Search

Electric shocks, the only effective therapy for ventricular fibrillation, also electroporate cardiac cells and contribute to the high-mortality post-cardiac arrest syndrome. Copolymers such as Poloxamer 188 (P188) are known to preserve the membrane integrity and viability of electroporated cells, but their utility against cardiac injury from cardiopulmonary resuscitation (CPR) remains to be established. We studied the time course of cell killing, mechanisms of cell death, and protection with P188 in AC16 human cardiomyocytes exposed to micro- or nanosecond pulsed electric field (μsPEF and nsPEF) shocks. A 3D printer was customized with an electrode holder to precisely position electrodes orthogonal to a cell monolayer in a nanofiber multiwell plate. Trains of nsPEF shocks (200, 300-ns pulses at 1.74 kV) or μsPEF shocks (20, 100-μs pulses at 300 V) produced a non-uniform electric field enabling efficient measurements of the lethal effect in a wide range of the electric field strength. Cell viability and caspase 3/7 expression were measured by fluorescent microscopy 2–24 h after the treatment. nsPEF shocks caused little or no caspase 3/7 activation; most of the lethally injured cells were permeable to propidium dye already at 2 h after the exposure. In contrast, μsPEF shocks caused strong activation of caspase 3/7 at 2 h and the number of dead cells grew up to 24 h, indicating the prevalence of the apoptotic death pathway. P188 at 0.2–1% reduced cell death, suggesting its potential utility in vivo to alleviate electric injury from defibrillation.

The quest for safe and effective ablation resulted in the development of nanosecond pulsed electric fields (nsPEF) technology for tumor treatment. For future applications of nsPEF in urothelial cancer treatment, we evaluated the effect of urine presence at the ablation site. We prepared artificial urine (AU) with compounds commonly present in the healthy human urine at physiological concentrations. We compared nsPEF cytotoxicity for cancerous (T24) and non-cancerous (SV-HUC-1) human urothelial cell lines pulsed either in the AU or in a physiological solution (PS). Cell monolayers were exposed to trains of 300-ns, 10-Hz pulses using a two-needle electrode assembly placed orthogonal to the monolayer. The assembly produced the electric field gradually weakening with the distance from the electrodes. The electric field which killed 50 % of cells (LD50) was measured by staining with propidium iodide and matching the stained area with the simulated electric field strength. nsPEF exposure in PS was more cytotoxic to cancer cells. The AU protected both healthy and cancer urothelial cells, increasing their LD50 1.4 and 1.6 times, respectively. Omitting urea from the AU reduced the LD50 for healthy and cancer urothelial cells. Testing the role of other AU components, we found that it was the high concentration of phosphates what also rendered the protective effect of the AU. Our findings suggest that the nsPEF ablation of bladder cancer will be less efficient if the bladder is filled with urine.

Electroporation, in particular with nanosecond pulses, is an efficient technique to generate nanometer-size membrane lesions without the use of toxins or other chemicals. The restoration of the membrane integrity takes minutes and is only partially dependent on [Ca

Exposure of living cells to intense nanosecond pulsed electric field (nsPEF) increases membrane permeability to small solutes, presumably by the formation of nanometer-size membrane lesions. Mechanisms responsible for the restoration of membrane integrity over the course of minutes after nsPEF have not been identified. This study explored if ESCRT-III and Annexin V calcium-dependent repair mechanisms, which play critical role in resealing large membrane lesions, are also activated by electroporation and contribute to the membrane resealing. The extent of membrane damage and the time course of resealing were monitored by the time-lapse imaging of propidium (Pr) uptake in human cervical carcinoma (HeLa) cells exposed to trains of 300-ns PEF. The removal of the extracellular Ca2+ slowed down the resealing, although did not prevent it. Recruitment of CHMP4B protein, a component of ESCRT-III complex, to the electroporated plasma membrane was not observed, thus providing no evidence for possible contribution of the macro-vesicle shedding mechanism. In contrast, silencing the AnxA5 gene impaired resealing and reduced the viability of nsPEF-treated cells. We conclude that Annexin V but not ESCRT-III was involved in the repair of HeLa cells permeabilized by 300-ns stimuli, but it was not the only and perhaps not the main repair mechanism.

Electroporation, in particular with nanosecond pulses, is an efficient technique to generate nanometer-size membrane lesions without the use of toxins or other chemicals. The restoration of the membrane integrity takes minutes and is only partially dependent on [Ca2+]. We explored the impact of Ca2+ on the kinetics of membrane resealing by monitoring the entry of a YO-PRO-1 dye (YP) in BPAE and HEK cells. Ca2+ was promptly removed or added after the electric pulse (EP) by a fast-step perfusion. YP entry increased sharply after the EP and gradually slowed down following either a single- or a double-exponential function. In BPAE cells permeabilized by a single 300- or 600-ns EP at 14 kV/cm in a Ca2+-free medium, perfusion with 2 mM of external Ca2+ advanced the 90% resealing and reduced the dye uptake about twofold. Membrane restoration was accomplished by a combination of fast, Ca2+-independent resealing (τ = 13–15 s) and slow, Ca2+-dependent processes (τ ~70 s with Ca2+ and ~ 110 s or more without it). These time constants did not change when the membrane damage was doubled by increasing EP duration from 300 to 600 ns. However, injury by microsecond-range EP (300 and 600 μs) took longer to recover even when the membrane initially was less damaged, presumably because of the larger size of pores made in the membrane. Full membrane recovery was not prevented by blocking both extra- and intracellular Ca2+ (by loading cells with BAPTA or after Ca2+ depletion from the reticulum), suggesting the recruitment of unknown Ca2+-independent repair mechanisms.

Tumor ablation by nanosecond pulsed electric fields (nsPEF) is an emerging therapeutic modality. We compared nsPEF cytotoxicity for human cell lines of cancerous (IMR-32, Hep G2, HT-1080, and HPAF-II) and non-cancerous origin (BJ and MRC-5) under strictly controlled and identical conditions. Adherent cells were uniformly treated by 300-ns PEF (0–2000 pulses, 1.8 kV/cm, 50 Hz) on indium tin oxide-covered glass coverslips, using the same media and serum. Cell survival plotted against the number of pulses displayed three distinct regions (initial resistivity, logarithmic survival decline, and residual resistivity) for all tested cell types, but with differences in LD(50) spanning as much as nearly 80-fold. The non-cancerous cells were less sensitive than IMR-32 neuroblastoma cells but more vulnerable than the other cancers tested. The cytotoxic efficiency showed no apparent correlation with cell or nuclear size, cell morphology, metabolism level, or the extent of membrane disruption by nsPEF. Increasing pulse duration to 9 μs (0.75 kV/cm, 5 Hz) produced a different selectivity pattern, suggesting that manipulation of PEF parameters can, at least for certain cancers, overcome their resistance to nsPEF ablation. Identifying mechanisms and cell markers of differential nsPEF susceptibility will critically contribute to the proper choice and outcome of nsPEF ablation therapies.

