What happens to the Na+ ions during an action potential?

AI Thread Summary
During the rising phase of an action potential, Na+ ions enter the cell through open sodium channels, leading to a temporary positive shift in membrane potential. Afterward, these sodium channels become inactivated, and potassium channels open, allowing K+ ions to flow out, which helps restore the original negative membrane potential. The Na+/K+ ATPase pump is not involved in the action potential itself but is crucial for maintaining ion gradients post-event. Additionally, chloride ions play a role in stabilizing membrane potential by moving against their concentration gradient when the membrane becomes too negative. Overall, the action potential is a complex interplay of ion movements facilitated by voltage-gated channels, with small ion currents resulting in significant changes in membrane potential.
  • #51
Andy Resnick said:
I think Rod would be rather upset to hear his work so misrepresented- ion channels do not pass water. Read the history of aquaporin: prior to the discovery of the water channel, it was assumed that water diffused through the lipid bilayer.
http://nobelprize.org/nobel_prizes/chemistry/laureates/2003/mackinnon-lecture.pdf
Prof R Mac Kinnon said:
The K+ ion pair could diffuse
back and forth between 1,3 and 2,4 configurations (bottom pathway), or
alternatively an ion could enter the filter from one side of the membrane as
the ion-water queue moves and a K+ exits at the opposite side (the top pathway).
Movements would have to be concerted because the filter is no wider
than a K+ ion or water molecule.
I think too.
 
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  • #52
  • #54
Well, now, I'm a bit more confused at this point. Probably should have paid more attention in cell bio way back when...

somasimple said:
The dynamics involved in a single realistic channel is far out of our computation possibility.
A single channel is unable to grasp the whole process, they work in a "collective" manner.
You need to simulate art least thousand and thousand of ions channels: I'm unable to do such a magical trick.

OK, am I correct in understanding this as follows – the behavior of a particular single ion channel is dependent on its environment in the membrane, namely surrounded by many other ion channels? That is, there is some sort of collective behavior among many ion channels that is not observable by single channel studies, where a single ion channel of interest will have noticeable differences in its behavior whether it's alone or if it's surrounded by many other ion channels. This sounds perfectly reasonable to me in principle, but then I have to wonder something. It was stated earlier that

somasimple said:
You're focused by results that are computations of integrations. That makes very good average values but... Averages are averages.

Ions cross membranes through ions channels! Do you expect that every ion get the same chance or velocity in this process?

If the important behavior to consider is of a collective nature (see the first quote in this post), why would it be important that not every ion might pass through the ion channel in exactly the same manner? You're interested in the collective effect of many ions passing through many ion channels, not just one ion through one ion channel. And why would it matter then that the Hodgkin-Huxley theory is one of averages and macroscopic/whole-cell behavior, and not single ion channels? Wouldn't it be rather appropriate then, as it describes (I'm figuring) the collective effect of many ion channels, which – according to the quote I have at the start of this post – is preferable to just focusing on a single ion channel which does not capture the full complexity of the process?

I understand the difficulties in carrying out large-scale biological simulations of membrane proteins and their surrounding lipid environment. However, I'm thinking that if the important effects only arise in the limit of thousands of ion channels (BTW, how firm of a limit is this threshold? Can you capture the emergence of collective effects for an ion channel surrounded by, say, 50 to 100 ion channels?), maybe a coarse-grained model based on more detailed single ion channel studies might be appropriate. That is, you plug the data/results from the best simulations you can run on a single channel into some sort of simulation where you're looking at a less-detailed array of many ion channels. I know people have done molecular dynamics studies on systems such as KcsA where they've simulated some of the bilayer and solvent, but I have the impression that sort of work is not directly relevant to the questions at hand.

Andy Resnick – Thank you for the response regarding single-channel patch clamping. It is greatly appreciated.
 
  • #55
I feel you're irritated there, Andy.

I do not "sustain" at any moment the content of your link.
Please, avoid the confusion.
I'm speaking about well known water bonds...
 
