Reversal potential - Revision history

imported>DreamRimmer bot II: Bot: Implementing outcome of RfC: converting list-defined references from {{reflist|refs=…}} to … for VisualEditor compatibility

2025-12-20T13:44:18Z

Bot: Implementing outcome of RfC: converting list-defined references from {{reflist|refs=…}} to <references>…</references> for VisualEditor compatibility

← Previous revision		Revision as of 13:44, 20 December 2025
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	{{Short description\|Membrane potential at which ionic current reverses}}		{{Short description\|Membrane potential at which ionic current reverses}}
	In a [[biological membrane]], the '''reversal potential''' is the [[membrane potential]] at which the direction of ionic current reverses. At the reversal potential, there is no net flow of ions from one side of the membrane to the other. For channels that are permeable to only a single type of ion, the reversal potential is identical to the [[equilibrium potential]] of the ion.<ref name="fundNeuro" /><ref name="Purves"/><ref name="expBrain"/>		In a [[biological membrane]], the '''reversal potential''' is the [[membrane potential]] at which the direction of ionic current reverses. At the reversal potential, there is no net flow of ions from one side of the membrane to the other. For channels that are permeable to only a single type of ion, the reversal potential is identical to the equilibrium potential of the ion.<ref name="fundNeuro" /><ref name="Purves"/><ref name="expBrain"/>

	==Equilibrium potential==		==Equilibrium potential==
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	==References==		==References==
	~~{{reflist\|refs=~~		<references>

	<!--<ref name="plonsey">{{cite book \|last1=Plonsey \|first1=Robert \|last2=Barr \|first2=Roger C. \|author-link=Robert Plonsey \|date=2007 \|title=Bioelectricity: A Quantitative Approach \|location=New York \|publisher=[[Springer Publishing\|Springer]] \|pages=57-64 \|isbn=978-0-387-48864-6}}</ref>-->		<!--<ref name="plonsey">{{cite book \|last1=Plonsey \|first1=Robert \|last2=Barr \|first2=Roger C. \|author-link=Robert Plonsey \|date=2007 \|title=Bioelectricity: A Quantitative Approach \|location=New York \|publisher=[[Springer Publishing\|Springer]] \|pages=57-64 \|isbn=978-0-387-48864-6}}</ref>-->

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	<ref name="expBrain">{{cite book \|last1=Mark \|first1=Bear \|last2=Connors \|first2=Barry \|date=2016 \|title=Neuroscience: Exploring the Brain \|publisher= Jones & Barlet Learning\|url = https://www.jblearning.com/catalog/productdetails/9781284211283\|page=64-127\|edition=4th Enhanced\|isbn=9781284211283}}</ref>		<ref name="expBrain">{{cite book \|last1=Mark \|first1=Bear \|last2=Connors \|first2=Barry \|date=2016 \|title=Neuroscience: Exploring the Brain \|publisher= Jones & Barlet Learning\|url = https://www.jblearning.com/catalog/productdetails/9781284211283\|page=64-127\|edition=4th Enhanced\|isbn=9781284211283}}</ref>

	<ref name="molBiol">{{Cite book \|last=Alberts \|first=Bruce ~~\|url=https://www.worldcat.org/oclc/887605755~~ \|title=Molecular biology of the cell \|date=2015 \|isbn=978-0-8153-4432-2 \|edition=6th \|location=New York, NY \|pages=615–616 \|oclc=887605755}}</ref>		<ref name="molBiol">{{Cite book \|last=Alberts \|first=Bruce \|title=Molecular biology of the cell \|date=2015 \|isbn=978-0-8153-4432-2 \|edition=6th \|location=New York, NY \|pages=615–616 \|oclc=887605755}}</ref>

	<ref name="theoNeuro">{{Cite book \|last=Abbott \|first=Laurence F. ~~\|url=https://www.worldcat.org/oclc/1225555646~~ \|title=Theoretical Neuroscience Computational and Mathematical Modeling of Neural Systems. \|date=2001 \|publisher=MIT Press \|others=Peter Dayan \|isbn=978-0-262-31142-7 \|location=Cambridge \|pages=158–160 \|oclc=1225555646}}</ref>		<ref name="theoNeuro">{{Cite book \|last=Abbott \|first=Laurence F. \|title=Theoretical Neuroscience Computational and Mathematical Modeling of Neural Systems. \|date=2001 \|publisher=MIT Press \|others=Peter Dayan \|isbn=978-0-262-31142-7 \|location=Cambridge \|pages=158–160 \|oclc=1225555646}}</ref>

