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

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pseudo-solubilities) in these media and the three partition coefficients are then<br />

discussed in more detail in Section 5.4. Armed with this knowledge we then address<br />

how this “laboratory” information can be applied to environmental media such as<br />

soils and aerosols.<br />

©2001 CRC Press LLC<br />

5.2 PROPERTIES OF PURE SUBSTANCES<br />

For reasons discussed later, it is important to ascertain if the substance of interest<br />

is solid, liquid, or vapor at the environmental temperature. This is obviously done<br />

by comparing this temperature with the melting and boiling points. Figure 5.2 is the<br />

familiar P-T diagram that enables the state of a substance to be determined. Of<br />

particular interest for solids is the supercooled liquid vapor pressure line, shown as<br />

a dashed line. This is the vapor pressure that a solid (such as naphthalene, which<br />

melts at 80°C) would have if it were liquid at 25°C. The reason it is not liquid at<br />

25°C is that naphthalene is able to achieve a lower free energy state by forming a<br />

crystal. Above 80°C, this lower energy state is not available, and the substance<br />

remains liquid. Above the boiling point, the liquid state is abandoned in favor of a<br />

vapor state. It is not possible to measure the supercooled liquid vapor pressure by<br />

direct experiment. It can be calculated as discussed shortly, and it can be measured<br />

Figure 5.2 P-T diagram for a pure substance.

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