  • #56
somasimple said:
http://nobelprize.org/nobel_prizes/chemistry/laureates/2003/mackinnon-lecture.pdf

I think too.

Ok, now we are getting somewhere. Again, this discussion would be a lot more efficient if you would simply put your ideas out there first, rather than requiring extensive back-and-forth to try and deduce your ideas.

From:

http://www.nature.com/nature/journal/v414/n6859/full/414023a0.html

'The structure sketched out the molecular basis of this specificity: a narrow 'selectivity filter' in the shape of an oxygen-lined electronegative tunnel in which dehydrated K+ (but not Na+) fits precisely. This structure rationalized why a K+ ion is so willing to leave its thermodynamically comfortable home in aqueous solution to enter the pore in a largely dehydrated form; the channel interior mimics the embrace of the water molecules in the inner hydration shell surrounding the ion in solution.

[...]

'Potassium ions are now seen in seven distinct sites along the pore-axis (Fig. 1a). Four of these reside in the narrow selectivity filter, and one in the wider hydrated cavity, as described earlier. By solving structures at varying ion concentrations, MacKinnon and colleagues argue that the four selectivity-filter sites are not all occupied simultaneously; rather, a pair of K+ ions separated by a single water molecule shifts in a concerted fashion between two configurations within the filter — inner and outer — occupying each about half the time (Fig. 1b).

[...]

'Most dramatically, in the position closest to the pore entrance a K+ ion is caught in flagrante, coordinated in front by four protein carbonyl groups reaching outwards, and behind by solvent; this must represent the long-postulated 'dehydration transition state' in which the ion sheds its water while entering the pore. It is now seen not to be a high-energy transition-state at all, but rather a true intermediate, an integral part of the flat landscape.'

This is all well and good, but I don't what this has to do with Sodium channels, which you consider to be the sole driver of an action potential spike, nor does it have to do with 'collective behavior' of thousands of channels, nor does it have anything to do with properties of lipid bilayers.

Consequently, now it's entirely unclear exactly *what* question you are trying to answer; we started with a discussion of the electrical dynamics of an action potential, to talking about sodium channel dynamics, and now you are discussing potassium channels.

Please take a moment to write out a coherent post discussing *your ideas*. Because right now I feel like I am chasing a moving target.
 
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  • #57
Mikz,

Some numbers about the original experiments on the giant squid axon;

1/ its diameter is 0.5 mm => 500 µm
2/ its speed is 20 ms-1
3/ Action potential length is 40,000 µm => 40 mm.
4/ Surface of this patch is 62,800,000 µm²
5/ it contains 20,700,000,000 ions channels
6/ its circumference is 1,571 µm
7/ this circumference has an average of 28,535 ion channels.
8/ each slice of 1 µm contains 518,000 ions channels.

I said thousand and thousands...

Andy, you're picky there. We know that membrane has K and Na channels.
 
  • #58
Ionic contrast terahertz near-field imaging of axonal water fluxes.

Masson JB, Sauviat MP, Martin JL, Gallot G.

Laboratoire d'Optique et Biosciences, Ecole Polytechnique, Centre National de la Recherche Scientifique Unité Mixte de Recherche 7645, Institut National de la Santé et de la Recherche Médicale U696, 91128 Palaiseau, France.

We demonstrate the direct and noninvasive imaging of functional neurons by ionic contrast terahertz near-field microscopy. This technique provides quantitative measurements of ionic concentrations in both the intracellular and extracellular compartments and opens the way to direct noninvasive imaging of neurons during electrical, toxin, or thermal stresses. Furthermore, neuronal activity results from both a precise control of transient variations in ionic conductances and a much less studied water exchange between the extracellular matrix and the intraaxonal compartment. The developed ionic contrast terahertz microscopy technique associated with a full three-dimensional simulation of the axon-aperture near-field system allows a precise measurement of the axon geometry and therefore the direct visualization of neuron swelling induced by temperature change or neurotoxin poisoning. Water influx as small as 20 fl per mum of axonal length can be measured. This technique should then provide grounds for the development of advanced functional neuroimaging methods based on diffusion anisotropy of water molecules.

