Page 71 - Instant notes
P. 71

Entropy and change     57


              ‘The entropy of an isolated system  increases for irreversible processes
              and remains constant in the course of reversible processes. The entropy of
              an isolated system never decreases’.

        The second law of thermodynamics may be expressed in a large number of ways, but all
        definitions are equivalent to the one given here. The statistical definition of entropy
        helps visualization of the second law. As all spontaneous changes take place in such a
        way as to increase the total entropy, it follows that they proceed so as to engineer the
        chaotic (rather than ordered) dispersal of matter and energy:
           ∆S total≥0

        The ‘>’ relation applies to irreversible processes, and the ‘=’ relation applies to reversible
        processes (see Topic B4). It is important to appreciate that the second law of
        thermodynamics as expressed above refers to an  isolated system. Most experimental
        systems cannot be regarded as being isolated, in which case the universe, being the next
        largest container of our system, effectively becomes the isolated system. In this case, the
        total entropy change is simply the sum of the entropy change in the system and in the
        surroundings, and this total must be greater than or equal to zero to comply with the
        second law of thermodynamics:
           ∆S system+∆S surroundings=∆S total≥0

        For instance, the system entropy change in the reaction between hydrogen and fluorine
                                                              −1
                                                                   −1
        gases to generate liquid hydrogen fluoride is found to be −210 J K  mol . Although this
        represents a decrease in entropy, the reaction proceeds spontaneously because the total
        entropy change is greater than zero. The  positive entropy change arises because  the
        reaction is exothermic, and the heat lost to the  surroundings  causes  ∆S surroundings to be
        positive, and of greater magnitude than ∆S system.


                                 Standard entropy change

        Any non-equilibrium process  leads to a change in  entropy. As entropy is a  state
        function, the change may be calculated from the standard entropies of the initial and final
        states of the system:


        For a chemical reaction, for example, the standard entropy of reaction is therefore the
        difference between the  standard  entropies of reactants and products, and may be
        calculated from:


        This expression resembles those used with other state functions, such as the enthalpy,
        and despite the slightly simpler form, the similarity with expressions for enthalpy is even
        closer than is initially evident. In the case of enthalpy for example, the corresponding
        equation is
   66   67   68   69   70   71   72   73   74   75   76