Alison's New App is now available on iOS and Android! Download Now

Module 1: Neuronal Biophysics

Study Reminders
Text Version

Set your study reminders

We will email you at these times to remind you to study.
  • Monday




























Hello in this session we will examine the ionic basis of the Action Potential in excitable cells, specifically neuronal cells. There are other excitable cells in the body, electrically excitable muscle cells, cardiac cells but we are talking about neuronal cells. So, the background we learned in the previous lectures that the resting membrane potential of a cell is about minus 60 mill volts in this squid joint axon, and it can be even lower than that in mammalian neurons. So, the resting membrane potential V subscript m when it changes from minus 60 to minus 55 that is depolarization happens then all get excited.

Now, it has to reach a threshold. So, the threshold is about 15 to 20 millivolts and with that, you get a spike of 100 millivolts and at last for about 1 millisecond approximately. So, this is the action potential and the first thing is it is all-or-nothing so when the membrane threshold is reached then you have the spike. It is invariant and the information is coded in the frequency number of spikes that occurred, it's not coded in shape or form. So, this is the critical point to note that the information of an action potential is coded in its frequency and it is all-or-nothing so it occurs when the membrane potential reaches the threshold.

So, in 1938, Cole and Curtis showed this is in marine biological laboratory Woods Hole Massachusetts, they showed that during the action potential the membrane permeability or its conductance to various ions increases 40 times from normal. So, subsequently the next year Hodgins and Huxley showed that the membrane potential changes from minus 60 millivolts to plus 40 nearly 100 millivolt change during the upstroke of the potential. So, on the right, you see the impedance change during an action potential. So, the action potential is the thick black line and it is superimposed on the impedance data which is the grey band and you see during the time course of the action potential, the grey band increases substantially, and then it comes back to normal. This widening of this impedance band reflects a change in the membrane resistance from 1000 ohms per square centimeter, it drops to 25 ohms per square centimeter. Please note that the membrane capacitance does not change, it is a passive property depends on the phospholipid layer so that does not change. Now, how do you measure impedance?

Now, if you remember from your high school that is a concept of Weston bridge where you have four resistors and they are all balanced and then they are balanced the central galvanometer is at 0 so one of the arms of the Weston bridge is the impedance measurement from the squid so that tells us what the impedance changes are.

So, how do we explain these impedance changes? I mean what happens? Because it comes back to the baseline. So, these can be explained if the selective permeability to sodium is reversed for a brief period that is sodium penetrates much faster than potassium, this sodium influx causes the intercellular compartment to become positive briefly with respect to the extracellular environment. So, looking at their actual data and some of their data still unrivaled in its clarity and clearness you see traces so trace 1 and 3 is the action potential of the squid giant axon in normal seawater. In 2, the sodium outside one-third of it has been replaced with isotonic dextrose and you see the action potential is much smaller. 3 is when you replace it back and then it comes back to normal. So, when the extra-cellular sodium is lowered the action potential becomes smaller when its totally sodium free then there are no action potentials. So, the action potential, the initial part of it is completely sodium ion-dependent.

So, how do they prove it? That are actually from the membrane? So, this was referred to an earlier lecture so you take this squid giant axon and you actually have a small roller and you roll out the cytoplasm inside and then you re-perfuse it with whatever solution you want, it has your potassium solution and it does not really matter it could be any potassium solution as long as the ph is around 7.5. So, you can replace the intercellular fluid with solution potassium sulphate action potentials look practically the same as it were with regular intercellular contents. So, on the right you see that area where the top figure is action potentials from a squid axon per-fused with potassium sulphate, and below are action potentials from the intact squid giant axon.

Neuronal membranes can be represented as an electrical circuit, all you engineers would understand this. It was proposed by Hodgkin and Huxley in the 50s and here C subscript m is the capacitance of the nerve membrane usually it is put at one micro ferret per square centimetre. In the middle is the diagram of an excitable membrane of a nerve fibre. So, cm is the capacitance RNa is with its battery below is the sodium channel Rk the resistance subscript potassium is the potassium channel and these are the main conductances And you also have an r leak which is small conductance where things it is not a perfect compartment so things keep leaking out and there will be a small potential due to that.

