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In  order  to  apply  atomic  mechanism  to  the  system  subjected  to  the
            process in thermodynamics and statistical thermodynamics, it is necessary
            that the atomic mechanisms of the process fall into one of following two
            classes:

            those so rapid that, in the time frame of the process of interest, the atomic
            states effectively visit all of their accessible range, bringing the system to
            its state of internal thermodynamic equilibrium; and

            those so slow that their progress can be neglected in the time frame of the
            process of interest.
                   The  rapid  atomic  mechanisms  represent  the  internal  energy  of  the
            system.  They  mediate  the  macroscopic  changes  that  are  of  interest  for

            thermodynamics  and  statistical  thermodynamics  because  they  quickly
            bring  the  system  close  enough  to  thermodynamic  equilibrium.  "When
            intermediate rates are present, thermodynamics and statistical mechanics

            cannot be applied." Such intermediate rate atomic processes do not bring
            the system near enough to thermodynamic equilibrium in the time frame of
            the  macroscopic  process  of  interest.  This  separation  of  time  scales  of

            atomic processes is a theme that recurs throughout the subject.
            For  example,  classical  thermodynamics  is  characterized  by  its  study  of
            materials  that  have  equations  of  state  or  characteristic  equations.  They

            express  equilibrium  relations  between  macroscopic  mechanical  variables
            and  temperature  and  internal  energy.  They  express  the  constitutive
            peculiarities of the material of the system. A classical material can usually
            be described by a function that makes pressure dependent on volume and

            temperature,  the  resulting  pressure  being  established  much  more  rapidly
            than any imposed change of volume or temperature.
            The present article takes a gradual approach to the subject, starting with a

            focus  on  cyclic  processes  and  thermodynamic  equilibrium,  and  then
            gradually beginning to further consider non-equilibrium systems.



                                             2.2      Internal Energy


                       In  thermodynamics,  the  internal  energy  is  the  total  energy

            contained by a thermodynamic system. Internal energy has two such major
            components as kinetic energy and potential energy. The kinetic energy is
            caused by the motion of the system of particles and the potential energy is

            associated with the static rest mass energy  of the constituents of matter,
            static electric energy of atoms within molecules or crystals, and the static




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