Page 84 - Basic physical chemistry for the atmospheric sciences
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70                  Basic physical chemistry

              Therefore,  the  total  number  of  moles  in  100  kg  of  dry  air  is
              2700 + 725 + 32.6 = 3460.  Hence, from Eq. (4. 2 )
                                      2700          8 . 0
                              l/J nitrogen =   = 0.  780  = 7  %
                                      3460
                                       725
                                                   2
                               lf!oxygen  =   = 0 . 2 1 0   =  1 .0%
                                      3460
                                       32.6
                                I/Jargon =  3460  = 0.00942 = 0.942%

              E x ercise 4.2. The apparent molecular weight of solution   is defined
                                                                Ma
              as
                                    Total mass of a solution
                              =
                           Ma   Total number of moles in solution
              What is the apparent molecular weight of dry air? Use the assumptions
              and values given in Exercise 4. 1 .
                Solution.  From  the  definition  of Ma  and  the  values  calculated  in
              Exercise 4. 1 ,   the apparent molecular weight of dry air is
                                    1 0 0 x  0 3
                                         1
                               Ma             28.9 g mole - 1
                                      3460


                               4.3  Factors  affecting solubility
              The tendency toward maximum randomness (entropy) causes a solid
              to  dissolve.  On  the  other  hand,  the  precipitation  of a  solid from  a
              solution  lowers  the  energy  of  the  system,  which  is  also  a  favored
              condition.  Equilibrium is reached when  the concentration of the sol­
              utes in a solution  s   such that the driving forces of these two opposing
                              i
              tendencies (randomness and minimum energy) are the same.  The en­
              ergy factor is measured by the change in heat content when 1  mole of
              a  solid dissolves;  this  is  called  the  heat  o f   solution.  An  increase  in
                                                             g
              temperature always favors the more random state (e. . , the dissolving
              process for a solid).  Consequently,  the  solubilities of solids increase
              with increasing temperature.
                Since gases are more random than liquids, randomness (or entropy)
              decreases as a gas dissolves in a liquid.  Therefore,  unlike soli s ,   the
                                                                      d
              tendency toward  maximum randomness favors the gas phase rather
              than the gas dissolving in a liquid. However, when a gas dissolves in a
              liquid, heat is  released, and  this favors  the  dissolving process.  As  in
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