Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 4 - Dynamics: Newton's Laws of Motion - Problems - Page 104: 47

Answer

(a) $m_A = 5.0 ~kg$ (b) $m_A = 1.0 \times 10^1 ~kg$

Work Step by Step

(a) Let's assume that the acceleration is zero. Let's consider the force equation for $m_A$. $\sum ~F_x = ma$ $F_T - F_f = 0$ $F_T = F_f$ Let's consider the force equation for $m_B$. $\sum ~F = ma$ $(m_B)~g - F_T = 0$ $F_T = (m_B) ~g$ $F_f = (m_B)~g$ $(m_A)(g)(\mu_s) = (m_B) ~g$ $m_A = \frac{(m_B)}{\mu_s} = \frac{2.0 ~kg}{0.40} = 5.0 ~kg$ (b) If the system is moving at a constant speed, then the acceleration is zero. We can use the same equations from part (a) to solve this part of the question. $F_f = (m_B)~g$ $(m_A)(g)(\mu_k) = (m_B) ~g$ $m_A = \frac{(m_B)}{\mu_k} = \frac{2.0 ~kg}{0.20} = 1.0 \times 10^1~kg$
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