- Quantitative models of the action potential
In

neurophysiology , several mathematical models of theaction potential have been developed, which fall into two basic types. The first type seeks to model the experimental data quantitatively, i.e., to reproduce the measurements of current and voltage exactly. The renownedHodgkin-Huxley model of the axon from the "Loligo " squid exemplifies such models.cite journal | author = Hodgkin AL, Huxley AF, Katz B |title = Measurements of current-voltage relations in the membrane of the giant axon of Loligo | journal = Journal of Physiology | year = 1952 | volume = 116 | pages = 424–448 | pmid = 14946713

cite journal | author = Hodgkin AL, Huxley AF |title = Currents carried by sodium and potassium ions through the membrane of the giant axon of Loligo|journal=Journal of Physiology | year = 1952 | volume = 116 | pages = 449–472 | pmid = 14946713

cite journal | author = Hodgkin AL, Huxley AF | title = The components of membrane conductance in the giant axon of Loligo | journal = J Physiol | year = 1952 | volume = 116 | pages= 473–496 | pmid = 14946714

cite journal | author=Hodgkin AL, Huxley AF | title = The dual effect of membrane potential on sodium conductance in the giant axon of Loligo | journal = J Physiol | year = 1952 | volume = 116 | pages = 497–506 | pmid = 14946715

cite journal | author = Hodgkin AL, Huxley AF | title = A quantitative description of membrane current and its application to conduction and excitation in nerve | journal = J Physiol | year = 1952 | volume = 117 | pages = 500–544 | pmid = 12991237] Although qualitatively correct, the H-H model does not describe every type of excitable membrane accurately, since it considers only two ions (sodium and potassium), each with only one type of voltage-sensitive channel. However, other ions such ascalcium may be important and there is a great diversity of channels for all ions.cite book | author = Yamada WM, Koch C, Adams PR | date = 1989 | chapter = Multiple Channels and Calcium Dynamics | title = Methods in Neuronal Modeling: From Synapses to Networks | editor = C. Koch, I Segev | publisher = Bradford Book, The MIT Press | location = Cambridge, MA | isbn = 0-262-11133-0 | pages = pp.97–133] As an example, thecardiac action potential illustrates how differently shaped action potentials can be generated on membranes with voltage-sensitive calcium channels and different types of sodium/potassium channels. The second type of mathematical model is a simplification of the first type; the goal is not to reproduce the experimental data, but to understand qualitatively the role of action potentials in neural circuits. For such a purpose, detailed physiological models may be unnecessarily complicated and may obscure the "forest for the trees". TheFitzhugh-Nagumo model is typical of this class, which is often studied for its entrainment behavior.cite book | author = Hoppensteadt FC | date = 1986 | title = An introduction to the mathematics of neurons | publisher = Cambridge University Press | location = Cambridge | isbn = 0-521-31574-3] Entrainment is commonly observed in nature, for example in the synchronized lighting of fireflies, which is coordinated by a burst of action potentials;cite journal

author = Hanson, F.E.

coauthors = Case, J.F.; Buck, E.; Buck, J.

year = 1971

title = Synchrony and Flash Entrainment in a New Guinea Firefly

journal = Science

volume = 174

issue = 4005

pages = 161-164

url = http://www.sciencemag.org/cgi/content/abstract/174/4005/161

accessdate = 2008-05-05] entrainment can also be observed in individual neurons.cite journal | author = Guttman R, Feldman L, Jacobsson E | date = 1980 | title = Frequency entrainment of squid axon | journal = J. Membr. Biol. | volume = 56 | pages = 9–18] Both types of models may be used to understand the behavior of smallbiological neural network s, such as thecentral pattern generator s responsible for some automatic reflex actions. cite book | author = Getting PA | date = 1989 | chapter = Reconstruction of Small Neural Networks | title = Methods in Neuronal Modeling: From Synapses to Networks | editor = C Koch and I Segev | publisher = Bradford Book, The MIT Press | location = Cambridge, MA | isbn = 0-262-11133-0 | pages = pp. 171–194] Such networks can generate a complex temporal pattern of action potentials that is used to coordinate muscular contractions, such as those involved in breathing or fast swimming to escape a predator.Hooper, Scott L. "Central Pattern Generators." "Embryonic ELS" (1999) http://www.els.net/elsonline/figpage/I0000206.html (2 of 2) [2/6/2001 11:42:28 AM] Online: Accessed 27 November 2007 [*http://crab-lab.zool.ohiou.edu/hooper/cpg.pdf*] .]**Hodgkin-Huxley model**In 1952