Transforming growth factor (TGF) β1, β2, and β3 (TGF-β1–TGF-β3, respectively) are small secreted signaling proteins that each signal through the TGF-β type I and type II receptors (TβRI and TβRII, respectively). However, TGF-β2, which is well-known to bind TβRII several hundred-fold more weakly than TGF-β1 and TGF-β3, has an additional requirement for betaglycan, a membrane-anchored nonsignaling receptor. Betaglycan has two domains that bind TGF-β2 at independent sites, but how it binds TGF-β2 to potentiate TβRII binding and how the complex with TGF-β, TβRII, and betaglycan undergoes the transition to the signaling complex with TGF-β, TβRII, and TβRI are not understood. To investigate the mechanism, the binding of the TGF-βs to the betaglycan extracellular domain, as well as its two independent binding domains, either directly or in combination with the TβRI and TβRII ectodomains, was studied using surface plasmon resonance, isothermal titration calorimetry, and size-exclusion chromatography. These studies show that betaglycan binds TGF-β homodimers with a 1:1 stoichiometry in a manner that allows one molecule of TβRII to bind. These studies further show that betaglycan modestly potentiates the binding of TβRII and must be displaced to allow TβRI to bind. These findings suggest that betaglycan functions to bind and concentrate TGF-β2 on the cell surface and thus promote the binding of TβRII by both membrane-localization effects and allostery. These studies further suggest that the transition to the signaling complex is mediated by the recruitment of TβRI, which simultaneously displaces betaglycan and stabilizes the bound TβRII by direct receptor–receptor contact.

Accumulating data indicates that some cancer treatments can restore anticancer immunosurveillance through the induction of tumor immunogenic cell death (ICD). Nanosecond pulsed electric fields (nsPEF) have been shown to efficiently ablate melanoma tumors. In this study we investigated the mechanisms and immunogenicity of nsPEF-induced cell death in B16F10 melanoma tumors. Our data show that in vitro nsPEF (20–200, 200-ns pulses, 7 kV/cm, 2 Hz) caused a rapid dose-dependent cell death which was not accompanied by caspase activation or PARP cleavage. The lack of nsPEF-induced apoptosis was confirmed in vivo in B16F10 tumors. NsPEF also failed to trigger ICD-linked responses such as necroptosis and autophagy. Our results point at necrosis as the primary mechanism of cell death induced by nsPEF in B16F10 cells. We finally compared the antitumor immunity in animals treated with nsPEF (750, 200-ns, 25 kV/cm, 2 Hz) with animals were tumors were surgically removed. Compared to the naïve group where all animals developed tumors, nsPEF and surgery protected 33% (6/18) and 28.6% (4/14) of the animals, respectively. Our data suggest that, under our experimental conditions, the local ablation by nsPEF restored but did not boost the natural antitumor immunity which stays dormant in the tumor-bearing host.

Conventional electric stimuli of micro- and millisecond duration excite or activate cells at voltages 10–100 times below the electroporation threshold. This ratio is remarkably different for nanosecond electric pulses (nsEP), which caused excitation and activation only at or above the electroporation threshold in diverse cell lines, primary cardiomyocytes, neurons, and chromaffin cells. Depolarization to the excitation threshold often results from (or is assisted by) the loss of the resting membrane potential due to ion leaks across the membrane permeabilized by nsEP. Slow membrane resealing and the build-up of electroporation damages prevent repetitive excitation by nsEP. However, peripheral nerves and muscles are exempt from this rule and withstand multiple cycles of excitation by nsEP without the loss of function or signs of electroporation. We show that the damage-free excitation by nsEP may be enabled by the membrane charging time constant sufficiently large to (1) cap the peak transmembrane voltage during nsEP below the electroporation threshold, and (2) extend the post-nsEP depolarization long enough to activate voltage-gated ion channels. The low excitatory efficacy of nsEP compared to longer pulses makes them advantageous for medical applications where the neuromuscular excitation is an unwanted side effect, such as electroporation-based cancer and tissue ablation.

The permeabilized condition of the cell membrane after electroporation can last minutes but the underlying mechanisms remain elusive. Previous studies suggest that lipid peroxidation could be responsible for the lasting leaky state of the membrane. The present study aims to link oxidation within the plasma membrane of live cells to permeabilization by electric pulses. We have introduced a method for the detection of oxidation by ratiometric fluorescence measurements of BODIPY-C11 dye using total internal reflection fluorescence (TIRF) microscopy, limiting the signal to the cell membrane. CHO-K1 cells were cultured on glass coverslips coated with an electroconductive indium tin oxide (ITO) layer, which enabled electroporation with micro- and submicrosecond pulses. No oxidation was observed with the electric field directed towards the ITO (cathode), even at field strengths much higher than that needed for permeabilization. Oxidation was readily detectable with the opposite polarity of pulses, but with the threshold higher than the permeabilization threshold. Moreover, a decrease in the medium conductance had opposite effects on permeabilization and lipid oxidation (it enhanced the former and suppressed the latter). We conclude that lipid oxidation can indeed occur at the plasma membrane after electric pulses, but it is not the cause of lasting membrane permeabilization.

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.

Cytosolic DNA sensors are a subgroup of pattern recognition receptors (PRRs) and are activated by the abnormal presence of the DNA in the cytosol. Their activation leads to the upregulation of pro-inflammatory cytokines and chemokines and can also induce cell death. The presence of cytosolic DNA sensors and inflammatory cytokines in TS/A murine mammary adenocarcinoma and WEHI 164 fibrosarcoma cells was demonstrated using real time reverse transcription polymerase chain reaction (RT-PCR), western blotting and enzyme-linked immunosorbent assay (ELISA). After electrotransfer of plasmid DNA (pDNA) using two pulse protocols, the upregulation of DNA-depended activator of interferon regulatory factor or Z-DNA binding protein 1 (DAI/ZBP1), DEAD (Asp-Glu-Ala-Asp) box polypeptide 60 (DDX60) and interferon-inducible protein 204 (p204) mRNAs was observed in both tumor cell lines, but their expression was pulse protocol dependent. A decrease in cell survival was also observed; it was cell type, DNA concentration and pulse protocol dependent. Furthermore, the different protocols of electrotransfer led to different cell death outcomes, necrosis and apoptosis, as indicated by an annexin V and 7AAD assays. The obtained data provide new insights on the presence of cytosolic DNA sensors in tumor cells and the activation of different types of cells death after electrotransfer of pDNA. These observations have important implications on the planning of gene therapy or DNA vaccination protocols.