PMID: 16547134 [PubMed - indexed for MEDLINE]
 
  • #59
Is the mobility of the pore walls and water molecules in the selectivity filter of KcsA channel functionally important?

Kraszewski S, Yesylevskyy SO, Boiteux C, Ramseyer C, Kharkyanen VN.

Institut UTINAM, Laboratoire de Physique Moléculaire, UMR CNRS 6213, Faculté des Sciences et Techniques, Université de Franche-Comté, 16 route de Gray, 25030 Besançon Cedex, La Bouloie, France.

We performed in-depth analysis of the forces which act on the K(+) ions in the selectivity filter of the KcsA channel in order to estimate the relative importance of static and dynamic influence of the filter wall and water molecules on ion permeation and selectivity. The forces were computed using the trajectories of all-atom molecular dynamics simulations. It is shown that the dynamics of the selectivity filter contributes about 3% to the net force acting on the ions and can be neglected in the studies focused on the macroscopic properties of the channel, such as the current. Among the filter atoms, only the pore-forming carbonyl groups can be considered as dynamic in the studies of microscopic events of conduction, while the dynamic effects from all other atoms are negligible. We also show that the dynamics of the water molecules in the filter can not be neglected. The fluctuating forces from the water molecules can be as strong as net forces from the pore walls and can effectively drive the ions through the local energy barriers in the filter.

PMID: 18404233 [PubMed - indexed for MEDLINE]
 
  • #60
somasimple said:
Mikz,

Some numbers about the original experiments on the giant squid axon;
<snip>

Andy, you're picky there. We know that membrane has K and Na channels.

Really...

somasimple said:
Hi All,

It is a fact that Na+ ions cross the membrane and enter the cell during the rising phase of the action potential. The process happens because Na ions channels are open.
Then the ions channels becomes inactivated/closed for a while.

What happens to the Na+ ions that entered the cell?

somasimple said:
I fully accept this explanation but if the rising is done by an influx then the decay must be done the same way in opposite direction (efflux) but all papers speak about Na ions channels inactivated or closed.
How is it possible to get a rapid decay when gates are closed?

somasimple said:
Well,
the K conductance is lower than the Na one and the number of K channel is 10 time lower than the Na one.
How is it possible that in quite the same time (because you excluded all other ions species) the voltage decays like it grew...quickly (but Na ions are confined inside and Na channels closed or inactive)?

somasimple said:
Cincinnatus,

I ask questions that seem important for the science community and it seems true that often I do not get any response. That is strange. I pointed out some basic violations of physics laws and the "faulty" drawings were removed from wikipedia because my argument was sufficiently strong.

<snip>

The theory must be refined. I have a theory that explains the fact, have you one that may explains this?
<snip>

somasimple said:
You're welcome.

A theory that explains the underlying mechanisms of:
  • refractory periods
  • propagation without "passive spread"
  • inactivation of Na channel
  • branching, acceleration...

and respects facts and laws of physics may be of some interest?


This is not really a discussion anymore- please put forth your ideas in a coherent manner now.
 
  • #61
This marvelous membrane capacitor.
A single cm² that carries 1µF. That is clearly extraordinary and may make a furious envy to many electronics suppliers.

Most of natures inventions are far superior to our own in design, function, and economy. Let's face it, God (or if you prefer, "Random Mutation Man") is simply a better engineer than we are.

Please take a moment to write out a coherent post discussing *your ideas*. Because right now I feel like I am chasing a moving target.

I noticed a post or so ago that it seemed as if the target of the debate isn't always the same thing. I don't think the conversation is exactly moving in circles though, the randomness of the conversation has definitely increased from page to page indicating that the conversation is evolving in a quite natural way.

Of course, I should mention at this point that I DO have a bottle of special mineral water for sale if anyone is interested...
 
