Action Potential: Passive Spread Current

In summary: Hi,In summary, the passive event of electrotonic conduction occurs when the space constant of a thin fiber is shorter than the duration of an action potential. This passive event enables the passive spread of an action potential along the length of the fiber. The normalized values of the space constant for a giant squid axon are 10 fold less than the necessary value. Myelinated fibers do not propagate action potentials.
  • #36
The two figures are linked and give us many lessons?
 
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  • #37
somasimple said:
I do not agree with theory but accept facts.
I also accept the facts, but I agree with the theory. Your disagreement with the cable theory is irrational since you have not yet demonstrated that the accepted facts contradict the theory. However, you are certainly free to have irrational opinions.
 
  • #38
DaleSpam said:
I also accept the facts, but I agree with the theory. Your disagreement with the cable theory is irrational since you have not yet demonstrated that the accepted facts contradict the theory. However, you are certainly free to have irrational opinions.

https://www.physicsforums.com/showpost.php?p=1874067&postcount=14
Where is the propagated delay within these graphs?
 
  • #39
somasimple said:
https://www.physicsforums.com/showpost.php?p=1874067&postcount=14
Where is the propagated delay within these graphs?
It is always hard to understand your plots since you never label anything and never describe your derivation. But from what I can guess (assuming you are doing everything correctly) you are modeling the cable equation response to a square pulse current input. If so, you correctly note that the cable model predicts that there is no delay between the "near" and "far" measurements, and also the cable model predicts that there is a decreasing amplitude between the "near" and "far" measurements.

This is in agreement with the measured experimental data (aka facts) as shown in http://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pubmed&pubmedid=16991863" . Note in the upper part of fig 7 how the amplitude decays between nodes of Ranvier; this fact agrees with the cable theory. Note in the lower part of fig 7 how there is no measurable propagation delay between the nodes of Ranvier; this fact also agrees with the cable theory.
 
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  • #40
This figure 7 is the proof I need.
It shows at nodes a quite stationary speed (quite = 0)
And a very high speed during under myelin.
Unfortunately, the AP shape remains quite the same.
As we said the AP duration is 0.5 ms (Huxley shows 0.3 but shrinks the curves by computation).

So we have, during a single AP, a speed that varies with a shape that do not!
They recorded the same duration! It is a fact.

You may replace the AP by a train.
Put three observers at Node 1, A1, in the middle of the internode, A2 and then at Node2, A3.

A1 sees the train normally at speed 23 m/s and the observation duration is 0.5 ms.
A2 sees the train normally at speed >> 23 m/s and the observation duration is 0.5 ms.
A3 sees the train normally at speed 23 m/s and the observation duration is 0.5 ms.

You violate some laws of physics for sure. A2 can't see the train during 0.5 ms.
 
  • #41
somasimple said:
So we have, during a single AP, a speed that varies with a shape that do not!
They recorded the same duration! It is a fact.

You may replace the AP by a train.
Put three observers at Node 1, A1, in the middle of the internode, A2 and then at Node2, A3.

A1 sees the train normally at speed 23 m/s and the observation duration is 0.5 ms.
A2 sees the train normally at speed >> 23 m/s and the observation duration is 0.5 ms.
A3 sees the train normally at speed 23 m/s and the observation duration is 0.5 ms.

You violate some laws of physics for sure. A2 can't see the train during 0.5 ms.

An observer at a single point cannot measure a speed. We must have observers at at least two points to measure a speed. So two observers in the internode will measure a higher speed than two observers who are placed several nodes apart.

I think it's quite ok for a shape to remain constant while the speed changes - like a car - it can accelerate and decelerate but its shape remains the same.
 
  • #42
I think it's quite ok for a shape to remain constant while the speed changes
No it is not possible at all.
If the length of the train is well defined then the duration of its observation must be shortened with speed.

A train isn't elastic at all. The cable theory expects the contrary but fig 7 denies it. You can't have a portion of a train that runs at 23 m/s then some wagons that runs at a higher speed and finally some others at the original speed.
 
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  • #43
somasimple said:
No it is not possible at all.
If the length of the train is well defined then the duration of its observation must be shortened with speed.

