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Modern  cosmology  has  established  that  not  only  the  notion  of  the
            heat death of the universe but also the early attempts to refute the notion
            are  erroneous:  important  physical  factors—above  all,  gravitation—were
            not taken into account. When gravitation is taken into account, the uniform

            isothermal distribution of matter is not at all the most probable distribution
            and does not correspond to maximum entropy. Observations show that the
            universe is decidedly non-steady state; it is expanding. Matter, which was

            nearly  uniform  at  the  start  of  the  expansion,  with  time  breaks  up  into
            individual  objects,  under  the  action  of  gravitational  forces,  forming
            galactic  clusters,  galaxies,  stars,  and  planets.  All  these  processes  are
            natural, proceed with increasing entropy, and do not require violation of

            the laws of thermodynamics. Even in the future, if gravitation is taken into
            account, these processes will not lead to a uniform isothermal state of the
            universe,  i.  e.,  to  its  heat  death.  The  universe  is  always  no  static  and

            continuously evolving.








                                                      CHAPTER 3

                                            Real Gases and Liquids


                3.1. Forces and Potential Energy of Molecular Interaction in Gases

               In  discussions  of  gases  two  important  assumptions,  which  are  not
            always  justified,  were  done.  We  have  assumed  that  the  volume  of  the

            molecules  themselves  is  negligible  in  comparison  with  the  total  space
            occupied by the gas and that the attractive forces between gas molecules
            are negligible. For experiments with gases such as oxygen and hydrogen at

            room temperature and ordinary pressures, these assumptions are justified.
            But at high pressure these assumptions are not valid and deviations from
            laws of ideal gas take place. For the ideal gases the factor of compression

            is the following

                                                            pV
                                                                                                            (3.1.1)
                                                           RT
            in accordance  with  Mendeleev-Klapeiron  equation      pV                    RT .  But  for

            real  gases  the  factor  of  compression  depends  on  the  pressure  and



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