Univ. of Illinois, Urbana-Champaign

Prof. Mark Nelson

This assignment is devoted to modeling voltage-dependent membrane currents in the squid giant axon using the Hodgkin-Huxley formalism. The equivalent circuit is shown below. To carry out this assignment, you'll need a copy of Hodgkin and Huxley's 1952 paper, "A quantitative description of membrane current and its application to conduction and excitation in nerve", J. Physiol. 117, 500-544.

** **

1. One of the most error-prone steps in implementing HH models is in
evaluating the voltage-dependent rate constants** ***alpha(v)
and beta(v). *For that reason,
it's always a good idea to check you implementation by plotting the time
constants and steady-state values as a function of voltage. It's much easier
to spot errors in these plots than in the raw rate plots. Recall*:*

(a) Write a set of six subroutines (alpha_m, beta_m, alpha_h, beta_h,
alpha_n and beta_n)
that return rate constants as a function of voltage for the HH state
variables m, n and h.
Use the expressions given in HH52 (eqs. 12, 13, 20, 21, 23, 24) BUT
REVERSE THE
SIGN OF THE VOLTAGE to conform to the modern voltage convention. Note
that some
of the expressions evaluate to the indeterminant form "0/0" at certain
voltages. Handle this
case properly in your subroutines by applying L'Hopitals Rule: i.e.
for* f(a) = g(a) = 0:*

(b) Generate and turn in plots of
TAU_{m}(v) , TAU_{h}(v), TAU_{n}(v),
m_{infty}(v) , h_{infty}(v) and n_{infty}(v)
for voltages in the range -50 <= v <= 150.

Check your results against the following figure.