Goldman equation

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WordNet

1. the act of regarding as equal (同)equating
2. a mathematical statement that two expressions are equal
3. United States anarchist (born in Russia) who opposed conscription; was deported to the Soviet Union in 1919 (1869-1940) (同)Emma Goldman

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1. 等式; 方程式

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出典(authority):フリー百科事典『ウィキペディア（Wikipedia）』「2015/11/25 17:30:19」(JST)

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Not to be confused with Goldman–Hodgkin–Katz flux equation.

The Goldman–Hodgkin–Katz voltage equation, more commonly known as the Goldman equation, is used in cell membrane physiology to determine the reversal potential across a cell's membrane, taking into account all of the ions that are permeant through that membrane.

The discoverers of this are David E. Goldman of Columbia University, and the English Nobel laureates Alan Lloyd Hodgkin and Bernard Katz.

Equation for monovalent ions

The GHK voltage equation for monovalent positive ionic species and negative:

This results in the following if we consider a membrane separating two -solutions:

It is "Nernst-like" but has a term for each permeant ion:

• = The membrane potential (in volts, equivalent to joules per coulomb)
• = the permeability for that ion (in meters per second)
• = the extracellular concentration of that ion (in moles per cubic meter, to match the other SI units)
• = the intracellular concentration of that ion (in moles per cubic meter)
• = The ideal gas constant (joules per kelvin per mole)
• = The temperature in kelvins
• = Faraday's constant (coulombs per mole)

The first term, before the parentheses, can be reduced to 61.5 mV for calculations at human body temperature (37 °C)

Note that the ionic charge determines the sign of the membrane potential contribution. Note also that during an action potential, although the membrane potential changes about 100mV, the concentrations of ions inside and outside the cell do not change significantly. They are always very close to their respective concentrations when the membrane is at their resting potential.

Calculating the first term

Using , , (assuming body temperature) and the fact that one volt is equal to one joule of energy per coulomb of charge, the equation

can be reduced to

$\begin{align} E_X & \approx \frac{.0267 \ \mathrm{ V}}{z} \ln \frac {X_o}{X_i} \\ & = \frac{26.7 \ \mathrm{ mV}}{z} \ln \frac {X_o}{X_i} \\ & \approx \frac{61.5 \ \mathrm{ mV} }{z} \log \frac {X_o}{X_i} & \text{ since } \ln 10 \approx 2.30 \end{align}$

Derivation

Goldman's equation seeks to determine the voltage E_m across a membrane. A Cartesian coordinate system is used to describe the system, with the z direction being perpendicular to the membrane. Assuming that the system is symmetrical in the x and y directions (around and along the axon, respectively), only the z direction need be considered; thus, the voltage E_m is the integral of the z component of the electric field across the membrane.

According to Goldman's model, only two factors influence the motion of ions across a permeable membrane: the average electric field and the difference in ionic concentration from one side of the membrane to the other. The electric field is assumed to be constant across the membrane, so that it can be set equal to E_m/L, where L is the thickness of the membrane. For a given ion denoted A with valence n_A, its flux j_A—in other words, the number of ions crossing per time and per area of the membrane—is given by the formula

$j_{\mathrm{A}} = -D_{\mathrm{A}} \left( \frac{d\left[ \mathrm{A}\right]}{dz} - \frac{n_{\mathrm{A}}F}{RT} \frac{E_{m}}{L} \left[ \mathrm{A}\right] \right)$

The first term corresponds to Fick's law of diffusion, which gives the flux due to diffusion down the concentration gradient, i.e., from high to low concentration. The constant D_A is the diffusion constant of the ion A. The second term reflects the flux due to the electric field, which increases linearly with the electric field; this is a Stokes-Einstein relation applied to electrophoretic mobility. The constants here are the charge valence n_A of the ion A (e.g., +1 for K⁺, +2 for Ca²⁺ and −1 for Cl⁻), the temperature T (in kelvins), the molar gas constant R, and the faraday F, which is the total charge of a mole of electrons.

Using the mathematical technique of separation of variables, the equation may be separated

$\frac{d\left[ \mathrm{A}\right]}{-\frac{j_{\mathrm{A}}}{D_{\mathrm{A}}} + \frac{n_{\mathrm{A}}FE_{m}}{RTL} \left[ \mathrm{A}\right]} = dz$

Integrating both sides from z=0 (inside the membrane) to z=L (outside the membrane) yields the solution

$j_{\mathrm{A}} = \mu n_{\mathrm{A}} P_{\mathrm{A}} \frac{\left[ \mathrm{A}\right]_{\mathrm{out}} - \left[ \mathrm{A}\right]_{\mathrm{in}} e^{n_{}\mu} }{1 - e^{n_{}\mu }}$

where μ is a dimensionless number

$\mu = \frac{F E_{m}}{RT}$

and P_A is the ionic permeability, defined here as

$P_{\mathrm{A}} = \frac{D_{\mathrm{A}}}{L}$

The electric current density J_A equals the charge q_A of the ion multiplied by the flux j_A

$J_{A} = q_{\mathrm{A}} j_{\mathrm{A}}$

Note: Current density has units of (Amperes/m²). Molar flux has units of (mol/(s m²)). Thus, to get current density from molar flux one needs to multiply by Faraday's constant F (Coulombs/mol). F will then cancel from the equation below. Since the valence has already been accounted for above, the charge q_A of each ion in the equation above, therefore, should be interpreted as +1 or -1 depending on the polarity of the ion.

