Tina Batista Napotnik’s research while affiliated with University of Ljubljana and other places

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Publications (21)


Cardiac Action Potentials, Ion Channels, and Gap Junctions
  • Chapter

December 2024

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8 Reads

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Tina Batista Napotnik

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It is the interplay between various ion channels within the membranes of cardiomyocytes that is responsible for depolarization and repolarization of the heart cells. Cell-to-cell coupling between myocytes is mediated via gap junction proteins and is involved in overall propagation of action potentials throughout the heart. In this chapter, different phases of the action potential of heart cells are discussed, and the role and characteristics of the most important ion channels that are active during these phases are conferred. Differences in the expressions of the various ion and gap junction channels under normal and certain pathological conditions are described.


S-HEK cells are able to generate APs whereas NS-HEK are not. (a,b) A monolayer of S-HEK (spiking HEK) cells, a brightfield (a) and a fluorescence image (b), the membranes are labelled with the ElectroFluor630 potentiometric probe. (c,d) A single 100 µs, 150 V/cm electric pulse can trigger AP (as determined by a membrane fluorescence signal from ElectroFluor630, combined from all the cells in the field of view) in S-HEK cells (c) but not in NS-HEK cells (d). Pulse was delivered at time zero. There is a delay between the pulse delivery and the onset of AP in Fc, which is analysed further in Fig. 3f.
The parameters of TMV responses triggered by the pulse sequence shown in Fig. 2a in excitable S-HEK and non-excitable NS-HEK cells. In (a), all the experiments with responses are counted and expressed as % of all experiments. In (b), the amplitude of TMV responses. In (c–e), the recovery of TMV is shown: the percentage of responses where 50% (c) or 90% (d) of recovery towards the baseline value was reached later than 2.5 s after the pulse (the end of observation time). (e) Time from the first peak to 25% recovery. (f) Time from pulse exposure to first peak. The results are expressed as medians with bars Q1 and Q3. Number of experiments: N = 20 for both cell variants. *Statistical difference between S-HEK and NS-HEK cells (p < 0.05), Fisher’s Exact test (a,c,d), Mann–Whitney Rank Sum Test (b,e,f).
Propidium uptake in S-HEK and NS-HEK cells after electric pulse exposure. Cells were either exposed to the pulse sequence shown in Fig. 2a, or a train of 8 × 100 µs pulses of 400 or 1000 V/cm, 1 Hz. (a) Propidium uptake was evaluated as the propidium fluorescence intensity in the nuclear area, background was subtracted. Two controls were used, one after 20 min and one after 5 min of propidium incubation, that served as control for the pulse sequence and pulse train, respectively. The results are expressed as medians with bars Q1 and Q3. Number of experiments: N = 6 for the train of pulses and N = 7 for the sequence. # show significant difference from control, One way ANOVA on ranks. (b,c) Representative propidium fluorescence images of excitable S-HEK cells after being exposed to the whole pulse sequence shown in Fig. 2a (b) or 8 × 100 µs, 1000 V/cm, 1 Hz (c).
Ca²⁺ response in S-HEK and NS-HEK to the pulse sequence shown in Fig. 2a. (a,b) Uptake of Ca²⁺ ions in S-HEK (a) and NS-HEK cells (b) exposed to the pulse sequence (results from a representative batch of cells), as determined by Fura-2 ratio 340/380. Fura-2 ratio was averaged over each whole image. A pulse was delivered at around 5th second after the image acquisition started (red arrow). In (c), all the experiments with responses are counted and expressed as % of all experiments. (d,e) Ca²⁺ response in S-HEK and NS-HEK exposed to the pulse sequence. Number of experiments with 0, 1 or more Ca²⁺ peaks in S-HEK (d) and NS-HEK (e) are counted and expressed as % of all experiments. (f) The amplitude of Ca²⁺ responses triggered by individual pulses of the pulse sequence. The results in (f) are expressed as medians with bars Q1 and Q3. Number of experiments: N = 11 for S-HEK cells and N = 7 for NS-HEK cells. *Statistical difference between S-HEK and NS-HEK cells (p < 0.05), Fisher’s Exact test (c), and Mann–Whitney Rank Sum Test (f).
(a–g) Modelling TMV response in S-HEK cells. (a) Response in TMV, denoted by Um, averaged over the membranes of all cells in the cell array model, depending on the applied electric field strength. The inset shows the distribution of the induced Um at the end of the applied 100 μs pulse. Cells are considered to be connected with gap junctions. (b) Same results as in (a), but considering that cells are not connected with gap junctions. (c) TMV response in the cell array model after including a description for the increase in membrane conductance gep due to electroporation. gep stays constant until the end of observation time. (d) Same results as in (c) but considering that gep recovers exponentially with characteristic time of 2 s. (e) Distribution of the normalized electric field and gep in the model of the cell monolayer. Eapp is the ratio between the applied voltage and electrode distance. (f) TMV response in region of interest (ROI) at the middle between the electrodes computed with the model of the cell monolayer. (g) Snapshots showing AP propagation along the monolayer and sustained depolarization between the electrodes when Eapp = 300 V/cm. Pulse is applied at time t = 0 s. (h,i) Modelling TMV response in a neuronal cell model. (h) Hodgkin-Huxley type equivalent circuit model with added resistor representing the increase in membrane conductance gep due to electroporation. (i) Computed TMV responses for different values of gep. gep stays constant until the end of observation time.