Alan Lloyd Hodgkin andAndrew Huxley developed a set of equations to fit their experimental voltage-clamp data on the axonal membrane. [*cite book | author = Nelson ME, Rinzel J| year= 1994|chapter= The Hodgkin-Huxley Model|title=The Book of GENESIS: Exploring Realistic Neural Models with the GEneral NEural SImulation System| editor= Bower J, Beeman D | publisher = Springer Verlag | location = New York|pages= pp. 29–49 | chapterurl=http://www.genesis-sim.org/GENESIS/iBoG/iBoGpdf/chapt4.pdf*] The model assumes that the membrane capacitance "C" is constant; thus, the transmembrane voltage "V" changes with the total transmembrane current "I"_{tot}according to the equation:$C\; frac\{dV\}\{dt\}\; =\; I\_\{mathrm\{tot\; =\; I\_\{mathrm\{ext\; +\; I\_\{mathrm\{Na\; +\; I\_\{mathrm\{K\; +\; I\_\{mathrm\{L$

where "I"

_{Na}, "I"_{K}, and "I"_{L}are currents conveyed through the local sodium channels, potassium channels, and "leakage" channels (a catch-all), respectively. The initial term "I"_{ext}represents the current arriving from external sources, such asexcitatory postsynaptic potential s from the dendrites or a scientist's electrode.The model further assumes that a given ion channel is either fully open or closed; if closed, its

conductance is zero, whereas if open, its conductance is some constant value "g". Hence, the net current through an ion channel depends on two variables: the probability "p"_{open}of the channel being open, and the difference in voltage from that ion's equilibrium voltage, "V" − "V"_{eq}. For example, the current through the potassium channel may be written as:$I\_\{mathrm\{K\; =\; g\_\{mathrm\{K\; left(\; V\; -\; E\_\{mathrm\{K\; ight)\; p\_\{mathrm\{open,\; K$

which is equivalent to

Ohm's law . By definition, no net current flows ("I"_{K}= 0) when the transmembrane voltage equals the equilibrium voltage of that ion (when "V" = "E"_{K}).To fit their data accurately, Hodgkin and Huxley assumed that each type of ion channel had multiple "gates", so that the channel was open only if all the gates were open and closed otherwise. They also assumed that the probability of a gate being open was independent of the other gates being open; this assumption was later validated for the inactivation gate.cite journal | author = Armstrong CM, Bezanilla F, Rojas E | date = 1973 | title = Destruction of sodium conductance inactivation in squid axons perfused with pronase | journal = J. Gen. Physiol. | volume = 48 | pages = 375–391

cite journal | author = Rojas E, Rudy B | date = 1976 | title = Destruction of the sodium conductance inactivation by a specific protease in perfused nerve fibres from "Loligo" | journal = J. Physiol. | volume = 262 | pages = 501–531] Hodgkin and Huxley modeled the voltage-sensitive potassium channel as having four gates; letting "p"_{"n"}denote the probability of a single such gate being open, the probability of the whole channel being open is the product of four such probabilities, i.e., "p"_{open, K}= "n"^{4}. Similarly, the probability of the voltage-sensitive sodium channel was modeled to have three similar gates of probability "m" and a fourth gate, associated with inactivation, of probability "h"; thus, "p"_{open, Na}= "m"^{3}"h". The probabilities for each gate are assumed to obey first-order kinetics:$frac\{dm\}\{dt\}\; =\; -\; frac\{m\; -\; m\_\{mathrm\{eq\}\{\; au\_\{m$

where both the equilibrium value "m"