Ca2 + activation and membrane electroporation by 10-ns and 4-ms electric pulses (nsEP and msEP) were compared in rat embryonic cardiomyocytes. The lowest electric field which triggered Ca2 + transients was expectedly higher for nsEP (36 kV/cm) than for msEP (0.09 kV/cm) but the respective doses were similar (190 and 460 mJ/g). At higher intensities, both stimuli triggered prolonged firing in quiescent cells. An increase of basal Ca2 + level by > 10 nM in cells with blocked voltage-gated Ca2 + channels and depleted Ca2 + depot occurred at 63 kV/cm (nsEP) or 0.14 kV/cm (msEP) and was regarded as electroporation threshold. These electric field values were at 150–230% of stimulation thresholds for both msEP and nsEP, notwithstanding a 400,000-fold difference in pulse duration. For comparable levels of electroporative Ca2 + uptake, msEP caused at least 10-fold greater uptake of propidium than nsEP, suggesting increased yield of larger pores. Electroporation by msEP started Ca2 + entry abruptly and locally at the electrode-facing poles of cell, followed by a slow diffusion to the center. In a stark contrast, nsEP evoked a “supra-electroporation” pattern of slower but spatially uniform Ca2 + entry. Thus nsEP and msEP had comparable dose efficiency, but differed profoundly in the size and localization of electropores.

Experiments with CHO cells exposed to 60 and 300 ns pulsed electric fields with amplitudes in the range from several kV/cm to tens of kV/cm, showed a decrease of the uptake of calcium ions by more than an order of magnitude when, immediately after a first pulse, a second one of opposite polarity was applied. This effect is assumed to be due to the reversal of the electrophoretic transport of ions through the electroporated membrane during the second phase of the bipolar pulse. This assumption, however, is only valid if electrophoresis is the dominant transport mechanism, rather than diffusion. Comparison of calculated calcium ion currents with experimental results showed that for nanosecond pulses, electrophoresis is at least as important as diffusion. By delaying the second pulse with respect to the first one, the effect of reverse electrophoresis is reduced. Consequently, separating nanosecond pulses of opposite polarity by up to approximately hundred microseconds allows us to vary the uptake of ions from very small values to that obtained with two pulses of the same polarity. The measured calcium ion uptake obtained with bipolar pulses also allowed us to determine the membrane pore recovery time. The calculated recovery time constants are on the order of ten microseconds.

Exposure to intense, nanosecond-duration electric pulses (nsEP) opens small but long-lived pores in the plasma membrane. We quantified the cell uptake of two membrane integrity marker dyes, YO-PRO-1 (YP) and propidium (Pr), in order to test whether the pore size is affected by the number of nsEP. The fluorescence of the dyes was calibrated against their concentrations by confocal imaging of stained homogenates of the cells. The calibrations revealed a two-phase dependence of Pr emission on the concentration (with a slower rise at < 4 µM), and a linear dependence for YP. CHO cells were exposed to nsEP trains (1 to 100 pulses, 60 ns, 13.2 kV/cm, 10 Hz) with Pr and YP in the medium, and the uptake of the dyes was monitored by time-lapse imaging for 3 min. Even a single nsEP triggered a modest but detectable entry of both dyes, which increased linearly when more pulses were applied. The influx of Pr per pulse was constant and independent of the pulse number. The influx of YP per pulse was highest with 1- and 2-pulse exposures, decreasing to about twice the Pr level for trains from 5 to 100 pulses. The constant YP/Pr influx ratio for trains of 5 to 100 pulses suggests that increasing the number of pulses permeabilizes cells to a greater extent by increasing the pore number and not the pore diameter.

Disruption of the actin cytoskeleton structures was reported as one of the characteristic effects of nanosecond-duration pulsed electric field (nsPEF) in both mammalian and plant cells. We utilized CHO cells that expressed the monomeric fluorescent protein (mApple) tagged to actin to test if nsPEF modifies the cell actin directly or as a consequence of cell membrane permeabilization. A train of four 600-ns pulses at 19.2 kV/cm (2 Hz) caused immediate cell membrane poration manifested by YO-PRO-1 dye uptake, gradual cell rounding and swelling. Concurrently, bright actin features were replaced by dimmer and uniform fluorescence of diffuse actin. To block the nsPEF-induced swelling, the bath buffer was isoosmotically supplemented with an electropore-impermeable solute (sucrose). A similar addition of a smaller, electropore-permeable solute (adonitol) served as a control. We demonstrated that sucrose efficiently blocked disassembly of actin features by nsPEF, whereas adonitol did not. Sucrose also attenuated bleaching of mApple-tagged actin in nsPEF-treated cells (as integrated over the cell volume), although did not fully prevent it. We conclude that disintegration of the actin cytoskeleton was a result of cell swelling, which, in turn, was caused by cell permeabilization by nsPEF and transmembrane diffusion of solutes which led to the osmotic imbalance.

We demonstrate that conditioning of mammalian cells by electroporation with nanosecond pulsed electric field (nsPEF) facilitates their response to the next nsPEF treatment. The experiments were designed to unambiguously separate the electroporation-induced sensitization and desensitization effects. Electroporation was achieved by bursts of 300-ns, 9 kV/cm pulses (50 Hz, n = 3–100) and quantified by propidium dye uptake within 11 min after the nsPEF exposure. We observed either sensitization to nsPEF or no change (when the conditioning was either too weak or too intense, or when the wait time after conditioning was too short). Within studied limits, conditioning never caused desensitization. With settings optimal for sensitization, the second nsPEF treatment became 2.5 times (25 °C) or even 6 times (37 °C) more effective than the same nsPEF treatment delivered without conditioning. The minimum wait time required for sensitization development was 30 s, with still longer delays increasing the effect. We show that the delayed hypersensitivity was not mediated by either cell swelling or oxidative effect of the conditioning treatment; biological mechanisms underlying the delayed electrosensitization remain to be elucidated. Optimizing nsPEF delivery protocols to induce sensitization can reduce the dose and adverse side effects of diverse medical treatments which require multiple pulse applications.

