatment. Summarising, multi-cell electrofusion increases considerably the absolute number of membrane proteins accessible in patch clamp experiments, thus presumably providing a convenient tool for the biophysical investigation of low-signal transporters and channels.     

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     

Electric field-induced fusion of isolated vacuoles and protoplasts of different developmental and metabolic provenience

Using an electric field pulse technique, we induced fusion between vacuoles and protoplasts of Kalanchoë daigremontiana , between protoplasts from etiolated and green leaf mesophyll, and between mesophyll protoplasts from plants of different physiological properties ( Avena sativa : C₃ mechanism of photosynthesis, Kalanchoë daigremontiana : crassulacean acid metabolism). Close membrane contact amongst protoplasts or between protoplasts and vacuoles (as required for fusion) was achieved by the application of an alternating, non-uniform electric field to the suspension. Due to the dielectrophoresis effect the cells attach to each other along the field lines. The fusion process is initiated by the injection of an electric field pulse of high intensity and short duration (μs range). The field intensity has to be sufficiently high to induce reversible breakdown in the area of close membrane contact. After the application of the field pulse, the fusion process is initiated and completed within seconds to a few minutes, depending on the material investigated.
Fusion occurs between protoplasts and vacuoles as well as between protoplasts of different species. Both tonoplast and plasma membranes completely intermingled, indicating that in contrast to suggestions in the literature these membranes are compatible. Furthermore the cytoplasms of etiolated and green protoplasts obviously do not mix after fusion is completed, as etioplasts and chloroplasts kept separated from each other. In all experiments the volume of the fusion product equalled the sum of the compartments that underwent fusion. The wide spectrum of possible applications resulting from these fusion experiments in relation to metabolic problems is discussed.     

Plasma membrane charging of Jurkat cells by nanosecond pulsed electric fields

The initial effect of nanosecond pulsed electric fields (nsPEFs) on cells is a change of charge distributions along membranes. This first response is observed as a sudden shift in the plasma transmembrane potential that is faster than can be attributed to any physiological event. These immediate, yet transient, effects are only measurable if the diagnostic is faster than the exposure, i.e., on a nanosecond time scale. In this study, we monitored changes in the plasma transmembrane potential of Jurkat cells exposed to nsPEFs of 60 ns and amplitudes from 5 to 90 kV/cm with a temporal resolution of 5 ns by means of the fast voltage-sensitive dye Annine-6. The measurements suggest the contribution of both dipole effects and asymmetric conduction currents across opposite sides of the cell to the charging. With the application of higher field strengths the membrane charges until a threshold voltage value of 1.4–1.6 V is attained at the anodic pole. This indicates when the ion exchange rates exceed charging currents, thus providing strong evidence for pore formation. Prior to reaching this threshold, the time for the charging of the membrane by conductive currents is qualitatively in agreement with accepted models of membrane charging, which predict longer charging times for lower field strengths. The comparison of the data with previous studies suggests that the sub-physiological induced ionic imbalances may trigger other intracellular signaling events leading to dramatic outcomes, such as apoptosis.     

Dependence of Electroporation Detection Threshold on Cell Radius: An Explanation to Observations Non Compatible with Schwan’s Equation Model

It is widely accepted that electroporation occurs when the cell transmembrane voltage induced by an external applied electric field reaches a threshold. Under this assumption, in order to trigger electroporation in a spherical cell, Schwan’s equation leads to an inversely proportional relationship between the cell radius and the minimum magnitude of the applied electric field. And, indeed, several publications report experimental evidences of an inverse relationship between the cell size and the field required to achieve electroporation. However, this dependence is not always observed or is not as steep as predicted by Schwan’s equation. The present numerical study attempts to explain these observations that do not fit Schwan’s equation on the basis of the interplay between cell membrane conductivity, permeability, and transmembrane voltage. For that, a single cell in suspension was modeled and the electric field necessary to achieve electroporation with a single pulse was determined according to two effectiveness criteria: a specific permeabilization level, understood as the relative area occupied by the pores during the pulse, and a final intracellular concentration of a molecule due to uptake by diffusion after the pulse, during membrane resealing. The results indicate that plausible model parameters can lead to divergent dependencies of the electric field threshold on the cell radius. These divergent dependencies were obtained through both criteria and using two different permeabilization models. This suggests that the interplay between cell membrane conductivity, permeability, and transmembrane voltage might be the cause of results which are noncompatible with the Schwan’s equation model.     

