Effect of pulse width on the dynamics of a deflated vesicle in unipolar and bipolar pulsed electric fields

TL;DR

This study computationally explores how pulse width and type affect the deformation and shape transitions of deflated vesicles in pulsed electric fields, revealing complex dynamics and shape outcomes dependent on pulse parameters.

Contribution

It introduces a detailed computational analysis of vesicle deformation under various pulsed electric fields, highlighting the influence of pulse type and width on vesicle shape dynamics.

Findings

Shape remains prolate for high conductivity ratio ($.1$)

Complex shape transitions occur at low conductivity ratio ($.1$)

Two-step pulses can control vesicle final shape

Abstract

Giant unilamellar vesicles subjected to pulsed direct-current (pulsed-DC) fields are promising biomimetic systems to investigate the electroporation of cells. In strong electric fields, vesicles undergo significant deformation, which strongly alters the transmembrane potential, consequently the electroporation. Previous theoretical studies investigated the electrodeformation of vesicles in DC fields (which are not pulsed). In this work, we computationally investigate the deformation of a deflated vesicle under unipolar, bipolar, and two-step unipolar pulses and show sensitive dependence of intermediate shapes on type of pulse and the pulse width. Starting with the stress-free initial shape of a deflated vesicle, which is similar to a prolate spheroid, the analysis is presented for the cases with higher and lower conductivities of the inner fluid medium relative to the outer fluid medium. For the ratio of inner to outer fluid conductivity, $\sigma_\mathrm{r}$ = 10, the shape always remains prolate, including when the field is turned off. For $\sigma_\mathrm{r} = 0.1$, several complex dynamics are observed, such as the prolate-to-oblate (PO), prolate-to-oblate-to-prolate (POP) shape transitions in time depending upon the strength of the field and the pulse properties. In this case, on turning off the field, a metastable oblate equilibrium shape is seen, that seems to be a characteristics of a deflated vesicle leading to POPO transitions. When a two-step unipolar pulse (a combination of a strong and a weak subpulse) is applied, a vesicle can reach an oblate or a prolate final shape depending upon the relative durations of the two subpulses.