Saltatory Conduction: single AP or not?

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Saltatory conduction allows action potentials (APs) to "hop" between nodes of Ranvier in myelinated axons, enhancing speed due to reduced charge leakage. The discussion raises questions about whether multiple APs can exist simultaneously at different nodes, as one AP can initiate before another ends, suggesting potential contradictions in existing theories. It is noted that while APs travel along the axon, they do not have identical time courses, leading to variations in their shape and timing at different locations. The cable theory, which describes the passive spread of electrical signals, is debated regarding its ability to account for the complexities of neuronal behavior, including the roles of ion channels and the effects of decay and delay on signal propagation. Overall, the conversation highlights ongoing inquiries into the mechanisms of neuronal signaling and the adequacy of theoretical models to explain observed phenomena.
  • #121
somasimple said:
Edit: In the model a node is connected to 2 internodes and must be at the same potential.
In data: the end of an internode is not at the same potential than the beginning of the next internode.

somasimple said:
Edit:
http://www.pubmedcentral.nih.gov/articlerender.fcgi?artid=1473353
see figure 1 for a more appropriate electric model.

The data doesn't show a discontinuity, just a quick change in voltage over distance (HS Fig. 11). But I agree that if the node and internode are each modeled as a single compartment, it looks like there will be some discontinuity. I suppose more compartments can be added for both the node and internode, or it could also be taken care of by a partial differential equation in which parameters vary continuously over space.

Moore 1978 does look more appropriate. Some papers that cite their work are:

Hartline DK, Colman DR. Rapid conduction and the evolution of giant axons and myelinated fibers. Curr Biol. 2007 Jan 9;17(1):R29-35.
http://www.pbrc.hawaii.edu/~danh/PDFs/Hartline&Colman_2007.pdf

Richardson AG, McIntyre CC, Grill WM.
Modelling the effects of electric fields on nerve fibres: influence of the myelin sheath. Med Biol Eng Comput. 2000 Jul;38(4):438-46.

McIntyre CC, Richardson AG, Grill WM.
Modeling the excitability of mammalian nerve fibers: influence of afterpotentials on the recovery cycle. J Neurophysiol. 2002 Feb;87(2):995-1006.
http://jn.physiology.org/cgi/content/full/87/2/995

Hartline's site: http://www.pbrc.hawaii.edu/~danh/
Grill's site: http://fds.duke.edu/db/pratt/BME/faculty/warren.grill/publications
 
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  • #122
granpa said:
because inductance is the electrical equivalent of mass.
http://en.wikipedia.org/wiki/Inductance
A neutral thing (water) seems unable to create electric field or voltage by itself.
 
  • #123
this all reminds me so much of the equivalent circuits of microscopic straight wires in megahertz microprocessor design. I've been trying to find a diagram but I don't even know what to google.

and if its being driven close to its limit (the speed of sound in water) then that is also similar to microprocessor wires being driven close to the speed of light.

both are semi-dc.
 
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  • #124
somasimple said:
http://en.wikipedia.org/wiki/Inductance
A neutral thing (water) seems unable to create electric field or voltage by itself.

it has mass and inductance is the electrical equivalent of mass. it is an 'equivalent circuit'.
 
  • #125
atyy said:
I suppose more compartments can be added for both the node and internode, or it could also be taken care of by a partial differential equation in which parameters vary continuously over space.
No, because adding a compartment does not change anything: Discontinuity will be... propagated,
And No because a model may be tortured until it fits your though but it is better when it sticks facts.
ps: I'll take a closer look to papers.

Granpa: Water may be a perfect silent actor.
Edit: I received "Biophysics of computation" By C Koch (it will help.)
 
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  • #126
http://www.edn.com/article/CA56702.html

http://www.ece.uci.edu/docs/hspice/hspice_2001_2-2874.jpg

http://www.ece.uci.edu/docs/hspice/hspice_2001_2-269.html

It is only during the initial surge of the voltage that a transmission line behaves as a constant impedance, with a value equal to its characteristic impedance. For this reason the characteristic impedance of a line is also called the surge impedance. The surge time during which the impedance is constant is the round trip time of flight, or twice the time delay. Reflections from the far end complicate the electrical behavior of the line after the surge time.
The instantaneous impedance measured at the front end of a transmission line is a complicated function of time. It depends on the nature of the terminations at the far end. When the line is shunted to ground with a resistor of value equal to the characteristic impedance of the line, there is no reflection back, and the front end of the line behaves as a resistive load. When the termination at the far end is open, the impedance at the front end starts out at the characteristic impedance and eventually, after multiple reflections, approaches an infinite impedance. During some periods the instantaneous impedance may be zero.

http://en.wikipedia.org/wiki/Impedance_mismatch

Impedance matching is the electronics design practice of setting the output impedance (ZS) of a signal source equal to the input impedance (ZL) of the load to which it is ultimately connected, usually in order to maximize the power transfer and minimize reflections from the load. This only applies when both are linear devices.
The concept of impedance matching was originally developed for electrical power, but can be applied to any other field where a form of energy (not just electrical) is transferred between a source and a load.

