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                        Chemical  thermodynamics















            Heat can  be  released  or absorbed  during  a  chemical  reaction.  This
            provides  a  powerful  method  for  studying  chemical  equilibrium  by
            means of chemical thermodynamics. Thermodynamics is based on  a
                                   e
            few fundamental postulat s ,   called the first, second, and third laws o f
            thermodynamics.  We will discuss these laws first, and then return to
            the subject of chemical equilibrium.


                       2.1  The first law of thermodynamics;  enthalpy
            In addition to the macroscopic kinetic and potential energy that a body
                                         s
            or system as a whole may posses ,   it also contains internal energy due
            to the kinetic and potential energy of its molecules or atoms. Increases
            in internal kinetic energy in  the form of molecular motions are  mani­
            fested as increases in the temperature of the system, while changes in
            the potential energy of the molecules  are caused by changes in their
            relative configurations.
                  u
              Let  s   suppose that a system of unit mass takes in a certain quantity
            of heat energy q  (measured in joules). As a result, the system may do
            a certain  amount of external  work  w  (also  measured  in joules). The
            excess  energy  supplied  to  the  system,  over and  above  the external
                                      q
            work done by the system, is  -  w  .  Therefore, if there is no change in
            the macroscopic kinetic and potential energy of the system, it follows
            from the principle of conservation of energy that the internal energy of
                                                i
                                      q
            the system must increase by  -  w  . That  s ,
                                     q  -  w  = u2 -  u 1             (2. 1)
            where u 1   and  u2 are the internal energies of a unit mass of the system
            before and after the change. In differential form Eq. (2. 1 ) becomes

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