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Genetically engineered HEK cells as a valuable tool for studying electroporation in excitable cells
  • Article
  • Full-text available

January 2024

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177 Reads

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10 Citations

Tina Batista Napotnik

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Electric pulses used in electroporation-based treatments have been shown to affect the excitability of muscle and neuronal cells. However, understanding the interplay between electroporation and electrophysiological response of excitable cells is complex, since both ion channel gating and electroporation depend on dynamic changes in the transmembrane voltage (TMV). In this study, a genetically engineered human embryonic kidney cells expressing NaV1.5 and Kir2.1, a minimal complementary channels required for excitability (named S-HEK), was characterized as a simple cell model used for studying the effects of electroporation in excitable cells. S-HEK cells and their non-excitable counterparts (NS-HEK) were exposed to 100 µs pulses of increasing electric field strength. Changes in TMV, plasma membrane permeability, and intracellular Ca²⁺ were monitored with fluorescence microscopy. We found that a very mild electroporation, undetectable with the classical propidium assay but associated with a transient increase in intracellular Ca²⁺, can already have a profound effect on excitability close to the electrostimulation threshold, as corroborated by multiscale computational modelling. These results are of great relevance for understanding the effects of pulse delivery on cell excitability observed in context of the rapidly developing cardiac pulsed field ablation as well as other electroporation-based treatments in excitable tissues.

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Figure 1. Geometries used to represent a cardiomyocyte with an electric field applied parallel to the long axis of the cell. (A) Prolate spheroid geometry, 120 µm long, 30 µm wide, and 30 µm high. (B) Real-shaped geometry 142 µm long, 36 µm wide, and 21 µm high. Both the real-shaped geometry and its prolate spheroid approximation were the same as in Milan et al. [30]. (C) The cell was at the center of the box when the electric field was applied parallel to the long axis of the cell. The violet-colored sides of the box represent the electrodes to which the voltage was applied.
Figure 2. The spatial distribution of transmembrane voltage (TMV) induced by a 10 ms pulse of (A) 1 V/cm (without electroporation) or (B) 500 V/cm (with electroporation). (C) The spatial distribution of the pore density (m −2 ) induced by the end of a 10 ms, 500 V/cm pulse (with electroporation). In each panel, the results are shown for prolate spheroid and real-shaped geometry when the electric field is applied either parallel or perpendicular to the long axis of the cell. The direction of the applied electric field is indicated by the arrows. Note different scales of TMV for panels (A,B).
Figure 5. Experimental measurements of calcium transients using Fura-2 ratio 340/380 peak change using H9c2 and AC16 cell lines when different pulse durations were applied (from 10 ms down to 100 ns) published by Dermol-ˇ Cerne et al. (A,B). *-statistically significant differences from control (p < 0.05), the Kruskal-Wallis One Way Analysis of Variance on Ranks, followed by Multiple Comparisons versus Control Group (the Dunn's Method), see Dermol-ˇ Cerne et al. [31]. Figure 5 (A,B) are reprinted with permission from [31]. (C) represents the ratio of the number of pores parallel/perpendicular obtained with the model using pulse durations and the electric field strengths of the one used in the experiments (A,B). The symbol [-] in the Y axis of (C) indicates that the unit of the ratio parallel/perpendicular is adimensional.
Characterization of Experimentally Observed Complex Interplay between Pulse Duration, Electrical Field Strength, and Cell Orientation on Electroporation Outcome Using a Time-Dependent Nonlinear Numerical Model

