The Hodgkin-Huxley equations are a nonlinear system of ordinary differential equations for the voltage and three gating variables
,
,
and
of an excitable membrane (Hodgkin and Huxley 1952). In a voltage convention with
currents proportional to
,
the spatially uniform system is
|
(1)
| |||
|
(2)
|
where the second equation applies to each in
.
Here
is the capacitance,
is the applied current, and the
and
are maximal conductances and reversal potentials for the
sodium, potassium, and leak terms. The voltage-dependent rates
and
are nonnegative. They make the interval
invariant for each gating variable since
at
and
at
.
If , a fixed voltage makes
relax exponentially to
|
(3)
|
For a constant applied current, substituting these values in the voltage equation reduces the search for an equilibrium point
to a scalar equation for .
Varying the applied current in the original parameter regime gives Hopf
bifurcations and branches of periodic orbits
(Hassard 1978).
The Morris-Lecar model uses a related conductance-based voltage equation with a single dynamic gate and an instantaneous calcium gate.