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    • https://phys.libretexts.org/Courses/Merrimack_College/Conservation_Laws_Newton's_Laws_and_Kinematics_version_2.0/25%3A_Thermodynamics/25.04%3A_The_Second_Law_and_Entropy
      In the course of each cycle, the engine would take in an amount of heat \(Q_h\) from a “hot reservoir,” give off (or “exhaust”) an amount of heat |\(Q_c\)| to a “cold reservoir,” and produce an amount...In the course of each cycle, the engine would take in an amount of heat \(Q_h\) from a “hot reservoir,” give off (or “exhaust”) an amount of heat |\(Q_c\)| to a “cold reservoir,” and produce an amount of work |\(W\)|. (I am using absolute value bars here because, from the point of view of the engine, \(Q_c\) and \(W\) must be negative quantities.) At the end of the cycle, the engine should be back to its initial state, so \(\Delta E_{engine} = 0\).
    • https://phys.libretexts.org/Bookshelves/University_Physics/University_Physics_I_-_Classical_Mechanics_(Gea-Banacloche)/13%3A_Thermodynamics/13.04%3A_The_Second_Law_and_Entropy
      In the course of each cycle, the engine would take in an amount of heat \(Q_h\) from a “hot reservoir,” give off (or “exhaust”) an amount of heat |\(Q_c\)| to a “cold reservoir,” and produce an amount...In the course of each cycle, the engine would take in an amount of heat \(Q_h\) from a “hot reservoir,” give off (or “exhaust”) an amount of heat |\(Q_c\)| to a “cold reservoir,” and produce an amount of work |\(W\)|. (I am using absolute value bars here because, from the point of view of the engine, \(Q_c\) and \(W\) must be negative quantities.) At the end of the cycle, the engine should be back to its initial state, so \(\Delta E_{engine} = 0\).

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