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# Osmotic coefficient

An osmotic coefficient φ is a quantity which characterises the deviation of a solvent from ideal behaviour, referenced to Raoult's law. The osmotic coefficient on a molality basis is defined by: $\varphi=\frac{\mu_A^*-\mu_A}{RTM_A\sum_i m_i}\,$

and on an amount fraction basis by: $\varphi=-\frac{\mu_A^*-\mu_A}{RT \ln x_A}\,$

where $\mu_A^*$ is the chemical potential of the pure solvent and μA is the chemical potential of the solvent in a solution, MA is its molar mass, xA its amount fraction, R the gas constant and T the temperature in kelvins. The latter osmotic coefficient is sometimes called the rational osmotic coefficient. The values for the two definitions are different, but since $\ln x_A = - \ln(1 + M_A \sum_i m_i) \approx - M_A \sum_i m_i,$

the two definitions are similar, and in fact both go to 1 as the concentration goes to zero.

In a single solute solution, the (molality based) osmotic coefficient and the solute activity coefficient are related to the excess Gibbs free energy Gex by the relations: $RTm(1-\varphi) = G_{ex} - m \frac{dG_{ex}}{dm}$ $RT\ln\gamma = \frac{dG_{ex}}{dm}$

and there is thus a differential relationship between them (temperature and pressure held constant):

d((φ − 1)m) = mdln γ

In ionic solutions, Debye-Hückel theory implies that

 (φ − 1) ∑ mi i

is asymptotic to $-\frac 2 3 A I^{3/2}$, where I is ionic strength and A is the Debye-Hückel constant (equal to about 1.17 for water at 25 °C). This means that, at least at low concentrations, the vapor pressure of the solvent will be greater than that predicted by Raoult's law. For instance, for solutions of magnesium chloride, the vapor pressure is slightly greater than that predicted by Raoult's law up to a concentration of 0.7 mol/kg, after which the vapor pressure is lower than Raoult's law predicts.

For aqueous solutions, the osmotic coefficients can be calculated theoretically by Pitzer equations or TCPC model.

Bromley equation, Pitzer equation, Davies equation

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