Symbol | Meaning |
| radial distance of the (field point, source point) from the axis of the cylinder |
| azimuthal angle |
| distance of the (field point, source point) along the axis of the cylinder |
I0 | magnitude of the current strength at the surface of the node of Ranvier |
p | radial distance from the cylindrical axis where the current magnitude vanishes |
| (starting, termination) point in time of the PWM-PPM waveform [8] of the ion channel current profile |
| Heaviside step function |
| Dirac delta function |
| electric potential at spatial (field) position and time t |
| volume source current density produced by an ion channel ring (with, without) time variation |
| position of the source element |
| permittivity of free space |
| azimuthal coordinates of the (field point, source point) |
| gradient operator |
| the net electric field due to the ion channel |
| two of the three unit vectors in the three-dimensional coordinate system |
| two radial distances used to generate the form of the current near the node |
| azimuthal thickness of the first ion channel in the ring of ion channels at the node of Ranvier |
| the membrance (capacitance, conductance) of the k-th axon |
| the transmembrane potential difference of the k-th axon at spatial position x and time t |
| a parameter introduced by Reutskiy, Rossoni and Tirozzi |
N | total number of axons in the tract |
r | “ratio” used in the simulations which indicates the strength of the current-mediated coupling between axons |
| the resistance per unit length of the axoplasm of each axonal fiber |
| the conductance of the (axoplasm, myelin sheath) of the k-th axon |
| the inclination of the k-th axon (without, with) z-dependence |
| a combination of parameters introduced by Chawla, Morgera and Snider (without, with) z-dependence |
| the total injected current at the node, including contributions from ionic current, as well as external stimulation |
| number of ion channels open at the present node at time t |
| two positive real numbers less than one which determine the fraction of the field that contributes towards a nodal current |
L | the total number of ion channels distributed uniformly over the nodal surface |