Fusion of mitochondria

In this communication we reported the fusion of mitochondria of hepatocytes extracted from a rat liver. It was found that fusion occurred at an electric field of 1.56-1.8 kV/cm at room temperature. Further increase in the field strength (greater than 1.8 kV/cm) was accompanied by the breakdown of mitochondria.     

Quantitative studies on the viability of yeast protoplasts following dielectrophoresis

Abstract Protoplasts from Saccharomyces cerevisiae and Saccharomyces diastaticus were collected in a non-homogeneous alternating electric field. The dependence of the viability of the protoplasts on different conditions of collection was tested by determining the regeneration rates in each case. The parameters varied in collection were the field strength (0.33 kV/cm–6.67 kV/cm), the frequency of the alternating field (1–2 MHz) and the collection time (2–10 min). The introduction of a new type of fusion chamber (meander chamber) permitted, for the first time, quantitative exposure of protoplasts to the electric field as well as their complete transference into the regeneration medium. The regeneration rates of yeast protoplasts collected under those conditions employed for electrofusion did not differ from those of protoplasts which had been maintained under the same experimental conditions but were not subject to the influence of an alternating electric field. The two yeast strains were fused together (collection 1 kV/cm; pulse 15 kV/cm; duration of pulse 40 μs) and the fusion products were introduced into a selection medium for regeneration. The fusion rate was about 4.8 × 10⁻⁴; on average 272 colonies grew on the selection medium for each chamber filling.     

Induction of chemiluminescence of peritoneal exudate macrophages after exposure to an electric field

The effect of the external high voltage electric field pulses on the suspension of rat peritoneal phagocytes has been investigated using chemiluminescent and turbodimetric methods. Single electric field pulses were found to activate macrophages, which was accompanied by a "flash" of chemiluminescence. Subthreshold electric field strength up to 0.8 kV/cm failed to alter macrophage activity. Maximum activation was observed at 2.2 kV/cm; with higher electric field intensity the effect diminished to zero. Drastic changes in light-scattering suspension properties at high electric field intensity indicate irreversible alterations of the barrier function of phagocyte membranes.     

Electric Field Pulses Can Induce Apoptosis

Injection of electric field pulses of high intensity (kV/cm) and short duration (microsecond range) into a cell suspension results in a temporary increase of the membrane permeability due to a reversible electric breakdown of the cell membrane. Here we demonstrate that application of supercritical field pulses between 4.5 and 8.1 kV/cm strength and 40 μsec duration induce typical features of apoptosis in Jurkat T-lymphoblasts and in HL-60 cells including DNA fragmentation and cleavage of the poly(ADP ribose) polymerase. Apoptosis induction did not depend on the presence of any particular electrolyte in the extracellular medium. However, no apoptosis was observed in solutions without a minimum amount of salt. Apoptotic DNA fragmentation was prevented by the caspase inhibitor zVAD. Received: 16 December 1998/Revised: 24 February 1999     

The effect of pulse field strength on electric field stimulated biosorption of uranium by Kluyveromyces marxianus IMB3

Summary Improved biosorption of uranium by Kluyveromyces marxianus IMB3 biomass was achieved by increasing the electric field strength of delivered pulses from 1.25kV/cm to 2.5kV/cm. Although this had little or no effect on the maximum biosorption capacity (q_max), at low concentrations of uranium the amount bound to the biomass increased from 70 to 140mg uranium/g biomass. Significant increases in the maximum biosorption capacities (119–180 mg uranium/g biomass) were observed when the pulse field strength was increased from 2.5kV/cm to 3.25kV/cm.     