Cellular effects caused by nanosecond electric pulses (nsEP) can be reduced by an electric field reversal, a phenomenon known as bipolar cancellation. The reason for this cancellation effect remains unknown. We hypothesized that assisted membrane discharge is the mechanism for bipolar cancellation. CHO-K1 cells bathed in high (16.1mS/cm; HCS) or low (1.8mS/cm; LCS) conductivity solutions were exposed to either one unipolar (300-ns) or two opposite polarity (300+300-ns; bipolar) nsEP (4-40kV/cm) with increasing interpulse intervals (0.1-50μs). Time-lapse YO-PRO-1 (YP) uptake revealed enhanced membrane permeabilization in LCS compared to HCS at all tested voltages. The time-dependence of bipolar cancellation was similar in both solutions, using either identical (22kV/cm) or isoeffective nsEP treatments (12 and 32kV/cm for LCS and HCS, respectively). However, cancellation was significantly stronger in LCS when the bipolar nsEP had no, or very short (1μs), interpulse intervals. Finally, bipolar cancellation was still present with interpulse intervals as long as 50μs, beyond the time expected for membrane discharge. Our findings do not support assisted membrane discharge as the mechanism for bipolar cancellation. Instead they exemplify the sustained action of nsEP that can be reversed long after the initial stimulus.

Opening of long-lived pores in the cell membrane is the principal primary effect of intense, nanosecond pulsed electric field (nsPEF). Here we demonstrate that the evolution of pores, cell survival, the time and the mode of cell death (necrotic or apoptotic) are determined by the level of external Ca(2+) after nsPEF. We also introduce a novel, minimally disruptive technique for nsEP exposure of adherent cells on indium tin oxide (ITO)-coated glass coverslips, which does not require cell detachment and enables fast exchanges of bath media. Increasing the Ca(2+) level from the nominal 2-5μM to 2mM for the first 60-90min after permeabilization by 300-nsPEF increased the early (necrotic) death in U937, CHO, and BPAE cells. With nominal Ca(2+), the inhibition of osmotic swelling rescued cells from the early necrosis and increased caspase 3/7 activation later on. However, the inhibition of swelling had a modest or no protective effect with 2mM Ca(2+) in the medium. With the nominal Ca(2+), most cells displayed gradual increase in YO-PRO-1 and propidium (Pr) uptake. With 2mM Ca(2+), the initially lower Pr uptake was eventually replaced by a massive and abrupt Pr entry (necrotic death). It was accompanied by a transient acceleration of the growth of membrane blebs due to the increase of the intracellular osmotic pressure. We conclude that the high-Ca(2+)-dependent necrotic death in nsPEF-treated cells is effected by a delayed, sudden, and osmotically-independent pore expansion (or de novo formation of larger pores), but not by the membrane rupture.

Summary Community-acquired respiratory distress syndrome (CARDS) toxin from Mycoplasma pneumoniae is a 591-amino-acid virulence factor with ADP-ribosyltransferase (ADPRT) and vacuolating activities. It is expressed at low levels during in vitro growth and at high levels during colonization of the lung. Exposure of experimental animals to purified recombinant CARDS toxin alone is sufficient to recapitulate the cytopathology and inflammatory responses associated with M. pneumoniae infection in humans and animals. Here, by molecular modelling, serial truncations and site-directed mutagenesis, we show that the N-terminal region is essential for ADP-ribosylating activity. Also, by systematic truncation and limited proteolysis experiments we identified a portion of the C-terminal region that mediates toxin binding to mammalian cell surfaces and subsequent internalization. In addition, the C-terminal region alone induces vacuolization in a manner similar to full-length toxin. Together, these data suggest that CARDS toxin has a unique architecture with functionally separable N-terminal and C-terminal domains.

Nanosecond-duration electric stimuli are distinguished by the ability to permeabilize intracellular membranes and recruit Ca2+ from intracellular stores. We quantified this effect in non-excitable cells (CHO) using ratiometric Ca2+ imaging with Fura-2. In a Ca(2+)-free medium, 10-, 60-, and 300-ns stimuli evoked Ca2+ transients by mobilization of Ca2+ from the endoplasmic reticulum. With 2 mM external Ca2+, the transients included both extra- and intracellular components. The recruitment of intracellular Ca2+ increased as the stimulus duration decreased. At the threshold of 200-300 nM, the transients were amplified by calcium-induced calcium release. We conclude that nanosecond stimuli mimic Ca2+ signaling while bypassing the usual receptor- and channels-mediated cascades. The recruitment of the intracellular Ca2+ can be controlled by the duration of the stimulus.

Cell permeabilization by electric pulses (EP), or electroporation, is widely used for intracellular delivery of drugs and plasmids, as well as for tumour and tissue ablation. We found that cells pre-treated with 100-μs EP develop delayed hypersensitivity to subsequent EP applications. Sensitizing B16 and CHO cells by splitting a single train of eight 100-μs EP into two trains of four EP each (with 5-min. interval) decreased the LD(50) 1.5-2 times. Sensitization profoundly enhanced the electroporation-assisted uptake of bleomycin, a cell-impermeable cytotoxic agent accepted for killing tumours by electrochemotherapy. EP exposures that were not lethal per se caused cell death in the presence of bleomycin and proportionally to its concentration. Sensitizing cells by a split-dose EP exposure increased bleomycin-mediated lethality to the same extent as a 10-fold increase in bleomycin concentration when using a single EP dose. Likewise, sensitization by a split-dose EP exposure (without changing the overall dose, pulse number, or amplitude) enhanced the electroporative uptake of propidium up to fivefold. Enhancement of the electroporative uptake appears a key mechanism of electrosensitization and may benefit electrochemotherapy and numerous applications that employ EP for cell permeabilization.

Electric pulses of nanosecond duration (nsEP) are emerging as a new modality for tissue ablation. Plasma membrane permeabilization by nsEP may cause osmotic imbalance, water uptake, cell swelling, and eventual membrane rupture. The present study was aimed to increase the cytotoxicity of nsEP by fostering water uptake and cell swelling. This aim was accomplished by lowering temperature after nsEP application, which delayed the membrane resealing and/or suppressed the cell volume mechanisms. The cell diameter in U-937 monocytes exposed to a train of 50, 300-ns pulses (100 Hz, 7 kV/cm) at room temperature and then incubated on ice for 30 min increased by 5.6 +/− 0.7 μm (40–50%), which contrasted little or no changes (1 +/− 0.3 μm

Cell sensitization is a phenomenon where increasing the duration of the electroporation treatment has been reported to increase cell permeabilization and decrease cell survival. Cell sensitization can be obtained by splitting one train of pulses in half and delivering the second half of the pulses after a delay. After the first half of the pulses is applied cells become more sensitive to the following electric pulses. Thus, efficiency of the treatment is sustained even if the second half of the pulses is of lower amplitude. In this study, cell sensitization was investigated in a wide range of electric field amplitudes. Twelve pulses of 100 μs were delivered either twelve in one train (one train protocol) or six in the first train and after 5 min another six in the second train (two trains protocol). In both protocols, the electric field of the first six pulses was varied while the electric field of the second six pulses was fixed or vice versa. Stable cell sensitization was obtained with two trains protocol in a wide range of “permeabilizing” electric fields. Cell survival was reduced up to twofold with the two trains protocol in comparison to the one train protocol. Cell sensitization has possible applications in tumor treatment and in soft tissue ablation. In tumor treatment fewer pulses of lower electric field could be applied and electrodes with larger inter-electrode distance could be used while the efficiency of the treatment would be at least as high as obtained now. In the future, research should focus on the still unknown mechanisms of cell sensitization and then extend to 3-dimensional tissue models and tissues.

Nanosecond pulsed electric field (nsPEF) is a novel modality for permeabilization of membranous structures and intracellular delivery of xenobiotics. We hypothesized that oxidative effects of nsPEF could be a separate primary mechanism responsible for bioeffects. ROS production in cultured cells and media exposed to 300-ns PEF (1-13 kV/cm) was assessed by oxidation of 2',7'-dichlorodihydrofluoresein (H(2)DCF), dihidroethidium (DHE), or Amplex Red. When a suspension of H(2)DCF-loaded cells was subjected to nsPEF, the yield of fluorescent 2',7'-dichlorofluorescein (DCF) increased proportionally to the pulse number and cell density. DCF emission increased with time after exposure in nsPEF-sensitive Jurkat cells, but remained stable in nsPEF-resistant U937 cells. In cell-free media, nsPEF facilitated the conversion of H(2)DCF into DCF. This effect was not related to heating and was reduced by catalase, but not by mannitol or superoxide dismutase. Formation of H(2)O(2) in nsPEF-treated media was confirmed by increased oxidation of Amplex Red. ROS increase within individual cells exposed to nsPEF was visualized by oxidation of DHE. We conclude that nsPEF can generate both extracellular (electrochemical) and intracellular ROS, including H(2)O(2) and possibly other species. Therefore, bioeffects of nsPEF are not limited to electropermeabilization; concurrent ROS formation may lead to cell stimulation and/or oxidative cell damage.

Nanosecond electric pulses (EP) disrupt cell membrane and organelles and cause cell death in a manner different from the conventional irreversible electroporation. We explored the cytotoxic effect of 10-ns EP (quantitation, mechanisms, efficiency, and specificity) in comparison with 300-ns, 1.8- and 9-μs EP.Effects in Jurkat and U937 cells were characterized by survival assays, DNA electrophoresis and flow cytometry.10-ns EP caused apoptotic or necrotic death within 2-20 h. Survival (S, %) followed the absorbed dose (D, J/g) as: S=alphaD((-K)), where coefficients K and alpha determined the slope and the "shoulder" of the survival curve. K was similar in all groups, whereas alpha was cell type- and pulse duration-dependent. Long pulses caused immediate propidium uptake and phosphatidylserine (PS) externalization, whereas 10-ns pulses caused PS externalization only.1.8- and 9-μs EP cause cell death efficiently and indiscriminately (LD₅₀ 1-3 J/g in both cell lines); 10-ns EP are less efficient, but very selective (LD₅₀ 50-80 J/g for Jurkat and 400-500 J/g for U937); 300-ns EP show intermediate effects. Shorter EP open propidium-impermeable, small membrane pores ("nanopores"), triggering different cell death mechanisms.Nanosecond EP can selectively target certain cells in medical applications like tumor ablation.

The exclusion of polar dyes by healthy cells is widely employed as a simple and reliable test for cell membrane integrity. However, commonly used dyes (propidium, Yo-Pro-1, trypan blue) cannot detect membrane defects which are smaller than the dye molecule itself, such as nanopores that form by exposure to ultrashort electric pulses (USEPs). Instead, here we demonstrate that opening of nanopores can be efficiently detected and studied by fluorescent measurement of Tl(+) uptake. Various mammalian cells (CHO, GH3, NG108), loaded with a Tl(+)-sensitive fluorophore FluxOR and subjected to USEPs in a Tl(+)-containing bath buffer, displayed an immediate (within100 ms), dose-dependent surge of fluorescence. In all tested cell lines, the threshold for membrane permeabilization to Tl(+) by 600-ns USEP was at 1-2 kV/cm, and the rate of Tl(+) uptake increased linearly with increasing the electric field. The lack of concurrent entry of larger dye molecules suggested that the size of nanopores is less than 1-1.5 nm. Tested ion channel inhibitors as well as removal of the extracellular Ca(2+) did not block the USEP effect. Addition of a Tl(+)-containing buffer within less than 10 min after USEP also caused a fluorescence surge, which confirms the minutes-long lifetime of nanopores. Overall, the technique of fluorescent detection of Tl(+) uptake proved highly effective, noninvasive and sensitive for visualization and analysis of membrane defects which are too small for conventional dye uptake detection methods.

Cell permeabilization by electric pulses (EPs), or electroporation, has been well established as a tool to indiscriminately increase membrane flows of water solutes down the concentration and voltage gradients. However, we found that EPs of nanosecond duration (nsEPs) trigger formation of voltage-sensitive and inward-rectifying membrane pores. NsEP-treated cells remain mostly impermeable to propidium, suggesting that the maximum pore size is approximately 1nm. The ion-channel-like properties of nsEP-opened nanopores vanish if they break into larger, propidium-permeable "conventional" pores. However, nanopores can be stable for many minutes and significantly impact cell electrolyte and water balance. Multiple nsEPs cause fast cell swelling and blebbing, whereas opening of larger pores with digitonin abolishes swelling and causes blebs to implode. The lipid nature of nsEP-opened nanopores is confirmed by fast externalization of phosphatidylserine residues. Nanopores constitute a previously unexplored ion transport pathway that supplements classic ion channels but is distinctly different from them.