Plant actin controls membrane permeability

The biological effects of electric pulses with low rise time, high field strength, and durations in the nanosecond range (nsPEFs) have attracted considerable biotechnological and medical interest. However, the cellular mechanisms causing membrane permeabilization by nanosecond pulsed electric fields are still far from being understood. We investigated the role of actin filaments for membrane permeability in plant cells using cell lines where different degrees of actin bundling had been introduced by genetic engineering. We demonstrate that stabilization of actin increases the stability of the plasma membrane against electric permeabilization recorded by penetration of Trypan Blue into the cytoplasm. By use of a cell line expressing the actin bundling WLIM domain under control of an inducible promotor we can activate membrane stabilization by the glucocorticoid analog dexamethasone. By total internal reflection fluorescence microscopy we can visualize a subset of the cytoskeleton that is directly adjacent to the plasma membrane. We conclude that this submembrane cytoskeleton stabilizes the plasma membrane against permeabilization through electric pulses.     

Cell synchronization effect on mammalian cell permeabilization and gene delivery by electric field

Electropermeabilization is a promising nonviral method for gene therapy. However, despite the fact that it is widely used to transfer genes into living cells, the steps that limit DNA transfer remain to be determined. Here, we report the effect of cell synchronization on membrane permeabilization and gene delivery by electric fields.Chinese hamster ovary (CHO) cells were synchronized by aphidicolin or butyrate treatment. Electro-mediated transfection of these cells was evaluated under electric field conditions leading to the same level of membrane permeabilization.Aphidicolin cell synchronization in G2/M phase leads to a slight increase in plasma membrane permeabilization but to a three-fold increase in percentage of transfected cells and to an eight-fold increase in gene expression. This increase in cell transfection is specifically due to the G2/M synchronization process. Indeed, cell synchronization in G1 phase by sodium butyrate has no effect on cell permeabilization and transfection.Our results suggest that the enhanced transfection level in G2/M phase is not simply due to enhanced permeabilization, but reinforce the statement that the melting of the nuclear membrane facilitates direct access of plasmid DNA to the nucleus.     

Cereal protoplast recalcitrance

Summary Cereal leaf protoplasts are extremely difficult to culture (recalcitrant) in vitro. There have been few reports of division and the protoplasts typically exhibit excessive enlargement and vacuolization with reduced cell wall deposition. Inasmuch as leaf base explants are capable of callus formation in vitro, protoplasts derived from this tissue must have lost the ability to divide as a consequence of changes induced by the wall-digestion process. We review evidence suggesting that the inhibition of mitosis in these protoplasts is a consequence of a cascade of events initiated at the plasma membrane. The enzyme treatment necessary for wall removal triggers membrane depolarization and other changes that can lead to the initiation of lipid peroxidation and oxidative stress. Mitotically inactive cereal leaf protoplasts are unable to mount a protective response to these degradative processes. Consequently, the resulting membrane perturbations and permeabilization give rise to secondary effects on the cytoskeleton and the cell wall. These effects include reduced or absent microtubules as well as reduced and uneven wall deposition. Such abnormalities are observed in cereal leaf protoplasts and are sufficient to account for recalcitrance because the occurrence of mitosis is strongly dependent on a normal cell wall and cytoskeleton. This paper is NRCC number 32475.     

Membrane Permeabilization in Relation to Inactivation Kinetics of Lactobacillus Species due to Pulsed Electric Fields

Membrane permeabilization due to pulsed electric field (PEF) treatment of gram-positive Lactobacillus cells was investigated by using propidium iodide uptake and single-cell analysis with flow cytometry. Electric field strength, energy input, treatment time, and growth phase affected membrane permeabilization of Lactobacillus plantarum during PEF treatment. A correlation between PEF inactivation and membrane permeabilization of L. plantarum cells was demonstrated, whereas no relationship was observed between membrane permeabilization and heat inactivation. The same results were obtained with a Lactobacillus fermentum strain, but the latter organism was more PEF resistant and exhibited less membrane permeabilization, indicating that various bacteria have different responses to PEF treatment. While membrane permeabilization was the main factor involved in the mechanism of inactivation, the growth phase and the acidity of the environment also influenced inactivation. By using flow cytometry it was possible to sort cells in the L. plantarum population based on different cell sizes and shapes, and the results were confirmed by image analysis. An apparent effect of morphology on membrane permeabilization was observed, and larger cells were more easily permeabilized than smaller cells. In conclusion, our results indicate that the ability of PEF treatment to cause membrane permeabilization is an important factor in determining inactivation. This finding should have an effect on the final choice of the processing parameters used so that all microorganisms can be inactivated and, consequently, on the use of PEF treatment as an alternative method for preserving food products.     

