Page 164 - Advanced thermodynamics for engineers
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150    CHAPTER 7 GENERAL THERMODYNAMIC RELATIONSHIPS




                The third Tds relationship is derived by assuming that
                                                 s ¼ sðp; vÞ:                             (7.42)

                                                 vs        vs
                                           ds ¼      dp þ      dv:                        (7.43)
                                                 vp        vv
                                                    v         p
                Now, by definition,

                                               vs        vs    vv
                                        c p ¼ T     ¼ T            ;
                                               vT        vv    vT
                                                   p        p      p
             giving

                                              vs     1    vT
                                                   ¼   c p     :
                                              vv     T    vv
                                                  p           p
                A similar expression can be derived for c v , and this enables the equation
                                                 vT          vT

                                        Tds ¼ c v     dp þ c p    dv                      (7.44)
                                                 vp  v       vv  p
             to be obtained. This is the third Tds relationship.


             7.3.1 VARIATION OF INTERNAL ENERGY AND ENTHALPY
             It is now possible to investigate the variation of internal energy and enthalpy with independent
             properties for gases obeying various gas laws.
                The internal energy of a substance can be expressed as

                                                 u ¼ uðT; vÞ:                             (7.45)
                Hence, the change in internal energy is
                                                 vu        vu

                                          du ¼       dT þ       dv                        (7.46)
                                                 vT  v     vv  T
                Now

                                                       vu

                                                 c v ¼
                                                       vT
                                                          v
             and from the Second Law,
                                               du ¼ Tds   pdv:                            (7.47)
                Substituting for Tds in Eqn (7.47) from first Tds relation (Eqn (7.38)) gives,

                                                       vp
                                         du ¼ c v dT þ T   dv   pdv                       (7.48)
                                                       vT
                                                           v
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