Geochemistry. William M. White

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are using subscripts to denote the component, and superscripts to denote the phase; aq denotes the liquid aqueous solution). We define our standard state as that of the pure substance. According to eqn. 3.48, the chemical potential of water in the solution can be expressed as:

      where images denotes the chemical potential of pure liquid water. Substituting eqn. 3.59 into 3.58 and rearranging, we have:

      or

      (The order is important: eqn. 3.60a describes the freezing process, 3.61 the melting process. These processes will have equal and opposite entropies, enthalpies, and free energies.) The left-hand side of eqn. 3.61 is the Gibbs free energy of melting for pure water, which we denote as images (images is 0 at the melting temperature of pure water, which we denote Tom, but nonzero at any other temperature).

      We may rewrite eqn. 3.61 as:

      If we assume that ΔH and ΔS are independent of temperature (which is not unreasonable over a limited temperature range) and we assume pressure is constant as well, the left-hand side of the equation may also be written as:

      Substituting eqn. 3.63 into 3.62:

      At the melting temperature of pure water, images is zero, so that:

equation

      Substituting this into eqn. 3.64 and rearranging:

      (3.65)equation

      Further rearrangement yields:

equation

      For a reasonably dilute solution, the activity of water will approximately equal its mole fraction, so that:

      The entropy of melting is always positive, and since X is always less than 1, the left-hand side of eqn. 3.66 must always be positive. Thus, the ratio images must always be greater than 1. So the temperature at which an aqueous solution will freeze will always be less than the melting point of pure water. Salting of roads is not a question of geochemical interest, but there are many examples of depression of the freezing point of geological interest. For example, the freezing point of the ocean is about –2°C, and this phenomenon is important in igneous petrology, as we shall see in the next chapter. A related phenomenon of geological interest is elevation of the boiling point of a liquid: for example, hydrothermal solutions boil at temperatures significantly above that of pure water. Can you demonstrate that elevation of the boiling point of an ideal solution depends only on the mole fraction of the solute?

      3.7.1 The nature of water and water–electrolyte interaction

      There is perhaps no compound more familiar to us than H2O. Commonplace though it might be, H2O is the most remarkable compound in nature. Its unusual properties include: the highest heat capacity of all solids and liquids except ammonia, the highest latent heat of vaporization of all substances, the highest surface tension of all liquids, its maximum density is at 4°C, with density decreasing below that temperature (negative coefficient of thermal expansion), the solid form is less dense than the liquid (negative Clapeyron slope), and finally, it is the best solvent known, dissolving more substances and in greater quantity than any other liquid. We will digress here briefly to consider the structure and properties of H2O and the nature of water–electrolyte interactions from a microscopic perspective.

Schematic illustration of the (a) Structure of the water molecule. Bond angle in the liquid phase is 108 degree, and 105 degree in the gas. The hydrogens 
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