April 2023

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290 Reads

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10 Citations

Electroporation is a biophysical phenomenon involving an increase in cell membrane permeability to molecules after a high-pulsed electric field is applied to the tissue. Currently, electroporation is being developed for non-thermal ablation of cardiac tissue to treat arrhythmias. Cardiomyocytes have been shown to be more affected by electroporation when oriented with their long axis parallel to the applied electric field. However, recent studies demonstrate that the preferentially affected orientation depends on the pulse parameters. To gain better insight into the influence of cell orientation on electroporation with different pulse parameters, we developed a time-dependent nonlinear numerical model where we calculated the induced transmembrane voltage and pores creation in the membrane due to electroporation. The numerical results show that the onset of electroporation is observed at lower electric field strengths for cells oriented parallel to the electric field for pulse durations ≥10 µs, and cells oriented perpendicular for pulse durations ~100 ns. For pulses of ~1 µs duration, electroporation is not very sensitive to cell orientation. Interestingly, as the electric field strength increases beyond the onset of electroporation, perpendicular cells become more affected irrespective of pulse duration. The results obtained using the developed time-dependent nonlinear model are corroborated by in vitro experimental measurements. Our study will contribute to the process of further development and optimization of pulsed-field ablation and gene therapy in cardiac treatments.



Figure 1. Effects of low-and intermediate-voltage pulsed electric fields on left ventricular myocyte shortening and intracellular Ca2+ ([Ca2+]i) at 1 minute after application. Representative sarcomere lengths and [Ca 2+ ] i traces obtained from an isolated left ventricular myocytes during baseline (control [Ctrl]) 1 Hz pacing and 1 minute after (T 0 +1 minute) a 100 µs electric pulse (EP) delivered at low-(80 V; A) and intermediate-voltage (140 V; B). Sarcomere shortening, expressed as a percentage of the resting sarcomere length (%RSL) was increased 1 minute after EP with a low-and an intermediate-voltage pulses (C). Ca 2+ transient (CaTr) amplitudes (D) and diastolic Ca 2+ levels (E) expressed in 340:380 ratio units (r.u.), were increased 1 minute after EP with an intermediate but not with a low-voltage pulse. Data are represented as mean±SE of the mean with individual values for each cell. N indicates number of animals; n, number of cells; and ns, not significant. Paired t test: ns, **P<0.01, ***P<0.001.
Figure 3. Voltage threshold for irreversible electroporation depends on myocyte orientation with respect to the electric field. Following an intermediate voltage pulse application (140 V, 100 µs), left ventricular myocytes (LVM) oriented parallel or perpendicular to the electric field were exposed to electric pulse (EP) of increasing voltage amplitudes until cell death was observed. A, Representative intracellular Ca 2+ ([Ca 2+ ] i ) traces obtained in a LVM oriented parallel to the electric field show the rise in diastolic Ca 2+ when incrementing voltage amplitudes. B, Lethal voltage thresholds differed according to cell orientation and with Fura-2. Data are represented as mean±SEr of the mean with individual values for each cell. C, Lethal diastolic Ca 2+ levels in perpendicular cells were reached at lower voltages than in parallel-oriented cells. Inset: cell orientation and electric field direction. Unpaired t test: ##P<0.01; ###P<0.001. N indicates number of animals; n, number of cells; and r.u., ratio units. Downloaded from http://ahajournals.org by on November 23, 2022
Figure 4. Effect of high-voltage pulsed electric field on sarcomere shortening and intracellular Ca2+ ([Ca2+]i) in left ventricular myocytes according to cell orientation. Representative sarcomere lengths and [Ca 2+ ] i traces obtained from an isolated left ventricular myocytes (LVM) during baseline (control [Ctrl]) 1 Hz pacing, during and after (T0+5min) a 100 µs high voltage electric pulse (EP) delivered to a parallel (A) and perpendicular-oriented cell (B) below their respective lethal threshold. Sarcomere shortening, expressed as a percentage of resting sarcomere length (%RSL) was increased 5 minutes after EP and returned to Ctrl level 15 minutes post-EP in parallel-oriented cells (C). Ca 2+ transients (CaTr) amplitude progressively decreased after EP (D) while diastolic levels increased (E). Similar trends on sarcomere shortening (F), CaTr amplitudes (G) and diastolic Ca 2+ levels (H) were observed in perpendicular-oriented cells. Data are represented as mean±SE of the mean with individual values for each cell. Repeated-measure 1-way ANOVA: *P<0.05, **P<0.01, #P<0.05, ##P<0.01, ###P<0.001. N indicates number of animals; n, number of cells; and r.u., ratio units. Downloaded from http://ahajournals.org by on November 23, 2022
Figure 5. Immediate effect of a monophasic single electric pulse (EP) on left ventricular myocyte diastolic Ca 2+ levels and spontaneous contractile activity. A, Representative intracellular Ca 2+ ([Ca 2+ ] i ) traces from left ventricular myocytes (LVMs) subjected to a low-(80 V), medium-(140 V), and highvoltage (here, 180 V in a perpendicular cell) 100 µs EP. B, The rise in diastolic Ca 2+ level induced by the EP increased when increasing pulse's amplitude. C, The time to reach maximum diastolic Ca 2+ level also tended to increase with the voltage of the electroporating pulse. D, Example of spontaneous contractions monitored before and after EP (intermediate voltage, 100 µs) in unpaced LVM. Prior to EP, when pacing was stopped, LV myocytes remained quiescent. Spontaneous contractions were observed in these cells 1-5 minutes after EP and their frequency decreased with time over 20 minutes. Data are represented as mean±SE of the mean with individual values for each cell. Unpaired t test: ###P<0.001. N indicates number of animals; n, number of cells; PFA, pulsed field ablation; and r.u., ratio units. Downloaded from http://ahajournals.org by on November 23, 2022
Reversible and Irreversible Effects of Electroporation on Contractility and Calcium Homeostasis in Isolated Cardiac Ventricular Myocytes

October 2022

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224 Reads

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20 Citations

Circulation Arrhythmia and Electrophysiology

Background: Irreversible electroporation is an energy form utilizing high-voltage pulsed electric field, leading to cellular homeostasis disruption and cell death. Recently, irreversible electroporation has shown promising results for the treatment of cardiac arrhythmias. However, reversible and irreversible effects of pulsed electric field on cardiac myocytes remain poorly understood. Here, we evaluated the influence of a monophasic single electric pulse (EP) on the contractility, Ca2+ homeostasis and recovery of cardiac myocytes. Methods: Isolated rat left ventricular myocytes were electroporated using single monophasic EP of different durations and voltages. Sarcomere length and intracellular Ca2+ were simultaneously monitored for up to 20 minutes after EP application in Fura-2 loaded left ventricular myocytes. Lethal voltage thresholds were determined using 100 µs and 10 ms pulses and by discriminating cell orientation with respect to the electric field. Results: Electroporation led to an immediate increase in intracellular Ca2+ which was dependent upon the voltage delivered to the cell. Intermediate-voltage EP (140 V, 100 µs) increased sarcomere shortening, Ca2+ transient amplitude, and diastolic Ca2+ level measured 1 minute post-EP. Although sarcomere shortening returned to pre-EP level within 5 minutes, Ca2+ transient amplitude decreased further below pre-EP level and diastolic Ca2+ level remained elevated within 20 minutes post-EP. Spontaneous contractions were observed after sublethal EP application but their frequency decreased progressively within 20 minutes. Lethal EP voltage threshold was lower in myocytes oriented perpendicular than parallel to the electric field using 100 µs pulses while an opposite effect was found using 10 ms pulses. Conclusions: Sublethal EP affected rat left ventricular myocytes contractility and disrupted Ca2+ homeostasis as a function of the EP voltage. Moreover, EP-induced lethality was preceded by a large increase in intracellular Ca2+ and was dependent upon the EP duration, amplitude and left ventricular myocytes orientation with respect to the electric field. These findings provide new insights into the effect of pulsed electric field on cardiac myocytes.


