Page 47 - Bruno Linder Elementary Physical Chemistry
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August 18, 2010 11:36      9in x 6in     b985-ch04     Elementary Physical Chemistry





                               32                   Elementary Physical Chemistry

                                  The standard entropies of H 2 (g), O 2 (g) and H 2 O (l) at 25 Care
                                                                                         ◦
                               respectively 130.7, 205.2, 70.0 kJ mol −1 , giving ∆S =(2 × 70.0 − 205.2 −
                               2 ×130.7)kJ = −326.6 kJ. [This is the correct way to calculate ∆S,since S
                               is a state function. Had we calculated ∆S from q/T , the result would have
                               been wrong. Why?]
                                  The rule that ∆S has to be positive in an irreversible change applies
                               to an isolated system. In the above example, the system is not isolated.
                               To get around this difficulty, the standard procedure is to consider also
                               the entropy of the surroundings (the rest of the universe), and regard the
                               system and surroundings as an isolated system. Thus,

                                               ∆S total =∆S system +∆S surroundings        (4.3)

                               4.4. The Entropy of the Surroundings
                               In treating the surrounding entropy, it is common practice to assume that
                               the surrounding changes reversibly even though the system may change
                               irreversibly. [The rationale is that the surrounding, being so enormous,
                               would change quasi-statically.]

                               Example 4.2. Let us return to the water reaction. It is found that at
                                 ◦
                               25 C and one atmosphere the heat released is −572 kJ mol −1 . As stated, the
                               heat released by the system is assumed to be absorbed by the surrounding
                               reversibly even though the system looses heat irreversibly.
                                  The heat absorbed by the surrounding is q P = +572 kJ and thus
                               ∆S surr = 572 kJ/298K = 1.92 kJ K −1  = 1920J K −1 . On the other hand,
                               the system entropy, as noted before, is ∆S sys = −327J K −1  and so ∆S tot
                               equals (−327 + 1920)J K −1  = 1539J K −1  and is positive, as it should be.
                                  In general, at constant T ,∆S surr = q surr/T = −q sys/T and if P is also
                               constant, and if there is no work other than pV work,

                                                      ∆S surr = −∆H sys /T                 (4.4)



                                 Comment: ∆H can always be related to q, regardless of whether q
                                 is reversible or irreversible. ∆S can only be equated to q/T if q is
                                 reversible.
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