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Equation 1 · From Origins to Frontier: A History of Systems and Computational Neuroscience

What does this equation mean?

CmdVdt=−gˉNam3h(V−ENa)−gˉKn4(V−EK)−gL(V−EL)+IextC_m \frac{dV}{dt} = -\bar{g}_{Na} m^3 h (V - E_{Na}) - \bar{g}_K n^4 (V - E_K) - g_L (V - E_L) + I_{ext}

Read the formula alongside the article passage below. Each part has a deeper page with its role in the equation, the supporting passage and nearby citations.

Inputs and operations-barg_Na m^3 h (V - E_Na) - barg_K n^4 (V - E_K) - g_L (V - E_L) + I_ext
Result or conditionC_m fracdVdt
How to read the two sides of this formula. Follow the article passage for the meaning of each quantity.

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.

Read it piece by piece

CmC_m

Symbol C_m

CmC_m is part of the quantity the equation computes from the expression on the right.

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dd

Symbol d

d is part of the quantity the equation computes from the expression on the right.

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VV

Symbol V

V occurs above the fraction bar. The numerator is divided by the entire denominator below it.

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tt

Symbol t

t occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

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gˉNa\bar{g}_{Na}

Symbol barg_Na

bargNg_Na is one of the signed contributions combined to compute the quantity on the left.

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m3m^3

Symbol m^3

m3m^3 is one of the signed contributions combined to compute the quantity on the left.

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hh

Symbol h

h is one of the signed contributions combined to compute the quantity on the left.

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ENaE_{Na}

Symbol E_Na

ENE_Na is one of the signed contributions combined to compute the quantity on the left.

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gˉK\bar{g}_K

Symbol barg_K

bargKg_K is one of the signed contributions combined to compute the quantity on the left.

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n4n^4

Symbol n^4

n4n^4 is one of the signed contributions combined to compute the quantity on the left.

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EKE_K

Symbol E_K

EKE_K is one of the signed contributions combined to compute the quantity on the left.

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gLg_L

Symbol g_L

gLg_L is one of the signed contributions combined to compute the quantity on the left.

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ELE_L

Symbol E_L

ELE_L is one of the signed contributions combined to compute the quantity on the left.

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IextI_{ext}

Symbol I_ext

IeI_ext is one of the signed contributions combined to compute the quantity on the left.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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fraction

fraction

Divide the expression above the line by the one below it.

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addition

addition

Add the term after the plus sign to the term or group before it.

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subtraction

subtraction

Subtract the following term or group from the preceding one. A leading minus marks a negative quantity.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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superscript

superscript

A raised number can be a power. When it is a label or bound, it selects a case or the upper limit of a sum; the formula’s structure distinguishes these uses.

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dVdV

Numerator: dV

The complete quantity above the fraction bar.

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dtdt

Denominator: dt

The complete quantity below the fraction bar; it must be nonzero for this division.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction. Read it with the definitions, units, and assumptions supplied by the article.

What the article says around this equation

The model’s core equation describes membrane current as the sum of capacitive, sodium, potassium, and leak components: CmdVdt=−gˉNam3h(V−ENa)−gˉKn4(V−EK)−gL(V−EL)+IextC_m \frac{dV}{dt} = -\bar{g}_{Na} m^3 h (V - E_{Na}) - \bar{g}_K n^4 (V - E_K) - g_L (V - E_L) + I_{ext}. where m , h , and n are voltage- and time-dependent gating variables each obeying their own first-order kinetics. This is worth stating in full because it is the paradigm the rest of the field either extends or reacts against: a biophysical mechanism, expressed as a dynamical system, fit to directly measured current, with no free parameter standing in for an unmeasured process. It is why the model is still taught unmodified, and why its two authors and John Eccles shared the 1963 Nobel Prize in Physiology or Medicine. It is also, strictly, a model of one…
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The model’s core equation describes membrane current as the sum of capacitive, sodium, potassium, and leak components: CmdVdt=−gˉNam3h(V−ENa)−gˉKn4(V−EK)−gL(V−EL)+IextC_m \frac{dV}{dt} = -\bar{g}_{Na} m^3 h (V - E_{Na}) - \bar{g}_K n^4 (V - E_K) - g_L (V - E_L) + I_{ext}. where m , h , and n are voltage- and time-dependent gating variables each obeying their own first-order kinetics. This is worth stating in full because it is the paradigm the rest of the field either extends or reacts against: a biophysical mechanism, expressed as a dynamical system, fit to directly measured current, with no free parameter standing in for an unmeasured process. It is why the model is still taught unmodified, and why its two authors and John Eccles shared the 1963 Nobel Prize in Physiology or Medicine. It is also, strictly, a model of one excitable membrane, not of a circuit, a computation, or a behavior — the questions that would define the next seventy years were exactly about what happens when this unit is multiplied by billions and wired into structure.

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Sources cited in the article section

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