Figure 3. Relative calcium ion (Ca 2+ ) concentration at the poles facing anode (+) and cathode (−) in cells (both parallel and perpendicular cells together) (A,C,E,G) and fura ratio difference between cathode and anode (B,D,F,H) after Figure 3. Relative calcium ion (Ca 2+ ) concentration at the poles facing anode (+) and cathode (−) in cells (both parallel and perpendicular cells together) (A,C,E,G) and fura ratio difference between cathode and anode (B,D,F,H) after electroporation with a single 100 ns, 40 kV/cm (A,B), 1 µs, 2500 V/cm (C,D), 10 µs, 1000 V/cm (E,F), and 100 µs, 400 V/cm pulse (G,H) as expressed in Fura-2 ratio 340/380 over time. Relative Ca 2+ concentration in cells was monitored with a fluorescent calcium indicator Fura-2, image acquisition was done every 250 ms. Results are presented as median from cells (only parallel and
Figure 5. The source of calcium ions for calcium concentration elevation after electroporation. Relative calcium concentration in H9c2 cells was monitored with a fluorescent calcium indicator Fura-2 and expressed as Fura-2 ratio 340/380 over time (subtracted baseline). Image acquisition was done every 250 ms. (A): H9c2 cells were exposed to a single pulse of 100 Figure 5. The source of calcium ions for calcium concentration elevation after electroporation. Relative calcium concentration in H9c2 cells was monitored with a fluorescent calcium indicator Fura-2 and expressed as Fura-2 ratio 340/380 over time (subtracted baseline). Image acquisition was done every 250 ms. (A): H9c2 cells were exposed to a single pulse of 100 ns, 40 kV/cm in conditions either without external Ca 2+ , but with EGTA present (no Ca, red) or in DMEM culture medium with Ca 2+ present (DMEM, yellow). Results are presented as mean from six (no Ca 2+ ) or nine (DMEM) experiments (5-13 cells per experiment analyzed). (B-D): The same cells were exposed to a single pulse of 1 µs, 2500 V/cm (B), 10 µs, 1000 V/cm (C), and 100 µs, 400 V/cm (D), first in conditions without external Ca 2+ but with EGTA present, and after that, the medium was changed to DMEM culture medium with Ca 2+ present. Results are presented as mean from four (B), five (C), and three (D) experiments (11-30 cells per experiment analyzed). Time of pulse application is noted with a red arrow. Vertical bars represent SD. Controls are experiments without pulse application.
Figure 6. The exposure of cells incubated with 100 nM thapsigargin (for 30 min) to a single 100 ns, 40 kV/cm pulse in media with (DMEM) or without Ca 2+ ions (SMEM and EGTA). Relative calcium concentration in H9c2 cells was monitored with a fluorescent calcium indicator Fura-2 and expressed as Fura-2 ratio 340/380 over time. Image acquisition was done every Figure 6. The exposure of cells incubated with 100 nM thapsigargin (for 30 min) to a single 100 ns, 40 kV/cm pulse in media with (DMEM) or without Ca 2+ ions (SMEM and EGTA). Relative calcium concentration in H9c2 cells was monitored with a fluorescent calcium indicator Fura-2 and expressed as Fura-2 ratio 340/380 over time. Image acquisition was done every 250 ms. (A): Relative calcium concentration in all cells exposed to a single 100 ns pulse in different media. Results are presented as mean ± SD from ten (no Ca 2+ ) or 14 (DMEM) experiments (3-11 cells per experiment analyzed). Controls are experiments without pulse application. (B): Fura ratio difference between cathode and anode in thapsigargin treated cells (both parallel and perpendicular cells together) after electroporation with a single 100 ns, 40 kV/cm in medium with Ca 2+ ions (DMEM). Results are presented as median from cells (only parallel and perpendicular cells) pooled from 14 experiments (12-30 cells analyzed), vertical bars represent Q1 and Q3. Time of pulse application is noted with a red arrow.
Pulse Duration Dependent Asymmetry in Molecular Transmembrane Transport Due to Electroporation in H9c2 Rat Cardiac Myoblast Cells In Vitro

October 2021

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135 Reads

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3 Citations

Electroporation (EP) is one of the successful physical methods for intracellular drug delivery, which temporarily permeabilizes plasma membrane by exposing cells to electric pulses. Orientation of cells in electric field is important for electroporation and, consequently, for transport of molecules through permeabilized plasma membrane. Uptake of molecules after electroporation are the greatest at poles of cells facing electrodes and is often asymmetrical. However, asymmetry reported was inconsistent and inconclusive—in different reports it was either preferentially anodal or cathodal. We investigated the asymmetry of polar uptake of calcium ions after electroporation with electric pulses of different durations, as the orientation of elongated cells affects electroporation to a different extent when using electric pulses of different durations in the range of 100 ns to 100 µs. The results show that with 1, 10, and 100 µs pulses, the uptake of calcium ions is greater at the pole closer to the cathode than at the pole closer to the anode. With shorter 100 ns pulses, the asymmetry is not observed. A different extent of electroporation at different parts of elongated cells, such as muscle or cardiac cells, may have an impact on electroporation-based treatments such as drug delivery, pulse-field ablation, and gene electrotransfection.


