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McKay, Donald. "Front matter" Multimedia Environmental Models ...

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©2001 CRC Press LLC<br />

5.4 PARTITION COEFFICIENTS<br />

5.4.1 Fugacity and Solubility Relationships<br />

If we have two immiscible phases or media (e.g., air and water or octanol and<br />

water), we can conduct experiments by shaking volumes of both phases with a small<br />

amount of solute such as benzene to achieve equilibrium, then measure the concentrations<br />

and plot the results as was shown in Figure 5.1. It is preferable to use<br />

identical concentration units in each phase of amount per unit volume but, when<br />

one phase is solid, it may be more convenient to express concentration in units such<br />

as amounts per unit mass (e.g., mg/g) to avoid estimating phase densities. The plot<br />

of the concentration data is often linear at low concentrations; therefore, we can write<br />

C 2/C 1 = K 21<br />

and the slope of the line is K 21. Some nonlinear systems are considered later. Now,<br />

since C 2 is Z 2f 2 and C 1 is Z 1f 1, and at equilibrium f 1 equals f 2, it follows that K 21 is<br />

Z 2/Z 1. A Z value can be regarded as “half” a partition coefficient. If we know Z for<br />

one phase (e.g., Z 1 as well as K 21), we can deduce the value of Z 2 as K 21Z 1. This<br />

proves to be a convenient method of estimating Z values.<br />

The line may extend until some solubility limit or “saturation” is reached. In<br />

water, this is the aqueous solubility, but, for some substances such as lower alcohols,<br />

there is no “solubility,” because the solute is miscible with water. In air, the “solubility”<br />

is related to the vapor pressure of the pure solute, which is the maximum<br />

partial pressure that the solute can achieve in the air phase.<br />

Partition coefficients are widely available and used for systems of air-water,<br />

aerosol-air, octanol-water, lipid-water, fat-water, hexane-water, “organic carbon”water,<br />

and various minerals with water.<br />

Applying the theory that was developed earlier and noting that, at equilibrium,<br />

the solute fugacities will be equal in both phases, we can define partition coefficients<br />

for air-liquid and liquid-liquid systems.<br />

For air-water as an example at a total atmospheric pressure P T,<br />

Thus,<br />

f = x ig if R = y iP T = P i<br />

y i/x i = g if R/P T<br />

But if we use concentrations C i (mol/m 3 ) instead of mole fraction, y i is C iAv A or<br />

C iART/P T where v A is the molar volume of air. Similarly, x i is C iWv W where v W is<br />

the molar volume of the solution and is approximately that of water. Since f R is also<br />

P S , the partition coefficient K AW is then given by<br />

K AW = C iA/C iW = g i v W f R/RT = g i v W P S /RT = S iA/S iW

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