diam · diam_changed · L · Ra
Sections are unbranched lengths of continuous cable connected together to form a neuron. Sections can be connected to form any tree-shaped structure but loops are not permitted. (You may, however, develop membrane mechanisms, such as electrical gap junctions which do not have the loop restriction. But be aware that the electrical current flows through such connections are calculated by a modified euler method instead of the more numerically robust fully implicit/crank-nicholson methods)
Do not confuse sections with segments. Sections are divided into segments of equal length for numerical simulation purposes (see nseg). NEURON uses segments to represent the electrical circuit shown below.
Ra
o/`--o--'\/\/`--o--'\/\/`--o--'\/\/`--o--'\o v
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--- --- --- ---
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--- --- --- ---
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-------------------------------------------- ground
Such segments are similar to compartments in compartmental modeling programs.
Section geometry is used to compute the area and axial resistance of each segment.
There are two ways to specify section geometry:
Choose the stylized method if the notions of cable length and diameter are authoritative and where 3-d shape is irrelevant. For plotting purposes, length and diameter will be used to generate 3-d info automatically for a stylized straight cylinder. (see define_shape())
Choose the 3-D method if the shape comes from 3-d reconstruction data or if your 3-d visualization is paramount. This method makes the 3-d info authoritative and automatically determines the abstract cable's length and diameter. With this method, you may change a section's length/diameter only by changing its 3-d info. (but see pt3dconst())
For simulations one needs to specify L, nseg, diam, Ra, and connectivity.
In the stylized specification, the shape model used for a section is a sequence of right circular cylinders of length, L/nseg, with diameter given by the diam range variable at the center of each segment. The area of a segment is PI*diam*L/nseg (micron2) and the half-segment axial resistance is .01*Ra*(L/2/nseg)/(PI*(diam/2)^2). The .01 factor is necessary to convert ohm-cm micron/micron2 to MegOhms. Ends of cylinders are not counted in the area and, in fact, the areas are very close to those of truncated cones as long as the diameter does not change too much.
forall delete_section()
create a
access a
nseg = 10
Ra = 100
L=1000
diam(0:1)=10:100
for (x) print x, diam(x), area(x), PI*diam(x)*L/nseg, ri(x), .01*Ra*(L/2/nseg)/(PI*(diam(x)/2)^2)
Note that the area (and length) of the 0,1 terminal ends is equal to 0 and the axial resistance is the sum of the adjacent half-segment resistances between segment and parent segment. Such, niceties allow the spatial discretization error to be proportional to (1/nseg)^2. However, for second order correctness, all point processes must be located at the center of the segments or at the ends and all branches should be connected at the ends or centers of segments. Note that if one increases nseg by a factor of 3, old centers are preserved.
For single compartment simulations it is most convenient to choose a membrane area of 100 micron2 so that point process currents (nanoamps) are equivalent to density currents (milliamps/cm2).
Also note that a single compartment of length = diameter has the same effective area as that of a sphere of the same diameter.
The following example demonstrates the automatic 3-d shape construction. The root section "a" is drawn with its 0 end (left) at the origin and is colored red.
Sections connected to its 1 end (sections b, c, d) get drawn from left to right. Sections descended from the 0 end (section e) of the root get drawn from right to left.
Especially note the diameter pattern of section c whose "1" end is connected to the "b" parent. You don't have to understand this if you always connect the "0" end to the parent.
forall delete_section()
create a, b, c, d, e
connect b(0), a(1)
connect c(1), b(1)
connect d(0), b(1)
connect e(0), a(0)
forall nseg=20
forall L=100
forall diam(0:1) = 10:40
objref s
s = new Shape()
s.show(0)
a s.color(2)
topology()
finitialize()
forall {
print secname()
for i=0,n3d()-1 print i, x3d(i), y3d(i), z3d(i), diam3d(i)
}
If you change the diameter or length, the Shape instances are automatically redrawn or when doNotify() is called. Segment area and axial resistance will be automatically recomputed prior to their use.
