Physics (10th Edition)

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

Chapter 6 - Work and Energy - Problems - Page 166: 24

Answer

$v_0=4.54m/s$

Work Step by Step

According to the work-energy theorem, $$W=\frac{1}{2}mv_f^2-\frac{1}{2}mv_0^2$$ We do not know the mass of the skier $m$ and his initial speed $v_0$. But we know $v_f=0$, so we can rewrite the equation: $$W=-\frac{1}{2}mv_0^2 (1)$$ Kinetic friction $f_k$ acts as the only force influencing the skier's motion by stopping it. $f_k$ opposes the motion in the opposite direction of the displacement, so $$W=(f_k\cos180)s=-f_ks$$ We have $f_k=\mu_kF_N=\mu_kmg$ (because there is no vertical acceleration). So, $$W=-\mu_kmgs (2)$$ From (1) and (2), we have $$-\frac{1}{2}mv_0^2=-\mu_kmgs$$ $$\frac{1}{2}v_0^2=\mu_kgs$$ $$v_0=\sqrt{2\mu_kgs}$$ We have $\mu_k=0.05$, $g=9.8m/s^2$ and $s=21m$ $$v_0=4.54m/s$$
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