_{eq}and the relaxation time constant τ_{"m"}depend on the instantaneous voltage "V" across the membrane. If "V" changes on a time-scale more slowly than τ_{"m"}, the "m" probability will always roughly equal its equilibrium value "m"_{eq}; however, if "V" changes more quickly, then "m" will lag behind "m"_{eq}. By fitting their voltage-clamp data, Hodgkin and Huxley were able to model how these equilibrium values and time constants varied with temperature and transmembrane voltage. The formulae are complex and depend exponentially on the voltage and temperature. For example, the time constant for sodium-channel activation probability "h" varies as 3^{(θ−6.3)/10}with the Celsius temperature θ, and with voltage "V" as:$frac\{1\}\{\; au\_\{h\; =\; 0.07\; e^\{-V/20\}\; +\; frac\{1\}\{1\; +\; e^\{3\; -\; V/10.$

In summary, the Hodgkin-Huxley equations are complex, non-linear

ordinary differential equation s in fourindependent variable s: the transmembrane voltage "V", and the probabilities "m", "h" and "n".cite book | author = Sato S, Fukai H, Nomura T, Doi S | date = 2005 | chapter = Bifurcation Analysis of the Hodgkin-Huxley Equations | title = Modeling in the Neurosciences: From Biological Systems to Neuromimetic Robotics | edition = 2nd edition | editor = Reeke GN, Poznanski RR, Lindsay KA, Rosenberg JR, Sporns O| publisher = CRC Press | location = Boca Raton | isbn = 978-0415328685 | pages = pp. 459–478] No general solution of these equations has been discovered. A less ambitious but generally applicable method for studying such non-linear dynamical systems is to consider their behavior in the vicinity of a fixed point.cite book | author = Guckenheimer J, Holmes P | date = 1986 | title = Nonlinear Oscillations, Dynamical Systems and Bifurcations of Vector Fields | edition = 2nd printing, revised and corrected | publisher = Springer Verlag | location = New York | isbn = 0-387-90819-6| pages = pp. 12–16] This analysis shows that the Hodgkin-Huxley system undergoes a transition from stable quiescence tobursting oscillations as the stimulating current "I"_{ext}is gradually increased; remarkably, the axon becomes stably quiescent again as the stimulating current is increased further still. [*cite journal | author = Sabah NH, Spangler RA | date = 1970 | title = Repetitive response of the Hodgkin-Huxley model for the squid giant axon | journal = Journal of Theoretical Biology | volume = 29 | pages = 155–171*] A more general study of the types of qualitative behavior of axons predicted by the Hodgkin-Huxley equations has also been carried out.

cite journal | author = Evans JW | date = 1972 | title = Nerve axon equations. I. Linear approximations | journal = Indiana U. Math. Journal | volume = 21 | pages = 877–885

cite journal | author = Evans JW, Feroe J | date = 1977 | title = Local stability theory of the nerve impulse | journal = Math. Biosci. | volume = 37 | pages = 23–50**Fitzhugh-Nagumo model**Because of the complexity of the Hodgkin-Huxley equations, various simplifications have been developed that exhibit qualitatively similar behavior. [

*cite journal | author = FitzHugh R | date = 1960 | title = Thresholds and plateaus in the Hodgkin-Huxley nerve equations | journal = J. Gen. Physiol. | volume = 43 | pages = 867–896*] The

