Goldman Equation
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Goldman 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 ${\displaystyle M}$ monovalent positive ionic species and ${\displaystyle A}$ negative:

${\displaystyle E_{m}={\frac {RT}{F}}\ln {\left({\frac {\sum _{i}^{n}P_{M_{i}^{+}}[M_{i}^{+}]_{\mathrm {out} }+\sum _{j}^{m}P_{A_{j}^{-}}[A_{j}^{-}]_{\mathrm {in} }}{\sum _{i}^{n}P_{M_{i}^{+}}[M_{i}^{+}]_{\mathrm {in} }+\sum _{j}^{m}P_{A_{j}^{-}}[A_{j}^{-}]_{\mathrm {out} }}}\right)}}$

This results in the following if we consider a membrane separating two ${\displaystyle \mathrm {K} _{x}\mathrm {Na} _{1-x}\mathrm {Cl} }$-solutions:[1][2][3]

${\displaystyle E_{m,\mathrm {K} _{x}\mathrm {\text{Na}} _{1-x}\mathrm {Cl} }={\frac {RT}{F}}\ln {\left({\frac {P_{\text{Na}}[{\text{Na}}^{+}]_{\mathrm {out} }+P_{\text{K}}[{\text{K}}^{+}]_{\mathrm {out} }+P_{\text{Cl}}[{\text{Cl}}^{-}]_{\mathrm {in} }}{P_{\text{Na}}[{\text{Na}}^{+}]_{\mathrm {in} }+P_{\text{K}}[{\text{K}}^{+}]_{\mathrm {in} }+P_{\text{Cl}}[{\text{Cl}}^{-}]_{\mathrm {out} }}}\right)}}$

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

${\displaystyle E_{m,{\text{Na}}}={\frac {RT}{F}}\ln {\left({\frac {P_{\text{Na}}[{\text{Na}}^{+}]_{\mathrm {out} }}{P_{\text{Na}}[{\text{Na}}^{+}]_{\mathrm {in} }}}\right)}={\frac {RT}{F}}\ln {\left({\frac {[{\text{Na}}^{+}]_{\mathrm {out} }}{[{\text{Na}}^{+}]_{\mathrm {in} }}}\right)}}$
• ${\displaystyle E_{m}}$ = the membrane potential (in volts, equivalent to joules per coulomb)
• ${\displaystyle P_{\mathrm {ion} }}$ = the selectivity for that ion (in meters per second)
• ${\displaystyle [\mathrm {ion} ]_{\mathrm {out} }}$ = the extracellular concentration of that ion (in moles per cubic meter, to match the other SI units)[4]
• ${\displaystyle [\mathrm {ion} ]_{\mathrm {in} }}$ = the intracellular concentration of that ion (in moles per cubic meter)[4]
• ${\displaystyle R}$ = the ideal gas constant (joules per kelvin per mole)[4]
• ${\displaystyle T}$ = the temperature in kelvins[4]
• ${\displaystyle F}$ = Faraday's constant (coulombs per mole)

${\displaystyle {\frac {RT}{F}}}$ is approximately 26.7 mV at human body temperature (37 °C); when factoring in the change-of-base formula between the natural logarithm, ln, and logarithm with base 10 ${\displaystyle ([\log _{10}\exp(1)]^{-1}=\ln(10)=2.30258...)}$, it becomes ${\displaystyle 26.7\,\mathrm {mV} \cdot 2.303=61.5\,\mathrm {mV} }$, a value often used in neuroscience.

${\displaystyle E_{X}=61.5\,\mathrm {mV} \cdot \log {\left({\frac {[X^{+}]_{\mathrm {out} }}{[X^{+}]_{\mathrm {in} }}}\right)}=-61.5\,\mathrm {mV} \cdot \log {\left({\frac {[X^{-}]_{\mathrm {out} }}{[X^{-}]_{\mathrm {in} }}}\right)}}$