So, the conducting pathways besides the capacitance they are represented by parallel channels because in the membrane with the phospholipids membrane, you have sodium channels, you have potassium channels, so each of these channels has a battery and a resistance, the battery is the electromotive force which pushes the ion into or outside the cell. So, at rest, the resistance for sodium is high which means, its reciprocal which we actually used rather than resistance which is g that is denoted by g which is the conductance is low compared to potassium.

So, let us analyse some electrical changes in axons during activity. First to recap the resting membrane potential of an axon is permeable to sodium but not solely permeable to, I am sorry, the resting membrane potential to the axon is solely permeable to potassium, it is not impermeable to sodium and is also permeable to chloride. So, the potential across such a membrane is given by the GHK field equation, where P is the permeability coefficient of each ion or the conductance. So, if we look at the equation it was we went through it in an earlier lecture. Instead of just potassium which gives us only the potassium ion affects, we also add in sodium and chloride and we call it a constant field equation because we assume that within the phospholipid membrane the potential is constant. So, when you put all these things aside then you get a realistic value of the resting membrane potential.

So, when the nerve membrane is depolarized by an outward flow of current so it becomes less negative inside, sodium permeability or g subscript Na rises immediately and sodium ions rush into the cell because of the concentration gradient, if you remember outside is seawater sodium is about 150, inside is about 18 to 20. So, it is huge rush of water rushing in our concentration gradient since water falling from a height you think of sodium ions. So, how does this occur, how does it depolarize? So, it can occurs in two ways, you can cause an outward current by applying a cathode or the adjacent segment or area has an action potential that action potential invades this segment and causes depolarization.

So, once sodium enters it lowers the membrane potential and causes further depolarization and then there is an explosive acceleration of sodium entry and that is the rising phase of the action potential, the cell inside becomes positive. It really nature reaches the equilibrium potential for sodium if you remember it is about plus 60 millivolts and if you see on the right you have the action potential, you have the intercellular electrode and that is in this squid giant axon.

So, then what happens is once it reaches the peak the net inward movement of sodium becomes 0 and that is the peak. So, the conductance of sodium stops, and sodium permeability falls. This is called sodium inactivation. And it reaches baseline in about 1 to 1.5 milliseconds.

So, what happens with potassium? So, at the peak of the spike, the potassium conductance rises, not with the sodium but a little delayed. It peaks about half a millisecond later and returns to normal in 3 milliseconds. After the generation of the action potential, the membrane potential repolarizes, becomes more negative and it goes below 0. So, here it comes down, and then it goes below 0. So, this is called hypopolarozation. It is gone below 0. This is depolarization and this is coming back to normal and this is hyperpolarization. And you know it is also called an after-hyperpolarization because it occurs after the action potential. Now, please bear in mind that a neuron can fire 60,000 to 90,000 times before it fatigues. So, it is very very efficient compared to all electronic devices and there is a lot of redundancy build in, these are huge safety margins. It fires because it losses energy and the energy has to be made up with the ATP phosphate transfer. But 60 to 90,000 times, is good to go.

So, now coming to the voltage clamp, we can measure from inside the cell, no problem. Why do we need to clamp the voltage? So, we do it to simplify the analysis. With the voltage clamp, we can measure current flow in a patch of membrane whose voltage 1 is maintained at a set level. This is called the command voltage or it can be changed stepwise using a feedback amplifier. So, you see the circuit on the right, you have a squid, you have a current passing electrode and then you have a signal generator with a command voltage and this is the kind of circuit that is used. We will get into details subsequently.

So, what is the advantage of the voltage clamp? So, remember potassium things are happening, the sodium things happening, voltages are happening and current is happening. So, this technique dissociates voltages and currents. So, we can hold the voltage constant and see what the current is or we can current clamp it and see what the voltage is. So, these techniques were developed by Kenneth Cole at MBLM, Massachusetts. And quickly, they were used by Hodgkin and Hugely in Plummet in Cambridge and they figure out the action potential with this technique. So, consider this circuit on the right, you have the axon, you have a current electrode and you have a voltage electrode. So, the idea is you keep the voltage constant and you see how much current passes at that particular voltage. And not only the amplitude but also the time course. So, in the two electrodes, the classic voltage-clamp technique, one electrode measures the voltage across the membrane while the other injects the current to keep the voltage constant.

