Symbol

Meaning

ρ , ρ

radial distance of the (field point, source point) from the axis of the cylinder

ϕ

azimuthal angle

z , z

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

r 1 , l 1

(starting, termination) point in time of the PWM-PPM waveform [8] of the ion channel current profile

U ( )

Heaviside step function

δ ( )

Dirac delta function

ϕ L F P ( r , t )

electric potential at spatial (field) position r and time t

I v ( r , t ) , I ( r )

volume source current density produced by an ion channel ring (with, without) time variation

r

position of the source element

ε

permittivity of free space

ϕ , ϕ

azimuthal coordinates of the (field point, source point)

gradient operator

E channel

the net electric field due to the ion channel

k ^ , e ^ ρ

two of the three unit vectors in the three-dimensional coordinate system

ρ 1 , ρ 2

two radial distances used to generate the form of the current near the node

Δ ϕ

azimuthal thickness of the first ion channel in the ring of ion channels at the node of Ranvier

c m , k , g m , k

the membrance (capacitance, conductance) of the k-th axon

V k ( x , t )

the transmembrane potential difference of the k-th axon at spatial position x and time t

α N

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

r f

the resistance per unit length of the axoplasm of each axonal fiber

G k axoplasm , G m , k

the conductance of the (axoplasm, myelin sheath) of the k-th axon

θ k , θ k ( z )

the inclination of the k-th axon (without, with) z-dependence

K p , K p ( z )

a combination of parameters introduced by Chawla, Morgera and Snider (without, with) z-dependence

I k injected

the total injected current at the node, including contributions from ionic current, as well as external stimulation

l ( t )

number of ion channels open at the present node at time t

γ , γ

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