To prevent all reflections of the signal back into the source, the load (which must be totally resistive) must be matched exactly to the source impedance (which again must be totally resistive)

https://www.physicsforums.com/showpost.php?p=1873931&postcount=2
 
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  • #127
Granpa,
I have already stated that the cable model has no inductance so it makes problem for an eventual delay.
BTW, having a delay is not a proof of an impedance existence.
 
  • #128
somasimple said:
Not at all.
http://www.sosmath.com/calculus/limcon/limcon05/limcon05.html" is a prerequisite for an electrical signal in a wire/cable.
There is discontinuities at internode/node junctions when the signal leaves the internode entering in the node and when it leaves the node entering to the next internode.
This is wrong, there is no continuity requirement.

Consider the wave equation in 1 spatial dimension (e.g. an electrical signal in a wire)
c^2 \frac{\partial ^2f}{\partial x^2}=\frac{\partial<br /> ^2f}{\partial t^2} (1)

This has the solution
f = H(x-ct) (2)
where H is the Heaviside unit step function

Equation (2) is discontinuous in both time and space and it remains discontinuous even in the limit as c goes to infinity. And similarly discontinuous solutions exist for the wave equation in 3 spatial dimensions.

The above is not even including discontinuities in the medium which can lead to solutions with even more complicated discontinuities. There is simply nothing about Maxwell's equations or circuit theory that requires continuity.
 
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  • #130
http://www.ece.uci.edu/docs/hspice/hspice_2001_2-2874.jpg

the interesting thing aboutthis model is that if yoi suddenly apply a dc voltage (turn on the water) then only the leading edge is affected. behind the leading edge the pipe is already full of water so the capacitors are irrelevant and the current isn't changing so the inductance (mass of the water. an inductor would be modeled as a constriction in the pipe) is irrelevant. only at the leading edge do these have any effect. the speed of the leading edge is v=1/√(L*C)

and as long as the inductance of one portion matches the inductance of the next then there is no reflection. it all becomes quite simple to visualize.

it also works if the pipe is emptying.
 
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  • #132
what is the maximum frequency at which the long myelinated axons of the spinal cord can transmit ap's?
 
  • #133
granpa said:
http://www.ece.uci.edu/docs/hspice/hspice_2001_2-2874.jpg

the interesting thing aboutthis model is that if yoi suddenly apply a dc voltage (turn on the water) then only the leading edge is affected. behind the leading edge the pipe is already full of water so the capacitors are irrelevant and the current isn't changing so the inductance (mass of the water. an inductor would be modeled as a constriction in the pipe) is irrelevant. only at the leading edge do these have any effect. the speed of the leading edge is v=1/√(L*C)
That is wrong. The charge of a capacitor isn't linear and its impedance changes from 0 to infinite => currunt is changing.

DaleSpam,
Are you masochist?
There is a quite soliton solution for unmyelinated axons and the function has a derivative at any portion => Continuity.
The case is totally different for myelinated axons => A discontinuity exists in regard of x.

How do you infer on the t variable? Are you able to rewind time or stop it...?
That is the fate of a temporal function: Time that inexorably flows without...discontinuity.
 
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  • #134
granpa said:
what is the maximum frequency at which the long myelinated axons of the spinal cord can transmit ap's?
In mammals the CV speed is 120~150 ms-1 but the firing rate is often < 200 HZ
 
  • #135
so more myelin or larger axon=less capacitance=greater voltage difference in signal=less delay at the node. (which kinda somehow makes sense)

the myelin doest have much effect on the speed of the wave across a single internode.
 
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  • #136
somasimple said:
That is wrong. The charge of a capacitor isn't linear and its impedance changes from 0 to infinite => currunt is changing.
.


not sure what you are saying. but the capacitors behind the leading edge are already full and the voltage isn't changing (its only changing at the leading edge) so the capacitors have no further effect and can be ignored.
 
  • #137
granpa said:
so more myelin or larger axon=less capacitance=greater voltage difference in signal=less delay at the node. (which kinda somehow makes sense)

the myelin doest have much effect on the speed of the wave across a single internode.

We are disagreeing on this. Computations have shown the contrary (in regard to length).