Cell Death Due To Electroporation – A Review

June 2021

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371 Reads

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344 Citations

Bioelectrochemistry

Exposure of cells to high voltage electric pulses increases transiently membrane permeability through membrane electroporation. Electroporation can be reversible and is used in gene transfer and enhanced drug delivery but can also lead to cell death. Electroporation resulting in cell death (termed as irreversible electroporation) has been successfully used as a new non-thermal ablation method of soft tissue such as tumours or arrhythmogenic heart tissue. Even though the mechanisms of cell death can influence the outcome of electroporation-based treatments due to use of different electric pulse parameters and conditions, these are not elucidated yet. We review the mechanisms of cell death after electroporation reported in literature, cell injuries that may lead to cell death after electroporation and membrane repair mechanisms involved. The knowledge of membrane repair and cell death mechanisms after cell exposure to electric pulses, targets of electric field in cells need to be identified to optimize existing and develop of new electroporation-based techniques used in medicine, biotechnology, and food technology.


Short microsecond pulses achieve homogeneous electroporation of elongated biological cells irrespective of their orientation in electric field

June 2020

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427 Reads

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33 Citations

In gene electrotransfer and cardiac ablation with irreversible electroporation, treated muscle cells are typically of elongated shape and their orientation may vary. Orientation of cells in electric field has been reported to affect electroporation, and hence electrodes placement and pulse parameters choice in treatments for achieving homogeneous effect in tissue is important. We investigated how cell orientation influences electroporation with respect to different pulse durations (ns to ms range), both experimentally and numerically. Experimentally detected electroporation (evaluated separately for cells parallel and perpendicular to electric field) via Ca2+ uptake in H9c2 and AC16 cardiomyocytes was numerically modeled using the asymptotic pore equation. Results showed that cell orientation affects electroporation extent: using short, nanosecond pulses, cells perpendicular to electric field are significantly more electroporated than parallel (up to 100-times more pores formed), and with long, millisecond pulses, cells parallel to electric field are more electroporated than perpendicular (up to 1000-times more pores formed). In the range of a few microseconds, cells of both orientations were electroporated to the same extent. Using pulses of a few microseconds lends itself as a new possible strategy in achieving homogeneous electroporation in tissue with elongated cells of different orientation (e.g. electroporation-based cardiac ablation).


Fig. 3. The dependence of PI and YP fluorescence intensity spectra on HI-PEMF treatment samples without (grey plot) or with added 20 nm Au NPs (red plot). Left of the gate (black solid line) are non-permeabilized cells while right of the gate are permeabilized cells.
Fig. 4. Permeabilization of cells after HI-PEMF treatment. Cells without added NPs (No NPs) and cell with added 5 nm or 20 nm Au NPs (+5 or +20 nm Au NPs) were used. The percentage of PI (red) and YP (green) fluorescent cells (A, C) as well as median fluorescence (B, D) after different incubation time are shown. Each sample and fluorescent dye have their own untreated sample; CTRL PI (blue) or CTRL YP (white). Asterisk (*) marks statistically significant difference (p < 0.05) between treated sample and its corresponding untreated sample.
Fig. 5. Bright filed (A-D) and fluorescence microscopy images (E-H) of permeabilization after HI-PEMF was applied in PI assay. HI-PEMF untreated sample without added NPs (A, E), HI-PEMF treated sample without added NPs (B, F), HI-PEMF untreated sample with added NPs (C, G) and HI-PEMF treated sample with added NPs (D, H).
Number of 5 and 20 nm Au NPs in two different buffers incubated with CHO cells and E. coli.
Contactless electroporation induced by high intensity pulsed electromagnetic fields via distributed nanoelectrodes

December 2019

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377 Reads

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32 Citations

Bioelectrochemistry

Pulsed electric fields (PEFs) can be used to transiently increase cell membrane permeability in procedures ranging from gene therapy to tumor eradication. Although very efficient, PEF-based therapies generally require the use of invasive electrodes, which cause pain and tissue damage. An emerging noninvasive, contactless alternative to PEFs are High Intensity Pulsed Electromagnetic Fields (HI-PEMF), whereby the electric field inside the tissue is induced remotely by external pulsed magnetic field. However, one of the current major drawbacks of HI-PEMFs is their inferior efficiency compared to PEFs. In this study we present the proof-of-concept that by adding highly conductive 5 and 20 nm gold nanoparticles (Au NPs), we can significantly potentiate the permeabilizing effect of HI-PEMFs, making it possible to permeabilize up to 80% of the cells with minimal or no effect on cell survival, compared to negligible percentage of permeabilized cells using HI-PEMF alone. Experiments, conducted on Chinese Hamster Ovary cells and Escherichia coli, suggest that Au NPs act as distributed nanoelectrodes, locally enhancing the electric field induced at the plasma membrane. Our findings open up an avenue of possibilities for combining naked as well as functionalized Au NPs with HI-PEMFs for noninvasive, remotely controlled smart drug delivery applications.


