Page 127 - Modern physical chemistry
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118                       Relationships between Phases

                          V
                          I

                          I
             V         ......-ol
                          I
                          I
                          I
                          I
                          I
                          I
                          I
                                        FIGURE 6.10  Variation in volume with temperature about a
                            T           first order transition.


                When all first derivatives of G are continuous but discontinuities appear in second
             derivatives, the transition is said to be second order. An example appears in figure 6.11.
             Differentiating equations (5.85) leads to the fomlUlas
                                        {:~~l ~[:)p <;,                              [6.23]





                                            2
                                           aG  _[av)  -aV                            [6.24]
                                           aTap - aT  p  -  ,

                                        ~[:~ 1 ~~[:;l ~pv.                           [6.25]



                The last step in line (6.23)  employs equation (5.21) at constant P;  the last steps in
             (6.24) and (6.25), formulas (4.84) and (4.85). At a second order transition, volume V and
             entropy S are continuous, while energy capacity Cp,  expansion coefficient a, and com-
             pressibility f3 jump by /lCp ,  Aa , and A{3.  See figures 6.12 and 6.13.



             G



                                     phase (2)





                     Phase (1)








                                                      FIGURE 6.11  Change in curvature of the free
                                                  T   energy curve at a second order transition.
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