The Kelvin equation describes the change in vapour pressure due to a curved liquid–vapor interface, such as the surface of a droplet. The vapor pressure at a convex surface is higher than that at a flat surface. The Kelvin equation is dependent upon thermodynamic principles and does not allude to special properties of materials. It is also used for determination of pore size distribution of a porous medium using adsorption porosimetry. The equation is named in honor of William Thomson, also known as Lord Kelvin.
Formulation The original form of the Kelvin equation, published in 1871, is:
p ( r 1 , r 2 ) = P − γ ρ v a p o r ( ρ l i q u i d − ρ v a p o r ) ( 1 r 1 + 1 r 2 ) , {\displaystyle p(r_{1},r_{2})=P-{\frac {\gamma \,\rho _{\rm {vapor}}}{(\rho _{\rm {liquid}}-\rho _{\rm {vapor}})}}\left({\frac {1}{r_{1}}}+{\frac {1}{r_{2}}}\right),}
where:
p ( r ) {\displaystyle p(r)} = vapor pressure at a curved interface of radius r {\displaystyle r}
P {\displaystyle P} = vapor pressure at flat interface ( r = ∞ {\displaystyle r=\infty } ) = p e q {\displaystyle p_{eq}}
γ {\displaystyle \gamma } = surface tension
ρ v a p o r {\displaystyle \rho _{\rm {vapor}}} = density of vapor
ρ l i q u i d {\displaystyle \rho _{\rm {liquid}}} = density of liquid
r 1 {\displaystyle r_{1}} , r 2 {\displaystyle r_{2}} = radii of curvature along the principal sections of the curved interface. This may be written in the following form, known as the Ostwald–Freundlich equation:
ln p p s a t = 2 γ V m r R T , {\displaystyle \ln {\frac {p}{p_{\rm {sat}}}}={\frac {2\gamma V_{\text{m}}}{rRT}},}
where p {\displaystyle p} is the actual vapour pressure,
p s a t {\displaystyle p_{\rm {sat}}} is the saturated vapour pressure when the surface is flat,
γ {\displaystyle \gamma } is the liquid/vapor surface tension, V m {\displaystyle V_{\text{m}}} is the molar volume of the liquid, R {\displaystyle R} is the universal gas constant, r {\displaystyle r} is the radius of the droplet, and T {\displaystyle T} is temperature. Equilibrium vapor pressure depends on droplet size.
If the curvature is convex, r {\displaystyle r} is positive, then p > p s a t {\displaystyle p>p_{\rm {sat}}}
If the curvature is concave, r {\displaystyle r} is negative, then p < p s a t {\displaystyle p<p_{\rm {sat}}}
… excerpt ends here. Continue reading the full article.