Fig. 4. Monitoring electroporation with fura-2. (A) CHO cells-bright field. (B) Ratio of fluorescence (F345/F385) for cells in control (non-porated cells). (C) Cells 1 min after electroporation with a 250 V/cm, 10 ms pulse. Brighter cells were electroporated. Arrow denotes the field direction. Bar represents 20 μm. Source: © 2011 IEEE. Reprinted, with permission, from Pucihar, G., Krmelj, J., Reberšek, M., Napotnik, T.B., and Miklavčič, D. (2011). Equivalent pulse parameters for electroporation. IEEE Trans. Biomed. Eng. 58, 3279-3288 [20].
Fig. 6. Schematic presentation of common setup in electroporation applications for measuring the conductivity before and after the pulse using a small signal with a tetrapolar configuration. Source: © 2016 Springer International Publishing. Castellví, Q., Mercadal, B., and Ivorra, A. (2016). Assessment of Electroporation by Electrical Impedance Methods. In Handbook of Electroporation, D. Miklavcic, ed. (Springer International Publishing), pp. 1-20 [262]. Reprinted with the permission of Springer International Publishing AG.
Fig. 7. Patch clamp recording in studies with nanosecond electric pulses: Nanosecond pulsed electric field (nsPEF) exposure of individual cells attached to a glass cover slip. NsPEF was delivered by a pair of electrodes (E1, E2) made of 125-μm diameter tungsten rod. These electrodes were placed symmetrically on the sides of the selected cell (center). Cells chosen for exposure or sham exposure were situated out of large cell clusters and showed no visible signs of damage or deterioration. A glass micropipette (MP) for patch-clamp recording was brought in contact with the exposed cell after nsPEF exposure. Source: © 2007 Elsevier. Reprinted from Pakhomov, A.G., Shevin, R., White, J.A., Kolb, J.F., Pakhomova, O.N., Joshi, R.P., and Schoenbach, K.H. (2007). Membrane permeabilization and cell damage by ultrashort electric field shocks. Arch. Biochem. Biophys. 465, 109-118 [76], with the permission of Elsevier.
In vitro electroporation detection methods – An overview

December 2017

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425 Reads

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168 Citations

Bioelectrochemistry

Exposing cells to an electric field leads to electroporation of the cell membrane which has already been explored and used in a number of applications in medicine and food biotechnology (e.g. electrochemotherapy, gene electrotransfer, extraction of biomolecules). The extent of electroporation depends on several conditions, including pulse parameters, types of cells and tissues, surrounding media, temperature etc. Each application requires a specific level of electroporation, so it must be explored in advance by employing methods for detecting electroporation. Electroporation detection is most often done by measuring increased transport of molecules across the membrane, into or out of the cell. We review here various methods of electroporation detection, together with their advantages and disadvantages. Electroporation detection can be carried out by using dyes (fluorophores or colour stains) or functional molecules, by measuring the efflux of biomolecules, by impedance measurements and voltage clamp techniques as well as by monitoring cell swelling. This review describes methods of detecting cell membrane electroporation in order to help researchers choose the most suitable ones for their specific experiments, considering available equipment and experimental conditions.


Citations (17)


... Finally, previous experiments have demonstrated that exposing biological samples to static magnetic fields (SMF) for durations ranging from minutes to days can alter neuronal excitatory thresholds and spiking rates, [14][15][16] , spinal cord conduction 17 , ion channel dynamics [18][19][20] , or gene expression 21 . These effects have been reported to emerge on the scale of a minute or longer and may extend beyond the exposure period. ...

Reference:

Magnetic activation of electrically active cells
Genetically engineered HEK cells as a valuable tool for studying electroporation in excitable cells

... Electroporation by high-voltage electric pulses transiently increases cardiomyocyte membrane permeability to hinder uncontrolled ion transport. Scuderi et al. attempted to identify the optimal combination of electrical strength, duration, and cell orientation for the best electroporation effect [22]. They developed a time-dependent nonlinear numerical model to simulate the effect of an electric field on the cardiomyocytes, which was then tested in vitro. ...