Effect of pulsed electric fields on the activity of neutral trehalase from beer yeast and RSM analysis

The trehalase activity plays an important role in extraction of trehalose from beer yeast. In this study, the effect of pulsed electric field processing on neutral trehalase activity in beer yeast was investigated. In order to develop and optimize a pulsed electric field (PEF) mathematical model for activating the neutral trehalase, we have investigated three variables, including electric field intensity (10-50 kV/cm), pulse duration (2-10 μs) and liquid-solid ratio (20-50 ml/g) and subsequently optimized them by response surface methodology (RSM). The experimental data were fitted to a second-order polynomial equation and profiled into the corresponding contour plots. Optimal condition obtained by RSM is as follows: electric field intensity 42.13 kV/cm, liquid-solid ratio 30.12 ml/g and pulse duration 5.46 μs. Under these conditions, with the trehalose decreased 8.879 mg/L, the PEF treatment had great effect on activating neutral trehalase in beer yeast cells.     

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.     

Electrical hemolysis of human and bovine red blood cells

Summary 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% hemolysis at 6 kV per cm, whereas increasing concentrations of phosphate, sulphate, sucrose, inulin and EDTA shift the onset and the 50% 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 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.     

Kinetics of permeability changes induced by electric impulses in chromaffin granules

Summary Electric field pulses, ranging in intensity from 20 to 50 kV/cm and in duration from 10 to 40 sec, caused a transient increase in the membrane permeability of chromaffin granules from the bovine adrenal medulla, that led to partial release of granule soluble constituents. This transient permeability change was long-lived, as compared to the pulse duration, and the main part of material efflux occurred after the termination of the pulse. During the latter phase the temporarily increased permeability decayed to its original value, in the absence of the electric field. This indicated that the structural perturbation induced in the membrane was transient and apparently reversible. The release event was characterized by a field-dependent permeability coefficient ranging from 2×10^–4 cm/sec at 30 kV/cm to 3×10^–3 cm/sec at 50 kV/cm. The resealing process of the membrane could be described by two relaxation times, both of which decreased with increasing field strength. ₁ varied from about 3.0 msec at 30 kV/cm to less than 2.0 msec at 50 kV/cm, while ₂ varied from about 100 to about 40 msec in the same interval of field strength. The distribution in the degree of filling of granules that had been partially depleted by an electric field pulse indicated that the population could be considered homogeneous with respect to release.     

Effects of various electric fields on the fusion and in vitro development of mouse two-cell embryos

This study was undertaken to examine the effects of various electric fields such as alternating current (a.c.) voltage, fusion pulse strength, pulse duration, pulse number and electrode geometry on blastomere fusion and developmental rates of mouse two-cell embryos. The a.c. voltages (6 and 12 V/mm) did not affect the fusion and developmental rates. High fusion and developmental rates were obtained when pulse strengths of 1.0 to 2.5 kV/cm, pulse durations of 30 to 90 mu sec and pulse numbers of 1 to 6 were applied using a wire chamber. Comparison of electrode geometries showed that fusion rates were similarly high (93 to 98%) when pulse strengths of 1.0 to 2.5 kV/cm were applied, regardless of the electrode geometry. However, significantly lower developmental rates were observed in a rectangular chamber compared with those in a wire chamber, except when the pulse strength was 1.0 kV/cm. It was further observed that in a rectangular chamber, the developmental rate decreased with increasing pulse strength from 1.0 to 2.0 and 2.5 kV/cm. The results of this study indicate that by using a wire chamber, electric fields can be successfully applied across a relatively wide range of pulse strength, duration and number to provide sufficiently high fusion and subsequent developmental rates. The fusion conditions did, however, vary with chambers of different electrode geometries.     

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.     

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.     

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.     

