Page 23 - 4498
P. 23

1.12. Ttransport     Phenomenon Mean    Frequency  of Molecules
                                     Collisions in Gas. Mean Free Path





                     In physics,     chemistry,    biology and  engineering, a transport
            phenomenon  is  any  of  various  mechanisms  by  which  particles  or

            quantities move from one place to another. Due  to such  movement  the
            particles  may  transport        mass,  heat  or          momentum.  For  example  if

            molecules transport mass  we observe diffusion.  Heat transfer is transport
            energy. The cause of internal friction or viscosity  is momentum transfer.
            Transport phenomena in gases are studied by the kinetic theory of gases,
            primarily  by the mean free path of molecules


                 Molecules in real gases have certain sizes and in the process of heat

            motion they continuously collide with each other. To find the number of
            collisions  of  the  chosen  molecule    it  will  be          supposed that all  other
            molecules are immobile and only one molecule moves. Due to collisions

            the trajectory of this  molecule is a broken line  (fig.1.12.1a). Imaginary
            transform  this broken line  in straight  one, as shown in  (fig.1.12.1b).
              In such a model the traveling molecule  will collide with those molecules
            that are located inside the cylinder    (fig.1.12.1b)    with the radius    r2  (r

            is the molecule radius)
                         
                   If  v  is the average speed of the molecule,  then the  length of the
            cylinder will be  v       t  (namely it is the distance that the molecule  will
            travel during the time  t ). The volume  of the    mentioned  cylinder is
                                                                              calculated                  as

                                                                                     2
                                                                                 vr 2    t  .     The
                                                                              number           of        the
                                                                              molecules  inside  the
                                                                     б        cylinder                    is:
                  а
                                     Figure 2.1.1                             N    n    vr 2  2    t     ,

                                                                              where    n    is        the
            molecule concentration.   Obviously, this      number  N  is a number of
            collisions at the time  t . Hence,

               the number of collisions z per second is  equal to:



                                                            23
   18   19   20   21   22   23   24   25   26   27   28