cite journal | author = Kepler TB, Abbott LF | Marder E | date = 1992 | title = Reduction of conductance-based neuron models | journal = Biological Cybernetics | volume = 66 | pages = 381–387Fitzhugh-Nagumo model is a typical example of such a simplified system.cite journal | author = FitzHugh R | date = 1961 | title = Impulses and physiological states in theoretical models of nerve membrane | journal = Biophysical Journal | volume = 1 | pages = 445–466] cite journal | author = Nagumo J, Arimoto S, Yoshizawa S | date = 1962 | title = An active pulse transmission line simulating nerve axon | journal = Proceedings of the IRE | volume = 50 | pages = 2061–2070] Based on thetunnel diode , the FHN model has only two independent variables, but exhibits a similar stability behavior to the full Hodgkin-Huxley equations.cite book | author = FitzHugh R | date = 1969 | chapter = Mathematical models of axcitation and propagation in nerve | title = Biological Engineering | editor = HP Schwann | publisher = McGraw-Hill | location = New York | pages = pp. 1–85] The equations are:$C\; frac\{dV\}\{dt\}\; =\; I\; -\; g(V),$

:$Lfrac\{dI\}\{dt\}\; =\; E\; -\; V\; -\; RI$

where "g(V)" is a function of the voltage "V" that has a region of negative slope in the middle, flanked by one maximum and one minimum (Figure FHN). A much-studied simple case of the Fitzhugh-Nagumo model is the Bonhoeffer-van der Pol nerve model, which is described by the equationscite journal | author = Bonhoeffer KF | date = 1948 | title = Activation of Passive Iron as a Model for the Excitation of Nerve | journal = J. Gen. Physiol. | volume = 32 | pages = 69–91

cite journal | author = Bonhoeffer KF | date = 1953 | title = Modelle der Nervenerregung | journal = Naturwissenschaften | volume = 40 | pages = 301–311

cite journal | author = van der Pol B | date = 1926 | title = On relaxation-oscillations | journal = Philosophical Magazine | volume = 2 | pages = 978–992

cite journal | author = van der Pol B, van der Mark J | date = 1928 | title = The heartbeat considered as a relaxation oscillation, and an electrical model of the heart | journal = Philosophical Magazine | volume = 6 | pages = 763–775

cite journal | author = van der Pol B, van der Mark J | date = 1929 | title = The heartbeat considered as a relaxation oscillation, and an electrical model of the heart | journal = Arch. Neerl. Physiol. | volume = 14 | pages = 418–443]:$C\; frac\{dV\}\{dt\}\; =\; I\; -\; epsilon\; left(frac\{V^\{3\{3\}\; -\; V\; ight),$

:$Lfrac\{dI\}\{dt\}\; =\; -\; V$

where the coefficient ε is assumed to be small. These equations can be combined into a second-order differential equation

:$C\; frac\{d^\{2\}V\}\{dt^\{2\; +\; epsilon\; left(\; V^\{2\}\; -\; 1\; ight)\; frac\{dV\}\{dt\}\; +\; frac\{V\}\{L\}\; =\; 0.$

This van der Pol equation has stimulated much research in the mathematics of nonlinear

dynamical system s. Op-amp circuits that realize the FHN and van der Pol models of the action potential have been developed by Keener.cite journal | author = Keener JP | date = 1983 | title = Analogue circuitry for the van der Pol and FitzHugh-Nagumo equations | journal = IEEE Trans. on Systems, Man and Cybernetics | volume = 13 | pages = 1010–1014]A hybrid of the Hodgkin-Huxley and FitzHugh-Nagumo models was developed by Morris and Lecar in 1981, and applied to the