There is such a current associated with every type of ion that can cross the membrane. By assumption, at the Goldman voltage E_m, the total current density is zero

$J_{tot} = \sum_{A} J_{A} = 0$

If all the ions are monovalent—that is, if all the n_A equal either +1 or -1—this equation can be written

$w - v e^{\mu} = 0$

whose solution is the Goldman equation

$\frac{F E_{m}}{RT} = \mu = \ln \frac{w}{v}$

where

$w = \sum_{\mathrm{cations\ C}} P_{\mathrm{C}} \left[ \mathrm{C}^{+} \right]_{\mathrm{out}} + \sum_{\mathrm{anions\ A}} P_{\mathrm{A}} \left[ \mathrm{A}^{-} \right]_{\mathrm{in}}$

$v = \sum_{\mathrm{cations\ C}} P_{\mathrm{C}} \left[ \mathrm{C}^{+} \right]_{\mathrm{in}} + \sum_{\mathrm{anions\ A}} P_{\mathrm{A}} \left[ \mathrm{A}^{-} \right]_{\mathrm{out}}$

If divalent ions such as calcium are considered, terms such as e^2μ appear, which is the square of e^μ; in this case, the formula for the Goldman equation can be solved using the quadratic formula.

See also

• Bioelectronics
• Cable theory
• GHK current equation
• Hindmarsh–Rose model
• Hodgkin–Huxley model
• Morris–Lecar model
• Nernst equation
• Saltatory conduction

References

External links

• Nernst/Goldman Equation Simulator
• Goldman-Hodgkin-Katz Equation Calculator
• Nernst/Goldman interactive Java applet The membrane voltage is calculated interactively as the number of ions are changed between the inside and outside of the cell.
• Potential, Impedance, and Rectification in Membranes by Goldman (1949)

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English Journal

• Comment on Tamagawa and Ikeda's reinterpretation of the Goldman-Hodgkin-Katz equation : Are transmembrane potentials caused by polarization?

• Heimburg T1.
• European biophysics journal : EBJ.Eur Biophys J.2018 Oct 5. doi: 10.1007/s00249-018-1335-x. [Epub ahead of print]
• PMID 30291392

• Another interpretation of the Goldman-Hodgkin-Katz equation based on Ling's adsorption theory.

• Tamagawa H1, Ikeda K2.
• European biophysics journal : EBJ.Eur Biophys J.2018 Sep 11. doi: 10.1007/s00249-018-1332-0. [Epub ahead of print]
• PMID 30203188

• Corneal Biomechanical Properties and Thickness in Primary Congenital Glaucoma and Normal Eyes: A Comparative Study.

• Zareei A1, Razeghinejad MR1,2, Salouti R1.
• Medical hypothesis, discovery & innovation ophthalmology journal.Med Hypothesis Discov Innov Ophthalmol.2018 Summer;7(2):68-72.
• PMID 30250855

Japanese Journal

• 電気化学的手法によるアルカリ骨材反応の迅速判定法に関する研究

• 関野 一男,露木 尚光
• 材料 60(9), 825-830, 2011
• … The membrane potential according to the equation for theory (Goldman equation) was calculated by substitution of the analysis value of Na, K and Si concentrations at aqueous electrolyte solutions.The results obtained were as follows : (1) The potential difference was measured with "Positive (+)" and "Negative (-)" values at testing periods of 3∼15minutes, by the use of "Innocuous" and "Deleterious" powder interpreted according to ASR chemical method (JIS A 1145), respectively. …
• NAID 130001027830

• Comparison of Estimation Accuracy of Body Density between Different Hydrostatics Weighing Methods without Head Submersion

• , , , ,
• Journal of physiological anthropology and applied human science 22(4), 175-179, 2003-07
• … (1988) and Donnelly and Sintek (1984) as referenced to Goldman and Buskirk's approach (1961). … Donnelly et al.'s method estimates Db from a regression equation using HW^<withoutHS>, moreover, Donnelly and Sintek's method estimates it from HW^<withoutHS> … In order to examine the consistency of estimation values of Db, the correlation coefficients between the estimation values and the reference (Goldman and Buskirk, 1961) were calculated. …
• NAID 110002528133

• Equation of state and intermolecular interactions in fluid hydrogen from Brillouin scattering at high pressures and temperatures

• Matsuishi Kiyoto,Gregoryanz Eugene,Mao Ho-kwang,Hemley Russell J.
• The journal of chemical physics 118(23), 10683-10695, 2003-06
• … From these sound velocity data together with previously reported volume and ultrasonic velocity data at low pressures and temperatures, we determined a Benedict-type P-V-T equation of state valid for fluid hydrogen up to the maximum pressures and temperatures of this study with an average deviation of 1.0% from the new and previously published experimental data. … Using the equation of state, the pressure and temperature dependences of thermodynamic properties were calculated. …
• NAID 120000833546

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