	}}		</references>

	==External links==		==External links==

imported>RandFreeman: Adding local short description: "Membrane potential at which ionic current reverses", overriding Wikidata description "in a biological membrane"

2025-06-24T21:56:30Z

Adding local short description: "Membrane potential at which ionic current reverses", overriding Wikidata description "in a biological membrane"

← Previous revision		Revision as of 21:56, 24 June 2025
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			{{Short description\|Membrane potential at which ionic current reverses}}
	In a [[biological membrane]], the '''reversal potential''' is the [[membrane potential]] at which the direction of ionic current reverses. At the reversal potential, there is no net flow of ions from one side of the membrane to the other. For channels that are permeable to only a single type of ion, the reversal potential is identical to the [[equilibrium potential]] of the ion.<ref name="fundNeuro" /><ref name="Purves"/><ref name="expBrain"/>		In a [[biological membrane]], the '''reversal potential''' is the [[membrane potential]] at which the direction of ionic current reverses. At the reversal potential, there is no net flow of ions from one side of the membrane to the other. For channels that are permeable to only a single type of ion, the reversal potential is identical to the [[equilibrium potential]] of the ion.<ref name="fundNeuro" /><ref name="Purves"/><ref name="expBrain"/>

imported>MrSwedishMeatballs: /* Use in research */

2025-04-21T18:13:56Z

Use in research

New page

In a [[biological membrane]], the '''reversal potential''' is the [[membrane potential]] at which the direction of ionic current reverses. At the reversal potential, there is no net flow of ions from one side of the membrane to the other. For channels that are permeable to only a single type of ion, the reversal potential is identical to the [[equilibrium potential]] of the ion.<ref name="fundNeuro" /><ref name="Purves"/><ref name="expBrain"/>

==Equilibrium potential==
The equilibrium potential for an ion is the [[membrane potential]] at which there is no net movement of the ion.<ref name="fundNeuro" /><ref name="Purves"/><ref name="expBrain"/> The flow of any inorganic ion, such as [[sodium|Na+]] or [[potassium|K+]], through an [[ion channel]] (since membranes are normally impermeable to ions) is driven by the [[electrochemical gradient]] for that ion.<ref name="fundNeuro" /><ref name="Purves"/><ref name="expBrain"/><ref name="molBiol" /> This gradient consists of two parts, the difference in the concentration of that ion across the membrane, and the voltage gradient.<ref name="molBiol" /> When these two influences balance each other, the electrochemical gradient for the ion is zero and there is no net flow of the ion through the channel; this also translates to no current across the membrane so long as only one ionic species is involved.<ref name="fundNeuro" /><ref name="Purves"/><ref name="expBrain"/><ref name="molBiol" /><ref name="theoNeuro" /> The voltage gradient at which this equilibrium is reached is the equilibrium potential for the ion and it can be calculated from the [[Nernst equation]].<ref name="fundNeuro" /><ref name="Purves"/><ref name="expBrain"/><ref name="molBiol" />

===Mathematical models and the driving force===
We can consider as an example a positively charged ion, such as [[potassium|K+]], and a negatively charged membrane, as it is commonly the case in most organisms.<ref name="molBiol" /><ref name="theoNeuro" /> The membrane voltage opposes the flow of the potassium ions out of the cell and the ions can leave the interior of the cell only if they have sufficient thermal energy to overcome the energy barrier produced by the negative membrane voltage.<ref name="theoNeuro" /> However, this biasing effect can be overcome by an opposing concentration gradient if the interior concentration is high enough which favours the potassium ions leaving the cell.<ref name="theoNeuro" />

An important concept related to the equilibrium potential is the '''driving force'''''.'' Driving force is simply defined as the difference between the actual membrane potential and an ion's equilibrium potential <math>V_\mathrm{m}-E_\mathrm{i}\ </math>where <math>E_\mathrm{i}\ </math>refers to the equilibrium potential for a specific ion.<ref name="theoNeuro" /> Relatedly, the membrane current per unit area due to the type <math>i </math> ion channel is given by the following equation:

:<math>i_\mathrm{i} = g_\mathrm{i} \left(V_\mathrm{m}-E_\mathrm{i}\right) </math>

where <math>V_\mathrm{m}-E_\mathrm{i}\ </math> is the driving force and <math>g_\mathrm{i} </math> is the [[Electrical resistivity and conductivity|specific conductance]], or conductance per unit area.<ref name="theoNeuro" /> Note that the ionic current will be zero if the membrane is impermeable to that ion in question or if the membrane voltage is exactly equal to the equilibrium potential of that ion.<ref name="theoNeuro" />

