Page 14 - 4498
P. 14

to480   m    , that corresponds  experimental data
                       s



                             1.6.Kinetic Interpretation of the Temperature

                   We know that a hotter body has greater internal energy than a similar

            colder body. Thus, higher temperature means higher internal energy and
            lower temperature means lower internal energy. According to the kinetic
            theory of gases, the   mean kinetic energy of its molecules is the same as

            temperature. So, the  unit of energy i J (joule). Therefore,

                                                     2
                                           2    m  v rms  
                                                                  temperatur  e  in  joule    (1.6.1)
                                           3       2      
                                                          

            But it is not convenient to use   temperature in joules; it is much more
            convenient to determine temperature in the thermodynamic scale in Kelvin

            (K).The Boltzmann Constant, symbolized by  k  or  k , is the relationship
                                                                                  B
            between absolute temperature and kinetic energy of molecule of an ideal

            gas.
                                                       2
                                              2    m  v rms  
                                                                k  T                                      (1.6.2)
                                              3      2      
                                                            


            or
                temperature in  joules   =   Boltzmann Constant    temperature in
            Kelvin (K)

                                 J
            and      k     , 8  31
                                 K

                According  to (6.2)  the main equation (5.1)of molecular-kinetic theory
            of ideal gas is possible to be written down as
                                                      p V   N  k   T                                              (1.6.3)

             or

                                                       p   n  k   T                                                   (1.6.4)







                                                            14
   9   10   11   12   13   14   15   16   17   18   19