In surface chemistry, the Hertz–Knudsen equation, also known as Knudsen–Langmuir equation describes evaporation rates, named after Heinrich Hertz and Martin Knudsen.
The Hertz–Knudsen equation describes the non-dissociative adsorption of a gas molecule on a surface by expressing the variation of the number of molecules impacting on the surfaces per unit of time as a function of the pressure of the gas and other parameters which characterise both the gas phase molecule and the surface:[1] [2]
| dN | |
| Adt |
\equiv\varphi=
| \alphap | |
| \sqrt{2\pimkBT |
where:
| Quantity | Description |
|---|---|
| A | Surface area (in m2) |
| N | Number of gas molecules |
| t | Time (in s) |
| φ | Flux of the gas molecules (in m−2 s−1) |
| α | Anomalous evaporation coefficient, 0 ≤ α ≤ 1, to match experimental results to theoretical predictions (Knudsen noted that experimental fluxes are lower than theoretical fluxes)[3] |
| p | The gas pressure (in Pa) |
| M | Molar mass (in kg mol−1) |
| m | Mass of a particle (in kg) |
| kB | Boltzmann constant |
| T | Temperature (in K) |
| R | Gas constant (J mol−1 K−1) |
| NA | Avogadro constant (mol−1) |