So, the experimenter sets up the voltage where the axons should be held. This is the command potential. So, the current is then injected into the cell in proportion to the difference, the delta between the present membrane potential and the command potential. This occurs continuously, therefore, clamping the membrane potential to the command potential. So, by measuring the amount of current injected to hold it at the command potential, we can determine the amplitude as well as the time course of ionic currents following across the membrane.

So, the advantages. The current injected into the axon is equal to the current following through the iconic channels of the membrane. Remember, current in membranes is not electrons but ions, and therefore you get a direct measurement of this current at the particular voltage. So, ion currents, ionic currents, sodium, potassium are both voltage and time-dependent. They become active at certain membrane potentials and do so at a particular rate. So, keeping the voltage constant at the voltage clamp, allows these two variables to be separated. The voltage dependence and kinetics of these ionic currents can therefore be measured directly. This was not possible before, this technique. So, thank you and in the next session, we will consider more details of the action potential.

So, Hodgkin and Huxley, I keep talking about them. They were high of Neuro Physiology, Electro Physiology as. And you see, on the right, Hodgkin is on the extreme right and Andrew Huxley is on the left and the apparatus they use, you have a cathode ray oscilloscope, you have an operating microdissection microscope and then things to infuse an electrode to record so on and so forth.

So, Helan Hodgkin or Sir Helan Hodgkin and Sir Andrew Huxley, they found out how the action potentials are generated in the squid giant axon and it was remarkable to reforce when they did it because though a lot of evidence had been accumulating, they were the first to prove the actual mechanisms, physiologist. So, they used the voltage-clamp technique which was developed by Cannet Curl at Woods Hole in Massachusetts to find mechanisms of action potentials generation, the squid giant axon. So, this is one of the nice things about science that people collaborate and are very generous and share their techniques and advances occur. Axons and neurons have a threshold for the initialization of action potential. So, the resting membrane potential is about minus 60 millivolts and if it goes up depolarises goes to a 0 to about minus 45, you have an action potential.

So, increasing the voltage from minus 60 to 0, produces a large transient flow of positive charges into the current is called inward current. This is followed by a sustained flow of positive charges out of the current, out of the cell, and is called outward current. So, voltage clamping experiments by Hodgkin and Huxley demonstrated that the inward current is due to sodium ions flowing into the cell and the outward current is caused by potassium ions moving out of the cell.

So, these currents, the sodium current or the potassium current, typically they are denoted by I subscript Na for sodium a current, and I subscript K for potassium current. Now, they can be selectively blocked and this block does not affect the other ionic flows. The block occurs at the sodium channel, there is a sensitive area, it is kind of a lock and key mechanism and there is this chemical compound called Tetrodotoxin, a short name to TTX. Now, this is a very powerful poison that is found in the Japanese pufferfish. It is a delicacy, they eat it but they carefully remove the TTX before eating, but even so every year many people die in Japan of TTX poisoning because it blocks the sodium channels at microscopic concentrations 10 to the minus 5 molar, only sodium channels are blocked and it is reversible.

So, similarly, with potassium, you have specific channel blocks for potassium. It only affects potassium channels. It is called TEA, Tetra Ethyl Ammonium. So, if you consider the plots on the right, you have an inward current. Look at the central thick line, you have an inward current and followed by an outward current. This is during the action potential. Now, suppose, you replace the sodium outside and make it sodium free seawater, you do not have any inward current, but you still have the outward current. And in this panel on the extreme right, the plot above is where you have a TTX blocked happening and you have only the potassium currents and these are the different command voltages. It is a voltage clamp minus 15, 0, 15, 30, 45, 60. So, you see it occurs later. When you block the potassium channels with TEA, you only have the sodium current, the inward current and that is the panel below. And these are the command voltages of the voltage clamp minus 15, 0, 15, 30, 45. And it is very fast and comes back to normal quickly.

So, using TTX we can selectively isolate the potassium current and examine its voltage dependence here. And similarly, in TEA tetraethylammonium we do the same thing and look at only the sodium channels because as sodium currents because you have blocked the potassium channels. (Refer Slide Time: 5:35) So, these channel blockers show some fundamental differences between sodium and potassium channels. The inward, let us consider the potassium I mean the sodium currents which are below. So, you have an inward current and it occurs fast but also rapidly inactivates and is transient. It inactivates even when the membrane potential is 0. The potassium currents, on the other hand, take some time to occur, and then they are long-lasting. And that is why they are called delayed and it is also called a rectifier, delayed rectifier. When you hear the word, term delayed rectifier, you think of potassium currents. So, the sodium current both activates and inactivates rapidly. While the potential current only activates slowly like so over here.