Mammalian cells exposed to electric field pulses of nanosecond duration (nsPEF; 60-ns, 12 kV/cm) experienced a profound and long-lasting increase in passive electrical conductance (G(m)) of the cell membrane, probably caused by opening of stable conductance pores (CPs). The CPs were permeable to Cl(-) and alkali metal cations, but not to larger molecules such as propidium iodide (PI). CPs gradually resealed; the process took minutes and could be observed even in dialyzed cells and in ATP- and glucose-free solutions. Cells subjected to long nsPEF trains (up to 200 pulses) underwent severe and immediate necrotic transformation (cell swelling, blebbing, cytoplasm granulation), but remained impermeable to PI for at least 30-60 min after the exposure. Both G(m) increase after short nsPEF trains and necrotic changes after long nsPEF trains were cell type-dependent: they were much weaker in HeLa than in GH3 cells. La(3+) and Gd(3+) ions significantly inhibited the nsPEF-induced G(m) increase (probably by blocking the CPs), and effectively protected intensely exposed cells from developing necrosis. We conclude that plasma membrane permeabilization is the principal cause of necrotic transformation in nsPEF-exposed cells and probably contributes to other known nsPEF bioeffects.

Acinetobacter baumannii is an environmentally resilient healthcare-associated opportunistic pathogen responsible for infections at many body sites. In the last 10 years, clinical strains resistant to many or all commonly used antibiotics have emerged globally. With few antimicrobial agents in the pharmaceutical pipeline, new and alternative agents are essential. Platelets secrete a large number of proteins, including proteins with antimicrobial activity. In a previous study, we demonstrated that donor platelet supernatants and plasma significantly inhibited the growth of a reference strain of A. baumannii in broth and on skin. This inhibition appeared to be unrelated to the platelet activation state. In this study, we demonstrate that this growth inhibition extends to clinical multidrug resistant isolates. We also demonstrate that there is no relationship between this activity and selected platelet-derived antimicrobial proteins. Instead, the donor plasma components complement and alpha-2 macroglobulin are implicated.

Significance The airway pathogen Mycoplasma pneumoniae ( Mp ) produces a virulence factor with ADP-ribosyltransferase and vacuolating activities known as Community-Acquired Respiratory Distress Syndrome Toxin (CARDS TX). Mammalian cells exposed to recombinant CARDS TX exhibit distinct patterns of ADP-ribosylated proteins and unusual vacuolation phenotypes with disruption of monolayer integrity, leading to cell death. Recombinant CARDS TX administered to naive mice induces an allergic-type inflammatory response and airway hyperreactivity, suggesting that an analogous response in humans may play a causal role in Mp -associated asthma. Here we present the structure of CARDS TX, the newest member of the well-recognized group of ADP-ribosylating toxins. The structure enhances understanding of Mp pathogenicity and provides a platform for the development of therapies to treat Mp -associated acute and chronic airway diseases.

The study explored the effect of ambient oxygen on mammalian cell survival after exposure to 10 ns duration, high voltage electrical pulses (nsEP, 80-90 or 120-130 kV/cm; 200-400 pulses per exposure). Cell samples were equilibrated with pure nitrogen, atmospheric air, or pure oxygen prior to the nsEP treatment and were returned to the incubator (air + 5% CO2) shortly after the exposure. The experiments established that survival of hypoxic Jurkat and U937 cells exceeded that of air-equilibrated controls about twofold (P < .01). Conversely, saturation of the medium with oxygen prior to exposure decreased Jurkat cell survival about 1.5 times, P < .01. Attenuation of the cytotoxic effect under hypoxic conditions resembled a well-known effect of oxygen on cell killing by sparsely ionizing radiations and may be indicative of the similarity of underlying cell damage mechanisms.

Transforming growth factor-beta (TGFbeta) isoforms initiate signaling by assembling a heterotetrameric complex of paired type I (TbetaRI) and type II (TbetaRII) receptors on the cell surface. Because two of the ligand isoforms (TGFbetas 1, 3) must first bind TbetaRII to recruit TbetaRI into the complex, and a third (TGFbeta2) requires a co-receptor, assembly is known to be sequential, cooperative and isoform-dependent. However the source of the cooperativity leading to recruitment of TbetaRI and the universality of the assembly mechanism with respect to isoforms remain unclear. Here, we show that the extracellular domain of TbetaRI (TbetaRI-ED) binds in vitro with high affinity to complexes of the extracellular domain of TbetaRII (TbetaRII-ED) and TGFbetas 1 or 3, but not to either ligand or receptor alone. Thus, recruitment of TbetaRI requires combined interactions with TbetaRII-ED and ligand, but not membrane attachment of the receptors. Cell-based assays show that TbetaRI-ED, like TbetaRII-ED, acts as an antagonist of TGFbeta signaling, indicating that receptor-receptor interaction is sufficient to compete against endogenous, membrane-localized receptors. On the other hand, neither TbetaRII-ED, nor TbetaRII-ED and TbetaRI-ED combined, form a complex with TGFbeta2, showing that receptor-receptor interaction is insufficient to compensate for weak ligand-receptor interaction. However, TbetaRII-ED does bind with high affinity to TGFbeta2-TM, a TGFbeta2 variant substituted at three positions to mimic TGFbetas 1 and 3 at the TbetaRII binding interface. This proves both necessary and sufficient for recruitment of TbetaRI-ED, suggesting that the three different TGFbeta isoforms induce assembly of the heterotetrameric receptor complex in the same general manner.

Community-acquired respiratory distress syndrome (CARDS) toxin from Mycoplasma pneumoniae is a 591-amino-acid virulence factor with ADP-ribosyltransferase (ADPRT) and vacuolating activities. It is expressed at low levels during in vitro growth and at high levels during colonization of the lung. Exposure of experimental animals to purified recombinant CARDS toxin alone is sufficient to recapitulate the cytopathology and inflammatory responses associated with M. pneumoniae infection in humans and animals. Here, by molecular modelling, serial truncations and site-directed mutagenesis, we show that the N-terminal region is essential for ADP-ribosylating activity. Also, by systematic truncation and limited proteolysis experiments we identified a portion of the C-terminal region that mediates toxin binding to mammalian cell surfaces and subsequent internalization. In addition, the C-terminal region alone induces vacuolization in a manner similar to full-length toxin. Together, these data suggest that CARDS toxin has a unique architecture with functionally separable N-terminal and C-terminal domains.

