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Calcium dynamics and IK-AHP

Most of the models that are commonly used treat the current as in (4) but we will see that calcium is somewhat special and requires a more complex approach.

Intracellular calcium is heavily buffered so that the concentration tends be be very low. As a consequence the reversal potential for calcium can not really be modeled as a fixed value. The intracellular calcium levels are on the order of 1000 times lower than extracellular calcium which accounts for the rather large reversal potential for calcium. The way that many researchers model calcium is through the constant field equation  
 \begin{displaymath}
I_{Ca} = P_{Ca} m^ph^q \frac{4 F^2}{RT} V
\left(\frac{[Ca]_{in} e^{2VF/RT} -
[Ca]_{out}}{e^{2VF/RT}-1}\right)\end{displaymath} (5)
where F=96480 Colombs/mole, $R=8.3145 J/mol-{}^\circ K$, PCa is the permeability, and T is the temperature in degrees Kelvin (centigrade plus 273).

NOTES:

To get some intuition behind this expression, define

\begin{displaymath}
E_{Ca} = \frac{RT}{2F}\ln\frac{[Ca]_{out}}{[Ca]_{in}}\end{displaymath}

as is usual. Then in the above, it is clear that V=ECa makes the current vanish so that the ``reversal potential'' is indeed the Nernst equilibrium for calcium and linearizing about this reversal potential, we get the slope

\begin{displaymath}
\bar{g}_{Ca} = \frac{2P_{Ca}F^3
E_{Ca}[Ca]_{out}/(RT)^2}{[Ca]_{out}/[Ca]_{in}-1}\end{displaymath}

which if you check has dimensions of conductance per unit area. Thus, we can approximate (5) by

\begin{displaymath}
I_{Ca} = \bar{g}_{Ca} (V - E_{Ca})\end{displaymath}

where ECa is the Nernst equilibrium potential. We will use the two interchangeably, but keep in mind that the constant field equation is more correct.



 
next up previous
Next: Intracellular Calcium dynamics Up: Channeling with Bard Previous: Some common currents in
G. Bard Ermentrout
1/29/1998