neural accommodation
Neural accommodation or neuronal accommodation occurs when a neuron or muscle cell is depolarised by slowly rising current (ramp depolarisation) in vitro.{{Cite journal
| last1 = Lucas | first1 = K.
| title = On the rate of variation of the exciting current as a factor in electric excitation
| journal = The Journal of Physiology
| volume = 36
| issue = 4–5
| pages = 253–274
| year = 1907
| pmid = 16992906
| pmc = 1533589
| doi=10.1113/jphysiol.1907.sp001231
| last1 = Vallbo | first1 = A. B.
| title = Accommodation Related to Inactivation of the Sodium Permeability in Single Myelinated Nerve Fibres from Xenopus Laevis
| journal = Acta Physiologica Scandinavica
| volume = 61
| pages = 429–444
| year = 1964
| pmid = 14209259
}} The Hodgkin–Huxley model also shows accommodation.{{Cite journal
| last1 = Hodgkin | first1 = A. L.
| last2 = Huxley | first2 = A. F.
| title = A quantitative description of membrane current and its application to conduction and excitation in nerve
| journal = The Journal of Physiology
| volume = 117
| issue = 4
| pages = 500–544
| year = 1952
| pmid = 12991237
| pmc = 1392413
| doi=10.1113/jphysiol.1952.sp004764
}} Sudden depolarisation of a nerve evokes propagated action potential by activating voltage-gated fast sodium channels incorporated in the cell membrane if the depolarisation is strong enough to reach threshold. The open sodium channels allow more sodium ions to flow into the cell and resulting in further depolarisation, which will subsequently open even more sodium channels. At a certain moment this process becomes regenerative (vicious cycle) and results in the rapid ascending phase of action potential. In parallel with the depolarisation and sodium channel activation, the inactivation process of the sodium channels is also driven by depolarisation. Since the inactivation is much slower than the activation process, during the regenerative phase of action potential, inactivation is unable to prevent the "chain reaction"-like rapid increase in the membrane voltage.
During neuronal accommodation, the slowly rising depolarisation drives the activation and inactivation, as well as the potassium gates simultaneously and never evokes action potential. Failure to evoke action potential by ramp depolarisation of any strength had been a great puzzle until Hodgkin and Huxley created their physical model of action potential. Later in their life they received a Nobel Prize for their influential discoveries. Neuronal accommodation can be explained in two ways. "First, during the passage of a constant cathodal current through the membrane, the potassium conductance and the degree of inactivation will rise, both factors raising the threshold. Secondly, the steady state ionic current at all strengths of depolarization is outward, so that an applied cathodal current which rises sufficiently slowly will never evoke a regenerative response from the membrane, and excitation will not occur." (quote from Hodgkin and Huxley)
In vivo physiologic condition accommodation breaks down, that is long-duration slowly rising current excites nerve fibers at a nearly constant intensity no matter how slowly this intensity is approached.{{Cite journal
| last1 = Hennings | first1 = K.
| last2 = Arendt-Nielsen | first2 = L.
| last3 = Andersen | first3 = O. K.
| title = Breakdown of accommodation in nerve: A possible role for persistent sodium current
| journal = Theoretical Biology and Medical Modelling
| volume = 2
| pages = 16
| year = 2005
| doi = 10.1186/1742-4682-2-16
| pmid = 15826303
| pmc =1090618
| doi-access = free
| last1 = Baker | first1 = M.
| last2 = Bostock | first2 = H.
| title = Depolarization changes the mechanism of accommodation in rat and human motor axons
| journal = The Journal of Physiology
| volume = 411
| pages = 545–561
| year = 1989
| pmid = 2614732
| pmc = 1190540
| doi=10.1113/jphysiol.1989.sp017589
}}
See also
References
{{reflist|30em}}
External links
- [http://thevirtualheart.org/HHindex.html Interactive Java applet of the HH model ] Parameters of the model can be changed as well as excitation parameters and phase space plottings of all the variables is possible.
- [http://www.ebi.ac.uk/biomodels-main/BIOMD0000000020 Direct link to Hodgkin-Huxley model] and a [http://www.ebi.ac.uk/biomodels-main/static-pages.do?page=ModelMonth%2F2006-09 Description] in BioModels Database
- {{cite journal | pmc = 1392219 | pmid=14946712 | volume=116 | issue=4 | title=Measurement of current-voltage relations in the membrane of the giant axon of Loligo | date=April 1952 | pages=424–48 | doi=10.1113/jphysiol.1952.sp004716 | journal=The Journal of Physiology| last1=Hodgkin | first1=A. L. | last2=Huxley | first2=A. F. | last3=Katz | first3=B. |doi-access=free }} Direct link to Hodgkin-Huxley paper #1 via PubMedCentral
- {{cite journal | pmc = 1392213 | pmid=14946713 | volume=116 | issue=4 | title=Currents carried by sodium and potassium ions through the membrane of the giant axon of Loligo | date=April 1952 | pages=449–72 | doi=10.1113/jphysiol.1952.sp004717 | journal=The Journal of Physiology| last1=Hodgkin | first1=A. L. | last2=Huxley | first2=A. F. |doi-access=free }} Direct link to Hodgkin-Huxley paper #2 via PubMedCentral
- {{cite journal | pmc = 1392209 | pmid=14946714 | volume=116 | issue=4 | title=The components of membrane conductance in the giant axon of Loligo | date=April 1952 | pages=473–96 | doi=10.1113/jphysiol.1952.sp004718 | journal=The Journal of Physiology| last1=Hodgkin | first1=A. L. | last2=Huxley | first2=A. F. |doi-access=free }} Direct link to Hodgkin-Huxley paper #3 via PubMedCentral
- {{cite journal | pmc = 1392212 | pmid=14946715 | volume=116 | issue=4 | title=The dual effect of membrane potential on sodium conductance in the giant axon of Loligo | date=April 1952 | pages=497–506 | doi=10.1113/jphysiol.1952.sp004719 | journal=The Journal of Physiology| last1=Hodgkin | first1=A. L. | last2=Huxley | first2=A. F. |doi-access=free }} Direct link to Hodgkin-Huxley paper #4 via PubMedCentral
- {{cite journal | pmc = 1392413 | pmid=12991237 | volume=117 | issue=4 | title=A quantitative description of membrane current and its application to conduction and excitation in nerve | date=August 1952 | pages=500–44 | doi=10.1113/jphysiol.1952.sp004764 | journal=The Journal of Physiology| last1=Hodgkin | first1=A. L. | last2=Huxley | first2=A. F. |doi-access=free }} Direct link to Hodgkin-Huxley paper #5 via PubMedCentral
- [http://www.demonstrations.wolfram.com/NeuralImpulsesTheActionPotentialInAction/ Neural Impulses: The Action Potential In Action] by Garrett Neske, The Wolfram Demonstrations Project
- [http://demonstrations.wolfram.com/HodgkinHuxleyActionPotentialModel/ Interactive Hodgkin-Huxley model] by Shimon Marom, The Wolfram Demonstrations Project
- [http://senselab.med.yale.edu/modeldb ModelDB] A computational neuroscience source code database containing 4 versions (in different simulators) of the original Hodgkin–Huxley model and hundreds of models that apply the Hodgkin–Huxley model to other channels in many electrically excitable cell types.
{{DEFAULTSORT:Hodgkin-Huxley Model}}