Ionic Conduction in Biological Nanopores Created by Ultrashort9 High-Intensity Pulses

Ultrashort, high-intensity electric pulses open nanopores in biological cell membranes. Ion transport in nanopore is analyzed using a numerical method that couples the Nernst-Planck equations for ionic concentrations, the Poisson equation for the electric potential, and Navier-Stokes equations for the fluid flow. Roles of the applied bias, pore size, as well as the surface charge lining the membrane are comprehensively examined through I-V characteristics, conductance variations of the pore. Our results show that the surface charge distribution has an impact on the ionic conduction due to mutual electrostatic force interference. In addition, a larger pore would conduct a larger ionic current thus being more conductive on the condition of the same bias applied, which would suggest a bias-dependent expansion of pores.

[1]  Juergen F. Kolb,et al.  Nanosecond pulsed electric fields cause melanomas to self-destruct , 2006 .

[2]  W. Hamilton,et al.  Effects of high electric fields on microorganisms: I. Killing of bacteria and yeasts , 1967 .

[3]  Laura Marcu,et al.  Calcium bursts induced by nanosecond electric pulses. , 2003, Biochemical and biophysical research communications.

[4]  Shu Xiao,et al.  Simulations of Voltage Transients Across Intracellular Mitochondrial Membranes Due to Nanosecond Electrical Pulses , 2014, IEEE Transactions on Plasma Science.

[5]  Wenbing Zhao,et al.  Simulation of Electroporation in Cell Using Bipolar AC Pulse , 2018, 2018 IEEE International Microwave Biomedical Conference (IMBioC).

[6]  Alan E Mark,et al.  Simulation of pore formation in lipid bilayers by mechanical stress and electric fields. , 2003, Journal of the American Chemical Society.

[7]  W. Krassowska,et al.  Electrical energy required to form large conducting pores. , 2003, Bioelectrochemistry.

[8]  Ravindra P. Joshi,et al.  Asymmetric conduction in biological nanopores created by high-intensity, nanosecond pulsing: Inference on internal charge lining the membrane based on a model study , 2015 .

[9]  W. Krassowska,et al.  Modeling postshock evolution of large electropores. , 2003, Physical review. E, Statistical, nonlinear, and soft matter physics.

[10]  Andrei G. Pakhomov,et al.  Analysis of Plasma Membrane Integrity by Fluorescent Detection of Tl+ Uptake , 2010, The Journal of Membrane Biology.

[11]  Ravindra P. Joshi,et al.  Simulation of nanoparticle based enhancement of cellular electroporation for biomedical applications , 2014 .

[12]  Hao Qiu Numerical Study of Poration and Ionic Conduction in Nanopores Caused by High-Intensity, Nanosecond Pulses in Cell , 2014 .

[13]  E. Neumann,et al.  Permeability changes induced by electric impulses in vesicular membranes , 1972, The Journal of Membrane Biology.

[14]  K. Schoenbach,et al.  Differential effects in cells exposed to ultra-short, high intensity electric fields: cell survival, DNA damage, and cell cycle analysis. , 2003, Mutation research.

[15]  Wenbing Zhao,et al.  Numerical Study of Pore Density Distribution and Pore Formation Energy , 2018, 2018 IEEE International Microwave Biomedical Conference (IMBioC).

[16]  Ravindra P. Joshi,et al.  Physics of nanoporation and water entry driven by a high-intensity, ultrashort electrical pulse in the presence of membrane hydrophobic interactions , 2013 .