  • #62
The chase is prohibited. I belong to a protected specie.
Unable to give the results about simple experiments? Some reasonable doubt insinuated into your mind?
Perhaps you need some more:
Did they remove the ions channels when they measured the membrane capacitance? No, because they didn't know they were there. But you know it!
Electroneutrality: Even Roderick MacKinnon is aware of ions hydration (just see the pictures provided in the Nobel Lecture). That makes a big problem to a polarized membrane as a capacitor since you must solve its boundaries limits: Does the violation stops at 0.5 nm, more, less but how? What is the effect of hydration on charged particles?

Please forget your cynicism and re-adopt a scientific profile: examine the facts and conclude by yourself.
 
  • #63
somasimple said:
Did they remove the ions channels when they measured the membrane capacitance? No, because they didn't know they were there. But you know it!
Why do you think the presence or absence of the ion channels would significantly change the capacitance of a membrane?
 
  • #64
Capacitance was measured with voltages/currents and there is voltage gated ions channels embedded in membrane.
 
  • #65
So what? That would change the conductance, not the capacitance. Conductance is a current which is proportional to a voltage, capacitance is a current which is proportional to the derivative of a voltage.
 
  • #66
And does a capacitor have latency? :biggrin:
So what?
And our conductances aren't linear at all!
 
  • #67
Your statement is unclear. The conductance of the membrane is a non-linear function of time and voltage. But conductance itself is a linear relationship between voltage and current. Do you understand the distinction? If not I will try again since I know there is some language barrier.

Also, what is the relevance to measuring the capacitance?
 
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  • #68
somasimple said:
This marvelous membrane capacitor.
A single cm² that carries 1µF. That is clearly extraordinary and may make a furious envy to many electronics suppliers.
By the way, this is rather silly. We make phospholipid bilayers synthetically all the time and they regularly approach this capacitance. In fact, the capacitance is used as an easy metric to test the quality of the synthetic membrane.

Electronics suppliers are in no way furious or envious. They know about this technology and could generate as much phospholipid membrane as they like. The reason they don't is because such capacitors would be rather delicate and temperature sensitive as well as having low maximum-voltage ratings.
 
  • #69
I understand clearly the differences but I do not understand why you refuse to reply to previous questions and give results from experiments that costs less than 1$ each.

OK, let's suppose that membrane is a capacitor:
1/ Where are the metal planes?
2/ Where are the wires?
3/ In a capacitor, current flows through wires and circuit, is it the same with membrane?
4/ In a capacitor, dielectric insulates the two metal plates. In membrane, dielectric allows the whole currents fluxes, why?
5/ In a capacitor current is made from electrons, is it the same?
6/ In a capacitor, the distributed charges are symmetric, is it the same?
7/ in a capacitor, exchanges occur exclusively (except leakage current) through wires and are vertical, how are you able to enable also (in propagation) a transversal one and what rules does it follow?
8/ In your schematic, capacitor is associated with ions channels (resistances). Since wires are in both cases situated in the "capacitor plates", how do you connect them?
9/ since AP requires only a tiny 0.04 % of available ions, why do they choose to be associated to their far neighbors from the right or the left since there is closer ones just under their entry point?
 
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  • #70
Perhaps the last question is a bit rude, sorry: You have to work around the well known electric law: current always takes the path of least resistance. (Of course, you may find an alternative explanation that may explain that laws may be violated... (sic)).
http://en.wikipedia.org/wiki/Path_of_least_resistance
 
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  • #71
somasimple said:
current always takes the path of least resistance.
This is a commonly-repeated phrase, but it is not true. Current always takes all paths.

somasimple said:
give results from experiments that costs less than 1$ each.
I have no idea what you are trying to say. Why should an experiment cost less than $1?