Expression of voltage-gated calcium channels augments cell susceptibility to membrane disruption by nanosecond pulsed electric field

We compared membrane permeabilization by nanosecond pulsed electric field (nsPEF) in HEK293 cells with and without assembled CaV1.3 L-type voltage-gated calcium channel (VGCC). Individual cells were subjected to one 300-ns pulse at 0 (sham exposure); 1.4; 1.8; or 2.3 kV/cm, and membrane permeabilization was evaluated by measuring whole-cell currents and by optical monitoring of cytosolic Ca²⁺. nsPEF had either no effect (0 and 1.4 kV/cm), or caused a lasting (>80 s) increase in the membrane conductance in about 50% of cells (1.8 kV/cm), or in all cells (2.3 kV/cm). The conductance pathway opened by nsPEF showed strong inward rectification, with maximum conductance increase for the inward current at the most negative membrane potentials. Although these potentials were below the depolarization threshold for VGCC activation, the increase in conductance in cells which expressed VGCC (VGCC+ cells) was about twofold greater than in cells which did not (VGCC− cells). Among VGCC+ cells, the nsPEF-induced increase in membrane conductance showed a positive correlation with the amplitude of VGCC current measured in the same cells prior to nsPEF exposure. These findings demonstrate that the expression of VGCC makes cells more susceptible to membrane permeabilization by nsPEF. Time-lapse imaging of nsPEF-induced Ca²⁺ transients confirmed permeabilization by a single 300-ns pulse at 1.8 or 2.3 kV/cm, but not at 1.4 kV/cm, and the transients were expectedly larger in VGCC+ cells. However, it remains to be established whether larger transients reflected additional Ca²⁺ entry through VGCC, or were a result of more severe electropermeabilization of VGCC+ cells.     

Somatic hybridization between human and mouse lymphoblast cells produced by an electric pulse-induced fusion technique

The technique of electric pulse-induced cell fusion (electro-fusion) was used to obtain heterokaryons between normal human lymphoblasts (HSC93) and mouse leukemic lymphoblasts (MCN151). The two types of cells were brought into contact in the cell suspension by dielectrophoresis with an alternating electric field (0.8 kV/cm, 100 kHz) in the presence of calcium ions and pronase E. Cell fusion was induced by giving two successive electric pulses (3.3 and 5 kV/cm, 10 microsec). Prior treatment of human (but not mouse) lymphoblasts with neuraminidase improved fusion efficiency. Differential staining of the two types of cells with Janus Green and Neutral Red showed that about 40% of the viable fused cells underwent heterokaryonic fusion. We concluded that electrofusion is an efficient method for obtaining heterokaryons from human and mouse lymphoblasts.     

Influence of Pulsed Electric Fields and Mitochondria-Cytoskeleton Interactions on Cell Respiration

Pulsed electric fields with microsecond pulse width (μsPEFs) are used clinically; namely, irreversible electroporation/Nanoknife is used for soft tissue tumor ablation. The μsPEF pulse parameters used in irreversible electroporation (0.5–1 kV/cm, 80–100 pulses, ～100 μs each, 1 Hz frequency) may cause an internal field to develop within the cell because of the disruption of the outer cell membrane and subsequent penetration of the electric field. An internal field may disrupt voltage-sensitive mitochondria, although the research literature has been relatively unclear regarding whether such disruptions occur with μsPEFs. This investigation reports the influence of clinically used μsPEF parameters on mitochondrial respiration in live cells. Using a high-throughput Agilent Seahorse machine, it was observed that μsPEF exposure comprising 80 pulses with amplitudes of 600 or 700 V/cm did not alter mitochondrial respiration in 4T1 cells measured after overnight postexposure recovery. To record alterations in mitochondrial function immediately after μsPEF exposure, high-resolution respirometry was used to measure the electron transport chain state via responses to glutamate-malate and ADP and mitochondrial membrane potential via response to carbonyl cyanide-p-trifluoromethoxyphenylhydrazone. In addition to measuring immediate mitochondrial responses to μsPEF exposure, measurements were also made on cells permeabilized using digitonin and those with compromised cytoskeleton due to actin depolymerization via treatment with the drug latrunculin B. The former treatment was used as a control to tease out the effects of plasma membrane permeabilization, whereas the latter was used to investigate indirect effects on the mitochondria that may occur if μsPEFs impact the cytoskeleton on which the mitochondria are anchored. Based on the results, it was concluded that within the pulse parameters tested, μsPEFs alone do not hinder mitochondrial physiology but can be used to impact the mitochondria upon compromising the actin. Mitochondrial susceptibility to μsPEF after actin depolymerization provides, to our knowledge, a novel avenue for cancer therapeutics.     

