First make sure that the Properties radio button is ON.
Now let's deal with m.
Clicking on m causes many changes in the appearance of the GateGUI.
Look at the area to the right of the canvas. This contains controls for specifying the "Power" for m and its associated "fractional conductance".
Change it to 3.
"Fractional conductance" is useful for kinetic scheme channel descriptions, in which different states may have different levels of conductance. For HH-style states, the "fractional conductance" is a constant multiplier that is applied to every instance of the state in the equation for channel conductance.
So just make sure that the "fractional conductance" of every HH-style state is 1.
- Example: if you change the "m fraction" to 0.7, the equation in the top panel of the Channel Builder will be
- g = gmax * (0.7*m)^3 * h
- instead of the desired
- g = gmax * m^3 * h
Now we need to specify the voltage dependence of the rate constants am and bm.
Specifying a functional form is easy--we only have to select from
the GateGUI's EquationType menu.
then down to
and over to
A*x / (1 - exp(-x)) where x = k*(v - d)
An aside : the other functional forms in the menu are constant, single exponential, logistic, and KSChanTable.Now the GateGUI looks like this
The parameters A, k, and d are all initially 0. A little rearranging of the equation for am shows us that A = 1, k = 0.1, and d = -40. Entering these values into the corresponding numeric fields gives us
Notice that the graph in the bottom half of the GateGUI shows the voltage dependence of am and bm. am increases nicely as membrane potential depolarizes, but bm remains 0 at all voltages.
Obviously we have to specify the voltage dependence of bm,
but it seems that the EquationType button has
until we realize that it was just pushed out of sight by the appearance of am's buttons for A, k, and d. There is a scroll bar on the right edge of this panel, and dragging this down
unmasks the EquationType button.
The new parameters for bm are all 0 but should be A = 4, k = -1/18, and d = -65. Making these changes, we now see this :
You may have to resize the window to see the full extent of the bottom half of the GateGUI tool. You also may want to use "View = plot" to rescale the display of am and bm.
Some interesting asides--
- Clicking on the "Display inf,tau" checkbox toggles the graph between plots of am and bm and plots of the voltage dependence of infm (steady state of m) and taum.
- The GateGUI's EquationType menu also allows gating properties to be specified in terms of steady state and time constant. The functional forms offered for inf,tau (constant, logistic, exponential) are the only ones necessary for a model in which the energy difference between states is linear with voltage and the energy barrier is also linear with voltage.
- The little squares on the am and bm graphs are "control points" that you can click on and drag to quickly change their A and d parameters. If the Adjust radio button is ON, vertical movement changes A, and horizontal movement changes d.
- If you click near a curve, the k parameter will be adjusted so that the little square control point does not move but the curve passes through the mouse location.
- If the Run checkbox is checked, NEURON automatically executes a new simulation every time you change a parameter. This can give quick insights into how parameter changes affect excitability. We'll return to this later.
Doesn't this seem like a good time to save to a session file?
Now we have to deal with h.
Click on h in the canvas. Specify its "power" and "fractional conductance" (hint: both 1).
You should end up with something like this:
Bring up the inf,tau plots for h. Check these plots to make sure they look like they should.
Before moving on to the next step, save the Channel Builder to a session file!
Next we will test our new channel in a model cell.
Copyright © 2004-2008 by N.T. Carnevale and M.L. Hines, All Rights Reserved.