somasimple said:
OK, let's suppose that membrane is a capacitor:
1/ Where are the metal planes?
2/ Where are the wires?
In an electronic circuit the charge carriers (electrons) are are free to move in the metal. In the neuron the charge carriers (cations) are are free to move in the electrolyte. The electrolytical fluid takes the place of the metal.
somasimple said:
3/ In a capacitor, current flows through wires and circuit, is it the same with membrane?
Yes. However there is also leakage current which occurs across the membrane as well as in commercial capacitors
somasimple said:
4/ In a capacitor, dielectric insulates the two metal plates. In membrane, dielectric allows the whole currents fluxes, why?
What do you mean?
somasimple said:
5/ In a capacitor current is made from electrons, is it the same?
No, the charge carriers are primarily cations as I mentioned above.
somasimple said:
6/ In a capacitor, the distributed charges are symmetric, is it the same?
Yes.
somasimple said:
7/ in a capacitor, exchanges occur exclusively (except leakage current) through wires and are vertical, how are you able to enable also (in propagation) a transversal one and what rules does it follow?
Please try again, there is a language problem and I didn't understand what you are asking. What are you trying to say with the word "vertical"?
somasimple said:
8/ In your schematic, capacitor is associated with ions channels (resistances). Since wires are in both cases situated in the "capacitor plates", how do you connect them?
No, the capacitor represents the capacitance of the membrane. The resistors represent the concudtance of the ion channels. And the batteries represent the Nernst potential of the bulk concentration gradients.
somasimple said:
9/ since AP requires only a tiny 0.04 % of available ions, why do they choose to be associated to their far neighbors from the right or the left since there is closer ones just under their entry point?
What do you mean by "associated to"? And what do you mean by "under their entry point"? Is this somehow related to the "vertical" from above?

Please try to take things slowly. Your questions don't seem to be unanswerable, but there is a considerable language barrier. I know it is hard to express things in a forigen language, and your English is much better than my French, but even so it is probably better to spend the effort to make one clear major question than to make 9 confusing or minor questions.

In any case, the bottom line is that the HH model works quite well. You are certainly free to propose a model which works even better, but in the absence of a better model it is somewhat silly to object so strenuously to this one.
 
  • #72
This is a commonly-repeated phrase, but it is not true. Current always takes all paths.
I will reply to the first statement because the subsequent responses will be useless if you do not solve this one.
Yes, current flows in all paths but prefers the least resistances.
So you admit the situation but I said I wasn't kind and it was a rude question.

So we said that entering ions are associated with their opposite counterions. The most of them are just under and some will make the job onto the right and onto the left.

NO! It can't work at all.

If I accept that a ion is associated in the internal milieu of the cell, I must also accept it was also the case, outside. That makes a big problem. You must, now, consider, that ions were also associated, outside.

Then, you must also fill the gap of initial conditions (IC); A solution where energy is low and where the model may function.
Of course, there is one with the hypothesis:
All ions are associated, on each side!
You solve the problem of electronegativity but you may encounter some bigger ones:
You have now salt crystals on each side of the cell.
Bad new for diffusion and too bad for currents: It is also a well known thing that crystals are effectively neutral but very good... insulators for the same reason.

This point of view has not my preference: I prefer water bondings for salts...
 
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  • #73
somasimple said:
I will reply to the first statement because the subsequent responses will be useless if you do not solve this one.
Yes, current flows in all paths but prefers the least resistances.
I don't like using human psychological terms like "prefers" to describe inanimate objects. I would say that current goes through all paths, but more current goes through the path of least resistance than through the other paths. This makes it clear that current is going through all paths and still covers the essence of the "path of least resistance" concept.
 
  • #74
The criticism is well received but the model remains still invalid.
 
  • #75
somasimple said:
NO! It can't work at all.

If I accept that a ion is associated in the internal milieu of the cell, I must also accept it was also the case, outside. That makes a big problem. You must, now, consider, that ions were also associated, outside.

Then, you must also fill the gap of initial conditions (IC); A solution where energy is low and where the model may function.
Of course, there is one with the hypothesis:
All ions are associated, on each side!
You solve the problem of electronegativity but you may encounter some bigger ones:
You have now salt crystals on each side of the cell.
You still haven't explained about what you mean by "associated".