Characterization of Experimentally Observed Complex Interplay between Pulse Duration, Electrical Field Strength, and Cell Orientation on Electroporation Outcome Using a Time-Dependent Nonlinear Numerical Model

... 3 Irreversible electroporation is used in standard PFA ablation to create robust lesions via disruption of the cellular membrane and induce apoptosis. 6 These are usually deployed in a sequence of several pulses. Chaigne et al., however, observed that single electrical pulses transiently influence calcium homeostasis and allow for subsequent recovery of cardiac myocytes. ...

Reversible and Irreversible Effects of Electroporation on Contractility and Calcium Homeostasis in Isolated Cardiac Ventricular Myocytes

Circulation Arrhythmia and Electrophysiology

... Finally, the level of EP could be more favorable in terms of the area of the electroporated membrane and/or the size of the electropores on the membrane facing the cathode. Indeed, studies have shown that the asymmetry with a cathodic preference for ion and dye uptake was observed after EP [48][49][50][51]. A similar pattern was also observed after siRNA electrotransfer in 3D spheroids [15]. ...

Pulse Duration Dependent Asymmetry in Molecular Transmembrane Transport Due to Electroporation in H9c2 Rat Cardiac Myoblast Cells In Vitro

... Short pulses with high amplitudes are used in Highoutput pacing in Cardiac Resynchronization Therapy to improve conduction velocity and cardiac output (Bavikati et al., 2012), to improve ventricular activation (Bonomini et al., 2017) and to achieve scar homogenization in ablation applications (Anderson et al., 2020). For too short pulses, the high pulse amplitudes can induce adverse effects for pacing purposes, namely, electroporation of cells, a process by which pores are created in the cell to either insert compounds (such as medications) into it or for "irreversible electroporation" to induce cell death (judicial cell death) (Napotnik, et al., 2021) by apoptosis, necrosis, or newer methods such as pyroptosis or necroptosis (Lv, et al., 2019). These effects are unwanted in pacing procedures. ...

Cell Death Due To Electroporation – A Review
  • Citing Article
  • June 2021

Bioelectrochemistry

... With millisecond pulses, there is a greater electroporation with a parallel orientation than perpendicular. Using microsecond pulses, cells of both orientations were electroporated to the same extent [12]. ...

Short microsecond pulses achieve homogeneous electroporation of elongated biological cells irrespective of their orientation in electric field

... Since then, a large number of experimental studies focusing on pulsed magnetic field-induced cell permeabilization have emerged. [2][3][4][5][6] Novickij et al. 's experiments found that a pulsed magnetic field with a magnetic induction strength of 2.9 T and an induced electric field of 7.25 V/cm could alter the permeability of mammalian cells. However, a pulsed magnetic field with a magnetic induction strength of 16.4 T and an induced electric field of 1.25 V/cm did not affect cell permeability. ...

Contactless electroporation induced by high intensity pulsed electromagnetic fields via distributed nanoelectrodes

Bioelectrochemistry

... Herein, YO-PRO-1 (YP) and propidium iodide (PI) cell staining assays were employed to detect the formation of nanopores in the electroporation. YP and PI are one of the most efficient nucleic acid stains that can dissociate into propidium cations in water and bind to DNA by intercalating between the bases [24]. The maximum diameter of a propidium cation is about 1.5 nm, which is substantially larger than the YO-PRO-1 molecule (0.5-1.0 nm) [25]. ...

In vitro electroporation detection methods – An overview

Bioelectrochemistry

... Moreover, the dye-based techniques require sampling during the post-treatment phase to detect electroporation efficiency. [23] Electrical-based methods offer relatively faster results, particularly with real-time conductivity measurements. However, they require a conductive contact of electrodes with the yeast suspensions, which might complicate the integration to high-voltage PEF systems. ...

Fluorescent Indicators of Membrane Permeabilization Due to Electroporation
  • Citing Chapter
  • August 2017

... A compromise in cell membrane allows the entry of propidium iodide (PI) into cells; PI then intercalates between the bases in nucleic acids and emits fluorescence. 19 Bis(1,3-dibutylbarbituric acid) trimethine oxonol (BOX) penetrates depolarized cells to bind lipid-rich components and emits fluorescence. 20 PI entry indicates membrane permeabilization, while BOX binding suggests membrane depolarization. ...

Fluorescent Indicators of Membrane Permeabilization Due to Electroporation
  • Citing Chapter
  • August 2016