==Use in research==
When Vm is at the reversal potential for an event such as a synaptic potential ({{math|''V''m − ''E''rev}} is equal to 0), the identity of the ions that flow during an EPC can be deduced by comparing the reversal potential of the EPC to the equilibrium potential for various ions. For instance several excitatory [[ionotropic]] ligand-gated [[neurotransmitter]] [[Receptor (biochemistry)|receptors]] including [[glutamate receptor]]s ([[AMPA]], [[NMDA]], and [[kainate]]), [[nicotinic]] [[acetylcholine]] (nACh), and [[serotonin]] (5-HT3) receptors are nonselective cation channels that pass Na+ and K+ in nearly equal proportions, giving the reversal potential close to zero. The inhibitory ionotropic ligand-gated neurotransmitter receptors that carry [[chloride|Cl−]], such as [[GABA]]A and [[glycine]] receptors, have reversal potentials close to the resting potential (approximately −70 mV) in neurons.<ref name="Purves" />

This line of reasoning led to the development of experiments (by Akira Takeuchi and Noriko Takeuchi in 1960) that demonstrated that acetylcholine-activated ion channels are approximately equally permeable to Na+ and K+ ions. The experiment was performed by lowering the external Na+ concentration, which lowers (makes more negative) the Na+ equilibrium potential and produces a negative shift in reversal potential. Conversely, increasing the external K+ concentration raises (makes more positive) the K+ equilibrium potential and produces a positive shift in reversal potential.<ref name="Purves" /> A general expression for reversal potential of synaptic events, including for decreases in conductance, has been derived.<ref>{{cite journal | vauthors = Brown JE, Muller KJ, Murray G | title = Reversal potential for an electrophysiological event generated by conductance changes: mathematical analysis | journal = Science | volume = 174 | issue = 4006 | pages = 318 | date = October 14, 1971 | pmid = 5119107 | doi = 10.1126/science.174.4006.318 | bibcode = 1971Sci...174..318B | s2cid = 34404730 }}</ref>

==See also==
*[[Electrochemical potential]]
*[[Membrane potential|Cell potential]]
*[[Goldman equation]]

==References==
{{reflist|refs=


<ref name="Purves">{{cite book | first= Dale |last=Purves| title = Neuroscience | url= https://global.oup.com/ushe/product/neuroscience-9781605353807?q=neuroscience&cc=us&lang=en | url-access= limited |edition=6th | publisher = Sinauer Associates | pages = 39–106 | year = 2017 | isbn = 9781605353807|display-authors=etal|author-link=Dale Purves}}</ref>

<ref name="fundNeuro">{{cite book |last1=Squire |first1=Larry |last2=Berg |first2=Darwin |date=2014 |title=Fundamental Neuroscience | url = https://www.sciencedirect.com/book/9780123858702/fundamental-neuroscience |publisher= Academic Press |pages=93–97| edition=4th |isbn=978-0-12-385870-2}}</ref>

<ref name="expBrain">{{cite book |last1=Mark |first1=Bear |last2=Connors |first2=Barry |date=2016 |title=Neuroscience: Exploring the Brain |publisher= Jones & Barlet Learning|url = https://www.jblearning.com/catalog/productdetails/9781284211283|page=64-127|edition=4th Enhanced|isbn=9781284211283}}</ref>

<ref name="molBiol">{{Cite book |last=Alberts |first=Bruce |url=https://www.worldcat.org/oclc/887605755 |title=Molecular biology of the cell |date=2015 |isbn=978-0-8153-4432-2 |edition=6th |location=New York, NY |pages=615–616 |oclc=887605755}}</ref>

<ref name="theoNeuro">{{Cite book |last=Abbott |first=Laurence F. |url=https://www.worldcat.org/oclc/1225555646 |title=Theoretical Neuroscience Computational and Mathematical Modeling of Neural Systems. |date=2001 |publisher=MIT Press |others=Peter Dayan |isbn=978-0-262-31142-7 |location=Cambridge |pages=158–160 |oclc=1225555646}}</ref>

}}

==External links==
* [http://www.nernstgoldman.physiology.arizona.edu/ Nernst/Goldman Equation Simulator]
* [http://www.physiologyweb.com/calculators/nernst_potential_calculator.html Nernst Equation Calculator]
* [http://www.physiologyweb.com/calculators/ghk_equation_calculator.html Goldman-Hodgkin-Katz Equation Calculator]
* [http://www.physiologyweb.com/calculators/electrochemical_driving_force_calculator.html Electrochemical Driving Force Calculator]

[[Category:Membrane biology]]
[[Category:Electrophysiology]]
[[Category:Cardiac electrophysiology]]
[[Category:Action potentials]]
[[Category:Walther Nernst]]