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CHAPTER 5: SECOND LAW OF THERMODYNAMICS



                                                                 CHAPTER 5

                                                                 SECOND LAW OF

                                                                 THERMODYNAMICS


                                                                 The  branch  of  physical  science  that
                                                                 deals  with  the  relations  between  heat
                                                                 and  other  forms  of  energy  such  as
                                                                 mechanical,  electrical,  or  chemical
                                                                 energy and by  extension,  of  the
                                                                 relationships  between  all forms  of
                                                                 energy.





               5.1 Concept of Second Law of Thermodynamics

               Whenever energy is converted from one form to another, some usable energy is lost in thermal energy that
               disperses into the environment. The terms usable energy involved is entropy which measure disorder of
               randomness. Fig. 5.1 below shown where the entropy occurred in the process ice cube change to liquid
               causing the change of entropy increase and reversely process the entropy is decreased.
















                                        Fig. 5.1: Entropy, S in phase change processes [5]



               5.2 Entropy in Heat Engine

               There exist a useful thermodynamics variable called entropy, S. A natural process that starts in equilibrium
               state and ends in another will go in the direction that causes the entropy of the system plus the environment
               to increase for an irreversible process and to remain constant for a reversible process. The Fig. 5.2 below
               represent the entropy in heat engine where from cold transfer to hot engine after heat, Q supplied to produce
               work, W [6].















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