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30                               Entropy Analysis in Thermal Engineering Systems


          efficiency are not entirely convincing. The Carnot principles—also called
          Carnot corollaries or propositions—state that
           I. the efficiency of an irreversible engine cannot exceed that of the revers-
             ible one operating between the same thermal reservoirs,
          II. all reversible engines operating between the same two thermal reservoirs
             possess the same efficiency.



          3.2.1 Proof of corollaries
          We now briefly review the method of demonstration of Carnot’s first cor-
          ollary, which can be found in nearly all engineering thermodynamics texts.
          The method was originally presented by Carnot himself to show that his
          ideal engine is the most efficient among all engines operating between
          two fixed temperature thermal reservoirs.
             Consider an arbitrary engine A (other than Carnot engine) that operates
          between two thermal reservoirs maintained at fixed temperatures; see
          Fig. 3.1. The amount of heat transferred from the high-temperature reser-
          voir to engine A is denoted by Q HA , and the amount of heat rejected by the
          engine to the low-temperature reservoir is Q LA . The first law requires the
          work production of engine A to be W A ¼Q HA  Q LA . Next, a Carnot
          engine C is placed between the same thermal reservoirs. It receives heat
          Q HC from the high-temperature reservoir, converts a portion of the heat
          to work W C , and rejects the unused portion of the heat, Q LC , to the
          low-temperature reservoir.
             Assume that engine A is more efficient than engine C and that the
          amount of heat transfer from the high-temperature reservoir to both engines
          is the same, i.e., Q HA ¼Q HC . Thus, W A >W C and Q LC >Q LA . The


                               High-temperature thermal reservoir, T H
                            Q HC             Q HA
                                    C               A
                                                           W net
                              Carnot          Arbitrary
                             refrigerator      engine


                             Q LC            Q LA
                               Low-temperature thermal reservoir, T L
          Fig. 3.1 Illustration of an arbitrary engine and a Carnot refrigerator operating between
          the same thermal reservoirs.
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