Sine wave electropermeabilization reveals the frequency-dependent response of the biological membranes

The permeabilization of biological membranes by electric fields, known as electroporation, has been traditionally performed with square electric pulses. These signals distribute the energy applied to cells in a wide frequency band. This paper investigates the use of sine waves, which are narrow band signals, to provoke electropermeabilization and the frequency dependence of this phenomenon.Single bursts of sine waves at different frequencies in the range from 8 kHz–130 kHz were applied to cells in vitro. Electroporation was studied in the plasma membrane and the internal organelles membrane using calcium as a permeabilization marker. Additionally, a double-shell electrical model was simulated to give a theoretical framework to our results.The electroporation efficiency shows a low pass filter frequency dependence for both the plasma membrane and the internal organelles membrane. The mismatch between the theoretical response and the observed behavior for the internal organelles membrane is explained by a two-step permeabilization process: first the permeabilization of the external membrane and afterwards that of the internal membranes. The simulations in the model confirm this two-step hypothesis when a variable plasma membrane conductivity is considered in the analysis.This study demonstrates how the use of narrow-band signals as sine waves is a suitable method to perform electroporation in a controlled manner. We suggest that the use of this type of signals could bring a simplification in the investigations of the very complex phenomenon of electroporation, thus representing an interesting option in future fundamental studies.     

Nanosecond electric pulses cause mitochondrial membrane permeabilization in Jurkat cells

Nanosecond, high‐voltage electric pulses (nsEP) induce permeabilization of the plasma membrane and the membranes of cell organelles, leading to various responses in cells including cytochrome c release from mitochondria and caspase activation associated with apoptosis. We report here evidence for nsEP‐induced permeabilization of mitochondrial membranes in living cells. Using three different methods with fluorescence indicators—rhodamine 123 (R123), tetramethyl rhodamine ethyl ester (TMRE), and cobalt‐quenched calcein—we have shown that multiple nsEP (five pulses or more, 4 ns duration, 10 MV/m, 1 kHz repetition rate) cause an increase of the inner mitochondrial membrane permeability and an associated loss of mitochondrial membrane potential. These effects could be a consequence of nsEP permeabilization of the inner mitochondrial membrane or the activation of mitochondrial membrane permeability transition pores. Plasma membrane permeabilization (YO‐PRO‐1 influx) was detected in addition to mitochondrial membrane permeabilization. Bioelectromagnetics 33:257–264, 2012. © 2011 Wiley Periodicals, Inc.     

Electroporation of DC-3F Cells Is a Dual Process

Treatment of biological material by pulsed electric fields is a versatile technique in biotechnology and biomedicine used, for example, in delivering DNA into cells (transfection), ablation of tumors, and food processing. Field exposure is associated with a membrane permeability increase usually ascribed to electroporation, i.e., formation of aqueous membrane pores. Knowledge of the underlying processes at the membrane level is predominantly built on theoretical considerations and molecular dynamics (MD) simulations. However, experimental data needed to monitor these processes with sufficient temporal resolution are scarce. The whole-cell patch-clamp technique was employed to investigate the effect of millisecond pulsed electric fields on DC-3F cells. Cellular membrane permeabilization was monitored by a conductance increase. For the first time, to our knowledge, it could be established experimentally that electroporation consists of two clearly separate processes: a rapid membrane poration (transient electroporation) that occurs while the membrane is depolarized or hyperpolarized to voltages beyond so-called threshold potentials (here, +201 mV and −231 mV, respectively) and is reversible within ∼100 ms after the pulse, and a long-term, or persistent, permeabilization covering the whole voltage range. The latter prevailed after the pulse for at least 40 min, the postpulse time span tested experimentally. With mildly depolarizing or hyperpolarizing pulses just above threshold potentials, the two processes could be separated, since persistent (but not transient) permeabilization required repetitive pulse exposure. Conductance increased stepwise and gradually with depolarizing and hyperpolarizing pulses, respectively. Persistent permeabilization could also be elicited by single depolarizing/hyperpolarizing pulses of very high field strength. Experimental measurements of propidium iodide uptake provided evidence of a real membrane phenomenon, rather than a mere patch-clamp artifact. In short, the response of DC-3F cells to strong pulsed electric fields was separated into a transient electroporation and a persistent permeabilization. The latter dominates postpulse membrane properties but to date has not been addressed by electroporation theory or MD simulations.     

Selective field effects on intracellular vacuoles and vesicle membranes with nanosecond electric pulses

Electric pulses across intact vesicles and cells can lead to transient increase in permeability of their membranes. We studied the integrity of these membranes in response to external electric pulses of high amplitude and submicrosecond duration with a primary aim of achieving selective permeabilization. These effects were examined in two separate model systems comprising of 1), a mixed population of 1,2-di-oleoyl-sn-glycero-3-phosphocholine phospholipid vesicles and in 2), single COS-7 cells, in which large endosomal membrane vacuoles were induced by stimulated endocytosis. It has been shown that large and rapidly varying external electric fields, with pulses shorter than the charging time of the outer-cell membrane, could substantially increase intracellular fields to achieve selective manipulations of intracellular organelles. The underlying principle of this earlier work is further developed and applied to the systems studied here. Under appropriate conditions, we show preferential permeabilization of one vesicle population in a mixed preparation of vesicles of similar size distribution. It is further shown that large endocytosed vacuoles in COS-7 cells can be selectively permeabilized with little effect on the integrity of outer cell membrane.     

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.     

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.