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Ideal and Real Gas Behavior                                                  15

            to condense into a liquid or even a solid, the volume reduces to a smaller but finite volume. This
            small volume will be proportional to the number of moles of gas as in

                                              ? 2 / n ¼ bn:

            Thus, a modified gas law was proposed by a Dutch physicist Johannes Diderik van der Waals
            (1837–1923) in 1873 in his doctoral thesis as a way to simulate the condensation of gases to liquids.
            He received the Nobel Prize for this work in 1910.

                                               2
                                              n
                                        P þ a      (V   nb) ¼ nRT
                                              V 2

            Chemical engineering students in this class will be aware of more accurate and complicated
            equations of state, but for this text we will be content to use the van der Waals equation as a useful
            treatment of real gases. Thus, parameters are available in terms of values of ‘‘a’’ and ‘‘b’’ for a
            number of gases and each gas has separate parameters, see Table 1.3. We may find some tables of
            these parameters in older units but lists are available in SI units as well.
              In the original 1873 doctoral thesis of van der Waals, the goal was to explain the process of
            condensation of gases to liquids in a smooth way. The ideal gas equation that predicts the PV product
            at any fixed temperature should be one branch of a hyperbola. Such ‘‘isotherm’’ curves are indeed
            found on a plot of pressure versus volume of a fixed amount of gas at constant temperature, for low
            pressures above the boiling point of a given material. However, as one lowers the temperature a small
            bump in the isotherm will be observed, which is at first an ‘‘inflection point’’ and then at still lower
            temperatures enters a region where there is a fog or mist of liquid condensate droplets. It is easy to
                                                                           2
            show that the van der Waals equation is cubic in V by multiplying through by V .
                           2
                          n
                 2                           2        3              2   2     3
                V   P þ a      (V   nb) ¼ nRTV  or PV   n(bP þ RT)V þ n aV   n ab ¼ 0:
                          V  2




                                TABLE 1.3
                                van der Waals Constants for Common Gases
                                               2
                                                     2
                                Gas         a (L bar=mol )      b (L=mol)
                                He             0.0346            0.0238
                                Ne             0.208             0.0167
                                               0.2452            0.0265
                                H 2
                                Ar             1.355             0.0320
                                               1.382             0.0319
                                O 2
                                N 2            1.370             0.0387
                                CO             1.472             0.0395
                                CH 4           2.303             0.0431
                                               3.658             0.0429
                                CO 2
                                               4.225             0.0371
                                NH 3
                                Source: Lide, D.R. Ed., CRC Handbook of Chemistry
                                      and Physics, 87th Edn., CRC Press, Boca Raton,
                                      FL, 2006–2007, p. 6–34.
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