Protein SRP19 is an important component of the signal recognition particle (SRP) as it promotes assembly of protein SRP54 with SRP RNA and recognizes a tetranucleotide loop. Structural features and RNA binding activities of SRP19 of the hyperthermophilic archaeon Archaeoglobus fulgidus were investigated. An updated alignment of SRP19 sequences predicted three conserved regions and two alpha-helices. With Af-SRP RNA the Af-SRP54 protein assembled into an A. fulgidus SRP which remained intact for many hours. Stable complexes were formed between Af-SRP19 and truncated SRP RNAs, including a 36-residue fragment representing helix 6 of A. fulgidus SRP RNA.

Community-acquired respiratory distress syndrome toxin (CARDS TX) is a 591-amino-acid protein with ADP-ribosyltransferase and vacuolating activities that damages the cells lining the respiratory tracts of patients infected with the bacterial pathogen Mycoplasma pneumoniae. Crystals of CARDS TX were grown in space group C2, with unit-cell parameters a = 191.4, b = 107.4, c = 222.1 A, beta = 90.6 degrees. A complete 2.2 A data set was obtained from a single CARDS TX crystal.

Binding of yeast ribosomal protein L5 with 5S rRNA has long been considered a promising model for studying molecular mechanisms of protein-RNA interactions. However, in vitro assembly of a ribonucleoprotein (RNP) complex from purified yeast ribosomal protein L5 (also known as L1, L1a, or YL3) and 5S rRNA proved to be difficult, thus limiting the utility of this model. In the present report, we present data on the successful in vitro assembly of a RNP complex using a fusion (MBP-L5) protein consisting of the yeast ribosomal protein L5 fused to the carboxyl terminus of the E. coli maltose-binding protein (MBP). We demonstrated that: 1) the MBP-L5 protein binds yeast 5S rRNA but not 5.8S rRNA in vitro; 2) the MBP protein itself does not bind yeast 5S rRNA; 3) formation of the RNP complex is proportional to the concentration of MBP-L5 protein and 5S rRNA; and 4) the MBP moiety of the fusion protein in the RNP complex can be removed with factor Xa. The electrophoretic mobility of the resultant RNP complex is indistinguishable from that of L5-5S rRNA complex isolated from the ribosome. Using this new experimental approach, we further showed that the RNA binding capability of a mutant L5 protein is decreased by 60% compared to the wild-type protein. Additionally, the mutant RNP complex migrates slower than the wild-type RNP complex suggesting that the mutant RNP complex has a less compact conformation. The finding provides a probable explanation for an earlier observation that the 60S ribosomal subunit containing the mutant protein is unstable.

In recent years, research into biological and medical effects of millimeter waves (MMW) has expanded greatly. This paper analyzes general trends in the area and briefly reviews the most significant publications, proceeding from cell-free systems, dosimetry, and spectroscopy issues through cultured cells and isolated organs to animals and humans. The studies reviewed demonstrate effects of low-intensity MMW (10 mW/cm2 and less) on cell growth and proliferation, activity of enzymes, state of cell genetic apparatus, function of excitable membranes, peripheral receptors, and other biological systems. In animals and humans, local MMW exposure stimulated tissue repair and regeneration, alleviated stress reactions, and facilitated recovery in a wide range of diseases (MMW therapy). Many reported MMW effects could not be readily explained by temperature changes during irradiation. The paper outlines some problems and uncertainties in the MMW research area, identifies tasks for future studies, and discusses possible implications for development of exposure safety criteria and guidelines.

Effects of millimeter waves (MMW) on cell survival and ultraviolet-induced reciprocal and non-reciprocal recombination and mutagenesis were studied in the diploid D7 strain of the yeast Saccharomyces cerevisiae. MMW exposures lasted for 30 min (0.13 mW cm−2, 61.02–61.42 GHz) and were followed in 60 min by a 100 J m−2 dose of 254 nm ultraviolet (UV) radiation. The effect of the exposures was evaluated from the colony-forming ability of the cells on complete and selective media, and from the number of aberrant colonies formed. The MMW pretreatment did not alter cell survival or the frequency of reverse mutations. The incidence of conversions was higher in most cases in the MMW-treated cells (p < 0.05). MMW also increased the scores of crossover and colored aberrants in isolated experiments, though the average increse for all experiments (performed with different MMW frequencies) was not statistically significant. The results suggested that the MMW irradiation did not alter the UV-induced mutagenesis, but could facilitate recombinagenic processes.

Genetic effects of ultrawide-band (UWB) radiation pulses were studied in the D7 strain of yeast Saccharomyces cerevisiae. Yeast cells were exposed in suspension for 30 min at the UWB pulse repetition rates of 0 Hz (sham treatment), 16 Hz, and 600 Hz. Measured parameters of UWB pulses were as following: 101-104 kV/m peak voltage, 164-166 ps rise time, 1.01-1.02 ns pulse width, and 0 Hz-2 GHz spectral bandwidth. Cells were plated immediately after the exposure and incubated for 7 days at 30°C; then normal and aberrant colonies (mitotic crossovers, segregants, revertants, and convertants) were scored. The experiments established no statistically significant effect of UWB exposure on the colony-forming ability of yeast cells or the occurrence of mutations and chromosome recombinations.

Electroporation-induced cell sensitization was described as the occurrence of a delayed hypersensitivity to electric pulses caused by pretreating cells with electric pulses. It was achieved by increasing the duration of the electroporation treatment at the same cumulative energy input. It could be exploited in electroporation-based treatments such as electrochemotherapy and tissue ablation with irreversible electroporation. The mechanisms responsible for cell sensitization, however, have not yet been identified. We investigated cell sensitization dynamics in five different electroporation buffers. We split a pulse train into two trains varying the delay between them and measured the propidium uptake by fluorescence microscopy. By fitting the first-order model to the experimental results, we determined the uptake due to each train (i.e. the first and the second) and the corresponding resealing constant. Cell sensitization was observed in the growth medium but not in other tested buffers. The effect of pulse repetition frequency, cell size change, cytoskeleton disruption and calcium influx do not adequately explain cell sensitization. Based on our results, we can conclude that cell sensitization is a sum of several processes and is buffer dependent. Further research is needed to determine its generality and to identify underlying mechanisms.

