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A cross the surface or membrane of every neuron is an electrical potential difference due to the presence of more negative ions on the inside of the membrane than the outside , the neuron said to be polarized , the inside of the cell is typically 60 -90 mv more negative than outside.
Integrative Physiological and Behavioral Science, 1995
Living cells create electric potential force, E, between their various phases by Q1Q2 at least three distinct mechanisms. Charge separation, F = (Eqn 1) creates the 41-l~Oerr2 Q potential, E = 4iieoerr of -120 to -145 mV between cytoplasmic and mitochondrial phases by unbalanced proton expulsion powered by the redox energy of the respiratory chain. Electrically unbalanced flow of Na + through voltage gated Na § channels raises the potential of nerve from -85 to +30 mV. The so-called resting potential of cells, which varies from -85 mV in heart to -4.5 mV in red cell, does not appear to result from the unbalanced flow of ions between phases, but rather to be a measure of the work required to move ions between phases. Movement of an ion between phases entails three types of energy. Concentration work is that required to move an ion between phases containing different concentrations of ions:
2011
We have modeled the electric potential profile, across the membranes of the ganglion neuron and neuroblastoma cells. We considered the resting and action potential states, and analyzed the influence of fixed charges of the membrane on the electric potential of the surface of the membranes of these cells, based on experimental values of membrane properties. The ganglion neuron portrays a healthy neuron, and the neuroblastoma cell, which is tumorous, represents a pathologic neuron. We numerically solved the non-linear Poisson-Boltzmann equation, by considering the densities of charges dissolved in an electrolytic solution and fixed on both glycocalyx and cytoplasmic proteins. We found important differences among the potential profiles of the two cells.
Cellular and Molecular Neurophysiology, 2015
The neuronal plasma membrane delimits the whole neuron, cell body, dendrites, dendritic spines, axon and axon terminals. It is a barrier between the intracellular and extracellular environments. The general structure of the neuronal plasma membrane is similar to that of other plasma membranes. It is made up of proteins inserted in a lipid bilayer, forming as a whole a 'fl uid mosaic' (Figure 3.1). However, insofar as there are functions that are exclusively neuronal, the neuronal membrane differs from other plasma membranes by the nature, density and spatial distribution of the proteins of which it is composed. The presence of a large diversity of transmembrane proteins called ionic channels (or simply 'channels') characterizes the neuronal plasma membrane. They allow the passive movement of ions across membranes and thus electrical signaling in the nervous system. Among the ions present in the nervous system fl uids, Na + , K + , Ca 2+ and Cl − ions seem to be responsible for almost all of the action. 3.1 THERE IS AN UNEQUAL DISTRIBUTION OF IONS ACROSS NEURONAL PLASMA MEMBRANE. THE NOTION OF CONCENTRATION GRADIENT 3.1.1 The plasma membrane separates two media of different ionic composition Regardless of the animal's environment (seawater, freshwater or air), potassium (K +) ions are the predominant cations in the intracellular fl uid and sodium (Na +) ions are the predominant cations in the extracellular fl uid. The main anions of the intracellular fl uid are organic molecules (P −): negatively charged amino acids (glutamate and aspartate), proteins, nucleic acids, phosphates, etc… which have a large molecular weight. In the extracellular fl uid, the predominant anions are chloride (Cl −) ions. A marked difference between cytosolic and extracellular Ca 2+ concentrations is also observed (Figure 3.2). O U T L I N E 3.1 There is an unequal distribution of ions across neuronal plasma membrane. The notion of concentration gradient 39 3.2 There is a difference of potential between the two faces of the membrane, called membrane potential (V m) 42 3.3 Concentration gradients and membrane potential determine the direction of the passive movements of ions through ionic channels: the electrochemical gradient 43 3.4 The passive diffusion of ions through an open channel creates a current 45 3.5 A particular membrane potential, the resting membrane potential V rest 46 3.6 A simple equivalent electrical circuit for the membrane at rest 48 3.7 How to experimentally change V rest 49 3.8 Summary 50
2016
We present a model for the electric potential profile across the membranes of neuronal cells. We considered the resting and action potential states, and analyzed the influence of fixed charges of the membrane on its electric potential, based on experimental values of membrane properties of the spinal ganglion neuron and the neuroblastoma cell. The spinal ganglion neuron represents a healthy neuron, and the neuroblastoma cell, which is tumorous, represents a pathological neuron. We numerically solved the non-linear Poisson-Boltzmann equation for the regions of the membrane model we have adopted, by considering the densities of charges dissolved in an electrolytic solution and fixed on both glycocalyx and cytoplasmic proteins. Our model predicts that there is a difference in the behavior of the electric potential profiles of the two types of cells, in response to changes in charge concentrations in the membrane. Our results also describe an insensitivity of the neuroblastoma cell memb...
