12.07.2015 Views

Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

SHOW MORE
SHOW LESS
  • No tags were found...

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

26 Electrophysiology of NeuronsInsideNa + (5-15 mM)K + (140 mM)Cl-(4 mM)Ca 2+ (0.1 µ M)A-(147 mM)ActiveTransportNa +Na + Na +PumpK + K +K +A -OutsideK + A - Na + Cl -Na + (145 mM)K + (5 mM)Cl-(110 mM)Ca 2+ (2.5-5 mM)A-(25 mM)Cl -PassiveRedistributionEquilibrium PotentialsNa + 62 log 1455= 90 mV62 log 14515= 61 mVK + 62 log 5140= −90 mVCl − −62 log 1104= −89 mVCa 2+ 31 log 2.510 −4 = 136 mV31 log 510 −4 = 146 mVFigure 2.1: Ion concentrations and Nernst equilibrium potentials (2.1) <strong>in</strong> a typicalmammalian neuron (modified from Johnston and Wu 1995). A − are membraneimpermeantanions. Temperature T = 37 ◦ C (310 ◦ K).every two K + ions pumped <strong>in</strong>, thereby ma<strong>in</strong>ta<strong>in</strong><strong>in</strong>g concentration gradients.2.1.1 Nernst potentialThere are two forces that drive each ion species through the membrane channel: concentrationand electric potential gradients. First, the ions diffuse down the concentrationgradient. For example, the K + ions depicted <strong>in</strong> Fig. 2.2a diffuse out of the cell becauseK + concentration <strong>in</strong>side is higher than that outside. While exit<strong>in</strong>g the cell, K + ionscarry positive charge with them and leave a net negative charge <strong>in</strong>side the cell (consist<strong>in</strong>gmostly of impermeable anions A − ), thereby produc<strong>in</strong>g the outward current. Thepositive and negative charges accumulate on the opposite sides of the membrane surfacecreat<strong>in</strong>g an electric potential gradient across the membrane – transmembrane potentialor membrane voltage. This potential slows down the diffusion of K + , s<strong>in</strong>ce K + ions areattracted to the negatively charged <strong>in</strong>terior and repelled from the positively chargedexterior of the membrane, as we illustrate <strong>in</strong> Fig. 2.2b. At some po<strong>in</strong>t an equilibriumis achieved: The concentration gradient and the electric potential gradient exert equaland opposite forces that counterbalance each other, and the net cross-membrane currentis zero, as <strong>in</strong> Fig. 2.2c. The value of such an equilibrium potential depends on theionic species, and it is given by the Nernst equation (Hille 2001)E ion = RTzF ln [Ion] out[Ion] <strong>in</strong>, (2.1)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!