The ionic charge determines the sign of the membrane potential contribution. 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 ${\displaystyle R\approx {\frac {8.3\ \mathrm {J} }{\mathrm {K} \cdot \mathrm {mol} }}}$, ${\displaystyle F\approx {\frac {9.6\times 10^{4}\ \mathrm {J} }{\mathrm {mol} \cdot \mathrm {V} }}}$, (assuming body temperature) ${\displaystyle T=37\ ^{\circ }\mathrm {C} =310\ \mathrm {K} }$ and the fact that one volt is equal to one joule of energy per coulomb of charge, the equation

${\displaystyle E_{X}={\frac {RT}{zF}}\ln {\frac {X_{o}}{X_{i}}}}$

can be reduced to

{\displaystyle {\begin{aligned}E_{X}&\approx {\frac {0.0267\ \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 2.303\end{aligned}}}

which is the Nernst equation.

## Derivation

Goldman's equation seeks to determine the voltage Em across a membrane.[5] 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 Em 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 Em/L, where L is the thickness of the membrane. For a given ion denoted A with valence nA, its flux jA--in other words, the number of ions crossing per time and per area of the membrane--is given by the formula

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

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 DA 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 nA 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

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

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

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

where ? is a dimensionless number

${\displaystyle \mu ={\frac {FE_{m}}{RT}}}$

and PA is the ionic permeability, defined here as

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

The electric current density JA equals the charge qA of the ion multiplied by the flux jA

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

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 qA 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; this is because each type of ion would require a distinct membrane potential to balance diffusion, but there can only be one membrane potential. By assumption, at the Goldman voltage Em, the total current density is zero

${\displaystyle J_{tot}=\sum _{A}J_{A}=0}$

(Although the current for each ion type considered here is nonzero, there are other pumps in the membrane, e.g. Na+/K+-ATPase, not considered here which serve to balance each individual ion's current, so that the ion concentrations on either side of the membrane do not change over time in equilibrium.) If all the ions are monovalent--that is, if all the nA equal either +1 or -1--this equation can be written

${\displaystyle w-ve^{\mu }=0}$

whose solution is the Goldman equation

${\displaystyle {\frac {FE_{m}}{RT}}=\mu =\ln {\frac {w}{v}}}$

where

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

If divalent ions such as calcium are considered, terms such as e2? appear, which is the square of e?; in this case, the formula for the Goldman equation can be solved using the quadratic formula.

## References

1. ^ Enderle, John (2005-01-01), Enderle, John D.; Blanchard, Susan M.; Bronzino, Joseph D. (eds.), "11 - BIOELECTRIC PHENOMENA", Introduction to Biomedical Engineering (Second Edition), Biomedical Engineering, Boston: Academic Press, pp. 627-691, doi:10.1016/b978-0-12-238662-6.50013-6, ISBN 978-0-12-238662-6, retrieved
2. ^ Reuss, Luis (2008-01-01), Alpern, ROBERT J.; Hebert, STEVEN C. (eds.), "CHAPTER 2 - Mechanisms of Ion Transport Across Cell Membranes and Epithelia", Seldin and Giebisch's The Kidney (Fourth Edition), San Diego: Academic Press, pp. 35-56, doi:10.1016/b978-012088488-9.50005-x, ISBN 978-0-12-088488-9, retrieved
3. ^ Enderle, John D. (2012-01-01), Enderle, John D.; Bronzino, Joseph D. (eds.), "Chapter 12 - Bioelectric Phenomena", Introduction to Biomedical Engineering (Third Edition), Biomedical Engineering, Boston: Academic Press, pp. 747-815, doi:10.1016/b978-0-12-374979-6.00012-5, ISBN 978-0-12-374979-6, retrieved
4. ^ a b c d Bhadra, Narendra (2015-01-01), Kilgore, Kevin (ed.), "2 - Physiological principles of electrical stimulation", Implantable Neuroprostheses for Restoring Function, Woodhead Publishing Series in Biomaterials, Woodhead Publishing, pp. 13-43, doi:10.1016/b978-1-78242-101-6.00002-1, ISBN 978-1-78242-101-6, retrieved
5. ^ Junge D (1981). Nerve and Muscle Excitation (2nd ed.). Sunderland, Massachusetts: Sinauer Associates. pp. 33-37. ISBN 0-87893-410-3.