Page 18 - 4498
P. 18

this constant is called the gas constant (or universal gas constant ) denoted
            by R.
                                                 J   mol
              In SI system        R  31,8                .  We obtain the following formula for
                                                    K
            1 mol of ideal gas:

                                                             p V   R  T                                            (1.8.2)
            For arbitrary amount of gas there is such formula:
                                                       m
                                                      p V   RT or p V   RT                        (1.8.3)
                                                       M
             This equation is named Mendeleev- Clapeyron equation, where m – mass

                                                m                                           m
            of gas, M- molar mass,                - number of moles.  Thus,               , then
                                                M                                          V

                                                           
                                                               p   RT                                           (1.8.4)
                                                          M

                                                 1.9. Dalton's Law


                    Dalton's law of partial pressures states that the pressure of a mixture
           of  non-reactive gases is simply a sum of partial pressures of individual
           components. Dalton's Law is as follows:



                                                           p   p   p ...   p                               (1.9.1)
                                                               2
                                                         1
                                                                          n
            Accordingly, the ideal gas equation of state is as the following:


                                                 m    RT      m                m
                                                   p   1      2  RT ...      n  RT               (1.9.2)
                                                 M 1  V      M  2              M  n



                                                       Dalton's law is not exactly valid for real

                                                       gases. Those deviations are considerably
                                                       large    at    high pressures.   In   such
                                                       conditions,  the  volume  occupied  by  the
                                                       molecules        can  become    significant

                                                       compared  to  the  free  space  between
                                                       them.  In  particular,      the  short  average
                                                       distances  between  molecules  raises  the

                                                       intensity  of    intermolecular     forces
                                                       between  gas  molecules  enough  to
                      Figure 9.1
                                                            18
   13   14   15   16   17   18   19   20   21   22   23