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where  S denotes some function of the thermodynamic co-ordinate.

                  The function  S is called entropy.   This equation enables us to calculate the change
            of the entropy  dS  for a reversible process.

                  1.6 Heat and Work
                  One of the main conceptions of the thermodynamic are Heat and Work.   Before it
            was  mentioned,  that  the  thermodynamic  system  interacts  with  environment  by
            performing  some  work  or  the  transferring  some  heat.  Thus we have two  ways energy
            exchange.      Work  is  a  measure  of  the  energy  transfer  by  mechanical  means,  such  as
            gravitational, electric or magnetic forces.
                  Heat is a measure of energy transfer by means of temperature differences. Heat is
            transferred by thermal motion of  the molecules.   The sense of heat …. is motion and
            nothing  else.      We  describe  many  common  temperatures  changes  as  the  transfer  of
            “something” from one body at higher temperature to another at the lower temperature,
            and this “something”  we call heat.
                  Work  and  heat  are  energy  characteristics  of  the  thermodynamic  process  and  they
            value depends on what kind of process is going.  We can speak about heat and work
            only as they enter  or leave  a  thermodynamic system.
                  1.6.1 Theory of Heat
                  Caloric Theory of Heat  According to this theory,  heat is a sort of invisible fluid,
            called the caloric. It is found that, when a body is heated,  its weight does not increase.
            This is explained by supposing that the caloric is weightless fluid. The caloric is also
            supposed to be a fluid which can neither be created or destroyed. Thus, when heat flows
            from one body to another,  we must have the relation: Heat Lost is equal Heat Gained.
            This relation has been verified by a large number of experiments.
                                            th
                Hence, throughout the 18   century,  almost all the physicists believed in the Caloric
            Theory.

                  Mechanical Theory  of Heat  It must be noted that according to the Caloric Theory
                                                                                                              th
            we can not create or produce heat.   But several experiments performed during the 19
            century clearly showed that it is possible to produce heat.   For example,  when we rub
            our hands together,  they become warm. This shows that heat can be produced by the
            process of rubbing.   This fact could not be  explained on the Caloric Theory, so this
            theory was rejected.
                 Now  we  believe  in  the  Mechanical  Theory    of  Heat.  It  is  supposed  that  some
            mechanical work is converted into heat during the process of rubbing.   Thus heat is not
            a fluid,  but only a form of energy.   The “heat” in a body is believed to be the kinetic
            energy of its molecules. The molecules of liquids and gases also move from place to
            place.   When two bodies are rubbed together,  their molecules are violently shaken by
            the process of rubbing.   This increase their kinetic energy, and so heat is produced. The
            source of this heat is the mechanical work, which is performed during the process of
            rubbing.



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