c12 JWBS043-Rogers September 13, 2010 11:27 Printer Name: Yet to Come
186 SOLUTION CHEMISTRY
12.5 HENRY’S LAW
The shape of thepBcurve in Fig. 12.3 suggests another model similar to Raoult’s
law but with a different slope for the lower (solute) end of the curve. According to
Henry’s law, the partial pressure, is the linear function found at the limit of infinitely
dilute solutions (in practice, very dilute solutions). Like the ideal gas law, it is a
limiting law (Rosenberg and Peticolas, 2004).
At relatively high concentrations of solute B, Henry’s law is a poor approximation
but it is clear from Fig. 12.4 that in the very dilute region near the vertical marker,
it is a better descriptor of the partial vapor pressure of B than Raoult’s law. On the
contrary, atXB→1 (toward the right in Fig. 12.4), B follows Raoult’s law. Now we
have a combined model:Raoult’s lawfor B acting as a solvent in high concentrations
andHenry’s lawfor B acting as a solute in low concentrations.
12.5.1 Henry’s Law Activities
We have encounteredactivitiesandactivity coefficientsbefore. A Henry’s law activity
of solute B in solvent A is shown as a vertical line well to the left on theXBaxis of
Fig. 12.4, whereXBis small. The activity coefficientγis the ratio of realpBto the
ideal, as determined by Henry’s law. For the behavior of B shown in Fig. 12.4, the
activity coefficient will beγ<1 in all cases because real behavior is always less than
ideal. It will approachγ=1 in the limit of infinite dilution. If the partial pressure
curve in Fig. 12.4 were below the Raoult’s law dotted line, all Henry’s law activity
coefficients would beγ>1.
The model we have described so far is for binary solutions in which the components
are mutually miscible (soluble in each other in all proportions). Everything we have
Α Β
XB
pB
pBo
FIGURE 12.4 Henry’s law for the partial pressure of component B as the solute. The solid
line is a Henry’s law extrapolation to infinite dilution of B. The dotted line is Raoult’s law.