Page 264 - Schaum's Outline of Theory and Problems of Applied Physics
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CHAP. 21]                            THERMODYNAMICS                                   249



        SOLVED PROBLEM 21.6
              The four-cylinder, four-stroke diesel engine of a car develops 60 kW at 2600 rev/min. The pistons of this
              engine are 100 mm in diameter, and they travel 130 mm. Find the average pressure on the pistons during
              each power stroke.

                  The area of each piston is
                                             πd  2  π(0.1m) 2        2
                                          A =    =         = 0.00785 m
                                               4       4
              In a four-stroke engine a power stroke occurs in each cylinder once every 2 rev, so there are 1300 power strokes
              per minute or 1300/60 = 21.7 strokes per second. Because the engine has four cylinders, its total power output is
               P = 4P c = 4pL An and
                                                     3
                                  P            60 × 10 W                 5
                            p =      =                           = 6.8 × 10 Pa = 6.8 bar
                                                        2
                                4LAn   (4)(0.13 m)(0.00785 m )(21.7/s)
        SECOND LAWOF THERMODYNAMICS
        Internal energy resides in the kinetic energies of randomly moving atoms and molecules, whereas the output of a
        heat engine appears in the ordered motions of a piston or a wheel. Since all physical systems in the universe tend
        to go in the opposite direction, from order to disorder, no heat engine can completely convert heat to mechanical
        energy or, in general, to work. This fundamental principle leads to the second law ofthermodynamics:Itis
        impossible to construct a continuously operating engine that takes heat from a source and performs an exactly
        equivalent amount of work.
            Because some of the heat input to a heat engine must be wasted and because heat flows from a hot reservoir
        to a cold one, every heat engine must have a low-temperature reservoir for exhaust heat to go to as well as a
        high-temperature reservoir from which the input heat is to come, as in Fig. 21-1.


        CARNOTENGINE
        An ideal heat engine is one in which every process that occurs is reversible without any loss of energy. Such an
        engine is not subject to such practical mechanisms of energy loss as friction and heat conduction to the outside
        world. An example of an ideal heat engine is the imaginary Carnot engine which consists of a cylinder filled











                              T 1                            T 2
                         High-temperature                Low-temperature
                            reservoir                      reservoir














        Fig. 21-6. (Top portion from Modern Technical Physics, 6th Ed., Arthur Beiser, c  1992. Reprinted by permission of
        Pearson Education, Inc.)
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