Under some circumstances, involving nonlinearly varying diameters across a section, at first sight surprising results can occur when the stylized method is used and a Shape instance is created. This is because under a define_shape() with no pre-existing 3-d points in a section, a number of 3-d points is created equal to the number of segments plus the end areas. When 3-d points exist, they determine the calculation of L, diam, area, and ri. Thus diam can change slightly merely due to shape creation. When L and diam are changed, there is first a change to the 3-d points and then L and diam are updated to reflect the actual values of these 3-d points. Due to multiple interpolation effects, specifying a nonlinearly varying diam will, in general, not give exactly the same diameter values as the case where no 3-d information exists. This effect is illustrated in the following example
forall delete_section()
objref s
proc pr() {
pt3dclear()
nseg = $1
diam = 10
diam(.34:.66) = 20:20
define_shape()
for(x) print x*L, diam(x), area(x), ri(x)
}
xpanel("change nseg")
xradiobutton("nseg = 3", "pr(3)")
xradiobutton("nseg = 11", "pr(11)")
xradiobutton("nseg = 101", "pr(101)")
xpanel()
create a
access a
nseg=3
{Ra=100 L=100}
diam=10
diam(.34:.66) = 20:20
for(x) print x*L, diam(x), area(x), ri(x)
s = new Shape()
s.show(0)
for i=0, n3d()-1 print i, arc3d(i), diam3d(i)
print "L=", L
for(x) print x*L, diam(x), area(x), ri(x)
The difference is that the 3-d points define a series of truncated cones instead of a series of right circular cylinders. The difference is reduced with larger nseg. With the stylized method, abrupt changes in diameter should only take place at the boundaries of sections if you wish to view shape and also make use of the fewest possible number of segments. But remember, end area of the abrupt changes is not calculated. For that, you need an explicit pair of 3-d points with the same location and different diameters.
3-d information for a section is kept in a list of (x,y,z,diam) "points". The first point is associated with the end of the section that is connected to the parent (NB: Not necessarily the 0 end) and the last point is associated with the opposite end. There must be at least two points and they should be ordered in terms of monotonically increasing arc length.
The root section is treated as the origin of the cell with respect to 3-d position. When any section's 3-d shape or length changes, all the sections in the child trees have their 3-d information translated to correspond to the new position. So, assuming the soma is the root section, to translate an entire cell to another location it suffices to change only the location of the soma. It will avoid confusion if, except for good reason, one attaches only the 0 end of a child section to a parent. This will ensure that the diam(x) as x ranges from 0 to 1 has the same sense as diam3d(i) as i ranges from 0 to n3d()-1.
The shape model used for a section when the pt3d list is non-empty is that of a sequence of truncated cones in which the pt3d points define the location and diameter of the ends. From this sequence of points, the effective area, diameter, and resistance is computed for each segment via a trapezoidal integration across the segment length. This takes into account the extra area due to sqrt(dx^2 + dy^2) for fast changing diameters (even degenerate cones of 0 length can be specified, ie. two points with same coordinates but different diameters) but no attempt is made to deal with centroid curvature effects on the area. Note that the number of 3d points used to describe a shape has nothing to do with nseg and does not affect simulation speed. (Although, of course, it does affect how fast one can draw the shape)
The following illustrates the notion of the 3-d points as describing a sequence of cones. Note that the segment area and resistance is different than the simplistic calculation used in the stylized method. In this case the area of the segment has very little to do with the diameter of the center of the segment.
forall delete_section()
create a
access a
Ra=100
nseg = 10
pt3dclear()
for i=0,30 {
x = PI*i/30
pt3dadd(200*sin(x), 200*cos(x), 0, 100*sin(4*x))
}
objref s
s = new Shape()
s.show(0)
print L
for (x) print x, diam(x), area(x), PI*diam(x)*L/nseg, ri(x), .01*Ra*(L/2/nseg)/(PI*(diam(x)/2)^2)
Note that at one point the diameter is numerically 0 and the axial resistance becomes essentially infinite thus decoupling the adjacent segments. Take care to avoid constructing spheres with a beginning and ending diameter of 0. No current would flow from the end to a connecting section. The end diameter should be the diameter of the end of the connecting section.
The following loads the pyramidal cell 3-d reconstruction from the demo directory of your neuron system. Notice that you can modify the length only if the pt3dconst mode is 1.
forall delete_section()
xopen("$(NEURONHOME)/demo/pyramid.nrn")
mode = 1
pt3dconst(mode)
objref s
s = new Shape()
s.action("dendrite_1[8] s.select()")
dendrite_1[8] s.color(2)
xpanel("Change Length")
xvalue("dendrite_1[8].L", "dendrite_1[8].L", 1)
xcheckbox("Can't change length", &mode, "pt3dconst(mode)")
xpanel()
See also
pt3dclear(), pt3dadd(), pt3dconst(), pt3dstyle(), n3d(), x3d(), y3d(), z3d(), diam3d(), arc3d() getSpineArea(), setSpineArea(), spine3d()
See also
If 3-D shape is not an issue it is sufficient to specify the section variables L (length in microns), Ra (axial resistivity in ohm-cm), and the range variable diam (diameter in microns).