PloS one, 2014
We present a model for the electric potential profile across the membranes of neuronal cells. We considered the resting and action potential states, and analyzed the influence of fixed charges of the membrane on its electric potential, based on experimental values of membrane properties of the spinal ganglion neuron and the neuroblastoma cell. The spinal ganglion neuron represents a healthy neuron, and the neuroblastoma cell, which is tumorous, represents a pathological neuron. We numerically solved the non-linear Poisson-Boltzmann equation for the regions of the membrane model we have adopted, by considering the densities of charges dissolved in an electrolytic solution and fixed on both glycocalyx and cytoplasmic proteins. Our model predicts that there is a difference in the behavior of the electric potential profiles of the two types of cells, in response to changes in charge concentrations in the membrane. Our results also describe an insensitivity of the neuroblastoma cell memb...
Clinical Aspects of Electroporation, 2011
An exposure of a cell to an external electric field results in the induced transmembrane voltage (DY m ) that superimposes to the resting voltage. This can have a range of effects, from modification of the activity of voltage-gated channels to membrane electroporation, and accurate knowledge of spatial distribution and time course of DY m is important for the understanding of these effects. In this chapter, we present the analytical, numerical, and experimental methods of determination of DY m , and combine them with the monitoring of electroporation-induced transmembrane molecular transport (TMT) in Chinese Hamster Ovary (CHO) cells. Potentiometric measurements are performed using di-8-ANEPPS, and TMT is monitored using propidium iodide. In isolated cells, we combine analytical derivation (for spherical cells) and numerical computation of DY m (for irregularly shaped cells) with potentiometric measurements to show that the latter are accurate and reliable. Monitoring of TMT in these same cells shows that it is confined to the regions with the highest |DY m |. We then review other parameters influencing electroporation of isolated cells, and proceed, through the intermediate case of dense suspensions, to cells in direct contact with each other. We use the scrape-loading test to show that the CHO cells in a monolayer are interconnected, and then study DY m and TMT in a cluster of four such cells. With low pulse amplitudes, the cluster behaves as one big cell, with DY m continuous along its outer boundary, reflecting the interconnections. With interconnections inhibited, the cells start to behave as individual entities, with DY m continuous along the plasma membrane of each cell. With the cluster exposed to porating (higher amplitude) pulses, TMT occurs in the membrane regions for which computations predict the highest |DY m | if the cells are modeled as insulated, suggesting that the interconnections are blocked by supraphysiological DY m , either directly by voltage gating or indirectly through changes in ionic concentrations caused by electroporation.
Biochemical and Biophysical Research Communications, 1990
Electric field induced permeabilization of cell membranes is an important technique for gene transfection and cell hybfidizationl-4. Mechanistic studies of this process revealed that the uptake of fluorescent indicator by plant protoplasts occurs predominantly on the hemisphere facing the positive electrode 5, while in erythrocyte ghosts the probes exit through the hemisphere facing the negative electrode 6. To reconcile these observations symmetrical pore formation and a mechanism of molecular exchange by electroosmosis has been proposedtL In light of these controversial observations, we conducted a systematic study ofelectropomtion of NIH3T3 cells with varying electric field strength, wavefonn and frequency. Our data revealed that (i) symmetrical permeabilization of the cell membrane occurs only with bipolar a.c. fields. (ii) When a critical membrane breakdown potential, Vc, is applied using either an unipolar a.c. fields or a single d.c. square pulse, the cell membrane becomes permeabilized only at the hemisphere facing the positive electrode. (iii) When the pulse -induced membrane potential, Vm, is approximately equal to or larger than the intrinsic membrane potential (i.e. using d.c. or unipolar a.c. field), asymmetric permeabilization was observed with the hemisphere facing the positive electrode being most permeable. (iv) The rate of fluorescent indicator uptake is dependent on the concentration of the indicator. These results indicate that electro-permeabilization of cell membranes is affected by its resting potential and that electroosmosis is not the dominant mechanism for the cellular uptake of foreign molecules in dectroporation.
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