2.2 Propagation in a uniform squid axon
A major goal of Hodgkin and Huxley was to show that their
equations for the ion channels was not only able to generate a
realistic membrane action potential in a uniform patch but
also that they would provide a reasonable propagating impulse
along an axon. Huxley had developed his own methods for accurate
numerical integration of an ordinary differential equation
for a membrane action potential but it took him
8 hours to calculate one with the tools available at that time -
manual calculators, requiring entry of data by hand and
"cranking" a lever to obtain the result of a single arithmetic
operation. The solution of the partial differential
equation describing the membrane voltage in space as well as
time for
the propagation of an impulse along an axon was completely out of
the question. Huxley worked around this problem by noting that,
for the restricted special case of propagation of an impulse with
constant form and velocity
along a uniform (in diameter and channel density) axon,
the "traveling wave equation", a simpler ordinary differential
equation could be used. Applying this equation, he had to guess
at the velocity of the propagating wave, run a calculation and
see
whether the solution was stable (returning to rest after a spike)
or unstable (flying off to + or - infinity). After the many
successive approximations required to find a value for the
velocity to many significant figures, Huxley was able to
calculate a reasonably shaped action potential- 18.8 M/S at a
temperature of 18.5C for an axon of 476 microns in diameter.
I have used this parameter set as a reference standard
against
which to check the accuracy of the output of our
computer programs. Of course NEURON 3.0 has undergone this
rigorous test. Today you need not be concerned with the problems
of how to solve partial differential equations nor with numerical
integration methods. You can be confident that they have been
taken care of so that you can
concentrate on the physiology of impulse propagation.
Run this program for a
uniform squid axon
to learn how
the velocity of propagation is changed by:
- axon diameter
- axial resistivity: 35.4ohm/cm for sea creatures, about 150
for land
- temperature
- channel density
- partial blocking of channels