Menu
Home Explore People Places Arts History Plants & Animals Science Life & Culture Technology
On this page
Born equation
Equation for Gibbs free energy of solvation

The Born equation can be used for estimating the electrostatic component of Gibbs free energy of solvation of an ion. It is an electrostatic model that treats the solvent as a continuous dielectric medium (it is thus one member of a class of methods known as continuum solvation methods).

The equation was derived by Max Born. Δ G = − N A z 2 e 2 8 π ε 0 r 0 ( 1 − 1 ε r ) {\displaystyle \Delta G=-{\frac {N_{\text{A}}z^{2}e^{2}}{8\pi \varepsilon _{0}r_{0}}}\left(1-{\frac {1}{\varepsilon _{\text{r}}}}\right)} where:

We don't have any images related to Born equation yet.
We don't have any YouTube videos related to Born equation yet.
We don't have any PDF documents related to Born equation yet.
We don't have any Books related to Born equation yet.
We don't have any archived web articles related to Born equation yet.

Derivation

The energy U stored in an electrostatic field distribution is: U = 1 2 ε 0 ε r ∫ | E | 2 d V {\displaystyle U={\frac {1}{2}}\varepsilon _{0}\varepsilon _{\text{r}}\int |{\bf {E}}|^{2}dV} Knowing the magnitude of the electric field of an ion in a medium of dielectric constant εr is | E | = z e 4 π ε 0 ε r r 2 {\displaystyle |{\bf {E}}|={\frac {ze}{4\pi \varepsilon _{0}\varepsilon _{r}r^{2}}}} and the volume element d V {\displaystyle dV} can be expressed as d V = 4 π r 2 d r {\displaystyle dV=4\pi r^{2}dr} , the energy U {\displaystyle U} can be written as: U = 1 2 ε 0 ε r ∫ r 0 ∞ ( z e 4 π ε 0 ε r r 2 ) 2 4 π r 2 d r = z 2 e 2 8 π ε 0 ε r r 0 {\displaystyle U={\frac {1}{2}}\varepsilon _{0}\varepsilon _{\text{r}}\int _{r_{0}}^{\infty }\left({\frac {ze}{4\pi \varepsilon _{0}\varepsilon _{\text{r}}r^{2}}}\right)^{2}4\pi r^{2}dr={\frac {z^{2}e^{2}}{8\pi \varepsilon _{0}\varepsilon _{\text{r}}r_{0}}}} Thus, the energy of solvation of the ion from gas phase (εr = 1) to a medium of dielectric constant εr is: Δ G N A = U ( ε r ) − U ( ε r = 1 ) = − z 2 e 2 8 π ε 0 r 0 ( 1 − 1 ε r ) {\displaystyle {\frac {\Delta G}{N_{\text{A}}}}=U(\varepsilon _{\text{r}})-U(\varepsilon _{\text{r}}=1)=-{\frac {z^{2}e^{2}}{8\pi \varepsilon _{0}r_{0}}}\left(1-{\frac {1}{\varepsilon _{\text{r}}}}\right)}

References

  1. Born, M. (1920-02-01). "Volumen und Hydratationswärme der Ionen". Zeitschrift für Physik (in German). 1 (1): 45–48. Bibcode:1920ZPhy....1...45B. doi:10.1007/BF01881023. ISSN 0044-3328. S2CID 92547891. https://doi.org/10.1007/BF01881023

  2. Atkins; De Paula (2006). Physical Chemistry (8th ed.). Oxford university press. p. 102. ISBN 0-7167-8759-8. 0-7167-8759-8