I don't understand how you make the completely random jump to salt formation. It is certainly not based on any understanding of correct physics. Do you understand how a salt crystal dissolves or forms in a good polar solvent like water?

somasimple said:
Bad new for diffusion and too bad for currents: It is also a well known thing that crystals are effectively neutral but very good... insulators for the same reason.
I am sorry, but you are completely mistaken. Do you understand what it means for a salt solution to be an electrolyte? It means precisely that you get both ionic currents and diffusion even even with both cations and anions present in the solution. This isn't even a biological phenomenon, it is simple high-school level chemistry. The concentrations are way to low to get salt formation, and there is diffusion and electrical conduction via ionic currents.
 
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  • #76
somasimple said:
The criticism is well received but the model remains still invalid.
No it is not invalid. It fits a wide range of experimental data within its domain of applicability. That is all that is required to validate a scientific model. I am having a hard time following your objections, but the simple fact remains that the HH model works. Therefore it is valid. End of story.

If you make any model (it doesn't have to have any physical inspiration as the HH model does), propose a hypothesis based on the model, perform the experiment, and get data supporting the hypothesis, then the model is validated. That is the nature of science.

As you perform more experiments you may get some experiments that don't match the model. Then you learn the limits of the domain of applicability for the model. That still doesn't make the model invalid within its already scientifically validated domain.

Some later person (like yourself) may come up with a better model that fits all the data including this new domain and, if the new model is valid, it must agree with the old model within the old model's limited domain. Such is the nature of the scientific method.
 
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  • #77
I do not understand how you produce an equal charge of opposite sign when you move (i.e) a Na+ ion from outside to inside.

My attempt was clearly silly as the model.
Perhaps you think that Na+ let's a "free" electron on the opposite side?
 
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  • #78
More simply,

with a simple example: KCl and water with a semi permeable membrane to K+. (High school).

IC:
The KCl is on the left (membrane at center).

Terminal conditions:
  1. Some K+ ions are at right and
  2. membrane is now polarized (becomes a capacitor).

Problem:
Describe how you obtain the second result?
 
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  • #79
  • #80
somasimple said:
I do not understand how you produce an equal charge of opposite sign when you move (i.e) a Na+ ion from outside to inside.

My attempt was clearly silly as the model.
Perhaps you think that Na+ let's a "free" electron on the opposite side?
No, in an electrolyte the primary charge carriers are dissolved ions. However, I don't understand why you think moving an ion from one side to the other should "produce" an equal charge of opposite sign. Since the electrolyte is, in bulk, electroneutral you know that there is already an anion in solution for every cation. So no anion needs to be produced, they already exist in the solution.

somasimple said:
KCl and water with a semi permeable membrane to K+. (High school).

IC:
The KCl is on the left (membrane at center).

Terminal conditions:
  1. Some K+ ions are at right and
  2. membrane is now polarized (becomes a capacitor).

Problem:
Describe how you obtain the second result?
Do you know the concept of http://en.wikipedia.org/wiki/Amperes_Law" to be useful. This is a very fundamental set of concepts that apply to many different systems, not just neurons. So I would most strongly encourage you to study this until you understand how the second result happens, but you will probably need to branch out beyond the links I have provided. Please, familiarize yourself with the fundamental concepts and post any follow-up questions that you have.
 
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  • #81
I know you consider that I'm an idiot.
Consider that I'm stubborn, too!

I'm now facing with a strange behavior from your own: Every time we're close to get, at last, a reply, you change abruptly and bring a ton of useless material that has nothing to see with the current question.

So, I'll restate one more time my simple "virtual" and well known experiment:

Two compartments are separated by a semi-permeable membrane oriented to the "water" side (semi permeable for K+).
IC:
compartment one contains water.
compartment two is filled with a solution of KCl (potassium chloride). Concentration doesn't matters but we will take 40 mM.
The membrane capacitor is supposed discharged, right?
http://nerve.bsd.uchicago.edu/rp1.htm

Then,
At a time t1, since some K+ have moved and now, the membrane must carry some charges since we have a potential difference?

