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Hodgkin-Huxley Equations


The Hodgkin-Huxley equations are a nonlinear system of ordinary differential equations for the voltage V and three gating variables m, h, and n of an excitable membrane (Hodgkin and Huxley 1952). In a voltage convention with currents proportional to V-E_j, the spatially uniform system is

CV^'=I(t)-g_(Na)m^3h(V-E_(Na))-g_Kn^4(V-E_K)-g_L(V-E_L)
(1)
q^'=alpha_q(V)(1-q)-beta_q(V)q,
(2)

where the second equation applies to each q in {m,h,n}. Here C>0 is the capacitance, I(t) is the applied current, and the g_j and E_j are maximal conductances and reversal potentials for the sodium, potassium, and leak terms. The voltage-dependent rates alpha_q(V) and beta_q(V) are nonnegative. They make the interval [0,1] invariant for each gating variable since q^'>=0 at q=0 and q^'<=0 at q=1.

If alpha_q(V)+beta_q(V)>0, a fixed voltage makes q relax exponentially to

 q_infty(V)=(alpha_q(V))/(alpha_q(V)+beta_q(V)).
(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 V. 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.


See also

Fitzhugh-Nagumo Equations, Hopf Bifurcation

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References

Hassard, B. "Bifurcation of Periodic Solutions of the Hodgkin-Huxley Model for the Squid Giant Axon." J. Theoret. Biol. 71, 401-420, 1978. https://doi.org/10.1016/0022-5193(78)90168-6.Hodgkin, A. L. and Huxley, A. F. "A Quantitative Description of Membrane Current and Its Application to Conduction and Excitation in Nerve." J. Physiol. 117, 500-544, 1952. https://doi.org/10.1113/jphysiol.1952.sp004764.

Cite this as:

Weisstein, Eric W. "Hodgkin-Huxley Equations." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/Hodgkin-HuxleyEquations.html

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