This page is devoted to
the basic goals and assumptions that Hodgkin and Huxley made. They had
hoped to determine how ions flow in and out of a neuron during an action
potential. They assumed that the action potential was associated with
an inflow of sodiam and potassium ions. They also assumed that the membrane
current could be broken up into a capacitance current and an ionic current.
This page is also devoted to an explanation of the equipment
and methods they used to determine how ions flow in and out of the neuron
during an action potential. Specifically, we explored the construction
and use of the voltage clamp and the construction of the electrodes they
placed in the axon.
Goals and Assumptions
Voltage Clamp
Electrodes
Results
The Goals and Assumptions of Hodgkin and Huxley
The goal of Hodgkin and Huxley’s experiments was to determine the
laws that govern how ions flow in and out of a neuron during an action
potential. At the beginning of their experimentation, Hodgkin and Huxley
knew that the action potential is associated with an inflow of sodium
and potassium ions. They also knew that the rate and amplitude of the
action potential are determined by concentrations of sodium on the outside
of the neuron.The main assumption that Hodgkin and Huxley made for their
experiments was that the membrane current can be divided into a capacitance
current (which is caused by a change in ion density on the outside and
inside of the surface of the membrane) as well as an ionic current which
depends on the movement of sodium and potassium through the membrane.
The Voltage Clamp
To measure how ions flow through the neuron membrane during an action
potential, Hodgkin and Huxley measured the flow of current through a determined
area of neural membrane from the axon of a giant squid. They were able
to keep the voltage through the membrane constant and uniform via a feedback
amplifier
Now, when performing their experiment, an operational amplifier can
be used instead of the feedback amplifier used in the experiment.
At the time that Hodgkin and Huxley first performed their experiment,
op-amps in their current state were not invented. The negative terminal
of the op-amp was connected to the command voltage source that was controlled
by the experimenters. The positive terminal was connected to an electrode
that was set up to measure the voltage across the membrane. The operational
amplifier works using negative feedback to make the voltage across the
membrane equal to the command voltage. The output of the op-amp is connected
to a second electrode that is meant to measure the current passing through
the membrane. Current is injected into the system through the second electrode
so that the error signal is as close to zero as possible. The membrane
current and voltage as measured from the two electrodes is also passed
through an oscilloscope (at the time of the experiment, Hodgkin and Huxley
refer to the oscilloscope as a D.C. amplifier and cathode ray oscillograph.
The Electrodes
Hodgkin and Huxley had to develop an interesting way of creating the
two electrodes they used in their experiment. The electrodes are made
of two silver wires (about 20 microns in diameter). They were places 20-30
mm deep inside the neuron. The outside of the wires was insulated except
along the tips of the wires. The axon was surrounded by a guard ring system
which contained the external electrodes used in the system (for current,
external electrode was connected to ground). The current wire extended
along the whole guard system. The voltage wire only extends as far as
the center partition. This is to ensure that current is flowing in a straight
line where the voltage was being measured. At the ends, current could
begin to curve, making the voltage measurements less accurate. For more
information on exactly how the electrodes were made, the axons removed,
and the guard system applied, please read their paper.
Results:
To test their apparatus, Hodgkin and Huxley ran a few simple experiments.
Here are the results of the experiments.
The purpose of this set of experiments was to determine
if the action potential could really be measured using their setup. The
voltage clamp was turned off. It was found that in general, different
amplitude depolarization inputs yielded the same general shaped output.
The current pulse consists of a brief surge that is 95% complete within
8 microseconds. The peak amplitude was about 50 mA/cm3. However, depolarizations
above a few milivolts yield more non-linear results. It was also found
that the membrane capacity was 0.9 microfarads per centimeter squared.
It was found that the threshold voltage for an action potential was 15
mV. During the voltage clamp experiment, it was noted that there was a
“slight gap” in the output from the membrane. This gap is
caused by the capacity current. Hodgkin and Huxley built a table of the
graphs of all the current responses for different voltage values. It was
found that the amplitude and shape of an impulse did not change with different
temperatures, but the rate did change. Higher temperatures yielded faster
responses.
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(Figure 1: Diagram of how the voltage
clamp apparatus was set up)

(Figure 2: Schematic of the feedback
amplifier originally used in 1952. Now an operational amplifier is used
instead)

(Figure 3: Diagram of the internal
electrode.The exposed portions of wire
areshown with heavier line)

(Figure 4: Diagram to illustrate the
arrangement of the internal and external electrodes to create the guard
system.A1, A2, A3 and A4 are all partitions. a, b, c, d, and e are electrodes)

(Figure 5: Side view of the guard
system through one of the partititions)

(Figure 6: Side view of the guard
system through the central channel C. c and d are silver wires. e is a
silver sheet)
(Figure 7: Diagram of the time course
of the membrane potential following a brief shock (magnitude of shock
on the x-axis) at 23 degrees Celcius)

(Figure 7: Diagram of the time course
of the membrane potential following a brief shock at 6 degrees Celcius)

(Figure 8: Diagram of the membrane
current under voltage clamp conditions. Inward current is represented
by upward deflection)

(Figure 9: Memebrane Current at different
temperatures. Voltage clamp conditions were not used)
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