Physics (10th Edition)

Published by Wiley
ISBN 10: 1118486897
ISBN 13: 978-1-11848-689-4

Chapter 6 - Work and Energy - Focus On Concepts - Page 165: 13

Answer

In d), it is not possible for mechanical energy to be conserved.

Work Step by Step

According to the principle of conservation of mechanical energy, $$E_f-E_0=0$$ $$\Big(\frac{1}{2}mv_f^2+mgh_f\Big)-\Big(\frac{1}{2}mv_0^2+mgh_0\Big)=0$$ $$\frac{1}{2}m(v_f^2-v_0^2)=mg(h_0-h_f)$$ This equation means: - If a car moves up a hill, or $(h_0-h_f)\lt0$, it follows that $(v_f^2-v_0^2)\lt0$, or the car's velocity has to continually decrease. - If a car moves down a hill, or $(h_0-h_f)\gt0$, it follows that $(v_f^2-v_0^2)\gt0$, or the car's velocity has to continually increase. - If a car moves along level ground, or $(h_0-h_f)=0$, it follows that $(v_f^2-v_0^2)=0$, or the car's velocity is constant. Therefore, only in d) is it not possible for mechanical energy to be conserved.
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