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Dynamical Systems in Neuroscience:

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50 Electrophysiology of NeuronsFigure 2.22: Alan Hodgk<strong>in</strong> (right) and Andrew Huxley (left) <strong>in</strong> their Plymouth Mar<strong>in</strong>eLab <strong>in</strong> 1949 (photo was k<strong>in</strong>dly provided by National Mar<strong>in</strong>e Biological Library,Plymouth, UK).Review of Important Concepts• Electrical signals <strong>in</strong> neurons are carried by Na + , Ca 2+ , K + , and Cl −ions, which move through membrane channels accord<strong>in</strong>g to theirelectrochemical gradients.• The membrane potential V is determ<strong>in</strong>ed by the membrane conductancesg i and correspond<strong>in</strong>g reversal potentials E i :C ˙V = I − ∑ ig i · (V − E i ) .• Neurons are excitable because the conductances depend on the membranepotential and time.• The most accepted description of k<strong>in</strong>etics of voltage-sensitive conductancesis the Hodgk<strong>in</strong>-Huxley gate model.• Voltage-gated activation of <strong>in</strong>ward Na + or Ca 2+ current depolarizes(<strong>in</strong>creases) the membrane potential.• Voltage-gated activation of outward K + or Cl − current hyperpolarizes(decreases) the membrane potential.• An action potential or spike is a brief regenerative depolarization ofthe membrane potential followed by its repolarization and possiblyhyperpolarization, as <strong>in</strong> Fig. 2.16.

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