Intense, nanosecond-duration electric pulses (nsEP) have been introduced as a novel modality to alter cellular function, with a mechanism of action qualitatively different from micro- and millisecond duration pulses used in electroporation. In this study, we determined the thresholds for plasma membrane injury (within 15 minutes) and cell death (at 24 hours) for 4 different cell types (CHO-K1, HeLa, Jurkat and U937). Plasma membrane injury was measured by flow cytometry using two fluorescent dyes, namely Annexin V-FITC, which binds to phosphatidylserine (PS) upon its externalization (subtle membrane injury), and propidium iodide (PI), which is typically impermeable to the cell, but enters when large pores are formed in the plasma membrane. In all cell types, 10-ns pulses caused phosphatidylserine (PS) externalization at low doses (

Chemical and physical insults such as electroporation may compromise the membrane integrity and allow leak ion currents through de-novo formed lipid pores. These pores are thought to short-circuit the membrane and hinder ion channels' physiological function rather than to complement it. However, here we report that brief electric stimuli can trigger formation of membrane pores with specific behaviors that are traditionally considered to be unique for protein ion channels; still other behaviors of these pores distinguish them from both “conventional” electropores and any known ion channels. We found that a single electric shock (600-ns duration, 1 to 5 kV/cm) causes minutes-long increase of membrane electrical conductance due to formation of long-lived, voltage- and current-sensitive, rectifying, cation-selective, asymmetrical pores of nanometer diameter (“nanopores”). Once induced, nanopores oscillate between open and quasi-open (electrically silent) states, followed by either gradual resealing or abrupt breakdown into larger pores, with immediate loss of nanopore-specific behaviors. The formation and extended lifetime of nanopores were verified by non-electrophysiological methods, namely by fluorescent detection of Tl+ uptake and of phosphatidylserine externalization. Apparently, nanopores are not unique to cell stimulation with nanosecond electric pulses, but may form under various physiological and pathological conditions. Nanopores appear adequately equipped for certain functions that are traditionally ascribed to ion channels. Clear distinction between nanopores- and ion channels-mediated currents may be critical for understanding how these currents are controlled.Supported by NIH (NCI) R01CA125482.

We found that ultra-short electric pulses (60 or 600 ns duration) applied to mammalian cells cause profound, dose-dependent increase of plasma membrane electrical conductance. This effect is detectable even minutes after the exposure and is explained by formation of long-lived, voltagesensitive, inward-rectifying pores of nanometer diameter (”nanopores”). The phenomenon of nanoelectroporation and the extended lifetime of nanopores can also be demonstrated by a surge of Tl + uptake in the presence of K + channel blockers, as well as in CHO cells that express no endogenous voltage-gated K + channels. Due to their long lifetime, nanopores can have significant impact on cell physiology.

Cell samples of the yeast Saccharomyces cerevisiae were exposed to 100 J/m2 of 254 nm ultraviolet (UV) radiation followed by a 30 min treatment with ultra-wide band (UWB) electromagnetic pulses. The UWB pulses (101-104 kV/m, 1.0 ns width, 165 ps rise time) were applied at the repetition rates of 0 Hz (sham), 16 Hz, or 600 Hz. The effect of exposures was evaluated from the colony-forming ability of the cells on complete and selective media and the number of aberrant colonies. The experiments established no effect of UWB exposure on the UV-induced reciprocal and non-reciprocal recombination, mutagenesis, or cell survival.

Protein SRP19 is an essential RNA-binding component of the signal recognition particle (SRP) in Archaea and Eucarya. A three-dimensional solution structure of the 104 residue SRP19 from the hyperthermophilic archaeon Archaeoglobus fulgidus, designated as Af19, was determined by NMR spectroscopy. Af19 contains three beta-strands, two alpha-helical regions, arranged in a betaalphabetabetaalpha topology, a 3(10) helix, and a disordered C-terminal tail. This fold is similar to the betaalphabetabetaalphabeta RNP motif present in numerous other RNA-binding proteins, which engage their cognate RNAs using conserved sequence motifs present within beta-strands 1 and 3. Mutagenesis studies of human SRP19, however, reveal the major contact sites with SRP RNA reside within loops 1, 3, and 4. These contacts were verified by the crystal structure of human SRP19 complexed to SRP RNA helix 6 reported subsequent to the submission of the manuscript. The crystal structure also reveals that, unlike canonical RNP motifs, SRP19 does not engage specific RNA bases through conserved sequence motifs present within beta-strands 1 and 3. Instead, SRP19 uses residues both within and flanking beta-strand 1 to stabilize the complex through direct and indirect contacts to the phosphate backbone of the tetraloop, leaving the bases of the tetraloop exposed. This, coupled with the fact that SRP19 appears relatively rigid and undergoes only minor changes in structure upon RNA binding, may underlie the molecular basis by which SRP19 functions to initiate SRP assembly.

Background Electroporation is a method of disrupting the integrity of cell membrane by electric pulses (EPs). Electrical modeling is widely employed to explain and study electroporation, but even most advanced models show limited predictive power. No studies have accounted for the biological consequences of electroporation as a factor that alters the cell's susceptibility to forthcoming EPs. Methodology/Principal Findings We focused first on the role of EP rate for membrane permeabilization and lethal effects in mammalian cells. The rate was varied from 0.001 to 2,000 Hz while keeping other parameters constant (2 to 3,750 pulses of 60-ns to 9-µs duration, 1.8 to 13.3 kV/cm). The efficiency of all EP treatments was minimal at high rates and started to increase gradually when the rate decreased below a certain value. Although this value ranged widely (0.1–500 Hz), it always corresponded to the overall treatment duration near 10 s. We further found that longer exposures were more efficient irrespective of the EP rate, and that splitting a high-rate EP train in two fractions with 1–5 min delay enhanced the effects severalfold. Conclusions/Significance For varied experimental conditions, EPs triggered a delayed and gradual sensitization to EPs. When a portion of a multi-pulse exposure was delivered to already sensitized cells, the overall effect markedly increased. Because of the sensitization, the lethality in EP-treated cells could be increased from 0 to 90% simply by increasing the exposure duration, or the exposure dose could be reduced twofold without reducing the effect. Many applications of electroporation can benefit from accounting for sensitization, by organizing the exposure either to maximize sensitization (e.g., for sterilization) or, for other applications, to completely or partially avoid it. In particular, harmful side effects of electroporation-based therapies (electrochemotherapy, gene therapies, tumor ablation) include convulsions, pain, heart fibrillation, and thermal damage. Sensitization can potentially be employed to reduce these side effects while preserving or increasing therapeutic efficiency.