Please describe the charges carried on each side (if needed) of the membrane that explains it functions as a capacitor and maintains charges?
Hope the question is sufficiently clear?
 
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  • #82
It doesn't matter how many of his questions that you answer. He doesn't think there's something in particular wrong with our understanding of action potential generation / propagation in neurons. Instead he's sure that the theory is wrong for a priori reasons and will keep changing the subject until you get tired of arguing with him.

If you google him you'll see that he's done the same thing on many fora including this one several other times. It's really pretty useless to keep answering his questions as he's never going to stop and say "oh I get it now".

Somasimple, why don't you just explain your theory? (in the IR forum here) It may well be that you can explain the data as well as or better than the Hodgkin-Huxley model (and it's extensions). Why not let us judge your hypothesis in the only way hypotheses can be, by testing them with real data.

Until then, the fact remains that the Hodgkin-Huxley model is very very good at making testable predictions and works better than any other model we currently have. This alone is reason enough to think that the model is at least a good approximation to the truth.
 
  • #83
Cincinnatus,

The same answer may apply to you. Are you unable to describe the thing?
 
  • #84
If you google him you'll see that he's done the same thing on many fora including this one several other times.
And I got, every time, different explanations. :confused:

Until then, the fact remains that the Hodgkin-Huxley model is very very good at making testable predictions
We are currently testing the initial conditions of this model and you refuse to explain the next mandatory step of its functionning. :confused:

Somasimple said:
Then,
At a time t1, since some K+ have moved and now, the membrane must carry some charges since we have a potential difference?

Please describe the charges carried on each side (if needed) of the membrane that explains it functions as a capacitor and maintains charges?
Hope the question is sufficiently clear?
Giving a good answer is the best way to smash me down!
Come on, it's my pleasure.
 
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  • #85
somasimple said:
I'm now facing with a strange behavior from your own: Every time we're close to get, at last, a reply, you change abruptly and bring a ton of useless material that has nothing to see with the current question.
It has everything to do with the current question. If you understood the principles I linked to then you would understand capacitors and how a membrane acts as one, as well as how a potential difference can be established by a chemical gradient. I take it then that you did not even bother to read what I provided.

somasimple said:
So, I'll restate one more time my simple "virtual" and well known experiment:

Two compartments are separated by a semi-permeable membrane oriented to the "water" side (semi permeable for K+).
IC:
compartment one contains water.
compartment two is filled with a solution of KCl (potassium chloride). Concentration doesn't matters but we will take 40 mM.
The membrane capacitor is supposed discharged, right?
http://nerve.bsd.uchicago.edu/rp1.htm

Then,
At a time t1, since some K+ have moved and now, the membrane must carry some charges since we have a potential difference?

Please describe the charges carried on each side (if needed) of the membrane that explains it functions as a capacitor and maintains charges?
Hope the question is sufficiently clear?
I will restate my answer. The concentration of K+ increases until it reaches the equilibrium potential described by the http://en.wikipedia.org/wiki/Goldman_equation" across the membrane shows that it must carry equal and opposite charge density on each side. Obviously, since the charge carriers in this electrolyte are K+ and Cl-, the charges will be K+ on one side and Cl- on the other.

I hope the answer is sufficiently clear. If you have some specific question about one of the above physical principles, please don't hesitate to ask. If you merely have another rant about HH not being valid, please back it up with some experimental data that HH fails to explain and present your alternative which does explain it.

Your failure to understand HH and the underlying principles is not a valid criticism.
 
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  • #86
For the lurkers following this thread, the Goldman equation which DaleSpam refers to in the previous post is the same as the equation we had been calling the GHK (Goldman-Hodgkin-Katz) equation earlier in this discussion. It is a variant of the Nernst equation which may be more familar to some people...

Anyway, somasimple doesn't seem to accept the GHK equation as applied to biological membranes...
 
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