Here is another aspect of discontinuity:
 

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  • #138
your messages have a tendency to be something more than cryptic. its not clear to me what you mean by 'in regard to length'. if your just saying that myelin does speed ip internode travel then ok. it may speed it up some but still the internode speed is so great that it hardly matters. it seems to me that it is the delay at the node that pretty much determines the net speed of the ap over many nodes.

http://www.pubmedcentral.nih.gov/pagerender.fcgi?artid=1392492&pageindex=8

what do you mean x1 and x2 are undefined? that article you originally linked to actually measured internode values. that's what started this conversation.
 
  • #139
And here is a graph that show the number of active nodes during a single propagated AP.
It becomes obvious that the energetic cost is dependent of speed and spike duration.
It is another proof of discontinuity.
 

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  • #140
granpa said:
your messages have a tendency to be something more than cryptic. its not clear to me what you mean by 'in regard to length'.
It was described earlier:
https://www.physicsforums.com/showthread.php?t=258168

granpa said:
what do you mean x1 and x2 are undefined? that article you originally linked to actually measured internode values. that's what started this conversation.

Onto the right of the picture:
x1 and x2 are taken on the apparent AP given by the apparent conduction velocity.
Thus you see an apparent AP at nodes (or wherever you want if you respect a constant interval) that is the result of synchrony of multiple firing nodes.
This apparent AP looks like an overlapping of time axis.
 
  • #141
those are actual measurements of an actual ap by electrodes placed 3 to an internode along a single axon. one by the node. another in the middle of the internode. the third by the node at the opposite end. this is repeated for several consecutive nodes.

they even go against what was expected. look at the backward propagating signal in curve c

notice the phrase 'from the same records as fig 6'
 
  • #142
granpa,
we don't care at all.
If an AP has a duration and a speed then it has a "length".
This last value determines the # of active nodes and their values (curve fitting).
you can't mix nodes with internodes if you respect a constant interval = internode lenght.
 
  • #143
granpa said:
they even go against what was expected. look at the backward propagating signal in curve C
This is not really a backward propagation since the peak stays at its place but a shortening of the falling phase.
 
  • #144
somasimple said:
This is not really a backward propagation since the peak stays at its place but a shortening of the falling phase.

absolutely. exactly right. its not the peak that's moving backward. its the falling phase. a nort of anti-ap that is moving backward (from the next node at coincidentally exactly the same time that that node fires its ap forward) returning the axon to its resting state.
 
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  • #145
granpa said:
absolutely. exactly right. its not the peak that's moving backward. its the falling phase. a nort of anti-ap that is moving backward (from the next node at coincidentally exactly the same time that that node fires its ap forward) returning the axon to its resting state.
Hmm, it is now, impossible to find a passive and electrical solution... :rolleyes:
 
  • #146
somasimple said:
Hmm, it is now, impossible to find a passive and electrical solution... :rolleyes:
not if the node from which from which the anti-ap propagates becomes (just before it fires) completely impassable to all ap's and anti-ap's. then its very simple
 
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  • #147
granpa said:
so more myelin or larger axon=less capacitance=greater voltage difference in signal=less delay at the node. (which kinda somehow makes sense)

The part I don't understand about this is membrane capacitance seems to always appear with membrane resistance in the equations: RmCm.

Myelin decreases capacitance, but increases resistance, so it does nothing to RmCm.

It would make a lot more sense to me if the standard explanation emphasized that myelin increases Rm to increase the length constant, in which case decreased Cm is needed to keep RmCm the same.
 
  • #148
I don't know anything about the standard explanation. and very little about time and length constants. (just a little about rlc circuits)

all i know is that myelin (and increased axon diameter) increases net speed of conduction which is apparently (http://www.pubmedcentral.nih.gov/pagerender.fcgi?artid=1392492&pageindex=8) mainly controlled by the delay at the node. I'm assuming passive conduction through the internode and virtually no leakage (cells can't be that leaky. they wouldn't survive). the only reason for the myelin then would be to increase capacitance and that means that fewer ions moving across the membrane produces a larger voltage difference.
 
  • #149
somasimple said:
Hmm, it is now, impossible to find a passive and electrical solution... :rolleyes:
Two currents are added in this configuration and it can't give such a solution, Granpa.
I insist.
see:
www.somasimple.com/flash_anims/node_01.swf

Atyy said:
Myelin decreases capacitance, but increases resistance, so it does nothing to RmCm.
A Nothing that increases speed is THE explanation. :smile:
 
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  • #150
somasimple said:
Two currents are added in this configuration and it can't give such a solution, Granpa.
I insist.

I'm afraid I have no idea what you mean by that.
 

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