A list of 3-D points with corresponding diameters describes the geometry of a given section.
buffersize = pt3dclear()
buffersize = pt3dclear(buffersize)
Description:
Add the 3d location and diameter point at the end of the current pt3d list. Assume that successive additions increase the arc length monotonically. When pt3d points exist in a section they are used to compute diam and L. When diam or L are changed and pt3dconst()==0 the 3-d info is changed to be consistent with the new values of L and diam. (Note: When L is changed, diam_shape() should be executed to adjust the 3-d info so that branches appear connected.) The existence of a spine at this point is signaled by a negative value for d.
pt3dconst(0)
pt3dconst(1)
If pt3dconst is set at 0, newly assigned values for d and L will automatically update pre-existing 3d information. pt3dconst returns its previous state on each call. Its original value is 0.
Note that the diam information transferred to the 3d point information comes from the current diameter of the segments and does not change the number of 3d points. Thus if there are a lot of 3d points the shape will appear as a string of uniform diameter cylinders each of length L/nseg. ie. after transfer diam3d(i) == diam(arc3d(i)). Then, after a call to an internal function such as area() or finitialize(), the 3d point info will be used to determine the values of the segment diameters.
Because of the three separate interpolations: hoc range spec -> segment diameter -> 3d point diam -> segment diameter, the final values of the segment diameter may be different from the case where 3d info does not exist.
Because of the surprises noted above, when using 3d points consider treating them as the authoritative diameter info and set pt3dconst(1).
3d points are automatically generated when one uses the nrniv Shape class. If you want the flexibility of being able to specify 3d diameter using range variable notation (eg diam(0:1) = 10:20) you will need to experiment with nseg and n3d() in order to understand the exact consequences of interpolation.
See also
style = pt3dstyle()
style = pt3dstyle(0)
style = pt3dstyle(1, x, y, z)
style = pt3dstyle(1, &x, &y, &z)
With no args, returns 1 if using a logical connection point.
With a first arg of 0, then style is NO logical connection point and (with pt3dconst() == 0 and define_shape is executed) the 3-d location info is translated so the first 3-d point coincides with the parent connection location. This is the classical and default behavior.
With a first arg of 1 and x,y,z value arguments, those values are used to define a logical connection point relative to the first 3-d point. When pt3dconst() == 0 and define_shape is executed, the 3-d location info is translated so that the logical connection point coincides with the parent connection location. Note that logical connection points have absolutely no effect on the electrical properties of the structure since they do not affect the length or area of a section. They are useful mostly for accurate visualization of a dendrite connected to the large diameter edge of a soma that happens to be far from the soma centroid. The logical connection point should be set to the location of the parent centroid connection, i.e. most often the 0.5 location of the soma. Note, that under translation and scaling, the relative position between the logical connection point and the first 3-d point is preserved.
With a first arg of 1 and x,y,z reference arguments, the x,y,z variables are assigned the values of the logical connection point (if the style in fact was 1).
See also
pt3dchange(i, x, y, z, diam)
pt3dchange(i, diam)
Change the i'th 3-d point info. If only two args then the second arg is the diameter and the location is unchanged.
pt3dchange(5, x3d(5), y3d(5), z3d(5), (spine3d(5)+1)/2 * diam3d(5))
leaves the pt3d info unchanged.
See also
Fill in empty pt3d information with a naive algorithm based on current values for L and diam. Sections that already have pt3d info are translated to ensure that their first point is at the same location as the parent. But see pt3dstyle() with regard to the use of a logical connection point if the translation ruins the visualization.
Note: This may not work right when a branch is connected to the interior of a parent section 0 < x < 1, rather only when it is connected to the parent at 0 or 1.
Return the area (in square microns) of the segment which contains x.
area(0) and area(1) = 0
Example:
for (x) print x, area(x), ri(x)will print the arc length, the segment area at that arc length, and the resistance along that length for the currently accessed section.
distance() or distance(0, x)
len = distance(x) or len = distance(1, x)
Compute the path distance between two points on a neuron. If a continuous path does not exist the return value is 1e20.
To overcome the old initialization restriction, distance(0, x) can be used to set the origin. Note that distance is measured from the centers of segments.
create a, b
connect b(0), a(1)
a { L = 1000 nseg = 5 }
b { L = 200 nseg = 5 }
{ a distance(0, 0.5) } // origin is center of a
b print distance(0.0) // 500
b print distance(0.5) // 600
b print distance(1.0) // 700
Warning
When subtrees are connected by ParallelContext.multisplit() , the distance function returns 1e20 if the path spans the split location.
See also
Signals the system that the coefficient matrix needs to be recalculated.
This is not needed since Ra is now a section variable and automatically sets diam_changed whenever any sections Ra is changed. Changing diam or any pt3d value will cause it to be set automatically.
Axial resistivity in ohm-cm. This used to be a global variable so that it was the same for all sections. Now, it is a section variable and must be set individually for each section. A simple way to set its value is forall Ra=35.4
Prior to 1/6/95 the default value for Ra was 34.5. Presently it is 35.4.