A train isn't elastic at all. The fig 7 expects the contrary. You can't have a portion of a train that runs at 23 m/s then some wagons that runs at a higher speed and finally some others at the original speed.

In your rough calculation, you calculated that APs must exist simultaneously over several nodes of Ranvier. The time window you used in that calculation was 1 ms, and depended on AP duration and speed. The data in Huxley and Stämpfli show that your calculation was good.

I think the next step should be to try to think of it on a finer time scale. Referring to Huxley and Stämpfli's Figure 6, you will see that in fact the simultaneous APs in the 1 ms window are not strictly simultaneous. At any instant of time, they are all at slightly different phases of their time course. So there is only a single AP propagating down the axon when you conceive of it on a fine time scale. So it is not like a train and and many wagons, it is really just like a single car.
 
  • #44
They are in line (arranged in a linear fashion) but the traveled distance is different at node vs internodes.
I'll bring a better graph.
 
  • #45
somasimple said:
They are in line (arranged in a linear fashion) but the traveled distance is different at node vs internodes.
I'll bring a better graph.

If it's a single action potential I don't see the problem. A single car can accelerate and decelerate any way it wants.

Which part is problematic? Do you think it's not a single AP? Or do you think a car cannot accelerate and decelerate any way and still stay the same shape?
 
  • #46
Which part is problematic?
The duration of the AP that remains constant.

A single car can accelerate and decelerate any way it wants.
You can't see these things during the same event (the first AP) since you observe a low speed at nodes and a fast at internodes. There is no interruption during the observations.

Here you're abused by the apparent velocity (23 m/s).
 
  • #47
A single car can accelerate and decelerate any way it wants.
Yes and no. You need transitions between speeds. You have not any transition in that cases.
 
  • #48
somasimple said:
The duration of the AP that remains constant.

Good point. The car analogy doesn't work.

Cable theory predicts that the AP should change shape while traveling in the internode - it should get smaller, and its peak should become broader. I wonder why we don't see that in the data. Is the change simply too small to see?

Edit: looking at Fig 7, lower panel, comparing trace A and C from distance 1 mm to 7 mm, they are not exactly parallel, so there is some change in shape.

Edit: Also the top panel of Fig 7 shows that the peak changes in the internode. However it is maximum at the centre - not my naive expectation - what's their explanation?
 
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  • #49
somasimple said:
This figure 7 is the proof I need.
It shows at nodes a quite stationary speed (quite = 0)
And a very high speed during under myelin.
Unfortunately, the AP shape remains quite the same.
As we said the AP duration is 0.5 ms (Huxley shows 0.3 but shrinks the curves by computation).

So we have, during a single AP, a speed that varies with a shape that do not!
They recorded the same duration! It is a fact.
You are clearly mistaken about http://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pubmed&pubmedid=16991863" showing that the shape of the AP is not changing. For example, in the bottom part of the figure note that at t = 0.55 ms the peak voltage (line B) is uniquely located at position d = 1 mm. In contrast, at t = 0.6 ms the peak voltage (line B) is simultaneously at all points from d = 1 mm to d = 3 mm. That is a definite change in shape, and this idea is repeated throughout the bottom part of fig 7.

I don't know what irrational bias against these models causes you to misunderstand the facts so eggregiously.

somasimple said:
You may replace the AP by a train.
Put three observers at Node 1, A1, in the middle of the internode, A2 and then at Node2, A3.

A1 sees the train normally at speed 23 m/s and the observation duration is 0.5 ms.
A2 sees the train normally at speed >> 23 m/s and the observation duration is 0.5 ms.
A3 sees the train normally at speed 23 m/s and the observation duration is 0.5 ms.

You violate some laws of physics for sure. A2 can't see the train during 0.5 ms.
The action potential is an electrical signal, not some massive rigid object like a train or a car. If you understood the data at all it would be clear to you that the shape does, in fact, change. It is not a massive body that resists acceleration (so you see saltatory conduction) nor does it resist deformation (so you see shape changes). The whole point of saltatory conduction is that the AP jumps and does not move at a steady speed like a train.

Get your facts correct.
 
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