And the potassium current, there is an interesting property, as long as the membrane potential is clamped at this particular voltage, it is activated. It keeps happening. And it does not inactivate, it is sustained. But the sodium channel is very different, it activates and deactivated fast and the interplay between these two processes causes the action potential.

So, at the time when they found this out, this physiological phenomenon, we were not sure, they were not sure, nobody was sure of what is the cellular mechanisms? What happens and the beauty of electrophysiology is you do not need to know to figure out what is happening, but if you want to go to the molecular level, you have to have some ideas. So, they speculate some kind of enzyme related activity, and that fit in. Subsequently, with molecular biology and the tools of molecular biology and structural chemistry, protein structure, we have now found that the sodium channel, there is a channel and it is sensitive to voltage and it inactivates and activates. And it is on the membrane.

So, these channels have a voltage-sensitive gate that opens with depolarization and closes with subsequent repolarization of the membrane potential. So, this process of turning on and turning off the potassium current is known as activation and deactivation. Simple enough. But the sodium channel is slightly different. It also exhibits voltage-dependent activation and deactivation, but the sodium channels become inactive also despite maintained depolarization, unlike the potassium channels. And on the right, you see the molecular structure, the postulated molecular structure of the sodium channels. It has 4 units and there is a place where TTX acts, Tetrodotoxin, and blocks it. And there is another blocker called saxitoxin similar to Tetrodotoxin blocks and below is the actual conformational, the biochemical. This would be the secondary, tertiary, and quaternary structures of the sodium channel.

So, channel activation and activation so the sodium channel not only activates and deactivates as mentioned earlier but also exhibits a separate process called inactivation, whereby the channels become blocked even though they are activated. So, removal of this inactivation is achieved by the removal of depolarization and is a process known as deinactivation. So, just to make it a little more complex, the sodium channels possess two voltage-sensitive processes; one is activation-deactivation and the other one is inactivation-deinactivation.

So, let us step back. Where is the action potential initiated generally? So, if you remember the microscopic lecture on the microscopic anatomy of the central nervous system, you have a cell. This is a pyramidal cell and you have all the dendrites which are not shown over here and then you have the axon going down covering myelin and stuff like that. Between the cell body, the soma, and the axon, there is a segment called IS, the initial segment. And that has a very high density of sodium channels compared to the rest of the soma and it is a very small compartment and it depolarises easily. So generally, action potentials are initiated in the initial segment and this is an electron microscopic image of the initial segment which is a kind of light red and hillock and the soma. The action hillock is where the initial segment begins and the initial segment ends where the axon with the myelination starts.

So, once a spike is initiated about 30 to 50 mu down the axon from the cell body in cortical pyramidal cells, this then propagates, so it moves. Now, it can move forward down the axon to the synaptic terminals where it causes the release of neurotransmitters or it can move backward antidromic. So, the first one is orthodromic where it moves forward. The second process where it moves backward is antidromic and it goes and into the cell body, into the cell dendrites and there it can modulate intercellular processes.

So, the refractory period. So, immediately after an action potential, for 1 millisecond, during that period, the cell is refractory. It will not be able to fire another action potential. This is because of the inactivated sodium channels. They have to recover. And regardless of the amount of current you gave, it will not be able to fire. So, this is the absolute refractory period of an axon.

The relative refractory period follows the absolute refractory period and here it is due to the there is after-hyperpolarization, the potassium channels act as a delayed rectifier. So, there is a continued outward diffusion of potassium. So, here is relatively refractory in the sense that if you use the same stimulus threshold to get the AP, that will not fire, but if you increase the stimulus current and you can force it to fire. So, the relative absolute refractory period is about 1 millisecond, the relative refractory period is about 2, 3, 4 milliseconds. It depends on the cell, but one is that this prevents the electrical activity from reverberating in an ensemble, in a network of neurons. Because otherwise, you could have reverberation occurring and if you have reverberation, then you have epilepsy. So, normally these processes prevent uncontrolled positive feedback reverberation from happening in the network. The other interesting thing is if you look at the absolute refractory period where it cannot be fired, that gives us an upper estimate of what is the maximum firing rate of a neuron. It has to be limited by the absolute refractory period. So, approximately over here. If it is 1 millisecond, and it would be the firing rate, the absolute firing rate of a neuron anywhere from 500 to 1000 hertz and that is it. It cannot be higher than that.

