Page 24 - [B._MURPHY,_C._MURPHY,_B._HATHAWAY]_A_working_meth
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8                                                    Chapter I
       molecules of  the  air, colliding with  the particles of the smoke. This
       is Brownian motion.
         The kinetic theory of gases is a model proposed to account for the
       observed properties of  gases. In order that  the model is applicable,
       certain assumptions are made. For this reason, gases are categorised
       into two types: (a) ideal gases (as defined previously) and (b) real gases
       (defined as non-ideal gases).


                Assumptions of the Kinetic Theory for an Ideal Gas
         1. Gases consist of  tiny molecules, which are so small and  so far
            apart  that  the  actual  size  of  the  molecules  is  negligible  in
           comparison to the large distance between them.
         2.  The molecules are totally independent of each other, i.e. there are
            no attractive or repulsive forces between the molecules.
         3. The molecules are in constant random motion. They collide with
           each other and with  the walls or sides of  the container, which
           changes the direction of linear motion.
         4.  For each elastic collision, there is no net loss of  kinetic energy.
           However, there may be transfer of energy between the particles
           in such a collision.
         5. The average kinetic energy, of all the molecules is assumed to be
            proportional to the absolute temperature T (measured in K) i.e.
            kinetic energy oc T.


          Validity of the Assumptions of the Kinetic Theory for an Ideal Gas
       Assumption I  This is largely true, since the compressibility of gases is
       very  high.  However, at high  pressures, when  a  gas  is  highly  com-
       pressed, it is not valid to state that the physical size of gas molecules is
       practically negligible compared with  the distances between the mole-
       cules.
       Assumption 2  This assumption is approximate, since gases diffuse or
       spread out to occupy all space available to them, i.e. there must be no
       appreciable binding force between the molecules. However, van  der
       Waals forces exist (intermolecular forces of attraction and repulsion),
       and with polar molecules, other attractive forces exist.
       Assumption  3 This  assumption  is  valid,  as  shown  by  Brownian
       motion.
       Assumptions 4 and 5  These assumptions are true, since in any elastic
       collision, kinetic energy is not lost.
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