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24                  Basic physical chemistry

              where  a  is  the specific volume of the system. On the other hand, for
                                                               s
              an  irreversible expansion between the same two state ,   Psurroundings <
              Psystem. Therefore,




              Hence,
                                                                       (2. 1 8 )

              Applying  the  first law  of thermodynamics in  the  form of Eq. (2. 1 )   to
              the reversible transformation




              Similarly, for the irreversible transformation

                                    q irrcv - Wirrev = U2 - U I
              Therefore,



              or,



              Since, from Eq. (2. 1 8), wrev - wirrev > 0, it follows that



              or,
                                                                       (2. 1 9 )

                If a system receives heat dqirre v  at temperature T during an irrevers­
              ible  transformation,  the  change  in the  entropy  of the  system is  not
              equal to dqirreJT.  Also,  for an  irreversible transformation there is no
              simple relationship between the change  in the entropy of the system
              and  the  change  in  the  entropy  of  its  surroundings.  H o wever,  the
              remaining part of the  second  law of thermodynamics states that the
              entropy o f   the  universe increases as a result o f   irreversible transf o r­
              mations.
                The  two  parts  of the second  law  of thermodynamics stated above
                                      w
              can be summarized as follo s :
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