Chemical potentials quantify a substance's tendency to undergo change, whether physical or chemical, within a system. They represent the change in Gibbs free energy when a single molecule is added, keeping temperature, pressure, and other component amounts constant. As partial molar Gibbs energies, they're intensive properties, unlike total Gibbs energy. They drive diffusion, phase transitions, and chemical reactions, seeking equilibrium by minimizing total free energy.
To calculate or simulate chemical potentials, we typically follow a few different approaches depending on the system and the level of approximation needed:
Using the fundamental relation:
$$ \mu_i=\mu_i^{\circ}+R T \ln a_i $$
For ideal gases: The activity $a_i$ is simply the partial pressure $P_i$ divided by a reference pressure $P^{\circ}$, so:
$$ \mu_i=\mu_i^{\circ}+R T \ln \frac{P_i}{P^{\circ}} $$
For ideal solutions: The activity is replaced by the molar fraction $x_i$ (assuming ideal behavior):
$$ \mu_i=\mu_i^{\circ}+R T \ln x_i $$
For real solutions: The activity $a_i$ is given by:
$$ a_i=\gamma_i x_i $$
where $\gamma_i$ is the activity coefficient (determined experimentally or via models such as Debye-Hückel, NRTL, UNIQUAC, etc.), leading to:
$$ \mu_i=\mu_i^{\circ}+R T \ln \left(\gamma_i x_i\right) $$
When analytical expressions are insufficient, numerical methods and molecular simulations can be used:
For quantum mechanical calculations, DFT can be used to compute Gibbs free energies of molecules in different phases, allowing direct computation of chemical potentials.
The CALPHAD method (CALculation of PHAse Diagrams) is used to predict chemical potentials based on experimental thermodynamic data and models.
If computational models are not available, chemical potentials can be inferred from: