Difference between revisions of "NumericalDiffEqs"

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(Numerical Solution of Differential Equations)
(Numerical Solution of Differential Equations)
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<math> \frac{dy}{dt} = f(y) </math>
 
<math> \frac{dy}{dt} = f(y) </math>
  
<big> <big> <big> <math> y_k = y_{k-1} + dt f(y_{k-1}) </math> </big> </big> </big>
+
<big> <big> <big> <math> y_k = y_{k-1} + dt / f(y_{k-1}) </math> </big> </big> </big>
 
   
 
   
 
Click here for [[Media:intuit.hoc|code]] for visualizing the numerical solution of differential equations.
 
Click here for [[Media:intuit.hoc|code]] for visualizing the numerical solution of differential equations.

Revision as of 23:39, 12 February 2009

Equilibrium Potentials

You can find the equilibrium potential for given channel conductances. Set the injected current to zero I = 0. Then fix and absorb the gating variables and maximal conductances  (g_L, g_{Na}, g_{K}) into single conductance variables  (G_L, G_{Na}, G_{K}) .

For example

 G_{K} = n^4 g_K

Then the differential equation for the membrane is

 C \frac{dV}{dt} = - G_L (V - E_L) - G_{Na} (V - E_{Na}) - G_K (V - E_K)

The equilibrium potential is the value of V such that  \frac{dV}{dt} is zero. You can plug in  \frac{dV}{dt} = 0 and solve for  V_{equilibrium}.

 V_{equilibrium} = \frac{G_L E_L + G_{Na} E_{Na} + G_K E_K}{G_L + G_{Na} + G_K}

The equilibrium potential is the weighted average of the reversal potentials -- weighted by the corresponding conductances. Note that the weights add to one.

Numerical Solution of Differential Equations

Remember the equation for the cell with only leak channels.

 C \frac{dV}{dt} = I(t) - g_L(V - E_L)

Let's simplify: suppose there is no injected current and that the reversal potential for the leak channels is  E_L = 0 . Then our equation is

 \frac{dV}{dt} = - \frac{g_L}{C} V

Using different letters for the variables (because this is done in the software linked below):

 \frac{dy}{dt} = - k y

Here k is the rate constant, 1/k is the time constant, 1/k is  \frac{C}{g_L} = RC in the notation above. A leaky cell is what is called an RC circuit -- a resistor and capacitor together in a circuit. The time constant of an RC circuit is RC. The bigger k, the higher the rate of convergence, and the smaller the time constant 1/k. The time constant is the time it takes the solution to decay to 1/e of its value.

Solution of differential equations happens at discrete times:  y_k , separated by small time intervals dt.

The simplest way of solving this equation is with Euler's method:

 y_k = y_{k-1} + dt (-k y_{k-1})

This is a special case of the general formula for Euler's method applied to the (vector) differential equation

 \frac{dy}{dt} = f(y)

 y_k = y_{k-1} + dt / f(y_{k-1})

Click here for code for visualizing the numerical solution of differential equations.