muscle fiber ofbarnacle s.cite journal | author = Morris C, Lecar H | date = 1981 | title = Voltage oscillations in the barnacle giant muscle fiber | journal = Biophysical Journal | volume = 35 | pages = 193–213] True to the barnacle's physiology, the Morris-Lecar model replaces the voltage-gated sodium current of the Hodgkin-Huxley model with a voltage-dependent calcium current. There is no inactivation (no "h" variable) and the calcium current equilibrates instantaneously, so that again, there are only two time-dependent variables: the transmembrane voltage "V" and the potassium gate probability "n". The bursting, entrainment and other mathematical properties of this model have been studied in detail.cite book | author = Rinzel J, Ermentrout GB | date = 1989 | chapter = Analysis of Neural Excitability and Oscillations | title = Methods in Neuronal Modeling: From Synapses to Networks | editor = C. Koch, I Segev | publisher = Bradford Book, The MIT Press | location = Cambridge, MA | isbn = 0-262-11133-0 | pages = pp. 135–169]The simplest models of the action potential are the "flush and fill" models (also called "integrate-and-fire" models), in which the input signal is summed (the "fill" phase) until it reaches a threshold, firing a pulse and resetting the summation to zero (the "flush" phase).cite journal | author = Keener JP, Hoppensteadt FC, Rinzel J | date = 1981 | title = Integrate-and-fire models of nerve membrane response to oscillatory input | journal = SIAM J. Appl. Math. | volume = 41 | pages = 503–517] All of these models are capable of exhibiting entrainment, which is commonly observed in nervous systems.

**Extracellular potentials and currents**Whereas the above models simulate the transmembrane voltage and current at a single patch of membrane, other mathematical models pertain to the voltages and currents in the ionic solution surrounding the neuron.cite book | author = Stevens CF | date = 1966 | title = Neurophysiology: A Primer | publisher = John Wiley and Sons | location = New York | pages = pp. 161–173 | id = LCCN|66|0|15872] Such models are helpful in interpreting data from extracellular electrodes, which were common prior to the invention of the glass pipette electrode that allowed intracellular recording.cite journal | author = Ling G, Gerard RW | date = 1949 | title = The normal membrane potential of frog sartorius fibers | journal = J. Cell. Comp. Physiol. | volume = 34 | pages = 383–396] The extracellular medium may be modeled as a normal isotropic ionic solution; in such solutions, the current follows the electric

field line s, according to the continuum form ofOhm's Law :$mathbf\{j\}\; =\; sigma\; mathbf\{E\}$

where

**j**and**E**are vectors representing thecurrent density andelectric field , respectively, and where σ is the conductivity. Thus,**j**can be found from**E**, which in turn may be found usingMaxwell's equations . Maxwell's equations can be reduced to a relatively simple problem ofelectrostatics , since the ionic concentrations change too slowly (compared to thespeed of light ) for magnetic effects to be important. Theelectric potential φ(**x**) at any extracellular point**x**can be solved usingGreen's identities :$phi(mathbf\{x\})\; =\; frac\{1\}\{4pisigma\_\{mathrm\{outside\}\; oint\_\{mathrm\{membranefrac\{partial\}\{partial\; n\}\; frac\{1\}\{left|\; mathbf\{x\}\; -\; oldsymbolxi\; ightleft\; [\; sigma\_\{mathrm\{outside\; phi\_\{mathrm\{outside(oldsymbolxi)\; -\; sigma\_\{mathrm\{insidephi\_\{mathrm\{inside(oldsymbolxi)\; ight]\; dS$

where the integration is over the complete surface of the membrane; $oldsymbolxi$ is a position on the membrane, σ

_{inside}and φ_{inside}are the conductivity and potential just within the membrane, and σ_{outside}and φ_{outside}the corresponding values just outside the membrane. Thus, given these σ and φ values on the membrane, the extracellular potential φ(**x**) can be calculated for any position**x**; in turn, the electric field**E**and current density**j**can be calculated from this potential field. [*cite journal | author = Lorente de No R | date = 1947 | title = A Study of Nerve Physiology | journal = Stud. Rockefeller Inst. Med. Research | volume = 132 | pages = Chap. 16*]

cite journal | author = Mauro A | date = 1960 | title = Properties of thin generators pertaining to electrophysiological potentials in volume conductors | journal = J. Neurophysiol. | volume = 23 | pages = 132–143

cite book | author = Woodbury JW | date = 1965 | chapter = Chapter 3: Potentials in a volume conductor | title = Physiology and Biophysics | editor = TC Ruch, HD Patton | publisher = W. B. Saunders Co. | location = Philadelphia | pages = pp.**ee also***

Biological neuron models **References****Further reading***

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