DH10B菌株高效电转化条件探究

以pUC19、pECBAC1、pCLD04541DNA以及3个不同大小的BACDNA为材料,研究了E.coli DH10B菌株在5个不同脉冲电场下的转化效率。研究发现,随着DNA片段大小的增加,最高转化效率和最适场强迅速减小。利用DH10B细胞转化pUC19 DNA的最适场强是21kV/cm,而190kb BAC DNA仅为13kV/cm;在最适场强下,40kb BAC DNA的转化效率约是190kb BAC DNA的50倍。通过大量数据绘制了不同因素影响下转化效率的变化曲线,优化了E.coli DH10B菌株电转化条件,为质粒的重组转化以及大片段基因组文库的构建奠定了基础。     

Phase transition of dimyristoylphosphatidylglycerol bilayers induced by electric field pulses

The phase transition of dimyristoylphosphatidylglycerol (DMPG) bilayers has been studied by measurements of light scattering under high electric field pulses. Midpoints of phase transitions have been identified by a clear discontinuity of field induced relaxation amplitudes. We show that the phase transition of DMPG suspensions in monovalent salt is virtually independent of the electric field strength up to approx. 35 kV/cm. A shift of the lipid phase by electric field pulses has been observed, however, for DMPG suspensions in the presence of Ca2+ ions. DMPG suspensions exhibit a jump of the phase transition temperature from 17 degrees C at Ca/DMPG molar ratios r less than 1/7 to 32 degrees C at r greater than 1/7. Field pulses of 60 to 100 microseconds applied to DMPG suspensions with Ca2+ at r greater than 1/7 induce discontinuities of relaxation amplitudes in the temperature range 15 to 22 degrees C in addition to the 'standard' one at 32 degrees C, when the electric field strength is above 15 kV/cm. These results indicate that electric field pulses induce a transition from the phase formed at 'high' Ca(2+)- to the one formed at 'low' Ca(2+)-ion concentrations. Our results are consistent with a dissociation field effect on Ca(2+)-lipid complexes which drives the phase transition.     

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.     

Ion selectivity of temperature-induced and electric field induced pores in dipalmitoylphosphatidylcholine vesicles

Temperature and electric field are known to alter the permeability of the bilayer membrane in phospholipid vesicles. A study of cation selectivity of these membrane pores is reported for multilamellar liposomes (MLV) and unilamellar large vesicles (ULV, 95 +/- 5 nm diameter) of dipalmitoylphosphatidylcholine (DPPC). The permeability of ULV to Rb+ was 1.0 X 10(-6) micrograms/s at 22 degrees C and increased to 1.1 X 10(-5) micrograms/s at the gel to liquid-crystalline transition temperature (Tm) of the bilayer, at 42 degrees C. The permeability of ULV to Rb+ continued to increase beyond the Tm and reached 1.0 X 10(-4) micrograms/s at 56 degrees C, a 100-fold increase over the permeability at 22 degrees C. In contrast, the permeability of ULV to Na+ showed a local maximum of 6.0 X 10(-6) micrograms/s at 42 degrees C and decreased at temperatures higher or lower than the Tm. For MLV, the permeability to both Rb+ and Na+ peaked dramatically at the phase transition temperature, 42 degrees C, and subsided at lower and higher temperatures. When ULV were exposed to an electric field, the permeability to Rb+, Na+, and sucrose surged at a field strength of 30 kV/cm; 30 kV/cm can induce a transmembrane potential of 210 mV. In ULV, the electrically perforated lipid bilayer exhibited selectivity for Rb+ over Na+ only at a narrow electric field range, between 31 and 33 kV/cm. For MLV, no well-defined breakdown voltage was recorded.(ABSTRACT TRUNCATED AT 250 WORDS)