This speed of action potential is propagation is affected by myelination. So, axons can either be myelinated where they have a covering of myelin which is insulation, we will study this in detail. Or it can be unmyelinated where it just has a cell membrane but there is no myelin. So, sensory and motor neurons of the peripheral nervous system, they are myelinated by a special glial cell called a Schwann cell. So, this forms a spiral wrapping of multiple layers of its cell wall around the axon. And typically, small vertebrate axons, like for example, Sea fibers that absorb pain, and invertebrate axons are not myelinated. Whereas, large vertebrate axons are often myelinated. We will get into the details of the advantages of myelination in just a little bit.

So, in the peripheral nervous system, which is the part of the nervous system outside the brain and the spinal cord, several Schwann cells wrap around the axon along its length and leave small gaps in between the curl nodes, nodes of Ranvier. So, here on the right, you have a Schwann cell and it is wrapping its membrane around the axon, keeps wrapping it so you have multiple layers. And in between two different such wrappings, you have a node where the axon is exposed and it is called the node of Ranvier. So, these are all names of anatomist Ranvier Schwann so on and so forth. In the central nervous system instead of the Schwann cell, you have oligodendrocyte, which is a kind of glial cell and each oligodendrocyte typically ensheaths multiple axons, Schwann cell on the one axon and the periphery oligodendrocyte multiple axons. But otherwise, it is the same purpose and function insulates the axon.

So, we will study this a little more detail in neuronal biophysics, but for now, this myelination of axon reduces its membrane capacitance by moving the electrical charge differences between inside and outside further apart, therefore, reducing their influence on each other. And this significantly increases the passive length constant of the axon. We will, the length constant briefly is the distance where the electrical potential decreases to one to the eth of its initial value that is, 37 percent of its initial value. We will get into details more but this increases the length constant. And here you have the details. A cross-section of an axon with its myelin cell, the Schwann cell is with its myelination layers. The Schwann cell which produces myelination is outside and in between myelin layers, you have this node. It is about 2 mu, 2 microns. It is a node of Ranvier. And typically, the distance between I mean differs in different axons but the internodal distance is anywhere from 300 to 2000 micron which is 0.3 to 2 millimeters.

So, the sodium channels which allow the upstroke of the action potential, they are concentrated at the nodes. So, the generation of an action potential at each node causes depolarization of several adjacent nodes and subsequent generation of action potential with an internodeal delay of only 20 microseconds. This is referred to as salutatory conduction. Demyelination of axons causes conduction failure of action potentials. For example, multiple Sclerosis where your latency is increased and finally it stops conducting or it could be that it could be that genetic and it could be post-viral infection cause the Landry Guillian-Barre syndrome where you have demyelination occurring and loss of nerve function, conduction failure.

So, some characteristics of central nervous system neurons. So, we talk mainly about the squid but this what happens in the squid as far as the action potential resting membrane, all these are pretty much the same if not very similar in all the neurons vertebrate, invertebrate, mammalian human study so far. But the details vary. So, in the human central nervous system neurons exhibit a wide variety of electrophysiological properties. They have multiple conductances, it is not just sodium and potassium, they may also have calcium. And you have different types of sodium, different types of potassium conductance, different types of calciums, and conductances. Now, in the squid we saw sodium currents are transient but they can be transient, they can also be persistent, and likewise, potassium currents they vary a lot in the voltage sensitivity and kinetics in different cells in this human central nervous system.

So, neurons talking of potassium, they have multiple subtypes of high threshold potassium currents. And there are low threshold potassium currents and they generate bursts of action potentials and after this when you have hyperpolarization, that also the process of high polarization activates ionic currents which are involved in rhythmic activity, central pattern generators in the brain stem which control heart rate, control respiration, rhythmic activity. So, thank you very much. In the next session, we shall consider aspects of Axonology and Neuronal Biophysics.